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arXiv 1003.0401cond-mat.mes-hallphysics.optics
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光子晶体波导中无序与局域场效应的相互作用

Interplay between disorder and local field effects in photonic crystal waveguides

M Patterson, S. Hughes

摘要:

我们引入了一个理论来描述无序诱导散射在光子晶体波导,特别是解决本地场效应和高折射率对比度扰动内的散射的影响。局部场效应被证明是增加预测的无序引起的散射损耗,并导致显着的谐振位移的波导模式。我们证明了两种类型的频率偏移,可以预期的平均频率偏移和RMS频率偏移,都在演唱会蓝移和拓宽标称能带结构。对于一个有代表性的波导,我们预测基本meV的频率偏移和能带结构加宽的电信工作频率,即使是最先进的制造。无序引起的展宽被发现增加的传播频率接近慢光制度(模式边缘),由于重组的电场分布。这些发现对高折射率对比度的纳米级波导产生了巨大的影响,并且对于光子晶体波导,表明名义上的慢光模式边缘甚至可能不存在。此外,我们的研究结果揭示了为什么迄今为止,它是不可能观察到的光子晶体波导的非常慢的光制度的新的光。

英文摘要:

We introduce a theory to describe disorder-induced scattering in photonic crystal waveguides, specifically addressing the influence of local field effects and scattering within high-index-contrast perturbations. Local field effects are shown to increase the predicted disorder-induced scattering loss and result in significant resonance shifts of the waveguide mode. We demonstrate that two types of frequency shifts can be expected, a mean frequency shift and a RMS frequency shift, both acting in concert to blueshift and broaden the nominal band structure. For a representative waveguide, we predict substantial meV frequency shifts and band structure broadening for a telecommunications operating frequency, even for state of the art fabrication. The disorder-induced broadening is found to increase as the propagation frequency approaches the slow light regime (mode edge) due to restructuring of the electric field distribution. These findings have a dramatic impact on high-index-contrast nanoscale waveguides, and, for photonic crystal waveguides, suggest that the nominal slow-light mode edge may not even exist. Furthermore, our results shed new light on why it has hitherto been impossible to observe the very slow light regime for photonic crystal waveguides.

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