The effect of Mo substitution on the phase formation and magnetic properties of RE2(Fe1−xMox)17 alloys (RE=Nd,Gd)

Spin reorientation and magnetic anisotropy in Y2Co17−xCrx (x=1.17–3.0) compounds

“…In the past decades, rare-earth (R) transition-metal (T) compounds of the R 2 T 17 type with T = Fe or Co have been attracting much attention due to possible practical applications of these compounds as high energy-product magnets [1][2][3][4][5][6][7][8][9][10][11]. A strong uniaxial magnetic anisotropy is required for achieving high coercivity, while the binary R 2 Co 17 compounds exhibit a weak uniaxial anisotropy only for the compounds with R = Sm, Er and Tm.…”

Magnetic properties of Sm2Co17−xCrx (0 ≤ x ≤ 3.0) compounds

“…During the past decades, rare earth (R) transition metal (T) compounds of the R 2 T 17 -type with T = Fe or Co have been attracting much attention due to the possible practical applications of these compounds as high-energy-product magnets [1][2][3][4][5][6][7][8][9][10][11]. A strong uniaxial magnetic anisotropy is required for achieving high coercivity, the binary R 2 Co 17 compounds exhibiting uniaxial anisotropy only for R = Sm, Er, and Tm.…”

A thermodynamic assessment of the Fe‐Gd‐Mo system

“…The quasibinary compound series (Fe 1‐ x Mo x ) 17 Gd 2 was studied regarding its homogeneity range at 1373 K and magnetic properties [6]. Using the X‐ray diffraction coupled with the Rietveld refinement technique the authors have found the substitution limit for Mo in the rhombohedral Th 2 Zn 17 ‐type crystal structure to be around x =0.05.…”