Abstract

Thin (100) wafers of single crystal undoped InSb have been strength tested by plane transverse bending. The strength of the wafers (≤ 800 mm in thickness) has been shown to depend on their mechanical treatment type. If the full mechanical treatment cycle is used (grinding + chemical polishing) the strength of the InSb wafers increases twofold (from 3.0 to 6.4 kg/mm2). We show that the strength dependence on mechanical treatment type for (100) wafers is similar to that for (111) wafers, the strength of (111) wafers being 2 times higher. The roughness of the thin wafers after the full mechanical treatment cycle has been measured using contact profilometry. After the full mechanical treatment cycle the roughness of the InSb wafers Ra decreases from 0.6 to 0.04 mm leading to general surface smoothening. We have compared the strength and roughness between (100) InSb and GaAs wafers. The roughness of InSb and GaAs wafers after the full mechanical treatment cycle decreases significantly: by 10 times for InSb due to the general surface smoothening and by 3 times for GaAs (Rz from 2.4 to 0.8 mm) due to a reduction of the peak roughness component. The full mechanical treatment cycle increases the strength of InSb wafers by removing damaged layers through the sequence of operations and reducing the risk of mechanical damage development.

Highlights

  • Single crystal indium antimonide is still among the main semiconductors used for the fabrication of electronic components in a broad application field of solid state electronics, i.e., optoelectronics

  • This material is used for the fabrication of linear and array photocells operated in the 3–5 mm wavelength range that are employed as photosensitive elements in heat vision systems [1]

  • Indium antimonide focal arrays are used in special purpose devices installed in airborne navigation and precision targeting systems, antiaircraft infrared tracking heads, marine infrared detectors and unmanned aircrafts

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Summary

Introduction

Single crystal indium antimonide is still among the main semiconductors used for the fabrication of electronic components in a broad application field of solid state electronics, i.e., optoelectronics. This material is used for the fabrication of linear and array photocells operated in the 3–5 mm wavelength range that are employed as photosensitive elements in heat vision systems [1]. These heat vision systems find general application in multiple fields of economy (medicine, materials science, environmental pollution monitoring etc.).

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