Design and Characterization of Superconducting Aluminum Spiral Resonators towards Planar Bosonic Qubits
POSTER
Abstract
Bosonic qubits have emerged as a promising method for performing quantum computation on superconducting qubits. Typically, they are realized by coupling a high Q 3D cavity (Qi>107 to 108) to a transmon qubit, which is then coupled to a low Q readout resonator (Q~104) [1, 2]. However, 3D cavities have a larger footprint compared to planar on-chip resonators, which can pose a challenge when scaling up bosonic qubit architectures. The most popular planar resonator is the coplanar waveguide (Qi>106), which tends to have lower Q-factor compared to 3D cavities. However, an effort was made to explore a geometric optimization to increase the internal quality factor, comparing Archimedian spiral resonators (ASRs) to coplanar waveguides using TiN as the superconductor [3]. Here, we discuss the prospects of using aluminum ASRs in planar bosonic qubit architectures as the storage resonator.
[1] M. Reagor et al., Appl. Phys. Lett. 102, 192604 (2013)
[2] A. Joshi, K. Noh, Y. Y. Gao, Quantum Sci. Technol. 6 033001 (2021)
[3] Y. Tominaga et al., EPJ Quantum Technol. 12, 60 (2025).
[1] M. Reagor et al., Appl. Phys. Lett. 102, 192604 (2013)
[2] A. Joshi, K. Noh, Y. Y. Gao, Quantum Sci. Technol. 6 033001 (2021)
[3] Y. Tominaga et al., EPJ Quantum Technol. 12, 60 (2025).
*The devices in this research were fabricated at MIT Lincoln Laboratory under the program Superconducting Qubits at Lincoln Laboratory (SQUILL). This material is based upon work supported by the Defense Advanced Research Projects Agency (DARPA) under Agreement No. HR00112490362, the National Science Foundation (NSF) Graduate Research Fellowship Program under Grant No. 2444110, and NSF-NRT QISE under Grant No. 2125924
Presenters
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Jin Ho Kang
- University of California, Los Angeles