2006
DOI: 10.1364/oe.14.003282
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Continuous-wave ultraviolet generation at 320 nm by intracavity frequency doubling of red-emitting Praseodymium lasers

Abstract: We describe a new approach for the generation of coherent ultraviolet radiation. Continuous-wave ultraviolet light at 320 nm has been obtained by intracavity frequency doubling of red-emitting Praseodymium lasers. Lasing at the 640-nm fundamental wavelength in Pr:LiYF(4) and Pr:BaY(2)F(8) was realized by employing an optically pumped semiconductor laser at 480 nm as pump source.Using LiB(3)O(5) as nonlinear medium, ~19 mW of ultraviolet radiation with ~9% optical efficiency with respect to absorbed power was r… Show more

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Cited by 84 publications
(33 citation statements)
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“…Figure 2a shows the onset of inhibition in WG I is at pump power of ∼0.4 W. Figure 2b shows the onset of inhibition in WG II is around a pump power of 0.3 W. Figure 2c shows the onset of inhibition in WG III is much lower, at a pump power of ∼0.24 W. It can be seen that for WG I, WG II and WG III, below the threshold pump power of inhibition, the maximum SHG power are 0.286, 0.226 and 0.195 W, which corresponds to conversion efficiencies of 71.5, 75.3 and 81.2 %, respectively. It is clear that the conversion efficiencies of the present proposal based on PPMgLN waveguides are predicted to be significantly higher than the reported results based on LBO crystals (Richter et al 2006). As the inhibition in WG I is relatively weaker than that in WG II and WG III, the maximum SHG power generated in WG I can reach 0.571 W which is apparently higher than that in WG II and WG III.…”
Section: Theoretical Modelcontrasting
confidence: 80%
“…Figure 2a shows the onset of inhibition in WG I is at pump power of ∼0.4 W. Figure 2b shows the onset of inhibition in WG II is around a pump power of 0.3 W. Figure 2c shows the onset of inhibition in WG III is much lower, at a pump power of ∼0.24 W. It can be seen that for WG I, WG II and WG III, below the threshold pump power of inhibition, the maximum SHG power are 0.286, 0.226 and 0.195 W, which corresponds to conversion efficiencies of 71.5, 75.3 and 81.2 %, respectively. It is clear that the conversion efficiencies of the present proposal based on PPMgLN waveguides are predicted to be significantly higher than the reported results based on LBO crystals (Richter et al 2006). As the inhibition in WG I is relatively weaker than that in WG II and WG III, the maximum SHG power generated in WG I can reach 0.571 W which is apparently higher than that in WG II and WG III.…”
Section: Theoretical Modelcontrasting
confidence: 80%
“…Recent reports [35][36][37] demonstrated efficient, room temperature visible lasing in several Pr-activated fluoride crystals under direct GaN diode laser pumping. It seems that further development of GaN-based semiconductor lasers emitting at wavelengths between 350 and 450 nm will allow to more efficiently exploit the potential of Pr 3+ -doped solidstate lasers.…”
Section: Discussionmentioning
confidence: 99%
“…As an example, initial experiments were performed on intracavity frequency doubling of 546 nm to 273 nm [115] and 698 nm to 349 nm [116]. Besides Pr 3+ :LiLuF 4 [117], frequency doubling of Pr 3+ -lasers in other host materials such as Pr 3+ :KY 3 F 10 [118], Pr 3+ :BaY 2 F 8 [87], and Pr 3+ :YAlO 3 [119] did not result in efficient generation of coherent UV radiation, yet. However, this should not be a general issue of these host materials.…”
Section: Figure 13mentioning
confidence: 99%