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Identifying of series resistance and interface states on rhenium/n-GaAs structures using C–V–T and G/ω–V–T characteristics in frequency ranged 50 kHz to 5 MHz

dc.contributor.authorÇiçek, Osman
dc.contributor.authorDurmuş, Haziret
dc.contributor.authorAltındal, Şemsettin
dc.date.accessioned2026-01-04T13:33:39Z
dc.date.issued2019-11-21
dc.description.abstractIn this study, Re/n-GaAs with a native oxide layer based on metal–semiconductor (MS) structures were produced and then, the capacitance–voltage–temperature (C–V–T) and the conductance–voltage–temperature (G/ω–V–T) data of them were obtained in the frequency ranged 50 kHz to 5 MHz. Using the raw data, the electronic parameters was calculated by the developed LabVIEW-based program. Methodologically, the series resistance (Rs) values were calculated from the measured capacitance (Cm) and conductivity (Gm) values, while the interface state (Nss) values were obtained from using the combined high (CHF)–low (CLF) frequency capacitance method by Nicollian and Brews. Experimentally, the C values increased with a decreasing frequency, while decreased with increasing temperatures in the depletion and accumulation regions. On the other hand, G/ω values decreased with increasing frequency in forward and reverse bias regions. It can be attributed that, the C and the G/ω values are quite affected by the presence of the Rs and the Nss in the forbidden energy gap and a native oxide layer between M and S. The Rs–V–T curves have especially peaks in accumulation and depletion regions at low frequency values, whereas these peaks decreased at high frequencies. In addition, the Nss–V–T curves give peaks in the range of − 0.1 V to 0.7 V at variable temperatures and the Nss values decrease with increasing temperature and shift towards negative bias regions. Experimental results indicate that the Rs and Nss are important parameters and so, these parameters must be considered in sensor applications based on Re/n-GaAs structures.
dc.description.urihttps://doi.org/10.1007/s10854-019-02578-1
dc.description.urihttps://dx.doi.org/10.1007/s10854-019-02578-1
dc.description.urihttps://avesis.gazi.edu.tr/publication/details/630cada8-07b9-4f9e-b2a4-860983ed6598/oai
dc.description.urihttps://hdl.handle.net/20.500.12395/38554
dc.identifier.doi10.1007/s10854-019-02578-1
dc.identifier.eissn1573-482X
dc.identifier.endpage713
dc.identifier.issn0957-4522
dc.identifier.openairedoi_dedup___::ea3ce794cca16e1714c8d482e9dd7726
dc.identifier.orcid0000-0002-2765-4165
dc.identifier.orcid0000-0002-5078-0709
dc.identifier.scopus2-s2.0-85075682854
dc.identifier.startpage704
dc.identifier.urihttps://hdl.handle.net/20.500.12597/37575
dc.identifier.volume31
dc.identifier.wos000497851000007
dc.language.isoeng
dc.publisherSpringer Science and Business Media LLC
dc.relation.ispartofJournal of Materials Science: Materials in Electronics
dc.rightsOPEN
dc.subjectresistance
dc.subjectconductance–voltage–temperature
dc.subjectG/ω-V-T
dc.subjectrhenium/n-GaAs
dc.subjectinterface states
dc.subjectcapacitance–voltage–temperature
dc.subjectC-V-T
dc.titleIdentifying of series resistance and interface states on rhenium/n-GaAs structures using C–V–T and G/ω–V–T characteristics in frequency ranged 50 kHz to 5 MHz
dc.typeArticle
dspace.entity.typePublication
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Using the raw data, the electronic parameters was calculated by the developed LabVIEW-based program. Methodologically, the series resistance (Rs) values were calculated from the measured capacitance (Cm) and conductivity (Gm) values, while the interface state (Nss) values were obtained from using the combined high (CHF)–low (CLF) frequency capacitance method by Nicollian and Brews. Experimentally, the C values increased with a decreasing frequency, while decreased with increasing temperatures in the depletion and accumulation regions. On the other hand, G/ω values decreased with increasing frequency in forward and reverse bias regions. It can be attributed that, the C and the G/ω values are quite affected by the presence of the Rs and the Nss in the forbidden energy gap and a native oxide layer between M and S. The Rs–V–T curves have especially peaks in accumulation and depletion regions at low frequency values, whereas these peaks decreased at high frequencies. In addition, the Nss–V–T curves give peaks in the range of − 0.1 V to 0.7 V at variable temperatures and the Nss values decrease with increasing temperature and shift towards negative bias regions. 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