Theory News on Bs(d)→μ+μ−B_{s(d)} \to μ^+μ^- Decays

preprint2012arXivOpen access

Abstract

The rare decays Bs(d)→μ+μ−B_{s(d)} \to μ^+μ^- play a key role for the testing of the Standard Model. An overview of the most recent theoretical predictions of the corresponding branching ratios is given, emphasizing that the sizable decay width difference ΔΓsΔΓ_s of the BsB_s-meson system affects the Bs→μ+μ−B_s\to μ^+μ^- channel. As a consequence, the calculated Standard Model branching ratio has to be upscaled by about 10% to BR(Bs→μ+μ−)=(3.54±0.30)×10−9(B_s\to μ^+μ^-)=(3.54\pm0.30)\times 10^{-9}. This prediction is the reference value for the comparison with the time-integrated experimental branching ratio, where LHCb has recently reported (3.2−1.2+1.5)×10−9(3.2^{+1.5}_{-1.2})\times10^{-9} corresponding to the first evidence for Bs→μ+μ−B_s\to μ^+μ^-. The ΔΓsΔΓ_s effects have also to be included in the constraints on the parameter space of New-Physics models following from the experimental data. Furthermore, ΔΓsΔΓ_s makes a new observable through the effective Bs→μ+μ−B_s\to μ^+μ^- lifetime accessible, which probes New Physics in a way complementary to the branching ratio and adds an exciting new topic to the agenda for the high-luminosity upgrade of the LHC.

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