Polymer dynamics in the depinned phase: metastability with logarithmic barriers

We consider the stochastic evolution of a (1 + 1)-dimensional polymer in the depinned regime. At equilibrium the system exhibits a double well structure: the polymer lies (essentially) either above or below the repulsive line. As a consequence, one expects a metastable behavior with rare jumps betwe...

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Bibliographic Details
Published in:Probability theory and related fields Vol. 153; no. 3-4; pp. 587 - 641
Main Authors: Caputo, Pietro, Lacoin, Hubert, Martinelli, Fabio, Simenhaus, François, Toninelli, Fabio Lucio
Format: Journal Article
Language:English
Published: Berlin/Heidelberg Springer-Verlag 01-08-2012
Springer Nature B.V
Springer Verlag
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Summary:We consider the stochastic evolution of a (1 + 1)-dimensional polymer in the depinned regime. At equilibrium the system exhibits a double well structure: the polymer lies (essentially) either above or below the repulsive line. As a consequence, one expects a metastable behavior with rare jumps between the two phases combined with a fast thermalization inside each phase. However, the energy barrier between these two phases is only logarithmic in the system size L and therefore the two relevant time scales are only polynomial in L with no clear-cut separation between them. The whole evolution is governed by a subtle competition between the diffusive behavior inside one phase and the jumps across the energy barriers. Our main results are: (i) a proof that the mixing time of the system lies between and ; (ii) the identification of two regions associated with the positive and negative phase of the polymer together with the proof of the asymptotic exponentiality of the tunneling time between them with rate equal to a half of the spectral gap.
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ISSN:0178-8051
1432-2064
DOI:10.1007/s00440-011-0355-6