Extensible 3D architecture for superconducting quantum computing

  1. Qiang Liu,
  2. Mengmeng Li,
  3. Kunzhe Dai,
  4. Ke Zhang,
  5. Guangming Xue,
  6. Xinsheng Tan,
  7. Haifeng Yu,
  8. and Yang Yu
Using a multi-layered printed circuit board, we propose a 3D architecture suitable for packaging supercon- ducting chips, especially chips that contain two-dimensional qubit arrays.
In our proposed architecture, the center strips of the buried coplanar waveguides protrude from the surface of a dielectric layer as contacts. Since the contacts extend beyond the surface of the dielectric layer, chips can simply be flip-chip packaged with on-chip receptacles clinging to the contacts. Using this scheme, we packaged a multi-qubit chip and per- formed single-qubit and two-qubit quantum gate operations. The results indicate that this 3D architecture provides a promising scheme for scalable quantum computing.

Realizing and manipulating space-time inversion symmetric topological semimetal bands with superconducting quantum circuits

  1. Xinsheng Tan,
  2. Yuxin Zhao,
  3. Qiang Liu,
  4. Guangming Xue,
  5. Haifeng Yu,
  6. Zidan Wang,
  7. and Yang Yu
We have experimentally realized novel space-time inversion (P-T) invariant Z2-type topological semimetal-bands, via an analogy between the momentum space and a controllable parameter
space in superconducting quantum circuits. By measuring the whole energy spectrum of system, we imaged clearly an exotic tunable gapless band structure of topological semimetals. Two topological quantum phase transitions from a topological semimetal to two kinds of insulators can be manipulated by continuously tuning the different parameters in the experimental setup, one of which captures the Z2 topology of the PT semimetal via merging a pair of nontrivial Z2 Dirac points. Remarkably, the topological robustness was demonstrated unambiguously, by adding a perturbation that breaks only the individual T and P symmetries but keeps the joint PT symmetry. In contrast, when another kind of PT -violated perturbation is introduced, a topologically trivial insulator gap is fully opened.