2022
DOI: 10.48550/arxiv.2203.16571
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Random quantum circuits are approximate unitary $t$-designs in depth $O\left(nt^{5+o(1)}\right)$

Jonas Haferkamp

Abstract: The applications of random quantum circuits range from quantum computing and quantum many-body systems to the physics of black holes. Many of these applications are related to the generation of quantum pseudorandomness: Random quantum circuits are known to approximate unitary t-designs. Unitary t-designs are probability distributions that mimic Haar randomness up to tth moments. In a seminal paper, Brandão, Harrow and Horodecki prove that random quantum circuits in a brickwork architecture of depth O(nt 10.5 … Show more

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Cited by 5 publications
(9 citation statements)
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“…The purpose of this paper is to show that a wide variety of Brownian quantum many-body systems form good approximate k-designs in time linear in k. This scal-ing of the time-to-design is essentially optimal in its kdependence up to a log k factor [12,18], so our results establish that these quantum chaotic model systems are optimal generators of quantum randomness [26]. Our calculations build on a growing body of work featuring random circuits and Brownian models [20,[27][28][29][30][31][32][33][34][35][36][37][38][39][40], which have been used to establish polynomial complexity growth in specific circuit constructions. Our Brownian spin and fermion models are based on similar technical methods, but the simple mean-field nature of our models allows us to straightforwardly establish linear complexity growth in a large-N limit.…”
Section: Introductionmentioning
confidence: 67%
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“…The purpose of this paper is to show that a wide variety of Brownian quantum many-body systems form good approximate k-designs in time linear in k. This scal-ing of the time-to-design is essentially optimal in its kdependence up to a log k factor [12,18], so our results establish that these quantum chaotic model systems are optimal generators of quantum randomness [26]. Our calculations build on a growing body of work featuring random circuits and Brownian models [20,[27][28][29][30][31][32][33][34][35][36][37][38][39][40], which have been used to establish polynomial complexity growth in specific circuit constructions. Our Brownian spin and fermion models are based on similar technical methods, but the simple mean-field nature of our models allows us to straightforwardly establish linear complexity growth in a large-N limit.…”
Section: Introductionmentioning
confidence: 67%
“…Before going further, we need to define good approximate k-designs. Given an ensemble E of unitaries acting on H, the k-th moment map ME,k acts on an operator X on H ⊗k as [39] ME,k (X) = E U ∈E U ⊗k X(U † ) ⊗k .…”
Section: Formal Definitions Of K-designsmentioning
confidence: 99%
“…Specifically, it is known that if one takes the local dimension to be large (e.g. q ≥ 6k 2 ) the spectral gap is constant and the design depth scales linearly in k. Quite recently, the exponent in Theorem 2 was improved from k 9.5 to k 4+o (1) via an improved RQC spectral gap [55].…”
Section: Designs From Local Quantum Circuitsmentioning
confidence: 99%
“…As the above theorem only holds for moments up to the square root of the dimension, we can use an exponentially small but k-independent spectral gap, proved in Refs. [19,55], to establish that exponentially deep random circuits form high degree designs.…”
Section: Designs From Local Quantum Circuitsmentioning
confidence: 99%
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