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Stimulated rotational Raman conversion has been efficiently demonstrated in all three molecular hydrogen isotopes with a 532-nm Q -switched pump source. Optimum gas pressures and pump focusing have been determined. Single pass conversion efficiencies of 80%, 75%, and 65% have been achieved at the first Stokes wavelengths with H2 , D2, and HD, respectively. The maximum efficiency is generally limited by further Raman conversion of the initially generated Stokes light. The thresholds were found to increase in the order H2 22. The relative thresholds of H2 and D2 are reasonably consistent with the calculated steady-state gains based on the population statistics and the linewidth data. Intermediate frequency shifts such as these may be useful by themselves, or in combination with other nonlinear techniques, as methods to achieve specific wavelengths for system applications 相似文献
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使用脉冲Nd:YAG四倍频激光抽运充有纯D2气体和D2/He混合气体的拉曼池.实验研究了受激拉曼散射的能量转换效率和能量稳定性与系统主要参量,包括抽运光能量、D2气体压强和加入惰性气体He的关系.实验表明,适量惰性气体He的加入在没有降低一阶斯托克斯散射光(S1,波长:289.04 nm)能量稳定性的前提下,有利于提高其能量转换效率,最大能量转换效率达到22.1%.通过实验分析,得到了受激拉曼散射一阶斯托克斯散射光的能量转化效率和能量稳定性的优化条件. 相似文献
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The authors propose and first demonstrate an LiNbO3 waveguide device with cascading quasi-phase-matched second harmonic generation and quasi-phase-matched sum-frequency generation for generation of a third harmonic wave. Ultraviolet light of 355 nm wavelength, which was the shortest value ever reported for LiNbO3 waveguide wavelength-convertors, was obtained with Nd:YAG laser light 相似文献
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A half watt of 266 nm radiation has been generated at a pulse rate of 25 kHz by using KD*P and KTP crystals to frequency quadruple a CW-pumped, acoustoopticQ -switched Nd:YAG laser. 相似文献
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An efficient, scalable, diode-pumped Nd laser design is reported. The gain element can be longitudinally pumped along five separate axes and is relatively simple to fabricate. Both Nd:YAG and Nd:YVO4 gain media were evaluated. Using five single-stripe laser diodes to pump the Nd:YAG, 3.94 W of absorbed power produced 2.1 W CW at 1.06 μm. The slope efficiency was 54 percent and the output was TEM00. The threshold power was 40 mW. No evidence of thermal saturation was observed up to the maximum pump power. Repetitively Q-switched operation is also reported. The maximum output power for Nd:YVO4 obtained with 2.9 W of pump power was 1.3 W. The slope efficiency was 47 percent 相似文献
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255 mW of 1.06 μm, CW, single-longitudinal-mode, TEM00 output has been obtained by end-pumping a twisted-mode cavity Nd:YAG laser with a 1 W diode laser. The key elements of the laser are two λ/4 waveplates (zero-order) placed at both ends of the laser crystal (Nd:YAG, φ3×8 mm). The fast axes of the waveplates are rotated by 90° with respect to each other and rotated by 45° with respect to an intercavity Brewster polariser. In addition, one of the waveplates acts as a resonator and mirror and input coupler for the pump radiation 相似文献
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以铌酸钡钠置于Nd:YAG腔内,采用温度匹配,进行了连续倍频激光的研究,获得0.53微米输出功率达瓦级水平,最高可达2.5瓦以上。 相似文献
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LD泵铺Nd:YVO4/Cr:YAG被动调Q绿光激光器 总被引:1,自引:1,他引:1
报道了一种LD近贴泵浦、KTP晶体腔内倍频的Nd:YVO4/Cr:YAG结构高重复频率被动调Q绿光激光器。在注入泵浦功率为750mW时,得到平均功率86mW、脉冲宽度26.6ns、重复频率79.2kHz、峰值功率41.1W的被动调Q脉冲绿光输出。 相似文献
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将振荡与放大光束分离,使其分别抽取工作物质不同部位的贮能,可以获得较高功率和效率,也降低了对工作物质光学均匀性的要求。 相似文献
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Nd:LaF3 and Nd:LaMgAl11O19 (LMA) are promising candidates for pulsed diode-laser-pumped lasers because they have relatively long upper state lifetimes and large absorption bandwidths compared to other Nd3+ doped materials. Crystal growth of LMA and the spectroscopic properties of both materials are described. Continuous-wave (CW) end-pumped lasers have been demonstrated in these materials using a Ti:Al2O3 laser to simulate the diode-laser pump source. Slope efficiencies of 47% for Nd:LaF3 and 32% for Nd:LMA were obtained. The results for Nd:LaF3 are typical for end-pumped, CW, Nd3+ lasers; the lower slope efficiency for Nd:LMA is attributed to excited-state absorption 相似文献
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H. Yamamoto 《Microelectronics Reliability》1996,36(2):151-168
A (linear or circular) connected-(r1, s1)-or-(r2, s2)-or-. .-or-(rk, sk)-out-of-(m, n): F lattice system is the (linear or circular) (m, n)-lattice system if the system fails whenever all components in a connected-(r1, s1)-submatrix or all components in a connected-(r2, s2)-submatrix or . . or all components in a connected-(rk, sk)-submatrix fail. This paper presents a recursive algorithm for the reliability of the (linear or circular) connected-(r1, s1)-or-(r2, s2)or-. .-or-(rk,sk)-out- of-(m, n):F lattice system. The recursive algorithm requires
time and
time in the linear case and the circular case, respectively Furthermore, we can reduce the more computing time in the statistically independent and identically distributed case or considering some special systems. Especially, the closed formula is given for the reliability of the linear connected-(2, 1)-or-(1, 2)-out-of-(m, 2): F lattice system in the statistically independent and identically distributed case. 相似文献
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用单纵模Nd:YAG二倍频激光(波长532nm,线宽0.003cm^-1,脉宽(半峰全宽,FWHM)6.5ns)抽运Hz/He气体,观察到很强的后向一阶斯托克斯(BS1)受激拉曼散射。在Hz的分压分别为1.0MPa和1.5MPa的Hz/He(体积比)(3/7)混合气体中,当抽运能量为92mJ时,后向一阶斯托克斯光的量子转换效率高达69%左右,而在纯Hz中后向一阶斯托克斯光的量子转换效率分别只有15%和18%。这是因为加入He增强了后向拉曼散射多普勒线宽的Dicke压窄效应,使后向一阶斯托克斯光的拉曼增益系数与前向一阶斯托克斯(FS1)光的拉曼增益系数的比率提高,而且因为后向一阶斯托克斯光与抽运光在反方向传播,它可以提取大部分抽运光的能量,并且脉冲被压窄到1.1ns,使后向一阶斯托克斯光峰值功率达到了抽运光的2.6倍。从激光光斑的强度分布可以观察到后向一阶斯托克斯光呈现为抽运光的相位共轭波。 相似文献
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LD抽运的Cr4+:YAG被动调Q Nd:YAG激光器 总被引:6,自引:4,他引:2
研究了不同谐振腔下不同透射率的Cr4+:YAG调Q的激光输出特性.采用透射率为82%的Cr4+:YAG,在抽运功率1.1 W时,激光重复频率小于3 kHz,单脉冲能量达20 μJ,可以作为微脉冲激光雷达的发射光源.分析和比较了实验结果和理论计算,两者吻合较好. 相似文献
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《Quantum Electronics, IEEE Journal of》2007,43(2):157-167
The continuous-wave laser operation of Nd-doped tetragonal NaLa(WO 4)2 crystal is studied at room temperature by optical pumping in the spectral region overlapping AlGaAs diode laser emission. This crystal has inhomogeneously broadened optical bands. From the room-temperature spectroscopic parameters determined it is found that the optimum Nd concentration for the 4F3/2rarr4IJ laser channels must be in the 3-5 at.% range. For J=11/2 and 13/2 channels (lambdaap1.06 and 1.3 mum) the most favourable polarization configuration is parallel to the crystallographic c axis, while for J=9/2 little polarization dependence of the laser efficiency is predicted. Laser operation was achieved with a 3.35 at.% Nd-doped sample grown by the Czochralski method. The laser operation was tested in an hemispherical optical cavity pumped by a Ti:sapphire laser. Stimulated emission at lambda=1056 nm was achieved for a wide spectral pumping range, lambda=790-820 nm. Stimulated Raman scattering was achieved in the picosecond regime with an efficiency similar to that of monoclinic KY(WO4)2 reference compound 相似文献