Deutsch
 
Benutzerhandbuch Datenschutzhinweis Impressum Kontakt
  DetailsucheBrowse

Datensatz

DATENSATZ AKTIONENEXPORT

Freigegeben

Zeitschriftenartikel

Electrical resistivity and thermodynamic properties of the ferromagnet Nd2Pt2In

MPG-Autoren
/persons/resource/persons126866

Strydom,  A. M.
Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

Externe Ressourcen
Es sind keine Externen Ressourcen verfügbar
Volltexte (frei zugänglich)
Es sind keine frei zugänglichen Volltexte verfügbar
Ergänzendes Material (frei zugänglich)
Es sind keine frei zugänglichen Ergänzenden Materialien verfügbar
Zitation

Tchokonte, M. B. T., Mboukam, J. J., Bashir, A. K. H., Sondezi, B. M., Kumar, K. R., Strydom, A. M., et al. (2018). Electrical resistivity and thermodynamic properties of the ferromagnet Nd2Pt2In. Journal of Alloys and Compounds, 753, 41-45. doi:10.1016/j.jallcom.2018.04.193.


Zitierlink: http://hdl.handle.net/21.11116/0000-0001-7B51-A
Zusammenfassung
The Nd2Pt2In compound was investigated by means of electrical resistivity rho(T), heat capacity C-p (T), magnetic susceptibility x(T), magnetization M(mu(0)(H) and magnetocaloric effect (MCE) measurements. The material orders ferromagnetically at T-C = 16 K with a second - order phase transition. In the ordered state, rho(T) can be represented in terms of ferromagnetic (FM) spin - wave dispersion with an energy gap Delta(R) = 13(1) K in zero field. In concert, the C-p(T) data in this region can be well described by the same model getting Delta(C) = 8(1) K in zero field. Above T-C, the rho(T) variation is characteristic of electron - phonon interaction in the presence of s - d scattering and crystalline-electric field (CEF). The 4f - electron specific heat shows a Schottky - type anomaly around 60 K associated with CEF. On the other hand, C-p(T) data of the non-magnetic homologue La2Pt2In can be described by the Debye - Einstein model, giving a Debye and Einstein temperature values of 190.3(5) K and 69.8(7) K respectively. At high temperatures, the x(T) data follows the Curie - Weiss relation with an effective magnetic moment mu(eff) = 3.61(2) mu(B) and a Weiss temperature theta(p) = 17(1) K. The magnitude of MCE was estimated from the isothermal magnetization data to be 6.25 J/(kg.K), 5.01 J/(kg.K), 3.18 J/(kg.K) and 0.47 J/(kg.K) for a field change of 7 T, 5 T, 3 T and 1 T, respectively. The characteristic behaviour of the isothermal magnetic entropy change points to a second order character of the FM phase transition. (C) 2018 Elsevier B.V. All rights reserved.