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Spectrum and couplings of SO(5) x U(1) gauge-Higgs unification model in warped spacetime Yutaka Sakamura (Osaka Univ.) with Yutaka Hosotani (Osaka Univ.) Phys.Lett.B645 (2007) 442 March 2, 2007@KEK B-L
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Introduction Structure of EW : unspecified yet Standard Higgs mechanism Little Higgs model (N.Arkani-Hamed, et al., JHEP 0208 (2002) 021 ) Higgsless model (C.Csaki, et al., PRD69 (2004) 055006) Gauge-Higgs unification model (GHU) (N.Manton, NPB158 (1979)141, D.B.Fairlie, PLB82(1979)97,…)
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Introduction Structure of EW : unspecified yet Standard Higgs mechanism Little Higgs model (N.Arkani-Hamed, et al., JHEP 0208 (2002) 021 ) Higgsless model (C.Csaki, et al., PRD69 (2004) 055006) Gauge-Higgs unification model (GHU) (N.Manton, NPB158 (1979)141, D.B.Fairlie, PLB82(1979)97,…) In GHU, Higgs mass is protected by Higher dimensional gauge symmetry
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spacetime: 5D flat ( ) gauge symmetry: Simplest model (SU(3) model)
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Z -Orbifold Parity Orbifold conditions: 2
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Higgs doublet
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(gauge-invariant) Wilson line phase determined by quantum effect
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Relations among mass scales
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Warped spacetime Randall, Sundrum, PRL83 (1999) 3370
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Relations among mass scales (warped case) (Hosotani, Mabe, PLB615 (2005) 257)
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Problem of SU(3) model Wrong value of the Weinberg angle Rho parameter deviates from one.
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Problem of SU(3) model Wrong value of the Weinberg angle Rho parameter deviates from one.
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Problem of SU(3) model Wrong value of the Weinberg angle Rho parameter deviates from one.
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SO(5) x U(1) model B-L Gauge fields: Agashe,Contino,Pomarol, NPB719(2005)165
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5D action
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Symmetry breaking
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Higgs doublet
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Symmetry breaking
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Higgs doublet: By using residual symemtry, Wilson line phase:
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Mass spectrum W boson: Z boson:
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Weak gauge boson masses
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Gauge couplings Weinberg angle Rho parameter
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WWZ Coupling SM value
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WWH, ZZH couplings
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Summary SO(5) x U(1) model in warped spacetime B-L
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Future work Specify the fermionic sector. Include the quantum effects. Determine the value of dynamically.
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