Physical Review · 1967 · 26 citations · 42 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsMagnetic MaterialsSpectroscopyCurie TemperatureElectron Spin Resonance SpectroscopyMagnetic SusceptibilityRelaxation MechanismsKerr EffectLongitudinal RelaxationMagnetic Field DependenceMagnetic Field Dependence Of RelaxationMagnetic RelaxationNuclear Magnetic Resonance RelaxationSpin RelaxationTransverse Relaxation Time
Magnetic relaxation in nickel above the Curie temperature (354\ifmmode^\circ\else\textdegree\fi{}C) has been studied up to a temperature of 450\ifmmode^\circ\else\textdegree\fi{}C. The spin-relaxation rate $\frac{1}{{\ensuremath{\tau}}_{r}}$, which is equal to the magnetic resonance half-width $\ensuremath{\Delta}\ensuremath{\omega}=\ensuremath{\gamma}\ensuremath{\Delta}H$, is determined from the field dependence of the microwave Kerr rotation. We fit the relaxation to an expression: $\frac{1}{{\ensuremath{\tau}}_{r}}=3(\frac{C}{T})(\frac{H}{M})\ensuremath{\omega}_{d}^{}{}_{}{}^{2}{\ensuremath{\tau}}_{c}$, where $C$ is the Curie constant, $T$ the absolute temperature, $\frac{M}{H}$ the transverse static susceptibility, ${\ensuremath{\omega}}_{d}$ the pseudodipolar coupling frequency, and ${\ensuremath{\tau}}_{c}$ the spin correlation time. At high temperatures, ${\ensuremath{\tau}}_{c}$ is constant and is set equal to $\frac{1}{{\ensuremath{\omega}}_{e}}$, the reciprocal exchange frequency, by a suitable choice of ${\ensuremath{\omega}}_{d}$. As the temperature is dropped below 420\ifmmode^\circ\else\textdegree\fi{}C, ${\ensuremath{\tau}}_{c}$ begins to increase as ${(T\ensuremath{-}{T}_{c})}^{\frac{\ensuremath{-}2}{3}}$. This increase in ${\ensuremath{\tau}}_{c}$ is compatible with critical-neutron-scattering studies of nickel and with measurements of the static susceptibility. Below 385\ifmmode^\circ\else\textdegree\fi{}K, ${\ensuremath{\tau}}_{c}$ remains constant at a value 1.8 times the high-temperature value. It is believed that the development of spin-wave excitations in this temperature range prevents a further increase in the spin correlation time. A shift in the spectroscopic splitting factor from $g=2.22$ below ${T}_{c}$ to $g=2.29$ above ${T}_{c}$ is observed. Well above ${T}_{c}$, a small amount of Kerr rotation, which is associated with the Hall effect, is observed. The magnitude of this rotation is consistent with the results of dc studies.
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Demagnetizing Factors of the General Ellipsoid
J. A. Osborn · Physical Review · 1945 · 2.3K citations
Natural Sciences, Electrical Engineering, Computational Geometry +7
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P. W. Anderson · Reviews of Modern Physics · 1953 · 1.3K citations
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J. S. Kouvel, Michael E. Fisher · Physical Review · 1964 · 1.3K citations
Progress in Low Temperature Physics.
Donald H. Andrews · Journal of the American Chemical Society · 1956 · 1.1K citations