A Fourier-engineered cos(2φ) qubit achieves spectral agreement with theory but its energy relaxation is limited by 1/f flux noise from residual first-harmonic fluctuations, unlike similar fluxonium qubits.
Feldstein-Bofill, L
4 Pith papers cite this work. Polarity classification is still indexing.
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Experimental demonstration of a WSi weak link in a 3D RF-SQUID showing non-sinusoidal current-phase relation with measured relaxation times of trapped persistent-current states.
Superconducting circuit hosts fractional fluxon states (fraxons) in a tailored Josephson potential to realize protected qudits with a STIRAP gate protocol.
A modified multi-mode rhombus circuit realizes a biased-noise superconducting qubit with measured average relaxation time of 500 microseconds in the biased regime versus 27 microseconds at frustration.
citing papers explorer
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Coherence limitations of a Fourier-engineered $\cos(2\varphi)$ transmon qubit
A Fourier-engineered cos(2φ) qubit achieves spectral agreement with theory but its energy relaxation is limited by 1/f flux noise from residual first-harmonic fluctuations, unlike similar fluxonium qubits.
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WSi weak link element with a non-sinusoidal current-phase relation
Experimental demonstration of a WSi weak link in a 3D RF-SQUID showing non-sinusoidal current-phase relation with measured relaxation times of trapped persistent-current states.
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Fraxonium: Fractional fluxon states for qudit encoding
Superconducting circuit hosts fractional fluxon states (fraxons) in a tailored Josephson potential to realize protected qudits with a STIRAP gate protocol.
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Revisiting the multi-mode rhombus circuit as a biased-noise qubit
A modified multi-mode rhombus circuit realizes a biased-noise superconducting qubit with measured average relaxation time of 500 microseconds in the biased regime versus 27 microseconds at frustration.