TY - JOUR
T1 - Fe4-xNixNb2O9 (x ≤ 1)
T2 - Nickel impact on the magnetoelectric properties of Fe4Nb2O9
AU - Maignan, Antoine
AU - Jiongo-Dongmo, Jacqueline Nadine
AU - Martin, Christine
AU - Lebedev, O. I.
AU - Damay, Françoise
AU - Wang, Xiao
AU - Kuo, Chang Yang
AU - Chang, Chun Fu
AU - Hu, Zhiwei
AU - Tjeng, Liu Hao
N1 - Publisher Copyright:
© 2022 Elsevier Masson SAS
PY - 2022/3
Y1 - 2022/3
N2 - We report the investigation of the Ni for Fe substitution in Fe4Nb2O9 by X-ray techniques (diffraction and absorption spectroscopy), transmission electron microscopy (TEM), magnetometry and magneto (di)electric measurements. Up to x = 1 in Fe4-xNixNb2O9, the structure remains trigonal, with a unit cell volume which decreases by −1.4% from x = 0 to 1, in accordance with the difference in the ionic radius of divalent iron and nickel whose oxidation states were obtained by XAS. Furthermore, EDX analyses and high resolution TEM confirm the homogeneous atomic distribution. The antiferromagnetic transition temperature TN = 75 K of Fe3NiNb2O9 (x = 1) is 18 K lower than that of Fe4Nb2O9. The magnetic field (H) dependence of the magnetization (M) of Fe3NiNb2O9 below TN exhibits a spin-flop like at about 1T, and a more ferromagnetic-like M(H) behaviour than that of Fe4Nb2O9. Similarly, below TN, the H-dependent electric polarization (P) for the x = 0.5 and 1 samples is steeper than the P(H) curve of the x = 0 compound. This points towards the key role of such chemical substitutions to induce larger magnetoelectric coefficient.
AB - We report the investigation of the Ni for Fe substitution in Fe4Nb2O9 by X-ray techniques (diffraction and absorption spectroscopy), transmission electron microscopy (TEM), magnetometry and magneto (di)electric measurements. Up to x = 1 in Fe4-xNixNb2O9, the structure remains trigonal, with a unit cell volume which decreases by −1.4% from x = 0 to 1, in accordance with the difference in the ionic radius of divalent iron and nickel whose oxidation states were obtained by XAS. Furthermore, EDX analyses and high resolution TEM confirm the homogeneous atomic distribution. The antiferromagnetic transition temperature TN = 75 K of Fe3NiNb2O9 (x = 1) is 18 K lower than that of Fe4Nb2O9. The magnetic field (H) dependence of the magnetization (M) of Fe3NiNb2O9 below TN exhibits a spin-flop like at about 1T, and a more ferromagnetic-like M(H) behaviour than that of Fe4Nb2O9. Similarly, below TN, the H-dependent electric polarization (P) for the x = 0.5 and 1 samples is steeper than the P(H) curve of the x = 0 compound. This points towards the key role of such chemical substitutions to induce larger magnetoelectric coefficient.
KW - Antiferromagnetism
KW - Magnetoelectric effect
KW - Transition-metal oxides
UR - http://www.scopus.com/inward/record.url?scp=85123033397&partnerID=8YFLogxK
U2 - 10.1016/j.solidstatesciences.2022.106821
DO - 10.1016/j.solidstatesciences.2022.106821
M3 - Article
AN - SCOPUS:85123033397
SN - 1293-2558
VL - 125
JO - Solid State Sciences
JF - Solid State Sciences
M1 - 106821
ER -