Compositional genesis of ferromagnetism in alloys PrNi2−xCox

•Cobalt atoms have magnetic moment 0.5 µB at all values of x.•Alloys with 0 ≤ x ≤ 0.2 are paramagnets at T ≥ 2 K.•Alloys with 0.4 ≤ x ≤ 0.8 are anisotropic cluster ferromagnets.•Alloys with 1 ≤ x ≤ 2 are long range ordered ferromagnets.•Calculated magnetization curves satisfactorily agree with exper...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Journal of magnetism and magnetic materials 2019-11, Vol.490, p.1, Article 165489
Hauptverfasser: Ermolenko, A.S., Korolev, A.V., Gerasimov, E.G., Gaviko, V.S., Terentev, P.B., Mushnikov, N.V.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
Beschreibung
Zusammenfassung:•Cobalt atoms have magnetic moment 0.5 µB at all values of x.•Alloys with 0 ≤ x ≤ 0.2 are paramagnets at T ≥ 2 K.•Alloys with 0.4 ≤ x ≤ 0.8 are anisotropic cluster ferromagnets.•Alloys with 1 ≤ x ≤ 2 are long range ordered ferromagnets.•Calculated magnetization curves satisfactorily agree with experimental ones. The structure and magnetic properties of PrNi2−xCox alloys are investigated over the entire concentration range 0 ≤ x ≤ 2. It is shown that there is a continuous series of disordered solid solutions with a structure of the MgCu2 type. In all alloys, cobalt atoms have a magnetic moment μCo = 0.5 μB. The ground magnetic state of the alloys depends on the composition. In the range 0 ≤ x ≤ 0.2, alloys are paramagnetic at a temperature T = 2 K, in the alloys with 0.4 ≤ x ≤ 0.8, ferromagnetic order occurs in clusters of cobalt atoms due to the exchange interaction of Co – Co. Their magnetization in small magnetic fields is realized via turnabout, by 180°, of the magnetic moments of individual clusters. In the alloys with 1.0 ≤ x ≤ 2.0, the long-range ferromagnetic order is established. The processes of technical magnetization reversal in them are effected via the motion of domain walls and rotation of the vectors of spontaneous magnetization. In all alloys, magnetic saturation is not achieved at T = 5 K even in a magnetic field of 200 kOe, which is associated with a large splitting of the ground J multiple of Pr3+ ions by the crystal field. Numerical calculations of the magnetization curves are performed. In the approximation of the independence of the parameters of the crystal field on the concentration, a satisfactory agreement between the calculated and experimental curves was obtained.
ISSN:0304-8853
1873-4766
DOI:10.1016/j.jmmm.2019.165489