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dc.contributor.author | Nigmatullin R. | |
dc.contributor.author | Khamzin A. | |
dc.contributor.author | Ghassib H. | |
dc.date.accessioned | 2018-09-17T21:49:02Z | |
dc.date.available | 2018-09-17T21:49:02Z | |
dc.date.issued | 2000 | |
dc.identifier.issn | 0038-1098 | |
dc.identifier.uri | https://dspace.kpfu.ru/xmlui/handle/net/135470 | |
dc.description.abstract | The classical two-dimensional Ising model is studied in the framework of the so-called static fluctuation approximation. This approximation hinges on the replacement of the square of the local-field operator with its mean value. The physical implication is that the true quantum-mechanical spectrum of this operator is replaced with a distribution; the moments of this distribution as well as the expectation value of the operator are then calculated self-consistently. With this single controllable approximation, the full thermodynamics and the pair correlation function of the classical two-dimensional Ising model are determined for the regular infinite lattice. The possible application to ultrathin ferroelectric films is discussed. © 1999 Elsevier Science Ltd. All rights reserved. | |
dc.relation.ispartofseries | Solid State Communications | |
dc.subject | A. Ferroelectrics | |
dc.subject | A. Thin films | |
dc.subject | D. Heat capacity | |
dc.subject | D. Order-disorder effects | |
dc.subject | D. Phase transitions | |
dc.title | The classical two-dimensional Ising model in the static fluctuation approximation | |
dc.type | Article | |
dc.relation.ispartofseries-issue | 5 | |
dc.relation.ispartofseries-volume | 113 | |
dc.collection | Публикации сотрудников КФУ | |
dc.relation.startpage | 257 | |
dc.source.id | SCOPUS00381098-2000-113-5-SID0033352865 |