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Cycloidal Spin Order in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>a</mml:mi></mml:math>-Axis Polarized Ferroelectric Phase of Orthorhombic Perovskite Manganite
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2008
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EngineeringSpin SystemsSpin TexturesMagnetic ResonanceOrthorhombic Perovskite Rmno3Spintronic MaterialSpin DynamicMagnetic MaterialsSpin PhenomenonCycloidal Spin OrderSpin Spiral PlaneMagnetismMultiferroicsMath XmlnsFerroelectric ApplicationQuantum MaterialsSpin PhysicsMaterials ScienceSpin-orbit EffectsOrthorhombic Perovskite ManganitePhysicsCrystallographySpintronicsNatural SciencesCondensed Matter PhysicsApplied PhysicsBc-spiral Plane
The ferroelectric state in an orthorhombic perovskite RMnO3 (R=Gd0.7Tb0.3) was proved by neutron scattering studies to show the cycloidal spin state with the ab-spiral plane and the spin-helicity dependent polarization vector along the a axis, sharing the microscopic origin (inverse Dzyaloshinskii-Moriya interaction) with the more widely observed P||c state (e.g., for R=Tb and Dy) with the bc-spiral plane. The magnetic-field induced polarization flop from P||c to P||a as well known for RMnO3 is thus assigned to the orthogonal flop of the spin spiral plane from bc to ab.
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