共查询到18条相似文献,搜索用时 156 毫秒
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透镜焦距及球面曲率的测量 总被引:2,自引:1,他引:1
概述目前透镜焦距及球面曲率半径的测量方法,介绍透镜焦距及球面曲率半径的准直光束补偿测量法的原理,指出该方法的关键是对补偿光束准直性的检测,提出一种用准直光束补偿和横向错位进行干涉测量透镜焦距及球面曲率的新方法。 相似文献
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长焦距测量的Talbot-Moiré法是研究热点,目前很多方法虽然都是基于Talbot现象和Moiré技术,但基本原理和实验方案各不相同,因此焦距计算公式也不相同。基于透镜位相变换作用,利用Talbot效应和Moiré条纹,通过图像处理的方法获得条纹的斜率变化,根据焦距与莫尔条纹斜率之间的关系求得透镜焦距。由于长焦透镜的焦距相对于被测透镜厚度大得多,完全可以看作是薄透镜对光束的变换,可用薄透镜对球面波的变换作用来近似表示其对高斯光束的变换。因此,该方法测量长焦透镜焦距对于高斯光束与非高斯光束焦距测量结果无差别,均适用。最后全面分析了该测量方法的误差及精度极限。在影响测量精度的各个误差因素中,光栅节距误差对焦距测量的影响最为显著。 相似文献
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长焦距测量的Talbot Moiré法是研究热点,目前很多方法虽然都是基于Talbot现象和Moiré技术,但基本原理和实验方案各不相同,因此焦距计算公式也不相同。基于透镜位相变换作用,利用Talbot效应和Moiré条纹,通过图像处理的方法获得条纹的斜率变化,根据焦距与莫尔条纹斜率之间的关系求得透镜焦距。由于长焦透镜的焦距相对于被测透镜厚度大得多,完全可以看作是薄透镜对光束的变换,可用薄透镜对球面波的变换作用来近似表示其对高斯光束的变换。因此,该方法测量长焦透镜焦距对于高斯光束与非高斯光束焦距测量结果无差别,均适用。最后全面分析了该测量方法的误差及精度极限。在影响测量精度的各个误差因素中,光栅节距误差对焦距测量的影响最为显著。 相似文献
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利用双光栅Lau效应测量透镜焦距 总被引:1,自引:1,他引:0
根据计量光栅的特点,可以利用双光栅效应测量透镜焦距.本文简述了利用双光栅Lau效应测量透镜焦距的实验原理、实验装置及测量方法,并计算了测量结果的不确定度. 相似文献
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《光学学报》2020,(4)
基于朗奇-泰伯效应及莫尔条纹技术,利用发散光和不等周期光栅的焦距测量方法被用于小口径长焦透镜的焦距测量。将一块曲率半径存在加工误差的平凹长焦透镜作为待测透镜进行焦距测量。在未知透镜真实曲率半径的情况下,首先计算待测透镜曲率半径误差对焦距检测精度的影响,并确定透镜在整个检测系统中的位置,然后进行透镜焦距实际测量,分别计算多组测量焦距值。通过对比发现,在未知待测透镜曲率半径的情况下,检测焦距的重复性、稳定性均一致,所测焦距均为33200~33270mm,且重复性精度高于±0.055%,测量精度优于焦深的1/5。结果充分说明,所提方法对小口径长焦透镜的焦距检测是可靠、有效的。 相似文献
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利用联合付里叶变换谱干涉法测量透镜焦距 总被引:3,自引:0,他引:3
本文提出了采用联合付里叶变换频谱干涉法测量透镜焦距的方法。输入面上两个分布完全相同的图像经光学付里叶变换在频谱面上得到二者付里叶变换频谱的干涉条纹,通过测量干涉条纹的间距即可得到透镜的焦距。该方法装置简单、操作调整方便;易于采用实时空间光调制器、CCD及微机实现快速自动测量,且具有较高的精度。文中进行了原理分析和实验验证。 相似文献
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一种测量透镜单色焦距的新方法 总被引:1,自引:0,他引:1
根据单狭缝衍射原理,提出了一种测量透镜单色焦距的新方法。结合光电扫描技术,使该方法既可适合于可见光区,又可用于不可见光区的测量,同对,可获得较高的测量精度。 相似文献
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Yuzhao Ma 《Optical Review》2012,19(3):125-130
In the present work the propagation of a partially coherent radially polarized beam through aligned and misaligned ABCD optical systems is discussed. The elements of the beam coherence-polarization matrix for a partially coherent radially polarized beam propagating through these systems are derived for the first time. Using the derived analytical results the intensity distribution of the focused partially coherent radially polarized beam after a low-NA lens is investigated. It is shown that the coherence of the light source affects the beam intensity profile at the focal plane significantly, while for the given coherence of the light source the focal length of the used lens does not affect the beam intensity profile at the focal plane. This is consistent with the case of a partially coherent Hermite-Gaussian beam, as expected. 相似文献
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A simple derivation, which relates the thermal lens focal length in solid state lasers to pump power and a method for direct
estimation of thermal lens focal length, is reported. This method is applicable to any type of stable resonator. The method
is used for the measurement of the thermal lens focal length with an accuracy of 8% in an axially pumped microchip laser.
The variation of focal length with pump power is also measured. 相似文献
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A novel means of focal length measurement is proposed based upon Hartmann–Shack principle of wavefront detection. Mathematical approaches of focal length measurement are deduced without the necessity of knowing the position of lens principle plane. In experiment, laser sources with wavelength of 633 nm and 780 nm are separately used and focal length of three pieces of doublets is measured under two wavelengths mentioned above. As were shown by the results, this method of focal length measurement could not only accurately measure lens focal length, but also evaluate chromatic aberration of them. Since the intensity of light is detected by CCD, optical characteristics of lens beyond the range of visible light are also measurable when response range of CCD allows. This new means of focal length measurement is characterized by high accuracy, fast measuring and easy to setup, thereby, it is applicable in wide fields of area. 相似文献