共查询到20条相似文献,搜索用时 11 毫秒
1.
A scalable diode-pumped Nd:YAG laser is described in which the gain element resembles a penta-prism. This design allows longitudinal pumping along five separate axes. Using five high-power single stripe laser diodes, 4.16 W of absorbed power produced 2.3 W CW at 1.06 μm. The slope efficiency was 56%, the output was plane polarized, and the laser operated in the TEM00 mode. The threshold power, was 48 mW. No evidence of thermal saturation was observed up to the maximum pump power. With an intracavity KTP crystal, 431 mW of CW amplitude-stable output at 532 nm was generated. Repetitive Q-switched operation is also reported 相似文献
2.
Frequency-stabilized diode-pumped Nd:YAG laser of high power 总被引:1,自引:0,他引:1
We describe a frequency-stabilized diode-pumped Nd:YAG laser of high power whose single-mode operation is obtained by suppressing the spatial hole burning through the twisted-mode technique. Active frequency stabilization is achieved by fringe side locking the laser beam to a reference Fabry-Perot cavity. Output power up to 800 mW in single-transverse and -longitudinal mode operation with a linewidth of less than 20 kHz is obtained 相似文献
3.
4.
5.
理论和实验研究了激光器谐振腔失谐对激光器性能的影响。一方面,理论上,基于准连续二极管泵浦、电光调Q固体激光器的特点,建立了包含谐振腔失谐修正函数的速率方程模型。通过数值仿真,模拟了不同激光模式、光斑半径、孔阑半径、孔阑位置情况下,谐振腔失谐对激光器损耗以及激光性能的影响。另一方面,实验测量了谐振腔失谐对激光器性能的影响。对于长250 mm、最小孔阑半径3.5 mm的凹凸非稳腔,凹面全反镜失谐比凸面输出镜失谐对激光器性能的影响大,当凹面全反镜水平方向失谐角度由0增加到490 rad时,激光能量由220 mJ下降到150.9 mJ,下降31.4%,脉冲宽度由5 ns增大到6.5 ns,实验结果和理论分析结果基本相符,说明激光模型的正确性。建立的模型与实验方法为预测激光器谐振腔失谐对激光器性能的影响提供了一种有效工具,为高可靠性激光器设计提供了依据。 相似文献
6.
An Nd:YAG 1-cm-long crystal has been used as the active medium for tunable single- and double-frequency lasers with a metallic absorbing thin-film selector. Cobalt and chromium thin films (210-nm thickness) were used for mode number and frequency control. The laser with a short cavity (25 mm) provided slow smooth tuning up to 6 GHz, the frequency chirp up to 4 GHz with repetition rate about 0.5 kHz and hop tuning over 150 GHz at a maximum pump power of 1.8 W. 520 mW of single-frequency output power was achieved. Double-frequency operation with a space of 1.5-2.5 GHz was realized in a laser with cavity length up to 100 mm 相似文献
7.
Nd:YAG激光治疗分泌性中耳炎 总被引:2,自引:0,他引:2
用Nd:YAG激光在鼓膜前方造孔,孔径2~3mm,多数病例听力改善在半年内未再出现中耳积液。激光治疗分泌性中耳炎具有显效、简单、安全,易于推广的实用价值。 相似文献
8.
激光二极管抽运Nd:YAG双薄片激光器 总被引:4,自引:6,他引:4
激光介质的热效应是高平均功率固体激光器面临的最大挑战,采用薄片激光介质是解决热效应的有效手段之一。当在抽运区尺寸远大于薄片厚度并且抽运光均匀分布的条件下,热流近似为沿厚度方向的一维分布,从而大大降低介质的热透镜效应和热致应力双折射。设计了四通光学耦合系统,通过提高二极管激光器阵列输出激光强度分布的均匀性,并优化经微柱透镜准直后光束的发散角,实现了抽运光的近平顶分布。采用两片1 mm厚的Nd∶YAG薄片激光介质,在两个峰值功率2000 W,占空比为15%的二极管激光器阵列抽运下,获得了峰值功率1440 W,平均功率216 W的准连续激光输出,光光转换效率达到36%,电光转换效率超过16%,在稳腔下测得的光束质量M2 因子约为12×13。 相似文献
9.
115-W Tm:YAG diode-pumped solid-state laser 总被引:12,自引:0,他引:12
Honea E.C. Beach R.J. Sutton S.B. Speth J.A. Mitchell S.C. Skidmore J.A. Emanuel M.A. Payne S.A. 《Quantum Electronics, IEEE Journal of》1997,33(9):1592-1600
A compact diode-pumped Tm:YAG laser capable of generating greater than 100 W of CW power at 2 μm has been demonstrated. A scalable diode end-pumping architecture is used in which 805-nm radiation, coupled to the wing of the Tm3+3H6-3H 4 absorption feature, is delivered to the end of the laser rod via a lens duct. To facilitate thermal management, undoped YAG end caps are diffusion bonded to the central doped portion of the laser rod. For 2% and 4% Tm-doped rods of the same length, the lower doping level results in higher power, indicating that cross relaxation is still efficient while offering lower thermal stress and reduced absorption at the laser wavelength. Output powers for various output coupler reflectivities are compared to the predictions of a quasi-three-level model. Thermal lensing, cavity stability, and stress-induced birefringence measurements are described. The beam quality was analyzed with the 2% Tm-doped rod and a flat output coupler, yielding M2 values of 14-23 相似文献
10.
The combined frequency noise spectrum of two lightwave Model 120-01A nonplanar ring oscillator lasers was measured by first heterodyne detecting the IF signal and then measuring the IF frequency noise using an RF frequency discriminator. The results indicated the presence of a 1/f 2 noise component in the power spectral density of the frequency fluctuations between 1 Hz and 1 kHz. After incorporating this 1/f 2 into the analysis of the optical phase tracking loop, the measured phase error variance closely matches the theoretical predictions 相似文献
11.
We present a theoretical study of the maximum single frequency power that can be obtained from a simple coaxially end-pumped Nd:YAG laser. The approach is general for four-level solid-state laser systems. It is shown that careful control of the pump beam geometry, cavity length, and crystal length can enhance single frequency performance 相似文献
12.
Efficient operation of a diode-pumped Nd:YAG laser at 938.5 nm is reported. A continuous wave output power of 3.9 W is obtained. Single-pass frequency doubling in periodically poled KTiOPO4 (KTP) delivered a power of 88 mW at 469 nm. By intracavity frequency doubling an output of 200 mW in the blue region is achieved 相似文献
13.
K. Kannan F. Frisken P.S. Atherton 《Photonics Technology Letters, IEEE》1991,3(2):124-126
The characteristics of an erbium-doped fiber amplifier pumped by a 532-nm diode-pumped Nd:YAG laser are presented. A maximum system gain of 31 dB at 591 Mb/s is obtained with a corresponding system noise of less than 0.5 dB. An amplified signal output power of greater than 10 mW was obtained, with a coupled pump power of 46 mW and a corresponding quantum efficiency of around 65%. By optimizing the erbium fiber design, higher system gains and saturation power levels are feasible. These figures, and in particular the combination of high output powers and low noise, establish the usefulness of this pump laser as a viable alternative to the semiconductor pump lasers currently under investigation at 1480 and 980 nm.<> 相似文献
14.
15.
16.
17.
Two experiments were carried out to measure the stored energy and heat deposited in the laser medium and to determine the heat parameter χ, defined as the heat deposited per unit of stored energy. The stored energy was calculated from small-signal gain measurements. The heat deposition was calculated from interferometric measurements of the thermally induced optical path length changes of the laser rod under test. χ is to be 1.1 in a 200-μs pump pulse, about one-third of the value obtained for flashpumped Nd:YAG. Without fluorescence decay, χ is 0.7 相似文献
18.
19.
Two-frequency injection-seeded Nd:YAG laser 总被引:1,自引:0,他引:1
Dual longitudinal mode (DLM) operation of a Nd:YAG laser is achieved by simultaneously injection seeding with two seed frequencies. We show that the relative energy in the two frequency components can be adjusted by varying the relative seed power, and that they have excellent spatial, angular, and temporal overlap. The result is a deeply modulated 1.06-μm pulse with a modulation frequency that can be tuned from 185 MHz to at least 17 GHz in 185 MHz increments. In addition to the two seeded frequencies, weak sidebands are also observed in the output spectra. Their energy content is typically less than 1% of that of the seeded modes. We discuss mechanisms which might cause them 相似文献
20.
我们研制了一台二极管连续端泵浦的Nd:YAG激光器,用国产激光二极管作泵浦源,泵浦激光波长为0.808μm。激光介质为φ5×5mm的Nd:YAG棒,输出激光波长为1.06μm,用CCD相机和图象处理系统记录和分析激光光斑,得到激光横模为TEM00模,当输入谐振腔的泵浦功率为225mW时,输出连续激光功率最高达76.4mW,光-光转移效率为33.9%,电光斜效率达到9.1%,并做了腔外倍频实验。 相似文献