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The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms

We compute perturbative QCD corrections to the lifetime splitting between the charged and neutral $B$ meson in the framework of the heavy quark expansion. These next-to-leading logarithmic corrections are necessary for a meaningful use of hadronic matrix elements of local operators from lattice gaug...

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Autores principales: Beneke, Martin, Buchalla, Gerhard, Greub, Christoph, Lenz, Alexander, Nierste, Ulrich
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(02)00561-8
http://cds.cern.ch/record/538259
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author Beneke, Martin
Buchalla, Gerhard
Greub, Christoph
Lenz, Alexander
Nierste, Ulrich
author_facet Beneke, Martin
Buchalla, Gerhard
Greub, Christoph
Lenz, Alexander
Nierste, Ulrich
author_sort Beneke, Martin
collection CERN
description We compute perturbative QCD corrections to the lifetime splitting between the charged and neutral $B$ meson in the framework of the heavy quark expansion. These next-to-leading logarithmic corrections are necessary for a meaningful use of hadronic matrix elements of local operators from lattice gauge theory. We find the uncertainties associated with the choices of renormalization scale and scheme significantly reduced compared to the leading-order result. We include the full dependence on the charm-quark mass $m_c$ without any approximations. Using hadronic matrix elements estimated in the literature with lattice QCD we obtain $\tau(B^+)/\tau(B^0_d)=1.053\pm 0.027\pm 0.017$, where the effects of unquenching and $1/m_b$ corrections are not yet included. The lifetime difference of heavy baryons $\Xi^0_b$ and $\Xi^-_b$ is also briefly discussed.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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spelling cern-5382592020-08-28T12:55:07Zdoi:10.1016/S0550-3213(02)00561-8http://cds.cern.ch/record/538259engBeneke, MartinBuchalla, GerhardGreub, ChristophLenz, AlexanderNierste, UlrichThe $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithmsParticle Physics - PhenomenologyWe compute perturbative QCD corrections to the lifetime splitting between the charged and neutral $B$ meson in the framework of the heavy quark expansion. These next-to-leading logarithmic corrections are necessary for a meaningful use of hadronic matrix elements of local operators from lattice gauge theory. We find the uncertainties associated with the choices of renormalization scale and scheme significantly reduced compared to the leading-order result. We include the full dependence on the charm-quark mass $m_c$ without any approximations. Using hadronic matrix elements estimated in the literature with lattice QCD we obtain $\tau(B^+)/\tau(B^0_d)=1.053\pm 0.027\pm 0.017$, where the effects of unquenching and $1/m_b$ corrections are not yet included. The lifetime difference of heavy baryons $\Xi^0_b$ and $\Xi^-_b$ is also briefly discussed.We compute perturbative QCD corrections to the lifetime splitting between the charged and neutral $B$ meson in the framework of the heavy quark expansion. These next-to-leading logarithmic corrections are necessary for a meaningful use of hadronic matrix elements of local operators from lattice gauge theory. We find the uncertainties associated with the choices of renormalization scale and scheme significantly reduced compared to the leading-order result. We include the full dependence on the charm-quark mass $m_c$ without any approximations. Using hadronic matrix elements estimated in the literature with lattice QCD we obtain $\tau(B^+)/\tau(B^0_d)=1.053\pm 0.027\pm 0.017$, where the effects of unquenching and $1/m_b$ corrections are not yet included. The lifetime difference of heavy baryons $\Xi^0_b$ and $\Xi^-_b$ is also briefly discussed.We compute perturbative QCD corrections to the lifetime splitting between the charged and neutral B meson in the framework of the heavy quark expansion. These next-to-leading logarithmic corrections are necessary for a meaningful use of hadronic matrix elements of local operators from lattice gauge theory. We find the uncertainties associated with the choices of renormalization scale and scheme significantly reduced compared to the leading-order result. We include the full dependence on the charm-quark mass m c without any approximations. Using hadronic matrix elements estimated in the literature with lattice QCD we obtain τ ( B + )/ τ ( B 0 d )=1.053±0.016±0.017, where the effects of unquenching and 1/ m b corrections are not yet included. The lifetime difference of heavy baryons Ξ 0 b and Ξ − b is also briefly discussed.hep-ph/0202106PITHA-02-05CERN-TH-2002-019BUTP-02-2FERMILAB-PUB-02-016-TBUTP-2002-2CERN-TH-2002-019FERMILAB-PUB-2002-016-TPITHA-2002-05oai:cds.cern.ch:5382592002-02-12
spellingShingle Particle Physics - Phenomenology
Beneke, Martin
Buchalla, Gerhard
Greub, Christoph
Lenz, Alexander
Nierste, Ulrich
The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms
title The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms
title_full The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms
title_fullStr The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms
title_full_unstemmed The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms
title_short The $B^{+}-B_{d}^{0}$ lifetime difference beyond leading logarithms
title_sort $b^{+}-b_{d}^{0}$ lifetime difference beyond leading logarithms
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(02)00561-8
http://cds.cern.ch/record/538259
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