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The Fourier transform
g:Rd → R
G(ω) =F (g) = g(s)exp(iωTs)ds∫
g(s) =F −1(G) =
12π( )
d exp(-iωTs)G(ω)dω∫
Properties of Fourier transforms
Convolution
Scaling
Translation
F (f ∗g) =F (f)F (g)
F (f(ag)) =
1a
F(ω / a)
F (f(g−b)) =exp(ib)F (f)
Parceval’s theorem
Relates space integration to frequency integration. Decomposes variability.
f(s)2ds∫ = F(ω) 2dω∫
Aliasing
Observe field at lattice of spacing . Since
the frequencies ω and ω’=ω+2πm/are aliases of each other, and indistinguishable.
The highest distinguishable frequency is π, the Nyquist frequency.
Zd
exp(iωTk)=exp(i ωT +2πmT
⎛
⎝⎜⎞
⎠⎟k)
=exp(iωTk)exp(i2πmTk)
Illustration of aliasing
Aliasing applet
Spectral representation
Stationary processes
Spectral process Y has stationary increments
If F has a density f, it is called the spectral density.
Z(s) = exp(isTω)dY(ω)Rd∫
E dY(ω) 2 =dF(ω)
Cov(Z(s1),Z(s2 )) = e i(s1-s2 )Tωf(ω)dωR2∫
Estimating the spectrum
For process observed on nxn grid, estimate spectrum by periodogram
Equivalent to DFT of sample covariance
In,n (ω) =1
(2πn)2 z(j)eiωTj
j∈J∑
2
ω =2πj
n; J = (n − 1) / 2⎢⎣ ⎥⎦,...,n − (n − 1) / 2⎢⎣ ⎥⎦{ }
2
Properties of the periodogram
Periodogram values at Fourier frequencies (j,k)πare
•uncorrelated
•asymptotically unbiased
•not consistent
To get a consistent estimate of the spectrum, smooth over nearby frequencies
Some common isotropic spectra
Squared exponential
Matérn
f(ω)=σ2
2παexp(− ω 2 / 4α)
C(r) =σ2 exp(−α r2 )
f(ω) =φ(α2 + ω 2 )−ν−1
C(r) =πφ(α r )ν K ν (α r )
2 ν−1Γ(ν + 1)α2 ν
A simulated process
Z(s) = gjk cos 2πjs1
m+
ks2
n⎡⎣⎢
⎤⎦⎥
+ Ujk
⎛⎝⎜
⎞⎠⎟k=−15
15
∑j=0
15
∑
gjk =exp(− j + 6 −ktan(20°) )
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
Spectrum of canopy heights
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).
l (θ) = logf(ω; θ) +
IN,N(ω)f(ω; θ)
⎧⎨⎩
⎫⎬⎭ω
∑
Using non-gridded data
Consider
where
Then Y is stationary with spectral density
Viewing Y as a lattice process, it has spectral density
Y(x) =−2 h(x −s)∫ Z(s)ds
h(x) =1( xi ≤ / 2, i =1,2)
fY (ω) =1
2 H(ω) 2fZ(ω)
f,Y (ω) = H(ω +2πq
)
2
fZq∈Z2∑ (ω +
2πq
)
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
Yn2 (x) =
1nx
h(s i −x)Z(s i )i∈J x
∑
Ig1Yn2(ω) =
1g1
2 (x)∑g1(x)Y
n2 (x)e−ixTω∑2
g1(x) =nx / n
LY
=n2
2π( )2 logf,Y (2πj / n) +
Ig1,Yn2
(2πj / n)
f,Y (2πj / n)
⎧⎨⎪
⎩⎪
⎫⎬⎪
⎭⎪j∑
A simulated example
Estimated variogram
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Evidence of anisotropy15o red60o green105o blue150o brown
Another view of anisotropy
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σe2 = 127.1(259)
σs2 = 68.8 (255)
θ = 10.7 (45)
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σe2 = 154.6 (134)
σs2 = 141.0 (127)
θ = 29.5 (35)
Geometric anisotropy
Recall that if we have an isotropic covariance (circular isocorrelation curves).
If for a linear transformation A, we have geometric anisotropy (elliptical isocorrelation curves).
General nonstationary correlation structures are typically locally geometrically anisotropic.
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C(x,y) = C( x − y )
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C(x,y) = C( Ax − Ay )
QuickTime™ and aTIFF (Uncompressed) decompressor
are needed to see this picture.
Lindgren & Rychlik transformation
′x = (2x + y + 109.15) / 2
′y = 4(−x + 2y − 154.5) / 3