Microwave-activated gates between a fluxonium and a transmon qubit
A. Ciani (Forschungszentrum Jülich, TU Delft - QuTech Advanced Research Centre, TU Delft - QCD/Terhal Group)
Boris Varbanov (TU Delft - QuTech Advanced Research Centre, TU Delft - QCD/Terhal Group)
N. Jolly (TU Delft - QuTech Advanced Research Centre, PSL Research University, TU Delft - QCD/Terhal Group)
Christian Kraglund Andersen (TU Delft - Andersen Lab, Kavli institute of nanoscience Delft, TU Delft - QuTech Advanced Research Centre)
Barbara Maria Terhal (Forschungszentrum Jülich, TU Delft - QuTech Advanced Research Centre, TU Delft - QCD/Terhal Group, Quantum Computing)
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Abstract
We propose and analyze two types of microwave-activated gates between a fluxonium and a transmon qubit, namely a cross-resonance (CR) and a CPHASE gate. The large frequency difference between a transmon and a fluxonium makes the realization of a two-qubit gate challenging. For a medium-frequency fluxonium qubit, the transmon-fluxonium system allows for a cross-resonance effect mediated by the higher levels of the fluxonium over a wide range of transmon frequencies. This allows one to realize the cross-resonance gate by driving the fluxonium at the transmon frequency, mitigating typical problems of the cross-resonance gate in transmon-transmon chips related to frequency targeting and residual ZZ coupling. However, when the fundamental frequency of the fluxonium enters the low-frequency regime below 100MHz, the cross-resonance effect decreases leading to long gate times. For this range of parameters, a fast microwave CPHASE gate can be implemented using the higher levels of the fluxonium. In both cases, we perform numerical simulations of the gate showing that a gate fidelity above 99% can be obtained with gate times between 100 and 300ns. Next to a detailed gate analysis, we perform a study of chip yield for a surface code lattice of fluxonia and transmons interacting via the proposed cross-resonance gate. We find a much better yield as compared to a transmon-only architecture with the cross-resonance gate as native two-qubit gate.