Abstract

We study polymers attached to spherical (circular) or paraboloidal (parabolic) probes in three (two) dimensions. Both self-avoiding and random walks are examined numerically. The behavior of a polymer of size R0R_0 attached to the tip of a probe with radius of curvature RR, differs qualitatively for large and small values of the ratio s=R0/Rs=R_0/R. We demonstrate that the scaled compliance (inverse force constant) S/R02S/R_0^2, and scaled mean position of the polymer end-point <x⊥>/R<x_\perp>/R can be expressed as a function of ss. Scaled compliance is anisotropic, and quite large in the direction parallel to the surface when R0∼RR_0\sim R. The exponent γγ, characterizing the number of polymer configurations, crosses over from a value of γ1γ_1 - characteristic of a planar boundary - at small ss to one reflecting the overall shape of the probe at large ss. For a spherical probe the crossover is to an unencumbered polymer, while for a parabolic probe we cannot rule out a new exponent.

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