1 State Key Laboratory for Superlattices and Microstructures, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China;
2 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
A long-/long-wave dual-color detector with N-M-π-B-π-M-N structure was developed based on a type-Ⅱ InAs/GaSb superlattice. The saturated responsivity was achieved under low bias voltage for both channels. The device could be operated as a single detector for sequential detection and showed high quantum efficiencies. The peak quantum efficiencies of long-wavelength infrared band-1 (blue channel) and long-wavelength infrared band-2 (red channel) were 44% at 6.3 μm under 20 mV and 57% at 9.1 μm under -60 mV, respectively. The optical performance for each channel was achieved using a 2μm thickness absorber. Due to the high QE, the specific detectivities of the blue and red channels reached 5.0×1011 cm·Hz1/2/W at 6.8 μm and 3.1×1011 cm·Hz1/2/W at 9.1 μm, respectively, at 77 K.
Sai-Halasz G A, Tsu R and Esaki L 1977 Appl. Phys. Lett. 30 651
[2]
Nguyen B M, Hoffman D, Wei Y J, Delaunay P Y, Hood A and Razeghi M 2007 Appl. Phys. Lett. 90 231108
[3]
Nguyen B M, Hoffman D, Delaunay P Y and Razeghi M 2007 Appl. Phys. Lett. 91 163511
[4]
Huang E K, Pour S A, Hoang M A, Haddadi A, Razeghi M and Tidrow M Z 2012 Opt. Lett. 37 2025
[5]
Ting D Z, Hill C J, Soibel A, Keo S A, Mumolo J M, Nguyen J and Gunapala S D 2009 Appl. Phys. Lett. 95 023508
[6]
Rodriguez J B, Plis E, Bishop G, Sharma Y D, Kim H, Dawson L R and Krishna S 2007 Appl. Phys. Lett. 91 043514
[7]
Han X, Xiang W, Hao H Y, Jiang D W, Yao Y, Wang G W, Xu Y Q and Niu Z C 2017 Chin. Phys. B 26 018505
[8]
Jiang Z, Han X, Sun Y Y, Guo C Y, Lv Y X, Hao H Y, Jiang D W, Wang G W, Xu Y Q and Niu Z C 2017 Infrared Phys. Technol. 86 159
[9]
Jiang D W, Xiang W, Guo F Y, Hao H Y, Han X, Li X C, Wang G W, Xu Y Q, Yu Q J and Niu Z C 2016 Chin. Phys. Lett. 33 048502
[10]
Sun Y Y, Lv Y X, Han X, Guo C Y, Jiang Z, Hao H Y, Jiang D W, Wang G W, Xu Y Q and Niu Z C 2017 Chin. Phys. B 26 098506
[11]
Huang E K and Razeghi M 2012 SPIE Proceedings - The International Society for Optical Engineering, 21-26 January 2012, San Francisco, United States, 82680Z
[12]
Plis E, Myers S A, Ramirez D A and Krishna S 2016 SPIE Defense + Security, 17-21 April 2016, Baltimore, United States, 981911
[13]
Rodriguez J B, Christol P, Cerutti L, Chevrier F and Joullié A 2005 J. Cryst. Growth 274 6
[14]
Ariyawansa G, Grupen M, Duran J M, Scheihing J E, Nelson T R and Eismann M T 2012 J. Appl. Phys. 111 073107
[15]
Razeghi M, Haddadi A, Dehzangi A, Chevallier R and Yang T 2017 SPIE Defense + Security, 9-13 April 2017, Anaheim, United States, 1017705
[16]
Martyniuk P, Wrobel J, Plis E, Madejczyk P, Kowalewski A, Gawron W, Krishna S and Rogalski A 2012 Semicond. Sci. Technol. 27 055002
[17]
Rogalski A, Martyniuk P and Kopytko M 2017 Appl. Phys. Rev. 4 031304
[1]
Strain compensated type II superlattices grown by molecular beam epitaxy Chao Ning(宁超), Tian Yu(于天), Rui-Xuan Sun(孙瑞轩), Shu-Man Liu(刘舒曼), Xiao-Ling Ye(叶小玲), Ning Zhuo(卓宁), Li-Jun Wang(王利军), Jun-Qi Liu(刘俊岐), Jin-Chuan Zhang(张锦川), Shen-Qiang Zhai(翟慎强), and Feng-Qi Liu(刘峰奇). Chin. Phys. B, 2023, 32(4): 046802.
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