TY - JOUR
T1 - Resonances of Characteristic Modes for Perfectly Conducting Objects
AU - Lappalainen, Joni
AU - Yla-Oijala, Pasi
AU - Tzarouchis, Dimitrios C.
AU - Sihvola, Ari
PY - 2017/10
Y1 - 2017/10
N2 - Resonances, i.e., extrema of the eigenvalues of characteristic modes for closed perfectly conducting objects are investigated. The characteristic modal solutions based on the electric, magnetic, and combined field integral operators (EFIO, MFIO, and CFIO) are studied and compared with analytical solutions for a sphere. All these formulations are found to capture both external (radiating) and internal (cavity) resonances predicted by the analytical expressions. At the internal resonances the eigenvalues obtained with the EFIO and MFIO-based approaches are not correct and the corresponding modes are non-unique. These solutions exhibit also a strong duality between the electric (TM) and magnetic (TE) type modes. A connection is found between the external and internal resonances and the condition numbers of the matrices. The modal expansion of the CFIObased solution is correct, even though it also experiences the non-uniqueness of the EFIO and MFIO-based solutions.
AB - Resonances, i.e., extrema of the eigenvalues of characteristic modes for closed perfectly conducting objects are investigated. The characteristic modal solutions based on the electric, magnetic, and combined field integral operators (EFIO, MFIO, and CFIO) are studied and compared with analytical solutions for a sphere. All these formulations are found to capture both external (radiating) and internal (cavity) resonances predicted by the analytical expressions. At the internal resonances the eigenvalues obtained with the EFIO and MFIO-based approaches are not correct and the corresponding modes are non-unique. These solutions exhibit also a strong duality between the electric (TM) and magnetic (TE) type modes. A connection is found between the external and internal resonances and the condition numbers of the matrices. The modal expansion of the CFIObased solution is correct, even though it also experiences the non-uniqueness of the EFIO and MFIO-based solutions.
KW - Antennas
KW - Cavity resonators
KW - Eigenvalues and eigenfunctions
KW - Electric field integral operator
KW - external resonance
KW - Integral equations
KW - internal resonance
KW - magnetic field integral operator
KW - Magnetic resonance imaging
KW - perfect electric conductor
KW - Resonant frequency
KW - theory of characteristic modes
UR - http://www.scopus.com/inward/record.url?scp=85028514452&partnerID=8YFLogxK
U2 - 10.1109/TAP.2017.2741063
DO - 10.1109/TAP.2017.2741063
M3 - Article
AN - SCOPUS:85028514452
SN - 0018-926X
VL - 65
SP - 5332
EP - 5339
JO - IEEE Transactions on Antennas and Propagation
JF - IEEE Transactions on Antennas and Propagation
IS - 10
ER -