Page 30 - A First Course In Stochastic Models
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COMPOUND POISSON PROCESSES                    21

                scheme for computing Poisson probabilities. An alternative method to compute the
                compound Poisson probabilities r j (t), j = 0, 1, . . . is to apply the discrete FFT
                method to the explicit expression (1.2.2) for the generating function of the r j (t);
                see Appendix D.


                Continuous compound Poisson distribution
                Suppose now that the non-negative random variables D i are continuously dis-
                tributed with probability distribution function A(x) = P {D 1 ≤ x} having the prob-
                ability density a(x). Then the compound Poisson variable X(t) has the positive
                mass e −λt  at point zero and a density on the positive real line. Let

                                                ∞
                                        ∗          −sx
                                       a (s) =    e  a(x) dx
                                               0
                be the Laplace transform of a(x). In the same way that (1.2.2) was derived,
                                                        ∗
                                      E[e −sX(t) ] = e −λt{1−a (s)} .
                Fix t > 0. How do we compute P {X(t) > x} as function of x? Several compu-
                tational methods can be used. The probability distribution function P {X(t) > x}
                for x ≥ 0 can be computed by using a numerical method for Laplace inver-
                sion; see Appendix F. By relation (E.7) in Appendix E, the Laplace transform of
                P {X(t) > x} is given by

                                                                ∗
                                ∞                     1 − e −λt{1−a (s)}

                                  e −sx  P {X(t) > x} dx =          .
                               0                            s
                If no explicit expression is available for a (s) (as is the case when the D i are
                                                    ∗
                lognormally distributed), an alternative is to use the integral equation
                                 t
                                                x
                 P {X(t) > x} =    1 − A(x) +   P {X(t − u) > x − y}a(y) dy λe −λu  du.
                                0             0
                This integral equation is easily obtained by conditioning on the epoch of the first
                Poisson event and by conditioning on D 1 . The corresponding integral equation
                for the density of X(t) can be numerically solved by applying the discretization
                algorithm given in Den Iseger et al. (1997). This discretization method uses spline
                functions and is very useful when one is content with an approximation error of
                about 10 −8 . Finally, for the special case of the D i having a gamma distribution,
                the probability P {X(t) > x} can simply be computed from
                                         ∞         n
                                             −λt  (λt)
                                                          n∗
                           P {X(t) > x} =   e       {1 − B (x)},  x > 0,
                                                 n!
                                         n=1
                where the n-fold convolution function B  n∗  (x) is the probability distribution func-
                tion of D 1 + · · · + D n . If the D i have a gamma distribution with shape parameter
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