Leakage detection for a transmon-based surface code

  1. B. M. Varbanov,
  2. F. Battistel,
  3. B. M. Tarasinski,
  4. V.P. Ostroukh,
  5. T. E. O'Brien,
  6. L. DiCarlo,
  7. and B. M. Terhal
Leakage outside of the qubit computational subspace, present in many leading experimental platforms, constitutes a threatening error for quantum error correction (QEC) for qubits. We
develop a leakage-detection scheme via Hidden Markov models (HMMs) for transmon-based implementations of the surface code. By performing realistic density-matrix simulations of the distance-3 surface code (Surface-17), we observe that leakage is sharply projected and leads to an increase in the surface-code defect probability of neighboring stabilizers. Together with the analog readout of the ancilla qubits, this increase enables the accurate detection of the time and location of leakage. We restore the logical error rate below the memory break-even point by post-selecting out leakage, discarding about 47% of the data. Leakage detection via HMMs opens the prospect for near-term QEC demonstrations, targeted leakage reduction and leakage-aware decoding and is applicable to other experimental platforms.

Protecting quantum entanglement from qubit errors and leakage via repetitive parity measurements

  1. C. C. Bultink,
  2. T. E. O'Brien,
  3. R. Vollmer,
  4. N. Muthusubramanian,
  5. M. W. Beekman,
  6. M. A. Rol,
  7. X. Fu,
  8. B. Tarasinski,
  9. V. Ostroukh,
  10. B. Varbanov,
  11. A. Bruno,
  12. and L. DiCarlo
Protecting quantum information from errors is essential for large-scale quantum computation. Quantum error correction (QEC) encodes information in entangled states of many qubits, and
performs parity measurements to identify errors without destroying the encoded information. However, traditional QEC cannot handle leakage from the qubit computational space. Leakage affects leading experimental platforms, based on trapped ions and superconducting circuits, which use effective qubits within many-level physical systems. We investigate how two-transmon entangled states evolve under repeated parity measurements, and demonstrate the use of hidden Markov models to detect leakage using only the record of parity measurement outcomes required for QEC. We show the stabilization of Bell states over up to 26 parity measurements by mitigating leakage using postselection, and correcting qubit errors using Pauli-frame transformations. Our leakage identification method is computationally efficient and thus compatible with real-time leakage tracking and correction in larger quantum processors.

Error Mitigation by Symmetry Verification on a Variational Quantum Eigensolver

  1. R. Sagastizabal,
  2. X. Bonet-Monroig,
  3. M. Singh,
  4. M. A. Rol,
  5. C. C. Bultink,
  6. X. Fu,
  7. C.H. Price,
  8. V.P. Ostroukh,
  9. N. Muthusubramanian,
  10. A. Bruno,
  11. M. Beekman,
  12. N. Haider,
  13. T. E. O'Brien,
  14. and L. DiCarlo
Variational quantum eigensolvers offer a small-scale testbed to demonstrate the performance of error mitigation techniques with low experimental overhead. We present successful error
mitigation by applying the recently proposed symmetry verification technique to the experimental estimation of the ground-state energy and ground state of the hydrogen molecule. A finely adjustable exchange interaction between two qubits in a circuit QED processor efficiently prepares variational ansatz states in the single-excitation subspace respecting the parity symmetry of the qubit-mapped Hamiltonian. Symmetry verification improves the energy and state estimates by mitigating the effects of qubit relaxation and residual qubit excitation, which violate the symmetry. A full-density-matrix simulation matching the experiment dissects the contribution of these mechanisms from other calibrated error sources. Enforcing positivity of the measured density matrix via scalable convex optimization correlates the energy and state estimate improvements when using symmetry verification, with interesting implications for determining system properties beyond the ground-state energy.

Restless Tuneup of High-Fidelity Qubit Gates

  1. M. A. Rol,
  2. C. C. Bultink,
  3. T. E. O'Brien,
  4. S.R. de Jong,
  5. L.S. Theis,
  6. X. Fu,
  7. F. Luthi,
  8. R.F.L. Vermeulen,
  9. J. C. de Sterke,
  10. A. Bruno,
  11. D. Deurloo,
  12. R. N. Schouten,
  13. F.K. Wilhelm,
  14. and L. DiCarlo
We present a tuneup protocol for qubit gates with tenfold speedup over traditional methods reliant on qubit initialization by energy relaxation. This speedup is achieved by constructing
a cost function for Nelder-Mead optimization from real-time correlation of non-demolition measurements interleaving gate operations without pause. Applying the protocol on a transmon qubit achieves 0.999 average Clifford fidelity in one minute, as independently verified using randomized benchmarking and gate set tomography. The adjustable sensitivity of the cost function allows detecting fractional changes in gate error with nearly constant signal-to-noise ratio. The restless concept demonstrated can be readily extended to the tuneup of two-qubit gates and measurement operations.

Active resonator reset in the nonlinear dispersive regime of circuit QED

  1. C. C. Bultink,
  2. M. A. Rol,
  3. T. E. O'Brien,
  4. X. Fu,
  5. B. C. S. Dikken,
  6. R. Vermeulen,
  7. J. C. de Sterke,
  8. A. Bruno,
  9. R. N. Schouten,
  10. and L. DiCarlo
We present two pulse schemes for actively depleting measurement photons from a readout resonator in the nonlinear dispersive regime of circuit QED. One method uses digital feedback
conditioned on the measurement outcome while the other is unconditional. In the absence of analytic forms and symmetries to exploit in this nonlinear regime, the depletion pulses are numerically optimized using the Powell method. We shorten the photon depletion time by more than six inverse resonator linewidths compared to passive depletion by waiting. We quantify the benefit by emulating an ancilla qubit performing repeated quantum parity checks in a repetition code. Fast depletion increases the mean number of cycles to a spurious error detection event from order 1 to 75 at a 1 microsecond cycle time.