dc.contributor.advisor |
Ahmed, Anees |
en_US |
dc.contributor.author |
AHMED, ANEES |
en_US |
dc.date.accessioned |
2013-05-03T07:15:05Z |
|
dc.date.available |
2013-05-03T07:15:05Z |
|
dc.date.issued |
2013-05 |
en_US |
dc.identifier.uri |
http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/237 |
|
dc.description.abstract |
The Falicov-Kimball model is the simplest model of correlated electrons which shows long range order. The Falicov-Kimball model is exactly solvable in the limit of in finite dimensions through the use of Dynamical Mean Field Theory (DMFT). This thesis reviews the Hubbard model and Falicov-Kimball Model
in some detail, and details the DMFT formalism. The DMFT formalism is used to investigate continuous second order phase transitions in Falicov-Kimball model. It is seen that the model shows phase transitions for every non-zero value of the interaction strength. |
en_US |
dc.language.iso |
en |
en_US |
dc.subject |
2013 |
|
dc.subject |
falicov-kimball |
en_US |
dc.subject |
DMFT |
en_US |
dc.subject |
phase transitions |
en_US |
dc.subject |
dynamical mean field theory |
en_US |
dc.title |
Dynamical mean field approach to phase transitions in the Falicov-Kimball model |
en_US |
dc.type |
Thesis |
en_US |
dc.type.degree |
BS-MS |
en_US |
dc.contributor.department |
Dept. of Physics |
en_US |
dc.contributor.registration |
20081006 |
en_US |