Meseguer-Sánchez Jaume, Popescu Catalin, García-Muñoz José Luis, Luetkens Hubertus, Taniashvili Grigol, Navarro-Moratalla Efrén, Guguchia Zurab, Santos Elton J G
Instituto de Ciencia Molecular, Universitat de Valéncia, Paterna, Spain.
CELLS-ALBA Synchrotron Light Facility, Cerdanyola del Valles, Barcelona, 08290, Spain.
Nat Commun. 2021 Nov 1;12(1):6265. doi: 10.1038/s41467-021-26342-4.
CrI has raised as an important system to the emergent field of two-dimensional van der Waals magnetic materials. However, it is still unclear why CrI which has a ferromagnetic rhombohedral structure in bulk, changed to anti-ferromagnetic monoclinic at thin layers. Here we show that this behaviour is due to the coexistence of both monoclinic and rhombohedral crystal phases followed by three magnetic transitions at T = 61 K, T = 50 K and T = 25 K. Each transition corresponds to a certain fraction of the magnetically ordered volume as well as monoclinic and rhombohedral proportion. The different phases are continuously accessed as a function of the temperature over a broad range of magnitudes. Our findings suggest that the challenge of understanding the magnetic properties of thin layers CrI is in general a coexisting structural-phase problem mediated by the volume-wise competition between magnetic phases already present in bulk.
CrI已成为二维范德华磁性材料新兴领域的一个重要体系。然而,尚不清楚为何块状具有铁磁菱面体结构的CrI在薄层时会转变为反铁磁单斜晶结构。在此我们表明,这种行为是由于单斜晶相和菱面体晶相共存,随后在T = 61 K、T = 50 K和T = 25 K发生了三次磁转变。每次转变都对应一定比例的磁有序体积以及单斜晶相和菱面体晶相的比例。在很宽的量级范围内,不同相作为温度的函数可连续获得。我们的研究结果表明,理解薄层CrI磁性特性的挑战总体上是一个由块状中已存在的磁相之间的体积竞争介导的共存结构相问题。