Changes between Version 67 and Version 68 of ALRM
 Timestamp:
 04/26/16 01:16:41 (4 years ago)
Legend:
 Unmodified
 Added
 Removed
 Modified

ALRM
v67 v68 26 26 gauge bosons (W' and Z') correspond to the SU(2)_R group. 27 27 28 The leftright symmetry is broken to the SM SU(2)_L×U(1)_Y, Y being the hypercharge, by the SU(2)_Rdoublet vev, then the electroweak symmetry is broken to the U(1)_em through the bidoublet and the SU(2)_ Rdoublet vevs. Accordingly, all ferminos and gauge bosons (except of course photon) become massive through the socalled Higgs mechanism.28 The leftright symmetry is broken to the SM SU(2)_L×U(1)_Y, Y being the hypercharge, by the SU(2)_Rdoublet vev, then the electroweak symmetry is broken to the U(1)_em through the bidoublet and the SU(2)_Ldoublet vevs. Accordingly, all ferminos and gauge bosons (except of course photon) become massive through the socalled Higgs mechanism. 29 29 30 30 Dirac (massive) neutrinos are considered with the mixing MNS matrix implemented with the normal hierarchy. Three mixed generations of quarks is considered and hence the general case of the CKM matrix is implemented. In addition, it was considered that the leftright symmetry is manifest, that is the left and right MNS and CKM mixing matrices are coincident. However, this can be to be generalized directly.