
Proceedings Paper
Control of residual background carriers in undoped mid-infrared InAs/GaSb superlatticesFormat | Member Price | Non-Member Price |
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Paper Abstract
The performance and operating temperature of infrared (IR) detectors is largely limited by thermal generation and noise processes in the active region of the device. Particularly, excess background charge carriers enhance Auger recombination and dark currents, and depress the detector figures of merit. Therefore, reducing background carriers in the undoped region of pin diodes is an important issue for developing high-operating temperature IR detectors. In this
paper, we discuss how, through low-temperature Hall measurements, we optimized several growth and design parameters to lower residual carrier densities in various mid-IR InAs/GaSb superlattice (SL) designs. Among the growth/processing parameters investigated in the 21 Å InAs/24 Å GaSb SLs, neither growth temperature nor in-situ
post-growth annealing significantly affected the overall carrier type and density. All of the mid-IR SL samples
investigated were residually p-type. The lowest carrier density (1.8x1011 cm-2) was achieved in SLs grown at 400 °C and
the density was not reduced any further by a post-growth anneal. The growth parameter that most affected the carrier
density was interface composition control. With a minor variation in interface shutter sequence, the carrier density
dramatically increased from ~2x1011 to 5x1012 cm-2, and the corresponding mobility dropped from 6600 to 26 cm2/Vs,
indicating a degradation of interface quality. However, the carrier density was further reduced to 1x1011 cm-2 by
increasing the GaSb layer width. More importantly, a dramatic improvement on the photoluminescence intensity was
achieved with wider GaSb SLs. The disadvantage is that as GaSb layer width increases from 24 to 48 Å, the photoluminescence peak position shifts from 4.1 to 3.4 μm, for a fixed InAs width of 21 Å, indicating a photodiode based on these wider designs would fall short of fully covering the 3 to 5 μm mid-IR spectral region.
Paper Details
Date Published: 26 January 2009
PDF: 9 pages
Proc. SPIE 7222, Quantum Sensing and Nanophotonic Devices VI, 72220Y (26 January 2009); doi: 10.1117/12.810520
Published in SPIE Proceedings Vol. 7222:
Quantum Sensing and Nanophotonic Devices VI
Manijeh Razeghi; Rengarajan Sudharsanan; Gail J. Brown, Editor(s)
PDF: 9 pages
Proc. SPIE 7222, Quantum Sensing and Nanophotonic Devices VI, 72220Y (26 January 2009); doi: 10.1117/12.810520
Show Author Affiliations
H. J. Haugan, Air Force Research Lab. (United States)
S. Elhamri, Univ. of Dayton (United States)
W. C. Mitchel, Air Force Research Lab. (United States)
B. Ullrich, Bowling Green State Univ. (United States)
S. Elhamri, Univ. of Dayton (United States)
W. C. Mitchel, Air Force Research Lab. (United States)
B. Ullrich, Bowling Green State Univ. (United States)
G. J Brown, Air Force Research Lab. (United States)
L. Grazulis, Air Force Research Lab. (United States)
S. Houston, Air Force Research Lab. (United States)
L. Grazulis, Air Force Research Lab. (United States)
S. Houston, Air Force Research Lab. (United States)
Published in SPIE Proceedings Vol. 7222:
Quantum Sensing and Nanophotonic Devices VI
Manijeh Razeghi; Rengarajan Sudharsanan; Gail J. Brown, Editor(s)
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