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State Space Approach to Signal Extraction Problems in Seismology Genshiro Kitagawa The Institute of Statistical Mathematics IMA, Minneapolis Nov. 15, 2001 Collaborators: Will Gersch (Univ. Hawaii) Tetsuo Takanami (Univ. Hokkaido) Norio Matsumoto (Geological Survey of Japan)
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Roles of Statistical Models Data Information Model as a “tool” for extracting information Modeling based on the characteristics of the object and the objective of the analysis. Unify information supplied by data and prior knowledge. Bayes models, state space models etc.
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Outline Method –Flexible Statistical Modeling –State Space Modeling Applications –Extraction of Signal from Noisy Data –Automatic Data Cleaning –Detection of Coseismic Effect in Groundwater Level –Analysis of OBS (Ocean Bottom Seismograph) Data JASA(1996) + ISR(2001) + some new
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Change of Statistical Problems Flexible Modeling Smoothness priors Automatic Procedures Huge Observations, Complex Systems Small Experimental, Survey Data Parametric Models + AIC
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Smoothness Prior Simple Smoothing Problem Observation Unknown Parameter Noise Penalized Least Squares Whittaker (1923), Shiller (1973), Akaike(1980), Kitagawa-Gersch(1996) Infidelity to the data Infidelity to smoothness
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Automatic Parameter Determination via Bayesian Interpretation Bayesian Interpretation Multiply by and exponentiate Determination of by ABIC (Akaike 1980) Crucial parameter Smoothness Prior
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Time Series Interpretation and State Space Modeling State Space Model Equivalent Model
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Applications of State Space Model Modeling Nonstationarity in mean Trend Estimation, Seasonal Adjustment in variance Time-Varying Variance Models, Volatility in covariance Time-Varying Coefficient Models, TVAR model Signal Extraction, Decomposition
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State Space Models Nonlinear Non-Gaussian General Linear Gaussian Nonlinear Non-Gaussian Discrete state Discrete obs.
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Kalman Filter Prediction Filter Smoothing Initial Prediction Filter
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Non-Gaussian Filter/Smoother Prediction Filter Smoother
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Recursive Filter/Smoother for State Estimation 0. Gaussian Approximation Kalman filter/smoother 1. Piecewise-linear or Step Approx. Non-Gaussian filter/smoother 2. Gaussian Mixture Approx. Gaussian-sum filter/smoother 3. Monte Carlo Based Method Sequential Monte Carlo filter/smoother True Normal approx. Piecewise Linear Step function Normal mixture Monte Carlo approx.
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Sequential Monte Carlo Filter System Noise Importance Weight (Bayes factor) Predictive Distribution Filter Distribution Resampling Gordon et al. (1993), Kitagawa (1996) Doucet, de Freitas and Gordon (2001) “Sequential Monte Carlo Methods in Practice”
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Self-Tuned State Space Model Augmented State Vector Non-Gaussian or Monte Carlo Smoother Simultaneous Estimation of State and Parameter Time-varying parameter
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Tools for Time Series Modeling Model Representaion – Generic: State Space Models – Specific: Smoothness Priors Estimation – State: Sequential Filters – Parameter: MLE, Bayes, SOSS Evaluation – AIC
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Examples 1. Detection of Micro Earthquakes 2. Extraction of Coseismic Effects 3. Analysis of OBS (Ocean Bottom Seismograph) Data
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Extraction of Signal From Noisy Data Basic Model Component Models Observed
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State Space Model
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Extraction of Micro Earthquake Observed Seismic Signal Background Noise 0 400 800 1200 1600 2000 2400 2800 15 0 -15 15 0 -15 15 0 -15 4 2 0 -2 -4 -6 Time-varying Variance (in log 10 )
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Extraction of Micro Earthquake Background Noise Earthquake Signal Observed
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Extraction of Earthquake Signal Observed S-wave P-wave Background Noise
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3D-Modeling P-wave S-wave E-W N-S U-D P-wave E-W N-S U-D S-wave
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Detection of Coseismic Effects Observation Well Geological Survey of Japan Precipitation Groundwater Level Air Pressure Earth Tide dT = 2min., 20years Japan Tokai Area 5M observations
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Detection of Coseismic Effect in Groundwater Level Difficulties Presence of many missing and outlying observations Outlier Missing Strongly affected by barometric air pressure, earth tide and rain
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Automatic Data Cleaning State Space Model Observation Noise Model
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Model for Outliers -5 -4 -3 -2 -1 0 1 2 3 4 5 Mixture -5 -4 -3 -2 -1 0 1 2 3 4 5
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Missing and Outlying Observations Gaussian Mixture OriginalCleaned
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Detection of Coseismic Effects 1981 1982 19831984 19851986 19871988 1989 1990 Strongly affected the covariates such as barometric air pressure, earth tide and rain Difficult to find out Coseismic Effect
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Pressure Effect Air Pressure Pressure Effect
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Extraction of Coseismic Effect Component Models Observation Trend Air Pressure Effect Earth Tide Effect Observation Noise
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State Space Representation
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AIC Values
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Precipitation Effect Original Pressure, Earth-Tide removed
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Extraction of Coseismic Effect Component Models Observation Trend Air Pressure Effect Earth Tide Effect Precipitation Effect Observation Noise
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State Space Model
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Groundwater Level Air Pressure Effect Earth Tide Effect Precipitation Effect min AIC model m=25, l=2, k=5 M=4.8, D=48km Extraction of Coseismic Effects Corrected Water Level
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Detected Coseismic Effect Original T+P+ET+R M=4.8 D=48km M=6.8 D=128km M=7.0 D=375km M=5.7 D=66km M=7.7 D=622km M=6.0 D=113km M=6.2 D=150km M=5.0 D=57km M=7.9 D=742km T+P+ET Signal
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Min AIC model m=25, l=2, k=5 Original Air Pressure Effect Earth Tide Effect P & ET Removed Precipitation Effect P , ET & R Removed
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Coseismic Effect 19811982 19831984 19851986 19871988 19891990 M=7.0 D=375km M=4.8 D=48km M=5.7 D=66km M=7.7 D=622km M=6.0 D=113km M=6.2 D=150km M=5.0 D=57km M=7.9 D=742km M=6.8 D=128km M=6.0 D=126km M=6.7 D=226km M=5.7 D=122km M=6.5 D=96km 1981 1982 19831984 19851986 19871988 1989 1990
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Effect of Earthquake Earthquake Water level Rain Water level Distance MagnitudeCoseismic Effect > 16cm > 4cm > 1cm
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Findings Drop of level Detected for earthquakes with M > 2.62 log D + 0.2 Amount of drop ~ f( M 2.62 log D ) Without coseismic effect water level increases 6cm/year increase of stress in this area?
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Exploring Underground Structure by OBS (Ocean Bottom Seismogram) Data Bottom OBS Sea Surface
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Observations by an Experiment Off Norway ( Depth 1500-2000m ) 39 OBS, (Distance: about 10km ) Air-gun Signal from a Ship ( 982 times: Interval 70sec., 200m ) Observation ( dT=1/256sec., T =60sec., 4- Ch ) 4 Channel Time Series N=15360, 982 39 series Hokkaido University + University of Bergen
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Time-Adjusted (Shifted) Time Series
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An Example of the Observations OBS-4 N=7500 M=1560 OBS-31 N=15360 M=982 High S/N Low S/N
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Direct wave, Reflection, Refraction Direct Wave Refraction Wave Reflection Wave
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Objectives Estimation of Underground Structure Detection of Reflection & Refraction Waves Estimation of parameters ( h j, v j ) Intermediate objectives
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Time series at hypocenter (D=0) Wave(0)Wave(000)Wave(00000) Wave(011)Wave(00011)
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Model for Decomposition Self-Organizing Model
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Decomposition of Ch-701 (D=4km) Observed
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Decomposition of Ch-721 (D=8km) Observed
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A Small Portion of Data
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“Spatial” Filter/Smoother k: Time-lag
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Spatial Model (Ignoring time series structure) Series j-1 Series j : Time-lag=k
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Local Cross-Correlation Function Time Location 08 730 630
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Spatial-Temporal Model
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Model of Propagation Path Parallel Structure Width Velocity Water
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Examples of Wave Path Wave(0)Wave(000)Wave(01) Wave(011)Wave(0121)Wave(000121) Wave(01221)Wave(012321)Wave(00012321)
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Path Models and Arrival Times
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Path models and arrival times(OBS4) Distance (km) Arrival Time (sec.)
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Local Time Lag -10 -8 -6 -4 -2 0 2 4 6 8 10 D: Distance (km) 876543210876543210 Arrival Time (sec.)
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Path Models and the Differences of the Arrival Times Between Adjacent Channels Epicentral Distance
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Model for Decomposition
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Spatial-Temporal Model Time-lag (Channel j-1 Channel j ) = k
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Spatial-Temporal Filtering
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Spatial-Temporal Decomposition Reflection waveDirect wave
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Mt. Usu Eruption Data Hokkaido, Japan March 31, 2000 13:07-
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Volatility and component models Hokkaido, Japan March 31, 2000 13:07-
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Decomposition
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Summary Signal extraction and knowledge discovery by statistical modeling Use of information from data and Prior knowledge State Space Modeling Filtering/smoothing & SOSS New findings, Automatic procedure
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Time-varying Spectrum AR model Autocovariance Spectrum Time-varying Nonstationary Time-varying AR model Time-varying spectrum
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Estimation of Nonstationary AR Model State Space Representation Model for Time-changes of Coefficients Kronecker product
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State Space Representation For k = 1 For k = 2 Kronecker Product
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State Space Representation Case: k = 1
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Time-varying Coefficients Gauss model Cauchy model
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Time-varying Spectrum
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Precipitation Effect
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Estimation of Arrival Time PS Estimation of Arrival Times Estimation of Hypocenter Locally Stationary AR Model Automatic Modeling by Information Criterion AIC Automatic & Fast Algorithm Prediction of Tsunami
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Estimation of Arrival Time Locally Stationary AR Model Seismic Signal Model Background Noise Seismic Signal Background Noise Model
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Estimation of Arrival Time AIC of the Total Models Min AIC Estimate of Arrival Time
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Model & Implementations LSAR model: Ozaki and Tong (1976) Householder implementation: Kitagawa and Akaike (1979) Kalman filter implementation:
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State Space Representation of AR Model New data y n
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Lower Order Models Levinson recursion
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Arrival Times of P-waves AIC 2000
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Arrival Times of S-waves AIC 100
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Posterior Probabilities of Arrival Times AIC: - 2(Bias corrected log-likelihood) Likelihood of the arrival time Posterior probability of the arrival time
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