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Structural and Magnetic Properties of Ni(1+x)MnSb Bulk Heusler Composite Materials

[Image: see text] Variation in structural and magnetic properties with changing valence electron count (VEC) has been studied well in the family of Heusler compounds, while such changes in VEC resulting in half-Heusler (HH) and full-Heusler (FH) composites have not been reported to observe their eff...

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Detalles Bibliográficos
Autores principales: Govind, Bal, Kumar, Ashish, Bano, Sahiba, Bhardwaj, Aman, Misra, Dinesh Kumar
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7271010/
https://www.ncbi.nlm.nih.gov/pubmed/32548368
http://dx.doi.org/10.1021/acsomega.9b03386
Descripción
Sumario:[Image: see text] Variation in structural and magnetic properties with changing valence electron count (VEC) has been studied well in the family of Heusler compounds, while such changes in VEC resulting in half-Heusler (HH) and full-Heusler (FH) composites have not been reported to observe their effect on the magnetic properties. Herein, we have synthesized the composite of HH and FH phases in Ni(1+x)MnSb (x = 0.0, 0.3, and 0.6) via changing VEC from 22 to 28 in order to investigate the structural and magnetic properties. Interestingly, a transition from half-metallic ferromagnetic to normal ferromagnetic was revealed in Ni(1+x)MnSb (x = 0.0, 0.3, and 0.6) materials with increasing VEC. The structural investigations of these materials were performed using a X-ray diffraction technique and analyzed by Rietveld Refinement software for all the samples. Rietveld analysis reveals the presence of a significant amount of the NiSb paramagnetic impurity phase in the HH NiMnSb system while in the case of Ni(1+x)MnSb (x = 0.3 and 0.6), no such impurity phase was observed. Only FH and HH phases in Ni(1+x)MnSb (x = 0.3 and 0.6) samples were noticed. The magnetic measurement performed on samples employing a vibrating sample magnetometer reveals the ferromagnetic ordering in all samples. A weak hysteresis loop with saturated magnetic moments ∼2.99 and 2.98 μ(B) at room temperature was observed for NiMnSb and Ni(1.3)MnSb, respectively, while a strong hysteresis loop with lower magnetic moment of 0.88 μ(B) was observed in the Ni(1.6)MnSb composite. Furthermore, the observed magnetic moments for the composite Ni(1.3)MnSb have been explained on the basis of the Slater–Pauling rule in relation to VEC.