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Matchgate circuit representation of fermionic Gaussian states: optimal preparation, approximation, and classical simulation

arXiv Quantum Physics
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⚡ Quantum Brief
Researchers led by Barbara Kraus and Frank Pollmann established optimal bounds for preparing fermionic Gaussian states (FGS) using matchgate circuits, proving these highly entangled states can be efficiently created with minimal quantum gates. The team derived exact gate-count limits for matchgate-only circuits and asymptotic bounds for general nearest-neighbor gates, providing rigorous benchmarks for quantum state preparation in condensed matter and quantum information systems. New algorithms were developed to construct circuits that meet these bounds, enabling exact or approximate FGS preparation while minimizing computational overhead, with direct applications in quantum simulation and error mitigation. A novel classical simulation method was introduced, leveraging FGS-generating circuits to efficiently model matchgate dynamics, reinforcing that these states remain classically tractable despite their entanglement complexity. The framework was extended to t-doped Gaussian states, hinting at broader applications for doped fermionic systems in quantum chemistry and materials science.
Matchgate circuit representation of fermionic Gaussian states: optimal preparation, approximation, and classical simulation

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Quantum Physics arXiv:2603.05675 (quant-ph) [Submitted on 5 Mar 2026] Title:Matchgate circuit representation of fermionic Gaussian states: optimal preparation, approximation, and classical simulation Authors:Marc Langer, Raúl Morral-Yepes, Adam Gammon-Smith, Frank Pollmann, Barbara Kraus View a PDF of the paper titled Matchgate circuit representation of fermionic Gaussian states: optimal preparation, approximation, and classical simulation, by Marc Langer and 4 other authors View PDF Abstract:Fermionic Gaussian states (FGSs) and the associated matchgate circuits play a central role in quantum information theory and condensed matter physics. Despite being possibly highly entangled, they can still be efficiently simulated on classical computers. We address the question of how to optimally create such states when using matchgate circuits acting on product states. To this end, we derive lower bounds on the number of gates required to prepare an arbitrary pure FGS: We establish both an asymptotic bound on the minimal gate count over general nearest-neighbor gate sets and an exact bound for circuits composed solely of matchgates. We present explicit algorithms whose constructions saturate these bounds, thereby proving their optimality. We furthermore determine when an FGS can be prepared with a circuit of any given depth, and derive an algorithm that constructs such a circuit whenever this condition is satisfied, either exactly or approximately. Our results have direct applications to (approximate) state preparation and to disentangling procedures. Moreover, we introduce a new classical simulation algorithm for matchgate circuits, based entirely on manipulating the generating circuits of the FGSs. Finally, we briefly study an extension of our framework for $t$-doped Gaussian states and circuits. Comments: Subjects: Quantum Physics (quant-ph) Cite as: arXiv:2603.05675 [quant-ph] (or arXiv:2603.05675v1 [quant-ph] for this version) https://doi.org/10.48550/arXiv.2603.05675 Focus to learn more arXiv-issued DOI via DataCite Submission history From: Marc Langer [view email] [v1] Thu, 5 Mar 2026 21:06:06 UTC (996 KB) Full-text links: Access Paper: View a PDF of the paper titled Matchgate circuit representation of fermionic Gaussian states: optimal preparation, approximation, and classical simulation, by Marc Langer and 4 other authorsView PDFTeX Source view license Current browse context: quant-ph new | recent | 2026-03 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?) Links to Code Toggle Papers with Code (What is Papers with Code?) 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