Magnetoelectric coupling at the interface of BiFeO3/La0.7Sr0.3MnO3 multilayers
arXiv:1012.1448 · doi:10.1103/PhysRevB.84.024422
Abstract
Electric-field controlled exchange bias in a heterostructure composed of the ferromagnetic manganite La0.7Sr0.3MO3 and the ferroelectric antiferromagnetic BiFeO3 has recently been demonstrated experimentally. By means of a microscopic model Hamiltonian we provide a possible explanation of the origin of this magnetoelectric coupling. We find, in agreement with experimental results, a net ferromagnetic moment at the BiFeO3 interface. The induced ferromagnetic moment is the result of the competition between the e_g-electrons double exchange and the t_2g-spins antiferromagnetic superexchange that dominate in bulk BiFeO3. The balance of these simultaneous ferromagnetic and antiferromagnetic tendencies is strongly affected by the interfacial electronic charge density which, in turn, can be controlled by the BiFeO3 ferroelectric polarization.
4 pages, including 4 figures
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Cited by in corpus (10)
- Induced magnetization in LaSrMnO/BiFeO superlattices
- The effect of interface roughness on exchange bias in La0.7Sr0.3MnO3 - BiFeO3 heterostructures
- Quantum-Confinement-Induced Magnetism in LaNiO-LaMnO Superlattices
- Microscopic model for the ferroelectric field effect in oxide heterostructures
- Magnetic properties of La(0.67)Sr(0.33)MnO3/BiFeO3(001) heterojunctions: chemically abrupt versus atomic intermixed interface
- Polaronic transport induced by competing interfacial magnetic order in a LaCaMnO/BiFeO heterostructure
- Room temperature large spontaneous exchange bias in hard-soft antiferromagnetic composite BiFeO3-TbMnO3
- The role of disorder in NaO and its implications for Na-O batteries
- A Real Space Description of Magnetic Field Induced Melting in the Charge Ordered Manganites: I. The Clean Limit
- A Real Space Description of Field Induced Melting in the Charge Ordered Manganites: II. the Disordered Case