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Random Quantum Circuits Beyond Moment Matching

Published 1 Oct 2026 in quant-ph | (2610.02135v1)

Abstract: Random quantum circuits aim to efficiently reproduce the statistical properties of ideal random quantum evolution. One approach is to construct approximate unitary designs, which match the moments of Haar-random unitaries up to a prescribed order with controlled error. In this work, we establish quantitative guarantees for how accurately these designs reproduce the full distributions of individual output probabilities. We show that, for every strong ε\varepsilon-approximate unitary kk-design on nn qubits, the distribution of each individual output probability is within O(2<sup>nk(k+2<sup>n)+ε)O\left(\sqrt{\frac{2<sup>n}{k(k+2<sup>n)}}+\varepsilon\right) in Kolmogorov distance of the finite-dimensional Porter-Thomas distribution, a beta distribution with parameters $1$ and $2n-1$. This bound is optimal up to constant factors, implying that a substantially better uniform bound requires additional structure. We further show that local invariance yields an exponential improvement in the dependence on kk, with guarantees also in the stronger metric of total variation: every strong ε\varepsilon-approximate unitary kk-design invariant under unitary translations acting on log⁡k+O(1)\log k+O(1) qubits achieves error 2<sup>−Ω(k)+O(ε)2<sup>{-Ω(k)}+O(\varepsilon) in Kolmogorov distance and 2<sup>−Ω(k)+O(εlog⁡(2/ε))2<sup>{-Ω(k)}+O(\varepsilon\log(2/\varepsilon)) in total variation distance. These results identify both the distributional accuracy guaranteed by moment matching and the additional structure that substantially improves it. As an application, we show that if the marginal distribution of each output probability of a strong approximate design is within Kolmogorov distance ηη of its Haar counterpart, then the expected Shannon entropy of the output distribution differs from its Haar value by O(η)O(\sqrtη).

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