Effective-lagrangian theory of broken chiralSU 3×SU 3
Author:
Publisher
Springer Science and Business Media LLC
Subject
General Physics and Astronomy
Link
http://link.springer.com/content/pdf/10.1007/BF02753991.pdf
Reference9 articles.
1. S. Weinberg:Phys. Rev.,166, 1568 (1968).
2. M. Gell-Mann, R. J. Oakes andB. Renner:Phys. Rev.,175, 2195 (1968).
3. A. J. Macfarlane andP. H. Weisz:Nuovo Cimento,55 A, 853 (1968).
4. Note thatColeman et al. (1) show that the only linear representations ofK 3, which can be realized by functions of theM i only, are of the type (R, R*)+(R*, R),i.e. (8, 1)+(1, 8) is excluded.
5. J. A. Cronin:Phys. Rev.,161, 1463 (1967).
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1. Meson-baryon scattering lengths in a chiral Lagrangian model;Physical Review D;1977-07-01
2. Generalized Nonlinear Lagrangian for Pseudoscalar and Scalar Mesons;Physical Review D;1973-07-15
3. Scalar mesons and symmetry breaking in SU(3) × SU(3) non-linear models;Nuclear Physics B;1972-10
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