Effects of surface treatments on flux tunable transmon qubits

  1. M. Mergenthaler,
  2. C. Müller,
  3. M. Ganzhorn,
  4. S. Paredes,
  5. P. Müller,
  6. G. Salis,
  7. V. P. Adiga,
  8. M. Brink,
  9. M. Sandberg,
  10. J. B. Hertzberg,
  11. S. Filipp,
  12. and A. Fuhrer
One of the main limitations in state-of-the art solid-state quantum processors are qubit decoherence and relaxation due to noise in their local environment. For the field to advance
towards full fault-tolerant quantum computing, a better understanding of the underlying microscopic noise sources is therefore needed. Adsorbates on surfaces, impurities at interfaces and material defects have been identified as sources of noise and dissipation in solid-state quantum devices. Here, we use an ultra-high vacuum package to study the impact of vacuum loading, UV-light exposure and ion irradiation treatments on coherence and slow parameter fluctuations of flux tunable superconducting transmon qubits. We analyse the effects of each of these surface treatments by comparing averages over many individual qubits and measurements before and after treatment. The treatments studied do not significantly impact the relaxation rate Γ1 and the echo dephasing rate Γe2, except for Ne ion bombardment which reduces Γ1. In contrast, flux noise parameters are improved by removing magnetic adsorbates from the chip surfaces with UV-light and NH3 treatments. Additionally, we demonstrate that SF6 ion bombardment can be used to adjust qubit frequencies in-situ and post fabrication without affecting qubit coherence at the sweet spot.

Ultrahigh Vacuum Packaging and Surface Cleaning for Quantum Devices

  1. M. Mergenthaler,
  2. S. Paredes,
  3. P. Müller,
  4. C. Müller,
  5. S. Filipp,
  6. M. Sandberg,
  7. J. Hertzberg,
  8. V. P. Adiga,
  9. M. Brink,
  10. and A. Fuhrer
We describe design, implementation and performance of an ultra-high vacuum (UHV) package for superconducting qubit chips or other surface sensitive quantum devices. The UHV loading
procedure allows for annealing, ultra-violet light irradiation, ion milling and surface passivation of quantum devices before sealing them into a measurement package. The package retains vacuum during the transfer to cryogenic temperatures by active pumping with a titanium getter layer. We characterize the treatment capabilities of the system and present measurements of flux tunable qubits with an average T1=84 μs and Techo2=134 μs after vacuum-loading these samples into a bottom loading dilution refrigerator in the UHV-package.

Benchmarking the noise sensitivity of different parametric two-qubit gates in a single superconducting quantum computing platform

  1. M. Ganzhorn,
  2. G. Salis,
  3. D. J. Egger,
  4. A. Fuhrer,
  5. M. Mergenthaler,
  6. C. Müller,
  7. P. Müller,
  8. S. Paredes,
  9. M. Pechal,
  10. M. Werninghaus,
  11. and S. Filipp
The possibility to utilize different types of two-qubit gates on a single quantum computing platform adds flexibility in the decomposition of quantum algorithms. A larger hardware-native
gate set may decrease the number of required gates, provided that all gates are realized with high fidelity. Here, we benchmark both controlled-Z (CZ) and exchange-type (iSWAP) gates using a parametrically driven tunable coupler that mediates the interaction between two superconducting qubits. Using randomized benchmarking protocols we estimate an error per gate of 0.9±0.03% and 1.3±0.4% fidelity for the CZ and the iSWAP gate, respectively. We argue that spurious ZZ-type couplings are the dominant error source for the iSWAP gate, and that phase stability of all microwave drives is of utmost importance. Such differences in the achievable fidelities for different two-qubit gates have to be taken into account when mapping quantum algorithms to real hardware.

Quantum Zeno effect in the strong measurement regime of circuit quantum electrodynamics

  1. D. H. Slichter,
  2. C. Müller,
  3. R. Vijay,
  4. S. J. Weber,
  5. A. Blais,
  6. and I. Siddiqi
We observe the quantum Zeno effect — where the act of measurement slows the rate of quantum state transitions — in a superconducting qubit using linear circuit quantum electrodynamics
readout and a near-quantum-limited following amplifier. Under simultaneous strong measurement and qubit drive, the qubit undergoes a series of quantum jumps between states. These jumps are visible in the experimental measurement record and are analyzed using maximum likelihood estimation to determine qubit transition rates. The observed rates agree with both analytical predictions and numerical simulations. The analysis methods are suitable for processing general noisy random telegraph signals