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Meet the professor

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Station density stays the same ... let station density grow, keeping ... where the sum is over Fourier frequencies, avoiding 0, and f is the spectral density ... – PowerPoint PPT presentation

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Title: Meet the professor


1
Meet the professor
  • Friday, January 23 at SFU
  • 430 Beer and snacks reception

2
Spatial Covariance
NRCSE
3
Valid covariance functions
  • Bochners theorem The class of covariance
    functions is the class of positive definite
    functions C
  • Why?

4
Spectral representation
  • By the spectral representation any isotropic
    continuous correlation on Rd is of the form
  • By isotropy, the expectation depends only on the
    distribution G of .
  • Let Y be uniform on the unit sphere. Then


5
Isotropic correlation
  • Jv(u) is a Bessel function of the first kind and
    order v.
  • Hence
  • and in the case d2
  • (Hankel transform)

6
The Bessel function J0
0.403
7
The exponential correlation
  • A commonly used correlation function is ?(v)
    ev/?. Corresponds to a Gaussian process with
    continuous but not differentiable sample paths.
  • More generally, ?(v) c(v0) (1-c)ev/? has a
    nugget c, corresponding to measurement error and
    spatial correlation at small distances.
  • All isotropic correlations are a mixture of a
    nugget and a continuous isotropic correlation.

8
The squared exponential
  • Using yields
  • corresponding to an underlying Gaussian field
    with analytic paths.
  • This is sometimes called the Gaussian covariance,
    for no really good reason.
  • A generalization is the power(ed) exponential
    correlation function,

9
The spherical
  • Corresponding variogram

nugget
sill
range
10
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11
The Matérn class
  • where is a modified Bessel function of
    the third kind and order ?. It corresponds to a
    spatial field with ?1 continuous derivatives
  • ?1/2 is exponential
  • ?1 is Whittles spatial correlation
  • yields squared exponential.

12
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13
Some other covariance/variogram families
Name Covariance Variogram
Wave
Rational quadratic
Linear None
Power law None
14
Estimation of variograms
  • Recall
  • Method of moments square of all pairwise
    differences, smoothed over lag bins
  • Problems Not necessarily a valid variogram
  • Not very robust

15
A robust empirical variogram estimator
  • (Z(x)-Z(y))2 is chi-squared for Gaussian data
  • Fourth root is variance stabilizing
  • Cressie and Hawkins

16
Least squares
  • Minimize
  • Alternatives
  • fourth root transformation
  • weighting by 1/?2
  • generalized least squares

17
Maximum likelihood
  • ZNn(?,?) ? ??(si-sj?) ? V(?)
  • Maximize
  • and q maximizes the profile likelihood

18
A peculiar ml fit
19
Some more fits
20
All together now...
21
Asymptotics
  • Increasing domain asymptotics let region of
    interest grow. Station density stays the same
  • Bad estimation at short distances, but
    effectively independent blocks far apart
  • Infill asymptotics let station density grow,
    keeping region fixed.
  • Good estimates at short distances. No effectively
    independent blocks, so technically trickier

22
Steins result
  • Covariance functions C0 and C1 are compatible if
    their Gaussian measures are mutually absolutely
    continuous. Sample at si, i1,...,n, predict at
    s (limit point of sampling points). Let ei(n) be
    kriging prediction error at s for Ci, and V0 the
    variance under C0 of some random variable.
  • If limnV0(e0(n))0, then

23
The Fourier transform
24
Properties of Fourier transforms
  • Convolution
  • Scaling
  • Translation

25
Parcevals theorem
  • Relates space integration to frequency
    integration. Decomposes variability.

26
Aliasing
  • Observe field at lattice of spacing ?.
    Since
  • the frequencies ? and ??2?m/??are aliases of
    each other, and indistinguishable.
  • The highest distinguishable frequency is ???, the
    Nyquist frequency.

27
Illustration of aliasing
  • Aliasing applet

28
Spectral representation
  • Stationary processes
  • Spectral process Y has stationary increments
  • If F has a density f, it is called the spectral
    density.

29
Estimating the spectrum
  • For process observed on nxn grid, estimate
    spectrum by periodogram
  • Equivalent to DFT of sample covariance

30
Properties of the periodogram
  • Periodogram values at Fourier frequencies
    (j,k)????are
  • uncorrelated
  • asymptotically unbiased
  • not consistent
  • To get a consistent estimate of the spectrum,
    smooth over nearby frequencies

31
Some common isotropic spectra
  • Squared exponential
  • Matérn

32
A simulated process
33
Thetford canopy heights
  • 39-year thinned commercial plantation of Scots
    pine in Thetford Forest, UK
  • Density 1000 trees/ha
  • 36m x 120m area surveyed for crown height
  • Focus on 32 x 32 subset

34
Spectrum of canopy heights
35
Whittle likelihood
  • Approximation to Gaussian likelihood using
    periodogram
  • where the sum is over Fourier frequencies,
    avoiding 0, and f is the spectral density
  • Takes O(N logN) operations to calculate
  • instead of O(N3).

36
Using non-gridded data
  • Consider
  • where
  • Then Y is stationary with spectral density
  • Viewing Y as a lattice process, it has spectral
    density

37
Estimation
  • Let
  • where Jx is the grid square with center x and nx
    is the number of sites in the square. Define the
    tapered periodogram
  • where . The Whittle
    likelihood is approximately

38
A simulated example
39
Estimated variogram
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