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Two-Higgs-doublet model
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Two-Higgs-doublet model : ウィキペディア英語版
Two-Higgs-doublet model
In particle physics, a two-Higgs-doublet model (2HDM) is an extension of the Standard Model in which a second Higgs doublet is added.
The addition of the second Higgs doublet leads to five physical states: the CP even neutral Higgs bosons h and H (where H is heavier than h by convention),
the CP odd pseudoscalar A and two charged Higgs bosons H^\pm. Such a model has six free parameters: four Higgs masses (m_h, m_H, m_A, m_), the ratio of the
two vacuum expectation values (\tan \beta) and a mixing angle (\alpha).
A special case is when \cos(\beta - \alpha) = 0, the so-called ''alignment limit'', in which the lighter CP even Higgs boson h has couplings like the Higgs boson of the Standard Model.
== Classification ==
Two-Higgs-doublet models can introduce Flavor-changing neutral currents which have not been observed so far.
The Glashow-Weinberg condition, requiring that each group of fermions (up-type quarks, down-type quarks and charged leptons)
couples exactly to one of the two doublets, is sufficient to avoid the prediction of flavor-changing neutral currents.
Depending on which type of fermions couples to which doublet \Phi, one can divide two-Higgs-doublet models into the following classes:
By convention, \Phi_2 is the doublet to which up-type quarks couple.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Two-Higgs-doublet model」の詳細全文を読む



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