English

Lifetimes and HQE

High Energy Physics - Phenomenology 2019-09-06 v3 High Energy Physics - Experiment

Abstract

Kolya Uraltsev was one of the inventors of the Heavy Quark Expansion (HQE), that describes inclusive weak decays of hadrons containing heavy quarks and in particular lifetimes. Besides giving a pedagogic introduction to the subject, we review the development and the current status of the HQE, which just recently passed several non-trivial experimental tests with an unprecedented precision. In view of many new experimental results for lifetimes of heavy hadrons, we also update several theory predictions: τ(B+)/τ(Bd)=1.040.01+0.05±0.02±0.01\tau (B^+) / \tau (B_d) = 1.04^{+0.05}_{-0.01} \pm 0.02 \pm 0.01, τ(Bs)/τ(Bd)=1.001±0.002\tau (B_s) / \tau (B_d) = 1.001 \pm 0.002, τ(Λb)/τ(Bd)=0.935±0.054\tau (\Lambda_b)/ \tau (B_d) = 0.935 \pm 0.054 and τˉ(Ξb0)/τˉ(Ξb+)=0.95±0.06\bar {\tau} (\Xi_b^0) / \bar{\tau} (\Xi_b^+) = 0.95 \pm 0.06. The theoretical precision is currently strongly limited by the unknown size of the non-perturbative matrix elements of four-quark operators, which could be determined with lattice simulations.

Cite

@article{arxiv.1405.3601,
  title  = {Lifetimes and HQE},
  author = {Alexander Lenz},
  journal= {arXiv preprint arXiv:1405.3601},
  year   = {2019}
}

Comments

53 pages, invited contribution to the Kolya Uraltsev Memorial Book; comments are welcome; typos corrected; nicer style file and new experimental results included; in v3 typo in the expression for $\tau (B_s) / \tau (B_d)$ corrected (Eq. 4.148)

R2 v1 2026-06-22T04:14:17.583Z