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聚噻吩与富勒烯衍生物共混物中光致离子对的时间分辨电子顺磁共振

Time-resolved electron paramagnetic resonance of photoinduced ion pairs in blends of polythiophene and fullerene derivatives.

作者信息

Franco Lorenzo, Ruzzi Marco, Corvaja Carlo

机构信息

Department of Chemical Sciences, University of Padova, Via Marzolo, 1-I-35131 Padova, Italy.

出版信息

J Phys Chem B. 2005 Jul 21;109(28):13431-5. doi: 10.1021/jp0514877.

Abstract

Substituted polythiophene and triethylenglycolpyrrolidino-C(60) blends are examined by time-resolved electron paramagnetic resonance (TR-EPR) at different temperatures. TR-EPR spectra recorded on the microsecond time scale after a short laser pulse are assigned to polythiophene and fullerene radical ion pairs, generated by electron transfer from the excited state of polythiophene to fullerene. At low temperatures, TR-EPR spectra show polarized lines with an antiphase emission/absorption pattern. The origin of the polarization pattern is described in the frame of spin correlated radical pair theory, in which two unpaired electron spins (on radical cation and anion, respectively) interact through isotropic spin exchange and anisotropic dipolar interactions. The polarization pattern is accounted for assuming a singlet excited state as the precursor of the charge-separated state. Spectral simulations yield dipolar and spin exchange coupling constants between unpaired electrons of the radical ion pair. Their values correspond to a mean distance between opposite charges of 22 A. When the temperature is increased, the spectra gradually loose their antiphase character and eventually consist of a signal totally in emission. This behavior is explained by a polarization mechanism involving a spin-selective charge recombination (ST(-1) mixing). The polarization pattern at different temperatures is examined in detail, and its generating mechanism is discussed.

摘要

通过时间分辨电子顺磁共振(TR-EPR)在不同温度下研究了取代聚噻吩与三甘醇吡咯烷基-C(60)的混合物。在短激光脉冲后微秒时间尺度上记录的TR-EPR光谱归属于由聚噻吩激发态向富勒烯的电子转移所产生的聚噻吩和富勒烯自由基离子对。在低温下,TR-EPR光谱显示出具有反相发射/吸收模式的极化线。极化模式的起源在自旋相关自由基对理论框架内进行了描述,其中两个未配对电子自旋(分别在自由基阳离子和阴离子上)通过各向同性自旋交换和各向异性偶极相互作用相互作用。极化模式是在假设单重激发态为电荷分离态前体的情况下得到解释的。光谱模拟得出了自由基离子对未配对电子之间的偶极和自旋交换耦合常数。它们的值对应于相反电荷之间的平均距离为22埃。当温度升高时,光谱逐渐失去其反相特征,最终由完全为发射的信号组成。这种行为通过涉及自旋选择性电荷复合(ST(-1)混合)的极化机制来解释。详细研究了不同温度下的极化模式,并讨论了其产生机制。

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