We consider an open system near a quantum critical point that is suddenly moved towards the critical point. The bath-dominated diffusive non-equilibrium dynamics after the quench is shown to follow scaling behavior, governed by a critical exponent that emerges in addition to the known equilibrium critical exponents. We determine this exponent and show that it describes universal prethermalized coarsening dynamics of the order parameter in an intermediate time regime. Implications of this quantum critical prethermalization are a powerlaw rise of order and correlations after an initial collapse of the equilibrium state and a crossover to thermalization that occurs arbitrarily late for sufficiently shallow quenches.Predicting the out-of-equilibrium dynamics of quantum many-body systems is a challenge of fundamental and practical importance. This research area has been boosted by recent experiments in cold-atom gases [1] and scaled-up quantum-circuits [2], by ultra-fast pump-probe measurements in correlated materials [3][4][5], and by performing heavy-ion collisions that explore the quark-gluon plasma [6]. In this context, the universality near a quantum critical point (QCP), well established in and near equilibrium, comes with the potential to make quantitative predictions for strongly interacting systems far from equilibrium. For example, the quantum version [7][8][9][10][11] of the Kibble-Zurek mechanism of defect formation [12,13] was developed for systems driven through a symmetry breaking QCP at a small, but finite rate. Similarly, near a QCP the long-time dynamics after a sudden change of Hamiltonian parameters, is governed by equilibrium exponents [14]. These phenomena occur in the regime of longest time scales.Recently, however, many physical systems away from equilibrium were identified which display novel dynamical behavior on intermediate time scales, a behavior often referred to as prethermalization [15][16][17][18][19][20][21][22][23][24][25]. The question arises whether one can expect universality during prethermalization if one drives a system towards a QCP. Even if this is done at a finite rate 1/τ , a system will fall out of equilibrium at some point, a behavior owed to the critical slowing down near the QCP. Then a scaling theory with characteristic time scale τ can be developed [10], where regions of the size of the freeze-out length ∝ τ 1/z emerge that behave like in equilibrium. z is the dynamic critical exponent. In case of a quantum quench, the time scale τ and the freeze-out length become comparable to microscopic time and length scales, respectively and the system instantly falls out of equilibrium. The detailed recovery of this out-of-equilibrium dynamics, along with the time dependence of length scales, order-parameter correlations, and the potential for outof-equilibrium universality are major theoretical and experimental challenges.In this Letter, we show that the time evolution of observables in an open system that is suddenly moved to a QCP displays universal behavior (see Fig. 1(a-b)...