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Conference Paper/Proceeding/Abstract 807 views

Deconfining transition in two-flavor QCD

Massimo D'Elia, L. Del Debbio, C. Pica, A. Di Giacomo, G. Paffuti, J.M. Carmona, Biagio Lucini Orcid Logo

Nuclear Physics B - Proceedings Supplements, Volume: "129", Pages: 689 - 691

Swansea University Author: Biagio Lucini Orcid Logo

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Abstract

The order and the nature of the finite-temperature phase transition of QCD with two flavors of dynamical quarks is investigated. An analysis of the critical exponent of the specific heat is performed through finite-size and finite-mass scaling of various susceptibilities. Dual superconductivity of Q...

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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/cronfa27950
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first_indexed 2016-05-15T01:22:52Z
last_indexed 2018-02-09T05:11:33Z
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spelling 2016-05-14T16:42:19.8879421 v2 27950 2016-05-14 Deconfining transition in two-flavor QCD 7e6fcfe060e07a351090e2a8aba363cf 0000-0001-8974-8266 Biagio Lucini Biagio Lucini true false 2016-05-14 SMA The order and the nature of the finite-temperature phase transition of QCD with two flavors of dynamical quarks is investigated. An analysis of the critical exponent of the specific heat is performed through finite-size and finite-mass scaling of various susceptibilities. Dual superconductivity of QCD vacuum is investigated using a disorder parameter, namely the v.e.v. of a monopole creation operator. Hybrid R simulations were run at lattice spatial sizes of $12^3$, $16^3$, $20^3$ and $32^3$ and temporal size $N_t=4$, with quark masses in the range $am_q = 0.3 - 0.01$. Conference Paper/Proceeding/Abstract Nuclear Physics B - Proceedings Supplements "129" 689 691 09205632 30 9 2003 2003-09-30 10.1016/S0920-5632(03)02682-3 http://inspirehep.net/record/627843 COLLEGE NANME Mathematics COLLEGE CODE SMA Swansea University 2016-05-14T16:42:19.8879421 2016-05-14T16:42:19.6539406 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Massimo D'Elia 1 L. Del Debbio 2 C. Pica 3 A. Di Giacomo 4 G. Paffuti 5 J.M. Carmona 6 Biagio Lucini 0000-0001-8974-8266 7
title Deconfining transition in two-flavor QCD
spellingShingle Deconfining transition in two-flavor QCD
Biagio Lucini
title_short Deconfining transition in two-flavor QCD
title_full Deconfining transition in two-flavor QCD
title_fullStr Deconfining transition in two-flavor QCD
title_full_unstemmed Deconfining transition in two-flavor QCD
title_sort Deconfining transition in two-flavor QCD
author_id_str_mv 7e6fcfe060e07a351090e2a8aba363cf
author_id_fullname_str_mv 7e6fcfe060e07a351090e2a8aba363cf_***_Biagio Lucini
author Biagio Lucini
author2 Massimo D'Elia
L. Del Debbio
C. Pica
A. Di Giacomo
G. Paffuti
J.M. Carmona
Biagio Lucini
format Conference Paper/Proceeding/Abstract
container_title Nuclear Physics B - Proceedings Supplements
container_volume "129"
container_start_page 689
publishDate 2003
institution Swansea University
issn 09205632
doi_str_mv 10.1016/S0920-5632(03)02682-3
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/627843
document_store_str 0
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description The order and the nature of the finite-temperature phase transition of QCD with two flavors of dynamical quarks is investigated. An analysis of the critical exponent of the specific heat is performed through finite-size and finite-mass scaling of various susceptibilities. Dual superconductivity of QCD vacuum is investigated using a disorder parameter, namely the v.e.v. of a monopole creation operator. Hybrid R simulations were run at lattice spatial sizes of $12^3$, $16^3$, $20^3$ and $32^3$ and temporal size $N_t=4$, with quark masses in the range $am_q = 0.3 - 0.01$.
published_date 2003-09-30T03:33:57Z
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