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CN109980056A - Gallium nitride based LED epitaxial slice and its manufacturing method - Google Patents

Gallium nitride based LED epitaxial slice and its manufacturing method Download PDF

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CN109980056A
CN109980056A CN201910152555.0A CN201910152555A CN109980056A CN 109980056 A CN109980056 A CN 109980056A CN 201910152555 A CN201910152555 A CN 201910152555A CN 109980056 A CN109980056 A CN 109980056A
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quantum well
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CN109980056B (en
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刘旺平
乔楠
吕蒙普
胡加辉
李鹏
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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]
    • H10H20/01Manufacture 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
    • H10H20/01335Manufacture 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 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
    • H10H20/811Bodies 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

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Abstract

本发明公开了一种氮化镓基发光二极管外延片及其制造方法,属于半导体技术领域。氮化镓基发光二极管外延片包括衬底、以及依次生长在衬底上的低温缓冲层、三维成核层、二维恢复层、未掺杂的GaN层、N型层、应力释放层、多量子阱层、电子阻挡层、P型层和P型接触层,应力释放层包括多个交替生长的第一超晶格结构和第二超晶格结构,第一超晶格结构为低温InGaN/GaN超晶格结构,第二超晶格结构为高温InGaN/GaN超晶格结构。本发明提供的发光二极管外延片可以优化V型坑的开口大小,提高LED的内量子发光效率,同时提高外延层的晶体质量。

The invention discloses a gallium nitride-based light-emitting diode epitaxial wafer and a manufacturing method thereof, belonging to the technical field of semiconductors. The gallium nitride-based light-emitting diode epitaxial wafer includes a substrate, and a low-temperature buffer layer, a three-dimensional nucleation layer, a two-dimensional recovery layer, an undoped GaN layer, an N-type layer, a stress release layer, a multi-layered The quantum well layer, the electron blocking layer, the P-type layer and the P-type contact layer, and the stress release layer includes a plurality of alternately grown first superlattice structures and second superlattice structures, and the first superlattice structure is low-temperature InGaN/ GaN superlattice structure, the second superlattice structure is a high temperature InGaN/GaN superlattice structure. The light-emitting diode epitaxial wafer provided by the invention can optimize the opening size of the V-shaped pit, improve the internal quantum luminous efficiency of the LED, and at the same time improve the crystal quality of the epitaxial layer.

Description

氮化镓基发光二极管外延片及其制造方法Gallium nitride-based light-emitting diode epitaxial wafer and manufacturing method thereof

技术领域technical field

本发明涉及半导体技术领域,特别涉及一种氮化镓基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 gallium nitride-based 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。LED作为一种高效、环保、绿色新型固态照明光源,正在被迅速广泛地应用到如交通信号灯、汽车内外灯、城市景观照明、手机背光源等领域中。LED (Light Emitting Diode, light-emitting diode) is a semiconductor electronic component that can emit light. As a high-efficiency, environmentally friendly and green new solid-state lighting source, LED is being rapidly and widely used in fields such as traffic lights, interior and exterior lights of automobiles, urban landscape lighting, and mobile phone backlights.

外延片是LED中的主要构成部分,现有的GaN基LED外延片包括蓝宝石衬底、以及依次层叠在蓝宝石衬底上的低温缓冲层、三维成核层、二维恢复层、未掺杂的GaN层、N型层、多量子阱层、电子阻挡层、P型层和P型接触层。由于蓝宝石衬底与GaN外延层之间存在较大的晶格失配,使得外延层中会产生应力,进而产生大量的穿透位错,应力和穿透位错沿外延片的层叠方向延伸到多量子阱层中会严重影响LED的发光。为了提高LED的发光效率,通常会在N型层和多量子阱层之间设置一层应力释放层,以释放底层应力,减少位错产生。Epitaxial wafers are the main components of LEDs. Existing GaN-based LED epitaxial wafers include a sapphire substrate, a low-temperature buffer layer, a three-dimensional nucleation layer, a two-dimensional recovery layer, and an undoped sapphire substrate sequentially stacked on the sapphire substrate. GaN layer, N-type layer, multiple quantum well layer, electron blocking layer, P-type layer and P-type contact layer. Due to the large lattice mismatch between the sapphire substrate and the GaN epitaxial layer, stress will be generated in the epitaxial layer, and then a large number of threading dislocations will be generated. The stress and threading dislocations extend along the stacking direction of the epitaxial wafer to In the multiple quantum well layer, the luminescence of the LED will be seriously affected. In order to improve the luminous efficiency of the LED, a stress release layer is usually arranged between the N-type layer and the multiple quantum well layer to release the underlying stress and reduce the generation of dislocations.

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 found that the prior art has at least the following problems:

由于现有技术中的应力释放层通常在低温恒温条件生长,以保证其应力释放的效果。而穿透位错在低温条件下会引发V型坑的形成,且在低温条件下,GaN的横向外延能力变差,V型坑的开口会逐渐增大。当V型坑开口过大时,V型坑倾斜面的势垒高度降低,对载流子限制能力减弱,会导致电子和空穴之间进行非辐射复合,使得LED的内量子发光效率降低。同时在低温条件下,形成的V型坑的密度会逐渐增多,从而导致外延层的晶体质量下降。Because the stress release layer in the prior art is usually grown at a low temperature and constant temperature to ensure its stress release effect. Threading dislocations will lead to the formation of V-type pits at low temperature, and under low temperature conditions, the lateral epitaxy capability of GaN will deteriorate, and the opening of V-type pits will gradually increase. When the opening of the V-shaped pit is too large, the potential barrier height of the inclined surface of the V-shaped pit is reduced, and the carrier confinement ability is weakened, which will lead to non-radiative recombination between electrons and holes, which reduces the internal quantum luminous efficiency of the LED. At the same time, under low temperature conditions, the density of the formed V-shaped pits will gradually increase, resulting in a decrease in the crystal quality of the epitaxial layer.

发明内容SUMMARY OF THE INVENTION

本发明实施例提供了一种氮化镓基发光二极管外延片及其制造方法,可以优化V型坑的开口大小,提高LED的内量子发光效率,同时提高外延层的晶体质量。所述技术方案如下:The embodiments of the present invention provide a gallium nitride-based light emitting diode epitaxial wafer and a manufacturing method thereof, which can optimize the opening size of the V-shaped pit, improve the internal quantum luminous efficiency of the LED, and simultaneously improve the crystal quality of the epitaxial layer. The technical solution is as follows:

一方面,本发明提供了一种氮化镓基发光二极管外延片,所述氮化镓基发光二极管外延片包括衬底、以及依次生长在所述衬底上的低温缓冲层、三维成核层、二维恢复层、未掺杂的GaN层、N型层、应力释放层、多量子阱层、电子阻挡层、P型层和P型接触层,In one aspect, the present invention provides a gallium nitride-based light-emitting diode epitaxial wafer, the gallium nitride-based light-emitting diode epitaxial wafer includes a substrate, and a low-temperature buffer layer and a three-dimensional nucleation layer sequentially grown on the substrate , 2D recovery layer, undoped GaN layer, N-type layer, stress release layer, multiple quantum well layer, electron blocking layer, P-type layer and P-type contact layer,

所述应力释放层包括多个交替生长的第一超晶格结构和第二超晶格结构,所述第一超晶格结构为低温InGaN/GaN超晶格结构,所述第二超晶格结构为高温InGaN/GaN超晶格结构。The stress release layer includes a plurality of alternately grown first superlattice structures and second superlattice structures, the first superlattice structure is a low-temperature InGaN/GaN superlattice structure, and the second superlattice structure is The structure is a high temperature InGaN/GaN superlattice structure.

进一步地,所述应力释放层的厚度为100~150nm。Further, the thickness of the stress release layer is 100-150 nm.

进一步地,所述多量子阱层包括靠近所述N型层的第一类多量子阱层、靠近所述P型层的第三类多量子阱层、以及位于所述第一类多量子阱层和所述第三类多量子阱层之间的第二类多量子阱层;Further, the multiple quantum well layer includes a first type multiple quantum well layer close to the N-type layer, a third type multiple quantum well layer close to the P type layer, and a first type multiple quantum well layer located at the a second type of multiple quantum well layer between the layer and the third type of multiple quantum well layer;

所述第一类多量子阱层由多个周期的InaGa1-aN/AlcGa1-cN超晶格组成,所述第二类多量子阱层由多个周期的InaGa1-aN/GaN超晶格组成,所述第三类多量子阱层由多个周期的InaGa1-aN/InbGa1-bN超晶格组成,0.1<a<1,0<b<0.3,b<a,0<c<0.2。The first type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/Al c Ga 1-c N superlattice, and the second type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/GaN superlattice, the third type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/In b Ga 1-b N superlattice, 0.1<a< 1, 0<b<0.3, b<a, 0<c<0.2.

进一步地,所述第一类量子阱层、所述第二类量子阱层和所述第三类量子阱层中的InaGa1-aN层的厚度均相等。Further, the thicknesses of the In a Ga 1-a N layers in the first type quantum well layer, the second type quantum well layer and the third type quantum well layer are all equal.

进一步地,所述第一类量子阱层中的AlcGa1-cN层、所述第二类量子阱层中的GaN层和所述第三类量子阱层中的InbGa1-bN层的厚度均相等。Further, the Al c Ga 1-c N layer in the first type of quantum well layer, the GaN layer in the second type of quantum well layer, and the In b Ga 1- in the third type of quantum well layer b The thicknesses of the N layers are all equal.

另一方面,本发明提供了一种氮化镓基发光二极管外延片的制造方法,所述制造方法包括:In another aspect, the present invention provides a method for manufacturing a gallium nitride-based 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低温缓冲层、三维成核层、二维恢复层、未掺杂的GaN层、N型层;growing a low-temperature buffer layer, a three-dimensional nucleation layer, a two-dimensional recovery layer, an undoped GaN layer, and an N-type layer in sequence on the substrate;

在所述N型层上生长应力释放层,所述应力释放层包括多个交替生长的第一超晶格结构和第二超晶格结构,所述第一超晶格结构为低温InGaN/GaN超晶格结构,所述第二超晶格结构为高温InGaN/GaN超晶格结构;A stress release layer is grown on the N-type layer, the stress release layer includes a plurality of alternately grown first superlattice structures and second superlattice structures, and the first superlattice structure is low temperature InGaN/GaN a superlattice structure, wherein the second superlattice structure is a high-temperature InGaN/GaN superlattice structure;

在所述应力释放层上依次生长多量子阱层、电子阻挡层、P型层和P型接触层。A multiple quantum well layer, an electron blocking layer, a P-type layer and a P-type contact layer are sequentially grown on the stress release layer.

进一步地,在所述N型层上生长应力释放层,包括:Further, growing a stress release layer on the N-type layer includes:

在780℃~880℃的温度下,生长所述第一超晶格结构;growing the first superlattice structure at a temperature of 780°C to 880°C;

在830℃~930℃的温度下,生长所述第二超晶格结构。The second superlattice structure is grown at a temperature of 830°C to 930°C.

进一步地,所述多量子阱层包括靠近所述N型层的第一类多量子阱层、靠近所述P型层的第三类多量子阱层、以及位于所述第一类多量子阱层和所述第三类多量子阱层之间的第二类多量子阱层;Further, the multiple quantum well layer includes a first type multiple quantum well layer close to the N-type layer, a third type multiple quantum well layer close to the P type layer, and a first type multiple quantum well layer located at the a second type of multiple quantum well layer between the layer and the third type of multiple quantum well layer;

所述第一类多量子阱层由多个周期的InaGa1-aN/AlcGa1-cN超晶格组成,所述第二类多量子阱层由多个周期的InaGa1-aN/GaN超晶格组成,所述第三类多量子阱层由多个周期的InaGa1-aN/InbGa1-bN超晶格组成,0.1<a<1,0<b<0.3,b<a,0<c<0.2。The first type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/Al c Ga 1-c N superlattice, and the second type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/GaN superlattice, the third type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/In b Ga 1-b N superlattice, 0.1<a< 1, 0<b<0.3, b<a, 0<c<0.2.

进一步地,所述第一类量子阱层、所述第二类量子阱层和所述第三类量子阱层中的InaGa1-aN层的厚度均相等。Further, the thicknesses of the In a Ga 1-a N layers in the first type quantum well layer, the second type quantum well layer and the third type quantum well layer are all equal.

进一步地,所述第一类量子阱层中的AlcGa1-cN层、所述第二类量子阱层中的GaN层和所述第三类量子阱层中的InbGa1-bN层的厚度均相等。Further, the Al c Ga 1-c N layer in the first type of quantum well layer, the GaN layer in the second type of quantum well layer, and the In b Ga 1- in the third type of quantum well layer b The thicknesses of the N layers are all equal.

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 solutions provided in the embodiments of the present invention are:

通过将应力释放层设置为包括多个交替生长的第一超晶格结构和第二超晶格结构。其中,第一超晶格结构为低温InGaN/GaN超晶格结构,第一超晶格结构采用低温生长而成,可以保证应力释放层具有较好的应力释放效果。但是第一超晶格结构在低温生长时会引发V型坑的形成,因此,本发明通过在第一超晶格结构之后生长第二超晶格结构,第二超晶格结构为高温InGaN/GaN超晶格结构,在高温条件下,GaN的横向外延能力增强,可以抑制V型坑的开口继续变大,从而将V型坑的开口控制在合适的范围内,避免了V型坑开口过大,造成LED的内量子发光效率降低的情况出现。同时在高温条件下,形成的V型坑的密度会逐渐减少,从而可以提高外延层的晶体质量。且本发明中的应力释放层包括多个交替生长的低温InGaN/GaN超晶格结构和高温InGaN/GaN超晶格结构,与单层结构的应力释放层(即只包括一个低温InGaN/GaN超晶格结构和一个高温InGaN/GaN超晶格结构)相比,对V型坑的开口控制效果更好。By disposing the stress release layer to include a plurality of alternately grown first superlattice structures and second superlattice structures. The first superlattice structure is a low-temperature InGaN/GaN superlattice structure, and the first superlattice structure is grown at a low temperature, which can ensure that the stress release layer has a good stress release effect. However, when the first superlattice structure is grown at a low temperature, the formation of V-type pits will be induced. Therefore, in the present invention, the second superlattice structure is grown after the first superlattice structure, and the second superlattice structure is high temperature InGaN/ GaN superlattice structure, under high temperature conditions, the lateral epitaxy capability of GaN is enhanced, which can restrain the opening of the V-shaped pit from continuing to increase, so as to control the opening of the V-shaped pit within a suitable range and avoid the excessive opening of the V-shaped pit. large, resulting in a decrease in the internal quantum luminous efficiency of the LED. At the same time, under high temperature conditions, the density of the formed V-shaped pits will gradually decrease, so that the crystal quality of the epitaxial layer can be improved. And the stress release layer in the present invention includes a plurality of alternately grown low-temperature InGaN/GaN superlattice structures and high-temperature InGaN/GaN superlattice structures, and the stress release layer of a single-layer structure (that is, only comprising a low-temperature InGaN/GaN superlattice structure) Compared with a high temperature InGaN/GaN superlattice structure), the opening control effect of the V-type pit is better.

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 illustrate the technical solutions in the embodiments of the present invention more clearly, the following briefly introduces the accompanying drawings used in the description of the embodiments. Obviously, the accompanying drawings in the following description are only some embodiments of the present invention. For those of ordinary skill in the art, other drawings can also be obtained from these drawings without creative effort.

图1是本发明实施例提供的一种V型坑在多量子阱层中的开口结构示意图;1 is a schematic diagram of an opening structure of a V-type pit in a multiple quantum well layer provided by an embodiment of the present invention;

图2是本发明实施例提供的一种氮化镓基发光二极管外延片的结构示意图;2 is a schematic structural diagram of a gallium nitride-based light-emitting diode epitaxial wafer provided by an embodiment of the present invention;

图3是本发明实施例提供的一种多量子阱层的结构示意图;3 is a schematic structural diagram of a multiple quantum well layer provided by an embodiment of the present invention;

图4是本发明实施例提供的一种氮化镓基发光二极管外延片的制造方法流程图。FIG. 4 is a flowchart of a method for manufacturing a gallium nitride-based light-emitting diode epitaxial wafer according to 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 objectives, technical solutions and advantages of the present invention clearer, the embodiments of the present invention will be further described in detail below with reference to the accompanying drawings.

图1是本发明实施例提供的一种V型坑在多量子阱层中的开口结构示意图,如图1所示,图1中的△L表示穿透位错的中心到V型坑边缘的扩散距离,△E表示V型坑的倾斜面上量子阱的势垒高度。由于蓝宝石衬底与GaN外延层之间存在较大的晶格失配,会产生大量的穿透位错,而穿透位错会成为载流子的泄露通道,进而捕获少部分的载流子形成非辐射复合中心,导致LED的发光效率下降。穿透位错在低温条件下会引发V型坑的形成。1 is a schematic diagram of an opening structure of a V-type pit in a multiple quantum well layer provided by an embodiment of the present invention. As shown in FIG. 1 , ΔL in FIG. 1 represents the distance from the center of the threading dislocation to the edge of the V-type pit. Diffusion distance, ΔE represents the barrier height of the quantum well on the inclined surface of the V-type pit. Due to the large lattice mismatch between the sapphire substrate and the GaN epitaxial layer, a large number of threading dislocations will be generated, and threading dislocations will become the leakage channels of carriers, thereby capturing a small part of the carriers. A non-radiative recombination center is formed, resulting in a decrease in the luminous efficiency of the LED. Threading dislocations can induce the formation of V-shaped pits at low temperature.

当V型坑的开口过小时,△L较小,穿透位错中心到V型坑边缘的扩散距离会相对较短,使得载流子更容易被捕获进入穿透位错中心;△E较大,V型坑的倾斜面具有更高的势垒,对载流子限制能力较强,可以有效钝化穿透位错的非辐射中心。When the opening of the V-shaped pit is too small, the ΔL is small, and the diffusion distance from the center of the threading dislocation to the edge of the V-shaped pit will be relatively short, making it easier for carriers to be captured into the center of the threading dislocation; The inclined surface of the V-shaped pit has a higher potential barrier, which has a strong ability to confine carriers and can effectively passivate the non-radiative center of threading dislocations.

当V型坑的开口过大时,△L较大,穿透位错中心到V型坑边缘的扩散距离会相对较长,可以抑制载流子进入非辐射复合中心;△E较小,V型坑的倾斜面的势垒高度降低,对载流子限制能力减弱,穿透位错仍然会成为载流子的泄露通道,进而捕获少部分的载流子形成非辐射复合中心,导致LED的发光效率下降。When the opening of the V-shaped pit is too large, the △L is large, and the diffusion distance from the center of the threading dislocation to the edge of the V-shaped pit will be relatively long, which can inhibit the carriers from entering the non-radiative recombination center; when the △E is small, the V The potential barrier height of the inclined surface of the pit is reduced, and the confinement ability of carriers is weakened. The threading dislocations will still become the leakage channels of the carriers, and then capture a small part of the carriers to form a non-radiative recombination center, resulting in the LED's degradation. Luminous efficiency decreases.

因此,V型坑的开口过大或过小都会影响LED的发光效率。本发明实施例提供了一种氮化镓基发光二极管外延片及其制造方法,可以优化V型坑的开口大小,提高LED的内量子发光效率,同时提高外延层的晶体质量。Therefore, if the opening of the V-shaped pit is too large or too small, the luminous efficiency of the LED will be affected. The embodiments of the present invention provide a gallium nitride-based light emitting diode epitaxial wafer and a manufacturing method thereof, which can optimize the opening size of the V-shaped pit, improve the internal quantum luminous efficiency of the LED, and simultaneously improve the crystal quality of the epitaxial layer.

图2是本发明实施例提供的一种氮化镓基发光二极管外延片的结构示意图,如图2所示,氮化镓基发光二极管外延片包括衬底1、以及依次生长在衬底1上的低温缓冲层2、三维成核层3、二维恢复层4、未掺杂的GaN层5、N型层6、应力释放层7、多量子阱层8、电子阻挡层9、P型层10和P型接触层11。FIG. 2 is a schematic structural diagram of a GaN-based light-emitting diode epitaxial wafer provided by an embodiment of the present invention. As shown in FIG. 2 , the GaN-based light-emitting diode epitaxial wafer includes a substrate 1 and is sequentially grown on the substrate 1 low temperature buffer layer 2, three-dimensional nucleation layer 3, two-dimensional recovery layer 4, undoped GaN layer 5, N-type layer 6, stress release layer 7, multiple quantum well layer 8, electron blocking layer 9, P-type layer 10 and P-type contact layer 11.

应力释放层7包括多个交替生长的第一超晶格结构71和第二超晶格结构72,第一超晶格结构71为低温InGaN/GaN超晶格结构,第二超晶格结构72为高温InGaN/GaN超晶格结构。The stress release layer 7 includes a plurality of alternately grown first superlattice structures 71 and second superlattice structures 72 , the first superlattice structure 71 is a low-temperature InGaN/GaN superlattice structure, and the second superlattice structure 72 It is a high temperature InGaN/GaN superlattice structure.

本发明实施例通过将应力释放层设置为包括多个交替生长的第一超晶格结构和第二超晶格结构。其中,第一超晶格结构为低温InGaN/GaN超晶格结构,第一超晶格结构采用低温生长而成,可以保证应力释放层具有较好的应力释放效果。但是第一超晶格结构在低温生长时会引发V型坑的形成,因此,本发明通过在第一超晶格结构之后生长第二超晶格结构,第二超晶格结构为高温InGaN/GaN超晶格结构,在高温条件下,GaN的横向外延能力增强,可以抑制V型坑的开口继续变大,从而将V型坑的开口控制在合适的范围内,避免了V型坑开口过大,造成LED的内量子发光效率降低的情况出现。同时在高温条件下,形成的V型坑的密度会逐渐减少,从而可以提高外延层的晶体质量。且本发明中的应力释放层包括多个交替生长的低温InGaN/GaN超晶格结构和高温InGaN/GaN超晶格结构,与单层结构的应力释放层(即只包括一个低温InGaN/GaN超晶格结构和一个高温InGaN/GaN超晶格结构)相比,对V型坑的开口控制效果更好。In the embodiment of the present invention, the stress release layer is configured to include a plurality of alternately grown first superlattice structures and second superlattice structures. The first superlattice structure is a low-temperature InGaN/GaN superlattice structure, and the first superlattice structure is grown at a low temperature, which can ensure that the stress release layer has a good stress release effect. However, when the first superlattice structure is grown at a low temperature, the formation of V-type pits will be induced. Therefore, in the present invention, the second superlattice structure is grown after the first superlattice structure, and the second superlattice structure is high temperature InGaN/ GaN superlattice structure, under high temperature conditions, the lateral epitaxy capability of GaN is enhanced, which can restrain the opening of the V-shaped pit from continuing to increase, so as to control the opening of the V-shaped pit within a suitable range and avoid the excessive opening of the V-shaped pit. large, resulting in a decrease in the internal quantum luminous efficiency of the LED. At the same time, under high temperature conditions, the density of the formed V-shaped pits will gradually decrease, so that the crystal quality of the epitaxial layer can be improved. And the stress release layer in the present invention includes a plurality of alternately grown low-temperature InGaN/GaN superlattice structures and high-temperature InGaN/GaN superlattice structures, and the stress release layer of a single-layer structure (that is, only comprising a low-temperature InGaN/GaN superlattice structure) Compared with a high temperature InGaN/GaN superlattice structure), the opening control effect of the V-type pit is better.

需要说明的是,在本实施例中可以通过发光效率的高低反推出较优的V型坑开口大小,其中V型坑的开口直径控制在200~300nm之间效果较好。It should be noted that, in this embodiment, a better opening size of the V-shaped pit can be deduced from the level of luminous efficiency, wherein the opening diameter of the V-shaped pit is controlled to be between 200 and 300 nm.

可选地,应力释放层7包括N个交替生长的第一超晶格结构71和第二超晶格结构72,2≤N≤12。若N的个数过多会导致低温、高温的转换次数较多,若N的个数过少,则无法有效控制V型坑的开口。Optionally, the stress release layer 7 includes N alternately grown first superlattice structures 71 and second superlattice structures 72 , where 2≦N≦12. If the number of N is too large, the number of switching between low temperature and high temperature will be large, and if the number of N is too small, the opening of the V-shaped pit cannot be effectively controlled.

示例性地,N=8。此时即可有效控制V型坑的开口,又不会使应力释放层的生长过程过于复杂。Illustratively, N=8. At this time, the opening of the V-shaped pit can be effectively controlled, and the growth process of the stress release layer will not be too complicated.

进一步地,第一超晶格结构71中的低温InGaN层71a和第二超晶格结构72中的高温InGaN层72a均为InxGa1-xN层,0.05<x<0.4。In的含量在该取值范围内时,应力释放层释放应力的效果最好。Further, the low temperature InGaN layer 71a in the first superlattice structure 71 and the high temperature InGaN layer 72a in the second superlattice structure 72 are both InxGa1 - xN layers, 0.05<x<0.4. When the content of In is within this value range, the stress-releasing layer has the best effect of stress-releasing.

可选地,第一超晶格结构71和第二超晶格结构72的厚度相等,以便于周期性的控制应力释放层的生长,使得V型坑的开口和V型坑的密度均匀变化。Optionally, the thicknesses of the first superlattice structure 71 and the second superlattice structure 72 are equal, so as to periodically control the growth of the stress relief layer, so that the opening of the V-shaped pits and the density of the V-shaped pits vary uniformly.

示例性地,第一超晶格结构71中的低温InGaN层71a和第二超晶格结构72中的高温InGaN层72a的厚度均为1~2nm。第一超晶格结构71中的GaN层71b和第二超晶格结构72中的GaN层72b的厚度均为10~40nm。Exemplarily, the thicknesses of the low temperature InGaN layer 71 a in the first superlattice structure 71 and the high temperature InGaN layer 72 a in the second superlattice structure 72 are both 1-2 nm. The thicknesses of the GaN layer 71b in the first superlattice structure 71 and the GaN layer 72b in the second superlattice structure 72 are both 10 to 40 nm.

在其它实现方式中,第一超晶格结构71和第二超晶格结构72的厚度也可以不相等。In other implementations, the thicknesses of the first superlattice structure 71 and the second superlattice structure 72 may also be unequal.

进一步地,应力释放层7的厚度为100~150nm。若应力释放层7的厚度过厚,会使得应力释放层7的晶体质量下降,若应力释放层7的厚度过,则起不到释放应力的作用。将应力释放层7的厚度设置为100~150nm,可以在保证应力释放层7的晶体质量同时,较好的释放底层应力。Further, the thickness of the stress release layer 7 is 100-150 nm. If the thickness of the stress relief layer 7 is too thick, the crystal quality of the stress relief layer 7 will decrease, and if the thickness of the stress relief layer 7 is too thick, the effect of stress relief will not be achieved. Setting the thickness of the stress release layer 7 to 100-150 nm can better release the underlying stress while ensuring the crystal quality of the stress release layer 7 .

图3是本发明实施例提供的一种多量子阱层的结构示意图,如图3所示,多量子阱层8包括靠近N型层6的第一类多量子阱层81、靠近P型层10的第三类多量子阱层83、以及位于第一类多量子阱层81和第三类多量子阱层83之间的第二类多量子阱层82。FIG. 3 is a schematic structural diagram of a multi-quantum well layer provided by an embodiment of the present invention. As shown in FIG. 3 , the multi-quantum well layer 8 includes a first-type multi-quantum well layer 81 close to the N-type layer 6 and a P-type layer close to the The third-type multi-quantum well layer 83 of 10, and the second-type multi-quantum well layer 82 located between the first-type multi-quantum well layer 81 and the third-type multi-quantum well layer 83.

第一类多量子阱层81由多个周期的InaGa1-aN/AlcGa1-cN超晶格组成,第二类多量子阱层82由多个周期的InaGa1-aN/GaN超晶格组成,第三类多量子阱层83由多个周期的InaGa1- aN/InbGa1-bN超晶格组成,0.1<a<1,0<b<0.3,b<a,0<c<0.2。The first type of multiple quantum well layer 81 is composed of multiple periods of In a Ga 1-a N/Al c Ga 1-c N superlattices, and the second type of multiple quantum well layer 82 is composed of multiple periods of In a Ga 1 -a N/GaN superlattice, the third type of multiple quantum well layer 83 is composed of multiple periods of In a Ga 1- a N/In b Ga 1-b N superlattice, 0.1<a<1,0 <b<0.3, b<a, 0<c<0.2.

由于AlGaN、GaN、InbGa1-bN这三种材料的禁带宽度的大小关系为:InGaN<GaN<AlGaN。因此,在应力释放层7中形成的V型坑的生长速率在InGaN、GaN、AlGaN这三种材料中逐渐减小。因此,在靠近N型层6的第一类多量子阱层81中采用AlGaN作为垒层,V型坑的生长速率较慢,可以从开始阶段抑制V型坑开口过快变大,避免V型坑延伸到靠近P型层10的多量子阱层8时开口变得过大,然后在第二类多量子阱层82和第三类多量子阱层83依次采用GaN和InGaN作为垒层,可以防止V型坑的开口过小。当V型坑的开口过小时,穿透位错到V型坑边缘的扩散距离会较短,使得载流子更容易被捕获进入穿透位错中心。The relationship between the forbidden band widths of the three materials, AlGaN, GaN, and InbGa1 - bN , is: InGaN<GaN<AlGaN. Therefore, the growth rate of the V-type pits formed in the stress relief layer 7 gradually decreases in the three materials of InGaN, GaN, and AlGaN. Therefore, when AlGaN is used as the barrier layer in the first-type multiple quantum well layer 81 close to the N-type layer 6, the growth rate of the V-type pit is relatively slow, and the opening of the V-type pit can be suppressed from becoming too fast and enlarged from the initial stage, so as to avoid the V-type pit. When the pit extends to the multiple quantum well layer 8 close to the P-type layer 10, the opening becomes too large, and then GaN and InGaN are used as the barrier layers in the second type multiple quantum well layer 82 and the third type multiple quantum well layer 83 in turn. Prevent the opening of the V-shaped pit from being too small. When the opening of the V-shaped pit is too small, the diffusion distance of the threading dislocation to the edge of the V-shaped pit will be shorter, making it easier for carriers to be trapped into the center of the threading dislocation.

进一步地,第一类量子阱层81、第二类量子阱层82和第三类量子阱层83中的InaGa1-aN层的厚度均相等,从而可以保证发光波长的一致性。Further, the thicknesses of the In a Ga 1-a N layers in the first type quantum well layer 81 , the second type quantum well layer 82 and the third type quantum well layer 83 are all equal, so that the uniformity of the emission wavelength can be ensured.

可选地,第一类量子阱层81中的InaGa1-aN层81a、第二类量子阱层82中的InaGa1-aN层82a、第三类量子阱层83中的InaGa1-aN层的厚度均为3~4nm。Optionally, the In a Ga 1-a N layer 81a in the first type quantum well layer 81, the In a Ga 1-a N layer 82a in the second type quantum well layer 82, and the third type quantum well layer 83 The thickness of the In a Ga 1-a N layers are all 3-4 nm.

进一步地,第一类量子阱层81中的AlcGa1-cN层81b、第二类量子阱层82中的GaN层82b和第三类量子阱层83中的InbGa1-bN层83b的厚度均相等,以便于生长控制V型坑的开口大小。Further, the AlcGa1 - cN layer 81b in the first type quantum well layer 81, the GaN layer 82b in the second type quantum well layer 82, and the InbGa1 -b in the third type quantum well layer 83 The thicknesses of the N layers 83b are all equal to facilitate growth and control the opening size of the V-shaped pit.

在其它实现方式中,第一类量子阱层81中的AlcGa1-cN层81b、第二类量子阱层82中的GaN层82b和第三类量子阱层83中的InbGa1-bN层83b的厚度也可以不相等。In other implementations, the AlcGa1 - cN layer 81b in the first type of quantum well layer 81, the GaN layer 82b in the second type of quantum well layer 82, and the InbGa in the third type of quantum well layer 83 The thickness of the 1-b N layer 83b may also be unequal.

可选地,第一类量子阱层81中的AlcGa1-cN层81b、第二类量子阱层82中的GaN层82b和第三类量子阱层83中的InbGa1-bN层83b的厚度均为9~20nm。Optionally, the AlcGa1 - cN layer 81b in the first type quantum well layer 81, the GaN layer 82b in the second type quantum well layer 82, and the InbGa1 - cN in the third type quantum well layer 83 b The thicknesses of the N layers 83b are all 9 to 20 nm.

可选地,衬底1可以为蓝宝石衬底。Alternatively, the substrate 1 may be a sapphire substrate.

可选地,低温缓冲层2可以为AlN缓冲层,或者GaN缓冲层。Optionally, the low temperature buffer layer 2 may be an AlN buffer layer or a GaN buffer layer.

可选地,三维成核层3可以为GaN层,厚度为400~600nm。Optionally, the three-dimensional nucleation layer 3 may be a GaN layer with a thickness of 400-600 nm.

可选地,二维恢复层4可以为GaN层,厚度为500~800nm。Optionally, the two-dimensional recovery layer 4 may be a GaN layer with a thickness of 500-800 nm.

可选地,未掺杂的GaN层5的厚度为1~2um。Optionally, the thickness of the undoped GaN layer 5 is 1˜2 μm.

可选地,N型层6可以为掺Si的GaN层,厚度为1~2um。Optionally, the N-type layer 6 may be a Si-doped GaN layer with a thickness of 1˜2 μm.

可选地,电子阻挡层9的厚度可以为20~100nm。Optionally, the thickness of the electron blocking layer 9 may be 20˜100 nm.

可选地,P型层10可以为GaN层,厚度为100~300nm。Optionally, the P-type layer 10 may be a GaN layer with a thickness of 100-300 nm.

可选地,发光二极管外延片还可以包括设置在P型层10上的P型接触层11。P型接触层11可以为重掺Mg的GaN层,厚度为50~100nm。Optionally, the light emitting diode epitaxial wafer may further include a P-type contact layer 11 disposed on the P-type layer 10 . The P-type contact layer 11 can be a heavily Mg-doped GaN layer with a thickness of 50-100 nm.

图4是本发明实施例提供的一种氮化镓基发光二极管外延片的制造方法流程图,如图4所示,该制造方法包括:FIG. 4 is a flowchart of a method for manufacturing a GaN-based light-emitting diode epitaxial wafer provided by an embodiment of the present invention. As shown in FIG. 4 , the manufacturing method includes:

步骤401、提供一衬底。Step 401, providing a substrate.

其中,衬底可采用[0001]晶向的Al2O3蓝宝石衬底。Wherein, the substrate can be an Al 2 O 3 sapphire substrate with [0001] crystal orientation.

进一步地,步骤401还可以包括:Further, step 401 may also include:

将衬底在氢气气氛中退火1~10min,以清洁衬底表面,然后对衬底进行氮化处理,氮化处理时的温度控制在1000~1200℃。The substrate is annealed in a hydrogen atmosphere for 1-10 minutes to clean the surface of the substrate, and then the substrate is subjected to nitridation treatment, and the temperature during the nitridation treatment is controlled at 1000-1200° C.

其中,衬底进行退火处理的方式取决于低温缓冲层的生长方式。The manner in which the substrate is annealed depends on the growth manner of the low temperature buffer layer.

当采用PVD(Physical Vapor Deposition,物理气相沉积)方法沉积低温缓冲层时,对衬底进行退火处理包括:将衬底放置到PVD设备的反应腔内,并对反应腔进行抽真空,抽真空的同时开始对衬底进行加热升温。当反应腔内的压力抽至低于1*10-7torr时,将加热温度稳定在350~750℃,对衬底进行烘烤,烘烤时间为2~12min。When the low temperature buffer layer is deposited by PVD (Physical Vapor Deposition) method, annealing the substrate includes: placing the substrate in the reaction chamber of the PVD equipment, and evacuating the reaction chamber. At the same time, the heating and heating of the substrate is started. When the pressure in the reaction chamber is pumped to less than 1*10 -7 torr, the heating temperature is stabilized at 350-750° C., and the substrate is baked for 2-12 minutes.

当采用MOCVD(Metal-organic Chemical Vapor Deposition,金属有机化合物化学气相沉淀)方法沉积低温缓冲层时,对衬底进行退火处理包括:将衬底放置到MOCVD设备的反应腔内,然后在氢气气氛中退火处理10分钟,清洁衬底表面,退火温度在1000℃与1100℃之间,压力在200torr~500torr之间。When the low temperature buffer layer is deposited by MOCVD (Metal-organic Chemical Vapor Deposition) method, the annealing treatment of the substrate includes: placing the substrate in the reaction chamber of the MOCVD equipment, and then in a hydrogen atmosphere The annealing treatment is performed for 10 minutes to clean the surface of the substrate. The annealing temperature is between 1000° C. and 1100° C. and the pressure is between 200torr and 500torr.

步骤402、在衬底上生长低温缓冲层。Step 402, growing a low temperature buffer layer on the substrate.

其中,低温缓冲层可以是GaN缓冲层,也可以是AlN缓冲层。The low temperature buffer layer may be a GaN buffer layer or an AlN buffer layer.

当低温缓冲层是GaN缓冲层时,可以采用MOCVD法生长低温缓冲层,包括:首先,将MOCVD设备的反应腔内温度调整至400℃~600℃,压力调整至200~600torr,生长15~35nm厚的GaN缓冲层。When the low-temperature buffer layer is a GaN buffer layer, the MOCVD method can be used to grow the low-temperature buffer layer, including: first, adjusting the temperature in the reaction chamber of the MOCVD equipment to 400-600°C, adjusting the pressure to 200-600torr, and growing 15-35nm Thick GaN buffer layer.

当低温缓冲层是AlN缓冲层时,可以采用PVD法生长低温缓冲层,包括:将PVD设备的反应腔内温度调整至400~700℃,溅射功率调整至3000~5000W,压力调整至为1~10mtorr,生长15~35nm厚的AlN缓冲层。When the low temperature buffer layer is an AlN buffer layer, the low temperature buffer layer can be grown by PVD method, including: adjusting the temperature in the reaction chamber of the PVD equipment to 400-700°C, adjusting the sputtering power to 3000-5000W, and adjusting the pressure to 1 ~10mtorr, grow 15~35nm thick AlN buffer layer.

需要说明的是,外延层中的未掺杂的GaN层、N型层、应力释放层、多量子阱层、电子阻挡层、P型层以及P型接触层均可以采用MOCVD法生长。在具体实现时,通常是将衬底放在石墨托盘上送入MOCVD设备的反应腔中进行外延材料的生长,因此上述生长过程中控制的温度和压力实际上是指反应腔内的温度和压力。具体地,采用三甲基镓或三甲基乙作为镓源,三乙基硼作为硼源,高纯氮气作为氮源,三甲基铟作为铟源,三甲基铝作为铝源,N型掺杂剂选用硅烷,P型掺杂剂选用二茂镁。It should be noted that the undoped GaN layer, N-type layer, stress release layer, multiple quantum well layer, electron blocking layer, P-type layer and P-type contact layer in the epitaxial layer can all be grown by MOCVD. In the specific implementation, the substrate is usually placed on a graphite tray and sent to the reaction chamber of the MOCVD equipment for the growth of the epitaxial material. Therefore, the temperature and pressure controlled in the above growth process actually refer to the temperature and pressure in the reaction chamber. . Specifically, using trimethyl gallium or trimethyl ethyl as the gallium source, triethyl boron as the boron source, high-purity nitrogen as the nitrogen source, trimethyl indium as the indium source, trimethyl aluminum as the aluminum source, N-type The dopant is selected from silane, and the P-type dopant is selected from magnesium locene.

步骤403、在低温缓冲层上生长三维成核层。Step 403 , growing a three-dimensional nucleation layer on the low temperature buffer layer.

在本实施例中,三维成核层可以为GaN层。In this embodiment, the three-dimensional nucleation layer may be a GaN layer.

示例性地,将反应室温度调节至1000~1050℃,反应室压力控制在300~600torr,生长厚度为400~600nm的三维成核层,生长时间为10~20min。Exemplarily, the temperature of the reaction chamber is adjusted to 1000-1050° C., the pressure of the reaction chamber is controlled to be 300-600 torr, a three-dimensional nucleation layer with a thickness of 400-600 nm is grown, and the growth time is 10-20 min.

步骤404、在三维成核层上生长二维缓冲层。Step 404 , growing a two-dimensional buffer layer on the three-dimensional nucleation layer.

在本实施例中,二维缓冲层可以为GaN层。In this embodiment, the two-dimensional buffer layer may be a GaN layer.

示例性地,将反应室温度调节至1050~1150℃,反应室压力控制在100~300torr,生长厚度为500~800nm的二维缓冲层,生长时间为20~40min。Exemplarily, the temperature of the reaction chamber is adjusted to 1050-1150° C., the pressure of the reaction chamber is controlled to be 100-300 torr, a two-dimensional buffer layer with a thickness of 500-800 nm is grown, and the growth time is 20-40 min.

步骤405、在二维缓冲层上生长未掺杂的GaN层。Step 405 , growing an undoped GaN layer on the two-dimensional buffer layer.

示例性地,将反应室温度调节至1050~1200℃,反应室压力控制在100~300torr,生长厚度为1~2um的未掺杂的GaN层。Exemplarily, the temperature of the reaction chamber is adjusted to 1050˜1200° C., the pressure of the reaction chamber is controlled to be 100˜300 torr, and an undoped GaN layer with a thickness of 1˜2 μm is grown.

步骤406、在未掺杂的GaN层上生长N型层。Step 406 , growing an N-type layer on the undoped GaN layer.

在本实施例中,N型层可以为掺Si的GaN层,Si掺杂浓度可以为1018cm-3~1020cm-3In this embodiment, the N-type layer may be a Si-doped GaN layer, and the Si doping concentration may be 10 18 cm -3 to 10 20 cm -3 .

示例性地,将反应室温度调节至1050~1200℃,反应室压力控制在100~300torr,生长厚度为1~2um的N型层。Exemplarily, the temperature of the reaction chamber is adjusted to 1050-1200° C., the pressure of the reaction chamber is controlled to be 100-300 torr, and an N-type layer with a thickness of 1-2 um is grown.

步骤407、在N型层上生长应力释放层。Step 407 , growing a stress release layer on the N-type layer.

在本实施例中,应力释放层包括多个交替生长的第一超晶格结构和第二超晶格结构,第一超晶格结构为低温InGaN/GaN超晶格结构,第二超晶格结构为高温InGaN/GaN超晶格结构。In this embodiment, the stress release layer includes a plurality of alternately grown first superlattice structures and second superlattice structures, the first superlattice structure is a low-temperature InGaN/GaN superlattice structure, and the second superlattice structure is a low-temperature InGaN/GaN superlattice structure. The structure is a high temperature InGaN/GaN superlattice structure.

可选地,应力释放层包括N个交替生长的第一超晶格结构和第二超晶格结构,2≤N≤12。Optionally, the stress release layer includes N alternately grown first superlattice structures and second superlattice structures, 2≤N≤12.

进一步地,第一超晶格结构中的低温InGaN层和第二超晶格结构中的高温InGaN层均为InxGa1-xN层,0.05<x<0.4。Further, the low temperature InGaN layer in the first superlattice structure and the high temperature InGaN layer in the second superlattice structure are both InxGa1 - xN layers, 0.05<x<0.4.

可选地,第一超晶格结构71和第二超晶格结构72的厚度相等,以便于周期性的控制应力释放层的生长,使得V型坑的开口和V型坑的密度均匀变化。Optionally, the thicknesses of the first superlattice structure 71 and the second superlattice structure 72 are equal, so as to periodically control the growth of the stress relief layer, so that the opening of the V-shaped pits and the density of the V-shaped pits vary uniformly.

示例性地,第一超晶格结构中的低温InGaN层和第二超晶格结构中的高温InGaN层的厚度均为1~2nm。第一超晶格结构中的GaN层和第二超晶格结构中的GaN层的厚度均为10~40nm。Exemplarily, the thicknesses of the low temperature InGaN layer in the first superlattice structure and the high temperature InGaN layer in the second superlattice structure are both 1-2 nm. The thicknesses of the GaN layer in the first superlattice structure and the GaN layer in the second superlattice structure are both 10 to 40 nm.

在其它实现方式中,第一超晶格结构71和第二超晶格结构72的厚度也可以不相等。In other implementations, the thicknesses of the first superlattice structure 71 and the second superlattice structure 72 may also be unequal.

进一步地,应力释放层的厚度为100~150nm。Further, the thickness of the stress release layer is 100-150 nm.

示例性地,步骤407可以包括:Exemplarily, step 407 may include:

在780℃~880℃的温度下,生长第一超晶格结构。At a temperature of 780°C to 880°C, the first superlattice structure is grown.

在830℃~930℃的温度下,生长第二超晶格结构。At a temperature of 830°C to 930°C, the second superlattice structure is grown.

示例性地,反应室压力控制在100~500torr,生长应力释放层。Exemplarily, the pressure of the reaction chamber is controlled at 100-500 torr, and the stress release layer is grown.

步骤408、在应力释放层上生长多量子阱层。Step 408 , growing a multiple quantum well layer on the stress release layer.

其中,多量子阱层包括靠近N型层的第一类多量子阱层、靠近P型层的第三类多量子阱层、以及位于第一类多量子阱层和第三类多量子阱层之间的第二类多量子阱层。The multi-quantum well layer includes a first-type multi-quantum well layer near the N-type layer, a third-type multi-quantum well layer near the P-type layer, and the first-type multi-quantum well layer and the third-type multi-quantum well layer The second type of multiple quantum well layers in between.

第一类多量子阱层由多个周期的InaGa1-aN/AlcGa1-cN超晶格组成,第二类多量子阱层由多个周期的InaGa1-aN/GaN超晶格组成,第三类多量子阱层由多个周期的InaGa1-aN/InbGa1-bN超晶格组成,0.1<a<1,0<b<0.3,b<a,0<c<0.2。The first type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/Al c Ga 1-c N superlattice, and the second type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/GaN superlattice, the third type of multiple quantum well layer is composed of multiple periods of In a Ga 1-a N/In b Ga 1-b N superlattice, 0.1<a<1, 0<b< 0.3, b<a, 0<c<0.2.

进一步地,第一类量子阱层、第二类量子阱层和第三类量子阱层中的InaGa1-aN层的厚度均相等,从而可以保证发光波长的一致性。Further, the thicknesses of the In a Ga 1-a N layers in the first type quantum well layer, the second type quantum well layer and the third type quantum well layer are all equal, so that the uniformity of the emission wavelength can be ensured.

示例性地,第一类量子阱层中的InaGa1-aN层、第二类量子阱层中的InaGa1-aN层、第三类量子阱层中的InaGa1-aN层的厚度均为3~4nm。Exemplarily, the In a Ga 1-a N layer in the first type of quantum well layer, the In a Ga 1-a N layer in the second type of quantum well layer, and the In a Ga 1 in the third type of quantum well layer -a The thickness of the N layer is all 3 to 4 nm.

进一步地,第一类量子阱层中的AlcGa1-cN层、第二类量子阱层中的GaN层和第三类量子阱层中的InbGa1-bN层的厚度均相等。Further, the thicknesses of the AlcGa1 - cN layer in the first type quantum well layer, the GaN layer in the second type quantum well layer and the InbGa1 - bN layer in the third type quantum well layer are all uniform. equal.

可选地,第一类量子阱层中的AlcGa1-cN层、第二类量子阱层中的GaN层和第三类量子阱层中的InbGa1-bN层的厚度均为9~20nm。Optionally, the thickness of the AlcGa1 - cN layer in the first type of quantum well layer, the GaN layer in the second type of quantum well layer and the InbGa1 - bN layer in the third type of quantum well layer Both are 9 to 20 nm.

在其它实现方式中,第一类量子阱层中的AlcGa1-cN层、第二类量子阱层中的GaN层和第三类量子阱层中的InbGa1-bN层的厚度也可以不相等。In other implementations, an AlcGa1 - cN layer in the first type of quantum well layer, a GaN layer in the second type of quantum well layer, and an InbGa1 - bN layer in the third type of quantum well layer The thicknesses can also be unequal.

可选地,第一类量子阱层中的InaGa1-aN层、第二类量子阱层中的InaGa1-aN层、第三类量子阱层中的InaGa1-aN层的生长温度和生长压力均相等。Optionally, the In a Ga 1-a N layer in the first type of quantum well layer, the In a Ga 1-a N layer in the second type of quantum well layer, and the In a Ga 1 in the third type of quantum well layer -a The growth temperature and growth pressure of the N layer are both equal.

可选地,第一类量子阱层中的AlGaN层、第二类量子阱层中的GaN层和第三类量子阱层中的InbGa1-bN层的生长温度和生长压力均相等。Optionally, the growth temperature and growth pressure of the AlGaN layer in the first type quantum well layer, the GaN layer in the second type quantum well layer and the InbGa1 - bN layer in the third type quantum well layer are all equal. .

示例性地,步骤408可以包括:Illustratively, step 408 may include:

控制反应室温度为750~830℃,反应室压力为100~500torr,生长第一类量子阱层中的InaGa1-aN层、第二类量子阱层中的InaGa1-aN层、第三类量子阱层中的InaGa1-aN层;The temperature of the reaction chamber is controlled to be 750-830°C, the pressure of the reaction chamber is 100-500torr, and the In a Ga 1-a N layer in the first type of quantum well layer and the In a Ga 1 -a in the second type of quantum well layer are grown The In a Ga 1-a N layer in the N layer and the third type of quantum well layer;

控制反应室温度为850~900℃,反应室压力为100~500torr,生长第一类量子阱层中的AlcGa1-cN层、第二类量子阱层中的GaN层和第三类量子阱层中的InbGa1-bN层。The temperature of the reaction chamber is controlled to be 850-900°C, and the pressure of the reaction chamber is 100-500torr, and the AlcGa1 - cN layer in the first type of quantum well layer, the GaN layer in the second type of quantum well layer and the third type of quantum well layer are grown The InbGa1 - bN layer in the quantum well layer.

步骤409、在多量子阱层上生长电子阻挡层。Step 409 , growing an electron blocking layer on the multiple quantum well layer.

在本实施例中,电子阻挡层可以为P型AlGaN层In this embodiment, the electron blocking layer may be a P-type AlGaN layer

示例性地,将反应室温度调节至800~1000℃,反应室压力控制在50~500torr,生长厚度为20~100nm的电子阻挡层。Exemplarily, the temperature of the reaction chamber is adjusted to 800-1000° C., the pressure of the reaction chamber is controlled to be 50-500 torr, and an electron blocking layer with a thickness of 20-100 nm is grown.

步骤410、在电子阻挡层上生长P型层。Step 410, growing a P-type layer on the electron blocking layer.

在本实施例中,P型层为掺Mg的GaN层,Mg的掺杂浓度可以为1×1019~1×1020cm-3In this embodiment, the P-type layer is a Mg-doped GaN layer, and the doping concentration of Mg may be 1×10 19 to 1×10 20 cm −3 .

示例性地,将反应室温度调节至850~950℃,反应室压力控制在100~300torr,生长厚度为100~300nm的P型层。Exemplarily, the temperature of the reaction chamber is adjusted to 850-950° C., the pressure of the reaction chamber is controlled to be 100-300 torr, and a P-type layer with a thickness of 100-300 nm is grown.

步骤411、在P型层上生长P型接触层。Step 411 , growing a P-type contact layer on the P-type layer.

在本实施例中,P型接触层可以为重掺Mg的GaN层。In this embodiment, the P-type contact layer may be a heavily Mg-doped GaN layer.

示例性地,将反应室温度调节至850~1000℃,反应室压力控制在100~300torr,生长厚度为50~100nm的P型接触层。Exemplarily, the temperature of the reaction chamber is adjusted to 850-1000° C., the pressure of the reaction chamber is controlled to be 100-300 torr, and a P-type contact layer with a thickness of 50-100 nm is grown.

在上述步骤完成之后,将反应室的温度降至650~850℃,在氮气气氛进行退火处理5~15min,而后逐渐降至室温,结束发光二极管的外延生长。After the above steps are completed, the temperature of the reaction chamber is lowered to 650-850° C., annealed in a nitrogen atmosphere for 5-15 minutes, and then gradually lowered to room temperature to complete the epitaxial growth of the light-emitting diode.

本发明实施例通过将应力释放层设置为包括多个交替生长的第一超晶格结构和第二超晶格结构。其中,第一超晶格结构为低温InGaN/GaN超晶格结构,第一超晶格结构采用低温生长而成,可以保证应力释放层具有较好的应力释放效果。但是第一超晶格结构在低温生长时会引发V型坑的形成,因此,本发明通过在第一超晶格结构之后生长第二超晶格结构,第二超晶格结构为高温InGaN/GaN超晶格结构,在高温条件下,GaN的横向外延能力增强,可以抑制V型坑的开口继续变大,从而将V型坑的开口控制在合适的范围内,避免了V型坑开口过大,造成LED的内量子发光效率降低的情况出现。同时在高温条件下,形成的V型坑的密度会逐渐减少,从而可以提高外延层的晶体质量。且本发明中的应力释放层包括多个交替生长的低温InGaN/GaN超晶格结构和高温InGaN/GaN超晶格结构,与单层结构的应力释放层(即只包括一个低温InGaN/GaN超晶格结构和一个高温InGaN/GaN超晶格结构)相比,对V型坑的开口控制效果更好。In the embodiment of the present invention, the stress release layer is configured to include a plurality of alternately grown first superlattice structures and second superlattice structures. The first superlattice structure is a low-temperature InGaN/GaN superlattice structure, and the first superlattice structure is grown at a low temperature, which can ensure that the stress release layer has a good stress release effect. However, when the first superlattice structure is grown at a low temperature, the formation of V-type pits will be induced. Therefore, in the present invention, the second superlattice structure is grown after the first superlattice structure, and the second superlattice structure is high temperature InGaN/ GaN superlattice structure, under high temperature conditions, the lateral epitaxy capability of GaN is enhanced, which can restrain the opening of the V-shaped pit from continuing to increase, so as to control the opening of the V-shaped pit within a suitable range and avoid the excessive opening of the V-shaped pit. large, resulting in a decrease in the internal quantum luminous efficiency of the LED. At the same time, under high temperature conditions, the density of the formed V-shaped pits will gradually decrease, so that the crystal quality of the epitaxial layer can be improved. And the stress release layer in the present invention includes a plurality of alternately grown low-temperature InGaN/GaN superlattice structures and high-temperature InGaN/GaN superlattice structures, and the stress release layer of a single-layer structure (that is, only comprising a low-temperature InGaN/GaN superlattice structure) Compared with a high temperature InGaN/GaN superlattice structure), the opening control effect of the V-type pit is better.

以上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 are only preferred embodiments of the present invention and are not intended to limit the present invention. Any modification, equivalent replacement, improvement, etc. made within the spirit and principle of the present invention shall be included in the protection scope of the present invention. Inside.

Claims (10)

1. a kind of gallium nitride based LED epitaxial slice, the gallium nitride based LED epitaxial slice include substrate and It successively grows low temperature buffer layer over the substrate, three-dimensional nucleating layer, two-dimentional retrieving layer, undoped GaN layer, N-type layer, answer Power releasing layer, multiple quantum well layer, electronic barrier layer, P-type layer and p-type contact layer, which is characterized in that
The stress release layer includes the first superlattice structure and the second superlattice structure of multiple alternating growths, described the first to surpass Lattice structure is low temperature InGaN/GaN superlattice structure, and second superlattice structure is high temperature InGaN/GaN superlattices knot Structure.
2. gallium nitride based LED epitaxial slice according to claim 1, which is characterized in that the stress release layer With a thickness of 100~150nm.
3. gallium nitride based LED epitaxial slice according to claim 1, which is characterized in that the multiple quantum well layer packet It includes the first kind multiple quantum well layer close to the N-type layer, the third class multiple quantum well layer close to the P-type layer and is located at institute State the second class multiple quantum well layer between first kind multiple quantum well layer and the third class multiple quantum well layer;
The first kind multiple quantum well layer by multiple periods InaGa1-aN/AlcGa1-cN superlattices composition, the second class volume Sub- well layer by multiple periods InaGa1-aN/GaN superlattices composition, the third class multiple quantum well layer is by multiple periods InaGa1-aN/InbGa1-bN superlattices composition, 0.1 < a < 1,0 <b < 0.3, b < a, 0 < c < 0.2.
4. gallium nitride based LED epitaxial slice according to claim 3, which is characterized in that the first kind Quantum Well In in layer, the second class quantum well layer and the third class quantum well layeraGa1-aN layers of thickness is equal.
5. gallium nitride based LED epitaxial slice according to claim 3, which is characterized in that the first kind Quantum Well Al in layercGa1-cN layers, the GaN layer in the second class quantum well layer and the In in the third class quantum well layerbGa1-bN layers Thickness be equal.
6. a kind of manufacturing method of gallium nitride based LED epitaxial slice, which is characterized in that the manufacturing method includes:
One substrate is provided;
Successively growing low temperature buffer layer, three-dimensional nucleating layer, two-dimentional retrieving layer, undoped GaN layer, N-type layer over the substrate;
The growth stress releasing layer in the N-type layer, the stress release layer include the first superlattices knot of multiple alternating growths Structure and the second superlattice structure, first superlattice structure are low temperature InGaN/GaN superlattice structure, second superlattices Structure is high temperature InGaN/GaN superlattice structure;
Multiple quantum well layer, electronic barrier layer, P-type layer and p-type contact layer are successively grown on the stress release layer.
7. manufacturing method according to claim 6, which is characterized in that the growth stress releasing layer in the N-type layer, packet It includes:
780 DEG C~880 DEG C at a temperature of, grow first superlattice structure;
830 DEG C~930 DEG C at a temperature of, grow second superlattice structure.
8. manufacturing method according to claim 6, which is characterized in that the multiple quantum well layer includes close to the N-type layer First kind multiple quantum well layer, close to the P-type layer third class multiple quantum well layer and be located at the first kind multiple quantum wells The second class multiple quantum well layer between layer and the third class multiple quantum well layer;
The first kind multiple quantum well layer by multiple periods InaGa1-aN/AlcGa1-cN superlattices composition, the second class volume Sub- well layer by multiple periods InaGa1-aN/GaN superlattices composition, the third class multiple quantum well layer is by multiple periods InaGa1-aN/InbGa1-bN superlattices composition, 0.1 < a < 1,0 <b < 0.3, b < a, 0 < c < 0.2.
9. manufacturing method according to claim 8, which is characterized in that the first kind quantum well layer, the second class amount In in sub- well layer and the third class quantum well layeraGa1-aN layers of thickness is equal.
10. manufacturing method according to claim 8, which is characterized in that the Al in the first kind quantum well layercGa1-cN Layer, the GaN layer in the second class quantum well layer and the In in the third class quantum well layerbGa1-bN layers of thickness is equal.
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