TY - JOUR
T1 - Gradual development of Γ5g antiferromagnetic moment in the giant negative thermal expansion material Mn3Cu1-x Ge x N (x∼0.5)
AU - Kodama, K.
AU - Iikubo, S.
AU - Takenaka, K.
AU - Takigawa, M.
AU - Takagi, H.
AU - Shamoto, S.
N1 - Copyright:
Copyright 2010 Elsevier B.V., All rights reserved.
PY - 2010/6/14
Y1 - 2010/6/14
N2 - The antiperovskite compound Mn3 Cu1-x Gex N with x∼0.5 has a giant negative thermal expansion coefficient due to the magnetovolume effect near room temperature. Competition between the Γ5g and Γ4g antiferromagnetic structures around the magnetic ordering temperature could be the driving force for such a phenomenon. In order to examine this possibility, we performed neutron-diffraction experiments on Mn3Cu0.5Ge0.5N and N 14 nuclear magnetic resonance experiments on Mn3 Cu0.6 Ge0.4 N. As a reference material, we also investigated Mn3 NiN, whose spin structure is represented by a linear combination of the Γ5g and Γ4g antiferromagnetic components. We conclude that in Mn3 Cu 1-x Gex N (x∼0.5), the Γ4g antiferromagnetic component is nearly absent and the competition between the Γ5g and Γ4g antiferromagnetic structures is irrelevant to the giant negative thermal expansion coefficient. The Γ5g antiferromagnetic ordered moment gradually develops with decreasing temperature. This provides a thorough justification for the analysis presented in the previous letter.
AB - The antiperovskite compound Mn3 Cu1-x Gex N with x∼0.5 has a giant negative thermal expansion coefficient due to the magnetovolume effect near room temperature. Competition between the Γ5g and Γ4g antiferromagnetic structures around the magnetic ordering temperature could be the driving force for such a phenomenon. In order to examine this possibility, we performed neutron-diffraction experiments on Mn3Cu0.5Ge0.5N and N 14 nuclear magnetic resonance experiments on Mn3 Cu0.6 Ge0.4 N. As a reference material, we also investigated Mn3 NiN, whose spin structure is represented by a linear combination of the Γ5g and Γ4g antiferromagnetic components. We conclude that in Mn3 Cu 1-x Gex N (x∼0.5), the Γ4g antiferromagnetic component is nearly absent and the competition between the Γ5g and Γ4g antiferromagnetic structures is irrelevant to the giant negative thermal expansion coefficient. The Γ5g antiferromagnetic ordered moment gradually develops with decreasing temperature. This provides a thorough justification for the analysis presented in the previous letter.
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U2 - 10.1103/PhysRevB.81.224419
DO - 10.1103/PhysRevB.81.224419
M3 - Article
AN - SCOPUS:77956327916
SN - 1098-0121
VL - 81
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 22
M1 - 224419
ER -