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突破二维范德华磁体中的默明-瓦格纳极限。

Breaking through the Mermin-Wagner limit in 2D van der Waals magnets.

作者信息

Jenkins Sarah, Rózsa Levente, Atxitia Unai, Evans Richard F L, Novoselov Kostya S, Santos Elton J G

机构信息

Department of Physics, University of York, York, YO10 5DD, UK.

TWIST Group, Institut für Physik, Johannes Gutenberg Universität, 55128, Mainz, Germany.

出版信息

Nat Commun. 2022 Nov 14;13(1):6917. doi: 10.1038/s41467-022-34389-0.

Abstract

The Mermin-Wagner theorem states that long-range magnetic order does not exist in one- (1D) or two-dimensional (2D) isotropic magnets with short-ranged interactions. Here we show that in finite-size 2D van der Waals magnets typically found in lab setups (within millimetres), short-range interactions can be large enough to allow the stabilisation of magnetic order at finite temperatures without any magnetic anisotropy. We demonstrate that magnetic ordering can be created in 2D flakes independent of the lattice symmetry due to the intrinsic nature of the spin exchange interactions and finite-size effects. Surprisingly we find that the crossover temperature, where the intrinsic magnetisation changes from superparamagnetic to a completely disordered paramagnetic regime, is weakly dependent on the system length, requiring giant sizes (e.g., of the order of the observable universe ~ 10 m) to observe the vanishing of the magnetic order as expected from the Mermin-Wagner theorem. Our findings indicate exchange interactions as the main ingredient for 2D magnetism.

摘要

默明-瓦格纳定理指出,在具有短程相互作用的一维(1D)或二维(2D)各向同性磁体中不存在长程磁有序。在此我们表明,在实验室装置中常见的有限尺寸二维范德华磁体(毫米范围内),短程相互作用可以足够大,从而在没有任何磁各向异性的情况下,允许在有限温度下稳定磁有序。我们证明,由于自旋交换相互作用的内在性质和有限尺寸效应,二维薄片中可以产生与晶格对称性无关的磁有序。令人惊讶的是,我们发现本征磁化强度从超顺磁转变为完全无序顺磁状态的转变温度对系统长度的依赖性较弱,需要极大的尺寸(例如,可观测宇宙量级~10米)才能观察到如默明-瓦格纳定理所预期的磁有序消失。我们的研究结果表明,交换相互作用是二维磁性的主要因素。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a454/9663506/102d4d37403e/41467_2022_34389_Fig1_HTML.jpg

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