High-fidelity optical readout of a superconducting qubit using a scalable piezo-optomechanical transducer

  1. T.C. van Thiel,
  2. M.J. Weaver,
  3. F. Berto,
  4. P. Duivestein,
  5. M. Lemang,
  6. K. Schuurman,
  7. M. Žemlička,
  8. F. Hijazi,
  9. A.C. Bernasconi,
  10. E. Lachman,
  11. M. Field,
  12. Y. Mohan,
  13. F. de Vries,
  14. N. Bultink,
  15. J. van Oven,
  16. J. Y. Mutus,
  17. R. Stockill,
  18. and S. Gröblacher
Superconducting quantum processors have made significant progress in size and computing potential. As a result, the practical cryogenic limitations of operating large numbers of superconductingqubits are becoming a bottleneck for further scaling. Due to the low thermal conductivity and the dense optical multiplexing capacity of telecommunications fiber, converting qubit signal processing to the optical domain using microwave-to-optics transduction would significantly relax the strain on cryogenic space and thermal budgets. Here, we demonstrate high-fidelity multi-shot optical readout through an optical fiber of a superconducting transmon qubit connected via a coaxial cable to a fully integrated piezo-optomechanical transducer. Using a demolition readout technique, we achieve a multi-shot readout fidelity of >99% at 6 μW of optical power transmitted into the cryostat with as few as 200 averages, without the use of a quantum-limited amplifier. With improved frequency matching between the transducer and the qubit readout resonator, we anticipate that single-shot optical readout is achievable. Due to the small footprint (<0.15mm2) and the modular fiber-based architecture, this device platform has the potential to scale towards use with thousands of qubits. Our results illustrate the potential of piezo-optomechanical transduction for low-dissipation operation of large quantum processors.[/expand]

Demonstration of Universal Parametric Entangling Gates on a Multi-Qubit Lattice

  1. M. Reagor,
  2. C. B. Osborn,
  3. N. Tezak,
  4. A. Staley,
  5. G. Prawiroatmodjo,
  6. M. Scheer,
  7. N. Alidoust,
  8. E. A. Sete,
  9. N. Didier,
  10. M. P. da Silva,
  11. E. Acala,
  12. J. Angeles,
  13. A. Bestwick,
  14. M. Block,
  15. B. Bloom,
  16. A. Bradley,
  17. C. Bui,
  18. S. Caldwell,
  19. L. Capelluto,
  20. R. Chilcott,
  21. J. Cordova,
  22. G. Crossman,
  23. M. Curtis,
  24. S. Deshpande,
  25. T. El Bouayadi,
  26. D. Girshovich,
  27. S. Hong,
  28. A. Hudson,
  29. P. Karalekas,
  30. K. Kuang,
  31. M. Lenihan,
  32. R. Manenti,
  33. T. Manning,
  34. J. Marshall,
  35. Y. Mohan,
  36. W. O'Brien,
  37. J. Otterbach,
  38. A. Papageorge,
  39. J.-P. Paquette,
  40. M. Pelstring,
  41. A. Polloreno,
  42. V. Rawat,
  43. C. A. Ryan,
  44. R. Renzas,
  45. N. Rubin,
  46. D. Russell,
  47. M. Rust,
  48. D. Scarabelli,
  49. M. Selvanayagam,
  50. R. Sinclair,
  51. R. Smith,
  52. M. Suska,
  53. T.-W. To,
  54. M. Vahidpour,
  55. N. Vodrahalli,
  56. T. Whyland,
  57. K. Yadav,
  58. W. Zeng,
  59. and C. T. Rigetti
We show that parametric coupling techniques can be used to generate selective entangling interactions for multi-qubit processors. By inducing coherent population exchange between adjacent
qubits under frequency modulation, we implement a universal gateset for a linear array of four superconducting qubits. An average process fidelity of =93% is measured by benchmarking three two-qubit gates with quantum process tomography. In order to test the suitability of these techniques for larger computations, we prepare a six-qubit register in all possible bitstring permutations and monitor the performance of a two-qubit gate on another pair of qubits. Across all these experiments, an average fidelity of =91.6±2.6% is observed. These results thus offer a path to a scalable architecture with high selectivity and low crosstalk.

Parametrically-Activated Entangling Gates Using Transmon Qubits

  1. S. Caldwell,
  2. N. Didier,
  3. C. A. Ryan,
  4. E. A. Sete,
  5. A. Hudson,
  6. P. Karalekas,
  7. R. Manenti,
  8. M. Reagor,
  9. M. P. da Silva,
  10. R. Sinclair,
  11. E. Acala,
  12. N. Alidoust,
  13. J. Angeles,
  14. A. Bestwick,
  15. M. Block,
  16. B. Bloom,
  17. A. Bradley,
  18. C. Bui,
  19. L. Capelluto,
  20. R. Chilcott,
  21. J. Cordova,
  22. G. Crossman,
  23. M. Curtis,
  24. S. Deshpande,
  25. T. El Bouayadi,
  26. D. Girshovich,
  27. S. Hong,
  28. K. Kuang,
  29. M. Lenihan,
  30. T. Manning,
  31. J. Marshall,
  32. Y. Mohan,
  33. W. O'Brien,
  34. C. Osborn,
  35. J. Otterbach,
  36. A. Papageorge,
  37. J.-P. Paquette,
  38. M. Pelstring,
  39. A. Polloreno,
  40. G. Prawiroatmodjo,
  41. V. Rawat,
  42. R. Renzas,
  43. N. Rubin,
  44. D. Russell,
  45. M. Rust,
  46. D. Scarabelli,
  47. M. Scheer,
  48. M. Selvanayagam,
  49. R. Smith,
  50. A. Staley,
  51. M. Suska,
  52. N. Tezak,
  53. T.-W. To,
  54. M. Vahidpour,
  55. N. Vodrahalli,
  56. T. Whyland,
  57. K. Yadav,
  58. W. Zeng,
  59. and C. Rigetti
We propose and implement a family of entangling qubit operations activated by radio-frequency flux pulses. By parametrically modulating the frequency of a tunable transmon, these operations
selectively actuate resonant exchange of excitations with a statically coupled, but otherwise off-resonant, neighboring transmon. This direct exchange of excitations between qubits obviates the need for mediator qubits or resonator modes, and it allows for the full utilization of all qubits in a scalable architecture. Moreover, we are able to activate three highly-selective resonances, corresponding to two different classes of entangling gates that enable universal quantum computation: an iSWAP and a controlled-Z rotation. This selectivity is enabled by resonance conditions that depend both on frequency and amplitude, and is helpful in avoiding frequency crowding in a scalable architecture. We report average process fidelities of F = 0.93 for a 135 ns iSWAP, and F = 0.92 for 175 ns and 270 ns controlled-Z operations.