共查询到16条相似文献,搜索用时 78 毫秒
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在考虑了光参量啁啾脉冲放大中的脉冲波形、相位失配和时间同步抖动情况下,给出了计算光参量啁啾脉冲放大增益特性更为完善的三波耦合理论模型。并在1 ns的时间同步抖动情况下,对比分析了光参量放大在小信号放大及饱和放大时的增益稳定性。光参量放大的时间同步抖动对增益影响非常大,使放大信号光脉冲的增益光谱发生了明显的偏移,波形不对称和整个增益降低;并且信号光光谱越宽,光参量放大间的时间同步抖动对其增益影响越严重;但随着参量放大增益饱和的出现和加深,信号光和抽运光之间的同步时间抖动对放大信号光的输出强度影响减弱,即在饱和放大处可以获得更稳定的放大信号光输出。 相似文献
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在考虑了光参量啁啾脉冲放大中的脉冲波形、相位失配和时间同步抖动情况下,给出了计算光参量啁啾脉冲放大增益特性更为完善的三波耦合理论模型。并在1 ns的时间同步抖动情况下,对比分析了光参量放大在小信号放大及饱和放大时的增益稳定性。光参量放大的时间同步抖动对增益影响非常大,使放大信号光脉冲的增益光谱发生了明显的偏移,波形不对称和整个增益降低;并且信号光光谱越宽,光参量放大间的时间同步抖动对其增益影响越严重;但随着参量放大增益饱和的出现和加深,信号光和抽运光之间的同步时间抖动对放大信号光的输出强度影响减弱,即在饱和放大处可以获得更稳定的放大信号光输出。 相似文献
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受激布里渊散射相位共轭光泵浦的高效率光学参量振荡器 总被引:2,自引:1,他引:1
报道了在Nd:YAG1.06μm激光器上,用受激布里渊散射(SBS)后向放大输出作泵浦光源,用光学参量振荡(OPO)的方法,获得1.57μm激光输出,最大输出能量为21.6mJ,相应的转换效率为32%,并与直接用Nd:YAG1.06μm激光泵浦结果相比较,效率提高1.9倍,阈值降低1.7倍,实验结果与理论分析符合的较好。 相似文献
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非共线相位匹配的参量增益分析 总被引:2,自引:0,他引:2
对非共线Ⅱ类相位匹配的KTP飞秒光学参量振荡器进行了分析和理论研究,用数值方法得出参量增益的变化曲线和参量光的光强分布,与共线相位匹配相比,非共线方案具有更高的参量增益,更好的光束质量,特别适合飞秒光学参量的振荡器。 相似文献
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在皮秒短脉冲泵浦的光参量啁啾脉冲放大(ps-OPCPA)系统中,泵浦光与信号光之间的高精度时间同步是需要解决的关键问题之一.本文基于中国工程物理研究院激光聚变研究中心的全OPCPA激光装置,对用于前端ps-OPCPA中泵浦光与信号光的高精度同步主动控制技术进行了详细研究.采用大啁啾信号光窄光谱光参量放大的主动反馈方式,通过合理设计反馈光路信号光的时域展宽啁啾系数,将泵浦光与信号光的同步时间抖动从ps量级降低至百fs量级的时间范围,从而极大地改善了前端ps-OPCPA的能量和光谱不稳定性:7 min测试时间内泵浦光与信号光相对同步时间抖动的均方根值(RMS)从458 fs改善至93 fs,输出能量RMS不稳定性从30.3%改善至3.15%,且维持光谱宽度大于100 nm的稳定宽光谱输出. 相似文献
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Spatial quantum optics and quantum information based on the high order transverse mode are of importance for the super-resolution measurement beyond the quantum noise level. We demonstrated experimentally the transverse plane TEM01 Hermite-Gauss quantum squeezing. The squeezed TEM01 mode is generated in a degenerate optical parametric amplifier with the nonlinear crystal of periodically poled KTiOPO4. The level of 2.2-dB squeezing is measured using a spatial balance homodyne detection system. 相似文献
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The intermodal interference of the LP01 and LP11 modes and determination of the equalization wavelength in the liquid-core optical fiber is presented. Theoretically was described the weakly guiding optical fiber with the constant core radius, where equalization wavelength is a function of the refractive indices of core and cladding. The dependence of equalization wavelength on refractive indices is employed for measurement of temperature. Temperature sensitivity using intermodal interference of modes LP01 and LP11 was documented in the liquid-core optical fiber consisted of fused silica as cladding and medicinal oil as a core. In the investigated temperature range the intermodal interference allows the temperature measurement with resolution of about 0.02 °C. 相似文献
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基于Hanbury Brown-Twiss(HBT)实验,我们借助于两个单光子计数模块,一个50/50分束器和一个快速计数卡(FastCom-P7888)研究了不同光场的二阶相干度。我们首先制备了脉冲相干光,连续相干光以及单原子发出的单光子源,并测量这几种不同光场的二阶相干度g(2)(τ)。我们通过测量俘获在磁光阱(MOT)和远失谐偶极阱(FORT)中的单原子在近共振连续激光激发下所辐射的荧光的二阶相干度,分别得到了g(2)(τ=0)=0.08和g(2)(τ=0)=0.09,借助于实验中产生的脉冲光与单原子,接下来我们将进行触发式单光子源的实验研究。 相似文献
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P.S. Fennell J.S. Dennis A.N. Hayhurst 《Proceedings of the Combustion Institute》2009,32(2):2051-2058
Measurements of the oxidation of a coal char in a fluidised bed have the advantages that the rates of heat and mass transfer to and from a reacting particle are large and characterised well. However, problems have arisen from a combination of the slow, but typical, response–time (4 s) of the analysers for CO and CO2 and the slow mixing of gases when filling a fairly large fluidised bed. The resulting time constant for the sampling system was 8 s and comparable to the time for combustion at 900 °C or above. The purpose of this work was to measure the kinetics of oxidation of a char in a smaller fluidised bed (with a shorter mixing time) using an analyser for CO and CO2 with a response time as low as 0.1 s. The result is that the oxidation of an anthracitic char is now found to be first order in O2 between 700 and 900 °C; at 900 °C the order previously measured was almost zero. The activation energy is now measured here to be 145 ± 25 kJ/mol, in agreement with some early work. 相似文献
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The effect of K on the morphology of Au nanoparticles deposited on TiO2(1 1 0) surface is investigated by STM-STS and AES methods. For comparison, the enhanced concentration of oxygen defect sites generated by Ar+ bombardment was also studied. It was found that both the K additive and the oxygen defect sites induce a pronounced decrease in the average size of the Au nanoparticles evolved at 320 K. On the clean TiO2(1 1 0) the average size of Au particles is 4.3 nm at approximately monolayer coverage of gold, while in the presence of K or oxygen vacancies this value decreased to 2.5 nm. In spite of the reduced average diameter detected at room temperature, the mean size of the Au nanoparticles increased significantly from 2.5 nm up to 7 nm on the effect of annealing at 500-700 K for K precoverages of 0.3-1 ML. For the clean and the Ar+ pretreated TiO2(1 1 0) surfaces the mean size of the Au particles changed only slightly on the effect of the same thermal treatments. 相似文献