Measurement Technique for Interface and Surface Conductivities at Millimeter-Wave Frequencies Using Dielectric Rod Resonator Excited by Nonradiative Dielectric Waveguide

• Published in: IEEE transactions on microwave theory and techniques 2022-05, Vol.70 (5), p.2750-2761
• Main Authors: Hirayama, Naoki, Nakayama, Akira, Yoshikawa, Hiromichi, Shimizu, Takashi, Kogami, Yoshinori
• Format: Article
• Language: English
• Subjects: Antenna measurements; Circuit design; Conductivity; Conductors; Copper-clad substrate; Dielectric measurement; dielectric rod resonator; Dielectric waveguides; Dielectrics; Excitation; interface conductivity; Loop antennas; Measurement techniques; Microwave frequencies; Millimeter wave measurements; Millimeter waves; millimeter-wave; nonradiative dielectric waveguide (NRD guide); Polytetrafluoroethylene; Resonators; Sapphire; Single crystals; Substrates; surface conductivity
• ISSN: 0018-9480; 1557-9670
• DOI: 10.1109/TMTT.2022.3157301

Herein, we propose a new technique for measuring interface and surface conductivities, \sigma _{i} and \sigma _{s} , of circuit substrates separately at millimeter-wave frequencies using a TE _{0m\delta } ( m =1 , 2, 3, \ldots, \delta < 1 ) mode single-crystal sapphire rod resonator excited via nonradiative dielectric waveguide (NRD guide). Here, \sigma _{i} represents an effective conductivity of conductor at the dielectric side. On the other hand, \sigma _{s} represents an effective conductivity at the shiny side of the conductor. Evaluating \sigma _{i} and \sigma _{s} separately is essential for high-precision circuit design at microwave and millimeter-wave frequencies and the development of low-loss circuit substrates. The superiority of NRD guide excitation compared with the conventional loop antenna excitation was confirmed through both experiments and simulations for the dielectric resonator at millimeter-wave frequencies. The feasibility of the proposed technique was verified by measuring \sigma _{i} and \sigma _{s} of the two types of commercially available copper-clad substrates, which were liquid-crystal-polymer-based and polytetrafluoroethylene-based substrates, at approximately 62, 74, and 80 GHz. In addition, we confirmed that these data were consistent with respect to the frequency with the measured results obtained using the conventional technique via loop antenna excitation at microwave frequencies, demonstrating the validity of the proposed technique. The measured results from 2 to 80 GHz showed that \sigma _{i} had a smaller value than \sig