The decisive role of magnetic anisotropy in honeycomb layered Li3Ni2SbO6 and Na3Ni2SbO6
The decisive role of magnetic anisotropy even in systems with small anisotropy is illustrated for the honeycomb-layered antiferromagnets A3Ni2SbO6 with A=Li and Na. Both systems evolve long range magnetic order below TN=14 and 16.5K, respectively. The magnetic phase diagrams obtained from static mag...
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| Main Authors: | , , , , |
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| Format: | Article (Journal) |
| Language: | English |
| Published: |
19 February 2019
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| In: |
Journal of magnetism and magnetic materials
Year: 2019, Volume: 481, Pages: 100-103 |
| ISSN: | 1873-4766 |
| DOI: | 10.1016/j.jmmm.2019.02.054 |
| Online Access: | Verlag, Volltext: https://doi.org/10.1016/j.jmmm.2019.02.054 Verlag, Volltext: http://www.sciencedirect.com/science/article/pii/S0304885318323345 
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| Author Notes: | J. Werner, W. Hergett, J. Park, C. Koo, E.A. Zvereva, A.N. Vasiliev, R. Klingeler |
MARC
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| 245 | 1 | 4 | |a The decisive role of magnetic anisotropy in honeycomb layered Li3Ni2SbO6 and Na3Ni2SbO6 |c J. Werner, W. Hergett, J. Park, C. Koo, E.A. Zvereva, A.N. Vasiliev, R. Klingeler |
| 246 | 3 | 3 | |a The decisive role of magnetic anisotropy in honeycomb layered Li 3 Ni 2 SbO 6 and Na 3 Ni 2 SbO 6 |
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| 520 | |a The decisive role of magnetic anisotropy even in systems with small anisotropy is illustrated for the honeycomb-layered antiferromagnets A3Ni2SbO6 with A=Li and Na. Both systems evolve long range magnetic order below TN=14 and 16.5K, respectively. The magnetic phase diagrams obtained from static magnetisation studies up to 15T imply competing antiferromagnetic phases and a tricritical point at TN. The phase boundaries are visible in the dynamic response of the antiferromagnetic resonance modes, too, which investigation by means of high frequency/high field electron spin resonance enables precise determination of magnetic anisotropy. The anisotropy gap amounts to Δ=360±2GHz in Na3Ni2SbO6 while in Li3Ni2SbO6 orthorhombicity is associated with Δ=198±4 and 218±4GHz. Above TN, the data imply short-range antiferromagnetic order up to at least 80K. The data suggest a crucial role of anisotropy for selecting the actual spin structure at B=0T. | ||
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