Universality of mean-field antiferromagnetic order in an anisotropic 3D Hubbard model at half-filling
E. Langmann, J. Lenells
TL;DR
The paper analyzes the universality of mean-field antiferromagnetic order in the anisotropic 3D Hubbard model at half-filling, focusing on how the interlayer hopping $t_z$ governs the density of states and the Néel temperature. Using Hartree--Fock theory and all-order density-of-states expansions, the authors derive precise small-$U$ asymptotics for $T_N$ and the AF gap, and show that the gap ratio $\hat{m}$ adheres to a universal BCS-like function $f_{BCS}$ for any $t_z>0$, while universality breaks down in the strictly 2D limit $t_z\to0$ with a distinct $\sqrt{U}$ correction. They also establish all-orders expansions for $N_0(\varepsilon)$ and $N_{t_z}(\varepsilon)$, analyze the $t_z\to0$ behavior of $N_{t_z}(0)$, and provide an exponentially small subleading term refinement for the mean-field description. The results clarify which universal features persist when moving from 3D to quasi-2D Hubbard systems and quantify the singular nature of the $t_z\to0$ limit, offering insight for modeling layered materials and cold-atom realizations.
Abstract
We study the 3D anisotropic Hubbard model on a cubic lattice with hopping parameter $t$ in the $x$- and $y$-directions and a possibly different hopping parameter $t_z$ in the $z$-direction; this model interpolates between the 2D and 3D Hubbard models corresponding to the limiting cases $t_z=0$ and $t_z=t$, respectively. We first derive all-order asymptotic expansions for the density of states. Using these expansions and units such that $t=1$, we analyze how the Néel temperature and the antiferromagnetic mean field depend on the coupling parameter, $U$, and on the hopping parameter $t_z$. We derive asymptotic formulas valid in the weak coupling regime, and we study in particular the transition from the three-dimensional to the two-dimensional model as $t_z \to 0$. It is found that the asymptotic formulas are qualitatively different for $t_z = 0$ (the two-dimensional case) and $t_z > 0$ (the case of nonzero hopping in the $z$-direction). Our results show that certain universality features of the three-dimensional Hubbard model are lost in the limit $t_z \to 0$ in which the three-dimensional model reduces to the two-dimensional model.
