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Heavy-meson bag parameters using gradient flow

Matthew Black1,2,*, Robert V. Harlander3, Jonas T. Kohnen3, Fabian Lange4,5, Antonio Rago6, Andrea Shindler3,7,8, and Oliver Witzel9

  • *Contact author: matthew.black@ed.ac.uk

Phys. Rev. D 114, 094503 – Published 5 November, 2026

DOI: https://doi.org/10.1103/47j9-h8s5

Abstract

We demonstrate the use of the gradient flow combined with the short flow-time expansion (GF+SFTX) as a renormalization procedure for four-quark operator matrix elements and associated bag parameters relevant to neutral heavy-meson mixing (ΔQ=2) and heavy-meson lifetimes (ΔQ=0). Using six RBC/UKQCD 2+1-flavor domain-wall fermion ensembles, we calculate for a charm-strange system with physical quark masses flowed bag parameters and match them to the MS¯ scheme using perturbative SFTX coefficients up to next-to-next-to-leading order in QCD. We employ a multiscale matching strategy and a renormalization-group improved flow-time evolution which allows for a reliable estimate of systematic uncertainties. For a fictitious neutral Ds meson, we obtain the ΔQ=2 MS¯ bag parameter B1MS¯(3  GeV)=0.7673(123), consistent with existing short-distance D0 mixing determinations. For the ΔQ=0 lifetime-ratio operator basis, we find the MS¯ results B1MS¯(3  GeV)=1.0524(97), B2MS¯(3  GeV)=0.9621(71), ε1MS¯(3  GeV)=−0.2275(76), and ε2MS¯(3  GeV)=−0.0005(8). We provide conversion formulae to reexpress these results for an arbitrary choice of evanescent operators. These results demonstrate that GF+SFTX can deliver precise determinations of dimension-six four-quark operators and establish a framework for future lattice computations including more complex operator bases, where the challenge of power-divergent mixing is shifted to the continuum and handled in the SFTX.

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Bag Parameters for Heavy Meson Lifetimes from a Lattice QCD Calculation at the SU(3)F-symmetric Point

Matthew Black, Robert V. Harlander, Jonas T. Kohnen, Fabian Lange, Antonio Rago, Andrea Shindler, and Oliver Witzel
Phys. Rev. Lett. 137, 191905 (2026)

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