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花菁聚集体的手性光学性质:从单体到束状的层次建模

Chiroptical properties of cyanine aggregates: hierarchical modelling from monomers to bundles.

作者信息

Bertocchi Francesco, Nizar Shahana, Sissa Cristina, Li Minghao, Ebbesen Thomas W, Genet Cyriaque, Painelli Anna

机构信息

Dipartimento di Scienze Chimiche, della Vita e della Sostenibilità Ambientale, Università di Parma Parco Area delle Scienze 17A Parma 43124 Italy

CNRS, CESQ-ISIS University of Strasbourg (UMR 7006) F-67000 Strasbourg France

出版信息

Chem Sci. 2024 Sep 9;15(39):16103-11. doi: 10.1039/d4sc04968c.

DOI:10.1039/d4sc04968c
PMID:39282648
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11393733/
Abstract

Some achiral cyanine dyes form well-ordered chiral assemblies exhibiting pronounced Circular Dichroism (CD) and Circularly Polarized Luminescence (CPL). Notably, achiral C8O3 cyanines self-assemble into tubular J-aggregates, which further organize into bundles displaying bisignate CD spectrum - hallmark of an exciton coupled system - and an unusual bisignated CPL. In contrast, the tubular aggregates display a monosignate CD spectrum. The mechanism underlying these intriguing features remains elusive. In the present work, a quantum-mechanical exciton model is proposed to elucidate the (chir)optical behaviour of C8O3 aggregates. A herringbone arrangement of C8O3 dyes within the tubular aggregates well reproduces the observed spectral signatures. The anomalous observation of a singular CD peak in tubular aggregates is ascribed to the intrinsic chirality of the monomeric units inside the aggregate, whereas the CD doublet characterizing the bundles is attributed to the exciton coupling between the constituent tubes. The bisignated CPL signal observed in bundles reveals significant anti-Kasha emission at room temperature and is quantitatively addressed accounting for a very tiny exciton splitting leading to a sizable thermal population of both exciton states. This study provides crucial insights on the complexity of C8O3 aggregation and on the origin of chiroptical response at various aggregation stages.

摘要

一些非手性花菁染料形成了有序的手性聚集体,表现出明显的圆二色性(CD)和圆偏振发光(CPL)。值得注意的是,非手性的C8O3花菁会自组装成管状J-聚集体,这些聚集体进一步组织成束,呈现出双符号CD光谱——这是激子耦合系统的标志——以及异常的双符号CPL。相比之下,管状聚集体呈现出单符号CD光谱。这些有趣特征背后的机制仍然难以捉摸。在本工作中,提出了一个量子力学激子模型来阐明C8O3聚集体的(手性)光学行为。C8O3染料在管状聚集体中的人字形排列很好地再现了观察到的光谱特征。管状聚集体中奇异CD峰的异常观测归因于聚集体内部单体单元的固有手性,而表征束的CD双峰则归因于组成管之间的激子耦合。在束中观察到的双符号CPL信号在室温下显示出显著的反卡莎发射,并通过考虑非常微小的激子分裂导致两个激子态的可观热布居进行了定量分析。这项研究为C8O3聚集的复杂性以及不同聚集阶段手性光学响应的起源提供了关键见解。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/a91475687078/d4sc04968c-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/d45849ecddc0/d4sc04968c-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/461b4bb05164/d4sc04968c-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/7f33cc05c4d1/d4sc04968c-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/a91475687078/d4sc04968c-f7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/d45849ecddc0/d4sc04968c-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/461b4bb05164/d4sc04968c-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/7f33cc05c4d1/d4sc04968c-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f9ac/11463287/a91475687078/d4sc04968c-f7.jpg

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