CN107516700A - Nitride semiconductor structure and semiconductor light emitting element - Google Patents
Nitride semiconductor structure and semiconductor light emitting element Download PDFInfo
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 143
- 150000004767 nitrides Chemical class 0.000 title claims abstract description 48
- 230000004888 barrier function Effects 0.000 claims abstract description 59
- 229910002704 AlGaN Inorganic materials 0.000 claims description 20
- 230000000903 blocking effect Effects 0.000 claims description 18
- 229910052738 indium Inorganic materials 0.000 claims description 17
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 claims description 16
- 239000002019 doping agent Substances 0.000 claims description 10
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 3
- 229910052799 carbon Inorganic materials 0.000 claims description 3
- 229910021480 group 4 element Inorganic materials 0.000 claims 2
- 239000000758 substrate Substances 0.000 abstract description 16
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- 230000007547 defect Effects 0.000 abstract description 6
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- 229910002601 GaN Inorganic materials 0.000 description 24
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- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 description 21
- 230000000694 effects Effects 0.000 description 18
- 239000000126 substance Substances 0.000 description 7
- FYYHWMGAXLPEAU-UHFFFAOYSA-N Magnesium Chemical compound [Mg] FYYHWMGAXLPEAU-UHFFFAOYSA-N 0.000 description 6
- 229910052749 magnesium Inorganic materials 0.000 description 6
- 239000011777 magnesium Substances 0.000 description 6
- 230000006798 recombination Effects 0.000 description 6
- 238000005215 recombination Methods 0.000 description 6
- 238000000034 method Methods 0.000 description 5
- 229910052782 aluminium Inorganic materials 0.000 description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 4
- AJGDITRVXRPLBY-UHFFFAOYSA-N aluminum indium Chemical group [Al].[In] AJGDITRVXRPLBY-UHFFFAOYSA-N 0.000 description 4
- 229910052710 silicon Inorganic materials 0.000 description 4
- 239000010703 silicon Substances 0.000 description 4
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 2
- HCHKCACWOHOZIP-UHFFFAOYSA-N Zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 description 2
- 238000005452 bending Methods 0.000 description 2
- BASFCYQUMIYNBI-UHFFFAOYSA-N platinum Chemical compound [Pt] BASFCYQUMIYNBI-UHFFFAOYSA-N 0.000 description 2
- 230000008569 process Effects 0.000 description 2
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- 229910052725 zinc Inorganic materials 0.000 description 2
- 239000011701 zinc Substances 0.000 description 2
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
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- 229910052733 gallium Inorganic materials 0.000 description 1
- 150000002259 gallium compounds Chemical class 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 238000001459 lithography Methods 0.000 description 1
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- 229910052751 metal Inorganic materials 0.000 description 1
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- 229910003465 moissanite Inorganic materials 0.000 description 1
- 238000001451 molecular beam epitaxy Methods 0.000 description 1
- 229910052759 nickel Inorganic materials 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 125000004433 nitrogen atom Chemical group N* 0.000 description 1
- 229910017464 nitrogen compound Inorganic materials 0.000 description 1
- 150000002830 nitrogen compounds Chemical class 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
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- 229910010271 silicon carbide Inorganic materials 0.000 description 1
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- XLOMVQKBTHCTTD-UHFFFAOYSA-N zinc oxide Inorganic materials [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 description 1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/81—Bodies
- H10H20/822—Materials of the light-emitting regions
- H10H20/824—Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP
- H10H20/825—Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/81—Bodies
- H10H20/811—Bodies having quantum effect structures or superlattices, e.g. tunnel junctions
- H10H20/812—Bodies having quantum effect structures or superlattices, e.g. tunnel junctions within the light-emitting regions, e.g. having quantum confinement structures
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/81—Bodies
- H10H20/815—Bodies having stress relaxation structures, e.g. buffer layers
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Abstract
Description
本发明专利申请是申请日为2013年1月25日,申请号为201310030319.4的名为“氮化物半导体结构及半导体发光元件”的发明专利申请的分案申请。The patent application of the present invention is a divisional application of the invention patent application named "Nitride Semiconductor Structure and Semiconductor Light-Emitting Element" with the application date of January 25, 2013 and the application number 201310030319.4.
技术领域technical field
本发明有关于一种氮化物半导体结构及半导体发光元件,尤其是指一种于多重量子井结构中使用四元氮化铝铟镓的阻障层与三元氮化铟镓的井层的氮化物半导体结构及半导体发光元件,属于半导体技术领域。The present invention relates to a nitride semiconductor structure and a semiconductor light-emitting element, in particular to a nitrogen compound that uses a barrier layer of quaternary aluminum indium gallium nitride and a well layer of ternary indium gallium nitride in a multiple quantum well structure A compound semiconductor structure and a semiconductor light-emitting element belong to the technical field of semiconductors.
背景技术Background technique
一般而言,氮化物发光二极管是将一缓冲层先形成于基板上,再于缓冲层上依序磊晶成长n型半导体层、发光层以及p型半导体层;接着,利用微影与蚀刻工艺移除部分的p型半导体层、部分的发光层,直至暴露出部分的n型半导体层为止;然后,分别于n型半导体层的暴露部分以及p型半导体层上形成n型电极与p型电极,而制作出发光二极管;其中,发光层具有氮化物半导体多重量子井结构(MQW),而多重量子井结构包括以重复的方式交替设置的井层(well)和阻障层(barrier),因为井层具有相对阻障层较低之能隙,使得在上述多重量子井结构中的每一个井层可以在量子力学上限制电子和电洞,造成电子和电洞分别从n型半导体层和p型半导体层注入,并在井层中结合,而发射出光粒子。In general, a nitride light-emitting diode is first formed on a substrate with a buffer layer, and then epitaxially grows an n-type semiconductor layer, a light-emitting layer, and a p-type semiconductor layer on the buffer layer; then, using lithography and etching processes removing part of the p-type semiconductor layer and part of the light-emitting layer until a part of the n-type semiconductor layer is exposed; then, forming an n-type electrode and a p-type electrode on the exposed part of the n-type semiconductor layer and the p-type semiconductor layer respectively , and produce a light-emitting diode; wherein, the light-emitting layer has a nitride semiconductor multiple quantum well structure (MQW), and the multiple quantum well structure includes well layers (well) and barrier layers (barrier) that are alternately arranged in a repeated manner, because The well layer has a lower energy gap than the barrier layer, so that each well layer in the above-mentioned multiple quantum well structure can limit electrons and holes in quantum mechanics, causing electrons and holes to flow from the n-type semiconductor layer and p Type semiconductor layer is injected and combined in the well layer to emit light particles.
目前,在多重量子井结构中约有1至30层的井层或阻障层,阻障层通常系以氮化镓GaN的材料所形成,而井层是以氮化铟镓InGaN所组成;然而,上述的多重量子井结构由于氮化铟镓与氮化镓晶格间存在有约10-15%的晶格不匹配度,导致晶格间产生强大的应力作用,使得在多重量子井结构中有压电场(piezoelectric field)的产生,且于成长氮化铟镓的过程中,当铟含量愈高时,所产生的压电场也就愈大,对晶体结构的影响也就愈大,而随着成长的厚度愈厚时,所累积的应力也就愈大,当晶体结构成长至超过某一个临界厚度(critical thickness),导致晶体结构无法再承受此应力作用时,则会产生较大的缺陷结构(例如V-形缺陷),使得一般井层具有一定的厚度限制,一般约为3nm左右。At present, there are about 1 to 30 well layers or barrier layers in the multiple quantum well structure. The barrier layer is usually formed of gallium nitride GaN, and the well layer is composed of indium gallium nitride InGaN; However, the above-mentioned multiple quantum well structure has a lattice mismatch of about 10-15% between the InGaN and GaN lattices, resulting in strong stress between the lattices, making the multiple quantum well structure There is a piezoelectric field (piezoelectric field), and in the process of growing InGaN, the higher the indium content, the larger the piezoelectric field generated, and the greater the impact on the crystal structure , and the greater the thickness of the growth, the greater the accumulated stress. When the crystal structure grows beyond a certain critical thickness (critical thickness), the crystal structure can no longer bear the stress, and a larger Large defect structures (such as V-shaped defects) make the general well layer have a certain thickness limit, generally about 3nm.
此外,上述的多重量子井结构也会因强大的极化电场作用的存在,而造成能带严重倾斜或弯曲,导致电子与电洞分开局限在井层的两侧,使得电子与电洞波函数(wavefunction)在空间上的重叠率降低,而降低电子与电洞的辐射再结合速率(radiativerecombination rate)及内部量子效率(IQE)。In addition, the above-mentioned multiple quantum well structure will also cause serious inclination or bending of the energy band due to the existence of a strong polarization electric field, causing electrons and holes to be separated and confined on both sides of the well layer, making the wave functions of electrons and holes (wavefunction) The overlap rate in space is reduced, and the radiation recombination rate (radiative recombination rate) and internal quantum efficiency (IQE) of electrons and holes are reduced.
鉴于上述现有的氮化物半导体发光元件在实际实施上仍具有多处的缺失,因此,研发出一种新型的氮化物半导体结构及半导体发光元件仍是本领域亟待解决的问题之一。In view of the fact that the existing nitride semiconductor light-emitting elements still have many deficiencies in actual implementation, it is still one of the problems to be solved urgently in this field to develop a novel nitride semiconductor structure and semiconductor light-emitting element.
发明内容Contents of the invention
为解决上述技术问题,本发明主要目的为提供一种氮化物半导体结构,其于发光层中使用四元氮化铝铟镓的阻障层与三元氮化铟镓的井层以改善因晶格失配所产生的应力作用,使得井层具有3.5nm-7nm的厚度,同时可提供较佳的载子局限,以提升内部量子效率。In order to solve the above technical problems, the main purpose of the present invention is to provide a nitride semiconductor structure, which uses a barrier layer of quaternary aluminum indium gallium nitride and a well layer of ternary indium gallium nitride in the light emitting layer to improve the crystallinity The stress effect caused by the lattice mismatch makes the well layer have a thickness of 3.5nm-7nm, and at the same time, it can provide better carrier confinement to improve the internal quantum efficiency.
本发明的另一目的为提供一种半导体发光元件,其至少包含有上述的氮化物半导体结构,使得半导体发光元件获得良好的发光效率。Another object of the present invention is to provide a semiconductor light-emitting element, which at least includes the above-mentioned nitride semiconductor structure, so that the semiconductor light-emitting element can obtain good luminous efficiency.
为达上述目的,本发明提供一种氮化物半导体结构,其主要于基板上配置有一第一型掺杂半导体层与一第二型掺杂半导体层,于所述第一型掺杂半导体层与所述第二型掺杂半导体层间配置有一发光层,所述发光层具有多重量子井结构,且所述多重量子井结构包含多个彼此交替堆栈的井层及阻障层,且每两层所述阻障层间具有一所述井层,所述阻障层为AlxInyGa1-x-yN,其中x及y满足0<x<1,0<y<1,0<x+y<1的数值,而所述井层为InzGa1-zN,其中0<z<1。In order to achieve the above object, the present invention provides a nitride semiconductor structure, which is mainly configured with a first-type doped semiconductor layer and a second-type doped semiconductor layer on the substrate, between the first-type doped semiconductor layer and the second-type doped semiconductor layer. A light-emitting layer is disposed between the second-type doped semiconductor layers, the light-emitting layer has a multiple quantum well structure, and the multiple quantum well structure includes a plurality of well layers and barrier layers stacked alternately with each other, and every two layers There is a well layer between the barrier layers, the barrier layer is Al x In y Ga 1-xy N, where x and y satisfy 0<x<1, 0<y<1, 0<x+ y<1, and the well layer is In z Ga 1-z N, where 0<z<1.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述井层具有3.5nm-7nm的厚度。According to a specific embodiment of the present invention, preferably, in the above nitride semiconductor structure, the well layer has a thickness of 3.5nm-7nm.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述阻障层具有5nm-12nm的厚度;且优选地,在上述氮化物半导体结构中,所述阻障层可掺杂有浓度为1016-1018cm-3的第一型掺质;使得阻障层可以减少载子遮蔽效应,以增加载子局限效应。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, the barrier layer has a thickness of 5nm-12nm; and preferably, in the above-mentioned nitride semiconductor structure, the barrier layer can be doped Doped with the first-type dopant with a concentration of 10 16 -10 18 cm -3 ; the barrier layer can reduce the carrier shielding effect and increase the carrier confinement effect.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,可于所述发光层与所述第二型掺杂半导体层间可配置有一电洞提供层;更优选地,所述电洞提供层为氮化铟镓InxGa1-xN,其中0<x<1,且所述电洞提供层可掺杂有浓度大于1018cm-3的第二型掺质,例如为镁或锌,优选为镁,以增加电洞的浓度。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, a hole-providing layer can be arranged between the light-emitting layer and the second-type doped semiconductor layer; more preferably, the The hole-providing layer is indium gallium nitride In x Ga 1-x N, where 0<x<1, and the hole-providing layer can be doped with a second-type dopant with a concentration greater than 10 18 cm -3 , for example Magnesium or zinc, preferably magnesium, to increase the concentration of holes.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述电洞提供层可掺杂有浓度为1017-1020cm-3的第四主族元素,由此提供更多的电洞进入发光层,进而增加电子电洞的结合。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, the hole providing layer may be doped with a fourth main group element at a concentration of 10 17 -10 20 cm -3 , thereby providing a more More holes enter the light-emitting layer, thereby increasing the combination of electrons and holes.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述电洞提供层的能隙大于多重量子井结构的井层的能隙,通过让电洞容易进入井层又防止电子逃脱,使得电子及电洞更容易局限在井层中,以增加电子电洞对覆合的机率。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, the energy gap of the hole providing layer is larger than the energy gap of the well layer of the multiple quantum well structure, by allowing the holes to easily enter the well layer and preventing The escape of electrons makes it easier for electrons and holes to be confined in the well layer, so as to increase the probability of recombination of electron-hole pairs.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,可于所述发光层与所述第一型掺杂半导体层间配置有一第一型载子阻隔层,且所述第一型载子阻隔层优选为AlxGa1-xN,其中0<x<1。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, a first-type carrier blocking layer may be disposed between the light-emitting layer and the first-type doped semiconductor layer, and the second The type-one carrier blocking layer is preferably AlxGa1 - xN , where 0<x<1.
根据本发明的具体实施方式,优选地,在上述氮化物半导体结构中,所述电洞提供层与所述第二型掺杂半导体层间配置有一第二型载子阻隔层,且所述第二型载子阻隔层优选为AlxGa1-xN,其中0<x<1。由此,利用含有铝的AlGaN的能带隙较GaN要高的特性,不仅可增加氮化物半导体的能带范围,亦使得载子可局限于多重量子井结构中,提高电子电洞覆合的机率,进而达到发光效率提升的功效。According to a specific embodiment of the present invention, preferably, in the above-mentioned nitride semiconductor structure, a second-type carrier blocking layer is arranged between the hole providing layer and the second-type doped semiconductor layer, and the first The second-type carrier blocking layer is preferably AlxGa1 - xN , where 0<x<1. Therefore, using the characteristic that the energy bandgap of AlGaN containing aluminum is higher than that of GaN can not only increase the energy band range of the nitride semiconductor, but also make the carrier can be confined in the multiple quantum well structure, and improve the electron-hole recombination. chance, and then achieve the effect of improving luminous efficiency.
本发明还提供一种半导体发光元件,其至少包含有:The present invention also provides a semiconductor light emitting element, which at least includes:
一基板;a substrate;
一第一型掺杂半导体层,其配置于所述基板上;a first-type doped semiconductor layer disposed on the substrate;
一发光层,其配置于所述第一型掺杂半导体层上,所述发光层具有多重量子井结构,所述多重量子井结构包含多个彼此交替堆栈的井层及阻障层,且每两层所述阻障层间具有一所述井层,所述阻障层为AlxInyGa1-x-yN,其中x及y满足0<x<1,0<y<1,0<x+y<1的数值,所述井层为InzGa1-zN,其中0<z<1;A light-emitting layer, which is configured on the first-type doped semiconductor layer, the light-emitting layer has a multiple quantum well structure, and the multiple quantum well structure includes a plurality of well layers and barrier layers stacked alternately, and each There is a well layer between the two barrier layers, the barrier layer is Al x In y Ga 1-xy N, wherein x and y satisfy 0<x<1, 0<y<1, 0< The value of x+y<1, the well layer is In z Ga 1-z N, where 0<z<1;
一第二型掺杂半导体层,其配置于所述发光层上;a second-type doped semiconductor layer disposed on the light-emitting layer;
一第一型电极,其以欧姆接触配置于所述第一型掺杂半导体层上;以及a first-type electrode disposed on the first-type doped semiconductor layer in ohmic contact; and
一第二型电极,其以欧姆接触配置于所述第二型掺杂半导体层上。A second-type electrode is configured on the second-type doped semiconductor layer in ohmic contact.
本发明的半导体发光元件至少包含如上述的氮化物半导体结构,以及二相配合地提供电能的第一型电极与第二型电极;由此,利用四元氮化铝铟镓的阻障层以及三元氮化铟镓的井层具有相同铟元素的特性,可调整四元组成条件以提供晶格匹配的组成,使得阻障层与井层的晶格常数较为相近,不仅可改善传统氮化铟镓的井层以及氮化镓的阻障层因晶格不匹配而产生的晶体缺陷现象,亦可改善因晶格失配所产生的应力作用,使得本发明的氮化物半导体结构的井层具有3.5nm-7nm的厚度,优选为4nm-5nm;同时,通过提高添加Al元素可提供阻障层较佳的载子局限,有效地将电子电洞局限于井层内,由此提升内部量子效率,使得半导体发光元件获得良好的发光效率。The semiconductor light-emitting element of the present invention at least includes the above-mentioned nitride semiconductor structure, and two first-type electrodes and second-type electrodes that cooperate to provide electric energy; thus, using the barrier layer of quaternary aluminum indium gallium nitride and The well layer of ternary InGaN has the characteristics of the same indium element, and the quaternary composition conditions can be adjusted to provide a lattice-matched composition, so that the lattice constants of the barrier layer and the well layer are relatively similar, which can not only improve the traditional nitride The crystal defects in the well layer of indium gallium and the barrier layer of gallium nitride due to lattice mismatch can also improve the stress effect caused by lattice mismatch, so that the well layer of the nitride semiconductor structure of the present invention It has a thickness of 3.5nm-7nm, preferably 4nm-5nm; at the same time, by increasing the addition of Al elements, it can provide better carrier confinement in the barrier layer, effectively confining electron holes in the well layer, thereby improving the internal quantum Efficiency, so that the semiconductor light-emitting element obtains good luminous efficiency.
再者,因四元氮化铝铟镓的阻障层以及三元氮化铟镓的井层可改善因晶格失配所产生的应力作用,进而有效降低多重量子井结构中压电场的产生,达到有效抑制压电效应及提升内部量子效率的功效,使得半导体发光元件可获得更佳的发光效率。Furthermore, the barrier layer of quaternary AlInGaN and the well layer of ternary InGaN can improve the stress effect caused by lattice mismatch, thereby effectively reducing the pressure of the piezoelectric field in the multiple quantum well structure. Produced to effectively suppress the piezoelectric effect and improve the internal quantum efficiency, so that the semiconductor light-emitting element can obtain better luminous efficiency.
附图说明Description of drawings
图1为本发明的一优选实施例提供的氮化物半导体结构的剖面示意图。FIG. 1 is a schematic cross-sectional view of a nitride semiconductor structure provided by a preferred embodiment of the present invention.
图2为根据本发明的优选实施例提供的氮化物半导体结构所制作的半导体发光元件的剖面示意图。Fig. 2 is a schematic cross-sectional view of a semiconductor light-emitting element made of a nitride semiconductor structure according to a preferred embodiment of the present invention.
主要组件符号说明:Description of main component symbols:
1 基板 2 缓冲层1 Substrate 2 Buffer layer
3 第一型掺杂半导体层 31 第一型电极3 first type doped semiconductor layer 31 first type electrode
4 第一型载子阻隔层4 Type I carrier blocking layer
5 发光层5 luminous layer
51 井层 52 阻障层51 well layer 52 barrier layer
6 第二型载子阻隔层6 Type II carrier blocking layer
7 第二型掺杂半导体层 71 第二型电极7 Second-type doped semiconductor layer 71 Second-type electrode
8 电洞提供层8 hole supply layer
具体实施方式detailed description
本发明的目的及其结构设计功能上的优点,将依据以下附图及优选实施例予以说明,以对本发明有更深入且具体的了解。The purpose of the present invention and its structural design and functional advantages will be described according to the following drawings and preferred embodiments, so as to have a more in-depth and specific understanding of the present invention.
首先,在以下实施例的描述中,应当理解,当指出一层(或膜)或一结构配置在另一个基板、另一层(或膜)、或另一结构“上”或“下”时,其可“直接”位于其它基板、层(或膜)、或另一结构,亦或者两者间具有一个以上的中间层以“间接”方式配置,可参照附图说明每一层所在位置。First of all, in the description of the following embodiments, it should be understood that when it is indicated that a layer (or film) or a structure is disposed "on" or "under" another substrate, another layer (or film), or another structure , which can be "directly" located on other substrates, layers (or films), or another structure, or have more than one intermediate layer between them in an "indirect" manner. The location of each layer can be described with reference to the drawings.
请参阅图1所示,其为本发明的一优选实施例提供的氮化物半导体结构的剖面示意图,其主要于基板1上配置有一第一型掺杂半导体层3与一第二型掺杂半导体层7,于第一型掺杂半导体层3与第二型掺杂半导体层7间配置有一发光层5,发光层5具有多重量子井结构,且多重量子井结构包含多个彼此交替堆栈的井层51及阻障层52,且每两阻障层52间具有一井层51,阻障层52由化学式AlxInyGa1-x-yN表示的四元材料所构成,其中x及y满足0<x<1,0<y<1,0<x+y<1的数值,而井层51由化学式InzGa1-zN表示的材料所构成,其中0<z<1,且井层51具有3.5nm-7nm的厚度,优选为4nm-5nm,而阻障层52具有5nm-12nm的厚度;其中阻障层52可掺杂有浓度为1016-1018cm-3的第一型掺质(例如为硅或锗),使得阻障层52可以减少载子遮蔽效应,以增加载子局限效应。Please refer to FIG. 1, which is a schematic cross-sectional view of a nitride semiconductor structure provided by a preferred embodiment of the present invention, which is mainly configured with a first-type doped semiconductor layer 3 and a second-type doped semiconductor layer on a substrate 1. Layer 7, a light-emitting layer 5 is disposed between the first-type doped semiconductor layer 3 and the second-type doped semiconductor layer 7, the light-emitting layer 5 has a multiple quantum well structure, and the multiple quantum well structure includes a plurality of alternately stacked wells Layer 51 and barrier layer 52, and there is a well layer 51 between every two barrier layers 52, the barrier layer 52 is made of a quaternary material represented by the chemical formula Al x In y Ga 1-xy N, wherein x and y satisfy 0<x<1, 0<y<1, 0<x+y<1, and the well layer 51 is made of the material represented by the chemical formula In z Ga 1-z N, where 0<z<1, and the well Layer 51 has a thickness of 3.5nm-7nm, preferably 4nm-5nm, and barrier layer 52 has a thickness of 5nm-12nm; wherein barrier layer 52 can be doped with a concentration of 10 16 -10 18 cm -3 of the first Type dopant (such as silicon or germanium), so that the barrier layer 52 can reduce the carrier shielding effect, so as to increase the carrier confinement effect.
此外,上述的氮化物半导体结构可于发光层5与第二型掺杂半导体层7间配置有一电洞提供层8,其中电洞提供层8为氮化铟镓InxGa1-xN,其中0<x<1,且电洞提供层8掺杂有浓度大于1018cm-3的第二型掺质,例如为镁或锌,优选为镁;再者,电洞提供层8可掺杂有浓度为1017-1020cm-3的第四主族元素,优选为碳,利用碳(4A族)取代五价的氮原子,使得电洞提供层8可具有高电洞浓度,由此提供更多的电洞进入发光层5,进而增加电子电洞的结合;再者,电洞提供层8的能隙大于多重量子井结构的井层51的能隙,由此可让电洞进入井层且又避免电子逃逸进入第二型掺杂半导体层7内。In addition, the above-mentioned nitride semiconductor structure can be provided with a hole-providing layer 8 between the light-emitting layer 5 and the second-type doped semiconductor layer 7, wherein the hole-providing layer 8 is indium gallium nitride In x Ga 1-x N, Where 0<x<1, and the hole-providing layer 8 is doped with a second-type dopant with a concentration greater than 10 18 cm -3 , such as magnesium or zinc, preferably magnesium; moreover, the hole-providing layer 8 can be doped with Doped with the fourth main group element with a concentration of 10 17 -10 20 cm -3 , preferably carbon, using carbon (group 4A) to replace the pentavalent nitrogen atom, so that the hole providing layer 8 can have a high hole concentration, by This provides more holes to enter the light-emitting layer 5, thereby increasing the combination of electron holes; moreover, the energy gap of the hole providing layer 8 is greater than the energy gap of the well layer 51 of the multiple quantum well structure, thus allowing the holes enter the well layer and prevent electrons from escaping into the second-type doped semiconductor layer 7 .
另外,发光层5与第一型掺杂半导体层3间亦可配置有一第一型载子阻隔层4,且第一型载子阻隔层4优选是由化学式AlxGa1-xN表示的材料所构成,其中0<x<1;而电洞提供层8与第二型掺杂半导体层7间配置有一第二型载子阻隔层6,且第二型载子阻隔层6由化学式AlxGa1-xN表示的材料所构成,其中0<x<1;由此,利用含有铝的AlGaN的能带隙较GaN要高的特性,不仅可增加氮化物半导体的能带范围,亦使得载子可局限于多重量子井结构中,提高电子电洞覆合的机率,进而达到增加发光效率的功效。In addition, a first-type carrier blocking layer 4 may also be disposed between the light-emitting layer 5 and the first-type doped semiconductor layer 3, and the first-type carrier blocking layer 4 is preferably represented by the chemical formula AlxGa1 - xN material, wherein 0<x<1; and a second-type carrier blocking layer 6 is arranged between the hole providing layer 8 and the second-type doped semiconductor layer 7, and the second-type carrier blocking layer 6 is composed of the chemical formula Al x Ga 1-x N, where 0<x<1; thus, using AlGaN containing aluminum, which has a higher energy band gap than GaN, can not only increase the energy band range of nitride semiconductors, but also The carrier can be confined in the multiple quantum well structure, and the probability of electron-hole recombination is increased, thereby achieving the effect of increasing luminous efficiency.
再者,基板1与第一型掺杂半导体层3间可配置有一缓冲层2,缓冲层2是由化学式AlXGa1-xN表示的材料所构成,其中0<x<1;而缓冲层2是用以改善第一型掺杂半导体层3成长于异质基板1上所产生的晶格常数不匹配(lattice mismatch)的问题,且缓冲层2的材料亦可例如是GaN、InGaN、SiC、ZnO等,且其形成方法可例如是于400-900℃的温度下进行低温磊晶成长。Furthermore, a buffer layer 2 may be arranged between the substrate 1 and the first-type doped semiconductor layer 3, and the buffer layer 2 is made of a material represented by the chemical formula Al X Ga 1-x N, wherein 0<x<1; Layer 2 is used to improve the problem of lattice mismatch (lattice mismatch) caused by the growth of the first-type doped semiconductor layer 3 on the heterogeneous substrate 1, and the material of the buffer layer 2 can also be, for example, GaN, InGaN, SiC, ZnO, etc., and the formation method can be, for example, low-temperature epitaxial growth at a temperature of 400-900°C.
上述实施例的氮化物半导体结构于实际实施使用时,首先基板1的材料可例如是蓝宝石(sapphire)、硅、SiC、ZnO或GaN基板等,而第一型掺杂半导体层3的材料可例如为硅或锗掺杂的氮化镓系列材料,第二型掺杂半导体层7的材料则可例如为镁或锌掺杂的氮化镓系列材料,其中第一型掺杂半导体层3、第二型掺杂半导体层7形成的方法可例如是进行有机金属化学气相沉积法(metalorganic chemical vapor deposition;MOCVD);而值得注意的,上述井层51与阻障层52优选的制作方法是利用有机金属蒸汽沉积法或分子束磊晶法(MBE)加以沉积,一般是使用含低烷基铟和镓化合物的气体混合物;所述阻障层52是于850-1000℃的温度沉积而形成,而所述井层51通常是在500-950℃的温度下形成;由此,由于多重量子井结构包含有氮化铝铟镓的阻障层52以及氮化铟镓的井层51,其具有相同的铟元素,使得阻障层52与井层51的晶格常数较为相近,可改善传统氮化镓的阻障层以及氮化铟镓的井层所造成的晶格不匹配而产生的晶体缺陷现象,且由于晶格间应力的产生主要是来由于材料间晶格常数的不匹配所造成的,由此亦可改善因晶格失配所产生应力作用,使得本发明的氮化物半导体结构的井层51具有3.5nm-7nm的厚度,优选为4nm-5nm。When the nitride semiconductor structure of the above-mentioned embodiment is actually implemented and used, first, the material of the substrate 1 can be, for example, sapphire (sapphire), silicon, SiC, ZnO or GaN substrate, etc., and the material of the first-type doped semiconductor layer 3 can be, for example, It is silicon or germanium-doped gallium nitride series material, and the material of the second-type doped semiconductor layer 7 can be, for example, magnesium or zinc-doped gallium nitride series material, wherein the first-type doped semiconductor layer 3, the second-type doped semiconductor layer 7 The method for forming the second-type doped semiconductor layer 7 can be, for example, metalorganic chemical vapor deposition (MOCVD); and it should be noted that the above-mentioned well layer 51 and barrier layer 52 are preferably prepared by using organic Deposited by metal vapor deposition or molecular beam epitaxy (MBE), generally using a gas mixture containing low alkyl indium and gallium compounds; the barrier layer 52 is formed by depositing at a temperature of 850-1000° C., and The well layer 51 is usually formed at a temperature of 500-950° C.; thus, since the multiple quantum well structure includes the barrier layer 52 of AlInGaN and the well layer 51 of InGaN, it has the same The indium element makes the lattice constants of the barrier layer 52 and the well layer 51 relatively similar, which can improve the crystal defects caused by the lattice mismatch caused by the barrier layer of traditional gallium nitride and the well layer of indium gallium nitride. Phenomenon, and since the inter-lattice stress is mainly caused by the mismatch of lattice constants between materials, it can also improve the stress effect caused by lattice mismatch, making the nitride semiconductor structure of the present invention The well layer 51 has a thickness of 3.5nm-7nm, preferably 4nm-5nm.
再者,因四元氮化铝铟镓的阻障层52以及氮化铟镓的井层51可改善因晶格失配所产生应力作用,进而有效降低多重量子井结构中压电场的产生,使得能带弯曲与倾斜的现象得到相当程度的改善,进而达到有效抑制压电效应及提升内部量子效率的功效。Furthermore, the barrier layer 52 of quaternary AlInGaN and the well layer 51 of InGaN can improve the stress effect caused by lattice mismatch, thereby effectively reducing the generation of piezoelectric field in the multiple quantum well structure , so that the phenomenon of energy band bending and inclination is improved to a considerable extent, and then achieves the effect of effectively suppressing the piezoelectric effect and improving the internal quantum efficiency.
请参阅图2所示,上述的氮化物半导体结构可应用于半导体发光元件中,图2为根据本发明的优选实施例提供的氮化物半导体结构所制作的半导体发光元件的剖面示意图,所述半导体发光元件至少包含有:Please refer to FIG. 2, the above-mentioned nitride semiconductor structure can be applied to semiconductor light-emitting elements. FIG. 2 is a schematic cross-sectional view of a semiconductor light-emitting element made of a nitride semiconductor structure according to a preferred embodiment of the present invention. Light emitting elements include at least:
一基板1;a substrate 1;
一第一型掺杂半导体层3,其配置于基板1上;其中,第一型掺杂半导体层3的材料可例如为硅或锗掺杂的氮化镓系列材料;A first-type doped semiconductor layer 3, which is disposed on the substrate 1; wherein, the material of the first-type doped semiconductor layer 3 can be, for example, silicon or germanium-doped gallium nitride series materials;
一发光层5,其配置于第一型掺杂半导体层3上,发光层5具有多重量子井结构,而多重量子井结构包含多个彼此交替堆栈的井层51及阻障层52,且每两阻障层52间具有一井层51,阻障层52由化学式AlxInyGa1-x-yN表示的材料所构成,其中,x及y满足0<x<1,0<y<1,0<x+y<1的数值,而井层51由化学式InzGa1-zN表示的材料所构成,其中0<z<1,且井层51具有3.5nm-7nm的厚度,优选为4nm-5nm;A light-emitting layer 5, which is disposed on the first-type doped semiconductor layer 3, the light-emitting layer 5 has a multiple quantum well structure, and the multiple quantum well structure includes a plurality of well layers 51 and barrier layers 52 stacked alternately, and each There is a well layer 51 between the two barrier layers 52, and the barrier layer 52 is composed of a material represented by the chemical formula Al x In y Ga 1-xy N, wherein x and y satisfy 0<x<1, 0<y<1 , the value of 0<x+y<1, and the well layer 51 is made of a material represented by the chemical formula In z Ga 1-z N, wherein 0<z<1, and the well layer 51 has a thickness of 3.5nm-7nm, preferably 4nm-5nm;
一第二型掺杂半导体层7,其配置于发光层5上,第二型掺杂半导体层7的材料可例如为镁或锌掺杂的氮化镓系列材料;A second-type doped semiconductor layer 7, which is disposed on the light-emitting layer 5, and the material of the second-type doped semiconductor layer 7 can be, for example, magnesium or zinc-doped gallium nitride series materials;
一第一型电极31,其以欧姆接触配置于第一型掺杂半导体层3上;以及a first-type electrode 31, which is configured on the first-type doped semiconductor layer 3 in an ohmic contact; and
一第二型电极71,其以欧姆接触配置于第二型掺杂半导体层7上;其中,第一型电极31与第二型电极71相配合地提供电能,且可以下列材料、但不仅限于这些材料所制成:钛、铝、金、铬、镍、铂及其合金等;其制作方法为本领域技术人员所公知的,且并非本发明的重点,因此,不再本发明中加以赘述。A second-type electrode 71, which is arranged on the second-type doped semiconductor layer 7 in ohmic contact; wherein, the first-type electrode 31 and the second-type electrode 71 cooperate to provide electric energy, and the following materials can be used, but not limited to Made of these materials: titanium, aluminum, gold, chromium, nickel, platinum and alloys thereof, etc.; its production method is well known to those skilled in the art, and is not the focus of the present invention, therefore, it is not repeated in the present invention .
此外,发光层5与第一型掺杂半导体层3间可配置一由AlxGa1-xN材料所构成的第一型载子阻隔层4,其中0<x<1;而发光层5与第二型掺杂半导体层7间亦可配置一由AlxGa1-xN材料所构成的第二型载子阻隔层6,其中0<x<1;由此,利用含有铝的AlGaN的能带隙较GaN要高的特性,不仅可增加氮化物半导体的能带范围,亦使得载子可局限于多重量子井结构中,提高电子电洞覆合的机率,进而达到增加发光效率的功效。In addition, a first-type carrier blocking layer 4 made of AlxGa1 - xN material can be disposed between the light-emitting layer 5 and the first-type doped semiconductor layer 3, where 0<x<1; and the light-emitting layer 5 A second-type carrier blocking layer 6 made of AlxGa1 - xN material can also be arranged between the second-type doped semiconductor layer 7, where 0<x<1; thus, using AlGaN containing aluminum The energy band gap of GaN is higher than that of GaN, which not only increases the energy band range of nitride semiconductors, but also allows carriers to be confined in the multiple quantum well structure, increasing the probability of electron-hole recombination, thereby achieving the goal of increasing luminous efficiency. effect.
再者,基板1与第一型掺杂半导体层3间可配置一由AlXGa1-xN所构成的缓冲层2,其中0<x<1,以改善第一型掺杂半导体层3成长于异质基板1上所产生的晶格常数不匹配的问题,且缓冲层2的材料亦可例如是GaN、InGaN、SiC、ZnO等。Furthermore, a buffer layer 2 made of AlxGa1 -xN can be disposed between the substrate 1 and the first-type doped semiconductor layer 3, where 0< x <1, to improve the performance of the first-type doped semiconductor layer 3. The problem of lattice constant mismatch caused by growth on the heterogeneous substrate 1, and the material of the buffer layer 2 can also be GaN, InGaN, SiC, ZnO, etc., for example.
由此,由上述的氮化物半导体结构实施说明可知,本发明的半导体发光元件通过四元氮化铝铟镓的阻障层52以及三元氮化铟镓的井层51具有相同铟元素的特性,利用调整四元组成条件以提供晶格匹配的组成,使得阻障层52与井层51的晶格常数较为相近,不仅可改善传统氮化镓的阻障层以及氮化铟镓的井层所造成的晶格不匹配而产生的晶体缺陷现象,且由于晶格间应力的产生主要是由于材料间晶格常数的不匹配所造成的,由此亦可改善因晶格失配所产生应力作用,使得本发明的氮化物半导体结构的井层51具有3.5nm-7nm的厚度,优选为4nm-5nm;同时,亦可提高添加Al元素以提供阻障层52较佳的载子局限,有效地将电子电洞局限于井层51内,由此提升内部量子效率,使得半导体发光元件获得良好的发光效率。Thus, it can be known from the description of the above nitride semiconductor structure implementation that the semiconductor light-emitting element of the present invention has the characteristics of the same indium element through the barrier layer 52 of the quaternary aluminum indium gallium nitride and the well layer 51 of the ternary indium gallium nitride. , by adjusting the quaternary composition conditions to provide a lattice-matched composition, the lattice constants of the barrier layer 52 and the well layer 51 are relatively similar, which can not only improve the barrier layer of traditional gallium nitride and the well layer of indium gallium nitride The crystal defect phenomenon caused by lattice mismatch, and because the stress between lattices is mainly caused by the mismatch of lattice constants between materials, it can also improve the stress caused by lattice mismatch function, so that the well layer 51 of the nitride semiconductor structure of the present invention has a thickness of 3.5nm-7nm, preferably 4nm-5nm; at the same time, it can also increase the addition of Al elements to provide better carrier confinement of the barrier layer 52, effectively The electron holes are effectively confined in the well layer 51, thereby improving the internal quantum efficiency, so that the semiconductor light-emitting element can obtain good luminous efficiency.
再者,因四元氮化铝铟镓的阻障层52以及三元氮化铟镓的井层51可改善因晶格失配所产生应力作用,进而有效降低多重量子井结构中压电场的产生,达到有效抑制压电效应及提升内部量子效率的功效,使得半导体发光元件可获得更佳的发光效率。Furthermore, the barrier layer 52 of the quaternary AlInGaN and the well layer 51 of the ternary InGaN can improve the stress effect caused by lattice mismatch, thereby effectively reducing the piezoelectric field in the multiple quantum well structure The generation of it can effectively suppress the piezoelectric effect and improve the internal quantum efficiency, so that the semiconductor light-emitting element can obtain better luminous efficiency.
综上所述,本发明的氮化物半导体结构及半导体发光元件,的确能通过上述所揭露的实施例,达到所预期的使用功效。To sum up, the nitride semiconductor structure and the semiconductor light-emitting device of the present invention can indeed achieve the expected use effects through the above-disclosed embodiments.
上述所揭露的附图及说明,仅为本发明的优选实施例,并非为限定本发明的保护范围;本领域一般技术人员,依据本发明的特征,所做的其它等效变化或修饰,皆应视为不脱离本发明的保护范围。The drawings and descriptions disclosed above are only preferred embodiments of the present invention, and are not intended to limit the protection scope of the present invention; other equivalent changes or modifications made by those skilled in the art based on the features of the present invention are all It should be regarded as not departing from the protection scope of the present invention.
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