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arxiv: 1610.08057 · v1 · pith:IJH4LKXU · submitted 2016-10-25 · quant-ph · cond-mat.dis-nn· cond-mat.mes-hall· cond-mat.str-el· physics.atom-ph

Observation of discrete time-crystalline order in a disordered dipolar many-body system

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classification quant-ph cond-mat.dis-nncond-mat.mes-hallcond-mat.str-elphysics.atom-ph
keywords orderdiscretedisorderedmany-bodyphasessystemstime-crystallinedipolar
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Understanding quantum dynamics away from equilibrium is an outstanding challenge in the modern physical sciences. It is well known that out-of-equilibrium systems can display a rich array of phenomena, ranging from self-organized synchronization to dynamical phase transitions. More recently, advances in the controlled manipulation of isolated many-body systems have enabled detailed studies of non-equilibrium phases in strongly interacting quantum matter. As a particularly striking example, the interplay of periodic driving, disorder, and strong interactions has recently been predicted to result in exotic "time-crystalline" phases, which spontaneously break the discrete time-translation symmetry of the underlying drive. Here, we report the experimental observation of such discrete time-crystalline order in a driven, disordered ensemble of $\sim 10^6$ dipolar spin impurities in diamond at room-temperature. We observe long-lived temporal correlations at integer multiples of the fundamental driving period, experimentally identify the phase boundary and find that the temporal order is protected by strong interactions; this order is remarkably stable against perturbations, even in the presence of slow thermalization. Our work opens the door to exploring dynamical phases of matter and controlling interacting, disordered many-body systems.

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