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堆叠方形晶格上的量子J1-J2反铁磁体:层间耦合对基态磁序的影响。

Quantum J1-J2 antiferromagnet on a stacked square lattice: influence of the interlayer coupling on the ground-state magnetic ordering.

作者信息

Schmalfuss D, Darradi R, Richter J, Schulenburg J, Ihle D

机构信息

Institut für Theoretische Physik, Universität Magdeburg, 39016 Magdeburg, Germany.

出版信息

Phys Rev Lett. 2006 Oct 13;97(15):157201. doi: 10.1103/PhysRevLett.97.157201. Epub 2006 Oct 10.

Abstract

Using the coupled-cluster method and the rotation-invariant Green's function method, we study the influence of the interlayer coupling Jperpendicular on the magnetic ordering in the ground state of the spin-1/2 J1-J2 frustrated Heisenberg antiferromagnet (J1-J2 model) on the stacked square lattice. In agreement with known results for the J1-J2 model on the strictly two-dimensional square lattice (Jperpendicular=0), we find that the phases with magnetic long-range order at small J2Jc2 are separated by a magnetically disordered (quantum paramagnetic) ground-state phase. Increasing the interlayer coupling Jperpendicular >0, the parameter region of this phase decreases, and, finally, the quantum paramagnetic phase disappears for quite small Jperpendicular approximately (0.2-0.3)J1.

摘要

利用耦合簇方法和旋转不变格林函数方法,我们研究了层间耦合(J_{\perp})对堆叠正方形晶格上自旋为(1/2)的(J_1-J_2)受挫海森堡反铁磁体((J_1-J_2)模型)基态磁有序的影响。与严格二维正方形晶格((J_{\perp}=0))上(J_1-J_2)模型的已知结果一致,我们发现,在小(J_2\lt J_{c1})和大(J_2\gt J_{c2})时具有磁长程序的相被磁无序(量子顺磁)基态相分隔。增加层间耦合(J_{\perp}\gt0),该相的参数区域减小,最终,对于相当小的(J_{\perp}\approx(0.2 - 0.3)J_1),量子顺磁相消失。

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