Cluster percolation and thermal critical behavior

Satz H (2002)
In: COMPUTER PHYSICS COMMUNICATIONS. 147. ELSEVIER SCIENCE BV: 46-51.

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Abstract
Continuous phase transitions in spin systems can be formulated as percolation of suitably defined clusters. We review this equivalence and then discuss how in a similar way, the color deconfinement transition in SU(2) gauge theory can be treated as a percolation phenomenon. In the presence of an external field, spin systems cease to show thermal critical behavior, but the geometric percolation transition persists (Kertesz line). For H not equal 0, we study the relation between percolation and pseudocritical behavior, both for continuous and first order transitions, and show that it leads to the necessity of an H-dependent cluster definition. A viable formulation of this kind could serve as a definition of deconfinement in QCD with dynamical quarks. (C) 2002 Elsevier Science B.V. All rights reserved.
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Satz H. Cluster percolation and thermal critical behavior. In: COMPUTER PHYSICS COMMUNICATIONS. Vol 147. ELSEVIER SCIENCE BV; 2002: 46-51.
Satz, H. (2002). Cluster percolation and thermal critical behavior. COMPUTER PHYSICS COMMUNICATIONS, 147(1-2), 46-51.
Satz, H. (2002). “Cluster percolation and thermal critical behavior” in COMPUTER PHYSICS COMMUNICATIONS, vol. 147, (ELSEVIER SCIENCE BV), 46-51.
Satz, H., 2002. Cluster percolation and thermal critical behavior. In COMPUTER PHYSICS COMMUNICATIONS. no.147 ELSEVIER SCIENCE BV, pp. 46-51.
H. Satz, “Cluster percolation and thermal critical behavior”, COMPUTER PHYSICS COMMUNICATIONS, vol. 147, ELSEVIER SCIENCE BV, 2002, pp.46-51.
Satz, H.: Cluster percolation and thermal critical behavior. COMPUTER PHYSICS COMMUNICATIONS. 147, p. 46-51. ELSEVIER SCIENCE BV (2002).
Satz, Helmut. “Cluster percolation and thermal critical behavior”. COMPUTER PHYSICS COMMUNICATIONS. ELSEVIER SCIENCE BV, 2002.Vol. 147. 46-51.
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