CN110718612A - Light emitting diode epitaxial wafer and manufacturing method thereof - Google Patents
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Abstract
本发明公开了一种发光二极管外延片及其制造方法,属于半导体技术领域。发光二极管外延片的多量子阱层的每个量子阱层均包括依次层叠的第一量子阱子层、第二量子阱子层和第三量子阱子层,第二量子阱子层的In/Ga比大于等于第一量子阱子层和第三量子阱子层的In/Ga比;第一量子阱子层中掺有Si;每个量子垒层均包括依次层叠的第一量子垒子层、第二量子垒子层和第三量子垒子层;第二量子垒子层的Si/Ga比大于等于第一量子垒子层和第三量子垒子层的Si/Ga比。该发光二极管外延片可以改善多量子阱层中的能带倾斜现象,增加电子和空穴的波函数在空间分布上的重叠度,提高LED的内量子效率。
The invention discloses a light-emitting diode epitaxial wafer and a manufacturing method thereof, belonging to the technical field of semiconductors. Each quantum well layer of the multiple quantum well layer of the light-emitting diode epitaxial wafer includes a first quantum well sublayer, a second quantum well sublayer and a third quantum well sublayer that are stacked in sequence, and the In/ The Ga ratio is greater than or equal to the In/Ga ratio of the first quantum well sublayer and the third quantum well sublayer; the first quantum well sublayer is doped with Si; each quantum barrier layer includes sequentially stacked first quantum barrier sublayers , the second quantum barrier sublayer and the third quantum barrier sublayer; the Si/Ga ratio of the second quantum barrier sublayer is greater than or equal to the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer. The light emitting diode epitaxial wafer can improve the energy band inclination phenomenon in the multiple quantum well layer, increase the overlapping degree of the wave functions of electrons and holes in the spatial distribution, and improve the internal quantum efficiency of the LED.
Description
技术领域technical field
本发明涉及半导体技术领域,特别涉及一种发光二极管外延片及其制造方法。The present invention relates to the technical field of semiconductors, in particular to a light emitting diode epitaxial wafer and a manufacturing method thereof.
背景技术Background technique
GaN(氮化镓)是制作LED(Light Emitting Diode,发光二极管)外延片的材料之一,GaN是极稳定的化合物和坚硬的高熔点材料,也是直接迁跃的宽带隙半导体材料,不仅具有良好的物理和化学性质,而且具有电子饱和速率高。热导率好、宽带禁度大和介电常数小等特点和强的抗辐照能力,可以用来制备稳定性能好,寿命长、耐腐蚀和耐高温的大功率器件。GaN (gallium nitride) is one of the materials for making LED (Light Emitting Diode, light emitting diode) epitaxial wafers. GaN is an extremely stable compound and a hard high melting point material, and is also a direct transition wide band gap semiconductor material. physical and chemical properties, and has a high electron saturation rate. It has the characteristics of good thermal conductivity, large broadband forbidden and small dielectric constant and strong anti-irradiation ability, which can be used to prepare high-power devices with good stability, long life, corrosion resistance and high temperature resistance.
通常,GaN基LED在蓝宝石衬底上进行外延生长。传统的GaN基LED外延结构一般采用InGaN/GaN超晶格结构作用多量子阱层。但是InGaN层和GaN层之间存在着很大的晶格失配,导致InGaN层和GaN层之间存在较大的压应力。压应力会产生压电极化电场,使得电子和空穴波函数的交叠减少,导致多量子阱层的能带倾斜,造成内量子效率的下降,从而影响LED发光效率。Typically, GaN-based LEDs are epitaxially grown on sapphire substrates. Traditional GaN-based LED epitaxial structures generally use InGaN/GaN superlattice structures as multiple quantum well layers. However, there is a large lattice mismatch between the InGaN layer and the GaN layer, resulting in a large compressive stress between the InGaN layer and the GaN layer. The compressive stress will generate a piezoelectric polarization electric field, which reduces the overlap of the wave functions of electrons and holes, leading to the inclination of the energy band of the multiple quantum well layer, resulting in a decrease in the internal quantum efficiency, thus affecting the luminous efficiency of LEDs.
发明内容SUMMARY OF THE INVENTION
本发明实施例提供了一种发光二极管外延片及其制造方法,可以改善多量子阱层中的能带倾斜现象,增加电子和空穴的波函数在空间分布上的重叠度,提高LED的内量子效率。所述技术方案如下:The embodiments of the present invention provide a light-emitting diode epitaxial wafer and a manufacturing method thereof, which can improve the energy band tilt phenomenon in the multiple quantum well layer, increase the overlap of the wave functions of electrons and holes in the spatial distribution, and improve the internal efficiency of the LED. quantum efficiency. The technical solution is as follows:
一方面,提供了一种发光二极管外延片,所述发光二极管外延片包括衬底、以及依次层叠在所述衬底上的缓冲层、未掺杂的GaN层、N型层、多量子阱层、电子阻挡层、P型层和P型接触层,所述多量子阱层包括交替生长的量子阱层和量子垒层,In one aspect, a light-emitting diode epitaxial wafer is provided, the light-emitting diode epitaxial wafer includes a substrate, and a buffer layer, an undoped GaN layer, an N-type layer, and a multiple quantum well layer sequentially stacked on the substrate , an electron blocking layer, a P-type layer and a P-type contact layer, the multiple quantum well layer comprising alternately grown quantum well layers and quantum barrier layers,
每个所述量子阱层均包括依次层叠的第一量子阱子层、第二量子阱子层和第三量子阱子层,所述第一量子阱子层、第二量子阱子层和第三量子阱子层均为InGaN层,所述第二量子阱子层的In/Ga比大于等于所述第一量子阱子层和所述第三量子阱子层的In/Ga比;所述第一量子阱子层中掺有Si,所述第一量子阱子层中Si的掺杂浓度为1*1017cm-3~3*1017cm-3;Each of the quantum well layers includes a first quantum well sublayer, a second quantum well sublayer and a third quantum well sublayer stacked in sequence, the first quantum well sublayer, the second quantum well sublayer and the third quantum well sublayer The three quantum well sublayers are all InGaN layers, and the In/Ga ratio of the second quantum well sublayer is greater than or equal to the In/Ga ratio of the first quantum well sublayer and the third quantum well sublayer; the The first quantum well sublayer is doped with Si, and the doping concentration of Si in the first quantum well sublayer is 1*10 17 cm -3 to 3*10 17 cm -3 ;
每个所述量子垒层均包括依次层叠的第一量子垒子层、第二量子垒子层和第三量子垒子层,所述第一量子垒子层、第二量子垒子层和第三量子垒子层均为掺Si的GaN层,所述量子垒子层中Si的掺杂浓度为3*1017cm-3~5*1017cm-3;所述第二量子垒子层的Si/Ga比大于等于所述第一量子垒子层和所述第三量子垒子层的Si/Ga比。Each of the quantum barrier layers includes a first quantum barrier sublayer, a second quantum barrier sublayer and a third quantum barrier sublayer stacked in sequence, the first quantum barrier sublayer, the second quantum barrier sublayer and the third quantum barrier sublayer The three quantum barrier sublayers are all Si-doped GaN layers, and the doping concentration of Si in the quantum barrier sublayer is 3*10 17 cm -3 to 5*10 17 cm -3 ; the second quantum barrier sublayer The Si/Ga ratio of is greater than or equal to the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer.
进一步地,所述第一量子阱子层、第二量子阱子层和第三量子阱子层的厚度比为1:m:1,4≤m≤6,m为正整数。Further, the thickness ratio of the first quantum well sublayer, the second quantum well sublayer and the third quantum well sublayer is 1:m:1, 4≤m≤6, and m is a positive integer.
进一步地,所述第一量子垒子层、第二量子垒子层和第三量子垒子层的厚度比为1:n:1,4≤n≤6,n为正整数。Further, the thickness ratio of the first quantum barrier sublayer, the second quantum barrier sublayer and the third quantum barrier sublayer is 1:n:1, 4≤n≤6, and n is a positive integer.
进一步地,所述第一量子垒子层的Si/Ga比随着厚度的增加而逐渐增加,所述第二量子垒子层的Si/Ga比恒定不变,所述第三量子垒子层的Si/Ga比随着厚度的增加而逐渐减少。Further, the Si/Ga ratio of the first quantum barrier sublayer gradually increases with the increase of the thickness, the Si/Ga ratio of the second quantum barrier sublayer is constant, and the third quantum barrier sublayer The Si/Ga ratio gradually decreases with increasing thickness.
进一步地,所述第一量子阱子层的Si/Ga比随着厚度的增加而逐渐减少。Further, the Si/Ga ratio of the first quantum well sublayer gradually decreases as the thickness increases.
进一步地,所述第一量子阱子层的Si/Ga比的最大值为所述第二量子垒子层的Si/Ga比的20~30%,所述第一量子垒子层的Si/Ga比的最小值为所述第二量子垒子层的Si/Ga比的20~30%,所述第三量子垒子层的Si/Ga比的最小值为所述第二量子垒子层的Si/Ga比的20~30%。Further, the maximum value of the Si/Ga ratio of the first quantum well sublayer is 20-30% of the Si/Ga ratio of the second quantum barrier sublayer, and the Si/Ga ratio of the first quantum barrier sublayer is 20-30%. The minimum value of the Ga ratio is 20-30% of the Si/Ga ratio of the second quantum barrier sublayer, and the minimum value of the Si/Ga ratio of the third quantum barrier sublayer is the second quantum barrier sublayer 20 to 30% of the Si/Ga ratio.
另一方面,提供了一种发光二极管外延片的制造方法,所述制造方法包括:In another aspect, a method for manufacturing a light-emitting diode epitaxial wafer is provided, the manufacturing method comprising:
提供一衬底;providing a substrate;
在所述衬底上依次生长低温缓冲层、未掺杂的GaN层、N型层、多量子阱层、电子阻挡层、P型层和P型接触层;growing a low temperature buffer layer, an undoped GaN layer, an N-type layer, a multiple quantum well layer, an electron blocking layer, a P-type layer and a P-type contact layer on the substrate in sequence;
其中,所述多量子阱层包括交替生长的量子阱层和量子垒层,每个所述量子阱层均包括依次层叠的第一量子阱子层、第二量子阱子层和第三量子阱子层,所述第一量子阱子层、第二量子阱子层和第三量子阱子层均为InGaN层,所述第二量子阱子层的In/Ga比大于所述第一量子阱子层和所述第三量子阱子层的In/Ga比;所述第一量子阱子层中掺有Si,所述第一量子阱子层中Si的掺杂浓度为1*1017cm-3~3*1017cm-3;The multiple quantum well layers include alternately grown quantum well layers and quantum barrier layers, and each of the quantum well layers includes a first quantum well sublayer, a second quantum well sublayer and a third quantum well layered in sequence sublayer, the first quantum well sublayer, the second quantum well sublayer and the third quantum well sublayer are all InGaN layers, and the In/Ga ratio of the second quantum well sublayer is greater than that of the first quantum well In/Ga ratio of the sublayer and the third quantum well sublayer; Si is doped in the first quantum well sublayer, and the doping concentration of Si in the first quantum well sublayer is 1*10 17 cm -3 to 3*10 17 cm -3 ;
每个所述量子垒层均包括依次层叠的第一量子垒子层、第二量子垒子层和第三量子垒子层,所述第一量子垒子层、第二量子垒子层和第三量子垒子层均为掺Si的GaN层,所述量子垒子层中Si的掺杂浓度为3*1017cm-3~5*1017cm-3;所述第二量子垒子层的Si/Ga比大于所述第一量子垒子层和所述第三量子垒子层的Si/Ga比。Each of the quantum barrier layers includes a first quantum barrier sublayer, a second quantum barrier sublayer and a third quantum barrier sublayer stacked in sequence, the first quantum barrier sublayer, the second quantum barrier sublayer and the third quantum barrier sublayer The three quantum barrier sublayers are all Si-doped GaN layers, and the doping concentration of Si in the quantum barrier sublayer is 3*10 17 cm -3 to 5*10 17 cm -3 ; the second quantum barrier sublayer The Si/Ga ratio of is greater than the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer.
进一步地,所述第一量子阱子层和所述第三量子阱子层的生长温度均大于等于所述第二量子阱子层的生长温度。Further, the growth temperature of the first quantum well sublayer and the third quantum well sublayer are both greater than or equal to the growth temperature of the second quantum well sublayer.
进一步地,所述第一量子垒子层和所述第三量子垒子层的生长温度均小于等于所述第二量子垒子层的生长温度。Further, the growth temperatures of the first quantum barrier sublayer and the third quantum barrier sublayer are both less than or equal to the growth temperature of the second quantum barrier sublayer.
进一步地,所述第一量子阱子层的Si/Ga比随着厚度的增加而逐渐减少。Further, the Si/Ga ratio of the first quantum well sublayer gradually decreases as the thickness increases.
本发明实施例提供的技术方案带来的有益效果是:The beneficial effects brought by the technical solutions provided in the embodiments of the present invention are:
通过将各个量子阱层分成三个子层,且第二量子阱子层的In/Ga比大于等于第一量子阱子层和第三量子阱子层的In/Ga比,因此,第二量子阱子层中的In含量较高,可以作为主要发光层,保证LED的发光效率。第一量子阱子层和第三量子阱子层中的In含量较低,且与量子垒层接触,可以减小量子阱层和量子垒层之间的晶格失配,从而减少压应力。同时,第一量子阱子层中掺有少量Si,可以增加量子阱层中的电子浓度,从而改善多量子阱层的能带倾斜现象,增加电子和空穴的波函数在空间分布上的重叠度,提高LED的内量子效率。且由于Si为杂质,在量子阱层中掺Si会影响阱层的晶体质量,而第一量子阱子层并非主要的发光层,因此,在第一量子阱子层中掺Si,可以减少Si杂质掺杂对阱层晶体质量的影响,从而保证阱层的发光效率。进一步地,通过将量子垒层分成三个子层,且第二量子垒子层的Si/Ga比大于等于第一量子垒子层和第三量子垒子层的Si/Ga比,即与量子阱层接触的第一量子垒子层和第三量子垒子层中的Si的掺杂浓度较少,可以保证第一量子垒子层和第三量子垒子层的晶体质量,从而提高阱垒之间的界面质量,进而可以进一步提高LED的发光效率。By dividing each quantum well layer into three sublayers, and the In/Ga ratio of the second quantum well sublayer is greater than or equal to the In/Ga ratio of the first quantum well sublayer and the third quantum well sublayer, therefore, the second quantum well The In content in the sublayer is relatively high, which can be used as the main light-emitting layer to ensure the light-emitting efficiency of the LED. The content of In in the first quantum well sublayer and the third quantum well sublayer is low, and they are in contact with the quantum barrier layer, which can reduce the lattice mismatch between the quantum well layer and the quantum barrier layer, thereby reducing compressive stress. At the same time, the first quantum well sublayer is doped with a small amount of Si, which can increase the electron concentration in the quantum well layer, thereby improving the energy band tilt phenomenon of the multiple quantum well layer and increasing the overlap of the spatial distribution of the wave functions of electrons and holes. degree, improve the internal quantum efficiency of LED. And since Si is an impurity, doping Si in the quantum well layer will affect the crystal quality of the well layer, and the first quantum well sublayer is not the main light-emitting layer. Therefore, doping Si in the first quantum well sublayer can reduce Si. The influence of impurity doping on the crystal quality of the well layer ensures the luminous efficiency of the well layer. Further, by dividing the quantum barrier layer into three sublayers, and the Si/Ga ratio of the second quantum barrier sublayer is greater than or equal to the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer, that is, the same as the quantum well. The doping concentration of Si in the first quantum barrier sublayer and the third quantum barrier sublayer in contact with each other is less, which can ensure the crystal quality of the first quantum barrier sublayer and the third quantum barrier sublayer, thereby improving the well barrier. The interface quality between the two can further improve the luminous efficiency of the LED.
附图说明Description of drawings
为了更清楚地说明本发明实施例中的技术方案,下面将对实施例描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to illustrate the technical solutions in the embodiments of the present invention more clearly, the following briefly introduces the accompanying drawings used in the description of the embodiments. Obviously, the accompanying drawings in the following description are only some embodiments of the present invention. For those of ordinary skill in the art, other drawings can also be obtained from these drawings without creative effort.
图1是本发明实施例提供的一种发光二极管外延片的结构示意图;1 is a schematic structural diagram of a light-emitting diode epitaxial wafer provided by an embodiment of the present invention;
图2是本发明实施例提供的一种多量子阱层的结构示意图;2 is a schematic structural diagram of a multiple quantum well layer provided by an embodiment of the present invention;
图3是本发明实施例提供的一种发光二极管外延片的制造方法的方法流程图;3 is a method flowchart of a method for manufacturing a light-emitting diode epitaxial wafer provided by an embodiment of the present invention;
图4是现有的多量子阱层的能带示意图;Fig. 4 is the energy band schematic diagram of the existing multiple quantum well layer;
图5是本发明实施例提供的多量子阱层的能带示意图。FIG. 5 is a schematic diagram of an energy band of a multiple quantum well layer provided by an embodiment of the present invention.
具体实施方式Detailed ways
为使本发明的目的、技术方案和优点更加清楚,下面将结合附图对本发明实施方式作进一步地详细描述。In order to make the objectives, technical solutions and advantages of the present invention clearer, the embodiments of the present invention will be further described in detail below with reference to the accompanying drawings.
本发明实施例提供了一种发光二极管外延片,图1是本发明实施例提供的一种发光二极管外延片的结构示意图,如图1所示,发光二极管外延片包括衬底1、以及依次层叠在衬底1上的缓冲层2、未掺杂的GaN层3、N型层4、多量子阱层5、低温P型层6、电子阻挡层7、高温P型层8和P型接触层9。An embodiment of the present invention provides a light-emitting diode epitaxial wafer. FIG. 1 is a schematic structural diagram of a light-emitting diode epitaxial wafer provided by an embodiment of the present invention. As shown in FIG. 1 , the light-emitting diode epitaxial wafer includes a
图2是本发明实施例提供的一种多量子阱层的结构示意图,如图2所示,多量子阱层5包括交替生长的多个量子阱层51和多个量子垒层52。2 is a schematic structural diagram of a multiple quantum well layer provided by an embodiment of the present invention. As shown in FIG. 2 , the multiple
每个量子阱层51均包括依次层叠的第一量子阱子层511、第二量子阱子层512和第三量子阱子层513。第一量子阱子层511、第二量子阱子层512和第三量子阱子层513均为InGaN层。第二量子阱子层512的In/Ga比大于等于第一量子阱子层511和第三量子阱子层513的In/Ga比。第一量子阱子层511中掺有Si,第一量子阱子层511中Si的掺杂浓度为1*1017cm-3~3*1017cm-3。Each
每个量子垒层52均包括依次层叠的第一量子垒子层521、第二量子垒子层522和第三量子垒子层523,第一量子垒子层521、第二量子垒子层522和第三量子垒子层523均为掺Si的GaN层,量子垒子层中Si的掺杂浓度为3*1017cm-3~5*1017cm-3;第二量子垒子层522的Si/Ga比大于等于第一量子垒子层521和第三量子垒子层523的Si/Ga比。Each
需要说明的是,In/Ga比表示In的掺杂浓度和Ga的掺杂浓度的比值,Si/Ga比表示Si的掺杂浓度和Ga的掺杂浓度的比值。在本实施例中,各个量子阱子层和各个量子垒子层中的Ga的掺杂浓度相等。It should be noted that the In/Ga ratio represents the ratio of the doping concentration of In and the doping concentration of Ga, and the Si/Ga ratio represents the ratio of the doping concentration of Si and the doping concentration of Ga. In this embodiment, the doping concentrations of Ga in each quantum well sublayer and each quantum barrier sublayer are equal.
本发明实施例通过将各个量子阱层分成三个子层,且第二量子阱子层的In/Ga比大于等于第一量子阱子层和第三量子阱子层的In/Ga比,因此,第二量子阱子层中的In含量较高,可以作为主要发光层,保证LED的发光效率。第一量子阱子层和第三量子阱子层中的In含量较低,且与量子垒层接触,可以减小量子阱层和量子垒层之间的晶格失配,从而减少压应力。同时,第一量子阱子层中掺有少量Si,可以增加量子阱层中的电子浓度,从而改善多量子阱层的能带倾斜现象,增加电子和空穴的波函数在空间分布上的重叠度,提高LED的内量子效率。且由于Si为杂质,在量子阱层中掺Si会影响阱层的晶体质量,而第一量子阱子层并非主要的发光层,因此,在第一量子阱子层中掺Si,可以减少Si杂质掺杂对阱层晶体质量的影响,从而保证阱层的发光效率。进一步地,通过将量子垒层分成三个子层,且第二量子垒子层的Si/Ga比大于等于第一量子垒子层和第三量子垒子层的Si/Ga比,即与量子阱层接触的第一量子垒子层和第三量子垒子层中的Si的掺杂浓度较少,可以保证第一量子垒子层和第三量子垒子层的晶体质量,从而提高阱垒之间的界面质量,进而可以进一步提高LED的发光效率。In the embodiment of the present invention, each quantum well layer is divided into three sublayers, and the In/Ga ratio of the second quantum well sublayer is greater than or equal to the In/Ga ratio of the first quantum well sublayer and the third quantum well sublayer. Therefore, The In content in the second quantum well sublayer is relatively high, which can be used as the main light-emitting layer to ensure the light-emitting efficiency of the LED. The content of In in the first quantum well sublayer and the third quantum well sublayer is low, and they are in contact with the quantum barrier layer, which can reduce the lattice mismatch between the quantum well layer and the quantum barrier layer, thereby reducing compressive stress. At the same time, the first quantum well sublayer is doped with a small amount of Si, which can increase the electron concentration in the quantum well layer, thereby improving the energy band tilt phenomenon of the multiple quantum well layer and increasing the overlap of the spatial distribution of the wave functions of electrons and holes. degree, improve the internal quantum efficiency of LED. And since Si is an impurity, doping Si in the quantum well layer will affect the crystal quality of the well layer, and the first quantum well sublayer is not the main light-emitting layer. Therefore, doping Si in the first quantum well sublayer can reduce Si. The influence of impurity doping on the crystal quality of the well layer ensures the luminous efficiency of the well layer. Further, by dividing the quantum barrier layer into three sublayers, and the Si/Ga ratio of the second quantum barrier sublayer is greater than or equal to the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer, that is, the same as the quantum well. The doping concentration of Si in the first quantum barrier sublayer and the third quantum barrier sublayer in contact with each other is less, which can ensure the crystal quality of the first quantum barrier sublayer and the third quantum barrier sublayer, thereby improving the well barrier. The interface quality between the two can further improve the luminous efficiency of the LED.
在本实施例中,多量子阱层5可以包括交替生长的8~15个量子阱层51和8~15个量子垒层52。In this embodiment, the multiple
进一步地,第一量子阱子层511、第二量子阱子层512和第三量子阱子层513的厚度比为1:m:1,4≤m≤6,m为正整数。由于第二量子阱子层为主要发光层,因此,将第二量子阱子层的厚度设置的较厚,可以保证各个量子阱层的发光亮度。同时将第一量子阱子层设置的较薄,可以防止第一量子阱子层中掺入Si杂质,对整个阱层的晶体质量产生影响。Further, the thickness ratio of the first quantum well sublayer 511 , the second quantum well sublayer 512 and the third quantum well sublayer 513 is 1:m:1, 4≤m≤6, and m is a positive integer. Since the second quantum well sublayer is the main light-emitting layer, setting the thickness of the second quantum well sublayer to be thick can ensure the light-emitting brightness of each quantum well layer. At the same time, setting the first quantum well sub-layer to be thinner can prevent Si impurities from being doped into the first quantum well sub-layer, which affects the crystal quality of the entire well layer.
需要说明的是,第一量子阱子层511、第二量子阱子层512和第三量子阱子层513的具体厚度比可以根据所需LED器件的发光波长大小选取。发光波长越长,需要的量子阱层In总量越多,第二量子阱子层的厚度可以设置的越厚。发光越长越短,需要的量子阱层In总量越少,第二量子阱子层的厚度可以设置的越薄。It should be noted that the specific thickness ratio of the first quantum well sublayer 511 , the second quantum well sublayer 512 and the third quantum well sublayer 513 can be selected according to the light emission wavelength of the desired LED device. The longer the light emission wavelength is, the more the total amount of In of the quantum well layer is required, and the thicker the thickness of the second quantum well sublayer can be set. The longer and shorter the light emission is, the less the total amount of In of the quantum well layer is required, and the thinner the thickness of the second quantum well sublayer can be set.
示例性地,当所需LED器件的发光波长为460nm~470nm时,可以将第一子层511、第二子层512和第三子层513的厚度比设置为1:4:1。当所需LED器件的发光波长为515nm~525nm时,可以将第一子层511、第二子层512和第三子层513的厚度比设置为1:5:1。当所需LED器件的发光波长为520nm~530nm时,可以将第一子层511、第二子层512和第三子层513的厚度比设置为1:6:1。Exemplarily, when the light emission wavelength of the desired LED device is 460 nm˜470 nm, the thickness ratio of the first sublayer 511 , the second sublayer 512 and the third sublayer 513 may be set to 1:4:1. When the light emission wavelength of the desired LED device is 515 nm˜525 nm, the thickness ratio of the first sublayer 511 , the second sublayer 512 and the third sublayer 513 may be set to 1:5:1. When the emission wavelength of the desired LED device is 520 nm˜530 nm, the thickness ratio of the first sublayer 511 , the second sublayer 512 and the third sublayer 513 may be set to 1:6:1.
可选地,各个量子阱层51的总厚度可以为2~3nm。若量子阱层51的厚度小于2nm,则可能由于量子阱层51的厚度太小而影响到量子阱层51中电子和空穴的复合发光,降低LED的发光效率。如果量子阱层51的厚度大于3nm,则可能由于量子阱层51的厚度太大而造成量子阱层51中产生更多的应力,影响量子阱层51的晶体质量从而影响LED的发光效率。Optionally, the total thickness of each
进一步地,第一量子垒子层521、第二量子垒子层522和第三量子垒子层523的厚度比为1:n:1,4≤n≤6,n为正整数。由于第二量子垒子层中Si的掺杂浓度最高,因此,第二量子垒子层可以作为主要的阻挡层,阻挡电子溢流。因此,将第二量子垒层的厚度设置的较厚,可以减少电子溢流。Further, the thickness ratio of the first quantum barrier sublayer 521 , the second quantum barrier sublayer 522 and the third quantum barrier sublayer 523 is 1:n:1, 4≤n≤6, and n is a positive integer. Since the doping concentration of Si in the second quantum barrier sublayer is the highest, the second quantum barrier sublayer can act as a main blocking layer to block electron overflow. Therefore, by setting the thickness of the second quantum barrier layer to be thick, the overflow of electrons can be reduced.
可选地,各个量子垒层52的总厚度可以为9~20nm。若量子垒层52的厚度小于9nm,则可能由于量子垒层52的厚度太小而起不到阻挡电子溢流的效果。若量子垒层52的厚度大于20nm,又很容易影响到载流子正常的迁移,对电子和空穴的复合起到阻挡作用,降低LED的发光效率。Optionally, the total thickness of each
进一步地,第一量子垒子层521的Si/Ga比随着厚度的增加而逐渐增加,第二量子垒子层522的Si/Ga比恒定不变,第三量子垒子层521的Si/Ga比随着厚度的增加而逐渐减少。则第一量子垒子层中的Si的掺杂浓度逐渐增加,第一量子垒子层中与量子阱层接触的部分的Si的掺杂浓度较少,有利于提高阱垒之间的界面质量。同样地,第三量子垒子层中与量子阱层接触的部分的Si的掺杂浓度逐渐较少,有利于有利于提高阱垒之间的界面质量。Further, the Si/Ga ratio of the first quantum barrier sublayer 521 gradually increases as the thickness increases, the Si/Ga ratio of the second quantum barrier sublayer 522 is constant, and the Si/Ga ratio of the third quantum barrier sublayer 521 is constant. The Ga ratio gradually decreases with increasing thickness. Then the doping concentration of Si in the first quantum barrier sublayer gradually increases, and the doping concentration of Si in the part in contact with the quantum well layer in the first quantum barrier sublayer is less, which is beneficial to improve the interface quality between the well barriers. . Similarly, the doping concentration of Si in the portion of the third quantum barrier sublayer in contact with the quantum well layer is gradually reduced, which is beneficial to improve the interface quality between the well barriers.
在本实施例中,第一量子垒子层511的Si/Ga比逐渐增加至第二量子垒子层512的Si/Ga比,第三量子垒子层513的Si/Ga比由第二量子垒子层的Si/Ga比逐渐减少,以形成平滑过渡。In this embodiment, the Si/Ga ratio of the first quantum barrier sublayer 511 is gradually increased to the Si/Ga ratio of the second quantum barrier sublayer 512, and the Si/Ga ratio of the third quantum barrier sublayer 513 is increased by the second quantum barrier sublayer 512. The Si/Ga ratio of the barrier layer is gradually reduced to form a smooth transition.
进一步地,第一量子阱子层511的Si/Ga比随着厚度的增加而逐渐减少。则第一量子阱子层511中靠近第二量子阱子层512的部分的Si的掺杂浓度较少,可以减少掺杂Si杂质对第二量子阱子层512所产生的影响。Further, the Si/Ga ratio of the first quantum well sublayer 511 gradually decreases as the thickness increases. Then, the doping concentration of Si in the portion of the first quantum well sublayer 511 close to the second quantum well sublayer 512 is less, which can reduce the influence of doping Si impurities on the second quantum well sublayer 512 .
可选地,第一量子阱子层的Si/Ga比的最大值为第二量子垒子层的Si/Ga比的20~30%。若第一量子阱子层中Si的掺杂浓度过低,则起不到改善阱层能带倾斜的作用,若第一量子阱子层中Si的掺杂浓度过高,则会影响量子阱层的晶体质量。Optionally, the maximum value of the Si/Ga ratio of the first quantum well sublayer is 20-30% of the Si/Ga ratio of the second quantum barrier sublayer. If the doping concentration of Si in the first quantum well sublayer is too low, the effect of improving the energy band inclination of the well layer cannot be achieved. If the doping concentration of Si in the first quantum well sublayer is too high, it will affect the quantum well. The crystal quality of the layer.
进一步地,第一量子垒子层的Si/Ga比的最小值为第二量子垒子层的Si/Ga比的20~30%,第三量子垒子层的Si/Ga比的最小值为第二量子垒子层的Si/Ga比的20~30%。此时即可以保证量子垒层能起到阻挡电子溢流的作用,又可以保证阱垒之间的界面质量。Further, the minimum value of the Si/Ga ratio of the first quantum barrier sublayer is 20-30% of the Si/Ga ratio of the second quantum barrier sublayer, and the minimum value of the Si/Ga ratio of the third quantum barrier sublayer is 20-30% of the Si/Ga ratio of the second quantum barrier layer. At this time, it can not only ensure that the quantum barrier layer can play a role in blocking electron overflow, but also can ensure the interface quality between the well barriers.
可选地,衬底1可以为蓝宝石衬底。Alternatively, the
可选地,缓冲层2可以为AlN层,厚度为15~35nm。Optionally, the
可选地,未掺杂的GaN层3的厚度为1~3um。Optionally, the thickness of the
可选地,N型层4可以为掺Si的GaN层,厚度为1~5um。Optionally, the N-
可选地,低温P型层6可以为掺Mg的GaN层,厚度为10~40nm。Optionally, the low-temperature P-
可选地,电子阻挡层7可以为掺Mg的AlGaN层,厚度为20~30nm,Mg的掺杂浓度小于1*1019cm-3。Optionally, the
可选地,P型层8可以为掺Mg的GaN层,厚度为10~30nm,Mg的掺杂浓度大于或等于1*1020cm-3。Optionally, the P-
可选地,P型接触层9可以为重掺杂Mg的GaN层,厚度为30~50nm,Mg的掺杂浓度大于或等于1*1020cm-3,Optionally, the P-type contact layer 9 may be a heavily Mg-doped GaN layer with a thickness of 30-50 nm, and the doping concentration of Mg is greater than or equal to 1*10 20 cm −3 ,
本发明实施例提供了一种发光二极管外延片的制造方法,用于制造实施例一提供的发光二极管外延片,图3是本发明实施例提供的一种发光二极管外延片的制造方法的方法流程图,如图3所示,该制造方法包括:An embodiment of the present invention provides a method for manufacturing a light-emitting diode epitaxial wafer, which is used to manufacture the light-emitting diode epitaxial wafer provided in the first embodiment. FIG. 3 is a method flow of the method for manufacturing a light-emitting diode epitaxial wafer provided by an embodiment of the present invention. Figure, as shown in Figure 3, the manufacturing method includes:
步骤301、提供一衬底。
在本实施例中,衬底为蓝宝石,可以将衬底放在石墨托盘上送入反应腔中进行外延材料的生长。In this embodiment, the substrate is sapphire, and the substrate can be placed on a graphite tray and sent into a reaction chamber to grow epitaxial materials.
步骤301还包括:Step 301 also includes:
控制反应室温度为1050℃,压力为200~500Torr,在纯氢气氛围对蓝宝石衬底进行退火处理5~6min,然后将蓝宝石衬底进行氮化处理。The temperature of the reaction chamber is controlled to be 1050° C., the pressure is 200 to 500 Torr, the sapphire substrate is annealed in a pure hydrogen atmosphere for 5 to 6 minutes, and then the sapphire substrate is subjected to nitridation treatment.
本发明运用Veeco EPIK700 MOCVD来生长高亮度GaN基LED外延片。采用高纯H2或高纯N2或高纯H2和高纯N2的混合气体作为载气,高纯NH3作为N源,三甲基镓(TMGa)及三乙基镓(TEGa)作为镓源,三甲基铟(TMIn)作为铟源,硅烷(SiH4)作为N型掺杂剂,三甲基铝(TMAl)作为铝源,二茂镁(CP2Mg)作为P型掺杂剂,衬底为(0001)面蓝宝石,反应室压力在50torr到600torr之间。The present invention uses Veeco EPIK700 MOCVD to grow high-brightness GaN-based LED epitaxial wafers. Use high-purity H2 or high-purity N2 or a mixture of high-purity H2 and high-purity N2 as the carrier gas, high-purity NH3 as the N source, trimethylgallium (TMGa) and triethylgallium (TEGa) as the gallium source, and three Methyl indium (TMIn) was used as the indium source, silane (SiH4) was used as the N-type dopant, trimethylaluminum (TMAl) was used as the aluminum source, and dicocene (CP 2 Mg) was used as the P-type dopant. The substrate was (0001) sapphire, the reaction chamber pressure is between 50torr and 600torr.
步骤302、在衬底上生长缓冲层。
其中,缓冲层为AlN层。The buffer layer is an AlN layer.
具体地,将衬底放置到PVD(Physical Vapor Deposition,物理气相沉积)设备的反应腔内,采用PVD法生长AlN缓冲层,包括:将PVD设备的反应腔内温度调整至400~700℃,溅射功率调整至3000~5000W,压力调整至为1~10mtorr,生长15~35nm厚的AlN缓冲层。Specifically, the substrate is placed in the reaction chamber of a PVD (Physical Vapor Deposition) equipment, and the AlN buffer layer is grown by the PVD method, including: adjusting the temperature in the reaction chamber of the PVD equipment to 400-700° C., sputtering The radiation power is adjusted to 3000-5000W, the pressure is adjusted to 1-10 mtorr, and an AlN buffer layer with a thickness of 15-35 nm is grown.
需要说明的是,外延层中的未掺杂的GaN层、N型层、多量子阱层、低温P型层、电子阻挡层、P型层以及P型接触层均可以采用MOCVD(Metal-organic Chemical VaporDeposition,金属有机化合物化学气相沉淀)法生长。在具体实现时,通常是将衬底放在石墨托盘上送入MOCVD设备的反应室中进行外延材料的生长,因此上述生长过程中控制的温度和压力实际上是指反应室内的温度和压力。具体地,采用三甲基镓或三甲基乙作为镓源,三乙基硼作为硼源,高纯氨气作为氮源,三甲基铟作为铟源,三甲基铝作为铝源,N型掺杂剂选用硅烷,P型掺杂剂选用二茂镁。It should be noted that MOCVD (Metal-organic Chemical VaporDeposition, metal organic compound chemical vapor deposition) method growth. In the specific implementation, the substrate is usually placed on a graphite tray and sent to the reaction chamber of the MOCVD equipment for the growth of the epitaxial material. Therefore, the temperature and pressure controlled in the above-mentioned growth process actually refer to the temperature and pressure in the reaction chamber. Specifically, trimethyl gallium or trimethyl ethyl is used as the gallium source, triethyl boron as the boron source, high-purity ammonia gas as the nitrogen source, trimethyl indium as the indium source, trimethyl aluminum as the aluminum source, N Silane is selected as the type dopant, and magnesium locene is selected as the P type dopant.
步骤303、在缓冲层上生长未掺杂的GaN层。
示例性地,将反应室温度控制在1000~1200℃,压力控制在100~500torr,生长厚度为1~3um的未掺杂的GaN层。Exemplarily, the temperature of the reaction chamber is controlled at 1000-1200° C., the pressure is controlled at 100-500 torr, and an undoped GaN layer with a thickness of 1-3um is grown.
步骤304、在未掺杂的GaN层上生长N型层。
其中,N型层为掺Si的GaN层,Si掺杂浓度可以为1018cm-3~1019cm-3。The N-type layer is a Si-doped GaN layer, and the Si doping concentration can be 10 18 cm -3 to 10 19 cm -3 .
示例性地,将反应室温度控制在1000~1200℃,压力控制在100~300torr,生长厚度为1~5um的N型GaN层。Exemplarily, the temperature of the reaction chamber is controlled at 1000-1200° C., the pressure is controlled at 100-300 torr, and an N-type GaN layer with a thickness of 1-5um is grown.
步骤305、在N型层上生长多量子阱层。
在本实施例中,多量子阱层5可以包括交替生长的8~15个量子阱层和8~15个量子垒层。In this embodiment, the multiple
每个量子阱层均包括依次层叠的第一量子阱子层、第二量子阱子层和第三量子阱子层。第一量子阱子层、第二量子阱子层和第三量子阱子层均为InGaN层,第二量子阱子层的In/Ga比大于等于第一量子阱子层和第三量子阱子层的In/Ga比。第一量子阱子层中掺有Si,第一量子阱子层中Si的掺杂浓度为1*1017cm-3~3*1017cm-3。Each quantum well layer includes a first quantum well sublayer, a second quantum well sublayer, and a third quantum well sublayer that are stacked in sequence. The first quantum well sublayer, the second quantum well sublayer and the third quantum well sublayer are all InGaN layers, and the In/Ga ratio of the second quantum well sublayer is greater than or equal to the first quantum well sublayer and the third quantum well sublayer The In/Ga ratio of the layer. The first quantum well sublayer is doped with Si, and the doping concentration of Si in the first quantum well sublayer is 1*10 17 cm -3 to 3*10 17 cm -3 .
每个量子垒层均包括依次层叠的第一量子垒子层、第二量子垒子层和第三量子垒子层。第一量子垒子层、第二量子垒子层和第三量子垒子层均为掺Si的GaN层,量子垒子层中Si的掺杂浓度为3*1017cm-3~5*1017cm-3。第二量子垒子层的Si/Ga比大于等于第一量子垒子层和第三量子垒子层的Si/Ga比。Each quantum barrier layer includes a first quantum barrier sublayer, a second quantum barrier sublayer and a third quantum barrier sublayer that are stacked in sequence. The first quantum barrier sublayer, the second quantum barrier sublayer and the third quantum barrier sublayer are all Si-doped GaN layers, and the doping concentration of Si in the quantum barrier sublayer is 3*10 17 cm -3 to 5*10 17 cm -3 . The Si/Ga ratio of the second quantum barrier sublayer is greater than or equal to the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer.
需要说明的是,In/Ga比表示In的掺杂浓度和Ga的掺杂浓度的比值,Si/Ga比表示Si的掺杂浓度和Ga的掺杂浓度的比值。在本实施例中,各个量子阱子层和各个量子垒子层中的Ga的掺杂浓度相等。It should be noted that the In/Ga ratio represents the ratio of the doping concentration of In and the doping concentration of Ga, and the Si/Ga ratio represents the ratio of the doping concentration of Si and the doping concentration of Ga. In this embodiment, the doping concentrations of Ga in each quantum well sublayer and each quantum barrier sublayer are equal.
进一步地,第一量子阱子层、第二量子阱子层和第三量子阱子层的厚度比为1:m:1,4≤m≤6,m为正整数。Further, the thickness ratio of the first quantum well sublayer, the second quantum well sublayer and the third quantum well sublayer is 1:m:1, 4≤m≤6, and m is a positive integer.
可选地,各个量子阱层的总厚度可以为2~3nm。Optionally, the total thickness of each quantum well layer may be 2˜3 nm.
需要说明的是,第一量子阱子层、第二量子阱子层和第三量子阱子层的具体厚度比可以根据所需LED器件的发光波长大小选取。It should be noted that the specific thickness ratio of the first quantum well sublayer, the second quantum well sublayer and the third quantum well sublayer can be selected according to the light emission wavelength of the desired LED device.
进一步地,第一量子垒子层、第二量子垒子层和第三量子垒子层的厚度比为1:n:1,4≤n≤6,n为正整数。Further, the thickness ratio of the first quantum barrier sublayer, the second quantum barrier sublayer and the third quantum barrier sublayer is 1:n:1, 4≤n≤6, and n is a positive integer.
可选地,各个量子垒层的总厚度可以为9~20nm。Optionally, the total thickness of each quantum barrier layer may be 9-20 nm.
进一步地,第一量子垒子层的Si/Ga比随着厚度的增加而逐渐增加,第二量子垒子层的Si/Ga比恒定不变,第三量子垒子层的Si/Ga比随着厚度的增加而逐渐减少。Further, the Si/Ga ratio of the first quantum barrier sublayer increases gradually with the increase of thickness, the Si/Ga ratio of the second quantum barrier sublayer is constant, and the Si/Ga ratio of the third quantum barrier sublayer increases with the increase of thickness. gradually decreases with increasing thickness.
进一步地,第一量子阱子层的Si/Ga比随着厚度的增加而逐渐减少。Further, the Si/Ga ratio of the first quantum well sublayer gradually decreases as the thickness increases.
进一步地,第一量子阱子层的Si/Ga比的最大值为第二量子垒子层的Si/Ga比的20~30%,第一量子垒子层的Si/Ga比的最小值为第二量子垒子层的Si/Ga比的20~30%,第三量子垒子层的Si/Ga比的最小值为第二量子垒子层的Si/Ga比的20~30%。Further, the maximum value of the Si/Ga ratio of the first quantum well sublayer is 20-30% of the Si/Ga ratio of the second quantum barrier sublayer, and the minimum value of the Si/Ga ratio of the first quantum barrier sublayer is The Si/Ga ratio of the second quantum barrier sublayer is 20-30%, and the minimum value of the Si/Ga ratio of the third quantum barrier sublayer is 20-30% of the Si/Ga ratio of the second quantum barrier sublayer.
可选地,第一量子阱子层和第三量子阱子层的生长温度均大于等于第二量子阱子层的生长温度。由于低温有利于In的并入,因此将第二量子阱子层的生长温度设置的较低,可以有利于提高第二量子阱子层的In/Ga比,从而有利于减少LED器件的发光的半波宽,提高LED器件发光集中度和发光强度。Optionally, the growth temperatures of the first quantum well sublayer and the third quantum well sublayer are both greater than or equal to the growth temperature of the second quantum well sublayer. Since low temperature is conducive to the incorporation of In, setting the growth temperature of the second quantum well sublayer to a lower value can be beneficial to increase the In/Ga ratio of the second quantum well sublayer, thereby reducing the luminous effect of the LED device. The half-wave width improves the luminous concentration and luminous intensity of the LED device.
在本实施例中,第一量子阱子层的生长温度逐渐降低至第二量子阱子层的生长温度,第二量子阱子层恒温生长,第三量子阱子层的生长温度由第二量子阱子层的生长温度逐渐升高,以形成平滑过渡。In this embodiment, the growth temperature of the first quantum well sublayer is gradually reduced to the growth temperature of the second quantum well sublayer, the second quantum well sublayer is grown at a constant temperature, and the growth temperature of the third quantum well sublayer is changed from the second quantum well sublayer to the growth temperature of the second quantum well sublayer. The growth temperature of the well sublayer is gradually increased to form a smooth transition.
可选地,第一量子阱子层的生长温度的最大值比第二量子阱子层的生长温度高30-50℃,第三量子阱子层的生长温度的最大值比第二量子阱子层的生长温度高30-50℃。Optionally, the maximum growth temperature of the first quantum well sublayer is 30-50°C higher than the growth temperature of the second quantum well sublayer, and the maximum growth temperature of the third quantum well sublayer is higher than that of the second quantum well sublayer. The growth temperature of the layers is 30-50°C higher.
示例性地,第一量子阱子层的生长温度由830~840℃逐渐降低至790~800℃,第二量子阱子层的生长温度为790~800℃,第三量子阱子层的生长温度由790~800℃逐渐升高至830~840℃。Exemplarily, the growth temperature of the first quantum well sublayer is gradually reduced from 830 to 840°C to 790 to 800°C, the growth temperature of the second quantum well sublayer is 790 to 800°C, and the growth temperature of the third quantum well sublayer is 790 to 800°C. It gradually increased from 790 to 800 °C to 830 to 840 °C.
可选地,第一量子阱子层和第三量子阱子层的生长温度均大于等于第二量子阱子层的生长温度。由于低温有利于In的并入,因此将第二量子阱子层的生长温度设置的较低,可以有利于提高第二量子阱子层的In/Ga比,从而有利于减少LED器件的发光的半波宽,提高LED器件发光集中度和发光强度。Optionally, the growth temperatures of the first quantum well sublayer and the third quantum well sublayer are both greater than or equal to the growth temperature of the second quantum well sublayer. Since low temperature is conducive to the incorporation of In, setting the growth temperature of the second quantum well sublayer to a lower value can be beneficial to increase the In/Ga ratio of the second quantum well sublayer, thereby reducing the luminous effect of the LED device. The half-wave width improves the luminous concentration and luminous intensity of the LED device.
在本实施例中,第一量子垒子层的生长温度逐渐升高至第二量子垒子层的生长温度,第二量子垒子层恒温生长,第三量子垒子层的生长温度由第二量子垒子层的生长温度逐渐降低,以形成平滑过渡。In this embodiment, the growth temperature of the first quantum barrier sublayer is gradually increased to the growth temperature of the second quantum barrier sublayer, the second quantum barrier sublayer is grown at constant temperature, and the growth temperature of the third quantum barrier sublayer is increased from the second quantum barrier sublayer to the growth temperature of the second quantum barrier sublayer. The growth temperature of the quantum barrier layer is gradually lowered to form a smooth transition.
可选地,第一量子垒子层的生长温度的最大值比第二量子垒子层的生长温度低20-30℃,第三量子垒子层的生长温度的最大值比第二量子垒子层的生长温度低30-30℃。Optionally, the maximum growth temperature of the first quantum barrier sublayer is 20-30° C. lower than the growth temperature of the second quantum barrier sublayer, and the maximum growth temperature of the third quantum barrier sublayer is lower than that of the second quantum barrier layer. The growth temperature of the layer is 30-30°C lower.
示例性地,第一量子垒子层的生长温度由830~840℃逐渐升高至850~870℃,第二量子垒子层的生长温度为850~870℃,第三量子垒子层的生长温度由850~870℃逐渐降低至830~840℃。Exemplarily, the growth temperature of the first quantum barrier sublayer is gradually increased from 830-840°C to 850-870°C, the growth temperature of the second quantum barrier sublayer is 850-870°C, and the growth temperature of the third quantum barrier sublayer is 850-870°C. The temperature was gradually decreased from 850 to 870°C to 830 to 840°C.
此时量子阱层与量子垒层的接触部分的温差较小,可以防止量子垒层的生长温度较高,破坏量子阱层的晶体质量,起到保护量子阱的作用。同时还可以减少量子阱中In的析出,提高LED器件的发光强度。At this time, the temperature difference between the contact portion of the quantum well layer and the quantum barrier layer is small, which can prevent the growth temperature of the quantum barrier layer from being high, damage the crystal quality of the quantum well layer, and protect the quantum well. At the same time, the precipitation of In in the quantum well can be reduced, and the luminous intensity of the LED device can be improved.
可选地,量子阱层和量子垒层的生长压力均为100~300Torr。Optionally, the growth pressures of the quantum well layer and the quantum barrier layer are both 100-300 Torr.
步骤306、在多量子阱层上生长低温P型层。
其中,低温P型层可以为掺Mg的GaN层,厚度为10~40um。The low-temperature P-type layer may be a Mg-doped GaN layer with a thickness of 10-40um.
示例性地,将反应室温度控制在700~800℃,压力控制在100~600Torr,生长厚度为10~40um的低温P型层。Exemplarily, the temperature of the reaction chamber is controlled at 700-800° C., the pressure is controlled at 100-600 Torr, and a low-temperature P-type layer with a thickness of 10-40 μm is grown.
步骤307、在低温P型层上生长电子阻挡层。
其中,电子阻挡层为掺Mg的AlGaN层,电子阻挡层中Mg的掺杂浓度小于1019cm-3。The electron blocking layer is a Mg-doped AlGaN layer, and the doping concentration of Mg in the electron blocking layer is less than 10 19 cm -3 .
示例性地,将反应室温度控制在900~1000℃,压力控制在100~300Torr,生长厚度为20~30nm的电子阻挡层。Exemplarily, the temperature of the reaction chamber is controlled at 900-1000° C., the pressure is controlled at 100-300 Torr, and an electron blocking layer with a thickness of 20-30 nm is grown.
步骤308、在电子阻挡层上生长P型层。
其中,P型层为掺Mg的GaN层,P型层中Mg的掺杂浓度大于或等于1020cm-3示例性地,将反应室温度控制在900~980℃,压力控制在300~600Torr,生长厚度为10~30nm的P型层。The P-type layer is a Mg-doped GaN layer, and the doping concentration of Mg in the P-type layer is greater than or equal to 10 20 cm -3 Exemplarily, the temperature of the reaction chamber is controlled at 900-980° C., and the pressure is controlled at 300-600 Torr , a P-type layer with a thickness of 10 to 30 nm is grown.
步骤309、在P型层上生长P型接触层。
其中,P型接触层可以为重掺杂Mg的GaN层,Mg的掺杂浓度大于或等于1*1020cm-3。The P-type contact layer may be a GaN layer heavily doped with Mg, and the doping concentration of Mg is greater than or equal to 1*10 20 cm −3 .
示例性地,将反应室温度控制在850~1050℃,压力控制在100~600Torr,生长厚度为30~50nm的P型接触层。Exemplarily, the temperature of the reaction chamber is controlled at 850-1050° C., the pressure is controlled at 100-600 Torr, and a P-type contact layer with a thickness of 30-50 nm is grown.
在上述步骤完成之后,将反应室的温度降至650~850℃,在氮气气氛进行退火处理5~15min,而后逐渐降至室温,结束发光二极管的外延生长。After the above steps are completed, the temperature of the reaction chamber is lowered to 650-850° C., annealed in a nitrogen atmosphere for 5-15 minutes, and then gradually lowered to room temperature to complete the epitaxial growth of the light-emitting diode.
图4是现有的多量子阱层的能带示意图,图5是本发明实施例提供的多量子阱层的能带示意图,如图4和图5所示,本发明提供的多量子阱层的能带较现有的多量子阱层的能带的倾斜程度有所改善,且电子和空穴的波函数在空间分布上的重叠区域增加。FIG. 4 is a schematic diagram of an energy band of an existing multi-quantum well layer, and FIG. 5 is a schematic diagram of an energy band of a multi-quantum well layer provided by an embodiment of the present invention. As shown in FIGS. 4 and 5 , the multi-quantum well layer provided by the present invention Compared with the existing multi-quantum well layer, the energy band inclination degree of the energy band is improved, and the overlapping area of the spatial distribution of the wave functions of electrons and holes is increased.
本发明实施例通过将各个量子阱层分成三个子层,且第二量子阱子层的In/Ga比大于等于第一量子阱子层和第三量子阱子层的In/Ga比,因此,第二量子阱子层中的In含量较高,可以作为主要发光层,保证LED的发光效率。第一量子阱子层和第三量子阱子层中的In含量较低,且与量子垒层接触,可以减小量子阱层和量子垒层之间的晶格失配,从而减少压应力。同时,第一量子阱子层中掺有少量Si,可以增加量子阱层中的电子浓度,从而改善多量子阱层的能带倾斜现象,增加电子和空穴的波函数在空间分布上的重叠度,提高LED的内量子效率。且由于Si为杂质,在量子阱层中掺Si会影响阱层的晶体质量,而第一量子阱子层并非主要的发光层,因此,在第一量子阱子层中掺Si,可以减少Si杂质掺杂对阱层晶体质量的影响,从而保证阱层的发光效率。进一步地,通过将量子垒层分成三个子层,且第二量子垒子层的Si/Ga比大于等于第一量子垒子层和第三量子垒子层的Si/Ga比,即与量子阱层接触的第一量子垒子层和第三量子垒子层中的Si的掺杂浓度较少,可以保证第一量子垒子层和第三量子垒子层的晶体质量,从而提高阱垒之间的界面质量,进而可以进一步提高LED的发光效率。In the embodiment of the present invention, each quantum well layer is divided into three sublayers, and the In/Ga ratio of the second quantum well sublayer is greater than or equal to the In/Ga ratio of the first quantum well sublayer and the third quantum well sublayer. Therefore, The In content in the second quantum well sublayer is relatively high, which can be used as the main light-emitting layer to ensure the light-emitting efficiency of the LED. The content of In in the first quantum well sublayer and the third quantum well sublayer is low, and they are in contact with the quantum barrier layer, which can reduce the lattice mismatch between the quantum well layer and the quantum barrier layer, thereby reducing compressive stress. At the same time, the first quantum well sublayer is doped with a small amount of Si, which can increase the electron concentration in the quantum well layer, thereby improving the energy band tilt phenomenon of the multiple quantum well layer and increasing the overlap of the spatial distribution of the wave functions of electrons and holes. degree, improve the internal quantum efficiency of LED. And since Si is an impurity, doping Si in the quantum well layer will affect the crystal quality of the well layer, and the first quantum well sublayer is not the main light-emitting layer. Therefore, doping Si in the first quantum well sublayer can reduce Si. The influence of impurity doping on the crystal quality of the well layer ensures the luminous efficiency of the well layer. Further, by dividing the quantum barrier layer into three sublayers, and the Si/Ga ratio of the second quantum barrier sublayer is greater than or equal to the Si/Ga ratio of the first quantum barrier sublayer and the third quantum barrier sublayer, that is, the same as the quantum well. The doping concentration of Si in the first quantum barrier sublayer and the third quantum barrier sublayer that are in contact with each other is less, which can ensure the crystal quality of the first quantum barrier sublayer and the third quantum barrier sublayer, thereby improving the well barrier. The interface quality between the two can further improve the luminous efficiency of the LED.
以上仅为本发明的较佳实施例,并不用以限制本发明,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above are only preferred embodiments of the present invention and are not intended to limit the present invention. Any modification, equivalent replacement, improvement, etc. made within the spirit and principle of the present invention shall be included in the protection scope of the present invention. Inside.
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