It appears you don't have support to open PDFs in this web browser. To view this file, Open with your PDF reader
Abstract
Many large unit-cell rare-earth transition metal ternary alloys of the type Ra(M1−xM’x)b exhibit non-monotonic ferrimagnetic Curie temperatures (TC) coupled to monotonic composition-controlled magnetization. Its origin remains an important long-standing puzzle in the absence of studies probing their temperature-dependent element-specific magnetism. Here, in order to resolve this issue and identify design principles for new R-M-M’ permanent magnets, we carry out x-ray magnetic circular dichroism (XMCD) for the series Gd6(Mn1−xFex)23, x = 0.0 − 0.75. The results show that the net Mn-moment reduces and switches from parallel to antiparallel for x ≥ 0.2, while the Fe-moment is always antiparallel to the Gd-moment. Kouvel-Fisher analyses of XMCD data reveals distinct sublattice TC’s and 3D Heisenberg criticality. Band structure calculations show magnetic moments and density of states consistent with experiments. The magnetic phase diagram shows three regions characterized by (i) Mn-sublattice bulk-TC > Gd-sublattice TC, (ii) a reduced common-TC for all sublattices, and (iii) Fe-sublattice bulk-TC > Gd-sublattice TC. The Mn-moment switching and gradual increase of Fe-moment combine to cause non-monotonic TC’s with monotonic magnetization. The study indicates the importance of element-specific TC’s for tuning magnetic properties.
Ternary alloys of rare-earths and transition metals exhibit complex ferrimagnetic behavior as a function of alloy compositions. Here, X-ray magnetic circular dichroism of the Gd6(Mn1−xFex)23 series is used to explain the composition dependence of sublattice Curie temperatures in terms of element-specific magnetic moment evolution.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Details





1 National Synchrotron Radiation Research Center, Hsinchu, Taiwan (GRID:grid.410766.2) (ISNI:0000 0001 0749 1496); National Yang Ming Chiao Tung University, International College of Semiconductor Technology, Hsinchu, Taiwan (GRID:grid.260539.b) (ISNI:0000 0001 2059 7017)
2 Université de Lorraine, Institut Jean Lamour, UMR 7198, CNRS, Nancy, France (GRID:grid.29172.3f) (ISNI:0000 0001 2194 6418)
3 National Synchrotron Radiation Research Center, Hsinchu, Taiwan (GRID:grid.410766.2) (ISNI:0000 0001 0749 1496)
4 National Yang Ming Chiao Tung University, International College of Semiconductor Technology, Hsinchu, Taiwan (GRID:grid.260539.b) (ISNI:0000 0001 2059 7017); National Yang Ming Chiao Tung University, Department of Materials Science and Engineering, Hsinchu, Taiwan (GRID:grid.260539.b) (ISNI:0000 0001 2059 7017)