Seunghyun Lee, S. Kodati, D. Fink, T. Ronningen, A. Jones, J. Campbell, M. Winslow, C. Grein, S. Krishna
{"title":"Multiplication characteristics of Al0.4Ga0.07In0.53As avalanche photodiodes grown as digital alloys on InP substrates","authors":"Seunghyun Lee, S. Kodati, D. Fink, T. Ronningen, A. Jones, J. Campbell, M. Winslow, C. Grein, S. Krishna","doi":"10.1109/DRC50226.2020.9135156","DOIUrl":null,"url":null,"abstract":"Avalanche photodiodes (APDs) are used in short- and mid-wave infrared applications such as optical communication, LIDAR and 3D imaging [1] due to their internal gain, which improves the signal to noise ratio (SNR). However, the multiplication gain ( M ) gives rise to excess noise, caused by the stochastic nature of impact ionization, which can significantly degrade the SNR of APDs. The excess noise is quantitatively measured by excess noise factor, F(M) that is expressed by McIntyre’s local field theory [1] , F(M) = kM + (1-k)[2-(1/M)] where k is the ratio of the impact ionization coefficients for electrons and holes. According to the equation above, the low excess noise factor in APDs can be attained by a low k value.","PeriodicalId":397182,"journal":{"name":"2020 Device Research Conference (DRC)","volume":"176 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2020 Device Research Conference (DRC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DRC50226.2020.9135156","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
Avalanche photodiodes (APDs) are used in short- and mid-wave infrared applications such as optical communication, LIDAR and 3D imaging [1] due to their internal gain, which improves the signal to noise ratio (SNR). However, the multiplication gain ( M ) gives rise to excess noise, caused by the stochastic nature of impact ionization, which can significantly degrade the SNR of APDs. The excess noise is quantitatively measured by excess noise factor, F(M) that is expressed by McIntyre’s local field theory [1] , F(M) = kM + (1-k)[2-(1/M)] where k is the ratio of the impact ionization coefficients for electrons and holes. According to the equation above, the low excess noise factor in APDs can be attained by a low k value.
雪崩光电二极管(apd)由于其内部增益提高了信噪比(SNR),被用于光通信、激光雷达和3D成像等短波和中波红外应用[1]。然而,由于碰撞电离的随机性,倍增增益(M)会产生过量的噪声,从而显著降低apd的信噪比。过量噪声通过过量噪声因子F(M)定量测量,过量噪声因子F(M)由McIntyre局部场论[1]表示,F(M) = kM + (1-k)[2-(1/M)],其中k为电子与空穴碰撞电离系数之比。由上式可知,低k值可以使apd的多余噪声系数低。