2007
DOI: 10.1142/9781860948299
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Random Polymer Models

Abstract: RANDOM POLYMER MODELS

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Cited by 128 publications
(291 citation statements)
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“…The existence of this limit, both P(dω)-a.s. and in L 1 (P), and the fact that f (β, p) is nonrandom are proved in [8] via super-additivity arguments. Notice that trivially Z β, p N ,ω ≥ 1 and hence f (β, p) ≥ 0 for all β, p. Zero is in fact the contribution to the free energy of the paths that never touch the wall: indeed, by restricting to the set of random walk trajectories that stay strictly positive until time N , one has By a standard coupling on the environment, it is clear that the function p → f (β, p) is nondecreasing.…”
Section: The Model and The Free Energymentioning
confidence: 96%
“…The existence of this limit, both P(dω)-a.s. and in L 1 (P), and the fact that f (β, p) is nonrandom are proved in [8] via super-additivity arguments. Notice that trivially Z β, p N ,ω ≥ 1 and hence f (β, p) ≥ 0 for all β, p. Zero is in fact the contribution to the free energy of the paths that never touch the wall: indeed, by restricting to the set of random walk trajectories that stay strictly positive until time N , one has By a standard coupling on the environment, it is clear that the function p → f (β, p) is nondecreasing.…”
Section: The Model and The Free Energymentioning
confidence: 96%
“…We sometimes denote the partition functions as Z When d = 1 and m = 0, the Markov chain (φ i ∈ R (or ∈ R + )) i∈D N may be interpreted as the heights of interfaces located in a plane measured from the position i on a reference line (x-axis), so that the system is called (1 + 1)-dimensional interface model with δ-pinning at 0, see [3,5,8,15]. See [14] for a relation to the polymer models.…”
Section: Weakly Pinned Gaussian Random Walksmentioning
confidence: 99%
“…The Markov chain, being transient at ε = 0, turns to be recurrent when the strength ε of the attractive force toward 0 increases and exceeds the critical value ε c or ε + c ; see [14] for random walks with discrete values. The asymptotic behavior of the free energies ξ ε and ξ ε,+ for ε close to their critical values is studied in Appendix A.…”
Section: Scaling Limits and Large Deviation Rate Functionalsmentioning
confidence: 99%
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“…The discrete analogue of Eq. (1.2) with positive summable kernel of infinite moment corresponds to the renewal sequence of a null-recurrent Markov chain [20], and under similar additional assumptions on the kernel, the hyperbolic decay of the sequence relies upon well-known results by Garsia and Lamperti [18] and Isaac [23]. Our second class of results in this paper employ the convergence rate of the resolvent r to investigate the long memory properties of the solution of the Itô-Volterra differential equation (1.1) and its discrete analogue.…”
Section: Introductionmentioning
confidence: 99%