1976
DOI: 10.1109/tmtt.1976.1128793
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A New Edge-Mode Isolator in the Very High Frequency Range

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1976
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Cited by 9 publications
(2 citation statements)
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“…By applying the DC bias, time‐average power density in the direction of propagation varies asymmetrically across the ferrite cross‐section. In consequence, the energy carried by the wave is displaced to one side of the top conductors ( field displacement ) [3]. If the direction of propagation is reversed, the distribution of time‐average power density is also reversed.…”
Section: Principle Of Operationmentioning
confidence: 99%
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“…By applying the DC bias, time‐average power density in the direction of propagation varies asymmetrically across the ferrite cross‐section. In consequence, the energy carried by the wave is displaced to one side of the top conductors ( field displacement ) [3]. If the direction of propagation is reversed, the distribution of time‐average power density is also reversed.…”
Section: Principle Of Operationmentioning
confidence: 99%
“…Accordingly, an edge-guided mode of propagation occurs in a wide microstrip transmission line using a ferrite slab magnetised perpendicular to the ground plane. Consequently, various versions of the edgemode isolator in microstrip and stripline have been proposed and demonstrated [2][3][4][5][6][7][8]. The edge-mode isolator is inherently broadband and the bandwidth can present two octaves or more [9].…”
mentioning
confidence: 99%