VSWIR to VLWIR MBE grown HgCdTe material and detectors for remote sensing applications

被引:33
作者
DSouza, AI
Dawson, LC
Anderson, EJ
Markum, AD
Tennant, WE
Bubulac, LO
Zandian, M
Pasko, JG
McLevige, WV
Edwall, DD
Derr, JW
Jandik, JE
机构
[1] ROCKWELL INT SCI CTR,THOUSAND OAKS,CA 91360
[2] ITT DEF & ELECT,FT WAYNE,IN 46801
关键词
HgCdTe; molecular beam epitaxy (MBE); remote sensing;
D O I
10.1007/s11664-997-0211-8
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
The molecular beam epitaxy (MBE) growth technology Is inherently flexible in its ability to change the Hg1-xCdxTe material's bandgap within a growth run and from growth run to growth run. This bandgap engineering flexibility permits tailoring the device architecture to the various specific requirements, Material with active layer x values ranging from similar to 0.198 to 0.570 have been grown and processed into detectors. This wide range in x values is perfectly suited for remote sensing applications, specifically the National Polar Orbiting Environmental Satellite System (NPOESS) program that requires imaging in a multitude of infrared spectral bands, ranging from the 1,58 to 1,64 mu m VSWIR (very short wave infrared) band to the 11.5 to 12.5 mu m LWIR (long wave infrared) band and beyond, These diverse spectral bands require high performance detectors, operating at two temperatures detectors for the VSWIR band operate near room temperature while the SWIR, MWIR (mid wave infra red), LWIR and VLWIR (very long wave infrared) detectors operate near 100K, because of constraints imposed by the cooler for the NPOESS program. This paper uses material parameters to calculate theoretical detector performance for a range of x values, This theoretical detector performance is compared with median measured detector optical and electrical data, Measured detector optical and electrical data, combined with noise model estimates of ROIC performance are used to calculate signal to noise ratio (SNR), for each spectral band, The SNR are compared with respect to the meteorological NPOESS system derived focal plane, The derived system focal plane requirements for NPOESS are met in all the spectral bands.
引用
收藏
页码:656 / 661
页数:6
相关论文
共 10 条
[1]   MOLECULAR-BEAM EPITAXY GROWTH AND INSITU ARSENIC DOPING OF P-ON-N HGCDTE HETEROJUNCTIONS [J].
ARIAS, J ;
ZANDIAN, M ;
PASKO, JG ;
SHIN, SH ;
BUBULAC, LO ;
DEWAMES, RE ;
TENNANT, WE .
JOURNAL OF APPLIED PHYSICS, 1991, 69 (04) :2143-2148
[2]   MBE HGCDTE HETEROSTRUCTURE P-ON-N PLANAR INFRARED PHOTODIODES [J].
ARIAS, JM ;
PASKO, JG ;
ZANDIAN, M ;
SHIN, SH ;
WILLIAMS, GM ;
BUBULAC, LO ;
DEWAMES, RE ;
TENNANT, WE .
JOURNAL OF ELECTRONIC MATERIALS, 1993, 22 (08) :1049-1053
[3]   PLANAR P-ON-N HGCDTE HETEROSTRUCTURE PHOTOVOLTAIC DETECTORS [J].
ARIAS, JM ;
PASKO, JG ;
ZANDIAN, M ;
SHIN, SH ;
WILLIAMS, GM ;
BUBULAC, LO ;
DEWAMES, RE ;
TENNANT, WE .
APPLIED PHYSICS LETTERS, 1993, 62 (09) :976-977
[4]   LONG AND MIDDLE WAVELENGTH INFRARED PHOTODIODES FABRICATED WITH HG1-XCDXTE GROWN BY MOLECULAR-BEAM EPITAXY [J].
ARIAS, JM ;
SHIN, SH ;
PASKO, JG ;
DEWAMES, RE ;
GERTNER, ER .
JOURNAL OF APPLIED PHYSICS, 1989, 65 (04) :1747-1753
[5]   MOLECULAR-BEAM EPITAXIAL HGCDTE MATERIAL CHARACTERISTICS AND DEVICE PERFORMANCE - REPRODUCIBILITY STATUS [J].
BAJAJ, J ;
ARIAS, JM ;
ZANDIAN, M ;
PASKO, JG ;
KOZLOWSKI, LJ ;
DEWAMES, RE ;
TENNANT, WE .
JOURNAL OF ELECTRONIC MATERIALS, 1995, 24 (09) :1067-1076
[6]  
BUBULAC LO, 1996 US WORKSH PHYS
[7]  
Shin S.H., 1993, J ELECT MAT, V22, P1049
[8]   1-F NOISE IN (HG,CD)TE PHOTO-DIODES [J].
TOBIN, SP ;
IWASA, S ;
TREDWELL, TJ .
IEEE TRANSACTIONS ON ELECTRON DEVICES, 1980, 27 (01) :43-48
[9]  
VYDYANATH HR, 1990, P IRIS DETECTOR SPEC, V1, P201
[10]  
WILLIAMS GM, 1994, J ELECT MAT, V24, P1239