2009
DOI: 10.1007/s00220-009-0737-0
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Fractional Moment Bounds and Disorder Relevance for Pinning Models

Abstract: We study the critical point of directed pinning/wetting models with quenched disorder. The distribution K(·) of the location of the first contact of the (free) polymer with the defect line is assumed to be of the form K(n) = n −α−1 L(n), with α ≥ 0 and L(·) slowly varying. The model undergoes a (de)-localization phase transition: the free energy (per unit length) is zero in the delocalized phase and positive in the localized phase. For α < 1/2 disorder is irrelevant: quenched and annealed critical points coinc… Show more

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Cited by 79 publications
(189 citation statements)
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“…Theorem 2.2 collects several results proven in a series of papers [4,10,16,17,19,28,29,31] in several manners, the full necessary and sufficient condition for disorder relevance (together with the sharp critical point shift when α = 1/2) being given only recently in [12]. In [12,19,28,29], the authors estimate the fractional moment of the partition function up to the correlation length by a change of measure argument, and then use a coarse-graining procedure to glue these estimates together.…”
Section: Results In the Iid Casementioning
confidence: 99%
“…Theorem 2.2 collects several results proven in a series of papers [4,10,16,17,19,28,29,31] in several manners, the full necessary and sufficient condition for disorder relevance (together with the sharp critical point shift when α = 1/2) being given only recently in [12]. In [12,19,28,29], the authors estimate the fractional moment of the partition function up to the correlation length by a change of measure argument, and then use a coarse-graining procedure to glue these estimates together.…”
Section: Results In the Iid Casementioning
confidence: 99%
“…it has been shown in [7] that in (3.27) one can take ε = 0 and c 0 is still positive. Theorem 3.6 has been proven in [19] and we give an outline of the proof in Section 5. The method is based on estimating fractional moments of the free energy, while (3.29) is derived by adapting the techniques yielding Theorem 3.5 (and a sketch of the proof is in Section 4).…”
Section: 4mentioning
confidence: 99%
“…A (rough) bound in the other direction is obtained by neglecting P h (n ∈ τ )K(N − n) in the right-hand side of (2.17), so that 19) which holds once again for every N . The sharp asymptotic result is…”
Section: The Critical Behavior Of the Free Energy Is Given Bymentioning
confidence: 99%
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