CN104779328A - LED structure - Google Patents
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- CN104779328A CN104779328A CN201410014540.5A CN201410014540A CN104779328A CN 104779328 A CN104779328 A CN 104779328A CN 201410014540 A CN201410014540 A CN 201410014540A CN 104779328 A CN104779328 A CN 104779328A
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- 239000004065 semiconductor Substances 0.000 claims abstract description 69
- 229910002601 GaN Inorganic materials 0.000 claims abstract description 47
- RNQKDQAVIXDKAG-UHFFFAOYSA-N aluminum gallium Chemical compound [Al].[Ga] RNQKDQAVIXDKAG-UHFFFAOYSA-N 0.000 claims abstract description 28
- 239000000758 substrate Substances 0.000 claims abstract description 12
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 claims description 20
- 229910052782 aluminium Inorganic materials 0.000 claims description 16
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 16
- 239000000463 material Substances 0.000 claims description 16
- AJGDITRVXRPLBY-UHFFFAOYSA-N aluminum indium Chemical compound [Al].[In] AJGDITRVXRPLBY-UHFFFAOYSA-N 0.000 claims description 2
- 238000010276 construction Methods 0.000 claims 13
- 239000004411 aluminium Substances 0.000 claims 4
- 241000209094 Oryza Species 0.000 claims 2
- 235000007164 Oryza sativa Nutrition 0.000 claims 2
- 235000009566 rice Nutrition 0.000 claims 2
- 229910002704 AlGaN Inorganic materials 0.000 abstract description 65
- 238000000605 extraction Methods 0.000 description 6
- XLOMVQKBTHCTTD-UHFFFAOYSA-N Zinc monoxide Chemical compound [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 3
- 230000007547 defect Effects 0.000 description 3
- 238000000407 epitaxy Methods 0.000 description 2
- -1 indium tin zinc Indium tin zinc oxide Chemical compound 0.000 description 2
- 230000031700 light absorption Effects 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- 239000011787 zinc oxide Substances 0.000 description 2
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- 238000002835 absorbance Methods 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- JAONJTDQXUSBGG-UHFFFAOYSA-N dialuminum;dizinc;oxygen(2-) Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Al+3].[Al+3].[Zn+2].[Zn+2] JAONJTDQXUSBGG-UHFFFAOYSA-N 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 229910052733 gallium Inorganic materials 0.000 description 1
- 229910052738 indium Inorganic materials 0.000 description 1
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 1
- AMGQUBHHOARCQH-UHFFFAOYSA-N indium;oxotin Chemical compound [In].[Sn]=O AMGQUBHHOARCQH-UHFFFAOYSA-N 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 229910052594 sapphire Inorganic materials 0.000 description 1
- 239000010980 sapphire Substances 0.000 description 1
- YVTHLONGBIQYBO-UHFFFAOYSA-N zinc indium(3+) oxygen(2-) Chemical compound [O--].[Zn++].[In+3] YVTHLONGBIQYBO-UHFFFAOYSA-N 0.000 description 1
Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/81—Bodies
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/81—Bodies
- H10H20/811—Bodies having quantum effect structures or superlattices, e.g. tunnel junctions
- H10H20/812—Bodies having quantum effect structures or superlattices, e.g. tunnel junctions within the light-emitting regions, e.g. having quantum confinement structures
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/81—Bodies
- H10H20/822—Materials of the light-emitting regions
- H10H20/824—Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP
- H10H20/825—Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
- H10H20/00—Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
- H10H20/80—Constructional details
- H10H20/83—Electrodes
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Abstract
Description
技术领域technical field
本发明是有关于一种半导体结构,且特别是有关于一种发光二极管结构。The present invention relates to a semiconductor structure, and more particularly to a light emitting diode structure.
背景技术Background technique
随着半导体科技的进步,现今的发光二极管已具备了高亮度的输出,加上发光二极管具有省电、体积小、低电压驱动以及不含汞等优点,因此发光二极管已广泛地应用在显示器与照明等领域。一般而言,发光二极管采用宽带隙半导体材料,如氮化镓(GaN)等材料,来进行制造。然而,当发光二极管的发光层放出近UV光或蓝光时,采用氮化镓所形成的P型半导体层会吸收波长约为365~490奈米左右的光,即会吸收近UV光与蓝光,进而影响整体发光二极管的出光效率。With the advancement of semiconductor technology, today's light-emitting diodes have a high-brightness output. In addition, light-emitting diodes have the advantages of power saving, small size, low-voltage drive, and mercury-free. Therefore, light-emitting diodes have been widely used in displays and lighting and other fields. Generally speaking, light-emitting diodes are manufactured using wide-bandgap semiconductor materials, such as gallium nitride (GaN) and other materials. However, when the light-emitting layer of the light-emitting diode emits near-UV light or blue light, the P-type semiconductor layer formed by gallium nitride will absorb light with a wavelength of about 365-490 nm, that is, it will absorb near-UV light and blue light. This further affects the light extraction efficiency of the overall light emitting diode.
发明内容Contents of the invention
本发明提供一种发光二极管结构,其具有较佳的出光效率。The invention provides a light emitting diode structure with better light extraction efficiency.
本发明的发光二极管结构,其包括基板、N型半导体层、发光层以及P型半导体层。N型半导体层配置于基板上。发光层适于发出主要发光波长介于365奈米至490奈米之间的光且配置于N型半导体层上。P型半导体层配置于发光层上,且包括P型氮化铝镓层。P型氮化铝镓层的厚度占整体P型半导体层的厚度的85%以上。The LED structure of the present invention includes a substrate, an N-type semiconductor layer, a light-emitting layer and a P-type semiconductor layer. The N-type semiconductor layer is configured on the substrate. The light-emitting layer is suitable for emitting light with a main light-emitting wavelength between 365 nm and 490 nm and is disposed on the N-type semiconductor layer. The P-type semiconductor layer is disposed on the light-emitting layer and includes a P-type AlGaN layer. The thickness of the P-type AlGaN layer accounts for more than 85% of the thickness of the entire P-type semiconductor layer.
在本发明的一实施例中,上述的P型半导体层为P型氮化铝镓层。In an embodiment of the present invention, the above-mentioned P-type semiconductor layer is a P-type AlGaN layer.
在本发明的一实施例中,上述的P型半导体层还包括P型氮化镓层,配置于P型氮化铝镓层上。P型氮化镓层的厚度占整体P型半导体层的厚度的15%以下。In an embodiment of the present invention, the above-mentioned P-type semiconductor layer further includes a P-type GaN layer disposed on the P-type AlGaN layer. The thickness of the P-type gallium nitride layer accounts for less than 15% of the thickness of the entire P-type semiconductor layer.
在本发明的一实施例中,上述的P型氮化铝镓层包括第一P型氮化铝镓层以及第二P型氮化铝镓层。第一P型氮化铝镓层中的铝含量不同于第二P型氮化铝镓层中的铝含量。In an embodiment of the present invention, the above-mentioned P-type AlGaN layer includes a first P-type AlGaN layer and a second P-type AlGaN layer. The aluminum content in the first P-type AlGaN layer is different from the aluminum content in the second P-type AlGaN layer.
在本发明的一实施例中,上述的第一P型氮化铝镓层位于第二P型氮化铝镓层与发光层之间,且第一P型氮化铝镓层中的铝含量大于第二P型氮化铝镓层中的铝含量。In an embodiment of the present invention, the above-mentioned first P-type AlGaN layer is located between the second P-type AlGaN layer and the light-emitting layer, and the aluminum content in the first P-type AlGaN layer greater than the aluminum content in the second P-type AlGaN layer.
在本发明的一实施例中,上述的第一P型氮化铝镓层的材料为AlxGa1-xN,且x为0.09~0.2。In an embodiment of the present invention, the material of the above-mentioned first P-type AlGaN layer is AlxGa1-xN, and x is 0.09˜0.2.
在本发明的一实施例中,上述的第二P型氮化铝镓层的材料为AlyGa1-yN,且y为0.01~0.15。In an embodiment of the present invention, the material of the second P-type AlGaN layer is AlyGa1-yN, and y is 0.01˜0.15.
在本发明的一实施例中,上述的第二P型氮化铝镓层的厚度大于第一P型氮化铝镓层的厚度。In an embodiment of the present invention, the thickness of the second P-type AlGaN layer is greater than the thickness of the first P-type AlGaN layer.
在本发明的一实施例中,上述的第一P型氮化铝镓层中的P型掺杂浓度大于第二P型氮化铝镓层的P型掺杂浓度。In an embodiment of the present invention, the P-type doping concentration in the first P-type AlGaN layer is greater than the P-type doping concentration in the second P-type AlGaN layer.
在本发明的一实施例中,上述的P型半导体层还包括P型氮化铝铟镓层,配置于P型氮化铝镓层与发光层之间。In an embodiment of the present invention, the above-mentioned P-type semiconductor layer further includes a P-type AlInGaN layer disposed between the P-type AlGaN layer and the light-emitting layer.
在本发明的一实施例中,上述的N型半导体层为N型氮化镓层。In an embodiment of the present invention, the above-mentioned N-type semiconductor layer is an N-type GaN layer.
在本发明的一实施例中,上述的发光二极管结构,还包括N型电极以及P型电极。N型电极配置于未被发光层所覆盖的N型半导体层上,且与N型半导体层电性连接。P型电极配置于P型半导体层上,且与P型半导体层电性连接。In an embodiment of the present invention, the above light emitting diode structure further includes an N-type electrode and a P-type electrode. The N-type electrode is arranged on the N-type semiconductor layer not covered by the light-emitting layer, and is electrically connected with the N-type semiconductor layer. The P-type electrode is disposed on the P-type semiconductor layer and electrically connected with the P-type semiconductor layer.
在本发明的一实施例中,上述的发光二极管结构还包括透明导电层,配置于P型半导体层上。In an embodiment of the present invention, the above light emitting diode structure further includes a transparent conductive layer disposed on the P-type semiconductor layer.
基于上述,由于本发明的P型氮化铝镓层的厚度占整体P型半导体层的厚度的85%以上,因此可以降低P型半导体层吸收发光层所发出的近UV光或蓝光。如此一来,本发明的发光二极管结构可具有较佳的出光效率。Based on the above, since the thickness of the P-type AlGaN layer of the present invention accounts for more than 85% of the thickness of the entire P-type semiconductor layer, it can reduce the absorption of near-UV light or blue light emitted by the light-emitting layer by the P-type semiconductor layer. In this way, the light emitting diode structure of the present invention can have better light extraction efficiency.
为让本发明的上述特征和优点能更明显易懂,下文特举实施例,并配合所附附图作详细说明如下。In order to make the above-mentioned features and advantages of the present invention more comprehensible, the following specific embodiments are described in detail together with the accompanying drawings.
附图说明Description of drawings
图1示出为本发明的一实施例的一种发光二极管结构的剖面示意图;FIG. 1 shows a schematic cross-sectional view of a light emitting diode structure according to an embodiment of the present invention;
图2示出为本发明的另一实施例的一种发光二极管结构的剖面示意图;2 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention;
图3示出为本发明的另一实施例的一种发光二极管结构的剖面示意图;3 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention;
图4示出为本发明的另一实施例的一种发光二极管结构的剖面示意图;4 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention;
图5示出为本发明的另一实施例的一种发光二极管结构的剖面示意图;5 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention;
图6示出为本发明的另一实施例的一种发光二极管结构的剖面示意图。FIG. 6 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention.
附图标记说明:Explanation of reference signs:
100a、100b、100c、100d、100e、100f:发光二极管结构;100a, 100b, 100c, 100d, 100e, 100f: light emitting diode structure;
110:基板;110: substrate;
120:N型半导体层;120: N-type semiconductor layer;
130:发光层;130: luminescent layer;
140a、140b、140c、140d、140e:P型半导体层;140a, 140b, 140c, 140d, 140e: P-type semiconductor layer;
142a、142b、142d:P型氮化铝镓层;142a, 142b, 142d: P-type aluminum gallium nitride layer;
142c1、142e1:第一P型氮化铝镓层;142c1, 142e1: the first P-type aluminum gallium nitride layer;
142c2、142e2:第二P型氮化铝镓层;142c2, 142e2: the second P-type aluminum gallium nitride layer;
144b:P型氮化镓层;144b: P-type gallium nitride layer;
144d、144e:P型氮化铝铟镓层;144d, 144e: P-type aluminum indium gallium nitride layer;
150:N型电极;150: N-type electrode;
160:P型电极;160: P-type electrode;
170:透明导电层;170: transparent conductive layer;
T1、T2:厚度。T1, T2: Thickness.
具体实施方式Detailed ways
图1示出为本发明的一实施例的一种发光二极管结构的剖面示意图。请参考图1,在本实施例中,发光二极管结构100a包括基板110、N型半导体层120、发光层130以及P型半导体层140a。N型半导体层120配置于基板110上。发光层130适于发出主要发光波长介于365奈米至490奈米之间的光且配置于N型半导体层120上。P型半导体层140a配置于发光层130上,且包括P型氮化铝镓层142a。P型氮化铝镓层142a的厚度占整体P型半导体层140a的厚度的85%以上。FIG. 1 is a schematic cross-sectional view of a light emitting diode structure according to an embodiment of the present invention. Please refer to FIG. 1 , in the present embodiment, the LED structure 100 a includes a substrate 110 , an N-type semiconductor layer 120 , a light-emitting layer 130 and a P-type semiconductor layer 140 a. The N-type semiconductor layer 120 is disposed on the substrate 110 . The light-emitting layer 130 is suitable for emitting light with a main light-emitting wavelength between 365 nm and 490 nm and is disposed on the N-type semiconductor layer 120 . The P-type semiconductor layer 140a is disposed on the light emitting layer 130 and includes a P-type AlGaN layer 142a. The thickness of the P-type AlGaN layer 142a accounts for more than 85% of the thickness of the entire P-type semiconductor layer 140a.
详细来说,在本实施例中,基板110例如是蓝宝石基板,而发光层130例如是氮化镓/氮化铟镓的量子井结构,但并不以此为限。N型半导体层120位于基板110与发光层130之间,且N型半导体层120的一部分暴露于发光层130之外。此处,N型半导体层120具体为N型氮化镓层。如图1所示,本实施例的P型半导体层140a具体为P型氮化铝镓层142a,意即整层的P型半导体层140a是由单一材料,即氮化铝镓,所形成。较佳地,P型氮化铝镓层142a的厚度为30奈米至100奈米。此外,本实施例的发光二极管结构100a还包括N型电极150以及P型电极160,其中N型电极150配置于未被发光层130所覆盖的N型半导体层120上且与N型半导体层120电性连接,而P型电极160配置于P型半导体层140a上且与P型半导体层140a电性连接。由上述元件的配置可得知,本实施例的发光二极管结构100a具体为蓝色发光二极管结构。In detail, in this embodiment, the substrate 110 is, for example, a sapphire substrate, and the light emitting layer 130 is, for example, a gallium nitride/indium gallium nitride quantum well structure, but not limited thereto. The N-type semiconductor layer 120 is located between the substrate 110 and the light-emitting layer 130 , and a part of the N-type semiconductor layer 120 is exposed outside the light-emitting layer 130 . Here, the N-type semiconductor layer 120 is specifically an N-type gallium nitride layer. As shown in FIG. 1 , the P-type semiconductor layer 140a of this embodiment is specifically a P-type AlGaN layer 142a, which means that the entire P-type semiconductor layer 140a is formed of a single material, ie, AlGaN. Preferably, the thickness of the P-type AlGaN layer 142a is 30 nm to 100 nm. In addition, the light emitting diode structure 100a of this embodiment also includes an N-type electrode 150 and a P-type electrode 160, wherein the N-type electrode 150 is disposed on the N-type semiconductor layer 120 not covered by the light-emitting layer 130 and is connected to the N-type semiconductor layer 120 are electrically connected, and the P-type electrode 160 is disposed on the P-type semiconductor layer 140a and electrically connected to the P-type semiconductor layer 140a. It can be seen from the arrangement of the above components that the light emitting diode structure 100 a of this embodiment is specifically a blue light emitting diode structure.
由于本实施例P型半导体层140a具体为P型氮化铝镓层142a,且P型氮化铝镓层142a材料特性并不会吸收近UV光或蓝色光波段的光线。因此,当发光层130发出光线时,光线可直接通过P型半导体层140a且不会被吸收。如此一来,本实施例的发光二极管结构100a可具有较佳的出光效率。Since the P-type semiconductor layer 140a in this embodiment is specifically the P-type AlGaN layer 142a, and the material properties of the P-type AlGaN layer 142a do not absorb light in the near-UV light or blue light band. Therefore, when the light-emitting layer 130 emits light, the light can directly pass through the P-type semiconductor layer 140a without being absorbed. In this way, the light emitting diode structure 100a of this embodiment can have better light extraction efficiency.
在此必须说明的是,下述实施例沿用前述实施例的元件标号与部分内容,其中采用相同的标号来表示相同或近似的元件,并且省略了相同技术内容的说明。关于省略部分的说明可参考前述实施例,下述实施例不再重复赘述。It must be noted here that the following embodiments use the component numbers and part of the content of the previous embodiments, wherein the same numbers are used to denote the same or similar components, and descriptions of the same technical content are omitted. For the description of omitted parts, reference may be made to the foregoing embodiments, and the following embodiments will not be repeated.
图2示出为本发明的另一实施例的一种发光二极管结构的剖面示意图。请参考图2,本实施例的发光二极管结构100b与图1的发光二极管结构100a相似,但二者主要差异之处在于:本实施例的P型半导体层140b是由P型氮化铝镓层142b以及P型氮化镓层144b所组成,其中P型氮化镓层144b配置于P型氮化铝镓层142b上。特别是,在本实施例中,P型氮化铝镓层142b的厚度占整体P型半导体层140b的厚度的85%以上,换言之,P型氮化镓层144b的厚度占整体P型半导体层140b的厚度的15%以下。较佳地,P型氮化镓层144b的厚度小于10奈米。FIG. 2 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention. Please refer to FIG. 2, the light emitting diode structure 100b of this embodiment is similar to the light emitting diode structure 100a of FIG. 142b and a P-type GaN layer 144b, wherein the P-type GaN layer 144b is disposed on the P-type AlGaN layer 142b. In particular, in this embodiment, the thickness of the P-type GaN layer 142b accounts for more than 85% of the thickness of the overall P-type semiconductor layer 140b, in other words, the thickness of the P-type GaN layer 144b accounts for 15% or less of the thickness of 140b. Preferably, the thickness of the P-type GaN layer 144b is less than 10 nm.
由于本实施例P型氮化铝镓层142b的厚度占整体P型半导体层140b的厚度的85%以上,且P型氮化铝镓层142b材料特性并不会吸收蓝色光波段的光线。依据比尔-朗伯定律(Beer–Lambert law)可得知,当一束平行单色光垂直通过某一均匀非散射的吸光物质时,其吸光度与吸光物质的浓度及吸收层厚度成正比。故,当发光层130发出光线时,由于会吸收蓝色光波的P型氮化镓层144b的厚度远小于P型氮化铝镓层142b的厚度,因此可以降低P型半导体层140b吸收发光层130所发出的近UV光或蓝光。如此一来,本实施例的发光二极管结构100b可具有较佳的出光效率。In this embodiment, the thickness of the P-type AlGaN layer 142b accounts for more than 85% of the thickness of the entire P-type semiconductor layer 140b, and the material properties of the P-type AlGaN layer 142b do not absorb blue light. According to the Beer-Lambert law, when a beam of parallel monochromatic light passes through a uniform non-scattering light-absorbing substance vertically, its absorbance is proportional to the concentration of the light-absorbing substance and the thickness of the absorbing layer. Therefore, when the light-emitting layer 130 emits light, since the thickness of the P-type gallium nitride layer 144b that absorbs blue light waves is much smaller than the thickness of the P-type aluminum gallium nitride layer 142b, the absorption of the light-emitting layer by the P-type semiconductor layer 140b can be reduced. 130 emits near UV light or blue light. In this way, the light emitting diode structure 100b of this embodiment can have better light extraction efficiency.
图3示出为本发明的另一实施例的一种发光二极管结构的剖面示意图。请参考图3,本实施例的发光二极管结构100c与图1的发光二极管结构100a相似,但二者主要差异之处在于:本实施例的P型半导体层140c具体为P型氮化铝镓层,其中P型氮化铝镓层包括第一P型氮化铝镓层142c1以及第二P型氮化铝镓层142c2,且第一P型氮化铝镓层142c1中的铝含量不同于第二P型氮化铝镓层142c2中的铝含量。较佳地,第一P型氮化铝镓层142c1位于第二P型氮化铝镓层142c2与发光层130之间,且第一P型氮化铝镓层142c1中的铝含量大于第二P型氮化铝镓层142c2中的铝含量。此处,第一P型氮化铝镓层142c1的材料为AlxGa1-xN,其中x为0.09~0.2。第二P型氮化铝镓层142c2的材料为AlyGa1-yN,其中的y为0.01~0.15。第二P型氮化铝镓层142c2的厚度T2大于第一P型氮化铝镓层142c1的厚度T1。FIG. 3 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention. Please refer to FIG. 3, the light emitting diode structure 100c of this embodiment is similar to the light emitting diode structure 100a of FIG. , wherein the P-type AlGaN layer includes a first P-type AlGaN layer 142c1 and a second P-type AlGaN layer 142c2, and the aluminum content in the first P-type AlGaN layer 142c1 is different from that of the first P-type AlGaN layer 142c1 Al content in the P-type AlGaN layer 142c2. Preferably, the first P-type AlGaN layer 142c1 is located between the second P-type AlGaN layer 142c2 and the light-emitting layer 130, and the aluminum content in the first P-type AlGaN layer 142c1 is greater than that of the second P-type AlGaN layer 142c1. Aluminum content in the P-type AlGaN layer 142c2. Here, the material of the first P-type AlGaN layer 142c1 is AlxGa1 -xN , where x is 0.09˜0.2. The material of the second P-type AlGaN layer 142c2 is AlyGa1 -yN , where y is 0.01˜0.15. The thickness T2 of the second P-type AlGaN layer 142c2 is greater than the thickness T1 of the first P-type AlGaN layer 142c1.
需说明的是,P型氮化铝镓层可减少吸光,但若P型氮化铝镓层中的铝含量太高,则较多的磊晶缺陷会造成复合载流子的损失且增加发光二极管结构内部的热量。再者,P型氮化铝镓层中的铝含量增加会造成另外一项影响,便是会使得p型氮化铝镓层阻值增加并使得电极制造更加困难。因此,本实施例的发光二极管结构100c通过靠近发光层130的第一P型氮化铝镓层142c1,其铝含量高,带隙(bandgap)会比较大,电子阻挡的效果比较好,能将未掉入的发光层130的电子弹回发光层130内,以增加光的效率。此外,第一P型氮化铝镓层142c1的厚度T1较薄,因此可减少因高含量的铝所造成的磊晶缺陷。It should be noted that the P-type AlGaN layer can reduce light absorption, but if the aluminum content in the P-type AlGaN layer is too high, more epitaxial defects will cause the loss of recombined carriers and increase the light emission. Heat inside the diode structure. Furthermore, the increase of the aluminum content in the p-type AlGaN layer will cause another effect, which is to increase the resistance of the p-type AlGaN layer and make electrode fabrication more difficult. Therefore, the light-emitting diode structure 100c of this embodiment passes through the first P-type aluminum gallium nitride layer 142c1 close to the light-emitting layer 130, which has a high aluminum content, a relatively large bandgap, and a relatively good electron blocking effect, which can Electrons that do not fall into the light emitting layer 130 bounce back into the light emitting layer 130 to increase light efficiency. In addition, the thickness T1 of the first P-type AlGaN layer 142c1 is relatively thin, so the epitaxial defects caused by the high content of Al can be reduced.
此外,本实施例的第一P型氮化铝镓层142c1中的P型掺杂浓度大于第二P型氮化铝镓层142c2的P型掺杂浓度。其中,P型掺杂多可以提供较多的空穴,而第一P型氮化铝镓层142c1较靠近发光层130,空穴容易进入发光层130,使空穴与电子在发光层130中相遇而接合,就以光子的形式释放出来。In addition, the P-type doping concentration in the first P-type AlGaN layer 142c1 of this embodiment is greater than the P-type doping concentration in the second P-type AlGaN layer 142c2. Among them, more P-type doping can provide more holes, and the first P-type aluminum gallium nitride layer 142c1 is closer to the light-emitting layer 130, and the holes can easily enter the light-emitting layer 130, so that holes and electrons in the light-emitting layer 130 When they meet and bond, they are released in the form of photons.
图4示出为本发明的另一实施例的一种发光二极管结构的剖面示意图。请参考图4,本实施例的发光二极管结构100d与图1的发光二极管结构100a相似,但二者主要差异之处在于:本实施例的P型半导体层140d是由P型氮化铝镓层142d以及P型氮化铝铟镓层144d所组成,其中P型氮化铝铟镓层144d配置于P型氮化铝镓层142d与发光层130之间。在本实施例中,P型氮化铝铟镓层144d可减缓P型氮化铝镓层142d与发光层130之间材料晶格不匹配的现象,可降低发光二极管结构100d在磊晶时产生的应力。FIG. 4 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention. Please refer to FIG. 4, the light emitting diode structure 100d of this embodiment is similar to the light emitting diode structure 100a of FIG. 142d and a P-type AlInGaN layer 144d, wherein the P-type AlInGaN layer 144d is disposed between the P-type AlInGaN layer 142d and the light emitting layer 130 . In this embodiment, the P-type AlInGaN layer 144d can alleviate the material lattice mismatch between the P-type AlGaN layer 142d and the light-emitting layer 130, and can reduce the generation of the light-emitting diode structure 100d during epitaxy. of stress.
图5示出为本发明的另一实施例的一种发光二极管结构的剖面示意图。请参考图5,本实施例的发光二极管结构100e与图1的发光二极管结构100a相似,但二者主要差异之处在于:本实施例的P型半导体层140e是由第一P型氮化铝镓层142e1、第二P型氮化铝镓层142e2以及P型氮化铝铟镓层144e所组成。第一P型氮化铝镓层142e1中的铝含量不同于第二P型氮化铝镓层142e2中的铝含量,较佳地,第一P型氮化铝镓层142e1的材料为AlxGa1-xN,其中x为0.09~0.2,而第二P型氮化铝镓层142e2的材料为AlyGa1-yN,其中的y为0.01~0.15。利用第一P型氮化铝镓层142e1与第二P型氮化铝镓层142e2的铝含量不同,可以避免吸光,同时又可减少磊晶缺陷及阻值高的问题。第一P型氮化铝镓层142e1配置于第二P型氮化铝镓层142e2与P型氮化铝铟镓层144e之间,而P型氮化铝铟镓层144e直接接触发光层130。P型氮化铝铟镓层144e可减缓第一P型氮化铝镓层142e1与发光层130之间材料晶格不匹配的现象,可降低发光二极管结构100e在磊晶时产生的应力。FIG. 5 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention. Please refer to FIG. 5, the light emitting diode structure 100e of this embodiment is similar to the light emitting diode structure 100a of FIG. The gallium layer 142e1 is composed of the second P-type AlGaN layer 142e2 and the P-type AlInGaN layer 144e. The aluminum content in the first P-type AlGaN layer 142e1 is different from the Al content in the second P-type AlGaN layer 142e2. Preferably, the material of the first P-type AlGaN layer 142e1 is Al x Ga 1-x N, wherein x is 0.09˜0.2, and the material of the second P-type aluminum gallium nitride layer 142e2 is AlyGa 1-y N, wherein y is 0.01˜0.15. By utilizing the difference in aluminum content between the first P-type AlGaN layer 142e1 and the second P-type AlGaN layer 142e2, light absorption can be avoided, and problems of epitaxial defects and high resistance can be reduced at the same time. The first P-type AlGaN layer 142e1 is disposed between the second P-type AlGaN layer 142e2 and the P-type AlInGaN layer 144e, and the P-type AlInGaN layer 144e directly contacts the light-emitting layer 130 . The P-type AlInGaN layer 144e can reduce the material lattice mismatch between the first P-type AlGaN layer 142e1 and the light-emitting layer 130, and can reduce the stress generated during epitaxy of the light-emitting diode structure 100e.
图6示出为本发明的另一实施例的一种发光二极管结构的剖面示意图。请参考图6,本实施例的发光二极管结构100f与图1的发光二极管结构100a相似,但二者主要差异之处在于:本实施例的发光二极管结构100f还包括透明导电层170,其中透明导电层170配置于P型半导体层140a上,且位于P型半导体层140a与P型电极160之间。P型半导体层140a可通过透明导电层170与P型电极160形成良好的欧姆接触(ohmic contact)。此处,透明导电层170的材质例如为铟锡氧化物(indium tin oxide,简称ITO)、铟锌氧化物(indium zinc oxide,简称IZO)、氧化锌(zinc oxide,简称ZnO)、铟锡锌氧化物(indium tin zinc oxide,简称ITZO)、铝锡氧化物(aluminum tin oxide,简称ATO)、铝锌氧化物(aluminum zinc oxide,简称AZO)或其他适当的透明导电材质。FIG. 6 is a schematic cross-sectional view of a light emitting diode structure according to another embodiment of the present invention. Please refer to FIG. 6, the light emitting diode structure 100f of this embodiment is similar to the light emitting diode structure 100a of FIG. The layer 170 is disposed on the P-type semiconductor layer 140 a and is located between the P-type semiconductor layer 140 a and the P-type electrode 160 . The P-type semiconductor layer 140 a can form a good ohmic contact with the P-type electrode 160 through the transparent conductive layer 170 . Here, the material of the transparent conductive layer 170 is, for example, indium tin oxide (ITO for short), indium zinc oxide (IZO for short), zinc oxide (ZnO for short), indium tin zinc Indium tin zinc oxide (ITZO for short), aluminum tin oxide (ATO for short), aluminum zinc oxide (AZO for short) or other appropriate transparent conductive materials.
综上所述,由于本发明的P型氮化铝镓层的厚度占整体P型半导体层的厚度的85%以上,因此可以降低P型半导体层吸收发光层所发出的近UV光或蓝光。如此一来,本发明的发光二极管结构可具有较佳的出光效率。In summary, since the thickness of the P-type AlGaN layer of the present invention accounts for more than 85% of the thickness of the entire P-type semiconductor layer, it can reduce the absorption of near-UV light or blue light emitted by the light-emitting layer by the P-type semiconductor layer. In this way, the light emitting diode structure of the present invention can have better light extraction efficiency.
最后应说明的是:以上各实施例仅用以说明本发明的技术方案,而非对其限制;尽管参照前述各实施例对本发明进行了详细的说明,本领域的普通技术人员应当理解:其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分或者全部技术特征进行等同替换;而这些修改或者替换,并不使相应技术方案的本质脱离本发明各实施例技术方案的范围。Finally, it should be noted that: the above embodiments are only used to illustrate the technical solutions of the present invention, rather than limiting them; although the present invention has been described in detail with reference to the foregoing embodiments, those of ordinary skill in the art should understand that: It is still possible to modify the technical solutions described in the foregoing embodiments, or perform equivalent replacements for some or all of the technical features; and these modifications or replacements do not make the essence of the corresponding technical solutions deviate from the technical solutions of the various embodiments of the present invention. scope.
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