“…We then find the transform-space expression dσ bg→tW (N ) =φ(N 1 )φ(N 2 ) dσ bg→tW (N ) , (2.2) where N 1 = N (m 2 W − u)/s and N 2 = N (m 2 W − t)/s. The cross section for tW production can be rewritten under Laplace transforms in refactorized form as a product of separate functions: a short-distance, infrared safe, hard function, H bg→tW ; a soft function, S bg→tW , which describes the emission of noncollinear soft gluons in the process; and functions ψ that describe collinear emission from the incoming partons [15,16,25,[28][29][30][31][32][33][34]. We have…”