首页> 外文会议>2019年第66回応用物理学会春季学術講演会講演予稿集 >Time-Resolved Photoluminescence Measurement of One-Dimensional Lead Bromide Organic- Inorganic Hybrid Perovskites
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Time-Resolved Photoluminescence Measurement of One-Dimensional Lead Bromide Organic- Inorganic Hybrid Perovskites

机译:一维溴化铅有机-无机杂化钙钛矿的时间分辨光致发光测量

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One-dimensional (1D) lead halide hybrid perovskites are attractive materials because they areexpected to show high and fast optical nonlinear effects owing to the enhanced electron density ofstates and electron-phonon interaction. The 1D perovskites are a low dimensional class of hybridperovskites in which octahedrons are connected in a chain and surrounded by organic cations. Thus,they can be considered as the crystalline bulk assemblies of 1D quantum confined materials. In ourprevious report, the structural dependence of the photoluminescence spectra of 1D lead bromideperovskites with three different structures was examined, where broadband luminescence due to selftrappedexcitons was observed in all the materials. To understand the detailed mechanism of thephotoluminescence we performed the time-resolved photoluminescence (PL) measurements of 1D leadbromide hybrid perovskite crystals with 4-ethylpyridine organic molecules. The orange curve in Fig. 1shows the photoluminescence spectrum of the specimen at 300 K. The absorption spectrum is alsopresented as a blue curve, showing that the absorption edge is around 3.4 eV. The luminescencelooked yellow and the spectrum was very broad with a large Stokes shift, which are characteristic forluminescence from self-trapped excitons (STE). In addition, at a temperature the same decay profileswere observed for the peak at 2.0 eV (620 nm) and 1.9, 1.8 eV, indicating that the photoluminescenceof the specimen due to STE with single nature. Fig. 2 depicts the decay profiles at the peak around 2.0eV at temperatures of 5, 100, and 200 K. As seen from the figure the experimental data were wellfitted using a single-exponential function: I(t)=I_(0exp)( t/τ), where I is the phosphorescence intensity,I_0 is the constants, and τ is the decay constant. As temperature increases the decay constant decreases,which were 4.9, 3.6, and 0.8 μs, at 5, 100, and 200 K, respectively. This behavior is similar to other 1Dlead halide perovskites.
机译:一维(1D)卤化铅杂钙钛矿是有吸引力的材料,因为它们是 由于增强的电子密度,有望显示出高而快速的光学非线性效应 态和电子-声子相互作用。一维钙钛矿是一种低维杂化体 钙钛矿,其中八面体成链连接,并被有机阳离子包围。因此, 它们可以被认为是一维量子约束材料的结晶体组装体。在我们的 以前的报告,一维溴化铅的光致发光光谱的结构依赖性 研究了具有三种不同结构的钙钛矿,其中由于自陷而导致宽带发光 在所有材料中均观察到激子。了解详细的机制 光致发光我们对一维铅进行了时间分辨光致发光(PL)测量 溴化物与4-乙基吡啶有机分子杂化的钙钛矿晶体。图1中的橙色曲线 显示了在300 K下样品的光致发光光谱。吸收光谱也为 呈现为蓝色曲线,表明吸收边约为3.4 eV。发光度 看起来是黄色的,光谱很宽,斯托克斯位移很大,这对于 自陷激子(STE)的发光。此外,在相同温度下的衰减曲线 在2.0 eV(620 nm)和1.9,1.8 eV处观察到峰,表明光致发光 由于STE具有单一性质而导致的样本数量。图2描绘了在2.0左右的峰值处的衰减曲线 eV在5、100和200 K的温度下。从图中可以看出,实验数据很好 使用单指数函数拟合:I(t)= I_(0exp)(t /τ),其中I是磷光强度, I_0是常数,τ是衰减常数。随着温度的升高,衰减常数减小, 在5、100和200 K时分别为4.9、3.6和0.8μs。此行为类似于其他1D 卤化钙钛矿。

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