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8B7 - Energy transfer and CW laser action in Ho<sup>3+</sup>:Er<sub>2</sub>O<sub>3</sub>
18
Citations
3
References
1966
Year
EngineeringLaser ScienceLaser ApplicationsLaser PhysicsLaser MaterialSuper-intense LasersHigh-power LasersOptical PropertiesOptical PumpingPhotonicsLaser PumpingPhysicsCrystal MaterialEnergy TransferAtomic PhysicsCrystallographyUnusual Laser MaterialLong CrystalDominant Pumping MechanismApplied PhysicsCrystalsHigh-energy Lasers
Er <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</inf> O <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</inf> : Ho <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3+</sup> is an unusual laser material in that the host crystal itself provides the dominant pumping mechanism by means of energy transfer. The additional pumping bands due to Er <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3+</sup> and the consequent efficient transfer of energy to the Ho <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3+</sup> laser ion lead to relatively low threshold laser operation: 5 joules pulsed and 200W CW for a 12mm long crystal at 77°K. The emission waveleng this 2.121μ, a region of good atmospheric transmission. Additional laser experiments were carried out at 145°K. Excitation and fluorescence spectra are discussed.
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