# Entanglement and fluctuations in the XXZ model with power-law interactions

## TL;DR

This paper explores how long-range power-law interactions in the XXZ model affect its ground-state properties, revealing three regimes with distinct behaviors and a continuously varying dynamical exponent that influences correlations and entanglement.

## Contribution

It identifies and characterizes three distinct interaction regimes in the long-range XXZ model, including a novel medium-range regime with a tunable dynamical exponent.

## Key findings

- Existence of three regimes depending on decay exponent and dimension
- In the medium-range regime, the dynamical exponent varies continuously
- Long-range interactions significantly alter correlation and entanglement scaling

## Abstract

We investigate the ground-state properties of the XXZ model with $1/r^{\alpha}$ interactions, describing spins interacting with long-range (LR) transverse (XX) ferromagnetic interactions and longitudinal (Z) antiferromagnetic interactions, or hardcore bosons with LR repulsion and hopping. The LR nature of the couplings allows us to quantitatively study the spectral, correlation and entanglement properties of the system by making use of linear spin-wave theory, supplemented with density-matrix renormalization group in one-dimensional systems. Our most important prediction is the existence of three distinct coupling regimes, depending on the decay exponent $\alpha$ and number of dimensions $d$: 1) a short-range regime for $\alpha > d + \sigma_c$ (where $\sigma_c = 1$ in the gapped N\'eel antiferromagnetic phase exhibited by the XXZ model, and $\sigma_c = 2$ in the gapless XY ferromagnetic phase), sharing the same properties as those of finite-range interactions ($\alpha=\infty$); 2) a long-range regime $\alpha < d$, sharing the same properties as those of the infinite-range interactions ($\alpha=0$) in the thermodynamic limit; and 3) a most intriguing medium-range regime for $d < \alpha < d+\sigma_c$, continuously interpolating between the finite-range and the infinite-range behavior. The latter regime is characterized by elementary excitations with a long-wavelength dispersion relation $\omega \approx \Delta_g + ck^z$ in the gapped phase, and $\omega \sim k^z$ in the gapless phase, exhibiting a continuously varying dynamical exponent $z = (\alpha - d) / \sigma_c$. In the gapless phase of the model the $z$ exponent is found to control the scaling of fluctuations, the decay of correlations, and a universal sub-dominant term in the entanglement entropy, leading to a very rich palette of behaviors for ground-state quantum correlations beyond what is known for finite-range interactions.