2020
DOI: 10.1038/s41586-020-2687-9
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The superconducting quasicharge qubit

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Cited by 79 publications
(66 citation statements)
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“…For realistic cQED parameters E J / = 2π × 20 GHz, E C = E J /67 [25], E Σ / = 2π × 30 GHz ≡ 1.5 E J [48] and d = 0.02, we obtain ω q = 2π × 3.28 GHz. Moreover, for an LC oscillator (or transmission line resonator) having values ω r L r = 200 kΩ [42], we eventually achieve g z (t) = 2π × 2.57 GHz corresponding to max(g z )/ω r = 0.5793. With this maximal value, it is possible to estimate the minimal time required to measure the qubit t min = π/(2ω r ), on a subnanosecond time scale, from optimal control theory.…”
mentioning
confidence: 89%
See 1 more Smart Citation
“…For realistic cQED parameters E J / = 2π × 20 GHz, E C = E J /67 [25], E Σ / = 2π × 30 GHz ≡ 1.5 E J [48] and d = 0.02, we obtain ω q = 2π × 3.28 GHz. Moreover, for an LC oscillator (or transmission line resonator) having values ω r L r = 200 kΩ [42], we eventually achieve g z (t) = 2π × 2.57 GHz corresponding to max(g z )/ω r = 0.5793. With this maximal value, it is possible to estimate the minimal time required to measure the qubit t min = π/(2ω r ), on a subnanosecond time scale, from optimal control theory.…”
mentioning
confidence: 89%
“…To achieve larger values of the coupling strength resulting in a faster measuring time, we require large impedance [41]. Along with it, the technological progress has made it possible to engineer inductances in the µH regime using arrays of Josephon junctions or taking into account kinetic inductors [42][43][44][45]. To estimate the value of the coupling strength we regard φ x /ϕ 0 = ϕ x /ϕ 0 = π/4, hence the qubit frequency turns into ω q = E 2 C + dE 2 Σ / .…”
mentioning
confidence: 99%
“…[24][25][26][27][28] ). The inductive shunt makes the device insensitive to charge noise 29 , while fluxnoise insensitivity can be reached for large values of the superinductance 30 . Recent realizations of the fluxonium qubit have shown long coherence times 31 , making these devices very attractive for quantum information processing.…”
Section: Dmrg Implementation Of the Fluxonium-qubit Hamiltonianmentioning
confidence: 99%
“…Superconducting materials with high kinetic inductance offer new opportunities in the design of highsensitivity photon detectors, wideband quantum amplifiers, and high-coherence quantum processors [1][2][3][4]. In particular, for the noise-resilient superconducting-qubits, a non-dissipative circuit element as characterized by a considerably high inductance (i.e., several hundred nanohenry to a few microhenry) is indispensable for charge-and flux-noise protection [5][6][7][8][9][10]. The magnitude of such inductance, as it is often the case, utterly exceeds the achievable geometric inductance in the nanofabricated superconducting circuits, making the utilization of intrinsic material properties such as kinetic inductance essential for its practical realizations.…”
Section: Introductionmentioning
confidence: 99%
“…The magnitude of such inductance, as it is often the case, utterly exceeds the achievable geometric inductance in the nanofabricated superconducting circuits, making the utilization of intrinsic material properties such as kinetic inductance essential for its practical realizations. Extensive research have thus been performed on superconducting materials with a large kinetic inductance, such as Josephsonjunction arrays (JJAs) [7,[10][11][12] and granular aluminum [13][14][15][16], for the high-inductance implementations.…”
Section: Introductionmentioning
confidence: 99%