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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.

Universality of mean-field antiferromagnetic order in an anisotropic 3D Hubbard model at half-filling

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 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- asymptotics for and the AF gap, and show that the gap ratio adheres to a universal BCS-like function for any , while universality breaks down in the strictly 2D limit with a distinct correction. They also establish all-orders expansions for and , analyze the behavior of , 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 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 in the - and -directions and a possibly different hopping parameter in the -direction; this model interpolates between the 2D and 3D Hubbard models corresponding to the limiting cases and , respectively. We first derive all-order asymptotic expansions for the density of states. Using these expansions and units such that , we analyze how the Néel temperature and the antiferromagnetic mean field depend on the coupling parameter, , and on the hopping parameter . 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 . It is found that the asymptotic formulas are qualitatively different for (the two-dimensional case) and (the case of nonzero hopping in the -direction). Our results show that certain universality features of the three-dimensional Hubbard model are lost in the limit in which the three-dimensional model reduces to the two-dimensional model.
Paper Structure (33 sections, 29 theorems, 239 equations, 9 figures)

This paper contains 33 sections, 29 theorems, 239 equations, 9 figures.

Key Result

Theorem 2.1

The two-dimensional density of states $N_0(\epsilon)$ given by (2Ddensityofstates) obeys the following asymptotic expansion to all orders as $\epsilon \downarrow 0$: The functions $A_{k,l}$ in (N0expansion) are defined in terms of the Gamma function $\Gamma(z)$ and the digamma function $\psi(z) = \frac{\Gamma'(z)}{\Gamma(z)}$ by where the principal branch is used for the logarithms. In particula

Figures (9)

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  • ...and 4 more figures

Theorems & Definitions (54)

  • Theorem 2.1: Behavior of $N_0(\epsilon)$ as $\epsilon \to 0$
  • Theorem 2.2: Behavior of $N_{t_z}(\epsilon)$ as $\epsilon \to 0$ for $t_z > 0$
  • Theorem 2.3: Behavior of $N_{t_z}(0)$ as $t_z \to 0$
  • Theorem 2.4: Small $U$ behavior of the 2D Néel temperature
  • proof
  • Theorem 2.5: Small $U$ behavior of the 3D Néel temperature
  • proof
  • Theorem 2.6: Small $U$ behavior of 2D mean field
  • proof
  • Theorem 2.7: Small $U$ behavior of 3D mean field
  • ...and 44 more