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Nonstationary covariance structures II NRCSE
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Drawbacks with deformation approach Oversmoothing of large areas Local deformations not local part of global fits Covariance shape does not change over space Limited class of nonstationary covariances
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Nonstationary spatial covariance: Basic idea: the parameters of a local variogram model–-nugget, range, sill, and anisotropy–vary spatially. Consider some pictures of applications from recent methodology publications.
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Major approaches: Haas, 1990, Moving window kriging Kim, Mallock & Holmes, 2005, Piecewise Gaussian modeling Nott & Dunsmuir, 2002, Biometrika, Average of locally stationary processes Fuentes, 2002, Kernel averaging of orthogonal, locally stationary processes. Pintore & Holmes, 2005, Fourier and Karhunen-Loeve expansions Higdon & Swall, 1998, 2000, Gaussian moving averages or “process convolution” model Nychka, Wikle & Royle, 2002. Wavelet expansion.
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Kim, Mallock & Holmes, JASA 2005 Piecewise Gaussian model for groundwater permeability data
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Fig. 2. Sydney wind pattern data. Contours of equal estimated correlation with two different fixed sites, shown by open squares: (a) location 33·85°S, 151·22°E, and (b) location 33·74°S, 149·88°E. The sites marked by dots show locations of the 45 monitored sites. Nott & Dunsmuire, 2002, Biometrika.
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Pintore & Holmes: Spatially adaptive non-stationary covariance functions via spatially adaptive spectra
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Thetford revisited Features depend on spatial location
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Kernel averaging Fuentes (2000): Introduce uncorrelated stationary processes Z k (s), k=1,...,K, defined on disjoint subregions S k and construct where w k (s) is a weight function related to dist(s,S k ). Then
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Spectral version so where Hence
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Estimating spectrum Asymptotically
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Details K = 9; h = 687 km Mixture of Matérn spectra
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An example Models-3 output, 81x87 grid, 36km x 36km. Hourly averaged nitric acid concentration week of 950711.
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Models-3 fit
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A spectral approach to nonstationary processes Spectral representation: s slowly varying square integrable, Y uncorrelated increments Hence is the space- varying spectral density Observe at grid; use FFT to estimate in nbd of s
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Testing for nonstationarity U(s,w) = log has approximately mean f(s, ) = log f s ( ) and constant variance in s and . Taking s 1,...,s n and 1,..., m sufficently well separated, we have approximately U ij = U(s i, j ) = f ij + ij with the ij iid. We can test for interaction between location and frequency (nonstationarity) using ANOVA.
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Details The general model has The hypothesis of no interaction ( ij =0) corresponds to additivity on log scale: (uniformly modulated process: Z 0 stationary) Stationarity corresponds to Tests based on approx 2 -distribution (known variance)
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Models-3 revisited Sourcedfsum of squares 22 Between spatial points 826.55663.75 Between frequencies 8366.849171 Interaction6430.54763.5 Total80423.9310598.25
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Moving averages A simple way of constructing stationary sequences is to average an iid sequence. A continuous time counterpart is, where is a random measure which is stationary and assigns independent random variables to disjoint sets, i.e., has stationary and independent increments.
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Lévy-Khinchine is the Lévy measure, and t is the Lévy process. We can construct it from a Poisson measure H(du,ds) on R 2 with intensity E(H(du,ds))= (du)ds and a standard Brownian motion B t as
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Examples Brownian motion with drift: t ~N( t, 2 t) (du)=0. Poisson process: t ~Po( t) = 2 =0, (du)= {1} (du) Gamma process: t ~ ( t, ) = 2 =0, (du)= e - u 1(u>0)du/u Cauchy process: = 2 =0, (du)= u -2 du/
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Spatial moving averages We can replace R for t with R 2 (or a general metric space) We can replace R for s with R 2 (or a general metric space) We can replace b(t-s) by b t (s) to relax stationarity We can let the intensity measure for H be an arbitrary measure (ds,du)
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Gaussian moving averages Higdon (1998), Swall (2000): Let be a Brownian motion without drift, and. This is a Gaussian process with correlation Account for nonstationarity by letting the kernel b vary with location:
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Details yields an explicit covariance function which is squared exponential with parameter changing with spatial location. The prior distribution describes “local ellipses,” i.e., smoothly changing random kernels.
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Local ellipses Foci
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Prior parametrization Foci chosen independently Gaussian with isotropic squared exponential covariance Another parameter describes the range of influence of a given ellipse. Prior gamma.
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Example Piazza Road Superfund cleanup. Dioxin applied to road seeped into groundwater.
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Posterior distribution
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