In probability theory and statistics, a Hawkes process is an age-dependent branching process driven by immigration from an inhomogeneous Poisson process. The process, named after Alan G. Hawkes, is also called a self-exciting point process., i.e., the occurrence of an event increases the likelihood of another event occurring. It has arrivals at times 0 < t 1 < t 2 < t 3 < ⋯ {\textstyle 0<t_{1}<t_{2}<t_{3}<\cdots } where the infinitesimal probability of an arrival during the time interval [ t , t + d t ) {\textstyle [t,t+dt)} is
λ t d t = ( μ ( t ) + ∑ t k : t k < t ϕ ( t − t k ) ) d t . {\displaystyle \lambda _{t}\,dt=\left(\mu (t)+\sum _{t_{k}\,:\,t_{k}\,<\,t}\phi (t-t_{k})\right)\,dt.}
The function μ {\textstyle \mu } is the intensity of an underlying Poisson process. The first arrival occurs at time t 1 {\textstyle t_{1}} and immediately after that, the intensity becomes μ ( t ) + ϕ ( t − t 1 ) {\textstyle \mu (t)+\phi (t-t_{1})} , and at the time t 2 {\textstyle t_{2}} of the second arrival the intensity jumps to μ ( t ) + ϕ ( t − t 1 ) + ϕ ( t − t 2 ) {\textstyle \mu (t)+\phi (t-t_{1})+\phi (t-t_{2})} and so on. During the time interval ( t k , t k + 1 ) {\textstyle (t_{k},t_{k+1})} , the process is the sum of k + 1 {\textstyle k+1} independent processes with intensities μ ( t ) , ϕ ( t − t 1 ) , … , ϕ ( t − t k ) . {\textstyle \mu (t),\phi (t-t_{1}),\ldots ,\phi (t-t_{k}).} The arrivals in the process whose intensity is ϕ ( t − t k ) {\textstyle \phi (t-t_{k})} are the "daughters" of the arrival at time t k . {\textstyle t_{k}.} The integral ∫ 0 ∞ ϕ ( t ) d t {\displaystyle \int _{0}^{\infty }\phi (t)\,dt} is the average number of daughters of each arrival and is called the branching ratio. Thus viewing some arrivals as descendants of earlier arrivals, we have a Galton–Watson branching process. The number of such descendants is finite with probability 1 if branching ratio is 1 or less. If the branching ratio is more than 1, then each arrival has positive probability of having infinitely many descendants.
… excerpt ends here. Continue reading the full article.
