We compute the next-to-leading order QCD corrections to spectator effects in the lifetime ratios of beauty hadrons. With respect to previous calculations, we take into account the non-vanishing value of the charm quark mass. We obtain the predictions tau (B+)/tau(B-d) = 1.06+/-0.02, tau(B-s)/tau(B-d) = 1.00+/-0.0 1 and tau(Lambda(b))/tau(B-d) = 0.90+/-0.05, in good agreement with the experimental results. In the case of tau(B-s)/tau(B-d) and tau(Lambda(b))/tau(B-d), however, some contributions, which either vanish in the vacuum insertion approximation or represent a pure NLO correction, have not been determined yet. (C) 2002 Elsevier Science B.V. All rights reserved
We calculate the charm-quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leading o...
Abstract We present updated predictions for lifetimes of doubly charmed baryons, within the heavy qu...
We calculate the charm-quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leadin...
We compute the next-to-leading order QCD corrections to spectator effects in the lifetime ratios of ...
We compute the next-to-leading order QCD corrections to spectator effects in the lifetime ratios of ...
Theoretical predictions of beauty hadron lifetimes, based on the heavy quark expansion up to and inc...
Theoretical predictions of beauty hadron lifetimes, based on the heavy quark expansion up to and inc...
The present status of the theoretical estimates of beauty hadron lifetime ratios and of width differ...
Although the B(s) and Lambda(b) hadrons differ only in the spectator quarks from the well-studied B(...
We compute the QCD corrections to the decay rate difference in the B_s- anti B_s system, #DELTA##GAM...
We present calculations of NNLO threshold corrections for beauty and charm production in {pi}{sup -}...
We extend Voloshin's recent analysis of charmed and beauty hyperon decays based on SU(3) symmetry an...
A review of the latest experimental results on charm and beauty particle lifetimes is presented toge...
The lifetime splitting between the B{sup +} and B{sub d}{sup 0} mesons has recently been calculated ...
In this paper, we study the B-c-meson exclusive decays to S-wave charmonia and light pseudoscalar or...
We calculate the charm-quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leading o...
Abstract We present updated predictions for lifetimes of doubly charmed baryons, within the heavy qu...
We calculate the charm-quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leadin...
We compute the next-to-leading order QCD corrections to spectator effects in the lifetime ratios of ...
We compute the next-to-leading order QCD corrections to spectator effects in the lifetime ratios of ...
Theoretical predictions of beauty hadron lifetimes, based on the heavy quark expansion up to and inc...
Theoretical predictions of beauty hadron lifetimes, based on the heavy quark expansion up to and inc...
The present status of the theoretical estimates of beauty hadron lifetime ratios and of width differ...
Although the B(s) and Lambda(b) hadrons differ only in the spectator quarks from the well-studied B(...
We compute the QCD corrections to the decay rate difference in the B_s- anti B_s system, #DELTA##GAM...
We present calculations of NNLO threshold corrections for beauty and charm production in {pi}{sup -}...
We extend Voloshin's recent analysis of charmed and beauty hyperon decays based on SU(3) symmetry an...
A review of the latest experimental results on charm and beauty particle lifetimes is presented toge...
The lifetime splitting between the B{sup +} and B{sub d}{sup 0} mesons has recently been calculated ...
In this paper, we study the B-c-meson exclusive decays to S-wave charmonia and light pseudoscalar or...
We calculate the charm-quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leading o...
Abstract We present updated predictions for lifetimes of doubly charmed baryons, within the heavy qu...
We calculate the charm-quark contribution to the decay K_L -> mu^+ mu^- in next-to-next-to-leadin...