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Titlebook: Atomic Masses and Fundamental Constants 6; Jerry A. Nolen,Walter Benenson Book 1980 Springer Science+Business Media New York 1980 Atomic m

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期刊全稱Atomic Masses and Fundamental Constants 6
影響因子2023Jerry A. Nolen,Walter Benenson
視頻videohttp://file.papertrans.cn/165/164744/164744.mp4
圖書封面Titlebook: Atomic Masses and Fundamental Constants 6;  Jerry A. Nolen,Walter Benenson Book 1980 Springer Science+Business Media New York 1980 Atomic m
影響因子The Sixth International Conference on Atomic Masses was held in East Lansing, Michigan, Sept. 18-21, 1979. The conference was initiated, organized, and sponsored by the Commission on Atomic Masses and Fundamental Constants of the International Union of Pure and Applied Physics. The members of the conference committee are listed below: W. Benenson, Chairman Michigan State University R. C. Barber University of-Manitoba E. R. Cohen Rockwell International Institute of Chemical Physics, V. I. Goldanskii Moscow J. C. Hardy Chalk River, Canada W. H. Johnson University of Minnesota E. Kashy Michigan State University Orsay, France R. Klapisch J. A. Nolen, Jr. Michigan State University R. G. H. Robertson Michigan State University E. Roeckl G. S. I. , Darmstadt B. N. Taylor National Bureau of Standards O. Schult IKF, Julich A. H. Wapstra IFO, Amsterdam N. Zeldes Racah Institute, Jerusalem The conference was a little different from the preceding one (in Paris, 1975) in that the fundamental constant aspects were limited to those directly related to atomic masses. The gap is to be filled by the second International Conference on Precision Measurement and Fundamental Constants which is now schedu
Pindex Book 1980
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Mass Measurements with Pion Double Charge Exchangeudy nuclei far from the line of stability. Early attempts by Gilly et al., at CERN failed because of the low pion intensities available at that time. The situation changed with the advent of high intensity pion beams at the ‘meson factories.’ DCX experiments by Burman et al.. at the Low Energy Pion
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The Shell Correction Method and Its Application to Nuclear Massesplet model is used for the macroscopic energy and the microscopic energy is calculated from the single-particle orbitals of the modified oscillator potential. Results for nuclei with A?90 are presented. Except for some closed shell nuclei, the discrepancies between experimental and theoretical shell
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Masses from Inhomogeneous Partial Difference Equations; A Shell-Model Approach for Light and Medium-ate difference operator D and calculate κ(N,Z) = D M(N,Z). The inhomogeneous partial difference equation . contains the original mass equation as a special solution. The most general solution of eq. (1) will include solutions of the homogeneous equation which can, for example, be used to generate sh
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