The recognition that large classes of quantum many-body systems have limited - or efficiently representable - entanglement in the ground and low-lying excited states led to dramatic advances in their numerical simulation via so-called tensor networks [1-6]. However, global dynamics elevates many particles into excited states, leading to macroscopic entanglement (seen both experimentally  and theoretically [8-13]) and the failure of tensor networks. Here, we show that for quantum transport - one of the most important cases of this breakdown - the fundamental issue is the canonical basis in which the scenario is cast: When particles flow through an interface, they scatter, generating a "bit" of entanglement between spatial regions with each event. The frequency basis naturally captures that - in the long time limit and in the absence of an inelastic event - particles tend to flow from a state with one frequency to a state of identical frequency. Recognizing this natural structure yields a striking - exponential in some cases - increase in simulation efficiency, greatly extending the attainable spatial and time scales. Using this approach, we give the first mapping of the conductance diagram of the paradigmatic Anderson impurity problem. The concepts here broaden the scope of tensor network simulation into hitherto inaccessible classes of non- equilibrium many-body problems.
Physical Review Letters
Quantum transport, Tensor networks, Simulation