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    Native three-body interactions in a superconducting lattice gauge quantum simulator

    J. H. Busnaina1, Z. Shi1, Jesús M. Alcaine-Cuervo2,3, Cindy X. Yang1, I. Nsanzineza1, E. Rico2,4,5,6, and C. M. Wilson1,*

    • 1Institute for Quantum Computing and Department of Electrical & Computer Engineering, University of Waterloo, Waterloo, Ontario, Canada N2L 3G1
    • 2EHU Quantum Center and Department of Physical Chemistry, University of the Basque Country UPV/EHU, P.O. Box 644, 48080 Bilbao, Spain
    • 3BCMaterials, Basque Center for Materials, Applications and Nanostructures, UPV/EHU Science Park, 48940 Leioa, Spain
    • 4DIPC-Donostia International Physics Center, Paseo Manuel de Lardizabal 4, 20018 San Sebastián, Spain
    • 5European Organization for Nuclear Research (CERN), 1211 Geneva, Switzerland
    • 6IKERBASQUE, Basque Foundation for Science, Plaza Euskadi 5, 48009 Bilbao, Spain

    • *Contact author: chris.wilson@uwaterloo.ca

    Phys. Rev. B 112, 134514 – Published 14 October, 2025

    DOI: https://doi.org/10.1103/6prx-zmdz

    Abstract

    While universal quantum computers remain under development, analog quantum simulators offer a powerful alternative for understanding complex systems in condensed matter, chemistry, and high-energy physics. One compelling application is the characterization of real-time lattice gauge theories (LGTs). LGTs are nonperturbative tools, utilizing discretized space-time to describe gauge-invariant models. They hold immense potential for understanding fundamental physics but require enforcing local constraints analogous to electromagnetism's Gauss's law. These constraints, which arise from gauge symmetries and dictate the form of the interaction between matter and gauge fields, are a significant challenge for simulators to enforce. Implementing these constraints at the hardware level in analog simulations is crucial. This requires realizing multibody interactions between matter and gauge-field elements, enabling them to evolve together while suppressing unwanted two-body interactions that violate the gauge symmetry. In this paper, we propose and implement a parametrically activated three-qubit interaction within a circuit quantum electrodynamics architecture. We experimentally demonstrate a minimal U(1) spin-12 model with a time evolution that intrinsically satisfies Gauss's law in the system. This design serves as the foundational block for simulating LGTs on a superconducting photonic lattice.

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