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Rigorous error bounds for dissipative thermal state preparation from weak system-bath coupling

arXiv Quantum Physics
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Researchers from Oxford, Cambridge, and RWTH Aachen demonstrate that weak system-bath coupling strengthens error bounds in dissipative thermal state preparation, scaling as J²—proving the "Lamb shift" effect can be controlled via coupling tuning. The study builds on recent provably efficient thermalization algorithms (Chen et al., 2025) but shifts focus to analog "collision models" using resettable ancilla qubits, offering a hardware-feasible alternative to digital Lindbladian simulations. A key breakthrough shows unitary evolution from the system Hamiltonian—previously overlooked—actively improves convergence to thermal states, tightening fixed-point error bounds beyond prior rigorous approaches. Randomized implementations suppress spectral resonances in driven many-body systems, with the team quantifying the added observable variance, addressing a critical practical hurdle for near-term quantum simulators. Numerical analyses of mixing times provide concrete guidelines for experimental realization, bridging theory with hardware constraints in quantum thermalization protocols.
Rigorous error bounds for dissipative thermal state preparation from weak system-bath coupling

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Quantum Physics arXiv:2605.03011 (quant-ph) [Submitted on 4 May 2026] Title:Rigorous error bounds for dissipative thermal state preparation from weak system-bath coupling Authors:Christopher Ong, S. A. Parameswaran, Benedikt Placke, Dominik Hahn View a PDF of the paper titled Rigorous error bounds for dissipative thermal state preparation from weak system-bath coupling, by Christopher Ong and 3 other authors View PDF Abstract:Thermal state preparation is a central challenge in the simulation of quantum many-body systems. Yet, provably efficient algorithms for this task were only introduced recently [Chen et al. Nature 646, 561 (2025)]. These algorithms are based on dissipative Lindbladian evolution which exactly fixes the thermal state. Controlled and efficient digital simulation of this evolution, although possible in principle, remains out of reach for present-day quantum hardware. Subsequent work has therefore focused on analog approximations of the proposed Lindbladians via `collision models' with relatively modest requirements -- a resettable bath of ancilla qubits whose couplings to the system can be tuned in time-dependent fashion -- while still admitting rigorous fixed-point error bounds. Existing rigorous approaches, however, do not exploit the fact that these constructions generically implement not only the desired Lindblad dynamics, but also an additional unitary evolution generated by the system Hamiltonian which may aid convergence to the thermal state [Lloyd and Abanin arXiv:2506.21318 (2025)]. Here, we show that this unitary contribution does indeed tighten the fixed-point error bound and demonstrate that it is rigorously controlled by the system-bath coupling strength $J$, scaling as $J^2$. This demonstrates that the effect of the spurious `Lamb shift' term generated by the system-bath interaction can be controlled by tuning $J$. We clarify the role, previously observed, of a randomized implementation in suppressing possible resonances of the drive with the many-body spectrum, and bound the additional variance that this randomization imposes on observables. Finally, we numerically study aspects of the protocol which are relevant for its practical realization, such as the mixing time. Comments: Subjects: Quantum Physics (quant-ph); Statistical Mechanics (cond-mat.stat-mech) Cite as: arXiv:2605.03011 [quant-ph] (or arXiv:2605.03011v1 [quant-ph] for this version) https://doi.org/10.48550/arXiv.2605.03011 Focus to learn more arXiv-issued DOI via DataCite (pending registration) Submission history From: Christopher Ong [view email] [v1] Mon, 4 May 2026 18:00:06 UTC (8,596 KB) Full-text links: Access Paper: View a PDF of the paper titled Rigorous error bounds for dissipative thermal state preparation from weak system-bath coupling, by Christopher Ong and 3 other authorsView PDFTeX Source view license Current browse context: quant-ph new | recent | 2026-05 Change to browse by: cond-mat cond-mat.stat-mech References & Citations INSPIRE HEP NASA ADSGoogle Scholar Semantic Scholar export BibTeX citation Loading... BibTeX formatted citation × loading... Data provided by: Bookmark Bibliographic Tools Bibliographic and Citation Tools Bibliographic Explorer Toggle Bibliographic Explorer (What is the Explorer?) Connected Papers Toggle Connected Papers (What is Connected Papers?) Litmaps Toggle Litmaps (What is Litmaps?) scite.ai Toggle scite Smart Citations (What are Smart Citations?) Code, Data, Media Code, Data and Media Associated with this Article alphaXiv Toggle alphaXiv (What is alphaXiv?) Links to Code Toggle CatalyzeX Code Finder for Papers (What is CatalyzeX?) DagsHub Toggle DagsHub (What is DagsHub?) GotitPub Toggle Gotit.pub (What is GotitPub?) Huggingface Toggle Hugging Face (What is Huggingface?) ScienceCast Toggle ScienceCast (What is ScienceCast?) Demos Demos Replicate Toggle Replicate (What is Replicate?) Spaces Toggle Hugging Face Spaces (What is Spaces?) Spaces Toggle TXYZ.AI (What is TXYZ.AI?) Related Papers Recommenders and Search Tools Link to Influence Flower Influence Flower (What are Influence Flowers?) Core recommender toggle CORE Recommender (What is CORE?) Author Venue Institution Topic About arXivLabs arXivLabs: experimental projects with community collaborators 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. Which authors of this paper are endorsers? | Disable MathJax (What is MathJax?)

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Source: arXiv Quantum Physics