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arXiv 1010.2837cond-mat.stat-mech
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刚性链极限下半柔性均聚物链持久长度的发散性

Divergence Of Persistent Length Of A Semiflexible Homopolymer Chain In The Stiff Chain Limit

Pramod Kumar Mishra

摘要:

在这份简短的报告中,我们重新审视了分析计算[Mishra,{ \it et al.},Physica A { \bf 323}(2003)453和Mishra,NewYork Sci. J. { \bf{3(1)} }(2010)32.]半柔性均聚物链的持久长度的%表示极刚性链极限,{ \bf $k\to0$(其中,$k$是链的刚度)}表示定向行走晶格模型的极刚性链极限,$k\to0$(其中,$k$是链的刚度)表示二维和三维定向行走晶格模型。我们对二维(正方形和长方形)和三维(立方形)格点的研究清楚地表明,持久长度按照表达式$(1-g_c)^{-1}$发散,其中$g_c$是无限长线性半柔性均聚物链聚合所需的步逸度的临界值,发散的性质与空间维数无关.这显然是正确的,因为在极端刚性链极限的情况下,聚合物链是一维物体,其形状像刚性杆。

英文摘要:

In this brief report, we revisit analytical calculation [Mishra, {\it et al.}, Physica A {\bf 323} (2003) 453 and Mishra, NewYork Sci. J. {\bf{3(1)}} (2010) 32.] of the persistent length of a semiflexible homopolymer chain in %the extremely stiff chain limit, {\bf $k\to0$ (where, $k$ is stiffness of the chain)} for directed walk lattice model the extremely stiff chain limit, $k\to0$ (where, $k$ is stiffness of the chain) for directed walk lattice model in two and three dimensions. Our study for two dimensional (square and rectangular) and three dimensional (cubic) lattice case clearly indicates that the persistent length diverges according to expression $(1-g_c)^{-1}$, where $g_c$ is the critical value of step fugacity required for polymerization of an infinitely long linear semiflexible homopolymer chain and nature of the divergence is independent of the space dimension. This is obviously true because in the case of extremely stiff chain limit the polymer chain is a one dimensional object and its shape is like a rigid rod.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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