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.
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.
Multi-photon dissipation -- a key resource for bosonic qubits -- is usually realized by parametrically pumping a Josephson coupler at the cost of spurious nonlinear terms. Here we instead engineer it using a dc-voltage-biased SQUID, such that these parasitic terms average out. We activate the conversion of one, two, or four photons of a high-Q mode into a single photon of a lossy mode. We characterize the two-photon dissipation by Wigner tomography, establishing dc-biased junctions as a resource for reservoir engineering and a viable route to cat-qubit stabilization.
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.
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.
Cat qubits exhibit a strong noise bias, meaning that errors are predominantly confined to a single error channel, which can be corrected using a simple one-dimensional error correction code. As a result, cat qubits quadratically reduce the number of physical qubits required to realise a fully protected logical qubit compared with conventional surface codes. Recently a Kerr cat qubit was for the first time controlled with four-wave mixing in a SNAIL device. In this project we propose a circuit architecture adapted for four-wave mixing in the form of a capacitively shunted Josephson junction array which we call Kerr Josephson junction array oscillator (KJJA-oscillator). The device is fixed in frequency and not flux tunable, making it resilient to flux noise. Moreover the device strongly suppresses high order non-linearities, and therefore offers low intrinsic dephasing. The mathematical description of the KJJA-oscillator is developed, from which two KJJA-oscillators is designed. With four wave mixing the squeezing term of the Kerr Hamiltonian is realised with two separate drives slightly detuned from the cavity. This makes it possible to place cavities in the full frequency range of the signal generator. The Kerr is chosen as a neutral value in the trade-off between fast operations and long coherence times, based of previous results in the literature. The fabricated chip is characterised and found to exhibit low coherence times, most likely due to low fabrication quality. There is no known direct readout mechanism for four-wave mixing known to the author, instead an ancillary transmon was used to perform parity measurements. To showcase the readout mechanism Wigner-tomography of the vacuum state was measured. Due to the time constraints of the thesis there was not time to stabilise cats and show noise biasing properties. The chip will in the future be used to show how noise biasing scales with increasing cat state size and for demonstration of a universal single gate set.
Quantum computing promises exponential advantages for simulating quantum systems and solving certain computational problems beyond the reach of classical computers, but the fragility of qubits and the resulting errors present a major challenge for scalable implementations. One promising approach is to engineer qubits whose physical noise processes are intrinsically biased, enabling more efficient quantum error correction. This dissertation investigates quantum computing with superconducting Kerr-cat qubits, a bosonic qubit architecture in which qubit states are encoded in coherent states of a nonlinear oscillator stabilized by a two-photon drive. This stabilization creates an effective double-well pseudo-potential that strongly suppresses bit-flip errors while enabling universal quantum control, leading to a noise-biased qubit. A superconducting device architecture based on SNAIL nonlinear oscillators is developed to realize Kerr-cat qubits with tunable parameters and high coherence, integrating readout resonators, dedicated filters, and microwave control lines for measurement and manipulation. Universal single-qubit gates are implemented using engineered single-photon and two-photon drives to deform the pseudo-potential, and a cat-quadrature readout method is employed to achieve high-fidelity quantum nondemolition measurement. The performance of the qubits is systematically characterized through lifetime measurements and benchmarking protocols, including quantum process tomography, gate set tomography, and dihedral randomized benchmarking, revealing a strongly biased noise structure with high performance. These results establish an experimental framework for the design, control, and characterization of Kerr-cat qubits and demonstrate their potential as hardware-efficient building blocks for scalable fault-tolerant quantum computing.
Parametric interactions are foundational to superconducting quantum technologies, yet conventional microwave-driven pumping introduces parasitic Kerr nonlinearities and higher-order harmonics that limit device performance. Josephson Photonics (JP) avoids these parasitics by utilizing dc-biased junctions but has remained constrained by high phase noise and the absence of a stable phase reference. Here, we overcome this limitation by integrating a Josephson voltage standard (JVS) to establish a noise-tolerant phase reference, and demonstrate that this reference is coherently transferred to an inelastic Cooper-pair tunneling amplifier (ICTA) via the superconducting order parameter. The resulting low-phase-noise architecture yields a 14-dB enhancement in averaged gain and better quantum-limited noise performance. Critically, the phase reference enables the first observation of phase-sensitive gain and squeezing in a dc-biased amplifier. By reconciling clean, Kerr-free nonlinearities with phase-coherent drive, our architecture establishes a robust platform for high-purity parametric processes in superconducting circuits.