slides

Bs(d)−Bˉs(d)B_{s(d)}-\bar{B}_{s(d)} Mixing and Bs→μ+μ−B_s\to\mu^+\mu^- Decay in the NMSSM with the Flavour Expansion Theorem

Abstract

In this paper, motivated by the observation that the Standard Model predictions are now above the experimental data for the mass difference ΔMs(d)\Delta M_{s(d)}, we perform a detailed study of Bs(d)−Bˉs(d)B_{s(d)}-\bar{B}_{s(d)} mixing and Bs→μ+μ−B_s\to\mu^+\mu^- decay in the Z3\mathbb{Z}_3-invariant NMSSM with non-minimal flavour violation, using the recently developed procedure based on the Flavour Expansion Theorem, with which one can perform a purely algebraic mass-insertion expansion of an amplitude written in the mass eigenstate basis without performing any diagrammatic calculations in the interaction/flavour basis. Specifically, we consider the finite orders of mass insertions for neutralinos but the general orders for squarks and charginos, under two sets of assumptions for the squark flavour structures (\textit{i.e.}, while the flavour-conserving off-diagonal element δ33LR\delta_{33}^\text{LR} is kept in both of these two sectors, only the flavour-violating off-diagonal elements δ23LL\delta_{23}^\text{LL} and δi3RR\delta_{i3}^\text{RR} (i=1,2i=1,2) are kept in the \text{LL} and \text{RR} sectors, respectively). Our analytic results are then expressed directly in terms of the initial Lagrangian parameters in the interaction/flavour basis, making it easy to impose the experimental bounds on them. It is found numerically that the NMSSM effects with the above two assumptions for the squark flavour structures can accommodate the observed deviation for ΔMs(d)\Delta M_{s(d)}, while complying with the experimental constraints from the branching ratios of Bs→μ+μ−B_s\to \mu^+ \mu^- and B→XsγB\to X_s\gamma decays.Comment: 48 pages, 7 figures, and 2 tables; More discussions and references added, final version to be published in JHE

    Similar works

    Full text

    thumbnail-image

    Available Versions