Based on the correlated ground-state wave function of an exactly solvable interacting one-dimensional twoelectron model Hamiltonian we address the switch-off of confining and interparticle interactions to calculate the exact time-evolving wave function from a prescribed correlated initial state. Using this evolving wave function, the time-dependent pair probability function R(is determined via the pair density n 2 (x 1 ,x 2 ,t) and single-particle density n(x,t). It is found that R(0,0,t = ∞) = R(0,0,t = 0) > 1, and R(x 1 ,x 2 ,t * ) = 1 at a finite t * for = 0 interparticle interaction strength in the initial two-electron model. By expanding n(x,t) in an infinite sum of closed-shell products of time-dependent normalized single-particle states and time-dependent occupation numbers P k ( ,t), the von Neumann entropy S( ,t) = − ∞ k=0 P k (t)lnP k (t) is calculated as well. The such-defined information entropy is zero at t * ( ) and its maximum in time is S( ,t = ∞) = S( ,t = 0).