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Volumn 65, Issue 6, 2002, Pages

Tightness of slip-linked polymer chains

Author keywords

[No Author keywords available]

Indexed keywords

FEYNMANN GRAPHS; POLYMER CHAINS; SLIDING RINGS; TOPOLOGICAL CONSTRAINTS;

EID: 41349097244     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.65.061103     Document Type: Article
Times cited : (38)

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    • Here and in the following we consider two configurations of a polymer chain different if they cannot be matched by translation. In addition, the origin of a given structure is fixed by a vertex point, i.e., a point where several legs of the polymer chain are joint. For a simply connected ring polymer, such a vertex is a two-vertex anywhere along the chain
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    • Note that the above factorization does not take place in structures where additional links are introduced, such as connecting the two corner loops in the necklace configuration sketched in Fig. 22(h); this creates conditional probabilities, and the associated arc diagrams no longer correspond to Hartree graphs
    • Note that the above factorization does not take place in structures where additional links are introduced, such as connecting the two corner loops in the necklace configuration sketched in Fig. 22(h); this creates conditional probabilities, and the associated arc diagrams no longer correspond to Hartree graphs.
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    • If the segments (Formula presented) are loose, the cutoff a is no longer relevant and characteristic lengths can be calculated by multiple integrals of the form (Formula presented)whose Laplace transform (Formula presented) (Formula presented)yields a simple product form by the integration theorem for the first integral and the convolution theorem for the remaining factors, and therefore (Formula presented)With similar expressions for the normalization, one obtains the results quoted in the text
    • If the segments (Formula presented) are loose, the cutoff a is no longer relevant and characteristic lengths can be calculated by multiple integrals of the form (Formula presented)whose Laplace transform (Formula presented) (Formula presented)yields a simple product form by the integration theorem for the first integral and the convolution theorem for the remaining factors, and therefore (Formula presented)With similar expressions for the normalization, one obtains the results quoted in the text.


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