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.

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.

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.

Direct identification of dilute surface spins on Al2O3: Origin of flux noise in quantum circuits

  1. S. E. de Graaf,
  2. A. A. Adamyan,
  3. T. Lindström,
  4. D. Erts,
  5. S. E. Kubatkin,
  6. A. Ya. Tzalenchuk,
  7. and A. V. Danilov
It is universally accepted that noise and decoherence affecting the performance of superconducting quantum circuits are consistent with the presence of spurious two-level systems (TLS).
In recent years bulk defects have been generally ruled out as the dominant source, and the search has focused on surfaces and interfaces. Despite a wide range of theoretical models and experimental efforts, the origin of these surface TLS still remains largely unknown, making further mitigation of TLS induced decoherence extremely challenging. Here we use a recently developed on-chip electron spin resonance (ESR) technique that allows us to detect spins with a very low surface coverage. We combine this technique with various surface treatments specifically to reveal the nature of native surface spins on Al2O3 — the mainstay of almost all solid state quantum devices. On a large number of samples we resolve three ESR peaks with the measured total paramagnetic spin density n=2.2×1017m−2, which matches the density inferred from the flux noise in SQUIDs. We show that two of these peaks originate from physisorbed atomic hydrogen which appears on the surface as a by-product of water dissociation. We suggest that the third peak is due to molecular oxygen on the Al2O3 surface captured at strong Lewis base defect sites, producing charged O−2. These results provide important information towards the origin of charge and flux noise in quantum circuits. Our findings open up a whole new approach to identification and controlled reduction of paramagnetic sources of noise in solid state quantum devices.

Dynamic parity recovery in a strongly driven Cooper-pair box

  1. S. E. de Graaf,
  2. J. Leppäkangas,
  3. A. Adamyan,
  4. A. V. Danilov,
  5. T. Lindström,
  6. M. Fogelström,
  7. T. Bauch,
  8. G. Johansson,
  9. and S. E. Kubatkin
We study a superconducting charge qubit coupled to an intensive electromagnetic field and probe changes in the resonance frequency of the formed dressed states. At large driving strengths,
exceeding the qubit energy-level splitting, this reveals the well known Landau-Zener-St\“uckelberg (LZS) interference structure of a longitudinally driven two-level system. For even stronger drives we observe a significant change in the LZS pattern and contrast. We attribute this to photon-assisted quasiparticle tunneling in the qubit. This results in the recovery of the qubit parity, eliminating effects of quasiparticle poisoning and leads to an enhanced interferometric response. The interference pattern becomes robust to quasiparticle poisoning and has a good potential for accurate charge sensing.