Microscale Lyapunov contraction precedes macroscopic seismic rupture in simulations

Introduction: Laboratory and numerical studies show that fault complexity, quantified by the Kaplan–Yorke dimension (effective number of dynamical degrees of freedom), can decrease as stress and load increase, but the reason remains uncertain. Materials and methods: We analyze a synthetic seismic cycle from a previously validated heterogeneous-rupture model: moment magnitude M W (macroscopic earthquake size) and its perturbation response Δ M W (magnitude change after a small energy increase). A thermodynamic estimate gives Λ , the sum of all Lyapunov exponents, which measure whether nearby states diverge (expansion) or converge (contraction). In sliding windows of W = 100 samples, k -nearest neighbors (KNN) forecasts yield a finite-horizon stability descriptor λ ^ M W , the slope of log forecast error versus forecast horizon. λ ^ M W is positive, negative or zero when errors grow (expansion), shrink (contraction) and are neutral, respectively. As M W is macroscopic, subtracting λ ^ M W from Λ leaves a residual λ R , the microscopic part. Slopes require straight-line fits (coefficient of determination R 2 ≥ 0.98, normalized mean absolute error ≤ 0.08) over four or more early horizons; robustness is tested with W = 80 and W = 120. Results: In M W , 334 of 460 windows (72.

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Publication Details

Journal
Academia Earth and Planetary Science
Published
2026-10-26
DOI
https://doi.org/10.20935/acadeps8619
Primary Topic
earthquake and tectonic studies
Type
article
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article

Microscale Lyapunov contraction precedes macroscopic seismic rupture in simulations

Patricio Venegas-Aravena, Andrei Velichko
Academia Earth and Planetary Science
earthquake and tectonic studies
article

Microscale Lyapunov contraction precedes macroscopic seismic rupture in simulations

Patricio Venegas-Aravena, Andrei Velichko
article en

Abstract

Introduction: Laboratory and numerical studies show that fault complexity, quantified by the Kaplan–Yorke dimension (effective number of dynamical degrees of freedom), can decrease as stress and load increase, but the reason remains uncertain. Materials and methods: We analyze a synthetic seismic cycle from a previously validated heterogeneous-rupture model: moment magnitude M W (macroscopic earthquake size) and its perturbation response Δ M W (magnitude change after a small energy increase). A thermodynamic estimate gives Λ , the sum of all Lyapunov exponents, which measure whether nearby states diverge (expansion) or converge (contraction). In sliding windows of W = 100 samples, k -nearest neighbors (KNN) forecasts yield a finite-horizon stability descriptor λ ^ M W , the slope of log forecast error versus forecast horizon. λ ^ M W is positive, negative or zero when errors grow (expansion), shrink (contraction) and are neutral, respectively. As M W is macroscopic, subtracting λ ^ M W from Λ leaves a residual λ R , the microscopic part. Slopes require straight-line fits (coefficient of determination R 2 ≥ 0.98, normalized mean absolute error ≤ 0.08) over four or more early horizons; robustness is tested with W = 80 and W = 120. Results: In M W , 334 of 460 windows (72.

Academia Earth and Planetary ScienceVol. 1(4)
Petrozavodsk State University (RU)
Openalex Percentile: Top 18%
earthquake and tectonic studies
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