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B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that

We present a short review of our most recent high statistics lattice determinations in the HQET of the following important parameters in B physics: the B--meson binding energy, $\overline{\Lambda}$ and the kinetic energy of the b quark in the B meson, $\lambda_1$, which due to the presence of power...

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Detalles Bibliográficos
Autores principales: Gimenez, V., Martinelli, G., Sachrajda, Christopher T.
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0920-5632(96)00661-5
http://cds.cern.ch/record/308413
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author Gimenez, V.
Martinelli, G.
Sachrajda, Christopher T.
author_facet Gimenez, V.
Martinelli, G.
Sachrajda, Christopher T.
author_sort Gimenez, V.
collection CERN
description We present a short review of our most recent high statistics lattice determinations in the HQET of the following important parameters in B physics: the B--meson binding energy, $\overline{\Lambda}$ and the kinetic energy of the b quark in the B meson, $\lambda_1$, which due to the presence of power divergences require a non--perturbative renormalization to be defined; the value in the HQET is determined by the matrix element of the chromo--magnetic operator between B meson states, $\lambda_2$; the B parameter of the $B^{0}$--$\bar{B}^{0}$ mixing, $B_{B}$, and the decay constant of the B meson, $f_{B}$. All these quantities have been computed using a sample of $600$ gauge field configurations on a $24^{3}\times 40$ lattice at $\beta=6.0$. For estimates by combining results from three independent lattice simulations at
id cern-308413
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1996
record_format invenio
spelling cern-3084132023-03-14T17:18:13Zdoi:10.1016/S0920-5632(96)00661-5http://cds.cern.ch/record/308413engGimenez, V.Martinelli, G.Sachrajda, Christopher T.B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all thatParticle Physics - LatticeWe present a short review of our most recent high statistics lattice determinations in the HQET of the following important parameters in B physics: the B--meson binding energy, $\overline{\Lambda}$ and the kinetic energy of the b quark in the B meson, $\lambda_1$, which due to the presence of power divergences require a non--perturbative renormalization to be defined; the value in the HQET is determined by the matrix element of the chromo--magnetic operator between B meson states, $\lambda_2$; the B parameter of the $B^{0}$--$\bar{B}^{0}$ mixing, $B_{B}$, and the decay constant of the B meson, $f_{B}$. All these quantities have been computed using a sample of $600$ gauge field configurations on a $24^{3}\times 40$ lattice at $\beta=6.0$. For estimates by combining results from three independent lattice simulations atWe present a short review of our most recent high statistics lattice determinations in the HQET of the following important parameters in B physics: the B--meson binding energy, $\overline{\Lambda}$ and the kinetic energy of the b quark in the B meson, $\lambda_1$, which due to the presence of power divergences require a non--perturbative renormalization to be defined; the $\overline{MS}$ running mass of the b quark, $\overline{m}_{b}(\overline{m}_{b})$; the $B~{*}$--$B$ mass splitting, whose value in the HQET is determined by the matrix element of the chromo--magnetic operator between B meson states, $\lambda_2$; the B parameter of the $B~{0}$--$\bar{B}~{0}$ mixing, $B_{B}$, and the decay constant of the B meson, $f_{B}$. All these quantities have been computed using a sample of $600$ gauge field configurations on a $24~{3}\times 40$ lattice at $\beta=6.0$. For $\overline{\Lambda}$ and $\overline{m}_{b}(\overline{m}_{b})$, we obtain our estimates by combining results from three independent lattice simulations at $\beta=6.0$, $6.2$ and $6.4$ on the same volume.hep-lat/9608039FTUV-96-49IFIC-96-57FTUV-96-49IFIC-96-57oai:cds.cern.ch:3084131996-08-08
spellingShingle Particle Physics - Lattice
Gimenez, V.
Martinelli, G.
Sachrajda, Christopher T.
B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that
title B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that
title_full B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that
title_fullStr B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that
title_full_unstemmed B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that
title_short B physics on the Lattice: $\overline{\Lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $B^{0}-\overline{B}^{0}$ mixing, $f_{B}$ and all that
title_sort b physics on the lattice: $\overline{\lambda}$, $\lambda_{1}$, $\overline{m}_{b}(\overline{m}_{b})$, $\lambda_2$, $b^{0}-\overline{b}^{0}$ mixing, $f_{b}$ and all that
topic Particle Physics - Lattice
url https://dx.doi.org/10.1016/S0920-5632(96)00661-5
http://cds.cern.ch/record/308413
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