paper

Polymer Translocation out of Planar Confinements

arXiv:0710.0147 · doi:10.1088/0953-8984/20/7/075101

Abstract

Polymer translocation in three dimensions out of planar confinements is studied in this paper. Three membranes are located at , and . These membranes are impenetrable, except for the middle one at , which has a narrow pore. A polymer with length is initially sandwiched between the membranes placed at and and translocates through this pore. We consider strong confinement (small ), where the polymer is essentially reduced to a two-dimensional polymer, with a radius of gyration scaling as $R^{\tinytext{(2D)}}_g \sim N^{ν_{\tinytext{2D}}}$; here, $ν_{\tinytext{2D}}=0.75$ is the Flory exponent in two dimensions. The polymer performs Rouse dynamics. Based on theoretical analysis and high-precision simulation data, we show that in the unbiased case , the dwell-time scales as $N^{2+ν_{\tinytext{2D}}}$, in perfect agreement with our previously published theoretical framework. For , the situation is equivalent to field-driven translocation in two dimensions. We show that in this case scales as $N^{2ν_{\tinytext{2D}}}$, in agreement with several existing numerical results in the literature. This result violates the earlier reported lower bound for for field-driven translocation. We argue, based on energy conservation, that the actual lower bound for is and not . Polymer translocation in such theoretically motivated geometries thus resolves some of the most fundamental issues that are the subjects of much heated debate in recent times.

Minor changes; 18+ pages, 8 figures, 5 tables, to appear in J. Phys: Cond. Mat

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Polymer Translocation out of Planar Confinements · wovepaper