2016
DOI: 10.2528/pierc15122902
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Effects of Superstrate Layer on the Resonant Characteristics of Superconducting Rectangular Microstrip Patch Antenna

Abstract: Abstract-The resonant characteristics of superconducting rectangular microstrip patch antenna with a superstrate layer are investigated using a full-wave spectral analysis in conjunction with the complex resistive boundary condition. The complex surface impedance of superconducting patch is determined using London's equation and the two-fluid model of Gorter and Casimir. Numerical results using the full-wave analysis presented here are in excellent agreement with theoretical and experimental results available … Show more

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Cited by 5 publications
(4 citation statements)
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References 22 publications
(37 reference statements)
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“…These behaviors agree very well with those reported elsewhere in [7]. Note that the abrupt change in the resonant frequency at temperatures near Tc can be attributed to a modification of the magnetic penetration depth of the YBCO [23]. It also observed that the resonant frequencies obtained when the superconducting patch is printed on PTFE are higher than those obtained when the superconducting patch is printed on the Boron nitride or Quartz because the effective relative permittivity of the PTFE is lower than the one of both anisotropic materials Boron nitride and Quartz.…”
Section: A / Hsupporting
confidence: 92%
“…These behaviors agree very well with those reported elsewhere in [7]. Note that the abrupt change in the resonant frequency at temperatures near Tc can be attributed to a modification of the magnetic penetration depth of the YBCO [23]. It also observed that the resonant frequencies obtained when the superconducting patch is printed on PTFE are higher than those obtained when the superconducting patch is printed on the Boron nitride or Quartz because the effective relative permittivity of the PTFE is lower than the one of both anisotropic materials Boron nitride and Quartz.…”
Section: A / Hsupporting
confidence: 92%
“…where T and U in Equations (11) and (12) are respectively the Chebyshev polynomials of the first and second kinds.…”
Section: Z Y Xmentioning
confidence: 99%
“…Consider the evaluation of the VHT of Equations (11) and (12). The basis functions given in Equations (13) and (14) are then Hankel transformed to obtainΨ np andΦ nq , whose expressions are given by [14].…”
Section: Z Y Xmentioning
confidence: 99%
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