TY - JOUR
T1 - Rotomagnetic coupling in fine-grained multiferroic BiFe O3
T2 - Theory and experiment
AU - Morozovska, Anna N.
AU - Eliseev, Eugene A.
AU - Glinchuk, Maya D.
AU - Fesenko, Olena M.
AU - Shvartsman, Vladimir V.
AU - Gopalan, Venkatraman
AU - Silibin, Maxim V.
AU - Karpinsky, Dmitry V.
N1 - Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/4/27
Y1 - 2018/4/27
N2 - Using Landau-Ginzburg-Devonshire (LGD) theory for BiFeO3 dense fine-grained ceramics with quasispherical grains and nanosized intergrain spaces enriched by elastic defects, we calculated a surprisingly strong size-induced increase in the antiferromagnetic transition temperature caused by the joint action of rotomagnetic and magnetostrictive coupling. Notably, all parameters included in the LGD functional have been extracted from experiments, not assumed. Complementarily, we performed experiments for dense BiFeO3 ceramics, which revealed that the shift of the antiferromagnetic transition is to TN∼690K instead of TN∼645K for a single crystal. To explain the result theoretically, we consider the possibility of controlling the antiferromagnetic state of multiferroic BiFeO3 via biquadratic antiferrodistortive rotomagnetic, rotoelectric, magnetoelectric, and magnetostrictive couplings. According to our calculations, the highest contribution is the rotostriction contribution, while the magnetostrictive and electrostriction contributions appear smaller.
AB - Using Landau-Ginzburg-Devonshire (LGD) theory for BiFeO3 dense fine-grained ceramics with quasispherical grains and nanosized intergrain spaces enriched by elastic defects, we calculated a surprisingly strong size-induced increase in the antiferromagnetic transition temperature caused by the joint action of rotomagnetic and magnetostrictive coupling. Notably, all parameters included in the LGD functional have been extracted from experiments, not assumed. Complementarily, we performed experiments for dense BiFeO3 ceramics, which revealed that the shift of the antiferromagnetic transition is to TN∼690K instead of TN∼645K for a single crystal. To explain the result theoretically, we consider the possibility of controlling the antiferromagnetic state of multiferroic BiFeO3 via biquadratic antiferrodistortive rotomagnetic, rotoelectric, magnetoelectric, and magnetostrictive couplings. According to our calculations, the highest contribution is the rotostriction contribution, while the magnetostrictive and electrostriction contributions appear smaller.
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U2 - 10.1103/PhysRevB.97.134115
DO - 10.1103/PhysRevB.97.134115
M3 - Article
AN - SCOPUS:85046821178
SN - 2469-9950
VL - 97
JO - Physical Review B
JF - Physical Review B
IS - 13
M1 - 134115
ER -