CN111913251B - A Hybrid Plasmonic Waveguide Supporting Simultaneous TE and TM Modes - Google Patents
A Hybrid Plasmonic Waveguide Supporting Simultaneous TE and TM Modes Download PDFInfo
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- 239000000463 material Substances 0.000 claims abstract description 28
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- 239000007769 metal material Substances 0.000 claims description 5
- 230000003287 optical effect Effects 0.000 abstract description 16
- 230000010287 polarization Effects 0.000 abstract description 7
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 abstract description 4
- 229910052681 coesite Inorganic materials 0.000 abstract description 3
- 229910052906 cristobalite Inorganic materials 0.000 abstract description 3
- 229910052751 metal Inorganic materials 0.000 abstract description 3
- 239000002184 metal Substances 0.000 abstract description 3
- 239000000377 silicon dioxide Substances 0.000 abstract description 3
- 229910052682 stishovite Inorganic materials 0.000 abstract description 3
- 229910052905 tridymite Inorganic materials 0.000 abstract description 3
- 230000010354 integration Effects 0.000 abstract description 2
- 239000000758 substrate Substances 0.000 abstract 1
- 230000005540 biological transmission Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 3
- 239000003989 dielectric material Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 229910000510 noble metal Inorganic materials 0.000 description 1
- 239000010970 precious metal Substances 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
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- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/122—Basic optical elements, e.g. light-guiding paths
- G02B6/1226—Basic optical elements, e.g. light-guiding paths involving surface plasmon interaction
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- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/126—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind using polarisation effects
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Abstract
Description
技术领域technical field
本发明属于亚波长光子学技术领域,具体涉及一种同时支持TE、TM模式的混合等离激元波导。The invention belongs to the technical field of subwavelength photonics, and in particular relates to a hybrid plasmon waveguide supporting both TE and TM modes.
背景技术:Background technique:
偏振态是光的重要特性之一,其矢量特性使得其与物质之间发生错综复杂的相互作用,依此人们得以制作各种各样的光学器件和光学系统。过去的研究主要针对的是空间均匀偏振态,如线偏振、圆偏振等等,对于这种情况,偏振态并不依赖于光束的空间位置。Polarization state is one of the important properties of light, and its vector properties make intricate interactions between it and matter, so people can make various optical devices and optical systems. Past studies have mainly focused on spatially uniform polarization states, such as linear polarization, circular polarization, etc., for which the polarization state does not depend on the spatial position of the beam.
混合等离激元波导(HPW)一般是由金属层和高折射率介质材料层中间夹着一层低折射率介质材料构成,HPW的性能与中间的低折射率介质层的厚度紧密相关:当介质层厚度较大时,两种模式是分开的,而且通常无法激发等离激元模式;而当介质层厚度减小到一定程度时,两种模式混合叠加成一种新的模式,此时光场主要局限在中间的低折射率介质材料层。Hybrid plasmon waveguide (HPW) is generally composed of a metal layer and a high-refractive-index dielectric material layer sandwiched by a low-refractive-index dielectric material. The performance of HPW is closely related to the thickness of the intermediate low-refractive-index dielectric layer: when When the thickness of the dielectric layer is large, the two modes are separated, and usually the plasmon mode cannot be excited; when the thickness of the dielectric layer is reduced to a certain extent, the two modes are mixed and superimposed into a new mode, and the light field Mainly confined to the middle layer of low refractive index dielectric material.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供一种同时支持TE、TM模式的混合等离激元波导,以改善已有结构性能。The purpose of the present invention is to provide a hybrid plasmon waveguide that supports both TE and TM modes to improve the performance of existing structures.
一种同时支持TE、TM模式的混合等离激元波导,包括垂直方向和水平方向混合而成的等离激元波导,所述垂直方向的等离激元波导由三层材料构成,包括第一层的高折射率材料,第二层的低折率材料和第三层的金属材料,所述水平方向的等离激元波导由三层材料构成,包括第一层的高折率材料,第二层的低折射率材料和第三层的金属材料,所述垂直方向与水平方向的第二层结构均位于第一层和第三层结构之间。A hybrid plasmon waveguide supporting TE and TM modes at the same time, including a plasmon waveguide mixed in a vertical direction and a horizontal direction, the vertical plasmon waveguide is composed of three layers of materials, including the first A layer of high refractive index material, a second layer of low refractive index material and a third layer of metal material, the horizontal plasmon waveguide is composed of three layers of materials, including the first layer of high refractive index material, The low refractive index material of the second layer and the metal material of the third layer, the second layer structures in the vertical direction and the horizontal direction are both located between the first layer and the third layer structure.
进一步的,所述高折射率材料Si的折射率是3.478,低折射率材料SiO2的折射率是1.44,低折射率材料空气的折射率是1。Further, the refractive index of the high refractive index material Si is 3.478, the refractive index of the low refractive index material SiO 2 is 1.44, and the refractive index of the low refractive index material air is 1.
进一步的,Si高度选取100~400nm之间,宽度选取100~300nm之间,低折射率层选取在30~80nm之间。Further, the height of Si is selected from 100 to 400 nm, the width of Si is selected from 100 to 300 nm, and the low refractive index layer is selected from 30 to 80 nm.
光场被很好的限制在低折射率介质层(空气、SiO2)中,同时在结构依然紧凑的情况下,具有低损耗长传播距离的特性。The optical field is well confined in the low-refractive-index dielectric layer (air, SiO 2 ), and at the same time, it has the characteristics of low loss and long propagation distance under the condition that the structure is still compact.
模式有效折射率的实部代表混合等离激元波导结构中的折射率,而虚部大小决定了混合模式在波导中传播时传输损耗的大小。The real part of the mode's effective refractive index represents the refractive index in the hybrid plasmonic waveguide structure, while the imaginary part determines the transmission loss of the hybrid mode propagating in the waveguide.
本发明的优点在于:该种同时支持TE、TM模式的混合等离激元波导:The advantages of the present invention are: the hybrid plasmon waveguide supporting TE and TM modes simultaneously:
(1)结构简单易设计,材料获取容易,制备易实现;(1) The structure is simple and easy to design, the material is easy to obtain, and the preparation is easy to realize;
(2)可以实现在不激发传统模式波导的前提下,在水平、垂直方向上分别支持TE、TM的混合等离激元模式,突破了现有结构的局限性;(2) The hybrid plasmon modes of TE and TM can be supported in the horizontal and vertical directions respectively without exciting the traditional mode waveguide, which breaks through the limitations of the existing structure;
(3)通过材料的适当选择和结构尺寸的合理设计,能保持较低的传输损耗;(3) Through proper selection of materials and reasonable design of structural dimensions, the transmission loss can be kept low;
(4)结构紧凑,因此便于光子集成,可应用于超高密度集成光路,易应用于高集成度的光波导芯片中。(4) The structure is compact, so it is convenient for photonic integration, can be applied to ultra-high-density integrated optical circuits, and is easy to be applied to high-integration optical waveguide chips.
附图说明Description of drawings
图1为实施例同时支持TE、TM模式的混合等离激元波导结构截面示意图。FIG. 1 is a schematic cross-sectional view of a hybrid plasmon waveguide structure supporting both TE and TM modes according to an embodiment.
图2为实施例波长为λ=1550nm的TE偏振光波导模式分布图。FIG. 2 is a mode distribution diagram of a TE polarized light waveguide with a wavelength of λ=1550 nm in an embodiment.
图3为实施例波长为λ=1550nm的TM偏振光波导模式分布图。FIG. 3 is a mode distribution diagram of a TM polarized light waveguide with a wavelength of λ=1550 nm in an embodiment.
图4为实施例波长为λ=1550nm的光波导模式有效折射率实部随Si的宽度的变化关系图。FIG. 4 is a graph showing the variation of the real part of the effective refractive index with the width of Si in an optical waveguide mode with a wavelength of λ=1550 nm.
图5为实施例波长为λ=1550nm的光波导模式有效折射率实部随Si的高度的变化关系图。FIG. 5 is a graph showing the variation relationship between the real part of the effective refractive index of the optical waveguide mode with the wavelength of λ=1550 nm and the height of Si according to the embodiment.
图6为实施例波长为λ=1550nm的光波导模式有效折射率实部随低折射率介质层厚度(SiO2的高度和空气层宽度)g的变化关系图。FIG. 6 is a graph showing the relationship between the real part of the effective refractive index and the thickness of the low refractive index dielectric layer (the height of SiO 2 and the width of the air layer) g in the optical waveguide mode with wavelength λ=1550 nm of the embodiment.
具体实施方式Detailed ways
为使本发明实现的技术手段、创作特征、达成目的与功效易于明白了解,下面结合具体实施方式,进一步阐述本发明。In order to make the technical means, creative features, achievement goals and effects realized by the present invention easy to understand, the present invention will be further described below with reference to the specific embodiments.
如图1所示,该同时支持TE、TM模式光波导模式的混合等离激元波导是由三种材料A、B与C构成的结构,分为左右两部分,分别是高折射率介质Si、低折射率介质SiO2与贵金属Ag。对应的SiO2的高度和左右两部分之间空气层的宽度为g。As shown in Figure 1, the hybrid plasmon waveguide supporting both TE and TM mode optical waveguide modes is a structure composed of three materials A, B and C, which are divided into two parts: the left and the right parts, which are the high refractive index medium Si. , low refractive index medium SiO 2 and precious metal Ag. The height of the corresponding SiO2 and the width of the air layer between the left and right parts are g.
本实施例中的高折射率介质、低折射率介质和贵金属为Si、SiO2和空气、Ag,其中Si的折射率为3.478,SiO2的折射率为1.44,空气折射率为1。对于1550nm波长光入射下,所对应金属银的折射率为0.145+11.438i。The high-refractive index medium, low-refractive index medium and noble metal in this embodiment are Si, SiO 2 , air, and Ag, wherein the refractive index of Si is 3.478, the refractive index of SiO 2 is 1.44, and the refractive index of air is 1. For the incident light of 1550nm wavelength, the corresponding refractive index of metallic silver is 0.145+11.438i.
图2和图3分别为为实施例波长为λ=1550nm的TE和TM偏振光波导模式分布图。其中低折射率介质层厚度(SiO2的高度和空气层宽度)g=50nm。由图可见,在1550nm波长光入射下,所述的混合等离激元波导在低折射率介质区域有明显的场增强效应,并且具有超强的模场限制能力。FIG. 2 and FIG. 3 are respectively the distribution diagrams of the TE and TM polarized light waveguide modes with the wavelength of λ=1550 nm in the embodiment. The thickness of the low-refractive-index dielectric layer (the height of SiO 2 and the width of the air layer) is g=50 nm. It can be seen from the figure that under the incident light of 1550 nm wavelength, the hybrid plasmon waveguide has obvious field enhancement effect in the low refractive index medium region, and has super strong mode field confinement ability.
图4为实施例波长为λ=1550nm的光波导模式有效折射率实部随Si的宽度w_si的变化关系。由图可见,光波导模式有效折射率实部随Si的宽度w_si的增大而增大,表明波导对传输模式限制能力随Si的宽度增加而增强。FIG. 4 shows the variation relationship between the real part of the effective refractive index of the optical waveguide mode with the wavelength of λ=1550 nm and the width w_si of Si according to the embodiment. It can be seen from the figure that the real part of the effective refractive index of the optical waveguide mode increases with the increase of the width w_si of Si, indicating that the confinement ability of the waveguide to the transmission mode increases with the increase of the width of Si.
图5为实施例波长为λ=1550nm的光波导模式有效折射率实部随Si的高度h_si的变化关系。由图可见,光波导模式有效折射率实部随Si的高度h_si的增大而增大,表明波导对传输模式限制能力随Si的高度增加而增强。FIG. 5 shows the variation relationship of the real part of the effective refractive index of the optical waveguide mode with the wavelength of λ=1550 nm with the height h_si of Si. It can be seen from the figure that the real part of the effective refractive index of the optical waveguide mode increases with the increase of the height h_si of Si, indicating that the confinement ability of the waveguide to the transmission mode increases with the increase of the height of Si.
图6为实施例波长为λ=1550nm的光波导模式有效折射率实部随低折射率介质层厚度(SiO2的高度和空气层宽度)g的变化关系。由图可见,光波导模式有效折射率实部随低折射率介质层厚度(SiO2的高度和空气层宽度)g增大而减小,表明波导对传输模式限制能力随低折射率介质层厚度增大而增强,且TM模式有效折射率实部较TE模式更大。FIG. 6 shows the variation relationship of the real part of the effective refractive index with the thickness of the low refractive index medium layer (the height of SiO 2 and the width of the air layer) g for the optical waveguide mode with wavelength λ=1550 nm of the embodiment. It can be seen from the figure that the real part of the effective refractive index of the optical waveguide mode decreases with the increase of the thickness of the low-refractive - index dielectric layer (the height of SiO and the width of the air layer) g, indicating that the waveguide's ability to confine the transmission mode increases with the thickness of the low-refractive-index dielectric layer. increases and increases, and the real part of the effective refractive index of the TM mode is larger than that of the TE mode.
由技术常识可知,本发明可以通过其它的不脱离其精神实质或必要特征的实施方案来实现。因此,上述公开的实施方案,就各方面而言,都只是举例说明,并不是仅有的。所有在本发明范围内或在等同于本发明的范围内的改变均被本发明包含。It is known from the technical common sense that the present invention can be realized by other embodiments without departing from its spirit or essential characteristics. Accordingly, the above-disclosed embodiments are, in all respects, illustrative and not exclusive. All changes within the scope of the present invention or within the scope equivalent to the present invention are encompassed by the present invention.
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