2001
DOI: 10.1016/s0375-9474(00)00554-6
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Percolation and deconfinement in SU(2) gauge theory

Abstract: The deconfinement transition in SU(2) gauge theory and the magnetization transition in the Ising model belong to the same universality class. The critical behaviour of the Ising model can be characterized either as spontaneous breaking of the Z 2 symmetry of spin states or as percolation of appropriately defined spin clusters. We show that deconfinement in SU(2) gauge theory can be specified as percolation of Polyakov loop clusters with Fortuin-Kasteleyn bond weights, leading to the same critical exponents as … Show more

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Cited by 22 publications
(17 citation statements)
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“…Then, we proceeded by showing as the magnetic phase transition that occurs in the twodimensional Ising model can be understood as a percolation phenomenon. In the last section, we presented the connection between SU (2) gauge theory and effective spin system, as argued by Satz and Fortunato [6,8].…”
Section: Conclusion and Future Perspectivesmentioning
confidence: 91%
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“…Then, we proceeded by showing as the magnetic phase transition that occurs in the twodimensional Ising model can be understood as a percolation phenomenon. In the last section, we presented the connection between SU (2) gauge theory and effective spin system, as argued by Satz and Fortunato [6,8].…”
Section: Conclusion and Future Perspectivesmentioning
confidence: 91%
“…Our motivation in this theory is driven basically by its possible relevance to the problem of color deconfinement in Quantum Chromodynamics (QCD). The connection between the two phenomena can be argued as follows [6,8].…”
Section: Percolation Theory and Deconfinement In Qcdmentioning
confidence: 99%
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“…At high temperatures, the Z(3) symmetric Polyakov loop potential has three degenerate minima, leading to a domain structure in the deconfined phase, where center symmetry spontaneously breaks into different gauge configurations in different spatial regions. Lattice QCD studies have confirmed the existence of these center domains for the SU(2) gauge group [4][5][6] and later for SU(3) [7][8][9][10]. The formation of such structures necessarily comes with domain walls, interpolating between the different values of Z(3) in neighboring domains [11,12].…”
Section: Introductionmentioning
confidence: 92%
“…The volume V = (aN s ) 3 depends on the spatial extent of the lattice aN s . Most studies of center domains change the temperature by varying the lattice spacing [9][10][11]17]. This is a problem because the volume of the lattice is changed as the temperature changes.…”
Section: Anisotropic Gauge Actionmentioning
confidence: 99%