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单分子水平上聚芴聚集体形成过程中链内形态的控制

Control of Intrachain Morphology in the Formation of Polyfluorene Aggregates on the Single-Molecule Level.

作者信息

Wilhelm Philipp, Blank Dominik, Lupton John M, Vogelsang Jan

机构信息

Institut für Experimentelle und Angewandte Physik, Universität Regensburg, Universitätsstraße 31, 93053, Regensburg, Germany.

出版信息

Chemphyschem. 2020 May 18;21(10):961-965. doi: 10.1002/cphc.202000118. Epub 2020 Apr 7.

DOI:10.1002/cphc.202000118
PMID:32255242
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7317353/
Abstract

Controlling the morphology of π-conjugated polymers for organic optoelectronic devices has long been a goal in the field of materials science. Since the morphology of a polymer chain is closely intertwined with its photophysical properties, it is desirable to be able to change the arrangement of the polymers at will. We investigate the π-conjugated polymer poly(9,9-dioctylfluorene) (PFO), which can exist in three distinctly different structural phases: the α-, β-, and γ-phase. Every phase has a different chain structure and a unique photoluminescence (PL) spectrum. Due to its unique properties and the pronounced spectral structure-property relations, PFO can be used as a model system to study the morphology of π-conjugated polymers. To avoid ensemble averaging, we examine the PL spectrum of single PFO chains embedded in a non-fluorescent matrix. With single-molecule spectroscopy the structural phase of every single chain can be determined, and changes can be monitored very easily. To manipulate the morphology, solvent vapor annealing (SVA) was applied, which leads to a diffusion of the polymer chains in the matrix. The β- and γ-phases appear during the self-assembly of single α-phase PFO chains into mesoscopic aggregates. The extent of β- and γ-phase formation is directed by the solvent-swelling protocol used for aggregation. Aggregation unequivocally promotes formation of the more planar β- and γ-phases. Once these lower-energy more ordered structural phases are formed, SVA cannot return the polymer chain to the less ordered phase by aggregate swelling.

摘要

长期以来,控制用于有机光电器件的π共轭聚合物的形态一直是材料科学领域的一个目标。由于聚合物链的形态与其光物理性质紧密相连,能够随意改变聚合物的排列是很有必要的。我们研究了π共轭聚合物聚(9,9 - 二辛基芴)(PFO),它可以以三种截然不同的结构相存在:α相、β相和γ相。每个相都有不同的链结构和独特的光致发光(PL)光谱。由于其独特的性质以及明显的光谱结构 - 性质关系,PFO可作为研究π共轭聚合物形态的模型系统。为避免系综平均,我们研究了嵌入非荧光基质中的单个PFO链的PL光谱。通过单分子光谱法,可以确定每条单链的结构相,并且变化很容易监测。为了操纵形态,采用了溶剂蒸汽退火(SVA),这导致聚合物链在基质中扩散。β相和γ相出现在单个α相PFO链自组装成介观聚集体的过程中。β相和γ相的形成程度由用于聚集的溶剂溶胀方案决定。聚集明确促进了更平面的β相和γ相的形成。一旦形成这些能量更低、更有序的结构相,SVA就不能通过聚集体溶胀使聚合物链回到无序程度较低的相。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/425b6b93cbb6/CPHC-21-961-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/083bc21cdd2d/CPHC-21-961-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/eaa43d75eaea/CPHC-21-961-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/4df8bf449258/CPHC-21-961-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/425b6b93cbb6/CPHC-21-961-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/083bc21cdd2d/CPHC-21-961-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/eaa43d75eaea/CPHC-21-961-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/4df8bf449258/CPHC-21-961-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/925c/7317353/425b6b93cbb6/CPHC-21-961-g004.jpg

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