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Magnetic susceptibilities, their temperature variation, and exchange constants of NiO
83
Citations
14
References
1984
Year
Magnetic PropertiesEngineeringPowder SampleMagnetic ResonanceChemistryMagnetic MaterialsMagnetoresistanceMagnetismSingle CrystalExchange ConstantsThermodynamicsMaterials SciencePhysicsMagnetic SusceptibilitiesMagnetic MaterialCrystallographyFerromagnetismHigh Temperature MaterialsNatural SciencesCryogenicsApplied PhysicsCondensed Matter PhysicsMagnetic Property
The temperature variation of the magnetic susceptibilities of NiO for a powder sample and a single crystal has been measured from 4.2 to 700 K. The single crystal was stressed along a $〈111〉$ direction on cooling through ${T}_{N}$ (=524 K) with successive stress magnitudes of 7, 30, and 42 bars, followed in each case by measurements of ${\ensuremath{\chi}}_{\ensuremath{\parallel}}^{*}$ [$\stackrel{\ensuremath{\rightarrow}}{\mathrm{H}}$ parallel to a (111) plane with $H=200$ Oe] from 4.2 to 700 K. From the behavior of ${\ensuremath{\chi}}_{\ensuremath{\parallel}}^{*}$ with stress, a stress of 30 bars was found to be sufficient to completely remove the $T$ domains. With the use of the data of initial powder susceptibility ${\ensuremath{\chi}}_{p}=\frac{({\ensuremath{\chi}}_{\ensuremath{\parallel}}+{2\ensuremath{\chi}}_{\ensuremath{\perp}})}{3}$ and ${\ensuremath{\chi}}_{\ensuremath{\parallel}}^{*}=\frac{({\ensuremath{\chi}}_{\ensuremath{\parallel}}+{\ensuremath{\chi}}_{\ensuremath{\perp}})}{2}$ at various temperatures, the temperature variation of ${\ensuremath{\chi}}_{\ensuremath{\parallel}}$ and ${\ensuremath{\chi}}_{\ensuremath{\perp}}$, the principal susceptibilities, is determined. After correcting for ${\ensuremath{\chi}}_{\mathrm{vv}}$ and ${\ensuremath{\chi}}_{d}$ (the Van Vleck and diamagnetic susceptibilities) with ${\ensuremath{\chi}}_{\mathrm{vv}}+{\ensuremath{\chi}}_{d}=3.2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$ ${\mathrm{cm}}^{3}$/g, $\ensuremath{\chi}({T}_{N})=8.8\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$ ${\mathrm{cm}}^{3}$/g, ${\ensuremath{\chi}}_{\ensuremath{\perp}}(0)=6.8\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$ ${\mathrm{cm}}^{3}$/g, and ${\ensuremath{\chi}}_{\ensuremath{\parallel}}(0)=0$ are determined. It is shown that the spin-wave theory correctly gives the ratio $\frac{\ensuremath{\chi}({T}_{N})}{{\ensuremath{\chi}}_{\ensuremath{\perp}}(0)}$ and the temperature dependence of ${\ensuremath{\chi}}_{\ensuremath{\parallel}}$ to about 200 K if the experimental value of the spin reduction $\ensuremath{\Delta}S=0.19$ is used for ${\mathrm{Ni}}^{2+}$. From the experimental values of $\ensuremath{\chi}({T}_{N})$ and ${T}_{N}$ and the use of random-phase-approximation Green's-function theory, the magnitudes of exchange constants for NiO, viz. ${J}_{1}=34$ K and ${J}_{2}=202$ K, are determined.
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