Current transport properties of (Au/Ni)/HfAlO3/n-Si metal–insulator–semiconductor junction

buir.contributor.authorArslan, Engin
buir.contributor.authorAalizadeh, Majid
buir.contributor.authorOzbay, Ekmel
buir.contributor.orcidAalizadeh, Majid|0000-0002-4312-1940
buir.contributor.orcidOzbay, Ekmel|0000-0003-2953-1828
dc.citation.volumeNumber148en_US
dc.contributor.authorArslan, Engin
dc.contributor.authorBadali, Yosef
dc.contributor.authorAalizadeh, Majid
dc.contributor.authorAltındal, Semsettin
dc.contributor.authorOzbay, Ekmel
dc.date.accessioned2022-04-26T13:12:27Z
dc.date.available2022-04-26T13:12:27Z
dc.date.issued2020-09-11
dc.departmentDepartment of Physicsen_US
dc.description.abstractIn this study, HfAlO3 ternary alloy thin film was grown on n-type silicon using the atomic layer deposition method. The current transport mechanisms in the (Au/Ni)/HfAlO3/n-Si junction were examined over a wide temperature range (80–360 K). The values obtained for the ideality factor (n) varied from 22.93 to 3.94 and the barrier height at zero bias (ФB0) ranged from 0.221 eV to 0.821 eV as the temperature changed from 80 to 360 K. The ΦB0–n and ΦB0–q/2 kT characteristics were investigated to explain the higher n values and non-ideal behavior of the Richardson curves. Two linear regions were found at low temperatures (LTs; 80–180 K) and high temperatures (HTs; 200–360 K), which indicated the presence of a Gaussian distribution barrier height and the average barrier heights (Φ‾B0) were identified. The values obtained for Φ‾Bo were 0.734 eV for LTs and 1.125 eV for HTs, and the values of σs were 0.085 V for LTs and 0.140 V for HTs. The values obtained for Nss decreased as the temperature increased and they varied between ~1012 and 1013 eV−1 cm−2. Finally, the dielectric behavior and conductivity of the (Au/Ni)/HfAlO3/n-Si junction were investigated at frequencies between 5 kHz and 2 MHz at room temperature. The values determined for ε′ and ε′′ at −1 V and 5 kHz were 2.1 and 3.53, respectively. © 2020en_US
dc.description.provenanceSubmitted by Cem Çağatay Akgün (cem.akgun@bilkent.edu.tr) on 2022-04-26T13:12:27Z No. of bitstreams: 1 Current_transport_properties_of_(AuNi)HfAlO3n_Si_metal_insulator_semiconductor_junction.pdf: 3905558 bytes, checksum: 127662e5fa1de280743b79c7223ff2d0 (MD5)en
dc.description.provenanceMade available in DSpace on 2022-04-26T13:12:27Z (GMT). No. of bitstreams: 1 Current_transport_properties_of_(AuNi)HfAlO3n_Si_metal_insulator_semiconductor_junction.pdf: 3905558 bytes, checksum: 127662e5fa1de280743b79c7223ff2d0 (MD5) Previous issue date: 2020-09-11en
dc.identifier.doi10.1016/j.jpcs.2020.109758en_US
dc.identifier.eissn1879-2553
dc.identifier.issn0022-3697
dc.identifier.urihttp://hdl.handle.net/11693/78159
dc.language.isoEnglishen_US
dc.publisherElsevier Ltden_US
dc.relation.isversionofhttps://dx.doi.org/10.1016/j.jpcs.2020.109758en_US
dc.source.titleJournal of Physics and Chemistry of Solidsen_US
dc.subjectCurrent transport mechanismen_US
dc.subjectDouble Gaussian distributionen_US
dc.subjectHfAlO3 ternary alloyen_US
dc.subjectTemperature dependenceen_US
dc.titleCurrent transport properties of (Au/Ni)/HfAlO3/n-Si metal–insulator–semiconductor junctionen_US
dc.typeArticleen_US

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