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This study confirms that Wilson fermions are essential for stabilizing topological phases in (2+1)D quantum electrodynamics, resolving theoretical ambiguities regarding Hamiltonian formulations. By explicitly breaking time-reversal symmetry, these fermions enable the realization of Chern insulators and quantum spin Hall states, which staggered fermions cannot achieve. These findings provide a critical roadmap for implementing complex topological matter simulations on emerging quantum computing hardware.
Wilson Fermions Enable Quantum Simulations of Topological Phases

Researchers demonstrate how Wilson fermions facilitate quantum simulations of (2+1)D quantum electrodynamics, crucial for realizing topological phases and Chern-Simons terms.
Researchers at the Helmholtz Institute, alongside collaborators from institutions including UCLA, MIT and Tsinghua University, have charted a path toward stable topological phases within quantum systems. The team’s work focuses on (2+1)D quantum electrodynamics (QED3) with Wilson fermions, a notoriously difficult area for quantum simulation due to its inherent complexity. This research demonstrates why staggered fermions cannot induce topological phases in this system, while Wilson fermions can support phases like Chern insulators and quantum spin Hall states, and further uncovers a detailed phase diagram for the two-flavor Wilson fermion model. These findings resolve ambiguities in existing theoretical frameworks and lay groundwork for future quantum simulations on emerging computing platforms. Wilson fermions, a specific type of fermion discretization, demonstrably enable the emergence of topological phases in (2+1)-dimensional quantum electrodynamics (QED3), a finding that resolves long-standing ambiguities in Hamiltonian formulations of lattice field theories. Unlike their staggered fermion counterparts, Wilson fermions facilitate a variety of topological phases, including Chern insulator and quantum spin Hall phases. This distinction arises from the way each fermion…
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