OSEFT or how to go beyond hard thermal loops
We show that effective field theory techniques can be applied in the high temperature T regime of plasmas to improve the accuracy of the physics of the hard scales (or scales of order T), and as a by-product, also that of the soft scales (or scales of order gT). At leading order in the coupling cons...
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2017-01-01
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Series: | EPJ Web of Conferences |
Online Access: | https://doi.org/10.1051/epjconf/201713707014 |
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doaj-cea0d8b485d64cf0b980719cf67f2df32021-08-02T12:42:12ZengEDP SciencesEPJ Web of Conferences2100-014X2017-01-011370701410.1051/epjconf/201713707014epjconf_conf2017_07014OSEFT or how to go beyond hard thermal loopsManuel Cristina0Soto Joan1Stetina Stephan2Instituto de Ciencias del Espacio (IEEC/CSIC) C. Can Magrans s.n.Departament de Fisica Quàntica i Astrofisica and Institut de Ciències del Cosmos, Universitat de BarcelonaInstitute for Nuclear Theory, University of WashingtonWe show that effective field theory techniques can be applied in the high temperature T regime of plasmas to improve the accuracy of the physics of the hard scales (or scales of order T), and as a by-product, also that of the soft scales (or scales of order gT). At leading order in the coupling constant the hard scales of the plasma can be viewed as on-shell classical particles. Based on this observation, and without any reference to the state of the system, we derive an effective field theory describing the quantum fluctuations around an on-shell fermion with energy p, described as a set of high dimension operators over the on-shell energy p. When applied to systems close to thermal equilibrium, where for most on-shell particles p ~ T, we show that the on-shell effective field theory (OSEFT) properly describes the HTL photon polarization tensor of QED, and its 1/T corrections. For the soft scales the first non-vanishing power correction turns out to be a perturbative correction to the HTL result.https://doi.org/10.1051/epjconf/201713707014 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Manuel Cristina Soto Joan Stetina Stephan |
spellingShingle |
Manuel Cristina Soto Joan Stetina Stephan OSEFT or how to go beyond hard thermal loops EPJ Web of Conferences |
author_facet |
Manuel Cristina Soto Joan Stetina Stephan |
author_sort |
Manuel Cristina |
title |
OSEFT or how to go beyond hard thermal loops |
title_short |
OSEFT or how to go beyond hard thermal loops |
title_full |
OSEFT or how to go beyond hard thermal loops |
title_fullStr |
OSEFT or how to go beyond hard thermal loops |
title_full_unstemmed |
OSEFT or how to go beyond hard thermal loops |
title_sort |
oseft or how to go beyond hard thermal loops |
publisher |
EDP Sciences |
series |
EPJ Web of Conferences |
issn |
2100-014X |
publishDate |
2017-01-01 |
description |
We show that effective field theory techniques can be applied in the high temperature T regime of plasmas to improve the accuracy of the physics of the hard scales (or scales of order T), and as a by-product, also that of the soft scales (or scales of order gT). At leading order in the coupling constant the hard scales of the plasma can be viewed as on-shell classical particles. Based on this observation, and without any reference to the state of the system, we derive an effective field theory describing the quantum fluctuations around an on-shell fermion with energy p, described as a set of high dimension operators over the on-shell energy p. When applied to systems close to thermal equilibrium, where for most on-shell particles p ~ T, we show that the on-shell effective field theory (OSEFT) properly describes the HTL photon polarization tensor of QED, and its 1/T corrections. For the soft scales the first non-vanishing power correction turns out to be a perturbative correction to the HTL result. |
url |
https://doi.org/10.1051/epjconf/201713707014 |
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AT manuelcristina oseftorhowtogobeyondhardthermalloops AT sotojoan oseftorhowtogobeyondhardthermalloops AT stetinastephan oseftorhowtogobeyondhardthermalloops |
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