The evolution of weak double layers in ion‐acoustic turbulence in one and two‐dimensional particle simulations is examined. Weak double layers (e&Jgr;≲Te) evolve in simulations when a subthermal electron drift is imposed on a long or nonperiodic system withTe/Ti≫1. Their growth rate increases with the electron drift, and they decay because of ion trapping. They do not form in weakly magnetized or unmagnetized two‐dimensional (2‐D) systems unless a nonuniformity is introduced in the initial or boundary conditions. When the plasma is strongly magnetized (&ohgr;ce>&ohgr;pe), they emerge from 2‐D ion‐acoustic turbulence as coherent structures localized transversely to the magnetic field.