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Dynamic Behavior of the Jahn−Teller Distorted Cu(H<sub>2</sub>O)<sub>6</sub><sup>2+</sup> Ion in Cu<sup>2+</sup> Doped Cs<sub>2</sub>[Zn(H<sub>2</sub>O)<sub>6</sub>](ZrF<sub>6</sub>)<sub>2</sub> and the Crystal Structure of the Host Lattice
42
Citations
15
References
2002
Year
Crystal StructureEngineeringTemperature DependenceSolid-state ChemistryChemistryIi-vi SemiconductorDynamic BehaviorSuperconductivityQuantum MaterialsSimilar LatticesMaterials ScienceInorganic ChemistryPhysicsCrystalline DefectsPhysical ChemistryDefect FormationElemental MetalCrystallographySolid-state PhysicCrystal Structure DesignTransition Metal ChalcogenidesHost LatticeNatural SciencesApplied PhysicsCondensed Matter Physics
The temperature dependence of the X- and Q-band EPR spectra of Cs(2)[Zn(H(2)O)(6)](ZrF(6))(2) containing approximately 1% Cu(2+) is reported. All three molecular g-values vary with temperature, and their behavior is interpreted using a model in which the potential surface of the Jahn-Teller distorted Cu(H(2)O)(6)(2+) ion is perturbed by an orthorhombic "strain" induced by interactions with the surrounding lattice. The strain parameters are significantly smaller than those reported previously for the Cu(H(2)O)(6)(2+) ion in similar lattices. The temperature dependence of the two higher g-values suggests that in the present compound the lattice interactions change slightly with temperature. The crystal structure of the Cs(2)[Zn(H(2)O)(6)](ZrF(6))(2) host is reported, and the geometry of the Zn(H(2)O)(6)(2+) ion is correlated with lattice strain parameters derived from the EPR spectrum of the guest Cu(2+) complex.
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