共查询到17条相似文献,搜索用时 250 毫秒
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光学相控阵光束扫描技术在激光雷达、空间光通信和光开关等领域拥有巨大的应用潜力。微透镜阵列光学相控阵可以通过微透镜阵列间μm量级的相对位移同时对多个出射光束的二维倾斜相位进行调制,从而实现大角度二维光束扫描,具有出射口径大、结构简单、体积小、微惯性、多功能等优点。首先介绍了微透镜阵列光学相控阵的扫描原理,之后对微透镜阵列光学相控阵国内外的发展现状、应用和现阶段存在的问题进行了阐述,最后对微透镜阵列光学相控阵的发展趋势进行了展望。 相似文献
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应用在相控阵雷达上的光学实时延迟线 总被引:1,自引:0,他引:1
相控阵天线是雷达技术的重要发展方向之一。电子相控阵雷达所遇到的问题是天线阵列孔径效应限制了雷达信号的瞬时带宽,使其不能满足通信和雷达技术的发展需要。光学实时延迟技术,可以解决这一问题。介绍了相控阵天线光实时延迟控制原理。并对几种典型的光实时延迟线的工作原理和技术特点作了简要的分析。 相似文献
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介绍了一种基于互耦补偿矩阵(MCCM)的迭代快速傅里叶变换(IFFT)技术,并将其应用于宽角度扫描相控阵的低旁瓣综合中。首先,在所提出的综合方法中,将互耦补偿矩阵引入到IFFT技术中以考虑阵元间的互耦效应,使考虑互耦的阵列远场重新满足方向图乘积原理。然后,提出了一款基片集成波导背腔结构的宽波束天线单元,该天线能够同时激励起TE110与TE210两种模式从而展宽其工作频带且具有宽波束性能,并且基于此单元分别建立了阵元数为35,75,100的宽角度扫描相控阵天线。最后,利用所提出的IFFT技术对这三个相控阵进行低旁瓣综合。与基于有源单元方向图遗传算法的对比结果表明,在-60°到60°的扫描范围内均能实现低旁瓣电平,并且IFFT优化算法具有更快的速度。 相似文献
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光学相控阵技术具有响应速度快、系统紧凑、功能多样和控制灵活等优点,在众多科学技术领域得到了广泛的应用。在近50年来的光学相控阵研究与应用中,涌现出了众多卓越的成果。为了对光学相控阵领域的发展进行梳理,简要回顾了光学相控阵技术的历史,并论述了光学相控阵技术的基本原理。从光束发射与接收等不同应用场景的角度,结合笔者的思考,深入介绍了光学相控阵在高品质的光源技术、激光相干合成技术、光束扫描技术、大气链路畸变控制技术以及合成孔径探测与成像技术多个领域的发展现状,并最后对光学相控阵技术的瓶颈与未来的发展研究趋势进行了评述。 相似文献
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将液晶作为平板光波导的上包层,构建了液晶光学相控阵器件.根据Frank-Oseen液晶连续体弹性形变理论与光栅衍射理论,研究分析了基于这种新型结构下液晶光学相控阵的传输特性,输出衍射特性和其它性能特性.研究结果表明,器件的传输电控相位延迟可以实现更大的光程差;阵列电极周期数目、电极宽度、电极间隔宽度等结构参量对器件的输出衍射光束的光强分布和半峰值全宽度影响很大,同时光束扫描的可行性得到论证;器件的响应时间提高了一个数量级,且其色散性能获得改善.为以后研制新型液晶光学相控阵提供了理论基础与技术设计依据. 相似文献
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B. Bellini M. A. Geday N. Bennis A. Spadło X. Quintana J. M. Otón R. Dąbrowski 《Opto-Electronics Review》2006,14(4):269-273
Liquid crystal (LC) phased arrays and gratings have been employed in optical switching and routing [1]. These diffractive
optic elements are of great interest because they can be scaled up to a large number of elements and their optical properties
can be electrically addressed with a low driving voltage. LC phase gratings have been achieved either by periodic addressing
of pixels or by using periodically-modified structures. The latter approach leads to less reconfigurable devices but the addressing
is simpler.
In this paper we focus on optical phased arrays where the phase is varied either continuously or discretely and where the
periodicity is induced by electrode configuration. We first describe a possible structure based on a conductive silicon wafer.
We argue that this structure can induce either continuously or discretely varying arrays while applying single voltage to
the array. In the second part we simulate the behaviour of such arrays. We base the simulation on a LC synthesized at the
Military University of Technology, this high-birefringence nematic LC shows in a 4-μm thick cell a linear phase shift range
of more than 360° between 1.2 V and 1.8 V. We calculate the distribution of the LC molecule director and assess the performance
of the array with respect to the applied voltage. Finally, the relevance of such technology for switchable phased arrays is
discussed. 相似文献
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Cascade arrangement of irregular optical phased arrays 总被引:1,自引:0,他引:1
We present the principle of cascade arrangement of irregular optical phased arrays. The optical phased-array beam deflector comprises arrayed optical waveguides that are spaced irregularly and arranged in a two-stage cascade. Relations between optical path differences and corresponding center-to-center spacings among elements in each stage are found, and phase matches between the two stages are achieved. Simulation shows a wide scanning angle with dramatically suppressed sidelobes. 相似文献
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引入负声源,导出了环形平面换能器声场的简洁表示式,计算了单个圆环、多个同心圆环同时激励及环阵相控聚焦声源产生的声场,分析了环的宽度、环数及聚焦点位置等因素对声场特征的影响。提出根据各阵元在声场中某点产生的声压的相位来确定各阵元电激励信号的延时,此方法较根据各阵元到该点的平均声程确定各阵元电激励信号的延时,能更难确地在该点实现聚焦。 相似文献
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微纳相控线阵超声换能器参数(阵元数目、阵元宽度及阵元间距)直接影响其横向声场分布,而其横向声场分布是能否实现高成像分辨率、大探测深度的决定性因素,也是制备换能器的主要依据。该文利用数值模拟研究微纳相控线阵超声换能器阵元参数对其横向声场中主瓣强度、-3 dB主瓣宽度、第一级旁瓣及栅瓣的影响。结果表明,主瓣强度随着阵元数目增加而增大,随阵元间距减小而增大,随着阵元宽度的增大呈现先增大后减小的趋势;-3 dB主瓣宽度随着阵元数目和阵元间距的增大而减小,随着阵元宽度的减小而减小;此外,减小阵元数目、减小阵元间距或增大阵元宽度均可以抑制旁瓣;栅瓣在阵元间距满足一定条件时可以完全消除。通过这些研究为微纳相控线阵超声换能器的优化设计与制备提供理论参考。 相似文献
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Numerical simulation and comparative analysis of acoustic fields formed by two-dimensional phased arrays designed for ultrasonic surgery are conducted for the case of scanning by several focuses (in particular, by nine focuses arranged in a line and also by an array of nine focuses forming a 3×3 square grid). Calculations are performed for arrays with elements positioned at the surface both regularly (in square, ring, or hexagonal patterns) and randomly. Criteria for evaluating the “quality” of the intensity distributions in the field formed by the array in the case of scanning by several focuses are proposed. The quality of the intensity distributions for arrays containing 255 and 256 elements 5 mm in diameter arranged in regular patterns on the array’s surface (in square, ring, or hexagonal patterns) is inferior to that for arrays containing 256 randomly positioned elements. Among the regular arrays, the highest quality of intensity distributions is obtained for ring arrays, and the lowest quality is obtained for arrays with elements arranged in square or hexagonal patterns. The irregularity in the element positioning the array’s surface improves the quality of intensity distributions by reducing the secondary intensity peaks in the field formed by the array and, primarily, in the focal plane. 相似文献