Optical Properties of Two-Dimensional Organic Conductors: Signatures of Charge Ordering and Correlation Effects
Optical Properties of Two-Dimensional Organic Conductors: Signatures of Charge Ordering and Correlation Effects
复制标题
二维有机导体的光学性质:电荷排序和相关效应的特征
DOI:
10.1002/chin.200505259
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发表时间:
2005
期刊:
影响因子:
--
通讯作者:
N. Drichko
中科院分区:
文献类型:
--
作者:
M. Dressel;N. Drichko
Optical studies, in a broad sense, are one of the most powerful techniques to characterize new materials and to investigate the properties of solids because electromagnetic waves cover a large range of energy and are sensitive to different kinds of excitation. We can obtain information not only on the electronic and the magnetic behavior, but also on the vibrational degrees of freedom, which include lattice properties as well as intramolecular vibrations. 1 In the radio frequency range and below, broad relaxational features can be observed if the lattice becomes soft, as known from ferroelectric phase transitions, but this spectral region is also of superior importance in cases of disorder or some sort of glassy behavior. Collective excitations which are relevant for density waves and other broken-symmetry ground states are located at low frequencies often well below the plasma frequency (Goldstone modes). These ground states of electronic and magnetic long-range order are of particular relevance in low-dimensional metals where the electron gas exhibits the tendency toward instabilities. 2 In the case of superconductivity, the energy gap in the single-particle density of states is expected in an energy range comparable to the superconducting transition temperature, ie, between microwave frequencies and the far-infrared spectral range. Of particular importance are effects due to electron-electron and electron-phonon interaction, which may lead to a certain frequency dependence of the scattering rate and an enhanced effective mass of the charge carriers. 1 The plasma edge for organic metals is commonly located in the infrared and only for a few exceptions of highly conducting materials even at higher energies. The unequivocal assignment of the optical response to conduction and valence electrons is already difficult in conventional materials if different electronic bands are involved; 1, 3-5 in general, no clear-cut distinction is possible in the case of synthetic metals. This fact makes the analysis of optical data of these compounds not a straightforward task, and it is also the reason for many discussions since the early days of molecular conductors. As known from classical semiconductors, interband transitions lead to pronounced signatures in the optical spectrum and can be analyzed in great detail. 6