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  • Access by Xinjiang University

Optical Absorption in Pure Single Crystal InSb at 298° and 78°K

S. W. Kurnick* and John M. Powell

  • Chicago Midway Laboratories, University of Chicago, Chicago, Illinois

  • *Present address: John Jay Hopkins Laboratory for Pure and Applied Science, General Atomic Division of General Dynamics Corporation, San Diego, California.
  • Now at Raulind Corporation, Chicago, Illinois.

Phys. Rev. 116, 597 – Published 1 November, 1959

DOI: https://doi.org/10.1103/PhysRev.116.597

Abstract

The absorption spectra of single crystal homogeneous InSb were measured in the spectral range 5 to 10 microns at temperatures of 78°K and 298°K. Primary emphasis was placed on the precise determination of absorption coefficients less than 400 cm1. Absorption spectra were measured in many samples over the following range of impurity concentrations. Net impurity concentrations, expressed in atoms cm3, ranged from 5×1015 to 9.5×1016 in p-type samples, and from 2×1015 to 3×1017 in n-type samples, as determined from Hall coefficients measured at 78°K.

In general, the spectral range covered included regions where the absorption was dominated by either free-carrier absorption or valence-conduction band transitions. Free-carrier absorption in p-type InSb indicates a simple valence-band structure about k=0, consisting of light and heavy hole bands. Free carrier cross sections at 298°K are σp=8.65×1016 cm2 per hole and σn=0.23×1016 cm2 per electron (at 9 μ). Whereas the free hole absorption coefficient is roughly independent of wavelength, the free electron absorption σn varies as λ2 and agrees well with the classical Zener-Drude model.

The main absorption edge at both temperatures may be extended to lower absorption coefficients α by subtracting the extrapolated free carrier absorption coefficients αc. The resultant band edge ln(ααc) values when plotted against the photoenergy (ω) fits a straight line. The slopes of these band edges increase at the lower temperature and decrease (either at 78° or 298°K) as the acceptor concentration in the optical sample increases. Various models previously proposed are compared with the experimental results.

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