Reduction for one-loop tensor Feynman integrals in the relativistic quantum field theories at finite temperature and/or finite density

Fuente: arXiv
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Autore principale: Chang, Hao-Ran
Natura: Preprint
Pubblicazione: 2020
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author Chang, Hao-Ran
author_facet Chang, Hao-Ran
contents The \emph{conventional} Passarino-Veltman reduction is a systematic procedure based on the Lorentz covariance, which can efficiently reduce the one-loop tensor Feynman integrals in the relativistic quantum field theories (QFTs) at zero temperature and zero density. However, the Lorentz covariance is explicitly broken when either of the temperature and density is finite, due to a rest reference frame of the many-body system in which the temperature and density are measured, rendering the \emph{conventional} Passarino-Veltman reduction not applicable anymore to reduce the one-loop tensor Feynman integrals therein. In this paper, we report a \emph{generalized} Passarino-Veltman reduction which can efficiently simplify the one-loop tensor Feynman integrals in the relativistic QFTs at finite temperature and/or finite density. The \emph{generalized} Passarino-Veltman reduction can analyze the one-loop tensor Feynman integrals in a wide range of physical systems described by the relativistic QFTs at finite temperature and/or finite density, such as quark-gluon plasma in nuclear physics.
format Preprint
id arxiv_https___arxiv_org_abs_2008_11314
institution arXiv
publishDate 2020
record_format arxiv
spellingShingle Reduction for one-loop tensor Feynman integrals in the relativistic quantum field theories at finite temperature and/or finite density
Chang, Hao-Ran
High Energy Physics - Phenomenology
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
Nuclear Theory
The \emph{conventional} Passarino-Veltman reduction is a systematic procedure based on the Lorentz covariance, which can efficiently reduce the one-loop tensor Feynman integrals in the relativistic quantum field theories (QFTs) at zero temperature and zero density. However, the Lorentz covariance is explicitly broken when either of the temperature and density is finite, due to a rest reference frame of the many-body system in which the temperature and density are measured, rendering the \emph{conventional} Passarino-Veltman reduction not applicable anymore to reduce the one-loop tensor Feynman integrals therein. In this paper, we report a \emph{generalized} Passarino-Veltman reduction which can efficiently simplify the one-loop tensor Feynman integrals in the relativistic QFTs at finite temperature and/or finite density. The \emph{generalized} Passarino-Veltman reduction can analyze the one-loop tensor Feynman integrals in a wide range of physical systems described by the relativistic QFTs at finite temperature and/or finite density, such as quark-gluon plasma in nuclear physics.
title Reduction for one-loop tensor Feynman integrals in the relativistic quantum field theories at finite temperature and/or finite density
topic High Energy Physics - Phenomenology
Mesoscale and Nanoscale Physics
Strongly Correlated Electrons
Nuclear Theory
url https://arxiv.org/abs/2008.11314