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Ge C, Liu Z, Zhu Y, Zhou Y, Jiang B, Zhu J, Yang X, Zhu Y, Yan S, Hu H, Song H, Li L, Chen C, Tang J. Insight into the High Mobility and Stability of In 2 O 3 :H Film. SMALL (WEINHEIM AN DER BERGSTRASSE, GERMANY) 2024; 20:e2304721. [PMID: 37670209 DOI: 10.1002/smll.202304721] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/05/2023] [Revised: 08/26/2023] [Indexed: 09/07/2023]
Abstract
Wide bandgap semiconductors, particularly In2 O3 :Sn (ITO), are widely used as transparent conductive electrodes in optoelectronic devices. Nevertheless, due to the strohave beenng scattering probability of high-concentration oxygen vacancy (VO ) defects, the mobility of ITO is always lower than 40 cm2 V-1 s-1 . Recently, hydrogen-doped In2 O3 (In2 O3 :H) films have been proven to have high mobility (>100 cm2 V-1 s-1 ), but the origin of this high mobility is still unclear. Herein, a high-resolution electron microscope and theoretical calculations are employed to investigate the atomic-scale mechanisms behind the high carrier mobility in In2 O3 :H films. It is found that VO can cause strong lattice distortion and large carrier scattering probability, resulting in low carrier mobility. Furthermore, hydrogen doping can simultaneously reduce the concentration of VO , which accounts for high carrier mobility. The thermal stability and acid-base corrosion mechanism of the In2 O3 :H film are investigated and found that hydrogen overflows from the film at high temperatures (>250 °C), while acidic or alkaline environments can cause damage to the In2 O3 grains themselves. Overall, this work provides insights into the essential reasons for high carrier mobility in In2 O3 :H and presents a new research approach to the doping and stability mechanisms of transparent conductive oxides.
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Affiliation(s)
- Ciyu Ge
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Zunyu Liu
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Yongchen Zhu
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Yilong Zhou
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Borui Jiang
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Jiaxing Zhu
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Xuke Yang
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Yongxin Zhu
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Shuyu Yan
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Haojun Hu
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Haisheng Song
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Luying Li
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
| | - Chao Chen
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
- Optics Valley Laboratory, Hubei, 430074, P. R. China
| | - Jiang Tang
- Wuhan National Laboratory for Optoelectronics (WNLO) and School of Optical and Electronic Information (SOEI), Huazhong University of Science and Technology, Wuhan, Hubei, 430074, P. R. China
- Optics Valley Laboratory, Hubei, 430074, P. R. China
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Yu J, Wang Y, Huang Y, Wang X, Guo J, Yang J, Zhao H. Structural and electronic properties of SnO 2 doped with non-metal elements. BEILSTEIN JOURNAL OF NANOTECHNOLOGY 2020; 11:1321-1328. [PMID: 32953376 PMCID: PMC7476588 DOI: 10.3762/bjnano.11.116] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 06/02/2020] [Accepted: 08/09/2020] [Indexed: 06/11/2023]
Abstract
Crystal structure and electronic properties of SnO2 doped with non-metal elements (F, S, C, B, and N) were studied using first-principles calculations. The theoretical results show that doping of non-metal elements cannot change the structure of SnO2 but result in a slight expansion of the lattice volume. The most obvious finding from the analysis is that F-doped SnO2 has the lowest defect binding energy. The doping with B and S introduced additional defect energy levels within the forbidden bandgap, which improved the crystal conductivity. The Fermi level shifts up due to the doping with B, F, and S, while the Fermi level of SnO2 doped with C or N has crossed the impurity level. The Fermi level of F-doped SnO2 is inside the conduction band, and the doped crystal possesses metallicity. The optical properties of SnO2 crystals doped with non-metal elements were analyzed and calculated. The SnO2 crystal doped with F had the highest reflectivity in the infrared region, and the reflectance of the crystals doped with N, C, S, and B decreased sequentially. Based on this theoretical calculations, F-doped SnO2 is found to be the best photoelectric material for preparing low-emissivity coatings.
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Affiliation(s)
- Jianyuan Yu
- College of Materials Science and Engineering, Yanshan University, Qinhuangdao 066004, China
- Department of Environmental and Chemical Engineering, Tangshan University, Tangshan, Hebei 063000, China
- Graphene Application Technology Tangshan Public Service Platform, Tangshan, Hebei 063000, China
| | - Yingeng Wang
- College of Materials Science and Engineering, Yanshan University, Qinhuangdao 066004, China
| | - Yan Huang
- Department of Environmental and Chemical Engineering, Tangshan University, Tangshan, Hebei 063000, China
- Graphene Application Technology Tangshan Public Service Platform, Tangshan, Hebei 063000, China
| | - Xiuwen Wang
- Department of Environmental and Chemical Engineering, Tangshan University, Tangshan, Hebei 063000, China
- Graphene Application Technology Tangshan Public Service Platform, Tangshan, Hebei 063000, China
| | - Jing Guo
- Graphene Application Technology Tangshan Public Service Platform, Tangshan, Hebei 063000, China
- School of Civil Engineering, Tangshan University, Tangshan, Hebei 063000, China
| | - Jingkai Yang
- College of Materials Science and Engineering, Yanshan University, Qinhuangdao 066004, China
- State Key Laboratory of Metastable Materials Science and Technology, China
| | - Hongli Zhao
- College of Materials Science and Engineering, Yanshan University, Qinhuangdao 066004, China
- State Key Laboratory of Metastable Materials Science and Technology, China
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Bhawna, Gupta A, Kumar P, Tyagi A, Kumar R, Kumar A, Singh P, Singh RP, Kumar V. Facile Synthesis of N‐Doped SnO
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Nanoparticles: A Cocatalyst‐Free Promising Photocatalyst for Hydrogen Generation. ChemistrySelect 2020. [DOI: 10.1002/slct.202001301] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/09/2023]
Affiliation(s)
- Bhawna
- Department of Chemistry, Kirori Mal CollegeUniversity of Delhi India
- Department of ChemistryUniversity of Delhi India
| | - Akanksha Gupta
- Department of Chemistry, Sri Venkateswara CollegeUniversity of Delhi India
| | - Prashant Kumar
- Department of Metallurgical Engineering and Material ScienceIndian Institute of Technology Bombay, Powai Mumbai India
| | - Adish Tyagi
- Chemistry DivisionBhabha Atomic Research Centre (BARC) Mumbai India
| | - Ravinder Kumar
- Department of ChemistryGurukula Kangri Vishwavidyalaya Haridwar India
| | - Ashwani Kumar
- Nanoscience Laboratory Institute CentreIndian Institute of Technology Roorkee India
| | - Prashant Singh
- Department of ChemistryAtma Ram Sanatan Dharma College, Delhi University New Delhi India
| | - R. P. Singh
- Department of Chemistry, Sri Venkateswara CollegeUniversity of Delhi India
| | - Vinod Kumar
- Department of Chemistry, Kirori Mal CollegeUniversity of Delhi India
- Special Centre for Nano SciencesJawaharlal Nehru University Delhi India
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