“…ðE cm Þ 1=2 cosðy cm Þ ¼ ðE n Þ 1=2 cosðy lab Þ À ðE f Þ 1=2 (15) where A is the mass number of the fissioning nucleus, m f and TKE are the initial fragment mass and total kinetic energy of fission fragments, respectively. The number of neutrons n(E n ,y) with energy E n per unit energy range and solid angle, registered at angle y with respect to the direction of motion of light fragments in the laboratory coordinate system, can be written as a sum of prompt neutrons emitted from light n L (E n ,y) and heavy n H (E n ,180Ày) fragments: nðE n ; yÞ ¼ nLðE n ; yÞ þ nHðE n ; 180 À yÞ.…”