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| 001 | 278944 | ||
| 005 | 20210129220953.0 | ||
| 024 | 7 | _ | |2 doi |a 10.1209/0295-5075/110/37007 |
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| 100 | 1 | _ | |0 P:(DE-HGF)0 |a Nair, Harikrishnan S. |b 0 |e Corresponding author |
| 245 | _ | _ | |a Spin-lattice coupling and frustrated magnetism in Fe-doped hexagonal LuMnO 3 |
| 260 | _ | _ | |a Les-Ulis |b EDP Science65224 |c 2015 |
| 264 | _ | 1 | |3 online |2 Crossref |b IOP Publishing |c 2015-05-19 |
| 264 | _ | 1 | |3 print |2 Crossref |b IOP Publishing |c 2015-05-01 |
| 264 | _ | 1 | |3 print |2 Crossref |b IOP Publishing |c 2015-05-01 |
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| 520 | _ | _ | |a Strong spin-lattice coupling and prominent frustration effects observed in the 50% Fe-doped frustrated hexagonal $(h)\text{LuMnO}_3$ are reported. A Néel transition at $T_{\mathrm{N}}\approx112\ \text{K}$ and a possible spin re-orientation transition at $T_{\mathrm{SR}}\approx55\ \text{K}$ are observed in the magnetization data. From neutron powder diffraction data, the nuclear structure at and below 300 K was refined in polar P63cm space group. While the magnetic structure of LuMnO3 belongs to the $\Gamma_4\ (P6'_3c'm)$ representation, that of LuFe0.5Mn0.5O3 belongs to $\Gamma_1\ (P6_3cm)$ which is supported by the strong intensity for the (100) reflection and also judging by the presence of spin-lattice coupling. The refined atomic positions for Lu and Mn/Fe indicate significant atomic displacements at $T_{\mathrm{N}}$ and $T_{\mathrm{SR}}$ which confirms strong spin-lattice coupling. Our results complement the discovery of room temperature multiferroicity in thin films of $h\text{LuFeO}_3$ and would give impetus to study LuFe1−x Mn x O3 systems as potential multiferroics where electric polarization is linked to giant atomic displacements. |
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| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Kumar, C. M. N. |b 2 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Pomjakushin, V. Y. |b 3 |
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| 773 | 1 | 8 | |a 10.1209/0295-5075/110/37007 |b : IOP Publishing, 2015-05-01 |n 3 |p 37007 |3 journal-article |2 Crossref |t EPL (Europhysics Letters) |v 110 |y 2015 |x 0295-5075 |
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