TY - JOUR
T1 - Microscopic model and phase diagrams of the multiferroic perovskite manganites
AU - Mochizuki, Masahito
AU - Furukawa, Nobuo
PY - 2009/10/19
Y1 - 2009/10/19
N2 - Orthorhombically distorted perovskite manganites, RMn O3 with R being a trivalent rare-earth ion, exhibit a variety of magnetic and electric phases including multiferroic (i.e., concurrently magnetic and ferroelectric) phases and fascinating magnetoelectric phenomena. We theoretically study the phase diagram of RMn O3 by constructing a microscopic spin model, which includes not only the superexchange interaction but also the single-ion anisotropy (SIA) and the Dzyaloshinsky-Moriya interaction (DMI). Analysis of this model using the Monte Carlo method reproduces the experimental phase diagrams as functions of the R -ion radius, which contain two different multiferroic states, i.e., the ab -plane spin cycloid with ferroelectric polarization P□a and the bc -plane spin cycloid with P□c. The orthorhombic lattice distortion or the second-neighbor spin exchanges enhanced by this distortion exquisitely controls the keen competition between these two phases through tuning the SIA and DMI energies. This leads to a lattice-distortion-induced reorientation of P from a to c in agreement with the experiments. We also discuss spin structures in the A -type antiferromagnetic state, those in the cycloidal spin states, origin and nature of the sinusoidal collinear spin state, and many other issues.
AB - Orthorhombically distorted perovskite manganites, RMn O3 with R being a trivalent rare-earth ion, exhibit a variety of magnetic and electric phases including multiferroic (i.e., concurrently magnetic and ferroelectric) phases and fascinating magnetoelectric phenomena. We theoretically study the phase diagram of RMn O3 by constructing a microscopic spin model, which includes not only the superexchange interaction but also the single-ion anisotropy (SIA) and the Dzyaloshinsky-Moriya interaction (DMI). Analysis of this model using the Monte Carlo method reproduces the experimental phase diagrams as functions of the R -ion radius, which contain two different multiferroic states, i.e., the ab -plane spin cycloid with ferroelectric polarization P□a and the bc -plane spin cycloid with P□c. The orthorhombic lattice distortion or the second-neighbor spin exchanges enhanced by this distortion exquisitely controls the keen competition between these two phases through tuning the SIA and DMI energies. This leads to a lattice-distortion-induced reorientation of P from a to c in agreement with the experiments. We also discuss spin structures in the A -type antiferromagnetic state, those in the cycloidal spin states, origin and nature of the sinusoidal collinear spin state, and many other issues.
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U2 - 10.1103/PhysRevB.80.134416
DO - 10.1103/PhysRevB.80.134416
M3 - Article
AN - SCOPUS:70749130155
VL - 80
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
SN - 0163-1829
IS - 13
M1 - 134416
ER -