Effects of doping and minority carrier lifetime on mid-wave infrared InGaAs/InAsSb superlattice nBn detector performance

被引:6
|
作者
Newell, A. T. [1 ,2 ]
Logan, J. V. [1 ]
Carrasco, R. A. [1 ]
Alsaad, Z. M. [1 ]
Hains, C. P. [1 ,3 ]
Duran, J. M. [4 ]
Ariyawansa, G. [4 ]
Balakrishnan, G. [2 ]
Maestas, D. [1 ]
Morath, C. P. [1 ]
Hawkins, S. D. [5 ]
Hendrickson, A. [5 ]
Webster, P. T. [1 ]
机构
[1] USAF, Res Lab, Space Vehicles Directorate, Kirtland Afb, NM 87117 USA
[2] Univ New Mexico, Ctr High Technol Mat, Albuquerque, NM 87106 USA
[3] A Tech LLC, BlueHalo Co ATA BlueHalo, Albuquerque, NM 87123 USA
[4] USAF, Res Lab, Sensors Directorate, Wright Patterson Afb, OH 45433 USA
[5] Sandia Natl Labs, Albuquerque, NM 87185 USA
关键词
Antimony compounds - Capacitance - Carrier concentration - Carrier lifetime - Dark currents - Infrared radiation - Molecular beam epitaxy - Semiconducting indium - Semiconducting indium gallium arsenide - Semiconductor quantum wells - Shot noise;
D O I
10.1063/5.0136409
中图分类号
O59 [应用物理学];
学科分类号
摘要
The effect of majority carrier concentration and minority carrier lifetime on the performance of mid-wave infrared (lambda(cutoff) = 5.5 mu m) nBn detectors with variably doped InGaAs/InAsSb type-II superlattice absorbers is investigated. The detector layer structures are grown by molecular beam epitaxy such that their absorbing layers are either undoped, uniformly doped with a target density of 4 * 10(15) cm(-3), or doped with a graded profile, and variable-area mesa detector arrays are fabricated. Each material ' s temperature-dependent minority carrier lifetime is determined by time-resolved photoluminescence, and majority carrier concentration is extracted from capacitance-voltage measurements. Detector performance is evaluated with dark current and photocurrent measurements, from which quantum efficiency and shot-noiselimited noise-equivalent irradiance are calculated. The two doped detectors have lower dark current densities compared to their undoped counterpart due to the reduction in diffusion current as well as suppression of depletion current. Although both intentionally doped devices exhibit lower minority carrier lifetimes relative to the undoped device, the device with graded doping maintains a comparable quantum efficiency to the undoped device. Ultimately, the graded doping structure exhibits the highest sensitivity with a shot noise-limited noise-equivalent irradiance of 6.3 * 10(10) photons/cm(2) s in low-background light conditions, within a factor of 4* of an infrared detector pixel with Rule 07 dark current density and unity quantum efficiency. A detailed analysis of the dark current, quantum efficiency, and minority carrier lifetime provides insight into the material and device design factors that must be considered to realize a device with optimal sensitivity.
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页数:6
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