aiqbench analysis
This paper is theoretical quantum many-body physics: a method that computes the Lieb-Robinson correlation function in transverse-field Ising chains with cost scaling linearly in system size, applied to chains over a thousand qubits. It also finds that increasing disorder localizes quantum information and that the correlation length peaks at the phase transition. For quantum readers, the practical interest is the classical simulation technique and what it implies about information spreading in spin systems relevant to quantum hardware, not any immediate device or algorithm.
The Lieb-Robinson correlation function for long disordered transverse-field Ising chains
arXiv:2512.22395v2 Announce Type: replace Abstract: The Lieb-Robinson correlation function can be used to characterize the propagation of quantum information in Ising chains. Considerable work has been done to establish bounds on this correlation function in various circumstances. To actually calculate the value of the correlation function directly typically requires a state space which grows exponentially with system size, and so is intractable for all but relatively small systems. We employ a recently-developed method that enables direct calculation of the Lieb--Robinson correlation function and which scales linearly with system size. This enables the computation for systems with more than a thousand qubits, revealing the propagation of quantum information down the chain. We extend this technique to the problem of Ising chains with randomly disordered coupling strengths. Increasing disorder causes localization of the quantum correlations and halts propagation of quantum information down the chain. We see light-cone isocontours therefore becoming vertical. The decay of correlations down the chain is characterized by a correlation length which in the paramagnetic phase increases quadratically with mean coupling strength and inverse quadratically with disorder level. The correlation length peaks at the phase transition. We map our general expression for the correlation function in the Ising system onto the probability density in the single particle tight-binding Su-Schrieffer-Heeger model for a specific initial condition.
Abstract:The Lieb-Robinson correlation function can be used to characterize the propagation of quantum information in Ising chains. Considerable work has been done to establish bounds on this correlation function in various circumstances. To actually calculate the value of the correlation function directly typically requires a state space which grows exponentially with system size, and so is intractable for all but relatively small systems. We employ a recently-developed method that enables direct calculation of the Lieb--Robinson correlation function and which scales linearly with system size. This enables the computation for systems with more than a thousand qubits, revealing the propagation of quantum information down the chain. We extend this technique to the problem of Ising chains with randomly disordered coupling strengths. Increasing disorder causes localization of the quantum correlations and halts propagation of quantum information down the chain. We see light-cone isocontours therefore becoming vertical. The decay of correlations down the chain is characterized by a correlation length which in the paramagnetic phase increases quadratically with mean coupling strength and inverse quadratically with disorder level. The correlation length peaks at the phase transition. We map our general expression for the correlation function in the Ising system onto the probability density in the single particle tight-binding Su-Schrieffer-Heeger model for a specific initial condition.
arXiv:2512.22395 [quant-ph]
(or arXiv:2512.22395v2 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2512.22395 Focus to learn more arXiv-issued DOI via DataCite
Phys. Rev. Research 8, 033292 (2026)
https://doi.org/10.1103/xd68-dpwm Focus to learn more DOI(s) linking to related resources
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Full text under the publisher's open licence · 316 words
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