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Jahn‐teller structure in <sup>3</sup>A<sub>2</sub>(<sup>3</sup>F) → <sup>3</sup>T<sub>1</sub> (<sup>3</sup>F) absorption band of CdS:Ti<sup>2+</sup>
31
Citations
19
References
1971
Year
Jahn‐teller StructureEngineeringElectronic StructureSemiconductorsAbsorption BandIi-vi SemiconductorType Vibrational ModesQuantum MaterialsTi 2+Materials ScienceQuantum SciencePhysicsPhysical ChemistryQuantum SolidQuantum ChemistrySolid-state PhysicTransition Metal ChalcogenidesNatural SciencesPhonon Energy 3.3Applied PhysicsCondensed Matter PhysicsPhonon
Abstract The absorption spectrum of Ti 2+ centres in CdS betwccn 0.3 and 1.5 eV is measured in the temperature range 10 to 295 °K The spectrum can be explained on the basis of crystal‐field theory. A detailed analysis of the temperature dependence of the 3 A 2 , → 3 T 1 ( 3 F) band shows that the triplet structure of this band is due to strong interaction with τ 2 type vibrational modes of phonon energy 3.3 meV. This analysis is based on the theory of Toyozawa and Inoue [6] and the method of moments of Henry et al. [14]. Effects of the autoionization of the 3 T 1 state (which has been shown to be located in the conduction band [13]) are believed to be seen at low temperatures.
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