New strategies for new physics search in B → K *vv̄ B → Kvv̄ and B → X 8vv̄ decays

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Abstract

The rare decay B K*ν is regarded as one of the important channels in B physics as it allows a transparent study of Z penguin and other electroweak penguin effects in New Physics (NP) scenarios in the absence of dipole operator contributions and Higgs (scalar) penguin contributions that are often more important than Z contributions in B K*ℓ +ℓ - and B s ℓ +ℓ - decays. We present a new analysis of B K*ν with improved form factors and of the decays B Kν and B X sν in the SM and in a number of NP scenarios like the general MSSM, general scenarios with modified Z/Z′ penguins and in a singlet scalar extension of the SM. We also summarize the results in the Littlest Higgs model with T-parity and a Randall-Sundrum (RS) model with custodial protection of left-handed Zd ij couplings. Our SM prediction BR(B K*ν) = (6.8 +1.0-1.1) × 10 -6 turns out to be significantly lower than the ones present in the literature. Our improved calculation BR(B X sν) = (2.70.2) × 10 -5 in the SM avoids the normalization to the BR(B X ce e) and, with less than 10% total uncertainty, is the most accurate to date. The results for the SM and NP scenarios can be transparently summarized in a (,η) plane analogous to the known (,) plane with a non-vanishing η signalling this time not CP violation but the presence of new right-handed down-quark flavour violating couplings which can be ideally probed by the decays in question. Measuring the three branching ratios and one additional polarization observable in B K*ν allows to overconstrain the resulting point in the (,η) plane with (,η) = (1,0) corresponding to the SM. We point out that the correlations of these three channels with the rare decays K + π +ν, K L π 0ν, B X sℓ +ℓ - and B s μ +μ - offer powerful tests of New Physics with new right-handed couplings and non-MFV interactions. © 2009 SISSA.

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APA

Altmannshofer, W., Buras, A. J., Straub, D. M., & Wick, M. (2009). New strategies for new physics search in B → K *vv̄ B → Kvv̄ and B → X 8vv̄ decays. Journal of High Energy Physics, 2009(4). https://doi.org/10.1088/1126-6708/2009/04/022

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