TY - JOUR
T1 - In pursuit of new physics with Bs,d 0 → ℓ + ℓ −
AU - Fleischer, Robert
AU - Jaarsma, Ruben
AU - Tetlalmatzi-Xolocotzi, Gilberto
PY - 2017/5/1
Y1 - 2017/5/1
N2 - Leptonic rare decays of Bs,d 0 mesons offer a powerful tool to search for physics beyond the Standard Model. The Bs 0 → μ+μ− decay has been observed at the Large Hadron Collider and the first measurement of the effective lifetime of this channel was presented, in accordance with the Standard Model. On the other hand, Bs 0 → τ+τ− and Bs 0 → e+e− have received considerably less attention: while LHCb has recently reported a first upper limit of 6.8 × 10−3 (95% C.L.) for the Bs 0 → τ+τ− branching ratio, the upper bound 2.8 × 10−7 (90% C.L.) for the branching ratio of Bs 0 → e+e− was reported by CDF back in 2009. We discuss the current status of the interpretation of the measurement of Bs 0 → μ+μ−, and explore the space for New-Physics effects in the other Bs,d 0 → ℓ+ℓ− decays in a scenario assuming flavour-universal Wilson coefficients of the relevant four-fermion operators. While the New-Physics effects are then strongly suppressed by the ratio mμ/mτ of the lepton masses in Bs 0 → τ+τ−, they are hugely enhanced by mμ/me in Bs 0 → e+e− and may result in a Bs 0 → e+e− branching ratio as large as about 5 times the one of Bs 0 → μ+μ−, which is about a factor of 20 below the CDF bound; a similar feature arises in Bd 0 → e+e−. Consequently, it would be most interesting to search for the Bs,d 0 → e+e− channels at the LHC and Belle II, which may result in an unambiguous signal for physics beyond the Standard Model.
AB - Leptonic rare decays of Bs,d 0 mesons offer a powerful tool to search for physics beyond the Standard Model. The Bs 0 → μ+μ− decay has been observed at the Large Hadron Collider and the first measurement of the effective lifetime of this channel was presented, in accordance with the Standard Model. On the other hand, Bs 0 → τ+τ− and Bs 0 → e+e− have received considerably less attention: while LHCb has recently reported a first upper limit of 6.8 × 10−3 (95% C.L.) for the Bs 0 → τ+τ− branching ratio, the upper bound 2.8 × 10−7 (90% C.L.) for the branching ratio of Bs 0 → e+e− was reported by CDF back in 2009. We discuss the current status of the interpretation of the measurement of Bs 0 → μ+μ−, and explore the space for New-Physics effects in the other Bs,d 0 → ℓ+ℓ− decays in a scenario assuming flavour-universal Wilson coefficients of the relevant four-fermion operators. While the New-Physics effects are then strongly suppressed by the ratio mμ/mτ of the lepton masses in Bs 0 → τ+τ−, they are hugely enhanced by mμ/me in Bs 0 → e+e− and may result in a Bs 0 → e+e− branching ratio as large as about 5 times the one of Bs 0 → μ+μ−, which is about a factor of 20 below the CDF bound; a similar feature arises in Bd 0 → e+e−. Consequently, it would be most interesting to search for the Bs,d 0 → e+e− channels at the LHC and Belle II, which may result in an unambiguous signal for physics beyond the Standard Model.
KW - Beyond Standard Model
KW - Heavy Quark Physics
KW - Supersymmetric Standard Model
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U2 - 10.1007/JHEP05(2017)156
DO - 10.1007/JHEP05(2017)156
M3 - Article
AN - SCOPUS:85020228783
SN - 1126-6708
VL - 2017
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 5
M1 - 156
ER -