CN113394319B - Deep ultraviolet light-emitting element and preparation method thereof - Google Patents
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Abstract
Description
技术领域technical field
本发明涉及半导体芯片技术领域,特别涉及一种深紫外发光元件及其制备方法。The invention relates to the technical field of semiconductor chips, in particular to a deep ultraviolet light-emitting element and a preparation method thereof.
背景技术Background technique
深紫外发光元件,其波长范围为200nm~300nm,发出的深紫外光可打断病毒和细菌的DNA或RNA,直接杀死病毒和细菌,可广泛应用于空气净化、自来水杀菌、家用空调杀菌、汽车空调杀菌等杀菌消毒领域。The deep ultraviolet light-emitting element has a wavelength range of 200nm to 300nm. The deep ultraviolet light emitted can interrupt the DNA or RNA of viruses and bacteria, and directly kill viruses and bacteria. It can be widely used in air purification, tap water sterilization, household air conditioning sterilization, Auto air conditioner sterilization and other sterilization fields.
深紫外发光元件的p型半导体层使用高Al组分的AlGaN,随着Al组分上升,Mg的掺杂和离化效率降低,从而导致深紫外发光元件的空穴浓度普遍低于1E17cm-2,而n型半导体层使用Si掺杂,Si的掺杂和离化效率较高,电子浓度普遍高于5E18cm-2。由于p型半导体层和n型半导体层的空穴和电子浓度差异较大,导致注入量子阱层的电子浓度远高于空穴浓度,进而导致电子空穴波函数在量子阱层的空间上分布极不一致,电子空穴复合效率低。在大电流注入情况下,多余的电子会溢出量子阱层,泄漏至p型半导体层,进而与空穴产生非辐射复合,进一步引起发光效率急剧下降。因此,电子和空穴在深紫外发光元件中浓度差异大、分布不均匀是导致其发光效率普遍低于5%的重要原因。The p-type semiconductor layer of the deep ultraviolet light emitting element uses AlGaN with high Al composition. As the Al composition increases, the doping and ionization efficiency of Mg decreases, resulting in the hole concentration of the deep ultraviolet light emitting element generally lower than 1E17cm -2 , while the n-type semiconductor layer is doped with Si, the doping and ionization efficiency of Si are high, and the electron concentration is generally higher than 5E18cm -2 . Due to the large difference in the concentration of holes and electrons between the p-type semiconductor layer and the n-type semiconductor layer, the concentration of electrons injected into the quantum well layer is much higher than the hole concentration, which in turn leads to the spatial distribution of the electron-hole wave function in the quantum well layer. Very inconsistent, the electron-hole recombination efficiency is low. In the case of large current injection, the excess electrons will overflow the quantum well layer and leak to the p-type semiconductor layer, and then generate non-radiative recombination with holes, further causing a sharp drop in luminous efficiency. Therefore, the large concentration difference and uneven distribution of electrons and holes in deep ultraviolet light-emitting elements are the important reasons for their luminous efficiency generally lower than 5%.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供一种深紫外发光元件及其制备方法,以解决电子和空穴在深紫外发光元件中浓度差异大和分布不均匀问题。The purpose of the present invention is to provide a deep ultraviolet light emitting element and a preparation method thereof, so as to solve the problems of large concentration difference and uneven distribution of electrons and holes in the deep ultraviolet light emitting element.
为了实现上述目的以及其他相关目的,本发明提供了一种深紫外发光元件,包括:衬底和位于所述衬底上的外延层,所述外延层从下至上依次包括:第一n型半导体层、阻拦层、量子阱层以及P型半导体层,其中,所述阻拦层包括至少两层空穴阻拦层以及每两层相邻的空穴阻拦层之间的第二n型半导体层。In order to achieve the above object and other related objects, the present invention provides a deep ultraviolet light-emitting element, comprising: a substrate and an epitaxial layer on the substrate, the epitaxial layer sequentially including from bottom to top: a first n-type semiconductor layer, blocking layer, quantum well layer and p-type semiconductor layer, wherein the blocking layer includes at least two hole blocking layers and a second n-type semiconductor layer between every two adjacent hole blocking layers.
可选的,在所述的深紫外发光元件中,所述阻拦层为三明治结构层,其包括层叠的第一空穴阻拦层、第二n型半导体层以及第二空穴阻拦层。Optionally, in the deep ultraviolet light emitting element, the blocking layer is a sandwich structure layer, which includes a stacked first hole blocking layer, a second n-type semiconductor layer and a second hole blocking layer.
可选的,在所述的深紫外发光元件中,所述第一空穴阻拦层的厚度为 Optionally, in the deep ultraviolet light-emitting element, the thickness of the first hole blocking layer is
可选的,在所述的深紫外发光元件中,所述第二空穴阻拦层的厚度为 Optionally, in the deep ultraviolet light-emitting element, the thickness of the second hole blocking layer is
可选的,在所述的深紫外发光元件中,所述第二n型半导体层的厚度为50nm~200nm。Optionally, in the deep ultraviolet light-emitting element, the thickness of the second n-type semiconductor layer is 50 nm˜200 nm.
可选的,在所述的深紫外发光元件中,所述空穴阻拦层的材质为AlGaN和AlN中的至少一种。Optionally, in the deep ultraviolet light emitting element, the material of the hole blocking layer is at least one of AlGaN and AlN.
可选的,在所述的深紫外发光元件中,所述空穴阻拦层的材质中的Al组分含量大于90%。Optionally, in the deep ultraviolet light-emitting element, the content of the Al component in the material of the hole blocking layer is greater than 90%.
可选的,在所述的深紫外发光元件中,所述第二n型半导体层的材质包括AlGaN。Optionally, in the deep ultraviolet light-emitting element, the material of the second n-type semiconductor layer includes AlGaN.
可选的,在所述的深紫外发光元件中,所述第二n型半导体层的材质中的Al组分含量与所述第一n型半导体层相同。Optionally, in the deep ultraviolet light emitting element, the Al component content in the material of the second n-type semiconductor layer is the same as that of the first n-type semiconductor layer.
可选的,在所述的深紫外发光元件中,所述第二n型半导体层的材质中的Al组分含量为50%~75%。Optionally, in the deep ultraviolet light-emitting element, the Al component content in the material of the second n-type semiconductor layer is 50% to 75%.
可选的,在所述的深紫外发光元件中,所述第一n型半导体层材质中掺杂有Si,且所述Si掺杂浓度为8E18cm-3~5E19cm-3。Optionally, in the deep ultraviolet light emitting element, the material of the first n-type semiconductor layer is doped with Si, and the Si doping concentration is 8E18cm −3 to 5E19cm −3 .
可选的,在所述的深紫外发光元件中,所述第二n型半导体层中掺杂有Si,且所述第二n型半导体层中的Si掺杂浓度为所述第一n型半导体层的Si掺杂浓度的1.6%~62.5%。Optionally, in the deep ultraviolet light-emitting element, the second n-type semiconductor layer is doped with Si, and the Si doping concentration in the second n-type semiconductor layer is the first n-type The Si doping concentration of the semiconductor layer is 1.6% to 62.5%.
可选的,在所述的深紫外发光元件中,所述第二n型半导体层的材质中的Si掺杂浓度为8E17cm-3~5E18cm-3。Optionally, in the deep ultraviolet light emitting element, the Si doping concentration in the material of the second n-type semiconductor layer is 8E17cm -3 to 5E18cm -3 .
可选的,在所述的深紫外发光元件中,所述P型半导体层包括p型电子阻拦层和位于所述p型电子阻拦层上的p型接触层。Optionally, in the deep ultraviolet light-emitting element, the p-type semiconductor layer includes a p-type electron blocking layer and a p-type contact layer on the p-type electron blocking layer.
可选的,在所述的深紫外发光元件中,所述p型电子阻拦层的材质包括AlGaN。Optionally, in the deep ultraviolet light-emitting element, the material of the p-type electron blocking layer includes AlGaN.
可选的,在所述的深紫外发光元件中,所述p型接触层的材质包括AlGaN和GaN中的至少一种。Optionally, in the deep ultraviolet light-emitting element, the material of the p-type contact layer includes at least one of AlGaN and GaN.
可选的,在所述的深紫外发光元件中,所述外延层还包括位于所述衬底和所述第一n型半导体层之间的AlN层。Optionally, in the deep ultraviolet light-emitting element, the epitaxial layer further includes an AlN layer located between the substrate and the first n-type semiconductor layer.
为了实现上述目的以及其他相关目的,本发明还提供了一种深紫外发光元件的制备方法,包括:In order to achieve the above purpose and other related purposes, the present invention also provides a preparation method of a deep ultraviolet light-emitting element, including:
提供一衬底;providing a substrate;
在所述衬底上形成外延层,所述外延层从下至上依次包括:第一n型半导体层、阻拦层、量子阱层以及P型半导体层,其中,所述阻拦层包括至少两层空穴阻拦层以及每两层相邻的空穴阻拦层之间的第二n型半导体层。An epitaxial layer is formed on the substrate, and the epitaxial layer includes, from bottom to top, a first n-type semiconductor layer, a blocking layer, a quantum well layer and a p-type semiconductor layer, wherein the blocking layer includes at least two empty layers A hole blocking layer and a second n-type semiconductor layer between every two adjacent hole blocking layers.
可选的,在所述的深紫外发光元件的制备方法中,所述阻拦层为三明治结构层,其包括层叠的第一空穴阻拦层、第二n型半导体层以及第二空穴阻拦层。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the blocking layer is a sandwich structure layer, which includes a stacked first hole blocking layer, a second n-type semiconductor layer and a second hole blocking layer. .
可选的,在所述的深紫外发光元件的制备方法中,所述第一空穴阻拦层的厚度为 Optionally, in the preparation method of the deep ultraviolet light-emitting element, the thickness of the first hole blocking layer is
可选的,在所述的深紫外发光元件的制备方法中,所述第二空穴阻拦层的厚度为 Optionally, in the preparation method of the deep ultraviolet light-emitting element, the thickness of the second hole blocking layer is
可选的,在所述的深紫外发光元件的制备方法中,所述第二n型半导体层的厚度为50nm~200nm。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the thickness of the second n-type semiconductor layer is 50 nm˜200 nm.
可选的,在所述的深紫外发光元件的制备方法中,所述空穴阻拦层的材质为AlGaN和AlN中的至少一种。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the material of the hole blocking layer is at least one of AlGaN and AlN.
可选的,在所述的深紫外发光元件的制备方法中,所述空穴阻拦层的材质中的Al组分含量大于90%。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the content of the Al component in the material of the hole blocking layer is greater than 90%.
可选的,在所述的深紫外发光元件的制备方法中,所述第二n型半导体层的材质包括AlGaN。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the material of the second n-type semiconductor layer includes AlGaN.
可选的,在所述的深紫外发光元件的制备方法中,所述第二n型半导体层的材质中的Al组分含量与所述第一n型半导体层相同。Optionally, in the preparation method of the deep ultraviolet light emitting element, the content of the Al component in the material of the second n-type semiconductor layer is the same as that of the first n-type semiconductor layer.
可选的,在所述的深紫外发光元件的制备方法中,所述第二n型半导体层的材质中的Al组分含量为50%~75%。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the content of the Al component in the material of the second n-type semiconductor layer is 50% to 75%.
可选的,在所述的深紫外发光元件的制备方法中,所述第一n型半导体层材质中掺杂有Si,且所述Si掺杂浓度为8E18cm-3~5E19cm-3。Optionally, in the preparation method of the deep ultraviolet light emitting element, the material of the first n-type semiconductor layer is doped with Si, and the Si doping concentration is 8E18cm -3 to 5E19cm -3 .
可选的,在所述的深紫外发光元件的制备方法中,所述第二n型半导体层中掺杂有Si,且所述第二n型半导体层中的Si掺杂浓度为所述第一n型半导体层的Si掺杂浓度的1.6%~62.5%。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the second n-type semiconductor layer is doped with Si, and the Si doping concentration in the second n-type semiconductor layer is the same as that of the first n-type semiconductor layer. The Si doping concentration of an n-type semiconductor layer is 1.6% to 62.5%.
可选的,在所述的深紫外发光元件的制备方法中,所述第二n型半导体层的材质中的Si掺杂浓度为8E17cm-3~5E18cm-3。Optionally, in the preparation method of the deep ultraviolet light emitting element, the Si doping concentration in the material of the second n-type semiconductor layer is 8E17cm -3 to 5E18cm -3 .
可选的,在所述的深紫外发光元件的制备方法中,所述P型半导体层包括p型电子阻拦层和位于所述p型电子阻拦层上的p型接触层。Optionally, in the method for preparing a deep ultraviolet light-emitting element, the p-type semiconductor layer includes a p-type electron blocking layer and a p-type contact layer on the p-type electron blocking layer.
可选的,在所述的深紫外发光元件的制备方法中,所述p型电子阻拦层的材质包括AlGaN。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the material of the p-type electron blocking layer includes AlGaN.
可选的,在所述的深紫外发光元件的制备方法中,所述p型接触层的材质包括AlGaN和GaN中的至少一种。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the material of the p-type contact layer includes at least one of AlGaN and GaN.
可选的,在所述的深紫外发光元件的制备方法中,所述外延层还包括位于所述衬底和所述第一n型半导体层之间的AlN层。Optionally, in the method for preparing a deep ultraviolet light-emitting element, the epitaxial layer further includes an AlN layer located between the substrate and the first n-type semiconductor layer.
可选的,在所述的深紫外发光元件的制备方法中,所述第一n型半导体层、阻拦层、量子阱层以及p型半导体层形成的工艺为MOCVD工艺、分子束外延工艺、HVPE工艺、等离子体辅助化学气相沉积以及溅射法中的任意一种。Optionally, in the preparation method of the deep ultraviolet light-emitting element, the process of forming the first n-type semiconductor layer, blocking layer, quantum well layer and p-type semiconductor layer is MOCVD process, molecular beam epitaxy process, HVPE process. process, plasma-assisted chemical vapor deposition, and sputtering.
与现有技术相比,本发明的技术方案具有以下有益效果:Compared with the prior art, the technical scheme of the present invention has the following beneficial effects:
本发明通过在所述第一n型半导体层与量子阱层之间增加阻拦层,可调控量子阱层中电子空穴波函数的分布,减少p型空穴往第一n型半导体层扩散跃迁,同时,该阻拦层形成高的电子势垒可减少电子往量子阱层的注入效率,减轻量子阱层的电子和空穴的差异程度,提升量子阱层中电子和空穴的电子波函数的交叠和复合几率,进而提升深紫外发光元件的量子转换效率,使得深紫发光元件的发光效率提升至5%~10%。In the present invention, by adding a blocking layer between the first n-type semiconductor layer and the quantum well layer, the distribution of the wave function of electron holes in the quantum well layer can be regulated, and the diffusion transition of p-type holes to the first n-type semiconductor layer can be reduced. At the same time, the blocking layer forms a high electron barrier, which can reduce the injection efficiency of electrons into the quantum well layer, reduce the difference between electrons and holes in the quantum well layer, and improve the electron wave function of electrons and holes in the quantum well layer. The probability of overlap and recombination is improved, thereby improving the quantum conversion efficiency of the deep-ultraviolet light-emitting element, so that the light-emitting efficiency of the deep-violet light-emitting element is increased to 5% to 10%.
附图说明Description of drawings
图1是本发明一实施例的紫外半导体发光元件的结构示意图;1 is a schematic structural diagram of an ultraviolet semiconductor light-emitting element according to an embodiment of the present invention;
图2是本发明一实施例的紫外半导体发光元件的制备方法的流程图;2 is a flow chart of a method for preparing an ultraviolet semiconductor light-emitting element according to an embodiment of the present invention;
其中,图1~图2中:Among them, in Figure 1 to Figure 2:
100-衬底,101-第一n型半导体层,102-阻拦层,1021-第一空穴阻拦层,1022-第二n型半导体层,1023-第二空穴阻拦层,103-量子阱层,104-p型半导体层,1041-p型电子阻拦层,1042-p型接触层,105-AlN层。100-substrate, 101-first n-type semiconductor layer, 102-blocking layer, 1021-first hole blocking layer, 1022-second n-type semiconductor layer, 1023-second hole blocking layer, 103-quantum well layer, 104-p-type semiconductor layer, 1041-p-type electron blocking layer, 1042-p-type contact layer, 105-AlN layer.
具体实施方式Detailed ways
现有技术中的深紫外发光元件中的p型半导体层和n型半导体层的空穴和电子浓度差异较大,导致注入量子阱层的电子浓度远高于空穴浓度,进而导致电子空穴波函数在量子阱层的空间上分布极不一致,电子空穴复合效率低。在大电流注入情况下,多余的电子会溢出量子阱层,泄漏至p型半导体层,与空穴产生非辐射复合,进一步引起发光效率急剧下降。因此,电子和空穴在深紫外发光元件中浓度差异大、分布不均匀是导致其发光效率普遍低于5%的重要原因。The concentration of holes and electrons in the p-type semiconductor layer and the n-type semiconductor layer in the deep ultraviolet light-emitting element in the prior art are quite different, resulting in that the concentration of electrons injected into the quantum well layer is much higher than the concentration of holes, which in turn leads to electron holes. The spatial distribution of the wave function in the quantum well layer is extremely inconsistent, and the electron-hole recombination efficiency is low. In the case of high current injection, the excess electrons will overflow the quantum well layer, leak into the p-type semiconductor layer, and generate non-radiative recombination with holes, further causing a sharp drop in luminous efficiency. Therefore, the large concentration difference and uneven distribution of electrons and holes in deep ultraviolet light-emitting elements are the important reasons for their luminous efficiency generally lower than 5%.
为了解决电子和空穴在紫外半导体发光元件中浓度差异大和分布不均匀问题,本发明提供了一种紫外半导体发光元件,通过在第一n型半导体层与量子阱层之间增加空穴阻拦层,可以减少p型空穴往第一n型半导体层扩散跃迁,同时,形成高的电子势垒可减少电子往量子阱层的注入效率,减轻量子阱层的电子和空穴的浓度差异程度,提升量子阱层中电子和空穴的电子波函数的交叠复合几率,进而提升深紫外半导体发光元件的量子转换效率。In order to solve the problems of large concentration difference and uneven distribution of electrons and holes in the ultraviolet semiconductor light-emitting element, the present invention provides an ultraviolet semiconductor light-emitting element, by adding a hole blocking layer between the first n-type semiconductor layer and the quantum well layer , which can reduce the diffusion transition of p-type holes to the first n-type semiconductor layer. At the same time, the formation of a high electron barrier can reduce the injection efficiency of electrons into the quantum well layer and reduce the concentration difference between electrons and holes in the quantum well layer. The overlapping recombination probability of the electron wave functions of electrons and holes in the quantum well layer is improved, thereby improving the quantum conversion efficiency of the deep ultraviolet semiconductor light-emitting element.
在对按照本发明的实施方式进行说明之前,事先对下述内容进行说明。首先,在本说明书中,未明确给出Al组成比,仅标记为“AlGaN”时,表示III族元素(Al、Ga的总和)与N的化学组成比为1:1,III族元素Al与Ga的比率不固定的任意的化合物。另外,仅标记为“AlN”或“GaN”时,分别表示Ga和Al不包含在组成比中,但通过仅标记为“AlGaN”,并不排除为AlN或GaN中的任一者。需要说明的是,Al组成比的值可以通过光致发光测定和X射线衍射测定等进行测定。Before describing the embodiment according to the present invention, the following will be described in advance. First of all, in this specification, the Al composition ratio is not explicitly given, and when it is only marked as "AlGaN", it means that the chemical composition ratio of group III elements (the sum of Al and Ga) and N is 1:1, and the group III elements Al and An arbitrary compound in which the ratio of Ga is not fixed. In addition, when only marked with "AlN" or "GaN", it means that Ga and Al are not included in the composition ratio, respectively, but only marked with "AlGaN" does not exclude either AlN or GaN. It should be noted that the value of the Al composition ratio can be measured by photoluminescence measurement, X-ray diffraction measurement, or the like.
另外,本说明书中,将电学上以p型形式发挥作用的层称为p型层,将电学上以n型形式发挥作用的层称为n型层。另一方面,未特意添加Mg、Si等特定的杂质,电学上不以p型或n型发挥作用的情况下,称为“i型”或“未掺杂”。未掺杂的层中可以混入制造过程中的不可避免的杂质,具体而言,载流子密度小(例如,小于4×10/cm)的情况下,在本说明书中称为“未掺杂”。另外,Mg、Si等杂质浓度的值采用通过SIMS分析得到的值。In addition, in this specification, the layer which functions as a p-type electrically is called a p-type layer, and the layer which functions as an n-type electrically is called an n-type layer. On the other hand, when specific impurities such as Mg and Si are not intentionally added and do not function as p-type or n-type electrically, it is referred to as "i-type" or "undoped". The undoped layer can be mixed with unavoidable impurities during the manufacturing process. Specifically, when the carrier density is small (for example, less than 4×10/cm), it is referred to as “undoped layer” in this specification. ". In addition, the value of the impurity concentration, such as Mg and Si, was obtained by SIMS analysis.
以下结合附图和具体实施例对本发明提出的深紫外发光元件及其制备方法作进一步详细说明。根据下面说明书,本发明的优点和特征将更清楚。需说明的是,附图均采用非常简化的形式且均使用非精准的比例,仅用以方便、明晰地辅助说明本发明实施例的目的。The deep ultraviolet light-emitting element and its preparation method proposed by the present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments. The advantages and features of the present invention will become more apparent from the following description. It should be noted that, the accompanying drawings are all in a very simplified form and in inaccurate scales, and are only used to facilitate and clearly assist the purpose of explaining the embodiments of the present invention.
参阅图1,本实施例提供的深紫外发光元件包括:衬底100和位于所述衬底100上的外延层,所述外延层从下至上依次包括:第一n型半导体层101、阻拦层102、量子阱层103以及P型半导体层104。其中,所述阻拦层102包括至少两层空穴阻拦层以及每两层相邻的空穴阻拦层之间的第二n型半导体层。Referring to FIG. 1 , the deep ultraviolet light emitting element provided in this embodiment includes: a
作为衬底100,优选使用能够透射由量子阱层103发出的光并从衬底侧发出深紫外光的衬底,可以使用例如蓝宝石衬底或单晶AlN衬底等。另外,作为衬底100,也可以使用在蓝宝石衬底的表面外延生长了未掺杂的AlN结构层的AlN模板衬底。为了提高光提取效率,衬底100的出光侧或其相反侧、或AlN模板衬底的AlN结构层的表面可以为凹凸形状。为了降低AlN结构层的位错,也可以实施高温(例如1500℃以上)退火处理。As the
在所述衬底100与所述第一n型半导体层101之间可以设置有AlN层105。所述AlN层105可以作为缓冲层,其用于缓和所述衬底100与所述第一n型半导体层101的晶格失配。当然所述AlN层105也可以作为非故意掺杂层等。An
所述第一n型半导体层101根据需要借由所述AlN层105设置于所述衬底100上,也可以将所述第一n型半导体层101直接设置在所述衬底100上。所述第一n型半导体层101可以采用常规的n型层,例如可以由n-AlGaN构成。所述第一n型半导体层101通过掺杂n型的掺杂剂,从而作为n型层发挥作用,作为n型掺杂剂的具体例子,可以列举出硅(Si)、锗(Ge)、锡(Sn)、硫(S)、氧(O)、钛(Ti)、锆(Zr)等,但不限于此。所述n型掺杂剂的掺杂剂浓度只要为所述第一n型半导体层101能够作为n型层发挥作用的掺杂剂浓度即可。进一步的,所述第一n型半导体层101中的n型的掺杂剂优选为Si,且所述Si的掺杂浓度优选为8E18cm-3~5E19cm-3。另外,所述第一n型半导体层101的带隙优选比量子阱层103(采用多量子阱结构时为阱层)的带隙更宽,相对于发出的深紫外光具有透射性。另外,所述第一n型半导体层101除了可以为单层结构、由多层构成的结构外,也可以采用超晶格结构。The first n-
所述阻拦层102包括至少两层空穴阻拦层以及每两层相邻的空穴阻拦层之间的第二n型半导体层。所述阻拦层102可以包括两层空间阻拦层以及一层第二n型半导体层,也可以包括三层空间阻拦层以及两层第二n型半导体层。例如,所述阻拦层102依次包括第一空穴阻拦层、第二n型半导体层以及第二空穴阻拦层;再例如,所述阻拦层102依次包括第一空穴阻拦层、第二n型半导体层、第二空穴阻拦层、第二n型半导体层、第一空穴阻拦层。所述第一空穴阻拦层和第二空穴阻拦层可以完全相同,当然也可以不完全相同,例如,材质、Al组分含量以及厚度等其中的至少一种参数不同。当然所述阻拦层102也可以包括四层以及五层空间阻拦层等,所述第二n型半导体层也做相应增加,在此不做赘述。The
优选的,所述阻拦层102为三明治结构,包括依次层叠的第一空穴阻拦层1021、第二n型半导体层1022以及第二空穴阻拦层1023,请参阅图1。以下实施例均以所述阻拦层102为三明治结构为例进行详细介绍。Preferably, the
所述阻拦层102包括层叠在所述第一n型半导体层101上的第一空穴阻拦层1021、第二n型半导体层1022以及第二空穴阻拦层1023。所述第一空穴阻拦层1021和第二空穴阻拦层1023的材质均可以为AlGaN以及AlN中的至少一种,即所述第一空穴阻拦层1021的材质可以与所述第二空穴阻拦层1023相同,也可以不同。例如,所述第一空穴阻拦层1021的材质为AlGaN,而所述第二空穴阻拦层1023的材质为AlN。所述第一空穴阻拦层1021和第二空穴阻拦层1023的材质中的Al组分含量均大于90%,且所述第一空穴阻拦层1021和第二空穴阻拦层1023的材质中的Al组分含量可以相同,也可以不同。例如,所述第一空穴阻拦层1021和所述第二空穴阻拦层1023的材质均为AlGaN,且Al组分含量均为95%。再例如,所述第一空穴阻拦层1021的材质均为AlGaN,且Al组分含量均为95%,而所述第二空穴阻拦层1023的材质为AlN。The
由于所述第一空穴阻拦层1021和所述第二空穴阻拦层1023为高Al组分的结构层,具有比较高的电子势垒,第一n型半导体层101中的电子进入量子阱层103需要更多的能量,因此,所述第一空穴阻拦层1021和所述第二空穴阻拦层1023能够降低电子往量子阱层103的注入效率。而且由波尔茨曼分布或狄拉克分布可知,空穴有概率可以跃迁到第一n型半导体层101,而由所述第一空穴阻拦层1021、第二n型半导体层1022以及第二空穴阻拦层1023组成的三明治结构通过高势垒以及能带调控能够减少p型空穴往第一n型半导体层101扩散跃迁,增加了p型空穴的注入效率。根据上述分析,所述阻拦层102,即第一空穴阻拦层1021、第二n型半导体层1022以及第二空穴阻拦层1023组成的三明治结构可以减轻量子阱层103的电子和空穴的浓度差异程度以及分布不均匀的问题。Since the first
由于AlGaN是高阻材料,Al组分越高,电子离化能越高,阻值越大,电压越高,因此所述第一空穴阻拦层1021和第二空穴阻拦层1023的厚度不能太厚,不能超过设计值,否则会由于所述第一空穴阻拦层1021和/或第二空穴阻拦层1023太厚,引起阻值急剧上升以及电压升高等问题。所述第一空穴阻拦层1021的厚度(设计值)优选为所述第二空穴阻拦层1023的厚度(设计值)优选为 Since AlGaN is a high resistance material, the higher the Al composition, the higher the electron ionization energy, the higher the resistance value and the higher the voltage, so the thickness of the first
所述第二n型半导体层1022用于控制注入量子阱层103的电子浓度,以及电流扩展。所述第二n型半导体层1022的材质包括AlGaN,但不限于此。所述第二n型半导体层1022的材质中的Al组分含量与所述第一n型半导体层101可以相同,也可以不同。优选的,所述第二n型半导体层1022的材质中的Al组分含量与所述第一n型半导体层101相同。所述第二n型半导体层1022的材质中的Al组分含量优选为50%~75%。所述第二n型半导体层1022中掺杂有n型的掺杂剂,所述n型的掺杂剂可以为硅(Si)、锗(Ge)、锡(Sn)、硫(S)、氧(O)、钛(Ti)、锆(Zr)等,但不限于此。进一步的,所述n型的掺杂剂优选为Si,且所述第二n型半导体层1022中的Si掺杂浓度远低于所述第一n型半导体层101的Si掺浓度,以达到控制注入量子阱层103的电子浓度,以及提高第一n型AlGaN层101的横向电流扩展的作用。进一步的,所述第二n型半导体层1022中的Si掺杂浓度为所述第一n型半导体层101的Si掺浓度的1.6%~62.5%。优选的,所述第二n型半导体层1022的材质中的Si掺杂浓度为8E17cm-3~5E18cm-3。所述第二n型半导体层1022的厚度优选为50nm~200nm。The second n-
所述量子阱层103设置于所述阻拦层102上。所述量子阱层103可以由单层结构构成,优选由重复Al组成比不同的AlGaN构成的阱层和势垒层而形成的多量子阱(MQW:Multiple Quantum Well)结构构成。需要说明的是,单层结构的情况下,发出深紫外光的层为量子阱层本身,多量子阱结构的情况下,发出深紫外光的层为阱层。量子阱层103为现有结构,在此不做赘述。The
设置于所述量子阱层103上的p型半导体层104,所述p型半导体层104可以包括p型电子阻拦层1041和p型接触层1042。所述p型电子阻拦层1041用于阻挡电子,防止电子过溢到p型接触层1042,进而将电子注入至量子阱层103内,以减少非辐射复合的发生,进一步提高深紫外发光元件的发光效率。The p-
所述p型电子阻拦层1041的材质优选为AlGaN,但不限于此。所述p型电子阻拦层1041的厚度没有特别限制。需要说明的是,p型电子阻拦层1041的厚度优选为比势垒层的厚度厚。另外,作为掺杂至p型电子阻拦层1041中的p型掺杂剂,可以列举出镁(Mg)、锌(Zn)、钙(Ca)、铍(Be)、锰(Mn)等,但不限于此。所述p型掺杂剂优选为Mg。所述p型电子阻拦层1041的掺杂剂浓度只要为能够作为p型的半导体层发挥作用的掺杂剂浓度即可,没有特别限定。The material of the p-type
所述p型接触层1042设置于p型电子阻拦层1041上。p型接触层1042是用于减少设置于其正上方的p侧电极与p型电子阻拦层1041之间的接触电阻的层。所述p型接触层1042的材质包括AlGaN和GaN中的至少一种,但不限于此。作为深紫外发光元件的p型接触层,一般使用易于增加空穴浓度的p型GaN层,也可以使用p型AlGaN层,虽然AlGaN层与GaN层相比可能空穴浓度会有稍许降低,但由于从发光层发出的深紫外光能够透过p型AlGaN层,因此深紫外发光元件整体的光提取效率得以提高,能够提高深紫外发光元件的发光输出。The p-
相对于现有的深紫外发光元件,本实施例在第一n型半导体层和量子阱层之间具有阻拦层,该结构可调控量子阱层中电子空穴波函数的分布,可减少p型空穴往第一n型半导体层扩散跃迁,同时,该阻拦层结构形成高的电子势垒可减少电子往量子阱层的注入效率,减轻量子阱层的电子空穴的差异程度,提升量子阱层中电子和空穴的电子波函数的交叠和复合几率,最终提升深紫外发光元件的量子转换效率,提升深紫外发光元件的发光效率至5%~10%。Compared with the existing deep ultraviolet light-emitting element, this embodiment has a blocking layer between the first n-type semiconductor layer and the quantum well layer. This structure can control the distribution of the electron-hole wave function in the quantum well layer, and can reduce the p-type Holes diffuse and transition to the first n-type semiconductor layer, and at the same time, the blocking layer structure forms a high electron barrier, which can reduce the injection efficiency of electrons into the quantum well layer, reduce the difference between electrons and holes in the quantum well layer, and improve the quantum well layer. The overlap and recombination probability of the electron wave functions of electrons and holes in the layer ultimately improve the quantum conversion efficiency of the deep ultraviolet light-emitting element, and increase the luminous efficiency of the deep ultraviolet light-emitting element to 5% to 10%.
除此之外,本发明还提供了一种上述所述的深紫外发光元件的制备方法,具体包括:In addition, the present invention also provides a preparation method of the above-mentioned deep ultraviolet light-emitting element, which specifically includes:
步骤S0:提供一衬底;Step S0: providing a substrate;
步骤S1:在所述衬底上形成外延层,所述外延层从下至上依次包括:第一n型半导体层、阻拦层、量子阱层以及P型半导体层,其中,所述阻拦层包括至少两层空穴阻拦层以及每两层相邻的空穴阻拦层之间的第二n型半导体层。Step S1 : forming an epitaxial layer on the substrate, the epitaxial layer sequentially includes from bottom to top: a first n-type semiconductor layer, a blocking layer, a quantum well layer and a p-type semiconductor layer, wherein the blocking layer includes at least Two hole blocking layers and a second n-type semiconductor layer between every two adjacent hole blocking layers.
优选的,所述阻拦层为三明治结构,包括依次层叠的第一空穴阻拦层、第二n型半导体层以及第二空穴阻拦层。Preferably, the blocking layer is a sandwich structure, comprising a first hole blocking layer, a second n-type semiconductor layer and a second hole blocking layer stacked in sequence.
在所述衬底与所述第一n型半导体层之间还可以设置有缓冲层,用于缓和所述衬底与所述第一n型半导体层的晶格失配。作为缓冲层,可以使用未掺杂的III族氮化物半导体层,例如AlN层。A buffer layer may also be provided between the substrate and the first n-type semiconductor layer for relaxing the lattice mismatch between the substrate and the first n-type semiconductor layer. As the buffer layer, an undoped group III nitride semiconductor layer such as an AlN layer can be used.
所述p型半导体层包括p型电子阻拦层和p型接触层,所述p型电子阻拦层用于阻挡电子,所述p型接触层用于减少设置于其正上方的p侧电极与p型电子阻拦层之间的接触电阻。The p-type semiconductor layer includes a p-type electron blocking layer and a p-type contact layer. The p-type electron blocking layer is used to block electrons. contact resistance between the electron blocking layers.
参阅图2,所述外延层的形成过程具体包括:Referring to FIG. 2, the formation process of the epitaxial layer specifically includes:
步骤S11:在所述衬底上形成缓冲层;Step S11: forming a buffer layer on the substrate;
步骤S12:在所述缓冲层上形成第一n型半导体层;Step S12: forming a first n-type semiconductor layer on the buffer layer;
步骤S13:在所述第一n型半导体层形成阻拦层;Step S13: forming a blocking layer on the first n-type semiconductor layer;
步骤S14:在所述阻拦层上形成量子阱层;Step S14: forming a quantum well layer on the blocking layer;
步骤S15:在所述量子阱层上形成p型半导体层。Step S15: forming a p-type semiconductor layer on the quantum well layer.
在所述步骤S13中,在所述阻拦层为三明治结构,包括依次层叠的第一空穴阻拦层、第二n型半导体层以及第二空穴阻拦层时,在所述第一n型半导体层形成阻拦层的具体过程包括:In the step S13, when the blocking layer is a sandwich structure including a first hole blocking layer, a second n-type semiconductor layer and a second hole blocking layer stacked in sequence, the first n-type semiconductor The specific process of forming the blocking layer includes:
步骤S131:在所述第一n型半导体层形成第一空穴阻拦层;Step S131: forming a first hole blocking layer on the first n-type semiconductor layer;
步骤S132:在所述第一空穴阻拦层上形成第二n型半导体层;Step S132: forming a second n-type semiconductor layer on the first hole blocking layer;
步骤S133:在所述第二n型半导体层形成第二空穴阻拦层。Step S133 : forming a second hole blocking layer on the second n-type semiconductor layer.
需要说明的是,在上述制备方法中,可以通过有机金属气相沉积(MOCVD:MetAlOrganic ChemicAl Vapor Deposition)法、分子束外延(MBE:Molecular Beam Epitaxy)法、HVPE(Hydride Vapor Phase Epitaxy,氢化物气相外延)法、等离子体辅助化学气相沉积(plasmachemicAl vapor deposition,PCVD)、溅射法等公知的薄膜生长方法形成所述深紫外发光元件,例如可以通过MOCVD法形成所述缓冲层、第一n型半导体层、第一空穴阻拦层、第二n型半导体层、第二空穴阻拦层、量子阱层以及p型半导体层。It should be noted that, in the above preparation method, metal organic vapor deposition (MOCVD: MetAlOrganicChemicAl Vapor Deposition) method, molecular beam epitaxy (MBE:Molecular Beam Epitaxy) method, HVPE (Hydride Vapor Phase Epitaxy, hydride vapor phase epitaxy) method can be used ) method, plasma-assisted chemical vapor deposition (plasmachemic Al vapor deposition, PCVD), sputtering method and other known thin film growth methods to form the deep ultraviolet light-emitting element, for example, the buffer layer, the first n-type semiconductor can be formed by MOCVD method layer, a first hole blocking layer, a second n-type semiconductor layer, a second hole blocking layer, a quantum well layer, and a p-type semiconductor layer.
相对于现有的深紫外发光元件的技术方案,本发明在第一n型半导体层和量子阱层之间设置阻拦层结构,该结构可调控量子阱层中电子空穴波函数的分布,可减少p型空穴往第一n型半导体层扩散跃迁,同时,该阻拦层结构形成高的电子势垒可减少电子往量子阱层的注入效率,减轻量子阱层的电子和空穴的浓度差异程度,提升量子阱层中电子和空穴的电子波函数的交叠和复合几率,最终提升深紫外发光元件的量子转换效率,提升深紫外发光元件的发光效率至5%~10%。Compared with the existing technical solutions of deep ultraviolet light-emitting elements, the present invention sets a blocking layer structure between the first n-type semiconductor layer and the quantum well layer, which can regulate the distribution of the electron-hole wave function in the quantum well layer, and can Reduce the diffusion transition of p-type holes to the first n-type semiconductor layer, and at the same time, the blocking layer structure forms a high electron barrier, which can reduce the injection efficiency of electrons into the quantum well layer and reduce the concentration difference between electrons and holes in the quantum well layer. It can improve the overlap and recombination probability of the electron wave functions of electrons and holes in the quantum well layer, and finally improve the quantum conversion efficiency of the deep ultraviolet light emitting element, and improve the luminous efficiency of the deep ultraviolet light emitting element to 5% to 10%.
此外,可以理解的是,虽然本发明已以较佳实施例披露如上,然而上述实施例并非用以限定本发明。对于任何熟悉本领域的技术人员而言,在不脱离本发明技术方案范围情况下,都可利用上述揭示的技术内容对本发明技术方案作出许多可能的变动和修饰,或修改为等同变化的等效实施例。因此,凡是未脱离本发明技术方案的内容,依据本发明的技术实质对以上实施例所做的任何简单修改、等同变化及修饰,均仍属于本发明技术方案保护的范围内。In addition, it should be understood that, although the present invention has been disclosed above with preferred embodiments, the above embodiments are not intended to limit the present invention. For any person skilled in the art, without departing from the scope of the technical solution of the present invention, many possible changes and modifications can be made to the technical solution of the present invention by using the technical content disclosed above, or modified into equivalents of equivalent changes Example. Therefore, any simple modifications, equivalent changes and modifications made to the above embodiments according to the technical essence of the present invention without departing from the content of the technical solutions of the present invention still fall within the protection scope of the technical solutions of the present invention.
而且还应该理解的是,本发明并不限于此处描述的特定的方法、化合物、材料、制造技术、用法和应用,它们可以变化。还应该理解的是,此处描述的术语仅仅用来描述特定实施例,而不是用来限制本发明的范围。必须注意的是,此处的以及所附权利要求中使用的单数形式“一个”、“一种”以及“该”包括复数基准,除非上下文明确表示相反意思。因此,例如,对“一个步骤”引述意味着对一个或多个步骤的引述,并且可能包括次级步骤。应该以最广义的含义来理解使用的所有连词。因此,词语“或”应该被理解为具有逻辑“或”的定义,而不是逻辑“异或”的定义,除非上下文明确表示相反意思。此处描述的结构将被理解为还引述该结构的功能等效物。可被解释为近似的语言应该被那样理解,除非上下文明确表示相反意思。It is also to be understood that this invention is not limited to the particular methods, compounds, materials, fabrication techniques, uses and applications described herein, which may vary. It should also be understood that the terminology described herein is used to describe particular embodiments only, and not to limit the scope of the present invention. It must be noted that as used herein and in the appended claims, the singular forms "a," "an," and "the" include plural references unless the context clearly dictates otherwise. Thus, for example, reference to "a step" means a reference to one or more steps, and possibly including sub-steps. All conjunctions used should be understood in their broadest sense. Accordingly, the word "or" should be understood to have the definition of logical "or" rather than the definition of logical "exclusive or" unless the context clearly dictates otherwise. A structure described herein is to be understood to also refer to functional equivalents of the structure. Language that can be interpreted as approximate should be understood as such, unless the context clearly dictates otherwise.
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