Wavelet Spectral Analysis Ken Nowak 7 December 2010.

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Presentation transcript:

Wavelet Spectral Analysis Ken Nowak 7 December 2010

Need for spectral analysis Many geo-physical data have quasi- periodic tendencies or underlying variability Spectral methods aid in detection and attribution of signals in data

Fourier Approach Limitations Results are limited to global Scales are at specific, discrete intervals –Per fourier theory, transformations at each scale are orthogonal

Wavelet Basics W f ( a,b)= f(x)  ( a,b) (x) dx  Morlet wavelet with a=0.5 Function to analyze Integrand of wavelet transform |W(a=0.5,b=6.5)| 2 =0 |W(a=0.5,b=14.1)| 2 =.44 b=2b=6.5b=14.1 graphics courtesy of Matt Dillin ∫ Wavelets detect non-stationary spectral components

Wavelet Basics Here we explore the Continuous Wavelet Transform (CWT) –No longer restricted to discrete scales –Ability to see “local” features Mexican hat wavelet Morlet wavelet

Global Wavelet Spectrum |W f ( a,b)| 2 function Wavelet spectrum a =2 a =1/2 Global wavelet spectrum Slide courtesy of Matt Dillin

Wavelet Details Convolutions between wavelet and data can be computed simultaneously via convolution theorem. Wavelet transform Wavelet function All convolutions at scale “a”

Analysis of Lee’s Ferry Data Local and global wavelet spectra Cone of influence Significance levels

Analysis of ENSO Data Characteristic ENSO timescale Global peak

Significance Levels Background Fourier spectrum for red noise process (normalized) Square of normal distribution is chi-square distribution, thus the 95% confidence level is given by: Where the 95 th percentile of a chi-square distribution is normalized by the degrees of freedom.

Scale-Averaged Wavelet Power SAWP creates a time series that reflects variability strength over time for a single or band of scales

Band Reconstructions We can also reconstruct all or part of the original data

PACF indicates AR-1 model Statistics capture observed values adequately Spectral range does not reflect observed spectrum Lee’s Ferry Flow Simulation

Wavelet Auto Regressive Method (WARM) Kwon et al., 2007

WARM and Non-stationary Spectra Power is smoothed across time domain instead of being concentrated in recent decades

WARM for Non-stationary Spectra

Results for Improved WARM

Wavelet Phase and Coherence Analysis of relationship between two data sets at range of scales and through time Correlation =.06

Wavelet Phase and Coherence

Cross Wavelet Transform For some data X and some data Y, wavelet transforms are given as: Thus the cross wavelet transform is defined as:

Phase Angle Cross wavelet transform (XWT) is complex. Phase angle between data X and data Y is simply the angle between the real and imaginary components of the XWT:

Coherence and Correlation Correlation of X and Y is given as: Which is similar to the coherence equation:

Summary Wavelets offer frequency-time localization of spectral power SAWP visualizes how power changes for a given scale or band as a time series “Band pass” reconstructions can be performed from the wavelet transform WARM is an attractive simulation method that captures spectral features

Summary Cross wavelet transform can offer phase and coherence between data sets Additional Resources: