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首页> 外文期刊>Journal of Applied Physics >Charge separation dynamics at bulk heterojunctions between poly(3-hexylthiophene) and PbS quantum dots
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Charge separation dynamics at bulk heterojunctions between poly(3-hexylthiophene) and PbS quantum dots

机译:聚(3-己基噻吩)和PbS量子点之间的本体异质结处的电荷分离动力学

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摘要

Photo-induced electron transfer between poly-(3-hexylthiophene) (P3HT) and small (2.4 nm) PbS quantum dots (QDs), capped by different ligands, was studied by picosecond and femtosecond time-resolved fluorescence and by photo-induced absorption (PIA) measurements. In line with previous experiments, we observed that the efficiency of the quenching of P3HT by PbS QDs increased upon decreasing the average thickness of the ligand shell. This trend was also observed in the PIA spectra and in prior work on the performance of photovoltaic devices where the active layer was a blend of P3HT with PbS QDs capped by different ligands. Combining the pico- and femtosecond fluorescence decays showed that the quenching in blend films of P3HT and PbS QDs treated with 1,4-benzenedithiol occurred over a broad time scale ranging from tens of femtoseconds to hundreds of picoseconds. This complex kinetics was attributed to exciton hopping followed by electron transfer to the conduction band of the QDs. We also compared the wavelength dependence of the internal quantum efficiency (IQE) in the hybrid photovoltaic devices to those devices where the photoactive layer consists of PbS QDs only. Although excitation in the first excitonic transition of the PbS QDs yielded a similar IQE in both devices, the IQE of the hybrid devices tripled at wavelengths where also P3HT started to absorb. This suggests that upon excitation of P3HT in the latter devices, charge generation occurs by photo-induced electron transfer from P3HT to the QDs rather than by energy transfer to the QDs followed by exciton dissociation in the QDs.
机译:通过皮秒和飞秒时间分辨荧光以及光诱导吸收研究了聚(3-己基噻吩)(P3HT)和小(2.4 nm)PbS量子点(QD)之间的光诱导电子转移,这些量子点被不同的配体封端。 (PIA)测量。与先前的实验一致,我们观察到,通过降低配体壳的平均厚度,PbS QD淬灭P3HT的效率会增加。在PIA光谱和光伏器件性能的先前工作中也观察到了这种趋势,其中活性层是P3HT与被不同配体封端的PbS QD的混合物。皮秒和飞秒荧光衰减的结合表明,用1,4-苯二硫醇处理的P3HT和PbS QD的共混膜的猝灭发生在数十飞秒到数百皮秒的较宽时间范围内。这种复杂的动力学归因于激子跳跃,然后电子转移到量子点的导带。我们还将混合光伏器件中的内部量子效率(IQE)与那些光敏层仅由PbS QD组成的器件的波长依赖性进行了比较。尽管在PbS QD的第一个激子跃迁中激发在两个器件中产生了相似的IQE,但是混合器件的IQE在P3HT也开始吸收的波长处增加了两倍。这表明在后一种器件中激发P3HT时,电荷的产生是通过从P3HT到QD的光诱导电子转移而不是能量转移到QD,然后在QD中进行激子解离而发生的。

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  • 来源
    《Journal of Applied Physics 》 |2015年第5期| 055502.1-055502.16| 共16页
  • 作者单位

    Laboratory of Photochemistry and Spectroscopy, Division of Molecular Imaging and Photonics, Chemistry Department, KULeuven, Celestijnenlaan 200F, B2404, 3001 Leuven, Belgium;

    Department of Physics, Energy and Semiconductor Research Laboratory, University of Oldenburg, Carl-von-Ossietzky-Str. 9-11, 26129 Oldenburg, Germany;

    Laboratory of Photochemistry and Spectroscopy, Division of Molecular Imaging and Photonics, Chemistry Department, KULeuven, Celestijnenlaan 200F, B2404, 3001 Leuven, Belgium;

    Laboratory of Photochemistry and Spectroscopy, Division of Molecular Imaging and Photonics, Chemistry Department, KULeuven, Celestijnenlaan 200F, B2404, 3001 Leuven, Belgium;

    Imec vzw, Kapeldreef 75, 3001 Leuven, Belgium;

    Imec vzw, Kapeldreef 75, 3001 Leuven, Belgium;

    Department of Physics, Energy and Semiconductor Research Laboratory, University of Oldenburg, Carl-von-Ossietzky-Str. 9-11, 26129 Oldenburg, Germany;

    Department of Physics, Energy and Semiconductor Research Laboratory, University of Oldenburg, Carl-von-Ossietzky-Str. 9-11, 26129 Oldenburg, Germany;

    Laboratory of Photochemistry and Spectroscopy, Division of Molecular Imaging and Photonics, Chemistry Department, KULeuven, Celestijnenlaan 200F, B2404, 3001 Leuven, Belgium;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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