Many-body localization and the area law in two dimensions
arXiv:2106.12861 · doi:10.1103/PhysRevB.106.L180201
Abstract
We study the high-energy phase diagram of a two-dimensional spin- Heisenberg model on a square lattice in the presence of either quenched or quasiperiodic disorder. The use of large-scale tensor network numerics allows us to compute the bipartite entanglement entropy for systems of up to lattice sites. We provide evidence for the existence of a many-body localized regime for large disorder strength that features an area law in excited states and that violates the eigenstate thermalization hypothesis. From a finite-size analysis, we determine an estimate for the critical disorder strength where the transition to the ergodic regime occurs in the quenched case.
6 pages, 6 figures
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- Characterizing dynamical criticality of many-body localization transitions from the Fock-space perspective
- Slowest and Fastest Information Scrambling in the Strongly Disordered XXZ Model
- Thermal avalanches in isolated many-body localized systems
- Benchmarking Quantum Simulators