ON A DYNAMIC THEORY OF QUENCHED RANDOM SYSTEM

A dynamical theory for quenched random system is developed in the framework of CTPGF. In steady states the results obtained coincide with those following from the quenched average of the free energy. The order parameter q, a matrix in general, becomes an integral part of the second order connected CTPGF. An equation to determine q is derived from the Dyson-Schwinger equation in this formalism. Some general properties of the CTPGF in a quenched random system are discussed.