物理光学 其他

TN652006010060声光效应实验研究=Experi mental investigation of acous-tooptic effect[刊,中]/李明(淮海工学院教务处.江苏,连云港(222005)),李冠成∥应用光学.—2005,26(6).—23-27介绍声光效应的最新理论进展。采用光栅假设,对各向同性介质中的声光效应作了简要讨论,导出了第m级衍射光的衍射效率公式。研究和介绍一种新的声光效应实验装置。在实验中,应用线阵CCD光强分布测量仪等,通过改变超声波的频率和功率,分别实现了对激光束方向的控制和强度的调制;定量给出了声光偏转量的关系曲线和声光调制测量的关系曲线。实验表明,在布喇格…     

布拉格衍射下半导体激光光强分布实验探讨

通过控制变量法,探究了声光效应中布拉格衍射下不同超声波频率、功率以及是否载入调制信息下衍射光斑的光强横向分布。并用MATLAB软件拟合了 0级和-1级衍射光的光强分布图,将实验结果与理论解释进行对比分析。     

相位、振幅调制两用声光调制器设计

针对实际应用中大多的光调制器只能实现单参数调制的情况,提出一种既可以调相又可以调幅的声光调制器的设计方案.运用矩阵级数解法求解正常声光相互作用Raman-Nath方程,通过计算机编程进行数值求解,得到衍射光的衍射光强和附加位相变化,从而指出以往解法的一些不合理性,并找到声波功率和衍射光的光强和位相的关系,为声光效应的位相调制和振幅调制设计提供了一种可行的方法.结合调制声波频率,可在同一个调制器上进行调幅、调相、调偏转方向.     

声光技术的进展

一、声光效应和声光器件 当声波在介质中传播时,由于物质的光弹效应,使介质的折射率发生周期性变化,从而也像相位光栅那样使光衍射.当超声波频率较低,声光互作用区较短时,入射光常被衍射成多级衍射光,这就是喇曼-奈斯衍射.如果超声波频率很高,光沿着适当的角度射入介质并通过较多的超声波阵面,则高次衍射光消失,只剩下0级和1级光,这就是布喇格衍射,这时入射光与衍射光的角度应满足布喇格方程即     

利用声光效应实现信息传输及再读取

利用声光效应通过调制激光传输声音信号,使用调幅电路将声音的电信号加载在高频信号上,信号驱动超声波换能器振动,超声波作用在激光入射的声光介质中产生声光效应使激光产生相应的衍射,衍射光斑光强随声音信号同步变化,光电探测器通过探测衍射光强产生相应电压,对输出电压信号的处理后就可以还原声音信号.     

声光器件特性分析及音频声光通信研究

分析了声光效应的基本原理及布拉格效应成立的条件,构建了声光器件特性测试实验装置。对声光器件中布拉格衍射的建立、声光调制的幅度特性及频率特性等基本特性进行了测量分析,对声光模拟信号传输的线性特性和音频频响关系进行了研究。     

声光衍射法测量液体中超声声强的数据处理方法

为将半导体激光器用于构建声光效应及声速声强测量教学实验装置,推导了超声光栅远场衍射光场分布,给出了超声光栅相位调制系数分别与声强和各级衍射光强度的关系,总结了从衍射光场图像提取声强值的数据处理方法.通过建立交替使用氦氖激光器或半导体激光器的实验系统,进行了液体中超声声强测量的比较实验,验证了半导体激光器作为光源实现声光衍射法超声声强测量的可行性.     

超声光栅实验中声致折射率变化的研究

为了研究声光效应中声致折射率变化情况,以超声光栅实验为基础,用CCD结合光强分析软件,分析了衍射光的强度分布;通过数值计算衍射光相对强度,比较得到了在超声场频率为10.27 MHz时,介质中的声光相位延迟Δ=1.2855 rad,声致折射率变化量Δn=3.014×10-6;进而讨论了电声换能器的机电耦合效率与超声频率的关系,给出当超声频率为10.33 MHz时,耦合效率最高,介质中折射率变化量最大;结果表明,在超声光栅实验中,引入这些测量内容,不仅能丰富实验内容,更能加深学生理解声光效应,扩展学生的知识面.     

光拍法测光速实验中的声光效应研究

对光拍法光速测量仪进行了简单的改造,研究了光拍法测光速实验中的声光效应.实验简单易行,声光效应产生的频移直观可见,并可得到频移量与超声波频率的关系.在光拍法测光速教学实验中增加对声光效应的研究有利于更好地理解声光效应及其在光拍法测光速中的应用.     

声光器件及其应用

声光器件,即用声光效应制做的元器件。它通过在介质内传播的超声波和光波之间的相互作用,达到控制光束的目的。声光器件所产生的频移和偏转角都很小,所以对非相干光没有什么实用价值。由于激光束的单色性好,方向性好,亮度高,并且整个激光束能量可以全部聚焦在衍射限大小的光斑内,所以通过声光器件可以对它的频率,方向和强度进行快速而有效的控制。声光器件的种类繁多,应用面很广。本文重点论述声光偏转和声光调制器的基本结构、工作原理、基本的设计特点、工作方式等,并侧重介绍了对激光束控制方面的应用。     

用He-Ne激光声光器件进行声光幅度调制和声光偏转实验

描述了用He－Ne激光声的声光器件进行的声光调制和声光偏转实验。调制曲线上有一个拐点，在拐点附近的一段曲线可看成直线，利用这段曲线进行调制可减少失真。     

双锥光纤中声光效应的理论分析

利用耦合模理论分析了在双锥光纤耦合区中声光的相互作用,讨论了在不同耦合区半径下扰动周期与声波频率的关系。计算了在双锥光纤中声光谐振耦合的波谱特性和模式转换效率、带宽与调制周期和耦合区长度的关系。介绍了声光的可调谐性。基于此效应可制作全光纤可变衰减器和可调滤波器。     

集成光学声光可调谐光谱仪的特性分析

提出了一种以集成光学声光可调谐滤波器作为分光元件的新型光谱仪 ,并详细介绍了这种光谱仪的具体特性。通过对这种光谱仪的特征方程、点扩展函数以及色散本领的详细分析 ,指出该光谱仪的分辨本领与器件的声光作用长度成正比 ,也与它的级联级数的平方根成正比。因此增加器件的声光作用长度比增加它的级联级数能更有效地提高光谱分辨率。另外还指出 ,准共线声光耦合是抑制侧瓣、提高分辨本领的有效途径。测试表明 ,当声光相互作用长度L =2 5mm ,声波导和光波导的夹角θ=0 .4 2°时 ,在中心频率 174MHz附近可获得带宽 1.4 4nm ,一级侧瓣 - 13.2dB ,模式转换效率大于 99%的结果。     

利用TeO2减少多模光纤出射场散斑干扰的研究

 为了减少多模光纤出射光场的散斑干扰,提出了把声光布拉格衍射效应所形成的不同衍射级耦合到多模光纤中,由于衍射级具有不同的偏振态,消弱了光场相干条件,进而在出射光场中消弱了散斑场的对比度,并通过对改变声场频率后得到的散斑场对比度的分析,证实了利用各向异性晶体TeO2能够控制散斑场对比度,改善出射场的高斯分布,得出了可以利用布拉格衍射效应减少散斑场干扰的可能性。     

Dynamic optical transfer function of an acoustooptic modulator with a damped sound wave

Based on a spatially dependent dynamic optical transfer function of an acoustooptic modulator, a dynamic model of light modulation by a sound signal under conditions of acoustic damping is developed. A system of equations describing the dynamics of the acoustooptic interaction is given. Solutions of this equation for arbitrary power level and spatial-time structure of a sound signal are found. It is shown that acoustooptic damping has the strongest effect in a nonlinear modulation regime. Here, the dissipation of an acoustic signal suppresses the higher harmonic of the dynamic optical transfer function. An analytical model of the dynamic optical transfer function for a low level of acoustooptic coupling is given. It is shown that when the pump beam aperture is much greater than the spatial size of an acoustic signal, the time response of the acoustooptic modulator response is identical within a phase factor to the amplitude profile of a pump beam apodized by the exponential dependence of the amplitude of a damped sound wave. Otherwise, the sound damping produces almost no distortions of a plane top of the acoustooptic modulator response to a pulsed signal and shows itself only under phase mismatch conditions. Here, the asymmetry of overshoots at the edges of the acoustooptic modulator response is observed. Calculated plots are presented, which illustrate the aforementioned specific features of the transient process under conditions of acoustic damping in the acoustooptic interaction in paratellurite.     

Effect of the spatial structure of an acoustic field on Bragg’s acoustooptic diffraction under strong acoustic anisotropy conditions

Bragg’s acoustooptic diffraction in an acoustically anisotropic medium is considered taking into account the two-dimensional spatial diffraction structure of the acoustic beam. The conditions are determined under which reverse transfer of optical power from the diffracted to the transmitted beam in the regime of 100% efficiency of diffraction is considerably suppressed. It is shown that this effect is due to diffraction bending of wave fronts of the acoustic beam in the acoustooptic diffraction plane. The problem of optimization of the piezoelectric transducer size and the spatial position of the input light beam is solved using the criterion of the minimal required power of the acoustic field. The results of simulation in a wide range of the acoustooptic interaction parameters for a Gaussian light beam are reported. The correctness of the model is confirmed experimentally. Recommendations for designers of acoustooptic devices are formulated.     

集成光学声光可调谐波长滤波器的研制

阐述了中心波长为１．５２３μｍ的集成光学声光可调谐波长滤波器的各项理论参数、制作工艺以及性能测试。在有效声光相互作用长度１６ｍｍ、射频驱动功率３５ｍＷ时,获得了模式转换效率大于９９％、插入损耗小于－４．ｄＢ、带宽１．６ｎｍ、３ｄＢ调谐范围为１４０ｎｍ的实验结果。     

声光调制实验的一种CCD成像改进方法

提出了声光调制实验的一种CCD成像改进的实验方法,即声光调制的入射光和衍射光成像于CCD上,对光斑图像进行编程处理,计算机给出光斑的位置。给出了实验步骤、图像处理算法和实验结果。     

Modulated angle beam ultrasonic spectroscopy for evaluation of imperfect interfaces and adhesive bonds

An experimental method incorporating high frequency pulsed angle beam ultrasonic measurements modulated by low frequency vibrations of a bonded structure is described. This method uses parametric/nonlinear mixing between high and low frequencies to characterize adhesive degradation. It is demonstrated that good quality (undamaged) bonds exhibit little dependence of ultrasonic signature on the overlay of low frequency vibration loads; however, environmentally degraded or imperfect bonds exhibit strong modulation of the resonance frequency of the ultrasonic signal reflected from the bond. The results are interpreted using a model for normal and oblique wave interaction with two nonlinear interfaces separated by an adhesive layer under quasi-static stress modulation.     

The temperature dependence of intensity and the function of the transition dipole moment for the induced optical absorption bands of oxygen in the region of the Herzberg photodissociation continuum (200–230 nm)

Application of coherent interaction of laser light with a focused ultrasonic wave to the technique of acoustooptic visualization in multiple-scattering media is discussed. By analyzing spatial distribution of the optical radiation modulated by ultrasound (the photocurrent at ultrasonic frequency), images of large-sized inhomogeneities embedded into the scattering medium have been obtained. A light-absorbing half-plane and a square with sides of 5 mm were used as the inhomogeneities. The visualization was performed under optimal conditions for measuring the alternating photocurrent calculated for the proposed model of coherent interaction between the laser and acoustic beams (the Raman-Nath diffraction). The alternating current at the ultrasonic frequency was obtained as a result of mixing the waves of the diffraction fields on the detector’s photocathode. All experimental values were obtained from a single measurement without averaging the alternating photocurrent at the ultrasonic frequency of 3 MHz, with the scattering parameter varying up to μL≤37.5, where μ is the extinction coefficient and L is the thickness of the scattering medium along the laser beam axis. The measured quantities varied in the course of the measurements by more than 10 orders of magnitude.