RMmodelsTailcorrelation: Covariance models valid for max-stable random fields

Description Details References See Also Examples

Description

This page summarizes the models that can be used for tail correlation functions.

Details

The following models are available:

Completely monotone functions allowing for arbitrary scale

RMbcw Model bridging stationary and intrinsically stationary processes for alpha <= 1 and beta < 0
RMdagum Dagum model with β < γ and γ ≤ 1
RMexp exponential model
RMgencauchy generalized Cauchy family with α ≤ 1 (and arbitrary β> 0)
RMmatern Whittle-Matern model with ν ≤ 1/2
RMstable symmetric stable family or powered exponential model with α ≤ 1
RMwhittle Whittle-Matern model, alternative parametrization with ν ≤ 1/2

Other isotropic models with arbitrary scale

RMnugget nugget effect model

Compactly supported covariance functions

RMaskey Askey's model
RMcircular circular model
RMconstant identically constant
RMcubic cubic model
RMgengneiting Wendland-Gneiting model; differentiable models with compact support
RMgneiting differentiable model with compact support
RMspheric spherical model

Anisotropic models

None up to now.

Basic Operators

RMmult, * product of covariance models
RMplus, + sum of covariance models or variograms

Operators related to process constructions

RMbernoulli correlation of binary fields
RMbrownresnick tcf of a Brown-Resnick process
RMschlather tcf of an extremal Gaussian process / Schlather process
RMm2r M2 process with monotone shape function
RMm3b M3 process with balls of random radius
RMmps M3 process with hyperplane polygons

See RMmodels for cartesian models.

References

See Also

coordinate systems, RM, RMmodels, RMtrafo.

Examples

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RFoptions(seed=0) ## *ANY* simulation will have the random seed 0; set
##                   RFoptions(seed=NA) to make them all random again
RFgetModelNames(type="tail")

## an example of a simple model
model <- RMexp(var=1.6, scale=0.5) + RMnugget(var=0) #exponential + nugget
plot(model)

RandomFields documentation built on Jan. 19, 2022, 1:06 a.m.