TWI497766B - Method for producing semiconductor device - Google Patents
Method for producing semiconductor device Download PDFInfo
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- TWI497766B TWI497766B TW101147220A TW101147220A TWI497766B TW I497766 B TWI497766 B TW I497766B TW 101147220 A TW101147220 A TW 101147220A TW 101147220 A TW101147220 A TW 101147220A TW I497766 B TWI497766 B TW I497766B
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- 239000004065 semiconductor Substances 0.000 title claims description 45
- 238000004519 manufacturing process Methods 0.000 title claims description 31
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 claims description 131
- 229910052757 nitrogen Inorganic materials 0.000 claims description 64
- 238000000137 annealing Methods 0.000 claims description 35
- 239000012159 carrier gas Substances 0.000 claims description 26
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 claims description 21
- 239000007789 gas Substances 0.000 claims description 19
- 239000001257 hydrogen Substances 0.000 claims description 18
- 229910052739 hydrogen Inorganic materials 0.000 claims description 18
- 238000005253 cladding Methods 0.000 claims description 10
- 238000000034 method Methods 0.000 claims description 7
- 239000011777 magnesium Substances 0.000 description 25
- 239000000203 mixture Substances 0.000 description 25
- 239000000758 substrate Substances 0.000 description 25
- 238000002156 mixing Methods 0.000 description 22
- QGZKDVFQNNGYKY-UHFFFAOYSA-N Ammonia Chemical compound N QGZKDVFQNNGYKY-UHFFFAOYSA-N 0.000 description 17
- 229910052594 sapphire Inorganic materials 0.000 description 16
- 239000010980 sapphire Substances 0.000 description 16
- 230000004913 activation Effects 0.000 description 15
- 230000007547 defect Effects 0.000 description 15
- 239000013078 crystal Substances 0.000 description 13
- 229910002704 AlGaN Inorganic materials 0.000 description 10
- 150000004767 nitrides Chemical class 0.000 description 9
- 230000004888 barrier function Effects 0.000 description 8
- 238000000151 deposition Methods 0.000 description 8
- 229910021529 ammonia Inorganic materials 0.000 description 7
- 125000004429 atom Chemical group 0.000 description 6
- DIOQZVSQGTUSAI-UHFFFAOYSA-N decane Chemical compound CCCCCCCCCC DIOQZVSQGTUSAI-UHFFFAOYSA-N 0.000 description 6
- 239000000463 material Substances 0.000 description 5
- 239000012299 nitrogen atmosphere Substances 0.000 description 5
- 238000001816 cooling Methods 0.000 description 4
- 125000004435 hydrogen atom Chemical group [H]* 0.000 description 4
- 239000012298 atmosphere Substances 0.000 description 3
- 238000005229 chemical vapour deposition Methods 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 229910001873 dinitrogen Inorganic materials 0.000 description 3
- 239000012535 impurity Substances 0.000 description 3
- 230000006798 recombination Effects 0.000 description 3
- 238000005215 recombination Methods 0.000 description 3
- 230000008901 benefit Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 239000013256 coordination polymer Substances 0.000 description 2
- 229910052733 gallium Inorganic materials 0.000 description 2
- 230000020169 heat generation Effects 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 150000002431 hydrogen Chemical class 0.000 description 2
- 230000001771 impaired effect Effects 0.000 description 2
- 230000006872 improvement Effects 0.000 description 2
- JLTRXTDYQLMHGR-UHFFFAOYSA-N trimethylaluminium Chemical compound C[Al](C)C JLTRXTDYQLMHGR-UHFFFAOYSA-N 0.000 description 2
- XCZXGTMEAKBVPV-UHFFFAOYSA-N trimethylgallium Chemical compound C[Ga](C)C XCZXGTMEAKBVPV-UHFFFAOYSA-N 0.000 description 2
- IBEFSUTVZWZJEL-UHFFFAOYSA-N trimethylindium Chemical compound C[In](C)C IBEFSUTVZWZJEL-UHFFFAOYSA-N 0.000 description 2
- KLSJWNVTNUYHDU-UHFFFAOYSA-N Amitrole Chemical compound NC1=NC=NN1 KLSJWNVTNUYHDU-UHFFFAOYSA-N 0.000 description 1
- MHYQBXJRURFKIN-UHFFFAOYSA-N C1(C=CC=C1)[Mg] Chemical compound C1(C=CC=C1)[Mg] MHYQBXJRURFKIN-UHFFFAOYSA-N 0.000 description 1
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- BLRPTPMANUNPDV-UHFFFAOYSA-N Silane Chemical compound [SiH4] BLRPTPMANUNPDV-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- TVFDJXOCXUVLDH-UHFFFAOYSA-N caesium atom Chemical group [Cs] TVFDJXOCXUVLDH-UHFFFAOYSA-N 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000002109 crystal growth method Methods 0.000 description 1
- 238000000354 decomposition reaction Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 239000002019 doping agent Substances 0.000 description 1
- 238000001312 dry etching Methods 0.000 description 1
- 230000001747 exhibiting effect Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 238000000605 extraction Methods 0.000 description 1
- 230000005669 field effect Effects 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
- 230000002401 inhibitory effect Effects 0.000 description 1
- 229910052749 magnesium Inorganic materials 0.000 description 1
- WGESBNRUPISICS-UHFFFAOYSA-N magnesium;cyclopenta-1,3-diene Chemical compound [Mg+2].C=1C=C[CH-]C=1.C=1C=C[CH-]C=1 WGESBNRUPISICS-UHFFFAOYSA-N 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 230000005012 migration Effects 0.000 description 1
- 238000013508 migration Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 125000004433 nitrogen atom Chemical group N* 0.000 description 1
- 229920001296 polysiloxane Polymers 0.000 description 1
- 238000005036 potential barrier Methods 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
- 229910052703 rhodium Inorganic materials 0.000 description 1
- 229910000077 silane Inorganic materials 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 230000003746 surface roughness Effects 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
- 230000005641 tunneling Effects 0.000 description 1
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Description
本發明關於製造半導體裝置的方法。更尤其,本發明關於包含由三族氮化物半導體所形成的p型接觸層及p型電極之半導體裝置的製造方法,該方法係意為改善在p型接觸層及p型電極之間的歐姆接觸。The present invention relates to a method of fabricating a semiconductor device. More particularly, the present invention relates to a method of fabricating a semiconductor device including a p-type contact layer and a p-type electrode formed of a group III nitride semiconductor, which is intended to improve ohmic between a p-type contact layer and a p-type electrode contact.
一般而言,半導體裝置包含p型電極、及與p型電極接觸的p型接觸層。當p型電極及p型接觸層之間的接觸電阻高時,可能產生熱,且熱的產生可能縮短裝置的有效壽命。又,當接觸電阻高時,半導體裝置的驅動電壓升高。In general, a semiconductor device includes a p-type electrode and a p-type contact layer in contact with the p-type electrode. When the contact resistance between the p-type electrode and the p-type contact layer is high, heat may be generated, and heat generation may shorten the effective life of the device. Also, when the contact resistance is high, the driving voltage of the semiconductor device rises.
尤其,為了減少由三族氮化物半導體所形成的p型接觸層及p型電極之間的接觸電阻,p型接觸層的電洞濃度必須增加。然而,由於在三族氮化物半導體層中形成深受子雜質能階,故在增加電洞濃度上遇到困難。In particular, in order to reduce the contact resistance between the p-type contact layer and the p-type electrode formed by the group III nitride semiconductor, the hole concentration of the p-type contact layer must be increased. However, since the deep acceptor impurity level is formed in the group III nitride semiconductor layer, difficulty is encountered in increasing the hole concentration.
因此,已為增加電洞密度而進行許多研究。例如,專利文件1揭露藉由降低p型接觸層的成長速率來實現約1018 /cm3 的電洞濃度之技術。Therefore, many studies have been conducted to increase the hole density. For example, Patent Document 1 discloses a technique of realizing a hole concentration of about 10 18 /cm 3 by reducing the growth rate of the p-type contact layer.
專利文件1:日本公開專利申請案第2003-23179號。Patent Document 1: Japanese Laid-Open Patent Application No. 2003-23179.
然而,即使當p型電極形成於具有此電洞濃度的p型接觸層上時,仍可能無法獲得較佳的歐姆接觸。同時,考慮到該層及該電極的功函數,故在達到由三族氮化物半導體所形成的p型接觸層及p型電極之間的歐姆接觸上遇到困難。However, even when a p-type electrode is formed on a p-type contact layer having such a hole concentration, a preferable ohmic contact may not be obtained. At the same time, considering the work function of the layer and the electrode, difficulty is encountered in achieving an ohmic contact between the p-type contact layer and the p-type electrode formed by the group III nitride semiconductor.
本發明已為解決涉及習知技術的前述問題而完成。因此,本發明 的目的係提供製造包含由氮化物半導體所形成的p型接觸層及p型電極之半導體裝置的方法,其中該方法係意為改善p型接觸層及p型電極之間的歐姆接觸。The present invention has been accomplished to solve the aforementioned problems related to the prior art. Therefore, the present invention The object is to provide a method of fabricating a semiconductor device including a p-type contact layer and a p-type electrode formed of a nitride semiconductor, wherein the method is intended to improve ohmic contact between the p-type contact layer and the p-type electrode.
在為解決前述問題之本發明的第一實施態樣中,提供有製造半導體裝置的方法,該半導體裝置包含p型電極、及其上形成p型電極且由三族氮化物半導體所形成的p型接觸層,該方法包含形成p型接觸層的步驟,該步驟包含第一子步驟,藉由使用氮與氫的混合氣體作為載運氣體形成第一p型接觸層;及第二子步驟,藉由使用氫作為載運氣體來形成第二p型接觸層。In a first embodiment of the present invention for solving the aforementioned problems, there is provided a method of manufacturing a semiconductor device comprising a p-type electrode, and a p formed thereon and formed of a group III nitride semiconductor a contact layer, the method comprising the step of forming a p-type contact layer, the step comprising a first sub-step of forming a first p-type contact layer by using a mixed gas of nitrogen and hydrogen as a carrier gas; and a second sub-step A second p-type contact layer is formed by using hydrogen as a carrier gas.
在經由該半導體裝置製造方法所製造的半導體裝置中,在p型接觸層及p型電極之間達成較佳的歐姆接觸;即在其之間達成低接觸電阻。因此,能減少電力消耗,且亦減少熱產生的總量。In the semiconductor device manufactured by the semiconductor device manufacturing method, a preferable ohmic contact is achieved between the p-type contact layer and the p-type electrode; that is, a low contact resistance is achieved therebetween. Therefore, power consumption can be reduced, and the total amount of heat generation is also reduced.
本發明的第二實施態樣係關於半導體裝置製造方法的具體實施例,其中第一子步驟使用其中氮對整體載運氣體的莫耳比(以下該比例可表示為”氮莫耳分率”)為40%至80%的載運氣體。此載運氣體的使用實現了具有減少的晶格缺陷之第一p型接觸層的形成。因此,如此形成的第一p型接觸層顯示更減少的電阻率。更佳地,氮莫耳分率為50%至75%。最佳地,氮莫耳分率為55%至70%。A second embodiment of the present invention is directed to a specific embodiment of a method of fabricating a semiconductor device, wherein the first substep uses a molar ratio of nitrogen to the overall carrier gas (hereinafter the ratio can be expressed as "nitrogen mole fraction") It is 40% to 80% of carrier gas. The use of this carrier gas achieves the formation of a first p-type contact layer with reduced lattice defects. Therefore, the first p-type contact layer thus formed exhibits a more reduced resistivity. More preferably, the nitrogen molar fraction is from 50% to 75%. Most preferably, the nitrogen molar fraction is from 55% to 70%.
本發明的第三實施態樣係關於半導體裝置製造方法的具體實施例,其中不執行用以減少p型接觸層電阻的退火步驟。此退火步驟的省略縮短了循環時間且改善了生產率。A third embodiment of the present invention is directed to a specific embodiment of a method of fabricating a semiconductor device in which an annealing step for reducing the resistance of a p-type contact layer is not performed. The omission of this annealing step shortens the cycle time and improves productivity.
本發明的第四實施態樣係關於半導體裝置製造方法的具體實施例,其中更包含在第二子步驟後、在氮大氣中冷卻包含p型接觸層的層狀產品之步驟。在氮大氣中該層狀產品的冷卻能預防氫對受子雜質的再結合。A fourth embodiment of the present invention is directed to a specific embodiment of a method of fabricating a semiconductor device, further comprising the step of cooling a layered product comprising a p-type contact layer in a nitrogen atmosphere after the second sub-step. Cooling of the layered product in a nitrogen atmosphere prevents recombination of hydrogen by the acceptor impurities.
本發明的第五實施態樣係關於半導體裝置製造方法的具體實施例,其中第二子步驟形成具有10 Å至100 Å的厚度之第二p型接觸層。當第二p型接觸層的厚度落入上述範圍內時,晶格缺陷係適當地形成於該層中。藉由穿隧效應,載子輕易地經由如此形成的晶格缺陷通過位能障壁。更佳地,第二p型接觸層的厚度為20 Å至90 Å。再更佳地,第二p型接觸 層的厚度係30 Å至70 Å。A fifth embodiment of the present invention is directed to a specific embodiment of a method of fabricating a semiconductor device, wherein the second sub-step forms a second p-type contact layer having a thickness of 10 Å to 100 Å. When the thickness of the second p-type contact layer falls within the above range, a lattice defect is appropriately formed in the layer. By tunneling, the carrier easily passes through the potential barrier through the lattice defects thus formed. More preferably, the second p-type contact layer has a thickness of from 20 Å to 90 Å. Even more preferably, the second p-type contact The thickness of the layer is 30 Å to 70 Å.
本發明的第六實施態樣係關於半導體裝置製造方法的具體實施例,其中在第二子步驟中形成第二p型接觸層的期間,該第二p型接觸層係以高於該第一p型接觸層的Mg濃度之濃度摻雜Mg,且該第二p型接觸層之的Mg濃度係調整至1×1020 /cm3 至1×1022 /cm3 。更佳地,Mg濃度係調整至2×1020 /cm3 至9×1021 /cm3 。再更佳地,Mg濃度係調整至5×1020 /cm3 至8×1021 /cm3 。這是因為當第二p型接觸層之Mg濃度落入上述範圍內時,較大量的晶格缺陷能形成於該層中。因此,在活化Mg之後,電子在p型電極及p型接觸層之間平順地移動。A sixth embodiment of the present invention is directed to a specific embodiment of a method of fabricating a semiconductor device, wherein during the forming of the second p-type contact layer in the second sub-step, the second p-type contact layer is higher than the first The concentration of the Mg concentration of the p-type contact layer is doped with Mg, and the Mg concentration of the second p-type contact layer is adjusted to 1 × 10 20 /cm 3 to 1 × 10 22 /cm 3 . More preferably, the Mg concentration is adjusted to 2 × 10 20 /cm 3 to 9 × 10 21 /cm 3 . More preferably, the Mg concentration is adjusted to 5 × 10 20 /cm 3 to 8 × 10 21 /cm 3 . This is because when the Mg concentration of the second p-type contact layer falls within the above range, a larger amount of lattice defects can be formed in the layer. Therefore, after the activation of Mg, electrons move smoothly between the p-type electrode and the p-type contact layer.
根據本發明,提供製造包含由氮化物半導體所形成的p型接觸層及p型電極之半導體裝置的方法,其中該方法係意為改善在p型接觸層及p型電極之間的歐姆接觸。According to the present invention, there is provided a method of fabricating a semiconductor device comprising a p-type contact layer and a p-type electrode formed of a nitride semiconductor, wherein the method is intended to improve ohmic contact between the p-type contact layer and the p-type electrode.
10‧‧‧藍寶石基板10‧‧‧Sapphire substrate
20‧‧‧低溫緩衝層20‧‧‧Low temperature buffer layer
30‧‧‧N型接觸層30‧‧‧N type contact layer
40‧‧‧N型ESD層40‧‧‧N type ESD layer
50‧‧‧N型SL層50‧‧‧N type SL layer
60‧‧‧MQW層60‧‧‧MQW layer
70‧‧‧P型披覆層70‧‧‧P type coating
80‧‧‧P型接觸層80‧‧‧P type contact layer
90‧‧‧層狀產品90‧‧‧Layered products
100‧‧‧發光裝置100‧‧‧Lighting device
N1‧‧‧N型電極N1‧‧‧N type electrode
P1‧‧‧P型電極P1‧‧‧P type electrode
隨著本發明之不同的其他目的、特徵、及許多伴隨的優點在相關於隨附圖式而考量時參照下列較佳實施例的詳述變得更加理解,其將容易被察知,其中:圖1示意地顯示根據實施例之半導體裝置的層狀結構;圖2A至2C顯示根據實施例(部份1)的半導體裝置製造方法;圖3顯示根據實施例(部份2)的半導體裝置製造方法;圖4係顯示經由根據實施例之半導體裝置製造方法所製造的發光裝置之第一p型接觸層的電洞濃度圖表;圖5係顯示經由根據實施例之半導體裝置製造方法所製造的發光裝置之第一p型接觸層中電洞遷移率的圖表;圖6係顯示經由根據實施例之半導體裝置製造方法所製造的發光裝置之第一p型接觸層中電阻率的圖表;圖7係顯示經由根據實施例之半導體裝置製造方法所製造的發光裝置之第一p型接觸層中活化百分比的圖表;且圖8係顯示在經由根據實施例之半導體裝置製造方法所製造的發光裝 置及習知發光裝置之間的輸出比較圖表。The other objects, features, and advantages of the present invention will become more apparent upon consideration of 1 schematically shows a layered structure of a semiconductor device according to an embodiment; FIGS. 2A to 2C show a method of fabricating a semiconductor device according to an embodiment (Part 1); and FIG. 3 shows a method of manufacturing a semiconductor device according to an embodiment (Part 2) FIG. 4 is a graph showing the hole concentration of the first p-type contact layer of the light-emitting device manufactured by the semiconductor device manufacturing method according to the embodiment; FIG. 5 is a view showing the light-emitting device manufactured by the semiconductor device manufacturing method according to the embodiment; a graph of hole mobility in the first p-type contact layer; FIG. 6 is a graph showing resistivity in the first p-type contact layer of the light-emitting device manufactured by the semiconductor device manufacturing method according to the embodiment; FIG. a graph of the percentage of activation in the first p-type contact layer of the light-emitting device manufactured by the semiconductor device manufacturing method according to the embodiment; and FIG. 8 is shown in accordance with an embodiment The method of manufacturing a light emitting semiconductor device fabricated loaded An output comparison chart between conventional light-emitting devices is placed.
本發明之具體實施例接下來將藉由以製造發光裝置(Light Emitting Device)的情況為例參照圖式來描述。然而,本發明並不限定於該實施例。亦即,本發明能適用於不同的半導體裝置,包含如場效改性電晶體(FEMT)的電晶體、光偵測器、及如LED或雷射二極體的發光裝置。自不待言,形成發光裝置的每一層之結構可不同於下列所述的實施例中所例示者。示意地顯示於圖式中之每一層的厚度並不對應至其實際數值。Specific embodiments of the present invention will be described next with reference to the drawings by taking a case of manufacturing a light emitting device. However, the invention is not limited to the embodiment. That is, the present invention can be applied to different semiconductor devices, including a transistor such as a field effect modified transistor (FEMT), a photodetector, and a light emitting device such as an LED or a laser diode. Needless to say, the structure of each layer forming the light-emitting device may be different from that exemplified in the embodiments described below. The thickness of each layer schematically shown in the drawings does not correspond to its actual value.
現將參照圖1描述經由根據本實施例之半導體裝置製造方法所製造的發光裝置100。該發光裝置100係由三族氮化物半導體所形成的半導體裝置。如圖1中所示,該發光裝置100包含藍寶石基板10、低溫緩衝層20、n型接觸層30、n型靜電放電(ESD,electrostatic discharge)層40、n型超晶格(SL,superlattice)層50、用作發光源的多重量子井(MQW,multiple quantum well)層60、p型披覆層70、及p型接觸層80,層20至80係以此順序形成於藍寶石基板10上。n型電極N1係形成於n型接觸層30上。p型電極P1係形成於p型接觸層80上。A light-emitting device 100 manufactured via the semiconductor device manufacturing method according to the present embodiment will now be described with reference to FIG. The light-emitting device 100 is a semiconductor device formed of a group III nitride semiconductor. As shown in FIG. 1, the light emitting device 100 includes a sapphire substrate 10, a low temperature buffer layer 20, an n-type contact layer 30, an n-type electrostatic discharge (ESD) layer 40, and an n-type superlattice (SL). The layer 50, a multiple quantum well (MQW) layer 60, a p-type cladding layer 70, and a p-type contact layer 80, which are used as light sources, are formed on the sapphire substrate 10 in this order. The n-type electrode N1 is formed on the n-type contact layer 30. The p-type electrode P1 is formed on the p-type contact layer 80.
上述的個別層係經由金屬-有機化學氣相沈積法(MOCVD,metal-organic chemical vapor deposition)而形成於藍寶石基板10之一表面上。藍寶石基板10的該表面可為了改善光萃取表現的目的而突起。藍寶石基板可由如以SiC、ZnO、Si或GaN所形成的另一成長基板代替。低溫緩衝層20係設置以轉移藍寶石基板10的結晶度至形成於緩衝層20之上的一層。低溫緩衝層20的例示材料包含AlN及GaN。The individual layers described above are formed on one surface of the sapphire substrate 10 via metal-organic chemical vapor deposition (MOCVD). This surface of the sapphire substrate 10 may be protruded for the purpose of improving the performance of light extraction. The sapphire substrate may be replaced by another growth substrate such as SiC, ZnO, Si or GaN. The low temperature buffer layer 20 is provided to transfer the crystallinity of the sapphire substrate 10 to a layer formed on the buffer layer 20. Exemplary materials for the low temperature buffer layer 20 include AlN and GaN.
n型接觸層30實際上與n型電極N1接觸。n型接觸層30係由以Si摻雜的GaN形成。層30的Si濃度為1×1018 /cm3 或更高。n型接觸層30可 為了改善n型接觸層30及n型電極之間歐姆接觸的目的,而由具有不同載子濃度之複數層所形成。The n-type contact layer 30 is actually in contact with the n-type electrode N1. The n-type contact layer 30 is formed of GaN doped with Si. The Si concentration of the layer 30 is 1 × 10 18 /cm 3 or higher. The n-type contact layer 30 may be formed of a plurality of layers having different carrier concentrations for the purpose of improving the ohmic contact between the n-type contact layer 30 and the n-type electrode.
n型ESD層40係設置以改進靜電放電;即,為預防每一半導體層的靜電放電。該n型ESD層40具有包含未摻雜的GaN層及Si摻雜GaN層之層狀結構。較佳地,Si摻雜係執行以獲得1×1018 /cm3 或更高的載子濃度。The n-type ESD layer 40 is provided to improve electrostatic discharge; that is, to prevent electrostatic discharge of each semiconductor layer. The n-type ESD layer 40 has a layered structure including an undoped GaN layer and a Si-doped GaN layer. Preferably, the Si doping is performed to obtain a carrier concentration of 1 × 10 18 /cm 3 or higher.
n型SL層50具有用以緩和施加至MQW層60的應力之超晶格結構。n型SL層50係藉由交替沈積GaN層及InGaN層而形成。除了這些層之外,還可沈積n-GaN層。尤其佳地,n-GaN層與MQW層60接觸。形成n型SL層50的層單元數量為10至20。n型SL層50的整體厚度為60 nm至80 nm。The n-type SL layer 50 has a superlattice structure for relieving stress applied to the MQW layer 60. The n-type SL layer 50 is formed by alternately depositing a GaN layer and an InGaN layer. In addition to these layers, an n-GaN layer may be deposited. More preferably, the n-GaN layer is in contact with the MQW layer 60. The number of layer units forming the n-type SL layer 50 is 10 to 20. The n-type SL layer 50 has an overall thickness of 60 nm to 80 nm.
MQW層60係經由電子及電洞的再結合而發光之發光層。因此,MQW層60係藉由交替沈積具有小能隙的井層及具有大能隙的阻障層而形成。井層可由InGaN形成,而阻障層可由AlGaN形成。替代地,井層可由GaN形成,而阻障層可由AlGaN形成。替代地,MQW層60可由這些層的任何組合形成;例如,層60可由重複的層單元形成,每一層單元包含四或更多層。The MQW layer 60 is a light-emitting layer that emits light by recombination of electrons and holes. Therefore, the MQW layer 60 is formed by alternately depositing a well layer having a small energy gap and a barrier layer having a large energy gap. The well layer may be formed of InGaN, and the barrier layer may be formed of AlGaN. Alternatively, the well layer may be formed of GaN, and the barrier layer may be formed of AlGaN. Alternatively, MQW layer 60 may be formed from any combination of these layers; for example, layer 60 may be formed of repeating layer units, each layer unit comprising four or more layers.
p型披覆層70係設置以預防電子擴散至p型接觸層80。p型披覆層70係藉由交替沈積包含p-InGaN層的層單元及包含p-AlGaN層的層單元而形成。重複的層單元之數量為12。重複的層單元之數量可為3至50。The p-type cladding layer 70 is provided to prevent electrons from diffusing to the p-type contact layer 80. The p-type cladding layer 70 is formed by alternately depositing layer units including a p-InGaN layer and layer units including a p-AlGaN layer. The number of repeated layer units is 12. The number of repeating layer units can range from 3 to 50.
p型接觸層80包含第一p型接觸層81及第二p型接觸層82。這些層之每一者係由以Mg摻雜p-GaN所形成。第二p型接觸層82實際上與p型電極P1接觸。因此,在發光裝置100中,第二p型接觸層82係定位在相對藍寶石基板10側的該側上。第一p型接觸層81係位在第二p型接觸層82的下方。The p-type contact layer 80 includes a first p-type contact layer 81 and a second p-type contact layer 82. Each of these layers is formed of Mg-doped p-GaN. The second p-type contact layer 82 is actually in contact with the p-type electrode P1. Therefore, in the light emitting device 100, the second p-type contact layer 82 is positioned on the side opposite to the sapphire substrate 10 side. The first p-type contact layer 81 is tied below the second p-type contact layer 82.
第一p型接觸層81係以Mg在1×1019 /cm3 至1×1020 /cm3 的濃度下摻雜。當Mg濃度落在此範圍內時,便在不使結晶度惡化的情況下達到高電洞濃度。第二p型接觸層82係以Mg在1×1020 /cm3 至1×1022 /cm3 的濃度下摻雜。亦即,第二p型接觸層82係在高於第一p型接觸層81之Mg濃度的濃度下以Mg摻雜。The first p-type contact layer 81 is doped with Mg at a concentration of 1 × 10 19 /cm 3 to 1 × 10 20 /cm 3 . When the Mg concentration falls within this range, the high hole concentration is achieved without deteriorating the crystallinity. The second p-type contact layer 82 is doped with Mg at a concentration of 1 × 10 20 /cm 3 to 1 × 10 22 /cm 3 . That is, the second p-type contact layer 82 is doped with Mg at a concentration higher than the Mg concentration of the first p-type contact layer 81.
第二p型接觸層82具有10 Å至100 Å的厚度。因此,第二p型接觸層82的厚度係足夠的薄。如下所述,用於形成第二p型接觸層82的載運氣體僅包含氫(即載運氣體並不包含氮)。因而,第二p型接觸層82顯示不佳的結晶度。因此,非常薄的蕭基能障(Schottky barrier)係形成於p型電極P1及第二p型接觸層82之間。The second p-type contact layer 82 has a thickness of 10 Å to 100 Å. Therefore, the thickness of the second p-type contact layer 82 is sufficiently thin. As described below, the carrier gas used to form the second p-type contact layer 82 contains only hydrogen (ie, the carrier gas does not contain nitrogen). Thus, the second p-type contact layer 82 exhibits poor crystallinity. Therefore, a very thin Schottky barrier is formed between the p-type electrode P1 and the second p-type contact layer 82.
因此,電洞從p型電極P1輕易地移動至第二p型接觸層82。亦即,來自p型電極P1的電洞輕易地穿過蕭基能障至第二p型接觸層82中。因此,在p型電極P1及p型接觸層80之間達成較佳的歐姆接觸。Therefore, the hole is easily moved from the p-type electrode P1 to the second p-type contact layer 82. That is, the hole from the p-type electrode P1 easily passes through the Schöne barrier to the second p-type contact layer 82. Therefore, a better ohmic contact is achieved between the p-type electrode P1 and the p-type contact layer 80.
在根據本實施例之半導體裝置製造方法中,前述的個別層係經由金屬-有機化學氣相沈積法(MOCVD)成長。根據本實施例之半導體裝置製造方法的屬性特徵存在於形成p型接觸層80的步驟中。該方法的步驟接下來將參照圖2及3加以描述。In the semiconductor device manufacturing method according to the present embodiment, the aforementioned individual layers are grown by metal-organic chemical vapor deposition (MOCVD). The attribute characteristics of the semiconductor device manufacturing method according to the present embodiment exist in the step of forming the p-type contact layer 80. The steps of the method will be described next with reference to Figures 2 and 3.
在本方法中所使用的載運氣體為氫(H2 ,hydrogen)、氮(N2 ,nitrogen)、或氫加氮(H2 +N2 )的混合氣體。氨氣(NH3 )係作為氮源使用。三甲基鎵(Ga(CH3 )3 ,trimethylgallium,以下可稱為”TMG”)係作為鎵源使用。三甲基銦(In(CH3 )3 ,trimethylindium,以下可稱為”TMI”)係作為銦源使用。三甲基鋁(Al(CH3 )3 ,trimethylaluminum,以下可稱為”TMA”)係作為鋁源使用。矽烷(SiH4 ,silane)係作為n型摻雜氣體使用。環戊二烯鎂(Mg(C5 H5 )2 ,cyclopentadienylmagnesium,以下可稱為”Cp2 Mg”)係作為p型摻雜氣體使用。The carrier gas used in the method is a mixed gas of hydrogen (H 2 , hydrogen), nitrogen (N 2 , nitrogen), or hydrogen plus nitrogen (H 2 + N 2 ). Ammonia gas (NH 3 ) is used as a nitrogen source. Trimethylgallium (Ga(CH 3 ) 3 , trimethylgallium, hereinafter referred to as "TMG") is used as a gallium source. Trimethyl indium (In(CH 3 ) 3 , trimethylindium, hereinafter referred to as "TMI") is used as an indium source. Trimethylaluminum (Al(CH 3 ) 3 , trimethylaluminum, hereinafter referred to as "TMA") is used as an aluminum source. Silicone (SiH 4 , silane) is used as an n-type dopant gas. Magnesium cyclopentadienide (Mg(C 5 H 5 ) 2 , cyclopentadienylmagnesium, hereinafter referred to as "Cp 2 Mg") is used as a p-type doping gas.
在本實施例中提供藍寶石基板10,且該藍寶石基板10係放置在MOVCD爐中。接著,藍寶石基板10係在氫氣大氣中受到清洗,以進而從藍寶石基板10的表面移除沉積物。然後,基板溫度提升到400℃,且AlN低溫緩衝層20係形成在藍寶石基板10上。A sapphire substrate 10 is provided in this embodiment, and the sapphire substrate 10 is placed in a MOVCD furnace. Next, the sapphire substrate 10 is cleaned in a hydrogen atmosphere to further remove deposits from the surface of the sapphire substrate 10. Then, the substrate temperature is raised to 400 ° C, and the AlN low temperature buffer layer 20 is formed on the sapphire substrate 10.
接下來,n型接觸層30係形成於低溫緩衝層20之上(見圖2A)。然後,基板溫度在氫氣(載運氣體)及氨氣的氣流下提昇至1,100℃。在基板溫度已達到1,100℃後,TMG、氨氣、及矽烷氣體(即雜質氣體)係供應以進而形成具有4.5×1018 /cm3 的Si濃度之n-GaN的n型接觸層30。Next, an n-type contact layer 30 is formed over the low temperature buffer layer 20 (see FIG. 2A). Then, the substrate temperature was raised to 1,100 ° C under a flow of hydrogen (carrier gas) and ammonia gas. After the substrate temperature has reached 1,100 ° C, TMG, ammonia gas, and decane gas (i.e., impurity gas) are supplied to further form an n-type contact layer 30 of n-GaN having a Si concentration of 4.5 × 10 18 /cm 3 .
接著,n型ESD層40係形成於n型接觸層30上。基板溫度係降低至900℃,且係形成包含未摻雜的GaN層及摻有Si摻雜的n-GaN層之層狀結構。在此情況下,成長溫度係較佳地調整至800至950℃。該n-GaN層較佳地具有由矽原子濃密度(atom/cm3 )及厚度(nm)的乘積所定義的特徵值:0.9×1020 至3.6×1020 (atom‧nm/cm3 )。Next, an n-type ESD layer 40 is formed on the n-type contact layer 30. The substrate temperature was lowered to 900 ° C, and a layered structure including an undoped GaN layer and an Si-doped n-GaN layer was formed. In this case, the growth temperature is preferably adjusted to 800 to 950 °C. The n-GaN layer preferably has a characteristic value defined by a product of a cesium atom concentration (atom/cm 3 ) and a thickness (nm): 0.9 × 10 20 to 3.6 × 10 20 (atom ‧ nm / cm 3 ) .
接下來,n型SL層50係形成於n型ESD層40上。該n型SL層50係由交替沈積具有2.5 nm厚度的InGaN層及具有2.5 nm厚度、摻有Si的Si摻雜n-GaN層所形成。具體而言,該n型SL層50係由週期性地沈積各包含InGaN層及摻有Si摻雜的n-GaN層的15個組合層單元所形成。InGaN層係在矽烷氣體、TMG、TMI、及氨的供應下、同時基板溫度維持在830℃而形成。n-GaN層係在矽烷氣體、TMG、及氨的供應下、同時基板溫度維持在830℃下而形成。因此,形成圖2B中所示的層狀結構。Next, an n-type SL layer 50 is formed on the n-type ESD layer 40. The n-type SL layer 50 is formed by alternately depositing an InGaN layer having a thickness of 2.5 nm and a Si-doped n-GaN layer having a thickness of 2.5 nm and doped with Si. Specifically, the n-type SL layer 50 is formed by periodically depositing 15 combined layer units each including an InGaN layer and a Si-doped n-GaN layer. The InGaN layer was formed under the supply of decane gas, TMG, TMI, and ammonia while maintaining the substrate temperature at 830 °C. The n-GaN layer was formed under the supply of decane gas, TMG, and ammonia while maintaining the substrate temperature at 830 °C. Thus, the layered structure shown in Fig. 2B is formed.
接著,MQW層60係形成於n型SL層50上。MQW層60具有其中InGaN層及AlGaN層以重複的方式交替沈積的結構。InGaN層係成長在750至800℃的成長溫度。原料氣體(即TMI、TMG、及氨)係為InGaN層之成長而供應。In成份比例係0.05至0.15%。以此方式成長的晶體層具有1至4 nm的厚度。Next, the MQW layer 60 is formed on the n-type SL layer 50. The MQW layer 60 has a structure in which an InGaN layer and an AlGaN layer are alternately deposited in a repeated manner. The InGaN layer is grown at a growth temperature of 750 to 800 °C. The material gases (i.e., TMI, TMG, and ammonia) are supplied as a growth of the InGaN layer. The In composition ratio is 0.05 to 0.15%. The crystal layer grown in this way has a thickness of 1 to 4 nm.
AlGaN層係在850至950℃的成長溫度下成長。原料氣體(即TMA、TMG、及氨)係為成長AlGaN層而供應。以此方式成長的晶層具有1 至6 nm的厚度。五層InGaN層及五層AlGaN層係交替地沈積。InGaN層或AlGaN層的數量係較佳地約3至約7。The AlGaN layer is grown at a growth temperature of 850 to 950 °C. The material gases (ie, TMA, TMG, and ammonia) are supplied as a grown AlGaN layer. The crystal layer grown in this way has 1 Thickness to 6 nm. Five layers of InGaN layer and five layers of AlGaN layer are alternately deposited. The number of InGaN layers or AlGaN layers is preferably from about 3 to about 7.
接下來,p型披覆層70係形成於MQW層60上。p型披覆層70具有其中p-InGaN層及p-AlGaN層以重複的方式交替地沈積之結構。具有1.7 nm的厚度的p-InGaN層(p-In0.05 Ga0.95 N層)係在CP2 Mg、TMI、TMG、及氨的供應之下、同時基板溫度維持在855℃下而形成。Next, a p-type cladding layer 70 is formed on the MQW layer 60. The p-type cladding layer 70 has a structure in which a p-InGaN layer and a p-AlGaN layer are alternately deposited in a repeated manner. A p-InGaN layer (p-In 0.05 Ga 0.95 N layer) having a thickness of 1.7 nm was formed under the supply of CP 2 Mg, TMI, TMG, and ammonia while maintaining the substrate temperature at 855 ° C.
具有3.0 nm厚度的p-AlGaN層係在CP2 Mg、TMA、TMG及氨的供應下、同時基板溫度維持在855℃而形成。因此,形成圖2C中所示的層狀結構。The p-AlGaN layer having a thickness of 3.0 nm was formed under the supply of CP 2 Mg, TMA, TMG, and ammonia while maintaining the substrate temperature at 855 ° C. Thus, the layered structure shown in Fig. 2C is formed.
接著,第一p型接觸層81係形成於p型披覆層70上(見圖3)。氮及氫的混合氣體係使用作為載運氣體。Next, a first p-type contact layer 81 is formed on the p-type cladding layer 70 (see FIG. 3). A mixed gas system of nitrogen and hydrogen is used as a carrier gas.
利用氫的存在之優點,增加了組成原子的遷移。因此,改善了晶體品質,並亦改善了該層的表面平滑度。然而,氫原子進入晶體並與Mg結合。該結合預防Mg的活化。因此,在第一p型接觸層82中的電洞濃度並不增加。The advantage of the presence of hydrogen increases the migration of constituent atoms. Therefore, the crystal quality is improved and the surface smoothness of the layer is also improved. However, a hydrogen atom enters the crystal and binds to Mg. This combination prevents the activation of Mg. Therefore, the hole concentration in the first p-type contact layer 82 does not increase.
相反地,氮氣能藉由禁止晶體的分解而預防氮原子從晶體移除。然而,氮氣可能造成結晶度的惡化。因此,載運氣體的氮莫耳分率必須調整至落在最理想的範圍內。Conversely, nitrogen can prevent nitrogen atoms from being removed from the crystal by inhibiting decomposition of the crystal. However, nitrogen may cause deterioration in crystallinity. Therefore, the nitrogen molar fraction of the carrier gas must be adjusted to fall within the most desirable range.
載運氣體的氮莫耳分率(即混合比(N2 /(H2 +N2 )))較佳地為40%至80%。該混合比更佳地為50%至75%。該比例的具體值將於下文中描述。如下所述,當混合比(N2 /(H2 +N2 ))低於40%時,無法達到足夠的電洞濃度,而當混合比(N2 /(H2 +N2 ))超過80%時,表面可能變粗糙且凹坑可能增加。The nitrogen molar fraction of the carrier gas (i.e., the mixing ratio (N 2 /(H 2 + N 2 ))) is preferably from 40% to 80%. The mixing ratio is more preferably from 50% to 75%. Specific values for this ratio will be described below. As described below, when the mixing ratio (N 2 /(H 2 +N 2 )) is less than 40%, a sufficient hole concentration cannot be obtained, and when the mixing ratio (N 2 /(H 2 +N 2 )) exceeds At 80%, the surface may become rough and pits may increase.
晶體成長溫度係調整至900℃至1,050℃。這是因為當溫度過度地低時,GaN的晶體品質受損,而當溫度超過1,050℃時,原料氣體在個別的 原料氣體抵達藍寶石基板10之前即反應。The crystal growth temperature was adjusted to 900 ° C to 1,050 ° C. This is because when the temperature is excessively low, the crystal quality of GaN is impaired, and when the temperature exceeds 1,050 ° C, the material gas is in individual The raw material gas reacts before it reaches the sapphire substrate 10.
第一p型接觸層81係以Mg在1×1019 /cm3 至1×1020 /cm3 的濃度摻雜。這是因為當摻雜Mg濃度為1×1020 /cm3 或更低時,晶格缺陷係較不可能形成在第一p型接觸層81中。第一p型接觸層81係形成為具有100Å至1,000Å的厚度。The first p-type contact layer 81 is doped with Mg at a concentration of 1 × 10 19 /cm 3 to 1 × 10 20 /cm 3 . This is because when the doping concentration of Mg is 1 × 10 20 / cm 3 or less, more lattice defects can not be formed based on the first p-type contact layer 81. The first p-type contact layer 81 is formed to have a thickness of 100 Å to 1,000 Å.
接著,第二p型接觸層82係形成於第一p型接觸層81上。為了在第二p型接觸層82中刻意形成大量晶格缺陷的目的,僅使用氫氣作為載運氣體。因此,氮氣的供應停止,且僅供應氫氣作為載運氣體。亦即,使用的載運氣體並不包含氮。然而,由於前述的層形成步驟係連續地在MOCVD爐的內部執行,故氮氣可能留在該爐的大氣中。Next, a second p-type contact layer 82 is formed on the first p-type contact layer 81. In order to intentionally form a large number of lattice defects in the second p-type contact layer 82, only hydrogen gas is used as the carrier gas. Therefore, the supply of nitrogen gas is stopped, and only hydrogen gas is supplied as the carrier gas. That is, the carrier gas used does not contain nitrogen. However, since the aforementioned layer forming step is continuously performed inside the MOCVD furnace, nitrogen may remain in the atmosphere of the furnace.
晶體成長溫度係調整至800℃至1,050℃。這是因為當成長溫度低於800℃時,GaN的晶體品質受損,而當成長溫度超過1,050℃時,反應可能在氨、Ga、Mg…等抵達藍寶石基板10前於反應爐的大氣中進行。The crystal growth temperature was adjusted to 800 ° C to 1,050 ° C. This is because when the growth temperature is lower than 800 ° C, the crystal quality of GaN is impaired, and when the growth temperature exceeds 1,050 ° C, the reaction may be carried out in the atmosphere of the reaction furnace before ammonia, Ga, Mg, etc. arrive at the sapphire substrate 10. .
第二p型接觸層82係以Mg在1×1020 /cm3 至1×1022 /cm3 的濃度摻雜。這是因為當摻雜Mg濃度為1×1020 /cm3 或更高時,晶格缺陷係較可能形成在所產生的半導體層中。The second p-type contact layer 82 is doped with Mg at a concentration of 1 × 10 20 /cm 3 to 1 × 10 22 /cm 3 . This is because when the doping Mg concentration is 1 × 10 20 /cm 3 or higher, lattice defects are more likely to be formed in the produced semiconductor layer.
第二p型接觸層82係形成為具有10Å至100Å的厚度。這是因為當厚度小於10Å時,在形成晶格缺陷上會遇到困難。由於GaN在c軸方向中具有5.185Å的晶格常數,故當層厚對應到兩或更多GaN分子層的厚度時容易形成晶格缺陷。然而,具有晶格缺陷的該層的厚度越大,其電阻越高。因此,第二p型接觸層82的厚度較佳地為100Å或更小,更佳地為20Å至90Å,再更佳地為30Å至70Å。The second p-type contact layer 82 is formed to have a thickness of 10 Å to 100 Å. This is because when the thickness is less than 10 Å, difficulties are encountered in forming lattice defects. Since GaN has a lattice constant of 5.185 Å in the c-axis direction, lattice defects are easily formed when the layer thickness corresponds to the thickness of two or more GaN molecular layers. However, the greater the thickness of the layer having lattice defects, the higher its resistance. Therefore, the thickness of the second p-type contact layer 82 is preferably 100 Å or less, more preferably 20 Å to 90 Å, still more preferably 30 Å to 70 Å.
接下來,MOCVD爐係在氮氣大氣中冷卻至環境溫度。具體而言,圖3中所示的層狀產品90係在氮氣大氣中冷卻以預防脫附的氫再結合進入層狀產品90中。Next, the MOCVD furnace was cooled to ambient temperature in a nitrogen atmosphere. Specifically, the layered product 90 shown in FIG. 3 is cooled in a nitrogen atmosphere to prevent recombination of desorbed hydrogen into the layered product 90.
接著,乾蝕刻係從p型接觸層80的上表面執行,以進而形成延伸到n型接觸層30中間部份的溝槽。然後,p型電極P1係形成於p型接觸層80上。該p型電極P1係藉由以Ni層、Au層、然後Al層的順序在p型接觸層80上沈積而形成。這些金屬之任何者可以ITO取代。又,Ni/Au配線電極可形成在ITO電極上。替代地,可使用Ag或Rh。n型電極N1係形成於n型接觸層30因此暴露的部份上。該n型電極N1係藉由以Ni層然後Au層的順序在n型接觸層30上沈積而形成。替代地,n型電極N1可藉由連續地沈積Ti層及Al層在n型接觸層30上而形成。Next, dry etching is performed from the upper surface of the p-type contact layer 80 to further form a trench extending to the intermediate portion of the n-type contact layer 30. Then, a p-type electrode P1 is formed on the p-type contact layer 80. The p-type electrode P1 is formed by depositing on the p-type contact layer 80 in the order of a Ni layer, an Au layer, and then an Al layer. Any of these metals can be replaced by ITO. Further, a Ni/Au wiring electrode can be formed on the ITO electrode. Alternatively, Ag or Rh can be used. The n-type electrode N1 is formed on the exposed portion of the n-type contact layer 30. The n-type electrode N1 is formed by depositing on the n-type contact layer 30 in the order of a Ni layer and then an Au layer. Alternatively, the n-type electrode N1 can be formed by continuously depositing a Ti layer and an Al layer on the n-type contact layer 30.
接下來,為了活化摻雜在其上的Mg之目的,層狀產品90係在氮大氣中受到熱處理(退火)。此退火步驟可在電極形成步驟之前、或在冷卻步驟之前執行。因此,製造了圖1中所顯示的發光裝置100。Next, in order to activate Mg doped thereon, the layered product 90 is subjected to heat treatment (annealing) in a nitrogen atmosphere. This annealing step can be performed before the electrode forming step or before the cooling step. Thus, the light emitting device 100 shown in Fig. 1 is fabricated.
在根據本實施例的發光裝置100中,p型接觸層80包含第一p型接觸層81及第二p型接觸層82。藉由第二p型接觸層82的存在之優點,在p型接觸層80及p型電極P1之間的蕭基能障具有小的厚度。因此,在p型接觸層80及p型電極P1之間達到高電洞傳導率。In the light emitting device 100 according to the present embodiment, the p-type contact layer 80 includes the first p-type contact layer 81 and the second p-type contact layer 82. By virtue of the existence of the second p-type contact layer 82, the Schindler barrier between the p-type contact layer 80 and the p-type electrode P1 has a small thickness. Therefore, high hole conductivity is achieved between the p-type contact layer 80 and the p-type electrode P1.
第二p型接觸層82具有許多晶格缺陷。自不待言,在第二p型接觸層82中晶格缺陷的數量多於在第一p型接觸層81中的晶格缺陷者。因此,在p型電極P1及第二p型接觸層82之間達到高電洞傳導率。The second p-type contact layer 82 has a number of lattice defects. Needless to say, the number of lattice defects in the second p-type contact layer 82 is larger than that in the first p-type contact layer 81. Therefore, high hole conductivity is achieved between the p-type electrode P1 and the second p-type contact layer 82.
現將描述其中並未設置第二p型接觸層82的情況。當p型電極P1與第一p型接觸層81接觸時,與其中第二p型接觸層82存在的情況相比,驅動電壓Vf變高。可理解地,相對厚的蕭基能障係形成於第一p型接觸層81及p型電極P1之間。A case in which the second p-type contact layer 82 is not provided will now be described. When the p-type electrode P1 is in contact with the first p-type contact layer 81, the driving voltage Vf becomes higher than in the case where the second p-type contact layer 82 exists. It is understood that a relatively thick Schottky barrier is formed between the first p-type contact layer 81 and the p-type electrode P1.
相反地,當設置第二P型接觸層82時,蕭基能障的厚度減少; 即電洞能在p型電極P1及p型接觸層80之間輕易移動。如上所述,在第二p型接觸層82中晶格缺陷的數量多於在第一p型接觸層81中的晶格缺陷者。因此,電洞能更容易地在p型電極P1及p型接觸層80之間移動。因此,根據本實施例之發光裝置100表現低電阻率。Conversely, when the second P-type contact layer 82 is disposed, the thickness of the Schindler barrier is reduced; That is, the hole can be easily moved between the p-type electrode P1 and the p-type contact layer 80. As described above, the number of lattice defects in the second p-type contact layer 82 is larger than that in the first p-type contact layer 81. Therefore, the hole can be more easily moved between the p-type electrode P1 and the p-type contact layer 80. Therefore, the light-emitting device 100 according to the present embodiment exhibits a low resistivity.
接下來將描述執行在根據本實施例之發光裝置100上的實驗結果。現將描述藉由改變用於形成第一p型接觸層81的載運氣體中之氮混合比所決定的物理值。Next, the experimental results performed on the light-emitting device 100 according to the present embodiment will be described. The physical value determined by changing the nitrogen mixture ratio in the carrier gas for forming the first p-type contact layer 81 will now be described.
圖4係顯示第一p型接觸層81的電洞濃度相關於氮混合比(N2 /(H2 +N2 ))之圖表。在圖4中,白色符號對應至在其中並未執行退火的情況中的值,且黑色符號對應至在其中執行退火的情況中的值。相同者將適用於圖5及6。4 is a graph showing the hole concentration of the first p-type contact layer 81 in relation to the nitrogen mixture ratio (N 2 /(H 2 +N 2 )). In FIG. 4, the white symbol corresponds to a value in the case where annealing is not performed, and the black symbol corresponds to a value in the case where annealing is performed. The same applies to Figures 5 and 6.
如圖4中所示,大致而言,其中執行退火的情況中電洞濃度係高於其中並未執行退火的情況中者。亦即在其中執行退火的情況中,不論氮混合比,電洞濃度皆足夠高。具體而言,達到約5×1016 /cm3 至約6×1016 /cm3 的電洞濃度。As shown in FIG. 4, roughly, in the case where annealing is performed, the hole concentration is higher than in the case where annealing is not performed. That is, in the case where annealing is performed, the hole concentration is sufficiently high regardless of the nitrogen mixture ratio. Specifically, a hole concentration of about 5 × 10 16 /cm 3 to about 6 × 10 16 /cm 3 is achieved.
相反地,在其中並未執行退火的情況中,電洞濃度係藉由增加氮濃度而增加。在其中氮混合比係調整至44%的情況中,即使當並未執行退火時,仍達到約2×1016 /cm3 至3×1016 /cm3 的電洞濃度。亦即,電洞濃度係在其中執行退火的情況中者的約1/2。因此可理解地,氫原子在退火前係與一半的Mg原子鍵結。Conversely, in the case where annealing is not performed, the hole concentration is increased by increasing the nitrogen concentration. In the case where the nitrogen mixture ratio was adjusted to 44%, a hole concentration of about 2 × 10 16 /cm 3 to 3 × 10 16 /cm 3 was reached even when annealing was not performed. That is, the hole concentration is about 1/2 of the case in which annealing is performed. Thus, it is understood that the hydrogen atoms are bonded to half of the Mg atoms before annealing.
在其中氮混合比係調整至66%的情況中,即使當退火並未執行時,仍達到約5×1016 /cm3 的電洞濃度。亦即,電洞濃度幾乎等於在其中執行退火的情況者。因此可理解地,實際上即使在退火之前仍無氫原子與Mg原子鍵結。因此當氮混合比係調整至44%或66%時,獲得足夠高的電洞濃度。In the case where the nitrogen mixture ratio was adjusted to 66%, a hole concentration of about 5 × 10 16 /cm 3 was reached even when annealing was not performed. That is, the hole concentration is almost equal to the case in which the annealing is performed. It is therefore understood that virtually no hydrogen atoms are bonded to the Mg atoms even before annealing. Therefore, when the nitrogen mixture ratio is adjusted to 44% or 66%, a sufficiently high hole concentration is obtained.
圖5係顯示第一p型接觸層81中的電洞遷移率相關於氮混合比(N2 /(H2 +N2 ))之圖表。如圖5中所示,在其中執行退火的情況及其中並未執行退火的情況之間觀察到較少電洞遷移率中的變異。當氮氣濃度增加時,電洞遷移率改善;即晶格缺陷減少。此指示形成具有好的晶體品質之p-GaN層。Fig. 5 is a graph showing the hole mobility in the first p-type contact layer 81 in relation to the nitrogen mixture ratio (N 2 /(H 2 + N 2 )). As shown in FIG. 5, variation in less hole mobility was observed between the case where annealing was performed and the case where annealing was not performed. As the nitrogen concentration increases, the hole mobility improves; that is, the lattice defects decrease. This indication forms a p-GaN layer with good crystal quality.
在其中氮混合比係調整至22%的情況中,當並未執行退火時獲得約2 cm2 /V‧s的電洞遷移率,而當執行退火時獲得約3 cm2 /V‧s的電洞遷移率。在其中氮混合比係調整至44%的情況中,不論是否執行退火皆獲得4 cm2 /V‧s的電洞遷移率。在其中氮混合比係調整至66%的情況中,不論是否執行退火皆獲得7至8 cm2 /V‧s的電洞遷移率。In the case where the nitrogen mixture ratio was adjusted to 22%, a hole mobility of about 2 cm 2 /V‧s was obtained when annealing was not performed, and about 3 cm 2 /V‧s was obtained when annealing was performed. Hole mobility. In the case where the nitrogen mixture ratio was adjusted to 44%, a hole mobility of 4 cm 2 /V‧s was obtained regardless of whether or not annealing was performed. In the case where the nitrogen mixture ratio was adjusted to 66%, a hole mobility of 7 to 8 cm 2 /V‧s was obtained regardless of whether or not annealing was performed.
因此,退火在電洞遷移率中造成輕微的差異。尤其當氮混合比係調整至44%或66%時,退火實際上在電洞遷移率中不造成差異。因而,能形成具有良好電洞傳導率之p-GaN層。Therefore, annealing causes a slight difference in hole mobility. Especially when the nitrogen mixing ratio is adjusted to 44% or 66%, annealing does not actually cause a difference in hole mobility. Thus, a p-GaN layer having good hole conductivity can be formed.
圖6係顯示第一p型接觸層81的電阻率相關於氮混合比(N2 /(H2 +N2 ))之圖表。如圖6中所示,大致來說,氮混合比越高,電阻率就越低。可理解地,此在電阻率中的減少係歸因於晶體品質改善的事實,且藉由晶格缺陷造成的電阻成份減少。此係由電洞遷移率的改善而證明。Fig. 6 is a graph showing the resistivity of the first p-type contact layer 81 in relation to the nitrogen mixture ratio (N 2 /(H 2 + N 2 )). As shown in FIG. 6, roughly, the higher the nitrogen mixing ratio, the lower the electrical resistivity. Understandably, this decrease in resistivity is due to the fact that the crystal quality is improved, and the resistance component due to lattice defects is reduced. This is evidenced by the improvement in hole mobility.
在其中氮混合比係調整至22%的情況中,未退火的第一p型接觸層81顯示約110Ω‧cm的電阻率,且退火的第一p型接觸層81顯示約40至約50Ω‧cm的電阻率。未退火的第一p型接觸層81的電阻率係退火的第一p型接觸層81者的約兩倍。亦即,氫原子在退火前仍與一半的Mg原子鍵結。In the case where the nitrogen mixing ratio is adjusted to 22%, the unannealed first p-type contact layer 81 exhibits a resistivity of about 110 Ω ‧ cm, and the annealed first p-type contact layer 81 exhibits about 40 to about 50 Ω The resistivity of cm. The resistivity of the unannealed first p-type contact layer 81 is about twice that of the annealed first p-type contact layer 81. That is, the hydrogen atoms are still bonded to half of the Mg atoms before annealing.
在其中氮混合比係調整至44%的情況中,未退火的第一p型接觸層81顯示約40至約70Ω‧cm的電阻率,其係幾乎等於在22%的氮混合比之情況中退火的第一p型接觸層81者。在其中氮混合比係調整至44%的情況中,退火的第一p型接觸層81顯示約20Ω‧cm的電阻率。亦即,未退 火的第一p型接觸層81的電阻率係退火的第一p型接觸層81者的約兩倍。In the case where the nitrogen mixture ratio is adjusted to 44%, the unannealed first p-type contact layer 81 exhibits a resistivity of about 40 to about 70 Ω ‧ cm, which is almost equal to the case of a nitrogen mixture ratio of 22% The first p-type contact layer 81 is annealed. In the case where the nitrogen mixture ratio was adjusted to 44%, the annealed first p-type contact layer 81 exhibited a resistivity of about 20 Ω ‧ cm. That is, not refunded The resistivity of the first p-type contact layer 81 of the fire is about twice that of the annealed first p-type contact layer 81.
在其中氮混合比係調整至66%的情況中,未退火的第一p型接觸層81顯示約15Ω‧cm的電阻率。在其中氮混合比係調整至66%的情況中,退火的第一p型接觸層81顯示約12Ω‧cm的電阻率。亦即,不論是否執行退火,這些層的電阻率係幾乎彼此相等。In the case where the nitrogen mixture ratio was adjusted to 66%, the unannealed first p-type contact layer 81 exhibited a resistivity of about 15 Ω ‧ cm. In the case where the nitrogen mixture ratio was adjusted to 66%, the annealed first p-type contact layer 81 exhibited a resistivity of about 12 Ω ‧ cm. That is, the resistivity of these layers is almost equal to each other regardless of whether or not annealing is performed.
在66%的氮混合比之情況中非退火的第一p型接觸層81的電阻率(即15Ω‧cm)係足夠地低於在22%的氮混合比之情況中退火的第一p型接觸層81的電阻率(即40至50Ω‧cm)。因此,當第一p型接觸層81藉由使用氮及氫的混合氣體作為載運氣體而形成時,該層的電阻非常有效地減少。The resistivity (i.e., 15 Ω ‧ cm) of the non-annealed first p-type contact layer 81 in the case of a 66% nitrogen mixture ratio is sufficiently lower than the first p-type annealed in the case of a nitrogen mixture ratio of 22% The resistivity of the contact layer 81 (i.e., 40 to 50 Ω ‧ cm). Therefore, when the first p-type contact layer 81 is formed by using a mixed gas of nitrogen and hydrogen as a carrier gas, the electric resistance of the layer is very effectively reduced.
圖7係顯示第一p型接觸層81的活化百分比相關於氮混合比(N2 /(H2 +N2 ))之圖表。在此圖表中,所有的值對應到其中執行退火的情況。Fig. 7 is a graph showing the percentage of activation of the first p-type contact layer 81 in relation to the nitrogen mixture ratio (N 2 /(H 2 + N 2 )). In this chart, all values correspond to the case in which annealing is performed.
如圖7中所示,在其中氮並未混合至載運氣體中(即僅使用氫)的情況,第一p型接觸層81顯示約0.12%的活化百分比。當氮混合比增加時,起初活化百分比降低。當氮混合比為22%時,第一p型接觸層81顯示約0.07%的活化百分比。As shown in Figure 7, in the case where nitrogen was not mixed into the carrier gas (i.e., only hydrogen was used), the first p-type contact layer 81 exhibited a percent activation of about 0.12%. As the nitrogen mixing ratio increases, the initial percentage of activation decreases. When the nitrogen mixing ratio was 22%, the first p-type contact layer 81 showed a percentage of activation of about 0.07%.
然而,當氮混合比進一步增加時,活化百分比亦增加。當氮混合比為35%或大約者時,活化百分比幾乎等於在其中氮混合比為0%的情況者。當氮混合比為40%或更多時達到足夠高的活化百分比。However, as the nitrogen mixing ratio is further increased, the percentage of activation also increases. When the nitrogen mixing ratio is 35% or about, the percentage of activation is almost equal to the case where the nitrogen mixing ratio is 0%. A sufficiently high percentage of activation is achieved when the nitrogen mixing ratio is 40% or more.
當氮混合比係調整至44%時,第一p型接觸層81顯示約0.14%的活化百分比。當氮混合比係調整至66%時,第一p型接觸層81顯示約0.21%的活化百分比,其係一足夠高的值。When the nitrogen mixing ratio was adjusted to 44%, the first p-type contact layer 81 showed an activation percentage of about 0.14%. When the nitrogen mixing ratio was adjusted to 66%, the first p-type contact layer 81 showed an activation percentage of about 0.21%, which was a sufficiently high value.
圖8係顯示其中第一p型接觸層81係由利用氫氣形成的情況(習知情況)、及其中第一p型接觸層81係由利用氮氣及氫氣的混合氣體(氮混合比:66%)形成的情況(本實施例)之間發光裝置的相對光強度比較之圖表。顯示在 圖8中的結果對應至其中執行退火的情況。在圖8中垂直軸對應至根據習知情況的光強度之相對光強度。自不待言,習知情況的相對光強度對應至100%。8 is a view showing a case where the first p-type contact layer 81 is formed by using hydrogen gas (conventional case), and a first p-type contact layer 81 thereof is a mixed gas using nitrogen gas and hydrogen gas (nitrogen mixture ratio: 66%) A graph comparing the relative light intensities of the light-emitting devices between the cases formed (this embodiment). show on The result in Fig. 8 corresponds to the case in which annealing is performed. In Fig. 8, the vertical axis corresponds to the relative light intensity of the light intensity according to the conventional case. Needless to say, the relative light intensity of the conventional situation corresponds to 100%.
如圖8中所示,在其中第一p型接觸層81係藉由使用氮氣及氫氣的混合氣體(氮混合比:66%)作為載運氣體而形成的情況,光輸出係高於在習知情況中者約10%。如上所述,這是因為藉由利用混合氣體作為載運氣體而製造的發光裝置顯示更佳的電阻率、電洞濃度、電洞遷移率、及活化百分比。As shown in FIG. 8, in the case where the first p-type contact layer 81 is formed by using a mixed gas of nitrogen gas and hydrogen gas (nitrogen mixture ratio: 66%) as a carrier gas, the light output system is higher than conventionally. In the case of about 10%. As described above, this is because the light-emitting device manufactured by using the mixed gas as the carrier gas exhibits better resistivity, hole concentration, hole mobility, and percentage of activation.
在這些實驗中,當氮混合比係調整至66%時獲得最佳結果,且即使當氮混合比係調整至44%時仍獲得良好的結果。因此可理解地,除了在其中氮混合比為44%至66%的情況之外,本發明還可適用於其中氮混合比係高於此範圍(即氮混合比為80或更少)的情況。然而,當氮混合比高時,可能出現表面粗糙或凹坑增加的情況。因而,氮混合比較佳地為50%至70%。可理解地,氮混合比更佳地為55%至70%。In these experiments, the best results were obtained when the nitrogen mixing ratio was adjusted to 66%, and good results were obtained even when the nitrogen mixture ratio was adjusted to 44%. Therefore, it is understood that the present invention is also applicable to the case where the nitrogen mixing ratio is higher than this range (i.e., the nitrogen mixing ratio is 80 or less), except in the case where the nitrogen mixing ratio is from 44% to 66%. . However, when the nitrogen mixing ratio is high, there may occur a case where the surface roughness or pits increase. Thus, nitrogen mixing is preferably from 50% to 70%. It is understood that the nitrogen mixing ratio is more preferably from 55% to 70%.
在本實施例中,退火(熱處理)係於p型電極P1及n型電極N1形成在層狀結構90上之後執行。然而,如圖4至6中所示,退火並不必然地執行。如按電洞濃度(見圖4)、電洞遷移率(見圖5)、電阻率(見圖6)、及活化百分比(見圖7)的數據可瞭解,即使當不執行退火時,仍能製造顯示相對低的電阻率之發光裝置。因此,一製造步驟能被省略;即,發光裝置係在改善的生產率中製造。In the present embodiment, annealing (heat treatment) is performed after the p-type electrode P1 and the n-type electrode N1 are formed on the layered structure 90. However, as shown in FIGS. 4 to 6, annealing is not necessarily performed. For example, according to the hole concentration (see Figure 4), hole mobility (see Figure 5), resistivity (see Figure 6), and percent activation (see Figure 7), even when annealing is not performed, A light-emitting device capable of exhibiting a relatively low resistivity can be manufactured. Therefore, a manufacturing step can be omitted; that is, the light-emitting device is manufactured with improved productivity.
在本實施例中,第一p型接觸層81及第二p型接觸層82之每一者係由p-GaN形成。然而,層81及82可由p-InGaN代替p-GaN而形成。由於p-GaN的使用實現了歐姆接觸的改善,故即使當使用具有小於p-GaN者的能隙之p-InGaN時,類似的結果仍係必然地獲得。In the present embodiment, each of the first p-type contact layer 81 and the second p-type contact layer 82 is formed of p-GaN. However, layers 81 and 82 may be formed by p-InGaN instead of p-GaN. Since the use of p-GaN achieves an improvement in ohmic contact, similar results are inevitably obtained even when p-InGaN having an energy gap smaller than that of p-GaN is used.
在具體的情況中,第一p型接觸層81係由p-GaN形成、且第二p型接觸層82係由p-InGaN形成。替代地,第一p型接觸層81可由p-InGaN形成、且第二p型接觸層82亦可由p-InGaN形成。在此情況中,第二p型接觸層82的In組成比例係較佳地調整至高於第一p型接觸層81者。In a specific case, the first p-type contact layer 81 is formed of p-GaN, and the second p-type contact layer 82 is formed of p-InGaN. Alternatively, the first p-type contact layer 81 may be formed of p-InGaN, and the second p-type contact layer 82 may also be formed of p-InGaN. In this case, the In composition ratio of the second p-type contact layer 82 is preferably adjusted to be higher than that of the first p-type contact layer 81.
如上所詳細描述,在根據本實施例之製造發光裝置100的方法中,第一p型接觸層81係經由使用氮及氫的混合氣體作為載運氣體的第一p型接觸層形成步驟而形成,且第二p型接觸層82係經由使用氫作為載運氣體的第二p型接觸層形成步驟而形成。As described in detail above, in the method of manufacturing the light-emitting device 100 according to the present embodiment, the first p-type contact layer 81 is formed via a first p-type contact layer forming step using a mixed gas of nitrogen and hydrogen as a carrier gas, And the second p-type contact layer 82 is formed via a second p-type contact layer forming step using hydrogen as a carrier gas.
因此,根據製造三族氮化物半導體發光裝置的方法,電洞遷移率能在p型接觸層80中被改善,且p型接觸層80及p型電極P1之間的接觸電阻能被減少。Therefore, according to the method of manufacturing the group III nitride semiconductor light-emitting device, the hole mobility can be improved in the p-type contact layer 80, and the contact resistance between the p-type contact layer 80 and the p-type electrode P1 can be reduced.
本實施例僅係例示,其不應被解釋為將本發明限制於該實施例。因此,自不待言,在不離開本發明之範疇的情況下可對本發明作成不同的修改及變化。本實施例中係使用顯示在圖3中的層狀結構90。然而,層狀產品的結構並不必然地限於圖3中所示者。例如,可選擇任何層狀結構,或可為了形成各層而決定層單元的任何數量。自不待言,p型接觸層80以外的層之組成可不同於本實施例中所述者。晶體成長並不必然地經由金屬-有機化學氣相沈積法(MOCVD)執行,且可使用任何其他使用載運氣體的晶體成長方法。This embodiment is merely illustrative, and should not be construed as limiting the invention to the embodiment. Therefore, it is to be understood that various modifications and changes can be made in the present invention without departing from the scope of the invention. The layered structure 90 shown in Fig. 3 is used in this embodiment. However, the structure of the layered product is not necessarily limited to that shown in FIG. For example, any layered structure may be selected, or any number of layer units may be determined in order to form the layers. Needless to say, the composition of the layers other than the p-type contact layer 80 may be different from that described in the embodiment. Crystal growth is not necessarily performed via metal-organic chemical vapor deposition (MOCVD), and any other crystal growth method using a carrier gas can be used.
10‧‧‧藍寶石基板10‧‧‧Sapphire substrate
20‧‧‧低溫緩衝層20‧‧‧Low temperature buffer layer
30‧‧‧N型接觸層30‧‧‧N type contact layer
40‧‧‧N型ESD層40‧‧‧N type ESD layer
50‧‧‧N型SL層50‧‧‧N type SL layer
60‧‧‧MQW層60‧‧‧MQW layer
70‧‧‧P型披覆層70‧‧‧P type coating
80‧‧‧P型接觸層80‧‧‧P type contact layer
100‧‧‧發光裝置100‧‧‧Lighting device
N1‧‧‧N型電極N1‧‧‧N type electrode
P1‧‧‧P型電極P1‧‧‧P type electrode
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