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操纵三重态:蒽衍生物中能量、吸收、寿命和湮没速率的调谐。

Manipulating triplet states: tuning energies, absorption, lifetimes, and annihilation rates in anthanthrene derivatives.

机构信息

Air Force Research Laboratory, Materials and Manufacturing Directorate, Functional Materials Division, Wright-Patterson AFB, Ohio 45433-7750, USA.

出版信息

Phys Chem Chem Phys. 2018 Nov 21;20(45):28412-28418. doi: 10.1039/c8cp06048g.

Abstract

The photophysical properties of anthanthrene, four anthanthrene derivatives containing varying phenyl and p-tBu-phenyl substituents, and two anthanthrones with phenyl and p-tBu-phenyl substituents are examined. In general, as the anthanthrenes and anthanthrones become more substituted, red-shifts are observed in the peak maxima of the ground- and excited-state absorption and fluorescence spectra. The anthanthrones have large (>0.8) intersystem crossing (ISC) quantum yields (ΦT) likely caused by nπ* character in the ground or excited states. A bromo-substituted anthanthrene has a unity ISC yield due to an ISC rate constant of 2.5 × 1010 s-1 caused by heavy-atom induced, spin-orbit coupling. This leads to low fluorescence quantum yields (ΦF) in these three derivatives. The parent anthanthrene and remaining derivatives behave much differently. All have ΦF values from 0.58-0.84 with lower ΦT values as radiative decay outcompetes ISC. The anthanthrones have remarkable excited-state absorption with strong, broad transitions across the visible region with weaker transitions extending to nearly two μm. The anthanthrenes have very similar-shaped, broad transitions in the visible which can be shifted ∼60 nm by controlling the substituents. The triplet lifetimes range from 31-1200 μs and increase as the ISC yields decrease; the bromo-substituted anthanthrene is the shortest, followed by the anthanthrones then the other anthanthrenes. The rate of triplet-triplet annihilation is also affected by the presence of substituents; as the amount of steric bulk is increased, the rate of annihilation decreases.

摘要

蒽、四个含不同苯基和对叔丁基苯基取代基的蒽衍生物,以及两个含苯基和对叔丁基苯基取代基的蒽并[9,10-d]噻吨的光物理性质进行了研究。一般来说,随着蒽和蒽并[9,10-d]噻吨的取代程度增加,基态和激发态吸收和荧光光谱的峰值最大值都会发生红移。蒽并[9,10-d]噻吨具有较大(>0.8)的系间窜越(ISC)量子产率(ΦT),可能是由于基态或激发态中的 nπ* 特征所致。由于重原子诱导的自旋轨道耦合,溴取代的蒽具有 unity ISC 产率,ISC 速率常数为 2.5×1010 s-1。这导致这三个衍生物的荧光量子产率(ΦF)较低。母体蒽和其余衍生物的行为则大不相同。所有的ΦF 值在 0.58-0.84 之间,较低的ΦT 值是由于辐射衰变与 ISC 竞争。蒽并[9,10-d]噻吨具有显著的激发态吸收,在可见光区域有很强的宽跃迁,较弱的跃迁延伸到近 2 μm。蒽衍生物在可见光区域具有非常相似形状的宽跃迁,可以通过控制取代基将其位移约 60nm。三重态寿命范围为 31-1200 μs,并且随着 ISC 产率的降低而增加;溴取代的蒽是最短的,其次是蒽并[9,10-d]噻吨,然后是其他蒽衍生物。三重态-三重态湮灭的速率也受到取代基的影响;随着空间位阻的增加,湮灭的速率降低。

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