WO2023024381A1 - Metasurface optical element, design method and structured light projection module - Google Patents

Metasurface optical element, design method and structured light projection module Download PDF

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Publication number
WO2023024381A1
WO2023024381A1 PCT/CN2021/142516 CN2021142516W WO2023024381A1 WO 2023024381 A1 WO2023024381 A1 WO 2023024381A1 CN 2021142516 W CN2021142516 W CN 2021142516W WO 2023024381 A1 WO2023024381 A1 WO 2023024381A1
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simulated
nano
optical element
antennas
phases
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PCT/CN2021/142516
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French (fr)
Chinese (zh)
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汪肇坤
伍未名
刘风雷
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浙江水晶光电科技股份有限公司
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Priority claimed from CN202110980167.9A external-priority patent/CN113671612A/en
Priority claimed from CN202110980751.4A external-priority patent/CN113671613A/en
Application filed by 浙江水晶光电科技股份有限公司 filed Critical 浙江水晶光电科技股份有限公司
Publication of WO2023024381A1 publication Critical patent/WO2023024381A1/en

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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/30Collimators
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/42Diffraction optics, i.e. systems including a diffractive element being designed for providing a diffractive effect
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B5/00Optical elements other than lenses
    • G02B5/18Diffraction gratings

Definitions

  • the present application relates to the field of optical technology, in particular, to a metasurface optical element, a design method, and a structured light projection module.
  • Structured light projects a specific pattern onto the surface of an object, collects it through the receiving module, calculates the position and depth information of the object according to the change of the light signal caused by the object, and then restores the entire depth space.
  • the pattern can be designed as stripes, regular lattices, grids, speckles, codes, etc., or even more complex light shapes.
  • the application range of structured light is more and more extensive, such as face recognition, gesture recognition, projector, three-dimensional (Three-dimensional, 3D) outline reconstruction, depth measurement, anti-counterfeiting identification, etc. Therefore, how to provide a projection module that stably emits structured light has become the focus of people's research.
  • the structured light projection module in the related art mainly includes a light source, a collimator lens and a diffractive optical element.
  • the collimator mirror and the diffractive optical element are discrete components, so that the entire module takes up a large space and the alignment accuracy is low.
  • the present application provides a metasurface optical element, a design method, and a structured light projection module, so as to at least improve the problem that the structured light projection module in the related art occupies a large space and has low alignment accuracy.
  • a metasurface optical element may include a substrate, and a plurality of nanoantennas arranged on the substrate to modulate the incident light beam through transmission phase, at least two nanoantennas in size Different and multiple nano-antenna arrays are distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase.
  • the orthographic projection of the nano-antenna on the substrate may be a C4 rotationally symmetric figure.
  • the orthographic projection of the nano-antenna can be circular.
  • the orthographic projection of the nano-antenna can be a square.
  • the plurality of nano-antennas may include a first antenna and a second antenna
  • the orthographic projection of the first antenna on the substrate may be a circle
  • the orthographic projection of the second antenna on the substrate may be a square.
  • the side length of the square may be 50nm to 500nm.
  • the diameter of the circular shape may be 50nm to 500nm.
  • the side length of the square may be 50nm to 500nm
  • the diameter of the circle may be 50nm to 500nm
  • the center-to-center distance between two adjacent nano-antennas may be 200nm to 600nm.
  • the heights of the multiple nano-antennas may be greater than 300nm.
  • the heights of the multiple nano-antennas may be the same.
  • the number of nanoantennas with different sizes may be greater than or equal to 4, and at least two nanoantennas have different sizes.
  • the substrate may be a transparent substrate, and the material of the transparent substrate may be quartz, glass or silicon oxide film.
  • the material of the nano-antenna can be silicon, titanium oxide, aluminum oxide or silicon nitride.
  • some embodiments of the present application provide a method for designing a metasurface optical element, the method may include:
  • Multiple analog phases are discretized to obtain multiple discrete phases, wherein the number of multiple nano-antennas on the base of the metasurface optical element corresponds to the number of multiple discrete phases, and the transmission phases of multiple nano-antennas correspond to their corresponding The discrete phases are the same.
  • the multiple first simulated nanoantennas can be A simulated nano-antenna and the plurality of second simulated nano-antennas are fine-tuned to optimize the simulation results, thereby optimizing the superposition phase.
  • obtaining the corresponding collimation phases of the plurality of first simulated nanoantennas arranged on the substrate may include:
  • the collimation phases corresponding to each of the plurality of first simulated nano-antennas are obtained according to the simulated focal length, the lens focusing equation and the distance between the centers of two adjacent first simulated nano-antennas.
  • the center-to-center distance between two adjacent first simulated nanoantennas may be determined according to the preset working wavelength of the first simulated nanoantennas and the field angle to be realized.
  • obtaining the respective diffraction phases corresponding to the plurality of second simulated nanoantennas arranged on the substrate may include:
  • the diffraction phases corresponding to each of the plurality of second simulated nano-antennas are obtained according to the simulated viewing angle and a preset algorithm.
  • the material of the metasurface optical element may be determined according to the required working wavelength.
  • the structured light projection module may include a light source and any of the above-mentioned metasurface optical elements.
  • the light source is located on the light incident side of the metasurface optical element.
  • the metasurface optics The element is used to collimate and diffract the light beam emitted by the light source.
  • the present application provides a metasurface optical element and its design method, and a structured light projection module.
  • the metasurface optical element includes a substrate, a plurality of nanoantennas arranged on the substrate to modulate the incident light beam through transmission phase, and at least two nanoantennas Multiple nano-antenna arrays with different sizes are distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase.
  • the formed metasurface optical element can have collimation and diffraction functions at the same time, that is, the collimation element and the diffraction element are integrated, which effectively reduces the space occupied by the existing collimation and diffraction independent of two optical elements.
  • the alignment assembly of the collimation element and the diffraction element is canceled, the alignment error caused by it can be effectively reduced.
  • FIG. 1 is one of the structural schematic diagrams of a metasurface optical element provided in the embodiment of the present application
  • Fig. 2 is the second structural schematic diagram of a metasurface optical element provided by the embodiment of the present application.
  • Fig. 3 is the third structural schematic diagram of a metasurface optical element provided by the embodiment of the present application.
  • Fig. 4 is the fourth structural schematic diagram of a metasurface optical element provided by the embodiment of the present application.
  • Fig. 5 is the fifth structural schematic diagram of a metasurface optical element provided by the embodiment of the present application.
  • Fig. 6 is the sixth structural schematic diagram of a metasurface optical element provided by the embodiment of the present application.
  • FIG. 7 is a schematic structural diagram of a structured light projection module provided in an embodiment of the present application.
  • FIG. 8 is a schematic flowchart of a method for designing a metasurface optical element provided in an embodiment of the present application.
  • Icons 10 - light source; 20 - speckle image; 100 - metasurface optical element; 110 - substrate; 120 - nanometer antenna; 121 - first antenna; 122 - second antenna.
  • Some embodiments of the present application provide a metasurface optical element.
  • the phase of the light beam incident on the nano-antenna 120 wherein, the transmission phase refers to the phase adjustment achieved by the metasurface through the optical path difference generated during the transmission of electromagnetic waves.
  • the specific principle is based on the theory of the equivalent refractive index of the medium. Using parameters such as length, width, and height, the nano-antennas 120 are arranged with different duty ratios to change the corresponding equivalent refractive index to achieve different transmission phases and achieve the purpose of adjusting the phase of the outgoing light.
  • the parameters such as the shape and geometric dimensions of the nano-antenna 120 in the metasurface optical element 100 by carefully designing the parameters such as the shape and geometric dimensions of the nano-antenna 120 in the metasurface optical element 100, different structures with the highest and equal transmittance and phase distribution between 0 and 2 ⁇ can be selected. They are arranged at the same center-to-center distance to realize the metasurface optical element 100 with both collimation and beam splitting functions.
  • the plurality of nanoantennas 120 disposed on the surface of the substrate 110 of the metasurface optical element 100 at least two nanoantennas 120 have different sizes, so that the nanoantennas 120 can have different transmission phases, thereby enabling Phase modulation is performed on the light beam incident on the nano-antenna 120 .
  • the effect of achieving both collimation and diffraction functions is better.
  • multiple nanoantennas 120 can be distributed on the upper surface of the substrate 110 in the form of an array, and when multiple nanoantennas 120 are laid out on the upper surface of the substrate 110, the The transmission phase is arranged, and the transmission phase of each nano-antenna 120 can be the superposition of the collimation phase and the diffraction phase.
  • the collimation phase can be when the nano-antenna 120 realizes the collimation function alone
  • the diffraction phase can also be the diffraction phase when the nano-antenna 120 realizes the diffraction function alone
  • the transmission phase of the nano-antenna 120 can be the superposition of the alignment phase and the diffraction phase, thus obtaining If the transmission phase of the nano-antenna 120 is obtained, similarly, the respective transmission phases of the remaining nano-antennas 120 can be obtained, so that each nano-antenna 120 can be arranged on the surface of the substrate 110 according to the corresponding transmission phase of each nano-antenna 120, and more
  • the transmission phase distribution of each nano-antenna 120 is between 0 and 2 ⁇ , and the distance between the centers of two adjacent nano-antennas 120 is the same.
  • the formed metasurface optical element 100 can have collimation and diffraction functions at the same time, that is, collimation
  • the integration of the collimation element and the diffraction element effectively reduces the space occupied by the existing collimation and diffraction elements as two independent optical elements.
  • the alignment assembly of the collimation element and the diffraction element is canceled, the The resulting alignment error.
  • the metasurface optical element 100 With the difficulty of design and process manufacturing, after the superposition phases of multiple nano-antennas 120 obtained by superimposing the collimation phase and the diffraction phase (that is, the simulated phase in the subsequent method embodiment), it can be obtained according to the metasurface
  • the simulated phase is obtained by the above superposition, in order to further improve the effect of the metasurface optical element when the collimation and diffraction functions are simultaneously realized, it is also possible to slightly fine-tune the multiple nano-antennas 120 that have obtained the simulated phase to optimize the simulation results, thereby optimizing the superposition phase.
  • the specific optimization method may be performed through an algorithm, which is not limited in this application.
  • the metasurface optical element 100 of the present application is based on a metasurface structure when realizing collimation and diffraction functions, it can also effectively improve diffraction efficiency and uniformity.
  • the metasurface optical element 100 can be mass-produced by semiconductor chip technology, for example, templates can be made by photolithography such as electron beam or deep ultraviolet exposure, and then samples can be manufactured by dry etching and other processes.
  • the substrate 110 can protect the metasurface optical element 100 and isolate dust, etc., without adding an additional cover, so the overall diffraction efficiency of the module will not be reduced.
  • the surface on the other side of the transparent substrate 110 is a plane without optical elements, so other optical elements or film layers can be arranged on it to expand the performance of the metasurface optical element 100, for example, it can be coated on the other side of the glass substrate 110.
  • An ITO layer may also be plated on the surface of the transparent substrate 110 for protection.
  • the orthographic projection of the nano-antenna 120 on the substrate 110 can be set as a C4 rotationally symmetric figure, that is, the orthographic projection rotated 90 degrees around the center point can coincide with the original figure.
  • the nano-antenna 120 can be a cuboid structure, and its orthographic projection on the substrate 110 is a square.
  • the side length L of the square is equal, so that the length of the square on two adjacent sides is The isotropy presented in the direction, the side length L of the square can be 50nm to 500nm.
  • the nanoantenna 120 can be a cylindrical structure, and its orthographic projection on the substrate 110 is a circle. In this way, using the property that the diameters of the circles are equal, the circles in each It is isotropic in the diameter direction, and the diameter of the circle can be 50nm to 500nm.
  • the nanoantenna 120 may include two parts, one part is a first antenna 121, and the other part is a second antenna 122.
  • the orthographic projection of the first antenna 121 on the substrate is circular, and the second part is a circular antenna.
  • the orthographic projection of the two antennas 122 on the substrate is a square, wherein the first antenna 121 and the second antenna 122 may be randomly distributed on the substrate 110 .
  • the diameter of the circle may be 50nm to 500nm, and the side length L of the square may be 50nm to 500nm.
  • the metasurface optical element 100 of the present application can be made insensitive to the polarization of the incident light, which can solve the problem caused by the different polarization of the light source 10 caused by the traditional diffractive optical element.
  • the heights of two adjacent nano-antennas 120 are the same, and the pattern sizes of at least two nano-antennas 120 on the plane parallel to the substrate 110 are different. In this way, on the premise that a plurality of nano-columns have the same height, through Different sizes of the at least two nanocolumns form differences, so as to have different transmission phases, so as to realize the modulation of the incident light beam.
  • the height of the nanoantenna (direction perpendicular to the substrate 110 ) is greater than 300 nm, for example, between 300 nm and 1000 nm.
  • the center-to-center distance between two adjacent nanoantennas 120 is less than 600 nm. In this way, the performance of the metasurface optical element 100 can be effectively improved.
  • the shapes of two adjacent nanoantennas 120 disposed on the substrate 110 may be different.
  • the number of nano-antennas 120 with different sizes disposed on the substrate 110 is greater than or equal to 4, so that the obtained metasurface optical element 100 is at least equivalent to a fourth-order diffractive optical element, and has a higher diffraction efficiency.
  • the number of nano-antennas 120 with different sizes arranged on the substrate 110 may be greater than or equal to 8, so that the obtained metasurface optical element 100 is at least equivalent to an 8th-order diffractive optical element, have higher diffraction efficiency.
  • the substrate 110 can be a transparent substrate 110 , so that the formed metasurface optical element 100 can have good light transmission.
  • the material of the transparent substrate 110 may be quartz, glass or silicon oxide film.
  • the material of the nano-antenna 120 may be silicon, titanium oxide, aluminum oxide or silicon nitride. In some implementations, when the nano-antenna 120 is made of silicon, it can be monocrystalline silicon, amorphous silicon, or polycrystalline silicon.
  • nanoantenna 120 may be a sub-wavelength optical antenna.
  • simulations are performed on nano-antenna pillars of different sizes and heights to obtain their transmittance and transmission phase distribution diagrams.
  • the selection is mainly based on the two requirements that the transmittance of the same polarization is the highest and equal, and the transmission phase is evenly distributed among 0-2 ⁇ .
  • Another aspect of the present application provides a method for designing a metasurface optical element 100, as shown in FIG. 8 , the method may include:
  • the metasurface optical element 100 When designing the metasurface optical element 100, it can first be obtained that when the metasurface optical element 100 is used to simulate the collimation function separately (hereinafter referred to as the simulated collimation element for ease of distinction), a plurality of first simulated nanoantennas in the simulation The phase distribution on the substrate of the collimation element, that is, the collimation phase of each first simulated nano-antenna that can realize the collimation function.
  • S020 Obtain the diffraction phases corresponding to each of the multiple second simulated nanoantennas arranged on the base of the simulated diffraction element, wherein the multiple first simulated nanoantennas are in one-to-one correspondence with the multiple second simulated nanoantennas.
  • the metasurface optical element 100 When designing the metasurface optical element 100, it can also be obtained that when the metasurface optical element 100 is used to simulate the diffraction function separately (for ease of distinction, hereinafter referred to as the simulated diffraction element), a plurality of second simulated antennas simulate collimation The phase distribution on the base of the element, that is, the diffraction phase of each second simulated nano-antenna capable of realizing the diffraction function.
  • S010 and S020 in different implementation manners, they may be performed in different orders.
  • both the simulated collimation element and the simulated diffraction element are structures presented by the metasurface optical element 100 when a single collimation or diffraction function is simulated, therefore, the arrangement of multiple first simulated nano-antennas of the simulated collimation element on the substrate
  • the positions are the same, and the numbers of the first simulated nano-antennas and the second simulated nano-antennas are also the same.
  • the multiple first simulated nanoantennas can be The collimated phases of the simulated nano-antennas and the corresponding diffraction phases of the second simulated nano-antennas are superimposed according to the corresponding relationship, so as to obtain multiple simulated phases.
  • the simulated phase is obtained by the above superposition, in order to further improve the effect of the metasurface optical element 100 when the collimation and diffraction functions are simultaneously realized, it is also possible to slightly fine-tune the multiple nanoantennas 120 that have obtained the simulated phase to optimize the simulation results, thereby optimizing superimposed phase.
  • the specific optimization method may be performed through an algorithm, which is not limited in this application.
  • S040 Discrete multiple analog phases to obtain multiple discrete phases, wherein the number of multiple nano-antennas on the substrate of the metasurface optical element corresponds to the number of multiple discrete phases, and the transmission phases of multiple nano-antennas correspond to their respective The corresponding discrete phases are the same.
  • the simulated phase is discretized to obtain a discrete phase
  • the discrete phase is the same as the number of nano-antennas 120 required by the meta-surface optical element 100
  • each nano-antenna 120 is The corresponding matching has a discrete phase
  • the discrete phase is the transmission phase of the nano-antenna 120.
  • the optical transfer function can be used.
  • the optical transfer function of the combined system is the product of the optical transfer functions of the subsystems, that is, amplitude multiplication and phase superposition That's it.
  • the metasurface optical element 100 of the present application is based on a metasurface structure when realizing collimation and diffraction functions, it can also effectively improve diffraction efficiency and uniformity.
  • the metasurface optical element 100 can be mass-produced by semiconductor chip technology, for example, templates can be made by photolithography such as electron beam or deep ultraviolet exposure, and then samples can be manufactured by dry etching and other processes.
  • the metasurface optical element 100, the simulated collimation element and the simulated diffraction element are all manufactured based on the metasurface process, therefore, the respective manufacturing processes of the three are the same, and the manufacturing cost is the same, that is, the metasurface optical element 100 of the present application is integrated with collimation and At the same time as the diffraction function, it can also avoid increasing costs.
  • the simulated focal length of the simulated collimation element and the simulated focal length of two adjacent first simulated nano-antennas can be obtained first.
  • the center-to-center distance between two adjacent nano-antennas of the metasurface optical element is equal to the center-to-center distance between two adjacent first simulated nano-antennas.
  • the simulated angle of view of the simulated diffraction element can be obtained first, and the simulated angle of view can be obtained according to requirements. reasonable assumptions. Then, the corresponding diffraction phases of the multiple second simulated nano-antennas are obtained according to the simulated viewing angle and a preset algorithm.
  • the preset algorithm may be a Fourier iterative algorithm, a genetic algorithm, or the like.
  • the material of the metasurface optical element 100 can be determined according to the required working wavelength, including the material of the substrate 110 and the material of the nano-antenna 120, and the nano-antenna 120 can be selected from a material with a high refractive index. material.
  • the distance between the centers of two adjacent nano-antennas 120 on the substrate 110 of the metasurface optical element 100 can also be determined according to the working wavelength and the viewing angle, for example, set to be less than 600 nm.
  • the nano-antenna 120 After determining the distance between the centers of the nano-antenna 120, use electromagnetic simulation software to simulate the nano-antenna 120 whose orthographic shape is a circle, a square or a square with rounded corners, etc., which have a certain degree of isotropic C4 rotational symmetry. , by optimizing the size and height of the nanostructures, multiple nanocolumns with the same height but different shapes and/or sizes are selected. The quantity can be 2, 4, 8 etc. In some embodiments, firstly, simulate nano-antenna pillars of different sizes and heights to obtain their transmittance and transmission phase distribution diagrams. When selecting the nano-antenna 120 , the selection is mainly based on the two requirements that the same polarization transmittance is the highest and equal, and the transmission phase is evenly distributed among 0-2 ⁇ .
  • Some embodiments of the present application provide a structured light projection module.
  • the light beam emitted by the light source 10 enters the nano-antenna 120 of the metasurface optical element 100, and through the phase modulation of the nano-antenna 120, the incident light beam is collimated and diffracted before exiting the target area.
  • the light source 10 is a vertical cavity surface emitting laser, it can correspondingly project a speckle image 20 on the target area. Since the collimation and diffraction are integrated through the metasurface optical element 100, the overall volume of the structured light projection module is relatively small.
  • the light source 10 can also be an LD laser that generates a point source, the light source 10 is light of arbitrary polarization, and the wavelength is from the ultraviolet band to the terahertz band.
  • the present application provides a metasurface optical element and its design method, and a structured light projection module.
  • the metasurface optical element includes a substrate, a plurality of nanoantennas arranged on the substrate to modulate the incident light beam through transmission phase, and at least two nanoantennas Multiple nano-antenna arrays with different sizes are distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase.
  • the formed metasurface optical element can have collimation and diffraction functions at the same time, that is, the collimation element and the diffraction element are integrated, which effectively reduces the space occupied by the existing collimation and diffraction independent of two optical elements.
  • the alignment assembly of the collimation element and the diffraction element is canceled, the alignment error caused by it can be effectively reduced.
  • metasurface optical element, design method, and structured light projection module of the present application are reproducible and can be used in various industrial applications.
  • the metasurface optical element, design method, and structured light projection module of the present application can be used in the field of optical technology.

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Abstract

The present application provides a metasurface optical element, a design method and a structured light projection module, which relate to the technical field of optics. The metasurface optical element comprises: a substrate and a plurality of nanometer antennas which are provided on the substrate and which modulate incident beams by means of transmission phases. The size of at least two nanometer antennas are different, and the plurality of nanometer antennas are distributed in an array on the substrate. The distance between the centers of two adjacent nanometer antennas is the same, and the transmission phase of each nanometer antenna is the superimposition of a collimation phase and a diffraction phase. Therefore, the formed metasurface optical element may have collimation and diffraction functions at the same time, that is, a collimation element and a diffraction element are integrated. Space occupied by existing collimation and diffraction elements as two independent optical elements is effectively reduced; meanwhile, since the alignment assembly of the collimation element and diffraction element is omitted, alignment error caused by the alignment assembly may thus be effectively reduced.

Description

一种超表面光学元件及设计方法、结构光投影模组A metasurface optical element, design method, and structured light projection module
相关申请的交叉引用Cross References to Related Applications
本申请要求于2021年8月25日提交中国国家知识产权局的申请号为202110980167.9、名称为“一种超表面光学元件及设计方法、结构光投影模组”的中国专利申请和于2021年8月25日提交中国国家知识产权局的申请号为202110980751.4、名称为“一种超表面光学元件及设计方法、结构光投影模组”的中国专利申请的优先权,其全部内容通过引用结合在本申请中。This application requires a Chinese patent application with the application number 202110980167.9 and titled "A Metasurface Optical Element and Design Method, Structured Light Projection Module" submitted to the State Intellectual Property Office of China on August 25, 2021 and filed on August 2021 The priority of the Chinese patent application with the application number 202110980751.4 and titled "A Metasurface Optical Element and Design Method, Structured Light Projection Module" submitted to the State Intellectual Property Office of China on April 25, the entire contents of which are incorporated herein by reference Applying.
技术领域technical field
本申请涉及光学技术领域,具体而言,涉及一种超表面光学元件及设计方法、结构光投影模组。The present application relates to the field of optical technology, in particular, to a metasurface optical element, a design method, and a structured light projection module.
背景技术Background technique
结构光(structure light)是通过投射特定的图案至物体表面,并通过接收模组采集,根据物体造成的光信号的变化来计算物体的位置及深度信息,进而复原整个深度空间。该图案可被设计成条纹形态、规则点阵形态、网格形态、散斑形态、编码形态等,甚至更复杂形态的光形。随着光学技术的发展,结构光的应用范围越来越广泛,比如人脸识别、手势识别、投影仪、三维(Three-dimensional,3D)轮廓重现、深度测量、防伪辨识等。因此如何提供一种稳定发射结构光的投影模组成为人们研究的重点。Structured light projects a specific pattern onto the surface of an object, collects it through the receiving module, calculates the position and depth information of the object according to the change of the light signal caused by the object, and then restores the entire depth space. The pattern can be designed as stripes, regular lattices, grids, speckles, codes, etc., or even more complex light shapes. With the development of optical technology, the application range of structured light is more and more extensive, such as face recognition, gesture recognition, projector, three-dimensional (Three-dimensional, 3D) outline reconstruction, depth measurement, anti-counterfeiting identification, etc. Therefore, how to provide a projection module that stably emits structured light has become the focus of people's research.
相关技术中的结构光投影模组主要包括光源、准直透镜以及衍射光学元件。相关技术的结构光投影模组中,准直镜和衍射光学元件为分立元件,使得整个模组占用空间较大,对位精度较低。The structured light projection module in the related art mainly includes a light source, a collimator lens and a diffractive optical element. In the structured light projection module of the related art, the collimator mirror and the diffractive optical element are discrete components, so that the entire module takes up a large space and the alignment accuracy is low.
发明内容Contents of the invention
本申请提供了超表面光学元件及设计方法、结构光投影模组,以至少改善相关技术中的结构光投影模组占用空间较大,对位精度较低的问题。The present application provides a metasurface optical element, a design method, and a structured light projection module, so as to at least improve the problem that the structured light projection module in the related art occupies a large space and has low alignment accuracy.
为实现上述目的,本申请实施例采用的技术方案如下:In order to achieve the above purpose, the technical solution adopted in the embodiment of the present application is as follows:
在本申请的一些实施例中,提供一种超表面光学元件,该超表面光学元件可以包括基底,设置于基底上的多个通过传输相位调制入射光束的纳米天线,至少两个纳米天线的尺寸不同且多个纳米天线阵列分布于基底一侧,相邻两个纳米天线的中心间距相同,每个纳米天线的传输相位为准直相位和衍射相位的叠加。In some embodiments of the present application, a metasurface optical element is provided. The metasurface optical element may include a substrate, and a plurality of nanoantennas arranged on the substrate to modulate the incident light beam through transmission phase, at least two nanoantennas in size Different and multiple nano-antenna arrays are distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase.
可选地,纳米天线在基底上的正投影可以为C4旋转对称图形。Optionally, the orthographic projection of the nano-antenna on the substrate may be a C4 rotationally symmetric figure.
可选地,纳米天线的正投影可以为圆形。Optionally, the orthographic projection of the nano-antenna can be circular.
可选地,纳米天线的正投影可以为正方形。Optionally, the orthographic projection of the nano-antenna can be a square.
可选地,多个纳米天线可以包括第一天线和第二天线,第一天线在基底的正投影可以 为圆形,第二天线在基底的正投影可以为正方形。Optionally, the plurality of nano-antennas may include a first antenna and a second antenna, the orthographic projection of the first antenna on the substrate may be a circle, and the orthographic projection of the second antenna on the substrate may be a square.
可选地,当纳米天线为正方形时,正方形的边长可以为50nm至500nm。Optionally, when the nano-antenna is a square, the side length of the square may be 50nm to 500nm.
可选地,当纳米天线为圆形时,圆形的直径可以为50nm至500nm。Optionally, when the nano-antenna is circular, the diameter of the circular shape may be 50nm to 500nm.
可选地,当纳米天线为正方形时,正方形的边长可以为50nm至500nm,当纳米天线为圆形时,圆形的直径可以为50nm至500nm。Optionally, when the nano-antenna is a square, the side length of the square may be 50nm to 500nm, and when the nano-antenna is circular, the diameter of the circle may be 50nm to 500nm.
可选地,相邻两个纳米天线的中心间距可以为200nm至600nm。Optionally, the center-to-center distance between two adjacent nano-antennas may be 200nm to 600nm.
可选地,多个纳米天线的高度均可以大于300nm。Optionally, the heights of the multiple nano-antennas may be greater than 300nm.
可选地,多个纳米天线的高度均可以相同。Optionally, the heights of the multiple nano-antennas may be the same.
可选地,尺寸不同的纳米天线的个数可以大于或等于4,至少两个纳米天线的尺寸不同。Optionally, the number of nanoantennas with different sizes may be greater than or equal to 4, and at least two nanoantennas have different sizes.
可选地,基底可以为透明基底,透明基底的材质可以为石英、玻璃或氧化硅薄膜。Optionally, the substrate may be a transparent substrate, and the material of the transparent substrate may be quartz, glass or silicon oxide film.
可选地,纳米天线的材质可以是硅、氧化钛、氧化铝或氮化硅。Optionally, the material of the nano-antenna can be silicon, titanium oxide, aluminum oxide or silicon nitride.
此外,本申请的一些实施例提供一种超表面光学元件设计方法,方法可以包括:In addition, some embodiments of the present application provide a method for designing a metasurface optical element, the method may include:
使用超表面光学元件在实现单一准直功能时所呈现的模拟准直元件,获取基底上设置的多个第一模拟纳米天线各自对应的准直相位;Using the simulated collimation element presented by the metasurface optical element when realizing a single collimation function, obtaining the corresponding collimation phases of the plurality of first simulated nano-antennas arranged on the substrate;
使用超表面光学元件在实现单一衍射功能时所呈现的模拟衍射元件,获取基底上设置的多个第二模拟纳米天线各自对应的衍射相位,其中,多个第一模拟纳米天线与多个第二模拟纳米天线的数量一一对应;Using the simulated diffraction element presented by the metasurface optical element when realizing a single diffraction function, obtain the respective diffraction phases of multiple second simulated nanoantennas set on the substrate, wherein the multiple first simulated nanoantennas and multiple second simulated nanoantennas The number of simulated nanoantennas corresponds one by one;
将多个第一模拟纳米天线的准直相位与各自对应的第二模拟纳米天线的衍射相位叠加得到多个模拟相位;superimposing the alignment phases of multiple first simulated nanoantennas with the diffraction phases of their corresponding second simulated nanoantennas to obtain multiple simulated phases;
对多个模拟相位进行离散得到多个离散相位,其中,超表面光学元件基底上的多个纳米天线的数量与多个离散相位的数量一一对应,多个纳米天线的传输相位与各自对应的离散相位相同。Multiple analog phases are discretized to obtain multiple discrete phases, wherein the number of multiple nano-antennas on the base of the metasurface optical element corresponds to the number of multiple discrete phases, and the transmission phases of multiple nano-antennas correspond to their corresponding The discrete phases are the same.
可选地,在将多个所述第一模拟纳米天线的准直相位与各自对应的所述第二模拟纳米天线的衍射相位叠加得到所述多个模拟相位之后,可以对所述多个第一模拟纳米天线和所述多个第二模拟纳米天线进行微调以优化模拟结果,从而优化叠加相位。Optionally, after the multiple simulated phases are obtained by superimposing the alignment phases of the multiple first simulated nanoantennas with the diffraction phases of the corresponding second simulated nanoantennas, the multiple first simulated nanoantennas can be A simulated nano-antenna and the plurality of second simulated nano-antennas are fine-tuned to optimize the simulation results, thereby optimizing the superposition phase.
可选地,获取基底上设置的多个第一模拟纳米天线各自对应的准直相位可以包括:Optionally, obtaining the corresponding collimation phases of the plurality of first simulated nanoantennas arranged on the substrate may include:
获取模拟准直元件的模拟焦距和相邻两个第一模拟纳米天线的中心间距;Obtaining the simulated focal length of the simulated collimation element and the center-to-center distance of two adjacent first simulated nano-antennas;
根据模拟焦距、透镜聚焦方程和相邻两个第一模拟纳米天线的中心间距得出多个第一模拟纳米天线各自对应的准直相位。The collimation phases corresponding to each of the plurality of first simulated nano-antennas are obtained according to the simulated focal length, the lens focusing equation and the distance between the centers of two adjacent first simulated nano-antennas.
可选地,相邻两个第一模拟纳米天线的中心间距可以是根据第一模拟纳米天线的预设工作波长和所要实现的视场角确定的。Optionally, the center-to-center distance between two adjacent first simulated nanoantennas may be determined according to the preset working wavelength of the first simulated nanoantennas and the field angle to be realized.
可选地,获取基底上设置的多个第二模拟纳米天线各自对应的衍射相位可以包括:Optionally, obtaining the respective diffraction phases corresponding to the plurality of second simulated nanoantennas arranged on the substrate may include:
获取模拟衍射元件的模拟视场角;Obtain the simulated viewing angle of the simulated diffraction element;
根据模拟视场角和预设算法得出多个第二模拟纳米天线各自对应的衍射相位。The diffraction phases corresponding to each of the plurality of second simulated nano-antennas are obtained according to the simulated viewing angle and a preset algorithm.
可选地,在获取基底上设置的多个第一模拟纳米天线各自对应的准直相位之前,可以根据所需要的工作波长确定超表面光学元件的材质。Optionally, before obtaining the collimation phases corresponding to the plurality of first simulated nano-antennas arranged on the substrate, the material of the metasurface optical element may be determined according to the required working wavelength.
本申请的另一些实施例提供一种结构光投影模组,该结构光投影模组可以包括光源以及上述任一种的超表面光学元件,光源位于超表面光学元件的入光侧,超表面光学元件用于对光源出射的光束进行准直和衍射。Other embodiments of the present application provide a structured light projection module. The structured light projection module may include a light source and any of the above-mentioned metasurface optical elements. The light source is located on the light incident side of the metasurface optical element. The metasurface optics The element is used to collimate and diffract the light beam emitted by the light source.
本申请的有益效果至少包括:The beneficial effects of the application at least include:
本申请提供了一种超表面光学元件及设计方法、结构光投影模组,超表面光学元件包括基底,设置于基底上的多个通过传输相位调制入射光束的纳米天线,至少两个纳米天线的尺寸不同且多个纳米天线阵列分布于基底一侧,相邻两个纳米天线的中心间距相同,每个纳米天线的传输相位为准直相位和衍射相位的叠加。如此,便可以使得形成的超表面光学元件能够同时具有准直和衍射功能,即将准直元件和衍射元件进行集成,有效降低了现有准直和衍射独立为两个光学元件所占用的空间,同时,由于取消了准直元件和衍射元件的对位装配,因此,能够有效降低其所导致的对位误差。The present application provides a metasurface optical element and its design method, and a structured light projection module. The metasurface optical element includes a substrate, a plurality of nanoantennas arranged on the substrate to modulate the incident light beam through transmission phase, and at least two nanoantennas Multiple nano-antenna arrays with different sizes are distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase. In this way, the formed metasurface optical element can have collimation and diffraction functions at the same time, that is, the collimation element and the diffraction element are integrated, which effectively reduces the space occupied by the existing collimation and diffraction independent of two optical elements. At the same time, since the alignment assembly of the collimation element and the diffraction element is canceled, the alignment error caused by it can be effectively reduced.
附图说明Description of drawings
为了更清楚地说明本申请实施例的技术方案,下面将对实施例中所需要使用的附图作简单地介绍,应当理解,以下附图仅示出了本申请的某些实施例,因此不应被看作是对范围的限定,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他相关的附图。In order to more clearly illustrate the technical solutions of the embodiments of the present application, the following will briefly introduce the accompanying drawings used in the embodiments. It should be understood that the following drawings only show some embodiments of the present application, so It should be regarded as a limitation on the scope, and those skilled in the art can also obtain other related drawings based on these drawings without creative work.
图1为本申请实施例提供的一种超表面光学元件的结构示意图之一;FIG. 1 is one of the structural schematic diagrams of a metasurface optical element provided in the embodiment of the present application;
图2为本申请实施例提供的一种超表面光学元件的结构示意图之二;Fig. 2 is the second structural schematic diagram of a metasurface optical element provided by the embodiment of the present application;
图3为本申请实施例提供的一种超表面光学元件的结构示意图之三;Fig. 3 is the third structural schematic diagram of a metasurface optical element provided by the embodiment of the present application;
图4为本申请实施例提供的一种超表面光学元件的结构示意图之四;Fig. 4 is the fourth structural schematic diagram of a metasurface optical element provided by the embodiment of the present application;
图5为本申请实施例提供的一种超表面光学元件的结构示意图之五;Fig. 5 is the fifth structural schematic diagram of a metasurface optical element provided by the embodiment of the present application;
图6为本申请实施例提供的一种超表面光学元件的结构示意图之六;Fig. 6 is the sixth structural schematic diagram of a metasurface optical element provided by the embodiment of the present application;
图7为本申请实施例提供的一种结构光投影模组的结构示意图;FIG. 7 is a schematic structural diagram of a structured light projection module provided in an embodiment of the present application;
图8为本申请实施例提供的一种超表面光学元件设计方法的流程示意图。FIG. 8 is a schematic flowchart of a method for designing a metasurface optical element provided in an embodiment of the present application.
图标:10-光源;20-散斑点图像;100-超表面光学元件;110-基底;120-纳米天线;121-第一天线;122-第二天线。Icons: 10 - light source; 20 - speckle image; 100 - metasurface optical element; 110 - substrate; 120 - nanometer antenna; 121 - first antenna; 122 - second antenna.
具体实施方式Detailed ways
为使本申请实施例的目的、技术方案和优点更加清楚,下面将结合本申请实施例中的附图,对本申请实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本申请一部分实施例,而不是全部的实施例。通常在此处附图中描述和示出的本申请实施例的组件可以以各种不同的配置来布置和设计。In order to make the purposes, technical solutions and advantages of the embodiments of the present application clearer, the technical solutions in the embodiments of the present application will be clearly and completely described below in conjunction with the drawings in the embodiments of the present application. Obviously, the described embodiments It is a part of the embodiments of this application, not all of them. The components of the embodiments of the application generally described and illustrated in the figures herein may be arranged and designed in a variety of different configurations.
因此,以下对在附图中提供的本申请的实施例的详细描述并非旨在限制要求保护的本申请的范围,而是仅仅表示本申请的选定实施例。需要说明的是,在不冲突的情况下,本申请的实施例中的各个特征可以相互结合,结合后的实施例依然在本申请的保护范围内。Accordingly, the following detailed description of the embodiments of the application provided in the accompanying drawings is not intended to limit the scope of the claimed application, but merely represents selected embodiments of the application. It should be noted that, in the case of no conflict, various features in the embodiments of the present application may be combined with each other, and the combined embodiments are still within the protection scope of the present application.
应注意到:相似的标号和字母在下面的附图中表示类似项,因此,一旦某一项在一个附图中被定义,则在随后的附图中不需要对其进行进一步定义和解释。It should be noted that like numerals and letters denote similar items in the following figures, therefore, once an item is defined in one figure, it does not require further definition and explanation in subsequent figures.
在本申请的描述中,需要说明的是,术语“中心”、“上”、“下”、“左”、“右”、“竖直”、“水平”、“内”、“外”等指示的方位或位置关系为基于附图所示的方位或位置关系,或者是该申请产品使用时惯常摆放的方位或位置关系,仅是为了便于描述本申请和简化描述,而不是指示或暗示所指的装置或元件必须具有特定的方位、以特定的方位构造和操作,因此不能理解为对本申请的限制。此外,术语“第一”、“第二”、“第三”等仅用于区分描述,而不能理解为指示或暗示相对重要性。In the description of this application, it should be noted that the terms "center", "upper", "lower", "left", "right", "vertical", "horizontal", "inner", "outer" etc. The indicated orientation or positional relationship is based on the orientation or positional relationship shown in the drawings, or the orientation or positional relationship that is usually placed when the application product is used, and is only for the convenience of describing the application and simplifying the description, rather than indicating or implying References to devices or elements must have a particular orientation, be constructed, and operate in a particular orientation and therefore should not be construed as limiting the application. In addition, the terms "first", "second", "third", etc. are only used for distinguishing descriptions, and should not be construed as indicating or implying relative importance.
本申请的一些实施例提供一种超表面光学元件,如图1所示,超表面光学元件可以包括基底110和设置于基底110上的多个纳米天线120,多个纳米天线120通过传输相位调制入射纳米天线120的光束的相位,其中,传输相位指超表面通过电磁波在传输过程中产生的光程差来实现相位调控,其具体原理基于介质等效折射率理论,通过调节纳米天线120结构的长度、宽度、高度等参数,利用不同占空比排列纳米天线120改变对应等效折射率,实现不同的传输相位,达到调控出射光的相位的目的。Some embodiments of the present application provide a metasurface optical element. As shown in FIG. The phase of the light beam incident on the nano-antenna 120, wherein, the transmission phase refers to the phase adjustment achieved by the metasurface through the optical path difference generated during the transmission of electromagnetic waves. The specific principle is based on the theory of the equivalent refractive index of the medium. Using parameters such as length, width, and height, the nano-antennas 120 are arranged with different duty ratios to change the corresponding equivalent refractive index to achieve different transmission phases and achieve the purpose of adjusting the phase of the outgoing light.
基于这种传输相位的原理,可以通过精心设计超表面光学元件100中纳米天线120的形状、几何尺寸等参数,挑选出具有透过率最高且相等,相位分布在0~2π的不同结构,将其以相同的中心间距排列,能够实现同时具有准直和分束功能的超表面光学元件100。在一些实施方式中,设置于超表面光学元件100的基底110表面的多个纳米天线120中,至少两个纳米天线120的尺寸不同,如此,能够使得纳米天线120具有不同的传输相位,进而能够对入射纳米天线120的光束进行相位调制。当然,随着尺寸不同的纳米天线的数量增多,其同时实现准直和衍射功能的效果越好。Based on the principle of this transmission phase, by carefully designing the parameters such as the shape and geometric dimensions of the nano-antenna 120 in the metasurface optical element 100, different structures with the highest and equal transmittance and phase distribution between 0 and 2π can be selected. They are arranged at the same center-to-center distance to realize the metasurface optical element 100 with both collimation and beam splitting functions. In some embodiments, among the plurality of nanoantennas 120 disposed on the surface of the substrate 110 of the metasurface optical element 100, at least two nanoantennas 120 have different sizes, so that the nanoantennas 120 can have different transmission phases, thereby enabling Phase modulation is performed on the light beam incident on the nano-antenna 120 . Of course, as the number of nano-antennas with different sizes increases, the effect of achieving both collimation and diffraction functions is better.
如图1和图4所示,多个纳米天线120可以以阵列的形式分布于基底110的上表面,多个纳米天线120在基底110的上表面进行布设时,可以根据每一个纳米天线120的传输相位进行布设,每一个纳米天线120的传输相位可以是准直相位和衍射相位的叠加,以一个纳米天线120为例进行说明:准直相位可以是该纳米天线120在单独实现准直功能时的 准直相位,同理,衍射相位也同样可以是该纳米天线120单独实现衍射功能时的衍射相位,那么,该纳米天线120的传输相位就可以是准直相位和衍射相位的叠加,从而得出该纳米天线120的传输相位,同理,便可以得出剩余纳米天线120各自的传输相位,如此,便可以按照每个纳米天线120各自所对应的传输相位在基底110表面进行布设,且多个纳米天线120的传输相位分布在0~2π之间,相邻两个纳米天线120的中心间距相同,如此,便可以使得形成的超表面光学元件100能够同时具有准直和衍射功能,即将准直元件和衍射元件进行集成,有效降低了现有准直和衍射独立为两个光学元件所占用的空间,同时,由于取消了准直元件和衍射元件的对位装配,因此,能够有效降低其所导致的对位误差。As shown in Figures 1 and 4, multiple nanoantennas 120 can be distributed on the upper surface of the substrate 110 in the form of an array, and when multiple nanoantennas 120 are laid out on the upper surface of the substrate 110, the The transmission phase is arranged, and the transmission phase of each nano-antenna 120 can be the superposition of the collimation phase and the diffraction phase. Taking a nano-antenna 120 as an example: the collimation phase can be when the nano-antenna 120 realizes the collimation function alone In the same way, the diffraction phase can also be the diffraction phase when the nano-antenna 120 realizes the diffraction function alone, then, the transmission phase of the nano-antenna 120 can be the superposition of the alignment phase and the diffraction phase, thus obtaining If the transmission phase of the nano-antenna 120 is obtained, similarly, the respective transmission phases of the remaining nano-antennas 120 can be obtained, so that each nano-antenna 120 can be arranged on the surface of the substrate 110 according to the corresponding transmission phase of each nano-antenna 120, and more The transmission phase distribution of each nano-antenna 120 is between 0 and 2π, and the distance between the centers of two adjacent nano-antennas 120 is the same. In this way, the formed metasurface optical element 100 can have collimation and diffraction functions at the same time, that is, collimation The integration of the collimation element and the diffraction element effectively reduces the space occupied by the existing collimation and diffraction elements as two independent optical elements. At the same time, since the alignment assembly of the collimation element and the diffraction element is canceled, the The resulting alignment error.
需要说明的是,考虑到设计以及工艺制造难度,在通过叠加准直相位和衍射相位后得到的多个纳米天线120的叠加相位(即后续方法实施例中的模拟相位)后,可以根据超表面光学元件100所需的纳米天线120个数,对模拟相位进行离散,得到离散相位,离散相位与超表面光学元件100所需的纳米天线120的个数相同,每个纳米天线120则被对应匹配具有一个离散相位,该离散相位即为该纳米天线120的传输相位,对具有传输相位的纳米天线120进行排布,即可得到具有准直和衍射功能的超表面光学元件100。It should be noted that, considering the difficulty of design and process manufacturing, after the superposition phases of multiple nano-antennas 120 obtained by superimposing the collimation phase and the diffraction phase (that is, the simulated phase in the subsequent method embodiment), it can be obtained according to the metasurface The number of nano-antennas 120 required by the optical element 100, the analog phase is discretized to obtain a discrete phase, the discrete phase is the same as the number of nano-antennas 120 required by the metasurface optical element 100, and each nano-antenna 120 is matched accordingly It has a discrete phase, and the discrete phase is the transmission phase of the nano-antenna 120. By arranging the nano-antennas 120 with the transmission phase, the metasurface optical element 100 with collimation and diffraction functions can be obtained.
在上述叠加得到模拟相位后,为了进一步的提高超表面光学元件同时实现准直和衍射功能时的效果,还可以对多个得到模拟相位的纳米天线120进行小幅微调以优化模拟结果,从而优化叠加相位。具体的优化方式可以是通过算法等进行,本申请对其不做限制。After the simulated phase is obtained by the above superposition, in order to further improve the effect of the metasurface optical element when the collimation and diffraction functions are simultaneously realized, it is also possible to slightly fine-tune the multiple nano-antennas 120 that have obtained the simulated phase to optimize the simulation results, thereby optimizing the superposition phase. The specific optimization method may be performed through an algorithm, which is not limited in this application.
此外,由于本申请超表面光学元件100在实现准直和衍射功能时,是基于超表面结构,因此,还可以有效提高衍射效率和均一性。同时,从制造工艺来讲,该超表面光学元件100可以通过半导体芯片工艺批量制造,例如可以通过电子束或者深紫外曝光等光刻方式制作模板,然后通过干法刻蚀等工艺制造样品。In addition, since the metasurface optical element 100 of the present application is based on a metasurface structure when realizing collimation and diffraction functions, it can also effectively improve diffraction efficiency and uniformity. At the same time, in terms of manufacturing process, the metasurface optical element 100 can be mass-produced by semiconductor chip technology, for example, templates can be made by photolithography such as electron beam or deep ultraviolet exposure, and then samples can be manufactured by dry etching and other processes.
实际使用中,基底110可以起到保护超表面光学元件100以及隔离灰尘等作用,不需要再额外增加盖板,因此不会降低模组整体的衍射效率。此外,透明基底110的另一侧表面为没有设置光学元件的平面,因此可以在其上设置其他光学元件或者膜层来扩展超表面光学元件100的性能,比如可以在玻璃基底110另一侧镀上抗反膜或者耐磨层等。也可以在透明基底110表面镀上ITO层,起到保护作用。In actual use, the substrate 110 can protect the metasurface optical element 100 and isolate dust, etc., without adding an additional cover, so the overall diffraction efficiency of the module will not be reduced. In addition, the surface on the other side of the transparent substrate 110 is a plane without optical elements, so other optical elements or film layers can be arranged on it to expand the performance of the metasurface optical element 100, for example, it can be coated on the other side of the glass substrate 110. Anti-reflective film or wear-resistant layer, etc. An ITO layer may also be plated on the surface of the transparent substrate 110 for protection.
可选地,可以将纳米天线120在基底110上的正投影设置为C4旋转对称图形,即正投影绕中心点旋转90度可以与原图形重合。Optionally, the orthographic projection of the nano-antenna 120 on the substrate 110 can be set as a C4 rotationally symmetric figure, that is, the orthographic projection rotated 90 degrees around the center point can coincide with the original figure.
在一些实施方式中,如图2和图5所示,纳米天线120可以是长方体结构,其在基底110上的正投影为正方形,如此,利用正方形边长L相等,使得正方形在相邻两边长方向上所呈现的各向同性,正方形的边长L可以为50nm至500nm。In some embodiments, as shown in FIG. 2 and FIG. 5 , the nano-antenna 120 can be a cuboid structure, and its orthographic projection on the substrate 110 is a square. In this way, the side length L of the square is equal, so that the length of the square on two adjacent sides is The isotropy presented in the direction, the side length L of the square can be 50nm to 500nm.
在一些实施方式中,如图3和图4所示,纳米天线120可以是圆柱结构,其在基底110 上的正投影为圆形,如此,利用圆形直径相等的特性,使得圆形在各个直径方向上所呈现出各向同性,圆形的直径可以为50nm至500nm。In some implementations, as shown in FIG. 3 and FIG. 4 , the nanoantenna 120 can be a cylindrical structure, and its orthographic projection on the substrate 110 is a circle. In this way, using the property that the diameters of the circles are equal, the circles in each It is isotropic in the diameter direction, and the diameter of the circle can be 50nm to 500nm.
在一些实施方式中,如图6所示,纳米天线120可以包括两部分,一部分为第一天线121,另一部分为第二天线122,第一天线121在基底上的正投影为圆形,第二天线122在基底上的正投影为正方形,其中,第一天线121和第二天线122可以是以随机分布的形式设置在基底110上。圆形的直径可以为50nm至500nm,正方形的边长L可以为50nm至500nm。In some implementations, as shown in FIG. 6 , the nanoantenna 120 may include two parts, one part is a first antenna 121, and the other part is a second antenna 122. The orthographic projection of the first antenna 121 on the substrate is circular, and the second part is a circular antenna. The orthographic projection of the two antennas 122 on the substrate is a square, wherein the first antenna 121 and the second antenna 122 may be randomly distributed on the substrate 110 . The diameter of the circle may be 50nm to 500nm, and the side length L of the square may be 50nm to 500nm.
在上述实施例中,由于纳米天线120均具有一定程度的各项同性,因此可以使得本申请的超表面光学元件100对入射光的偏振不敏感,能够解决传统衍射光学元件因为光源10偏振不同引入的分束不均匀的问题。In the above-mentioned embodiments, since the nano-antennas 120 have a certain degree of isotropy, the metasurface optical element 100 of the present application can be made insensitive to the polarization of the incident light, which can solve the problem caused by the different polarization of the light source 10 caused by the traditional diffractive optical element. The problem of uneven beam splitting.
在一些实施方式中,相邻两个纳米天线120的高度相同,至少两个纳米天线120在平行基底110的平面上的图形尺寸不同,如此,能够在多个纳米柱高度相同的前提下,通过至少两纳米柱的尺寸不同形成差异化,从而具备不同的传输相位,以此实现对入射光束的调制。In some embodiments, the heights of two adjacent nano-antennas 120 are the same, and the pattern sizes of at least two nano-antennas 120 on the plane parallel to the substrate 110 are different. In this way, on the premise that a plurality of nano-columns have the same height, through Different sizes of the at least two nanocolumns form differences, so as to have different transmission phases, so as to realize the modulation of the incident light beam.
在一些实施方式中,纳米天线的高(垂直基底110的方向)大于300nm,例如在300nm至1000nm之间。In some embodiments, the height of the nanoantenna (direction perpendicular to the substrate 110 ) is greater than 300 nm, for example, between 300 nm and 1000 nm.
在一些实施方式中,相邻两个纳米天线120的中心间距小于600nm。如此,能够有效提高超表面光学元件100的性能。In some embodiments, the center-to-center distance between two adjacent nanoantennas 120 is less than 600 nm. In this way, the performance of the metasurface optical element 100 can be effectively improved.
在一些实施方式中,设置于基底110上的相邻两个纳米天线120的形状可以均不相同。In some embodiments, the shapes of two adjacent nanoantennas 120 disposed on the substrate 110 may be different.
在一些实施方式中,设置于基底110上的尺寸不同的纳米天线120的个数大于或等于4,如此,得到的超表面光学元件100至少相当于4阶的衍射光学元件,具有较高的衍射效率。当然,在其它实施方式中,还可以是设置于基底110上的尺寸不同的纳米天线120的个数大于或等于8,如此,得到的超表面光学元件100至少相当于8阶的衍射光学元件,具有更高的衍射效率。In some embodiments, the number of nano-antennas 120 with different sizes disposed on the substrate 110 is greater than or equal to 4, so that the obtained metasurface optical element 100 is at least equivalent to a fourth-order diffractive optical element, and has a higher diffraction efficiency. Of course, in other embodiments, the number of nano-antennas 120 with different sizes arranged on the substrate 110 may be greater than or equal to 8, so that the obtained metasurface optical element 100 is at least equivalent to an 8th-order diffractive optical element, have higher diffraction efficiency.
在一些实施方式中,基底110可以为透明基底110,如此,能够使得形成的超表面光学元件100具备良好的透光性。在一些实施方式中,透明基底110的材质可以是石英、玻璃或氧化硅薄膜。In some embodiments, the substrate 110 can be a transparent substrate 110 , so that the formed metasurface optical element 100 can have good light transmission. In some implementations, the material of the transparent substrate 110 may be quartz, glass or silicon oxide film.
在一些实施方式中,纳米天线120的材质可以是硅、氧化钛、氧化铝或氮化硅。在一些实施方式中,纳米天线120的是硅时,可以是单晶硅、非晶硅或多晶硅等。In some embodiments, the material of the nano-antenna 120 may be silicon, titanium oxide, aluminum oxide or silicon nitride. In some implementations, when the nano-antenna 120 is made of silicon, it can be monocrystalline silicon, amorphous silicon, or polycrystalline silicon.
在一些实施方式中,纳米天线120的可以是亚波长光学天线。In some embodiments, nanoantenna 120 may be a sub-wavelength optical antenna.
在一些实施方式中,首先对不同尺寸和高度的纳米天线柱进行模拟仿真,得到它们的透过率和传输相位分布图。在选取纳米天线120时,主要根据相同偏振透过率最高且相等, 传输相位均匀分布在0~2π之中两个要求进行选取。In some embodiments, firstly, simulations are performed on nano-antenna pillars of different sizes and heights to obtain their transmittance and transmission phase distribution diagrams. When selecting the nano-antenna 120 , the selection is mainly based on the two requirements that the transmittance of the same polarization is the highest and equal, and the transmission phase is evenly distributed among 0-2π.
本申请的另一方面,提供一种超表面光学元件100设计方法,如图8所示,方法可以包括:Another aspect of the present application provides a method for designing a metasurface optical element 100, as shown in FIG. 8 , the method may include:
S010:获取模拟准直元件基底上设置的多个第一模拟纳米天线各自对应的准直相位。S010: Obtain collimation phases corresponding to each of the plurality of first simulated nano-antennas disposed on the substrate of the simulated collimation element.
在对超表面光学元件100进行设计时,可以先获取通过超表面光学元件100在模拟单独实现准直功能(为便于区分以下称为模拟准直元件)时,多个第一模拟纳米天线在模拟准直元件的基底上的相位分布,也即每一个第一模拟纳米天线各自能够实现准直功能的准直相位。When designing the metasurface optical element 100, it can first be obtained that when the metasurface optical element 100 is used to simulate the collimation function separately (hereinafter referred to as the simulated collimation element for ease of distinction), a plurality of first simulated nanoantennas in the simulation The phase distribution on the substrate of the collimation element, that is, the collimation phase of each first simulated nano-antenna that can realize the collimation function.
S020:获取模拟衍射元件基底上设置的多个第二模拟纳米天线各自对应的衍射相位,其中,多个第一模拟纳米天线与多个第二模拟纳米天线的数量一一对应。S020: Obtain the diffraction phases corresponding to each of the multiple second simulated nanoantennas arranged on the base of the simulated diffraction element, wherein the multiple first simulated nanoantennas are in one-to-one correspondence with the multiple second simulated nanoantennas.
在对超表面光学元件100进行设计时,还可以获取通过超表面光学元件100在模拟单独实现衍射功能(为便于区分,以下称为模拟衍射元件)时,多个第二模拟天线在模拟准直元件的基底上的相位分布,也即每一个第二模拟纳米天线各自能够实现衍射功能的衍射相位。执行S010和S020时,在不同实施方式中,可以以不同的顺序进行。When designing the metasurface optical element 100, it can also be obtained that when the metasurface optical element 100 is used to simulate the diffraction function separately (for ease of distinction, hereinafter referred to as the simulated diffraction element), a plurality of second simulated antennas simulate collimation The phase distribution on the base of the element, that is, the diffraction phase of each second simulated nano-antenna capable of realizing the diffraction function. When executing S010 and S020, in different implementation manners, they may be performed in different orders.
由于模拟准直元件和模拟衍射元件均是由超表面光学元件100模拟实现单一准直或衍射功能时所呈现的结构,因此,模拟准直元件的多个第一模拟纳米天线在基底上的布设和模拟衍射元件的多个第二模拟纳米天线在基底上的布设呈一一对应的状态,即每一个第一模拟纳米天线都和其所对应的一个第二模拟纳米天线的基底上的所处位置相同,且第一模拟纳米天线和第二模拟纳米天线的数量也相同。Since both the simulated collimation element and the simulated diffraction element are structures presented by the metasurface optical element 100 when a single collimation or diffraction function is simulated, therefore, the arrangement of multiple first simulated nano-antennas of the simulated collimation element on the substrate There is a one-to-one correspondence with the layout of multiple second simulated nanoantennas of simulated diffraction elements on the substrate, that is, each first simulated nanoantenna is located on the substrate of a corresponding second simulated nanoantenna. The positions are the same, and the numbers of the first simulated nano-antennas and the second simulated nano-antennas are also the same.
S030:将多个第一模拟纳米天线的准直相位与各自对应的第二模拟纳米天线的衍射相位叠加得到多个模拟相位。S030: Superimpose the collimation phases of the multiple first simulated nanoantennas with the diffraction phases of the respective corresponding second simulated nanoantennas to obtain multiple simulated phases.
通过S010和S020获取到模拟准直元件上的多个第一模拟纳米天线各自的准直相位和模拟衍射元件上的多个第二模拟纳米天线各自的衍射相位后,便可以将多个第一模拟纳米天线的准直相位和各自所对应的第二模拟纳米天线的衍射相位按照对应关系进行叠加,从而得到多个模拟相位。After the respective collimation phases of the multiple first simulated nanoantennas on the simulated collimation element and the respective diffraction phases of the multiple second simulated nanoantennas on the simulated diffraction element are obtained through S010 and S020, the multiple first simulated nanoantennas can be The collimated phases of the simulated nano-antennas and the corresponding diffraction phases of the second simulated nano-antennas are superimposed according to the corresponding relationship, so as to obtain multiple simulated phases.
在上述叠加得到模拟相位后,为了进一步的提高超表面光学元件100同时实现准直和衍射功能时的效果,还可以对多个得到模拟相位的纳米天线120进行小幅微调以优化模拟结果,从而优化叠加相位。具体的优化方式可以是通过算法等进行,本申请对其不做限制。After the simulated phase is obtained by the above superposition, in order to further improve the effect of the metasurface optical element 100 when the collimation and diffraction functions are simultaneously realized, it is also possible to slightly fine-tune the multiple nanoantennas 120 that have obtained the simulated phase to optimize the simulation results, thereby optimizing superimposed phase. The specific optimization method may be performed through an algorithm, which is not limited in this application.
S040:对多个模拟相位进行离散得到多个离散相位,其中,超表面光学元件基底上的多个纳米天线的数量与多个离散相位的数量一一对应,多个纳米天线的传输相位与各自对应的离散相位相同。S040: Discrete multiple analog phases to obtain multiple discrete phases, wherein the number of multiple nano-antennas on the substrate of the metasurface optical element corresponds to the number of multiple discrete phases, and the transmission phases of multiple nano-antennas correspond to their respective The corresponding discrete phases are the same.
根据超表面光学元件100所需的纳米天线120个数,对模拟相位进行离散,得到离散 相位,离散相位与超表面光学元件100所需的纳米天线120的个数相同,每个纳米天线120则被对应匹配具有一个离散相位,该离散相位即为该纳米天线120的传输相位,对具有传输相位的纳米天线120进行排布,即可得到具有准直和衍射功能的超构表面光学元件。如此,便可以使得布设后的超表面光学元件100同时实现准直和衍射的功能,即将准直和衍射进行集成。需要说明的是,在实现准直和衍射功能的集成时,可以通过光学传递函数,若干成像系统串联时,合成系统的光学传递函数是子系统光学传递函数的乘积,即振幅相乘,相位叠加即可。According to the number of nano-antennas 120 required by the metasurface optical element 100, the simulated phase is discretized to obtain a discrete phase, the discrete phase is the same as the number of nano-antennas 120 required by the meta-surface optical element 100, and each nano-antenna 120 is The corresponding matching has a discrete phase, and the discrete phase is the transmission phase of the nano-antenna 120. By arranging the nano-antennas 120 with the transmission phase, a metasurface optical element with collimation and diffraction functions can be obtained. In this way, the arranged metasurface optical element 100 can realize the functions of collimation and diffraction at the same time, that is, integrate collimation and diffraction. It should be noted that when realizing the integration of collimation and diffraction functions, the optical transfer function can be used. When several imaging systems are connected in series, the optical transfer function of the combined system is the product of the optical transfer functions of the subsystems, that is, amplitude multiplication and phase superposition That's it.
此外,由于本申请超表面光学元件100在实现准直和衍射功能时,是基于超表面结构,因此,还可以有效提高衍射效率和均一性。同时,从制造工艺来讲,该超表面光学元件100可以通过半导体芯片工艺批量制造,例如可以通过电子束或者深紫外曝光等光刻方式制作模板,然后通过干法刻蚀等工艺制造样品。其中超表面光学元件100、模拟准直元件和模拟衍射元件均基于超表面工艺制造,因此,三者各自的制程相同,制造成本相同,即本申请的超表面光学元件100在集成有准直和衍射功能的同时,还能够避免增加成本。In addition, since the metasurface optical element 100 of the present application is based on a metasurface structure when realizing collimation and diffraction functions, it can also effectively improve diffraction efficiency and uniformity. At the same time, in terms of manufacturing process, the metasurface optical element 100 can be mass-produced by semiconductor chip technology, for example, templates can be made by photolithography such as electron beam or deep ultraviolet exposure, and then samples can be manufactured by dry etching and other processes. Wherein the metasurface optical element 100, the simulated collimation element and the simulated diffraction element are all manufactured based on the metasurface process, therefore, the respective manufacturing processes of the three are the same, and the manufacturing cost is the same, that is, the metasurface optical element 100 of the present application is integrated with collimation and At the same time as the diffraction function, it can also avoid increasing costs.
在一些实施方式中,通过S010获取模拟准直元件基底上设置的多个第一模拟纳米天线各自对应的准直相位时,可以先获取模拟准直元件的模拟焦距和相邻两个第一模拟纳米天线的中心间距,其中,模拟焦距可以预设,相邻两个第一模拟纳米天线的中心间距相同,且相邻两个第一模拟纳米天线的中心间距可以根据第一模拟纳米天线的预设工作波长和所要实现的视场角确定。然后根据模拟焦距、透镜聚焦方程和相邻两个第一模拟纳米天线的中心间距得出多个第一模拟纳米天线各自对应的准直相位。需要说明的是,超表面光学元件的相邻两个纳米天线的中心间距与相邻两个第一模拟纳米天线的中心间距相等。In some implementations, when the collimation phases corresponding to the plurality of first simulated nano-antennas set on the base of the simulated collimation element are obtained through S010, the simulated focal length of the simulated collimation element and the simulated focal length of two adjacent first simulated nano-antennas can be obtained first. The distance between the centers of the nano-antennas, wherein the analog focal length can be preset, the center-to-center distances of two adjacent first simulated nano-antennas are the same, and the center-to-center distances of two adjacent first simulated nano-antennas can be based on the preset distance of the first simulated nano-antenna Set the working wavelength and the field angle to be realized. Then, according to the simulated focal length, the lens focusing equation and the distance between the centers of two adjacent first simulated nano-antennas, the respective collimation phases corresponding to each of the multiple first simulated nano-antennas are obtained. It should be noted that the center-to-center distance between two adjacent nano-antennas of the metasurface optical element is equal to the center-to-center distance between two adjacent first simulated nano-antennas.
在一些实施方式中,通过S020获取模拟衍射元件基底上设置的多个第二模拟纳米天线各自对应的衍射相位时,可以先获取模拟衍射元件的模拟视场角,该模拟视场角可以根据需求合理预设。然后根据模拟视场角和预设算法得出多个第二模拟纳米天线各自对应的衍射相位。在一些实施方式中,预设算法可以是傅里叶迭代算法或遗传算法等。In some embodiments, when the diffraction phases corresponding to the multiple second simulated nano-antennas provided on the base of the simulated diffraction element are obtained through S020, the simulated angle of view of the simulated diffraction element can be obtained first, and the simulated angle of view can be obtained according to requirements. reasonable assumptions. Then, the corresponding diffraction phases of the multiple second simulated nano-antennas are obtained according to the simulated viewing angle and a preset algorithm. In some implementation manners, the preset algorithm may be a Fourier iterative algorithm, a genetic algorithm, or the like.
在一些实施方式中,在S010之前,可以先根据所需工作的工作波长来确定超表面光学元件100的材质,包括基底110的材质和纳米天线120的材质,纳米天线120可以选取高折射率的材质。还可以根据工作波长和视场角确定超表面光学元件100基底110上的相邻两个纳米天线120的中心间距,例如设置为小于600nm。在确定好纳米天线120的中心间距后,使用电磁仿真软件对正投影的形状为圆形、正方形或带圆角的正方形等具有一定程度的各项同性的C4旋转对称图形的纳米天线120进行仿真,通过对纳米结构的尺寸和高度进行优化,选出多个高度相同,形状和/或尺寸不同的纳米柱。数量可以是2个、4个、8个等。在一些实施方式中,首先对不同尺寸和高度的纳米天线柱进行模拟仿真,得到它们 的透过率和传输相位分布图。在选取纳米天线120时,主要根据相同偏振透过率最高且相等,传输相位均匀分布在0~2π之中两个要求进行选取。In some embodiments, before S010, the material of the metasurface optical element 100 can be determined according to the required working wavelength, including the material of the substrate 110 and the material of the nano-antenna 120, and the nano-antenna 120 can be selected from a material with a high refractive index. material. The distance between the centers of two adjacent nano-antennas 120 on the substrate 110 of the metasurface optical element 100 can also be determined according to the working wavelength and the viewing angle, for example, set to be less than 600 nm. After determining the distance between the centers of the nano-antenna 120, use electromagnetic simulation software to simulate the nano-antenna 120 whose orthographic shape is a circle, a square or a square with rounded corners, etc., which have a certain degree of isotropic C4 rotational symmetry. , by optimizing the size and height of the nanostructures, multiple nanocolumns with the same height but different shapes and/or sizes are selected. The quantity can be 2, 4, 8 etc. In some embodiments, firstly, simulate nano-antenna pillars of different sizes and heights to obtain their transmittance and transmission phase distribution diagrams. When selecting the nano-antenna 120 , the selection is mainly based on the two requirements that the same polarization transmittance is the highest and equal, and the transmission phase is evenly distributed among 0-2π.
本申请的一些实施例提供了一种结构光投影模组,如图7所示,结构光投影模组可以包括光源10以及上述任一种的超表面光学元件100,光源10位于超表面光学元件100的入光侧,光源10出射的光束经超表面光学元件100的纳米天线120入射,通过纳米天线120的相位调制,对入射的光束进行准直和衍射后出射在目标区域。当光源10为垂直腔面发射激光器时,能够对应在目标区域投射散斑点图像20。由于通过超表面光学元件100集成了准直和衍射,因此,该结构光投影模组的整体体积较。在一些实施方式中,光源10还可以是产生点源的LD激光器,光源10为任意偏振光,波长为紫外波段到太赫兹波段。Some embodiments of the present application provide a structured light projection module. As shown in FIG. On the light-incident side of 100, the light beam emitted by the light source 10 enters the nano-antenna 120 of the metasurface optical element 100, and through the phase modulation of the nano-antenna 120, the incident light beam is collimated and diffracted before exiting the target area. When the light source 10 is a vertical cavity surface emitting laser, it can correspondingly project a speckle image 20 on the target area. Since the collimation and diffraction are integrated through the metasurface optical element 100, the overall volume of the structured light projection module is relatively small. In some embodiments, the light source 10 can also be an LD laser that generates a point source, the light source 10 is light of arbitrary polarization, and the wavelength is from the ultraviolet band to the terahertz band.
以上所述仅为本申请的优选实施例而已,并不用于限制本申请,对于本领域的技术人员来说,本申请可以有各种更改和变化。凡在本申请的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本申请的保护范围之内。The above descriptions are only preferred embodiments of the present application, and are not intended to limit the present application. For those skilled in the art, there may be various modifications and changes in the present application. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of this application shall be included within the protection scope of this application.
工业实用性Industrial Applicability
本申请提供了一种超表面光学元件及设计方法、结构光投影模组,超表面光学元件包括基底,设置于基底上的多个通过传输相位调制入射光束的纳米天线,至少两个纳米天线的尺寸不同且多个纳米天线阵列分布于基底的一侧,相邻两个纳米天线的中心间距相同,每个纳米天线的传输相位为准直相位和衍射相位的叠加。如此,便可以使得形成的超表面光学元件能够同时具有准直和衍射功能,即将准直元件和衍射元件进行集成,有效降低了现有准直和衍射独立为两个光学元件所占用的空间,同时,由于取消了准直元件和衍射元件的对位装配,因此,能够有效降低其所导致的对位误差。The present application provides a metasurface optical element and its design method, and a structured light projection module. The metasurface optical element includes a substrate, a plurality of nanoantennas arranged on the substrate to modulate the incident light beam through transmission phase, and at least two nanoantennas Multiple nano-antenna arrays with different sizes are distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase. In this way, the formed metasurface optical element can have collimation and diffraction functions at the same time, that is, the collimation element and the diffraction element are integrated, which effectively reduces the space occupied by the existing collimation and diffraction independent of two optical elements. At the same time, since the alignment assembly of the collimation element and the diffraction element is canceled, the alignment error caused by it can be effectively reduced.
此外,可以理解的是,本申请的超表面光学元件及设计方法、结构光投影模组是可以重现的,并且可以用在多种工业应用中。例如,本申请的超表面光学元件及设计方法、结构光投影模组可以用于光学技术领域。In addition, it can be understood that the metasurface optical element, design method, and structured light projection module of the present application are reproducible and can be used in various industrial applications. For example, the metasurface optical element, design method, and structured light projection module of the present application can be used in the field of optical technology.

Claims (15)

  1. 一种超表面光学元件,其特征在于,包括基底,设置于所述基底上的多个通过传输相位调制入射光束的纳米天线,至少两个所述纳米天线的尺寸不同且多个所述纳米天线阵列分布于所述基底一侧,相邻两个所述纳米天线的中心间距相同,每个所述纳米天线的传输相位为准直相位和衍射相位的叠加。A metasurface optical element, characterized in that it includes a base, a plurality of nano-antennas arranged on the base through transmission phase modulation of incident light beams, at least two of the nano-antennas have different sizes and a plurality of the nano-antennas The array is distributed on one side of the substrate, the distance between the centers of two adjacent nano-antennas is the same, and the transmission phase of each nano-antenna is the superposition of the collimation phase and the diffraction phase.
  2. 如权利要求1所述的超表面光学元件,其特征在于,所述纳米天线在所述基底上的正投影为C4旋转对称图形。The metasurface optical element according to claim 1, wherein the orthographic projection of the nano-antenna on the substrate is a C4 rotationally symmetric figure.
  3. 如权利要求2所述的超表面光学元件,其特征在于,所述纳米天线的正投影为圆形;或,所述纳米天线的正投影为正方形;或,多个所述纳米天线包括第一天线和第二天线,所述第一天线在所述基底的正投影为圆形,所述第二天线在所述基底的正投影为正方形。The metasurface optical element according to claim 2, wherein the orthographic projection of the nano-antenna is a circle; or, the orthographic projection of the nano-antenna is a square; or, a plurality of the nano-antennas include a first For the antenna and the second antenna, the orthographic projection of the first antenna on the base is a circle, and the orthographic projection of the second antenna on the base is a square.
  4. 如权利要求3所述的超表面光学元件,其特征在于,当所述纳米天线为正方形时,所述正方形的边长为50nm至500nm;和/或,当所述纳米天线为圆形时,所述圆形的直径为50nm至500nm。The metasurface optical element according to claim 3, wherein when the nano-antenna is a square, the side length of the square is 50nm to 500nm; and/or, when the nano-antenna is circular, The diameter of the circle is 50nm to 500nm.
  5. 如权利要求1至4中的任一项所述的超表面光学元件,其特征在于,相邻两个所述纳米天线的中心间距200nm至600nm;多个所述纳米天线的高度均大于300nm。The metasurface optical element according to any one of claims 1 to 4, wherein the center-to-center distance between two adjacent nano-antennas is 200 nm to 600 nm; the heights of multiple nano-antennas are all greater than 300 nm.
  6. 如权利要求1至5中的任一项所述的超表面光学元件,其特征在于,多个所述纳米天线的高度均相同;尺寸不同的所述纳米天线的个数大于或等于4。The metasurface optical element according to any one of claims 1 to 5, wherein the heights of the plurality of nano-antennas are the same; the number of the nano-antennas with different sizes is greater than or equal to 4.
  7. 如权利要求1至6中的任一项所述的超表面光学元件,其特征在于,所述基底为透明基底,所述透明基底的材质为石英、玻璃或氧化硅薄膜。The metasurface optical element according to any one of claims 1 to 6, wherein the substrate is a transparent substrate, and the material of the transparent substrate is quartz, glass or silicon oxide film.
  8. 如权利要求1至7中的任一项所述的超表面光学元件,其特征在于,所述纳米天线的材质是硅、氧化钛、氧化铝或氮化硅。The metasurface optical element according to any one of claims 1 to 7, wherein the nano-antenna is made of silicon, titanium oxide, aluminum oxide or silicon nitride.
  9. 一种超表面光学元件设计方法,其特征在于,所述方法包括:A method for designing a metasurface optical element, characterized in that the method comprises:
    使用超表面光学元件在实现单一准直功能时所呈现的模拟准直元件,获取基底上设置的多个第一模拟纳米天线各自对应的准直相位;Using the simulated collimation element presented by the metasurface optical element when realizing a single collimation function, obtaining the corresponding collimation phases of the plurality of first simulated nano-antennas arranged on the substrate;
    使用超表面光学元件在实现单一衍射功能时所呈现的模拟衍射元件,获取基底上设置的多个第二模拟纳米天线各自对应的衍射相位,其中,所述多个第一模拟纳米天线与所述多个第二模拟纳米天线的数量一一对应;Using the simulated diffraction element presented by the metasurface optical element when realizing a single diffraction function, the respective diffraction phases corresponding to the multiple second simulated nano-antennas set on the substrate are obtained, wherein the multiple first simulated nano-antennas are the same as the The number of multiple second simulated nano-antennas corresponds to each other;
    将多个所述第一模拟纳米天线的准直相位与各自对应的所述第二模拟纳米天线的衍射相位叠加得到多个模拟相位;superimposing the collimated phases of the first simulated nanoantennas with the diffraction phases of the corresponding second simulated nanoantennas to obtain multiple simulated phases;
    对所述多个模拟相位进行离散得到多个离散相位,其中,所述超表面光学元件基底上的多个纳米天线的数量与所述多个离散相位的数量一一对应,所述多个纳米天线的传输相位与各自对应的所述离散相位相同。Discrete the multiple simulated phases to obtain multiple discrete phases, wherein the number of multiple nano-antennas on the base of the metasurface optical element corresponds to the number of the multiple discrete phases one-to-one, and the multiple nano-antennas The transmission phases of the antennas are the same as the respective discrete phases.
  10. 如权利要求9所述的超表面光学元件设计方法,其特征在于,在将多个所述第一模拟纳米天线的准直相位与各自对应的所述第二模拟纳米天线的衍射相位叠加得到所述多个模拟相位之后,对所述多个第一模拟纳米天线和所述多个第二模拟纳米天线进行微调以优化模拟结果,从而优化叠加相位。The method for designing a metasurface optical element according to claim 9, wherein the alignment phases of a plurality of the first simulated nanoantennas are superimposed with the diffraction phases of the respective corresponding second simulated nanoantennas to obtain the obtained After the plurality of simulated phases, the plurality of first simulated nanoantennas and the plurality of second simulated nanoantennas are fine-tuned to optimize the simulation results, thereby optimizing the superposition phase.
  11. 如权利要求9或10所述的超表面光学元件设计方法,其特征在于,所述获取基底上设置的多个第一模拟纳米天线各自对应的准直相位包括:The metasurface optical element design method as claimed in claim 9 or 10, wherein the collimation phase corresponding to each of the plurality of first simulated nano-antennas provided on the acquisition substrate comprises:
    获取所述模拟准直元件的模拟焦距和相邻两个所述第一模拟纳米天线的中心间距;Acquiring the simulated focal length of the simulated collimation element and the center-to-center distance of two adjacent first simulated nano-antennas;
    根据所述模拟焦距、透镜聚焦方程和所述第一模拟纳米天线的中心间距得出所述多个第一模拟纳米天线各自对应的准直相位。The corresponding collimation phases of the plurality of first simulated nano-antennas are obtained according to the simulated focal length, the lens focusing equation and the center-to-center distance of the first simulated nano-antennas.
  12. 如权利要求11所述的超表面光学元件设计方法,其特征在于,相邻两个第一模拟纳米天线的中心间距是根据所述第一模拟纳米天线的预设工作波长和所要实现的视场角确定的。The method for designing a metasurface optical element according to claim 11, wherein the distance between the centers of two adjacent first simulated nanoantennas is based on the preset working wavelength and the field of view to be realized of the first simulated nanoantennas angle is fixed.
  13. 如权利要求9至12中的任一项所述的超表面光学元件设计方法,其特征在于,所述获取基底上设置的多个第二模拟纳米天线各自对应的衍射相位包括:The metasurface optical element design method according to any one of claims 9 to 12, wherein said acquisition of the corresponding diffraction phases of a plurality of second simulated nano-antennas arranged on the substrate comprises:
    获取所述模拟衍射元件的模拟视场角;Acquiring a simulated viewing angle of the simulated diffraction element;
    根据所述模拟视场角和预设算法得出所述多个第二模拟纳米天线各自对应的衍射相位。The respective diffraction phases corresponding to the plurality of second simulated nano-antennas are obtained according to the simulated viewing angle and a preset algorithm.
  14. 如权利要求9至13中的任一项所述的超表面光学元件设计方法,其特征在于,在获取基底上设置的多个第一模拟纳米天线各自对应的准直相位之前,根据所需的工作波长来确定所述超表面光学元件的材质。The method for designing a metasurface optical element according to any one of claims 9 to 13, wherein, before acquiring the corresponding collimation phases of a plurality of first simulated nanoantennas arranged on the substrate, according to the required The working wavelength is used to determine the material of the metasurface optical element.
  15. 一种结构光投影模组,其特征在于,包括光源以及如权利要求1至8任一项所述的超表面光学元件,所述光源位于所述超表面光学元件的入光侧,所述超表面光学元件用于对所述光源出射的光束进行准直和衍射。A structured light projection module, characterized in that it includes a light source and the metasurface optical element according to any one of claims 1 to 8, the light source is located on the light incident side of the metasurface optical element, and the metasurface optical element The surface optical element is used to collimate and diffract the light beam emitted by the light source.
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