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Spin exchange-enabled quantum simulator for large-scale non-Abelian gauge theories

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arxiv 2305.06373 v3 pith:74W4NI7I submitted 2023-05-10 cond-mat.quant-gas cond-mat.str-elhep-latquant-ph

classification cond-mat.quant-gascond-mat.str-elhep-latquant-ph
keywords gaugelarge-scalelgtsmathrmnon-abelianquantumtermsapproach
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abstract

A central requirement for the faithful implementation of large-scale lattice gauge theories (LGTs) on quantum simulators is the protection of the underlying gauge symmetry. Recent advancements in the experimental realizations of large-scale LGTs have been impressive, albeit mostly restricted to Abelian gauge groups. Guided by this requirement for gauge protection, we propose an experimentally feasible approach to implement large-scale non-Abelian $\mathrm{SU}(N)$ and $\mathrm{U}(N)$ LGTs with dynamical matter in $d+1$D, enabled by two-body spin-exchange interactions realizing local emergent gauge-symmetry stabilizer terms. We present two concrete proposals for $2+1$D $\mathrm{SU}(2)$ and $\mathrm{U}(2)$ LGTs, including dynamical bosonic matter and induced plaquette terms, that can be readily implemented in current ultracold-molecule and next-generation ultracold-atom platforms. We provide numerical benchmarks showcasing experimentally accessible dynamics, and demonstrate the stability of the underlying non-Abelian gauge invariance. We develop a method to obtain the effective gauge-invariant model featuring the relevant magnetic plaquette and minimal gauge-matter coupling terms. Our approach paves the way towards near-term realizations of large-scale non-Abelian quantum link models in analog quantum simulators.

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Cited by 2 Pith papers

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    quant-ph 2025-06 conditional novelty 8.0 of 10

    Fermion extensions of the orbifold-lattice simulation framework achieve O(L^d) gates per Trotter step for QCD-like theories without oracles.

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    hep-ph 2024-11 conditional novelty 6.0 of 10

    A direct second-quantized qubit encoding of the light-front QCD Hamiltonian is used to classically emulate in-medium jet evolution with up to three-particle Fock states.

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