| dc.contributor.author | Hove, Joakim | eng |
| dc.date.accessioned | 2005-12-12T14:57:51Z | |
| dc.date.available | 2005-12-12T14:57:51Z | |
| dc.date.issued | 2005-11-30 | eng |
| dc.Published | Journal of physics. A, Mathematical, nuclear and general 2005 38: 10893-10904 | en |
| dc.identifier.issn | 0301-0015 | en_US |
| dc.identifier.uri | https://hdl.handle.net/1956/854 | |
| dc.description.abstract | Due to Fortuin and Kastelyin the q state Potts model has a representation as a sum over random graphs, generalizing the Potts model to arbitrary q is based on this representation. A key element of the random cluster representation is the combinatorial factor ΓG(C, E), which is the number of ways to form C distinct clusters, consisting of totally E edges. We have devised a method to calculate ΓG(C, E) from Monte Carlo simulations. | en_US |
| dc.format.extent | 360266 bytes | eng |
| dc.format.mimetype | application/pdf | eng |
| dc.language.iso | eng | eng |
| dc.publisher | Institute of Physics Publishing | en_US |
| dc.title | The number of link and cluster states: the core of the 2D q state Potts model | en_US |
| dc.type | Peer reviewed | |
| dc.type | Journal article | |
| dc.identifier.doi | https://doi.org/10.1088/0305-4470/38/50/002 | |
