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CsPbBr3钙钛矿单晶的制备及其光电探测器的研究
Preparation of CsPbBr3 Perovskite Single Crystal and Research on Its Photodetector

DOI: 10.12677/APP.2021.1112053, PP. 445-452

Keywords: 钙钛矿,单晶,探测器
Perovskite
, Single Crystal, Detector

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Abstract:

与有机–无机杂化钙钛矿相比,全无机钙钛矿CsPbX3 (X = Cl, Br, I)中A位不含有易于热挥发的有机阳离子,因此具有更高的稳定性。全无机钙钛矿单晶具有低的缺陷密度,高的载流子迁移率,因而被广泛地用于制备光电器件。然而传统制造CsPbBr3单晶的方法,如布里奇曼熔融法、反温度结晶和反溶剂蒸汽辅助结晶等,往往依赖于高温、复杂工艺和真空环境。而且晶体质量相对较差,存在大量缺陷,严重影响器件性能。本研究工作中,我们使用了一种两段式升温法,通过缓慢蒸发溶剂控制钙钛矿在低温高质量成核,进而升高温度快速结晶生长,最终获得高质量的CsPbBr3块状单晶。利用该CsPbBr3钙钛矿单晶构建金属–半导体–金属结构的光电探测器,该器件展现出优异的光电性能,在1 V工作电压下,器件在540 nm处的响应度为2.68 × 10?3 A?W?1,在2 V电压下,光暗电流比可达2.23 × 103。同时它展现了快速的响应时间(上升时间:8.3 μs;下降时间:684.9 μs)。
Compared with the organic-inorganic hybrid perovskite, the all-inorganic perovskite CsPbX3 (X = Cl, Br, I) don’t contain organic cations that are prone to thermal volatilization, so it has higher stability. All-inorganic perovskite single crystals have low defect density and high carrier mobility, so they are widely used to prepare optoelectronic devices. However, traditional methods for manufacturing CsPbBr3 single crystals, such as Bridgman method, inverse temperature crystallization, and anti-solvent vapor assisted crystallization, often rely on high temperatures, complex processes, and vacuum environments. Moreover, the crystal quality is relatively poor, and there are a large number of defects, which seriously affect the performance of the device. In this research, we used a two-stage heating method to control the high-quality nucleation of perovskite at low temperature by slowly evaporating the solvent, and then increasing the temperature to rapidly crystal growth, and finally obtaining high-quality CsPbBr3 bulk single crystals. The CsPbBr3 perovskite single crystal is used to construct a photodetector with a metal-semiconductor-metal structure. The device exhibits excellent photoelectric performance. Under a bias of 1 V, the response of the device at 540 nm is 2.68 × 10?3 A?W?1. Under the bias of 2 V, the ratio of light to dark current is 2.23 × 103. At the same time, it exhibits a fast response time (rise time: 8.3 μs; fall time: 684.9 μs).

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