On the Critical Point of the Random Walk Pinning Model in Dimension d=3
We consider the Random Walk Pinning Model studied in [3] and [2]: this is a random walk X on Z d , whose law is modified by the exponential of β times L N (X , Y), the collision local time up to time N with the (quenched) trajectory Y of another d-dimensional random walk. If β exceeds a certain crit...
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Published in | Electronic journal of probability Vol. 15; no. none; pp. 654 - 683 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Institute of Mathematical Statistics (IMS)
01.01.2010
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Subjects | |
Online Access | Get full text |
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Summary: | We consider the Random Walk Pinning Model studied in [3] and [2]: this is a random walk X on Z d , whose law is modified by the exponential of β times L N (X , Y), the collision local time up to time N with the (quenched) trajectory Y of another d-dimensional random walk. If β exceeds a certain critical value β c , the two walks stick together for typical Y realizations (localized phase). A natural question is whether the disorder is relevant or not, that is whether the quenched and annealed systems have the same critical behavior. Birkner and Sun [3] proved that β c coincides with the critical point of the annealed Random Walk Pinning Model if the space dimension is d = 1 or d = 2, and that it differs from it in dimension d ≥ 4 (for d ≥ 5, the result was proven also in [2]). Here, we consider the open case of the marginal dimension d = 3, and we prove non-coincidence of the critical points. |
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ISSN: | 1083-6489 1083-6489 |
DOI: | 10.1214/EJP.v15-761 |