2013
DOI: 10.1063/1.4775584
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Dynamics of semiflexible regular hyperbranched polymers

Abstract: We study the dynamics of semiflexible Vicsek fractals (SVF) following the framework established by Dolgushev and Blumen [J. Chem. Phys. 131, 044905 (2009)], a scheme which allows to model semiflexible treelike polymers of arbitrary architecture. We show, extending the methods used in the treatment of semiflexible dendrimers by Fürstenberg et al. [J. Chem. Phys. 136, 154904 (2012)], that in this way the Langevin-dynamics of SVF can be treated to a large part analytically. For this we show for arbitrary Vicsek f… Show more

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Cited by 33 publications
(61 citation statements)
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“…Such a procedure was first introduced for fully flexible dendrimers of functionality f = 3 [43] and later extended to arbitrary functionalities [47,48]; see also recent general results [49] for flexible dendritic structures. The works in [39,40] illustrate that an extension of the procedure is also applicable to semiflexible dendrimers and semiflexible Vicsek fractals. Here, we find (G + 1) groups of eigenvectors for a T-fractal of generation G. Among them, the first G groups are based on the branches Z (1) to Z (G) , whereas the (G + 1)-th group involves the motion of all beads, including the central one (in the case of semiflexible dendrimers [39], the groups 1 to G represent the dynamics of dendrons of the generations 1 to G, and the (G + 1)-th group involves the motion of all dendrimer's beads).…”
Section: Hierarchical Eigenmodes Of T-fractalsmentioning
confidence: 99%
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“…Such a procedure was first introduced for fully flexible dendrimers of functionality f = 3 [43] and later extended to arbitrary functionalities [47,48]; see also recent general results [49] for flexible dendritic structures. The works in [39,40] illustrate that an extension of the procedure is also applicable to semiflexible dendrimers and semiflexible Vicsek fractals. Here, we find (G + 1) groups of eigenvectors for a T-fractal of generation G. Among them, the first G groups are based on the branches Z (1) to Z (G) , whereas the (G + 1)-th group involves the motion of all beads, including the central one (in the case of semiflexible dendrimers [39], the groups 1 to G represent the dynamics of dendrons of the generations 1 to G, and the (G + 1)-th group involves the motion of all dendrimer's beads).…”
Section: Hierarchical Eigenmodes Of T-fractalsmentioning
confidence: 99%
“…In Equation (40), the F(n − 1) × F(n − 1) matrix A n−1 describes the two terminal Z (n−1) branches, whereas the internal Z (n−1) branch is described by the (F(n) − F(n − 1)) × (F(n) − F(n − 1)) matrix L n−1 . The blocks W 12 and W 21 reflect the interaction of the two external branches with the internal branch.…”
Section: Reduced Matricesmentioning
confidence: 99%
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