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Carrier Compensation Induced by Thermal Annealing in Al-Doped ZnO Films.

作者信息

Koida Takashi, Kaneko Tetsuya, Shibata Hajime

机构信息

Research Center for Photovoltaics, National Institute of Advanced Industrial Science and Technology (AIST), Central 2, Umezono 1-1-1, Tsukuba, Ibaraki 305-8568, Japan.

School of Engineering, Tokai University, 4-1-1, Kitakaname, Hiratsuka, Kanagawa 259-1292, Japan.

出版信息

Materials (Basel). 2017 Feb 8;10(2):141. doi: 10.3390/ma10020141.

DOI:10.3390/ma10020141
PMID:28772501
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5459124/
Abstract

This study investigated carrier compensation induced by thermal annealing in sputtered ZnO:Al (Al₂O₃: 0.25, 0.5, 1.0, and 2.0 wt %) films. The films were post-annealed in a N₂ atmosphere at low (1 × 10 atm) and high (1 × 10 atm) oxygen partial pressures (). In ZnO:Al films with low Al contents (i.e., 0.25 wt %), the carrier density () began to decrease at annealing temperatures () of 600 °C at low . At higher and/or Al contents, values began to decrease significantly at lower (ca. 400 °C). In addition, Zn became desorbed from the films during heating in a high vacuum (i.e., <1 × 10⁷ Pa). These results suggest the following: (i) Zn interstitials and Zn vacancies are created in the ZnO lattice during post-annealing treatments, thereby leading to carrier compensation by acceptor-type Zn vacancies; (ii) The compensation behavior is significantly enhanced for ZnO:Al films with high Al contents.

摘要
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/9f7a356d49fe/materials-10-00141-g016.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/3ab3f6bca359/materials-10-00141-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/ac8fab8083a7/materials-10-00141-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/0cfc5f630167/materials-10-00141-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/755cae061121/materials-10-00141-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/cdb50fddf4b3/materials-10-00141-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/bd779b36a7d8/materials-10-00141-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/6252deb5e445/materials-10-00141-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/0a1317f6c65d/materials-10-00141-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/aa7353f2fc30/materials-10-00141-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/c7dfc79f8bf9/materials-10-00141-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/92e4385bc09c/materials-10-00141-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/ee291caebd3e/materials-10-00141-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/f78514de7714/materials-10-00141-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/28a141615f3e/materials-10-00141-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/c06733eda0f2/materials-10-00141-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/9f7a356d49fe/materials-10-00141-g016.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/3ab3f6bca359/materials-10-00141-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/ac8fab8083a7/materials-10-00141-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/0cfc5f630167/materials-10-00141-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/755cae061121/materials-10-00141-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/cdb50fddf4b3/materials-10-00141-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/bd779b36a7d8/materials-10-00141-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/6252deb5e445/materials-10-00141-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/0a1317f6c65d/materials-10-00141-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/aa7353f2fc30/materials-10-00141-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/c7dfc79f8bf9/materials-10-00141-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/92e4385bc09c/materials-10-00141-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/ee291caebd3e/materials-10-00141-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/f78514de7714/materials-10-00141-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/28a141615f3e/materials-10-00141-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/c06733eda0f2/materials-10-00141-g015.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/01b6/5459124/9f7a356d49fe/materials-10-00141-g016.jpg

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本文引用的文献

1
Transparent Conducting Oxides for Photovoltaics: Manipulation of Fermi Level, Work Function and Energy Band Alignment.用于光伏的透明导电氧化物:费米能级、功函数和能带排列的调控
Materials (Basel). 2010 Nov 2;3(11):4892-4914. doi: 10.3390/ma3114892.
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Hydrogenated cation vacancies in semiconducting oxides.半导体氧化物中的氢化阳离子空位。
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Dopability, intrinsic conductivity, and nonstoichiometry of transparent conducting oxides.
透明导电氧化物的可掺杂性、本征导电性和非化学计量比。
Phys Rev Lett. 2007 Jan 26;98(4):045501. doi: 10.1103/PhysRevLett.98.045501. Epub 2007 Jan 23.
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Evidence of the Zn vacancy acting as the dominant acceptor in n-type ZnO.锌空位作为n型氧化锌中主要受主的证据。
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