Demonstrating Quantum Error Correction that Extends the Lifetime of Quantum Information

  1. Nissim Ofek,
  2. Andrei Petrenko,
  3. Reinier Heeres,
  4. Philip Reinhold,
  5. Zaki Leghtas,
  6. Brian Vlastakis,
  7. Yehan Liu,
  8. Luigi Frunzio,
  9. S. M. Girvin,
  10. Liang Jiang,
  11. Mazyar Mirrahimi,
  12. M. H. Devoret,
  13. and R. J. Schoelkopf
The remarkable discovery of Quantum Error Correction (QEC), which can overcome the errors experienced by a bit of quantum information (qubit), was a critical advance that gives hope
for eventually realizing practical quantum computers. In principle, a system that implements QEC can actually pass a „break-even“ point and preserve quantum information for longer than the lifetime of its constituent parts. Reaching the break-even point, however, has thus far remained an outstanding and challenging goal. Several previous works have demonstrated elements of QEC in NMR, ions, nitrogen vacancy (NV) centers, photons, and superconducting transmons. However, these works primarily illustrate the signatures or scaling properties of QEC codes rather than test the capacity of the system to extend the lifetime of quantum information over time. Here we demonstrate a QEC system that reaches the break-even point by suppressing the natural errors due to energy loss for a qubit logically encoded in superpositions of coherent states, or cat states of a superconducting resonator. Moreover, the experiment implements a full QEC protocol by using real-time feedback to encode, monitor naturally occurring errors, decode, and correct. As measured by full process tomography, the enhanced lifetime of the encoded information is 320 microseconds without any post-selection. This is 20 times greater than that of the system’s transmon, over twice as long as an uncorrected logical encoding, and 10% longer than the highest quality element of the system (the resonator’s 0, 1 Fock states). Our results illustrate the power of novel, hardware efficient qubit encodings over traditional QEC schemes. Furthermore, they advance the field of experimental error correction from confirming the basic concepts to exploring the metrics that drive system performance and the challenges in implementing a fault-tolerant system.

Comparing and combining measurement-based and driven-dissipative entanglement stabilization

  1. Yehan Liu,
  2. Shyam Shankar,
  3. Nissim Ofek,
  4. Michael Hatridge,
  5. Anirudh Narla,
  6. Katrina Sliwa,
  7. Luigi Frunzio,
  8. Robert J. Schoelkopf,
  9. and Michel H. Devoret
We demonstrate and contrast two approaches to the stabilization of qubit entanglement by feedback. Our demonstration is built on a feedback platform consisting of two superconducting
qubits coupled to a cavity which are measured by a nearly-quantum-limited measurement chain and controlled by high-speed classical logic circuits. This platform is used to stabilize entanglement by two nominally distinct schemes: a „passive“ reservoir engineering method and an „active“ correction based on conditional parity measurements. In view of the instrumental roles that these two feedback paradigms play in quantum error-correction and quantum control, we directly compare them on the same experimental setup. Further, we show that a second layer of feedback can be added to each of these schemes, which heralds the presence of a high-fidelity entangled state in realtime. This „nested“ feedback brings about a marked entanglement fidelity improvement without sacrificing success probability.

Violating Bell’s inequality with an artificial atom and a cat state in a cavity

  1. Brian Vlastakis,
  2. Andrei Petrenko,
  3. Nissim Ofek,
  4. Luayn Sun,
  5. Zaki Leghtas,
  6. Katrina Sliwa,
  7. Yehan Liu,
  8. Michael Hatridge,
  9. Jacob Blumoff,
  10. Luigi Frunzio,
  11. Mazyar Mirrahimi,
  12. Liang Jiang,
  13. M. H. Devoret,
  14. and R. J. Schoelkopf
The `Schr“odinger’s cat‘ thought experiment highlights the counterintuitive facet of quantum theory that entanglement can exist between microscopic and macroscopic
systems, producing a superposition of distinguishable states like the fictitious cat that is both alive and dead. The hallmark of entanglement is the detection of strong correlations between systems, for example by the violation of Bell’s inequality. Using the CHSH variant of the Bell test, this violation has been observed with photons, atoms, solid state spins, and artificial atoms in superconducting circuits. For larger, more distinguishable states, the conflict between quantum predictions and our classical expectations is typically resolved due to the rapid onset of decoherence. To investigate this reconciliation, one can employ a superposition of coherent states in an oscillator, known as a cat state. In contrast to discrete systems, one can continuously vary the size of the prepared cat state and therefore its dependence on decoherence. Here we demonstrate and quantify entanglement between an artificial atom and a cat state in a cavity, which we call a `Bell-cat‘ state. We use a circuit QED architecture, high-fidelity measurements, and real-time feedback control to violate Bell’s inequality without post-selection or corrections for measurement inefficiencies. Furthermore, we investigate the influence of decoherence by continuously varying the size of created Bell-cat states and characterize the entangled system by joint Wigner tomography. These techniques provide a toolset for quantum information processing with entangled qubits and resonators. While recent results have demonstrated a high level of control of such systems, this experiment demonstrates that information can be extracted efficiently and with high fidelity, a crucial requirement for quantum computing with resonators.