Weak global symmetry
Author:
Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Link
http://link.springer.com/content/pdf/10.1007/BF02860196.pdf
Reference10 articles.
1. R. Feynman andM. Gell-Mann:Phys. Rev.,109, 193 (1958).
2. M. Gell-Mann andA. H. Rosenfeld:Ann. Rev. Nucl. Sci.,7, 407 (1957). The earlier literature can be traced back from this source.
3. The evidence and theory is reviewed byR. H. Dalitz:Rev. Mod. Phys.,31, 823 (1959).
4. See alsoR. L. Cool, B. Cork, J. W. Cronin andW. A. Wenzel:Phys. Rev.,114, 912 (1959).
5. S. Okubo, R. E. Marshak, E. C. G. Sudarshan, W. B. Teutsch andS. Weinberg:Phys. Rev.,112, 665 (1958). This rule implies a definite relation between the K 0 2 and K+ decay rates:R(K 0 2 →π±+e∓+ν)=2R(K+→π0+e++ν), and similarly for μ-meson decay modes.
Cited by 38 articles. 订阅此论文施引文献 订阅此论文施引文献，注册后可以免费订阅5篇论文的施引文献，订阅后可以查看论文全部施引文献
1. Possible lines of research into weak-interaction effects in atomic physics;Uspekhi Fizicheskih Nauk;1976
2. Search for RareK+Decays. II.K+→π+νν¯;Physical Review D;1973-12-01
3. A theory of universal weak interaction of leptons;Lettere al Nuovo Cimento;1972-08
4. Limits on theK+→π++ν+ν¯andK+→π++nγDecay Rates;Physical Review D;1971-07-01
5. Broken SU(3) as a Particle Symmetry**Supported in part by the National Science Foundation.;Group Theory and its Applications;1968
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