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CN107819059A - Nitride semiconductor structure and semiconductor light emitting element - Google Patents

Nitride semiconductor structure and semiconductor light emitting element Download PDF

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CN107819059A
CN107819059A CN201711125219.4A CN201711125219A CN107819059A CN 107819059 A CN107819059 A CN 107819059A CN 201711125219 A CN201711125219 A CN 201711125219A CN 107819059 A CN107819059 A CN 107819059A
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type semiconductor
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nitride
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王信介
李玉柱
吴俊德
林京亮
李允立
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Genesis Photonics Inc
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/811Bodies having quantum effect structures or superlattices, e.g. tunnel junctions
    • H10H20/812Bodies having quantum effect structures or superlattices, e.g. tunnel junctions within the light-emitting regions, e.g. having quantum confinement structures
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/815Bodies having stress relaxation structures, e.g. buffer layers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/816Bodies having carrier transport control structures, e.g. highly-doped semiconductor layers or current-blocking structures
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/816Bodies having carrier transport control structures, e.g. highly-doped semiconductor layers or current-blocking structures
    • H10H20/8162Current-blocking structures
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/822Materials of the light-emitting regions
    • H10H20/824Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP
    • H10H20/825Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/822Materials of the light-emitting regions
    • H10H20/824Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP
    • H10H20/825Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN
    • H10H20/8252Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN characterised by the dopants

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Abstract

The invention relates to a nitride semiconductor structure and a semiconductor light-emitting element. The nitride semiconductor structure is mainly provided with a light emitting layer between an N-type semiconductor layer and a P-type semiconductor layer, a quaternary carrier active layer is arranged between the light emitting layer and the P-type semiconductor layer, and the quaternary carrier active layer is aluminum indium gallium Al nitridexInyGa1‑x‑yN, wherein x and y are 0<x<1、0<y<1、0<x+y<A value of 1. The semiconductor light-emitting element comprises the nitride semiconductor structure on a substrate, and an N-type electrode and a P-type electrode which are matched with each other to provide electric energy. Therefore, compared with the known P-AlGaN electron blocking layer, the nitride semiconductor structure and the semiconductor light-emitting element can improve the effect that holes enter the multi-quantum well structure, and simultaneously achieve the purpose of inhibiting electrons from escaping to enter the P-type semiconductor layer, so that the combination probability of the holes is increased, and the light-emitting efficiency is further improved.

Description

氮化物半导体结构及半导体发光元件Nitride semiconductor structure and semiconductor light emitting element

相关分案申请related divisional application

本申请为申请日为2013年1月25日,申请号为201310028759.6,发明名称为“氮化物半导体结构及半导体发光元件”的专利的分案申请。This application is a divisional application of a patent with an application date of January 25, 2013, an application number of 201310028759.6, and an invention title of "Nitride Semiconductor Structure and Semiconductor Light-Emitting Element".

技术领域technical field

本发明有关于一种氮化物半导体结构及半导体发光元件,尤其是指一种于发光层与P型半导体层间配置有一氮化铝铟镓AlxInyGa1-x-yN的四元载子活性层的氮化物半导体结构及半导体发光元件,属于半导体技术领域。The present invention relates to a nitride semiconductor structure and a semiconductor light-emitting element, in particular to a quaternary carrier in which aluminum indium gallium nitride Al x In y Ga 1-xy N is arranged between a light-emitting layer and a P-type semiconductor layer A nitride semiconductor structure of an active layer and a semiconductor light-emitting element belong to the technical field of semiconductors.

背景技术Background technique

近年来,由于磊晶与工艺技术的进步,使发光二极管成为极具潜力的固态照明光源之一;其中,以氮化镓(GaN)为主要制造材料的发光二极管现已成为固态照明(Solid-state lighting,SSL)建造中的重要元件之一;氮化镓LED由于具有元件体积小、无汞污染、发光效率高及寿命长等优点,已成为最新兴的光电半导体材料之一,且其发光波长几乎涵盖了可见光的范围,更使其成为极具潜力的发光二极管材料。In recent years, due to the advancement of epitaxy and process technology, light-emitting diodes have become one of the most promising solid-state lighting sources; among them, light-emitting diodes with gallium nitride (GaN) as the main manufacturing material have now become solid-state lighting (Solid- State lighting (SSL) is one of the important components in the construction; gallium nitride LED has become one of the latest optoelectronic semiconductor materials due to its advantages of small size, no mercury pollution, high luminous efficiency and long life, and its luminous The wavelength almost covers the range of visible light, making it a very potential material for light-emitting diodes.

一般而言,氮化镓LED是将一缓冲层先形成于基板上,再于缓冲层上依序磊晶成长N型半导体层、发光层以及P型半导体层;接着,利用微影与蚀刻工艺移除部分的P型半导体层、部分的发光层,直至暴露出部分的N型半导体层为止;然后,分别于N型半导体层的暴露部分以及P型半导体层上形成N型电极与P型电极,而制作出发光二极管;其中,发光层为多重量子井结构(MQW),而多重量子井结构包括以重复的方式交替设置的量子井层(well)和量子阻障层(barrier),因为量子井层具有相对量子阻障层较低的能隙,使得在上述多重量子井结构中的每一个量子井层可以在量子力学上限制电子和电洞,造成电子和电洞分别从N型半导体层和P型半导体层注入,并在量子井层中结合,而发射出光子。Generally speaking, a gallium nitride LED first forms a buffer layer on the substrate, and then epitaxially grows an N-type semiconductor layer, a light-emitting layer, and a P-type semiconductor layer on the buffer layer; then, using lithography and etching processes removing part of the P-type semiconductor layer and part of the light-emitting layer until a part of the N-type semiconductor layer is exposed; then, forming an N-type electrode and a P-type electrode on the exposed part of the N-type semiconductor layer and the P-type semiconductor layer respectively , and produce a light-emitting diode; wherein, the light-emitting layer is a multiple quantum well structure (MQW), and the multiple quantum well structure includes quantum well layers (well) and quantum barrier layers (barrier) that are alternately arranged in a repeated manner, because quantum The well layer has a relatively lower energy gap than the quantum barrier layer, so that each quantum well layer in the above-mentioned multiple quantum well structure can limit electrons and holes quantum mechanically, causing electrons and holes to flow from the N-type semiconductor layer respectively. It is injected into the P-type semiconductor layer and combined in the quantum well layer to emit photons.

然而,上述的发光二极管因诸多因素(例如:电流拥塞(current crowding)、差排缺陷(dislocation)等),进而影响其发光效率;理论上,发光二极管的发光效率取决于外部量子效率与其本身的内部量子效率(internal quantum efficiency)及光取出效率(light-extraction efficiency);所谓的内部量子效率是由材料特性及质量所决定,至于光取出效率则是从元件内部发出至周围空气的辐射比例,光取出效率是取决于当辐射离开元件内部时所发生的损耗,造成上述损耗的主要原因之一是由于形成元件的表面层的半导体材料具有高折射系数(refraction coefficient),导致光在该材料表面产生全反射(total reflection)而无法发射出去,而若光取出效率提升,则半导体发光元件的外部量子效率亦随之提升;因此,针对提升内部量子效率以及光取出效率,近几年已发展出许多技术,例如使用铟锡氧化物(Indium Tin Oxide;ITO)当电流传输层、采用覆晶结构(flip-chip)、利用图形化(PSS)的蓝宝石基板,以及使用电流阻挡层(current block layer;CBL)等;其中,于提升内部量子效率的技术中,亦有业者于多重量子井结构与P型半导体层之间配置有一层高能隙(band gap)的P型载子阻隔层,其又可称为电子阻挡层(electronblocking layer,EBL),进而使得更多的载子被局限在量子井层中,以提高电子电洞覆合的机率,增加发光效率,进而达到发光二极管亮度提升的功效。However, the luminous efficiency of the aforementioned light-emitting diodes is affected by many factors (such as current crowding, dislocation, etc.); theoretically, the luminous efficiency of a light-emitting diode depends on the external quantum efficiency and its own Internal quantum efficiency (internal quantum efficiency) and light-extraction efficiency (light-extraction efficiency); the so-called internal quantum efficiency is determined by the characteristics and quality of the material, and the light-extraction efficiency is the ratio of radiation emitted from the inside of the component to the surrounding air. The light extraction efficiency depends on the loss that occurs when the radiation leaves the interior of the element. One of the main reasons for the above loss is that the semiconductor material forming the surface layer of the element has a high refraction coefficient (refraction coefficient), which causes light to pass through the surface of the material Total reflection (total reflection) cannot be emitted, and if the light extraction efficiency is improved, the external quantum efficiency of the semiconductor light-emitting element will also be improved; therefore, in recent years, in order to improve the internal quantum efficiency and light extraction efficiency, developed Many technologies, such as using Indium Tin Oxide (ITO) as a current transport layer, using a flip-chip structure (flip-chip), using a patterned (PSS) sapphire substrate, and using a current block layer (current block layer) ; CBL) etc.; wherein, in the technology of improving the internal quantum efficiency, there is also a P-type carrier blocking layer with a high energy gap (band gap) between the multiple quantum well structure and the P-type semiconductor layer, which is also It can be called electron blocking layer (electronblocking layer, EBL), so that more carriers are confined in the quantum well layer, so as to increase the probability of electron hole recombination, increase the luminous efficiency, and then achieve the effect of improving the brightness of light emitting diodes .

现有的电子阻挡层由具有相当大能隙的P型AlGaN层形成,由此防止由N型半导体层注入的电子溢流至P型半导体层中,使得电子可有效地限制在量子井层内,以提升发光二极管的内部量子效率;然而,P-AlGaN的电子阻挡层虽具有相当大的能隙以阻挡电子溢流现象,但相对地亦导致电洞注入发光层的效果变差;再者,由于多重量子井结构一般是以InGaN的量子井层以及GaN的量子阻障层所形成,而本质上,P-AlGaN的电子阻挡层和GaN的量子阻障层具有非常高的晶格错配,使得InGaN量子井层因晶格错配会严重地受到压缩应力的作用,而这种压缩应力改变了每一个量子井层的能带结构,从而使在量子井层内的电子和电洞在空间上彼此分开,导致发光二极管的发光效率降低;再者,上述压缩应力亦会劣化相邻的GaN量子阻障层和InGaN量子井层之间的界面特性,从而在界面处损失载子,亦影响发光二极管的的发光效率。The existing electron blocking layer is formed of a P-type AlGaN layer with a relatively large energy gap, thereby preventing electrons injected from the N-type semiconductor layer from overflowing into the P-type semiconductor layer, so that the electrons can be effectively confined in the quantum well layer , to improve the internal quantum efficiency of light-emitting diodes; however, although the electron blocking layer of P-AlGaN has a considerable energy gap to prevent electron overflow, it also leads to a relatively poor effect of hole injection into the light-emitting layer; moreover , because the multiple quantum well structure is generally formed by the quantum well layer of InGaN and the quantum barrier layer of GaN, but in essence, the electron blocking layer of P-AlGaN and the quantum barrier layer of GaN have a very high lattice mismatch , so that the InGaN quantum well layer will be seriously affected by compressive stress due to lattice mismatch, and this compressive stress changes the energy band structure of each quantum well layer, so that the electrons and holes in the quantum well layer Spatially separated from each other, resulting in a reduction in the luminous efficiency of the light-emitting diode; moreover, the above-mentioned compressive stress will also deteriorate the interface characteristics between the adjacent GaN quantum barrier layer and the InGaN quantum well layer, thereby losing carriers at the interface, and also Affects the luminous efficiency of light-emitting diodes.

鉴于上述现有的氮化物半导体发光元件在实际实施上仍具有多处的缺失,因此,研发出一种新型的氮化物半导体结构及半导体发光元件仍是本领域亟待解决的问题之一。In view of the fact that the existing nitride semiconductor light-emitting elements still have many deficiencies in actual implementation, it is still one of the problems to be solved urgently in this field to develop a novel nitride semiconductor structure and semiconductor light-emitting element.

发明内容Contents of the invention

为解决上述技术问题,本发明的主要目的为提供一种氮化物半导体结构,其通过于发光层与P型半导体层间配置一氮化铝铟镓AlxInyGa1-x-yN的四元载子活性层,以提升电洞进入多重量子井结构的效果,同时亦可达到避免电子逃逸进入P型半导体层的目的,使得电子与电洞结合机率增加,以获得良好的发光效率。In order to solve the above-mentioned technical problems, the main purpose of the present invention is to provide a nitride semiconductor structure, which is configured by a quaternary of aluminum indium gallium nitride Al x In y Ga 1-xy N between the light-emitting layer and the P-type semiconductor layer. The carrier active layer is used to enhance the effect of holes entering the multiple quantum well structure, and at the same time, it can also achieve the purpose of preventing electrons from escaping into the P-type semiconductor layer, so that the combination probability of electrons and holes is increased to obtain good luminous efficiency.

为达上述目的,本发明提供一种氮化物半导体结构,其包含一N型半导体层以及一P型半导体层,于N型半导体层与P型半导体层间配置有一发光层,发光层与P型半导体层间配置有一四元载子活性层,且四元载子活性层为氮化铝铟镓AlxInyGa1-x-yN,其中x及y为满足0<x<1、0<y<1、0<x+y<1的数值。其中,优选地,所述四元载子活性层的x范围为0<x≤0.4;此外,优选地,所述四元载子活性层的y范围为0<y≤0.2。To achieve the above object, the present invention provides a nitride semiconductor structure, which includes an N-type semiconductor layer and a P-type semiconductor layer, a light-emitting layer is arranged between the N-type semiconductor layer and the P-type semiconductor layer, and the light-emitting layer and the P-type semiconductor layer A quaternary carrier active layer is arranged between the semiconductor layers, and the quaternary carrier active layer is aluminum indium gallium nitride Al x In y Ga 1-xy N, where x and y satisfy 0<x<1, 0< The value of y<1, 0<x+y<1. Wherein, preferably, the range of x of the quaternary carrier active layer is 0<x≤0.4; moreover, preferably, the range of y of the quaternary carrier active layer is 0<y≤0.2.

根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述发光层具有多重量子井结构,且多重量子井结构可由氮化铟镓的井层及氮化镓的阻障层交替堆栈所形成,且紧邻于多重量子井结构的最后一井层的四元载子活性层的能隙大于多重量子井结构的阻障层的能隙;其中,更优选地,所述四元载子活性层的能隙高于阻障层的能隙1%-15%。由此,其与公知的P-AlGaN电子阻挡层相较下,不仅提升电洞进入多重量子井结构的效果,亦同时达到抑制电子逃逸进入P型半导体层的目的,使得电子与电洞结合机率增加,进一步提升发光效率。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, the light-emitting layer has a multiple quantum well structure, and the multiple quantum well structure can be composed of a well layer of indium gallium nitride and a barrier layer of gallium nitride. The energy gap of the quaternary carrier active layer formed by alternating stacks and adjacent to the last well layer of the multiple quantum well structure is greater than the energy gap of the barrier layer of the multiple quantum well structure; wherein, more preferably, the quaternary The energy gap of the carrier active layer is 1%-15% higher than that of the barrier layer. Therefore, compared with the known P-AlGaN electron blocking layer, it not only improves the effect of holes entering the multiple quantum well structure, but also achieves the purpose of inhibiting electrons from escaping into the P-type semiconductor layer, so that the probability of electrons and holes combining increase to further enhance the luminous efficiency.

根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述四元载子活性层掺杂有浓度为1016-1019cm-3的第四主族元素;更优选地,所述第四主族元素为碳;由此利用第四主族元素取代五价的氮原子,以多一个带正电电洞,使得四元载子活性层可具有高电洞浓度,以提供更多的电洞进入发光层,进而增加电子电洞结合的情况。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, the quaternary carrier active layer is doped with elements of the fourth main group at a concentration of 10 16 -10 19 cm -3 ; more preferably , the fourth main group element is carbon; thus, the fourth main group element is used to replace the pentavalent nitrogen atom to have one more positively charged hole, so that the quaternary carrier active layer can have a high hole concentration to Provide more holes into the light-emitting layer, thereby increasing the combination of electrons and holes.

根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述四元载子活性层掺杂有浓度大于1018cm-3的P型掺质。其中,更优选地,所述P型掺质可例如为镁。According to a specific embodiment of the present invention, preferably, in the above nitride semiconductor structure, the quaternary carrier active layer is doped with a P-type dopant with a concentration greater than 10 18 cm −3 . Wherein, more preferably, the P-type dopant may be, for example, magnesium.

根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述四元载子活性层的厚度为50-300nm。According to a specific embodiment of the present invention, preferably, in the above nitride semiconductor structure, the thickness of the quaternary carrier active layer is 50-300 nm.

另外,根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,于发光层与N型半导体层间亦可配置有一N型载子阻隔层(例如为N型氮化铝镓等),且N型载子阻隔层由具有大于发光层的能隙的材料所制成,同理,N型载子阻隔层由具有高于发光层的能隙的材料所制成,以避免电洞逃逸进入N型半导体层内,以提高电子电洞结合的机率。In addition, according to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, an N-type carrier blocking layer (such as N-type aluminum gallium nitride, etc.) may also be arranged between the light-emitting layer and the N-type semiconductor layer. ), and the N-type carrier blocking layer is made of a material with an energy gap larger than that of the light-emitting layer. Similarly, the N-type carrier blocking layer is made of a material with a higher energy gap than the light-emitting layer to avoid electrical Holes escape into the N-type semiconductor layer to increase the probability of electron-hole combination.

本发明还提供一种半导体发光元件,其至少包含有:The present invention also provides a semiconductor light emitting element, which at least includes:

一基板;a substrate;

一N型半导体层,其配置于所述基板上;an N-type semiconductor layer configured on the substrate;

一发光层,其配置于所述N型半导体层上;a light-emitting layer configured on the N-type semiconductor layer;

一四元载子活性层,其配置于所述发光层上,所述四元载子活性层为氮化铝铟镓AlxInyGa1-x-yN,其中x及y为满足0<x<1、0<y<1、0<x+y<1的数值;A quaternary carrier active layer, which is arranged on the light-emitting layer, the quaternary carrier active layer is aluminum indium gallium nitride Al x In y Ga 1-xy N, where x and y satisfy 0<x Values <1, 0<y<1, 0<x+y<1;

一P型半导体层,其配置于所述四元载子活性层上;A P-type semiconductor layer configured on the quaternary carrier active layer;

一N型电极,其以欧姆接触配置于所述N型半导体层上;以及an N-type electrode disposed on the N-type semiconductor layer in ohmic contact; and

一P型电极,其以欧姆接触配置于所述P型半导体层上。A P-type electrode is configured on the P-type semiconductor layer by ohmic contact.

本发明的半导体发光元件于一基板上包含上述的氮化物半导体结构,以及二相配合提供电能的N型电极与P型电极;由此,控制四元载子活性层中铟的含量,使得四元载子活性层的能隙高于阻障层的能隙,不仅可提升电洞进入多重量子井结构,以及达到抑制电子逃逸进入P型半导体层的功效,使得电子与电洞结合机率增加,更可作为P型半导体层与发光层间的缓冲层,以改善P型半导体层与发光层所产生的晶格失配造成晶体质量劣化的问题;此外,通过四元载子活性层的第四主族元素掺质可降低因Mg-H键结所造成的不活化现象,使Mg活化而具有受体的有效作用,进而使得四元载子活性层具有高电洞浓度,提供更多的电洞进入发光层,增加电子电洞结合的情况,以便半导体发光元件可呈现出足够低的阻抗,进而获得更佳的发光效率。The semiconductor light-emitting element of the present invention includes the above-mentioned nitride semiconductor structure on a substrate, and two N-type electrodes and P-type electrodes that cooperate to provide electric energy; thus, the content of indium in the quaternary carrier active layer is controlled, so that four The energy gap of the meta-carrier active layer is higher than the energy gap of the barrier layer, which not only enhances the entry of holes into the multiple quantum well structure, but also achieves the effect of inhibiting electrons from escaping into the P-type semiconductor layer, increasing the probability of electrons and holes combining. It can also be used as a buffer layer between the P-type semiconductor layer and the light-emitting layer to improve the problem of crystal quality degradation caused by the lattice mismatch between the P-type semiconductor layer and the light-emitting layer; The main group element dopant can reduce the inactivation phenomenon caused by the Mg-H bond, activate the Mg and have the effective effect of the acceptor, and then make the quaternary carrier active layer have a high hole concentration and provide more electricity. Holes enter the light-emitting layer to increase the combination of electrons and holes, so that the semiconductor light-emitting element can exhibit a sufficiently low impedance, thereby obtaining better luminous efficiency.

再者,根据本发明的具体实施方式,优选地,在上述半导体发光元件中,亦可于基板与N型半导体层间表面形成有一缓冲层,所述缓冲层为氮化铝镓AlzGa1-zN,其中0<z<1;以解决因晶格差异所产生的磊晶差排现象。Furthermore, according to a specific embodiment of the present invention, preferably, in the above-mentioned semiconductor light-emitting element, a buffer layer may also be formed on the surface between the substrate and the N-type semiconductor layer, and the buffer layer is aluminum gallium nitride Al z Ga 1 -z N, where 0<z<1; to solve epitaxial dislocation caused by lattice difference.

附图说明Description of drawings

图1为本发明的一优选实施例提供的氮化物半导体结构的剖面示意图。FIG. 1 is a schematic cross-sectional view of a nitride semiconductor structure provided by a preferred embodiment of the present invention.

图2为根据本发明的优选实施例提供的氮化物半导体结构所制作的半导体发光元件的剖面示意图。Fig. 2 is a schematic cross-sectional view of a semiconductor light-emitting element made of a nitride semiconductor structure according to a preferred embodiment of the present invention.

主要组件符号说明:Description of main component symbols:

1基板 2N型半导体层1 Substrate 2N-type semiconductor layer

21N型电极 3P型半导体层21N type electrode 3P type semiconductor layer

31P型电极 4发光层31P type electrode 4 light-emitting layer

41阻障层 42井层41 barrier layer 42 well layer

5四元载子活性层 6N型载子阻隔层5 Quaternary carrier active layer 6N-type carrier blocking layer

7缓冲层7 buffer layers

具体实施方式Detailed ways

本发明的目的及其结构设计功能上的优点,将依据以下附图及优选实施例予以说明,以对本发明有更深入且具体的了解。The purpose of the present invention and its structural design and functional advantages will be described according to the following drawings and preferred embodiments, so as to have a more in-depth and specific understanding of the present invention.

首先,在以下实施例的描述中,应当理解当指出一层(或膜)或一结构配置在另一个基板、另一层(或膜)、或另一结构“上”或“下”时,其可“直接”位于其它基板、层(或膜)、或另一结构,亦或者两者间具有一个以上的中间层以“间接”方式配置,可参照附图说明每一层所在位置。First, in the description of the following embodiments, it should be understood that when it is indicated that a layer (or film) or a structure is disposed "on" or "under" another substrate, another layer (or film), or another structure, It can be "directly" located on other substrates, layers (or films), or another structure, or can be configured "indirectly" with more than one intermediate layer between them. The location of each layer can be described with reference to the drawings.

请参阅图1所示,其为本发明的一优选实施例提供的氮化物半导体结构的剖面示意图,其包含有一N型半导体层2以及一P型半导体层3,于N型半导体层2与P型半导体层3间配置有一发光层4(active layer),发光层4与P型半导体层3间配置有一四元载子活性层5,且四元载子活性层5为氮化铝铟镓AlxInyGa1-x-yN,其中x及y为满足0<x<1、0<y<1、0<x+y<1的数值;此外,上述的四元载子活性层5掺杂有浓度为1016-1019cm-3的第四主族元素(优选为碳);于本实施例中,N型半导体层2是N型氮化镓系半导体层,而P型半导体层3是P型氮化镓系半导体层。Please refer to FIG. 1, which is a schematic cross-sectional view of a nitride semiconductor structure provided by a preferred embodiment of the present invention, which includes an N-type semiconductor layer 2 and a P-type semiconductor layer 3, between the N-type semiconductor layer 2 and the P-type semiconductor layer. A light-emitting layer 4 (active layer) is arranged between the P-type semiconductor layers 3, and a quaternary carrier active layer 5 is arranged between the light-emitting layer 4 and the P-type semiconductor layer 3, and the quaternary carrier active layer 5 is aluminum indium gallium nitride Al x In y Ga 1-xy N, wherein x and y are values satisfying 0<x<1, 0<y<1, 0<x+y<1; in addition, the above-mentioned quaternary carrier active layer 5 is doped Doped with a fourth main group element (preferably carbon) at a concentration of 10 16 -10 19 cm -3 ; in this embodiment, the N-type semiconductor layer 2 is an N-type gallium nitride-based semiconductor layer, and the P-type semiconductor layer 3 is a p-type gallium nitride-based semiconductor layer.

再者,上述的四元载子活性层5掺杂有浓度大于1018cm-3的P型掺质(可例如为镁),并且,优选地,四元载子活性层5的厚度为50-300nm。Furthermore, the above-mentioned quaternary carrier active layer 5 is doped with a P-type dopant (such as magnesium) with a concentration greater than 10 18 cm -3 , and, preferably, the thickness of the quaternary carrier active layer 5 is 50 -300nm.

此外,上述的发光层4具有多重量子井结构;其中,多重量子井结构可由氮化铟镓的井层42及氮化镓的阻障层41交替堆栈所形成,且紧邻于多重量子井结构的最后一井层42的四元载子活性层5的能隙大于多重量子井结构的阻障层41的能隙,其中,优选地,四元载子活性层5的能隙高于阻障层41的能隙1%-15%;由此,与公知的P-AlGaN电子阻挡层相较下,不仅提升电洞进入多重量子井结构的效果,亦同时达到抑制电子逃逸进入P型半导体层3的目的,使得电子与电洞结合机率增加,进一步提升发光效率;另外,于发光层4与N型半导体层2间亦可配置有一N型载子阻隔层6,且N型载子阻隔层6由具有高于发光层4的能隙的材料所制成;于本实施例中,其为N型氮化铝镓(N-AlGaN),以此避免电洞逃逸进入N型半导体层2内。In addition, the above-mentioned light-emitting layer 4 has a multiple quantum well structure; wherein, the multiple quantum well structure can be formed by alternately stacking the well layer 42 of InGaN and the barrier layer 41 of GaN, and is adjacent to the multiple quantum well structure. The energy gap of the quaternary carrier active layer 5 of the last well layer 42 is greater than the energy gap of the barrier layer 41 of the multiple quantum well structure, wherein, preferably, the energy gap of the quaternary carrier active layer 5 is higher than that of the barrier layer The energy gap of 41 is 1%-15%. Therefore, compared with the known P-AlGaN electron blocking layer, it not only improves the effect of holes entering the multiple quantum well structure, but also suppresses the escape of electrons into the P-type semiconductor layer3 The purpose is to increase the combination probability of electrons and holes, and further improve the luminous efficiency; in addition, an N-type carrier blocking layer 6 can also be arranged between the light-emitting layer 4 and the N-type semiconductor layer 2, and the N-type carrier blocking layer 6 It is made of a material with a higher energy gap than the light-emitting layer 4; in this embodiment, it is N-type aluminum gallium nitride (N-AlGaN), so as to prevent holes from escaping into the N-type semiconductor layer 2 .

在此值得注意的,由于以AlxInyGa1-x-yN材料所形成的四元载子活性层5是位于P型半导体层3与发光层4之间,通过控制四元载子活性层5中铟的含量,使得四元载子活性层5的铟含量等于或低于多重量子井结构的井层42的铟含量,进而形成能隙大于井层阻障层41能隙1%-15%的四元载子活性层5,使得载子可局限在多重量子井结构的井层42中,以增加电子电洞覆合的机率,进而提升内部量子效率,达到有效增强半导体发光元件发光效率的功效;此外,本发明的四元载子活性层5可作为P型半导体层3与发光层4间的缓冲层,以改善P型半导体层3与发光层4所产生的晶格失配造成晶体质量劣化的问题;同时,更可减低井层42受到压缩应力的影响,使得于井层42内的电子和电洞在空间上更为聚集,有效地将电子电洞局限于每一个井层42内,以提升内部量子效率;此外,压缩应力的减少亦增强相邻的GaN阻障层41和InGaN井层42之间的界面特性,以改善界面处的载子损耗,亦可增加内部量子效率。It is worth noting here that since the quaternary carrier active layer 5 formed of Al x In y Ga 1-xy N material is located between the P-type semiconductor layer 3 and the light-emitting layer 4, by controlling the quaternary carrier active layer The content of indium in 5 makes the indium content of the quaternary carrier active layer 5 equal to or lower than the indium content of the well layer 42 of the multiple quantum well structure, thereby forming an energy gap greater than the energy gap of the well barrier layer 41 by 1%-15 % of the quaternary carrier active layer 5, so that the carrier can be confined in the well layer 42 of the multiple quantum well structure, so as to increase the probability of electron hole recombination, thereby improving the internal quantum efficiency, and effectively enhancing the luminous efficiency of the semiconductor light-emitting element In addition, the quaternary carrier active layer 5 of the present invention can be used as a buffer layer between the P-type semiconductor layer 3 and the light-emitting layer 4 to improve the lattice mismatch caused by the P-type semiconductor layer 3 and the light-emitting layer 4. The problem of crystal quality deterioration; at the same time, it can reduce the impact of compressive stress on the well layer 42, so that the electrons and holes in the well layer 42 are more concentrated in space, effectively confining the electron holes to each well layer 42, to improve the internal quantum efficiency; in addition, the reduction of the compressive stress also enhances the interface characteristics between the adjacent GaN barrier layer 41 and the InGaN well layer 42, so as to improve the carrier loss at the interface and increase the internal quantum efficiency. efficiency.

上述实施例的氮化物半导体结构于实际实施使用时,由于四元载子活性层5的能隙高于阻障层41的能隙1%-15%,不仅可达到抑制电子溢流的功效,亦能提升电洞注入的效果,使得电子与电洞结合机率增加,进一步提升发光效率;此外,由于四元载子活性层5掺杂有浓度为1016-1019cm-3的第四主族元素,利用第四主族元素取代五价的氮原子,以此多一个带正电电洞,使得四元载子活性层5可具有高电洞浓度,上述的第四主族元素可例如为碳(C)、硅(Si)、锗(Ge)、锡(Sn)、铅(Pb)等,其中,优选地,第四主族元素为碳,其原因为:在磊晶的过程中,碳会与由氨气分解出的氢反应并形成稳定的化合物CH4,而脱离氮化物半导体,故H的含量降低,也连带使得Mg-H键结的情况因此降低,造成Mg具有离子型态的有效作用,因此,四元载子活性层5可具有高电洞浓度,由此提供更多的电洞进入发光层4,进而增加电子电洞结合的情况;值得注意的,若第四主族元素于四元载子活性层5中掺杂浓度小于1016cm-3,无法具有电洞提供的效果,若第四主族元素掺杂浓度大于1019cm-3,则会产生阻值变高的问题,优选的掺杂浓度为5×1016-5×1018cm-3When the nitride semiconductor structure of the above embodiment is actually implemented and used, since the energy gap of the quaternary carrier active layer 5 is 1%-15% higher than the energy gap of the barrier layer 41, not only the effect of suppressing the overflow of electrons can be achieved, It can also improve the effect of hole injection, increase the combination probability of electrons and holes, and further improve the luminous efficiency; in addition, since the quaternary carrier active layer 5 is doped with the fourth main body with a concentration of 10 16 -10 19 cm -3 Group elements, use the fourth main group element to replace the pentavalent nitrogen atom, so as to add a positively charged hole, so that the quaternary carrier active layer 5 can have a high hole concentration, the above-mentioned fourth main group element can be, for example Carbon (C), silicon (Si), germanium (Ge), tin (Sn), lead (Pb), etc., wherein, preferably, the fourth main group element is carbon, the reason is: in the process of epitaxy , the carbon will react with the hydrogen decomposed from the ammonia gas and form a stable compound CH 4 , which is separated from the nitride semiconductor, so the content of H is reduced, and the bonding of Mg-H is also reduced, causing Mg to have an ionic state, therefore, the quaternary carrier active layer 5 can have a high hole concentration, thereby providing more holes to enter the light-emitting layer 4, thereby increasing the combination of electrons and holes; it is noteworthy that if the fourth The doping concentration of the main group elements in the quaternary carrier active layer 5 is less than 10 16 cm -3 , which cannot provide the effect of holes. If the doping concentration of the fourth main group elements is greater than 10 19 cm -3 , resistance will be generated. If the value becomes high, the preferred doping concentration is 5×10 16 -5×10 18 cm -3 .

请参阅图2所示,上述的氮化物半导体结构可应用于半导体发光元件中,图2为根据本发明的优选实施例提供的氮化物半导体结构所制作的半导体发光元件的剖面示意图,所述半导体发光元件至少包含有:Please refer to FIG. 2, the above-mentioned nitride semiconductor structure can be applied to semiconductor light-emitting elements. FIG. 2 is a schematic cross-sectional view of a semiconductor light-emitting element made of a nitride semiconductor structure according to a preferred embodiment of the present invention. Light emitting elements include at least:

一基板1;a substrate 1;

一N型半导体层2,其配置于基板1上;An N-type semiconductor layer 2 configured on the substrate 1;

一发光层4,其配置于N型半导体层2上;其中,发光层4具有多重量子井结构,且多重量子井结构可由氮化铟镓的井层42及氮化镓的阻障层41交替堆栈所形成,并于每两阻障层41间具有一井层42;A light-emitting layer 4, which is arranged on the N-type semiconductor layer 2; wherein, the light-emitting layer 4 has a multiple quantum well structure, and the multiple quantum well structure can be alternated by well layers 42 of indium gallium nitride and barrier layers 41 of gallium nitride formed by a stack, and has a well layer 42 between every two barrier layers 41;

一四元载子活性层5,其配置于发光层4上,四元载子活性层5为氮化铝铟镓AlxInyGa1-x-yN,其中x及y为满足0<x<1、0<y<1、0<x+y<1的数值,优选可为0<x≤0.4、0<y≤0.2;再者,四元载子活性层5掺杂有浓度为1016-1019cm-3的第四主族元素(优选为碳);其中,优选地,四元载子活性层5的厚度为50-300nm,且可掺杂有浓度大于1018cm-3的P型掺质(例如为镁),且四元载子活性层5的能隙大于多重量子井结构的阻障层41的能隙,优选为高于阻障层41能隙的1%-15%;A quaternary carrier active layer 5, which is arranged on the light-emitting layer 4, the quaternary carrier active layer 5 is aluminum indium gallium nitride Al x In y Ga 1-xy N, wherein x and y satisfy 0<x< 1. Values of 0<y<1, 0<x+y<1, preferably 0<x≤0.4, 0<y≤0.2; moreover, the quaternary carrier active layer 5 is doped with a concentration of 10 16 -10 19 cm -3 of the fourth main group element (preferably carbon); wherein, preferably, the thickness of the quaternary carrier active layer 5 is 50-300nm, and can be doped with a concentration greater than 10 18 cm -3 P-type dopant (such as magnesium), and the energy gap of the quaternary carrier active layer 5 is greater than the energy gap of the barrier layer 41 of the multiple quantum well structure, preferably 1%-15% higher than the energy gap of the barrier layer 41 %;

一P型半导体层3,其配置于四元载子活性层5上;A P-type semiconductor layer 3 configured on the quaternary carrier active layer 5;

一N型电极21,其以欧姆接触配置于N型半导体层2上;以及An N-type electrode 21, which is configured on the N-type semiconductor layer 2 with an ohmic contact; and

一P型电极31,其以欧姆接触配置于P型半导体层3上;其中,N型电极21、P型电极31相配合地提供电能,且可以下列材料、但不仅限于这些材料所制成:钛、铝、金、铬、镍、铂及其合金等,而其工艺方法为本领域一般技术人员所公知的,且并非本发明的重点,因此,不再本发明中加以赘述。A P-type electrode 31, which is configured on the P-type semiconductor layer 3 with ohmic contact; wherein, the N-type electrode 21 and the P-type electrode 31 cooperate to provide electric energy, and can be made of the following materials, but not limited to these materials: Titanium, aluminum, gold, chromium, nickel, platinum and their alloys, etc., and their processing methods are well known to those skilled in the art, and are not the focus of the present invention, so they will not be repeated in the present invention.

此外,于发光层4与N型半导体层2间可进一步配置有一N型载子阻隔层6,且N型载子阻隔层6由具有高于发光层4的能隙的材料所制成;再者,为解决因晶格差异所产生的磊晶差排现象,亦可于基板1与N型半导体层2间形成有一缓冲层7,缓冲层7为氮化铝镓AlzGa1-zN,其中0<z<1。In addition, an N-type carrier blocking layer 6 can be further arranged between the light-emitting layer 4 and the N-type semiconductor layer 2, and the N-type carrier blocking layer 6 is made of a material having an energy gap higher than that of the light-emitting layer 4; Or, in order to solve the epitaxial dislocation phenomenon caused by the lattice difference, a buffer layer 7 can also be formed between the substrate 1 and the N-type semiconductor layer 2, and the buffer layer 7 is aluminum gallium nitride Al z Ga 1-z N , where 0<z<1.

由上述的氮化物半导体结构的实施说明可知,本发明的半导体发光元件通过控制四元载子活性层5中铟的含量,使得四元载子活性层5的能隙高于阻障层41的能隙1%-15%,不仅可提升电洞进入多重量子井结构,以及达到抑制电子逃逸进入P型半导体层3的功效,使得电子与电洞结合机率增加,更可作为P型半导体层3与发光层4间的缓冲层7,以改善P型半导体层3与发光层4所产生的晶格失配造成晶体质量劣化的问题;此外,通过四元载子活性层5的第四主族元素掺质可降低因Mg-H键结所造成的不活化现象,使Mg活化而具有受体的有效作用,进而使得四元载子活性层5具有高电洞浓度,提供更多的电洞进入发光层4,增加电子电洞结合的情况,以便半导体发光元件可呈现出足够低的阻抗,进而获得更佳的发光效率。It can be seen from the above description of the implementation of the nitride semiconductor structure that the semiconductor light-emitting element of the present invention controls the content of indium in the quaternary carrier active layer 5 so that the energy gap of the quaternary carrier active layer 5 is higher than that of the barrier layer 41. The energy gap is 1%-15%, which can not only improve the entry of holes into the multiple quantum well structure, but also achieve the effect of inhibiting electrons from escaping into the P-type semiconductor layer 3, so that the combination probability of electrons and holes increases, and can be used as a P-type semiconductor layer 3 and the buffer layer 7 between the light emitting layer 4 to improve the crystal quality deterioration caused by the lattice mismatch between the P-type semiconductor layer 3 and the light emitting layer 4; in addition, the fourth main group of the quaternary carrier active layer 5 The element dopant can reduce the inactivation phenomenon caused by the Mg-H bond, activate the Mg and have the effective effect of the acceptor, and then make the quaternary carrier active layer 5 have a high hole concentration and provide more holes Entering the light-emitting layer 4, the combination of electrons and holes is increased, so that the semiconductor light-emitting element can exhibit a sufficiently low impedance, thereby obtaining better luminous efficiency.

Claims (10)

  1. A kind of 1. nitride semiconductor structure, it is characterised in that including:
    One p type semiconductor layer;
    One n type semiconductor layer;
    One luminescent layer, between the p type semiconductor layer and the n type semiconductor layer;And
    The gallium nitride carrier active layer of one p-type, between the p type semiconductor layer and the luminescent layer, the p-type gallium nitride Be carrier active layer material include aluminium and indium at least one, and the gallium nitride carrier active layer of the p-type doped with carbon and Magnesium, wherein the doping concentration of the carbon is 5 × 1016~5 × 1018cm-3
  2. 2. nitride semiconductor structure as claimed in claim 1, it is characterised in that the doping concentration of the magnesium admixture is more than 1018cm-3
  3. 3. nitride semiconductor structure as claimed in claim 1, it is characterised in that also including a carrier barrier layer, positioned at institute State between n type semiconductor layer and the luminescent layer.
  4. 4. nitride semiconductor structure as claimed in claim 3, it is characterised in that the energy gap of the carrier barrier layer is higher than institute State the energy gap of luminescent layer.
  5. 5. nitride semiconductor structure as claimed in claim 3, it is characterised in that the material of the carrier barrier layer includes N Type aluminium gallium nitride alloy.
  6. 6. nitride semiconductor structure as claimed in claim 1, it is characterised in that the luminescent layer has multiple quantum trap knot Structure, the multiple quantum well construction include the well layer and barrier layer of a plurality of stackings alternating with each other, the gallium nitride carrier of p-type Active layer is in close proximity to the multiple quantum well construction, and the energy gap of the gallium nitride carrier active layer of the p-type is more than the barrier The energy gap of layer.
  7. 7. nitride semiconductor structure as claimed in claim 6, it is characterised in that also including a carrier barrier layer, the load Sub- barrier layer is between the n type semiconductor layer and the luminescent layer, wherein the material of the carrier barrier layer includes N-type nitrogen Change gallium aluminium.
  8. A kind of 8. nitride semiconductor structure, it is characterised in that including:
    One p type semiconductor layer, include a carbon enrichment layer, wherein the carbon enrichment layer material include Al-In-Ga-N and doped with Magnesium admixture and carbon admixture;
    One n type semiconductor layer;And
    One luminescent layer, between the p type semiconductor layer and the n type semiconductor layer, and the carbon enrichment layer position is in the P The side for being adjacent to the luminescent layer of type semiconductor layer.
  9. 9. nitride semiconductor structure as claimed in claim 8, it is characterised in that the luminescent layer has multiple quantum trap knot Structure, the multiple quantum well construction include the well layer and barrier layer of a plurality of stackings alternating with each other, and the carbon enrichment layer is in close proximity to The multiple quantum well construction, and the energy gap of the carbon enrichment layer is more than the energy gap of the barrier layer.
  10. 10. nitride semiconductor structure as claimed in claim 9, it is characterised in that the energy gap of the carbon enrichment layer is more than institute State the energy gap 1%~15% of barrier layer.
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