CN112054097A - Purple light LED epitaxial structure and manufacturing method - Google Patents
Purple light LED epitaxial structure and manufacturing method Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及一种发光二极管制作中的结构设计及制作方法。The invention relates to a structure design and a manufacturing method in the manufacture of a light-emitting diode.
背景技术Background technique
日前,日常家用产品的杀菌功能开始逐渐收到消费者的关注,ALGaN基 UVC-LED相比传统的紫外汞灯,由于其不使用汞,同时无需预热的特性,所 以在环保及节能方面具有特别大的优势,未来UVC-LED会大量进入商业空 调,表面杀菌与净水等应用市场,会带来UVC-LED新的增加需求,但是 UVC-LED结构中需要高AL组分的铝镓氮ALGaN材料,目前的生长技术无 法得到低缺陷密度的ALGaN材料,同时ALGaN量子阱结构存在较大的自发 极化和压电极化现象,造成能带弯曲,形成斯塔克效应QCSE,受其影响,量 子阱中的辐射复合效率非常低,因此通过减小ALGaN量子阱结构中的斯达克 效应QCSE,增加辐射复合效率,从而提高发光效率成为一个关键的技术问题。A few days ago, the sterilization function of daily household products has gradually attracted the attention of consumers. Compared with traditional ultraviolet mercury lamps, ALGaN-based UVC-LEDs do not use mercury and do not require preheating. Therefore, they have the advantages of environmental protection and energy saving. A particularly great advantage. In the future, UVC-LEDs will enter a large number of commercial air-conditioning, surface sterilization and water purification applications, which will bring new increased demand for UVC-LEDs. However, the structure of UVC-LEDs requires aluminum gallium nitride with high AL composition. ALGaN materials, the current growth technology cannot obtain ALGaN materials with low defect density, and the ALGaN quantum well structure has large spontaneous polarization and piezoelectric polarization, resulting in energy band bending and the formation of Stark effect QCSE, which is affected by it. , the radiative recombination efficiency in the quantum well is very low, so by reducing the Stark effect QCSE in the ALGaN quantum well structure, increasing the radiative recombination efficiency, thereby improving the luminous efficiency has become a key technical issue.
现有技术存在以下问题:目前,ALGaN基UVC-LED减小斯达克效应 QCSE的主要方法为ALGaN量子垒和ALGaN阻挡层中的AL组分进行线性 优化,从而降低量子阱的能带弯曲,达到限制斯达克效应QCSE的目的,从 而提升电子和空穴的复合,提高复合效率,但是该方法同时会降低空穴的注 入效率,因此改善效果有限。现有技术方案申请号201510300906已提出了 ALGaN和ALInGaN的技术方案,201811468293也有了ALN和ALGaN的技 术方案。针对上述的情况,我们要设计一种包含了新型阻挡层(N个循环结 构:氮化铝/ALxGa(1-x)N/ALaInbGa(1-a-b)N)的深紫外外延片制备方法,能 有效限制斯塔克效应QCSE,同时又提升了空穴的注入效果。The existing technology has the following problems: At present, the main method for reducing the QCSE of the Stark effect in ALGaN-based UVC-LEDs is to linearly optimize the ALGaN quantum barrier and the AL composition in the ALGaN barrier layer, thereby reducing the energy band bending of the quantum well, The purpose of limiting the Stark effect QCSE is achieved, thereby enhancing the recombination of electrons and holes and improving the recombination efficiency, but this method will reduce the injection efficiency of holes at the same time, so the improvement effect is limited. The prior art solution application number 201510300906 has proposed technical solutions for ALGaN and ALInGaN, and 201811468293 also has technical solutions for ALN and ALGaN. In view of the above situation, we want to design a deep ultraviolet epitaxial wafer preparation method including a novel barrier layer (N cycle structure: aluminum nitride/ALxGa(1-x)N/ALaInbGa(1-a-b)N), which can Effectively limit the Stark effect QCSE, and at the same time improve the hole injection effect.
发明内容SUMMARY OF THE INVENTION
为此,需要提供一种可提高紫光LED发光效率的外延片,解决现有技术 中电子迁移不足的问题。Therefore, it is necessary to provide an epitaxial wafer that can improve the luminous efficiency of a violet LED, and solve the problem of insufficient electron migration in the prior art.
一种紫光LED的外延结构制作方法,包括如下步骤,A method for fabricating an epitaxial structure of a violet LED, comprising the following steps:
S100、在衬底上溅射ALN薄膜;S100, sputtering an ALN film on the substrate;
S102、在所述ALN薄膜上生长一层铝镓氮缓冲层;S102, growing an aluminum gallium nitride buffer layer on the ALN film;
S103、在铝镓氮缓冲层上生长一层非掺杂的铝镓氮层;S103 , growing an undoped aluminum gallium nitride layer on the aluminum gallium nitride buffer layer;
S104、在非掺杂的铝镓氮上生长一层N型铝镓氮;S104, growing a layer of N-type AlGaN on the undoped AlGaN;
S105、在N型铝镓氮上生长应力释放层;S105, growing a stress release layer on the N-type AlGaN;
S106、在应力释放层上生长高温量子阱结构;S106, growing a high temperature quantum well structure on the stress release layer;
S107、在所述高温量子阱结构上生长发光量子阱结构;S107, growing a light-emitting quantum well structure on the high temperature quantum well structure;
S108、在所述的发光量子阱结构上生长阻挡层,所述阻挡层为铝镓氮阻 挡层,包括多个循环的(氮化铝/ALxGa(1-x)N/ALaInbGa(1-a-b)N);S108, growing a barrier layer on the light-emitting quantum well structure, where the barrier layer is an aluminum gallium nitride barrier layer, including multiple cycles of (AlN/AL x Ga (1-x) N/AL a In b Ga (1-ab) N);
S109、在所述的阻挡层结构上生长P型铝镓氮结构;S109, growing a P-type AlGaN structure on the barrier layer structure;
S110、在所述的P型铝镓氮上生长重掺杂P型ALGaN。S110 , growing heavily doped P-type ALGaN on the P-type AlGaN.
进一步地,在步骤S100之后还进行步骤,利用MOCVD,将所述ALN 薄膜缓冲层进行高温处理,温度1200-1300℃,转速1000-1200RPM,压力 200-750Torr;Further, after step S100, a further step is performed, using MOCVD to perform high temperature treatment on the ALN thin film buffer layer, the temperature is 1200-1300°C, the rotational speed is 1000-1200RPM, and the pressure is 200-750Torr;
具体地,步骤S100具体为,利用PECVD设备在蓝宝石衬底上溅射厚度 10-25nm之间的ALN薄膜。Specifically, step S100 is specifically, using PECVD equipment to sputter an ALN film with a thickness of 10-25 nm on the sapphire substrate.
具体地,所述铝镓氮阻挡层包括多个循环的(氮化铝/Mg掺杂的 ALxGa(1-x)N/ALaInbGa(1-a-b)N)。Specifically, the AlGaN barrier layer includes multiple cycles of (AlN/Mg-doped ALxGa(1- x ) N/ ALaInbGa (1- ab ) N).
进一步地,步骤S110所述的重掺杂的P型ALGaN层厚度5-10nm,Mg 掺杂浓度4E21,压力为400-800Torr。Further, the thickness of the heavily doped P-type ALGaN layer described in step S110 is 5-10 nm, the Mg doping concentration is 4E21, and the pressure is 400-800 Torr.
一种紫光LED的外延结构,包括衬底1上依次生长的如下部分:An epitaxial structure of a violet LED, comprising the following parts sequentially grown on a substrate 1:
ALN薄膜2;ALN
铝镓氮缓冲层3;AlGaN
非掺杂的铝镓氮层4;undoped aluminum
N型铝镓氮层5;N-type aluminum
应力释放层6;
高温量子阱结构7;High temperature
发光量子阱结构8;Light-emitting
阻挡层9,所述阻挡层为铝镓氮阻挡层,包括多个循环的(氮化铝 /ALxGa(1-x)N/ALaInbGa(1-a-b)N);A
P型铝镓氮结构10;P-
重掺杂P型ALGaN 11。Heavily doped P-type ALGaN 11.
进一步地,所述衬底为蓝宝石衬底。Further, the substrate is a sapphire substrate.
具体地,所述铝镓氮阻挡层包括多个循环的(氮化铝/Mg掺杂的 ALxGa(1-x)N/ALaInbGa(1-a-b)N)。Specifically, the AlGaN barrier layer includes multiple cycles of (AlN/Mg-doped ALxGa(1- x ) N/ ALaInbGa (1- ab ) N).
具体地,所述的重掺杂的P型ALGaN层厚度5-10nm,掺杂类型为Mg 掺杂。Specifically, the thickness of the heavily doped P-type ALGaN layer is 5-10 nm, and the doping type is Mg doping.
本发明通过蓝宝石上溅射ALN缓冲层,减少蓝宝石和ALGaN材料之间 因失配较大产生的缺陷,从而提高整个外延层的晶体质量,减少量子阱结构 中的位错和缺陷,降低因缺陷产生的非辐射复合,提高内量子效应,另一方 面还通过铝镓氮阻挡层(包含氮化铝/Mg掺杂ALxGa(1-x)N/ALaInbGa(1-a-b)N) 结构可以有效限制量子阱结构中的斯达克效应QCS,同时循环结构中的Mg 掺杂ALxGa(1-x)N增加材料界面的二维电子气,从而提升空穴注入发光区的能 力,提升发光区中电子和空穴的复合效率。从而获得了高质量的ALGaN基 紫光LED外延片使得紫光LED外延片提升约5-35%。By sputtering the ALN buffer layer on the sapphire, the invention reduces the defects caused by the large mismatch between the sapphire and the ALGaN material, thereby improving the crystal quality of the entire epitaxial layer, reducing dislocations and defects in the quantum well structure, and reducing defects caused by The resulting non-radiative recombination improves the internal quantum effect, and on the other hand also passes through the AlGaN barrier layer (containing AlN/Mg doped AL x Ga(1-x)N/AL a In b Ga(1-ab) The N) structure can effectively confine the Stark effect QCS in the quantum well structure, while the Mg-doped AL x Ga (1-x) N in the cyclic structure increases the two-dimensional electron gas at the material interface, thereby enhancing hole injection into the light-emitting region The ability to improve the recombination efficiency of electrons and holes in the light-emitting region. Thereby, a high-quality ALGaN-based violet LED epitaxial wafer is obtained, which improves the violet LED epitaxial wafer by about 5-35%.
附图说明Description of drawings
图1为具体实施方式所述的紫光外延片制作方法流程示意图;1 is a schematic flowchart of a method for fabricating a UV epitaxial wafer according to the specific embodiment;
图2为具体实施方式所述的紫光外延片结构示意图。FIG. 2 is a schematic diagram of the structure of the ultraviolet epitaxial wafer according to the specific embodiment.
附图标记说明Description of reference numerals
1、衬底:1. Substrate:
2、ALN薄膜;2. ALN film;
3、铝镓氮缓冲层;3. AlGaN buffer layer;
4、非掺杂的铝镓氮层;4. Undoped AlGaN layer;
5、N型铝镓氮层;5. N-type aluminum gallium nitride layer;
6、应力释放层;6. Stress release layer;
7、高温量子阱结构;7. High temperature quantum well structure;
8、发光量子阱结构;8. Light-emitting quantum well structure;
9、阻挡层;9. Barrier layer;
10、P型铝镓氮结构;10. P-type AlGaN structure;
11、重掺杂P型ALGaN。11. Heavy doped P-type ALGaN.
具体实施方式Detailed ways
为详细说明技术方案的技术内容、构造特征、所实现目的及效果,以下 结合具体实施例并配合附图详予说明。In order to describe in detail the technical content, structural features, achieved objects and effects of the technical solutions, the following detailed descriptions are given in conjunction with specific embodiments and in conjunction with the accompanying drawings.
请参阅图1,为一种紫光LED的外延结构制作方法,包括如下步骤,Please refer to FIG. 1 , which is a method for fabricating an epitaxial structure of a violet LED, including the following steps:
一种紫光LED的外延结构制作方法,包括如下步骤,A method for fabricating an epitaxial structure of a violet LED, comprising the following steps:
S100、在衬底上溅射ALN薄膜;S100, sputtering an ALN film on the substrate;
S102、在所述ALN薄膜上生长一层铝镓氮缓冲层;S102, growing an aluminum gallium nitride buffer layer on the ALN film;
S103、在铝镓氮缓冲层上生长一层非掺杂的铝镓氮层;S103 , growing an undoped aluminum gallium nitride layer on the aluminum gallium nitride buffer layer;
S104、在非掺杂的铝镓氮上生长一层N型铝镓氮;S104, growing a layer of N-type AlGaN on the undoped AlGaN;
S105、在N型铝镓氮上生长应力释放层;S105, growing a stress release layer on the N-type AlGaN;
S106、在应力释放层上生长高温量子阱结构;S106, growing a high temperature quantum well structure on the stress release layer;
S107、在所述高温量子阱结构上生长发光量子阱结构;S107, growing a light-emitting quantum well structure on the high temperature quantum well structure;
S108、在所述的发光量子阱结构上生长阻挡层,所述阻挡层为铝镓氮阻 挡层,包括多个循环的(氮化铝/ALxGa(1-x)N/ALaInbGa(1-a-b)N);S108, growing a barrier layer on the light-emitting quantum well structure, where the barrier layer is an aluminum gallium nitride barrier layer, including multiple cycles of (AlN/AL x Ga (1-x) N/AL a In b Ga (1-ab) N);
S109、在所述的阻挡层结构上生长P型铝镓氮结构;S109, growing a P-type AlGaN structure on the barrier layer structure;
S110、在所述的生长P型铝镓氮上生长重掺杂P型ALGaN。S110 , growing heavily doped P-type ALGaN on the growing P-type AlGaN.
以下通过具体实施例对具体的步骤进行说明。The specific steps are described below through specific embodiments.
S100、利用PECVD设备在蓝宝石衬底上溅射一定厚度的ALN薄膜,具 体的厚度可以设置在10-25nm之间,目的是为了减少蓝宝石和ALGaN材料之 间因为晶格失配产生的应力和缺陷,从而提高后续生长ALGaN材料的晶体质 量。在上述步骤中,所述溅射以高纯度AL靶材和氩气、氧气等等离子气体为 反应源,进行磁控溅射,使用温度为400-800℃,优选温度为650℃,ALN厚 度12-22nm,优选厚度为16nm,氧气流量为0.5-3sccm,优选为3sccm,氮气用量为80-300sccm,优选用量为100sccm。S100, using PECVD equipment to sputter a certain thickness of ALN film on the sapphire substrate, the specific thickness can be set between 10-25nm, the purpose is to reduce the stress and defects caused by lattice mismatch between the sapphire and ALGaN materials , thereby improving the crystal quality of the subsequently grown ALGaN material. In the above steps, the sputtering uses high-purity AL target material and plasma gas such as argon, oxygen, etc. as the reaction source, and performs magnetron sputtering. -22nm, preferably the thickness is 16nm, the oxygen flow rate is 0.5-3 sccm, preferably 3 sccm, the nitrogen dosage is 80-300 sccm, and the preferred dosage is 100 sccm.
S101、还可以利用MOCVD,将所述生长ALN薄膜缓冲层进行高温处理, 温度1200-1300℃,转速1000-1200RPM,压力200-750Torr,H2用量120-400slm。 未特别提及的温度、转速、压力均为MOVCD的环境设置参数,下同。通过 上述步骤分两个阶段分别溅射ALN薄膜缓冲层及进行高温处理,能够减少蓝 宝石和ALGaN材料之间因失配较大产生的缺陷,从而提高整个外延层的晶体 质量,减少量子阱结构中的位错和缺陷,降低因缺陷产生的非辐射复合,提 高内量子效应。S101. MOCVD can also be used to perform high temperature treatment on the grown ALN thin film buffer layer at a temperature of 1200-1300° C., a rotation speed of 1000-1200 RPM, a pressure of 200-750 Torr, and a H2 consumption of 120-400 slm. The temperature, rotation speed and pressure not mentioned in particular are the environment setting parameters of MOVCD, the same below. By sputtering the ALN thin film buffer layer in two stages and performing high-temperature treatment through the above steps, the defects caused by the large mismatch between the sapphire and ALGaN materials can be reduced, thereby improving the crystal quality of the entire epitaxial layer and reducing the number of defects in the quantum well structure. dislocations and defects, reduce the non-radiative recombination caused by defects, and improve the internal quantum effect.
S102、利用MOCVD,在所述ALN薄膜上生长一层铝镓氮缓冲层,厚度 10-15nm,温度550-850℃,转速500-600RPM,压力200-750Torr,H2用量 150-400slm,N2用量50-150slm,氨气用量50-200slm。S102. Using MOCVD, grow an AlGaN buffer layer on the ALN film, with a thickness of 10-15nm, a temperature of 550-850°C, a rotational speed of 500-600RPM, a pressure of 200-750Torr, the amount of H2 150-400slm, and the amount of N2 50 -150slm, ammonia consumption 50-200slm.
S103、在铝镓氮缓冲层上生长一层非掺杂的铝镓氮层,厚度1.5-1.8um, 温度1100-1150℃,转速800-1200RPM,压力50-750Torr。S103 , growing an undoped AlGaN layer on the AlGaN buffer layer with a thickness of 1.5-1.8um, a temperature of 1100-1150° C., a rotational speed of 800-1200 RPM, and a pressure of 50-750 Torr.
在具体的设计实施例中,步骤S103中的非掺杂ALGaN层共分为四层结 构,第一层温度900-1050℃,TMGa(三甲基镓)用量为800sccm,TMAL(三 甲基镓)用量为120sccm;第二层温度1050-1100,TMGa用量为1400sccm, TMAL用量为200sccm;第三层温度900-1050℃,TMGa用量为800sccm,TMAL 用量为120sccm,第四层温度1100-1150℃,TMGa用量为1800sccm,TMAL 用量为300sccm。In a specific design example, the undoped ALGaN layer in step S103 is divided into a four-layer structure, the temperature of the first layer is 900-1050° C., the amount of TMGa (trimethyl gallium) is 800 sccm, and the amount of TMAL (trimethyl gallium) is 800 sccm. The temperature of the second layer is 1050-1100, the amount of TMGa is 1400sccm, and the amount of TMAL is 200sccm; the temperature of the third layer is 900-1050℃, the amount of TMGa is 800sccm, the amount of TMAL is 120sccm, and the temperature of the fourth layer is 1100-1150℃ , the amount of TMGa is 1800sccm, and the amount of TMAL is 300sccm.
S104、在非掺杂铝镓氮上再生长一层N型铝镓氮;生长厚度1.5-2um, 温度1000-1200℃,转速800-1200RPM,压力100-750Torr,Si掺杂浓度约 1E19-1E20。S104, grow another layer of N-type AlGaN on the undoped AlGaN; the growth thickness is 1.5-2um, the temperature is 1000-1200°C, the rotation speed is 800-1200RPM, the pressure is 100-750Torr, and the Si doping concentration is about 1E19-1E20 .
S105、在N型铝镓氮上生长应力释放层;厚度0.15-0.3um,温度700-1000℃, 转速500-1200RPM,压力100-750Torr。S105 , growing a stress release layer on the N-type AlGaN; the thickness is 0.15-0.3um, the temperature is 700-1000° C., the rotational speed is 500-1200RPM, and the pressure is 100-750Torr.
S106、在应力释放层上生长高温量子阱结构(InGaN/ALGaN量子阱结构), 这里的高温量子阱结构由3-7个周期组成,厚度0.05-0.25um,温度850-900℃, 转速600-800RPM,压力100-750Torr。S106, growing a high-temperature quantum well structure (InGaN/ALGaN quantum well structure) on the stress release layer, where the high-temperature quantum well structure consists of 3-7 periods, a thickness of 0.05-0.25um, a temperature of 850-900° C., and a rotational speed of 600- 800RPM, pressure 100-750Torr.
S107、在所述的高温量子阱结构上在发光量子阱结构(InGaN/ALGaN量 子阱结构),由10-12个周期组成,厚度0.1-1.0um,温度850-950℃,转速 600-800RPM,压力100-750Torr。此处连续设置的两个量子阱,前者为高温, 后面为低温,主要原因是量子阱底部温度均为1000摄氏度以上,发光区量子 阱温度通常为750度(通常认为是低温),如果直接在反应腔体内在1000度 后直接生长低温量子阱,则会影响量子阱的质量,所以在中间加了个MQW 结构,温度约在850左右,目的是将腔体的温度缓慢降下来,从而可以保证 发光区量子阱温度的晶体质量。S107, on the high-temperature quantum well structure, a light-emitting quantum well structure (InGaN/ALGaN quantum well structure), consisting of 10-12 periods, a thickness of 0.1-1.0um, a temperature of 850-950°C, and a rotational speed of 600-800RPM, Pressure 100-750Torr. The two quantum wells set up in succession here, the former is high temperature and the latter is low temperature. The direct growth of low-temperature quantum wells in the reaction chamber after 1000 degrees will affect the quality of the quantum wells, so an MQW structure is added in the middle, and the temperature is about 850 degrees. The purpose is to reduce the temperature of the chamber slowly, so as to ensure Crystal quality of quantum well temperature in the light-emitting region.
S108、在所述的发光量子阱结构上生长新型阻挡层,该阻挡层包括多个循 环的(氮化铝/ALxGa(1-x)N/ALaInbGa(1-a-b)N),具体的实施例,可由6-15个周期组 成,厚度0.01-1.0um,温度850-900℃,转速600-800RPM,压力50-500Torr, 反应腔体。上述阻挡层可以有效限制量子阱结构中的斯达克效应QCS。作为 更进一步的实施例,铝镓氮阻挡层的成分为(氮化铝/Mg掺杂ALxGa(1-x)N/ALaInbGa(1-a-b)N)结构。同时循环结构中的Mg掺杂ALxGa(1-x)N增加材料界面的二维电子气,从而提升空穴注入发光区的能力,提升发光区中 电子和空穴的复合效率。S108, growing a novel barrier layer on the light-emitting quantum well structure, the barrier layer comprising a plurality of cycles of (AlN/AL x Ga (1-x) N/AL a In b Ga (1-ab) N ), a specific embodiment may consist of 6-15 cycles, the thickness is 0.01-1.0um, the temperature is 850-900°C, the rotational speed is 600-800RPM, the pressure is 50-500Torr, and the reaction chamber is used. The above-mentioned barrier layer can effectively confine the Stark effect QCS in the quantum well structure. As a further embodiment, the composition of the AlGaN barrier layer is an (AlN/Mg-doped ALxGa(1- x ) N/ ALaInbGa (1- ab ) N) structure. At the same time, the Mg-doped AL x Ga (1-x) N in the cyclic structure increases the two-dimensional electron gas at the material interface, thereby improving the ability of holes to be injected into the light-emitting region and improving the recombination efficiency of electrons and holes in the light-emitting region.
S109、在所述的阻挡层结构上生长P型铝镓氮结构,厚度20nm-100nm, Mg掺杂浓度1E20-5E20;S109, growing a P-type AlGaN structure on the barrier layer structure, with a thickness of 20nm-100nm, and a Mg doping concentration of 1E20-5E20;
S110、在所述的生长P型铝镓氮上生长重掺杂P型ALGaN,增加重掺杂 P型ALGaN目的是为了芯片制作过程中,ALGaN半导体材料上做金属电极, 可以形成良好的金半接触,该层厚度5-10nm,Mg掺杂浓度4E21,压力为 400-800Torr。在制作此种重掺杂P型ALGaN结构时,优选的实施例中,压力 可以选为650Torr,在该条件下,Mg在ALGaN材料中的掺杂效率最佳,可以 通过减少生产过程中Mg源的使用量,从而减少含Mg副产物并入ALGaN材 料中,进而在一定程度上减少Mg副产物对光的散射,从而提高出光效率。S110 , growing heavily doped P-type ALGaN on the growing P-type AlGaN, the purpose of adding heavily doped P-type ALGaN is to make a metal electrode on the ALGaN semiconductor material in the chip fabrication process, which can form a good gold half Contact, the layer thickness is 5-10nm, the Mg doping concentration is 4E21, and the pressure is 400-800Torr. When making such a heavily doped P-type ALGaN structure, in a preferred embodiment, the pressure can be selected to be 650 Torr. Under this condition, the doping efficiency of Mg in the ALGaN material is the best, which can be achieved by reducing the Mg source in the production process. Therefore, the incorporation of Mg-containing by-products into the ALGaN material can be reduced, thereby reducing the scattering of light by Mg by-products to a certain extent, thereby improving the light extraction efficiency.
最后对上述的ALGaN材料进行N2环境下的退火处理,完成紫光LED 外延片的生长。Finally, the above-mentioned ALGaN material is annealed in the N2 environment to complete the growth of the violet LED epitaxial wafer.
在某些进一步的实施例中,阻挡层的成分还进行改进为(氮化铝/MgNb 掺杂ALxGa(1-x)N/ALaInbGa(1-a-b)N),中间层掺杂Mg、Nb元素,能够更好地改 善材料界面的二维电子气,从而提升空穴注入发光区的能力,Nb掺杂属于我 司在众多金属掺杂剂中选择出的一种,通过改善掺杂条件掺入Nb元素,掺杂 会影响阻挡效果,空穴的注入能力会收到影响。我们的方案经过上千次实验 后,得出微量的铌和Mg掺杂可以解决这个空穴的注入能力。相对于现有技术 的对比样为ALN/ALGaN阻挡层的LED,发光能力提升5%-35%。In some further embodiments, the composition of the barrier layer is also modified to (Aluminum Nitride/MgNb doped ALxGa(1- x ) N/ ALaInbGa (1- ab ) N), the intermediate layer Doping Mg and Nb elements can better improve the two-dimensional electron gas at the material interface, thereby improving the ability of holes to inject into the light-emitting region. Nb doping is one of the metal dopants selected by our company. Improve the doping conditions and add Nb element, the doping will affect the blocking effect, and the hole injection ability will be affected. After thousands of experiments in our scheme, it is concluded that a small amount of niobium and Mg doping can solve the hole injection ability. Compared with the LED with the ALN/ALGaN barrier layer in the prior art, the luminous capacity is improved by 5%-35%.
在如图2所示的实施例中,本方案还提供一种紫光LED的外延结构,包 括衬底1上依次生长的如下部分:In the embodiment shown in Figure 2, the present solution also provides an epitaxial structure of a violet LED, comprising the following parts grown sequentially on the substrate 1:
ALN薄膜2;
铝镓氮缓冲层3;
非掺杂的铝镓氮层4;undoped aluminum
N型铝镓氮层5;N-type aluminum
应力释放层6;
高温量子阱结构7;High temperature
发光量子阱结构8;Light-emitting
阻挡层9,所述阻挡层为铝镓氮阻挡层,包括多个循环的(氮化铝 /ALxGa(1-x)N/ALaInbGa(1-a-b)N);A
P型铝镓氮结构10;P-
重掺杂P型ALGaN 11。Heavily doped P-
上述外延结构通过设计ALN薄膜,具体的厚度可以设置在10-25nm之间, 目的是为了减少蓝宝石和ALGaN材料之间因为晶格失配产生的应力和缺陷, 从而提高后续生长ALGaN材料的晶体质量。还通过设计铝镓氮阻挡层(包含 氮化铝/ALxGa(1-x)N/ALaInbGa(1-a-b)N)结构可以有效限制量子阱结构中的斯达 克效应QCS,从而提高紫光LED外延片的光效。The above epitaxial structure is designed by the ALN film, and the specific thickness can be set between 10-25nm, the purpose is to reduce the stress and defects caused by the lattice mismatch between the sapphire and the ALGaN material, thereby improving the crystal quality of the subsequently grown ALGaN material. . The Stark effect QCS in the quantum well structure can also be effectively limited by designing the AlGaN barrier layer (including AlN/AL x Ga (1-x) N/AL a In b Ga (1-ab) N) structure , thereby improving the light efficiency of the violet LED epitaxial wafer.
进一步地实施例中,该结构的衬底为M型蓝宝石衬底。In a further embodiment, the substrate of the structure is an M-type sapphire substrate.
具体地,所述铝镓氮阻挡层包括多个循环的(氮化铝/Mg掺杂的 ALxGa(1-x)N/ALaInbGa(1-a-b)N)。Specifically, the AlGaN barrier layer includes multiple cycles of (AlN/Mg-doped ALxGa(1- x ) N/ ALaInbGa (1- ab ) N).
具体地,所述的重掺杂的P型ALGaN层厚度5-10nm,掺杂类型为Mg 掺杂。Mg在ALGaN材料中的掺杂效率最佳,可以通过减少生产过程中Mg 源的使用量,从而减少含Mg副产物并入ALGaN材料中,进而在一定程度上 减少Mg副产物对光的散射,从而提高出光效率。Specifically, the thickness of the heavily doped P-type ALGaN layer is 5-10 nm, and the doping type is Mg doping. The doping efficiency of Mg in ALGaN materials is the best. By reducing the amount of Mg source used in the production process, the incorporation of Mg-containing by-products into ALGaN materials can be reduced, thereby reducing the scattering of light by Mg by-products to a certain extent. Thus, the light extraction efficiency is improved.
需要说明的是,尽管在本文中已经对上述各实施例进行了描述,但并非 因此限制本发明的专利保护范围。因此,基于本发明的创新理念,对本文所 述实施例进行的变更和修改,或利用本发明说明书及附图内容所作的等效结 构或等效流程变换,直接或间接地将以上技术方案运用在其他相关的技术领 域,均包括在本发明专利的保护范围之内。It should be noted that, although the above-mentioned embodiments have been described herein, it does not limit the scope of the patent protection of the present invention. Therefore, based on the innovative concept of the present invention, changes and modifications to the embodiments described herein, or equivalent structures or equivalent process transformations made by using the contents of the description and drawings of the present invention, directly or indirectly apply the above technical solutions In other related technical fields, all are included in the protection scope of the patent of the present invention.
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