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Published byGeorgia Malone Modified over 6 years ago
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Extremely High Q-factor Dielectric Resonators for Millimeter Wave Applications Jerzy Krupka§, Michael E. Tobar* § Institute of Microelectronics and Optoelectronics, Department of Electronics, Warsaw University of Technology, Warsaw, Poland *Frequency Standards and Metrology Research Group, Physics Department, the University of Western Australia
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Dielectric resonator partially shielded by metal enclosure
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Cylindrical dielectric resonator in metal enclosure
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Geometric factor versus size of metal enclosure d/h=2.0, Dc/d=Lc/h
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a) Q-factor and b) electric energy filling factor versus size of metal enclosure
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Geometric factors of TEn01 modes of shielded spherical dielectric resonator
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Q-factors due to radiation of TEn01 modes versus permittivity for an open spherical resonator
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Electric field distribution (1D) for TE103 mode of 5 layer YAG resonator b) and empty cavity
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Electric field distribution (2D) for 3 layer YAG resonator G=10800 Ohm pe2=0.09466
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Electric field distribution (2D) for TE103 mode of 5 layer YAG resonator G= Ohm pe2+pe4=
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Electric field distribution (1D) for TE101 mode of 5 layer YAG resonator
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Electric field distribution (2D) for TE101 mode of 5 layer YAG resonator G=475 Ohm pe2+pe4=0.7509
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Q-factor of spherical Bragg reflection dielectric resonators versus frequency a) TE102 mode (3 layers) b) TE103 mode (5 layers)
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Q-factor optimization for YAG resonator
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Measurements on the TE102 mode of 3 layer spherical Bragg resonator made of YAG
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