2020
DOI: 10.1063/1.5140742
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Self-trapped hole and impurity-related broad luminescence in β-Ga2O3

Abstract: Self-trapped hole and impurity-related broad luminescence in β-Ga 2 O 3

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Cited by 104 publications
(65 citation statements)
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“…It is noticeable that the UV region is fitted by two UV Gaussian peaks, because photogenerated holes can be self‐trapped by two different oxygen sites. [ 48,49 ] The ratio of the total integrated area of BL and GL to UV represents the proportion of defects in the β‐Ga 2 O 3 film. The ratio decreases with increase in the growth temperature, as shown in Figure 9b.…”
Section: Resultsmentioning
confidence: 99%
“…It is noticeable that the UV region is fitted by two UV Gaussian peaks, because photogenerated holes can be self‐trapped by two different oxygen sites. [ 48,49 ] The ratio of the total integrated area of BL and GL to UV represents the proportion of defects in the β‐Ga 2 O 3 film. The ratio decreases with increase in the growth temperature, as shown in Figure 9b.…”
Section: Resultsmentioning
confidence: 99%
“…Hybrid functional calculations show that self-trapped holes and many extrinsic defects can give rise to very broad luminescence bands 18 [Xe]4f 14 5d 5 2 T 2 (I) split by spin-orbital coupling:…”
Section: Icpmsmentioning
confidence: 99%
“…I – V characteristics in Figure 9 have a slight shift (≈−0.3 V) of current minima in the dark state, which possibly attributed to the charge trapping and de‐trapping at the metal/Ga 2 O 3 interface, a well‐known phenomenon for Ga 2 O 3 . [ 33 ] Our PDs have Schottky contacts at the front side and ohmic at the backside. When PDs are under the forward bias or UV illumination, before measuring the dark current, the holes may trap near the Schottky junction via self‐trapping [ 33 ] and or at deep level acceptor states.…”
Section: Resultsmentioning
confidence: 99%
“…[ 33 ] Our PDs have Schottky contacts at the front side and ohmic at the backside. When PDs are under the forward bias or UV illumination, before measuring the dark current, the holes may trap near the Schottky junction via self‐trapping [ 33 ] and or at deep level acceptor states. This may be the reason why we observe the shift in the I – V measurements for some devices, because the density of deep level acceptor levels is not the same for all the samples.…”
Section: Resultsmentioning
confidence: 99%