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用于增强p型CuO光阴极电荷传输的最佳n型Al掺杂ZnO覆盖层

Optimal n-Type Al-Doped ZnO Overlayers for Charge Transport Enhancement in p-Type CuO Photocathodes.

作者信息

Lee Hak Hyeon, Kim Dong Su, Choi Ji Hoon, Kim Young Been, Jung Sung Hyeon, Sarker Swagotom, Deshpande Nishad G, Suh Hee Won, Cho Hyung Koun

机构信息

School of Advanced Materials Science and Engineering, Sungkyunkwan University, 2066 Seobu-ro, Jangan-gu, Suwon, Gyeonggi-do 16419, Korea.

Research Center for Advanced Materials Technology, Sungkyunkwan University, 2066 Seobu-ro, Jangan-gu, Suwon, Gyeonggi-do 16419, Korea.

出版信息

Micromachines (Basel). 2021 Mar 22;12(3):338. doi: 10.3390/mi12030338.

DOI:10.3390/mi12030338
PMID:33810027
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8004703/
Abstract

An effective strategy for improving the charge transport efficiency of p-type CuO photocathodes is the use of counter n-type semiconductors with a proper band alignment, preferably using Al-doped ZnO (AZO). Atomic layer deposition (ALD)-prepared AZO films show an increase in the built-in potential at the CuO/AZO interface as well as an excellent conformal coating with a thin thickness on irregular CuO. Considering the thin thickness of the AZO overlayers, it is expected that the composition of the Al and the layer stacking sequence in the ALD process will significantly influence the charge transport behavior and the photoelectrochemical (PEC) performance. We designed various stacking orders of AZO overlayers where the stacking layers consisted of AlO (or Al) and ZnO using the atomically controlled ALD process. Al doping in ZnO results in a wide bandgap and does not degrade the absorption efficiency of CuO. The best PEC performance was obtained for the sample with an AZO overlayer containing conductive Al layers in the bottom and top regions. The CuO/AZO/TiO/Pt photoelectrode with this overlayer exhibits an open circuit potential of 0.63 V and maintains a high cathodic photocurrent value of approximately -3.2 mA cm at 0 V for over 100 min.

摘要

提高p型CuO光阴极电荷传输效率的一种有效策略是使用具有适当能带排列的反型n型半导体,最好是使用铝掺杂氧化锌(AZO)。通过原子层沉积(ALD)制备的AZO薄膜在CuO/AZO界面处的内建电位有所增加,并且在不规则的CuO上具有优异的保形涂层,厚度很薄。考虑到AZO覆盖层的薄厚度,预计ALD过程中铝的组成和层堆叠顺序将显著影响电荷传输行为和光电化学(PEC)性能。我们使用原子控制的ALD工艺设计了各种AZO覆盖层的堆叠顺序,其中堆叠层由AlO(或Al)和ZnO组成。ZnO中的铝掺杂导致宽带隙,并且不会降低CuO的吸收效率。对于底部和顶部区域含有导电Al层的AZO覆盖层样品,获得了最佳的PEC性能。具有这种覆盖层的CuO/AZO/TiO/Pt光电极在0 V时的开路电位为0.63 V,并在100多分钟内保持约-3.2 mA cm的高阴极光电流值。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/9592e368358a/micromachines-12-00338-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/47004c661325/micromachines-12-00338-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/dd5c9f3b24f7/micromachines-12-00338-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/27390d55a893/micromachines-12-00338-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/9995125f48cc/micromachines-12-00338-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/3411e03eda7c/micromachines-12-00338-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/9592e368358a/micromachines-12-00338-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/47004c661325/micromachines-12-00338-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/dd5c9f3b24f7/micromachines-12-00338-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/27390d55a893/micromachines-12-00338-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/9995125f48cc/micromachines-12-00338-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/3411e03eda7c/micromachines-12-00338-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5033/8004703/9592e368358a/micromachines-12-00338-g006.jpg

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