When a system thermalizes it loses all local memory of its initial conditions. This is a general feature of open systems and is well described by equilibrium statistical mechanics. Even within a closed (or reversible) quantum system, where unitary time evolution retains all information about its initial state, subsystems can still thermalize using the rest of the system as an effective heat bath. Exceptions to quantum thermalization have been predicted and observed, but typically require inherent symmetries or noninteracting particles in the presence of static disorder. The prediction of many-body localization (MBL), in which disordered quantum systems can fail to thermalize in spite of strong interactions and high excitation energy, was therefore surprising and has attracted considerable theoretical attention. Here we experimentally generate MBL states by applying an Ising Hamiltonian with long-range interactions and programmably random disorder to ten spins initialized far from equilibrium. We observe the essential signatures of MBL: memory retention of the initial state, a Poissonian distribution of energy level spacings, and entanglement growth in the system at long times. Our platform can be scaled to higher numbers of spins, where detailed modeling of MBL becomes impossible due to the complexity of representing such entangled quantum states. Moreover, the high degree of control in our experiment may guide the use of MBL states as potential quantum memories in naturally disordered quantum systems.

UR - http://arxiv.org/abs/1508.07026v1 U5 - 10.1038/nphys3783 ER - TY - JOUR T1 - Non-local propagation of correlations in long-range interacting quantum systems JF - Nature Y1 - 2014 A1 - Philip Richerme A1 - Zhe-Xuan Gong A1 - Aaron Lee A1 - Crystal Senko A1 - Jacob Smith A1 - Michael Foss-Feig A1 - Spyridon Michalakis A1 - Alexey V. Gorshkov A1 - Christopher Monroe AB - The maximum speed with which information can propagate in a quantum many-body system directly affects how quickly disparate parts of the system can become correlated and how difficult the system will be to describe numerically. For systems with only short-range interactions, Lieb and Robinson derived a constant-velocity bound that limits correlations to within a linear effective light cone. However, little is known about the propagation speed in systems with long-range interactions, since the best long-range bound is too loose to give the correct light-cone shape for any known spin model and since analytic solutions rarely exist. In this work, we experimentally determine the spatial and time-dependent correlations of a far-from-equilibrium quantum many-body system evolving under a long-range Ising- or XY-model Hamiltonian. For several different interaction ranges, we extract the shape of the light cone and measure the velocity with which correlations propagate through the system. In many cases we find increasing propagation velocities, which violate the Lieb-Robinson prediction, and in one instance cannot be explained by any existing theory. Our results demonstrate that even modestly-sized quantum simulators are well-poised for studying complicated many-body systems that are intractable to classical computation. VL - 511 U4 - 198 - 201 UR - http://arxiv.org/abs/1401.5088v1 CP - 7508 J1 - Nature U5 - 10.1038/nature13450 ER - TY - JOUR T1 - Experimental Performance of a Quantum Simulator: Optimizing Adiabatic Evolution and Identifying Many-Body Ground States JF - Physical Review A Y1 - 2013 A1 - Philip Richerme A1 - Crystal Senko A1 - Jacob Smith A1 - Aaron Lee A1 - Simcha Korenblit A1 - Christopher Monroe AB - We use local adiabatic evolution to experimentally create and determine the ground state spin ordering of a fully-connected Ising model with up to 14 spins. Local adiabatic evolution -- in which the system evolution rate is a function of the instantaneous energy gap -- is found to maximize the ground state probability compared with other adiabatic methods while only requiring knowledge of the lowest $\sim N$ of the $2^N$ Hamiltonian eigenvalues. We also demonstrate that the ground state ordering can be experimentally identified as the most probable of all possible spin configurations, even when the evolution is highly non-adiabatic. VL - 88 UR - http://arxiv.org/abs/1305.2253v1 CP - 1 J1 - Phys. Rev. A U5 - 10.1103/PhysRevA.88.012334 ER - TY - JOUR T1 - Quantum Catalysis of Magnetic Phase Transitions in a Quantum Simulator JF - Physical Review Letters Y1 - 2013 A1 - Philip Richerme A1 - Crystal Senko A1 - Simcha Korenblit A1 - Jacob Smith A1 - Aaron Lee A1 - Rajibul Islam A1 - Wesley C. Campbell A1 - Christopher Monroe AB - We control quantum fluctuations to create the ground state magnetic phases of a classical Ising model with a tunable longitudinal magnetic field using a system of 6 to 10 atomic ion spins. Due to the long-range Ising interactions, the various ground state spin configurations are separated by multiple first-order phase transitions, which in our zero temperature system cannot be driven by thermal fluctuations. We instead use a transverse magnetic field as a quantum catalyst to observe the first steps of the complete fractal devil's staircase, which emerges in the thermodynamic limit and can be mapped to a large number of many-body and energy-optimization problems. VL - 111 UR - http://arxiv.org/abs/1303.6983v2 CP - 10 J1 - Phys. Rev. Lett. U5 - 10.1103/PhysRevLett.111.100506 ER -