G. Umana-Membreno, B. Klein, H. Kala, J. Antoszewski, G. Gautam, M. N. Kutty, E. Plis, S. Krishna, L. Faraone
{"title":"Vertical transport in InAs/GaSb type-II superlattices","authors":"G. Umana-Membreno, B. Klein, H. Kala, J. Antoszewski, G. Gautam, M. N. Kutty, E. Plis, S. Krishna, L. Faraone","doi":"10.1109/COMMAD.2012.6472332","DOIUrl":null,"url":null,"abstract":"In this work, we report on the measurement of vertical transport parameters in p-doped InAs/GaSb type-II superlattices for long-wavelength infrared detectors. Since the Hall effect technique cannot be used for vertical transport measurements, a magnetoresistance approach has been used. The magnetore-sistance data was obtained at electric fields not exceeding 25 V/cm and magnetic fields up to 12T. It is shown that at room temperature the sample conductivity is due to four distinct carriers, associated with the majority carrier holes, side-wall inversion layer electrons, and two minority carrier electrons likely associated with two distinct conduction band levels.","PeriodicalId":136573,"journal":{"name":"COMMAD 2012","volume":"19 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2012-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"COMMAD 2012","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/COMMAD.2012.6472332","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
In this work, we report on the measurement of vertical transport parameters in p-doped InAs/GaSb type-II superlattices for long-wavelength infrared detectors. Since the Hall effect technique cannot be used for vertical transport measurements, a magnetoresistance approach has been used. The magnetore-sistance data was obtained at electric fields not exceeding 25 V/cm and magnetic fields up to 12T. It is shown that at room temperature the sample conductivity is due to four distinct carriers, associated with the majority carrier holes, side-wall inversion layer electrons, and two minority carrier electrons likely associated with two distinct conduction band levels.