CP Violation in Bˉ0→D∗+μ−νˉμ{\bar B}^0\to D^{*+}μ^-{\barν}_μ

preprint2019arXivOpen access

Abstract

In order to explain the observed anomalies in the measurements of RD(∗)R_{D^{(*)}} and RJ/ψR_{J/ψ}, a variety of new-physics (NP) models that contribute to b→cτ−νˉb\to cτ^-{\barν} have been proposed. In this paper, we show how CP-violating observables can be used to distinguish these NP models. Because p⃗τ{\vec p}_τ cannot be measured (the decay products of the ττ include the undetected ντν_τ), obtaining the angular distribution of Bˉ0→D∗+τ−νˉτ{\bar B}^0\to D^{*+}τ^{-}{\barν}_τ is problematic. Instead, we focus here on Bˉ0→D∗+(→D0π+)μ−νˉμ{\bar B}^0\to D^{*+}(\to D^0 π^+)μ^- {\barν}_μ. This process may also receive contributions from the same NP, and LHCb intends to measure the CP-violating angular asymmetries in this decay. There are two classes of NP models that contribute to b→cμ−νˉμb\to cμ^-{\barν}_μ. These involve (i) a W′W' (two types) or (ii) a leptoquark (LQ) (six types). The most popular NP models predict no CP-violating effects, so the measurement of nonzero CP-violating symmetries would rule them out. Furthermore these measurements allow one to distinguish the W′W' and LQ models, and to differentiate among several LQ models.

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