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1.
Room temperature, multi-wavelength operation in 0.3% doped Er:YAG laser with double etalons pumped by a MgO:PPLN laser locked at 1532 nm was reported. Lasing occurred predominantly at 1645.1 nm and 1617.2 nm. 350 mW of 1645.1 nm, 160 mW of 1617.2 nm output were achieved under total incident pump power of 7 W.  相似文献   

2.
Gao C  Zhu L  Wang R  Gao M  Zheng Y  Wang L 《Optics letters》2012,37(11):1859-1861
A monolithic 1645 nm Er:YAG nonplanar ring oscillator (NPRO) resonantly pumped by a 1532 nm fiber laser is demonstrated. For reducing the energy-transfer upconversion effect, a 0.5% doped Er:YAG nonplanar crystal was used. An up to 6.1 W single frequency laser output at 1645 nm was obtained, with a slope efficiency of 55.2% and an optical efficiency of 48.0%. The linewidth of the Er:YAG NPRO was 14.4 kHz.  相似文献   

3.
A diode end-pumped single-frequency Tm:YAG laser at room temperature was reported. The maximal output power of single-frequency is 30 mW by using two uncoated etalons. We obtained a single frequency Tm:YAG laser at 2008.14 nm. The single-longitudinal-mode laser can be used as a seed laser for coherent wind measurements and differential absorption LIDAR systems.  相似文献   

4.
A diode end-pumped single-frequency Tm:YAG laser at room temperature is reported. The maximal output power of single-frequency is as high as 60 mW by using two uncoated fused YAG etalons, which are respectively 0.1 and 1.0 mm thick. We obtained a single frequency Tm:YAG laser at 2013.91 nm. The change of the lasing wavelength on temperature was also measured. The single-longitudinal-mode laser can be used as a seed laser for coherent wind measurements and differential absorption LIDAR systems.  相似文献   

5.
Diode end-pumped single-frequency Tm:GdVO4 laser at room temperature was reported. The maximal output power of single-frequency is as high as 51 mW by using two uncoated fused YAG etalons, which are respectively 0.05 mm thick and 1 mm thick. We obtained the single frequency Tm:GdVO4 laser at 1919.7 nm. The slope efficiency is 1.4%. The single-longitudinal-mode (SLM) laser can be used as a seed laser for coherent wind measurements and differential absorption LIDAR systems.  相似文献   

6.
Dai TY  Ju YL  Yao BQ  Shen YJ  Wang W  Wang YZ 《Optics letters》2012,37(11):1850-1852
We demonstrated a 1.91 μm pumped, injection-seeded Q-switched Ho:YAG laser operating at room temperature. By inserting two Fabry-Perot etalons into the laser cavity, single-frequency Tm, Ho:YAG seed lasing was achieved at a wavelength of 2090.9 nm, with a typical output power of 60 mW. Single-frequency, nearly transform-limited Q-switched operation of the Ho:YAG laser was achieved by injection seeding. The output energy of the single-frequency Q-switched pulse is 7.6 mJ, with a pulse width of 132 ns and a repetition rate of 100 Hz. We measured the pulse spectrum, half-width of which was 3.5 MHz, by a heterodyne technique.  相似文献   

7.
A compact design for a single mode Tm:YAG laser is presented. With two thin infrasil etalons as the only intracavity tuning elements a tuning range from 1940 to 2030 nm with a gap between 2000 and 2020 nm can be realized. The laser emits in two longitudinal modes separated by 1 GHz. Pumped with 500 mW power from a Ti:sapphire laser at 786 nm the output is above 50 mW over the entire tuning range. Frequencies can be rapidly varied over a range of 4 GHz.  相似文献   

8.
A diode end-pumped Tm:GdVO4 laser at room temperature is reported. The maximal output power of single-frequency is as high as 34 mW by using two uncoated fused etalons, which are respectively 0.05 mm thick YAG and 1mm thick quartz. We obtained the single frequency Tm:GdVO4 laser at 1897.6 nm with the slope efficiency of 1.3%. The single-longitudinal-mode (SLM) laser can be used as a seed laser for coherent wind measurements and differential absorption LIDAR systems.  相似文献   

9.
A resonantly pumped Q-switched Er:YAG laser at 1645 nm was reported. 1 mJ of output pulse energy was achieved for Q-switched operation at 100 Hz repetition rate under total incident pump power of 4 W. An output peak power of 14 kW and pulse width of 60.6 ns were obtained.  相似文献   

10.
The study describes efficient, acousto-optic Q-switching of Er:YAG laser at the 1645 nm eye-safe wavelength. For longitudinal pumping at wavelength 1532 nm, linear-polarized 10 W Erbium fiber laser radiation was used. The investigated Er:YAG crystals were 25 and 40 mm long and their Erbium concentration was 0.20 and 0.25%, respectively. For giant pulse generation, a fused silica acousto-optic modulator was inserted inside the Er:YAG laser oscillator. For a maximum incident pump power of 7.95 W, pulse energy up to 4.1 mJ was generated with pulse duration 34 ns at 500-Hz repetition rate; the corresponding peak power was 119 kW.  相似文献   

11.
In this paper, we present experimental results concerning on the laser characteristics of Tm:YAG laser and Tm: GdVO4 laser. At room temperature, the maximum output power of Tm:YAG laser and Tm:GdVO4 laser is 210 and 145 mW, respectively. High efficiency can be achieved for both lasers at room temperature. Nevertheless, compared with Tm:GdVO4 laser, Tm:YAG laser can operate on single frequency with high power easily. As much as 60 mW of 2013.9 nm single-longitudinal-mode (SLM) laser was achieved for Tm:YAG laser. For Tm:GdVO4 laser 51 mW of 1919.7 nm SLM laser was achieved. The SLM Tm:YAG laser is better for using as a seed laser for coherent wind measurements and differential absorption LIDAR systems.  相似文献   

12.
A diode end-pumped single-frequency Tm:GdVO4 laser at room temperature was reported. The maximal output power of single-frequency is as high as 66 mW by using two uncoated fused etalons, which are respectively 0.05 mm thick YAG and 1 mm thick quartz. We obtained the single frequency Tm:GdVO4 laser at 1875.1 nm. The slope efficiency is 1.5%. The change of the lasing wavelength on temperature was also measured. The single-longitudinal-mode (SLM) laser can be used as a seed laser for coherent wind measurements and differential absorption LIDAR systems.  相似文献   

13.
We present a Tm-doped fiber laser pumped Fabry-Perot etalons Ho:YAG laser based on a corner cube.A maximum single-longitudinal-mode and fundamental transverse mode output power of 478 mW at the waveiength of 2091.06 nm is achieved with a pump power of 16.3 W,corresponding to an opticai-to-optical efficiency of 2.9%and a slope efficiency of 7.9%.The single-longitudinal-mode and fundamental transverse mode are less sensitive to the rotating of the corner cube.The results indicate the potential impact of a single-longitudinal-mode Ho:YAG laser with corner cube geometry to improve the anti-maladjustment stability.  相似文献   

14.
We present a 2.09 μm single-longitudinal-mode sandwich-type YAG/Ho:YAG/YAG ceramic laser pumped by a Tm-doped fiber laser for the first time. A pair of F-P etalons was used to achieve tunable single-longitudinal-mode operation. The maximum single-longitudinal-mode output power of 530 mW at 2091.4 nm was obtained with an absorbed pump power of 8.06 W, corresponding to an optical conversion efficiency of 6.6% and a slope efficiency of 12.7%. Wavelength tunable was achieved by tuning the angle of etalons and the wavelength could be tuned from 2091.1 nm to 2092.1 nm, corresponding to a tuning frequency of 68 GHz. The M2 factor was measured to be 1.23.  相似文献   

15.
全固化非平面单频Nd:YAG环形激光器   总被引:5,自引:3,他引:2  
张宽收  张云 《光学学报》1996,16(8):041-1044
利用Nd:YAG激光增益介质的法拉第效应,以及光束在非平面环形谐振腔中传播产生的偏振面旋转,使激光二极管泵浦的环形Nd:YAG激光器单向运转,获得单频激光输出,最大单纵模激光(1.064μm)输出为365mW,功率波动小于2%,短期频率漂移小于45MHz,并利用内腔倍频技术得到单频绿光输出,最大单纵模绿光(532nm)输出为75mW,功率波动小于4%。  相似文献   

16.
We report a diode pumped single frequency Tm:YAG laser with two coated fused silica etalons as mode selectors. The maximum single frequency output power was 681 mW with the pumping power of 4.83 W. The slope efficiency of single-frequency laser was 20.5% and the optical-to-optical conversion efficiency was 14.2%. According to the experimental results, we developed a prototype with the maximum single frequency output power of 249 mW and the slope efficiency of 23.1%. The frequency tuning was investigated by changing the temperature of the crystal. A tuning coefficient of 2.57 GHz/°C was obtained. The beam propagation factors M2 were measured as 1.01 in both directions. The linewidth of the single frequency was 40 kHz.  相似文献   

17.
A single-frequency Tm:YAG laser at room temperature is presented. With two thin etalons as the intra-cavity tuning elements, the maximum output power 69.5 mW is obtained at room temperature. The slope efficiency is 10.2% and the optical to optical conversion efficiency of 4.02%. The central wavelength is 2012.5 nm. A temperature stability of 0.1 °C corresponds to a frequency stability of 74 MHz observed by wave meter in 50 s.  相似文献   

18.
A diode-pumped high-power single-longitudinal-mode (SLM) Tm:YAG laser was investigated. To obtain a single-frequency 2 μm laser output, Fabry–Perot (F–P) etalons combined with a volume Bragg grating (VBG) were used as frequency selection devices. The transmission losses of the VBG and etalons were analyzed and the angles of F–P etalons were optimized theoretically. Considering the gains and the insertion losses, the output wavelength of the Tm:YAG laser was estimated to be 2012.47 nm. Using this method, as much as 574 mW SLM laser was obtained experimentally, corresponding to a slope-efficiency of 18.6% and an optical-to-optical efficiency of 8.2%. The output wavelength was measured to be 2012.47 nm, which was in excellent agreement with the theoretical result. The power instability was less than 1% in 30 minutes test, and the degree of the linear polarization was over 20 dB.  相似文献   

19.
Wang  Kai  Cai  Jun  Ding  Yu  Zhao  Wanli 《Journal of Russian Laser Research》2022,43(2):254-257
Journal of Russian Laser Research - We present an efficient continuous wave Tm:Y2O3 ceramic laser resonantly pumped by a 1645 nm Er:YAG laser. With an absorbed pump power of 5.9 W, we achieve a...  相似文献   

20.
We report a resonantly fiber-laser-pumped Er:YAG laser operating at the eye-safe wavelength of 1645 nm, exhibiting 43% optical efficiency and 54% incident slope efficiency and emitting 7-W average power when repetitively Q switched at 10 kHz. To our knowledge, this is the best performance (conversion efficiency and average power) obtained from a bulk solid-state Q-switched erbium laser. At a 1.1-kHz pulse repetition frequency the laser produces 3.4-mJ pulses with a corresponding peak power of 162 kW. Frequency doubling to produce 822.5-nm, 4.7-kW pulses at 10 kHz was performed to demonstrate the laser's utility.  相似文献   

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