Chiral perturbation theory

Fuente: arXiv
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Main Author: Meißner, Ulf-G.
Format: Preprint
Published: 2024
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author Meißner, Ulf-G.
author_facet Meißner, Ulf-G.
contents In the limit of vanishing up, down and strange quark masses, QCD exhibits a chiral symmetry. This symmetry is broken spontaneously to its vector subgroup, giving rise to Goldstone bosons. These acquire a small mass through the explicit chiral symmetry breaking for non-vanishing quark masses. The consequences of these broken symmetries can be investigated in a suitably tailored effective field theory called chiral pertubation theory. It admits a perturbative expansion in the external momenta and the Goldstone boson masses and can be systematically analyzed in terms of a loop expansion. The appearing ultraviolet divergences in loop diagrams can be dealt with order-by-order through the Goldstone boson contact interactions. Matter fields like the lowest-lying baryons can also included, leading to a rich and testable phenomenology of low-energy QCD.
format Preprint
id arxiv_https___arxiv_org_abs_2410_21912
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Chiral perturbation theory
Meißner, Ulf-G.
High Energy Physics - Phenomenology
High Energy Physics - Experiment
High Energy Physics - Theory
Nuclear Experiment
Nuclear Theory
In the limit of vanishing up, down and strange quark masses, QCD exhibits a chiral symmetry. This symmetry is broken spontaneously to its vector subgroup, giving rise to Goldstone bosons. These acquire a small mass through the explicit chiral symmetry breaking for non-vanishing quark masses. The consequences of these broken symmetries can be investigated in a suitably tailored effective field theory called chiral pertubation theory. It admits a perturbative expansion in the external momenta and the Goldstone boson masses and can be systematically analyzed in terms of a loop expansion. The appearing ultraviolet divergences in loop diagrams can be dealt with order-by-order through the Goldstone boson contact interactions. Matter fields like the lowest-lying baryons can also included, leading to a rich and testable phenomenology of low-energy QCD.
title Chiral perturbation theory
topic High Energy Physics - Phenomenology
High Energy Physics - Experiment
High Energy Physics - Theory
Nuclear Experiment
Nuclear Theory
url https://arxiv.org/abs/2410.21912