“…First, specializing to the systems of type I, II, and VI, the repulsive character of the interparticle potentials j(xj -Xk) and fr(xj -xk), respectively, can be exploited to prove that the 8 1 dynamics leads to soliton scattering. Specifically, Moser's argument can be adapted to the 8 1 flow [3], yielding here (3.22) and, once more, (2.43). Therefore, the functions sk: t i---> Sk ( x(t), p(t)) reduce to symmetric functions of matrices L± = diag ( exp(f3pt), ... , exp(f3pt)) for t -> ±oo.…”