Fast Differentiation of Hyperbolic Chaos

Abstract We derive the ‘fast response’ formula for the linear response, the parameter derivatives of long-time-averaged statistics, of hyperbolic deterministic and chaotic systems. The expression is pointwisely defined, so we can compute the linear response in high-dimensions via Monte-Carlo-type algorithms. This has two parts, where the shadowing contribution is computed by the nonintrusive shadowing algorithm. The unstable contribution is expressed by renormalized second-order tangent equations; importantly, it does not contain any distributional derivatives. The algorithm’s cost is solving u , the unstable dimension, and many first-order and second-order tangent equations along a long orbit; the main error is the sampling error of the orbit. We numerically demonstrate the algorithm on a 21-dimensional example, which is difficult for previous methods.

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Publication Details

Journal
Archive for Rational Mechanics and Analysis
Published
2025-12-17
DOI
https://doi.org/10.1007/s00205-025-02160-6
Primary Topic
Chaos control and synchronization
Type
article
Field-Weighted Citation Impact
0.00

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article

Fast Differentiation of Hyperbolic Chaos

Angxiu Ni
Archive for Rational Mechanics and Analysis
Chaos control and synchronization
article

Fast Differentiation of Hyperbolic Chaos

Angxiu Ni
article en

Abstract

Abstract We derive the ‘fast response’ formula for the linear response, the parameter derivatives of long-time-averaged statistics, of hyperbolic deterministic and chaotic systems. The expression is pointwisely defined, so we can compute the linear response in high-dimensions via Monte-Carlo-type algorithms. This has two parts, where the shadowing contribution is computed by the nonintrusive shadowing algorithm. The unstable contribution is expressed by renormalized second-order tangent equations; importantly, it does not contain any distributional derivatives. The algorithm’s cost is solving u , the unstable dimension, and many first-order and second-order tangent equations along a long orbit; the main error is the sampling error of the orbit. We numerically demonstrate the algorithm on a 21-dimensional example, which is difficult for previous methods.

Archive for Rational Mechanics and AnalysisVol. 250(1)
University of California, Irvine (US)
China Postdoctoral Science Foundation
Openalex Percentile: Top 67%
Chaos control and synchronization
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