2011
DOI: 10.1002/lapl.201110041
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Continuous-wave green thin-disk laser at 524 nm based on frequency-doubled diode-pumped Yb:GSO crystal

Abstract: We report what is believed to be the first demonstration of diode-pumped continuous-wave (CW) thin-disk Yb3+-doped Gd2SiO5 (Yb:GSO) laser at 1048 nm. With a 3.8% output coupler, the maximum output power is 1.38 W under a pump power of 17.8 W. Moreover, intracavity second-harmonic generation (SHG) has also been achieved with a power of 337 mW at 524 nm by using a LiB3O5 (LBO) nonlinear crystal. At the output power level of 337 mW, the green power stability is better than 5% and the ellipticity of spot is 0.97.

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Cited by 8 publications
(5 citation statements)
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“…The generation of ultrashort laser pulses in the visible, particularly the green, has always been of great interest, owing to its vast potential for industrial and scientific applications [2], including pumping of ultrafast optical parametric oscillators [3]. In the absence of suitable laser gain media, the development of high-power green sources over the past 50 years has relied almost exclusively on SHG in various birefringent [4][5][6][7][8][9][10] and quasi-phase-matched (QPM) [11] nonlinear materials. Although QPM nonlinear crystals such as periodically poled KTiOPO 4 and MgO-doped stoichiometric LiTaO 3 , with high nonlinearity (d eff ∼ 9 pm V −1 ) and long interaction lengths up to 30 mm, have been successfully deployed in single-pass configuration to generate high-power single-frequency green radiation in the continuous-wave (cw) regime [12][13][14], the narrow spectral acceptance bandwidth for SHG (∼0.25 nm • cm) limits the useful interaction length, precluding their use in the ultrafast regime, where large spectral bandwidths are involved.…”
Section: Introductionmentioning
confidence: 99%
“…The generation of ultrashort laser pulses in the visible, particularly the green, has always been of great interest, owing to its vast potential for industrial and scientific applications [2], including pumping of ultrafast optical parametric oscillators [3]. In the absence of suitable laser gain media, the development of high-power green sources over the past 50 years has relied almost exclusively on SHG in various birefringent [4][5][6][7][8][9][10] and quasi-phase-matched (QPM) [11] nonlinear materials. Although QPM nonlinear crystals such as periodically poled KTiOPO 4 and MgO-doped stoichiometric LiTaO 3 , with high nonlinearity (d eff ∼ 9 pm V −1 ) and long interaction lengths up to 30 mm, have been successfully deployed in single-pass configuration to generate high-power single-frequency green radiation in the continuous-wave (cw) regime [12][13][14], the narrow spectral acceptance bandwidth for SHG (∼0.25 nm • cm) limits the useful interaction length, precluding their use in the ultrafast regime, where large spectral bandwidths are involved.…”
Section: Introductionmentioning
confidence: 99%
“…In addition, Yb 3+ doped media have broader absorp tion spectrum and broader emission bandwidths. The Yb 3+ doped oxy orthosilicates crystals have been real ized to exhibit excellent broadband performance, large ground state splitting and high thermal conduc tivity [3][4][5][6][7]. Efficient mode locked laser operations have already been demonstrated in numerous of Yb 3+ doped materials [8][9][10][11][12][13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…Yb 3+ doped crystals are highly suitable for use as gain media for ultrafast lasers. Until now, various diode pumped Yb-doped continuous-wave and ultrafast lasers have been demonstrated [27][28][29][30]. A promising ytterbium-doped alloyed oxyorthosilicate crystal Yb:LuYSiO 5 (Yb:LYSO) exhibits combined advantages of both Yb:LSO and Yb:YSO crystals, such as large ground-state splittings, broad absorption and emission spectra and excellent mechanical property.…”
Section: Introductionmentioning
confidence: 99%