TW201103163A - Nitirde semiconductor light emitting diode device and method of fabricating the same - Google Patents
Nitirde semiconductor light emitting diode device and method of fabricating the same Download PDFInfo
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- 239000004065 semiconductor Substances 0.000 title claims abstract description 79
- 238000004519 manufacturing process Methods 0.000 title description 7
- 150000004767 nitrides Chemical class 0.000 claims abstract description 116
- 230000004888 barrier function Effects 0.000 claims abstract description 115
- 239000000758 substrate Substances 0.000 claims abstract description 57
- 239000000463 material Substances 0.000 claims description 80
- 230000000737 periodic effect Effects 0.000 claims description 16
- 239000011777 magnesium Substances 0.000 claims description 7
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 claims description 6
- FYYHWMGAXLPEAU-UHFFFAOYSA-N Magnesium Chemical compound [Mg] FYYHWMGAXLPEAU-UHFFFAOYSA-N 0.000 claims description 6
- 229910052749 magnesium Inorganic materials 0.000 claims description 6
- 229910052757 nitrogen Inorganic materials 0.000 claims description 6
- 150000001875 compounds Chemical class 0.000 claims description 5
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical group [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 claims description 5
- 229910052594 sapphire Inorganic materials 0.000 claims description 5
- 239000010980 sapphire Substances 0.000 claims description 5
- 229910052727 yttrium Inorganic materials 0.000 claims description 5
- VWQVUPCCIRVNHF-UHFFFAOYSA-N yttrium atom Chemical compound [Y] VWQVUPCCIRVNHF-UHFFFAOYSA-N 0.000 claims description 5
- 239000011701 zinc Substances 0.000 claims description 5
- HCHKCACWOHOZIP-UHFFFAOYSA-N Zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 claims description 4
- 229910052725 zinc Inorganic materials 0.000 claims description 4
- XLOMVQKBTHCTTD-UHFFFAOYSA-N zinc oxide Inorganic materials [Zn]=O XLOMVQKBTHCTTD-UHFFFAOYSA-N 0.000 claims description 3
- 229910002601 GaN Inorganic materials 0.000 claims description 2
- KJTLSVCANCCWHF-UHFFFAOYSA-N Ruthenium Chemical compound [Ru] KJTLSVCANCCWHF-UHFFFAOYSA-N 0.000 claims description 2
- 238000010030 laminating Methods 0.000 claims description 2
- 229910003465 moissanite Inorganic materials 0.000 claims description 2
- 229910052707 ruthenium Inorganic materials 0.000 claims description 2
- 229910010271 silicon carbide Inorganic materials 0.000 claims description 2
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 claims 2
- 230000003287 optical effect Effects 0.000 claims 2
- 208000001613 Gambling Diseases 0.000 claims 1
- 229910052786 argon Inorganic materials 0.000 claims 1
- 125000005842 heteroatom Chemical group 0.000 claims 1
- 229910052741 iridium Inorganic materials 0.000 claims 1
- GKOZUEZYRPOHIO-UHFFFAOYSA-N iridium atom Chemical compound [Ir] GKOZUEZYRPOHIO-UHFFFAOYSA-N 0.000 claims 1
- 238000000034 method Methods 0.000 description 20
- 238000009826 distribution Methods 0.000 description 12
- 238000010586 diagram Methods 0.000 description 10
- 239000013078 crystal Substances 0.000 description 9
- 239000004020 conductor Substances 0.000 description 8
- 239000012535 impurity Substances 0.000 description 8
- 230000000694 effects Effects 0.000 description 6
- 238000005229 chemical vapour deposition Methods 0.000 description 5
- 125000002524 organometallic group Chemical group 0.000 description 5
- 230000015572 biosynthetic process Effects 0.000 description 4
- 230000007547 defect Effects 0.000 description 4
- 238000003475 lamination Methods 0.000 description 4
- 238000001451 molecular beam epitaxy Methods 0.000 description 4
- 230000000903 blocking effect Effects 0.000 description 3
- 238000000605 extraction Methods 0.000 description 3
- 229910052732 germanium Inorganic materials 0.000 description 3
- 238000005121 nitriding Methods 0.000 description 3
- 210000004508 polar body Anatomy 0.000 description 3
- 229910052691 Erbium Inorganic materials 0.000 description 2
- UYAHIZSMUZPPFV-UHFFFAOYSA-N erbium Chemical compound [Er] UYAHIZSMUZPPFV-UHFFFAOYSA-N 0.000 description 2
- QJGQUHMNIGDVPM-UHFFFAOYSA-N nitrogen group Chemical group [N] QJGQUHMNIGDVPM-UHFFFAOYSA-N 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 230000009467 reduction Effects 0.000 description 2
- 239000004575 stone Substances 0.000 description 2
- 238000007740 vapor deposition Methods 0.000 description 2
- 229910002704 AlGaN Inorganic materials 0.000 description 1
- 241000238631 Hexapoda Species 0.000 description 1
- IOVCWXUNBOPUCH-UHFFFAOYSA-M Nitrite anion Chemical compound [O-]N=O IOVCWXUNBOPUCH-UHFFFAOYSA-M 0.000 description 1
- 229910052772 Samarium Inorganic materials 0.000 description 1
- -1 Sic Substances 0.000 description 1
- 229910007709 ZnTe Inorganic materials 0.000 description 1
- 235000019994 cava Nutrition 0.000 description 1
- 210000004027 cell Anatomy 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 229910000366 copper(II) sulfate Inorganic materials 0.000 description 1
- JZCCFEFSEZPSOG-UHFFFAOYSA-L copper(II) sulfate pentahydrate Chemical compound O.O.O.O.O.[Cu+2].[O-]S([O-])(=O)=O JZCCFEFSEZPSOG-UHFFFAOYSA-L 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 238000005538 encapsulation Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000407 epitaxy Methods 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- BIXHRBFZLLFBFL-UHFFFAOYSA-N germanium nitride Chemical group N#[Ge]N([Ge]#N)[Ge]#N BIXHRBFZLLFBFL-UHFFFAOYSA-N 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 229910052746 lanthanum Inorganic materials 0.000 description 1
- FZLIPJUXYLNCLC-UHFFFAOYSA-N lanthanum atom Chemical compound [La] FZLIPJUXYLNCLC-UHFFFAOYSA-N 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000002488 metal-organic chemical vapour deposition Methods 0.000 description 1
- 239000008267 milk Substances 0.000 description 1
- 210000004080 milk Anatomy 0.000 description 1
- 235000013336 milk Nutrition 0.000 description 1
- KZUNJOHGWZRPMI-UHFFFAOYSA-N samarium atom Chemical compound [Sm] KZUNJOHGWZRPMI-UHFFFAOYSA-N 0.000 description 1
- 239000004576 sand Substances 0.000 description 1
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 239000002689 soil Substances 0.000 description 1
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- 230000008016 vaporization Effects 0.000 description 1
- 238000009834 vaporization Methods 0.000 description 1
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Abstract
Description
201103163 P51970143TW 29729twf.doc/n 六、發明說明: 【發明所屬之技術領域】 別是ΪΓ—種半導體元件及其製造方法,且特 物半導體發光二極體—蚱 diode ’ LED)元件及其製造方法。 【先前技術】 高效㈣勃發展, 因同時具有高發光效能 j。+導體化合物材料 價格低廉等優點,逐漸成調變範圍大、 物半導體材料適合作為該光至/ 、机。其中,氮化 可以應用於全彩顯示器、發光q t之發光波段的材料, 導體雷射等方面,特別是, 肢、咼頻電子元件、半 元件’ ϋ此受卿泛注意。L目自熱⑽藍光發光二極體 習知的發光二極體元 型摻雜層、主動層與P型摻雜/1序2成在基板上的N 型摻雜層分別電性連接及與N型摻雜層及p 阻障層及位於量子阻障層令的量子 1 :=,括二量子 (band gap)需大於量子 里子阻障層之能隙 後逃脫,以增加電子電洞對结:的::止载子掉入量子井 井的材料為响』,其中般而言,量子 層的材料會選擇與量子丄與1之間。量子阻障 ㈣場對發光效率的影變^吊數相近的_以減少 θ)踢加A】以提高量子阻障層 201103163 x -»^ /vi43TW 29729twf.doc/n 之能隙至大於量子井之能隙到一定程度,如 AUGaylriiiyN,其中X、y介於〇與1之間。然而,大量添 加A1含量會導致後續成長之量子井之結晶品質的下降,因 此容易造成凹洞(pits),增加漏電流,也無法有效抑制壓 電效應(piezo effect)及提升内部光取出效率(internal quantum efficiency ; IQE )。 美國專利公開案US20080093610中揭露了一種氮化 物半導體發光元件,其主動區之量子阻障層為多層 (腿ltilayer)結構。此專利之量子阻障層包括InGaN層、 AlInN層、及inGaN/GaN超晶格結構,可以與p型摻雜層 形成良好介面,且避免N型摻雜層之Mg擴散到主動層 中。然而,包含AlInN之量子阻障層若要有足夠大的能隙 差’A1含量需添加到15%以上,且是否能達到所需之量子 阻障仍然令人質疑。另外,大量提高Ai含量並無法有效降 低量子井與量子阻障層之間的壓電效應。 【發明内容】 Μ有f 2,Ϊ糾提供—種氮㈣料體發光二極體 夠幫助釋括:元氮化物的超晶格結構,能 止歸因於氮化物的超晶格結構,能夠防 之晶體缺陷,以提;阻P早層之間的晶格失配而產生 电子電洞對結合的機率,進而提升内 201103163 29729twf.doc/a 部光輸出效率。 本發明提出一種氮化物半導體發光二極體元件,包括 基才=、N型摻雜層、主動層、p型播雜層、第一電極 二電極。N雜雜層位於基板之—側 其包括至少一量子井結構。量子== 以及位於量子阻障層之間的量子井。量子 氮化物的超晶格結構°Ρ型摻雜層位於主動 雜層曝露出的平台上或位於基板的極位於Ν型摻 括施例中,上述之四元氮化物的材料包 ai—a-bN ’ a、b分別介於Oij之門 超晶格結構由週# 且a b<卜201103163 P51970143TW 29729twf.doc/n VI. Description of the invention: [Technical field of the invention] A semiconductor element and a method for manufacturing the same, and a semiconductor diode, a diode element, and a method of manufacturing the same . [Prior Art] Efficient (four) development, because of high luminous efficiency at the same time j. + Conductor compound material The advantages of low price, etc., gradually become a large range of modulation, and the material semiconductor material is suitable as the light to / machine. Among them, nitriding can be applied to full-color displays, materials for emitting light-emitting bands, conductor lasers, and the like, in particular, limbs, chirped electronic components, and half-components. L-directed self-heating (10) blue light-emitting diodes, the light-emitting diode-type doped layer, the active layer and the P-type doping/1 sequence 2 are electrically connected to the N-type doped layer on the substrate, respectively. The N-type doped layer and the p-barrier layer and the quantum 1 := located in the quantum barrier layer allow the band gap to escape larger than the energy gap of the quantum lining barrier layer to increase the electron hole to the junction :: The material that falls into the quantum well is the sound of the carrier. In general, the material of the quantum layer is chosen to be between the quantum 丄 and 1. Quantum Barrier (4) Field Effect on Luminous Efficiency ^The number of hangs is similar _ to reduce θ) Kicking A] to increase the energy barrier of the quantum barrier layer 201103163 x -»^ /vi43TW 29729twf.doc/n to be larger than the quantum well The energy gap is to a certain extent, such as AUGaylriiiyN, where X and y are between 〇 and 1. However, the large addition of the A1 content causes a decrease in the crystal quality of the subsequently grown quantum well, which tends to cause pits, increase leakage current, and effectively suppress the piezo effect and enhance the internal light extraction efficiency ( Internal quantum efficiency ; IQE ). A nitride semiconductor light-emitting element is disclosed in U.S. Patent Publication No. US20080093610, in which the quantum barrier layer of the active region is a multi-layered structure. The quantum barrier layer of this patent includes an InGaN layer, an AlInN layer, and an inGaN/GaN superlattice structure, which can form a good interface with the p-type doped layer and prevent Mg diffusion of the N-type doped layer into the active layer. However, if the quantum barrier layer containing AlInN has a sufficiently large energy gap, the 'A1 content needs to be added to more than 15%, and whether the desired quantum barrier can be achieved is still questionable. In addition, a large increase in the Ai content does not effectively reduce the piezoelectric effect between the quantum well and the quantum barrier layer. SUMMARY OF THE INVENTION Μ has f 2, Ϊ 提供 provides a nitrogen (four) material light-emitting diode can help to explain: the super-lattice structure of the meta-nitride, can be attributed to the superlattice structure of the nitride, capable of Prevent crystal defects, to improve the lattice mismatch between the early layers of P to produce the probability of electron hole pair bonding, and then improve the light output efficiency of the internal 201103163 29729twf.doc/a. The present invention provides a nitride semiconductor light-emitting diode element comprising a base, an N-type doped layer, an active layer, a p-type hybrid layer, and a first electrode and two electrodes. The N impurity layer is located on the side of the substrate and includes at least one quantum well structure. Quantum == and a quantum well located between the quantum barrier layers. Super-lattice structure of quantum nitride The Ρ-type doping layer is located on the exposed platform of the active impurity layer or the pole of the substrate is located in the 掺-type doping embodiment, and the above-mentioned quaternary nitride material package ai-a- bN ' a, b are respectively between the Oij gate superlattice structure by week # and a b<
層、週_ ^^〜的 A1JnbGai-a-bN層與 AlcIndGai.c dN * ^ Alt! A1JnbGai-N ^ 灿乂 :ΓΓbTN層與GaN層、或週期層疊白 d、七層所組成,其中C、 等於d。另冰如間’ d Ha不等於c,b不 且超晶格結敎職層㈣錄為至少兩次, 50_之^母—層的厚度例如是介於約〇·5 rnn至約Layer, week _ ^ ^ ~ A1JnbGai-a-bN layer and AlcIndGai.c dN * ^ Alt! A1JnbGai-N ^ Chan: ΓΓ bTN layer and GaN layer, or periodic stacking white d, seven layers, of which C, Equal to d. Another ice such as 'd Ha is not equal to c, b and the superlattice knotted layer (4) is recorded at least twice, the thickness of the 50_^^-layer is, for example, between about 〇·5 rnn to about
InfGawHH—貫施例中’上述之量子井的材料包括 in + p<1/ p IWpN’f、n、P分別介於〇與1之間, 介於約中’上述之量子井的厚度例如是 um玍約20 nm之間。 〜 201103163 P51970143TW 29729twf.doc/n 在本發明之一實施例中,上述之主動層的厚度例如3 介於約3 nm至約500 nm之間。 疋 在本發明之一實施例中’上述之主動層包括單—息 井結構。 里子 在本發明之一實施例中,上述之主動層包括多數 子井結構。 里 在本發明之一實施例中,上述之基板的材料包括藍 石、矽、SiC、ZnO 或 GaN。 在本發明之-實施例中,上述^型摻雜層的 括摻砍或錯的GaN。 在本發明之一實施例中,上述之^型 括摻鎂或鋅的GaN。 …的材枓包 在本發明之一實施例中,上述之氮化物半 括位於基板及Μ摻雜層之間的緩衝層= ^的 ^ 包括⑽、AlqGai_qN、Sic、Zn〇、ZnTe(^ gN ’其中q介於〇與1之間。 極體實闕+,上衫氮絲料體發光二 層。;δ力摻雜層及絲叙間的應力舒緩 ίη^_3層與GaN層組成 且層、,、°構,其中m介於_與0.3之間。 才㈣在明之—實施例中,上述之氮化物半導體發光-極體兀件更包括位於ρ 光- 觸層。 /雅層及第—電極之間的Ρ型接 在本發明之-實施财,上述之氮化物半導體發光二 201103163 P51970143TW 29729twf.doc/n 極體元件更包括位於P型摻雜層及主動層之間的電子阻障 層。 本發明另提出-種氮化物半導體發光二極體元件,包 括基板、N型摻雜層、主動層、p娜雜層、電子阻障層、 第-電極及第二電極。N型摻雜層位於基板之一側上 ==型摻雜層上,其包括至少-量子井結構。量子 二量子阻障層以及位於量子阻障層之間的量子 層及主位層上。電子阻障層位於Ρ型摻雜 曰丄 阻障層為包括四元氮化物的超 能隙高於量子阻障層的能隙。 A1 Int發明實施例中’ i述之四元氮化物的材料包括 AlgInhGai.g_hN,g、i^別介於 〇與 ^化括 超晶格結構由週期層聶的 g h<l。 層、週期層疊的A1 In G g h層與ΑΙίΙη^_ΗΝ 叠的 AlgInhGaij 、週期層InfGawHH—In the example, the material of the quantum well described above includes in + p <1/ p IWpN'f, n, P are between 〇 and 1, respectively, and the thickness of the quantum well described above is, for example, Um玍 is between about 20 nm. ~ 201103163 P51970143TW 29729twf.doc/n In one embodiment of the invention, the active layer has a thickness of, for example, 3 between about 3 nm and about 500 nm. In one embodiment of the invention, the active layer described above comprises a single-well structure. In one embodiment of the invention, the active layer comprises a majority sub-well structure. In an embodiment of the invention, the material of the substrate comprises bluestone, yttrium, SiC, ZnO or GaN. In an embodiment of the invention, the above-mentioned doped layer includes GaN doped or erroneous. In one embodiment of the invention, the above-described type includes GaN doped with magnesium or zinc. In one embodiment of the present invention, the nitride layer is provided in a buffer layer between the substrate and the erbium doped layer = ^^ including (10), AlqGai_qN, Sic, Zn〇, ZnTe (^ gN 'where q is between 〇 and 1. The polar body is 阙+, and the upper nitrite body emits two layers. The δ force-doped layer and the wire are relieved. ίη^_3 layer and GaN layer are composed and layer , wherein, m is between _ and 0.3. (4) In the embodiment, the nitride semiconductor light-emitting element further includes a photo-contact layer. - The Ρ type between the electrodes is connected to the present invention, and the above-mentioned nitride semiconductor light-emitting diode 201103163 P51970143TW 29729twf.doc/n the polar body element further includes an electron barrier between the P-type doped layer and the active layer The present invention further provides a nitride semiconductor light-emitting diode element comprising a substrate, an N-type doped layer, an active layer, a p-a hybrid layer, an electron barrier layer, a first electrode and a second electrode. The impurity layer is located on one side of the substrate on the == doped layer, which includes at least a quantum well structure. Quantum two quantum barrier And a quantum layer and a host layer between the quantum barrier layers. The electron barrier layer is located in the germanium-type doped germanium barrier layer, and the ultra-energy gap including the quaternary nitride is higher than the energy gap of the quantum barrier layer. The material of the quaternary nitride described in the embodiment of the invention includes AlgInhGai.g_hN, g, i, and g, and the superlattice structure is composed of g h<l of the periodic layer. Periodically stacked A1 In G gh layer and ΑΙίΙη^_ΗΝ stacked AlgInhGaij, periodic layer
AynhGai_g.hN層、j_ θ /週期層疊的 j、k分別介於〇與j之問々,.曰+?⑽層所組成,其中i、 等於j。另外,和曰 1』<1,且§不等於丨,}1不 、J另卜超日日格結構之週期 且超晶格結構中每_戶的,且的久數為至少兩次, 50 _之間。 叫度例如是介於約0.5職至約 在本料之―#_t,The AynhGai_g.hN layer, j_ θ / periodic lamination j, k are respectively composed of 〇 and j, 曰+?(10) layers, where i is equal to j. In addition, 曰1』<1, and § is not equal to 丨,}1 does not, J is the period of the super-day grid structure and every _ household in the superlattice structure, and the duration is at least twice. Between 50 _. The degree of calling is, for example, between about 0.5 and about _#_t in the material.
Ind.fN或AlnGajni N,f 里于开的材枓包括 P HpN f、n、P分別介於0與1之間, 201103163 P51970143TW 29729t\vf.doc/n 且 n + p < 在本發明之-實施例中,上述之量子井的厚度例 介於約1 nm至約20 nm之間。 在本發明之-實施例中,上述之主動層的厚度例 介於約3 nm至約500 nm之間。 在本發明之-實施例中,上述之主動層包 井結構。 平里千 • ㈣之—實施财,上述之主動層包括多數個量 子井結構。 i 在本發明之一實施例中,上述之基板的材料包括駐窗 石、矽、SiC、ZnO 或 GaN。 貝 祕之一實施例中’上述之N型摻雜層的材料包 括摻矽或鍺的GaN。 括摻明之一實施例中’上述之P型摻雜層的材料包 括摻鎂或鋅的GaN。 ♦ 之—實關中,上述之氮化物半導體發光二 彳 於基缺N雜闕之間的緩衝層。緩 =的::包,N、AlqGai·#、如、办… 其中q介於〇與1之間。 極體實施例中,上述之氮化物半導體發光二 芦ίϋ 型換雜層及主動層之間的應力舒緩 白韻的材料包括由InmG^N層與⑽層組成 I層、'、D構,其中m介於001與03之間。 在本發明之一實施例中,上述之氮化物半導體發光二 201103163 r-ί 1 ^ / υ 1 j IW 29729twf.doc/n =元件更包括位於P歸雜層及第—電極 觸層。 文 括αΪ發:ί出一種氮化物半導體發光二極體元件,包 摻雜層、主動層、ρ型掺雜層、電子阻障層、 =電極及第—電極。Ν型摻雜層位於基板之—側上。主 動曰位於Ν型摻雜層上,其包括至 二量子阻障層以及位於量子阻障層之t的;: 阻障層為包括第1元氮化物的第—超晶格結 構雜層位於主動 層及主動層之間,型摻雜 的ίίΓ 且電子阻障層的能隙高於量子阻障層 4雜層曝路出的平台上或位於基板的另一側上。 料勺明之一實施例中’上述之第-四元氮化物的材 枓包括AIaKGai_a_bN,a、b分別介於q與i之間,且& +匕 二7—超晶格結構由週期層疊的AlaInbGai.a.bN層盘 居ϋ日1層、週期層疊的A1JnbGai.a-bN層與1咖』 曰、θ 的AUnbGah.bN層與GaN層、或週期層蟲 的 AlaInbGai.bN 層、IneGai eN 層與 _ 層所組成,^ ; 別介於°與1之間,G + d<:l,h不等於c,b + 。,外,第一超晶格結構之週期層疊的次數為至The material in the Ind.fN or AlnGajni N,f includes P HpN f, n, P between 0 and 1, respectively, 201103163 P51970143TW 29729t\vf.doc/n and n + p < In an embodiment, the thickness of the quantum well described above is between about 1 nm and about 20 nm. In the embodiment of the invention, the thickness of the active layer is, for example, between about 3 nm and about 500 nm. In an embodiment of the invention, the active layer encapsulation structure described above. Ping Liqian • (4)—The implementation of the above-mentioned active layer includes most of the quantum well structures. In one embodiment of the invention, the material of the substrate comprises a window stone, ruthenium, SiC, ZnO or GaN. In one embodiment of the invention, the material of the above-mentioned N-type doped layer includes erbium-doped or erbium-doped GaN. The material of the P-type doped layer described above in one embodiment of the invention includes GaN doped with magnesium or zinc. ♦ In the real-time, the above-mentioned nitride semiconductor emits light in a buffer layer between the N-stacks. Slow =:: package, N, AlqGai·#, such as, do... where q is between 〇 and 1. In the polar body embodiment, the material for the stress relaxation whiteness between the nitride semiconductor light-emitting layer and the active layer includes an InmG^N layer and a (10) layer composed of an I layer, ', D structure, wherein m is between 001 and 03. In an embodiment of the present invention, the nitride semiconductor light-emitting device is further provided on the P-corrugated layer and the first-electrode contact layer. The invention includes a nitride semiconductor light-emitting diode element including a doped layer, an active layer, a p-type doped layer, an electron barrier layer, an =electrode and a first electrode. The erbium doped layer is on the side of the substrate. The active germanium is located on the germanium-type doped layer, and includes the second quantum barrier layer and the quantum barrier layer at t; the barrier layer is a first-superlattice structure impurity layer including the first-weight nitride Between the layer and the active layer, the energy gap of the type doped λ and the electron barrier layer is higher than the exposed surface of the quantum barrier layer 4 or on the other side of the substrate. In one embodiment of the present invention, the material of the above-mentioned quaternary nitride includes AAIKGai_a_bN, a and b are respectively between q and i, and the & +匕2-7-superlattice structure is periodically stacked. The AlaInbGai.a.bN layer is on the 1st floor, the A1JnbGai.a-bN layer and the 1ca 』 周期, the AUnbGah.bN layer and the GaN layer of the θ, or the AlaInbGai.bN layer of the periodic layer insect, IneGai eN The layer is composed of _ layer, ^ ; is between ° and 1, G + d <: l, h is not equal to c, b + . , outside, the number of times of the first superlattice structure is cascaded to
且第超0曰格結構中每一層的厚度例如是介於約 〇.5nm 至約 50nm 之間。 、、、J 本發明之一實施例中,上述之第二四元氮化物的材料 201103163 F51970143TW 29729twf.doc/n 包括AlgInhGai-g_hN,g、h分別介於〇與i之間,且g地< 1。第二超晶格結構由週期層疊的八^叫Gai_g hN層盘And the thickness of each of the super-zero grid structures is, for example, between about 〇.5 nm and about 50 nm. In one embodiment of the present invention, the second quaternary nitride material 201103163 F51970143TW 29729twf.doc/n includes AlgInhGai-g_hN, g and h are respectively between 〇 and i, and g is <; 1. The second superlattice structure is composed of periodically stacked eight-gauge Gai_g hN layer disks
AlJnjGawN層、週期層疊的叫邮〜钟N層與ΙηΛ㈤ 層、週期層疊的AlgInhGai.g.hN層與⑽層、或週期層叠 的AlglnhGai-g-hN層、InkGai_kN層與GaN層所組成,其中 1 Ί k分別介於G與1之間,i + j < i,且g不等於},匕 不等於j。另外,第二超晶格結構之週期層疊的次數為至The AlJnjGawN layer, the periodic layered layer of the mailing layer N and the ΙηΛ (five) layer, the periodically stacked AlgInhGai.g.hN layer and the (10) layer, or the periodically stacked AlglnhGai-g-hN layer, the InkGai_kN layer and the GaN layer, wherein Ί k is between G and 1, respectively, i + j < i, and g is not equal to }, and 匕 is not equal to j. In addition, the number of times of the second superlattice structure is cascaded to
J兩次,且第二超晶格結構中每—層的厚度例如是介於約 〇.5nm至約5〇nm之間。 在本發明之—實施例巾,上述之量子井的材料包括 nfGai-fN 或 AlnGapIn—N,f、n、p 分別介於 〇 盥 且 η + ρ< 1 〇 』J is twice, and the thickness of each layer in the second superlattice structure is, for example, between about 〇5 nm to about 5 〇 nm. In the embodiment of the present invention, the material of the quantum well includes nfGai-fN or AlnGapIn-N, and f, n, and p are respectively 〇 且 and η + ρ < 1 〇 』
在本發明之一實施例中, 介於約1 nm至約20 nm之間 在本發明之一實施例中, 介於約3nm至約500 nm之間 在本發明之一實施例中, 井結構。 在本發明之一實施例中, 子井結構。 在本發明之一實施例中, 石、砂、SiC、ZnO 或 GaN。 上述之量子井的厚度例如是 上述之主動層的厚度例如是 〇 上述之主動層包括單一量子 上述之主動層包括多數個量 上述之基板的材料包括藍寶 在本發明之一實施例中,上述 括穆石夕或錯的GaN。 U雜層的材料包 11 201103163 P51970143TW 29729twf.doc/n 在本發明之一實施例中 括摻鎮或辞的GaN。 上述之P型摻雜層的材料包 在本發日狀—纽财,上叙氮化物料體發光二 =兀件更包括位於基板及;^型摻雜層之間的缓衝層。缓 衝層的材料包括GaN、AlqGai qN、%、Zn〇、ZnTe〇或In one embodiment of the invention, between about 1 nm and about 20 nm, in one embodiment of the invention, between about 3 nm and about 500 nm, in one embodiment of the invention, the well structure . In an embodiment of the invention, the sub-well structure. In one embodiment of the invention, stone, sand, SiC, ZnO or GaN. The thickness of the quantum well is, for example, the thickness of the active layer, for example, the active layer includes a single quantum, and the active layer includes a plurality of materials of the substrate, including a sapphire. In an embodiment of the present invention, the above Including Mu Shi Xi or wrong GaN. Material package of U-hetero layer 11 201103163 P51970143TW 29729twf.doc/n In one embodiment of the invention, GaN is incorporated. The material of the P-type doped layer described above is included in the present invention, and the nitriding material of the nitriding material body includes a buffer layer between the substrate and the doped layer. The material of the buffer layer includes GaN, AlqGai qN, %, Zn〇, ZnTe〇 or
MgN,其中q介於〇與i之間。MgN, where q is between 〇 and i.
在本發明之-實施例中,上述之氮化物半導體發光二 f體元件更包括位於N型摻雜層及主動層之間的應力舒緩 層:應力舒缓層的材料包括由InmGai mN層與⑽層組成 的璺層結構,其中m介於〇 〇1與〇 3之間。 在本發明之-實施例中,上述之氮化物半導體發光二 極體7L件更包括位於P型摻雜層及第—電極之間㈣型接 觸層。 基於上述,本發明之量子阻障層為包括四元·物的 超晶格結構’㈣幫轉放絲叙應力,目此能有效 制壓電效應,提升後續成長之量子井的結晶品質,及減少In an embodiment of the invention, the nitride semiconductor light emitting body element further comprises a stress relaxation layer between the N-type doped layer and the active layer: the material of the stress relaxation layer comprises an InmGai mN layer and a (10) layer A layered structure consisting of m between 〇〇1 and 〇3. In the embodiment of the present invention, the nitride semiconductor light-emitting diode 7L further includes a (four) type contact layer between the P-type doped layer and the first electrode. Based on the above, the quantum barrier layer of the present invention is a superlattice structure including a quaternary material, and the effect of the piezoelectric effect is improved, thereby improving the crystal quality of the subsequently grown quantum well, and cut back
漏電流的發生。此外,本發明之電子轉層為包括另—四 凡氮化物的超日曰日格結構’能夠防止歸因於量子阻障層 子阻障層之間的晶格失配而產生之晶體缺陷,如錯 凹洞等等。 久 為讓本發明之上述特徵和優點能更明顯易懂,下文 舉實施例,並配合所附圖式作詳細說明如下。 、 【實施方式】 12 201103163 λ j i 7 / υ i*+3TW 29729twf.d〇c/n 第一實施例 目1A為依縣發㈣—實關鱗稍氮化物 體發光二極體元件之示意剖面圖。 睛參,圖1Α,首先,提供基板100。基板100的材料 例如是藍寶石(sapphire)、矽、Sic、Zn〇或GaN。接著, 於基板100的一側上形成!^型摻雜層1〇2。^_型摻雜層1〇2 的材料例如是摻石夕或鍺的GaN,且其形成方法例如是進行 有機金屬化學氣相沉積法(metalorganic chemical vapw • deposition ; M0CVD)。在一實施例中,N型擦雜層ι〇2 例如是具有平台(mesa) 1〇9,以供後續形成之第二 110之用。 在一貫施例中,在形成N型摻雜層1〇2的步驟之前, 也可以選擇性地於基板丨㈨及^^型摻雜層1〇2之間形成缓 衝$ 1(Π。缓衝層1〇1是作為缓衝N型摻雜層1〇2成長於 異質基板上而產生之晶格常數不匹配(lattice mismatch) 的問題。緩衝層ιοί的材料例如是GaN、AlqGai qN、Sic、 • Zn〇、ZnTe〇或MgN,其中q介於〇與1之間,且其形成 方法例如是進行低溫磊晶成長(4〇〇〜9〇〇。〇。 然後,於N型摻雜層1〇2上形成主動層。主動層 104的厚度例如是介於約3 nm至約5〇〇 nm之間。主動層 包括至少一量子井結構,其中此量子井結構包括依序 形成在N型摻雜層上1 〇2上的量子阻障層(quantum barder layer) l〇4a、量子井(quantum weu) i〇4b 及另一量子阻 障層104a。主動層l〇4也就是發光層,利用上述之量子井 13 201103163 j.W 29729twf.doc/n 結構’電子電洞對會在量子井1G4b中結合而釋放出光子。 本發明之量子阻障層l〇4a為包括四元氮化物 (quaternary nitride )的超晶格結構(哪⑷如以 structure)。換句話說’量子阻障層1〇知之超晶格結構的 材料可以為四兀氮化物與另_四元氣化物、四元氮化物與 二兀氮化物、四兀氮化物與二元氮化物、或四元氮化物、 二70氮化物與二元氮化物所組成。在一實施例中,量子阻 障層l〇4a之四元說化物的材料例如是八咖伽』,其中 a、b分別介於〇與1之間,且a + b < j。因此,量子阻障 · 層104a之超晶格結構可以由週期層疊(peri〇dica取 hm^ated)的 A1JnbGai-a-bN 層與 A1JndGai』層、週期 層®的AlJnbGanbN層與ineGai eN層、週期層疊的 AlaInbGai_a.bN 層與 GaN 層、或週期層疊的 A1JnbGai a_bN 層、heGa^N層與GaN層所組成,其中c、d、e分別介於 〇與1之間’ c + d < ;1 ’且a不等於c,b不等於d。上述 之超晶格結構之週期層疊的次數為至少兩次,且其每一層 的厚度例如是介於約〇.5nm至約5〇nm之間。圖1A的左 側,量子阻障層1()4a之能帶分佈圖(banddiag腿),自 · 於里子阻障層l〇4a為具有週期層疊之至少二材料層所形 成^超晶格結構’其中之-的材料為四元氮化物,因此其 能帶分佈圖呈週期變化。量子阻障層1〇如的厚度可以由超 晶格結構中之每一材料層的厚度及週期層叠的次數而決 定。 , 此外,1子井104b的材料例如是InfGai fN或 14 201103163 P51970143TW 29729twf.doc/nThe occurrence of leakage current. In addition, the electron-transferring layer of the present invention is a super-corrugated cell structure including the other-four nitrides, which can prevent crystal defects caused by lattice mismatch between the quantum barrier layer barrier layers. Such as wrong pits and so on. The above-described features and advantages of the present invention will become more apparent from the following description. [Embodiment] 12 201103163 λ ji 7 / υ i*+3TW 29729twf.d〇c/n The first embodiment is 1A is a schematic section of a light-emitting diode component of Yixianfa (4)-Shiguan scale-slightly nitrided object Figure. In the first place, the substrate 100 is provided. The material of the substrate 100 is, for example, sapphire, samarium, Sic, Zn or GaN. Next, it is formed on one side of the substrate 100! ^ Type doped layer 1 〇 2. The material of the ^_ type doped layer 1〇2 is, for example, GaN doped with lanthanum or yttrium, and is formed by, for example, metalorganic chemical vapw deposition (M0CVD). In one embodiment, the N-type wipe layer ι 2 is, for example, having a platform (mesa) 1 〇 9 for subsequent formation of the second 110. In a consistent embodiment, before the step of forming the N-type doped layer 1〇2, a buffer of $1 may be selectively formed between the substrate (9) and the doped layer 1〇2. The punch layer 1〇1 is a problem of lattice mismatch caused by the growth of the buffer N-type doped layer 1〇2 on a heterogeneous substrate. The material of the buffer layer ιοί is GaN, AlqGai qN, Sic, for example. • Zn〇, ZnTe〇 or MgN, where q is between 〇 and 1, and is formed by, for example, low-temperature epitaxial growth (4〇〇~9〇〇.〇. Then, in the N-type doped layer An active layer is formed on 1 2. The thickness of the active layer 104 is, for example, between about 3 nm and about 5 〇〇 nm. The active layer includes at least one quantum well structure, wherein the quantum well structure includes sequentially formed in the N-type a quantum barder layer l〇4a, a quantum well (i)4b, and another quantum barrier layer 104a on the doped layer. The active layer l〇4 is also a light-emitting layer. Using the above-mentioned quantum well 13 201103163 jW 29729twf.doc/n structure 'electronic hole pair will be combined in quantum well 1G4b to release photons The quantum barrier layer 104a of the present invention is a superlattice structure including quaternary nitride (which is, for example, in structure). In other words, the quantum barrier layer 1 is known as a superlattice structure. The material may be a tetra-n-nitride and another quaternary vapor, a quaternary nitride and a germanium nitride, a tetra-n-nitride and a binary nitride, or a quaternary nitride, a two-nitride and a binary nitride. In one embodiment, the material of the quaternary structure of the quantum barrier layer 10a is, for example, eight ga ga, wherein a and b are between 〇 and 1, respectively, and a + b < j. Therefore, the superlattice structure of the quantum barrier layer 104a can be formed by periodically laminating (A1JnbGai-a-bN layer and A1JndGai" layer of the peri〇dica, AlJnbGanbN layer and ineGai eN layer of the periodic layer®, period The stacked AlaInbGai_a.bN layer and the GaN layer, or the periodically stacked A1JnbGai a_bN layer, the heGa^N layer and the GaN layer, wherein c, d, and e are between 〇 and 1 respectively 'c + d < 'And a is not equal to c, b is not equal to d. The number of cycles of the superlattice structure described above is at least twice. The thickness of each layer is, for example, between about 〇5 nm and about 5 〇 nm. On the left side of Fig. 1A, the energy band distribution of the quantum barrier layer 1 () 4a (banddiag leg), from the lining barrier The layer l〇4a is a quaternary nitride in which the material of the super-lattice structure formed by at least two material layers which are periodically laminated, and thus the band diagram of the energy band changes periodically. The thickness of the quantum barrier layer 1 can be determined by the thickness of each material layer in the superlattice structure and the number of times of periodic lamination. In addition, the material of the 1 sub well 104b is, for example, InfGai fN or 14 201103163 P51970143TW 29729twf.doc/n
AlnGapInupN,其中f、η、p分別介於〇與i之間,且n + p < 1。量子井104b的厚度例如是介於約} nm至約2〇 nm 之間。另外,里子阻j1 早層l〇4a及量子井;i 〇4b的形成方法 例如是進行有機金屬化學氣相沉積法(metal〇rganic chemical vapor deposition ; MOCVD )或分子束磊晶法 (molecular-beam epitaxy ; MBE),且其生長溫度例如是介於 約600°C至約900°C之間。 # 在一實施例中,量子阻障層l〇4a例如是具有週期層疊 之AlaInbGai_a_bN層與lneGai_eN層所形成的超晶格結構, 且量子井104b的材料例如是Inf〇ai fN。首先,以有機金屬 化學氣相沉積法或分子束磊晶法於生長溫度6〇〇〜9〇〇。〇之 間於N型摻雜層1〇2上形成ineGal eN層,再於7〇〇〜90CTC 的溫度下於IneGai-eN層的表面形成AlaInbGai a bN層,然 後=週期層豐至少兩次的方式形成具有超晶格結構的量 子阻障層1Q4a。之後,於量子轉層l〇4a的表面於 60040(TC形成材料為Inf〇ai fN之量子井1〇牝。繼之,以 • t述的方法製作另-量子阻障層购於量子井1〇4b上, 元成八有單里子井結構(single quantum well structure ) 之主動層104。 特別要說明的是,由於本發明之量子阻障層104a為 =括四;^化物的超晶格結構,因此不但可以滿足量子阻 P早層之,隙至少大於量子井之能隙〇 2eV以上的需求,而 且^以幫助釋放主動層刚之應力,有效降低壓電效應。 另夕’本發明之量子阻障層1Q4a有助於提升後續成長之量 15 201103163 P5I970143TW 29729twf.doc/n 子井104b的結晶品質’降低缺陷凹洞的產生,、、| 電流的發生,及提升内部光取出效率。AlnGapInupN, where f, η, p are between 〇 and i, respectively, and n + p < The thickness of the quantum well 104b is, for example, between about Å nm and about 2 〇 nm. In addition, lining resists j1 early layer l〇4a and quantum well; i 〇4b is formed by metal 〇rganic chemical vapor deposition (MOCVD) or molecular beam epitaxy (molecular-beam). Epitaxy; MBE), and its growth temperature is, for example, between about 600 ° C and about 900 ° C. In one embodiment, the quantum barrier layer 10a is, for example, a superlattice structure formed by a layer of AlaInbGai_a_bN and a layer of lneGai_eN which are periodically stacked, and the material of the quantum well 104b is, for example, Inf〇ai fN. First, the growth temperature is 6 〇〇 to 9 以 by the organometallic chemical vapor deposition method or the molecular beam epitaxy method. An ineGal eN layer is formed on the N-doped layer 1〇2, and an AlaInbGai a bN layer is formed on the surface of the IneGai-eN layer at a temperature of 7〇〇~90CTC, and then the periodic layer is at least twice. The method forms a quantum barrier layer 1Q4a having a superlattice structure. Then, on the surface of the quantum layer l〇4a at 60040 (the TC forming material is a quantum well of Inf〇ai fN). Subsequently, another quantum barrier layer is fabricated by the method described in the t-quantum well 1 On 〇4b, Yuan Chengba has an active layer 104 of a single quantum well structure. In particular, since the quantum barrier layer 104a of the present invention is a quadruple structure, the superlattice structure of the compound is formed. Therefore, not only can the quantum resist P early layer be satisfied, the gap is at least greater than the energy gap of the quantum well 〇 2 eV or more, and ^ can help release the stress of the active layer and effectively reduce the piezoelectric effect. The barrier layer 1Q4a helps to increase the amount of subsequent growth. 15 201103163 P5I970143TW 29729twf.doc/n The crystal quality of the sub-well 104b reduces the generation of defective pits, the generation of current, and the efficiency of internal light extraction.
在-實施例中’在形成主動層1〇4的步驟 以選擇性地於N型摻雜層102及主動層1〇4 I 舒緩層(strain-release layer) 103。應力舒緩 ' 二 釋放主動層104之應力。應力舒緩層‘例Γ是ίIn the embodiment, the step of forming the active layer 1 〇 4 is performed to selectively the N-type doped layer 102 and the active layer 1 I 4 strain-release layer 103. The stress relieves the stress of the active layer 104. Stress relief layer ‘example is ί
InmGa卜mN層與GaN層所組成的叠芦姓 也她r〇,其中m介於0.01與0.3之^ j ( lamina_ 』―™1 Τη (Τ-ο χτThe InmGa b mN layer and the GaN layer are composed of the same name, and m is between 0.01 and 0.3 ^ j ( lamina_ 』 - TM1 Τη (Τ-ο χτ
層與GaN層的厚度例如是分別介於約 m 1'mN 丄 mi ^ 矣勺 5 0 π τη 間。應力舒缓層103的形成方法例如β隹〜” 氣相沉積法。 U疋進仃麵金屬化學 之後,請繼續參照圖认,於主動層1〇4上 :二二=法广是進行有機金屬化學氣相沉積 法。在-貫施例中,在形成ρ型換雜層106的步驟之前, 也可以於主動層刚及Ρ型摻雜層1G6之間形成電子阻障 層 105 (electron blocking layer)。電子阻障層 1〇5 是進— 步地阻擔電子逃出主動層刚,因此電子阻障層1〇5的能 隙局於量子阻障層馳的鋪。電子轉層奶例如為 AlGaN層或是A1GaN層與GaN層所域的超晶格結構。 繼之’於P型摻雜層106上形成第一電極·。第一 電極108 @材料例如是Cr/Au、IT〇 $ Zn〇。在一實施例 中,在形成第-電極108的步驟之前,也可以選擇性地於 P型摻雜層106及第-電極⑽之間形成p型接觸層ι〇7、。 16 201103163 P51970143TW 29729twf.doc/n P型接觸層107是作為降低P型摻雜層i〇6與第一電極i〇8 之間的阻抗。P型接觸層107的材料例如是摻鎂或鋅的 G aN ’且其形成方法例如是進行有機金屬化學氣相沉積法。The thickness of the layer and the GaN layer is, for example, between about m 1 'mN 丄 mi ^ 矣 5 5 0 π τη. The method for forming the stress relaxation layer 103 is, for example, β隹~” vapor deposition method. After U疋进仃面metal chemistry, please continue to refer to the figure, on the active layer 1〇4: 2nd=Faguang is performing organometallic chemistry Vapor deposition method. In the embodiment, an electron blocking layer 105 may be formed between the active layer and the doped layer 1G6 before the step of forming the p-type impurity layer 106. The electron barrier layer 1〇5 further resists electrons from escaping the active layer, so that the energy barrier of the electron barrier layer 1〇5 is spread over the quantum barrier layer. The electron-transferred layer milk is, for example, AlGaN. The layer is either a superlattice structure of the A1GaN layer and the GaN layer. Next, a first electrode is formed on the P-type doped layer 106. The first electrode 108 @material is, for example, Cr/Au, IT〇$ Zn〇 In an embodiment, a p-type contact layer ι7 may be selectively formed between the P-type doping layer 106 and the first electrode (10) before the step of forming the first electrode 108. 16 201103163 P51970143TW 29729twf The .doc/n P-type contact layer 107 serves to reduce the impedance between the P-type doping layer i〇6 and the first electrode i〇8. The material of the contact layer 107 is, for example, G aN ' doped with magnesium or zinc and is formed by, for example, performing an organometallic chemical vapor deposition method.
接著,於N型摻雜層102曝露出的平台1〇9上形成第 一電極no。第二電極11〇的材料例如是Ni/Au或 Ti/Al/Ti/Au。至此,完成第一實施例之氮化物半導體發光 一極體元件之製造流程。特別要說明的是,當基板1〇〇的 材料為導電材料如GaN時,第二電極110也可以形成於基 板100的另一側上’如圖1B所示,因此N型摻雜層1〇2 也不需要形成平台109供第二電極11〇之用。 曰 接下來,將說明第一實施例之氮化物半導體获# 一係 體元件的結構。請參照圖1AWB,本發明之氮 體發光二極體元件包括基板1〇〇、;^型摻雜層丨〇2、主動層 1〇4、p型摻雜層106、第一電極108及第二電極ιι〇。& 型摻雜層1〇2位於基板刚之一側上。主動層刚位於N 型換雜層102上,其包括至少一量子井結構。量子井结構 ,二量子阻障層HMa以及位於量子阻障層购之^的 Γ3。量子阻障層104a為包括四元氮化物的超晶 才。、、,。構。P型摻雜層106位於主動層1〇4上。 層觸上。第二電極11G位於N型摻雜層曝 =的平口磨上或位於基板刚的另—側上。此外,緩 =1“〇1位於基板則與N型摻雜層1〇2 <間,作 里推雜層102成長於異質基板上而產生之晶格常數 配的問題。應力舒緩層103位於N型摻雜層102及主動層 17 201103163. 29729twf.doc/n 104之間,作為釋放主動層l〇4之應力。電子阻障層ι〇5 位於主動層1〇4及P型摻雜層1〇6之間,以進—步^阻擋 電子逃出主動層10OP型接觸層107位於;p型換^層 及第一電極108之間,作為降低p型摻雜層1〇6與第a一電 極108之間的阻抗。 ' 上述之實施例是以包括單一量子井結構之主動層為 例來說明之’但本發明並不以此為限。熟知本技藝者^了 解’本發明之主動層也可以為多重量子井結構 quantum well structure)。也就是說,本發明之主動層包括 籲 多數個量子井結構,其中量子阻障層104a與量子井1〇扑 是以交替疊層至少兩次的方式配置在應力舒緩層1〇3上, 如圖1C及圖1D所示。 第二實施例 圖2A為依據本發明第二實施例所繪示的氮化物半導 體發光一極體元件之示意剖面圖。 凊參照圖2A,首先,提供基板2〇〇。接著,於基板2〇〇Next, a first electrode no is formed on the land 1〇9 exposed by the N-type doping layer 102. The material of the second electrode 11A is, for example, Ni/Au or Ti/Al/Ti/Au. Thus far, the manufacturing process of the nitride semiconductor light-emitting diode element of the first embodiment is completed. In particular, when the material of the substrate 1 is a conductive material such as GaN, the second electrode 110 may also be formed on the other side of the substrate 100 as shown in FIG. 1B, and thus the N-type doped layer 1〇 2 It is also not necessary to form the platform 109 for the second electrode 11 .曰 Next, the structure of the nitride semiconductor obtained by the first embodiment will be explained. Referring to FIG. 1AWB, the nitrogen-emitting diode component of the present invention comprises a substrate 1 , a doped layer 2 , an active layer 1 , a p-doped layer 106 , a first electrode 108 , and a first Two electrodes ιι〇. The & type doped layer 1〇2 is located on one side of the substrate. The active layer is just on the N-type impurity layer 102 and includes at least one quantum well structure. Quantum well structure, two quantum barrier layer HMa and Γ3 located in the quantum barrier layer. The quantum barrier layer 104a is a supercrystal including a quaternary nitride. ,,,. Structure. The P-type doped layer 106 is on the active layer 1〇4. The layer touches. The second electrode 11G is located on the flat-blade of the N-type doped layer or on the other side of the substrate. In addition, the retardation = "the problem that the 常数1 is located between the substrate and the N-type doped layer 1 〇 2 <, the lattice constant of the absorbing layer 102 growing on the heterogeneous substrate is generated. The stress relaxation layer 103 is located. Between the N-type doped layer 102 and the active layer 17 201103163. 29729twf.doc/n 104, as the stress releasing the active layer l〇4, the electron barrier layer ι〇5 is located in the active layer 1〇4 and the P-type doped layer Between 1 and 6, the electron-escape active layer 10OP-type contact layer 107 is located between the p-type layer and the first electrode 108 as the p-type doped layer 1〇6 and the first The impedance between an electrode 108. The above embodiment is exemplified by an active layer including a single quantum well structure, but the present invention is not limited thereto. Those skilled in the art will understand that the present invention is active. The layer may also be a quantum well structure. That is, the active layer of the present invention includes a plurality of quantum well structures, wherein the quantum barrier layer 104a and the quantum well 1 are alternately stacked at least twice. The manner is disposed on the stress relief layer 1〇3, as shown in FIG. 1C and FIG. 1D. 2A according to a second embodiment of the present invention is a nitride semiconductor light emitting depicted a schematic cross-sectional view of a pole of the element. Chill Referring to Figure 2A, first, a substrate 2〇〇. Next, the substrate 2〇〇
的一側上形成N型摻雜層2〇2。在一實施例中,在形成N 型推雜層202的步驟之前,也可以選擇性地於基板2〇〇及 N型彳參雜層202之間形成缓衝層2(n。基板2〇〇、缓衝層 2〇1與N型摻雜層2〇2的材料與形成方法與第一實施例類 似,於此不再贅述。 然後’於N型摻雜層2〇2上形成主動層2〇4。主動層 勺厚度例如疋介於約3 nm至約5〇〇 nm之間。主動層 18 201103163 P51970143TW 29729twf.doc/n 204包括至少一量子井結構,其中此量子井結構包括依序 形成在N型摻雜層上202上的量子阻障層2〇4a、量子井 204b及另一量子阻障層204a。量子阻障層2〇4&的材料例 如是 GaN、InxGai-xN 或 AlxGayIni_x_yN,其中 x、y 分別介 於〇與1之間,且x + y < !。量子井1〇4b的材料例如是 InfGauN 或 AlnGapIribn-pN,其中 f、n、p 分別介於 〇 與 1 之間,且η + Ρ<1。量子井i〇4b的厚度例如是介於約lnmAn N-type doping layer 2〇2 is formed on one side. In an embodiment, before the step of forming the N-type doping layer 202, the buffer layer 2 (n. substrate 2) may be selectively formed between the substrate 2 and the N-type germanium doping layer 202. The material and formation method of the buffer layer 2〇1 and the N-type doping layer 2〇2 are similar to those of the first embodiment, and will not be described here. Then, the active layer 2 is formed on the N-type doping layer 2〇2. 〇 4. The active layer spoon thickness, for example, 疋 is between about 3 nm and about 5 〇〇 nm. The active layer 18 201103163 P51970143TW 29729twf.doc/n 204 includes at least one quantum well structure, wherein the quantum well structure includes sequential formation a quantum barrier layer 2〇4a, a quantum well 204b, and another quantum barrier layer 204a on the N-type doped layer 202. The material of the quantum barrier layer 2〇4& is, for example, GaN, InxGai-xN or AlxGayIni_x_yN, Where x and y are between 〇 and 1, respectively, and x + y < !. The material of the quantum well 1〇4b is, for example, InfGauN or AlnGapIribn-pN, where f, n, p are between 〇 and 1, respectively And η + Ρ < 1. The thickness of the quantum well i 〇 4b is, for example, about 1 nm
至約20 rnn之間。另外,量子阻障層1〇知及量子井1〇牝 的形成方法例如是進行有機金屬化學氣相沉積法或分子 蟲晶法。 之後 .一於主動層204上形成電子阻障層2〇5。電 障層205為包括四元氮化物的超晶格結構。換句話說, 子阻障層205之超晶格結構的材料可以為四元氮化物與 一四元氮化物、四元氮化物與三元氮化物、四元氮化^ 二元氮化物、或四元氮化物、三械化物與二元氮化物 組成。在一實施例中,電子阻障層2〇5之四元氮^物 料例如疋AlglnhGai-g-hN,其中g、h分別介於〇與丄之門Between about 20 rnn. Further, the quantum barrier layer 1 is known to be a method of forming a quantum well, for example, an organometallic chemical vapor deposition method or a molecular crystal method. Thereafter, an electron barrier layer 2〇5 is formed on the active layer 204. The barrier layer 205 is a superlattice structure including a quaternary nitride. In other words, the material of the superlattice structure of the sub-barrier layer 205 may be a quaternary nitride and a quaternary nitride, a quaternary nitride and a ternary nitride, a quaternary nitride, a binary nitride, or It consists of quaternary nitrides, tribodies and binary nitrides. In one embodiment, the quaternary nitrogen material of the electron barrier layer 2〇5 is, for example, 疋AlglnhGai-g-hN, wherein g and h are respectively located between the gates of 〇 and 丄
且g+h< ;1。因此,電子阻障層2〇5之超晶格結構可二 週期層疊的 AlgInhGai_g_hN 層與 AliInjGai i jN 的 AlgInhGaKg_hN 層與 inkGai kN 層、週期層^ AlgliihG^N層與GaN層、或週期層疊的 層、InkGai_kN層與GaN層所組成,其中丨 ΙΟ與 1 之間, 尤隹认. u '刀別介 J 1 J 1且g不寺於i,h不等於卜 1¥層205之超晶格結構之週期層疊的次數為至少兩次, 19 201103163 P51970143TW 29729twf.doc/n 其每-層的厚度例如是介於約G 5nm至約Μ·之間。圖 2A的右側為電子阻障層2〇5之能帶分佈圖,由於電子阻障 層205為具有週期層疊之至少二材料層所形成的超晶格結 構’其中之-的材料為四元氮化物,因此其能帶分佈圖呈 週期變化。電子阻障層205的厚度可以由超晶格結構中之 每一材料層的厚度及週期層疊的次數而決定。 另外,電子阻p爭層205的形成方法例如是進行有機金 屬化學氣相沉積法或分子束磊晶法,且其生長溫度例如是介 於約6〇〇c至約ii〇(Tc之間。由於本發明之電子阻障層2〇5 φ 為包括四元氮化物的超晶格結構,因此可以防止歸因於量 子阻障層204a與電子阻障層205之間的晶格失配而產生之 晶體缺陷,如錯位以及凹洞等等。另外,本發明之量子阻 障層204a、量子井204b及電子阻障層205可以在同一個 反應腔室中完成,降低成本與減少製造發光二極體元件的 時間。 之後,請繼續參照圖2A ,於電子阻障層205上形成p 型摻雜層206。繼之,於p型摻雜層2〇6上形成第一電極 208。在一實施例中,在形成第一電極2〇8的步驟之前,也 響 可以選擇性地於P型摻雜層206及第一電極208之間形成 P型接觸層207。接著,於N型摻雜層1〇2曝露出的平台 209上形成第二電極210。至此,完成第二實施例之氮化物 半導體發光二極體元件之製造流程。P型摻雜層206、p型 接觸層207、第一電極208與第二電極210的材料與形成 方法與第一貫化例類似’於此不再資述。特另lj要說明的是, 20 201103163 t〇iy/ui43TW 29729twf.doc/n 當基板200的材料為導電材料如祕時,第二電極2 可以形成於基板200的另—側上,如圖2B所示,因 型摻雜層202也不需要形成平台209供第二電極21〇之 接下來,將說明第二實施例之氮化物 結構。請參照圖M2B,本發明之氮二; 二X光—極體兀件包括基板200、N型摻雜層202、主動 贫4、電子阻障層205、P型摻雜層206、第-電極雇^ 第一電極210。N型摻雜層2〇2位於基板2〇〇之一側上。 =層日2〇4位於N型換雜層2〇2上,其包括至少—量 ΡΪ層i子井結構5括二量子阻障層2G4a以及位於量子阻 204曰卜^之間的量子井2〇4b°P型摻雜層206位於主動層 之間,^子阻障層2〇5位於?型摻雜層206及主動層20曰4 構,日H巾電子阻障層2G5為包括四元氮化物的超晶格結 好阻障層2〇5的能隙高於量子阻障層綱a的能 位於N二電極208位於P型摻雜層206上。第二電極21〇 的另叫接雜層202曝露出的平台209上或位於基板200 層202則上。此外,緩衝層2〇1位於基板200與N型摻雜 層2〇4之間,應力舒緩層203位於N型摻雜層202及主動 一之間,且P型接觸層207位於P型摻雜層206及第 电極208之間。 之,—量子井結構之主騎為例來說明 Φ:、發明並不以此為限。圖2C與2D為第二實施例之 曰為多重量子井結構的示意圖。 21 201103163 P51970143TW 29729twf.doc/n 第三實施例 圖3A為依據本發明第三實施例所繪示的氮化物半導 •體發光二極體元件之示意剖面圖。 在第一、第二實施例中,分別以量子阻障層、電子阻 障層為包括四元氮化物的超晶格結構為例來說明之,伸本 發明並不以此為限。熟知本技藝者應了解,量子阻障層及 電子阻障層也可以依製程需要而同時為具有四元氮化:的 ,晶格結構,如第三實施例所示。圖3A的左側為量子阻 障層304a之能帶分佈圖,由於量子阻障層3〇4&為具有週 期層豐之至少二材料層所形成的超晶格結構,其中之一的 材料為四元氮化物,因此其能帶分佈圖呈週期變化。圖3a 的右側為電子阻障層305之能帶分佈圖,由於電子阻障層 為具有週期層疊之至少二材料層所形成的超晶格結 構,其中之一的材料為四元氮化物,因此其能帶分 週期變化。 第三實施例的各層材料及形成方法與第一、第二實施 =似’於此不再_,側單說明第三實施例之氮化物 ;導體發光二極體元件的結構。請參照圖3A及3B,本發 明之氮化物半導體發光二極體元件包括基板300、N型摻 ^層302、主動層3〇4、電子阻障層305、P型摻雜層306、 —電極308及第二電極31〇。N型摻雜層3〇2位於基板 之一側上。主動層304位於N型摻雜層302上,其包 、。里子井結構’量子井結構包括二量子阻障層304a 以及位於量子阻障層304a之間的量子井304b。量子阻障 22 201103163 P51970143TW 29729twf.doc/n 層l〇4a為包括四元氮化物的超晶格結構。 位於主動層綱上。電子阻障層3。5參= 及主動層綱之間,其中電子阻障層305為^另闕四元 氮化物的超晶格結構,且電子阻障層3Q5 於= ΓΤ:的。第—電極308位於p型摻雜層里306 ^第二電極3HM立於㈣摻雜層3〇2曝露 f或位於基板遍的另一側上。此外,緩衝層則位从 板300與N型摻雜層302之問,雍a 、土 摻雜層302及主動層304 ^應日力p舒緩層3〇3位於_ … 之間,且Ρ型接觸層307位於ρ 垔摻雜層306及第一電極3〇8之間。 、 圖3八與犯以單—量子井結敎 主動層為夕重置子井結構的示意圖。 综上所述,本發明之量子阻障層為包括四元氮化物 ’能夠幫助釋放主動層之應力,因此能有效抑 ς:效應’提升後續成長之量子井的結晶品質,及減少 =能隙差(G.2〜2 eV),以增加载子阻障,提升電g 洞對結合的機率’進而提升内部絲出效率。 另外,本發明之電子阻障層為包括另一四元氮化 =格結構’能夠防止歸因於量子阻障層與電子阻障層之 間的晶格失配而產生之晶體缺陷,如錯仙及凹洞等等。 再者’本發明之包括四元氮化物之量子阻障 阻障層可錄製程需要而單獨存在或同時存在,且本= 201103163 29729twf.doc/n 之量子阻障層、量子井及電子阻 室中,,降低成本與減少製造發: 本:ff明已以實施例揭露如上,然;= =之術領域中具有通常知識者,在不脫離 發日二之内’當可作些許之更動與潤飾,故本 I月之保5蒦乾圍當視後附之申請專利範圍所界定者為準。 【圖式簡單說明】 墓辦為依據本發明第—實施例所奢示的—氮化物半 wit—極體元件之示意剖面圖,其左側為量子阻障層 之月b帶分佈圖。 為依據本發明第—實施例崎示的另—氮化物 層之能體元件之示意剖面圖’其左側為量子阻障 丰為依據本發明第—實施例崎示的又一氮化物 1導4先二極體元件之示意剖面圖,其左 層之能帶分佈圖。 巧里卞I丨早 圖1D為依據本發明第一實施例所繪示 :導體發光二極體元件之示意剖面圖,其左側:量= 層之能帶分佈圖。 里丁丨且丨早 圖2Α為依據本發明第二實施例所繪示的— = 體元件之示意刹面圖’其右側為電伟障層 圖2B為依據本發明第二實施例所繪示的另一氮化物 24 201103163 P51970143TW 29729twf.doc/n 障 半導體發光二極體元件之示意到面圖 層之能帶分佈圖。 圖2C為依據本發明第二實施例所繪示的又〜 半導體發光二極體元件之示意㈣圖,其右㈣電 層之能帶分佈圖。 卞卩且障 圖2D為依據本發明第二實施例所繪示的再 半導體發光二極體元件之示意剑面圖,其右側為物 層之能帶分佈圖。 兒十卩且障 圖3A為依據本發明第三實施例所繪示的 導體發光二紐元件之示意 1 $匕物半 之能:分佈圖,且其右側為電子阻障層之能帶分::障層 為依據本發明第三實施例狀示的另1。 光二極體元件之示意刮面圖,其左側為量$物 層之二刀佈圖,且其右 層 :障 二極^件之示意剖面圖,其左側為量 ίIn刀Γ,且其右側為電子阻障層之能帶分佈^ 半導:二f爾發明第三實施例所繪示的再 丰w發先二極體元件之氣化物 層之能帶分佈圖,且其右側;i子 25 201103163 P51970143TW 29729twf.doc/n 【主要元件符號說明】 100、 200、300 :基底 101、 201、301 :缓衝層 102、 202、302 : N 型摻雜層 103、 203、303 :應力舒緩層 104、 204、304 :主動層 104a、204a、304a :量子阻障層 104b、204b、304b :量子井 105、 205、305 :電子阻障層 106、 206、306 : P 型掺雜層 107、 207、307 : P 型接觸層 108、 208、308 :第一電極 109、 209、309 :平台 110、 210、310 :第二電極 26And g+h<;1. Therefore, the superlattice structure of the electron barrier layer 2〇5 may be a two-period laminated AlgInhGai_g_hN layer and an AliInjGaKg_hN layer and an inkGai kN layer, a periodic layer, an AlgliihG^N layer and a GaN layer, or a periodically layered layer of AliInjGai i jN, InkGai_kN layer and GaN layer, which is between 丨ΙΟ and 1, especially 隹 .. u '刀别介J 1 J 1 and g not temple in i, h is not equal to Bu 1 205 layer superlattice structure The number of times of periodic lamination is at least twice, 19 201103163 P51970143TW 29729twf.doc/n The thickness per layer is, for example, between about G 5 nm and about Μ·. 2A is the energy band distribution diagram of the electron barrier layer 2〇5, since the electron barrier layer 205 is a superlattice structure formed by periodically stacking at least two material layers, wherein the material is quaternary nitrogen. The compound, therefore its band profile changes periodically. The thickness of the electron blocking layer 205 can be determined by the thickness of each material layer in the superlattice structure and the number of times of periodic lamination. In addition, the method of forming the electron blocking layer 205 is, for example, performing an organometallic chemical vapor deposition method or a molecular beam epitaxy method, and the growth temperature thereof is, for example, between about 6 〇〇c and about ii 〇 (Tc). Since the electron barrier layer 2〇5 φ of the present invention is a superlattice structure including a quaternary nitride, it is possible to prevent generation due to lattice mismatch between the quantum barrier layer 204a and the electron barrier layer 205. Crystal defects, such as misalignment and pits, etc. In addition, the quantum barrier layer 204a, the quantum well 204b and the electron barrier layer 205 of the present invention can be completed in the same reaction chamber, reducing cost and reducing manufacturing of light-emitting diodes. The time of the body element. Thereafter, referring to FIG. 2A, a p-type doping layer 206 is formed on the electron barrier layer 205. Next, a first electrode 208 is formed on the p-type doping layer 2〇6. In the example, before the step of forming the first electrode 2〇8, the P-type contact layer 207 may be selectively formed between the P-type doping layer 206 and the first electrode 208. Then, the N-type doped layer is formed. The second electrode 210 is formed on the exposed platform 209. At this point, the second is completed. The manufacturing process of the nitride semiconductor light-emitting diode element of the embodiment. The material and formation method of the P-type doping layer 206, the p-type contact layer 207, the first electrode 208 and the second electrode 210 are similar to those of the first embodiment. The second electrode 2 can be formed on the substrate 200 when the material of the substrate 200 is a conductive material, such as a secret, when the material of the substrate 200 is a conductive material such as a secret. On the side, as shown in FIG. 2B, the type doping layer 202 does not need to form the terrace 209 for the second electrode 21, and the nitride structure of the second embodiment will be described. Referring to FIG. The nitrogen-emitting diode comprises a substrate 200, an N-doped layer 202, an active layer 4, an electron barrier layer 205, a P-doped layer 206, and a first electrode 210. The N-type doped layer 2〇2 is located on one side of the substrate 2〇〇. The layer 2〇4 is located on the N-type impurity layer 2〇2, which includes at least the ΡΪ layer of the sub-well structure 5 The barrier layer 2G4a and the quantum well 2〇4b°P-type doped layer 206 between the quantum resistors 204 are located between the active layers, and the barrier layer is 2〇5 In the doped layer 206 and the active layer 20曰4, the H-glass electronic barrier layer 2G5 is a superlattice barrier layer including a quaternary nitride, and the energy gap is higher than the quantum barrier layer. The energy of the class A can be located on the P-doped layer 206. The second electrode 21A is also disposed on the platform 209 exposed by the impurity layer 202 or on the substrate 200 layer 202. In addition, the buffer layer 2 〇1 is located between the substrate 200 and the N-type doped layer 2〇4, the stress relaxation layer 203 is located between the N-type doped layer 202 and the active one, and the P-type contact layer 207 is located at the P-type doped layer 206 and the first Between poles 208. The main ride of the quantum well structure is taken as an example to illustrate Φ: The invention is not limited to this. 2C and 2D are schematic views showing the structure of the second embodiment as a multiple quantum well structure. 21 201103163 P51970143TW 29729twf.doc/n Third Embodiment FIG. 3A is a schematic cross-sectional view showing a nitride semiconductor light-emitting diode element according to a third embodiment of the present invention. In the first and second embodiments, the quantum barrier layer and the electron barrier layer are respectively described as a superlattice structure including a quaternary nitride, and the invention is not limited thereto. It is well known to those skilled in the art that the quantum barrier layer and the electron barrier layer can also have a quaternary nitrided, lattice structure as required by the process, as shown in the third embodiment. The left side of FIG. 3A is an energy band distribution diagram of the quantum barrier layer 304a. Since the quantum barrier layer 3〇4& is a superlattice structure formed by at least two material layers having a periodic layer, one of the materials is four. The meta-nitride, so its band diagram changes periodically. The right side of FIG. 3a is an energy band distribution diagram of the electron barrier layer 305. Since the electron barrier layer is a superlattice structure formed by periodically stacking at least two material layers, one of the materials is a quaternary nitride, It can change in cycles. The materials and forming methods of the layers of the third embodiment are the same as those of the first and second embodiments. The nitride of the third embodiment and the structure of the conductor light-emitting diode elements will be described. 3A and 3B, the nitride semiconductor light-emitting diode device of the present invention comprises a substrate 300, an N-type doped layer 302, an active layer 3〇4, an electron barrier layer 305, a P-type doped layer 306, and an electrode. 308 and the second electrode 31〇. The N-type doped layer 3〇2 is located on one side of the substrate. The active layer 304 is located on the N-type doped layer 302, which is packaged. The neutron well structure 'quantum well structure includes a second quantum barrier layer 304a and a quantum well 304b between the quantum barrier layers 304a. Quantum Barrier 22 201103163 P51970143TW 29729twf.doc/n Layer l〇4a is a superlattice structure comprising a quaternary nitride. Located on the active floor. The electron barrier layer is between 3. 5 and the active layer, wherein the electron barrier layer 305 is a super-lattice structure of a quaternary nitride, and the electron barrier layer 3Q5 is at ΓΤ:. The first electrode 308 is located in the p-doped layer 306. The second electrode 3HM is exposed to the (four) doped layer 3〇2 or is located on the other side of the substrate. In addition, the buffer layer is located between the plate 300 and the N-type doped layer 302, and the 雍a, the soil doped layer 302, and the active layer 304 are located between the _, and the 日 type The contact layer 307 is located between the p-doped layer 306 and the first electrode 3〇8. Figure 3 is a schematic diagram of the structure of the reset sub-well with a single-quantum well crust active layer. In summary, the quantum barrier layer of the present invention includes a quaternary nitride which can help release the stress of the active layer, and thus can effectively suppress: the effect of 'improving the crystal quality of the subsequent growth of the quantum well, and reducing = energy gap Poor (G.2~2 eV) to increase the carrier barrier and improve the probability of the combination of the electric g hole and the internal wire extraction efficiency. In addition, the electron barrier layer of the present invention includes another quaternary nitride = lattice structure to prevent crystal defects caused by lattice mismatch between the quantum barrier layer and the electron barrier layer, such as Fairy and caves, etc. Furthermore, the quantum barrier barrier layer comprising the quaternary nitride of the present invention may exist separately or simultaneously at the same time as the recording process, and the quantum barrier layer, the quantum well and the electronic resistance chamber of the present invention are 201103163 29729twf.doc/n In the middle, the cost reduction and the reduction of manufacturing hair: Ben: ff has been disclosed in the above example, however; = = the field of the general knowledge in the field of technology, without leaving the day 2, when you can make some changes Retouching, so the warranty of this I month is as defined in the scope of the patent application. BRIEF DESCRIPTION OF THE DRAWINGS The tomb is a schematic cross-sectional view of a nitride half-wit-pole element according to the first embodiment of the present invention, and the left side is a monthly b-band distribution map of the quantum barrier layer. A schematic cross-sectional view of an energy element of a further nitride layer according to a first embodiment of the present invention, wherein the left side is a quantum barrier, and the further nitride 1 is 4 according to the first embodiment of the present invention. A schematic cross-sectional view of the first diode element, the energy band distribution diagram of the left layer. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1D is a schematic cross-sectional view of a conductor light-emitting diode element according to a first embodiment of the present invention, the left side of which: the amount = the energy band distribution of the layer. 。 丨 丨 图 图 图 依据 依据 依据 依据 依据 依据 依据 依据 依据 依据 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意 示意Another nitride 24 201103163 P51970143TW 29729twf.doc/n The band diagram of the schematic layer-to-face layer of the barrier semiconductor light-emitting diode component. 2C is a schematic (four) diagram of a semiconductor light-emitting diode element according to a second embodiment of the present invention, showing the energy band distribution of the right (four) electrical layer. 2D is a schematic sword view of a re-semiconductor LED device according to a second embodiment of the present invention, the right side of which is the energy band distribution of the object layer. FIG. 3A is a schematic diagram of a conductor light-emitting two-component element according to a third embodiment of the present invention: a distribution map, and the right side of the electron barrier layer is: The barrier layer is another one according to the third embodiment of the present invention. A schematic plan view of a photodiode element, the left side of which is a two-knife pattern of the quantity of the object layer, and the right side of which is a schematic sectional view of the barrier element, the left side of which is the quantity ίIn knife, and the right side thereof is The energy band distribution of the electron barrier layer is a semi-conductor: the energy band distribution map of the vaporization layer of the re-birth-first diode element depicted in the third embodiment of the invention, and its right side; 201103163 P51970143TW 29729twf.doc/n [Description of main component symbols] 100, 200, 300: substrate 101, 201, 301: buffer layer 102, 202, 302: N-type doping layer 103, 203, 303: stress relaxation layer 104 204, 304: active layers 104a, 204a, 304a: quantum barrier layers 104b, 204b, 304b: quantum wells 105, 205, 305: electron barrier layers 106, 206, 306: P-type doped layers 107, 207, 307 : P type contact layer 108 , 208 , 308 : first electrode 109 , 209 , 309 : platform 110 , 210 , 310 : second electrode 26
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| TW98123908A TWI384657B (en) | 2009-07-15 | 2009-07-15 | Nitirde semiconductor light emitting diode device |
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103178171A (en) * | 2013-02-28 | 2013-06-26 | 溧阳市宏达电机有限公司 | High-luminance light emitting diode |
| CN103474538A (en) * | 2013-09-25 | 2013-12-25 | 湘能华磊光电股份有限公司 | Light-emitting diode (LED) epitaxial wafer, manufacturing method of LED epitaxial wafer and LED chip including LED epitaxial wafer |
| TWI509835B (en) * | 2013-10-01 | 2015-11-21 | Opto Tech Corp | White light diode |
| US9923119B2 (en) | 2013-10-01 | 2018-03-20 | Opto Tech Corporation | White LED chip and white LED packaging device |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6335546B1 (en) * | 1998-07-31 | 2002-01-01 | Sharp Kabushiki Kaisha | Nitride semiconductor structure, method for producing a nitride semiconductor structure, and light emitting device |
| JP2001210915A (en) * | 2000-01-24 | 2001-08-03 | Sony Corp | Semiconductor light emitting device |
| TW497277B (en) * | 2000-03-10 | 2002-08-01 | Toshiba Corp | Semiconductor light emitting device and method for manufacturing the same |
| KR100664985B1 (en) * | 2004-10-26 | 2007-01-09 | 삼성전기주식회사 | Nitride-based semiconductor device |
| KR100659579B1 (en) * | 2004-12-08 | 2006-12-20 | 한국전자통신연구원 | Light Emitting Diode and Method for Preparing Light Emitting Diode |
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2009
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN103178171A (en) * | 2013-02-28 | 2013-06-26 | 溧阳市宏达电机有限公司 | High-luminance light emitting diode |
| CN103474538A (en) * | 2013-09-25 | 2013-12-25 | 湘能华磊光电股份有限公司 | Light-emitting diode (LED) epitaxial wafer, manufacturing method of LED epitaxial wafer and LED chip including LED epitaxial wafer |
| TWI509835B (en) * | 2013-10-01 | 2015-11-21 | Opto Tech Corp | White light diode |
| US9923119B2 (en) | 2013-10-01 | 2018-03-20 | Opto Tech Corporation | White LED chip and white LED packaging device |
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| TWI384657B (en) | 2013-02-01 |
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