“…The methodology used herein is, in many aspects, very similar to that utilized in the previous works of Croft et al 24,25 and Morita et al 26,27 except that reactive channels are also taken into consideration as a collision-induced outcome. Thus, upon a H + D 2 (υ, j) reactive collision (or likewise D + HD), the probability of detecting a scattered HD(υ , j ) product (or D 2 ) by a detector placed at Ω = (θ, φ), at a given collision en-ergy E coll , is governed by the state-to-state scattering amplitude 33 f J nn (θ, E coll ), i.e.…”