Radiation of a Magnetic Dipole in an Infinite Anisotropic Plasma Medium
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Abstract
The radiation of a magnetic dipole in an infinite anisotropic plasma medium is analyzed. A three-dimensional Fourier transform is employed to compute the field which is represented by using a dyadic formulation and it is shown that the far field can be expressed as a sum of two separate spherical waves. As an example, radiation patterns of the dipole parallel to the geomagnetic field in two different frequency regions are calculated.
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Cite this article:
LI Kai. Radiation of a Magnetic Dipole in an Infinite Anisotropic Plasma Medium[J]. Chin. Phys. Lett., 1998, 15(12): 898-900.
LI Kai. Radiation of a Magnetic Dipole in an Infinite Anisotropic Plasma Medium[J]. Chin. Phys. Lett., 1998, 15(12): 898-900.
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LI Kai. Radiation of a Magnetic Dipole in an Infinite Anisotropic Plasma Medium[J]. Chin. Phys. Lett., 1998, 15(12): 898-900.
LI Kai. Radiation of a Magnetic Dipole in an Infinite Anisotropic Plasma Medium[J]. Chin. Phys. Lett., 1998, 15(12): 898-900.
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