suffstat(model, X=data.ppm(model))
"ppm"
)."ppp"
).coef(model)
.model
is evaluated for the point pattern X
.
This computation is useful for various Monte Carlo methods.
Here model
should be a point process model (object of class
"ppm"
, see ppm.object
), typically obtained
from the model-fitting function ppm
. The argument
X
should be a point pattern (object of class "ppp"
). Every point process model fitted by ppm
has
a probability density of the form
$$f(x) = Z(\theta) \exp(\theta^T S(x))$$
where $x$ denotes a typical realisation (i.e. a point pattern),
$\theta$ is the vector of model coefficients,
$Z(\theta)$ is a normalising constant,
and $S(x)$ is a function of the realisation $x$, called the
``canonical sufficient statistic'' of the model.
For example, the stationary Poisson process has canonical sufficient statistic $S(x)=n(x)$, the number of points in $x$. The stationary Strauss process with interaction range $r$ (and fitted with no edge correction) has canonical sufficient statistic $S(x)=(n(x),s(x))$ where $s(x)$ is the number of pairs of points in $x$ which are closer than a distance $r$ to each other.
suffstat(model, X)
returns the value of $S(x)$, where $S$ is
the canonical sufficient statistic associated with model
,
evaluated when $x$ is the given point pattern X
.
The result is a numeric vector, with entries which correspond to the
entries of the coefficient vector coef(model)
.
The sufficient statistic $S$
does not depend on the fitted coefficients
of the model. However it does depend on the irregular parameters
which are fixed in the original call to ppm
, for
example, the interaction range r
of the Strauss process.
The sufficient statistic also depends on the edge correction that was used to fit the model. For example in a Strauss process,
correction="none"
, the sufficient
statistic is$S(x) = (n(x), s(x))$where$n(x)$is the
number of points and$s(x)$is the number of pairs of points
which are closer than$r$units apart.correction="periodic"
, the sufficient
statistic is the same as above, except that distances are measured
in the periodic sense.correction="translate"
, then$n(x)$is unchanged
but$s(x)$is replaced by a weighted sum (the sum of the translation
correction weights for all pairs of points which are closer than$r$units apart).correction="border"
(the default), then points lying less than$r$units from the boundary of the observation window are
treated as fixed. Thus$n(x)$is
replaced by the number$n_r(x)$of points lying at least$r$units from
the boundary of the observation window, and$s(x)$is replaced by
the number$s_r(x)$of pairs of points, which are closer
than$r$units apart, and at least one of which lies
more than$r$units from the boundary of the observation window. Non-finite values of the sufficient statistic (NA
or
-Inf
) may be returned if the point pattern X
is
not a possible realisation of the model (i.e. if X
has zero
probability of occurring under model
for all values of
the canonical coefficients $\theta$).
ppm
data(swedishpines)
fitS <- ppm(swedishpines, ~1, Strauss(7))
X <- rpoispp(summary(swedishpines)$intensity, win=swedishpines$window)
suffstat(fitS, X)
Run the code above in your browser using DataLab