Mimar Sinan Güzel Sanatlar Üniversitesi Açık Bilim, Sanat Arşivi

Açık Bilim, Sanat Arşivi, Mimar Sinan Güzel Sanatlar Üniversitesi tarafından doğrudan ve dolaylı olarak yayınlanan; kitap, makale, tez, bildiri, rapor gibi tüm akademik kaynakları uluslararası standartlarda dijital ortamda depolar, Üniversitenin akademik performansını izlemeye aracılık eder, kaynakları uzun süreli saklar ve yayınların etkisini artırmak için telif haklarına uygun olarak Açık Erişime sunar.

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dc.contributor.authorOylumluoglu, G.
dc.contributor.authorMirioglu, S.
dc.contributor.authorAksu, S.
dc.contributor.authorErkaslan, U.
dc.contributor.authorSiddiki, A.
dc.date.accessioned2025-01-09T20:14:35Z
dc.date.available2025-01-09T20:14:35Z
dc.date.issued2015
dc.identifier.issn1386-9477
dc.identifier.issn1873-1759
dc.identifier.urihttps://doi.org/10.1016/j.physe.2015.06.010
dc.identifier.urihttps://hdl.handle.net/20.500.14124/9152
dc.description.abstractQuasi-two dimensional electron systems exhibit peculiar transport effects depending on their density profiles and temperature. A usual two dimensional electron system is assumed to have a 6 like density distribution along the crystal growth direction. However, once the confining quantum well is sufficiently large, this situation is changed and the density can no longer be assumed as a 6 function. In addition, it is known that the density profile is not a single peaked function, instead can present more than one maxima, depending on the well width. In this work, the electron density distributions in the growth direction considering a variety of wide quantum wells are investigated as a function of temperature. We show that the double peak in the density profile varies from symmetric (similar peak height) to asymmetric while changing the temperature for particular growth parameters. The alternation from symmetric to asymmetric density profiles is known to exhibit intriguing phase transitions and is decisive in defining the properties of the ground state wavefunction in the presence of an external magnetic field, i.e from insulating phases to even denominator fractional quantum Hall states. Here, by solving the temperature and material dependent Schrodinger and Poisson equations self-consistently, we found that such a phase transition may be elaborated by taking into account direct Coulomb interactions together with temperature. (C) 2015 Elsevier B.V. All rights reserved.en_US
dc.language.isoengen_US
dc.publisherElsevieren_US
dc.relation.ispartofPhysica E-Low-Dimensional Systems & Nanostructuresen_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subjectTheory and modelingen_US
dc.subjectHigh-field and nonlinear effectsen_US
dc.titleTemperature dependent symmetry to asymmetry transition in wide quantum wellsen_US
dc.typearticleen_US
dc.authoridSiddiki, Afif/0000-0001-5045-0358
dc.departmentMimar Sinan Güzel Sanatlar Üniversitesien_US
dc.identifier.doi10.1016/j.physe.2015.06.010
dc.identifier.volume74en_US
dc.identifier.startpage193en_US
dc.identifier.endpage197en_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.identifier.wosqualityQ3
dc.identifier.wosWOS:000361952400028
dc.identifier.scopus2-s2.0-84937217462
dc.identifier.scopusqualityQ1
dc.indekslendigikaynakWeb of Scienceen_US
dc.indekslendigikaynakScopusen_US
dc.snmzKA_20250105


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