We consider continuous and discrete Schrödinger systems with selfadjoint matrix potentials and with additional dependence on time (i.e., dynamical Schrödinger systems). Transformed and explicit solutions are constructed using our generalized (GBDT) version of the Bäcklund-Darboux transformation. Asymptotic expansions of these solutions in time are of interest.The dependence of our solutions of (1.1) and (1.2) on time is described by the factor e itA , where A is a parameter matrix (generalized eigenvalue) of the GBDT transformation. Since A is not necessarily self-adjoint and may have Jordan cells of different orders, the asymptotic expansion of our solutions of (1.1) and (1.2) essentially differs (see Remark 3.4) from the classical Jensen-Kato formulas (see [15] as well as further references in [7,8]).As usual, R denotes the set of real values, N is the set of natural numbers, and the complex plane is denoted by C. Notation S * stands for the matrix which is the conjugate transpose of S, we write S > 0 when S is a positivedefinite matrix, and I m stands for the m × m identity matrix. The notation J = diag{J 1 , J 2 , . . .} means that J is a diagonal or block diagonal matrix with the entries (or block entries) J 1 , J 2 and so on.