Changes between Version 91 and Version 92 of ALRM

Timestamp:

May 28, 2016, 9:04:30 PM (8 years ago)

Author:

Mustafa Ashry

Comment:

--

ALRM

@@ -29 +29 @@
 Dirac (massive) neutrinos are considered with the mixing MNS matrix implemented in the normal hierarchy. The case of Majorana neutrinos is considered in many other models' files and can be brought to be implemented here easily. Three mixed generations of quarks are considered and hence the general case of the CKM matrix is implemented. In addition, it was considered that the left-right symmetry is manifest, that is the left and right MNS and CKM mixing matrices are coincident. However, this can be generalized directly.
 
-The 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.
+The model contains ten physical Higgs bosons: four neutral ''CP''-even higgs bosons, one (the lightest) of which is considered to be the SM-like one with mass fixed to have the value ''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.
 
 Minimization conditions and spectrum relations are all used to express the whole model parameters and spectra in terms of only five independent (external) parameters: ''tanbeta, lambda_2, lambda_3, alpha_1, alpha_2''. As in any two-Higgs doublet model, e.g., MSSM, ''tanbeta'' is the ratio between two vevs. The parameters ''lambda_2, lambda_3, alpha_1, alpha_2'' are dimensionless potential parameters. The charged Higgs masses are implemented as external parameters.