Changes between Version 54 and Version 55 of ALRM


Ignore:
Timestamp:
Apr 25, 2016, 3:18:42 PM (8 years ago)
Author:
Mustafa Ashry
Comment:

--

Legend:

Unmodified
Added
Removed
Modified
  • ALRM

    v54 v55  
    3333The 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.
    3434
    35 The case of (massive) Dirac is considered with the MNS matrix is implemented with the normal hierarchy. Three mixed generation of quarks is considered.
     35Dirac (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.
    3636
    3737The model contains ten physical Higgs bosons: four neutral CP-even higgs bosons, one (the lightest) of which is fixed to have a mass mh=125 GeV. Four charged Higgs bosons and two CP-odd pseudoscalar Higgs bosons. The mass spectrum is calculated and the rotation matrices are implemented analytically.