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First lattice calculation of the B-meson binding and kinetic energies

We present the first lattice calculation of the B-meson binding energy \labar and of the kinetic energy -\lambda_1/2 m_Q of the heavy-quark inside the pseudoscalar B-meson. This calculation has required the non-perturbative subtraction of the power divergences present in matrix elements of the Lagra...

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Autores principales: Crisafulli, M., Gimenez, V., Martinelli, G., Sachrajda, Christopher T.
Lenguaje:eng
Publicado: 1995
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(95)00507-2
http://cds.cern.ch/record/282670
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author Crisafulli, M.
Gimenez, V.
Martinelli, G.
Sachrajda, Christopher T.
author_facet Crisafulli, M.
Gimenez, V.
Martinelli, G.
Sachrajda, Christopher T.
author_sort Crisafulli, M.
collection CERN
description We present the first lattice calculation of the B-meson binding energy \labar and of the kinetic energy -\lambda_1/2 m_Q of the heavy-quark inside the pseudoscalar B-meson. This calculation has required the non-perturbative subtraction of the power divergences present in matrix elements of the Lagrangian operator \bar h D_4 h and of the kinetic energy operator \bar h \vec D^2 h. The non-perturbative renormalisation of the relevant operators has been implemented by imposing suitable renormalisation conditions on quark matrix elements, in the Landau gauge. Our numerical results have been obtained from several independent numerical simulations at \beta=6.0 and 6.2, and using, for the meson correlators, the results obtained by the APE group at the same values of \beta. Our best estimate, obtained by combining results at different values of \beta, is \labar =190 \err{50}{30} MeV. For the \overline{MS} running mass, we obtain \overline {m}_b(\overline {m}_b) =4.17 \pm 0.06 GeV, in reasonable agreement with previous determinations. From a subset of 36 configurations, we were only able to establish a loose upper bound on the b-quark kinetic energy in a B-meson, \lambda_1=\langle B \vert \bar h \vec{D}^{2} h \vert B \rangle /(2 M_B )<~1\, GeV^2. This shows that a much larger statistical sample is needed to determine this important parameter.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1995
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spelling cern-2826702023-03-14T18:56:09Zdoi:10.1016/0550-3213(95)00507-2http://cds.cern.ch/record/282670engCrisafulli, M.Gimenez, V.Martinelli, G.Sachrajda, Christopher T.First lattice calculation of the B-meson binding and kinetic energiesParticle Physics - PhenomenologyWe present the first lattice calculation of the B-meson binding energy \labar and of the kinetic energy -\lambda_1/2 m_Q of the heavy-quark inside the pseudoscalar B-meson. This calculation has required the non-perturbative subtraction of the power divergences present in matrix elements of the Lagrangian operator \bar h D_4 h and of the kinetic energy operator \bar h \vec D^2 h. The non-perturbative renormalisation of the relevant operators has been implemented by imposing suitable renormalisation conditions on quark matrix elements, in the Landau gauge. Our numerical results have been obtained from several independent numerical simulations at \beta=6.0 and 6.2, and using, for the meson correlators, the results obtained by the APE group at the same values of \beta. Our best estimate, obtained by combining results at different values of \beta, is \labar =190 \err{50}{30} MeV. For the \overline{MS} running mass, we obtain \overline {m}_b(\overline {m}_b) =4.17 \pm 0.06 GeV, in reasonable agreement with previous determinations. From a subset of 36 configurations, we were only able to establish a loose upper bound on the b-quark kinetic energy in a B-meson, \lambda_1=\langle B \vert \bar h \vec{D}^{2} h \vert B \rangle /(2 M_B )<~1\, GeV^2. This shows that a much larger statistical sample is needed to determine this important parameter.We present the first lattice calculation of the B-meson binding energy $\labar$ and of the kinetic energy $-\lambda_1/2 m_Q$ of the heavy-quark inside the pseudoscalar B-meson. This calculation has required the non-perturbative subtraction of the power divergences present in matrix elements of the Lagrangian operator $\bar h D_4 h$ and of the kinetic energy operator $\bar h \vec D~2 h$. The non-perturbative renormalisation of the relevant operators has been implemented by imposing suitable renormalisation conditions on quark matrix elements, in the Landau gauge. Our numerical results have been obtained from several independent numerical simulations at $\beta=6.0$ and $6.2$, and using, for the meson correlators, the results obtained by the APE group at the same values of $\beta$. Our best estimate, obtained by combining results at different values of $\beta$, is $\labar =190 \err{50}{30}$ MeV. For the $\overline{MS}$ running mass, we obtain $\overline {m}_b(\overline {m}_b) =4.17 \pm 0.06$ GeV, in reasonable agreement with previous determinations. From a subset of 36 configurations, we were only able to establish a loose upper bound on the $b$-quark kinetic energy in a $B$-meson, $\lambda_1=\langle B \vert \bar h \vec{D}~{2} h \vert B \rangle /(2 M_B )<$1\, GeV$~2$. This shows that a much larger statistical sample is needed to determine this important parameter.We present the first lattice calculation of the B-meson binding energy Λ and of the kinetic energy − λ 1 /2 m Q of the heavy-quark inside the pseudoscalar B-meson. This calculation has required the non-perturbative subtraction of the power divergences present in matrix elements of the Lagrangian operator h − D 4 h and of the kinetic energy operator h − D 2 h . The non-perturbative renormalisation of the relevant operators has been implemented by imposing suitable renormalisation conditions on quark matrix elements, in the Landau gauge. Our numerical results have been obtained from several independent numerical simulations at β = 6.0 and 6.2, and using, for the meson correlators, the results obtained by the APE group at the same values of β. Our best estimate, obtained by combining results at different values of β, is Λ − = 190 −30 +50 MeV . For the MS running mass, we obtain m b ( m b ) = 4.17 ± 0.06 GeV , in reasonable agreement with previous determinations. From a subset of 36 configurations, we were only able to establish a loose upper bound on the b-quark kinetic energy in a B -meson, Λ = 〈B∥ h − D 2 h∥B〉/(2M B ) < 1 GeV 2 . This shows that a much larger statistical sample is needed to determine this important parameter.hep-ph/9506210CERN-TH-7521-94ROME-94-1071SHEP-94-95-14CERN-TH-7521-94ROMA-1-1071oai:cds.cern.ch:2826701995-06-01
spellingShingle Particle Physics - Phenomenology
Crisafulli, M.
Gimenez, V.
Martinelli, G.
Sachrajda, Christopher T.
First lattice calculation of the B-meson binding and kinetic energies
title First lattice calculation of the B-meson binding and kinetic energies
title_full First lattice calculation of the B-meson binding and kinetic energies
title_fullStr First lattice calculation of the B-meson binding and kinetic energies
title_full_unstemmed First lattice calculation of the B-meson binding and kinetic energies
title_short First lattice calculation of the B-meson binding and kinetic energies
title_sort first lattice calculation of the b-meson binding and kinetic energies
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0550-3213(95)00507-2
http://cds.cern.ch/record/282670
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