Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physica C Superconductivity

Superconducting Pb as material for coplanar waveguide resonators on GaAs substrates

Maximilian Köpke, J. Weis

Published Jun 25, 2014• 5 citations
Publisher
DOI
10.1016/j.physc.2014.06.008

Related papers

Phononic Losses in Superconducting Coplanar Waveguide Resonators on Piezoelectric Substrates

Marco Scigliuzzo, Laure E. Bruhat, Andreas Bengtsson +2 more

Bulletin of the American Physical Society•Mar 6, 2019•0 citations

Superconducting coplanar waveguide resonators for electron spin resonance applications

Anthony J. Sigillito, Ryan Jock, A.M. Tyryshkin +2 more

Bulletin of the American Physical Society•Mar 20, 2013•0 citations

Modeling dielectric loss in superconducting coplanar-waveguide resonators

Veikka Taka

•Dec 18, 2020•0 citations

Dielectric Loss in Superconducting NbN (200) CPW Resonator Developed on Si Substrate

Wei Qiu, Kazumasa Makise, Hirotaka Terai

In current superconducting qubit circuit development, coherence time is limited by low-frequency flux noise introduced from localized two-level systems (TLSs) in the fabricated superconducting circuit, including superconducting materials, the interface between thin films, and the substrate. As a part of the effect to tackle this issue from a substrate standpoint, we succeed in fabricating NbN (200) oriented coplanar waveguide resonator (CPWR) on a thin titanium nitride (TiN) (200) buffered Si (100) substrate. The internal loss is close to 3 × 10-5nearphoton> ~1, improved from ~2 × 10-4in NbN (200) CPWR fabricated on MgO (100). For NbN (200) resonators grown on Si (100), the internal loss shows microwave energy independent. To further clarity if this energy independence is due to the change of substrate material, we also fabricated TiN (200) CPWR on Si (100). In contrast to NbN (200) CPWR, the loss of TiN (200) resonator shows a strong microwave dependent, an indication of TLSs originated from the interface and the surface. We suggest TLSs in NbN (200) CPWR are dominated from different mechanism other than arising from the interface and surface.

IEEE Transactions on Applied Superconductivity•Jan 9, 2017•5 citations

SUPERCONDUCTING COPLANAR WAVEGUIDE RESONATOR AND ITSKINETIC INDUCTANCE ONTHE HIGH RESISTIVITY SILICON SUBSTRATE

Zhan Yu Kang

A Superconducting coplanar waveguide(SCPW) resonator on the high resistivity silicon substrate which works at the microwave frequency is presented.We introduce the design,fabrication,measurement and data analysis.SCPW resonators with the material of NbN and Nb are measured to be compared.Since theKinetic inductance has a great influence on the resonator,we fabricate SCPW resonators with different thickness.The experimental results are compared with the theoretical ones.

Diwen wuli xuebao•Jan 1, 2013•0 citations

Fabrication and Characterisation of Superconducting Coplanar Waveguide Resonators for Circuit QED Applications

Martin G oppl, R. J. Schoelkopf, Andreas J. Wallraff

Bulletin of the American Physical Society•Mar 11, 2008•0 citations
In current superconducting qubit circuit development, coherence time is limited by low-frequency flux noise introduced from localized two-level systems (TLSs) in the fabricated superconducting circuit, including superconducting materials, the interface between thin films, and the substrate. As a part of the effect to tackle this issue from a substrate standpoint, we succeed in fabricating NbN (200) oriented coplanar waveguide resonator (CPWR) on a thin titanium nitride (TiN) (200) buffered Si (100) substrate. The internal loss is close to 3 × 10-5nearphoton> ~1, improved from ~2 × 10-4in NbN (200) CPWR fabricated on MgO (100). For NbN (200) resonators grown on Si (100), the internal loss shows microwave energy independent. To further clarity if this energy independence is due to the change of substrate material, we also fabricated TiN (200) CPWR on Si (100). In contrast to NbN (200) CPWR, the loss of TiN (200) resonator shows a strong microwave dependent, an indication of TLSs originated from the interface and the surface. We suggest TLSs in NbN (200) CPWR are dominated from different mechanism other than arising from the interface and surface.