DCM中C_3H_6O受激拉曼散射荧光增强特性

本文报道了DCM增强C3H6O受激拉曼散射荧光增强特性研究结果。实验测量了在不同的DCM浓度、不同的泵浦激光强度以及不同的Stokes入射信号条件下Stokes波输出能量,发现当DCM浓度为2×10-4mol/L时,Stokes波最大增强因子达到5.7,Stokes强度随入射激光增强而增强,过强的Stokes输入信号则可能导致Stokes波增益饱和。     

宽频带KrF激光在SF_6介质中的SBS实验研究

宽频带ＫｒＦ激光泵浦高纯度高气压ＳＦ＿６气体产生了受激布里渊背向散射（ＳＢＳ）。实验研究了ＳＢＳ的强度和反射率随泵浦光强和ＳＦ＿６介质密度的变化，测得在ＳＦ＿６气压为１ＭＰａ时，泵浦光能量为１２０ｍＪ，ＳＢＳ光最大能量为１３ｍＪ，反射率为１０％，产生ＳＢＳ的泵浦光阈值１．１８×１０￣４ＭＷ／ｃｍ￣２。实验验证了ＳＢＳ光与泵浦光相位共轭特性，近场均匀性有很大改善，远场光束质量有一定改善，在泵浦光能量１３３ｍＪ，脉宽２５ｎｓ时，得到了脉宽６．８ｎｓ的ＳＢＳ光输出。脉宽压缩比为４。     

KrF激光在SF_6气体中受激布里渊散射的研究

用线宽０．５ｃｍ￣（－１）、脉宽２３ｎｓ的ＫｒＦ激光（２４８ｎｍ）在低气压ＳＦ＿６气体中进行受激布里渊散射（ＳＢＳ）的实验研究。测量了ＳＢＳ反射率随泵浦光能量、气体气压、透镜焦距等实验条件的变化关系，分析和讨论了气体气压、透镜瑞利范围对ＳＢＳ阈值的影响。     

光学材料中横向SBS的稳态分析

从非线性光学的耦合波理论出发,建立了种子光入射的窄带泵浦的横向受激布里渊散射的二维理论模型,并对稳态情形进行了数值模拟,得到了散射光强的二维分布。计算表明,散射光场在入射面内呈现出“局部集中”的特点,而且由于“空间压缩”效应,使得获得的最大散射光强远大于初始泵浦光强。还分析了光场及材料参数对获得的散射光强的影响,得出：入射的激光功率密度越大,光学元件的横向尺寸越长,材料的吸收系数越小,受激散射产生的散射光和弹性声波强度就越大,在材料内部引起的应力也越强,从而越有可能造成材料的破坏。     

光学材料中横向SBS的稳态分析

 从非线性光学的耦合波理论出发，建立了种子光入射的窄带泵浦的横向受激布里渊散射的二维理论模型，并对稳态情形进行了数值模拟，得到了散射光强的二维分布。计算表明，散射光场在入射面内呈现出“局部集中”的特点，而且由于“空间压缩”效应，使得获得的最大散射光强远大于初始泵浦光强。还分析了光场及材料参数对获得的散射光强的影响，得出：入射的激光功率密度越大，光学元件的横向尺寸越长，材料的吸收系数越小，受激散射产生的散射光和弹性声波强度就越大，在材料内部引起的应力也越强，从而越有可能造成材料的破坏。     

宽带KrF激光泵浦SBS的研究

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。     

宽带KrF激光泵浦SBS的研究

 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。     

基于SBS效应激光波长对光学材料损伤的影响

从耦合波理论出发,采用纵向受激布里渊散射(SBS)模型,通过时域有限差分法数值求解了瞬态SBS耦合波方程组,得到了泵浦光、Stokes光强度及声波产生应力随时间的分布;研究了在三种常见波长激光（基频、倍频和三倍频）作用下SBS效应的发展过程及其对光学材料损伤过程的影响。结果表明：种子光作用主要体现在SBS起振阶段,一旦进入稳态阶段,Stokes光强及应力发展的最大值、稳态值依赖于泵浦光的大小;在相同脉冲宽度下,激光波长越短,SBS发生越早,发展越快,更易造成光学元件的力学损伤;三倍频激光产生最大应力为基频光产生最大应力的100倍,且相比于倍频激光,产生最大应力的时刻要提前15 ns。     

基于SBS效应激光波长对光学材料损伤的影响

从耦合波理论出发,采用纵向受激布里渊散射(SBS)模型,通过时域有限差分法数值求解了瞬态SBS耦合波方程组,得到了泵浦光、Stokes光强度及声波产生应力随时间的分布;研究了在三种常见波长激光(基频、倍频和三倍频)作用下SBS效应的发展过程及其对光学材料损伤过程的影响。结果表明:种子光作用主要体现在SBS起振阶段,一旦进入稳态阶段,Stokes光强及应力发展的最大值、稳态值依赖于泵浦光的大小;在相同脉冲宽度下,激光波长越短,SBS发生越早,发展越快,更易造成光学元件的力学损伤;三倍频激光产生最大应力为基频光产生最大应力的100倍,且相比于倍频激光,产生最大应力的时刻要提前15ns。     

在激光大气传输中利用SBS阈值效应实现小面积信标的研究

在理论上建立起将受激布里渊散射（SBS）与激光大气传输过程相结合的激光补偿传输的数学模型,并进行了数值模拟,提出并证明了利用SBS阈值效应可以将相位共轭光会聚到目标上一个小面积上,从而在目标上主动获得小面积信标光斑。利用SBS实现激光大气补偿传输（传输距离250m）的实验研究,证实了上述理论预期。     

基于受激布里渊散射的波长间隔可变多波长光纤激光器

提出了一个基于自激发受激布里渊散射的波长间隔可变多波长光纤激光器.利用单模光纤中自激发产生的非线性布里渊增益和掺铒光纤的线性增益组成混合增益光纤激光器,从而使光纤激光器在室温下产生稳定的多波长输出.改变双折射光纤环镜滤波器中保偏光纤的长度,可以实现波长间隔可变多波长激光产生,提高了多波长光纤激光器操作的灵活性和实用性.实验实现了波长间隔从0.8 nm至0.076 nm可变的多波长激光产生,波长数随波长间隔减小而增加,间隔为0.08 nm的激光波长数达86.     

受激布里渊散射相位共轭效应数值解

本文从联立麦克斯韦方程和介质的声振动方程出发，在缓变振幅近似及小信号近似下得到耦合波振幅方程，以丙酮（Ｃ＿３Ｈ＿６Ｏ）为ＳＢＳ介质，利用计算机进行了受激布里渊散射相位共轭效应数值求解，得到ＳＢＳ阈值、饱和效应及二维情况下的ＳＢＳ相位共轭效应。理论计算表明，在小信号情况下受激布里渊散射具有良好的相位共轭效果。     

若丹明6G共振增强苯(C6H6)的受激拉曼散射实验研究

报道了若丹明6G乙醇溶液中苯的受激拉曼散射Stokes波共振放大的实验研究.在特定的染料溶液浓度下,1阶、2阶Stokes波得到有效放大,放大倍数分别为3.81和6.1.对荧光共振放大SRS的物理机制进行了分析讨论.     

利用受激布里渊散射效应补偿激光大气传输过程中的畸变

提出了利用受激布里渊散射的阈值效应主动在非配合,扩展目标上实现小面积信标的方法,在不同的大气扰动条件（Cn^2=10^-16--10^-12)下,对激光的远距离（10km)补偿传输过程进行了模拟计算,获得了到达目标上的相位共轭光的光强分布。分别在不同的实验环境进行了激光补偿传输实验,其中激光补偿传输距离最远达到250m。实验结果证实了利用受激布里渊散射实现激光大气传输补偿的有效性,证明利用阈值效应在目标上主动获得小面积信标的方法是可行的。     

Giant gain enhancement in surface‐confined resonant Stimulated Brillouin Scattering

The notion that Stimulated Brillouin Scattering (SBS) is primarily defined by bulk material properties has been overturned by recent work on nanoscale waveguides. It is now understood that boundary forces of radiation pressure and electrostriction appearing in such highly confined waveguides can make a significant contribution to the Brillouin gain. Here, this concept is extended to show that gain enhancement does not require nanoscale or subwavelength features, but generally appears where optical and acoustic fields are simultaneously confined near a free surface or material interface. This situation routinely occurs in whispering gallery resonators (WGRs), making gain enhancements much more accessible than previously thought. To illustrate this concept, the first full‐vectorial analytic model for SBS in WGRs is developed, including optical boundary forces, and the SBS gain in common silica WGR geometries is computationally evaluated. These results predict that gains 10⁴ times greater than the predictions of scalar theory may appear in WGRs even in the 100 μm size range. Further, trapezoidal cross‐section microdisks can exhibit very large SBS gains approaching 10² m⁻¹W⁻¹. With resonant amplification included, extreme gains on the order of 10¹² m⁻¹W⁻¹ may be realized, which is 10⁸ times greater than the highest predicted gains in linear waveguide systems.

     

Beam Combination using Stimulated Brillouin Scattering for the Ultimate High Power-Energy Laser System Operating at High Repetition Rate over 10 Hz for Laser Fusion Driver

After the laser was invented in 1960, a phase conjugation mirror has been respected to be the most fantastic one for the laser resonator composition because it can compensate any distortions of the laser beams occurred by the many inhomogenuities of the laser media and optical components. Among the many phase conjugation configurations, the stimulated Brillouin scattering phase conjugation mirror is the most simple one and many researchers have tried to utilize it to develop high power/energy laser systems. For realizing a high energy/power laser system the thermal problem is the most difficult to solve, and some researchers suggested a beam combination technique to reduce the thermal load of the big laser media to many small sized ones. To accomplish the beam combination using stimulated Brillouin scattering phase conjugation mirrors (SBS-PCMs), it is necessary to lock/control the phases of the SBS-PCMs. And some researchers have developed several ways for it, but they can lock the phases of a limited number of beams overlapped at the foci less than 5, or lock the phases by back-seeding technique but it loses the phase conjugation characteristics. For realization of the laser fusion driver, it is necessary to combine more than 10 or 100 beams. And the authors have developed recently a new phase controlling/locking technique which is isolated and independent totally from other beams and it can be applied to an unlimited number of beams in principle.     

Dynamics of Stimulated Brillouin Scattering in a Short and High-Finesse Fiber Fabry-Perot Resonator

We theoretically investigate the dynamics of stimulated Brillouin scattering (SBS) in a short fiber Fabry-Perot resonator with reflection mirrors. The analysis is based on the coherent six-wave model including an optical Kerr effect and the linear cavity detunings for the pump and created Stokes waves are taken into account in the formulation. The instabilities including periodic, quasi-periodic and chaotic oscillations can occur owing to the Kerr effect even if the fiber resonator is so short as to ensure a single longitudinal-mode operation. The threshold power for SBS and the boundary power between the stable and unstable regions are numerically calculated as a function of the amplitude reflectance of mirrors for different cavity detunings. The dynamics of SBS and these two critical powers depend on the amplitude reflectance and the cavity detuning. Although an increase in the mirror reflectance decreases the threshold power for SBS, it may limit the utility of SBS since the stable region is narrow and the output power levels of the pump and Stokes waves are low.     

单模光纤受激布里渊散射阈值的研究

为了研究单模光纤对城域网和接入网以及FTTH的容量与性能的提升,使用大功率、窄线宽的高性能光纤激光器作为系统光源,分别测量了3种光纤到户用单模光纤的受激布里渊散射（SBS）阁值。从理论上分析了光纤SBS阂值估算公式及影响阂值的因素,理论估算值与实验测量值吻合很好。实验发现的一种G．652D光纤具有高达12mw的SBS阈值,对此进行了分析。     

Beam Recombination Characteristics in Array Laser Amplification Using Stimulated Brillouin Scattering Phase Conjugation

Beam recombination characteristics were numerically investigated in array laser amplification using stimulated Brillouin scattering phase conjugation. To clarify the effect of piston errors due to imperfect phase locking, spatial intensity profiles of the beam recombination output were calculated in both the near and the far field on the basis of Rayleigh-Sommerfeld diffraction theory. The analyses indicate that piston errors are seriously detrimental to the quality of a beam recombination output and should be eliminated by a proper phase locking. It is also found that the gap between the beam splitting-combining wedges has a negligible effect.Presented at 1996 International Workshop on Interferometry (IWI ‘96), August 27-29, Saitama, Japan.