Observation of temperature-dependent capture cross section for main deep-levels in β-Ga2O3
Direct observation of the capture cross section is challenging due to the need for extremely short filling pulses in the two-gate Deep-Level Transient Spectroscopy (DLTS). Simple estimation of the cross section can be done from DLTS and admittance spectroscopy data but it is not feasible to distingu...
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Veröffentlicht in: | Journal of applied physics 2024-07, Vol.136 (2) |
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Hauptverfasser: | , , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Direct observation of the capture cross section is challenging due to the need for extremely short filling pulses in the two-gate Deep-Level Transient Spectroscopy (DLTS). Simple estimation of the cross section can be done from DLTS and admittance spectroscopy 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-Ga2O3 that has been gathered by our group since 2017. Based on the gathered data, we propose a derivation of apparent activation energy
(
E
a
m
) and capture cross section
(
σ
n
m
) assuming the temperature dependent capture via the multiphonon emission model, which resulted in a strong correlation between
E
a
m and
σ
n
m according to the Meyer–Neldel rule, which allowed us to estimate low- and high-temperature capture coefficients
C
0 and
C
1 as well as capture barrier
E
b. It also has been shown that without considering the temperature dependence of capture cross section, the experimental values of
σ
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” (
E
a and
σ
n) considering two additional parameters (
E
M
N and
σ
00) and to verify the density functional theory computation of deep-level recombination properties. |
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ISSN: | 0021-8979 1089-7550 |
DOI: | 10.1063/5.0209322 |