Abstract

Dynamics in correlated quantum matter is a hard problem, as its exact solution generally involves a computational effort that grows exponentially with the number of constituents. While a remarkable progress has been witnessed in recent years for one-dimensional systems, much less has been achieved for interacting quantum models in higher dimensions, since they incorporate an additional layer of complexity. In this work, we employ a variational method that allows for an efficient and controlled computation of the dynamics of quantum many-body systems in one and higher dimensions. The approach presented here introduces a variational class of wavefunctions based on complex networks of classical spins akin to artificial neural networks, which can be constructed in a controlled fashion. We provide a detailed prescription for such constructions and illustrate their performance by studying quantum quenches in one- and two-dimensional models. In particular, we investigate the nonequilibrium dynamics of a genuinely interacting two-dimensional lattice gauge theory, the quantum link model, for which we have recently shown -- employing the technique discussed thoroughly in this paper -- that it features disorder-free localization dynamics [P. Karpov et al., Phys. Rev. Lett. 126, 130401 (2021)]. The present work not only supplies a framework to address purely theoretical questions but also could be used to provide a theoretical description of experiments in quantum simulators, which have recently seen an increased effort targeting two-dimensional geometries. Importantly, our method can be applied to any quantum many-body system with a well-defined classical limit.

Highlights

  • One of the main challenges in quantum many-body dynamics is that unless the model under study is exactly solvable, the numerical overhead required to find an exact solution grows, in general, exponentially with the number of degrees of freedom

  • We have introduced a numerical variational scheme for the study of dynamics in correlated quantum systems in one and higher dimensions

  • Our method relies on an efficient representation of the many-body wave function, in terms of complex networks of classical spin variables

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Summary

Introduction

One of the main challenges in quantum many-body dynamics is that unless the model under study is exactly solvable, the numerical overhead required to find an exact solution grows, in general, exponentially with the number of degrees of freedom. The majority of the advances have been achieved for one-dimensional (1D) systems, for which there exist a set of reliable methods that can simulate efficiently the dynamics of lattice models. The primary example of such set of techniques is tensor network algorithms such as the time-dependent density matrix renormalization group (or its variants TEBD and tMPS) [17,18,19,20,21,22,23,24], which uses a matrix product state [25,26,27] representation of the wave function and solves the dynamics, for instance, via a Trotter

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