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Mean area of self-avoiding loops.
| Content Provider | Semantic Scholar |
|---|---|
| Author | Cardy |
| Copyright Year | 1994 |
| Abstract | The mean area of two-dimensional unpressurised vesicles, or self-avoiding loops of fixed length $N$, behaves for large $N$ as $A_0 N^{3/2}$, while their mean square radius of gyration behaves as $R^2_0 N^{3/2}$. The amplitude ratio $A_0/R_0^2$ is computed exactly and found to equal $4\pi/5$. The physics of the pressurised case, both in the inflated and collapsed phases, may be usefully related to that of a complex O(n) field theory coupled to a U(1) gauge field, in the limit $n \to 0$. |
| Starting Page | 1580 |
| Ending Page | 1583 |
| Page Count | 4 |
| File Format | PDF HTM / HTML |
| DOI | 10.1103/PhysRevLett.72.1580 |
| PubMed reference number | 10055648 |
| Journal | Medline |
| Volume Number | 72 |
| Issue Number | 11 |
| Alternate Webpage(s) | http://arxiv.org/pdf/cond-mat/9310013v2.pdf |
| Alternate Webpage(s) | https://arxiv.org/pdf/cond-mat/9310013v2.pdf |
| Alternate Webpage(s) | https://doi.org/10.1103/PhysRevLett.72.1580 |
| Journal | Physical review letters |
| Language | English |
| Access Restriction | Open |
| Content Type | Text |
| Resource Type | Article |
