Where are the edge-states near the quantum point contacts? A self-consistent approach
dc.authorid | Siddiki, Afif/0000-0001-5045-0358 | |
dc.authorwosid | Mese, Ali ihsan/JXX-8717-2024 | |
dc.contributor.author | Siddiki, A. | |
dc.contributor.author | Cicek, E. | |
dc.contributor.author | Eksi, D. | |
dc.contributor.author | Mese, A. I. | |
dc.contributor.author | Aktas, S. | |
dc.contributor.author | Hakioglu, T. | |
dc.date.accessioned | 2024-06-12T11:00:02Z | |
dc.date.available | 2024-06-12T11:00:02Z | |
dc.date.issued | 2008 | |
dc.department | Trakya Üniversitesi | en_US |
dc.description | 17th International Conference on Electronic Properties of Two-Dimensional Systems -- JUL 15-20, 2007 -- Genoa, ITALY | en_US |
dc.description.abstract | In this work, we calculate the current distribution, in the close vicinity of the quantum point contacts (QPCs), taking into account the Coulomb interaction. In the first step, we calculate the bare confinement potential of a generic QPC and, in the presence of a perpendicular magnetic field, obtain the positions of the incompressible edge states (IES) taking into account electron-electron interaction within the Thomas-Fermi theory of screening. Using a local version of Ohm's law, together with a relevant conductivity model, we also calculate the current distribution. We observe that, the imposed external current is confined locally into the incompressible strips. Our calculations demonstrate that, the inclusion of the electron-electron interaction, strongly changes the general picture of the transport through the QPCs. (C) 2007 Elsevier B.V. All rights reserved. | en_US |
dc.description.sponsorship | European Off Aerosp Res & Dev,Air Force Off Sci Res,USAF Res Lab,Off Naval Res Global,Int Union Pure & Appl Phys,Scuola Normale Superiore Pisa,Int Ctr Theoret Phys,Oxford Instruments,Off Naval Res,Natl Enterprise NanoSci & NanoTechnol CNR INFM,Fondazione Carige Genova | en_US |
dc.identifier.doi | 10.1016/j.physe.2007.08.097 | |
dc.identifier.endpage | 1162 | en_US |
dc.identifier.issn | 1386-9477 | |
dc.identifier.issn | 1873-1759 | |
dc.identifier.issue | 5 | en_US |
dc.identifier.scopus | 2-s2.0-39649093626 | en_US |
dc.identifier.scopusquality | Q2 | en_US |
dc.identifier.startpage | 1160 | en_US |
dc.identifier.uri | https://doi.org/10.1016/j.physe.2007.08.097 | |
dc.identifier.uri | https://hdl.handle.net/20.500.14551/20677 | |
dc.identifier.volume | 40 | en_US |
dc.identifier.wos | WOS:000254646400064 | en_US |
dc.identifier.wosquality | Q3 | en_US |
dc.indekslendigikaynak | Web of Science | en_US |
dc.indekslendigikaynak | Scopus | en_US |
dc.language.iso | en | en_US |
dc.publisher | Elsevier | en_US |
dc.relation.ispartof | Physica E-Low-Dimensional Systems & Nanostructures | en_US |
dc.relation.publicationcategory | Konferans Öğesi - Uluslararası - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/openAccess | en_US |
dc.subject | Edge States | en_US |
dc.subject | Quantum Hall Effect | en_US |
dc.subject | Screening | en_US |
dc.subject | Quantum Point Contact's | en_US |
dc.subject | Mach-Zehnder Interferometer | en_US |
dc.title | Where are the edge-states near the quantum point contacts? A self-consistent approach | en_US |
dc.type | Conference Object | en_US |