Abstract

We scrutinize the penguin dominated $ B_s \to K^+ K^-$ decay mode involving $b \to s$ quark level transition in family non-universal $Z^ \prime$ and vector-like down quark model. There is discrepancy in the standard model branching ratio value of this mode with the experimental results reported by Belle, CDF and LHCb Collaborations. Additionally, the measured values of CP-violating asymmetries $ C_{K^+K^-}$ and $ S_{K^+K^-}$ deviate from the SM results. We constrain the new parameter space by using the existing experimental limits on leptonic $ B_s\to \ell \ell$ ($\ell = e, \mu, \tau$) processes. We then check the effects of new physics on the branching ratio and CP violating parameters of the $ B_s \to K^+ K^-$ process.

Highlights

  • The in-depth search for physics beyond the standard model (SM) plays an important role in the area of particle physics

  • It is known that the CP asymmetry, the symmetry violation of combination of charge conjugation (C) and parity (P), is the main source for matterantimatter asymmetry that is observed in our present universe

  • We study the new physics impact due to vectorlike down quark (VLDQ) model [18,19,20,21] where an extra SUð2ÞL singlet down type quark has been added to SM quark sector which includes a CP

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Summary

INTRODUCTION

The in-depth search for physics beyond the standard model (SM) plays an important role in the area of particle physics. We would like to study the b → s penguin dominated Bs → KþK− decay mode which appears to have discrepancies in standard model values of CP-averaged branching ratio and CP-violating parameters with the corresponding observed values. There is a possibility of contribution to both decays along with Bs → μþμ− mode in the new physics scenario Inspired by these discrepancies of the Bs → KþK− decay mode, we would like to investigate, in QCD factorization approach, the new physics (NP) effect on CP-averaged branching ratio as well as the CP violation parameters arising due to Z0 model where an extra Uð1Þ0 gauge boson Z0 takes part in the play. Ð8Þ where q and p are mixing parameters which are connected to the standard model CKM elements as q p

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Z0 MODEL
CONCLUSION
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