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1.
We report for the first time a continuous-wave (CW) coherent radiation at 480 nm by intracavity sum-frequency generation of 900 nm Neodymium Doped Strontium and Lanthanum Aluminate (Nd:ASL) laser and 1030 nm Yb:Y3Al5O12 (Yb:YAG) laser. Blue laser is obtained by using a doubly cavity, type-I critical phase matching LiB3O5 (LBO) crystal sum-frequency mixing. With total pump power of 28.6 W, the blue laser at 480 nm of 170 mW is obtained. At the output power level of 170 mW, the blue power stability is better than 4.7% and laser beam quality M 2 factor is 1.43.  相似文献   

2.
A compact and efficient intra-cavity doubled, actively Q-switched diode-pumped Nd:YAG laser has been developed. It generates as much as 1.55 W at 532 nm, with pulses of 400 ns at a repetition rate of 15 kHz, with an overall optical-to-optical efficiency of 15.5%. A beam quality factor M2 ≈ 2.35 has been measured at this power level.  相似文献   

3.
We present for the first time a Nd:YAG laser emitting at 1319 nm intracavity pumped by a 946 nm diode-pumped Nd:YAG laser. A 809 nm laser diode is used to pump the first Nd:YAG crystal emitting at 946 nm, and the second Nd:YAG laser emitting at 1319 nm intracavity pumped at 946 nm. Intracavity sumfrequency mixing at 946 and 1319 nm was then realized in a LBO crystal to reach the yellow range. We obtained a continuous-wave output power of 158 mW at 551 nm with a pump laser diode emitting 18.7 W at 809 nm.  相似文献   

4.
报道了一台800 Hz,6.2 W外腔和频的589 nm黄光激光器。基频激光器均采用双棒串接平平对称腔,增益介质为Nd:YAG晶体,采用声光调Q方式分别获得11.1 W的1 064 nm激光和12.6 W的1 319 nm激光。和频晶体采用三硼酸锂(LBO),尺寸为4 mm×4 mm×30 mm,采用Ⅰ类非临界相位匹配。将两束激光通过分光镜合束,聚集后注入LBO晶体,获得589 nm黄光最大输出功率为6.2 W,脉宽为50 ns,和频效率26.2%。x方向和y方向的光束质量平方因子分别为3.20和3.61。  相似文献   

5.
 报道了一台800 Hz,6.2 W外腔和频的589 nm黄光激光器。基频激光器均采用双棒串接平平对称腔,增益介质为Nd:YAG晶体,采用声光调Q方式分别获得11.1 W的1 064 nm激光和12.6 W的1 319 nm激光。和频晶体采用三硼酸锂(LBO),尺寸为4 mm×4 mm×30 mm,采用Ⅰ类非临界相位匹配。将两束激光通过分光镜合束,聚集后注入LBO晶体,获得589 nm黄光最大输出功率为6.2 W,脉宽为50 ns,和频效率26.2%。x方向和y方向的光束质量平方因子分别为3.20和3.61。  相似文献   

6.
Chen YF  Tsai SW 《Optics letters》2002,27(6):397-399
A compact high-power yellow pulsed laser has been demonstrated by use of intracavity sum-frequency mixing in a diode-end-pumped Q -switched Nd:YVO(4) dual-wavelength laser. A three-mirror configuration forming two separate laser cavities is used to optimize the gain match for simultaneous dual-wavelength emission in Q -switched operation. Under the optimum cavity-length condition, the highest yellow average power is 340 mW and the peak power is 2 kW, obtained at 12.5 W of pump power.  相似文献   

7.
The modelocking of a Nd:YAG laser using second-harmonic generation in an external cavity as the only pulse shortening process is reported. The output of a long pulse Nd:YAG laser was simultaneously modelocked and Q-switched. The average pulse duration was 30–50 ps and the peak power was in the range 60–160 kW.  相似文献   

8.
We demonstrated a diode-pumped Nd:YAG laser with a plano-concave resonator. When the pump power is 1.57 W, the output power of 1123-nm laser is 132 mW at the temperature of 20 ℃, and the power change is less than 2% in an hour. A periodically poled LiNbOa (PPLN) was used as outer cavity frequency-doubling crystal and 561-nm laser was observed.  相似文献   

9.
We report an L-shaped symmetrical co-folding-arm plane-plane diode pumped solid-state yellow laser at 589 nm by using intracavity sum-frequency mixing. By carefully designing the cavity and employing various techniques to optimize the laser’s specifications, a quasi-continuous-wave (QCW) free-oscillation yellow laser source, which has an average output power of 8.1 W, a beam quality factor of M2 = 2.3, and a repetition rate of 1.1 kHz, is developed. The generation of yellow laser at 589 nm is achieved by intracavity sum-frequency mixing between the laser lines at 1319 nm and 1064 nm of an Nd:YAG laser in a KTP crystal. To the best of our knowledge, the 8.1 W output at 589 nm is higher than any other diode pumped solid-state yellow laser generated by intracavity sum-frequency generation so far.  相似文献   

10.
The dynamical behaviour of a Q-switched, flashlamp-pumped Nd: YAG laser cooled to 253 K was investigated. The build-up time of photons in the resonator at 946 nm was 20 times longer than for 1064 nm generation in a Q-mode of operation. A type I second- and fourth-harmonic generation was obtained in KDP and BBO nonlinear optical crystals. A reproducible spectral line width of the second-harmonic generation =2.6 GHz within a tuning range of =146 GHz was achieved. A comparison between experimental and theoretical results is presented.  相似文献   

11.
LD泵浦Nd:YAG 946 nm/1 064 nm双波长运转及腔内和频   总被引:3,自引:1,他引:3       下载免费PDF全文
用国产半导体激光二极管(LD)端面泵浦NdYAG晶体, 通过优化激光谐振腔反射膜系,调节1 064 nm谱线的线性损耗以达到与弱谱线946 nm的增益匹配,在室温下实现1 064 nm和946 nm双波长连续运转,并通过I类临界相位匹配LBO晶体腔内和频在国内首次实现500.8 nm青色激光连续输出.当泵浦注入功率为1.4W时和频青色激光最大输出达20 mW,光-光转换效率为1.4%,功率稳定性24 h内优于±3%.  相似文献   

12.
We report on a laser diode end-pumped Nd:YAG blue laser using a three-mirror-folded cavity. Three different crystals cut for type-I critical phase matching are used for the intra-cavity frequency doubling of the laser: 10-mm-long LiB3O5 (LBO), 15-mm-long LBO, and 10-mm-long BiB3O6 (BIBO). Up to 2.41 W of continuous wave output power in the blue spectral range at 473 nm is achieved with BIBO crystal (1.89 W with LBO) at the incident pump power of 16 W, the light-to-light conversion efficiency is about 15.1%.  相似文献   

13.
Chen YF  Tsai SW  Wang SC  Huang YC  Lin TC  Wong BC 《Optics letters》2002,27(20):1809-1811
We report efficient generation of cw yellow light by use of single-pass sum-frequency mixing from a diode-pumped Nd:YVO(4) dual-wavelength laser with periodically poled lithium niobate. A diode-pumped Nd:YVO(4) dual-wavelength laser is implemented with a three-mirror cavity, and the optimum oscillation condition is obtained from theoretical analysis. We extracted 78 mW of power at 593 nm from 1.2 W at 1064 nm and from 1.0 W at 1342 nm in a beam with excellent quality. The output power could probably be increased to ~92 mW by antireflection coating of the crystal.  相似文献   

14.
We present our studies on dual wavelength operation using a single Nd:YVO4 crystal and its intracavity sum frequency generation by considering the influence of the thermal lensing effect on the performance of the laser. A KTP crystal cut for type-II phase matching was used for intracavity sum frequency generation in the cavity at an appropriate location for efficient and stable yellow output power. More than 550 mW of stable CW yellow-orange beam at 593.5 nm with beam quality parameter (M 2) ~4. 3 was obtained. The total pump to yellow beam conversion efficiency was estimated to be 3.83%.  相似文献   

15.
Li  B. Z.  Su  X. X.  Guo  L. J.  Lin  J. Q.  Gao  X.  Li  X. K.  Zhang  X. H.  Jin  G. Y.  Sun  G. C. 《Laser Physics》2011,21(6):1061-1063
We report for the first time a coherent orange-red radiation at 616 nm by intracavity sum-frequency generation of the 1080 and 1433 nm laser-lines of two Nd:YAP lasers. Orange-red laser is obtained by using a doubly linear resonator, type-II critical phase matching KTiOPO4 (KTP) crystal sum-frequency mixing. With a total diode pump power of 26.5 W (8.7 W pump power for 1080 nm Nd:YAP laser and 17.8 W pump power for 1433 nm Nd:YAP laser), TEM00 mode orange-red laser at 616 nm of 127 mW is obtained. The power stability in 30 min is better than 3.3%.  相似文献   

16.
We present a near diffraction-limited 1 064-nm Nd:YAG rod laser with output power of 82.3 W(M~2≈1.38). The power fluctuation over two hours is better than±1.1%.Pulsed 1064-nm laser with an average power of 66.6 W and pulse width of 46 ns are achieved when the laser is Q-switched at a repetition rate of 10 kHz.The short pulse duration stems from the short cavity as well as the high-gain laser modules. Using intracavity-frequency-doubling,a 35.0-W near diffraction-limited 532-nm green laser(M~2≈1.32) is achieved with a pulse width of 43 ns.  相似文献   

17.
We report for the first time a continuous-wave (CW) coherent radiation at 485 nm by intracavity sum-frequency generation of 916 nm Nd:LuVO4 laser and 1030 nm Yb:YAG laser. Blue laser is obtained by using a doubly cavity, type-II critical phase matching KTP crystal sum-frequency mixing. With total pump power of 30.2 W, TEM00 mode blue laser at 485 nm of 179 mW is obtained. The blue power stability in 30 min is better than 3%.  相似文献   

18.
We demonstrated a linearly polarized continuous-wave Nd:YAG laser operating at a 1357-nm single-wavelength, by a 808-nm diode as an end-pump source. We chose a Brewster-angle-cut Nd:YAG laser host crystal, due to its two salient features as follow: linearly polarized laser output and single-wavelength oscillation can be easily obtained. In this paper, a continuous-wave all-solid-state single-wavelength laser operating at 1357 nm is demonstrated with a diode-end-pumped Brewster-cut Nd:YAG laser. The laser had a 1.03-W maximum output power under an incident pump power of 15.0 W, a 12.7% slope efficiency, a 6.9% optical-to-optical conversion efficiency, a 0.14-nm spectral linewidth and a 3% power-output stability within 30 min. PACS 42.55.Rz; 42.55.Xi; 42.70.Hj  相似文献   

19.
J. H. Liu  G. C. Sun  Y. D. Lee 《Laser Physics》2012,22(7):1199-1201
We report a continuous-wave (CW) yellow laser emission by sum-frequency mixing in Nd:YVO4 crystal. Using type-II critical phase-matching KTP crystal, a yellow laser at 593.5 nm is obtained by 1064 and 1342 nm intracavity sum-frequency mixing. The maximum laser output power of 2.1 W is obtained when an incident pump laser of 18.2 W is used. At the output power level of 2.1 W, the output stability is better than 3.2%.  相似文献   

20.
Mu X  Ding YJ 《Optics letters》2005,30(11):1372-1374
A new route for efficiently generating coherent blue light has been explored based on intracavity effective third-harmonic generation in one partly periodically poled KTiOPO4 crystal placed inside the cavity of a diode-pumped Nd:YAG laser. To achieve efficient conversion, we use a dual-temperature oven to separately control the phase-matching conditions for the two second-order nonlinear processes. In addition, a Fabry-Perot cavity at 660 nm is incorporated into the crystal to increase the blue power significantly. When the laser is Q switched to produce long pulses, an average power of 118 mW is generated at 440 nm at a pump power of 10 W.  相似文献   

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