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A.", "clpid": "Rubi\u00f1o-Martin-J-A" }, { "family_name": "Rusholme", "given_name": "B.", "orcid": "0000-0001-7648-4142", "clpid": "Rusholme-Benjamin" }, { "family_name": "Sandri", "given_name": "M.", "clpid": "Sandri-M" }, { "family_name": "Santos", "given_name": "D.", "clpid": "Santos-D" }, { "family_name": "Savelainen", "given_name": "M.", "clpid": "Savelainen-M" }, { "family_name": "Savini", "given_name": "G.", "clpid": "Savini-G" }, { "family_name": "Schwarz", "given_name": "R.", "clpid": "Schwarz-R" }, { "family_name": "Scott", "given_name": "D.", "orcid": "0000-0002-6878-9840", "clpid": "Scott-Douglas" }, { "family_name": "Seiffert", "given_name": "M. D.", "clpid": "Seiffert-M-D" }, { "family_name": "Sheehy", "given_name": "C. D.", "clpid": "Sheehy-C-D" }, { "family_name": "Spencer", "given_name": "L. D.", "clpid": "Spencer-L-D" }, { "family_name": "Staniszewski", "given_name": "Z. K.", "clpid": "Staniszewski-Z-K" }, { "family_name": "Stolyarov", "given_name": "V.", "clpid": "Stolyarov-V" }, { "family_name": "Sudiwala", "given_name": "R.", "clpid": "Sudiwala-R" }, { "family_name": "Sunyaev", "given_name": "R. A.", "clpid": "Sunyaev-R-A" }, { "family_name": "Sutton", "given_name": "D.", "clpid": "Sutton-D" }, { "family_name": "Suur-Uski", "given_name": "A.-S.", "clpid": "Suur-Uski-A-S" }, { "family_name": "Sygnet", "given_name": "J.-F.", "clpid": "Sygnet-J-F" }, { "family_name": "Tauber", "given_name": "J. A.", "clpid": "Tauber-J-A" }, { "family_name": "Teply", "given_name": "G. P.", "clpid": "Teply-G-P" }, { "family_name": "Terenzi", "given_name": "L.", "clpid": "Terenzi-L" }, { "family_name": "Thompson", "given_name": "K. L.", "clpid": "Thompson-K-L" }, { "family_name": "Toffolatti", "given_name": "L.", "clpid": "Toffolatti-L" }, { "family_name": "Tolan", "given_name": "J. E.", "clpid": "Tolan-J-E" }, { "family_name": "Tomasi", "given_name": "M.", "clpid": "Tomasi-M" }, { "family_name": "Tristram", "given_name": "M.", "clpid": "Tristram-M" }, { "family_name": "Tucci", "given_name": "M.", "clpid": "Tucci-M" }, { "family_name": "Turner", "given_name": "A. D.", "clpid": "Turner-A-D" }, { "family_name": "Valenziano", "given_name": "L.", "clpid": "Valenziano-L" }, { "family_name": "Valiviita", "given_name": "J.", "clpid": "Valiviita-J" }, { "family_name": "Van Tent", "given_name": "B.", "clpid": "Van-Tent-B" }, { "family_name": "Vibert", "given_name": "L.", "clpid": "Vibert-L" }, { "family_name": "Vielva", "given_name": "P.", "clpid": "Vielva-P" }, { "family_name": "Vieregg", "given_name": "A. G.", "clpid": "Vieregg-A-G" }, { "family_name": "Villa", "given_name": "F.", "clpid": "Villa-F" }, { "family_name": "Wade", "given_name": "L. A.", "clpid": "Wade-L-A" }, { "family_name": "Wandelt", "given_name": "B. D.", "orcid": "0000-0002-5854-8269", "clpid": "Wandelt-Benjamin-D" }, { "family_name": "Watson", "given_name": "R.", "clpid": "Watson-R" }, { "family_name": "Weber", "given_name": "A. C.", "clpid": "Weber-A-C" }, { "family_name": "Wehus", "given_name": "I. K.", "clpid": "Wehus-I-K" }, { "family_name": "White", "given_name": "M.", "clpid": "White-M" }, { "family_name": "White", "given_name": "S. D. M.", "clpid": "White-S-D-M" }, { "family_name": "Willmert", "given_name": "J.", "clpid": "Willmert-J" }, { "family_name": "Wong", "given_name": "C. L.", "clpid": "Wong-C-L" }, { "family_name": "Yoon", "given_name": "K. W.", "clpid": "Yoon-K-W" }, { "family_name": "Yvon", "given_name": "D.", "clpid": "Yvon-D" }, { "family_name": "Zacchei", "given_name": "A.", "clpid": "Zacchei-A" }, { "family_name": "Zonca", "given_name": "A.", "clpid": "Zonca-A" }, { "literal": "Planck Collaboration" }, { "literal": "BICEP2 Collaboration" } ], "abstract": "We report the results of a joint analysis of data from BICEP2/Keck Array and Planck. BICEP2 and Keck Array have observed the same approximately 400\u2009\u2009deg2 patch of sky centered on RA 0 h, Dec. \u221257.5\u00b0. The combined maps reach a depth of 57 nK deg in Stokes Q and U in a band centered at 150 GHz. Planck has observed the full sky in polarization at seven frequencies from 30 to 353 GHz, but much less deeply in any given region (1.2\u2009\u2009\u03bcK deg in Q and U at 143 GHz). We detect 150\u00d7353 cross-correlation in B modes at high significance. We fit the single- and cross-frequency power spectra at frequencies \u2265150\u2009\u2009GHz to a lensed-\u039bCDM model that includes dust and a possible contribution from inflationary gravitational waves (as parametrized by the tensor-to-scalar ratio r), using a prior on the frequency spectral behavior of polarized dust emission from previous Planck analysis of other regions of the sky. We find strong evidence for dust and no statistically significant evidence for tensor modes. We probe various model variations and extensions, including adding a synchrotron component in combination with lower frequency data, and find that these make little difference to the r constraint. Finally, we present an alternative analysis which is similar to a map-based cleaning of the dust contribution, and show that this gives similar constraints. The final result is expressed as a likelihood curve for r, and yields an upper limit r0.05<0.12 at 95% confidence. Marginalizing over dust and r, lensing B modes are detected at 7.0\u03c3 significance.", "doi": "10.1103/PhysRevLett.114.101301", "issn": "0031-9007", "publisher": "American Physical Society", "publication": "Physical Review Letters", "publication_date": "2015-03-09", "series_number": "10", "volume": "114", "issue": "10", "pages": "Art. No. 101301" }, { "id": "authors:15vw0-hb528", "collection": "authors", "collection_id": "15vw0-hb528", "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110104-104430745", "type": "article", "title": "Experimental spectroscopic temperature measurement in the reflected wave region of a shock tube using the OH^2\u2211 \u2192 ^2\u03a0 band system", "author": [ { "family_name": "Watson", "given_name": "Ronald", "clpid": "Watson-R" } ], "abstract": "Experimental measurements of the population temperature behind the reflected shock in a shock tube are presented. Emission from two wave length intervals of the OH^2\u2211 \u2192 ^2\u03a0 electronic band system was measured photoelectrically, the signals observed being generated by a narrow core of hot\ngas in the reflected shock region looking axially up the tube. The ratio of the rate of increase of intensity,\nper unit increase of optical depth, in the two spectral regions is a unique function of the temperature for\na transparent gas. The linearity of the signal increase with time represents an experimental verification\nof the transparency and equilibrium of the test gas.\nIn the temperature range of 3300-4300\u00b0K (M_s ~ 4), the measured spectroscopic temperature was in good agreement with the calculated equilibrium temperature, the estimated accuracy of the spectroscopic temperature being \u00b1 75\u00b0K. A relaxation time of about 25 \u00b5sec was observed for the (2,2) and (3,3) vibration bands to reach statistical equilibrium with the lower (0,0) and (1,1) vibrational levels in the ^2\u2211\nstate from which the emission occurred.", "doi": "10.1016/0022-4073(63)90036-0", "issn": "0022-4073", "publisher": "Elsevier", "publication": "Journal of Quantitative Spectroscopy and Radiative Transfer", "publication_date": "1963-07", "series_number": "3", "volume": "3", "issue": "3", "pages": "255-264" }, { "id": "authors:j609h-as617", "collection": "authors", "collection_id": "j609h-as617", "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110106-152408147", "type": "article", "title": "Procedure for reliable preparation of shock tube test gas mixtures containing water vapor", "author": [ { "family_name": "Watson", "given_name": "Ronald", "clpid": "Watson-R" } ], "abstract": "N/A", "doi": "10.1063/1.1717700", "issn": "0034-6748", "publisher": "American Institute of Physics", "publication": "Review of Scientific Instruments", "publication_date": "1962-10", "series_number": "10", "volume": "33", "issue": "10", "pages": "1113-1114" }, { "id": "authors:jp0h3-gsq02", "collection": "authors", "collection_id": "jp0h3-gsq02", "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110106-131913150", "type": "article", "title": "Temperature measurement on the OH ^2\u03a3\u2192^2\u03a0 band system for a transparent gas in a shock tube", "author": [ { "family_name": "Watson", "given_name": "Ronald", "clpid": "Watson-R" } ], "abstract": "N/A", "doi": "10.1016/0022-4073(62)90006-7", "issn": "0022-4073", "publisher": "Elsevier", "publication": "Journal of Quantitative Spectroscopy and Radiative Transfer", "publication_date": "1962-07", "series_number": "3", "volume": "2", "issue": "3", "pages": "301-303" }, { "id": "authors:1mprq-tbj76", "collection": "authors", "collection_id": "1mprq-tbj76", "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110106-135634209", "type": "article", "title": "Reduction of ultraviolet scattering from a continuous light source in a littrow type monochromator", "author": [ { "family_name": "Watson", "given_name": "Ronald", "clpid": "Watson-R" } ], "abstract": "Quantitative spectroscopic experiments in shock tubes such as f-number measurements [for example (1)] require an absolute calibration of the optical system, monochromator, and detector. This is very often done for ultraviolet transitions around 3000-3500A with a tungsten strip filament lamp for which emissivities are known (2).", "doi": "10.1366/000370262774416164", "issn": "0003-7028", "publisher": "Society for Applied Spectroscopy", "publication": "Applied Spectroscopy", "publication_date": "1962-05", "series_number": "5", "volume": "16", "issue": "5", "pages": "164-165" }, { "id": "authors:rz0ga-7sp02", "collection": "authors", "collection_id": "rz0ga-7sp02", "cite_using_url": "https://resolver.caltech.edu/CaltechAUTHORS:20110111-082616427", "type": "article", "title": "Effect of scale size on a rocket engine with suddenly frozen nozzle flow", "author": [ { "family_name": "Watson", "given_name": "Ronald", "clpid": "Watson-R" } ], "abstract": "Recent analytical work by Bray indicates that single\nelement, chemically reacting systems, e.g., H_2 \u21cb 2H, may\nsuddenly freeze their composition at some point in a high\nspeed nozzle and then remain at fixed composition\nthroughout the remainder of the expansion. This sudden\nfreezing or \"quenching\" phenomenon was also apparent\nin some theoretical calculations reported by Hall et al.\nand has been verified experimentally by Wegener. It\nis the purpose of this note to show qualitatively how\nBray's sudden-freezing criterion is related to engine size\nby the scale factor for geometrically similar engines having\nn on equilibrium nozzle flows and in which a propellant\nsystem is used for which Bray's analysis is valid.", "issn": "0097-4056", "publisher": "American Rocket Society", "publication": "ARS Journal", "publication_date": "1961-03", "series_number": "3", "volume": "31", "issue": "3", "pages": "452-453" } ]