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This paper advances the mathematical understanding of Lee-Yang tensors and Suzuki-Fisher Hamiltonians, establishing new geometric bounds for spectral gaps in quantum many-body systems. By generalizing lemmas from complex Perron-Frobenius theory, it clarifies the conditions under which Gibbs states maintain specific analytic properties across all inverse temperatures. These theoretical results are foundational for analyzing phase transitions and stability in quantum simulation algorithms.
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The Geometry of Lee-Yang Tensors

arXiv2 min read

arXiv:2610.09485v1 Announce Type: new Abstract: We provide a geometric description of Lee-Yang tensors, building upon several recent results of Bravyi, Gosset, Liu, and Wong. By applying tools from complex Perron-Frobenius theory, we generalize one of their key lemmas to bound the spectral ratio of non-normal operators with Lee-Yang radius greater than one. As a direct consequence, we provide a local-to-global principle for bounding spectral gaps of Suzuki-Fisher Hamiltonians, a family of $2$-local Hamiltonians, using only the Lee-Yang radius of each local operator to bound the gap from below. On the other hand, we develop a simple perturbative technique to show that the Gibbs states of $k$-local Hamiltonians, $k \geq 3$, cannot have Lee-Yang radius at least one for all inverse temperatures $\beta \geq 0$. We apply this same method to conclude that Suzuki-Fisher Hamiltonians are precisely those Hamiltonians whose Gibbs states are Lee-Yang at all inverse temperatures $\beta \geq 0$.

Abstract:We provide a geometric description of Lee-Yang tensors, building upon several recent results of Bravyi, Gosset, Liu, and Wong. By applying tools from complex Perron-Frobenius theory, we generalize one of their key lemmas to bound the spectral ratio of non-normal operators with Lee-Yang radius greater than one. As a direct consequence, we provide a local-to-global principle for bounding spectral gaps of Suzuki-Fisher Hamiltonians, a family of $2$-local Hamiltonians, using only the Lee-Yang radius of each local operator to bound the gap from below. On the other hand, we develop a simple perturbative technique to show that the Gibbs states of $k$-local Hamiltonians, $k \geq 3$, cannot have Lee-Yang radius at least one for all inverse temperatures $\beta \geq 0$. We apply this same method to conclude that Suzuki-Fisher Hamiltonians are precisely those Hamiltonians whose Gibbs states are Lee-Yang at all inverse temperatures $\beta \geq 0$.

Quantum Physics (quant-ph); Mathematical Physics (math-ph); Complex Variables (math.CV)

arXiv:2610.09485 [quant-ph]

(or arXiv:2610.09485v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2610.09485 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 245 words

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