{"title":"Optoelectronic bistability at low temperature avalanche breakdown in GaAs epitaxial films","authors":"O. Ryabushkin","doi":"10.1117/12.2294892","DOIUrl":null,"url":null,"abstract":"The object of this report is a new type of optoelectronic bistability in n-GaAs epitaxial films at helium temperatures based on the phenomenon of low-temperature impurity breakdown. The bistability mechanism is related with the following two factors: 1. The films possess an S-shaped current-voltage characteristic (CVC) that is light-sensetive (Fig. 1) [ 1] . Light illumination changes the characteristic point Ith, Vao I., V. of the CVC which limit the region of negative differential resistence, here Ith, Va-current and voltage of the threshold points, I., Vi--those of the sustaining points. Under photoexcitation Vlh falls to the value Vtia and Tot increases to Ina . This property of the CVC allows to realize the light-induced electric switching when the external circuit is properly chosen. . _ .•","PeriodicalId":322470,"journal":{"name":"Marketplace for Industrial Lasers","volume":"16 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-12-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Marketplace for Industrial Lasers","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.2294892","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
The object of this report is a new type of optoelectronic bistability in n-GaAs epitaxial films at helium temperatures based on the phenomenon of low-temperature impurity breakdown. The bistability mechanism is related with the following two factors: 1. The films possess an S-shaped current-voltage characteristic (CVC) that is light-sensetive (Fig. 1) [ 1] . Light illumination changes the characteristic point Ith, Vao I., V. of the CVC which limit the region of negative differential resistence, here Ith, Va-current and voltage of the threshold points, I., Vi--those of the sustaining points. Under photoexcitation Vlh falls to the value Vtia and Tot increases to Ina . This property of the CVC allows to realize the light-induced electric switching when the external circuit is properly chosen. . _ .•