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14
                              Poisson Approximation
                              14.1 Introduction

                              In the past few years, mathematicians have developed a powerful technique
                              known as the Chen-Stein method [2, 5] for approximating the distribution
                              of a sum of weakly dependent Bernoulli random variables. In contrast to
                              many asymptotic methods, this approximation carries with it explicit error
                              bounds. Let X α be a Bernoulli random variable with success probability p α ,
                              where α ranges over some finite index set I. It is natural to speculate that

                              the sum S =       X α is approximately Poisson with mean λ =  p α .
                                            α∈I                                          α∈I
                              The Chen-Stein method estimates the error in this approximation using
                              the total variation distance between two integer-valued random variables
                              Y and Z. This distance is defined by
                                        	L(Y ) −L(Z)	 =    sup | Pr(Y ∈ A) − Pr(Z ∈ A)|,
                                                           A⊂N
                              where L denotes distribution, and N denotes the integers. Taking A = {0}
                              in this definition yields the useful inequality

                                          | Pr(Y =0) − Pr(Z =0)|≤	L(Y ) −L(Z)	.
                                The coupling method is one technique for explicitly bounding the total

                              variation distance between S =    X α and a Poisson random variable
                                                             α∈I
                              Z with the same mean λ [5, 15]. In many concrete examples, it is possible
                              to construct for each α two random variables U α and V α on a common
                              probability space in such a way that V α is distributed as S − 1 conditional
                              on the event X α = 1 and U α is distributed as S unconditionally. The bound
                                                            1 − e −λ
                                         	L(S) −L(Z)	Ø                 p α E(|U α − V α |)  (14.1)
                                                               λ
                                                                   α∈I
                              then applies. Because U α and V α live on the same probability space, they
                              are said to be coupled. If U α ≥ V α for all α, then the simplified bound

                                                               1 − e −λ
                                             	L(S) −L(Z)	Ø            [λ − Var(S)]        (14.2)
                                                                  λ
                              holds. Inequality (14.2) shows that Var(S) ≈ E(S) is a sufficient as well as
                              a necessary condition for S to be approximately Poisson.
                                The neighborhood method of bounding the total variation distance
                              exploits certain neighborhoods of dependency B α associated with each α
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