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Unusual Electrical Transport Driven by the Competition between Antiferromagnetism and Ferromagnetism in Antiperovskite Mn(3)Zn(1−x)Co(x)N

The magnetic, electrical transport and thermal expansion properties of Mn(3)Zn(1−x)Co(x)N (x = 0.2, 0.4, 0.5, 0.7, 0.9) have been systematically investigated. Co-doping in Mn(3)ZnN complicates the magnetic interactions, leading to a competition between antiferromagnetism and ferromagnetism. Abrupt r...

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Detalles Bibliográficos
Autores principales: Chu, Lihua, Ding, Lei, Wang, Cong, Li, Meicheng, Guo, Yanjiao, Liu, Zhuohai
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5848983/
https://www.ncbi.nlm.nih.gov/pubmed/29439522
http://dx.doi.org/10.3390/ma11020286
Descripción
Sumario:The magnetic, electrical transport and thermal expansion properties of Mn(3)Zn(1−x)Co(x)N (x = 0.2, 0.4, 0.5, 0.7, 0.9) have been systematically investigated. Co-doping in Mn(3)ZnN complicates the magnetic interactions, leading to a competition between antiferromagnetism and ferromagnetism. Abrupt resistivity jump phenomenon and negative thermal expansion behavior, both associated with the complex magnetic transition, are revealed in all studied cases. Furthermore, semiconductor-like transport behavior is found in sample x = 0.7, distinct from the metallic behavior in other samples. Below 50 K, resistivity minimum is observed in samples x = 0.4, 0.7, and 0.9, mainly caused by e-e scattering mechanism. We finally discussed the strong correlation among unusual electrical transport, negative thermal expansion and magnetic transition in Mn(3)Zn(1−x)Co(x)N, which allows us to conclude that the observed unusual electrical transport properties are attributed to the shift of the Fermi energy surface entailed by the abrupt lattice contraction.