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用全饱和激光模型对既含有加性又含有倍增噪声的激光场进行理论分析,求出了强度相关时间Tc的数值解和有效本征值λeff的解析解。与实验测量相比较表明,全饱和激光模型与实验吻合得最好,而三次激光模型的偏差较大。 相似文献
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定态双向环形气体激光中的饱和效应 总被引:1,自引:1,他引:0
从理论上分析了双向环形气体激光中的全饱和效应,导出了定态激光强度分布函数的解析形式,算出了定态双模强度的自相关和相相关函数。与激光的三次模型 实验测相比较,激光的全饱和模型与实验测量符合更,而三次模型的结果偏差较大。 相似文献
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研究了单模激光中的倍增噪声和饱和效应,导出了定态激光强度的平均值和归一化方差.同实验值相比较,理论与实验在阈值附近符合得很好.而在远高于阈值时,含有饱和效应的激光模型能更好地描述实际应用中的激光. 相似文献
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用含有背散射和饱和效应的双模激光场的理论模型讨论了背散射和外加注入信号对环形激光场的统计性质的影响。结果表明,背散射可以抑制系统的涨落。对于均匀展宽的双向环形激光场,注入信号可以将其中的弱模光场由非相干光驱动成为相干光,而对于非均匀展宽的环形激光场则没有这种驱动效应。进一步研究发现,这种驱动效应与注入信号的强弱及两模式光场的抽运参量差异△α有关。 相似文献
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开展了多波段激光(750~970 nm)对彩色CCD成像系统的外场干扰实验,测得了不同辐照条件下对外场1.3 km处彩色CCD成像系统的干扰效果;建立了彩色CCD相机的激光干扰模型,对实验结果进行了理论验证与分析。理论与实验结果表明:强激光对彩色CCD成像系统的干扰效果明显,CCD靶面出现了明显的光饱和和串扰现象,光饱和区域的形成是由激光束进入光学系统后发生衍射效应造成的;到靶激光功率密度越强,CCD靶面光饱和面积越大,激光干扰效果越好;单波段750 nm激光作用下,到靶功率密度为4.2 kW/cm2,CCD靶面的光饱和面积为0.88 mm×0.97 mm;多波段激光(750~970 nm)作用下,到靶功率密度为20.7 kW/cm2,CCD靶面发生全靶面饱和现象;仿真结果与实验结果基本一致,证明了理论模型的正确性。对远场干扰能力计算结果表明:随着干扰距离的增加,到靶功率密度减小,激光干扰效果变差。 相似文献
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LENGFeng ZHUShi-Qun 《理论物理通讯》2001,35(1):87-92
The Statistical Properties of a homogeneously broadened ring laser with an injected signal are investigated and the normalized two-mode intensity auto-and cross-correlation functions are calculated by a full saturation laser theory with backscattering.The theoretical predictions are in good agreement with the experimental measurements.Further inverstigation reveals that the backscattering can reduce the fluctuations in the system while the full saturation effect plays a major role when the laser is operated above threshold.It is also quite important to notice that the injected signal can drive the weak mode from incoherent light to coherent light. 相似文献
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采用与信标发射接收系统参数匹配的长脉冲光源,可在脉冲回光时间内产生较亮星等的钠信标,既有利于提高信标探测的信噪比,也有利于实现自适应光学系统的高频闭环校正.基于450 mm直径望远镜和大能量长脉冲光源,开展了钠信标探测实验,得到了长脉冲光源产生的钠信标回光特性.通过CCD和光电倍增管,采集得到了不同发射能量、出射偏振态下的回光强度,并获得了最大强度为15万光子/m2/pulse的回光,对应脉冲回光时间内约4.1等星的亮度.分析推算了实验条件下钠原子的柱密度.实验全过程未出现明显的饱和现象,验证了采用长脉冲钠信标光源避免饱和效应、得到高亮度钠信标的可行性. 相似文献
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The dynamical properties of two-mode ring laser with different values of mode coupling constants are investigated by the full saturation laser theory with an injected signal. By a one-dimensional approximation, the intensity correlation time Tc and effective eigenvalue λeff11 are calculated. The effects of backscattering and injected signal are discussed. 相似文献
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We report the experimental study of the enhanced backscattering from a random rough surface through a laser dye-doped polymer. The sample is a slice of pyrromethene-doped polymer coupled with a two-dimensional rough gold layer with a large slope. When the sample is illuminated with an s-polarized He-Ne laser and pumped by a cw argon-ion laser, amplified backscattering is observed. The enhanced backscattering peak increases sharply and its width narrows for a sample with low dielectric constant |?(2)|. 相似文献
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The effect of backscattering on the behavior of a dye ring laser is investigated by photoelectric counting measurements. It is found that there exist two laser regimes, a low backscattering regime in which the laser exhibits meta-bistability and random mode switching, and a high backscattering regime in which switching is suppressed. In the latter case the photon statistics are similar to those of a single-mode standing wave dye laser. 相似文献
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R. Serna C. N. Afonso F. Catalina N. Teixeira M. F. da Silva J. C. Soares 《Applied Physics A: Materials Science & Processing》1992,54(6):538-542
Thin films consisting of 3 or 4 Sb and Ge alternating layers are irradiated with single nanosecond laser pulses (12 ns, 193 nm). Real time reflectivity (RTR) measurements are performed during irradiation, and Rutherford backscattering spectrometry (RBS) is used to obtain the concentration depth profiles before and after irradiation. Interdiffusion of the elements takes place at the layer interfaces within the liquid phase. The reflectivity transients allow to determine the laser energy thresholds both to induce and to saturate the process being both thresholds dependent on the multilayer configuration. It is found that the energy threshold to initiate the process is lower when Sb is at the surface while the saturation is reached at lower energy densities in those configurations with thinner layers. 相似文献
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在单模光纤中放大的反斯托克斯拉曼背向自发散射的温度效应 总被引:8,自引:0,他引:8
在单模光纤中,输入的激光功率大于阈值时.出现放大的反斯托克斯拉曼背向自发散射现象。实验发现:放大的反斯托克斯拉曼背向自发散射具有温度效应.与反斯托克斯拉曼背向自发散射一样,放大的拉曼散射光的光子通量受到光纤温度的调制。反斯托克斯拉曼背向白发散射的放大效应抑制了单模光纤中的相干噪声,改善了系统的信噪比。实验还发现.放大的反斯托克斯扎曼背向自发散射空域曲线上放大的端点位置随激发功率的增高前移并具有一定的规律性。放大的反斯托克斯拉曼背向自发散射的温度效应作为一种新的测温原理,已应用于远程30km分布光纤温度传感器系统。 相似文献
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针对水下激光探测系统的水体后向散射光的计算,给出了系统的光学几何结构,分析了不同距离处的激光光斑与接收视场区域的位置变化关系并进行了定量计算。依据光传输理论建立了水体后向散射光的计算模型,根据模型的算法步骤编写了计算机程序。结合水下激光探测系统的具体参数进行了实例计算,绘制了后向散射光信号波形,并与试验获取的信号波形对比分析,验证了算法的可行性和正确性。研究了使用实测后向散射光信号数据估计水体光学特性参数的方法,通过估算的参数重新绘制曲线并反向叠加在测量数据曲线上以抵消水体后向散射光对目标信号的影响从而能够提取目标信息。 相似文献
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Results of long-term continuous measurements of the atmospheric backscattering amplification coefficient on a 2-km-long near-ground path with the use of a two-channel micropulse lidar based on a waveguide laser are presented. It is shown that the backscattering amplification coefficient has a pronounced daily variation. In the night and in the afternoon, atmospheric backscattering amplification is maximal and the amplification coefficient can exceed 2. The amplification is low or absent in morning and evening hours at neutral temperature stratification in the near-ground layer of the atmosphere. The backscattering amplification coefficient increases with an increase in the structure constant of the air refracting index and variance of the image jitter of the illumination spot created by the probing laser beam on the wall of a 2-km-distant building. 相似文献
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为探索舰船尾流后向光学检测方法,研究了尾流气泡对水中激光脉冲后向散射特性的影响。首先基于Fournier Forand 体积散射函数,利用蒙特卡罗(Monte-Carlo)方法理论分析了近距离尾流气泡对激光脉冲后向散射特性的影响。然后,采用蓝绿激光脉冲作为光源,实验研究了模拟尾流气泡对激光脉冲后向散射信号的影响。研究表明,尾流气泡的存在会使得激光脉冲后向散射信号前沿位置在时域左移,后沿位置在时域右移,信号时域宽度增加,能量增强,峰值增大且位置在时域左移。最后根据研究结果提出了一种基于激光脉冲后向散射信号特征变化的舰船尾流气泡后向检测方法。 相似文献