TW202026233A - Patterned photoelectric substrate with improved luminous efficiency, light-emitting diode and manufacturing method thereof including forming first and second patterned structures, forming first and second metal layers, and forming a filling layer - Google Patents
Patterned photoelectric substrate with improved luminous efficiency, light-emitting diode and manufacturing method thereof including forming first and second patterned structures, forming first and second metal layers, and forming a filling layer Download PDFInfo
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- H01L33/00—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/20—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a particular shape, e.g. curved or truncated substrate
- H01L33/22—Roughened surfaces, e.g. at the interface between epitaxial layers
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- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
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Abstract
Description
本發明係關於一種具有提升發光效率之圖案化光電基板、發光二極體及其製作方法,尤指一種兼具有微米級第一圖案結構及次微米級第二圖案化結構之基板,及具有該基板之發光二極體,並於第二圖案化結構內設置填充層,並填平第二圖案化結構,以提升發光二極體之發光效率。The present invention relates to a patterned photoelectric substrate, a light emitting diode and a manufacturing method thereof with improved luminous efficiency, in particular to a substrate with both a micron-level first patterned structure and a sub-micron-level second patterned structure, and The light-emitting diode of the substrate is provided with a filling layer in the second patterned structure, and the second patterned structure is filled to improve the luminous efficiency of the light-emitting diode.
人類照明歷史發展至今已進入固態照明時代,發光亮度更亮、售價更低廉、壽命更長、穩定性更高..等特性需求為固態照明產業共同追求的目標。而照明市場首重發光二極體之亮度需求,一般而言,發光二極體的最大光輸出(Lmax )主要由外部量子效率(ηext )及最大操作電流(Imax )所決定,即Lmax =ηext ×Imax ,其中,外部量子效率(ηext )又為內部量子效率(ηint )及光萃取效率(ηextr )所決定,即ηext =ηint ×ηextr 。目前一般藍光發光二極體的內部量子效率已達70%以上,然而綠光發光二極體的內部量子效率卻驟降至40%以下,因此,藉由提升內部量子效率與光萃取效率以改善發光二極體的外部量子效率或增加發光二極體的發光亮度仍存在很大空間。The development of human lighting history has entered the era of solid-state lighting. The characteristics of brighter brightness, lower price, longer life, and higher stability are the goals that the solid-state lighting industry pursues. The lighting market first emphasizes the brightness requirements of light-emitting diodes. Generally speaking, the maximum light output (L max ) of the light-emitting diode is mainly determined by the external quantum efficiency (η ext ) and the maximum operating current (I max ), namely L max =η ext ×I max , where the external quantum efficiency (η ext ) is in turn determined by the internal quantum efficiency (η int ) and the light extraction efficiency (η extr ), that is, η ext =η int ×η extr . At present, the internal quantum efficiency of general blue light emitting diodes has reached more than 70%, but the internal quantum efficiency of green light emitting diodes has dropped to below 40%. Therefore, the internal quantum efficiency and light extraction efficiency are improved by improving There is still a lot of room for the external quantum efficiency of light-emitting diodes or to increase the brightness of light-emitting diodes.
由於氮化鎵與藍寶石基板間之晶格不匹配程度高達16%,當以藍寶石基板作為基材,進行氮化鎵薄膜磊晶時,氮化鎵薄膜內部會存在著應力,並出現許多不同種類差排缺陷,使氮化鎵薄膜差排密度達109 至1010 cm-2 ,嚴重影響磊晶薄膜品質,且缺陷通常扮演非輻射的復合中心,造成發光效率降低。因此,圖案化藍寶石基板製作技術的開發,其關鍵在於缺陷密度的降低,以實質提升氮化鎵薄膜磊晶品質及增加發光亮度。藉由氮化鎵薄膜在圖案基板側壁上成長以改變氮化鎵薄膜差排缺陷成長方向,差排缺陷將彎曲90°,使互相交錯形成堆疊錯位等消除缺陷,並且在磊晶時透過三維應力釋放減少缺陷形成,降低薄膜內部差排密度以提升晶體品質。目前研究亦指出使用圖案藍寶石基板成長之氮化鎵薄膜發現可以降低差排缺陷密度到108 至109 cm-2 ,並進一步提升發光二極體的內部量子效率及發光亮度。Since the lattice mismatch between gallium nitride and sapphire substrate is as high as 16%, when the sapphire substrate is used as the substrate for epitaxy of gallium nitride film, there will be stress inside the gallium nitride film, and many different types appear The differential row defects make the differential row density of the gallium nitride film reach 10 9 to 10 10 cm -2 , which seriously affects the quality of the epitaxial film, and the defects usually act as non-radiative recombination centers, resulting in reduced luminous efficiency. Therefore, the key to the development of patterned sapphire substrate manufacturing technology is to reduce the defect density, so as to substantially improve the epitaxial quality of the gallium nitride film and increase the luminous brightness. The GaN film grows on the sidewall of the patterned substrate to change the growth direction of the GaN film's differential defect. The differential defect will be bent by 90° to form a stack and dislocation to eliminate defects, and through three-dimensional stress during epitaxy The release reduces the formation of defects and reduces the density of the internal dislocation of the film to improve the crystal quality. Current research has also pointed out that GaN films grown on patterned sapphire substrates have been found to reduce the density of row defects to 10 8 to 10 9 cm -2 , and further improve the internal quantum efficiency and luminance of light-emitting diodes.
在最新的研究中,亦有使用次微米尺度圖案基板來成長發光二極體結構,對於同一面積之圖案基板,縮小圖案尺寸增加圖案數量將提升側向成長的有效區域面積,側向成長機制增強,造成更容易改變成長方向並形成堆疊錯位以消除差排缺陷,及大幅減低薄膜內部差排密度,同時由於圖案間距較短,易在氮化鎵磊晶時形成空洞阻擋缺陷延伸,提升氮化鎵薄膜磊晶品質。研究結果顯示,使用微米尺度圖案藍寶石基板成長之氮化鎵薄膜可以降低差排密度到108 cm-2 ,如將圖案基板改成次微米尺度時,由於單位體積應力釋放程度增加,則可將差排密度降低至107 cm-2 或更低。In the latest research, there are also sub-micron-scale patterned substrates to grow light-emitting diode structures. For patterned substrates of the same area, reducing the pattern size and increasing the number of patterns will increase the effective area of lateral growth, and the mechanism of lateral growth will be enhanced. , Which makes it easier to change the growth direction and form stacking dislocations to eliminate the row defects, and greatly reduce the row density inside the film. At the same time, due to the short pattern spacing, it is easy to form voids in the gallium nitride epitaxy to prevent the defect extension and improve the nitride Ga film epitaxial quality. The research results show that GaN films grown on a micron-scale patterned sapphire substrate can reduce the displacement density to 10 8 cm -2 . If the patterned substrate is changed to a sub-micron scale, the stress release per unit volume can be increased. The differential row density is reduced to 10 7 cm -2 or less.
已知技術中,如中華民國公告專利第I396297號,係揭示一種發光二極體,包括:基板,具有微米級孔洞於其中;作為緩衝層之奈米級多孔性光子晶體結構,形成於基板之上;第一型磊晶層,形成於上述緩衝層多孔性光子晶體結構之上;發光層,形成於上述第一型磊晶層之上;第二型磊晶層,形成於上述發光層之上;第一接觸電極,形成於上述該第一型磊晶層之上;以及,第二接觸電極,形成於上述第二型磊晶層之上。Known technologies, such as the Republic of China Patent Publication No. I396297, disclose a light-emitting diode, including: a substrate with micron-level holes in it; a nano-porous photonic crystal structure as a buffer layer formed on the substrate On; the first type epitaxial layer is formed on the porous photonic crystal structure of the buffer layer; the light emitting layer is formed on the first type epitaxial layer; the second type epitaxial layer is formed on the light emitting layer On; a first contact electrode is formed on the above-mentioned first type epitaxial layer; and, a second contact electrode is formed on the above-mentioned second type epitaxial layer.
另一中華民國公開專利第201251113號,係揭示一種LED基板之製造方法、LED基板及白光LED構造,主要目的係為使LED發出演色性佳之高亮度白光,該基板之反射面上係形成複數頂部呈曲面之凸起顆粒,該些凸起顆粒之底部寬度為2微米至4微米,高度為1.2微米至1.8微米,相鄰凸起顆粒之間距則為0.6微米至3微米,並使一氮化銦鎵磊晶層於通電後發出波長為380至410奈米範圍內之紫外光,紫外光經由該基板之反射面及該些凸起顆粒反射,並激發混合氧化鋅及釔鋁石榴石之螢光物質而產生紫外光之互補色光,而於相互混色後,由一封裝體散射出演色性佳之高亮度白光,而可用於照明等用途。Another Republic of China Patent No. 201251113 discloses a method for manufacturing an LED substrate, an LED substrate and a white LED structure. The main purpose is to make the LED emit high-brightness white light with good color rendering. The reflective surface of the substrate is formed with plural The top of the convex particles are curved. The bottom width of the convex particles is 2 to 4 microns, and the height is 1.2 to 1.8 microns. The distance between adjacent convex particles is 0.6 to 3 microns. The indium gallium epitaxial layer emits ultraviolet light with a wavelength in the range of 380 to 410 nanometers after being energized. The ultraviolet light is reflected by the reflective surface of the substrate and the convex particles, and excites the mixed zinc oxide and yttrium aluminum garnet. Fluorescent substances generate complementary colors of ultraviolet light, and after mixing with each other, high-brightness white light with good color rendering is scattered by a package, which can be used for lighting and other purposes.
然而,上述發明二極體中,主要都是藉由單獨在基板上形成一奈米級多孔性光子晶體結構或微米級凸起顆粒以提高發光二極體之發光效率,然而,前述微米級或奈米級結構設計對於降低差排密度程度或提升發光效率的程度都仍有其本質上的限制。However, in the above-mentioned invention diodes, the luminous efficiency of the light-emitting diode is mainly improved by separately forming a nanometer-scale porous photonic crystal structure or micron-scale protruding particles on the substrate. However, the aforementioned micron-scale or Nano-level structure design still has its own inherent limitations for reducing the degree of differential row density or improving the degree of luminous efficiency.
此外,如本案申請人申請的中華民國專利申請案第102111662號,係揭示一種光電元件的基板,提供至少一光電元件形成於該基板的一上表面,其特徵在於,該基板的該上表面具有複數個微米結構與複數個次微米結構以構成一粗糙表面,其中該些次微米結構的尺寸小於該些微米結構。藉此,可改善基板之光學漫射率,並可增進成長於基板上的磊晶薄膜材料品質,進而提升光電元件之光萃取效率,達到提升整體光電元件之發光亮度。本發明另提供一種光電元件。其中,該前案為本案申請人所提出藉由微米結構及次微米結構之組合以增進磊晶薄膜材料品質或提升整體光電元件之發光亮度。In addition, for example, the ROC Patent Application No. 102111662 filed by the applicant in this case discloses a substrate of an optoelectronic element, providing at least one optoelectronic element formed on an upper surface of the substrate, characterized in that the upper surface of the substrate has A plurality of micron structures and a plurality of sub-micron structures form a rough surface, wherein the size of the sub-micron structures is smaller than the micron structures. In this way, the optical diffusion rate of the substrate can be improved, and the quality of the epitaxial film material grown on the substrate can be improved, thereby increasing the light extraction efficiency of the optoelectronic device, and achieving the improvement of the light-emitting brightness of the entire optoelectronic device. The invention also provides a photoelectric element. Among them, the previous proposal was proposed by the applicant to improve the quality of epitaxial thin film materials or improve the luminous brightness of the overall optoelectronic device through the combination of microstructure and submicron structure.
再者,在磊晶層覆蓋到基板的過程中,若基板上的圖案包括凹槽結構,則凹槽的深寬比例與磊晶層的磊晶速率快慢具有相對應的關係。 進一步而言,若凹槽具有較高的深寬比,亦即凹槽深度較深,寬度較小,則凹槽結構容易因為磊晶層磊晶速率較快而無法被磊晶層即時地完全覆蓋填滿;然而,若為了將磊晶層即時地完全覆蓋填滿凹槽而降低磊晶速率,將因此降低生產效能。Furthermore, during the process of covering the epitaxial layer on the substrate, if the pattern on the substrate includes a groove structure, the depth-to-width ratio of the groove has a corresponding relationship with the epitaxial rate of the epitaxial layer. Furthermore, if the groove has a higher aspect ratio, that is, the groove depth is deeper and the width is smaller, the groove structure is likely to be unable to be instantly completed by the epitaxial layer due to the fast epitaxial layer. Covering and filling; However, if the epitaxial rate is reduced in order to completely cover and fill the groove with the epitaxial layer in real time, the production efficiency will be reduced.
承上所述,當磊晶層無法完全覆蓋填滿基板上的凹槽結構時,將使得凹槽結構與磊晶層之間存在大量存在空隙。進一步而言,由於光線進入到不同介質時,亦即由磊晶層進入到凹槽中的空隙,全反射因而增加,因此,凹槽結構中的空隙將使得LED由發光層發出光線的行進方向改變而困在凹槽結構中,形成較差的光提取效率,亦即降低發光二極體的發光效率。As mentioned above, when the epitaxial layer cannot completely cover and fill the groove structure on the substrate, there will be a large number of gaps between the groove structure and the epitaxial layer. Furthermore, when light enters different media, that is, when the light enters the gap in the groove from the epitaxial layer, the total reflection increases. Therefore, the gap in the groove structure will cause the LED to emit light from the light-emitting layer to travel direction Changed and trapped in the groove structure, resulting in poor light extraction efficiency, that is, reducing the luminous efficiency of the light-emitting diode.
因此,目前急需發展出一種具有提升發光效率之圖案化光電基板及具有該基板之發光二極體,其可以有效降提高發光二極體之發光效率,進而提高發光二極體之應用性及價值實有其需要。Therefore, there is an urgent need to develop a patterned photoelectric substrate with improved luminous efficiency and a light-emitting diode with the substrate, which can effectively reduce and increase the luminous efficiency of the light-emitting diode, thereby improving the applicability and value of the light-emitting diode There is a need.
本發明之主要目的係在提供一種具有提升發光效率之圖案化光電基板及其製作方法,其可藉由基板表面之圖案化結構以及填充層填滿於其凹槽結構內,進而使發光二極體具有更穩定且更優異的發光效率及性能。The main purpose of the present invention is to provide a patterned optoelectronic substrate with improved luminous efficiency and a manufacturing method thereof, which can be filled in the groove structure by the patterned structure on the surface of the substrate and the filling layer to make the light emitting diode The body has more stable and better luminous efficiency and performance.
為達成上述目的,本發明係提供一種具有提升發光效率之圖案化光電基板之製作方法,其步驟包括:In order to achieve the above objective, the present invention provides a method for manufacturing a patterned photoelectric substrate with improved luminous efficiency, the steps of which include:
步驟S1:提供一基板;Step S1: Provide a substrate;
步驟S2:藉由一第一蝕刻處理於該基板表面形成一第一圖案化結構及一間隔區域;Step S2: forming a first patterned structure and a spacer area on the surface of the substrate by a first etching process;
步驟S3:形成一第一金屬層及一第二金屬層於該基板上之該第一圖案化結構及該間隔區域表面;Step S3: forming a first metal layer and a second metal layer on the first patterned structure and the surface of the spacer area on the substrate;
步驟S4:藉由一第二蝕刻處理於該第二金屬層上形成一第二圖案化結構,該第二圖案化結構係位於該第一圖案化結構及該間隔區域上方之其中一者或兩者;Step S4: A second patterned structure is formed on the second metal layer by a second etching process, and the second patterned structure is located at one or both of the first patterned structure and the spacer area. By;
步驟S5:藉由一第三蝕刻處理使該第二圖案化結構向下延伸至該第一金屬層及該基板之部分表面;Step S5: extend the second patterned structure down to the first metal layer and part of the surface of the substrate by a third etching process;
步驟S6:藉由一酸液處理以自該基板上移除該第一金屬層及該第二金屬層,以形成具有該第一圖案化結構及該第二圖案化結構之該基板;Step S6: removing the first metal layer and the second metal layer from the substrate by an acid treatment to form the substrate having the first patterned structure and the second patterned structure;
以及步驟S7:以一預定成長速率形成一填充層填滿於該第二圖案化結構內。And step S7: forming a filling layer at a predetermined growth rate to fill the second patterned structure.
所述之具有提升發光效率之圖案化光電基板之製作方法,其中,該第二圖案化結構之該結構形狀係為一次微米級凹槽結構,且其深寬比介於0.3:1至20:1之間。In the method for fabricating a patterned optoelectronic substrate with improved luminous efficiency, the structure of the second patterned structure is a primary micron-level groove structure, and its aspect ratio is between 0.3:1 and 20: 1 between.
所述之具有提升發光效率之圖案化光電基板之製作方法,該填充層係以物理氣相沈積方式填滿於該第二圖案化結構之內。In the method for manufacturing a patterned optoelectronic substrate with improved luminous efficiency, the filling layer is filled in the second patterned structure by physical vapor deposition.
所述之具有提升發光效率之圖案化光電基板之製作方法,其中,該次微米級凹槽結構包括一多邊形結構。In the method for fabricating a patterned photoelectric substrate with improved luminous efficiency, the sub-micron groove structure includes a polygonal structure.
所述之具有提升發光效率之圖案化光電基板之製作方法,其中,該預定成長速率介於每秒0.01至3.0奈米之間。In the method for manufacturing a patterned optoelectronic substrate with improved luminous efficiency, the predetermined growth rate is between 0.01 and 3.0 nanometers per second.
所述之具有提升發光效率之圖案化光電基板之製作方法,其中,該填充層所使用的材料為折射係數介於1.7~2.5之間。In the method for fabricating a patterned photoelectric substrate with improved luminous efficiency, the material used for the filling layer has a refractive index between 1.7 and 2.5.
一種具有提升發光效率之圖案化光電基板,包括:一第一圖案化結構,係為一微米級突出結構或一微米級凹槽結構;一間隔區域;一第二圖案化結構,係為一次微米級凹槽結構,並形成於該第一圖案化結構及該間隔區域上之其中一者或兩者;以及一填充層,設置於該第二圖案化結構之次微米級凹槽結構內。A patterned photoelectric substrate with improved luminous efficiency, comprising: a first patterned structure, which is a micron-level protruding structure or a micron-level groove structure; a spacer area; and a second patterned structure, which is a micron level A level groove structure is formed on one or both of the first patterned structure and the spacer area; and a filling layer is disposed in the submicron level groove structure of the second patterned structure.
所述之具有提升發光效率之圖案化光電基板,其中,該第一圖案化結構或該第二圖案化結構係為圓錐狀、圓弧狀、圓柱狀、角錐狀或角柱狀。The patterned photoelectric substrate with improved luminous efficiency, wherein the first patterned structure or the second patterned structure is in the shape of a cone, arc, cylinder, pyramid or prism.
所述之具有提升發光效率之圖案化光電基板,其中,該次微米級凹槽結構之深寬比介於0.3:1至20:1之間。In the patterned photoelectric substrate with improved luminous efficiency, the aspect ratio of the sub-micron groove structure is between 0.3:1 and 20:1.
所述之具有提升發光效率之圖案化光電基板,其中,該填充層係選用折射係數1.7~2.5之間之材料。In the patterned photoelectric substrate with improved luminous efficiency, the filling layer is made of materials with a refractive index between 1.7 and 2.5.
一種具有提升發光效率之圖案化光電基板之發光二極體,包括:一基板,該基板係為前述中任一項所述之具有提升發光效率之圖案化光電基板;一緩衝層,設置於該基板上;以及一光電元件,設置於該緩衝層上,且該光電元件包含:一第一半導體層、一發光層、及第二半導體層,其中,該第一半導體層係接合至該緩衝層;該發光層,夾設於該第一半導體層及該第二半導體層之間。A light-emitting diode with a patterned photoelectric substrate with improved luminous efficiency, comprising: a substrate, the substrate being the patterned photoelectric substrate with improved luminous efficiency as described in any one of the foregoing; a buffer layer disposed on the On the substrate; and an optoelectronic element disposed on the buffer layer, and the optoelectronic element includes: a first semiconductor layer, a light emitting layer, and a second semiconductor layer, wherein the first semiconductor layer is bonded to the buffer layer ; The light-emitting layer is sandwiched between the first semiconductor layer and the second semiconductor layer.
所述之發光二極體,其中,更包括一第一電極及一第二電極,該第一電極及該第二電極係分別電性接合於該第一半導體層及該第二半導體層。The light-emitting diode further includes a first electrode and a second electrode. The first electrode and the second electrode are electrically connected to the first semiconductor layer and the second semiconductor layer, respectively.
以下係藉由特定的具體實施例說明本發明之實施方式,熟習此技藝之人士可由本說明書所揭示之內容輕易地了解本發明之其他優點與功效。本發明亦可藉由其他不同的具體實施例加以施行或應用,本說明書中的各項細節亦可針對不同觀點與應用,在不悖離本發明之精神下進行各種修飾與變更。The following is a specific embodiment to illustrate the implementation of the present invention. Those skilled in the art can easily understand the other advantages and effects of the present invention from the content disclosed in this specification. The present invention can also be implemented or applied by other different specific embodiments, and various details in this specification can also be modified and changed according to different viewpoints and applications without departing from the spirit of the present invention.
請參考圖1及圖2A至2J,為本發明所提出之一種具有提升發光效率之圖案化光電基板之製作方法,包括以下步驟:Please refer to FIG. 1 and FIGS. 2A to 2J, which are a method of fabricating a patterned photoelectric substrate with improved luminous efficiency proposed by the present invention, including the following steps:
步驟S1:提供一基板10;在一實施例中,基板10係選用一平面表面的一藍寶石基板,或選用一平面表面的矽基板亦可(參考圖2A)。Step S1: Provide a
步驟S2:藉由第一蝕刻處理於基板10表面形成第一圖案化結構11及間隔區域12(參考圖2B);在一實施例中,第一蝕刻處理處理可為一等向性蝕刻(Isotropic etching)或一非等向性蝕刻(Anisotropic etching),其中,可為電感式偶合電漿反應性離子蝕刻法(ICP-RIE)、化學液蝕刻法、乾式蝕刻法、電漿蝕刻法、或雷射加工法。此外,等向性蝕刻可利用化學蝕刻液(例如強酸)在高溫環境下進行化學蝕刻反應,以在基板10上製作出具有一定週期性之微米級突出或凹槽結構;此外,非等向性蝕刻程序為先在基板10上形成一圖案化光阻層,再利用電感式耦合電漿反應性離子蝕刻(ICP-RIE)技術進行蝕刻,以選擇性地移除部分基板10,同樣可達到上述形成具有一定週期性之微米級突出或凹槽結構之目的。Step S2: Form a first
此外,在步驟S2中,更包括提供一第一光阻層(未圖示)設置於基板10之部分表面上,使第一蝕刻處理可為選擇性地移除部分的基板10;此外,在前述本發明之一種具有提升發光效率之圖案化光電基板之製作方法中,該第一圖案化結構11可為一微米級突出結構(如圖2B所示)或一微米級凹槽結構,且間隔區域12可為一平面結構。於本發明之一態樣中,第一圖案化結構11可為一微米級突出結構,其高度為1.2微米至2微米,外徑為1微米至5微米,相鄰的該第一圖案化結構11之間距(即為該間隔區域12之長度或寬度)為0.1微米至1微米。此外,於本發明之另一態樣中,第一圖案化結構11可為一微米級凹槽結構,此部分將於後面詳細說明。In addition, in step S2, it further includes providing a first photoresist layer (not shown) on a part of the surface of the
步驟S3:形成第一金屬層13及一第二金屬層14於基板10上的第一圖案化結構11及間隔區域12表面(參考圖2C);其中,第一金屬層13或第二屬層14之形成可藉由塗佈法、化學電鍍法、濺鍍法、蒸鍍法、陰極電弧法、或化學氣相沉積法,其中,蒸鍍法包括電子束蒸鍍法、熱蒸鍍法、高週波蒸鍍法、或雷射蒸鍍法等,本發明並未侷限於此。在此,本發明所揭露之一種具有提升發光效率之圖案化光電基板之製作方法中,第一金屬層13為至少一選擇由鈦、鉻、鉬、或二氧化矽(SiO2
)組合等所組成之群組,且第一金屬層13之厚度可為1奈米至1微米;此外,第二金屬層14為鋁,且第二金屬層14之厚度可為10奈米至100微米。而於本發明之另一態樣中,第一金屬層13則選用鈦為主。Step S3: forming a
步驟S4:藉由第二蝕刻處理於第二金屬層14上形成第二圖案化結構15,此第二圖案化結構15係位於第一圖案化結構11及間隔區域12上方之其中一者或兩者(參考圖2D);在一實施例中,第二蝕刻處理是使用一陽極氧化鋁處理(anodic aluminum oxide,AAO),但並不以此為限。以使用陽極氧化鋁處理來說,其包含提供一第二光阻層設置於第一圖案化結構11上方之第二金屬層14的表面,使該陽極氧化鋁處理可為選擇性地移除部分的間隔區域12上方之該第二金屬層14,因此,第二圖案化結構15可形成於間隔區域12上方之第二金屬層14,但第一圖案化結構11上方之第二金屬層14則不會具有該第二圖案化結構15。另一實施例,在前述本發明之一種具有提升發光效率之圖案化光電基板之製作方法中,於步驟S4中,更包括提供第二光阻層設置於間隔區域12上方之第二金屬層14表面,使陽極氧化鋁處理可為選擇性地移除部分的第一圖案化結構11上方之第二金屬層14,因此,第二圖案化結構15可形成於第一圖案化結構11上方之第二金屬層14,但間隔區域12上方之第二金屬層14則不會具有該第二圖案化結構15。Step S4: A second patterned
步驟S5:藉由第三蝕刻處理使第二圖案化結構15向下延伸至第一金屬層13及基板10之部分表面(參考圖2E);在此所述的第三蝕刻處理的方式可以同前述之第一蝕刻處理,在此則不再贅述。Step S5: The second
步驟S6:藉由一酸液處理以自基板10上移除第一金屬層13及第二金屬層14,以形成具有第一圖案化結構11及第二圖案化結構15之基板10(參考圖2F),而在此所指的酸液,可以使用例如草酸(H2
C2
O4
)、硫酸(H2
SO4
)、磷酸(H3
PO4
)等等,或者是依需求以及搭配處理的時間,可以多種酸液調配而成,例如,以氫氟酸:硝酸:醋酸,以比例為2:3:10調配而成,並酸洗約2分鐘。Step S6: Remove the
步驟S7:以一預定成長速率形成一填充層16於第二圖案化結構15內,如圖2G與其局部放大圖2H所示。在此,填充層16可以用物理氣相沈積方式(Physical Vapor Deposition)以一預定成長速率所形成,例如濺鍍、蒸鍍的方式,將填充層16填滿於第二圖案化結構15之內,而預定成長速率則介於每秒0.01至3.0奈米之間為較佳方式。Step S7: forming a
其中,前述的第二圖案化結構15之結構形狀係為一次微米級凹槽結構,且其深寬比介於0.3:1至20:1之間。且此次微米級凹槽結構包括一多邊形結構,包括一梯形結構、一錐形結構、一弧形結構、一柱形結構或一角形結構。此外,要特別說明的是,填充層16所使用的材料不特別侷限,可選用折射係數介於1.7~2.5之間的材料為較佳的方式,例如藍寶石(折射係數1.7)、氮化鋁AlN、氮化矽SiN、二氧化矽SiO2
、氮化鈦TiN或氮化鎵(折射係數為2.5)皆可。Wherein, the structure shape of the aforementioned second
請參考圖2I,要特別說明的是,填充層16除了充滿於第二圖案化結構15之內,此填充層16也會存在於第一圖案化結構11與間隔區域12之上。此外,也請參考圖2J,此為第二圖案化結構15的另一個實施態樣,此第二圖案化結構15的結構形狀為角錐狀之次微米級凹槽結構,在此實施例中,填充層16係選用氮化鎵材料,以每秒0.01~3.0奈米之間的預定成長速率,將第二圖案化結構15中的角椎狀的凹槽空隙填滿,據此,應用本發明所提出的具有提升發光效率之圖案化光電基板之製作方法,進一步應用於製成發光二極體的產品,透過角椎狀的次微米級凹槽結構,可提高入光量,又透過填充層16填滿於此第二圖案化結構15之內,可以避免造成光線的全反射現象,大幅度的增加出光量,進一步提高發光效率。Please refer to FIG. 2I. It should be noted that, in addition to filling the second
於本發明之另一實施例中,填充層16包括氮化鋁,若基板10使用藍寶石的材質,由於氮化鋁與藍寶石材質的折射係數相近,光線在進入到不同介質的臨界角可達到大約42.5度,據此,可消除光線進入到不同介質產生的全反射現象。此外,於本發明之另一實施例中,填充層16係以濺鍍或原子層沈積方法形成於基板10的第二圖案化結構15內,但是並不以此為限。In another embodiment of the present invention, the filling
此外,在前述本發明之一種具有提升發光效率之圖案化光電基板之製作方法中,於步驟S7之後,更包括提供一緩衝層40及一光電元件形成於該基板20上,使該基板20可結合該緩衝層40及該光電元件以形成一發光二極體30或一太陽能電池,將於後續圖3A進一步說明。In addition, in the aforementioned method of manufacturing a patterned photoelectric substrate with improved luminous efficiency, after step S7, it further includes providing a
請參考圖2K,本發明再提出另一種實施例,為一種具有提升發光效率之圖案化光電基板20,包括: 一第一圖案化結構21,在此實施例中,第一圖案化結構21為一微米級凹槽結構;以及一間隔區域22;一第二圖案化結構25,係為一次微米級凹槽結構,形成於第一圖案化結構21及間隔區域22上之其中一者或兩者;以及一填充層26,設置於第二圖案化結構25之次微米級凹槽結構內。本實施例與前述實施例之一種具有提升發光效率之圖案化光電基板10的製作流程大致相同,除了在第一圖案化結構21之凹凸型態不同。本實施例係提供一第一光阻層(圖未顯示)設置於基板20部分表面上,使第一蝕刻處理為選擇性地移除部分的基板20,以形成具有圓錐狀之微米級凹槽結構之第一圖案化結構21及平面結構之間隔區域22;接著,並依據前述之製作流程,使第一圖案化結構21上含有複數個第二圖案化結構25,以形成具有第一圖案化結構21及第二圖案化結構25之具有提升發光效率之圖案化光電基板20,接著設置填充層26,並將第二圖案化結構25填滿填平。2K, the present invention provides another embodiment, which is a patterned
在一實施例中,第一圖案化結構21或第二圖案化結構26係為圓錐狀、圓弧狀、圓柱狀、角錐狀或角柱狀,或者,也可以是一多邊形結構,包括一梯形結構、一錐形結構、一弧形結構、一柱形結構或一角形結構等,皆不侷限。In an embodiment, the first
要特別說明的是,第二圖案化結構26的次微米級凹槽結構之深寬比介於0.3:1至20:1之間。而填充層26係選用折射係數1.7~2.5之間之材料,例如藍寶石(折射係數1.7)或氮化鎵(折射係數為2.5)皆可。It should be particularly noted that the aspect ratio of the sub-micron groove structure of the second
請參考圖3A,為本發明所提出之一種具有提升發光效率之圖案化光電基板之發光二極體30,而所述光電基板如前述之一種具有提升發光效率之圖案化光電基板20,具有一第一圖案化結構21、間隔區域22以及第二圖案化結構25,以及填充層26設置於第二圖案化結構25內或基板20上方,在此不再贅述。Please refer to FIG. 3A, which is a light-emitting
一緩衝層40,設置於基板20上,其中,在如圖2H的實施例中,緩衝層40設置在所述的第一圖案化結構21、間隔區域22之上,而填充層26則填充於第二圖案化結構25與緩衝層40之間。而在如圖2I的實施例中,填充層26係分別填充於第一圖案化結構21、間隔區域22、及第二圖案化結構25之上,則緩衝層40便與填充層26相結合。A
一光電元件,設置於此緩衝層40上,且光電元件包含:一第一半導體層51、一發光層52、及第二半導體層53,其中,第一半導體層51係接合至緩衝層40;發光層52則夾設於第一半導體層51及第二半導體層53之間。An optoelectronic element is disposed on the
其中,第一半導體層51及第二半導體層53為具有相對電性,例如,第一半導體層51及第二半導體層53分為P型半導體層及N型半導體層,或第一半導體層51及第二半導體層53分為N型半導體層及P型半導體層。此外,在前述本發明之一種發光二極體30中,更包括一第一電極54及一第二電極55,第一電極54及第二電極55為分別電性接合於第一半導體層51及第二半導體層53,且第一電極54及第一半導體層51或第二電極55及第二半導體層53具有相同的電性,例如,第一電極54及第一半導體層51均為正電性,第二電極55及第二半導體層53均為負電性,或者,第一電極54及第一半導體層51均為負電性,第二電極55及第二半導體層53均為正電性。此外,在前述本發明所揭露之發光二極體30中,光電元件可以為一直通式發光二極體、側通式發光二極體、或覆晶式發光二極體,本發明並未侷限於此。Among them, the
請參考圖3B,要特別說明的是,本發明所提出的發光二極體30,其所使用的基板20為具有一填充層26,至少設置於第二圖案化結構25內,因此,當緩衝層40設置於基板20上方時,緩衝層40與填充層26之間具有一接合部261,此接合部261可以如圖2H所示,填充層26填滿、填平於第二圖案化結構25內,然後緩衝層40將會分別與間隔區域、填充層以及第一圖案化結構結合,而接合部261則呈現平坦的結構;另一實施態樣,可以如圖2I或圖2J,填充層26除了填滿於第二圖案化結構內,也平均設置於間隔區域與第一圖案化結構之上,因此,結合部261亦呈現較平坦的結構;請參考圖3B,另一種實施態樣中,填充層26填充於第二圖案化結構25內並與緩衝層40接合時,結合部261具有一凹陷結構,特別適用於第二圖案化結構25的深寬比屬於較深的結構時,可以利用濺鍍的製程,先將第二圖案化結構25較深的空隙填充後(在此指填充層26),後續再配合MOCVD磊晶速率,控制水平與垂直的成長,使緩衝層40則接續於此填充層26之上,進而使整體結構中,避免有中空的結構產生。Please refer to FIG. 3B. It should be particularly noted that the
此外,在前述本發明之一種發光二極體中,緩衝層40可為一氮化鎵(GaN)、氮化鋁(AlN)、氮化鋁鎵(AlGaN)、或其類似物、或其組合,用以降低該基板20(如,藍寶石基板)及該光電元件(如,發光二極體之氮化鎵磊晶層)間之晶格不匹配所造成之應力,進而達到降低光電元件內缺陷數量之目的;此外,除了利用氮化鎵磊晶層作為該光電元件以形成一發光二極體30之外,於本發明之另一態樣中,更可以選用一太陽能基板作為該光電元件以形成一太陽能電池,此時,該緩衝層40也可以為一非晶矽碳化物,同樣也可用以降低該基板20(如,藍寶石基板)及該太陽能單晶層或太陽能多晶層間之晶格不匹配所造成之應力,進而達到降低光電元件內缺陷數量之目的,且本發明並未侷限於此。In addition, in the aforementioned light emitting diode of the present invention, the
據此,本發明所提出一種發光二極體30,由於其所使用的基板20是如前所述的一種具有提升發光效率之圖案化光電基板,其透過第二圖案化結構25係為一次微米級凹槽結構,可提高入光量,再者,又透過使用一預定的成長速率將填充層26填滿於此第二圖案化結構25之內,可以避免造成光線的全反射現象,大幅度的增加入光量,進一步提高發光效率,進而使整個發光二極體30具有更穩定且更優異的發光效率及性能。Accordingly, the present invention proposes a light-emitting
請參閱圖4及圖5,其係為各種範圍的光線波長在基板上不同深寬比的凹槽結構中的漫反射率(DR;diffuse reflectance)與漫穿透射(DT;diffuse transmittance)的實驗數據圖。圖6係為漫反射率、漫穿透率與深寬比的關係圖,而圖中標示的AR值即為深寬比。在圖4及圖5中可看出,當基板上沒有次微米級凹槽結構或微米級凹槽結構,而僅有藍寶石的基板(Bare)時,無論光線波長為何,偵測器偵測到的DR與DT的比率皆維持在0.2%。Please refer to Figure 4 and Figure 5, which are the diffuse reflectance (DR; diffuse reflectance) and diffuse transmittance (DT; diffuse transmittance) of the groove structure with different aspect ratios on the substrate for various wavelengths of light. Experimental data graph. Figure 6 is a graph showing the relationship between diffuse reflectance, diffuse transmittance and aspect ratio, and the AR value indicated in the figure is the aspect ratio. As can be seen in Figures 4 and 5, when there is no sub-micron groove structure or micro-scale groove structure on the substrate, but only the sapphire substrate (Bare), no matter the wavelength of the light, the detector detects The ratio of DR to DT is maintained at 0.2%.
然而,當基板上設置次微米級凹槽結構或微米級凹槽結構時,在相同的光線波長下,隨者深寬比越大,DR與DT則隨之增加,因而可有效提升LED光萃取效率。圖4亦可看出隨者深寬比越大,DR與DT亦隨之增加。However, when a sub-micron groove structure or a micron groove structure is provided on the substrate, under the same wavelength of light, as the aspect ratio increases, the DR and DT increase, which can effectively improve the LED light extraction effectiveness. Figure 4 can also see that as the aspect ratio increases, DR and DT also increase.
請參閱圖7及圖8,其係為不同深寬比凹槽結構基板上成長LED結構層的電子顯微鏡側視圖。承上所述,雖然在先前技術中已揭露在基板上設置次微米級凹槽結構或微米級凹槽結構的技術特徵,且由上述內容可知隨著凹槽結構的深寬比越大,DR與DT則隨之增加。然而,在實際的磊晶製程中,若使用MOCVD的技術在基板上生成磊晶層,將遭遇到無法完全填平具有高深寬比之凹槽結構的技術瓶頸。如圖8所示,雖然具有較低深寬比(較淺)的凹槽結構比較容易填平,然而,如圖7所示,具有較高深寬比(較深)的凹槽結構將不容易填平,因此,將使得LED磊晶結構在高深寬比的奈米圖案藍寶石基板(NPSS; nanoscale-patterned sapphire substrates)中留下空隙,使得LED發出光線無法順利從藍寶石基板中導出。換句話說,即使在基板上設置有高深寬比的次微米級凹槽結構或微米級凹槽結構,然而,在無法突破現有磊晶製程的情況下,仍無法有效提升LED光萃取效率。Please refer to FIGS. 7 and 8, which are electron microscope side views of growing LED structure layers on substrates with groove structures with different aspect ratios. Continuing from the above, although the prior art has disclosed the technical features of providing a sub-micron-level groove structure or a micro-level groove structure on the substrate, and from the above content, it can be seen that as the aspect ratio of the groove structure is greater, the DR And DT will increase accordingly. However, in the actual epitaxial process, if the MOCVD technology is used to generate an epitaxial layer on the substrate, it will encounter a technical bottleneck that cannot completely fill the groove structure with a high aspect ratio. As shown in Figure 8, although a groove structure with a lower aspect ratio (shallower) is easier to fill, however, as shown in Fig. 7, a groove structure with a higher aspect ratio (deeper) will not be easy Filling, therefore, will cause the LED epitaxial structure to leave gaps in nanoscale-patterned sapphire substrates (NPSS) with high aspect ratio, so that the light emitted by the LED cannot be smoothly derived from the sapphire substrate. In other words, even if a submicron-level groove structure or a micro-level groove structure with a high aspect ratio is provided on the substrate, the LED light extraction efficiency cannot be effectively improved when the existing epitaxial process cannot be broken.
請參閱圖9、圖10及圖11,其依序為基板上之凹槽結構具有空隙的LED結構、基板上無凹槽結構的LED結構以及基板上之凹槽結構完全填平的LED結構示意圖。圖9所示即是前述具有高深寬比的凹槽結構,雖然具有越高深寬比的基板在理論上來說可提高光萃取效率,但由於此凹槽為次微米級凹槽結構或微米級凹槽結構,因此經過後續的MOCVD製程之後,其凹槽結構就會如圖9所示,在圖9中可看出,由於基板上之凹槽結構具有空隙,因此,當光線由LED的介質入射至基板上的凹槽結構時,基板上的凹槽結構係為空氣介質,其折射率為1,而基板上的LED磊晶層以氮化鎵為例,其折射率為2.5,因此,若考慮到全反射的狀況,根據光學的snell's law,LED的光線將產生23.5度的臨界角,使得光線被反射回LED的磊晶層,無法逃逸到大氣中。Please refer to Figure 9, Figure 10 and Figure 11, which in turn are LED structures with gaps in the groove structure on the substrate, LED structures without groove structure on the substrate, and LED structures with the groove structure on the substrate completely filled. . Figure 9 shows the aforementioned groove structure with high aspect ratio. Although a substrate with a higher aspect ratio can theoretically improve the light extraction efficiency, the groove is a sub-micron groove structure or a micron-level groove. The groove structure, so after the subsequent MOCVD process, the groove structure will be as shown in Figure 9. As can be seen in Figure 9, because the groove structure on the substrate has gaps, when the light enters the LED medium To the groove structure on the substrate, the groove structure on the substrate is an air medium, and its refractive index is 1, while the LED epitaxial layer on the substrate uses gallium nitride as an example, and its refractive index is 2.5. Therefore, if Taking into account the condition of total reflection, according to the snell's law of optics, the light of the LED will produce a critical angle of 23.5 degrees, so that the light is reflected back to the epitaxial layer of the LED and cannot escape into the atmosphere.
如圖10所示,為基板上無凹槽結構的實施態樣,因此,以藍寶石基板(Sapphire)為例,其折射率為1.7,氮化鎵其折射率為2.5,因此,若考慮到全反射的狀況,LED的光線將產生42.5度的臨界角。如圖11所示,為另一種凹槽結構的實施態樣,但並不以此為限,本發明所要表達的重點在於,由於其基板上的凹槽結構已經完全填平,因此,在基板上仍可保有次微米級凹槽結構或微米級凹槽結構的情況下,LED的光線仍可產生42.5度的臨界角。據此,可有效提升LED光萃取效率。換句話說,雖然具有高深寬比的NPSS對於光萃取效率有提升效益,但其前提為LED的凹槽結構必須填滿、填平。據此,透過本發明所提出的一種具有提升發光效率之圖案化光電基板,其透過第二圖案化結構係為一次微米級凹槽結構,可提高入光量,再者,又透過使用一預定的成長速率將填充層填滿於此第二圖案化結構之內,可以避免造成光線的全反射現象,大幅度的增加入光量,進一步提高發光效率,進而使整個發光二極體具有更穩定且更優異的發光效率及性能。As shown in Figure 10, it is the implementation of the structure without grooves on the substrate. Therefore, taking a sapphire substrate (Sapphire) as an example, its refractive index is 1.7, and the refractive index of gallium nitride is 2.5. Therefore, if you consider the total In the reflected state, the light of the LED will produce a critical angle of 42.5 degrees. As shown in FIG. 11, it is another embodiment of the groove structure, but it is not limited to this. The key point of the present invention is that since the groove structure on the substrate has been completely filled, the substrate Under the condition that the sub-micron-level groove structure or the micro-level groove structure can still be maintained on the upper surface, the light of the LED can still generate a critical angle of 42.5 degrees. Accordingly, the LED light extraction efficiency can be effectively improved. In other words, although NPSS with a high aspect ratio is beneficial to light extraction efficiency, the premise is that the groove structure of the LED must be filled and leveled. Accordingly, through the patterned optoelectronic substrate with improved luminous efficiency proposed by the present invention, the second patterned structure is a micron-level groove structure, which can increase the amount of light incident. Furthermore, by using a predetermined The growth rate fills the filling layer in the second patterned structure, which can avoid the phenomenon of total reflection of light, greatly increase the amount of light incident, and further improve the luminous efficiency, thereby making the entire light-emitting diode more stable and more efficient. Excellent luminous efficiency and performance.
圖12為圖9至圖11各種基板上之凹槽結構填充態樣的LED發光效率比較圖,其中,Y軸指的是光強度,單位為mcd(毫坎德拉),標示為HAR-LED係指圖9的態樣,基板上之凹槽結構具有空隙的LED結構,標示B-LED係指圖10態樣中,基板上無凹槽結構的LED結構,以及標示為LAR-LED為圖11之態樣,基板上之凹槽結構完全填平的LED結構,可以得知,以LAR-LED的光強度最高。此外,圖9至圖11的實施態樣,係來自使用一具有平面的藍寶石基板上挖出奈米的孔洞加上微米結構的圖案後(奈米圖案藍寶石基板NPSS),所進行的實驗,當然,也是適用於複合型的基板。Figure 12 is a comparison diagram of the LED luminous efficiency of the filling state of the groove structure on the various substrates of Figures 9 to 11, where the Y axis refers to the light intensity, the unit is mcd (millicandela), and the label is HAR-LED means In the aspect of FIG. 9, the groove structure on the substrate has an LED structure with gaps, the label B-LED refers to the LED structure without groove structure on the substrate in the aspect of FIG. 10, and the LED structure labeled LAR-LED is the one in FIG. As for the LED structure in which the groove structure on the substrate is completely filled, it can be known that the LAR-LED has the highest light intensity. In addition, the implementation aspects of Figures 9 to 11 are derived from experiments carried out by using a flat sapphire substrate to excavate nano-holes and adding a micro-structure pattern (nano-patterned sapphire substrate NPSS). Of course It is also suitable for composite substrates.
上述實施例僅係為了方便說明而舉例而已,本發明所主張之權利範圍自應以申請專利範圍所述為準,而非僅限於上述實施例。The above-mentioned embodiments are merely examples for the convenience of description, and the scope of rights claimed in the present invention should be subject to the scope of the patent application, rather than being limited to the above-mentioned embodiments.
S1、S2、S3、S4、S5、S6、S7:步驟
10、20:基板
30:發光二極體
11、21:第一圖案化結構
12、22:間隔區域
13:第一金屬層
14:第二金屬層
15、25:第二圖案化結構
16、26:填充層
40:緩衝層
51:第一半導體層
52:發光層
53:第二半導體層
54:第一電極
55:第二電極
261:接合部
S1, S2, S3, S4, S5, S6, S7: steps
10, 20: substrate
30: LED
11.21: The first
圖1為本發明之一種具有提升發光效率之圖案化光電基板之製作方法的步驟流程圖。 圖2A至2J係本發明之具有提升發光效率之圖案化光電基板的一實施例示意圖。 圖2I為填充層之另一實施態樣。 圖2J為第二圖案化結構之另一實施態樣。 圖2K係本發明所提出之一種具有提升發光效率之圖案化光電基板之另一實施態樣。 圖3A與圖3B係本發明所提出之一種具有提升發光效率之圖案化光電基板之發光二極體。 圖4及圖5係為各種範圍的光線波長在基板上不同深寬比的凹槽結構中的漫反射率與漫穿透率的實驗數據圖。 圖6係為入射光450mm時,具凹槽結構基板之漫反射率、漫穿透率與深寬比的關係圖。 圖7及圖8係為不同深寬比之具凹槽結構基板,成長LED結構層後的電子顯微鏡圖。 圖9係為基板上之凹槽結構具有空隙的LED結構示意圖與光軌跡行進圖。 圖10係為基板上無凹槽結構的LED結構示意圖與光軌跡行進圖。 圖11係為基板上之凹槽結構完全填平的LED結構示意圖與光軌跡行進圖。 圖12為圖9至圖11各種基板上之凹槽結構填充態樣的LED發光效率比較圖。FIG. 1 is a flow chart of the manufacturing method of a patterned optoelectronic substrate with improved luminous efficiency according to the present invention. 2A to 2J are schematic diagrams of an embodiment of the patterned photoelectric substrate with improved luminous efficiency of the present invention. FIG. 2I shows another embodiment of the filling layer. FIG. 2J is another implementation aspect of the second patterned structure. 2K is another embodiment of a patterned photoelectric substrate with improved luminous efficiency proposed by the present invention. 3A and 3B are a light-emitting diode with a patterned photoelectric substrate with improved luminous efficiency proposed by the present invention. 4 and 5 are experimental data diagrams of the diffuse reflectance and diffuse transmittance of the groove structure with different aspect ratios on the substrate for various wavelengths of light. Figure 6 is a graph showing the relationship between diffuse reflectance, diffuse transmittance and aspect ratio of a substrate with groove structure when incident light is 450mm. Figures 7 and 8 are electron microscope images of substrates with grooved structures with different aspect ratios after growing LED structure layers. FIG. 9 is a schematic diagram of an LED structure with a gap in the groove structure on the substrate and a diagram of the light trace. FIG. 10 is a schematic diagram of the structure of an LED without a groove structure on the substrate and a diagram of the light trace. FIG. 11 is a schematic diagram of the LED structure and the light track travel diagram with the groove structure on the substrate completely filled. FIG. 12 is a comparison diagram of the luminous efficiency of LEDs in the filling state of the groove structure on the various substrates of FIG. 9 to FIG. 11.
S1、S2、S3、S4、S5、S6、S7:步驟 S1, S2, S3, S4, S5, S6, S7: steps
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