Please use this identifier to cite or link to this item: https://ah.lib.nccu.edu.tw/handle/140.119/71425
DC FieldValueLanguage
dc.contributor應數系en_US
dc.creator張書銓zh_TW
dc.creatorChang, Shu-Chiuanen_US
dc.creator陳隆奇zh_TW
dc.creatorChen, Lung-Chien_US
dc.creator李欣芸zh_TW
dc.creatorLee, Hsin-Yunen_US
dc.date2013.10en_US
dc.date.accessioned2014-11-13T09:26:16Z-
dc.date.available2014-11-13T09:26:16Z-
dc.date.issued2014-11-13T09:26:16Z-
dc.identifier.urihttp://nccur.lib.nccu.edu.tw/handle/140.119/71425-
dc.description.abstractWe present the numbers of ice model configurations (with Boltzmann factors equal to one) I(n)I(n) on the two-dimensional Sierpinski gasket SG(n)SG(n) at stage nn. The upper and lower bounds for the entropy per site, defined as limv→∞lnI(n)/vlimv→∞lnI(n)/v, where vv is the number of vertices on SG(n)SG(n), are derived in terms of the results at a certain stage. As the difference between these bounds converges quickly to zero as the calculated stage increases, the numerical value of the entropy can be evaluated with more than a hundred significant figures accuracy. The corresponding result of the ice model on the generalized two-dimensional Sierpinski gasket SGb(n)SGb(n) with b=3b=3 is also obtained, and the general upper and lower bounds for the entropy per site for arbitrary bb are conjectured. We also consider the number of eight-vertex model configurations on SG(n)SG(n) and the number of generalized vertex models Eb(n)Eb(n) on SGb(n)SGb(n), and obtain exactly Eb(n)=2{2(b+1)[b(b+1)/2]n+b+4}/(b+2)Eb(n)=2{2(b+1)[b(b+1)/2]n+b+4}/(b+2). It follows that the entropy per site is View the MathML sourcelimv→∞lnEb(n)/v=2(b+1)b+4ln2.en_US
dc.format.extent577308 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoen_US-
dc.relationPhysica A, 392(8), 1776-1787en_US
dc.subjectIce model;Eight-vertex model;Sierpinski gasket;Recursion relations;Entropyen_US
dc.titleIce model and eight-vertex model on the two-dimensional Sierpinski gasketen_US
dc.typearticleen
dc.identifier.doi10.1016/j.physa.2013.01.005-
dc.doi.urihttp://dx.doi.org/10.1016/j.physa.2013.01.005-
item.cerifentitytypePublications-
item.fulltextWith Fulltext-
item.grantfulltextrestricted-
item.languageiso639-1en_US-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.openairetypearticle-
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