Magnetic state selected by magnetic dipole interaction in the kagome antiferromagnet NaBa2Mn3F11
dc.contributor.author | Hayashida, S | en_AU |
dc.contributor.author | Ishikawa, H | en_AU |
dc.contributor.author | Okamoto, Y | en_AU |
dc.contributor.author | Okubo, T | en_AU |
dc.contributor.author | Hiroi, Z | en_AU |
dc.contributor.author | Avdeev, M | en_AU |
dc.contributor.author | Manuel, P | en_AU |
dc.contributor.author | Hagihala, M | en_AU |
dc.contributor.author | Soda, M | en_AU |
dc.contributor.author | Masuda, T | en_AU |
dc.date.accessioned | 2021-06-28T19:59:21Z | en_AU |
dc.date.available | 2021-06-28T19:59:21Z | en_AU |
dc.date.issued | 2018-02-12 | en_AU |
dc.date.statistics | 2021-06-16 | en_AU |
dc.description.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 | en_AU |
dc.identifier.articlenumber | 54411 | en_AU |
dc.identifier.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 | en_AU |
dc.identifier.issn | 2469-9969 | en_AU |
dc.identifier.issue | 5 | en_AU |
dc.identifier.journaltitle | Physical Review B | en_AU |
dc.identifier.uri | https://doi.org/10.1103/PhysRevB.97.054411 | en_AU |
dc.identifier.uri | https://apo.ansto.gov.au/dspace/handle/10238/10910 | en_AU |
dc.identifier.volume | 97 | en_AU |
dc.language.iso | en | en_AU |
dc.publisher | American Physical Society | en_AU |
dc.subject | Magnetism | en_AU |
dc.subject | Phase transformations | en_AU |
dc.subject | Neutron diffraction | en_AU |
dc.subject | Bragg curve | en_AU |
dc.subject | Antiferromagnetism | en_AU |
dc.subject | Magnetic dipoles | en_AU |
dc.title | Magnetic state selected by magnetic dipole interaction in the kagome antiferromagnet NaBa2Mn3F11 | en_AU |
dc.type | Journal Article | en_AU |
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