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This research establishes fundamental no-go theorems proving that non-local interactions are unavoidable in Hamiltonian simulations of non-Abelian lattice gauge theories, presenting a significant theoretical barrier for quantum computing approaches to QCD. The authors demonstrate that while certain mitigation strategies work for Abelian U(1) systems, they lead to inconsistencies when applied to the more complex non-Abelian cases required for realistic particle physics modeling. These findings are critical for quantum algorithm designers aiming to develop efficient, scalable simulations near the continuum limit without relying on currently infeasible local formulations.
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No-go theorems for dual Hamiltonians of Non-Abelian Lattice Gauge Theories

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2609.39780v1 Announce Type: cross Abstract: Hamiltonian simulations of lattice gauge theories promise new insights into the inner workings of QCD. The rapid development of quantum computing hardware suggests that large scale simulations may soon become feasible. However, no efficient formulation suitable for simulations near the continuum limit is currently known for the non-Abelian case, and existing candidates typically feature long range interactions in the electric part of the Hamiltonian. We prove that such non- localities are unavoidable when the gauge configuration is reparametrised while preserving both the number of degrees of freedom and the fundamental commutation relations. We then attempt to mitigate this by introducing additional gauge links alongside additional constraints. Although this approach is successful in U(1), we prove that the corresponding construction is inconsistent for non-Abelian lattice gauge theories.

Abstract:Hamiltonian simulations of lattice gauge theories promise new insights into the inner workings of QCD. The rapid development of quantum computing hardware suggests that large scale simulations may soon become feasible. However, no efficient formulation suitable for simulations near the continuum limit is currently known for the non-Abelian case, and existing candidates typically feature long range interactions in the electric part of the Hamiltonian. We prove that such non- localities are unavoidable when the gauge configuration is reparametrised while preserving both the number of degrees of freedom and the fundamental commutation relations. We then attempt to mitigate this by introducing additional gauge links alongside additional constraints. Although this approach is successful in U(1), we prove that the corresponding construction is inconsistent for non-Abelian lattice gauge theories.

arXiv:2609.39780 [hep-lat]

(or arXiv:2609.39780v1 [hep-lat] for this version)

https://doi.org/10.48550/arXiv.2609.39780 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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