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Next: Simulating Finite Point Processes Up: Limit Models from Strauss Previous: Conditional Strauss Processes

Unconditional Strauss Processes

Applying Proposition 1 to the unconditional Strauss process, any tex2html_wrap_inline2319 with tex2html_wrap_inline3251 is a direction of recession. But if tex2html_wrap_inline3253 then tex2html_wrap_inline3255 and the limit obtained using the proposition is the uninteresting process that has no points with probability one.

If tex2html_wrap_inline3257 and tex2html_wrap_inline3259 , then

displaymath3261

The process obtained by conditioning a Strauss process on tex2html_wrap_inline3263 is the general hard core process. Note that one obtains the same hard core process by conditioning any Strauss process tex2html_wrap_inline3265 for any tex2html_wrap_inline3267 . Thus we obtain the complete family of hard core processes by conditioning Strauss processes tex2html_wrap_inline2381 with tex2html_wrap_inline3145 , that is, Poisson processes. This connexion between the Strauss process and hard core process is, of course, well-known, though not usually derived using general properties of exponential families. The reason for drawing the connexion here, is that we will also be interested in other point process models for which there is no existing literature. The point of the proposition is that whenever we consider a point process model that is an exponential family a natural question arises as to what models arise from taking limits in directions of recession using Proposition 1.

There is still one kind of direction of recession left to consider. If tex2html_wrap_inline3273 and tex2html_wrap_inline3259 , then the characterization of tex2html_wrap_inline3277 is not obvious. Every such vector is a direction of recession. To see this we divide S into m disjoint subregions of radius less than r so that any two points in a subregion are neighbours. If there are tex2html_wrap_inline3285 points in the ith subregion, then tex2html_wrap_inline3289 and tex2html_wrap_inline3291 . It is easy to see that the latter is minimized over a real ntuples tex2html_wrap_inline3293 when tex2html_wrap_inline3295 . Hence

displaymath3297

Since this is quadratic in n(x), it follows that tex2html_wrap_inline3301 is bounded on tex2html_wrap_inline2343 . Thus tex2html_wrap_inline3263 , the set of x where the least upper bound is achieved, is nonempty, and a limit process in the direction tex2html_wrap_inline2319 can be defined. What it not clear, is what the process or the set tex2html_wrap_inline3263 looks like. Perhaps this is related to the strange plots of unconditional Strauss processes exhibited by Professor Møller at the meeting.


next up previous
Next: Simulating Finite Point Processes Up: Limit Models from Strauss Previous: Conditional Strauss Processes

Charles Geyer
Fri Jul 5 15:26:21 CDT 1996