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Stat 5101 Lecture Notes - School of Statistics

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122 <strong>Stat</strong> <strong>5101</strong> (Geyer) Course <strong>Notes</strong>because the measure <strong>of</strong> the union <strong>of</strong> disjoint regions is the sum <strong>of</strong> the measures.This is also obvious from linearity <strong>of</strong> expectation. We must haveE(X 1 + ···+X n )=E(X 1 )+···+E(X n ).Corollary 4.6. The conditional distribution <strong>of</strong> a Poisson process in a regionA c given the process in A is the same as the unconditional distribution <strong>of</strong> theprocess in A c .In other words, finding the point pattern in A tells you nothing whatsoeverabout the pattern in A c . The pattern in A c has the same distributionconditionally or unconditionally.Pro<strong>of</strong>. By Definition 4.4.1 and Theorem 4.4 N B is independent <strong>of</strong> N C whenB ⊂ A c and C ⊂ A. Since this is true for all such C, the random variable N Bis independent <strong>of</strong> the whole pattern in A, and its conditional distribution giventhe pattern in A is the same as its unconditional distribution. Theorem 4.4 saysPoisson distributions <strong>of</strong> the N B for all subsets B <strong>of</strong> A c imply that the processin A c is a Poisson process.4.4.3 One-Dimensional Poisson ProcessesIn this section we consider Poisson processes in one-dimensional space, thatis, on the real line. So a realization <strong>of</strong> the process is a pattern <strong>of</strong> points on theline. For specificity, we will call the dimension along the line “time” because formany applications it is time. For example, the calls arriving at a telephone exchangeare <strong>of</strong>ten modeled by a Poisson process. So are the arrivals <strong>of</strong> customersat a bank teller’s window, or at a toll plaza on an toll road. But you shouldremember that there is nothing in the theory specific to time. The theory is thesame for all one-dimensional Poisson processes.Continuing the time metaphor, the points <strong>of</strong> the process will always in therest <strong>of</strong> this section be called arrivals. The time from a fixed point to the nextarrival is called the waiting time until the arrival.The special case <strong>of</strong> the gamma distribution with shape parameter one iscalled the exponential distribution, denoted Exp(λ). Its density isf(x) =λe −λx , x > 0. (4.10)Theorem 4.7. The distribution <strong>of</strong> the waiting time in a homogeneous Poissonprocess with rate parameter λ is Exp(λ). The distribution is the same unconditionally,or conditional on the past history up to and including the time westart waiting.Call the waiting time X and the point where we start waiting a. Fix anx>0, let A =(a, a + x), and let Y = N (a,a+x) be the number <strong>of</strong> arrivals in theinterval A. Then Y has a Poisson distribution with mean λm(A) =λx, since

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