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Dispersion relations from the hard thermal loop effective action in a magnetic field

Dispersion relations for fermions at high temperature and in a background magnetic field are calculated in two different ways. First from a straightforward one-loop calculation where, in the weak field limit, we find an expression closely related to the standard dispersion relations in the absence o...

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Autor principal: Elmfors, Per
Lenguaje:eng
Publicado: 1995
Materias:
Acceso en línea:http://cds.cern.ch/record/289771
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author Elmfors, Per
author_facet Elmfors, Per
author_sort Elmfors, Per
collection CERN
description Dispersion relations for fermions at high temperature and in a background magnetic field are calculated in two different ways. First from a straightforward one-loop calculation where, in the weak field limit, we find an expression closely related to the standard dispersion relations in the absence of the magnetic field. Secondly, we derive the dispersion relations directly from the Hard Thermal Loop effective action, which allows for an exact solution (i.e. to all orders in the external field), up to the last numerical integrals.
id cern-289771
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1995
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spelling cern-2897712023-03-14T16:35:07Zhttp://cds.cern.ch/record/289771engElmfors, PerDispersion relations from the hard thermal loop effective action in a magnetic fieldParticle Physics - PhenomenologyDispersion relations for fermions at high temperature and in a background magnetic field are calculated in two different ways. First from a straightforward one-loop calculation where, in the weak field limit, we find an expression closely related to the standard dispersion relations in the absence of the magnetic field. Secondly, we derive the dispersion relations directly from the Hard Thermal Loop effective action, which allows for an exact solution (i.e. to all orders in the external field), up to the last numerical integrals.Dispersion relations for fermions at high temperature and in a background magnetic field are calculated in two different ways. First from a straightforward one-loop calculation where, in the weak field limit, we find an expression closely related to the standard dispersion relations in the absence of the magnetic field. Secondly, we derive the dispersion relations directly from the Hard Thermal Loop effective action, which allows for an exact solution (i.e. to all orders in the external field), up to the last numerical integrals.hep-ph/9510314CERN-TH-95-274oai:cds.cern.ch:2897711995-10-17
spellingShingle Particle Physics - Phenomenology
Elmfors, Per
Dispersion relations from the hard thermal loop effective action in a magnetic field
title Dispersion relations from the hard thermal loop effective action in a magnetic field
title_full Dispersion relations from the hard thermal loop effective action in a magnetic field
title_fullStr Dispersion relations from the hard thermal loop effective action in a magnetic field
title_full_unstemmed Dispersion relations from the hard thermal loop effective action in a magnetic field
title_short Dispersion relations from the hard thermal loop effective action in a magnetic field
title_sort dispersion relations from the hard thermal loop effective action in a magnetic field
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/289771
work_keys_str_mv AT elmforsper dispersionrelationsfromthehardthermalloopeffectiveactioninamagneticfield