Investigating Higher Order Statistics and Gaussianity Steve Penn, Syracuse University LIGO-G010132-00-Z Synopsis Introduction to Higher Order Statistics » 1D: Correlation, Coherence, Power Spectra » 2D: Bicorrelation, Bicoherence, Bispectrum » 3D… Bispectrum diagnostic Gaussianity Test Linearity Test LSC • March 2001 Syracuse University Experimental Relativity Group 2 What are Higher Order Statistics? 1D Statistics: » Correlation: Cxy t x yt d X f Y f Sxy f * » Power Spectral Density: C2 x t » Coherence: C xy f X f X f S2x f * Sxy f S2 x f S2 y f – Tells us power and phase coherence at a given frequency LSC • March 2001 Syracuse University Experimental Relativity Group 3 Second Order Statistics 2D Statistics: » Cumulant: Cxyz t, t x yt z t d X f1 Y f2 Z f1 f2 Sxyz f1 , f2 * » Bispectral Density: C3x t X f1 X f2 X f1 f2 S3x f1 , f2 * » Bicoherence: C xyz f Sxyz f1 , f2 S2 x f1 S2y f2 S2z f1 , f2 – Tells us power and phase coherence at a coupled frequency LSC • March 2001 Syracuse University Experimental Relativity Group 4 Zero-lag Cumulants Mean Cx 0 Variance C2 x 0 Skewness C3x 0 0 if Symmetric Kurtosis C4 x 0 0 if Gaussian Useful statictical values, but… Skewness = 0 does not prove symmetry Kurtosis = 0 does not prove Gaussianity Variations in skew and kurtosis not well quantified. LSC • March 2001 Syracuse University Experimental Relativity Group 5 Why Higher Order Statistics? For a Gaussian process:Cnx t 0, for n 2 For independent processes: z t x t yt , Cnz t Cnx t Cny t Cny t n2 Allows for separation of Gaussian process for n>2 » Visual check of frequency coupling and phase noise » Statistical test for the probability of gaussianity and linearity » Iterative process to reconstruct nongaussian signal from the higher order cumulants LSC • March 2001 Syracuse University Experimental Relativity Group 6 Gaussianity Monitor Diagnostic Plot: » Time series, Power spectrum, Two perspectives of the histogram of time series with gaussian fit Bispectrum and Bicoherence Plot Gaussianity test: C 3x f1 , f2 dU 2D Summary file: 2 » Frame, channel, mean, variance, skew, kurtosis, gaussianity probability LSC • March 2001 Syracuse University Experimental Relativity Group 7 Bispectrum Unique Area fN f2=2fN-f1 0 LSC • March 2001 f1=f2 fN Syracuse University Experimental Relativity Group 8 LSC • March 2001 Syracuse University Experimental Relativity Group 9 LSC • March 2001 Syracuse University Experimental Relativity Group 10 LSC • March 2001 Syracuse University Experimental Relativity Group 11 Status and Conclusions Using the HOSA package in Matlab was not practical. We needed a monitor running in DMT. Old Bispectral algorithm extremely slow (100*realtime) New algorithm using FFTW appears to be near realtime Now we can analyze some data!! Upcoming additions: » Better windowing » User selectable time interval Record user selectedRelativity s limit Group LSC •»March 2001 # events Syracuseabove University Experimental » Plot/Set reference distribution for each channel. 12 LSC • March 2001 Syracuse University Experimental Relativity Group 13
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