Anisotropy-mediated reentrant localization

TL;DR

This paper investigates how anisotropic dipole interactions in a 2D system cause reentrant localization phenomena, with localization transitions driven by the tilt parameter, supported by numerical and analytical evidence of power-law localized states.

Contribution

It reveals the role of dipole anisotropy in inducing reentrant localization and identifies specific transition points, expanding understanding of long-range interacting disordered systems.

Findings

Localization transitions occur at specific tilt values related to the interaction power

Power-law localized eigenstates obey a duality in their decay rates

Localized states coexist with ergodic extended states at spectral edges

Abstract

We consider a 2d dipolar system, $d=2$, with the generalized dipole-dipole interaction $\sim r^{-a}$, and the power $a$ 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 $\beta$ of the dipoles giving rise to the anisotropic dipole exchange leads to the non-trivial reentrant localization beyond the locator expansion, $a<d$, unlike the models with random dipole orientation. The Anderson transitions are found to occur at the finite values of the tilt parameter $\beta = a$, $0<a<d$, and $\beta = a/(a-d/2)$, $d/2<a<d$, 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 $a\leftrightarrow 2d-a$ of their spatial decay rate, on the localized side of the transition, $a>a_{AT}$. 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.