Magnetic properties of LaFe2−xCoxSi: A new two-phase naturally formed composite alloy
Source abstract
Abstract
We report the effect of Fe by Co substitution on the structural and magnetic properties of the two-phase “composite” alloy LaFe2−xCoxSi as prepared by the suction casting technique. This alloy contains LaFe13−x−yCoxSiy (cubic NaZn13-type) and LaFe1−xCoxSi (tetragonal CeFeSi-type) as constituents, with a compositional ratio between the two phases of ≈40 wt. % NaZn13-type and ≈60 wt. % CeFeSi-type; this ratio remains relatively the same for all the compositions investigated despite the Co content. As expected, while the Co-doping in LaFe2−xCoxSi increases the Curie temperature from 199 K (at H = 20 kOe) and 215 K (at H = 50 kOe) for the pure LaFe2Si, to 274 K (at H = 20 kOe) and 277 K (at H = 50 kOe) for the Co substituted LaFe1.7Co0.3Si alloy, it has the opposite effect on the magnetocaloric effect, reported in terms of the magnetic entropy change (ΔSM), which decreases with increasing the Co content. The full width at the half-maximum value of magnetic entropy changes also increases significantly with Co doping going from 14 K (at H = 20 kOe) in the pure LaFe2Si alloy to 46 K (at H = 20 kOe) in the Co-doped LaFe2−xCoxSi. The magnetic and magnetocaloric properties of LaFe2−xCoxSi alloys for x = 0, 0.1, 0.2, and 0.3 are discussed in this article.
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Research context
OpenAlex topics: Magnetic and transport properties of perovskites and related materials · Rare-earth and actinide compounds · Shape Memory Alloy Transformations
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics, SUNY Buffalo State College 1 , Buffalo, New York 14222, USA
Engineering Technology, SUNY Buffalo State College 2 , Buffalo, New York 14222, USA
Funding
National Science Foundation · Office of Undergraduate Research, SUNY Buffalo State
References (21)
Show source-provided references
1. Int. J. Refrig. · 2014 · 37 · 8410.1016/j.ijrefrig.2013.09.025 ↗
2. Appl. Phys. Lett. · 2001 · 79 · 65310.1063/1.1388157 ↗
3. Chem. Mater. · 2020 · 32 · 180710.1021/acs.chemmater.9b03915 ↗
4. J. Solid State Chem. · 2016 · 233 · 9510.1016/j.jssc.2015.10.016 ↗
5. Phys. Rev. B · 2020 · 101 · 06441510.1103/physrevb.101.064415 ↗
6. Acta Mater. · 2021 · 215 · 11708310.1016/j.actamat.2021.117083 ↗
7. J. Phys.: Condens. Matter · 2003 · 15 · 526910.1088/0953-8984/15/30/309 ↗
8. Adv. Mater. · 2009 · 21 · 454510.1002/adma.200901072 ↗
9. J. Phys.: Condens. Matter · 2003 · 15 · 7385
10. 2005
11. J. Magn. Magn. Mater. · 2010 · 322 · 69210.1016/j.jmmm.2009.10.043 ↗
12. J. Phys. D: Appl. Phys. · 2018 · 51 · 11500310.1088/1361-6463/aaad28 ↗
13. Adv. Electron. Mater. · 2018 · 4 · 170063610.1002/aelm.201700636 ↗
14. Mater. Charact. · 2019 · 147 · 51210.1016/j.matchar.2018.06.036 ↗
15. J. Alloys Compd. · 2016 · 680 · 26810.1016/j.jallcom.2016.04.120 ↗
16. J. Alloys Compd. · 1992 · 189 · 4910.1016/0925-8388(92)90045-b ↗
17. J. Appl. Crystallogr. · 1977 · 10 · 7310.1107/s0021889877012898 ↗
18. 2003
19. J. Magn. Magn. Mater. · 1999 · 200 · 4410.1016/s0304-8853(99)00397-2 ↗
20. 1965
21. Mater. Sci. Forum · 1999 · 315–317 · 6910.4028/www.scientific.net/msf.315-317.69 ↗