Abstract

We have used the envelope function formalism to investigate the bands structure of LWIR type II SL InAs(d1=2.18d2)/In0.25Ga0.75Sb(d2=21.5A). Thus, we extracted optical and transport parameters as the band gap, cut off wavelength, carriers effective mass, Fermi level and the density of state. Our results show that the higher optical cut-off wavelength can be achieved with smaller layer thicknesses. The semiconductor-semi metal transition was studied as a function of temperature. Our results permit us the interpretations of Hall and Shubnikov-de Haas effects. These results are in agreement with experimental results in literature and a guide for engineering infrared detectors.

Highlights

  • There are a several efforts in developing infrared materials for Very Long Wavelength Infrared (VLWIR) photodetection with the optical cut-off wavelengths λc ≥ 7.5 μm in the atmospheric window

  • The key lies in the fact that by increasing indium composition in In1−xGaxSb layer, the corresponding lattice constant increases

  • We note that in the previous years, a very few works were reported to verify the theoretical performance of InAs/InGaSb SLs for LWIR and VLWIR photodetection

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Summary

INTRODUCTION

There are a several efforts in developing infrared materials for Very Long Wavelength Infrared (VLWIR) photodetection with the optical cut-off wavelengths λc ≥ 7.5 μm in the atmospheric window. InAs/In1−xGaxSb type-II superlattices (SLs) are still the most promising candidate In this area, Smith and Mailhiot [1] have shown that this material system provides distinctive advantages suitable for VLWIR photodetection. The theory of band structure is necessary for describing the effects of external excitations on transport parameters and properties of optoelectronics devices [5] Owing to this lack of studies, we have investigated the bands structure of presented LWIR type II SL InAs (d1 = 47 Å)/Ga0.75In0.25Sb(d2 = 21.5 Å) with d1/d2 = 2.186 along the wave vector kz in the growth. In each host material and for a given energy, the two–band Kane model [10] gives the wave vector (k2i + k2p).

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