English

Next-to-next-to-leading QCD corrections to the $\mathbf{B^+}$-$\mathbf{B_d^0}$, $\mathbf{D^+}$-$\mathbf{D^0}$, and $\mathbf{D_s^+}$-$\mathbf{D^0}$ lifetime ratios

High Energy Physics - Phenomenology 2026-04-29 v1

Abstract

The total decay widths of heavy mesons can be systematically calculated in terms of an expansion in the two parameters 1/mQ1/m_Q and αs(mQ)\alpha_s(m_Q), where Q=c,bQ=c,b denotes the heavy quark. The dominant contributions to meson lifetime splittings stem from terms which are suppressed by 1/mQ31/m_Q^3 with respect to the leading universal contribution to the total decay width. We calculate three-loop contributions of order αs2/mq3\alpha_s^2/m_q^3 to the lifetime ratios τ(B+)/τ(Bd0)\tau(B^+)/\tau(B_d^0), τ(D+)/τ(D0)\tau(D^+)/\tau(D^0), and τ(Ds+)/τ(D0)\tau(D_s^+)/\tau(D^0) in the limit of exact isospin and V-spin symmetry, respectively. Furthermore, we present new αs/mq3\alpha_s/m_q^3 corrections to the Cabibbo-suppressed terms in τ(B+)/τ(Bd0)\tau(B^+)/\tau(B_d^0). Combining our perturbative coefficients with hadronic matrix elements calculated from Heavy Quark Effective Theory sum rules, we find τ(B+)/τ(Bd0)=1.072±0.024\tau(B^+)/\tau(B_d^0)= {1.072 \pm 0.024 }. Using hadronic matrix elements from a recent lattice QCD calculation we find τ(D+)/τ(D0)=2.344±0.170\tau(D^+)/\tau(D^0)={2.344 \pm 0.170} and τ(Ds+)/τ(D0)=1.289±0.042\tau(D_s^+)/\tau(D^0)={1.289 \pm 0.042}. We find good agreement of our predictions with experimental data, which constitutes a successful probe of the calculations of hadronic matrix elements and permits estimates of the unknown 1/mQ41/m_Q^4 contributions as well as the V-spin breaking terms in τ(Ds+)/τ(D0)\tau(D_s^+)/\tau(D^0).

Keywords

Cite

@article{arxiv.2604.24841,
  title  = {Next-to-next-to-leading QCD corrections to the $\mathbf{B^+}$-$\mathbf{B_d^0}$, $\mathbf{D^+}$-$\mathbf{D^0}$, and $\mathbf{D_s^+}$-$\mathbf{D^0}$ lifetime ratios},
  author = {Francesco Moretti and Ulrich Nierste and Pascal Reeck and Matthias Steinhauser},
  journal= {arXiv preprint arXiv:2604.24841},
  year   = {2026}
}