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Dense quark–gluon plasma in strong magnetic fields
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 ∼ 0.16 GeV ) and nonzero baryon densities (baryon chemical potential μ B < 0.5 GeV ) in an external uniform magnetic field ( e B <...
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Published in: | The European physical journal. C, Particles and fields Particles and fields, 2019-12, Vol.79 (12), p.1-7, Article 1040 |
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container_issue | 12 |
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container_title | The European physical journal. C, Particles and fields |
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creator | Abramchuk, R. A. Andreichikov, M. A. Khaidukov, Z. V. Simonov, Yu. A. |
description | 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
∼
0.16
GeV
) and nonzero baryon densities (baryon chemical potential
μ
B
<
0.5
GeV
) in an external uniform magnetic field (
e
B
<
0.5
GeV
2
). 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. |
doi_str_mv | 10.1140/epjc/s10052-019-7548-z |
format | article |
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1
<
T
/
T
c
<
3
,
T
c
∼
0.16
GeV
) and nonzero baryon densities (baryon chemical potential
μ
B
<
0.5
GeV
) in an external uniform magnetic field (
e
B
<
0.5
GeV
2
). 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.</description><identifier>ISSN: 1434-6044</identifier><identifier>EISSN: 1434-6052</identifier><identifier>DOI: 10.1140/epjc/s10052-019-7548-z</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Astronomy ; Astrophysics and Cosmology ; Baryons ; Chemical potential ; Correlation analysis ; Density ; Elementary Particles ; Gluons ; Hadrons ; Heavy Ions ; High temperature ; Magnetic fields ; Magnetic permeability ; Magnetism ; Measurement Science and Instrumentation ; Nuclear Energy ; Nuclear Physics ; Organic chemistry ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quark-gluon plasma ; Quarks ; Regular Article - Theoretical Physics ; Specific heat ; String Theory</subject><ispartof>The European physical journal. C, Particles and fields, 2019-12, Vol.79 (12), p.1-7, Article 1040</ispartof><rights>The Author(s) 2019</rights><rights>COPYRIGHT 2019 Springer</rights><rights>The European Physical Journal C is a copyright of Springer, (2019). All Rights Reserved. This work is published under https://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c518t-457c82636c9b5ad13495c885a853db17c02b84b70330ab8e5699ef6c7bc91e323</citedby><cites>FETCH-LOGICAL-c518t-457c82636c9b5ad13495c885a853db17c02b84b70330ab8e5699ef6c7bc91e323</cites><orcidid>0000-0001-6258-0133</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2331383727/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2331383727?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,25753,27924,27925,37012,44590,75126</link.rule.ids></links><search><creatorcontrib>Abramchuk, R. A.</creatorcontrib><creatorcontrib>Andreichikov, M. A.</creatorcontrib><creatorcontrib>Khaidukov, Z. V.</creatorcontrib><creatorcontrib>Simonov, Yu. A.</creatorcontrib><title>Dense quark–gluon plasma in strong magnetic fields</title><title>The European physical journal. C, Particles and fields</title><addtitle>Eur. Phys. J. C</addtitle><description>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
∼
0.16
GeV
) and nonzero baryon densities (baryon chemical potential
μ
B
<
0.5
GeV
) in an external uniform magnetic field (
e
B
<
0.5
GeV
2
). 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.</description><subject>Astronomy</subject><subject>Astrophysics and Cosmology</subject><subject>Baryons</subject><subject>Chemical potential</subject><subject>Correlation analysis</subject><subject>Density</subject><subject>Elementary Particles</subject><subject>Gluons</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>High temperature</subject><subject>Magnetic fields</subject><subject>Magnetic permeability</subject><subject>Magnetism</subject><subject>Measurement Science and Instrumentation</subject><subject>Nuclear Energy</subject><subject>Nuclear Physics</subject><subject>Organic chemistry</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quark-gluon plasma</subject><subject>Quarks</subject><subject>Regular Article - Theoretical Physics</subject><subject>Specific heat</subject><subject>String Theory</subject><issn>1434-6044</issn><issn>1434-6052</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><sourceid>DOA</sourceid><recordid>eNqFkc1O3TAQhaOKSgXaV6gisWIRGMe_WSKg9EpISP1ZW7YziXKba1_sRAJWfQfekCfBt0EgVpUXY43Od3RGpyi-EjghhMEpbtfuNBEAXldAmkpypqqHD8U-YZRVIq_3Xv-MfSoOUloDQM1A7RfsAn3C8nY28c_T38d-nIMvt6NJG1MOvkxTDL4vN6b3OA2u7AYc2_S5-NiZMeGXl3lY_P52-ev8e3V9c7U6P7uuHCdqqhiXTtWCCtdYblpCWcOdUtwoTltLpIPaKmYlUArGKuSiabATTlrXEKQ1PSxWi28bzFpv47Ax8V4HM-h_ixB7bWKONaKGVjrrBCiLihnlmk4yobBtaW0pEJW9jhavbQy3M6ZJr8McfY6va0oJVVTWMqtOFlVvsunguzBF4_JrcTO44LEb8v5MECD5RNFk4PgdkDUT3k29mVPSq58_3mvFonUxpBSxez2JgN5VqXdV6qVKnavUuyr1QwblAqYM-B7jW_b_kM99K6N2</recordid><startdate>20191201</startdate><enddate>20191201</enddate><creator>Abramchuk, R. A.</creator><creator>Andreichikov, M. A.</creator><creator>Khaidukov, Z. V.</creator><creator>Simonov, Yu. A.</creator><general>Springer Berlin Heidelberg</general><general>Springer</general><general>Springer Nature B.V</general><general>SpringerOpen</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>ISR</scope><scope>7U5</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>DOA</scope><orcidid>https://orcid.org/0000-0001-6258-0133</orcidid></search><sort><creationdate>20191201</creationdate><title>Dense quark–gluon plasma in strong magnetic fields</title><author>Abramchuk, R. A. ; Andreichikov, M. A. ; Khaidukov, Z. V. ; Simonov, Yu. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c518t-457c82636c9b5ad13495c885a853db17c02b84b70330ab8e5699ef6c7bc91e323</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Astronomy</topic><topic>Astrophysics and Cosmology</topic><topic>Baryons</topic><topic>Chemical potential</topic><topic>Correlation analysis</topic><topic>Density</topic><topic>Elementary Particles</topic><topic>Gluons</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>High temperature</topic><topic>Magnetic fields</topic><topic>Magnetic permeability</topic><topic>Magnetism</topic><topic>Measurement Science and Instrumentation</topic><topic>Nuclear Energy</topic><topic>Nuclear Physics</topic><topic>Organic chemistry</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quark-gluon plasma</topic><topic>Quarks</topic><topic>Regular Article - Theoretical Physics</topic><topic>Specific heat</topic><topic>String Theory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Abramchuk, R. 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C, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Abramchuk, R. A.</au><au>Andreichikov, M. A.</au><au>Khaidukov, Z. V.</au><au>Simonov, Yu. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dense quark–gluon plasma in strong magnetic fields</atitle><jtitle>The European physical journal. C, Particles and fields</jtitle><stitle>Eur. Phys. J. C</stitle><date>2019-12-01</date><risdate>2019</risdate><volume>79</volume><issue>12</issue><spage>1</spage><epage>7</epage><pages>1-7</pages><artnum>1040</artnum><issn>1434-6044</issn><eissn>1434-6052</eissn><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
∼
0.16
GeV
) and nonzero baryon densities (baryon chemical potential
μ
B
<
0.5
GeV
) in an external uniform magnetic field (
e
B
<
0.5
GeV
2
). 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.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epjc/s10052-019-7548-z</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0001-6258-0133</orcidid><oa>free_for_read</oa></addata></record> |
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language | eng |
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source | Publicly Available Content Database (Proquest) (PQ_SDU_P3); Springer Nature - SpringerLink Journals - Fully Open Access |
subjects | Astronomy Astrophysics and Cosmology Baryons Chemical potential Correlation analysis Density Elementary Particles Gluons Hadrons Heavy Ions High temperature Magnetic fields Magnetic permeability Magnetism Measurement Science and Instrumentation Nuclear Energy Nuclear Physics Organic chemistry Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quark-gluon plasma Quarks Regular Article - Theoretical Physics Specific heat String Theory |
title | Dense quark–gluon plasma in strong magnetic fields |
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