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The magnetic structure of YMnO<sub>3</sub>perovskite revisited
160
Citations
19
References
2002
Year
Magnetic PropertiesEngineeringLow-dimensional MagnetismMagnetic ResonanceMagnetic MaterialsSinusoidal Magnetic StructureMagnetismMultiferroicsQuantum MaterialsOrthorhombic Perovskite Ymno3Magnetic StructureMaterials SciencePhysicsPerovskite MaterialsMagnetoelasticityDistorted PerovskiteMagnetic MaterialCrystallographyLead-free PerovskitesSpintronicsFerromagnetismNatural SciencesCondensed Matter PhysicsApplied PhysicsMagnetic Property
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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