Readout errors in superconducting qubits include incorrect state assignment, bit flips within the computational subspace, and leakage to non-computational states. These errors requiredifferent mitigation strategies, yet conventional measurement fidelity and repeatability metrics do not resolve their individual contributions. Previous repeated-readout studies have shown that temporal correlations reveal additional information about readout errors. Here we introduce the Readout Error Decoder (RED), which converts repeated thresholded binary records into a channel-resolved error budget. Controlled error injections validate the channel-specific response of the decoder. We demonstrate RED on both fluxonium and transmon qubits and across distinct leakage-lifetime regimes. RED identifies the error channels limiting readout performance without requiring dedicated discrimination of non-computational states, providing a basis for targeted readout optimization across different qubit modalities.
We report superconducting fluxonium qubits with coherence times largely limited by energy relaxation and reproducibly satisfying T2 > 100 microseconds (T2 > 300 microseconds in onedevice). Moreover, given the state of the art values of the surface loss tangent and the 1/f flux noise amplitude, coherence can be further improved beyond 1 millisecond. Our results violate a common viewpoint that the number of Josephson junctions in a superconducting circuit — over 100 here — must be minimized for best qubit coherence. We outline how the unique to fluxonium combination of long coherence time and large anharmonicity can benefit both gate-based and adiabatic quantum computing.
Vacuum fluctuations fundamentally affect an atom by inducing a fnite excited state lifetime along with a Lamb shift of its transition frequency. Here we report the reverse effect: modifcationof vacuum by a single atom in circuit quantum electrodynamics. Our one-dimensional vacuum is a long section of a high wave impedance (comparable to resistance quantum) superconducting transmission line. It is directly wired to a transmon qubit circuit. Owing to the combination of high impedance and galvanic connection, the transmon’s spontaneous emission linewidth can greatly exceed the discrete transmission line modes spacing. This condition defines a previously unexplored superstrong coupling regime of quantum electrodynamics where many vacuum modes hybridize with each other through interactions with a single atom. We explore this regime by spectroscopically measuring the positions of over 100 consecutive transmission line resonances. The atom reveals itself as a broad peak in the vacuum’s density of states (DOS) together with the Kerr and cross-Kerr interaction of photons at frequencies within the DOS peak. Both dispersive effects are well described by a dissipative Caldeira-Leggett model of our circuit, with the transmon’s quartic anharmonicity treated as a perturbation. Non-perturbative modifications of such a vacuum, including inelastic scattering of single photons, are expected upon replacing the transmon by more anharmonic circuits, with broad implications for simulating critical dynamics of quantum impurity models.