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Some Important Continuous Distributions                         207

           The superscripts T and   1 denote, respectively, matrix transpose and matrix
           inverse. Again, we see that a joint normal distribution is completely specified
           by the first-order and second-order joint moments.
             It is instructive to derive the joint characteristic function associated with X.
           As seen from Section 4.5.3, it is defined by
                         …t 1 ; t 2 ; ... ; t n †ˆ   …t†
                    X 1 X 2 ...X n      X
                                     ˆ Efexp‰j…t 1 X 1 ‡     ‡ t n X n †Šg
                                         1      1                        …7:32†
                                       Z      Z
                                                       T
                                     ˆ            exp…jt x†f …x†dx;
                                                           X
                                         1      1
           which gives, on substituting Equation (7.30) into Equation (7.32),
                                                 1
                                             T
                                                   T
                                  …t†ˆ exp jm t   t  t ;                 …7:33†
                                 X
                                                 2
                 T
           where t ˆ  [t 1  t 2      t n ].
             Joint moments of X can be obtained by differentiating joint characteristic
           function   X (t) with respect to t and setting t ˆ  0. The expectation
           EfX X  2 m 2      X g,  for example, is given by
                        m n
               m 1
                        n
              1
                                                q m 1 ‡m 2 ‡   ‡m n

                   m 1
               EfX X  m 2      X gˆ j  …m 1 ‡m 2 ‡   ‡m n †    …t†       …7:34†
                            m n
                   1  2     n                    m 1  m 2  m n  X
                                               qt qt      qt n
                                                 1  2             tˆ0
             It is clear that, since joint moments of the first-order and second-order
           completely specify the joint normal distribution, these moments also determine
           joint moments of orders higher than 2. We can show that, in the case when
           random variables X 1 , X 2 ,      , X n  have zero means, all odd-order moments of
           these random variables vanish, and, for n even,
                               X
              EfX 1 X 2     X n gˆ  EfX m 1  X m 2  gEfX m 2  X m 3  g    EfX m n 1  X m n g  …7:35†
                              m 1 ;...;m n
           The  sum  above  is taken  over  all  possible  combinations  of  n/2  pairs  of  the
           n  random  variables.  The number  of  terms  in  the summation  is  (1)(3)(5)
           (n    3)(n    1).


           7.2.4  SUMS  OF  NORMAL  RANDOM  VARIABLES

           We have seen through discussions and examples that sums of random variables
           arise in a number of problem formulations. In the case of normal random
           variables, we have the following important result (Theorem 7.4).








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