Phototric Band Structure of Surface Modes

S.C. Kitann, W. Barnes, J. Sambles
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Abstract

Wavelength scale periodic structures are of great current interest since they may be used to modify the interaction between light and matter [I]. In particular photonic band gaps may be used both to suppress [Z] and enhance [3] spontaneous emission. Recently we have studied band gaps for surface rather than bulk modes, and have shown that these may also be used to control spontaneous emission from a thin layer of dye 141. Such gaps occur when electromagnetic modes propagate on periodically modulated surfaces. We report on a detailed study to look at how the surface mode band structure depends on the surface profile. Our system comprised a corrugated metallic swfpce, fabricated using holographic techniques. Such a surface supports the propagation of surface plasmons. For M appropriate grating pitch Bragg scattering of the surface plasmon mode reds m the formation of a band gap. Using a convergent beam technique we are able to directly image the dispersion curve for the surface modes. With this technique we have determined how the band structure depends on the nature ofthe surface profile. The figure below shows how the width and central frequency of the gap valy as a hction of cormgation depth. The experimwtal data is seen to be well modelled by a recent theory [SI, indicated by the solid Line m the figures. The band gap described above only prohibits propagation over a small range of directions about the nod to the grating grooves. We have mersurcd how the band gap depends on the propagation direction and discuss the implications for the desiga of a photonic surface, ie one which prohibits the propagation of surface modes m all directions.
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表面模式的光电能带结构
波长尺度的周期结构是目前非常感兴趣的,因为它们可以用来改变光与物质之间的相互作用[1]。特别是光子带隙可以用来抑制[Z]和增强[3]自发发射。最近,我们研究了表面而非体模式的带隙,并表明这些带隙也可用于控制薄层染料141的自发发射。当电磁模式在周期性调制表面上传播时,就会出现这种间隙。我们报告了一项详细的研究,以了解表面模式带结构如何取决于表面轮廓。我们的系统包括一个波纹金属面板,使用全息技术制造。这样的表面支持表面等离子体的传播。对于合适的光栅间距M,表面等离子体模的布拉格散射M形成带隙。使用会聚光束技术,我们能够直接成像色散曲线的表面模式。通过这种技术,我们已经确定了带结构如何取决于表面轮廓的性质。下图显示了间隙谷的宽度和中心频率如何作为组合深度的函数。最近的理论[SI]很好地模拟了实验数据,如图中的实线所示。上述带隙仅禁止在关于光栅凹槽点头的小范围方向上传播。我们讨论了带隙如何依赖于传播方向,并讨论了设计光子表面的意义,即禁止表面模式向各个方向传播的表面。
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