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@ARTICLE{Barannik:826481,
      author       = {Barannik, A. A. and Vitusevich, Svetlana and Protsenko, I.
                      А. and Kharchenko, М. S. and Cherpak, Nikolay T.},
      title        = {{RADIATION} {Q}-{FACTOR} {OF} {DIFFERENTSHAPE} {DIELECTRIC}
                      {RESONATORS} {WITH} {TESTED} {CONDUCTORS} {AND} {LIQUID}
                      {DIELECTRICSPGI}-8},
      journal      = {Telecommunications and radio engineering},
      volume       = {75},
      number       = {3},
      issn         = {0040-2508},
      address      = {New York, NY},
      publisher    = {Scripta Technica, Inc.},
      reportid     = {FZJ-2017-00706},
      pages        = {235 - 245},
      year         = {2016},
      abstract     = {Whispering gallery mode dielectric resonators are used as
                      measuring cells to determine the electrophysical
                      characteristics of materials. It is necessary to choose the
                      resonator structure possessing acceptable radiation Q-factor
                      values. Calculation of the radiation Q-factor by analytical
                      methods is possible for simple symmetric structures only.
                      Numerical investigations of different-shape leucosapphire
                      resonators with limiting conducting end plates and without
                      them are carried out in the Ka-band. The disk resonators
                      with one conducting end plate are studied experimentally as
                      well. The effect of tested material sample introduction in
                      the electromagnetic field on the resonator field
                      distribution, frequency and radiation Q-factor is shown. The
                      application opportunity of measurement cells based on such
                      resonators for determination of the (super)conductor
                      microwave impedance and permittivity of dielectric liquids
                      is analyzed. The results obtained can be used for choosing
                      the resonator measurement cell with a negligible radiation
                      loss.},
      cin          = {PGI-8 / ICS-8 / JARA-FIT},
      ddc          = {620},
      cid          = {I:(DE-Juel1)PGI-8-20110106 / I:(DE-Juel1)ICS-8-20110106 /
                      $I:(DE-82)080009_20140620$},
      pnm          = {523 - Controlling Configuration-Based Phenomena (POF3-523)},
      pid          = {G:(DE-HGF)POF3-523},
      typ          = {PUB:(DE-HGF)16},
      doi          = {10.1615/TelecomRadEng.v75.i3.50},
      url          = {https://juser.fz-juelich.de/record/826481},
}