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Computational Geophysics and Data Analysis1

Correlations

Correlations

Correlation of time series Similarity Time shitfs

Applications Correlation of rotations/strains and translations Ambient noise correlations Coda correlations Random media: correlation length

Scope: Appreciate that the use of noise (and coda) plus correlation techniques is one of the most innovative direction in data analysis at the moment: passive imaging

Computational Geophysics and Data Analysis2

Correlations

Discrete Correlation

Correlation plays a central role in the study of time series. In general, correlation gives a quantitative estimate of the degree of similarity between two functions.

The correlation of functions g and f both with N samples is defined as:

Correlation plays a central role in the study of time series. In general, correlation gives a quantitative estimate of the degree of similarity between two functions.

The correlation of functions g and f both with N samples is defined as:

1,,2,1,0

1 1

0

Nk

fgN

rkN

iikik

Computational Geophysics and Data Analysis3

Correlations

Auto-correlation

Auto-correlation

Computational Geophysics and Data Analysis4

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Cross-correlation

Lag between two functions

Cross-correlation

Computational Geophysics and Data Analysis5

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Cross-correlation: Random functions

Computational Geophysics and Data Analysis6

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Auto-correlation: Random functions

Computational Geophysics and Data Analysis7

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Auto-correlation: Seismic signal

Computational Geophysics and Data Analysis8

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Theoretical relation rotation rate and transverse acceleration

plane-wave propagation

Plane transversely polarized wave propagating in x-direction with phase velocity c Plane transversely polarized wave propagating in x-direction with phase velocity c

kctkxftxu y /)(),( kctkxftxu y /)(),(

)(),(),( 2 tkxftxutxa yy )(),(),( 2 tkxftxutxa yy Acceleration

ctxtxa 2),(/),( ctxtxa 2),(/),(

Rotation rate and acceleration should be in phase and the amplitudes scaled by two times the horizontal phase velocity

Rotation rate and acceleration should be in phase and the amplitudes scaled by two times the horizontal phase velocity

Rotation rate

)(

2

1,0,00,,0

2

1),( tkxfkutx y

)(

2

1,0,00,,0

2

1),( tkxfkutx y

Computational Geophysics and Data Analysis9

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Mw = 8.3 Tokachi-oki 25.09.2003transverse acceleration – rotation rate

From Igel et al., GRL, 2005

Computational Geophysics and Data Analysis10

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Max. cross-corr. coefficient in sliding time window transverse acceleration – rotation rate

Small tele-seismic event

P-onset

S-waveLove waves Aftershock

Computational Geophysics and Data Analysis11

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M8.3 Tokachi-oki, 25 September 2003phase velocities ( + observations, o theory)

From Igel et al. (GRL, 2005)

Horizontal phase velocity in sliding time window

Computational Geophysics and Data Analysis12

Correlations

Sumatra M8.3 12.9.2007

P

P Coda

Computational Geophysics and Data Analysis13

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… CC as a function of time …observable for all events!

Computational Geophysics and Data Analysis14

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Rotational signals in the P-coda?azimuth dependence

Computational Geophysics and Data Analysis15

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P-Coda energy direction… comes from all directions …

correlations in P-coda window

Computational Geophysics and Data Analysis16

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Noise correlation - principle

From Campillo et al.

Computational Geophysics and Data Analysis17

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Uneven noise distribution

Computational Geophysics and Data Analysis18

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Surface waves and noise

Cross-correlate noise observed over long

time scales at different locations

Vary frequency range, dispersion?

Computational Geophysics and Data Analysis19

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Surface wave dispersion

Computational Geophysics and Data Analysis20

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US Array stations

Computational Geophysics and Data Analysis21

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Recovery of Green‘s function

Computational Geophysics and Data Analysis22

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Disersion curves

All from Shapiro et al., 2004

Computational Geophysics and Data Analysis23

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Tomography without earthquakes!

Computational Geophysics and Data Analysis24

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Global scale!

Nishida et al., Nature, 2009.

Computational Geophysics and Data Analysis25

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Correlations and the coda

Computational Geophysics and Data Analysis26

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Velocity changes by CC

Computational Geophysics and Data Analysis27

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Remote triggering (from CCs)

Taka’aki Taira, Paul G. Silver, Fenglin Niu & Robert M. Nadeau:

Remote triggering of fault-strength changes on the San Andreas fault at Parkfield

Nature 461, 636-639 (1 October 2009) | doi:10.1038/nature08395; Received 25 April 2009; Accepted 6 August 2009

Computational Geophysics and Data Analysis28

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Remote triggering of fault-strength changes on the San Andreas fault at Parkfield

Taka’aki Taira, Paul G. Silver, Fenglin Niu & Robert M. Nadeau

Key message:• Connection between

significant changes in scattering parameters and fault strength and dynamic stress

Seismic network

Computational Geophysics and Data Analysis29

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Principle

Method:• Compare waveforms of

repeating earthquake sequences

• Quantity: Decorrelation index D(t) = 1-Cmax(t)

• Insensitive to variations in near-station environment(Snieder, Gret, Douma & Scales 2002)

Computational Geophysics and Data Analysis31

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Changes in scatterer properties:•Increase in Decorrelation index after 1992 Landers earthquake (Mw=7.3, 65 kPa dyn. stress)

•Strong increase in Decorrelation index after 2004 Parkfield earthquake (Mw=6.0, distance ~20 km)

•Increase in Decorrelation index after 2004 Sumatra Earthquake (Mw=9.1, 10kPa dyn. stress)

•But: No traces of 1999 Hector Mine, 2002 Denali and 2003 San Simeon (dyn. stresses all two times above 2004 Sumatra)

True?

Computational Geophysics and Data Analysis32

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Correlations and random media:

Generation of random media:

Define spectrum Random Phase Back transform usig

inverse FFT

Computational Geophysics and Data Analysis33

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Random media:

Computational Geophysics and Data Analysis34

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P-SH scattering simulations with ADER-DG

translations

rotations

Computational Geophysics and Data Analysis35

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P-SH scatteringsimulations with ADER-DG

Computational Geophysics and Data Analysis36

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Random mantle models

Computational Geophysics and Data Analysis37

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Random models

Computational Geophysics and Data Analysis38

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Convergence to the right spectrum

Computational Geophysics and Data Analysis39

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Mantle models

Computational Geophysics and Data Analysis40

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Waves through random models

Computational Geophysics and Data Analysis41

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Summary

The simple correlation technique has turned into one of the most important processing tools for seismograms

Passive imaging is the process with which noise recordings can be used to infer information on structure

Correlation of noisy seismograms from two stations allows in principle the reconstruction of the Green‘s function between the two stations

A whole new family of tomographic tools emerged CC techniques are ideal to identify time-dependent changes in the

structure (scattering) The ideal tool to quantify similarity (e.g., frequency dependent)

between various signals (e.g., rotations, strains with translations)

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