Regularity determines the quantum loading cost of rough functions

We determine the gate complexity of amplitude encoding (loading) for rough functions. For a function of Hölder regularity s > 0 and target infidelity δ, the worst-case cost is Θ̃(δ^{-1/(2s)}), independent of the number of qubits n for every s > 0. The tilde hides factors polylogarithmic in n and 1/δ. Upper bound. The construction is explicit. The function is approximated by piecewise polynomials of degree below ⌈s⌉ on 2^J dyadic intervals. The resulting state is an arbitrary state on about J qubits, followed by a fixed polynomial isometry that is the same for every interval and acts on only O(log(1/δ)) qubits; the remaining qubits are put in |+⟩ by Hadamard gates. No periodicity and no quantum wavelet transform are needed. For 0 < s ≤ 1 the construction reduces to Haar coarse-graining. Lower bound. A packing argument over sign patterns gives the matching lower bound. It holds for any finite gate set and allows ancillas and mixed outputs. A Gaussian version, based on Anderson’s inequality and small-ball probabilities, extends it to correlated Gaussian vectors. Combined with a bound on the smallest eigenvalue of the level-wise Haar covariance, it shows that loading a given fractional Brownian path with Hurst index H costs Θ̃(δ^{-1/(2H)}) with high probability. For rough-volatility paths (H ≈ 0.1) this is δ^{-5}

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-14
DOI
https://doi.org/10.5281/zenodo.23383168
Primary Topic
Quantum Computing Algorithms and Architecture
Type
preprint
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preprint

Regularity determines the quantum loading cost of rough functions

ming Cheng
Zenodo (CERN European Organization for Nuclear Research)
Quantum Computing Algorithms and Architecture
preprint

Regularity determines the quantum loading cost of rough functions

ming Cheng
preprint en

Abstract

We determine the gate complexity of amplitude encoding (loading) for rough functions. For a function of Hölder regularity s > 0 and target infidelity δ, the worst-case cost is Θ̃(δ^{-1/(2s)}), independent of the number of qubits n for every s > 0. The tilde hides factors polylogarithmic in n and 1/δ. Upper bound. The construction is explicit. The function is approximated by piecewise polynomials of degree below ⌈s⌉ on 2^J dyadic intervals. The resulting state is an arbitrary state on about J qubits, followed by a fixed polynomial isometry that is the same for every interval and acts on only O(log(1/δ)) qubits; the remaining qubits are put in |+⟩ by Hadamard gates. No periodicity and no quantum wavelet transform are needed. For 0 < s ≤ 1 the construction reduces to Haar coarse-graining. Lower bound. A packing argument over sign patterns gives the matching lower bound. It holds for any finite gate set and allows ancillas and mixed outputs. A Gaussian version, based on Anderson’s inequality and small-ball probabilities, extends it to correlated Gaussian vectors. Combined with a bound on the smallest eigenvalue of the level-wise Haar covariance, it shows that loading a given fractional Brownian path with Hurst index H costs Θ̃(δ^{-1/(2H)}) with high probability. For rough-volatility paths (H ≈ 0.1) this is δ^{-5}

Zenodo (CERN European Organization for Nuclear Research)
"Dunarea de Jos" University of Galati (RO)
Quantum Computing Algorithms and Architecture
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