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Peculiarties of the Electronic and Electron Vibrational Spectra of Organic Conductors: BEDT-TTF Salts of Alpha-Type Structure

机译:有机导体的电子和电子振动谱的奇特特征:α型结构的BEDT-TTF盐

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摘要

Polarised infrared reflectivity spectra of some ET-based conducting salts of alpha-type structure are measured and compared: (ET)_2I_3 (Ⅰ), (ET)_2TIHg(XCN)_4 (X ο S,Se) (Ⅱ) and (ET)_8[Hg_4Br_(12)(CH_3C_6H_4Cl)_2] (Ⅲ). For both Ⅰ and Ⅱ the electronic reflectivity is greater for the polarisation perpendicular to ET stacks. However, a resolved electron vibrational band in the region of 1 100-1 400 cm~(-1) is observed for Ⅱ in the polarisation characterised by lower electronic reflectivity in contrast with the spectra of Ⅰ. Another difference between Ⅰ and Ⅱ is the absence of the pronounced plasma edge in the region of 4 000 cm~(-1) in the spectra of Ⅱ, which may be due to high electron damping. For Ⅲ the electronic reflectivity is low and no resolved electron vibrational band in the region of 1 100-1 400 cm~(-1) is observed. The peculiarities of the electron-vibrational spectra of Ⅰ, Ⅱ and Ⅲ may be due to the details of the crystal structure.
机译:测量并比较了一些ET型α型结构的导电盐的偏振红外反射光谱:(ET)_2I_3(Ⅰ),(ET)_2TIHg(XCN)_4(XοS,Se)(Ⅱ)和(ET )_8 [Hg_4Br_(12)(CH_3C_6H_4Cl)_2](Ⅲ)。对于Ⅰ和Ⅱ而言,垂直于ET叠层的偏振的电子反射率都更大。然而,对于Ⅱ,在极化中观察到一个解析的电子振动带,其范围为1100-1400 cm〜(-1),与Ⅰ的光谱相比,其电子反射率较低。 Ⅰ和Ⅱ之间的另一个区别是在Ⅱ的光谱中在4000 cm〜(-1)区域没有明显的等离子体边缘,这可能是由于高电子阻尼引起的。对于Ⅲ,电子反射率低,在1 100-1 400 cm〜(-1)范围内未观察到分辨的电子振动带。 Ⅰ,Ⅱ和Ⅲ型电子振动光谱的特殊性可能是由于晶体结构的细节所致。

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