Finite- N effects for ideal polymer chains near a flat impenetrable wall

This paper addresses the statistical mechanics of ideal polymer chains next to a hard wall. The principal quantity of interest, from which all monomer densities can be calculated, is the partition function, G N ( z ) , for a chain of N discrete monomers with one end fixed a distance z from the wall....

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Bibliographic Details
Published in:The European physical journal. E, Soft matter and biological physics Vol. 29; no. 1; pp. 107 - 115
Main Authors: Matsen, M. W., Kim, J. U., Likhtman, A. E.
Format: Journal Article
Language:English
Published: Berlin/Heidelberg Springer-Verlag 01-05-2009
EDP Sciences
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Summary:This paper addresses the statistical mechanics of ideal polymer chains next to a hard wall. The principal quantity of interest, from which all monomer densities can be calculated, is the partition function, G N ( z ) , for a chain of N discrete monomers with one end fixed a distance z from the wall. It is well accepted that in the limit of infinite N , G N ( z ) satisfies the diffusion equation with the Dirichlet boundary condition, G N (0) = 0 , unless the wall possesses a sufficient attraction, in which case the Robin boundary condition, G N (0) = - G N ′ (0) , applies with a positive coefficient, . Here we investigate the leading N -1/2 correction, G N ( z ) . Prior to the adsorption threshold, G N ( z ) is found to involve two distinct parts: a Gaussian correction (for z aN 1/2 with a model-dependent amplitude, A , and a proximal-layer correction (for z a described by a model-dependent function, B ( z ) .
ISSN:1292-8941
1292-895X
DOI:10.1140/epje/i2009-10454-2