2004
DOI: 10.1364/josaa.21.000975
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Transmission of an inhomogeneous plane wave through an electrically small aperture in a perfectly conducting plane screen

Abstract: Most solutions for electromagnetic diffraction by a circular aperture in a perfectly conducting plane screen are for an incident homogeneous (propagating) plane wave. When the aperture is electrically small (dimensions small compared to the wavelength), the well-known transmission coefficient behaves as the fourth power of the diameter/wavelength. We consider the case in which the incident field is an inhomogeneous (evanescent) plane wave. Numerical calculations for the electrically small circular aperture sho… Show more

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Cited by 4 publications
(4 citation statements)
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“…5(a), we first note the large enhancement of the transmitted field, which is related to the increase in the magnitude of the incident aperture field when κ xi > 1, as is evident from (1). This phenomenon, which is consistent with the findings of Petersson and Smith [2], also confirms the crucial role played by the evanescent fields, such as surface waves and surface plasmons [58], in the extraordinary optical transmission (EOT) by subwavelength apertures in (real) metallic screens [1]. Hence, one way to achieve the EOT is to excite strongly evanescent fields at the input face, e.g., by texturing the metal surface in the vicinity of the aperture [59], which facilitates the coupling of the incident wave to a surface plasmon.…”
Section: Sample Numerical Resultssupporting
confidence: 93%
See 1 more Smart Citation
“…5(a), we first note the large enhancement of the transmitted field, which is related to the increase in the magnitude of the incident aperture field when κ xi > 1, as is evident from (1). This phenomenon, which is consistent with the findings of Petersson and Smith [2], also confirms the crucial role played by the evanescent fields, such as surface waves and surface plasmons [58], in the extraordinary optical transmission (EOT) by subwavelength apertures in (real) metallic screens [1]. Hence, one way to achieve the EOT is to excite strongly evanescent fields at the input face, e.g., by texturing the metal surface in the vicinity of the aperture [59], which facilitates the coupling of the incident wave to a surface plasmon.…”
Section: Sample Numerical Resultssupporting
confidence: 93%
“…2 Without loss of generality, the amplitude of E i is set to unity. We assume the e jωt time convention and SI units.…”
Section: Statement Of the Problemmentioning
confidence: 99%
“…The magnetic field plots exhibit a distinct intermediate zone with a drop off rate of 1/z 2 . Comparing the homogeneous and evanescent illumination results, we note a significant near-zone electric field enhancement in the latter case, with a concomitant enhancement in transmission efficiency [17]. For the evanescent TM wave, we note a null in the axial plot of |E x |, which is a near-field phenomenon also predicted by the quasi-static analysis.…”
Section: Sample Numerical Resultssupporting
confidence: 64%
“…For generality, we also allow for an inhomogeneous plane wave, evanescent along the z axis [17], where κ xi may be any real number with the corresponding κ zi given as…”
Section: Formulationmentioning
confidence: 99%