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Magnetic studies of some orthovanadates
134
Citations
13
References
1995
Year
EngineeringMagnetic ResonanceMagnetic StudiesSpintronic MaterialSpin DynamicSpin PhenomenonMagnetic MaterialsMagnetismQuantum MaterialsPerovskites LPhase ChangePhysicsMagnetic MeasurementQuantum MagnetismRoom TemperatureNatural SciencesApplied PhysicsCondensed Matter PhysicsMagnetic PropertyMagnetic Field
The perovskites L${\mathrm{VO}}_{3}$ (L=La, Lu, or Y) are canted-spin antiferromagnets. Magnetic susceptibility measurements made on cooling from room temperature in a field of 1 kOe or on heating after cooling in 1 kOe give rise to a sample magnetization M that is oriented in opposition to the magnetizing field below 138 K in ${\mathrm{LaVO}}_{3}$, but in the direction of the magnetizing field in ${\mathrm{LuVO}}_{3}$ and ${\mathrm{YVO}}_{3}$. Orientation of the M in ${\mathrm{LaVO}}_{3}$ in opposition to the magnetizing field H occurs on cooling through a first-order magneto- strictive transition at 138 K${\mathit{T}}_{\mathit{N}}$\ensuremath{\approxeq}142 K that enhances the ${\mathit{V}}^{3+}$ ion orbital angular momentum. In ${\mathrm{YVO}}_{3}$, a first-order magnetic-order phase change at 78 K ${\mathit{T}}_{\mathit{N}}$\ensuremath{\approxeq}114 K shows no evidence of a discontinuous change in the ${\mathrm{V}}^{3+}$ ion orbital angular momentum. The same is true for a phase change in ${\mathrm{LuVO}}_{3}$ at 83 K${\mathit{T}}_{\mathit{N}}$\ensuremath{\approxeq}105 K that leaves the magnetic order unchanged. A high-pressure (P\ensuremath{\ge}8 kbar) ${\mathrm{LaVO}}_{3}$ phase metastable below 250 \ifmmode^\circ\else\textdegree\fi{}C is antiferromagnetic without spin canting. The ``anomalous diamagnetism'' previously reported for field-cooled ${\mathrm{LaVO}}_{3}$ is interpreted to reflect the first observation of a change in the direction of the persistent currents at an ion associated with a discontinuous change in an unquenched orbital angular momentum contribution to the atomic moment; a spin-orbit coupling stronger than the Zeemann coupling of the spin to the magnetizing field reverses the entire atomic moment ${\mathrm{\ensuremath{\mu}}}_{\mathit{J}}$=gJ${\mathrm{\ensuremath{\mu}}}_{\mathit{B}}$. Substitution of La by Lu or Y applies a chemical pressure that suppresses the first-order magnetostrictive distortion responsible for the anomalous diamagnetism.
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