2014
DOI: 10.1016/j.spl.2014.01.032
|View full text |Cite
|
Sign up to set email alerts
|

Trajectory composition of Poisson time changes and Markov counting systems

Abstract: Changing time of simple continuous-time Markov counting processes by independent unit-rate Poisson processes results in Markov counting processes for which we provide closed-form transition rates via composition of trajectories and with which we construct novel, simpler infinitesimally over-dispersed processes.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2018
2018
2020
2020

Publication Types

Select...
1
1

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(1 citation statement)
references
References 31 publications
(47 reference statements)
0
1
0
Order By: Relevance
“…Simultaneous transitions can occur under some conditions (see, e.g., Bretó, 2012a; Kozubowski and Podgórski, 2009; Lee and Whitmore, 1993) when time is changed by a stochastic process or clock (see, e.g., Bochner, 1949; Barndorff-Nielsen and Shiryaev, 2010). In particular, simultaneous transitions arise naturally when individual transitions are accumulated and released at once at discontinuity points of paths of the new time, as happens when time is changed by a Poisson clock (Bretó, 2014a) or by the gamma clock of Section 4.1. Although such simultaneous transitions are necessary for overdispersion of continuous-time Markov chains (Bretó and Ionides, 2011), overdispersion can be described in different terms, e.g., in terms of randomized transition rates, as in the following example.…”
Section: Overdispersion In Transmission Modelsmentioning
confidence: 99%
“…Simultaneous transitions can occur under some conditions (see, e.g., Bretó, 2012a; Kozubowski and Podgórski, 2009; Lee and Whitmore, 1993) when time is changed by a stochastic process or clock (see, e.g., Bochner, 1949; Barndorff-Nielsen and Shiryaev, 2010). In particular, simultaneous transitions arise naturally when individual transitions are accumulated and released at once at discontinuity points of paths of the new time, as happens when time is changed by a Poisson clock (Bretó, 2014a) or by the gamma clock of Section 4.1. Although such simultaneous transitions are necessary for overdispersion of continuous-time Markov chains (Bretó and Ionides, 2011), overdispersion can be described in different terms, e.g., in terms of randomized transition rates, as in the following example.…”
Section: Overdispersion In Transmission Modelsmentioning
confidence: 99%