Weinberg, S.; Non-Abelian Gauge Theories of the Strong Interactions
Phys. Rev. Lett. 31 (1973) 494;
Abstracts
A class of non-Abelian gauge theories of strong interactions is described, for which parity and strangeness are automatically conserved, and for which the nonconservations of parity and strangeness produced by weak interactions are automatically of order /mW2 rather than of order . When such theories are "asymptotically free,'' the order- weak correction
to natural zeroth-order symmetries may be calculated ignoring all effects of strong interactions. Speculations are offered on a possible theory of quarks.
Related references More (earlier) information appears in D. J. Gross and F. Wilczek, Phys. Rev. Lett. 30 (1973) 1343;
H. D. Politzer, Phys. Rev. Lett. 30 (1973) 1346;
See also S. Weinberg, Phys. Rev. Lett. 29 (1972) 1698;
S. L. Glashow, R. Jackiw, and S. S. Shei, Phys. Rev. 187 (1969) 1416;
H. Gregori and S. L. Glashow, Phys. Rev. D8 (1973) 2457;
K. Wilson, Phys. Rev. 179 (1969) 1499;
C. G. Callan, Phys. Rev. D5 (1972) 3202;
S. L. Glashow and S. Weinberg, Phys. Rev. Lett. 20 (1968) 224;
M. Gell-Mann, R. J. Oakes, and B. Renner, Phys. Rev. 175 (1968) 2195;
S. Weinberg, Phys. Rev. Lett. 29 (1972) 338;
I. Bars, M. B. Halpern, and M. Yoshimura, Phys. Rev. Lett. 29 (1972) 969;
H. Gregori and S. L. Glashow, Phys. Rev. D6 (1972) 2977;
Record comments
Final formulation of QCD and the Standard Model Lagrangian.