Abstract

The effects of high energy neutron irradiation on the deep level defect concentration profile throughout the bandgap of β-Ga2O3 were investigated by a combination of deep level optical spectroscopy (DLOS) and deep level transient spectroscopy (DLTS). For the unintentionally doped edge-defined film-fed growth-grown (010) β-Ga2O3 substrates investigated here, it was found that the dominant effects of neutron irradiation were to produce defects detected by DLOS having energy levels of EC −1.29 eV and EC −2.00 eV, with no discernable impact on traps within ∼1 eV of the conduction band edge. Commensurate with the introduction of these states was a significant amount of net doping reduction, for which lighted capacitance-voltage studies revealed that both of these irradiation-induced deep states are responsible, likely through a compensation mechanism. The sensitivity of the EC −1.29 eV and EC −2.00 eV states on irradiation suggests an intrinsic source, and whereas the EC −2.00 eV state was already present in the as-grown material, the EC −1.29 eV state was not detected prior to irradiation. DLOS and DLTS revealed other defect states at EC −0.63 eV, EC −0.81 eV, and EC −4.48 eV, but none of these responded to neutron irradiation for two different 1 MeV equivalent fluences 8.5 × 1014 cm−2 and 1.7 × 1015 cm−2, which is consistent with the behavior expected for defect states having an extrinsic source.

Highlights

  • The substrates were processed into Schottky diode test structures consisting of an 8 nm thick, semi-transparent Ni Schottky contact and an ∼430 nm Ti/Al/Ni/Au Ohmic metal stack deposited in an ∼200 nm-deep trench exposed by BCl3-based reactive ion etching (RIE)

  • deep level optical spectroscopy (DLOS) measurements, which are based on optically stimulated emission of trapped electrons to the conduction band to observe deep levels, were used to characterize the remainder of the ∼4.8 eV bandgap not seen by deep level transient spectroscopy (DLTS)

  • We explore the specific defects created by the neutron irradiation to understand the physics of compensation

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Summary

Introduction

All investigations were performed on commercially available Tamura UID β-Ga2O3 (010) substrates grown by EFG.20 The substrates were processed into Schottky diode test structures consisting of an 8 nm thick, semi-transparent Ni Schottky contact (to allow optical penetration for DLOS) and an ∼430 nm Ti/Al/Ni/Au Ohmic metal stack deposited in an ∼200 nm-deep trench exposed by BCl3-based reactive ion etching (RIE).

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