The method of equivalent edge currents (MEC) has some ambiguity about definition of edge currents at general edge points except for diffraction points. The modified edge representation is introduced to overcome this ambiguity. The modified edge is the fictitious one which is defined so as to satisfy the diffraction law for given directions of incidence and observation. The equivalent edge currents for physical optics (PO) components at general edge points are obtained by utilizing these fictitious edges and the classical Keller's diffraction coefficients. High potentials of these currents are numerically demonstrated for diffraction from a disk, a square plate and a parabolic reflector.
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Tsutomu MURASAKI, Makoto ANDO, "Equivalent Edge Currents by the Modified Edge Representation: Physical Optics Components" in IEICE TRANSACTIONS on Electronics,
vol. E75-C, no. 5, pp. 617-626, May 1992, doi: .
Abstract: The method of equivalent edge currents (MEC) has some ambiguity about definition of edge currents at general edge points except for diffraction points. The modified edge representation is introduced to overcome this ambiguity. The modified edge is the fictitious one which is defined so as to satisfy the diffraction law for given directions of incidence and observation. The equivalent edge currents for physical optics (PO) components at general edge points are obtained by utilizing these fictitious edges and the classical Keller's diffraction coefficients. High potentials of these currents are numerically demonstrated for diffraction from a disk, a square plate and a parabolic reflector.
URL: https://global.ieice.org/en_transactions/electronics/10.1587/e75-c_5_617/_p
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@ARTICLE{e75-c_5_617,
author={Tsutomu MURASAKI, Makoto ANDO, },
journal={IEICE TRANSACTIONS on Electronics},
title={Equivalent Edge Currents by the Modified Edge Representation: Physical Optics Components},
year={1992},
volume={E75-C},
number={5},
pages={617-626},
abstract={The method of equivalent edge currents (MEC) has some ambiguity about definition of edge currents at general edge points except for diffraction points. The modified edge representation is introduced to overcome this ambiguity. The modified edge is the fictitious one which is defined so as to satisfy the diffraction law for given directions of incidence and observation. The equivalent edge currents for physical optics (PO) components at general edge points are obtained by utilizing these fictitious edges and the classical Keller's diffraction coefficients. High potentials of these currents are numerically demonstrated for diffraction from a disk, a square plate and a parabolic reflector.},
keywords={},
doi={},
ISSN={},
month={May},}
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TY - JOUR
TI - Equivalent Edge Currents by the Modified Edge Representation: Physical Optics Components
T2 - IEICE TRANSACTIONS on Electronics
SP - 617
EP - 626
AU - Tsutomu MURASAKI
AU - Makoto ANDO
PY - 1992
DO -
JO - IEICE TRANSACTIONS on Electronics
SN -
VL - E75-C
IS - 5
JA - IEICE TRANSACTIONS on Electronics
Y1 - May 1992
AB - The method of equivalent edge currents (MEC) has some ambiguity about definition of edge currents at general edge points except for diffraction points. The modified edge representation is introduced to overcome this ambiguity. The modified edge is the fictitious one which is defined so as to satisfy the diffraction law for given directions of incidence and observation. The equivalent edge currents for physical optics (PO) components at general edge points are obtained by utilizing these fictitious edges and the classical Keller's diffraction coefficients. High potentials of these currents are numerically demonstrated for diffraction from a disk, a square plate and a parabolic reflector.
ER -