Roles of Bond Alternation in Magnetic Phase Diagram of RMnO3
arXiv:1006.3996 · doi:10.1143/JPSJ.79.033708
Abstract
In order to investigate nature of the antiferromagnetic structures in perovskite RMnO3, we study a Heisenberg J1-J2 model with bond alternation using analytical and numerical approaches. The magnetic phase diagram which includes incommensurate spiral states and commensurate collinear states is reproduced. We discuss that the magnetic structure with up-up-down-down spin configuration (E-type structure) and the ferroelectricity emerge cooperatively to stabilize this phase. Magnetoelastic couplings are crucial to understand the magnetic and electric phase diagram of RMnO3.
arXiv comment5 pages, 6 figures
References in corpus (10)
- Spin current and magneto-electric effect in non-collinear magnets
- Ferroelectricity in spiral magnets
- Role of the Dzyaloshinskii-Moriya interaction in multiferroic perovskites
- Distorted Perovskite with e_g^1 Configuration as a Frustrated Spin System
- Ferroelectricity in the Magnetic E-Phase of Orthorhombic Perovskites
- Collinear-to-Spiral Spin Transformation without Changing Modulation Wavelength upon Ferroelectric Transition in Tb1-xDyxMnO3
- Origin of electromagnon excitations in \textit{R}MnO
- Microscopic Model and Phase Diagrams of the Multiferroic Perovskite Manganites
- Origin of the multiferroic spiral spin-order in the RMnO3 perovskites
- Frustrated classical Heisenberg model in 1 dimension with added nearest-neighbor biquadratic exchange interactions
Cited by in corpus (4)
- Perovskite Manganites Hosting Versatile Multiferroic Phases with Symmetric and Antisymmetric Exchange Strictions
- Theory of spin-phonon coupling in multiferroic Mn perovskites
- Single-axis dependent structural and multiferroic properties of orthorhombic RMnO (R = Gd - Lu)
- Modeling and Physics of Multiferroic Perovskite Manganites