Changes between Version 64 and Version 65 of ALRM
 Timestamp:
 04/25/16 18:58:46 (4 years ago)
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ALRM
v64 v65 28 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. 29 29 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. 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. 31 31 32 32 The model contains ten physical Higgs bosons: four neutral CPeven higgs bosons, one (the lightest) of which is fixed to have a mass mh=125 GeV. Four charged Higgs bosons and two CPodd pseudoscalar Higgs bosons. The mass spectrum is calculated and the rotation matrices are implemented analytically.