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Electronic Structure of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>F</mml:mi></mml:math>Centers: Hyperfine Interactions in Electron Spin Resonance
170
Citations
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References
1953
Year
EngineeringNuclear PhysicsNuclear Magnetic MomentsMagnetic ResonanceAtomic OrbitalsSpin DynamicElectronic StructureSpin PhenomenonElectron PhysicMath XmlnsQuantum MaterialsSpin PhysicsPhysicsNuclear TheoryAtomic PhysicsQuantum MagnetismMicrowave SpectroscopySpintronicsNatural SciencesElectron Spin ResonanceApplied PhysicsCondensed Matter PhysicsObserved WidthIon Structure
It is shown that the observed width of the microwave electron spin resonance absorption lines associated with $F$ centers in KCl, NaCl, and KBr crystals can be attributed to hyperfine interactions between the $F$-center electron and the nuclear magnetic moments of the ions adjacent to the $F$ center. The width arises from the distribution of nuclear moment components. Theoretical calculations of the width are in good agreement with observation provided that the $F$-center wave function is treated as a linear combination of atomic orbitals; wave functions calculated on continuum models are shown to be unsatisfactory. The theory is confirmed by a comparison of observations on $F$ centers in crystals of ${\mathrm{K}}^{39}$Cl and ${\mathrm{K}}^{41}$Cl. If the width is attributed to interactions with the nearest sets of K and Cl ions, the experiments lead directly to quantitative values of the electronic charge density at the K and Cl nuclei: one finds ${|\ensuremath{\Psi}(\mathrm{K})|}^{2}=0.70\ifmmode\times\else\texttimes\fi{}{10}^{24}$ ${\mathrm{cm}}^{\ensuremath{-}3}$ and ${|\ensuremath{\Psi}(\mathrm{Cl})|}^{2}=0.12\ifmmode\times\else\texttimes\fi{}{10}^{24}$ ${\mathrm{cm}}^{\ensuremath{-}3}$.
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