Fast Hamiltonian engineering from cut polytope geometry

arXiv:2609.36006 · quant-ph, cond-mat.quant-gas · Submitted 2026-09-28 · Read on arXiv

quant-ph, cond-mat.quant-gas

Submitted: 2026-09-28

Updated: 2026-09-28

Comments: 51 pages, 10 figures

Code: https://github.com/ThomasJFriese/cut-polytope-hamiltonian-enginee

License: http://creativecommons.org/licenses/by/4.0/

The gist: Hamiltonian engineering (HE) simulates quantum dynamics under a target Hamiltonian using a native entangling system Hamiltonian and restricted control, with applications from quantum gate design to

Terminology

Abstract

Hamiltonian engineering (HE) simulates quantum dynamics under a target Hamiltonian using a native entangling system Hamiltonian and restricted control, with applications from quantum gate design to analog quantum simulation. Observing that, for many systems, formulating HE as a linear program only requires specific commutation relations between the control pulses and the system Hamiltonian, we provide a unified framework for broad classes of 2-local qubit, qudit, and fermionic systems. We reformulate time-optimal HE as a complex k-cut polytope problem, with k the number of distinct phases in these commutation relations, and prove it NP-complete for every finite k. We therefore relax the polytope to the elliptope and apply a Krivine-type rounding, yielding pulses informed by the system and target Hamiltonians, which we then use in a linear program. We derive how many informed pulses are necessary and sufficient for the linear program to be reliably feasible. Additionally mixing in uniformly sampled pulses guarantees a solution close to the relaxation value from O(m) pulses, with m the number of interaction terms. Together with upper and lower bounds on the optimal quantum run time, this yields an O(sqrt m) approximation ratio. In benchmarks on a fully connected Ising model, a chiral clock model for qudits, and the fermionic Harper-Hofstadter model, our approach attains near-optimal quantum run times wherever the optimum is computable, reaches run times that saturate with the lattice size in the fermionic case, and outperforms state-of-the-art methods with O(m) pulses. This establishes a unified approach with provable guarantees to the automatic programming of analog quantum simulators.

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