TW200814355A - High brightness light emitting diode - Google Patents

High brightness light emitting diode Download PDF

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TW200814355A
TW200814355A TW95133465A TW95133465A TW200814355A TW 200814355 A TW200814355 A TW 200814355A TW 95133465 A TW95133465 A TW 95133465A TW 95133465 A TW95133465 A TW 95133465A TW 200814355 A TW200814355 A TW 200814355A
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layer
light
emitting diode
type
electrodes
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TW95133465A
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Chinese (zh)
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TWI313942B (en
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hai-wen Xu
zhi-kui Xu
kuan-ren Zhong
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Genesis Photonics Inc
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Abstract

The invention provides a high brightness light emitting diode. It includes: a plate substrate; a quantum unit formed by a layer of gallium nitride series semiconductor on the said substratefor producing light by quantum effect; and two electrodes forming ohm contact with the quantum unit for providing electrical power. Each electrode comprises: an insulation layer formed by insulation material which becomes heterojunction energy band with quantum unit; a reflection layer with high reflection coefficient material formed on the insulation layer for compensating the Fresnel loss of reflection layer; and at least one electric conduction layer formed on the reflection layer with electric conduction material to conduct the diffusion current. It can form a Schottky rectified contact. The current can concentrate and pass through the central region to increase the inner quantum effect of the said region. The present invention increases the total brightness of emitting light and reduce the overheat problem of component at the same time.

Description

200814355 九、發明說明: 【發明所屬之技術領域】 〜本lx明疋有關於一種固態發光元件,特別是指一種高 焭度的發光二極體。 【先前技術】 發光二極體具有壽命長、省電、體積小、驅動電壓低 反應速率快、辨識率高等優點,是新—代的光源選擇之 ,週遭的日常生活中隨處可見其蹤影應用。 參閱圖1,一般,發光二極體i包含一塊矩形板狀的基 材11層以氮化鎵系的半導體材料磊晶形成在該基材n 上的里子單元12、一層形成在該量子單元12頂面的電流擴 散層13 ’及二片可提供電能的電極14。 鬼基材Π 般疋由晶格常數與該量子單元相匹配的 材料,例如藍寶石構成。 該層量子單元12具有一層與該基材^連接且包括有一 塊中央區124及一塊環圍該中央區124之外環區125的第 一型披覆層121 ( cladding layer)、一層自該第一型批覆層 121之中央區124頂面向上形成的活性層123 ( active lay^) ,及一層自該活性層123頂面向上形成的第二型批覆層122 ,該第一、二型披覆層121、122相對該活性層123形成量 子月b卩平而可以光電效應產生光。該量子單元12之第一型批 覆層121的中央區124、活性層123與第二型批覆層122, 以及形成在該第二型披覆層122上的電流擴散層13構成元 件主要向外發光的Mesa平台區100。 5 200814355 該電流擴散層η以可透光且可使電流分散均勻的材料 構成’例如錮錫氧化物(業界習稱ΙΤ〇),而可使得以電極 η施加電能時’電流水平橫向均勻地擴散流通後再垂直通 過該量子單元12而使其提昇發光效率。 *該二電極14是以例如銅、銀等金屬及/或其合金構成而 成薄片狀,彼此相對遠離地設於該發光二極體丨的兩對角 角落,並分別與該量子單元12的第—型披覆層i2i以及咳200814355 IX. Description of the invention: [Technical field to which the invention pertains] The present invention relates to a solid-state light-emitting element, and more particularly to a high-intensity light-emitting diode. [Prior Art] The light-emitting diode has the advantages of long life, low power consumption, small volume, low driving voltage, fast reaction rate, high recognition rate, etc. It is a new-generation light source, and its trace applications can be seen everywhere in daily life. Referring to FIG. 1, in general, the light-emitting diode i includes a rectangular plate-shaped substrate 11 layer. A GaN-based semiconductor material is epitaxially formed on the substrate n, and a layer is formed on the substrate. The top surface of the current diffusion layer 13' and the two electrodes 14 provide electrical energy. The ghost substrate is composed of a material whose lattice constant matches the quantum unit, such as sapphire. The quantum unit 12 has a layer connected to the substrate and includes a central region 124 and a first cladding layer 121 surrounding the outer region 125 of the central region 124, a layer from the first An active layer 123 formed on the top surface of the central portion 124 of the first type of cladding layer 121, and a second type of cladding layer 122 formed on the top surface of the active layer 123, the first type and the second type are covered. The layers 121, 122 form a quantum moon b flat with respect to the active layer 123 to generate light by a photoelectric effect. The central region 124 of the first type cladding layer 121 of the quantum unit 12, the active layer 123 and the second type cladding layer 122, and the current diffusion layer 13 formed on the second type cladding layer 122 constitute a main outward light emitting component. Mesa platform area 100. 5 200814355 The current diffusion layer η is made of a material that can transmit light and has a uniform current dispersion, such as bismuth tin oxide (known in the industry), so that the current level can be uniformly spread laterally when the electrode η is applied with electric energy. After passing through the quantum unit 12, it is circulated and raised to improve luminous efficiency. * The two electrodes 14 are formed in a sheet shape by a metal such as copper or silver and/or an alloy thereof, and are disposed at two diagonal corners of the light-emitting diode 相对 relatively far apart from each other, and are respectively associated with the quantum unit 12 Type-coating layer i2i and cough

電流擴散層13麟接觸’而可對該量子單元12提供電能 使該量子單元12產生光。 當自該二電極14施加電能時,電流擴散方式是如圖中 假想線箭號所示,自該片與電流擴散層13相歐姆接觸的電 極14側周面經過該電流擴散層13橫向水平分散流通,以 及自忒片與電流擴散層13相歐姆接觸的電極14底面直接 向下通過該電流擴散層14之後’再垂直向下擴散流通過量 子單元12的第二型彼覆層122、活性層123與第一型披覆 層121,而由於基材11的阻抗相對極大於該第一型披覆層 121,因此電流沿著第一型披覆層121底部橫向水平流向該 另一片與該第一型披覆層121相歐姆接觸的電極14成通路 ,使得量子單元12以光電效應產生光子,進而使該發光二 極體1發光。 由於電流擴散的過程是選擇阻抗最小、路徑最短的通 道進行,因此’大部分的電流會直接自該片與電流擴散層 13相歐姆接觸的電極14底面直接向下通過該電流擴散層 13 ’再垂直向下擴散流通過量子單元12而產生光,其他部 6 200814355 刀的电/瓜才θ自w亥電:流擴散層13橫向水平分散流通後再垂 ; 直擴散流通過量子單元12而產生光,因此,位於該片與電 流擴散層13相歐姆接觸的電極14下方區域發生内部量子 效應之機率的面積比相對其他部分區域(主要是Mesa平台 區100)反而較多,而成為光的主要產生區域,而在同時, 此區域產生的光在向外行進時,反而會被該片電極14反射 回1¾光-極體1内部進而轉變成内熱,無法向外射出,也 •, 目此’不但浪費了擴散流通過此區域的電流,也會產生元 _ 件過熱的問題。 因此,若能有效規劃發光二極體電流〗的擴散路徑, 使電流相對集中通過可以直接向外發光的區域(M⑽平台 區議),不但可以增加發光二極體i的發光亮度,同時: 也可以解決元件過熱的問題。 【發明内容】 一因此,本發明之目的,即在提供一種無元件過熱問題 的高亮度發光二極體。 於是,本發明高亮度發光二極體,&含一塊板狀基材 、-層量子單元、一片第一電極,及一片第二電板。 该1子單元以氮化鎵系半導體材料形成在該基材上並 具有層肖该基材連接且包括有一 士鬼中央區及一塊環圍該 中央區之外環區的第一型披覆層、一層自該第一型批覆層 之中央區頂面向上形成的活性層、—層自該活性層頂面: 上形成的第二型批覆層,及二個分別形成在該第一型披覆 層之外環區與該第二型披覆層表面的凹孔,該第一、二型 7 200814355 批覆層相對該活性層成量子能障而LV 土+ iThe current spreading layer 13 is in contact with each other to supply electrical energy to the quantum unit 12 to cause the quantum unit 12 to generate light. When electric energy is applied from the two electrodes 14, the current diffusion mode is as shown by an imaginary line arrow in the figure, and the circumferential surface of the electrode 14 from which the sheet is in ohmic contact with the current diffusion layer 13 is laterally dispersed horizontally through the current diffusion layer 13. Circulating, and the bottom surface of the electrode 14 in ohmic contact with the current diffusion layer 13 is directly passed downwardly through the current diffusion layer 14 and then diffuses vertically downward through the second type of the cladding layer 122 of the quantum unit 12, the active layer. 123 and the first type of cladding layer 121, and since the impedance of the substrate 11 is relatively greater than the first type of cladding layer 121, the current flows horizontally to the other piece along the bottom of the first type of cladding layer 121 and the first The electrode 14 of the one-type cladding layer 121 in ohmic contact forms a path, so that the quantum unit 12 generates photons by the photoelectric effect, thereby causing the light-emitting diode 1 to emit light. Since the process of current spreading is performed by selecting the channel with the smallest impedance and the shortest path, most of the current will pass directly from the bottom surface of the electrode 14 in ohmic contact with the current diffusion layer 13 through the current diffusion layer 13 ' The vertical downward diffusion flow generates light through the quantum unit 12, and the other portion 6 200814355 knife electric/cucumber θ self-ww: the flow diffusion layer 13 is horizontally dispersed and then circulated; the direct diffusion flow is generated by the quantum unit 12 Light, therefore, the area where the internal quantum effect occurs in the region below the electrode 14 in which the sheet is in ohmic contact with the current diffusion layer 13 is more than the other partial regions (mainly the Mesa platform region 100), and becomes the main light. The area is generated, and at the same time, the light generated by the area is reflected by the sheet electrode 14 back to the inside of the light-pole body 1 and converted into internal heat, which cannot be emitted outward, and also 'Not only the waste current flowing through this area is wasted, but also the problem of overheating. Therefore, if the diffusion path of the LED current can be effectively planned, the current can be relatively concentrated through the region that can directly emit light (M(10) platform area), which can not only increase the luminance of the light-emitting diode i, but also: It can solve the problem of overheating of components. SUMMARY OF THE INVENTION Accordingly, it is an object of the present invention to provide a high brightness light emitting diode without element overheating problems. Thus, the high-intensity light-emitting diode of the present invention comprises a plate-shaped substrate, a --layer quantum unit, a first electrode, and a second electrode. The subunit is formed on the substrate by a gallium nitride based semiconductor material and has a layer connected to the substrate and includes a central region of the ghost and a first type of cladding layer surrounding the outer region of the central region. An active layer formed from a top surface of the central portion of the first type of cladding layer, a layer from the top surface of the active layer: a second type of cladding layer formed thereon, and two layers respectively formed on the first type of cladding layer a recessed hole in the outer ring region of the layer and the surface of the second type of cladding layer, the first and second type 7 200814355 batch coating forms a quantum energy barrier with respect to the active layer and LV soil + i

該片第一電極設置在該其中之一個凹孔中 層由絕緣材料構成之第一絕緣層、一層由具有 材料自該第一絕緣層頂面向上形成之第一反 由導電材料自該第一反射層頂面向上形成且 覆層相歐姆接觸的第一導電層。 該片第二電極設置在該另一個凹孔中並可與該片第The first electrode of the sheet is disposed in the one of the recessed holes, wherein the first insulating layer is made of an insulating material, and the first insulating layer is made of a material from the top surface of the first insulating layer. The first conductive layer is formed with the top of the layer facing upward and the cladding layer is in ohmic contact. The second electrode of the sheet is disposed in the other recessed hole and is compatible with the sheet

接觸的第二導電層。Contacted second conductive layer.

應第二電極下方的區域,使電流相對集中通過其他可以直 接向外發光的區域,並同時造成異質能階帶(barrier energy band),形成蕭基特整流接觸(Sch〇uky c〇ntact),進而增 加务光一極體的發光亮度並同時解決元件過熱的問題。 【實施方式】 有關本發明之前述及其他技術内容、特點與功效,在 以下配合參考圖式之二個較佳實施例的詳細說明中,將可 清楚的呈現。 在本發明被詳細描述之前,要注意的是,在以下的說 明内容中’類似的元件是以相同的編號來表示。 參閱圖2,本發明高亮度發光二極體2之一第一較佳實 200814355 施例,包含一塊成矩形狀的基材21、一層由氮化鎵系的 半導體材料蠢晶形成在該基材21上的量子單元22、一層形 成在該量子單元22頂面的電流擴散層23、一片第一電極3 ,及一片與該片第一電極3相配合用以提供電能的第二電 才圣4 〇The area underneath the second electrode is such that the current is relatively concentrated through other regions that can directly illuminate outward, and at the same time, a barrier energy band is formed, forming a Schottky rectifying contact (Sch〇uky c〇ntact). In turn, the brightness of the light-emitting body is increased, and at the same time, the problem of overheating of the components is solved. The above and other technical contents, features and effects of the present invention will be apparent from the following detailed description of the preferred embodiments of the invention. Before the present invention is described in detail, it is to be noted that in the following description, similar elements are denoted by the same reference numerals. Referring to FIG. 2, a first preferred embodiment of the high-brightness light-emitting diode 2 of the present invention includes a rectangular substrate 21 and a layer of a gallium nitride-based semiconductor material formed on the substrate. a quantum unit 22 on 21, a current diffusion layer 23 formed on the top surface of the quantum unit 22, a first electrode 3, and a second electric source 4 for cooperating with the first electrode 3 of the sheet for supplying electric energy 〇

該塊基材21具有一層由具有高導熱係數材料構成已將 内熱導離的底層211,及一層由具有高反射係數材料形成在 該底層211上用以反射光的主反射層212。 该層S子單元22具有一層與該基材21之主反射層212 表面連接且包括有一塊中央區224及一塊環圍該中央區224 之外環區225的第一型披覆層221、一層自該第一型批覆層 221之中央區224頂面向上形成的活性層223、一層自該活 性層223頂面向上形成的第二型批覆層222,二個分別形成 在該第一型彼覆層221之外環區225與該第二型披覆層222 表面的凹孔226。該第一、二型彼覆層221、222相對該活 性層223形成量子能障而可以光電效應產生光。該量子單 元22之第-型批覆層221的中央區似、活性層奶與第 -型批覆層222,以及形成在該第二型披覆層222上的電流 擴散層23構成元件主要向外發光的^平台區謂。該兩 ㈣孔226彼此相對遠離地設於該發光二極體2的兩對角 角落,且該形成在第—型披覆層221之外環區225的凹孔 226,其深度不超過該第-型披覆層221與基材21連接的 底面,該另-個形成在第二型披覆層222的凹孔似 度亦不超過該第二型披覆層222與活性層如連接的2 200814355 、該電流擴散層23以可透光且可使電流分散均勻的材料 構成,例如銦錫氧化物(業界習稱ITO),而可使得以電極 14施加電能時,電流水平橫向均勻地擴散流通,進而:垂 直擴散通過該量子單元12以提昇内部發光效率。 該片第一電極3設置在形成於該第一型披覆層221之 225的凹孔226巾’並具有一層由絕緣材料構成之 弟絶緣層31、—層由具有高反射係數材料自該第一嗜緣 ==上形成之第一反射層32,及一層由導電材料自 歐1^=3?面向上形成且與該第—型批覆層如相 型披覆#221 4電層33,該第一絕緣層31與臨接的第一 披伋層22!因為材料的差異造成 基特整流,該第-反射…造成光的一次、二= 1可補料失;構成該第—絕❹3緣 如氮切氧化…χ)、 4匕銘("A1 η、长 v 1A〇2 j 'The block substrate 21 has a base layer 211 which is made of a material having a high thermal conductivity and which conducts internal heat, and a layer which is formed of a material having a high reflectance on the bottom layer 211 for reflecting light. The S subunit 22 has a layer connected to the surface of the main reflective layer 212 of the substrate 21 and includes a central region 224 and a first type of cladding layer 221 and a layer surrounding the outer region 225 of the central region 224. An active layer 223 formed from a top surface of the central portion 224 of the first type of cladding layer 221, and a second type of cladding layer 222 formed from a top surface of the active layer 223, two of which are respectively formed on the first type The outer annular region 225 of the layer 221 and the concave hole 226 on the surface of the second type cladding layer 222. The first and second type cladding layers 221 and 222 form a quantum energy barrier with respect to the active layer 223 to generate light by a photoelectric effect. The central region of the first-type cladding layer 221 of the quantum unit 22, the active layer milk and the first-type cladding layer 222, and the current diffusion layer 23 formed on the second-type cladding layer 222 constitute a component that mainly emits light outward. The ^ platform area is said. The two (four) holes 226 are disposed at opposite corners of the light-emitting diode 2 at a distance from each other, and the recess 226 formed in the outer ring region 225 of the first-type cladding layer 221 has a depth not exceeding the first a bottom surface of the -type cladding layer 221 connected to the substrate 21, and the recessed hole similarity formed in the second type cladding layer 222 does not exceed the second type of cladding layer 222 and the active layer such as the connection 2 200814355, the current diffusion layer 23 is made of a material that can transmit light and can uniformly disperse current, for example, indium tin oxide (known in the industry as ITO), and the current level can be uniformly and laterally diffused when the electrode 14 is applied with electric energy. And further: vertically diffusing through the quantum unit 12 to enhance internal luminous efficiency. The first electrode 3 of the sheet is disposed in a recess 226 formed in the 225 of the first type cladding layer 221 and has a layer of insulating layer 31 made of an insulating material, and the layer is made of a material having a high reflection coefficient. a first reflective layer 32 formed on the faint edge ==, and a layer formed of a conductive material from the surface of the metal 1^=3? and coated with the first type of cladding layer such as a phase pattern #221 4 electrical layer 33, The first insulating layer 31 and the adjacent first plenum layer 22! The base rectification is caused by the difference of the materials, and the first reflection and the second =1 can be replenished; Such as nitrogen cut oxidation...χ), 4匕铭("A1 η, long v 1A〇2 j '

Ta〇) 2/、乳化錯(Zr〇2)、氧化鋅(Zn〇)、氧化釦( h〇5)、氟化鎂(MgF2)、氮化鈦(T -( 射層32盥第一墓贲麻。 ^手構成苐一反 欽、鋼、銅鈾I 4是例·如金、銘、銀、錄、 巴、鈒專金屬,及/或此等金屬所$ μ yv 金,同時需注意的是構成第一反射層32料:所成的合 大於構成第-導w 33 之材枓的阻值必須 年臨。 層33之材料的阻值,另外,該芦篦一道 =3可分別由上述的金屬,及/或合金形成至少二 联'豐構成,而可獲得更佳的導電效果。 層v電 4片弟二電極4設置在形成於該第二型披覆層222的 10 200814355 凹孔226中並穿通過該雷 ,並且有使得頂面裸露在外界 有層由絶緣材料構成之第二絕緣層41、…呈 有高反射係數材料自該第- 層由具 发弟一、%緣層41頂面向上 反射層42,及一層由導電材料自該 ^ Λ' Β ^ir m, ^ 一反射層42頂面向上 幵/成且與该層電流擴散声 ,、戚層13电連接同時與該層第二型批覆 層222相歐姆接魍沾梦-推Λ ^ 土仙復 的第該第二絕緣層與臨接 = 覆層、電流擴散層因為材料的差異造成異質能Ta〇) 2/, emulsified wrong (Zr〇2), zinc oxide (Zn〇), oxidized buckle (h〇5), magnesium fluoride (MgF2), titanium nitride (T-(shot layer 32盥 first tomb)贲麻. ^Hand composition 苐一反钦, steel, copper uranium I 4 is an example · such as gold, Ming, silver, recorded, Pakistan, 鈒 special metal, and / or these metals $ μ yv gold, while paying attention The material of the first reflective layer 32 is formed: the resultant value is greater than the resistance of the material constituting the first guide w 33. The resistance of the material of the layer 33, in addition, the reed together = 3 can be respectively The above metal, and/or alloy forms at least a double 'bumpy structure, and a better conductive effect can be obtained. The layer v electric 4 pieces of the second electrode 4 are disposed on the 10 200814355 concave formed on the second type cladding layer 222 The hole 226 passes through the mine and has a second insulating layer 41 made of an insulating material on the outside surface, and has a high reflection coefficient material from the first layer. The top of the layer 41 faces the upper reflective layer 42, and one layer is made of a conductive material from the Λ' Β ^ir m, ^ a top of the reflective layer 42 faces up and down and the current is diffused with the layer, and the layer 13 is electrically Pifu simultaneously access the second-type layer, an ohmic layer 222 sprite dip dream - Soil push Λ ^ Sin complex of the second insulating layer and the adjacent portion = coating, because of differences in the current spreading layer material can result in a heterogeneous

階r而形成蕭基特整流接觸,該第二反射層42可造成光 的二次反射,而可補償菲淫斯損失;類似地,構成 该第一I緣層41之絕緣材料是例如氮化碎(則ο、氧化石夕 (Sax)、氧化鈦(Ti〇2)、氧化鋁⑼^小氧化錯⑺〜 )、氧化鋅(ZnO)、氧化鈕(Ta2〇5)、氟化鎂(Μ#〗)、氮 :匕鈦(TlN) #,構成第二反射層42與第二導電層43的材 料是例如金、銘、銀、錢、欽、錮、銅、韵、錢、錶等金 屬及/或此等金屬所成的合金5同時需注意的是構成第二 反射層42之材料的阻值必須大於構成第二導電層43之材 料的阻值,另外,該層弟二導電層43可分別由上述的金屬 及/或合金形成至少一層導電膜辱疊構成,而可獲得更佳 的導電效果。 當自第一、二電極3、4施加電能時,電流擴散方式是 如圖中假想線箭號所示,由於電流被第一電極3的第一絕 緣層31阻絕,而自第一電極3與電流擴散層23相電連接 的第—導電層33侧周面經過該電流擴散層23橫向水平分 散’再自電流擴散層23向下擴散流通過量子單元22的第 11 200814355 二型彼覆層222、活性層223與第一型披覆層221,再沿著 第一型披覆層221底部橫向水平流向擴散,並由於第二電 極4的第二絕緣層41阻絕而再向上流動後自該第二電極4 之第二導電層43侧周面進入該第二電極4成通路,使該量 子單元22以内部量子效應產生光子,進而使發光二極體2 發光。 由於第一、二電極3、4之第一、二絕緣層3i、4i的 阻絕’因此對應H、二電極3、4下方的區域幾乎是沒 有電流擴散流動的,也因此,此量子單元22對應此區域的 部分是幾乎不產生光子的區域,所以,此區域不會發生產 生的光因為第-、二電極3、4的阻擔反射而重回元件内部 ,進而造成元件過熱的問題。 —絕大部分的電流自第—電極3的第—導電層%侧周面 :士電流擴散層23橫向水平傳導後,再對應向下流通過量 j單元22臬應此部份的區域,流向第二電極4的第二導電 層43的側周面形成通路,而使得該量子單元22㈣應區 ,以内部量子效應產生光子’也就是說,絕大多數的電流 是集中擴散通過該量子單元對應元件可以直接將光向外 隹出之Mesa平台區1〇〇的區域,而有效將所有提供的電流 木中後產生光,因而可以有效提昇元件的發光亮度。 “此外,部分仍未能直接自Mesa平台區1〇〇向外射出的 光’則再次藉由該塊基材21的主反射層212與第―、二電 極3 :、4的第-、二反射層32、42形成一次、二次反射, 進而補償菲涅斯損失’並自Mesa平台區1〇〇向外射出,以 12 200814355 增加整體發光亮度且可同時避免產>生内熱的問題。 參閱圖3,本發明高亮度發光二極體之一第二較佳實施 例,是與該第一較佳實施例所述相似,其不同處僅在於該 第一、一電極3、4之第一、二絕緣層3卜41,的態樣而已 ,由於其他結構均已於前述說明中所詳述,在此不再多加 重複贅述。The step r forms a Schottky rectifying contact, and the second reflecting layer 42 can cause secondary reflection of light to compensate for the loss of Philippine smear; similarly, the insulating material constituting the first I-edge layer 41 is, for example, nitrided. Broken (then, oxidized stone (Sax), titanium oxide (Ti〇2), alumina (9) ^ small oxidized (7) ~), zinc oxide (ZnO), oxidation button (Ta2 〇 5), magnesium fluoride (Μ #〗), nitrogen: 匕Ti (TlN) #, the material constituting the second reflective layer 42 and the second conductive layer 43 is metal such as gold, Ming, silver, money, Chin, 锢, copper, rhyme, money, table, etc. And/or the alloy 5 formed by the metals, it should be noted that the resistance of the material constituting the second reflective layer 42 must be greater than the resistance of the material constituting the second conductive layer 43. In addition, the layer of the second conductive layer 43 At least one layer of the conductive film may be formed by the above-mentioned metal and/or alloy, respectively, to obtain a better conductive effect. When electric energy is applied from the first and second electrodes 3, 4, the current diffusion mode is as indicated by an imaginary line arrow in the figure, since the current is blocked by the first insulating layer 31 of the first electrode 3, and from the first electrode 3 The side surface of the first conductive layer 33 electrically connected to the current diffusion layer 23 is laterally horizontally dispersed through the current diffusion layer 23, and is diffused downward from the current diffusion layer 23 to flow through the quantum unit 22 of the 11th 200814355 type 2 cladding layer 222. The active layer 223 and the first type of cladding layer 221 are further horizontally and horizontally diffused along the bottom of the first type of cladding layer 221, and are further flowed upward due to the second insulating layer 41 of the second electrode 4 being blocked. The peripheral surface of the second conductive layer 43 of the two electrodes 4 enters the second electrode 4 to form a path, and the quantum unit 22 generates photons by internal quantum effects, thereby causing the light-emitting diode 2 to emit light. Since the first and second insulating layers 3i, 4i of the first and second electrodes 3, 4 are blocked, the area under the H and the two electrodes 3, 4 has almost no current diffusion flow, and therefore, the quantum unit 22 corresponds to The portion of this region is a region where photons are hardly generated. Therefore, light generated in this region does not return to the inside of the element due to the reflection of the first and second electrodes 3 and 4, which causes the component to overheat. - most of the current flows from the side surface of the first conductive layer of the first electrode 3 to the side of the first conductive layer: the current diffusion layer 23 is horizontally and horizontally distributed, and then flows to the area where the excess element j 22 flows downward, and flows to the first portion. The side peripheral surface of the second conductive layer 43 of the two electrodes 4 forms a passage, so that the quantum unit 22 (4) should be a region to generate photons with internal quantum effects. That is, most of the current is concentrated and diffused through the corresponding elements of the quantum unit. The light can be directly extracted from the area of the Mesa platform area of the Mesa platform area, and all the supplied currents are effectively generated in the wood, thereby effectively improving the luminance of the element. "In addition, some of the light that has not yet been directly emitted from the Mesa platform area" is again passed through the main reflection layer 212 of the block substrate 21 and the first and second electrodes of the first and second electrodes 3: The reflective layers 32, 42 form primary and secondary reflections, which compensate for the Fresnel loss' and are emitted outward from the Mesa platform area. The overall illumination brightness is increased by 12 200814355 and the heat generation problem can be avoided at the same time. Referring to FIG. 3, a second preferred embodiment of the high-brightness light-emitting diode of the present invention is similar to that described in the first preferred embodiment except that the first and first electrodes 3 and 4 are different. The first and second insulating layers 3 are in the form of 41, and since other structures have been described in detail in the foregoing description, the detailed description thereof will not be repeated here.

該第一、二電極3、4的第一、二絕緣層31,、41,分別 具有多數穿孔而形成預定圖像,而當自第一、二電極3,、4, 施加電能時,電流擴散方式是如圖中假想線箭號所示,其 中大部分的電流由於第-絕緣層31,的阻播,而自第一電極 3’與電流擴散層23相電連接的第一導電層33側周面經過該 =流,散層23橫向水平分散流通,再垂直向下擴散流通過 里子早7L 22產生光;少部分的電流則因為第一絕緣層31, 之夕數牙孔形成的多數擴散通道的效應,而循著此些假想 的擴散通道向下流通過量子單元22進而產生光。 雖然,將電流集中擴散通過對應於元件可以主要向外 出光的Mesa平台區刚進而產生可以直接向外界射出光的 方式,可以提昇發光二極髓2的發光亮度,同時避免對應 第一、二電極3,、4,下方之區域產生光而欲向外射出時,會 被第-、二電極3’、4’阻擋反射回元件中,進而產生内熱的 問題。 、E疋富电k迥於果甲時也同時會產生元件工作壽命減 少的問題,所以在本第二較佳實施例巾,特地設計第一、 二電極3,、4,的第一、二絕緣層31,、4i,具有多數穿孔而成 13 200814355The first and second insulating layers 31, 41 of the first and second electrodes 3, 4 respectively have a plurality of perforations to form a predetermined image, and when electric energy is applied from the first and second electrodes 3, 4, current is diffused. The mode is shown by the imaginary line arrow in the figure, wherein most of the current is blocked by the first insulating layer 31, and the first conductive layer 33 side electrically connected from the first electrode 3' to the current spreading layer 23 is provided. After the circumferential surface passes through the flow, the scattered layer 23 is horizontally dispersed horizontally, and then vertically diffused downwardly through the lining to generate light 7L 22; a small part of the current is due to the first insulating layer 31, and the majority of the diffusion of the occlusion is formed. The effect of the channel, followed by such imaginary diffusion channels, flows down through the quantum unit 22 to produce light. Although the current is concentrated and diffused through the Mesa platform region corresponding to the component which can mainly emit light, and then the light can be directly emitted to the outside, the luminance of the light-emitting diode 2 can be improved, and the corresponding first and second electrodes can be avoided. 3, 4, when the lower area produces light and is intended to be emitted outward, it will be blocked by the first and second electrodes 3', 4' from being reflected back into the element, thereby causing internal heat problems. In the second preferred embodiment, the first and second electrodes 3, 4, the first and second are specifically designed to reduce the working life of the component. The insulating layers 31, 4i have a plurality of perforations 13 200814355

預w樣,藉由該等穿孔造成產生多數供電流擴散的擴散 通運的效應’使得部分電流可循此些假想的通道擴散,而 在對應於第-、二電極3,、4,下方的區域產生光,進而分散 電流以避免元件工作壽命減少的問題;而在此同時,為了 避免此等區域所產生的光因為第―、二電極3,、4,本身的限 制而轉變成内熱的問題’在本例中亦是類似於上例所說明 的二是藉由基材21的主反射層212與第—、二電極3,、4, 的第…二反射層32、42相配合使光產生-次、二次反射 ’以補償菲沒斯損失,進而將光自對應厘⑽平台區刚向 外射出,以同時增加元件的發光亮度。 .‘·T &上述„兒明可知,本發明高亮度發光二極體主要是 邑緣材料|有两反射係婁文的材料,及^電材料开》成之 絕緣層、反射層與導電層構成第一、二電極,藉著絕緣層 形成異貝旎階帶的提昇,確保電流在電流擴散層中擴散傳 導’進而將'電流集中通過對應可直接向外發射光之平 口區100的量子單元22而產生直接向外射出的光,以有效 提昇元件的电光冗度’同時’也盡量減少對應於第一、二 電極下方不易將光直接射出的區域產生光,而避免了此區 域產生光時因為第一、二電極的阻擋反射而重回元件内部 ,進而造成S件過熱的問題;此外,本發明也藉由第一、 黾極之反射層,以及基材的主反射層的設計,造成内部 量子效應產生之光的-次、二次反射,以補償菲淫斯損失 ,進而使内部產生的光更能有效集中自Mesa平台區向外射 出,而提昇元件整體的發光亮度,確實達到本發明的創作 14 200814355 目的。 .弋 惟以上所述者,僅為本發明之較佳實施例而已,當不 =以此限疋本發明實施之範圍,#大凡依本發明中請專利 範圍及發明說明内容所作之簡單的等效變化與修飾,皆仍 屬本發明專利涵蓋之範圍内。 【圖式簡單說明】 圖1是一剖視示意圖,說明習知的發光二極體,並說 月其内部電流擴散的狀況; 之一 =2是一剖視不意圖,說明本發明高亮度發光二極體 一第〜較佳實施例,並說明其内部電流擴散的狀況;及 一圖3是一剖視示意圖,說明本發明高亮度發光二極體 第〜較佳實施例,並說明其内部電流擴散的狀況。 15 200814355 【主要元件符號說明】 100 Mesa平台區 226 凹孔 2 發光二極體 23 電流擴散層 21 基材 3、 3, 第一電極 211 底層 31、 ‘31, 第一絕緣層 212 主反射層 32 第一反射層 22 量子單元 33 第一導電層 221 第一型批覆層 4、 4, 第一電極 222 第二型批覆層 41、 •41, 第二絕緣層 223 活性層 42 第二反射層 224 中央區 43 第二導電層 225 外環區 16Pre-w, the effect of the diffusion conduction that causes most of the current to diffuse by the perforations is such that part of the current can be diffused through the imaginary channels, and in the region below the first and second electrodes 3, 4, Producing light, and then dispersing the current to avoid the problem of reducing the working life of the component; at the same time, in order to avoid the problem that the light generated in these regions is converted into internal heat due to the limitation of the first and second electrodes 3, 4, In the present example, similar to the above description, the second reflective layer 212 of the substrate 21 is combined with the second and second electrodes 3, 4 of the second and second electrodes 3, 4 to make the light The -secondary and secondary reflections are generated to compensate for the loss of the phenotype, and then the light is emitted directly from the corresponding PCT (10) platform region to simultaneously increase the luminance of the component. .································································································· The layer constitutes the first and second electrodes, and the enhancement of the metabolite layer by the insulating layer ensures that the current diffuses and conducts in the current diffusion layer to further concentrate the current through the quantum corresponding to the flat region 100 which can directly emit light outward. The unit 22 generates light that is directly emitted outward to effectively increase the electrical and optical redundancy of the component. At the same time, it also minimizes the generation of light corresponding to the region under the first and second electrodes that is not easy to directly emit light, thereby avoiding light generated in this region. The problem of overheating of the S component due to the blocking reflection of the first and second electrodes, thereby causing the problem of overheating of the S component; in addition, the present invention also utilizes the first, the reflective layer of the drain, and the design of the main reflective layer of the substrate, The secondary and secondary reflections of the light produced by the internal quantum effect to compensate for the loss of the Philippine sensation, so that the internally generated light can be more effectively concentrated from the Mesa platform area, and the overall component is improved. The illuminating brightness does not achieve the purpose of the present invention. The above is only the preferred embodiment of the present invention, and is not limited to the scope of the present invention. The simple equivalent changes and modifications made in the scope of the patent and the description of the invention are still within the scope of the invention. [Simplified illustration] FIG. 1 is a schematic cross-sectional view showing a conventional light-emitting diode Body, and said the state of internal current diffusion; one = 2 is a cross-sectional view, illustrating a high-brightness light-emitting diode of the present invention - a preferred embodiment, and illustrating its internal current diffusion; Figure 3 is a cross-sectional view showing the high-brightness light-emitting diode of the present invention in a preferred embodiment, and illustrating the state of internal current diffusion. 15 200814355 [Main component symbol description] 100 Mesa platform area 226 recessed hole 2 Light-emitting diode 23 current diffusion layer 21 substrate 3, 3, first electrode 211 bottom layer 31, '31, first insulating layer 212 main reflective layer 32 first reflective layer 22 quantum unit 33 Conductive layer 221 first type cladding layer 4, 4, first electrode 222 second type cladding layer 41, 41, second insulating layer 223 active layer 42 second reflective layer 224 central region 43 second conductive layer 225 outer ring region 16

Claims (1)

200814355 申請專利範圍: 種 亮度發光二極體,包含 一塊板狀基材; 一層量子單元’以氮化鎵系半導體材料形成在該基 材^並具有-層與該基材連接且包括有—塊中央區及一 塊環圍該中央區之外環區的第—型披覆層、—層自該第 -型批覆層之中央區頂面向上形成的活性層、—層" 活性層頂面向上形成的第二型批覆層,及二個分㈣: 在该弟-型披覆層之外環區與該第二型披覆層表面的凹 孔,該第-、二型批覆層相對該活性層成量子能障而以 光電效應產生光; ” 一片第-電極’設置在形成於該第—型披覆層之外 %區的凹孔中’並具有—層由絕緣材料構成之第-絕緣 層 ' 一層由具有高反射係數材料自該第—絕緣層頂面向 上形成之第-反射層5及一層由導電材料自該第一反射 層頂面向上形成且與該第-型批覆層相歐姆接觸的第一 導電層;及 -片第二電極’設置在形成於該第二型披覆層表面 ::孔中並可與該片第一電極相配合對該量子單元提供 電能’亡具有一層由絕緣材料構成之第二絕緣層、一層 々由具有面反射係數材料自該第二絕緣層頂面向上形成之 第:反射層’及—層由導電材料自該第二反射層頂面向 上φ成且與该第二型批覆層相歐姆接觸的第r導電層。 2·依射請專利範圍第1項所述之高亮度發光二極體,其 17 200814355 中,§亥塊基材具有一 ,— 層由具有高反射係數 材枓形成在该底層上的主反射層。 3. 依據申請專利範圍第2項所述曰之高亮度發光二極體,更 包含-層由透明且可導電的材料形成在該第二 上的電流擴散層。 3 4. 依射請專利範圍第3項所述之高亮度發光二極體,立 中,該第一、二電極之第-、二絕緣層是分別選自由; 列所構成之群組形成:氮化石夕、氧化石夕、氧化鈦、氧化 紹、氧化錯、氧化鋅'氧化纽、氟化鎂、氮化鈦。 5. 依據申請專利範圍第4項所述之高亮度發光二極體,盆 :,構成該第-、二電極之第―、二反射層之材料的阻 大於構成該第一、二電極之第一、二導電 阻值。 ^ Τ,該第一、二電極之第一、二導電層分別包括至少一 層選自由下列所構成之群組所形成的導電膜:金、鋁、 銀、铑、鈦、錮、銅、鉑、鈀、銥,及此等之組合。 7·依據申請多利範圍第6項所述之高亮度發光二極體,其 中,该第一、二電極之第一、二反射層分別選自由下列 所構成之群組所形成:金、鋁、銀、铑、鈦、銦、鋼、 舶、鈀、銥,及此等之組合。 8.依據申請專利範圍第7項所述之高亮度發光二極體,盆 ,該第一、二電極之·第一、二絕緣層分別具有複數可 供電流穿過擴散的穿孔而成預定態樣。 18200814355 Patent application scope: a brightness light-emitting diode comprising a plate-shaped substrate; a quantum unit 'formed on the substrate by a gallium nitride-based semiconductor material and having a layer connected to the substrate and including a block a central zone and a first-type coating layer surrounding the outer ring zone of the central zone, an active layer formed from the top surface of the central zone of the first-type cladding layer, a layer " an active layer top surface Forming a second type of coating layer, and two sub-divisions (4): in the outer ring region of the disc-type coating layer and the concave hole on the surface of the second type coating layer, the first- and second-type coating layers are opposite to the activity The layer is formed into a quantum energy barrier to generate light by a photoelectric effect; a piece of the first electrode is disposed in a recess formed in the % region outside the first cladding layer and has a first insulating layer composed of an insulating material a layer of a first reflective layer 5 formed of a material having a high reflectance from the top surface of the first insulating layer and a layer formed of a conductive material from the top surface of the first reflective layer and ohmic with the first type of cladding layer Contacted first conductive layer; and - sheet second The pole is disposed in the surface of the second type of cladding layer: and can cooperate with the first electrode of the sheet to supply electrical energy to the quantum unit. The anode has a second insulating layer composed of an insulating material and a layer of germanium. The first reflective layer formed from the top surface of the second insulating layer has a surface reflection coefficient material and the layer is made of a conductive material from the top surface of the second reflective layer and is in ohmic contact with the second type of cladding layer. The r-th conductive layer. 2. The high-brightness light-emitting diode according to the first item of the patent scope, in the case of 2008 200835355, the § hai block substrate has one, the layer is formed by a material having a high reflection coefficient The main reflective layer on the bottom layer. 3. The high-brightness light-emitting diode according to the second aspect of the patent application, further comprising a layer of a current diffusion layer formed of a transparent and electrically conductive material. 3 4. According to the high-brightness light-emitting diode according to item 3 of the patent scope, the first and second insulating layers of the first and second electrodes are respectively selected from the group consisting of: Nitride, oxidized stone, titanium oxide, oxidation绍, Oxidation error, Zinc oxide 'oxidation, magnesium fluoride, titanium nitride. 5. According to the high-brightness light-emitting diode according to item 4 of the patent application scope, the basin: constitutes the first and second electrodes The resistance of the material of the two reflective layers is greater than the first and second conductive resistance values of the first and second electrodes. ^ Τ, the first and second conductive layers of the first and second electrodes respectively comprise at least one layer selected from the following a conductive film formed by a group consisting of gold, aluminum, silver, iridium, titanium, ruthenium, copper, platinum, palladium, rhodium, and the like. 7. According to the high brightness described in the sixth item of the application a light emitting diode, wherein the first and second reflective layers of the first and second electrodes are respectively selected from the group consisting of gold, aluminum, silver, tantalum, titanium, indium, steel, palladium, palladium, Oh, and the combination of these. 8. The high-intensity light-emitting diode according to item 7 of the patent application scope, the first and second insulating layers of the first and second electrodes respectively have a plurality of perforations for allowing current to flow through the diffusion to form a predetermined state. kind. 18
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI419369B (en) * 2009-11-06 2013-12-11
TWI453956B (en) * 2010-12-31 2014-09-21

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI419369B (en) * 2009-11-06 2013-12-11
TWI453956B (en) * 2010-12-31 2014-09-21

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