Certain two-dimensional (2D) materials exhibit intriguing properties such as valley polarization 1 , ferroelectricity 2 , superconductivity 3 and charge-density waves 4,5 . Many of these materials can be manually assembled into atomic-scale multilayer devices 6,7 under ambient conditions, owing to their exceptional chemical stability. Efforts have been made to add a magnetic degree of freedom to these 2D materials via defects, but only local magnetism has been achieved 8-10 . Only with the recent discoveries of 2D materials supporting intrinsic ferromagnetism have stacked spintronic devices become realistic 11-15 . Assembling 2D multilayer devices with these ferromagnets under ambient conditions remains challenging due to their sensitivity to environmental degradation, and magnetic order at room temperature is rare in van der Waals materials. Here, we report the growth of air-stable ultra-thin epsilon-phase iron oxide crystals that exhibit magnetic order at room temperature. These crystals require no passivation and can be prepared in large quantity by cost-effective chemical vapor deposition (CVD). We find that the epsilon phase, which is energetically unfavorable and does not form in bulk, can be easily made in 2D down to a seven unit-cell thickness. Magneto-optical Kerr effect (MOKE) magnetometry of individual crystals shows that even at this ultrathin limit the epsilon phase exhibits robust magnetism with coercive fields of hundreds of mT. These measurements highlight the advantages of ultrathin iron oxide as a promising candidate towards air-stable 2D magnetism and integration into 2D spintronic devices.Iron oxides are abundant in nature and are present in almost every domain on earth, including the atmosphere, biosphere and lithosphere. 16 They are also among the most studied metal oxides, having been applied exhaustively for technological applications such as data storage and catalysis, and biomedical applications such as drug delivery, medical imaging, and cancer treatment. 16 The most common polymorphs of iron oxide are -Fe2O3 (hematitie), -Fe2O3 (maghemite), and Fe3O4 (magnetite), which exist in both bulk and nanoscale forms. In contrast, -Fe2O3 is a rare phase with little natural existence and has only been found at the nanoscale. 17 It has received far less research interest than the other polymorphs, due partially to its difficulty in preparation, as it cannot be grown in bulk. However, -Fe2O3 has a variety of interesting characteristics, such as ferrimagnetism, multiferroicity 18 , and a large coercive field 19 , motivating investigation into growth techniques and properties. Figure 1Phase identification by Raman spectroscopy. 22 out of 23 thin crystal samples measured on the same substrate are phase. Only the thickest is −Fe 2 O 3 , suggesting that Fe2O3 preferentially forms into a stable phase in 2D, unlike in bulk.
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