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Improvement Of Coupling Characteristics Of Sapphire Quasioptical Dielectric Resonator By Microstrip Line

机译:微带线改善蓝宝石准光学介质谐振器的耦合特性

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Regularities of coupling of the leucosapphire quasioptical dielectric resonator (QDR) to the polytetrafluorethylene reinforced microstrip line (MSL) are experimentally investigated in the Ka-band. It is suggested to organize coupling in within the "QDR over MSL" space that is different from a known coupling "QDR on a MSL substrate". It is shown that at coupling with the help of the "QDR over MSL" the loss of the resonance field energy in a substrate is negligibly small as compared to the eigen losses in QDR. Presence of several coupling areas separated by zones of lack of coupling both for quasi-E and for quasi-H modes is revealed. Open resonators with metallic phase-correcting mirrors and sapphire dielectric resonators excited at higher azimuth modes of oscillations (whispering gallery mode waves) possess the highest value of the Q-factor in the millimeter band of radio waves under the room temperature. The latter resonators are usually called quasioptical dielectric resonators (QDR). In the devices where frequency control is not necessary, for example, at stabilization of the heterodyne frequency or in the filters, the preference is given to QDR due to their advantage in weight and dimension parameters. This advantage is especially evident in development of the modules using the microstrip design. The generally accepted method for the microstrip line (MSL) coupling with QDR is positioning of the resonator directly upon the dielectric substrate near the strip [1]. It is the same technique as that used at excitation of the dielectric resonators at lower modes [2,3]. It is quite apparent that using this method is related to inevitable losses δs for scattering of the accumulated in the resonator energy within the dielectric and on the metal screen of MSL because the field of eigen modes of QDR is concentrated not only inside the resonator but in the environment as well.
机译:在Ka波段中,实验研究了亮蓝宝石准光学介电共振器(QDR)与聚四氟乙烯增强微带线(MSL)耦合的规律。建议在“ MSL上的QDR”空间内组织耦合,这与已知的“ MSL基板上的QDR”耦合不同。结果表明,与“ QDR over MSL”相结合,与QDR的本征损耗相比,基片中共振场能量的损耗可忽略不计。揭示了由准E模式和准H模式的缺乏耦合区域分隔的几个耦合区域的存在。在室温下,带有金属相位校正镜的开放式谐振器和在较高方位角的振荡模式(耳语回廊模式波)激发的蓝宝石介电谐振器在无线电波的毫米波带中具有最高的Q值。后者的谐振器通常称为准光介电谐振器(QDR)。在不需要频率控制的设备中(例如,在外差频率稳定时)或在滤波器中,由于QDR在重量和尺寸参数方面的优势,因此优先选择QDR。在使用微带设计开发模块时,这一优势尤为明显。与QDR耦合的微带线(MSL)的公认方法是将谐振器直接放置在靠近带[1]的介电基板上。它与在较低模式下激发介电共振器的技术相同[2,3]。很明显,使用此方法与不可避免的损耗δs有关,因为损耗的δs会散射电介质内部和MSL金属屏上谐振器能量中的累积,因为QDR的本征模场不仅集中在谐振器内部,而且集中在环境也是如此。

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