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This study establishes genuine multipartite nonlocality as the critical resource enabling universal computation in fermionic systems, distinguishing it from classical simulability and mean-field states. By certifying this phenomenon on 48 qubits of IBM processors, the research provides a concrete benchmark for understanding the limits of free fermion simulations versus full quantum advantage.
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Genuine Multipartite Nonlocality Is Fermionic Magic

arXiv1 min read

arXiv:2609.39411v1 Announce Type: new Abstract: A system of free fermions can be simulated on a classical computer, and a single non-Gaussian state makes it a universal quantum computer. We show that the same line bounds quantum nonlocality. Measured as fermionic qubits, free fermions carry the Bell nonlocality of one entangled pair, no more, however many parties share them, and are never genuinely multipartite nonlocal. Fermion parity is the reason. Genuine multipartite nonlocality is thus the resource of universal fermionic computation, cannot arise from any mean-field state, and we certify it on $48$ qubits of IBM processors.

Abstract:A system of free fermions can be simulated on a classical computer, and a single non-Gaussian state makes it a universal quantum computer. We show that the same line bounds quantum nonlocality. Measured as fermionic qubits, free fermions carry the Bell nonlocality of one entangled pair, no more, however many parties share them, and are never genuinely multipartite nonlocal. Fermion parity is the reason. Genuine multipartite nonlocality is thus the resource of universal fermionic computation, cannot arise from any mean-field state, and we certify it on $48$ qubits of IBM processors.

arXiv:2609.39411 [quant-ph]

(or arXiv:2609.39411v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.39411 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 182 words

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