Competing magnetic interactions, structure and magnetocaloric effect in Mn3Sn1-xZnxC antiperovskite carbides

Journal Article (2023)
Author(s)

Anika Kiecana (TU Delft - RST/Fundamental Aspects of Materials and Energy)

W. Schaefers (Student TU Delft)

M. Thijs (Student TU Delft)

B.J.R. Dankelman (TU Delft - RID/TS/Technici Pool)

Hamutu Ojiyed (External organisation)

I. Batashev (Radboud Universiteit Nijmegen)

Fengqi Zhang (TU Delft - RST/Fundamental Aspects of Materials and Energy)

Niels van Dijk (TU Delft - RST/Fundamental Aspects of Materials and Energy)

EH Brück (TU Delft - RST/Fundamental Aspects of Materials and Energy)

Research Group
RST/Fundamental Aspects of Materials and Energy
Copyright
© 2023 A. Kiecana, W. Schaefers, M. Thijs, B.J.R. Dankelman, H. Ojiyed, I. Batashev, F. Zhang, N.H. van Dijk, E.H. Brück
DOI related publication
https://doi.org/10.1016/j.jmmm.2023.170782
More Info
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Publication Year
2023
Language
English
Copyright
© 2023 A. Kiecana, W. Schaefers, M. Thijs, B.J.R. Dankelman, H. Ojiyed, I. Batashev, F. Zhang, N.H. van Dijk, E.H. Brück
Research Group
RST/Fundamental Aspects of Materials and Energy
Volume number
577
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Abstract

Structural, magnetic and magnetocaloric properties of Mn3Sn1-xZnxC antiperovskite carbides have been studied. With increasing Zn content the first-order magnetic transition (FOMT) is weakened. The Curie temperature (TC) reduces first from 273 to 197 K and when x > 0.3, TC increases, reaching its maximum of 430 K for x = 1.0. An increase in TC is accompanied by pronounced changes in magnetic behaviour and a significant rise in magnetization from 21.82(4) to 76.2(2) Am2kg−1 for x = 0.8 in the maximum applied magnetic field of 5 T. Neutron powder diffraction (NPD) was employed to study the magnetic structure of Mn3Sn1-xZnxC compounds. The refinement of the NPD data for x = 0.3 revealed a magnetic structure with propagation vector k = (½,½,0) with a decrease in the canted antiferromagnetic (AFM) moment, which results in a reduction of the negative volume change at the magnetic transition and a decrease in the magnetocaloric effect (MCE). For x = 0.4, the magnetic structure is described by a propagation vector k = (½,½,½) for the AFM moment which dominates at low temperature, with the presence of a minor ferromagnetic (FM) component with a k = (0, 0, 0) propagation vector, which confirms the presence of the ferrimagnetic (FiM) state. For a higher Zn content (x = 0.6), the magnetic moment originates mainly from the FM component found on three independent Mn positions and an additional AFM moment oriented in the a-b plane. The results presented confirm the presence of competing AFM-FM interactions in Mn3Sn1-xZnxC antiperovskite carbides.