Identification and Mitigation of Conducting Package Losses for Quantum Superconducting Devices

  1. Yizhou Huang,
  2. Yi-Hsiang Huang,
  3. Haozhi Wang,
  4. Zach Steffen,
  5. Jonathan Cripe,
  6. F. C. Wellstood,
  7. and B. S. Palmer
Low-loss superconducting microwave devices are required for quantum computation. Here, we present a series of measurements and simulations showing that conducting losses in the packaging
of our superconducting resonator devices affect the maximum achievable internal quality factors (Qi) for a series of thin-film Al quarter-wave resonators with fundamental resonant frequencies varying between 4.9 and 5.8 GHz. By utilizing resonators with different widths and gaps, we sampled different electromagnetic energy volumes for the resonators affecting Qi. When the backside of the sapphire substrate of the resonator device is adhered to a Cu package with a conducting silver glue, a monotonic decrease in the maximum achievable Qi is found as the electromagnetic sampling volume is increased. This is a result of induced currents in large surface resistance regions and dissipation underneath the substrate. By placing a hole underneath the substrate and using superconducting material for the package, we decrease the ohmic losses and increase the maximum Qi for the larger size resonators.

Characterization of Asymmetric Gap-Engineered Josephson Junctions and 3D Transmon Qubits

  1. Zach Steffen,
  2. S. K. Dutta,
  3. Haozhi Wang,
  4. Kungang Li,
  5. Yizhou Huang,
  6. Yi-Hsiang Huang,
  7. Advait Mathur,
  8. F. C. Wellstood,
  9. and B. S. Palmer
We have fabricated and characterized asymmetric gap-engineered junctions and transmon devices. To create Josephson junctions with asymmetric gaps, Ti was used to proximitize and lower
the superconducting gap of the Al counter-electrode. DC IV measurements of these small, proximitized Josephson junctions show a reduced gap and larger excess current for voltage biases below the superconducting gap when compared to standard Al/AlOx/Al junctions. The energy relaxation time constant for an Al/AlOx/Al/Ti 3D transmon was T1 = 1 {\mu}s, over two orders of magnitude shorter than the measured T1 = 134 {\mu}s of a standard Al/AlOx/Al 3D transmon. Intentionally adding disorder between the Al and Ti layers reduces the proximity effect and subgap current while increasing the relaxation time to T1 = 32 {\mu}s.

Perspective: Reproducible Coherence Characterization of Superconducting Quantum Devices

  1. Corey Rae H McRae,
  2. Gregory M Stiehl,
  3. Haozhi Wang,
  4. Sheng-Xiang Lin,
  5. Shane A. Caldwell,
  6. David P. Pappas,
  7. Josh Mutus,
  8. and Joshua Combes
As the field of superconducting quantum computing approaches maturity, optimization of single-device performance is proving to be a promising avenue towards large-scale quantum computers.
However, this optimization is possible only if performance metrics can be accurately compared among measurements, devices, and laboratories. Currently such comparisons are inaccurate or impossible due to understudied errors from a plethora of sources. In this Perspective, we outline the current state of error analysis for qubits and resonators in superconducting quantum circuits, and discuss what future investigations are required before superconducting quantum device optimization can be realized.

Cryogenic single-port calibration for superconducting microwave resonator measurements

  1. Haozhi Wang,
  2. S. Singh,
  3. C.R.H. McRae,
  4. J.C. Bardin,
  5. S.-X. Lin,
  6. N. Messaoudi,
  7. A.R. Castelli,
  8. Y. J. Rosen,
  9. E. T. Holland,
  10. D. P. Pappas,
  11. and J. Y. Mutus
Superconducting circuit testing and materials loss characterization requires robust and reliable methods for the extraction of internal and coupling quality factors of microwave resonators.
A common method, imposed by limitations on the device design or experimental configuration, is the single-port reflection geometry, i.e. reflection-mode. However, impedance mismatches in cryogenic systems must be accounted for through calibration of the measurement chain while it is at low temperatures. In this paper, we demonstrate a data-based, single-port calibration using commercial microwave standards and a vector network analyzer (VNA) with samples at millikelvin temperature in a dilution refrigerator, making this method useful for measurements of quantum phenomena. Finally, we cross reference our data-based, single-port calibration and reflection measurement with over-coupled 2D- and 3D-resonators against well established two-port techniques corroborating the validity of our method.

Materials loss measurements using superconducting microwave resonators

  1. Corey Rae Harrington McRae,
  2. Haozhi Wang,
  3. Jiansong Gao,
  4. Michael Vissers,
  5. Teresa Brecht,
  6. Andrew Dunsworth,
  7. David Pappas,
  8. and Josh Mutus
The performance of superconducting circuits for quantum computing is limited by materials losses. In particular, coherence times are typically bounded by two-level system (TLS) losses
at single photon powers and millikelvin temperatures. The identification of low loss fabrication techniques, materials, and thin film dielectrics is critical to achieving scalable architectures for superconducting quantum computing. Superconducting microwave resonators provide a convenient qubit proxy for assessing performance and studying TLS loss and other mechanisms relevant to superconducting circuits such as non-equilibrium quasiparticles and magnetic flux vortices. In this review article, we provide an overview of considerations for designing accurate resonator experiments to characterize loss, including applicable types of loss, cryogenic setup, device design, and methods for extracting material and interface losses, summarizing techniques that have been evolving for over two decades. Results from measurements of a wide variety of materials and processes are also summarized. Lastly, we present recommendations for the reporting of loss data from superconducting microwave resonators to facilitate materials comparisons across the field.

Overlap junctions for superconducting quantum electronics and amplifiers

  1. Mustafa Bal,
  2. Junling Long,
  3. Ruichen Zhao,
  4. Haozhi Wang,
  5. Sungoh Park,
  6. Corey Rae Harrington McRae,
  7. Tongyu Zhao,
  8. Russell E. Lake,
  9. Daniil Frolov,
  10. Roman Pilipenko,
  11. Silvia Zorzetti,
  12. Alexander Romanenko,
  13. and David P. Pappas
Due to their unique properties as lossless, nonlinear circuit elements, Josephson junctions lie at the heart of superconducting quantum information processing. Previously, we demonstrated
a two-layer, submicrometer-scale overlap junction fabrication process suitable for qubits with long coherence times. Here, we extend the overlap junction fabrication process to micrometer-scale junctions. This allows us to fabricate other superconducting quantum devices. For example, we demonstrate an overlap-junction-based Josephson parametric amplifier that uses only 2 layers. This efficient fabrication process yields frequency-tunable devices with negligible insertion loss and a gain of ~ 30 dB. Compared to other processes, the overlap junction allows for fabrication with minimal infrastructure, high yield, and state-of-the-art device performance.

Superconducting metamaterials and qubits

  1. B. L. T. Plourde,
  2. Haozhi Wang,
  3. Francisco Rouxinol,
  4. and M. D. LaHaye
Superconducting thin-film metamaterial resonators can provide a dense microwave mode spectrum with potential applications in quantum information science. We report on the fabrication
and low-temperature measurement of metamaterial transmission-line resonators patterned from Al thin films. We also describe multiple approaches for numerical simulations of the microwave properties of these structures, along with comparisons with the measured transmission spectra. The ability to predict the mode spectrum based on the chip layout provides a path towards future designs integrating metamaterial resonators with superconducting qubits.