TWI353675B - Manufacturing method of two-dimensional photonic c - Google Patents

Manufacturing method of two-dimensional photonic c Download PDF

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TWI353675B
TWI353675B TW96115704A TW96115704A TWI353675B TW I353675 B TWI353675 B TW I353675B TW 96115704 A TW96115704 A TW 96115704A TW 96115704 A TW96115704 A TW 96115704A TW I353675 B TWI353675 B TW I353675B
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light
material layer
photosensitive material
emitting diode
layer
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TW96115704A
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TW200845408A (en
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Mei Li Hsieh
Chung Hsiang Lin
Shieh Yueh Yang
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Mei Li Hsieh
Chung Hsiang Lin
Shieh Yueh Yang
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1353675 23541twf.doc/〇〇6 九、發明說明: 【發明所屬之技術領域】 制本發明是有關於一種發光二極體内二維光子晶體的 製作方法,且特別是有關於一種可經由一次性(one-shot)的 曝光動作來形成大面積二維光子晶體的方法。 【先前技術】 ^由於發光二極體的發光現象不屬於熱發光或放電發 光,而是屬於冷性發光,所以發光二極體裝置的壽命可長 達十萬小時以上,且無須暖燈時間(idlingtime)。此外, 發光一極體裝置具有反應速度快(約為1〇·9秒)、體積小、 用電省、污染低(不含水銀)、高可靠度、適合量產等優 點,因此其應用的領域十分廣泛。 一般而言,發光二極體主要包含一基底、一發光疊層 以及多個電極,其中發光疊層係由P型摻雜層、主動層以 及N型摻雜層依序堆疊而成^當N型播雜層與p型摻雜層 之間形成-電位鱗’電子與制便會在主動層結合,而 產生光線。 上述之發光二極體的發光效率主要取決於主動層的 量子效率,以及發光二極體的光取出效率(extraction efficiency)。其中,主動層之量子效率的提升主要取決於主 動層之結晶品質及其結構的良窳,而光取出效率的提 取決於主動層發出之光線的有效利用率。 在習知技術中提出了許多利用元件表面圖案來提高 發光一極體之出光效率的方法,例如光子晶體(photonic 1353675 2354Itwf‘doc/006 便是f見的—種方式,其主要是在發光二極體内形 成光子晶體結構,藉以改變主動層所發出之光線的折射方 式,以減少光線的全反射,相對提高出射至發光二極體外 的光強度比率’因此能有效提升發光二極體的光取出效率。 近年來,更有相關研究實現了在發光二極體上的二維 光子晶體(two-dimensional photonic crystal,2DPC)的應 用。經過驗證,此種二維光子晶體可在發光二極體的光取 出效率上提供更好的改善效果。 S知技術多是藉由電子束微影(e_beam lithography)技 術,在發光二極體的發光疊層表面上形成上述之二維光子 晶體。此種方法因為需要使用電子束在發光疊層表面上逐 一製作微結構,因此製程時間冗長,微結構的面積尺寸也 會受到限制’不符合實際量產的需求。1353675 23541twf.doc/〇〇6 IX. Description of the Invention: [Technical Field] The present invention relates to a method for fabricating a two-dimensional photonic crystal in a light-emitting diode, and particularly relates to a disposable A one-shot exposure operation to form a large-area two-dimensional photonic crystal. [Prior Art] ^ Since the luminescence phenomenon of the illuminating diode is not a thermal luminescence or a discharge luminescence, but a cold luminescence, the lifetime of the illuminating diode device can be as long as 100,000 hours or more, and no warming time is required ( Idlingtime). In addition, the light-emitting one-pole device has the advantages of fast reaction speed (about 1 〇·9 seconds), small volume, low power consumption, low pollution (no mercury), high reliability, and suitable mass production, so its application The field is very extensive. In general, the light emitting diode mainly comprises a substrate, a light emitting layer and a plurality of electrodes, wherein the light emitting layer is sequentially stacked by the P type doping layer, the active layer and the N type doping layer. Forming a -potential scale between the type of miscellaneous layer and the p-type doped layer, electrons and fabrics combine in the active layer to generate light. The luminous efficiency of the above-described light-emitting diode mainly depends on the quantum efficiency of the active layer and the extraction efficiency of the light-emitting diode. Among them, the improvement of the quantum efficiency of the active layer mainly depends on the crystal quality of the active layer and its structure, and the efficiency of light extraction depends on the effective utilization of the light emitted by the active layer. In the prior art, many methods for utilizing the surface pattern of the element to improve the light extraction efficiency of the light-emitting body are proposed, such as photonic crystal (photonic 1353675 2354Itwf'doc/006 is a way of seeing, mainly in the light-emitting two A photonic crystal structure is formed in the polar body to change the refractive mode of the light emitted by the active layer to reduce the total reflection of the light and relatively increase the ratio of the light intensity emitted to the outer surface of the light-emitting diode. Therefore, the light of the light-emitting diode can be effectively improved. Extraction efficiency. In recent years, more relevant research has realized the application of two-dimensional photonic crystal (2DPC) on light-emitting diodes. It has been verified that such two-dimensional photonic crystals can be used in light-emitting diodes. The light extraction efficiency provides a better improvement effect. The S-known technology mostly forms the above-mentioned two-dimensional photonic crystal on the surface of the light-emitting layer of the light-emitting diode by electron beam lithography (e_beam lithography) technology. The method requires an electron beam to form a microstructure on the surface of the light-emitting laminate one by one, so the process time is long and the area size of the microstructure is also Will be restricted 'not meeting the needs of actual mass production.

Kim 等人在期刊 Appl. Phys. Lett. 87, 203508 (2005)另 提出一種藉由兩階段的全像曝光(two_step h〇1〇graphic 6父卩〇511代)技術來形成具有方形陣列(1^(^1^111&1_抓吵)孔洞 之二維光子晶體的方法,其雖然可以解決上述電子束製程 的部分問題’但由於在製程中必須旋轉發光二極體,因此 所/成之一維光子晶體結構的幾何穩定性(geometry stability)不佳。 另一方面,就生產製造而言,能否在發光二極體内製 作出大面積的二維光子晶體’亦是一項重要的議題。目前 的報告資料中’二維光子晶體的面積大多是長寬各約為數 百個微米(μπι)的大小。此面積大小實不敷大量生產應用。 23541twf.doc/〇〇6 【發明内容】 本發明關於一種發光 ^ ......... ...... 徑媸内大面積二維光子晶體 的製作方法,可提高㈣二極體的光取出效^ ^Kim et al., in the journal Appl. Phys. Lett. 87, 203508 (2005), proposes a two-stage holographic exposure (two_step h〇1〇graphic 6 father 511 generation) technique to form a square array (1). ^(^1^111&1_grabbing) the method of two-dimensional photonic crystal of a hole, although it can solve some of the problems of the above-mentioned electron beam process', but since it is necessary to rotate the light-emitting diode in the process, it is The geometric stability of the one-dimensional photonic crystal structure is not good. On the other hand, in terms of manufacturing, it is also important to make a large-area two-dimensional photonic crystal in the light-emitting diode. Topic. In the current report, the area of two-dimensional photonic crystals is mostly about several hundred micrometers (μπι) in length and width. This area is not large enough for mass production applications. 23541twf.doc/〇〇6 [Invention The present invention relates to a method for fabricating a large-area two-dimensional photonic crystal in a borehole, which can improve the light extraction effect of the (four) diode.

程簡單,並可形成具有高幾何穩定性的二維光子晶體。I 本發明另關於一種可用於大面積之二維光 程的光學系統’其可直接提供大面積的二維干涉圖案,— 以形成具有對應之晶格排列的大面積二維光子晶體。9 為具體描述本發明之内容,在此提出一 内二維光子晶體的製作方法。首先,提供—發趙The process is simple and can form a two-dimensional photonic crystal with high geometric stability. The invention further relates to an optical system that can be used for large-area two-dimensional optical paths, which can directly provide a large-area two-dimensional interference pattern, to form a large-area two-dimensional photonic crystal having a corresponding lattice arrangement. 9 To specifically describe the contents of the present invention, a method of fabricating an inner two-dimensional photonic crystal is proposed herein. First of all, provide - send Zhao

並且形成-感光材料層於發光二極體上。接著,提供至少 三道光線域光材料層上,並使上述錢在感光材料層^ 形成-大面積之二維干涉_,以藉由此二維干涉圖^ 感光材料層進行曝光。織,移除被曝光或未被曝光部^ 的感光材料層’以在感光材料層上形成—罩幕圖案。” 轉移感光材料層上的罩幕圖案至發光二極體上/以在’ 二極體上形成大面積之二維光子晶體的一微結構。X 在本發明之-實闕巾,上述轉移罩幕圖案至發光二 極體上的方法例如是直接喊光材制作為罩幕來圖案 發光二極體,之後再移除感光材料層。 在本發明之-實施财,更可以在形減光材料層之 前’先形成-中間層於發光二極體上。此外,轉移軍幕圖 案至毛光—極體上的方法例如是先藉由感光材料層作為罩 幕來圖案化_間層。接著,移除感光材料層,再以圖案化 後之中間層作為罩幕來圖案化發光二極體。之後,移除中 Ι353ύ75 23541twf.doc/006 間層 在本發明之-實施例中,上述微結構 多個孔洞或微柱。此外’所形成之二維干、、:ί列配置的 列的光強度週期變化,可包括方形或三:j案疋陣列排 (coherent)^^ 〇 ^ ^And forming a layer of photosensitive material on the light emitting diode. Next, at least three light-domain optical material layers are provided, and the above-mentioned money is formed in the photosensitive material layer - a large-area two-dimensional interference _ to expose by the two-dimensional interference pattern. The photosensitive material layer ' of the exposed or unexposed portion is removed to form a mask pattern on the photosensitive material layer. Transferring the mask pattern on the photosensitive material layer to the light-emitting diode / forming a microstructure of a large-area two-dimensional photonic crystal on the 'diode. X. In the present invention - the actual wipe, the transfer cover The method of the curtain pattern to the light-emitting diode is, for example, directly shouting the light material to form a mask to pattern the light-emitting diode, and then removing the photosensitive material layer. In the present invention, the light-reducing material can be further used. Before the layer is formed, the intermediate layer is formed on the light-emitting diode. In addition, the method of transferring the military curtain pattern to the hair-light body is, for example, first patterning the interlayer by using the photosensitive material layer as a mask. Then, The photosensitive material layer is removed, and the patterned intermediate layer is used as a mask to pattern the light-emitting diodes. Thereafter, the intermediate layer 353ύ75 23541 twf.doc/006 is removed. In the embodiment of the present invention, the above microstructure Multiple holes or microcolumns. In addition, the resulting two-dimensional dry, : ί column configuration of the light intensity cycle changes, may include square or three: j case 疋 array row (coherent) ^ ^ 〇 ^ ^

圖案的光強度分佈例如可表示為: v = ⑽喊作,,u = 123 其中/(W)代表該二維光干涉圖案在x y ^向上的 光強度’五代表光線的電場強度代表光線方向,峨表 光線的初始相位、代表兩相鄰人射級之偏振方向的^ 角。 在本發明之一實施例中,二維干涉圖案的三角形陣列 週期可為心A/tVIsir^/2)],又代表光線的波長,而0代表兩相 鄰入射光線的夾角。The light intensity distribution of the pattern can be expressed, for example, as: v = (10) shouting, u = 123 where /(W) represents the light intensity of the two-dimensional optical interference pattern in the xy ^ direction 'five represents the electric field strength of the light representing the direction of the light, The initial phase of the ray, the angle representing the polarization direction of the two adjacent human emitters. In one embodiment of the invention, the triangular array period of the two-dimensional interference pattern may be the heart A/tVIsir^/2)], which also represents the wavelength of the light, and 0 represents the angle between the two adjacent incident rays.

在本發明之一實施例中,例如是藉由一光學系統提供 光線於感光材料層上。此光學系統包括一光源、一擴束模 組、一分光模組、及光學鏡組。其中光源可提供一主光線 至擴束模組,以獲得寬束的光線。擴束後之光線繼而進入 分光模組,將光線分成三道或三道以上之寬束光線。利用 光學鏡組’將分光後的多道寬束光線引導至感光材料層 上’以形成大面積二維干涉圖案。 本發明藉由多道光線直接形成二維干涉圖案,用以製 1353675 23541twf.doc/006 作,維光子晶體的微結構,不僅製程較為簡單迅速,且因 為疋經由-次性的曝光動作來轉移二維干涉圖案,使得 形成的二維光子晶體結構具有較佳的幾何穩定性。 ▲為讓本發明之上述和其他目的、特徵和優點能更 易懂’下文特舉實施例,並配合所_式,作詳細說明如 下0 【實施方式】 Θ 1、·.θ示本發明之一實施例的一種發光二極體内二 光子晶體的製作流程。首先,如步驟UG所示,提供=發 光二極體,並且形成一感光材料層於發光二極體上。此^ 的感光材料層可為—般常見的正型光阻材料或負型光阻 料。 接著,如步驟120所示,提供多道光線於感光材料層 上,並使上述光線在感光材料層上形成一大面積之二維干 涉圖案,以藉由此二維干涉圖案對感光材料層進行曝光。 上述之光線的數量通常為三道以上,其例如是具有高同調 性的光線,以形成有效的干涉效果。圖2即繪示本發明所 形成的一種三角形陣列的二維干涉圖案,其中亮點21〇代 表光線之間產生建設性干涉的位置,且亮點21〇是呈三角 形的陣列排列。將此二維干涉圖案投射至感光材料層上, 便可對感光材料層進行曝光,而在感光材料層上形成對應 的曝光圖案。 " 在實際應用上,例如可應用雷射光源’並經由光學元 件的作用來形成上述之大面積的二維干涉圖案。圖3即繪 丄力3675 23541twfd〇c/〇〇6 示本發明之一實施例的一種可產生大面積的二維干涉圖案 的光源系統。如圖3所示,光源系統3〇〇包括光源31〇、 擴束模組320、分光模組330、光學鏡組340。其甲分光模 組可由第一分光元件33〇a及第二分光元件33〇b所組成, ,,鏡組340則可由多個反射鏡34〇a構成。光源31〇例如 是雷射光源,其可輸出一雷射光至擴束模組32〇。雷射光 :過,束模組320之後,其光束面積會被擴大成為擴束的 雷射光L。擴束之雷射光L繼之入射第一分光元件33加, 而第一分光元件330a可將擴束之雷射光L分光成為第— 光線L1與第二光線L2。第二分光元件33〇b可接收第二光 線L2,並且再將第二光線L2分光成為第三光線與第 四光線。光學鏡組340之反射鏡340a,其可將第一光 線L1、第三光線L3以及第四光線反射至發光二極體 350 的同—位置,以形成二維干涉圖案。在本實施例中, 由於第—光線U、第三光線L3以及第四綠L4皆為寬 束之光線,因此可形成大面積之二維干涉圖案。 、值得’主思的是,上述所提的光學系統或二維干涉圖案 僅^舉例之用,並非是適用於本發明的唯一二維干涉圖案 或是可產生二維干涉_的光學系統。本領域的技術人員 在參照上述實施例的說明之後,當可依據實際情形調整光 學系統的架構’例如光學元件的種類、數量與位置,而所 形成的二維干涉圖案也可依需求而有所不同。 請再同時參考圖2與3,上述所形成之二維干涉圖案 的光強度分佈例如可表示為: 1353675 23541twf.doc/006 ί:二:二種製作方法由於僅需對發光二極體進行-次 大面積二維光子晶體結構也具形成的In one embodiment of the invention, light is provided on the layer of photosensitive material, for example, by an optical system. The optical system includes a light source, a beam expanding module, a beam splitting module, and an optical lens assembly. The light source can provide a main ray to the beam expander module to obtain a wide beam of light. The expanded light then enters the beam splitting module, splitting the light into three or more broad beams of light. The optical multi-beam light beam is guided onto the photosensitive material layer by the optical lens group ' to form a large-area two-dimensional interference pattern. The invention directly forms a two-dimensional interference pattern by using multiple rays, and is used to make 1353675 23541 twf.doc/006, and the microstructure of the photonic crystal is not only simple and rapid, but also because the 疋 is transferred by the exposure action. The two-dimensional interference pattern makes the formed two-dimensional photonic crystal structure have better geometric stability. The above and other objects, features and advantages of the present invention will become more apparent. The following detailed description of the embodiments of the present invention will be described in detail as follows: [Embodiment] Θ 1, θ. A production process of a two-photon crystal in a light-emitting diode in an embodiment. First, as shown in step UG, a = light-emitting diode is provided, and a layer of photosensitive material is formed on the light-emitting diode. The photosensitive material layer of this ^ can be a generally common positive photoresist material or a negative photoresist material. Next, as shown in step 120, a plurality of rays are provided on the photosensitive material layer, and the light is formed on the photosensitive material layer to form a large-area two-dimensional interference pattern, thereby performing the photosensitive material layer by the two-dimensional interference pattern. exposure. The number of rays described above is usually three or more, which is, for example, light having a high homology to form an effective interference effect. 2 is a two-dimensional interference pattern of a triangular array formed by the present invention, wherein the bright spots 21 〇 represent the positions where constructive interference occurs between the light rays, and the bright spots 21 〇 are arranged in a triangular array. By projecting the two-dimensional interference pattern onto the photosensitive material layer, the photosensitive material layer can be exposed while a corresponding exposure pattern is formed on the photosensitive material layer. " In practical applications, for example, a laser light source can be applied and a large-area two-dimensional interference pattern described above can be formed via the action of optical elements. Fig. 3 is a diagram showing a light source system which can produce a large-area two-dimensional interference pattern according to an embodiment of the present invention. As shown in FIG. 3, the light source system 3 includes a light source 31A, a beam expander module 320, a beam splitting module 330, and an optical mirror group 340. The armor optical module can be composed of a first beam splitting element 33a and a second beam splitting element 33a, and the mirror group 340 can be composed of a plurality of mirrors 34A. The light source 31 is, for example, a laser light source that outputs a laser beam to the beam expander module 32A. Laser light: After the beam module 320, its beam area is enlarged to become the expanded laser light L. The expanded laser light L is incident on the first beam splitting element 33, and the first beam splitting element 330a splits the expanded laser light L into a first light ray L1 and a second light ray L2. The second beam splitting element 33〇b receives the second light line L2 and further splits the second light beam L2 into a third light and a fourth light. The mirror 340a of the optical lens group 340 reflects the first light L1, the third light L3, and the fourth light to the same position of the light emitting diode 350 to form a two-dimensional interference pattern. In the present embodiment, since the first light ray U, the third light ray L3, and the fourth green light L4 are all broad ray rays, a large-area two-dimensional interference pattern can be formed. It is worthwhile to think that the above-mentioned optical system or two-dimensional interference pattern is merely used as an example, and is not the only two-dimensional interference pattern applicable to the present invention or an optical system that can generate two-dimensional interference. After referring to the description of the above embodiments, those skilled in the art can adjust the structure of the optical system, such as the type, quantity and position of the optical components, according to actual conditions, and the formed two-dimensional interference pattern can also be required according to requirements. different. Referring to FIGS. 2 and 3 at the same time, the light intensity distribution of the two-dimensional interference pattern formed above can be expressed, for example, as follows: 1353675 23541twf.doc/006 ί: 2: The two manufacturing methods are only required for the light-emitting diode - Sub-large area two-dimensional photonic crystal structure is also formed

Si,二極體的光取出效率。另-方面I發明I: 束學系統來得到寬束的光線,並可藉:寬 2面:的二維光子晶體結構。如此,將可大幅縮短大面 積之-維光子晶體的製作時程,而有利於量產。 了文將再舉例&明應用本發明之内容。請參考圖6, 本發日月之—實施朗—種具有二維光子晶體的發光 :極體。發光二極體600可以是目前常見的藍、綠、白光 ^光二極料,町係舉—個實例來說明,但並非用以限 ^其應用範圍。發光二極體_主要包括基板_、發光 且層620透明導電層630、電極642、電極644以及絕緣 層650等。基板610例如是一磊晶基板,而發光疊層62〇 ,置於基板610上,而二維光子晶體66〇便是形成於發光 豐層620表面。更詳細而言,上述之發光疊層62〇由下而 上例如依序由一苐一半導體摻雜層622、一主動層624以 及一第—半導體摻雜層626所構成,而二維光子晶體660 疋位於最上層之第二半導體摻雜層626的表面。透明導電 層630位於第二半導體摻雜層626表面,而電極642與644 分別位於第一半導體摻雜層622與透明導電層630上。此 外’絕緣層650位於透明導電層630下方,以將電極642 與第二半導體摻雜層626分隔開。 14 C S ) 1353675 2354Itwf.doc/006Si, the light extraction efficiency of the diode. Another aspect I invention I: The beam system to obtain a wide beam of light, and can borrow: a two-dimensional: two-dimensional photonic crystal structure. In this way, the production time of the large-area-dimensional photonic crystal can be greatly shortened, which is advantageous for mass production. The text will be further exemplified by the application of the present invention. Please refer to FIG. 6, the luminosity of the present invention - the implementation of luminescence with a two-dimensional photonic crystal: polar body. The light-emitting diode 600 can be a common blue, green, white light photo-polar material, and the example is used to illustrate, but it is not limited to its application range. The light-emitting diode _ mainly includes a substrate _, a light-emitting layer 620, a transparent conductive layer 630, an electrode 642, an electrode 644, an insulating layer 650, and the like. The substrate 610 is, for example, an epitaxial substrate, and the light-emitting layer 62 is placed on the substrate 610, and the two-dimensional photonic crystal 66 is formed on the surface of the light-emitting layer 620. In more detail, the above-mentioned light-emitting layer 62 is composed of, for example, a semiconductor doping layer 622, an active layer 624 and a first semiconductor doping layer 626 from bottom to top, and a two-dimensional photonic crystal. 660 疋 is located on the surface of the uppermost second semiconductor doped layer 626. The transparent conductive layer 630 is located on the surface of the second semiconductor doped layer 626, and the electrodes 642 and 644 are respectively located on the first semiconductor doped layer 622 and the transparent conductive layer 630. Further, the insulating layer 650 is positioned under the transparent conductive layer 630 to separate the electrode 642 from the second semiconductor doped layer 626. 14 C S ) 1353675 2354Itwf.doc/006

在本實施例中,第—半導體摻雜層622與第二半導體 摻雜層626例如分別為n型氮化鎵(祕)層以 鎵(㈣)層。⑽,本發明並不㈣第—半導體推雜層 622、第一半導體摻雜層026、主動層π4甚或其他膜層的 材質’圖6所繪示之發光二極體_的架構也並非用以限 定本發明的顧範壽。舉凡财的發光二極體皆可應用本 發明的製作方法形成二維光子晶體,以提升其發光效率。 由;^二維光子晶體66〇主要的功能就是改變光的折 射,使得主動層624發出的光能夠順利的發散出來,而不 會全反射至發光一極體600内部,因此上述具有二維光子 晶 660的發光二極體600將可具有較高的光取出效率^ 圖7Α繪示傳統之發光二極體(LED)與結合本發明之 維光子晶體的發光二極體(PCLED),其工作電壓與驅動 體 電流的特徵曲線。此兩種發光二極體的面積大小皆為1χ1 mm2。由圖7A可以得知,本發明所提出的發光二極體In the present embodiment, the first semiconductor doped layer 622 and the second semiconductor doped layer 626 are, for example, an n-type gallium nitride (secret) layer and a gallium ((four)) layer, respectively. (10), the present invention does not (4) the first semiconductor doping layer 622, the first semiconductor doping layer 026, the active layer π4 or even other material layers of the material 'the structure of the light-emitting diode _ shown in Figure 6 is not used Gu Fanshou of the present invention is defined. The two-dimensional photonic crystal can be formed by using the fabrication method of the present invention to improve the luminous efficiency. The main function of the two-dimensional photonic crystal 66 is to change the refraction of light so that the light emitted by the active layer 624 can be smoothly diffused without being totally reflected into the interior of the light-emitting body 600, so that the above two-dimensional photon The light-emitting diode 600 of the crystal 660 will have a higher light extraction efficiency. Figure 7A shows a conventional light-emitting diode (LED) and a light-emitting diode (PCLED) incorporating the photovoltaic photonic crystal of the present invention, which works. Characteristic curve of voltage and driver current. Both of the two types of light-emitting diodes have an area of 1 χ 1 mm 2 . As can be seen from FIG. 7A, the light-emitting diode proposed by the present invention

(PCLED)具有與習知類似的電壓-電流特徵曲線,可以符合 常規的標準。 σ 此外’圖7Β繪示傳統之發光二極體(LED)與本發明之 發光二極體(PCLED),其驅動電流與發光強度的特徵曲 線。由圖7B中可以得知’在相同的驅動電流下,本發明 之發光二極體(PCLED)的發光強度為傳統發光二極體 (LED)之發光強度的兩倍以上。換言之’本發明所提出的 技術確實能夠有效增加發光·一極體的光取出效率,進而提 高其發光效率。 15 23541twf.doc/〇〇6 心另二圖8繪示傳統之發光二極體卿)盘本發明之 發先二極體(PCLED则絲型分佈,衫佈錢 Ϊ角2 3兩5之光強度進行歸-化(一―後的結 可以提古料知’本發明卿成之二維光子晶體不僅 更進-步而言,若將 =:)的背光源,將有助於提升顯二=(: 本發已以實施例揭露如上’然其並非用以限定 明之於神2 領域中具有通常知識者,在不脫離本發 明之“::巧内,當可作些許之更動與潤飾,因此本發 【圖見後附之申請專利範圍所界定者為準。 光子-實施例的-種發光二極體内二維 圖案圖2繪示本發明所形成的一種三角形陣列的二維干涉 唯干本剌之—實施_~種可產生大面積之二 、、隹干以圖案的光源系統。 -雜f =Α〜4Ε與目5A〜5G分別為本發明之不同實施例的 一、准先子晶體的製程示意圖。 的發本發明之—實施綱—種具有二維光子晶體 1353675 23541twf.doc/006 圖7A繪示傳統之發光二極體與妹 子晶體的發光二極體,其工# # 、σ 〇本發月之二維光 圖7Β緣示傳統之發動電流的特徵曲線。 體,其_狀躲錢度本㈣之發光二極 圖8繪示傳統孓發光二極體與明 出光光型分佈。 、X之發光二極體的(PCLED) has a voltage-current characteristic curve similar to that of the conventional one, which can conform to conventional standards. σ In addition, Fig. 7A shows a characteristic curve of driving current and luminous intensity of a conventional light emitting diode (LED) and a light emitting diode (PCLED) of the present invention. As can be seen from Fig. 7B, the luminous intensity of the light-emitting diode (PCLED) of the present invention is twice or more the luminous intensity of a conventional light-emitting diode (LED) under the same driving current. In other words, the technique proposed by the present invention can effectively increase the light extraction efficiency of the light-emitting body and the light-emitting efficiency. 15 23541twf.doc/〇〇6 The heart of the other two Figure 8 shows the traditional light-emitting diodes) disk of the invention first hairpin (PCLED silk distribution, shirt cloth money corner 2 3 two 5 light The intensity is normalized (the one-after the knot can be used to know the ancient material). The two-dimensional photonic crystal of the invention is not only more advanced, but if it is =:), it will help to improve the display. = (: The present disclosure has been disclosed above by way of example. However, it is not intended to limit the ordinary knowledge in the field of God 2, and without any departure from the present invention, when a little change and refinement can be made, Therefore, the present invention [as defined in the appended patent application scope. The photon-embodiment of the two-dimensional pattern in the light-emitting diode Figure 2 shows the two-dimensional interference of a triangular array formed by the present invention. Dry 剌 — 实施 实施 实施 实施 实施 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 可 - - - - - - - - - - - - - - - - - - - - - - Schematic diagram of the process of the sub-crystal. The invention of the invention - the implementation of the species has a two-dimensional photonic crystal 1353675 23541twf.doc / 006 Figure 7A The luminous diode of the traditional light-emitting diode and the sister crystal is shown, and the two-dimensional light diagram of the # 〇 发 发 示 示 示 示 示 示 示 示 示 示 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征 特征The light-emitting diode of Figure 4 shows the traditional 孓-emitting diode and the light-emitting type distribution. The light-emitting diode of X

【主要元件符號說明】 210 :亮點 d:二維干涉圖案的週期 300 :光源系統 310 :光源 320 :擴束模組 330 :分光模組 330a、330b :分光元件 340 :光學鏡組[Description of main component symbols] 210: Highlights d: Period of two-dimensional interference pattern 300: Light source system 310: Light source 320: Expanding module 330: Beam splitting module 330a, 330b: Beam splitting element 340: Optical mirror group

340a :反射鏡 350 :發光二極體 L、L1 〜L4、L’ :光線 :任兩相鄰光線具有夾角 410 :發光二極體 410a :二維光子晶體 420 :感光材料層 422 :曝光後的部份感光材料層 420a :罩幕圖案 17 1353675 23541twf.doc/006 510 :發光二極體 510a :二維光子晶體 520 :感光材料層 522 :曝光後的部份感光材料層 530 :中間層 520a、530a :第一罩幕圖案 600 :發光二極體 610 :基板 620 :發光疊層 622、626 :半導體摻雜層 624 :主動層 630 :透明導電層 642 :電極 644 :電極 650 :絕緣層 660 :二維光子晶體 18340a: mirror 350: light-emitting diodes L, L1 to L4, L': light: any two adjacent rays have an angle 410: light-emitting diode 410a: two-dimensional photonic crystal 420: photosensitive material layer 422: after exposure Part of the photosensitive material layer 420a: mask pattern 17 1353675 23541twf.doc/006 510: light-emitting diode 510a: two-dimensional photonic crystal 520: photosensitive material layer 522: exposed portion of photosensitive material layer 530: intermediate layer 520a, 530a: first mask pattern 600: light emitting diode 610: substrate 620: light emitting layer 622, 626: semiconductor doping layer 624: active layer 630: transparent conductive layer 642: electrode 644: electrode 650: insulating layer 660: Two-dimensional photonic crystal 18

Claims (1)

1353675 * * |ρ年3月ι日修(更)正i i〇0'3'2 十、申請專利範圍: 1. -種發光二極體内二維光子晶體的製作方法,包 括: 提供一發光二極體; 形成-感光材料層於該發光二極體上,其中該感光材 料層為正型光阻材料與負型光阻材料其中之一; 提供至少二道光線於該感光材料層上,並使該些光線 在該感光材料層上形成-二維干涉圖案,以藉由該二维干 涉圖案+對該感光材料層進行曝光,其中該些光線為雷射光; 若該感光材料層為正型光阻材料,則移除被曝光部份 的該感光材料層’若該感光材料層為負型光阻材料,則移 除未曝光部份的該感光材料層,以在該感光材料層上形成 一罩幕圖案;以及 轉移該感光材料層上的該罩幕圖案至該發光二極體 上’以在該發光二極體上形成該二維光子晶體的一微結構。 2. 如申請專利範圍第丨項所述之二維光子晶體的製 作方法,其_轉移該罩幕圖案至該發光二極體上的方法包 括: 以該感光材料層作為罩幕來圖案化該發光二極體;以 及 移除該感光材料層。 3. 如申凊專利範圍第1項所述之二維光子晶體的製 作方法,更包括在形成該感光材料層之前,形成一中間層 於該發光二極體上,其中該中間層對該感光材料層與該發 19 1353675 100-3-2 光二極體具有蝕刻選擇效果。 4.如U利範®第3項所述之二維光子晶體的势 作方法,其t轉移料幕瞧⑽發光二極體上的方奸 括: 以該感光材料層作為罩幕來圖案化該中間層; 移除該感光材料層; 以該圖案化之中間層作為罩幕來圖案化該發光二極 體;以及 移除該中間層。 專鄉㈣1項所叙"維奸晶體的製 作方法,Ί该微結構包括陣列配置的多個孔洞或微柱。 6. 如申請專利範圍第5項所述之二維光子晶體的製 作=法,軒涉_包鱗觸 期 性變化,.以對應形成陣列排列的該些孔洞或微柱強又週』 7. 如申請專利範圍第i項所述之 作方法,其+藉由餘兮⑪丄△千日日體的製 層上,且該先學Lt: 先線於該感光材料 供:主先線’其中該主光線為雷射光; 擴束模組,將入射之主光線的光束擴大. 的主先線刀先成為至少三道光線;以及 设 -光學鏡組’料分光後的光喊光材料層上。 20 1353675 23541TW_J1353675 * * | ρ年月月 修日修 (more) 正 ii〇0'3'2 X. Patent application scope: 1. - A method for producing two-dimensional photonic crystals in a light-emitting diode, including: providing a light a diode-forming photo-sensitive material layer on the light-emitting diode, wherein the photosensitive material layer is one of a positive-type photoresist material and a negative-type photoresist material; providing at least two light rays on the photosensitive material layer, And causing the light to form a two-dimensional interference pattern on the photosensitive material layer to expose the photosensitive material layer by the two-dimensional interference pattern +, wherein the light is laser light; if the photosensitive material layer is positive The photoresist material removes the photosensitive material layer of the exposed portion. If the photosensitive material layer is a negative photoresist material, the unexposed portion of the photosensitive material layer is removed to be on the photosensitive material layer. Forming a mask pattern; and transferring the mask pattern on the photosensitive material layer onto the light emitting diode to form a microstructure of the two-dimensional photonic crystal on the light emitting diode. 2. The method according to claim 2, wherein the method of transferring the mask pattern onto the light emitting diode comprises: patterning the photosensitive material layer as a mask a light emitting diode; and removing the photosensitive material layer. 3. The method for fabricating a two-dimensional photonic crystal according to claim 1, further comprising forming an intermediate layer on the light-emitting diode before forming the photosensitive material layer, wherein the intermediate layer is sensitive to the light-emitting diode The material layer and the hair 19 1353675 100-3-2 photodiode have an etching selection effect. 4. The method for the two-dimensional photonic crystal described in U.S. Patent No. 3, wherein the t-transfer material 瞧(10) is on the illuminating diode: the photographic material layer is used as a mask to pattern the An intermediate layer; removing the photosensitive material layer; patterning the light emitting diode with the patterned intermediate layer as a mask; and removing the intermediate layer. The hometown (4) refers to the method of making a traitor, and the microstructure includes a plurality of holes or microcolumns arranged in an array. 6. As in the production of the two-dimensional photonic crystal described in item 5 of the patent application, Xuan _ _ squama striate changes, in order to form the array of the holes or micro-columns strong and weekly. For example, in the method described in the scope of claim i, the + is performed on the layer of the eleventh day of the eleventh day, and the first is Lt: the first line is provided for the photosensitive material: the main line ' The chief ray is a laser beam; the beam expanding module enlarges the beam of the incident chief ray. The main priming knife first becomes at least three rays; and the optical mirror group is configured to illuminate the light puncturing material layer. . 20 1353675 23541TW_J 110 120 130110 120 130 140 1353675 23541TW-J140 1353675 23541TW-J S ) 1353675 23541TV/.JS) 1353675 23541TV/.J 420 410 420 410 圖4B ΓΊΓΊΓΊΠΓΊΓΊΓΊΠ420 410 420 410 Figure 4B ΓΊΓΊΓΊΠΓΊΓΊΓΊΠ 420α 420 410 圖4C420α 420 410 Figure 4C 圖4D 420α 420 410 410α 圖4Ε 410 1353675Figure 4D 420α 420 410 410α Figure 4Ε 410 1353675 m vuiw^i^^aemiM%mMV.Mt--^=: 圖5Am vuiw^i^^aemiM%mMV.Mt--^=: Figure 5A 圖5B -520 •530 -510Figure 5B - 520 • 530 - 510 520α imnnnnnrnnf520α imnnnnnrnnf 圖5CFigure 5C 1353675 23541 TW_J1353675 23541 TW_J 520α 520 530 510 圖5D 530α520α 520 530 510 Figure 5D 530α 530α 530 510 圖5Ε530α 530 510 Figure 5Ε 530α 530 510530α 530 510 圖5F 510α 510αFigure 5F 510α 510α 圖5G 1353675 23541 TW_JFigure 5G 1353675 23541 TW_J 642642 620 [626 624 622 644620 [626 624 622 644 610610 600 1353675600 1353675 GQ ffi (•n*D) mm Id—— Gywl®— IGQ ffi (•n*D) mm Id——Gywl®—I (yuu) r—MLlscOJ 1353675 23541TW_J ----傳統IID PCLED(yuu) r-MLlscOJ 1353675 23541TW_J ----Traditional IID PCLED 角度(Deg.) β ιAngle (Deg.) β ι
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