Perimeter Length and Form Factor of Two-Dimensional Polymer Melts
| dc.creator | Meyer, H. | |
| dc.creator | Kreer, T. | |
| dc.creator | Aichele, M. | |
| dc.creator | Cavallo, A. | |
| dc.creator | Johner, A. | |
| dc.creator | Baschnagel, J. | |
| dc.creator | Wittmer, J. P. | |
| dc.date | 2009-05-07 | |
| dc.date.accessioned | 2026-07-07T13:12:38Z | |
| dc.date.available | 2026-07-07T13:12:38Z | |
| dc.description | Self-avoiding polymers in two-dimensional ($d=2$) melts are known to adopt compact configurations of typical size $R(N) \sim N^{1/d}$ with $N$ being the chain length. Using molecular dynamics simulations we show that the irregular shapes of these chains are characterized by a perimeter length $L(N) \sim R(N)^{\dpm}$ of fractal dimension $\dpm = d-Θ_2 =5/4$ with $Θ_2=3/4$ being a well-known contact exponent. Due to the self-similar structure of the chains, compactness and perimeter fractality repeat for subchains of all arc-lengths $s$ down to a few monomers. The Kratky representation of the intramolecular form factor $F(q)$ reveals a strong non-monotonous behavior with $q^2F(q) \sim 1/(qN^{1/d})^{Θ_2}$ in the intermediate regime of the wavevector $q$. Measuring the scattering of labeled subchains %($s F(q) \sim L(s)$) the form factor may allow to test our predictions in real experiments. | |
| dc.description | 4 pages, 4 figures, accepted for PRE Rapid Communications | |
| dc.identifier | https://arxiv.org/abs/0905.1002 | |
| dc.identifier | http://arxiv.org/abs/0905.1002 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/229637 | |
| dc.subject | Soft Condensed Matter | |
| dc.title | Perimeter Length and Form Factor of Two-Dimensional Polymer Melts | |
| dc.type | text |