Effectuality of Barrier Height Inhomogeneity on the Current-Voltage-Temperature Characteristics of Metal Semiconductor Structures with CdZnO Interlayer

dc.contributor.authorTascioglu, Ilke
dc.contributor.authorTan, Serhat Orkun
dc.contributor.authorYakuphanoğlu, Fahrettin
dc.contributor.authorAltindal, Semsettin
dc.date.accessioned2026-08-12T17:33:43Z
dc.date.issued2018
dc.departmentFırat Üniversitesi
dc.description.abstractCurrent-conduction/transport mechanisms (CCMs or CTMs) through barrier and barrier height (BH) formation in the Al/(CdZnO)/p-Si/Al diodes, which were prepared by the sol-gel method, were examined in the range of 110-380 K. The decrease of zero-bias BH (Phi(Bo)) and increase of ideality factor (n) with decreasing temperature were observed. The classic Richardson plot indicated two distinct linear regions that correspond to low and high temperature range (LTR and HTR), respectively. Contrary to this, the acquired Richardson constant value (A*) was much lower than its theoretical value (32 A cm(-2) K-2). Such abnormal behavior of the Phi(Bo), n and A* was attributed to the evidence of the barrier inhomogeneities, especially at low temperature. Therefore, the Phi(Bo-)n, Phi(Bo) and (n(-1) - n) versus q/2kT plots were sketched to acquire significant clues for the Gaussian distribution (GD) of the BHs at rectifier contact area with the mean BH ((Phi) over bar (Bo)) and standard deviation (sigma(so)), which also have two linear parts with distinct slopes. (Phi) over bar and sigma(so) were calculated from the slope and intercept of Phi(Bo) versus q/2kT plot as 0.802 eV and 0.066 V for LTR, 1.043 eV and 0.106 V for HTR, respectively. The (Phi) over bar (Bo) and A* were acquired by utilizing the sigma(so) values and using the Richardson plot as 0.626 eV and 14.26 A cm(-2) K-2 for LTR and 1.021 eV and 32.53 A cm(-2) K-2 for HTR, respectively. Thus, the I-V-T characteristics of the Al/(CdZnO)/p-Si/Al diodes at forward biases were successfully elucidated by the double-GD of BHs with mean BHs of 0.626 eV and 1.021 eV, respectively.
dc.identifier.doi10.1007/s11664-018-6495-z
dc.identifier.endpage6066
dc.identifier.issn0361-5235
dc.identifier.issn1543-186X
dc.identifier.issue10
dc.identifier.orcid0000-0001-9563-4396
dc.identifier.scopus2-s2.0-85049682489
dc.identifier.scopusqualityQ2
dc.identifier.startpage6059
dc.identifier.urihttps://doi.org/10.1007/s11664-018-6495-z
dc.identifier.urihttps://hdl.handle.net/11508/57129
dc.identifier.volume47
dc.identifier.wosWOS:000443021000054
dc.identifier.wosqualityQ2
dc.indekslendigikaynakWeb of Science
dc.indekslendigikaynakScopus
dc.language.isoen
dc.publisherSpringer
dc.relation.ispartofJournal of Electronic Materials
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.snmzKA_WoS_20260511
dc.subjectCdZnO thin films
dc.subjectcurrent-transport mechanisms
dc.subjectbarrier height inhomogeneity
dc.subjectdouble Gaussian distribution
dc.titleEffectuality of Barrier Height Inhomogeneity on the Current-Voltage-Temperature Characteristics of Metal Semiconductor Structures with CdZnO Interlayer
dc.typeArticle

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