{ "id": "1607.01285", "version": "v1", "published": "2016-07-05T14:54:38.000Z", "updated": "2016-07-05T14:54:38.000Z", "title": "Detecting a many-body mobility edge with quantum quenches", "authors": [ "Piero Naldesi", "Elisa Ercolessi", "Tommaso Roscilde" ], "categories": [ "cond-mat.dis-nn", "cond-mat.str-el", "quant-ph" ], "abstract": "The many-body localization (MBL) transition is a quantum phase transition involving highly excited eigenstates of a disordered quantum many-body Hamiltonian, which evolve from \"extended/ergodic\" (exhibiting extensive entanglement entropies and fluctuations) to \"localized\" (exhibiting area-law scaling of entanglement and fluctuations). The MBL transition can be driven by the strength of disorder in a given spectral range, or by the energy density at fixed disorder - if the system possesses a many-body mobility edge. Here we propose to explore the latter mechanism by using \"quantum-quench spectroscopy\", namely via quantum quenches of variable width which prepare the state of the system in a superposition of eigenstates of the Hamiltonian within a controllable spectral region. Studying numerically a chain of interacting spinless fermions in a quasi-periodic potential, we argue that this system has a many-body mobility edge; and we show that its existence translates into a clear dynamical transition in the time evolution immediately following a quench in the strength of the quasi-periodic potential, as well as a transition in the scaling properties of the quasi-stationary state at long times. Our results suggest a practical scheme for the experimental observation of many-body mobility edges using cold-atom setups.", "revisions": [ { "version": "v1", "updated": "2016-07-05T14:54:38.000Z" } ], "analyses": { "keywords": [ "many-body mobility edge", "quantum quenches", "quasi-periodic potential", "quantum phase transition", "disordered quantum many-body hamiltonian" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }