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Volumn 70, Issue 3, 2004, Pages

Deconfining phase transition as a matrix model of renormalized Polyakov loops

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE; MATHEMATICAL ANALYSIS; MATHEMATICAL MODEL; NUCLEAR PHYSICS; PHASE TRANSITION; QUARK; THERMODYNAMICS;

EID: 37649031618     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.70.034511     Document Type: Article
Times cited : (196)

References (189)
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    • J. Zinn-Justin, Quantum Field Theory and Critical Phenomena (Clarendon Press, Oxford, 1997).
    • J. Zinn-Justin, Quantum Field Theory and Critical Phenomena (Clarendon Press, Oxford, 1997).
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    • T. Eguchi and H. Kawai, Phys. Rev. Lett. 48, 1063 (1982); with (Formula presented) our (6) is their (18).
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    • Eguchi, T.1    Kawai, H.2
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    • Yu. Makeenko, hep-th/0001047
    • Yu. Makeenko, hep-th/0001047
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    • P. Cvitanovic, http://www.nbi.dk/GroupTheory
    • P. Cvitanovic, http://www.nbi.dk/GroupTheory
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    • A. Dumitru, J. Lenaghan, R. D. Pisarski, and K. Splittorff (unpublished).
    • A. Dumitru, J. Lenaghan, R. D. Pisarski, and K. Splittorff (unpublished).
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    • There is no deconfining transition in two spacetime dimensions. Gauge theories have no dynamical degrees of freedom, and all Wilson lines can be computed from free field theory: G. Grignani, G.W. Semenoff, and P. Sodano, hep-th/9503109
    • Grignani, G.1    Semenoff, G.W.2    Sodano, P.3
  • 182
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    • Ann. Phys. (N.Y.)J.M. Aroca and Y. Kubyshin, 283, 11 (2000).
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    • Aroca, J.M.1    Kubyshin, Y.2
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    • Phys. Rev. DThe loop string tension, (Formula presented) corresponds to a surface tied down on four sides, setting the transverse fluctuations to vanish at (Formula presented) This follows from the potential at zero temperature, O. Alvarez, 24, 440 (1981); by replacing (Formula presented) These two string tensions agree at (Formula presented) but differ at (Formula presented) In a large d expansion, (Formula presented)where (Formula presented) and (Formula presented) is the string tension at zero temperature. Surfaces for the loop string tension fluctuate less, so while (Formula presented) vanishes at (Formula presented) (Formula presented) does not vanish until (Formula presented) and (Formula presented)
    • (1981) , vol.24 , pp. 440
    • Alvarez, O.1


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