Yin Wenyan, Wang Wenbing. THE DYADIC GREEN S FUNCTION THEORY FOR ONE/TWO CYLINDRICAL LAYERS OF CHIRAL MEDIUM AND ITS APPLICATIONS[J]. Journal of Electronics & Information Technology, 1994, 16(2): 163-172.
Citation:
Yin Wenyan, Wang Wenbing. THE DYADIC GREEN S FUNCTION THEORY FOR ONE/TWO CYLINDRICAL LAYERS OF CHIRAL MEDIUM AND ITS APPLICATIONS[J]. Journal of Electronics & Information Technology, 1994, 16(2): 163-172.
Yin Wenyan, Wang Wenbing. THE DYADIC GREEN S FUNCTION THEORY FOR ONE/TWO CYLINDRICAL LAYERS OF CHIRAL MEDIUM AND ITS APPLICATIONS[J]. Journal of Electronics & Information Technology, 1994, 16(2): 163-172.
Citation:
Yin Wenyan, Wang Wenbing. THE DYADIC GREEN S FUNCTION THEORY FOR ONE/TWO CYLINDRICAL LAYERS OF CHIRAL MEDIUM AND ITS APPLICATIONS[J]. Journal of Electronics & Information Technology, 1994, 16(2): 163-172.
The expression of dyadic Green s function for one and two cylindrical layers of chiral medium are derived by using the method of scattering superposition, for which the electric current sources are placed both inside and outside of a chiral cylinder and a cylindrical chirodome. Then the radiation characteristics of a point dipole antenna on the axis of the chiral cylinder and cylindrical chirodome are analysed. The results show that the polarized states of radiated fields can be changed by choosing the size of chiral cylinder or the thickness of cylindrical chirodome. Also, the expressions of dyadic Green's function given in thid paper can be directly use to analyse the radiation characteristics of cylindrical chirostrip antenna.
Ali M J. Opt. Soc. Am. A, 1992. 9(3): 413-423.[2]Yin Wenyan, Wang Wenbing. The Eigenfunetion Expansions of Dyadic Greens Function in Unbounded Chiral Medium and Applications. Proceeding, of International Symposium on Antennas and EM Theory, Xian: Oct. 1992, 21-25.[3]Lakhtakio A J. Int. Electron., 1991, 7(1):139-144.[4]Engheta N, et el. J. Appl. Phys., 1990, 67(2):639-647.[5]Jaggard D L, et al. Electron[J].Lett.1989, 15(3):173-174
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