Chiral electroweak gauge interactions
- Department of Physics Astronomy, Wayne State University, Detroit, MI (USA)
The hypercharge U(1){sub {ital Y}} of the standard electroweak model is split into chiral hypercharges U(1){sub {ital L}}{times}U(1){sub {ital R}}. Under the new gauge symmetry SU(2){sub {ital L}}{times}U(1){sub {ital L}}{times}U(1){sub {ital R}}, quarks and leptons are left-handed doublets transforming only under SU(2){sub {ital L}}{times}U(1){sub {ital L}} and right-handed singlets transforming only under U(1){sub {ital R}}. Consistent with the measurements of the mass of the standard massive neutral boson {ital Z}{sup 0} at the SLAC and CERN colliders and the neutral-current couplings involving neutrino beams and electron beams, the additional massive neutral gauge boson can be as light as a few hundred GeV. The model utilizes the generalized see saw mechanism of Gell-Mann, Ramond, and Slansky to give masses to all the fermions of the theory.
- DOE Contract Number:
- FG02-85ER40209
- OSTI ID:
- 6228179
- Journal Information:
- Physical Review, D (Particles Fields); (USA), Vol. 42:7; ISSN 0556-2821
- Country of Publication:
- United States
- Language:
- English
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FERMIONS
NEUTRAL-CURRENT INTERACTIONS
WEINBERG-SALAM GAUGE MODEL
U-1 GROUPS
CHIRAL SYMMETRY
COUPLING
ELECTRON BEAMS
GAUGE INVARIANCE
LAGRANGIAN FUNCTION
MASS
NEUTRINO BEAMS
STANDARD MODEL
SU-2 GROUPS
SU-3 GROUPS
SYMMETRY BREAKING
Z NEUTRAL BOSONS
BEAMS
BOSONS
ELEMENTARY PARTICLES
FIELD THEORIES
FUNCTIONS
INTERACTIONS
INTERMEDIATE BOSONS
INTERMEDIATE VECTOR BOSONS
INVARIANCE PRINCIPLES
LEPTON BEAMS
LIE GROUPS
MATHEMATICAL MODELS
PARTICLE BEAMS
PARTICLE INTERACTIONS
PARTICLE MODELS
SU GROUPS
SYMMETRY
SYMMETRY GROUPS
U GROUPS
UNIFIED GAUGE MODELS
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