Ferroelectric Photovoltaic Effect

Gao Rongli, Zhenhua Wang, Fu Chunlin, C. Wei, Chen Gang, Deng Xiaoling
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引用次数: 2

Abstract

Tetragonal BiFeO 3 films with the thickness of 30 nm were grown epitaxially on (001) ori - ented LaAlO 3 substrate by using pulsed laser deposition (PLD). The transverse photovol - taic effects were studied as a function of the sample directions in-plane as well as the angle between the linearly polarized light and the plane of the sample along X and Y directions. The absorption onset and the direct band gap are ~2.25 and ~2.52 eV, respectively. The pho - tocurrent depends not only on the sample directions in-plane but also on the angle between the linearly polarized light and the plane of the sample along X and Y directions. The results indicate that the bulk photovoltaic effect together with the depolarization field was ascribed to this phenomenon. Detailed analysis presents that the polarization direction is along [110] direction and this depolarization field induced photocurrent is equal to ~3.53 μA/cm 2 . The BPV induced photocurrent can be approximate described as Jx ≈ 2.23cos(2 θ ), such an angu lar dependence of photocurrent is produced as a consequence of asymmetric microscopic processes of carriers such as excitation and recombination.
铁电光伏效应
采用脉冲激光沉积(PLD)技术在(001)纳米laalo3衬底上外延生长了厚度为30 nm的四边形bifeo3薄膜。研究了横向光电效应与样品平面内方向以及线偏振光与样品平面沿X和Y方向夹角的关系。吸收起始值和直接带隙分别为~2.25和~2.52 eV。光电流不仅与样品平面内方向有关,还与线偏振光与样品平面沿X和Y方向的夹角有关。结果表明,体光伏效应和退极化场是造成这一现象的主要原因。详细分析表明,极化方向沿[110]方向,该去极化场产生的光电流为~3.53 μA/ cm2。BPV诱导的光电流可以近似描述为Jx≈2.23cos(2 θ),这种光电流的角度依赖性是由于载流子的激发和复合等不对称微观过程产生的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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