Explicit Hamiltonians Inducing Volume Law for Entanglement Entropy in Fermionic Lattices

TL;DR

This paper constructs explicit Hamiltonians for free fermions on lattices that produce ground states with volume law entanglement entropy, linking Fermi surface topology to entanglement scaling.

Contribution

It introduces explicit Hamiltonians with ground states exhibiting volume law entanglement and explores intermediate entanglement regimes in fermionic models.

Findings

Explicit Hamiltonians induce volume law entanglement.

Fractal Fermi surfaces relate to entanglement scaling.

Intermediate entanglement regimes with fractal Fermi surfaces.

Abstract

We show how the area law for the entanglement entropy may be violated by free fermions on a lattice and look for conditions leading to the emergence of a volume law. We give an explicit construction of the states with maximal entanglement entropy based on the fact that, once a bipartition of the lattice in two complementary sets $A$ and $\bar{A}$ is given, the states with maximal entanglement entropy (volume law) may be factored into Bell-pairs (BP) formed by two states with support on $A$ and $\bar{A}$. We then exhibit, for translational invariant fermionic systems on a lattice, an Hamiltonian whose ground state is such to yield an exact volume law. As expected, the corresponding Fermi surface has a fractal topology. We also provide some examples of fermionic models for which the ground state may have an entanglement entropy $S_A$ between the area and the volume law, building an explicit example of a one-dimensional free fermion model where $S_A (L) \propto L^\beta$ with $\beta$ being intermediate between $\beta = 0$ (area law) and $\beta = 1$ (BP-state inducing volume law). For this model, the dispersion relation has a "zig-zag" structure leading to a fractal Fermi surface whose counting box dimension equals, for large lattices, $\beta$. Our analysis clearly relates the violation of the area law for the entanglement entropy of the ground state to the emergence of a non-trivial topology of the Fermi surface.