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AbstractAbstract
[en] The predictions of the standard model (solar and electroweak) for solar neutrino experiments will be described, with special emphasis on quantitative estimates of the uncertainties in the predictions. An argument--which uses detailed Monte Carlo studies of the solar-model-predictions--will be presented which demonstrates that the existing solar neutrino experiments cannot be reconciled unless new weak interaction physics changes the shape of the 8Be neutrino energy spectrum. Additional arguments that suggest that new physics is required will be summarized. The predictions for next-generation experiments that are independent of details of solar models will be highlighted. An urgent appeal will be made for performing a measurement of the p(7Be, γ)8B reaction using a radioactive beam of 7Be
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Fall meeting of the Division of Nuclear Physics of the American Physical Society; Pacific Grove, CA (United States); 20-23 Oct 1993; CONF-931044--
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No abstract available
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de Boer, J. (ed.); p. 681-716; 1973; American Elsevier Publishing Co., Inc; New York; International conference on nuclear physics; Munich, F.R. Germany; 27 Aug 1973
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Book
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No abstract available
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Melissinos, A. C. (ed.); p. 243-246; 1971; American Inst. of Physics; New York; Meeting on particles and fields; Rochester, N. Y; 30 Aug 1971
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Book
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[en] The general features of the galactic environment of the solar system are described. The principal components of the distribution of matter in the solar vicinity are discussed. Special emphasis is placed upon the question of determining the total amount of matter in the vicinity of the sun
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Smoluchowski, R.; Bahcall, J.M.; Matthews, M.S; p. 3-12; 1986; p. 3-12; University of Arizona Press; Tucson, AZ (USA)
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Book
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No abstract available
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Astrophysical Journal; v. 172(2); p. 265-282
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No abstract available
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Astrophysical Journal; v. 179(3); p. 699-703
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[en] To predict the likely distribution of stars around a massive black hole in the core of a cluster of stars, an equation of the Fokker-Planck type is derived that describes the diffusion of stars in the 1/r gravitational well of the black hole, by star-star gravitational collisions. The main assumptions are: (1) the distribution of stars is described by a single-particle distribution function that is shperically symmetric in coordinate space and approximately isotropic in velocity space; (2) the stars have equal masses; (3) star mass very-much-less-thanblack-hole massvery-much-less-thancluster-core mass; (4) a star is destroyed by star-star collisions or by tidal forces when its binding energy in the well exceeds a specified large value; (5) binaries are unimportant. Numerical solutions for the time-dependent equations indicate that the equilibrium star density, closely approached within a collision time, approximates an r-7/4 power law throughout most of the well. The same equilibrium power law obtains for nonisotropic distribution functions whose anisotropy is independent of r. Stars in bound orbits about a black hole diffuse slowly into its gravitational well under equilibrium conditions. A black hole of approximately-less-than103 M/sub sun/ may accrete stars primarily by capture from unbound orbits.Theshape of the star distribution near the cluster center that might be observed with small diaphragms is predicted. As a function of diaphragm size, the velocity dispersion and line profile that might be measured spectroscopically is calculated. Some calculations are also presented for an open slit configuration. For globular clusters in our Galaxy, one might be able to detect black holes with masses approximately-greater-than5 x 103 M/sub sun/ and, with a large space telescope, masses approximately-greater-than103 M/sub sun/. An approximate formula for the mean distance of a massive black hole from the center of mass of the unbound stars is also presented
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Astrophysical Journal; v. 209(1); p. 214-232
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No abstract available
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Astrophysical Journal; v. 179(2); p. 381-389
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No abstract available
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Astrophysical Journal; v. 178(1); p. L1-L4
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No abstract available
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Comments on Astrophysics and Space Physics; v. 4(4); p. 95-99
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