| Literature DB >> 30997712 |
Ping Kwan Johnny Wong1, Wen Zhang2, Fabio Bussolotti3, Xinmao Yin2, Tun Seng Herng4, Lei Zhang1,2, Yu Li Huang2, Giovanni Vinai5, Sridevi Krishnamurthi6, Danil W Bukhvalov7,8, Yu Jie Zheng2, Rebekah Chua2, Alpha T N'Diaye9, Simon A Morton9, Chao-Yao Yang10, Kui-Hon Ou Yang10, Piero Torelli5, Wei Chen1,2,11, Kuan Eng Johnson Goh2,3, Jun Ding4, Minn-Tsong Lin10, Geert Brocks6, Michel P de Jong12, Antonio H Castro Neto1,2, Andrew Thye Shen Wee1,2.
Abstract
Monolayer VSe2 , featuring both charge density wave and magnetism phenomena, represents a unique van der Waals magnet in the family of metallic 2D transition-metal dichalcogenides (2D-TMDs). Herein, by means of in situ microscopy and spectroscopic techniques, including scanning tunneling microscopy/spectroscopy, synchrotron X-ray and angle-resolved photoemission, and X-ray absorption, direct spectroscopic signatures are established, that identify the metallic 1T-phase and vanadium 3d1 electronic configuration in monolayer VSe2 grown on graphite by molecular-beam epitaxy. Element-specific X-ray magnetic circular dichroism, complemented with magnetic susceptibility measurements, further reveals monolayer VSe2 as a frustrated magnet, with its spins exhibiting subtle correlations, albeit in the absence of a long-range magnetic order down to 2 K and up to a 7 T magnetic field. This observation is attributed to the relative stability of the ferromagnetic and antiferromagnetic ground states, arising from its atomic-scale structural features, such as rotational disorders and edges. The results of this study extend the current understanding of metallic 2D-TMDs in the search for exotic low-dimensional quantum phenomena, and stimulate further theoretical and experimental studies on van der Waals monolayer magnets.Entities:
Keywords: 2D materials; monolayer magnet; spin frustration; van der Waals epitaxy; vanadium diselenide
Year: 2019 PMID: 30997712 DOI: 10.1002/adma.201901185
Source DB: PubMed Journal: Adv Mater ISSN: 0935-9648 Impact factor: 30.849