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1.
激光二极管泵浦Nd:YAG 946nm激光器及倍频研究   总被引:6,自引:2,他引:4  
杜戈果  李富铭 《光子学报》2001,30(11):1392-1395
提出如何克服准三能级再吸收损耗和抑制寄生振荡实现LD泵浦的Nd:YAG946nm激光器.在室温下946nm连续输出大于120mW,斜率效率接近10%,同时采用KNbO3晶体实现了腔内倍频的蓝色激光输出.对实验结果进行了分析并提出了改进措施.  相似文献   

2.
本文为泵浦质子交换准相位匹配波导器 Li Nb O3 提供了激光光源 ,用 80 8nm半导体激光器泵浦 Nd∶ YAG晶体 ,在室温下获得 946 nm激光连续输出大于 1 2 0 m W,斜率效率9.8% ,并且在国内首次实现了 LD泵浦 Nd∶YAG/ KNb O3 4 73 nm蓝色激光器的连续运转 ,报道了初步的实验结果并对此进行了详细的分析 ,提出了改进方案 .  相似文献   

3.
LD泵浦Nd:YAG/LBO结构660 nm红光激光器   总被引:3,自引:3,他引:0  
郑权陈颖新  钱龙生 《光子学报》2003,32(10):1153-1155
采用国产LD泵浦Nd:YAG晶体,通过谐振腔镜的膜系选择获得了Nd3+离子中波长为1319 nm的受激辐射振荡,首次用I类临界位相匹配LBO进行腔内倍频,实现了660 nm红色激光的高效倍频输出.当泵浦注入功率为800 mW时,660 nm激光基横模(TEM00)输出功率为46 mW,光光转换效率高达5.75%.  相似文献   

4.
向列相液晶染料可调谐激光器的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
刘永军  孙伟民  刘晓颀  姚丽双  鲁兴海  宣丽 《物理学报》2012,61(11):114211-114211
对向列相液晶染料的可调谐激光器进行了光学特性研究. 以650 nm为中 心波长设计了SiO2和TiO2多层膜的一维光子晶体, 以激光染料与向列相液晶的混合物作为增益介质层, 制备了波长可调谐激光器.用Nd: YAG倍频脉冲激光器输出的532 nm激光抽运所制备的激光器样品得出如下光学特性: 激光发射波长随温度调谐范围为605.5---639.8 nm, 达到34.3 nm, 随电压调谐范围为634.5---619.5 nm, 达到15 nm. 发射激光每脉冲的阈值能量为12.3 μJ, 激光线宽小于1 nm.  相似文献   

5.
掺铬的镁橄榄石晶体连续波可调谐激光器   总被引:2,自引:1,他引:1  
阮双琛  侯洵 《光子学报》1998,27(2):97-99
本文报道了连续波Nd:YAG激光器泵浦掺铬镁橄榄石(Cr4+:forsterite)晶体获得了连续波可调谐运转,该激光器采用Nd:YAG激光器的1.06μm谱线泵浦Φ5×9mm的Cr4+:forsterite晶体.在吸收泵浦功率为8.7W时,得到1.05W的连续波输出.当在腔内放置色散元件后,其调谐范围是1186nm~1306nm,同时详细研究了输出功率随温度和输出镜透过率的变化特性.  相似文献   

6.
LD泵浦Nd:YVO4/KTP/BBO紫外激光器   总被引:3,自引:0,他引:3  
本文报道在国内首次实现的LD泵浦的四倍频连续紫外激光器的实验结果.首先研究了LD泵浦的Nd:YVO4激光器,在普通平-平腔结构下,得到斜效率55.68%,激光输出波长1064nm;利用KTP作为倍频晶体,实现腔内倍频,在泵浦功率11.85W时得到绿光(532nm)输出1.35W,光-光转换效率11%;用BBO晶体进行外腔谐振倍频,得到紫外光(266nm)输出.  相似文献   

7.
LD侧泵浦Nd:YAG板条双程功率放大器初步研究   总被引:6,自引:6,他引:0       下载免费PDF全文
 对二极管激光侧泵浦Nd:YAG板条双程功率放大器进行了初步的研究,给出了激光器的数值模拟结果,建立了二极管侧面泵浦Nd:YAG板条激光主振荡-多程放大(MOPA)系统;在100Hz重复频率时,实验获得单脉冲能量为51.9mJ的输出,光束质量M 2小于2,脉冲能量起伏小于2%, 实验结果与数值计算结果相符合。  相似文献   

8.
 建立了LD预泵浦的被动调Q平平腔Cr4+,Nd3+:YAG微片激光器模型,分析了预泵浦参数与激光脉冲时间特性的关系,设计了LD预泵浦的Cr4+,Nd3+:YAG微片激光器实验,测量了不同预泵浦参数下激光单脉冲以及脉冲序列的时间特性。实验结果与数值计算结果基本符合:调节预泵浦参数使每个泵浦脉冲刚好对应输出单个激光脉冲时,固定脉冲泵浦宽度,脉冲泵浦速率随连续泵浦速率的增加呈一次函数减小;固定连续泵浦速率,脉冲泵浦速率随脉冲泵浦宽度的增加呈非线性函数减小。结果还表明,激光脉冲半高全宽随整体泵浦速率的增加而减小,峰值功率随整体泵浦速率的增加而增加;当整体泵浦速率在阈值附近变动时,激光单脉冲时间特性的变化最为明显。  相似文献   

9.
 为提高固体激光器的能量利用率,增大输出能量,将双掺Nd:Ce:YAG晶体的输出特性与普通Nd:YAG晶体进行了对比研究。分析了Nd3+和Ce3+的吸收光谱对激光晶体初始阈值反转粒子数的影响,结果显示:双掺Nd:Ce:YAG晶体可以提高晶体对泵浦光能量的利用率及激光器的输出能量,且可降低阈值泵浦能量。并分别检测了Nd:Ce:YAG激光晶体与Nd:YAG晶体的输出激光能量和阈值泵浦能量,实验结果表明:在输入电压为750 V时,Nd:Ce:YAG晶体与Nd:YAG晶体的输出能量分别为651.5 mJ 和390.4 mJ,能量利用率分别为2.31%和1.38%,激光振荡需要的泵浦能量阈值分别为10.56 mJ和15.21 mJ,且普通Nd:YAG晶体的斜效率为0.36%,而双掺Nd:Ce:YAG晶体的为0.49% 。  相似文献   

10.
利用激光谐振腔内标准具的选模调谐特性和激光晶体自身的标准具作用,通过调节插入标准具和激光晶体的倾斜度及微调谐振腔长度,在LD泵浦Nd:YVO4单频激光器上实现了精确调谐,最大可调谐范围约100GHz.  相似文献   

11.
Yong-liang Li  Yu-lan Zhang 《Optik》2011,122(8):743-745
A sum-frequency yellow-green laser at 554.9 nm is reported by this paper, 946 nm wavelength is obtained from 4F3/2-4I9/2 transition in Nd:YAG and 1342 nm wavelength is obtained from 4F3/2-4I13/2 transition in Nd:YVO4. Using a doubly folded-cavity type-II critical phase matching KTP crystal intra cavity to make 946 nm laser from Nd:YAG and 1342 nm laser from Nd:YVO4 frequency summed, with incident pumped power of 30 W in Nd:YAG and 20 W in Nd:YVO4, TEM00 mode yellow-green laser at 554.9 nm at 1.15 W is obtained and its M2 factor is less than 1.22. The experimental results show that the Nd:YAG and Nd:YVO4 crystals intra-cavity sum-frequency mixing is an effective method for yellow-green laser and it can be applied to other two laser crystals to obtain more all-solid-state lasers with different wavelengths.  相似文献   

12.
Output performances of passively Q-switched, composite Nd:YAG/Cr4+:YAG lasers that consisted of bonded, all-poly-crystalline ceramics Nd:YAG and Cr4+:YAG are reported. Laser pulses at 1.06 μm with 2.5-mJ energy and 1.9-MW peak power are obtained from a 1.1-at % Nd:YAG/Cr4+:YAG ceramics that was quasi-continuous-wave (quasi-CW) pumped with a diode laser. Single-pass frequency doubling with LiB3O5 (LBO) nonlinear crystal at room temperature yielded green laser pulses at 532 nm of 0.36-mJ energy and 0.3-MW peak power, with a conversion efficiency of 0.27.  相似文献   

13.
Laser emission in the 0.94-, 1.06- and 1.34-micron ranges in diluted and concentrated Nd:YAG crystals longitudinally pumped by a 885-nm diode laser on the 4 I 9/24 F 3/2 transition is investigated. Continuous-wave operation at watt level in all these wavelength ranges is demonstrated with a 1.0-at. % Nd:YAG crystal; however, the laser performance is impeded by the low pump absorption efficiency. Improved output power and overall efficiency were obtained with a highly doped 2.5-at. % Nd:YAG crystal: 5.5 W at 1.06 μm and 3.8 W at 1.34 μm with 0.38 and 0.26 efficiencies, respectively. Comparative results with traditional pumping at 809 nm into the highly absorbing 4 F 5/2 level are presented, showing the advantage of the direct 4 F 3/2 pumping. The influence of the lasing wavelength and of the Nd concentration on the thermal effects induced by the optical pumping in the laser material is discussed. A clear relation between the heat generated in the Nd:YAG crystals in lasing and non-lasing regimes, a function of the Nd doping, is demonstrated. PACS 42.55.Rz; 42.60.By; 42.60.Da  相似文献   

14.
We have fabricated Cr3+ and Nd3+ co-doped YAG (Cr;Nd:YAG) ceramics, and investigated their optical properties and laser characteristics. The Cr;Nd:YAG has two broad absorption bands at around 440 nm (4A24T1) and 600 nm (4A24T2) respectively, caused by Cr3+ ions. In the case of pumping at 440 nm, the maximum effective lifetime of the Cr;Nd:YAG was 737 μs with a 0.1 at% Cr3+ and 1.0 at% Nd3+ co-doped YAG sample. Cr3+ ions take a role of an effective sensitizer to convert the UV light of flashlamp. For single-shot laser operation, a 10.4 J output energy at 1064 nm was obtained with 0.1 at% Cr3+ and 1.0 at% Nd3+ co-doped YAG ceramic rod with a laser efficiency of 4.9%. The laser efficiency was found to be more than twice that of a 1.0 at % Nd3+:YAG ceramic rod.  相似文献   

15.
We present theoretical and experimental investigations on ground-state direct pumping at 869 nm into the emitting level 4F3/2 of end-pumped quasi-three-level Nd:YAG lasers operating at 946 nm. We have demonstrated, what we believe is for the first time, a Nd:YAG laser at 946 nm directly pumped by diodes and obtained 1.6 W of output power.  相似文献   

16.
N. Pavel 《Laser Physics》2010,20(1):215-221
Continuous-wave (CW) simultaneous laser emission on the 0.9-μm 4 F 3/24 I 9/2 transition and the 4 F 3/24 I 11/2 transition at 1.06 μm is obtained in Nd-based laser crystals of thin-disk geometry and using a multi-pass pumping scheme. A Nd:Y3Al5O12 (Nd:YAG) thin disk emitted simultaneous laser radiation at 946 and 1064 nm with 5.1 W output power, and Nd:YVO4 and Nd:GdVO4 thin-disk lasers with more than 3 W output power at 0.91 and 1.06 μm were realized. The ratio between the output power at one of the wavelengths and the total output power could be varied by the laser resonator design. An intracavity frequency-doubled Nd:YVO4 thin-disk laser with alternate green at 532 nm and “deep-blue” at 457 nm generation of high average output powers is demonstrated.  相似文献   

17.
A continuous-wave high-power Nd:YAG laser operating on the 4F3/24I9/2 transition at 946 nm and intracavity frequency-doubled to 473 nm by a KNbO3 nonlinear crystal at room temperature is reported. The Nd:YAG laser outputs a randomly polarized beam of 3.8 W maximum power (38% optical-to-optical efficiency and 44% slope efficiency with respect to the absorbed pump power) at the 946 nm fundamental wavelength. Intracavity frequency-doubling with a 2.0-mm thick KNbO3 crystal in a linear resonator yielded 159-mW single-ended blue-output with 4.8% optical-to-optical conversion efficiency versus the absorbed pump power. The 473-nm maximum power of 418 mW with 11.6% optical-to-optical conversion efficiency in absorbed power was obtained from a V-type resonator; the overall optical-to-optical conversion efficiency was 6.7%, while the conversion of the available infrared power reached 50%.  相似文献   

18.
The continuous-wave high efficiency laser emission of Nd:YAG at the fundamental wavelength of 1319 nm and its 659.5-nm second harmonic obtained by intracavity frequency doubling with an LBO nonlinear crystal is investigated under pumping by diode laser at 885 nm (on the 4 F 3/24 I 13/2 transition). An end-pumped Nd:YAG crystal yielded 9.1 W at 1319 nm of continuous-wave output power for 18.2 W of absorbed pump power. The slope efficiency with respect to the absorbed pump power is 0.55. Furthermore, 5.2 W 659.5 nm red light is acquired by frequency doubling, resulting in an optical-to-optical efficiency with respect to the absorbed pump power of 0.286. Comparative results obtained for the pump with diode laser at 808 nm (on the 4 F 5/24 I 13/2 transition) are given in order to prove the advantages of the 885 nm wavelength pumping.  相似文献   

19.
We describe the output performances of the 1116 nm 4 F 3/2-4 I 11/2 transition (generally used for a 1064 nm transition) in Nd:YAG under in-band pumping with diode laser at the 809 nm wavelength. An end-pumped Nd:YAG crystal yielded 680 mW of continuous-wave (CW) output power for 18.2 W of incident pump power. Moreover, intracavity second-harmonic generation (SHG) has also been achieved with a power of 97 mW at 558 nm by using a LiB3O5 (LBO) nonlinear crystal. The yellow-green beam quality factor M 2 was less than 1.21. The yellow-green power stability was less 2.5% in 4 h.  相似文献   

20.

We report continuous-wave (CW) and passively Q-switched Nd :GdVO4 lasers on 4F3/24I13/2 transition directly pumped by an 880 nm diode laser. A widely investigated Nd :GdVO4 laser at about 1341 nm is operated with a maximum output power of 5.23 W and a slope efficiency of about 30.6%. Using an etalon for wavelength selection, we realize laser emission at about 1344 nm, for the first time to our knowledge, in a Nd :GdVO4 laser, with a maximum output power of 4.19 W and a slope efficiency of 20.1%. Moreover, we achieve simultaneous dual-wavelength lasing at 1341 and 1344 nm with a maximum output power of 2.27 W and a slope efficiency of 13.5%, respectively. Using V3+ :YAG as a saturable absorber, stable Q switching is obtained at about 1341 nm with a maximum average output power of 1.15 W. The pulse width is 52.8 ns at a repetition rate of 279.8 kHz.

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