4.6 Article

Highly Sensitive Reflective-Mode Phase-Variation Permittivity Sensor Based on a Coplanar Waveguide Terminated With an Open Complementary Split Ring Resonator (OCSRR)

期刊

IEEE ACCESS
卷 9, 期 -, 页码 27928-27944

出版社

IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
DOI: 10.1109/ACCESS.2021.3058575

关键词

Coplanar waveguide (CPW); dielectric characterization; microwave sensor; open complementary split ring resonator (OCSRR); phase-variation sensor; reflective-mode sensor

资金

  1. Ministerio de Ciencia e Innovacion (MICINN)-Spain [TEC2016-75650-R, PID2019-103904RB-I00]
  2. Generalitat de Catalunya [2017SGR-1159]
  3. Institucio Catalana de Recerca i Estudis Avancats
  4. European Regional Development Fund (ERDF)
  5. Secreteraria d'Universitats i Recerca (Gen. Cat.)
  6. European Social Fund
  7. Juan de la Cierva Program [IJCI-2017-31339, IJC2019-040786-]

向作者/读者索取更多资源

This paper introduces a reflective-mode phase-variation microwave sensor utilizing OCSRR for high sensitivity, and investigates the effects of losses on the output variable, which can be used to estimate the loss tangent of the material.
This paper presents a one-port reflective-mode phase-variation microwave sensor consisting of a coplanar waveguide (CPW) transmission line terminated with a grounded open complementary split ring resonator (OCSRR). The sensor is useful for measuring the dielectric constant of the so-called material under test (MUT), which should be placed in contact with the OCSRR, the sensitive element. The output variable is the phase of the reflection coefficient. Design guidelines for the implementation of highly sensitive sensors are derived in the paper, and validated through simulation and experiment. As compared to other reflective-mode phase-variation sensors based on open-ended sensing lines, the designed and fabricated devices exhibit a very small sensitive region by virtue of the use of an electrically small resonant element, the OCSRR. The relevant figure of merit, defined as the ratio between the maximum sensitivity and the size of the sensing area (expressed in terms of the squared wavelength), is as high as FoM $= 5643 degrees/lambda(2) in one of the reported prototypes. Moreover, the paper analyzes the effects of losses. From this study, it is concluded that MUT losses do not significantly affect the output variable, provided losses are small. It is also demonstrated that the sensor is useful to estimate the loss tangent of the considered MUT samples.

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