Circularly Polarized Luminescence Inversion in AIE-Active Crystal Enabled by Solvent-Induced Transition Dipole Moment Regulation

IF 13.7 Q1 CHEMISTRY, MULTIDISCIPLINARY
Xiaofei Niu, Xinwen Ou, Shizhe Ren, Ke Wang, Fengyan Song, Xiaobin Dong, Wu-Jie Guo, Hui-Qing Peng, Zujin Zhao, Jacky W. Y. Lam, Yong Sheng Zhao, Fei Li, Shu-Yan Yu, Ben Zhong Tang
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Abstract

Control of the dissymmetry of circularly polarized luminescence (CPL) is intriguing and has great potential for applications in the field of optics. The traditional control strategy involves using the opposite enantiomers to achieve reversal of CPL signs. However, regulating CPL reversal by controlling only the transition dipole moments without changing molecular or supramolecular chirality remains a challenge. Herein, we developed a couple of crystal materials based on axially chiral aggregation-induced emission luminogens (AIEgens). These materials exhibit achiral solvent-induced CPL sign inversion with identical helical structures and molecular chirality in their crystalline states. (R)-BPAuCzT displays (+)-CPL with a dissymmetry factor of luminescence (glum) value of +9.81 × 10−4 (560 nm), while (R)-BPAuCzC exhibits (−)-CPL with a glum value of −1.02 × 10−3 (560 nm). Time-dependent density functional theory calculations show that the magnetic and electric transition dipole moments at S1 → S0 of the (R)-BPAuCzC unit cell are considerably influenced by the cocrystallized solvent molecules, revealing a solvent-induced CPL inversion mechanism. The nonbonding interactions between the solvent molecules (i.e., tetrahydrofuran or CDCl3) and AIEgens in the crystal play a crucial role in the manipulation of the transition dipole moment of these crystal materials. Moreover, microrods of (R)-BPAuCzT, (R)-BPAuCzC, and (R)-BPAuCzDCE exhibit optical waveguide properties with relatively low optical-loss coefficients of 187.3, 567.4, and 65.2 dB/cm, respectively. These findings can help in developing a new strategy toward controlling CPL signals and providing a potential application for future integrated photonic circuits.

Abstract Image

溶剂诱导跃迁偶极矩调控使aie活性晶体圆极化发光反转
圆偏振光不对称性的控制在光学领域具有广阔的应用前景。传统的控制策略包括使用相反的对映体来实现CPL信号的逆转。然而,仅通过控制跃迁偶极矩而不改变分子或超分子手性来调节CPL反转仍然是一个挑战。在此,我们开发了几种基于轴向手性聚集诱导发射发光物质(AIEgens)的晶体材料。这些材料表现出非手性溶剂诱导的CPL符号反转,在晶体状态下具有相同的螺旋结构和分子手性。(R)-BPAuCzT显示(+)-CPL,发光不对称因子(glum)值为+9.81 × 10−4 (560 nm), (R)-BPAuCzC显示(−)-CPL,发光不对称因子(glum)值为−1.02 × 10−3 (560 nm)。随时间密度泛函理论计算表明,(R)-BPAuCzC单体胞S1→S0处的磁跃迁偶极矩和电跃迁偶极矩受到共结晶溶剂分子的显著影响,揭示了溶剂诱导的CPL反转机制。溶剂分子(即四氢呋喃或CDCl3)与晶体中的AIEgens之间的非键相互作用在这些晶体材料的过渡偶极矩的操纵中起着至关重要的作用。此外,(R)-BPAuCzT、(R)-BPAuCzC和(R)-BPAuCzDCE的微棒具有相对较低的光损耗系数,分别为187.3、567.4和65.2 dB/cm。这些发现有助于开发控制CPL信号的新策略,并为未来的集成光子电路提供潜在的应用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
17.40
自引率
0.00%
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审稿时长
7 weeks
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