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1.
为了减小四频差动激光陀螺(DILAG)的磁敏感性,研究了工作点对磁敏感性的影响.根据理论分析,磁敏感性主要来自于左、右旋陀螺相对比例因子修正的不对称,它与工作点有关,在最佳工作点下为零.通过在DILAG增益管上缠绕线圈产生轴向磁场,调节附着于腔平移镜上的压电换能器的驱动电压改变工作点,得到磁灵敏度随工作点的变化规律.结果表明,DILAG在最佳工作点下对外界磁场不敏感,且在每个工作区存在唯一的最佳工作点.DILAG工作在最佳工作点可以使外界干扰在差动中消除,因而有利于提高其性能.为了保证DILAG工作在最佳工作点,必须改变传统的光强差稳频方式.  相似文献   

2.
零闭锁激光陀螺(ZLG)增益曲线不对称导致左、右旋陀螺的比例因子修正系数不相等,使得当陀螺稳频工作点与磁不敏感点存在频率差时,陀螺零偏对外界磁场变化敏感,降低了陀螺的精度并限制了使用环境。利用兰姆半经典理论分析计算了比例因子修正系数与增损比的关系,并得到了陀螺的磁不敏感点与放电电流的关系,从信号处理系统中排除放电电流变化对控制信号的影响,并进行了实验验证。理论计算和实验结果均表明,线性地改变陀螺放电电流,陀螺磁不敏感点位置会因增益曲线的增损比变化而发生相应线性改变,进而能够通过控制放电电流降低陀螺的磁灵敏度。  相似文献   

3.
 针对目前四频差动激光陀螺光学解调方案可靠性和温度特性差的特点,介绍一种基于FPGA的数字拍频解调方案。分析了四频差动激光陀螺数字拍频解调对电路系统的需求,对数字拍频解调的关键部件——低通滤波器进行了设计与实现。根据四频差动激光陀螺的特性参数计算滤波器的通带截止频率及阻带截止频率,使用MATLAB的滤波器设计和分析工具FDATool完成了有限冲击响应(FIR)数字滤波器的参数设计,并利用Xilinx公司的FPGA集成开发环境ISE实现FIR数字滤波器的片上系统设计。仿真和实验结果表明,所设计的FIR数字滤波器对四频差动激光陀螺的和频分量衰减达到-66 dB,满足四频差动激光陀螺拍频解调的需求,并有助于实现四频差动激光陀螺的小型化和数字化。  相似文献   

4.
四频差动激光陀螺中的S—P各向异性效应   总被引:7,自引:0,他引:7  
杨在富  袁晓东 《光学学报》1998,18(9):255-1260
理论分析了四频差动激光陀螺中左,右旋椭圆偏振模式的非对称性,这种非对称性激光陀螺性能的影响是至关重要的,而引起这种非对称性的物理因素是环形的S-P相位和损耗的各向异性。  相似文献   

5.
为了简化四频差动激光陀螺的信号读出系统,采用了一种基于FPGA实现的数字电路解调方案取代传统的合光棱镜中的1/4波片和偏振片来分离左、右旋陀螺信号。简述了四频差动激光陀螺的信号读出原理及解调电路方案,设计了主要由A/D转换器和FPGA构成的四频陀螺信号读出系统。通过Quartus Ⅱ等EDA工具在软件上对系统予以了实现,并针对其主要功能模块进行了仿真验证。仿真结果表明,将四频陀螺信号转化为数字信号后,利用FPGA实现信号解调并最终达到分离左、右旋陀螺信号的方案是可行的,该方案将有助于全数字化激光陀螺的研制。  相似文献   

6.
与腔内运行线偏振光的抖动陀螺相比,腔内运行圆偏振光的零闭锁激光陀螺对磁场更为敏感.为了减小零闭锁激光陀螺的磁敏感性,理论分析了其磁敏感特性.当左、右旋陀螺的比例因子修正相等时,陀螺零偏不随磁场的变化而变化,同时陀螺比例因子线性度也将得到改善.试验测试了零闭锁激光陀螺的磁敏感性,结果表明陀螺存在磁不敏感点.试验结果与理论分析吻合.与传统的被动磁屏蔽方法相比,通过主动控制使得零闭锁激光陀螺工作在磁不敏感点的方法对于降低该陀螺的磁灵敏度和提高准确度具有实用价值.  相似文献   

7.
杨建强  廖丹 《应用光学》2009,30(3):514-518
为研究石英晶体温度效应对四频差动激光陀螺的影响,从陀螺的自再现传播矩阵出发,结合石英晶体旋光率随温度变化的经验公式,利用琼斯矩阵求本征模的方法,得出了四频差动激光陀螺腔内光场本征偏振态与温度的关系并进行了数值分析,得到椭圆度和左右旋差损随温度变化的曲线。结果表明,石英晶体温度效应对偏振特性的影响与反射镜片的振幅反射率和反射相移有密切关系,对于典型陀螺参量,在-60℃~60℃范围内石英晶体温度效应导致左右旋差损从0增加至10-6量级, 椭圆度从0.122增至0.138。  相似文献   

8.
四频差动激光陀螺最佳工作点实时控制技术   总被引:1,自引:0,他引:1  
王飞  龙兴武  汪之国 《光学学报》2012,32(11):1123001
为了降低四频差动激光陀螺(FMDLG)零偏对外界因素影响的敏感性,采用了最佳工作点实时控制技术。该技术使用色散平衡和稳频偏置的方法,对增益区磁场和失谐频率进行小幅度正弦调制,在FMDLG输出零偏中解调出误差信号,经负反馈控制回路使FMDLG在对外界干扰敏感性最小的唯一最佳工作点下工作。与仅使用光强差进行稳频的传统方法相比,最佳工作点控制技术大大降低了FMDLG的磁敏感度和零偏稳定性,证实了FMDLG最佳工作点实时控制技术的有效性;静态、动态测试实验结果证明了该技术的正确性。  相似文献   

9.
为了解决光强差稳频系统易受光电元件参量影响的问题,设计了一套用于异面腔四频差动激光陀螺的小抖动稳频系统。采用高频放大和幅度检波电路检出四频差动激光陀螺顺时针(或逆时针)输出光束的拍频幅度,然后用模数转换器采集到数字信号处理器(DSP)内。四频差动激光陀螺正常工作时拍频幅度取极大值,因此可通过对腔长进行小抖动调制实现稳频。利用DSP设计了一套数字式稳频系统,1 s取样的稳频精度为2×10-9,更重要的是稳频点不受光电元件参量变化的影响。设计的小抖动稳频电路精度高、通用性好,对提高四频差动激光陀螺适应恶劣环境的能力有一定的价值。  相似文献   

10.
四频差动激光陀螺小抖动稳频初步研究   总被引:3,自引:0,他引:3  
为避免传统光强差稳频方式的缺陷,提出了四频差动激光陀螺小抖动稳频方法.从四频陀螺工作原理出发,分析了小抖动稳频的特性和难点,如鉴频灵敏度较低、陀螺参量不当时工作点有严重偏移、工作模式不易判别、陀螺零漂受稳频精度影响大.针对每一难点提出,解决办法,特别是极低噪声电路的设计技术是提高四频陀螺小抖动稳频精度的关键.提出的解决方案为进一步实验研究提供了理论指导.  相似文献   

11.
针对当前四频差动激光陀螺(DLG)读出系统结构复杂、易受温度影响等问题,对现有读出系统进行了改进,设计了使用电子信号处理代替光学信号处理来分离左、右旋陀螺信号的新型读出系统。通过对一个DLG同时使用新旧两套不同的读出系统进行测试,得到了相同的测试结果,表明电子信号处理和光学信号处理在分离左、右旋陀螺信号方面是等效的。在此基础上,首先使用模数转换器对DLG的光电转换信号进行采样,然后进行了数字信号处理,并研制出了全数字化读出系统。新型读出系统不使用四分之一波片和偏振片等光学元件,具有温度稳定性好、结构简单、全数字化等优点,有利于四频陀螺性能的提高和批量生产。  相似文献   

12.
 理论上推导出了环形激光器对S光和P光相位延迟差与其拍频峰对应的压电陶瓷电压差的关系式,分析了方形环形激光器对S光和P 光的频率响应特性,通过测量拍频峰电压差实现环形激光器反射镜相位延迟差测量。通过搭建环形激光器频率响应特性测试系统,从实验上验证了理论计算的正确性。结果表明,该方法测量误差小于1.5%,满足环形激光器反射镜相位延迟差测量要求。  相似文献   

13.
The frequency-dependent circular dichroism is proposed to extend the wave manipulating capability of coding metasurfaces. As a proof of concept, the bispectral circular dichroic coding metasurfaces (CDCMs) are realized using circular dichroism resonators (CDRs) implemented via introducing loss resistors into the circular polarization conversion resonators. The CDRs are distinguished into left-handed CDRs and right-handed CDRs. Left-handed CDRs absorb left-handed circularly polarized (LCP) wave and convert right-handed circularly polarized (RCP) wave into LCP wave. Conversely, they are defined as right-handed CDRs. Two bispectral CDRs are designed with the left-handed (right-handed) and right-handed (left-handed) working bands in 7–8.5 and 22.2–22.5 GHz, respectively. And then, 1 bit bispectral CDCM with 0101…/1010… coding sequence is designed. Simulated results indicate that the designed CDCM strongly absorb the incident LCP (RCP) waves in the frequency region 7–8.5 GHz (22.2–22.5 GHz), but the incident RCP (LCP) waves are anomalously reflected into four beams of the LCP (RCP) waves with high efficiency. The measured results agree well with the simulations. The results in this work may provide an effective solution for the inverse and helicity-dependent manipulation of the electromagnetic waves in two distinct frequency regions.  相似文献   

14.
New modes of propagation for a single, intense beam of light have been theoretically studied in the frequency region of giant two photon absorption (GTA) to excitonic molecule (EM) states. Self-consistent solutions for left and right circularly polarized (LCP and RCP respectively) components have been obtained for the polariton dispersion equations which include the ω- and k-dependent self-energy term for exciton due to the GTA process to EM. There are two types of solutions: [I] k(LCP) = k(RCP), [II] k(LCP) ≠ k(RCP). The induced branch for the former has a half of EM mass. There are experimental observations which support the existence of such new propagation modes.  相似文献   

15.
Asymmetric transmission (AT) reflects the conversion efficiency of a chiral nanostructure for circularly polarized light and is widely used in polarization and optoelectronic devices. In this study, a new mechanism is proposed to generate AT when a planar chiral nanostructure is illuminated under left‐handed circularly polarized (LCP) and right‐handed circularly polarized (RCP) light illumination. The new mechanism can be achieved by breaking the symmetry of the designed planar chiral nanostructure which give rise to a new transmittance peak and dip at a particular wavelength under RCP and LCP light illumination, respectively. The proposed new mechanism is also capable of actively tuning the generated resonant modes. Besides this, when graphene strips are added to the designed planar chiral nanostructure, similar results are obtained as that from breaking the symmetry of the planar chiral nanostructure. In this case, the generated AT could also be actively tuned by varying the Fermi energies of graphene strips.  相似文献   

16.
The theory describing the far-field emission from a dipole source embedded inside a chiral sculptured thin film (CSTF), based on a spectral Green function formalism, was further developed to allow for infiltration of the void regions of the CSTF by a fluid. In doing so, the extended Bruggeman homogenization formalism — which accommodates constituent particles that are small compared to wavelength but not vanishingly small — was used to estimate the relative permittivity parameters of the infiltrated CSTF. For a numerical example, we found that left circularly polarized (LCP) light was preferentially emitted through one face of the CSTF while right circularly polarized (RCP) light was preferentially emitted through the opposite face, at wavelengths within the Bragg regime. The centre wavelength for the preferential emission of LCP/RCP light was red shifted as the refractive index of the infiltrating fluid increased from unity, and this red shift was accentuated when the size of the constituent particles in our homogenization model was increased. Also, the bandwidth of the preferential LCP/RCP emission regime decreased as the refractive index of the infiltrating fluid increased from unity.  相似文献   

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