CN2842451Y - Polarization beam splitter based on photon crystal positive-negative refraction - Google Patents
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Abstract
一种基于光子晶体正负折射的偏振分束器。在衬底上的介质材料中二维周期性排列的空气柱子阵列,或金属柱子阵列,或另一种介质材料柱子阵列构成光子晶体;或在衬底上以二维周期性排列的金属柱子阵列或介质材料柱子阵列构成光子晶体。入射电磁波波束从环境界面入射后,一个在环境界面上经历负折射,入射电磁波波束和折射电磁波波束在光子晶体与环境界面的法线的同一侧;另一个在环境界面上经历正折射,入射电磁波波束和折射电磁波波束分别位于法线的两侧,把两个偏振态的电磁波波束分开,实现偏振分束。本实用新型利用光子晶体实现了偏振分光,两个偏振态的电磁波束都工作在透射模式,具有小尺寸、易于集成、工艺简单等优点,可以用于微波段和光波段。
A polarizing beam splitter based on photonic crystal positive and negative refraction. A two-dimensional periodic array of air pillars in the dielectric material on the substrate, or an array of metal pillars, or another dielectric material pillar array constitutes a photonic crystal; or a two-dimensional periodic array of metal pillars on the substrate Or an array of dielectric material pillars constitutes a photonic crystal. After the incident electromagnetic wave beam is incident from the environmental interface, one experiences negative refraction on the environmental interface, and the incident electromagnetic wave beam and the refracted electromagnetic wave beam are on the same side of the normal line between the photonic crystal and the environmental interface; the other experiences positive refraction on the environmental interface, and the incident electromagnetic wave beam The wave beam and the refracted electromagnetic wave beam are respectively located on both sides of the normal line, and the electromagnetic wave beams of the two polarization states are separated to realize polarization beam splitting. The utility model realizes polarization splitting by using photonic crystals, and the electromagnetic wave beams of two polarization states work in the transmission mode, has the advantages of small size, easy integration, simple process, etc., and can be used in microwave and optical bands.
Description
技术领域technical field
本实用新型涉及偏振分束器件,特别是一种基于光子晶体正负折射的偏振分束器。The utility model relates to a polarization beam splitter, in particular to a polarization beam splitter based on positive and negative refraction of photonic crystals.
背景技术Background technique
光子晶体(Photonic Crystal)是一种人工制作的周期性结构[J.D.Joannopoulos,Photonic crystals:Molding the flow of light,Princeton,1995],利用介质材料如氧化铝、二氧化硅、硅、砷化镓、磷化铟等制作的二维周期性结构,也可以是在介质背景中二维周期性分布的金属柱子阵列。所述的二维周期性是指,阵列中任何相邻的三个柱子的中心的连线构成等腰直角三角形的正方晶格,或构成等边三角形的三角晶格。最短连线的长度称为晶格常数。因为微波和光波同为电磁波,它们的行为同样遵循Maxwell方程,所以光子晶体可以应用在微波段和光波段,只是两个波段的尺寸大小不同。Photonic Crystal (Photonic Crystal) is an artificial periodic structure [J.D.Joannopoulos, Photonic crystals: Molding the flow of light, Princeton, 1995], using dielectric materials such as alumina, silicon dioxide, silicon, gallium arsenide, The two-dimensional periodic structure made of indium phosphide can also be a two-dimensional periodic distribution of metal pillar arrays in the dielectric background. The two-dimensional periodicity means that the line connecting the centers of any three adjacent pillars in the array forms a square lattice of isosceles right triangles, or a triangular lattice of equilateral triangles. The length of the shortest line is called the lattice constant. Because microwaves and light waves are both electromagnetic waves, and their behaviors also follow the Maxwell equation, photonic crystals can be applied in both microwave and light bands, but the sizes of the two bands are different.
对于普通的材料,电磁波束在不同材料的界面上发生的是正折射,即,入射波[如光子晶体,M.Notomi,Theory oflight propagation in strongly modulatedphotonic crystals:Refractionlike behavior in the vicinity of the photonic band gap,Phys.Rev.B 62,10696,2000]与周围环境(如普通材料或空气)的界面上,电磁波束可以发生负折射,即,入射波束和折射波束在界面法线的同一侧。For ordinary materials, what happens to the electromagnetic beam at the interface of different materials is positive refraction, that is, the incident wave [such as photonic crystal, M. Phys.Rev.B 62, 10696, 2000] At the interface with the surrounding environment (such as ordinary materials or air), the electromagnetic beam can be negatively refracted, that is, the incident beam and the refracted beam are on the same side of the interface normal.
文献[S.Kim,Opt.Lett.28,2384,2003]利用光子晶体的不同偏振态的禁带位置不同设计了一种偏振分束器,即一个偏振态的电磁波束可以透过光子晶体,而另一个偏振态的电磁波束被反射。文献[X.Y.Chen,Chinese Phys.Lett.21,1285,2004]设计了光子晶体线缺陷Y型分支波导,一个分支波导透过一个偏振态的电磁波而反射另一个偏振态的电磁波,另一个分支波导则反过来。Literature [S.Kim, Opt.Lett.28, 2384, 2003] designed a polarization beam splitter by using the different positions of the forbidden bands of different polarization states of photonic crystals, that is, the electromagnetic beam of one polarization state can pass through the photonic crystal, The electromagnetic beam of the other polarization state is reflected. Literature [X.Y.Chen, Chinese Phys.Lett.21, 1285, 2004] designed a photonic crystal line defect Y-shaped branch waveguide, one branch waveguide transmits electromagnetic waves of one polarization state and reflects electromagnetic waves of another polarization state, and the other branch waveguide the other way around.
发明内容Contents of the invention
本实用新型的目的是提供一种基于光子晶体正负折射的偏振分束器。The purpose of the utility model is to provide a polarization beam splitter based on positive and negative refraction of photonic crystals.
本实用新型采用的技术方案是:The technical scheme that the utility model adopts is:
一、基于光子晶体正负折射的偏振分束器,有二种结构形式:1. Polarizing beam splitters based on positive and negative refraction of photonic crystals have two structural forms:
1)在衬底上的介质材料中二维周期性排列的空气柱子阵列,或金属柱子阵列,或另一种介质材料柱子阵列构成光子晶体。1) A two-dimensional periodic array of air pillars, or a metal pillar array, or another dielectric material pillar array in the dielectric material on the substrate constitutes a photonic crystal.
2)在衬底上以二维周期性排列的金属柱子阵列或介质材料柱子阵列构成光子晶体。2) A photonic crystal is composed of a two-dimensional periodic array of metal pillars or dielectric material pillars on the substrate.
所述的二维周期性是指,阵列中任何相邻的三个柱子的中心的连线构成等腰直角三角形的正方晶格,或构成等边三角形的三角晶格。The two-dimensional periodicity means that the line connecting the centers of any three adjacent pillars in the array forms a square lattice of isosceles right triangles, or a triangular lattice of equilateral triangles.
所述的阵列的形状为长方形或三角形。The shape of the array is rectangle or triangle.
二、基于光子晶体正负折射效应的偏振分束方法:以长方形或三角形的光子晶体,作为电磁波的偏振分束元件,入射电磁波波束含有两个偏振态,从环境界面入射后,其中一个偏振态的电磁波束在环境界面上经历负折射,入射电磁波波束和折射电磁波波束在光子晶体与环境界面的法线的同一侧;另一个偏振态的电磁波波束在光子晶体与环境界面上经历正折射,入射电磁波波束和折射电磁波波束分别位于法线的两侧,从而把两个偏振态的电磁波波束分开,实现偏振分束。2. Polarization beam splitting method based on positive and negative refraction effects of photonic crystals: Rectangular or triangular photonic crystals are used as polarization beam splitting elements of electromagnetic waves. The incident electromagnetic wave beam contains two polarization states. After incident from the environmental interface, one of the polarization states The electromagnetic beam of the polarization state experiences negative refraction on the interface of the environment, and the incident electromagnetic wave beam and the refracted electromagnetic wave beam are on the same side of the normal line of the photonic crystal and the environment interface; the electromagnetic wave beam of the other polarization state experiences positive refraction on the photonic crystal and the environment interface, and the incident electromagnetic wave beam The electromagnetic wave beam and the refracted electromagnetic wave beam are respectively located on both sides of the normal line, so as to separate the electromagnetic wave beams of the two polarization states and realize polarization beam splitting.
入射电磁波波束与法线的夹角为10°~80°。The included angle between the incident electromagnetic wave beam and the normal is 10°-80°.
本实用新型具有的有益的效果是:本器件利用光子晶体实现了偏振分光,两个偏振态的电磁波束都工作在透射模式,具有小尺寸、易于集成、工艺简单等优点,可以用于微波段和光波段。The beneficial effects of the utility model are: the device uses photonic crystals to realize polarization splitting, and the electromagnetic beams of the two polarization states work in the transmission mode. It has the advantages of small size, easy integration, simple process, etc., and can be used in microwave and light bands.
附图说明Description of drawings
图1是介质材料中柱子阵列构成的平板形光子晶体偏振分束器的结构原理示意图;Fig. 1 is a schematic diagram of the structure and principle of a planar photonic crystal polarization beam splitter composed of a pillar array in a dielectric material;
图2是图1的A-A剖视图;Fig. 2 is A-A sectional view of Fig. 1;
图3是三角形偏振分束器的结构原理示意图;Fig. 3 is a schematic diagram of the structure and principle of a triangular polarizing beam splitter;
图4是空气中柱子阵列构成的平板形光子晶体偏振分束器的结构原理示意图;Fig. 4 is a schematic diagram of the structure and principle of a planar photonic crystal polarization beam splitter composed of a column array in the air;
图5是图4的B-B剖视图;Fig. 5 is the B-B sectional view of Fig. 4;
图6是光子晶体能带结构特征示意图;Fig. 6 is a schematic diagram of photonic crystal energy band structure characteristics;
图7是氧化铝中三角晶格排列的银圆柱阵列构成的光子晶体的能带结构,黑圆圈代表TE偏振,黑方块代表TM偏振;Figure 7 is the energy band structure of a photonic crystal composed of silver cylinder arrays arranged in a triangular lattice in alumina. The black circles represent TE polarization, and the black squares represent TM polarization;
图8是空气中三角晶格排列的砷化镓圆柱阵列构成的光子晶体的能带结构,(a)TE偏振,(b)TM偏振。Fig. 8 is the energy band structure of a photonic crystal composed of a gallium arsenide cylindrical array arranged in a triangular lattice in air, (a) TE polarization, (b) TM polarization.
图中:1、平板形状,2、三角形状,3、入射电磁波波束,4、折射电磁波波束,5、折射电磁波波束,6、环境界面,7、法线,8、介质材料,9、衬底,10、介质材料柱子阵列。In the figure: 1. Flat plate shape, 2. Triangular shape, 3. Incident electromagnetic wave beam, 4. Refracted electromagnetic wave beam, 5. Refracted electromagnetic wave beam, 6. Environmental interface, 7. Normal line, 8. Dielectric material, 9. Substrate , 10. Dielectric material pillar array.
具体实施方式Detailed ways
如图1、图2所示,在衬底9上的介质材料8中二维周期性排列的空气柱子阵列,或金属柱子阵列,或另一种介质材料柱子阵列构成光子晶体。As shown in FIG. 1 and FIG. 2 , a two-dimensional periodic array of air pillars, or a metal pillar array, or another dielectric material pillar array in the dielectric material 8 on the substrate 9 constitutes a photonic crystal.
如图4、图5所示,在衬底9上以二维周期性排列的金属柱子阵列或介质材料柱子阵列10构成光子晶体。As shown in FIG. 4 and FIG. 5 , a two-dimensional periodic arrangement of metal pillar arrays or dielectric
所述的二维周期性是指,阵列中任何相邻的三个柱子的中心的连线构成等腰直角三角形的正方晶格,或构成等边三角形的三角晶格。The two-dimensional periodicity means that the line connecting the centers of any three adjacent pillars in the array forms a square lattice of isosceles right triangles, or a triangular lattice of equilateral triangles.
所述的阵列的形状为长方形1(如图1、图4所示)或三角形2(如图3所示)。The shape of the array is rectangle 1 (as shown in FIG. 1 and FIG. 4 ) or triangle 2 (as shown in FIG. 3 ).
所述的介质材料板的材料为氧化铝、二氧化硅、硅、砷化镓或磷化铟。The material of the dielectric material plate is aluminum oxide, silicon dioxide, silicon, gallium arsenide or indium phosphide.
基于光子晶体正负折射效应的偏振分束方法:以长方形1或三角形2的光子晶体,作为电磁波的偏振分束元件,入射电磁波波束3含有两个偏振态,从环境界面6入射后,其中一个偏振态的电磁波束在环境界面上经历负折射,入射电磁波波束3和折射电磁波波束4在光子晶体与环境界面6的法线7的同一侧;另一个偏振态的电磁波波束在光子晶体与环境界面6上经历正折射,入射电磁波波束3和折射电磁波波束5分别位于法线7的两侧,从而把两个偏振态的电磁波波束分开,实现偏振分束。Polarization beam splitting method based on the positive and negative refraction effects of photonic crystals: the photonic crystal of rectangle 1 or triangle 2 is used as the polarization beam splitting element of electromagnetic waves, and the incident electromagnetic wave beam 3 contains two polarization states. After incident from the environment interface 6, one of them The electromagnetic beam of the polarization state experiences negative refraction on the environment interface, and the incident electromagnetic wave beam 3 and the refracted
入射电磁波波束3与法线7的夹角为10°~80°。The included angle between the incident electromagnetic wave beam 3 and the normal line 7 is 10°-80°.
本实用新型涉及的光子晶体,其工作频率范围内的能带特征具有图6的特征,即,对于偏振态I来说,随着波矢增大频率减小,光子晶体对这个偏振态表现出负折射效应;对于偏振态II来说,随着波矢增大频率也增大,光子晶体对这个偏振态表现出正折射效应。能带具有图6的特征的光子晶体就是本实用新型的偏振分束元件。把光子晶体切成平板型或三角形,入射电磁波波束在一个界面上斜入射就可以实现偏振分束。The photonic crystal involved in the utility model has the characteristics of the energy band in the working frequency range as shown in Fig. 6, that is, for the polarization state I, as the wave vector increases and the frequency decreases, the photonic crystal exhibits Negative refraction effect; for polarization state II, as the wave vector increases, the frequency also increases, and the photonic crystal exhibits a positive refraction effect for this polarization state. The photonic crystal whose energy band has the characteristic of Fig. 6 is the polarization beam splitting element of the present invention. The photonic crystal is cut into a flat plate or a triangle, and the incident electromagnetic wave beam is obliquely incident on an interface to realize polarization beam splitting.
实施例1:基于介质背景银纳米线阵列的偏振分束器Embodiment 1: Polarizing beam splitter based on dielectric background silver nanowire array
这里的光子晶体是氧化铝背景中三角晶格排列的银圆柱阵列,晶格常数a=300nm。当银圆柱半径r=0.255a时,该光子晶体在频率ω=0.40(2πc/a)时,TE偏振的等效折射率是-1而TM偏振的等效折射率是+1,相应的能带结构如图7。The photonic crystal here is an array of silver cylinders arranged in a triangular lattice in an alumina background, and the lattice constant a=300nm. When the silver cylinder radius r=0.255a, when the photonic crystal is at the frequency ω=0.40(2πc/a), the equivalent refractive index of TE polarization is -1 and the equivalent refractive index of TM polarization is +1, the corresponding energy The belt structure is shown in Figure 7.
实施例2:基于介质圆柱阵列的偏振分束器Embodiment 2: Polarizing Beam Splitter Based on Dielectric Cylindrical Array
这里的光子晶体是空气中三角晶格排列的砷化镓圆柱阵列,晶格常数a=1155nm,圆柱半径r=0.15a。图8给出了这种光子晶体的能带结构,工作频率为ω=0.75-0.79(2πc/a)。TE偏振工作在负折射,而TM偏振是正折射。The photonic crystal here is a gallium arsenide cylinder array arranged in a triangular lattice in the air, the lattice constant a=1155nm, and the cylinder radius r=0.15a. Figure 8 shows the energy band structure of this photonic crystal, the working frequency is ω=0.75-0.79(2πc/a). TE polarization operates at negative refraction, while TM polarization is positive refraction.
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