In this work we report on a new mechanism to generate dissipative steady state entanglement in two coupled qubits driven by strong periodic ac fields. We show that steady entanglement can be generated at one side of a multiphoton resonance between a non-entangled ground state and an entangled excited state. The degree of entanglement can be tuned as a function of the amplitude of the periodic drive. A rich dynamic behavior with creation, death and revival of entanglement can be observed for certain parameter regimes, accessible in current experimental devices.The generation and stabilization of entanglement is one of the main challenges in quantum information applications. In recent years strategies based on the creation of steady state entanglement through engineered dissipation have been discussed theoretically [1-3] and demonstrated in experiments [4][5][6][7][8][9][10]. In this scheme, the system of interest is driven by external fields and coupled to a reservoir, developing a nontrivial non-equilibrium dynamics that leads to a highly entangled steady state. The effective relaxation rates can be tuned by adequately designing the quantum reservoir, the system-reservoir couplings or the driving protocols. Experimental demonstrations include realizations with trapped ions [4-6], atomic ensembles [7], and superconducting qubits [8][9][10]. Another strategy for entanglement stabilization are measurement based protocols, which have been implemented, for example, in coupled superconducting qubits [11][12][13][14][15].The different proposed mechanisms for driven dissipative entanglement generation utilize weak resonant drivings to tailor the relaxation processes [1-10]. However, for large amplitude periodic drivings, interesting non perturbative effects are known to exist. Among these, coherent destruction of tunneling [16][17][18], Landau-Zener-Stückelberg (LZS) interferometry [19][20][21][22][23][24][25][26][27][28] and bathmediated population inversion [11,[29][30][31] have been studied in two-level systems.Relying on these later effects, we present a new mechanism to induce steady state entanglement. Using as a test system two coupled qubits, we will demonstrate that the entanglement in the steady state can be induced and tuned by changing the amplitude of a driving periodic field. One of our main results is advanced in Fig.1(a) where we show how the concurrence (a measure of entanglement) can be increased or decreased as a function of the amplitude of the periodic driving.In this work we consider two coupled qubits with HamiltonianĤ s (t) =Ĥ 0 +V (t), wherê+ with σ (i) z,x,+,− the Pauli matrices in the Hilbert space of FIG. 1. (a) Plots of the steady state concurrence, C∞, as function of the driving amplitude A/ω for 0/ω = 3 (green line) and 0/ω = 4.1 (black line). (b) Colour map of C∞ versus A/ω and 0/ω. (c) Eigenenergies Ei of the system Hamiltonian H0 as a function of 0/ω. Along this work, we choose ∆2/∆1 = 1.5 , J/∆1 = −25 and ω/∆1 = 10. The bath temperature is taken as T b /∆1 = 0.0467 and for the bath spec...