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CN108831974A - A light-emitting diode epitaxial wafer and its manufacturing method - Google Patents

A light-emitting diode epitaxial wafer and its manufacturing method Download PDF

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CN108831974A
CN108831974A CN201810395843.4A CN201810395843A CN108831974A CN 108831974 A CN108831974 A CN 108831974A CN 201810395843 A CN201810395843 A CN 201810395843A CN 108831974 A CN108831974 A CN 108831974A
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CN108831974B (en
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魏晓骏
郭炳磊
李鹏
胡加辉
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Boe Huacan Optoelectronics Suzhou Co ltd
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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
    • H10H20/816Bodies 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]
    • H10H20/01Manufacture or treatment
    • H10H20/011Manufacture or treatment of bodies, e.g. forming semiconductor layers
    • H10H20/013Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials
    • H10H20/0133Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials with a substrate not being Group III-V materials
    • 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]
    • H10H20/01Manufacture or treatment
    • H10H20/011Manufacture or treatment of bodies, e.g. forming semiconductor layers
    • H10H20/013Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials
    • H10H20/0137Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials the light-emitting regions comprising nitride materials
    • 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
    • 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

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Abstract

本发明公开了一种发光二极管外延片及其制造方法,属于半导体技术领域。包括衬底、缓冲层、未掺杂的GaN层、N型层、有源层、低温P型层、电子阻挡层、高温P型层和P型接触层,电子阻挡层为包括N个周期的AlxGa1‑xN/AlN/GaN/InyGa1‑ yN超晶格结构,N为大于等于2的正整数,电子阻挡层的厚度为10~25nm。与现有的厚度大于50nm的电子阻挡层相比,本发明提供的电子阻挡层的厚度大大减小,进而减少了材料间的极化和应力作用,降低了电子阻挡层在价带异质结界面产生的价带带阶,使得空穴能够更好的注入有源层,则空穴的浓度增加,更多的空穴可以在有源层中与电子复合发光,提高了LED的发光效率。

The invention discloses a light-emitting diode epitaxial wafer and a manufacturing method thereof, belonging to the technical field of semiconductors. Including substrate, buffer layer, undoped GaN layer, N-type layer, active layer, low-temperature P-type layer, electron blocking layer, high-temperature P-type layer and P-type contact layer, and the electron blocking layer includes N periods Al x Ga 1‑x N/AlN/GaN/In y Ga 1‑ y N superlattice structure, N is a positive integer greater than or equal to 2, and the thickness of the electron blocking layer is 10-25 nm. Compared with the existing electron blocking layer with a thickness greater than 50nm, the thickness of the electron blocking layer provided by the present invention is greatly reduced, thereby reducing the polarization and stress between materials, and reducing the electron blocking layer in the valence band heterojunction. The valence band order generated by the interface enables holes to be better injected into the active layer, and the concentration of holes increases, and more holes can recombine with electrons in the active layer to emit light, which improves the luminous efficiency of the LED.

Description

一种发光二极管外延片及其制造方法A light-emitting diode epitaxial wafer and its manufacturing method

技术领域technical field

本发明涉及半导体技术领域,特别涉及一种发光二极管外延片及其制造方法。The invention relates to the technical field of semiconductors, in particular to a light-emitting diode epitaxial wafer and a manufacturing method thereof.

背景技术Background technique

LED(Light Emitting Diode,发光二极管)是一种能发光的半导体电子元件。作为一种高效、环保、绿色新型固态照明光源,正在被迅速广泛地得到应用,如交通信号灯、汽车内外灯、城市景观照明、手机背光源等。LED (Light Emitting Diode, Light Emitting Diode) is a semiconductor electronic component that can emit light. As an efficient, environmentally friendly and green new solid-state lighting source, it is being rapidly and widely used, such as traffic lights, car interior and exterior lights, urban landscape lighting, mobile phone backlights, etc.

外延片是LED中的主要构成部分,现有的GaN基LED外延片包括衬底和设置在衬底上的GaN基外延层,GaN基外延层包括依次层叠在衬底上的缓冲层、未掺杂的GaN层、N型层(N型区)、有源层、电子阻挡层、高温P型层(P型区)和P型接触层。N型区提供的电子和P型区提供的空穴在有源层复合发光。其中电子阻挡层通常为AlGaN层或多个周期的AlGaN/InGaN超晶格结构,电子阻挡层的厚度大于50nm。The epitaxial wafer is the main component of the LED. The existing GaN-based LED epitaxial wafer includes a substrate and a GaN-based epitaxial layer arranged on the substrate. The GaN-based epitaxial layer includes a buffer layer stacked on the substrate, an undoped Doped GaN layer, N-type layer (N-type region), active layer, electron blocking layer, high-temperature P-type layer (P-type region) and P-type contact layer. The electrons provided by the N-type region and the holes provided by the P-type region recombine and emit light in the active layer. The electron blocking layer is usually an AlGaN layer or a multi-period AlGaN/InGaN superlattice structure, and the thickness of the electron blocking layer is greater than 50 nm.

在实现本发明的过程中,发明人发现现有技术至少存在以下问题:In the process of realizing the present invention, the inventor finds that there are at least the following problems in the prior art:

现有的LED外延片中,电子阻挡层设计得较厚(通常大于50nm),较厚的电子阻挡层会导致材料间的极化和应力作用,同时会产生一个高的价带阻碍空穴向有源层迁移,因此N型区提供的电子的浓度比P型区中提供的空穴的浓度高,电子的迁移率比空穴快很多,导致电子和空穴的复合发光效率降低,从而使得LED的发光效率降低。In the existing LED epitaxial wafers, the electron blocking layer is designed to be thicker (usually greater than 50nm), and the thicker electron blocking layer will cause polarization and stress between materials, and at the same time, a high valence band will be generated to hinder the direction of holes. The active layer migrates, so the concentration of electrons provided by the N-type region is higher than the concentration of holes provided by the P-type region, and the mobility of electrons is much faster than that of holes, resulting in a decrease in the recombination luminescence efficiency of electrons and holes, thus making The luminous efficiency of the LED decreases.

发明内容Contents of the invention

为了解决现有技术中电子阻挡层设计得较厚,使得LED的发光效率降低的问题,本发明实施例提供了一种发光二极管外延片及其制造方法。所述技术方案如下:In order to solve the problem in the prior art that the electron blocking layer is designed to be relatively thick, which reduces the luminous efficiency of the LED, an embodiment of the present invention provides a light emitting diode epitaxial wafer and a manufacturing method thereof. Described technical scheme is as follows:

一方面,本发明提供了一种发光二极管外延片,所述发光二极管外延片包括衬底,以及依次层叠在所述衬底上的缓冲层、未掺杂的GaN层、N型层、有源层、低温P型层、电子阻挡层、高温P型层和P型接触层,所述低温P型层为GaN层,In one aspect, the present invention provides a light-emitting diode epitaxial wafer, the light-emitting diode epitaxial wafer includes a substrate, and a buffer layer, an undoped GaN layer, an N-type layer, an active layer, a low-temperature P-type layer, an electron blocking layer, a high-temperature P-type layer and a P-type contact layer, the low-temperature P-type layer is a GaN layer,

所述电子阻挡层为包括N个周期的AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构,0.05<x<0.15,0.2<y<0.4,N为大于等于2的正整数,所述电子阻挡层的厚度为10~25nm。The electron blocking layer is an Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure including N periods, 0.05<x<0.15, 0.2<y<0.4, and N is greater than It is a positive integer equal to 2, and the thickness of the electron blocking layer is 10-25 nm.

进一步地,在所述AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个AlxGa1-xN子层的厚度为0.5~1.5nm。Further, the thickness of each AlxGa1 - xN sublayer in the AlxGa1 - xN /AlN/GaN/InyGa1 -yN superlattice structure is 0.5-1.5nm.

进一步地,在所述AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个AlN子层的厚度为0.5~1.5nm。Further, the thickness of each AlN sublayer in the Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure is 0.5-1.5 nm.

进一步地,在所述AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个GaN子层的厚度为1~2nm。Further, the thickness of each GaN sublayer in the Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure is 1-2 nm.

进一步地,在所述AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个InyGa1-yN子层的厚度为1~2nm。Further, the thickness of each In y Ga 1-y N sublayer in the Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure is 1-2 nm.

进一步地,2≤N≤5。Further, 2≤N≤5.

进一步地,x=0.1,y=0.38。Further, x=0.1, y=0.38.

另一方面,本发明实施例提供了一种发光二极管外延片的制造方法,所述制造方法包括:On the other hand, an embodiment of the present invention provides a method for manufacturing a light-emitting diode epitaxial wafer, the manufacturing method comprising:

提供一衬底;providing a substrate;

在所述衬底上依次生长缓冲层、未掺杂的GaN层、N型层、有源层和低温P型层,所述低温P型层为GaN层;sequentially growing a buffer layer, an undoped GaN layer, an N-type layer, an active layer, and a low-temperature P-type layer on the substrate, the low-temperature P-type layer being a GaN layer;

在所述低温P型层上生长电子阻挡层,所述电子阻挡层为包括N个周期的AlxGa1- xN/AlN/GaN/InyGa1-yN超晶格结构,0.05<x<0.15,0.2<y<0.4,N为大于等于2的正整数,所述电子阻挡层的厚度为10~25nm;An electron blocking layer is grown on the low-temperature P-type layer, and the electron blocking layer is an AlxGa1 - xN /AlN/GaN/InyGa1 -yN superlattice structure including N periods, 0.05<x<0.15,0.2<y<0.4, N is a positive integer greater than or equal to 2, and the thickness of the electron blocking layer is 10-25nm;

在所述电子阻挡层上生长高温P型层和P型接触层。A high-temperature P-type layer and a P-type contact layer are grown on the electron blocking layer.

进一步地,所述电子阻挡层的生长温度为850~1080℃。Further, the growth temperature of the electron blocking layer is 850-1080°C.

进一步地,所述电子阻挡层的生长压力为200~500Torr。Further, the growth pressure of the electron blocking layer is 200-500 Torr.

本发明实施例提供的技术方案带来的有益效果是:The beneficial effects brought by the technical solution provided by the embodiments of the present invention are:

将电子阻挡层设置成包括N个周期的AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构,其中,由于低温P型层为GaN层,而电子阻挡层中的AlN层与低温P型GaN层晶格失配,因此设置AlxGa1-xN作为缓冲层,可以降低电子阻挡层与低温P型层的晶格失配。AlN层能够形成一个较高的势垒能级,阻挡电子的迁移,同时由于AlN层和GaN层之间的界面晶格失配大,因此AlN层和GaN层之间可以产生一定的二维电子气,以提供更多的空穴,并提高载流子的迁移速率。InyGa1-yN层可以增强二维电子气的产生,进一步地提供更多的空穴,提高载流子的迁移速率。且本发明中的电子阻挡层的厚度为10~25nm,与现有的厚度大于50nm的电子阻挡层相比,厚度大大减小,进而减少了材料间的极化和应力作用,降低了高Al组分的电子阻挡层在价带异质结界面产生的价带带阶,使得空穴能够更好的注入有源层,则空穴的浓度增加,更多的空穴可以在有源层中与电子复合发光,提高了LED的发光效率。The electron blocking layer is set to include N periods of Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure, wherein, because the low-temperature P-type layer is a GaN layer, and the electron blocking layer The AlN layer and the low-temperature P-type GaN layer have a lattice mismatch, so setting Al x Ga 1-x N as a buffer layer can reduce the lattice mismatch between the electron blocking layer and the low-temperature P-type layer. The AlN layer can form a higher barrier energy level to block the migration of electrons. At the same time, due to the large interface lattice mismatch between the AlN layer and the GaN layer, certain two-dimensional electrons can be generated between the AlN layer and the GaN layer. gas to provide more holes and increase the mobility of carriers. The In y Ga 1-y N layer can enhance the generation of two-dimensional electron gas, further provide more holes, and increase the mobility of carriers. And the thickness of the electron blocking layer in the present invention is 10-25nm, compared with the existing electron blocking layer with a thickness greater than 50nm, the thickness is greatly reduced, thereby reducing the polarization and stress between materials, reducing the high Al The electronic blocking layer of the component produces a valence band band level at the valence band heterojunction interface, so that holes can be better injected into the active layer, and the concentration of holes increases, and more holes can be in the active layer Combined with electrons to emit light, the luminous efficiency of LED is improved.

附图说明Description of drawings

为了更清楚地说明本发明实施例中的技术方案,下面将对实施例描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the drawings that need to be used in the description of the embodiments will be briefly introduced below. Obviously, the drawings in the following description are only some embodiments of the present invention. For those skilled in the art, other drawings can also be obtained based on these drawings without creative effort.

图1是本发明实施例提供的一种发光二极管外延片的结构示意图;FIG. 1 is a schematic structural view of a light-emitting diode epitaxial wafer provided by an embodiment of the present invention;

图2是本发明实施例提供的一种发光二极管外延片的制造方法的方法流程图。Fig. 2 is a method flowchart of a method for manufacturing a light emitting diode epitaxial wafer provided by an embodiment of the present invention.

具体实施方式Detailed ways

为使本发明的目的、技术方案和优点更加清楚,下面将结合附图对本发明实施方式作进一步地详细描述。In order to make the object, technical solution and advantages of the present invention clearer, the embodiments of the present invention will be further described in detail below in conjunction with the accompanying drawings.

本发明实施例提供了一种发光二极管外延片,图1是本发明实施例提供的一种发光二极管外延片的结构示意图,如图1所示,发光二极管外延片包括衬底1,以及依次层叠在衬底1上的缓冲层2、未掺杂的GaN层3、N型层4、有源层5、低温P型层6、电子阻挡层7、高温P型层8和P型接触层9,低温P型层6为GaN层。An embodiment of the present invention provides a light-emitting diode epitaxial wafer. FIG. 1 is a schematic structural view of a light-emitting diode epitaxial wafer provided by an embodiment of the present invention. As shown in FIG. 1, the light-emitting diode epitaxial wafer includes a substrate 1, and sequentially stacked Buffer layer 2, undoped GaN layer 3, N-type layer 4, active layer 5, low-temperature P-type layer 6, electron blocking layer 7, high-temperature P-type layer 8 and P-type contact layer 9 on substrate 1 , the low-temperature P-type layer 6 is a GaN layer.

其中,电子阻挡层7为包括N个周期的AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构,0.05<x<0.15,0.2<y<0.4,N为大于等于2的正整数,电子阻挡层7的厚度为10~25nm。Wherein, the electron blocking layer 7 is an AlxGa1 - xN /AlN/GaN/InyGa1 -yN superlattice structure including N periods, 0.05<x<0.15, 0.2<y<0.4, and N is A positive integer greater than or equal to 2, and the thickness of the electron blocking layer 7 is 10-25 nm.

通过将电子阻挡层设置成包括N个周期的AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构,其中,由于低温P型层为GaN层,而电子阻挡层中的AlN层与低温P型GaN层晶格失配,因此设置AlxGa1-xN作为缓冲层,可以降低电子阻挡层与低温P型层的晶格失配。AlN层能够形成一个较高的势垒能级,阻挡电子的迁移,同时由于AlN层和GaN层之间的界面晶格失配大,因此AlN层和GaN层之间可以产生一定的二维电子气,以提供更多的空穴,并提高载流子的迁移速率。InyGa1-yN层可以增强二维电子气的产生,进一步地提供更多的空穴,提高载流子的迁移速率。且本发明中的电子阻挡层的厚度为10~25nm,与现有的厚度大于50nm的电子阻挡层相比,厚度大大减小,进而减少了材料间的极化和应力作用,降低了高Al组分的电子阻挡层在价带异质结界面产生的价带带阶,使得空穴能够更好的注入有源层,则空穴的浓度增加,更多的空穴可以在有源层中与电子复合发光,提高了LED的发光效率。By setting the electron blocking layer as an Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure including N periods, wherein, since the low-temperature P-type layer is a GaN layer, the electron blocking The AlN layer in the layer has a lattice mismatch with the low-temperature P-type GaN layer, so setting AlxGa1 - xN as a buffer layer can reduce the lattice mismatch between the electron blocking layer and the low-temperature P-type layer. The AlN layer can form a higher barrier energy level to block the migration of electrons. At the same time, due to the large interface lattice mismatch between the AlN layer and the GaN layer, certain two-dimensional electrons can be generated between the AlN layer and the GaN layer. gas to provide more holes and increase the mobility of carriers. The In y Ga 1-y N layer can enhance the generation of two-dimensional electron gas, further provide more holes, and increase the mobility of carriers. And the thickness of the electron blocking layer in the present invention is 10-25nm, compared with the existing electron blocking layer with a thickness greater than 50nm, the thickness is greatly reduced, thereby reducing the polarization and stress between materials, reducing the high Al The electronic blocking layer of the component produces a valence band band level at the valence band heterojunction interface, so that holes can be better injected into the active layer, and the concentration of holes increases, and more holes can be in the active layer Combined with electrons to emit light, the luminous efficiency of LED is improved.

优选地,x=0.1,y=0.38。此时LED的发光效率最好。Preferably, x=0.1, y=0.38. At this time, the luminous efficiency of the LED is the best.

具体地,在电子阻挡层7的每个AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中均包括AlxGa1-xN子层71、AlN子层72、GaN子层73和InyGa1-yN子层74。Specifically, each AlxGa1 - xN /AlN/GaN/InyGa1 -yN superlattice structure of the electron blocking layer 7 includes AlxGa1 -xN sublayers 71, AlN sublayers layer 72 , GaN sublayer 73 and In y Ga 1-y N sublayer 74 .

进一步地,每个AlxGa1-xN子层71的厚度为0.5~1.5nm。若每个AlxGa1-xN子层71的厚度小于0.5nm,则起不到降低电子阻挡层7与低温P型层6的晶格失配的作用,若每个AlxGa1- xN子层71的厚度大于1.5nm,则会造成浪费,还会导致电子阻挡层7的厚度过厚,影响LED的发光效率。Further, the thickness of each Al x Ga 1-x N sublayer 71 is 0.5-1.5 nm. If the thickness of each AlxGa1 -xN sublayer 71 is less than 0.5nm, it will not be effective in reducing the lattice mismatch between the electron blocking layer 7 and the low-temperature P-type layer 6. If each AlxGa1 - xN sublayer 71 If the thickness of the x N sublayer 71 is greater than 1.5 nm, it will cause waste, and also cause the thickness of the electron blocking layer 7 to be too thick, which will affect the luminous efficiency of the LED.

优选地,每个AlxGa1-xN子层71的厚度为1nm。此时既能起到降低电子阻挡层7与低温P型层6之间的晶格失配的作用,又能够保证电子阻挡层7的厚度不会过厚,造成浪费。Preferably, the thickness of each AlxGa1 -xN sublayer 71 is 1 nm. At this time, it can not only reduce the lattice mismatch between the electron blocking layer 7 and the low-temperature P-type layer 6 , but also ensure that the thickness of the electron blocking layer 7 will not be too thick, resulting in waste.

进一步地,每个AlN子层72的厚度为0.5~1.5nm。若每个AlN子层72的厚度小于0.5nm,则起不到阻挡电子的作用。若每个AlN子层72的厚度大于1.5nm,则会造成浪费,还会导致电子阻挡层7的厚度过厚,影响LED的发光效率。Further, the thickness of each AlN sub-layer 72 is 0.5-1.5 nm. If the thickness of each AlN sublayer 72 is less than 0.5 nm, it will not be able to block electrons. If the thickness of each AlN sub-layer 72 is greater than 1.5 nm, it will cause waste, and also cause the thickness of the electron blocking layer 7 to be too thick, which will affect the luminous efficiency of the LED.

优选地,每个AlN子层72的厚度为1nm。此时既能起到阻挡电子的作用,又能够保证电子阻挡层7的厚度不会过厚,造成浪费。Preferably, each AlN sublayer 72 has a thickness of 1 nm. At this time, it can not only block electrons, but also ensure that the thickness of the electron blocking layer 7 will not be too thick, resulting in waste.

进一步地,每个GaN子层73的厚度为1~2nm。若每个GaN子层73的厚度小于1nm,则无法产生一定的二维电子气,以提供更多的空穴,提高载流子的迁移速率,若每个GaN子层73的厚度大于2nm,则会造成浪费,还会导致电子阻挡层7的厚度过厚,影响LED的发光效率。Further, the thickness of each GaN sub-layer 73 is 1-2 nm. If the thickness of each GaN sublayer 73 is less than 1nm, a certain two-dimensional electron gas cannot be generated to provide more holes and increase the mobility of carriers. If the thickness of each GaN sublayer 73 is greater than 2nm, It will cause waste, and also cause the thickness of the electron blocking layer 7 to be too thick, which will affect the luminous efficiency of the LED.

优选地,每个GaN子层73的厚度为1nm。此时既能与AlN子层72产生一定的二维电子气,以提供更多的空穴,提高载流子的迁移速率,又能够保证电子阻挡层7的厚度不会过厚,造成浪费。Preferably, the thickness of each GaN sub-layer 73 is 1 nm. At this time, a certain two-dimensional electron gas can be generated with the AlN sublayer 72 to provide more holes and increase the mobility of carriers, and it can also ensure that the thickness of the electron blocking layer 7 will not be too thick, resulting in waste.

进一步地,每个InyGa1-yN子层74的厚度为1~2nm。若每个InyGa1-yN子层74的厚度小于1nm,则无法增强二维电子气的产生,若每个InyGa1-yN子层74的厚度大于2nm,则会造成浪费,还会导致电子阻挡层7的厚度过厚,影响LED的发光效率。Further, the thickness of each In y Ga 1-y N sublayer 74 is 1-2 nm. If the thickness of each In y Ga 1-y N sub-layer 74 is less than 1 nm, the generation of two-dimensional electron gas cannot be enhanced, and if the thickness of each In y Ga 1-y N sub-layer 74 is greater than 2 nm, it will cause waste , will also cause the thickness of the electron blocking layer 7 to be too thick, which will affect the luminous efficiency of the LED.

优选地,每个InyGa1-yN子层74的厚度为2nm。此时既能帮助AlN子层72和GaN子层73之间产生更多的二维电子气,进一步提供更多的空穴,提高载流子的迁移速率,又能够保证电子阻挡层7的厚度不会过厚,造成浪费。Preferably, the thickness of each In y Ga 1-y N sublayer 74 is 2 nm. At this time, it can not only help to generate more two-dimensional electron gas between the AlN sublayer 72 and the GaN sublayer 73, further provide more holes, improve the mobility of carriers, but also ensure the thickness of the electron blocking layer 7 It will not be too thick and cause waste.

其中,2≤N≤5。若N小于2,则会导致电子阻挡层7的厚度过薄,无法起到阻挡电子,增加空穴,提高载流子的迁移速率的作用。若N大于5,则会导致电子阻挡层7的厚度过厚,降低LED的发光效率。Among them, 2≤N≤5. If N is less than 2, the thickness of the electron blocking layer 7 will be too thin, which cannot block electrons, increase holes, and increase the mobility of carriers. If N is greater than 5, the thickness of the electron blocking layer 7 will be too thick, reducing the luminous efficiency of the LED.

可选地,衬底1可以为(0001)晶向的蓝宝石衬底。Optionally, the substrate 1 may be a sapphire substrate with a (0001) crystal orientation.

可选地,缓冲层2可以为GaN层,厚度可以为15~35nm。Optionally, the buffer layer 2 may be a GaN layer with a thickness of 15-35 nm.

可选地,未掺杂的GaN层3的厚度可以为1~5um。Optionally, the thickness of the undoped GaN layer 3 may be 1-5 um.

可选地,N型层4可以为掺Si的GaN层,其中Si的掺杂浓度范围为1018cm-3~1019cm-3;N型层4的厚度可以为1~5um。Optionally, the N-type layer 4 may be a Si-doped GaN layer, wherein the doping concentration of Si ranges from 10 18 cm −3 to 10 19 cm −3 ; the thickness of the N-type layer 4 may be 1-5 um.

可选地,有源层5可以由5~11个周期的InxGa1-xN阱层51和GaN垒层52超晶格结构组成,其中,每层InxGa1-xN阱层51的厚度可以为2~3nm,每层GaN垒层52的厚度可以为9~20nm。Optionally, the active layer 5 may be composed of 5-11 periods of In x Ga 1-x N well layer 51 and GaN barrier layer 52 superlattice structure, wherein each layer of In x Ga 1-x N well layer The thickness of 51 may be 2-3 nm, and the thickness of each GaN barrier layer 52 may be 9-20 nm.

可选地,高温P型层8可以为GaN层,厚度可以为20~50nm。Optionally, the high-temperature P-type layer 8 may be a GaN layer with a thickness of 20-50 nm.

可选地,P型接触层9可以为GaN层,厚度可以为5~300nm。Optionally, the P-type contact layer 9 may be a GaN layer with a thickness of 5-300 nm.

实施例二Embodiment two

本发明实施例提供了一种发光二极管外延片的制造方法,用于制造实施例一提供的发光二极管外延片,图2是本发明实施例提供的一种发光二极管外延片的制造方法的方法流程图,如图2所示,该制造方法包括:An embodiment of the present invention provides a method for manufacturing a light-emitting diode epitaxial wafer, which is used to manufacture the light-emitting diode epitaxial wafer provided in Embodiment 1. FIG. 2 is a process flow of a method for manufacturing a light-emitting diode epitaxial wafer provided by an embodiment of the present invention. Figure, as shown in Figure 2, the manufacturing method comprises:

步骤201、提供一衬底。Step 201, providing a substrate.

可选地,衬底为(0001)晶向的Al2O3蓝宝石衬底。Optionally, the substrate is an Al 2 O 3 sapphire substrate with a (0001) crystal orientation.

具体地,该步骤201包括:Specifically, this step 201 includes:

在氢气气氛下,高温处理衬底8min。其中,反应室温度为1000~1200℃,反应室压力控制在200~500torr。Under the hydrogen atmosphere, the substrate was treated at high temperature for 8 minutes. Wherein, the temperature of the reaction chamber is 1000-1200° C., and the pressure of the reaction chamber is controlled at 200-500 torr.

步骤202、在衬底上生长缓冲层。Step 202, growing a buffer layer on the substrate.

具体地,缓冲层为GaN层,厚度为15~35nm。反应室温度为400~600℃,反应室压力控制在400~600torr。Specifically, the buffer layer is a GaN layer with a thickness of 15-35 nm. The temperature of the reaction chamber is 400-600° C., and the pressure of the reaction chamber is controlled at 400-600 torr.

进一步地,步骤202还包括:Further, step 202 also includes:

控制反应室压力不变,温度升高至1000℃~1200℃,对缓冲进行原位退火处理5~10min。The pressure of the reaction chamber is controlled to be constant, the temperature is raised to 1000° C. to 1200° C., and the buffer is annealed in situ for 5 to 10 minutes.

步骤203、在缓冲层上生长未掺杂的GaN层。Step 203 , growing an undoped GaN layer on the buffer layer.

在本实施例中,未掺杂的GaN层厚度为1~5um。生长未掺杂的GaN层时,反应室温度为1000~1100℃,反应室压力控制在100~500torr。In this embodiment, the thickness of the undoped GaN layer is 1-5 um. When growing the undoped GaN layer, the temperature of the reaction chamber is 1000-1100° C., and the pressure of the reaction chamber is controlled at 100-500 torr.

步骤204、在未掺杂的GaN层上生长N型层。Step 204 , growing an N-type layer on the undoped GaN layer.

在本实施例中,N型层为掺Si的GaN层,Si掺杂浓度在1018cm-3~1019cm-3之间,厚度为1~5um。生长N型层时,反应室温度为1000~1200℃,反应室压力控制在100~500torr。In this embodiment, the N-type layer is a GaN layer doped with Si, the Si doping concentration is between 10 18 cm −3 and 10 19 cm −3 , and the thickness is 1˜5 μm. When growing the N-type layer, the temperature of the reaction chamber is 1000-1200° C., and the pressure of the reaction chamber is controlled at 100-500 torr.

步骤205、在N型层上生长有源层。Step 205 , growing an active layer on the N-type layer.

有源层可以为包括5~11个周期的InxGa1-xN阱层和GaN垒层超晶格结构,0≤x≤1。其中,每层InxGa1-xN阱层的厚度为2~3nm,每层GaN垒层的厚度为9~20nm。The active layer may be a superlattice structure including 5-11 periods of In x Ga 1-x N well layers and GaN barrier layers, 0≤x≤1. Wherein, the thickness of each In x Ga 1-x N well layer is 2-3 nm, and the thickness of each GaN barrier layer is 9-20 nm.

具体地,生长有源层时,反应室压力控制在100~500torr。生长InxGa1-xN阱层时,反应室温度为720~829℃。生长GaN垒层时,反应室温度为850~959℃。Specifically, when growing the active layer, the pressure in the reaction chamber is controlled at 100-500 torr. When growing the In x Ga 1-x N well layer, the temperature of the reaction chamber is 720-829°C. When growing the GaN barrier layer, the temperature of the reaction chamber is 850-959°C.

步骤206、在有源层上生长低温P型层。Step 206 , growing a low-temperature P-type layer on the active layer.

在本实施例中,低温P型层为GaN层,厚度为20~100nm。生长高温P型层时,反应室温度为700~900℃,反应室压力控制在100~300torr。In this embodiment, the low-temperature P-type layer is a GaN layer with a thickness of 20-100 nm. When growing a high-temperature P-type layer, the temperature of the reaction chamber is 700-900° C., and the pressure of the reaction chamber is controlled at 100-300 torr.

步骤207、在低温P型层上生长电子阻挡层。Step 207 , growing an electron blocking layer on the low-temperature P-type layer.

具体地,电子阻挡层为包括N个周期的AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构,0.05<x<0.15,0.2<y<0.4,N为大于等于2的正整数。Specifically, the electron blocking layer is an Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure including N periods, 0.05<x<0.15, 0.2<y<0.4, and N is A positive integer greater than or equal to 2.

优选地,x=0.1,y=0.38。此时LED的发光效率最好。Preferably, x=0.1, y=0.38. At this time, the luminous efficiency of the LED is the best.

进一步地,在AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个AlxGa1-xN子层的厚度为0.5~1.5nm。若每个AlxGa1-xN子层的厚度小于0.5nm,则起不到降低电子阻挡层与低温P型层的晶格失配的作用,若每个AlxGa1-xN子层的厚度大于1.5nm,则会造成浪费,还会导致电子阻挡层的厚度过厚,影响LED的发光效率。Further, the thickness of each AlxGa1 - xN sublayer in the AlxGa1 - xN/AlN/GaN/InyGa1 -yN superlattice structure is 0.5-1.5nm. If the thickness of each Al x Ga 1-x N sublayer is less than 0.5nm, it will not be effective in reducing the lattice mismatch between the electron blocking layer and the low-temperature P-type layer. If each Al x Ga 1-x N sublayer If the thickness of the layer is greater than 1.5nm, it will cause waste, and also cause the thickness of the electron blocking layer to be too thick, which will affect the luminous efficiency of the LED.

进一步地,在AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个AlN子层的厚度为0.5~1.5nm。若每个AlN子层的厚度小于0.5nm,则起不到阻挡电子的作用。若每个AlN子层的厚度大于1.5nm,则会造成浪费,还会导致电子阻挡层的厚度过厚,影响LED的发光效率。Further, the thickness of each AlN sublayer in the AlxGa1 - xN /AlN/GaN/InyGa1 -yN superlattice structure is 0.5-1.5nm. If the thickness of each AlN sub-layer is less than 0.5nm, it will not play the role of blocking electrons. If the thickness of each AlN sub-layer is greater than 1.5 nm, it will cause waste, and also cause the thickness of the electron blocking layer to be too thick, which will affect the luminous efficiency of the LED.

进一步地,在AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个GaN子层的厚度为1~2nm。若每个GaN子层的厚度小于1nm,则无法产生一定的二维电子气,以提供更多的空穴,提高载流子的迁移速率,若每个GaN子层的厚度大于2nm,则会造成浪费,还会导致电子阻挡层的厚度过厚,影响LED的发光效率。Further, the thickness of each GaN sublayer in the Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure is 1-2 nm. If the thickness of each GaN sublayer is less than 1nm, a certain two-dimensional electron gas cannot be generated to provide more holes and increase the mobility of carriers. If the thickness of each GaN sublayer is greater than 2nm, it will It causes waste, and also causes the thickness of the electron blocking layer to be too thick, which affects the luminous efficiency of the LED.

进一步地,在AlxGa1-xN/AlN/GaN/InyGa1-yN超晶格结构中每个InyGa1-yN子层的厚度为1~2nm。若每个InyGa1-yN子层的厚度小于1nm,则无法增强二维电子气的产生,若每个InyGa1-yN子层的厚度大于2nm,则会造成浪费,还会导致电子阻挡层的厚度过厚,影响LED的发光效率。Further, the thickness of each In y Ga 1-y N sublayer in the Al x Ga 1-x N/AlN/GaN/In y Ga 1-y N superlattice structure is 1-2 nm. If the thickness of each In y Ga 1-y N sublayer is less than 1 nm, the generation of two-dimensional electron gas cannot be enhanced, and if the thickness of each In y Ga 1-y N sublayer is greater than 2 nm, it will cause waste, and also It will cause the thickness of the electron blocking layer to be too thick, which will affect the luminous efficiency of the LED.

其中,2≤N≤5。若N小于2,则会导致电子阻挡层的厚度过薄,无法起到阻挡电子,增加空穴,提高载流子的迁移速率的作用。若N大于5,则会导致电子阻挡层的厚度过厚,降低LED的发光效率。Among them, 2≤N≤5. If N is less than 2, the thickness of the electron blocking layer will be too thin, which cannot block electrons, increase holes, and increase the mobility of carriers. If N is greater than 5, the thickness of the electron blocking layer will be too thick, reducing the luminous efficiency of the LED.

在本实施例中,每个AlxGa1-xN子层的厚度为1nm,每个AlN子层的厚度为1nm,每个GaN子层的厚度为1nm,每个InyGa1-yN子层的厚度为2nm,2≤N≤5,电子阻挡层6的厚度为10~25nm。In this embodiment, each AlxGa1 - xN sublayer has a thickness of 1nm, each AlN sublayer has a thickness of 1nm, each GaN sublayer has a thickness of 1nm, and each InyGa1 - y The thickness of the N sublayer is 2nm, 2≤N≤5, and the thickness of the electron blocking layer 6 is 10-25nm.

步骤208、在电子阻挡层上生长高温P型层。Step 208 , growing a high-temperature P-type layer on the electron blocking layer.

在本实施例中,高温P型层为GaN层,厚度为20~50nm。生长高温P型层时,反应室温度为850~1080℃,反应室压力控制在100~300torr。In this embodiment, the high-temperature P-type layer is a GaN layer with a thickness of 20-50 nm. When growing a high-temperature P-type layer, the temperature of the reaction chamber is 850-1080° C., and the pressure of the reaction chamber is controlled at 100-300 torr.

步骤209、在高温P型层上生长P型接触层。Step 209 , growing a P-type contact layer on the high-temperature P-type layer.

在本实施例中,P型接触层为GaN层,厚度为5~300nm。生长P型层时,反应室温度为850~1050℃,反应室压力控制在100~300torr。In this embodiment, the P-type contact layer is a GaN layer with a thickness of 5-300 nm. When growing the P-type layer, the temperature of the reaction chamber is 850-1050° C., and the pressure of the reaction chamber is controlled at 100-300 torr.

外延片生长结束后,将反应腔温度降低至650℃~850℃,在氮气气氛中将外延片退火处理5~15min,然后降至室温,外延生长结束。After the growth of the epitaxial wafer is completed, the temperature of the reaction chamber is lowered to 650° C. to 850° C., and the epitaxial wafer is annealed in a nitrogen atmosphere for 5 to 15 minutes, and then lowered to room temperature, and the epitaxial growth ends.

在结束上述发光二极管外延片的生长之后,将反应室的温度降至600~900℃,在PN2气氛进行退火处理10~30min,而后逐渐降至室温,随后,经过清洗、沉积、光刻和刻蚀后续加工工艺制成单颗9*27mil的芯片。After the growth of the above-mentioned light-emitting diode epitaxial wafer is completed, the temperature of the reaction chamber is lowered to 600-900 ° C, annealing is performed in a PN 2 atmosphere for 10-30 minutes, and then gradually lowered to room temperature, and then, after cleaning, deposition, photolithography and A single 9*27mil chip is made by the subsequent etching process.

经过测试后发现,采用现有技术制成的LED芯片,在20mA驱动电流下的光强为104mW,采用本发明实施例提供的制造方法制成的LED芯片,在20mA驱动电流下的光强为106mW,发光效率约提升了2%。After testing, it is found that the light intensity of the LED chip made by using the prior art is 104mW under the driving current of 20mA, and the light intensity of the LED chip made by the manufacturing method provided by the embodiment of the present invention is 104mW under the driving current of 20mA. 106mW, the luminous efficiency has increased by about 2%.

以上所述仅为本发明的较佳实施例,并不用以限制本发明,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included in the protection of the present invention. within range.

Claims (10)

1. a kind of LED epitaxial slice, the LED epitaxial slice includes substrate, and is sequentially laminated on the lining Buffer layer, undoped GaN layer, N-type layer, active layer, low temperature P-type layer, electronic barrier layer, high temperature P-type layer and p-type on bottom connect Contact layer, the low temperature P-type layer are GaN layer, which is characterized in that
The electronic barrier layer is the Al for including N number of periodxGa1-xN/AlN/GaN/InyGa1-yN superlattice structure, 0.05<x< 0.15,0.2<y<0.4, N is positive integer more than or equal to 2, the electronic barrier layer with a thickness of 10~25nm.
2. LED epitaxial slice according to claim 1, which is characterized in that in the AlxGa1-xN/AlN/GaN/ InyGa1-yEach Al in N superlattice structurexGa1-xN sublayer with a thickness of 0.5~1.5nm.
3. LED epitaxial slice according to claim 1 or 2, which is characterized in that in the AlxGa1-xN/AlN/ GaN/InyGa1-yEach AlN sublayer with a thickness of 0.5~1.5nm in N superlattice structure.
4. LED epitaxial slice according to claim 1 or 2, which is characterized in that in the AlxGa1-xN/AlN/ GaN/InyGa1-yEach GaN sublayer with a thickness of 1~2nm in N superlattice structure.
5. LED epitaxial slice according to claim 1 or 2, which is characterized in that in the AlxGa1-xN/AlN/ GaN/InyGa1-yEach In in N superlattice structureyGa1-yN sublayer with a thickness of 1~2nm.
6. LED epitaxial slice according to claim 1 or 2, which is characterized in that 2≤N≤5.
7. LED epitaxial slice according to claim 1 or 2, which is characterized in that x=0.1, y=0.38.
8. a kind of manufacturing method of LED epitaxial slice, which is characterized in that the manufacturing method includes:
One substrate is provided;
Successively grown buffer layer, undoped GaN layer, N-type layer, active layer and low temperature P-type layer over the substrate, the low temperature P-type layer is GaN layer;
Electronic barrier layer is grown in the low temperature P-type layer, the electronic barrier layer is the Al for including N number of periodxGa1-xN/AlN/ GaN/InyGa1-yN superlattice structure, 0.05<x<0.15,0.2<y<0.4, N is the positive integer more than or equal to 2, the electronics resistance Barrier with a thickness of 10~25nm;
High temperature P-type layer and p-type contact layer are grown on the electronic barrier layer.
9. manufacturing method according to claim 8, which is characterized in that the growth temperature of the electronic barrier layer be 850~ 1080℃。
10. manufacturing method according to claim 8 or claim 9, which is characterized in that the growth pressure of the electronic barrier layer is 200~500Torr.
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