We make the simple observation that there exists a universal unitarity triangle for all models, like the SM, the Two Higgs Doublet Models I and II and the MSSM with minimal flavour violation, that do not have any new operators beyond those present in the SM and in which all flavour changing transitions are governed by the CKM matrix with no new phases beyond the CKM phase. This universal triangle can be determined in the near future from the ratio (ΔM)d/(ΔM)s and sin2β measured first through the CP asymmetry in Bd0→ψKS and later in decays. Also suitable ratios of the branching ratios for and Bd,s→μ+μ− and the angle γ measured by means of CP asymmetries in B decays can be used for this determination. Comparison of this universal triangle with the nonuniversal triangles extracted in each model using ε, (ΔM)d and various branching ratios for rare decays will allow to find out in a transparent manner which of these models, if any, is singled out by experiment. A virtue of the universal triangle is that it allows to separate the determination of the CKM parameters from the determination of new parameters present in the extensions of the SM considered here.

Universal unitarity triangle and physics beyond the standard model

GAMBINO, Paolo;
2001-01-01

Abstract

We make the simple observation that there exists a universal unitarity triangle for all models, like the SM, the Two Higgs Doublet Models I and II and the MSSM with minimal flavour violation, that do not have any new operators beyond those present in the SM and in which all flavour changing transitions are governed by the CKM matrix with no new phases beyond the CKM phase. This universal triangle can be determined in the near future from the ratio (ΔM)d/(ΔM)s and sin2β measured first through the CP asymmetry in Bd0→ψKS and later in decays. Also suitable ratios of the branching ratios for and Bd,s→μ+μ− and the angle γ measured by means of CP asymmetries in B decays can be used for this determination. Comparison of this universal triangle with the nonuniversal triangles extracted in each model using ε, (ΔM)d and various branching ratios for rare decays will allow to find out in a transparent manner which of these models, if any, is singled out by experiment. A virtue of the universal triangle is that it allows to separate the determination of the CKM parameters from the determination of new parameters present in the extensions of the SM considered here.
2001
500
161
167
http://www.sciencedirect.com/science/article/pii/S0370269301000612
A.J. Buras; P. Gambino; M. Gorbahn; S. Jäger; L. Silvestrini
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/104652
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