4.8 Article

Disorder-Free Localization in an Interacting 2D Lattice Gauge Theory

Journal

PHYSICAL REVIEW LETTERS
Volume 126, Issue 13, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.126.130401

Keywords

-

Funding

  1. Alexander von Humboldt Foundation
  2. Ministry of Science and Higher Education of the Russian Federation (NUST MISiS) [K2-2020-038]
  3. European Research Council (ERC) under the European Union [853443]
  4. Deutsche Forschungsgemeinschaft via the Gottfried Wilhelm Leibniz Prize program
  5. European Union's Horizon 2020 research and innovation programme under the Marie Sklodowska-Curie Grant [701647]
  6. Leopoldina Fellowship Programme of the German National Academy of Sciences Leopoldina [LPDS 2018-07]
  7. Simons Foundation
  8. European Research Council (ERC) [853443] Funding Source: European Research Council (ERC)

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The concept of disorder-free localization as a mechanism for ergodicity breaking in low-dimensional homogeneous lattice gauge theories is introduced in this study. Surprisingly, nonergodic behavior can also be observed in genuinely interacting systems in two spatial dimensions due to this mechanism. Furthermore, the study shows that the gauge invariance can act as an alternative robust localization mechanism surviving in higher dimensions in the presence of interactions.
Disorder-free localization has been recently introduced as a mechanism for ergodicity breaking in low-dimensional homogeneous lattice gauge theories caused by local constraints imposed by gauge invariance. We show that also genuinely interacting systems in two spatial dimensions can become nonergodic as a consequence of this mechanism. This result is all the more surprising since the conventional many-body localization is conjectured to be unstable in two dimensions; hence the gauge invariance represents an alternative robust localization mechanism surviving in higher dimensions in the presence of interactions. Specifically, we demonstrate nonergodic behavior in the quantum link model by obtaining a bound on the localization-delocalization transition through a classical correlated percolation problem implying a fragmentation of Hilbert space on the nonergodic side of the transition. We study the quantum dynamics in this system by introducing the method of variational classical networks, an efficient and perturbatively controlled representation of the wave function in terms of a network of classical spins akin to artificial neural networks. We identify a distinguishing dynamical signature by studying the propagation of line defects, yielding different light cone structures in the localized and ergodic phases, respectively. The methods we introduce in this work can be applied to any lattice gauge theory with finite-dimensional local Hilbert spaces irrespective of spatial dimensionality.

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