Please use this identifier to cite or link to this item: http://localhost:80/handle/1956/854
Full metadata record
DC FieldValueLanguage
dc.creatorHove, Joakim-
dc.date2005-12-12T14:57:51Z-
dc.date2005-12-12T14:57:51Z-
dc.date2005-11-30-
dc.date.accessioned2019-07-20T06:44:05Z-
dc.date.available2019-07-20T06:44:05Z-
dc.identifierJournal of physics. A, Mathematical, nuclear and general 2005 38: 10893-10904-
dc.identifier0301-0015-
dc.identifierhttp://hdl.handle.net/1956/854-
dc.identifier10.1088/0305-4470/38/50/002-
dc.identifier.urihttp://localhost:80/handle/1956/854-
dc.descriptionDue 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.-
dc.descriptionPeer reviewed-
dc.format360266 bytes-
dc.formatapplication/pdf-
dc.languageeng-
dc.publisherInstitute of Physics Publishing-
dc.titleThe number of link and cluster states: the core of the 2D q state Potts model-
dc.typeJournal Article-
Appears in Collections:Department of Earth Science

Files in This Item:
Click on the URI links for accessing contents.
Full metadata record
DC FieldValueLanguage
dc.creatorHove, Joakim-
dc.date2005-12-12T14:57:51Z-
dc.date2005-12-12T14:57:51Z-
dc.date2005-11-30-
dc.date.accessioned2019-07-20T06:44:05Z-
dc.date.available2019-07-20T06:44:05Z-
dc.identifierJournal of physics. A, Mathematical, nuclear and general 2005 38: 10893-10904-
dc.identifier0301-0015-
dc.identifierhttp://hdl.handle.net/1956/854-
dc.identifier10.1088/0305-4470/38/50/002-
dc.identifier.urihttp://localhost:80/handle/1956/854-
dc.descriptionDue 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.-
dc.descriptionPeer reviewed-
dc.format360266 bytes-
dc.formatapplication/pdf-
dc.languageeng-
dc.publisherInstitute of Physics Publishing-
dc.titleThe number of link and cluster states: the core of the 2D q state Potts model-
dc.typeJournal Article-
Appears in Collections:Department of Earth Science

Files in This Item:
Click on the URI links for accessing contents.
Full metadata record
DC FieldValueLanguage
dc.creatorHove, Joakim-
dc.date2005-12-12T14:57:51Z-
dc.date2005-12-12T14:57:51Z-
dc.date2005-11-30-
dc.date.accessioned2019-07-20T06:44:05Z-
dc.date.available2019-07-20T06:44:05Z-
dc.identifierJournal of physics. A, Mathematical, nuclear and general 2005 38: 10893-10904-
dc.identifier0301-0015-
dc.identifierhttp://hdl.handle.net/1956/854-
dc.identifier10.1088/0305-4470/38/50/002-
dc.identifier.urihttp://localhost:80/handle/1956/854-
dc.descriptionDue 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.-
dc.descriptionPeer reviewed-
dc.format360266 bytes-
dc.formatapplication/pdf-
dc.languageeng-
dc.publisherInstitute of Physics Publishing-
dc.titleThe number of link and cluster states: the core of the 2D q state Potts model-
dc.typeJournal Article-
Appears in Collections:Department of Earth Science

Files in This Item:
Click on the URI links for accessing contents.