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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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