Quantum bath suppression in a superconducting circuit by immersion cooling

  1. M. Lucas,
  2. A. V. Danilov,
  3. L. V. Levitin,
  4. A. Jayaraman,
  5. A. J. Casey,
  6. L. Faoro,
  7. A. Ya. Tzalenchuk,
  8. S. E. Kubatkin,
  9. J. Saunders,
  10. and S. E. de Graaf
Quantum circuits interact with the environment via several temperature-dependent degrees of freedom. Yet, multiple experiments to-date have shown that most properties of superconducting
devices appear to plateau out at T≈50 mK — far above the refrigerator base temperature. This is for example reflected in the thermal state population of qubits, in excess numbers of quasiparticles, and polarisation of surface spins — factors contributing to reduced coherence. We demonstrate how to remove this thermal constraint by operating a circuit immersed in liquid 3He. This allows to efficiently cool the decohering environment of a superconducting resonator, and we see a continuous change in measured physical quantities down to previously unexplored sub-mK temperatures. The 3He acts as a heat sink which increases the energy relaxation rate of the quantum bath coupled to the circuit a thousand times, yet the suppressed bath does not introduce additional circuit losses or noise. Such quantum bath suppression can reduce decoherence in quantum circuits and opens a route for both thermal and coherence management in quantum processors.

Correlated Charge Noise and Relaxation Errors in Superconducting Qubits

  1. C. D. Wilen,
  2. S. Abdullah,
  3. N. A. Kurinsky,
  4. C. Stanford,
  5. L. Cardani,
  6. G. D'Imperio,
  7. C. Tomei,
  8. L. Faoro,
  9. L.B. Ioffe,
  10. C. H. Liu,
  11. A. Opremcak,
  12. B. G. Christensen,
  13. J. L. DuBois,
  14. and R. McDermott
The central challenge in building a quantum computer is error correction. Unlike classical bits, which are susceptible to only one type of error, quantum bits („qubits“)
are susceptible to two types of error, corresponding to flips of the qubit state about the X- and Z-directions. While the Heisenberg Uncertainty Principle precludes simultaneous monitoring of X- and Z-flips on a single qubit, it is possible to encode quantum information in large arrays of entangled qubits that enable accurate monitoring of all errors in the system, provided the error rate is low. Another crucial requirement is that errors cannot be correlated. Here, we characterize a superconducting multiqubit circuit and find that charge fluctuations are highly correlated on a length scale over 600~μm; moreover, discrete charge jumps are accompanied by a strong transient suppression of qubit energy relaxation time across the millimeter-scale chip. The resulting correlated errors are explained in terms of the charging event and phonon-mediated quasiparticle poisoning associated with absorption of gamma rays and cosmic-ray muons in the qubit substrate. Robust quantum error correction will require the development of mitigation strategies to protect multiqubit arrays from correlated errors due to particle impacts.

Two-level systems in superconducting quantum devices due to trapped quasiparticles

  1. S. E. de Graaf,
  2. L. Faoro,
  3. L.B. Ioffe,
  4. S. Mahashabde,
  5. J. J. Burnett,
  6. T. Lindström,
  7. S. E. Kubatkin,
  8. A. V. Danilov,
  9. and A. Ya. Tzalenchuk
A major issue for the implementation of large scale superconducting quantum circuits is the interaction with interfacial two-level system defects (TLS) that leads to qubit relaxation
and impedes qubit operation in certain frequency ranges that also drift in time. Another major challenge comes from non-equilibrium quasiparticles (QPs) that result in qubit dephasing and relaxation. In this work we show that such QPs can also serve as a source of TLS. Using spectral and temporal mapping of TLS-induced fluctuations in frequency tunable resonators, we identify a subset of the general TLS population that are highly coherent TLS with a low reconfiguration temperature ∼ 300 mK, and a non-uniform density of states. These properties can be understood if these TLS are formed by QPs trapped in shallow subgap states formed by spatial fluctutations of the superconducting order parameter Δ. Magnetic field measurements of one such TLS reveals a link to superconductivity. Our results imply that trapped QPs can induce qubit relaxation.

Anomalous Charge Noise in Superconducting Qubits

  1. B. G. Christensen,
  2. C. D. Wilen,
  3. A. Opremcak,
  4. J. Nelson,
  5. F. Schlenker,
  6. C. H. Zimonick,
  7. L. Faoro,
  8. L.B. Ioffe,
  9. Y. J. Rosen,
  10. J. L. DuBois,
  11. B. L. T. Plourde,
  12. and R. McDermott
We have used Ramsey tomography to characterize charge noise in a weakly charge-sensitive superconducting qubit. We find a charge noise that scales with frequency as 1/fα over 5 decades
with α=1.93 and a magnitude Sq(1Hz)=2.9×10−4 e2/Hz. The noise exponent and magnitude of the low-frequency noise are much larger than those seen in prior work on single electron transistors, yet are consistent with reports of frequency noise in other superconducting qubits. Moreover, we observe frequent large-amplitude jumps in offset charge exceeding 0.1e; these large discrete charge jumps are incompatible with a picture of localized dipole-like two-level fluctuators. The data reveal an unexpected dependence of charge noise on device scale and suggest models involving either charge drift or fluctuating patch potentials.

Suppression of 1/f noise in solid state quantum devices by surface spin desorption

  1. S. E. de Graaf,
  2. L. Faoro,
  3. J. Burnett,
  4. A. A. Adamyan,
  5. A. Ya. Tzalenchuk,
  6. S. E. Kubatkin,
  7. T. Lindström,
  8. and A. V. Danilov
Noise and decoherence due to spurious two-level systems (TLS) located at material interfaces is a long-standing issue in solid state quantum technologies. Efforts to mitigate the effects
of TLS have been hampered by a lack of surface analysis tools sensitive enough to identify their chemical and physical nature. Here we measure the dielectric loss, frequency noise and electron spin resonance (ESR) spectrum in superconducting resonators and demonstrate that desorption of surface spins is accompanied by an almost tenfold reduction in the frequency noise. We provide experimental evidence that simultaneously reveals the chemical signatures of adsorbed magnetic moments and demonstrates their coupling via the electric-field degree of freedom to the resonator, causing dielectric (charge) noise in solid state quantum devices.