In2O3 gap states in amorphous and poly-crystalline phases: Band tail and defect level characterization by subgap photocurrent spectroscopy

A nanometer-thick indium oxide (In2O3) layer is studied in terms of gap states, by means of subgap photocurrent spectroscopy. The In2O3 layer is prepared by atomic layer deposition, where its nanostructure is changed from an amorphous to poly-crystalline phase, via changing the layer thickness. Two groups of gap states are distinguished: shallow and deep levels, reflecting the valence band (VB) tail and a specific type of defects, respectively. The VB tail is clearly broadened for the amorphous phase, where the broadening is characterized by the Urbach energy, e.g., 326 ±30 meV. The deep-level defect states are recognized at ≈ 2.3 eV from the conduction band edge, with a distribution of ≲110 meV. Interestingly, the energy level and distribution are not strongly changed, regardless of an amorphous or poly-crystalline structure.

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Publication Details

Journal
Applied Physics Letters
Published
2025-11-03
DOI
https://doi.org/10.1063/5.0276910
Citations
1
Primary Topic
ZnO doping and properties
Type
article
Field-Weighted Citation Impact
0.52
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article

In2O3 gap states in amorphous and poly-crystalline phases: Band tail and defect level characterization by subgap photocurrent spectroscopy

Tatsuro Maeda, Shota Nunomura, Hitoshi Tampo, Chia-Tsong Chen
1 citations
Applied Physics Letters
ZnO doping and properties
0.52
article

In2O3 gap states in amorphous and poly-crystalline phases: Band tail and defect level characterization by subgap photocurrent spectroscopy

Tatsuro Maeda, Shota Nunomura, Hitoshi Tampo, Chia-Tsong Chen
article en
1 citations

Abstract

A nanometer-thick indium oxide (In2O3) layer is studied in terms of gap states, by means of subgap photocurrent spectroscopy. The In2O3 layer is prepared by atomic layer deposition, where its nanostructure is changed from an amorphous to poly-crystalline phase, via changing the layer thickness. Two groups of gap states are distinguished: shallow and deep levels, reflecting the valence band (VB) tail and a specific type of defects, respectively. The VB tail is clearly broadened for the amorphous phase, where the broadening is characterized by the Urbach energy, e.g., 326 ±30 meV. The deep-level defect states are recognized at ≈ 2.3 eV from the conduction band edge, with a distribution of ≲110 meV. Interestingly, the energy level and distribution are not strongly changed, regardless of an amorphous or poly-crystalline structure.

Applied Physics LettersVol. 127(18)
National Institute of Advanced Industrial Science and Technology (JP)
Openalex Percentile: Top 31%
ZnO doping and properties
0.52
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