TWI688464B - Bionic brightness-enhancing film, its preparation method and applied optical element - Google Patents
Bionic brightness-enhancing film, its preparation method and applied optical element Download PDFInfo
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Abstract
本發明係有關一種仿生增亮膜、其製法及其應用的光學元件,其包括聚苯乙烯奈米球合成步驟、非緊密單層奈米球陣列模板製備步驟及透明增亮層製備步驟。聚苯乙烯奈米球合成步驟係以無乳化劑之乳化聚合反應合成為聚苯乙烯奈米球懸浮液。非緊密單層奈米球陣列模板製備步驟係以(LB)沉積法將聚苯乙烯奈米球懸浮液中之聚苯乙烯奈米球於基板表面組裝排列成一單層非緊密的奈米球陣列模板。透明增亮層製備步驟係將奈米球陣列模板透過奈米壓印微影技術製作成具有次波長結構的模板,再將模板翻模後印製於應用件上,使應用件形成透明增亮層,俾能藉由模仿草蟬翅膀表面所製作出的透明增亮層,除能有效的減緩封裝材料與空氣間的折射率差異,使LED的發光效率提高。 The invention relates to a bionic brightness enhancing film, a method for manufacturing the same, and an optical element using the same, which includes a polystyrene nanosphere synthesis step, a non-compact single-layer nanosphere array template preparation step, and a transparent brightness enhancement layer preparation step. The synthesis step of polystyrene nanospheres is synthesized by emulsification polymerization without emulsifier into polystyrene nanosphere suspension. The preparation step of the non-compact single-layer nanosphere array template is to assemble and arrange the polystyrene nanospheres in the polystyrene nanosphere suspension on the substrate surface into a single-layer non-compact nanosphere array by (LB) deposition method template. The preparation step of the transparent brightness enhancement layer is to make the nanosphere array template into a template with a sub-wavelength structure through the nanoimprint lithography technology, and then print the template on the application part after turning the mold to make the application part transparent and brighten The layer can be used to imitate the transparent brightness enhancement layer made by imitating the surface of grasshopper's wings, in addition to effectively reducing the difference in refractive index between the packaging material and the air, and improving the luminous efficiency of the LED.
Description
本發明係有關一種仿生增亮膜、其製法及其應用的光學元件,尤指一種可以藉由模仿草蟬翅膀表面所製作出之透明增亮層的仿生增亮膜技術。 The invention relates to a bionic brightness enhancing film, a method for manufacturing the same, and optical elements for its application, in particular to a bionic brightness enhancing film technology that can be made by imitating a transparent brightness enhancing layer made on the surface of grasshopper wings.
在全球節能減碳趨勢下,如何提高光電元件的利用率及減少能量的消耗,在能源供應吃緊的情況下變得格外重要。發光二極體(Light-Emitting Diode,LED)是具有體積小,光波長固定、耗電量小等特性的照明元件,而被廣泛應用。但由於LED礙於構裝形式和封裝樹脂的影響,常造成全反射發生於不同材質的界面處,光線無法有效導出,導致其外部量子效率只剩下約15%。根據菲涅耳(Fresnel)理論,光反射會發生在折射率不同的兩個物質的界面處。透過公式(1)可知,當光從具有折射率為n1的介質進入另一種折射率為ng的介質時,由於折射率的不匹配會造成反射(Reflection)現象。 In the global trend of energy saving and carbon reduction, how to improve the utilization rate of photovoltaic elements and reduce energy consumption becomes particularly important in the case of tight energy supply. Light-Emitting Diode (LED) is a lighting element with characteristics of small volume, fixed light wavelength, low power consumption, etc., and is widely used. However, due to the influence of the LED on the structure and the encapsulation resin, the total reflection often occurs at the interface of different materials, and the light cannot be effectively exported, resulting in only about 15% of its external quantum efficiency. According to Fresnel theory, light reflection occurs at the interface between two substances with different refractive indices. It can be seen from formula (1) that when light enters another medium with a refractive index of n g from a medium with a refractive index of n 1 , the reflection phenomenon may be caused due to the mismatch of the refractive indexes.
R(%)=[(n1-ng)/(n1+ng)]2 (1) R(%)=[(n 1 -n g )/(n 1 +n g )] 2 (1)
目前已經有許多降低界面處反射以提高光電元件發光效益的方法。例如,目前多在鏡片表面以濺鍍(Sputtering deposition)方式鍍上多層不同折射率差異約0.1左右的材料來製作光學膜,以提高其抗反射效果,但是利用濺鍍方式製作多層膜的工序十分複雜且良率低、成本高。而除了濺 鍍沉積法之外,也可利用破壞性干涉(Destructive interference)的方式來達到抗反射的目的。但使用破壞性干涉的方式來解決抗反射的問題時,通常只能破壞特定波長的光與其波長相近的光。上述方法皆無法有效的克服光電元件在界面處反光所造成出光率的損失。 There are many methods to reduce the reflection at the interface to improve the luminous efficiency of the photovoltaic element. For example, at present, the surface of the lens is mostly sputtered (Sputtering deposition) with multiple layers of materials with different refractive index differences of about 0.1 to make an optical film to improve its anti-reflection effect, but the process of making a multilayer film by sputtering Complex, low yield and high cost. And besides splashing In addition to the plating deposition method, destructive interference (Destructive interference) can also be used to achieve the purpose of anti-reflection. However, when destructive interference is used to solve the problem of anti-reflection, it is usually only possible to destroy light of a specific wavelength and light with a wavelength close to it. None of the above methods can effectively overcome the loss of light output caused by the reflection of the photoelectric element at the interface.
科學家在電子顯微鏡底下也觀察到螢火蟲的發光器,發現鱗屑狀表面具有週期性的鋸齒狀陣列結構,並將其運用於OLED上,發現它能有效地提升其光通量。此外我們也發現草蟬透明翅膀上也有類似的奈米乳突狀週期性的陣列,由電子顯微鏡照片可觀察到草蟬翅膀表面乳突陣列的間距約為225nm,高度約為270nm(見圖1)。由於其結構週期小於可見光的波長,因此可視為一種次波長結構。 Scientists also observed the firefly's light emitter under the electron microscope and found that the scaly surface has a periodic zigzag array structure, and applied it to the OLED, and found that it can effectively increase its luminous flux. In addition, we also found that there are similar nanopapillary periodic arrays on the transparent wings of grasshoppers. From the electron micrographs, it can be observed that the distance of the papillary arrays on the surface of grasshoppers is about 225nm, and the height is about 270nm (see Figure 1) ). Since its structural period is smaller than the wavelength of visible light, it can be regarded as a sub-wavelength structure.
昆蟲為了在不斷變化的環境中生存,經過數百萬甚至數十億年演化出獨特的身體結構。在自然界中,夜行性的飛蛾其複眼是由數千個直徑約20~30nm的六角形小眼所構成,其中每個小眼的角膜表面都具有規則排列的奈米乳突狀陣列(Corneal nipple array)結構,以避免複眼造成的反光被天敵發現。此種奈米乳突狀陣列,早於1962年被Miller與Bernhard等人所發現,此種奈米級的特殊排列,可視為一種次波長結構(Sub-wavelength structure,SWS)。接著1991年Southwell率先提出以蛾眼效應原理設計出週期性的抗反射陣列,並利用此法來探討其折射率變化。文中提及為了避免繞射現象的產生,抗反射陣列的週期需小於可見光的波長,即達到次波長結構。可藉由公式(2)計算出合適的結構週期,其中p為次波長結構之週期,l為欲達到抗反射之波長,n s 為次波長結構之材料折射率。 In order to survive in a constantly changing environment, insects have evolved unique body structures after millions or even billions of years. In nature, the compound eye of a nocturnal moth is composed of thousands of hexagonal small eyes with a diameter of about 20 to 30 nm, and the corneal surface of each small eye has a regularly arranged nanopapillary array (Corneal nipple array) structure to prevent the reflection caused by compound eyes from being discovered by natural enemies. This kind of nanopapillary array was discovered by Miller and Bernhard et al. in 1962. This kind of nano-level special arrangement can be regarded as a sub-wavelength structure (SWS). Then in 1991, Southwell first proposed to design a periodic anti-reflective array based on the principle of moth-eye effect, and used this method to explore its refractive index changes. It is mentioned that in order to avoid the occurrence of diffraction, the period of the anti-reflection array needs to be less than the wavelength of visible light, that is, to reach the sub-wavelength structure. The appropriate structural period can be calculated by formula (2), where p is the period of the sub-wavelength structure, l is the wavelength to be anti-reflected, and n s is the refractive index of the material of the sub-wavelength structure.
主要是因其奈米柱間之間距小於可見光波長的一半。當光波遇到此種結構時,光波會根據漸變折射率(Gradient refractive index)理論,使光沿著深度軸的方向呈緩和的連續變化。就像是光線穿過層層折射率相近的材質,使得任意角度入射的光幾乎都能被次波長結構所吸收。次波長結構能有效抑制不一樣波長的反射光,如紫外光、可見光、紅外光等,導致其反射率極低。公式(3)為藉由等效介質理論(Effective medium theory)推導所獲得的次波長結構的等效折射率。其中,neff為等效折射率,f為次波長結構所占之填充係數(Fill factor),na為次波長材料的折射率,nb為空氣的折射率。 Mainly because the distance between nanopillars is less than half of the visible wavelength. When the light wave encounters such a structure, the light wave will gradually and continuously change along the depth axis according to the gradient refractive index theory. It is like the light passing through layers of materials with similar refractive index, so that light incident at any angle can be almost absorbed by the sub-wavelength structure. The sub-wavelength structure can effectively suppress the reflected light of different wavelengths, such as ultraviolet light, visible light, infrared light, etc., resulting in extremely low reflectivity. Formula (3) is the equivalent refractive index of the sub-wavelength structure obtained by deriving the effective medium theory. Wherein, n eff is the equivalent refractive index, f is the sub-wavelength structure occupies the fill factor (Fill factor), n a is the refractive index of the material times the wavelength, n b is the refractive index of air.
本發明係由中華民國專利資訊檢索系統針對關鍵字:「增亮膜」、「光導膜」等關鍵字進行交叉搜尋,並針對相關專利差異性進行探討,相關專利則如下列所述: In the present invention, the patent information retrieval system of the Republic of China conducts a cross-search on keywords such as "brightening film", "light guide film" and other keywords, and discusses the differences of related patents. The related patents are as follows:
1.專利名稱:發光裝置和顯示器(專利公開號I570965)該發明所揭露的發光裝置包含基板、光源組件、光取出層和第一光學粒子。光源組件包含發光元件與封裝結構。發光元件設置於基板。發光元件具出光面,且封裝結構設置於出光面。光取出層設置於光源組件的封裝結構。光取出層具相對的第一表面和第二表面,且第二表面面向光源組件。第一光學粒子嵌設於光取出層並且突出於第一表面。第一光學粒子具第一折射率,光取出層具一第二折射率,且封裝結構具一第三折射率。第一折射率大於空 氣之折射率,且第二折射率大於第一折射率與第三折射率。根據本發明所揭露的發光裝置以及包含此發光裝置的顯示器,當光源組件產生之光線自光取出層出射至發光裝置外部時,部分光線先自光取出層入射至第一光學粒子中,接著再從第一光學粒子入射至發光裝置外部。由於光取出層的第二折射率大於第一光學粒子的第一折射率,且第一折射率大於空氣之折射率,因此發光裝置於第一表面具有較為緩和的折射率變化,有助於避免光線自光取出層入射至發光裝置外部時產生全反射,進一步提升發光裝置的光取出效率。該研究的光取出方式與本發明利用仿蟬翼之表面次波長結構有所差異。 1. Patent name: Light-emitting device and display (Patent Publication No. I570965) The light-emitting device disclosed in this invention includes a substrate, a light source assembly, a light extraction layer, and first optical particles. The light source assembly includes a light emitting element and a packaging structure. The light emitting element is provided on the substrate. The light emitting element has a light emitting surface, and the packaging structure is disposed on the light emitting surface. The light extraction layer is provided in the packaging structure of the light source assembly. The light extraction layer has opposing first and second surfaces, and the second surface faces the light source assembly. The first optical particles are embedded in the light extraction layer and protrude from the first surface. The first optical particle has a first refractive index, the light extraction layer has a second refractive index, and the packaging structure has a third refractive index. The first refractive index is greater than empty The refractive index of gas, and the second refractive index is greater than the first refractive index and the third refractive index. According to the light-emitting device and the display including the light-emitting device disclosed in the present invention, when the light generated by the light source assembly exits from the light extraction layer to the outside of the light-emitting device, part of the light first enters the first optical particles from the light extraction layer, and then The first optical particles are incident outside the light emitting device. Since the second refractive index of the light extraction layer is greater than the first refractive index of the first optical particles, and the first refractive index is greater than the refractive index of air, the light emitting device has a relatively gentle refractive index change on the first surface, which helps to avoid When light enters the outside of the light emitting device from the light extraction layer, it is totally reflected, which further improves the light extraction efficiency of the light emitting device. The light extraction method of this study is different from the surface sub-wavelength structure of the present invention using the imitating cicada wings.
2.專利名稱:製造光導膜的方法(專利公開號I582475)該發明係關於一種製造光導膜的方法。光導(lightguide)是一種膜,在其上下表面之間提供對於光的實質全內反射。光係自一或多個光源而入射於該膜的邊緣(該邊緣係垂直於該膜的上下表面)。光導膜在該上下表面包括有經織構的輪廓(textured profile)時能用作為背光單元,以便使光自光導膜散射出。經織構的表面藉由折射及/或全反射而將光重新導出於光導膜之外。該發明提供一種製造光導膜的方法,包含:(a)提供一光導膜,具有一上表面及一下表面,而供光在該上表面與該下表面之間為實質全內反射;(b)施加一可流動性且可固化的材料於至少該下表面而成一圖案;(c)施加一表面織構於該材料;以及(d)固化該材料,而使於位在該光導膜上所得到經表面織構的圖案得以自該光導膜提取出光。在步驟(b)中所施加的該材料可包括一可固化樹脂。其可包括散射奈米顆粒(例,TiO2),以促進散射。其可包括紫外光調降浸灰添加劑,諸如:UV吸收劑或是磷光劑之類的活性成分。其可應用於高解析 度印刷處理,例如:噴墨印刷或網版印刷。該材料的用量可隨著整個該表面而改變。特別是,該材料可僅施加於該光導膜提取出光的部分。在步驟(b)之前,可於該表面施加一表面改質劑,例,聚合物或低聚物。此種表面改質的作用可為平坦化、表面能改變、或修改或匹配折射率。步驟(c)中所施加的織構可經配置而配合該材料之圖案以增進光散射。該織構可為均佈於整個該表面、或是隨著整個該表面而改變,以有效地產生均勻照明或產生照明會變化的圖案。該織構可包括一隨機粗糙化的輪廓或是週期性幾何微結構,例如:角柱形、角錐形、圓錐形及/或微透鏡形。步驟(c)可包括例如捲對式凸印(reel-to-reel embossing)或沖壓凸印(stamping embossing)。為了提供具有兩個相對的織構表面,步驟(b)、(c)及(d)中能夠對該光導膜之上表面與下表面予以執行上述的可選特徵。該研究之光導膜製作方法與本發明利用微奈米壓印製作增亮膜方式與光導結構有所差異。 2. Patent name: Method of manufacturing light guide film (Patent Publication No. I582475) This invention relates to a method of manufacturing light guide film. A lightguide is a film that provides substantial total internal reflection of light between its upper and lower surfaces. The light is incident on the edge of the film from one or more light sources (the edge is perpendicular to the upper and lower surfaces of the film). The light guide film can be used as a backlight unit when the upper and lower surfaces include a textured profile to scatter light from the light guide film. The textured surface redirects light out of the light guide film by refraction and/or total reflection. The invention provides a method for manufacturing a light guide film, comprising: (a) providing a light guide film having an upper surface and a lower surface, and the light supply is substantially total internal reflection between the upper surface and the lower surface; (b) Applying a flowable and curable material to at least the lower surface to form a pattern; (c) applying a surface texture to the material; and (d) curing the material so that it is obtained on the light guide film The surface textured pattern can extract light from the light guide film. The material applied in step (b) may include a curable resin. It may include scattering nanoparticles (eg, TiO 2 ) to promote scattering. It may include ultraviolet light-regulating leaching additives, such as active ingredients such as UV absorbers or phosphorescent agents. It can be applied to high-resolution printing processes, such as inkjet printing or screen printing. The amount of the material can vary with the entire surface. In particular, the material may be applied only to the portion where the light guide film extracts light. Before step (b), a surface modifier such as polymer or oligomer can be applied to the surface. The effect of such surface modification may be to flatten, change the surface energy, or modify or match the refractive index. The texture applied in step (c) can be configured to match the pattern of the material to enhance light scattering. The texture can be uniformly distributed on the entire surface, or can change along with the entire surface, so as to effectively produce uniform illumination or produce patterns in which the illumination changes. The texture may include a randomly roughened profile or periodic geometric microstructures, such as: prismatic, pyramidal, conical, and/or microlens shaped. Step (c) may include, for example, reel-to-reel embossing or stamping embossing. In order to provide two opposite textured surfaces, the optional features described above can be performed on the upper and lower surfaces of the light guide film in steps (b), (c) and (d). The manufacturing method of the light guide film in this study is different from the method and the light guide structure of the invention for making the brightness enhancement film by micro-nano imprinting.
3.專利名稱:具有微結構增亮膜的照明裝置(專利公開號I452231)該發明涉及一種能夠照明的器具,尤指一種具有微結構增亮膜的照明裝置。目前一般現有的平面光源,所投射出的光源場形為Lambertian,即朗伯光源。平面光源所射出的光線的發散角大,容易造成發光效率不佳以及中心發光強度偏低的缺點,當應用於照明裝置,例如車尾燈時,需要採用多顆OLED(有機發光二極)才能達到法規對於照明亮度的要求,如此會大幅增加製造成本。該發明所運用的技術手段在於提供一種具有微結構增亮膜的照明裝置,包括:一殼體;一平面光源,其固設於該殼體內並設有一頂面;一微結構增亮膜,其固設於該殼體並位於該平面光源的頂面的上方;該微結構增亮膜為一能夠透光的薄狀片體並設有一頂部、一底面及一菲涅 爾聚光部,,該微結構增亮膜的底面為一平面,該菲涅爾聚光部位於該微結構增亮膜的頂部,該菲涅爾聚光部設有一中心及一外周緣,該菲涅爾聚光部於垂直方向的截面形狀呈鋸齒狀並自該中心開始朝向該外周緣而呈兩次以上的週期性變化,其中,於第一次週期的部份形成一第一聚光區,該第一聚光區包括有複數個圍繞的鋸齒,該複數個鋸齒相互鄰接並以該中心而呈圍繞分布;於第二次週期的部份形成一第二聚光區,該第二聚光區圍繞並鄰接於該第一聚光區;該第二聚光區的鋸齒的排列順序、截面形狀皆與該第一聚光區相同;以及一反射體,其固設於該殼體內並圍繞於該平面光源。該專利之微結構增亮膜與本發明透過模仿草蟬翅翼表面結構之次波長結構增亮膜有所差異。 3. Patent name: Illumination device with microstructure brightness enhancement film (Patent Publication No. I452231) This invention relates to an appliance capable of illuminating, in particular to an illumination device with microstructure brightness enhancement film. At present, generally existing planar light sources project a light source field shape of Lambertian, namely Lambertian light source. The divergence angle of the light emitted by the planar light source is large, which is easy to cause the shortcomings of poor luminous efficiency and low central luminous intensity. When used in lighting devices, such as rear lights, multiple OLEDs (organic light-emitting diodes) are required to achieve The requirements of the regulations on the brightness of lighting will greatly increase the manufacturing cost. The technical means used in this invention is to provide a lighting device with a microstructure brightness enhancement film, including: a housing; a planar light source, which is fixed in the housing and is provided with a top surface; and a microstructure brightness enhancement film, It is fixed on the housing and located above the top surface of the planar light source; the microstructure brightness enhancement film is a thin sheet that can transmit light and is provided with a top, a bottom surface and a Fresnel Concentration part, the bottom surface of the microstructure brightness enhancement film is a plane, the Fresnel light concentration part is located on the top of the microstructure brightness enhancement film, the Fresnel light concentration part is provided with a center and an outer periphery, The cross-sectional shape of the Fresnel condensing part in the vertical direction is zigzag, and from the center toward the outer periphery, there are more than two periodic changes, wherein a first condensing is formed in the part of the first cycle Light zone, the first condensing zone includes a plurality of surrounding serrations, the plurality of serrations are adjacent to each other and are distributed around the center; a second condensing zone is formed in the part of the second cycle The second light-concentrating area surrounds and is adjacent to the first light-concentrating area; the arrangement order and cross-sectional shape of the saw teeth of the second light-concentrating area are the same as the first light-concentrating area; and a reflector is fixed to the shell The body and surrounding the plane light source. The microstructure brightness enhancement film of this patent is different from the present invention by imitating the subwavelength structure brightness enhancement film of the wing surface structure of the grasshopper.
有鑑於上述該等專利確實皆未臻完善,仍有再改善的必要性,緣是,本發明人等乃經不斷的努力研發之下,終於研發出一套有別於上述習知技術的本發明。 In view of the fact that the above patents have indeed not been perfected, there is still a need for further improvement. The reason is that after continuous research and development, the inventors have finally developed a set of books that are different from the above-mentioned conventional technologies. invention.
本發明主要目的在於提供一種仿生增亮膜、其製法及其應用的光學元件,主要是藉由模仿草蟬翅膀表面所製作出的透明增亮層,除能有效減緩封裝材料與空氣間的折射率差異之外,並能有效提升發光二極體發光效率或其他光學元件的透光能力。達成本發明主要目的之技術手段,係包括聚苯乙烯奈米球合成步驟、非緊密單層奈米球陣列模板製備步驟及透明增亮層製備步驟。聚苯乙烯奈米球合成步驟係以無乳化劑之乳化聚合反應合成為聚苯乙烯奈米球懸浮液。非緊密單層奈米球陣列模板製備步驟係以藍牟耳(Langmuir-Blodgett,LB)沉積法將聚苯乙烯奈米球懸浮液中之 聚苯乙烯奈米球於基板表面組裝排列成一單層非緊密的奈米球陣列模板。透明增亮層製備步驟係將奈米球陣列模板透過奈米壓印微影技術製作成具有次波長結構的模板,再將模板翻模後印製於應用件上,使應用件形成透明增亮層。 The main purpose of the present invention is to provide a bionic brightening film, its manufacturing method and the optical element used therefor, mainly by imitating the transparent brightening layer made by imitating the surface of grasshopper wings, in addition to effectively reducing the refraction between the packaging material and the air In addition to the rate difference, it can effectively improve the luminous efficiency of the light-emitting diode or the light-transmitting ability of other optical components. The technical means to achieve the main purpose of the invention include a polystyrene nanosphere synthesis step, a non-compact single-layer nanosphere array template preparation step and a transparent brightness enhancement layer preparation step. The synthesis step of polystyrene nanospheres is synthesized by emulsification polymerization without emulsifier into polystyrene nanosphere suspension. The preparation step of the non-compact single-layer nanosphere array template is to use the Langmuir-Blodgett (LB) deposition method to deposit the polystyrene nanosphere suspension in The polystyrene nanospheres are assembled on the surface of the substrate to form a single-layer non-compact nanosphere array template. The preparation step of the transparent brightness enhancement layer is to make the nanosphere array template into a template with a sub-wavelength structure through the nanoimprint lithography technology, and then print the template on the application part after turning the mold to make the application part transparent and brighten Floor.
10‧‧‧超基板 10‧‧‧Super substrate
11‧‧‧奈米球陣列模板 11‧‧‧Nano ball array template
12‧‧‧LB槽 12‧‧‧LB slot
13‧‧‧奈米球 13‧‧‧Nano ball
14‧‧‧PDMS模仁 14‧‧‧ PDMS mold kernel
15‧‧‧紫外線光學固化膠 15‧‧‧UV optical curing adhesive
20‧‧‧應用件 20‧‧‧Application
21‧‧‧透明增亮層 21‧‧‧Transparent brightening layer
圖1(a)係草蟬翅膀表面乳突陣列每條約1um的電子顯微鏡照片;(b)係草蟬翅膀表面乳突陣列每條約100um的電子顯微鏡照片。 Fig. 1 (a) is an electron microscope photograph of the papillary array on the surface of the grasshopper's wings 1um per treaty; (b) is an electron microscope photograph of the papillary array on the surface of the grasshopper's wings 100um per treaty.
圖2(a)係本發明非緊密單層奈米球陣列模板製備步驟的流程示意圖;(b)係本發明透明增亮層製備步驟的前段流程示意圖;(c)係本發明透明增亮層製備步驟的後段流程示意圖。 Fig. 2 (a) is a schematic flow chart of the preparation steps of the non-compact single-layer nanosphere array template of the present invention; (b) is a schematic flowchart of the front stage of the preparation step of the transparent brightening layer of the present invention; (c) is a transparent brightening layer of the present invention Schematic diagram of the latter stage of the preparation step.
圖3係本發明奈米微球粒徑分佈示意,其中直徑為(a)為197nm;(b)為255nm;(c)為300nm。 Fig. 3 is a schematic diagram of the particle size distribution of the nanomicrospheres of the present invention, wherein the diameter is (a) 197nm; (b) 255nm; (c) 300nm.
圖4係本發明奈米微球之電子顯微鏡照片具有不同尺寸外徑,其中(a)為氧電漿蝕刻處理之前的照片;(b)為氧電漿蝕刻處理之後的照片;(c)是(b)的的橫截面之電子顯微鏡圖像。 FIG. 4 is an electron microscope photograph of nanospheres of the present invention having different sizes and outer diameters, where (a) is a photograph before oxygen plasma etching; (b) is a photograph after oxygen plasma etching; (c) is (b) The electron microscope image of the cross section.
圖5係本發明以AFM觀察翻模複製後所得具次波長結構的表面形貌及其所對應之縱剖面圖。 FIG. 5 is a longitudinal cross-sectional view of the surface morphology of the sub-wavelength structure obtained by the AFM observation after the mode is copied by the present invention.
圖6係本發明具BEL結構覆蓋之玻璃的反射與穿透光譜對照示意。 FIG. 6 is a comparison diagram of the reflection and transmission spectra of the glass covered by the BEL structure of the present invention.
圖7(a)為一般白光燈泡的EL光譜;圖7(b)(c)(d)分別是以粒徑197、255、300nm之奈米球所衍生製作具有BEL結構玻璃覆蓋在和圖7(a)相同的白光LED燈泡表面所量測到的發光光譜示意圖。 Fig. 7(a) is the EL spectrum of a general white light bulb; Fig. 7(b)(c)(d) is derived from nanospheres with a particle size of 197, 255, and 300 nm, respectively, and is made of glass with a BEL structure. (a) Schematic diagram of the luminescence spectrum measured on the surface of the same white LED bulb.
為讓 貴審查委員能進一步瞭解本發明整體的技術特徵與達成本發明目的之技術手段,玆以具體實施例並配合圖式加以詳細說明:依據所知,發光二極體(Light-Emitting Diode,LED)由於耗電量低、壽命長,用途廣泛。但由於在構裝上常於不同材質的界面處會產生反射或全反射現象而降低其光萃率,因此,如何提高LED的發光效益,在重視能源利用率的年代便顯得格外重要。在大自然中,草蟬為了避免被天敵捕食,在歷經長時間的演化後在其翅翼上形成了一種特殊的次波長陣列結構能有效降低翅翼表面的反光,達到避敵的作用。於是,本發明係以粒徑255nm聚苯乙烯奈米球所翻印的TMPTA增亮層,除能有效降低反射率至0.87%,並保有最高穿光學透率達96.9%,亦能將LED的發光強度提升55%。本發明所提供之製程技術,未來尚能應用於微精密產業與光電產業的發展上。 In order to enable your reviewing committee to further understand the overall technical features of the present invention and the technical means to achieve the purpose of the invention, specific examples and drawings are used to explain in detail: According to the knowledge, the light-emitting diode (Light-Emitting Diode, (LED) Because of low power consumption and long life, it is widely used. However, due to the fact that reflection or total reflection will often occur at the interface of different materials on the structure to reduce its light extraction rate, how to improve the luminous efficiency of LEDs is particularly important in the era of energy efficiency. In nature, in order to avoid being preyed by natural enemies, grasshoppers have formed a special sub-wavelength array structure on their wings after a long period of evolution, which can effectively reduce the reflection on the surface of the wings and avoid the enemy. Therefore, the present invention is a TMPTA brightening layer printed with a polystyrene nanosphere with a particle size of 255nm. In addition to effectively reducing the reflectance to 0.87%, and maintaining the highest transmissivity of optical transmission to 96.9%, it can also emit light from the LED. Strength increased by 55%. The process technology provided by the present invention can still be applied to the development of micro-precision industry and optoelectronic industry in the future.
請配合參看圖1~4所示,為達成本發明主要目的之實施例,係包括下列步驟: Please refer to Figures 1 to 4 for the implementation of the main purpose of the invention, which includes the following steps:
(a)聚苯乙烯奈米球合成步驟:係以無乳化劑的乳化聚合反應合成為聚苯乙烯奈米球懸浮液。 (a) Synthesis step of polystyrene nanospheres: It is synthesized by emulsification polymerization without emulsifier into polystyrene nanosphere suspension.
(b)非緊密單層奈米球陣列模板製備步驟:以Langmuir-Blodgett(LB)沉積法將聚苯乙烯奈米球懸浮液中之聚苯乙烯奈米球13於一基板10(如透光玻璃)表面組裝排列成一單層非緊密的奈米球陣列模板11。
(b) Preparation of non-compact single-layer nanosphere array template: Langmuir-Blodgett (LB) deposition method is used to deposit
(c)透明增亮層21製備步驟:係將奈米球陣列模板11透過奈米壓印微影技術製作成具有次波長結構的奈米球陣列模板11,再將奈米球陣列模板
11翻模後印製於一應用件20上,使該應用件20上形成一具低反射與高透光特性的透明增亮層21。
(c) Preparation step of the transparent brightness enhancement layer 21: the nano-ball array template 11 is made into a nano-ball array template 11 with a sub-wavelength structure through the nanoimprint lithography technology, and then the nano-ball array template
11 Printed on an
具體的,於上述聚苯乙烯奈米球13合成步驟中,係於四頸反應瓶內加入35~45mg(較佳為40mg)磺酸鈉(4-styrenesulfonic acid sodium salt hydrate,NaSS;Alfa Aesar)共聚單體、5~15g(較佳為8g)苯乙烯單體(styrene,St;Sigma-Aldrich)、75~95mg(較佳為87mg)的過硫酸鉀(potassium persulfate,KPS;J.T.Baker)做為起始劑與70~90g(較佳為80g)去離子水(deionized water),利用機械攪拌裝置以轉速280~320rpm(較佳為300rpm)均勻攪拌,再搭配冷凝回流裝置於氮氣環境下連續反應約1天後,再將所製備的該聚苯乙烯奈米微球懸浮液透過型離心機以轉速5500~6500rpm(較佳為6000rpm)進行離心15~25分鐘(較佳為20分鐘),隨後取出上層液即可獲得粒徑均一的聚苯乙烯奈米球懸浮液。
Specifically, in the above synthesis step of
具體的,於上述非緊密單層奈米球陣列模板11製備步驟中,係將基板10浸泡於40~60ml(較佳為50ml)的0.25M氫氧化鈉水溶液中15~25分鐘(較佳為20分鐘)進行親水性改質,改質完成後以離子水進行沖洗,並浸泡於去離子水中待用;為了順利鋪展聚苯乙烯奈米微球於LB槽12之水面上,本發明選擇60%乙醇(ethanol;Merck)水溶液做為分散溶劑,將其混入聚合後之聚苯乙烯奈米球懸浮液中,再將180~220ml二次離子水倒入自組裝LB(Langmuir-Blodgett)槽12中,再將改質過的親水性基板10斜置於LB槽12擋板邊緣,利用蠕動幫浦將聚苯乙烯奈米球懸浮液滴於親水性基板10表面,使聚苯乙烯奈米球13藉由擴散的方式均勻分散於氣-液界面,使原本雜亂分佈的聚苯乙烯奈米球13透過自組裝排列方式擠壓形成單層的緊密排列。其中,為了使單層的緊密排列的聚苯乙烯陣列中的奈米球13的粒徑縮
小形成非緊密(non-close-packed)的陣列結構以做為後續次波長結構模板11之用,本發明利用功率40W,氧氣流量為0.7sccm的氧氣電漿(oxygen plasma treatment;Plasma Cleaner,PCD 150,All Real Tech.)分別對所聚合的不同尺寸的聚苯乙烯奈米球13緊密單層陣列模板11進行氧電漿蝕刻處理,其過程如圖2(a)所示,經氧電漿蝕刻處理後,即可使奈米球13縮小,並使奈米球13間形成間距。
Specifically, in the above preparation step of the non-compact single-layer nanosphere array template 11, the
具體的,於上述增亮層製備步驟中,係將矽油(silicone oil,Sigma-Aldrich)、硬化劑(curing agent)、聚二甲基矽氧烷(polydimethylsiloxane,PDMS;Sylgard 184,Dow Corning)之主劑(base)以質量比為1.5~2.5:1:9~11(較佳為2:1:10)的比例混合均勻後,靜置於冰箱在攝氏4度左右的溫度環境約25~35分鐘(較佳為30分鐘),使其消泡,將其緩慢澆注於非緊密陣列的奈米球陣列模板11表面,再將其置於攝氏50~70℃(較佳為60℃)真空烘箱中烘烤1.5~2.5小時(較佳為2小時),固化後脫模(demold),以獲得凹洞狀PDMS模仁14,其流程如圖2(b);然後將紫外線光學固化膠15(trimethylolpropane Triacrylate,TMPTA;shirakawa)均勻滴覆於應用件20表面,再將凹洞狀PDMS模仁14覆蓋於應用件20之紫外線光學固化膠15上,並以1.5~2.5kg/cm2(較佳為2kg/cm2的壓力)的壓力進行壓印,最後再以紫外光(Philips Actinic BL TL 8W,365nm,5mW/cm2)照射30~50分鐘(較佳為40分鐘),使其固化脫模後,以獲得表面具有次波長結構的應用件20(如透光玻璃基板)。 Specifically, in the above step of preparing the brightness enhancement layer, silicone oil (Sigma-Aldrich), curing agent (curing agent), polydimethylsiloxane (PDMS; Sylgard 184, Dow Corning) are used After mixing the base agent in a mass ratio of 1.5~2.5:1:9~11 (preferably 2:1:10), put it in a refrigerator at a temperature of about 4 degrees Celsius for about 25~35 Minutes (preferably 30 minutes) to defoam, slowly cast it on the surface of the nano-ball array template 11 of the non-compact array, and then place it in a vacuum oven at 50~70℃ (preferably 60℃) Bake for 1.5~2.5 hours (preferably 2 hours), demold after curing to obtain the cavity-shaped PDMS mold core 14, the process is shown in Figure 2(b); then the UV optical curing adhesive 15( trimethylolpropane Triacrylate, TMPTA; shirakawa) uniformly drip on the surface of the application 20, and then cover the concave PDMS mold 14 on the ultraviolet optical curing adhesive 15 of the application 20, and use 1.5~2.5kg/cm 2 (preferably Pressure of 2kg/cm 2 ), and finally irradiated with ultraviolet light (Philips Actinic BL TL 8W, 365nm, 5mW/cm 2 ) for 30 to 50 minutes (preferably 40 minutes) to cure and remove After the mold, an application 20 (such as a light-transmitting glass substrate) having a sub-wavelength structure on the surface is obtained.
本發明較具體的應實施例中,上述應用件20係為光學元件,該光學元件係為發光二極體LED的透明上蓋;或是為顯示器的玻璃基板;或是太陽能電池的玻璃基板。
In a more specific embodiment of the present invention, the above-mentioned
本發明利用動態光散射粒徑分析及界面電位分析儀
(Zetasizer;3000HS,Malvern Instruments)量測合成之聚苯乙烯奈米球13之平均粒徑。以場發射型掃描式電子顯微鏡(Field Emission Scanning Electron Microscope,FE-SEM;JSM-7610F,JEOL)觀察緊密與非緊密聚苯乙烯單層奈米球13陣列之排列情形。以原子力顯微鏡(Atomic Force Microscopy,AFM,DI 3100,Digital Instruments)量測次波長陣列之表面形貌、深度及週期。利用紫外線可見光分光光譜儀(UV-Vis Spectrophotometer;Cary 50,Varian)量測所製作完成之TMPTA增亮膜之穿透與反射光譜。製作完成之增亮膜的光亮度(Luminance)等特性由高分辨率光纖光譜儀(High-resolution fiber optic spectrometer;HR2000+CG-UV-NIR)進行量測。
The invention utilizes dynamic light scattering particle size analysis and interface potential analyzer
(Zetasizer; 3000HS, Malvern Instruments) measured the average particle size of the synthesized
為了要製作出高寬比較佳的SWS結構,本發明合成了三種尺寸大小不同的聚苯乙烯奈米球13。經由動態光散射粒徑分析儀測量其平均粒徑大小分別為197、255、300nm,奈米球13粒徑的分散係數(Polydispersity Index,PdI)則分別為0.021、0.012、0.009,顯示出所聚合的奈米球13粒徑相當均一,如圖3(a)(b)(c)所示。
In order to produce a SWS structure with better height and width, the present invention synthesizes three
為探討氧氣電漿處理時間對奈米球13粒徑之影響,圖4(a)之SEM照片為經由Langmuir-Blodgett(LB)裝置進行自組裝沉積後所形成的單層緊密排列陣列,奈米球13之平均粒徑分別約為197、255、300nm。透過氧氣電漿處理可有效地將聚苯乙烯奈米球13之尺寸分別縮小至175、224、247nm,使奈米球13間產生間距,如圖4(b)所示。若奈米球13太小,經氧電漿蝕刻後表面形貌會呈現不規則形狀,見圖4(b),如此會降低次波長結構的光學抗反射能力。圖4(c)為對應於圖4(b)之截面圖。
In order to explore the effect of oxygen plasma treatment time on the particle size of
圖5為以AFM觀察翻模複製後所得具次波長結構的表面形貌及其所對應之縱剖面圖。圖5(a),(b),(c)為以TMPTA材料分別對粒徑為197,255,300nm奈米球13所製作之奈米陣列模仁所複製具乳凸狀陣列之增亮膜,其所對應的高度(h)與寬度(d)分別約為175nm與113nm,235nm與221nm,
247nm與287nm,而其高寬比則分別為1.54,1.06與0.86。其中,以粒徑255nm的聚苯乙烯奈米球13所製作的奈米陣列在經過氧電漿蝕刻使粒徑縮小後所形成的間距,較容易使PDMS溶膠滲入奈米球13之間的縫隙,使後續翻模所得到的次波長結構的高寬比較接近琉璃草蟬翅膀上的乳突狀陣列結構的高寬比(見圖1(c)約1.20)。
FIG. 5 is an AFM observation of the surface morphology of the sub-wavelength structure and the corresponding longitudinal cross-sectional view obtained after the over-mold replication. Fig. 5 (a), (b), (c) is a brightness enhancement film with a convex-shaped array replicated by a TMPTA material on a nano-array die made of nano-particles with a particle size of 197, 255, and 300 nm, respectively. The corresponding height (h) and width (d) are about 175nm and 113nm, 235nm and 221nm,
247nm and 287nm, and its aspect ratio is 1.54, 1.06 and 0.86 respectively. Among them, the nano-array made of polystyrene nano-
圖6(a),(b)-(i)(ii)(iii)為以粒徑197、255、300nm的奈米球13所衍生製作出具有BEL結構覆蓋之玻璃,(v)為裸玻璃,所對應之光學最低反射率與最高穿透率分別為1.63、0.87、1.34、4.00%,與92.1、96.9、95.6、90.0%。由圖6(a,b)(ii)可以觀察到以粒徑為255nm奈米球13所製作之BEL結構能有效提升玻璃之穿透度達到最大值(96.9%)且又同時能將其光學反射率降到最低(0.87%)。根據Hadobas等人研究發現抗反射效果會隨SWS結構中高寬比值的增加而更趨明顯[19]。以197nm之奈米球13所衍生製作的BEL膜,雖然是三者中具有最高的高寬比值(1.54)者,但由於粒徑較小的奈米球13在氧電漿蝕刻過程容易造成堆疊與位移,使其無法形成較完美的週期排列,(見圖4(b)之SEM照片),導致無法達到預期的最大值。
Fig. 6 (a), (b)-(i)(ii)(iii) is a glass with BEL structure covered by
圖7(a)為一般的白光LED(Huankwun,150cd/m2)燈泡的EL光譜,其發光強度值約為0.99,而圖7(b)(c)(d)則是以粒徑197、255、300nm之奈米球13所衍生製作具有BEL結構玻璃覆蓋在和圖7(a)相同的白光LED燈泡表面所量測到的發光光譜,其強度值分別為1.16、1.36、1.53。以粒徑255nm奈米球13所製作之BEL結構增亮層可使LED的發光值由0.99增加到1.53,增強了約55%。此外,我們也觀察到LED不管有無增亮層發光光譜並不會位移。次波長結構陣列能有效的降低界面處的光反射並能提高其光學穿透度。而抗反射能力的提升可由等效介質理論中次波長結構的填充因子(Fill factor)與等效折射率的改變加以解釋,即配合公式(2)與公式(4)進行說明。
Fig. 7(a) is the EL spectrum of a general white LED (Huankwun, 150cd/m 2 ) bulb, and its luminous intensity value is about 0.99, while FIG. 7(b)(c)(d) is based on the particle size of 197, The luminescence spectrum measured by the 255 and 300
公式(4)中,f為次波長結構中之填充因子,A為具次波長結構的奈米球13陣列所佔之面積,Aunit為單位晶胞之面積,a1與a2分別為氧氣電漿處理前與後之奈米球13直徑,其中a1值可由SEM照片(見圖4(a))得知,分別為197、255、300nm;a2值則可由SEM圖(見圖4(b))得知,分別為175、224、247nm。圖8為奈米球13以六方緊密排列所形成之結構,經氧氣電漿處理前後其粒徑變化之示意圖。
In formula (4), f is the fill factor in the sub-wavelength structure, A is the area occupied by the array of
將a1、a2其代入公式(4)中,即可得到由197、255、300nm奈米球13所衍生製作之增亮膜的填充因子f分別為0.7157、0.6998、0.6148。隨後再將f值代入公式(3)即可得到neff分別為1.3301、1.3226、1.2819。若將上述數據與玻璃的折射率(n=1.50)代入公式(1),可獲得對應的反射率理論值約為0.36、0.39、0.61%。由表1可知,奈米球13陣列的球體粒徑越大者,所對應的填充因子會越小,反射率會越高。反射率的理論值與實驗值有所差異,可能的原因如下:一是奈米球13經氧氣電漿蝕刻會造成其表面粗糙化,導致其外形已不再是完美的圓球狀;二為反射率的理論值是由填充因子所推導出來,但填充因子僅計算圓球體的投影面積的變化,並未考慮到球體高度的改變。由於本發明所製作之抗反射結構僅覆蓋於玻璃基板10的一側,若可將此結構複製於玻璃基板10的兩側,必能增加其透光率[20]。本發明藉由草蟬翅膀表面次波長結構所製作出的仿生透明增亮層21,確實能有效減緩玻璃基板10與空氣二者間折射率的差異,提高LED的發光效率提高。本發明所提供的增亮層相關製程技術,未來在固態照明、顯示器與
太陽能電池產業的應用上,將具有相當大的發展潛力。本發明利用聚苯乙烯奈米球13及氧氣電漿蝕刻技術與自組裝裝置,快速製作具週期性的單層非緊密奈米球13陣列,並結合奈米壓印技術成功地製備出仿草蟬翅翼的透明增亮層21。藉由仿生結構之製作,除能有效地降低界面處的反射率至0.87%外,亦能提高LED的發光效率達55%,且不會使發光光譜發生位移。本發明所提供之增亮層製作技術,具有提高光學穿透度、避免反光及抗反射等功效,除可應用於照明產業之外,未來在顯示器(LED或OLED)的玻璃基板、太陽能電池的玻璃基板等光學元件,生物檢測儀器、瞄準鏡及望遠鏡等光學元件,智慧行動電話、平板電腦及穿載式手錶之顯示面板的貼膜或相關光學元件製作等產業上,亦極具應用價值與發展潛力。
Substituting a 1 and a 2 into formula (4), the fill factor f of the brightness enhancement film derived from 197, 255, and 300
以上所述,僅為本發明之可行實施例,並非用以限定本發明之專利範圍,凡舉依據下列請求項所述之內容、特徵以及其精神而為之其他變化的等效實施,皆應包含於本發明之專利範圍內。本發明所具體界定於請求項之結構特徵,未見於同類物品,且具實用性與進步性,已符合發明專利要件,爰依法具文提出申請,謹請 鈞局依法核予專利,以維護本申請人合法之權益。 The above is only a feasible embodiment of the present invention and is not intended to limit the patent scope of the present invention. Any equivalent implementation of other changes based on the content, features and spirit described in the following claims should be Included in the patent scope of the present invention. The structural features of the invention specifically defined in the claim are not found in similar items, and are practical and progressive. They have met the requirements of the invention patent. You have filed an application in accordance with the law, and I would like to ask the Jun Bureau to approve the patent in accordance with the law to maintain this. The applicant's legal rights and interests.
10‧‧‧基板 10‧‧‧ substrate
11‧‧‧奈米球陣列模板 11‧‧‧Nano ball array template
12‧‧‧LB槽 12‧‧‧LB slot
13‧‧‧奈米球 13‧‧‧Nano ball
14‧‧‧PDMS模仁 14‧‧‧ PDMS mold kernel
15‧‧‧紫外線光學固化膠 15‧‧‧UV optical curing adhesive
20‧‧‧應用件 20‧‧‧Application
21‧‧‧透明增亮層 21‧‧‧Transparent brightening layer
Claims (6)
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Citations (4)
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US20140166092A1 (en) * | 2012-12-14 | 2014-06-19 | Robert Bosch Gmbh | Method of Fabricating Nanocone Texture on Glass and Transparent Conductors |
TW201431660A (en) * | 2012-12-13 | 2014-08-16 | Oji Holdings Corp | Metal mold for forming optical element, method for forming metal mold, and optical element |
TW201725120A (en) * | 2015-10-21 | 2017-07-16 | Fujifilm Corp | Anti-reflective film and method for producing same |
TW201821442A (en) * | 2016-12-09 | 2018-06-16 | 國立虎尾科技大學 | Method for manufacturing anti-reflective hydrophobic transparent coating with subwavelength structure and applications thereof increasing light utilization efficiency by reducing energy loss |
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TW201431660A (en) * | 2012-12-13 | 2014-08-16 | Oji Holdings Corp | Metal mold for forming optical element, method for forming metal mold, and optical element |
US20140166092A1 (en) * | 2012-12-14 | 2014-06-19 | Robert Bosch Gmbh | Method of Fabricating Nanocone Texture on Glass and Transparent Conductors |
TW201725120A (en) * | 2015-10-21 | 2017-07-16 | Fujifilm Corp | Anti-reflective film and method for producing same |
TW201821442A (en) * | 2016-12-09 | 2018-06-16 | 國立虎尾科技大學 | Method for manufacturing anti-reflective hydrophobic transparent coating with subwavelength structure and applications thereof increasing light utilization efficiency by reducing energy loss |
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