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Title: | Magnetic state selected by magnetic dipole interaction in the kagome antiferromagnet NaBa2Mn3F11 |
Authors: | Hayashida, S Ishikawa, H Okamoto, Y Okubo, T Hiroi, Z Avdeev, M Manuel, P Hagihala, M Soda, M Masuda, T |
Keywords: | Magnetism Phase transformations Neutron diffraction Bragg curve Antiferromagnetism Magnetic dipoles |
Issue Date: | 12-Feb-2018 |
Publisher: | American Physical Society |
Citation: | Hayashida, S., Ishikawa, H., Okamoto, Y., Okubo, T., Hiroi, Z., Avdeev, M., Manuel, P., Hagihala, M., Soda, M., & Masuda, T. (2018). Magnetic state selected by magnetic dipole interaction in the kagome antiferromagnet NaBa2Mn3F11. Physical Review B, 97(5), 054411. doi:10.1103/PhysRevB.97.054411 |
Abstract: | We haved studied the ground state of the classical kagome antiferromagnet NaBa2Mn3F11. Strong magnetic Bragg peaks observed for d spacings shorter than 6.0 Å were indexed by the propagation vector of k0=(0,0,0). Additional peaks with weak intensities in the d-spacing range above 8.0 Å were indexed by the incommensurate vector of k1=[0.3209(2),0.3209(2),0] and k2=[0.3338(4),0.3338(4),0]. Magnetic structure analysis unveils a 120∘ structure with the tail-chase geometry having k0 modulated by the incommensurate vector. A classical calculation of the Heisenberg kagome antiferromagnet with antiferromagnetic second-neighbor interaction, for which the ground state a k0120∘ degenerated structure, reveals that the magnetic dipole-dipole (MDD) interaction including up to the fourth neighbor terms selects the tail-chase structure. The observed modulation of the tail-chase structure is attributed to a small perturbation such as the long-range MDD interaction or the interlayer interaction. ©2018 American Physical Society |
URI: | https://doi.org/10.1103/PhysRevB.97.054411 https://apo.ansto.gov.au/dspace/handle/10238/10910 |
ISSN: | 2469-9969 |
Appears in Collections: | Journal Articles |
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