“…[1], however, a difFerent form was used for the two-particle inclusive distribution, namely, p~[ki, kg) = pi(ki)pg(k, ) + J d x, d'z, m(z, , k, ) w(2, , k, ) cos(ST"Sk"). (4) The form (4) was also derived in Ref. [7] as an approximation to the complete, nonanalytic result.…”