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This research introduces a method to quantify quantum "magic"—a resource essential for computational advantage—using out-of-time-order correlators in arbitrary states, including thermal ensembles. By establishing that this measure vanishes precisely for Clifford evolutions, the work provides a rigorous lower bound on the number of non-Clifford $T$ gates required to simulate specific quantum dynamics. The findings directly advance our understanding of quantum simulation complexity and the physical detectability of resources necessary for universal quantum computation.
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Pauli instability in arbitrary states: detecting magic in physical correlators

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arXiv:2609.40032v1 Announce Type: new Abstract: Measures of non-stabilizerness (``magic'') of a quantum evolution quantify how hard it is to simulate on a classical computer. A natural question is how to extract information about magic from physical correlators, for example at finite temperature or in the ground state. In this paper we show how to measure magic using out-of-time-order correlators evaluated in an arbitrary state. For every full-rank state, and in particular for every Gibbs state, the resulting quantity vanishes if and only if the evolution is Clifford. We establish its basic properties, relate it to the stabilizer entropy of the Choi state, and prove that, even with a single fixed probe operator, it gives a lower bound on the number of $T$ gates needed to implement the dynamics in any circuit architecture.

Abstract:Measures of non-stabilizerness (``magic'') of a quantum evolution quantify how hard it is to simulate on a classical computer. A natural question is how to extract information about magic from physical correlators, for example at finite temperature or in the ground state. In this paper we show how to measure magic using out-of-time-order correlators evaluated in an arbitrary state. For every full-rank state, and in particular for every Gibbs state, the resulting quantity vanishes if and only if the evolution is Clifford. We establish its basic properties, relate it to the stabilizer entropy of the Choi state, and prove that, even with a single fixed probe operator, it gives a lower bound on the number of $T$ gates needed to implement the dynamics in any circuit architecture.

Quantum Physics (quant-ph); Statistical Mechanics (cond-mat.stat-mech); High Energy Physics - Theory (hep-th)

arXiv:2609.40032 [quant-ph]

(or arXiv:2609.40032v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.40032 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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