Changes between Version 57 and Version 58 of ALRM
- Timestamp:
- Apr 25, 2016, 3:25:26 PM (8 years ago)
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ALRM
v57 v58 31 31 gauge bosons (W' and Z') correspond to the SU(2)_R group. 32 32 33 The left-right symmetry is broken to the SM SU(2)_L×U(1)_Y, Y being the hypercharge, by the SU(2)_R-doublet vev, then the electroweak symmetry is broken to the U(1) electromagnetism through the bidoublet and the SU(2)_R-doublet vevs. Accordingly, all ferminos and gauge bosons (except of course photon) become massive through the so-called Higgs mechanism.33 The left-right symmetry is broken to the SM SU(2)_L×U(1)_Y, Y being the hypercharge, by the SU(2)_R-doublet vev, then the electroweak symmetry is broken to the U(1)_em through the bidoublet and the SU(2)_R-doublet vevs. Accordingly, all ferminos and gauge bosons (except of course photon) become massive through the so-called Higgs mechanism. 34 34 35 35 Dirac (massive) neutrinos are considered with the mixing MNS matrix implemented with the normal hierarchy. Three mixed generation of quarks is considered and hence the general case of the CKM matrix is implemented.
