Loading…

Intrinsic magnetic properties of the RFe11Ti (R = Y and Gd) alloys by Co, Zr and C doping

We present theoretical investigations on the electronic and magnetic properties of the RFe11-xCoxTiCz and R1-yZryFe11Ti (R = Y and Gd; x = 0–3, y = 0–0.1, z = 0 and 1) alloys describing the dependence of the magnetic properties (magnetic moments, magneto-crystalline anisotropy, exchange-coupling par...

Full description

Saved in:
Bibliographic Details
Published in:Solid state communications 2022-11, Vol.355, p.114922, Article 114922
Main Authors: Benea, D., Hirian, R., Gutoiu, S., Isnard, O., Pop, V.
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:We present theoretical investigations on the electronic and magnetic properties of the RFe11-xCoxTiCz and R1-yZryFe11Ti (R = Y and Gd; x = 0–3, y = 0–0.1, z = 0 and 1) alloys describing the dependence of the magnetic properties (magnetic moments, magneto-crystalline anisotropy, exchange-coupling parameters and Curie temperatures) on the R/Zr and Fe/Co ratios and by C addition. According to our calculations for YFe11-xCoxTi, the total magnetic moment and magnetocrystalline anisotropy energy (MAE) are maximized for x = 1. On the other hand, Co doping enhances the MAE but reduces the total magnetic moment in GdFe11-xCoxTi alloys. The doping adding one C atom to the near-neighbour environment of Fe 8j site affects the magnetic moments of Fe changing their magnitude sequence. Also, Zr for R substitution and C addition have lower impact on MAE, compared with Co for Fe substitution in RFe11Ti-type alloys. The calculated exchange-coupling parameters show highest values between Fe 8i spins, followed by Fe 8i – Fe 8j spins for all investigated alloys. The corresponding mean-field approach estimated Curie temperatures show qualitative agreement with available experimental data. •Intrinsic magnetic properties of RFe11-xCoxTiCz (x = 0–3, z = 1) and R1-yZryFe11Ti(y = 0.1) for R = Y, Gd.•Co preferential occupation for 8j and 8f sites determined by total energy calculations.•Increase of Fe spin moments and Tc by Co doping found for both RFe11-xCoxTi alloys, R = Y and Gd.•The site-dependent MAE evolutions by Co, Zr and C doping are analysed.•Minor impact on intrinsic properties induced by Zr doping, on opposite to C addition.
ISSN:0038-1098
1879-2766
DOI:10.1016/j.ssc.2022.114922