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Case IV: experiments on signals of cases II and III with imposed additive Gaussian noise.

By Amir E. BozorgMagham (763102), Safa Motesharrei (763103), Stephen G. Penny (763104) and Eugenia Kalnay (763105)


<p>We consider noise levels at 5% and 10% of the standard deviation of the original signals in cases II and III. (a) Δ<i>ρ</i> at <i>L</i> = 500 as a function of </p><p><math><mrow><msub><mi>η</mi><mo>¯</mo><mi>N</mi></msub><mo>/</mo><msub><mi>μ</mi><mo>¯</mo><mi>N</mi></msub></mrow></math></p> for signals of case II. (b) Δ<i>ρ</i> at <i>L</i> = 500 as a function of <p><math><mrow><msub><mi>η</mi><mo>¯</mo><mi>N</mi></msub><mo>/</mo><msub><mi>μ</mi><mo>¯</mo><mrow><mi>W</mi><mi>b</mi></mrow></msub></mrow></math></p> for signals of case III. Δ<i>ρ</i> = 0 and <p><math><mrow><msub><mi>η</mi><mo>¯</mo><mi>N</mi></msub><mo>/</mo><msub><mi>μ</mi><mo>¯</mo><mi>N</mi></msub><mo>=</mo><mn>1</mn></mrow></math></p> are shown by dashed, bold lines.<p></p

Topics: Uncategorised, ccm, results show, Convergent Cross Mapping, experiment, iii, Causality Analysis, Lorenz systems, coefficient schemes, case IV, cases II, Dynamical System Physical systems, time span
Year: 2015
DOI identifier: 10.1371/journal.pone.0131226.g008
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Provided by: FigShare
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