Electron-Lattice Interaction Scattering Mobility in Tl<sub>2</Sub>ingase<sub>4< Single Crystals

dc.authoridQasrawi, Atef Fayez/0000-0001-8193-6975
dc.authoridGasanly, Nizami/0000-0002-3199-6686
dc.authoridGasanly, Nizami/0000-0002-3199-6686
dc.authorscopusid6603962677
dc.authorscopusid35580905900
dc.authorwosidQasrawi, Atef Fayez/R-4409-2019
dc.authorwosidGasanly, Nizami/HRE-1447-2023
dc.authorwosidGasanly, Nizami/ABA-2249-2020
dc.contributor.authorQasrawi, A. F.
dc.contributor.authorGasanly, N. M.
dc.contributor.otherDepartment of Electrical & Electronics Engineering
dc.date.accessioned2024-07-05T14:34:05Z
dc.date.available2024-07-05T14:34:05Z
dc.date.issued2008
dc.departmentAtılım Universityen_US
dc.department-temp[Qasrawi, A. F.] Atilim Univ, Dept Elect & Elect Engn, TR-06836 Ankara, Turkey; [Qasrawi, A. F.] Alquds Open Univ, Fac Educ, Jenin, Israel; [Gasanly, N. M.] Middle E Tech Univ, Dept Phys, TR-06531 Ankara, Turkeyen_US
dc.descriptionQasrawi, Atef Fayez/0000-0001-8193-6975; Gasanly, Nizami/0000-0002-3199-6686; Gasanly, Nizami/0000-0002-3199-6686en_US
dc.description.abstractIn this work, the dark electrical resistivity, charge carrier density and Hall mobility of Tl(2)InGaSe(4) single crystal have been recorded and analyzed to investigate the dominant scattering mechanism in the crystal. The data analyses have shown that this crystal exhibits an extrinsic n-type conduction. The temperature-dependent dark electrical resistivity analysis reflected the existence of two energy levels as 0.396 and 0.512 eV, being dominant above and below 260 K, respectively. The temperature dependence of the carrier density was analyzed by using the single-donor-single-acceptor model. The latter analysis has shown that the above maintained 0.512 eV energy level is a donor impurity level. The compensation ratio for this crystal is determined as 0.96. The Hall mobility of Tl(2)InGaSe(4) is found to be limited by the scattering of electron-acoustic phonon interactions. The calculated theoretical acoustic phonon scattering mobility agrees with the experimental one under the condition that the acoustic deformation potential is 12.5 eV.en_US
dc.identifier.citationcount2
dc.identifier.doi10.1088/0953-8984/20/15/155204
dc.identifier.issn0953-8984
dc.identifier.issue15en_US
dc.identifier.scopus2-s2.0-42549120212
dc.identifier.urihttps://doi.org/10.1088/0953-8984/20/15/155204
dc.identifier.urihttps://hdl.handle.net/20.500.14411/1017
dc.identifier.volume20en_US
dc.identifier.wosWOS:000254329200014
dc.identifier.wosqualityQ3
dc.institutionauthorQasrawı, Atef Fayez Hasan
dc.language.isoenen_US
dc.publisherIop Publishing Ltden_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.scopus.citedbyCount2
dc.subject[No Keyword Available]en_US
dc.titleElectron-Lattice Interaction Scattering Mobility in Tl<sub>2</Sub>ingase<sub>4< Single Crystalsen_US
dc.typeArticleen_US
dc.wos.citedbyCount2
dspace.entity.typePublication
relation.isAuthorOfPublication1138e68c-e06a-4ee2-a5ec-1dd89a3ecc2c
relation.isAuthorOfPublication.latestForDiscovery1138e68c-e06a-4ee2-a5ec-1dd89a3ecc2c
relation.isOrgUnitOfPublicationc3c9b34a-b165-4cd6-8959-dc25e91e206b
relation.isOrgUnitOfPublication.latestForDiscoveryc3c9b34a-b165-4cd6-8959-dc25e91e206b

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