Transmon Qubit Chip on Single-Crystal Tantalum (110) film

ORAL

Abstract

Recent reports on using Ta films to replace Nb films as the platform for superconducting qubits show longer relaxation time [1][2] and potential for applications in quantum circuit dynamics. However, how the crystallinity of Ta films affect the qubit relaxation time remains relatively unexplored. Here, we study the transmon qubits and coplanar waveguide resonators fabricated on single-crystalline and polycrystalline Ta(110) films grown on sapphire substrates. The fabrication processes were optimized to minimize loss. The fabricated chips were characterized in a dilution refrigerator at 10 mK. Quarter-wavelength resonators were coupled to a common feedline. The internal quality factors (Qi) of the resonators were extracted by fitting the measured transmission (S21) across the feedline. The relaxation time (T1) and coherence time (T2) were obtained by time-domain microwave measurements. Our results indicate that single-crystalline Ta(110) films exhibit lower two-level system (TLS) loss compared to polycrystalline Ta films. The resonator internal quality factor at low photon number limit (QLP) suggests that there are more TLS defects in the polycrystalline Ta film. Transmon qubits fabricated on single-crystalline Ta films show ~50% longer T1 time than those fabricated on polycrystalline Ta films. Our work unveils the impacts of grain boundaries (through which TLS may form) on the overall loss tangents. The higher quality factors and longer T1 time demonstrate the promise of using single-crystal Ta films for developing high-quality quantum circuits.

Publication: [1] A. P. M. Place et al., New material platform for superconducting transmon qubits with coherence times exceeding 0.3 milliseconds, Nat. Comm. 12, 1779 (2021).
[2] C. Wang et al., Towards practical quantum computers: transmon qubit with a lifetime approaching 0.5 milliseconds, npj Quantum Information 8, 3 (2022).

Presenters

  • Ping-Lien Lee

    • National Yang Ming Chiao Tung University
    • Department of Electrophysics, National Yang Ming Chiao Tung University

Authors

  • Ping-Lien Lee

    • National Yang Ming Chiao Tung University
    • Department of Electrophysics, National Yang Ming Chiao Tung University
  • Chih-Yao Shih

    • National Yang Ming Chiao Tung University
    • Department of Electrophysics, National Yang Ming Chiao Tung University
  • Hsiang-Huan Lee

    • Department of Electrophysics, National Yang Ming Chiao Tung University
  • Jaw-Shen Tsai

    • RIKEN Center for Quantum Computing (RQC)
  • Sheng-Shiuan Yeh

    • International College of Semiconductor Technology, National Yang Ming Chiao Tung University, Hsinchu 30010
    • International College of Semiconductor Technology, National Yang Ming Chiao Tung University
  • Wen-Hao Chang

    • Department of Electrophysics, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
    • Academia Sinica
    • National Yang Ming Chiao Tung University, Academia Sinica
    • Department of Electrophysics, National Yang Ming Chiao Tung University