TY - GEN
T1 - MWIR InAsSb XBn detectors for high operating temperatures
AU - Klipstein, Philip
AU - Klin, Olga
AU - Grossman, Steve
AU - Snapi, Noam
AU - Yaakobovitz, Barak
AU - Brumer, Maya
AU - Lukomsky, Inna
AU - Aronov, Daniel
AU - Yassen, Michael
AU - Yofis, Boris
AU - Glozman, Alex
AU - Fishman, Tal
AU - Berkowitz, Eyal
AU - Magen, Osnat
AU - Shtrichman, Itay
AU - Weiss, Eliezer
PY - 2010
Y1 - 2010
N2 - An XBn photovoltaic device has a band profile similar to that of a standard homojunction p-n diode, except that the depletion region is made from a wide bandgap barrier material with a negligible valence band offset but a large conduction band offset. In this notation, "X" stands for the n- or p-type contact layer, "B", for the n-type, wide bandgap, barrier layer, and "n", for the n-type, narrow bandgap, active layer. In this work, we report on the fabrication of XBn devices, which were grown by Molecular Beam Epitaxy (MBE) on GaSb substrates. Each structure has an InAsSb active layer of thickness ∼1.5μm and a 0.2-0.5μm thick AlSbAs barrier layer. Good growth uniformity was achieved with lattice matching of better than 500ppm. Selected layers have been processed into devices which operate with a high internal quantum efficiency at a bias of ∼0.1-0.2V, and which exhibit a very low dark current due to the strong suppression of the current component due to bulk Generation-Recombination processes. From dark current measurements, a minority carrier lifetime of >670nS has been estimated in devices with an active layer doping of ∼4×1015cm-3. In optimized, lattice matched, devices with this doping and an active layer thickness of 4μm, a cut-off wavelength of ∼ 4.0 - 4.1μm is expected at 160K, with a dark current density of ∼10-6 A cm-2 and a quantum efficiency of >70% (λ<4μm). These figures correspond to BLIP operation at 160K with a photocurrent to dark current ratio of ∼4 at f/3.
AB - An XBn photovoltaic device has a band profile similar to that of a standard homojunction p-n diode, except that the depletion region is made from a wide bandgap barrier material with a negligible valence band offset but a large conduction band offset. In this notation, "X" stands for the n- or p-type contact layer, "B", for the n-type, wide bandgap, barrier layer, and "n", for the n-type, narrow bandgap, active layer. In this work, we report on the fabrication of XBn devices, which were grown by Molecular Beam Epitaxy (MBE) on GaSb substrates. Each structure has an InAsSb active layer of thickness ∼1.5μm and a 0.2-0.5μm thick AlSbAs barrier layer. Good growth uniformity was achieved with lattice matching of better than 500ppm. Selected layers have been processed into devices which operate with a high internal quantum efficiency at a bias of ∼0.1-0.2V, and which exhibit a very low dark current due to the strong suppression of the current component due to bulk Generation-Recombination processes. From dark current measurements, a minority carrier lifetime of >670nS has been estimated in devices with an active layer doping of ∼4×1015cm-3. In optimized, lattice matched, devices with this doping and an active layer thickness of 4μm, a cut-off wavelength of ∼ 4.0 - 4.1μm is expected at 160K, with a dark current density of ∼10-6 A cm-2 and a quantum efficiency of >70% (λ<4μm). These figures correspond to BLIP operation at 160K with a photocurrent to dark current ratio of ∼4 at f/3.
KW - Dark Current
KW - Diffusion Current
KW - Focal Plane Array
KW - Generation-Recombination Current
KW - High Operating Temperature
KW - Indium Arsenide Antimonide
KW - Infrared Detector
KW - Shockley-Read-Hall
KW - XBn
KW - nBn
UR - http://www.scopus.com/inward/record.url?scp=79953701080&partnerID=8YFLogxK
U2 - 10.1117/12.849503
DO - 10.1117/12.849503
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AN - SCOPUS:79953701080
SN - 9780819481245
T3 - Proceedings of SPIE - The International Society for Optical Engineering
BT - Infrared Technology and Applications XXXVI
T2 - Infrared Technology and Applications XXXVI
Y2 - 5 April 2010 through 9 April 2010
ER -