The frequency-domain transmission line matrix method-a new concept

A frequency-domain transmission line matrix (TLM) method for the frequency-selective S-matrix computation of 3D waveguide discontinuities is presented. It combines the flexibility of the conventional TLM method with the computational efficiency of frequency-domain methods. The basis for this technique is the excitation of an impulse train of sinusoidally modulated magnitude, which retains the form of an impulse while its envelope contains the information of the structure at the modulation frequency. Utilizing the diakoptics technique in conjunction with the concept of the intrinsic scattering matrix, the original electromagnetic field problem is simplified to a matrix algebra problem. A variety of structures have been analyzed in order to check the accuracy of the approach, and excellent agreement has been observed in all cases. S-parameters for CPW air-bridges including finite thickness and conductivity of the metallizations are computed. The effect of superconducting air-bridges is analyzed. >

[1]  R. H. Jansen,et al.  The Microstrip Step Discontinuity: A Revised Description , 1986 .

[2]  P. Saguet,et al.  An improvement for the t.l.m. method , 1980 .

[3]  N.R.S. Simons,et al.  Method for modelling free space boundaries in TLM situations , 1990 .

[4]  Zhang Xiaolei,et al.  Time-domain finite difference approach to the calculation of the frequency-dependent characteristics of microstrip discontinuities , 1988 .

[5]  T. Kitazawa,et al.  Analysis of shielded coplanar waveguide step discontinuity considering the finite metallization thickness effect , 1991, 1991 IEEE MTT-S International Microwave Symposium Digest.

[6]  P. Saguet,et al.  Le maillage rectangulaire et le changement de maille dans la méthode TLM en deux dimensions (Rectangular meshing and mesh change in the 2D TLM method) , 1981 .

[7]  R. Vahldieck,et al.  Full-wave analysis of guiding structures using a 2-D array of 3-D TLM nodes , 1993 .

[8]  Masanori Koshiba,et al.  Three-dimensional finite-element solution of dielectric scattering obstacles in a rectangular waveguide , 1990 .

[9]  Peter B. Johns,et al.  Numerical solution of 2-dimensional scattering problems using a transmission-line matrix , 1971 .

[10]  P. Johns A Symmetrical Condensed Node for the TLM Method , 1987 .

[11]  B. Hunt,et al.  Design and performance of a high-T/sub c/ superconductor coplanar waveguide filter , 1991 .

[12]  H. Chaloupka A coupled-line model for the scattering by dielectric and ferrimagnetic obstacles in waveguides , 1980 .

[13]  Wolfgang J. R. Hoefer,et al.  The Transmission-Line Matrix Method--Theory and Applications , 1985 .

[14]  R. J. Lomax,et al.  A finite-difference transmission line matrix method incorporating a nonlinear device model , 1990 .

[15]  L. S. Riggs,et al.  Modelling of materials with electric and magnetic losses with the symmetrical condensed TLM method , 1990 .

[16]  P.P.M. So,et al.  A two-dimensional transmission line matrix microwave field simulator using new concepts and procedures , 1989 .

[17]  P. Naylor,et al.  New three dimensional symmetrical condensed lossy node for solution of electromagnetic wave problems by TLM , 1990 .

[18]  S. Ramo,et al.  Fields and Waves in Communication Electronics , 1966 .

[19]  V. Fouad Hanna,et al.  Theoretical and Experimental Investigation of Open Microstrip Gap Discontinuities , 1988, 1988 18th European Microwave Conference.