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		<title>Chaos and Fractal Toolkit expanded with Correlation Integral and Lyapunov analysis</title>
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		<description>edge's Blog: Chaos and Fractal Toolkit expanded with Correlation Integral and Lyapunov analysis</description>
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			<title>Original Blog Entry: Chaos and Fractal Toolkit expanded with Correlation Integral and Lyapunov analysis</title>
			<link>/blogentry/30655</link>
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			<pubDate>Sun, 21 Jun 2009 23:12:33 GMT</pubDate>
			<dc:creator>edge</dc:creator>
			<description><![CDATA[<p>Re-encoded Mathematica notebook (ref. 1) into C++ classes, calculations were checked by hand and Henon attractor has emerged together with the exact Correlation Integral in the agreement with Fractal Dimension calculations from other sources. (approximately ~ 1.26) [Best Fit: Y = -1.36378 + 1.2656 X]<br /><br />Correlation Integral is of the form Log[Corr] = D Log [R] and its importance lies in detecting chaos/fractal property in a data series.<br /><br />Henon attractor has specific fractal dimension (approx 1.26) and exhibits chaotic orbits around an attractor (see below) these orbits are invariant in a sense that they exhibit certain pseudo periodicity (pseudo, as the points will not re-generate in the exact position in the number plane but rather do so on ever enlarging scale)<br /><br />Next in this project is Lyapunov exponent, which measures how fast this scale expansion happens, if the rate is slow, the orbits can be of stable/periodic or chaotic type<br /><br />(they can also start to escape to infinity or converge to point).<br /><br />Hurst exponent will tell us how smooth trajectories are (and is related to fractal dimension), we already have its first manifestation in Correlation Integral in the Henon attractor, it i useful insofar as to be able to approximate one data series with another (ie Henon map with some n-dimensional embedding added)<br /><br />Below are various images and output displays related to the above, much still has to be done, but serious progress has been made.<br /><br />Best fit (linear) Best Fit: Y = -1.36378 + 1.2656 X<br /><br />in the full agreement with independent calculation of Hurst exponent for Henon map attractor (~ 2.26)<br /><br />Lyapunov exponents for various (random) sequences<br /><br />1 periodic -0.103898<br /><br />3 chaotic 0.565543<br /><br />4 chaotic 0.259456<br /><br />5 chaotic 0.8249<br /><br />8 chaotic 0.465392<br /><br />9 chaotic 0.381847<br /><br />10 periodic -0.0727799<br /><br />11 chaotic 0.669459<br /><br />12 periodic -0.178313<br /><br />13 periodic -0.0211324<br /><br />14 chaotic 0.802993<br /><br />15 chaotic 0.469818<br /><br />16 chaotic 0.196232<br /><br />17 chaotic 0.976126<br /><br />Results (88 seconds)<br /><br />Infinite: 0 (0.0%)<br /><br />Point : 4 (22.2%)<br /><br />Stable : 0 (0.0%)<br /><br />Periodic: 4 (22.2%)<br /><br />Chaotic : 10 (55.6%)<br /><br />Attractor images (only stable (0 found in this particular trial), periodic and chaotic images are displayed (infinite and point have no visual representation possible)<br /><br />References:<br /><br />1. Testing Chaos and Fractal Properties in Economic Time Series<br /><br />http://www.internationalmathematicasymposium.org/IMS99/paper25/ims99paper25.pdf<br /><br />2. Numerical best fit linear estimation to determine Correlation Integral were performed using GSL - GNU Scientific Library:<br /><br />http://www.gnu.org/software/gsl/<br /><br />3. Images showcasing attractors and their Lyapunov exponents were generated using ideas and sample application found at:<br /><br />http://www.technocosm.org/chaos/attr-part2.html<br /><br />... &#x5b;&#xa0;<a href="/blogentry/30655">More</a>&#xa0;&#x5d;</p>]]></description>
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