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Enriching the Standard Model With a family of CP even and odd Higgs fields IAS School Jan 10, 2012 Nanyang Technological University Singapore

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The Standard Model Lagrangian

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The Yukawa Coupling Sum over color indices suppressed Family indices

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CP transformation

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The Standard Model Lagrangian CP is manifestly broken

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The Yukawa Coupling

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Enriching the Standard Model

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Higgs fields carry the family tree

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CP transformation

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The New Higgs Field symmetric Anti- symmetric

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CP transformation

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The Yukawa Coupling

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CP transformation

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Enriching the Standard Model CP Spontaneously broken

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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 New Vacuum Original Symmetry Surviving Symmetry

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Spontaneous Symmetry Breaking Nambu-Goldstone Bosons

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Maximal CP Violation Friedberg – Lee Timeon Field

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Fermion Mass Matrix Mass Hierarchy

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Two-Generations Cabibbo Kobayashi-Maskawa Matrix

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Two-Generations Cabibbo Kobayashi-Maskawa Matrix

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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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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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W and Z masses W and Z gauge interactions unchanged

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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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