Abstract

We study supersymmetric (SUSY) effects on $C_7(\mu_b)$ and $C'_7(\mu_b)$ which are the Wilson coefficients (WCs) for $b \to s \gamma$ at b-quark mass scale $\mu_b$ and are closely related to radiative $B$-meson decays. The SUSY-loop contributions to $C_7(\mu_b)$ and $C'_7(\mu_b)$ are calculated at leading order (LO) in the Minimal Supersymmetric Standard Model (MSSM) with general quark-flavour violation (QFV). For the first time we perform a systematic MSSM parameter scan for the WCs $C_7(\mu_b)$ and $C'_7(\mu_b)$ respecting all the relevant constraints, i.e. the theoretical constraints from vacuum stability conditions and the experimental constraints, such as those from $K$- and $B$-meson data and electroweak precision data, as well as recent limits on SUSY particle masses and the 125 GeV Higgs boson data from LHC experiments. From the parameter scan we find the following: (1) The MSSM contribution to Re($C_7(\mu_b)$) can be as large as $\sim \pm 0.05$, which could correspond to about 3$\sigma$ significance of New Physics (NP) signal in the future LHCb and Belle II experiments. (2) The MSSM contribution to Re($C'_7(\mu_b)$) can be as large as $\sim -0.08$, which could correspond to about 4$\sigma$ significance of NP signal in the future LHCb and Belle II experiments. (3) These large MSSM contributions to the WCs are mainly due to (i) large scharm-stop mixing and large scharm/stop involved trilinear couplings, (ii) large sstrange-sbottom mixing and large sstrange-sbottom involved trilinear couplings and (iii) large bottom Yukawa coupling $Y_b$ for large $\tan\beta$ and large top Yukawa coupling $Y_t$. In case such large NP contributions to the WCs are really observed in the future experiments at Belle II and LHCb Upgrade, this could be the imprint of QFV SUSY (the MSSM with general QFV).

Highlights

  • Our present knowledge of elementary particle physics is very successfully described by the Standard Model (SM) of electroweak and strong interactions

  • (3) These large Minimal Supersymmetric Standard Model (MSSM) contributions to the Wilson coefficients (WCs) are mainly due to (i) large scharm-stop mixing and large scharm/stop involved trilinear couplings TU23, TU32 and TU33, (ii) large sstrange-sbottom mixing and large sstrange-sbottom involved trilinear couplings TD23, TD32 and TD33 and (iii) large bottom Yukawa coupling Yb for large tan β and large top Yukawa coupling Yt. In case such large New Physics (NP) contributions to the WCs are really observed in the future experiments at Belle II and the LHCb Upgrade, this could be the imprint of quark-flavor violation (QFV) SUSY and would encourage to perform further studies of the WCs C07ðμbÞ and CM7 SSMðμbÞ at higher order (NLO/NNLO) level in this model

  • The SUSY-loop contributions to the C7ðμbÞ and C07ðμbÞ are calculated at leading order (LO) in the Minimal Supersymmetric Standard Model with general quark-flavor violation

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Summary

INTRODUCTION

Our present knowledge of elementary particle physics is very successfully described by the Standard Model (SM) of electroweak and strong interactions. We calculate the SUSY-loop contributions to C7ðμbÞ and C07ðμbÞ at leading order (LO) in the Minimal Supersymmetric Standard Model (MSSM) with general quark-flavor violation (QFV) due to squark generation mixing. In the numerical computation of the WCs, we perform a MSSM parameter scan respecting all the relevant theoretical and experimental constraints, such as those from vacuum stability conditions, those from K- and B-meson data, the 125 GeV Higgs boson data from LHC, and electroweak precision data, as well as recent limits on SUSY particle (sparticle) masses from LHC experiments. There is no systematic numerical study on the SUSY-loop contributions to C7ðμbÞ and in the MSSM with general QFV.. LO we thoroughly perform such a systematic study with special emphasis on the importance of SUSY QFV in order to clarify a possibility that an imprint of SUSY can be found in radiative B-meson decays, focusing on the WCs C7ðμbÞ and C07ðμbÞ.

SQUARK MASS MATRICES IN THE MSSM WITH FLAVOR VIOLATION
PARAMETER SCAN
WC C7ðμbÞ AND C07ðμbÞ IN THE MSSM WITH QFV
CONCLUSIONS
Findings
Uγ ðM2Qββ þ
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