CN106328773B - A kind of iii-nitride light emitting devices and preparation method thereof - Google Patents
A kind of iii-nitride light emitting devices and preparation method thereof Download PDFInfo
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- 150000004767 nitrides Chemical class 0.000 claims abstract description 46
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- 238000004519 manufacturing process Methods 0.000 claims abstract description 6
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- 238000002488 metal-organic chemical vapour deposition Methods 0.000 claims description 6
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- 229910002546 FeCo Inorganic materials 0.000 claims description 4
- 238000000151 deposition Methods 0.000 claims description 4
- 238000000407 epitaxy Methods 0.000 claims description 3
- 229910019974 CrSi Inorganic materials 0.000 claims description 2
- 229910052748 manganese Inorganic materials 0.000 claims description 2
- QDOXWKRWXJOMAK-UHFFFAOYSA-N chromium(III) oxide Inorganic materials O=[Cr]O[Cr]=O QDOXWKRWXJOMAK-UHFFFAOYSA-N 0.000 claims 1
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- SZVJSHCCFOBDDC-UHFFFAOYSA-N iron(II,III) oxide Inorganic materials O=[Fe]O[Fe]O[Fe]=O SZVJSHCCFOBDDC-UHFFFAOYSA-N 0.000 claims 1
- 239000000203 mixture Substances 0.000 claims 1
- 150000002830 nitrogen compounds Chemical group 0.000 claims 1
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- H—ELECTRICITY
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- 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]
- H10H20/01—Manufacture or treatment
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- H10H20/013—Manufacture or treatment of bodies, e.g. forming semiconductor layers having light-emitting regions comprising only Group III-V materials
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- H10H20/80—Constructional details
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- 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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- H10H—INORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
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- H10H20/80—Constructional details
- H10H20/84—Coatings, e.g. passivation layers or antireflective coatings
- H10H20/841—Reflective coatings, e.g. dielectric Bragg reflectors
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Abstract
本发明公开了一种氮化物发光二极管及其制作方法,在P型氮化物和N型氮化物中插入应力控制层/反射层/电磁场发生层的复合结构,在电流通过电磁场发生层时,因电磁感应产生磁场,控制应力控制层产生应力,从而调控多量子阱受的应力类型和大小,提高发光二极管的o光比例和量子阱的载流子跃迁复合效率,提升发光效率和改善efficiency droop效应。
The invention discloses a nitride light-emitting diode and a manufacturing method thereof. A composite structure of a stress control layer/reflection layer/electromagnetic field generating layer is inserted into a P-type nitride and an N-type nitride. When a current passes through the electromagnetic field generating layer, due to Electromagnetic induction generates a magnetic field, and controls the stress control layer to generate stress, thereby regulating the type and magnitude of stress received by multiple quantum wells, improving the o-light ratio of light-emitting diodes and the carrier transition recombination efficiency of quantum wells, improving luminous efficiency and improving the efficiency droop effect .
Description
技术领域technical field
本发明涉及半导体光电器件领域,特别是一种氮化物发光二极管及其制作方法。The invention relates to the field of semiconductor optoelectronic devices, in particular to a nitride light-emitting diode and a manufacturing method thereof.
背景技术Background technique
现今,发光二极管(LED),特别是氮化物发光二极管因其较高的发光效率,在普通照明领域已取得广泛的应用。III族氮化物发光二极管为单轴介质晶体,其波动方程存在两种不同的解,一种沿光轴传播的寻常光线,简称o光(Ordinary Light),其电场E与光轴垂直E⊥c;另一种垂直光轴传播的非常光线,简称e光(Extraordinary),其电场E与光轴平行E∥c。o光为电子从导带底至重空穴带和轻空穴带的跃迁,而e光为电子从导带底至晶体场分裂出的空穴带的跃迁。对于III族氮化物发光二极管,材料的发光主要为电子从导带底至价带顶的空穴跃迁复合,由于III族氮化物存在光学各向异性,平行于c轴的光不易出射。Nowadays, light-emitting diodes (LEDs), especially nitride light-emitting diodes, have been widely used in the field of general lighting due to their high luminous efficiency. Group III nitride light-emitting diodes are uniaxial dielectric crystals, and there are two different solutions to the wave equation. One kind of ordinary light propagates along the optical axis, referred to as o light (Ordinary Light), and its electric field E is perpendicular to the optical axis E⊥c ; Another extraordinary ray propagating perpendicular to the optical axis, referred to as e light (Extraordinary), its electric field E is parallel to the optical axis E∥c. The o light is the transition of electrons from the bottom of the conduction band to the heavy hole band and the light hole band, and the e light is the transition of electrons from the bottom of the conduction band to the hole band split by the crystal field. For III-nitride light-emitting diodes, the luminescence of the material is mainly the recombination of electrons from the bottom of the conduction band to the top of the valence band. Due to the optical anisotropy of III-nitrides, light parallel to the c-axis is not easy to exit.
氮化物发光二极管在电流流入的情况下,电子注入会使晶格膨胀,同时,热效应会使衬底和外延层的应力发生改变,从而使其受到的压应力变小(参考文献:ScientificReports, 5:17227; DOI: 10.1038/srep17227)。随着注入电流的上升,压应力逐渐降至零,并变为张应力,并伴随着发光效率的急剧下降。为了获得较高的发光效率,改善Efficiency Droop效应,有必要提升在注入条件下氮化物发光二极管的压应力。When the current flows in the nitride light-emitting diode, the electron injection will expand the crystal lattice, and at the same time, the thermal effect will change the stress of the substrate and the epitaxial layer, so that the compressive stress it receives will be reduced (reference: ScientificReports, 5 :17227; DOI: 10.1038/srep17227). As the injection current increases, the compressive stress gradually drops to zero and turns into tensile stress, accompanied by a sharp drop in luminous efficiency. In order to obtain higher luminous efficiency and improve the Efficiency Droop effect, it is necessary to increase the compressive stress of the nitride light-emitting diode under implantation conditions.
发明内容Contents of the invention
为解决上述技术问题,本发明的目的在于:提供一种氮化物发光二极管及其制作方法,在P型氮化物和N型氮化物中插入应力控制层/反射层/电磁场发生层的复合结构,在电流通过电磁场发生层时,因电磁感应产生磁场,控制应力控制层产生应力,从而调控多量子阱受的应力类型和大小,提高发光二极管的o光比例和量子阱的载流子跃迁复合效率,提升发光效率和改善efficiency droop效应。In order to solve the above-mentioned technical problems, the purpose of the present invention is to provide a nitride light-emitting diode and its manufacturing method, inserting a composite structure of stress control layer/reflective layer/electromagnetic field generating layer in P-type nitride and N-type nitride, When the current passes through the electromagnetic field generation layer, a magnetic field is generated due to electromagnetic induction, and the stress control layer generates stress, thereby regulating the type and magnitude of the stress received by the multi-quantum wells, and improving the o-light ratio of the light-emitting diode and the carrier transition recombination efficiency of the quantum wells , enhance luminous efficiency and improve efficiency droop effect.
根据本发明的第一方面:一种氮化物发光二极管,依次包括衬底,缓冲层,N型氮化物,多量子阱以及P型氮化物,其特征在于:在所述P型氮化物和N型氮化物中插入应力控制层/反射层/电磁场发生层组成的复合结构。According to the first aspect of the present invention: a nitride light-emitting diode, which sequentially includes a substrate, a buffer layer, an N-type nitride, multiple quantum wells, and a P-type nitride, is characterized in that: the P-type nitride and the N-type A composite structure composed of a stress control layer/reflection layer/electromagnetic field generation layer inserted into a type nitride.
反射层用于防止电磁场发生层和应力控制层材料吸收多量子阱发出的光,当电流流经电磁场发生层时引起电磁感应效应,产生磁场;磁场控制应力控制层产生应力,从而调控多量子阱受的应力类型和大小,提高发光二极管的o光比例和量子阱的载流子跃迁复合效率,提升发光效率和改善efficiency droop效应。The reflective layer is used to prevent the materials of the electromagnetic field generation layer and the stress control layer from absorbing the light emitted by the multi-quantum wells. When the current flows through the electromagnetic field generation layer, it will cause an electromagnetic induction effect and generate a magnetic field; the magnetic field controls the stress control layer to generate stress, thereby regulating the multi-quantum wells The type and size of the stress, improve the o-light ratio of the light-emitting diode and the carrier transition recombination efficiency of the quantum well, improve the luminous efficiency and improve the efficiency droop effect.
进一步地,所述电磁场发生层随发光二极管的电流注入引起电磁感应产生磁场,该磁场的大小受电磁发生层的磁性材料和注入电流大小控制。Further, the electromagnetic field generating layer generates a magnetic field by electromagnetic induction with the current injection of the light emitting diode, and the magnitude of the magnetic field is controlled by the magnetic material of the electromagnetic generating layer and the magnitude of the injected current.
进一步地,所述P型氮化物和N型氮化物中插入应力控制层的位置一一对应,应力控制层材料为磁致弹性材料,受到磁场作用时,晶格常数会发生改变,从而产生张应力或压应力。Further, the position of inserting the stress control layer in the P-type nitride and the N-type nitride corresponds to each other, and the material of the stress control layer is a magnetoelastic material, and when subjected to a magnetic field, the lattice constant will change, thereby generating tension stress or compressive stress.
进一步地,所述应力控制层的厚度为10~900nm,优选500nm。Further, the stress control layer has a thickness of 10-900 nm, preferably 500 nm.
进一步地,所述反射层的材料为Al、DBR、ODR或以上三种的组合,优选DBR。Further, the material of the reflective layer is Al, DBR, ODR or a combination of the above three, preferably DBR.
进一步地,所述电磁场发生层为磁性材料,包含Ni、Co、Mn、FeCo、Fe3O4、Cr2O3、Fe2CrSi等单质或化合物的纳米球,大小为10~900nm,优选200nm。Further, the electromagnetic field generating layer is a magnetic material, including Ni, Co, Mn, FeCo, Fe 3 O 4 , Cr 2 O 3 , Fe 2 CrSi and other simple substances or nanospheres of compounds, with a size of 10-900nm, preferably 200nm .
根据本发明的第二方面:一种氮化物发光二极管的制作方法,包含以下步骤:According to a second aspect of the present invention: a method for manufacturing a nitride light-emitting diode, comprising the following steps:
(1)在衬底上依次外延生长缓冲层,N型氮化物,形成第一外延片;(1) Epitaxial growth of buffer layer and N-type nitride on the substrate in sequence to form the first epitaxial wafer;
(2)将第一外延片取出反应室,在N型氮化物上蚀刻出第一沟道,然后依次沉积电磁场发生层,再沉积反射层和磁致弹性材料,形成第一模板;(2) Take the first epitaxial wafer out of the reaction chamber, etch the first channel on the N-type nitride, then deposit the electromagnetic field generating layer in sequence, and then deposit the reflective layer and magnetoelastic material to form the first template;
(3)将第一模板重新放入MOCVD反应室,进行二次外延生长N型氮化物、多量子阱、P型氮化物,形成第二外延片;(3) Put the first template back into the MOCVD reaction chamber for secondary epitaxial growth of N-type nitride, multiple quantum wells, and P-type nitride to form a second epitaxial wafer;
(4)将第二外延片取出反应室,蚀刻出第二沟道,然后依次沉积应力控制层、反射层和电磁场发生层,该沟道与第一沟道的坐标一一对应,形成第二模板;(4) Take the second epitaxial wafer out of the reaction chamber, etch out the second channel, and then deposit the stress control layer, reflective layer and electromagnetic field generating layer in sequence. The coordinates of the channel correspond to the first channel one by one, forming the second channel. template;
(5)将第二模板重新放入MOCVD反应室,进行三次外延生长P型氮化物,形成最终的第三外延片。(5) Put the second template back into the MOCVD reaction chamber, and perform epitaxial growth of P-type nitride three times to form the final third epitaxial wafer.
进一步地,所述第一沟道、第二沟道的深度为100~1000nm,长度为1~10μm,宽度为1~10μm 。Further, the first channel and the second channel have a depth of 100-1000 nm, a length of 1-10 μm, and a width of 1-10 μm.
附图说明Description of drawings
图1为本发明实施例的氮化物发光二极管的示意图。FIG. 1 is a schematic diagram of a nitride light emitting diode according to an embodiment of the present invention.
图2为本发明实施例的氮化物发光二极管与传统发光二极管在不同电流作用下的应力差异比较图。FIG. 2 is a comparison diagram of the stress difference between the nitride light-emitting diode of the embodiment of the present invention and the traditional light-emitting diode under different currents.
图示说明:100:衬底,101:缓冲层,102:N型氮化物,103:电磁场发生层,104:反射层,105:应力控制层,106:多量子阱,107:P型层。Illustration: 100: substrate, 101: buffer layer, 102: N-type nitride, 103: electromagnetic field generating layer, 104: reflective layer, 105: stress control layer, 106: multiple quantum wells, 107: P-type layer.
具体实施方式Detailed ways
本发明所提出的一种氮化物发光二极管,依次包括衬底100,缓冲层101,N型氮化物102,应力控制层103/反射层104/电磁场发生层105的复合结构,多量子阱106,P型氮化物107,在P型氮化物107和N型氮化物102中插入应力控制层/DBR/电磁场发生层的复合结构,反射层104用于防止电磁场发生层吸光,当电流流经电磁场发生层105时产生电磁感应效应,产生磁场;磁场控制应力控制层103产生应力,从而调控多量子阱受的应力类型和大小,提高发光二极管的o光比例和量子阱的载流子跃迁复合效率,提升发光效率和改善efficiency droop。A nitride light-emitting diode proposed by the present invention sequentially includes a substrate 100, a buffer layer 101, an N-type nitride 102, a composite structure of a stress control layer 103/reflective layer 104/electromagnetic field generating layer 105, a multiple quantum well 106, P-type nitride 107, a composite structure of stress control layer/DBR/electromagnetic field generation layer inserted in P-type nitride 107 and N-type nitride 102, reflective layer 104 is used to prevent the electromagnetic field generation layer from absorbing light, when the current flows through the electromagnetic field When the layer 105 produces an electromagnetic induction effect, a magnetic field is generated; the magnetic field controls the stress to control the layer 103 to generate stress, thereby regulating the type and size of the stress received by the multi-quantum wells, improving the o-light ratio of the light-emitting diode and the carrier transition recombination efficiency of the quantum wells, Improve luminous efficiency and improve efficiency droop.
首先,在蓝宝石衬底100上依次外延生长衬底100,缓冲层101,N型氮化物102,形成第一外延片;然后,将第一外延片取出,在N型氮化物102上蚀刻出第一沟道,深度为1μm,长度为2μm,宽度为2μm,分别沉积200nmFeCo纳米球的电磁场发生层,再沉积DBR和500nm的磁致弹性材料,作为应力控制层103,形成第一模板;接着,将第一模板重新放入MOCVD反应室,进行二次外延,继续生长N型氮化物盖住应力控制层103/DBR反射率104/电磁场发生层105的复合结构,继续生长多量子阱106和P型氮化物107,形成第二外延片;然后,将第二外延片取出蚀刻出第二沟道,深度为1μm,长度为2μm,宽度为2μm,在沟道上依次沉积500nm的磁致弹性材料的应力控制层103、DBR反射层104和200nm粒径的FeCo纳米球的电磁场发生层105,形成第二模板;最后,将第二模板重新放入MOCVD反应室,进行三次外延继续生长P型氮化物107,盖住应力控制层103/DBR反射层104/电磁场发生层105的复合结构。First, on the sapphire substrate 100, epitaxially grow the substrate 100, the buffer layer 101, and the N-type nitride 102 in order to form the first epitaxial wafer; then, take out the first epitaxial wafer, and etch the first epitaxial wafer on the N-type nitride 102. A channel with a depth of 1 μm, a length of 2 μm, and a width of 2 μm, respectively depositing an electromagnetic field generating layer of 200 nm FeCo nanospheres, and then depositing a DBR and a 500 nm magnetoelastic material as the stress control layer 103 to form a first template; then, Put the first template back into the MOCVD reaction chamber, perform secondary epitaxy, continue to grow N-type nitride to cover the composite structure of stress control layer 103/DBR reflectivity 104/electromagnetic field generation layer 105, and continue to grow multiple quantum wells 106 and P type nitride 107 to form a second epitaxial wafer; then, take out the second epitaxial wafer and etch a second trench with a depth of 1 μm, a length of 2 μm, and a width of 2 μm, and sequentially deposit 500 nm of magnetoelastic material on the trench Stress control layer 103, DBR reflective layer 104, and electromagnetic field generating layer 105 of FeCo nanospheres with a particle size of 200nm form a second template; finally, put the second template back into the MOCVD reaction chamber for three epitaxy to continue growing P-type nitride 107 , covering the composite structure of the stress control layer 103 /DBR reflective layer 104 /electromagnetic field generating layer 105 .
当电流流经电磁场发生层时,产生磁场,且磁场随着电流的上升而增强,控制磁致弹性材料产生压应力,以抵消因发光二极管结温上升和电流注入产生的压应力的减小,如图2所示;当注入电流小于300mA时,由电磁场产生的压应力小于发光二极管的压应力减少的幅度,发光二极管的多量子阱受到的压应力呈下降趋势;当注入电流超过300mA时,由电磁场产生的压应力大于发光二极管的压应力减少的幅度,发光二极管的多量子阱受到的压应力呈上升趋势。上升的压应力可以提高发光二极管的o光比例和量子阱的载流子跃迁复合效率,提升发光效率和改善efficiency droop。When the current flows through the electromagnetic field generating layer, a magnetic field is generated, and the magnetic field increases as the current rises, and the magnetoelastic material is controlled to generate compressive stress to offset the decrease in the compressive stress caused by the rise in the junction temperature of the light-emitting diode and the current injection. As shown in Figure 2; when the injection current is less than 300mA, the compressive stress generated by the electromagnetic field is less than the magnitude of the reduction of the compressive stress of the light-emitting diode, and the compressive stress received by the multiple quantum wells of the light-emitting diode shows a downward trend; when the injection current exceeds 300mA, The compressive stress generated by the electromagnetic field is greater than the reduction range of the compressive stress of the light-emitting diode, and the compressive stress suffered by the multiple quantum wells of the light-emitting diode shows an upward trend. The rising compressive stress can improve the o-light ratio of the light-emitting diode and the carrier transition recombination efficiency of the quantum well, improve the luminous efficiency and improve the efficiency droop.
以上实施方式仅用于说明本发明,而并非用于限定本发明,本领域的技术人员,在不脱离本发明的精神和范围的情况下,可以对本发明做出各种修饰和变动,因此所有等同的技术方案也属于本发明的范畴,本发明的专利保护范围应视权利要求书范围限定。The above embodiments are only used to illustrate the present invention, rather than to limit the present invention. Those skilled in the art can make various modifications and changes to the present invention without departing from the spirit and scope of the present invention. Therefore, all Equivalent technical solutions also belong to the category of the present invention, and the scope of patent protection of the present invention should be limited according to the scope of claims.
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| CN105047771A (en) * | 2015-07-10 | 2015-11-11 | 厦门市三安光电科技有限公司 | Nitride light emitting diode |
| CN105098000A (en) * | 2014-05-16 | 2015-11-25 | 北京纳米能源与系统研究所 | Composite structure of regulating LED luminous intensity through magnetic field, and manufacturing method |
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| CN105098000A (en) * | 2014-05-16 | 2015-11-25 | 北京纳米能源与系统研究所 | Composite structure of regulating LED luminous intensity through magnetic field, and manufacturing method |
| CN105047771A (en) * | 2015-07-10 | 2015-11-11 | 厦门市三安光电科技有限公司 | Nitride light emitting diode |
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