激光束低频位相误差叠加规律研究

 用随机位相屏模拟光学元件产生的低频位相误差，并用RMS位相梯度对低频位相误差进行统计量化，通过对激光束传输过程进行模拟，对低频位相误差的叠加规律有了新发现，并对位相误差叠加规律进行了修改，为位相校正提供了理论上的依据；通过对光束聚焦过程进行研究，得到了低频位相误差影响光束焦斑尺寸的初步规律；并在此基础上提出了一种光束质量控制的新方法。     

低频位相误差新校正方法模拟研究

 就多程放大系统中产生的低频位相噪声，提出用位相补偿反射镜来进行补偿的静态校正方法。用随机位相屏模拟光学元件产生的低频位相噪声，建立光传输模拟模型，引入等效位相片的概念，将数个光学元件对位相的影响简化为等效位相片，在此基础上对位相补偿反射镜的校正原理进行阐述。进而对双程光路校正过程进行了模拟研究，得到了很好的校正效果。     

带受激布里渊散射池的位相共轭激光器输出的空间特性

本文应用传输矩阵的方法对受激布里渊散射位相共轭腔输出的空间特性进行了分析及编程计算，给出了各种参数下受激布里渊散射－位相共轭腔的传输光束轮廓图，同时给出了实验结果与之相比较，提出了设计受激布里渊散射共轭腔时应注意的问题及几种实用的受激布里渊散射位相共轭腔的腔型。     

激光束低频畸变波前模型的计算模拟

在分析强激光束低频位相噪声特点的基础上 ,采用位相均方根梯度表征激光束的低频位相噪声并结合随机位相屏构建相应的畸变波前模型。通过模拟计算 ,给出低频位相噪声的均方根梯度与聚焦光斑尺寸的初步规律。     

激光束低频畸变波前模型的计算模拟

 在分析强激光束低频位相噪声特点的基础上,采用位相均方根梯度表征激光束的低频位相噪声并结合随机位相屏构建相应的畸变波前模型。通过模拟计算,给出低频位相噪声的均方根梯度与聚焦光斑尺寸的初步规律。     

位相畸变对强紫外激光在空气中长程传输的影响

 采用瞬态受激旋转拉曼散射（SRRS）模型,详细考虑了激光脉冲的位相变化、时间波形、泵浦光的衰减、斯托克斯光的非线性放大以及初始的随机斯托克斯散射场等诸多因素,研究了空间位相畸变对空气中长程传输过程中产生的SRRS效应的影响。研究结果表明：位相畸变对阈值条件和时间特性影响较小,而对光束质量影响较为明显;随着位相畸变的增大,光束的能量分布变得极不均匀,光束的光强对比度也明显变大,从而使激光光束质量变差,而且当传输距离达到阈值条件后,随着传输距离的增加,光束质量将进一步变差。     

位相畸变激光束的谐波转换

首次在理论上研究了位相畸变激光束的谐波转换，从波动方程出发，应用空间频谱方法处理位相畸变光束的非线性耦合问题，建立了适用于位相畸变且空间光强不均匀光束的谐波转换的理论模型。     

位相可控液晶空间光调制器的研究

论述了平行排列液晶的位相调制理论，进行了理论结果的计算模拟．研制出平行取向TFT型液晶空间光调制器并分析了其位相调制特性.结果表明,此平行取向的液晶空间光调制器可用于位相调制，其调整量优于0.7 μm，最小调整步长是0.052 μm．在ZYGO干涉仪上进行的位相控制实验，得到了很好的实验结果．     

离轴位相奇点的动态传输

推导出高斯背景的离轴位相奇点光束的半屏衍射解析公式,详细研究了离轴位相奇点的动态传输.结果表明,半屏衍射,偏移量和传输距离都会影响位相奇点的传输行为和衍射场位相奇点的分布.改变偏移量和传输距离,衍射场伴随有位相奇点的产生,移动和湮没. 关键词： 奇点光学 离轴位相奇点光束 半屏衍射 光涡漩     

自锁定半导体激光器中强度压缩及位相噪声的减小

采用外部F-P腔自锁定单模量子阱半导体激光器，观察到强度噪声的压缩现象，并同时大幅度降低了位相起伏.在35MHz附近观察到19.3%的强度压缩，对应激光输出的压缩度为37.8%，在9kHz-100MHz范围内观察到约3个数量级的位相噪声降低.获得了近最小测不准态. 关键词：     

光束畸变对连续相位板性能的影响

研究了光线追迹和随机相位滤波作为初始相位设计的连续相位板下,光束畸变对连续相位板整形性能的影响。结果表明:随机相位滤波得到的连续相位板相比光线追迹获得的连续相位板,在幅度畸变、离焦的容忍度等方面都有优越性;进一步分析了相位畸变、对准误差、口径误差等对连续相位板性能的影响,确定了相位畸变是影响性能的首要因素,并且大目标焦斑的畸变宽容度更大,由此引入了波前的相对畸变因子,在所定义的连续相位板性能标准下,波前容忍度为0.5。     

随机高斯型相位板的束匀滑特性

 针对激光系统对光束匀滑的需求,设计了高斯型连续相位板,并对其远场特性进行了研究。分别计算了相干长度为39,30,10和3 mm的高斯相位板远场光斑分布,结果显示相位板自身相关长度是决定远场能量分布的重要因素,当相干长度大于10 mm时,由于不满足各态历经条件,远场光斑分布能量分散。当相干长度小于10 mm后,由于满足各态历经条件,远场光斑能量将接近理想的高斯分布特性。通过数值计算模拟了相干长度为3 mm的连续相位板对畸变光束进行匀滑处理的过程,演示了束匀滑处理结果。通过比较匀滑前后远场光斑的能量分布,显示了畸变光束通过连续相位板后远场光斑能量分布变化情况,通过相位板后,光斑形状明显接近理想高斯分布情况。     

A modified phase diversity diffraction wavefront sensor with a grating

The phase diversity wavefront sensor is one of the tools used to estimate wavefront aberration, and it is often used as a wavefront sensor in adaptive optics systems. However, the performance of the traditional phase diversity wavefront sensor is limited by the accuracy and dynamic ranges of the intensity distribution at the focus and defocus positions of the CCD camera. In this paper, a modified phase diversity wavefront sensor based on a diffraction grating is proposed to improve the ability to measure the wavefront aberration with larger amplitude and higher spatial frequency. The basic principle and the optics construction of the proposed method are also described in detail. The noise propagation property of the proposed method is also analysed by using the numerical simulation method, and comparison between the diffraction grating phase diversity wavefront sensor and the traditional phase diversity wavefront sensor is also made. The simulation results show that the diffraction grating phase diversity wavefront sensor can obviously improve the ability to measure the wavefront aberration, especially the wavefront aberration with larger amplitude and higher spatial frequency.     

自由热射流流场的光学不均匀性数值研究

 通过建立物理模型，求解层流N-S方程，用数值方法模拟了二维热射流流场的有序大涡结构，计算了流场不同流向位置的光程值，分析了射流流场混合层的光学特性，得出了气动光学流场由于流场中大尺度涡结构的存在所引起的光学不均匀性，大涡结构中奇点所导致的光学畸变最大，在一定条件下大涡结构有散焦作用。     

A modified phase diversity wavefront sensor with a diffraction grating

Phase diversity wavefront sensor is one of the useful tools to estimate the wavefront aberration, and it is often used as a wavefront sensor in adaptive optics system. However, the performance of the traditional phase diversity wavefront sensor is limited by the accuracy and dynamic ranges of the intensity distribution at focus and defocus positions of the CCD camera. In this paper, a modified phase diversity wavefront sensor based on a diffraction grating is proposed to improve the ability to measure the wavefront aberration with larger amplitude and higher spatial frequency. The basic principle and the optics construction of the proposed method are also described in detail. The noise propagation property of the proposed method is also analysed by using the numerical simulation method, and comparison between the diffraction grating phase diversity wavefront sensor and the traditional phase diversity wavefront sensor is also made. The simulation results show that the diffraction grating phase diversity wavefront sensor can obviously improve the ability to measure the wavefront aberration, especially the wavefront aberration with larger amplitude and higher spatial frequency.     

双锥光纤滤波器的研制

实验研究了熔锥条件对双锥光纤滤波器的影响。提出一个高斯模型，预测锥的几何形状。获得了窄带带通双锥光纤滤波器以及带阻中心波长分别为１３５ｎｍ和１５５９ｎｍ的带阻双锥光纤滤波器。     

Influence of the abdominal wall on the nonlinear propagation of focused therapeutic ultrasound

This article theoretically studies the influence of inhomogeneous abdominal walls on focused therapeutic ultrasound based on the phase screen model. An inhomogeneous tissue is considered as a combination of a homogeneous medium and a phase aberration screen. Variations of acoustic parameters such as peak positive pressure, peak negative pressure, and acoustic intensity are discussed with respect to the phase screen statistics of human abdominal walls. Results indicate that the abdominal wall can result in energy loss of the sound in the focal plane. For a typical human abdominal wall with correlation length of 7.9~mm and variance of 0.36, the peak acoustic intensity radiated from a 1~MHz transmitter with a radius of 30~mm can be reduced by about 14% at the focal plane.     

Nonresonant third harmonic generation in thallium vapour

Feasibility of nonresonant third harmonic generation in thallium is investigated. The third order susceptibility, for driving frequencies in the visible region, is calculated and the phase matching with Ar as buffer gas is investigated. Other related quantities like coherence length, minimum pulse lengths required to get phase matching and power input requirements to achieve 50% conversion are also calculated.