Many-body Aharonov-Bohm caging in a lattice of rings

TL;DR

This paper investigates many-body Aharonov-Bohm caging phenomena in a lattice of rings loaded with ultracold bosons, revealing topological band structures and caging effects even with dispersive spectra, using analytical and numerical methods.

Contribution

It introduces a tunable lattice system with engineered flux and topological properties, demonstrating many-body caging effects in a novel ring lattice setup.

Findings

Observation of topological flat bands in the system.

Demonstration of many-body Aharonov-Bohm caging effects.

Analytical and numerical validation of the phenomena.

Abstract

We study a system of a few ultracold bosons loaded into the states with orbital angular momentum $l=1$ of a one-dimensional staggered lattice of rings. Local eigenstates with winding numbers $+l$ and $-l$ form a Creutz ladder with a real dimension and a synthetic one. States with opposite winding numbers in adjacent rings are coupled through complex tunnelings, which can be tuned by modifying the central angle $\phi$ of the lattice. We analyze both the single-particle case and the few boson bound-state subspaces for the regime of strong interactions using perturbation theory, showing how the geometry of the system can be engineered to produce an effective $\pi$-flux through the plaquettes. We find non-trivial topological band structures and many-body Aharonov-Bohm caging in the $N$-particle subspaces even in the presence of a dispersive single-particle spectrum. Additionally, we study the family of models where the angle $\phi$ is introduced at an arbitrary lattice periodicity $\Gamma$. For $\Gamma>2$, the $\pi$-flux becomes non-uniform, which enlarges the spatial extent of the Aharonov-Bohm caging as the number of flat bands in the spectrum increases. All the analytical results are benchmarked through exact diagonalization.