{"title":"Особенности поведения высокочастотной проводимости неупорядоченных полупроводников с ростом температуры","authors":"М.А. Ормонт, Н.В. Валенко","doi":"10.21883/ftt.2023.07.55852.98","DOIUrl":null,"url":null,"abstract":"The peculiarities of the behavior of high-frequency conductivity of disordered semiconductors associated with the hopping transport of electrons in the impurity band with increasing temperature were studied. Via the pair approximation, it is shown that the transition (crossover) observed at low temperatures (T ≈ 1 K) in the terahertz frequency range from an almost linear to a quadratic frequency dependence of the real part of conductivity can stay on with increasing temperature and be caused by the transition from relaxation conductivity with a variable-range (frequency-dependent) hopping distance to phononless conductivity with a fixed- range hopping distance.","PeriodicalId":24077,"journal":{"name":"Физика твердого тела","volume":"21 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Физика твердого тела","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21883/ftt.2023.07.55852.98","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The peculiarities of the behavior of high-frequency conductivity of disordered semiconductors associated with the hopping transport of electrons in the impurity band with increasing temperature were studied. Via the pair approximation, it is shown that the transition (crossover) observed at low temperatures (T ≈ 1 K) in the terahertz frequency range from an almost linear to a quadratic frequency dependence of the real part of conductivity can stay on with increasing temperature and be caused by the transition from relaxation conductivity with a variable-range (frequency-dependent) hopping distance to phononless conductivity with a fixed- range hopping distance.