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Dynamic and Control of Josephson superconducting circuits in strong field regime

Léon Carde

Published Nov 25, 2025• 0 citations

Abstract

Bistable systems are central to information processing, from classical bits to quantum qubits. Their robustness relies on mitigating switching errors, or bit flips. While a classical potential barrier suppresses thermal bit flips, quantum systems also suffer from phase-flip errors that degrade superpositions. "Cat" qubits leverage the principle of a potential barrier to exponentially suppress bit flips, but at the expense of a marginal increase in phase flips. This unique error bias simplifies quantum error correction, making cat qubits a promising platform for fault-tolerant quantum computation.This thesis first investigates the scaling of bit-flip errors in cat qubits as a function of their size. Using path integral techniques, we predict the switching rate in a single-mode bistable open quantum system. Drawing inspiration from systems satisfying detailed balance, we identify a set of non-idealities that nonetheless preserve the optimal scaling of ideal cat qubits.We then turn to the analysis of a superconducting circuit composed of Josephson junctions that implements a dissipative cat qubit. The nonlinear dissipation that is key to stabilizing a cat qubit originates from a parametrically activated coupling between the memory and a lossy mode. Our perturbative analysis uncovers parasitic drive-activated nonlinearities that amplify phase-flip errors as the cat-state stabilization strength increases, which ultimately alters the performance of a repetition code.Finally, we present the integration of the methods developed in this thesis into a complete simulation stack for superconducting circuits. We exemplify this integration with an ab initio study of a recently developed cascaded single-microwave-photon detector.

DOI: 10.70675/085b3d05z1869z46daz8989z0db4316dec47

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Bistable systems are central to information processing, from classical bits to quantum qubits. Their robustness relies on mitigating switching errors, or bit flips. While a classical potential barrier suppresses thermal bit flips, quantum systems also suffer from phase-flip errors that degrade superpositions. "Cat" qubits leverage the principle of a potential barrier to exponentially suppress bit flips, but at the expense of a marginal increase in phase flips. This unique error bias simplifies quantum error correction, making cat qubits a promising platform for fault-tolerant quantum computation.This thesis first investigates the scaling of bit-flip errors in cat qubits as a function of their size. Using path integral techniques, we predict the switching rate in a single-mode bistable open quantum system. Drawing inspiration from systems satisfying detailed balance, we identify a set of non-idealities that nonetheless preserve the optimal scaling of ideal cat qubits.We then turn to the analysis of a superconducting circuit composed of Josephson junctions that implements a dissipative cat qubit. The nonlinear dissipation that is key to stabilizing a cat qubit originates from a parametrically activated coupling between the memory and a lossy mode. Our perturbative analysis uncovers parasitic drive-activated nonlinearities that amplify phase-flip errors as the cat-state stabilization strength increases, which ultimately alters the performance of a repetition code.Finally, we present the integration of the methods developed in this thesis into a complete simulation stack for superconducting circuits. We exemplify this integration with an ab initio study of a recently developed cascaded single-microwave-photon detector.

Quantum computing is a relatively new computing paradigm that leverages entanglement to implement algorithms beyond the reach of classical hardware. Superconducting quantum circuits have emerged as a platform to build quantum processors, with demonstrations of quantum supremacy over classical supercomputers and quantum error correction beyond fault tolerance. However, current noisy devices require significant improvements to unlock the full potential of quantum algorithms.This thesis investigates intrinsic noise channels in superconducting circuits and the design of noise-resilient qubits. By characterizing high-quality superconducting resonators, we identify lossy dielectric materials at the interfaces as the dominant loss mechanism, which we mitigate via targeted surface treatments. Subsequently, we leverage Josephson junction nonlinearity to engineer noise-biased qubits utilizing the Kerr parametric oscillator (KPO). By analyzing the efficiency of strong, far-off-resonance driving to facilitate three- and four-wave mixing processes, we demonstrate high-fidelity operations on Fock, Kerr-cat, and dual-rail qubits. For the Kerr-cat qubit, we introduce a novel 2D architecture that enables strong light-matter coupling with suppressed Purcell decay, yielding millisecond-scale bit-flip lifetimes. Within this same architecture, we demonstrate a longitudinal qubit readout with a

99.6\%

quantum nondemolition score, alongside a high-fidelity universal single-qubit gate set, all while maintaining bit-flip error suppression. Finally, we exploit the efficient wave-mixing of strongly coupled, far-detuned KPOs to realize a dynamically protected dual-rail qubit exhibiting both erasure bias and high-fidelity single-qubit gates.

Cat qubits, for which logical |0⟩ and |1⟩ are coherent states |±α⟩ of a harmonic mode, offer a promising route towards quantum error correction. Using dissipation to our advantage so that photon pairs of the harmonic mode are exchanged with single photons of its environment, it is possible to stabilize the logical states and exponentially increase the bit-flip time of the cat qubit with the photon number |α|2 . A large two-photon dissipation rate κ2 ensures fast qubit manipulation and short error-correction cycles, which are instrumental to correct the remaining phase-flip errors in a repetition code of cat qubits. Here, we introduce and operate an autoparametric superconducting circuit that couples a mode containing the cat qubit to a lossy mode whose frequency is set at twice that of the cat mode. This passive coupling does not require a parametric pump, and it reaches a rate κ2/2π≈2 MHz . With such a strong two-photon dissipation, bit-flip errors of the autoparametric cat qubit are prevented for a characteristic time up to 0.3 s with only a mild impact on phase-flip errors. In addition, we illustrate how the phase of a quantum superposition between |α⟩ and |−α⟩ can be arbitrarily changed by driving the harmonic mode while keeping the engineered dissipation active. Published by the American Physical Society 2024

These are the lecture notes from the 2019 Les Houches Summer School on "Quantum Information Machines". After a brief introduction to quantum error correction and bosonic codes, we focus on the case of cat qubits stabilized by a nonlinear multi-photon driven dissipation process. We argue that such a system can be seen as a self-correcting qubit where bit-flip errors are robustly and exponentially suppressed. Next, we provide some experimental directions to engineer such a multi-photon driven dissipation process with superconducting circuits. Finally, we analyze various logical gates that can be implemented without re-introducing bit-flip errors. This set of bias-preserving gates pave the way towards a hardware-efficient and fault-tolerant quantum processor.

DC-voltage-biased Josephson junctions have been recently employed in superconducting circuits for Hamiltonian engineering, demonstrating microwave amplification, single photon sources and entangled photon generation. Compared to more conventional approaches based on parametric pumps, this solution typically enables larger interaction strengths. In the context of quantum information, a two-to-one photon interaction can stabilize cat qubits, where bit-flip errors are exponentially suppressed, promising significant resource savings for quantum error correction. This work investigates how the DC bias approach to Hamiltonian engineering can benefit cat qubits. We find a simple circuit design that is predicted to showcase a two-to-one photon exchange rate larger than that of the parametric pump-based implementation while dynamically averaging typically resonant parasitic terms such as Kerr and cross Kerr. In addition to addressing qubit stabilization, we propose to use injection locking with a cat-qubit adapted frequency filter to prevent long-term drifts of the cat qubit angle associated to DC voltage noise. The whole scheme is simulated without rotating-wave approximations, highlighting for the first time the amplitude of related oscillatory effects in cat-qubit stabilization schemes. This study lays the groundwork for the experimental realization of such a circuit.

Dissipatively stabilized cat qubits provide a promising route toward fault-tolerant quantum computation, exhibiting exponential suppression of bit-flip errors with increasing phase-space separation of the logical states, while incurring only a linear increase in phase-flip errors. Existing implementations rely on engineered two-photon dissipation via nonlinear coupling to a lossy environment, an approach largely confined to superconducting platforms and limited by spurious decay channels and finite dissipation rates. Here, we propose a fundamentally different stabilization paradigm based on repeated interactions with an auxiliary two-level system mediated by a quadratic Hamiltonian, enabling dissipative stabilization without reservoir engineering. Our approach overcomes key limitations of existing schemes and is compatible with a wider class of experimental platforms. Furthermore, it preserves the noise bias and extends to squeezed cat qubits, rendering single-photon loss errors partially correctable.

These are the lecture notes from the 2019 Les Houches Summer School on “Quantum Information Machines”. After a brief introduction to quantum error correction and bosonic codes, we focus on the case of cat qubits stabilized by a nonlinear multi-photon driven dissipation process. We argue that such a system can be seen as a self-correcting qubit where bit-flip errors are robustly and exponentially suppressed. Next, we provide some experimental directions to engineer such a multi-photon driven dissipation process with superconducting circuits. Finally, we analyze various logical gates that can be implemented without re-introducing bit-flip errors. This set of bias-preserving gates pave the way towards a hardware-efficient and fault-tolerant quantum processor.