Journal of Physics Condensed Matter · 2002 · 161 citations · 19 references
Natural SciencesMaterials EngineeringMaterials ScienceCondensed Matter PhysicsCrystal StructureMagnetic MaterialsAntiferromagnetismMagnetic OxidesMagnetic Properties Of SolidsMagnetism In SolidsMagnetism Of Inorganic CompoundsPerovskite MaterialsMagnetic PerovskitesMagnetic Structure DeterminationMagnetic Sublattice StructureOxide PerovskitesPerovskite Crystal StructurePerovskite GroupPolycrystalline MaterialsTemperature-dependent Ordering
The magnetic structure of the orthorhombic perovskite YMnO3 has been investigated. A study on a polycrystalline sample based on neutron diffraction data and magnetization measurements has shown that YMnO3 becomes magnetically ordered below TN = 42 K. In the space group Pnma, the sinusoidal magnetic structure is defined by a (Cx,0,0) mode and characterized by the propagation vector k = (kx,0,0). The kx-component increases from 0.420(4), immediately below the ordering temperature, to 0.435(2) at T = 28.7 K. Below 28 K the kx-component remains unchanged. The sinusoidal spin arrangement remains stable down to 1.7 K; at this temperature the amplitude of the sinusoid is Ak = 3.89(6) µB. YMnO3 is the most distorted perovskite of the RMnO3 series (R = rare earths); the observed sinusoidal magnetic structure is in contrast with those exhibited by the less-distorted members (i.e. LaMnO3), which are commensurate-type antiferromagnetic structures.
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Ferromagnetic compounds of manganese with perovskite structure
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