1986
DOI: 10.1109/tap.1986.1143950
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The physical optics fields of an aperture on a perfectly conducting screen in terms of line integrals

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Cited by 32 publications
(14 citation statements)
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“…Using the characteristic function which is unity for and zero for , we can rewrite (4) in a compact form for the electric and magnetic field as (5) Equation (5) provides an alternative exact representation of the aperture field , with the advantage that the field can be exactly represented as a line integral along the contour , as proved next. The electric field radiated by the lateral surface is given by (6) where is the distance between the integration point along the strip and the observation point .…”
Section: Line-integral Formulation For Uniform Aperture Distribumentioning
confidence: 99%
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“…Using the characteristic function which is unity for and zero for , we can rewrite (4) in a compact form for the electric and magnetic field as (5) Equation (5) provides an alternative exact representation of the aperture field , with the advantage that the field can be exactly represented as a line integral along the contour , as proved next. The electric field radiated by the lateral surface is given by (6) where is the distance between the integration point along the strip and the observation point .…”
Section: Line-integral Formulation For Uniform Aperture Distribumentioning
confidence: 99%
“…A modern applicationoriented reformulation of the surface-to-line integral reduction is due to Asvestas [5]; his technique was generalized in [6] to PO scattering from a perfectly conducting flat face. The procedure presented here while specializing with a simplified formulation the work presented in [4] to the case of reflector antennas, leads to an interesting generalization to nonuniform aperture fields.…”
Section: Introductionmentioning
confidence: 99%
“…The first achievements in this direction are due to Maggi [1] and Asvestas [2], while a very recent contribution can be found in [3].…”
Section: Introductionmentioning
confidence: 99%
“…Dispersion compensating fibers (DCFs) and linearly chirped fiber Bragg gratings (CFBGs) have been successfully used to provide dispersion compensation for systems in order to transmit much longer distance without electronic repeaters. However, DCF has high loss because its field is mismatched with SMF, high nonlinearity because of its small core diameter, and high polarization-mode dispersion (PMD) because of its complex waveguide structure [1][2][3][4]. DCF can only completely compensate one channel of wavelength-division multiplexer (WDM) dispersion [3,4], and rudimental dispersion seriously limits the transmissive distance without an electronic repeater.…”
Section: Introductionmentioning
confidence: 99%
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