Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD

Using quenched and unquenched chiral perturbation theory we compute vector and axial current two-point functions at finite volume and fixed gauge field topology, in the so-called \epsilon-regime of QCD. A comparison of these results with finite volume lattice calculations allows to determine the par...

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Detalles Bibliográficos
Autores principales: Damgaard, P.H., Hernandez, P., Jansen, K., Laine, M., Lellouch, L.
Lenguaje:eng
Publicado: 2003
Materias:
Particle Physics - Lattice
Acceso en línea:https://dx.doi.org/10.1016/S0920-5632(03)02703-8
http://cds.cern.ch/record/640974
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author Damgaard, P.H.
Hernandez, P.
Jansen, K.
Laine, M.
Lellouch, L.
author_facet Damgaard, P.H.
Hernandez, P.
Jansen, K.
Laine, M.
Lellouch, L.
author_sort Damgaard, P.H.
collection CERN
description Using quenched and unquenched chiral perturbation theory we compute vector and axial current two-point functions at finite volume and fixed gauge field topology, in the so-called \epsilon-regime of QCD. A comparison of these results with finite volume lattice calculations allows to determine the parameters of the corresponding chiral Lagrangians.
id cern-640974
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2003
record_format invenio
spelling cern-6409742023-03-14T20:26:36Zdoi:10.1016/S0920-5632(03)02703-8http://cds.cern.ch/record/640974engDamgaard, P.H.Hernandez, P.Jansen, K.Laine, M.Lellouch, L.Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCDParticle Physics - LatticeUsing quenched and unquenched chiral perturbation theory we compute vector and axial current two-point functions at finite volume and fixed gauge field topology, in the so-called \epsilon-regime of QCD. A comparison of these results with finite volume lattice calculations allows to determine the parameters of the corresponding chiral Lagrangians.Using quenched and unquenched chiral perturbation theory we compute vector and axial current two-point functions at finite volume and fixed gauge field topology, in the so-called \epsilon-regime of QCD. A comparison of these results with finite volume lattice calculations allows to determine the parameters of the corresponding chiral Lagrangians.hep-lat/0309015DESY-03-191oai:cds.cern.ch:6409742003
spellingShingle Particle Physics - Lattice
Damgaard, P.H.
Hernandez, P.
Jansen, K.
Laine, M.
Lellouch, L.
Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD
title Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD
title_full Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD
title_fullStr Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD
title_full_unstemmed Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD
title_short Vector and Axial-Vector Propagators in the $\epsilon$-Regime of QCD
title_sort vector and axial-vector propagators in the $\epsilon$-regime of qcd
topic Particle Physics - Lattice
url https://dx.doi.org/10.1016/S0920-5632(03)02703-8
http://cds.cern.ch/record/640974
work_keys_str_mv AT damgaardph vectorandaxialvectorpropagatorsintheepsilonregimeofqcd
AT hernandezp vectorandaxialvectorpropagatorsintheepsilonregimeofqcd
AT jansenk vectorandaxialvectorpropagatorsintheepsilonregimeofqcd
AT lainem vectorandaxialvectorpropagatorsintheepsilonregimeofqcd
AT lellouchl vectorandaxialvectorpropagatorsintheepsilonregimeofqcd

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