CN108198919A - 一种复合量子阱外延片 - Google Patents

一种复合量子阱外延片 Download PDF

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CN108198919A
CN108198919A CN201711430361.XA CN201711430361A CN108198919A CN 108198919 A CN108198919 A CN 108198919A CN 201711430361 A CN201711430361 A CN 201711430361A CN 108198919 A CN108198919 A CN 108198919A
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CN108198919B (zh
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宁如光
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Nanchang Kaijie Semiconductor Technology Co., Ltd
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
    • H01L33/04Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a quantum effect structure or superlattice, e.g. tunnel junction
    • H01L33/06Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a quantum effect structure or superlattice, e.g. tunnel junction within the light emitting region, e.g. quantum confinement structure or tunnel barrier
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
    • H01L33/10Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a light reflecting structure, e.g. semiconductor Bragg reflector
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
    • H01L33/12Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a stress relaxation structure, e.g. buffer layer
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
    • H01L33/26Materials of the light emitting region
    • H01L33/30Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table
    • H01L33/32Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table containing nitrogen

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Abstract

本发明提供的一种复合量子阱外延片,包括GaAs衬底,在GaAs衬底上依次外延生长缓冲层、AlGaAs/AlAs(DBR)反射层、n‑AlInP限制层、n‑AlGaInP波导层、突变MQW有源层、渐变MQW有源层、p‑AlGaInP波导层、p‑AlInP限制层和p‑GaP电流扩展层;突变MQW有源层和渐变MQW有源层材料为AlGaInP。本发明公开的一种复合量子阱外延片,通过对突变量子阱和渐变量子阱的组合设计,限制电子在量子阱结构中的快速移动,增强空穴载流子的移动能力,从而提高电子与空穴载流子的复合几率,能提高LED芯片的内量子发光效率。

Description

一种复合量子阱外延片
技术领域
本发明属于半导体二极管技术领域,具体涉及一种复合量子阱外延片。
背景技术
现如今,高亮度AlGaInP基发光二极管的应用极为广泛,从传统的显示、指示、按键背光、灯饰等领域扩展到汽车尾灯、背光源等高端应用方面。对于In组分为0.5,(AlxGa1-x)0.5In0.5P材料的晶格常数可以与GaAs衬底完全匹配,通过对Al和Ga组分的调节,可以发出红、橙、黄、黄绿光(波长650-560nm)。因此提高发光效率,对于LED整个行业具有极大的经济效益,同时也促进了各相关行业的产业升级。
发明内容
本发明为提高LED芯片的内量子发光效率,提供一种复合量子阱外延片,通过对突变量子阱和渐变量子阱的组合设计,限制电子在量子阱结构中的快速移动,增强空穴载流子的移动能力,从而提高电子与空穴载流子的复合几率。
为了解决本发明的技术问题,本发明是通过以下技术方案实现的:一种复合量子阱外延片,包括GaAs衬底100,在所述GaAs衬底100上依次外延生长缓冲层101、AlGaAs/AlAs(DBR)反射层102、n-AlInP限制层103、n-AlGaInP波导层104、突变MQW有源层105、渐变MQW有源层106、p-AlGaInP波导层107、p-AlInP限制层108和p-GaP电流扩展层109;所述突变MQW有源层105和渐变MQW有源层106材料为AlGaInP;所述缓冲层101厚度为0.5μm,掺杂浓度为5×1017cm-3,所述AlGaAs/AlAs(DBR)反射层102厚度为1.6μm,掺杂浓度为2×1018
优选地,所述n-AlInP限制层103厚度为0.5μm,掺杂浓度为2×1018
优选地,所述n-AlGaInP波导层104厚度为0.1μm,掺杂浓度为3×1017cm-3
优选地,所述突变MQW有源层105厚度为6nm。
优选地,所述渐变MQW有源层106厚度为4nm。
优选地,所述p-AlGaInP波导层107厚度0.1μm,掺杂浓度为5×1017cm-3
优选地,所述p-AlInP限制层108厚度为0.8μm,掺杂浓度为6×1017
优选地,所述p-GaP电流扩展层109厚度为5μm,掺杂浓度大于1×1018cm-3
与现有技术相比,本发明获得的有益效果是:
本发明公开的一种复合量子阱外延片,通过对突变量子阱和渐变量子阱的组合设计,限制电子在量子阱结构中的快速移动,增强空穴载流子的移动能力,从而提高电子与空穴载流子的复合几率,能提高LED芯片的内量子发光效率。
附图说明
图1为本发明结构示意图。
图2为复合量子阱结构设计示意图。
附图标记:100、GaAs衬底;101、缓冲层;102、AlGaAs/AlAs(DBR)反射层;103、n-AlInP限制层;104、n-AlGaInP波导层;105、突变MQW有源层;106、渐变MQW有源层;107、p-AlGaInP波导层;108、p-AlInP限制层;109、p-GaP电流扩展层。
具体实施方式
下面结合附图,对实施例进行详细说明。
参见附图1,一种复合量子阱外延片,包括GaAs衬底100,在所述GaAs衬底100上依次外延生长缓冲层101、AlGaAs/AlAs(DBR)反射层102、n-AlInP限制层103、n-AlGaInP波导层104、突变MQW有源层105、渐变MQW有源层106、p-AlGaInP波导层107、p-AlInP限制层108和p-GaP电流扩展层109;所述突变MQW有源层105和渐变MQW有源层106材料为AlGaInP。
参见附图2,一种复合量子阱外延片,通过突变量子阱限制电子在量子阱结构中的移动速度,通过渐变量子阱增强空穴载流子的移动能力,如此即可提高电子与空穴载流子的复合几率,从而提高LED芯片的内量子发光效率。
进一步地,本发明采用的设备为MOCVD。
进一步地,本发明使用的MO源为TMGa、TMAl和TMIn。
进一步地,本发明使用的掺杂源为Cp2Mg和SiH4
进一步地,本发明使用的特气为AsH3和PH3
进一步地,在GaAs衬底100上以730℃温度生长n-GaAs缓冲层101,厚度为0.5μm,掺杂浓度为5×1017cm-3
进一步地,在n-GaAs缓冲层101上以730℃生长AlGaAs/AlAs(DBR)反射层102,厚度为1.6μm,掺杂浓度为2×1018cm-3
进一步地,在AlGaAs/AlAs(DBR)反射层102上以730℃生长n-AlInP限制层103,厚度为0.5μm,掺杂浓度为2×1018cm-3
进一步地,在n-AlInP限制层103上以710℃生长n-AlGaInP波导层104,厚度为0.1μm,掺杂浓度为3×1017cm-3
进一步地,在n-AlGaInP波导层104上以710℃生长突变MQW有源层105,厚度为6nm。
进一步地,在突变MQW有源层105上以710℃生长渐变MQW有源层106,厚度为4nm。
进一步地,在渐变MQW有源层106上以710℃生长p-AlGaInP波导层107,厚度为0.1μm,掺杂浓度为为5×1017cm-3
进一步地,在p-AlGaInP波导层107上以730℃生长p-AlInP限制层108,厚度为0.8μm,掺杂浓度为为6×1017cm-3
进一步地,在p-AlInP限制层108上以730℃生长p-GaP电流扩展层109,厚度为5μm,掺杂浓度为1×1018cm-3
以上列举的仅是本发明的具体实施例之一。显然,本发明不限于以上实施例,还可以有许多类似的改形。本领域的普通技术人员能从本发明公开的内容直接导出或联想到的所有变形,均应认为是本发明所要保护的范围。

Claims (8)

1.一种复合量子阱外延片,其特征在于:包括GaAs衬底(100),在所述GaAs衬底(100)上依次外延生长缓冲层(101)、AlGaAs/AlAs(DBR)反射层(102)、n-AlInP限制层(103)、n-AlGaInP波导层(104)、突变MQW有源层(105)、渐变MQW有源层(106)、p-AlGaInP波导层(107)、p-AlInP限制层(108)和p-GaP电流扩展层(109),所述突变MQW有源层(105)和渐变MQW有源层(106)材料为AlGaInP;所述缓冲层(101)厚度为0.5μm,掺杂浓度为5×1017cm-3,所述AlGaAs/AlAs(DBR)反射层(102)厚度为1.6μm,掺杂浓度为2×1018
2.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述n-AlInP限制层(103)厚度为0.5μm,掺杂浓度为2×1018
3.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述n-AlGaInP波导层(104)厚度为0.1μm,掺杂浓度为3×1017cm-3
4.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述突变MQW有源层(105)厚度为6nm。
5.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述渐变MQW有源层(106)厚度为4nm。
6.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述p-AlGaInP波导层(107)厚度0.1μm,掺杂浓度为5×1017cm-3
7.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述p-AlInP限制层(108)厚度为0.8μm,掺杂浓度为6×1017
8.如权利要求1所述的一种复合量子阱外延片,其特征在于:所述p-GaP电流扩展层(109)厚度为5μm,掺杂浓度大于1×1018cm-3
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CN111478181A (zh) * 2019-01-23 2020-07-31 潍坊华光光电子有限公司 一种多波长激光器的制备方法
CN112909138A (zh) * 2021-01-04 2021-06-04 华灿光电(苏州)有限公司 AlGaInP发光二极管的外延片及其制备方法
CN112909138B (zh) * 2021-01-04 2022-05-20 华灿光电(苏州)有限公司 AlGaInP发光二极管的外延片及其制备方法

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