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CN102306691B - Method for raising light emitting diode luminescence efficiency - Google Patents

Method for raising light emitting diode luminescence efficiency Download PDF

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CN102306691B
CN102306691B CN201110258718.7A CN201110258718A CN102306691B CN 102306691 B CN102306691 B CN 102306691B CN 201110258718 A CN201110258718 A CN 201110258718A CN 102306691 B CN102306691 B CN 102306691B
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韩杰
魏世祯
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Jingcan Optoelectronics Guangdong Co ltd
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HC Semitek Corp
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Abstract

The invention discloses a method for raising light emitting diode luminescence efficiency. A novel method is employed to a growth mode of a barrier layer in a luminescent layer in a light emitting diode epitaxial wafer structure: through growing barrier layers of different thicknesses, compound efficiency of an electron hole is raised, thus luminescence efficiency is raised. According to design of the method, high compound efficiency is ensured, low forward voltage is maintained, through increasing thickness of a barrier layer close to a side of an N type layer, migration motion of an electron is restricted, the electron is prevented from passing an MQW area to compound with the hole at a P type layer, thus thickness of a barrier layer close to a side of the P type layer is reduced, and the hole is facilitated to pass the barrier layer and compound with the electron at quantum well to raise light extraction efficiency.

Description

一种提高发光二极管发光效率的方法A method for improving the luminous efficiency of light-emitting diodes

技术领域 technical field

本发明涉及一种能够应用于半导体发光二极管,特别是氮化镓基蓝绿光发光二极管,能有效提高其发光效率的一种新方法。The invention relates to a new method which can be applied to semiconductor light-emitting diodes, especially gallium nitride-based blue-green light-emitting diodes, and can effectively improve its luminous efficiency.

背景技术 Background technique

半导体发光二极管具有体积小、效率高和寿命长等优点,在交通指示、户外全色显示等领域有着广泛的应用。尤其是利用大功率发光二极管(LED)可能实现半导体固态照明,引起人类照明史的革命,从而逐渐成为目前光电子学领域的研究热点。然而,目前产业化的LED发光效率只有50lm/W左右,其效率还较传统的光源低很多。为了获得高亮度的LED,关键要提高器件的量子效率。Semiconductor light-emitting diodes have the advantages of small size, high efficiency and long life, and are widely used in traffic indication, outdoor full-color display and other fields. In particular, the use of high-power light-emitting diodes (LEDs) may realize semiconductor solid-state lighting, which has caused a revolution in the history of human lighting, and has gradually become a research hotspot in the field of optoelectronics. However, the current industrialized LED luminous efficiency is only about 50lm/W, which is much lower than traditional light sources. In order to obtain high-brightness LEDs, the key is to improve the quantum efficiency of the device.

发明内容 Contents of the invention

本发明的目的在于提出一种新的方法增加半导体发光二极管的量子效率,这种方法直接运用于外延片生长工艺中,通过改变发光层MQW中垒层的厚度,提高电子与空穴在MQW中复合的效率从而增加其发光效率。The purpose of the present invention is to propose a new method to increase the quantum efficiency of semiconductor light-emitting diodes. This method is directly applied to the epitaxial wafer growth process. By changing the thickness of the barrier layer in the light-emitting layer MQW, the electrons and holes in the MQW are improved The efficiency of recombination increases its luminous efficiency.

本发明的技术方案为:一种提高发光二极管发光效率的结构,该二极管外延片结构从下向上的顺序依次为衬底,低温缓冲层,高温缓冲层,N型层,N型层,N型层,N型层,发光层,P型层,P型层,P型层。发光层MQW(多量子阱)中采用具有不同厚度的垒层来提高发光效率:靠近N型层一侧的垒层厚度为15nm到25nm,而靠近P型层一侧的垒层的厚度在5到15nm。垒层的生长厚度介于5nm至20nm之间,生长温度介于800℃至1050℃之间,V/IH摩尔比介于1000至20000之间。发光层MQW中,垒层的结构可以是AlxInyGal-x-yN 0≤x<1,0≤y<1,x+y<1。发光层MQW中间X个垒层的厚度较厚,其余Y个垒层的厚度较薄,且中间X个垒层的厚度大于其余Y个垒层的厚度。The technical solution of the present invention is: a structure for improving the luminous efficiency of a light-emitting diode. The sequence of the diode epitaxial wafer structure from bottom to top is substrate, low-temperature buffer layer, high-temperature buffer layer, N-type layer, N-type layer, N-type layer, N-type layer, light-emitting layer, P-type layer, P-type layer, P-type layer. In the light-emitting layer MQW (Multiple Quantum Well), barrier layers with different thicknesses are used to improve luminous efficiency: the thickness of the barrier layer near the N-type layer is 15nm to 25nm, and the thickness of the barrier layer near the P-type layer is 5nm. to 15nm. The growth thickness of the barrier layer is between 5nm and 20nm, the growth temperature is between 800°C and 1050°C, and the V/IH molar ratio is between 1000 and 20000. In the light-emitting layer MQW, the structure of the barrier layer may be AlxInyGal-x-yN 0≤x<1, 0≤y<1, x+y<1. The X barrier layers in the middle of the light-emitting layer MQW are thicker, the remaining Y barrier layers are thinner, and the X barrier layers in the middle are thicker than the remaining Y barrier layers.

本发明以高纯氢气(H2)或氮气(N2)作为载气,以三甲基镓(TMGa)、三甲基铝(TMAl)、三甲基铟(TMIn)和氨气(NH3)分别作为Ga、Al、In和N源,用硅烷(SiH4)、二茂镁(Cp2Mg)分别作为n、p型掺杂剂。In the present invention, high-purity hydrogen (H2) or nitrogen (N2) is used as carrier gas, and trimethylgallium (TMGa), trimethylaluminum (TMAl), trimethylindium (TMIn) and ammonia (NH3) are respectively used as Ga, Al, In and N sources, use silane (SiH4), dimagnesium (Cp2Mg) as n and p type dopants respectively.

外延结构如图四所示:The epitaxial structure is shown in Figure 4:

(1)衬底1(1) Substrate 1

在本发明所述衬底1是适合氮化镓及其它半导体外延材料生长的材料,如:氮化镓单晶、蓝宝石、单晶硅、碳化硅(SiC)单晶等等。The substrate 1 in the present invention is a material suitable for the growth of gallium nitride and other semiconductor epitaxial materials, such as gallium nitride single crystal, sapphire, single crystal silicon, silicon carbide (SiC) single crystal, and the like.

首先将衬底材料在氢气气氛里进行退火,清洁衬底表面,温度控制在1050℃与1180℃之间,然后进行氮化处理;First, anneal the substrate material in a hydrogen atmosphere, clean the substrate surface, control the temperature between 1050°C and 1180°C, and then perform nitriding treatment;

(2)低温缓冲层2(2) Low temperature buffer layer 2

将温度下降到500℃与650℃之间,生长15至30nm厚的低温GaN成核层,此生长过程时,生长压力在300Torr至760Torr之间,V/III摩尔比在500至3000之间;Lower the temperature to between 500°C and 650°C, and grow a low-temperature GaN nucleation layer with a thickness of 15 to 30 nm. During this growth process, the growth pressure is between 300 Torr and 760 Torr, and the V/III molar ratio is between 500 and 3000;

(3)高温缓冲层3(3) High temperature buffer layer 3

低温缓冲层2生长结束后,停止通入TMGa,将衬底温度升高到1000℃至1200℃之间,对低温缓冲层2在原位进行退火处理,退火时间在5分钟至10分钟之间;退火之后,将温度调节到1000℃至1200℃之间,在较低的V/III摩尔比条件下外延生长厚度为0.8μm至2μm之间的高温不掺杂的GaN,此生长过程时,生长压力在50Torr至760Torr之间,V/III摩尔比在300至3000之间;After the growth of the low-temperature buffer layer 2 is completed, stop feeding TMGa, raise the substrate temperature to between 1000°C and 1200°C, and anneal the low-temperature buffer layer 2 in situ, and the annealing time is between 5 minutes and 10 minutes ; After annealing, adjust the temperature to between 1000°C and 1200°C, and epitaxially grow high-temperature undoped GaN with a thickness between 0.8 μm and 2 μm under the condition of a relatively low V/III molar ratio. During this growth process, The growth pressure is between 50Torr and 760Torr, and the V/III molar ratio is between 300 and 3000;

(4)N型层4(4) N-type layer 4

U-GaN 3生长结束后,生长一层掺杂浓度梯度增加的的N型层4,厚度在0.2μm至1μm之间,生长温度在1000℃至1200℃之间,生长压力在50Torr至760Torr之间,V/III摩尔比在300至3000之间;After the growth of U-GaN 3 is completed, grow an N-type layer 4 with a gradient increase in doping concentration, the thickness is between 0.2 μm and 1 μm, the growth temperature is between 1000 ° C and 1200 ° C, and the growth pressure is between 50 Torr and 760 Torr Between, the V/III molar ratio is between 300 and 3000;

(5)N型层5(5) N-type layer 5

N型层4生长结束后,生长掺杂浓度稳定的N型层5,厚度在1.2μm至3.5μm之间,生长温度在1000℃至1200℃之间,生长压力在50Torr至760Torr之间,V/III摩尔比在300至3000之间;After the growth of the N-type layer 4 is completed, an N-type layer 5 with a stable doping concentration is grown, the thickness is between 1.2 μm and 3.5 μm, the growth temperature is between 1000° C. and 1200° C., the growth pressure is between 50 Torr and 760 Torr, V /III molar ratio between 300 and 3000;

(6)N型层6(6) N-type layer 6

N型层5生长结束后,生长N型层6,厚度在10nm至100nm之间,生长温度在1000℃至1200℃之间,生长压力在50Torr至760Torr之间,V/III摩尔比在300至3000之间;After the growth of N-type layer 5 is completed, grow N-type layer 6 with a thickness between 10nm and 100nm, a growth temperature between 1000°C and 1200°C, a growth pressure between 50Torr and 760Torr, and a V/III molar ratio between 300 and 1200°C. Between 3000;

(7)N型层7(7) N-type layer 7

N型层6生长结束后,生长N型层7,厚度在10nm至50nm之间;掺杂浓度稳定,生长温度在1000℃至1200℃之间,生长压力在50Torr至760Torr之间,V/III摩尔比在300至3000之间;After the growth of N-type layer 6 is completed, grow N-type layer 7 with a thickness between 10nm and 50nm; the doping concentration is stable, the growth temperature is between 1000°C and 1200°C, and the growth pressure is between 50Torr and 760Torr, V/III The molar ratio is between 300 and 3000;

(8)发光层MWQ 8(8) Light-emitting layer MWQ 8

发光层8由6至15个周期的InaGa1-aN(0<a<1)/GaN多量子阱组成。阱的厚度在2nm至3nm之间,生长温度在720至820℃之间,生长压力在200Torr至400Tor r之间,V/III摩尔比在300至5000之间;垒的厚度在5至30nm之间,生长温度在820至920℃之间,生长压力在200Torr至400Torr之间,V/III摩尔比在300至5000之间;The light-emitting layer 8 is composed of 6 to 15 periods of InaGa1-aN (0<a<1)/GaN multiple quantum wells. The thickness of the well is between 2nm and 3nm, the growth temperature is between 720 and 820°C, the growth pressure is between 200Torr and 400Tor r, the V/III molar ratio is between 300 and 5000; the thickness of the barrier is between 5 and 30nm The growth temperature is between 820 and 920°C, the growth pressure is between 200Torr and 400Torr, and the V/III molar ratio is between 300 and 5000;

(9)P型层9(9) P-type layer 9

6至15个周期的InaGa1-aN(0<a<1)/GaN多量子阱发光层8生长结束后,升高温,温度控制在950℃至1080℃之间,生长压力50Torr至500Torr之间,V/III摩尔比1000至20000之间,生长厚度10nm至200nm之间的P型AlxInyGa1-x-yN(0<x<1,0≤y<1,x+y<1)宽禁带电子阻挡层。该层禁带宽度大于最后一个barrier的禁带宽度,可控制在4eV与5.5eV之间;该层Mg掺杂浓度Mg/Ga摩尔比介于1/100至1/4之间。After 6 to 15 cycles of InaGa1-aN (0<a<1)/GaN multi-quantum well light-emitting layer 8 growth, the temperature is raised, the temperature is controlled between 950°C and 1080°C, and the growth pressure is between 50Torr and 500Torr. P-type AlxInyGa1-x-yN (0<x<1, 0≤y<1, x+y<1) wide bandgap electron barrier with V/III molar ratio between 1000 and 20000 and growth thickness between 10nm and 200nm layer. The forbidden band width of this layer is larger than that of the last barrier, which can be controlled between 4eV and 5.5eV; the Mg doping concentration of this layer, the Mg/Ga molar ratio is between 1/100 and 1/4.

(10)P型层10(10) P-type layer 10

P型层9生长结束后,生长厚度为100nm至800nm之间的P型AlxInyGa1-x-yN(0≤x<1,0≤y<1,x+y<1)层,即P型层10,该层Mg掺杂浓度Mg/Ga摩尔比介于1/100至1/4之间,其生长温度850℃至1050℃之间。After the growth of the P-type layer 9 is completed, grow a P-type AlxInyGa1-x-yN (0≤x<1, 0≤y<1, x+y<1) layer with a thickness between 100nm and 800nm, that is, the P-type layer 10 The Mg doping concentration Mg/Ga molar ratio of the layer is between 1/100 and 1/4, and the growth temperature is between 850°C and 1050°C.

(11)P型层11(11) P-type layer 11

P型层10生长结束后,生长P型接触层,其生长温度850℃至1050℃之间,生长压力100Torr至760Torr之间,V/III摩尔比介于1000至20000之间,该层Mg掺杂浓度Mg/Ga摩尔比介于1/100至1/4之间,生长厚度介于5nm至20nm之间。After the growth of the P-type layer 10 is completed, the P-type contact layer is grown, the growth temperature is between 850°C and 1050°C, the growth pressure is between 100Torr and 760Torr, and the V/III molar ratio is between 1000 and 20000. This layer is Mg-doped The impurity concentration Mg/Ga molar ratio is between 1/100 and 1/4, and the growth thickness is between 5nm and 20nm.

外延生长结束后,将反应腔的温度降至650至850℃之间,纯氮气氛围进行退火处理5至15min,然后降至室温,结束外延生长。After the epitaxial growth is completed, the temperature of the reaction chamber is lowered to 650-850° C., annealing is performed in a pure nitrogen atmosphere for 5 to 15 minutes, and then the temperature is lowered to room temperature to end the epitaxial growth.

随后,经过清洗、沉积、光刻和刻蚀等半导体加工工艺制成单颗小尺寸芯片。Subsequently, a single small-sized chip is made through semiconductor processing processes such as cleaning, deposition, photolithography, and etching.

本发明的优点在于:本发明所述的这种外延生长工艺的设计不仅提高了电子空穴复合效率,而且可以降低工作电压,提升ESD良率,改善漏电。The advantage of the present invention is that: the design of the epitaxial growth process described in the present invention not only improves the electron-hole recombination efficiency, but also can reduce the working voltage, improve the ESD yield, and improve leakage.

附图说明 Description of drawings

图1芯片结构图;Fig. 1 chip structure diagram;

图2为传统的LED结构的MQW区域结构示意图;FIG. 2 is a schematic diagram of the MQW region structure of a traditional LED structure;

图3为本发明一种提高发光二极管发光效率的方法MQW区域结构示意图;3 is a schematic diagram of the MQW region structure of a method for improving the luminous efficiency of a light-emitting diode according to the present invention;

图4为本发明一种提高发光二极管发光效率的方法MQW区域结构示意图;4 is a schematic diagram of the MQW region structure of a method for improving the luminous efficiency of a light-emitting diode according to the present invention;

图5为本发明一种提高发光二极管发光效率的方法MQW区域结构示意图。FIG. 5 is a schematic diagram of the MQW region structure of a method for improving the luminous efficiency of a light-emitting diode according to the present invention.

图中:In the picture:

其中1为衬底、2为低温缓冲层、3为高温缓冲层、4、5、6、7为符合N型层、8为发光层、9、10、11为符合P型层、12为透明导电层(Ni/Au或者ITO)、13为P电极、14为N电极、101为量子阱、102为量子垒、201为量子阱、202 203 204 205 206为量子垒、301为量子阱、302303为量子垒、401为量子阱、402403为量子垒。Among them, 1 is the substrate, 2 is the low-temperature buffer layer, 3 is the high-temperature buffer layer, 4, 5, 6, and 7 are N-type layers, 8 is the light-emitting layer, 9, 10, and 11 are P-type layers, and 12 is transparent Conductive layer (Ni/Au or ITO), 13 is P electrode, 14 is N electrode, 101 is quantum well, 102 is quantum barrier, 201 is quantum well, 202 203 204 205 206 is quantum barrier, 301 is quantum well, 302303 is a quantum barrier, 401 is a quantum well, and 402403 is a quantum barrier.

具体实施方式 Detailed ways

下面结合实施例对本发明做进一步的说明,本发明所有的实施例均利用Thomas Swan(AIXTRON子公司)CCS MOCVD系统实施。Below in conjunction with embodiment the present invention is described further, all embodiments of the present invention all utilize Thomas Swan (AIXTRON subsidiary company) CCS MOCVD system to implement.

实施例1Example 1

如图一所示:As shown in Figure 1:

(1)衬底1(1) Substrate 1

首先将蓝宝石衬底在温度为1120℃,纯氢气气氛里进行退火,然后进行氮化处理;First, anneal the sapphire substrate at a temperature of 1120°C in a pure hydrogen atmosphere, and then perform nitriding treatment;

(2)低温缓冲层2(2) Low temperature buffer layer 2

将温度下降到585℃,生长20nm厚的低温GaN成核层,此生长过程时,生长压力为420Torr,V/III摩尔比为900;Lower the temperature to 585°C to grow a 20nm-thick low-temperature GaN nucleation layer. During this growth process, the growth pressure is 420 Torr, and the V/III molar ratio is 900;

(3)高温缓冲层3(3) High temperature buffer layer 3

低温缓冲层2生长结束后,停止通入TMGa,将衬底温度升高1120℃,对低温缓冲层2在原位进行退火处理,退火时间为8分钟;退火之后,将温度调节到1120℃,在较低的V/III摩尔比条件下外延生长厚度为1.2μm的高温不掺杂的GaN,此生长过程中,生长压力在200Torr,V/III摩尔比为1500;After the growth of the low-temperature buffer layer 2 is completed, stop feeding TMGa, raise the substrate temperature by 1120° C., and perform annealing treatment on the low-temperature buffer layer 2 in situ. The annealing time is 8 minutes; after the annealing, adjust the temperature to 1120° C. Epitaxial growth of high-temperature undoped GaN with a thickness of 1.2 μm under a lower V/III molar ratio. During this growth process, the growth pressure is 200 Torr, and the V/III molar ratio is 1500;

(4)N型层4(4) N-type layer 4

高温缓冲层3生长结束后,生长一层掺杂浓度梯度增加的的N型层,掺杂浓度从1×1017/cm3变化到5×1018/cm3,厚度为0.8μm,生长温度为1120℃,生长压力为150Torr,V/III摩尔比为1800;After the growth of the high-temperature buffer layer 3 is completed, an N-type layer with a gradient increase in doping concentration is grown, the doping concentration is changed from 1×1017/cm3 to 5×1018/cm3, the thickness is 0.8 μm, and the growth temperature is 1120°C. The growth pressure is 150 Torr, and the V/III molar ratio is 1800;

(5)N型层5(5) N-type layer 5

N型层4生长结束后,生长掺杂浓度稳定的N型层5,厚度为3.5μm,生长温度为1120℃,生长压力为150Torr,V/III摩尔比为1800;After the growth of the N-type layer 4 is completed, an N-type layer 5 with a stable doping concentration is grown, with a thickness of 3.5 μm, a growth temperature of 1120° C., a growth pressure of 150 Torr, and a V/III molar ratio of 1800;

(6)N型层6(6) N-type layer 6

N型层5生长结束后,生长N型层6,厚度为20nm,掺杂浓度稳定,浓度低于N型层4的平均浓度,低于N型层5的掺杂浓度,远低于N型层7的掺杂浓度,其目的是为了提高载流子的迁移率;生长温度为1120℃,生长压力为150Torr,V/III摩尔比为2800;After the growth of N-type layer 5 is completed, grow N-type layer 6 with a thickness of 20nm and a stable doping concentration, which is lower than the average concentration of N-type layer 4, lower than the doping concentration of N-type layer 5, and far lower than N-type The doping concentration of layer 7 is to increase the mobility of carriers; the growth temperature is 1120°C, the growth pressure is 150 Torr, and the V/III molar ratio is 2800;

(7)N型层7(7) N-type layer 7

N型层6生长结束后,生长N型层7,厚度为10nm,掺杂浓度稳定,浓度高于N型层5,该层是整个N型区域浓度最高的区域,其目的是为了获得更高的载流子浓度。生长温度为1120℃,生长压力为150Torr,V/III摩尔比为2800;After the growth of N-type layer 6 is completed, grow N-type layer 7 with a thickness of 10nm, a stable doping concentration, and a concentration higher than that of N-type layer 5. This layer is the region with the highest concentration in the entire N-type region, and its purpose is to obtain a higher concentration. carrier concentration. The growth temperature is 1120°C, the growth pressure is 150 Torr, and the V/III molar ratio is 2800;

(8)发光层MQW 8(8) Light-emitting layer MQW 8

发光层8由6个周期的In0.3Ga0.7N/GaN多量子阱组成。阱的厚度为2.5nm,生长温度为780℃,生长压力为200Torr,V/III摩尔比为4500;垒的厚度为18nm,生长温度为900℃,生长压力为200Torr,V/III摩尔比为4500;The light emitting layer 8 is composed of 6 periods of In 0.3 Ga 0.7 N/GaN multiple quantum wells. The thickness of the well is 2.5nm, the growth temperature is 780°C, the growth pressure is 200Torr, and the V/III molar ratio is 4500; the thickness of the barrier is 18nm, the growth temperature is 900°C, the growth pressure is 200Torr, and the V/III molar ratio is 4500 ;

如图2所示,靠近N型层一侧202的厚度介于18到24nm,垒层厚度202>203>204>205>206,靠近P型层一侧最后一个垒层206的厚度介于5到15nm。As shown in FIG. 2, the thickness of the side 202 close to the N-type layer is between 18 and 24 nm, the thickness of the barrier layer 202 > 203 > 204 > 205 > 206, and the thickness of the last barrier layer 206 close to the P-type layer is between 5 and 5 nm. to 15nm.

(9)P型层9(9) P-type layer 9

6至15个周期的InaGa1-aN(0<a<1)/GaN多量子阱发光层8生长结束后,升高温,温度控制在950℃至1080℃之间,生长压力50Torr至500Torr之间,V/III摩尔比1000至20000之间,生长厚度10nm至200nm之间的P型AlxInyGa1-x-yN(0<x<1,0≤y<1,x+y<1)宽禁带电子阻挡层。该层禁带宽度大于最后一个barrier的禁带宽度,可控制在4eV与5.5eV之间;该层Mg掺杂浓度Mg/Ga摩尔比介于1/100至1/4之间。After 6 to 15 cycles of InaGa1-aN (0<a<1)/GaN multi-quantum well light-emitting layer 8 growth, the temperature is raised, the temperature is controlled between 950°C and 1080°C, and the growth pressure is between 50Torr and 500Torr. P-type AlxInyGa1-x-yN (0<x<1, 0≤y<1, x+y<1) wide bandgap electron barrier with V/III molar ratio between 1000 and 20000 and growth thickness between 10nm and 200nm layer. The forbidden band width of this layer is larger than that of the last barrier, which can be controlled between 4eV and 5.5eV; the Mg doping concentration of this layer, the Mg/Ga molar ratio is between 1/100 and 1/4.

(10)P型层10(10) P-type layer 10

P型层9生长结束后,生长0.4μm厚的P型层10,即:P型AlxInyGa1-x-yN(0≤x<1,0≤y<1,x+y<1),该层的禁带宽度大于最后一个barrier的禁带宽度,但小于P型层9的禁带宽度。其生长温度1000℃,生长压力200Torr,V/III摩尔比8000,P型层Mg的掺杂浓度Mg/Ga摩尔比为:1/80。After the growth of the P-type layer 9, grow a 0.4 μm thick P-type layer 10, namely: P-type AlxInyGa1-x-yN (0≤x<1, 0≤y<1, x+y<1), the layer The forbidden band width is greater than the forbidden band width of the last barrier, but smaller than the forbidden band width of the P-type layer 9 . The growth temperature is 1000° C., the growth pressure is 200 Torr, the V/III molar ratio is 8000, and the Mg doping concentration Mg/Ga molar ratio of the P-type layer Mg is: 1/80.

(11)P型层11(11) P-type layer 11

P型层10生长结束后,生长P型接触层,即P型层11,生长温度为1050℃,生长压力为200Torr,V/III摩尔比10000,P型掺杂浓度为1×1020/cm3,生长厚度为15nm。After the growth of the P-type layer 10 is completed, the P-type contact layer, that is, the P-type layer 11, is grown at a growth temperature of 1050° C., a growth pressure of 200 Torr, a V/III molar ratio of 10000, and a P-type doping concentration of 1×1020/cm3. The growth thickness was 15 nm.

所有外延生长结束后,将反应腔的温度降至800℃,纯氮气氛围进行退火处理10min,然后降至室温,结束外延生长。After all the epitaxial growth is completed, the temperature of the reaction chamber is lowered to 800° C., annealing is performed in a pure nitrogen atmosphere for 10 min, and then the temperature is lowered to room temperature to end the epitaxial growth.

(12)ITO透明导电层12(12) ITO transparent conductive layer 12

(13)P电极13(13) P electrode 13

(14)N电极14(14) N electrode 14

实施例1,经过清洗、沉积、光刻和刻蚀等半导体加工工艺制程后,分割成尺寸大小为10×8mil的LED芯片。经LED芯片测试,测试电流10mA,单颗小芯片光输出功率为6.5mW,工作电压3.21V,可抗静电:人体模式5000V。而传统的外延生长方式,相同芯片制程的单颗小芯片光的输出功率仅为5mW。Embodiment 1, after cleaning, deposition, photolithography and etching and other semiconductor processing processes, it is divided into LED chips with a size of 10×8 mil. After the LED chip test, the test current is 10mA, the light output power of a single small chip is 6.5mW, the working voltage is 3.21V, and it can be anti-static: the human body model is 5000V. In the traditional epitaxial growth method, the light output power of a single small chip with the same chip manufacturing process is only 5mW.

实施例2Example 2

实施例2,外延层1、2、3、4、5、6、7、9、10、11层的生长方式均与实施例1相同。不同之处在于发光层MQW中垒层的生长方法:如图3所示,靠近N型层一侧前三个垒层302的厚度相同介于12到24nm,中间三个垒层303的厚度相同介于16到30nm,靠近P型层一侧最后三个垒层302的厚度相同介于12到24nm。其中中间三个垒层302的厚度最厚。In Example 2, the growth methods of the epitaxial layers 1, 2, 3, 4, 5, 6, 7, 9, 10, and 11 are the same as those in Example 1. The difference lies in the growth method of the barrier layer in the light-emitting layer MQW: as shown in Figure 3, the thickness of the first three barrier layers 302 on the side close to the N-type layer is the same, ranging from 12 to 24 nm, and the thickness of the middle three barrier layers 303 is the same The thicknesses of the last three barrier layers 302 on the side close to the P-type layer are also between 12 and 24 nm. Among them, the middle three barrier layers 302 have the thickest thickness.

实施例3Example 3

实施例3,外延层1、2、3、4、5、6、7、9、10、11层的生长方式均与实施例1相同。不同之处在于发光层MQW中垒层的生长方法:如图4所示,靠近N型层一侧前三个垒层402的厚度相同介于16到30nm,靠近P型层一侧最后六个垒层403的厚度相同介于12到24nm。其中靠近N型层一侧前三个垒层的厚度最厚。In Example 3, the growth methods of the epitaxial layers 1, 2, 3, 4, 5, 6, 7, 9, 10, and 11 are the same as those in Example 1. The difference lies in the growth method of the barrier layer in the light-emitting layer MQW: as shown in Figure 4, the thickness of the first three barrier layers 402 on the side close to the N-type layer is the same, ranging from 16 to 30 nm, and the thickness of the last six barrier layers 402 on the side close to the P-type layer is the same. The thickness of the barrier layer 403 also ranges from 12 to 24 nm. Among them, the thickness of the first three barrier layers on the side close to the N-type layer is the thickest.

经过同样条件的芯片制程与测试,10×8mil单颗小芯片光输出功率为6.3mW,工作电压3.15V,可抗静电:人体模式5000V。After the chip manufacturing process and testing under the same conditions, the optical output power of a 10×8mil single small chip is 6.3mW, the working voltage is 3.15V, and it can be antistatic: the human body model is 5000V.

Claims (3)

1.一种提高发光二极管发光效率的方法,该发光二极管外延片结构从下向上的顺序依次为衬底,低温缓冲层,高温缓冲层,第一N型层,第二N型层,第三N型层,第四N型层,发光层,第一P型层,第二P型层,第三P型层;其特征在于:发光层中采用具有不同厚度的垒层来提高发光效率:靠近N型层一侧的垒层厚度为15nm到20nm,而靠近P型层一侧的垒层的厚度在5到15nm;垒层的生长厚度介于5nm至20nm之间,生长温度介于800℃至1050℃之间,V/III摩尔比介于1000至20000之间。  1. A method for improving the luminous efficiency of a light-emitting diode. The sequence of the epitaxial wafer structure of the light-emitting diode is a substrate, a low-temperature buffer layer, a high-temperature buffer layer, a first N-type layer, a second N-type layer, and a third N-type layer from bottom to top. N-type layer, the fourth N-type layer, light-emitting layer, the first P-type layer, the second P-type layer, and the third P-type layer; it is characterized in that: barrier layers with different thicknesses are used in the light-emitting layer to improve luminous efficiency: The thickness of the barrier layer near the N-type layer is 15nm to 20nm, while the thickness of the barrier layer near the P-type layer is 5nm to 15nm; the growth thickness of the barrier layer is between 5nm and 20nm, and the growth temperature is between 800 °C to 1050 °C, V/III molar ratio is between 1000 and 20000. the 2.如权利要求1所述提高发光二极管发光效率的方法,其特征在于:发光层中,垒层的结构可以是AlxInyGa1-x-yN  0≤x<1,0≤y<1,x+y<1。  2. The method for improving the luminous efficiency of light-emitting diodes as claimed in claim 1, characterized in that: in the light-emitting layer, the structure of the barrier layer can be AlxInyGa1-x-yN 0≤x<1, 0≤y<1, x+y <1. the 3.如权利要求1或2所述提高发光二极管发光效率的方法,其特征在于:发光层中间X个垒层的厚度较厚,其余Y个垒层的厚度较薄,且中间X个垒层的厚度大于其余Y个垒层的厚度。  3. The method for improving the luminous efficiency of a light-emitting diode as claimed in claim 1 or 2, wherein the X barrier layers in the middle of the light-emitting layer are thicker, the remaining Y barrier layers are thinner, and the X barrier layers in the middle are thicker. The thickness of is greater than the thickness of the remaining Y barrier layers. the
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