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首页> 外文期刊>Physical Review, B. Condensed Matter >ANALYSIS OF THE PHOTOCURRENT ACTION SPECTRA OF MEH-PPV POLYMER PHOTODIODES
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ANALYSIS OF THE PHOTOCURRENT ACTION SPECTRA OF MEH-PPV POLYMER PHOTODIODES

机译:MEH-PPV聚合物光电二极管的光电流作用谱分析

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We have measured the photocurrent action spectra of the conjugated polymers poly[2-methoxy, 5 ethyl (2' hexyloxy) paraphenylenevinylene] (MEH-PPV) and poly(phenylenevinylene) (PPV) in sandwich cells between indium tin oxide (ITO) and aluminum electrodes. Under forward bias and illumination through ITO, the photocurrent spectrum is broad and has a maximum at high energy, where the absorption coefficient is greatest (the symbatic response). Under reverse bias and illumination through ITO, the photocurrent spectrum consists of a very narrow peak (the full width at half maximum is 0.1 eV), located in the low-energy tail of the absorption profile (the antibatic response). Several established models attempt to explain this behavior and to relate the photocurrent action spectrum to the absorption coefficient, considering penetration depth of the light and diffusion of excitons or directly photogenerated charges. At a qualitative level many of these seem to provide an adequate description. In this paper, we undertake a quantitative examination of these models and we find that none of them can reproduce the very narrow antibatic response that we observe in both MEH-PPV and PPV. Upon exposure to air, we observe an enhancement of the photocurrent by a much greater factor than the dark current, from which we conclude that charge generation is mediated by exciton dissociation. As the temperature decreases we observe a progressive redshift of the absorption edge, although the photocurrent onset undergoes a much smaller redshift. We therefore conclude that the narrow antibatic peak is due to a specific enhancement of dissociation upon excitation at low energy. We propose that the particularly sharp onset of photocurrent at low energy may be due to enhanced intermolecular charge separation within crystallite grains between those neighboring conjugated segments that are more extended and more planar. [References: 95]
机译:我们已经测量了在铟锡氧化物(ITO)和ITO之间的夹层电池中共轭聚合物聚[2-甲氧基,5-乙基(2'己氧基)对亚苯基亚乙烯基](MEH-PPV)和聚(亚苯基亚乙烯基)(PPV)的光电流作用谱。铝电极。在正向偏置和通过ITO照射下,光电流谱很宽,在高能量下具有最大值,在该处吸收系数最大(符号响应)。在反向偏置和通过ITO照射下,光电流谱由一个非常窄的峰(半峰全宽为0.1 eV)组成,该峰位于吸收曲线的低能尾部(反击响应)。考虑到光的穿透深度和激子或直接光生电荷的扩散,一些建立的模型试图解释这种行为并使光电流作用谱与吸收系数相关。从质量上讲,其中许多似乎提供了足够的描述。在本文中,我们对这些模型进行了定量检查,结果发现它们都无法重现我们在MEH-PPV和PPV中观察到的非常狭窄的反击反应。暴露于空气后,我们观察到光电流的增强比暗电流大得多,由此可以得出结论,电荷产生是由激子解离介导的。随着温度降低,我们观察到吸收边的渐进性红移,尽管光电流开始经历的红移小得多。因此,我们得出的结论是,窄的抗反射峰是由于在低能量激发时解离的特定增强。我们提出在低能量下光电流的特别尖锐的开始可能是由于在那些更延伸和更平坦的相邻共轭链段之间的微晶晶粒内增强的分子间电荷分离。 [参考:95]

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