选用新介质的双池受激布里渊散射系统的研究

从介质化学结构与吸收系数的关系入手，寻找出系列吸收系数小，适合作为放大池介质的新介质，例如四氯乙烯(C₂Cl₄)，1，3-六氯丁二烯(C₄Cl₆)和六氟化苯(C₆F₆)等，并计算或测量了入射光波长为1.064μm时的新介质受激布里渊散射(SBS)参数.在双池SBS系统的放大池中分别选用C₂Cl₄和C₄Cl₆，振荡池中均选用光学击穿阈值高，并且布里渊频移与C₂Cl₄和C₄Cl₆的布里渊频移非常接近的乙醇(C₂H₅OH)，并利用Nd:YAG调Q激光器研究了该系统的性能.实验结果表明，该系统具有高负载能力，高相位共轭保真度和高能量反射率稳定度等性能. 关键词： 受激布里渊散射 双池SBS系统 新介质     

利用不同介质进行布里渊放大的研究

研究了受激布里渊散射振_放双池系统中振荡池和放大池选用不同种类介质的情况.理论分析 结果表明，当两种介质的布里渊频移接近，布里渊线宽有交叉时，系统仍具有放大作用.采 用CCl4作为放大池介质，CCl4/CS2的混合介质作为振荡池介质，利用Nd:YAG调Q 激光研究了布里渊频移的偏离对布里渊放大的影响，结果表明，当布里渊频移的偏离较小时 ，其种子光放大率和种子光脉宽压缩率仍然很大.采用CS2作为放大池介质，苯作为振荡池 介质，对振 放双池系统进行了实验研究，其种子光放大率达到44，种子光脉宽压缩率为 72，相位共轭保真度为98%，种子光放大率的稳定度小于3%. 关键词： 受激布里渊散射 布里渊放大 布里渊频移 布里渊线宽     

混合介质的SBS参数随混合比变化的研究

从混合介质的折射率、黏度、密度和声速等物理量随混合比的变化关系入手,推导出了混合介质的布里渊线宽、声子寿命和增益系数等受激布里渊散射(SBS)参数随混合比的变化关系.数值模拟了HT-70/FC-72混合介质的布里渊线宽、声子寿命和增益系数随FC-72体积分数的变化关系,并测定了该混合介质的吸收系数和光学击穿阈值随FC-72体积分数的变化关系.结果表明,HT-70/FC-72混合介质的SBS参数随FC-72体积分数单调变化,不出现极值现象.混合介质的选用不仅增加了SBS介质的种类,而且能够满足SBS系统对不 关键词： 受激布里渊散射 混合介质 SBS参数     

选用混合介质优化介质和控制受激布里渊散射特性的研究

本文提出了选用混合介质优化介质和控制其SBS特性的方案.分析了全氟碳化合物系列液体介质具有良好互溶性的缘故,数值模拟了HT-230/FC-72混合介质的增益系数、声子寿命和布里渊频移随混合比的变化曲线.在Countinuum Nd:YAG种子注入激光系统中测定了HT-230/FC-72混合介质的吸收系数和光学击穿阈值随混合比的变化,并实验研究了混合介质的能量反射率和Stokes光脉冲波形随混合比的变化.通过选用混合介质不仅优化介质,而且在一定范围之内可控制其SBS特性. 关键词： 受激布里渊散射 混合介质 优化介质 控制SBS特性     

氯化钠水溶液的受激布里渊散射效应研究

研究了氯化钠水溶液的受激布里渊散射效应,在实验上得到了 SBS 谱,并从而计算了 SBS 频移、STOKES 线宽、氯化钠水溶液的声速、体积压缩系数以及声子寿命。同时也测量了 SBS 阈值、能量转换率以及脉冲压缩系数。对实验结果进行了理论分析。     

变温条件下受激布里渊散射增益系数的实验测量

从理论及实验上分析了介质温度对受激布里渊散射(stimulated Brillouin scattering, SBS)阈值及增益系数的影响.在理论分析的基础上, 提出了一种通过测量SBS阈值来决定介质SBS增益系数的新方法. 实验及测量结果表明, SBS增益系数会随着介质温度的增加而呈现指数上升的趋势. 关键词： 受激布里渊散射 阈值 增益系数     

受激布里渊散射新介质——全氟胺的研究

本文从介质化学结构与受激布里渊散射(SBS)特性的关系入手,寻找出了SBS特性良好的全氟胺系列新介质——FC-131,FC-3283,FC-40,FC-43,FC-70等,并测定或计算出了新介质的SBS参数. 结果表明,新介质的吸收系数均小于10^-3 cm^-1,光学击穿阈值均高于100 GW/cm². 全氟胺系列新介质不仅具有良好的SBS特性,而且还具有无毒、低挥发性和高稳定性等一系列独特的物理化学性质. 新介质的发现不仅增加SBS介质的种类,而且能够有效提高SBS系统的性能,对于SBS相位共轭镜在高功率激光系统中的应用打下了良好的基础. 关键词： 受激布里渊散射(SBS) 全氟胺 吸收系数 光学击穿阈值     

利用受激布里渊散射能量反射率测量液体介质运动黏度方法的研究

本文提出了一种利用受激布里渊散射(SBS)能量反射率的变化测定不同温度时的液体介质运动黏度的方法.液体介质的运动黏度随温度而变化,这导致了介质增益系数和SBS能量反射率的变化,因此通过SBS能量反射率的变化可测定不同温度时的液体介质的运动黏度.在Countinuum Nd: YAG种子注入激光系统中测定了不同温度时的水的运动黏度并与运动黏度计测定的结果进行了比较.用本方法获得的不同温度时的水的运动黏度测量值与运动黏度计测量值很接近,相对误差小于5%. 关键词： 受激布里渊散射 SBS能量反射率 温度 运动黏度     

受激布里渊散射对激光在水中衰减特性的影响

测量了不同能量的光束,通过不同长度的水介质在窄线宽与宽线宽两种情况下的衰减系数,研究了受激布里渊散射对激光在水中衰减特性的影响.结果发现,激光光束在水中传播时的衰减系数与激光光强和线宽有关,而不是通常情况下所认为的常数.还从理论上进行了分析. 关键词： 衰减系数 受激布里渊散射     

光脉冲编码对基于拉曼放大的布里渊光时域分析系统的影响

报道了光脉冲编码对基于拉曼放大的布里渊光时域分析系统(BOTDA)的影响. 实验表明,光脉冲编码能够在保证较高空间分辨率的同时减小布里渊频移的不确定性. 实验实现了49.6 km传感距离, 在整段传感光纤上温度分辨率1 ℃,空间分辨率2.5 m. 本文实验测量并分析了系统的信噪比和光功率分布特性. 关键词： 分布式光纤传感 受激拉曼散射 布里渊增益 布里渊光时域分析系统(BOTDA)     

Investigation on improving characteristics of two-cell SBS system with CCl4/C2H5OH liquid mixture

In order to improve the performance of the two-cell stimulated Brillouin scattering （SBS） system, this paper proposes the methods of using mixtures, which require amplifier media to have small absorption rate, and generator media to have high optical breakdown threshold and Brillouin frequency shift equal to that of the amplification media. The characteristics of the two-cell SBS system are studied experimentally by using CCl4 as amplifier medium and CCl4, C2H5OH and CCl4/C2H5OH liquid mixture as generator medium pumped by Nd：YAG Q-switched laser. The obtained results show that liquid mixture in generator cell improves the power load ability, phase conjugation fidelity, energy reflectivity （ER） and ER stability.     

Study on two-cell stimulated Brillouin scattering system with mixture medium

In this paper,a method of choosing mixture medium in two-cell stimulated Brillouinscattering(SBS)system to improve the system performance is proposed.The Brillouin frequency shift(BFS)of mixture medium varies with the mixing ratio andthus the difference of the BFS between the two cells can be eliminated.The two-cellSBS system with acetone(C3H6O)in its generator cell and mixture liquid ofCCl4/C2Cl4 in its amplifier cell is investigated.The C3H6O has a high optical breakdown threshold and the mixture liquid of CCl4/C2Cl4 has a small absorption coeffi-cient and the same BFS as that of C3H6O when the volume fraction of CCl4 is 4%.Compared with two-cell SBS system with the same liquid(C2Cl4)or different liquid(C3H6O and C2Cl4)in generator and amplifier cell,the SBS system with mixture liq-uid(CCl4/C2Cl4)in amplifier cell and C3H6O in generator cell improves thepower-load,energy reflectivity(ER),phase conjugation(PC)fidelity and ER stabil-ity.     

Numerical analysis of stimulated Brillouin scattering in high-power double-clad fiber lasers

A theoretical analysis of stimulated Brillouin scattering (SBS) in linear cavity Yb³⁺-doped double-clad fiber lasers is presented by solving the steady-state rate equations with the SBS. The effects of cavity length, fiber core diameter, input mirror reflectivity at Stokes wavelength, Yb³⁺ concentration and laser linewidth on the SBS are discussed. Numerical results show that the SBS threshold power can be improved by shortening the cavity length, using large mode area fiber, reducing the input mirror reflectivity at Stokes wavelength, lowering the Yb³⁺ concentration and broadening the laser linewidth, and the influence of the laser linewidth on the SBS threshold power is more noticeable than other system parameters.     

Submillimeter-wave ESR measurements of low-dimensional quantum spin systems

Temperature-dependent electron spin resonance (ESR) measurements of two low-dimensional quantum spin systems, theS = 1/2 spin-ladder system Cu₂(1,4-diazacycloheptane)₂Cl₄ (Cu₂(C₅H₁₂N₂)₂Cl₄) and the gaplessS = 1 bond-alternating one-dimensional antiferromagnettrans-Ni(333-tet)(N₃)(ClO₄), have been performed. X-band electron spin resonance (ESR) measurements of single-crystal Cu₂(C₅H₁₂N₂)₂Cl₄ show the increase of linewidth and anisotropicg-shifts below 8 K similar to those known for one-dimensional antiferromagnet. On the other hand, Ni(333-tet)(N₃)(ClO₄) has broad line-width and ESR has been observed for the first time by our high-field ESR. Its linewidth increases as the temperature is decreased, while theg-shift seems to be isotropic and theg-value decreases as the temperature is decreased. Thisg-shift can be connected to the quantum fluctuation of the system.     

Observations of wavefront reproduction by stimulated Brillouin and Raman scattering as a function of pump power and waveguide dimensions

Experimental investigations have been made of wavefront reproduction (WFR) by backward stimulated Raman scattering (SRS) and backward stimulated Brillouin scattering (SBS) in CS₂ and C₇H₆O using a linearly polarized ruby pump at λ=0.694 μm. The studies were carried out as a function of the length and cross-section of the optical waveguide and the pump power at the input to the nonlinear medium; curves showing the percentage of nonreproduced backscattered radiation versus power into the waveguide are presented. In all of the cases studied the degree of reproduction by SBS was higher than that by SRS and the efficiency of WFR for both SBS and SRS improved as the pump power into the waveguide was increased, the bore diameter of the lightpipe decreased, and the length of active media decreased.     

Spectrum evolutions of spontaneous and pump-depleted stimulated Brillouin scatterings in liquid media

A theoretical model for calculating spontaneous and stimulated Brillouin scattering(SBS) spectra is described. An empirical formula for the Stokes output spectral linewidth, a function of spontaneous Brillouin linewidth and the exponential gain coefficient, is obtained by the calculated data fitting. The formula holds true for two cases involving pump undepletion and depletion. The lineshape change from spontaneous to highly pump-depleted SBS spectra is also investigated. The result shows that for the pump power below the SBS threshold, the Stokes output spectral lineshape evolves from Lorentzian to approximately Gaussian as the pump power increases. For the pump power near or beyond the threshold, the SBS spectrum is in the form of a steady Gaussian profile, and the spectral linewidth comes to a certain value about 7 times narrower than the spontaneous one. The theoretical results are experimentally demonstrated by using several common liquid media.