Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model

We present an analytic calculation of the paramagnetic and diamagnetic contributions to the one-loop effective action in the SU(2) Higgs model. The paramagnetic contribution is produced by the gauge boson, while the diamagnetic contribution is produced by the gauge boson and the ghost. In the limit,...

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Main Author: Dmitry Antonov
Format: Article
Language:English
Published: MDPI AG 2019-10-01
Series:Symmetry
Subjects:
Online Access:https://www.mdpi.com/2073-8994/11/10/1237
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author Dmitry Antonov
author_facet Dmitry Antonov
author_sort Dmitry Antonov
collection DOAJ
description We present an analytic calculation of the paramagnetic and diamagnetic contributions to the one-loop effective action in the SU(2) Higgs model. The paramagnetic contribution is produced by the gauge boson, while the diamagnetic contribution is produced by the gauge boson and the ghost. In the limit, where these particles are massless, the standard result of −12 for the ratio of the paramagnetic to the diamagnetic contribution is reproduced. If the mass of the gauge boson and the ghost become much larger than the inverse vacuum correlation lengths of the Yang−Mills vacuum, the value of the ratio goes to −8. We also find that the same values of the ratio are achieved in the deconfinement phase of the model, up to the temperatures at which the dimensional reduction occurs.
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spelling doaj.art-69e231d3db924eed84658897385020ef2022-12-22T04:23:13ZengMDPI AGSymmetry2073-89942019-10-011110123710.3390/sym11101237sym11101237Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs ModelDmitry Antonov0Formerly at Departamento de Física and CFIF, Instituto Superior Técnico, ULisboa, Av. Rovisco Pais, 1049-001 Lisbon, PortugalWe present an analytic calculation of the paramagnetic and diamagnetic contributions to the one-loop effective action in the SU(2) Higgs model. The paramagnetic contribution is produced by the gauge boson, while the diamagnetic contribution is produced by the gauge boson and the ghost. In the limit, where these particles are massless, the standard result of −12 for the ratio of the paramagnetic to the diamagnetic contribution is reproduced. If the mass of the gauge boson and the ghost become much larger than the inverse vacuum correlation lengths of the Yang−Mills vacuum, the value of the ratio goes to −8. We also find that the same values of the ratio are achieved in the deconfinement phase of the model, up to the temperatures at which the dimensional reduction occurs.https://www.mdpi.com/2073-8994/11/10/1237higgs modelyang–mills vacuumeffective actionworld-line formalismwilson loop
spellingShingle Dmitry Antonov
Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model
Symmetry
higgs model
yang–mills vacuum
effective action
world-line formalism
wilson loop
title Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model
title_full Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model
title_fullStr Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model
title_full_unstemmed Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model
title_short Paramagnetic versus Diamagnetic Interaction in the SU(2) Higgs Model
title_sort paramagnetic versus diamagnetic interaction in the su 2 higgs model
topic higgs model
yang–mills vacuum
effective action
world-line formalism
wilson loop
url https://www.mdpi.com/2073-8994/11/10/1237
work_keys_str_mv AT dmitryantonov paramagneticversusdiamagneticinteractioninthesu2higgsmodel