Dark Current Reduction in Near Infrared P-I-N Detector Diodes Fabricated from In.75Ga.25As Grown by Molecular Beam Epitaxy on InP Substrates

1996 ◽  
Vol 450 ◽  
Author(s):  
M. Micovic ◽  
W. Z. Cai ◽  
Y. Ren ◽  
J. Neal ◽  
S. F. Nelson ◽  
...  

ABSTRACTWe have investigated several approaches to improve the material quality of lattice-mismatched In.75Ga.25As grown by Molecular Beam Epitaxy (MBE) on (100) InP substrates. They include linear grading of In composition from lattice matched In.53Ga.47As to In.75Ga.25As in a 1 μm buffer layer grown at reduced substrate temperature, in combination with various in situ annealing and material regrowth steps. The material was used for fabrication of mesa-structure p-i-n photodetectors with 2.2 μm cutoff wavelength. The room temperature dark current density at 1 V reverse bias was approximately 2 mA/cm2 in all structures that were subjected to anneal and regrowth process, a factor of three improvement over reference samples which were not subjected to annealing and regrowth. The dark current density at 15 V reverse bias (10 mA/cm2 for the best devices) was at least two orders of magnitude lower in all annealed samples than in reference samples. These results suggest that the MBE grown material can be an attractive alternative to the vapor phase epitaxy (VPE) grown material which is commonly used for fabrication of these detectors.

Author(s):  
М.А. Суханов ◽  
А.К. Бакаров ◽  
Д.Ю. Протасов ◽  
К.С. Журавлёв

A photodetector heterostructure based on AlInSb / InSb grown by molecular beam epitaxy was presented. Mesastructures of various diameters were fabricated and the temperature dependence of the dark current was measured. It was shown that the built-in barrier blocks the flow of the main charge carriers, thereby reducing the dark current density, in comparison with the pin structure based on InSb. By measuring the dependence of the dark current on the size of the mesastructure, it was shown that the bulk component of the current prevails over the surface component.


2008 ◽  
Vol 93 (4) ◽  
pp. 041913 ◽  
Author(s):  
Houssam Chouaib ◽  
Catherine Bru-Chevallier ◽  
Aleksandra Apostoluk ◽  
Wojciech Rudno-Rudzinski ◽  
Melania Lijadi ◽  
...  

2016 ◽  
Vol 14 (2) ◽  
pp. 022501-22505
Author(s):  
Yu Dong Yu Dong ◽  
Guanglong Wang Guanglong Wang ◽  
Haiqiao Ni Haiqiao Ni ◽  
Kangming Pei Kangming Pei ◽  
Zhongtao Qiao Zhongtao Qiao ◽  
...  

Photonics ◽  
2020 ◽  
Vol 7 (3) ◽  
pp. 76
Author(s):  
U. Zavala-Moran ◽  
M. Bouschet ◽  
J. Perez ◽  
R. Alchaar ◽  
S. Bernhardt ◽  
...  

In this paper, a full set of structural, optical and electrical characterizations performed on midwave infrared barrier detectors based on a Ga-free InAs/InAsSb type-II superlattice, grown by molecular beam epitaxy (MBE) on a GaSb substrate, are reported and analyzed. a Minority carrier lifetime value equal to 1 µs at 80 K, carried out on dedicated structure showing photoluminescence peak position at 4.9 µm, is extracted from a time resolved photoluminescence measurement. Dark current density as low as 3.2 × 10−5 A/cm2 at 150 K is reported on the corresponding device exhibiting a 50% cut-off wavelength around 5 µm. A performance analysis through normalized spectral response and dark current density-voltage characteristics was performed to determine both the operating bias and the different dark current regimes.


Photonics ◽  
2020 ◽  
Vol 7 (3) ◽  
pp. 68
Author(s):  
Arash Dehzangi ◽  
Donghai Wu ◽  
Ryan McClintock ◽  
Jiakai Li ◽  
Alexander Jaud ◽  
...  

In this letter, we report the demonstration of a pBn planar mid-wavelength infrared photodetectors based on type-II InAs/InAs1−xSbx superlattices, using silicon ion-implantation to isolate the devices. At 77 K the photodetectors exhibited peak responsivity of 0.76 A/W at 3.8 µm, corresponding to a quantum efficiency, without anti-reflection coating, of 21.5% under an applied bias of +40 mV with a 100% cut-off wavelength of 4.6 µm. With a dark current density of 5.21 × 10−6 A/cm2, under +40 mV applied bias and at 77 K, the photodetector exhibited a specific detectivity of 4.95 × 1011 cm·Hz1/2/W.


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