TWI285448B - Light-emitting diode with high resistivity insulation structure - Google Patents

Light-emitting diode with high resistivity insulation structure Download PDF

Info

Publication number
TWI285448B
TWI285448B TW95108574A TW95108574A TWI285448B TW I285448 B TWI285448 B TW I285448B TW 95108574 A TW95108574 A TW 95108574A TW 95108574 A TW95108574 A TW 95108574A TW I285448 B TWI285448 B TW I285448B
Authority
TW
Taiwan
Prior art keywords
light
layer
type
insulating structure
resistance insulating
Prior art date
Application number
TW95108574A
Other languages
Chinese (zh)
Other versions
TW200735405A (en
Inventor
Kuan-Ren Jung
Hai-Wen Shiu
Jr-Kuei Shiu
Original Assignee
Genesis Photonics Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Genesis Photonics Inc filed Critical Genesis Photonics Inc
Priority to TW95108574A priority Critical patent/TWI285448B/en
Application granted granted Critical
Publication of TWI285448B publication Critical patent/TWI285448B/en
Publication of TW200735405A publication Critical patent/TW200735405A/en

Links

Landscapes

  • Led Devices (AREA)

Abstract

This invention relates to a light-emitting diode (LED) with high resistivity insulation structure, which is characterized in that a high resistivity insulation structure in imaginary line between two electrodes and having depth less than the active layer is formed downwards on the surface of the p-cladding layer of the LED and/or the indium-tin-oxide (ITO) layer. The high resistivity insulation structure has high resistance in comparison with the p-cladding layer so that, when the electrodes are supplying electrical energy, the path of the active layer for the electric current to distribute and pass is increased. Therefore, over-heating on local region due to concentrated electric current on a specific region is prevented to ensure service life of the LED.

Description

1285448 九、發明說明: 【發明所屬之技術領域】 本發明是有關於一種固態發光元件,特別是指一種發 光二極體。 【先前技術】 由於固態發光元件具有壽命長、省電、體積小、驅動 電壓低、反應速率快、辨識率高等優點,是新一代的光源 種類之一,特別是發光二極體,已廣為應用在週遭的曰常 生活中。 參閱圖1、圖2, 一般,發光二極體丨包含一基材u、 至少一磊晶形成在該基材u上的量子單元12、一形成在該 ΐ子單兀12頂面的透明導電層13,及二可提供電能的電極 14 〇 4基材11是由晶格常數與該量子單元相匹配的材料構 成,舉例來說,該量子單元丨2是屬氮化鎵系的半導體材料 .時’該基材11則為易於磊晶的藍寶石。 邊5子單元12自該基材11頂面向上磊晶形成,具有一 第一型披覆層121 ( cladding layer )、一第二型批覆層122, 及一在該第一、二型批覆層121、122之間的活性層123( active layer),該第一、二型披覆層121、122相對該活性層 123形成量子能障而可以光電效應產生光;該第一、二型彼 覆層121、122分別為η型披覆層與p型彼覆層;且,一般 為提昇發光效率,均會以複數量子單元為最佳設計,但在 本例與圖示中,為使說明清楚起見,僅以一量子單元12為 5 1285448 例說明。 該透明導電層13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,電流均勻地流通過該量子單元12而使其提 昇發光效率。 該二電極14彼此相對遠離地設於該發光二極體的兩對 角角洛,並與該量子單元12的第一型披覆層121以及該透1285448 IX. Description of the Invention: [Technical Field] The present invention relates to a solid-state light-emitting element, and more particularly to a light-emitting diode. [Prior Art] Since the solid-state light-emitting element has the advantages of long life, power saving, small volume, low driving voltage, fast reaction rate, high recognition rate, etc., it is one of a new generation of light source types, especially a light-emitting diode, which has been widely used. It is used in everyday life. Referring to FIG. 1 and FIG. 2, in general, the LED assembly comprises a substrate u, at least one quantum unit 12 epitaxially formed on the substrate u, and a transparent conductive layer formed on the top surface of the dice 12 Layer 13, and two electrodes 14 for supplying electric energy 〇4 substrate 11 is composed of a material whose lattice constant matches the quantum unit. For example, the quantum unit 丨2 is a gallium nitride-based semiconductor material. When the substrate 11 is a sapphire that is easy to epitaxial. The edge 5 subunit 12 is formed by epitaxial epitaxy from the top surface of the substrate 11 and has a first cladding layer 121, a second cladding layer 122, and a first and second type cladding layer. An active layer 123 between 121 and 122, the first and second type cladding layers 121 and 122 form a quantum energy barrier with respect to the active layer 123 to generate light by photoelectric effect; the first and second types are covered by each other; The layers 121 and 122 are respectively an n-type cladding layer and a p-type cladding layer; and generally, in order to improve luminous efficiency, a plurality of subunits are optimally designed, but in this example and the illustration, for clarity of explanation For the sake of illustration, only one quantum unit 12 is illustrated as 5 1285448. The transparent conductive layer 13 is made of a material that can transmit light and has a uniform current dispersion, such as indium tin oxide (referred to as ITO in the industry), so that when the electrode 14 is applied with electric energy, a current flows uniformly through the quantum unit 12 . It makes it improve luminous efficiency. The two electrodes 14 are disposed at opposite angles of the light emitting diode relative to each other, and the first type of cladding layer 121 of the quantum unit 12 and the through electrode

明導電層13毆姆接觸,而可對該量子單元12提供電能使 該量子單元12產生光。 s自该二電極14施加電能時,電流經過該透明導電層 13分散流通過該量子單元12,而使該量子單元丨2以光電 效應產生光子,進而使該發光二極體1發光。 由於第型披覆層121的電阻率小於第二型披覆層i22 丄所以當自該二電極14施加電能時,電流會相對較集中於 電極14的四周而未能均勻分散,並以兩電極14之假想連 線的最短路徑分散行進(如圖2中箭號所示),也因此,該 毛光-極冑1會因為電流分散較集中在此等區域而造成此 等區域過熱,U導致該發光二極體i的工作壽命縮短。 斤以目岫的發光二極體需要加以改進,以避免電流 ,皇土的問題-’-疫隨先韻危梅Γ 【發明内容】 均勻 因此,本發明之目的,即在提供一 而不集中於特定區域的發光二極體。 種可以使電流分散 於是,本發明一 種具有高阻態絕緣結構之發光二極體 1285448 極,及一高阻態絕緣 包含一基材、至少一量子單元 結構 〜該量子單元與該基材連接並自祕材向上依序具有一 弟-型彼覆層、一活性層,及一第二型批覆層,該第一、 二型披覆層相對該活性層形成量子能障而可使該量子單元 以光電效應產生光。 4 -電極分別與該第_、二型批覆層形成歐姆接觸, 而可對該量子單S提供電能而使該量子單元產生光。 _該高阻態絕緣結構形成在該第二型披覆層中並位於該 一電極假想連線之間,日知 間且相對该弟二型批覆層具有高電阻 率而使電流分散通過該活性層時的路徑增加而不集中。 透明導電層 此外’本發明之另一種具有高阻態絕緣結構之發光二 極體,包含-基材、至少一量子單元、 一 電極,及一高阻態絕緣結構。 該量子單元與該基材連接並自該基材向 第一型披覆層、一活性声,及皆^χχ 斤八有 石Γ玍層,及一弟二型批覆層,該、 二型披覆層相對該活性層形 t 以光電效應產生光。7成里子4而可使該量子單元 該透明導電層連接在 ……β 里子早70相反於與該基材連接 的頂面上,疋可透光且可使電流均勻分散。 該二電極分別與該第一型批覆層 姆接觸,而可對竽旦工时—上日 净电層相£人 。 亥里子早兀提供電能使該量子單元產生光 該高阻態絕緣社播 構自㈣明導電層向下形成並位於該 7 1285448 二電極假想連線之間,且相對該透明導電層具有高電 而使電流分散通過該活性層時的路徑增加而不集中。 千 本發明的功效在於以自?型批覆層,及/或自透明 層表面向下形成且深度未達活性層的高阻態絕緣結構二 流分散路徑增加,並使得該量子單元的異f能階帶择、: 隧效應減少’讓電流不致於過度集中而造成局部區 ’確保發光二極體的卫作壽纟。 錢The conductive layer 13 is in contact with the ohmic layer, and the quantum unit 12 can be supplied with electrical energy to cause the quantum unit 12 to generate light. When electric energy is applied from the two electrodes 14, a current flows through the transparent conductive layer 13 through the quantum unit 12, and the quantum unit 丨2 generates photons by photoelectric effect, thereby causing the light-emitting diode 1 to emit light. Since the resistivity of the first type cladding layer 121 is smaller than that of the second type cladding layer i22, when electric energy is applied from the two electrodes 14, the current is relatively concentrated on the periphery of the electrode 14 and is not uniformly dispersed, and the two electrodes are used. The shortest path of the imaginary connection of 14 is dispersed (as indicated by the arrow in Fig. 2). Therefore, the glare-pole 胄1 will cause overheating of these areas due to the current dispersion being concentrated in these areas, resulting in U The operating life of the light-emitting diode i is shortened. The illuminating LEDs that need to be witnessed need to be improved to avoid the current, the problem of the emperor soil-'--------------------------------------------------- Light-emitting diodes in a specific area. The present invention can disperse current, and a high-resistance insulating structure of the light-emitting diode 1285448 pole, and a high-resistance insulation comprise a substrate, at least one quantum unit structure - the quantum unit is connected to the substrate The self-secret material has a brother-type coating layer, an active layer, and a second type coating layer, and the first and second type coating layers form a quantum energy barrier with respect to the active layer to enable the quantum unit Light is produced by the photoelectric effect. The 4 - electrodes respectively form an ohmic contact with the first and second type cladding layers, and the quantum single S can be supplied with electric energy to cause the quantum unit to generate light. Forming the high-resistance insulating structure in the second type of cladding layer between the imaginary connection of the electrode, and having a high resistivity relative to the second type of cladding layer to cause current to disperse through the activity The path at the time of the layer increases without concentration. Transparent Conductive Layer In addition, the light-emitting diode of the present invention having a high-resistance insulating structure comprises a substrate, at least one quantum unit, an electrode, and a high-resistance insulating structure. The quantum unit is connected to the substrate and from the substrate to the first type of coating layer, an active sound, and both of the layers of the stone layer, and the second type of coating layer, the second type The coating produces light with a photoelectric effect relative to the active layer shape t. 7 mils 4 can be used to connect the transparent conductive layer to the top surface of the substrate, which is opposite to the top surface of the substrate, which can transmit light and uniformly disperse the current. The two electrodes are respectively in contact with the first type of cladding layer, and can be used for the working hours of the first day. Hailizi provides electric energy to make the quantum unit produce light. The high-resistance insulating material is formed downward from the (four) bright conductive layer and located between the 7 1285448 two-electrode imaginary connection, and has high power relative to the transparent conductive layer. The path when the current is dispersed through the active layer is increased without concentration. What is the effect of the invention? a type of cladding layer, and/or a two-flow dispersion path of a high-resistance insulating structure formed downward from the surface of the transparent layer and having a depth less than the active layer, and the hetero-energy band of the quantum element is selected, and the tunneling effect is reduced. The current is not over-concentrated and causes localized areas to ensure the life of the light-emitting diode. money

【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 清楚的呈現。 將可 在本發明被詳細描述之前,要注意的是,在以下的說 月内今中,類似的元件是以相同的編號來表示。 、參閱圖3、圖4,本發明—種具有高阻態絕緣結構之發 光-極體2的-第-較佳實施例,是包含-基材21、至少 :蟲晶形成在該基材21上的量子單元22、二可提供電能的 電極24,及一高阻態絕緣結構3。 /基材21疋由晶格常數與該量子單元22相匹配的材 ;斗構成舉例來說,该量子單元22是屬氮化錄系的半導體 材料時,該基材21貝丨]為易於蠢晶的藍寶石。 該量子單元22自該基材21頂面向上磊晶形成,具有 第型披覆層221、一第二型批覆層222,及一在該第一 、二型批覆層221、222之間的活性層223,該第一、二塑 覆層221 222相對該活性層223形成量子能障而可以光 8 1285448 電效應產生光;該第一、二型披覆層221、222分別為n型 坡覆層與P型披覆層;且,-般為提昇發光效率,均會以 複數量子單元為最佳設計,但在本例與圖示中,為使^明 清楚起見,僅以一量子單元22為例說明。 兄 該二電極24彼此相對遠離地分別設置在該量子單元 =第一型披覆I 221以及該第二型批覆層222上早並^亥2 弟-、二型批覆層221、222相毆姆接觸,而可對 wThe 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 accompanying drawings. 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. 3 and FIG. 4, the present invention - a preferred embodiment of a light-emitting body 2 having a high-resistance insulating structure, comprises a substrate 21, at least: insect crystals are formed on the substrate 21 The upper quantum unit 22, the second electrode 24 for supplying electrical energy, and the high-resistance insulating structure 3. / Substrate 21A is a material whose lattice constant is matched with the quantum unit 22; for example, when the quantum unit 22 is a semiconductor material of a nitride-based system, the substrate 21 is easy to be stupid Crystal sapphire. The quantum unit 22 is epitaxially formed from the top surface of the substrate 21, and has a first cladding layer 221, a second cladding layer 222, and an activity between the first and second cladding layers 221 and 222. The layer 223, the first and second plastic coatings 221 222 form a quantum energy barrier with respect to the active layer 223, and can generate light by the electrical effect of the light 12 1285448; the first and second type cladding layers 221 and 222 are respectively n-type slopes. Layer and P-type cladding layer; and, in order to improve luminous efficiency, the complex number of subunits are optimally designed, but in this example and the illustration, for the sake of clarity, only one quantum unit is used. 22 is an example. The two electrodes 24 are disposed opposite to each other on the quantum unit=first type cladding I 221 and the second type cladding layer 222, respectively, and the second type of coatings 221 and 222 are opposite to each other. Contact, but can be w

元22提供電能使該量子單元22產生光。 Λ里早 該高阻態絕緣結構3形成在該第二型披覆層奶中並 位於該二電極24之假想連線之間,且相 222呈古古〜弟一型批覆層 /、有…率,使得電流是以沿自該高阻態絕緣妹構3 二電極24之假想連線兩端的較長路徑(如圖中 則娩所不)分散通過該量子單元22’進而可 的路徑增加,該量子單元22的異質能階帶増加、穿::應 減少’進而讓電流不致於過度集中而造成局部區域過^ 確保發光二極體2的工作壽命。 ^ 13…、 在本例中,該高阻態絕緣結構3是—自該第二 層222表面向下形成深度在1000A〜70_人之覆 由空氣相對第二型批覆4 222具有高電阻率,曰藉 電流分散的路徑增加的功效;當然,例如更在此二: 填於電阻率相對極高於該第二型批覆 曰 ,或是不先形成凹槽,直接在第二型批^ =阻質材料 置摻雜職濃度、深度的„ l 之對應位 ,也都可以使得電流以如圖中箭號所示之路徑分散= .1285448 虽子單元22,進而可使得電流分散的路徑增加,進而讓電 "丨L不致於過度木中而造成局部區域過熱,確保發光二極體2 的工作奇命。 與習知發光二極體1相似地,當自該二電極24施加電 能時,電流分散流通過該量子單& 22,而使該量子單元22 以光迅效應產生光子,進而使該發光二極體2向外發光。Element 22 provides electrical energy to cause the quantum unit 22 to produce light. The high-resistance insulating structure 3 is formed in the second type of coating layer milk and located between the imaginary lines of the two electrodes 24, and the phase 222 is in the form of a Gu Gu ~ Di-type coating / ... Rate, such that the current is increased along the longer path of the imaginary line connecting the two electrodes 24 from the high resistance state (not shown in the figure) through the quantum unit 22'. The heterogeneous energy level band of the quantum unit 22 is increased and worn: "There should be a reduction in the current, so that the current is not excessively concentrated, causing a local area to pass through ^ to ensure the working life of the light-emitting diode 2. ^ 13... In this example, the high-resistance insulating structure 3 is formed from the surface of the second layer 222 to a depth of 1000A to 70%, and the air is relatively high in resistivity with respect to the second type of cladding 4 222. , the effect of increasing the path by the current dispersion; of course, for example, in the second: filling the resistivity is relatively higher than the second type of coating, or not forming the groove first, directly in the second type ^ = The corresponding position of the doping concentration and depth of the resistive material can also cause the current to be dispersed in the path indicated by the arrow in the figure. .1285448 Although the subunit 22 can further increase the path of current dispersion, In turn, the electricity "丨L is not excessively exposed to the wood, causing local overheating to ensure the working life of the light-emitting diode 2. Similar to the conventional light-emitting diode 1, when electric energy is applied from the two electrodes 24, The current dispersion flow passes through the quantum single & 22, and the quantum unit 22 generates photons by the light fast effect, thereby causing the light emitting diode 2 to emit light outward.

而在電流分散通過的過程中,因為電阻率相對較高於 ▲第-型披覆$ 221的高阻態絕緣結構3的阻播,電流會 以/口自4冋阻悲絕緣結構3相對遠離該二電極之假想連 線的兩端,而相對該二電極24之假想連線較為長的路徑分 散通過該活性層223,也因此電流不致於過度集中而造成局 部區域過熱,而可確保發光二極體2的工作壽命。 參閱圖5、ϋ 6,本發明一種具有高阻態絕緣結構之發 光二極體2,的一第二較佳實施例,是包含一基材21、至少 一蟲晶形成在該基材21上的量子單a 22、一形成在該量子 單元22頂面的透明導電層4、二可提供電能的電極24,及 一高阻態絕緣結構3。 該基材21《由晶格常數與該量子單元22相匹配的材 料構成,舉例來說,該量子單元22是屬氮化鎵系的半導體 材料時,該基材21則為易於磊晶的藍寶石。 該量子單元22自該基材21頂面向上蟲晶形成,具有 -第-型披覆層221、一第二型批覆層222,及一在該第一 -型批復層221、222之間的活性層223,該第一、二型 披覆層221、222相對該活性層223形成量子能障而可以光 10 1285448 電效應產生光;該第一、二型彼覆層221、222分別為n型 披覆層與p型披覆層,且,一般為提昇發光效率,均會以 複數量子單元為最佳設計,但在本例與圖示中,為使說明 清楚起見,僅以一量子單元22為例說明。 該透明導電層4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In the process of current dispersion, because the resistivity is relatively higher than that of the high-resistance insulating structure 3 of the ▲-type cladding $221, the current will be relatively far from the 4 冋 悲 绝缘 3 The two ends of the imaginary connection of the two electrodes are separated from the active layer 223 by a relatively long path with respect to the imaginary connection of the two electrodes 24, so that the current is not excessively concentrated and the local area is overheated, thereby ensuring the light emission. The working life of the polar body 2. Referring to FIG. 5 and FIG. 6, a second preferred embodiment of a light-emitting diode 2 having a high-resistance insulating structure comprises a substrate 21 on which at least one crystallite is formed. The quantum single a 22, a transparent conductive layer 4 formed on the top surface of the quantum unit 22, two electrodes 24 for supplying electrical energy, and a high-resistance insulating structure 3. The substrate 21 is composed of a material whose lattice constant matches the quantum unit 22. For example, when the quantum unit 22 is a gallium nitride-based semiconductor material, the substrate 21 is a sapphire which is easy to be epitaxial. . The quantum unit 22 is formed from the top surface of the substrate 21 and has a --type cladding layer 221, a second-type cladding layer 222, and a first-type batch layer 221, 222. The active layer 223, the first and second type cladding layers 221, 222 form a quantum energy barrier with respect to the active layer 223, and can generate light by the electrical effect of the light 10 1285448; the first and second type cladding layers 221, 222 are respectively n The type of cladding layer and the p-type cladding layer, and generally, to improve the luminous efficiency, the plurality of subunits are optimally designed, but in this example and the illustration, for the sake of clarity, only one quantum is used. Unit 22 is taken as an example. The transparent conductive layer 4 is made of a material that can transmit light and has a uniform current dispersion, such as indium tin oxide (known in the industry as ITO), and can be used as an electrode.

24施加電能時,電流均勻地流通過該量子單元22而提昇發 光效率。 該二電極24彼此相對遠離地分別設置在該量子單元22 的第一型披覆層221以及該透明導電層4上,並與該第一 型批覆層221與該透明導電層4相毆姆接觸,而可對該量 子單元22提供電能使該量子單元22產生光。 該向阻態絕緣結構3自該透明導電 曰1丨~卜彤成,深 又在1000A 70000A,並位於該二電極24之假想連線之間 ,時㈣該透明導電層4、第二型批覆層222具有高電阻 率’使付電流是以沿自該高阻態絕緣結構3相對遠離該二 電極24之假想連線兩端的較長路徑(如圖中箭號所示)分 政通過該量子單元22’進而可使得電流分散的路徑增加, =子單元22的異質能階帶增加、穿随效應減少,進而讓 弘机不致於過度集中而造# 體2的工作壽命。…部區域過熱,確保發光二極 在本例中,該高阻態絶 ^ . 緣、、、〇構3疋一自該透明導雷矣 面向下形成並深入至該第二 逍3 ¥包表 ^ , t抵覆層222的凹槽,Μ由* 乳相對該透明導電層4、繁— 猎工 力〜型批覆層222具有高電阻率, 1285448 而達到使得電流分散的路徑增加的功效;當然,例如更在 此凹槽中容填電阻率相對極高於該透明導電層4、第二型批 伋s 222的问阻質材料,或是不形成凹槽而直接摻雜預定 濃度、深度的雜質已形成此等高阻態絕緣結構,也都可以 使得私分散的路徑增加,進而讓電流不致於過度集中而 造成局部區域過熱,確保發光二極體2的工作壽命。When electrical energy is applied 24, current flows uniformly through the quantum unit 22 to enhance the luminous efficiency. The two electrodes 24 are respectively disposed on the first type of cladding layer 221 of the quantum unit 22 and the transparent conductive layer 4, and are in contact with the transparent layer 4 and the transparent conductive layer 4 The quantum unit 22 can be supplied with electrical energy to cause the quantum unit 22 to generate light. The transparent conductive layer 3 is formed from the transparent conductive layer 1 , and is deeper at 1000A 70000 A, and is located between the imaginary lines of the two electrodes 24, and (4) the transparent conductive layer 4 and the second type of cladding layer 222. Having a high resistivity 'the current is passed through the quantum unit 22 along a longer path (shown by an arrow in the figure) along the imaginary line from the high-resistance insulating structure 3 relatively far from the two electrodes 24 'In turn, the path of current dispersion is increased, and the heterogeneous energy level band of the subunit 22 is increased, and the wear-through effect is reduced, so that the Hong machine is not excessively concentrated to create the working life of the body 2. The area of the ... is overheated, ensuring that the light-emitting diode is in this example, and the high-resistance state is formed. The edge, the 〇 structure, the 〇 疋 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自 自^, t the groove of the cladding layer 222, the thickness of the current dispersion path is achieved by the *milk relative to the transparent conductive layer 4, the complex-type cladding layer 222 having a high resistivity, 1285448; For example, in the groove, the resistivity is relatively higher than that of the transparent conductive layer 4 and the second type of 汲 s 222, or is directly doped with a predetermined concentration and depth without forming a groove. Impurities have formed such high-resistance insulating structures, which can also increase the privately dispersed path, thereby preventing the current from being excessively concentrated and causing local area overheating, and ensuring the working life of the light-emitting diode 2.

此外,該高阻態絕緣結構3的深度可以僅位於該透明 ^私層4中,或是更向下深入至該第二型批覆層22,但無 論深度為何,均不可接觸該活性層⑵,以免造成短路使得 發光二極體2成為廢品。 一上例相似,當自该二電極24施加電能時,電流經過 該透明導電層4分散流通過該量子單元22,而使該量子單 疋22以光電效應產生光子,進而使該發光二極體2向外發 光;而在電流分散通過中,因為高阻態絕緣結才冓3的阻絕 ,可使電流以沿自該高阻態絕緣結構3相對遠離該二電極 Μ之假想連線的兩端分散通過該活性| 223,而使得電流 不致於過度集中而造成局部區域過熱,確保發光二極體2 的工作壽命。 综上述說明可知’本發明發光二極體2是以相對該第 二型披覆層222,及/或該透明導電層4具有高電阻率 阻態絕緣結構3’使得當以電極24施加電能時,電流是以 :自該高阻態絕緣結構3 _遠離二電極2 4之假想連線兩 端的較長路徑分散通過,進而佬 — 册 ^ 運而使侍里子早兀22的異質能階 可曰口、牙陡效應減少’並可使得電荷密度分配均勻,電 12In addition, the depth of the high-resistance insulating structure 3 may be located only in the transparent transparent layer 4 or deeper down to the second-type cladding layer 22, but the active layer (2) may not be contacted regardless of the depth. In order to avoid a short circuit, the light-emitting diode 2 becomes a waste product. Similarly, in the above example, when electric energy is applied from the two electrodes 24, a current flows through the transparent conductive layer 4 through the quantum unit 22, so that the quantum unit 22 generates photons by photoelectric effect, thereby causing the light-emitting diode. 2 illuminating outward; and in the current dispersion, because the high-resistance insulating junction is blocked by the 冓3, the current can be made at both ends of the imaginary connection from the high-resistance insulating structure 3 relatively far from the two-electrode Μ Dispersing through the activity | 223, so that the current is not excessively concentrated, causing local area overheating, ensuring the working life of the light-emitting diode 2. In view of the above description, it can be seen that the light-emitting diode 2 of the present invention is opposite to the second-type cladding layer 222, and/or the transparent conductive layer 4 has a high-resistivity resistive insulating structure 3' such that when electric energy is applied by the electrode 24. The current is: a long path from the two ends of the imaginary connection of the high-resistance insulating structure 3 _ away from the two electrodes 24, and then the heterogeneous energy level of the waiter is as early as 22 The mouth and tooth steepness effect is reduced' and the charge density can be evenly distributed.

1285448 流不致於過度集中於转宗p 0 r^ ^ 韦R特疋£域,確實可以改善習知 極體1電流會相對較集中於電極14的、 x - 4 一電極14的1285448 The flow does not over-concentrate on the recursive p 0 r^ ^ Wei R special field, which can improve the conventional polar body 1 current will be relatively concentrated on the electrode 14, x - 4 electrode 14

假想連線等處,而導致部分區域過熱,進而縮短卫作μ 的缺點,確實達到本發明的創作目的。 ! °P 惟以上所述者,僅為本發明之較佳實施例而已,當 能以此限定本發明實施之範圍,即大凡依本發明中^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,說明一習知的發光二極體; 圖2是一俯視圖,辅助說明圖丨之發光二極體; 圖3是一剖視示意圖,說明本發明具有高阻態絕緣結 構之發光二極體的一第一較佳實施例; 圖4是一俯視圖,輔助說明圖3之發光二極體; 圖5是一剖視不意圖,說明本發明具有高阻態絕緣結 構之發光二極體的一第二較佳實施例;及 圖6是一俯視圖,輔助說明圖5之發光二極體。 13 1285448Imaginary connection, etc., which leads to overheating of some areas, thereby shortening the shortcomings of the maintenance μ, and indeed achieves the creative purpose of the present invention. ! The above is only the preferred embodiment of the present invention, and the scope of the present invention can be limited thereto, that is, the simple equivalent change according to the scope of the present invention and the description of the invention. And modifications: are still within the scope of the invention patent. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a cross-sectional view showing a conventional light-emitting diode; FIG. 2 is a plan view for explaining the light-emitting diode of FIG. 3; FIG. 3 is a cross-sectional view showing the present A first preferred embodiment of the invention discloses a light-emitting diode having a high-resistance insulating structure; FIG. 4 is a plan view for explaining the light-emitting diode of FIG. 3; FIG. 5 is a cross-sectional view showing the present invention. A second preferred embodiment of a light-emitting diode of a high-resistance insulating structure; and FIG. 6 is a top view of the light-emitting diode of FIG. 13 1285448

【主要元件符號說明】 1 發光二極體 21 基材 11 基材 22 量子單元 12 量子單元 221 第一型批覆層 121 第一型批覆層 222 第二型批覆層 122 第二型批覆層 223 活性層 123 活性層 24 電極 13 透明導電層 3 高阻態絕緣結構 14 電極 4 透明導電層 2 發光二極體[Main component symbol description] 1 Light-emitting diode 21 Substrate 11 Substrate 22 Quantum unit 12 Quantum unit 221 First-type cladding layer 121 First-type cladding layer 222 Second-type cladding layer 122 Second-type cladding layer 223 Active layer 123 active layer 24 electrode 13 transparent conductive layer 3 high resistance insulating structure 14 electrode 4 transparent conductive layer 2 light emitting diode

1414

Claims (1)

1285448 十、申請專利範圍: 1 · 一種具有高阻態絕緣結構之發光二極體,包含: 一基材; 至少一量子單元’與該基材連接並自該基材向上依 序具有一第一型披覆層、一活性層,及一第二型批覆層 ,該第一、二型披覆層相對該活性層形成量子能障而可 使該量子單元以光電效應產生光; 二電極,分別與該第一、二型批覆層形成歐姆接觸 而了對5亥里子單元提供電能而使該量子單元產生光; —阿丨儿思犯涿苑稱,形成在該第二型披覆層中並位 於該二電極假想連線之間,且相對該第二型批覆層具有 南電阻率而使電流分散通過該活性層時的路徑增加而不 集中。 2.依據申請專利範圍第,項所述之具有高阻態絕緣結構之 發光一極體’其中,該高阻態絕緣結構包括一自該第二 型批覆層表面向下形成且深度在麵A〜7G_A之間的 凹槽。 3· t射請專利範圍第1項所述之具有高阻態絕緣結構之 I:先一極體’其中,該高阻態絕緣結構包括一自該第二 型批覆層表面向下形成且、、吨 成且/衣度在1000A〜70000人之間的 凹槽,及一容填於該凹柃由 萝感认古 曰中龟阻率相對極高於該第二蜇 批覆層的面阻質材料。 4.反據申請專利範圍第i項 疋之具有鬲阻恶絕緣結構之 15 1285448 發光一極體’其中’該高阻態絕緣結構是自該第二型批 覆層表面向下摻雜預定濃度之雜質且深度在 1000人〜70000A之間構成。 一種具有高阻態絕緣結構之發光二極體,包含: 一基材; 至少一量子單元,與該基材連接並自該基材向上依 序具有一第一型彼覆層、一活性層,及一第二型批覆層1285448 X. Patent application scope: 1 · A light-emitting diode having a high-resistance insulating structure, comprising: a substrate; at least one quantum unit 'connected to the substrate and sequentially having a first from the substrate a coating layer, an active layer, and a second type of cladding layer, the first and second type cladding layers form a quantum energy barrier with respect to the active layer to enable the quantum unit to generate light by a photoelectric effect; Forming an ohmic contact with the first and second type of cladding layers and supplying power to the 5 mile subunit to cause the quantum unit to generate light; - Auntie thinks that the formation is in the second type of cladding layer and Located between the two electrode imaginary wires, and having a south resistivity relative to the second type of cladding layer, the path when the current is dispersed through the active layer is increased and not concentrated. 2. The light-emitting diode of the high-resistance insulating structure according to the scope of the patent application, wherein the high-resistance insulating structure comprises a surface formed downward from the surface of the second-type cladding layer and having a depth in the surface A The groove between ~7G_A. The present invention has a high-resistance insulating structure I: a first-pole body, wherein the high-resistance insulating structure includes a surface formed downward from the surface of the second-type cladding layer, a groove of between 1000A and 70,000 people, and a cavity filled with the surface resistivity of the second layer of the coating. material. 4. In accordance with the scope of the patent application, item i, 15, 1585448, a light-emitting one, wherein the high-resistance insulating structure is doped downward from the surface of the second type of cladding layer by a predetermined concentration Impurities and a depth of between 1,000 and 70000 A. A light-emitting diode having a high-resistance insulating structure, comprising: a substrate; at least one quantum unit connected to the substrate and sequentially having a first type of cladding layer and an active layer from the substrate And a second type of coating ,该第一、二型披覆層相對該活性層形成量子能障而可 使該量子單元以光電效應產生光;- 一透明導電層,連接在該量子單元相反於與該基材 連接的頂面上,是可透光且可使電流均勻分散·, 導電層相 子單元產 一電極,分別與該第一型批覆層與該透明 歐姆接_,而可對該量子單元提供電能使該量 生光;及The first and second type cladding layers form a quantum energy barrier with respect to the active layer to enable the quantum unit to generate light by a photoelectric effect; a transparent conductive layer connected to the top of the quantum unit opposite to the substrate On the surface, the light is permeable and the current can be uniformly dispersed. The conductive layer phase sub-unit produces an electrode, and the first type of cladding layer and the transparent ohmic connection respectively, and the quantum unit can be supplied with electric energy to make the quantity Raw light; and 一鬲阻態絕緣結構,自 於該二電極假想連線之間, 電阻率而使電流分散通過該 中0 該透明導電層向下形成並位 且相對該透明導電層具有高 活性層時的路徑增加而不集 6. 依據申請專利範圍第 發光二極體,其中, 導電層表面向下形成 槽。— 5項所述之具有高阻態絕緣結構之 向阻態矣巴緣結構包括一自該透明 且深度在1000A〜70000A之間的凹a barrier state insulating structure, wherein a current is dispersed from the imaginary connection between the two electrodes, and the current is dispersed through the middle 0. The transparent conductive layer is formed downward and has a high active layer with respect to the transparent conductive layer. Addition and not set 6. According to the patent application range, the light-emitting diodes, wherein the surface of the conductive layer forms a groove downward. - The high-resistance insulating structure having a high-resistance insulating structure includes a concave from the transparent and having a depth of between 1000A and 70,000A. 依據申請專利範圍第 發光二極體,其中, 5項所述之具有高阻態絕緣結構之 該高阻態絕緣結構包括—自該透明 16 1285448 導電層表面向下形成且深度在ΙΟΟΟΑ〜70000人之間的凹 槽,及一容填於該凹槽中電阻率相對極高於該該透明導 電層的高阻質材料。According to the patent application scope, the light-emitting diode, wherein the high-resistance insulating structure having the high-resistance insulating structure includes: - the surface of the conductive layer formed from the transparent 16 1285448 is formed downward and the depth is ΙΟΟΟΑ~70000 A groove between the groove and a high-resistance material having a resistivity relatively higher than that of the transparent conductive layer. 1717
TW95108574A 2006-03-14 2006-03-14 Light-emitting diode with high resistivity insulation structure TWI285448B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
TW95108574A TWI285448B (en) 2006-03-14 2006-03-14 Light-emitting diode with high resistivity insulation structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
TW95108574A TWI285448B (en) 2006-03-14 2006-03-14 Light-emitting diode with high resistivity insulation structure

Publications (2)

Publication Number Publication Date
TWI285448B true TWI285448B (en) 2007-08-11
TW200735405A TW200735405A (en) 2007-09-16

Family

ID=39456726

Family Applications (1)

Application Number Title Priority Date Filing Date
TW95108574A TWI285448B (en) 2006-03-14 2006-03-14 Light-emitting diode with high resistivity insulation structure

Country Status (1)

Country Link
TW (1) TWI285448B (en)

Also Published As

Publication number Publication date
TW200735405A (en) 2007-09-16

Similar Documents

Publication Publication Date Title
TWI527261B (en) Light-emitting device
US9673355B2 (en) Light emitting diode having electrode pads
US9356213B2 (en) Manufacturing method of a light-emitting device having a patterned substrate
TWI470824B (en) Electrode structure and light-emitting device using the same
CN102315239B (en) Photoelectric cell
CN105895763A (en) Light-Emitting Diode Chip
US20150108492A1 (en) Light-emitting diode
US20080296595A1 (en) Light emitting diode with high illumination
TWI702737B (en) Light-emitting diode device
CN111048639B (en) Front-mounted integrated unit light-emitting diode
TW201205879A (en) Light emitting device
EP2590234A1 (en) Solid state light emitting semiconductor device
TWI285448B (en) Light-emitting diode with high resistivity insulation structure
TWM436224U (en)
TWI284995B (en) Light emitting diode
KR20140037500A (en) A semiconductor light emitting diode
KR101547322B1 (en) Light emitting diode package
CN109449263A (en) A kind of light emitting diode and preparation method thereof
CN105140369B (en) Light emitting diode structure
TWI610464B (en) Light emitting diode structure
JP2004228297A (en) Semiconductor light emitting device
CN107431105A (en) Luminescent device with reflector and top contact
CN105244426A (en) Structure capable of preventing light-emitting diode from being broken down by reverse voltage and manufacturing method thereof
TWI289946B (en) LED with current-limiting layer
TW517399B (en) Light emitting diode with transparent substrate

Legal Events

Date Code Title Description
MM4A Annulment or lapse of patent due to non-payment of fees