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    Metastability of (d+n)-dimensional elastic manifolds

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    We investigate the depinning of a massive elastic manifold with dd internal dimensions, embedded in a (d+n)(d+n)-dimensional space, and subject to an isotropic pinning potential V(u)=V(u).V({\bf u})=V(|{\bf u}|). The tunneling process is driven by a small external force F.{\bf F}. We find the zero temperature and high temperature instantons and show that for the case 1d61\le d\le 6 the problem exhibits a sharp transition from quantum to classical behavior: At low temperatures T<TcT<T_{c} the Euclidean action is constant up to exponentially small corrections, while for T>Tc,T> T_{c}, SEucl(d,T)/=U(d)/T.{S_{\rm Eucl}(d,T)}/{\hbar} = {U(d)}/{T}. The results are universal and do not depend on the detailed shape of the trapping potential V(u)V({\bf u}). Possible applications of the problem to the depinning of vortices in high-TcT_{c} superconductors and nucleation in dd-dimensional phase transitions are discussed. In addition, we determine the high-temperature asymptotics of the preexponential factor for the (1+1)(1+1)-dimensional problem.Comment: RevTeX, 10 pages, 3 figures inserte
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