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结构可良好寻址的硼二吡咯-卟啉-富勒烯多聚体中的超快能量和电子转移

Ultrafast energy and electron transfers in structurally well addressable BODIPY-porphyrin-fullerene polyads.

作者信息

Gao Di, Aly Shawkat M, Karsenti Paul-Ludovic, Brisard Gessie, Harvey Pierre D

机构信息

Departement de chimie, Université de Sherbrooke, Sherbrooke, QC J1K 2R1, Canada.

出版信息

Phys Chem Chem Phys. 2017 Jan 25;19(4):2926-2939. doi: 10.1039/c6cp08000f.

Abstract

Two electron transfer polyads built upon [C]-[ZnP]-[BODIPY] (1) and [ZnP]-ZnP(-[C]) (2), where [C] = N-methyl-2-phenyl-3,4-fulleropyrrolidine, [BODIPY] = boron dipyrromethane, and [ZnP] = zinc(ii) porphyrin, were synthesized along with their corresponding energy transfer polyads [ZnP]-[BODIPY] (1a) and [ZnP]-[ZnP]-[BODIPY] (2a) as well as relevant models. These polyads were studied using cyclic voltammetry, DFT computations, steady state and time-resolved fluorescence spectroscopy, and fs transient absorption spectroscopy. The rates for energy transfer, k, [BODIPY]* → [ZnP] are ∼2.8 × 10 s for both 1a and 2a, with an efficiency of 99%. Concurrently, the fast appearance of the [C]˙ anion for 1 and 2 indicates that the charge separation occurs on the 20-30 ps timescale with the rates of electron transfer, k, [ZnP]*/[C] → [ZnP]˙/[C]˙ of ∼0.9 × 10 to ∼3.8 × 10 s. The latter value is among the fastest for these types of polyads. Conversely, the charge recombination operates on the ns timescale. These rates are comparable to or faster than those reported for other more flexible [C]-[ZnP]-[BODIPY] polyads, which can be rationalized by the donor-acceptor separations.

摘要

合成了基于[C]-[ZnP]-[BODIPY](1)和[ZnP]-ZnP(-[C])(2)的两个电子转移多联体,其中[C]=N-甲基-2-苯基-3,4-富勒吡咯烷,[BODIPY]=硼二吡咯甲烷,[ZnP]=锌(II)卟啉,以及它们相应的能量转移多联体[ZnP]-[BODIPY](1a)和[ZnP]-[ZnP]-[BODIPY](2a)和相关模型。使用循环伏安法、密度泛函理论计算、稳态和时间分辨荧光光谱以及飞秒瞬态吸收光谱对这些多联体进行了研究。对于1a和2a,从[BODIPY]到[ZnP]的能量转移速率k约为2.8×10⁹ s⁻¹,效率为99%。同时,对于1和2,[C]˙阴离子的快速出现表明电荷分离发生在20 - 30 ps的时间尺度上,电子转移速率k,从[ZnP]/[C]到[ZnP]˙/[C]˙约为0.9×10¹²到3.8×10¹² s⁻¹。后一个值是这类多联体中最快的之一。相反,电荷复合在纳秒时间尺度上进行。这些速率与其他更灵活的[C]-[ZnP]-[BODIPY]多联体报道的速率相当或更快,这可以通过供体 - 受体间距来解释。

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