2014
DOI: 10.1111/rssb.12061
|View full text |Cite
|
Sign up to set email alerts
|

Stochastic Partial Differential Equation Based Modelling of Large Space–Time Data Sets

Abstract: Increasingly larger data sets of processes in space and time ask for statistical models and methods that can cope with such data. We show that the solution of a stochastic advectiondiffusion partial differential equation provides a flexible model class for spatio-temporal processes which is computationally feasible also for large data sets. The Gaussian process defined through the stochastic partial differential equation has in general a nonseparable covariance structure. Furthermore, its parameters can be phy… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

1
109
0

Year Published

2015
2015
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 86 publications
(110 citation statements)
references
References 122 publications
(203 reference statements)
1
109
0
Order By: Relevance
“…The covariance function given here is fundamentally different from the other covariance functions defined and used by other authors. We further show that the second‐order spectral density function of the spatio‐temporal random process defined here through the aforementioned Laplace operator on the DFTs includes all the second‐order spectra of the processes so far defined through the stochastic versions of the Laplace equation such as the heat equation (transport–diffusion equation of Jones and Zhang (), Lindgren et al (), and Sigrist et al ()), wave equation, and Helmholtz equation. The second‐order spectral density function obtained here corresponds to a non‐separable random process.…”
Section: Introductionmentioning
confidence: 77%
See 3 more Smart Citations
“…The covariance function given here is fundamentally different from the other covariance functions defined and used by other authors. We further show that the second‐order spectral density function of the spatio‐temporal random process defined here through the aforementioned Laplace operator on the DFTs includes all the second‐order spectra of the processes so far defined through the stochastic versions of the Laplace equation such as the heat equation (transport–diffusion equation of Jones and Zhang (), Lindgren et al (), and Sigrist et al ()), wave equation, and Helmholtz equation. The second‐order spectral density function obtained here corresponds to a non‐separable random process.…”
Section: Introductionmentioning
confidence: 77%
“…By substituting the spectral representations for the processes { Y t ( s )} and { e t ( s ) } and equating the integrands, after taking expectations of the squared modulus we can show that the spatio‐temporal spectral density function of the process { Y t ( s )} is given by fY()falseλ_,ω1/[()λ12+λ22+γ22+ω2]. We note that no closed form for the covariance function is available in this case (see Sigrist et al ()).…”
Section: A Cspde and An Expression For The Spectrum G‖‖boldh()ωmentioning
confidence: 97%
See 2 more Smart Citations
“…Sigrist et al [80] utilizes stochastic advection diffusion partial differential equations (SPDEs) to improve the precipitation forecasts for northern Switzerland using Big Data from a numerical weather prediction model. They find that following the application of SPDE, the forecasts are greatly improved in comparison to the raw forecasts attained via the numerical model.…”
Section: Forecasting With Big Data In Environmentmentioning
confidence: 99%