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The form in (42) is not readily obtainable by a change of variables directly in (41) However, by rst extending (41) to two dimensions (x and y), where one of the dimensions (y) is integrated over the half-plane, a change of variables from rectangular to polar coordinates readily produces (42) Furthermore, (42) can be obtained directly by a straightforward change of variables of a standard known integral involving Q(x), in particular, Eq (33632) in Ref 5 Both of these techniques for arriving at (42) are described in Appendix 4A Another derivation of (42) is given in Ref.

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6 and is based on the fact that since the product of two independent random variables, one of which is a Rayleigh and the other a sinusoidal random process with random phase, is a Gaussian random variable, determining the CDF of this product variable is equivalent to evaluating the Gaussian Q-function Finally, Tellambura and Annamalai [25] offer other derivations of the Craig representation in (42), some of which bear similarity to those discussed above On the basis of our previous discussion, it is clear that Q(x) of (4.

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2) is in the desired form, that is, in addition to the advantage of having nite integration limits independent of the argument of the function x, it has the further advantage that the integrand now has a Gaussian form with respect to x ! We shall see in 5 that this exponential dependence of the integrand on the argument of the Q-function will play a very important role in simplifying the evaluation of performance results for coherent communication over generalized fading channels Before exploiting this property of (42) in great detail, however, we wish to give further insight into the alternative de nition of the Gaussian Q-function with regard to how it relates to the well-known Chernoff bound Note that the maximum of the integrand in (42) occurs when = /2 [ie, the integrand achieves its maximum value, viz.

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, exp x 2 /2 at the upper limit] Thus, replacing the integrand by its maximum value, we immediately get the wellknown upper bound on Q(x), namely, Q(x) 1 exp x 2 /2 , which is the Chernoff 2 bound As we shall see on many occasions later in the book, the advantage of this observation is that the form of Q(x) in (42) allows manipulations akin to those afforded by the Chernoff bound but without the necessity of invoking a bound ! In principle, one simply operates on the integrand in the same fashion as if the Qfunction had been replaced by the Chernoff bound, and then at the end performs a single integration over the variable For example, many problems dealing with.

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