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Analysing spatial point patterns in R - CSIRO

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156 Gibbs models<br />

26 Gibbs models<br />

One way to construct a statistical model (<strong>in</strong> any field of statistics) is to write down its probability<br />

density. Advantages of do<strong>in</strong>g this are:<br />

the functional form of the density reflects its probabilistic properties.<br />

terms or factors <strong>in</strong> the density often have an <strong>in</strong>terpretation as ‘components’ of the model.<br />

it is easy to <strong>in</strong>troduce terms that represent the dependence of the model on covariates,<br />

etc.<br />

This approach is useful provided the density can be written down, and provided the density<br />

is tractable.<br />

Spatial <strong>po<strong>in</strong>t</strong> process models that are constructed by writ<strong>in</strong>g down their probability densities<br />

are called ‘Gibbs processes’. Good references on Gibbs <strong>po<strong>in</strong>t</strong> processes are [63, 31].<br />

26.1 Probability densities<br />

It is possible to def<strong>in</strong>e probability densities for <strong>spatial</strong> <strong>po<strong>in</strong>t</strong> processes that live <strong>in</strong>side a bounded<br />

w<strong>in</strong>dow W.<br />

The probability density will be a function f(x) def<strong>in</strong>ed for each f<strong>in</strong>ite configuration x =<br />

{x 1 ,... ,x n } of <strong>po<strong>in</strong>t</strong>s x i ∈ W for any n ≥ 0. Notice that the number of <strong>po<strong>in</strong>t</strong>s n is not fixed,<br />

and may be zero. Apart from this peculiarity, probability densities for <strong>po<strong>in</strong>t</strong> processes behave<br />

much like probability densities <strong>in</strong> more familiar contexts.<br />

That’s all you need to know for applications. If you’re <strong>in</strong>terested <strong>in</strong> the mathematical<br />

technicalities, read on; otherwise, skip to section 26.2.<br />

A <strong>po<strong>in</strong>t</strong> process X <strong>in</strong>side W is def<strong>in</strong>ed to have probability density f if and only if, for any<br />

nonnegative <strong>in</strong>tegrable function h,<br />

∑<br />

∞ ∫ ∫<br />

E[h(X)] = e −|W | h(∅)f(∅) + e −|W | 1<br />

· · · h({x 1 ,...,x n })f({x 1 ,...,x n })dx 1 · · · dx n<br />

n!<br />

n=1 W W<br />

(31)<br />

where |W | denotes the area of W.<br />

In particular, the probability that X conta<strong>in</strong>s exactly n <strong>po<strong>in</strong>t</strong>s is<br />

p n = P{n(X) = n} = e−|W | ∫<br />

n!<br />

W<br />

∫<br />

· · · f({x 1 ,... ,x n })dx 1 · · · dx n<br />

W<br />

for n ≥ 1 and p 0 = P{n(X) = 0} = e −|W | f(∅). Given that there are exactly n <strong>po<strong>in</strong>t</strong>s, the<br />

conditional jo<strong>in</strong>t density of the locations x 1 ,... ,x n is f({x 1 ,... ,x n })/p n .<br />

26.2 Poisson processes<br />

The uniform Poisson process with <strong>in</strong>tensity 1 has probability density f(x) ≡ 1.<br />

The uniform Poisson process <strong>in</strong> W with <strong>in</strong>tensity λ has probability density<br />

f(x) = α λ n(x) (32)<br />

where n(x) is the number of <strong>po<strong>in</strong>t</strong>s <strong>in</strong> the configuration x, and the constant α is<br />

α = e (1−λ)|W | .<br />

Copyright<strong>CSIRO</strong> 2010

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