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                                                      4.4 Cumulants                          111

                        aX + b is given by exp(bt)M X (at), it is clear that repeated differentiation of this expression
                        with respect to t will lead to a fairly complicated expression; specifically, by Leibnitz’s rule
                        for differentiation (see Appendix 3), the nth moment of aX + b is given by
                                             n
                                                 n  n− j  j  j
                                                   b   a E(X ), n = 0, 1,....
                                                 j
                                             j=0
                        Similarly, the moment-generating of X + Y is given by M X (t)M Y (t) and differentiating this
                        function can lead to a complicated result.
                          In both cases, the situation is simplified if, instead of using the moment-generating
                        function itself, we use the log of the moment-generating function. For instance, if M aX+b
                        denotes the moment-generating function of aX + b, then

                                               log M aX+b (t) = bt + log M X (at)
                        and the derivatives of log M aX+b (t)at t = 0havea relatively simple relationship to the
                        derivatives of log M X (at). Of course, these derivatives no longer represent the moments
                        of the distribution, although they will be functions of the moments; these functions of the
                        moments are called the cumulants of the distribution. In this section, the basic theory of
                        cumulants is presented.
                          Let X denote a real-valued random variable with moment-generating function M X (t),
                        |t| <δ. The cumulant-generating function of X is defined as

                                                K X (t) = log M X (t), |t| <δ.
                        Since, by Theorem 4.8, M X has a power series expansion for t near 0, the cumulant-
                        generating function may be expanded

                                                         ∞
                                                           κ j  j

                                                 K X (t) =    t , |t| <δ
                                                            j!
                                                        j=1
                        where κ 1 ,κ 2 ,... are constants that depend on the distribution of X. These constants are
                        called the cumulants of the distribution or, more simply, the cumulants of X. The constant
                        κ j will be called the jth cumulant of X;we may also write the jth cumulant of X as κ j (X).
                          Hence, the cumulants may be obtained by differentiation of K X ,in the same way that
                        the moments of a distribution may be obtained by differentiation of the moment-generating
                        function:
                                                  d  j

                                             κ j =   K X (t)   ,  j = 1, 2,....
                                                  dt  j    t=0
                        Example 4.17 (Standard normal distribution). Let Z denote a random variable with a
                        standard normal distribution. It is straightforward to show that the moment-generating
                        function of this distribution is given by
                                       ∞
                                                 1         1  2          2

                             M Z (t) =   exp(tz)√    exp − z    dz = exp(t /2), −∞ < t < ∞
                                                (2π)       2
                                      −∞
                        and, hence, the cumulant-generating function is given by
                                                       1  2
                                               K Z (t) =  t , −∞ < t < ∞.
                                                       2
                        It follows that κ 1 = 0, κ 2 = 1, and κ j = 0, j = 3, 4,....
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