CN101782666A - Helical metal wire grating circuit polarizer - Google Patents
Helical metal wire grating circuit polarizer Download PDFInfo
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- 229910052751 metal Inorganic materials 0.000 title claims abstract description 47
- 239000002184 metal Substances 0.000 title claims abstract description 47
- 239000000758 substrate Substances 0.000 claims abstract description 15
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims abstract description 12
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims abstract description 10
- 230000000737 periodic effect Effects 0.000 claims description 8
- 239000000463 material Substances 0.000 claims description 6
- 229910052782 aluminium Inorganic materials 0.000 claims description 5
- 238000002834 transmittance Methods 0.000 abstract description 20
- 230000003287 optical effect Effects 0.000 abstract description 16
- 230000008033 biological extinction Effects 0.000 abstract description 14
- 230000010287 polarization Effects 0.000 abstract description 3
- 238000001874 polarisation spectroscopy Methods 0.000 abstract description 2
- 238000001228 spectrum Methods 0.000 abstract description 2
- 239000007787 solid Substances 0.000 description 6
- 229920002120 photoresistant polymer Polymers 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 4
- 239000010931 gold Substances 0.000 description 4
- 229910052737 gold Inorganic materials 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 238000002360 preparation method Methods 0.000 description 4
- 238000004070 electrodeposition Methods 0.000 description 3
- 239000007769 metal material Substances 0.000 description 3
- 230000001427 coherent effect Effects 0.000 description 2
- 238000005530 etching Methods 0.000 description 2
- 238000001459 lithography Methods 0.000 description 1
- 239000002070 nanowire Substances 0.000 description 1
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Abstract
一种螺旋状金属线栅圆偏振器,属于光学器件,目的在于使其在可见光波段具有较宽的工作波长,且器件尺寸小、结构紧凑、易于集成。本发明的圆偏振器,在石英玻璃基板上沉积有N个均匀分布的螺旋状的铝金属线栅,金属线栅直径40-60纳米,螺旋状的螺旋周期数大于等于2周,螺旋状的金属线栅间距190-290纳米,螺旋周期间距150-400纳米,螺旋直径100纳米,N≥106。本发明能够工作在可见光光谱范围,工作波长范围可以达到580-730纳米,偏振消光比大于8.8∶1,偏振光透过率大于67%,且器件尺寸小、结构紧凑、易于集成,适用于偏振分光、彩色显示、激光技术等领域。
The invention discloses a helical metal wire grid circular polarizer, which belongs to an optical device, and aims to make it have a wider working wavelength in the visible light band, and the device has a small size, a compact structure, and is easy to integrate. In the circular polarizer of the present invention, N evenly distributed helical aluminum metal wire grids are deposited on the quartz glass substrate, the metal wire grids have a diameter of 40-60 nanometers, and the number of helical helical periods is greater than or equal to 2 weeks. The pitch of the metal wire grid is 190-290 nanometers, the pitch of the helix is 150-400 nanometers, the diameter of the helix is 100 nanometers, and N≥10 6 . The invention can work in the visible light spectrum range, the working wavelength range can reach 580-730 nanometers, the polarization extinction ratio is greater than 8.8:1, the polarized light transmittance is greater than 67%, and the device is small in size, compact in structure and easy to integrate, and is suitable for polarization Spectroscopy, color display, laser technology and other fields.
Description
技术领域technical field
本发明属于光学器件,特别涉及一种螺旋状金属线栅圆偏振器。The invention belongs to optical devices, in particular to a spiral metal wire grid circular polarizer.
背景技术Background technique
圆偏振器是光学领域的一种重要偏振元器件,它在偏振分光、彩色显示、激光技术等领域得到了令人瞩目的应用。目前在光学领域,通常做法是利用线偏振片和四分之一波片两个分离元器件构成圆偏振器,其工作原理是:光束通过线偏振片后成为线偏振光,然后再以一定偏振角度通过四分之一波片,最终得到圆偏振光。这种结构的缺点非常明显:1.工作波长范围较窄,这主要是因为四分之一波片的工作波长范围较窄,因此该结构不能得到宽波长范围的圆偏振光;2.该结构使用的是两个分离光学元件,因此器件尺寸大,不易集成。Circular polarizer is an important polarizing component in the field of optics. It has been widely used in polarization splitting, color display, laser technology and other fields. At present, in the field of optics, it is common practice to use two separate components, a linear polarizer and a quarter-wave plate, to form a circular polarizer. The angle is passed through a quarter-wave plate, and circularly polarized light is finally obtained. The disadvantages of this structure are very obvious: 1. The working wavelength range is narrow, mainly because the working wavelength range of the quarter-wave plate is narrow, so this structure cannot obtain circularly polarized light with a wide wavelength range; 2. The structure Two separate optical components are used, so the device size is large and not easy to integrate.
利用螺旋状金属线栅获得圆偏振光是在2009年9月由德国卡尔斯鲁厄大学的研究人员首先发现的,见Justyna K.Gansel,等.“Circular Polarizer Gold HelixPhotonic Metamaterial as Broadband,”Science 325,1513(2009)。但是他们研究范围仅局限于下面两个方面:1.金属线栅材料为金;2.工作波长范围在3-6微米的红外波段。由于他们所使用的材料金在可见光范围内的光学特性远不如材料铝好,以及他们提出的螺旋状金属线栅尺寸过大,所以根本不能适用于可见光波段。另外,他们也没有提出适用于其它波段的圆偏振器的结构,也没有对其它金属材料进行讨论。Obtaining circularly polarized light using a helical metal wire grid was first discovered by researchers at the University of Karlsruhe in Germany in September 2009, see Justyna K.Gansel, et al. "Circular Polarizer Gold Helix Photonic Metamaterial as Broadband," Science 325 , 1513 (2009). But their research scope is limited to the following two aspects: 1. The metal wire grid material is gold; 2. The working wavelength range is in the infrared band of 3-6 microns. Since the optical properties of the gold they used in the visible light range are far inferior to the aluminum material, and the helical metal wire grid they proposed is too large, it cannot be applied to the visible light band at all. In addition, they did not propose the structure of circular polarizers suitable for other wavelength bands, nor did they discuss other metal materials.
发明内容Contents of the invention
本发明提出一种螺旋状金属线栅圆偏振器,目的在于使其在可见光波段具有较宽的工作波长范围,且器件尺寸小、结构紧凑、易于集成。The invention proposes a helical metal wire grid circular polarizer with the purpose of making it have a wider working wavelength range in the visible light band, and the device has a small size, a compact structure and is easy to integrate.
本发明的一种螺旋状金属线栅圆偏振器,在基板上沉积有N个均匀分布的螺旋状的金属线栅,其特征在于:A spiral metal wire grid circular polarizer of the present invention has N uniformly distributed spiral metal wire grids deposited on the substrate, and is characterized in that:
所述基板为石英玻璃;所述金属线栅的材料为金属铝,金属线栅直径40-60纳米,螺旋状的螺旋周期数大于等于2周,螺旋状的金属线栅间距190-290纳米,螺旋周期间距150-400纳米,螺旋直径100纳米,N≥106。The substrate is quartz glass; the material of the metal wire grid is metal aluminum, the diameter of the metal wire grid is 40-60 nanometers, the number of helical helical periods is greater than or equal to 2, and the pitch of the helical metal wire grid is 190-290 nanometers. The helical periodic pitch is 150-400 nanometers, the helical diameter is 100 nanometers, and N≥10 6 .
本发明螺旋状金属线栅圆偏振器的制备方法,包括下述步骤:The preparation method of the spiral metal wire grid circular polarizer of the present invention comprises the following steps:
(1).在基板表面沉积导电膜;(1). Deposit a conductive film on the surface of the substrate;
(2).在导电膜上旋涂光刻胶;(2). Spin-coat photoresist on the conductive film;
(3).通过深紫外相干刻蚀,在光刻胶中形成几十纳米量级N个均匀分布的螺旋状空气隙;(3). Through deep ultraviolet coherent etching, N uniformly distributed helical air gaps on the order of tens of nanometers are formed in the photoresist;
(4).通过电化学沉积,在N个均匀分布的螺旋状空气隙中沉积金属材料,形成螺旋状的金属线栅;(4). By electrochemical deposition, metal materials are deposited in N uniformly distributed spiral air gaps to form a spiral metal wire grid;
(5).除去螺旋状的金属线栅之间的光刻胶。(5). Remove the photoresist between the spiral metal wire grids.
在制备过程中,步骤(3)和步骤(4)是比较重要的两个步骤。形成几十纳米线宽的结构对于一般光刻来讲有一定难度,2007年美国一研究小组成功的运用深紫外相干刻蚀的方法得到了大范围线宽小于40纳米的金属线栅结构,见J.J.Wang,F.Walters,X.M.Liu,P.Sciortino,and X.G.Deng,“High-performance,large area,deep ultraviolet to infrared polarizers based on 40nm line/78nm spacenanowire grids,”Appl.Phys.Lett.90,61104(2007);这为步骤(3)的实施提供了依据。另外,运用电化学沉积的方法在螺旋结构中沉积金属材料也是完全可行的,见Justyna K.Gansel,等.“Circular Polarizer Gold Helix Photonic Metamaterialas Broadband,”Science 325,1513(2009)。In the preparation process, step (3) and step (4) are two more important steps. Forming a structure with a line width of tens of nanometers is difficult for general lithography. In 2007, a research team in the United States successfully used the method of deep ultraviolet coherent etching to obtain a large-scale metal wire grid structure with a line width of less than 40 nanometers. See J.J.Wang, F.Walters, X.M.Liu, P.Sciortino, and X.G.Deng, "High-performance, large area, deep ultraviolet to infrared polarizers based on 40nm line/78nm spacenanowire grids," Appl.Phys.Lett.90, 61104 (2007); this provides a basis for the implementation of step (3). In addition, it is completely feasible to deposit metal materials in a helical structure by electrochemical deposition, see Justyna K. Gansel, et al. "Circular Polarizer Gold Helix Photonic Metamaterialas Broadband," Science 325, 1513 (2009).
与现有螺旋状圆偏振器相比,通过调整和优化螺旋状金属纳米线栅的参数(如:线栅直径、螺旋周期数等),本发明能够工作在波长更短的可见光光谱范围,其工作波长范围可以达到580-730纳米,偏振消光比大于8.8∶1,偏振光透过率大于67%,优于现有的可见光偏振器,且器件尺寸小、结构紧凑、易于集成,适用于偏振分光、彩色显示、激光技术等领域。Compared with the existing helical circular polarizer, by adjusting and optimizing the parameters of the helical metal nanowire grid (such as: wire grid diameter, number of helical periods, etc.), the present invention can work in the visible light spectrum range with a shorter wavelength, and its The working wavelength range can reach 580-730 nanometers, the polarization extinction ratio is greater than 8.8:1, and the polarized light transmittance is greater than 67%, which is superior to existing visible light polarizers, and the device is small in size, compact in structure, easy to integrate, and suitable for polarization Spectroscopy, color display, laser technology and other fields.
附图说明Description of drawings
图1(a)为本发明的结构示意图;Fig. 1 (a) is the structural representation of the present invention;
图1(b)为本发明的俯视图;Fig. 1 (b) is the top view of the present invention;
图l(c)为本发明的侧视图;Fig. 1 (c) is the side view of the present invention;
图2(a)为用FDTD算法模拟左旋圆偏光经过本发明时,不同时刻光场的分布图;Fig. 2 (a) is the distribution diagram of the light field at different times when the FDTD algorithm is used to simulate left-handed circularly polarized light passing through the present invention;
图2(b)为为用FDTD算法模拟右旋圆偏光经过本发明时,不同时刻光场的分布图;Fig. 2 (b) is for using the FDTD algorithm to simulate right-handed circularly polarized light passing through the present invention, the distribution diagram of the light field at different times;
图3为实施例1的光学特性曲线;Fig. 3 is the optical characteristic curve of
图4为实施例2的光学特性曲线;Fig. 4 is the optical characteristic curve of
图5为实施例3的光学特性曲线;Fig. 5 is the optical characteristic curve of
图6为实施例4的光学特性曲线;Fig. 6 is the optical characteristic curve of
图7为实施例5的光学特性曲线;Fig. 7 is the optical characteristic curve of embodiment 5;
图8为实施例6的光学特性曲线;Fig. 8 is the optical characteristic curve of embodiment 6;
图9(a)~图9(e)为本发明的制备方法工艺流程图。Fig. 9(a) to Fig. 9(e) are process flow diagrams of the preparation method of the present invention.
具体实施方式Detailed ways
如图1(a)~图1(c)所示,本发明在基板1上沉积有N个均匀分布的螺旋状的金属线栅2,所述基板为石英玻璃;所述金属线栅的材料为金属铝,金属线栅直径SD为40-60纳米,螺旋状的螺旋周期数CN大于等于2,螺旋状的金属线栅间距CW为190-290纳米,螺旋周期间距CS为150-400纳米,螺旋直径CD为100纳米,N≥106。As shown in Fig. 1 (a) ~ Fig. 1 (c), the present invention is deposited with N uniformly distributed spiral
图2(a)为用FDTD算法模拟左旋圆偏光经过本发明时,不同时刻光场的分布图;图2(b)为为用FDTD算法模拟右旋圆偏光经过本发明时,不同时刻光场的分布图;从图中可以看出左旋圆偏振光在经过偏振器后,大部分能量被反射掉了,而右旋圆偏振光的大部分能量则可以顺利的通过偏振器。Fig. 2 (a) is the distribution diagram of the light field at different times when simulating left-handed circularly polarized light with the FDTD algorithm passes through the present invention; It can be seen from the figure that most of the energy of the left-handed circularly polarized light is reflected after passing through the polarizer, while most of the energy of the right-handed circularly polarized light can pass through the polarizer smoothly.
实施例1:石英玻璃基板1上沉积有106个均匀分布的螺旋状的铝金属线栅2,金属线栅直径SD为40纳米,螺旋状的螺旋周期数CN等于2,螺旋状的金属线栅间距CW为190纳米,螺旋周期间距CS为200纳米,螺旋直径CD为100纳米;Embodiment 1: 10 6 evenly distributed helical aluminum
图3所示为实施例1的光学特性曲线,图中,空心矩形框描绘的曲线为右旋圆偏振光透过率,空心三角形框描绘的曲线为左旋圆偏振光透过率,黑色实心框描绘的曲线为消光比;Fig. 3 shows the optical characteristic curve of
本实施例工作波长范围、平均透过率、平均消光比分别为0.5~0.75μm、73%、19.7∶1。In this embodiment, the working wavelength range, average transmittance, and average extinction ratio are 0.5-0.75 μm, 73%, and 19.7:1, respectively.
实施例2:石英玻璃基板1上沉积有106个均匀分布的螺旋状的铝金属线栅2,金属线栅直径SD为60纳米,螺旋状的螺旋周期数CN等于2,螺旋状的金属线栅间距CW为190纳米,螺旋周期间距CS为200纳米,螺旋直径CD为100纳米;Embodiment 2: 10 6 evenly distributed helical aluminum
图4所示为实施例2的光学特性曲线,图中,空心矩形框描绘的曲线为右旋圆偏振光透过率,空心三角形框描绘的曲线为左旋圆偏振光透过率,黑色实心框描绘的曲线为消光比;Fig. 4 shows the optical characteristic curve of
本实施例工作波长范围、平均透过率、平均消光比分别为0.4-0.77μm、69%、26.3∶1。In this embodiment, the working wavelength range, average transmittance, and average extinction ratio are 0.4-0.77 μm, 69%, and 26.3:1, respectively.
实施例3:石英玻璃基板1上沉积有106个均匀分布的螺旋状的铝金属线栅2,金属线栅直径SD为40纳米,螺旋状的螺旋周期数CN等于4,螺旋状的金属线栅间距CW为190纳米,螺旋周期间距CS为200纳米,螺旋直径CD为100纳米;Embodiment 3: 10 6 evenly distributed helical aluminum
图5所示为实施例3的光学特性曲线,图中,空心矩形框描绘的曲线为右旋圆偏振光透过率,空心三角形框描绘的曲线为左旋圆偏振光透过率,黑色实心框描绘的曲线为消光比;Fig. 5 shows the optical characteristic curve of
本实施例工作波长范围、平均透过率、平均消光比分别为0.42-0.83μm、58%、46.3∶1。In this embodiment, the working wavelength range, average transmittance, and average extinction ratio are 0.42-0.83 μm, 58%, and 46.3:1, respectively.
实施例4:石英玻璃基板1上沉积有106个均匀分布的螺旋状的铝金属线栅2,金属线栅直径SD为40纳米,螺旋状的螺旋周期数CN等于2,螺旋状的金属线栅间距CW为290纳米,螺旋周期间距CS为200纳米,螺旋直径CD为100纳米;Embodiment 4: 10 6 uniformly distributed helical aluminum
图6所示为实施例4的光学特性曲线,图中,空心矩形框描绘的曲线为右旋圆偏振光透过率,空心三角形框描绘的曲线为左旋圆偏振光透过率,黑色实心框描绘的曲线为消光比;Fig. 6 shows the optical characteristic curve of
本实施例工作波长范围、平均透过率、平均消光比分别为0.55-0.73μm、85%、8.8∶1。In this embodiment, the working wavelength range, average transmittance, and average extinction ratio are 0.55-0.73 μm, 85%, and 8.8:1, respectively.
实施例5:石英玻璃基板1上沉积有106个均匀分布的螺旋状的铝金属线栅2,金属线栅直径SD为40纳米,螺旋状的螺旋周期数CN等于2,螺旋状的金属线栅间距CW为190纳米,螺旋周期间距CS为150纳米,螺旋直径CD为100纳米;Embodiment 5: 10 6 uniformly distributed helical aluminum
图7所示为实施例5的光学特性曲线,图中,空心矩形框描绘的曲线为右旋圆偏振光透过率,空心三角形框描绘的曲线为左旋圆偏振光透过率,黑色实心框描绘的曲线为消光比;Fig. 7 shows the optical characteristic curve of embodiment 5, among the figure, the curve that hollow rectangular frame depicts is right-handed circularly polarized light transmittance, the curve that hollow triangular frame depicts is left-handed circularly polarized light transmittance, black solid frame The curve depicted is the extinction ratio;
本实施例工作波长范围、平均透过率、平均消光比分别为0.39-0.79μm、67%、12.1∶1。In this embodiment, the working wavelength range, average transmittance, and average extinction ratio are 0.39-0.79 μm, 67%, and 12.1:1, respectively.
实施例6:石英玻璃基板1上沉积有106个均匀分布的螺旋状的铝金属线栅2,金属线栅直径SD为40纳米,螺旋状的螺旋周期数CN等于2,螺旋状的金属线栅间距CW为190纳米,螺旋周期间距CS为400纳米,螺旋直径CD为100纳米;Embodiment 6: 10 6 evenly distributed helical aluminum
图8所示为实施例6的光学特性曲线,图中,空心矩形框描绘的曲线为右旋圆偏振光透过率,空心三角形框描绘的曲线为左旋圆偏振光透过率,黑色实心框描绘的曲线为消光比;Fig. 8 shows the optical characteristic curve of embodiment 6, among the figure, the curve that the hollow rectangular frame depicts is the right-handed circularly polarized light transmittance, the curve that the hollow triangular frame depicts is the left-handed circularly polarized light transmittance, and the black solid frame The curve depicted is the extinction ratio;
本实施例工作波长范围、平均透过率、平均消光比分别为0.58-0.75μm、78%、138∶1。In this embodiment, the working wavelength range, average transmittance, and average extinction ratio are 0.58-0.75 μm, 78%, and 138:1, respectively.
图9(a)~图9(e)所示为本发明的制备方法工艺流程图。图9(a).在基板表面沉积导电膜;图9(b).在导电膜上旋涂光刻胶;图9(c).通过深紫外相干刻蚀,在光刻胶中形成几十纳米量级N个均匀分布的螺旋状空气隙;图9(d).通过电化学沉积,在N个均匀分布的螺旋状空气隙中沉积金属铝材料,形成螺旋状的金属线栅;图9(e).除去螺旋状的金属线栅之间的光刻胶,最终形成螺旋状金属线栅圆偏振器。Figure 9(a) to Figure 9(e) show the process flow chart of the preparation method of the present invention. Figure 9(a). Deposit a conductive film on the surface of the substrate; Figure 9(b). Spin-coat photoresist on the conductive film; Figure 9(c). Form tens of N uniformly distributed helical air gaps at the nanoscale; Figure 9(d). Metal aluminum materials are deposited in N uniformly distributed helical air gaps by electrochemical deposition to form a helical metal wire grid; Figure 9 (e). Removing the photoresist between the helical metal wire grids to finally form a helical metal wire grid circular polarizer.
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