CN105022106A - Absorber of ultra wide band of visible and near-infrared band and preparation method thereof - Google Patents
Absorber of ultra wide band of visible and near-infrared band and preparation method thereof Download PDFInfo
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Abstract
本发明公开了一种可见-近红外波段的超宽带吸收器及其制备方法,包括:可见-近红外波段的超宽带吸收器由基底和五层光学薄膜组成,最底层薄膜为金属吸收层,在金属吸收层上面是锗层,在锗层的上面为剩余三层,由下至上材料折射率逐渐减小。本发明基于金属吸收层的阻挡入射作用结合锗层的宽波段减反膜层,构建了宽波段的无透射的减反结构,实现了高效率、角度不敏感的可见-近红外波段超宽带吸收,在性能上完全超越了传统的吸收器。本发明的吸收器是紧凑的多层薄膜结构,相比于传统的宽带吸收器以及近些年提出的人工电磁吸收器,结构更加简单,避免了复杂的纳米加工技术,生产成本显著下降,生产周期显著缩短,便于大规模、批量化生产。
The invention discloses an ultra-broadband absorber in the visible-near-infrared band and a preparation method thereof, comprising: the ultra-broadband absorber in the visible-near-infrared band is composed of a substrate and five layers of optical films, the bottom film is a metal absorbing layer, Above the metal absorption layer is a germanium layer, and above the germanium layer are the remaining three layers, and the refractive index of the material decreases gradually from bottom to top. Based on the incident blocking effect of the metal absorption layer combined with the wide-band anti-reflection film layer of the germanium layer, the invention constructs a wide-band non-transmission anti-reflection structure, and realizes high-efficiency, angle-insensitive ultra-broadband absorption in the visible-near-infrared band , completely surpassing the traditional absorber in performance. The absorber of the present invention is a compact multi-layer thin film structure. Compared with the traditional broadband absorber and the artificial electromagnetic absorber proposed in recent years, the structure is simpler, the complex nano-processing technology is avoided, and the production cost is significantly reduced. The cycle is significantly shortened, which is convenient for large-scale and batch production.
Description
技术领域technical field
本发明属于杂散光消除、空间探测、成像、光热转换及电磁吸收等领域,具体涉及一种可见—近红外波段的超宽带吸收器。The invention belongs to the fields of stray light elimination, space detection, imaging, light-to-heat conversion, electromagnetic absorption, etc., and specifically relates to an ultra-broadband absorber in the visible-near-infrared band.
背景技术Background technique
由于可见—红外宽波段吸收器可以在诸多不同的新领域发挥重大作用,因而近些年可见—红外宽波段吸收器获得了广泛研究,从而使得越来越宽波段的吸收器被制备出。近年来,研究人员提出了各种电磁波人工电磁结构的近红外吸收器。其中,Chen等利用液滴蒸发的方法在镀有介质层的金属基底上形成随机排列的金纳米棒,实现近红外900nm—1600nm波段的高吸收(Near-infrared broadband absorber with film-coupled multilayernanorods,Optics Lett.38,2247-2249(2013));Zhou等利用侧向沉积的特点制备出多层的交替介质/金属的锥形结构,实现近红外宽波段的较高吸收(Experiment and Theory of the Broadband Absorption by a TaperedHyperbolic Metamaterial Array,ACS Photonics 1,618-624(2014));Ji等提出了一种在银反射镜表面交替堆积金属颗粒和氧化硅薄膜的结构,从而实现300nm—1100nm波段平均96%以上的高吸收(Plasmonic broadband absorberby stacking multiple metallic nanoparticle layers,Appl.Phys.Lett.106,161107(2015))。Since the visible-infrared broadband absorber can play an important role in many different new fields, the visible-infrared broadband absorber has been extensively studied in recent years, so that more and more broadband absorbers have been prepared. In recent years, researchers have proposed various near-infrared absorbers for electromagnetic waves with artificial electromagnetic structures. Among them, Chen et al. used the method of droplet evaporation to form randomly arranged gold nanorods on a metal substrate coated with a dielectric layer to achieve high absorption in the near-infrared 900nm-1600nm band (Near-infrared broadband absorber with film-coupled multilayernanorods, Optics Lett.38,2247-2249(2013)); Zhou et al. used the characteristics of lateral deposition to prepare a multi-layer alternating dielectric/metal cone structure to achieve higher absorption in the near-infrared broadband (Experiment and Theory of the Broadband Absorption by a Tapered Hyperbolic Metamaterial Array, ACS Photonics 1,618-624(2014)); Ji et al proposed a structure in which metal particles and silicon oxide films are alternately stacked on the surface of a silver mirror, so as to achieve an average of more than 96% in the 300nm-1100nm band High absorption (Plasmonic broadband absorber by stacking multiple metallic nanoparticle layers, Appl. Phys. Lett. 106, 161107 (2015)).
但是上述方法制备过程较为复杂,耗时较长,制备成本高,不利于大面积量化生产。However, the preparation process of the above method is relatively complicated, takes a long time, and the preparation cost is high, which is not conducive to large-scale quantitative production.
目前相关的文献报道主要有:The current relevant literature reports mainly include:
申请号为201510163240.8的中国专利文献公开了一种基于级联结构超材料的超宽带吸收器,该吸收器由9个介质层,9个金属层组成,第1~3介质层和金属层为直径相同的圆柱,第4~6介质层和金属层为直径相同的圆柱,第7~9介质层和金属层为直径相同的圆柱,该吸收器整体结构较为复杂,且对入射角度要求较高。The Chinese patent document with the application number 201510163240.8 discloses an ultra-broadband absorber based on cascaded metamaterials. The absorber consists of 9 dielectric layers and 9 metal layers. The first to third dielectric layers and metal layers are diameters For the same cylinder, the 4th to 6th dielectric layers and metal layers are cylinders with the same diameter, and the 7th to 9th dielectric layers and metal layers are cylinders with the same diameter.
申请号为201410020841.9的中国专利文献公开了一种基于可见到近红外波段吸收膜系结构,其在任意衬底上采用气相沉积、液相沉积依次生长金属薄膜层、介质薄膜层,其中金属薄膜层厚度为80nm-1μm,介质薄膜层厚度为1nm-200nm,金属颗粒无序分布层中等效薄膜层平均高度为5nm-100nm,颗粒平均尺寸为10nm-200nm,金属颗粒表面覆盖率为3%-90%。结构相对比较简单,但是其吸收率不好。The Chinese patent document with the application number 201410020841.9 discloses a structure based on absorbing films in the visible to near-infrared bands, which uses vapor deposition and liquid deposition to sequentially grow a metal thin film layer and a dielectric thin film layer on any substrate, wherein the metal thin film layer The thickness is 80nm-1μm, the thickness of the dielectric film layer is 1nm-200nm, the average height of the equivalent film layer in the metal particle disorder distribution layer is 5nm-100nm, the average particle size is 10nm-200nm, and the surface coverage of metal particles is 3%-90 %. The structure is relatively simple, but its absorption rate is not good.
申请号为201110410712.7的中国专利文献公开了一种太阳能选择性吸收涂层,该涂层由双层或三层结构组成:第一层为抛光后的不锈钢基底,第二层为Cu1.5Mn1.5O4复合氧化物吸收层,第三层由TiO2薄膜构成减反层,自下而上排列。该涂层的吸收率均低于0.9,且制备工艺复杂。The Chinese patent document with application number 201110410712.7 discloses a solar selective absorption coating, which consists of a double-layer or three-layer structure: the first layer is a polished stainless steel substrate, and the second layer is Cu1.5Mn1.5O4 Composite oxide absorption layer, the third layer is composed of TiO2 thin film anti-reflection layer, arranged from bottom to top. The absorptivity of the coating is lower than 0.9, and the preparation process is complicated.
发明内容Contents of the invention
本发明提供了一种可见-近红外波段的超宽带吸收器,该吸收器所能覆盖的吸收波段更宽,吸收性能更好,还具有较好的入射角度不敏感性。The invention provides an ultra-broadband absorber in the visible-near-infrared band. The absorber can cover a wider absorption band, has better absorption performance, and has better incident angle insensitivity.
本发明同时提供了一种可见-近红外波段的超宽带吸收器的制备方法,该方方法制备方便,成本低,便于大规模、批量化生产。The invention also provides a method for preparing an ultra-broadband absorber in the visible-near-infrared band, which is convenient for preparation, low in cost, and convenient for large-scale and batch production.
一种可见-近红外波段的超宽带吸收器,包括基底,所述基底上依次设有金属吸收层、锗层以及三层宽波段减反膜层;所述三层宽波段减反膜层分别包括依次设置在锗层上的底层、中间层和最外层,底层、中间层和最外层的折射率逐渐减小。An ultra-broadband absorber in the visible-near-infrared band, including a base, on which a metal absorption layer, a germanium layer, and three layers of wide-band anti-reflection coatings are sequentially arranged; the three-layer wide-band anti-reflection coatings are respectively It includes a bottom layer, a middle layer and an outermost layer sequentially arranged on the germanium layer, and the refractive indexes of the bottom layer, the middle layer and the outermost layer gradually decrease.
下面为基于上述方案的优选的方案:Below is the preferred scheme based on the above-mentioned scheme:
基底材料没有限制,作为优选,所述基底可以选择K9,熔融石英,浮法玻璃等玻璃材料,也可以选择硅,砷化镓等半导体材料。进一步优选为硅片。The substrate material is not limited, and preferably, the substrate can be selected from glass materials such as K9, fused silica, float glass, or semiconductor materials such as silicon and gallium arsenide. More preferably, it is a silicon wafer.
作为优选,所述金属吸收层可以选择铬、钛、铱、钨、镍以及上述材料的合金;作为进一步优选,所述金属吸收层可以选择铬。所述金属吸收层的厚度应大于100nm;进一步优选为100-500nm;跟进一步优选为150-300nm。Preferably, the metal absorption layer can be selected from chromium, titanium, iridium, tungsten, nickel and alloys of the above materials; as a further preference, the metal absorption layer can be selected from chromium. The thickness of the metal absorption layer should be greater than 100 nm; more preferably 100-500 nm; and more preferably 150-300 nm.
作为优选,所述锗层为10nm—40nm;Preferably, the germanium layer is 10nm-40nm;
作为优选,三层宽波段减反膜层由下至上材料折射率逐渐减小,靠近锗层的底层薄膜材料选择硅,厚度为10nm—40nm,进一步优选的厚度为15nm—35nm;所述中间层薄膜材料可以选择二氧化钛、氧化铪、氧化钽、氮化硅等高折射率介质材料,厚度为30nm—80nm,进一步优选的厚度为35nm—60nm;所述最外层薄膜材料可以选择氟化镁、二氧化硅、氟化钇等低折射率介质材料,厚度为70nm—130nm,进一步优选的厚度为80nm—120m。本发明三层宽波段减反膜层由下至上优选为硅、二氧化钛、氟化镁。Preferably, the refractive index of the three-layer broadband anti-reflection film layer gradually decreases from bottom to top, and the bottom film material close to the germanium layer is selected from silicon, with a thickness of 10nm-40nm, and a further preferred thickness of 15nm-35nm; the middle layer The film material can be selected from titanium dioxide, hafnium oxide, tantalum oxide, silicon nitride and other high-refractive index dielectric materials, with a thickness of 30nm-80nm, and a further preferred thickness of 35nm-60nm; the outermost film material can be selected from magnesium fluoride, Low refractive index dielectric materials such as silicon dioxide and yttrium fluoride have a thickness of 70nm-130nm, and a further preferred thickness is 80nm-120m. The three-layer broadband anti-reflection film layer of the present invention is preferably silicon, titanium dioxide, and magnesium fluoride from bottom to top.
本发明同时还提供了一种可见-近红外波段的超宽带吸收器的制备方法,包括如下步骤:The present invention also provides a preparation method of an ultra-broadband absorber in the visible-near-infrared band, comprising the following steps:
(1)根据所要求的吸收器带宽要求和吸收率要求,通过优化各层薄膜的厚度,设计出符合要求的膜系;该步骤可采用现有的软件实现优化操作;(1) According to the required absorber bandwidth requirements and absorption rate requirements, by optimizing the thickness of each layer of film, design a film system that meets the requirements; this step can use existing software to achieve optimization operations;
(2)将基底放入丙酮溶液中超声,接着用乙醇清洗基底;然后将基底放入乙醇溶液中超声,接着用去离子水清洗基底;最后将基底放入去离子水中超声,接着用去离子水再次清洗基底;(2) Put the substrate in acetone solution for ultrasonication, then wash the substrate with ethanol; then put the substrate in ethanol solution for ultrasonication, then wash the substrate with deionized water; finally put the substrate in deionized water for ultrasonication, and then wash it with deionized water Water washes the substrate again;
(3)采用真空镀膜依次沉积各膜层,得到可见—近红外波段的超宽带吸收器。(3) Each film layer is sequentially deposited by vacuum coating to obtain an ultra-broadband absorber in the visible-near infrared band.
作为优选,步骤(2)中,每次超声的时间一般为5-30min;进一步优选为5-10min。As a preference, in step (2), the time for each ultrasound is generally 5-30 minutes; more preferably 5-10 minutes.
本发明的可见—近红外波段的超宽带吸收器,相比于传统的吸收器,它所能覆盖的吸收波段更宽,吸收性能更好,还具有较好的入射角度不敏感性。因此本发明的可见—近红外波段的超宽波段吸收性能上完全超越了传统的吸收器。由于本发明的可见—近红外波段的超宽带吸收器结构是紧凑的多层薄膜结构,相比于传统的宽带吸收器以及近些年提出的人工电磁吸收器,结构更加简单。正由于其紧凑的多层薄膜结构,本发明的可见—近红外波段的超宽带吸收器避免了复杂的纳米加工技术,例如电子束加工技术、聚焦离子束刻蚀技术、反应离子刻蚀技术、光刻技术等等,从而使得生产成本显著下降,生产周期显著缩短,从而便于大规模、批量化生产。Compared with the traditional absorber, the visible-near-infrared ultra-broadband absorber of the present invention can cover a wider absorption band, have better absorption performance, and have better incident angle insensitivity. Therefore, the ultra-wide band absorption performance of the visible-near-infrared band of the present invention completely surpasses the traditional absorber. Since the structure of the ultra-broadband absorber in the visible-near-infrared band of the present invention is a compact multi-layer film structure, the structure is simpler than the traditional broadband absorber and the artificial electromagnetic absorber proposed in recent years. Just because of its compact multi-layer film structure, the ultra-broadband absorber in the visible-near-infrared band of the present invention avoids complex nano-processing technologies, such as electron beam processing technology, focused ion beam etching technology, reactive ion etching technology, Photolithography technology, etc., so that the production cost is significantly reduced, and the production cycle is significantly shortened, thereby facilitating large-scale and batch production.
本发明基于金属吸收层的阻挡入射作用结合锗层的宽波段减反膜层,从而构建了宽波段的无透射的减反结构,因而实现了高效率、角度不敏感的可见—近红外波段超宽带吸收。本发明的可见—近红外波段的超宽带吸收器结构简单,制备方便,成本低,适于大面积批量化地生产,从而使得可见—近红外波段的超宽带吸收器的制备成本大大降低。因此该发明有望在光热转换、电磁吸收、探测以及成像等方面广泛应用,为我国国民经济、社会发展、科学技术和国防建设等领域作出贡献。The present invention is based on the incident blocking effect of the metal absorption layer combined with the wide-band anti-reflection film layer of the germanium layer, thereby constructing a wide-band non-transmission anti-reflection structure, thereby realizing a high-efficiency, angle-insensitive visible-near-infrared band ultra- broadband absorption. The visible-near-infrared band ultra-broadband absorber of the present invention has simple structure, convenient preparation, low cost, and is suitable for large-area batch production, thereby greatly reducing the preparation cost of the visible-near-infrared band ultra-broadband absorber. Therefore, this invention is expected to be widely used in light-to-heat conversion, electromagnetic absorption, detection, and imaging, and contribute to the fields of national economy, social development, science and technology, and national defense construction in our country.
附图说明Description of drawings
图1为本发明可见—近红外波段的超宽带吸收器的结构示意图;Fig. 1 is the structural representation of the ultra-broadband absorber of visible-near-infrared band of the present invention;
图2为本发明可见—近红外波段的超宽带吸收器的制备流程图;Fig. 2 is the preparation flowchart of the ultra-broadband absorber of visible-near infrared band of the present invention;
图3为本发明可见—近红外波段的超宽带吸收器的超宽带吸收机理分析图;Fig. 3 is the analysis diagram of the ultra-broadband absorption mechanism of the ultra-broadband absorber in the visible-near-infrared band of the present invention;
图4为不同吸收带宽要求和吸收率要求的样品的吸收光谱图:Figure 4 is the absorption spectrum diagram of samples with different absorption bandwidth requirements and absorptivity requirements:
图4(a)为实施例1制备的吸收器样品的吸收光谱,400nm—1200nm波段,平均吸收率98.75%以上;Fig. 4 (a) is the absorption spectrum of the absorber sample prepared in embodiment 1, 400nm-1200nm band, the average absorption rate is more than 98.75%;
图4(b)为实施例2制备的吸收器样品的吸收光谱,400nm—2000nm波段,平均吸收率97.75%以上;Fig. 4 (b) is the absorption spectrum of the absorber sample prepared in embodiment 2, 400nm-2000nm band, the average absorption rate is more than 97.75%;
图4(c)为实施例3制备的吸收器样品的吸收光谱,400nm—1200nm波段,平均吸收率99%以上;Fig. 4 (c) is the absorption spectrum of the absorber sample prepared in embodiment 3, 400nm-1200nm band, the average absorption rate is more than 99%;
图4(d)为实施例4制备的吸收器样品的吸收光谱,400nm—2000nm波段,平均吸收率96.2%以上;Fig. 4 (d) is the absorption spectrum of the absorber sample prepared in embodiment 4, 400nm-2000nm band, the average absorption rate is more than 96.2%;
图4(e)为实施例5制备的吸收器样品的吸收光谱,400nm—1200nm波段,平均吸收率98.8%以上;Fig. 4 (e) is the absorption spectrum of the absorber sample prepared in embodiment 5, 400nm-1200nm band, average absorption rate is more than 98.8%;
图4(f)为实施例6制备的吸收器样品的吸收光谱,400nm—2000nm,平均吸收率95.2%以上。Fig. 4(f) is the absorption spectrum of the absorber sample prepared in Example 6, 400nm-2000nm, the average absorption rate is above 95.2%.
具体实施方式Detailed ways
下面结合附图对本发明进行详细说明。The present invention will be described in detail below in conjunction with the accompanying drawings.
如图1所示,一种可见—近红外波段的超宽带吸收器由基底1和五层薄膜组成。基底1材料没有限制,可以选择K9,熔融石英,浮法玻璃等玻璃材料,也可以选择硅,砷化镓等半导体材料。最底层薄膜为金属吸收层2,该层厚度应大于100nm以阻挡入射光透射进入基板;在金属吸收层上面是锗层3,厚度为10nm—40nm,在锗层的上面为三层薄膜(4-6),由下至上材料折射率逐渐减小,该三层可看成锗的宽波段减反膜层。金属吸收层2可以选择铬、钛、铱、钨、镍以及上述材料的合金,本发明金属吸收层2优选为铬。三层宽波段减反膜层(4-6)由下至上材料折射率逐渐减小,靠近锗层3的膜层4薄膜材料选择硅,厚度为10nm—40nm,中间层5薄膜材料可以选择二氧化钛、氧化铪、氧化钽、氮化硅等高折射率介质材料,厚度为30nm—80nm,最外层6薄膜材料可以选择氟化镁、二氧化硅、氟化钇等低折射率介质材料,厚度为70nm—130nm。本发明三层宽波段减反膜层由下至上优选为硅、二氧化钛、氟化镁。As shown in Figure 1, an ultra-broadband absorber in the visible-near infrared band consists of a substrate 1 and five layers of thin films. The material of the substrate 1 is not limited, glass materials such as K9, fused silica, and float glass can be selected, and semiconductor materials such as silicon and gallium arsenide can also be selected. The bottom film is a metal absorption layer 2, and the thickness of this layer should be greater than 100nm to prevent incident light from entering the substrate; above the metal absorption layer is a germanium layer 3, with a thickness of 10nm-40nm, and above the germanium layer is a three-layer thin film (4 -6), the refractive index of the material decreases gradually from bottom to top, and the three layers can be regarded as a wide-band anti-reflection coating layer of germanium. The metal absorption layer 2 can be selected from chromium, titanium, iridium, tungsten, nickel and alloys of the above materials, and the metal absorption layer 2 of the present invention is preferably chromium. The three-layer broadband anti-reflection film (4-6) gradually reduces the refractive index from bottom to top. The film material of the film layer 4 close to the germanium layer 3 is silicon, and the thickness is 10nm-40nm. The film material of the middle layer 5 can be titanium dioxide. , hafnium oxide, tantalum oxide, silicon nitride and other high refractive index dielectric materials, the thickness is 30nm-80nm, the outermost layer 6 thin film materials can choose magnesium fluoride, silicon dioxide, yttrium fluoride and other low refractive index dielectric materials, the thickness It is 70nm-130nm. The three-layer broadband anti-reflection film layer of the present invention is preferably silicon, titanium dioxide, and magnesium fluoride from bottom to top.
一种可见—近红外波段的超宽带吸收器的制备方法,包括以下步骤,如图2所示:A preparation method of an ultra-broadband absorber in the visible-near-infrared band, comprising the following steps, as shown in Figure 2:
1)根据所要求的吸收器带宽要求和吸收率要求,通过优化各层薄膜的厚度,设计出符合要求的膜系;1) According to the required absorber bandwidth requirements and absorption rate requirements, by optimizing the thickness of each layer of film, design a film system that meets the requirements;
2)将基片放入丙酮溶液中超声8分钟,接着用乙醇清洗基片;然后将基片(基底)放入乙醇溶液中超声8分钟,接着用去离子水清洗基片;最后将基片放入去离子水中超声8分钟,接着用去离子水再次清洗基片;2) put the substrate into the acetone solution for 8 minutes, then clean the substrate with ethanol; then put the substrate (substrate) into the ethanol solution for 8 minutes, then clean the substrate with deionized water; finally clean the substrate Put it in deionized water for 8 minutes, and then wash the substrate again with deionized water;
3)采用真空镀膜技术依次沉积各膜层,得到可见—近红外波段的超宽带吸收器;3) Vacuum coating technology is used to deposit each film layer in sequence to obtain an ultra-broadband absorber in the visible-near infrared band;
本发明一种可见—近红外波段的超宽带吸收器的超宽带吸收是基于利用了渐变折射率材料堆积同时形成了多个谐振的机理。如图3,随着膜层的堆积,原先出现的各个谐振反射谷都向长波方向平移,同时,在短波方向出现与该膜层相对应的谐振反射谷。除此之外,随着膜层的堆积,最外层折射率逐渐减小,形成具有减反特性的渐变折射率膜系,使得整体反射率不断降低,从而使得吸收不断增加。因此,本发明一种可见—近红外波段的超宽带吸收器的结构是形成超宽带吸收的最主要原因。The ultra-broadband absorption of the ultra-broadband absorber in the visible-near-infrared band of the present invention is based on the mechanism that multiple resonances are formed simultaneously by stacking graded refractive index materials. As shown in Figure 3, with the accumulation of the film layers, the resonant reflection valleys that originally appeared are translated to the long-wave direction, and at the same time, the resonant reflection valleys corresponding to the film layer appear in the short-wave direction. In addition, with the accumulation of the film layers, the refractive index of the outermost layer gradually decreases, forming a graded refractive index film system with anti-reflection properties, which makes the overall reflectivity decrease continuously, thereby increasing the absorption. Therefore, the structure of an ultra-broadband absorber in the visible-near-infrared band of the present invention is the most important reason for forming the ultra-broadband absorption.
具体实施例方式:Specific embodiment mode:
实施例1:可见—近红外波段超宽带吸收器,预期吸收带宽为400nm—1200nm,平均吸收率在98%以上,本发明设计制备的吸收器样品的吸收光谱如图4(a)所示,平均吸收率98.75%以上,所对应的基底材料为硅片,所对应的膜层材料依次为铬、锗、硅、二氧化钛、氟化镁,各膜层所对应的膜层厚度分别为200nm(铬)、18nm(锗)、19nm(硅)、35nm(二氧化钛)、80nm(氟化镁)。Embodiment 1: Visible-near-infrared band ultra-broadband absorber, the expected absorption bandwidth is 400nm-1200nm, and the average absorption rate is above 98%. The absorption spectrum of the absorber sample prepared by the present invention is as shown in Figure 4 (a), The average absorption rate is above 98.75%. The corresponding substrate material is silicon wafer, and the corresponding film layer materials are sequentially chromium, germanium, silicon, titanium dioxide, magnesium fluoride, and the film thickness corresponding to each film layer is 200nm (chromium ), 18nm (germanium), 19nm (silicon), 35nm (titanium dioxide), 80nm (magnesium fluoride).
实施例2:可见—近红外波段超宽带吸收器,预期吸收带宽为400nm—2000nm,各波长吸收率在90%以上,本发明设计制备的吸收器样品的吸收光谱如图4(b)所示,平均吸收率97.75%%以上,所对应的基底材料为硅片,所对应的膜层材料依次为铬、锗、硅、二氧化钛、氟化镁,各膜层所对应的膜层厚度分别为200nm(铬)、33nm(锗)、32nm(硅)、56nm(二氧化钛)、118nm(氟化镁)。Embodiment 2: Visible-near-infrared band ultra-broadband absorber, the expected absorption bandwidth is 400nm-2000nm, and the absorption rate of each wavelength is above 90%. The absorption spectrum of the absorber sample prepared by the present invention is shown in Figure 4 (b) , the average absorption rate is above 97.75%, the corresponding substrate material is silicon wafer, and the corresponding film layer materials are chromium, germanium, silicon, titanium dioxide, magnesium fluoride in sequence, and the film thickness corresponding to each film layer is 200nm (chromium), 33nm (germanium), 32nm (silicon), 56nm (titanium dioxide), 118nm (magnesium fluoride).
实施例3:与实施例1基本相同,不同之处在于将铬替换为钛,其余条件与实施例1相同,本发明设计的吸收光谱如图4(c)所示,平均吸收率99%以上,各膜层所对应的膜层厚度分别为200nm(钛)、12nm(锗)、17nm(硅)、38nm(二氧化钛)、89nm(氟化镁)。Embodiment 3: basically the same as Embodiment 1, the difference is that chromium is replaced by titanium, all the other conditions are the same as in Embodiment 1, the absorption spectrum designed by the present invention is shown in Figure 4 (c), and the average absorption rate is more than 99% , the film thickness corresponding to each film layer is 200nm (titanium), 12nm (germanium), 17nm (silicon), 38nm (titanium dioxide), 89nm (magnesium fluoride).
实施例4:与实施例2基本相同,不同之处在于将铬替换为钛,其余条件与实施例2相同,本发明设计的吸收光谱如图4(d)所示,平均吸收率96.2%以上,各膜层所对应的膜层厚度分别为200nm(钛)、23nm(锗)、31nm(硅)、55nm(二氧化钛)、119nm(氟化镁)。Embodiment 4: basically the same as Embodiment 2, the difference is that chromium is replaced by titanium, all the other conditions are the same as in Embodiment 2, the absorption spectrum designed by the present invention is shown in Figure 4 (d), and the average absorption rate is more than 96.2% , the film thickness corresponding to each film layer is 200nm (titanium), 23nm (germanium), 31nm (silicon), 55nm (titanium dioxide), 119nm (magnesium fluoride).
实施例5:与实施例1基本相同,不同之处在于将二氧化钛替换为氧化钽,其余条件与实施例1相同,本发明设计的吸收光谱如图4(e)所示,平均吸收率98.8%以上,各膜层所对应的膜层厚度分别为200nm(钛)、18nm(锗)、21nm(硅)、48nm(氧化钽)、101nm(氟化镁)。Embodiment 5: basically the same as Embodiment 1, the difference is that titanium dioxide is replaced by tantalum oxide, all the other conditions are the same as in Embodiment 1, the absorption spectrum designed by the present invention is shown in Figure 4 (e), and the average absorption rate is 98.8% Above, the film thickness corresponding to each film layer is 200nm (titanium), 18nm (germanium), 21nm (silicon), 48nm (tantalum oxide), and 101nm (magnesium fluoride).
实施例6:与实施例2基本相同,不同之处在于将氟化镁替换为二氧化硅,其余条件与实施例2相同,本发明设计的吸收光谱如图4(f)所示,平均吸收率95.2%以上,各膜层所对应的膜层厚度分别为200nm(钛)、32nm(锗)、33nm(硅)、56nm(二氧化钛)、111nm(氟化镁)。Embodiment 6: basically the same as Embodiment 2, the difference is that magnesium fluoride is replaced by silicon dioxide, all the other conditions are the same as in Embodiment 2, the absorption spectrum designed by the present invention is as shown in Figure 4 (f), and the average absorption The ratio is above 95.2%, and the corresponding film thicknesses of each film layer are 200nm (titanium), 32nm (germanium), 33nm (silicon), 56nm (titanium dioxide), and 111nm (magnesium fluoride).
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