Abstract

A general analysis of possible violation of CP in processes like tau rightarrow Kpi nu , for unpolarized tau is presented. In this paper, we derive the new contributions to the effective Hamiltonian governs vert Delta S vert =1 semileptonic tau decays in the framework of two Higgs doublet model with generic Yukawa structure and Leptoquarks models. Within these models, we list all operators, in the effective Hamiltonian and provide analytical expression for their corresponding Wilson coefficients. Moreover, we analyze the role of the different contributions, originating from the scalar, vecor and tensor hadronic currents, in generating direct CP asymmetry in the decay rate of tau ^-rightarrow K^-pi ^0nu _tau . We show that non vanishing direct CP asymmetry in the decay rate of tau ^-rightarrow K^-pi ^0nu _tau can be generated due to the presence of both, the weak phase in the Wilson coefficient corresponding to the tensor operator and the strong phase difference resulting from the interference between the form factors expressing the matrix elements of the vector and tensor hadronic currents. After taking into account all relevant constraints, we find that the generated direct CP asymmetry is of order 10^{-8} which is several orders of magnitude larger than the standard model prediction. We show also that, in two Higgs doublet model with generic Yukawa structure , direct local or non integrated CP violation can be as large as 0.3 % not far from experimental possibilities. This kind of asymmetry can be generated due to the interference between vector and scalar contributions with different weak phases which is not the case in the SM.

Highlights

  • The most evident fail of the Standard Model (SM) is the absence of a mechanism to explain baryogenesis, even if all CP violation (CPV) processes measured are consistent with SM predictions [1,2,3,4,5,6,7,8,9,10]

  • Switching off new physics (NP) contributions to the differential decay width, we show in Sects. 3 and 4 that no direct CP asymmetry in the decay rate of τ − → K −π 0ντ can be generated in the SM at tree-level

  • We investigate the direct CP asymmetry for a general new physics model that can contribute to the effective Hamiltonian in Eq (3) with Wilson coefficients denoted by CiN P

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Summary

Introduction

The most evident fail of the Standard Model (SM) is the absence of a mechanism to explain baryogenesis, even if all CP violation (CPV) processes measured are consistent with SM predictions [1,2,3,4,5,6,7,8,9,10]. As it is well known, to have direct CPV one needs two interfering contributions with different weak and strong phases In these decays once the angular integral is done the interfering signal vanish. From the expression of SM , direct CP asymmetry in the decay rate will vanish due to the absence of the weak phase, CVSM is real, and due to the remark that the form factors f+(s) and f0(s) do not interfere and the relative strong phase essential for CP asymmetry vanishes. To generate no vanishing CP asymmetry in the decay rate within SM, it is essential to consider higher order terms contributing to the amplitude as done in Ref.

Integrated CP violation asymmetries
H S v mτ sin β 4π 2m2H Vus
Nonintegrated CP violation asymmetries
Conclusion
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