<p>We compute next-to-next-to-leading order corrections to the decay width difference of mass eigenstates and the charge-parity (CP) asymmetry <i>a</i><sub>fs</sub> in flavour-specific decays of neutral <i>B</i> mesons. We include both current-current and penguin operators at three-loop order. All input integrals in the transition amplitude are reduced to a small set of master integrals which depend on the ratio of the charm and bottom quark masses. The latter are computed using semi-analytic methods which provide deep expansions around properly selected values of <i>m</i><sub><i>c</i></sub><i>/m</i><sub><i>b</i></sub>. We provide numerical results for ∆Γ and ∆Γ<i>/</i>∆<i>M</i>, both for the <i>B</i><sub><i>d</i></sub> and <i>B</i><sub><i>s</i></sub> system, including a detailed uncertainty analysis. Using the experimental value for the mass difference ∆<i>M</i><sub><i>s</i></sub> we predict ∆Γ<sub><i>s</i></sub> = (0<i>.</i>078 ± 0<i>.</i>015) ps<sup><i>−</i>1</sup>. For the CP asymmetries we find <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>a</mi> <mi>fs</mi> <mi>s</mi> </msubsup> <mo>=</mo> <mfenced close=")" open="("> <mrow> <mn>2.27</mn> <mo>±</mo> <mn>0.13</mn> </mrow> </mfenced> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>5</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {a}_{\textrm{fs}}^s=\left(2.27\pm 0.13\right)\times {10}^{-5} \)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi>a</mi> <mi>fs</mi> <mi>d</mi> </msubsup> <mo>=</mo> <mo>−</mo> <mfenced close=")" open="("> <mrow> <mn>5.19</mn> <mo>±</mo> <mn>0.30</mn> </mrow> </mfenced> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>4</mn> </mrow> </msup> </math></EquationSource> <EquationSource Format="TEX">\( {a}_{\textrm{fs}}^d=-\left(5.19\pm 0.30\right)\times {10}^{-4} \)</EquationSource> </InlineEquation>. Furthermore, we show that the ratios (∆Γ<sub><i>s</i></sub><i>/</i>∆<i>M</i><sub><i>s</i></sub>)<i>/</i>(∆Γ<sub><i>d</i></sub><i>/</i>∆<i>M</i><sub><i>d</i></sub>) and ∆Γ<sub><i>d</i></sub><i>/</i>∆Γ<sub><i>s</i></sub> can be predicted with high precision. The former quantity permits the prediction ∆Γ<sub><i>d</i></sub> = (0<i>.</i>00215 ± 0<i>.</i>00013) ps<sup><i>−</i>1</sup> from the measurements of ∆<i>M</i><sub><i>d,s</i></sub> and ∆Γ<sub><i>s</i></sub>. We further discuss the impact of ∆Γ<sub><i>d</i></sub><i>/</i>∆Γ<sub><i>s</i></sub> on the CKM unitarity triangle and present ready-to-use formulae which permit improved predictions once updated results for the operator matrix elements are available.</p>

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Complete next-to-next-to-leading order QCD corrections to the decay matrix in B-meson mixing at leading power

  • Ulrich Nierste,
  • Pascal Reeck,
  • Vladyslav Shtabovenko,
  • Matthias Steinhauser

摘要

We compute next-to-next-to-leading order corrections to the decay width difference of mass eigenstates and the charge-parity (CP) asymmetry afs in flavour-specific decays of neutral B mesons. We include both current-current and penguin operators at three-loop order. All input integrals in the transition amplitude are reduced to a small set of master integrals which depend on the ratio of the charm and bottom quark masses. The latter are computed using semi-analytic methods which provide deep expansions around properly selected values of mc/mb. We provide numerical results for ∆Γ and ∆Γ/M, both for the Bd and Bs system, including a detailed uncertainty analysis. Using the experimental value for the mass difference ∆Ms we predict ∆Γs = (0.078 ± 0.015) ps1. For the CP asymmetries we find a fs s = 2.27 ± 0.13 × 10 5 \( {a}_{\textrm{fs}}^s=\left(2.27\pm 0.13\right)\times {10}^{-5} \) and a fs d = 5.19 ± 0.30 × 10 4 \( {a}_{\textrm{fs}}^d=-\left(5.19\pm 0.30\right)\times {10}^{-4} \) . Furthermore, we show that the ratios (∆Γs/Ms)/(∆Γd/Md) and ∆Γd/∆Γs can be predicted with high precision. The former quantity permits the prediction ∆Γd = (0.00215 ± 0.00013) ps1 from the measurements of ∆Md,s and ∆Γs. We further discuss the impact of ∆Γd/∆Γs on the CKM unitarity triangle and present ready-to-use formulae which permit improved predictions once updated results for the operator matrix elements are available.