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arXiv quant-ph/9806045quant-ph
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色散电磁模的量子理论

Quantum theory of dispersive electromagnetic modes

P. D. Drummond, M. Hillery

摘要:

从多极耦合原子与电磁场相互作用出发,得到了非均匀固体色散的量子理论。所得到的色散关系等价于从Drude-Lorentz模型得到的标准经典Sellmeir方程。在均匀(平面波)的情况下,我们得到了详细的量子模式结构的耦合极化激元场,并表明,在所有分支的色散关系的模式扩展完全定义的折射率和群速度的极化激元。我们展示了一个简单的程序,完全对角化的哈密顿在一个,两个或三维的环境中,即使在存在的纵向声子激子色散,和任意数量的共振跃迁与不同的频率。这是必要的,因为必须包括至少一个声子(I.R.)和一个激子(U. V.)模式,以便准确地表示透明固体介质中的色散。我们的对角化方法不需要一个明确的解决方案的色散关系,而是依赖于柯西轮廓积分的分析性质,在所有可能的模式频率。当存在纵向声子色散时,修改相关的群速度项,使其仅包括群速度的纯电磁部分。

英文摘要:

A quantum theory of dispersion for an inhomogeneous solid is obtained, from a starting point of multipolar coupled atoms interacting with an electromagnetic field. The dispersion relations obtained are equivalent to the standard classical Sellmeir equations obtained from the Drude-Lorentz model. In the homogeneous (plane-wave) case, we obtain the detailed quantum mode structure of the coupled polariton fields, and show that the mode expansion in all branches of the dispersion relation is completely defined by the refractive index and the group-velocity for the polaritons. We demonstrate a straightforward procedure for exactly diagonalizing the Hamiltonian in one, two or three-dimensional environments, even in the presence of longitudinal phonon-exciton dispersion, and an arbitrary number of resonant transitions with different frequencies. This is essential, since it is necessary to include at least one phonon (I.R.) and one exciton (U.V.) mode, in order to accurately represent dispersion in transparent solid media. Our method of diagonalization does not require an explicit solution of the dispersion relation, but relies instead on the analytic properties of Cauchy contour integrals over all possible mode frequencies. When there is longitudinal phonon dispersion, the relevant group-velocity term is modified so that it only includes the purely electromagnetic part of the group velocity.

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