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Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit

We present results for lattice QCD in the limit of infinite gauge coupling, obtained from a worm-type Monte Carlo algorithm on a discrete spatial lattice but with continuous Euclidean time. This is obtained by sending both the anisotropy parameter gamma^2 \sim a/a_t and the number of time-slices N_\...

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Detalles Bibliográficos
Autores principales: Unger, Wolfgang, de Forcrand, Philippe
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:https://dx.doi.org/10.1088/0954-3899/38/12/124190
http://cds.cern.ch/record/1366491
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author Unger, Wolfgang
de Forcrand, Philippe
author_facet Unger, Wolfgang
de Forcrand, Philippe
author_sort Unger, Wolfgang
collection CERN
description We present results for lattice QCD in the limit of infinite gauge coupling, obtained from a worm-type Monte Carlo algorithm on a discrete spatial lattice but with continuous Euclidean time. This is obtained by sending both the anisotropy parameter gamma^2 \sim a/a_t and the number of time-slices N_\tau to infinity, keeping the ratio \gamma^2/N_\tau \sim aT fixed. The obvious gain is that no continuum extrapolation N_\tau -> \infty has to be carried out. Moreover, the algorithm is faster and the sign problem disappears. We compare our computations with those on discrete lattices. We determine the phase diagram as a function of temperature and baryon chemical potential.
id cern-1366491
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2011
record_format invenio
spelling cern-13664912019-09-30T06:29:59Zdoi:10.1088/0954-3899/38/12/124190http://cds.cern.ch/record/1366491engUnger, Wolfgangde Forcrand, PhilippeContinuous Time Monte Carlo for Lattice QCD in the Strong Coupling LimitParticle Physics - LatticeWe present results for lattice QCD in the limit of infinite gauge coupling, obtained from a worm-type Monte Carlo algorithm on a discrete spatial lattice but with continuous Euclidean time. This is obtained by sending both the anisotropy parameter gamma^2 \sim a/a_t and the number of time-slices N_\tau to infinity, keeping the ratio \gamma^2/N_\tau \sim aT fixed. The obvious gain is that no continuum extrapolation N_\tau -> \infty has to be carried out. Moreover, the algorithm is faster and the sign problem disappears. We compare our computations with those on discrete lattices. We determine the phase diagram as a function of temperature and baryon chemical potential.arXiv:1107.1553CERN-PH-TH-2011-158oai:cds.cern.ch:13664912011-07-11
spellingShingle Particle Physics - Lattice
Unger, Wolfgang
de Forcrand, Philippe
Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit
title Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit
title_full Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit
title_fullStr Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit
title_full_unstemmed Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit
title_short Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit
title_sort continuous time monte carlo for lattice qcd in the strong coupling limit
topic Particle Physics - Lattice
url https://dx.doi.org/10.1088/0954-3899/38/12/124190
http://cds.cern.ch/record/1366491
work_keys_str_mv AT ungerwolfgang continuoustimemontecarloforlatticeqcdinthestrongcouplinglimit
AT deforcrandphilippe continuoustimemontecarloforlatticeqcdinthestrongcouplinglimit