1990
DOI: 10.1109/22.64564
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A rigorous dispersive characterization of microstrip cross and T junctions

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Cited by 101 publications
(34 citation statements)
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“…n and g (2) m are PSW-P basis functions which have been used for the currents on the lines in the coupling region [10], and f, h are current distributions in uniform and infinitely long lines which were obtained by 1-dimensional spectral domain. The currents must be continuous at the boundaries x = x 1 , x 2 and z = z 1 , z 2 , so:…”
Section: The Methods Of Analysismentioning
confidence: 99%
“…n and g (2) m are PSW-P basis functions which have been used for the currents on the lines in the coupling region [10], and f, h are current distributions in uniform and infinitely long lines which were obtained by 1-dimensional spectral domain. The currents must be continuous at the boundaries x = x 1 , x 2 and z = z 1 , z 2 , so:…”
Section: The Methods Of Analysismentioning
confidence: 99%
“…These functions are Maxwellian type functions defined in [20,22]. In the perturbed regions, however, pulse and PSW-S sub-sectional basis functions (g x m and g z m ), discussed in [23], are used to accommodate possible high variations in the current distributions and also to add flexibility to the structure configuration. For currents on the ring resonator as defined in (2b), (2c), triangular basis functions have been utilized as shown in Fig.…”
Section: Basis Functionsmentioning
confidence: 99%
“…Coupling between parallel microstrip lines, which results the main cause of crosstalk, is generally predicted using quasi-static approaches [1][2][3][4][5][6][7][8][9], or full-wave techniques [10][11][12][13]. These techniques have been also employed to analyze the frequency behavior of microstrip discontinuities, such as T-junctions [14], gaps [15][16][17][18][19], bends [20], line crossings [21], and to investigate the field radiated from microstrip discontinuities [22] or interconnecting lines [23].…”
Section: Introductionmentioning
confidence: 99%