The squeezed Kerr oscillator: spectral kissing and phase-flip robustness

  1. Nicholas E. Frattini,
  2. Rodrigo G. Cortiñas,
  3. Jayameenakshi Venkatraman,
  4. Xu Xiao,
  5. Qile Su,
  6. Chan U Lei,
  7. Benjamin J. Chapman,
  8. Vidul R. Joshi,
  9. S. M. Girvin,
  10. Robert J. Schoelkopf,
  11. Shruti Puri,
  12. and Michel H. Devoret
By applying a microwave drive to a specially designed Josephson circuit, we have realized an elementary quantum optics model, the squeezed Kerr oscillator. This model displays, as the
squeezing amplitude is increased, a cross-over from a single ground state regime to a doubly-degenerate ground state regime. In the latter case, the ground state manifold is spanned by Schrödinger-cat states, i.e. quantum superpositions of coherent states with opposite phases. For the first time, having resolved up to the tenth excited state in a spectroscopic experiment, we confirm that the proposed emergent static effective Hamiltonian correctly describes the system, despite its driven character. We also find that the lifetime of the coherent state components of the cat states increases in steps as a function of the squeezing amplitude. We interpret the staircase pattern as resulting from pairwise level kissing in the excited state spectrum. Considering the Kerr-cat qubit encoded in this ground state manifold, we achieve for the first time quantum nondemolition readout fidelities greater than 99%, and enhancement of the phase-flip lifetime by more than two orders of magnitude, while retaining universal quantum control. Our experiment illustrates the crucial role of parametric drive Hamiltonian engineering for hardware-efficient quantum computation.

Distinguishing parity-switching mechanisms in a superconducting qubit

  1. Spencer Diamond,
  2. Valla Fatemi,
  3. Max Hays,
  4. Heekun Nho,
  5. Pavel D. Kurilovich,
  6. Thomas Connolly,
  7. Vidul R. Joshi,
  8. Kyle Serniak,
  9. Luigi Frunzio,
  10. Leonid I. Glazman,
  11. and Michel H. Devoret
Single-charge tunneling is a decoherence mechanism affecting superconducting qubits, yet the origin of excess quasiparticle excitations (QPs) responsible for this tunneling in superconducting
devices is not fully understood. We measure the flux dependence of charge-parity (or simply, „parity“) switching in an offset-charge-sensitive transmon qubit to identify the contributions of photon-assisted parity switching and QP generation to the overall parity-switching rate. The parity-switching rate exhibits a qubit-state-dependent peak in the flux dependence, indicating a cold distribution of excess QPs which are predominantly trapped in the low-gap film of the device. Moreover, we find that the photon-assisted process contributes significantly to both parity switching and the generation of excess QPs by fitting to a model that self-consistently incorporates photon-assisted parity switching as well as inter-film QP dynamics.