{"title":"High field conduction mechanism of the evaporated cadmium arsenide thin films","authors":"M. Din, R. D. Gould","doi":"10.1109/SMELEC.1998.781173","DOIUrl":null,"url":null,"abstract":"Cadmium arsenide is a II-V semiconductor which exhibits n-type intrinsic conductivity with high mobility. Potential applications include magnetoresistors and both thermal and photodetectors, which require electrical characterisation over a wide range of deposition and measurement conditions. The films were prepared by vacuum evaporation with deposition rates of 0.5 nm s/sup -1/ and substrate temperatures maintained at constant values of 293 K-393 K. Sandwich-type samples were deposited with film thicknesses of 0.1-1.1 /spl mu/m using evaporated electrodes of Ag and occasionally Au or Al. Above a typical electric field F/sub b/ of up to 5/spl times/10/sup 7/ V m/sup -1/, all samples showed instabilities characteristic of dielectric breakdown or electroforming. Below this field, they showed a high-field conduction process with log J/spl prop/V/sup 1/2/, where J is the current density and V the applied voltage. This type of dependence is indicative of carrier excitation over a potential barrier whose effective barrier height has been lowered by the high electric field. The field-lowering coefficient /spl beta/ had a value of (1.2-5.3)/spl times/10/sup -5/ eV m/sup 1/2/ V/sup -1/2/, which is reasonably consistent with the theoretical value of /spl beta//sub PF/=2.19/spl times/10/sup -5/ eV m/sup 1/2/ V/sup -1/2/ expected when the field-lowering occurs at donor-like centres in the semiconductor (Poole-Frenkel effect). For thinner films, Schottky emission was more probable. The effects of the film thickness, electrode materials, deposition rate, and substrate temperature on the conductivity behaviour are discussed.","PeriodicalId":356206,"journal":{"name":"ICSE'98. 1998 IEEE International Conference on Semiconductor Electronics. Proceedings (Cat. No.98EX187)","volume":"29 5","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"ICSE'98. 1998 IEEE International Conference on Semiconductor Electronics. Proceedings (Cat. No.98EX187)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SMELEC.1998.781173","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
Cadmium arsenide is a II-V semiconductor which exhibits n-type intrinsic conductivity with high mobility. Potential applications include magnetoresistors and both thermal and photodetectors, which require electrical characterisation over a wide range of deposition and measurement conditions. The films were prepared by vacuum evaporation with deposition rates of 0.5 nm s/sup -1/ and substrate temperatures maintained at constant values of 293 K-393 K. Sandwich-type samples were deposited with film thicknesses of 0.1-1.1 /spl mu/m using evaporated electrodes of Ag and occasionally Au or Al. Above a typical electric field F/sub b/ of up to 5/spl times/10/sup 7/ V m/sup -1/, all samples showed instabilities characteristic of dielectric breakdown or electroforming. Below this field, they showed a high-field conduction process with log J/spl prop/V/sup 1/2/, where J is the current density and V the applied voltage. This type of dependence is indicative of carrier excitation over a potential barrier whose effective barrier height has been lowered by the high electric field. The field-lowering coefficient /spl beta/ had a value of (1.2-5.3)/spl times/10/sup -5/ eV m/sup 1/2/ V/sup -1/2/, which is reasonably consistent with the theoretical value of /spl beta//sub PF/=2.19/spl times/10/sup -5/ eV m/sup 1/2/ V/sup -1/2/ expected when the field-lowering occurs at donor-like centres in the semiconductor (Poole-Frenkel effect). For thinner films, Schottky emission was more probable. The effects of the film thickness, electrode materials, deposition rate, and substrate temperature on the conductivity behaviour are discussed.