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 |
|