Chen Zhihui, Zhang Qi, Zhu Menglong, Chen Hao, Wang Xinyun, Xiao Si, Loh Kian Ping, Eda Goki, Meng Jianqiao, He Jun
Hunan Key Laboratory of Nanophononics and Devices, School of Physics and Electronics, Central South University, 932 South Lushan Road, Changsha, Hunan 410083, P.R. China.
Department of Physics, National University of Singapore, 2 Science Drive 3, 117542, Singapore.
J Phys Chem Lett. 2021 Jul 29;12(29):7010-7018. doi: 10.1021/acs.jpclett.1c01890. Epub 2021 Jul 21.
Two-dimensional (2D) organic-inorganic hybrid perovskites (OIHPs) with superior nonlinear optical (NLO) properties show great versatility in frequency upconversion applications. Optical anisotropy plays an indispensable role in interpreting the interactions between incoming photons and crystal structure. Recently, the in-plane anisotropic NLO properties of 2D OIHPs have been reported and attracted much attention. However, the structure-related NLO anisotropy of the 2D OIHP framework is not well-established. Here, NLO properties of (CH(CH)NH)PbI (PEPI), (CHNH)PbI (C6H11), and (CHNH)PbI (C4PI) were systematically studied to interrogate the correlation between the in-plane anisotropic NLO responses and its lattice structure. In-plane nonparametric NLO responses, e.g., two-photon photoluminescence (2PPL) and three-photon photoluminescence (3PPL), manifest similar anisotropy configurations for PEPI, C6H11, and C4PI regardless of aromatic, cyclic, or linear organic molecules; however, the anisotropies of THG signals are strongly dependent on the specific crystal structures of the individual flakes, and they are much higher than that of the multiphoton excited photoluminescence.
具有卓越非线性光学(NLO)特性的二维(2D)有机-无机杂化钙钛矿(OIHPs)在频率上转换应用中展现出极大的通用性。光学各向异性在解释入射光子与晶体结构之间的相互作用方面发挥着不可或缺的作用。最近,二维OIHPs的面内各向异性NLO特性已被报道并引起了广泛关注。然而,二维OIHP框架中与结构相关的NLO各向异性尚未得到充分确立。在此,对(CH(CH)NH)PbI(PEPI)、(CHNH)PbI(C6H11)和(CHNH)PbI(C4PI)的NLO特性进行了系统研究,以探究面内各向异性NLO响应与其晶格结构之间的相关性。面内非参数NLO响应,例如双光子光致发光(2PPL)和三光子光致发光(3PPL),对于PEPI、C6H11和C4PI表现出相似的各向异性构型,无论其有机分子是芳香族、环状还是线性的;然而,三次谐波产生(THG)信号的各向异性强烈依赖于单个薄片的特定晶体结构,并且远高于多光子激发光致发光的各向异性。