2006
DOI: 10.1063/1.2388651
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Effects of longitudinal field on transmitted near field in doped semi-infinite semiconductors with a surface conducting sheet

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Cited by 18 publications
(25 citation statements)
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“…They can, however, still be electrically separated from each other by an energy barrier. 11 Light incident from z Ͻ 0 is diffracted by the grating in both the reflected ͑z Ͻ 0͒ and the transmitted ͑z Ͼ 0͒ regions. The diffraction ͑Bragg͒ modes of EMFs are excited by the induced optical polarization at the interface from both the conducting sheet and grating.…”
Section: Model and Theorymentioning
confidence: 99%
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“…They can, however, still be electrically separated from each other by an energy barrier. 11 Light incident from z Ͻ 0 is diffracted by the grating in both the reflected ͑z Ͻ 0͒ and the transmitted ͑z Ͼ 0͒ regions. The diffraction ͑Bragg͒ modes of EMFs are excited by the induced optical polarization at the interface from both the conducting sheet and grating.…”
Section: Model and Theorymentioning
confidence: 99%
“…Our model is different from previously studied structures, such as a metal film or a metal grating between two semi-infinite dielectric materials ͑no longitudinal field͒, two semi-infinite metals ͑no surface plasmon͒, and a semi-infinite metal next to a half-space of air ͑no grating diffraction͒. It is a generalization of our previous study 11 on the effect of a longitudinal field by adding a metallic grating on top of the conducting sheet in order to generate and mix diffracted EMFs. It also extends our recent work 16 on the coupling of the electronically modulated 2D plasmon and the SP by including the retardation and longitudinal-field effects in calculating the diffracted near and far EMFs.…”
Section: Introductionmentioning
confidence: 95%
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“…If there exist conduction electrons, in addition to bound electrons in charged point defects, with concentration n 0 , effective mass m * and homogeneous broadening γ e in the host material containing generated point defects, the matrix elements of the dielectric function are found to be (Huang et al, 2006):…”
Section: ( )mentioning
confidence: 99%
“…All these methods are spatially local and adiabatic in time, thereby neglecting the nonlocal dynamic relationship [30], [31] between the induced material polarization and the total EM field in the Maxwell equations, but can be applied to dielectric host materials in which there are no free charged carriers. In addition, the absorption from the longitudinal field due to the induced plasma wave in 2 metals [32] has been neglected, which tends to underestimate the loss of SPP waves propagating along the interface between air and metals.…”
Section: Introductionmentioning
confidence: 99%