Effect of anisotropy on the ground-state magnetic ordering of the spin-half quantum $J_1^{XXZ}$--$J_2^{XXZ}$ model on the square lattice

TL;DR

This study investigates how anisotropy influences the ground-state magnetic phases of the 2D quantum $J_1^{XXZ}$--$J_2^{XXZ}$ model on a square lattice, revealing quantum triple points and an intermediate disordered phase.

Contribution

The paper provides a high-order coupled cluster analysis of the anisotropic $J_1$-$J_2$ model, identifying quantum triple points and the emergence of a disordered phase between classical magnetic states.

Findings

Identification of two quantum triple points at specific anisotropy and frustration ratios.

Existence of an intermediate magnetically-disordered phase separating N{é}el and stripe phases.

Confirmation of classical phase transition behaviors at high anisotropy values.

Abstract

We study the zero-temperature phase diagram of the 2D quantum $J_{1}^{XXZ}$--$J_{2}^{XXZ}$ spin-1/2 anisotropic Heisenberg model on the square lattice. In particular, the effects of the anisotropy $\Delta$ on the $z$-aligned N\'{e}el and (collinear) stripe states, as well as on the $xy$-planar-aligned N\'{e}el and collinear stripe states, are examined. All four of these quasiclassical states are chosen in turn as model states on top of which we systematically include the quantum correlations using a coupled cluster method analysis carried out to very high orders. We find strong evidence for two {\it quantum triple points} (QTP's) at ($\Delta ^{c} = -0.10 \pm 0.15, J_{2}^{c}/J_{1} = 0.505 \pm 0.015$) and ($\Delta ^{c} = 2.05 \pm 0.15, J_{2}^{c}/J_{1} = 0.530 \pm 0.015$), between which an intermediate magnetically-disordered phase emerges to separate the quasiclassical N\'{e}el and stripe collinear phases. Above the upper QTP ($\Delta \gtrsim 2.0$) we find a direct first-order phase transition between the N\'{e}el and stripe phases, exactly as for the classical case. The $z$-aligned and $xy$-planar-aligned phases meet precisely at $\Delta = 1$, also as for the classical case. For all values of the anisotropy parameter between those of the two QTP's there exists a narrow range of values of $J_{2}/J_{1}$, $\alpha^{c_1}(\Delta)<J_{2}/J_{1} <\alpha^{c_2}(\Delta)$, centered near the point of maximum classical frustration, $J_{2}/J_{1} = {1/2}$, for which the intermediate phase exists. This range is widest precisely at the isotropic point, $\Delta = 1$, where $\alpha^{c_1}(1) = 0.44 \pm 0.01$ and $\alpha^{c_2}(1) = 0.59 \pm 0.01$. The two QTP's are characterized by values $\Delta = \Delta^{c}$ at which $\alpha^{c_1}(\Delta^{c})=\alpha^{c_2}(\Delta^{c})$.