Enriching the Standard Model With a family of CP even and odd Higgs fields IAS School Jan 13, 2012 Nanyang Technological University Singapore
The Standard Model Lagrangian
The Yukawa Coupling lepton
Enriching the Standard Model Lepton
The New Higgs Field symmetric Anti- symmetric
Fermion Mass Matrix Results by Gupta
Fermion Mass Matrix
Cabibbo Kobayashi-Maskawa Matrix Results by Gupta
Lepton Mass Matrix
Symmetric Lepton Mass Matrix
Transformation to Mass Eigenstates
See-Saw Mechanism Flavor Neutrino Mass Matrix
See-Saw Mechanism Flavor Neutrino Mass Matrix
and the is the diagonal mass matgrix for the heavy right-handed neutrinos
Type II Degeneracy
Type I Degeneracy
a =
PMNS Matrix
Experimental Indications Gulsheen Ahuja
The Higgs Potential
Laplacian.wordpress.com
Spontaneous Symmetry Breaking New Vacuum
Spontaneous Symmetry Breaking Nambu-Goldstone Bosons
Fermion Mass Matrix Mass Hierarchy
The New Higgs Potential Tree Level Higgs Potential with minimum at new vacuum
The New Higgs Potential New Vacuum
The Higgs Potential Goldstone Bosons
The Higgs Potential Physical Higgs Field Up Quark Sector
The Higgs Potential PseudoGoldstone Bosons
The Higgs Potential PseudoGoldstone Bosons
Soft Breaking Terms Markos Maniatis
Flavor Diagonality Flavor Changing Amplitude
FCNC condition
Flavor Diagonality Flavor Changing Amplitude
Enriching the Standard Model Implications for LHC 1.Higgs family has a rich hierarchy While some are heavy to conform to constraints from rare decays, there will be some `pseudo-Goldstone bosons’ that are low. 2.The Higgs bosons are not CP eigenstates and so there will be analogs of K L and K S oscillations. 3.The parameters of CKM matrices related to the hierarchies of Higgs family.