Abstract
CrI(3) 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(3) 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(C1) = 61 K, T(C2) = 50 K and T(C3) = 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(3) is in general a coexisting structural-phase problem mediated by the volume-wise competition between magnetic phases already present in bulk.