Challenging B ¯ s → D s ∗ form factors with the heavy quark expansion

Recent publications by three lattice QCD collaborations have provided an unprecedented wealth of theoretical predictions for the B¯q→Dq∗ form factors, for spectator flavours q = u/d and q = s. We analyse these predictions within the framework of the heavy-quark expansion (HQE) to order αs, 1/mb, and 1/mc2. For the first time, our analysis imposes unitarity bounds for all of the B¯q∗→Dq∗ form factors; this includes newly identified tensor form factors arising in B¯q∗→Dq∗. This enables us to treat all form factors in the same fashion. At the level of our present analysis, the inclusion of the tensor bounds is not yet constraining the HQE parameter space. We find the lattice QCD results to be well compatible with each other in a joint HQE fit as well as with QCD sum rule estimates that were used in previous HQE analyses. This is in contrast to the strong variability of the posterior predictions, in particular of the form factors ratios R0 and R2. Using the posterior distributions of our HQE analysis, we provide predictions for angular observables and LFU ratios in the B¯q→Dq∗ℓ−ν¯ decays.

Publication Details

Journal
Durham Research Online (Durham University)
Published
2025-11-11
DOI
https://doi.org/10.1007/jhep11%282025%29051
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
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article

Challenging B ¯ s → D s ∗ form factors with the heavy quark expansion

Durham Research Online (Durham University)
Quantum Chromodynamics and Particle Interactions
article

Challenging B ¯ s → D s ∗ form factors with the heavy quark expansion

article en

Abstract

Recent publications by three lattice QCD collaborations have provided an unprecedented wealth of theoretical predictions for the B¯q→Dq∗ form factors, for spectator flavours q = u/d and q = s. We analyse these predictions within the framework of the heavy-quark expansion (HQE) to order αs, 1/mb, and 1/mc2. For the first time, our analysis imposes unitarity bounds for all of the B¯q∗→Dq∗ form factors; this includes newly identified tensor form factors arising in B¯q∗→Dq∗. This enables us to treat all form factors in the same fashion. At the level of our present analysis, the inclusion of the tensor bounds is not yet constraining the HQE parameter space. We find the lattice QCD results to be well compatible with each other in a joint HQE fit as well as with QCD sum rule estimates that were used in previous HQE analyses. This is in contrast to the strong variability of the posterior predictions, in particular of the form factors ratios R0 and R2. Using the posterior distributions of our HQE analysis, we provide predictions for angular observables and LFU ratios in the B¯q→Dq∗ℓ−ν¯ decays.

Durham Research Online (Durham University)
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Openalex Percentile: Top 25%
Quantum Chromodynamics and Particle Interactions
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