paper

Anisotropy-mediated reentrant localization

arXiv:2002.00013 · doi:10.21468/SciPostPhys.13.5.116

Abstract

We consider a 2d dipolar system, , with the generalized dipole-dipole interaction , and the power controlled experimentally in trapped-ion or Rydberg-atom systems via their interaction with cavity modes. We focus on the dilute dipolar excitation case when the problem can be effectively considered as single-particle with the interaction providing long-range dipolar-like hopping. We show that the spatially homogeneous tilt of the dipoles giving rise to the anisotropic dipole exchange leads to the non-trivial reentrant localization beyond the locator expansion, , unlike the models with random dipole orientation. The Anderson transitions are found to occur at the finite values of the tilt parameter , , and , , showing the robustness of the localization at small and large anisotropy values. Both extensive numerical calculations and analytical methods show power-law localized eigenstates in the bulk of the spectrum, obeying recently discovered duality of their spatial decay rate, on the localized side of the transition, . This localization emerges due to the presence of the ergodic extended states at either spectral edge, which constitute a zero fraction of states in the thermodynamic limit, decaying though extremely slowly with the system size.

21 pages, 11 figures, 75 references (in 5.5 pages) + 2 pages, 2 figures in Appendices

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