| dc.contributor.author | Aktaş H. | |
| dc.date.accessioned | 2020-06-25T15:13:14Z | |
| dc.date.available | 2020-06-25T15:13:14Z | |
| dc.date.issued | 2001 | |
| dc.identifier.citation | Aktaş, H. (2001). Double transition effect in Anderson transition. Turkish Journal of Physics, 25(5), 431 - 438. | en_US |
| dc.identifier.issn | 13000101 | |
| dc.identifier.uri | https://hdl.handle.net/20.500.12587/1676 | |
| dc.description.abstract | In this work we have studied the electronic mobility ? within a completely disordered lattice system by using the strong interatomic hopping potential V(r) = (-r/a0)exp(-r/a0) for site representation of the Hamiltonian. It is shown that a metallic system of a completely disordered lattice first goes insulating and then goes back to metallic again at higher atomic density ?. | en_US |
| dc.language.iso | eng | en_US |
| dc.rights | info:eu-repo/semantics/openAccess | en_US |
| dc.subject | Anderson transition | en_US |
| dc.subject | Double transition effect | en_US |
| dc.title | Double transition effect in Anderson transition | en_US |
| dc.type | article | en_US |
| dc.contributor.department | Kırıkkale Üniversitesi | en_US |
| dc.identifier.volume | 25 | en_US |
| dc.identifier.issue | 5 | en_US |
| dc.identifier.startpage | 431 | en_US |
| dc.identifier.endpage | 438 | en_US |
| dc.relation.journal | Turkish Journal of Physics | en_US |
| dc.relation.publicationcategory | Makale - Ulusal Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
