共查询到18条相似文献,搜索用时 62 毫秒
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光阱刚度是描述光镊对粒子进行操控的重要力学指标,实际使用过程中会受到激光功率的影响。采用均方位移法及玻尔兹曼统计法对搭建的光镊系统进行光阱刚度的标定,利用图像采集方法进行微粒位移的测量,并对两种方法的测量结果进行了比较。为了提高光阱刚度的标定结果的准确性,分析了光路放大倍数、温度变化对最后标定结果的精度影响。结果表明,两种方法进行标定的结果基本相同;光阱刚度在低激光功率(1 mW ~20 mW)范围时随功率近似线性增加,在高功率情况下(25 mW~60 mW)随功率增加不再线性增加,而是趋于一个饱和值。此外,光路放大倍数标定的精确性对标定的精度影响较大,10%的相对误差时,标定结果产生23%的变化,温度对标定的精度影响较小,0.1 ℃的温度变化导致标定结果0.034%的变化。 相似文献
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光镊是研究单分子生物物理特性的独特工具, 因而光镊设备的研发是一个极为重要的课题. 本文根据矩阵光学, 对基于有限远共轭显微镜的光镊操控光路进行计算, 得出了阱位径向操控和轴向操控方程, 并分析了光束调控系统、 共焦系统后置透镜和耦合透镜安装位置误差及物镜轴向位置调整对光镊阱位径向及轴向操控精度的影响. 计算结果显示, 当物镜初级像面和耦合透镜像方焦面完全重合, 光束调控系统和耦合透镜的距离误差对阱位径向和轴向操控精度没有影响. 光镊系统元器件定位不准时, 基于无限远共轭显微镜光镊的阱位径向操控误差和轴向操控误差都小于基于有限远共轭显微镜光镊的阱位径向操控误差和轴向操控误差. 当光镊耦合透镜定位误差控制在小于10 mm时, 基于有限远共轭显微镜光镊的径向和轴向操控误差分别小于5.9%和11.4%, 有限远共轭显微镜仍然存在改造为光镊的价值.本文理论为基于有限远共轭显微镜的光镊设计、改造和操控提供理论和实验指导.
关键词:
光镊
光学设计
矩阵
误差 相似文献
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采用四象限探测器和功率谱密度法,搭建了一套快速标定光镊三维光阱刚度的测量系统.实验中,用四象限探测器记录微粒做受限布朗运动时的位置信息,用功率谱密度法标定光阱刚度,测得了直径0.97μm SiO2小球和直径1μm PMMA小球的光阱刚度与激光功率的关系.结果表明:对于SiO2小球,当激光功率为50~120mW时,光阱刚度与激光功率成正比;对于PMMA小球,当激光功率为80~130mW时,光阱刚度与激光功率成正比.该光镊系统可用于生物、物理等微观领域研究的高准确度测力系统. 相似文献
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光镊技术捕获单个液滴并进行受激拉曼测量,在气溶胶动力学过程的研究方面取得了很大进展。然而,对于大气颗粒物之间通过碰撞完成由外混到内混的转变过程的定量分析,需要实现多种液滴同时捕获、操纵、碰并过程的精密观测。本文报道利用多光阱光镊技术对多液滴进行抓获,从而实现液滴之间的碰并复合过程的观测。为了实现多液滴的抓取,我们在单光镊技术的基础上,引进了声光偏转系统(AOD),这是多光阱光镊的核心技术。可以有效的将单光阱转化为多光阱,从而根据需要抓取一定数量的液滴,同时为后期的多液滴光谱测试奠定了基础。 相似文献
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传统的光镊技术使用单个物镜同时进行光学捕获与显微成像,使得捕获与成像区域被限制在物镜焦平面附近,无法同时观察到沿光轴方向(即Z向)捕获的多个微粒.本文提出一种轴平面(XZ平面)GerchbergSaxton迭代算法来产生沿轴向分布的多光阱阵列,将轴平面成像技术与光镊结合,实现了沿轴向对二氧化硅微球的多光阱同时捕获与实时观测.通过视频分析法测量了多个二氧化硅微球在轴向光镊阵列中的布朗运动,并标定了光阱刚度.本文提出的轴向多光阱微粒捕获与实时观测技术为光学微操纵提供了一个新的观测视角和操纵方法,为生物医学、物理学等相关领域研究提供了一种新的技术手段. 相似文献
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以超连续谱激光器作为捕获光源,首次提出并搭建了超连续谱双光束光纤光阱实验系统,实现了聚苯乙烯微球的捕获和操控。通过改变光纤端面间隔和调整捕获光功率的方式精确控制微球的位置,采用CCD图像分析方法实现了微球位置的精确测量。对微球受限布朗运动下的位置变化进行傅里叶变换,计算得到功率谱,与理论功率谱函数拟合后求出了其光阱刚度。结果表明,捕获光束的功率为28 mW时,光阱刚度达到1.3×10-6N/m,高于相同实验条件下单波长光纤光阱的刚度。与传统采用单色光作为捕获光源的光镊系统不同,超连续谱双光束光阱系统利用其宽谱优势,通过研究被捕获微粒的散射光谱信息可获取其尺寸、折射率等物理特征参数。 相似文献
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This paper proposes a scheme of axial triple-well optical dipole trap by employing a simple optical system composed of a circular cosine grating and a lens. Three optical wells separated averagely by ~37 μm were created when illuminating by a YAG laser with power 1 mW. These wells with average trapping depth ~0.5 μK and volume ~74 μm3 are suitable to trap and manipulate an atomic Bose--Einstein condensation (BEC). Due to a controllable grating implemented by a spatial light modulator, an evolution between a triple-well trap and a single-well one is achievable by adjusting the height of potential barrier between adjacent wells. Based on this novel triple-well potentials, the loading and splitting of BEC, as well as the interference between three freely expanding BECs, are also numerically stimulated within the framework of mean-field treatment. By fitting three cosine functions with three Gaussian envelopes to interference fringe, the information of relative phases among three condensates is extracted. 相似文献
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Calculation of axial optical forces exerted on medium-sized particles by optical trap 总被引:1,自引:0,他引:1
Fang-Lin Mao Qi-Rong Xing Kai Wang Li-Ying Lang Lu Chai Qing-Yue Wang 《Optics & Laser Technology》2007,39(1):34-39
Optical trapping has become an efficient technique of trapping and manipulating micrometer and sub-micrometer dimension particles. Particles in the range between the applicable regime of ray optics theory (ROT) and the Rayleigh regime (so-called medium-sized particles) are focused on. By using ROT and the generalized Lorenz–Mie theory (GLMT), axial optical forces and their dependences on particle sizes and beam waists are presented. Furthermore, by comparing the numerical results of these two theories, the applicability of the GLMT to particles of arbitrary size and the limit of ROT in the region of small particles are analyzed. A new criterion of the applicable region of ROT is obtained, i.e. the relative particle size β=2πa/λ20, where a is the particle radius and λ is the wavelength of light. The theoretical results will be of great help to the design and optimization of the most efficient optical trap. 相似文献
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Since the introduction of computer-controlled spatial light modulators (SLMs), holographic optical tweezers have become an
important tool for dynamic parallel optical manipulation. In this paper we clarify the usefulness of a new configuration for
optical trapping that creates light patterns using the combination of a diffractive optical element (DOE) and an SLM. This
configuration not only enables the use of the higher part of the SLM’s diffraction efficiency curve, because a simple hologram
can be chosen for the SLM, but also achieves three-dimensional dynamic optical manipulation over a large spatial range. By
switching blaze-like holograms displayed on the SLM, we demonstrated simultaneous transportation of three 6-μm-diameter polystyrene
beads over a range of 90 μm in the vertical direction and 37.5 μm in the horizontal direction. Compared with the same manipulation
executed using only the SLM, the range of this method is extended four-fold in the vertical direction and three-fold in the
horizontal direction. 相似文献