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How to Construct Random Unitaries

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arxiv 2410.10116 v3 pith:J4Z2KR27 submitted 2024-10-14 quant-ph cs.CCcs.CLmath-phmath.MP

classification quant-phcs.CCcs.CLmath-phmath.MP
keywords prusunitariesunitaryefficienthaar-randommakesnotionquantum
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

The existence of pseudorandom unitaries (PRUs) -- efficient quantum circuits that are computationally indistinguishable from Haar-random unitaries -- has been a central open question, with significant implications for cryptography, complexity theory, and fundamental physics. In this work, we close this question by proving that PRUs exist, assuming that any quantum-secure one-way function exists. We establish this result for both (1) the standard notion of PRUs, which are secure against any efficient adversary that makes queries to the unitary $U$, and (2) a stronger notion of PRUs, which are secure even against adversaries that can query both the unitary $U$ and its inverse $U^\dagger$. In the process, we prove that any algorithm that makes queries to a Haar-random unitary can be efficiently simulated on a quantum computer, up to inverse-exponential trace distance.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Quantum Simulation of Random Unitaries from Clebsch-Gordan Transforms

    quant-ph 2025-09 accept novelty 7.0 of 10

    Clebsch-Gordan transforms give exact compressed oracles for Haar-random unitary group actions, with efficient circuits for U(d).

  2. Pseudorandom Dynamics in the SYK Model and Cryptographic Censorship in JT Gravity

    hep-th 2026-05 unverdicted novelty 6.0 of 10

    SYK disorder is shown to be an approximate unitary k-design for poly(N) k; under the planted-SYK hardness conjecture this yields gravitationally pseudorandom unitaries, implying cryptographic censorship in JT gravity ...

  3. Non-Clifford Cost of Random Unitaries

    quant-ph 2025-05 unverdicted novelty 6.0 of 10

    Rigorous bounds establish that t = Theta(k^2) non-Clifford gates are necessary and sufficient for frame-potential approximation to unitary k-designs while t = Theta(nk) suffices for relative-error k-designs.

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