The generating function for spanning forests on a lattice is related to the q-state Potts model in a certain q to 0 limit, and extends the analogous notion for spanning trees, or dense self-avoiding branched polymers. Recent works have found a combinatorial perturbative equivalence also with the (quadratic action) O(n) model in the limit n to -1, the expansion parameter t counting the number of components of the forest. We give a random-matrix formulation of this model on the ensemble of degree-k random planar lattices. For k=3, a correspondence is found with the Kostov solution of the loop-gas problem, which arise as a reformulation of the (logarithmic action) O(n) model, at n=-2. Then, we show how to perform an expansion around the t=0 theory. In the thermodynamic limit, at any order in $t$ we have a finite sum of finite-dimensional Cauchy integrals. The leading contribution comes from a peculiar class of terms, for which a resummation can be performed exactly.

Spanning forests on random planar lattices / S. Caracciolo, A. Sportiello. - In: JOURNAL OF STATISTICAL PHYSICS. - ISSN 0022-4715. - 135:5-6(2009), pp. 1063-1104.

Spanning forests on random planar lattices

S. Caracciolo
Primo
;
A. Sportiello
Ultimo
2009

Abstract

The generating function for spanning forests on a lattice is related to the q-state Potts model in a certain q to 0 limit, and extends the analogous notion for spanning trees, or dense self-avoiding branched polymers. Recent works have found a combinatorial perturbative equivalence also with the (quadratic action) O(n) model in the limit n to -1, the expansion parameter t counting the number of components of the forest. We give a random-matrix formulation of this model on the ensemble of degree-k random planar lattices. For k=3, a correspondence is found with the Kostov solution of the loop-gas problem, which arise as a reformulation of the (logarithmic action) O(n) model, at n=-2. Then, we show how to perform an expansion around the t=0 theory. In the thermodynamic limit, at any order in $t$ we have a finite sum of finite-dimensional Cauchy integrals. The leading contribution comes from a peculiar class of terms, for which a resummation can be performed exactly.
O(n)-invariant σ-model; O(n)-vector model; Potts model; Random matrices; Self-avoiding polymers; Spanning forests; Spanning trees
Settore FIS/02 - Fisica Teorica, Modelli e Metodi Matematici
2009
http://www.springerlink.com/content/u6n1m7471x83p702/
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2434/66804
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