TY - JOUR
T1 - Unified gauge theories of hadrons and leptons
AU - Bars, I.
AU - Halpern, M. B.
AU - Yoshimura, M.
PY - 1973
Y1 - 1973
N2 - If we insist on SU(3) - SU(3) classification for hadrons, in the presence of the known low-lying multiplets, we are led to models of the following nature: Before spontaneous breakdown, we have two commuting gauge groups, hadronic and leptonic. This divides such models into three sectors: hadrons, leptons, and a third unconventional set of (presumably high-mass) scalar mesons which serve to connect the two "known" worlds. Spontaneous breakdown induces appropriate masses and all usual strong, weak, and electromagnetic couplings. Intimate connections are seen between these three fundamental forces.
AB - If we insist on SU(3) - SU(3) classification for hadrons, in the presence of the known low-lying multiplets, we are led to models of the following nature: Before spontaneous breakdown, we have two commuting gauge groups, hadronic and leptonic. This divides such models into three sectors: hadrons, leptons, and a third unconventional set of (presumably high-mass) scalar mesons which serve to connect the two "known" worlds. Spontaneous breakdown induces appropriate masses and all usual strong, weak, and electromagnetic couplings. Intimate connections are seen between these three fundamental forces.
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U2 - 10.1103/PhysRevD.7.1233
DO - 10.1103/PhysRevD.7.1233
M3 - Article
AN - SCOPUS:35949031049
VL - 7
SP - 1233
EP - 1251
JO - Physical review D: Particles and fields
JF - Physical review D: Particles and fields
SN - 0556-2821
IS - 4
ER -