quant-phAug 25, 2026

Provable Quantum-Classical Separation for Continuous Gibbs Sampling

Authors: Enrico Olivucci, Mariia Sobchuk, Sehmimul Hoque, Jeffrey Hnybida, Kyungho W. Kim, Ala Shayeghi, Pooya Ronagh

Organizations: 1Irr´eversible Inc., Sherbrooke, Qu´ebec, Canada · Institute for Quantum Computing, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada · Department of Physics and Astronomy, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada · 4Perimeter Institute for Theoretical Physics, Waterloo, Ontario N2L 2Y5, Canada · 5National Research Council Canada, Waterloo, Ontario, N2L 3G1, Canada · 6Microsoft, Redmond, WA 98052, USA

Abstract

We prove the first quantum-classical separation for a sampling problem over a continuous domain. For a class of Gibbs states p∝e−βEp\propto e^{-βE} on the torus Td\mathbb{T}^d with smooth (ss-Gevrey) potential and barrier amplitude α=eβΔα=e^{βΔ}, where Δ=max⁡E−min⁡EΔ= \max E-\min E, every classical algorithm querying the value, gradient, or any higher-order derivatives of the log-density requires Ω(α)Ω(α) queries to sample at constant accuracy in total variation distance, while a quantum algorithm based on quantum singular value thresholding and temperature annealing samples with O~(α)\tilde{O}\left(\sqrtα\right) queries to an oracle for the gradient. The advantage is quadratic in the barrier amplitude, which becomes exponential in the dimension, eΩ(d)e^{Ω(d)}, at low temperature. The classical bound is information-theoretic, holding for every classical algorithm with query access to the Gibbs potential and its derivatives at any order.

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