We present an exact solution of the one-dimensional random field Ising mode
l (RFIM) with synchronous rather than sequential spin-dynamics, whose equil
ibrium state is characterized by a temperature-dependent pseudo-Hamiltonian
, based upon a suitable adaptation of the techniques originally developed f
or the sequential (Glauber) dynamics RFIM. Although deriving the solution i
s somewhat more involved in the present model than in the case of the seque
ntial RFIM, we are able to prove rigorously that the physics of the two RFI
M versions are asymptotically identical. We thus recover the familiar devil
's staircase form for the integrated density of local magnetizations, and f
ind a non-zero ground state entropy with an infinite number of singularitie
s as a function of the random field strength.