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1.
反常氧化碲声光偏转器控制理论研究   总被引:1,自引:0,他引:1  
厉国华  金韬 《光子学报》2009,38(5):1141-1144
根据晶体的声光特性以及反常布喇格衍射的Dixon方程,得出了氧化碲声光偏转器在反常布拉格衍射条件下的参量矢量关系.分析了超声波方向、入射光角度、衍射光角度与声波频率之间的关系.针对卫星光通信中衍射角固定的应用情况,通过数值求解和参量拟合,建立了一个基于平面方程的简单控制模型.利用该模型可以很快得到超声控制频率,使衍射角固定不变.  相似文献   

2.
反常氧化碲声光偏转器控制理论研究   总被引:1,自引:1,他引:0  
根据晶体的声光特性以及反常布喇格衍射的Dixon方程,得出了氧化碲声光偏转器在反常布拉格衍射条件下的参量矢量关系.分析了超声波方向、入射光角度、衍射光角度与声波频率之间的关系.针对卫星光通信中衍射角固定的应用情况,通过数值求解和参量拟合,建立了一个基于平面方程的简单控制模型.利用该模型可以很快得到超声控制频率,使衍射角固定不变.  相似文献   

3.
声光偏转效应可用于信号载频相关信息的测量。但当多个射频信号同时加载到声光偏转器时,在布拉格条件下信号间将发生互调现象,给信号检测带来很大的困难,尤其是三阶互调光束的干扰尤为严重。针对这种声光衍射产生的互调干扰,从声光衍射互作用原理出发,讨论了产生互调现象的条件、衍射分布和信号频谱图。通过理论分析,提出了减小互调现象的方法和措施。构建测试系统平台,对多路信号同时到达声光偏转器时产生互调干扰的程度进行了实验验证。在声光偏转器有效带宽内,衍射效率一定的情况下,通过适当控制射频驱动功率,保证声光偏转器工作在线性区域,可有效地减小互调干扰,从而有利于系统的信号检测。  相似文献   

4.
定义了压电晶体的增劲声光系数,它反映压电晶体中声光、电光和压电效应共同作用的结果。从参量互作用基本理论出发,同时考虑声光效应、电光效应和压电效应三个因素,用一个压电增劲声光系数来表示三种因素的共同作用,导出表面波声光布拉格互作用的耦合波方程。并求解得出相应衍射效率的计算公式。该式说明在弱声光互作用条件下,衍射导光波强度与超声功率成正比。表面波声光器件具有体积小、工作稳定、能耗小、易于集成等优点。可以用作光偏转器、光调制器、滤光器。在光通信以及各类实时信号处理,如相关、卷积、频谱分析、矩阵光计算等领域具有广泛的应用前景。  相似文献   

5.
多频声光互作用的研究   总被引:1,自引:1,他引:0  
赵启大 《光学学报》1989,9(2):28-134
本文推导出包括正常和反常声光互作用在内的多频声光耦合波方程的普适形式,并得出两个独立超声波信号时布拉格状态下方程的解.分析了多频声光互作用的各种线性和非线性效应,包括衍射效率、压缩、交叉调制和各级互调制强度等,并指出反常与正常多频声光衍射的差异.结论是反常多频声光互作用情况下,各级互调制模强度与主衍射模强度的比值小于正常多频声光互作用情况下的相应比值.实验结果与理论分析相符.  相似文献   

6.
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  相似文献   

7.
相位、振幅调制两用声光调制器设计   总被引:6,自引:3,他引:3  
陈海波  陈芳  佘卫龙 《光子学报》2003,32(2):166-169
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.  相似文献   

8.
反常声电光偏转器   总被引:7,自引:1,他引:6       下载免费PDF全文
本文介绍的新型声光偏转器可提高传统光偏转器的带宽,制作了一个LN反常声电光偏转器,中心频率为60MHz测试结果表明,带宽由原来的26MHz提高到37MHz。  相似文献   

9.
声光可调谐滤光器的等值点理论   总被引:2,自引:0,他引:2  
系统地给出了满足平行切线动量匹配条件下的声光相互作用关系曲线 ,发现仅当光的入射方向与晶体光轴间的夹角约为 5 6°时 ,在可见至近红外光谱范围内 ,同一声波矢量可使o光入射e光衍射和e光入射o光衍射同时满足平行切线动量匹配条件 ,并且这两束衍射光的波长相等。称这一特殊的角度为声光可调谐滤光器理论设计的等值点 ,并通过实验验证了这一分析结果的正确性。应用等值点原理设计声光可调谐滤光器 ,在不降低波长分辨率的前提下可大幅度提高光谱测量的信噪比  相似文献   

10.
多重散射理论声光耦合波方程的龙格-库塔法数值分析   总被引:2,自引:1,他引:1  
朱京平  李阳  唐锐歆  侯洵 《光子学报》2005,34(2):284-287
提出利用直观、方便且具有普遍性的4阶龙格-库塔(R-K)方法求解基于多重散射理论推导出的声光耦合波方程, 模拟计算布喇格衍射下衍射效率随各关键参数的变化关系, 分析入射光偏离Bragg角对Bragg衍射光效率的影响程度, 以及最佳Bragg衍射效率所需参数的选取问题. 模拟结果表明:Q(Klein-Cook参数)=4π时Bragg衍射效率可达97%, 证实了特征长度作为选取声光互作用长度的合理性.  相似文献   

11.
The two main constrains on the characteristics of the acousto-optic deflector are the acoustic sound attenuation and velocity. These two parameters will determine the resolution and the radio frequency bandwidth.Due to a double degenerated phase matching condition on a specific acousto-optic deflector configuration, the possibility of an improvement on the resolution of the acousto optic deflector becomes evident. This degenerescence is the result of the action of a D.C. electric field by the electro-optic effect. This configuration presents several advantages upon the early related works based on optical activity of selected materials and enables a wideband interaction in such a way that the number of resolvable channels is kept high. This has implications on the acousto-optic spectrometers for wideband radio astronomy research.  相似文献   

12.
廖欣  何宁  陈明  陈名松 《光学学报》2008,28(s2):278-282
为使现代电子侦察技术能适应信号密集、宽频谱、大动态的电磁环境, 提出了一种基于声光偏转器实现相关光信号处理的方法, 分析了射频信号频率变化与布拉格衍射角的关系, 讨论了声光偏转效应对信号频率的空间滤波特性; 在理论分析的基础上, 构建了在可见光范围内实现声光偏转的相干光信号探测的实验系统, 并通过计算机仿真对比, 验证了这种方法的可行性。实验表明, 采用波长为630 nm的单频激光, 带宽为200 MHz的声光偏转器, 其频率分辨率优于1 MHz, 频率信号的空间分离效果明显, 接收灵敏度和信噪比得到改善。  相似文献   

13.
A new acousto-optic deflector with a wide angular scanning range and a high diffraction efficiency has been studied. The device uses an additional deflector, which allows the angle of incidence of the input beam to be adjusted in order to fulfill the Bragg phase–matching condition over the entire scanning range of the main deflector. The characteristics of an anisotropic two-crystal deflector based on paratellurite crystals have been measured. It has been established experimentally that the operating bandwidth of the device is 32 MHz for a diffraction coefficient no less than 90%, which determines a light beam scanning angle of 50 mrad.  相似文献   

14.
在飞秒激光随机扫描双光子显微成像系统中使用宽带二维声光偏转器扫描飞秒激光,可以增大扫描角度至74 mrad,增大双光子显微成像范围。但宽带二维声光偏转器在大角度扫描时引入的色散较大,造成成像范围边缘的光斑严重畸变,边缘光斑直径达2.3 μm,影响边缘视场的成像质量。为了提高成像质量,设计了一种新的色散补偿方法,基于衍射透镜组成的开普勒望远系统,可以同时补偿不同扫描角度的不同色散。经过色散补偿后成像边缘的光斑直径小于1 μm,使系统获得大范围扫描成像的同时,所有扫描角度的色散都能够得到很好的补偿,在整个视场范围内光斑直径小于1 μm,实现更均匀的荧光激发,均匀成像。  相似文献   

15.
Paek EG  Choe JY  Oh TK 《Optics letters》1998,23(16):1322-1324
An experimental acousto-optic tunable filter that has a narrow spectral bandwidth (0.2 nm at 1550 nm) and a fast (10-micros) tuning capability with a continuous tuning range of approximately 50 nm is described. The tunable filter consists of an acousto-optic beam deflector with a diffraction grating whose grating vector is transverse to the direction of light propagation.  相似文献   

16.
An original acousto-optic deflector is based on the anisotropic diffraction in the paratellurite crystal. The deflector is characterized by a relatively high diffraction efficiency for depolarized laser radiation. The deflector consists of two sequential acousto-optic cells. Each cell deflects one of the orthogonally polarized components of the originally depolarized radiation. The first and second cells scan the low- and highfrequency parts of the angular interval, respectively. The simultaneous and independent operation of the cells makes it possible to use the entire optical (laser) power. A frequency band of 32 MHz is almost reached for depolarized radiation with a wavelength of 1.06 µm and the absolute angular interval is 50 mrad at a total efficiency of no less than 70%.  相似文献   

17.
A strong acousto-optic interaction of bounded light and sound beams of a Gaussian shape is considered for different geometries permitting long-term interaction. The anisotropic spreading of an acoustic beam in the course of its propagation is taken into account. The spectra of light beams are described by a Gaussian-polynomial expression, and a set of differential equations is derived which allows one to describe various geometries of acousto-optic diffraction. It is demonstrated that the transmission function of an acousto-optic cell essentially depends on the ratio between the dimensions of the light and sound beams and on the angle between the propagation direction of the diffracted beam and that of the incident beam. The degree of spreading of the acoustic beam noticeably affects the suppression of the transmission side lobes.  相似文献   

18.
Theoretical analysis of the performance of the acousto-optic light deflector is described. Detailed calculations for LiIO3-SF6 glass structure including the influence of the bonding layer and Q-factor on the frequency response of the deflector are presented. A method of increasing the bandwidth in the presence of the bonding layer is given.  相似文献   

19.
The nonreciprocal effect under collinear acousto-optic interaction in the low- and high-frequency regimes is studied theoretically. The magnitudes of nonreciprocity determined from the ultrasonic frequency and from the wavelength of light are shown to be quantitatively identical. An expression that governs the magnitude of the nonreciprocity and that is valid for both low- and high-frequency regimes of the collinear acousto-optic interaction is obtained. The shape and width of the frequency characteristic of the collinear acousto-optic interaction calculated in the low diffraction efficiency approximation are shown to be the same in the low- and high-frequency regimes. The dependence of the frequency bandwidth of the collinear acousto-optic interaction on the ultrasonic-wave attenuation and diffraction efficiency is obtained. The magnitude of the nonreciprocal effect in some of the crystals used in acousto-optics is estimated numerically. The nonreciprocity of the collinear interaction is shown to be substantially stronger in the high-frequency regime relative to the low-frequency regime. Sapphire is proved to be an optimal material for experimental realization of the nonreciprocal effect in the high-frequency regime.  相似文献   

20.
S. N. Antonov 《Technical Physics》2016,61(10):1597-1601
A new type of acousto-optic deflector based on anisotropic diffraction in paratellurite crystal is developed. Specific features of the method and proposed device are related to the broadening of the angular scanning range at a relatively high diffraction efficiency. The method is based on the application of the properties of the Bragg diffraction at phase modulation indices of 3π. Significant broadening of the frequency band at a relatively high diffraction efficiency is observed at high phase-modulation indices. Simultaneous application of indices of π and 3π allows a decrease in the control power to practically acceptable levels that provide continuous operation.  相似文献   

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