Effects of quasiparticle tunnelling in a circuit-QED realization of a strongly driven two-level system

Leppäkangas, Juha; Graaf, S. E. de; Adamyan, A.; Fogelström, Mikael; Danilov, Andrey; Lindström, Tobias; Kubatkin, Sergey; Johansson, Göran

doi:10.1088/0953-4075/46/22/224019

Cited by 6 publications

(4 citation statements)

References 44 publications

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“…(Wilson et al, 2007(Wilson et al, , 2010, where an emphasis was made on the dressed state description, and in Refs. Leppäkangas et al, 2013), where the emphasis was made on quasiparticle tunneling. An analogous qubit was also probed by a nanomechanical resonator (LaHaye et al, 2009), where a charge qubit state influenced the displacement of the resonator, of which the resonant frequency was probed.…”

Section: A Superconducting Circuitsmentioning

confidence: 99%

Quantum Control via Landau-Zener-Stückelberg-Majorana Transitions

Ivakhnenko¹,

Shevchenko²,

Nori³

2022

Preprint

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H. Comparison of different methods IV. Interferometry A. Superconducting circuits B. Semiconductor quantum dots C. Donors and impurities (atomic qubits) D. Graphene E. Microscopic systems F. Other systems G. Multilevel systems V. Quantum control A. Coherent control of microscopic and mesoscopic structures B. Universal single-and two-qubit control C. Shortcuts to adiabaticity D. Adiabatic quantum computation VI. Related classical coherent phenomena VII. Conclusion 1. With near-adiabatic limit (Landau) 2. With parabolic cylinder functions (Zener) 3. With contour integrals (Majorana) 4. With WKB approximation and phase integral method (Stückelberg) 5. Duration of the LZSM transition B. Description of a periodically driven two-level system 1. Adiabatic-impulse model a. Adiabatic evolution b. Multiple-passage evolution 2. Rotating-wave approximation (RWA) 3. Floquet theory 4. Rate equation and white noise approach a. Transition rate b. Rate equation c. From Bessel to Airy d. Double-passage regime ReferencesAbbreviations and most-often-used symbols Because this review article is quite long, for the readers' convenience, we present the main abbreviations used. This list also includes some of the topics covered.

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Section: A Superconducting Circuitsmentioning

confidence: 99%

Quantum Control via Landau-Zener-Stückelberg-Majorana Transitions

Ivakhnenko¹,

Shevchenko²,

Nori³

2022

Preprint

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“…In particular, we demonstrate that in a specific experimentally feasible parameter regime, squeezing at a high photon number can be achieved even in the presence of maximum gate-charge disorder. It follows that this device is robust against strong thermal noise in the DC-voltage bias 34 and nonequilibrium quasiparticles in the CPTs [35][36][37][38] .…”

Section: Introductionmentioning

confidence: 87%

Creating photon-number squeezed strong microwave fields by a Cooper-pair injection laser

2017

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The use of artificial atoms as an active lasing medium opens a way to construct novel sources of nonclassical radiation. An example is the creation of photon-number squeezed light. Here we present a design of a laser consisting of multiple Cooper-pair transistors coupled to a microwave resonator. Over a broad range of experimentally realizable parameters, this laser creates photonnumber squeezed microwave radiation, characterized by a Fano factor F ≪ 1, at a very high resonator photon number. We investigate the impact of gate-charge disorder in a Cooper-pair transistor and show that the system can create squeezed strong microwave fields even in the presence of maximum disorder.

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“…[812]). There have been several experiments studying LZSM physics in strongly driven SQCs and similar systems [158,325,337,[813][814][815][816][817]. Extensions to a biharmonic drive [818] and multiple qubits [819] have also been studied.…”

Section: Strongly Driven Multiphoton Processesmentioning

confidence: 99%

Microwave photonics with superconducting quantum circuits

Gu,

Kockum,

Miranowicz

et al. 2017

Preprint

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In the past 20 years, impressive progress has been made both experimentally and theoretically in superconducting quantum circuits, which provide a platform for manipulating microwave photons. This emerging field of superconducting quantum microwave circuits has been driven by many new interesting phenomena in microwave photonics and quantum information processing. For instance, the interaction between superconducting quantum circuits and single microwave photons can reach the regimes of strong, ultra-strong, and even deep-strong coupling. Many higher-order effects, unusual and less familiar in traditional cavity quantum electrodynamics with natural atoms, have been experimentally observed, e.g., giant Kerr effects, multi-photon processes, and single-atom induced bistability of microwave photons. These developments may lead to improved understanding of the counterintuitive properties of quantum mechanics, and speed up applications ranging from microwave photonics to superconducting quantum information processing. In this article, we review experimental and theoretical progress in microwave photonics with superconducting quantum circuits. We hope that this global review can provide a useful roadmap for this rapidly developing field.

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Effects of quasiparticle tunnelling in a circuit-QED realization of a strongly driven two-level system

Cited by 6 publications

References 44 publications

Quantum Control via Landau-Zener-Stückelberg-Majorana Transitions

Quantum Control via Landau-Zener-Stückelberg-Majorana Transitions

Creating photon-number squeezed strong microwave fields by a Cooper-pair injection laser

Microwave photonics with superconducting quantum circuits

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