References
- Craddock , I. J. and Railton , C. J. 1992 . Application of the FDTD method and a full time-domain near-field transform to the problem of radiation from a PCB . Journal of Electromagnetic Waves and Applications , 6 ( No. 23 ) : 5 – 18 .
- Harrington , R. F. 1961 . Time-Harmonic Electromagnetic Fields , New York : McGraw-Hill .
- Kragalott , M. , Kluskens , M. S. and Pala , W. P. 1997 . Timedomain fields exterior to a two-dimensional FDTD space . IEEE Transaction on Antennas and Propagation , 45 ( No. 11 ) : 1655 – 1663 .
- Luebbers , R. J. , Kunz , K. S. , Schneider , M. and Hunsberger , F. 1991 . A finite-difference time-domain near zone to far zone transformation . IEEE Transactions on Antennas and Propagation , 39 ( No. 4 ) : 429 – 433 .
- Mouysset , V. 2005 . On an approximation of propagated fields by the non-stationnary Maxwell’s equations, homogeneous, outside a bounded domain . Compte Rendus de l’Académie des Sciences, Série I , 341 ( No. 10 ) : 641 – 646 .
- Mouysset , V. , Mazet , P. A. and Borderies , P. A multi-domain decomposition method to solve scattering problems in time domain . submitted
- Shlager , K. L. and Smith , G. S. 1994 . Near-field to near-field transformation for use with the FDTD method and its application with pulsed antenna problems . Electronics Letters , 30 ( No. 16 ) : 1262 – 1264 .
- Shlager , K. L. and Smith , G. S. 1995 . Comparison of two FDTD near-field to near-field transformations applied to pulsed antenna problems . Electronics Letters , 31 ( No. 12 ) : 410 – 413 .
- Stratton , J. A. 1941 . Electromagnetic Theory , New York : McGraw-Hill .
- Taflove , A. and Hagness , S. C. 2000 . Computational Electrodynamics , Artech House .
- Yee , K. S. 1966 . Numerical solution of initial boundary value problems involving Maxwell’s equations in isotropic Media . IEEE Transactions on Antennas and Propagation , 14 : 302 – 307 .
- Yee , K. S. 1991 . Time-domain extrapolation to the far field based on FDTD calculations . IEEE Transactions on Antennas and Propagation , 39 : 410 – 413 .