rmhmodel.default | R Documentation |
Builds a description of a point process model for use in simulating the model by the Metropolis-Hastings algorithm.
## Default S3 method:
rmhmodel(...,
cif=NULL, par=NULL, w=NULL, trend=NULL, types=NULL)
... |
Ignored. |
cif |
Character string specifying the choice of model |
par |
Parameters of the model |
w |
Spatial window in which to simulate |
trend |
Specification of the trend in the model |
types |
A vector of factor levels defining the possible marks, for a multitype process. |
The generic function rmhmodel
takes a
description of a point process model in some format, and
converts it into an object of class "rmhmodel"
so that simulations of the model can be generated using
the Metropolis-Hastings algorithm rmh
.
This function rmhmodel.default
is the default method.
It builds a description of the point process model
from the simple arguments listed.
The argument cif
is a character string specifying the choice of
interpoint interaction for the point process. The current options are
'areaint'
Area-interaction process.
'badgey'
Baddeley-Geyer (hybrid Geyer) process.
'dgs'
Diggle, Gates and Stibbard (1987) process
'diggra'
Diggle and Gratton (1984) process
'fiksel'
Fiksel double exponential process (Fiksel, 1984).
'geyer'
Saturation process (Geyer, 1999).
'hardcore'
Hard core process
'lennard'
Lennard-Jones process
'lookup'
General isotropic pairwise interaction process, with the interaction function specified via a “lookup table”.
'multihard'
Multitype hardcore process
'penttinen'
The Penttinen process
'strauss'
The Strauss process
'straush'
The Strauss process with hard core
'sftcr'
The Softcore process
'straussm'
The multitype Strauss process
'straushm'
Multitype Strauss process with hard core
'triplets'
Triplets process (Geyer, 1999).
It is also possible to specify a hybrid of these interactions
in the sense of Baddeley et al (2013).
In this case, cif
is a character vector containing names from
the list above. For example, cif=c('strauss', 'geyer')
would
specify a hybrid of the Strauss and Geyer models.
The argument par
supplies parameter values appropriate to
the conditional intensity function being invoked.
For the interactions listed above, these parameters are:
(Area-interaction process.) A named list with components
beta,eta,r
which are respectively the “base”
intensity, the scaled interaction parameter and the
interaction radius.
(Baddeley-Geyer process.)
A named list with components
beta
(the “base” intensity), gamma
(a vector
of non-negative interaction parameters), r
(a vector
of interaction radii, of the same length as gamma
,
in increasing order), and sat
(the saturation
parameter(s); this may be a scalar, or a vector of the same
length as gamma
and r
; all values should be at
least 1). Note that because of the presence of “saturation”
the gamma
values are permitted to be larger than 1.
(Diggle, Gates, and Stibbard process.
See Diggle, Gates, and Stibbard (1987))
A named list with components
beta
and rho
. This process has pairwise interaction
function equal to
e(t) = \sin^2\left(\frac{\pi t}{2\rho}\right)
for t < \rho
, and equal to 1
for t \ge \rho
.
(Diggle-Gratton process. See Diggle and Gratton (1984)
and Diggle, Gates and Stibbard (1987).)
A named list with components beta
,
kappa
, delta
and rho
. This process has
pairwise interaction function e(t)
equal to 0
for t < \delta
, equal to
\left(\frac{t-\delta}{\rho-\delta}\right)^\kappa
for \delta \le t < \rho
,
and equal to 1 for t \ge \rho
.
Note that here we use the symbol
\kappa
where Diggle, Gates, and Stibbard use
\beta
since we reserve the symbol \beta
for an intensity parameter.
(Fiksel double exponential process, see Fiksel (1984))
A named list with components beta
,
r
, hc
, kappa
and a
. This process has
pairwise interaction function e(t)
equal to 0
for t < hc
, equal to
\exp(a \exp(- \kappa t))
for hc \le t < r
,
and equal to 1 for t \ge r
.
(Geyer's saturation process. See Geyer (1999).)
A named list
with components beta
, gamma
, r
, and sat
.
The components beta
, gamma
, r
are as for
the Strauss model, and sat
is the “saturation”
parameter. The model is Geyer's “saturation” point process
model, a modification of the Strauss process in which
we effectively impose an upper limit (sat
) on the number of
neighbours which will be counted as close to a given point.
Explicitly, a saturation point process with interaction
radius r
, saturation threshold s
, and
parameters \beta
and \gamma
,
is the point process in which each point x_i
in the pattern X
contributes a factor
\beta \gamma^{\min(s, t(x_i,X))}
to the probability density of the point pattern,
where t(x_i,X)
denotes the number of
“r
-close neighbours” of x_i
in the
pattern X
.
If the saturation threshold s
is infinite,
the Geyer process reduces to a Strauss process
with interaction parameter \gamma^2
rather than \gamma
.
(Hard core process.) A named list
with components beta
and hc
where beta
is the base intensity and hc
is the
hard core distance.
This process has pairwise interaction function e(t)
equal to 1 if t > hc
and 0 if t <= hc
.
(Lennard-Jones process.) A named list
with components sigma
and epsilon
,
where sigma
is the characteristic diameter
and epsilon
is the well depth.
See LennardJones
for explanation.
(Multitype hard core process.) A named list
with components beta
and hradii
,
where beta
is a vector of base intensities for each type
of point, and hradii
is a matrix of hard core radii
between each pair of types.
(Penttinen process.) A named list with components
beta,gamma,r
which are respectively the “base”
intensity, the pairwise interaction parameter, and the disc radius.
Note that gamma
must be less than or equal to 1.
See Penttinen
for explanation.
(Note that there is also an algorithm for perfect simulation
of the Penttinen process, rPenttinen
)
(Strauss process.) A named list with components
beta,gamma,r
which are respectively the “base”
intensity, the pairwise interaction parameter and the
interaction radius. Note that gamma
must be less than
or equal to 1.
(Note that there is also an algorithm for perfect simulation
of the Strauss process, rStrauss
)
(Strauss process with hardcore.) A named list with
entries beta,gamma,r,hc
where beta
, gamma
,
and r
are as for the Strauss process, and hc
is
the hardcore radius. Of course hc
must be less than
r
.
(Softcore process.) A named list with components
beta,sigma,kappa
. Again beta
is a “base”
intensity. The pairwise interaction between two points
u \neq v
is
\exp \left \{
- \left ( \frac{\sigma}{||u-v||} \right )^{2/\kappa}
\right \}
Note that it is necessary that 0 < \kappa < 1
.
(Multitype Strauss process.) A named list with components
beta
:
A vector of “base” intensities, one for each possible type.
gamma
:
A symmetric matrix of interaction parameters,
with \gamma_{ij}
pertaining to the interaction between
type i
and type j
.
radii
:
A symmetric matrix of interaction radii, with
entries r_{ij}
pertaining to the interaction between type
i
and type j
.
(Multitype Strauss process with hardcore.)
A named list with components beta
and gamma
as for straussm
and
two “radii” components:
iradii
: the interaction radii
hradii
: the hardcore radii
which are both symmetric matrices of nonnegative numbers.
The entries of hradii
must be less than the
corresponding entries
of iradii
.
(Triplets process.) A named list with components
beta,gamma,r
which are respectively the “base”
intensity, the triplet interaction parameter and the
interaction radius. Note that gamma
must be less than
or equal to 1.
(Arbitrary pairwise interaction process with isotropic interaction.)
A named list with components
beta
, r
, and h
, or just with components
beta
and h
.
This model is the pairwise interaction process
with an isotropic interaction given by any chosen function H
.
Each pair of points x_i, x_j
in the
point pattern contributes
a factor H(d(x_i, x_j))
to the probability density, where d
denotes distance
and H
is the pair interaction function.
The component beta
is a
(positive) scalar which determines the “base” intensity
of the process.
In this implementation, H
must be a step function.
It is specified by the user in one of two ways.
as a vector of values:
If r
is present, then r
is assumed to
give the locations of jumps in the function H
,
while the vector h
gives the corresponding
values of the function.
Specifically, the interaction function
H(t)
takes the value h[1]
for distances t
in the interval
[0, r[1])
; takes the value h[i]
for distances t
in the interval
[r[i-1], r[i])
where
i = 2,\ldots, n
;
and takes the value 1 for t \ge r[n]
.
Here n
denotes the length of r
.
The components r
and h
must be numeric vectors of equal length.
The r
values must be strictly positive, and
sorted in increasing order.
The entries of h
must be non-negative.
If any entry of h
is greater than 1,
then the entry h[1]
must be 0 (otherwise the specified
process is non-existent).
Greatest efficiency is achieved if the values of
r
are equally spaced.
[Note: The usage of r
and h
has changed from the previous usage in spatstat
versions 1.4-7 to 1.5-1, in which ascending order was not required,
and in which the first entry of r
had to be 0.]
as a stepfun object:
If r
is absent, then h
must be
an object of class "stepfun"
specifying
a step function. Such objects are created by
stepfun
.
The stepfun object h
must be right-continuous
(which is the default using stepfun
.)
The values of the step function must all be nonnegative.
The values must all be less than 1
unless the function is identically zero on some initial
interval [0,r)
. The rightmost value (the value of
h(t)
for large t
) must be equal to 1.
Greatest efficiency is achieved if the jumps (the “knots” of the step function) are equally spaced.
For a hybrid model, the argument par
should be a list,
of the same length as cif
, such that par[[i]]
is a list of the parameters required for the interaction
cif[i]
. See the Examples.
The optional argument trend
determines the spatial trend in the model,
if it has one. It should be a function or image
(or a list of such, if the model is multitype)
to provide the value of the trend at an arbitrary point.
A trend
function may be a function of any number of arguments,
but the first two must be the x,y
coordinates of
a point. Auxiliary arguments may be passed
to the trend
function at the time of simulation,
via the ...
argument to rmh
.
The function must be vectorized.
That is, it must be capable of accepting vector valued
x
and y
arguments. Put another way,
it must be capable of calculating the trend value at a
number of points, simultaneously, and should return the
vector of corresponding trend values.
An image (see im.object
)
provides the trend values at a grid of
points in the observation window and determines the trend
value at other points as the value at the nearest grid point.
Note that the trend or trends must be non-negative; no checking is done for this.
The optional argument w
specifies the window
in which the pattern is to be generated. If specified, it must be in
a form which can be coerced to an object of class owin
by as.owin
.
The optional argument types
specifies the possible
types in a multitype point process. If the model being simulated
is multitype, and types
is not specified, then this vector
defaults to 1:ntypes
where ntypes
is the number of
types.
An object of class "rmhmodel"
, which is essentially
a list of parameter values for the model.
There is a print
method for this class, which prints
a sensible description of the model chosen.
For the lookup
cif,
the entries of the r
component of par
must be strictly positive and sorted into ascending order.
Note that if you specify the lookup
pairwise interaction
function via stepfun()
the arguments x
and y
which are passed to stepfun()
are slightly
different from r
and h
: length(y)
is equal
to 1+length(x)
; the final entry of y
must be equal
to 1 — i.e. this value is explicitly supplied by the user rather
than getting tacked on internally.
The step function returned by stepfun()
must be right
continuous (this is the default behaviour of stepfun()
)
otherwise an error is given.
and \rolf
Baddeley, A., Turner, R., Mateu, J. and Bevan, A. (2013)
Hybrids of Gibbs point process models and their implementation.
Journal of Statistical Software 55:11, 1–43.
DOI: 10.18637/jss.v055.i11
Diggle, P. J. (2003) Statistical Analysis of Spatial Point Patterns (2nd ed.) Arnold, London.
Diggle, P.J. and Gratton, R.J. (1984) Monte Carlo methods of inference for implicit statistical models. Journal of the Royal Statistical Society, series B 46, 193 – 212.
Diggle, P.J., Gates, D.J., and Stibbard, A. (1987) A nonparametric estimator for pairwise-interaction point processes. Biometrika 74, 763 – 770. Scandinavian Journal of Statistics 21, 359–373.
Fiksel, T. (1984) Estimation of parameterized pair potentials of marked and non-marked Gibbsian point processes. Electronische Informationsverabeitung und Kybernetika 20, 270–278.
Geyer, C.J. (1999) Likelihood Inference for Spatial Point Processes. Chapter 3 in O.E. Barndorff-Nielsen, W.S. Kendall and M.N.M. Van Lieshout (eds) Stochastic Geometry: Likelihood and Computation, Chapman and Hall / CRC, Monographs on Statistics and Applied Probability, number 80. Pages 79–140.
rmh
,
rmhcontrol
,
rmhstart
,
ppm
,
\rmhInteractionsList.
# Strauss process:
mod01 <- rmhmodel(cif="strauss",par=list(beta=2,gamma=0.2,r=0.7),
w=c(0,10,0,10))
mod01
# The above could also be simulated using 'rStrauss'
# Strauss with hardcore:
mod04 <- rmhmodel(cif="straush",par=list(beta=2,gamma=0.2,r=0.7,hc=0.3),
w=owin(c(0,10),c(0,5)))
# Hard core:
mod05 <- rmhmodel(cif="hardcore",par=list(beta=2,hc=0.3),
w=square(5))
# Soft core:
w <- square(10)
mod07 <- rmhmodel(cif="sftcr",
par=list(beta=0.8,sigma=0.1,kappa=0.5),
w=w)
# Penttinen process:
modpen <- rmhmodel(cif="penttinen",par=list(beta=2,gamma=0.6,r=1),
w=c(0,10,0,10))
# Area-interaction process:
mod42 <- rmhmodel(cif="areaint",par=list(beta=2,eta=1.6,r=0.7),
w=c(0,10,0,10))
# Baddeley-Geyer process:
mod99 <- rmhmodel(cif="badgey",par=list(beta=0.3,
gamma=c(0.2,1.8,2.4),r=c(0.035,0.07,0.14),sat=5),
w=unit.square())
# Multitype Strauss:
beta <- c(0.027,0.008)
gmma <- matrix(c(0.43,0.98,0.98,0.36),2,2)
r <- matrix(c(45,45,45,45),2,2)
mod08 <- rmhmodel(cif="straussm",
par=list(beta=beta,gamma=gmma,radii=r),
w=square(250))
# specify types
mod09 <- rmhmodel(cif="straussm",
par=list(beta=beta,gamma=gmma,radii=r),
w=square(250),
types=c("A", "B"))
# Multitype Hardcore:
rhc <- matrix(c(9.1,5.0,5.0,2.5),2,2)
mod08hard <- rmhmodel(cif="multihard",
par=list(beta=beta,hradii=rhc),
w=square(250),
types=c("A", "B"))
# Multitype Strauss hardcore with trends for each type:
beta <- c(0.27,0.08)
ri <- matrix(c(45,45,45,45),2,2)
rhc <- matrix(c(9.1,5.0,5.0,2.5),2,2)
tr3 <- function(x,y){x <- x/250; y <- y/250;
exp((6*x + 5*y - 18*x^2 + 12*x*y - 9*y^2)/6)
}
# log quadratic trend
tr4 <- function(x,y){x <- x/250; y <- y/250;
exp(-0.6*x+0.5*y)}
# log linear trend
mod10 <- rmhmodel(cif="straushm",par=list(beta=beta,gamma=gmma,
iradii=ri,hradii=rhc),w=c(0,250,0,250),
trend=list(tr3,tr4))
# Triplets process:
mod11 <- rmhmodel(cif="triplets",par=list(beta=2,gamma=0.2,r=0.7),
w=c(0,10,0,10))
# Lookup (interaction function h_2 from page 76, Diggle (2003)):
r <- seq(from=0,to=0.2,length=101)[-1] # Drop 0.
h <- 20*(r-0.05)
h[r<0.05] <- 0
h[r>0.10] <- 1
mod17 <- rmhmodel(cif="lookup",par=list(beta=4000,h=h,r=r),w=c(0,1,0,1))
# hybrid model
modhy <- rmhmodel(cif=c('strauss', 'geyer'),
par=list(list(beta=100,gamma=0.5,r=0.05),
list(beta=1, gamma=0.7,r=0.1, sat=2)),
w=square(1))
modhy
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