WO2020037813A1 - Double-lug circular diffraction diaphragm and vortex optical topological charge number detection system and method - Google Patents

Double-lug circular diffraction diaphragm and vortex optical topological charge number detection system and method Download PDF

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WO2020037813A1
WO2020037813A1 PCT/CN2018/112176 CN2018112176W WO2020037813A1 WO 2020037813 A1 WO2020037813 A1 WO 2020037813A1 CN 2018112176 W CN2018112176 W CN 2018112176W WO 2020037813 A1 WO2020037813 A1 WO 2020037813A1
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diffraction
light
vortex
arc
diaphragm
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PCT/CN2018/112176
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Chinese (zh)
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陈书青
张安
陈学钰
谢智强
王佩佩
刘俊敏
苏明样
贺炎亮
李瑛�
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深圳大学
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J11/00Measuring the characteristics of individual optical pulses or of optical pulse trains

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  • the invention relates to the field of information optics, in particular to a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and detection method.
  • a vortex beam is a structured beam that carries orbital angular momentum. It has a special spiral wavefront structure and a fixed topological charge. This kind of light beam with spiral phase structure will form a ring with orbital angular momentum when focusing, instead of the ordinary spot, it is mainly caused by the phase singularity.
  • Allen et al. Pointed out that the spiral phase distribution of a vortex beam can be described by the exp (il ⁇ ) phase function, with each photon carrying Orbital angular momentum.
  • l is the topological charge number ⁇ of the vortex light is the azimuth, and Is the Planck constant divided by 2 ⁇ .
  • each photon of a monochromatic vortex beam can theoretically carry both orbital angular momentum (OAM) and spin angular momentum (SAM), which affect the polarization and spatial distribution of vortex light, respectively.
  • OFAM orbital angular momentum
  • SAM spin angular momentum
  • recent studies have shown that vortex beams have great application value in the fields of optical tweezers, light capture, and quantum information technology research because of their ability to manipulate micro / nano particles.
  • the use of orbital angular momentum modes can effectively realize the transfer of information and greatly expand the capacity of transmitting information.
  • orbital angular momentum is an important parameter for describing the characteristics of vortex beams.
  • the above measurement methods can effectively determine the topological charge of vortex light, there are certain challenges in practical applications.
  • the size of the topological charge is often related to the size and arrangement of the porous.
  • the arrangement of sigma seriously affects its measurement accuracy.
  • the ring-band Fourier measurement method and cross-spectrum density function method can accurately measure the topological charge, the experimental system structure is more complicated and is not suitable for practical applications.
  • an object of the present invention is to provide a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and a detection method, which aim to solve the existing topological charge of vortex light measurement in the field of information optics
  • the method of numerical accuracy is not enough and the system structure is more complicated.
  • a binaural circular diffractive diaphragm includes a binaural circular diffractive aperture.
  • the binaural circular diffractive aperture is mainly composed of a first circular arc and a first circular arc having a double twist line and a circle center located at the symmetrical center of the double twist line. Two arcs
  • the first arc is connected to the upper side of the double button line
  • the second arc is connected to the lower side of the double button line
  • the lateral length of the double button line is the same as the first circle.
  • the ratio of the radii of the arcs is (2.5-3.2): 1; the binaural circular diffraction holes are bilaterally symmetrical.
  • the radius of the second arc is not equal to the radius of the first arc, forming an up-and-down asymmetric structure.
  • a ratio of a lateral length of the double twist line to a radius of the first arc is 31:11.
  • a radius of the first arc is 0.55 mm
  • a radius of the second arc is 0.605 mm
  • a lateral length of the double twist line is 1.55 mm.
  • a vortex light topology charge number detection system includes a vortex light generation module, a diaphragm diffraction module, and a light intensity detection module in order according to a beam propagation path.
  • the diaphragm diffraction module is provided with the above-mentioned binaural circular diffraction.
  • the vortex light generation module includes a light source for generating a Gaussian beam, a polarizer for changing a polarization direction of light, and a light for changing light.
  • the diaphragm diffraction module includes a diffraction screen for diffracting, a polarizer for adjusting light polarization, and a Fourier for generating light.
  • the transformed Fourier transform unit wherein the diffraction screen is loaded with the binaural circular diffraction diaphragm.
  • the light intensity detection module includes a light beam amplification system for expanding a beam and a light intensity photographing device for recording, wherein the light beam
  • the magnification system is a combination of two confocal convex lenses or a beam expander.
  • the focal lengths of the two confocal convex lenses are 25 mm and 75 mm, respectively, and the light intensity photographing device is a CCD detector.
  • a method for detecting the topological charge number of vortex light which uses the binaural circular diffraction diaphragm as described above to diffract vortex light to obtain the far-field diffraction intensity distribution of the vortex light, and then detects the far-field diffraction intensity distribution.
  • the present invention provides a binaural circular diffractive diaphragm as described above, and the vortex light passes through the binaural circular hole to generate a special light intensity distribution, so as to detect the topological charge of the vortex beam.
  • the invention can measure the topological charge of vortex light through diffraction of a single aperture, thereby avoiding the influence of the arrangement accuracy of multi-aperture mesopores on the measurement accuracy; and in adjusting the vortex beam to be coaxial with the binaural circular aperture At this time, even if there is a certain deviation, the diffracted light intensity distribution can still achieve the purpose of detecting the topological charge of the vortex light.
  • the center of the beam coincides with the center of the aperture, the phenomenon is most clear and obvious. Therefore, this technical solution allows the vortex beam to be rounded with both ears
  • the apertures are not strictly aligned and have a certain tolerance for detection operation errors.
  • FIG. 1 is a schematic diagram of a binaural circular diffraction aperture of the present invention.
  • FIG. 2 is a final external view of a binaural circular diffraction hole according to the present invention.
  • FIG. 3 is a schematic diagram of a module structure of a vortex optical topology charge number detection system according to the present invention.
  • FIG. 4 is a detailed schematic structural diagram of a vortex optical topological charge number detection system according to the present invention.
  • the present invention provides a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and detection method.
  • a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and detection method.
  • the structure of the binaural circular diffraction diaphragm provided by the present invention is shown in FIG. 1 and includes a binaural circular diffraction hole.
  • the binaural circular diffraction hole is mainly composed of a double button line 1 and a circle center are located on the double button line.
  • the symmetry center O is formed by a first arc 2 and a second arc 3.
  • the first arc 2 is connected to the upper side of the double twisted line
  • the second arc 3 is connected to the lower side of the double twisted line 1
  • the radius Ra of the first arc 2 is (2.5-3.2): 1
  • the binaural circular diffraction apertures are bilaterally symmetrical, and the shape of the binaural circular diffraction apertures finally formed is shown in FIG. 2 .
  • the radius Rb of the second arc 3 is not equal to the radius Ra of the first arc 2, and Rb can be made slightly larger or smaller than Ra, forming an up-and-down asymmetric structure, so that the diffraction pattern can distinguish the vortex beam.
  • the positive and negative of the topological charge is not equal to the radius Ra of the first arc 2, and Rb can be made slightly larger or smaller than Ra, forming an up-and-down asymmetric structure, so that the diffraction pattern can distinguish the vortex beam.
  • a ratio of a lateral length of the double twisted line to a radius of the first arc is 31:11, and a better diffraction effect can be obtained.
  • a preferred parameter of a binaural circular diffraction aperture is that the radius of the first arc is 0.55 mm, the radius of the second arc is 0.605 mm, and the lateral length of the double twisted line is 1.55 mm.
  • the vortex light passes through the binaural circular diffractive diaphragm to generate a special light intensity distribution, so as to detect the topological charge of the vortex beam.
  • the invention can measure the topological charge of vortex light through diffraction of a single aperture, thereby avoiding the influence of the arrangement accuracy of multi-aperture mesopores on the measurement accuracy; and in adjusting the vortex beam to be coaxial with the binaural circular aperture At this time, even if there is a certain deviation, the diffracted light intensity distribution can still achieve the purpose of detecting the topological charge of the vortex light.
  • the center of the beam coincides with the center of the aperture, the phenomenon is most clear and obvious. Therefore, this technical solution allows the vortex beam to be rounded with both ears
  • the apertures are not strictly aligned and have a certain tolerance for detection operation errors.
  • the present invention also provides a preferred embodiment of a vortex light topology charge number detection system, which is mainly used in the field of information optics.
  • a vortex light generation module 4 for different topologies
  • diaphragm diffraction module 5 for diffracting incident vortex light with different topological charges and forming a special light intensity distribution through Fourier transform
  • light intensity detection module 6 for Detecting the diffracted light intensity distribution
  • the diaphragm diffraction module is provided with the binaural circular diffraction diaphragm as described above for diffracting the vortex beam incident on the diaphragm diffraction module.
  • the topological charge of the vortex beam can be judged only by the light intensity distribution after the beam is diffracted through the aperture. Fewer optical elements are used, and the measurement results are intuitive and easy to read, which is convenient for practical operation.
  • the vortex light generating module 4 includes: a light source 41 for generating a Gaussian beam, a polarizer 42 for changing a polarization direction of the light, and a phase for changing the light.
  • the light source may be a He-Ne laser with a wavelength of 632.5 nm, and the polarizing plate is a half-wave plate.
  • the diaphragm diffraction module 5 includes a diffraction screen 51 for diffracting, a polarizer 52 for adjusting the polarization of light, and a Fourier transform unit 53 for generating a Fourier transform. Loaded with the binaural circular diffractive diaphragm.
  • the polarizer may be a Glan prism
  • the Fourier transform unit may be a convex lens having a focal length of 50 mm.
  • the light intensity detection module 6 includes: a beam magnification system 61 for expanding a beam and a light intensity photographing device 62 for recording, wherein the beam amplification system is a combination of two confocal convex lenses or a beam expanding mirror.
  • the focal lengths of the two confocal convex lenses may be set to 25 mm and 75 mm, respectively, and the light intensity photographing device may be a CCD detector.
  • the present invention also provides a method for detecting the topological charge of vortex light, which uses the binaural circular diffractive diaphragm as described above to diffract vortex light to obtain the far-field diffraction intensity distribution of the vortex light, and then diffracts the far-field light. The intensity distribution is detected.
  • This method can measure the topological charge of vortex light through single aperture diffraction, and has a certain tolerance for detection operation errors.
  • the Gaussian light emitted from the light source 41 passes through the polarizing plate 42 to generate horizontally polarized light and enters the vortex light generating device 43 to generate multi-level vortex light, and then filters the zero-order vortex light through the diaphragm 44.
  • the outgoing vortex beam can be approximated as:
  • Laguerre-Gaussian (LG) vortex beam where l is the topological charge, p is the radial parameter, r is the radial component, ⁇ is the phase, w 0 is the beam waist radius, and w (z) is at z Corset size,
  • z r is the Rayleigh distance
  • z is the beam transmission distance
  • k is the wave vector
  • the phase factor exp (-il ⁇ ) indicates that the beam has a spiral structure
  • i is an imaginary unit.
  • the generated vortex light is directly incident on the diffractive screen 51.
  • a diffraction phenomenon occurs.
  • the diffractive screen is provided with a binaural circular diffraction diaphragm.
  • the binaural circular diffraction hole of the binaural circular diffraction diaphragm is composed of a double button line 1.
  • the first arc 2 and the second arc 3 are both located at the center of symmetry O of the double twisted line.
  • the amplitude transmittance function T (x, y) of the double twisted line and the amplitude transmittance function M (x, y) of the two arcs can be expressed as:
  • x, y represent the horizontal and vertical coordinates of the function
  • a is half of the horizontal length of the double button line, as shown in the label of Figure 1
  • cric represents the circular function
  • R a is the radius of the first arc
  • R b is the second arc.
  • Radius the overall amplitude transmittance function after superposition can be expressed as:
  • t represents the amplitude transmittance function of the binaural circular hole
  • ⁇ and ⁇ are the horizontal and vertical coordinates of the function.
  • I represents the diffraction intensity distribution function
  • x and y are the horizontal and vertical coordinates of the function
  • z is the beam transmission distance
  • i is the imaginary unit
  • k is the wave vector
  • is the wavelength.
  • F denotes a Fourier transform function.
  • the polarizer 52, the Fourier transform unit 53 and the beam magnification system 61 are used to adjust and receive it in the direct-incidence light-intensity photographing device 62.
  • the diffraction pattern of the topological charge of vortex light is used to determine the topological charge. .
  • the present invention provides a binaural circular diffractive diaphragm and vortex light topological charge number detection system and detection method.
  • the vortex light generates a special light intensity distribution after passing through the binaural circular hole of the present invention, and realizes Detection of Topological Charge of Vortex Beams.
  • the invention can measure the topological charge of vortex light through diffraction of a single aperture, thereby avoiding the influence of the arrangement accuracy of multi-aperture mesopores on the measurement accuracy; and in adjusting the vortex beam to be coaxial with the binaural circular aperture At this time, even if there is a certain deviation, the diffracted light intensity distribution can still achieve the purpose of detecting the topological charge of the vortex light.
  • the present invention also provides a vortex light topological charge detection system based on the binaural circular diffractive diaphragm.
  • the topological charge of the vortex beam can be determined only by the light intensity distribution after the beam is diffracted through the aperture. There are fewer optical components, and the measurement results are intuitive and easy to read, which is convenient for practical operation.

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  • General Physics & Mathematics (AREA)
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Abstract

Disclosed by the present invention are a double-lug circular diffraction diaphragm and a vortex optical topological charge number detection system and detection method, the double-lug circular diffraction diaphragm comprising double-lug circular diffraction holes, wherein the double-lug circular diffraction hole is mainly formed by a lemniscate, a first arc and a second arc, the centers of the first arc and the second arc being located in the symmetric center of the lemniscate; the first arc is connected to the upper side of the lemniscate, the second arc is connected to the lower side of the lemniscate, and the ratio of the transverse length of the lemniscate to the radius of the first arc is (2.5-3.2): 1; and the double-lug circular diffraction holes are bilaterally symmetrical. According to the present invention, a vortex optical topological charge number may be measured by means of single aperture diffraction, so that the influence of the arrangement accuracy of multi-aperture mesopores on measurement precision is avoided. When a vortex light beam is adjusted to be coaxial with a double-lug circular aperture, the purpose of detecting the vortex optical topological charge number may still be achieved by diffraction light intensity distribution, even though a certain deviation exists. Therefore, the present technical solution has certain tolerance for detection operation error.

Description

双耳圆形衍射光阑及涡旋光拓扑荷数检测系统与检测方法Binocular circular diffraction diaphragm and vortex light topological charge number detection system and detection method 技术领域Technical field
本发明涉及信息光学领域,尤其涉及一种双耳圆形衍射光阑及涡旋光拓扑荷数检测系统与检测方法。The invention relates to the field of information optics, in particular to a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and detection method.
背景技术Background technique
涡旋光束是一种携带有轨道角动量的结构化光束,它具有特殊的螺旋波前结构和固定的拓扑荷数。这种具有螺旋相位结构的光束聚焦时会形成具有轨道角动量的环,而不是普通的点光斑,它主要是由相位奇点引起的。1992年,Allen等人指出涡旋光束的螺旋型相位分布可用exp(ilθ)相位函数来描述,每一光子上携带有
Figure PCTCN2018112176-appb-000001
的轨道角动量。其中l为涡旋光的拓扑荷数θ是方位角,并且
Figure PCTCN2018112176-appb-000002
是普朗克常数除以2π。也就是说,一束单色涡旋光束的每一光子理论上可同时携带有轨道角动量(OAM)和自旋角动量(SAM),它们分别影响着涡旋光的偏振和空间分布。近年来研究表明,由于涡旋光束具有微/纳米粒子的操控能力,在光镊、光俘获和量子信息技术研究等领域具有巨大的应用价值。特别是在量子信息技术研究领域,由于轨道角动量模式之间的无限正交性的存在,利用轨道角动量模式将能有效实现信息的传递,很大程度上扩大传输信息的容量。在涡旋光束研究中,轨道角动量作为描述涡旋光束特性的一个重要参数,如何高效测定轨道角动量的大小已成为重中之重,而轨道角动量的大小就是通过涡旋光束的拓扑荷数l来体现的,拓扑荷数l体现了光束绕奇点一周的相位变化规律。因此,探索一种更为高效的方法来检测涡旋光束的拓扑荷数具有很重要的研究意义。
A vortex beam is a structured beam that carries orbital angular momentum. It has a special spiral wavefront structure and a fixed topological charge. This kind of light beam with spiral phase structure will form a ring with orbital angular momentum when focusing, instead of the ordinary spot, it is mainly caused by the phase singularity. In 1992, Allen et al. Pointed out that the spiral phase distribution of a vortex beam can be described by the exp (ilθ) phase function, with each photon carrying
Figure PCTCN2018112176-appb-000001
Orbital angular momentum. Where l is the topological charge number θ of the vortex light is the azimuth, and
Figure PCTCN2018112176-appb-000002
Is the Planck constant divided by 2π. In other words, each photon of a monochromatic vortex beam can theoretically carry both orbital angular momentum (OAM) and spin angular momentum (SAM), which affect the polarization and spatial distribution of vortex light, respectively. Recent studies have shown that vortex beams have great application value in the fields of optical tweezers, light capture, and quantum information technology research because of their ability to manipulate micro / nano particles. Especially in the field of quantum information technology research, due to the existence of infinite orthogonality between orbital angular momentum modes, the use of orbital angular momentum modes can effectively realize the transfer of information and greatly expand the capacity of transmitting information. In the study of vortex beams, orbital angular momentum is an important parameter for describing the characteristics of vortex beams. How to efficiently determine the magnitude of orbital angular momentum has become a top priority, and the magnitude of orbital angular momentum is the topological load through the vortex beam Reflected by the number l, the topological charge number l reflects the phase change law of the beam around the singular point. Therefore, it is of great research significance to explore a more efficient method to detect the topological charge of vortex beams.
近些年来,在拓扑荷数测量研究中,科研工作者已经发现了几种比较有效的测量方法。2008年,Gregarious C.G Berkhout和Marco W.Beijersbergen等人提出一种多孔方法测量涡旋光束的轨道角动量。2009年王涛等人基于菲涅尔衍射积分理论,对拉盖尔高斯光束的单缝衍射特性进行了研究。同年国承山、卢磊磊等人提出了环带傅里叶变换法测量涡旋光束的拓扑荷数。2012年杨元杰等人利用交叉谱密度函数法测量部分相干涡旋光的轨道角动量。In recent years, in the research of topological charge measurement, researchers have found several more effective measurement methods. In 2008, Gregarious C.G. Berkhout and Marco W. Beijersbergen et al. Proposed a porous method to measure the orbital angular momentum of vortex beams. In 2009, Wang Tao et al. Studied the single-slit diffraction characteristics of Laguerre-Gaussian beams based on Fresnel diffraction integral theory. In the same year, Guo Chengshan, Lu Leilei and others proposed the annular band Fourier transform method to measure the topological charge of vortex beams. In 2012, Yang Yuanjie and others used the cross-spectral density function method to measure the orbital angular momentum of partially coherent vortex light.
上述的测量方法虽均能有效测定涡旋光的拓扑荷数,但在现实应用中却存在 一定的挑战,比如在多孔测量法中,拓扑荷数的大小往往与多孔的尺寸和排布息息相关,孔径的排布严重影响其测量精度,环带傅里叶测量法和交叉谱密度函数法虽能较为准确的测量拓扑荷数,但其实验系统结构较为复杂,不适合实际应用。Although the above measurement methods can effectively determine the topological charge of vortex light, there are certain challenges in practical applications. For example, in the porous measurement method, the size of the topological charge is often related to the size and arrangement of the porous. The arrangement of sigma seriously affects its measurement accuracy. Although the ring-band Fourier measurement method and cross-spectrum density function method can accurately measure the topological charge, the experimental system structure is more complicated and is not suitable for practical applications.
因此,现有技术还有待于改进和发展。Therefore, the existing technology needs to be improved and developed.
发明内容Summary of the Invention
鉴于上述现有技术的不足,本发明的目的在于提供一种双耳圆形衍射光阑及涡旋光拓扑荷数检测系统与检测方法,旨在解决现有信息光学领域的测量涡旋光的拓扑荷数的方法精度不够以及系统结构较为复杂的问题。In view of the above-mentioned shortcomings of the prior art, an object of the present invention is to provide a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and a detection method, which aim to solve the existing topological charge of vortex light measurement in the field of information optics The method of numerical accuracy is not enough and the system structure is more complicated.
本发明的技术方案如下:The technical solution of the present invention is as follows:
一种双耳圆形衍射光阑,包括双耳圆形衍射孔,所述双耳圆形衍射孔主要由双纽线、圆心均位于所述双纽线的对称中心的第一圆弧和第二圆弧构成;A binaural circular diffractive diaphragm includes a binaural circular diffractive aperture. The binaural circular diffractive aperture is mainly composed of a first circular arc and a first circular arc having a double twist line and a circle center located at the symmetrical center of the double twist line. Two arcs
其中,所述第一圆弧连接于所述双纽线的上侧,所述第二圆弧连接于所述双纽线的下侧,所述双纽线的横向长度与所述第一圆弧的半径之比为(2.5-3.2):1;所述双耳圆形衍射孔左右对称。Wherein, the first arc is connected to the upper side of the double button line, the second arc is connected to the lower side of the double button line, and the lateral length of the double button line is the same as the first circle. The ratio of the radii of the arcs is (2.5-3.2): 1; the binaural circular diffraction holes are bilaterally symmetrical.
所述的双耳圆形衍射光阑,其中,所述第二圆弧的半径不等于所述第一圆弧的半径,形成上下非对称结构。In the binaural circular diffractive diaphragm, the radius of the second arc is not equal to the radius of the first arc, forming an up-and-down asymmetric structure.
所述的双耳圆形衍射光阑,其中,所述双纽线的横向长度与所述第一圆弧的半径之比为31:11。In the binaural circular diffractive diaphragm, a ratio of a lateral length of the double twist line to a radius of the first arc is 31:11.
所述的双耳圆形衍射光阑,其中,所述第一圆弧的半径为0.55mm,所述第二圆弧的半径为0.605mm,所述双纽线的横向长为1.55mm。In the binaural circular diffraction diaphragm, a radius of the first arc is 0.55 mm, a radius of the second arc is 0.605 mm, and a lateral length of the double twist line is 1.55 mm.
一种涡旋光拓扑荷数检测系统,按照光束传播路径,依次包括涡旋光产生模块、光阑衍射模块和光强检测模块,所述光阑衍射模块中设置有如上所述的双耳圆形衍射光阑,用于衍射入射到所述光阑衍射模块上的涡旋光束。A vortex light topology charge number detection system includes a vortex light generation module, a diaphragm diffraction module, and a light intensity detection module in order according to a beam propagation path. The diaphragm diffraction module is provided with the above-mentioned binaural circular diffraction. A diaphragm for diffracting a vortex beam incident on the diaphragm diffraction module.
所述的涡旋光拓扑荷数检测系统,其中,按照光束传播路径,所述涡旋光生成模块依次包括:用于产生高斯光束的光源、用于改变光偏振方向的偏振片、用于改变光的相位的涡旋光产生装置和用于筛选涡旋光的光阑,其中,所述涡旋光产生装置为反射式相位型空间光调制器、螺旋相位板或者超表面。According to the vortex light topology charge number detection system, according to a beam propagation path, the vortex light generation module includes a light source for generating a Gaussian beam, a polarizer for changing a polarization direction of light, and a light for changing light. A phase vortex light generating device and a diaphragm for screening vortex light, wherein the vortex light generating device is a reflective phase-type spatial light modulator, a spiral phase plate, or a metasurface.
所述的涡旋光拓扑荷数检测系统,其中,按照光束传播路径,所述光阑衍射模块依次包括:用于发生衍射的衍射屏、用于调节光偏振的偏振镜和用于产生傅 里叶变换的傅里叶变换单元,其中,所述衍射屏上加载有所述双耳圆形衍射光阑。In the vortex light topology charge number detection system, according to a beam propagation path, the diaphragm diffraction module includes a diffraction screen for diffracting, a polarizer for adjusting light polarization, and a Fourier for generating light. The transformed Fourier transform unit, wherein the diffraction screen is loaded with the binaural circular diffraction diaphragm.
所述的涡旋光拓扑荷数检测系统,其中,按照光束传播路径,所述光强检测模块依次包括:用于扩束的光束放大系统和用于记录的光强拍摄装置,其中,所述光束放大系统为两个共焦的凸透镜组合或扩束镜。According to the vortex light topology charge number detection system, according to a light beam propagation path, the light intensity detection module includes a light beam amplification system for expanding a beam and a light intensity photographing device for recording, wherein the light beam The magnification system is a combination of two confocal convex lenses or a beam expander.
所述的涡旋光拓扑荷数检测系统,其中,两个共焦的凸透镜的焦距分别为25mm和75mm,所述光强拍摄装置为CCD探测器。In the vortex light topology charge number detection system, the focal lengths of the two confocal convex lenses are 25 mm and 75 mm, respectively, and the light intensity photographing device is a CCD detector.
一种涡旋光拓扑荷数检测方法,采用如上所述的双耳圆形衍射光阑对涡旋光进行衍射,得到涡旋光的远场衍射强度分布,然后对所述远场衍射强度分布进行探测。A method for detecting the topological charge number of vortex light, which uses the binaural circular diffraction diaphragm as described above to diffract vortex light to obtain the far-field diffraction intensity distribution of the vortex light, and then detects the far-field diffraction intensity distribution.
有益效果:本发明提供了一种如上所述的双耳圆形衍射光阑,涡旋光经过双耳圆形孔后产生特殊的光强分布,实现对涡旋光束拓扑荷数的检测。本发明通过单个孔径衍射,即可完成对涡旋光拓扑荷数的测量,从而避免了多孔径中孔的排布精度对测量精度的影响;并且在调节涡旋光束与双耳圆形孔径共轴时,即使有一定偏差,衍射光强分布仍能达到检测涡旋光拓扑荷数的目的,当光束中心与孔径中心重合时,现象最为清晰明显,因此本技术方案允许涡旋光束与双耳圆形孔径非严格对准,对检测操作误差具有一定的容忍度。Beneficial effect: The present invention provides a binaural circular diffractive diaphragm as described above, and the vortex light passes through the binaural circular hole to generate a special light intensity distribution, so as to detect the topological charge of the vortex beam. The invention can measure the topological charge of vortex light through diffraction of a single aperture, thereby avoiding the influence of the arrangement accuracy of multi-aperture mesopores on the measurement accuracy; and in adjusting the vortex beam to be coaxial with the binaural circular aperture At this time, even if there is a certain deviation, the diffracted light intensity distribution can still achieve the purpose of detecting the topological charge of the vortex light. When the center of the beam coincides with the center of the aperture, the phenomenon is most clear and obvious. Therefore, this technical solution allows the vortex beam to be rounded with both ears The apertures are not strictly aligned and have a certain tolerance for detection operation errors.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
图1为本发明的双耳圆形衍射孔的示意图。FIG. 1 is a schematic diagram of a binaural circular diffraction aperture of the present invention.
图2为本发明的双耳圆形衍射孔的最终外形图。FIG. 2 is a final external view of a binaural circular diffraction hole according to the present invention.
图3为本发明的涡旋光拓扑荷数检测系统的模块结构示意图。FIG. 3 is a schematic diagram of a module structure of a vortex optical topology charge number detection system according to the present invention.
图4为本发明的涡旋光拓扑荷数检测系统的具体结构示意图。FIG. 4 is a detailed schematic structural diagram of a vortex optical topological charge number detection system according to the present invention.
具体实施方式detailed description
本发明提供了一种双耳圆形衍射光阑及涡旋光拓扑荷数检测系统与检测方法,为使本发明的目的、技术方案及效果更加清楚、明确,以下对本发明进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。The present invention provides a binaural circular diffractive diaphragm and a vortex light topological charge number detection system and detection method. In order to make the purpose, technical solution, and effect of the present invention clearer and clearer, the present invention is further described in detail below. It should be understood that the specific embodiments described herein are only used to explain the present invention and are not intended to limit the present invention.
需要说明的是,本发明所述的“上侧”、“下侧”、“左”、“右”等方位术语,均是以图1为参考,具体地随着图形摆放角度的不同,本发明的技术方案的描述会有所不同。It should be noted that the azimuth terms such as “upper side”, “lower side”, “left side”, and “right side” in the present invention are all based on FIG. 1, and specifically according to the different angles of the graphics, The description of the technical solution of the present invention will be different.
本发明提供的双耳圆形衍射光阑的结构如图1所示,包括双耳圆形衍射孔,所述双耳圆形衍射孔主要由双纽线1、圆心均位于所述双纽线的对称中心O的第一圆弧2和第二圆弧3构成。The structure of the binaural circular diffraction diaphragm provided by the present invention is shown in FIG. 1 and includes a binaural circular diffraction hole. The binaural circular diffraction hole is mainly composed of a double button line 1 and a circle center are located on the double button line. The symmetry center O is formed by a first arc 2 and a second arc 3.
其中,所述第一圆弧2连接于所述双纽线的上侧,所述第二圆弧3连接于所述双纽线1的下侧,所述双纽线1的横向长度(2a)与所述第一圆弧2的半径Ra之比为(2.5-3.2):1;所述双耳圆形衍射孔左右对称,最终形成的双耳圆形衍射孔的形状如图2所示。Wherein, the first arc 2 is connected to the upper side of the double twisted line, the second arc 3 is connected to the lower side of the double twisted line 1, and the lateral length of the double twisted line 1 (2a ) And the radius Ra of the first arc 2 is (2.5-3.2): 1; the binaural circular diffraction apertures are bilaterally symmetrical, and the shape of the binaural circular diffraction apertures finally formed is shown in FIG. 2 .
优选的,所述第二圆弧3的半径Rb不等于所述第一圆弧2的半径Ra,可以让Rb略大于或略小于Ra,形成上下非对称结构,使衍射图案可以区分涡旋光束拓扑荷数的正负。Preferably, the radius Rb of the second arc 3 is not equal to the radius Ra of the first arc 2, and Rb can be made slightly larger or smaller than Ra, forming an up-and-down asymmetric structure, so that the diffraction pattern can distinguish the vortex beam. The positive and negative of the topological charge.
优选的,所述双纽线的横向长度与所述第一圆弧的半径之比为31:11,可以获得更好的衍射效果。较优的一种双耳圆形衍射孔参数为:所述第一圆弧的半径为0.55mm,所述第二圆弧的半径为0.605mm,所述双纽线的横向长为1.55mm。Preferably, a ratio of a lateral length of the double twisted line to a radius of the first arc is 31:11, and a better diffraction effect can be obtained. A preferred parameter of a binaural circular diffraction aperture is that the radius of the first arc is 0.55 mm, the radius of the second arc is 0.605 mm, and the lateral length of the double twisted line is 1.55 mm.
本发明的双耳圆形衍射光阑,涡旋光经过所述双耳圆形衍射光阑后产生特殊的光强分布,实现对涡旋光束拓扑荷数的检测。本发明通过单个孔径衍射,即可完成对涡旋光拓扑荷数的测量,从而避免了多孔径中孔的排布精度对测量精度的影响;并且在调节涡旋光束与双耳圆形孔径共轴时,即使有一定偏差,衍射光强分布仍能达到检测涡旋光拓扑荷数的目的,当光束中心与孔径中心重合时,现象最为清晰明显,因此本技术方案允许涡旋光束与双耳圆形孔径非严格对准,对检测操作误差具有一定的容忍度。In the binaural circular diffractive diaphragm of the present invention, the vortex light passes through the binaural circular diffractive diaphragm to generate a special light intensity distribution, so as to detect the topological charge of the vortex beam. The invention can measure the topological charge of vortex light through diffraction of a single aperture, thereby avoiding the influence of the arrangement accuracy of multi-aperture mesopores on the measurement accuracy; and in adjusting the vortex beam to be coaxial with the binaural circular aperture At this time, even if there is a certain deviation, the diffracted light intensity distribution can still achieve the purpose of detecting the topological charge of the vortex light. When the center of the beam coincides with the center of the aperture, the phenomenon is most clear and obvious. Therefore, this technical solution allows the vortex beam to be rounded with both ears The apertures are not strictly aligned and have a certain tolerance for detection operation errors.
本发明还提供了一种涡旋光拓扑荷数检测系统的较佳实施例,主要应用在信息光学领域,如图3所示,按照光束传播路径,依次包括涡旋光产生模块4(用于不同拓扑荷值涡旋光的生成)、光阑衍射模块5(用于对入射的具有不同拓扑荷的涡旋光进行衍射并通过傅里叶变换形成特殊的光强分布)和光强检测模块6(用于对衍射光强分布进行探测),所述光阑衍射模块中设置有如上所述的双耳圆形衍射光阑,用于衍射入射到所述光阑衍射模块上的涡旋光束。本系统中,只需通过光束经过孔径衍射后的光强分布,即可判断涡旋光束的拓扑荷数,所用到的光学元件较少,且测量结果直观易读,便于实际操作。The present invention also provides a preferred embodiment of a vortex light topology charge number detection system, which is mainly used in the field of information optics. As shown in FIG. 3, according to the beam propagation path, a vortex light generation module 4 (for different topologies) is sequentially included. Generation of charge vortex light), diaphragm diffraction module 5 (for diffracting incident vortex light with different topological charges and forming a special light intensity distribution through Fourier transform) and light intensity detection module 6 (for Detecting the diffracted light intensity distribution), the diaphragm diffraction module is provided with the binaural circular diffraction diaphragm as described above for diffracting the vortex beam incident on the diaphragm diffraction module. In this system, the topological charge of the vortex beam can be judged only by the light intensity distribution after the beam is diffracted through the aperture. Fewer optical elements are used, and the measurement results are intuitive and easy to read, which is convenient for practical operation.
具体地,如图4所示,按照光束传播路径,所述涡旋光生成模块4依次包括: 用于产生高斯光束的光源41、用于改变光偏振方向的偏振片42、用于改变光的相位的涡旋光产生装置43和用于筛选涡旋光的光阑44,其中,所述涡旋光产生装置43可以为反射式相位型空间光调制器、螺旋相位板或者超表面。光源可以是波长为632.5nm的He-Ne激光器,偏振片为二分之一波片。Specifically, as shown in FIG. 4, according to the beam propagation path, the vortex light generating module 4 includes: a light source 41 for generating a Gaussian beam, a polarizer 42 for changing a polarization direction of the light, and a phase for changing the light. The vortex light generating device 43 and the diaphragm 44 for screening vortex light, wherein the vortex light generating device 43 may be a reflective phase-type spatial light modulator, a spiral phase plate, or a metasurface. The light source may be a He-Ne laser with a wavelength of 632.5 nm, and the polarizing plate is a half-wave plate.
所述光阑衍射模块5依次包括:用于发生衍射的衍射屏51、用于调节光偏振的偏振镜52和用于产生傅里叶变换的傅里叶变换单元53,其中,所述衍射屏上加载有所述双耳圆形衍射光阑。具体地点,所述偏振镜可以为格兰棱镜,所述傅里叶变换单元可以为焦距为50mm的凸透镜。The diaphragm diffraction module 5 includes a diffraction screen 51 for diffracting, a polarizer 52 for adjusting the polarization of light, and a Fourier transform unit 53 for generating a Fourier transform. Loaded with the binaural circular diffractive diaphragm. Specifically, the polarizer may be a Glan prism, and the Fourier transform unit may be a convex lens having a focal length of 50 mm.
所述光强检测模块6包括:用于扩束的光束放大系统61和用于记录的光强拍摄装置62,其中,所述光束放大系统为两个共焦的凸透镜组合或扩束镜。具体的,两个共焦的凸透镜的焦距可以分别设置为25mm和75mm,所述光强拍摄装置可以为CCD探测器。The light intensity detection module 6 includes: a beam magnification system 61 for expanding a beam and a light intensity photographing device 62 for recording, wherein the beam amplification system is a combination of two confocal convex lenses or a beam expanding mirror. Specifically, the focal lengths of the two confocal convex lenses may be set to 25 mm and 75 mm, respectively, and the light intensity photographing device may be a CCD detector.
本发明还提供了一种涡旋光拓扑荷数检测方法,采用如上所述的双耳圆形衍射光阑对涡旋光进行衍射,得到涡旋光的远场衍射强度分布,然后对所述远场衍射强度分布进行探测。本方法通过单个孔径衍射,即可完成对涡旋光拓扑荷数的测量,并对检测操作误差具有一定的容忍度。The present invention also provides a method for detecting the topological charge of vortex light, which uses the binaural circular diffractive diaphragm as described above to diffract vortex light to obtain the far-field diffraction intensity distribution of the vortex light, and then diffracts the far-field light. The intensity distribution is detected. This method can measure the topological charge of vortex light through single aperture diffraction, and has a certain tolerance for detection operation errors.
下面结合图4对本发明的原理进一步详细说明。The principle of the present invention will be further described in detail below with reference to FIG. 4.
光源41出射的高斯光,经过偏振片42后产生水平偏振光入射到涡旋光产生装置43,产生多级涡旋光,然后经过光阑44筛选出零级涡旋光。此时,出射的涡旋光束的可近似表示为:The Gaussian light emitted from the light source 41 passes through the polarizing plate 42 to generate horizontally polarized light and enters the vortex light generating device 43 to generate multi-level vortex light, and then filters the zero-order vortex light through the diaphragm 44. At this time, the outgoing vortex beam can be approximated as:
Figure PCTCN2018112176-appb-000003
Figure PCTCN2018112176-appb-000003
其中
Figure PCTCN2018112176-appb-000004
代表拉盖尔-高斯(LG)涡旋光束,l为拓扑荷大小,p为径向参数,r为径向分量,φ为相位,w 0为束腰半径,w(z)为z处的束腰大小,
Figure PCTCN2018112176-appb-000005
为缔合拉盖尔多项式,z r为瑞利距离,z为光束传输距离,k为波矢,相位因子exp(-ilφ)表示该光束具有螺旋结构,i为虚数单位。
among them
Figure PCTCN2018112176-appb-000004
Laguerre-Gaussian (LG) vortex beam, where l is the topological charge, p is the radial parameter, r is the radial component, φ is the phase, w 0 is the beam waist radius, and w (z) is at z Corset size,
Figure PCTCN2018112176-appb-000005
To associate Laguerre polynomials, z r is the Rayleigh distance, z is the beam transmission distance, k is the wave vector, the phase factor exp (-ilφ) indicates that the beam has a spiral structure, and i is an imaginary unit.
产生出的涡旋光直入射到衍射屏51中发生衍射现象,衍射屏中设置有双耳圆形衍射光阑,双耳圆形衍射光阑的双耳圆形衍射孔由双纽线1、圆心均位于所述双纽线的对称中心O的第一圆弧2和第二圆弧3构成。双纽线的振幅透过率函数T(x,y)以及两个圆弧的振幅透过率函数M(x,y)可分别表示为:The generated vortex light is directly incident on the diffractive screen 51. A diffraction phenomenon occurs. The diffractive screen is provided with a binaural circular diffraction diaphragm. The binaural circular diffraction hole of the binaural circular diffraction diaphragm is composed of a double button line 1. The first arc 2 and the second arc 3 are both located at the center of symmetry O of the double twisted line. The amplitude transmittance function T (x, y) of the double twisted line and the amplitude transmittance function M (x, y) of the two arcs can be expressed as:
Figure PCTCN2018112176-appb-000006
Figure PCTCN2018112176-appb-000006
Figure PCTCN2018112176-appb-000007
Figure PCTCN2018112176-appb-000007
其中x,y代表函数的横纵坐标,a为双纽线横向长度的一半,见图1的标注,cric表示圆形函数,R a第一圆弧的半径,R b代表第二圆弧的半径,叠加后整体振幅透过率函数可表示为: Among them, x, y represent the horizontal and vertical coordinates of the function, a is half of the horizontal length of the double button line, as shown in the label of Figure 1, cric represents the circular function, R a is the radius of the first arc, and R b is the second arc. Radius, the overall amplitude transmittance function after superposition can be expressed as:
Figure PCTCN2018112176-appb-000008
Figure PCTCN2018112176-appb-000008
上式中,t代表双耳圆形孔振幅透过率函数,ξ和η为该函数的横纵坐标。将双耳圆形孔振幅透过率函数t(ξ,η)代入远场衍射强度公式,即可得到涡旋光通过双耳圆形孔径后的远场衍射强度分布,可表示为:In the above formula, t represents the amplitude transmittance function of the binaural circular hole, and ξ and η are the horizontal and vertical coordinates of the function. Substituting the binaural circular aperture amplitude transmittance function t (ξ, η) into the far-field diffraction intensity formula, the far-field diffraction intensity distribution of the vortex light passing through the binaural circular aperture can be obtained as:
Figure PCTCN2018112176-appb-000009
Figure PCTCN2018112176-appb-000009
上式中,I代表衍射强度分布函数,x和y是该函数的横纵坐标,z为光束传输距离,i为虚数单位,k为波矢,λ为波长,
Figure PCTCN2018112176-appb-000010
表示拉盖尔-高斯(LG)涡旋光束,F表示傅里叶变换函数。
In the above formula, I represents the diffraction intensity distribution function, x and y are the horizontal and vertical coordinates of the function, z is the beam transmission distance, i is the imaginary unit, k is the wave vector, and λ is the wavelength.
Figure PCTCN2018112176-appb-000010
Denotes a Laguerre-Gaussian (LG) vortex beam, and F denotes a Fourier transform function.
最后,利用偏振镜52、傅里叶变换单元53和光束放大系统61对其进行调整并后直入射光强拍摄装置62中进行接收,利用涡旋光拓扑荷数的衍射图案实现拓扑荷数的判别。Finally, the polarizer 52, the Fourier transform unit 53 and the beam magnification system 61 are used to adjust and receive it in the direct-incidence light-intensity photographing device 62. The diffraction pattern of the topological charge of vortex light is used to determine the topological charge. .
综上所述,本发明提供了一种双耳圆形衍射光阑及涡旋光拓扑荷数检测系统与检测方法,涡旋光经过本发明的双耳圆形孔后产生特殊的光强分布,实现对涡旋光束拓扑荷数的检测。本发明通过单个孔径衍射,即可完成对涡旋光拓扑荷数的测量,从而避免了多孔径中孔的排布精度对测量精度的影响;并且在调节涡旋光束与双耳圆形孔径共轴时,即使有一定偏差,衍射光强分布仍能达到检测涡旋光拓扑荷数的目的,当光束中心与孔径中心重合时,现象最为清晰明显,因此本技术方案允许涡旋光束与双耳圆形孔径非严格对准,对检测操作误差具有一定的容忍度。同时本发明还提供了基于所述双耳圆形衍射光阑的涡旋光拓扑荷数检测系统,只需通过光束经过孔径衍射后的光强分布,即可判断涡旋光束的拓扑荷数,所用到的光学元件较少,且测量结果直观易读,便于实际操作。In summary, the present invention provides a binaural circular diffractive diaphragm and vortex light topological charge number detection system and detection method. The vortex light generates a special light intensity distribution after passing through the binaural circular hole of the present invention, and realizes Detection of Topological Charge of Vortex Beams. The invention can measure the topological charge of vortex light through diffraction of a single aperture, thereby avoiding the influence of the arrangement accuracy of multi-aperture mesopores on the measurement accuracy; and in adjusting the vortex beam to be coaxial with the binaural circular aperture At this time, even if there is a certain deviation, the diffracted light intensity distribution can still achieve the purpose of detecting the topological charge of the vortex light. When the center of the beam coincides with the center of the aperture, the phenomenon is most clear and obvious. Therefore, this technical solution allows the vortex beam to be rounded with both ears The apertures are not strictly aligned and have a certain tolerance for detection operation errors. At the same time, the present invention also provides a vortex light topological charge detection system based on the binaural circular diffractive diaphragm. The topological charge of the vortex beam can be determined only by the light intensity distribution after the beam is diffracted through the aperture. There are fewer optical components, and the measurement results are intuitive and easy to read, which is convenient for practical operation.
应当理解的是,本发明的应用不限于上述的举例,对本领域普通技术人员来说,可以根据上述说明加以改进或变换,所有这些改进和变换都应属于本发明所附权利要求的保护范围。It should be understood that the application of the present invention is not limited to the above examples. For those of ordinary skill in the art, improvements or changes can be made according to the above description, and all these improvements and changes should fall within the protection scope of the appended claims of the present invention.

Claims (10)

  1. 一种双耳圆形衍射光阑,其特征在于,包括双耳圆形衍射孔,所述双耳圆形衍射孔主要由双纽线、圆心均位于所述双纽线的对称中心的第一圆弧和第二圆弧构成;A binaural circular diffractive diaphragm, characterized in that it comprises a binaural circular diffraction aperture, said binaural circular diffraction aperture is mainly composed of a double button line and a circle center located at the first center of symmetry of the double button line. A circular arc and a second circular arc;
    其中,所述第一圆弧连接于所述双纽线的上侧,所述第二圆弧连接于所述双纽线的下侧,所述双纽线的横向长度与所述第一圆弧的半径之比为(2.5-3.2):1;所述双耳圆形衍射孔左右对称。Wherein, the first arc is connected to the upper side of the double button line, the second arc is connected to the lower side of the double button line, and the lateral length of the double button line is the same as the first circle. The ratio of the radii of the arcs is (2.5-3.2): 1; the binaural circular diffraction holes are bilaterally symmetrical.
  2. 根据权利要求1所述的双耳圆形衍射光阑,其特征在于,所述第二圆弧的半径不等于所述第一圆弧的半径,形成上下非对称结构。The binaural circular diffractive diaphragm according to claim 1, wherein a radius of the second arc is not equal to a radius of the first arc, forming an up-and-down asymmetric structure.
  3. 根据权利要求1所述的双耳圆形衍射光阑,其特征在于,所述双纽线的横向长度与所述第一圆弧的半径之比为31:11。The binaural circular diffractive diaphragm according to claim 1, wherein a ratio of a lateral length of the double twist line to a radius of the first arc is 31:11.
  4. 根据权利要求3所述的双耳圆形衍射光阑,其特征在于,所述第一圆弧的半径为0.55mm,所述第二圆弧的半径为0.605mm,所述双纽线的横向长为1.55mm。The binaural circular diffractive diaphragm according to claim 3, wherein a radius of the first arc is 0.55 mm, a radius of the second arc is 0.605 mm, and a transverse direction of the double twist line is The length is 1.55mm.
  5. 一种涡旋光拓扑荷数检测系统,其特征在于,按照光束传播路径,依次包括涡旋光产生模块、光阑衍射模块和光强检测模块,所述光阑衍射模块中设置有权利要求1-4任一所述的双耳圆形衍射光阑,用于衍射入射到所述光阑衍射模块上的涡旋光束。A vortex light topology charge number detection system, characterized in that, according to a light beam propagation path, a vortex light generation module, a diaphragm diffraction module, and a light intensity detection module are sequentially included, and the diaphragm diffraction module is provided with claims 1-4 Any of the binaural circular diffraction diaphragms is used to diffract the vortex beam incident on the diaphragm diffraction module.
  6. 根据权利要求5所述的涡旋光拓扑荷数检测系统,其特征在于,按照光束传播路径,所述涡旋光生成模块依次包括:用于产生高斯光束的光源、用于改变光偏振方向的偏振片、用于改变光的相位的涡旋光产生装置和用于筛选涡旋光的光阑,其中,所述涡旋光产生装置为反射式相位型空间光调制器、螺旋相位板或者超表面。The vortex light topology charge number detection system according to claim 5, wherein the vortex light generation module comprises a light source for generating a Gaussian light beam and a polarizer for changing a polarization direction of the light according to a beam propagation path. A vortex light generating device for changing the phase of light and a diaphragm for screening the vortex light, wherein the vortex light generating device is a reflective phase-type spatial light modulator, a spiral phase plate, or a metasurface.
  7. 根据权利要求5所述的涡旋光拓扑荷数检测系统,其特征在于,按照光束传播路径,所述光阑衍射模块依次包括:用于发生衍射的衍射屏、用于调节光偏振的偏振镜和用于产生傅里叶变换的傅里叶变换单元,其中,所述衍射屏上加载有所述双耳圆形衍射光阑。The vortex light topology charge number detection system according to claim 5, characterized in that, in accordance with the beam propagation path, the diaphragm diffraction module comprises a diffraction screen for generating diffraction, a polarizer for adjusting light polarization, and A Fourier transform unit for generating a Fourier transform, wherein the binaural circular diffraction diaphragm is loaded on the diffraction screen.
  8. 根据权利要求5所述的涡旋光拓扑荷数检测系统,其特征在于,按照光束传播路径,所述光强检测模块依次包括:用于扩束的光束放大系统和用于记录的光强拍摄装置,其中,所述光束放大系统为两个共焦的凸透镜组合或扩束镜。The vortex light topology charge number detection system according to claim 5, characterized in that, according to the beam propagation path, the light intensity detection module comprises: a beam amplification system for expanding a beam and a light intensity photographing device for recording Wherein, the beam magnification system is a combination of two confocal convex lenses or a beam expander.
  9. 根据权利要求8所述的涡旋光拓扑荷数检测系统,其特征在于,两个共焦的凸透镜的焦距分别为25mm和75mm,所述光强拍摄装置为CCD探测器。The vortex light topology charge number detection system according to claim 8, wherein the focal lengths of the two confocal convex lenses are 25 mm and 75 mm, respectively, and the light intensity photographing device is a CCD detector.
  10. 一种涡旋光拓扑荷数检测方法,其特征在于,采用权利要求1-4任一所述的双耳圆形衍射光阑对涡旋光进行衍射,得到涡旋光的远场衍射强度分布,然后对所述远场衍射强度分布进行探测。A method for detecting the topological charge of vortex light, characterized in that the vortex light is diffracted by using the binaural circular diffraction diaphragm according to any one of claims 1-4, and the far-field diffraction intensity distribution of vortex light is obtained, and then The far-field diffraction intensity distribution is detected.
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