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双重态-单重态发射中的自旋多重性效应:单个电子的光物理结果。

Spin multiplicity effects in doublet singlet emission: the photophysical consequences of a single electron.

作者信息

Wehrmann Caleb M, Imran Muhammad, Pointer Craig, Fredin Lisa A, Young Elizabeth R, Chen Mark S

机构信息

Department of Chemistry, Lehigh University Bethlehem PA 18015 USA

出版信息

Chem Sci. 2020 Sep 10;11(37):10212-10219. doi: 10.1039/d0sc04211k.

Abstract

Ambient-stable fluorescent radicals have recently emerged as promising luminescent materials; however, tailoring their properties has been difficult due to the limited photophysical understanding of open-shell organic systems. Here we report the experimental and computational analysis of a redox pair of π-conjugated fluorescent molecules that differ by one electron. A π-dication () and π-radical cation () demonstrate different absorption spectra, but similar red emission ( = ∼630 nm), excitation maxima ( = ∼530 nm), fluorescence lifetimes (1-10 ns), and even excited-state (non-emissive) lifetimes when measured by transient absorption spectroscopy. Despite their experimental similarities, time-dependent density functional theory (TDDFT) studies reveal that and emission mechanisms are distinct and rely on different electronic transitions. Excited-state reorganization occurs by hole relaxation in singlet , while doublet undergoes a Jahn-Teller distortion by bending its π-backbone in order to facilitate spin-pairing between singly occupied molecular orbitals. This relationship between the excited-state dynamics of and its π-backbone geometry illustrates a potential strategy for developing π-conjugated radicals with new emission properties. Additionally, by comparing TDDFT and CIS (configuration interaction singles) excitations, we show that unrestricted TDDFT accurately reproduces experimental absorption spectra and provides an opportunity to examine the relaxed excited-state properties of large open-shell molecules like .

摘要

环境稳定的荧光自由基最近已成为有前景的发光材料;然而,由于对开壳有机体系的光物理理解有限,调整其性质一直很困难。在此,我们报告了一对相差一个电子的π共轭荧光分子氧化还原对的实验和计算分析。一个π二价阳离子()和π自由基阳离子()表现出不同的吸收光谱,但红色发射相似( = ∼630 nm)、激发最大值相似( = ∼530 nm)、荧光寿命相似(1 - 10 ns),甚至在用瞬态吸收光谱测量时激发态(非发射)寿命也相似。尽管它们在实验上有相似之处,但含时密度泛函理论(TDDFT)研究表明和的发射机制不同,且依赖于不同的电子跃迁。在单重态中,激发态重组通过空穴弛豫发生,而双重态通过弯曲其π主链经历 Jahn - Teller 畸变,以促进单占据分子轨道之间的自旋配对。和其π主链几何结构的激发态动力学之间的这种关系说明了开发具有新发射性质的π共轭自由基的潜在策略。此外,通过比较 TDDFT 和 CIS(单组态相互作用)激发,我们表明无限制 TDDFT 能准确再现实验吸收光谱,并为研究像这样的大型开壳分子的弛豫激发态性质提供了机会。

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