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Electroweak baryogenesis and quantum corrections to the triple Higgs boson coupling

Shinya Kanemura, Yasuhiro Okada, Eibun Senaha

Abstract

A phenomenological consequence of electroweak baryogenesis is studied in connection with the Higgs physics. In a two Higgs double model, the first order phase transition can be strong enough to allow the electroweak baryogenesis due to the effect of extra Higgs bosons. We investigate the quantum correction to the triple coupling of the lightest Higgs boson in such a scenario, and find that the condition of the strong first order phase transition necessarily leads to the deviation of at least 10 percent from the standard model prediction. Such magnitude of the deviation can be identified in future $e^+e^-$ linear collider experiments. We also discuss the minimal supersymmetric standard model with the light stop scenario, and point out that a sizable correction appears in the triple coupling for successful electroweak baryogenesis.

Electroweak baryogenesis and quantum corrections to the triple Higgs boson coupling

Abstract

A phenomenological consequence of electroweak baryogenesis is studied in connection with the Higgs physics. In a two Higgs double model, the first order phase transition can be strong enough to allow the electroweak baryogenesis due to the effect of extra Higgs bosons. We investigate the quantum correction to the triple coupling of the lightest Higgs boson in such a scenario, and find that the condition of the strong first order phase transition necessarily leads to the deviation of at least 10 percent from the standard model prediction. Such magnitude of the deviation can be identified in future linear collider experiments. We also discuss the minimal supersymmetric standard model with the light stop scenario, and point out that a sizable correction appears in the triple coupling for successful electroweak baryogenesis.

Paper Structure

This paper contains 14 equations, 1 figure.

Figures (1)

  • Figure 1: The straight line stands for the critical line which satisfied the condition, $\varphi_c/T_c=1$. The dashed lines are the deviation of hhh coupling from the SM value, where $\Delta \lambda_{hhh}^{\hbox{\scriptsize{THDM}}}\equiv \lambda_{hhh}^{\hbox{\scriptsize{eff}}} (\hbox{THDM})-\lambda_{hhh}^{\hbox{\scriptsize{eff}}}(\hbox{SM})$.