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104                    Fundamentals of Probability and Statistics for Engineers

           and therefore
                                          1  Z  u
                              p …x†ˆ lim       Efe j…X x†t gdt
                               X
                                     u!1 2u
                                              u
                                                                        …4:67†
                                          1  Z  u   jtx
                                   ˆ lim       e     X …t†dt;
                                     u!1 2u
                                              u
           which gives the desired inversion formula.
             In summary, the transform pairs given by Equations (4.46), (4.47), (4.58),
           and (4.64) are collected and presented below for easy reference. For a contin-
           uous random variable X,

                                      Z  1              9
                                           jtx
                                 X …t†ˆ   e f …x†dx;    >
                                              X
                                                        >
                                        1               >
                                                        =
                                                                        …4:68†
                                       1  Z  1   jtx    >
                               f …x†ˆ        e          >
                                                        >
                                X                 X …t†dt; ;
                                      2    1
           and, for a discrete random variable X,
                                     X
                                                         9
                                X …t†ˆ  e  jtx i p …x i †;
                                            X            >
                                                         >
                                      i                  =              …4:69†
                                         1  Z  u   jtx   >
                             p …x†ˆ lim       e     X …t†dt: ;
                                                         >
                              X
                                     u!1 2u
                                             u
           Of the two sets, Equations (4.68) for the continuous case are more important in
           terms of applicability. As we shall see in Chapter 5, probability mass functions
           for discrete random variables can be found directly without resorting to their
           characteristic functions.
             As we have mentioned before, the characteristic function is particularly
           useful for the study of a sum of independent random variables. In this connec-
           tion, let us state the following important theorem, (Theorem 4.3).
             Theorem 4.3: The characteristic function of a sum of independent random
           variables is equal to the product of the characteristic functions of the individual
           random variables.

             Proof of Theorem 4.3: Let

                                  Y ˆ X 1 ‡ X 2 ‡     ‡ X n :           …4:70†








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