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Constructing heavy-quark sum rule for b→c meson and baryon decays

Motoi Endo1,2,3, Syuhei Iguro4,3, Satoshi Mishima5, and Ryoutaro Watanabe6

Phys. Rev. D 113, 014021 – Published 20 January, 2026

DOI: https://doi.org/10.1103/xs7x-jcrd

Abstract

We study heavy-hadron semileptonic decays proceeding via b→c transition, such as B→D(*)τν¯τ and Λb→Λcτν¯τ. In the heavy-quark limit, where the heavy-quark symmetry holds, we provide a fundamental framework for heavy-quark sum rules among these decays based on the spin decomposition picture. The relation holds directly for the squared amplitudes without requiring phase-space integration. We then apply this relation to reproduce the sum rule among B→D(*)τν¯τ and Λb→Λcτν¯τ. Furthermore, we derive new sum rules for Ωb→Ωc(*) transitions and those involving excited states, such as B→{D0*,D1*} and B→{D1,D2*}.

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