Abstract
We analyze the charge-noise induced coherence time of the fluxonium qubit as a function of the number of array junctions in the device, . The pure dephasing rate decreases with , but we find that the relaxation rate increases, so achieves an optimum as a function of . This optimum can be much smaller than the number typically chosen in experiments, yielding a route to improved fluxonium coherence and simplified device fabrication at the same time.
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