Climate data: Long range dependent or nonstationary?

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Climate data: Long range dependent or
nonstationary?
Dependence, Stability, and Extremes Workshop
The Fields Institute
Toronto, Ontario, Canada
6 May 2016
Mark M. Meerschaert
Department of Statistics and Probability
Michigan State University
mcubed@stt.msu.edu
http://www.stt.msu.edu/users/mcubed
Partially supported by NSF FRG grant DMS-1462156, NSF INSPIRE grant EAR-1344280,
and ARO MURI grant W911NF-15-1-0562.
Abstract
A North American Regional Climate Change Assessment Program (NARCCAP) climate model was used to generate 29 years
of daily maximum temperature data at around 16,000 spatial
locations in North America. Our ultimate goal is to develop accurate models for forecasting extreme weather conditions, e.g.,
heat waves. The goal of this talk is to develop a reasonable time
series model for the temperature data at any given spatial location. Future work will also consider the spatial pattern. Since
the data shows a strong seasonal variation, as well as long range
correlations, it is not clear a priori whether to apply a model with
long range dependence, or periodic stationarity, or both. It has
been observed, e.g., in financial time series, that nonstationarity
can mimic long range dependence. We will see that this is also
the case for climate data. Hence a periodically stationary time
series model may be indicated.
Acknowledgments
Paul L. Anderson, Maths and Computer Science, Albion College
Metin Eroglu, Statistics and Probability, Michigan State U
Joshua French, Math and Statistical Sci., U Colorado Denver
Piotr Kokoszka, Statistics, Colorado State University
Stilian Stoev, Statistics, University of Michigan
NARCCAP data set
Data is freely available at http://www.narccap.ucar.edu/ from the
North American Regional Climate Change Assessment Program
(NARCCAP) .
Data Source: Canadian Regional Climate Model (CRCM) +
Community Climate System Model (CCSM)
CRCM is a detailed local climate model from the Canadian Centre for Climate Modelling and Analysis.
CCSM is a global circulation climate model from the USA National Center for Atmospheric Research (NCAR) in Boulder CO.
A complete data set (no missing values) of maximum daily surface air temperature (◦K) on a 140×115 grid over much of North
America covers N = 29 years, 2041–2069.
NARCCAP data set
Xn(sk , tj ) = max temperature at location sk on day tj of year n
Xn(sk , tj ) − μ̂(sk , tj )
Standardize: Yn(sk , tj ) =
where
σ̂(sk , tj )
N
1 X n (s k , t j )
μ̂(sk , tj ) =
N n=1
σ̂(sk , tj )2 =
N 2
1
Xn(sk , tj ) − μ̂(sk , tj ) .
N − 1 n=1
Heat wave statistic:
Z ∗ (s k , t j ) =
⎡
min
k∈IK (k)
⎤
⎢1
⎣
t −<t ≤t
j
i j
⎥
Y n (s k , t j ) ⎦
K = 50 nearest neighbors, = 9 day moving average
Nearest neighbor map
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Heat wave map
Probability that Z ∗(sk , tj ) > 1 (mild heat wave)
70
z=1
60
0.8
50
40
0.4
30
0.2
20
latitude
0.6
200
220
240
260
280
300
320
Heat wave map
Probability that Z ∗(sk , tj ) > 2 (strong heat wave)
70
z=2
60
0.08
50
40
0.04
30
0.02
0.00
20
latitude
0.06
200
220
240
260
280
300
320
Long range dependence?
Autocorrelation at one site suggests LRD.
0.0
0.2
0.4
ACF
0.6
0.8
1.0
Series Y
0
10
20
Lag
30
40
Check spectral density
−2
−4
−6
−8
log(spec)
0
2
4
Power law spectral density also suggests LRD d = 0.9.
−8
−6
−4
log(freq)
−2
LRD and heavy tails
Hill estimator also indicates heavy tail with α ≈ 1.5.
+,//6+)7
DOSKD
U
3DJH
Question: Is Yn(sk , tj ) stationary?
Oscillation in the ACF suggests periodic behavior.
0.0
0.2
0.4
ACF
0.6
0.8
1.0
Series Y
0
100
200
Lag
300
400
Periodic ARMA model
One spatial location: X̃365 (n−1)+t = Xn(sk , t)
PARMAS (p, q) model:
Xt −
p
φt(j)Xt−j = εt +
j=1
q
θt(j)εt−j
j=1
Mean-centered data Xt = X̃t − μt
Standardized errors δt = σt−1εt assumed IID
Parameters φt(j), θt(j), σt all periodic with period S = 365.
R package perARMA is quite convenient
Periodic mean
290
285
280
275
270
seasonal mean
295
300
Plot suggests some seasonal variation. Is SARIMA enough?
0
100
200
t
300
Periodic standard deviation
7
6
5
4
3
seasonal standard deviation
8
SARIMA needs σt constant. Is standardizing enough?
0
100
200
t
300
Periodic autocorrelation function at lag 1
0.6
0.4
0.2
seasonal ACF at lag 1
0.8
Standardizing does not produce a stationary process.
0
100
200
t
300
Fit a periodic AR(1) via perARMA
Residuals indicate a good fit. Nonstationary data mimics LRD!
0.0
0.2
0.4
ACF
0.6
0.8
1.0
Series resid
0
10
20
30
40
Model residuals are approximately normal
PAR(1) residuals via perARMA close to a normal PDF.
)UHTXHQF\
3$5UHVLG
A cautionary tale
Temperature data exhibits a heavy tail with infinite mean α < 2
Standardized data exhibits LRD d = 0.9
Periodic ARMA model removes the heavy tail
Periodic ARMA model removes the LRD
Nonstationary data mimics LRD and heavy tail!
Smoothing the PARMA parameters
Discrete Fourier transform smooths PAR(1) coefficients φt(1)
ϭ͘Ϯ
ϭ
Ϭ͘ϴ
ƉŚŝ
Ϭ͘ϲ
ƉŚŝ^ŵŽŽƚŚ
Ϭ͘ϰ
Ϭ͘Ϯ
Ϭ
Ϭ
ϭϬϬ
ϮϬϬ
ϯϬϬ
Smoothing the seasonal standard deviation
Discrete Fourier transform smooths PAR(1) coefficients σt
ϲ
ϱ
ϰ
ƐŝŐŵĂ
ϯ
ƐŝŐŵĂ^ŵŽŽƚŚ
Ϯ
ϭ
Ϭ
Ϭ
ϭϬϬ
ϮϬϬ
ϯϬϬ
Residuals of the smoothed PAR(1) model
Smoothed model has only 4 parameters. Residuals still uncorrelated.
0.0
0.2
0.4
ACF
0.6
0.8
1.0
Series stdresid
0
10
20
Lag
30
40
Residuals of the smoothed PAR(1) model
Histogram of smoothed PAR(1) residuals fits a normal PDF reasonably well, but with a bit of negative skewness.
900
800
700
Frequency
600
500
400
300
200
100
0
-4.8
-3.6
-2.4
-1.2
0.0
perARMAresid
1.2
2.4
3.6
Test on three 10 × 10 grids
Try a PAR(p) model on three test grids. Find p = 1 is sufficient
in SW grid, p = 3 enough for North-Central and Eastern grids.
Check ACF for some randomly selected sites
Residual ACF plots, at four sites in the SW grid, PAR(1) model
fit using Yule-Walker method via perARMA.
Series residout[, 50]
0.6
0.2
0.0
0.0
10
20
30
40
0
10
20
30
Lag
Lag
Series residout[, 75]
Series residout[, 100]
40
0.6
0.4
0.0
0.0
0.2
0.2
0.4
ACF
0.6
0.8
0.8
1.0
1.0
0
ACF
0.4
ACF
0.6
0.4
0.2
ACF
0.8
0.8
1.0
1.0
Series residout[, 25]
0
10
20
Lag
30
40
0
10
20
Lag
30
40
Spatial cross-correlation at nearby sites
Center site in SW grid and 4 nearest neighbors (in longitude)
residout[, 55] & residout[, 54]
0.0
0.0
0.2
0.4
ACF
0.2
ACF
0.4
0.6
0.6
0.8
residout[, 55] & residout[, 53]
−20
0
20
−20
0
20
Lag
residout[, 55] & residout[, 56]
residout[, 55] & residout[, 57]
0.2
0.4
ACF
0.4
0.0
0.2
0.0
ACF
0.6
0.6
0.8
0.8
Lag
−20
0
Lag
20
−20
0
Lag
20
Spatial cross-correlation at nearby sites
Center site in SW grid and 4 nearest neighbors (in latitude).
Perhaps a spatial AR(1) will be sufficient?
residout[, 55] & residout[, 45]
0.6
0.0
0.0
0.2
0.4
ACF
0.4
0.2
ACF
0.6
0.8
0.8
residout[, 55] & residout[, 35]
−20
0
20
−20
0
20
Lag
residout[, 55] & residout[, 65]
residout[, 55] & residout[, 75]
0.2
0.4
ACF
0.4
0.2
0.0
0.0
ACF
0.6
0.6
0.8
0.8
Lag
−20
0
Lag
20
−20
0
Lag
20
References
1. I.B. Aban and M.M. Meerschaert, Shifted Hill’s estimator for heavy tails. Communications in Statistics: Simulation and Computation, Vol. 30 (2001), No. 4, pp. 949–962.
2. I.B. Aban, M.M. Meerschaert, and A.K. Panorska, Parameter Estimation for the Truncated Pareto Distribution, Journal of the American Statistical Association: Theory and
Methods, Volume 101 (2006), Number 473, pp. 270–277.
3. P.L. Anderson and M.M. Meerschaert, Periodic moving averages of random variables
with regularly varying tails, The Annals of Statistics, Vol. 25 (1997), No. 2, pp.
771–185.
4. P.L. Anderson, M.M. Meerschaert, Y.G. Tesfaye, Fourier-PARMA Models and Their
Application to Modeling of River Flows, Journal of Hydrologic Engineering, Vol. 12
(2007), No. 5, pp. 462–472.
5. Y.G. Tesfaye, P.L. Anderson, and M.M. Meerschaert, Asymptotic results for FourierPARMA time series, Journal of Time Series Analysis, Vol. 32 (2011), No. 2, pp.
157–174.
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