English

Observation of Temperature-Dependent Capture Cross-Section for Main Deep-Levels in $\beta$-Ga2O3

Materials Science 2024-10-29 v1 Other Condensed Matter Applied Physics

Abstract

Direct observation of capture cross-section is challenging due to the need of extremely short filling pulses in the two-gate Deep-Level Transient Spectroscopy (DLTS). Simple estimation of cross-section can be done from DLTS and Admittance Spectroscopy (AS) data, but it is not feasible to distinguish temperature dependence of pre-exponential and exponential parts of the emission rate equation with sufficient precision conducting a single experiment. This paper presents experimental data of deep-levels in β\beta-Ga2O3 that has been gathered by our group since 2017. Based on the gathered data we propose a derivation of apparent activation energy (EamE_a^m) and capture cross-section (σnm\sigma_n^m) assuming temperature dependent capture via multiphonon emission model, which resulted in strong correlation between EamE_a^m and σnm\sigma_n^m according to Meyer-Neldel rule, which allowed us to estimate low- and high-temperature capture coefficients C0C_0 and C1C_1 as well as capture barrier EbE_b. It also has been shown that without considering the temperature dependence of capture cross-section, the experimental values of σn\sigma_n are overestimated by 1-3 orders of magnitude. A careful consideration of the data also allows to be more certain identifying deep-levels by their "fingerprints" (EaE_a and σn\sigma_n) considering two additional parameters (EMNE_{MN} and σ00\sigma_{00}) and to verify the density functional theory (DFT) computation of deep-level recombination properties.

Keywords

Cite

@article{arxiv.2410.20509,
  title  = {Observation of Temperature-Dependent Capture Cross-Section for Main Deep-Levels in $\beta$-Ga2O3},
  author = {A. A. Vasilev and A. I. Kochkova and A. Y. Polyakov and A. A. Romanov and N. R. Matros and L. A. Alexanyan and I. V. Shchemerov and S. J. Pearton},
  journal= {arXiv preprint arXiv:2410.20509},
  year   = {2024}
}