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Mechanism of a population inversion between the<sup>4</sup><i>I</i><sub>11/2</sub>and<sup>4</sup><i>I</i><sub>13/2</sub>levels of the Er<sup>3+</sup>ion in Y<sub>3</sub>AI<sub>5</sub>O<sub>12</sub>crystals
20
Citations
1
References
1980
Year
EngineeringNuclear PhysicsAbsorption SpectroscopyElectronic Excited StateOptical PropertiesPopulation InversionBiophysicsPhotoluminescencePhysicsAtomic PhysicsEr3+ CrystalsCrystallographyStark ComponentsExcited State PropertyEr3+ IonNatural SciencesSpectroscopyCondensed Matter PhysicsApplied Physics
Studies of the spectra of stimulated emission from Y3AI5O12:Er3+ crystals (4I11/2–4I13/2) containing 20 wt.% activator ions, showed that, as the temperature decreased from 300 to 77°K, a change was observed in the emission wavelength (at T = 300°K it was found that λ1 = 2.9364 μλ2 = 2.8310μ and at T = 77°K it was found that λ1 = 2.6930 μ, λ2 = 2.8970 μ). This could not be attributed to a thermal redistribution of the populations of the Stark components of the 4I11/2 and 4I13/2 upper and lower active levels. An analysis of the results showed that the temperature shift of the stimulated emission spectrum was due to changes in the processes of relaxation of excitation from the upper levels of the Er3+ ion which caused substantial changes in the populations of the 4I11/2 and 4I13/2 multiplets.
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