Dense quark–gluon plasma in strong magnetic fields

Abstract A non-perturbative (np) method of Field correlators (FCM) was applied to study QCD at temperatures above the deconfinement transition ($$1<T/T_c<3,~T_c\sim 0.16~\mathrm{GeV}$$ 1<T/Tc<3,Tc∼0.16GeV ) and nonzero baryon densities (baryon chemical potential $$\mu _B<0.5~\mathrm{G...

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Main Authors: R. A. Abramchuk, M. A. Andreichikov, Z. V. Khaidukov, Yu. A. Simonov
Format: Article
Language:English
Published: SpringerOpen 2019-12-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-019-7548-z
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author R. A. Abramchuk
M. A. Andreichikov
Z. V. Khaidukov
Yu. A. Simonov
author_facet R. A. Abramchuk
M. A. Andreichikov
Z. V. Khaidukov
Yu. A. Simonov
author_sort R. A. Abramchuk
collection DOAJ
description Abstract A non-perturbative (np) method of Field correlators (FCM) was applied to study QCD at temperatures above the deconfinement transition ($$1<T/T_c<3,~T_c\sim 0.16~\mathrm{GeV}$$ 1<T/Tc<3,Tc∼0.16GeV ) and nonzero baryon densities (baryon chemical potential $$\mu _B<0.5~\mathrm{GeV}$$ μB<0.5GeV ) in an external uniform magnetic field ($$eB<0.5~\mathrm{GeV}^2$$ eB<0.5GeV2 ). Within FCM, the np high-temperature dynamics is embodied in the Polyakov loop and in the Debye mass due to the Color-Magnetic confinement. Analytic expressions for quark pressure and magnetic susceptibility were obtained. The expressions were represented as series and in integral form. Magnetic susceptibility was found to increase rapidly with temperature and slowly with density. The results at the zero density limit are in agreement with lattice data.
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spelling doaj.art-0d7cbc608be84a8c9f7468edd32b30182022-12-21T23:30:05ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-12-0179121710.1140/epjc/s10052-019-7548-zDense quark–gluon plasma in strong magnetic fieldsR. A. Abramchuk0M. A. Andreichikov1Z. V. Khaidukov2Yu. A. Simonov3Moscow Institute of Physics and TechnologyMoscow Institute of Physics and TechnologyMoscow Institute of Physics and TechnologyInstitute for Theoretical and Experimental Physics of NRC “Kurchatov Institute”Abstract A non-perturbative (np) method of Field correlators (FCM) was applied to study QCD at temperatures above the deconfinement transition ($$1<T/T_c<3,~T_c\sim 0.16~\mathrm{GeV}$$ 1<T/Tc<3,Tc∼0.16GeV ) and nonzero baryon densities (baryon chemical potential $$\mu _B<0.5~\mathrm{GeV}$$ μB<0.5GeV ) in an external uniform magnetic field ($$eB<0.5~\mathrm{GeV}^2$$ eB<0.5GeV2 ). Within FCM, the np high-temperature dynamics is embodied in the Polyakov loop and in the Debye mass due to the Color-Magnetic confinement. Analytic expressions for quark pressure and magnetic susceptibility were obtained. The expressions were represented as series and in integral form. Magnetic susceptibility was found to increase rapidly with temperature and slowly with density. The results at the zero density limit are in agreement with lattice data.https://doi.org/10.1140/epjc/s10052-019-7548-z
spellingShingle R. A. Abramchuk
M. A. Andreichikov
Z. V. Khaidukov
Yu. A. Simonov
Dense quark–gluon plasma in strong magnetic fields
European Physical Journal C: Particles and Fields
title Dense quark–gluon plasma in strong magnetic fields
title_full Dense quark–gluon plasma in strong magnetic fields
title_fullStr Dense quark–gluon plasma in strong magnetic fields
title_full_unstemmed Dense quark–gluon plasma in strong magnetic fields
title_short Dense quark–gluon plasma in strong magnetic fields
title_sort dense quark gluon plasma in strong magnetic fields
url https://doi.org/10.1140/epjc/s10052-019-7548-z
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AT maandreichikov densequarkgluonplasmainstrongmagneticfields
AT zvkhaidukov densequarkgluonplasmainstrongmagneticfields
AT yuasimonov densequarkgluonplasmainstrongmagneticfields