TWI459593B - Structure of light emitting diodes for increase of light emitting efficiency - Google Patents

Structure of light emitting diodes for increase of light emitting efficiency Download PDF

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TWI459593B
TWI459593B TW098120691A TW98120691A TWI459593B TW I459593 B TWI459593 B TW I459593B TW 098120691 A TW098120691 A TW 098120691A TW 98120691 A TW98120691 A TW 98120691A TW I459593 B TWI459593 B TW I459593B
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TW201101539A (en
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Fu Der Lai
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發光二極體增加發光效率之結構 Light-emitting diode structure for increasing luminous efficiency

本發明係有關於一種發光二極體增加發光效率之結構,尤其是指一種不僅可增加發光效率,同時能產生、誘發更多的光子,增加發光二極體之發光亮度,而在其整體施行使用上更增實用價值性之發光二極體增加發光效率之結構創新設計者。 The invention relates to a structure in which a light-emitting diode increases luminous efficiency, in particular, a method capable of not only increasing luminous efficiency, but also generating and inducing more photons and increasing the luminous brightness of the light-emitting diode, and performing the whole in its entirety. A structural innovation designer who uses a more practical value-added light-emitting diode to increase luminous efficiency.

按,近年來發光二極體的相關技術如雨後春筍般的蓬勃發展,各界研究的方向不外乎是如何提升發光二極體的內部量子效率〔Internal Quantum Efficiency〕、外部量子效率〔External Quantum Efficiency〕及光萃取率〔Light Extraction〕,於是有人開始將光子晶體之技術與發光二極體相結合,另外近年來也有些研究指出利用雷射在金屬與半導體介面激發表面電漿可增強光電流效應與量子效應,其目的無非是為了提高外部之量子效率徑而提升發光效率。 According to recent years, the related technologies of light-emitting diodes have sprung up, and the direction of research in all walks of life is nothing more than how to improve the internal quantum efficiency of the light-emitting diodes and the external quantum efficiency [External Quantum Efficiency]. And the light extraction rate [Light Extraction], so some people began to combine the technology of photonic crystals with light-emitting diodes. In addition, some studies in recent years have pointed out that the use of lasers to excite surface electrodes in metal and semiconductor interfaces can enhance the photocurrent effect. The quantum effect, its purpose is nothing more than to improve the external quantum efficiency path and improve luminous efficiency.

目前普遍使用的藍光發光二極體材料為氮化鎵〔GaN〕材料,氮化鎵在波長400nm時的折射率為2.5左右,是個折射率相當高的材料。因為如此,發光二極體產生的光大部分會被反射回材料內,最後被材料本身所吸收,導致較低的外部量子效率。儘管由於磊晶技術的改進,內部量 子效率可以達到90%以上,但是外部量子效率低,導致整體的發光效率變差。因此改善發光二極體之外部量子效率成為目前固態照明重要的課題之一。 The blue light-emitting diode material currently in common use is a gallium nitride (GaN) material, and gallium nitride has a refractive index of about 2.5 at a wavelength of 400 nm, and is a material having a relatively high refractive index. Because of this, most of the light produced by the LEDs is reflected back into the material and eventually absorbed by the material itself, resulting in lower external quantum efficiency. Despite the improvement of the epitaxial technology, the internal volume The sub-efficiency can reach more than 90%, but the external quantum efficiency is low, resulting in poor overall luminous efficiency. Therefore, improving the external quantum efficiency of the light-emitting diode has become one of the important topics in solid-state lighting.

於學者提出光子晶體的概念,指出電磁波在週期排列的介質中,會形成類似半導體能帶結構的能隙現象後。自此,光子晶體的研究便開始被發展與探討;利用光子晶體提升發光二極體之外部量子效率,一直都是光子晶體團隊研究的目標。 The concept of photonic crystals is proposed by scholars. It is pointed out that electromagnetic waves in a periodically arranged medium will form a band gap similar to that of a semiconductor band structure. Since then, the research of photonic crystals has been developed and explored; the use of photonic crystals to enhance the external quantum efficiency of light-emitting diodes has always been the goal of the photonic crystal team.

發光二極體若不加任何技術,只經由原本P-N Junction電子電洞結合的方式形成光子取出來,大約只有15%能夠轉換成光,其他則會因為折射、反射而或者留在半導體內部,被材料吸收,成為熱能損耗。因此發光二極體業者便需要發展許多技術,減少反射、設計有效折射或增加光耦合或光誘發,儘量讓光的取出效率增加,其中表面光子晶體化是一個相當成功的方式,使用該方式可以減少內部反射及向外散射的光。隨著分子束磊晶〔Molecular Beam Epitaxy;MBE〕和有機金屬化學氣相磊晶法〔Metal organic chemical vapor deposition;MOCVD〕磊晶技術的發展成熟,發光二極體的內部量子效率〔Internal Quantum Efficiency〕已經達到相當高的效率。 If the light-emitting diode is not added with any technology, only the original PN Junction electron hole is combined to form photons, and only about 15% can be converted into light, and others will be refraction, reflection or remain inside the semiconductor. The material absorbs and becomes a heat loss. Therefore, the light-emitting diode industry needs to develop many techniques to reduce reflection, design effective refraction or increase optical coupling or light induction, and try to increase the efficiency of light extraction. Surface photonic crystallization is a quite successful way. Reduce internal reflection and outward scattering of light. With the development of Molecular Beam Epitaxy (MBE) and Metal Organic Chemical Vapor Deposition (MOCVD), the internal quantum efficiency of the LED (Internal Quantum Efficiency) 〕 has achieved quite high efficiency.

內部量子效率的定義為順向電流注入發光二極體,在發光層中電子轉換成光子發光的數量比例。儘管目前所生產的高亮度發光二極體其內部的量子效率已經很高,但是外部量子效率還是很低,以藍光而言甚至不到10%,而造成其外部量子效率過低的原因有很多,如電流的非均勻分布或是因為半導體材料高折射係數及半導體裡一些缺陷的緣故導致光不 容易發射至外界而被半導體材料本身吸收或被基板吸收。因此真正的出光效率〔又稱之為外部量子效率;External Quantum Efficiency〕並不相等於內部量子效率,外部量子效率定義為內部量子效率乘上一取出效率〔Extraction Efficiency〕。 Internal quantum efficiency is defined as the ratio of the amount of electrons converted into photon luminescence in the luminescent layer by the forward current injection into the luminescent diode. Although the quantum brightness of the high-brightness light-emitting diodes currently produced is already high, the external quantum efficiency is still very low, even less than 10% in terms of blue light, and there are many reasons for the external quantum efficiency being too low. , such as the non-uniform distribution of current or because of the high refractive index of semiconductor materials and some defects in the semiconductor It is easily emitted to the outside and absorbed by the semiconductor material itself or absorbed by the substrate. Therefore, the true light extraction efficiency (also known as external quantum efficiency; External Quantum Efficiency) is not equal to the internal quantum efficiency, and the external quantum efficiency is defined as the internal quantum efficiency multiplied by the extraction efficiency [Extraction Efficiency].

光子晶體是在波長尺度上對物質進行物質結構的改造,使得該物質能夠控制光子的行為。光子晶體主要是在能隙結構中載入缺陷,形成破壞周期結構的局部區域,只有某些波長的光子才能在這個缺陷區域存在和傳播,而在這個區域以外的介質中,那些波長的光子能量是被禁止的。 Photonic crystals modify the material structure of a substance on a wavelength scale, enabling the substance to control the behavior of photons. Photonic crystals mainly load defects in the energy gap structure, forming a local region that destroys the periodic structure. Only photons of certain wavelengths can exist and propagate in this defect region, and in the medium outside this region, the photon energy of those wavelengths It is forbidden.

晶體內部的原子是周期性且呈現有序排列,正是這種周期勢場的存在,使得運動的電子受到周期勢場的布拉格散射,從而形成能帶結構,能帶與能帶之間可能存在帶隙。電子波的能量如果落在帶隙中,就無法繼續傳播,不論是電磁波還是光波只要受到周期性調制,都有能帶結構,也都有可能出現帶隙,而能量落在帶隙中的波同樣不能傳播。 The atoms inside the crystal are periodic and appear in an ordered arrangement. It is the existence of this periodic potential field that causes the moving electrons to be scattered by the Bragg of the periodic potential field, thus forming an energy band structure, and there may be a band between the energy band and the energy band. Bandgap. If the energy of the electron wave falls in the band gap, it cannot continue to propagate. Whether the electromagnetic wave or the light wave is periodically modulated, there is a band structure, and a band gap may occur, and the wave whose energy falls in the band gap The same cannot be spread.

換言之,半導體中離子的周期性排列產生了能帶結構,而能帶又控制著載流子在半導體中的運動。相同的在光子晶體中是由光的折射率指數的周期性變化產生了光帶隙結構,從而由光帶隙結構控制著光在光子晶體中的運動。 In other words, the periodic arrangement of ions in the semiconductor creates an energy band structure that in turn controls the movement of carriers in the semiconductor. The same in the photonic crystal is the optical band gap structure caused by the periodic variation of the refractive index of the light, so that the movement of the light in the photonic crystal is controlled by the optical band gap structure.

光子晶體的結構就如同半導體材料在晶格結點周期性的出現離子一樣,光子晶體是在高折射率材料的某些位置周期性的出現低折射率的材料。高低折射率的材料交替排列形成周期性結構就可以產生光子晶體帶隙,而周期排列的低折射率位點之間的距離大小不同,導致了一定距離大小的光子晶體只對一定頻率的光波產生能帶效應,也就是只有某種頻 率的光才會在某種周期距離一定的光子晶體中被完全禁止傳播。 The structure of a photonic crystal is just like the periodic appearance of a semiconductor material at a lattice junction. A photonic crystal is a material that periodically exhibits a low refractive index at certain locations of a high refractive index material. The high and low refractive index materials are alternately arranged to form a periodic structure to produce a photonic crystal band gap, and the distance between the periodically arranged low refractive index sites is different, resulting in a photonic crystal of a certain distance only generating light waves of a certain frequency. Band effect, that is, only some frequency The rate of light is completely forbidden to propagate in a photonic crystal with a certain period of time.

高亮度是發光二極體取代傳統照明設備所必需的條件,而要達到高亮度就同時必須提昇發光二極體的內部量子效率以及外部量子效率。內部量子效率藉由成熟的磊晶技術與先進的製程技術可以達到,而外部量子效率因為全內反射的關係,效率一直都相當的有限。 High brightness is a necessary condition for a light-emitting diode to replace a conventional lighting device, and to achieve high brightness, it is necessary to increase the internal quantum efficiency and external quantum efficiency of the light-emitting diode. Internal quantum efficiency can be achieved by sophisticated epitaxial technology and advanced process technology, while external quantum efficiency is always limited due to total internal reflection.

利用光子晶體提升發光二極體外部量子效率不外乎是克服它的全內反射,使得發光效率增加,其主要機制為: The use of photonic crystals to enhance the external quantum efficiency of a light-emitting diode is nothing more than overcoming its total internal reflection, resulting in an increase in luminous efficiency. The main mechanisms are:

1.表面的週期性結構造成光的散射,破壞原本應該被全內反射的光,而允許更多的光子逃離出材料。 1. The periodic structure of the surface causes scattering of light, destroying light that would otherwise be totally internally reflected, and allowing more photons to escape the material.

2.光子晶體形成特殊的能帶結構,而發光波長落在光子晶內,使得在氮化鎵發光二極體材料內的傳播模態〔guide mode〕被萃取出來。 2. The photonic crystal forms a special band structure, and the emission wavelength falls within the photonic crystal, so that the propagation mode in the gallium nitride light-emitting diode material is extracted.

此兩種機制效應有著不同的特性,第一種機制效應藉由散射方式提升出光量,其克服全反射方式類似於表面粗化,第二種機制效應主要是藉由能隙的方式將本來限制在材料中的傳播模態萃取出來。 The two mechanism effects have different characteristics. The first mechanism effect enhances the amount of light by means of scattering. The method of overcoming the total reflection is similar to the surface roughening. The second mechanism effect is mainly limited by the energy gap. Propagation mode extraction in the material.

然而,上述發光二極體結構設計雖可達到其既定的發光照明之預期功效,但於其實際操作施行使用上卻發現,該發光二極體之發光效率仍不佳,致令發光二極體在整體結構設計上仍存有改進之空間。 However, although the above-mentioned light-emitting diode structure design can achieve the intended effect of the predetermined light-emitting illumination, it is found that the luminous efficiency of the light-emitting diode is still poor, resulting in a light-emitting diode. There is still room for improvement in the overall structural design.

緣是,發明人有鑑於此,秉持多年該相關行業之豐富設計開發及實際製作經驗,針對現有之結構及缺失予以研究改良,提供一種發光二極體增加發光效率之結構,以期達到更佳實用價值性之目的者。 In view of this, the inventor has been in the process of researching and improving the existing structures and defects by providing rich experience in design and development and actual production of the relevant industries for many years, and providing a structure in which the light-emitting diodes increase luminous efficiency, in order to achieve better practicality. The purpose of value.

本發明之發光二極體增加發光效率之結構,其主要係於氮化 鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面,該錐形孔洞之開口直徑小於2μm,且錐形孔洞之深度為68.8nm~215.5nm,且同時於氮化鎵發光二極體磊晶片上披覆有微粒或膜層狀之單層奈米金屬層、亦或是微粒或膜層狀之一陶瓷層與一奈米金屬層;藉此,不僅可增加發光效率,同時能產生、誘發更多的光子,增加發光二極體之發光亮度,而在其整體施行使用上更增實用價值性者。 The structure of the light-emitting diode of the present invention increases luminous efficiency, which is mainly based on nitriding A gallium-emitting diode epitaxial wafer is formed with a rough surface having a plurality of tapered holes having an opening diameter of less than 2 μm and a tapered hole having a depth of 68.8 nm to 215.5 nm and simultaneously emitting a gallium nitride luminescence dipole The body-expanding wafer is coated with a single-layer nano-metal layer of a particle or a film layer, or a ceramic layer of a particle or a film layer and a nano metal layer; thereby, not only the luminous efficiency but also the luminous efficiency can be increased. Producing, inducing more photons, increasing the brightness of the light-emitting diodes, and increasing the practical value in its overall implementation.

第一圖:本發明之製作流程圖 First drawing: the flow chart of the invention

第二圖:本發明之錐形孔洞俯視放大示意圖 Second drawing: enlarged view of the tapered hole of the present invention

第三圖:本發明之錐形孔洞側視剖視放大示意圖(深度68.8nm) Third: enlarged side view of the tapered hole of the present invention (depth 68.8 nm)

第四圖:本發明之錐形孔洞側視剖視放大示意圖(深度118.5nm) Fourth drawing: enlarged side view of the tapered hole of the present invention (depth 118.5 nm)

第五圖:本發明之錐形孔洞側視剖視放大示意圖(深度165.6nm) Fig. 5 is a side elevational cross-sectional view showing the tapered hole of the present invention (depth 165.6 nm)

第六圖:本發明之錐形孔洞側視剖視放大示意圖(深度215.5nm) Figure 6 is a side elevational cross-sectional view of the tapered hole of the present invention (depth 215.5 nm)

第七圖:本發明具粗化之發光二極體之電流電壓量測圖 Figure 7: Current and voltage measurement diagram of the light-emitting diode with coarsening of the present invention

第八圖:本發明具粗化之發光二極體之光亮度量測圖 Figure 8: Photometric measurement of the light-emitting diode of the present invention with roughening

第九圖:本發明具光子誘發體之發光二極體之電流電壓量測圖 Ninth diagram: current and voltage measurement diagram of the light-emitting diode with photon inducer of the present invention

第十圖:本發明具光子誘發體之發光二極體之光亮度量測圖 Figure 10: Photoluminescence measurement of the light-emitting diode with photon inducer of the present invention

為令本發明所運用之技術內容、發明目的及其達成之功效有更完整且清楚的揭露,茲於下詳細說明之,並請一併參閱所揭之圖式及圖號:首先,請參閱第一圖本發明之製作流程圖所示,本發明主要係於氮化鎵發光二極體磊晶片上使用正光阻作為阻擋層(mask),利用蝕刻或機械加工方法之技術在氮化鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面,該錐形孔洞之開口直徑小於2μm,且錐形孔洞之深度為68.8nm~215.5nm,再披覆有微粒或膜層狀之單層奈米金屬層,此單層奈米金屬層當光子的誘發體,如:金(Au),亦或是微粒或膜層狀之一陶瓷層與一奈米金屬層,此一陶瓷層與一奈米金屬層當光子的誘發體,如:二氧化矽(SiO2)與金(Au),該微粒或膜層尺寸於3μm以下,再將之帶入後續之發光二極體元件的製程。 For a more complete and clear disclosure of the technical content, the purpose of the invention and the effects thereof achieved by the present invention, the following is a detailed description, and please refer to the drawings and drawings: First, please refer to The first figure shows the flow chart of the present invention. The present invention mainly uses a positive photoresist as a mask on a gallium nitride light-emitting diode epitaxial wafer, and emits light in gallium nitride by a technique of etching or mechanical processing. A rough surface having a plurality of tapered holes is formed on the diode epitaxial wafer, the opening diameter of the tapered hole is less than 2 μm, and the depth of the tapered hole is 68.8 nm to 215.5 nm, and the particle or film layer is coated. a layer of nano-metal, the single-layer nano-metal layer is a photon inducer, such as gold (Au), or a ceramic layer of a particle or a film layer and a nano metal layer, the ceramic layer A nano metal layer is an inducer of photons, such as cerium oxide (SiO2) and gold (Au), and the particle or film layer has a size of 3 μm or less, and is then brought into the subsequent process of the light-emitting diode element.

其中,該錐形孔洞詳細製程步驟描述如下: The detailed process steps of the tapered hole are described as follows:

一、晶片清洗(wafer cleanning) First, wafer cleaning (wafer cleanning)

依序將晶片浸放入鹽酸(HCL)、丙酮(ACE)、異丙醇(IPA)等溶劑之中,以超音波震盪器震盪清洗約3分鐘;重覆此步驟兩次。以超因波震盪器震盪清洗完成之後再以去離子水沖洗,將晶片表面殘留的有機液體洗去完全,最後再以低壓氮氣吹乾,完成清洗的步驟。 The wafer was immersed in a solvent such as hydrochloric acid (HCL), acetone (ACE), or isopropyl alcohol (IPA) in sequence, and washed with an ultrasonic oscillator for about 3 minutes; this step was repeated twice. After the shock cleaning by the hyper-wave oscillator is completed, the organic liquid remaining on the surface of the wafer is completely washed away by washing with deionized water, and finally dried by low-pressure nitrogen gas to complete the cleaning step.

二、光學微影(photolithography)技術定義孔洞陣列結構 Second, optical lithography (photolithography) technology defines the hole array structure

(1)烘烤:將晶片至於100℃的熱平台上軟烤2分鐘,以去除晶片表面之水汽。 (1) Baking: The wafer was soft baked on a hot plate at 100 ° C for 2 minutes to remove moisture on the surface of the wafer.

(2)光阻層塗佈:採用正光阻(EG-516),以3000rpm/min的轉速預轉10秒,再以5000rpm/min的轉速旋轉20秒。 (2) Photoresist layer coating: using a positive photoresist (EG-516), pre-rotating at 3000 rpm/min for 10 seconds, and then rotating at 5000 rpm/min for 20 seconds.

(3)軟烤光阻:將晶片置於100℃的熱平台上軟烤2分鐘,使圖像轉移時光阻不至沾黏於光罩上。 (3) Soft-baked photoresist: The wafer was placed on a hot plate at 100 ° C for 2 minutes, so that the light was not adhered to the mask when the image was transferred.

(4)曝光:將樣品試片置於光罩對準儀上,並以汞燈照射144mJ能量以完成圖像轉移。 (4) Exposure: The sample test piece was placed on a reticle aligner, and 144 mJ of energy was irradiated with a mercury lamp to complete image transfer.

(5)曝後烤:將晶片置於100℃的熱平台上軟烤4分鐘,以消除駐波效應。 (5) Bake after exposure: The wafer was placed on a hot plate at 100 ° C for 4 minutes to eliminate the standing wave effect.

(6)顯影:將曝光完成之晶片置於顯影液中,顯影50秒之後再以去離子水沖洗定影。 (6) Development: The exposed wafer was placed in a developing solution, developed for 50 seconds, and then rinsed with deionized water to fix.

(7)硬烤光阻:將晶片置於140℃的熱平台上硬烤40分鐘,以增加光阻層抗乾蝕刻的能力。 (7) Hard baked photoresist: The wafer was baked on a hot plate at 140 ° C for 40 minutes to increase the resistance of the photoresist layer to dry etching.

三、電感藕合電漿蝕刻系統(Inductively Coupled Plasma Etching System;ICP) Inductively Coupled Plasma Etching System (ICP)

使用電感藕合電漿蝕刻系統(Inductively Coupled Plasma Etching System;ICP),通入N2:5sccm、Ar:10sccm、CL2:20sccm氣體來蝕刻氮化鎵,而蝕刻後之奈米錐形孔洞圖形即如第二圖本發明之錐形孔洞俯視放大示意圖所示,且能依不同使用需求形成不同深度〔請一併參閱第三圖本發明之錐形孔洞側視剖視放大示意圖(深度68.8nm)、第四圖本發明之錐形孔洞側視剖視放大示意圖(深度118.5nm)、第五圖本發明之錐形孔洞側視剖視放大示意圖(深度165.6nm)及第六圖本發明之錐形孔洞側視剖視放大示意圖(深度215.5nm)所示〕。 Inductively Coupled Plasma Etching System (ICP) is used to pass through N2:5 sccm, Ar:10 sccm, and CL2:20 sccm gas to etch gallium nitride, and the tapered nanopore hole pattern is as follows. The second figure shows a tapered view of the tapered hole of the present invention, and can be formed into different depths according to different use requirements (please refer to the third figure for a side view of the tapered hole of the present invention (a depth of 68.8 nm), 4 is a side elevational cross-sectional view of a tapered hole of the present invention (depth 118.5 nm), a fifth side view of the tapered hole of the present invention, a side view (a depth of 165.6 nm) and a sixth figure of the present invention The enlarged side view of the hole is shown in an enlarged view (depth: 215.5 nm)].

如此一來,請參閱第七圖本發明具粗化(即表面具不同深度的錐形孔洞)之發光二極體之電流電壓量測圖所示,使得於蝕刻深度為68.8nm、118.5nm、165.6nm及215.5nm且電流20mA時,所量測之正向電壓(Vf)值分別為3.079伏特、3.047伏特、3.049伏特及3.074伏特,相較於對照組(STD)在20mA時所量測之正向電壓(Vf)值為2.997伏特約高出2.2%左右幾乎無明顯之增加。 In this way, please refer to the seventh figure, the current and voltage measurement diagram of the light-emitting diode with roughening (ie, tapered holes with different depths on the surface), so that the etching depth is 68.8 nm, 118.5 nm, The forward voltage (Vf) values measured at 165.6 nm and 215.5 nm at a current of 20 mA were 3.079 volts, 3.047 volts, 3.049 volts, and 3.074 volts, respectively, compared to the control group (STD) at 20 mA. The forward voltage (Vf) value of 2.997 volts is about 2.2% higher, with almost no significant increase.

另請再一併參閱第八圖本發明具粗化之發光二極體之光亮度量測圖所示,於氮化鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面的不同深度都有助於光的取出率,其平均光亮度增加了24%左右,其中又以深度165.6nm與對照組(STD)相比較增加30%為最多。 Please also refer to the eighth embodiment of the present invention, as shown in the light intensity measurement diagram of the light-emitting diode of the present invention, forming a rough surface having a plurality of tapered holes on the gallium nitride light-emitting diode. The depth contributes to the light extraction rate, and the average light brightness increases by about 24%, and the depth is 165.6 nm, which is the most increased by 30% compared with the control group (STD).

請再一併參閱第九圖本發明具光子誘發體(即於已粗化之氮化鎵發光二極體磊晶片的錐形孔洞內披覆陶瓷層(SiO2)及奈米金屬層)之發光二極體之電流電壓量測圖所示,使得於蝕刻深度為68.8nm、118.5nm、165.6nm及215.5nm且電流20mA時,所量測之正向電壓(Vf)值分別為3.089伏特、3.076伏特、3.087伏特及2.788伏特,相較於對照組(STD)在20mA時所量測之正向電壓(Vf)值為2.997伏特約高出2.9%左右幾乎無明顯之增加。 Please refer to the ninth figure for the luminescence of the photon inducer (that is, the ceramic layer (SiO2) and the nano metal layer in the tapered hole of the roughened gallium nitride light-emitting diode epitaxial wafer). The current and voltage measurements of the diode show that the measured forward voltage (Vf) values are 3.089 volts, 3.076 at etch depths of 68.8 nm, 118.5 nm, 165.6 nm, and 215.5 nm and currents of 20 mA, respectively. Volt, 3.087 volts, and 2.788 volts, the forward voltage (Vf) value measured at 20 mA compared to the control group (STD) was about 2.97 volts, which was about 2.9% higher than the apparent increase.

另請再一併參閱第十圖本發明具光子誘發體之發光二極體之光亮度量測圖所示,於氮化鎵發光二極體磊晶片上形成具有諸多不同深度的錐形孔洞再於錐形孔洞內披覆陶瓷層(SiO2)及奈米金屬層,使得光的取出率再提高,其平均光亮度增加53%左右,其中又以深度1700Å(165.6nm)與對照組(STD)相比較增加61%為最多,且由於在氮化鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面,故注入的電流大部份由離發光層較遠 處注入,所以不會有漏電流之情況發生。 Please also refer to the tenth figure of the photoluminescence of the photon-inducing body of the present invention, and form a tapered hole having a plurality of different depths on the gallium nitride light-emitting diode. The ceramic layer (SiO2) and the nano-metal layer are covered in the tapered hole, so that the light extraction rate is increased, and the average brightness is increased by about 53%, and the depth is 1700 Å (165.6 nm) and the control group (STD). Compared with the increase of 61%, and because of the rough surface with many tapered holes formed on the gallium nitride light-emitting diode, the injected current is mostly far from the light-emitting layer. Injected, so there will be no leakage current.

藉由以上所述,該架構之組成與使用實施說明可知,本發明與現有架構相較之下,本發明由於主要係於氮化鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面,且同時於氮化鎵發光二極體磊晶片上披覆有微粒或膜層狀之單層奈米金屬層、亦或是微粒或膜層狀之一陶瓷層與一奈米金屬層當光子的誘發體,不僅可增加發光效率,同時能產生、誘發更多的光子,增加發光二極體之發光亮度,而在其整體施行使用上更增實用價值性者。 As described above, the composition and use of the architecture show that the present invention is compared with the existing architecture, and the present invention is mainly formed on the gallium nitride light-emitting diode epitaxial wafer to form a rough surface having a plurality of tapered holes. And at the same time, on the gallium nitride light-emitting diode epitaxial wafer, a single-layer nano-metal layer coated with a particle or a film layer, or a ceramic layer of a particle or a film layer and a nano metal layer are The photon inducer not only increases the luminous efficiency, but also generates and induces more photons, increases the luminance of the light-emitting diode, and increases the practical value in its overall implementation.

然而前述之實施例或圖式並非限定本發明之產品結構或使用方式,任何所屬技術領域中具有通常知識者之適當變化或修飾,皆應視為不脫離本發明之專利範疇。 However, the above-described embodiments or drawings are not intended to limit the structure or the use of the present invention, and any suitable variations or modifications of the invention will be apparent to those skilled in the art.

綜上所述,本發明實施例確能達到所預期之使用功效,又其所揭露之具體構造,不僅未曾見諸於同類產品中,亦未曾公開於申請前,誠已完全符合專利法之規定與要求,爰依法提出發明專利之申請,懇請惠予審查,並賜准專利,則實感德便。 In summary, the embodiments of the present invention can achieve the expected use efficiency, and the specific structure disclosed therein has not been seen in similar products, nor has it been disclosed before the application, and has completely complied with the provisions of the Patent Law. And the request, the application for the invention of a patent in accordance with the law, please forgive the review, and grant the patent, it is really sensible.

Claims (14)

一種發光二極體增加發光效率之結構,其主要係於氮化鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面,該錐形孔洞之開口直徑小於2μm,且錐形孔洞之深度為68.8nm~215.5nm,且於氮化鎵發光二極體磊晶片上披覆金屬層。 A structure in which a light-emitting diode increases luminous efficiency, and is mainly formed on a gallium nitride light-emitting diode epitaxial wafer to form a rough surface having a plurality of tapered holes having an opening diameter of less than 2 μm and a taper The depth of the hole is 68.8 nm to 215.5 nm, and the metal layer is coated on the gallium nitride light emitting diode. 如申請專利範圍第1項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上所形成之錐形孔洞粗糙面係以蝕刻方式蝕刻形成。 The structure of the light-emitting diode according to claim 1, wherein the tapered surface of the gallium nitride light-emitting diode is formed by etching. 如申請專利範圍第1項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上所形成之錐形孔洞粗糙面係以機械加工方法形成。 The structure of the light-emitting diode according to claim 1, wherein the tapered hole rough surface formed on the gallium nitride light-emitting diode wafer is formed by a mechanical processing method. 如申請專利範圍第1項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之金屬層為微粒狀。 The structure of the light-emitting diode according to claim 1, wherein the metal layer coated on the gallium nitride light-emitting diode is in the form of particles. 如申請專利範圍第1項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之金屬層為膜層狀。 The structure of the light-emitting diode according to claim 1 is characterized in that the metal layer coated on the gallium nitride light-emitting diode is a film layer. 如申請專利範圍第1項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之金屬層為金(Au)。 The structure of the light-emitting diode according to claim 1 is characterized in that the metal layer coated on the gallium nitride light-emitting diode is gold (Au). 如申請專利範圍第1項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之金屬層尺寸於3μm以下。 The structure of the light-emitting diode according to claim 1 is characterized in that the metal layer of the gallium nitride light-emitting diode is over 3 μm . 一種發光二極體增加發光效率之結構,其主要係主要係於氮化鎵發光二極體磊晶片上形成具有諸多錐形孔洞之粗糙面,該錐形孔洞之開口直徑小於2μm,且錐形孔洞之深度為68.8nm~215.5nm,且於氮化鎵發光二極體磊晶 片上披覆一陶瓷層與一金屬層。 A structure in which a light-emitting diode increases luminous efficiency, which is mainly formed on a gallium nitride light-emitting diode epitaxial wafer to form a rough surface having a plurality of tapered holes having an opening diameter of less than 2 μm , and The tapered hole has a depth of 68.8 nm to 215.5 nm, and a ceramic layer and a metal layer are coated on the gallium nitride light emitting diode. 如申請專利範圍第8項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上所形成之錐形孔洞粗糙面係以蝕刻方式蝕刻形成。 The structure of the light-emitting diode according to claim 8 is characterized in that the tapered hole rough surface formed on the gallium nitride light-emitting diode wafer is etched by etching. 如申請專利範圍第8項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上所形成之錐形孔洞粗糙面係以機械加工方法形成。 The structure of the light-emitting diode according to claim 8 is characterized in that the tapered hole rough surface formed on the gallium nitride light-emitting diode wafer is formed by a mechanical processing method. 如申請專利範圍第8項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之一陶瓷層與一金屬層為微粒狀。 The light-emitting diode according to claim 8 is characterized in that the GaN light-emitting diode is coated with a ceramic layer and a metal layer in a particulate form. 如申請專利範圍第8項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之一陶瓷層與一金屬層為膜層狀。 The light-emitting diode according to claim 8 is characterized in that the GaN light-emitting diode is coated with a ceramic layer and a metal layer as a film layer. 如申請專利範圍第8項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之陶瓷層為二氧化矽(SiO2)、金屬層為金(Au)。 The structure of the light-emitting diode according to claim 8 is characterized in that the ceramic layer coated on the gallium nitride light-emitting diode is cerium oxide (SiO2) and the metal layer is gold ( Au). 如申請專利範圍第8項所述發光二極體增加發光效率之結構,其中,該氮化鎵發光二極體磊晶片上披覆之一陶瓷層與一金屬層尺寸於3μm以下。 The light-emitting diode according to claim 8 is characterized in that the GaN light-emitting diode is coated with a ceramic layer and a metal layer having a size of 3 μm or less.
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TW200847482A (en) * 2006-11-28 2008-12-01 Luxtaltek Corp Pyramidal photonic crystal light emitting device
TW200832740A (en) * 2007-01-24 2008-08-01 Tera Xtal Technology Corp Light emitting diode structure and manufacturing method of the same
TW200924248A (en) * 2007-09-28 2009-06-01 Samsung Electro Mech Method of forming fine patterns and method of manufacturing semiconductor light emitting device using the same

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