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首页> 外文期刊>Physical Review, B. Condensed Matter >Near-field and far-field scattering of surface plasmon polaritons by one-dimensional surface defects
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Near-field and far-field scattering of surface plasmon polaritons by one-dimensional surface defects

机译:一维表面缺陷对表面等离激元极化子的近场和远场散射

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摘要

A rigorous formulation for the scattering of surface plasmon polaritons (SPP's) from a one-dimensional surface defect of any shape that yields the electromagnetic field in the vacuum half-space above the vacuum-metal interface is developed by the use of an impedance boundary condition. The electric and magnetic near fields, the angular distribution of the far-field radiation into vacuum due to SPP-photon coupling, and the SPP reflection and transmission coefficients are calculated by numerically solving the k-space integral equation upon which the formulation is based. In particular, we consider Gaussian-shaped defects (either protuberances or indentations) and study the dependence of the above-mentioned physical quantities on their lie half-width a and height h. SPP reflection is significant for narrow defects (a less than or equal to lambda/5, for either protuberances or indentations, where lambda is the wavelength of the SPP); maximum reflection (plasmon mirrors) is achieved-for a approximate to lambda/10. For increasing defect widths, protuberances and indentations behave differently. The former give rise to a monotonic increase of radiation at the expense of SPP transmission for increasing defect half-width. However, indentations exhibit a significant increase of radiation (decrease of SPP transmission) for half-widths of the order of or smaller than the wavelength, but tend to total SPP transmission in an oscillatory manner upon further increasing the half-width. Both the position of the maximum radiation and the oscillation period depend on the defect height, which in all other cases only affects the process quantitatively. Light emitters might thus be associated with either wide indentations or protuberances with widths that are of the order of or smaller than the wavelength. [S0163-1829(99)01735-X]. [References: 42]
机译:通过使用阻抗边界条件,开发了一种严格的公式,用于从任何形状的一维表面缺陷中散射表面等离振子极化子(SPP's),从而在真空金属界面上方的真空半空间中产生电磁场。 。通过数值求解公式所依据的k空间积分方程,可以计算出电磁近场,由于SPP-光子耦合而进入真空的远场辐射的角度分布以及SPP反射和透射系数。特别是,我们考虑了高斯形状的缺陷(突起或凹陷),并研究了上述物理量对它们的半角宽度a和高度h的依赖性。 SPP反射对于狭窄的缺陷(对于隆起或压痕,小于或等于λ/ 5,其中λ是SPP的波长)而言很重要;达到最大反射(等离子镜)-大约为λ/ 10。对于增加的缺陷宽度,突起和压痕的行为有所不同。前者以增加缺陷半宽度为代价的SPP传输为代价,导致辐射单调增加。但是,压痕对于波长等于或小于波长的一半宽度显示出辐射的显着增加(SPP透射的减小),但是当进一步增加一半宽度时,压痕倾向于以振荡的方式使SPP透射总数增加。最大辐射的位置和振荡周期都取决于缺陷高度,在所有其他情况下,缺陷高度仅定量地影响工艺。因此,发光器可能与宽的凹口或具有与波长量级或小于波长的宽度的突起相关联。 [S0163-1829(99)01735-X]。 [参考:42]

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