“…We implement the strong-coupling formalism following References [ 19 , 36 , 37 , 38 , 39 , 40 , 41 ] to arrive at the master equation describing the time evolution of the density matrix of the coupled QDs system (See Appendix A ) under Born, Markov, and the secular approximation [ 19 , 21 , 34 ]. It is important to note here that the strong coupling formalism refers to the coupling between the dots, while the system–bath coupling is still assumed to be weak so that the Born–Markov approximation can safely be implemented [ 19 , 36 , 37 , 38 , 39 , 40 , 41 ]. This implies that the Lindbladians are obtained on the basis of the eigenstates of the full system Hamiltonian .…”