State-of-the-art Type II antimonide-based superlattice photodiodes for infrared detection and imaging

Manijeh Razeghi; Binh-Minh Nguyen; Pierre-Yves Delaunay; Edward Kwei-wei Huang; Siamak Abdollahi Pour; Paritosh Manukar; Simeon Bogdanov

doi:10.1117/12.828421

9 September 2009 State-of-the-art Type II antimonide-based superlattice photodiodes for infrared detection and imaging

Manijeh Razeghi, Binh-Minh Nguyen, Pierre-Yves Delaunay, Edward Kwei-wei Huang, Siamak Abdollahi Pour, Paritosh Manukar, Simeon Bogdanov

Author Affiliations +

Proceedings Volume 7467, Nanophotonics and Macrophotonics for Space Environments III; 74670T (2009) https://doi.org/10.1117/12.828421
Event: SPIE Optical Engineering + Applications, 2009, San Diego, California, United States

Abstract

Type-II InAs/GaSb Superlattice (SL), a system of multi interacting quantum wells was first introduced by Nobel Laureate L. Esaki in the 1970s. Since then, this low dimensional system has drawn a lot of attention for its attractive quantum mechanics properties and its grand potential for the emergence into the application world, especially in infrared detection. In recent years, Type-II InAs/GaSb superlattice photo-detectors have experienced significant improvements in material quality, structural designs and imaging applications which elevated the performances of Type-II InAs/GaSb superlattice photodetectors to a comparable level to the state-of-the-art Mercury Cadmium Telluride. We will present in this talk the current status of the state-of-the-art Type II superlattice photodetectors and focal plane arrays, and the future outlook for this material system.

Citation Download Citation

Manijeh Razeghi, Binh-Minh Nguyen, Pierre-Yves Delaunay, Edward Kwei-wei Huang, Siamak Abdollahi Pour, Paritosh Manukar, and Simeon Bogdanov "State-of-the-art Type II antimonide-based superlattice photodiodes for infrared detection and imaging", Proc. SPIE 7467, Nanophotonics and Macrophotonics for Space Environments III, 74670T (9 September 2009); https://doi.org/10.1117/12.828421

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