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Leontovich Relations in Thermal Field Theory
The application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle...
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Lenguaje: | eng |
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2000
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Acceso en línea: | https://dx.doi.org/10.1007/s100520000440 http://cds.cern.ch/record/434994 |
_version_ | 1780895384841748480 |
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author | Thoma, Markus H. |
author_facet | Thoma, Markus H. |
author_sort | Thoma, Markus H. |
collection | CERN |
description | The application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle in a relativistic plasma and the radiation of energetic photons from a quark-gluon plasma are considered. Within the leading logarithmic approximation the results based on the hard thermal loop resummation technique are reproduced easily. However, the method presented here is more general and provides exact expressions, which allow in principle non-perturbative calculations. |
id | cern-434994 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2000 |
record_format | invenio |
spelling | cern-4349942023-03-14T17:02:42Zdoi:10.1007/s100520000440http://cds.cern.ch/record/434994engThoma, Markus H.Leontovich Relations in Thermal Field TheoryParticle Physics - PhenomenologyThe application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle in a relativistic plasma and the radiation of energetic photons from a quark-gluon plasma are considered. Within the leading logarithmic approximation the results based on the hard thermal loop resummation technique are reproduced easily. However, the method presented here is more general and provides exact expressions, which allow in principle non-perturbative calculations.The application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle in a relativistic plasma and the radiation of energetic photons from a quark-gluon plasma are considered. Within the leading logarithmic approximation the results based on the hard thermal loop resummation technique are reproduced easily. However, the method presented here is more general and provides exact expressions, which allow in principle non-perturbative calculations.The application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle in a relativistic plasma and the radiation of energetic photons from a quark-gluon plasma are considered. Within the leading logarithmic approximation the results based on the hard thermal loop resummation technique are reproduced easily. However, the method presented here is more general and provides exact expressions, which allow in principle non-perturbative calculations.The application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle in a relativistic plasma and the radiation of energetic photons from a quark-gluon plasma are considered. Within the leading logarithmic approximation the results based on the hard thermal loop resummation technique are reproduced easily. However, the method presented here is more general and provides exact expressions, which allow in principle non-perturbative calculations.The application of generalized Kramers-Kronig relations, the so-called Leontovich relations, to thermal field theory is discussed. Medium effects contained in the full, thermal propagators can easily be taken into account by this method. As examples the collisional energy loss of a charged particle in a relativistic plasma and the radiation of energetic photons from a quark-gluon plasma are considered. Within the leading logarithmic approximation the results based on the hard thermal loop resummation technique are reproduced easily. However, the method presented here is more general and provides exact expressions, which allow in principle non-perturbative calculations.hep-ph/0004146oai:cds.cern.ch:4349942000 |
spellingShingle | Particle Physics - Phenomenology Thoma, Markus H. Leontovich Relations in Thermal Field Theory |
title | Leontovich Relations in Thermal Field Theory |
title_full | Leontovich Relations in Thermal Field Theory |
title_fullStr | Leontovich Relations in Thermal Field Theory |
title_full_unstemmed | Leontovich Relations in Thermal Field Theory |
title_short | Leontovich Relations in Thermal Field Theory |
title_sort | leontovich relations in thermal field theory |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/s100520000440 http://cds.cern.ch/record/434994 |
work_keys_str_mv | AT thomamarkush leontovichrelationsinthermalfieldtheory |