[
    {
        "id": "authors:6fa8w-y2e92",
        "collection": "authors",
        "collection_id": "6fa8w-y2e92",
        "cite_using_url": "https://authors.library.caltech.edu/records/6fa8w-y2e92",
        "type": "article",
        "title": "A recently identified mass-transport deposit stack in the Guaymas Basin, Gulf of California (M\u00e9xico), and its implication in the basin tectonics",
        "author": [
            {
                "family_name": "Pi\u00f1a",
                "given_name": "A.",
                "orcid": "0000-0002-9755-6704",
                "clpid": "Pi\u00f1a-Adriana"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Lizarralde",
                "given_name": "D."
            },
            {
                "family_name": "Hart",
                "given_name": "S."
            },
            {
                "family_name": "Marsaglia",
                "given_name": "K.",
                "orcid": "0000-0001-5430-4630"
            },
            {
                "family_name": "Gallegos-Castillo",
                "given_name": "C.",
                "orcid": "0009-0008-3262-990X"
            },
            {
                "family_name": "Berndt",
                "given_name": "C.",
                "orcid": "0000-0001-5055-0180"
            },
            {
                "family_name": "Gonz\u00e1lez-Fern\u00e1ndez",
                "given_name": "A.",
                "orcid": "0000-0002-0910-8240"
            },
            {
                "family_name": "Mortera-Guti\u00e9rrez",
                "given_name": "C.",
                "orcid": "0000-0002-8522-004X"
            },
            {
                "family_name": "Mart\u00edn-Barajas",
                "given_name": "A.",
                "orcid": "0000-0003-0338-8154"
            }
        ],
        "abstract": "<div class=\"Abstracts u-font-serif\">\n<div class=\"abstract author\">\n<div>\n<div class=\"u-margin-s-bottom\">A large mass transport deposit (MTD) stack has been identified in the Guaymas Basin using seventeen high-resolution seismic reflection profiles and sediment core analysis. Guaymas Basin is a young, marginal basin characterized by active seafloor spreading in the central Gulf of California, Mexico. The large stack includes five distinct MTD units of variable thickness, area, and volume, characterized by a predominantly transparent seismic reflection facies with small sections of laterally discontinuous reflectors and bumpy upper and erosional lower surfaces. Based on analysis of sediment cores from Site U1551A from International Ocean Discovery Program Expedition 385, we define MTD lithofacies and use sand provenance to infer that the MTD stack originated from the Yaqui Delta region of the Sonoran margin, transporting material to the south-west. We suggest that a combination of high sedimentation rates and active tectonics contributed to the MTD events. &lsquo;Flower structures&rsquo; observed in margin-crossing profiles indicate that the MTD stack buried a part of the transform fault separating the Guaymas Basin and the continental Sonoran margin. Seismic reflection interpretations suggest that part of the MTD stack filled the southern graben applying local stresses that drove a change of the sediment surface expression of plate spreading in the sediment-filled basin. In response to the MTD emplacement and the southern graben fill, an additional northern seafloor graben in the Guaymas Basin developed. Our results contribute to the understanding of the interactions among high sedimentation rates, continental slope stability, and active tectonics; and the influence of those interactions on the surface expression of plate spreading in the Guaymas Basin.</div>\n</div>\n</div>\n</div>",
        "doi": "10.1016/j.margeo.2025.107592",
        "issn": "0025-3227",
        "publisher": "Elsevier",
        "publication": "Marine Geology",
        "publication_date": "2025-10",
        "volume": "488",
        "pages": "107592"
    },
    {
        "id": "authors:4kv23-t7252",
        "collection": "authors",
        "collection_id": "4kv23-t7252",
        "cite_using_url": "https://authors.library.caltech.edu/records/4kv23-t7252",
        "type": "article",
        "title": "Fault interactions and subsurface deformation in the Mexicali valley: Implications for seismic hazard assessment at the M\u00e9xico-USA border",
        "author": [
            {
                "family_name": "Gallegos-Castillo",
                "given_name": "Cristian A."
            },
            {
                "family_name": "Gonz\u00e1lez-Escobar",
                "given_name": "Mario",
                "orcid": "0000-0002-6061-9695"
            },
            {
                "family_name": "Reyes-L\u00f3pez",
                "given_name": "Jaime A."
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Arregui-Ojeda",
                "given_name": "Sergio M."
            },
            {
                "family_name": "Reyes-Mart\u00ednez",
                "given_name": "Carlos Sim\u00f3n"
            },
            {
                "family_name": "Mastache-Rom\u00e1n",
                "given_name": "Edgar A."
            }
        ],
        "abstract": "<div class=\"Abstracts u-font-serif\">\n<div class=\"abstract author\">\n<div>\n<div class=\"u-margin-s-bottom\">This study investigates both previously known and unidentified subsurface deformation structures in the northwesternmost sector of the Mexicali Valley, M&eacute;xico, near the international border with the USA. Several subsurface structures, including the Michoac&aacute;n fault, have been identified between the Imperial-Laguna Salada fault zones by analyzing seismic reflection profiles, and their locations have been correlated with seismicity patterns. This study highlights the northward extension of the Michoac&aacute;n fault beyond the border with the United States. While the trace of this fault has been reported elsewhere, some evidence has associated the existing deformation with a distinct, previously unknown structure; herein, named the Progreso Fault. The Dixieland Fault (USA) is not observed in M&eacute;xico; however, the interaction of these faults plays a significant role in the regional seismic activity. Slip is distributed throughout the sector and is not concentrated on specific faults such as the Michoac&aacute;n or Imperial. Faults with different orientations located between the Michoac&aacute;n and Imperial Fault zones represent the potential northern limit of the Cerro Prieto Pull-Apart Basin. Additionally, several sub-basins have been identified in the study area. Although the two-dimensional seismic imagery used in this study does not allow for slip rate calculations on the faults, the observed structures provide valuable information about displacement and subsurface deformation in the region. The structures reported here contribute to the SCEC Community Fault Model (CFM), which integrates seismic reflection and other geological and geophysical data to define fault geometries. The CFM serves as a key input for physics-based fault system modeling and probabilistic seismic hazard assessments, including the Uniform California Earthquake Rupture Forecast (UCERF3). Consequently, the findings will aid in understanding regional fault interactions, providing essential constraints for future research and facilitating a better understanding of seismic hazards in the M&eacute;xico-USA border region.</div>\n</div>\n</div>\n</div>",
        "doi": "10.1016/j.tecto.2025.230803",
        "issn": "0040-1951",
        "publisher": "Elsevier",
        "publication": "Tectonophysics",
        "publication_date": "2025-08-04",
        "volume": "910",
        "pages": "230803"
    },
    {
        "id": "authors:c50fb-v4g76",
        "collection": "authors",
        "collection_id": "c50fb-v4g76",
        "cite_using_url": "https://authors.library.caltech.edu/records/c50fb-v4g76",
        "type": "article",
        "title": "Sill Stacking in Subseafloor Unconsolidated Sediments and Control on Sustained Hydrothermal Systems: Evidence From IODP Drilling in the Guaymas Basin, Gulf of California",
        "author": [
            {
                "family_name": "Galerne",
                "given_name": "Christophe",
                "orcid": "0000-0001-9696-205X"
            },
            {
                "family_name": "Cheviet",
                "given_name": "Alban",
                "orcid": "0000-0001-9960-029X"
            },
            {
                "family_name": "Kahl",
                "given_name": "Wolf\u2010Achim",
                "orcid": "0000-0003-3342-9893"
            },
            {
                "family_name": "Wiggers",
                "given_name": "Christin",
                "orcid": "0000-0003-0991-9796"
            },
            {
                "family_name": "Bach",
                "given_name": "Wolfgang"
            },
            {
                "family_name": "Neumann",
                "given_name": "Florian"
            },
            {
                "family_name": "Buatier",
                "given_name": "Martine"
            },
            {
                "family_name": "H\u00f6fig",
                "given_name": "Tobias W."
            },
            {
                "family_name": "Lizarralde",
                "given_name": "Daniel",
                "orcid": "0000-0001-6152-6039"
            },
            {
                "family_name": "Teske",
                "given_name": "Andreas",
                "orcid": "0000-0003-3669-5425"
            },
            {
                "family_name": "Pe\u00f1a\u2010Salinas",
                "given_name": "Manet",
                "orcid": "0000-0002-5835-0455"
            },
            {
                "family_name": "Karstens",
                "given_name": "Jens",
                "orcid": "0000-0002-9434-2479"
            },
            {
                "family_name": "B\u00f6ttner",
                "given_name": "Christoph",
                "orcid": "0000-0001-7321-0699"
            },
            {
                "family_name": "Berndt",
                "given_name": "Christian",
                "orcid": "0000-0001-5055-0180"
            },
            {
                "family_name": "Aiello",
                "given_name": "Ivano W.",
                "orcid": "0000-0001-9794-6852"
            },
            {
                "family_name": "Marsaglia",
                "given_name": "Kathleen M."
            },
            {
                "family_name": "Gontharet",
                "given_name": "Swanne"
            },
            {
                "family_name": "Kuhnert",
                "given_name": "Henning",
                "orcid": "0000-0001-5242-4495"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Negrete\u2010Aranda",
                "given_name": "Raquel",
                "orcid": "0000-0003-3049-4374"
            },
            {
                "family_name": "Zhang",
                "given_name": "Junli",
                "orcid": "0000-0002-2546-8633"
            },
            {
                "family_name": "Kopf",
                "given_name": "Achim"
            }
        ],
        "abstract": "<div class=\"article-section__content en main\">\n<p>Magma emplacement in the top unconsolidated sediments of rift basins is poorly understood. We compare two shallow sills from the Guaymas Basin (Gulf of California) using core data and analyses from IODP Expedition 385, and high-resolution 2D seismic data. We show that magma stalling in the top uncemented sediment layer is controlled by the transition from siliceous claystone to uncemented silica-rich sediment, favoring flat sill formation. Space is created through a combination of viscous indentation, magma-sediment mingling and fluidization processes. We show that sills emplace above the opal-A/CT diagenetic barrier. Our model suggests that in low magma input regions sills emplace at constant depth from the seafloor, while high magma input leads to upward stacking of sills, culminating in a funnel-shaped intrusions. Our petrophysical, petrographic, and textural analyses show that magma-sediment mingling creates significant porosity (up to 20%) through thermal cracking of the assimilated sediment. Stable isotope data suggest carbonate formation at 70&ndash;90&deg;C, consistent with background geothermal gradient at 250&ndash;325 m depth. The unconsolidated, water-rich host sediments produce little thermogenic gas through contact metamorphism, but deep diagenetically formed gas bypasses the low-permeability top sediments via hydrothermal fluids flowing through the magma plumbing system. This hydrothermal system provides a steady supply of hydrocarbons at temperatures amendable for microbial life, serving as an incubator that may be abundant in magma-rich young rift basins and play a key role in sustaining subseafloor ecosystems.</p>\n</div>",
        "doi": "10.1029/2024jb030354",
        "issn": "2169-9313",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research: Solid Earth",
        "publication_date": "2025-03",
        "series_number": "3",
        "volume": "130",
        "issue": "3",
        "pages": "e2024JB030354"
    },
    {
        "id": "authors:2c1xr-18s12",
        "collection": "authors",
        "collection_id": "2c1xr-18s12",
        "cite_using_url": "https://authors.library.caltech.edu/records/2c1xr-18s12",
        "type": "article",
        "title": "Nitrogen isotope homogenization of dissolved ammonium with depth and \u00b9\u2075N enrichment of ammonium during incorporation into expandable layer silicates in organic-rich marine sediment from Guaymas Basin, Gulf of California",
        "author": [
            {
                "family_name": "Yamanaka",
                "given_name": "Toshiro"
            },
            {
                "family_name": "Sakamoto",
                "given_name": "Arisa"
            },
            {
                "family_name": "Kiyokawa",
                "given_name": "Kanon"
            },
            {
                "family_name": "Jo",
                "given_name": "Jaeguk"
            },
            {
                "family_name": "Onishi",
                "given_name": "Yuji"
            },
            {
                "family_name": "Kuwahara",
                "given_name": "Yoshihiro"
            },
            {
                "family_name": "Kim",
                "given_name": "Ji-Hoon"
            },
            {
                "family_name": "Pastor",
                "given_name": "Lucie C."
            },
            {
                "family_name": "Teske",
                "given_name": "Andreas"
            },
            {
                "family_name": "Lizarralde",
                "given_name": "Daniel"
            },
            {
                "family_name": "H\u00f6fig",
                "given_name": "Tobias W."
            },
            {
                "family_name": "Aiello",
                "given_name": "Ivano W."
            },
            {
                "family_name": "Ash",
                "given_name": "Jeanine L."
            },
            {
                "family_name": "Bojanova",
                "given_name": "Diana P."
            },
            {
                "family_name": "Buatier",
                "given_name": "Martine D."
            },
            {
                "family_name": "Edgcomb",
                "given_name": "Virginia P."
            },
            {
                "family_name": "Galerne",
                "given_name": "Christophe Y."
            },
            {
                "family_name": "Gontharet",
                "given_name": "Swanne"
            },
            {
                "family_name": "Heuer",
                "given_name": "Verena B."
            },
            {
                "family_name": "Jiang",
                "given_name": "Shijun"
            },
            {
                "family_name": "Kars",
                "given_name": "Myriam A.C."
            },
            {
                "family_name": "Koornneef",
                "given_name": "Louise M.T."
            },
            {
                "family_name": "Marsaglia",
                "given_name": "Kathleen M."
            },
            {
                "family_name": "Meyer",
                "given_name": "Nicolette R."
            },
            {
                "family_name": "Morono",
                "given_name": "Yuki"
            },
            {
                "family_name": "Negrete-Aranda",
                "given_name": "Raquel"
            },
            {
                "family_name": "Neumann",
                "given_name": "Florian"
            },
            {
                "family_name": "Pe\u00f1a-Salinas",
                "given_name": "Manet E."
            },
            {
                "family_name": "P\u00e9rez-Cruz",
                "given_name": "Ligia L."
            },
            {
                "family_name": "Ran",
                "given_name": "Lihua"
            },
            {
                "family_name": "Riboulleau",
                "given_name": "Armelle"
            },
            {
                "family_name": "Sarao",
                "given_name": "John A."
            },
            {
                "family_name": "Schubert",
                "given_name": "Florian"
            },
            {
                "family_name": "Singh",
                "given_name": "S. Khogenkumar"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Toffin",
                "given_name": "Laurent"
            },
            {
                "family_name": "Xie",
                "given_name": "Wei"
            },
            {
                "family_name": "Zhuang",
                "given_name": "Guangchao"
            }
        ],
        "contributor": [
            {
                "family_name": "IODP Expedition 385 Scientists"
            }
        ],
        "abstract": "<div class=\"Abstracts u-font-serif\">\n<div class=\"abstract author\">\n<div>\n<div class=\"u-margin-s-bottom\">Sedimentary nitrogen isotopic ratios are used as a proxy for ancient biogeochemical cycles on Earth's surface. It is generally accepted that sediment hole tops record primary signatures because organic nitrogen (ON) is predominant in this part of the hole. In contrast to such early to middle diagenetic stages, it is well known that heavier nitrogen isotope&nbsp;<sup>15</sup>N tends to enrich in sedimentary rocks during later diagenetic and metamorphic stages. However, there are some critical gaps in our understanding of nitrogen isotopic alteration associated with abiotic processes during early-middle diagenesis. In this study, we examined the isotope ratios of ammonium nitrogen in interstitial water (IW) and total nitrogen (TN), including exchangeable ammonium and mineral nitrogen, in the solid-phase of organic-rich-sediment recovered by International Ocean Discovery Program (IODP) Expedition 385 cores drilled in the Guaymas Basin, Gulf of California, that contained ammonium-rich IW. The isotopic ratios (&delta;<sup>15</sup>N value) of TN are the most variable with depth compared to any other type of nitrogen. This variation can be interpreted as reflecting changes in the water mass environment in the basin caused by glacial&ndash;interglacial climate changes, modifying the &delta;<sup>15</sup>N values of the marine primary producers. Thus, the &delta;<sup>15</sup>N value of TN is a proxy for environmental change in the basin, while each component of TN shows different trends. The &delta;<sup>15</sup>N values of IW and exchangeable ammonium did not exhibit significant changes with depth, but the latter values are about 3 &permil; enriched in&nbsp;<sup>15</sup>N. This may be due to advective transport of solute into adjacent layers followed by the formation of an isotopic equilibrium between IW and exchangeable ammonium in the case of fast sediment accumulation rate. The &delta;<sup>15</sup>N value of exchangeable ammonium is the highest among the other types of nitrogen with one exception, where the &delta;<sup>15</sup>N value of TN is the highest. The calculated &delta;<sup>15</sup>N values of ON based on mass balance are almost the same as those of associated TN in the shallow sediment layers (&lt; 150&nbsp;m below seafloor), but the difference in the &delta;<sup>15</sup>N values of TN and ON are significant in the deeper layers, where proportions of ON contents are &lt;50%. In particular, in the layer where the &delta;<sup>15</sup>N value of TN is the highest, that of ON shows an even higher value and the difference reaches 3.5 &permil;. The &delta;<sup>15</sup>N values of mineral nitrogen are similar to that of IW ammonium except the surface layers. Under such conditions, when &delta;<sup>15</sup>N value of TN is intermediate between those of mineral nitrogen and exchangeable ammonium, calculated &delta;<sup>15</sup>N value of ON is close to that of TN. On the other hand, if &delta;<sup>15</sup>N value of TN is out of the range between mineral nitrogen and exchangeable ammonium, it causes further difference in &delta;<sup>15</sup>N value of ON. It means that the fluctuation of &delta;<sup>15</sup>N values of TN is reduced relative to those of ON through depth. It has been considered that &delta;<sup>15</sup>N value of TN in sediment is similar to that of ON, and changes in the &delta;<sup>15</sup>N value of TN due to diagenesis are limited, but in such environment ON fluctuations over depth may be slightly underestimated.</div>\n</div>\n</div>\n</div>\n<div></div>",
        "doi": "10.1016/j.chemgeo.2024.122203",
        "issn": "0009-2541",
        "publisher": "Elsevier",
        "publication": "Chemical Geology",
        "publication_date": "2024-10-20",
        "volume": "666",
        "pages": "122203"
    },
    {
        "id": "authors:44rre-98m53",
        "collection": "authors",
        "collection_id": "44rre-98m53",
        "cite_using_url": "https://authors.library.caltech.edu/records/44rre-98m53",
        "type": "article",
        "title": "Mineralization kinetics of biosiliceous sediments in hot subseafloors",
        "author": [
            {
                "family_name": "Aiello",
                "given_name": "Ivano W.",
                "orcid": "0000-0001-9794-6852",
                "clpid": "Aiello-Ivano-W"
            },
            {
                "family_name": "H\u00f6fig",
                "given_name": "Tobias W.",
                "orcid": "0000-0002-9254-4528",
                "clpid": "H\u00f6fig-Tobias-W"
            },
            {
                "family_name": "Riboulleau",
                "given_name": "Armelle",
                "orcid": "0000-0002-2717-8330",
                "clpid": "Riboulleau-Armelle"
            },
            {
                "family_name": "Teske",
                "given_name": "Andreas P.",
                "clpid": "Teske-Andreas-P"
            },
            {
                "family_name": "Lizarralde",
                "given_name": "Daniel",
                "orcid": "0000-0001-6152-6039",
                "clpid": "Lizarralde-Daniel"
            },
            {
                "family_name": "Ash",
                "given_name": "Jeanine L.",
                "clpid": "Ash-Jeanine-L"
            },
            {
                "family_name": "Bojanova",
                "given_name": "Diana P.",
                "clpid": "Bojanova-Diana-P"
            },
            {
                "family_name": "Buatier",
                "given_name": "Martine D.",
                "orcid": "0000-0003-3863-5127",
                "clpid": "Buatier-Martine-D"
            },
            {
                "family_name": "Edgcomb",
                "given_name": "Virginia P.",
                "clpid": "Edgcomb-Virginia-P"
            },
            {
                "family_name": "Galerne",
                "given_name": "Christophe Y.",
                "orcid": "0000-0001-9696-205X",
                "clpid": "Galerne-Christophe-Y"
            },
            {
                "family_name": "Gontharet",
                "given_name": "Swanne",
                "clpid": "Gontharet-Swanne"
            },
            {
                "family_name": "Heuer",
                "given_name": "Verena B.",
                "orcid": "0000-0002-1856-116X",
                "clpid": "Heuer-Verena-B"
            },
            {
                "family_name": "Jiang",
                "given_name": "Shijun",
                "clpid": "Jiang-Shijun"
            },
            {
                "family_name": "Kars",
                "given_name": "Myriam A.C.",
                "orcid": "0000-0002-4984-1412",
                "clpid": "Kars-Myriam-A-C"
            },
            {
                "family_name": "Kim",
                "given_name": "Koornneef",
                "orcid": "0000-0003-2430-3869",
                "clpid": "Kim-Koornneef"
            },
            {
                "family_name": "Koornneef",
                "given_name": "Louise M.T.",
                "orcid": "0000-0002-8016-1167",
                "clpid": "Koornneef-Louise-M-T"
            },
            {
                "family_name": "Marsaglia",
                "given_name": "Kathleen M.",
                "orcid": "0000-0001-5430-4630",
                "clpid": "Marsaglia-Kathleen-M"
            },
            {
                "family_name": "Meyer",
                "given_name": "Nicolette R.",
                "clpid": "Meyer-Nicolette-R"
            },
            {
                "family_name": "Morono",
                "given_name": "Yuki",
                "clpid": "Morono-Yuki"
            },
            {
                "family_name": "Negrete-Aranda",
                "given_name": "Raquel",
                "clpid": "Negrete-Aranda-Raquel"
            },
            {
                "family_name": "Neumann",
                "given_name": "Florian",
                "orcid": "0000-0002-9666-5087",
                "clpid": "Neumann-Florian"
            },
            {
                "family_name": "Pastor",
                "given_name": "Lucie C.",
                "orcid": "0000-0001-9732-8907",
                "clpid": "Pastor-Lucie-C"
            },
            {
                "family_name": "Pe\u00f1a-Salinas",
                "given_name": "Manet E.",
                "orcid": "0000-0002-5835-0455",
                "clpid": "Pe\u00f1a-Salinas-Manet-E"
            },
            {
                "family_name": "P\u00e9rez-Cruz",
                "given_name": "Ligia L.",
                "clpid": "P\u00e9rez-Cruz-Ligia-L"
            },
            {
                "family_name": "Ran",
                "given_name": "Lihua",
                "clpid": "Ran-Lihua"
            },
            {
                "family_name": "Sarao",
                "given_name": "John A.",
                "clpid": "Sarao-John-A"
            },
            {
                "family_name": "Schubert",
                "given_name": "Florian",
                "clpid": "Schubert-Florian"
            },
            {
                "family_name": "Khogenkumar Singh",
                "given_name": "S.",
                "clpid": "Khogenkumar-Singh-S"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Toffin",
                "given_name": "Laurent",
                "clpid": "Toffin-Laurent"
            },
            {
                "family_name": "Xie",
                "given_name": "Wei",
                "orcid": "0000-0002-9742-9369",
                "clpid": "Xie-Wei"
            },
            {
                "family_name": "Yamanaka",
                "given_name": "Toshiro",
                "clpid": "Yamanaka-Toshiro"
            },
            {
                "family_name": "Zhuang",
                "given_name": "Guangchao",
                "clpid": "Zhuang-Guangchao"
            }
        ],
        "abstract": "<div class=\"Abstracts u-font-serif\">\n<div class=\"abstract author\">\n<div>\n<p>Temperature affects the timing of the transformation of amorphous silica (opal-A) into crystalline (opal-CT) exponentially. Thus, in hot subseafloor environments opal-A is expected to convert into opal-CT at relatively shallow burial depths, where&nbsp;<em>in situ</em>&nbsp;temperatures do not exceed&nbsp;&sim;56&nbsp;&deg;C, as it has been previously observed at various deep-sea sites and in onshore rock outcrops as well as assessed during lab experiments. The response of biosilica (biogenic opal-A)&nbsp;<a class=\"topic-link\" title=\"Learn more about diagenesis from ScienceDirect's AI-generated Topic Pages\" href=\"https://www.sciencedirect.com/topics/earth-and-planetary-sciences/diagenesis\">diagenesis</a>&nbsp;to steep&nbsp;<a class=\"topic-link\" title=\"Learn more about geothermal gradients from ScienceDirect's AI-generated Topic Pages\" href=\"https://www.sciencedirect.com/topics/earth-and-planetary-sciences/geothermal-gradient\">geothermal gradients</a>&nbsp;(&sim;224&ndash;529&nbsp;&deg;C/km) at extremely high&nbsp;<a class=\"topic-link\" title=\"Learn more about sedimentation rates from ScienceDirect's AI-generated Topic Pages\" href=\"https://www.sciencedirect.com/topics/earth-and-planetary-sciences/sedimentation-rate\">sedimentation rates</a>&nbsp;(&sim;1 m/kyr) was examined in cores from off-axis boreholes drilled by the International Ocean Discovery Program (IODP) Expedition 385 in the actively spreading, intrusive sill-riddled Guaymas Basin at the Gulf of California (Mexico) rifted margin. At three sites drilled by IODP Expedition 385 (U1545, U1546, and U1547), the conversion from amorphous opal (&minus;A) to crystalline opal (&minus;CT) occurs in relatively deep (up to&nbsp;&sim;330 mbsf) and unexpectedly hot (<em>in situ</em>&nbsp;temperatures of&nbsp;&sim;74&ndash;79&nbsp;&deg;C) subseafloor conditions. This observation indicates a significantly slower reaction kinetics of biosilica transformation than previously reported. A compilation of empirical data that include biosiliceous basins with a similarly hot subseafloor (Sea of Japan and Bering Sea) yield new kinetic parameters that account for the slower rates of silica transformation. Thus, current kinetic models for the prediction of opal-A to &minus;CT conversion face limitations when burial rates exceed those typical of biogenic sedimentation in open-ocean conditions. At Guaymas Basin Site U1545, where there is no evidence of sill-related metamorphic overprint, the d-spacing of the opal-CT (1&nbsp;0&nbsp;1) peak correlates linearly with&nbsp;<em>in situ</em> temperature between&nbsp;&sim;75 and 110&nbsp;&deg;C throughout the opal-CT zone, thus, providing a local silica paleothermometry proxy that can be used to calculate the maximum temperature to which opal-CT sediment has been subjected.</p>\n</div>\n</div>\n</div>\n<div></div>",
        "doi": "10.1016/j.gca.2024.07.005",
        "issn": "0016-7037",
        "publisher": "Elsevier",
        "publication": "Geochimica et Cosmochimica Acta",
        "publication_date": "2024-09-01",
        "volume": "380",
        "pages": "71-82"
    },
    {
        "id": "authors:fjnzj-d1y66",
        "collection": "authors",
        "collection_id": "fjnzj-d1y66",
        "cite_using_url": "https://authors.library.caltech.edu/records/fjnzj-d1y66",
        "type": "article",
        "title": "Synthesis of Current Seismicity and Tectonics Along the 1857 M_w 7.9 Fort Tejon Earthquake Rupture and the Southernmost San Andreas Fault, California, USA",
        "author": [
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Jones",
                "given_name": "Lucile M.",
                "orcid": "0000-0002-2690-3051",
                "clpid": "Jones-L-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Husker",
                "given_name": "Allen L.",
                "orcid": "0000-0003-1139-0502",
                "clpid": "Husker-Allen-L"
            }
        ],
        "abstract": "<div class=\"article-section__content en main\">\n<p>We evaluate seismicity and tectonics along the San Andreas Fault (SAF) in southern California to elucidate ongoing near-field crustal deformation processes. The principal slip surfaces (PSSs) or the fault core that accommodate major earthquakes, form the boundary between the tectonic plates. We analyze seismicity catalogs extending back to 1857, 1932, and 1981 with progressively improved magnitude of completeness and spatial resolution. The 1857 to present statewide catalog that is complete at M5.5+ documents minimal aftershock activity for the M<sub>w</sub>7.9 1857 and 1906 M<sub>w</sub>7.8 San Francisco earthquakes. The higher quality 1932 and 1981 catalogs show that the PSSs (the rupture zone) of the 1857 M<sub>w</sub>7.9 Fort Tejon earthquake exhibits remarkable seismic quiescence both in the core and in the adjacent extended-damage zone. Further south, the fault core is still aseismic but the shape of the SAF is more complex, and the rate of adjacent seismicity is much higher. This fault complexity and the seismicity rate are larger the more the strike of the SAF deviates from the Pacific plate velocity-vector direction. The focal mechanisms of the SAF adjacent earthquakes are also heterogeneous and rarely have strikes and dips that are consistent with slip on the nearby PSSs. We infer that the southern SAF is locked, and a lack of seismicity at the core of the fault may be a standard feature of faults that almost exclusively accommodate high-slip rates by producing major earthquakes. Correspondingly future aftershock sequences of major earthquakes on the southern SAF will likely have below average aftershock productivity.</p>\n</div>",
        "doi": "10.1029/2024jb028893",
        "issn": "2169-9313",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research: Solid Earth",
        "publication_date": "2024-06",
        "series_number": "6",
        "volume": "129",
        "issue": "6",
        "pages": "e2024JB028893"
    },
    {
        "id": "authors:r56f7-h9z29",
        "collection": "authors",
        "collection_id": "r56f7-h9z29",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220916-666042000",
        "type": "article",
        "title": "Seismicity in a weak crust: the transtensional tectonics of the Brawley Seismic Zone section of the Pacific-North America Plate Boundary in Southern California, USA",
        "author": [
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Husker",
                "given_name": "Allen",
                "orcid": "0000-0003-1139-0502",
                "clpid": "Husker-Allen-L"
            }
        ],
        "abstract": "The Brawley Seismic Zone (BSZ) is a \u223c58-km-long section of the Pacific\u2013North America Plate boundary that connects the southernmost San Andreas Fault (SAF) and the Imperial Fault in southern California. We analyse the BSZ as two segments: a north segment, dominated by SAF tectonics, and a south segment that accommodates a higher level of seismicity. The south segment includes a \u223c6 km wide right lateral step-over that includes the Salton Sea geothermal field (SSGF) and Holocene subaerial lava domes at the south end of the Salton Sea, called Salton Buttes. In general, the 40 yr (1981\u20132021) of BSZ seismicity is characterized by transitory sequences that often are accommodated simultaneously or in quick succession on intricate ladder-like faults. These sequences rarely reactivate faults associated with previous seismicity alignments but rather activate adjacent faults, sometimes located within less than 1 km. They can include several events of similar size as the mainshock, followed by bursts of aftershocks sometimes located away from the mainshock rupture. The seismicity rate and the spatial geometrical complexity varies between the BSZ-north and BSZ-south segments. The 24-km-long BSZ-north accommodates a \u223c12-km-long linear trend of seismicity that extends from the SAF terminus into the Salton Sea, where moderate-sized northeast striking sequences form the rungs in a ladder-structure in a weak crust. The seismicity in this area is most likely influenced by the stress state of the SAF. In contrast, the 34 km long BSZ-south segment, which also has a weak crust, has accommodated larger sequences that illuminate irregular ladder-type faulting, with aftershocks defining linear distributions striking either north or northeast. The focal mechanisms exhibit a mostly strike-slip style of faulting with minor dip-slip faulting in the south Salton Sea area as well as the Mesquite basin to the south. The state of stress, as determined from focal mechanisms, consists of almost horizontal \u03c3\u2081, and \u03c3\u2083 with vertical \u03c3\u2082. The activation angle between the trend of \u03c3\u2081 and the preferred nodal plane of the largest nearby event decreases systematically from north to south along the long-axis of the BSZ. In the step-over zone, the Holocene volcanism and the frequent seismicity sequences suggest crustal extension as well as associated reduced crustal strength as compared to other parts of the BSZ. The presence of weak, thin, hot crust and distributed ladder-like or conjugate predominantly strike-slip faulting suggests that the whole BSZ acts as a several kilometre wide fault zone where no prominent principal slip surfaces are required to accommodate moderate-sized (M6+) earthquakes.",
        "doi": "10.1093/gji/ggac205",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2022-10",
        "series_number": "1",
        "volume": "231",
        "issue": "1",
        "pages": "717-735"
    },
    {
        "id": "authors:tkmc5-mf195",
        "collection": "authors",
        "collection_id": "tkmc5-mf195",
        "cite_using_url": "https://authors.library.caltech.edu/records/tkmc5-mf195",
        "type": "article",
        "title": "Structure of the Northern Altar Pull-Apart Basin Revealed by a 2D Reflection Seismic Survey: Evolution of the Gulf of California Shear Zone in Northwest Mexico",
        "author": [
            {
                "family_name": "Huerta",
                "given_name": "Jorge Antonio Puente",
                "orcid": "0000-0003-0392-2775"
            },
            {
                "family_name": "Gonz\u00e1lez-Escobar",
                "given_name": "Mario",
                "orcid": "0000-0002-6061-9695"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The northern Gulf of California and Salton Trough contain segmented marginal basins abandoned during the oblique rift system's evolution during Late Miocene-Early Pliocene. The Altar basin, in northwestern Sonora, Mexico, contains a\u2009&gt;\u20095\u00a0km-thick sedimentary record representing the first marine incursion (Late Miocene) of the Gulf of California seaway followed by the first deltaic deposits of the Colorado River. 2D reflection seismic lines were processed and interpreted to characterize tectonostratigraphic features of the transtensional Pacific-North America plate boundary in the northern Altar basin (deep structure, faults controlling the subsidence and accumulation of deltaic deposits). The results show the acoustic basement becoming increasingly shallow toward the northeast, new NW-trending faults, and three major seismic reflectors defining the base of three units: A (oldest), B, and C (youngest). Through similarities in sequence stratigraphy and fauna, we correlate Unit A with the Bouse Formation (SW Arizona and SE California), implying its presence in northwest Mexico. The Altar fault strikes\u2009~\u2009N45\u00b0W and aligns with the Dunas fault (SE California), suggesting that these faults are the same continuous structure. Seismic horizons above horizon C are less affected by faults. In contrast, horizons A, B and C are cut by faults, have steeper dips, and are laterally discontinuous. We propose the deposition of unfaulted strata occurred after the latest Pliocene abandonment of the Altar basin. Cessation of major transtensional activity in the Altar basin is coincident with a regional westward shift of transtensional plate boundary deformation, preserving a record of the evolving Gulf of California shear zone in northwest Mexico.",
        "doi": "10.1007/s00024-022-03138-1",
        "issn": "0033-4553",
        "publisher": "Springer Science and Business Media LLC",
        "publication": "Pure and Applied Geophysics",
        "publication_date": "2022-09",
        "series_number": "9",
        "volume": "179",
        "issue": "9",
        "pages": "3191-3216"
    },
    {
        "id": "authors:gtfmy-wjv41",
        "collection": "authors",
        "collection_id": "gtfmy-wjv41",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220422-974200",
        "type": "article",
        "title": "Shallow distributed faulting in the Imperial Valley, California, USA",
        "author": [
            {
                "family_name": "Sahakian",
                "given_name": "Valerie J.",
                "clpid": "Sahakian-Valerie-J"
            },
            {
                "family_name": "Derosier",
                "given_name": "Boe J.",
                "clpid": "Derosier-Boe-J"
            },
            {
                "family_name": "Rockwell",
                "given_name": "Thomas K.",
                "orcid": "0000-0001-5319-6447",
                "clpid": "Rockwell-Thomas-K"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "In the tectonically complex Imperial Valley, California (USA), the Imperial fault (IF) is often considered to be the primary fault at the U.S.-Mexico border; however, its strain partitioning and interactions with other faults are not well understood. Despite inferred evidence of other major faults (e.g., seismicity), it is difficult to obtain a holistic view of this system due to anthropogenic surface modifications. To better define the structural configuration of the plate-boundary strain in this region, we collected high-resolution shallow seismic imaging data in the All American Canal, crossing the Imperial, Dixieland, and Michoac\u00e1n faults. These data image shallow (&lt;25 m) structures on and near the mapped trace of the Imperial fault, as well as the Michoac\u00e1n fault and adjacent stepover. Integration of our data with nearby terrestrial cores provides age constraints on Imperial fault deformation. These data suggest that the Michoac\u00e1n fault, unmapped in the United States, is active and likely produces dynamic or off-fault deformation within its stepover to the Dixieland fault. Together, these data support more strain partitioning than previously documented in this region.",
        "doi": "10.1130/g49572.1",
        "issn": "0091-7613",
        "publisher": "Geological Society of America",
        "publication": "Geology",
        "publication_date": "2022-05-01",
        "series_number": "5",
        "volume": "50",
        "issue": "5",
        "pages": "626-630"
    },
    {
        "id": "authors:p1r9x-dvx10",
        "collection": "authors",
        "collection_id": "p1r9x-dvx10",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220414-27940000",
        "type": "article",
        "title": "Co-seismic and post-seismic deformation for the 1995 Colima\u2013Jalisco and 2003 Tecom\u00e1n thrust earthquakes, Mexico subduction zone, from modelling of GPS data",
        "author": [
            {
                "family_name": "Cosenza-Muralles",
                "given_name": "B.",
                "orcid": "0000-0002-4626-2757",
                "clpid": "Cosenza-Muralles-Ana-Beatriz"
            },
            {
                "family_name": "DeMets",
                "given_name": "C.",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "M\u00e1rquez-Az\u00faa",
                "given_name": "B.",
                "clpid": "M\u00e1rquez-Az\u00faa-Bertha"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "orcid": "0000-0003-1683-0247",
                "clpid": "S\u00e1nchez-Zamora-Osvaldo"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Cabral-Cano",
                "given_name": "E.",
                "orcid": "0000-0002-9143-2401",
                "clpid": "Cabral-Cano-Enrique"
            },
            {
                "family_name": "McCaffrey",
                "given_name": "R.",
                "orcid": "0000-0002-1291-3494",
                "clpid": "McCaffrey-Robert"
            }
        ],
        "abstract": "We invert \u223c25\u00a0yr of campaign and continuous Global Positioning System daily positions at 62 sites in southwestern Mexico to estimate co-seismic and post-seismic afterslip solutions for the 1995 M_w = 8.0 Colima\u2013Jalisco and the 2003 M_w = 7.5 Tecom\u00e1n earthquakes, and the long-term velocity of each GPS site. Estimates of the viscoelastic effects of both earthquakes from a 3-D model with an elastic crust and subducting slab, and linear Maxwell viscoelastic mantle are used to correct the GPS position time-series prior to our time-dependent inversions. The preferred model, which optimizes the fit to data from several years of rapid post-seismic deformation after the larger 1995 earthquake, has a mantle Maxwell time of 15\u00a0yr (viscosity of 2 \u00d7 10\u00b9\u2079 Pa\u2009s), although upper-mantle viscosities as low as 5 \u00d7 10\u00b9\u2078 Pa\u2009s cannot be excluded. Our geodetic slip solutions for both earthquakes agree well with previous estimates derived from seismic data or via static co-seismic offset modelling. The afterslip solutions for both earthquakes suggest that most afterslip coincided with the rupture areas or occurred farther downdip and had cumulative moments similar to or larger than the co-seismic moments. Afterslip thus appears to relieve significant stress along the Rivera plate subduction interface, including the area of the interface between a region of deep non-volcanic tremor and the shallower seismogenic zone. We compare the locations of the seismogenic zone, afterslip and tremor in our study area to those of the neighbouring Guerrero and Oaxaca segments of the Mexico subduction zone. Our newly derived interseismic GPS site velocities, the first for western Mexico that are corrected for the co-seismic and post-seismic effects of the 1995 and 2003 earthquakes, are essential for future estimates of the interseismic subduction interface locking and hence the associated seismic hazard.",
        "doi": "10.1093/gji/ggab435",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2022-03",
        "series_number": "3",
        "volume": "228",
        "issue": "3",
        "pages": "2137-2173"
    },
    {
        "id": "authors:42k5z-qqf19",
        "collection": "authors",
        "collection_id": "42k5z-qqf19",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220414-27889000",
        "type": "article",
        "title": "GPS-derived interseismic fault locking along the Jalisco\u2013Colima segment of the Mexico subduction zone",
        "author": [
            {
                "family_name": "Cosenza-Muralles",
                "given_name": "B.",
                "orcid": "0000-0002-4626-2757",
                "clpid": "Cosenza-Muralles-Ana-Beatriz"
            },
            {
                "family_name": "DeMets",
                "given_name": "C.",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "M\u00e1rquez-Az\u00faa",
                "given_name": "B.",
                "clpid": "M\u00e1rquez-Az\u00faa-Bertha"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "orcid": "0000-0003-1683-0247",
                "clpid": "S\u00e1nchez-Zamora-Osvaldo"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Cabral-Cano",
                "given_name": "E.",
                "orcid": "0000-0002-9143-2401",
                "clpid": "Cabral-Cano-Enrique"
            },
            {
                "family_name": "McCaffrey",
                "given_name": "R.",
                "orcid": "0000-0002-1291-3494",
                "clpid": "McCaffrey-Robert"
            }
        ],
        "abstract": "Northeastward subduction of the oceanic Rivera and Cocos plates in western Mexico poses a poorly understood seismic hazard to the overlying areas of the North America plate. We estimate the magnitude and distribution of interseismic locking along the northern \u223c500\u00a0km of the Mexico subduction zone, with a series of elastic half-space inversions that optimize the fits to the velocities of 57 GPS stations in western Mexico. All velocities were corrected for the co-seismic, afterslip and viscoelastic rebound effects of the 1995 Colima\u2013Jalisco and 2003 Tecom\u00e1n earthquakes. We explore the robustness of interseismic locking estimates to a variety of mantle Maxwell times that are required for the viscoelastic corrections, to the maximum permitted depth for locking of the subduction interface and to the location assigned to the Rivera\u2013Cocos\u2013North America plate triple junction offshore from western Mexico. The best-fitting locking solutions are associated with a maximum locking depth of 40\u00a0km, a triple junction location \u223c50\u00a0km northwest of the Manzanillo Trough and a mantle Maxwell time of 15\u00a0yr (viscosity of 2 \u00d7 10\u00b9\u2079 Pa s). Checkerboard tests show that the locking distribution is best resolved at intermediate depths (10\u201340\u00a0km). All of our inversions define a gradual transition from strong locking (i.e. 70\u2013100 per cent) of most (70\u00a0per\u00a0cent) of the Rivera\u2013North America subduction interface to strong but less uniform locking below the Manzanillo Trough, where oceanic lithosphere transitional between the Cocos and Rivera plate subducts, to weak to moderate locking (averaging 55 per cent) of the Michoac\u00e1n segment of the Cocos\u2013North America interface. Strong locking of the \u223c125-km-long trench segment offshore from Puerto Vallarta and other developed coastal areas, where our modelling indicates an average annual elastic slip-rate deficit of \u223c20\u00a0mm yr\u207b\u00b9, implies that \u223c1.8\u00a0m of unrelieved plate slip has accrued since the segment last ruptured in 1932, sufficient for an M \u223c 8.0 earthquake.",
        "doi": "10.1093/gji/ggab436",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2022-03",
        "series_number": "3",
        "volume": "228",
        "issue": "3",
        "pages": "2174-2197"
    },
    {
        "id": "authors:94qx8-4f481",
        "collection": "authors",
        "collection_id": "94qx8-4f481",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220211-236563500",
        "type": "article",
        "title": "Stress transition from horizontal to vertical forces during subduction initiation",
        "author": [
            {
                "family_name": "Shuck",
                "given_name": "Brandon",
                "orcid": "0000-0003-2543-721X",
                "clpid": "Shuck-Brandon"
            },
            {
                "family_name": "Gulick",
                "given_name": "Sean P. S.",
                "orcid": "0000-0003-4740-9068",
                "clpid": "Gulick-Sean-P-S"
            },
            {
                "family_name": "Van Avendonk",
                "given_name": "Harm J. A.",
                "orcid": "0000-0002-8016-2653",
                "clpid": "Van-Avendonk-Harm-J-A"
            },
            {
                "family_name": "Gurnis",
                "given_name": "Michael",
                "orcid": "0000-0003-1704-597X",
                "clpid": "Gurnis-M"
            },
            {
                "family_name": "Sutherland",
                "given_name": "Rupert",
                "orcid": "0000-0001-7430-0055",
                "clpid": "Sutherland-Rupert"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hightower",
                "given_name": "Erin",
                "orcid": "0000-0002-4734-5159",
                "clpid": "Hightower-Erin-J"
            }
        ],
        "abstract": "Subduction zones are fundamental to plate tectonics, yet how they initiate remains enigmatic. Geodynamic models suggest that if horizontal forces dominate, the upper plate experiences compression and uplift followed by extension and subsidence, whereas vertically forced subduction involves only extension. Geologic evidence of past subduction initiation events has been interpreted in terms of these alternatives; however, it is unclear whether they are mutually exclusive or represent different stages of early subduction. Here, we present seismic images of the Puysegur plate boundary south of New Zealand that reveal space\u2013time relations of stress during subduction initiation. Our data show evidence for a stress transition (compression followed by extension) that spread from north to south as the trench nucleated and propagated along the plate boundary. Both the magnitude and duration of compression diminish from north (8\u2009Myr) to south (5\u2009Myr). This indicates that transition to self-sustaining subduction accelerates after nucleation of a downgoing slab increases driving forces and decreases fault strength near the propagating tipline of the nascent trench. Instead of horizontally forced versus vertically forced initiation, we propose a four-dimensional evolution, where horizontal forces initially dominate at the site of nucleation, but with time, vertical forces accelerate, propagate along strike and facilitate the development of self-sustaining subduction.",
        "doi": "10.1038/s41561-021-00880-4",
        "issn": "1752-0894",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Geoscience",
        "publication_date": "2022-02",
        "series_number": "2",
        "volume": "15",
        "issue": "2",
        "pages": "149-155"
    },
    {
        "id": "authors:vdsqt-v9h15",
        "collection": "authors",
        "collection_id": "vdsqt-v9h15",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20220203-136695400",
        "type": "article",
        "title": "Microcontinent Breakup and Links to Possible Plate Boundary Reorganization in the Northern Gulf of California, M\u00e9xico",
        "author": [
            {
                "family_name": "Higa",
                "given_name": "Justin T.",
                "orcid": "0000-0001-8688-9645",
                "clpid": "Higa-Justin-T"
            },
            {
                "family_name": "Brown",
                "given_name": "Nathan D.",
                "orcid": "0000-0002-7385-8679",
                "clpid": "Brown-Nathan-D"
            },
            {
                "family_name": "Moon",
                "given_name": "Seulgi",
                "orcid": "0000-0001-5207-1781",
                "clpid": "Moon-Seulgi"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Sabbeth",
                "given_name": "Leah",
                "orcid": "0000-0001-6615-7949",
                "clpid": "Sabbeth-Leah"
            },
            {
                "family_name": "Bennett",
                "given_name": "Scott E. K.",
                "orcid": "0000-0002-9772-4122",
                "clpid": "Bennett-Scott-E-K"
            },
            {
                "family_name": "Mart\u00edn-Barajas",
                "given_name": "Arturo",
                "orcid": "0000-0003-0338-8154",
                "clpid": "Mart\u00edn-Barajas-Arturo"
            },
            {
                "family_name": "Argueta",
                "given_name": "Marina O.",
                "orcid": "0000-0002-3403-2620",
                "clpid": "Argueta-Marina-O"
            }
        ],
        "abstract": "Faults on microcontinents record the dynamic evolution of plate boundaries. However, most microcontinents are submarine and difficult to study. Here, we show that the southern part of the Isla \u00c1ngel de la Guarda (IAG) microcontinent, in the northern Gulf of California rift, is densely faulted by a late Quaternary-active normal fault zone. To characterize the onshore kinematics of this Almeja fault zone, we integrated remote fault mapping using high-resolution satellite- and drone-based topography with neotectonic field-mapping. We produced 13 luminescence ages from sediment deposits offset or impounded by faults to constrain the timing of fault offsets. We found that north-striking normal faults in the Almeja fault zone continue offshore to the south and likely into the nascent North Salsipuedes basin southwest of IAG. Late Pleistocene and Holocene luminescence ages indicate that the most recent onshore fault activity occurred in the last \u223c50 kyr. These observations suggest that the North Salsipuedes basin is kinematically linked with and continues onshore as the active Almeja fault zone. We suggest that fragmentation of the evolving IAG microcontinent may not yet be complete and that the Pacific-North America plate boundary is either not fully localized onto the Ballenas transform fault and Lower Delfin pull-apart basin or is in the initial stage of a plate boundary reorganization.",
        "doi": "10.1029/2021tc006933",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "2022-01",
        "series_number": "1",
        "volume": "41",
        "issue": "1",
        "pages": "Art. No. e2021TC006933"
    },
    {
        "id": "authors:9ykp1-ps351",
        "collection": "authors",
        "collection_id": "9ykp1-ps351",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201022-104923841",
        "type": "article",
        "title": "Moho Depth of Northern Baja California, Mexico, From Teleseismic Receiver Functions",
        "author": [
            {
                "family_name": "Ramirez",
                "given_name": "E. E.",
                "orcid": "0000-0002-8515-1128",
                "clpid": "Ramirez-Erik-E"
            },
            {
                "family_name": "Bataille",
                "given_name": "Klaus",
                "orcid": "0000-0001-6006-6747",
                "clpid": "Bataille-Klaus-D"
            },
            {
                "family_name": "Vidal-Villegas",
                "given_name": "J. A.",
                "orcid": "0000-0002-5845-8829",
                "clpid": "Vidal-Villegas-J-Antonio"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Ram\u00edrez-Hern\u00e1ndez",
                "given_name": "J.",
                "orcid": "0000-0001-5427-1752",
                "clpid": "Ram\u00edrez-Hern\u00e1ndez-Jorge"
            }
        ],
        "abstract": "We estimated Moho depths from data recorded by permanent and temporary broadband seismic stations deployed in northern Baja California, Mexico, using the receiver function technique. This region is composed of two subregions of contrasting geological and topographical characteristics: the Peninsular Ranges of Baja California (PRBC), a batholith with high elevations (up to 2,600 m); and the Mexicali Valley (MV) region, a sedimentary environment close to sea level. Crustal thickness derived from the P-to-S converted phases at 29 seismic stations were analyzed in three profiles: Two that cross the two subregions, in \u223cW-E direction, and the third one that runs over the PRBC in a N-S direction. For the PRBC, Moho depths vary from 35 to 45 km, from 33\u00b0N to 32\u00b0N; and from 30 to 46 km depth from 32\u00b0N to 30.5\u00b0N. From a profile that crosses the subregions in the W-E direction; Moho depths vary from 45 to \u223c34 km under western and eastern PRBC, respectively; with an abrupt change of depth under the Main Gulf Escarpment (30\u00b0), from \u223c32 to 30 km; and depths of 17\u201320 km under the MV. Moho depths of the profile in an \u223c W-E direction at \u223c31.5\u00b0N are from \u223c30 to 40 km, under topography that increases from 0 to 2,600 m; and became shallower (16 km depth) as the profile reaches the Gulf of California. These results show that deeper Moho is related to higher elevations with an abrupt change under the Main Gulf Escarpment, except for western PRBC where the Moho depth is not simply reflecting isostatic compensation.",
        "doi": "10.1029/2020EA001463",
        "issn": "2333-5084",
        "publisher": "American Geophysical Union",
        "publication": "Earth and Space Science",
        "publication_date": "2021-06",
        "series_number": "6",
        "volume": "8",
        "issue": "6",
        "pages": "Art. No. e2020EA001463"
    },
    {
        "id": "authors:abev1-jz859",
        "collection": "authors",
        "collection_id": "abev1-jz859",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201023-130721209",
        "type": "article",
        "title": "Strike-Slip Enables Subduction Initiation Beneath a Failed Rift: New Seismic Constraints From Puysegur Margin, New Zealand",
        "author": [
            {
                "family_name": "Shuck",
                "given_name": "Brandon",
                "orcid": "0000-0003-2543-721X",
                "clpid": "Shuck-Brandon"
            },
            {
                "family_name": "Van Avendonk",
                "given_name": "Harm",
                "orcid": "0000-0002-8016-2653",
                "clpid": "Van-Avendonk-Harm-J-A"
            },
            {
                "family_name": "Gulick",
                "given_name": "Sean P. S.",
                "orcid": "0000-0003-4740-9068",
                "clpid": "Gulick-Sean-P-S"
            },
            {
                "family_name": "Gurnis",
                "given_name": "Michael",
                "orcid": "0000-0003-1704-597X",
                "clpid": "Gurnis-M"
            },
            {
                "family_name": "Sutherland",
                "given_name": "Rupert",
                "orcid": "0000-0001-7430-0055",
                "clpid": "Sutherland-Rupert"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Patel",
                "given_name": "Jiten",
                "orcid": "0000-0001-6952-4708",
                "clpid": "Patel-Jiten"
            },
            {
                "family_name": "Hightower",
                "given_name": "Erin",
                "orcid": "0000-0002-4734-5159",
                "clpid": "Hightower-Erin-J"
            },
            {
                "family_name": "Saustrup",
                "given_name": "Steffen",
                "clpid": "Saustrup-Steffen"
            },
            {
                "family_name": "Hess",
                "given_name": "Thomas",
                "clpid": "Hess-Thomas"
            }
        ],
        "abstract": "Subduction initiation often takes advantage of previously weakened lithosphere and may preferentially nucleate along pre\u2010existing plate boundaries. To evaluate how past tectonic regimes and inherited lithospheric structure might lead to self\u2010sustaining subduction, we present an analysis of the Puysegur Trench, a young subduction zone with a rapidly evolving tectonic history. The Puysegur margin, south of New Zealand, has experienced a transformation from rifting to seafloor spreading to strike\u2010slip, and most recently to incipient subduction, all in the last \u223c45 million years. Here we present deep\u2010penetrating multichannel reflection and ocean\u2010bottom seismometer tomographic images to document crustal structures along the margin. Our images reveal that the overriding Pacific Plate beneath the Solander Basin contains stretched continental crust with magmatic intrusions, which formed from Eocene\u2010Oligocene rifting between the Campbell and Challenger plateaus. Rifting was more advanced to the south, yet never proceeded to breakup and seafloor spreading in the Solander Basin as previously thought. Subsequent strike\u2010slip deformation translated continental crust northward causing an oblique collisional zone, with trailing \u223c10 Myr old oceanic lithosphere. Incipient subduction transpired as oceanic lithosphere from the south forcibly underthrust the continent\u2010collision zone. We suggest that subduction initiation at the Puysegur Trench was assisted by inherited buoyancy contrasts and structural weaknesses that were imprinted into the lithosphere during earlier phases of continental rifting and strike\u2010slip along the plate boundary. The Puysegur margin demonstrates that forced nucleation along a strike\u2010slip boundary is a viable subduction initiation scenario and should be considered throughout Earth's history.",
        "doi": "10.1029/2020TC006436",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "2021-05",
        "series_number": "5",
        "volume": "40",
        "issue": "5",
        "pages": "Art. No. e2020TC006436"
    },
    {
        "id": "authors:vqdtd-2mh27",
        "collection": "authors",
        "collection_id": "vqdtd-2mh27",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20210413-121133507",
        "type": "article",
        "title": "Cenozoic continental rifting in the north-western Ross Sea",
        "author": [
            {
                "family_name": "Davey",
                "given_name": "Fred J.",
                "orcid": "0000-0003-1294-5290",
                "clpid": "Davey-Fred-J"
            },
            {
                "family_name": "Cande",
                "given_name": "Stephen",
                "clpid": "Cande-Stephen"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Marine gravity and seismic data are used to derive a preliminary crustal model for the Central Basin of the northern Ross Sea. The model is consistent with the presence of a thick (8\u2005km) ocean crust. Existing geophysical data indicates the rift forming the Central Basin continues, with offsets, into the Central Trough further south. Using limited existing data on the age (61\u201353\u2005Ma), and the amount and direction of extension of the Central rift system, an estimate is made of the pole of rotation for 61\u201353\u2005Ma (79\u00b0S, 170\u00b0W and rotation 6\u00b0). This pole of rotation and those for 43\u201326\u2005Ma and 26\u201310\u2005Ma, previously derived, are used to reconstruct the northern Ross Sea margin prior to 61\u2005Ma. The reconstruction shows a close fit of the continental components.",
        "doi": "10.1080/00288306.2021.1891942",
        "issn": "0028-8306",
        "publisher": "Informa UK Limited",
        "publication": "New Zealand Journal of Geology and Geophysics",
        "publication_date": "2021-03-04",
        "series_number": "3",
        "volume": "65",
        "issue": "3",
        "pages": "389-396"
    },
    {
        "id": "authors:bs3mh-qjz96",
        "collection": "authors",
        "collection_id": "bs3mh-qjz96",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20200519-132017615",
        "type": "article",
        "title": "Stratigraphic architecture of Solander Basin records Southern Ocean currents and subduction initiation beneath southwest New Zealand",
        "author": [
            {
                "family_name": "Patel",
                "given_name": "Jiten",
                "orcid": "0000-0001-6952-4708",
                "clpid": "Patel-Jiten"
            },
            {
                "family_name": "Sutherland",
                "given_name": "Rupert",
                "orcid": "0000-0001-7430-0055",
                "clpid": "Sutherland-Rupert"
            },
            {
                "family_name": "Gurnis",
                "given_name": "Michael",
                "orcid": "0000-0003-1704-597X",
                "clpid": "Gurnis-M"
            },
            {
                "family_name": "Van Avendonk",
                "given_name": "Harm",
                "orcid": "0000-0002-8016-2653",
                "clpid": "Van-Avendonk-Harm-J-A"
            },
            {
                "family_name": "Gulick",
                "given_name": "Sean P. S.",
                "orcid": "0000-0003-4740-9068",
                "clpid": "Gulick-Sean-P-S"
            },
            {
                "family_name": "Shuck",
                "given_name": "Brandon",
                "orcid": "0000-0003-2543-721X",
                "clpid": "Shuck-Brandon"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hightower",
                "given_name": "Erin",
                "orcid": "0000-0002-4734-5159",
                "clpid": "Hightower-Erin-J"
            }
        ],
        "abstract": "Solander Basin is currently characterised by subduction initiation at the Pacific\u2010Australia plate boundary, where high biological productivity is found at the northern edge of the Antarctic Circumpolar Current. Sedimentary architecture results from tectonic influences on accommodation space, sediment supply, and ocean currents (via physiography); and climate influence on ocean currents and biological productivity. We present the first seismic\u2010stratigraphic analysis of Solander Basin based on high\u2010fold seismic\u2010reflection data (voyage MGL1803, SISIE). Solander Trough physiography formed by Eocene rifting, but basinal strata are mostly younger than ~17 Ma, when we infer Puysegur Ridge formed and sheltered Solander Basin from bottom currents, and mountain growth onshore increased sediment supply. Initial inversion on the Tauru Fault started at ~15 Ma, but reverse faulting from 12 to ~8 Ma on both the Tauru and Parara Faults was likely associated with reorganization and formation of the subduction thrust. The new seabed topography forced sediment pathways to become channelized at low points or antecedent gorges. Since 5 Ma, southern Puysegur Ridge and Fiordland mountains spread out towards the east and Solander Anticline grew in response to ongoing subduction and growth of a slab. Solander Basin had high sedimentation rates because: (1) it is sheltered from bottom currents by Puysegur Ridge; and (2) it has a mountainous land area that supplies sediment to its northern end. Sedimentary architecture is asymmetric due to the Subtropical Front, which moves pelagic and hemi\u2010pelagic sediment, including dilute parts of gravity flows, eastward and accretes contourites to the shelf south of Stewart Island. Levees, scours, drifts, and ridges of folded sediment characterize western Solander Basin, whereas hemi\u2010pelagic drape and secondary gravity flows are found east of the meandering axial Solander Channel. The high\u2010resolution record of climate and tectonics that Solander Basin contains may yield excellent sites for future scientific ocean drilling.",
        "doi": "10.1111/bre.12473",
        "issn": "0950-091X",
        "publisher": "Wiley",
        "publication": "Basin Research",
        "publication_date": "2021-02",
        "series_number": "1",
        "volume": "33",
        "issue": "1",
        "pages": "403-426"
    },
    {
        "id": "authors:dzgj9-y8y49",
        "collection": "authors",
        "collection_id": "dzgj9-y8y49",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201105-160425687",
        "type": "article",
        "title": "The Lavic Lake Fault: A Long-Term Cumulative Slip Analysis via Combined Field Work and Thermal Infrared Hyperspectral Airborne Remote Sensing",
        "author": [
            {
                "family_name": "Witkosky",
                "given_name": "Rebecca A.",
                "orcid": "0000-0001-8531-8779",
                "clpid": "Witkosky-Rebecca-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Tratt",
                "given_name": "David M.",
                "orcid": "0000-0002-3942-6848",
                "clpid": "Tratt-David-M"
            },
            {
                "family_name": "Buckland",
                "given_name": "Kerry N.",
                "clpid": "Buckland-Kerry-N"
            },
            {
                "family_name": "Adams",
                "given_name": "Paul M.",
                "clpid": "Adams-Paul-M"
            },
            {
                "family_name": "Johnson",
                "given_name": "Patrick D.",
                "clpid": "Johnson-Patrick-D"
            },
            {
                "family_name": "Lynch",
                "given_name": "David K.",
                "clpid": "Lynch-David-K"
            },
            {
                "family_name": "Sousa",
                "given_name": "Francis J.",
                "orcid": "0000-0003-1623-4023",
                "clpid": "Sousa-Francis-J"
            }
        ],
        "abstract": "The 1999 Hector Mine earthquake ruptured to the surface in eastern California, with &gt;5 m peak right-lateral slip on the Lavic Lake fault. The cumulative offset and geologic slip rate of this fault are not well defined, which inhibits tectonic reconstructions and risk assessment of the Eastern California Shear Zone (ECSZ). With thermal infrared hyperspectral airborne imagery, field data, and auxiliary information from legacy geologic maps, we created lithologic maps of the area using supervised and unsupervised classifications of the remote sensing imagery. We optimized a data processing sequence for supervised classifications, resulting in lithologic maps over a test area with an overall accuracy of 71 \u00b1 1% with respect to ground-truth geologic mapping. Using all of the data and maps, we identified offset bedrock features that yield piercing points along the main Lavic Lake fault and indicate a 1036 +27/\u221226 m net slip, with 1008 +14/\u221217 m horizontal and 241 +51/\u221247 m vertical components. For the contribution from distributed shear, modern off-fault deformation values from another study imply a larger horizontal slip component of 1276 +18/\u221222 m. Within the constraints, we estimate a geologic slip rate of &lt;4 mm/yr, which does not increase the sum geologic Mojave ECSZ rate to current geodetic values. Our result supports previous suggestions that transient tectonic activity in this area may be responsible for the discrepancy between long-term geologic and present-day geodetic rates.",
        "doi": "10.3390/rs12213586",
        "issn": "2072-4292",
        "publisher": "MDPI",
        "publication": "Remote Sensing",
        "publication_date": "2020-11-02",
        "series_number": "21",
        "volume": "12",
        "issue": "21",
        "pages": "Art. No. 3586"
    },
    {
        "id": "authors:54w0x-h7v34",
        "collection": "authors",
        "collection_id": "54w0x-h7v34",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201007-140342146",
        "type": "article",
        "title": "Continental Interior and Edge Breakup at Convergent Margins Induced by Subduction Direction Reversal: A Numerical Modeling Study Applied to the South China Sea Margin",
        "author": [
            {
                "family_name": "Li",
                "given_name": "Fucheng",
                "orcid": "0000-0001-7761-9133",
                "clpid": "Li-Fucheng"
            },
            {
                "family_name": "Sun",
                "given_name": "Zhen",
                "orcid": "0000-0002-2991-9999",
                "clpid": "Sun-Zhen"
            },
            {
                "family_name": "Yang",
                "given_name": "Hongfeng",
                "orcid": "0000-0002-5925-6487",
                "clpid": "Yang-Hongfeng"
            },
            {
                "family_name": "Lin",
                "given_name": "Jian",
                "orcid": "0000-0002-6831-2014",
                "clpid": "Lin-Jian"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Zhao",
                "given_name": "Zhongxian",
                "orcid": "0000-0002-5096-4743",
                "clpid": "Zhao-Zhongxian"
            },
            {
                "family_name": "Xu",
                "given_name": "Hehua",
                "clpid": "Xu-Hehua"
            },
            {
                "family_name": "Sun",
                "given_name": "Longtao",
                "clpid": "Sun-Longtao"
            }
        ],
        "abstract": "The dynamics of continental breakup at convergent margins has been described as the results of backarc opening caused by slab rollback or drag force induced by subduction direction reversal. Although the rollback hypothesis has been intensively studied, our understanding of the consequence of subduction direction reversal remains limited. Using thermo\u2010mechanical modeling based on constraints from the South China Sea (SCS) region, we investigate how subduction direction reversal controls the breakup of convergent margins. The numerical results show that two distinct breakup modes, namely, continental interior and edge breakup (\"edge\" refers to continent above the plate boundary interface), may develop depending on the \"maturity\" of the convergent margin and the age of the oceanic lithosphere. For a slab age of ~15 to ~45 Ma, increasing the duration of subduction promotes the continental interior breakup mode, where a large block of the continental material is separated from the overriding plate. In contrast, the continental edge breakup mode develops when the subduction is a short\u2010duration event, and in this mode, a wide zone of less continuous continental fragments and tearing of the subducted slab occur. These two modes are consistent with the interior (relic late Mesozoic arc) and edge (relic forearc) rifting characteristics in the western and eastern SCS margin, suggesting that variation in the northwest\u2010directed subduction duration of the Proto\u2010SCS might be a reason for the differential breakup locus along the strike of the SCS margin. Besides, a two\u2010segment trench associated with the northwest\u2010directed subduction is implied in the present\u2010day SCS region.",
        "doi": "10.1029/2020tc006409",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "2020-11",
        "series_number": "11",
        "volume": "39",
        "issue": "11",
        "pages": "Art. No. e2020TC006409"
    },
    {
        "id": "authors:1xf94-16f16",
        "collection": "authors",
        "collection_id": "1xf94-16f16",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20200210-081539156",
        "type": "article",
        "title": "Scales of Stress Heterogeneity Near Active Faults in the Santa Barbara Channel, Southern California",
        "author": [
            {
                "family_name": "Persaud",
                "given_name": "Patricia",
                "orcid": "0000-0003-3462-7023",
                "clpid": "Persaud-P"
            },
            {
                "family_name": "Pritchard",
                "given_name": "Edward H.",
                "clpid": "Pritchard-E-H"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The Santa Barbara Channel represents the offshore portion of the Ventura Basin in Southern California. Ongoing transpression related to a regional left step in the San Andreas Fault has led to the formation of E\u2010W trending en\u2010echelon fault systems that accommodate localized shortening across the basin. Recent studies have suggested that faults within the channel could be capable of a multisegment rupture and producing a M_w 7.7\u20138.1 tsunamigenic earthquake. However, dynamic rupture models producing these results do not account for stress heterogeneity. With only sparse information available on the stress field in this region, further borehole\u2010derived stress constraints are essential for obtaining a more comprehensive understanding of the hazards related to the complex fault systems. We used caliper logs from 19 wells obtained from industry to identify stress\u2010induced borehole breakouts beneath the Holly and Gail oil platforms in the channel. Our newly developed forward modeling technique provides constraints on the orientations and relative magnitudes of the three principal stresses. At Gail, we determine a reverse faulting stress regime (S_(Hmax) = 1.7; S_(hmin) = 1.6; SV = 1.0) and an S_(Hmax) azimuth of N45\u00b0E. Our results are consistent with local structures, which reflect deeper regional scale trends, and with similar studies onshore nearby. At Holly, an S_(Hmax) rotation from ~N36\u00b0W to ~N57\u00b0E occurs across ~100 m depth in a single well and differs from nearby results, indicating that short\u2010length scale (&lt;10 km laterally and &lt;1 km in depth) stress heterogeneity is associated with complex changes in fault geometry.",
        "doi": "10.1029/2019gc008744",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2020-01",
        "series_number": "1",
        "volume": "21",
        "issue": "1",
        "pages": "Art. No. e2019GC008744"
    },
    {
        "id": "authors:gwyw4-6f378",
        "collection": "authors",
        "collection_id": "gwyw4-6f378",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190909-093502804",
        "type": "article",
        "title": "Seismic characteristics and evolution of post-rift igneous complexes and hydrothermal vents in the Lingshui sag (Qiongdongnan basin), northwestern South China Sea",
        "author": [
            {
                "family_name": "Wang",
                "given_name": "Lijie",
                "clpid": "Wang-Lijie"
            },
            {
                "family_name": "Sun",
                "given_name": "Zhen",
                "clpid": "Sun-Zhen"
            },
            {
                "family_name": "Yang",
                "given_name": "Jinhai",
                "clpid": "Yang-Jinhai"
            },
            {
                "family_name": "Sun",
                "given_name": "Zhipeng",
                "clpid": "Sun-Zhipeng"
            },
            {
                "family_name": "Zhu",
                "given_name": "Jitian",
                "clpid": "Zhu-Jitian"
            },
            {
                "family_name": "Zhuo",
                "given_name": "Haiteng",
                "orcid": "0000-0001-7769-3296",
                "clpid": "Zhou-Haiteng"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The study of morphology, distribution, and characteristics of igneous complexes has great significance to the understanding of magma plumbing processes, geodynamics, and tectonic evolution of continental margins. Previous studies concentrated partly on the magma-rich rifted basins, where the lateral magma transport mainly affects the igneous complexes' connection and distribution. However, due to seismic wave shielding effects of the large shallow magmatic bodies, the underlying igneous complexes and their corresponding magma plumbing systems in the magma-poor rifted margins are still in debate. In this study, 2D/3D seismic data and well data are utilized to describe the morphology, architecture, and spatial-temporal distribution of igneous complexes in the Lingshui sag of the Qiongdongnan basin, northwestern South China Sea margin. The identified igneous complexes include 98 intrusive sills and feeder dykes beneath some of the isolated sills. Twenty-six cone-shaped mounds that overlie intruded sills through internal disturbed conduits were also described. Drilled well samples and seismic expressions suggest that these mounds are hydrothermal vents. A uniform Bottom Mounds Horizon of these vents suggests that they probably formed at the same time. Constrained by biostratigraphic data and sedimentation rate of underlying and overlying sedimentary layers, the magma emplacement was dated to the middle Miocene (ca. 14.6\u202fMa). Most of the hydrothermal vents are distributed along the F2 fault zone and have direct linkage with the underlying sills, while the large sill complexes that are connected with limited vents are mainly present above the hyperextended continental crust, where the crust thins to 6\u201310\u202fkm. The sills intruded into different layers, from the lower Oligocene to the lower Miocene and the emplaced depth of sills is 1.2\u20136.3\u202fkm, whether or not they feed any vents above. Unlike most of the large volume and laterally linked sills found in the magma-rich rifted margins, the scattered distribution of sills at different levels indicates that dykes probably play an important role in magma transport, which might coexist with numerous polygonal or small faults and interference reflections. This work highlights the critical role of basin structures in controlling the distribution of post-rift igneous complexes in magma-poor margins, including thinned continental crust, sedimentary thickness, and faults.",
        "doi": "10.1016/j.margeo.2019.106043",
        "issn": "0025-3227",
        "publisher": "Elsevier",
        "publication": "Marine Geology",
        "publication_date": "2019-12",
        "volume": "418",
        "pages": "Art. No. 106043"
    },
    {
        "id": "authors:1h41c-jj666",
        "collection": "authors",
        "collection_id": "1h41c-jj666",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20191017-132811087",
        "type": "article",
        "title": "Microstructures documenting Cenozoic extension processes in the northern continental margin of the South China Sea",
        "author": [
            {
                "family_name": "Sun",
                "given_name": "Liheng",
                "clpid": "Sun-Liheng"
            },
            {
                "family_name": "Sun",
                "given_name": "Zhen",
                "clpid": "Sun-Zhen"
            },
            {
                "family_name": "Huang",
                "given_name": "Xiaolong",
                "clpid": "Huang-Xiaolong"
            },
            {
                "family_name": "Jiang",
                "given_name": "Yingde",
                "clpid": "Jiang-Yingde"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann Miriam",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "In order to investigate the thinning process of the northern continental margin of the South China Sea, petrographic and microstructural analysis were carried out on 20 greenschistfacies mylonite samples, which were obtained from Site U1504 of IODP Expedition 367/368 in the Outer Margin High of the region. The mineral assemblage of the greenschist-facies mylonite is chlorite + epidotite + albite (Ab = 94.7\u201399.9) + quartz, which contains 10-30% gravel components. Microstructural analysis indicates that the greenschist-facies mylonite experienced two episodes of deformation:early ductile deformation followed by a later stage of brittle deformatio. Both episodes of deformation suggest an extensional environment. The extensive development of bulging recrystallization (BLG) of quartz, microscopic fractures and fine granulation of albite suggest that the temperature of ductile deformation is about 300-400\u00b0C, compatiable with a ductile shearing at shallow crust levels (~5-10 km). Petrographic features suggest that the greenschist-facies mylonite might originate from volcanic sedimentary rocks or sedimentary rocks affected by the intrusion of mafic magma. Combined with seismic interpretation, we propose that the greenschist-facies mylonite might be formed by crustal exhumation after thick Mesozoic sediments were denuded by a major extension.",
        "doi": "10.1080/00206814.2019.1669079",
        "issn": "0020-6814",
        "publisher": "Taylor & Francis",
        "publication": "International Geology Review",
        "publication_date": "2019-09-29",
        "series_number": "7-8",
        "volume": "62",
        "issue": "7-8",
        "pages": "1094-1107"
    },
    {
        "id": "authors:tnn0j-vja51",
        "collection": "authors",
        "collection_id": "tnn0j-vja51",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190613-105022288",
        "type": "article",
        "title": "Incipient subduction at the contact with stretched continental crust: The Puysegur Trench",
        "author": [
            {
                "family_name": "Gurnis",
                "given_name": "Michael",
                "orcid": "0000-0003-1704-597X",
                "clpid": "Gurnis-M"
            },
            {
                "family_name": "Van Avendonk",
                "given_name": "Harm",
                "orcid": "0000-0002-8016-2653",
                "clpid": "Van-Avendonk-Harm-J-A"
            },
            {
                "family_name": "Gulick",
                "given_name": "Sean P. S.",
                "orcid": "0000-0003-4740-9068",
                "clpid": "Gulick-Sean-P-S"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Sutherland",
                "given_name": "Rupert",
                "clpid": "Sutherland-Rupert"
            },
            {
                "family_name": "Hightower",
                "given_name": "Erin",
                "orcid": "0000-0002-4734-5159",
                "clpid": "Hightower-Erin-J"
            },
            {
                "family_name": "Shuck",
                "given_name": "Brandon",
                "orcid": "0000-0003-2543-721X",
                "clpid": "Shuck-Brandon"
            },
            {
                "family_name": "Patel",
                "given_name": "Jiten",
                "clpid": "Patel-Jiten"
            },
            {
                "family_name": "Williams",
                "given_name": "Ethan",
                "orcid": "0000-0002-7917-4104",
                "clpid": "Williams-Ethan-F"
            },
            {
                "family_name": "Kardell",
                "given_name": "Dominik",
                "clpid": "Kardell-Dominik"
            },
            {
                "family_name": "Herzig",
                "given_name": "Erich",
                "clpid": "Herzig-Erich"
            },
            {
                "family_name": "Idini",
                "given_name": "Benjamin",
                "orcid": "0000-0002-2697-3893",
                "clpid": "Idini-Benjamin"
            },
            {
                "family_name": "Graham",
                "given_name": "Kenny",
                "clpid": "Graham-Kenny"
            },
            {
                "family_name": "Estep",
                "given_name": "Justin",
                "orcid": "0000-0002-2004-4786",
                "clpid": "Estep-Justin"
            },
            {
                "family_name": "Carrington",
                "given_name": "Luke",
                "clpid": "Carrington-Luke"
            }
        ],
        "abstract": "A seismic Benioff zone and plate kinematics show Puysegur Trench south of New Zealand transitioning to subduction. Because the local structure and its influence on subduction initiation is poorly understood, we conducted a seismic survey with ocean bottom seismometers and multichannel seismic profiles. Our early results show that the overriding Pacific Plate beneath the Solander Basin is composed of block-faulted and thinned continental crust, and the inner trench wall of northern Puysegur Ridge is composed of folded and faulted sediment. The megathrust interface has been imaged and shows \u223c500 m of downgoing, undisturbed sediments. Combining plate kinematic history with seismic velocity-inferred density, we show that the density difference across the plate boundary changed as oblique strike-slip plate motion juxtaposed dense oceanic crust with thinned continental crust. The density difference rapidly increased 18 to 15 Ma, coincident with subduction initiation, suggesting that compositional differences have a large influence on subduction initiation.",
        "doi": "10.1016/j.epsl.2019.05.044",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "2019-08-15",
        "volume": "520",
        "pages": "212-219"
    },
    {
        "id": "authors:fcrye-ppr31",
        "collection": "authors",
        "collection_id": "fcrye-ppr31",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190313-105427114",
        "type": "article",
        "title": "A Crustal Velocity Model for the Peninsular Ranges of Baja California and Southwestern Laguna Salada, Mexico",
        "author": [
            {
                "family_name": "Ram\u00edrez Ramos",
                "given_name": "Erik Esteban",
                "clpid": "Ram\u00edrez-Ramos-E-E"
            },
            {
                "family_name": "Vidal-Villegas",
                "given_name": "Jos\u00e9 Antonio",
                "clpid": "Vidal-Villegas-J-A"
            },
            {
                "family_name": "Ram\u00edrez-Hern\u00e1ndez",
                "given_name": "Jorge",
                "clpid": "Ram\u00edrez-Hern\u00e1ndez-J"
            },
            {
                "family_name": "Gonz\u00e1lez-Fern\u00e1ndez",
                "given_name": "Antonio",
                "clpid": "Gonz\u00e1lez-Fern\u00e1ndez-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann Miriam",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "To see any change in seismic velocities that may be associated with an abrupt change in the regional geology (granitic rock in contact with sediments), we conducted a refraction seismic study in the Peninsular Ranges of Baja California, which is in the Mexico\u2013southwestern Laguna Salada (LS) region. We installed 30 three\u2010component portable seismic stations, supplemented with two permanent six\u2010component stations of the Northwest Mexico Seismic Network (RESNOM). The stations, spaced \u223c6\u2009\u2009km along a refraction profile, recorded two blasts; these were the direct shot located to the south of the city of Ensenada and the reverse shot in the southwestern LS (southwest\u2013northeast direction). Record sections show seismograms with impulsive P arrivals at nearby stations. Rays from the two blasts were modeled (using asymptotic ray theory) to obtain a P\u2010wave velocity model from 0 to \u223c15\u2009\u2009km depth along the refraction profile. Our modeling results are as follows: in the southwestern part of the profile (0\u201325 km distance), a low\u2010velocity zone of \u223c2\u2009\u2009km/s exists between the depths of 0 and 3.5 km; in Sierra Ju\u00e1rez, the mean P\u2010wave velocity is \u223c5.6\u2009\u2009km/s between the depths of 0 and 5 km; and in southwestern LS, a low\u2010velocity layer of \u223c2.5\u2009\u2009km/s exists between the depths of 0 and \u223c3\u2009\u2009km. We also modeled a layer of \u223c6.5\u2009\u2009km/s between 4 and 12 km in the Ensenada\u2013Ojos Negros region, and between the depths of 4 and 8 km below the southwestern LS. From a profile distance of 0 to 50 km, a velocity zone of \u223c6.7\u2009\u2009km/s appears between the depths of 12 and 15 km.",
        "doi": "10.1785/0220180248",
        "issn": "0895-0695",
        "publisher": "Seismological Society of America",
        "publication": "Seismological Research Letters",
        "publication_date": "2019-05-01",
        "series_number": "3",
        "volume": "90",
        "issue": "3",
        "pages": "1219-1229"
    },
    {
        "id": "authors:1n2hw-t5398",
        "collection": "authors",
        "collection_id": "1n2hw-t5398",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20190412-073116409",
        "type": "article",
        "title": "Three-Dimensional Basin and Fault Structure From a Detailed Seismic Velocity Model of Coachella Valley, Southern California",
        "author": [
            {
                "family_name": "Ajala",
                "given_name": "Rasheed",
                "orcid": "0000-0001-5650-8362",
                "clpid": "Ajala-R"
            },
            {
                "family_name": "Persaud",
                "given_name": "Patricia",
                "orcid": "0000-0003-3462-7023",
                "clpid": "Persaud-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Fuis",
                "given_name": "Gary S.",
                "clpid": "Fuis-G-S"
            },
            {
                "family_name": "Hole",
                "given_name": "John A.",
                "orcid": "0000-0002-5349-9111",
                "clpid": "Hole-J-A"
            },
            {
                "family_name": "Goldman",
                "given_name": "Mark",
                "clpid": "Goldman-M"
            },
            {
                "family_name": "Scheirer",
                "given_name": "Daniel",
                "clpid": "Scheirer-D-S"
            }
        ],
        "abstract": "The Coachella Valley in the northern Salton Trough is known to produce destructive earthquakes, making it a high seismic hazard area. Knowledge of the seismic velocity structure and geometry of the sedimentary basins and fault zones is required to improve earthquake hazard estimates in this region. We simultaneously inverted first P wave travel times from the Southern California Seismic Network (39,998 local earthquakes) and explosions (251 land/sea shots) from the 2011 Salton Seismic Imaging Project to obtain a 3\u2010D seismic velocity model. Earthquakes with focal depths \u226410 km were selected to focus on the upper crustal structure. Strong lateral velocity contrasts in the top ~3 km correlate well with the surface geology, including the low\u2010velocity (&lt;5 km/s) sedimentary basin and the high\u2010velocity crystalline basement rocks outside the valley. Sediment thickness is ~4 km in the southeastern valley near the Salton Sea and decreases to &lt;2 km at the northwestern end of the valley. Eastward thickening of sediments toward the San Andreas fault within the valley defines Coachella Valley basin asymmetry. In the Peninsular Ranges, zones of relatively high seismic velocities (~6.4 km/s) between 2\u2010 and 4\u2010km depth may be related to Late Cretaceous mylonite rocks or older inherited basement structures. Other high\u2010velocity domains exist in the model down to 9\u2010km depth and help define crustal heterogeneity. We identify a potential fault zone in Lost Horse Valley unassociated with mapped faults in Southern California from the combined interpretation of surface geology, seismicity, and lateral velocity changes in the model.",
        "doi": "10.1029/2018JB016260",
        "issn": "2169-9313",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research. Solid Earth",
        "publication_date": "2019-05",
        "series_number": "5",
        "volume": "124",
        "issue": "5",
        "pages": "4728-4750"
    },
    {
        "id": "authors:3by6n-ph356",
        "collection": "authors",
        "collection_id": "3by6n-ph356",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20180627-101506778",
        "type": "article",
        "title": "Rapid transition from continental breakup to igneous oceanic crust in the South China Sea",
        "author": [
            {
                "family_name": "Larsen",
                "given_name": "H. C.",
                "clpid": "Larsen-H-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hinojosa",
                "given_name": "J.",
                "orcid": "0000-0002-8589-102X",
                "clpid": "Hinojosa-J-L"
            }
        ],
        "abstract": "Continental breakup represents the successful process of rifting and thinning of the continental lithosphere, leading to plate rupture and initiation of oceanic crust formation. Magmatism during breakup seems to follow a path of either excessive, transient magmatism (magma-rich margins) or of igneous starvation (magma-poor margins). The latter type is characterized by extreme continental lithospheric extension and mantle exhumation prior to igneous oceanic crust formation. Discovery of magma-poor margins has raised fundamental questions about the onset of ocean-floor type magmatism, and has guided interpretation of seismic data across many rifted margins, including the highly extended northern South China Sea margin. Here we report International Ocean Discovery Program drilling data from the northern South China Sea margin, testing the magma-poor margin model outside the North Atlantic. Contrary to expectations, results show initiation of Mid-Ocean Ridge basalt type magmatism during breakup, with a narrow and rapid transition into igneous oceanic crust. Coring and seismic data suggest that fast lithospheric extension without mantle exhumation generated a margin structure between the two endmembers. Asthenospheric upwelling yielding Mid-Ocean Ridge basalt-type magmatism from normal-temperature mantle during final breakup is interpreted to reflect rapid rifting within thin pre-rift lithosphere.",
        "doi": "10.1038/s41561-018-0198-1",
        "issn": "1752-0894",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Geoscience",
        "publication_date": "2018-10",
        "series_number": "10",
        "volume": "11",
        "issue": "10",
        "pages": "782-789"
    },
    {
        "id": "authors:wb5pg-ear41",
        "collection": "authors",
        "collection_id": "wb5pg-ear41",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170222-145907573",
        "type": "article",
        "title": "Active tectonics in the Gulf of California and seismicity (M > 3.0) for the period 2002\u20132014",
        "author": [
            {
                "family_name": "Castro",
                "given_name": "R. R.",
                "clpid": "Castro-R-R"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hauksson",
                "given_name": "E.",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Clayton",
                "given_name": "R. W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            }
        ],
        "abstract": "We present a catalog of accurate epicenter coordinates of earthquakes located in the Gulf of California (GoC) in the period 2002\u20132014 that permits us to analyze the seismotectonics and to estimate the depth of the seismogenic zone of this region. For the period April 2002 to December 2014 we use body-wave arrival times from regional stations of the Broadband Seismological Network of the GoC (RESBAN) operated by CICESE to improve hypocenter locations reported by global catalogs. For the northern region of the GoC (30\u00b0N\u201332\u00b0N) we added relocated events from the 2011-Hauksson-Yang-Shearer, Waveform Relocated Earthquake Catalog for Southern California (Hauksson et al., 2012; Lin et al., 2007). From October 2005 to October 2006 we incorporated hypcenters located by Sumy et al. (2013) in the southern GoC combining an array of ocean-bottom seismographs, of the SCOOBA experiment, with onshore stations of the NARS-Baja array. This well constrained catalog of seismicity highlights zones of active tectonics and seismic deformation within the North America-Pacific plate boundary. We estimate that the minimum magnitude of completeness of this catalog is Mc = 3.3 \u00b1 0.1 and the b = 0.92 \u00b1 0.04 value of the Gutenberg-Richter relation. We find that most earthquakes in the southern GoC are generated by transform faults and this region is more active than the central GoC region. However, the northern region, where most deformation is generated by oblique faults is as active as the southern region. We used the ISC catalog to evaluate the size distribution of seismicity of these regions, and the b value of the Gutenberg-Richter relation and found that b is slightly lower in the central GoC (b = 0.86 \u00b1 0.02) compared to the northern (b = 1.14 \u00b1 0.04) and the southern (b = 1.11 \u00b1 0.04) regions. We observed seismicity that occurs in the Stable Central Peninsular Province, despite the fact that significant active deformation has not been identified in this region.",
        "doi": "10.1016/j.tecto.2017.02.015",
        "issn": "0040-1951",
        "publisher": "Elsevier",
        "publication": "Tectonophysics",
        "publication_date": "2017-11-13",
        "volume": "719-720",
        "pages": "4-16"
    },
    {
        "id": "authors:3sac1-rae05",
        "collection": "authors",
        "collection_id": "3sac1-rae05",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170705-073528849",
        "type": "article",
        "title": "Subsurface Geometry of the San Andreas Fault in Southern California: Results from the Salton Seismic Imaging Project (SSIP) and Strong Ground Motion Expectations",
        "author": [
            {
                "family_name": "Fuis",
                "given_name": "Gary S.",
                "clpid": "Fuis-G-S"
            },
            {
                "family_name": "Bauer",
                "given_name": "Klaus",
                "clpid": "Bauer-K"
            },
            {
                "family_name": "Goldman",
                "given_name": "Mark R.",
                "clpid": "Goldman-M-R"
            },
            {
                "family_name": "Ryberg",
                "given_name": "Trond",
                "clpid": "Ryberg-T"
            },
            {
                "family_name": "Langenheim",
                "given_name": "Victoria E.",
                "clpid": "Langenheim-V-E"
            },
            {
                "family_name": "Scheirer",
                "given_name": "Daniel S.",
                "clpid": "Scheirer-D-S"
            },
            {
                "family_name": "Rymer",
                "given_name": "Michael J.",
                "clpid": "Rymer-M-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hole",
                "given_name": "John A.",
                "orcid": "0000-0002-5349-9111",
                "clpid": "Hole-J-A"
            },
            {
                "family_name": "Catchings",
                "given_name": "Rufus D.",
                "clpid": "Catchings-R-D"
            },
            {
                "family_name": "Graves",
                "given_name": "Robert W.",
                "clpid": "Graves-R-W"
            },
            {
                "family_name": "Aagaard",
                "given_name": "Brad",
                "clpid": "Aagaard-B-T"
            }
        ],
        "abstract": "The San Andreas fault (SAF) is one of the most studied strike\u2010slip faults in the world; yet its subsurface geometry is still uncertain in most locations. The Salton Seismic Imaging Project (SSIP) was undertaken to image the structure surrounding the SAF and also its subsurface geometry. We present SSIP studies at two locations in the Coachella Valley of the northern Salton trough. On our line 4, a fault\u2010crossing profile just north of the Salton Sea, sedimentary basin depth reaches 4 km southwest of the SAF. On our line 6, a fault\u2010crossing profile at the north end of the Coachella Valley, sedimentary basin depth is \u223c2\u20133\u2009\u2009km and centered on the central, most active trace of the SAF. Subsurface geometry of the SAF and nearby faults along these two lines is determined using a new method of seismic\u2010reflection imaging, combined with potential\u2010field studies and earthquakes. Below a 6\u20139 km depth range, the SAF dips \u223c50\u00b0\u201360\u00b0 NE, and above this depth range it dips more steeply. Nearby faults are also imaged in the upper 10 km, many of which dip steeply and project to mapped surface fault traces. These secondary faults may join the SAF at depths below about 10 km to form a flower\u2010like structure. In Appendix D, we show that rupture on a northeast\u2010dipping SAF, using a single plane that approximates the two dips seen in our study, produces shaking that differs from shaking calculated for the Great California ShakeOut, for which the southern SAF was modeled as vertical in most places: shorter\u2010period (T&lt;1\u2009\u2009s) shaking is increased locally by up to a factor of 2 on the hanging wall and is decreased locally by up to a factor of 2 on the footwall, compared to shaking calculated for a vertical fault.",
        "doi": "10.1785/0120160309",
        "issn": "0037-1106",
        "publisher": "Seismological Society of America",
        "publication": "Bulletin of the Seismological Society of America",
        "publication_date": "2017-08",
        "series_number": "4",
        "volume": "107",
        "issue": "4",
        "pages": "1642-1662"
    },
    {
        "id": "authors:3ptje-xec95",
        "collection": "authors",
        "collection_id": "3ptje-xec95",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170720-074723751",
        "type": "article",
        "title": "Observations of remotely triggered seismicity in Salton Sea and Coso geothermal regions, Southern California, USA, after big (M_W>7.8) teleseismic earthquakes",
        "author": [
            {
                "family_name": "Castro",
                "given_name": "Ra\u00fal R.",
                "clpid": "Castro-R-R"
            },
            {
                "family_name": "Clayton",
                "given_name": "Robert",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            },
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "A relocated catalog was used to search for changes in seismicity rate in the Salton Sea and the Coso geothermal regions, southern California, USA, during and after large (M_W&gt;7.8) teleseismic earthquakes. Seismicity in these two regions was analyzed within 30- day windows before and after the occurrence of five major earthquakes: the 2002 Denali fault, Alaska (M_W 7.9); the 2004 Sumatra-Andaman (M_W 9.2); the 2010 Central Chile (M_W 8.8); the 2011 Tohoku-Oki, Japan (M_W 9.1); and the 2012 Offshore Northern Sumatra (M_W 8.6) earthquakes. \n\nThe Denali (M_W 7.9) earthquake coincided with an increase in seismicity in the Salton Sea region the day when this remote event occurred, indicating that instantaneous triggered seismicity was likely related with the passage of its surface waves. However, in the Coso region the seismicity rate remained approximately constant during the 30-day observation period. The seismicity after the 2004 Sumatra-Andaman (M_W 9.2) earthquake increased in both regions 9 days after the mega-earthquake. The seismicity after the 2010 Chile (M_W 8.8) earthquake increased in both regions approximately 14 days after the remote event. The seismicity in Salton Sea and Coso regions increased 17 and 14 days, respectively, after the 2011 Japan (M_W 9.1) earthquake, suggesting that delayed triggered seismicity was induced after the passage of the surface waves in both regions. Similarly, 6 and 16 days after the 2012 northern Sumatra (M_W 8.6) earthquake the seismicity also increased in Salton Sea and Coso regions, respectively. These observations can be interpreted as evidence of instantaneous and delayed dynamic triggering induced by large remote earthquakes. The maximum magnitude of the delayed triggered swarm increased with the strength (M_0/D) of the mega-earthquake and, the stronger the remote earthquake, the longer the delay time.",
        "issn": "0016-7169",
        "publisher": "Union Fisica Mexicana",
        "publication": "Geofisica Internacional",
        "publication_date": "2017-07",
        "series_number": "3",
        "volume": "56",
        "issue": "3",
        "pages": "269-286"
    },
    {
        "id": "authors:y62qc-5ch85",
        "collection": "authors",
        "collection_id": "y62qc-5ch85",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20161109-071414936",
        "type": "article",
        "title": "Source Functions and Path Effects from Earthquakes in the Farallon Transform Fault Region, Gulf of California, Mexico that Occurred on October 2013",
        "author": [
            {
                "family_name": "Castro",
                "given_name": "Ra\u00fal R.",
                "clpid": "Castro-R-R"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Clayton",
                "given_name": "Robert W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            }
        ],
        "abstract": "We determined source spectral functions, Q and site effects using regional records of body waves from the October 19, 2013 (M_w = 6.6) earthquake and eight aftershocks located 90 km east of Loreto, Baja California Sur, Mexico. We also analyzed records from a foreshock with magnitude 3.3 that occurred 47 days before the mainshock. The epicenters of this sequence are located in the south-central region of the Gulf of California (GoC) near and on the Farallon transform fault. This is one of the most active regions of the GoC, where most of the large earthquakes have strike\u2013slip mechanisms. Based on the distribution of the aftershocks, the rupture propagated northwest with a rupture length of approximately 27 km. We calculated 3-component P- and S-wave spectra from ten events recorded by eleven stations of the Broadband Seismological Network of the GoC (RESBAN). These stations are located around the GoC and provide good azimuthal coverage (the average station gap is 39\u00b0). The spectral records were corrected for site effects, which were estimated calculating average spectral ratios between horizontal and vertical components (HVSR method). The site-corrected spectra were then inverted to determine the source functions and to estimate the attenuation quality factor Q. The values of Q resulting from the spectral inversion can be approximated by the relations Q_P =48.1\u00b11.1f^(0.88\u00b10.04)  and Q_S =135.4\u00b11.1f^(0.58\u00b10.03) and are consistent with previous estimates reported by Vidales-Basurto et al. (Bull Seism Soc Am 104:2027\u20132042, 2014) for the south-central GoC. The stress drop estimates, obtained using the \u03c92 model, are below 1.7 MPa, with the highest stress drops determined for the mainshock and the aftershocks located in the ridge zone. We used the values of Q obtained to recalculate source and site effects with a different spectral inversion scheme. We found that sites with low S-wave amplification also tend to have low P-wave amplification, except for stations BAHB, GUYB and SFQB, located on igneous rocks, where the P-wave site amplification is higher.",
        "doi": "10.1007/s00024-016-1346-4",
        "issn": "0033-4553",
        "publisher": "Springer",
        "publication": "Pure and Applied Geophysics",
        "publication_date": "2017-06",
        "series_number": "6",
        "volume": "174",
        "issue": "6",
        "pages": "2239-2256"
    },
    {
        "id": "authors:nt1ej-4hn92",
        "collection": "authors",
        "collection_id": "nt1ej-4hn92",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170223-074555793",
        "type": "article",
        "title": "Seismic imaging of the metamorphism of young sediment into new crystalline crust in the actively rifting Imperial Valley, California",
        "author": [
            {
                "family_name": "Han",
                "given_name": "Liang",
                "clpid": "Han-Liang"
            },
            {
                "family_name": "Hole",
                "given_name": "John A.",
                "orcid": "0000-0002-5349-9111",
                "clpid": "Hole-J-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Fuis",
                "given_name": "Gary S.",
                "clpid": "Fuis-G-S"
            },
            {
                "family_name": "Williams",
                "given_name": "Colin F.",
                "clpid": "Williams-C-F"
            },
            {
                "family_name": "Delph",
                "given_name": "Jonathan R.",
                "clpid": "Delph-J-R"
            },
            {
                "family_name": "Davenport",
                "given_name": "Kathy K.",
                "clpid": "Davenport-K-K"
            },
            {
                "family_name": "Livers",
                "given_name": "Amanda J.",
                "clpid": "Livers-A-J"
            }
        ],
        "abstract": "Plate-boundary rifting between transform faults is opening the Imperial Valley of southern California and the rift is rapidly filling with sediment from the Colorado River. Three 65\u201390 km long seismic refraction profiles across and along the valley, acquired as part of the 2011 Salton Seismic Imaging Project, were analyzed to constrain upper crustal structure and the transition from sediment to underlying crystalline rock. Both first arrival travel-time tomography and frequency-domain full-waveform inversion were applied to provide P-wave velocity models down to \u223c7 km depth. The valley margins are fault-bounded, beyond which thinner sediment has been deposited on preexisting crystalline rocks. Within the central basin, seismic velocity increases continuously from \u223c1.8 km/s sediment at the surface to &gt;6 km/s crystalline rock with no sharp discontinuity. Borehole data show young sediment is progressively metamorphosed into crystalline rock. The seismic velocity gradient with depth decreases approximately at the 4 km/s contour, which coincides with changes in the porosity and density gradient in borehole core samples. This change occurs at \u223c3 km depth in most of the valley, but at only \u223c1.5 km depth in the Salton Sea geothermal field. We interpret progressive metamorphism caused by high heat flow to be creating new crystalline crust throughout the valley at a rate comparable to the \u22652 km/Myr sedimentation rate. The newly formed crystalline crust extends to at least 7\u20138 km depth, and it is shallower and faster where heat flow is higher. Most of the active seismicity occurs within this new crust.",
        "doi": "10.1002/2016GC006610",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2016-11",
        "series_number": "11",
        "volume": "17",
        "issue": "11",
        "pages": "4566-4584"
    },
    {
        "id": "authors:nd2rw-qvd59",
        "collection": "authors",
        "collection_id": "nd2rw-qvd59",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20161222-100807138",
        "type": "article",
        "title": "Continental rupture and the creation of new crust in the Salton Trough rift, Southern California and northern Mexico: Results from the Salton Seismic Imaging Project",
        "author": [
            {
                "family_name": "Han",
                "given_name": "Liang",
                "clpid": "Han-Liang"
            },
            {
                "family_name": "Hole",
                "given_name": "John A.",
                "orcid": "0000-0002-5349-9111",
                "clpid": "Hole-J-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Fuis",
                "given_name": "Gary S.",
                "clpid": "Fuis-G-S"
            },
            {
                "family_name": "Kell",
                "given_name": "Annie",
                "clpid": "Kell-A"
            },
            {
                "family_name": "Driscoll",
                "given_name": "Neal W.",
                "clpid": "Driscoll-N-W"
            },
            {
                "family_name": "Kent",
                "given_name": "Graham M.",
                "clpid": "Kent-G-M"
            },
            {
                "family_name": "Harding",
                "given_name": "Alistair J.",
                "clpid": "Harding-A-J"
            },
            {
                "family_name": "Rymer",
                "given_name": "Michael J.",
                "clpid": "Rymer-M-J"
            },
            {
                "family_name": "Gonz\u00e1lez-Fern\u00e1ndez",
                "given_name": "Antonio",
                "clpid": "Gonz\u00e1lez-Fern\u00e1ndez-A"
            },
            {
                "family_name": "L\u00e1zaro-Mancilla",
                "given_name": "Octavio",
                "clpid": "L\u00e1zaro-Mancilla-O"
            }
        ],
        "abstract": "A refraction and wide-angle reflection seismic profile along the axis of the Salton Trough, California and Mexico, was analyzed to constrain crustal and upper mantle seismic velocity structure during active continental rifting. From the northern Salton Sea to the southern Imperial Valley, the crust is 17\u201318\u2009km thick and approximately one-dimensional. The transition at depth from Colorado River sediment to underlying crystalline rock is gradual and is not a depositional surface. The crystalline rock from ~3 to ~8\u2009km depth is interpreted as sediment metamorphosed by high heat flow. Deeper felsic crystalline rock could be stretched preexisting crust or higher-grade metamorphosed sediment. The lower crust below ~12\u2009km depth is interpreted to be gabbro emplaced by rift-related magmatic intrusion by underplating. Low upper mantle velocity indicates high temperature and partial melting. Under the Coachella Valley, sediment thins to the north and the underlying crystalline rock is interpreted as granitic basement. Mafic rock does not exist at 12\u201318\u2009km depth as it does to the south, and a weak reflection suggests Moho at ~28\u2009km depth. Structure in adjacent Mexico has slower midcrustal velocity, and rocks with mantle velocity must be much deeper than in the Imperial Valley. Slower velocity and thicker crust in the Coachella and Mexicali valleys define the rift zone between them to be &gt;100\u2009km wide in the direction of plate motion. North American lithosphere in the central Salton Trough has been rifted apart and is being replaced by new crust created by magmatism, sedimentation, and metamorphism.",
        "doi": "10.1002/2016JB013139",
        "issn": "2169-9313",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research. Solid Earth",
        "publication_date": "2016-10",
        "series_number": "10",
        "volume": "121",
        "issue": "10",
        "pages": "7469-7489"
    },
    {
        "id": "authors:9a2nt-1hr32",
        "collection": "authors",
        "collection_id": "9a2nt-1hr32",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20160726-090423974",
        "type": "article",
        "title": "Fault zone characteristics and basin complexity in the southern Salton Trough, California",
        "author": [
            {
                "family_name": "Persaud",
                "given_name": "Patricia",
                "orcid": "0000-0003-3462-7023",
                "clpid": "Persaud-P"
            },
            {
                "family_name": "Ma",
                "given_name": "Yiran",
                "orcid": "0000-0002-8369-3310",
                "clpid": "Ma-Yiran"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hole",
                "given_name": "John A.",
                "orcid": "0000-0002-5349-9111",
                "clpid": "Hole-J-A"
            },
            {
                "family_name": "Fuis",
                "given_name": "Gary S.",
                "clpid": "Fuis-G-S"
            },
            {
                "family_name": "Han",
                "given_name": "Liang",
                "clpid": "Han-Liang"
            }
        ],
        "abstract": "Ongoing oblique slip at the Pacific\u2013North America plate boundary in the Salton Trough produced the Imperial Valley (California, USA), a seismically active area with deformation distributed across a complex network of exposed and buried faults. To better understand the shallow crustal structure in this region and the connectivity of faults and seismicity lineaments, we used data primarily from the Salton Seismic Imaging Project to construct a three-dimensional P-wave velocity model down to 8 km depth and a velocity profile to 15 km depth, both at 1 km grid spacing. A V_P = 5.65\u20135.85 km/s layer of possibly metamorphosed sediments within, and crystalline basement outside, the valley is locally as thick as 5 km, but is thickest and deepest in fault zones and near seismicity lineaments, suggesting a causative relationship between the low velocities and faulting. Both seismicity lineaments and surface faults control the structural architecture of the western part of the larger wedge-shaped basin, where two deep subbasins are located. We estimate basement depths, and show that high velocities at shallow depths and possible basement highs characterize the geothermal areas.",
        "doi": "10.1130/G38033.1",
        "issn": "0091-7613",
        "publisher": "Geological Society of America",
        "publication": "Geology",
        "publication_date": "2016-09",
        "series_number": "9",
        "volume": "44",
        "issue": "9",
        "pages": "747-750"
    },
    {
        "id": "authors:k5w0d-3y741",
        "collection": "authors",
        "collection_id": "k5w0d-3y741",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20160720-154304105",
        "type": "article",
        "title": "Focal mechanisms and size distribution of earthquakes beneath the Krafla central volcano, NE Iceland",
        "author": [
            {
                "family_name": "Schuler",
                "given_name": "Juerg",
                "clpid": "Schuler-J"
            },
            {
                "family_name": "Pugh",
                "given_name": "David J.",
                "clpid": "Pugh-D-J"
            },
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "White",
                "given_name": "Robert S.",
                "clpid": "White-R-S"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Brandsd\u00f3ttir",
                "given_name": "Brynd\u00eds",
                "clpid": "Brandsd\u00f3ttir-B"
            }
        ],
        "abstract": "Seismicity was monitored beneath the Krafla central volcano, NE Iceland, between 2009 and 2012 during a period of volcanic quiescence, when most earthquakes occured within the shallow geothermal field. The highest concentration of earthquakes is located close to the rock-melt transition zone as the IDDP-1 wellbore suggests, and decays quickly at greater depths. We recorded multiple swarms of microearthquakes, which coincide often with periods of changes in geothermal field operations, and found that about one third of the total number of earthquakes are repeating events. The event size distribution, evaluated within the central caldera, indicates average crustal values with b = 0.79 \u00b1 0.04. No significant spatial b-value contrasts are resolved within the geothermal field nor in the vicinity of the drilled melt. Besides the seismicity analysis, focal mechanisms are calculated for 342 events. Most of these short-period events have source radiation patterns consistent with double-couple (DC) mechanisms. A few events are attributed to non-shear faulting mechanisms with geothermal fluids likely playing an important role in their source processes. Diverse faulting styles are inferred from DC events, but normal faulting prevails in the central caldera. The best-fitting compressional and tensional axes of DC mechanisms are interpreted in terms of the principal stress or deformation-rate orientations across the plate boundary rift. Maximum compressive stress directions are near-vertically aligned in different study volumes, as expected in an extensional tectonic setting. Beneath the natural geothermal fields, the least compressive stress axis is found to align with the regional spreading direction. In the main geothermal field both horizontal stresses appear to have similar magnitudes causing a diversity of focal mechanisms.",
        "doi": "10.1002/2016JB013213",
        "issn": "2169-9313",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research. Solid Earth",
        "publication_date": "2016-07",
        "series_number": "7",
        "volume": "121",
        "issue": "7",
        "pages": "5152-5168"
    },
    {
        "id": "authors:h2dby-zqc30",
        "collection": "authors",
        "collection_id": "h2dby-zqc30",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20160915-090411864",
        "type": "article",
        "title": "Synchronous oceanic spreading and continental rifting in West Antarctica",
        "author": [
            {
                "family_name": "Davey",
                "given_name": "F. J.",
                "clpid": "Davey-F-J"
            },
            {
                "family_name": "Granot",
                "given_name": "R.",
                "clpid": "Granot-R"
            },
            {
                "family_name": "Cande",
                "given_name": "S. C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Selvans",
                "given_name": "M.",
                "clpid": "Selvans-M-M"
            },
            {
                "family_name": "Ferraccioli",
                "given_name": "F.",
                "clpid": "Ferraccioli-F"
            }
        ],
        "abstract": "Magnetic anomalies associated with new ocean crust formation in the Adare Basin off north-western Ross Sea (43\u201326\u2009Ma) can be traced directly into the Northern Basin that underlies the adjacent morphological continental shelf, implying a continuity in the emplacement of oceanic crust. Steep gravity gradients along the margins of the Northern Basin, particularly in the east, suggest that little extension and thinning of continental crust occurred before it ruptured and the new oceanic crust formed, unlike most other continental rifts and the Victoria Land Basin further south. A preexisting weak crust and localization of strain by strike-slip faulting are proposed as the factors allowing the rapid rupture of continental crust.",
        "doi": "10.1002/2016GL069087",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "2016-06-28",
        "series_number": "12",
        "volume": "43",
        "issue": "12",
        "pages": "6162-6169"
    },
    {
        "id": "authors:zn4v2-fe443",
        "collection": "authors",
        "collection_id": "zn4v2-fe443",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20160119-093854474",
        "type": "article",
        "title": "Seismic imaging of the shallow crust beneath the Krafla central volcano, NE Iceland",
        "author": [
            {
                "family_name": "Schuler",
                "given_name": "Juerg",
                "clpid": "Schuler-J"
            },
            {
                "family_name": "Greenfield",
                "given_name": "Tim",
                "clpid": "Greenfield-T"
            },
            {
                "family_name": "White",
                "given_name": "Robert S.",
                "clpid": "White-R-S"
            },
            {
                "family_name": "Roecker",
                "given_name": "Steven W.",
                "clpid": "Roecker-S-W"
            },
            {
                "family_name": "Brandsd\u00f3ttir",
                "given_name": "Brynd\u00eds",
                "clpid": "Brandsd\u00f3ttir-B"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Tarasewicz",
                "given_name": "Jon",
                "clpid": "Tarasewicz-J"
            },
            {
                "family_name": "Martens",
                "given_name": "Hilary R.",
                "orcid": "0000-0003-2860-9013",
                "clpid": "Martens-H-R"
            },
            {
                "family_name": "Pugh",
                "given_name": "David",
                "clpid": "Pugh-D"
            }
        ],
        "abstract": "We studied the seismic velocity structure beneath the Krafla central volcano, NE Iceland, by performing 3-D tomographic inversions of 1453 earthquakes recorded by a temporary local seismic network between 2009 and 2012. The seismicity is concentrated primarily around the Leirhnj\u00fakur geothermal field near the center of the Krafla caldera. To obtain robust velocity models, we incorporated active seismic data from previous surveys. The Krafla central volcano has a relatively complex velocity structure with higher P wave velocities (V_p) underneath regions of higher topographic relief and two distinct low-V_p anomalies beneath the Leirhnj\u00fakur geothermal field. The latter match well with two attenuating bodies inferred from S wave shadows during the Krafla rifting episode of 1974\u20131985. Within the Leirhnj\u00fakur geothermalreservoir, we resolved a shallow (\u22120.5 to 0.5 km below sea level; bsl) region with low-V_p/V_s values and a deeper (0.5\u20131.5 km bsl) high-V_p/V_s zone. We interpret the difference in the velocity ratios of the two zones to be caused by higher rock porosities and crack densities in the shallow region and lower porosities and crack densities in the deeper region. A strong low-V_p/V_s anomaly underlies these zones, where a superheated steam zone within felsic rock overlies rhyolitic melt.",
        "doi": "10.1002/2015JB012350",
        "issn": "2169-9313",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research. Solid Earth",
        "publication_date": "2015-10",
        "series_number": "10",
        "volume": "120",
        "issue": "10",
        "pages": "7156-7173"
    },
    {
        "id": "authors:97cr7-vre81",
        "collection": "authors",
        "collection_id": "97cr7-vre81",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20150430-094007973",
        "type": "article",
        "title": "Fault\u2010Slip Distribution of the 1999 M_w 7.1 Hector Mine Earthquake, California, Estimated from Postearthquake Airborne LiDAR Data",
        "author": [
            {
                "family_name": "Chen",
                "given_name": "T.",
                "clpid": "Chen-Tao"
            },
            {
                "family_name": "Akciz",
                "given_name": "S. O.",
                "clpid": "Akciz-Sinan-O"
            },
            {
                "family_name": "Hudnut",
                "given_name": "K. W.",
                "orcid": "0000-0002-3168-4797",
                "clpid": "Hudnut-K-W"
            },
            {
                "family_name": "Zhang",
                "given_name": "D. Z.",
                "clpid": "Zhang-D-Z"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The 16 October 1999 Hector Mine earthquake (M_w 7.1) was the first large earthquake for which postearthquake airborne Light Detection and Ranging (LiDAR) data were collected to image the fault surface rupture. In this work, we present measurements of both vertical and horizontal slip along the entire surface rupture of this earthquake based on airborne LiDAR data acquired in April 2000. We examine the details of the along\u2010fault slip distribution of this earthquake based on 255 horizontal and 85 vertical displacements using a 0.5 m digital elevation model derived from the LiDAR imagery. The slip measurements based on the LiDAR dataset are highest in the epicentral region, and taper in both directions, consistent with earlier findings by other works. The maximum dextral displacement measured from LiDAR imagery is 6.60\u00b11.10\u2009\u2009m, located about 700 m south of the highest field measurement (5.25\u00b10.85\u2009\u2009m). Our results also illustrate the difficulty in resolving displacements smaller than 1 m using LiDAR imagery alone. We analyze slip variation to see if it is affected by rock type and whether variations are statistically significant. This study demonstrates that a postearthquake airborne LiDAR survey can produce an along\u2010fault horizontal and vertical offset distribution plot of a quality comparable to a reconnaissance field survey. Although LiDAR data can provide a higher sampling density and enable rapid data analysis for documenting slip distributions, we find that, relative to field methods, it has a limited ability to resolve slip that is distributed over several fault strands across a zone. We recommend a combined approach that merges field observation with LiDAR analysis, so that the best attributes of both quantitative topographic and geological insight are utilized in concert to make best estimates of offsets and their uncertainties.",
        "doi": "10.1785/0120130108",
        "issn": "0037-1106",
        "publisher": "Seismological Society of America",
        "publication": "Bulletin of the Seismological Society of America",
        "publication_date": "2015-04",
        "series_number": "2A",
        "volume": "105",
        "issue": "2A",
        "pages": "776-790"
    },
    {
        "id": "authors:9kp4h-qrc22",
        "collection": "authors",
        "collection_id": "9kp4h-qrc22",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20150219-100201807",
        "type": "article",
        "title": "A Crustal Velocity Model for the Southern Mexicali Valley, Baja California, Mexico",
        "author": [
            {
                "family_name": "Ram\u00edrez-Ramos",
                "given_name": "Erik E.",
                "clpid": "Ram\u00edrez-Ramos-E-E"
            },
            {
                "family_name": "Vidal-Villegas",
                "given_name": "Antonio",
                "clpid": "Vidal-Villegas-A"
            },
            {
                "family_name": "Gonz\u00e1lez-Fern\u00e1ndez",
                "given_name": "Antonio",
                "clpid": "Gonz\u00e1lez-Fern\u00e1ndez-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "In northern Baja California, the two largest regions with different geological characteristics are the granitic Peninsular Ranges of Baja California (PRBC) and the sedimentary environment of the Mexicali Valley (Lomnitz et al., 1970). The boundary of these two regions is the Main Gulf Escarpment (Fig. 1). The northern Baja California peninsula has active normal and strike\u2010slip faults originating from the transtensional limit between the Pacific and North America plates (Stock et al., 1991).",
        "doi": "10.1785/0220140007",
        "issn": "0895-0695",
        "publisher": "Seismological Society of America",
        "publication": "Seismological Research Letters",
        "publication_date": "2015-01",
        "series_number": "1",
        "volume": "86",
        "issue": "1",
        "pages": "181-191"
    },
    {
        "id": "authors:qmzxx-d2n74",
        "collection": "authors",
        "collection_id": "qmzxx-d2n74",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140926-090020854",
        "type": "article",
        "title": "Deep crustal structure of the Adare and Northern Basins, Ross Sea, Antarctica, from sonobuoy data",
        "author": [
            {
                "family_name": "Selvans",
                "given_name": "M. M.",
                "clpid": "Selvans-M-M"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Clayton",
                "given_name": "R. W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            },
            {
                "family_name": "Cande",
                "given_name": "S.",
                "clpid": "Cande-S"
            },
            {
                "family_name": "Granot",
                "given_name": "R.",
                "clpid": "Granot-R"
            }
        ],
        "abstract": "Extension associated with ultraslow seafloor spreading within the Adare Basin, in oceanic crust just north of the continental shelf in the Ross Sea, Antarctica, extended south into the Northern Basin. Magnetic and gravity anomaly data suggest continuity of crustal structure across the continental shelf break that separates the Adare and Northern Basins. We use sonobuoy refraction data and multi-channel seismic (MCS) reflection data collected during research cruise NBP0701, including 71 new sonobuoy records, to provide constraints on crustal structure in the Adare and Northern Basins. Adjacent 1D sonobuoy profiles along several MCS lines reveal deep crustal structure in the vicinity of the continental shelf break, and agree with additional sonobuoy data that document fast crustal velocities (6000\u20138000 m/s) at shallow depths (1\u20136 km below sea level) from the Adare Basin to the continental shelf, a structure consistent with that of other ultraslow-spread crust. Our determination of crustal structure in the Northern Basin only extends through sedimentary rock to the basement rock, and so cannot help to distinguish between different hypotheses for formation of the basin.",
        "doi": "10.1016/j.epsl.2014.08.029",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "2014-11-01",
        "volume": "405",
        "pages": "220-230"
    },
    {
        "id": "authors:q1mnd-03c05",
        "collection": "authors",
        "collection_id": "q1mnd-03c05",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140904-090345033",
        "type": "article",
        "title": "Assembly of a large earthquake from a complex fault system: Surface rupture kinematics of the 4 April 2010 El Mayor\u2013Cucapah (Mexico) M_w 7.2 earthquake",
        "author": [
            {
                "family_name": "Fletcher",
                "given_name": "John M.",
                "clpid": "Fletcher-J-M"
            },
            {
                "family_name": "Teran",
                "given_name": "Orlando J.",
                "clpid": "Teran-O-J"
            },
            {
                "family_name": "Rockwell",
                "given_name": "Thomas K.",
                "clpid": "Rockwell-T-K"
            },
            {
                "family_name": "Oskin",
                "given_name": "Michael",
                "orcid": "0000-0002-6631-5326",
                "clpid": "Oskin-M-E"
            },
            {
                "family_name": "Hudnut",
                "given_name": "Kenneth W.",
                "orcid": "0000-0002-3168-4797",
                "clpid": "Hudnut-K-W"
            },
            {
                "family_name": "Mueller",
                "given_name": "Karl J.",
                "clpid": "Mueller-K-J"
            },
            {
                "family_name": "Spelz",
                "given_name": "Ronald M.",
                "clpid": "Spelz-R-M"
            },
            {
                "family_name": "Akciz",
                "given_name": "Sinan O.",
                "clpid": "Akciz-S-O"
            },
            {
                "family_name": "Masana",
                "given_name": "Eulalia",
                "clpid": "Masana-E"
            },
            {
                "family_name": "Faneros",
                "given_name": "Geoff",
                "clpid": "Faneros-G"
            },
            {
                "family_name": "Fielding",
                "given_name": "Eric J.",
                "orcid": "0000-0002-6648-8067",
                "clpid": "Fielding-E-J"
            },
            {
                "family_name": "Leprince",
                "given_name": "S\u00e9bastien",
                "orcid": "0000-0003-4555-8975",
                "clpid": "Leprince-S"
            },
            {
                "family_name": "Morelan",
                "given_name": "Alexander E.",
                "clpid": "Morelan-A-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Lynch",
                "given_name": "David K.",
                "clpid": "Lynch-D-K"
            },
            {
                "family_name": "Elliott",
                "given_name": "Austin J.",
                "clpid": "Elliott-A-J"
            },
            {
                "family_name": "Gold",
                "given_name": "Peter",
                "clpid": "Gold-Peter"
            },
            {
                "family_name": "Liu-Zeng",
                "given_name": "Jing",
                "clpid": "Liu-Zeng-Jing"
            },
            {
                "family_name": "Gonz\u00e1lez-Ortega",
                "given_name": "Alejandro",
                "clpid": "Gonz\u00e1lez-Ortega-A"
            },
            {
                "family_name": "Hinojosa-Corona",
                "given_name": "Alejandro",
                "clpid": "Hinojosa-Corona-A"
            },
            {
                "family_name": "Gonz\u00e1lez-Garc\u00eda",
                "given_name": "Javier",
                "clpid": "Gonz\u00e1lez-Garc\u00eda-J"
            }
        ],
        "abstract": "The 4 April 2010 moment magnitude (M_w) 7.2 El Mayor\u2013Cucapah earthquake revealed the existence of a previously unidentified fault system in Mexico that extends \u223c120 km from the northern tip of the Gulf of California to the U.S.\u2013Mexico border. The system strikes northwest and is composed of at least seven major faults linked by numerous smaller faults, making this one of the most complex surface ruptures ever documented along the Pacific\u2013North America plate boundary. Rupture propagated bilaterally through three distinct kinematic and geomorphic domains. Southeast of the epicenter, a broad region of distributed fracturing, liquefaction, and discontinuous fault rupture was controlled by a buried, southwest-dipping, dextral-normal fault system that extends \u223c53 km across the southern Colorado River delta. Northwest of the epicenter, the sense of vertical slip reverses as rupture propagated through multiple strands of an imbricate stack of east-dipping dextral-normal faults that extend \u223c55 km through the Sierra Cucapah. However, some coseismic slip (10\u201330 cm) was partitioned onto the west-dipping Laguna Salada fault, which extends parallel to the main rupture and defines the western margin of the Sierra Cucapah. In the northernmost domain, rupture terminates on a series of several north-northeast\u2013striking cross-faults with minor offset (&lt;8 cm) that cut uplifted and folded sediments of the northern Colorado River delta in the Yuha Desert.\n\nIn the Sierra Cucapah, primary rupture occurred on four major faults separated by one fault branch and two accommodation zones. The accommodation zones are distributed in a left-stepping en echelon geometry, such that rupture passed systematically to structurally lower faults. The structurally lowest fault that ruptured in this event is inclined as shallowly as \u223c20\u00b0. Net surface offsets in the Sierra Cucapah average \u223c200 cm, with some reaching 300\u2013400 cm, and rupture kinematics vary greatly along strike. Nonetheless, instantaneous extension directions are consistently oriented \u223c085\u00b0 and the dominant slip direction is \u223c310\u00b0, which is slightly (\u223c10\u00b0) more westerly than the expected azimuth of relative plate motion, but considerably more oblique to other nearby historical ruptures such as the 1992 Landers earthquake. Complex multifault ruptures are common in the central portion of the Pacific North American plate margin, which is affected by restraining bend tectonics, gravitational potential energy gradients, and the inherently three-dimensional strain of the transtensional and transpressional shear regimes that operate in this region.",
        "doi": "10.1130/GES00933.1",
        "issn": "1553-040X",
        "publisher": "Geological Society of America",
        "publication": "Geosphere",
        "publication_date": "2014-08",
        "series_number": "4",
        "volume": "10",
        "issue": "4",
        "pages": "797-827"
    },
    {
        "id": "authors:x40qg-b4592",
        "collection": "authors",
        "collection_id": "x40qg-b4592",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140626-084743314",
        "type": "article",
        "title": "Community infrastructure and repository for marine magnetic identifications",
        "author": [
            {
                "family_name": "Seton",
                "given_name": "Maria",
                "orcid": "0000-0001-8541-1367",
                "clpid": "Seton-Maria"
            },
            {
                "family_name": "Whittaker",
                "given_name": "Joanne M.",
                "clpid": "Whittaker-oanne-M"
            },
            {
                "family_name": "Wessel",
                "given_name": "Paul",
                "clpid": "Wessel-Paul"
            },
            {
                "family_name": "M\u00fcller",
                "given_name": "R. Dietmar",
                "orcid": "0000-0002-3334-5764",
                "clpid": "M\u00fcller-R-Dietmar"
            },
            {
                "family_name": "DeMets",
                "given_name": "Charles",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "Merkouriev",
                "given_name": "Sergey",
                "clpid": "Merkouriev-Sergey"
            },
            {
                "family_name": "Cande",
                "given_name": "Steve",
                "clpid": "Cande-Steve-C"
            },
            {
                "family_name": "Gaina",
                "given_name": "Carmen",
                "clpid": "Gaina-Carmen"
            },
            {
                "family_name": "Eagles",
                "given_name": "Graeme",
                "clpid": "Eagles-Graeme"
            },
            {
                "family_name": "Granot",
                "given_name": "Roi",
                "clpid": "Granot-Roi"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Wright",
                "given_name": "Nicky",
                "clpid": "Wright-Nicky-M"
            },
            {
                "family_name": "Williams",
                "given_name": "Simon E.",
                "orcid": "0000-0003-4670-8883",
                "clpid": "Williams-Simon-E"
            }
        ],
        "abstract": "Magnetic anomaly identifications underpin plate tectonic reconstructions and form the primary data set from which the age of the oceanic lithosphere and seafloor spreading regimes in the ocean basins can be determined. Although these identifications are an invaluable resource, their usefulness to the wider scientific community has been limited due to the lack of a central community infrastructure to organize, host, and update these interpretations. We have developed an open-source, community-driven online infrastructure as a repository for quality-checked magnetic anomaly identifications from all ocean basins. We provide a global sample data set that comprises 96,733 individually picked magnetic anomaly\nidentifications organized by ocean basin and publication reference, and provide accompanying Hellingerformat\nfiles, where available. Our infrastructure is designed to facilitate research in plate tectonic reconstructions or research that relies on an assessment of plate reconstructions, for both experts and nonexperts alike. To further enhance the existing repository and strengthen its value, we encourage others in the community to contribute to this effort.",
        "doi": "10.1002/2013GC005176",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2014-04",
        "series_number": "4",
        "volume": "15",
        "issue": "4",
        "pages": "1629-1641"
    },
    {
        "id": "authors:pe68v-c4f64",
        "collection": "authors",
        "collection_id": "pe68v-c4f64",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140403-094603730",
        "type": "article",
        "title": "Active Pacific North America Plate boundary tectonics as evidenced by seismicity in the oceanic lithosphere offshore Baja California, Mexico",
        "author": [
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Kanamori",
                "given_name": "Hiroo",
                "orcid": "0000-0001-8219-9428",
                "clpid": "Kanamori-H"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Cormier",
                "given_name": "Marie-Helene",
                "clpid": "Cormier-M-H"
            },
            {
                "family_name": "Legg",
                "given_name": "Mark",
                "clpid": "Legg-M"
            }
        ],
        "abstract": "Pacific Ocean crust west of southwest North America was formed by Cenozoic seafloor spreading between the large Pacific Plate and smaller microplates. The eastern limit of this seafloor, the continent\u2013ocean boundary, is the fossil trench along which the microplates subducted and were mostly destroyed in Miocene time. The Pacific\u2013North America Plate boundary motion today is concentrated on continental fault systems well to the east, and this region of oceanic crust is generally thought to be within the rigid Pacific Plate. Yet, the 2012 December 14 M_w 6.3 earthquake that occurred about 275\u2009km west of Ensenada, Baja California, Mexico, is evidence for continued tectonism in this oceanic part of the Pacific Plate. The preferred main shock centroid depth of 20\u2009km was located close to the bottom of the seismogenic thickness of the young oceanic lithosphere. The focal mechanism, derived from both teleseismic P-wave inversion and W-phase analysis of the main shock waveforms, and the 12 aftershocks of M \u223c3\u20134 are consistent with normal faulting on northeast striking nodal planes, which align with surface mapped extensional tectonic trends such as volcanic features in the region. Previous Global Positioning System (GPS) measurements on offshore islands in the California Continental Borderland had detected some distributed Pacific and North America relative plate motion strain that could extend into the epicentral region. The release of this lithospheric strain along existing zones of weakness is a more likely cause of this seismicity than current thermal contraction of the oceanic lithosphere or volcanism. The main shock caused weak to moderate ground shaking in the coastal zones of southern California, USA, and Baja California, Mexico, but the tsunami was negligible.",
        "doi": "10.1093/gji/ggt467",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2014-03",
        "series_number": "3",
        "volume": "196",
        "issue": "3",
        "pages": "1619-1630"
    },
    {
        "id": "authors:0zyrf-re018",
        "collection": "authors",
        "collection_id": "0zyrf-re018",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140613-081909428",
        "type": "article",
        "title": "The Ayyubid Orogen: An Ophiolite Obduction-Driven Orogen in the Late Cretaceous of the Neo-Tethyan South Margin",
        "author": [
            {
                "family_name": "\u015eeng\u00f6r",
                "given_name": "A. M. Cel\u00e2l",
                "clpid": "\u015eeng\u00f6r-A-M-C"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "A minimum 5000-km long obduction-driven orogeny of medial to late Cretaceous age is located between Cyrenaica in eastern Libya and Oman. It is herein called the Ayyubid Orogen after the Ayyubid Empire that covered much of its territory. The Ayyubid orogen is distinct from other Alpide orogens and has two main parts: a western, mainly germanotype belt and an eastern mainly alpinotype belt. The germanotype belt formed largely as a result of an aborted obduction, whereas the alpinotype part formed as a result of successful and large-scale obduction events that choked a nascent subduction zone. The mainly germanotype part coincides with Erich Krenkel's Syrian Arc (Syrischer Bogen) and the alpinotype part with Ricou's  Peri-Arabian Ophiolitic Crescent (Croissant Ophiolitique p\u00e9ri-Arabe). These belts formed as a consequence of the interaction of one of the now-vanished Tethyan plates and Afro-Arabia. The Africa-Eurasia relative motion has influenced the orogen's evolution, but was not the main causative agent. Similar large and complex obduction-driven orogens similar to the Ayyubids may exist along the Ordovician Newfoundland/Scotland margin of the Caledonides and along the Ordovician European margin of the Uralides.",
        "doi": "10.12789/geocanj.2014.41.042",
        "issn": "0315-0941",
        "publisher": "Geological Association of Canada",
        "publication": "Geoscience Canada",
        "publication_date": "2014",
        "volume": "41",
        "pages": "225-254"
    },
    {
        "id": "authors:e2pxz-g6m67",
        "collection": "authors",
        "collection_id": "e2pxz-g6m67",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20130412-114502163",
        "type": "article",
        "title": "Report on the August 2012 Brawley Earthquake Swarm in Imperial Valley, Southern California",
        "author": [
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Bilham",
                "given_name": "Roger",
                "clpid": "Bilham-R"
            },
            {
                "family_name": "Boese",
                "given_name": "Maren",
                "clpid": "Boese-M"
            },
            {
                "family_name": "Chen",
                "given_name": "Xiaowei",
                "clpid": "Chen-Xiaowei"
            },
            {
                "family_name": "Fielding",
                "given_name": "Eric J.",
                "orcid": "0000-0002-6648-8067",
                "clpid": "Fielding-E-J"
            },
            {
                "family_name": "Galetzka",
                "given_name": "John",
                "clpid": "Galetzka-J"
            },
            {
                "family_name": "Hudnut",
                "given_name": "Kenneth W.",
                "orcid": "0000-0002-3168-4797",
                "clpid": "Hudnut-K-W"
            },
            {
                "family_name": "Hutton",
                "given_name": "Kate",
                "clpid": "Hutton-K"
            },
            {
                "family_name": "Jones",
                "given_name": "Lucile M.",
                "orcid": "0000-0002-2690-3051",
                "clpid": "Jones-L-M"
            },
            {
                "family_name": "Kanamori",
                "given_name": "Hiroo",
                "orcid": "0000-0001-8219-9428",
                "clpid": "Kanamori-H"
            },
            {
                "family_name": "Shearer",
                "given_name": "Peter M.",
                "orcid": "0000-0002-2992-7630",
                "clpid": "Shearer-P-M"
            },
            {
                "family_name": "Steidl",
                "given_name": "Jamie",
                "clpid": "Steidl-J"
            },
            {
                "family_name": "Treiman",
                "given_name": "Jerry",
                "clpid": "Treiman-J"
            },
            {
                "family_name": "Wei",
                "given_name": "Shengji",
                "clpid": "Wei-Shengji"
            },
            {
                "family_name": "Yang",
                "given_name": "Wenzheng",
                "clpid": "Yang-Wenzheng"
            }
        ],
        "abstract": "The 2012 Brawley earthquake swarm occurred in the Brawley Seismic Zone (BSZ) within the Imperial Valley of southern California (Fig. 1). The BSZ is the northernmost extensional segment of the Pacific\u2013North America plate boundary system. Johnson and Hill (1982) used the distribution of seismicity since the 1930s to outline the geographical extent of the BSZ, defining boundaries of the BSZ as shown in Figure 1. Its north\u2013south extent ranges from the northern section of the Imperial fault, starting approximately 10 km north of the United States\u2013Mexico international border and connecting to the southern end of the San Andreas fault, where it terminates in the Salton Sea. Larsen and Reilinger (1991), who defined a similar geographical extent of the BSZ, argued that the BSZ was migrating to the northwest, which they associated with the propagation of the Gulf of California rift system into the North American continent. During the seismically active period of the 1970s, the BSZ produced close to half of the earthquakes recorded in California (Johnson and Hill, 1982; Hutton et al., 2010). However, for two decades following the 1979 Imperial Valley mainshock M_w 6.4 and its aftershock sequence, the BSZ was much less active. In general, the BSZ seismicity is indicative of right-lateral strike-slip plate motion accompanied by crustal thinning as well as possible associated fluid movements in the crust (Chen and Shearer, 2011). The 2012 Brawley swarm produced more than 600 events recorded by the United States Geological Survey (USGS)\u2013California Institute of Technology (Caltech) Southern California Seismic Network (SCSN). Other monitoring instruments in the region, such as the Global Positioning System (GPS) network, creepmeters, and the Wildlife Liquefaction Array (WLA) also recorded signals from the largest events. In addition, Interferometric Synthetic Aperture Radar (InSAR) satellites collected images from space.",
        "doi": "10.1785/0220120169",
        "issn": "0895-0695",
        "publisher": "Seismological Society of America",
        "publication": "Seismological Research Letters",
        "publication_date": "2013-03",
        "series_number": "2",
        "volume": "84",
        "issue": "2",
        "pages": "177-189"
    },
    {
        "id": "authors:wk99g-6mm49",
        "collection": "authors",
        "collection_id": "wk99g-6mm49",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20130516-133349919",
        "type": "article",
        "title": "Revised Eocene-Oligocene kinematics for the West Antarctic rift system",
        "author": [
            {
                "family_name": "Granot",
                "given_name": "R.",
                "clpid": "Granot-R"
            },
            {
                "family_name": "Cande",
                "given_name": "S. C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Damaske",
                "given_name": "D.",
                "clpid": "Damaske-D"
            }
        ],
        "abstract": "Past plate motion between East and West Antarctica along the West Antarctic rift system had important regional and global implications. Although extensively studied, the kinematics of the rift during Eocene-Oligocene time still remains elusive. Based on a recent detailed aeromagnetic survey from the Adare and Northern Basins, located in the northwestern Ross Sea, we present the first well-constrained kinematic model with four rotations for Anomalies 12o, 13o, 16y, and 18o (26.5\u201340.13\u2009Ma). These rotation poles form a cluster suggesting a stable sense of motion during that period of time. The poles are located close to the central part of the rift implying that the local motion varied from extension in the western Ross Sea sector (Adare Basin, Northern Basin, and Victoria Land Basin) to dextral transcurrent motion in the Ross Ice Shelf and to oblique convergence in the eastern end of the rift zone. The results confirm previous estimates of 95\u2009km of extension in the Victoria Land Basin.",
        "doi": "10.1029/2012GL054181",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "2013-01-28",
        "series_number": "2",
        "volume": "40",
        "issue": "2",
        "pages": "279-284"
    },
    {
        "id": "authors:j4ra2-jy780",
        "collection": "authors",
        "collection_id": "j4ra2-jy780",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20131220-135844497",
        "type": "article",
        "title": "Geochemistry of the extensive peralkaline pyroclastic flow deposit of NW Mexico, based on conventional and handheld X-ray fluorescence. Implications in a regional context",
        "author": [
            {
                "family_name": "Vidal-Solano",
                "given_name": "J. R.",
                "clpid": "Vidal-Solano-J-R"
            },
            {
                "family_name": "Lozano Santa Cruz",
                "given_name": "R.",
                "clpid": "Lozano-Santa-Cruz-R"
            },
            {
                "family_name": "Zamora",
                "given_name": "O.",
                "clpid": "Zamora-O"
            },
            {
                "family_name": "Mendoza-Cordova",
                "given_name": "A.",
                "clpid": "Mendoza-Cordova-A"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Chemical analyses conducted on the surface of rock slabs under a combination of two X-ray spectrometry methods, wavelength dispersive XRF and energy dispersive XRF, are used to establish a geochemical correlation between the studied samples. This proves to be an excellent method for the characterization of volcanic glasses, particularly when particles of exotic origin are present, because the effect of these is not easily eliminated by conventional whole rock analysis. Analyses of glassy rhyolites (ignimbrites and lava flows) in northwestern Mexico establish a geochemical signature for the samples, providing criteria that allow us to: a) correlate them with a peralkaline volcanic event, previously reported, that occurred during Middle Miocene time; b) distinguish them from other metaluminous varieties in the region and, c) propose a correlation between all the peralkaline vitrophyres that crop out within the studied area, of at least 50.000 km^2, validating the hypothesis that they are related to the same volcanic event. Finally, based on the results of this study and previous geological investigations, it is proposed that a distance of more than 100 km between the geographical location of the thickest peralkaline deposits in Sonora, is probably related to a displacement along transtensional dextral faults during the Late Miocene.",
        "doi": "10.5209/rev_JIGE.2013.v39.n1.41754",
        "issn": "1698-6180",
        "publisher": "Universidad Complutense de Madrid",
        "publication": "Journal of Iberian Geology",
        "publication_date": "2013",
        "series_number": "1",
        "volume": "39",
        "issue": "1",
        "pages": "121-130"
    },
    {
        "id": "authors:7xbda-vhc33",
        "collection": "authors",
        "collection_id": "7xbda-vhc33",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20131004-131249954",
        "type": "article",
        "title": "Petrograf\u00eda, geoqu\u00edmica, petrof\u00e1brica y paleomagnetismo de la Toba de San Felipe en la regi\u00f3n de Catavi\u00f1a, Baja California, M\u00e9xico",
        "author": [
            {
                "family_name": "Olgu\u00edn-Villa",
                "given_name": "Angel Enrique",
                "clpid": "Olgu\u00edn-Villa-A-E"
            },
            {
                "family_name": "Vidal-Solano",
                "given_name": "Jes\u00fas Roberto",
                "clpid": "Vidal-Solano-J-R"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann Miriam",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "A pyroclastic density current deposit has been recognized within the middle Miocene sequences\nin the Catavi\u00f1a region, Baja California. The rhyolitic deposit is a poorly welded ignimbrite and has\nreduced thicknesses (&lt;30 m), corresponding to distal facies from the source area. The mineral assemblage\nsanidine&gt;green clinopyroxene&gt;fayalite is analogous to that of all ignimbrite deposits of this nature in\nnorthwestern Mexico. Geochemical studies emphasize, first, the peralkaline character defining a comendite\nvariety for the rhyolitic magma, and second, that higher concentrations of Sr and Ba are distinctive features\nof the Catavi\u00f1a ignimbrite, which are related to the incorporation of xenocrysts during its emplacement.\nPaleomagnetic and geochemical studies correlate this deposit with the Tuff of San Felipe-Ignimbrite of\nHermosillo (TSF-IGH). These outcrops represent the westernmost remains of the TSF-IGH event in NW\nMexico and the southernmost outcrops in Baja California. The isopach map, petrofabric and magnetic\nfabric results of this work make possible a model for the TSF-IGH emplacement, which considers that\nthe pyroclastic flow came from Sonora invading the area from east to west.",
        "issn": "1026-8774",
        "publisher": "Universidad Nacional Aut\u00f3noma de M\u00e9xico",
        "publication": "Revista Mexicana de Ciencias Geol\u00f3gicas",
        "publication_date": "2013",
        "series_number": "2",
        "volume": "30",
        "issue": "2",
        "pages": "282-298"
    },
    {
        "id": "authors:2byfk-atb33",
        "collection": "authors",
        "collection_id": "2byfk-atb33",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20121130-081922437",
        "type": "article",
        "title": "The 2012 Sumatra great earthquake sequence",
        "author": [
            {
                "family_name": "Duputel",
                "given_name": "Zacharie",
                "clpid": "Duputel-Z"
            },
            {
                "family_name": "Kanamori",
                "given_name": "Hiroo",
                "orcid": "0000-0001-8219-9428",
                "clpid": "Kanamori-H"
            },
            {
                "family_name": "Tsai",
                "given_name": "Victor C.",
                "orcid": "0000-0003-1809-6672",
                "clpid": "Tsai-V-C"
            },
            {
                "family_name": "Rivera",
                "given_name": "Luis",
                "orcid": "0000-0002-0726-5445",
                "clpid": "Rivera-L"
            },
            {
                "family_name": "Meng",
                "given_name": "Lingsen",
                "orcid": "0000-0003-2428-0548",
                "clpid": "Meng-Lingsen"
            },
            {
                "family_name": "Ampuero",
                "given_name": "Jean-Paul",
                "orcid": "0000-0002-4827-7987",
                "clpid": "Ampuero-J-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The equatorial Indian Ocean is a well known place of active intraplate deformation defying the conventional view of rigid plates separated by narrow boundaries where deformation is confined. On 11 April 2012, this region was hit in a couple of hours by two of the largest strike-slip earthquakes ever recorded (moment magnitudes Mw=8.6 and 8.2). Broadband seismological observations of the Mw=8.6 mainshock indicate a large centroid depth (\u223c30 km) and remarkable rupture complexity. Detailed study of the surface-wave directivity and moment rate functions clearly indicates the partition of the rupture into at least two distinct subevents. To account for these observations, we developed a procedure to invert for multiple-point-source parameters. The optimum source model at long period consists of two point sources separated by about 209 km with magnitudes Mw=8.5 and 8.3. To explain the remaining discrepancies between predicted and observed surface waves, we can refine this model by adding directivity along the WNW\u2013ESE axis. However, we do not exclude more complicated models. To analyze the Mw=8.2 aftershock, we removed the perturbation due to large surface-wave arrivals of the Mw=8.6 mainshock by subtracting the corresponding synthetics computed for the two-subevent model. Analysis of the surface-wave amplitudes suggests that the Mw=8.2 aftershock had a large centroid depth between 30 km and 40 km. This major earthquake sequence brings a new perspective to the seismotectonics of the equatorial Indian Ocean and reveals active deep lithospheric deformation.",
        "doi": "10.1016/j.epsl.2012.07.017",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "2012-10-15",
        "volume": "351",
        "pages": "247-257"
    },
    {
        "id": "authors:t3504-94518",
        "collection": "authors",
        "collection_id": "t3504-94518",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20120816-082822417",
        "type": "article",
        "title": "Earthquake in a Maze: Compressional Rupture Branching During the 2012 M_w 8.6 Sumatra Earthquake",
        "author": [
            {
                "family_name": "Meng",
                "given_name": "L.",
                "orcid": "0000-0003-2428-0548",
                "clpid": "Meng-Lingsen"
            },
            {
                "family_name": "Ampuero",
                "given_name": "J.-P.",
                "orcid": "0000-0002-4827-7987",
                "clpid": "Ampuero-J-P"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Duputel",
                "given_name": "Z.",
                "clpid": "Duputel-Z"
            },
            {
                "family_name": "Luo",
                "given_name": "Y.",
                "orcid": "0000-0002-1165-6107",
                "clpid": "Luo-Yingdi"
            },
            {
                "family_name": "Tsai",
                "given_name": "V. C.",
                "orcid": "0000-0003-1809-6672",
                "clpid": "Tsai-V-C"
            }
        ],
        "abstract": "Seismological observations of the 2012 moment magnitude 8.6 Sumatra earthquake reveal unprecedented complexity of dynamic rupture. The surprisingly large magnitude results from the combination of deep extent, high stress drop, and rupture of multiple faults. Back-projection source imaging indicates that the rupture occurred on distinct planes in an orthogonal conjugate fault system, with relatively slow rupture speed. The east-southeast\u2013west-northwest ruptures add a new dimension to the seismotectonics of the Wharton Basin, which was previously thought to be controlled by north-south strike-slip faulting. The rupture turned twice into the compressive quadrant, against the preferred branching direction predicted by dynamic Coulomb stress calculations. Orthogonal faulting and compressional branching indicate that rupture was controlled by a pressure-insensitive strength of the deep oceanic lithosphere.",
        "doi": "10.1126/science.1224030",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "2012-08-10",
        "series_number": "6095",
        "volume": "337",
        "issue": "6095",
        "pages": "724-726"
    },
    {
        "id": "authors:3chsf-kfk37",
        "collection": "authors",
        "collection_id": "3chsf-kfk37",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20120412-132057738",
        "type": "article",
        "title": "Using overlapping sonobuoy data from the Ross Sea to construct a 2D deep crustal velocity model",
        "author": [
            {
                "family_name": "Selvans",
                "given_name": "M. M.",
                "clpid": "Selvans-M-M"
            },
            {
                "family_name": "Clayton",
                "given_name": "R. W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Granot",
                "given_name": "R.",
                "clpid": "Granot-R"
            }
        ],
        "abstract": "Sonobuoys provide an alternative to using long streamers while conducting multi-channel seismic (MCS) studies, in order to provide deeper velocity control. We present analysis and modeling techniques for interpreting the sonobuoy data and illustrate the method with ten overlapping sonobuoys collected in the Ross Sea, offshore from Antarctica. We demonstrate the importance of using the MCS data to correct for ocean currents and changes in ship navigation, which is required before using standard methods for obtaining a 1D velocity profile from each sonobuoy. We verify our 1D velocity models using acoustic finite-difference (FD) modeling and by performing depth migration on the data, and demonstrate the usefulness of FD modeling for tying interval velocities to the shallow crust imaged using MCS data. Finally, we show how overlapping sonobuoys along an MCS line can be used to construct a 2D velocity model of the crust. The velocity model reveals a thin crust (5.5 \u00b1 0.4 km) at the boundary between the Adare and Northern Basins, and implies that the crustal structure of the Northern Basin may be more similar to that of the oceanic crust in the Adare Basin than to the stretched continental crust further south in the Ross Sea.",
        "doi": "10.1007/s11001-011-9143-z",
        "issn": "0025-3235",
        "publisher": "Springer Verlag",
        "publication": "Marine Geophysical Research",
        "publication_date": "2012-03",
        "series_number": "1",
        "volume": "33",
        "issue": "1",
        "pages": "17-32"
    },
    {
        "id": "authors:tqtrt-jpv33",
        "collection": "authors",
        "collection_id": "tqtrt-jpv33",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110802-141212219",
        "type": "article",
        "title": "The 2010 M_w 7.2 El Mayor-Cucapah Earthquake Sequence, Baja California, Mexico and Southernmost California, USA: Active Seismotectonics along the Mexican Pacific Margin",
        "author": [
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hutton",
                "given_name": "Kate",
                "clpid": "Hutton-K"
            },
            {
                "family_name": "Yang",
                "given_name": "Wenzheng",
                "clpid": "Yang-Wenzheng"
            },
            {
                "family_name": "Vidal-Villegas",
                "given_name": "J. Antonio",
                "clpid": "Vidal-Villegas-J-A"
            },
            {
                "family_name": "Kanamori",
                "given_name": "Hiroo",
                "orcid": "0000-0001-8219-9428",
                "clpid": "Kanamori-H"
            }
        ],
        "abstract": "The El Mayor-Cucapah earthquake sequence started with a few foreshocks in March 2010, and a second sequence of 15 foreshocks of M &gt; 2 (up to M4.4) that occurred during the 24 h preceding the mainshock. The foreshocks occurred along a north\u2013south trend near the mainshock epicenter. The M_w 7.2 mainshock on April 4 exhibited complex faulting, possibly starting with a ~M6 normal faulting event, followed ~15 s later by the main event, which included simultaneous normal and right-lateral strike-slip faulting. The aftershock zone extends for 120 km from the south end of the Elsinore fault zone north of the US\u2013Mexico border almost to the northern tip of the Gulf of California. The waveform-relocated aftershocks form two abutting clusters, each about 50 km long, as well as a 10 km north\u2013south aftershock zone just north of the epicenter of the mainshock. Even though the Baja California data are included, the magnitude of completeness and the hypocentral errors increase gradually with distance south of the international border. The spatial distribution of large aftershocks is asymmetric with five M5+ aftershocks located to the south of the mainshock, and only one M5.7 aftershock, but numerous smaller aftershocks to the north. Further, the northwest aftershock cluster exhibits complex faulting on both northwest and northeast planes. Thus, the aftershocks also express a complex pattern of stress release along strike. The overall rate of decay of the aftershocks is similar to the rate of decay of a generic California aftershock sequence. In addition, some triggered seismicity was recorded along the Elsinore and San Jacinto faults to the north, but significant northward migration of aftershocks has not occurred. The synthesis of the El Mayor-Cucapah sequence reveals transtensional regional tectonics, including the westward growth of the Mexicali Valley and the transfer of Pacific\u2013North America plate motion from the Gulf of California in the south into the southernmost San Andreas fault system to the north. We propose that the location of the 2010 El Mayor-Cucapah, as well as the 1992 Landers and 1999 Hector Mine earthquakes, may have been controlled by the bends in the plate boundary.",
        "doi": "10.1007/s00024-010-0209-7",
        "issn": "0033-4553",
        "publisher": "Springer",
        "publication": "Pure and Applied Geophysics",
        "publication_date": "2011-08",
        "series_number": "8-9",
        "volume": "168",
        "issue": "8-9",
        "pages": "1255-1277"
    },
    {
        "id": "authors:g8jew-bms44",
        "collection": "authors",
        "collection_id": "g8jew-bms44",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110801-133119672",
        "type": "article",
        "title": "Constraints on Jalisco Block Motion and Tectonics of the Guadalajara Triple Junction from 1998\u20132001 Campaign GPS Data",
        "author": [
            {
                "family_name": "Selvans",
                "given_name": "Michelle M.",
                "clpid": "Selvans-Michelle-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "DeMets",
                "given_name": "Charles",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "Sanchez",
                "given_name": "Osvaldo",
                "clpid": "Sanchez-Osvaldo"
            },
            {
                "family_name": "Marquez-Azua",
                "given_name": "Bertha",
                "clpid": "Marquez-Azua-Bertha"
            }
        ],
        "abstract": "A GPS campaign network in the state of Jalisco was\noccupied for ~36 h per station most years between 1995 and\n2005; we use data from 1998\u20132001 to investigate tectonic motion and interseismic deformation in the Jalisco area with respect to the North America plate. The twelve stations used in this analysis provide coverage of the Jalisco Block and adjacent North America plate, and show a pattern of motion that implies some contribution to Jalisco Block boundary deformation from both tectonic motion\nand interseismic deformation due to the offshore 1995 earthquake. The consistent direction and magnitude of station motion on the Jalisco Block with respect to the North America reference frame, ~2 mm/year to the southwest (95% confidence level), perhaps can be attributed to tectonic motion. However, some station velocities within and across the boundaries of the Jalisco Block are also non-zero (95% confidence level), and the overall pattern of\nstation velocities indicates both viscoelastic response to the 1995 earthquake and partial coupling of the subduction interface (together termed \"interseismic deformation\"). Our results show motion across the northern Colima rift, the eastern boundary of the Jalisco Block, which is likely to be sinistral oblique extension rather than pure extension. We constrain extension across both the Colima rift and the northeastern boundary of the Jalisco Block, the Tepic-\nZacoalco rift, to \u22648 mm/year (95% confidence level), slow compared to relative rates of motion at nearby plate boundaries.",
        "doi": "10.1007/s00024-010-0201-2",
        "issn": "0033-4553",
        "publisher": "Springer",
        "publication": "Pure and Applied Geophysics",
        "publication_date": "2011-08",
        "series_number": "8-9",
        "volume": "168",
        "issue": "8-9",
        "pages": "1435-1447"
    },
    {
        "id": "authors:n1v9k-q3s54",
        "collection": "authors",
        "collection_id": "n1v9k-q3s54",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110801-073428119",
        "type": "article",
        "title": "Double-difference Relocation of the Aftershocks of the Tecom\u00e1n, Colima, Mexico Earthquake of 22 January 2003",
        "author": [
            {
                "family_name": "Andrews",
                "given_name": "Vanessa",
                "clpid": "Andrews-V"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Ram\u00edrez V\u00e1zquez",
                "given_name": "Carlos Ariel",
                "clpid": "Ram\u00edrez-V\u00e1zquez-C-A"
            },
            {
                "family_name": "Reyes-D\u00e1vila",
                "given_name": "Gabriel",
                "clpid": "Reyes-D\u00e1vila-G"
            }
        ],
        "abstract": "On 22 January 2003, the M_w = 7.6 Tecom\u00e1n earthquake struck offshore of the state of Colima, Mexico, near the diffuse triple junction between the Cocos, Rivera, and North American plates. Three-hundred and fifty aftershocks of the Tecom\u00e1n earthquake with magnitudes between 2.6 and 5.8, each recorded by at least 7 stations, are relocated using the double difference method. Initial locations are determined using P and S readings from the Red Sismol\u00f3gica Telem\u00e9trica del Estado de Colima (RESCO) and a 1-D velocity model. Because only eight RESCO stations were operating immediately following the Tecom\u00e1n earthquake, uncertainties in the initial locations and depths are fairly large, with average uncertainties of 8.0 km in depth and 1.4 km in the north\u2013south and east\u2013west directions. Events occurring between 24 January and 31 January were located using not only RESCO phase readings but also additional P and S readings from 11 temporary stations. Average uncertainties decrease to 0.8 km in depth, 0.3 km in the east\u2013west direction, and 0.7 km in the north\u2013south direction for events occurring while the temporary stations were deployed. While some preliminary studies of the early aftershocks suggested that they were dominated by shallow events above the plate interface, our results place the majority of aftershocks along the plate interface, for a slab dipping between approximately 20\u00b0 and 30\u00b0. This is consistent with the slab positions inferred from geodetic studies. We do see some upper plate aftershocks that may correspond to forearc fault zones, and faults inland in the upper plate, particularly among events occurring more than 3 months after the mainshock.",
        "doi": "10.1007/s00024-010-0203-0",
        "issn": "0033-4553",
        "publisher": "Springer",
        "publication": "Pure and Applied Geophysics",
        "publication_date": "2011-08",
        "series_number": "8-9",
        "volume": "168",
        "issue": "8-9",
        "pages": "1331-1338"
    },
    {
        "id": "authors:dm2p0-da335",
        "collection": "authors",
        "collection_id": "dm2p0-da335",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110815-111337829",
        "type": "article",
        "title": "Quantifying the forces needed for the rapid change of Pacific plate motion at 6 Ma",
        "author": [
            {
                "family_name": "Austermann",
                "given_name": "Jacqueline",
                "clpid": "Austermann-J"
            },
            {
                "family_name": "Ben-Avraham",
                "given_name": "Zvi",
                "clpid": "Ben-Avraham-Z"
            },
            {
                "family_name": "Bird",
                "given_name": "Peter",
                "clpid": "Bird-P"
            },
            {
                "family_name": "Heidbach",
                "given_name": "Oliver",
                "clpid": "Heidbach-O"
            },
            {
                "family_name": "Schubert",
                "given_name": "Gerald",
                "clpid": "Schubert-G"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Studies have documented several rapid changes along the Pacific\u2013North American, Pacific\u2013Antarctic and Pacific\u2013Australian plate boundaries in latest Miocene to earliest Pliocene time consistent with a sudden clockwise rotation of Pacific plate velocity relative to hotspots during this period. We test the hypothesis that this change in plate motion was initiated by cessation of subduction along the northern Melanesian arc due to the collision between the arc and the Ontong Java plateau. This hypothesis has long been formulated but never tested quantitatively. We use a geomechanical model of the lithosphere to determine the changes in plate boundary forces that are necessary to obtain the observed change in the Pacific plate motion. Our model results show that the change in motion can be explained by a clockwise rotation of the slab-related (basal-strength) component of plate driving force. The change of slab-related force from a post-6 Ma to a pre-6 Ma setting is perpendicular to the arc and points towards the Australian plate. The force per unit length is in the range of currently accepted values for subduction zones. Since there have been no other relevant changes at subduction zones along the Pacific plate boundary during the latest Miocene, we relate this change in slab-related force to the former southward-dipping Pacific plate slab along the northern Melanesian arc system which is now detached. Our model results suggest that rapid changes in plate motion can be triggered by slab detachment, with consequences for plate boundary processes even at great distances from the event.",
        "doi": "10.1016/j.epsl.2011.04.043",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "2011-07-15",
        "series_number": "3-4",
        "volume": "307",
        "issue": "3-4",
        "pages": "289-297"
    },
    {
        "id": "authors:xa103-4x681",
        "collection": "authors",
        "collection_id": "xa103-4x681",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110104-091738151",
        "type": "article",
        "title": "Submarine landslides along the Malacca Strait-Mergui Basin shelf margin: Insights from sequence-stratigraphic analysis",
        "author": [
            {
                "family_name": "Lin",
                "given_name": "Yu\u2010nung Nina",
                "clpid": "Lin-Y-N-N"
            },
            {
                "family_name": "Sieh",
                "given_name": "Kerry",
                "orcid": "0000-0002-7311-2447",
                "clpid": "Sieh-K-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The enormously destructive tsunami of December 2004, caused by sudden motion of the Sunda megathrust beneath the Indian Ocean, raised concerns about tectonically induced tsunami worldwide. Submarine landslides may also trigger dangerous tsunami. However, the potential and repeat time for such events is in most places poorly known due to inadequate exploration of the sea floor and age constraints. The high sediment flux and tectonic subsidence rate of the Malacca Strait-Mergui Basin shelf margin NE of northernmost Sumatra provide a favorable environment to generate and preserve submarine landslides. From ten seismic reflection profiles acquired in 2006, we identify three sediment packages that exhibit sliding characteristics such as headscarps, distorted beds and debris-toe structures. We assign lowstand marine isotope stages to the paleo-shoreline indicators observed in the profiles. We then determine the ages of these submarine landslides as 20\u201330 ka, 342\u2013364 ka and 435\u2013480 ka by the paleo-shoreline indicators that bound the top and bottom of the slide bodies. This sequence-stratigraphic approach shows that these events occurred near times of sea-level lowstands, which implies that a large amount of direct sediment influx during glacial periods is an essential precondition for basin-margin submarine landsliding. Spatiotemporal variations of sediment input due to lobe switching or Asian monsoon intensity changes also control basin-margin instability. Because we are currently at a highstand stage, and sediment flux to the continental margin is relatively small, so the chance of having a repeat submarine landslide and landslide tsunami along this basin-margin is low.",
        "doi": "10.1029/2009JB007050",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "2010-12-02",
        "volume": "115",
        "pages": "Art. No. B12102"
    },
    {
        "id": "authors:rnv4r-3n217",
        "collection": "authors",
        "collection_id": "rnv4r-3n217",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20101206-100510765",
        "type": "article",
        "title": "Abyssal hill deflections at Pacific-Antarctic ridge-transform intersections",
        "author": [
            {
                "family_name": "Croon",
                "given_name": "Marcel B.",
                "clpid": "Croon-M-B"
            },
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Nearly complete coverage of shipboard multibeam bathymetry data at the right-stepping Menard and Pitman Fracture Zones allowed us to map abyssal hill deviations along their traces. In this study we distinguish between (1) J-shaped curvatures at their origin, where modeling is addressing primary volcanism and faulting following a curved zone, and (2) straight abyssal hills getting bent in anti-J-shaped curvatures, in response to increased coupling across the transform fault, after they were formed. We compared the mapped abyssal hill deflections to a detailed plate motion model for the Pacific-Antarctic Ridge to test how abyssal hill curvature correlates to changes in plate motion direction, which lead to periods of transtension or transpression. This test was based on the number and size of the abyssal hill deflections. The observations show a high abundance of J-shaped abyssal hills during periods of significant clockwise change in plate motion direction, which leads to transtension. The tip of the ridge axis can deflect up to 60\u00b0 into the transform fault in response to changes in the stress field at ridge-transform intersections. This is observed, in particular, at the Pitman Fracture Zone, where there has been a \u223c15\u00b0 clockwise rotation of the spreading direction azimuth during the last 9 Myr. In addition, we observed anti-J-shaped curvatures at Menard, Pitman, and Heirtzler Fracture Zones during periods of transpression when increased coupling across an oceanic transform fault is partially accommodated by distributed strike-slip deformation rather than solely by discontinuous displacement at the transform fault. Anti-J-shaped deflections typically develop in seafloor less than 2 Myr old when the oceanic lithosphere is thin.",
        "doi": "10.1029/2010GC003236",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2010-11-09",
        "volume": "11",
        "pages": "Art. No. Q11004"
    },
    {
        "id": "authors:6w7nz-f0409",
        "collection": "authors",
        "collection_id": "6w7nz-f0409",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20100830-113018904",
        "type": "article",
        "title": "Postspreading rifting in the Adare Basin, Antarctica: Regional tectonic consequences",
        "author": [
            {
                "family_name": "Granot",
                "given_name": "R.",
                "clpid": "Granot-R"
            },
            {
                "family_name": "Cande",
                "given_name": "S. C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Davey",
                "given_name": "F. J.",
                "clpid": "Davey-F-J"
            },
            {
                "family_name": "Clayton",
                "given_name": "R. W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            }
        ],
        "abstract": "Extension during the middle Cenozoic (43\u201326 Ma) in the north end of the West Antarctic rift system (WARS) is well constrained by seafloor magnetic anomalies formed at the extinct Adare spreading axis. Kinematic solutions for this time interval suggest a southward decrease in relative motion between East and West Antarctica. Here we present multichannel seismic reflection and seafloor mapping data acquired within and near the Adare Basin on a recent geophysical cruise. We have traced the ANTOSTRAT seismic stratigraphic framework from the northwest Ross Sea into the Adare Basin, verified and tied to DSDP drill sites 273 and 274. Our results reveal three distinct periods of tectonic activity. An early localized deformational event took place close to the cessation of seafloor spreading in the Adare Basin (~24 Ma). It reactivated a few normal faults and initiated the formation of the Adare Trough. A prominent pulse of rifting in the early Miocene (~17 Ma) resulted in normal faulting that initiated tilted blocks. The overall trend of structures was NE\u2013SW, linking the event with the activity outside the basin. It resulted in major uplift of the Adare Trough and marks the last extensional phase of the Adare Basin. Recent volcanic vents (Pliocene to present day) tend to align with the early Miocene structures and the on-land Hallett volcanic province. This latest phase of tectonic activity also involves near-vertical normal faulting (still active in places) with negligible horizontal consequences. The early Miocene extensional event found within the Adare Basin does not require a change in the relative motion between East and West Antarctica. However, the lack of subsequent rifting within the Adare Basin coupled with the formation of the Terror Rift and an on-land and subice extension within the WARS require a pronounced change in the kinematics of the rift. These observations indicate that extension increased southward, therefore suggesting that a major change in relative plate motion took place in the middle Miocene. The late Miocene pole of rotation might have been located north of the Adare Basin, with opposite opening sign compared to the Eocene-Oligocene pole.",
        "doi": "10.1029/2010GC003105",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2010-08-04",
        "volume": "11",
        "pages": "Art. No. Q08005"
    },
    {
        "id": "authors:ngpqk-75f38",
        "collection": "authors",
        "collection_id": "ngpqk-75f38",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20091012-125444405",
        "type": "article",
        "title": "Pulling plates apart",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The Salton Sea is located in a sedimentary basin at the southern termination of the San Andreas fault. High-resolution seismic data indicate that the basin formed and grew by active subsidence at its southern end.",
        "doi": "10.1038/ngeo597",
        "issn": "1752-0894",
        "publisher": "Nature Publishing Group",
        "publication": "Nature Geoscience",
        "publication_date": "2009-08",
        "series_number": "8",
        "volume": "2",
        "issue": "8",
        "pages": "541-542"
    },
    {
        "id": "authors:zhah0-71484",
        "collection": "authors",
        "collection_id": "zhah0-71484",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20090821-081957305",
        "type": "article",
        "title": "Slowing of India's convergence with Eurasia since 20 Ma and its implications for Tibetan mantle dynamics",
        "author": [
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Reconstructions of the relative positions of the India and Eurasia plates, using recently revised histories of movement between India and Somalia and between North America and Eurasia and of the opening of the East African Rift, show that India's convergence rate with Eurasia slowed by more than 40% between 20 and 10 Ma. Much evidence suggests that beginning in that interval, the Tibetan Plateau grew outward rapidly and that radially oriented compressive strain in the area surrounding Tibet increased. An abrupt increase in the mean elevation of the plateau provides a simple explanation for all of these changes. Elementary calculations show that removal of mantle lithosphere from beneath Tibet, or from just part of it, would lead to both a modest increase in the mean elevation of the plateau of ~1 km and a substantial change in the balance of forces per unit length applied to the India and Eurasia plates.",
        "doi": "10.1029/2008TC002271",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "2009-05-16",
        "volume": "28",
        "pages": "TC3001"
    },
    {
        "id": "authors:70bvz-g4q90",
        "collection": "authors",
        "collection_id": "70bvz-g4q90",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:VIDbsgf08",
        "type": "article",
        "title": "Isotope geochemistry and petrogenesis of peralkaline Middle Miocene ignimbrites from central Sonora: relationship with continental break-up and the birth of the Gulf of California",
        "author": [
            {
                "family_name": "Vidal Solano",
                "given_name": "Jes\u00fas R.",
                "clpid": "Vidal-Solano-Jes\u00fas-R"
            },
            {
                "family_name": "Lapierre",
                "given_name": "Henriette",
                "clpid": "Lapierre-Henriette"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Demant",
                "given_name": "Alain",
                "clpid": "Demant-Alain"
            },
            {
                "family_name": "Paz Moreno",
                "given_name": "Francisco A.",
                "clpid": "Paz-Moreno-Francisco-A"
            },
            {
                "family_name": "Bosch",
                "given_name": "Delphine",
                "clpid": "Bosch-Delphine"
            },
            {
                "family_name": "Brunet",
                "given_name": "Pierre",
                "clpid": "Brunet-Pierre"
            },
            {
                "family_name": "Amortegui",
                "given_name": "Andrea",
                "clpid": "Amortegui-Andrea"
            }
        ],
        "abstract": "Middle Miocene peralkaline ignimbrites constitute a specific geodynamic marker of the early stage of opening of the Gulf of California, preserved either in central Sonora or the Puertecitos area, in Baja California. Very uniform ages (12-12.5 Ma) obtained on these rocks show that this volcanic episode corresponds to a specific stage in the tectonic evolution of the proto-gulf area. Field observations and slightly different Sr and Nd isotopic signatures support eruptions from several small volume magma batches rather than from a large-volume caldera forming event. Isotopic ratios help to constrain the petrogenesis of the peralkaline liquids by fractional crystallization of transitional basalts in a shallow reservoir, with slight contamination by Precambrian upper crustal material. Less differentiated glomeroporphyritic icelandites erupted at about 11 Ma, mark an increase in the magma production rate and highlight an easier access to the surface, illustrating an advanced stage in the weakening of the continental crust. The tilting of the Middle Tertiary sequences results from a major change in the tectonic regime, from E-W extension giving rise to N-S grabens, to NNW-SSE strike-slip motion that can be related to the transfer of Baja California from North America to the Pacific plate. The location of peralkaline volcanism coincides with the southern edge of the Precambrian crust and the southernmost extension of the California slab window at 12.5 Ma.",
        "doi": "10.2113/gssgfbull.179.5.453",
        "issn": "0037-9409",
        "publisher": "Soci\u00e9t\u00e9 G\u00e9ologique de France",
        "publication": "Bulletin de la Soci\u00e9t\u00e9 G\u00e9ologique de France",
        "publication_date": "2008-09",
        "series_number": "5",
        "volume": "179",
        "issue": "5",
        "pages": "453-464"
    },
    {
        "id": "authors:gvzg4-hst13",
        "collection": "authors",
        "collection_id": "gvzg4-hst13",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:CROggg08",
        "type": "article",
        "title": "Revised Pacific-Antarctic plate motions and geophysics of the Menard Fracture Zone",
        "author": [
            {
                "family_name": "Croon",
                "given_name": "Marcel B.",
                "clpid": "Croon-M-B"
            },
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "A reconnaissance survey of multibeam bathymetry and magnetic anomaly data of the Menard Fracture Zone allows for significant refinement of plate motion history of the South Pacific over the last 44 million years. The right-stepping Menard Fracture Zone developed at the northern end of the Pacific-Antarctic Ridge within a propagating rift system that generated the Hudson microplate and formed the conjugate Henry and Hudson Troughs as a response to a major plate reorganization \u223c45 million years ago. Two splays, originally about 30 to 35 km apart, narrowed gradually to a corridor of 5 to 10 km width, while lineation azimuths experienced an 8\u00b0 counterclockwise reorientation owing to changes in spreading direction between chrons C13o and C6C (33 to 24 million years ago). We use the improved Pacific-Antarctic plate motions to analyze the development of the southwest end of the Pacific-Antarctic Ridge. Owing to a 45\u00b0 counterclockwise reorientation between chrons C27 and C20 (61 to 44 million years ago) this section of the ridge became a long transform fault connected to the Macquarie Triple Junction. Following a clockwise change starting around chron C13o (33 million years ago), the transform fault opened. A counterclockwise change starting around chron C10y (28 millions years ago) again led to a long transform fault between chrons C6C and C5y (24 to 10 million years ago). A second period of clockwise reorientation starting around chron C5y (10 million years ago) put the transform fault into extension, forming an array of 15 en echelon transform faults and short linking spreading centers.",
        "doi": "10.1029/2008GC002019",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2008-07-01",
        "series_number": "7",
        "volume": "9",
        "issue": "7",
        "pages": "2008GC002019"
    },
    {
        "id": "authors:7797z-9gr15",
        "collection": "authors",
        "collection_id": "7797z-9gr15",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20121001-090154547",
        "type": "article",
        "title": "Vertical tectonics of the High Plateau region, Manihiki Plateau, Western Pacific, from seismic stratigraphy",
        "author": [
            {
                "family_name": "Ai",
                "given_name": "Huirong-Anita",
                "clpid": "Ai-Huirong-Anita"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Clayton",
                "given_name": "Robert",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            },
            {
                "family_name": "Luyendyk",
                "given_name": "Bruce",
                "clpid": "Luyendyk-B"
            }
        ],
        "abstract": "The Manihiki Plateau is an elevated oceanic volcanic plateau that was formed mostly in Early Cretaceous time by hotspot activity. We analyze new seismic reflection data acquired on cruise KIWI 12 over the High Plateau region in the southeast of the plateau, to look for direct evidence of the location of the heat source and the timing of uplift, subsidence and faulting. These data are correlated with previous seismic reflection lines from cruise CATO 3, and with the results at DSDP Site 317 at the northern edge of the High Plateau. Seven key reflectors are identified from the seismic reflection profiles and the resulting isopach maps show local variations in thickness in the southeastern part of the High Plateau, suggesting a subsidence (cooling) event in this region during Late Cretaceous and up to Early Eocene time. We model this as a hotspot, active and centered on the High Plateau area during Early Cretaceous time in a near-ridge environment. The basement and Early Cretaceous volcaniclastic layers were formed by subaerial and shallow-water eruption due to the volcanic activity. After that, the plateau experienced erosion. The cessation of hotspot activity and subsequent heat loss by Late Cretaceous time caused the plateau to subside rapidly. The eastern and southern portions of the High Plateau were rifted away following the cessation of hot spot activity. As the southeastern portion of the High Plateau was originally higher and above the calcium carbonate compensation depth, it accumulated more sediments than the surrounding plateau regions. Apparently coeval with the rapid subsidence of the plateau are normal faults found at the SE edge of the plateau. Since Early Eocene time, the plateau subsided to its present depth without significant deformation.",
        "doi": "10.1007/s11001-008-9042-0",
        "issn": "0025-3235",
        "publisher": "Springer Verlag",
        "publication": "Marine Geophysical Research",
        "publication_date": "2008-01",
        "series_number": "1",
        "volume": "29",
        "issue": "1",
        "pages": "13-26"
    },
    {
        "id": "authors:4w4dw-sq068",
        "collection": "authors",
        "collection_id": "4w4dw-sq068",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20180427-155654058",
        "type": "article",
        "title": "COBBOOM: The Continental Breakkup and Birth of Oceans Mission",
        "author": [
            {
                "family_name": "Sawyer",
                "given_name": "Dale S.",
                "clpid": "Sawyer-D-S"
            },
            {
                "family_name": "Coffin",
                "given_name": "Millard F.",
                "clpid": "Coffin-M-F"
            },
            {
                "family_name": "Reston",
                "given_name": "Timothy J.",
                "clpid": "Reston-T-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hopper",
                "given_name": "John R.",
                "clpid": "Hopper-J-R"
            }
        ],
        "abstract": "The rupture of continents and creation of new oceans is a fundamental yet primitively understood aspect of the plate tectonic cycle. Building upon past achievements by ocean drilling and geophysical and geologic studies, we propose \"The Continental Breakup and Birth of Oceans Mission (COBBOOM)\" as the next major phase of discovery, for which sampling by drilling will be essential. \n\nIn September 2006, fifty-one scientists from six continents gathered in Pontresina, Switzerland to discuss current knowledge of continental breakup and sedimentary basin formation and how the Integrated Ocean Drilling Program (IODP) can deepen that knowledge (Coffin et al., 2006). Workshop participants discussed a global array of rifted margins (Fig. 1), formulated the critical problems to be addressed by future drilling and related investigations, and identified key rift systems poised for IODP investigations.",
        "doi": "10.2204/iodp.sd.5.02.2007",
        "issn": "1816-3459",
        "publisher": "ICDP/IODP",
        "publication": "Scientific Drilling",
        "publication_date": "2007-09-01",
        "volume": "5",
        "pages": "13-25"
    },
    {
        "id": "authors:cg32j-dyt38",
        "collection": "authors",
        "collection_id": "cg32j-dyt38",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20201202-151324692",
        "type": "article",
        "title": "COBBOOM: The Continental Breakup and Birth of Oceans Mission",
        "author": [
            {
                "family_name": "Sawyer",
                "given_name": "Dale S.",
                "clpid": "Sawyer-Dale-S"
            },
            {
                "family_name": "Coffin",
                "given_name": "Millard F.",
                "clpid": "Coffin-Millard-F"
            },
            {
                "family_name": "Reston",
                "given_name": "Timothy J.",
                "clpid": "Reston-Timothy-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hopper",
                "given_name": "John R.",
                "clpid": "Hopper-John-R"
            }
        ],
        "abstract": "The rupture of continents and creation of new oceans is a\nfundamental yet primitively understood aspect of the plate\ntectonic cycle. Building upon past achievements by ocean\ndrilling and geophysical and geologic studies, we propose\n\"The Continental Breakup and Birth of Oceans Mission\n(COBBOOM)\" as the next major phase of discovery, for\nwhich sampling by drilling will be essential.",
        "doi": "10.2204/iodp.sd.5.02.2007",
        "issn": "1816-3459",
        "publisher": "ICDP/IODP",
        "publication": "Scientific Drilling",
        "publication_date": "2007-09",
        "volume": "5",
        "pages": "13-25"
    },
    {
        "id": "authors:6cgfm-sfr78",
        "collection": "authors",
        "collection_id": "6cgfm-sfr78",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20100222-095232667",
        "type": "article",
        "title": "A geodetic study of the 2003 January 22 Tecom\u00e1n, Colima, Mexico earthquake",
        "author": [
            {
                "family_name": "Schmitt",
                "given_name": "Stuart V.",
                "clpid": "Schmitt-Stuart-V"
            },
            {
                "family_name": "DeMets",
                "given_name": "Charles",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "clpid": "S\u00e1nchez-Osvaldo"
            },
            {
                "family_name": "M\u00e1rquez-Az\u00faa",
                "given_name": "B.",
                "clpid": "M\u00e1rquez-Az\u00faa-Bertha"
            },
            {
                "family_name": "Reyes",
                "given_name": "G.",
                "clpid": "Reyes-G"
            }
        ],
        "abstract": "We use coseismic displacements and aftershock information from Global Positioning System (GPS) measurements at 27 sites in western Mexico and a 12-station local seismic network to determine the characteristics of the 2003 January  22 M_w = 7.2  subduction thrust earthquake near Tecom\u00e1n, Colima, Mexico. Estimates of the earthquake moment, slip direction and best-fitting slip distribution are derived by optimizing the fit to the GPS displacements for a 3-D finite element mesh that simulates the study area. The calculated moment release is  9.1 \u00d7 10^(19) N m (M_w = 7.2) , with maximum slip of 2 m at a depth of 24 km and a maximum rupture depth of 35\u201340 km. The inversion indicates that coseismic rupture extended downdip from depths of 9 to 40 km along a 80 km along-strike region that is bounded by the edges of the Manzanillo Trough. The optimal solution is robust with respect to plausible changes in the subduction interface geometry and differing subsets of the data. A comparison of the cumulative post-seismic slip that can be inferred separately from earthquake aftershocks and GPS measurements within a year of the earthquake indicates that 95 per cent or more of the post-seismic deformation was aseismic. Near-term post-seismic measurements indicate that slip propagated downdip to areas of the subduction interface beneath the coastline within days following the earthquake, as also occurred after the nearby  M_w = 8.0  Colima-Jalisco subduction earthquake in 1995. The similar behaviours and locations of the 1995/2003 earthquake sequence to two earthquakes in June of 1932 suggests that thrust earthquakes along the subduction interface northwest of the Manzanillo Trough may trigger earthquakes in the vicinity of the Manzanillo Trough; however, our modelling of Coulomb stress changes caused by the 1995 earthquake indicate that it induced only modest unclamping of the subduction interface in the vicinity of the Tecom\u00e1n rupture. In addition, GPS measurements indicate that elastic shortening characterized areas onshore from the Tecom\u00e1n rupture from mid-1997 up until the time of the rupture, consistent with progressively stronger clamping of the subduction interface during this period. This precludes any obvious triggering relationship with the 1995 earthquake. The apparent coincidence of the edge of both the 1932 and 1995/2003 rupture sequences with the edge of the Manzanillo Trough may indicate that the trough is a mechanical barrier to along-strike rupture propagation. This implies a limit to the area of potential slip and hence rupture magnitude during future large earthquakes in this region.",
        "doi": "10.1111/j.1365-246X.2006.03322.x",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2007-05",
        "series_number": "2",
        "volume": "169",
        "issue": "2",
        "pages": "389-406"
    },
    {
        "id": "authors:cjvsd-xah13",
        "collection": "authors",
        "collection_id": "cjvsd-xah13",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20121001-094812502",
        "type": "article",
        "title": "History of the Cretaceous Osbourn spreading center",
        "author": [
            {
                "family_name": "Downey",
                "given_name": "Nathan J.",
                "clpid": "Downey-N-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Clayton",
                "given_name": "Robert W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            },
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            }
        ],
        "abstract": "The Osbourn Trough is a fossil spreading center that rifted apart the Manihiki and Hikurangi Plateaus during Cretaceous time. Previous models of the Osbourn spreading center are based on data collected near the trough axis, and therefore only constrain the history of the Osbourn spreading center during the last few Ma of spreading. Our data set includes multibeam data collected northward to the Manihiki Plateau, allowing us to examine seafloor morphology created during the entire active period of the Osbourn spreading center, as well as several additional multibeam data sets that provide the opportunity to examine the relationship between the Osbourn paleospreading center and the Cretaceous Pacific-Phoenix ridge. The axial gravity of the trough is similar to the gravity found at other extinct slow-intermediate spreading rate ridges. Magnetic field measurements indicate that spreading at the trough ceased during Chron C34. Abyssal-hill trends indicate that spreading during the early history of the Osbourn spreading center occurred at 15\u00b0\u201320\u00b0. The east-west component of this spreading explains the modern east-west offset of the Manihiki and Hikurangi Plateaus. Spreading rotated to 2\u00b0\u20135\u00b0 prior to extinction. Abyssal-hill RMS amplitudes show that a decrease in spreading rate, from &gt;7 cm/yr to 2\u20136 cm/yr full-spreading rate, occurred \u223c2\u20136 Ma prior to ridge extinction. Our data analysis is unable to determine the exact spreading rate of the Osbourn spreading center prior to the slowing event. The temporal constraints provided by our data show that the Osbourn spreading center ceased spreading prior to 87 Ma or 93 Ma, depending on whether the Manihiki and Hikurangi Plateaus rifted at 115 Ma or 121 Ma. Our model resolves the conflict between regional models of Osbourn spreading with models based on trough characteristics by showing that spreading at the Osbourn spreading center was decoupled from Pacific-Phoenix spreading.",
        "doi": "10.1029/2006JB004550",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "2007-04-06",
        "series_number": "B4",
        "volume": "112",
        "issue": "B4",
        "pages": "Art. No. B04102"
    },
    {
        "id": "authors:5p52g-ef570",
        "collection": "authors",
        "collection_id": "5p52g-ef570",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140522-084410391",
        "type": "article",
        "title": "Extension in the western Ross Sea region-links between Adare Basin and Victoria Land Basin",
        "author": [
            {
                "family_name": "Davey",
                "given_name": "F. J.",
                "clpid": "Davey-F-J"
            },
            {
                "family_name": "Cande",
                "given_name": "S. C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Spreading in the Adare Basin off north-western Ross Sea (43\u201326 Ma) and extension in the Victoria Land Basin (VLB, &gt; 36 Ma) are used to constrain the pole of rotation for the Adare Basin, providing a rifting model for the region for the past 45 Ma. The offset from Northern Basin to VLB at about 74\u00b0S coincides with the linear Polar-3 magnetic anomaly, inferred to be caused by a major 48 - 34 Ma igneous intrusion. The style of extension apparently changed at about 34 Ma, with the end of intrusion at the Polar-3 anomaly, a change from highly asymmetric extension in Adare Basin, and the onset of major subsidence on the flanks of VLB. Ductile lower crustal and lithospheric flow is proposed as the cause of the inferred thick crust underlying southern Adare Basin, and a result of the constraining of extension to the adjacent contiguous Northern Basin.",
        "doi": "10.1029/2006GL027383",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "2006-10-27",
        "series_number": "20",
        "volume": "33",
        "issue": "20",
        "pages": "Art. No. L20315"
    },
    {
        "id": "authors:r5199-44m21",
        "collection": "authors",
        "collection_id": "r5199-44m21",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140416-152556111",
        "type": "article",
        "title": "The Hawaiian-Emperor Bend: Older than expected",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The kink in the Hawaiian-Emperor seamount chain in the Pacific Ocean was initiated ~50 million years ago, at a time when major plate motion changes occurred.",
        "doi": "10.1126/science.1131789",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "2006-09-01",
        "series_number": "5791",
        "volume": "313",
        "issue": "5791",
        "pages": "1250-1251"
    },
    {
        "id": "authors:pbq3e-wpq66",
        "collection": "authors",
        "collection_id": "pbq3e-wpq66",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:MULggg05",
        "type": "article",
        "title": "Crustal structure and rift flank uplift of the Adare Trough, Antarctica",
        "author": [
            {
                "family_name": "M\u00fcller",
                "given_name": "R. Dietmar",
                "orcid": "0000-0002-3334-5764",
                "clpid": "M\u00fcller-R-D"
            },
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Keller",
                "given_name": "William R.",
                "clpid": "Keller-W-R"
            }
        ],
        "abstract": "The Adare Trough, located 100 km northeast of Cape Adare, Antarctica, represents the extinct third arm of a Tertiary spreading ridge between East and West Antarctica. It is characterized by pronounced asymmetric rift flanks elevated up to over 2 km above the trough's basement, accompanied by a large positive mantle Bouguer anomaly. On the basis of recently acquired seismic reflection and ship gravity data, we invert mantle Bouguer anomalies from the Adare Trough and obtain an unexpectedly large oceanic crustal thickness maximum of 9\u201310.5 km underneath the extinct ridge. A regional positive residual basement depth anomaly between 1 and 2.5 km in amplitude characterizes ocean crust from offshore Victoria Land to the Balleny Islands and north of Iselin Bank. The observations and models indicate that the mid/late Tertiary episode of slow spreading between East and West Antarctica was associated with a mantle thermal anomaly. The increasing crustal thickness toward the extinct ridge indicates that this thermal mantle anomaly may have increased in amplitude through time during the Adare spreading episode. This scenario is supported by a mantle convection model, which indicates the formation and strengthening of a major regional negative upper mantle density anomaly in the southwest Pacific in the last 50 million years. The total amount of post-26 Ma extension associated with Adare Trough normal faulting was about 7.5 km, in anomalously thick oceanic crust with a lithospheric effective elastic thickness (EET) between 3.5 and 5 km. This corresponds to an age between 3 and 5 million years based on a thermal boundary layer model and supports a scenario in which the Adare Trough formed soon after spreading between East and West Antarctica ceased, confined to relatively weak lithosphere with anomalously thick oceanic crust. There is little evidence for major subsequent structural activity in the Adare trough area from the available seismic data, indicating that this part of the West Antarctic Rift system became largely inactive in the early Miocene, with the exception of minor structural reactivation which is visible in the seismic data as offsets up to end of the early Pliocene.",
        "doi": "10.1029/2005GC001027",
        "issn": "1525-2027",
        "publisher": "American Geophysical Union",
        "publication": "Geochemistry, Geophysics, Geosystems",
        "publication_date": "2005-11-23",
        "series_number": "11",
        "volume": "6",
        "issue": "11",
        "pages": "2005GC001027"
    },
    {
        "id": "authors:djbja-q6t79",
        "collection": "authors",
        "collection_id": "djbja-q6t79",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140522-071230681",
        "type": "article",
        "title": "Mapping variations in weight percent silica measured from multispectral thermal infrared imagery\u2014Examples from the Hiller Mountains, Nevada, USA and Tres Virgenes-La Reforma, Baja California Sur, Mexico",
        "author": [
            {
                "family_name": "Hook",
                "given_name": "Simon J.",
                "clpid": "Hook-S-J"
            },
            {
                "family_name": "Dmochowski",
                "given_name": "Jane E.",
                "clpid": "Dmochowski-J-E"
            },
            {
                "family_name": "Howard",
                "given_name": "Keith A.",
                "clpid": "Howard-K-A"
            },
            {
                "family_name": "Rowan",
                "given_name": "Lawrence C.",
                "clpid": "Rowan-L-C"
            },
            {
                "family_name": "Karlstrom",
                "given_name": "Karl E.",
                "clpid": "Karlstrom-K-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Remotely sensed multispectral thermal infrared (8\u201313 \u03bcm) images are increasingly being used to map variations in surface silicate mineralogy. These studies utilize the shift to longer wavelengths in the main spectral feature in minerals in this wavelength region (reststrahlen band) as the mineralogy changes from felsic to mafic. An approach is described for determining the amount of this shift and then using the shift with a reference curve, derived from laboratory data, to remotely determine the weight percent SiO_2 of the surface. The approach has broad applicability to many study areas and can also be fine-tuned to give greater accuracy in a particular study area if field samples are available. The approach was assessed using airborne multispectral thermal infrared images from the Hiller Mountains, Nevada, USA and the Tres Virgenes-La Reforma, Baja California Sur, Mexico. Results indicate the general approach slightly overestimates the weight percent SiO_2 of low silica rocks (e.g. basalt) and underestimates the weight percent SiO_2 of high silica rocks (e.g. granite). Fine tuning the general approach with measurements from field samples provided good results for both areas with errors in the recovered weight percent SiO_2 of a few percent. The map units identified by these techniques and traditional mapping at the Hiller Mountains demonstrate the continuity of the crystalline rocks from the Hiller Mountains southward to the White Hills supporting the idea that these ranges represent an essentially continuous footwall block below a regional detachment. Results from the Baja California data verify the most recent volcanism to be basaltic\u2013andesite",
        "doi": "10.1016/j.rse.2004.11.020",
        "issn": "0034-4257",
        "publisher": "Elsevier",
        "publication": "Remote Sensing of Environment",
        "publication_date": "2005-04-15",
        "series_number": "3",
        "volume": "95",
        "issue": "3",
        "pages": "273-289"
    },
    {
        "id": "authors:5kbte-70m64",
        "collection": "authors",
        "collection_id": "5kbte-70m64",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140416-090150847",
        "type": "article",
        "title": "Pacific-Antarctic-Australia motion and the formation of the Macquarie Plate",
        "author": [
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Magnetic anomaly and fracture zone data on the Southeast Indian Ridge (SEIR) are analysed in order to constrain the kinematic history of the Macquarie Plate, the region of the Australian Plate roughly east of 145\u00b0E and south of 52\u00b0S. Finite rotations for Australia\u2013Antarctic motion are determined for nine chrons (2Ay, 3Ay, 5o, 6o, 8o, 10o, 12o, 13o and 17o) using data limited to the region between 88\u00b0E and 139\u00b0E. These rotations are used to generate synthetic flowlines which are compared with the observed trends of the easternmost fracture zones on the SEIR. An analysis of the synthetic flowlines shows that the Macquarie Plate region has behaved as an independent rigid plate for roughly the last 6 Myr. Finite rotations for Macquarie\u2013Antarctic motion are determined for chrons 2Ay and 3Ay. These rotations are summed with Australia\u2013Antarctic rotations to determine Macquarie\u2013Australia rotations. We find that the best-fit Macquarie\u2013Australia rotation poles lie within the zone of diffuse intraplate seismicity in the South Tasman Sea separating the Macquarie Plate from the main part of the Australian Plate. Motion of the Macquarie Plate relative to the Pacific Plate for chrons 2Ay and 3Ay is determined by summing Macquarie\u2013Antarctic and Antarctic\u2013Pacific rotations. The Pacific\u2013Macquarie rotations predict a smaller rate of convergence perpendicular to the Hjort Trench than the Pacific\u2013Australia rotations. The onset of the deformation of the South Tasman Sea and the development of the Macquarie Plate appears to have been triggered by the subduction of young, buoyant oceanic crust near the Hjort Trench and coincided with a clockwise change in Pacific\u2013Australia motion around 6 Ma. The revised Pacific\u2013Australia rotations also have implications for the tectonics of the Alpine Fault Zone of New Zealand. We find that changes in relative displacement along the Alpine Fault have been small over the last 20 Myr. The average rate of convergence over the last 6 Myr is about 40 per cent smaller than in previous models.",
        "doi": "10.1111/j.1365-246X.2004.02224.x",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2004-04",
        "series_number": "1",
        "volume": "157",
        "issue": "1",
        "pages": "399-414"
    },
    {
        "id": "authors:n9n1e-hn262",
        "collection": "authors",
        "collection_id": "n9n1e-hn262",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20101123-103005860",
        "type": "article",
        "title": "Cenozoic evolution of Neotethys and implications for the causes of plate motions",
        "author": [
            {
                "family_name": "McQuarrie",
                "given_name": "N.",
                "clpid": "McQuarrie-N"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Verdel",
                "given_name": "C.",
                "clpid": "Verdel-C"
            },
            {
                "family_name": "Wernicke",
                "given_name": "B. P.",
                "orcid": "0000-0002-7659-8358",
                "clpid": "Wernicke-B-P"
            }
        ],
        "abstract": "Africa-North America-Eurasia plate circuit rotations, combined with Red Sea rotations and new estimates of crustal shortening in Iran define the Cenozoic history of the Neotethyan ocean between Arabia and Eurasia. The new constraints indicate that Arabia-Eurasia convergence has been fairly constant at 2 to 3 cm/yr since 56 Ma with slowing of Africa-Eurasia motion to &lt;1 cm/yr near 25 Ma, coeval with the opening of the Red Sea. Ocean closure occurred no later than 10 Ma, and could have occurred prior to this time only if a large amount of continental lithosphere was subducted, suggesting that slowing of Africa significantly predated the Arabia-Eurasia collision. These kinematics imply that Africa's disconnection with the negative buoyancy of the downgoing slab of lithosphere beneath southern Eurasia slowed its motion. The slow, steady rate of northward subduction since 56 Ma contrasts with strongly variable rates of magma production in the Urumieh-Dokhtar arc, implying magma production rate in continental arcs is not linked to subduction rate.",
        "doi": "10.1029/2003GL017992",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "2003-10-21",
        "series_number": "20",
        "volume": "30",
        "issue": "20",
        "pages": "Art. No. 2036"
    },
    {
        "id": "authors:7ky1b-mwv82",
        "collection": "authors",
        "collection_id": "7ky1b-mwv82",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140423-095857093",
        "type": "article",
        "title": "Pacific-North America plate motion and opening of the Upper Delf\u00edn basin, northern Gulf of California, Mexico",
        "author": [
            {
                "family_name": "Oskin",
                "given_name": "Michael",
                "orcid": "0000-0002-6631-5326",
                "clpid": "Oskin-M-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Correlation of conjugate rifted margins of the Upper Delf\u00edn basin constrains the timing and amount of transtensional opening along the Pacific\u2013North America plate boundary in the northern Gulf of California. Lithologic, geochemical, paleomagnetic, and geochronologic data from a set of four ignimbrites, consisting of eight distinctive cooling units, are shown to correlate from northeastern Baja California to Isla Tibur\u00f3n and adjacent areas of western Sonora. These matching ignimbrites are the ca. 12.6 Ma tuff of San Felipe, the 6.3 \u00b1 0.2 Ma tuffs of Mesa Cuadrada (Tmr3 and Tmr4), the tuffs of Dead Battery Canyon (Tmr5), and the 6.1 \u00b1 0.5 Ma tuffs of Arroyo El Canelo. Offset distributions and facies patterns of these ignimbrites support 255 \u00b1 10 km of opening between conjugate rifted margins of the Upper Delf\u00edn basin. Addition of deformation from the continental margins of this basin indicates at least 276 \u00b1 13 km of Pacific\u2013North America plate motion between coastal Sonora and the main gulf escarpment in Baja California since ca. 6 Ma; a further 20 \u00b1 10 km of northwestward displacement of Isla Tibur\u00f3n relative to coastal Sonora occurred sometime after 12.6 Ma. These reconstructions agree with earlier estimates of slip across the Gulf of California and on the San Andreas fault system of southern California, but require that the Pacific\u2013North America plate boundary became localized in the gulf at ca. 6 Ma. The restored continental margins of the Upper Delf\u00edn basin show that only a 20\u201325 km width of upper continental crust has foundered beneath this part of the northern Gulf of California. This result suggests that most of the crustal area formed by opening of the Upper Delf\u00edn basin was either exhumed from lower-crustal levels or is new transitional oceanic crust.",
        "doi": "10.1130/B25154.1",
        "issn": "0016-7606",
        "publisher": "Geological Society of America",
        "publication": "Geological Society of America Bulletin",
        "publication_date": "2003-10",
        "series_number": "10",
        "volume": "115",
        "issue": "10",
        "pages": "1173-1190"
    },
    {
        "id": "authors:4c6qz-9xv89",
        "collection": "authors",
        "collection_id": "4c6qz-9xv89",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110107-085232264",
        "type": "article",
        "title": "Hotspots Come Unstuck",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Volcanic hotspots are widely believed to be caused by fixed volcanic sources deep in the mantle. In her Perspective, Stock highlights the report by Tarduno et al., whose paleomagnetic data cast doubt on the fixity of the hotspot underlying the Hawaiian-Emperor seamounts. The data suggest that not only plate motion but also mantle flow have determined the latitudes of the islands and seamounts in the chain. With current data, it is difficult to say whether the base of the hotspot has remained fixed or whether it is a third variable determining the motion of surface volcanism with time.",
        "doi": "10.1126/science.1089049",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "2003-08-22",
        "series_number": "5636",
        "volume": "301",
        "issue": "5636",
        "pages": "1059-1060"
    },
    {
        "id": "authors:pt5a9-90t57",
        "collection": "authors",
        "collection_id": "pt5a9-90t57",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140522-093031612",
        "type": "article",
        "title": "Active deformation and shallow structure of the Wagner,\n Consag, and Delf\u00edn Basins, northern Gulf of California, Mexico",
        "author": [
            {
                "family_name": "Persaud",
                "given_name": "Patricia",
                "orcid": "0000-0003-3462-7023",
                "clpid": "Persaud-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Steckler",
                "given_name": "Michael S.",
                "clpid": "Steckler-M-S"
            },
            {
                "family_name": "Mart\u00edn-Barajas",
                "given_name": "Arturo",
                "clpid": "Mart\u00edn-Barajas-A"
            },
            {
                "family_name": "Diebold",
                "given_name": "John B.",
                "clpid": "Diebold-J-B"
            },
            {
                "family_name": "Gonz\u00e1lez-Fern\u00e1ndez",
                "given_name": "Antonio",
                "clpid": "Gonz\u00e1lez-Fern\u00e1ndez-A"
            },
            {
                "family_name": "Mountain",
                "given_name": "Gregory S.",
                "clpid": "Mountain-G-S"
            }
        ],
        "abstract": "Oblique rifting began synchronously along the length of the Gulf of California at 6 Ma, yet there is no evidence for the existence of oceanic crust or a spreading transform fault system in the northern Gulf. Instead, multichannel seismic data show a broad shallow depression, \u223c70 \u00d7 200 km, marked by active distributed deformation and six \u223c10-km-wide segmented basins lacking well-defined transform faults. We present detailed images of faulting and magmatism based on the high resolution and quality of these data. The northern Gulf crust contains a dense (up to 18 faults in 5 km) complex network of mainly oblique-normal faults, with small offsets, dips of 60\u201380\u00b0 and strikes of N-N30\u00b0E. Faults with seafloor offsets of tens of meters bound the Lower and two Upper Delf\u00edn Basins. These subparallel basins developed along splays from a transtensional zone at the NW end of the Ballenas Transform Fault. Twelve volcanic knolls were identified and are associated with the strands or horsetails from this zone. A structural connection between the two Upper Delf\u00edn Basins is evident in the switching of the center of extension along axis. Sonobuoy refraction data suggest that the basement consists of mixed igneous sedimentary material, atypical of mid-ocean ridges. On the basis of the near-surface manifestations of active faulting and magmatism, seafloor spreading will likely first occur in the Lower Delf\u00edn Basin. We suggest the transition to seafloor spreading is delayed by the lack of strain-partitioned and focused deformation as a consequence of shear in a broad zone beneath a thick sediment cover.",
        "doi": "10.1029/2002JB001937",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "2003-07-31",
        "series_number": "B7",
        "volume": "108",
        "issue": "B7",
        "pages": "Art. No. 2355"
    },
    {
        "id": "authors:mhgwm-s1d24",
        "collection": "authors",
        "collection_id": "mhgwm-s1d24",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140904-141111178",
        "type": "article",
        "title": "Three distinct types of hotspots in the Earth's mantle",
        "author": [
            {
                "family_name": "Courtillot",
                "given_name": "Vincent",
                "clpid": "Courtillot-V"
            },
            {
                "family_name": "Davaille",
                "given_name": "Anne",
                "clpid": "Davaille-A"
            },
            {
                "family_name": "Besse",
                "given_name": "Jean",
                "clpid": "Besse-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The origin of mantle hotspots is a controversial topic. Only seven ('primary') out of 49 hotspots meet criteria aimed at detecting a very deep origin (three in the Pacific, four in the Indo-Atlantic hemisphere). In each hemisphere these move slowly, whereas there has been up to 50 mm/a motion between the two hemispheres prior to 50 Ma ago. This correlates with latitudinal shifts in the Hawaiian and Reunion hotspots, and with a change in true polar wander. We propose that hotspots may come from distinct mantle boundary layers, and that the primary ones trace shifts in quadrupolar convection in the lower mantle.",
        "doi": "10.1016/S0012-821X(02)01048-8",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "2003-01-10",
        "series_number": "3-4",
        "volume": "205",
        "issue": "3-4",
        "pages": "295-308"
    },
    {
        "id": "authors:z6y7m-dzt90",
        "collection": "authors",
        "collection_id": "z6y7m-dzt90",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140416-103726426",
        "type": "article",
        "title": "Marine incursion synchronous with plate-boundary localization in the Gulf of California",
        "author": [
            {
                "family_name": "Oskin",
                "given_name": "Michael",
                "orcid": "0000-0002-6631-5326",
                "clpid": "Oskin-M-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Volcanic strata on southwest Isla Tibur\u00f3n define the age of interstratified marine rocks and, through revision of existing correlations, the age of the proto\u2013Gulf of California marine incursion. A 5.7 \u00b1 0.2 Ma ash flow was emplaced at the base of the marine section. A rhyodacite dike and its related lava flow, dated as 11.2 \u00b1 1.3 Ma, 3.7 \u00b1 0.9 Ma, and 4.2 \u00b1 1.8 Ma, intrudes and overlies, respectively, the marine rocks. The 11.2 Ma age, which was the core datum for a middle Miocene proto\u2013Gulf of California origin for the underlying rocks, is discordant with all other isotopic and microfossil ages. An alternative interpretation, utilizing all available geologic and geochronologic data except this discordant age, is that marine strata on Isla Tibur\u00f3n are latest Miocene to early Pliocene age. Reinterpretation of these strata supports a simplified history of marine incursion into the Gulf of California. Marine rocks as old as 8.2 Ma in the southern Gulf of California indicate an early marine incursion, perhaps flooding a region of more intense proto\u2013Gulf of California continental extension. Flooding of the entire basin by 6.5\u20136.3 Ma correlates to the sudden onset of significant Pacific\u2013North American plate-boundary motion within the Gulf of California.",
        "doi": "10.1130/0091-7613(2003)031<0023:MISWPB>2.0.CO;2",
        "issn": "0091-7613",
        "publisher": "Geological Society of America",
        "publication": "Geology",
        "publication_date": "2003-01",
        "series_number": "1",
        "volume": "31",
        "issue": "1",
        "pages": "23-26"
    },
    {
        "id": "authors:hxvqd-k4e69",
        "collection": "authors",
        "collection_id": "hxvqd-k4e69",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-125909434",
        "type": "article",
        "title": "Rapid postseismic transients in subduction zones from\n continuous GPS",
        "author": [
            {
                "family_name": "Melbourne",
                "given_name": "Timothy I.",
                "clpid": "Melbourne-T-I"
            },
            {
                "family_name": "Webb",
                "given_name": "Frank H.",
                "clpid": "Webb-F-H"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Reigber",
                "given_name": "Christoph",
                "clpid": "Reigber-C"
            }
        ],
        "abstract": "Continuous GPS time series from three of four recently measured, large subduction earthquakes document triggered rapid postseismic fault creep, representing an additional moment release upward of 25% over the weeks following their main shocks. Data from two M_w = 8.0 and M_w = 8.4 events constrain the postseismic centroids to lie down dip from the lower limit of coseismic faulting, and show that afterslip along the primary coseismic asperities is significantly less important than triggered deep creep. Time series for another M_w = 7.7 event show 30% postseismic energy release, but here we cannot differentiate between afterslip and triggered deeper creep. A fourth M_w = 8.1 event, which occurred in the broad Chilean seismogenic zone, shows no postseismic deformation, despite coseismic offsets in excess of 1 m. For the three events which are followed by postseismic deformation, stress transferred to the inferred centroids (at 34,  60,  and 36 km depths) by their respective main shock asperities increased reverse shear stress by 0.5, 0.8, and 0.2 bar with a comparatively small decrease in normal stress (0.01 bar), constraining the Coulomb stress increase required to force slip along the metastable plate interface. Deep triggered slip of this nature is invisible without continuous geodesy but on the basis of these earthquakes would appear to constitute an important mode of strain release from beneath the seismogenic zones of convergent margins. These events, captured by some of the first permanent GPS networks, show that deep moment release is often modulated by seismogenic rupture updip and underscore the need for continuous geodesy to fully quantify the spectrum of moment release in great earthquakes.",
        "doi": "10.1029/2001JB000555",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "2002-10",
        "series_number": "B10",
        "volume": "107",
        "issue": "B10",
        "pages": "Art. No. 2241"
    },
    {
        "id": "authors:z8291-9mm93",
        "collection": "authors",
        "collection_id": "z8291-9mm93",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20121001-150237189",
        "type": "article",
        "title": "Mid-Cretaceous tectonic evolution of the Tongareva triple junction in the southwestern Pacific Basin",
        "author": [
            {
                "family_name": "Larson",
                "given_name": "Roger L.",
                "clpid": "Larson-R-L"
            },
            {
                "family_name": "Pockalny",
                "given_name": "Robert A.",
                "clpid": "Pockalny-R-A"
            },
            {
                "family_name": "Viso",
                "given_name": "Richard F.",
                "clpid": "Viso-R-F"
            },
            {
                "family_name": "Erba",
                "given_name": "Elisabetta",
                "clpid": "Erba-E"
            },
            {
                "family_name": "Abrams",
                "given_name": "Lewis J.",
                "clpid": "Abrams-L-J"
            },
            {
                "family_name": "Luyendyk",
                "given_name": "Bruce P.",
                "clpid": "Luyendyk-B-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Clayton",
                "given_name": "Robert W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            }
        ],
        "abstract": "The trace of the ridge-ridge-ridge triple junction that connected the Pacific, Farallon, and Phoenix plates during mid-Cretaceous time originates at the northeast corner of the Manihiki Plateau near the Tongareva atoll, for which the structure is named. The triple junction trace extends &gt;3250 km south-southeast, to and beyond a magnetic anomaly 34 bight. It is identified by the intersection of nearly orthogonal abyssal hill fabrics, which mark the former intersections of the Pacific-Phoenix and Pacific-Farallon Ridges. A distinct trough is commonly present at the intersection. A volcanic episode from 125 to 120 Ma created the Manihiki Plateau with at least twice its present volume, and displaced the triple junction southeast from the Nova-Canton Trough to the newly formed Manihiki Plateau. Almost simultaneously, the plateau was rifted by the new triple junction system, and large fragments of the plateau were rafted away to the south and east. The Tongareva triple junction originated ca. 119 Ma, when carbonate sedimentation began atop the Manihiki Plateau. Subsequent spreading rates on the Pacific-Phoenix and Pacific-Farallon Ridges averaged 18\u201320 cm/yr until 84 Ma.",
        "doi": "10.1130/0091-7613(2002)030<0067:MCTEOT>2.0.CO;2",
        "issn": "0091-7613",
        "publisher": "Geological Society of America",
        "publication": "Geology",
        "publication_date": "2002-01",
        "series_number": "1",
        "volume": "30",
        "issue": "1",
        "pages": "67-70"
    },
    {
        "id": "authors:8j2zh-3y436",
        "collection": "authors",
        "collection_id": "8j2zh-3y436",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-145647377",
        "type": "article",
        "title": "Homogeneous vs heterogeneous subduction zone models: Coseismic and postseismic deformation",
        "author": [
            {
                "family_name": "Masterlark",
                "given_name": "T.",
                "orcid": "0000-0001-8317-7167",
                "clpid": "Masterlark-Timothy"
            },
            {
                "family_name": "DeMets",
                "given_name": "C.",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "Wang",
                "given_name": "H. F.",
                "clpid": "Wang-H-F"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "clpid": "S\u00e1nchez-Osvaldo"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "A finite-element model (FEM) incorporating geologic properties characteristic of a subduction zone is compared with FEMs approximating homogeneous elastic half-spaces (HEHS)s to investigate the effect of heterogeneity on coseismic and postseismic deformation predictions for the 1995 Colima-Jalisco M_w =8.0 earthquake. The FEMs are used to compute a coefficient matrix relating displacements at observation points due to unit dislocations of contact-node pairs on the fault surface. The Green's function responses are used to solve the inverse problem of estimating dislocation distributions from coseismic GPS displacements. Predictions from the FEM with heterogeneous material properties, loaded with either of the HEHS dislocation distributions, significantly overestimate coseismic displacements. Postseismic deformation predictions are also sensitive to the coseismic dislocation distribution, which drives poroelastic and viscoelastic relaxation. FEM-generated Green's functions, which allow for spatial variations in material properties, are thus preferable to those that assume a simple HEHS because the latter leads to dislocation distributions unsuitable for predicting the postseismic response.",
        "doi": "10.1029/2001GL013612",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "2001-11-01",
        "series_number": "21",
        "volume": "28",
        "issue": "21",
        "pages": "4047-4050"
    },
    {
        "id": "authors:qst38-yh281",
        "collection": "authors",
        "collection_id": "qst38-yh281",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-132949940",
        "type": "article",
        "title": "Slip kinematics and dynamics during and after the 1995 October 9 M_w=8.0 Colima\u2013Jalisco earthquake, Mexico, from GPS geodetic constraints",
        "author": [
            {
                "family_name": "Hutton",
                "given_name": "W.",
                "clpid": "Hutton-W"
            },
            {
                "family_name": "DeMets",
                "given_name": "C.",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "clpid": "S\u00e1nchez-Osvaldo"
            },
            {
                "family_name": "Su\u00e1rez",
                "given_name": "G.",
                "orcid": "0000-0002-2011-4924",
                "clpid": "Su\u00e1rez-Genaro"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We use horizontal and vertical crustal displacements derived from GPS measurements at 26 sites in western Mexico to study the coseismic and post-seismic kinematics and dynamics of the 1995 October 9 (M_w=8.0) Colima\u2013Jalisco earthquake along the Middle America Trench. The measurements bracket the entire landward edge of the approximately 150 km long rupture zone and span a 4 yr period for most sites. We solve for the temporal evolution of slip along the subduction interface by inverting GPS displacements for the coseismic and four post-seismic intervals (March 1995\u2013March 1999), subject to the assumption that the crust responds elastically to slip along a shallow-dipping, curved subduction interface. Coseismic rupture of up to 5 m was largely focused above depths of 20 km and was limited to a 120\u2013140 km long segment of the subduction zone. Within one week of the earthquake, post-seismic slip migrated downdip to depths of 16\u201335 km, where it has since decayed logarithmically. We also find evidence for shallow aseismic slip during 1996 or early 1997 northwest of the coseismic rupture zone and increasingly widespread relocking of shallow regions of the subduction interface after early 1997. The relative lack of afterslip in shallow regions of the subduction interface suggests that the interface lies in the unstable frictional regime and hence is strongly coupled between earthquakes. By 1999, the cumulative slip moment associated with post-seismic slip equaled \u223c70 per cent of the coseismic moment, with nearly all of this slip occurring downdip from the coseismic rupture zone. The migration of slip after the earthquake to a deeper and presumably velocity-strengthening area of the subduction interface and the logarithmic decay of afterslip conform to the qualitative and quantitative predictions of a model in which the fault kinematics are prescribed by rate- and state-variable frictional laws. However, misfits to the geodetic displacements exceed the average displacement uncertainties for all epochs, implying one or more of the following: (1) the elastic response is heterogeneous due to slip along unmodelled upper crustal faults or variations in the elastic properties of the crust; (2) other post-seismic mechanisms such as viscoelastic or poroelastic effects contribute to or possibly dominate the post-seismic response; (3) we have underestimated the uncertainties in the GPS displacements.",
        "doi": "10.1046/j.1365-246X.2001.00472.x",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "2001-09",
        "series_number": "3",
        "volume": "146",
        "issue": "3",
        "pages": "637-658"
    },
    {
        "id": "authors:dhrjf-ekv54",
        "collection": "authors",
        "collection_id": "dhrjf-ekv54",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140416-090645328",
        "type": "article",
        "title": "Evolution of the Malvinas Plate South of Africa",
        "author": [
            {
                "family_name": "Marks",
                "given_name": "K. M.",
                "clpid": "Marks-K-M"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We confirm that a Malvinas Plate is required in the Agulhas Basin during the Late Cretaceous because: (1) oblique Mercator plots of marine gravity show that fracture zones generated on the Agulhas rift, as well as the Agulhas Fracture Zone, do not lie on small circles about the 33o-28y South America-Africa stage pole and were therefore not formed by South America-Africa spreading, (2) the 33o-28y South America-Africa stage rotation does not bring 33o magnetic anomalies on the Malvinas Plate into alignment with their conjugates on the African Plate, and (3) errors in the 33o-28y South America-Africa stage rotation cannot account for the misalignment. We present improved Malvinas-Africa finite rotations determined by interpreting magnetic anomaly data in light of fracture zones and extinct spreading rift segments (the Agulhas rift) that are clearly revealed in satellite-derived marine gravity fields covering the Agulhas Basin. The tectonic history of the Malvinas Plate is chronicled through gravity field reconstructions that use the improved Malvinas-Africa finite rotations and more recent South America-Africa and Antarctica-Africa finite rotations. Newly-mapped triple junction traces on the Antarctic, South American, Malvinas, and African Plates, combined with geometric and magnetic constraints observed in the reconstructions, enable us to investigate the locations of the elusive western and southern boundaries of the Malvinas Plate.",
        "doi": "10.1023/A:1014638325616",
        "issn": "0025-3235",
        "publisher": "Springer Verlag",
        "publication": "Marine Geophysical Researches",
        "publication_date": "2001-07",
        "series_number": "4",
        "volume": "22",
        "issue": "4",
        "pages": "289-302"
    },
    {
        "id": "authors:sdmh5-t5072",
        "collection": "authors",
        "collection_id": "sdmh5-t5072",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-110426833",
        "type": "article",
        "title": "Rapid localization of Pacific\u2013North America plate motion in the Gulf of California",
        "author": [
            {
                "family_name": "Oskin",
                "given_name": "Michael",
                "orcid": "0000-0002-6631-5326",
                "clpid": "Oskin-M-E"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Mart\u00edn-Barajas",
                "given_name": "Arturo",
                "clpid": "Mart\u00edn-Barajas-A"
            }
        ],
        "abstract": "Correlation of late Miocene volcaniclastic strata across the northern Gulf of California shows that the Pacific\u2013North America plate boundary localized east of the Baja California peninsula ca. 6 Ma. Dextral offset of the 12.6 Ma Tuff of San Felipe and a pair of overlying ca. 6.3 Ma pyroclastic flows indicate at least 255 \u00b1 10 km of displacement along an azimuth of 310\u00b0. Isopach and facies trends of the Tuff of San Felipe support no more than a few tens of kilometers of additional dextral displacement between 12.6 and 6.3 Ma. These constraints indicate that nearly all of the dextral displacement between the Pacific and North American plates prior to 6.3 Ma was accommodated outside of the gulf region, and by 4.7 Ma, the plate boundary motion was localized in the Gulf of California. Although continental extension has accounted for a component of plate boundary motion in northwestern Mexico since cessation of subduction offshore of southern Baja California at 12.5 Ma, transfer of Baja California to the Pacific plate was delayed by at least 6\u20137 m.y.",
        "doi": "10.1130/0091-7613(2001)029<0459:RLOPNA>2.0.CO;2",
        "issn": "0091-7613",
        "publisher": "Geological Society of America",
        "publication": "Geology",
        "publication_date": "2001-05",
        "series_number": "5",
        "volume": "29",
        "issue": "5",
        "pages": "459-462"
    },
    {
        "id": "authors:a3p8m-yvd13",
        "collection": "authors",
        "collection_id": "a3p8m-yvd13",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-125536360",
        "type": "article",
        "title": "Structural controls on the continent-ocean transition in the northern Gulf of California",
        "author": [
            {
                "family_name": "Nagy",
                "given_name": "Elizabeth A.",
                "clpid": "Nagy-E-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "In the Gulf of California the Pacific-North America plate boundary changes character from an oceanic-type spreading center and transform fault system (to the south) to a region of diffuse continental deformation (to the north). The presence of spreading centers commonly inferred in the northernmost gulf is not supported by bathymetric, heat flow, gravity, or seismic data which indicate significant differences north and south of latitude \u223c30\u00b0N. We suggest instead that north of \u223c30\u00b0N a continent-ocean transition begins which we name the Wagner Transition Zone (WTZ). Diffuse deformation characterizes the WTZ where slip occurs along reactivated north to NNW striking normal faults developed during late Miocene or Pliocene ENE directed extension. Transtensional deformation varies from ENE directed extension along dip-slip faults in the west to dextral shear along the coast to dextral-oblique slip along inferred north to NNW striking faults submerged in the northern gulf. By accounting for rotational and extensional plate motion deformation in northeastern Baja California, vector constraints require that submerged structures accommodate \u223c30 mm/yr of slip in a direction slightly clockwise of the relative plate motion direction. The juxtaposition of the discrete spreading center system in the central gulf with the diffuse WTZ appears to have been a stable configuration since 4\u20136 Ma, perhaps controlling the evolution of spreading center jumps between Upper and Lower Tibur\u00f3n and Delfin basins due to the juxtaposition of kinematically partitioned structural domains. Different histories of prerift extension and subduction-related arc magmatism along the length of the gulf, partly related to the migration of the Rivera triple junction, may explain the location of the continent-ocean transition.",
        "doi": "10.1029/1999JB900402",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "2000-07-10",
        "series_number": "B7",
        "volume": "105",
        "issue": "B7",
        "pages": "16251-16269"
    },
    {
        "id": "authors:nnh4h-g1h25",
        "collection": "authors",
        "collection_id": "nnh4h-g1h25",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-140339355",
        "type": "article",
        "title": "Morphology and origin of the Osbourn Trough",
        "author": [
            {
                "family_name": "Billen",
                "given_name": "Magali I.",
                "orcid": "0000-0002-7316-1791",
                "clpid": "Billen-M-I"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The Osbourn Trough is a 900 km long, east-west trending gravity low, visible in satellite altimetry data, which intersects the Tonga Trench at 25\u00b030\u2032S. A recent survey collected gravity, magnetic, echo sounder, and swath bathymetry data on three adjacent, north-south trending ship tracks centered on the trough. The linear gravity low is 20\u201330 mGal less than the regional value and is accompanied by a flat-lying, 200\u2013500 m deep sediment-filled valley. Swath bathymetry images reveal several parallel, east-west trending linear ridges and valleys on either side of the main trough as well as other morphologic features characteristic of relict spreading centers, including a prominent inside corner high and possible pseudo-fault trace. The presence of magnetic anomalies (possibly anomalies 33 and 32) suggests that the seafloor here was formed after the end of the Cretaceous Normal Superchron (anomaly 34). These data support the conclusion that this trough is a spreading center, which stopped spreading in Late Cretaceous time. The existence of this feature has important implications for tectonic reconstructions in this region. The Osbourn Trough could be part of the fossil spreading center between the Pacific Plate and a fragment of the Phoenix Plate, the Bellingshausen Plate. This would require the seafloor between the Osbourn Trough and the Chatham Rise to the south to be a remnant fragment of the Bellingshausen Plate. This remnant may have joined to the Pacific Plate when the Hikurangi Plateau entered the Gondwana subduction zone at the Chatham Rise possibly causing the cessation of spreading on the Osbourn Trough.",
        "doi": "10.1029/2000JB900035",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "2000-06-10",
        "series_number": "B6",
        "volume": "105",
        "issue": "B6",
        "pages": "13481-13489"
    },
    {
        "id": "authors:k7dm6-e6c07",
        "collection": "authors",
        "collection_id": "k7dm6-e6c07",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140417-091012374",
        "type": "article",
        "title": "An age constraint on Gulf of California rifting from the Santa Rosal\u00eda basin, Baja California Sur, Mexico",
        "author": [
            {
                "family_name": "Holt",
                "given_name": "John W.",
                "clpid": "Holt-J-W"
            },
            {
                "family_name": "Holt",
                "given_name": "Elizabeth W.",
                "clpid": "Holt-E-W"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Marine rocks of the Santa Rosal\u00eda basin, Baja California Sur, were sampled in a pilot study to determine their suitability for magnetostratigraphy and geochronology with the goal of providing an age constraint on Gulf of California rifting. Progressive demagnetization of samples from the Boleo Formation, the earliest marine sequence overlying the deeply eroded basement, reveals a high-coercivity characteristic remanent magnetization (ChRM) in addition to a low-coercivity overprint. The ChRM appears to be a primary magnetic remanence with stratigraphically bound normal- and reversed-polarity directions. A single ^(40)Ar/^(39)Ar isotopic age of 6.76 \u00b1 0.90 Ma (2\u03c3) was obtained for the cinta colorada, a tephra deposit of reversed paleomagnetic polarity within the Boleo Formation. The age of the cinta colorada is refined by calculating isotopic age probabilities for each of the reversed-polarity intervals of the geomagnetic polarity time scale (GPTS) in the \u00b12\u03c3 range 5.86\u20137.66 Ma. The interval with the highest probability is 6.57\u20136.94 Ma. In conjunction with the isotopic age, preliminary magnetostratigraphy of the Boleo Formation is correlated with the GPTS in order to further delineate the onset of marine sedimentation. The most likely correlation yields an age of 6.93\u20137.09 Ma (GPTS subchron C3Bn) for the base of the Boleo Formation and 6.14\u20136.27 Ma for the top. This correlation, indicating an average sedimentation rate of 28 \u00b1 4 cm/k.y., could be significantly altered if a more thorough magnetostratigraphy proved the existence of additional polarity intervals in the Boleo Formation. However, even if the isotopic age of the cinta colorada is used as the only age constraint, the result is consistent with data from the northern Gulf of California and shows that rifting started much earlier than the ca. 3.6 Ma commencement of sea-floor spreading at the mouth of the Gulf of California. The deposition of the Boleo Formation was probably related to an early phase of gulf rifting caused by a change in Pacific\u2013North American plate motions.",
        "doi": "10.1130/0016-7606(2000)112<0540:AACOGO>2.3.CO;2",
        "issn": "0016-7606",
        "publisher": "Geological Society of America",
        "publication": "Geological Society of America Bulletin",
        "publication_date": "2000-04",
        "series_number": "4",
        "volume": "112",
        "issue": "4",
        "pages": "540-549"
    },
    {
        "id": "authors:h4ksa-ej836",
        "collection": "authors",
        "collection_id": "h4ksa-ej836",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20170427-105445312",
        "type": "article",
        "title": "Introduction to special issue: \"The influence of plate interaction on post-Laramide magmatism and tectonics in Mexico\"",
        "author": [
            {
                "family_name": "Ferrari",
                "given_name": "Luca",
                "clpid": "Ferrari-L"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Fucugauchi",
                "given_name": "Jaime Urrutia",
                "clpid": "Fucugauchi-J-U"
            }
        ],
        "abstract": "Among convergent margins, Mexico is an excellent site for studying along-strike variation in plate tectonics at the trench and its effect on the accompanying volcanism and tectonics in the overriding plate. The progressive fragmentation and consumption of the Farallon plate and the interaction between the Pacific and North America plates during the Cenozoic produced some unique geologic features. These include the Sierra Madre Occidental, one of the largest silicic igneous provinces on Earth, and the Trans-Mexican Volcanic Belt, a complex continental volcanic arc underlain by two of the youngest slabs in the world. In addition, extension occurred concurrently in much of the region affected by volcanism, producing a significant part of the southern Basin and Range province, and the reactivation of older basement structures which controlled the emplacement of volcanism.",
        "doi": "10.1016/S0040-1951(99)00303-0",
        "issn": "0040-1951",
        "publisher": "Elsevier",
        "publication": "Tectonophysics",
        "publication_date": "2000-03-10",
        "series_number": "1-4",
        "volume": "318",
        "issue": "1-4",
        "pages": "vii-ix"
    },
    {
        "id": "authors:nxhm2-tg655",
        "collection": "authors",
        "collection_id": "nxhm2-tg655",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-074414969",
        "type": "article",
        "title": "Cenozoic motion between East and West Antarctica",
        "author": [
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "M\u00fcller",
                "given_name": "R. Dietmar",
                "orcid": "0000-0002-3334-5764",
                "clpid": "M\u00fcller-R-D"
            },
            {
                "family_name": "Ishihara",
                "given_name": "Takemi",
                "clpid": "Ishihara-Takemi"
            }
        ],
        "abstract": "The West Antarctic rift system is the result of late Mesozoic and Cenozoic extension between East and West Antarctica, and represents one of the largest active continental rift systems on Earth. But the timing and magnitude of the plate motions leading to the development of this rift system remain poorly known, because of a lack of magnetic anomaly and fracture zone constraints on seafloor spreading. Here we report on magnetic data, gravity data and swath bathymetry collected in several areas of the south Tasman Sea and northern Ross Sea. These results enable us to calculate mid-Cenozoic rotation parameters for East and West Antarctica. These rotations show that there was roughly 180 km of separation in the western Ross Sea embayment in Eocene and Oligocene time. This episode of extension provides a tectonic setting for several significant Cenozoic tectonic events in the Ross Sea embayment including the uplift of the Transantarctic Mountains and the deposition of large thicknesses of Oligocene sediments. Inclusion of this East\u2013West Antarctic motion in the plate circuit linking the Australia, Antarctic and Pacific plates removes a puzzling gap between the Lord Howe rise and Campbell plateau found in previous early Tertiary reconstructions of the New Zealand region. Determination of this East\u2013West Antarctic motion also resolves a long standing controversy regarding the contribution of deformation in this region to the global plate circuit linking the Pacific to the rest of the world.",
        "doi": "10.1038/35004501",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "2000-03-09",
        "series_number": "6774",
        "volume": "404",
        "issue": "6774",
        "pages": "145-150"
    },
    {
        "id": "authors:srsez-7hp03",
        "collection": "authors",
        "collection_id": "srsez-7hp03",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-073556126",
        "type": "article",
        "title": "The Tuff of San Felipe: an extensive middle Miocene pyroclastic flow deposit in Baja California, Mexico",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Lewis",
                "given_name": "Claudia J.",
                "clpid": "Lewis-C-J"
            },
            {
                "family_name": "Nagy",
                "given_name": "Elizabeth A.",
                "clpid": "Nagy-E-A"
            }
        ],
        "abstract": "We document the existence of a widespread Miocene ash-flow tuff sheet in northeastern Baja California, Mexico. The Tuff of San Felipe (new name) was erupted from a vent east of the Sierra San Felipe of NE Baja California at ca. 12.6 Ma. This is the only widespread middle Miocene pyroclastic flow deposit identified in northeastern Baja California. Its distinctive age and widespread distribution make it an important marker horizon for structural reconstruction of this part of the Gulf Extensional Province, which is on the Pacific plate. The vent position, near the modern Gulf of California coast, allows the possibility that exposures of the Tuff of San Felipe may be preserved east of the Gulf on the North America plate in Sonora, yielding a tie point for the past relative position of the two plates. This paper summarizes all known information including petrography, geochemistry, geochronology, paleomagnetics, geographic distribution, and field appearance of this important tuff. It is a densely welded, crystal-rich, lithic-lapilli pyroclastic flow deposit, with 5\u201315% alkali feldspar, and can be 180 m thick in some locations near the vent. The Tuff of San Felipe is &gt;40 m thick up to 40 km SW of the vent and &gt;10 m thick at least 25 km NNW of the vent. A minimum volume estimate for the deposit is 54 km^3. Some recent ^(40)Ar/^(39)Ar age determinations suggest that the tuff is about 12.6 Ma in age. In all locations studied, the Tuff of San Felipe has a unique, low-inclination, reversed magnetization, which may record a field transition or a geomagnetic excursion within reversed polarity subchron C5Ar.2r (12.401 to 12.678 Ma). This low-inclination magnetization, as well as the mineralogy and age, is key to correlating the tuff across the region, because deposits are highly disrupted by subsequent normal faulting and outcrops are sparse and discontinuous away from the vent. The documentation of these characteristics is important because the Tuff of San Felipe is a key structural marker for the subsequent development of the Pacific\u2013North America plate boundary in the Gulf of California, and it will be important to identify this tuff in outcrops elsewhere on the Baja California Peninsula and on the North America plate in Sonora.",
        "doi": "10.1016/S0377-0273(99)00079-7",
        "issn": "0377-0273",
        "publisher": "Elsevier",
        "publication": "Journal of Volcanology and Geothermal Research",
        "publication_date": "1999-11-15",
        "series_number": "1-2",
        "volume": "93",
        "issue": "1-2",
        "pages": "53-74"
    },
    {
        "id": "authors:3zwtm-7cs09",
        "collection": "authors",
        "collection_id": "3zwtm-7cs09",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-080523933",
        "type": "article",
        "title": "Age and stratigraphic relationships of pre- and syn-rift volcanic deposits in the northern Puertecitos Volcanic Province, Baja California, Mexico",
        "author": [
            {
                "family_name": "Nagy",
                "given_name": "Elizabeth A.",
                "clpid": "Nagy-E-A"
            },
            {
                "family_name": "Grove",
                "given_name": "Marty",
                "clpid": "Grove-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Geologic mapping of volcanic strata of the northern Puertecitos Volcanic Province (PVP) in northeastern Baja California, Mexico, performed in conjunction with ^(40)Ar/^(39)Ar analysis and petrochemical study, documents the Miocene geologic history of a well-preserved volcanic succession within the northern Sierra Santa Isabel and its relationship to the evolving Pacific\u2013North America plate boundary. Subduction-related volcanic deposits, well-exposed in profile along the northern margin of the PVP in the informally named Santa Isabel Wash region, span pre-17 to 15 Ma. Minor rift-related volcanism occurred at \u223c12.5 and \u223c9 Ma, prior to voluminous PVP-forming volcanism at \u223c6\u20136.5 Ma. Isochron ages typically exhibit precision (1\u03c3) for plagioclase of \u00b12\u20137% and for anorthoclase and sanidine of \u00b12\u20135%, and replicate analysis of an internal anorthoclase standard indicate \u223c1\u20132% reproducibility within a given irradiation and \u223c2.5% for samples irradiated separately. Improved local correlations made possible by the rich stratigraphic section preserved in Santa Isabel Wash help constrain the relationships of several widespread pyroclastic flow deposits in northeastern Baja California. These correlations are important for both paleomagnetic studies within the region and for establishing geologic ties across the Gulf of California. The combined mapping and age results imply that most extensional deformation in the study area is post-6 Ma, although some earlier faulting and the development of the pre-6 Ma Matom\u0131\u0301 accommodation zone are also documented. Results support a transitional plate boundary model which implies that much of the Pacific\u2013North America relative plate motion north of Delf\u0131\u0301n basin (i.e., the northernmost Gulf of California) is accommodated on N- to NNW-striking faults developed during Late Miocene ENE-directed extension. The model predicts a zone of divergence east of the PVP which provides a structural mechanism for the positions and jumps of nearby Gulf of California spreading centers (Upper and Lower Tibur\u00f3n and Delf\u0131\u0301n basins) since 6 Ma, and relates major pulses of PVP volcanism at \u223c6 and \u223c3 Ma to these offshore spreading center adjustments. Results also imply that most extensional deformation in Santa Isabel Wash is the result of incorporation of the PVP into the Gulf Extensional Province \u223c2\u20133 Ma due to northwestward propagation of the Guaymas fracture zone. Rotational deformation north of the PVP may have begun contemporaneously with this adjustment along the Gulf Extensional Province rift margin.",
        "doi": "10.1016/S0377-0273(99)00080-3",
        "issn": "0377-0273",
        "publisher": "Elsevier",
        "publication": "Journal of Volcanology and Geothermal Research",
        "publication_date": "1999-11-15",
        "series_number": "1-2",
        "volume": "93",
        "issue": "1-2",
        "pages": "1-30"
    },
    {
        "id": "authors:7g7sf-n9e77",
        "collection": "authors",
        "collection_id": "7g7sf-n9e77",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20121016-104022644",
        "type": "article",
        "title": "Constraints on the proposed Marie Byrd Land-Bellingshausen Plate Boundary from seismic reflection data",
        "author": [
            {
                "family_name": "Heinemann",
                "given_name": "J.",
                "clpid": "Heinemann-J"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Clayton",
                "given_name": "R. W.",
                "orcid": "0000-0003-3323-3508",
                "clpid": "Clayton-R-W"
            },
            {
                "family_name": "Hafner",
                "given_name": "K.",
                "clpid": "Hafner-K"
            },
            {
                "family_name": "Cande",
                "given_name": "S.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Raymond",
                "given_name": "C.",
                "orcid": "0000-0002-4213-8097",
                "clpid": "Raymond-Carol-A"
            }
        ],
        "abstract": "Single-channel and multichannel marine seismic data off the coast of West Antarctica collected during two Nathaniel B. Palmer cruises (NP92-8 and NP96-2) in the vicinity of 65\u00b0S to 71\u00b0S, 220\u00b0E to 250\u00b0E, reveal a NNW trending graben. We interpret this graben to be part of the paleodivergent plate boundary between the Marie Byrd Land and Bellingshausen plates. This graben coincides with a \u2212520 nT magnetic anomaly to the NNW and a \u2212720 nT anomaly to the SSE, as well as a 20 mGal negative gravity anomaly. Seismic profiles subparallel to the graben (22 km/Ma half-spreading rate) reveal greater seafloor roughness to the NE, where seafloor spreading was slower, than to the SW (27 km/Ma half-spreading rate). These data allow the position of the Marie Byrd Land-Bellingshausen plate boundary to be constrained more precisely than has previously been possible, with a trend of N17\u00b0W from 68.52\u00b0S, 233.65\u00b0E to 68.41\u00b0S, 233.56\u00b0E. The sediment-filled graben has normal separation of sedimentary layers varying from 740\u00b130 m to 580\u00b120 m imaged in seafloor of age A33y (74 Ma).",
        "doi": "10.1029/1998JB900079",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1999-11-10",
        "series_number": "B11",
        "volume": "104",
        "issue": "B11",
        "pages": "25321-25330"
    },
    {
        "id": "authors:cvjj2-fky62",
        "collection": "authors",
        "collection_id": "cvjj2-fky62",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-124308456",
        "type": "article",
        "title": "Evolution of the Australian-Antarctic discordance since Miocene time",
        "author": [
            {
                "family_name": "Marks",
                "given_name": "Karen M.",
                "clpid": "Marks-K-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Quinn",
                "given_name": "Katherine J.",
                "clpid": "Quinn-K-J"
            }
        ],
        "abstract": "In this study we chronicle the development of the Australian-Antarctic discordance (AAD), the crenelated portion of the Southeast Indian Ridge between \u223c120\u00b0 and 128\u00b0E, since anomaly 6y time (19 Ma). We reconstruct satellite-derived marine gravity fields and depth anomalies at selected times by first removing anomalies overlying seafloor younger than the selected age, and then rotating the remaining anomalies through improved finite rotations based on a very detailed set of magnetic anomaly identifications. Our gravity field reconstructions reveal that the overall length of the Australian-Antarctic plate boundary within the AAD has been increasing since 19 Ma. Concomitantly, the number of propagating rifts and fracture zones in the vicinity of the discordance has increased dramatically in recent times, effectively dividing it into its present-day configuration of five distinct spreading corridors (B1-B5) that are offset alternately to the north and south and exhibit varying degrees of asymmetric spreading. Our bathymetric reconstructions show that the regional, arcuate-shaped, negative depth anomaly (deeper than predicted by normal lithospheric cooling models) presently centered on the discordance began migrating westward before anomaly 5ad time (\u223c14.4 Ma), and that a localized depth anomaly low, which at time 5ad lay on the ridge axis in spreading corridor B5, has been split apart by subsequent seafloor spreading. The magnetic anomaly patterns suggest that the depth anomaly is not always associated with a particularly contorted plate boundary geometry. Although the plate boundary within the AAD has been getting progressively more crenelated with time, this effect shows little to no migration along the ridge axis since 19 Ma. Thus any geodynamic models of the evolution of the discordance must account for the following observations: (1) the crenelation of the plate boundary within the AAD has increased with time, (2) the center of the crenelated zone does not appear to have migrated along the ridge crest, and (3) both the depth anomaly and the isotopic boundary between Pacific and Indian mantle have been migrating westward along the ridge axis but at apparently different rates. We suggest that both along-axis migration of the depth anomaly and isotopic boundary, as well as temporal variation in the upwelling mantle material beneath the AAD, and local tectonic effects are required in order to explain these observations.",
        "doi": "10.1029/1998JB900075",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1999-03-10",
        "series_number": "B3",
        "volume": "104",
        "issue": "B3",
        "pages": "4967-4981"
    },
    {
        "id": "authors:xq7hc-91s55",
        "collection": "authors",
        "collection_id": "xq7hc-91s55",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-071657302",
        "type": "article",
        "title": "Late Miocene to Recent transtensional tectonics in the Sierra San Ferm\u00edn, northeastern Baja California, Mexico",
        "author": [
            {
                "family_name": "Lewis",
                "given_name": "Claudia J.",
                "clpid": "Lewis-C-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Basins and ranges within part of the Gulf of California Extensional Province (Mexico) have experienced complex distributed deformation, including normal and strike-slip faulting and block rotations, linked to dextral shear at the Pacific\u2013North America plate boundary. In the Sierra San Ferm\u0131\u0301n and southern Sierra San Felipe (northeastern Baja California), normal faulting began between 12.5 and 6 Ma, although most extension occurred between about 6 and 3 Ma, strongly influencing thickness and distribution of ash-flow tuffs and sedimentary deposits. Extension is generally &lt;10% in 6 Ma rocks and somewhat more in 12.5 Ma rocks. Inversion of kinematic data, interpreted together with published paleomagnetic data, suggests that the axis of least principal stress was oriented between W\u2013E and SW\u2013NE in late Miocene time. Our data indicate an important change in the amount of dextral shear, but not necessarily the least principal stress direction (WSW\u2013ENE), at about 3 Ma. Structural constraints limit significant sinistral strike-slip faulting, conjugate to the dextral plate boundary, to the last \u223c3 My. Progressive changes in the geometry of faulting through time are consistent with regional strain partitioning within the Pacific\u2013North America plate boundary zone, and are predicted by physical and analytical models of oblique divergence as the orientation of the stretching vector \u03b1 changes to lower and lower values.",
        "doi": "10.1016/S0191-8141(98)00038-8",
        "issn": "0191-8141",
        "publisher": "Elsevier",
        "publication": "Journal of Structural Geology",
        "publication_date": "1998-08",
        "series_number": "8",
        "volume": "20",
        "issue": "8",
        "pages": "1043-1063"
    },
    {
        "id": "authors:98v7x-79c44",
        "collection": "authors",
        "collection_id": "98v7x-79c44",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140923-145247866",
        "type": "article",
        "title": "The tectonic history of the Tasman Sea: A puzzle with 13 pieces",
        "author": [
            {
                "family_name": "Gaina",
                "given_name": "Carmen",
                "clpid": "Gaina-C"
            },
            {
                "family_name": "M\u00fcller",
                "given_name": "R. Dietmar",
                "orcid": "0000-0002-3334-5764",
                "clpid": "M\u00fcller-R-D"
            },
            {
                "family_name": "Royer",
                "given_name": "Jean-Yves",
                "clpid": "Royer-J-Y"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hardebeck",
                "given_name": "Jeanne",
                "clpid": "Hardebeck-J-L"
            },
            {
                "family_name": "Symonds",
                "given_name": "Phil",
                "clpid": "Symonds-P"
            }
        ],
        "abstract": "We present a new model for the tectonic evolution of the Tasman Sea based on dense satellite altimetry data and a new shipboard data set. We utilized a combined set of revised magnetic anomaly and fracture zone interpretations to calculate relative motions and their uncertainties between the Australian and the Lord Howe Rise plates from 73.6 Ma to 52 Ma when spreading ceased. From chron 31 (67.7 Ma) to chron 29 (64.0 Ma) the model implies, transpression between the Chesterfield and the Marion plateaus, followed by strike-slip motion. This transpression may have been responsible for the formation of the Capricorn Basin south of the Marion Plateau. Another major tectonic event took place at chron 27 (61.2 Ma), when a counterclockwise change in spreading direction occurred, contemporaneous with a similar event in the southwest Pacific Ocean. The early opening of the Tasman Sea cannot be modeled by a simple two-plate system because (1) rifting in this basin propagated from south to north in several stages and (2) several rifts failed. We identified 13 continental blocks which acted as microplates between 90 Ma and 64 Ma. Our model is constrained by tectonic lineaments visible in the gravity anomaly grid and interpreted as strike-slip faults, by magnetic anomaly, bathymetry and seismic data, and in case of the South Tasman Rise, by the age and affinity of dredged rocks. By combining all this information we derived finite rotations that describe the dispersal of these tectonic elements during the early opening of the Tasman Sea.",
        "doi": "10.1029/98JB00386",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1998-06-10",
        "series_number": "B6",
        "volume": "103",
        "issue": "B6",
        "pages": "12413-12433"
    },
    {
        "id": "authors:vmv4m-84g03",
        "collection": "authors",
        "collection_id": "vmv4m-84g03",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140902-135954936",
        "type": "article",
        "title": "Pacific-North America Plate Tectonics of the Neogene Southwestern United States: An Update",
        "author": [
            {
                "family_name": "Atwater",
                "given_name": "Tanya",
                "clpid": "Atwater-T"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We use updated rotations within the Pacific-Antarctica-Africa-North America plate circuit to calculate Pacific-North America plate reconstructions for times since chron 13 (33 Ma). The direction of motion of the Pacific plate relative to stable North America was fairly steady between chrons 13 and 4, and then changed and moved in a more northerly direction from chron 4 to the present (8 Ma to the present). No Pliocene changes in Pacific-North America plate motion are resolvable in these data, suggesting that Pliocene changes in deformation style along the boundary were not driven by changes in plate motion. However, the chron 4 change in Pacific-North America plate motion appears to correlate very closely to a change in direction of extension documented between the Sierra Nevada and the Colorado Plateau. Our best solution for the displacement with respect to stable North America of a point on the Pacific plate that is now near the Mendocino triple junction is that from 30 to 12 Ma the point was displaced along an azimuth of \u223cN60\u00b0W at rate of \u223c33 mm/yr; from 12 Ma to about 8 Ma the azimuth of displacement was about the same as previously, but the rate was faster (\u223c52 mm/yr); and since 8 Ma the point was displaced along an azimuth of N37\u00b0W at a rate of \u223c52 mm/yr.\n\nWe compare plate-circuit reconstructions of the edge of the Pacific plate to continental deformation reconstructions of North American tectonic elements across the Basin and Range province and elsewhere in order to evaluate the relationship of this deformation to the plate motions. The oceanic displacements correspond remarkably well to the continental reconstructions where deformations of the latter have been quantified along a path across the Colorado Plateau and central California. They also supply strong constraints for the deformation budgets of regions to the north and south, in Cascadia and northern Mexico, respectively.\n\nWe examine slab-window formation and evolution in a detailed re-analysis of the spreading geometry of the post-Farallon microplates, from 28 to 19 Ma. Development of the slab window seems linked to early Miocene volcanism and deformation in the Mojave Desert, although detailed correlations await clarification of early Miocene reconstructions of the Tehachapi Mountains. We then trace the post-20 Ma motion of the Mendocino slab window edge beneath the Sierran-Great Valley block and find that it drifted steadily north, then stalled just north of Sutter Buttes at \u223c4 Ma.",
        "doi": "10.1080/00206819809465216",
        "issn": "0020-6814",
        "publisher": "Taylor & Francis",
        "publication": "International Geology Review",
        "publication_date": "1998-05",
        "series_number": "5",
        "volume": "40",
        "issue": "5",
        "pages": "375-402"
    },
    {
        "id": "authors:jsjqs-p1257",
        "collection": "authors",
        "collection_id": "jsjqs-p1257",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-070221525",
        "type": "article",
        "title": "Pacific-North America Plate Tectonics of the Neogene\n Southwestern United States: An Update",
        "author": [
            {
                "family_name": "Atwater",
                "given_name": "Tanya",
                "clpid": "Atwater-T"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We use updated rotations within the Pacific-Antarctica-Africa-North America plate circuit to calculate Pacific-North America plate reconstructions for times since chron 13 (33 Ma). The direction of motion of the Pacific plate relative to stable North America was fairly steady between chrons 13 and 4, and then changed and moved in a more northerly direction from chron 4 to the present (8 Ma to the present). No Pliocene changes in Pacific-North America plate motion are resolvable in these data, suggesting that Pliocene changes in deformation style along the boundary were not driven by changes in plate motion. However, the chron 4 change in Pacific-North America plate motion appears to correlate very closely to a change in direction of extension documented between the Sierra Nevada and the Colorado Plateau. Our best solution for the displacement with respect to stable North America of a point on the Pacific plate that is now near the Mendocino triple junction is that from 30 to 12 Ma the point was displaced along an azimuth of \u223cN60\u00b0W at rate of \u223c33 mm/yr; from 12 Ma to about 8 Ma the azimuth of displacement was about the same as previously, but the rate was faster (\u223c52 mm/yr); and since 8 Ma the point was displaced along an azimuth of N37\u00b0W at a rate of \u223c52 mm/yr.\n\nWe compare plate-circuit reconstructions of the edge of the Pacific plate to continental deformation reconstructions of North American tectonic elements across the Basin and Range province and elsewhere in order to evaluate the relationship of this deformation to the plate motions. The oceanic displacements correspond remarkably well to the continental reconstructions where deformations of the latter have been quantified along a path across the Colorado Plateau and central California. They also supply strong constraints for the deformation budgets of regions to the north and south, in Cascadia and northern Mexico, respectively.\n\nWe examine slab-window formation and evolution in a detailed re-analysis of the spreading geometry of the post-Farallon microplates, from 28 to 19 Ma. Development of the slab window seems linked to early Miocene volcanism and deformation in the Mojave Desert, although detailed correlations await clarification of early Miocene reconstructions of the Tehachapi Mountains. We then trace the post-20 Ma motion of the Mendocino slab window edge beneath the Sierran-Great Valley block and find that it drifted steadily north, then stalled just north of Sutter Buttes at \u223c4 Ma.",
        "doi": "10.1080/00206819809465216",
        "issn": "0020-6814",
        "publisher": "Taylor & Francis",
        "publication": "International Geology Review",
        "publication_date": "1998-05",
        "series_number": "5",
        "volume": "40",
        "issue": "5",
        "pages": "375-402"
    },
    {
        "id": "authors:cthjx-9ex61",
        "collection": "authors",
        "collection_id": "cthjx-9ex61",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141028-074046308",
        "type": "article",
        "title": "New Constraints on Plate Tectonic Puzzle of the SW Pacific",
        "author": [
            {
                "family_name": "Cande",
                "given_name": "S. C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Raymond",
                "given_name": "C.",
                "orcid": "0000-0002-4213-8097",
                "clpid": "Raymond-Carol-A"
            },
            {
                "family_name": "M\u00fcller",
                "given_name": "R. D.",
                "orcid": "0000-0002-3334-5764",
                "clpid": "M\u00fcller-R-D"
            }
        ],
        "abstract": "A long-standing problem in the tectonics of the southwest Pacific has been the lack of closure of the plate circuit linking the Antarctic, Australia, Lord Howe Rise, and Pacific plates in late Cretaceous and early Tertiary time [Molnar et al., 1975]. Avoiding unacceptable overlaps and underlaps in reconstructions of these plates requires invoking relative motion on one or more nebulous plate boundaries somewhere along the plate circuit, such as between East and West Antarctica, within West Antarctica [Stock and Molnar, 1987], or perhaps between the Lord Howe Rise and Challenger Plateau in the Tasman Sea [Lawver and Gahagan, 1994]. This problem is of more than mere local interest since the motion of the Pacific plate relative to the rest of the globe is constrained through its connection with West Antarctica.",
        "doi": "10.1029/98EO00053",
        "issn": "0096-3941",
        "publisher": "American Geophysical Union",
        "publication": "Eos",
        "publication_date": "1998-02-17",
        "series_number": "7",
        "volume": "79",
        "issue": "7",
        "pages": "81-82"
    },
    {
        "id": "authors:k55bk-9ww59",
        "collection": "authors",
        "collection_id": "k55bk-9ww59",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-123711983",
        "type": "article",
        "title": "Paleomagnetic evidence of localized vertical axis rotation during Neogene extension, Sierra San Ferm\u00edn, northeastern Baja California, Mexico",
        "author": [
            {
                "family_name": "Lewis",
                "given_name": "Claudia J.",
                "clpid": "Lewis-C-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Paleomagnetic data from Sierra San Ferm\u00edn in the Gulf of California Extensional Province indicate that localized clockwise rotations about vertical axes occurred during Pliocene through Recent extension and dextral shear. Relative declination discordances in upper Miocene and Pliocene ash flow tuffs indicate a net clockwise rotation of 30\u00b0 \u00b1 16\u00b0. Clockwise rotation between 12.5 and 6 Ma is statistically insignificant (11\u00b0 \u00b1 17\u00b0). Structural observations and geochronological data suggest that rotations in this area began post-6 Ma, comprising uniform-sense block rotations (oblique divergence) associated with extension and dextral slip in the northwest striking boundary between the Pacific and North American plates. Northeast striking sinistral-slip faults and north striking normal faults accommodate distributed dextral shear in this area, allowing fault blocks to rotate in a clockwise sense. A model for oblique divergence predicts \u223c21 km of shear in the direction of relative plate motion and \u223c20% (\u223c7 km) ENE directed extension, perpendicular to the Main Gulf Escarpment. A broad region of northeastern Baja California may have undergone similar distributed shear. Two possible dynamic models may explain this shear. In one model, rotation accumulates above a deep, subhorizontal, basal shear zone. Rotating blocks may extend downward to a detachment beneath the extensional province, either a low-angle eastward continuation of the San Pedro M\u00e1rtir fault or to a basal shear surface on top of a subducted remnant of the Farallon plate. Alternatively, distributed dextral shear may be the surface manifestation of a deep vertical shear zone linking transform faults in the northern gulf with dextral transpeninsular faults. In either case, shear may have transferred northward onto faults west of the San Andreas fault, contributing to late Miocene to Recent clockwise rotation of the Western Transverse Ranges. This shear is not accounted for in the 300 km of dextral slip computed from cross-gulf geologic tie points.",
        "doi": "10.1029/97JB02673",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1998-02-10",
        "series_number": "B2",
        "volume": "103",
        "issue": "B2",
        "pages": "2455-2470"
    },
    {
        "id": "authors:d2md1-bgz59",
        "collection": "authors",
        "collection_id": "d2md1-bgz59",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140411-144331262",
        "type": "article",
        "title": "Early Tertiary gravity field reconstructions of the Southwest Pacific",
        "author": [
            {
                "family_name": "Marks",
                "given_name": "K. M.",
                "clpid": "Marks-K-M"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The aim of our study is to chronicle the development of plate boundaries in the Southwest Pacific Ocean during the early Tertiary. This region has been the subject of numerous and often conflicting studies that have attempted to construct the history of plate motion and plate boundary evolution as the Australia and Pacific plates separated from Antarctica. Our novel approach entails reconstructing gravity fields from satellite altimeter gravity by first removing anomalies overlying seafloor younger than a selected age, and then rotating the remaining anomalies through appropriate finite rotations. Our reconstructions reveal: (1) an extensional plate boundary (the Iselin rift) existed between West and East Antarctica prior to A24 time; (2) the arrival of the Southeast Indian ridge (SEIR) at the Tasman ridge (prior to A24) led to the extinction of the Iselin rift as well as the conversion of the easternmost portion of the Tasman plate boundary (between the SEIR and the Iselin rift) into a transform fault on the Pacific\u2013Antarctic ridge; and (3) an early (A24 or younger) inception of the Australia\u2013Pacific plate boundary. Our scenario for the opening of the Southwest Pacific Ocean can explain the present-day gravity anomalies and magnetic isochrons observed in the northwest Ross Sea. We find that the East Antarctic seafloor northeast of the Iselin Bank was generated by spreading on the Tasman ridge prior to A24 time.",
        "doi": "10.1016/S0012-821X(97)00139-8",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "1997-11",
        "series_number": "1-4",
        "volume": "152",
        "issue": "1-4",
        "pages": "267-274"
    },
    {
        "id": "authors:86tj7-j8z81",
        "collection": "authors",
        "collection_id": "86tj7-j8z81",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-112237965",
        "type": "article",
        "title": "Using borehole breakouts to constrain the complete stress tensor: Results from the Sijan Deep Drilling Project and offshore Santa Maria Basin, California",
        "author": [
            {
                "family_name": "Zajac",
                "given_name": "Blair J.",
                "clpid": "Zajac-B-J"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We use borehole breakouts in nonvertical drill holes to constrain the directions of the three principal stresses and their relative magnitudes. In this paper we start by modifying previously published breakout selection criteria to work with highly deviated borehole data. We present a forward modeling technique using genetic algorithms and a nongradient N-dimensional optimizer to find the best fitting stress state for a set of breakout data. The stress state is parameterized by three Euler angles and the stress state ratio \u00f8. A technique is developed to determine the 95% confidence weighted misfit between a model and the data. We then map out the 95% misfit confidence limits on the best fitting stress state. This technique is applied to data published by Qian and Pedersen [1991]. Removing their constraint of a vertical principal stress direction reduces the misfit between the stress state and the breakout data. We find that the best fitting stress state they report with a vertical principal stress direction lies outside our 95% confidence limits. We also invert breakouts in the offshore Santa Maria Basin, California. These data show a \"thrust faulting\" stress state with the maximum principal stress,\nS_1, at N148.5\u00b0E plunging 31.5\u00b0. The 95% confidence range for the azimuth of S_1 ranges from N143.0\u00b0E to N198.1\u00b0E. The stress ratio \u00f8 was found to be 0.82l^1_(0.584).",
        "doi": "10.1029/96JB03914",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1997-05-10",
        "series_number": "B5",
        "volume": "102",
        "issue": "B5",
        "pages": "10083-10100"
    },
    {
        "id": "authors:79mjr-y5w53",
        "collection": "authors",
        "collection_id": "79mjr-y5w53",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-135006071",
        "type": "article",
        "title": "The geodetic signature of the M8.0 Oct. 9, 1995, Jalisco subduction earthquake",
        "author": [
            {
                "family_name": "Melbourne",
                "given_name": "T.",
                "orcid": "0000-0003-1870-3962",
                "clpid": "Melbourne-Timothy-I"
            },
            {
                "family_name": "Carmichael",
                "given_name": "I.",
                "clpid": "Carmichael-Ian-S-E"
            },
            {
                "family_name": "DeMets",
                "given_name": "C.",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "Hudnut",
                "given_name": "K.",
                "orcid": "0000-0002-3168-4797",
                "clpid": "Hudnut-Kenneth-W"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "clpid": "S\u00e1nchez-Osvaldo"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Su\u00e1rez",
                "given_name": "G.",
                "orcid": "0000-0002-2011-4924",
                "clpid": "Su\u00e1rez-Genaro"
            },
            {
                "family_name": "Webb",
                "given_name": "F.",
                "clpid": "Webb-Frank-H"
            }
        ],
        "abstract": "The October, 1995 Mw 8.0 Jalisco subduction earthquake has provided a thorough geodetic observation of the coseismic subduction process. An 11 station regional GPS network located directly onshore of the rupture demonstrates consistent vertical subsidence verified by tide gauge data and southwest-directed extension, with measured displacements reaching 1 meter. Unusually shallow and non-uniform faulting is required to explain the displacements. We determine that up to 5 meters of slip occurred within the upper 15 km of the thrust fault zone and 2 meters possibly as shallow as 8 km, and that slip was likely distributed in two main patches. The paucity of continental sediments in this subduction zone could be responsible for the anomalously shallow faulting.",
        "doi": "10.1029/97GL00370",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "1997-03-15",
        "series_number": "6",
        "volume": "24",
        "issue": "6",
        "pages": "715-718"
    },
    {
        "id": "authors:2be3a-q1e49",
        "collection": "authors",
        "collection_id": "2be3a-q1e49",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140415-093934915",
        "type": "article",
        "title": "Compression directions in southern California (from Santa Barbara to Los Angeles Basin) obtained from borehole breakouts",
        "author": [
            {
                "family_name": "Wilde",
                "given_name": "Melita",
                "clpid": "Wilde-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Borehole elongation in 71 drill holes was used to infer breakout orientation and directions of maximum horizontal principal stress S_H for six areas west of the San Andreas fault in southern California: Santa Barbara, Ojai, Central Ventura Basin, East Ventura Basin, West Los Angeles Basin, and East Los Angeles Basin. Breakouts were determined from analysis of oriented four-arm caliper data. The breakouts form at the position of the maximum compressive stress on the borehole wall; if the borehole is vertical and parallel to one of the principal stress directions, the breakouts will form parallel to the minimum horizontal principal stress S_h orthogonal to the maximum horizontal principal stress S_H. Observations from deviated boreholes permit some constraints on the relative magnitudes of the principal stresses. In most cases the data permit either a thrust faulting (S_v",
        "doi": "10.1029/96JB03734",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1997-03-10",
        "series_number": "B3",
        "volume": "102",
        "issue": "B3",
        "pages": "4969-4983"
    },
    {
        "id": "authors:3gw4y-aqn27",
        "collection": "authors",
        "collection_id": "3gw4y-aqn27",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141021-153139625",
        "type": "article",
        "title": "Geophysical Secrets Beneath Antarctic Waters",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Cruising around Antarctica is a perk that a group of us from Caltech have\nenjoyed over the past few years. You might be curious about how we book\none of these cruises. First of all, we write a proposal and send it to the National\nScience Foundation, which has an Office of Polar Programs and an\nOffice of Marine Geology and Geophysics. If the proposal is approved, we're\nscheduled for time on board one of the NSF ships. We had proposed several\nprojects to answer some nagging place-tectonic questions about the history\nand evolution of the Antarctica place, which may hold the key to understanding\nmovement of some of the other plates and ocher global geophysical\nproblems, such as relative motions among the hot Spots.",
        "issn": "0013-7812",
        "publisher": "California Institute of Technology",
        "publication": "Engineering and Science",
        "publication_date": "1997",
        "series_number": "3",
        "volume": "60",
        "issue": "3",
        "pages": "18-27"
    },
    {
        "id": "authors:zszqz-qd356",
        "collection": "authors",
        "collection_id": "zszqz-qd356",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-132129630",
        "type": "article",
        "title": "Compression directions north of the San Fernando Valley determined from borehole breakouts",
        "author": [
            {
                "family_name": "Kerkela",
                "given_name": "Stacy",
                "clpid": "Kerkela-S"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Borehole breakouts in 4 nearly vertical oil wells, and several other deviated holes, in the San Fernando Valley and Santa Susana Mountains suggest a maximum horizontal compressive stress direction (S_H) of N49\u00b0W. These wells provide information about the stress field from 1974 to 1983 in the uppermost crust (&lt;3 km depth) near the aftershock zones of the January 1994 Northridge earthquake and the February 1971 Sylmar earthquake. This direction of S_H is anomalous with respect to the N to NNE directions of S_H seen in other regional data, but is consistent with the structural complexity of this zone, including local changes in strike of major thrust fault zones and the presence of lateral ramps in both the Santa Susana and San Fernando faults.",
        "doi": "10.1029/96GL03054",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "1996-11-15",
        "series_number": "23",
        "volume": "23",
        "issue": "23",
        "pages": "3365-3368"
    },
    {
        "id": "authors:td61j-ze307",
        "collection": "authors",
        "collection_id": "td61j-ze307",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140909-083626726",
        "type": "article",
        "title": "Geophysics of the Pitman Fracture Zone and Pacific-Antarctic Plate Motions During the Cenozoic",
        "author": [
            {
                "family_name": "Cande",
                "given_name": "Steven C.",
                "clpid": "Cande-S-C"
            },
            {
                "family_name": "Raymond",
                "given_name": "Carol A.",
                "orcid": "0000-0002-4213-8097",
                "clpid": "Raymond-Carol-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Haxby",
                "given_name": "W. F.",
                "clpid": "Haxby-W-F"
            }
        ],
        "abstract": "Multibeam bathymetry and magnetometer data from the Pitman fracture zone (FZ) permit construction of a plate motion history for the South Pacific over the past 65 million years. Reconstructions show that motion between the Antarctic and Bellingshausen plates was smaller than previously hypothesized and ended earlier, at chron C27 (61 million years ago). The fixed hot-spot hypothesis and published paleomagnetic data require additional motion elsewhere during the early Tertiary, either between East Antarctica and West Antarctica or between the North and South Pacific. A plate reorganization at chron C27 initiated the Pitman FZ and may have been responsible for the other right-stepping fracture zones along the ridge. An abrupt (8\u00b0) clockwise rotation in the abyssal hill fabric along the Pitman flowline near the young end of chron C3a (5.9 million years ago) dates the major change in Pacific-Antarctic relative motion in the late Neogene.",
        "doi": "10.1126/science.270.5238.947",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "1995-11-10",
        "series_number": "5238",
        "volume": "270",
        "issue": "5238",
        "pages": "947-953"
    },
    {
        "id": "authors:3rt4t-4f616",
        "collection": "authors",
        "collection_id": "3rt4t-4f616",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141028-071200804",
        "type": "article",
        "title": "Anticipating the Successor to Mexico's Largest Historical Earthquake",
        "author": [
            {
                "family_name": "DeMets",
                "given_name": "C.",
                "orcid": "0000-0001-7460-1165",
                "clpid": "DeMets-Charles"
            },
            {
                "family_name": "Carmichael",
                "given_name": "I.",
                "clpid": "Carmichael-Ian-S-E"
            },
            {
                "family_name": "Melbourne",
                "given_name": "T.",
                "orcid": "0000-0003-1870-3962",
                "clpid": "Melbourne-Timothy-I"
            },
            {
                "family_name": "S\u00e1nchez",
                "given_name": "O.",
                "clpid": "S\u00e1nchez-Osvaldo"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Su\u00e1rez",
                "given_name": "G.",
                "orcid": "0000-0002-2011-4924",
                "clpid": "Su\u00e1rez-Genaro"
            },
            {
                "family_name": "Hudnut",
                "given_name": "K.",
                "orcid": "0000-0002-3168-4797",
                "clpid": "Hudnut-Kenneth-W"
            }
        ],
        "abstract": "Note in proof: On October 9, as this article was being prepared for publication, a magnitude 7.6 earthquake occurred beneath the Jalisco region and caused significant loss of life and property. This earthquake highlights the societal need for accurate measurements of crustal strain rates in earthquake-prone zones. In the coming months, we plan to measure the amount of displacement that occurred within the GPS network during and after this earthquake.",
        "doi": "10.1029/95EO00255",
        "issn": "0096-3941",
        "publisher": "American Geophysical Union",
        "publication": "Eos",
        "publication_date": "1995-10-17",
        "series_number": "42",
        "volume": "76",
        "issue": "42",
        "pages": "417-424"
    },
    {
        "id": "authors:s7zq1-c2y61",
        "collection": "authors",
        "collection_id": "s7zq1-c2y61",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-114127033",
        "type": "article",
        "title": "Asymmetric Seafloor Spreading and Short Ridge Jumps in the Australian-Antarctic Discordance",
        "author": [
            {
                "family_name": "Marks",
                "given_name": "Karen M.",
                "clpid": "Marks-K-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The crenulated geometry of the Southeast Indian ridge within the Australian-Antarctic discordance is formed by numerous spreading ridge segments that are offset, alternately to the north and south, by transform faults. Suggested causes for these offsets, which largely developed since ~ 20 Ma, include asymmetric seafloor spreading, ridge jumps, and propagating rifts that have transferred seafloor from one flank of the spreading ridge to the other. Each of these processes has operated at different times in different locations of the discordance; here we document an instance where a small (~ 20 km), young (&lt; 0.2 Ma), southward ridge jump has contributed to the observed asymmetry. When aeromagnetic anomalies from the Project Investigator-1 survey are superposed on gravity anomalies computed from Geosat GM and ERM data, we find that in segment B4 of the discordance (between 125\u00b0 and 126\u00b0 E), the roughly east-west-trending gravity low, correlated with the axial valley, is 20\u201325 km south of the ridge axis position inferred from the center of magnetic anomaly 1. Elsewhere in the discordance, the inferred locations of the ridge axis from magnetics and gravity are in excellent agreement. Ship track data confirm these observations: portions of Moana Wave track crossing the ridge in B4 show that a topographic valley correlated with the gravity anomaly low lies south of the center of magnetic anomaly 1; while other ship track data that cross the spreading ridge in segments B3 and B5 demonstrate good agreement between the axial valley, the gravity anomaly low, and the central magnetic anomaly. Based on these observations, we speculate that the ridge axis in B4 has recently jumped to the south, from a ridge location closer to the center of the young normally magnetized crust, to that of the gravity anomaly low. The position of the gravity low essentially at the edge of normally magnetized crust requires a very recent (&lt; 0.2 Ma) arrival of the ridge in this new location. Because this ridge jump is so young, it may be a promising location for future detailed studies of the dynamics, kinematics, and thermal effects of ridge jumps.",
        "doi": "10.1007/BF01227040",
        "issn": "0025-3235",
        "publisher": "Springer Verlag",
        "publication": "Marine Geophysical Researches",
        "publication_date": "1995-08",
        "series_number": "4",
        "volume": "17",
        "issue": "4",
        "pages": "361-373"
    },
    {
        "id": "authors:0bg55-5p922",
        "collection": "authors",
        "collection_id": "0bg55-5p922",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140414-131946230",
        "type": "article",
        "title": "Arc-rift transition volcanism in the Puertecitos Volcanic Province, northeastern Baja California, Mexico",
        "author": [
            {
                "family_name": "Mart\u00edn-Barajas",
                "given_name": "Arturo",
                "clpid": "Mart\u00edn-Barajas-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Layer",
                "given_name": "Paul",
                "clpid": "Layer-P"
            },
            {
                "family_name": "Hausback",
                "given_name": "Brian",
                "clpid": "Haukback-B"
            },
            {
                "family_name": "Renne",
                "given_name": "Paul",
                "clpid": "Renne-P-R"
            },
            {
                "family_name": "L\u00f3pez-Mart\u00ednez",
                "given_name": "Margarita",
                "clpid": "L\u00f3pez-Mart\u00ednez-M"
            }
        ],
        "abstract": "The Neogene Puertecitos Volcanic Province of northeastern Baja California records a transition from arc-related volcanic activity to rift volcanism associated with opening of the Gulf of California. The eastern Puertecitos Volcanic Province is divided into three volcanic sequences based on mapping, petrology, and ^(40)Ar/^(39)Ar geochronology. The lowest sequence comprises early to middle Miocene (20\u201316 Ma) arc-related andesitic lava flows, volcanic necks, and proximal pyroclastic and epiclastic deposits up to 400 m in thickness, with minor basaltic lava flows. Following the initiation of crustal extension in the region (11\u20136 Ma), synrift volcanism produced two rhyolitic sequences that discordantly overlie the arc-related rocks. The older synrift sequence (6.4\u20135.8 Ma) is composed of rhyolite domes and a series of pyroclastic flows up to 300 m thick. The upper sequence (3.2\u20132.7 Ma) consists of ash-flow tuffs and pumice-lapilli pyroclastic flows, collectively up to 200 m thick. Minor andesite eruptions followed each episode of silicic synrift volcanism. Synvolcanic faults produced topographic relief that controlled deposition of the pyroclastic flows and caused gentler dips upsection. Rhyolite domes are aligned parallel to the predominant north-northwest to north-northeast fault pattern.\n\nAll three volcanic sequences are calc-alkaline. However, the synrift andesite is characterized by lower K_(2)O, lower incompatible element concentrations, and less fractionation of light rare earth elements than the arc-related basalt and andesite. This suggests that the primary melts were more primitive for synrift andesite than for the arc-related rocks.",
        "doi": "10.1130/0016-7606(1995)107<0407:ARTVIT>2.3.CO;2",
        "issn": "0016-7606",
        "publisher": "Geological Society of America",
        "publication": "Geological Society of America Bulletin",
        "publication_date": "1995-04",
        "series_number": "4",
        "volume": "107",
        "issue": "4",
        "pages": "407-424"
    },
    {
        "id": "authors:mdth9-4yp93",
        "collection": "authors",
        "collection_id": "mdth9-4yp93",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140703-094936902",
        "type": "article",
        "title": "Do microplates in subduction zones leave a geological record?",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Lee",
                "given_name": "Jeffrey",
                "clpid": "Lee-J"
            }
        ],
        "abstract": "Active microplate boundaries in ocean-continent subduction zones may induce deformation of the overlying plate and spatial or geochemical variations in the volcanic arc. We discuss two modern cases. The first is the South Gorda-Juan de Fuca plate boundary in the Cascadia subduction zone, where there is little or no effect on the overriding plate and the oceanic plate takes up much of the deformation. The second case is the Cocos-Rivera plate boundary in the Middle America trench, where the overlying Colima graben contains substantial deformation in a zone extending from the trench to the volcanic arc and the sub-duction-related volcanism is spatially and geochemically complex. We apply these observations to boundaries of the Arguello, Monterey, Guadalupe, and Magdalena microplates, which existed in the subduction zone west of Baja California at various times from 20 to 12.5 Ma. The past positions of these boundaries relative to Baja California are constrained by global plate reconstructions, closure of the Gulf of California, and an estimate of extension in the Mexican Basin and Range province. Existing regional mapping and our additional reconnaissance mapping show that Paleocene to Eocene fluvial and marine sedimentary rocks south of Ensenada along the western Baja California peninsula and eastward to the mid-Miocene volcanic arc are undeformed. Limited available data reveal no major spatial or geochemical variations in the mid-Miocene volcanic arc that might correlate with the past positions of the microplate boundaries. Thus these microplate boundaries had little to no effect on the overriding continental plate. The nature of Guadalupe and Magdalena interactions with North America may have been closer to the South Gorda-Juan de Fuca example, with possible internal deformation of the microplates. The Monterey and Arguello microplates may have behaved like the modern Explorer plate, with largely strike-slip motion relative to North America during their last stages of existence. Tectonic patterns similar to these examples may be expected from other plate boundaries where a plate is fragmenting as it enters a subduction zone (e.g., the Aluk plate in the trench beneath West Antarctica in early Tertiary time). Whether these microplates subsequently become attached to the overriding continental plate or to a larger oceanic plate and whether this causes deformation in the region of the former subduction zone may depend on the velocities of the nearby major plates and the relative orientations of the microplate boundaries.",
        "doi": "10.1029/94TC01808",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "1994-12",
        "series_number": "6",
        "volume": "13",
        "issue": "6",
        "pages": "1472-1487"
    },
    {
        "id": "authors:43g3x-3xd75",
        "collection": "authors",
        "collection_id": "43g3x-3xd75",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-101338987",
        "type": "article",
        "title": "Testing the Porcupine Plate Hypothesis",
        "author": [
            {
                "family_name": "Gerstell",
                "given_name": "M. F.",
                "clpid": "Gerstell-M-F"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "The Porcupine Plate, postulated in 1986 to explain difficulties in reconstructing anomalies 21 and 24 in the North Atlantic, is re-examined. Focusing sharply on the spreading segments nearest to Charlie-Gibbs Fracture Zone casts doubt on the Porcupine Plate hypothesis.",
        "doi": "10.1007/BF01224748",
        "issn": "0025-3235",
        "publisher": "Springer Verlag",
        "publication": "Marine Geophysical Researches",
        "publication_date": "1994-08",
        "series_number": "4",
        "volume": "16",
        "issue": "4",
        "pages": "315-323"
    },
    {
        "id": "authors:69f7t-be654",
        "collection": "authors",
        "collection_id": "69f7t-be654",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141010-100018449",
        "type": "article",
        "title": "Variations in ridge morphology and depth-age relationships on the Pacific-Antarctic Ridge",
        "author": [
            {
                "family_name": "Marks",
                "given_name": "Karen M.",
                "clpid": "Marks-K-M"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Adjacent segments of the Pacific-Antarctic ridge display significantly different morphologies and depth-age relationships over seafloor younger than 36 Ma. The spreading corridor southwest of Fracture Zone XII is characterized by a rift valley and an usually small subsidence constant of 226\u00b113 m/m.y.^(\u00bd), while the two spreading corridors immediately northeast of Fracture Zone XII have an axial high and a subsidence constant consistent with the global average. This abrupt variation in ridge morphology is not usually characteristic of medium-rate spreading centers, nor is such an abrupt variation expected of adjacent ridge segments that are spreading at the same rate. We suggest that a thermal anomaly beneath the ridge may influence the first-order effects of spreading rate and lithospheric cooling enough to produce the observed rift valley and axial high and the different subsidence constants. Although we are not certain what would produce the thermal anomaly here, we speculate that when the spreading rate on the Pacific-Antarctic ridge increased from slow to intermediate rates since 20 Ma, so did the need for materials for accretion, which may be supplied in part by along-axis asthenospheric flow from hotspots or a hot region to the northeast. A sufficient supply of hot asthenosphere may still be lacking in the ridge segment with the axial valley to the southwest, leaving it cooler and starved for accretionary materials.",
        "doi": "10.1029/93JB02760",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1994-01-10",
        "series_number": "B1",
        "volume": "99",
        "issue": "B1",
        "pages": "531-541"
    },
    {
        "id": "authors:27aph-y0v59",
        "collection": "authors",
        "collection_id": "27aph-y0v59",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141021-152733674",
        "type": "article",
        "title": "Baja California: The Geology of Rifting",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Those of us who live in the Los Angeles region\nknow that this is an area of active tectonics. We\nhave earthquakes; we have many large mountains\nnearby that are testimony to the great power of\nthe forces that are moving and deforming the\nsurface of the earth here; and we have the San\nAndreas fault as our local tourist attraction. But\nthis great fault is not just local. Besides extending\nnorthward it also continues south toward the\nGulf of California, where a series of structures\nrepresents its continuation under water. All of\nthese structures are part of the major boundary\nbetween the Pacific plate and the North America\nplate. So even though we don't think of Los\nAngeles and the Gulf of California as being similar\nin many ways, they're tectonically connected\nbecause they sit on the same plate boundary and\nsuffer many of the same kinds of deformation due\nto motions between these two plates.",
        "issn": "0013-7812",
        "publisher": "California Institute of Technology",
        "publication": "Engineering and Science",
        "publication_date": "1993-09",
        "series_number": "1",
        "volume": "57",
        "issue": "1",
        "pages": "14-23"
    },
    {
        "id": "authors:t10eq-b5t89",
        "collection": "authors",
        "collection_id": "t10eq-b5t89",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141020-102614297",
        "type": "article",
        "title": "Tect\u00f3nica de placas y la Evoluci\u00f3n del Bloque Jalisco, M\u00e9xico",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "El Bloque Jalisco representa lo que se reconoce\ncomo un bloque tect\u00f3nico, o microplaca, mas o mer os\nrigido (Fig. 1a). Sabemos que se mueve de manera\nindependiente con respecto a las placas circundantes\n(Rivera y Norte America) a traves de dos zonas de\ndeformaci\u00f3n continental (el rift o graben de Tepic-Zacoalco\ny el rift o graben de Colima) ya lo largo de una\nzona de subduccion en su l\u00edmite costero con la placa\noceanica de Rivera. Los rifts de Tepic-Zacoalco y de\nColima se unen con el rift de Chapala, en el l\u00edmite NE del\nbloque Jalisco, dando lugar a lo que es escencialmente\nun punto triple continental, cerca de Guadalajara,\nformado por la uni\u00f3n de: el bloque de Jalisco, el bloque\nde Michoac\u00e1n y la placa de Norte America.\n\nEl desarrollo del bloque Jalisco, como bloque\nindependiente, parece estar relacionado\ngeometricamente con la forma y din\u00e1mica de la placa\nde Rivera, asi como tambi\u00e9n con la evoluci\u00f3n del punto\ntriple continental cerca de Guadalajara ya mencionado.\n\nEl estudio del bloque Jalisco representa un\nbuen laboratorio para el desarrollode modelos tectonicos\nque nos permitan estudiar el inicio de movimientos de,\nmicroplacas, as\u00ed como el fen\u00f3meno de una posible\ncaptura de un bloque continental por otra placa\nescencialmente oceanica (Luhr et al, 1985; Allan, 1990).\nPor ello resulta interesante saber con detalle como fue\nsu evoluci\u00f3n y como es su movimiento actual, con\nrespecto a las placas circundantes.",
        "issn": "0186-1891",
        "publisher": "Uni\u00f3n Geof\u00edsica Mexicana",
        "publication": "GEOS",
        "publication_date": "1993-07",
        "series_number": "3",
        "volume": "13",
        "issue": "3",
        "pages": "3-9"
    },
    {
        "id": "authors:v23rd-n3c69",
        "collection": "authors",
        "collection_id": "v23rd-n3c69",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20130311-145649896",
        "type": "article",
        "title": "Near-Field Investigations of the Landers Earthquake Sequence, April to July 1992",
        "author": [
            {
                "family_name": "Sieh",
                "given_name": "Kerry",
                "orcid": "0000-0002-7311-2447",
                "clpid": "Sieh-K-E"
            },
            {
                "family_name": "Jones",
                "given_name": "Lucile",
                "orcid": "0000-0002-2690-3051",
                "clpid": "Jones-L-M"
            },
            {
                "family_name": "Hauksson",
                "given_name": "Egill",
                "orcid": "0000-0002-6834-5051",
                "clpid": "Hauksson-E"
            },
            {
                "family_name": "Hudnut",
                "given_name": "Kenneth",
                "orcid": "0000-0002-3168-4797",
                "clpid": "Hudnut-K-W"
            },
            {
                "family_name": "Eberhard-Phillips",
                "given_name": "Donna",
                "clpid": "Eberhard-Phillips-D"
            },
            {
                "family_name": "Heaton",
                "given_name": "Thomas",
                "orcid": "0000-0003-3363-2197",
                "clpid": "Heaton-T-H"
            },
            {
                "family_name": "Hough",
                "given_name": "Susan",
                "orcid": "0000-0002-5980-2986",
                "clpid": "Hough-S-E"
            },
            {
                "family_name": "Hutton",
                "given_name": "Kate",
                "clpid": "Hutton-K"
            },
            {
                "family_name": "Kanamori",
                "given_name": "Hiroo",
                "orcid": "0000-0001-8219-9428",
                "clpid": "Kanamori-H"
            },
            {
                "family_name": "Lilje",
                "given_name": "Anne",
                "clpid": "Lilje-A"
            },
            {
                "family_name": "Lindvall",
                "given_name": "Scott",
                "clpid": "Lindvall-S-C"
            },
            {
                "family_name": "McGill",
                "given_name": "Sally F.",
                "clpid": "McGill-S-F"
            },
            {
                "family_name": "Mori",
                "given_name": "James",
                "clpid": "Mori-Jim"
            },
            {
                "family_name": "Rubin",
                "given_name": "Charles",
                "clpid": "Rubin-C-M"
            },
            {
                "family_name": "Spotila",
                "given_name": "James A.",
                "clpid": "Spotila-J-A"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Thio",
                "given_name": "Hong Kie",
                "clpid": "Thio-Hong-Kie"
            },
            {
                "family_name": "Treiman",
                "given_name": "Jerome",
                "clpid": "Treiman-J"
            },
            {
                "family_name": "Wernicke",
                "given_name": "Brian",
                "orcid": "0000-0002-7659-8358",
                "clpid": "Wernicke-B-P"
            },
            {
                "family_name": "Zachariasen",
                "given_name": "Judith",
                "clpid": "Zachariasen-J"
            }
        ],
        "abstract": "The Landers earthquake, which had a moment magnitude (M_w) of 7.3, was the largest earthquake to strike the contiguous United States in 40 years. This earthquake resulted from the rupture of five major and many minor right-lateral faults near the southern end of the eastern California shear zone, just north of the San Andreas fault. Its M_w 6.1 preshock and M_w 6.2 aftershock had their own aftershocks and foreshocks. Surficial geological observations are consistent with local and far-field seismologic observations of the earthquake. Large surficial offsets (as great as 6 meters) and a relatively short rupture length (85 kilometers) are consistent with seismological calculations of a high stress drop (200 bars), which is in turn consistent with an apparently long recurrence interval for these faults.",
        "doi": "10.1126/science.260.5105.171",
        "issn": "0036-8075",
        "publisher": "American Association for the Advancement of Science",
        "publication": "Science",
        "publication_date": "1993-04-09",
        "series_number": "5105",
        "volume": "260",
        "issue": "5105",
        "pages": "171-176"
    },
    {
        "id": "authors:bq0fr-7vv59",
        "collection": "authors",
        "collection_id": "bq0fr-7vv59",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-112636029",
        "type": "article",
        "title": "Quantitative determination of uncertainties in seismic refraction prospecting",
        "author": [
            {
                "family_name": "Liu",
                "given_name": "Chuanhai",
                "clpid": "Liu-Chuanhai"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We present a model of the propagation of refracted seismic waves in planar (horizontal or dipping) layered structures in which we quantify the errors from various sources. The model, called the (mixed) variance component model, separates the errors originating on the surface from those due to inhomogeneities of subsurface layers. The model starts with the assumption of homogeneous (constant-velocity) layers, but by taking the principal errors into account, variations from this model (including degree of velocity inhomogeneity, vertical velocity gradients, and gradational interfaces) can be identified.A complete solution to the variance component model by Bayesian methods relies on the Gibbs sampler, a recently well-developed statistical technique. Using the Gibbs sampler and Monte Carlo methods, we can estimate the posterior distributions of any parameter of interest. Thus, in addition to estimating the various errors, we can obtain the velocity-versus-depth curve with its confidence intervals at any relevant point along the line.We analyze data from a crustal-scale refraction line to illustrate both features of this method. The results indicate that the conventional linear regression model for the first arrivals is inappropriate for this data set. As might be expected, geophone spacing strongly affects our ability to resolve the heterogeneities. Differences in the amount of velocity heterogeneity in different layers can be resolved, and may be useful for lithologic characterization. For this crustal-scale problem, a velocity profile derived from this method is an improvement over simple linear interpretations, but it could be further refined by more comprehensive methods attempting to match later arrivals and wave amplitudes as well as first arrivals. The method could also be applied to smaller-scale refraction problems, such as determination of refraction statics, or constraints on the degree of probable lateral variations in velocity of shallow layers, for improved processing of reflection data.",
        "issn": "0016-8033",
        "publisher": "Society of Exploration Geophysicists",
        "publication": "Geophysics",
        "publication_date": "1993-04",
        "series_number": "4",
        "volume": "58",
        "issue": "4",
        "pages": "553-563"
    },
    {
        "id": "authors:384fy-s4613",
        "collection": "authors",
        "collection_id": "384fy-s4613",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-104751105",
        "type": "article",
        "title": "Reply to Jurdy & Stefanick comment",
        "author": [
            {
                "family_name": "Chang",
                "given_name": "Ted",
                "clpid": "Chang-T"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            }
        ],
        "abstract": "We disagree with virtually all of what Jurdy &amp; Stefanick\nhave written. Part of our disagreement stems from personal\nopinions about what is 'simple', 'arbitrary', 'artificial',\n'undesirable', etc., but other disagreements are more\nprofound and reveal a very different understanding of finite\nrotations. Jurdy &amp; Stefanick raise two basic objections. One\nconcerns statistical questions that were not meant to be part\nof Chang et al. (1990). The other addresses the main issue of\nour paper, the parametrization of uncertainties of rotations.\nThey suggest that both our approach is flawed and that\ntheirs, outlined in Jurdy &amp; Stefanick (1987), is better.\nExcept possibly for their opinion of what constitutes a\ncovariance matrix, we try not to indulge the reader with\nlong discussions of questions of personal preference, but\ninstead to confine our response to these basic questions.",
        "doi": "10.1111/j.1365-246X.1992.tb00724.x",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "1992-07",
        "series_number": "1",
        "volume": "110",
        "issue": "1",
        "pages": "215-217"
    },
    {
        "id": "authors:1a0z4-1db72",
        "collection": "authors",
        "collection_id": "1a0z4-1db72",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20141017-105639817",
        "type": "article",
        "title": "The rotation group in plate tectonics and the representation of uncertainties of plate reconstructions",
        "author": [
            {
                "family_name": "Chang",
                "given_name": "T.",
                "clpid": "Chang-T"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Molnar",
                "given_name": "P.",
                "clpid": "Molnar-P"
            }
        ],
        "abstract": "The calculation of the uncertainty in an estimated rotation requires a parametrization of the rotation group; that is, a unique mapping of the rotation group to a point in 3-D Euclidean space, R^3. Numerous parametrizations of a rotation exist, including: (1) the latitude and longitude of the axis of rotation and the angle of rotation; (2) a representation as a Cartesian vector with length equal to the rotation angle and direction parallel to the rotation axis; (3) Euler angles; or (4) unit length quaternions (or, equivalently, Cayley-Klein parameters). \nThe uncertainty in a rotation is determined by the effect of nearby rotations on the rotated data. The uncertainty in a rotation is small, if rotations close to the best fitting rotation degrade the fit of the data by a large amount, and it is large, if only rotations differing by a large amount cause such a degradation. Ideally, we would like to parametrize the rotations in such a way so that their representation as points in R^3 would have the property that the distance between two points in R3 reflects the effects of the corresponding rotations on the fit of the data. It can be shown mathematically that this is impossible, but for rotations of small angle, it can be done to close approximation by using vectors in Cartesian coordinates. Thus, we are led to parametrizing the uncertainty separately from the parametrization of the best fitting rotation. This approach results in simpler, more efficient calculations than if uncertainties are described in terms of rotation parameters (i.e., latitude, longitude, and the angle). We illustrate this with the example of equations for determining the uncertainty in a composite rotation from the uncertainties of its constituents.",
        "doi": "10.1111/j.1365-246X.1990.tb05576.x",
        "issn": "0956-540X",
        "publisher": "Royal Astronomical Society",
        "publication": "Geophysical Journal International",
        "publication_date": "1990-06",
        "series_number": "3",
        "volume": "101",
        "issue": "3",
        "pages": "649-661"
    },
    {
        "id": "authors:r8c1e-wt278",
        "collection": "authors",
        "collection_id": "r8c1e-wt278",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-103153269",
        "type": "article",
        "title": "Miocene to recent structural development of an extensional accommodation zone, northeastern Baja California, Mexico",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hodges",
                "given_name": "K. V.",
                "orcid": "0000-0003-2805-8899",
                "clpid": "Hodges-K-V"
            }
        ],
        "abstract": "The Gulf of California Extensional Province in northeastern Baja California contains a major structural transition from a northern domain of widely spaced basins and ranges to a southern domain of closely spaced, NNW-striking high-angle faults. In the northern domain, the western boundary of the province (the Main Gulf Escarpment) is a single listric normal fault, the San Pedro M\u00e1rtir fault; in the southern domain it is a 5 km wide zone of numerous E-dipping high-angle normal faults. The western half of this structural transition, studied here, does not occur by a single 'transfer fault' but rather by: (1) transfer of displacement from the San Pedro M\u00e1rtir fault onto multiple fault zones in the footwall, without intervening cross-faults; and (2) increased southward disruption of the hanging wall by WNW-striking strike-slip faults (oblique to the extension direction) and NNW-striking normal faults and extension fractures. This structural transition involves both the hanging wall and the footwall of the escarpment. The lack of a discrete transfer structure is attributed either to insufficient extension (&lt;10%) or to a gradual change in geometry of the basal detachment.",
        "doi": "10.1016/0191-8141(90)90016-R",
        "issn": "0191-8141",
        "publisher": "Elsevier",
        "publication": "Journal of Structural Geology",
        "publication_date": "1990",
        "series_number": "3",
        "volume": "12",
        "issue": "3",
        "pages": "315-328"
    },
    {
        "id": "authors:pk135-dab43",
        "collection": "authors",
        "collection_id": "pk135-dab43",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140905-142821870",
        "type": "article",
        "title": "Evolution of extensional basins and basin and range topography west of Death Valley, California",
        "author": [
            {
                "family_name": "Hodges",
                "given_name": "K. V.",
                "orcid": "0000-0003-2805-8899",
                "clpid": "Hodges-K-V"
            },
            {
                "family_name": "McKenna",
                "given_name": "L. W.",
                "clpid": "McKenna-L-W"
            },
            {
                "family_name": "Stock",
                "given_name": "J.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Knapp",
                "given_name": "J.",
                "clpid": "Knapp-J"
            },
            {
                "family_name": "Page",
                "given_name": "L.",
                "clpid": "Page-L"
            },
            {
                "family_name": "Sternlof",
                "given_name": "K.",
                "clpid": "Sternlof-K"
            },
            {
                "family_name": "Silverberg",
                "given_name": "D.",
                "clpid": "Silverberg-D"
            },
            {
                "family_name": "W\u00fcst",
                "given_name": "G.",
                "clpid": "W\u00fcst-G"
            },
            {
                "family_name": "Walker",
                "given_name": "J. D.",
                "clpid": "Walker-J-D"
            }
        ],
        "abstract": "Neogene extension in the Death Valley region, SE California, has produced a variety of sedimentary basins. Diachronous movements on an array of strike-slip and normal fault systems have resulted in the uplift and preservation of older basins in modern ranges. One of the best exposed of these is the Nova basin on the western flank of the Panamint Mountains. The Nova basin includes over 2000 m of sedimentary and volcanic rocks deposited during denudation of the Panamint Mountains metamorphic core complex in late Miocene (?) \u2013 early Pliocene time. The principal growth structure for the basin was the Emigrant detachment, which initiated and moved at a low angle. Modern Panamint Valley, west of the range, developed as a consequence of Late Pliocene - Recent, kinematically linked movement on the right-slip, high-angle Hunter Mountain fault zone and the low-angle Panamint Valley detachment. Detailed mapping of the intersection between the Emigrant and Panamint Valley detachments demonstrates that segments of the earlier system remained active during development of Panamint Valley and, thus, during development of modern Basin and Range topography as well. These results indicate that large-scale extension in the Death Valley region, accommodated by movement on low- to moderate-angle normal fault systems and high-angle strike-slip fault systems, is a continuing process. Basin and Range topography in the Panamint Valley - Death Valley area was generated at least in part by displacements on low-angle detachments rather than high-angle normal faults.",
        "doi": "10.1029/TC008i003p00453",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "1989-06",
        "series_number": "3",
        "volume": "8",
        "issue": "3",
        "pages": "453-467"
    },
    {
        "id": "authors:1ba9w-86f87",
        "collection": "authors",
        "collection_id": "1ba9w-86f87",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140905-141154013",
        "type": "article",
        "title": "Pre-Pliocene Extension around the Gulf of California and the transfer of Baja California to the Pacific Plate",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Hodges",
                "given_name": "K. V.",
                "orcid": "0000-0003-2805-8899",
                "clpid": "Hodges-K-V"
            }
        ],
        "abstract": "Late Miocene (12\u20135 Ma) extension around the edges of the Gulf of California has been alternatively attributed to \"Basin and Range\" extension, back arc extension, or development of the Pacific-North America plate boundary. This extension was ENE directed and similar in structural style to extension in the Basin and Range province. Timing constraints permit nearly synchronous onset of this deformation in a belt extending SSE from northernmost Baja California to the mouth of the gulf. Where this extensional faulting continued through Pliocene time to the present, synchronous with motion on the modern transform plate boundary in the Gulf of California, no change in direction of extension can be resolved. Revised constraints on Pacific-North America plate motion support the development of this late Miocene extension as a component of Pacific-North America displacement that could not be accommodated by strike-slip displacement along the existing plate boundary west of the Baja California peninsula. This scenario implies that transfer of Baja California from the North America plate to the Pacific plate was a gradual process, beginning about 12\u201310 Ma, when motion of the Pacific plate relative to North America was partitioned into separate regimes of strike-slip and dip-slip displacement on opposite sides of Baja California.",
        "doi": "10.1029/TC008i001p00099",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "1989-02",
        "series_number": "1",
        "volume": "8",
        "issue": "1",
        "pages": "99-115"
    },
    {
        "id": "authors:nd1n4-79k09",
        "collection": "authors",
        "collection_id": "nd1n4-79k09",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140924-074741801",
        "type": "article",
        "title": "Sequence and geochronology of Miocene rocks adjacent to the main gulf escarpment: southern Valle Chico, Baja California Norte, Mexico",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Geologic mapping and K/Ar dating of Tertiary rocks in NE Baja California, at latitude 30\u00b0 30' N, reveal a history\nof volcanism from 20 Ma to at least 6 Ma. From 20 to 15 Ma, basalt, andesite and pyroclastic flows locally covered\nthe Cretaceous and older batholithic and prebatholithic rocks. These deposits were followed by up to\n300 m of additional pyroclastic flows, reworked tuff, basalt, sandstone and conglomerate. Subsequent eruptions\nbetween 11 and 6 Ma produced andesite to rhyolite flows and breccias. Eruptions at about 6 Ma covered\nthe region with up to an additional 300 m of pyroclastic flows, ash fall deposits and welded vitric tuff. These\nunits cap the high plateaus of the northwestern corner of the Puertecitos volcanic province. Local undated volcanic\nunits may be younger than 6 Ma. The tilting, faulting and topographic relief associated with the Main Gulf\nEscarpment began developing sometime between 11 and 6 Ma; variations in thickness of the pre- I I Ma units arc\nnot generally fault-related, although variations in thickness of the 6 Ma deposits arc. The alignment of four\nprc-6 Ma volcanic vents along a NNW trend parallel to the present escarpment suggests that ascent of the magmas\nmay have been structurally controlled by Late Miocene extensional faults.",
        "issn": "0016-7169",
        "publisher": "Union Fisica Mexicana",
        "publication": "Geofisica Internacional",
        "publication_date": "1989",
        "series_number": "5",
        "volume": "28",
        "issue": "5",
        "pages": "851-896"
    },
    {
        "id": "authors:6tewp-k3750",
        "collection": "authors",
        "collection_id": "6tewp-k3750",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140919-130409131",
        "type": "article",
        "title": "Continuation of a deep borehole stress measurement profile near the San Andreas Fault: 2. Hydraulic fracturing stress measurements at Black Butte, Mojave Desert, California",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Healy",
                "given_name": "J. H.",
                "clpid": "Healy-J-H"
            }
        ],
        "abstract": "Hydraulic fracturing stress measurements were obtained in the Black Butte drill hole, 18 km northeast of the San Andreas fault in the Mojave Desert, at depths from 251 to 635 m. In all tests the least and greatest horizontal principal stresses (S_h and S_H, respectively) exceeded the vertical stress (S_\u03bd), indicating a thrust faulting stress regime. A single good-quality hydraulic fracture impression from 309 m depth indicates an S_H direction of N41\u00b0E \u00b1 10\u00b0. This S_H direction should be interpreted with caution because it is based on only one observation. This orientation is fairly compatible with nearby surface stress measurements but is incompatible with most of the hydraulic fracturing stress orientations reported from comparable depths in the Mojave Desert and is not favorable for right-lateral slip on either the San Andreas fault or NW striking faults present farther to the east. The stress regime measured in the Black Butte hole is comparable to that measured at nearby shallow depths but differs from the strike-slip or transitional (strike-slip to thrust faulting) stress regime present at similar depths in two nearby holes: Crystallaire, 4 km northeast of fhe San Andreas fault, and Hi Vista, 32 km northeast of the San Andreas fault. The S_H direction measured in these holes is approximately 60\u00b0 counterclockwise of that observed in the Black Butte hole. The differences in stress magnitudes and orientation among these holes substantiate previous indications of local variations in stress in the upper kilometer of the crust in this area and cast doubt on the validity of linear elastic models in which the effects of the San Andreas fault dominate the stress field in the western Mojave Desert.",
        "doi": "10.1029/JB093iB12p15196",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1988-12-10",
        "series_number": "B12",
        "volume": "93",
        "issue": "B12",
        "pages": "15196-15206"
    },
    {
        "id": "authors:epy4q-qex07",
        "collection": "authors",
        "collection_id": "epy4q-qex07",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140905-135601264",
        "type": "article",
        "title": "Uncertainties and implications of the Late Cretaceous and Tertiary position of North America relative to the Farallon, Kula, and Pacific Plates",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            }
        ],
        "abstract": "We present updated global plate reconstructions and calculated uncertainties of the Pacific, Kula, and Farallon/Vancouver plates relative to North America for selected times since 68 Ma. Improved magnetic data from the Indian Ocean decrease the uncertainties in. the global plate circuit approach; these uncertainties are now considerably smaller than those inherent in equivalent reconstructions based on the assumption of fixed hotspots. Major differences between these results and those of others are due to our use of more detailed Africa-North America reconstructions, separate Vancouver and Farallon plate reconstructions, and the assumption of a rigid Antarctica plate during Cenozoic time. The uncertainties in the relative positions of the Pacific and North America plates since the time of anomaly 7 (26 Ma) range up to \u00b1100 km in position, or from 1 to 3 m.y. in time. If the Mendocino triple junction initiated at about 28.5 Ma, its position would have been at 31.3\u00b0N \u00b1 130 km relative to fixed North America. Unacceptable overlap of oceanic crust of the Pacific plate with continental crust of western North America in the anomaly 10 (30 Ma) reconstruction is a minimum of 340\u00b1200 km along an azimuth of N60\u00b0E and may be accounted for by Basin and Range extension. Pacific-North America displacement in the past 20 Ma is found to be considerably less than that calculated by fixed hotspot reconstructions. Farallon (Vancouver)-North America convergence velocity decreased greatly between the times of anomalies 24 and 21 (56 to 50 Ma), prior to the 43 Ma age of the Hawaiian-Emperor bend and the often quoted 40 Ma \"end\" of the Laramide orogeny. A change in direction of Farallon-North America convergence occurred sometime between 50 and 42 Ma and also may not correlate with the time of the Hawaiian-Emperor bend. The lack of data from subducted parts of the Farallon and Kula plates permits many possibilities regarding the position of the Kula-Farallon ridge, the age of subducted crust, or the position of oceanic plateaus during the Laramide orogeny, leaving open the question of the relationship between plate tectonic scenarios and tectonic style during Laramide time. Displacements of points on the various oceanic plates along the west coast of an arbitrarily fixed North America during the interval between anomalies 30/31 and 18 (68 to 42 Ma) are found to be: Pacific plate, 1700\u00b1200 km northward; Farallon plate, 3200\u00b1400 km northeastward; Vancouver plate, 3000\u00b1400 km northeastward; Kula plate, if attached to the Pacific plate after A24 time, 2500\u00b1400 km northward.",
        "doi": "10.1029/TC007i006p01339",
        "issn": "0278-7407",
        "publisher": "American Geophysical Union",
        "publication": "Tectonics",
        "publication_date": "1988-12",
        "series_number": "6",
        "volume": "7",
        "issue": "6",
        "pages": "1339-1384"
    },
    {
        "id": "authors:cnzd0-2m391",
        "collection": "authors",
        "collection_id": "cnzd0-2m391",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-110656708",
        "type": "article",
        "title": "The Cenozoic and Late Cretaceous evolution of the Indian Ocean Basin: uncertainties in the reconstructed positions of the Indian, African and Antarctic plates",
        "author": [
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Pardo-Casas",
                "given_name": "Federico",
                "clpid": "Pardo-Casas-F"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Reconstructions of the relative positions of the Indian, African, and Antarctic plates and their uncertainties are given for the times of selected magnetic anomalies that could be identified on adjacent pairs of these plates. Among the most certain reconstructions are those for the Antarctic and African plates, which can be determined directly from recently published magnetic anomalies from both sides of the Southwest Indian Ridge. As Patriat and his colleagues reported, there was an important change in direction and a decrease in rate of separation between Africa and Antarctica between the times of anomalies 33 and 20. India moved rapidly away from both Africa and Antarctica in the Late Cretaceous and early Tertiary periods, but slowed markedly near the time of anomaly 20 (\u2245 45 Myr). The positions of the Indian plate with respect to the others are poorly constrained between the times of anomaly 5 (\u2245 10 Myr) and anomaly 23 (\u2245 54 Myr), but using the reconstructions of the African and Antarctic plates, the uncertainties can be reduced. Despite the relatively large uncertainties, the positions of anomalies 5, 6, and 13 on the Antarctic and Indian plates apparently cannot be described by the same parameters that describe the history of separation of Australia and Antarctica. Therefore, Stein and Okal's contention that Australia and India lie on separate plates appears to be valid not only for the present, but for the last 35 Myr.",
        "doi": "10.1111/j.1365-2117.1988.tb00003.x",
        "issn": "0950-091X",
        "publisher": "Blackwell Publishing",
        "publication": "Basin Research",
        "publication_date": "1988-03",
        "series_number": "1",
        "volume": "1",
        "issue": "1",
        "pages": "23-40"
    },
    {
        "id": "authors:6wrkv-3xj19",
        "collection": "authors",
        "collection_id": "6wrkv-3xj19",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-093025883",
        "type": "article",
        "title": "Relative motions of hotspots in the Pacific, Atlantic and Indian Oceans since late Cretaceous time",
        "author": [
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "Combinations of global plate reconstructions reveal average velocities for the last 50 to 65 million years of 10 to 20 mm yr^(\u22121) between the Hawaiian hotspot and those beneath Iceland, Tristan da Cunha, R\u00e9union, St. Paul's Island, and Kerguelen. Therefore hotspots do not define a fixed reference frame. Uncertainties in these reconstructions are less than the errors incurred by assuming fixed hotspots and less than the differences among various proposed frames of reference of fixed hotspots.",
        "doi": "10.1038/327587a0",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "1987-06-18",
        "series_number": "6123",
        "volume": "327",
        "issue": "6123",
        "pages": "587-591"
    },
    {
        "id": "authors:7bkvn-zba05",
        "collection": "authors",
        "collection_id": "7bkvn-zba05",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-111301499",
        "type": "article",
        "title": "Revised history of early Tertiary plate motion in the south-west Pacific",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            }
        ],
        "abstract": "Reanalysis of early Tertiary magnetic anomalies on the Pacific plate south of the Campbell Plateau indicates that in early Tertiary time there was a previously unrecognized triple junction of the Pacific, the Antarctic, and a third plate now beneath the Bellingshausen sea. Corresponding revised parameters for Pacific\u2013Antarctica motion do not require early Tertiary displacements within Antarctica or New Zealand, but suggest a change in direction of the Pacific plate over the hotspots of approximately the same sense and timing as the Hawaiian\u2013Emperor bend.",
        "doi": "10.1038/325495a0",
        "issn": "0028-0836",
        "publisher": "Nature Publishing Group",
        "publication": "Nature",
        "publication_date": "1987-02-05",
        "series_number": "6104",
        "volume": "325",
        "issue": "6104",
        "pages": "495-499"
    },
    {
        "id": "authors:cpkqr-83v72",
        "collection": "authors",
        "collection_id": "cpkqr-83v72",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140919-123757633",
        "type": "article",
        "title": "A method for bounding uncertainties in combined plate reconstructions",
        "author": [
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We present a method for calculating uncertainties in plate reconstructions that does not describe the uncertainty in terms of uncertainties in pole positions and rotation angles. If a fit of magnetic anomalies of the same age and fracture zones that were active as transform faults at that time can be found, such a reconstruction can be perturbed and degraded by small rotations about each of three orthogonal axes (partial uncertainty poles). If the uncertainty in the reconstruction is a consequence of independent, small, but acceptable, rotations about these axes, then the uncertainties in reconstructed points will be elliptical in shape. The dimensions and orientation of such ellipses will depend upon the magnitudes of the perturbing rotations and upon the relative geometry of the partial uncertainty poles and the points in question. In a sequence of rotations, each rotation will contribute an elliptical region of uncertainty for each reconstructed point, and these ellipses can be combined as independent statistical quantities to obtain a confidence ellipse for the sequence of rotations. As a test, we calculated uncertainties for three points on the Pacific plate with respect to North America at the time of anomaly 6 (20 Ma). The computed uncertainties are similar in shape to those that we previously obtained for a sequence of marginally acceptable rotations, but the major axes of the ellipses presented here are about 25% shorter.",
        "doi": "10.1029/JB090iB14p12537",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1985-12-10",
        "series_number": "B14",
        "volume": "90",
        "issue": "B14",
        "pages": "12537-12544"
    },
    {
        "id": "authors:cbqg6-38x81",
        "collection": "authors",
        "collection_id": "cbqg6-38x81",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140903-101724783",
        "type": "article",
        "title": "A geophysical study of Mesquite Valley: Nevada-California border",
        "author": [
            {
                "family_name": "Park",
                "given_name": "Stephen",
                "clpid": "Park-Stephen"
            },
            {
                "family_name": "Brome",
                "given_name": "Isabel",
                "clpid": "Brome-I"
            },
            {
                "family_name": "Cunningham",
                "given_name": "Paul",
                "clpid": "Cunningham-P"
            },
            {
                "family_name": "Harris",
                "given_name": "Ruth",
                "clpid": "Harris-R"
            },
            {
                "family_name": "Hess",
                "given_name": "Thomas",
                "clpid": "Hess-T"
            },
            {
                "family_name": "Hodges",
                "given_name": "John",
                "clpid": "Hodges-J"
            },
            {
                "family_name": "Kirkpatrick",
                "given_name": "Dwight",
                "clpid": "Kirkpatrick-D"
            },
            {
                "family_name": "Madden",
                "given_name": "Theodore",
                "clpid": "Madden-T"
            },
            {
                "family_name": "Mellen",
                "given_name": "Michael",
                "clpid": "Mellen-M"
            },
            {
                "family_name": "Menoher",
                "given_name": "Jeffrey",
                "clpid": "Menoher-J"
            },
            {
                "family_name": "Michael",
                "given_name": "Andrew",
                "clpid": "Michael-A-J"
            },
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Murray",
                "given_name": "Mark",
                "clpid": "Murray-M"
            },
            {
                "family_name": "Olgaard",
                "given_name": "David",
                "clpid": "Olgaard-D"
            },
            {
                "family_name": "Standley",
                "given_name": "Pamela",
                "clpid": "Standley-P"
            },
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Stork",
                "given_name": "Christof",
                "clpid": "Stork-C"
            },
            {
                "family_name": "Wray",
                "given_name": "S. Tanner",
                "clpid": "Wray-S-T"
            },
            {
                "literal": "MIT Field Geophysics Course"
            }
        ],
        "abstract": "This paper reports the results of a geophysical investigation of a sedimentary basin, Mesquite Valley, and its surrounding area in the Basin and Range province of the western United States. Mesquite Valley is located about 40 km south-southwest of Las Vegas, Nevada, and straddles the border between Nevada and California (Figure 1). It is surrounded on three sides by mountains in which Paleozoic sedimentary rocks and Precambrian granites and gneisses crop out (Figure 1) [Burchfiel et al., 1974; Durchfiel and Davis, 1971; Hewett, 1956]. Unlike most basins in the Basin and Range province, however, there are no clearly active, range-bounding normal faults, and, in general, the surrounding topography is more subdued than in the regions farther west or north.",
        "doi": "10.1029/JB090iB10p08685",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1985-09-10",
        "series_number": "B10",
        "volume": "90",
        "issue": "B10",
        "pages": "8685-8689"
    },
    {
        "id": "authors:hvcmm-y9232",
        "collection": "authors",
        "collection_id": "hvcmm-y9232",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140919-111922215",
        "type": "article",
        "title": "Hydraulic fracturing stress measurements at Yucca Mountain, Nevada, and relationship to the regional stress field",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Healy",
                "given_name": "J. H.",
                "clpid": "Healy-J-H"
            },
            {
                "family_name": "Hickman",
                "given_name": "S. H.",
                "clpid": "Hickman-S-H"
            },
            {
                "family_name": "Zoback",
                "given_name": "M. D.",
                "orcid": "0000-0002-8851-2099",
                "clpid": "Zoback-M-D"
            }
        ],
        "abstract": "Hydraulic fracturing stress measurements and acoustic borehole televiewer logs were run in holes USW G-1 and USW G-2 at Yucca Mountain as part of the Nevada Nuclear Waste Storage Investigations for the U.S. Department of Energy. Eight tests in the saturated zone, at depths from 646 to 1288 m, yielded values of the least horizontal stress S_h that are considerably lower than the vertical principal stress S_v. In tests for which the greatest horizontal principal stress S_H could be determined, it was found to be less than S_v, indicating a normal faulting stress regime. The borehole televiewer logs showed the presence of long (in excess of 10 m), vertical, drilling-induced fractures in the first 300 m below the water table. These are believed to form by the propagation of small preexisting cracks under the excess downhole fluid pressures (up to 5.2 MPa) applied during drilling. The presence of these drilling-induced hydrofractures provides further confirmation of the low value of the least horizontal stresses. A least horizontal principal stress direction of N60\u00b0W\u2013N65\u00b0W is indicated by the orientation of the drilling-induced hydrofractures (N25\u00b0E\u2013N30\u00b0E), and the orientation of stress-induced well bore breakouts in the lower part of USW G-2 (N65\u00b0W). This direction is in good agreement with indicators of stress direction from elsewhere at the Nevada Test Site. The observed stress magnitudes and directions were examined for the possibility of slip on preexisting faults. Using these data, the Coulomb criterion for frictional sliding suggests that for coefficients of friction close to 0.6, movement on favorably oriented faults could be expected. For coefficients of friction of 1.0, preexisting faults of all orientations should be stable. Laboratory studies on the Yucca Mountain tuffs, reported elsewhere, yield coefficients of friction ranging from 0.6 to 0.9.",
        "doi": "10.1029/JB090iB10p08691",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1985-09-10",
        "series_number": "B10",
        "volume": "90",
        "issue": "B10",
        "pages": "8691-8706"
    },
    {
        "id": "authors:2mw5y-jxz06",
        "collection": "authors",
        "collection_id": "2mw5y-jxz06",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140909-082204506",
        "type": "article",
        "title": "The configuration of the seismic zone and the downgoing slab in southern Peru",
        "author": [
            {
                "family_name": "Grange",
                "given_name": "F.",
                "clpid": "Grange-F"
            },
            {
                "family_name": "Cunningham",
                "given_name": "P.",
                "clpid": "Cunningham-P"
            },
            {
                "family_name": "Gagnepain",
                "given_name": "J.",
                "clpid": "Gagnepain-J"
            },
            {
                "family_name": "Hatzfeld",
                "given_name": "D.",
                "clpid": "Hatzfeld-D"
            },
            {
                "family_name": "Molnar",
                "given_name": "P.",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Ocola",
                "given_name": "L.",
                "clpid": "Ocola-L"
            },
            {
                "family_name": "Rodr\u00edgues",
                "given_name": "A.",
                "clpid": "Rodr\u00edgues-A"
            },
            {
                "family_name": "Roecker",
                "given_name": "S. W.",
                "clpid": "Roecker-S-W"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Su\u00e1rez",
                "given_name": "G.",
                "orcid": "0000-0002-2011-4924",
                "clpid": "Su\u00e1rez-Genaro"
            }
        ],
        "abstract": "Using data from temporary networks of portable seismographs in southern Peru, we located 888 shallow and intermediate depth events near a proposed discontinuity in the seismic zone there. These events reveal a prominent contortion, instead of a discontinuity, that trends approximately N80\u00b0E, parallel to the direction of relative plate motion. North of about 15\u00b0S, the seismic zone beneath Peru is nearly horizontal, but south of about 15.5\u00b0S, it dips at about 25\u00b0. Volcanoes lie above the more steeply dipping zone where earthquakes occur between 120 and 140 km, and the volcanic line in southern Peru stops abruptly at the contortion.",
        "doi": "10.1029/GL011i001p00038",
        "issn": "0094-8276",
        "publisher": "American Geophysical Union",
        "publication": "Geophysical Research Letters",
        "publication_date": "1984-01",
        "series_number": "1",
        "volume": "11",
        "issue": "1",
        "pages": "38-41"
    },
    {
        "id": "authors:x2x6q-x7z97",
        "collection": "authors",
        "collection_id": "x2x6q-x7z97",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140909-085349745",
        "type": "article",
        "title": "Microearthquake seismicity and active tectonics of northwestern Greece",
        "author": [
            {
                "family_name": "King",
                "given_name": "G. C. P.",
                "clpid": "King-G-C-P"
            },
            {
                "family_name": "Tselentis",
                "given_name": "A.",
                "clpid": "Tselentis-A"
            },
            {
                "family_name": "Gomberg",
                "given_name": "J.",
                "clpid": "Gomberg-J-S"
            },
            {
                "family_name": "Molnar",
                "given_name": "P.",
                "clpid": "Molnar-P"
            },
            {
                "family_name": "Roecker",
                "given_name": "S. W.",
                "clpid": "Roecker-S-W"
            },
            {
                "family_name": "Sinvhal",
                "given_name": "H.",
                "clpid": "Sinvhal-H"
            },
            {
                "family_name": "Soufleris",
                "given_name": "C.",
                "clpid": "Soufleris-C"
            },
            {
                "family_name": "Stock",
                "given_name": "J. M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            }
        ],
        "abstract": "We carried out a microearthquake survey lasting for six weeks in northwest Greece using 18 portable seismograph stations to examine a region in which normal and thrust faulting have been reported in close proximity to one another. With this array we located 148 events and determined fault plane solutions for eight events using only rays radiated upwards. The seismicity of the region is diffuse with events extending to depths of nearly 30 km, and there is a minimum in activity near a depth of 15 km. The fault plane solutions exhibit a wide spectrum of fault types and orientations and are not consistent with simple zones of shortening or extension. Neither tractions applied to the edges or bottom of the region nor deviatoric stresses that compensate for lateral variations in crustal thickness can account for the variety of fault plane solutions. We think that the complicated behavior is a manifestation of inhomogeneous deformation due, at least in part, to a pre-existing complicated juxtaposition of structures and formations.",
        "doi": "10.1016/0012-821X(83)90141-3",
        "issn": "0012-821X",
        "publisher": "Elsevier",
        "publication": "Earth and Planetary Science Letters",
        "publication_date": "1983-12",
        "volume": "66",
        "pages": "279-288"
    },
    {
        "id": "authors:h5f7j-61323",
        "collection": "authors",
        "collection_id": "h5f7j-61323",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-095209670",
        "type": "article",
        "title": "Some geometrical aspects of uncertainties in combined plate reconstructions",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann M.",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            }
        ],
        "abstract": "The uncertainties in both the position of a pole of rotation and the rotation angle describing a plate reconstruction depend not only on the number and quality of data used but also on two geometrical factors: the length of plate boundary represented by the data, and the distance from the best-fit pole to the center of the data region. We describe a simple geometrical method that can be used to calculate minimum uncertainties in reconstructions, based on positions of magnetic anomalies and fracture zones with finite uncertainties. Uncertainties in pole positions and angles corresponding to 10-km uncertainty in individual data points can, when combined, yield uncertainties in reconstructed positions greatly in excess of 10 km per rotation. For example, an uncertainty of 10 km in anomaly 6 reconstructions in the South Pacific, southeast Indian, northwest Indian, and North Atlantic Oceans would result in uncertainty of up to 190 km in the reconstructed position of the Pacific plate with respect to North America at 19.8 m.y. B.P. Existing data show that the realistic uncertainties for this case are twice as large as the calculated minimum uncertainties.",
        "doi": "10.1130/0091-7613(1983)11<697:SGAOUI>2.0.CO;2",
        "issn": "0091-7613",
        "publisher": "Geological Society of America",
        "publication": "Geology",
        "publication_date": "1983-12",
        "series_number": "12",
        "volume": "11",
        "issue": "12",
        "pages": "697-701"
    },
    {
        "id": "authors:9nak4-5dq03",
        "collection": "authors",
        "collection_id": "9nak4-5dq03",
        "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20140908-091504745",
        "type": "article",
        "title": "Uncertainties in the relative positions of the Australia, Antarctica, Lord Howe, and Pacific Plates since the Late Cretaceous",
        "author": [
            {
                "family_name": "Stock",
                "given_name": "Joann",
                "orcid": "0000-0003-4816-7865",
                "clpid": "Stock-J-M"
            },
            {
                "family_name": "Molnar",
                "given_name": "Peter",
                "clpid": "Molnar-P"
            }
        ],
        "abstract": "We determined parameters that describe finite rotations and their uncertainty regions for relative plate motion at the spreading centers between the Pacific and Antarctica plates, between Australia and Antarctica, and between the Lord Howe Rise and Australia. We combined these to yield a range of possible finite rotations describing the relative positions of the Pacific, Australia, Antarctica, and Lord Howe plates since the Late Cretaceous. If the Pacific-Australia plate boundary has had its present trend since anomaly 18 time, reconstructions show 330\u00b1110 km of motion of the Pacific plate relative to the Lord Howe Rise since anomaly 5 time (9.8 m.y.), 420\u00b1110 km since anomaly 6 time (19.5 m.y.), 770\u00b1330 km since anomaly 13 time (35.6 m.y.), and 820\u00b1260 km since anomaly 18 time (43.0 m.y.). We examined two cases for times prior to anomaly 18, assuming a Late Cretaceous age of Australia-Antarctica separation. If a plate boundary existed between the Lord Howe Rise and Pacific plates since the Late Cretaceous, with no plate boundary in Antarctica, reconstructions with the Lord Howe Rise fixed predict 610 \u00b1 200 km of westward motion of the Pacific plate between the times of anomalies 31 and 22, followed by 260\u00b1100 km of northward motion between the times of anomalies 22 and 18. If the Lord Howe Rise was fixed to the Pacific plate until the Eocene, but a plate boundary existed between East and West Antarctica, reconstructions show very little motion across this boundary between the times of anomalies 31 and 22, followed by convergence between the times of anomalies 22 and 18. This second case also brings 70\u201380 m.y. paleomagnetic poles from the Pacific and East Antarctica plates into better agreement than the first case, but large uncertainties in the reconstructions do not allow the first case to be conclusively eliminated.",
        "doi": "10.1029/JB087iB06p04697",
        "issn": "0148-0227",
        "publisher": "American Geophysical Union",
        "publication": "Journal of Geophysical Research B",
        "publication_date": "1982-06-10",
        "series_number": "B6",
        "volume": "87",
        "issue": "B6",
        "pages": "4697-4714"
    }
]