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The non-perturbative QCD Debye mass from a Wilson line operator

According to a proposal by Arnold and Yaffe, the non-perturbative g^2T-contribution to the Debye mass in the deconfined QCD plasma phase can be determined from a single Wilson line operator in the three-dimensional pure SU(3) gauge theory. We extend a previous SU(2) measurement of this quantity to t...

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Autores principales: Laine, M., Philipsen, O.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(99)00641-3
http://cds.cern.ch/record/386617
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author Laine, M.
Philipsen, O.
author_facet Laine, M.
Philipsen, O.
author_sort Laine, M.
collection CERN
description According to a proposal by Arnold and Yaffe, the non-perturbative g^2T-contribution to the Debye mass in the deconfined QCD plasma phase can be determined from a single Wilson line operator in the three-dimensional pure SU(3) gauge theory. We extend a previous SU(2) measurement of this quantity to the physical SU(3) case. We find a numerical coefficient which is more accurate and smaller than that obtained previously with another method, but still very large compared with the naive expectation: the correction is larger than the leading term up to T ~ 10^7 T_c, corresponding to g^2 ~ 0.4. At moderate temperatures T ~ 2 T_c, a consistent picture emerges where the Debye mass is m_D ~ 6T, the lightest gauge invariant screening mass in the system is ~ 3T, and the purely magnetic operators couple dominantly to a scale ~ 6T. Electric (~ gT) and magnetic (~ g^2T) scales are therefore strongly overlapping close to the phase transition, and the colour-electric fields play an essential role in the dynamics.
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institution Organización Europea para la Investigación Nuclear
language eng
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spelling cern-3866172023-03-14T18:44:58Zdoi:10.1016/S0370-2693(99)00641-3http://cds.cern.ch/record/386617engLaine, M.Philipsen, O.The non-perturbative QCD Debye mass from a Wilson line operatorParticle Physics - LatticeAccording to a proposal by Arnold and Yaffe, the non-perturbative g^2T-contribution to the Debye mass in the deconfined QCD plasma phase can be determined from a single Wilson line operator in the three-dimensional pure SU(3) gauge theory. We extend a previous SU(2) measurement of this quantity to the physical SU(3) case. We find a numerical coefficient which is more accurate and smaller than that obtained previously with another method, but still very large compared with the naive expectation: the correction is larger than the leading term up to T ~ 10^7 T_c, corresponding to g^2 ~ 0.4. At moderate temperatures T ~ 2 T_c, a consistent picture emerges where the Debye mass is m_D ~ 6T, the lightest gauge invariant screening mass in the system is ~ 3T, and the purely magnetic operators couple dominantly to a scale ~ 6T. Electric (~ gT) and magnetic (~ g^2T) scales are therefore strongly overlapping close to the phase transition, and the colour-electric fields play an essential role in the dynamics.According to a proposal by Arnold and Yaffe, the non-perturbative g^2T-contribution to the Debye mass in the deconfined QCD plasma phase can be determined from a single Wilson line operator in the three-dimensional pure SU(3) gauge theory. We extend a previous SU(2) measurement of this quantity to the physical SU(3) case. We find a numerical coefficient which is more accurate and smaller than that obtained previously with another method, but still very large compared with the naive expectation: the correction is larger than the leading term up to T ~ 10^7 T_c, corresponding to g^2 ~ 0.4. At moderate temperatures T ~ 2 T_c, a consistent picture emerges where the Debye mass is m_D ~ 6T, the lightest gauge invariant screening mass in the system is ~ 3T, and the purely magnetic operators couple dominantly to a scale ~ 6T. Electric (~ gT) and magnetic (~ g^2T) scales are therefore strongly overlapping close to the phase transition, and the colour-electric fields play an essential role in the dynamics.According to a proposal by Arnold and Yaffe, the non-perturbative g 2 T -contribution to the Debye mass in the deconfined QCD plasma phase can be determined from a single Wilson line operator in the three-dimensional pure SU(3) gauge theory. We extend a previous SU(2) measurement of this quantity to the physical SU(3) case. We find a numerical coefficient which is more accurate and smaller than that obtained previously with another method, but still very large compared with the naive expectation: the correction is larger than the leading term up to T ∼10 7 T c , corresponding to g 2 ∼0.4. At moderate temperatures T ∼2 T c , a consistent picture emerges where the Debye mass is m D ∼6 T , the lightest gauge invariant screening mass in the system is ∼3 T , and the purely magnetic operators couple dominantly to a scale ∼6 T . Electric (∼ gT ) and magnetic (∼ g 2 T ) scales are therefore strongly overlapping close to the phase transition, and the colour-electric fields play an essential role in the dynamics.hep-lat/9905004CERN-TH-99-124CERN-TH-99-124oai:cds.cern.ch:3866171999-05-06
spellingShingle Particle Physics - Lattice
Laine, M.
Philipsen, O.
The non-perturbative QCD Debye mass from a Wilson line operator
title The non-perturbative QCD Debye mass from a Wilson line operator
title_full The non-perturbative QCD Debye mass from a Wilson line operator
title_fullStr The non-perturbative QCD Debye mass from a Wilson line operator
title_full_unstemmed The non-perturbative QCD Debye mass from a Wilson line operator
title_short The non-perturbative QCD Debye mass from a Wilson line operator
title_sort non-perturbative qcd debye mass from a wilson line operator
topic Particle Physics - Lattice
url https://dx.doi.org/10.1016/S0370-2693(99)00641-3
http://cds.cern.ch/record/386617
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