Low-characteristic-impedance superconducting tadpole resonators in the sub-gigahertz regime

We demonstrate a simple and versatile resonator design based on a short strip of a typical coplanar waveguide shorted at one end to the ground and shunted at the other end with a large parallel-plate capacitor. Due to the shape of the structure, we coin it the tadpole resonator. The design allows tailoring the characteristic impedance of the resonator to especially suit applications requiring low values. We demonstrate characteristic impedances ranging from <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:msub><a:mi>Z</a:mi><a:mi mathvariant="normal">c</a:mi></a:msub><a:mo>=</a:mo><a:mn>2</a:mn></a:mrow></a:math> to <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mn>10</c:mn><c:mspace width="0.16em"/><c:mi mathvariant="normal">Ω</c:mi></c:mrow></c:math> and a frequency range from <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:mrow><f:msub><f:mi>f</f:mi><f:mi mathvariant="normal">r</f:mi></f:msub><f:mo>=</f:mo><f:mn>290</f:mn><f:mspace width="0.16em"/><f:mi>MHz</f:mi></f:mrow></f:math> to <i:math xmlns:i="http://www.w3.org/1998/Math/MathML"><i:mrow><i:mn>1.1</i:mn><i:mspace width="0.16em"/><i:mi>GHz</i:mi></i:mrow></i:math> while reaching internal quality factors of order <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"><k:mrow><k:msub><k:mi>Q</k:mi><k:mi>int</k:mi></k:msub><k:mo>=</k:mo><k:mn>8.5</k:mn><k:mo>×</k:mo><k:msup><k:mn>10</k:mn><k:mn>3</k:mn></k:msup></k:mrow></k:math> translating into a loss tangent of <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:mrow><l:mo form="prefix">tan</l:mo><l:mrow><l:mo>(</l:mo><l:mi>δ</l:mi><l:mo>)</l:mo></l:mrow><l:mo>=</l:mo><l:mn>1.2</l:mn><l:mo>×</l:mo><l:msup><l:mn>10</l:mn><l:mrow><l:mo>−</l:mo><l:mn>4</l:mn></l:mrow></l:msup></l:mrow></l:math> for the aluminum oxide used as the dielectric in the parallel-plate capacitor. We conclude that these tadpole resonators are well suited for applications requiring low frequency and low characteristic impedance while maintaining a small footprint on chip. The low characteristic impedance of the tadpole resonator renders it a promising candidate for achieving strong inductive coupling to other microwave components. Published by the American Physical Society 2024

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Journal
Physical Review Research
Published
2024-12-19
DOI
https://doi.org/10.1103/physrevresearch.6.043297
Citations
1
Primary Topic
Physics of Superconductivity and Magnetism
Type
article
Field-Weighted Citation Impact
0.31

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article

Low-characteristic-impedance superconducting tadpole resonators in the sub-gigahertz regime

Mikko Möttönen, Jian Ma, Heikki Suominen, Priyank Singh et al.
1 citations
Physical Review Research
Physics of Superconductivity and Magnetism
0.31
article

Low-characteristic-impedance superconducting tadpole resonators in the sub-gigahertz regime

Mikko Möttönen, Jian Ma, Heikki Suominen, Priyank Singh, Miika Rasola, Samuel Klaver, Tuomas Uusnäkki
article en
1 citations

Abstract

We demonstrate a simple and versatile resonator design based on a short strip of a typical coplanar waveguide shorted at one end to the ground and shunted at the other end with a large parallel-plate capacitor. Due to the shape of the structure, we coin it the tadpole resonator. The design allows tailoring the characteristic impedance of the resonator to especially suit applications requiring low values. We demonstrate characteristic impedances ranging from <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:msub><a:mi>Z</a:mi><a:mi mathvariant="normal">c</a:mi></a:msub><a:mo>=</a:mo><a:mn>2</a:mn></a:mrow></a:math> to <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:mrow><c:mn>10</c:mn><c:mspace width="0.16em"/><c:mi mathvariant="normal">Ω</c:mi></c:mrow></c:math> and a frequency range from <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:mrow><f:msub><f:mi>f</f:mi><f:mi mathvariant="normal">r</f:mi></f:msub><f:mo>=</f:mo><f:mn>290</f:mn><f:mspace width="0.16em"/><f:mi>MHz</f:mi></f:mrow></f:math> to <i:math xmlns:i="http://www.w3.org/1998/Math/MathML"><i:mrow><i:mn>1.1</i:mn><i:mspace width="0.16em"/><i:mi>GHz</i:mi></i:mrow></i:math> while reaching internal quality factors of order <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"><k:mrow><k:msub><k:mi>Q</k:mi><k:mi>int</k:mi></k:msub><k:mo>=</k:mo><k:mn>8.5</k:mn><k:mo>×</k:mo><k:msup><k:mn>10</k:mn><k:mn>3</k:mn></k:msup></k:mrow></k:math> translating into a loss tangent of <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:mrow><l:mo form="prefix">tan</l:mo><l:mrow><l:mo>(</l:mo><l:mi>δ</l:mi><l:mo>)</l:mo></l:mrow><l:mo>=</l:mo><l:mn>1.2</l:mn><l:mo>×</l:mo><l:msup><l:mn>10</l:mn><l:mrow><l:mo>−</l:mo><l:mn>4</l:mn></l:mrow></l:msup></l:mrow></l:math> for the aluminum oxide used as the dielectric in the parallel-plate capacitor. We conclude that these tadpole resonators are well suited for applications requiring low frequency and low characteristic impedance while maintaining a small footprint on chip. The low characteristic impedance of the tadpole resonator renders it a promising candidate for achieving strong inductive coupling to other microwave components. Published by the American Physical Society 2024

Physical Review ResearchVol. 6(4)
VTT Technical Research Centre of Finland (FI), Aalto University (FI)
Academy of Finland, Aalto-Yliopisto, Business Finland, H2020 European Research Council
Openalex Percentile: Top 40%
Physics of Superconductivity and Magnetism
0.31
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