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Please use this identifier to cite or link to this item: http://apo.ansto.gov.au/dspace/handle/10238/7018

Title: Spin-cycloid instability as the origin of weak ferromagnetism in the disordered perovskite Bi0.8La0.2Fe0.5Mn0.5O3
Authors: Bertinshaw, J
Cortie, DL
Cheng, ZX
Avdeev, M
Studer, AJ
Klose, F
Ulrich, C
Wang, XL
Keywords: NEUTRON DIFFRACTION
MAGNETOMETERS
CRYSTALLOGRAPHY
ANTIFERROMAGNETIC MATERIALS
PEROVSKITE
EXPERIMENT PLANNING
Issue Date: 23-Apr-2014
Publisher: APS Physics
Citation: Bertinshaw, J., Cortie, D. L., Cheng, Z. X., Avdeev, M., Studer, A. J., Klose, F., . . . Wang, X. L. (2014). Spin-cycloid instability as the origin of weak ferromagnetism in the disordered perovskite Bi0.8La0.2Fe0.5Mn0.5O3 . Physical Review B, 89(14), 144422.
Abstract: Powder neutron diffraction and magnetometry studies have been conducted to investigate the crystallographic and magnetic structure of Bi0.8La0.2Fe0.5Mn0.5O3. The compound stabilizes in the Imma orthorhombic crystal symmetry in the measured temperature range of 5 to 380 K, with a transition to antiferromagnetic order at TN≈240 K. The spin cycloid present for BiFeO3 is found to be absent with 50% Mn3+ cation substitution, leading to G-type antiferromagnetic order with an enhanced out-of-plane canted ferromagnetic component, evident from measurable weak-ferromagnetic hysteresis. Structural modifications do not solely explain this behavior, indicating that modified electron exchange interactions must be taken into account. A classical spin simulation was developed to investigate the effect of random substitution in a disordered pseudocubic perovskite. The calculations took into account the nearest-neighbor, next-nearest-neighbor, and Dzyaloshinskii-Moriya interactions, along with the local spin anisotropy. Using this framework to extend the established Hamiltonian model for BiFeO3, we show that only certain types of perturbations at a magnetic defect and the surrounding molecular fields trigger a simultaneous collapse of cycloidal order and the emergence of the long-range weak-ferromagnetic component. By adopting values for the Mn molecular fields appropriate for REMnO3 (RE= rare earth), simulations of BiMn0.5Fe0.5O3 exhibit the key magnetic properties of our experimental observations.© 2014, American Physical Society.
URI: http://dx.doi.org/10.1103/PhysRevB.89.144422
http://apo.ansto.gov.au/dspace/handle/10238/7018
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