TY - JOUR
T1 - Magnetic imaging and domain nucleation in CrSBr down to the 2D limit
AU - Zur, Yishay
AU - Noah, Avia
AU - Boix-Constant, Carla
AU - Mañas-Valero, Samuel
AU - Fridman, Nofar
AU - Rama-Eiroa, Ricardo
AU - Huber, Martin E.
AU - Santos, Elton J. G.
AU - Coronado, Eugenio
AU - Anahory, Yonathan
N1 - Funding Information:
This work was supported by the European Research Council (ERC) grant No. 802952 and the Israel Science Foundation (ISF) Grant No. 645/23. The international collaboration in this work was fostered by the EU‐COST Action CA21144. C.B.‐C., S.M.‐V., and E.C. acknowledge financial support from the European Union (ERC AdG Mol‐2D 788222 and FET OPEN SINFONIA 964396), the Spanish MCIN (2D‐HETEROS PID2020‐117152RB‐100, cofinanced by FEDER, the Excellence Unit “María de Maeztu” CEX2019‐000919‐M), the Generalitat Valenciana (PROMETEO Program, and the PO FEDER Program IDIFEDER/2018/061), as well as the Advanced Materials program (supported by MCIN, with funding from the European Union NextGenerationEU (PRTR‐C17.I1) and Generalitat Valenciana). E.J.G.S. acknowledges computational resources through CIRRUS Tier‐2 HPC Service (ec131 Cirrus Project) at EPCC ( http://www.cirrus.ac.uk ) funded by the University of Edinburgh and EPSRC (EP/P020267/1); ARCHER2 UK National Supercomputing Service via Project d429. E.J.G.S. acknowledges the EPSRC Open Fellowship (EP/T021578/1), and the Edinburgh‐Rice Strategic Collaboration Awards for funding support. The authors would like to thank Amir Capua for fruitful discussions. The authors thank Atzmon Vakahi and Sergei Remennik for technical support. R.R.‐E. would like to thank Sarah Jenkins for technical support on the simulations and helpful discussions.
Funding Information:
This work was supported by the European Research Council (ERC) grant No. 802952 and the Israel Science Foundation (ISF) Grant No. 645/23. The international collaboration in this work was fostered by the EU-COST Action CA21144. C.B.-C., S.M.-V., and E.C. acknowledge financial support from the European Union (ERC AdG Mol-2D 788222 and FET OPEN SINFONIA 964396), the Spanish MCIN (2D-HETEROS PID2020-117152RB-100, cofinanced by FEDER, the Excellence Unit “María de Maeztu” CEX2019-000919-M), the Generalitat Valenciana (PROMETEO Program, and the PO FEDER Program IDIFEDER/2018/061), as well as the Advanced Materials program (supported by MCIN, with funding from the European Union NextGenerationEU (PRTR-C17.I1) and Generalitat Valenciana). E.J.G.S. acknowledges computational resources through CIRRUS Tier-2 HPC Service (ec131 Cirrus Project) at EPCC (http://www.cirrus.ac.uk) funded by the University of Edinburgh and EPSRC (EP/P020267/1); ARCHER2 UK National Supercomputing Service via Project d429. E.J.G.S. acknowledges the EPSRC Open Fellowship (EP/T021578/1), and the Edinburgh-Rice Strategic Collaboration Awards for funding support. The authors would like to thank Amir Capua for fruitful discussions. The authors thank Atzmon Vakahi and Sergei Remennik for technical support. R.R.-E. would like to thank Sarah Jenkins for technical support on the simulations and helpful discussions.
Publisher Copyright:
© 2023 The Authors. Advanced Materials published by Wiley-VCH GmbH.
PY - 2023/11/23
Y1 - 2023/11/23
N2 - Recent advancements in 2D materials have revealed the potential of van der Waals magnets, and specifically of their magnetic anisotropy that allows applications down to the 2D limit. Among these materials, CrSBr has emerged as a promising candidate, because its intriguing magnetic and electronic properties have appeal for both fundamental and applied research in spintronics or magnonics. Here, nano SQUID-on-tip (SOT) microscopy is used to obtain direct magnetic imaging of CrSBr flakes with thicknesses ranging from monolayer (N=1) to few-layer (N=5). The ferromagnetic order is preserved down to the monolayer, while the antiferromagnetic coupling of the layers starts from the bilayer case. For odd layers, at zero applied magnetic field, the stray field resulting from the uncompensated layer is directly imaged. The progressive spin reorientation along the out-of-plane direction (hard axis) is also measured with a finite applied magnetic field, allowing to evaluate the anisotropy constant, which remains stable down to the monolayer and is close to the bulk value. Finally, by selecting the applied magnetic field protocol, the formation of N\'eel magnetic domain walls is observed down to the single layer limit.
AB - Recent advancements in 2D materials have revealed the potential of van der Waals magnets, and specifically of their magnetic anisotropy that allows applications down to the 2D limit. Among these materials, CrSBr has emerged as a promising candidate, because its intriguing magnetic and electronic properties have appeal for both fundamental and applied research in spintronics or magnonics. Here, nano SQUID-on-tip (SOT) microscopy is used to obtain direct magnetic imaging of CrSBr flakes with thicknesses ranging from monolayer (N=1) to few-layer (N=5). The ferromagnetic order is preserved down to the monolayer, while the antiferromagnetic coupling of the layers starts from the bilayer case. For odd layers, at zero applied magnetic field, the stray field resulting from the uncompensated layer is directly imaged. The progressive spin reorientation along the out-of-plane direction (hard axis) is also measured with a finite applied magnetic field, allowing to evaluate the anisotropy constant, which remains stable down to the monolayer and is close to the bulk value. Finally, by selecting the applied magnetic field protocol, the formation of N\'eel magnetic domain walls is observed down to the single layer limit.
KW - 2D magnetism
KW - van der Waals anti-ferromagnet
KW - Magnetic domains
KW - Scanning SQUID-on-tip microscopy
KW - CrSBr
U2 - 10.1002/adma.202307195
DO - 10.1002/adma.202307195
M3 - Article
SN - 0935-9648
VL - 35
SP - 1
EP - 9
JO - Advanced Materials
JF - Advanced Materials
IS - 47
M1 - 2307195
ER -