Double transition effect in Anderson transition

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.department	Kırıkkale Üniversitesi
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.identifier.citation	Aktaş, H. (2001). Double transition effect in Anderson transition. Turkish Journal of Physics, 25(5), 431 - 438.	en_US
dc.identifier.endpage	438	en_US
dc.identifier.issn	13000101
dc.identifier.issue	5	en_US
dc.identifier.scopus	2-s2.0-0034884988
dc.identifier.scopusquality	Q2
dc.identifier.startpage	431	en_US
dc.identifier.trdizinid	33642
dc.identifier.uri	https://hdl.handle.net/20.500.12587/1676
dc.identifier.volume	25	en_US
dc.indekslendigikaynak	Scopus
dc.indekslendigikaynak	TR-Dizin
dc.language.iso	en
dc.relation.ispartof	Turkish Journal of Physics
dc.relation.publicationcategory	Makale - Ulusal Hakemli Dergi - Kurum Öğretim Elemanı	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

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