Non-perturbative O(a) improvement of lattice QCD

The coefficients multiplying the counterterms required for O($a$) improvement of the action and the isovector axial current in lattice QCD are computed non-perturbatively, in the quenched approximation and for bare gauge couplings $g_0$ in the range $0 \leq g_0 \leq 1$. A finite-size method based on...

Descripción completa

Detalles Bibliográficos
Autores principales: Luscher, Martin, Sint, Stefan, Sommer, Rainer, Weisz, Peter, Wolff, Ulli
Lenguaje:eng
Publicado: 1996
Materias:
Particle Physics - Lattice
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(97)00080-1
http://cds.cern.ch/record/311117
_version_ 1780890097025024000
author Luscher, Martin
Sint, Stefan
Sommer, Rainer
Weisz, Peter
Wolff, Ulli
author_facet Luscher, Martin
Sint, Stefan
Sommer, Rainer
Weisz, Peter
Wolff, Ulli
author_sort Luscher, Martin
collection CERN
description The coefficients multiplying the counterterms required for O($a$) improvement of the action and the isovector axial current in lattice QCD are computed non-perturbatively, in the quenched approximation and for bare gauge couplings $g_0$ in the range $0 \leq g_0 \leq 1$. A finite-size method based on the Schrödinger functional is employed, which enables us to perform all calculations at zero or nearly zero quark mass. As a by-product the critical hopping parameter $\kappa_c$ is obtained at all couplings considered.
id cern-311117
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1996
record_format invenio
spelling cern-3111172021-09-17T03:04:18Zdoi:10.1016/S0550-3213(97)00080-1http://cds.cern.ch/record/311117engLuscher, MartinSint, StefanSommer, RainerWeisz, PeterWolff, UlliNon-perturbative O(a) improvement of lattice QCDParticle Physics - LatticeThe coefficients multiplying the counterterms required for O($a$) improvement of the action and the isovector axial current in lattice QCD are computed non-perturbatively, in the quenched approximation and for bare gauge couplings $g_0$ in the range $0 \leq g_0 \leq 1$. A finite-size method based on the Schrödinger functional is employed, which enables us to perform all calculations at zero or nearly zero quark mass. As a by-product the critical hopping parameter $\kappa_c$ is obtained at all couplings considered.The coefficients multiplying the counterterms required for O($a$) improvement of the action and the isovector axial current in lattice QCD are computed non-perturbatively, in the quenched approximation and for bare gauge couplings $g_0$ in the range $0 \leq g_0 \leq 1$. A finite-size method based on the Schr\"odinger functional is employed, which enables us to perform all calculations at zero or nearly zero quark mass. As a by-product the critical hopping parameter $\kappa_c$ is obtained at all couplings considered.The coefficients multiplying the counterterms required for O($a$) improvement of the action and the isovector axial current in lattice QCD are computed non-perturbatively, in the quenched approximation and for bare gauge couplings $g_0$ in the range $0 \leq g_0 \leq 1$. A finite-size method based on the Schr\"odinger functional is employed, which enables us to perform all calculations at zero or nearly zero quark mass. As a by-product the critical hopping parameter $\kappa_c$ is obtained at all couplings considered.The coefficients multiplying the counterterms required for O( a ) improvement of the action and the isovector axial current in lattice QCD are computed non-perturbatively, in the quenched approximation and for bare gauge couplings g 0 i range 0 ⩽ g 0 ⩽ 1. A finite-size method based on the Schrödinger functional is employed, which enables us to perform all calculations at z nearly zero quark mass. As a by-product the critical hopping parameter κ c is obtained at all couplings considered.hep-lat/9609035CERN-TH-96-218DESY-96-180HUB-EP-96-46MPI-PHT-96-75FSU-SCRI-96-101CERN-TH-96-218DESY-96-180FSU-SCRI-96-101HUB-EP-96-46MPI-PHT-96-75oai:cds.cern.ch:3111171996-09-19
spellingShingle Particle Physics - Lattice
Luscher, Martin
Sint, Stefan
Sommer, Rainer
Weisz, Peter
Wolff, Ulli
Non-perturbative O(a) improvement of lattice QCD
title Non-perturbative O(a) improvement of lattice QCD
title_full Non-perturbative O(a) improvement of lattice QCD
title_fullStr Non-perturbative O(a) improvement of lattice QCD
title_full_unstemmed Non-perturbative O(a) improvement of lattice QCD
title_short Non-perturbative O(a) improvement of lattice QCD
title_sort non-perturbative o(a) improvement of lattice qcd
topic Particle Physics - Lattice
url https://dx.doi.org/10.1016/S0550-3213(97)00080-1
http://cds.cern.ch/record/311117
work_keys_str_mv AT luschermartin nonperturbativeoaimprovementoflatticeqcd
AT sintstefan nonperturbativeoaimprovementoflatticeqcd
AT sommerrainer nonperturbativeoaimprovementoflatticeqcd
AT weiszpeter nonperturbativeoaimprovementoflatticeqcd
AT wolffulli nonperturbativeoaimprovementoflatticeqcd

Ejemplares similares