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

Author:

Newell A. T.12ORCID,Logan J. V.1ORCID,Carrasco R. A.1ORCID,Alsaad Z. M.1ORCID,Hains C. P.13ORCID,Duran J. M.4ORCID,Ariyawansa G.4ORCID,Balakrishnan G.2ORCID,Maestas D.1ORCID,Morath C. P.1ORCID,Hawkins S. D.5ORCID,Hendrickson A.5ORCID,Webster P. T.1ORCID

Affiliation:

1. Air Force Research Laboratory, Space Vehicles Directorate, Kirtland AFB 1 , New Mexico 87117, USA

2. Center for High Technology Materials, University of New Mexico 2 , Albuquerque, New Mexico 87106, USA

3. A-Tech, LLC, a BlueHalo company (ATA BlueHalo) 3 , Albuquerque, New Mexico 87123, USA

4. Air Force Research Laboratory, Sensors Directorate 4 , Wright-Patterson AFB, Ohio 45433, USA

5. Sandia National Laboratories 5 , Albuquerque, New Mexico 87185, USA

Abstract

The effect of majority carrier concentration and minority carrier lifetime on the performance of mid-wave infrared ( λ cutoff = 5.5   μ 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 × 1015 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-noise-limited 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 × 1010 photons/cm2 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.

Funder

Air Force Research Laboratory

Publisher

AIP Publishing

Subject

Physics and Astronomy (miscellaneous)

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