Posted

Islam Faisal, Anand Natarajan, Alexander Poremba (May 26 2026).
Abstract: Commuting Hamiltonians lie at the boundary between classical constraint satisfaction and quantum many-body physics, exhibiting rich quantum structure while remaining more tractable than general noncommuting models. In contrast, physical Hamiltonians are rarely exactly commuting, which naturally motivates the study of almost commuting Hamiltonians. Despite their relevance, the implications of approximate commutation are only poorly understood. In this work, we show how to efficiently approximate any almost commuting 22-local qubit Hamiltonian by a commuting one: we give a locality-preserving algorithmic rounding technique that maps any 22-local Hamiltonian H=∑i=1mhiH=\sum_{i=1}^m h_i with ∥[hi,hj]∥≤ϵ\|[h_i,h_j]\| \leq \epsilon to a nearby Hamiltonian H^\hat{H} whose terms pair-wise commute, and which is within overall distance ∥H−H^∥=O(m ϵ1/6)\|H-\hat{H}\| = O(m\,\epsilon^{1/6}). As a consequence, we show that δ\delta-approximations to the ground energy for ϵ\epsilon-almost commuting 22-local qubit Hamiltonians lie in NP\mathsf{NP} when δ≫mϵ1/6\delta \gg m\epsilon^{1/6}, extending the classical containment well beyond the commuting setting. Finally, we present two applications of our rounding framework: Gibbs sampling and fast Hamiltonian simulation for almost commuting systems.

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