TY - JOUR
T1 - Nanoscale measurement of giant saturation magnetization in α″-Fe16N2 by electron energy-loss magnetic chiral dichroism
AU - Chen, Xinfeng
AU - Higashikozono, Soma
AU - Ito, Keita
AU - Jin, Lei
AU - Ho, Ping Luen
AU - Yu, Chu Ping
AU - Tai, Nyan Hwa
AU - Mayer, Joachim
AU - Dunin-Borkowski, Rafal E.
AU - Suemasu, Takashi
AU - Zhong, Xiaoyan
N1 - Funding Information:
The work was supported financially by the National Key Research and Development Program [2016YFB0700402], National Natural Science Foundation of China [11834009, 51761135131, 51822105, 51671112, 51788104] National Basic Research Program of China [2015CB921700], Fund of Key Laboratory of Advanced Materials of Ministry of Education [2018AML12] and the RWTH Aachen University - Tsinghua University Junior Research Fellowship scheme. R.D.-B. is grateful for funding from the European Research Council under the European Union's Seventh Framework Program [FP7/2007-2013]/ERC grant agreement number 320832. This work made use of the resources of the National Center for Electron Microscopy in Beijing and the Ernst Ruska-Centre for Microscopy and Spectroscopy with Electrons in Forschungszentrum Jülich. The authors thank Prof. J. Zhu, Prof. J-P. Wang and Dr. Q. Q. Lan for valuable discussions and contributions to this work.
Publisher Copyright:
© 2019 Elsevier B.V.
PY - 2019/8
Y1 - 2019/8
N2 - Metastable α″-Fe16N2 thin films were reported to have a giant saturation magnetization of above 2200 emu/cm3 in 1972 and have been considered as candidates for next-generation rare-earth-free permanent magnetic materials. However, their magnetic properties have not been confirmed unequivocally. As a result of the limited spatial resolution of most magnetic characterization techniques, it is challenging to measure the saturation magnetization of the α″-Fe16N2 phase, as it is often mixed with the parent α′-Fe8N phase in thin films. Here, we use electron energy-loss magnetic chiral dichroism (EMCD), aberration-corrected transmission electron microscopy, X-ray diffraction and macroscopic magnetic measurements to study α″-Fe16N2 (containing ordered N atoms) and α′-Fe8N (containing disordered N atoms). The ratio of saturation magnetization in α″-Fe16N2 to that in α′-Fe8N is determined to be 1.31 ± 0.10 from quantitative EMCD measurements and dynamical diffraction calculations, confirming the giant saturation magnetization of α″-Fe16N2. Crystallographic information is also obtained about the two phases, which are mixed on the nanoscale.
AB - Metastable α″-Fe16N2 thin films were reported to have a giant saturation magnetization of above 2200 emu/cm3 in 1972 and have been considered as candidates for next-generation rare-earth-free permanent magnetic materials. However, their magnetic properties have not been confirmed unequivocally. As a result of the limited spatial resolution of most magnetic characterization techniques, it is challenging to measure the saturation magnetization of the α″-Fe16N2 phase, as it is often mixed with the parent α′-Fe8N phase in thin films. Here, we use electron energy-loss magnetic chiral dichroism (EMCD), aberration-corrected transmission electron microscopy, X-ray diffraction and macroscopic magnetic measurements to study α″-Fe16N2 (containing ordered N atoms) and α′-Fe8N (containing disordered N atoms). The ratio of saturation magnetization in α″-Fe16N2 to that in α′-Fe8N is determined to be 1.31 ± 0.10 from quantitative EMCD measurements and dynamical diffraction calculations, confirming the giant saturation magnetization of α″-Fe16N2. Crystallographic information is also obtained about the two phases, which are mixed on the nanoscale.
KW - Electron energy-loss magnetic chiral dichroism
KW - Giant saturation magnetization
KW - Rare-earth-free permanent magnetic materials
KW - α″-FeN, high spatial resolution
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U2 - 10.1016/j.ultramic.2019.02.016
DO - 10.1016/j.ultramic.2019.02.016
M3 - Article
C2 - 30862364
AN - SCOPUS:85062665871
SN - 0304-3991
VL - 203
SP - 37
EP - 43
JO - Ultramicroscopy
JF - Ultramicroscopy
ER -