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CN106784181B - Method and structure for improving luminous efficiency of green light or longer wavelength InGaN quantum well - Google Patents

Method and structure for improving luminous efficiency of green light or longer wavelength InGaN quantum well Download PDF

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CN106784181B
CN106784181B CN201611153017.6A CN201611153017A CN106784181B CN 106784181 B CN106784181 B CN 106784181B CN 201611153017 A CN201611153017 A CN 201611153017A CN 106784181 B CN106784181 B CN 106784181B
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CN106784181A (en
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田爱琴
刘建平
张书明
李德尧
张立群
杨辉
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Suzhou Institute of Nano Tech and Nano Bionics of CAS
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    • H01S5/34333Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer based on Ga(In)N or Ga(In)P, e.g. blue laser
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Abstract

The invention discloses a method and a structure for improving the luminous efficiency of a green light or longer wavelength InGaN quantum well. The method comprises the following steps: adopting a substrate with atomic steps, wherein the chamfer angle formed by adjacent atomic steps on the substrate is more than 0.2 degrees; forming a buffer layer on the atomic step surface; forming a high-temperature n-type GaN layer on the buffer layer; an InGaN quantum well is formed on the high temperature n-type GaN layer. The method for improving the light emitting efficiency of the InGaN quantum well by adopting the substrate with the large chamfer angle adopts the substrate with the chamfer angle larger than 0.2 degrees to grow the active region of the green light or longer wavelength InGaN quantum well, can realize the atomic step flow growth of the green light or longer wavelength InGaN quantum well, improve the appearance of the atomic step flow growth, and improve the internal quantum efficiency of the InGaN quantum well. In addition, the InGaN quantum well prepared by the method can be widely applied to GaN-based green light or longer-wavelength LEDs and GaN-based green light or longer-wavelength lasers, and can also be widely applied to multi-quantum well solar cells.

Description

提高绿光或更长波长InGaN量子阱发光效率的方法及结构Method and structure for improving luminous efficiency of green light or longer wavelength InGaN quantum wells

技术领域technical field

本发明属于半导体技术领域,具体地讲,涉及一种提高绿光或更长波长InGaN量子阱发光效率的方法及结构。The invention belongs to the technical field of semiconductors, and in particular relates to a method and a structure for improving the luminous efficiency of a green light or longer wavelength InGaN quantum well.

背景技术Background technique

GaN基绿光或更长波长激光器和LED在半导体显示与照明方面有非常广泛的应用。InGaN量子阱有源区作为GaN基激光器和LED的核心结构,其生长行为、形貌对InGaN量子阱的光学性质和器件的性能有非常重要的影响。GaN-based green or longer wavelength lasers and LEDs are widely used in semiconductor displays and lighting. The InGaN quantum well active region is the core structure of GaN-based lasers and LEDs, and its growth behavior and morphology have a very important impact on the optical properties of InGaN quantum wells and device performance.

由于InN的平衡蒸汽压非常高,并且In-N键能弱,导致InN的分解温度低。因此,高In组分的InGaN必须在低温下生长以保证足够多的In并入外延层。一般用MOCVD生长InGaN的温度大概在650℃~750℃之间。但通常在较低的生长温度下,表面原子的迁移率低,迁移距离短。对于绿光或更长波长InGaN量子阱,由于InGaN量子阱层有更高的In组分以获得长波长发光,在采用MOCVD的方法生长时,需要更低的温度与更高的In/Ga比。当在斜切角较小的衬底上外延生长时,由于原子台阶宽度较大,原子落到样品表面的时候不能迁移到原子台阶边缘适合并入的位置并入,而是直接在原子台阶表面成核,这种情况下InGaN的AFM形貌一般是一些沿原子台阶分布的二维岛状的形貌。在这种二维岛的形貌之上再生长量子垒层,会导致InGaN量子阱和量子垒层之间的表面粗糙,进而影响InGaN量子阱有源区的光学性能。Since the equilibrium vapor pressure of InN is very high and the In-N bond energy is weak, the decomposition temperature of InN is low. Therefore, InGaN with high In composition must be grown at low temperature to ensure sufficient In incorporation into the epitaxial layer. Generally, the temperature for growing InGaN by MOCVD is between 650°C and 750°C. But usually at lower growth temperatures, the mobility of surface atoms is low and the migration distance is short. For green light or longer wavelength InGaN quantum wells, since the InGaN quantum well layer has a higher In composition to obtain long-wavelength luminescence, a lower temperature and a higher In/Ga ratio are required when growing by MOCVD. . When epitaxial growth is carried out on a substrate with a small chamfer angle, due to the large width of the atomic step, when the atoms fall on the surface of the sample, they cannot migrate to the position where the edge of the atomic step is suitable for incorporation, but directly on the surface of the atomic step. Nucleation, the AFM morphology of InGaN in this case is generally some two-dimensional island-like morphology distributed along the atomic steps. Regrowing the quantum barrier layer on top of this 2D island morphology will cause the surface roughness between the InGaN quantum well and the quantum barrier layer, which in turn affects the optical properties of the InGaN quantum well active region.

发明内容SUMMARY OF THE INVENTION

为了解决上述现有技术中存在的问题,本发明的目的在于提供一种提高绿光或更长波长InGaN量子阱发光效率的方法,从而得到呈原子台阶流生长且内量子效率高的InGaN量子阱。In order to solve the above-mentioned problems in the prior art, the purpose of the present invention is to provide a method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells, so as to obtain InGaN quantum wells grown in atomic step flow and with high internal quantum efficiency .

本发明提供了一种提高绿光或更长波长InGaN量子阱发光效率的方法,其包括:The present invention provides a method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells, comprising:

采用一具有原子台阶的衬底,其中所述衬底上相邻原子台阶形成的斜切角大于0.2°;Using a substrate with atomic steps, wherein the chamfer angle formed by adjacent atomic steps on the substrate is greater than 0.2°;

在所述原子台阶面上形成缓冲层;forming a buffer layer on the atomic step surface;

在所述缓冲层上形成高温n型GaN层;forming a high temperature n-type GaN layer on the buffer layer;

在所述高温n型GaN层上形成InGaN量子阱。InGaN quantum wells are formed on the high temperature n-type GaN layer.

进一步地,每相邻两个原子台阶形成的斜切角相等;和/或所述衬底上相邻原子台阶形成的斜切角为0.2°~15°。Further, the chamfer angle formed by every two adjacent atomic steps is equal; and/or the chamfer angle formed by adjacent atomic steps on the substrate is 0.2°˜15°.

进一步地,所述缓冲层为低温不掺杂GaN层,所述低温不掺杂GaN层的厚度为10nm~30nm。Further, the buffer layer is a low temperature undoped GaN layer, and the thickness of the low temperature undoped GaN layer is 10 nm˜30 nm.

进一步地,所述高温n型GaN层的厚度小于5000nm。Further, the thickness of the high temperature n-type GaN layer is less than 5000 nm.

进一步地,所述高温n型GaN层的电子浓度在1017cm-3到1019cm-3之间。Further, the electron concentration of the high temperature n-type GaN layer is between 10 17 cm -3 and 10 19 cm -3 .

进一步地,所述绿光或更长波长InGaN量子阱为不掺杂的InxGa1-xN量子阱。Further, the green light or longer wavelength InGaN quantum well is an undoped InxGa1 - xN quantum well.

进一步地,所述InxGa1-xN量子阱的厚度为1nm~5nm,且所述InxGa1-xN量子阱的In组分随InGaN量子阱发光波长的增加而增大。Further, the thickness of the InxGa1 - xN quantum well is 1 nm˜5 nm, and the In composition of the InxGa1 - xN quantum well increases with the increase of the emission wavelength of the InGaN quantum well.

进一步地,每一级原子台阶上形成的InGaN量子阱呈原子台阶流形貌。Further, the InGaN quantum wells formed on each level of atomic steps have an atomic step flow morphology.

进一步地,所述InGaN量子阱的原子台阶高度与相邻高一级原子台阶的高度相等。Further, the height of the atomic step of the InGaN quantum well is equal to the height of the adjacent one-step higher atomic step.

本发明还提供了一种利用如上所述的方法来提高绿光或更长波长InGaN量子阱发光效率的结构,包括:衬底,具有原子台阶,且相邻原子台阶形成的斜切角大于0.2°;缓冲层,形成在所述原子台阶面上;高温n型GaN层,形成在所述缓冲层上;InGaN量子阱,形成在所述高温n型GaN层上。The present invention also provides a structure for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells by using the above method, comprising: a substrate with atomic steps, and the chamfer angle formed by adjacent atomic steps is greater than 0.2 °; a buffer layer is formed on the atomic step surface; a high temperature n-type GaN layer is formed on the buffer layer; an InGaN quantum well is formed on the high temperature n-type GaN layer.

本发明的有益效果:本发明的提高绿光或更长波长InGaN量子阱发光效率的方法采用斜切角大于0.2°的衬底生长绿光或更长波长InGaN量子阱有源区,可以实现绿光或更长波长InGaN量子阱的原子台阶流生长,改善其形貌,并提高InGaN量子阱的内量子效率。此外,由上述方法制备得到的InGaN量子阱既可以广泛应用于GaN基绿光或更长波长LED、GaN基绿光或更长波长激光器中,也可以广泛应用于多量子阱太阳能电池中。Beneficial effects of the present invention: the method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells of the present invention uses a substrate with a chamfer angle greater than 0.2° to grow green light or longer wavelength InGaN quantum well active regions, which can realize green light Atomic step flow growth of optical or longer wavelength InGaN quantum wells, improving their morphology and increasing the internal quantum efficiency of InGaN quantum wells. In addition, the InGaN quantum well prepared by the above method can be widely used not only in GaN-based green light or longer wavelength LEDs, GaN-based green light or longer wavelength lasers, but also in multi-quantum well solar cells.

附图说明Description of drawings

通过结合附图进行的以下描述,本发明的实施例的上述和其它方面、特点和优点将变得更加清楚,附图中:The above and other aspects, features and advantages of embodiments of the present invention will become more apparent from the following description taken in conjunction with the accompanying drawings, in which:

图1是本发明实施例的提高绿光或更长波长InGaN量子阱发光效率的方法的步骤流程图;1 is a flow chart of the steps of a method for improving the luminous efficiency of a green light or longer wavelength InGaN quantum well according to an embodiment of the present invention;

图2是由本发明实施例的方法制备得到的绿光或更长波长InGaN量子阱结构的材料结构示意图;2 is a schematic diagram of the material structure of a green light or longer wavelength InGaN quantum well structure prepared by the method of an embodiment of the present invention;

图3是由本发明实施例的方法制备得到的绿光或更长波长InGaN量子阱结构的立体图;3 is a perspective view of a green light or longer wavelength InGaN quantum well structure prepared by the method of an embodiment of the present invention;

图4是本发明实施例的衬底的斜切角与原子台阶宽度关系示意图;4 is a schematic diagram of the relationship between the chamfer angle and the atomic step width of a substrate according to an embodiment of the present invention;

图5(a)是在斜切角度为0.2°的GaN衬底上形成的绿光InGaN量子阱的AFM形貌图;Figure 5(a) is an AFM topography of a green light InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.2°;

图5(b)是在斜切角度为0.54°的GaN衬底上形成的绿光InGaN量子阱的AFM形貌图;Figure 5(b) is an AFM topography of a green light InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.54°;

图5(c)是在斜切角度为0.6°的GaN衬底上形成的绿光InGaN量子阱的AFM形貌图;Figure 5(c) is an AFM topography of a green light InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.6°;

图6(a)是在斜切角度为0.2°的GaN衬底上形成的绿光InGaN量子阱的变温PL测试结果曲线图;Fig. 6(a) is a graph showing the result of a variable temperature PL test of a green light InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.2°;

图6(b)是在斜切角度为0.56°的GaN衬底上形成的绿光InGaN量子阱的变温PL测试结果曲线图。Fig. 6(b) is a graph showing the result of a variable temperature PL test of a green light InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.56°.

具体实施方式Detailed ways

以下,将参照附图来详细描述本发明的实施例。然而,可以以许多不同的形式来实施本发明,并且本发明不应该被解释为限制于这里阐述的具体实施例。相反,提供这些实施例是为了解释本发明的原理及其实际应用,从而本领域的其他技术人员能够理解本发明的各种实施例和适合于特定预期应用的各种修改。相同的标号在整个说明书和附图中可用来表示相同的元件。Hereinafter, embodiments of the present invention will be described in detail with reference to the accompanying drawings. The present invention may, however, be embodied in many different forms and should not be construed as limited to the specific embodiments set forth herein. Rather, these embodiments are provided to explain the principles of the invention and its practical applications, to thereby enable others skilled in the art to understand the invention for various embodiments and with various modifications as are suited to the particular intended use. The same reference numbers may be used throughout the specification and drawings to refer to the same elements.

在附图中,为了使组件清晰展示,夸大了层和区域的厚度。此外,相同的标号在整个说明书和附图中可用来表示相同的元件。In the drawings, the thicknesses of layers and regions are exaggerated for clarity of illustration of components. Furthermore, the same reference numbers may be used throughout the specification and drawings to refer to the same elements.

图1是本发明实施例的提高绿光或更长波长InGaN量子阱发光效率的方法的步骤流程图。FIG. 1 is a flow chart of steps of a method for improving the luminous efficiency of a green light or longer wavelength InGaN quantum well according to an embodiment of the present invention.

参照图1,本发明的实施例提供了一种提高绿光或更长波长InGaN量子阱发光效率的方法,其包括以下步骤:Referring to FIG. 1, an embodiment of the present invention provides a method for improving the luminous efficiency of a green light or longer wavelength InGaN quantum well, which includes the following steps:

步骤S1:采用一具有原子台阶的衬底,其中所述衬底上相邻原子台阶形成的斜切角大于0.2°;Step S1: using a substrate with atomic steps, wherein the chamfer angle formed by adjacent atomic steps on the substrate is greater than 0.2°;

步骤S2:在所述原子台阶面上形成缓冲层;Step S2: forming a buffer layer on the atomic step surface;

步骤S3:在所述缓冲层上形成高温n型GaN层;Step S3: forming a high temperature n-type GaN layer on the buffer layer;

步骤S4:在所述高温n型GaN层上形成InGaN量子阱。Step S4: forming InGaN quantum wells on the high temperature n-type GaN layer.

图2是由本发明实施例的方法制备得到的InGaN量子阱结构的材料结构示意图。图3是由本发明实施例的方法制备得到的InGaN量子阱结构的立体图。FIG. 2 is a schematic diagram of the material structure of the InGaN quantum well structure prepared by the method of the embodiment of the present invention. FIG. 3 is a perspective view of an InGaN quantum well structure prepared by the method of an embodiment of the present invention.

参照图2和图3,采用上述方法,制备得到如图2和图3所示的用于提高绿光或更长波长InGaN量子阱发光效率的结构,在这里,简称为InGaN量子阱结构。该InGaN量子阱结构包括衬底1、缓冲层2、高温n型GaN层3、InGaN量子阱4。其中,衬底1具有原子台阶,且相邻原子台阶形成的斜切角大于0.2°。缓冲层2形成在所述原子台阶面上。高温n型GaN层3形成在缓冲层2上。InGaN量子阱4形成在所述高温n型GaN层3上。Referring to FIGS. 2 and 3 , using the above method, a structure for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells as shown in FIGS. 2 and 3 is prepared, which is referred to as an InGaN quantum well structure here. The InGaN quantum well structure includes a substrate 1 , a buffer layer 2 , a high temperature n-type GaN layer 3 , and an InGaN quantum well 4 . The substrate 1 has atomic steps, and the chamfer angle formed by adjacent atomic steps is greater than 0.2°. The buffer layer 2 is formed on the atomic step surface. The high temperature n-type GaN layer 3 is formed on the buffer layer 2 . InGaN quantum wells 4 are formed on the high temperature n-type GaN layer 3 .

结合步骤S1,衬底1可以是GaN衬底,也可以是蓝宝石衬底或SiC衬底或Si衬底。本发明并不限制于此。Combined with step S1, the substrate 1 may be a GaN substrate, or a sapphire substrate, a SiC substrate, or a Si substrate. The present invention is not limited to this.

图4是本发明实施例的衬底的斜切角与原子台阶宽度关系示意图。FIG. 4 is a schematic diagram of the relationship between the chamfer angle and the atomic step width of the substrate according to an embodiment of the present invention.

减小衬底1的表面原子台阶宽度,在低温下生长高In组分绿光或更长波长InGaN量子阱4时,原子能够迁移到原子台阶边缘并入,以原子台阶流生长模式生长,获得好的表面形貌与晶体质量。如图4所示,图4为斜切角与原子台阶宽度关系示意图。假定衬底1的相邻两个原子台阶之间的坡度为斜切角α,原子台阶的高度为h,Lt为原子台阶宽度,则tanα=h/Lt,即Lt=h/tanα。那么当原子台阶高度h一定时,原子台阶宽度Lt随衬底1斜切角α的增大而减小。在本实施例中,相邻两个原子台阶之间的坡度大于0.2°,即采用斜切角α大于0.2°的衬底1生长高In组分绿光或更长波长InGaN量子阱4。衬底1的斜切角α越大时,表面原子台阶的宽度越小,低温下生长时原子能够迁移到原子台阶边缘并入,形成原子台阶流的生长模式。进一步地,相邻原子台阶形成的斜切角α可以是大于0.2°小于15°,对于绿光InGaN量子阱优选为0.4°~0.7°,而对于更长波长InGaN量子阱,最优斜切角更大,本发明并不限制于此。The atomic step width on the surface of the substrate 1 is reduced, and when the high In composition green light or the longer wavelength InGaN quantum well 4 is grown at a low temperature, the atoms can migrate to the edge of the atomic step and be incorporated, and grow in the atomic step flow growth mode to obtain Good surface morphology and crystal quality. As shown in FIG. 4 , FIG. 4 is a schematic diagram showing the relationship between the chamfer angle and the width of the atomic step. Assuming that the slope between two adjacent atomic steps of the substrate 1 is the chamfer angle α, the height of the atomic steps is h, and Lt is the width of the atomic steps, then tanα=h/Lt, that is, Lt=h/tanα. Then, when the atomic step height h is constant, the atomic step width Lt decreases with the increase of the chamfer angle α of the substrate 1 . In this embodiment, the slope between two adjacent atomic steps is greater than 0.2°, that is, the substrate 1 with the chamfer angle α greater than 0.2° is used to grow high In composition green light or longer wavelength InGaN quantum wells 4 . When the chamfer angle α of the substrate 1 is larger, the width of the atomic steps on the surface is smaller, and the atoms can migrate to the edge of the atomic steps and merge into the atomic steps during growth at low temperature, forming the growth mode of atomic step flow. Further, the chamfer angle α formed by the adjacent atomic steps can be greater than 0.2° and less than 15°. For green light InGaN quantum wells, it is preferably 0.4° to 0.7°, and for longer wavelength InGaN quantum wells, the optimal chamfer angle is larger, the present invention is not limited thereto.

优选地,在本实施例中,所述原子台阶为规则递增型台阶。每相邻两个原子台阶形成的斜切角α相等。Preferably, in this embodiment, the atomic steps are regularly increasing steps. The chamfer angle α formed by every two adjacent atomic steps is equal.

结合步骤S2、S3、S4,缓冲层2、高温n型GaN层3和InGaN量子阱4的生长方法可以是MOCVD也可以是MBE。MOCVD指的是在气相外延生长(VPE)的基础上发展起来的一种新型气相外延生长技术。MBE指的是一种分子束外延的晶体生长技术。但本发明并不限制于此。Combining steps S2, S3 and S4, the growth method of the buffer layer 2, the high temperature n-type GaN layer 3 and the InGaN quantum well 4 can be MOCVD or MBE. MOCVD refers to a new type of vapor phase epitaxy growth technology developed on the basis of vapor phase epitaxy (VPE). MBE refers to a crystal growth technique of molecular beam epitaxy. However, the present invention is not limited to this.

具体地,结合步骤S2,缓冲层2形成在衬底1的原子台阶面上,缓冲层2具体为低温不掺杂GaN层。具体地,低温不掺杂GaN层的厚度为10nm~30nm。Specifically, in combination with step S2, the buffer layer 2 is formed on the atomic step surface of the substrate 1, and the buffer layer 2 is specifically a low-temperature undoped GaN layer. Specifically, the thickness of the low-temperature undoped GaN layer is 10 nm˜30 nm.

结合步骤S3,高温n型GaN层3形成在缓冲层2上,其厚度小于5000nm,电子浓度在1017cm-3到1019cm-3之间。Combined with step S3, a high temperature n-type GaN layer 3 is formed on the buffer layer 2, the thickness of which is less than 5000 nm, and the electron concentration is between 10 17 cm -3 and 10 19 cm -3 .

在本实施例中,低温不掺杂GaN层(缓冲层2)和高温n型GaN层3依次形成在原子台阶的上表面之上,即原子台阶宽为Lt的表面(如图4所示)上。In this embodiment, the low-temperature undoped GaN layer (buffer layer 2 ) and the high-temperature n-type GaN layer 3 are sequentially formed on the upper surface of the atomic step, that is, the surface with the atomic step width Lt (as shown in FIG. 4 ) superior.

结合步骤S4,InGaN量子阱4为不掺杂的InxGa1-xN量子阱。InxGa1-xN量子阱的厚度为1nm~5nm之间,其In组分随InGaN量子阱发光波长的增加而增大,例如发光波长为520nm的InGaN量子阱中的In组分大约为25%,发光波长更长的InGaN量子阱中的In组分也更高。Combined with step S4, the InGaN quantum well 4 is an undoped InxGa1 - xN quantum well. The thickness of the In x Ga 1-x N quantum well is between 1 nm and 5 nm, and its In composition increases with the increase of the emission wavelength of the InGaN quantum well. For example, the In composition in the InGaN quantum well with the emission wavelength of 520 nm is approximately 25%, and the In composition in the InGaN quantum wells with longer emission wavelengths is also higher.

从图3中可知,每一级原子台阶上的InGaN量子阱4呈原子台阶流形貌,且每一级原子台阶上的InGaN量子阱4恰好布满该原子台阶。或者说InGaN量子阱4分布于原子台阶水平台阶面外沿。更具体地,InGaN量子阱4与其相邻的高级原子台阶的上表面齐平,或者说他们位于同一高度(同一水平面)上。It can be seen from FIG. 3 that the InGaN quantum wells 4 on each atomic step have an atomic step flow shape, and the InGaN quantum wells 4 on each atomic step are exactly filled with the atomic steps. In other words, the InGaN quantum wells 4 are distributed on the outer edge of the horizontal step plane of the atomic step. More specifically, the InGaN quantum well 4 is flush with the upper surface of its adjacent high-level atomic steps, or they are located at the same height (same level).

根据本发明实施例的采用大斜切角衬底提高InGaN量子阱发光效率的方法,采用斜切角大的衬底1来依次生长缓冲层2、高温n型GaN层3、InGaN量子阱4,由于衬底1原子台阶的宽度窄,因此在特定温度特定生长速率下生长绿光或更长波长InGaN量子阱4时,原子的迁移距离一定,当原子台阶的宽度较窄时,原子有更大几率迁移到原子台阶边缘并入原子台阶,从而形成原子台阶流生长模式。通过变温PL测试内量子效率发现本发明实施例的原子台阶流生长模式的InGaN量子阱4有更高的内量子效率。According to the method for improving the luminous efficiency of an InGaN quantum well by using a substrate with a large chamfer angle according to an embodiment of the present invention, a substrate 1 with a large chamfer angle is used to sequentially grow the buffer layer 2, the high-temperature n-type GaN layer 3, and the InGaN quantum well 4, Since the width of the atomic steps of the substrate 1 is narrow, when the green light or longer wavelength InGaN quantum wells 4 are grown at a specific temperature and a specific growth rate, the migration distance of the atoms is certain. When the width of the atomic steps is narrow, the atoms have a larger The probability migrates to the edge of the atomic step and merges into the atomic step, thus forming the atomic step flow growth mode. It is found that the InGaN quantum well 4 in the atomic step flow growth mode of the embodiment of the present invention has a higher internal quantum efficiency by measuring the internal quantum efficiency of the variable temperature PL.

图5(a)是在斜切角度为0.2°的GaN衬底上形成的InGaN量子阱4的AFM形貌图。图5(b)是在斜切角度为0.54°的GaN衬底上形成的InGaN量子阱的AFM形貌图。图5(c)是在斜切角度为0.6°的GaN衬底上形成的InGaN量子阱的AFM形貌图。FIG. 5( a ) is an AFM topography diagram of an InGaN quantum well 4 formed on a GaN substrate with a chamfer angle of 0.2°. Figure 5(b) is an AFM topography of an InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.54°. Figure 5(c) is an AFM topography of an InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.6°.

需要说明的是,在该测试中采用的是绿光InGaN量子阱。由图5(a)~图5(c)的AFM形貌测试结果可知,在斜切角较小的衬底1上生长的绿光InGaN量子阱4的表面形貌是沿原子台阶分布的二维岛形貌,并且原子台阶宽度较大。在斜切角较大的衬底1上生长的绿光InGaN量子阱4的表面形貌是原子台阶流形貌,并且原子台阶宽度较小。It should be noted that the green light InGaN quantum well was used in this test. From the AFM topography test results in Figures 5(a) to 5(c), it can be seen that the surface topography of the green light InGaN quantum well 4 grown on the substrate 1 with a small chamfer angle is a two-dimensional distribution along the atomic steps. Viy island morphology, and the atomic step width is large. The surface morphology of the green light InGaN quantum well 4 grown on the substrate 1 with a larger chamfer angle is an atomic step flow morphology, and the atomic step width is small.

图6(a)是在斜切角度为0.2°的GaN衬底上形成的InGaN量子阱的变温PL测试结果曲线图。图6(b)是在斜切角度为0.56°的GaN衬底上形成的绿光InGaN量子阱的变温PL测试结果曲线图。其中,横坐标表示的是1000除以温度的数值,纵坐标表示的是PL积分强度。FIG. 6( a ) is a graph showing the result of a variable temperature PL test of an InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.2°. Fig. 6(b) is a graph showing the result of a variable temperature PL test of a green light InGaN quantum well formed on a GaN substrate with a chamfer angle of 0.56°. Among them, the abscissa represents the value of 1000 divided by the temperature, and the ordinate represents the PL integral intensity.

结合图6(a)和图6(b)可以看出,当斜切角从0.2°增加到0.56°,绿光InGaN量子阱4的内量子效率(IQE)从0.67%增加到3.5%。因此采用斜切角大于0.2°的衬底1生长绿光InGaN量子阱4可以有效提高绿光InGaN量子阱4的内量子效率。6(a) and 6(b), it can be seen that when the chamfer angle increases from 0.2° to 0.56°, the internal quantum efficiency (IQE) of the green InGaN quantum well 4 increases from 0.67% to 3.5%. Therefore, using the substrate 1 with the chamfer angle greater than 0.2° to grow the green light InGaN quantum well 4 can effectively improve the internal quantum efficiency of the green light InGaN quantum well 4 .

综上所述,根据本发明的实施例,采用斜切角大于0.2°的衬底生长绿光或更长波长InGaN量子阱有源区,可以实现绿光或更长波长InGaN量子阱的原子台阶流生长,改善其形貌,并提高InGaN量子阱的内量子效率。此外,通过上述方法制备得到的InGaN量子阱既可以广泛应用于GaN基绿光或更长波长LED、GaN基绿光或更长波长激光器中,也可以广泛应用于多量子阱太阳能电池中。To sum up, according to the embodiments of the present invention, using a substrate with a chamfer angle greater than 0.2° to grow green light or longer wavelength InGaN quantum well active regions can realize the atomic steps of green light or longer wavelength InGaN quantum wells flow growth, improve its morphology, and increase the internal quantum efficiency of InGaN quantum wells. In addition, the InGaN quantum well prepared by the above method can be widely used not only in GaN-based green light or longer wavelength LEDs, GaN-based green light or longer wavelength lasers, but also in multi-quantum well solar cells.

虽然已经参照特定实施例示出并描述了本发明,但是本领域的技术人员将理解:在不脱离由权利要求及其等同物限定的本发明的精神和范围的情况下,可在此进行形式和细节上的各种变化。While the invention has been shown and described with reference to specific embodiments, those skilled in the art will appreciate that forms and Various changes in details.

Claims (10)

1.一种提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,包括:1. a method of improving green light or longer wavelength InGaN quantum well luminous efficiency, is characterized in that, comprises: 采用一具有原子台阶的衬底,所述衬底上相邻原子台阶形成的斜切角为0.2~0.7°;A substrate with atomic steps is used, and the chamfer angle formed by adjacent atomic steps on the substrate is 0.2-0.7°; 在所述原子台阶面上形成缓冲层;forming a buffer layer on the atomic step surface; 在所述缓冲层上形成高温n型GaN层;forming a high temperature n-type GaN layer on the buffer layer; 在所述高温n型GaN层上形成InGaN量子阱;forming an InGaN quantum well on the high temperature n-type GaN layer; 其中,所述InGaN量子阱的发光波长不小于520nm,所述InGaN量子阱的In组分不小于25%,所述在所述高温n型GaN层上形成InGaN量子阱的生长方法是MOCVD。Wherein, the emission wavelength of the InGaN quantum well is not less than 520 nm, the In composition of the InGaN quantum well is not less than 25%, and the growth method for forming the InGaN quantum well on the high temperature n-type GaN layer is MOCVD. 2.根据权利要求1所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,每相邻两个原子台阶形成的斜切角相等。2 . The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to claim 1 , wherein the chamfer angles formed by every two adjacent atomic steps are equal. 3 . 3.根据权利要求1所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,所述缓冲层为低温不掺杂GaN层,所述低温不掺杂GaN层的厚度为10nm~30nm。3. The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to claim 1, wherein the buffer layer is a low temperature undoped GaN layer, and the thickness of the low temperature undoped GaN layer is It is 10nm~30nm. 4.根据权利要求1所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,所述高温n型GaN层的厚度小于5000nm。4 . The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to claim 1 , wherein the thickness of the high temperature n-type GaN layer is less than 5000 nm. 5 . 5.根据权利要求1所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,所述高温n型GaN层的电子浓度在1017cm-3到1019cm-3之间。5. The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to claim 1, wherein the electron concentration of the high temperature n-type GaN layer is 10 17 cm -3 to 10 19 cm -3 between. 6.根据权利要求1所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,所述InGaN量子阱为不掺杂的InxGa1-xN量子阱。6. The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to claim 1, wherein the InGaN quantum wells are undoped InxGa1 - xN quantum wells. 7.根据权利要求6所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,所述InxGa1-xN量子阱的厚度为1nm~5nm,且所述InxGa1-xN量子阱的In组分随InGaN量子阱发光波长的增加而增大。7 . The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to claim 6 , wherein the InxGa1 - xN quantum well has a thickness of 1 nm to 5 nm, and the In The In composition of the xGa1 - xN quantum well increases with the increase of the emission wavelength of the InGaN quantum well. 8.根据权利要求1至7任一项所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,每一级原子台阶上形成的InGaN量子阱呈原子台阶流形貌。8. The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to any one of claims 1 to 7, wherein the InGaN quantum wells formed on each level of atomic steps are in atomic step flow morphology . 9.根据权利要求1至7任一项所述的提高绿光或更长波长InGaN量子阱发光效率的方法,其特征在于,所述InGaN量子阱的高度与相邻高一级原子台阶的高度相等。9. The method for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells according to any one of claims 1 to 7, wherein the height of the InGaN quantum wells is the same as the height of an adjacent higher atomic step equal. 10.一种利用权利要求1至9任一项所述的方法来提高绿光或更长波长InGaN量子阱发光效率的结构,其特征在于,包括:10. A structure for improving the luminous efficiency of green light or longer wavelength InGaN quantum wells using the method according to any one of claims 1 to 9, characterized in that, comprising: 衬底,具有原子台阶,且相邻原子台阶形成的斜切角大于0.2°;A substrate with atomic steps, and the chamfer angle formed by adjacent atomic steps is greater than 0.2°; 缓冲层,形成在所述原子台阶面上;a buffer layer, formed on the atomic step surface; 高温n型GaN层,形成在所述缓冲层上;a high temperature n-type GaN layer formed on the buffer layer; InGaN量子阱,形成在所述高温n型GaN层上。InGaN quantum wells are formed on the high temperature n-type GaN layer.
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