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5 results for “Chaotic Systems”

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zenodo48/100

Model output used in the manuscript "The evolution of a non-autonomous chaotic system under non-periodic forcing: a climate change example"

<p>This *.zip file contains the model output from ensemble simulations for the Lorenz 84-Stommel 61 model (<a href="https://doi.org/10.1034/j.1600-0870.2001.00241.x" target="_blank" rel="noopener">Van Veen et al, 2001</a>; <a href="https://dx.doi.org/10.1088/1748-9326/8/3/034021" target="_blank" rel="noopener">Daron and Stainforth, 2013</a>). To run these simulations, we used the Low-EFFourth ensemble generator (<a href="https://doi.org/10.48550/arXiv.2506.03313" target="_blank" rel="noopener">de Melo Vir&iacute;ssimo, 2025a</a>; <a href="https://doi.org/10.5281/zenodo.15566109" target="_blank" rel="noopener">de Melo Vir&iacute;ssimo, 2025b</a>), which is a MATLAB-based framework that allows for large ensembles of low-dimensional dynamical systems to be run and studied in a systematic way (<a href="https://doi.org/10.5194/egusphere-egu23-14755" target="_blank" rel="noopener">de Melo Vir&iacute;ssimo and Stainforth, 2023</a>).</p> <p>These model outputs are presented and discussed in the article "<em>The evolution of a non-autonomouys chaotic system under non-periodic forcing: a climate change example</em>", published by Chaos (<a href="https://doi.org/10.1063/5.0180870" target="_blank" rel="noopener">de Melo Vir&iacute;ssimo et al., 2024</a>). The manuscript describes the experiments performed, the parameter values used and the modifications done to the original L84-S61 model. For this matter, we also refer you to <a href="https://dx.doi.org/10.1088/1748-9326/8/3/034021" target="_blank" rel="noopener">Daron and Stainforth (2013)</a>.</p> <p>All files uploaded were generated from simulations run by the authors.</p> <p>For specific information about each file uploaded, please refer to the README file. If you have any questions, please feel free to contact me.</p> <p><strong>Note:</strong> This version (v1.1) is the same version as v1.0 but with the correct README file.</p>

opencc-by-4.0Sep 2023View details →
zenodo36/100

Machine Learning for predicting chaotic systems – Data

<p>The data used in our article "Machine Learning for Predicting Chaotic Systems" - <a href="https://arxiv.org/abs/2407.20158">https://arxiv.org/abs/2407.20158</a></p> <p>DeebDbDysts*.zip contain the Dysts database, DeebDbLorenz*.zip the DeebLorenz database (with DeebDbLorenzBig*.zip being the "extension" dataset for Lorenz63std with different time series lengths).</p> <p>The observation and truth data of the Dysts database originates from <a href="https://github.com/williamgilpin/dysts">https://github.com/williamgilpin/dysts</a> (we converted the data format from json to csv).</p> <p>For DeebLorenz, we used the R package <a href="https://github.com/chroetz/DEEBdata">DEEBdata</a> to create it.</p>

opencc-by-4.0Jul 2024View details →
zenodo36/100

Learning Dissipative Dynamics in Chaotic Systems (Datasets)

<p>We present the datasets for NeurIPS 2022 paper <a href="https://arxiv.org/abs/2106.06898">"Learning Dissipative Dynamics in Chaotic Systems."</a> In this work, we propose a machine learning framework, which we call the Markov Neural Operator (MNO), to learn the underlying solution operator for dissipative chaotic systems, showing that the resulting learned operator accurately captures short-time trajectories and long-time statistical behavior.</p> <p>In our work, we present results in the finite-dimensional toy system Lorenz-63. We showcase results on the 1D Kuramoto&ndash;Sivashinsky (KS) and on the 2D Navier-Stokes (Kolmogorov flows) PDEs. We present the datasets for Lorenz-63, KS, and Navier-Stokes (Reynolds numbers 40, 500, and 5000).</p> <p>The data is stored as .npy and .mat&nbsp;files:</p> <ul> <li><strong>L63.mat:&nbsp;</strong>Lorenz-63 data (one long trajectory of 10000 seconds)</li> <li><strong>KS.mat:</strong>&nbsp;1D Kuramoto&ndash;Sivashinsky data (1200 trajectories, 500 time-steps each)</li> <li><strong>2D_NS_Re40.npy: </strong>2D Navier-Stokes data (200 trajectories, 500 time-steps each) at 64 x 64&nbsp;spatial resolution.</li> <li><strong>2D_NS_Re500.npy: </strong>2D Navier-Stokes data (1000 trajectories, 500 time-steps each) at 64 x 64 spatial resolution with Reynolds number 500.</li> <li><strong>2D_NS_Re5000.npy: </strong>2D Navier-Stokes data (100 trajectories, 500 time-steps each) at 128 x 128 spatial resolution with Reynolds number 5000.</li> </ul>

opencc-by-4.0Nov 2022View details →
zenodo32/100

Time series of chaotic systems

<div> <div>&nbsp;</div> </div> <div> <p>Long time series of chaotic systems, all three-dimensional. Can be used in short- and long-term forecasting, reconstruction, etc.</p> <p>Codes in GitHub: https://github.com/Zheng-Meng/Dynamics-Reconstruction-ML.</p> <p>We used the dataset in dynamics reconstruction from sparse observations with no training on target systems:</p> <p>Zhai, Zheng-Meng, Jun-Yin Huang, Benjamin D. Stern, and Ying-Cheng Lai. "Reconstructing dynamics from sparse observations with no training on target system." <em>arXiv preprint arXiv:2410.21222</em> (2024).</p> <p>In addition, two folders with additional data, data_response, which is generated by dysts (https://github.com/williamgilpin/dysts) and data_nonautonomous, are provided for further evaluation of the dynamics reconstruction framework.</p> <p>&nbsp;</p> </div>

opencc-by-4.0Oct 2024View details →
zenodo28/100

Chaotic Dynamics in a Two-Droplet Pilot Wave System: A Numerical Simulation

<p>Data set and results for our university modeling project.</p>

opencc-by-4.0Jul 2022View details →

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International Brain Laboratory public data

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