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溅射镀膜TiO薄膜作为钝化和空穴传输层用于改进太阳能燃料WO/CuWO光阳极的能量转换

Sputter-Coated TiO Films as Passivation and Hole Transfer Layers for Improved Energy Conversion with Solar Fuel WO/CuWO Photoanodes.

作者信息

Escaliante Lucas Caniati, Azevedo Neto Nilton Francelosi, Mendoza Hervin Errol, Xiao Chengcan, Kandel Rajesh, da Silva Jose Humberto Dias, Osterloh Frank E

机构信息

School of Sciences, Graduate Program in Materials Science and Technology─POSMAT, Universidade Estadual Paulista─UNESP, Avenida Engenheiro Luis Edmundo Carrijo Coube, 14-01, Bauru, São Paulo 17033-360, Brazil.

Plasma and Processes Laboratory, Instituto Tecnológico de Aeronáutica─ITA, Praça Marechal Eduardo Gomes, 50, São José dos Campos, São Paulo 12228-900, Brazil.

出版信息

ACS Appl Mater Interfaces. 2024 Dec 18;16(50):69229-69238. doi: 10.1021/acsami.4c14214. Epub 2024 Dec 3.

Abstract

Atomic-layer-deposited (ALD) "leaky" TiO has gained interest as a charge-selective protection layer for semiconductor solar fuel electrodes. Here, the use of sputter-deposited TiO layers as hole-selective contacts for WO/CuWO type-2 heterojunction water oxidation photoanodes is demonstrated for the first time. TiO protection layers with varying thicknesses (2 to 128 nm) were deposited by using the radio frequency (RF) magnetron sputtering technique. The resulting TiO films are amorphous as evidenced by Raman spectroscopy and powder X-ray diffraction (XRD). Photoelectrochemical scans and vibrating Kelvin probe photovoltage spectroscopy show that 2-8 nm TiO layers nearly double the photocurrent to 0.97 mA cm under AM1.5 illumination (19% AQE at 350 nm), increase the surface photovoltage signal by 25%, and increase the WO/CuWO effective band gap. These outcomes can be attributed to the selectivity of TiO for photoholes. Additionally, SPV data suggest that TiO overlayers suppress copper-based surface recombination defects. Reduced photocurrents and photovoltages are measured in thicker TiO films (16 to 128 nm) as a result of an increasing hole transfer resistance and because of light shading effects according to photoaction spectra. The TiO films also improve the stability of the WO/CuWO photoelectrodes, allowing nearly constant O evolution over 3 h after an initial 20-35% loss. Overall, this work establishes RF magnetron sputtering as a useful method to install amorphous TiO passivation layers for improved WO/CuWO solar fuel photoelectrodes. Furthermore, we show how the combination of PEC and SPV measurements provides insight into the function of the TiO coatings.

摘要

原子层沉积(ALD)的“漏电流型”TiO作为半导体太阳能燃料电极的电荷选择性保护层受到了关注。在此,首次展示了使用溅射沉积的TiO层作为WO/CuWO 2型异质结水氧化光阳极的空穴选择性接触。通过射频(RF)磁控溅射技术沉积了不同厚度(2至128纳米)的TiO保护层。拉曼光谱和粉末X射线衍射(XRD)表明,所得TiO薄膜为非晶态。光电化学扫描和振动开尔文探针光电压光谱表明,在AM1.5光照下(350纳米处的外量子效率为19%),2至8纳米厚的TiO层使光电流几乎翻倍至0.97毫安/平方厘米,表面光电压信号增加25%,并增大了WO/CuWO的有效带隙。这些结果可归因于TiO对光生空穴的选择性。此外,表面光电压(SPV)数据表明,TiO覆盖层抑制了基于铜的表面复合缺陷。由于空穴转移电阻增加以及根据光电流谱的光遮蔽效应,在较厚的TiO薄膜(16至128纳米)中测量到光电流和光电压降低。TiO薄膜还提高了WO/CuWO光电极的稳定性,在初始损失20%至35%后,能在3小时内实现几乎恒定的析氧。总体而言,这项工作确立了射频磁控溅射作为一种有用的方法,可为改进的WO/CuWO太阳能燃料光电极安装非晶态TiO钝化层。此外,我们展示了光电化学(PEC)和表面光电压(SPV)测量相结合如何深入了解TiO涂层的功能。

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