Hauptseite > Publikationsdatenbank > Nanoscale measurement of giant saturation magnetization in α″-Fe16N2 by electron energy-loss magnetic chiral dichroism > print |
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024 | 7 | _ | |a 10.1016/j.ultramic.2019.02.016 |2 doi |
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100 | 1 | _ | |a Chen, Xinfeng |0 P:(DE-HGF)0 |b 0 |
245 | _ | _ | |a Nanoscale measurement of giant saturation magnetization in α″-Fe16N2 by electron energy-loss magnetic chiral dichroism |
260 | _ | _ | |a Amsterdam |c 2019 |b Elsevier Science |
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520 | _ | _ | |a 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. |
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700 | 1 | _ | |a Zhong, Xiaoyan |0 P:(DE-HGF)0 |b 10 |e Corresponding author |
773 | _ | _ | |a 10.1016/j.ultramic.2019.02.016 |g Vol. 203, p. 37 - 43 |0 PERI:(DE-600)1479043-9 |p 37 - 43 |t Ultramicroscopy |v 203 |y 2019 |x 0304-3991 |
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