WO2019113815A1 - Semiconductor structure and manufacturing process thereof - Google Patents
Semiconductor structure and manufacturing process thereof Download PDFInfo
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- WO2019113815A1 WO2019113815A1 PCT/CN2017/115805 CN2017115805W WO2019113815A1 WO 2019113815 A1 WO2019113815 A1 WO 2019113815A1 CN 2017115805 W CN2017115805 W CN 2017115805W WO 2019113815 A1 WO2019113815 A1 WO 2019113815A1
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 45
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 11
- 238000000034 method Methods 0.000 claims abstract description 23
- 230000004888 barrier function Effects 0.000 claims abstract description 19
- 230000008569 process Effects 0.000 claims abstract description 19
- 229910002704 AlGaN Inorganic materials 0.000 claims abstract description 10
- 230000007704 transition Effects 0.000 claims abstract description 7
- 229910052782 aluminium Inorganic materials 0.000 claims abstract description 6
- 229910052796 boron Inorganic materials 0.000 claims abstract description 6
- 239000002184 metal Substances 0.000 claims abstract description 6
- 229910052751 metal Inorganic materials 0.000 claims abstract description 6
- 229910052733 gallium Inorganic materials 0.000 claims abstract description 5
- 230000002596 correlated effect Effects 0.000 claims abstract description 4
- 238000005520 cutting process Methods 0.000 claims description 14
- 230000000737 periodic effect Effects 0.000 claims description 8
- 238000002347 injection Methods 0.000 abstract description 11
- 239000007924 injection Substances 0.000 abstract description 11
- 238000000407 epitaxy Methods 0.000 abstract description 9
- 239000000758 substrate Substances 0.000 description 12
- 239000000463 material Substances 0.000 description 6
- 229910052594 sapphire Inorganic materials 0.000 description 6
- 239000010980 sapphire Substances 0.000 description 6
- 230000005540 biological transmission Effects 0.000 description 4
- 230000004913 activation Effects 0.000 description 2
- 230000000903 blocking effect Effects 0.000 description 2
- 230000002349 favourable effect Effects 0.000 description 2
- 150000004767 nitrides Chemical class 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 230000005525 hole transport Effects 0.000 description 1
- 230000005012 migration Effects 0.000 description 1
- 238000013508 migration Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 238000002360 preparation method Methods 0.000 description 1
- 239000000243 solution Substances 0.000 description 1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/04—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a quantum effect structure or superlattice, e.g. tunnel junction
- H01L33/06—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a quantum effect structure or superlattice, e.g. tunnel junction within the light emitting region, e.g. quantum confinement structure or tunnel barrier
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/02—Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
- H01L33/26—Materials of the light emitting region
- H01L33/30—Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table
- H01L33/32—Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table containing nitrogen
Definitions
- the present invention relates to the field of semiconductors, and in particular to a semiconductor structure and a fabrication process thereof.
- III-V nitride light-emitting diodes have the advantages of high efficiency, energy saving, environmental protection and long life, and have important applications in solid-state lighting. As the application range of III-V nitride light-emitting diodes increases, the requirements for the photoelectric characteristics of light-emitting diodes become higher and higher.
- the low concentration of holes in the p-type layer and poor migration ability limit the performance of the UV-LED, and the activation energy of Mg in AlGaN is as high as 180-510 meV, so that the hole concentration at room temperature is obtained. Very low, only a few Mg can be activated.
- the higher the activation energy of Mg in the p-type AlGaN electron blocking layer the lower the hole concentration, and the more the hole injection can be blocked, which directly affects the luminous efficiency of the light-emitting diode. How to increase the injection rate of holes is an urgent problem to be solved by those skilled in the art.
- the present invention provides a semiconductor structure and a fabrication process thereof.
- the solution to the technical problem of the present invention is to provide a semiconductor structure, which in turn includes a superlattice transition layer, n-type AlGaN, an active region, an ultrashort periodic superlattice layer, and p-type BGaN; the ultrashort periodic supercrystal
- the grid layer is p-BxAlyGa1-x-yN/BmAlnGa1-m-nN, which includes multiple layers of alternating settings a barrier layer and a well layer, the barrier layer being p-type BxAlyGa1-x-yN, wherein 0 ⁇ x ⁇ 0.15, 0.5 ⁇ y ⁇ 0.65, and the well layer is p-type BmAlnGa1-m-nN, wherein 0 ⁇ m ⁇ 0.15, 0.35 ⁇ n ⁇ 0.50, one barrier layer and one adjacent well layer form a period, and the thickness of one period is greater than or equal to 1 nm and less than or equal to 2 nm.
- the thickness of the one cycle is 1 nm.
- the ultra-short period superlattice layer comprises 20-50 cycles.
- a layer of BAlGaN EBL is further included between the active region and the ultra-short period superlattice layer.
- Another aspect of the present invention is to provide a semiconductor structure fabrication process for fabricating the above semiconductor structure, wherein the B, Al, and Ga metal sources in the semiconductor structure are turned on and off in proportion. And the ratio of the on-off time is positively correlated with the epitaxial temperature; the on-off is alternately formed to form a pulse mode, and one pass-time and an adjacent cut-off time together constitute one cycle of the pulse.
- the time of the access is between 5 s and 10 s, and the time for cutting off the flow is between 2 s and 4 s.
- the access time is between 8s and 12s, and the cut-off flow time is between 2s and 4s; during the well layer epitaxy, the access time is between 5s. Between -10s, the time to cut off the flow is between 2s and 4s.
- the access time is between 5 s and 10 s, and the cut-off flow time is between 2 s and 4 s; during the well layer epitaxy, the access time is between 8 s. Between -12s, the time to cut off the flow is between 2s and 4s.
- the epitaxial temperature is between 1000 ° C and 1050 ° C.
- the epitaxial temperature is 1050 °C.
- a semiconductor structure according to a first embodiment of the present invention forms an ultra-short period superlattice and has a small thickness of one period, and a microstrip is formed inside the ultra-short period superlattice for cavity formation.
- Straight path transmission The internal energy band is more conducive to the transport of holes, and the rate at which holes are transported inside is higher, thereby increasing the injection rate of holes.
- the process adopts boundary temperature pulse epitaxy, that is, B, Al, Ga and other metal sources are turned on and off according to the ratio, and the higher the epitaxial temperature, the larger the ratio of on-off time, making it easier for the semiconductor to form ultra-short period super
- the crystal lattice increases the injection rate of holes inside the semiconductor.
- FIG. 1 is a schematic view showing a semiconductor structure according to a first embodiment of the present invention
- FIG. 2 is a schematic view showing the internal structure of a BAlGaN ultra-short period superlattice in a semiconductor structure according to a first embodiment of the present invention
- FIG. 3 is a schematic view showing the energy band structure of a p-type layer in a semiconductor structure of a device according to a first embodiment of the present invention
- a semiconductor structure 1 includes a sapphire substrate 11, an AlN layer 12, a superlattice transition layer 13, an n-type AlGaN 14, an active region 15, and a BAlGaN EBL layer 16 in order from bottom to top.
- EBL electron-blocking layer, electron blocking layer
- ultra-short period superlattice layer 17 and p-type BGaN 18 in all embodiments, upper, lower, left, right, inner, outer, etc. position qualifiers are limited to designation
- the superlattice transition layer 13 is an Al t Ga 1-t N/AlzGa 1-z N quantum well or an AlN/AlGaN quantum well or AlGaN.
- Gradient layer, t, z is greater than 0 and less than 1.
- the sapphire substrate 11 in the semiconductor structure 1 can be omitted, that is, the sapphire substrate 11 is peeled off.
- the sapphire substrate 11 may be replaced, that is, the superlattice transition layer 13 may be grown on a semiconductor structure having a sapphire substrate 11, or may be grown on a substrate made of AlN or other materials. The structure of the semiconductor.
- the ultra-short period superlattice layer 17 is pB x Al y Ga 1-xy N/B m Al n Ga 1-mn N, which includes a plurality of layers of barrier layers 171 and well layers alternately disposed.
- the barrier layer 171 is p-type B x Al y Ga 1-xy N, where 0 ⁇ x ⁇ 0.15, 0.5 ⁇ y ⁇ 0.65
- the well layer 172 is p-type B m Al n Ga 1-mn N Where 0 ⁇ m ⁇ 0.15, 0.35 ⁇ n ⁇ 0.50.
- a barrier layer 171 and a neighboring well layer 172 together form a period having a thickness d between 1 nm and 2 nm.
- the period thickness is 1 nm
- the ultrashort period superlattice 17 includes 20-50 cycles with a thickness of 20d-50d.
- the internal energy band of the ultra-short period superlattice layer 17 includes an A conduction band and a B valence band, wherein the A conduction band is used for electron transport and the B valence band is used for hole transport.
- the A conduction band and the B valence band are arranged in parallel with an approximate sine wave and the two are transverse waves of equal period, and the distance between the peak of the A conduction band and the trough of the B valence band is L (ie, the A conduction band and the B price)
- L the distance between the peak of the A conduction band and the trough of the B valence band
- L the distance between the peak of the A conduction band and the trough of the B valence band
- the width of the whole direction perpendicular to the propagation direction is L
- the length of one period of the A conduction band and the B valence band is J1+J2
- the size of L corresponds to the energy band width of the barrier layer 171, J1
- the size
- the hole has poor transmission capability in the p-type layer, resulting in low hole injection efficiency.
- the ultra-short period superlattice layer structure is favorable for forming the microstrip W in the valence band.
- the longitudinal transmission capability of the hole is enhanced, the injection efficiency of the hole is improved, and the working voltage of the device is lowered, which provides a good foundation for the preparation of the high-power deep ultraviolet LED, and improves the luminous efficiency of the light-emitting diode.
- the introduction of B reduces the difficulty of p-type doping of the barrier layer 171 and the well layer 172 material, and increases the carrier concentration of the p-type.
- a second embodiment of the present invention provides a semiconductor structure and a fabricator thereof
- a semiconductor structure 1 provided by the first embodiment of the present invention, which includes the following steps:
- Step S1 providing a substrate.
- the substrate is a sapphire substrate or an AlN substrate or other suitable material for the substrate.
- Step S2 a superlattice transition layer 13, an n-type AlGaN 14, an active region 15, a BAlGaN EBL layer 16, an ultrashort periodic superlattice layer 17, and a p-type BGaN 18 are sequentially formed on the substrate.
- the ultra-short period superlattice 17 is implemented by using a boundary temperature pulse epitaxy method to ensure the existence of the interface of the superlattice and the step flow growth of the epitaxial material under different epitaxial flows, in this embodiment.
- the epitaxial temperature T is between 1000 ° C and 1050 ° C, and the optimum value is 1050 ° C.
- the NH 3 is continuously supplied, and the metal sources such as B, Al, and Ga are turned on and off according to the ratio, and the higher the epitaxial temperature, the larger the ratio of the on-off time, that is, the ratio of the on-off time and The epitaxial temperature is positively correlated.
- the time of the access is between 5s and 10s
- the time for cutting off the flow is between 2s and 4s
- the time for the cut-off flow is 2s.
- the time for the flow and the cut-off flow is between Between 5:2 and 10:2, and the on and off of the B source alternately form a pulse mode, and one access time and an adjacent cut time together constitute one cycle of the pulse.
- the access time is between 8s and 12s, the time for cutting off the flow is between 2s and 4s, and the optimal time for the cutoff flow is 2s.
- the time for cutting off the flow is between 8:2-12:2, and the Al source of the barrier layer 171 alternates with the pulse to form a pulse mode; during the epitaxial process of the well layer 172, the access time is between 5s- Between 10s, the time to cut off the flow is between 2s and 4s, the optimal time for cutting off the flow is 2s, and the time for entering and cutting off the flow is between 5:2 and 10:2.
- the Al source of the well layer 172 alternately forms a pulse mode, and one pass time and an adjacent cut time together constitute one cycle of the pulse.
- the access time is between 5-10s
- the time for cutting off the flow is between 2s-4s
- the optimal time for the cutoff flow is 2s
- the access is
- the time for cutting off the flow is between 5:2 and 10:2
- the Al source of the barrier layer 171 alternates with the pulse to form a pulse mode, and one access time and an adjacent cut time together constitute a pulse.
- a cycle for the Ga source, during the epitaxial process of the barrier layer 171, the access time is between 5-10s, the time for cutting off the flow is between 2s-4s, and the optimal time for the cutoff flow is 2s, the access is And the time for cutting off the flow is between 5:2 and 10:2, and the Al source of the barrier layer 171 alternates with the pulse to form a pulse mode, and one access time and an adjacent cut time together constitute a pulse.
- a cycle for the Ga
- the access time is between 8s and 12s
- the time for cutting off the flow is between 2s and 4s
- the time for the cutoff flow is optimally 2s
- the flow rate of the cut-in and cut-off is The time is between 8:2 and 12:2
- the Ga source of the well layer 172 alternates to form a pulse mode, and an access time and an adjacent cut-off time together constitute one cycle of the pulse.
- a semiconductor structure according to a first embodiment of the present invention forms an ultra-short period superlattice and has a small period thickness, and a microstrip is formed inside the ultra-short period superlattice to provide a linear path for holes.
- the transmission makes its internal energy band more favorable for the transport of holes, the velocity of holes transported inside it is higher, thereby increasing the injection rate of holes, and the introduction of B element greatly increases the cavity ratio and further improves the cavity. Injection rate.
- a semiconductor structure is fabricated by using a boundary temperature pulse epitaxy method, and a metal source such as B, Al, or Ga is turned on and off in proportion, and the higher the epitaxial temperature, the higher the ratio of the on-off time. Larger, it is easier to form an ultra-short period superlattice inside the semiconductor, thereby increasing the injection rate of holes inside the semiconductor.
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Abstract
A semiconductor structure sequentially comprises a superlattice transition layer, n-type AlGaN, an active region, an ultra-short period superlattice layer, and p-type BGaN. The ultra-short period superlattice layer is p-BxAlyGa1-x-yN/BmAlnGa1-m-nN, and comprises a plurality of alternately disposed barrier layers and well layers. The barrier layers are p-type BxAlyGa1-x-yN, wherein 0 < x ≤ 0.15, and 0.5 ≤ y ≤0.65. The well layers are p-type BmAlnGa1-m-nN, wherein 0 < m ≤ 0.15, and 0.35 ≤ n ≤ 0.50. One barrier layer and one adjacent well layer form a period, and the thickness of one period is greater than or equal to 1 nm and less than or equal to 2 nm. A process for manufacturing the semiconductor structure is provided. Metal sources B, Al, and Ga in the semiconductor structure perform on-off processing according to a ratio thereof, and a ratio of on and off times and an epitaxy temperature are positively correlated. A pulse mode is formed by on-off alternation. One on time and one adjacent off time together form a pulse period. The semiconductor structure and the process thereof of the present invention improve semiconductor hole injection rates.
Description
本发明涉及半导体领域,特别涉及一种半导体结构及其制作工艺。The present invention relates to the field of semiconductors, and in particular to a semiconductor structure and a fabrication process thereof.
III-V族氮化物发光二极管具有高效、节能、环保、寿命长等优点,在固态照明领域有着重要的应用。随着III-V族氮化物发光二极管应用范围的增加,对发光二极管的光电特性的要求也越来越高。III-V nitride light-emitting diodes have the advantages of high efficiency, energy saving, environmental protection and long life, and have important applications in solid-state lighting. As the application range of III-V nitride light-emitting diodes increases, the requirements for the photoelectric characteristics of light-emitting diodes become higher and higher.
在现有技术中,UV-LED中,p型层中空穴的浓度低和迁移能力差限制了UV-LED的性能,Mg在AlGaN的激活能高达180-510meV,使得在室温下的空穴浓度很低,只有少数的Mg可以被激活。随着Al浓度的增加,Mg在p型AlGaN电子阻挡层的激活能就越高,空穴浓度就越低,也越能阻挡空穴的注入,直接影响了发光二级管的发光效率。如何提高空穴的注入率是本领域专业人员急需解决的问题。In the prior art, in the UV-LED, the low concentration of holes in the p-type layer and poor migration ability limit the performance of the UV-LED, and the activation energy of Mg in AlGaN is as high as 180-510 meV, so that the hole concentration at room temperature is obtained. Very low, only a few Mg can be activated. With the increase of Al concentration, the higher the activation energy of Mg in the p-type AlGaN electron blocking layer, the lower the hole concentration, and the more the hole injection can be blocked, which directly affects the luminous efficiency of the light-emitting diode. How to increase the injection rate of holes is an urgent problem to be solved by those skilled in the art.
【发明内容】[Summary of the Invention]
为了克服现有技术中p型AlGaN空穴浓度低和空穴迁移能力差的问题,本发明提供了一种半导体结构及其制作工艺。In order to overcome the problems of low hole concentration and poor hole mobility of p-type AlGaN in the prior art, the present invention provides a semiconductor structure and a fabrication process thereof.
本发明解决技术问题的方案是提供一种半导体结构,其依次包括超晶格过渡层、n型AlGaN、有源区、超短周期超晶格层以及p型BGaN;所述超短周期超晶格层为p-BxAlyGa1-x-yN/BmAlnGa1-m-nN,其包括多层交替设置
的垒层和阱层,所述垒层为p型BxAlyGa1-x-yN,其中0<x≤0.15,0.5≤y≤0.65,所述阱层为p型BmAlnGa1-m-nN,其中0<m≤0.15,0.35≤n≤0.50,一个垒层与相邻的一个阱层组成一周期,一个周期的厚度大于等于1nm小于等于2nm。The solution to the technical problem of the present invention is to provide a semiconductor structure, which in turn includes a superlattice transition layer, n-type AlGaN, an active region, an ultrashort periodic superlattice layer, and p-type BGaN; the ultrashort periodic supercrystal The grid layer is p-BxAlyGa1-x-yN/BmAlnGa1-m-nN, which includes multiple layers of alternating settings
a barrier layer and a well layer, the barrier layer being p-type BxAlyGa1-x-yN, wherein 0<x≤0.15, 0.5≤y≤0.65, and the well layer is p-type BmAlnGa1-m-nN, wherein 0<m ≤0.15, 0.35≤n≤0.50, one barrier layer and one adjacent well layer form a period, and the thickness of one period is greater than or equal to 1 nm and less than or equal to 2 nm.
优选地,所述一个周期的厚度为1nm。Preferably, the thickness of the one cycle is 1 nm.
优选地,所述超短周期超晶格层包括20-50个周期。Preferably, the ultra-short period superlattice layer comprises 20-50 cycles.
优选地,还包括BAlGaN EBL层,其介于有源区和超短周期超晶格层之间。Preferably, a layer of BAlGaN EBL is further included between the active region and the ultra-short period superlattice layer.
本发明解决技术问题的又一方案是提供一种半导体结构的制作工艺,其用于制作上述的半导体结构,其中,所述半导体结构中的B、Al、Ga金属源按照比例进行通和断处理,且通断时间的比例与外延温度正相关;通与断交替进行形成脉冲方式,一个通入时间和相邻的一个切断时间共同组成脉冲的一个周期。Another aspect of the present invention is to provide a semiconductor structure fabrication process for fabricating the above semiconductor structure, wherein the B, Al, and Ga metal sources in the semiconductor structure are turned on and off in proportion. And the ratio of the on-off time is positively correlated with the epitaxial temperature; the on-off is alternately formed to form a pulse mode, and one pass-time and an adjacent cut-off time together constitute one cycle of the pulse.
优选地,对于B源,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间。Preferably, for the B source, the time of the access is between 5 s and 10 s, and the time for cutting off the flow is between 2 s and 4 s.
优选地,对于Al源,垒层外延过程中,通入的时间介于8s-12s之间,切断流量的时间介于2s-4s之间;阱层外延过程中,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间。Preferably, for the Al source, during the epitaxial layer epitaxy, the access time is between 8s and 12s, and the cut-off flow time is between 2s and 4s; during the well layer epitaxy, the access time is between 5s. Between -10s, the time to cut off the flow is between 2s and 4s.
优选地,对于Ga源,垒层外延过程中,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间;阱层外延过程中,通入的时间介于8s-12s之间,切断流量的时间介于2s-4s之间。Preferably, for the Ga source, during the epitaxial layer epitaxy, the access time is between 5 s and 10 s, and the cut-off flow time is between 2 s and 4 s; during the well layer epitaxy, the access time is between 8 s. Between -12s, the time to cut off the flow is between 2s and 4s.
优选地,所述超短周期超晶格形成时,其外延温度介于1000℃-1050℃之间。Preferably, when the ultra-short period superlattice is formed, the epitaxial temperature is between 1000 ° C and 1050 ° C.
优选地,所述外延温度为1050℃。Preferably, the epitaxial temperature is 1050 °C.
与现有技术相比,本发明第一实施例一种半导体结构通过形成超短周期超晶格且其一个周期的厚度很小,所述超短周期超晶格内部形成微带供空穴呈直线路径传输使
其内部能带更有利于空穴的传输,空穴在其内部传输的速度更高从而提高了空穴的注入率。并且该超短周期超晶格的材料中引入B元素,大大增加了P型半导体层的空穴浓度,从而提高了半导体内部空穴的注入率;本发明第二实施例一种半导体结构的制作工艺通过采用边界温度脉冲外延方式,即B、Al、Ga等金属源按照比例进行通和断处理,且外延温度越高,通断时间的比例越大,使半导体内部更容易形成超短周期超晶格,从而提高了半导体内部空穴的注入率。Compared with the prior art, a semiconductor structure according to a first embodiment of the present invention forms an ultra-short period superlattice and has a small thickness of one period, and a microstrip is formed inside the ultra-short period superlattice for cavity formation. Straight path transmission
The internal energy band is more conducive to the transport of holes, and the rate at which holes are transported inside is higher, thereby increasing the injection rate of holes. And introducing the B element into the material of the ultra-short period superlattice, greatly increasing the hole concentration of the P-type semiconductor layer, thereby improving the injection rate of holes in the semiconductor; and fabricating the semiconductor structure according to the second embodiment of the present invention The process adopts boundary temperature pulse epitaxy, that is, B, Al, Ga and other metal sources are turned on and off according to the ratio, and the higher the epitaxial temperature, the larger the ratio of on-off time, making it easier for the semiconductor to form ultra-short period super The crystal lattice increases the injection rate of holes inside the semiconductor.
图1是本发明第一实施例一种半导体结构示意图;1 is a schematic view showing a semiconductor structure according to a first embodiment of the present invention;
图2是本发明第一实施例一种半导体结构中BAlGaN超短周期超晶格内部结构示意图;2 is a schematic view showing the internal structure of a BAlGaN ultra-short period superlattice in a semiconductor structure according to a first embodiment of the present invention;
图3是本发明第一实施例一种半导体结构在器件工作状态下p型层的能带结构示意图;3 is a schematic view showing the energy band structure of a p-type layer in a semiconductor structure of a device according to a first embodiment of the present invention;
为了使本发明的目的,技术方案及优点更加清楚明白,以下结合附图及实施实例,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。The present invention will be further described in detail below with reference to the accompanying drawings and embodiments. It is understood that the specific embodiments described herein are merely illustrative of the invention and are not intended to limit the invention.
请参阅图1,本发明第一实施例一种半导体结构1从下至上依次包括蓝宝石衬底11、AlN层12、超晶格过渡层13、n型AlGaN14、有源区15、BAlGaN EBL层16(EBL,electron-blocking layer,电子阻挡层)、超短周期超晶格层17和p型BGaN18(在所有实施例中,上、下、左、右、内、外等位置限定词仅限于指定视图上的相对位置,而非绝对位置),在本实施例中,所述超晶格过渡层13为AltGa1-tN/AlzGa1-zN量子阱或者AlN/AlGaN量子阱或者
AlGaN渐变层,t、z大于0小于1。作为一种变形,所述一种半导体结构1中的蓝宝石衬底11可以省略,即蓝宝石衬底11被剥离。作为另一种变形,蓝宝石衬底11可以替换,即所述超晶格过渡层13可以生长在具有蓝宝石衬底11的半导体结构上,也可以生长在以AlN为衬底或者其他材质为衬底的半导体结构上。Referring to FIG. 1, a semiconductor structure 1 according to a first embodiment of the present invention includes a sapphire substrate 11, an AlN layer 12, a superlattice transition layer 13, an n-type AlGaN 14, an active region 15, and a BAlGaN EBL layer 16 in order from bottom to top. (EBL, electron-blocking layer, electron blocking layer), ultra-short period superlattice layer 17 and p-type BGaN 18 (in all embodiments, upper, lower, left, right, inner, outer, etc. position qualifiers are limited to designation In the present embodiment, the superlattice transition layer 13 is an Al t Ga 1-t N/AlzGa 1-z N quantum well or an AlN/AlGaN quantum well or AlGaN. Gradient layer, t, z is greater than 0 and less than 1. As a variant, the sapphire substrate 11 in the semiconductor structure 1 can be omitted, that is, the sapphire substrate 11 is peeled off. As another variation, the sapphire substrate 11 may be replaced, that is, the superlattice transition layer 13 may be grown on a semiconductor structure having a sapphire substrate 11, or may be grown on a substrate made of AlN or other materials. The structure of the semiconductor.
请进一步参阅图2,所述超短周期超晶格层17为p-BxAlyGa1-x-yN/BmAlnGa1-m-nN,其包括多层交替设置的垒层171和阱层172,所述垒层171为p型BxAlyGa1-x-yN,其中0<x≤0.15,0.5≤y≤0.65,所述阱层172为p型BmAlnGa1-m-nN,其中0<m≤0.15,0.35≤n≤0.50。一个垒层171与相邻阱层172共同组成一周期,该周期的厚度d介于1nm-2nm之间,在本实施例中,其周期厚度为1nm,所述超短周期超晶格17包括20-50个周期,厚度为20d-50d。Referring to FIG. 2, the ultra-short period superlattice layer 17 is pB x Al y Ga 1-xy N/B m Al n Ga 1-mn N, which includes a plurality of layers of barrier layers 171 and well layers alternately disposed. 172, the barrier layer 171 is p-type B x Al y Ga 1-xy N, where 0 < x ≤ 0.15, 0.5 ≤ y ≤ 0.65, and the well layer 172 is p-type B m Al n Ga 1-mn N Where 0 < m ≤ 0.15, 0.35 ≤ n ≤ 0.50. A barrier layer 171 and a neighboring well layer 172 together form a period having a thickness d between 1 nm and 2 nm. In the present embodiment, the period thickness is 1 nm, and the ultrashort period superlattice 17 includes 20-50 cycles with a thickness of 20d-50d.
请进一步参阅图3,所述超短周期超晶格层17内部能带包括A导带和B价带,其中A导带用于供电子传输,B价带用于供空穴传输。所述A导带和B价带呈近似正弦波并列传输且该两者为周期相等的横波,A导带的波峰到B价带的波谷之间的距离为L(即A导带与B价带互成一体时其整体与传播方向垂直的方向上宽度为L),A导带和B价带的一个周期长度为J1+J2,L的大小对应所述垒层171的能带宽度,J1的大小对应所述垒层171的厚度,J2的大小对应所述阱层172的厚度。在现有技术中,空穴在p型层传输能力差,导致空穴注入效率较低,而本实施例中,所述超短周期超晶格层结构有利于在价带形成微带W,增强了空穴的纵向传输能力,提高了空穴的注入效率,且降低器件的工作电压,为大功率深紫外LED的制备提供了良好的基础,在提高发光二级管的发光效率方面起到关键作用。除此之外,通过B的引入会降低垒层171和阱层172材料p型掺杂的实现难度,提高了p型的载流子浓度。Referring to FIG. 3, the internal energy band of the ultra-short period superlattice layer 17 includes an A conduction band and a B valence band, wherein the A conduction band is used for electron transport and the B valence band is used for hole transport. The A conduction band and the B valence band are arranged in parallel with an approximate sine wave and the two are transverse waves of equal period, and the distance between the peak of the A conduction band and the trough of the B valence band is L (ie, the A conduction band and the B price) When the strips are integrated with each other, the width of the whole direction perpendicular to the propagation direction is L), and the length of one period of the A conduction band and the B valence band is J1+J2, and the size of L corresponds to the energy band width of the barrier layer 171, J1 The size corresponds to the thickness of the barrier layer 171, and the size of J2 corresponds to the thickness of the well layer 172. In the prior art, the hole has poor transmission capability in the p-type layer, resulting in low hole injection efficiency. In the embodiment, the ultra-short period superlattice layer structure is favorable for forming the microstrip W in the valence band. The longitudinal transmission capability of the hole is enhanced, the injection efficiency of the hole is improved, and the working voltage of the device is lowered, which provides a good foundation for the preparation of the high-power deep ultraviolet LED, and improves the luminous efficiency of the light-emitting diode. Key role. In addition, the introduction of B reduces the difficulty of p-type doping of the barrier layer 171 and the well layer 172 material, and increases the carrier concentration of the p-type.
本发明第二实施例提供一种半导体结构及其制作工
艺(以下工艺流程中提到的结构请参阅本发明第一实施例提供的一种半导体结构1的视图及编号),其包括如下步骤:A second embodiment of the present invention provides a semiconductor structure and a fabricator thereof
For the structure mentioned in the following process flow, please refer to the view and number of a semiconductor structure 1 provided by the first embodiment of the present invention, which includes the following steps:
步骤S1:提供一衬底。所述衬底为蓝宝石衬底或者AlN衬底或者其他适合做衬底的材质。Step S1: providing a substrate. The substrate is a sapphire substrate or an AlN substrate or other suitable material for the substrate.
步骤S2:在所述衬底上依次形成超晶格过渡层13、n型AlGaN14、有源区15、BAlGaN EBL层16、超短周期超晶格层17和p型BGaN18。Step S2: a superlattice transition layer 13, an n-type AlGaN 14, an active region 15, a BAlGaN EBL layer 16, an ultrashort periodic superlattice layer 17, and a p-type BGaN 18 are sequentially formed on the substrate.
在该步骤S2中,所述超短周期超晶格17的实现采用边界温度脉冲外延方式,在不同的外延流量下保证超晶格的界面存在和外延材料的台阶流生长,在本实施例中,所述外延温度T介于1000℃-1050℃之间,最佳值为1050℃。In the step S2, the ultra-short period superlattice 17 is implemented by using a boundary temperature pulse epitaxy method to ensure the existence of the interface of the superlattice and the step flow growth of the epitaxial material under different epitaxial flows, in this embodiment. The epitaxial temperature T is between 1000 ° C and 1050 ° C, and the optimum value is 1050 ° C.
在外延过程中保持NH3的持续通入,同时B、Al、Ga等金属源按照比例进行通和断处理,且外延温度越高,通断时间的比例越大,即通断时间的比例与外延温度正相关。对于B源,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间,该切断流量的时间最佳值为2s,所述通入和切断流量的时间介于5:2-10:2之间,且所述B源的通与断交替进行形成脉冲方式,一个通入时间和相邻的一个切断时间共同组成脉冲的一个周期。对于Al源,垒层171外延过程中,通入的时间介于8s-12s之间,切断流量的时间介于2s-4s之间,该切断流量的时间最佳值为2s,所述通入和切断流量的时间介于8:2-12:2之间,且所述垒层171的Al源通与断交替进行形成脉冲方式;阱层172外延过程中,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间,该切断流量的时间最佳值为2s,所述通入和切断流量的时间介于5:2-10:2之间,且所述阱层172的Al源通与断交替进行形成脉冲方式,一个通入时间和相邻的一个切断时间共同组成脉冲的一个周期。对于Ga源,垒层171外延过程中,通入的时间介于5-10s之间,切断流量的时间介于2s-4s之间,该切断流量的时间最佳值为2s,
所述通入和切断流量的时间介于5:2-10:2之间,且所述垒层171的Al源通与断交替进行形成脉冲方式,一个通入时间和相邻的一个切断时间共同组成脉冲的一个周期。阱层172外延过程中,通入的时间介于8s-12s之间,切断流量的时间介于2s-4s之间,该切断流量的时间最佳值为2s,所述通入和切断流量的时间介于8:2-12:2之间,且所述阱层172的Ga源通与断交替进行形成脉冲方式,一个通入时间和相邻的一个切断时间共同组成脉冲的一个周期。通过采用边界温度脉冲外延方式,在不同的外延流量下保证超晶格的界面存在和外延材料的台阶流生长,使所述半导体结构1内的超短周期超晶格17的周期厚度为1nm。In the epitaxial process, the NH 3 is continuously supplied, and the metal sources such as B, Al, and Ga are turned on and off according to the ratio, and the higher the epitaxial temperature, the larger the ratio of the on-off time, that is, the ratio of the on-off time and The epitaxial temperature is positively correlated. For the B source, the time of the access is between 5s and 10s, the time for cutting off the flow is between 2s and 4s, and the time for the cut-off flow is 2s. The time for the flow and the cut-off flow is between Between 5:2 and 10:2, and the on and off of the B source alternately form a pulse mode, and one access time and an adjacent cut time together constitute one cycle of the pulse. For the Al source, during the epitaxial process of the barrier layer 171, the access time is between 8s and 12s, the time for cutting off the flow is between 2s and 4s, and the optimal time for the cutoff flow is 2s. And the time for cutting off the flow is between 8:2-12:2, and the Al source of the barrier layer 171 alternates with the pulse to form a pulse mode; during the epitaxial process of the well layer 172, the access time is between 5s- Between 10s, the time to cut off the flow is between 2s and 4s, the optimal time for cutting off the flow is 2s, and the time for entering and cutting off the flow is between 5:2 and 10:2. The Al source of the well layer 172 alternately forms a pulse mode, and one pass time and an adjacent cut time together constitute one cycle of the pulse. For the Ga source, during the epitaxial process of the barrier layer 171, the access time is between 5-10s, the time for cutting off the flow is between 2s-4s, and the optimal time for the cutoff flow is 2s, the access is And the time for cutting off the flow is between 5:2 and 10:2, and the Al source of the barrier layer 171 alternates with the pulse to form a pulse mode, and one access time and an adjacent cut time together constitute a pulse. A cycle. During the epitaxial process of the well layer 172, the access time is between 8s and 12s, the time for cutting off the flow is between 2s and 4s, and the time for the cutoff flow is optimally 2s, and the flow rate of the cut-in and cut-off is The time is between 8:2 and 12:2, and the Ga source of the well layer 172 alternates to form a pulse mode, and an access time and an adjacent cut-off time together constitute one cycle of the pulse. By using the boundary temperature pulse epitaxy method, the existence of the interface of the superlattice and the step flow growth of the epitaxial material are ensured under different epitaxial flow rates, so that the periodic thickness of the ultrashort period superlattice 17 in the semiconductor structure 1 is 1 nm.
与现有技术相比,本发明第一实施例一种半导体结构通过形成超短周期超晶格且其周期厚度较小,所述超短周期超晶格内部形成微带供空穴呈直线路径传输使其内部能带更有利于空穴的传输,空穴在其内部传输的速度更高从而提高了空穴的注入率,并且,B元素的引入,大大提高空穴率,进一步提高空穴注入率。本发明第二实施例一种半导体结构的制作工艺通过采用边界温度脉冲外延方式,同时B、Al、Ga等金属源按照比例进行通和断处理,且外延温度越高,通断时间的比例越大,使半导体内部更容易形成超短周期超晶格,从而提高了半导体内部空穴的注入率。Compared with the prior art, a semiconductor structure according to a first embodiment of the present invention forms an ultra-short period superlattice and has a small period thickness, and a microstrip is formed inside the ultra-short period superlattice to provide a linear path for holes. The transmission makes its internal energy band more favorable for the transport of holes, the velocity of holes transported inside it is higher, thereby increasing the injection rate of holes, and the introduction of B element greatly increases the cavity ratio and further improves the cavity. Injection rate. According to a second embodiment of the present invention, a semiconductor structure is fabricated by using a boundary temperature pulse epitaxy method, and a metal source such as B, Al, or Ga is turned on and off in proportion, and the higher the epitaxial temperature, the higher the ratio of the on-off time. Larger, it is easier to form an ultra-short period superlattice inside the semiconductor, thereby increasing the injection rate of holes inside the semiconductor.
以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的原则之内所作的任何修改,等同替换和改进等均应包含本发明的保护范围之内。
The above is only the preferred embodiment of the present invention, and is not intended to limit the present invention, and any modifications, equivalents, and improvements made within the principles of the present invention should be included in the scope of the present invention.
Claims (10)
- 一种半导体结构,其特征在于:依次包括超晶格过渡层、n型AlGaN、有源区、超短周期超晶格层以及p型BGaN;所述超短周期超晶格层为p-BxAlyGa1-x-yN/BmAlnGa1-m-nN,其包括多层交替设置的垒层和阱层,所述垒层为p型BxAlyGa1-x-yN,其中0<x≤0.15,0.5≤y≤0.65,所述阱层为p型BmAlnGa1-m-nN,其中0<m≤0.15,0.35≤n≤0.50,一个垒层与相邻的一个阱层组成一周期,一个周期的厚度大于等于1nm小于等于2nm。A semiconductor structure, comprising: a superlattice transition layer, an n-type AlGaN, an active region, an ultrashort periodic superlattice layer, and p-type BGaN in sequence; the ultrashort periodic superlattice layer is pB x Al y Ga 1-xy N/B m Al n Ga 1-mn N, which includes a plurality of barrier layers and well layers alternately disposed, the barrier layer being p-type B x Al y Ga 1-xy N, wherein 0< x ≤ 0.15, 0.5 ≤ y ≤ 0.65, the well layer is p-type B m Al n Ga 1-mn N, where 0 < m ≤ 0.15, 0.35 ≤ n ≤ 0.50, one barrier layer and an adjacent well layer The composition is one cycle, and the thickness of one cycle is greater than or equal to 1 nm and less than or equal to 2 nm.
- 如权利要求1所述的一种半导体结构,其特征在于:所述一个周期的厚度为1nm。A semiconductor structure according to claim 1, wherein said one period has a thickness of 1 nm.
- 如权利要求1所述的一种半导体结构,其特征在于:所述超短周期超晶格层包括20-50个周期。A semiconductor structure according to claim 1 wherein said ultrashort periodic superlattice layer comprises 20-50 cycles.
- 如权利要求1所述的一种半导体结构,其特征在于:还包括BAlGaN EBL层,其介于有源区和超短周期超晶格层之间。A semiconductor structure according to claim 1 further comprising a layer of BAlGaN EBL interposed between the active region and the ultrashort periodic superlattice layer.
- 一种半导体结构的制作工艺,其用于制作如权利要求1-4任一项所述的半导体结构,其特征在于:所述半导体结构中的B、Al、Ga金属源按照比例进行通和断处理,且通断时间的比例与外延温度正相关;通与断交替进行形成脉冲方式,一个通入时间和相邻的一个切断时间共同组成脉冲的一个周期。A semiconductor structure fabrication process for fabricating a semiconductor structure according to any one of claims 1 to 4, wherein the B, Al, and Ga metal sources in the semiconductor structure are turned on and off in proportion Processing, and the ratio of the on-off time is positively correlated with the epitaxial temperature; the on-and-off alternately forms the pulse mode, and one access time and an adjacent cut-off time together constitute one cycle of the pulse.
- 如权利要求5所述的一种半导体结构的制作工艺,其特征在于:对于B源,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间。 The fabrication process of a semiconductor structure according to claim 5, wherein the time for the B source is between 5 s and 10 s, and the time for cutting off the flow is between 2 s and 4 s.
- 如权利要求5所述的一种半导体结构的制作工艺,其特征在于:对于Al源,垒层外延过程中,通入的时间介于8s-12s之间,切断流量的时间介于2s-4s之间;阱层外延过程中,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间。The fabrication process of a semiconductor structure according to claim 5, wherein, for the Al source, during the epitaxial process, the time of the access is between 8s and 12s, and the time for cutting off the flow is between 2s and 4s. During the extension of the well layer, the access time is between 5s and 10s, and the time for cutting off the flow is between 2s and 4s.
- 如权利要求5所述的一种半导体结构的制作工艺,其特征在于:对于Ga源,垒层外延过程中,通入的时间介于5s-10s之间,切断流量的时间介于2s-4s之间;阱层外延过程中,通入的时间介于8s-12s之间,切断流量的时间介于2s-4s之间。The fabrication process of a semiconductor structure according to claim 5, characterized in that, for the Ga source, the time of the access layer is between 5 s and 10 s, and the time for cutting off the flow is between 2 s and 4 s. During the extension of the well layer, the access time is between 8s and 12s, and the time for cutting off the flow is between 2s and 4s.
- 如权利要求5所述的一种半导体结构的制作工艺,其特征在于:所述超短周期超晶格形成时,其外延温度介于1000℃-1050℃之间。The fabrication process of a semiconductor structure according to claim 5, wherein when the ultrashort period superlattice is formed, the epitaxial temperature is between 1000 ° C and 1050 ° C.
- 如权利要求9所述的一种半导体结构的制作工艺,其特征在于:所述外延温度为1050℃。 A fabrication process for a semiconductor structure according to claim 9, wherein said epitaxial temperature is 1050 °C.
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