Driven translocation of a polymer: fluctuations at work
arXiv:1211.5533 · doi:10.1103/PhysRevE.87.032147
Abstract
The impact of thermal fluctuations on the translocation dynamics of a polymer chain driven through a narrow pore has been investigated theoretically and by means of extensive Molecular-Dynamics (MD) simulation. The theoretical consideration is based on the so-called velocity Langevin (V-Langevin) equation which determines the progress of the translocation in terms of the number of polymer segments, , that have passed through the pore at time due to a driving force . The formalism is based only on the assumption that, due to thermal fluctuations, the translocation velocity is a Gaussian random process as suggested by our MD data. With this in mind we have derived the corresponding Fokker-Planck equation (FPE) which has a nonlinear drift term and diffusion term with a {\em time-dependent} diffusion coefficient . Our MD simulation reveals that the driven translocation process follows a {\em super}diffusive law with a running diffusion coefficient where . This finding is then used in the numerical solution of the FPE which yields an important result: for comparatively small driving forces fluctuations facilitate the translocation dynamics. As a consequence, the exponent which describes the scaling of the mean translocation time with the length of the polymer, is found to diminish. Thus, taking thermal fluctuations into account, one can explain the systematic discrepancy between theoretically predicted duration of a driven translocation process, considered usually as a deterministic event, and measurements in computer simulations. In the non-driven case, , the translocation is slightly subdiffusive and can be treated within the framework of fractional Brownian motion (fBm).
13 pages, 8 figures
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