We investigate the ac electric field induced quantum anomalous Hall effect in honeycomb lattices and derive the full phase diagram for arbitrary field amplitude and phase polarization. We show how to induce antichiral edge modes as well as topological phases characterized by a Chern number larger than 1 by means of suitable drivings. In particular, we find that the Chern number develops plateaus as a function of the frequency, providing a time-dependent analog to the ones in the quantum Hall effect. Introduction. The realization of different topological states of matter is one of the major challenges for both fundamental reasons and technological perspectives. Several of these states have been originally predicted in the honeycomb lattice, whose Dirac-like band structure brings the system at a critical point of a topological phase transition. There, the development of gaps by different mechanisms results in a variety of topological phases [1,2]. In this line, the quantum spin Hall phase was first obtained in HgTe quantum wells [3,4], where the topological phase transition was controlled by the thickness of the quantum well. Likewise, the quantum anomalous Hall effect (QAHE)-for which time-reversal symmetry (TRS) is broken in the absence of a magnetic field-was originally proposed by Haldane in the honeycomb lattice [1]. However, despite the success of the theoretical model, it has been very difficult to achieve experimentally, until very recently in doped topological insulators [5].Simultaneously, different techniques have been proposed to externally control the topological properties of a system. One of the most promising consists in periodically driving the system in order to achieve a topological phase transition [6][7][8][9][10][11]. Proposals with a time periodic driving in semiconductors [6,12], optical lattices [13], or graphene [7,[14][15][16][17][18] have been suggested to achieve various dynamical generalizations of static topological phases, called Floquet topological phases [12], and have been recently observed in photonic crystals [19]. Importantly for our purposes, the previous studies for the honeycomb lattice were restricted either to numerical calculations in finite-size systems, where the physical mechanism driving the topological phase transitions was not clear, or to very high frequencies and low-energy approximations, where most of the phase diagram remained unknown.In the present work, we derive the full phase diagram of periodically driven honeycomb lattices in the QAHE regime, by explicitly calculating the Chern number of the Floquet bands. Our model is valid for arbitrary field frequency, amplitude, and polarization and therefore goes beyond the single Dirac cone description and the rotating wave approximation. Surprisingly, we find that a clockwise driving may also lead to counterclockwise (or antichiral) edge states, and demonstrate that their appearance is linked to two distinct band inversion mechanisms. Moreover, we show how to induce topological phases with Chern numbers larger tha...