Adventures in Coulomb Gauge
Abstract
We study the phase structure of SU(2) gauge theories at zero and high temperature, with and without scalar matter fields, in terms of the symmetric/broken realization of the remnant gauge symmetry which exists after fixing to Coulomb gauge. The symmetric realization is associated with a linearly rising color Coulomb potential (which we compute numerically), and is a necessary but not sufficient condition for confinement.
- Authors:
- Publication Date:
- Research Org.:
- Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States)
- Sponsoring Org.:
- Physics Division
- OSTI Identifier:
- 965354
- Report Number(s):
- LBNL-53999
TRN: US0903835
- DOE Contract Number:
- DE-AC02-05CH11231
- Resource Type:
- Conference
- Resource Relation:
- Conference: International Conference on Color Confinement and Hadrons In Quantum Chromodynamics -- Confinement 2003 , Wako, Japan, 21-24 Jul 2003
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72; COLOR; CONFINEMENT; COULOMB FIELD; HADRONS; QUANTUM CHROMODYNAMICS; SCALARS; SYMMETRY
Citation Formats
Greensite, J, and Olejnik, S. Adventures in Coulomb Gauge. United States: N. p., 2003.
Web.
Greensite, J, & Olejnik, S. Adventures in Coulomb Gauge. United States.
Greensite, J, and Olejnik, S. 2003.
"Adventures in Coulomb Gauge". United States. https://www.osti.gov/servlets/purl/965354.
@article{osti_965354,
title = {Adventures in Coulomb Gauge},
author = {Greensite, J and Olejnik, S},
abstractNote = {We study the phase structure of SU(2) gauge theories at zero and high temperature, with and without scalar matter fields, in terms of the symmetric/broken realization of the remnant gauge symmetry which exists after fixing to Coulomb gauge. The symmetric realization is associated with a linearly rising color Coulomb potential (which we compute numerically), and is a necessary but not sufficient condition for confinement.},
doi = {},
url = {https://www.osti.gov/biblio/965354},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Fri Sep 26 00:00:00 EDT 2003},
month = {Fri Sep 26 00:00:00 EDT 2003}
}
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