Abstract

We consider the {B}_s^0 → μ+μ−γ effective lifetime, and the related CP-phase sensitive quantity {A}_{{Delta Gamma}_s}^{mu mu gamma} , as a way to obtain qualitatively new insights on the current B-decay discrepancies. Through a fit comparing pre- to post-Moriond-2021 data we identify a few theory benchmark scenarios addressing these discrepancies, and featuring large CP violation in addition. We then explore the possibility of telling apart these scenarios with {A}_{{Delta Gamma}_s}^{mu mu gamma} , once resonance-modeling and form-factor uncertainties are taken into account. We do so in both regions of low and high invariant di-lepton mass-squared q2. For low q2, we show how to shape the integration range in order to reduce the impact of the ϕ-resonance modelling on the {A}_{{Delta Gamma}_s}^{mu mu gamma} prediction. For high q2, we find that the corresponding pollution from broad-charmonium resonances has a surprisingly small effect on {A}_{{Delta Gamma}_s}^{mu mu gamma} . This is due to a number of cancellations, that can be traced back to the complete dominance of semi-leptonic operator contributions for high q2 — at variance with low q2 — and to {A}_{{Delta Gamma}_s}^{mu mu gamma} behaving like a ratio-of-amplitudes observable. Our study suggests that {A}_{{Delta Gamma}_s}^{mu mu gamma} is — especially at high q2 — a potentially valuable probe of short-distance CP-violating effects in the very same Wilson coefficients that are associated to current b → s discrepancies. Its discriminating power, however, relies on progress in form-factor uncertainties. Interestingly, high q2 is the region where {B}_s^0 → μ+μ−γ is already being accessed experimentally, and the region where form factors are more accessible through non-perturbative QCD methods.

Highlights

  • For low q2, we show how to shape the integration range in order to reduce the impact of the φresonance modelling on the Aμ∆μΓγs pollution from broad-charmonium prediction. resonances

  • Our study suggests that Aμ∆μΓγs is — especially at high q2 — a potentially valuable probe of short-distance CP-violating effects in the very same Wilson coefficients that are associated to current b → s discrepancies

  • The effective lifetime of Bs0 → μμγ allows to access the quantity known as Aμ∆μΓγs, which offers a sensitive probe of new CP-violating effects in b → s-sector Wilson coefficients

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Summary

Basics and main formulæ

Given a final state f common to both the Bs0 and the Bs0, the most ‘natural’ experimental observable assuming equal production rates for a Bs0 and a Bs0 is the ‘untagged’ rate [32, 36]. With dΦf an element of n-body phase space for the final state f [37], and where Af (t) denote the amplitudes of decay to f for a Bs-meson that was a Bs at t = 0. The parameter Af∆Γs relating the two branching ratios is final-state as well as model dependent. Since the φM dependence is the same in Af /Af and in Af A∗f , the latter appearing in eq (2.13), we see that Af∆Γs is phase-convention independent, as well-known [36, 40]. Given the very Aμ∆μΓγs definition, complex phases in any of the Wilson-coefficient combinations contribute to ‘misaligning’ numerator and denominator. To address the hadronic sensitivity of Aμ∆μΓγs in detail, we have to first establish theory scenarios to use as benchmarks

Parenthesis: a CPV global fit in the light of recent data
NP sensitivity at high q2
Impact of broad charmonium
Impact of form-factor modelling
Experimental outlook and conclusions
A Amplitudes and form factors: basic notation
D On the near-cancellation of broad-charmonium uncertainties
Findings
E Table of inputs

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