Heteroepitaxial oxide/α-Ta(110) films on sapphire(11-20) – growth, structure, transport, and microwave properties

ORAL

Abstract

For building high-performance superconducting qubits and supportive circuits like a high-Q microwave resonator, we need to precisely control material properties in film crystallinity, hetero-interfaces, and capped oxide layer. Ta superconducting films are usually exposed to air, inevitably forming a native oxide layer, which may enhance energy relaxation channels such as two-level systems (TLS) for superconducting circuits.1 Here, growth of heteroepitaxial deposited-oxide/α-Ta films on a-plane sapphire substrates was achieved in a multi-chamber UHV system.2,3 The research aims to investigate the microwave properties of the in-situ deposited heterostructures to understand dielectric losses in superconducting quantum circuits.

α-Ta films 35 nm in thickness grew epitaxially in (110) orientation on (11-20) sapphire substrates, followed with in-situ growth of epitaxial and amorphous Al2O3 films. The presence of Pendellösung fringes indicates a high degree of structural coherence over the entire film thickness. The root mean square roughness of the Ta films is 0.8 nm. After the in-situ oxide deposition, the surface roughness decreases to 0.47 nm. The Ta film has a critical temperature of 4.29 K and a high residual resistance ratio of 16.



1. Crowley et al., PRX 13, 041005 (2023).

2. Kwo et al., Appl. Phys. Lett. 49, 319 (1986).

3. Lin et al., J. Cryst. Growth 512, 223 (2019).

* The support from the Natl. Sci. Technol. Council in Taiwan through NSTC 112-2119-M-007-009 and 112-2811-M-007-056 is acknowledged.

Presenters

  • Yi-Ting Cheng

    National Tsing Hua University, Department of Physics, National Tsing Hua University

Authors

  • Yi-Ting Cheng

    National Tsing Hua University, Department of Physics, National Tsing Hua University

  • Hsien-Wen Wan

    Graduate Institute of Applied Physics and Dept. of Physics, National Taiwan University, Graduate Institute of Applied Physics and Department of Physics, National Taiwan University, National Taiwan University

  • Chao-Kai Cheng

    Graduate Institute of Applied Physics and Dept. of Physics, National Taiwan University, National Taiwan University, Graduate Institute of Applied Physics and Department of Physics, National Taiwan University

  • Ko-Hsuan Chen

    Department of Physics, National Tsing Hua University

  • Jui-Min Chia

    Department of Physics, National Tsing Hua University

  • Chia-Hung Hsu

    National Synchrotron Radiation Research Center, Hsinchu 30076, Taiwan, Scientific Research Division, NSRRC, Hsinchu, National Synchrotron Radiation Research Center

  • Yen-Hsiang Lin

    Department of Physics, National Tsing Hua University

  • Jueinai Kwo

    National Tsing Hua University, Department of Physics, National Tsing Hua University, Natl Tsing Hua Univ

  • Minghwei Hong

    National Taiwan University, Graduate Institute of Applied Physics and Dept. of Physics, National Taiwan University, Graduate Institute of Applied Physics and Department of Physics, National Taiwan University, Natl Taiwan Univ