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Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory

Z. Schram, A. Hart, M. Teper, Biagio Lucini Orcid Logo

Journal of High Energy Physics, Volume: "0011", Issue: 11, Pages: 043 - 043

Swansea University Author: Biagio Lucini Orcid Logo

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DOI (Published version): 10.1088/1126-6708/2000/11/043

Abstract

We calculate the Euclidean action of a pair of Z2 monopoles (instantons), as a function of their spatial separation, in D=2+1 SU(2) lattice gauge theory. We do so both above and below the deconfining transition at T=Tc. At high T, and at large separation, we find that the monopole `interaction'...

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Published in: Journal of High Energy Physics
ISSN: 1029-8479
Published: 2000
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URI: https://cronfa.swan.ac.uk/Record/cronfa27964
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spelling 2016-05-14T16:42:30.2308084 v2 27964 2016-05-14 Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory 7e6fcfe060e07a351090e2a8aba363cf 0000-0001-8974-8266 Biagio Lucini Biagio Lucini true false 2016-05-14 SMA We calculate the Euclidean action of a pair of Z2 monopoles (instantons), as a function of their spatial separation, in D=2+1 SU(2) lattice gauge theory. We do so both above and below the deconfining transition at T=Tc. At high T, and at large separation, we find that the monopole `interaction' grows linearly with distance: the flux between the monopoles forms a flux tube (exactly like a finite portion of a Z2 domain wall) so that the monopoles are linearly confined. At short distances the interaction is well described by a Coulomb interaction with, at most, a very small screening mass, possibly equal to the Debye electric screening mass. At low T the interaction can be described by a simple screened Coulomb (i.e. Yukawa) interaction with a screening mass that can be interpreted as the mass of a `constituent gluon'. None of this is unexpected, but it helps to resolve some apparent controversies in the recent literature. Journal Article Journal of High Energy Physics "0011" 11 043 043 1029-8479 31 10 2000 2000-10-31 10.1088/1126-6708/2000/11/043 http://inspirehep.net/record/534739 COLLEGE NANME Mathematics COLLEGE CODE SMA Swansea University 2016-05-14T16:42:30.2308084 2016-05-14T16:42:29.7628054 Faculty of Science and Engineering School of Biosciences, Geography and Physics - Physics Z. Schram 1 A. Hart 2 M. Teper 3 Biagio Lucini 0000-0001-8974-8266 4
title Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
spellingShingle Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
Biagio Lucini
title_short Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
title_full Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
title_fullStr Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
title_full_unstemmed Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
title_sort Bbb Z2 monopoles in D = 2+1 SU(2) lattice gauge theory
author_id_str_mv 7e6fcfe060e07a351090e2a8aba363cf
author_id_fullname_str_mv 7e6fcfe060e07a351090e2a8aba363cf_***_Biagio Lucini
author Biagio Lucini
author2 Z. Schram
A. Hart
M. Teper
Biagio Lucini
format Journal article
container_title Journal of High Energy Physics
container_volume "0011"
container_issue 11
container_start_page 043
publishDate 2000
institution Swansea University
issn 1029-8479
doi_str_mv 10.1088/1126-6708/2000/11/043
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/534739
document_store_str 0
active_str 0
description We calculate the Euclidean action of a pair of Z2 monopoles (instantons), as a function of their spatial separation, in D=2+1 SU(2) lattice gauge theory. We do so both above and below the deconfining transition at T=Tc. At high T, and at large separation, we find that the monopole `interaction' grows linearly with distance: the flux between the monopoles forms a flux tube (exactly like a finite portion of a Z2 domain wall) so that the monopoles are linearly confined. At short distances the interaction is well described by a Coulomb interaction with, at most, a very small screening mass, possibly equal to the Debye electric screening mass. At low T the interaction can be described by a simple screened Coulomb (i.e. Yukawa) interaction with a screening mass that can be interpreted as the mass of a `constituent gluon'. None of this is unexpected, but it helps to resolve some apparent controversies in the recent literature.
published_date 2000-10-31T03:33:59Z
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score 11.013148

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