首页> 外文期刊>Chemistry of Materials: A Publication of the American Chemistry Society >Phase-Change Behavior and Nonlinear Optical Second and Third Harmonic Generation of the One-Dimensional K(l-x)CsXPSe6 and Metastable beta-CsPSe6
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Phase-Change Behavior and Nonlinear Optical Second and Third Harmonic Generation of the One-Dimensional K(l-x)CsXPSe6 and Metastable beta-CsPSe6

机译:一维K(l-x)CsXPSe6和亚稳β-CsPSe6的相变行为和非线性光学二次谐波和三次谐波生成

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摘要

The APSe(6) (A = K, K(1-x)Csx, Cs) family of one-dimensional (1D) materials was studied to examine the effects of the cation size on the nonlinear optical (NLO) response. The family has high-performing NLO properties with the noncentrosymmetric parent material, KPSe6, having infinite 1D chains of 1/(infinity)[PSe6-]. This structure has been successfully substituted with cesium up to K0.6Cs0.4PSe6 while retaining the polar character. All compounds crystallize in the space group Pca2(1) and have band gaps of 2.1 eV. In situ powder X-ray diffraction experiments using synchrotron radiation were used to determine the specifics of the amorphous to crystalline behavior and the crystallization and melting kinetics of the APSe(6) system. These measurements revealed a new phase, beta-CsPSe6, which is metastable and crystallizes in the noncentrosymmetric tetragonal space group P (4) over bar2(1)c with a = 12.526(2) angstrom, c = 12.781(3) angstrom, V = 2005.3(6) angstrom(3), and Z = 8. The structure is composed of 2 sets of mutually perpendicular 1/8[PSe6-] chains charge-balanced by Cs cations, and the band gap of beta-CsPSe6 is 1.9 eV. Second harmonic generation (SHG) measurements demonstrate that substitution of Cs into KPSe6 maintains the strong NLO signal with a very high SHG coefficient (chi((2))) of similar to 150 pm/V for K(1-x)CsxPSe6 and 30 pm/V for beta-CsPSe6. Laser-induced damage threshold analysis reveals APSe(6) exhibits two-photon absorption (2PA) at 1064 nm with input laser intensity greater than 1 GW/cm(2) and optical damage from 2PA at similar to 2 GW/cm(2). The materials also exhibit strong third harmonic generation (THG) with THG coefficients (chi((3)) x 10(5)) for KPSe6, K0.6Cs0.4PSe6, alpha-CsPSe6, and beta-CsPSe6 to be 2.6, 3.1, 1.8, and 1.1 pm(2)/V-2, respectively.
机译:研究了一维(1D)材料的APSe(6)(A = K,K(1-x)Csx,Cs)系列,以研究阳离子尺寸对非线性光学(NLO)响应的影响。该家族具有高性能的NLO属性,非中心对称的母体材料KPSe6具有1 /(无穷大)[PSe6-]的无限一维链。此结构已成功被铯取代为K0.6Cs0.4PSe6,同时保留了极性特征。所有化合物在空间群Pca2(1)中结晶,带隙为2.1 eV。使用同步加速器辐射的原位粉末X射线衍射实验用于确定非晶态对晶体行为以及APSe(6)系统的结晶和熔融动力学的特征。这些测量结果揭示了一个新相beta-CsPSe6,它在bar2(1)c上的非定心四方空间群P(4)中是亚稳态的,且结晶为a = 12.526(2)埃,c = 12.781(3)埃,V = 2005.3(6)埃(3),Z =8。该结构由2组相互垂直的1/8 [PSe6-]链组成,这些链通过Cs阳离子进行电荷平衡,β-CsPSe6的带隙为1.9。 eV。二次谐波生成(SHG)测量表明,将Cs替换为KPSe6可以保持强大的NLO信号,并且具有非常高的SHG系数(chi((2))),对于K(1-x)CsxPSe6和30而言,类似于150 pm / V beta-CsPSe6的pm / V。激光诱导的损伤阈值分析显示,APSe(6)在1064 nm处表现出双光子吸收(2PA),输入激光强度大于1 GW / cm(2),而2PA的光学损伤接近2 GW / cm(2) 。对于KPSe6,K0.6Cs0.4PSe6,α-CsPSe6和beta-CsPSe6,这些材料还表现出较强的三次谐波(THG),THG系数(chi((3))x 10(5))为2.6、3.1,分别为1.8和1.1 pm(2)/ V-2。

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