2023
DOI: 10.1103/physreva.108.042408
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Measuring nonstabilizerness via multifractal flatness

Xhek Turkeshi,
Marco Schirò,
Piotr Sierant
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Cited by 14 publications
(6 citation statements)
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“…The lack of recovery of the OTOC signals a non-Clifford and entangling random quantum circuit dynamics in particular (and non-integrable dynamics in general), as stated in [62] and shown by numerical simulations of reference [63, figure 7, p 29]. As a side note, intriguingly, entanglement and non-stabilizerness are not entirely uncorrelated properties, as it has recently been shown that the flatness of the entanglement spectrum [73,74] can be used to certify non-stabilizerness of quantum states.…”
Section: Scrambling and Quantum Chaosmentioning
confidence: 87%
“…The lack of recovery of the OTOC signals a non-Clifford and entangling random quantum circuit dynamics in particular (and non-integrable dynamics in general), as stated in [62] and shown by numerical simulations of reference [63, figure 7, p 29]. As a side note, intriguingly, entanglement and non-stabilizerness are not entirely uncorrelated properties, as it has recently been shown that the flatness of the entanglement spectrum [73,74] can be used to certify non-stabilizerness of quantum states.…”
Section: Scrambling and Quantum Chaosmentioning
confidence: 87%
“…Interesting research direction going forward is to combine our sampling approach with experiment [30] or approximate numerical methods such as tensor networks [32,46] and neural networks [33]. Our method can be used alongside or as a complement to other existing approximation methods [47][48][49][50][51][52]. Specifically, the algorithm introduced in [48] is an efficient method for measuring Tsallis stabilizer entropy which has a direct relation to stabilizer Renyi entropy.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…Nevertheless, due to the invariance of the considered circuits under local basis rotations, our results remain valid for any basis of obtained by a unitary transformation of the computational basis, where belongs to the unitary group for a single qudit. For the computational basis, , which defines the “book” boundary condition for each qudit [ 83 , 84 ]: where the superscript in bookkeeps the number of the affected qudit. For later convenience, we recast the problem in the superoperator formalism.…”
Section: Methodsmentioning
confidence: 99%
“…We begin our discussion by reviewing the Hilbert space delocalization of random states [ 21 , 83 ] which correspond to the stationary ensemble of states obtained under the action of sufficiently deep random circuits. Uniformly distributed random states in the Hilbert space are obtained from a reference state via a unitary operation U acting globally on the system of N qudits, drawn with the Haar measure from the N qudit unitary group , where d is the qudit local Hilbert space dimension.…”
Section: Delocalization Properties Of Random Haar Statesmentioning
confidence: 99%
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