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1.
研究了利用运动光栅的多普勒效应进行切向位移的遥测技术。提出了测量光路,采用声光调制器作为分光和频移器件并用于鉴向,实现了50m的远距离光栅位移遥测。达到测量分辨率0.8μm,光栅位移40mm,最大累积误差优于34μm。并用理论分析和实验,证明了远距离目标的焦深及其计算方法,导出了计算公式。 相似文献
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分析了单声光移频器构成的外差式激光多普勒测振计中声光移频器驱动信号的频率稳定性和信号功率对待测振动信号的影响.为了降低声光移频器驱动信号频率漂移的影响,提出双声光移频器构成的外差式激光多普勒测振计,并基于直接数字频率合成技术,以相位噪音低、初始相位可控的芯片AD9912为核心器件,完成了声光移频器驱动信号生成及处理模块的设计.开展了双声光移频器组成的外差式激光多普勒测振计的振动测量实验,结果表明,驱动信号生成装置可以驱动声光移频器正常工作,且测振计的本底噪音在0~10kHz频带范围内呈现平坦分布,0~1kHz频段内噪音得到明显抑制,较单声光移频器构成的外差式激光多普勒测振计有显著改善. 相似文献
3.
分析了单声光移频器构成的外差式激光多普勒测振计中声光移频器驱动信号的频率稳定性和信号功率对待测振动信号的影响.为了降低声光移频器驱动信号频率漂移的影响,提出双声光移频器构成的外差式激光多普勒测振计,并基于直接数字频率合成技术,以相位噪音低、初始相位可控的芯片AD9912为核心器件,完成了声光移频器驱动信号生成及处理模块的设计.开展了双声光移频器组成的外差式激光多普勒测振计的振动测量实验,结果表明,驱动信号生成装置可以驱动声光移频器正常工作,且测振计的本底噪音在0~10kHz频带范围内呈现平坦分布,0~1kHz频段内噪音得到明显抑制,较单声光移频器构成的外差式激光多普勒测振计有显著改善. 相似文献
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通过光纤频移干涉技术测量了超声在光纤中产生的多普勒频移,提出一种光纤超声传感方法.将缠绕在压电陶瓷上的光纤环接入到频移干涉萨格拉克干涉仪中,以压电陶瓷作为超声波信号源,调节声光调制器使得干涉信号偏置在零点,达到系统灵敏度最高,通过干涉信号的频率和幅值测量到了超声引起光纤环中发生的多普勒频移,进而获得了作用在光纤环上的超声波信号.实验结果表明,用该方法测量超声频率的相对误差为0.001%,频响在所测量的20~200kHz范围内具有良好的线性.该方法在管道健康监测、固体内部裂缝监测、大型机械装备结构损伤监测等方面具有应用前景. 相似文献
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《中国光学》2019,(2)
采用双声光调制器光路快速偏转技术与自准直光栅法实现CO_2激光全波段快调谐同光路输出。首先对声光调制器特性进行实验研究,结果显示:声光调制器偏转角度约为4. 4°,与运用布拉格方程计算结果相符;且激光单次通过声光调制器移频量为40. 68 MHz,与声光驱动器射频频率一致,将激光往返多次经声光调制器的移频量叠加。进而,开展基于声光调制器的CO_2激光快调谐实验研究,运用两个对称布置的同驱动频率声光调制器补偿声光移频,实现偏转光路振荡输出,运用光栅法在直线光路中实现激光全波段可调谐输出。最终,在声光调制器时序控制下,实现双波长激光快调谐同光路输出,选定激光波长的切换时间约为1 ms,脉宽小于300 ns,且双波长切换速度不受CO_2激光跃迁谱带的限制。 相似文献
7.
频移分离型三维激光多普勒测速仪研究 总被引:2,自引:0,他引:2
研究一种采用频移分离方法的新型三维激光多普勒测速仪(3DLDV)。该仪器以单色He-Ne激光器和单只光电探测器并配合简单的光学发射和接收系统即实现了三维速度分量的同时测量。三个分量的速度信号由声光调制器引入的三种光学频移区分,通过电子滤波器完成信号的相互分离。在光学发射系统设计中采用独特的单轴四光束结构,通过光束组合形成三双光束差动模式的激光多普勒测速仪光。本文中还给出了该仪器的系统设计参数并分析 相似文献
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激光多普勒技术在固体测量方面的运用 总被引:5,自引:1,他引:4
介绍了激光多普勒测量技术的原理和后散射型固体表面测量方式。通过声光调制器的偏频后 ,能够确定物体的运动方向。对多普勒信号进行光学外差处理并对多普勒信号进行测相 ,可以提高测量的精度。用差动微分多普勒技术进行测量 ,可以消除由固体表面特性和激光光强的波动引起的误差。 相似文献
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为在能量天平动圈位移测量中实现大范围纳米精度法-珀干涉绝对距离测量, 提出了声光移频器双通道配置, 实现了调谐范围为200 MHz的可调谐频差. 通过分析声光移频器调制带宽与衍射效率的平衡与入射光束聚焦透镜的关系, 确定透镜的最佳焦距范围; 利用零级光斑分布特点准确定位入射光束, 保证一级衍射光束质量. 声光移频器在调制带宽内的实验单通道和双通道峰值衍射效率分别为79.54%, 61.41%; 声光移频器双通道配置输出的一级衍射光束与入射本征光束的拍频范围为440-640 MHz, 是单通道调制带宽输出220-320 MHz的两倍, 信噪比好. 理论分析表明, 声光移频器双通道配置方法实现的可调谐频差可测量腔长变化范围约为53 mm的折叠法-珀腔. 相似文献
11.
V. M. Kotov 《Acoustical Physics》2002,48(5):572-575
A technique for the acoustooptic multiplication of the frequency shift of an optical beam is proposed. The technique is based on the cascade diffraction of the beam by a single acoustic wave with the use of Bragg polarization splitting in a uniaxial crystal. The fundamental possibility of the practical realization of the technique is confirmed experimentally by using anisotropic acoustooptic diffraction in LiNbO3. 相似文献
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The acousto-optic control of light polarization due to diffraction by leaky acoustic waves in ZX-LiNbO? has been demonstrated. The randomly polarized light of 633 nm wavelength is converted by the anisotropic diffraction into two beams with mutually orthogonal polarizations, the relative intensities of which depend on the light incidence angle and acoustic frequency. Variation in acoustic frequency from 108 to 112 MHz rotates the polarization of the output optical beam by 90°. The acousto-optic control is accomplished entirely by electronic means and can be applied for implementation of fast polarization converters. 相似文献
13.
Acoustooptic Bragg diffraction without overemodulation (i.e., with the extended high-efficiency region on the diffraction
efficiency dependence vs. sound amplitude) is studied theoretically and experimentally. It is found that this effect appears
in the case of a symmetrically nonuniform acoustic field and is due to the equality of additional opposite phase shifts of
light beams passing through symmetric regions of the acoustic field. The situation is considered when an acoustic field is
excited by a three-section phased-array transducer. The conditions are determined, in which reverse optical power transfer
from the diffracted beam to transmitted beam (overemodulation) in the case of a high (close to 100%) diffraction efficiency
is considerably suppressed. In the case of a phased array, the effect weakly depends on the frequency of sound and the size
of transducer sections, which makes it possible to observe it in a wide range of acoustooptic interaction parameters. 相似文献
14.
By the use of the vector diffraction theory, the focusing properties of radially polarized Bessel-like beam with radial cosine wave front phase through a high numerical-aperture (NA) lens are investigated theoretically and numerically in this work. The wave front phase distribution is a cosine function of radial coordinate. Calculation results show that focus shift is considerably influenced by changing frequency parameter C and topological charge. An increase on the focus shift C, the total intensity pattern changes remarkably and it focuses along the optical propagation axis. Thus, the focal shift direction can be adjusted by the change of the frequency parameter in cosine function. In this paper, the generation of the focal spot allows an increase in focal length in the axial direction of the incident beam propagation. Under higher numerical aperture (NA = 0.95), the effect of the frequency parameter and topological charge on the focal pattern gets stronger. 相似文献
15.
The subject of investigation is the formation of a highly efficient multiple-beam diffraction field resulting from acoustooptic diffraction by a periodically modulated acoustic wave and acoustic signal composed of a set of independently generated equidistant frequency components. Conditions for minimization of optical losses associated with higher diffraction orders are analyzed. A highly efficient multiple-beam diffraction field is formed by optimizing the phases and amplitudes of signal independent components. A technique of acoustooptic measurements at a high laser radiation intensity is developed, and the basics of the theory are verified experimentally. An attempt to split the power of a laser beam propagating through an optical fiber into seven channels of equal intensities is realized with a net efficiency of 80%. 相似文献
16.
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. 相似文献
17.
针对SiO2光波导声光布拉格器件,计算了SiO2非对称平板波导TE模式的横向场分布;给出了SiO2/ZnO/Air层状介质结构的性能方程、运动方程和麦克斯韦方程,推导出这种层状结构的特征方程,并结合所满足的边界条件,得到了各层介质的位移及电磁场分布;计算了声表面波所引起的光学相对介质隔离率张量的变化,最后讨论了声光衍射效率和光场与声场的重叠积分、声功率、声频率、声孔径和光波导参数之间的关系。结果表明,在低频范围内光场与声表面波场重叠良好;低阶模的重叠积分始终大于高阶模重叠积分,最低阶模与声表面波相互作用最强,所需声功率最小;当声功率一定时,增加声孔径可以提高衍射效率。 相似文献
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19.
A superluminescent diode monolithically integrated with a surface acoustic wave Bragg-cell to operate as a beam deflector is proposed. The analysis procedures for determining the acoustic and optical modes, and modal diffraction of the optical beam are employed to develop a practical model for the integrated device. Results from this model are used to assess the operational characteristics of the proposed integrated device and to provide design guidelines. 相似文献
20.
K. Prabakaran K. B. Rajesh T. V. S. Pillai R. Chandrasekaran Z. Jaroszewicz 《Optical and Quantum Electronics》2013,45(6):563-570
Focal shift in radially polarized beam with radial cosine phase wavefront are investigated theoretically by vector diffraction theory. The wavefront phase distribution is cosine function of radial coordinate. Simulation results show that when the radially polarized beam with radial cosine wavefront phase is focused, the focal pattern differs considerably with frequency parameter in the cosine function term. On increasing C, focus can shift along optical axis and focal pattern changes remarkably. Focus may move in different direction under different condition. Focal shift distance fluctuates on increasing C, and fluctuation amplitude also increases simultaneously. In addition, focal shift direction can also be adjusted by changing frequency parameter in cosine function. 相似文献