as a result of our ansatz's plus the imposition of a good large N limit and time reversal invariance. We have two evolution equations pa = Z(P0Fal, PbFba) = 1. %)/ b(gt.(eA(41-416))tin 9(.4•44.14-4‘1))ba) = Loa + Z ( n°) ti(e",-.6)),„b nb where ok, = Va. and Rafr and 'lid, satisfy the properties