2012
DOI: 10.7452/lapl.201210024
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Continuous-wave Nd:GYSGG laser around 1.3 μm

Abstract: The operating characteristics of a Nd:GYSGG laser in the 1.3 µm wavelength band based on the transition 4 F 3/2 → 4 I 13/2 is demonstrated. Using two different output couplers, single wavelengths operation at 1336 nm and dual-wavelength operation at 1321/1336 nm are obtained. The 1329 nm laser spectrum is also found when the pump level is relatively weak. The stimulated emission cross section of the 1336 nm laser line is estimated to be 1.12 time of that of the 1321 nm laser line. The output power of 1.98 W at… Show more

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Cited by 17 publications
(8 citation statements)
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“…However, to achieve the 1.4 μm laser operation, stringent requirements should be fulfilled, such as a high-finesse cavity and good suppression of the 1.3 μm laser oscillation. The first Nd:GYSGG laser in the 1.3-1.35 μm wavelength range was reported in 2012 [31]. Using a diode-end-pumped plane-parallel cavity with different out-coupling efficiencies of 8.4 and 6.0%, single-wavelength operation at 1336 nm and dual-wavelength operation at 1321/1336 nm with a minor wavelength at 1330 nm were achieved with variable power proportions according to the pump intensity.…”
Section: Nd:gysgg Laser Operating In the 13-145 µM Rangementioning
confidence: 99%
See 1 more Smart Citation
“…However, to achieve the 1.4 μm laser operation, stringent requirements should be fulfilled, such as a high-finesse cavity and good suppression of the 1.3 μm laser oscillation. The first Nd:GYSGG laser in the 1.3-1.35 μm wavelength range was reported in 2012 [31]. Using a diode-end-pumped plane-parallel cavity with different out-coupling efficiencies of 8.4 and 6.0%, single-wavelength operation at 1336 nm and dual-wavelength operation at 1321/1336 nm with a minor wavelength at 1330 nm were achieved with variable power proportions according to the pump intensity.…”
Section: Nd:gysgg Laser Operating In the 13-145 µM Rangementioning
confidence: 99%
“…Although AO Q-switching is a conventional and preferred approach for generating stable laser pulses, passive Q-switching is sometimes superior due to its narrower pulse width and higher peak power with a much shorter cavity. As an excellent candidate for saturable absorbers working in the The first Nd:GYSGG laser in the 1.3-1.35 µm wavelength range was reported in 2012 [31]. Using a diode-end-pumped plane-parallel cavity with different out-coupling efficiencies of 8.4 and 6.0%, single-wavelength operation at 1336 nm and dual-wavelength operation at 1321/1336 nm with a minor wavelength at 1330 nm were achieved with variable power proportions according to the pump intensity.…”
Section: Nd:gysgg Laser Operating In the 13-145 µM Rangementioning
confidence: 99%
“…The laser characteristics researches of Nd:GYSGG have achieved great breakthrough, recently. For example, the continuous wave (CW), acousto‐optic (A‐O) and passively Q‐switch laser performance of Nd:GYSGG with dual‐wavelength output at 1061.5 nm and 1058.4 nm has been reported by K. Zhong et al . The mode‐lock laser performance of Nd:GYSGG with a single wavelength at 1061 nm has been demonstrated by B.Y.…”
Section: Introductionmentioning
confidence: 99%
“…Most recently, Xu reported the self-Qswitched dual-wavelength operation of the Yb: CGB crystal [18]. With an inhomogeneous broadening of the emission spectra, lower emission cross-sections (1.58 × 10 −19 cm 2 ), and longer upper laser level lifetime (220 μs), Nd:GYSGG crystal is beneficial to generate dual-wavelength and high energy Q-switched laser pulses [19,20]. However, there is no report about the SQS operation of the Nd:GYSGG crystal with dual-wavelength.…”
mentioning
confidence: 98%