{"title":"基于ii型InAs/GaSb超晶格的长波红外探测器","authors":"C. Jian","doi":"10.3724/sp.j.1010.2013.00210","DOIUrl":null,"url":null,"abstract":"A 12.5 μm long wavelength infrared detector based on InAs/GaSb Type-Ⅱ superlattice was presented in this work.Superlattice materials were grown on GaSb substrates using MBE technology.Absorber structure for long wavelength detector was designed to be 15ML(InAs)/7ML(GaSb).The detector used a PBIN multiple heterostructures to decrease the dark current.The dark current I-V curve,responsivity spectra and blackbody current responsivity were measured at 77 K.At this temperature,RmaxA product was 2.5 Ωcm2 for the device with a photo sensitive area of 100 μm× 100μm.At zero bias,a current responsivity of 1.29 A/W was measured for the detector,which correspond to a blackbody detectivity of 2.1×109 cmHz1/2/W.Quantum efficiency at 11 μm was measured to be 14.3%.Dark current characteristics were simulated with four kinds of probable transport mechanisms.The results showed that the dominated dark current of the detector is Generation-Recombination current.","PeriodicalId":50181,"journal":{"name":"红外与毫米波学报","volume":"1 1","pages":""},"PeriodicalIF":0.6000,"publicationDate":"2013-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Long wavelength infrared detector based on Type-II InAs/GaSb superlattice\",\"authors\":\"C. Jian\",\"doi\":\"10.3724/sp.j.1010.2013.00210\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A 12.5 μm long wavelength infrared detector based on InAs/GaSb Type-Ⅱ superlattice was presented in this work.Superlattice materials were grown on GaSb substrates using MBE technology.Absorber structure for long wavelength detector was designed to be 15ML(InAs)/7ML(GaSb).The detector used a PBIN multiple heterostructures to decrease the dark current.The dark current I-V curve,responsivity spectra and blackbody current responsivity were measured at 77 K.At this temperature,RmaxA product was 2.5 Ωcm2 for the device with a photo sensitive area of 100 μm× 100μm.At zero bias,a current responsivity of 1.29 A/W was measured for the detector,which correspond to a blackbody detectivity of 2.1×109 cmHz1/2/W.Quantum efficiency at 11 μm was measured to be 14.3%.Dark current characteristics were simulated with four kinds of probable transport mechanisms.The results showed that the dominated dark current of the detector is Generation-Recombination current.\",\"PeriodicalId\":50181,\"journal\":{\"name\":\"红外与毫米波学报\",\"volume\":\"1 1\",\"pages\":\"\"},\"PeriodicalIF\":0.6000,\"publicationDate\":\"2013-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"红外与毫米波学报\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.3724/sp.j.1010.2013.00210\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"红外与毫米波学报","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.3724/sp.j.1010.2013.00210","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"OPTICS","Score":null,"Total":0}
Long wavelength infrared detector based on Type-II InAs/GaSb superlattice
A 12.5 μm long wavelength infrared detector based on InAs/GaSb Type-Ⅱ superlattice was presented in this work.Superlattice materials were grown on GaSb substrates using MBE technology.Absorber structure for long wavelength detector was designed to be 15ML(InAs)/7ML(GaSb).The detector used a PBIN multiple heterostructures to decrease the dark current.The dark current I-V curve,responsivity spectra and blackbody current responsivity were measured at 77 K.At this temperature,RmaxA product was 2.5 Ωcm2 for the device with a photo sensitive area of 100 μm× 100μm.At zero bias,a current responsivity of 1.29 A/W was measured for the detector,which correspond to a blackbody detectivity of 2.1×109 cmHz1/2/W.Quantum efficiency at 11 μm was measured to be 14.3%.Dark current characteristics were simulated with four kinds of probable transport mechanisms.The results showed that the dominated dark current of the detector is Generation-Recombination current.