CN109709630B - A method for generating subwavelength vortex beam arrays based on metal nanometasurfaces - Google Patents

A method for generating subwavelength vortex beam arrays based on metal nanometasurfaces Download PDF

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CN109709630B
CN109709630B CN201910104113.9A CN201910104113A CN109709630B CN 109709630 B CN109709630 B CN 109709630B CN 201910104113 A CN201910104113 A CN 201910104113A CN 109709630 B CN109709630 B CN 109709630B
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quartz glass
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nanorod
photoresist
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CN109709630A (en
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黄小平
孙静泊
张培峰
黄秋莹
周杰
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University of Electronic Science and Technology of China
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Abstract

本发明提出了一种基于金属纳米超表面的亚波长涡旋光束阵列产生方法,其首先制备出由金属纳米棒阵列构成的特定金属纳米超表面结构,然后通过圆偏振光垂直照射该特定金属纳米超表面结构,由此将圆偏振光转变成亚波长尺度的涡旋波束阵列,本发明还通过合理设计金属纳米棒的尺寸及排布,制备出可产生亚波长旋涡光束阵列的特定金属纳米超表面结构,相较于其他旋涡光束产生方式,本发明所用方法具有结构简单、和易于集成、光强分布均匀等优点,并且该方法产生的涡旋光束阵列不仅能够在信息传输与存储中增强信息安全性与容量,在微粒捕获中一次性捕获大量粒子,而且能同时探测不同物体的运动特性,拓展了旋涡光束的应用领域。

Figure 201910104113

The invention proposes a method for generating a subwavelength vortex beam array based on a metal nanometer metasurface, which firstly prepares a specific metal nanometer metasurface structure composed of a metal nanorod array, and then vertically irradiates the specific metal nanometer with circularly polarized light Metasurface structure, thereby converting circularly polarized light into a subwavelength vortex beam array, the present invention also prepares a specific metal nanometer supersurface capable of generating a subwavelength vortex beam array by rationally designing the size and arrangement of the metal nanorods. Surface structure, compared with other vortex beam generation methods, the method used in the present invention has the advantages of simple structure, easy integration, uniform light intensity distribution, etc., and the vortex beam array generated by this method can not only enhance information in information transmission and storage Safety and capacity, a large number of particles can be captured at one time in particle capture, and the motion characteristics of different objects can be detected at the same time, which expands the application field of vortex beams.

Figure 201910104113

Description

基于金属纳米超表面的亚波长涡旋光束阵列产生方法A method for generating subwavelength vortex beam arrays based on metal nanometasurfaces

技术领域technical field

本发明涉及微纳光学中新型光场调控领域,具体涉及到一种基于金属纳米超表面的亚波长涡旋光束阵列产生方法。The invention relates to the field of novel light field regulation in micro-nano optics, in particular to a method for generating a subwavelength vortex beam array based on a metal nanometer metasurface.

背景技术Background technique

涡旋光束又称为光学旋涡,是一种具有孤立奇点的光场,其中携带相位奇点的称为相位涡旋光束(Orbital Angular Momentum,OAM),相位涡旋光束的波矢量有方位项,且绕着旋涡中心旋转,在光学表达式μ0(r,θ,z)=μ0(r,z)exp(ilθ)exp(-ikz)中存在相位因子exp(ilθ),其中,r为距离原点处的位移矢量,μ0表示振幅,θ表示方位角,z表示传播距离,l为它的拓扑荷数,k为波数,大小为

Figure BDA0001966258640000011
λ表示入射光的波长。由于不同的拓扑荷数,每个光子携带的轨道角动量
Figure BDA0001966258640000012
不同。涡旋光束的中心为一个微米级的暗斑,且对微纳粒子操控时无热损耗效应,这使得涡旋光束在微纳操控领域有着广泛的应用,同时涡旋光束对粒子囚禁时,会通过轨道角动量让粒子发生旋转,因此也被称为“光学扳手”。涡旋光束在长距离传输时稳定性强,且理论上具有无限正交状态,同轴传输的不同方位角的涡旋光束之间是相互正交的,光束之间的串扰最小,所以光束可以有效地复用和解复用,这使得涡旋光束在保密通信领域有着巨大的应用前景。另外,涡旋光束还在生物医学、微观力学、天文学、量子信息处理等领域有着巨大的应用潜力。A vortex beam, also known as an optical vortex, is a light field with an isolated singularity. The phase singularity is called a phase vortex beam (Orbital Angular Momentum, OAM). The wave vector of the phase vortex beam has an azimuth term. , and rotates around the center of the vortex, there is a phase factor exp(ilθ) in the optical expression μ 0 (r,θ,z)=μ 0 (r,z)exp(ilθ)exp(-ikz), where r is the displacement vector at the distance from the origin, μ 0 represents the amplitude, θ represents the azimuth angle, z represents the propagation distance, l is its topological charge number, k is the wave number, and the magnitude is
Figure BDA0001966258640000011
λ represents the wavelength of incident light. The orbital angular momentum carried by each photon due to the different topological charge numbers
Figure BDA0001966258640000012
different. The center of the vortex beam is a micron-scale dark spot, and there is no heat loss effect when manipulating micro-nano particles, which makes the vortex beam have a wide range of applications in the field of micro-nano manipulation. At the same time, when the vortex beam traps the particles, it will Particles are rotated by orbital angular momentum, hence the name "optical wrench". Vortex beams have strong stability during long-distance transmission, and theoretically have an infinite orthogonal state. Effectively multiplexing and demultiplexing, this makes vortex beams have great application prospects in the field of secure communications. In addition, vortex beams also have great application potential in biomedicine, micromechanics, astronomy, quantum information processing and other fields.

目前产生涡旋光束的方法主要包括:螺旋相位板法、几何模式转换法、空间光调制器法及计算全息法等。螺旋相位板法是通过具有螺旋型相位的期间对光附加一个螺旋型的相位,几何模式变化是通过光学器件改变入射光的模式,这两种方法的本质都是对入射光的光程进行调制从何使得不同位置具有不同的相位,但光程的积累使得器件必须具备一定的物理尺寸,这也成了限制其向微型化、集成化发展的一个重要因素;空间光调制器法及计算全息法是通过全息原理再现涡旋光束,这种方式能产生多个涡旋光束,但光束光能分布不均匀,且不同阶的光束之间会有重叠,因此难以从中分离出单一拓扑荷数的涡旋光束。尽管产生涡旋光束的方法有多种,但都存在一些缺陷,且应用场景有限。因此,研究出一种能够产生光能分布均匀、无高阶衍射影响,亚波长尺度的涡旋光束阵列产生器在微纳光学领域具有重要的意义。At present, the methods for generating vortex beams mainly include: helical phase plate method, geometric mode conversion method, spatial light modulator method and computational holography method. The helical phase plate method is to add a helical phase to the light through the period of the helical phase, and the geometric mode change is to change the mode of the incident light through optical devices. The essence of these two methods is to modulate the optical path of the incident light. How can different positions have different phases, but the accumulation of optical paths makes the device must have a certain physical size, which has also become an important factor limiting its development to miniaturization and integration; spatial light modulator method and computational holography The method is to reproduce the vortex beam through the holographic principle. This method can generate multiple vortex beams, but the light energy distribution of the beams is not uniform, and the beams of different orders will overlap, so it is difficult to separate a single topological charge from them. Vortex beam. Although there are many ways to generate vortex beams, they all have some drawbacks and limited application scenarios. Therefore, it is of great significance in the field of micro-nano optics to develop a subwavelength-scale vortex beam array generator that can produce uniform light energy distribution without high-order diffraction effects.

1984年,英国Berry教授首次提出几何相位的概念。Berry研究发现,当一个绝热物理系统从初态沿着某一路径(在一定的参数空间或者态空间)演变一个周期并回到初始状态时,其最终态与初始态并不等效,而需要增加一个额外的相位因子(Quantal phasefactors accom panying adiabatic changes,M.V.Berry,Proceedings of the RoyalSociety A:Mathematical,Physical and Engineering Sciences,Vol.392,No.1802,pages 45–57,08March 1984);1956年,印度拉曼研究所Pancharatnam教授研究得到电磁波在偏振态转化过程中会产生一个额外的相位(Generalized theory of interference andits applications,Pancharatnam S.,Proc eedings of the Indian Academy ofSciences-Section A,Vol.44,No.5,pages 247–262,30October 1956)。某一偏振态的电磁波,沿庞加莱球表面某一路径演变并回到初态,其终态与初始态相差一个相位因子,其值等于演变路径测地线所围闭合环路立体角的一半。基于这些理论,相关研究者提出了几何相位型超表面的概念。通过亚波长金属或介质结构在二维平面的几何曲向来调控电磁波相位参量,从而构造出想要的波前,进而得到了包括平面成像透镜、定向表面波耦合器、超震荡透镜、涡旋光束发生器、涡旋光分束器在内的一系列复杂平面光学器件。本发明正是基于几何相位型超表面研究得到了一种亚波长涡旋光束阵列产生方法。In 1984, British Professor Berry first proposed the concept of geometric phase. Berry's research found that when an adiabatic physical system evolves from the initial state along a certain path (in a certain parameter space or state space) for a period and returns to the initial state, its final state is not equivalent to the initial state, but needs to be Add an extra phase factor (Quantal phasefactors accom panying adiabatic changes, M.V.Berry, Proceedings of the Royal Society A:Mathematical,Physical and Engineering Sciences, Vol.392, No.1802, pages 45–57, 08March 1984); 1956, Professor Pancharatnam of the Indian Institute of Raman Research found that the electromagnetic wave will generate an additional phase during the transformation of the polarization state (Generalized theory of interference and its applications, Pancharatnam S., Proceedings of the Indian Academy of Sciences-Section A, Vol.44, No. .5, pages 247–262, 30 October 1956). The electromagnetic wave of a certain polarization state evolves along a certain path on the surface of the Poincaré sphere and returns to the initial state. half. Based on these theories, related researchers have proposed the concept of geometric phase-type metasurfaces. The electromagnetic wave phase parameters are controlled by the geometric curvature of the subwavelength metal or dielectric structure in the two-dimensional plane, so as to construct the desired wavefront, and then obtain a plane imaging lens, a directional surface wave coupler, a superoscillating lens, and a vortex beam. A series of complex planar optics including generators, vortex beam splitters. The invention obtains a subwavelength vortex beam array generation method based on the research of the geometric phase type metasurface.

在上述背景技术中,如螺旋相位板法、几何模式转换法、空间光调制器法及计算全息法等涡旋光束产生方法都存在一些缺陷,应用场景有限。本发明研究设计了一种基于金属纳米超表面的亚波长涡旋光束阵列产生方法,不仅能够在信息传输与存储中增强信息安全性与容量,在微纳操控中同时捕获操控大量粒子,而且能同时探测不同物体的运动特性,拓展了旋涡光束的应用领域。In the above-mentioned background technologies, vortex beam generating methods such as the spiral phase plate method, the geometric mode conversion method, the spatial light modulator method, and the computational holography method all have some defects and have limited application scenarios. The invention researches and designs a method for generating a subwavelength vortex beam array based on a metal nanometer metasurface, which can not only enhance information security and capacity in information transmission and storage, but also capture and manipulate a large number of particles in micro-nano manipulation. At the same time, the motion characteristics of different objects are detected, which expands the application field of vortex beams.

发明内容SUMMARY OF THE INVENTION

本发明的目的在于将涡旋光束阵列的振幅与相位转化成金属纳米棒的尺寸与旋转角,通过合理设计金属纳米棒的尺寸及旋转角,实现对入射光束振幅与相位的同时调控,并采用电子束刻蚀方法制备周期分布的金属纳米棒阵列,由此构成金属纳米超表面结构,在圆偏振光从金属纳米超表面结构底部正入射下,金属纳米超表面结构形成的透射区域产生光能分布均匀的亚波长尺度的涡旋光束阵列,以解决背景技术中存在的问题。本发明的基于金属纳米超表面的亚波长涡旋光束阵列产生方法相较其他涡旋光束产生发方式,具有结构简单、易于集成等优势。The purpose of the invention is to convert the amplitude and phase of the vortex beam array into the size and rotation angle of the metal nanorods, and realize the simultaneous regulation of the amplitude and phase of the incident beam by reasonably designing the size and rotation angle of the metal nanorods. Electron beam etching method prepares metal nanorod arrays with periodic distribution, thereby forming metal nanometer metasurface structure. Under the normal incidence of circularly polarized light from the bottom of metal nanometer metasurface structure, the transmission area formed by metal nanometer metasurface structure generates light energy A vortex beam array with a uniform distribution of sub-wavelength scales is used to solve the problems existing in the background art. Compared with other vortex beam generation methods, the method for generating a subwavelength vortex beam array based on a metal nano-metasurface of the present invention has the advantages of simple structure, easy integration and the like.

本发明的基于金属纳米超表面的亚波长涡旋光束阵列产生方法包括:首先制备出由金属纳米棒阵列和石英玻璃基底构成的整体呈长方体形状的特定金属纳米超表面结构,所述金属纳米棒阵列包含n个金属纳米棒,其中,n为正整数且n>4,所述金属纳米棒周期排布在所述石英玻璃基底的上表面上,以所述金属纳米棒阵列上表面所在平面中任意一点为原点,从该原点出发,所述特定金属纳米超表面结构的长度和宽度方向分别为X轴和Y轴、所述特定金属纳米超表面结构厚度的反方向为Z轴;然后将波长为532nm的圆偏振光从Z<0的区域垂直照射到特定金属纳米超表面结构,所述圆偏振光与任意一个金属纳米棒作用后,其光波相位就附加一个相位因子2θ,其中θ为任意一个金属纳米棒长轴与X轴的夹角,因每一个金属纳米棒的长轴与X轴的夹角θ不同,从Z=0的XY平面透射出来的圆偏振光在Z>0的透射区域的不同位置呈现不同的相位,X和Y轴两个方向上相邻的4个金属纳米棒产生一个涡旋光束,该涡旋光束的直径为180nm,由于金属纳米棒阵列的作用,在Z>0的透射区域产生光能分布均匀且相位螺旋分布的亚波长尺度的涡旋光束阵列。The method for generating a subwavelength vortex beam array based on a metal nanometer metasurface of the present invention includes: firstly preparing a specific metal nanometer metasurface structure composed of a metal nanorod array and a quartz glass substrate, which is in the shape of a cuboid as a whole, the metal nanorods The array includes n metal nanorods, where n is a positive integer and n>4, the metal nanorods are periodically arranged on the upper surface of the quartz glass substrate, and the upper surface of the metal nanorod array is in the plane Any point is the origin, starting from this origin, the length and width directions of the specific metal nano-metasurface structure are the X-axis and the Y-axis respectively, and the opposite direction of the thickness of the specific metal nano-metasurface structure is the Z-axis; then the wavelength The circularly polarized light of 532 nm is vertically irradiated to a specific metal nano-metasurface structure from the region of Z < 0. After the circularly polarized light interacts with any metal nanorod, a phase factor 2θ is added to the light wave phase, where θ is any The angle between the long axis of a metal nanorod and the X axis, because the long axis of each metal nanorod is different from the angle θ between the long axis and the X axis, the circularly polarized light transmitted from the XY plane with Z=0 is transmitted at Z>0. Different positions of the region present different phases, and the four adjacent metal nanorods in the X and Y axes generate a vortex beam with a diameter of 180 nm. Due to the effect of the metal nanorod array, in Z The transmission region > 0 produces a subwavelength-scale vortex beam array with uniform light energy distribution and phase helical distribution.

其中,制备特定金属纳米超表面结构的具体方法包括如下步骤:Wherein, the specific method of preparing specific metal nanometer metasurface structure comprises the following steps:

S1)在石英玻璃基底上旋涂光刻胶S1) Spin-coating photoresist on quartz glass substrate

S11)清洗石英玻璃基底S11) Cleaning the quartz glass substrate

将长方体形状的原始石英玻璃基底放置于浓度为0.5mol/L,温度为35℃~50℃的HCl溶液中,静置10分钟后,将石英玻璃基底放在50℃左右的纯水中浸泡5分钟,取出石英玻璃基底再用50℃左右的纯水进行二次清洗,完成石英玻璃基底的化学清洗;Place the original quartz glass substrate in the shape of a cuboid in a HCl solution with a concentration of 0.5 mol/L and a temperature of 35°C to 50°C. After standing for 10 minutes, place the quartz glass substrate in pure water at about 50°C for 5 minutes. minutes, take out the quartz glass substrate and perform secondary cleaning with pure water at about 50°C to complete the chemical cleaning of the quartz glass substrate;

S12)烘干石英玻璃基底S12) drying the quartz glass substrate

将经过步骤S11)处理的石英玻璃基底放置在清洗篮上,并向清洗篮内通入温度为80℃左右的高洁净空气或者氮气,持续10~20分钟,待石英玻璃基底和清洗篮充分干燥后,石英玻璃基底的烘干完成;Place the quartz glass substrate processed in step S11) on the cleaning basket, and pass high-clean air or nitrogen gas with a temperature of about 80°C into the cleaning basket for 10 to 20 minutes, until the quartz glass substrate and the cleaning basket are fully dried. After that, the drying of the quartz glass substrate is completed;

S13)旋涂光刻胶S13) Spin coating photoresist

将经过步骤S12)处理的石英玻璃基底吸附在真空卡盘上,调整真空卡盘转速为500rpm,并向石英玻璃基底上表面中心滴入光刻胶,5秒后,将真空卡盘转速提高到3000~7000rpm,甩胶30秒,形成厚度为140nm的光刻胶涂层;The quartz glass substrate processed in step S12) is adsorbed on the vacuum chuck, the rotation speed of the vacuum chuck is adjusted to 500rpm, and photoresist is dripped into the center of the upper surface of the quartz glass substrate. After 5 seconds, the rotation speed of the vacuum chuck is increased to 500 rpm. 3000 ~ 7000rpm, sling for 30 seconds to form a photoresist coating with a thickness of 140nm;

S14)匀胶后软烘石英玻璃基底S14) Soft-bake the quartz glass substrate after sizing

待光刻胶在石英玻璃基底上表面涂布均匀后,将经过步骤S13)处理的石英玻璃基底放在80℃的真空热板上软烘2~5分钟;After the photoresist is evenly coated on the upper surface of the quartz glass substrate, the quartz glass substrate processed in step S13) is placed on a vacuum hot plate at 80° C. for soft baking for 2 to 5 minutes;

S2)电子束曝光得到图形S2) Electron beam exposure to obtain a pattern

S21)聚焦电子束曝光S21) Focused electron beam exposure

用加速电压为30KV,光斑尺寸为30nm,曝光剂量为25μc/cm2的电子束矢量曝光机对经过步骤S1)处理后的石英玻璃基底进行曝光,利用预设程序控制电子束矢量曝光机以在石英玻璃基底上表面得到光刻胶纳米棒的棒长均为90nm,棒宽均为30nm,厚度均为140~150nm的光刻胶纳米棒阵列图形,其中光刻胶纳米棒阵列图形中每1行和每1列的光刻胶纳米棒分别与X轴呈45°、-45°夹角间隔排列,且任意两根相邻的光刻胶纳米棒几何中心之间的距离均为180nm;Use an electron beam vector exposure machine with an accelerating voltage of 30KV, a spot size of 30nm, and an exposure dose of 25 μc/cm 2 to expose the quartz glass substrate processed in step S1), and use a preset program to control the electron beam vector exposure machine. The photoresist nanorod array pattern obtained on the upper surface of the quartz glass substrate has a rod length of 90 nm, a rod width of 30 nm, and a thickness of 140-150 nm. The photoresist nanorods in the row and each column are arranged at an angle of 45° and -45° respectively with the X axis, and the distance between the geometric centers of any two adjacent photoresist nanorods is 180 nm;

S22)曝光后烘干石英玻璃基底S22) drying the quartz glass substrate after exposure

将经过步骤S21)处理后的石英玻璃基底放置于150℃~170℃的烤箱中,烘烤90分钟,并在常温环境中静置冷却30分钟;Place the quartz glass substrate processed in step S21) in an oven at 150°C to 170°C, bake for 90 minutes, and stand for 30 minutes in a normal temperature environment;

S3)显影S3) Development

S31)显影、定影S31) developing, fixing

将经过步骤S2)处理后的石英玻璃基底浸没在温度为21±0.2℃的显影液中60~120秒,然后放入异丙醇溶液中30~40秒,完成定影,得到位于石英玻璃基底上表面的纳米棒阵列图形;The quartz glass substrate processed in step S2) is immersed in a developing solution with a temperature of 21±0.2° C. for 60 to 120 seconds, and then placed in an isopropanol solution for 30 to 40 seconds to complete the fixing, and obtain a solution on the quartz glass substrate. The nanorod array pattern on the surface;

S32)定影后烘干基片S32) drying the substrate after fixing

取出经过步骤S31)处理后的石英玻璃基底放在80℃的真空热板上软烘2~5分钟,得到位于石英玻璃基底上表面的烘干的纳米棒阵列图形;Take out the quartz glass substrate processed in step S31) and place it on a vacuum hot plate at 80° C. for soft baking for 2 to 5 minutes to obtain a dried nanorod array pattern on the upper surface of the quartz glass substrate;

S33)图形检查、蒸发金属膜S33) Pattern inspection, evaporating metal film

利用扫描电子显微观测技术对经过步骤S32)处理后的石英玻璃基底上表面的烘干的纳米棒阵列图形进行检查,确定该烘干的纳米棒阵列图形合格后用热蒸发台对石英玻璃基底进行金属金(Au)蒸发,其中金(Au)的厚度为20nm~30nm;The dried nanorod array pattern on the upper surface of the quartz glass substrate processed in step S32) is inspected by scanning electron microscopic observation technology. After confirming that the dried nanorod array pattern is qualified, the quartz glass substrate is subjected to a thermal evaporation table. Evaporating metal gold (Au), wherein the thickness of gold (Au) is 20nm-30nm;

S34)去除光刻胶得到金属图形S34) remove the photoresist to obtain the metal pattern

对经过步骤S33)处理后的石英玻璃基底进行丙酮剥离,去除残留的电子束光刻胶和金属金,在石英玻璃基底上表面得到金纳米棒阵列,其中,该金纳米棒阵列中的金纳米棒尺寸均为长90nm,宽30nm,厚25nm,金纳米棒阵列中每1行和每1列的金纳米棒分别与X轴呈45°、-45°夹角间隔排列,且任意两根相邻的金纳米棒几何中心之间的距离均为180nm,由此得到特定金属纳米超表面结构。Acetone peeling is performed on the quartz glass substrate treated in step S33), the residual electron beam photoresist and metal gold are removed, and a gold nanorod array is obtained on the upper surface of the quartz glass substrate, wherein the gold nanorods in the gold nanorod array are The rods are all 90nm long, 30nm wide, and 25nm thick. The gold nanorods in each row and column of the gold nanorod array are arranged at an angle of 45° and -45° with the X axis, respectively, and any two of them are in phase. The distances between the geometric centers of adjacent gold nanorods are all 180 nm, thereby obtaining a specific metal nano-metasurface structure.

本发明通过合理设计金属纳米棒的尺寸及排布,并利用电子束刻蚀这一较成熟的微纳加工方法,制备出可产生亚波长旋涡光束阵列的周期性金属纳米棒超表面。相较于其他旋涡光束产生方式,本发明所用方法具有结构简单、和易于集成、光强分布均匀等优点。并且该方法产生的涡旋光束阵列不仅能够在信息传输与存储中增强信息安全性与容量,在微粒捕获中一次性捕获大量粒子,而且能同时探测不同物体的运动特性,拓展了旋涡光束的应用领域。The present invention prepares a periodic metal nanorod metasurface capable of generating subwavelength vortex beam arrays by rationally designing the size and arrangement of the metal nanorods and using electron beam etching, a relatively mature micro-nano processing method. Compared with other vortex beam generating methods, the method used in the present invention has the advantages of simple structure, easy integration, uniform light intensity distribution, and the like. In addition, the vortex beam array generated by this method can not only enhance information security and capacity in information transmission and storage, capture a large number of particles at one time in particle capture, but also detect the motion characteristics of different objects at the same time, expanding the application of vortex beams. field.

附图说明Description of drawings

图1是本发明金属纳米超表面结构的示意图Fig. 1 is the schematic diagram of the metal nanometer metasurface structure of the present invention

图2是时域有限差分仿真得到的透射区域(Z>0的区域)沿Z轴距离金纳米棒阵列100nm处单个涡旋光束相位分布图;Figure 2 is a phase distribution diagram of a single vortex beam at a distance of 100 nm from the gold nanorod array along the Z axis in the transmission region (Z>0 region) obtained by finite difference time domain simulation;

图3是时域有限差分得到的仿真结果:(a)透射区域(Z>0的区域)沿Z轴距离金纳米棒阵列100nm处光强分布图;(b)透射区域(Z>0的区域)沿Z轴距离金纳米棒阵列100nm处相位分布图Figure 3 shows the simulation results obtained by finite difference time domain: (a) the light intensity distribution in the transmission region (Z>0 region) along the Z axis at a distance of 100 nm from the gold nanorod array; (b) the transmission region (Z>0 region) ) phase distribution at 100 nm from the gold nanorod array along the Z axis

图4是电子束刻蚀得到金纳米棒阵列的扫描电子显微镜照片Figure 4 is a scanning electron microscope photograph of gold nanorod arrays obtained by electron beam etching

具体实施方式Detailed ways

下面结合附图对本发明作进一步详细的描述。The present invention will be described in further detail below with reference to the accompanying drawings.

本发明的基于金属纳米超表面的亚波长涡旋光束阵列产生方法首先制备出特定金属纳米超表面结构,其制备是采用长方体形状的高透射石英玻璃作为基底,利用电子束刻蚀工艺在基底上表面制备出周期排布的金纳米棒阵列,所述金纳米棒阵列包含n个金纳米棒,其中,n为正整数且n>4,以所述金纳米棒阵列上表面所在平面中任意一点为原点,从该原点出发,所述特定金属纳米超表面结构的长度和宽度方向分别为X轴和Y轴、所述特定金属纳米超表面结构厚度的反方向为Z轴,即金纳米棒阵列的上表面位于Z=0处的XY平面上,并且金纳米棒的尺寸均为90nm×30nm×25nm,并且分别以横向、纵向与X轴分别呈45°、-45°夹角交错排布,即金纳米棒以360nm±10nm周期间隔排列,由于在金纳米棒阵列的每1行每1列上,金纳米棒都是以180nm为间隔,与X轴分别呈45°、-45°夹角间隔排列的,从一个与X轴呈45°夹角排列的金纳米棒到该行或者该列上的下一个与X轴呈45°夹角排列的金纳米棒之间均间隔了360nm,加上允许误差范围,故称金纳米棒阵列中的金纳米棒以360nm±10nm为周期间隔排列;然后将波长为532nm的圆偏振光从Z<0的区域垂直照射到特定金属纳米超表面结构,所述圆偏振光与任意一个金纳米棒作用后,其光波相位就附加一个相位因子2θ,其中θ为任意一个金纳米棒长轴与X轴的夹角,因每一个金纳米棒的长轴与X轴的夹角θ不同,从Z=0处的XY平面透射出来的圆偏振光在Z>0的透射区域的不同位置呈现不同的相位,X和Y轴两个方向上相邻的4个金纳米棒产生一个涡旋光束,该涡旋光束的直径为180nm,即涡旋光束的直径小于入射圆偏振光的波长,因此在金纳米棒阵列的作用下,在Z>0的透射区域产生光能分布均匀且相位螺旋分布的亚波长尺度的涡旋光束阵列。The method for generating a subwavelength vortex beam array based on a metal nanometer metasurface of the present invention firstly prepares a specific metal nanometer metasurface structure. A gold nanorod array with periodic arrangement is prepared on the surface, and the gold nanorod array includes n gold nanorods, wherein, n is a positive integer and n>4, and any point in the plane where the upper surface of the gold nanorod array is located As the origin, starting from this origin, the length and width directions of the specific metal nano-metasurface structure are the X axis and the Y axis, respectively, and the opposite direction of the thickness of the specific metal nano-metasurface structure is the Z axis, that is, the gold nanorod array. The upper surface is located on the XY plane at Z=0, and the size of the gold nanorods is 90nm×30nm×25nm, and they are staggered at an angle of 45° and -45° in the transverse direction, the longitudinal direction and the X axis, respectively, that is, gold The nanorods are arranged at a periodic interval of 360nm±10nm, because in every row and every column of the gold nanorod array, the gold nanorods are arranged at an interval of 180nm, and are arranged at an angle of 45° and -45° respectively with the X axis. , there is an interval of 360nm from a gold nanorod arranged at an angle of 45° to the X axis to the next gold nanorod arranged at an angle of 45° to the X axis in this row or column, plus the allowable Therefore, the gold nanorods in the gold nanorod array are arranged at periodic intervals of 360 nm ± 10 nm; then circularly polarized light with a wavelength of 532 nm is irradiated vertically from the region of Z < 0 to the specific metal nano-metasurface structure. After the circularly polarized light interacts with any gold nanorod, the phase of its light wave is added with a phase factor 2θ, where θ is the angle between the long axis of any gold nanorod and the X axis, because the long axis of each gold nanorod and X The included angle θ of the axes is different, and the circularly polarized light transmitted from the XY plane at Z=0 presents different phases at different positions in the transmission area of Z>0. The nanorods generate a vortex beam with a diameter of 180nm, that is, the diameter of the vortex beam is smaller than the wavelength of the incident circularly polarized light, so under the action of the gold nanorod array, light is generated in the transmission region of Z>0 A subwavelength-scale vortex beam array with uniform distribution and phase helical distribution.

本发明中制备特定金属纳米超表面结构的具体方法包括如下步骤:The specific method for preparing the specific metal nanometer metasurface structure in the present invention comprises the following steps:

S1)在石英玻璃基底上旋涂光刻胶S1) Spin-coating photoresist on quartz glass substrate

S11)清洗石英玻璃基底S11) Cleaning the quartz glass substrate

将折射率为90%,最高耐温为1500℃,厚度为3mm,长度和宽度均为800nm的长方体形状的高纯度石英玻璃基底放置于浓度为0.5mol/L,温度为45℃的HCl溶液中,静置10分钟后,将石英玻璃基底放在50℃左右的纯水中浸泡5分钟,取出石英玻璃基底再用50℃左右的纯水进行二次清洗,完成石英玻璃基底的化学清洗;A high-purity quartz glass substrate with a refractive index of 90%, a maximum temperature resistance of 1500°C, a thickness of 3mm, and a length and width of 800nm was placed in a HCl solution with a concentration of 0.5mol/L and a temperature of 45°C. , after standing for 10 minutes, soak the quartz glass substrate in pure water at about 50 °C for 5 minutes, take out the quartz glass substrate and then use pure water at about 50 °C for secondary cleaning to complete the chemical cleaning of the quartz glass substrate;

S12)烘干石英玻璃基底S12) drying the quartz glass substrate

将经过步骤S11)处理的石英玻璃基底放置在清洗篮上,并向清洗篮内通入温度为80℃左右的高洁净空气或者氮气,持续10~20分钟,待石英玻璃基底和清洗篮充分干燥后,石英玻璃基底的烘干完成;Place the quartz glass substrate processed in step S11) on the cleaning basket, and pass high-clean air or nitrogen gas with a temperature of about 80°C into the cleaning basket for 10 to 20 minutes, until the quartz glass substrate and the cleaning basket are fully dried. After that, the drying of the quartz glass substrate is completed;

S13)旋涂光刻胶S13) Spin coating photoresist

将经过步骤S12)处理的石英玻璃基底吸附在真空卡盘上,调整真空卡盘转速为500rpm,并向石英玻璃基底上表面中心滴入浓度为5%的聚甲基丙烯酸甲酯(polymethylMethacrylate,PMMA)光刻胶,5秒后,将真空卡盘转速提高到3000~7000rpm,甩胶30秒,形成厚度为140nm的光刻胶涂层;The quartz glass substrate processed in step S12) is adsorbed on the vacuum chuck, the rotation speed of the vacuum chuck is adjusted to 500 rpm, and polymethyl methacrylate (PMMA) with a concentration of 5% is dripped into the center of the upper surface of the quartz glass substrate. ) photoresist, after 5 seconds, the speed of the vacuum chuck is increased to 3000-7000rpm, and the glue is spun for 30 seconds to form a photoresist coating with a thickness of 140nm;

S14)匀胶后软烘石英玻璃基底S14) Soft-bake the quartz glass substrate after sizing

待光刻胶在石英玻璃基底上表面涂布均匀后,将经过步骤S13)处理的石英玻璃基底放在80℃的真空热板上软烘2~5分钟;After the photoresist is evenly coated on the upper surface of the quartz glass substrate, the quartz glass substrate processed in step S13) is placed on a vacuum hot plate at 80° C. for soft baking for 2 to 5 minutes;

S2)电子束曝光得到图形S2) Electron beam exposure to obtain a pattern

S21)聚焦电子束曝光S21) Focused electron beam exposure

用光斑尺寸为30nm,加速电压为30KV,曝光剂量25μc/cm2的型号为Raith 150的电子束矢量曝光机对经过步骤S1)处理后的石英玻璃基底进行矢量曝光,利用预设程序控制电子束矢量曝光机以在石英玻璃基底上表面得到光刻胶纳米棒的棒长均为90nm,棒宽均为30nm,厚度均为150nm的光刻胶纳米棒阵列图形,其中光刻胶纳米棒阵列图形中每1行和每1列的光刻胶纳米棒分别与X轴呈45°、-45°夹角间隔排列,且任意两根相邻的光刻胶纳米棒几何中心之间的距离均为180nm。Use a Raith 150 electron beam vector exposure machine with a spot size of 30nm, an acceleration voltage of 30KV, and an exposure dose of 25μc/cm 2 to perform vector exposure on the quartz glass substrate processed in step S1), and use a preset program to control the electron beam. The vector exposure machine is used to obtain photoresist nanorod array patterns with photoresist nanorods on the upper surface of the quartz glass substrate. The rod length is 90 nm, the rod width is 30 nm, and the thickness is 150 nm. The photoresist nanorod array pattern is The photoresist nanorods in each row and column are arranged at an angle of 45° and -45° respectively with the X axis, and the distance between the geometric centers of any two adjacent photoresist nanorods is 180nm.

S22)曝光后烘干石英玻璃基底S22) drying the quartz glass substrate after exposure

将经过步骤S21)处理后的石英玻璃基底放置于170℃的烤箱中,烘烤90分钟,并在常温环境中静置冷却30分钟;Place the quartz glass substrate processed in step S21) in an oven at 170°C, bake for 90 minutes, and stand for 30 minutes in a normal temperature environment;

S3)显影S3) Development

S31)显影、定影S31) developing, fixing

将经过步骤S2)处理后的石英玻璃基底浸没在温度为21±0.2℃的四甲基二戊酮(MIBK)和异丙醇(IPA)以1:3的比例混合的显影液中100秒,然后放入异丙醇溶液中40秒,完成定影,得到位于石英玻璃基底上表面的纳米棒阵列图形;Immerse the quartz glass substrate processed in step S2) in a developing solution in which tetramethyldipentanone (MIBK) and isopropanol (IPA) are mixed at a temperature of 21±0.2° C. in a ratio of 1:3 for 100 seconds, Then put it into the isopropanol solution for 40 seconds to complete the fixing to obtain the nanorod array pattern on the upper surface of the quartz glass substrate;

S32)定影后烘干基片S32) drying the substrate after fixing

取出经过步骤S31)处理后的石英玻璃基底放在80℃的真空热板上软烘2~5分钟,得到位于石英玻璃基底上表面的烘干的纳米棒阵列图形;Take out the quartz glass substrate processed in step S31) and place it on a vacuum hot plate at 80° C. for soft baking for 2 to 5 minutes to obtain a dried nanorod array pattern on the upper surface of the quartz glass substrate;

S33)图形检查、蒸发金属膜S33) Pattern inspection, evaporating metal film

利用扫描电子显微(SEM)观测技术对经过步骤S32)处理后的石英玻璃基底上表面的烘干的纳米棒阵列图形进行检查,确定该烘干的纳米棒阵列图形合格后用热蒸发台对石英玻璃基底蒸发1层25nm厚的金属金(Au);Scanning electron microscopy (SEM) observation technology is used to inspect the dried nanorod array pattern on the upper surface of the quartz glass substrate after step S32), and after confirming that the dried nanorod array pattern is qualified, a thermal evaporation table is used to inspect the pattern. A layer of metal gold (Au) with a thickness of 25 nm was evaporated from a quartz glass substrate;

S34)去除光刻胶得到金属图形S34) remove the photoresist to obtain the metal pattern

对经过步骤S33)处理后的石英玻璃基底进行丙酮剥离,去除残留的电子束光刻胶和金属金,在石英玻璃基底上表面得到金纳米棒阵列,其中,该金纳米棒阵列中的金纳米棒尺寸均为长90nm,宽30nm,厚25nm,金纳米棒阵列中每1行和每1列的金纳米棒分别与X轴呈45°、-45°夹角间隔排列,且任意两根相邻的金纳米棒几何中心之间的距离均为180nm,由此得到特定金属纳米超表面结构。图4是其扫描电子显微镜(SEM)照片,图4中的100nm仅作为标尺。Acetone peeling is performed on the quartz glass substrate treated in step S33), the residual electron beam photoresist and metal gold are removed, and a gold nanorod array is obtained on the upper surface of the quartz glass substrate, wherein the gold nanorods in the gold nanorod array are The rods are all 90nm long, 30nm wide, and 25nm thick. The gold nanorods in each row and column of the gold nanorod array are arranged at an angle of 45° and -45° with the X axis, respectively, and any two of them are in phase. The distances between the geometric centers of adjacent gold nanorods are all 180 nm, thereby obtaining a specific metal nano-metasurface structure. Fig. 4 is a scanning electron microscope (SEM) photograph thereof, and 100 nm in Fig. 4 is only used as a scale.

图2~图3是利用时域有限差分方法仿真由金属纳米棒阵列构成的上述特定金属纳米超表面结构的亚波长周期性旋涡光束产生效果:Figures 2 to 3 show the effect of subwavelength periodic vortex beam generation of the above-mentioned specific metal nano-metasurface structure composed of metal nanorod arrays by using the finite difference time domain method:

首先设置25个分别以横向、纵向与X轴分别呈45°、-45°夹角间隔排列且皆以360nm周期间隔排列的金纳米棒阵列,如图1所示,其中,25个金纳米棒的长度均为90nm,宽度均为30nm,厚度均为25nm,如图1所示;然后将仿真区域设置为400nm×400nm×2000nm,并设置波长为532nm的左旋圆偏振光从特定金属纳米超表面结构的底部垂直照射到该特定金属纳米超表面结构的金纳米棒阵列中;接着在透射区域(Z>0的区域)沿Z轴距离金纳米棒阵列上表面20nm,50nm,100nm,500nm,1000nm,2000nm处分别设置一个场监视器,用以分别监测各监视器所在位置的电场、磁场等;最后通过仿真计算得到透射区域各个位置的电场强度分布,场矢量相位分布等。图3(a)表示特定金属纳米超表面结构的透射区域沿Z轴距离纳米棒阵列100nm处的电场强度分布,其光能量较为集中呈周期性分布;图3(b)表示特定金属纳米超表面结构的透射区域沿Z轴距离纳米棒阵列100nm处的相位分布,可以看到其相位以图3(a)的每个螺旋中心(即光强最强点)为中心,相位呈-π~π螺旋分布。上述仿真结果表明一束圆偏振光垂直照射到本发明制备出的特定金属纳米超表面结构后,从Z=0的XY平面透射出来的圆偏振光转变成了亚波长的涡旋光束阵列;图2是将图3(b)的某一单个涡旋光束的数据单独提取出来重新画图的结果,以得到比较明显的螺旋效果。First, set 25 gold nanorod arrays arranged at 45° and -45° angles in the horizontal, vertical, and X-axis, respectively, and all of them are arranged at 360 nm periodic intervals, as shown in Figure 1. Among them, 25 gold nanorods The lengths are 90nm, the widths are 30nm, and the thicknesses are 25nm, as shown in Figure 1; then the simulation area is set to 400nm × 400nm × 2000nm, and the left-handed circularly polarized light with a wavelength of 532nm is set from the specific metal nano-metasurface The bottom of the structure is irradiated vertically into the gold nanorod array of the specific metal nanometasurface structure; then in the transmission region (Z>0 region) along the Z axis from the upper surface of the gold nanorod array 20nm, 50nm, 100nm, 500nm, 1000nm , a field monitor is set up at 2000nm to monitor the electric field and magnetic field at the location of each monitor respectively; finally, the electric field intensity distribution and field vector phase distribution of each position in the transmission area are obtained through simulation calculation. Figure 3(a) shows the electric field intensity distribution in the transmission region of the specific metal nano-metasurface structure at a distance of 100 nm from the nanorod array along the Z axis, and its light energy is relatively concentrated and periodically distributed; Figure 3(b) shows the specific metal nano-metasurface The phase distribution of the transmission area of the structure along the Z axis at a distance of 100 nm from the nanorod array, it can be seen that the phase is centered on the center of each helix (ie, the strongest point of light intensity) in Figure 3(a), and the phase is -π ~ π Spiral distribution. The above simulation results show that after a beam of circularly polarized light is vertically irradiated to the specific metal nano-metasurface structure prepared by the present invention, the circularly polarized light transmitted from the XY plane of Z=0 is transformed into a subwavelength vortex beam array; Fig. 2 is the result of separately extracting the data of a single vortex beam in Fig. 3(b) and redrawing it, so as to obtain a more obvious helical effect.

本发明通过合理设计金属纳米棒的尺寸及排布,并利用电子束刻蚀这一较成熟的微纳加工方法,制备出可产生亚波长旋涡光束阵列的周期性金属纳米棒超表面。相较于其他旋涡光束产生方式,本发明所用方法具有结构简单、和易于集成、光强分布均匀等优点。并且该方法产生的涡旋光束阵列不仅能够在信息传输与存储中增强信息安全性与容量,在微粒捕获中一次性捕获大量粒子,而且能同时探测不同物体的运动特性,拓展了旋涡光束的应用领域。The present invention prepares a periodic metal nanorod metasurface capable of generating subwavelength vortex beam arrays by rationally designing the size and arrangement of the metal nanorods and using electron beam etching, a relatively mature micro-nano processing method. Compared with other vortex beam generating methods, the method used in the present invention has the advantages of simple structure, easy integration, uniform light intensity distribution, and the like. In addition, the vortex beam array generated by this method can not only enhance information security and capacity in information transmission and storage, capture a large number of particles at one time in particle capture, but also detect the motion characteristics of different objects at the same time, expanding the application of vortex beams. field.

尽管上面对本发明说明性的具体实施方式进行了描述,以便于本技术领域的技术人员理解本发明,但应该清楚,本发明不限于具体实时方式的范围。凡采用等同替换或等效替换,这些变化是显而易见,一切利用本发明构思的发明创造均在保护之列。While illustrative specific embodiments of the present invention have been described above to facilitate understanding of the invention by those skilled in the art, it should be clear that the invention is not limited in scope to specific real-time implementations. Where equivalent replacements or equivalent replacements are adopted, these changes are obvious, and all inventions and creations utilizing the concept of the present invention are included in the protection list.

Claims (9)

1. A method for generating a sub-wavelength vortex beam array based on a metal nano super surface is characterized by comprising the steps of firstly preparing a specific metal nano super surface structure which is formed by a metal nanorod array and a quartz glass substrate and is integrally in a cuboid shape, wherein the metal nanorod array comprises n metal nanorods, n is a positive integer and is greater than 4, the metal nanorods are periodically distributed on the upper surface of the quartz glass substrate, the specific metal nano super surface structure is emitted from an original point which is any point in a plane where the upper surface of the metal nanorod array is located, the length and width directions of the specific metal nano super surface structure are respectively an X axis and a Y axis, and the reverse direction of the thickness of the specific metal nano super surface structure is a Z axis; then, circularly polarized light with the wavelength of 532nm is vertically irradiated to the specific metal nano super-surface structure from a region with the Z being less than 0, after the circularly polarized light acts with any one metal nanorod, a phase factor 2 theta is added to the light wave phase, wherein theta is the included angle between the long axis of any one metal nanorod and the X axis, because the included angle theta between the long axis of each metal nanorod and the X axis is different, the circularly polarized light transmitted from the XY plane at the position with the Z being 0 presents different phases at different positions of a transmission region with the Z being more than 0, 4 metal nanorods adjacent in the two directions of the X axis and the Y axis generate a vortex light beam, the diameter of the vortex light beam is 180nm, and due to the action of the metal nanorod array, a vortex light beam array with the sub-wavelength scale with uniform light energy distribution and spiral phase distribution is generated in the transmission region with the Z being more than;
wherein, the preparation method of the specific metal nano super surface structure comprises the following steps:
s1) spin-coating photoresist on a quartz glass substrate
S11) cleaning the silica glass substrate
Placing an original quartz glass substrate in a cuboid shape in HCl solution with the concentration of 0.5mol/L and the temperature of 35-50 ℃, standing for 10 minutes, placing the quartz glass substrate in pure water with the temperature of about 50 ℃ for soaking for 5 minutes, taking out the quartz glass substrate, and then carrying out secondary cleaning by using the pure water with the temperature of about 50 ℃ to complete the chemical cleaning of the quartz glass substrate;
s12) drying the quartz glass substrate
Placing the quartz glass substrate treated in the step S11) on a cleaning basket, introducing high-clean air or nitrogen at the temperature of about 80 ℃ into the cleaning basket for 10-20 minutes, and drying the quartz glass substrate after the quartz glass substrate and the cleaning basket are fully dried;
s13) spin-on resist
Adsorbing the quartz glass substrate treated in the step S12) on a vacuum chuck, adjusting the rotating speed of the vacuum chuck to 500rpm, dripping photoresist into the center of the upper surface of the quartz glass substrate, and after 5 seconds, increasing the rotating speed of the vacuum chuck to 3000-7000 rpm, and spinning the photoresist for 30 seconds to form a photoresist coating with the thickness of 140 nm;
s14) soft baking of quartz glass substrate after glue homogenizing
After the photoresist is uniformly coated on the upper surface of the quartz glass substrate, placing the quartz glass substrate treated in the step S13) on a vacuum hot plate at 80 ℃ for soft baking for 2-5 minutes;
s2) exposing with electron beam to obtain pattern
S21) focused electron beam exposure
Accelerating voltage of 30KV, light spot size of 30nm, and exposure dose of 25 μ c/cm2Exposing the quartz glass substrate processed in the step S1), and controlling the electron beam vector exposure machine by using a preset program to obtain a photoresist nanorod array pattern with the length of each nanorod being 90nm, the width of each nanorod being 30nm and the thickness of each nanorod being 140-150 nm on the upper surface of the quartz glass substrate, wherein the photoresist nanorods of each row and each column in the photoresist nanorod array pattern are respectively arranged at intervals at an included angle of 45 degrees to 45 degrees with the X axis, and the distance between the geometric centers of any two adjacent photoresist nanorods is 180 nm;
s22) baking the quartz glass substrate after exposure
Placing the quartz glass substrate treated in the step S21) in an oven at 150-170 ℃, baking for 90 minutes, and standing and cooling for 30 minutes in a normal temperature environment;
s3) development
S31) developing and fixing
Immersing the quartz glass substrate processed in the step S2) in a developing solution at the temperature of 21 +/-0.2 ℃ for 60-120 seconds, and then putting the quartz glass substrate in an isopropanol solution for 30-40 seconds to complete fixation, so as to obtain a nanorod array pattern on the upper surface of the quartz glass substrate;
s32) post-fixing baking substrate
Taking out the quartz glass substrate treated in the step S31), and placing the quartz glass substrate on a vacuum hot plate at 80 ℃ for soft drying for 2-5 minutes to obtain a dried nanorod array pattern on the upper surface of the quartz glass substrate;
s33) pattern inspection, evaporating the metal film
Inspecting the dried nanorod array pattern on the upper surface of the quartz glass substrate treated in the step S32) by using a scanning electron microscopy observation technology, and evaporating metal gold (Au) on the quartz glass substrate by using a thermal evaporation table after determining that the dried nanorod array pattern is qualified, wherein the thickness of the gold (Au) is 20-30 nm;
s34) removing the photoresist to obtain a metal pattern
And (2) stripping the quartz glass substrate treated in the step S33) with acetone to remove residual electron beam photoresist and metal gold, and obtaining a gold nanorod array on the upper surface of the quartz glass substrate, wherein the sizes of the gold nanorods in the gold nanorod array are all 90nm long, 30nm wide and 25nm thick, every 1 row and every 1 column of the gold nanorods in the gold nanorod array are respectively arranged at intervals with an included angle of 45 degrees to 45 degrees with the X axis, and the distance between the geometric centers of any two adjacent gold nanorods is 180nm, so that the specific metal nano super-surface structure is obtained.
2. The method for generating a sub-wavelength vortex beam array based on metal nano-super surface according to claim 1, wherein the original quartz glass substrate in the step S11) is high-purity quartz glass with a thickness of 3mm, a length and a width of 800nm, a light transmittance of more than 90% and a maximum temperature resistance of 1500 ℃.
3. The method for generating the sub-wavelength vortex beam array based on the metal nano-super surface according to claim 2, wherein the photoresist in the step S13) is polymethyl methacrylate (PMMA) with a concentration of 5%.
4. The method as claimed in claim 3, wherein the developing solution of step S31) is a mixture of tetramethylcyclopentanone (MIBK) and isopropyl alcohol (IPA) at a ratio of 1: 3.
5. The method for generating the sub-wavelength vortex beam array based on the metal nano-super surface according to claim 3, wherein the temperature of the HCl solution in the step S11) is 45 ℃.
6. The method for generating the sub-wavelength vortex beam array based on the metal nano-super surface according to claim 4, wherein the oven temperature in the step S22) is 170 ℃.
7. The method for generating the sub-wavelength vortex beam array based on the metal nano-super surface according to claim 5, wherein the quartz glass substrate is immersed in the developing solution for 100 seconds and placed in the isopropanol solution for 40 seconds in the step S31).
8. The method for generating the sub-wavelength vortex beam array based on the metal nano-super surface according to claim 5, wherein the thickness of the gold (Au) in the step S33) is 25 nm.
9. The method for generating the sub-wavelength vortex beam array based on the metal nano-super surface according to any one of claims 1 to 8, wherein the circularly polarized light is left-handed circularly polarized light.
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