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1.
干涉法测量晶体电光系数实验装置的改进   总被引:7,自引:1,他引:6  
尹鑫 《光学学报》1989,9(4):53-356
用一台泰曼干涉仪,以压电晶体的逆压电效应补偿晶体电光效应所引起的光程变化,提供了一种简单、迅速和高灵敏度测量晶体电光系数的方法.  相似文献   

2.
用干涉仪的方法测量了Ce:BaTiO3晶体的低频电光系数和压电系数.排除压电效应对光通过晶体引起相位的变化,得到低频下经极化的Ce:BaTiO3单晶的电光系数r42=1945±220pm/V和r13=11.8±1pm/V.从而,为研究Ce:BaTiO3晶体的光折变效应和理论计算提供了精确的线性电光系数 关键词:  相似文献   

3.
干涉法测量晶体的压电系数   总被引:1,自引:0,他引:1  
我们用一台泰曼干涉仪,以DKDP晶体的电光效应补偿由于晶体反压电效应听引起的光程差,提供了一种简单、迅速和高灵敏度测量晶体压电系数的方法.  相似文献   

4.
基于声光效应的光束偏转控制理论研究   总被引:3,自引:0,他引:3  
付琼  金韬  周诠 《光子学报》2007,36(6):1083-1087
基于参量互作用观点及声光互作用原理,构建了入射光为高斯光并且存在声波吸收情况下的声光偏转器模型.基于此模型研究了超声波频率、声波功率和光束入射角对衍射光的影响.对比了有声波吸收和无声波吸收两种情况下上述三个参量对衍射光产生的不同影响.计算结果表明,同无声光吸收时相比,当存在声波吸收时,偏转器的衍射效率将减小,导致衍射波形畸变,光强峰值位置发生偏移.  相似文献   

5.
本文通过解压电效应的基本方程,应用一维近似理论,结合边界条件,得出压电共振晶体中电场是不均匀的,它将导致“电光栅”的产生。“电光栅”与“声光栅”可以相互耦合,产生“高次光栅”。压电诱导声光(PESD)调制器中的一次电光效应更有助于对入射光束的衍射和调制。实验结果证实本文结论。 关键词:  相似文献   

6.
铁电薄膜物理学与集成铁电学专题研讨会在南京大学举行铁电体是一类具有自发电极化且其极化矢量在外电场作用下反转的电介质,它具有压电、热释电、电光、声光、光折变、非线性光学效应和高介电系数等特性,早就引起材料科学及物理学界的重视。近年来,由于制膜技术和微电...  相似文献   

7.
通过对四方、立方晶系的纵向电光效应和多维正常声光效应的研究,选定了四方晶系的KDP晶体和立方晶系的GaP晶体作为多维正常声电光器件的最佳晶体,并通过计算两种晶体的声光互作用性能参量,确定了它们的二维、三维、四维正常声电光效应的最佳工作模式。研究结果为多维正常声电光器件的设计与制作打下了良好基础。多维声电光器件在多路光通信和多通道光信息处理中有应用前景。  相似文献   

8.
《物理》1994,23(12):762-763
我国铁电薄膜物理学与集成铁电学若干重要问题的研究建议(提纲)1.学术背景铁电体为一类具有自发电极化,而且其极化矢量可以在外电场作用下反转的电介质,它们同时具有压电、热释电、电光、声光、光折变、非线性光学等效应及高介电系数。作为光电功能材料,铁电体早在...  相似文献   

9.
LiNbO_3(简称LN)晶体是60年代发展起来的新材料。它是铁电体,具有压电、电光、声光等多种效应,且易于用提拉法在c轴方向生长出大块单晶,故应用颇为广泛。由于其压电性,它在超声领域中也占有重要地位。尤其LN+35°Y切板,具有机电耦合系数较高、频率常数较高、介电常数较低以及高温性能好等多种优点。很适宜于作高频和高温超声检测器的压电元件。因此,常希望采用此种晶体切板。  相似文献   

10.
声光调制器利用声光晶体的声光效应对输入信号进行外调制。另外,实验结果也表明:由声光调制器出射的衍射光存在偏振态的改变。旋转起偏器的透振方向,拉曼—纳斯衍射的一级衍射光的偏振态发生变化;且各级衍射光的偏振度随着透振方向的改变而发生周期性的变化。  相似文献   

11.
When a surface acoustic wave (SAW) propagates on the surface of a GaAs semiconductor, coupling between electrons in the two-dimensional electron gas beneath the interface and the elastic host crystal through piezoelectric interaction will attenuate the SAW. The coupling coemcient is ~alculated for the SAW propagating along an arbitrary direction. It is found that the coupling strength is strongly dependent on the propagating direction. When the SAW propagates along the [011] direction, the coupling becomes quite weak.  相似文献   

12.
When a surface acoustic wave (SAW) propagates on the surface of a GaAs semiconductor, coupling between electrons in the two-dimensional electron gas beneath the interface and the elastic host crystal through piezoelectric interaction will attenuate the SAW. The coupling coefficient is calculated for the SAW propagating along an arbitrary direction. It is found that the coupling strength is strongly dependent on the propagating direction. When the SAW propagates along the [011] direction, the coupling becomes quite weak.  相似文献   

13.
Electro-magneto-acoustic SH waves propagating oblique to the periodic layered piezoelectric structures are studied under the coupling of the acoustic wave and the electromagnetic wave. Band structures of the so-called piezoelectric superlattice and phononic/photonic crystal are given both at acoustic frequencies and at optical frequencies. For the periodic layered piezoelectric structures, phonon-polaritons (the coupling modes of the phonons and photons) are found not only happening near the center of the Brillouin zone (in the long-wavelength limit) at acoustic frequencies, but also being able to appear in the whole Brillouin zone at optical frequencies. Appearing of these phonon-polaritons may provide a way to design a new type of acousto-optic devices.  相似文献   

14.
声电光效应的耦合波方程理论   总被引:9,自引:2,他引:7  
俞宽新  赵启大 《光学学报》1998,18(4):66-470
将声光效应与电光效应的耦合波方程相结合,统一为声电光效应的耦合波方程,并对之进行求解,给出声电光效应的衍射效率公式。  相似文献   

15.
The modulation of an intense electromagnetic beam induced by the acousto-optic (AO) effect has been analysed in a transversely magnetised semiconductor-plasma medium. The effect of carrier diffusion on the threshold field and gain profile of the modulated wave has been extremely investigated using coupled mode theory. The origin of the AO interaction is assumed to lie in the induced nonlinear diffusion current density of the medium. By considering the modulation process as a four wave parametric interaction an expression for effective third-order AO susceptibility describing the phenomena has been deduced. The modulation is greatly modified by propagation characteristics such as dispersion and diffraction due to dielectric relaxation of the acoustic mode. The threshold pump field and the steady state growth rates are estimated from the effective third-order polarisation in the plasma medium. Analytical estimation reveals that in the presence of enhanced diffusion due to excess charge carriers the modulated beam can be effectively amplified in a dispersionless acoustic wave regime. The presence of an external dc magnetic field is found to be favourable for the onset of diffusion induced modulational amplification of the modulated wave in heavily doped regime. Received 5 November 2001  相似文献   

16.
The influence of the dimension of an acousto-optic cell in the plane orthogonal to the plane of acousto-optic diffraction on the acoustic field structure and, consequently, on acousto-optic diffraction is studied theoretically and experimentally. A method is suggested for approximate calculation of the acoustic field with regard to the acoustic column reflection from the crystal faces. Based on this method, the influence of the acousto-optic cell dimensions is analyzed in a wide range of ratios between the height of the piezoelectric transducer and the height of the crystal. A region of acoustic power concentration is predicted to arise both for parallel faces and for slight wedging. A number of statements are demonstrated with paratellurite used as an interaction medium. The results may be useful in designing acousto-optic devices.  相似文献   

17.
A spatial Fourier transform approach is proposed to investigate the effects of polarization changes and beam profile deformation of light during acousto-optic (AO) interaction in isotropic media. The behaviour of the total scattered optical fields inside the AO cell can be properly described by a vector wave equation of which the permittivity is perturbed by an acoustic wave propagating inside the medium. In the Bragg regime, using a spatial Fourier transform approach, two coupled differential equations can be derived from the wave equation to depict AO interaction in the spatial frequency domain. Analytic solutions, which comprise the effects of changing polarization, beam deformation and propagating diffraction, can be found from the coupled equations. Detailed numerical simulations, including Fourier transforming the incident light profile to calculate the spectra of the scattered light beams and, hence, their profiles in space using the inverse transform, are presented.  相似文献   

18.
The propagation and reflection of bulk ultrasonic waves in a paratellurite crystal have been investigated by the acousto-optic method. Simultaneous excitation of two acoustic waves by one piezoelectric transducer has been observed in a cell of complex, specially chosen configuration. Maximally efficient conversion of the energy of a quasi-longitudinal wave into a single reflected quasi-shear wave with a walkoff angle 72° is implemented for the reflection from a free crystal boundary. The wave beam compression by a factor of 7 is observed for this reflection. A reflection (close to backward) of waves with an angle of spatial separation of the incident and reflected beams equal to 8° is also implemented. The acousto-optic figure of merit values of the medium are calculated for arbitrary propagation and polarization directions of the interacting light and ultrasonic waves. Possible applications of the effects studied in acousto-optics and acoustoelectronics are indicated.  相似文献   

19.
The features of noncollinear acousto-optic interaction in gyrotropic crystals in the intermediate diffraction regime and the regime of Bragg diffraction were investigated. The dependence of the efficiency of diffraction in gyrotropic paratellurite, tellurium, and quartz crystals on the intensity of the ultrasonic wave, acousto-optic interaction length, and incident-light polarization was investigated. It is shown that the gyrotropy of the crystal is responsible for the appearance of a multiple-peak structure of the Bragg maximum. It has been established that in the case of propagation of incident and diffracted waves in the vicinity of the optical axis of the crystal, the diffraction efficiency is independent of the polarization state of the incident light. The results of theoretical calculations are in agreement with the experimental results obtained for uniaxial crystals. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 67, No. 1, pp. 105–110, January–February, 2000.  相似文献   

20.
Anisotropic acousto-optic diffraction in biaxial crystal of alpha-iodic acid has been studied in the case in which the wave vector of the ultrasound is almost orthogonal to one of the optical axes and the directions of incident and diffracted light beams are close to the optical axis. It is shown that, owing to the complex form of wave surfaces in the field of optical axes of a biaxial crystal, the considered variant of acousto-optic interaction is very sensitive to changes in the direction of the wave vector of the ultrasound that imposes special requirements to accuracy of manufacturing of acousto-optic devices.  相似文献   

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