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Abstract

Photoelectrical characteristics of scanning IR detectors with implemented time delay and integration mode are analyzed. A new “shifted cellular” layout of photosensitive elements in the FPA structure is proposed. Advantages of the new FPA configuration in terms of threshold sensitivity for small-size/point objects are demonstrated. The analysis is based on the Monte Carlo simulation of the diffusion process of photogenerated minority charge carriers in the photosensitive layer photodiode arrays. The analysis is performed taking into account the main photoelectric parameters of FPA elements: photosensitive layer thickness, diffusion length of charge carriers, optical absorption length, their design parameters: geometric sizes of FPA elements, diameters of p-n junctions, and design parameters of the optical system: optical-spot diameter.

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Authors and Affiliations

S. A. Dvoretsky
A. P. Kovchavtsev
I. I. Lee
V. G. Polovinkin
G. Yu. Sidorov
M. V. Yakushev
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Abstract

Studies of background donor concentration (BDC) in HgCdTe samples grown with different types of technology were performed with the use of ion milling as a means of eliminating the compensating acceptors. In bulk crystals, films grown with liquid phase epitaxy and films fabricated with molecular beam epitaxy (MBE) on Si substrates, BDC of the order of ~1014 cm-3 was revealed. Films grown with metal−organic chemical vapour deposition and with MBE on GaAs substrates showed BDC of the order of ~1015 cm-3. A possibility of assessing the BDC in acceptor (arsenic)−doped HgCdTe was demon− strated. In general, the studies showed the effectiveness of ion milling as a method of reducing electrical compensation in n−type MCT and as an excellent tool for assisting evaluation of BDC.

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Authors and Affiliations

I.I. Izhnin
K.D. Mynbaev
A.V. Voitsekhovsky
A.G. Korotaev
O.I. Fitsych
M. Pociask-Bialy
S.A. Dvoretsky
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Abstract

Effect of annealing on the structural properties of arsenic-implanted mercury cadmium telluride film grown by molecular beam epitaxy was studied with the use of transmission electron microscopy and optical reflection. Strong influence of the graded-gap surface layer grown on top of the film on the behaviour of implantation-induced defects under arsenic activation annealing was revealed and interpreted.

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Authors and Affiliations

I.I Izhninab
O.I. Fitsych
Z. Świątek
Y. Morgiel
O.Yu. Bonchyk
H.V. Savytskyy
K.D. Mynbaev
A.V. Voitsekhovskii
A.G. Korotaev
M.V. Yakushev
V.S. Varavin
S.A. Dvoretsky
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Abstract

We present an overview of our technological achievements in the implementation of detector structures based on mercury cadmium telluride (MCT) heterostructures and nanostructures for IR and THz spectral ranges. We use a special MBE design set for the epitaxial layer growth on (013) GaAs substrates with ZnTe and CdTe buffer layers up to 3” in diameter with the precise ellipsometric monitoring in situ. The growth of MCT alloy heterostructures with the optimal composition distribution throughout the thickness allows for the realization of different types of many-layered heterostructures and quantum wells to prepare the material for fabricating single- or dual-band IR and THz detectors.

We also present the two-color broad-band bolometric detectors based on the epitaxial MCT layers that are sensitive in 150–300-GHz subterahertz and infrared ranges from 3 to 10 μm, which operate at the ambient or liquid nitrogen temperatures as photoconductors, as well as the detectors based on planar HgTe quantum wells. The design and dimensions of THz detector antennas are optimized for reasonable detector sensitivity values. A special diffraction limited optical system for the detector testing was designed and manufactured. We represent here the THz images of objects hidden behind a plasterboard or foam plastic packaging, obtained at the radiation frequencies of 70, 140, and 275 GHz, respectively.

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Authors and Affiliations

S.A. Dvoretsky
N.N. Mikhailov
V.G. Remesnik
Yu.G. Sidorov
V.A. Shvets
D.G. Ikusov
V.S. Varavin
J.V. Gumenjuk-Sichevska
A.G. Golenkov
I.O. Lysiuk
Z.F. Tsybrii
A.V. Shevchik-Shekera
F.F. Sizov
A.V. Latyshev
A.L. Aseev

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