“…The scission configurations have axially-symmetric densities that are dumbbell-shaped and can readily be divided into heavy (z < z N ) and light (z > z N ) FFs, where z N locates the minimum of the density. By adapting standard symmetry restoration techniques [41][42][43] to the case of FFs, angular momentum distributions of the heavy (F = H) and the light fragment (F = L) for each configuration |Φ(q) can be calculated as…”