References
T. D. Lee, S. Weinberg andB. Zumino:Phys. Rev. Lett,20, 224 (1968);T. D. Lee andB. Zumino:Phys. Rev.,163, 1667 (1966).
R. Acharya, P. Narayanaswamy andT. S. Santhanam:Phys. Rev. (to be published).
S. L. Adler:Phys. Rev.,177, 2426 (1969), footnote (11).
J. Goldstone, A. Salam andS. Weinberg:Phys. Rev.,127, 965 (1962).
I. S. Gerstein, H. J. Schnitzer andS. Weinberg:Phys. Rev.,175, 1873 (1968);I. S. Gerstein andH. J. Schnitzer:Phys. Rev.,175, 1876 (1968).
B. W. Lee:Nucl. Phys.,9 B, 649 (1969).
M. Gell-Mann, R. J. Oakes andB. Renner:Phys. Rev.,175 2195 (1969).
E.g.,R. Arnowitt,M. H. Friedman andP. Nath:Phys. Rev.,174 2008 (1968)
See,e.g.,S. Weinberg:Lectures in Brandeis Summer Institute in Theoretical Physics (New York, 1964).
The contribution from the lowest two-particle state is known in field theory. SeeS. D. Drell, A. C. Finn andA. C. Hearn:Phys. Rev.,136, B 1439 (1964).
M. Gell-Mann:Phys. Rev.,125, 1067 (1962).
This relation was first derived byS. L. Glashow andS. Weinberg:Phys. Rev. Lett,20, 224 (1968);
Breaking along the «3”-direction would perhaps be eliminated by appealing to stability conditions. See,e.g.,C. Cicogna,F. Strocchi andR. V. Caffarelli:Phys. Rev. D,1, 1197 (1970).
Such relations are now well known. See,e.g.,Y. Y. Lee:Nuovo Cimento,64A, 474 (1969);A. K. Bhargava andTulsi Dass:Phys. Rev. D,1, 649 (1970).
S. L. Adler:Phys. Rev.,137, B 1022 (1965).
W. I. Weisberger:Phys. Rev.,143, 1302 (1966).
S. Weinberg:Phys. Rev. Lett.,17, 616 (1966).
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Narayanaswamy, P. Axial-vector current-field identity and spontaneous symmetry breakdown. Lett. Nuovo Cimento 1, 185–190 (1971). https://doi.org/10.1007/BF02785084
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DOI: https://doi.org/10.1007/BF02785084