中波碲镉汞雪崩光电二极管的增益特性
[1] Singh A, Srivastav V, Pal R. HgCdTe avalanche photodiodes: A review [J]. Optics & Laser Technology, 2011, 43:1358-1370.
[2] Rothman J, de Borniol E, Gravrand O, et al. HgCdTe APD-focal plane array development at DEFIR [J]. Proc. of SPIE, 2010, 7834: 78340O-1-78340O-1-8.
[3] Kinch M A, Beck J D, Wan C F, et al. HgCdTe electron avalanche photodiodes [J]. Journal of Electronic Materials, 2004, 33(6):630-639.
[4] Beck J D, Wan C F, Kinch M A, et al. MWIR HgCdTe avalanche photodiodes [J]. Proc. of SPIE, 2001, 4454:188-197.
[5] Beck J D, Wan C F, Kinch M A, et al. The HgCdTe electron avalanche photodiode [J]. Journal of Electronic Materials, 2006, 35(6):1166-1173.
[6] Beck J, Woodall M, Scritchfield R, et al. Gated IR imaging with 128x128 HgCdTe electron avalanche photodiode FPA [J]. Proc. of SPIE, 2007, 6542: 654217-1-654217-18.
[7] Baker I, Duncan S, Copley J. A low noise, laser-gated imaging system for long range target identification [J]. Proc. of SPIE, 2004, 5406:133-144.
[8] Baker I, Owton D, Trundle K, et al. Advanced infrared detectors for mult imode active and passive imaging applications [J].Proc. of SPIE, 2008, 69402:69402L-1-69402L-11.
[9] de Borniol E, Guellec F, Rothman J, et al. HgCdTe-based APD focal plane array for 2D and 3D active imaging: first results on a 320×256 with 30 ?m pitch demonstrator [J]. Proc. of SPIE, 2010, 7660:76603D-1-76603D-9.
[10] de Borniol E, Rothman J, Guellec F, et al. Active three-dimensional and thermal imaging with a 30 μm pitch 320×256 HgCdTe avalanche photodiode focal plane array [J]. Optical Engineering, 2012, 51(6):061305-1-061305-6.
[11] Kerlain A, Bonnouvier G, Rubaldo L, et al. Performance of mid-wave infrared HgCdTe e-avalanche photodiodes [J]. Journal of Electronic Materials, 2012, 41(10):2943-2948.
[12] Kinch M A. A theoretical model for the hgcdte electron avalanche photodiode [J]. Journal of Electronic Materials, 2008, 37(9):1453-1459.
[13] Rothman J, Mollard L, Gout S, et al. History-dependent impact ionization theory applied to HgCdTe e-APDs [J]. Journal of Electronic Materials, 2011, 40(8):1757-1768.
[14] LIU Xing-Xin. Status of HgCdTe avalanche photodiode arrays [J].Laser&Infrared(刘兴新. 碲镉汞雪崩光电二极管发展现状.激光与红外), 2009,39(9):909-913.
[17] Bertazzi F, Moresco M, Penna M, et al. Full-band monte carlo simulation of HgCdTe APDs [J]. Journal of Electronic Materials, 2010, 39(7):912-917.
[18] Qiu W C, Hu W D, Chen L, et al. Dark current transport and avalanche mechanism in HgCdTe electron-avalanche photodiodes [J]. IEEE Transactions on Electron Devices, 2015, 62:1926-1931.
[19] Li Q, He J L, Hu W D, et al. Influencing sources for dark current transport and avalanche mechanisms in planar and mesa HgCdTe p-i-n electron-avalanche photodiodes [J]. IEEE Transactions on Electron Devices, 2018, 65:572-576.
李雄军, 韩福忠, 李立华, 李东升, 胡彦博, 杨登泉, 杨超伟, 孔金丞, 舒恂, 庄继胜, 赵俊. 中波碲镉汞雪崩光电二极管的增益特性[J]. 红外与毫米波学报, 2019, 38(2): 02175. LI Xiong-Jun, HAN Fu-Zhong, LI Li-Hua, LI Dong-Sheng, HU Yan-Bo, YANG Deng-Quan, YANG Chao-Wei, KONG Jin-Cheng, SHU Xun, ZHUANG Ji-Sheng, ZHAO Jun. Gain characteristics of MW HgCdTe avalanche photodiodes[J]. Journal of Infrared and Millimeter Waves, 2019, 38(2): 02175.