2008
DOI: 10.1109/lmwc.2008.2002454
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Design of a Substrate Integrated Waveguide (SIW) Filter Using a Novel Topology of Coupling

Abstract: International audienceWe report on a new topology of coupling between substrate integrated circular cavities designed to produce particular filtering functions through combination with the classical iris-based coupling. This coupling is achieved by a grounded coplanar line etched at the top of cavities. This topology was used to realize a Ku-Band third-order filter, whose synthesis, electromagnetic simulation with HFSS, and experimental performances are presented here

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Cited by 84 publications
(64 citation statements)
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“…For the circular SIW resonator, the electric field is vertically polarized, and the magnetic field is circular within the cavity [13]. The fundamental mode is TM 010 mode, and the resonant frequency f 01 can be calculated by:…”
Section: Proposed Multilayer Second-order Mixed Coupling Filter With mentioning
confidence: 99%
“…For the circular SIW resonator, the electric field is vertically polarized, and the magnetic field is circular within the cavity [13]. The fundamental mode is TM 010 mode, and the resonant frequency f 01 can be calculated by:…”
Section: Proposed Multilayer Second-order Mixed Coupling Filter With mentioning
confidence: 99%
“…TE 201 -mode in folded-SIW cavity is taken as a resonator for passband implement. Therefore, the signs of coupling coefficients M 13 and M 23 are different. Figure 5(b) plots the magnetic coupling coefficients versus pc 1 .…”
Section: Filter Designmentioning
confidence: 99%
“…In order to move TZ to the lower stopband, TE 201 -mode in SIW cavity is used to filter design [12], and then, larger sizes are inevitable. To get a negative cross-coupling in trisection topology, coplanar waveguide (CPW) structure is etched on the top metal layer of the SIW cavities [13,14]. Nonphysical couplings implemented by higher or lower modes in waveguides are used to generate the finite TZs far away from the passband for improved stopband performance [15].…”
Section: Introductionmentioning
confidence: 99%
“…The distance between centre line of the aperture and circle centre d; the length of the stub l (calculated from centre line of the aperture); /4), h 0 = 2 mm, w 0 = 0.2 mm, R 0 = 1.6 mm, the transition structure was modeled with solid wall firstly and then the solid wall was replaced by vias-array under the guidelines of references [8][9][10][11], Some applications of SICC can be found in references [12][13][14], some important design guidelines can be found in [15][16][17][18][19]. The radius of the cavity R and the gap location d were two key parameters in designing of the transition structure; the R can be calculated with (3), and the parameter d was approximately λ g /4 ; the width of the microstrip lines were calculated to guarantee a 50 Ω impedance.…”
Section: Design Of the Sicc Transitionmentioning
confidence: 99%