“…In terms of the vectors p 1 ± p 2 and the symmetrized (gerade and ungerade) amplitudes a g,u [1,8,19]; note that f ͑g,u͒ =2a g,u .] The parametrization of our symmetrized amplitudes in terms of Legendre polynomials and reduced matrix elements follows immediately from that for the functions f͑p , pЈ , cos ͒ [7] and g͑p , pЈ , cos ͒, g s ͑p , pЈ , cos ͒ [18].…”