MTT-S International Microwave Symposium Digest
DOI: 10.1109/mwsym.1975.1123346
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Design of Ferrite Differential Phase Shift Sections

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Cited by 18 publications
(13 citation statements)
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“…For "weak " and "strong" bias magnetic field the elements of the permeability tensor µ, µ a are well determined in [2].…”
Section: Permeability Tensormentioning
confidence: 99%
See 2 more Smart Citations
“…For "weak " and "strong" bias magnetic field the elements of the permeability tensor µ, µ a are well determined in [2].…”
Section: Permeability Tensormentioning
confidence: 99%
“…Then, owing to the relation (10) the total electric field is given by Assume that the ferrite guide is excited at the plane z = 0 by left hand circularly polarized LHCP wave described as superposition of two linearly polarized base waves. With this input wave the initial conditions at the input plane are given by E(z = 0) = e + = e 1 + je 2 and…”
Section: Operation Principlesmentioning
confidence: 99%
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“…The phase shift section comprises of a metallised ferrite rod and a ferrite yoke placed over this rod. Each of these elements involves design considerations and in-depth trade-offs for achieving an optimum phase shifter design using mathematical formulae [2][3][4] . Advanced softwares are also being used to design and simulate the passive RF devices.…”
Section: Virtual Prototyping and Development Of Rotary Field Ferrite mentioning
confidence: 99%
“…Fixed nonreciprocal quarter-wave plates are located beyond both ends of the phase shifting region. These elements use a transverse fourpole magnetic bias field [5] to produce a frequency-dependent differential phase of approximately 90 degrees, and convert between linearly polarized waves at the device terminals and the circularly polarized waves needed in the phase shifting region. The nonreciprocal quarter-wave plates generate opposite senses of circular polarization in the phase shifting region for the two directions of propagation.…”
Section: Introductionmentioning
confidence: 99%