C-60分子中表面和体积偶极振荡的耦合

M. Brack, P. Winkler, M. Murthy
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引用次数: 6

摘要

我们首先简要回顾了“局部电流近似”(LCA),它是从一般变分原理推导出来的,作为有限费米子系统中从量子力学平均场基态开始的强集体激发的半经典描述。我们以金属团簇中耦合的平动和压缩偶极激发为例来说明它。然后讨论了C$_{60}$分子(巴克敏斯特富勒烯)中的集体电子偶极子激发。我们表明,在半经典LCA中,纯平移模式(“表面等离子体”)与压缩体积模式的耦合与微观时间相关密度泛函(TDLDA)计算产生了半定量的一致,而两种理论都与最近对“体积等离子体”的实验观察产生了定性的一致。
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Coupling of Surface and Volume Dipole Oscillations in C-60 Molecules
We first give a short review of the ``local-current approximation'' (LCA), derived from a general variation principle, which serves as a semiclassical description of strongly collective excitations in finite fermion systems starting from their quantum-mechanical mean-field ground state. We illustrate it for the example of coupled translational and compressional dipole excitations in metal clusters. We then discuss collective electronic dipole excitations in C$_{60}$ molecules (Buckminster fullerenes). We show that the coupling of the pure translational mode (``surface plasmon'') with compressional volume modes in the semiclasscial LCA yields semi-quantitative agreement with microscopic time-dependent density functional (TDLDA) calculations, while both theories yield qualitative agreement with the recent experimental observation of a ``volume plasmon''.
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