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SU(N) gauge theories near Tc

M. Teper, U. Wenger, Biagio Lucini Orcid Logo

Nuclear Physics B - Proceedings Supplements, Volume: "129", Pages: 569 - 571

Swansea University Author: Biagio Lucini Orcid Logo

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DOI (Published version): 10.1016/S0920-5632(03)02644-6

Abstract

We study the deconfinement phase transition in SU(N) gauge theories for $N$=2,3,4,6,8. The transition is first order for $N \ge 3$, with the strength increasing as $N$ increases. We extrapolate $T_c/\sqrt{\sigma}$ to the continuum limit for each $N$, and observe a rapid approach to the large $N$ lim...

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Published in: Nuclear Physics B - Proceedings Supplements
ISSN: 09205632
Published: 2003
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URI: https://cronfa.swan.ac.uk/Record/cronfa27947
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first_indexed 2016-05-15T01:22:52Z
last_indexed 2018-02-09T05:11:33Z
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spelling 2016-05-14T16:42:18.2343315 v2 27947 2016-05-14 SU(N) gauge theories near Tc 7e6fcfe060e07a351090e2a8aba363cf 0000-0001-8974-8266 Biagio Lucini Biagio Lucini true false 2016-05-14 SMA We study the deconfinement phase transition in SU(N) gauge theories for $N$=2,3,4,6,8. The transition is first order for $N \ge 3$, with the strength increasing as $N$ increases. We extrapolate $T_c/\sqrt{\sigma}$ to the continuum limit for each $N$, and observe a rapid approach to the large $N$ limit. As $N$ increases the phase transition becomes clear-cut on smaller spatial volumes, indicating the absence of (non-singular) finite volume corrections at $N=\infty$ -- reminiscent of large $N$ reduction. The observed rapid increase of the inter-phase surface tension with $N$ may indicate that for $N=\infty$ the deconfinement transition cannot, in practise, occur. Conference Paper/Proceeding/Abstract Nuclear Physics B - Proceedings Supplements "129" 569 571 09205632 30 9 2003 2003-09-30 10.1016/S0920-5632(03)02644-6 http://inspirehep.net/record/627216 COLLEGE NANME Mathematics COLLEGE CODE SMA Swansea University 2016-05-14T16:42:18.2343315 2016-05-14T16:42:18.0471303 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics M. Teper 1 U. Wenger 2 Biagio Lucini 0000-0001-8974-8266 3
title SU(N) gauge theories near Tc
spellingShingle SU(N) gauge theories near Tc
Biagio Lucini
title_short SU(N) gauge theories near Tc
title_full SU(N) gauge theories near Tc
title_fullStr SU(N) gauge theories near Tc
title_full_unstemmed SU(N) gauge theories near Tc
title_sort SU(N) gauge theories near Tc
author_id_str_mv 7e6fcfe060e07a351090e2a8aba363cf
author_id_fullname_str_mv 7e6fcfe060e07a351090e2a8aba363cf_***_Biagio Lucini
author Biagio Lucini
author2 M. Teper
U. Wenger
Biagio Lucini
format Conference Paper/Proceeding/Abstract
container_title Nuclear Physics B - Proceedings Supplements
container_volume "129"
container_start_page 569
publishDate 2003
institution Swansea University
issn 09205632
doi_str_mv 10.1016/S0920-5632(03)02644-6
college_str Faculty of Science and Engineering
hierarchytype
hierarchy_top_id facultyofscienceandengineering
hierarchy_top_title Faculty of Science and Engineering
hierarchy_parent_id facultyofscienceandengineering
hierarchy_parent_title Faculty of Science and Engineering
department_str School of Biosciences, Geography and Physics - Physics{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Biosciences, Geography and Physics - Physics
url http://inspirehep.net/record/627216
document_store_str 0
active_str 0
description We study the deconfinement phase transition in SU(N) gauge theories for $N$=2,3,4,6,8. The transition is first order for $N \ge 3$, with the strength increasing as $N$ increases. We extrapolate $T_c/\sqrt{\sigma}$ to the continuum limit for each $N$, and observe a rapid approach to the large $N$ limit. As $N$ increases the phase transition becomes clear-cut on smaller spatial volumes, indicating the absence of (non-singular) finite volume corrections at $N=\infty$ -- reminiscent of large $N$ reduction. The observed rapid increase of the inter-phase surface tension with $N$ may indicate that for $N=\infty$ the deconfinement transition cannot, in practise, occur.
published_date 2003-09-30T03:33:57Z
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score 11.036706

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