aiqbench analysis
This research establishes rigorous rates of exponential relative-entropy decay for infinite-dimensional quantum Gibbs samplers, advancing the theoretical understanding of convergence in complex quantum systems like Bose-Hubbard models and Coulomb gases. By leveraging perturbative stability theory for hypercontractive estimates, the study provides critical mathematical bounds essential for analyzing the efficiency of quantum sampling algorithms in high-dimensional Hilbert spaces.
Hypercontractivity and entropy decay for infinite-dimensional quantum Gibbs samplers
arXiv:2610.06764v1 Announce Type: new Abstract: We derive rates of exponential relative-entropy decay for a broad class of infinite-dimensional quantum Gibbs samplers. A key technical ingredient is a perturbative stability theory for hypercontractive estimates and logarithmic Sobolev inequalities. For suitably chosen dissipative couplings, we obtain exponential entropy decay for full multimode Bose-Hubbard samplers with arbitrary hopping and repulsive density interactions. For harmonically confined quantum Coulomb gases and molecular systems, we prove exponential entropy decay for every fixed finite-rank low-energy truncation of the interaction. Finally, we exhibit a periodic charging model with a positive spectral gap but no finite-time $L^2$-to-$L^p$ bound for any $p>2$.
Abstract:We derive rates of exponential relative-entropy decay for a broad class of infinite-dimensional quantum Gibbs samplers. A key technical ingredient is a perturbative stability theory for hypercontractive estimates and logarithmic Sobolev inequalities. For suitably chosen dissipative couplings, we obtain exponential entropy decay for full multimode Bose-Hubbard samplers with arbitrary hopping and repulsive density interactions. For harmonically confined quantum Coulomb gases and molecular systems, we prove exponential entropy decay for every fixed finite-rank low-energy truncation of the interaction. Finally, we exhibit a periodic charging model with a positive spectral gap but no finite-time $L^2$-to-$L^p$ bound for any $p>2$.
arXiv:2610.06764 [quant-ph]
(or arXiv:2610.06764v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2610.06764 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
arXivLabs is a framework that allows collaborators to develop and share new arXiv features directly on our website.
Both individuals and organizations that work with arXivLabs have embraced and accepted our values of openness, community, excellence, and user data privacy. arXiv is committed to these values and only works with partners that adhere to them.
Have an idea for a project that will add value for arXiv's community? Learn more about arXivLabs.
Full text under the publisher's open licence · 188 words
Related coverage

Gibbs state preparation for commuting Hamiltonian: Mapping to classical Gibbs sampling
Quantum Journal · Sep 18, 2026

Researchers Link Entropy Decay to BKM Coercivity
Quantum Zeitgeist · Sep 18, 2026
Relative Entropy Decay via BKM coercivity for Quantum Markov Semigroups
arXiv · Sep 15, 2026

Researchers chart collective entanglement in quantum matter
Quantum Zeitgeist · Sep 10, 2026