Qubit-compatible substrates with superconducting through-silicon vias

  1. K. Grigoras,
  2. N. Yurttagül,
  3. J.-P. Kaikkonen,
  4. E. T. Mannila,
  5. P. Eskelinen,
  6. D. P. Lozano,
  7. H.-X. Li,
  8. M. Rommel,
  9. D. Shiri,
  10. N. Tiencken,
  11. S. Simbierowicz,
  12. A. Ronzani,
  13. J. Hätinen,
  14. D. Datta,
  15. V. Vesterinen,
  16. L. Grönberg,
  17. J. Biznárová,
  18. A. Fadavi Roudsari,
  19. S. Kosen,
  20. A. Osman,
  21. J. Hassel,
  22. J. Bylander,
  23. and J. Govenius
We fabricate and characterize superconducting through-silicon vias and electrodes suitable for superconducting quantum processors. We measure internal quality factors of a million for
test resonators excited at single-photon levels, when vias are used to stitch ground planes on the front and back sides of the wafer. This resonator performance is on par with the state of the art for silicon-based planar solutions, despite the presence of vias. Via stitching of ground planes is an important enabling technology for increasing the physical size of quantum processor chips, and is a first step toward more complex quantum devices with three-dimensional integration.

Simplified Josephson-junction fabrication process for reproducibly high-performance superconducting qubits

  1. A. Osman,
  2. J. Simon,
  3. A. Bengtsson,
  4. S. Kosen,
  5. P. Krantz,
  6. D. Perez,
  7. M. Scigliuzzo,
  8. Jonas Bylander,
  9. and A. Fadavi Roudsari
We introduce a simplified fabrication technique for Josephson junctions and demonstrate superconducting Xmon qubits with T1 relaxation times averaging above 50 μs (Q>1.5× 106). Current
shadow-evaporation techniques for aluminum-based Josephson junctions require a separate lithography step to deposit a patch that makes a galvanic, superconducting connection between the junction electrodes and the circuit wiring layer. The patch connection eliminates parasitic junctions, which otherwise contribute significantly to dielectric loss. In our patch-integrated cross-type (PICT) junction technique, we use one lithography step and one vacuum cycle to evaporate both the junction electrodes and the patch. In a study of more than 3600 junctions, we show an average resistance variation of 3.7% on a wafer that contains forty 0.5×0.5-cm2 chips, with junction areas ranging between 0.01 and 0.16 μm2. The average on-chip spread in resistance is 2.7%, with 20 chips varying between 1.4 and 2%. For the junction sizes used for transmon qubits, we deduce a wafer-level transition-frequency variation of 1.7-2.5%. We show that 60-70% of this variation is attributed to junction-area fluctuations, while the rest is caused by tunnel-junction inhomogeneity. Such high frequency predictability is a requirement for scaling-up the number of qubits in a quantum computer.