A 2D Double Perovskite Based on the Chiral Cystaminium Cation Exhibiting Multiple Switches in Quadratic Nonlinear Optical Response

化学 卤化物 二次方程 非线性系统 相(物质) 非线性光学 化学物理 二次谐波产生 相变 钙钛矿(结构) 密度泛函理论 手性(物理) 带隙 凝聚态物理 航程(航空) 大气温度范围 谐波 领域(数学) 非线性光学 分子物理学 理论(学习稳定性) 固态 结构稳定性 极地的 计算化学 化学稳定性 结晶学
作者
Maria Maniadi,Nicolas Mercier,Alexandre Abhervé,Denis Gindre,Elodie Tailleur,Sébastien Pillet,Valérie Dupray,Christos Tyrpenou,George Volonakis
出处
期刊:Journal of the American Chemical Society [American Chemical Society]
卷期号:147 (44): 40708-40718 被引量:3
标识
DOI:10.1021/jacs.5c13444
摘要

High Resolution Image Download MS PowerPoint Slide Over the past decade, double halide perovskites with 2D structural architectures have emerged as a promising alternative to lead-based halide perovskites in the field of semiconductors, motivated by the need to reduce the use of toxic metals. In this work, we present an example of a new 2D lead-free compound, (Cyst) 2 AgSbBr 8, exhibiting switchable nonlinear (SHG, second harmonic generation) optical properties. The use of the cystaminium cation (Cyst 2+ ) which exhibits helical chirality (M and P conformations) helped in inducing phase transitions due to conformational interconversion in the solid state. Four structural phases p 1–4 have been identified in the room temperature (RT/20 °C)–120 °C range. The I (SHG) = f ( T ) curve defines an unprecedented hysteretic behavior with a SHG OFF state at low ( T < 4 °C) and high ( T > 50 °C) temperature, while in the 4 °C–50 °C temperature range, both SHG(OFF) and (ON) states can occur as a result of the existence of the SHG-inactive p 1 phase and the SHG-active p 2 phase. The temperature range around RT for which these two phases are stable is also unprecedented. This allows to store hidden information at RT, which can be erased either by heating ( T > 50 °C) or cooling ( T < 4 °C) leading to all SHG(ON) or SHF(OFF) domains at RT, respectively. Density Functional Theory (DFT) calculations showed a direct band gap for the all phases. Calculations for the relative stability of the different phases confirmed that p 1 is the most thermodynamically stable phase, with p 2 located slightly higher in energy.
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