2023
DOI: 10.1103/physrevapplied.19.024066
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Tunable Superconducting Flux Qubits with Long Coherence Times

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Cited by 7 publications
(5 citation statements)
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“…Here, we do not consider the kinetic inductance of the loop as the geometric inductance of the loop is much larger than the kinetic inductance, which is estimated according to ref. [37]. Under these conditions, the flux quantization conditions of the f ε1 , f ε2 , and f α loops are…”
Section: Longitudinal Coupling In Concentric C-shunt Flux Qubitmentioning
confidence: 99%
See 1 more Smart Citation
“…Here, we do not consider the kinetic inductance of the loop as the geometric inductance of the loop is much larger than the kinetic inductance, which is estimated according to ref. [37]. Under these conditions, the flux quantization conditions of the f ε1 , f ε2 , and f α loops are…”
Section: Longitudinal Coupling In Concentric C-shunt Flux Qubitmentioning
confidence: 99%
“…Here, we do not consider the kinetic inductance of the loop as the geometric inductance of the loop is much larger than the kinetic inductance, which is estimated according to ref. [37]. Under these conditions, the flux quantization conditions of the f ε1 , f ε2 , and f α loops areϕ3+ϕ1+ϕ2+2πfε1=2πNε1$$\left(\phi\right)_{3} + \left(\phi\right)_{1} + \left(\phi\right)_{2} + 2 \pi f_{\epsilon 1}^{&aposx;} = 2 \pi N_{\epsilon 1}$$ϕ4ϕ1ϕ2+2πfε2=2πNε2$$- \left(\phi\right)_{4} - \left(\phi\right)_{1} - \left(\phi\right)_{2} + 2 \pi f_{\epsilon 2}^{&aposx;} = 2 \pi N_{\epsilon 2}$$ϕ3ϕ4+2πfα=2πNα$$\left(\phi\right)_{3} - \left(\phi\right)_{4} + 2 \pi f_{\alpha}^{&aposx;} = 2 \pi N_{\alpha}$$respectively.…”
Section: Longitudinal Coupling In Concentric C‐shunt Flux Qubitmentioning
confidence: 99%
“…For experimentally realistic values of the magnetic moment μ and of the relaxation or coherence times T 1 and T 2 , we refer to Refs. [17,40]. This set of parameters leads us to the final inaccuracy in the magnetic-field estimation of approximately 10 −12 T. We analyze the algorithm through the simulation of detection of magnetic fields in the range of [0; 50] nT, requiring the initial time of t 0 ≈ 40 ns, which is implementable using state-of-the-art transmon qubits [41].…”
Section: A Parametersmentioning
confidence: 99%
“…A major milestone was the introduction of the Transmon qubit [13], which provides remarkable protection against dephasing. In a recent decade, remarkable progress has been made in extending coherence times [14,15], and demonstrating high-fidelity single-and two-qubit gates [16][17][18][19][20][21][22][23]. Such advances are enabled not only by technological improvements but also by innovations in qubit architectural designs [24][25][26].…”
Section: Introductionmentioning
confidence: 99%