3D integrated superconducting qubits

  1. D. Rosenberg,
  2. D. Kim,
  3. R. Das,
  4. D. Yost,
  5. S. Gustavsson,
  6. D. Hover,
  7. P. Krantz,
  8. A. Melville,
  9. L. Racz,
  10. G. O. Samach,
  11. S. J. Weber,
  12. F. Yan,
  13. J. Yoder,
  14. A.J. Kerman,
  15. and W. D. Oliver
As the field of superconducting quantum computing advances from the few-qubit stage to larger-scale processors, qubit addressability and extensibility will necessitate the use of 3D
integration and packaging. While 3D integration is well-developed for commercial electronics, relatively little work has been performed to determine its compatibility with high-coherence solid-state qubits. Of particular concern, qubit coherence times can be suppressed by the requisite processing steps and close proximity of another chip. In this work, we use a flip-chip process to bond a chip with superconducting flux qubits to another chip containing structures for qubit readout and control. We demonstrate that high qubit coherence (T1, T2,echo>20μs) is maintained in a flip-chip geometry in the presence of galvanic, capacitive, and inductive coupling between the chips.

The Flux Qubit Revisited

  1. F. Yan,
  2. S. Gustavsson,
  3. A. Kamal,
  4. J. Birenbaum,
  5. A. P. Sears,
  6. D. Hover,
  7. T.J. Gudmundsen,
  8. J.L. Yoder,
  9. T. P. Orlando,
  10. J. Clarke,
  11. A.J. Kerman,
  12. and W. D. Oliver
The scalable application of quantum information science will stand on reproducible and controllable high-coherence quantum bits (qubits). In this work, we revisit the design and fabrication
of the superconducting flux qubit, achieving a planar device with broad frequency tunability, strong anharmonicity, high reproducibility, and coherence times in excess of 40 us at its flux-insensitive point. Qubit relaxation times across 21 qubits of widely varying designs are consistently matched with a single model involving ohmic charge noise, quasiparticle fluctuations, resonator loss, and 1/f flux noise, a noise source previously considered primarily in the context of dephasing. We furthermore demonstrate that qubit dephasing at the flux-insensitive point is dominated by residual thermal photons in the readout resonator. The resulting photon shot noise is mitigated using a dynamical decoupling protocol, reaching T2 ~ 80 us , approximately the 2T1 limit. In addition to realizing a dramatically improved flux qubit, our results uniquely identify photon shot noise as limiting T2 in contemporary state-of-art qubits based on transverse qubit-resonator interaction.