Advanced Functional Materials· 2026Q1
Shallow Trap States Control Electrical Performance of Amorphous Oxide Semiconductor Thin‐Film Transistors
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- Q1SCImago
- 2026year
Short summary
Shallow defect states near the conduction band mobility edge, measured by ultrabroadband photoconduction (UP‐DoS) microscopy, accurately predict the electrical performance of amorphous InGaZnO (a‐IGZO) thin‐film transistors (TFTs) without adjustable parameters.
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Key points
- Ultrabroadband photoconduction (UP‐DoS) microscopy precisely measures subgap density of states (DoS) in a‐IGZO TFTs to within 0.1 eV of the mobility edge.
- Measured subgap DoS accurately predicts TFT transfer curves, showing shallow defect states rigidly tune subthreshold swing, threshold voltage, and drift mobility.
- The dominant trap controlling performance is at 0.32 eV below the conduction band, attributed to a Ga‐Ga‐In oxygen‐vacancy defect.
- In‐enrichment studies and DFT+U simulations link observed subgap peaks to specific vacancy‐cation coordination environments.
AI-generated from the title and abstract; the full text is not read.
Abstract
ABSTRACT The performance of n ‐type amorphous oxide semiconductor thin‐film transistors (TFTs) is controlled by the electronic states near the conduction band mobility edge. Here, the full subgap density of states (DoS) of amorphous InGaZnO (a‐IGZO) TFTs, used in display panels and dynamic random‐access memory (DRAM) development, is measured by ultrabroadband photoconduction (UP‐DoS) microscopy to within 0.1 eV of the mobility edge. The measured subgap DoS for 25 TFT processing conditions accurately predicts each transfer curve, showing how shallow defect states are electron traps that rigidly tune subthreshold swing, threshold voltage, and drift mobility. For a set of TFTs, the subthreshold transfer characteristics can be simulated independently by the experimental shallow‐defect DoS, with no adjustable parameters. The full transfer curve is simulated by introducing a single parameter: the conduction band tail energy. Additionally, each simulation reveals how the shallow trap density controls subthreshold behavior and can be directly extracted from transfer curves. Finally, a systematic In‐enrichment study, combined with DFT+U DoS simulations, enables identification of vacancy‐cation coordination environments for experimentally observed subgap peaks. The dominant trap controlling conventional a‐IGZO TFT performance is centered at 0.32 eV below the conduction band mobility edge and is attributed to a Ga‐Ga‐In oxygen‐vacancy defect.
The authors' abstract, as published at the source. Advanced Functional Materials, 2026 · DOI ↗
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Field: Electrical and Electronic Engineering
Electrical and Electronic EngineeringEngineering