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1.
采用放大1064?nm掺镱光纤激光器作为泵浦源,实现了中红外3.8?μm?MgO:PPLN光参量振荡(OPO)激光输出.在泵浦源中,采用分布式反馈激光器(DFB)作为种子源来实现光纤激光窄线宽的调制,实现线宽2.5?nm到0.1?nm的压缩,最大平均输出功率可达40?W.进一步对不同泵浦线宽条件下中红外3.8?μm?M...  相似文献   

2.
We demonstrate a diode-pump Tm~(3+)t-doped all-fiber laser operating at 1908 nm based on a master oscillator power amplifier(MOPA) configuration. In our work, 152 W of laser output power is generated by a total incident pump power of 434 W at 790 nm, corresponding to the total optical efficiency of 35%. The laser wavelength is1908.29 nm. To the best of our knowledge, it is the highest output power reached around 1908 nm with such a narrow linewidth of 0.18 nm based on a MOPA configuration.  相似文献   

3.
利用相位共轭极化拍频光谱术对V型三能级系统中的光子回波进行了研究,当抽运光束为宽带线宽且相对时间延迟〉0时,单光子四波混频对应于三脉冲受激光子回波。抽运光束为宽带线宽且相对时间延心〈0的情形与抽运光束为窄带线宽的情形类似,这种技术在测量激发态之间的能级分裂时,可得到消除多谱勒增宽的测量精度。  相似文献   

4.
百瓦级全光纤结构单频掺铥主振荡功率放大器   总被引:2,自引:1,他引:1       下载免费PDF全文
报道了平均功率超过百瓦的单频掺铥全光纤结构主振荡功率放大器。使用线宽小于100kHz、中心波长为1.97μm的单频种子源进行级联放大,主放大器的斜率效率为50%。监测放大器的回光功率和光谱,没有发现受激布里渊散射以及其他非线性效应。通过增加泵浦功率,可以获得更高功率的掺铥单频放大输出。  相似文献   

5.
报道了一台基于同带泵浦技术的主振荡功率放大(MOPA)结构超荧光光纤光源。首先利用自行搭建的超荧光种子源获得了半高全宽(FWHM)线宽10.3 nm的宽谱超荧光种子,经光谱滤波得到FWHM线宽1.8 nm的窄谱种子光;种子光经二级预放大器放大至104.4 W后注入主放大器;主放大器最高输出功率3.14 kW,最高输出功率时光光转换效率80.74%,光谱FWHM线宽4.68 nm,光束质量因子为1.59。进一步提高系统泵浦功率有望获得更高功率输出。  相似文献   

6.
王岩山  王珏  常哲  彭万敬  孙殷宏  马毅  高清松  张凯  唐淳 《强激光与粒子束》2020,32(1):011006-1-011006-3
基于简单的主振荡功率放大结构,演示了一种高功率窄线宽线性偏振全光纤激光器,其最大输出功率为3.08 kW,3 dB线宽为0.2 nm。在整个功率缩放过程中,偏振消光比约为94%,光束质量M 2约为1.4。这是国内外首次实现3 kW全保偏光纤激光输出,与基于相位调制的窄线宽激光器相比,该激光器可实现近似的线宽,同时具有受激布里渊散射阈值高、系统结构简单、成本低等特点。  相似文献   

7.
一种基于增益调制技术的全光纤化脉冲Yb光纤激光器   总被引:1,自引:1,他引:0  
以波长为975 nm的半导体激光器作为泵浦源,周期性地脉冲泵浦一个包含Yb掺杂光纤和光纤光栅对的Yb光纤激光器,实现了基于增益调制技术的全光纤化高功率Yb光纤激光器的稳定脉冲输出.在50 kHz重频下,采用20 W的泵浦功率和2.4 μs的泵浦脉冲宽度,获得了1 060 nm波长脉冲宽度仅100 ns的稳定脉冲激光输出,单脉冲激光能量约为20 μJ.以此作为脉冲激光种子进行功率放大,获得了性能稳定的全光纤结构高功率脉冲激光输出,放大后单脉冲能量超过200 μJ,激光放大器斜率效率达到60%.  相似文献   

8.
The output of two grating-stabilized external-cavity diode lasers was injected into a semiconductor tapered amplif ier in a master oscillator-power amplif ier (MOPA) configuration. At a wavelength of 671 nm this configuration produced 210 mW of power in a diffraction-limited mode with two frequency components of narrow linewidth. The frequency difference delta was varied from 20 MHz to 12 GHz, while the power ratio of the two components was freely adjustable. For delta < 2 GHz additional frequency sidebands appear in the output of the MOPA. This configuration is a f lexible and simple high-power cw laser source for light with multiple narrow-linewidth frequency components.  相似文献   

9.
Physical principles, new ways and means of creation, schemes, characteristics and features of efficient high-power tunable pulse Raman lasers, operating in the near and middle ir are reviewed. The paper includes: tunable dye and Nd lasers as pump sources; promising active media and their optimal excitation methods; optical systems for producing spatially homogeneous pumping; the physics of Raman oscillators and their practical schemes, efficient high pulse energy liquid N2 and compressed H2 Raman oscillators, covering several bands in the range between 1.4 and 9.2 μm; the physics and construction of efficient tunable Raman amplifiers-convertors, amplifying in the saturation regime of spontaneously scattered or beforehand produced and collimated external Stokes signals, obtained in the spectral range between 0.83 μm and 18 μm. Raman laser using a, so-called, broadband pump where the linewidth of pumping light is broader than the spontaneous scattering linewidth, are also discussed. Features of both amplification and oscillation regimes of such broadband pumped Raman lasers are reported, and conditions for the efficient frequency conversion are determined.  相似文献   

10.
We develop an injection-seeded single-frequency neodymium-doped yttrium aluminum garnet (Nd:YAG) laser with 500 Hz repetition rate and high peak power. The laser construction is designed as seed injection and master oscillator power amplifier (MOPA) including single-frequency master oscillator, extra-cavity frequency doubling crystal, and round-trip power amplifier. The master oscillator can emit 1,064 nm laser of 8.4 mJ with 6.8 ns pulse width at the pump energy equal to 23 mJ. A green laser energy of 1.1 mJ is obtained by setting the proper temperature of the LBO crystal. The pulse energy of 1,064 nm laser decreases to 6.5 mJ after passing through the LBO crystal and rises to 25.3 mJ after a round-trip power amplifier corresponding to the extraction efficiency of 29%. The final output pulse width is 6.5 ns, representing a peak power of 3.9 MW. The 1,064 nm laser beam quality factor M2 of the master oscillator and the amplified one are 1.3 and 1.5, respectively. The laser will be used to generate mid-infrared where the 532 nm laser with narrow pulse width is to pump sheet optical parametric oscillator (OPO) and the 1,064 nm laser with high peak power to pump the OPO.  相似文献   

11.
理论和实验研究了宽带(15GHz)KrF激光泵浦的受激布里渊散射(SBS)在SF6介质中的转换效率和脉宽压缩比的规律。介质在1.6MPa、透镜焦距为15cm和30cm时,测得SBS最大反射率分别为40%和45%,当泵浦能量大于60mJ时SBS反射率开始趋于平坦;介质在0.85MPa、透镜焦距在30cm时,SBS脉宽压缩比随泵浦能量的上升而下降,最大压缩比为5。建立了宽带多模KrF激光泵浦的SBS理论模型,假设宽带KrF激光光谱谱线由若干窄带谱线组成,这些窄带谱线之间在产生SBS过程中有一定程度的耦合。给出了理论模型结果,并与实验结果进行了比较。  相似文献   

12.
董磊  刘欣悦  陈浩 《中国光学》2015,8(5):800-805
为了研制激光干涉成像所需的主振荡功率放大(MOPA)结构脉冲单频激光器,本文完成MOPA激光器的种子源即声光调Q脉冲单频1 064 nm激光器的特性研究,同时完成种子源腔外倍频绿光特性研究。脉冲单频激光器采用声光调Q模块实现脉宽约20 ns的1 064 nm脉冲激光输出,采用环形腔设计并采用一组不同厚度的标准具实现单纵模运转。实验研究基频1 064nm和倍频532 nm激光脉冲的线宽,得出在全脉宽范围内都具有较高时间相干性的结论。实验分别获得脉宽约28 ns峰值功率约6.5 kW的1 064 nm脉冲单频激光和脉宽约20 ns、峰值功率约0.5 kW的532 nm脉冲单频激光,腔外倍频效率为5.6%。实验同时也验证了腔外倍频的激光脉宽压缩效应。  相似文献   

13.
 理论和实验研究了宽带(15GHz)KrF激光泵浦的受激布里渊散射(SBS)在SF6介质中的转换效率和脉宽压缩比的规律。介质在1.6MPa、透镜焦距为15cm和30cm时,测得SBS最大反射率分别为40%和45%,当泵浦能量大于60mJ时SBS反射率开始趋于平坦;介质在0.85MPa、透镜焦距在30cm时,SBS脉宽压缩比随泵浦能量的上升而下降,最大压缩比为5。建立了宽带多模KrF激光泵浦的SBS理论模型,假设宽带KrF激光光谱谱线由若干窄带谱线组成,这些窄带谱线之间在产生SBS过程中有一定程度的耦合。给出了理论模型结果,并与实验结果进行了比较。  相似文献   

14.
UMSCTS中光子回波的研究   总被引:2,自引:0,他引:2       下载免费PDF全文
张彦鹏  朱京平  唐天同  付盘铭 《物理学报》1998,47(10):1651-1657
对级联三能级系统超快调制光谱学(UMSCTS)中的光子回波进行了研究.当宽带线宽且相对时延τ>0时单光子和双光子四波混频分别对应于三脉冲受激光子回波与和频三能级光子回波.宽带τ<0时与窄带情形类似. 关键词:  相似文献   

15.
We present a nonlinear ytterbium-doped fiber amplifier based on enhanced nonlinear effects that can produce a flat broadband spectrum ranging from 1050–1225 nm with a maximum average output power of 7.8 W at 14 W pump power.Its repetition rate is 89 MHz. Using a pair of gratings and two knife edges as a filter, wavelength tunable picosecond pulses of tens to hundreds of milliwatts can be obtained in the broadband spectrum range. The output power, pulse width, and spectrum(center wavelength and linewidth) are adjusted by tuning the distance of the grating pair and/or the knife edges.Fixing the distance between the two gratings at 15 mm and keeping the output spectrum linewidth at approximately 20 nm,the shortest pulse width obtained is less than 1 ps centered at 1080 nm. The longest wavelength of the short pulses is around1200 nm, and its output power and pulse width are 40 m W and 5.79 ps, respectively. The generation of a flat broadband spectrum is also discussed in this paper.  相似文献   

16.
An efficient narrow-linewidth single-frequency(SF) Yb-doped all-fiber master oscillator power amplifier(MOPA)laser operating at 1064.3 nm is demonstrated experimentally.A ring cavity SF fiber laser is used as the seed source for the MOPA system and the Yb-doped fibers are employed as the gain medium or the saturable absorber.The SF operation is observed to be stable without mode hopping.The highest output power of 266 mW is obtained under the 400 mW pump power with the corresponding slope efficiency of 66.2%.The linewidth of the amplified output laser is approximately 1 kHz and its optical signal-to-noise ratio is over 45 dB.  相似文献   

17.
The reflecting properties of the Fizeau interferometer are used to obtain efficient spectral condensation and tuning of short pulse dye lasers. It is pointed out that the formation of multibeam interference fringes with a divergent beam leads to angular dispersion and resurgence of a part of the beam outside the impact area, which can be used to obtain selective feedback in a laser cavity. With a single Fizeau wedge used as a mirror in a 2 ns pulse laser, a linewidth of 0.01 nm is obtained and the tuning range is of the order of 10 nm. The Fizeau wedge mirror also permits an easy switch from a broadband laser emission to a tunable narrow line or to a tunable narrow hole in a broadband laser spectrum.  相似文献   

18.
粟荣涛  张鹏飞  周朴  肖虎  王小林  段磊  吕品  许晓军 《物理学报》2018,67(15):154202-154202
窄线宽纳秒脉冲光纤拉曼放大器在非线性频率变换、遥感探测和量子信息等领域有广泛的应用前景.综合考虑受激拉曼散射(stimulated Raman scattering,SRS)、受激布里渊散射(stimulated Brillouin scattering,SBS)、自相位调制(self-phase modulation)和交叉相位调制(cross-phase modulation)等非线性效应,建立了窄线宽纳秒脉冲光纤拉曼放大器的非线性动力学模型.仿真分析了放大器中脉冲激光的时频演化特性,对比研究了抽运脉冲宽度、光纤长度和信号光功率等因素对放大器性能的影响.研究发现,上述因素会影响放大器的SRS阈值、SBS阈值、输出激光线宽、激光转换效率等.例如,当脉冲宽度为800 ns时,SBS随着抽运功率的增加而发生,限制了激光功率的提升;减短抽运脉宽可以抑制SBS,但是输出激光的线宽易于展宽到数百MHz以上;增加光纤长度可以获得更低的SRS阈值和更高的转换效率,但是SBS效应和光谱展宽程度也随之增强.系统搭建中需要平衡各非线性效应,选择合适的系统参数.研究内容可以为窄线宽纳秒脉冲光纤拉曼放大器的设计搭建提供参考.  相似文献   

19.
We presented a Nd:YAG master oscillator power amplifier (MOPA) with the compact LD double-end pumped configuration. To acquire the homogenous absorption distribution, a composite short Nd:YAG rod has been employed as the amplification medium and the rod side was well polished to cause total internal reflection (TIR) at the internal wall of the rod. Because the axes of pump LDs and the seed laser occupy the same position, it is relatively easy to obtain both the satisfied mode-matching efficiency and the high absorption efficiency by using two stacked-LD modules. A seed laser, with the input energy of 15 mJ and the pulse width of 46 ns, was amplified through the MOPA structure with the one-pass gain of about 1.2. We have not found any parasitic oscillations from both ends of the amplifier rod until the total pump LD power reached 420 W. The proposed scheme is thought to be useful in a multiple-pass MOPA system for high-average-power applications.  相似文献   

20.
Effect of temporal jitter on the performance of copper vapor laser (CVL) master oscillator power amplifier (MOPA) chain using Monte-Carlo techniques was studied. The MOPA chain comprised an oscillator and five amplification stages. Amplification of CVL signal in each amplifier stage was modeled using rate equation based optical model. The effect of temporal jitter on the pulse energy stability in CVL MOPA chain was estimated for various jitter values. Our studies show that the pulse energy spread and the pulse energy instability increases with increase in jitter which in turn depends on the gain pulse width and the jitter considered. Pulse to pulse gain variation in CVL MOPA chain was studied along with temporal jitter. The acceptable tolerance limit on temporal jitter is ±4 ns for a pulse energy stability of 5% of CVL MOPA chain.  相似文献   

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