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对于电磁引导模式的单向激发的近场干扰
Francisco J Rodríguez-Fortuño1, Giuseppe Marino, Pavel Ginzburg
1Department of Physics, King's College London, Strand, London WC2R 2LS, UK.
概括
近场干扰通过利用发射器的矢量结构来控制光辐射. 这使引导模式的单向激发成为可能,可以通过极化进行切换,为光学设备提供了新的可能性.
科学领域:
- 电磁主义 电磁主义
- 接近场光学近场光学
- 塑制剂是一种塑制剂.
背景情况:
- 波干扰是光学的一个核心概念,通常涉及具有不同相位的波.
- 常规干扰在控制光辐射方向性方面是有限的.
- 近场相互作用的矢量性质对于先进的光学控制至关重要.
研究的目的:
- 调查近场矢量结构在控制光辐射中的作用.
- 通过自我干扰来证明引导电磁模式的单向激发.
- 为了探索极化可切换的表面波激发.
主要方法:
- 从一个循环极化二极管的近场干扰的理论分析.
- 实验演示使用金膜中的单个照明裂来模拟双极.
- 测量表面等离子体激发和方向性.
主要成果:
- 双极的近场自我干扰导致引导模式的单向激发.
- 没有观察到偏好的远场辐射方向.
- 在一个对称的结构中实现了单向的表面-等离子激发,可以通过极化进行切换.
结论:
- 近场的矢量结构对于通过自我干扰控制辐射至关重要.
- 在没有方向远场辐射的情况下,单向引导模式激发是可能的.
- 极化控制提供了一种方法来切换表面波方向性.
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