P-Type Spin-Coated Sol–Gel Cr<sub>2</sub>O<sub>3</sub> Layer by Postannealing in Vacuum

The hole carriers of spin-coated sol-gel Cr<sub>2</sub>O<sub>3</sub> could be activated successfully by postannealing at a temperature of more than 500 °C in a vacuum without doping. The sheet hole concentration increased with the increase in the postannealing temperature and could reach 5 × 10<sup>14</sup> cm<sup>-2</sup> at a postannealing temperature of 680 °C. However, activating the hole carriers for annealing Cr<sub>2</sub>O<sub>3</sub> in N<sub>2</sub> ambient at a low pressure of 3 mTorr and a temperature of 560 °C or higher was difficult. The N<sub>2</sub>-annealed Cr<sub>2</sub>O<sub>3</sub> could regain the same electrical properties as vacuum-annealed Cr<sub>2</sub>O<sub>3</sub> by annealing under vacuum again. A comparison of the deconvoluted XPS spectra of the postannealed Cr<sub>2</sub>O<sub>3</sub> in a vacuum and in N<sub>2</sub> ambient showed that the amount of Cr<sup>2+</sup>, Cr<sup>4+</sup>, Cr<sup>5+</sup>, Cr<sup>6+</sup>, and O vacancies was strongly correlated with the hole carrier creation of Cr<sub>2</sub>O<sub>3</sub>.

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Publication Details

Journal
ACS Omega
Published
2025-08-05
DOI
https://doi.org/10.1021/acsomega.5c02540
Citations
2
Primary Topic
Copper-based nanomaterials and applications
Type
article
Field-Weighted Citation Impact
1.04

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article

P-Type Spin-Coated Sol–Gel Cr2O3 Layer by Postannealing in Vacuum

Chan-Hung Hsu, Sheng-Po Chang, Wei‐Chih Lai, B. H. Wu et al.
2 citations
ACS Omega
Copper-based nanomaterials and applications
1.04
article

P-Type Spin-Coated Sol–Gel Cr2O3 Layer by Postannealing in Vacuum

Chan-Hung Hsu, Sheng-Po Chang, Wei‐Chih Lai, B. H. Wu, Shoou‐Jinn Chang, Jinn‐Kong Sheu, Po‐Han Chen, Cheng-Huang Kuo
article en
2 citations

Abstract

The hole carriers of spin-coated sol-gel Cr<sub>2</sub>O<sub>3</sub> could be activated successfully by postannealing at a temperature of more than 500 °C in a vacuum without doping. The sheet hole concentration increased with the increase in the postannealing temperature and could reach 5 × 10<sup>14</sup> cm<sup>-2</sup> at a postannealing temperature of 680 °C. However, activating the hole carriers for annealing Cr<sub>2</sub>O<sub>3</sub> in N<sub>2</sub> ambient at a low pressure of 3 mTorr and a temperature of 560 °C or higher was difficult. The N<sub>2</sub>-annealed Cr<sub>2</sub>O<sub>3</sub> could regain the same electrical properties as vacuum-annealed Cr<sub>2</sub>O<sub>3</sub> by annealing under vacuum again. A comparison of the deconvoluted XPS spectra of the postannealed Cr<sub>2</sub>O<sub>3</sub> in a vacuum and in N<sub>2</sub> ambient showed that the amount of Cr<sup>2+</sup>, Cr<sup>4+</sup>, Cr<sup>5+</sup>, Cr<sup>6+</sup>, and O vacancies was strongly correlated with the hole carrier creation of Cr<sub>2</sub>O<sub>3</sub>.

ACS OmegaVol. 10(32)
University of Science and Technology (YE), National Yang Ming Chiao Tung University (TW), Applied Photonics (United Kingdom) (GB), EM Photonics (United States) (US), Institute of Microelectronics (CN), Fraunhofer Institute for Integrated Circuits (DE), National Kaohsiung University of Science and Technology (TW), United Microelectronics (United States) (US), National Cheng Kung University (TW)
National Science and Technology Council
Affordable and clean energy
Openalex Percentile: Top 23%
Copper-based nanomaterials and applications
1.04
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