Generalized Shock Models Based on a Cluster Point Process

2006 ◽  
Vol 55 (3) ◽  
pp. 542-550 ◽  
Author(s):  
J.-M. Bai ◽  
Z.-H. Li ◽  
X.-B. Kong
Author(s):  
Francisco J. Martin-Vega ◽  
Yuanwei Liu ◽  
Gerardo Gomez ◽  
Mari Carmen Aguayo-Torres ◽  
Maged Elkashlan

2020 ◽  
Vol 35 ◽  
pp. 100414
Author(s):  
Nancy L. Garcia ◽  
Peter Guttorp ◽  
Guilherme Ludwig

1996 ◽  
Vol 28 (2) ◽  
pp. 346-355 ◽  
Author(s):  
A. J. Baddeley ◽  
M. N. M. Van Lieshout ◽  
J. Møller

We show that a Poisson cluster point process is a nearest-neighbour Markov point process [2] if the clusters have uniformly bounded diameter. It is typically not a finite-range Markov point process in the sense of Ripley and Kelly [12]. Furthermore, when the parent Poisson process is replaced by a Markov or nearest-neighbour Markov point process, the resulting cluster process is also nearest-neighbour Markov, provided all clusters are non-empty. In particular, the nearest-neighbour Markov property is preserved when points of the process are independently randomly translated, but not when they are randomly thinned.


1989 ◽  
Vol 26 (4) ◽  
pp. 793-806 ◽  
Author(s):  
Keigo Yamada

We consider an additive shock process where shocks occur according to a Poisson point process and they are accumulated in an appropriate way to the damage. It is shown that suitably normalized shock processes converge weakly to a process which is represented as a sum of a stable process and a deterministic process.


1977 ◽  
Vol 14 (03) ◽  
pp. 464-474
Author(s):  
C. D. Lai

A two-dimensional Poisson cluster point process is formulated by the use of a probability generating functional. Moment measures of both the cluster centre and member processes are discussed. An example is provided, and the magnitude frequency law is proved in this case.


1989 ◽  
Vol 26 (04) ◽  
pp. 793-806
Author(s):  
Keigo Yamada

We consider an additive shock process where shocks occur according to a Poisson point process and they are accumulated in an appropriate way to the damage. It is shown that suitably normalized shock processes converge weakly to a process which is represented as a sum of a stable process and a deterministic process.


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