共查询到17条相似文献,搜索用时 140 毫秒
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钾原子中由四波,六波混频过程产生的相干辐射 总被引:2,自引:1,他引:1
当双光子共振激发钾原子于6S能级时,由光泵受激辐射,串级受激辐射参与的四波、六波混频以及电离复合的布居过程,产生了位于可见区的诸多相干辐射,文中对混频机制进行了分析和讨论,并对所测得的相干辐射进行了标识。 相似文献
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钾原子中多种受激辐射参与的混频过程 总被引:2,自引:1,他引:1
当双原子共振激发钾原子于6S能级时,由光泵受激辐射和电离复合受激辐射参与的六波或四波混频,产生了位于紫外和紫区的诸多相干辐射、文中对多种混频机制进行了分析和讨论,并对所测得的相干辐射线进行了标识. 相似文献
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双光子激发钠原子所产生的级联受激辐射光子与入射激光双光子可产生光波混频。实验共观测到十一条六波混频与十条四波混频谱线。理论分析表明脉冲激光泵浦下的光波混频过程仍可用稳态近似计算混频光强。非线性极化系数X不仅与基态布居数也与激发态布居数有关。X的共振增强效应对获得强混频输出有重要作用。 相似文献
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本文报道以等频二步激发钠分子-原子系统,观测到强度随泵浦光的调谐而呈振荡变化的3P—4P受激喇曼散射,以及对应4D—4P和4F—3D跃迁的红外受激辐射和由四波混频产生的816.8~822.1nm区内可调谐相干辐射。文中对这些过程进行了分析讨论。 相似文献
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本文首次报道了由钾分子-原子系统的混合激发和碰撞能量转移过程产生4F→3D受激辐射以及由钾原子的4S→4F偶极禁戒双光子共振产生4F→3D受激辐射和四波混频的研究结果。 相似文献
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利用汞原子6~1S_0—7~1S_0双光子共振四波和频产生了125nm的相干辐射.对双光子共振增强效应、双光子共振克尔(Kerr)效应进行了研究.讨论了平面波和聚焦情况下最佳相位匹配的条件.实验中还观测到了四波参量振荡和四波差频的信号输出. 相似文献
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UV coherent radiation at 330.2 nm and IR stimulated radiations at 2.34μm,2.21μm and 1.64μm were generated via processes of unequal-frequency two-photon(3S-6S)resonantly enhanced excitation and equal frequency hybrid resonant excitation with particularexcited wavelength in Na_2-Na system.The competition of the two processes is obviously. 相似文献
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本文报道了以620.6 ̄665.0nm范围内任意波长激光作用下产生的锂分子高位态紫外扩散带受激辐射的实验结果,在锂分子-原子系统中,由激光双光子激发、并通过碰撞能量转移过程以及多光子电离复合过程使锂分子高位态获得布居,从而得到紫外区扩散受激辐射,该辐射来自较高的某个三重态向低排斥态a^3Σu^+的跃迁的结果。文中对有关的辐射特性及激发机制进行了详细的分析和讨论。 相似文献
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Tunable coherent radiation around 840, 830, and 795 nm has been generated upon two-photon excitation of sodium 4d and 5s levels, respectively. The generation is due to special parametric processes. A molecular nature of the emissions, as recently proposed, can be ruled out by the performed investigations. 相似文献
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599.2 nm diffuse band radiation generated by two-photon exciting molecular and atomic potassium 总被引:1,自引:0,他引:1
Diffuse band radiation around 599. 2 nm in K_2 was generated by the two photon pumping potassium dimers or by the two-photon resonant pumping atomic potassium with following atoms-molecules collision energy transfer. The pumping wavelengths are in a wide range of 697-745 nm. The relevant mechanisms were discussed. 相似文献
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An analysis of the results of previous studies of stimulated scattering of UV pulses in liquids has shown that they disagree with the theory of stimulated scattering. To resolve the inconsistency, stimulated scattering of XeCl excimer laser radiation (λ = 308 nm) with pulse duration τ ≈ 8 ns in liquid hexane is investigated experimentally. A theoretical analysis of the results obtained revealed a new nonlinear optical phenomenon: stimulated thermal scattering induced by the heating due to two-photon absorption, called two-photon stimulated thermal scattering (two-photon STS-2). The stimulated backscatter spectrum contains a previously unknown line corresponding to two-photon STS-2 and a newly discovered SBS line in the UV region. The line is observed in experiment on liquid hexane and is characterized by the frequency shift ΩB = 0.33 cm?1 relative to the pump wavelength λ = 308 nm, in complete agreement with the theory of stimulated Brillouin scattering (SBS). The spectral line called the SBS line in previous studies has a frequency shift much smaller than that predicted by the SBS theory and must be interpreted as an unshifted two-photon STS-2 line. When two-photon STS-2 is used to obtain a phase-conjugate wave, the phase-conjugation fidelity is lower than that achieved by using SBS because of thermal self-action and slow decay of the thermal grating. 相似文献