2002
DOI: 10.1016/s0370-2693(02)02639-4
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Correlation between ΔMs and B0s,d→μ+μ− in supersymmetry at large tanβ

Abstract: Considering the MSSM with the CKM matrix as the only source of flavour violation and heavy supersymmetric particles at large tan β, we analyze the correlation between the increase of the rates of the decays B 0 s,d → µ + µ − and the suppression of ∆M s , that are caused by the enhanced flavour changing neutral Higgs couplings to down-type quarks. We give analytic formulae for the neutral and charged Higgs couplings to quarks including large tan β resummed corrections in the SU (2) × U (1) limit and comment bri… Show more

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Cited by 146 publications
(164 citation statements)
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“…We note that the tan 4 β S enhanced contributions to the coefficients C 2,3 whose presence is pointed out in Ref. [9], do not impact significantly for the range of SUSY parameters that we consider (tan β S < 35 and |θt| < π/10).…”
Section: Susy Contributionssupporting
confidence: 58%
“…We note that the tan 4 β S enhanced contributions to the coefficients C 2,3 whose presence is pointed out in Ref. [9], do not impact significantly for the range of SUSY parameters that we consider (tan β S < 35 and |θt| < π/10).…”
Section: Susy Contributionssupporting
confidence: 58%
“…Lastly, we note that in contrast to the B s system [35], D → ℓ + ℓ − does not receive a sizable contribution from Higgs boson exchange with large tan β. This is because in this case, the loop-induced term to the Yukawa couplings is proportional to v d (i.e., the vev of the Higgs doublet that generates masses for the down-type quarks) which is the smaller of the two vevs and hence does not compensate for the small loop factor.…”
Section: B Minimal Supersymmetric Standard Modelmentioning
confidence: 76%
“…The minimal supersymmetric SM (MSSM) with large ratio tan β of the Higgs vacuum expectation values and no new sources of flavour violation in the supersymmetry-breaking Lagrangian is an example of such a minimally flavour-violating (MFV) theory, which nevertheless may exhibit sizeable differences from the SM due to Higgs exchange. The leptonic B s → µ + µ − and B + → τ + ν τ decays have been extensively studied in this model, as well as meson mixing and B → Dτ ν τ [1,2,3,4,5,6,7,8,9,10,11,12,13]. Higgs exchange also generates scalar four-quark operators, which contribute to non-leptonic B decays.…”
Section: Introductionmentioning
confidence: 99%