TWI224872B - White light-emitting diode and its manufacturing method - Google Patents

White light-emitting diode and its manufacturing method Download PDF

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TWI224872B
TWI224872B TW92105775A TW92105775A TWI224872B TW I224872 B TWI224872 B TW I224872B TW 92105775 A TW92105775 A TW 92105775A TW 92105775 A TW92105775 A TW 92105775A TW I224872 B TWI224872 B TW I224872B
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light
layer
emitting
emitting portion
buffer layer
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TW92105775A
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TW200419819A (en
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Mu-Ren Lai
Jia-Cheng Liou
Jiung-Yu Jang
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Vtera Technology Inc
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Abstract

A kind of white light-emitting diode (LED) and its manufacturing method are disclosed in the present invention. The diode contains the first conducting electrode, a substrate, the first light-emitting part, two buffering layer regions (BxGa1-xP and InxGa1-xN) with gradient variations, the second light-emitting part and the second conducting electrode. When an external voltage difference is added between the second conducting electrode and the first conducting electrode, a current is generated to flow through the second light emitting part, the buffering layer region and the first light-emitting part such that the active layer of the first light-emitting part emits light within the first wavelength range and the second active layer of the second light-emitting part emits light within the second wavelength range. By mixing light within the first wavelength range together with light within the second wavelength range, white light can be obtained.

Description

12248721224872

【發明所屬之技術領域】 本發明係有 4主口丨# •工θ %赏无二極體及其萝作士 4, 特別猎由二層呈梯度變化之 r 、衣作方法 '^緩衝層區(BY G a】P ;5 了 n r λΤ Ν 传以將黃光二極體及藍光二極體可-次完‘以 【先前技術】 & 發光二極體(Light Emitting M〇de,UD) :的半導體元件1用電流通過時二極體内: =(分別為帶負電的電子與帶正電的電洞)之相上個: 月<3 Ϊ以光的形式釋放。由於只要在發 二。將 :極小電流之便可發光,且屬於冷;發;,不 絲燈,熱發光原i,具有亮度高、體積小、耗電::鑛 發熱量少和壽命長等優點。 里小 傳統發光二極體的發光特性皆以單一主波峰 peak wavelength)及狹窄半高寬(fuU width 〇f〔lgnle maxim·,FWHM)為訴求,所以發光二極體所發射的比 是很純的單一顏色光,例如砷化鋁鎵發光二極體發f線白 光、磷化鎵發光二極體發綠色光。另外,透 4、、工色 材料糸統,或同一材料系統但不同組成比例,π㈤> N __ 4 1製作出不 同顏色不同亮度的發光二極體,例如調變磷砷 之鱗和坤的組成比,或填化鋁鎵銦中之鋁、键 ’ , 緣和銦的組成 比,皆可製作涵蓋紅、黃、綠三色的高亮度發一 ^ 極 。 上述各種材料所組成及選用的結構和製作方法 光二極體均只發出很純(半高寬很窄)的單色光 ^ 、早一主波[Technical field to which the invention belongs] The present invention has 4 main ports 丨 # θ θ% reward diode and its masterpiece 4, especially hunting for the r, clothing method with a gradient change from the two layers' ^ buffer layer Area (BY G a) P; 5 nr λΤ Ν pass to the yellow light diode and blue light diode can be-times finished 'with [prior art] & Light Emitting Mould (UD) : When the semiconductor element 1 is passed by a current: = (respectively negatively charged electrons and positively charged holes) The phase of the previous: Month < 3 Ϊ is released in the form of light. 2. Will: Light can be emitted with very small current, and belongs to cold; hair ;, non-filament lamp, thermal luminescence i, has the advantages of high brightness, small size, power consumption: less heat generation and long life of the mine. The luminous characteristics of traditional light-emitting diodes are based on a single main peak peak wavelength and a narrow half-width-of-height (fuU width 0f (lgnle maxim ·, FWHM)). Therefore, the ratio emitted by the light-emitting diode is a very pure single Color light, such as f-line white light from aluminum gallium arsenide light emitting diode, green light from gallium phosphide light emitting diodeIn addition, through the 4, color system, or the same material system but different composition ratios, π㈤> N _ 4 1 to produce light-emitting diodes with different colors and different brightness, such as the composition of the scale of phosphorous and arsenic and kun Ratio, or the composition ratio of aluminum, bonds', edges and indium in AlGaIn, can produce high-brightness electrodes covering red, yellow, and green. The composition and the selected structure and manufacturing method of the above materials The photodiodes emit only pure monochromatic light (half-width-height and narrow-width) ^, one main wave earlier

0769-9102TWF(nl) ; VTERA-91-010-TW ; Phoelip.ptd 12248720769-9102TWF (nl); VTERA-91-010-TW; Phoelip.ptd 1224872

自從發光二極體發明迄今以來,人們一直在 以ί光二極體作為照明光源,隨著發光二極體製造 不断進步和新型材料的開發及應肖,尤其是白:術的 體的出現,使得發光二極體應用領域逐漸跨足至極 ^體具有體積小(多顆、多種組合)、發熱量=先二 :上)耗=、,、低電流起動)、壽命長(1^ ^ / Λ (可在高頻操作)、環保(耐震、耐衝擊 :)可平面::回:’沒有污染,有[綠色照明光源]之 有白熾燈泡之缺點(高耗電、易碎及曰光燈 iV疋大被Λ界二好在未來10年内’成為替代傳統照明器 具的一大潛力商品。 f白光發光二極體的製成技術中,主要係利用顏色的 s來達到形成白光的效果,以人類眼睛所能見的白光形 式至少須兩種光之混合,例如組合單色的黃光和薛光, 過調整發光強度的比例’混合此二種色光達到形成白光的 效果;也可由組合紅光、綠光和藍光,透過調整發光強度 的比例,混合此三種色光達到白光的效果。 在上述白光發光二極體 (黃光和藍光),係在藍光晶 (yttrium aluminum garnet 體激發乙鋁石榴石螢光粉, 的製作技術中,二波長混合光 粒上塗一層乙鋁石榴石螢光粉 ,YAG) ’利用藍光發光二極 以產生與藍光互補的黃光,再Since the invention of light-emitting diodes so far, people have been using light-emitting diodes as illumination light sources. With the continuous progress of light-emitting diode manufacturing and the development of new materials and applications, especially the emergence of the white body, the The application field of light-emitting diodes gradually reaches to the limit. The body has a small volume (multiple pieces, multiple combinations), calorific value = first two: upper) power consumption =, ,, low current start), long life (1 ^ ^ / Λ ( Can operate at high frequency), environmental protection (vibration resistance, shock resistance :) can be flat :: back: 'no pollution, there are the disadvantages of incandescent light bulbs with [green lighting light source] (high power consumption, fragile and iV 疋) In the next 10 years, it will become a great commodity to replace traditional lighting appliances. F White light emitting diode manufacturing technology mainly uses the color s to achieve the effect of forming white light to the human eye. The visible white light form must be mixed with at least two kinds of light, for example, a combination of monochromatic yellow light and Xue light. By adjusting the ratio of the luminous intensity, 'mixing the two color lights can achieve the effect of forming white light; it can also be combined by red light and green light. And blue light, through Adjust the ratio of luminous intensity and mix the three colors to achieve the effect of white light. In the above-mentioned white light emitting diodes (yellow light and blue light), the production technology of blue aluminum crystal (yttrium aluminum garnet) excites the aluminum aluminum garnet phosphor, The two-wavelength mixed light particles are coated with a layer of aluminum aluminum garnet fluorescent powder (YAG) 'Using a blue light emitting diode to generate a yellow light complementary to the blue light, and then

1224872 五、發明說明(3) 利用透鏡原理,將互補的黃光和藍光予以混合,得到所需 的白光。請參照第1圖,係顯示此白光發光二極體之結構 剖面圖,該白色發光二極體燈泡是利用一顆氮化鎵藍色發 光二極體晶粒12和YAG螢光材料14組合而成,發光二極體 晶粒12具有一陰極及一陽極在其表面,發光二極體晶粒12 置於金屬接腳13上之凹槽(cavity)17*,並將發光二極體 晶粒1 2之二表面電極分別連接至金屬接腳丨3及金屬接腳 15,再以螢光材料14覆蓋填充金屬接腳13上的凹槽17中, 最後再以封裝材料1 6將整個晶粒丨2連同金屬接腳丨3、丨5的 端部封裝固定。 當電流從負極流至正極時,氮化鎵發光二極體晶粒12 發出波長接近460nra的藍光。一部分的藍光通過YAG螢光材 料14至外部,而其他留滯在YAG螢光材料14的藍光則被 YAG螢光材料14所吸收,進一步轉換成具較長波長(55〇nm) 的黃光。由YAG螢光材料14所發出的黃光(螢光)及氮化鎵 發光二極體晶粒1 2所發出的藍光自然的混合而產生白光, 請參照第2圖’係顯示此白光發光二極體之發光示意圖。 雖然利用氮化鍊發光二極體加γ A g螢光材料可以達到產生 白光的目的,不過這樣的作法有幾項缺點存在。首先便是 由於藉由YAG吸收藍光使之轉換成黃光,部分能量被YAG吸 收而未轉換成光,使得氮化鎵加上YAG的二極體結構其外 部量子效率由原本氮化鎵發光二極體的5%左右,下降為3〇/〇 左右’連V降低發光效率及亮度。且由於YAG的轉換效'''率 約1 0%,如此低的效率若欲維持黃光與藍光的比例以求1224872 V. Description of the invention (3) Using the principle of lens, the complementary yellow light and blue light are mixed to obtain the required white light. Please refer to FIG. 1, which is a cross-sectional view showing the structure of the white light emitting diode. The white light emitting diode bulb is a combination of a gallium nitride blue light emitting diode grain 12 and a YAG fluorescent material 14. The light-emitting diode crystal grains 12 have a cathode and an anode on its surface, the light-emitting diode crystal grains 12 are placed in a cavity 17 * on the metal pin 13, and the light-emitting diode crystal grains 12 are formed. 1 2 bis The surface electrodes are connected to the metal pins 3 and 15 respectively, and then the fluorescent material 14 is used to fill the grooves 17 on the metal pins 13 and finally the entire die is filled with the packaging material 16丨 2 and the metal pins 丨 3, 丨 5 are packaged and fixed at the ends. When a current flows from the negative electrode to the positive electrode, the gallium nitride light emitting diode crystal 12 emits blue light with a wavelength close to 460 nra. A part of the blue light passes through the YAG fluorescent material 14 to the outside, while the other blue light remaining in the YAG fluorescent material 14 is absorbed by the YAG fluorescent material 14 and is further converted into a yellow light with a longer wavelength (55 nm). The yellow light (fluorescence) emitted by the YAG fluorescent material 14 and the blue light emitted by the gallium nitride light emitting diode grains 12 are naturally mixed to generate white light. Please refer to FIG. 2 to show the white light emitting two Schematic diagram of the polar body. Although the use of nitrided chain light-emitting diodes and γ A g fluorescent materials can achieve the purpose of generating white light, there are several disadvantages to this approach. The first is that because YAG absorbs blue light and converts it to yellow light, part of the energy is absorbed by YAG but not converted to light, so that the external quantum efficiency of the diode structure of gallium nitride plus YAG is changed from the original About 5% of the polar body is reduced to about 30/0. Even V reduces the luminous efficiency and brightness. And because the conversion efficiency of YAG is about 10%, such a low efficiency is necessary to maintain the ratio of yellow light to blue light.

0769-9102TWF(nl) ; VTERA-91-010-TW ; Phoelip.ptd 第7頁 12248720769-9102TWF (nl); VTERA-91-010-TW; Phoelip.ptd Page 7 1224872

螢=所需白光’YAG螢光材料的組成勢必增力σ,導致yag =料厚度變厚,而厚的YAG螢光材料層將降低元件發 亮度,使外部量子效率更差。且營光粉本身有 二二〇lfe time)衰退的缺點,導致發光色溫隨著使用時 :“口而不易控制’將造成產品使用一定年限後產生色 因而此種白色發光二極體的壽命也相對地受到了限 相較於上述單晶片(Singie chip)型的白光發光二極 另種f曰日片(随11:1 chlp )白光發光二極體則是將 :::、藍三種發光二極體形成同一元件,利用三原色混 :士產生白光。這種方式由於紅、、綠、藍三種發光二極體 :、半導體材質彼此差異極大’因此驅動電路的設計也變得 =為煩瑣複雜,因為若有三顆晶片,就必須針對三 =阻、電壓等加以㈣,因此量產將受到極大限制。且 务出紅、綠、藍之三種發光層其個別發光效率不易匹配, 故f不易形成高效率之白光發光二極體。t因為三顆晶片 的哀減速率不ί§] ’使用一段時間後將產生色偏,使光的品 貝變差,因此採用單晶片(single chip)方式較多晶片 (raulti chip)來的可行。 一種利用紫外光發光二極體(uv LED)激發之白 二極體也被提出來。由於紫外線(uv)發光二極體元:豆 外部量子效率可超過20%以上,若以此來激發三波長螢牛光、 體,便可得到高效率的白光發光二極體。纟由於紫光 的能量極南,且紫外光易使封製材料(塑膠)變質及螢光粉Fluorescence = required white light ’The composition of the YAG fluorescent material is bound to increase σ, resulting in a thick yag = material, and a thick layer of YAG fluorescent material will reduce the brightness of the device and make external quantum efficiency worse. And the camping powder itself has a disadvantage of 220fe time), which causes the color temperature of the light to be emitted with the use of: "It is not easy to control the mouth" will cause the product to produce color after a certain number of years of use, so the life of this white light emitting diode Relatively limited, compared to the single-chip (Singie chip) type white light-emitting diode, the other f is a Japanese film (with 11: 1 chlp), and the white light-emitting diode is: The polar body forms the same element, and the three primary colors are mixed: the white light is generated. In this way, the red, green, and blue light-emitting diodes: and semiconductor materials are very different from each other. Therefore, the design of the driving circuit also becomes cumbersome and complicated. Because if there are three chips, it must be targeted for three resistors, voltage, etc., so mass production will be greatly limited. And the three light-emitting layers of red, green, and blue cannot easily match the individual luminous efficiency, so f is not easy to form high. The efficiency of white light-emitting diodes. Because the deceleration rate of the three chips is not used, the color shift will occur after a period of use, which will worsen the light quality of the light, so the single chip method is more suitable. It is feasible to use a faulti chip. A white diode using ultraviolet light emitting diode (uv LED) excitation is also proposed. Due to the ultraviolet (uv) light emitting diode element: the external quantum efficiency of the bean can exceed 20 % Or more, if this is used to excite the three-wavelength fluorescent light and body, a high-efficiency white light-emitting diode can be obtained. 纟 Because the energy of purple light is extremely south, and ultraviolet light is likely to deteriorate the sealing material (plastic) and fluorescein Light powder

12248721224872

五、發明說明(5) 劣化等問題,使得此種元件使用壽命大幅降低。 而在美國專利第6, 33 7, 536號中也揭露出一種利用石西 化辞(ZnSe)為基板之白光發光二極體,請參照第3圖,係 顯示此白光發光二極體之結構剖面圖。其利用包含碼化^ 與2111^0(1^86之多層結構發出藍光,來激發石西化鋅基板之又 光中心而產生黃光,混合後獲得白色光,請參照圖,安 係顯示此白光發光二極體之發光示意圖。但是其利用石西化 鋅基板吸收來至發光層所發出的光而由硒化辞基板激發出 另一固疋顏色的光,故其不易組合成適當色溫之白光發光 二極體,且其發光效率較一般二極體產品來的低,產品壽 命也需進一步改善。 一 口口可 【發明内容】 有鑑於此,本發明另提供一種白光發光二極體及其身 作方法,藉由一層呈梯度變化之缓衝層區(& g七p及 InxGa^N)將其具有兩個發光部分於一單晶片(s chip)上,且可一次完成長晶動作,各自發出藍光及黃 光,在自然混合後可獲致白光,可免除上述習知之白光每 光二極體其壽命較短、結構複雜及發光效率不佳等問題1 且藍光及育光為各別發光,使發光效率更易匹配。 本發明所提供一種白光發光二極體及其製作方法,肩 由二層呈梯度變化之緩衝層區(BxGaixP&InxGa^N):可於1 不同之基底上形成白光發光二極體,有別於 二極體只能在固定基底形成之技術’且可利;V. Description of the invention (5) Problems such as deterioration have significantly reduced the service life of such components. In US Patent No. 6, 33 7, 536, a white light-emitting diode using ZnSe as a substrate is also disclosed. Please refer to FIG. 3, which shows a structural cross-section of the white light-emitting diode. Illustration. It uses a multilayer structure containing coded ^ and 2111 ^ 0 (1 ^ 86 to emit blue light to excite the light center of a petrified zinc substrate to generate yellow light. After mixing, white light is obtained. Please refer to the figure. The white light is shown in the system Schematic diagram of the light-emitting diode. However, it uses the silicon substrate to absorb light emitted from the light-emitting layer and excites another solid-colored light from the selenide substrate, so it is not easy to combine it into white light with an appropriate color temperature. Diode, and its luminous efficiency is lower than that of ordinary diode products, and the product life also needs to be further improved. In one mouth, it can be described [Summary of the Invention] In view of this, the present invention further provides a white light emitting diode and its body Method, with a buffer layer region (& g7p and InxGa ^ N) with a gradient change, it has two light-emitting parts on a single chip (s chip), and can complete the growth of the crystal at one time, each It emits blue light and yellow light, and can get white light after natural mixing, which can avoid the conventional white light. Each light diode has short life, complex structure, and poor luminous efficiency. 1 And blue light and light are separately emitted. The luminous efficiency is easier to match. The present invention provides a white light emitting diode and a manufacturing method thereof. The shoulder layer consists of two buffer layers (BxGaixP & InxGa ^ N) with gradient changes: white light emitting diodes can be formed on different substrates. Polar body is different from the technology that diode can only be formed on a fixed substrate.

1224872 五、發明說明(6) 降低二極體元件中各磊晶層之間的晶袼不匹配(丨a 11丨⑶ mismatch),使各磊晶層之間的晶格更加匹配,以降低二 極體元件中之線缺陷,提供具完美結晶度之白光發光二極 體。 為獲致上述之目的,本發明所述之白光發光二極體, 分、至少二層呈梯度變化之 、一第二發光部分及一第二 第一導電性電極形成電接觸 缚層、一第一發光部分活性 缚層依序形成於上述基底上 缓衝層區形成於上述第一發 緩衝層區係由一層或一層以 部分中之第一型束縛層、活 於上述缓衝層區上。第二導 第二型束缚層形成電接觸。 當外加一電位差於第二 電極之間時,產生一電流, 緩衝層區、及一第一發光部 發出第一波長範圍之光線、 二波長範圍之光線,利用此 長範圍之光線自然混合而獲 本發明亦關於上述之白 少包括以下步驟:提供一基j 極、一暴底、一第一發光部 緩衝層區(BxGa^P 及 InxGai_xN) 導電性電極。上述基底與上述 。上述第一發光部分第一型束 層及一第一發光部分第二型束 ’且構成苐'一發光部分。上述 光部分第二型束缚層之上,該 上之緩衝層所構成。第二發光 性層及第二型束缚層依序形成 電性電極與上述第二發光部分 導電性電極流及該第一導電性 此電流通過該第二發光部分、 分’使該第一發光部分活性層 胃第二發光部分活性層發出第 第一波長範圍之光線及第二波 致白光。 光發光二極體其製造方法,至 :’其與一第一導電性電極接1224872 V. Description of the invention (6) Reducing the mismatch between the epitaxial layers in the diode element (丨 a 11 丨 ⑶ mismatch), so that the lattice between the epitaxial layers is more matched to reduce the Linear defects in polar elements provide white light-emitting diodes with perfect crystallinity. In order to achieve the above-mentioned object, the white light-emitting diode according to the present invention includes at least two layers that have a gradient change, a second light-emitting portion, and a second first conductive electrode to form an electrical contact binding layer, a first The active binding layer of the light emitting part is sequentially formed on the substrate. The buffer layer region is formed on the first buffer layer region. The buffer layer region is formed by one or a part of the first type binding layer on the buffer layer region. Second Conduction The second type tie layer forms electrical contact. When a potential difference is applied between the second electrodes, a current is generated, and the buffer layer region and a first light emitting part emit light of the first wavelength range and light of the two wavelength ranges, and are obtained by natural mixing of the light in this long range. The present invention also includes the following steps for providing a base electrode, a bottom electrode, and a first light emitting portion buffer layer region (BxGa ^ P and InxGai_xN) conductive electrodes. The above substrate and the above. The above-mentioned first light-emitting part first-type beam layer and a first light-emitting part second-type beam 'constitute a light-emitting part. The above-mentioned optical portion is a second-type binding layer, and a buffer layer is formed thereon. The second light-emitting layer and the second-type binding layer sequentially form an electrical electrode and the above-mentioned second light-emitting portion of the conductive electrode, and the first conductivity is passed through the second light-emitting portion, and the first light-emitting portion is divided by the current. The active layer of the second light-emitting part of the stomach emits light of a first wavelength range and second wave-induced white light. Light-emitting diode, its manufacturing method, to: 'It is connected with a first conductive electrode

1224872 五 、發明說明(7) ,,依序形成一第一發光部分第一型+ ^ π、一 μ 邛分活性層及一第一發光部分第二型束缚層於弟一發光 展:構成第一發光部分;形成至少二層呈梯度m J基底上 曰品BxGa卜XP及InxGa卜ΧΝ)於上述第一發光部分欠—之緩衝 =之上;依序形成一第二發光部分第一型束缚層一型^束縛 光部分活性層及一第二發光部分第二型束缚;於::: :層區上,.以構成第二發光部分,最後形成一第二導= “極於上述第二發光部分第二型束缚層部分表面上。 基於本發明之另一目的,本發明所述之基底,其上更 可形成至少二層呈梯度變化之緩衝層dGai χΡ及 inxGa卜ΧΝ)。 Χ 本發明之特徵在於本發明所述之白光發光二極體為單 晶片(single chip)型白光發光二極體,且其同時具有第 一發光部分及第二光發部分於單晶片上,可各自發出藍色 波長及黃色波長的光,自然混合後便能獲致白光。本發明 所述之白光發光二極體所發出的藍光及黃光皆由二極體本 身所發出,無需利用刺激其他介質(螢光粉或是硒化鋅基 板)來發出黃光。 本發明之另一特徵在於本發明所述之白光發光二極體 利用至少至少二層呈梯度變化之緩衝層區(BxGa^P及 I nxGai_x N)設置於二極體基底與第一發光部分之間、第一發 光部分與第二發光部分之間或是同時設置,且該缓衝層區 之晶格常數呈現梯度變化。靠近基底的缓衝層區底部具有 一第一晶格常數與基底之晶格常數略為相近,此晶格常數1224872 V. Description of the invention (7), forming a first light-emitting part of the first type + ^ π, a μ 邛 active layer, and a first light-emitting part of the second type binding layer in order to form a light-emitting exhibition: A light-emitting part; forming at least two layers with gradients of mJ on the substrate (BxGa, XP, and InxGa), above the first light-emitting part is under the buffer =, and sequentially forming a second light-emitting part, the first type binding Layer-type ^ binding light part active layer and a second light-emitting part of the second type binding; on ::: layer area, to form a second light-emitting part, and finally form a second guide = "extremely above the second On the surface of the second-type binding layer portion of the light-emitting portion. Based on another object of the present invention, the substrate according to the present invention can further form at least two buffer layers (dGai χP and inxGa (B × N)) which have gradient changes. The invention is characterized in that the white light emitting diode according to the present invention is a single chip type white light emitting diode, and it also has a first light emitting portion and a second light emitting portion on the single wafer, which can be emitted separately. Blue and yellow light After natural mixing, white light can be obtained. The blue light and yellow light emitted by the white light emitting diode according to the present invention are emitted by the diode itself, without the need to stimulate other media (fluorescent powder or zinc selenide substrate) Another feature of the present invention is that the white light-emitting diode according to the present invention utilizes at least two buffer layer regions (BxGa ^ P and InxGai_x N) which are gradiently changed to be disposed on the diode substrate and The first light-emitting part, the first light-emitting part and the second light-emitting part are arranged at the same time, and the lattice constant of the buffer layer region shows a gradient change. The bottom of the buffer layer region near the substrate has a first crystal. The lattice constant is slightly similar to the lattice constant of the substrate. This lattice constant

12248721224872

再遞增或遞減,以趨近适 數,且使第二晶格常數;;層…所具有之第二晶格常 格常數略為相近—發光部分第-型束缚層之晶 區底部具有ϋ格f 近第—發光部分的缓衝層 之晶格常數略為相㊉,:一發光部分第二型束缚層 緩衝層區表面所具有之第曰曰,數再遞增或遞,咸’以趨近 與第二發光部分第—型格常數二且使第四晶格常數 i朿、、專層之晶格常數略為相近。 為使本發明之上 ^ k目的、特徵能更明顯易懂,下 舉較佳貫施例,並配合所 口尸汁附圖式,作詳細說明如下: 【實施方式】 本發明之白色發光二極體主要是利用單一發光二極體 發出藍光波及黃光波長的光,藉以合成白色光。基本上, 若欲以兩種不同的主波峰合成白A,則一般是採用波長約 為43〇nra的藍色光及波長約為56〇nm的黃色光。 以下请配合麥照第5圖之白光發光二極體結構剖面 圖,以詳細說明本發明。 二本發明所述之白光發光二極體結構其一較佳實施例, 请參照第5圖,可至少包括:一基底丨〇 〇、一第一發光部分 第一型束缚層122形成於該基底1〇〇之上、一第一發光部分 活性層1 24及一第一發光部分第二型束縛層丨26依序形成於 f述第一發光部分第一型束缚層丨2 2上,且第一發光部分 第一型束缚層1 2 2、第一發光部分活性層丨2 4及第一發光部Increase or decrease again to approach the proper number and make the second lattice constant; the second lattice constant lattice constants of the layer ... are slightly similar-the bottom of the crystal region of the type-type binding layer of the light emitting part has a lattice f The lattice constants of the buffer layer near the first light-emitting part are slightly different: the number of the surface of the buffer layer area of the second type of binding layer of a light-emitting part is increased or increased, and the number of The second light-emitting part has a first lattice constant of two and the fourth lattice constant i 朿, the lattice constant of the monolayer are slightly similar. In order to make the objectives and features of the present invention more obvious and easy to understand, the following preferred embodiments are described below, and in accordance with the drawings of the corpse juice, the detailed description is as follows: [Embodiment] The white light-emitting diode 2 of the present invention The polar body mainly uses a single light-emitting diode to emit blue light and yellow light, thereby synthesizing white light. Basically, if white A is to be synthesized with two different main peaks, blue light with a wavelength of about 43 nm and yellow light with a wavelength of about 56 nm are generally used. In the following, please refer to the cross-sectional view of the structure of the white light emitting diode of FIG. 5 of Maizhao to describe the present invention in detail. A preferred embodiment of the white light emitting diode structure according to the present invention, as shown in FIG. 5, may include at least: a substrate, a first light emitting portion, and a first type binding layer 122 formed on the substrate. Above 100, a first light-emitting part active layer 124 and a first light-emitting part second-type binding layer 26 are sequentially formed on the first light-emitting part first-type binding layer 22, and the first A light emitting part of the first type binding layer 1 2 2, a first light emitting part active layer 丨 2 4 and a first light emitting part

1224872 五、發明說明(9) 分第=型束缚層126構成第一發光部分120。 声126一之緩上衝,\區=形成於上述第一發光部分第二型束缚 ^構成。一 μ 層區13〇可由—層或一層以上之緩衝層 弟一發光部分第一型束缚層142、一 部分活性層1 44及一笛-八忠如八— 弟一毛九 ^ ^ ^ 弟一毛先口15刀弟二型束缚層1 46依序形 成於上述緩衝層區130上,且第二發光部分第一型束缚層 142、弟二發光部分活性層144及第二發光部分第二型束缚 層146構成第二發光部分14〇。當電流通過第一發光 120時,第-發光部分活性層124發出—第—波長的光^而 當電流通過第二發光部分140時,第一發光部分活性層144 發出一第二波長的光。當第一波長的光與第二 合時可獲致白光。 焚日〕尤他 上述之結構可更包括使緩衝層區13〇之晶格常數呈現 梯度(grading)變化,在一較佳實施例中,可以使緩 區130底部之晶格常數與第一發光部分第二型束缚層I? 9 面具有之第一晶格常數(ci)相近,而緩衝層區13〇之曰义 常數逐漸變化’使緩衝層區130表面之晶格常數相近 二發光部分第一型束缚層142底部所具有之一第二曰夂= 數(C2)。簡言之,缓衝層區130之晶格常數係由 常數(C1)逐漸改變至第二晶格常數(C2)。其中,緩曰曰^品 1 30之晶格常數的梯度變化例如可藉由調整緩衝層區之^組^ 成比例以達成。 本發明所述之白光發光二極體係具有一第二導電性 極3 0 0與上述白光發光一極體結構之第二發光部分第一 / 刀乐"型1224872 V. Description of the invention (9) The first type light-emitting portion 120 is constituted by the sub-type binding layer 126. The sound 126 is gradually overshooting, and \ zone = forms a second-type restraint formed in the first light-emitting portion. A μ layer region 13 can be composed of one or more buffer layers, a light-emitting part of the first type binding layer 142, a part of the active layer 144, and a flute-Hachijoru eighth. Brother Yi Mao Jiu ^ ^ Brother Yi Mao The first 15-blade second-type binding layer 1 46 is sequentially formed on the buffer layer region 130, and the second light-emitting portion is a first-type binding layer 142, the second light-emitting portion is an active layer 144, and the second light-emitting portion is a second-type binding. The layer 146 constitutes the second light emitting portion 14o. When the current passes through the first light-emitting portion 120, the first-light-emitting-portion active layer 124 emits light of the first wavelength. When the current passes through the second light-emitting portion 140, the first-light-emitting portion active layer 144 emits light of the second wavelength. When the light of the first wavelength is combined with the second, white light is obtained. [Sunburn] The above-mentioned structure may further include changing the lattice constant of the buffer layer region 13 to a grading change. In a preferred embodiment, the lattice constant at the bottom of the buffer region 130 and the first light emission may be changed. The first lattice constant (ci) of the second type binding layer I? 9 is similar, and the meaning constant of the buffer layer region 130 is gradually changed to make the lattice constant of the surface of the buffer layer region 130 close. The second type of binding layer 142 has a second number (C2). In short, the lattice constant of the buffer layer region 130 is gradually changed from the constant (C1) to the second lattice constant (C2). Among them, the gradient change of the lattice constant of the product 1 30 can be achieved by, for example, adjusting the composition of the buffer layer region in proportion. The white light emitting diode system according to the present invention has a second conductive electrode 300 and the second light emitting part of the white light emitting monopolar structure described above.

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束缚層1 4 6做電接觸 及具有 弟 白光發光二極體結構之基板]〇〇 :::性:極2⑽與上述 係顯示一較佳實施例之白’凊筝照第6圖, 例中,本發明所述之白光發在某些較佳實施 2 〇 0也可為形成於第一發光 弟一導電性電極 區上,使第-導電性電極舆 Γ例之白光發光二極體。上述與基板形成電1觸一的第 可為金屬接點、金屬層、金屬接腳或任 2為一極體電極接觸端之電導平台(接點),不過此 W化圖式,僅以電極接觸端表示之。 …、 以下再配合參照第5圖,舉例說明適用於本發明之 層材質組合。 例:h參照第2圖所示,基底1〇〇可為砷化鎵(GaAs)、磷 化,(GaP)、矽(Si)或碳化矽(3c_sic),上述第一發光部 分第一型束缚層122可為磷化鋁鎵銦(A1GaInp)系化合物, 上述第一發光部分活性層丨24可為磷化鋁鎵銦(A丨Ga丨np)系 化合物’上述第一發光部分第二型束缚層丨26可為磷化鋁 鎵銦(A1 GalnP)系化合物,其表面具有一第一晶格常數 C1。上述緩衝層區130可為一由BxGa(ix)P所構成之第一緩衝 層及一由InyGa(1_y)N所構成之第二缓衝層,其中osx^i、〇 -y - 1 ’且第二缓衝層係形成於第一緩衝層上與第二發 光部分第一型束缚層底部相鄰。上述X可由〇至1,以使緩 衝層區1 3 0底部之晶格常數與第一晶格常數c 1相近及使第The binding layer 1 4 6 is used for electrical contact and a substrate with a white light emitting diode structure. 〇〇 ::: 性 : 极 2⑽ and the above is a white 'Zhengzhao photo showing a preferred embodiment of FIG. 6, in the example In some preferred embodiments, the white light emission described in the present invention may also be a white light-emitting diode formed on a conductive electrode region of the first light-emitting diode, so that the first conductive electrode is a white light-emitting diode. The first contact with the substrate for electrical contact may be a metal contact, a metal layer, a metal pin, or any of the conductive platforms (contacts) that are the contact ends of a polar body electrode, but this W-shaped diagram uses only electrodes The contact end indicates this. …, And in conjunction with reference to FIG. 5 below, examples of layer material combinations applicable to the present invention are illustrated. Example: As shown in FIG. 2, the substrate 100 may be gallium arsenide (GaAs), phosphide (GaP), silicon (Si), or silicon carbide (3c_sic). The layer 122 may be an aluminum gallium indium phosphide (A1GaInp) -based compound, and the above-mentioned first light-emitting part active layer 丨 24 may be an aluminum gallium indium phosphide (A 丨 Ga 丨 np) -based compound. The layer 26 may be an aluminum gallium indium phosphide (A1 GalnP) -based compound, and a surface thereof has a first lattice constant C1. The above buffer layer region 130 may be a first buffer layer composed of BxGa (ix) P and a second buffer layer composed of InyGa (1_y) N, where osx ^ i, 0-y-1 'and The second buffer layer is formed on the first buffer layer and is adjacent to the bottom of the first light-emitting portion of the first type binding layer. The above X can be from 0 to 1, so that the lattice constant at the bottom of the buffer layer region 130 is close to the first lattice constant c 1 and the first

1224872 五、發明說明(11) 緩衝層與接壤之第二緩衝層的晶格常數相近。 r a 1「1 ϋ第一入& *部分第一型束缚層可為氮化紹鎵銦 (A1GaInN)糸化合物,其表面具有一第一晶袼常數以。上 、’〔之y可由0至1,以使緩衝層區丨3 〇表面之晶格常數與第二 晶格常數C2相近及使第二緩衝層與接壤之第一缓衝層的晶 格#數相近。上述第二發光部分活性層可為氮化鋁鎵銦 (AlGalnN)系化合物,以及上述第二發光部分第二型束缚 層可為氮化铭鎵銦(A 1 G a I η N)系化合物。 當電流通過第一發光部分丨2 〇時,由磷化鋁鎵銦 (A 1 Ga I ηΡ)系化合物所構成之第一發光部分活性層丨2 4會發 出一黃色波長的光(波長約5 6 0nm),而當電流通過第二發 光部分140時,由氮化鋁鎵銦(A1GaInN)系化合物構成之第 一發光部分活性層1 4 4會發出一藍色波長的光(波長約 4 3 0 n m)。當黃色波長的光與藍色波長的光自然混合時可獲 致白光。 本發明上述之白光發光二極體,在上述白光發光二極 體結構除第一發光部份及第二發光部份之間包括一第二緩 衝層區,其基板及第一發光部份之間,更可包括一第一緩 衝層區,請參照第8圖。如上所述之白光發光二極體結構 可至少包括:一基底100、一第一緩衝層區110、一第一發 光部分第一型束缚層122形成於該第一緩衝層區110之上、 一第一發光部分活性層1 24及一第一發光部分第二型束缚 層126依序形成於上述第一發光部分第一型束缚層122上, 一第二緩衝層區1 5 0形成於上述第一發光部分第二型束缚1224872 V. Description of the invention (11) The lattice constants of the buffer layer and the adjacent second buffer layer are similar. ra 1 ″ 1 ϋFirst entry & * Some first type binding layers may be gallium indium nitride (A1GaInN) 糸 compounds, the surface of which has a first crystalline 袼 constant. Above, '[, y may be from 0 to 1. In order to make the lattice constant of the surface of the buffer layer region and the second lattice constant C2 close and the number of the lattice # of the second buffer layer and the bordering first buffer layer close. The above-mentioned second light emitting part is active The layer may be an aluminum gallium nitride (AlGalnN) -based compound, and the second light-emitting portion of the second type binding layer may be an indium gallium nitride (A 1 G a I η N) -based compound. When a current passes through the first light The part of the first light-emitting part active layer composed of aluminum gallium indium phosphide (A 1 Ga I η) series compound at 2 o’clock will emit a light with a yellow wavelength (wavelength of about 5 60 nm), and when When a current passes through the second light-emitting portion 140, the first light-emitting portion active layer 14 composed of an aluminum gallium indium (A1GaInN) -based compound emits a light of blue wavelength (wavelength of about 4 30 nm). When yellow When the light of the wavelength and the light of the blue wavelength are naturally mixed, white light can be obtained. The white light emitting diode of the present invention, The above white light emitting diode structure includes a second buffer layer region between the first light emitting portion and the second light emitting portion, and further includes a first buffer layer region between the substrate and the first light emitting portion. Please refer to Fig. 8. The white light emitting diode structure as described above may include at least: a substrate 100, a first buffer layer region 110, and a first light emitting portion of the first type binding layer 122 formed on the first buffer layer. Above the region 110, a first light-emitting portion active layer 124 and a first light-emitting portion second-type binding layer 126 are sequentially formed on the first light-emitting portion first-type binding layer 122, and a second buffer layer region 1 50 formed in the above-mentioned first light-emitting part of the second type bond

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層126之上,該第二緩衝層區15〇可由一 ^ 衝厣斛娃Λ、 斤々χ 曰4 々从上之緩 曰斤構成。一弟二务光部分第一型束缚層142、一 一 f光部分活性層144及一第二發光部分第二型束缚居146一 序形成於上述第二緩衝層區15〇上。 曰 上述之結構可使第一緩衝層區110之晶格常數 度(grading)變化,在一較佳實施例中,可以使第_ 層區130之晶格常數由基板1〇〇所具有之第一晶袼常 逐漸改變至第一發光部分第一型束缚層丨22所具有之第二 晶格常數(C2);可以使第二緩衝層區15〇之晶格常數由^ 一發光部分第二型束缚層1 2 6所具有之第三晶格常數(c 逐漸改變至第二發光部分第一型束縛層丨42所具 晶格常數(C4) 乐 以下再配合參照第7圖,舉例說明本發明及適 發明之各層材質組合。 、本 例2:參照第7圖所示,基底1〇〇可為矽(Si)或碳化石夕 Uc —sic),其具有一第一晶格常數C1。在上述基底形成一 第一緩衝層區110,第一緩衝層區110可為由BnGa(i n)p所構 成之第一缓衝層及InmGa^J所構成之第二緩衝層所構成, 其中〇Sn$l、0Sm$l。上述之η可由0至1,以使第一緩 衝層區110底部之晶格常數與第一晶格常數C1相近及使第 一緩衝層與接壤之第二緩衝層的晶格常數相近。形成一第 一發光部分第一型束缚層122於第一緩衝層區110上,其表 面具有一第二晶格常數C2。上述之m可由0至1,以使第一 缓衝層區11 0表面之晶格常數與第二晶格常數C2相近及使Above the layer 126, the second buffer layer region 150 may be composed of a single layer, a pair of layers, and a pair of layers. A first-type binding layer 142, a first-type binding layer 142, a second-light-emitting portion active layer 144, and a second light-emitting portion second-type binding layer 146 are sequentially formed on the second buffer layer region 150. That is, the structure described above can change the lattice constant of the first buffer layer region 110. In a preferred embodiment, the lattice constant of the first layer region 130 can be changed from that of the substrate 100. A crystal is often gradually changed to the second lattice constant (C2) of the first light-emitting portion of the first type binding layer 22; the lattice constant of the second buffer layer region 15 can be changed from ^ The third lattice constant (c gradually changes to the second light-emitting part of the first type binding layer in the second light-emitting portion of the second-type binding layer 1 2 6) (42) The lattice constant (C4) of the second light-emitting layer The material combination of the layers of the invention and suitable inventions. 2. This example 2: Referring to FIG. 7, the substrate 100 may be silicon (Si) or carbide (Uc — sic), which has a first lattice constant C1. A first buffer layer region 110 is formed on the above substrate. The first buffer layer region 110 may be a first buffer layer composed of BnGa (in) p and a second buffer layer composed of InmGa ^ J, where Sn $ l, 0Sm $ l. The above-mentioned η can be from 0 to 1, so that the lattice constant at the bottom of the first buffer layer region 110 is close to the first lattice constant C1 and the lattice constants of the first buffer layer and the second buffer layer adjacent thereto are close. A first light-emitting portion of the first type binding layer 122 is formed on the first buffer layer region 110, and the mask has a second lattice constant C2. The above m can be from 0 to 1, so that the lattice constant of the surface of the first buffer layer region 110 is close to the second lattice constant C2 and

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1224872 五、發明說明(13) --- 第二緩衝層與接壌之第一緩衝層的晶格常數相近。第一發 光部分第一型束缚層122可為氮化鋁鎵銦(A1GaInN)系化合 物。以上述第一緩衝層區為蝕刻停止層,選擇性蝕刻 上述第一發光部分第一型束缚層丨2 2,以露出部分的上述 第一緩衝層區110,並形成一第一導電性電極2〇〇於其部分 表面上。 形成一第一發光部分活性層丨24於上述第一發光部分 第一型束缚層1 22上,第一發光部分活性層丨24可為氮化鋁 録姻(A1 Gal nN)系化合物。形成一第一發光部分第二型束 缚層1 26於第一發光部分活性層丨24上,第一發光部分第二 型束缚層126可為氮化鋁鎵銦(A1GaInN)系化合物,直表面 具有-第三晶格常數C3。接著,形成一第二緩衝㈣於 第-發光部分第二型束缚層126上。上述第二緩衝層區係 包括一由IriyG%—y〕N所構成之第一緩衝層及一由 構成之第二緩衝層,其中、〇gyg,且第= 缓衝斤 層係形成於第二緩衝層下與第一發光部分第二型 126相鄰上述之y可由〇至1,以使第二緩衝層區丨5〇底曰部 之晶格常數與第二晶格常數C3相折艿枯諠 - > μ _ @ t Β s & 近使弟—緩衝層與接壤 之第一緩衝層的晶格常數相近。 形成一第二發光部分第一型束缚層142於 衝層區150上,而上述第-菸氺邱八筮 別+ l乐一、& &九部分弟一型束缚層U2可為 填化銘鎵銦(A1GaInP)系化合物,其表面具有二^四曰於 常數C4。上述之X可由〇至1,以使第— 日曰α 汉弟一緩衝層區矣而之 晶格常數與第四晶格常數C4相近及使第_ lbU表面之 k汉使弟一綾衝層與接壤1224872 V. Description of the invention (13) --- The lattice constants of the second buffer layer and the first buffer layer connected are similar. The first light emitting portion of the first type tie layer 122 may be an aluminum gallium indium nitride (A1GaInN) -based compound. The first buffer layer region is used as an etching stop layer to selectively etch the first light-emitting portion of the first type binding layer 丨 2 2 to expose a portion of the first buffer layer region 110 and form a first conductive electrode 2 〇〇 on its surface. A first light emitting part active layer 24 is formed on the first light emitting part first type binding layer 122, and the first light emitting part active layer 24 may be an aluminum nitride (A1 Gal nN) -based compound. A first light emitting part second type binding layer 126 is formed on the first light emitting part active layer 丨 24. The first light emitting part second type binding layer 126 may be an aluminum gallium indium nitride (A1GaInN) series compound, and the straight surface has -The third lattice constant C3. Next, a second buffer layer is formed on the second-type binding layer 126 of the -light emitting portion. The above-mentioned second buffer layer system includes a first buffer layer composed of IriyG% -y] N and a second buffer layer composed of which, 0gyg, and the third buffer layer is formed in the second Under the buffer layer, the first y and the second type 126 are adjacent to each other. The above-mentioned y can be from 0 to 1, so that the lattice constant of the second buffer layer region and the second lattice constant C3 are collapsed. Noise-> μ _ @ t Β s & Recently, the lattice constants of the buffer layer and the adjacent first buffer layer are close. A second light-emitting portion of the first-type binding layer 142 is formed on the punching layer 150, and the aforementioned -Yanqiu Qiba Babebe + l Leyi, & & & Nine-Party Type-I binding layer U2 may be filled The indium gallium indium (A1GaInP) -based compound has a surface constant of C4 on the surface. The above-mentioned X can be from 0 to 1, so that the first day of the α-Handi-buffer layer region has a lattice constant close to the fourth lattice constant C4 and the k-Han of the _lbU surface is washed away. Bordering

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之第一緩衝層的晶格當翁如析。片严^ 性声144及楚-π 依序形成第二發光部分活 第二π Φ «第先邛分第二型束缚層146於第二發光部分 I is U 1 Ρ Τ /上,第二發光部分活性層144可為氮化鋁 鎵銦(A 1 G a I η Ν)糸化合物,而楚-政,A ! , 〇 _ . ^ 物 而弟一發光部分第二型束缚層 1 4 6可為鼠化紹嫁銘](八】〇只了 |^、金/1_人。 , uibalnN)糸化合物。形成一第二導電 性電極3 0 0於上述第-蘇忠立κ八@ ^ &乐一 ^先部分弟二型束缚層丨4 6部分表面 上0 當電流通過第一發光部分120時,由氮化鋁鎵銦 A1 GajnD系化合物所構成之第一發光部分活性層丨24會發 出藍色波長的光(波長約43〇nm),而當電流通過第二發 光部分1 4 0時,由磷化鋁鎵銦(A丨Ga丨系化合物構成之第 二發光部分活性層144會發出一黃色f長的光(波長約 5 6 0nm)。當黃色波長的光與藍色波長的光自然混合時可獲 致白光。 以下說明形成BnGa+uP做為緩衝層之一較佳實施例。 首先’基底可先以適當化學溶液清洗,接著在%氣氛下, 將基底加熱至適當溫度,例如9 〇 〇〜11 8 0 °C,較佳為1 0 3 0 C,利用_化物氣相蠢晶法(halide vapor phase epitaxy),以H2作為承載氣體(carrier gas),氣化硼 (BC13)、三甲基鎵(trimethyl gal 1 ium ; TMG)與氯化磷 (PC13)或疋;|l化侧(BC13)、三甲基鎵(trimethyl gallium ; TMG)與磷化氫(PH3)作為前驅物。於溫度約100〇 °C上下進行高溫磷化硼層磊晶,反應约6 〇分鐘,其厚度約The lattice of the first buffer layer is like a crystal. The sound of the film ^ and the sound 144 and Chu-π sequentially form the second light-emitting portion or the second π Φ «first first-type second type binding layer 146 on the second light-emitting portion I is U 1 Ρ / /, the second light-emitting Part of the active layer 144 may be an aluminum gallium indium (A 1 G a I η Ν) compound, while Chu-Zheng, A !, 〇_. ^ And the light emitting part of the second type binding layer 1 4 6 may To marry the rattles of the Shao Mingming] (eight) 0 only | ^, gold / 1 person., UibalnN) 糸 compounds. A second conductive electrode 3 0 0 is formed in the above-Su Zhongli κ 八 @ ^ & 乐 一 ^ first part of the second type binding layer 丨 4 6 on the surface of 0 when the current passes through the first light emitting part 120, by nitrogen The active layer of the first light-emitting part composed of aluminum gallium indium A1 GajnD-based compound 24 emits light of blue wavelength (wavelength about 43nm), and when the current passes through the second light-emitting part 1 40, it is phosphorylated The second light-emitting part of the active layer 144 composed of aluminum gallium indium (A 丨 Ga 丨 series compound) emits a yellow light f (wavelength about 560 nm). When the light of yellow wavelength and the light of blue wavelength are naturally mixed, White light is obtained. The following is a description of a preferred embodiment of forming BnGa + uP as a buffer layer. First, the substrate can be cleaned with a suitable chemical solution first, and then the substrate can be heated to a suitable temperature in a% atmosphere, such as 900 ~ 11 80 ° C, preferably 10 3 0 C, using halide vapor phase epitaxy, H2 as carrier gas, boron gas (BC13), trimethylgallium (Trimethyl gal 1 ium; TMG) and phosphorus chloride (PC13) or tritium; | l side (BC13) Trimethyl gallium (trimethyl gallium; TMG). And phosphine (PH3) as a precursor for high temperature boron phosphide epitaxial layer at a temperature of about 100〇 ° C and down, the reaction for about 6 minutes square, a thickness of about

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五、發明說明(15) 為4 5 6 0 n m。藉由改變各前驅物之含量比例,π Α計》成不同組 成比例之多層堆疊層BnGa^wP,使晶格常數呈現梯度變 化。此方法所形成之BnGa(1_n)P緩衝層係為高溫)p<緩 層。然而,本發明亦可於該高溫KGahJ緩衝層與1_^底之-間設置一低溫磷化硼(BP)緩衝層,該低溫磷化緩衝 層係於溫度約3 0 0 °C之下形成。 、一 而緩衝層InyGa卜yN可利用MOVCVD法製成,例如以三甲 基銦(trimethy indium ;TMIn)、三甲基鎵(trimethyl gal 1 ium ; TMG)以及NH3為前驅物而形成,藉由改變各前驅 物之含量比例,以形成不同組成比例之多層堆疊層5. Description of the invention (15) is 4 5 6 0 n m. By changing the content ratio of each precursor, the multi-layer stacking layer BnGa ^ wP with different composition ratios can be used to make the lattice constants change gradients. The BnGa (1_n) P buffer layer formed by this method is a high-temperature) p < moderate layer. However, the present invention may also provide a low-temperature boron phosphide (BP) buffer layer between the high-temperature KGahJ buffer layer and the bottom surface, and the low-temperature phosphate buffer layer is formed at a temperature of about 300 ° C. 1. The buffer layer InyGa and yN can be made by MOVCVD, for example, using trimethy indium (TMIn), trimethyl gal 1 ium (TMG), and NH3 as precursors. Change the content ratio of each precursor to form multiple stacked layers with different composition ratios

InyGa卜yN。 再者,緩衝層InxGahP可利用MOVCVD法製成,例如以 三甲基銦(trimethy indium ; TMIn)、三甲基嫁 (trimethyl gal 1 ium ; TMG)以及磷化氫(PH3)為前驅物而形 成’藉由改變各前驅物之含量比例,以形成不同組成比例 之多層堆疊層InxGai_xP。 以下說明形成第一型束缚層之一較佳實施方式。形成 構化I呂鎵銦(A 1 G a I η P)系化合物之前驅物可包括三甲基|呂 ((CH3)3A1)、三曱基鎵((CH3)3Ga)與三甲基銦((CH3)3In)及 填化氫(PHS)當作未反應材料、形成氮化鋁鎵銦(A1GaInN) 系化合物之前驅物可包括三甲基鋁((CH3 )3 A 1)、三甲基鎵 ((CH3)3Ga)與三甲基銦((CH3)3In)及氮化氫(NH3)當作未反 應材料,利用減小壓力的MOCVD法形成磷化鋁鎵銦系化合 物。反應時供應&與N2氣體,溫度例如約為5 0 0〜80 0InyGabuyN. Furthermore, the buffer layer InxGahP can be made by MOVCVD, for example, it is formed by using trimethy indium (TMIn), trimethyl gal 1 ium (TMG), and phosphine (PH3) as precursors. 'By changing the content ratio of each precursor, a multilayer stacking layer InxGai_xP with different composition ratios is formed. A preferred embodiment of forming the first type of tie layer is described below. The precursors for the formation of the structured I LuGa indium (A 1 G a I η P) series compounds may include trimethyl | Lu ((CH3) 3A1), trifluorenyl gallium ((CH3) 3Ga), and trimethylindium (( CH3) 3In) and hydrogen-filled hydrogen (PHS) are used as unreacted materials, and precursors for forming aluminum gallium indium nitride (A1GaInN) -based compounds may include trimethylaluminum ((CH3) 3 A 1), trimethylgallium ((CH3) 3Ga), trimethylindium ((CH3) 3In), and hydrogen nitride (NH3) were used as unreacted materials, and an aluminum gallium indium phosphide-based compound was formed by a reduced pressure MOCVD method. Supply & and N2 gas during reaction, temperature is about 50 0 ~ 80 0, for example

1224872 五、發明說明(16) 一 ---- 下可使用二乙基鋅((Hs夂Ζ η )當作鋅的摻雜來源,或使 用石西化氫(IS e )當作摻雜物的反應材料。 .另外,活性層同樣可利用M0VCVD法,例如以三甲基鋁 (trunethy aluminum ;TMA1)、三曱基銦(trimethy indium,TMIn)、三甲基鎵(trimethyl gallium ; TMG)以 及氮化氫(N Hs)(或麟化氫(p % ))為前驅物而形成,反應時 ,應I與I氣體,溫度例如約為5 0 0〜80 0 °C下。較佳者可 藉由改變各前驅物之含量比例,以形成不同組成比例之多 層堆疊層。 第二型束缚層例如可形成磷化鋁鎵銦(A i Ga〗np )系化 合物,前驅物可包括三甲基鋁((Ch3)3A1)、三甲基鎵((Ch3) Ja)與三甲基銦((CH3)3In)及磷化氫(pi)當作未反應材3 料 或形成氛化銘叙銦(A1G a I η N)系化合物,前驅物可包 括三甲基銘((CH3)3A1)、三甲基鎵((CH3)3Ga)與三曱基銦 ((C Hs夂I η)及氮化氫(n Hs)當作未反應材料,利用減小壓力 的Μ 0 C V D法形成礙化紹鎵銦系化合物。反應時供應札與&氣 體’溫度例如約為5 0 0〜8 0 0 °C下,可例如以鎂(Mg)摻雜成 P型‘電型恶’或者例如以硫(§)換雜成η型導電型態。 根據本發明所述之白先發光二極體及其製造方法,本 發明具有以下之優點: 1 ·本發明之白色發光二極體係二極體本身通電流後即 可發出二波長之光,再後混合可獲致白光,無需結合螢光 材料或其他激發介質,因此不會因為螢光材料或其他激發1224872 V. Description of the invention (16) a ---- It is possible to use diethyl zinc ((Hs 夂 Z η)) as the doping source of zinc, or use hesparite (IS e) as the dopant. Reactive materials. In addition, the MOVCVD method can also be used for the active layer. For example, trimethyl aluminum (TMA1), trimethy indium (TMIn), trimethyl gallium (TMG), and nitrogen can be used. Hydrogen hydride (N Hs) (or hydrogen hydride (p%)) is formed as a precursor. During the reaction, I and I gas should be used, and the temperature is, for example, about 500 ~ 80 0 ° C. The better one can borrow The content ratio of each precursor is changed to form multilayer stacking layers with different composition ratios. The second type of binding layer can form, for example, an aluminum gallium indium phosphide (A i Ga〗 np) -based compound, and the precursor may include trimethyl aluminum. ((Ch3) 3A1), trimethylgallium ((Ch3) Ja), trimethylindium ((CH3) 3In), and phosphine (pi) are used as unreacted materials or form indium ( A1G a I η N) -based compounds, the precursors may include trimethylammonium ((CH3) 3A1), trimethylgallium ((CH3) 3Ga), and trifluorene-based indium ((C Hs 夂 I η)) and nitride Hydrogen (n Hs) As an unreacted material, a reduced pressure M0 CVD method is used to form a gallium indium-based gallium indium-based compound. During the reaction, the temperature of the supply gas & gas is, for example, about 500 to 800 ° C. For example, Doping with magnesium (Mg) into a P-type 'electrical-type evil' or, for example, replacing with sulfur (§) into an η-type conductive type. According to the white pre-emitting diode and the manufacturing method thereof, the present invention It has the following advantages: 1. The white light-emitting diode system of the present invention can emit light of two wavelengths after passing through the current, and then mixed to obtain white light without the need to combine fluorescent materials or other excitation media, so it will not Because of fluorescent materials or other excitation

1224872 五、發明說明(17) 介負之哥命而影響一極體之表現。 〇α 2.本發明所述=白光發光二極體兩發光部分皆形成於 單顆二極體上,為單晶片(single chip)型白光發光二極 體,驅動電路設計容易,不需藉由組合多顆發光二極體, 可大大地降低生產成本,並降低包裝及電路控制的困難。 3:由於用來混合成白先的波長皆由白光發光二極體本 身自行發出’而二極體之發光色溫不易隨著使用時間而改 變,且發光效率易匹配,所以本發明之白光發光二極體之 光波長易於控制,不會像利用激發介質所得之二極體,豆 光波長易隨溫度或操作電壓增加(減少)而改變。 〃 七4_ =發明之白光發光二極體,其利用不同之基底(導 :2不、冑白可)上形成白光發光二極體,有別於習知白 =光二極體只能在固定基底形成之技術,且可利用緩衝 曰降低一極體兀件中各磊晶層之間的晶格不匹配⑹ :二1二各遙晶層之間的晶格更加匹配,以降低二 =几件中之線缺陷,提供具完美結晶度之白光發光二極 本發明雖以較佳實施例揭露如u ^ ^ 本發明的範圍,任何熟習此項技蓺’广、並非用以限定 保護範圍當視後附之申請專利此本發明之 视阁所界定者為準。1224872 V. Description of the invention (17) The life of a negative influences the performance of a polar body. 〇α 2. According to the present invention, the two light-emitting parts of the white light-emitting diode are formed on a single diode, which is a single chip type white light-emitting diode, and the driving circuit is easy to design without using a Combining multiple light-emitting diodes can greatly reduce production costs and reduce packaging and circuit control difficulties. 3: Since the wavelengths used to mix into white are all emitted by the white light-emitting diode itself, and the color temperature of the diode is not easy to change with the use time, and the light-emitting efficiency is easy to match, the white light-emitting diode of the present invention The light wavelength of the polar body is easy to control. Unlike the diode obtained by using an excitation medium, the light wavelength of the bean is easy to change with increasing (decreasing) temperature or operating voltage.七 七 4_ = Invented white light emitting diode, which uses different substrates (Guide: 2 No, 胄 白 可) to form white light emitting diodes, which is different from the conventional white = light diode can only be fixed on the substrate Formation technology, and the buffer can be used to reduce the lattice mismatch between the epitaxial layers in a polar element. 二: The lattices between the telemorphic layers are more matched to reduce two = several pieces. Medium line defect, providing white light emitting diodes with perfect crystallinity. Although the present invention discloses the scope of the present invention in a preferred embodiment, anyone familiar with this technology is broad and not intended to limit the scope of protection. The attached patent application is subject to the definition of the present invention.

1224872 圖式簡單說明 第1圖及第2圖係顯示習知之白光發光二極體之結構剖 面圖及發光示意圖。 第3圖及第4圖係顯示另一習知之白光發光二極體之結 構剖面圖及發光示意圖。 第5圖係顯示根據本發明白光發光二極體結構之一較 佳實施例結構剖面圖。 第6圖係顯示根據本發明之一較佳實施例的白光發光 二極體剖面圖。 第7圖係顯示根據本發明之另一較佳實施例的白光發 光二極體剖面圖。 第8圖係顯示根據本發明白光發光二極體結構之另一 較佳實施例結構剖面圖。 【符號說明】 1 2〜晶粒, 1 3、1 5〜金屬接腳; 14〜螢光材料; 16〜封裝材料; 1 7〜凹槽; 2 1〜二極體; 22〜蠢晶發光材料, 23、25〜金屬接腳; 2 4〜鋅化硒基板; 2 6〜封裝材料;1224872 Brief Description of Drawings Figures 1 and 2 are cross-sectional views and light-emitting diagrams showing a conventional white light-emitting diode. 3 and 4 are cross-sectional views and light emission diagrams of another conventional white light-emitting diode structure. Fig. 5 is a sectional view showing the structure of a preferred embodiment of a white light emitting diode structure according to the present invention. Fig. 6 is a cross-sectional view showing a white light emitting diode according to a preferred embodiment of the present invention. Fig. 7 is a cross-sectional view showing a white light emitting diode according to another preferred embodiment of the present invention. Fig. 8 is a sectional view showing the structure of another preferred embodiment of the white light emitting diode structure according to the present invention. [Symbol description] 1 2 ~ crystal grains, 1 3, 1 5 ~ metal pins; 14 ~ fluorescent materials; 16 ~ packaging materials; 1 7 ~ grooves; 2 1 ~ diodes; 22 ~ stupid luminescent materials , 23, 25 ~ metal pins; 2 4 ~ selenium zinc substrate; 2 6 ~ packaging materials;

0769-9102TWF(nl) ; VTERA-91-010-TW ; Phoelip.ptd 第 22 頁 1224872 圖式簡單說明 100〜基底; 1 1 0〜第一緩衝層區; 120〜第一發光部分; 122〜第一發光部分第一型束缚層; 124〜第一發光部分活性層; 126〜第一發光部分第二型束缚層; 1 3 0〜緩衝層區; 1 4 0〜第二發光部分; 142〜第二發光部分第一型束缚層; 144〜第二發光部分活性層; 146〜第二發光部分第二型束缚層; 1 5 0〜第二緩衝層區; 2 0 0〜第一導電性電極; 3 0 0〜第二導電性電極; C ;1〜第一晶格常數; C2〜第二晶格常數; C3〜第三晶格常數; C4〜第四晶格常數; E〜二極體之電激發光; B〜藍色波長的光 F〜螢光材料被激發產生的光;以及 Y〜黃色波長的光。0769-9102TWF (nl); VTERA-91-010-TW; Phoelip.ptd Page 22 1224872 Schematic description of 100 ~ substrate; 1 1 0 ~ first buffer layer area; 120 ~ first light emitting part; 122 ~ first A light emitting part of the first type binding layer; 124 to the first light emitting part active layer; 126 to the first light emitting part of the second type binding layer; 130 to the buffer layer area; 1 40 to the second light emitting part; 142 to the first Two light-emitting portions of the first type binding layer; 144 to the second light-emitting portion of the active layer; 146 to the second light-emitting portion of the second type binding layer; 150 to the second buffer layer region; 200 to the first conductive electrode; 3 0 0 ~ second conductive electrode; C; 1 ~ first lattice constant; C2 ~ second lattice constant; C3 ~ third lattice constant; C4 ~ fourth lattice constant; E ~ of the diode Electrically-excited light; B ~ blue wavelength light; F ~ fluorescent material is excited; and Y ~ yellow wavelength light.

0769-9102TWF(nl) ; VTERA-91-010-TW ; Phoelip.ptd 第23頁0769-9102TWF (nl); VTERA-91-010-TW; Phoelip.ptd page 23

Claims (1)

1224872 案號 92105775 六、申請專利範圍 1· 一種白光發光二極體,其至少包括· 一第一導電性電極; · 一基底,與上述第一導電性電極形 底包括绅化鎵(GaAs)、碟化鎵(GaP) 妾觸/且5亥基 (3C-sic); 夕(Si)或石反化矽 修正本 層及一 上,且 姻(A 1 G 層之上 成,其 層及一 衝層區 化鋁鎵 形成電 當 電極之 衝層區 第一波 長範圍 範圍之 第一發光部分第一型束缚層、—第 第一發光部分第二型束缚層依序形 構成第一發光部分,該第一發^ alnP)系化合物; 九^ 第一緩衝層區形成於上述第一發光 ,該第一緩衝層區係由BxGa(i—χ)ρ&1 中 0 $1、0 Sy $1 ; 第二發光部分第一型束缚層、一第 第一發光部分第一型束缚層依序形 上,且構成第二發光部分,該第二 銦(AlGalnN)系化合物;以及 第二導電性電極與上述第二發光部 接觸, 外加一電位差於第二導電性電極流 間時,產生一電流,此電流通過第 、及第一發光部分,使該第一發光 長範圍之光線、或第一發光部分活 之光線,且藉由該第一波長範圍之 光線混合獲致白光。 一發光部分活性 成於上述基底 分包括磷化鋁鎵 部分第二型束缚 ny Ga(1—y) N 所構 二發光部分活性 成於上迷第—& 發光部分包:ΐ 分第 型束缚 及該第~ ^ 二發光部< 部分活性馬 性層發出| 光線及第二 層1224872 Case No. 92105775 6. Scope of patent application 1. A white light-emitting diode, which includes at least a first conductive electrode; a substrate and the first conductive electrode shaped base including GaAs, GaP is in contact with and 5H-based (3C-sic); Si (Si) or stone-reversed silicon corrects this layer and the first layer, and the marriage (A 1 G layer is formed above, its layer and a The first light-emitting portion of the first light-emitting portion of the first layer of the first wavelength range and the second light-emitting portion of the first light-emitting portion of the first layer of the punching layer region of the electrical electrode in the punching layer sequentially form the first light-emitting portion. The first emission ^ alnP) series compound; nine ^ first buffer layer region is formed in the first light emission, the first buffer layer region is 0 $ 1, 0 Sy $ 1 in BxGa (i-χ) ρ &1; The two light emitting portions of the first type binding layer and the first light emitting portion of the first type binding layer are sequentially shaped and constitute a second light emitting portion, the second indium (AlGalnN) -based compound; and a second conductive electrode and the above. When the second light-emitting portion is in contact, and a potential difference is applied between the second conductive electrodes Generates a current, this current through the first, and the first light emitting portion, so that the light emitting wavelength range of the first or of the first light emitting part of a living, and by the light of the first wavelength range attainable mixed white light. A light-emitting part is active in the above-mentioned substrate, including the aluminum gallium phosphide part of the second type binding ny Ga (1-y) N. The two light-emitting part is active in the above-mentioned light-emitting part: ΐ sub-type binding And the first ~ ^ two light emitting parts < part of the active equine layer emits | light and the second layer 0769-9102TWfl(4.2) ; VTERA-91-010-TW ; ICE.ptc 第24頁0769-9102TWfl (4.2); VTERA-91-010-TW; ICE.ptc page 24 1224872 --—--裝號 921(1577^___年月日_修正__ /、、申δ奮專利範圍 2 ·如申請專利範圍第1項所述之白光發光二極體,其 中上述基底及上述第一發光部分第一型束缚層之間更存在 卓一緩衝層區。 3 ·如申請專利範圍第2項所述之白光發光二極體,其 中上述第一緩衝層及上述第二緩衝層之上下接面晶格常數 分別四配於上述第一發光部分第二型束缚層表面、上述第 二發光部分第一型束缚層底部、上述基底表面及上述第一 發光部分第一型束縛層底部之晶格常數。 4 ·如申請專利範圍第2項所述之白光發光二極體,其 中该第二緩衝層區係包括一由Bx G au_x) Ρ及I ny G a(1_y) Ν所構 成,其中 O^xSl、〇$y$l。 5 · —種白光發光二極體之製作方法,至少包括下列步 驟: 提供一基底,其與一第一導電性電極接觸,且該基底 包括砷化鎵(GaAs)、構化鎵(GaP)、矽(Si)或碳化矽(30 sic); 依序形成一第一發光部分第一型束缚層、一第一發光 部分活性層及一第一發光部分第二型束缚層於上述基底上 ’以構成第一發光部分,該第一發光部分包括磷化鋁鎵銦 (AlGal nP)系化合物; 形成一緩衝層區於上述第一發光部分第二型束缚層之 上,該緩衝層區係由BxGa(1_xJ及InyGa(w)N所構成,其中0 ^ X ^ 1 ' 0 ^ y ^ 1 ; 依序形成一第二發光部分第一型束缚層、一第二發光1224872 ----- installation number 921 (1577 ^ ___ year_revision__ / ,, apply for δFen patent scope 2 · white light-emitting diode as described in the first scope of the patent application, wherein the above substrate There is also a buffer region between the first type of the first light-emitting portion and the first type binding layer. 3 · The white light-emitting diode according to item 2 of the patent application scope, wherein the first buffer layer and the second buffer layer The lattice constants of the upper and lower junctions of the layer are respectively arranged on the surface of the first light-emitting portion second type tie layer, the bottom of the second light-emitting portion first type tie layer, the base surface, and the first light-emitting portion first type tie layer. Lattice constant at the bottom. 4 · The white light-emitting diode as described in item 2 of the patent application range, wherein the second buffer layer region includes a Bx G au_x) P and I ny G a (1_y) Ν Composition, where O ^ xSl, 〇 $ y $ l. 5 · A method for manufacturing a white light emitting diode, including at least the following steps: providing a substrate which is in contact with a first conductive electrode, and the substrate includes gallium arsenide (GaAs), structured gallium (GaP), Silicon (Si) or silicon carbide (30 sic); sequentially forming a first light emitting part, a first type binding layer, a first light emitting part, an active layer, and a first light emitting portion, a second type binding layer on the substrate; A first light-emitting portion is formed, and the first light-emitting portion includes an AlGal nP-based compound; a buffer layer region is formed on the second type binding layer of the first light-emitting portion, and the buffer layer region is made of BxGa (1_xJ and InyGa (w) N, in which 0 ^ X ^ 1 '0 ^ y ^ 1; sequentially forming a second light emitting part of the first type binding layer, a second light emitting 0769-9102TWfl(4.2) ; VTERA-91-010-TW ; ICE.ptc 第 25 頁0769-9102TWfl (4.2); VTERA-91-010-TW; ICE.ptc page 25 六、申請專利範圍 一^^2. _ 邛刀’舌性層及一第二發光部分一 區上,以構成第二發光部分,誃:型束缚層於上述緩衝層 鎵銦UlGalnN)系化合物·,以及"卓二發光部分包括氮化鋁 形成一第二導電性電極於上 缚層部分表面上。 、上述第二發光部分第二型束 方法6· ΐ !請專利範圍第5項所述白光發光二極體之製作 3中上述基底及上述第-發光部分第-型束缚層之 間更存在一第二緩衝層區。 7,·=申清專利乾圍第6項所述白光發光二極體之製作 晶格當^ ^十述第緩衝層及上述第二緩衝層之上下接面 面、上述第二發光部八Ϊ弟—發光部分第二型束缚層表 及上述第一發光部一型束缚層底部、上述基底表面 8·如申請專利範圍;f束缚層底部之晶格常數。 方法,其中該第二緩衝I。項所述白光發光二極體之製作 N所構成,其中〇 :區係包括一由BxGa(1_x)P及InyGa(1_y) 〜、0蕊y $ 1。Sixth, the scope of application for a patent ^^ 2. _ 邛 刀 'tongue layer and a second light-emitting part on a region to constitute a second light-emitting part, 誃: type binding layer on the above buffer layer gallium indium (UlGalnN) series compounds · And "The two light emitting parts include aluminum nitride to form a second conductive electrode on the surface of the upper tie layer part. 2. The second light emitting part and the second type beam method 6. ΐ! There is more between the above substrate and the first light emitting part and the first type binding layer in the production of the white light emitting diode described in item 5 of the patent scope. The second buffer layer region. 7, · = The lattice of the white light-emitting diode described in item 6 of Shenqing Patent Qianwei. ^ ^ The tenth buffer layer and the upper and lower contact surfaces of the second buffer layer, and the second light-emitting portion. The second-type binding layer surface of the light-emitting part and the bottom of the first-type binding layer of the first light-emitting portion and the above-mentioned substrate surface 8 as in the scope of the patent application; f Lattice constant at the bottom of the binding layer. Method, wherein the second buffer I. The white light emitting diode described in the item is composed of N, where 0: the system includes a BxGa (1_x) P and InyGa (1_y) ~, 0 y $ 1. 第26頁Page 26
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104124315A (en) * 2013-04-28 2014-10-29 晶元光电股份有限公司 Photoelectric element
TWI578564B (en) * 2013-04-23 2017-04-11 晶元光電股份有限公司 Optoelectronic device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI578564B (en) * 2013-04-23 2017-04-11 晶元光電股份有限公司 Optoelectronic device
CN104124315A (en) * 2013-04-28 2014-10-29 晶元光电股份有限公司 Photoelectric element
CN104124315B (en) * 2013-04-28 2018-11-30 晶元光电股份有限公司 Photoelectric cell

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