2006
DOI: 10.1016/j.jcrysgro.2006.04.020
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Advances in growth of fiber crystal by the LHPG technique. Application to the optimization of Yb3+-doped CaF2 laser crystals

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Cited by 16 publications
(9 citation statements)
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“…G=exp[σ g σ a Nτ(N)l] [9] where σ g is the gain cross-section with respect to the quasi three-level situation for lasers between first excited and ground state, σ a is the pump absorption cross-section for the pumping wavelength, whereas N , τ(N) and l have been defined above.…”
Section: Model Approach For Optimization Of Laser Crystalsmentioning
confidence: 99%
“…G=exp[σ g σ a Nτ(N)l] [9] where σ g is the gain cross-section with respect to the quasi three-level situation for lasers between first excited and ground state, σ a is the pump absorption cross-section for the pumping wavelength, whereas N , τ(N) and l have been defined above.…”
Section: Model Approach For Optimization Of Laser Crystalsmentioning
confidence: 99%
“…The LHPG technique is based on the utilization of a CO 2 laser beam as the heating source. Limited by the laser power, the source rod is typically 0.5-1 mm in diameter [19], so this method is always adapted to explore new laser crystals. Unfortunately there are some materials that LHPG method is not suitable to be used as a growth technique, due to thermodynamic or kinetic consideration.…”
Section: Introductionmentioning
confidence: 99%
“…In our previous studies, Ca 1-x Yb x F 2þx crystals were grown by either simple melting or by laser heated pedestal growth (LHPG) technique (Ito et al, 2004;Boulon et al, 2006) under Ar atmosphere by growing Yb 3þ concentration gradient fiber in order to understand involved concentration quenching mechanisms. In addition, high-quality large size crystals (more than 10 inches) have also been grown by Czochralski technique under CF 4 atmosphere (Jouini et al, 2008).…”
Section: Introductionmentioning
confidence: 99%