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Enriching the Standard Model With a family of CP even and odd Higgs fields IAS School Jan 13, 2012 Nanyang Technological University Singapore
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The Standard Model Lagrangian
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The Yukawa Coupling lepton
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Enriching the Standard Model Lepton
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The New Higgs Field symmetric Anti- symmetric
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Fermion Mass Matrix Results by Gupta
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Fermion Mass Matrix
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Cabibbo Kobayashi-Maskawa Matrix Results by Gupta
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Lepton Mass Matrix
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Symmetric Lepton Mass Matrix
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Transformation to Mass Eigenstates
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See-Saw Mechanism Flavor Neutrino Mass Matrix
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See-Saw Mechanism Flavor Neutrino Mass Matrix
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and the is the diagonal mass matgrix for the heavy right-handed neutrinos
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Type II Degeneracy
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Type I Degeneracy
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a = - 0.0153
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PMNS Matrix
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Experimental Indications Gulsheen Ahuja
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The Higgs Potential
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Laplacian.wordpress.com
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Spontaneous Symmetry Breaking New Vacuum
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Spontaneous Symmetry Breaking Nambu-Goldstone Bosons
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Fermion Mass Matrix Mass Hierarchy
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The New Higgs Potential Tree Level Higgs Potential with minimum at new vacuum
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The New Higgs Potential New Vacuum
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The Higgs Potential Goldstone Bosons
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The Higgs Potential Physical Higgs Field Up Quark Sector
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The Higgs Potential PseudoGoldstone Bosons
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The Higgs Potential PseudoGoldstone Bosons
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Soft Breaking Terms Markos Maniatis
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Flavor Diagonality Flavor Changing Amplitude
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FCNC condition
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Flavor Diagonality Flavor Changing Amplitude
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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.
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