- Open Access
Efficient Quantum Optimization via Dynamical Simulation
PRX Quantum 7, 033026 – Published 12 August, 2026
DOI: https://doi.org/10.1103/t59v-8flk
Abstract
We provide several quantum algorithms for continuous optimization that do not require gradient estimation. Instead, we encode the optimization problem into the dynamics of a physical system and coherently simulate the time evolution. We focus on the setting where the objective function can only be accessed via a phase oracle. Our first two algorithms can find local optima of a differentiable function by simulating either classical or quantum dynamics with friction via a time-dependent Hamiltonian. We show that for the benchmark problem of optimizing a locally quadratic objective function, these methods require a total of queries to a phase oracle to find an -approximate local optimum, where is the condition number of the Hessian matrix and is the discretization spacing. In contrast, we show that methods based on gradient descent require queries. This corresponds to an exponential separation between the query upper bounds for the benchmark problem. Our third algorithm can find the global optimum of by preparing a classical low-temperature thermal state via simulation of the classical Liouvillian operator associated with the Nosé Hamiltonian. We use results from the quantum thermodynamics literature to bound the thermalization time for the discrete system. Additionally, we analyze barren plateau effects that commonly plague quantum optimization algorithms and observe that our approach is vastly less sensitive to this problem than standard gradient-based optimization. Our results suggest that these dynamical optimization approaches may be far more scalable for future quantum machine learning, optimization and variational experiments than was widely believed.
Physics Subject Headings (PhySH)
Popular Summary
We have created a quantum algorithm for local optimization problems, which gives favorable results over existing algorithms in situations in which the access to the function is provided through an encoding into the phases of a quantum state, and when the target function changes in one direction way faster than compared to the others. We accomplish this by encoding the target function into a time-dependent Hamiltonian that mimics the dynamics of a time-independent dissipative system. The dissipative dynamics suck energy out of the system, making the system lose energy and converge to a local minima. We give rigorous bounds on convergence time and amount of quantum sources needed to execute the algorithm, in addition to numerical simulations on small systems.
Article Text
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