Many-body localization

The common intuition says that generic isolated quantum systems even when prepared in a strongly non-equilibrium settings quickly reach the thermal equilibrium (thermalize). The only known exceptions are non-interacting systems, Bethe-ansatz integrable systems in one spatial dimension, and many-body localization.

The many-body localized phase is the localized phase with interactions. The breakdown of thermalization in the many-body localized phase can be understood from the emergent quasi-local integrals of motion. In our research we aim to better understand the properties of the many-body localized phase. In addition, we are interested in better understanding the delocalization transition, as it may provide valuable insights into possible mechanisms of thermalization and its breakdown.

Below we provide some examples of recent results in this direction.

Probing dynamics by matrix elements

In order to determine generic non-equilibrium dynamics of the generic local observable O one needs two ingredients. The spectrum of the many-body Hamiltonian and the matrix elements of the operator O in the basis of eigenstates completely specify evolution of the local observable O. Moreover, the matrix elements at small energy differences correspond to the long-time dynamics that may be very hard to access in the thermalizing system.

Using these insights, we studied the properties of the matrix elements across the many-body localization transition in the recent preprint arXiv:1610.02389. In particular, we used matrix elements to define the (many-body) Thouless energy ETh which corresponds to the inverse time scale of relaxation. The behavior of this Thouless energy reveals the critical fan preceding localization transition. In addition, we associate the critical region with the onset of broad distributions and typicality breakdown.