CN110873909A - An ultra-broadband polarization-insensitive absorber in all ultraviolet-mid-infrared bands - Google Patents
An ultra-broadband polarization-insensitive absorber in all ultraviolet-mid-infrared bands Download PDFInfo
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- G—PHYSICS
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- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/003—Light absorbing elements
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B1/00—Optical elements characterised by the material of which they are made; Optical coatings for optical elements
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Abstract
本发明提供了一种全紫外‑中红外波段的超宽带偏振不敏感吸收器,包括基底和设置在所述基底上呈周期性排列的超材料单元结构,所述超材料单元结构包括依次设置的多层介质/金属膜和单层介质膜/金属,还包括设置在所述多层介质/金属膜外层的外层介电圆柱环,所述外层介电圆柱环的高度小于所述多层介质/金属膜的高度。本发明的吸收器频带为200~2000nm,覆盖全紫外、可见光、近红外和中间红外波段,吸收率平均值高达94.3%,吸收率最高可达99.89%,且对偏振光不敏感,成本较低,可用于太阳能收集和紫外防护。
The invention provides an ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band, comprising a substrate and a metamaterial unit structure arranged on the substrate in a periodic arrangement, and the metamaterial unit structure includes sequentially arranged metamaterial unit structures. The multi-layer dielectric/metal film and the single-layer dielectric film/metal also include an outer dielectric cylindrical ring arranged on the outer layer of the multi-layer dielectric/metal film, and the height of the outer dielectric cylindrical ring is smaller than that of the multi-layer dielectric cylindrical ring. Height of layer dielectric/metal film. The absorber of the invention has a frequency band of 200-2000 nm, covers all ultraviolet, visible light, near-infrared and mid-infrared wavebands, the average absorption rate is as high as 94.3%, the absorption rate is as high as 99.89%, and it is insensitive to polarized light and low in cost. , can be used for solar energy harvesting and UV protection.
Description
技术领域technical field
本发明涉及超材料及电磁功能技术领域,尤其涉及一种全紫外-中红外波段的超宽带偏振不敏感吸收器。The invention relates to the technical field of metamaterials and electromagnetic functions, in particular to an ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band.
背景技术Background technique
全球能源危机和大气污染问题日益突出,太阳能作为一种理想的清洁能源受到许多国家的关注。太阳光辐射到地面的能量光谱主要由紫外(9%)、可见光(46%)和红外(45%)三个波段组成。传统的太阳能光伏电池仅能吸收可见光波段的能量并且吸收率不高,使太阳光谱中的能量不被有效吸收。同时,光伏太阳能电池易受四季、昼夜阴晴等气象条件影响,尤其在阴暗天气和夜晚,传统光伏电池几乎失去了作用。因此需要一种高吸收率、宽波段的太阳能收集技术,能以较高的效率吸收紫外到红外波段的光。The global energy crisis and air pollution problems have become increasingly prominent. As an ideal clean energy, solar energy has attracted the attention of many countries. The energy spectrum of sunlight radiated to the ground is mainly composed of three bands: ultraviolet (9%), visible light (46%) and infrared (45%). Traditional solar photovoltaic cells can only absorb energy in the visible light band and the absorption rate is not high, so that the energy in the solar spectrum is not effectively absorbed. At the same time, photovoltaic solar cells are easily affected by weather conditions such as four seasons, cloudy day and night, especially in dark weather and night, traditional photovoltaic cells almost lose their function. Therefore, there is a need for a high-absorption, broadband solar energy collection technology that can absorb light in the ultraviolet to infrared wavelengths with high efficiency.
目前,为了实现宽频带的吸收,相关技术人员已经做了一些研究,大多数光学完美吸收器都需要比较复杂的结构。随着微纳尺度加工技术的迅速发展,技术人员已经提出并制造了多种超材料结构来实现宽谱段的吸收,并且本领域相关研究人员已经对其性质做了大量的研究。然而,现有的超材料结构主要存在三个问题:1、简单超材料结构的吸收率较低,且对于斜入射光比较敏感,实现不了宽波段光谱的吸收;2、为了保证高吸收率,超材料结构需要精巧的结构设计,这加大了工艺实现难度,制备成本高,使吸收器的推广受到限制;3、超材料结构大都使用贵金属金/银等高电导率的金属材料,这严重限制了将其他材料应用于吸收器中,使得生产成本增高,不宜于推广加工生产。At present, in order to achieve broadband absorption, relevant technical personnel have done some research, and most optical perfect absorbers need relatively complex structures. With the rapid development of micro- and nano-scale processing technology, technicians have proposed and fabricated a variety of metamaterial structures to achieve wide-spectrum absorption, and relevant researchers in the field have done a lot of research on their properties. However, the existing metamaterial structures mainly have three problems: 1. The absorption rate of simple metamaterial structures is low, and they are sensitive to oblique incident light, so they cannot achieve broadband spectral absorption; 2. In order to ensure high absorption rate, Metamaterial structures require sophisticated structural design, which increases the difficulty of process realization, high fabrication costs, and limits the promotion of absorbers; 3. Most metamaterial structures use high-conductivity metal materials such as precious metals gold/silver, which is a serious problem. The application of other materials in the absorber is restricted, which increases the production cost and is not suitable for promotion of processing and production.
发明内容SUMMARY OF THE INVENTION
本发明旨在解决上述问题,提供一种具有吸收率高、所覆盖的吸收频带更宽、还具有较好的入射角度不敏感性的全紫外-中红外波段的超宽带偏振不敏感吸收器。The present invention aims to solve the above problems, and provides an ultra-broadband polarization insensitive absorber with high absorption rate, wider absorption frequency band covered, and better incident angle insensitivity in the full ultraviolet-mid-infrared wavelength band.
为实现上述目的,本发明提供了如下方案:For achieving the above object, the present invention provides the following scheme:
一种全紫外-中红外波段的超宽带偏振不敏感吸收器,包括基底和设置在所述基底上呈周期性排列的超材料单元结构,所述超材料单元结构包括依次设置的多层介质/金属膜和单层介质膜/金属,还包括设置在所述多层介质/金属膜外层的外层介电圆柱环,所述外层介电圆柱环的高度小于所述多层介质/金属膜的高度。An ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band, comprising a substrate and a metamaterial unit structure arranged on the substrate in a periodic arrangement, the metamaterial unit structure comprising sequentially arranged multilayer media/ A metal film and a single-layer dielectric film/metal, further comprising an outer dielectric cylindrical ring disposed on the outer layer of the multilayer dielectric/metal film, and the height of the outer dielectric cylindrical ring is smaller than that of the multilayer dielectric/metal height of the membrane.
优选地,所述基底的材料为铁、铝或铜。Preferably, the material of the substrate is iron, aluminum or copper.
优选地,所述基底的厚度为180~220mm。Preferably, the thickness of the substrate is 180-220 mm.
优选地,所述多层介质/金属膜和单层介质膜/金属为十字型结构。Preferably, the multi-layer dielectric/metal film and the single-layer dielectric film/metal have a cross-shaped structure.
优选地,所述多层介质/金属膜为交替设置的介质条和金属膜,所述介质条的厚度大于所述金属膜的厚度;Preferably, the multilayer dielectric/metal films are alternately arranged dielectric strips and metal films, and the thickness of the dielectric strips is greater than the thickness of the metal films;
优选地,所述单层介质膜/金属为依次设置的介质膜和金属条,所述金属条的厚度大于所述介质膜的厚度。Preferably, the single-layer dielectric film/metal is a dielectric film and a metal strip arranged in sequence, and the thickness of the metal strip is greater than the thickness of the dielectric film.
优选地,所述多层介质/金属膜的臂长为80~120nm,臂宽为55~100nm;所述介质条的厚度为140~150nm,所述金属膜的厚度为10~15nm;Preferably, the arm length of the multilayer dielectric/metal film is 80-120 nm, and the arm width is 55-100 nm; the thickness of the dielectric strip is 140-150 nm, and the thickness of the metal film is 10-15 nm;
优选地,所述介质膜的臂长为80~120nm,臂宽为55~100nm,厚度为10~15nm;所述金属条的臂长为26~36nm,臂宽为22~32nm,厚度为40~60nm。Preferably, the arm length of the dielectric film is 80-120 nm, the arm width is 55-100 nm, and the thickness is 10-15 nm; the arm length of the metal strip is 26-36 nm, the arm width is 22-32 nm, and the thickness is 40 nm ~60nm.
优选地,所述介质条的材料为硅、二氧化硅、氮化硅、氧化铝或氟化镁,与所述介质条相邻的两层所述金属膜的材料不同,分别为金或银,以及铁、铝或铜;Preferably, the material of the dielectric strip is silicon, silicon dioxide, silicon nitride, aluminum oxide or magnesium fluoride, and the material of the two metal films adjacent to the dielectric strip is different from that of gold or silver, respectively. , and iron, aluminium or copper;
优选地,所述介质膜的材料为硅、二氧化硅、氮化硅、氧化铝或氟化镁,所述金属条的材料为铁、铝或铜。Preferably, the material of the dielectric film is silicon, silicon dioxide, silicon nitride, aluminum oxide or magnesium fluoride, and the material of the metal strip is iron, aluminum or copper.
优选地,所述外层介电圆柱环的材料为硅、二氧化硅、氮化硅、氧化铝或氟化镁,内半径为110~170nm,外半径为130~190nm,高度为540~705nm。Preferably, the material of the outer dielectric cylindrical ring is silicon, silicon dioxide, silicon nitride, aluminum oxide or magnesium fluoride, the inner radius is 110-170 nm, the outer radius is 130-190 nm, and the height is 540-705 nm .
优选地,所述超材料单元结构的阵列周期为260~380nm。Preferably, the array period of the metamaterial unit structure is 260-380 nm.
本发明提供的一种全紫外-中红外波段的超宽带偏振不敏感吸收器,在太阳能捕获和紫外防护中的应用。The invention provides an ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band, which is used in solar energy capture and ultraviolet protection.
本发明可取得如下有益效果:The present invention can achieve the following beneficial effects:
1、本发明的吸收器整体关于xoz平面和yoz平面对称,使得吸收器对入射光偏振不敏感;采用多层介质/金属膜结构,利用多层介质/金属结构产生的慢波效应,拓宽了吸收器的吸收频带宽度;顶层采用单层介质膜/金属结构,激发了紫外到可见光区的局域表面等离激元(LSP)模式,从而增强了吸收率。1. The absorber of the present invention is symmetrical about the xoz plane and the yoz plane as a whole, so that the absorber is not sensitive to the polarization of incident light; the multi-layer dielectric/metal film structure is adopted, and the slow wave effect generated by the multi-layer dielectric/metal structure is used to widen the The absorption bandwidth of the absorber; the top layer adopts a single-layer dielectric film/metal structure, which excites localized surface plasmon (LSP) modes in the ultraviolet to visible region, thereby enhancing the absorption rate.
2、本发明提供的外层介电圆柱环,其高度低于多层介质/金属膜结构,易与多层介质/金属膜结构产生耦合作用,同时激发表面等离激元共振(SPR),增大了吸收器的吸收频带宽度。2. The outer dielectric cylindrical ring provided by the present invention has a height lower than that of the multi-layer dielectric/metal film structure, and is easily coupled with the multi-layer dielectric/metal film structure, and at the same time excites surface plasmon resonance (SPR), The absorption bandwidth of the absorber is increased.
3、本发明采用十字型结构的多层介质/金属膜结构,易于激发电偶极子谐振和磁偶极子谐振,使得电场强度和磁场强度增大,更多的电磁波可以被所述结构捕获,从而增加了吸收率。3. The present invention adopts the multi-layer dielectric/metal film structure of the cross-shaped structure, which is easy to excite the electric dipole resonance and the magnetic dipole resonance, so that the electric field strength and magnetic field strength increase, and more electromagnetic waves can be captured by the structure. , thereby increasing the absorption rate.
4、本发明的吸收器频带为200~2000nm,覆盖全紫外、可见光、近红外和中间红外波段,吸收率平均值高达94.3%,吸收率最高可达99.89%。4. The frequency band of the absorber of the present invention is 200-2000 nm, covering all ultraviolet, visible, near-infrared and mid-infrared bands, the average absorption rate is as high as 94.3%, and the maximum absorption rate is as high as 99.89%.
5、本发明提供的吸收器吸收性能优良,结构简单,制造成本较低,实用性较强,灵活性较高,且有利于推广应用。5. The absorber provided by the present invention has excellent absorption performance, simple structure, low manufacturing cost, strong practicability, high flexibility, and is favorable for popularization and application.
附图说明Description of drawings
图1为本发明优选实施例的全紫外-中红外波段的超宽带偏振不敏感吸收器的结构示意图;1 is a schematic structural diagram of an ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band of a preferred embodiment of the present invention;
图2为本发明优选实施例的超材料单元结构的示意图;Fig. 2 is the schematic diagram of the metamaterial unit structure of the preferred embodiment of the present invention;
图3为本发明优选实施例的超材料单元结构的俯视图和侧视图;3 is a top view and a side view of a metamaterial unit structure according to a preferred embodiment of the present invention;
图4为本发明优选实施例的硅圆柱环俯视图;4 is a top view of a silicon cylindrical ring according to a preferred embodiment of the present invention;
图5为本发明优选实施例的多层介质/金属膜和单层介质膜/金属的结构示意图;5 is a schematic structural diagram of a multi-layer dielectric/metal film and a single-layer dielectric film/metal according to a preferred embodiment of the present invention;
图6为本发明优选实施例的全紫外-中红外波段的超宽带偏振不敏感吸收器的超宽带吸收器反射率仿真图;Fig. 6 is the ultra-broadband absorber reflectivity simulation diagram of the ultra-broadband polarization-insensitive absorber of the full ultraviolet-mid-infrared waveband of the preferred embodiment of the present invention;
图7为本发明优选实施例的全紫外-中红外波段的超宽带偏振不敏感吸收器的超宽带吸收器吸收率仿真图。7 is a simulation diagram of an ultra-broadband absorber absorption rate of an ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band according to a preferred embodiment of the present invention.
具体实施方式Detailed ways
下面将结合本发明的实施例中的附图,对本发明的实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only a part of the embodiments of the present invention, rather than all the embodiments. . Based on the embodiments of the present invention, all other embodiments obtained by those of ordinary skill in the art without creative efforts shall fall within the protection scope of the present invention.
实施例1:Example 1:
如图1~图5所示,一种全紫外-中红外波段的超宽带偏振不敏感吸收器,包括基底1和设置在基底1上呈周期性排列的超材料单元结构。其中,超材料单元结构包括依次设置的多层介质/金属膜2和单层介质膜/金属3,还包括设置在多层介质/金属膜2外层的外层介电圆柱环4,该外层介电圆柱环4的高度小于多层介质/金属膜2的高度。其中,基底1材料为金属铁,基底1镀一层足够厚的金属铁薄膜,使透射率变为0,入射波将最大限度地进入到吸收器内部被吸收损耗,因此设计基底1厚度为Hd=200mm。多层介质/金属膜2由交替设置的十字型结构的介质条21和金属膜22组成,共有六层介质条21和金属膜22。其中,介质条21的材料为硅,金属膜22的材料为金和铁交替设置,即多层介质/金属膜2的结构从下到上依次为硅条、金膜、硅条、铁膜、硅条、金膜、硅条、铁膜、硅条、金膜、硅条、铁膜。介质条21和金属膜22的臂长相等和臂宽也相等,臂长L1=94.5nm,臂宽W1=82nm,介质条21的厚度H1=145nm,金属膜2厚度H2=10nm。本发明采用十字型结构的多层介质/金属膜结构,易于激发电偶极子谐振和磁偶极子谐振,使得电场强度和磁场强度增大,更多的电磁波可以被所述结构捕获,从而增加了吸收率;同时多层介质/金属结构产生的慢波效应,拓宽了吸收器的吸收频带宽度。单层介质膜/金属3由从下到上依次设置的十字型结构的介质膜31和金属条32组成,介质膜31的材料为硅,金属条32的材料为铁。其中介质膜31的臂长和臂宽与介质条21和金属膜22的相等,厚度较薄为H3=10nm;金属条32的臂长和臂宽较小分别为:L2=31.5nm,W2=27nm,厚度H4=50nm。由于介质膜31较薄和金属条32臂长与臂宽较小,更易于激发紫外到可见光区的局域表面等离激元(LSP)模式,增强结构吸收率。外层介电圆柱环4材料为硅,圆柱环内半径r=142nm,外半径R=162nm,高度Hr=610nm,外层介电圆柱环4高度低于多层介质/金属膜2,易与内层的多层十字形结构产生耦合作用,同时激发表面等离激元共振(SPR),增大了吸收器的带宽。超材料单元结构的阵列周期为324nm,单元结构的基底1尺寸长度为L=324nm,宽度为W=324nm。As shown in FIGS. 1 to 5 , an ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band includes a
将本实施例中的吸收器结构经软件FDTD Solutions对吸收器的吸收率进行仿真计算,在垂直入射情况下,其反射频谱如图6所示,吸收频谱如图7所示。吸收率的计算公式为:A=1-R-T,式中R为反射率,T为透射率。通过合理优化设计吸收器的结构参数和材料,使吸收器在设定的特定频率的阻抗与自由空间的阻抗相匹配(即吸收材料的有效介电常数与有效磁导率相等)。此时,由于电磁波完全进入吸收器而几乎不被反射,反射率R接近与零,如图6所示;其次,金属反射层使电磁波不能透过该材料,使得透射率T也为零;这样电磁波被完全限制在该器件内部,从而实现近乎100%的完美吸收。仿真结果表明,该设计表现出良好的特性,如图7所示,吸收器平均吸收率为94.3%,频带宽度达到1800nm(波段为200nm~2000nm),最大吸收率高达99.89%。The absorber structure in this embodiment is simulated and calculated by the software FDTD Solutions to the absorption rate of the absorber. In the case of vertical incidence, its reflection spectrum is shown in Figure 6, and its absorption spectrum is shown in Figure 7. The formula for calculating the absorption rate is: A=1-R-T, where R is the reflectivity and T is the transmittance. By reasonably optimizing the structural parameters and materials of the absorber, the impedance of the absorber at the set specific frequency is matched with the impedance of the free space (that is, the effective permittivity of the absorber is equal to the effective permeability). At this time, since the electromagnetic wave completely enters the absorber and is hardly reflected, the reflectivity R is close to zero, as shown in Figure 6; secondly, the metal reflective layer makes the electromagnetic wave impermeable to the material, so that the transmittance T is also zero; in this way Electromagnetic waves are completely confined inside the device, resulting in nearly 100% perfect absorption. The simulation results show that the design shows good characteristics. As shown in Figure 7, the average absorption rate of the absorber is 94.3%, the frequency band width reaches 1800nm (the wavelength range is 200nm-2000nm), and the maximum absorption rate is as high as 99.89%.
实施例2:Example 2:
本实施例全紫外-中红外波段的超宽带偏振不敏感吸收器,结构与实施例1相似,不同之处在于,基底1的厚度Hd=210mm;多层介质/金属膜2共有八层介质条21和金属膜22,即多层介质/金属膜2的结构从下到上依次为硅条、金膜、硅条、铁膜、硅条、金膜、硅条、铁膜、硅条、金膜、硅条、铁膜、硅条、金膜、硅条、铁膜;介质条21和金属膜22的臂长L1=100nm,臂宽W1=70nm,介质条21的厚度H1=150nm,金属膜2厚度H2=15nm。介质膜31的臂长和臂宽与介质条21和金属膜22的相等,厚度较薄为H3=15nm;金属条32的臂长和臂宽较小分别为:L2=35nm,W2=30nm,厚度H4=55nm。外层介电圆柱环4的内半径r=165nm,外半径R=185nm,高度Hr=700nm。超材料单元结构的阵列周期为370nm,单元结构的基底1尺寸长度为L=370nm,宽度为W=370nm。The structure of the ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band of this embodiment is similar to that of the first embodiment, the difference is that the thickness of the
将本实施例中的吸收器结构经软件FDTD Solutions对吸收器的吸收率进行仿真计算,在垂直入射情况下,吸收器平均吸收率为92.3%,频带宽度达到1800nm(波段为200nm~2000nm),最大吸收率高达99.32%。The absorber structure in this embodiment is simulated and calculated by the software FDTD Solutions to the absorber absorption rate. In the case of vertical incidence, the average absorption rate of the absorber is 92.3%, and the frequency band width reaches 1800nm (the wavelength range is 200nm~2000nm), The maximum absorption rate is as high as 99.32%.
实施例3:Example 3:
本实施例全紫外-中红外波段的超宽带偏振不敏感吸收器,结构与实施例1相似,不同之处在于,基底1的材料为铝,厚度Hd=180mm;多层介质/金属膜2共有四层,其中,介质条21的材料为二氧化硅,金属膜22的材料为银和铝交替设置,即多层介质/金属膜2的结构从下到上依次为二氧化硅条、银膜、二氧化硅条、铝膜、二氧化硅条、银膜、二氧化硅条、铝膜;介质条21和金属膜22的臂长L1=85nm,臂宽W1=60nm,介质条21的厚度H1=140nm,金属膜2厚度H2=12nm。单层介质膜/金属3中,介质膜31的材料为二氧化硅,金属条32的材料为铝;介质膜31的臂长和臂宽与介质条21和金属膜22的相等,厚度较薄为H3=12nm;金属条32的臂长和臂宽较小分别为:L2=30nm,W2=23nm,厚度H4=40nm。外层介电圆柱环4的内半径r=110nm,外半径R=135nm,高度Hr=540nm。超材料单元结构的阵列周期为260nm,单元结构的基底1尺寸长度为L=260nm,宽度为W=260nm。The structure of the ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band of this embodiment is similar to that of
将本实施例中的吸收器结构经软件FDTD Solutions对吸收器的吸收率进行仿真计算,在垂直入射情况下,吸收器平均吸收率为90.5%,频带宽度达到1800nm(波段为200nm~2000nm),最大吸收率高达99.22%。The absorber structure in this embodiment is simulated and calculated by the software FDTD Solutions to the absorber absorption rate. In the case of vertical incidence, the average absorption rate of the absorber is 90.5%, and the frequency band width reaches 1800nm (the wavelength range is 200nm~2000nm), The maximum absorption rate is as high as 99.22%.
实施例4:Example 4:
本实施例全紫外-中红外波段的超宽带偏振不敏感吸收器,结构与实施例1相似,不同之处在于,基底1的材料为铜,厚度Hd=190mm;多层介质/金属膜2中,介质条21的材料为氟化镁,金属膜22的材料为金和铜交替设置,即多层介质/金属膜2的结构从下到上依次为氟化镁条、金膜、氟化镁条、铜膜、氟化镁条、金膜、氟化镁条、铜膜、氟化镁条、金膜、氟化镁条、铜膜;介质条21和金属膜22的臂长L1=105nm,臂宽W1=88nm,介质条21的厚度H1=142nm,金属膜2厚度H2=13nm。单层介质膜/金属3中,介质膜31的材料为氟化镁,金属条32的材料为铜;介质膜31的臂长和臂宽与介质条21和金属膜22的相等,厚度较薄为H3=13nm;金属条32的臂长和臂宽较小分别为:L2=28.5nm,W2=25nm,厚度H4=45nm。外层介电圆柱环4的内半径r=128nm,外半径R=150nm,高度Hr=650nm。超材料单元结构的阵列周期为300nm,单元结构的基底1尺寸长度为L=300nm,宽度为W=300nm。The ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared waveband of this embodiment is similar in structure to that of
将本实施例中的吸收器结构经软件FDTD Solutions对吸收器的吸收率进行仿真计算,在垂直入射情况下,吸收器平均吸收率为92.4%,频带宽度达到1800nm(波段为200nm~2000nm),最大吸收率高达99.38%。The absorber structure in this embodiment is simulated and calculated by the software FDTD Solutions to the absorber absorption rate. In the case of vertical incidence, the average absorption rate of the absorber is 92.4%, and the frequency bandwidth reaches 1800nm (the wavelength range is 200nm~2000nm), The maximum absorption rate is as high as 99.38%.
实施例5:Example 5:
本实施例全紫外-中红外波段的超宽带偏振不敏感吸收器,结构与实施例1相似,不同之处在于,基底1的厚度Hd=220mm;多层介质/金属膜2共有四层,其中,介质条21的材料为氮化硅,金属膜22的材料为金和铁交替设置,即多层介质/金属膜2的结构从下到上依次为硅条、金膜、硅条、铁膜、硅条、金膜、硅条、铁膜;介质条21和金属膜22的臂长L1=115.5nm,臂宽W1=95nm,介质条21的厚度H1=148nm,金属膜2厚度H2=14nm。单层介质膜/金属3中,介质膜31的材料为氮化硅,介质膜31的臂长和臂宽与介质条21和金属膜22的相等,厚度较薄为H3=14nm;金属条32的臂长和臂宽较小分别为:L2=26nm,W2=22nm,厚度H4=60nm。外层介电圆柱环4的内半径r=150nm,外半径R=174nm,高度Hr=560nm。超材料单元结构的阵列周期为348nm,单元结构的基底1尺寸长度为L=348nm,宽度为W=348nm。The structure of the ultra-broadband polarization-insensitive absorber in the full ultraviolet-mid-infrared band of this embodiment is similar to that of
将本实施例中的吸收器结构经软件FDTD Solutions对吸收器的吸收率进行仿真计算,在垂直入射情况下,吸收器平均吸收率为91.8%,频带宽度达到1800nm(波段为200nm~2000nm),最大吸收率高达99.45%。The absorber structure in this embodiment is simulated and calculated by the software FDTD Solutions to the absorber absorption rate. In the case of vertical incidence, the average absorption rate of the absorber is 91.8%, and the frequency bandwidth reaches 1800nm (the wavelength range is 200nm~2000nm), The maximum absorption rate is as high as 99.45%.
最后应说明的是:以上所述仅为本发明的优选实施例而已,并不用于限制本发明,尽管参照前述实施例对本发明进行了详细的说明,对于本领域的技术人员来说,其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分技术特征进行等同替换,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。Finally, it should be noted that the above descriptions are only preferred embodiments of the present invention, and are not intended to limit the present invention. Although the present invention has been described in detail with reference to the foregoing embodiments, for those skilled in the art, the The technical solutions described in the foregoing embodiments can be modified, or some technical features thereof can be equivalently replaced, and any modifications, equivalent replacements, improvements, etc. made within the spirit and principle of the present invention shall be included. within the protection scope of the present invention.
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CN114460673A (en) * | 2022-01-21 | 2022-05-10 | 中南大学 | A high temperature solar spectrum selective absorber based on plasmon resonance and its preparation method |
CN114460673B (en) * | 2022-01-21 | 2023-05-26 | 中南大学 | High-temperature solar spectrum selective absorber based on plasmon resonance and preparation method thereof |
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