Abstract

We point out that the recently increased value of the angle gamma in the unitarity triangle (UT), determined in tree-level decays to be gamma =(74.0^{+5.0}_{-5.8})^circ by the LHCb collaboration, combined with the most recent value of |V_{cb}| implies an enhancement of Delta M_{d} over the data in the ballpark of 30%. This is larger by roughly a factor of two than the enhancement of Delta M_{s} that is independent of gamma . This disparity of enhancements is problematic for models with constrained minimal flavour violation (CMFV) and also for U(2)^3 models. In view of the prospects of measuring gamma with the precision of pm 1^circ by Belle II and LHCb in the coming years, we propose to use the angles gamma and beta together with |V_{cb}| and |V_{us}| as the fundamental parameters of the CKM matrix until |V_{ub}| from tree-level decays will be known precisely. Displaying Delta M_{s,d} as functions of gamma clearly demonstrates the tension between the value of gamma from tree-level decays, free from new physics (NP) contributions, and Delta M_{s,d} calculated in CMFV and U(2)^3 models and thus exhibits the presence of NP contributions to Delta M_{s,d} beyond these frameworks. We calculate the values of |V_{ub}| and |V_{td}| as functions of gamma and |V_{cb}| and discuss the implications of our results for varepsilon _K and rare K and B decays. We also briefly discuss a future strategy in which beta , possibly affected by NP, is replaced by |V_{ub}|.

Highlights

  • The F = 2 transitions in the down-quark sector, that is Bs0,d − Bs0,d and K 0 − K 0 mixings, have been vital in constraining the standard model (SM) and in the search for new physics (NP) for several decades [1,2]

  • Displaying Ms,d as functions of γ clearly demonstrates the tension between the value of γ from tree-level decays, free from new physics (NP) contributions, and Ms,d calculated in constrained minimal flavour violation (CMFV) and U (2)3 models and exhibits the presence of NP contributions to Ms,d beyond these frameworks

  • In view of the improved value of γ, we decided to use it as an input in the present analysis, instead of the usual determination of the unitarity triangle (UT) in CMFV models through Sψ KS (β) and the side Rt of the UT determined from the ratio Md / Ms and ξ in (9)

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Summary

Introduction

On the other hand the tree-level determination of the angle γ has significantly been improved in the last years by various measurements of the LHCb collaboration, with the latest average being [5]1 γ = (74.0−+55..80)◦. This number has not changed with respect to our 2016 analysis, and displays a 1.8σ tension with the improved tree level measurement in (4).. In view of the improved value of γ , we decided to use it as an input in the present analysis, instead of the usual determination of the UT in CMFV models through Sψ KS (β) and the side Rt of the UT determined from the ratio Md / Ms and ξ in (9).

Deriving the UT and the CKM matrix
Calculating observables
Going beyond CMFV
Findings
Summary
Full Text
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