TWI545798B - Nitride semiconductor light emitting device and manufacturing method thereof - Google Patents

Nitride semiconductor light emitting device and manufacturing method thereof Download PDF

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TWI545798B
TWI545798B TW103141259A TW103141259A TWI545798B TW I545798 B TWI545798 B TW I545798B TW 103141259 A TW103141259 A TW 103141259A TW 103141259 A TW103141259 A TW 103141259A TW I545798 B TWI545798 B TW I545798B
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nitride semiconductor
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Katsuji Iguchi
Mayuko Fudeta
Kazuya Araki
Eiji Yamada
Akihiro Urata
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Sharp Kk
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氮化物半導體發光元件及其製造方法 Nitride semiconductor light-emitting element and method of manufacturing same

本發明係關於氮化物半導體發光元件及其製造方法。 The present invention relates to a nitride semiconductor light-emitting element and a method of manufacturing the same.

包含氮之III-V族化合物半導體(III族氮化物半導體)係具有與具有自紅外線區域至紫外線區域之波長的光之能量相當之帶隙能量。因此,III族氮化物半導體可使用作為發出具有自紅外線區域至紫外線區域之波長的光之發光元件之材料、或作為接收具有自紅外線區域至紫外線區域之波長的光之受光元件之材料。 The III-V compound semiconductor (III-nitride semiconductor) containing nitrogen has a band gap energy equivalent to the energy of light having a wavelength from the infrared region to the ultraviolet region. Therefore, the group III nitride semiconductor can be used as a material for emitting a light-emitting element having light having a wavelength from an infrared region to an ultraviolet region, or as a material for receiving a light-receiving element having light having a wavelength from an infrared region to an ultraviolet region.

又,構成III族氮化物半導體之原子間之結合較強,III族氮化物半導體之絕緣破壞電壓較高,其飽和電子速度較大。藉此,III族氮化物半導體亦可使用作為耐高溫、高輸出、高頻電晶體等之電子設備之材料。再者,III族氮化物半導體因幾乎不危害環境,故亦作為易於處理之材料備受矚目。 Further, the bonding between the atoms constituting the group III nitride semiconductor is strong, and the breakdown breakdown voltage of the group III nitride semiconductor is high, and the saturation electron velocity is large. Thereby, the group III nitride semiconductor can also be used as a material of an electronic device such as a high temperature resistant, high output, high frequency transistor, or the like. Furthermore, Group III nitride semiconductors have attracted attention as materials that are easy to handle because they hardly harm the environment.

於使用此III族氮化物半導體之氮化物半導體發光元件中,作為發光層,一般採用量子井構造。若電壓施加於氮化物半導體發光元件,則於構成發光層之井層中,電子與電洞再結合而產生光。發光層亦可為單一量子井(Single Quantum Well(SQW))構造,又可為井層與障壁層交替積層之多重量子井(Multiple Quantum Well(MQW))構造。 In the nitride semiconductor light-emitting device using the group III nitride semiconductor, a quantum well structure is generally used as the light-emitting layer. When a voltage is applied to the nitride semiconductor light-emitting element, electrons and holes are recombined in the well layer constituting the light-emitting layer to generate light. The luminescent layer can also be a single quantum well (SQW) structure or a multiple quantum well (MQW) structure in which the well layer and the barrier layer are alternately stacked.

為了使用如上述之優異材料即III族氮化物半導體製造實用之氮化物半導體發光元件,必須於特定之基板上形成包含III族氮化物半導體之薄膜(III族氮化物半導體層),且形成特定之元件構造。 In order to manufacture a practical nitride semiconductor light-emitting device using a Group III nitride semiconductor as the above-described excellent material, it is necessary to form a film (Group III nitride semiconductor layer) containing a Group III nitride semiconductor on a specific substrate, and form a specific one. Component construction.

此處,作為基板,最好使用包含具有可使III族氮化物半導體層於基板上直接成長之晶格常數或熱膨脹係數等之III族氮化物半導體之基板。作為包含III族氮化物半導體之基板,可例舉例如氮化鎵(GaN)基板等。然而,GaN基板於現況中由於其尺寸較小而為2英吋以下,且價格極高,故並不實用。因此,於現況中,作為氮化物半導體發光元件之製造用基板,係使用與III族氮化物半導體之晶格常數差及熱膨脹係數差較大之藍寶石基板或碳化矽(SiC)基板等。 Here, as the substrate, a substrate containing a group III nitride semiconductor having a lattice constant or a thermal expansion coefficient which allows the group III nitride semiconductor layer to directly grow on the substrate is preferably used. As the substrate including the group III nitride semiconductor, for example, a gallium nitride (GaN) substrate or the like can be exemplified. However, the GaN substrate is not practical in the current state because it has a small size of 2 inches or less and is extremely expensive. Therefore, in the current state of the art, a substrate for manufacturing a nitride semiconductor light-emitting device is a sapphire substrate or a tantalum carbide (SiC) substrate having a large difference in lattice constant and a large difference in thermal expansion coefficient from the group III nitride semiconductor.

於藍寶石與GaN(III族氮化物半導體之代表例)之間存在約16%左右之晶格常數差。於SiC與GaN之間存在約6%左右之晶格常數差。在如此大小之晶格常數差存在於基板材料與成長於該基板上之III族氮化物半導體之間時,一般難以使包含III族氮化物半導體之結晶磊晶成長於基板上。例如,於藍寶石基板上使GaN結晶直接磊晶成長時,存在無法避免GaN結晶之3維成長,而無法獲得具有平坦表面之GaN結晶之問題。 There is a difference in lattice constant of about 16% between sapphire and GaN (a representative example of a group III nitride semiconductor). There is a difference in lattice constant of about 6% between SiC and GaN. When a difference in lattice constant of such a size exists between the substrate material and the group III nitride semiconductor grown on the substrate, it is generally difficult to crystallize the crystal containing the group III nitride semiconductor on the substrate. For example, when GaN crystals are directly epitaxially grown on a sapphire substrate, there is a problem in that three-dimensional growth of GaN crystals cannot be avoided, and GaN crystals having a flat surface cannot be obtained.

因此,於基板與III族氮化物半導體層之間,一般進行形成用以消除基板材料與III族氮化物半導體之間之晶格常數差之稱為所謂緩衝層之層。 Therefore, between the substrate and the group III nitride semiconductor layer, a layer called a buffer layer for eliminating a difference in lattice constant between the substrate material and the group III nitride semiconductor is generally formed.

例如,於日本特開平2-229476號公報中,記述有於藍寶石基板上藉由有機金屬氣相成長法(MOVPE法)形成包含AlN之緩衝層後,使包含AlxGa1-xN之III族氮化物半導體層成長之方法。 For example, in JP-A No. 2-229476, a buffer layer containing AlN is formed on a sapphire substrate by an organometallic vapor phase growth method (MOVPE method), and then Al x Ga 1-x N is included. A method of growing a nitride semiconductor layer.

於日本特開2006-324694號公報中,記述有為了使高品質氮化物半導體膜成長,而使氮化物半導體膜自基板之凸部上側向成長至該基板之凹部上。 In order to grow a high-quality nitride semiconductor film, the nitride semiconductor film is grown from the convex portion of the substrate to the concave portion of the substrate in order to grow the high-quality nitride semiconductor film.

於日本特開2006-352084號公報中,記述有下述所示之方法作為III族氮化物半導體層之成長方法。首先,準備經實施凹凸加工之藍寶石基板。其次,自藍寶石基板之凹部底面開始GaN之磊晶成長,且以 成為將該底面作為底邊,於斜面具有相對於藍寶石基板之主表面傾斜之晶面之二等邊三角形之剖面形狀之方式使GaN成長。繼而,若於以橫方向成長為支配之條件設定成長條件並繼續成長,則GaN層係其厚度增加且於藍寶石基板之凸部上擴展,繼而與自鄰接之藍寶石基板之凹部成長之GaN層彼此於藍寶石基板之凸部上接觸。 A method of growing a group III nitride semiconductor layer as described below is described in Japanese Laid-Open Patent Publication No. 2006-352084. First, a sapphire substrate subjected to embossing processing is prepared. Secondly, the epitaxial growth of GaN is started from the bottom surface of the concave portion of the sapphire substrate, and The GaN is grown so that the bottom surface is a base and the cross-sectional shape of the equilateral triangle having a crystal plane inclined with respect to the main surface of the sapphire substrate. Then, if the growth conditions are set under the conditions of growth in the lateral direction and continue to grow, the GaN layer is increased in thickness and spread over the convex portion of the sapphire substrate, and then the GaN layers growing from the concave portions of the adjacent sapphire substrate are mutually grown. Contacted on the convex portion of the sapphire substrate.

於國際公開第2011/074534號中,記述有若於基板上配置特定之凸部且使基底層成長,則於結晶成長初期獲得結晶性優異之結晶成長膜,並製造附有優異磊晶膜之模板基板。於國際公開第2011/074534號公報中,記述有若使用結晶性優異之模板基板形成發光層,則可製造光取出效率優異之高輸出之半導體發光元件。 In the case of arranging a specific convex portion on a substrate and growing the underlayer, the crystal growth film having excellent crystallinity at the initial stage of crystal growth is obtained, and an excellent epitaxial film is produced. Template substrate. In the case of forming a light-emitting layer using a template substrate having excellent crystallinity, it is possible to produce a high-output semiconductor light-emitting device having excellent light extraction efficiency.

在根據國際公開第2011/074534號記述之方法製造半導體發光元件時,必須於自模板基板之製造步驟進行至下一步驟時進行成膜裝置之變更或模板基板等之成膜裝置間之搬送等。此時,模板基板等係暴露於大氣、氧、氮、氫或氬等之氣體中。又,模板基板等係經過降溫至適於搬送之溫度等之某些熱製程。因此,於製造方法變更之邊界面,容易引起自然氧化膜等之形成、n型摻雜物之過剩摻雜、或晶格缺陷之集中等。藉此,形成於該邊界面上之氮化物半導體層之膜質劣化。又,於製造之半導體發光元件中,會引起洩漏電流之增加或靜電耐壓之降低等。基於該等缺陷,使用所謂之藉由於H2與NH3之混合氣體環境且1000℃以上之高溫下於模板基板上形成n型氮化物半導體層,而還原上述自然氧化膜之方法。 When manufacturing a semiconductor light-emitting device according to the method described in International Publication No. 2011/074534, it is necessary to change the film forming apparatus or transfer between the film forming apparatuses such as the template substrate from the manufacturing step of the template substrate to the next step. . At this time, the template substrate or the like is exposed to a gas such as air, oxygen, nitrogen, hydrogen or argon. Further, the template substrate or the like is subjected to some thermal processes such as temperature reduction to a temperature suitable for transport. Therefore, formation of a natural oxide film or the like, excessive doping of an n-type dopant, or concentration of lattice defects is likely to occur at the boundary surface where the manufacturing method is changed. Thereby, the film quality of the nitride semiconductor layer formed on the boundary surface is deteriorated. Further, in the manufactured semiconductor light-emitting device, an increase in leakage current or a decrease in electrostatic withstand voltage is caused. Based on these defects, a method of reducing the above-described natural oxide film by forming an n-type nitride semiconductor layer on a template substrate at a high temperature of 1000 ° C or higher by using a mixed gas atmosphere of H 2 and NH 3 is used.

然而,若於1000℃以上之高溫下形成n型氮化物半導體層,則n型氮化物半導體層形成後之降溫步驟需要較長時間。因此,引起每單位時間之處理能力(處理量:Throughput)減少。又,因高溫處理而於成膜裝置之腔室內附著有強固且大量的附著物,故必須頻繁維護成膜 裝置。 However, if the n-type nitride semiconductor layer is formed at a high temperature of 1000 ° C or higher, the temperature lowering step after the formation of the n-type nitride semiconductor layer takes a long time. Therefore, the processing capacity per unit time (processing amount: Throughput) is reduced. Moreover, due to the high temperature treatment, a strong and large amount of deposits adhere to the chamber of the film forming apparatus, so the film formation must be frequently maintained. Device.

本發明係鑒於該點而完成者,其目的在於提高氮化物半導體發光元件之生產性。 The present invention has been made in view of the above, and an object thereof is to improve the productivity of a nitride semiconductor light-emitting device.

本發明人等發現即使自模板基板之形成等之於高溫之成膜步驟結束後,以低於模板基板之形成溫度之溫度使n型氮化物半導體層成長,氮化物半導體發光元件之特性亦未劣化。即,發現藉由在形成模板基板後,於溫度下降至較n型氮化物半導體層之成長溫度更低之溫度(較佳為100℃以下)後,再提高溫度形成n型氮化物半導體層,可防止所得之氮化物半導體發光元件之特性劣化,且提高氮化物半導體發光元件之生產性。進而,發現在溫度下降至較n型氮化物半導體層之成長溫度更低之溫度後,暫時自成長裝置之腔室內取出模板基板,且將該模板基板放入不同腔室內後,以較形成該模板基板之溫度更低之溫度形成n型氮化物半導體層較為有效。 The inventors of the present invention have found that the characteristics of the nitride semiconductor light-emitting device are not increased even when the n-type nitride semiconductor layer is grown at a temperature lower than the temperature at which the template substrate is formed, after the formation of the template substrate at a high temperature. Deterioration. That is, it is found that after the formation of the template substrate, after the temperature is lowered to a temperature lower than the growth temperature of the n-type nitride semiconductor layer (preferably 100 ° C or lower), the temperature is increased to form an n-type nitride semiconductor layer. The deterioration of the characteristics of the obtained nitride semiconductor light-emitting element can be prevented, and the productivity of the nitride semiconductor light-emitting element can be improved. Further, after the temperature is lowered to a temperature lower than the growth temperature of the n-type nitride semiconductor layer, the template substrate is temporarily taken out from the chamber of the growth device, and the template substrate is placed in a different chamber to form the same. It is effective to form an n-type nitride semiconductor layer at a temperature lower than the temperature of the template substrate.

本發明之氮化物半導體發光元件包含:包含1層以上之第1n型氮化物半導體層之第1積層體、包含與第1積層體之第1面相接之第2n型氮化物半導體層之第2積層體、設於第2積層體上之發光層、及設於發光層上之p型氮化物半導體層。第2n型氮化物半導體層係以較形成第1n型氮化物半導體層之溫度更低之溫度形成。 The nitride semiconductor light-emitting device of the present invention includes: a first laminate including one or more first n-type nitride semiconductor layers; and a second n-type nitride semiconductor layer including a first surface of the first laminate. A laminate, a light-emitting layer provided on the second laminate, and a p-type nitride semiconductor layer provided on the light-emitting layer. The second n-type nitride semiconductor layer is formed at a lower temperature than the temperature at which the first n-type nitride semiconductor layer is formed.

於本發明之氮化物半導體發光元件中,第2n型氮化物半導體層之形成溫度係低於第1n型氮化物半導體層之形成溫度。因此,由於可縮短第2n型氮化物半導體層之形成後之降溫步驟所需要之時間,故可維持較高處理量。又,與第2n型氮化物半導體層之形成溫度為高溫之情形相比,附著於形成第2n型氮化物半導體層之裝置之腔室的附著物量減少。藉此,維護形成第2積層體(第2積層體包含第2n型氮化物半導體層)之裝置之頻率降低。基於該等原因,氮化物半導體發光元件之生產性變高。 In the nitride semiconductor light-emitting device of the present invention, the formation temperature of the second n-type nitride semiconductor layer is lower than the formation temperature of the first n-type nitride semiconductor layer. Therefore, since the time required for the temperature lowering step after the formation of the second n-type nitride semiconductor layer can be shortened, a high processing amount can be maintained. Moreover, the amount of deposits adhering to the chamber of the apparatus for forming the second n-type nitride semiconductor layer is reduced as compared with the case where the formation temperature of the second n-type nitride semiconductor layer is high. Thereby, the frequency of the apparatus for forming the second layered body (the second layered body including the second n-type nitride semiconductor layer) is maintained. For these reasons, the productivity of the nitride semiconductor light-emitting element becomes high.

第2積層體較佳係於第2n型氮化物半導體層與發光層之間,進而包含1層以上之第3n型氮化物半導體層。第3n型氮化物半導體層較佳以第2n型氮化物半導體層之形成溫度以下之溫度形成。 The second layered body is preferably between the second n-type nitride semiconductor layer and the light-emitting layer, and further includes one or more third n-type nitride semiconductor layers. The third n-type nitride semiconductor layer is preferably formed at a temperature lower than the formation temperature of the second n-type nitride semiconductor layer.

構成第1積層體之第1面的半導體層較佳為非摻雜層。該情形時,第2n型氮化物半導體層較佳為摻雜層。 The semiconductor layer constituting the first surface of the first layered body is preferably an undoped layer. In this case, the second n-type nitride semiconductor layer is preferably a doped layer.

構成第1積層體之第1面之半導體層較佳為摻雜層。該情形時,第2n型氮化物半導體層較佳為非摻雜層。 The semiconductor layer constituting the first surface of the first layered body is preferably a doped layer. In this case, the second n-type nitride semiconductor layer is preferably an undoped layer.

本發明之氮化物半導體發光元件之製造方法係至少包含:形成包含1層以上之第1n型氮化物半導體層之第1積層體之步驟;形成包含與第1積層體之第1面相接之第2n型氮化物半導體層之第2積層體之步驟;於第2積層體上形成發光層之步驟;及於發光層上形成p型氮化物半導體層之步驟。以較形成第1n型氮化物半導體層之溫度更低之溫度形成第2n型氮化物半導體層。在形成第1積層體之步驟後且形成第2積層體之步驟前,進而包含降溫至較形成第2積層體之溫度更低之溫度之降溫步驟。 The method for producing a nitride semiconductor light-emitting device according to the present invention includes at least a step of forming a first layered body including a first n-type nitride semiconductor layer of one or more layers, and forming a layer including the first surface of the first layered body. a step of forming a second layered body of the second n-type nitride semiconductor layer; a step of forming a light-emitting layer on the second layered body; and a step of forming a p-type nitride semiconductor layer on the light-emitting layer. The second n-type nitride semiconductor layer is formed at a lower temperature than the temperature at which the first n-type nitride semiconductor layer is formed. After the step of forming the first layered body and before the step of forming the second layered body, a step of lowering the temperature to a temperature lower than the temperature at which the second layered body is formed is further included.

於本發明之氮化物半導體元件之製造方法中,與第1積層體之第1面相接之第2n型氮化物半導體層之形成溫度係低於第1n型氮化物半導體層之形成溫度。又,在形成第1積層體之步驟後且形成第2積層體之步驟前,降溫至較第2積層體之形成溫度更低之溫度。基於此等,由於可縮短第2n型氮化物半導體層之形成後之降溫步驟所需之時間,故可維持較高的處理量。又,與第2n型氮化物半導體層之形成溫度為高溫之情形相比,附著於形成第2n型氮化物半導體層之裝置之腔室內之附著物量減少。藉此,維護形成第2積層體(第2積層體包含第2n型氮化物半導體層)之裝置之頻率降低。如上所述,氮化物半導體發光元件之生產性變高。 In the method for producing a nitride semiconductor device of the present invention, the formation temperature of the second n-type nitride semiconductor layer which is in contact with the first surface of the first layered body is lower than the formation temperature of the first n-type nitride semiconductor layer. Further, before the step of forming the first layered body and before the step of forming the second layered body, the temperature is lowered to a temperature lower than the temperature at which the second layered body is formed. Based on this, since the time required for the temperature lowering step after the formation of the second n-type nitride semiconductor layer can be shortened, a high processing amount can be maintained. Moreover, the amount of deposits adhering to the chamber in which the second n-type nitride semiconductor layer is formed is reduced as compared with the case where the formation temperature of the second n-type nitride semiconductor layer is high. Thereby, the frequency of the apparatus for forming the second layered body (the second layered body including the second n-type nitride semiconductor layer) is maintained. As described above, the productivity of the nitride semiconductor light-emitting element becomes high.

在形成第1積層體之步驟後且形成第2積層體之步驟前,較佳進 而包含使第1積層體暴露於大氣中的步驟。 After the step of forming the first layered body and before the step of forming the second layered body, it is preferred to It includes a step of exposing the first laminate to the atmosphere.

本發明之上述及其他目的、特徵、狀態及優點係可根據關聯附加之圖式進行理解之本發明相關之下述詳細說明得以明確。 The above and other objects, features, aspects and advantages of the present invention will become apparent from

1‧‧‧氮化物半導體發光元件 1‧‧‧Nitride semiconductor light-emitting elements

3‧‧‧基板 3‧‧‧Substrate

3a‧‧‧凸部 3a‧‧‧ convex

3b‧‧‧凹部 3b‧‧‧ recess

3t‧‧‧假想三角形 3t‧‧‧imaginary triangle

5‧‧‧緩衝層 5‧‧‧buffer layer

6‧‧‧第1積層體 6‧‧‧1st laminate

7‧‧‧基底層 7‧‧‧ basal layer

8‧‧‧n型接觸層 8‧‧‧n type contact layer

8A‧‧‧n型接觸層 8A‧‧‧n type contact layer

8B‧‧‧n型接觸層 8B‧‧‧n type contact layer

9‧‧‧n型調變摻雜層 9‧‧‧n type modulation doping layer

9A‧‧‧n+9A‧‧‧n + layer

9B‧‧‧n-9B‧‧‧n - layer

10‧‧‧V凹坑產生層 10‧‧‧V pit generation layer

11‧‧‧第2積層體 11‧‧‧2nd layered body

14‧‧‧發光層 14‧‧‧Lighting layer

14A‧‧‧障壁層 14A‧‧‧Baffle

14A0~14A7‧‧‧障壁層 14A0~14A7‧‧‧Baffle layer

14AZ‧‧‧障壁層 14AZ‧‧ ‧ barrier layer

14W~14W2‧‧‧井層 14W~14W2‧‧‧ Well

15‧‧‧V凹坑 15‧‧‧V pit

16‧‧‧p型氮化物半導體層 16‧‧‧p-type nitride semiconductor layer

17‧‧‧p型氮化物半導體層 17‧‧‧p-type nitride semiconductor layer

18‧‧‧p型氮化物半導體層 18‧‧‧p-type nitride semiconductor layer

21‧‧‧n側電極 21‧‧‧n side electrode

23‧‧‧透明電極 23‧‧‧Transparent electrode

25‧‧‧p側電極 25‧‧‧p side electrode

27‧‧‧透明保護膜 27‧‧‧Transparent protective film

30‧‧‧台面部 30‧‧‧Face

61‧‧‧第1面 61‧‧‧1st

71‧‧‧第1基底層 71‧‧‧1st basal layer

71a‧‧‧傾斜晶面 71a‧‧‧Sloping facets

71b‧‧‧上表面 71b‧‧‧ upper surface

75‧‧‧第2基底層 75‧‧‧2nd basal layer

75b‧‧‧上表面 75b‧‧‧ upper surface

121‧‧‧多層構造體 121‧‧‧Multilayer structure

121A‧‧‧氮化物半導體層 121A‧‧‧ nitride semiconductor layer

121B‧‧‧氮化物半導體層 121B‧‧‧ nitride semiconductor layer

122‧‧‧超晶格層 122‧‧‧Superlattice layer

122A‧‧‧寬帶隙層 122A‧‧‧ wide band gap layer

122B‧‧‧窄帶隙層 122B‧‧‧Narrow band gap layer

123‧‧‧非摻雜氮化物半導體層 123‧‧‧Undoped nitride semiconductor layer

124‧‧‧n型氮化物半導體層 124‧‧‧n type nitride semiconductor layer

Eg‧‧‧帶隙能量 Eg‧‧‧ band gap energy

圖1係本發明之一實施形態之氮化物半導體發光元件之概略剖面圖。 Fig. 1 is a schematic cross-sectional view showing a nitride semiconductor light-emitting device according to an embodiment of the present invention.

圖2係圖1所示之氮化物半導體發光元件之概略俯視圖。 Fig. 2 is a schematic plan view showing a nitride semiconductor light-emitting device shown in Fig. 1;

圖3係示意性顯示圖1所示之氮化物半導體發光元件之n型接觸層至p型氮化物半導體層之帶隙能量Eg之大小之能量圖。 Fig. 3 is an energy diagram schematically showing the magnitude of the band gap energy Eg of the n-type contact layer to the p-type nitride semiconductor layer of the nitride semiconductor light-emitting device shown in Fig. 1.

圖4係圖1所示之氮化物半導體發光元件之基板之放大俯視圖。 4 is an enlarged plan view showing a substrate of the nitride semiconductor light-emitting device shown in FIG. 1.

圖5(a)係顯示圖1所示之氮化物半導體發光元件之製造步驟之溫度分佈之圖表,圖5(b)係顯示比較例1之氮化物半導體發光元件之製造步驟之溫度分佈之圖表。 5(a) is a graph showing a temperature distribution of a manufacturing step of the nitride semiconductor light-emitting device shown in FIG. 1, and FIG. 5(b) is a graph showing a temperature distribution of a manufacturing step of the nitride semiconductor light-emitting device of Comparative Example 1. .

圖6係實施例6之氮化物半導體發光元件之概略剖面圖。 Fig. 6 is a schematic cross-sectional view showing a nitride semiconductor light-emitting device of a sixth embodiment.

圖7係示意性顯示實施例6所示之氮化物半導體發光元件之n型接觸層至p型氮化物半導體層之帶隙能量Eg之大小之能量圖。 Fig. 7 is an energy diagram schematically showing the magnitude of the band gap energy Eg of the n-type contact layer to the p-type nitride semiconductor layer of the nitride semiconductor light-emitting device shown in Example 6.

以下,使用圖式說明本發明之氮化物半導體發光元件。另,於本發明之圖式中,同一參照符號係表示同一部分或相當部分者。又,長度、寬度、厚度、深度等之尺寸關係係為了使圖式明確化與簡略化而進行適當變更,並非表示實際尺寸關係者。 Hereinafter, the nitride semiconductor light-emitting device of the present invention will be described using a schematic diagram. In the drawings, the same reference numerals are used to refer to the same or equivalent parts. Further, the dimensional relationship of the length, the width, the thickness, the depth, and the like is appropriately changed in order to clarify and simplify the drawing, and does not indicate the actual size relationship.

以下,為了表示位置關係,而將記述於圖1下側之部分表示為「下」,且將記述於圖1上側之部分表示為「上」。這是為圖簡便而進行之表示,不同於相對重力方向而定之「上」及「下」。 Hereinafter, in order to show the positional relationship, the portion described on the lower side in FIG. 1 is referred to as "lower", and the portion described on the upper side in FIG. 1 is referred to as "upper". This is an indication of the simplicity of the diagram, which is different from the "up" and "down" depending on the direction of gravity.

「障壁層」係表示被井層所夾之層。未被井層夾著的障壁層係表示為「最初之障壁層」或「最後之障壁層」,與被井層夾著的障壁 層相比改變了表述。 The "barrier layer" is the layer that is sandwiched by the well layer. The barrier layer that is not sandwiched by the well layer is expressed as the "initial barrier layer" or the "last barrier layer", and the barrier that is sandwiched by the well layer The layer changes the expression.

使用「摻雜物濃度」、及伴隨n型摻雜物或p型摻雜物之摻雜而產生之電子或電洞之濃度即「載子濃度」。該等之關係予以後述。 The "dopant concentration" and the concentration of electrons or holes generated by doping with an n-type dopant or a p-type dopant are "carrier concentration". These relationships will be described later.

所謂「載子氣體」係III族原料氣體、V族原料氣體及摻雜物原料氣體以外之氣體。構成載子氣體之原子未被取入膜中等。 The "carrier gas" is a gas other than the group III source gas, the group V source gas, and the dopant source gas. The atoms constituting the carrier gas are not taken into the film or the like.

「n型氮化物半導體層」亦可包含實用上不妨礙電子流動之程度之厚度的低載子濃度之n型層或非摻雜層。「p型氮化物半導體層」亦可包含實用上不妨礙電洞流動之程度之厚度的低載子濃度之p型層或非摻雜層。所謂「實用上不妨礙」意指氮化物半導體發光元件之動作電壓為實用位準。 The "n-type nitride semiconductor layer" may also include an n-type layer or an undoped layer having a low carrier concentration which is practically not to impede the extent of electron flow. The "p-type nitride semiconductor layer" may also include a p-type layer or an undoped layer having a low carrier concentration which is practically not inhibiting the thickness of the hole. The term "practical does not hinder" means that the operating voltage of the nitride semiconductor light-emitting element is a practical level.

<氮化物半導體發光元件之構造> <Configuration of Nitride Semiconductor Light Emitting Element>

圖1及圖2分別為本發明之一實施形態之氮化物半導體發光元件1之概略剖面圖及概略俯視圖。圖1係相當於圖2所示之I-I線之剖面圖。圖3係示意性顯示圖1所示之氮化物半導體發光元件1之n型接觸層8至p型氮化物半導體層16之帶隙能量Eg之大小之能量圖。圖3之縱軸方向係表示圖1所示之氮化物半導體發光元件1之上下方向,圖3之橫軸之Eg係示意性表示各層中的帶隙能量之大小。於圖3中,於摻雜了n型摻雜物之層之右側標註小點且記述為「n」。圖4係圖1所示之氮化物半導體發光元件1之基板3之放大俯視圖。 1 and 2 are a schematic cross-sectional view and a schematic plan view of a nitride semiconductor light-emitting device 1 according to an embodiment of the present invention. Fig. 1 is a cross-sectional view corresponding to the I-I line shown in Fig. 2. 3 is an energy diagram schematically showing the magnitude of the band gap energy Eg of the n-type contact layer 8 to the p-type nitride semiconductor layer 16 of the nitride semiconductor light-emitting element 1 shown in FIG. 1. The vertical axis direction of Fig. 3 indicates the upper and lower directions of the nitride semiconductor light-emitting element 1 shown in Fig. 1, and the Eg of the horizontal axis of Fig. 3 schematically indicates the magnitude of the band gap energy in each layer. In FIG. 3, a small dot is indicated on the right side of the layer doped with the n-type dopant and described as "n". 4 is an enlarged plan view showing a substrate 3 of the nitride semiconductor light-emitting device 1 shown in FIG. 1.

圖1所示之氮化物半導體發光元件1包含:第1積層體6、第2積層體11、發光層14、及p型氮化物半導體層16、17、18。於本實施形態中,將基板3、緩衝層5、基底層7、n型接觸層8、及n型調變摻雜層9積層而成之部分稱為第1積層體6,且將V凹坑產生層10、多層構造體121、超晶格層122積層而成之部分稱為第2積層體11,以使彼此加以區別。 The nitride semiconductor light-emitting device 1 shown in FIG. 1 includes a first layered body 6, a second layered body 11, a light-emitting layer 14, and p-type nitride semiconductor layers 16, 17, and 18. In the present embodiment, a portion in which the substrate 3, the buffer layer 5, the underlayer 7, the n-type contact layer 8, and the n-type modulation doping layer 9 are laminated is referred to as a first layered body 6, and V-concave The portion in which the pit generating layer 10, the multilayer structure 121, and the superlattice layer 122 are laminated is referred to as a second laminated body 11 so as to be distinguished from each other.

於本實施形態中,n型接觸層8及n型調變摻雜層9之至少一者相 當於申請專利範圍中的「第1n型氮化物半導體層」,V凹坑產生層10相當於申請專利範圍中的「第2n型氮化物半導體層」,構成多層構造體121及超晶格層122之至少一者之層中至少一層相當於申請專利範圍中的「第3n型氮化物半導體層」。 In this embodiment, at least one of the n-type contact layer 8 and the n-type modulation doping layer 9 In the "1n-type nitride semiconductor layer" in the patent application, the V-pit generation layer 10 corresponds to the "2n-type nitride semiconductor layer" in the patent application, and constitutes the multilayer structure 121 and the superlattice layer. At least one of the layers of at least one of 122 corresponds to the "3n-type nitride semiconductor layer" in the patent application.

本發明之特徵在於,將n型氮化物半導體層之形成分離成兩個階段,且於後續形成步驟中,不進行成為處理量減少之主要原因之高溫處理即可形成n型氮化物半導體層之方面。又,重要的是作為第2積層體11而最初形成之層係於低溫下形成之n型氮化物半導體層。因此,於本發明中,並未限定於作為第2積層體11而最初形成之層係作為V凹坑產生層10發揮功能之層,亦未限定於在V凹坑產生層10之後形成作為多層構造體121及超晶格層122分別發揮功能之層。然而,於本發明中,只要作為第2積層體11而最初形成之層係作為V凹坑產生層10發揮功能之層,且,於V凹坑產生層10之後形成作為多層構造體121及超晶格層122分別發揮功能之層,即可期待組合之相乘效果。 The present invention is characterized in that the formation of the n-type nitride semiconductor layer is separated into two stages, and in the subsequent formation step, the n-type nitride semiconductor layer can be formed without performing high-temperature processing which is the main cause of the reduction in the amount of processing. aspect. Further, it is important that the layer initially formed as the second layered body 11 is an n-type nitride semiconductor layer formed at a low temperature. Therefore, in the present invention, the layer which is first formed as the second layered body 11 is not limited to the layer which functions as the V-pit generation layer 10, and is not limited to the layer formed after the V-pit generation layer 10 as a plurality of layers. Each of the structure 121 and the superlattice layer 122 functions as a layer. However, in the present invention, the layer which is initially formed as the second layered body 11 functions as a layer of the V-pit generation layer 10, and is formed as a multilayer structure 121 and super after the V-pit generation layer 10. The lattice layer 122 functions as a layer, and the synergistic effect of the combination can be expected.

第1積層體6之一部分、第2積層體11、發光層14、及p型氮化物半導體層16、17、18係被蝕刻而構成台面部30。於p型氮化物半導體層18上,介隔透明電極23設有p側電極25。於台面部30之外側(圖1右側),n型接觸層8之上表面之一部分自n型調變摻雜層9等露出,於n型接觸層8之露出面上設有n側電極21。透明保護膜27覆蓋透明電極23與藉由蝕刻而露出之各層之側面,且露出n側電極21與p側電極25。 One portion of the first layered body 6, the second layered body 11, the light-emitting layer 14, and the p-type nitride semiconductor layers 16, 17, 18 are etched to constitute the mesa portion 30. On the p-type nitride semiconductor layer 18, a p-side electrode 25 is provided through the transparent electrode 23. On the outer side of the mesa portion 30 (on the right side of FIG. 1), a portion of the upper surface of the n-type contact layer 8 is exposed from the n-type modulation doped layer 9 or the like, and an n-side electrode 21 is provided on the exposed surface of the n-type contact layer 8. . The transparent protective film 27 covers the transparent electrode 23 and the side faces of the respective layers exposed by etching, and exposes the n-side electrode 21 and the p-side electrode 25.

若以超高倍率STEM(Scanning Transmission Electron Microscopy:掃描透射電子顯微鏡)觀察氮化物半導體發光元件1之剖面,則確認產生了V凹坑15。於本實施形態之氮化物半導體發光元件1中,藉由設置V凹坑產生層10,而控制V凹坑15之產生。 When the cross section of the nitride semiconductor light-emitting device 1 was observed by a super high-magnification STEM (Scanning Transmission Electron Microscopy), it was confirmed that the V-pit 15 was generated. In the nitride semiconductor light-emitting device 1 of the present embodiment, the V-pit generation layer 10 is provided to control the generation of the V-pits 15.

<第1積層體> <1st laminated body>

第1積層體6於本實施形態中係包含基板3、緩衝層5、基底層7、 n型接觸層8、及n型調變摻雜層9,但若包含n型接觸層8及n型調變摻雜層9中至少一者即可。本實施形態之氮化物半導體發光元件1亦可不包含基板3,於該情形時,第1積層體6係包含基底層7、n型接觸層8、及n型調變摻雜層9。 In the present embodiment, the first layered body 6 includes the substrate 3, the buffer layer 5, and the base layer 7, The n-type contact layer 8 and the n-type modulation doping layer 9 may include at least one of the n-type contact layer 8 and the n-type modulation doping layer 9. The nitride semiconductor light-emitting device 1 of the present embodiment may not include the substrate 3. In this case, the first layered body 6 includes the under layer 7, the n-type contact layer 8, and the n-type modulation doping layer 9.

第1積層體6具有第1面61。第1面61意指第1積層體6之表面且連接V凹坑產生層10(第2n型氮化物半導體層)之面。本實施形態之第1積層體6係於基板3上依序積層緩衝層5、基底層7、n型接觸層8、n型調變摻雜層9而構成,因而第1面61相當於n型調變摻雜層9之上表面(位於與n型接觸層8和n型調變摻雜層9之界面為相反側之n型調變摻雜層9之面)。 The first layered body 6 has a first surface 61. The first surface 61 means the surface of the first layered body 6 and is connected to the surface of the V-pit generation layer 10 (the second n-type nitride semiconductor layer). The first layered body 6 of the present embodiment is formed by sequentially laminating the buffer layer 5, the underlying layer 7, the n-type contact layer 8, and the n-type modulation doping layer 9 on the substrate 3. Therefore, the first surface 61 corresponds to n. The upper surface of the type modulation doping layer 9 (the surface of the n-type modulation doping layer 9 on the opposite side to the interface between the n-type contact layer 8 and the n-type modulation doping layer 9).

構成第1面61之半導體層較佳為非摻雜層(例如下述之n-層9B)。該情形時,V凹坑產生層10較佳為摻雜層。於本說明書中,「構成第1面61之半導體層」相當於構成n型調變摻雜層9之2層以上之層中距離n型接觸層8最遠之層。「非摻雜層」不僅意指完全未摻雜導電性摻雜物之層,亦指結晶成長中無意摻雜導電型摻雜物之層。即,非摻雜層係例如亦可包含0cm-3以上3×1018cm-3以下之導電性摻雜物。「摻雜層」意指結晶成長中刻意摻雜導電性摻雜物之層。摻雜層較佳例如包含1×1019cm-3以上之導電性摻雜物。 The semiconductor layer constituting the first surface 61 is preferably an undoped layer (for example, n - layer 9B described below). In this case, the V-pit generation layer 10 is preferably a doped layer. In the present specification, the "semiconductor layer constituting the first surface 61" corresponds to the layer which is the farthest from the n-type contact layer 8 among the two or more layers constituting the n-type modulation doping layer 9. An "undoped layer" means not only a layer that is completely undoped with a conductive dopant, but also a layer that is unintentionally doped with a conductive dopant during crystal growth. That is, the undoped layer may include, for example, a conductive dopant of 0 cm -3 or more and 3 × 10 18 cm -3 or less. By "doped layer" is meant a layer that is intentionally doped with a conductive dopant during crystal growth. The doped layer preferably contains, for example, a conductive dopant of 1 × 10 19 cm -3 or more.

構成第1面61之半導體層亦可為摻雜層(例如下述之n+層9A)。該情形時,V凹坑產生層10亦可為非摻雜層。 The semiconductor layer constituting the first surface 61 may be a doped layer (for example, the n + layer 9A described below). In this case, the V-pit generation layer 10 may also be an undoped layer.

<基板> <Substrate>

基板3亦可為例如藍寶石基板等之絕緣性基板,又可為包含GaN、SiC或ZnO等之導電性基板。基板3之厚度較佳於氮化物半導體層成長時為900μm以上1200μm以下,且較佳於所製造之氮化物半導體發光元件1中為50μm以上300μm以下。即,氮化物半導體發光元件1之製造方法亦可包含研磨基板3之步驟。又,氮化物半導體發光元件 1之製造方法亦可包含去除基板3之步驟。 The substrate 3 may be an insulating substrate such as a sapphire substrate or a conductive substrate including GaN, SiC or ZnO. The thickness of the substrate 3 is preferably 900 μm or more and 1200 μm or less when the nitride semiconductor layer is grown, and is preferably 50 μm or more and 300 μm or less in the nitride semiconductor light-emitting device 1 to be produced. That is, the method of manufacturing the nitride semiconductor light-emitting device 1 may include the step of polishing the substrate 3. Further, a nitride semiconductor light-emitting element The manufacturing method of 1 may also include the step of removing the substrate 3.

設有緩衝層5等之基板3之面(基板3之上表面)較佳如圖1所示具有凸部3a與凹部3b交替形成之凹凸形狀。凸部3a較佳如圖4所示於基板3之上表面中具有略圓形形狀,且較佳如圖4所示配置於假想三角形3t之頂點。相鄰之凸部3a之頂點之間隔(圖4所示之假想三角形3t之1邊)較佳為1μm以上5μm以下。凸部3a亦可於側視時具有梯形形狀,凸部3a之頂點較佳如圖1所示帶圓。 The surface of the substrate 3 on which the buffer layer 5 or the like is provided (the upper surface of the substrate 3) preferably has an uneven shape in which the convex portion 3a and the concave portion 3b are alternately formed as shown in FIG. The convex portion 3a preferably has a slightly circular shape in the upper surface of the substrate 3 as shown in FIG. 4, and is preferably disposed at the apex of the imaginary triangle 3t as shown in FIG. The interval between the apexes of the adjacent convex portions 3a (one side of the imaginary triangle 3t shown in Fig. 4) is preferably 1 μm or more and 5 μm or less. The convex portion 3a may also have a trapezoidal shape when viewed from the side, and the apex of the convex portion 3a is preferably rounded as shown in FIG.

<緩衝層> <buffer layer>

緩衝層5係設於基板3之凸部3a上與其凹部3b上。緩衝層5較佳例如為AlsoGatoOuoN1-uo(0≦s0≦1、0≦t0≦1、0≦u0≦1、s0+t0≠0)層,更佳為AlN層或AlON層。緩衝層5為AlON層時,AlON層中之N之極小一部分(0.5~2%)被置換成氧。藉此,因以沿基板3之成長表面之法線方向伸長之方式形成緩衝層5,故獲得包含結晶粒之整齊柱狀結晶之集合體之緩衝層5。緩衝層5之厚度並未特別限定,較佳為3nm以上100nm以下,更佳為5nm以上50nm以下。若緩衝層5係藉由濺鍍法形成之AlON層,則X線光譜所顯現之峰值之半值寬度(基底層7之結晶品質之指標)變窄。藉此,緩衝層5較佳為藉由濺鍍法形成之AlON層。 The buffer layer 5 is provided on the convex portion 3a of the substrate 3 and on the concave portion 3b thereof. The buffer layer 5 is preferably, for example, a layer of Al so Ga to O uo N 1-uo (0≦s0≦1, 0≦t0≦1, 0≦u0≦1, s0+t0≠0), more preferably an AlN layer or AlON layer. When the buffer layer 5 is an AlON layer, a very small portion (0.5 to 2%) of N in the AlON layer is replaced with oxygen. Thereby, since the buffer layer 5 is formed so as to be elongated in the normal direction of the growth surface of the substrate 3, the buffer layer 5 including the aggregate of the uniform columnar crystals of the crystal grains is obtained. The thickness of the buffer layer 5 is not particularly limited, but is preferably 3 nm or more and 100 nm or less, and more preferably 5 nm or more and 50 nm or less. When the buffer layer 5 is an AlON layer formed by a sputtering method, the half value width of the peak appearing in the X-ray spectrum (the index of the crystal quality of the underlayer 7) is narrowed. Thereby, the buffer layer 5 is preferably an AlON layer formed by sputtering.

<基底層> <base layer>

基底層7較佳具有第1基底層71與第2基底層75。藉此,X線光譜所顯現之峰值之半值寬度(基底層7之結晶品質之指標)變窄,即,基底層7之結晶品質變高。第1基底層71係隔著緩衝層5設於基板3之凹部3b上,較佳具有包含傾斜晶面71a之側面視略三角形之形狀,亦可具有上表面71b。「傾斜晶面」係於相對於基板3之凹部3b以10度以上之角度傾斜之方向延伸之面,較佳為氮化物半導體結晶面。第2基底層75係覆蓋第1基底層71且隔著緩衝層5覆蓋基板3之凸部3a,並與緩衝層5及第1基底層71相接。與n型接觸層8相接之基底層7之面(基底層7 之上表面75b)為平坦。於本說明書中,除特別限定之情形外,將第1基底層71與第2基底層75概括表示為基底層7。 The base layer 7 preferably has a first base layer 71 and a second base layer 75. Thereby, the half value width of the peak appearing in the X-ray spectrum (the index of the crystal quality of the underlayer 7) is narrowed, that is, the crystal quality of the underlayer 7 becomes high. The first base layer 71 is provided on the concave portion 3b of the substrate 3 via the buffer layer 5, and preferably has a shape in which the side surface including the inclined crystal surface 71a is slightly triangular, and may have an upper surface 71b. The "inclined crystal face" is a surface extending in a direction inclined by an angle of 10 degrees or more with respect to the concave portion 3b of the substrate 3, and is preferably a nitride semiconductor crystal face. The second base layer 75 covers the first base layer 71 and covers the convex portion 3 a of the substrate 3 via the buffer layer 5 , and is in contact with the buffer layer 5 and the first base layer 71 . The surface of the base layer 7 that is in contact with the n-type contact layer 8 (base layer 7) The upper surface 75b) is flat. In the present specification, the first base layer 71 and the second base layer 75 are collectively shown as the base layer 7 unless otherwise specified.

第1基底層71較佳例如包含Alx2Gay2Inz2N(0≦x2≦1、0≦y2≦1、0≦z2≦1、x2+y2+z2≠0)。第2基底層75較佳例如包含Alx3Gay3Inz3N(0≦x3≦1、0≦y3≦1、0≦z3≦1、x3+y3+z3≠0)。 The first base layer 71 preferably contains, for example, Al x2 Ga y2 In z2 N (0≦x2≦1, 0≦y2≦1, 0≦z2≦1, x2+y2+z2≠0). The second underlayer 75 preferably includes, for example, Al x3 Ga y3 In z3 N (0≦x3≦1, 0≦y3≦1, 0≦z3≦1, x3+y3+z3≠0).

第1基底層71及第2基底層75較佳分別為包含Ga作為III族元素之氮化物半導體層。藉此,可不延續包含柱狀結晶之集合體之緩衝層5中之錯位等之結晶缺陷而形成第1基底層71及第2基底層75。為了不延續緩衝層5中之結晶缺陷而設置第1基底層71及第2基底層75,必須於與緩衝層5之界面(緩衝層5之上表面)附近形成錯位環。若第1基底層71及第2基底層75為包含Ga之III族氮化物半導體層,則於與緩衝層5之界面附近容易產生錯位環。即,若第1基底層71及第2基底層75為包含Ga作為III族元素之氮化物半導體層,則緩衝層5中之結晶缺陷於與緩衝層5之界面附近環化並密閉。藉此,可防止緩衝層5中的結晶缺陷延續至第1基底層71及第2基底層75。例如,第1基底層71包含Alx2Gay2N(0≦x2<1、0<y2<1),第2基底層75包含Alx3Gay3N(0≦x3<1、0<y3<1)之情形時,尤其第1基底層71及第2基底層75分別包含GaN之情形時,緩衝層5中的結晶缺陷容易於與緩衝層5之界面附近環化並密閉。藉此,獲得具有錯位密度較小之良好結晶品質之第1基底層71及第2基底層75。 Each of the first underlayer 71 and the second underlayer 75 is preferably a nitride semiconductor layer containing Ga as a group III element. Thereby, the first underlayer 71 and the second underlayer 75 can be formed without continuing the crystal defects such as the dislocation in the buffer layer 5 including the aggregate of the columnar crystals. In order to provide the first base layer 71 and the second base layer 75 without continuing the crystal defects in the buffer layer 5, it is necessary to form a misalignment ring in the vicinity of the interface with the buffer layer 5 (the upper surface of the buffer layer 5). When the first underlayer 71 and the second underlayer 75 are Group III nitride semiconductor layers containing Ga, a misaligned loop is likely to occur in the vicinity of the interface with the buffer layer 5. In other words, when the first underlayer 71 and the second underlayer 75 are nitride semiconductor layers containing Ga as a group III element, crystal defects in the buffer layer 5 are cyclized and sealed in the vicinity of the interface with the buffer layer 5. Thereby, it is possible to prevent the crystal defects in the buffer layer 5 from continuing to the first base layer 71 and the second base layer 75. For example, the first underlayer 71 includes Al x2 Ga y2 N (0≦x2<1, 0<y2<1), and the second underlayer 75 includes Al x3 Ga y3 N (0≦x3<1, 0<y3<1) In the case where GaN is included in each of the first underlayer 71 and the second underlayer 75, the crystal defects in the buffer layer 5 are easily cyclized and sealed near the interface with the buffer layer 5. Thereby, the first underlayer 71 and the second underlayer 75 having a good crystal quality with a small dislocation density are obtained.

第1基底層71及第2基底層75亦可包含有例如1×1017cm-3以上1×1019cm-3以下之n型摻雜物。基底層7所含之n型摻雜物較佳例如為Si、Ge及Sn中至少一者,更佳為Si。於n型摻雜物為Si之情形時,n型摻雜物之原料氣體較佳例如為矽烷或乙矽烷。然而,就維持良好結晶品質之觀點,第1基底層71及第2基底層75較佳分別為非摻雜層。 The first underlayer 71 and the second underlayer 75 may include, for example, an n-type dopant of 1 × 10 17 cm -3 or more and 1 × 10 19 cm -3 or less. The n-type dopant contained in the underlayer 7 is preferably at least one of Si, Ge, and Sn, and more preferably Si. In the case where the n-type dopant is Si, the material gas of the n-type dopant is preferably, for example, decane or decane. However, from the viewpoint of maintaining good crystal quality, the first underlayer 71 and the second underlayer 75 are preferably undoped layers, respectively.

基底層7之厚度(與基板3之凹部3b相接之基底層7之面與基底層7 之上表面75b之間之距離)並未特別限定。基底層7之厚度若較大則越大基底層7中之結晶缺陷越少。然而,若基底層7之厚度大至某程度以上,則有基底層7中結晶缺陷減少之效果已飽和之情況。基於該等原因,基底層7之厚度較佳為1μm以上8μm以下,更佳為3μm以上5μm以下。 The thickness of the base layer 7 (the surface of the base layer 7 and the base layer 7 which are in contact with the recess 3b of the substrate 3) The distance between the upper surfaces 75b) is not particularly limited. If the thickness of the base layer 7 is large, the crystal defects in the base layer 7 are smaller. However, if the thickness of the underlayer 7 is as large as a certain level or more, the effect of reducing the crystal defects in the underlayer 7 may be saturated. For these reasons, the thickness of the underlayer 7 is preferably 1 μm or more and 8 μm or less, more preferably 3 μm or more and 5 μm or less.

第1基底層71及第2基底層75之形成方法較佳分別為MOCVD(Metal Organic Chemical Vapor Deposition:有機金屬化學氣相沈積)法。第1基底層71較佳以形成傾斜晶面71a之晶面成長模式成長。藉此,形成結晶缺陷少、結晶品質高之第1基底層71。第2基底層75較佳以可嵌入傾斜晶面71a且形成平坦上表面75b之嵌入成長模式成長。藉此,形成具有平坦上表面75b,且結晶缺陷少、結晶品質高之第2基底層75。 The method of forming the first underlayer 71 and the second underlayer 75 is preferably MOCVD (Metal Organic Chemical Vapor Deposition). The first underlayer 71 preferably grows in a crystal growth mode in which the inclined crystal faces 71a are formed. Thereby, the first underlayer 71 having few crystal defects and high crystal quality is formed. The second base layer 75 is preferably grown in an embedded growth mode in which the inclined crystal face 71a can be embedded and the flat upper surface 75b is formed. Thereby, the second underlayer 75 having the flat upper surface 75b and having few crystal defects and high crystal quality is formed.

第1基底層71及第2基底層75之成長溫度較佳為800℃以上1250℃以下,更佳為900℃以上1150℃以下。藉此,可形成結晶缺陷少且結晶品質優異之第1基底層71及第2基底層75。於本說明書中,「成長溫度」意指使該層結晶成長時之基板3之溫度。 The growth temperature of the first underlayer 71 and the second underlayer 75 is preferably 800° C. or higher and 1250° C. or lower, and more preferably 900° C. or higher and 1150° C. or lower. Thereby, the first underlayer 71 and the second underlayer 75 having few crystal defects and excellent crystal quality can be formed. In the present specification, "growth temperature" means the temperature of the substrate 3 when the layer is crystal grown.

<n型接觸層> <n type contact layer>

n型接觸層8係設於第2基底層75之上表面75b上。n型接觸層8較佳為例如於Als2Gat2Inu2N(0≦s2≦1、0≦t2≦1、0≦u2≦1、s2+t2+u2≒1)層中摻雜了n型摻雜物之層,更佳為於Als2Ga1-s2N(0≦s2≦1,較佳為0≦s2≦0.5,更佳為0≦s2≦0.1)層中摻雜了n型摻雜物之層。n型接觸層8亦可進而包含非摻雜層或低載子濃度層等。 The n-type contact layer 8 is provided on the upper surface 75b of the second base layer 75. The n-type contact layer 8 is preferably doped with, for example, a layer of Al s2 Ga t2 In u2 N (0≦s2≦1, 0≦t2≦1, 0≦u2≦1, s2+t2+u2≒1). The layer of the type dopant is more preferably doped with an n-type layer in the layer of Al s2 Ga 1-s2 N (0≦s2≦1, preferably 0≦s2≦0.5, more preferably 0≦s2≦0.1). A layer of dopants. The n-type contact layer 8 may further comprise an undoped layer or a low carrier concentration layer or the like.

n型接觸層8所含之n型摻雜物並未特別限定,但較佳為Si、P、As或Sb等,更佳為Si。n型接觸層8之n型摻雜物濃度並未特別限定,較佳為1×1019cm-3The n-type dopant contained in the n-type contact layer 8 is not particularly limited, but is preferably Si, P, As or Sb, and more preferably Si. The n-type dopant concentration of the n-type contact layer 8 is not particularly limited, but is preferably 1 × 10 19 cm -3 .

n型接觸層8之厚度越厚,n型接觸層8之電阻變得越低。然而, 若n型接觸層8之厚度太大,則會招致氮化物半導體發光元件1之製造成本上升。基於兼顧兩者,因而n型接觸層8之最大厚度較佳為1μm以上10μm以下。 The thicker the n-type contact layer 8 is, the lower the resistance of the n-type contact layer 8 becomes. however, If the thickness of the n-type contact layer 8 is too large, the manufacturing cost of the nitride semiconductor light-emitting element 1 is increased. The maximum thickness of the n-type contact layer 8 is preferably 1 μm or more and 10 μm or less, based on both.

n型接觸層8之構成並未特別限定。例如,亦可藉由連續形成n型接觸層8A與n型接觸層8B,而將n型接觸層8設為單層。n型接觸層8亦可包含3層以上之n型氮化物半導體層。n型接觸層8包含2層以上之n型氮化物半導體層之情形,2層以上之n型氮化物半導體層可包含相同一組成,亦可包含不同組成。又,2層以上之n型氮化物半導體層可具有相同厚度,亦可具有不同厚度。 The configuration of the n-type contact layer 8 is not particularly limited. For example, the n-type contact layer 8 may be formed as a single layer by continuously forming the n-type contact layer 8A and the n-type contact layer 8B. The n-type contact layer 8 may also include three or more n-type nitride semiconductor layers. When the n-type contact layer 8 includes two or more n-type nitride semiconductor layers, the two or more n-type nitride semiconductor layers may have the same composition or may have different compositions. Further, the two or more n-type nitride semiconductor layers may have the same thickness or may have different thicknesses.

<調變摻雜層> <Modulated doped layer>

n型調變摻雜層9較佳設於n型接觸層8上,例如使n+層9A與n-層9B交替積層而構成。「調變摻雜層」意指摻雜物之量不同之2種以上之層交替積層之層。 The n-type modulation doped layer 9 is preferably provided on the n-type contact layer 8, and is formed by, for example, alternately stacking the n + layer 9A and the n - layer 9B. The "modulation-doped layer" means a layer in which two or more layers of different amounts of dopants are alternately laminated.

n+層9A較佳為n型摻雜物濃度為1.0×1019cm-3以上之Als3Gat3Inu3N(0≦s3≦1、0≦t3≦1、0≦u3≦1、s3+t3+u3≒1)層,更佳為n型摻雜物濃度為1.0×1019cm-3以上之GaN層。n型摻雜物並未特別限定,較佳為Si、P、As或Sb等,更佳為Si。 The n + layer 9A is preferably an Al s3 Ga t3 In u3 N having an n-type dopant concentration of 1.0 × 10 19 cm -3 or more (0≦s3≦1, 0≦t3≦1, 0≦u3≦1, s3) The +t3+u3≒1) layer is more preferably a GaN layer having an n-type dopant concentration of 1.0 × 10 19 cm -3 or more. The n-type dopant is not particularly limited, and is preferably Si, P, As or Sb, etc., more preferably Si.

n-層9B較佳為與n+層9A相比n型摻雜物濃度較低之氮化物半導體層,更佳為n型摻雜物濃度為3×1018cm-3以下之Als4Gat4Inu4N(0≦s4≦1、0≦t4≦1、0≦u4≦1、s4+t4+u4≒1)層,進而更佳為非摻雜層。例如,n-層9B較佳為n型摻雜物濃度為3×1018cm-3以下之GaN層,更佳為非摻雜GaN層。 The n - layer 9B is preferably a nitride semiconductor layer having a lower n-type dopant concentration than the n + layer 9A, more preferably an Al s4 Ga having an n-type dopant concentration of 3 × 10 18 cm -3 or less. T4 In u4 N (0≦s4≦1, 0≦t4≦1, 0≦u4≦1, s4+t4+u4≒1) layer, and more preferably an undoped layer. For example, the n - layer 9B is preferably a GaN layer having an n-type dopant concentration of 3 × 10 18 cm -3 or less, more preferably an undoped GaN layer.

n+層9A及n-層9B之各者之積層數並未特別限定。n型調變摻雜層9可具有2組以上之n+層9A與n-層9B之組合,亦可僅包含1層之n-層9B。 The number of layers of each of the n + layer 9A and the n - layer 9B is not particularly limited. The n-type modulation doped layer 9 may have a combination of two or more n + layers 9A and n - layers 9B, or may include only one layer of n - layer 9B.

n+層9A之各厚度較佳例如為5nm以上500nm以下。n-層9B之各厚度較佳例如為5nm以上500nm以下。 The thickness of each of the n + layers 9A is preferably, for example, 5 nm or more and 500 nm or less. The thickness of each of the n - layers 9B is preferably, for example, 5 nm or more and 500 nm or less.

<第2積層體> <2nd laminated body>

第2積層體11包含V凹坑產生層10、多層構造體121、及超晶格層122。V凹坑產生層10較佳於低於第1積層體6之形成溫度之溫度形成,例如較佳於比n型接觸層8或n型調變摻雜層9之成長溫度(形成第1n型氮化物半導體層之溫度)低之溫度形成。 The second layered body 11 includes a V-pit generation layer 10, a multilayer structure 121, and a superlattice layer 122. The V-pit generation layer 10 is preferably formed at a temperature lower than the formation temperature of the first laminate body 6, for example, preferably higher than the growth temperature of the n-type contact layer 8 or the n-type modulation doping layer 9 (formation of the first n-type) The temperature of the nitride semiconductor layer is formed at a low temperature.

與第1積層體6相接之層更佳於950℃以下形成。藉此,在V凹坑產生層10與第1積層體6相接之情形時,該V凹坑產生層10更佳於950℃以下形成。 The layer in contact with the first layered body 6 is more preferably formed at 950 ° C or lower. Thereby, when the V-pit generation layer 10 is in contact with the first layered body 6, the V-pit generation layer 10 is more preferably formed at 950 ° C or lower.

第2積層體11以不同組成之複數層構成之情形時(例如第2積層體11以V凹坑產生層10、多層構造體121及超晶格層122構成之情形),與第1積層體6相接之層進而較佳於850℃以下之溫度形成。因此,V凹坑產生層10與第1積層體6相接之情形時,該V凹坑產生層10進而較佳於850℃以下形成。 When the second layered body 11 is composed of a plurality of layers having different compositions (for example, when the second layered body 11 is composed of the V-pit generating layer 10, the multilayered structure 121, and the superlattice layer 122), and the first layered body The 6-joined layer is further preferably formed at a temperature of 850 ° C or lower. Therefore, when the V-pit generation layer 10 is in contact with the first layered body 6, the V-pit generation layer 10 is further preferably formed at 850 ° C or lower.

如上所述,因可縮短第2積層體11形成後之降溫步驟所需要之時間,故可維持較高之處理量。又,與V凹坑產生層10之成長溫度為高溫之情形相比,附著於形成V凹坑產生層10之裝置之腔室之附著物量減少。藉此,維護形成第2積層體11之裝置之頻率降低。基於該等原因,氮化物半導體發光元件1之生產性變高。V凹坑產生層10更佳於700℃以上之溫度形成,進而更佳於750℃以上之溫度形成。藉此,可維持較高之MQW發光層14之發光效率。 As described above, since the time required for the temperature lowering step after the formation of the second layered body 11 can be shortened, a high throughput can be maintained. Further, the amount of adhering matter adhering to the chamber of the apparatus for forming the V-pit generation layer 10 is reduced as compared with the case where the growth temperature of the V-pit generation layer 10 is high. Thereby, the frequency of maintaining the apparatus for forming the second layered body 11 is lowered. For these reasons, the productivity of the nitride semiconductor light-emitting element 1 becomes high. The V-pit generation layer 10 is more preferably formed at a temperature of 700 ° C or higher, and more preferably formed at a temperature of 750 ° C or higher. Thereby, the luminous efficiency of the higher MQW light-emitting layer 14 can be maintained.

另,於下文中,作為第2積層體11之構成之一例,顯示第2積層體11係具備V凹坑產生層10、多層構造體121、及超晶格層122之構成。然而,第2積層體11之構成並未限定於以下所示之構成。例如,第2積層體11可包含單一層,亦可包含雜質濃度或組成不同之複數層。 In the following, as a configuration of the second layered product 11, the second layered body 11 is provided with a V-pit generation layer 10, a multilayer structure 121, and a superlattice layer 122. However, the configuration of the second layered body 11 is not limited to the configuration shown below. For example, the second layered body 11 may include a single layer, and may also include a plurality of layers having different impurity concentrations or compositions.

多層構造體121較佳於V凹坑產生層10之成長溫度以下之溫度形成,更佳於與V凹坑產生層10之成長溫度同一溫度形成。若多層構造 體121之成長溫度為V凹坑產生層10之成長溫度以下,則獲得V凹坑15之大小變大之效果。所謂「多層構造體121於V凹坑產生層10之成長溫度以下之溫度形成」意指多層構造體121之成長溫度為(V凹坑產生層10之成長溫度-250℃)以上且V凹坑產生層10之成長溫度以下,且多層構造體121之成長溫度較佳為(V凹坑產生層10之成長溫度-150℃)以上且V凹坑產生層10之成長溫度以下。所謂「多層構造體121於與V凹坑產生層10之成長溫度相同之溫度形成」意指多層構造體121之成長溫度為(V凹坑產生層10之成長溫度±10℃)。以上亦可說是超晶格層122之成長溫度。 The multilayer structure 121 is preferably formed at a temperature lower than the growth temperature of the V-pit generation layer 10, and more preferably formed at the same temperature as the growth temperature of the V-pit generation layer 10. Multilayer construction When the growth temperature of the body 121 is equal to or lower than the growth temperature of the V-pit generation layer 10, the effect of increasing the size of the V-pit 15 is obtained. The "the temperature at which the multilayer structure 121 is formed at a temperature lower than the growth temperature of the V-pit generation layer 10" means that the growth temperature of the multilayer structure 121 is (the growth temperature of the V-pit generation layer -250 ° C) or more and the V-pit The growth temperature of the layer 10 is not more than the growth temperature of the layer 10, and the growth temperature of the multilayer structure 121 is preferably (the growth temperature of the V-pit layer 10 is -150 ° C) or more and the growth temperature of the V-pit generation layer 10 is not more than the growth temperature. The "multilayer structure 121 is formed at the same temperature as the growth temperature of the V-pit generation layer 10" means that the growth temperature of the multilayer structure 121 is (the growth temperature of the V-pit generation layer 10 is ±10 ° C). The above can also be said to be the growth temperature of the superlattice layer 122.

多層構造體121之成長溫度只要為V凹坑產生層10之成長溫度以下,即可獲得V凹坑15之大小變大之效果。然而,若多層構造體121之成長溫度過低,則會致使多層構造體121之膜質降低。因此,多層構造體121之成長溫度較佳為600℃以上,進而較佳為700℃以上。此亦可說是超晶格層122之成長溫度。以下,分別顯示第2積層體11之構成要件。 When the growth temperature of the multilayer structure 121 is equal to or lower than the growth temperature of the V-pit generation layer 10, the effect of increasing the size of the V-pit 15 can be obtained. However, if the growth temperature of the multilayer structure 121 is too low, the film quality of the multilayer structure 121 is lowered. Therefore, the growth temperature of the multilayer structure 121 is preferably 600 ° C or higher, and more preferably 700 ° C or higher. This can also be said to be the growth temperature of the superlattice layer 122. Hereinafter, the constituent elements of the second layered body 11 are respectively shown.

<V凹坑產生層> <V pit generation layer>

V凹坑產生層10係與第1積層體6之第1面61相接,用以形成V凹坑15之層,以使V凹坑15起點之平均位置位於比作為發光層實效發揮功能之層(於本實施形態中為發光層14)更位於第1積層體6側之層(於本實施形態中為超晶格層122)內。所謂「V凹坑15起點」意指V凹坑15之底部(圖1中的V凹坑15之最下端部)。所謂「V凹坑15之起點之平均位置」意指使V凹坑15起點位置於氮化物半導體發光元件1之厚度方向(圖1中上下方向)平均化而得之位置。 The V-pit generation layer 10 is in contact with the first surface 61 of the first layered body 6 to form a layer of the V-pit 15 so that the average position of the starting point of the V-pit 15 is more effective than the function as a light-emitting layer. The layer (in the present embodiment, the light-emitting layer 14) is located further in the layer on the side of the first layered body 6 (in the present embodiment, the superlattice layer 122). The "starting point of the V-pit 15" means the bottom of the V-pit 15 (the lowermost end of the V-pit 15 in Fig. 1). The "average position of the starting point of the V-pit 15" means a position obtained by averaging the starting point of the V-pit 15 in the thickness direction of the nitride semiconductor light-emitting element 1 (vertical direction in FIG. 1).

V凹坑產生層10較佳例如為厚度係25nm之高摻雜n型GaN層。所謂「高摻雜」意指與位於V凹坑產生層10之下之n型接觸層8或n型調變摻雜層9相比有意義(例如1.1倍以上,較佳為1.4倍以上,更佳為1.8 倍以上)增高n型摻雜濃度。具體而言,V凹坑產生層10之n型摻雜濃度較佳為5×1018cm-3以上,更佳為7×1018cm-3以上,進而較佳為1×1019cm-3以上。藉此,因V凹坑產生層10之膜質低於n型調變摻雜層9之膜質,故V凹坑產生層10之V凹坑產生效果有效發揮。 The V-pit generation layer 10 is preferably, for example, a highly doped n-type GaN layer having a thickness of 25 nm. The term "highly doped" means that it is more meaningful than the n-type contact layer 8 or the n-type modulation doping layer 9 located under the V-pit generation layer 10 (for example, 1.1 times or more, preferably 1.4 times or more, more Better than 1.8 times) increase the n-type doping concentration. Specifically, the n-type doping concentration of the V-pit generation layer 10 is preferably 5 × 10 18 cm -3 or more, more preferably 7 × 10 18 cm -3 or more, and still more preferably 1 × 10 19 cm - 3 or more. Thereby, since the film quality of the V-pit generation layer 10 is lower than that of the n-type modulation doping layer 9, the V-pit generation effect of the V-pit generation layer 10 is effectively exerted.

然而,若V凹坑產生層10之n型摻雜物濃度變得過高,則會招致形成於V凹坑產生層10上之發光層14之發光效率之降低。因此,V凹坑產生層10之n型摻雜物濃度較佳為n型調變摻雜層9之n+層9A之n型摻雜物濃度之10倍以下,進而較佳為n型調變摻雜層9之n+層9A之n型摻雜物濃度之3倍以下。 However, if the n-type dopant concentration of the V-pit generation layer 10 becomes too high, the luminous efficiency of the light-emitting layer 14 formed on the V-pit generation layer 10 is lowered. Therefore, the n-type dopant concentration of the V-pit generation layer 10 is preferably 10 times or less of the n-type dopant concentration of the n + layer 9A of the n-type modulation doped layer 9, and is preferably n-type. The concentration of the n-type dopant of the n + layer 9A of the doped layer 9 is 3 times or less.

V凹坑產生層10之n型摻雜物濃度亦可與n型調變摻雜層9之n+層9A之n型摻雜物濃度相同。該情形時,可使藉由V凹坑產生層10產生之V凹坑15之大小增大。藉此,可降低ESD(Electro-Static Discharge:靜電放電)所引起之不良率。 The n-type dopant concentration of the V-pit layer 10 may also be the same as the n-type dopant concentration of the n + layer 9A of the n-type modulation doping layer 9. In this case, the size of the V-pit 15 generated by the V-pit generation layer 10 can be increased. Thereby, the defect rate caused by ESD (Electro-Static Discharge) can be reduced.

V凹坑產生層10較佳與第1積層體6之第1面61相比有意義(例如1.1倍上,較佳為1.4倍以上,更佳為1.8倍以上)增高n型摻雜物濃度。藉此,V凹坑產生層10之V凹坑產生效果進而有效發揮。 The V-pit generation layer 10 is preferably more meaningful than the first surface 61 of the first layered body 6 (for example, 1.1 times, preferably 1.4 times or more, more preferably 1.8 times or more), and the n-type dopant concentration is increased. Thereby, the V-pit generation effect of the V-pit generation layer 10 is effectively exerted.

另,構成第1積層體6之第1面61之半導體層為n+層9A之情形時,V凹坑產生層10亦可為非摻雜層,例如,較佳為厚度係10nm之非摻雜氮化物半導體層。 When the semiconductor layer constituting the first surface 61 of the first layered body 6 is the n + layer 9A, the V-pit generation layer 10 may be an undoped layer, for example, preferably 10 nm thick. A heteronitride semiconductor layer.

V凹坑產生層10較佳例如為於Als5Gat5Inu5N(0≦s5≦1、0≦t5≦1、0≦u5≦1、s5+t5+u5≒1)層中摻雜了n型摻雜物之層,更佳於Inu5Ga1-u5N(0≦u5≦1,較佳為0≦u5≦0.5,更佳為0≦u5≦0.15)層中摻雜n型摻雜物之層。於V凹坑產生層10包含In之情形時,V凹坑產生層10之In組成比較佳高於n型調變摻雜層9之n+層9A及n-層9B之各In組成比。藉此,亦因V凹坑產生層10之膜質低於n型調變摻雜層9之膜質,故V凹坑產生層10之V凹坑產生效果有效發揮。 The V-pit generation layer 10 is preferably doped, for example, in a layer of Al s5 Ga t5 In u5 N (0≦s5≦1, 0≦t5≦1, 0≦u5≦1, s5+t5+u5≒1). The layer of the n-type dopant is more preferably doped with n-type doping in the layer of In u5 Ga 1-u5 N (0≦u5≦1, preferably 0≦u5≦0.5, more preferably 0≦u5≦0.15) The layer of debris. In the case where the V-pit generation layer 10 contains In, the In composition of the V-pit generation layer 10 is preferably higher than the respective In composition ratios of the n + layer 9A and the n - layer 9B of the n-type modulation doping layer 9. Thereby, since the film quality of the V-pit generation layer 10 is lower than that of the n-type modulation doping layer 9, the V-pit generation effect of the V-pit generation layer 10 is effectively exerted.

V凹坑產生層10之厚度較佳為5nm以上,更佳為10nm以上。藉此,貫通錯位之每單位個數之V凹坑數變多。 The thickness of the V-pit generation layer 10 is preferably 5 nm or more, more preferably 10 nm or more. Thereby, the number of V-pits per unit number of the through-dislocation increases.

<多層構造體> <Multilayer structure>

於本實施形態之氮化物半導體發光元件1中,V凹坑15起點比發光層14更位於第1積層體6側。藉此,因構成發光層14之障壁層(尤其非摻雜障壁層)之層數增加,而可使有助於發光之發光層14之體積增加(下述)。藉此,可維持較高之大電流驅動時之發光效率,又可維持較高之高溫下之發光效率。然而,若藉由增加構成發光層14之障壁層(尤其非摻雜障壁層)之層數而增加有助於發光之發光層14之體積,則可知ESD所引起之不良率增加。 In the nitride semiconductor light-emitting device 1 of the present embodiment, the starting point of the V-pit 15 is located closer to the first layered body 6 than the light-emitting layer 14. Thereby, the number of layers of the barrier layer (especially the non-doped barrier layer) constituting the light-emitting layer 14 is increased, and the volume of the light-emitting layer 14 contributing to light emission can be increased (described below). Thereby, the luminous efficiency at the time of driving at a high current can be maintained, and the luminous efficiency at a high temperature can be maintained. However, if the volume of the light-emitting layer 14 which contributes to light emission is increased by increasing the number of layers of the barrier layer (especially, the non-doped barrier layer) constituting the light-emitting layer 14, it is understood that the defect rate caused by ESD is increased.

另一方面,若增加構成發光層14之障壁層(尤其非摻雜障壁層)之層數,則V凹坑產生層10與有助於發光之發光層14之間隔變窄。其結果,成為V凹坑15之起點位於有助於發光之發光層14附近而不佳。為了使V凹坑15之起點之平均位置不存在於發光層14(至少發光層14之上部)內,較佳儘可能使V凹坑產生層10與發光層14分開。然而,若為了達到該目的而增厚設於發光層14與V凹坑產生層10之間之超晶格層122之厚度,則會招致發光層14之品質劣化。此外,亦會招致氮化物半導體發光元件1之生產性之降低。 On the other hand, if the number of layers of the barrier layer (especially the non-doped barrier layer) constituting the light-emitting layer 14 is increased, the interval between the V-pit generation layer 10 and the light-emitting layer 14 which contributes to light emission is narrowed. As a result, it is not preferable that the starting point of the V-pit 15 is located near the light-emitting layer 14 which contributes to light emission. In order to prevent the average position of the starting point of the V-pit 15 from being present in the light-emitting layer 14 (at least the upper portion of the light-emitting layer 14), it is preferable to separate the V-pit generation layer 10 from the light-emitting layer 14 as much as possible. However, if the thickness of the superlattice layer 122 provided between the light-emitting layer 14 and the V-pit generation layer 10 is increased in order to achieve the object, the quality of the light-emitting layer 14 is deteriorated. Further, the productivity of the nitride semiconductor light-emitting element 1 is also lowered.

若以儘可能分離V凹坑產生層10與發光層14為目的,而於V凹坑產生層10與超晶格層122之間於V凹坑產生層10之成長溫度以下之溫度僅加厚形成n型GaN層,則會招致高溫驅動時及大電流驅動時之發光效率之降低,且會招致ESD所引起之不良率之增加。作為其理由,認為如下所示。若於V凹坑產生層10之成長溫度以下之溫度加厚形成n型GaN層(例如200nm以上),則該n型GaN層之成長表面成為凹凸形狀(該n型GaN層之成長表面顯現白濁)。因此,對形成於該n型GaN層上之層造成不良影響之故。例如,致使形成於該n型GaN層上之層之 結晶品質降低。 For the purpose of separating the V-pit generation layer 10 and the light-emitting layer 14 as much as possible, the temperature between the V-pit generation layer 10 and the superlattice layer 122 below the growth temperature of the V-pit generation layer 10 is only thickened. When the n-type GaN layer is formed, the luminous efficiency at the time of high-temperature driving and large-current driving is lowered, and the defect rate caused by ESD is increased. The reason for this is considered as follows. When an n-type GaN layer (for example, 200 nm or more) is formed at a temperature lower than the growth temperature of the V-pit generation layer 10, the grown surface of the n-type GaN layer has an uneven shape (the growth surface of the n-type GaN layer appears white turbid) ). Therefore, it adversely affects the layer formed on the n-type GaN layer. For example, causing a layer formed on the n-type GaN layer The crystal quality is lowered.

然而,若於V凹坑產生層10與超晶格層122之間設有多層構造體121,則因可防止多層構造體121之成長表面成為凹凸形狀,故可維持較高之形成於多層構造體121上之層之結晶品質。藉此,可維持較高之高溫驅動時或大電流驅動時之發光效率,且降低ESD所引起之不良率。說明多層構造體121之構成。 However, when the multilayer structure 121 is provided between the V-pit generation layer 10 and the superlattice layer 122, since the growth surface of the multilayer structure 121 can be prevented from being uneven, it can be maintained in a multilayer structure. The crystalline quality of the layer on the body 121. Thereby, the luminous efficiency at the time of high-temperature driving or high-current driving can be maintained, and the defective rate caused by ESD can be reduced. The configuration of the multilayer structure 121 will be described.

多層構造體121較佳為帶隙能量不同之複數種氮化物半導體層積層而構成者,即帶隙能量相對較大之氮化物半導體層121A與帶隙能量相對較小之氮化物半導體層121B交替積層而構成者。藉此,V凹坑產生層10所產生之V凹坑15之大小變大。藉此,ESD所引起之不良率降低。又,超晶格層122之厚度及發光層14之厚度變大。另,構成多層構造體121之各層厚度較佳大於構成超晶格層122之各層厚度。 The multilayer structure 121 is preferably composed of a plurality of nitride semiconductor layer layers having different band gap energies, that is, the nitride semiconductor layer 121A having a relatively large band gap energy and the nitride semiconductor layer 121B having a relatively small band gap energy are alternately formed. It is composed of layers. Thereby, the size of the V-pit 15 generated by the V-pit generation layer 10 becomes large. Thereby, the defect rate caused by ESD is lowered. Further, the thickness of the superlattice layer 122 and the thickness of the light-emitting layer 14 become large. Further, the thickness of each layer constituting the multilayer structure 121 is preferably larger than the thickness of each layer constituting the superlattice layer 122.

構成多層構造體121之氮化物半導體層之n型摻雜物濃度較佳均低於V凹坑產生層10之n型摻雜物濃度,較佳為例如7×1017cm-3以下。如此若多層構造體121之n型摻雜物濃度降低,則因於反向偏壓施加時空乏層變廣,故可緩和反向電壓施加時被施加於發光層14之電場。藉此,可使多層構造體121與超晶格層122一起作為電場緩和層而發揮功能。另,若氮化物半導體發光元件1之驅動電壓未超過容許範圍,亦可將構成多層構造體121之氮化物半導體層作為非摻雜層。 The n-type dopant concentration of the nitride semiconductor layer constituting the multilayer structure 121 is preferably lower than the n-type dopant concentration of the V-pit generation layer 10, and is preferably, for example, 7 × 10 17 cm -3 or less. As described above, when the n-type dopant concentration of the multilayer structure 121 is lowered, the depletion layer is widened by the application of the reverse bias voltage, so that the electric field applied to the light-emitting layer 14 at the time of application of the reverse voltage can be alleviated. Thereby, the multilayer structure 121 and the superlattice layer 122 can function together as an electric field relaxation layer. Further, when the driving voltage of the nitride semiconductor light-emitting device 1 does not exceed the allowable range, the nitride semiconductor layer constituting the multilayer structure 121 may be an undoped layer.

雖未明確多層構造體121中帶隙能量相對較小之氮化物半導體層(例如InGaN層或n型InGaN層)121B係必要之理由,但認為係如下所示之理由。若於V凹坑產生層10之成長溫度以下之溫度,在帶隙能量相對較大之氮化物半導體層(例如GaN或n型GaN層等)121A之成長中途使帶隙能量相對較小之氮化物半導體層121B成長,則促進構成帶隙能量相對較大之氮化物半導體層121A之材料之2維成長。因此,即使多層構造體121之總厚度增加,亦可防止多層構造體121之總厚度增加所 造成之不良影響及於多層構造體121上成長之層(例如超晶格層122等)。例如,藉由增加多層構造體121之總厚度,可防止超晶格層122之結晶品質降低。 Although the reason why the nitride semiconductor layer (for example, InGaN layer or n-type InGaN layer) 121B having a relatively small band gap energy in the multilayer structure 121 is not necessary is considered to be the reason as shown below. If the temperature is below the growth temperature of the V-pit generation layer 10, the nitrogen having a relatively small band gap energy is grown in the growth of the nitride semiconductor layer (for example, GaN or n-type GaN layer) 121A having a relatively large band gap energy. When the semiconductor layer 121B is grown, the two-dimensional growth of the material constituting the nitride semiconductor layer 121A having a relatively large band gap energy is promoted. Therefore, even if the total thickness of the multilayer structure 121 is increased, the total thickness of the multilayer structure 121 can be prevented from increasing. The adverse effect and the layer grown on the multilayer structure 121 (for example, the superlattice layer 122, etc.). For example, by increasing the total thickness of the multilayer structure 121, the crystal quality of the superlattice layer 122 can be prevented from being lowered.

為了有效獲得此效果,帶隙能量相對較小之氮化物半導體層121B之厚度較佳薄於帶隙能量相對較大之氮化物半導體層121A之厚度,更佳為帶隙能量相對較大之氮化物半導體層121A之厚度之1/5倍以上1/2倍以下。另,帶隙能量相對較大之氮化物半導體層121A之厚度更佳為5nm以上100nm以下,進而較佳為10nm以上40nm以下。 In order to effectively obtain this effect, the thickness of the nitride semiconductor layer 121B having a relatively small band gap energy is preferably thinner than the thickness of the nitride semiconductor layer 121A having a relatively large band gap energy, and more preferably a nitrogen having a relatively large band gap energy. The thickness of the semiconductor layer 121A is 1/5 times or more and 1/2 times or less. Further, the thickness of the nitride semiconductor layer 121A having a relatively large band gap energy is preferably 5 nm or more and 100 nm or less, and more preferably 10 nm or more and 40 nm or less.

多層構造體121之一例係於V凹坑產生層10上依序積層有厚度為7nm之n型InGaN層、厚度為30nm之n型GaN層、厚度為7nm之n型InGaN層及厚度為20nm之n型GaN層者。 One example of the multilayer structure 121 is an n-type InGaN layer having a thickness of 7 nm, an n-type GaN layer having a thickness of 30 nm, an n-type InGaN layer having a thickness of 7 nm, and a thickness of 20 nm, which are sequentially stacked on the V-pit generation layer 10. N-type GaN layer.

構成多層構造體121之氮化物半導體層之具體組成並未特別限定。帶隙能量相對較大之氮化物半導體層121A較佳例如為Ali1Gaj1In(1-i1-j1)N(0≦i1<1、0<j1≦1)層,更佳為GaN層。帶隙能量相對較小之氮化物半導體層121B較佳例如為Ali2Gaj2In(1-i2-j2)N(0≦i2<1、0≦j2<1、j1<j2)層,更佳為Gaj3In(1-j3)N(0<j3<1)層。進而具體而言,多層構造體121亦可為Ali1Gaj1In(1-i1-j1)N(0≦i1<1、0<j1≦1)層與Ali2Gaj2In(1-i2-j2)N(0≦i2<1、0≦j2<1、j1<j2)層交替積層而構成者,又可為GaN層與Gaj3In(1-j3)N(0<j3<1)層交替積層而構成者。 The specific composition of the nitride semiconductor layer constituting the multilayer structure 121 is not particularly limited. The nitride semiconductor layer 121A having a relatively large band gap energy is preferably, for example, an Al i1 Ga j1 In (1-i1-j1) N (0≦i1<1, 0<j1≦1) layer, more preferably a GaN layer. The nitride semiconductor layer 121B having a relatively small band gap energy is preferably, for example, a layer of Al i2 Ga j2 In (1-i2-j2) N (0≦i2<1, 0≦j2<1, j1<j2), more preferably Is a layer of Ga j3 In (1-j3) N (0<j3<1). More specifically, the multilayer structure 121 may also be an Al i1 Ga j1 In (1-i1-j1) N (0≦i1<1, 0<j1≦1) layer and Al i2 Ga j2 In (1-i2- J2) N (0≦i2<1, 0≦j2<1, j1<j2) layers are alternately layered, and may be a GaN layer and a Ga j3 In (1-j3) N (0<j3<1) layer It is composed of alternate layers.

構成多層構造體121之氮化物半導體層包含In之情形時,帶隙能量相對較小之氮化物半導體121B中的In組成比較佳與超晶格層122中的In組成比同程度(±5%)。藉此,於多層構造體121之形成後形成超晶格層122時可省略變更In之原料氣體之供給量之工序。藉此,進而提高氮化物半導體發光元件1之生產性。更佳係於帶隙能量相對較小之氮化物半導體層121B為Gaj3In(1-j3)N(0<j3<1)層時,Gaj3In(1-j3)N(0<j3<1)層中的In組成比(1-j3)與構成超晶格層122之窄帶隙層122B(下 述)中的In組成比相同。 When the nitride semiconductor layer constituting the multilayer structure 121 contains In, the composition of In in the nitride semiconductor 121B having a relatively small band gap energy is preferably the same as the composition ratio of In in the superlattice layer 122 (±5%). ). Thereby, when the superlattice layer 122 is formed after the formation of the multilayer structure 121, the step of changing the supply amount of the material gas of In can be omitted. Thereby, the productivity of the nitride semiconductor light-emitting device 1 is further improved. More preferably, when the nitride semiconductor layer 121B having a relatively small band gap energy is a layer of Ga j3 In (1-j3) N (0<j3<1), Ga j3 In (1-j3) N (0<j3< 1) The In composition ratio (1-j3) in the layer is the same as the In composition ratio in the narrow band gap layer 122B (described below) constituting the superlattice layer 122.

帶隙能量相對較大之氮化物半導體層121A及帶隙能量相對較小之氮化物半導體層121B之各者之層數並未特別限定。多層構造121較佳具有2組以上之帶隙能量相對較大之氮化物半導體層121A及帶隙能量相對較小之氮化物半導體層121B。藉此,可增大多層構造體121之厚度。藉此,V凹坑15起點之平均位置係多數較超晶格層122於厚度方向中央附近更靠向第1積層體6側。因此,可維持較高之高溫驅動時或大電流驅動時之發光效率。 The number of layers of each of the nitride semiconductor layer 121A having a relatively large band gap energy and the nitride semiconductor layer 121B having a relatively small band gap energy is not particularly limited. The multilayer structure 121 preferably has two or more nitride semiconductor layers 121A having a relatively large band gap energy and a nitride semiconductor layer 121B having a relatively small band gap energy. Thereby, the thickness of the multilayer structure 121 can be increased. Thereby, the average position of the starting point of the V-pit 15 is more toward the first layered body 6 side than the center of the superlattice layer 122 in the thickness direction. Therefore, the luminous efficiency at the time of high-temperature driving or high-current driving can be maintained.

<超晶格層> <Superlattice layer>

於V凹坑產生層10與發光層14之間即多層構造體121上,設有超晶格層122。超晶格層122之主要作用係使V凹坑產生層10更自發光層14離開而設,且將V凹坑15起點之位置設於發光層14內之下側或超晶格層122內。超晶格層122可包含單層,亦可2~3層積層而構成。 A superlattice layer 122 is provided between the V-pit generation layer 10 and the light-emitting layer 14, that is, on the multilayer structure 121. The main function of the superlattice layer 122 is such that the V-pit generation layer 10 is further separated from the light-emitting layer 14, and the position of the starting point of the V-pit 15 is set in the lower side of the light-emitting layer 14 or in the superlattice layer 122. . The superlattice layer 122 may comprise a single layer or a layer of 2 to 3 layers.

所謂「超晶格層」意指包含藉由交替積層非常薄之結晶層,而使其週期構造較基本單位晶格更長之結晶晶格之層。超晶格層122係積層複數種氮化物半導體層且構成超晶格構造,如圖3所示之帶隙能量相對較大之寬帶隙層122A與帶隙能量相對較小之窄帶隙層122B交替積層而構成超晶格構造。 By "superlattice layer" is meant a layer comprising a crystalline lattice having a periodic structure that is substantially thinner than a substantially unitary crystal lattice by alternately laminating a very thin crystalline layer. The superlattice layer 122 is formed by laminating a plurality of nitride semiconductor layers and constituting a superlattice structure, and the wide band gap layer 122A having a relatively large band gap energy as shown in FIG. 3 is alternated with the narrow band gap layer 122B having a relatively small band gap energy. The layers are laminated to form a superlattice structure.

超晶格層122亦可依序積層與寬帶隙層122A及窄帶隙層122B不同之1層以上之半導體層、寬帶隙層122A、及窄帶隙層122B而構成超晶格構造。超晶格層122之一週期之長度(寬帶隙層122A之厚度與窄帶隙層122B之厚度之合計)較佳短於下述之發光層14之一週期之長度,更佳例如為1nm以上10nm以下。 The superlattice layer 122 may also sequentially stack a semiconductor layer, a wide band gap layer 122A, and a narrow band gap layer 122B which are different from the wide band gap layer 122A and the narrow band gap layer 122B to form a superlattice structure. The length of one period of the superlattice layer 122 (the total thickness of the wide band gap layer 122A and the thickness of the narrow band gap layer 122B) is preferably shorter than the length of one period of the light-emitting layer 14 described below, and more preferably, for example, 1 nm or more and 10 nm. the following.

各寬帶隙層122A較佳例如為Ala1Gab1In(1-a1-b1)N(0≦a1≦1、0<b1≦1)層,更佳為GaN層。各窄帶隙層122B較佳較寬帶隙層122A帶隙能量要小,更佳較各井層14W(下述)帶隙能量要大。窄帶隙層122B較佳 例如為Ala2Gab2In(1-a2-b2)N(0≦a2<1、0<b2<1、(1-a1-b1)<(1-a2-b2))層,更佳為Gab2In(1-b2)N(0<b2<1)層。 Each of the wide band gap layers 122A is preferably, for example, a layer of Al a1 Ga b1 In (1-a1-b1) N (0≦a1≦1, 0<b1≦1), more preferably a GaN layer. Each narrow band gap layer 122B preferably has a smaller band gap energy than the wide band gap layer 122A, and more preferably has a larger band gap energy than each well layer 14W (described below). The narrow band gap layer 122B is preferably, for example, Al a2 Ga b2 In (1-a2-b2) N (0≦a2<1, 0<b2<1, (1-a1-b1)<(1-a2-b2)) The layer is more preferably a Ga b2 In (1-b2) N (0 < b2 < 1) layer.

各寬帶隙層122A及各窄帶隙層122B之至少一者較佳包含n型摻雜物,且較佳例如包含1×1019cm-3以上之n型摻雜物。n型摻雜物並未特別限定,較佳例如為Si、P、As或Sb等,更佳為Si。 At least one of each of the wide bandgap layer 122A and each of the narrow bandgap layers 122B preferably includes an n-type dopant, and preferably contains, for example, an n-type dopant of 1 × 10 19 cm -3 or more. The n-type dopant is not particularly limited, and is preferably, for example, Si, P, As, or Sb, and more preferably Si.

若寬帶隙層122A與窄帶隙層122B之兩者為非摻雜層,則有驅動電壓上升之情況。另一方面,若構成超晶格層122之氮化物半導體層全部為摻雜層,則由於反向偏壓施加時空乏層難以擴大,故電子難以脫離超晶格層122。因此,存在無法充分獲得電場緩和效果之情形。然而,超晶格層122亦具有為了將電子注入發光層14而設置之層。藉此,若將位於發光層14側之至少2層之氮化物半導體層設為摻雜層,且將較該摻雜層位於更靠向第1積層體6側之氮化物半導體層設為非摻雜層,則可增加注入發光層14之電子數。藉此,發光輸出提高,且驅動電壓降低。然而,若非摻雜層之厚度變厚,則由於為了移動電子有必要施加電壓,因而有驅動電壓增大之情況。為了維持較低之驅動電壓,較佳將位於第1積層體6側之至少2層之氮化物半導體層設為非摻雜層。 If both the wide band gap layer 122A and the narrow band gap layer 122B are undoped layers, there is a case where the driving voltage rises. On the other hand, if all of the nitride semiconductor layers constituting the superlattice layer 122 are doped layers, it is difficult to expand the depletion layer due to the application of the reverse bias, so that it is difficult for electrons to escape from the superlattice layer 122. Therefore, there is a case where the electric field relaxation effect cannot be sufficiently obtained. However, the superlattice layer 122 also has a layer provided to inject electrons into the light-emitting layer 14. Thereby, at least two nitride semiconductor layers located on the side of the light-emitting layer 14 are doped, and the nitride semiconductor layer located on the side closer to the first laminated body 6 is set to be smaller than the doped layer. By doping the layer, the number of electrons injected into the luminescent layer 14 can be increased. Thereby, the light output is increased and the driving voltage is lowered. However, if the thickness of the undoped layer is increased, it is necessary to apply a voltage for moving electrons, and thus the driving voltage is increased. In order to maintain a low driving voltage, it is preferable to form at least two nitride semiconductor layers on the side of the first layered body 6 as an undoped layer.

寬帶隙層122A與窄帶隙層122B之各層數並未特別限定。超晶格層122較佳具有20組以上之寬帶隙層122A及窄帶隙層122B。藉此,可進而自發光層14隔離V凹坑產生層10而設置。因此,可將V凹坑15起點之平均位置設於超晶格層122內。 The number of layers of the wide band gap layer 122A and the narrow band gap layer 122B is not particularly limited. The superlattice layer 122 preferably has more than 20 sets of the wide band gap layer 122A and the narrow band gap layer 122B. Thereby, the V-pit generation layer 10 can be further provided from the light-emitting layer 14 to be provided. Therefore, the average position of the starting point of the V-pit 15 can be set in the superlattice layer 122.

超晶格層122具有20組以上之寬帶隙層122A及窄帶隙層122B之情形時,位於發光層14側之5組之寬帶隙層122A及窄帶隙層122B較佳為摻雜層。藉此,由於可進而增加注入發光層14之電子數,故發光輸出進而提高,驅動電壓進而降低。 When the superlattice layer 122 has 20 or more wide band gap layers 122A and narrow band gap layers 122B, the five sets of the wide band gap layer 122A and the narrow band gap layer 122B on the side of the light emitting layer 14 are preferably doped layers. Thereby, since the number of electrons injected into the light-emitting layer 14 can be further increased, the light-emission output is further increased, and the driving voltage is further lowered.

於超晶格層122之其他例中,非摻雜超晶格構造與摻雜超晶格構 造依序設於多層構造體121上。非摻雜超晶格構造較佳包含17組之非摻雜之寬帶隙層122A及非摻雜之窄帶隙層122B。摻雜超晶格構造較佳包含3組之摻雜之寬帶隙層122A及摻雜之窄帶隙層122B。 In other examples of superlattice layer 122, undoped superlattice structure and doped superlattice The fabrication is sequentially performed on the multilayer structure 121. The undoped superlattice structure preferably comprises 17 sets of undoped wide bandgap layer 122A and undoped narrow bandgap layer 122B. The doped superlattice structure preferably comprises three sets of doped wide bandgap layers 122A and doped narrow bandgap layers 122B.

於超晶格層122之又其他例中,第1摻雜超晶格構造、非摻雜超晶格構造、第2摻雜超晶格構造依序設於多層構造體121上。第1及第2摻雜超晶格構造較佳分別包含5組之摻雜之寬帶隙層122A及摻雜之窄帶隙層122B。非摻雜超晶格構造較佳包含10組之非摻雜之寬帶隙層122A及非摻雜之窄帶隙層122B。 In still another example of the superlattice layer 122, the first doped superlattice structure, the undoped superlattice structure, and the second doped superlattice structure are sequentially provided on the multilayer structure 121. The first and second doped superlattice structures preferably each comprise five sets of doped wide bandgap layers 122A and doped narrow bandgap layers 122B. The undoped superlattice structure preferably comprises 10 sets of undoped wide bandgap layer 122A and undoped narrow bandgap layer 122B.

超晶格層122係為了進而提高發光層14之特性而設置之層,對於氮化物半導體發光元件1而言並非必須之構成要件。然而,若於V凹坑產生層10與發光層14之間設置超晶格層122,則可使V凹坑產生層10與發光層14隔開。藉此,可使V凹坑15起點之平均位置不存在於發光層14(至少發光層14之上部)內。因此,氮化物半導體發光元件1較佳於V凹坑產生層10與發光層14之間包含超晶格層122。較佳係超晶格層122之厚度為40nm以上,更佳為超晶格層122之厚度為50nm以上,進而較佳為超晶格層122之厚度為60nm以上。另一方面,若超晶格層122之厚度過大,則有致使發光層14之結晶品質劣化之虞。因此,超晶格層122之厚度較佳為100nm以下,更佳為80nm以下。另,寬帶隙層122A之各厚度較佳例如為1nm以上3nm以下。窄帶隙層122B之各厚度較佳例如為1nm以上3nm以下。 The superlattice layer 122 is a layer that is provided to further improve the characteristics of the light-emitting layer 14, and is not essential for the nitride semiconductor light-emitting device 1. However, if the superlattice layer 122 is provided between the V-pit generation layer 10 and the light-emitting layer 14, the V-pit generation layer 10 and the light-emitting layer 14 can be separated. Thereby, the average position of the starting point of the V-pit 15 can be prevented from being present in the light-emitting layer 14 (at least the upper portion of the light-emitting layer 14). Therefore, the nitride semiconductor light-emitting element 1 preferably includes the superlattice layer 122 between the V-pit generation layer 10 and the light-emitting layer 14. Preferably, the thickness of the superlattice layer 122 is 40 nm or more, more preferably the thickness of the superlattice layer 122 is 50 nm or more, and further preferably the thickness of the superlattice layer 122 is 60 nm or more. On the other hand, if the thickness of the superlattice layer 122 is too large, the crystal quality of the light-emitting layer 14 is deteriorated. Therefore, the thickness of the superlattice layer 122 is preferably 100 nm or less, more preferably 80 nm or less. Further, the thickness of each of the wide band gap layers 122A is preferably, for example, 1 nm or more and 3 nm or less. The thickness of each of the narrow band gap layers 122B is preferably, for example, 1 nm or more and 3 nm or less.

<發光層> <Light Emitting Layer>

發光層14係設於第2積層體11上。於發光層14上部分地形成V凹坑15。所謂「部分地形成V凹坑15」意指以AFM(Atomic Force Microscope:原子力顯微鏡)觀察發光層14之上表面時觀察到V凹坑15於發光層14之上表面成點狀。發光層14之上表面中的V凹坑數之密度較佳為1×108cm-2以上1×1010cm-2以下。以往雖亦於發光層形成V凹 坑,但以往之發光層之上表面中的V凹坑數之密度未滿1×108cm-2The light-emitting layer 14 is provided on the second layered body 11. V pits 15 are partially formed on the light emitting layer 14. By "partially forming the V-pit 15", it is observed that the V-pit 15 is observed as a dot on the upper surface of the light-emitting layer 14 when the upper surface of the light-emitting layer 14 is observed by an AFM (Atomic Force Microscope). The density of the number of V-pits in the upper surface of the light-emitting layer 14 is preferably 1 × 10 8 cm -2 or more and 1 × 10 10 cm -2 or less. In the past, although V-pits were formed in the light-emitting layer, the density of the number of V-pits in the upper surface of the conventional light-emitting layer was less than 1 × 10 8 cm -2 .

發光層14較佳如圖3所示,具有交替積層障壁層14A與井層14W之積層構造。於超晶格層122之正上方,較佳設置最初之障壁層14AZ。於井層14W中位於最靠近p型氮化物半導體層16側之井層14W1上,較佳設置最後之障壁層14A0。 The light-emitting layer 14 is preferably as shown in FIG. 3, and has a laminated structure in which the barrier layer 14A and the well layer 14W are alternately laminated. Immediately above the superlattice layer 122, an initial barrier layer 14AZ is preferably provided. The last barrier layer 14A0 is preferably disposed on the well layer 14W1 closest to the p-type nitride semiconductor layer 16 side in the well layer 14W.

於本實施形態中,為了識別各障壁層14A及井層14W,自p型氮化物半導體層16朝向晶格層122附註編號且表述為井層14W1、障壁層14A1、井層14W2、障壁層14A2、...等。另,除特定各障壁層14A及各井層14W之各者之情形外,表述為「障壁層14A」及「井層14W」。 In the present embodiment, in order to identify each of the barrier layer 14A and the well layer 14W, the p-type nitride semiconductor layer 16 is numbered toward the lattice layer 122 and is expressed as a well layer 14W1, a barrier layer 14A1, a well layer 14W2, and a barrier layer 14A2. ,...Wait. In addition, it is expressed as "barrier layer 14A" and "well layer 14W" except for the case where each of the barrier layers 14A and each of the well layers 14W is specified.

發光層14亦可具有依序積層1層以上之與障壁層14A及井層14W不同之半導體層、障壁層14A、及井層14W之積層構造。又,發光層14之一週期(障壁層14A之厚度與井層14W之厚度之和)之長度較佳例如為5nm以上100nm以下。 The light-emitting layer 14 may have a laminated structure in which one or more layers of the semiconductor layer, the barrier layer 14A, and the well layer 14W which are different from the barrier layer 14A and the well layer 14W are sequentially laminated. Further, the length of one period of the light-emitting layer 14 (the sum of the thickness of the barrier layer 14A and the thickness of the well layer 14W) is preferably, for example, 5 nm or more and 100 nm or less.

各井層14W之組成較佳配合氮化物半導體發光元件1所求得之發光波長進行調整,例如,較佳為AlcGadIn(1-c-d)N(0≦c<1、0<d≦1),更佳為未含Al之IneGa(1-e)N(0<e≦1)。在使氮化物半導體發光元件1發出例如波長375nm以下之紫外光之情形時,因必須增大發光層14之帶隙能量,故各井層14W之組成較佳包含Al。 The composition of each well layer 14W is preferably adjusted in accordance with the wavelength of light emitted by the nitride semiconductor light-emitting device 1, and is preferably, for example, Al c Ga d In (1-cd) N (0≦c<1, 0<d) ≦1) is more preferably In e Ga (1-e) N (0<e≦1) which does not contain Al. When the nitride semiconductor light-emitting element 1 emits ultraviolet light having a wavelength of, for example, 375 nm or less, since the band gap energy of the light-emitting layer 14 must be increased, the composition of each well layer 14W preferably contains Al.

各井層14W之組成較好相同。藉此,可使因各井層14W中使電子與電洞再結合而發光之波長相同。因此,可使氮化物半導體發光元件1之發光光譜寬度變窄。 The composition of each well layer 14W is preferably the same. Thereby, the wavelength of light emitted by recombining electrons and holes in each well layer 14W can be made the same. Therefore, the width of the light-emitting spectrum of the nitride semiconductor light-emitting element 1 can be narrowed.

位於p型氮化物半導體層16側之井層14W較佳儘量不含摻雜物。若換言之,較佳係未導入摻雜物原料而使位於p型氮化物半導體層16側之井層14W成長。藉此,因不易於各井層14W中引起非發光再結合,故發光效率良好。另一方面,位於第1積層體6側之井層14W亦可包含n型摻雜物。藉此,具有氮化物半導體發光元件1之驅動電壓降低 之傾向。 The well layer 14W on the side of the p-type nitride semiconductor layer 16 is preferably free of dopants as much as possible. In other words, it is preferable that the well layer 14W located on the side of the p-type nitride semiconductor layer 16 is grown without introducing a dopant material. Thereby, since it is not easy to cause non-lighting recombination in each well layer 14W, the luminous efficiency is good. On the other hand, the well layer 14W located on the side of the first layered body 6 may also contain an n-type dopant. Thereby, the driving voltage of the nitride semiconductor light-emitting element 1 is lowered. The tendency.

各井層14W之厚度並未特別限定,較佳分別相同。若各井層14W之厚度相同,則各井層14W之量子位準亦相同。因此,藉由各井層14W中的電子與電洞之再結合,於各井層14W中產生相同波長之光。因此,氮化物半導體發光元件1之發光光譜寬度變窄,故較佳。另一方面,若刻意使井層14W之組成或厚度不同,則可使氮化物半導體發光元件1之發光光譜寬度變寬。在將氮化物半導體發光元件1用於照明等用途之情形時,因氮化物半導體發光元件1之發光光譜寬度較寬時較佳,故較佳刻意使井層14W之組成或厚度不同。例如,較佳於1nm以上7nm以下之範圍內適當設定各井層14W之厚度。藉此,可維持較高之發光效率。 The thickness of each well layer 14W is not particularly limited, and is preferably the same. If the thickness of each well layer 14W is the same, the quantum level of each well layer 14W is also the same. Therefore, light of the same wavelength is generated in each well layer 14W by recombination of electrons and holes in each well layer 14W. Therefore, the width of the light-emitting spectrum of the nitride semiconductor light-emitting device 1 is preferably narrow. On the other hand, if the composition or thickness of the well layer 14W is deliberately different, the width of the light-emitting spectrum of the nitride semiconductor light-emitting device 1 can be made wider. When the nitride semiconductor light-emitting device 1 is used for applications such as illumination, since the width of the light-emitting spectrum of the nitride semiconductor light-emitting device 1 is wider, it is preferable to intentionally make the composition or thickness of the well layer 14W different. For example, it is preferable to appropriately set the thickness of each well layer 14W in the range of 1 nm or more and 7 nm or less. Thereby, high luminous efficiency can be maintained.

構成各障壁層14A(14A1~14A7)、最初障壁層14AZ及最後障壁層14A0之材料較佳為與分別構成各井層14W之材料相比帶隙能量較大者。具體而言,各障壁層14A(14A1~14A7)、最初障壁層14AZ及最後障壁層14A0較佳包含AlfGagIn(1-f-g)N(0≦f<1、0<g≦1),更佳包含未含Al之InhGa(1-h)N(0<h≦1、e>h),進而較佳包含構成井層14W之材料與晶格常數大致相同之AlfGagIn(1-f-g)N(0≦f<1、0<g≦1)。 The material constituting each of the barrier layers 14A (14A1 to 14A7), the first barrier layer 14AZ, and the last barrier layer 14A0 is preferably larger than the material constituting each of the well layers 14W. Specifically, each of the barrier layers 14A (14A1 to 14A7), the first barrier layer 14AZ, and the last barrier layer 14A0 preferably include Al f Ga g In (1-fg) N (0≦f<1, 0<g≦1). More preferably, it includes In h Ga (1-h) N (0<h≦1, e>h) which does not contain Al, and further preferably contains Al f Ga g which is substantially the same as the lattice constant of the material constituting the well layer 14W. In (1-fg) N (0≦f<1, 0<g≦1).

各障壁層14A之厚度並未特別限定,較佳為1nm以上10nm以下,更佳為3nm以上7nm以下。各障壁層14A之厚度越薄驅動電壓越低,若各障壁層14A之厚度極端薄,則有發光效率降低之傾向。最初之障壁層14AZ之厚度並未特別限定,較佳為1nm以上10nm以下。最後之障壁層14A0之厚度並未特別限定,較佳為1nm以上40nm以下。 The thickness of each barrier layer 14A is not particularly limited, but is preferably 1 nm or more and 10 nm or less, and more preferably 3 nm or more and 7 nm or less. The thinner the thickness of each of the barrier layers 14A is, the lower the driving voltage is. If the thickness of each of the barrier layers 14A is extremely thin, the luminous efficiency tends to be lowered. The thickness of the first barrier layer 14AZ is not particularly limited, but is preferably 1 nm or more and 10 nm or less. The thickness of the last barrier layer 14A0 is not particularly limited, but is preferably 1 nm or more and 40 nm or less.

各障壁層14A(14A1~14A7)及最初障壁層14AZ中的n型擦雜物濃度並未特別限定,較佳根據需要適當設定。又,複數障壁層14A中,位於第1積層體6側之障壁層14A較佳包含n型摻雜物,位於p型氮化物半導體層16側之障壁層14A較佳包含較位於第1積層體6側之障壁層 14A更低濃度之n型摻雜物、或不含n型摻雜物。各障壁層14A(14A1~14A7)、最初障壁層14AZ及最後障壁層14A0亦可刻意地包含n型摻雜物。又,於各障壁層14A(14A1~14A7)、最初障壁層14AZ及最後障壁層14A0中,藉由p型氮化物半導體層16、17、18之成長時之熱擴散而摻雜p型摻雜物。 The concentration of the n-type dopant in each of the barrier layers 14A (14A1 to 14A7) and the first barrier layer 14AZ is not particularly limited, and is preferably set as appropriate. Further, in the plurality of barrier layers 14A, the barrier layer 14A on the side of the first laminate 6 preferably includes an n-type dopant, and the barrier layer 14A on the side of the p-type nitride semiconductor layer 16 preferably contains the first laminate. 6-side barrier layer 14A lower concentration n-type dopant, or no n-type dopant. Each of the barrier layers 14A (14A1 to 14A7), the first barrier layer 14AZ, and the last barrier layer 14A0 may also intentionally contain an n-type dopant. Further, in each of the barrier layers 14A (14A1 to 14A7), the first barrier layer 14AZ, and the last barrier layer 14A0, p-type doping is doped by thermal diffusion during growth of the p-type nitride semiconductor layers 16, 17, 18. Things.

井層14W之層數並未特別限定,較佳例如為2層以上20層以下,更佳為3層以上15層以下,進而較佳為4層以上12層以下。 The number of layers of the well layer 14W is not particularly limited, but is preferably 2 or more and 20 or less, more preferably 3 or more and 15 or less, and still more preferably 4 or more and 12 or less.

<p型氮化物半導體層> <p type nitride semiconductor layer>

p型氮化物半導體層16、17、18係依序設於發光層14上。p型氮化物半導體層之層數並未限定於3層,亦可為2層以下,又可為4層以上。p型氮化物半導體層16、17、18較佳例如為於Als6Gat6Inu6N(0≦s6≦1、0≦t6≦1、0≦u6≦1、s6+t6+u6≠0)層中摻雜p型摻雜物之層,更佳為於Als6Ga(1-s6)N(0<s6≦0.4,較佳為0.1≦s6≦0.3)層中摻雜p型摻雜物之層。例如,p型氮化物半導體層16為p型AlGaN層,p型氮化物半導體層17為p型GaN層,p型氮化物半導體層18為p型摻雜物濃度較p型氮化物半導體層17更高之p型GaN層。 The p-type nitride semiconductor layers 16, 17, and 18 are sequentially provided on the light-emitting layer 14. The number of layers of the p-type nitride semiconductor layer is not limited to three, and may be two or less, or four or more. The p-type nitride semiconductor layers 16, 17, 18 are preferably, for example, Al s6 Ga t6 In u6 N (0≦s6≦1, 0≦t6≦1, 0≦u6≦1, s6+t6+u6≠0) a layer doped with a p-type dopant in the layer, more preferably a p-type dopant doped in a layer of Al s6 Ga (1-s6) N (0<s6≦0.4, preferably 0.1≦s6≦0.3) Layer. For example, the p-type nitride semiconductor layer 16 is a p-type AlGaN layer, the p-type nitride semiconductor layer 17 is a p-type GaN layer, and the p-type nitride semiconductor layer 18 has a p-type dopant concentration higher than that of the p-type nitride semiconductor layer 17. A higher p-type GaN layer.

p型摻雜物並未特別限定,較佳例如為Mg。p型氮化物半導體層16、17、18之載子濃度較佳為1×1017cm-3以上。此處,p型摻雜物之活性率為0.01左右,因而p型氮化物半導體層16、17、18之p型摻雜物濃度(與載子濃度不同)較佳為1×1019cm-3以上。其中,p型氮化物半導體層16中位於發光層14側之部分之p型摻雜物濃度亦可未滿1×1019cm-3The p-type dopant is not particularly limited, and is preferably, for example, Mg. The carrier concentration of the p-type nitride semiconductor layers 16, 17, 18 is preferably 1 × 10 17 cm -3 or more. Here, the activity ratio of the p-type dopant is about 0.01, and thus the p-type dopant concentration (different from the carrier concentration) of the p-type nitride semiconductor layers 16, 17, 18 is preferably 1 × 10 19 cm - 3 or more. The p-type dopant concentration in the portion of the p-type nitride semiconductor layer 16 on the side of the light-emitting layer 14 may be less than 1 × 10 19 cm -3 .

p型氮化物半導體層16、17、18之合計之厚度並未特別限定,較佳為50nm以上300nm以下。若p型氮化物半導體層16、17、18之厚度變薄,則因其成長時之加熱時間變短,故可防止p型摻雜物向發光層14擴散。 The total thickness of the p-type nitride semiconductor layers 16, 17, and 18 is not particularly limited, but is preferably 50 nm or more and 300 nm or less. When the thickness of the p-type nitride semiconductor layers 16, 17, and 18 is reduced, the heating time during the growth is shortened, so that the p-type dopant can be prevented from diffusing into the light-emitting layer 14.

<n側電極、透明電極、p側電極> <n side electrode, transparent electrode, p side electrode>

n側電極21及p側電極25係用以對氮化物半導體發光元件1供給驅動電力之電極。圖2中圖示有僅以焊墊電極部分構成n側電極21及p側電極25之情形。然而,以電流擴散為目的之細長突出部(枝電極)亦可連接於圖2所示之n側電極21及p側電極25。又,於p側電極25更下側,較佳設置有用以防止電流朝p側電極25注入之絕緣層。藉此,可使發光層14發出之光被p側電極25遮蔽之量減少。 The n-side electrode 21 and the p-side electrode 25 are electrodes for supplying driving power to the nitride semiconductor light-emitting device 1. FIG. 2 shows a case where the n-side electrode 21 and the p-side electrode 25 are formed only by pad electrode portions. However, the elongated protrusion (branch electrode) for the purpose of current spreading may be connected to the n-side electrode 21 and the p-side electrode 25 shown in FIG. Further, on the lower side of the p-side electrode 25, an insulating layer for preventing an electric current from being injected into the p-side electrode 25 is preferably provided. Thereby, the amount of light emitted from the light-emitting layer 14 can be reduced by the p-side electrode 25.

n側電極21較佳例如具有鈦層、鋁層及金層依序積層之積層構造。假定於n側電極21進行打線結合之情形,n側電極21之厚度較佳為1μm以上。 The n-side electrode 21 preferably has, for example, a laminated structure in which a titanium layer, an aluminum layer, and a gold layer are sequentially laminated. It is assumed that the thickness of the n-side electrode 21 is preferably 1 μm or more in the case where the n-side electrode 21 is bonded by wire bonding.

p側電極25係較佳例如具有鎳層、鋁層、鈦層及金層依序積層之積層構造,亦可包含與n側電極21相同材料。假定於p側電極25進行打線結合之情形,p側電極25之厚度較佳為1μm以上。 The p-side electrode 25 preferably has a laminated structure in which a nickel layer, an aluminum layer, a titanium layer, and a gold layer are sequentially laminated, and may include the same material as the n-side electrode 21. It is assumed that the thickness of the p-side electrode 25 is preferably 1 μm or more in the case where the p-side electrode 25 is bonded by wire bonding.

透明電極23較佳包含例如ITO(Indium Tin Oxide:氧化銦錫)或IZO(Indium Zinc Oxide:氧化銦鋅)等之透明導電材料,更佳具有20nm以上200nm以下之厚度。 The transparent electrode 23 preferably contains a transparent conductive material such as ITO (Indium Tin Oxide) or IZO (Indium Zinc Oxide), and more preferably has a thickness of 20 nm or more and 200 nm or less.

<V凹坑起點> <V pit start point>

於本實施形態之氮化物半導體發光元件1中,V凹坑15起點之大部分不存在於發光層14內,其過半數量被認為存在於超晶格層122內。V凹坑15係被認為由貫通錯位而引起,故認為貫通錯位多數位於V凹坑15之內側。因此,可抑制注入發光層14之電子及電洞到達V凹坑15內側之貫通錯位。因此,認為可抑制為了於貫通錯位中捕獲電子及電洞而產生非發光再結合之情形。藉此,可維持較高之發光效率。該效果於高溫下或大電流驅動時尤為顯著。 In the nitride semiconductor light-emitting device 1 of the present embodiment, most of the starting point of the V-pit 15 does not exist in the light-emitting layer 14, and a majority of the number is considered to exist in the superlattice layer 122. The V-pit 15 is considered to be caused by the through-dislocation, and it is considered that the through-dislocation is mostly located inside the V-pit 15. Therefore, it is possible to suppress the penetration of the electrons and holes injected into the light-emitting layer 14 into the inside of the V-pit 15. Therefore, it is considered that it is possible to suppress the occurrence of non-light-emitting recombination in order to capture electrons and holes in the through-dislocation. Thereby, high luminous efficiency can be maintained. This effect is particularly noticeable at high temperatures or when driven at high currents.

詳細而言,因高溫下對發光層14之注入載子(電洞或電子)之移動活潑,故注入載子到達貫通錯位之機率增大。然而,於本實施形態之 氮化物半導體發光元件1中,因發光層14內之貫通錯位較多被V凹坑15覆蓋(因貫通錯位多存在於V凹坑15之內側),故抑制貫通錯位之非發光再結合。藉此,可維持較高之高溫下之發光效率。 Specifically, since the movement of the injection carrier (hole or electron) to the light-emitting layer 14 is active at a high temperature, the probability of the injected carrier reaching the through-dislocation is increased. However, in the embodiment In the nitride semiconductor light-emitting device 1, since the through-dislocation in the light-emitting layer 14 is mostly covered by the V-pit 15 (the inside of the V-pit 15 is often caused by the through-dislocation), the non-light-emitting recombination of the through-dislocation is suppressed. Thereby, the luminous efficiency at a high temperature can be maintained.

又,因V凹坑15起點位於較發光層14更下側,故可增加障壁層(尤其非摻雜物障壁層)之層數,且增加發光層14之體積。藉此,可維持較高之大電流驅動時之發光效率。 Moreover, since the starting point of the V-pit 15 is located on the lower side of the light-emitting layer 14, the number of layers of the barrier layer (especially the non-dopant barrier layer) can be increased, and the volume of the light-emitting layer 14 can be increased. Thereby, the luminous efficiency at the time of driving at a high current can be maintained.

<關於載子濃度與摻雜物濃度> <About carrier concentration and dopant concentration>

載子濃度意指電子或電洞之濃度,不由n型摻雜物之量或p型摻雜物之量決定。此般之載子濃度意指基於氮化物半導體發光元件1之電壓對電容特性之結果算出,且未注入電流之狀態之載子濃度,為自離子化之雜質、供體化之結晶缺陷及受體化之結晶缺陷所產生之載子之合計。 The carrier concentration means the concentration of electrons or holes, not determined by the amount of n-type dopant or the amount of p-type dopant. The carrier concentration is calculated based on the voltage characteristic of the nitride semiconductor light-emitting device 1 and the carrier concentration in the state where the current is not injected, and is a self-ionized impurity, a crystallized defect of the donor, and a The total number of carriers produced by the crystallized defects of the body.

n型摻雜物即Si等之活性化率高。藉此,可認為n型載子濃度與n型摻雜物濃度大致相同。又,n型摻雜物濃度可藉由以SIMS(Secondary Ion Mass Spectroscopy:二次離子質譜儀)量測深度方向之濃度分佈而簡單求得。再者,摻雜物濃度之相對關係(比例)係與載子濃度之相對關係(比例)大致相同。只要將由量測而得之n型摻雜物濃度於厚度方向平均化,即可獲得平均n型摻雜物濃度。 The activation rate of the n-type dopant, that is, Si or the like is high. Thereby, the n-type carrier concentration can be considered to be substantially the same as the n-type dopant concentration. Further, the n-type dopant concentration can be easily obtained by measuring the concentration distribution in the depth direction by SIMS (Secondary Ion Mass Spectroscopy). Further, the relative relationship (ratio) of the dopant concentration is substantially the same as the relative relationship (ratio) of the carrier concentration. The average n-type dopant concentration can be obtained by averaging the measured n-type dopant concentration in the thickness direction.

<關於n型調變摻雜層與超晶格層之其他作用、效果> <Other effects and effects on the n-type modulation doping layer and superlattice layer>

於本實施形態之氮化物半導體發光元件1中,於n型接觸層8與發光層14之間,自n型接觸層8側起依序積層有n型調變摻雜層9、V凹坑產生層10、多層構造體121及超晶格層122。藉此,在成為ESD破壞之原因之反向偏壓方向之高電壓施加於n側電極21與p側電極25之間之情形時,空乏層於n型調變摻雜層9及超晶格層122側伸長。藉此,可降低施加於發光層14之反向偏移電壓(電場)。因此,產生ESD破壞之臨限值電壓(即ESD耐壓)變高。 In the nitride semiconductor light-emitting device 1 of the present embodiment, an n-type modulation doped layer 9 and a V-pit are sequentially stacked from the n-type contact layer 8 side between the n-type contact layer 8 and the light-emitting layer 14. The layer 10, the multilayer structure 121, and the superlattice layer 122 are produced. Thereby, when a high voltage in the reverse bias direction which is the cause of ESD destruction is applied between the n-side electrode 21 and the p-side electrode 25, the depletion layer is formed in the n-type modulation doping layer 9 and the superlattice. The layer 122 is elongated on the side. Thereby, the reverse offset voltage (electric field) applied to the light-emitting layer 14 can be reduced. Therefore, the threshold voltage (i.e., ESD withstand voltage) that causes ESD destruction becomes high.

於本實施形態之氮化物半導體發光元件以1刻意地不導入V凹坑15之方式構成之情形時,亦可使於順向施加偏移電壓時之洩漏電流更有效地降低,且可防止V凹坑15之形成所引起之發光面積降低。因此,於該情形時,亦可有效防止氮化物半導體發光元件1之發光特性降低。 In the case where the nitride semiconductor light-emitting device of the present embodiment is configured such that the V-pit 15 is not intentionally introduced, the leakage current when the offset voltage is applied in the forward direction can be more effectively reduced, and the V can be prevented. The light-emitting area caused by the formation of the pits 15 is lowered. Therefore, in this case as well, the light-emitting characteristics of the nitride semiconductor light-emitting element 1 can be effectively prevented from being lowered.

於本實施形態之氮化物半導體發光元件1僅包含n型調變摻雜層9或超晶格層122之任一者之情形,亦可獲得上述作用及效果。然而,本實施形態之氮化物半導體發光元件1較佳包含n型調變摻雜層9及超晶格層122兩者。藉此,ESD耐壓變高。可使於順向施加偏移電壓時之洩漏電流更有效地降低,且可防止V凹坑15之形成所引起之發光面積之降低。 In the case where the nitride semiconductor light-emitting device 1 of the present embodiment includes only one of the n-type modulation doped layer 9 or the superlattice layer 122, the above-described actions and effects can be obtained. However, the nitride semiconductor light-emitting device 1 of the present embodiment preferably includes both the n-type modulation doped layer 9 and the superlattice layer 122. Thereby, the ESD withstand voltage becomes high. The leakage current when the offset voltage is applied in the forward direction can be more effectively reduced, and the decrease in the light-emitting area caused by the formation of the V-pit 15 can be prevented.

<氮化物半導體發光元件之製造> <Manufacture of nitride semiconductor light-emitting element>

圖5(a)係顯示圖1所示之氮化物半導體發光元件1之製造步驟之溫度分佈之圖表。圖5(a)之縱軸表示成長溫度,圖5(a)之橫軸表示成長時間。另,圖5(b)係顯示下述比較例1之氮化物半導體發光元件之製造步驟中的溫度分佈之圖表。 Fig. 5(a) is a graph showing the temperature distribution of the manufacturing steps of the nitride semiconductor light-emitting device 1 shown in Fig. 1. The vertical axis of Fig. 5(a) indicates the growth temperature, and the horizontal axis of Fig. 5(a) indicates the growth time. In addition, FIG. 5(b) is a graph showing the temperature distribution in the manufacturing steps of the nitride semiconductor light-emitting device of Comparative Example 1 below.

首先,形成第1積層體6。藉由例如濺鍍法等於基板3上形成緩衝層5後,藉由例如MOCVD法於緩衝層5上依序形成基底層7、n型接觸層8及n型調變摻雜層9。基底層7、n型接觸層8及n型調變摻雜層9較佳於第1結晶成長裝置內成長。該等之層較佳在800℃以上1250℃以下成長,更佳在900℃以上1150℃以下成長。 First, the first layered body 6 is formed. After the buffer layer 5 is formed on the substrate 3 by sputtering, for example, the underlayer 7, the n-type contact layer 8, and the n-type modulation doping layer 9 are sequentially formed on the buffer layer 5 by, for example, MOCVD. The underlayer 7, the n-type contact layer 8, and the n-type modulation doped layer 9 are preferably grown in the first crystal growth apparatus. These layers are preferably grown at 800 ° C or higher and 1250 ° C or lower, more preferably at 900 ° C or higher and 1150 ° C or lower.

第1基底層71較佳以形成傾斜晶面71a之晶面成長模式成長。第2基底層75較佳以可嵌入傾斜晶面71a且形成平坦上表面75b之嵌入成長模式成長。具體而言,第1基底層71較佳於較第2基底層75更易3維成長之環境氣體下形成,更佳於與第2基底層75相比更高壓且低溫下形成。例如,第1基底層71較佳於500Torr之壓力下且990℃之溫度下形 成,第2基底層75較佳於200Torr之壓力下且1080℃之溫度下形成。 The first underlayer 71 preferably grows in a crystal growth mode in which the inclined crystal faces 71a are formed. The second base layer 75 is preferably grown in an embedded growth mode in which the inclined crystal face 71a can be embedded and the flat upper surface 75b is formed. Specifically, the first underlayer 71 is preferably formed under an ambient gas which is more easily grown in three dimensions than the second underlayer 75, and more preferably formed at a higher pressure and lower temperature than the second underlayer 75. For example, the first base layer 71 is preferably formed under a pressure of 500 Torr and a temperature of 990 ° C. The second underlayer 75 is preferably formed under a pressure of 200 Torr and at a temperature of 1080 °C.

形成第1積層體6後,使溫度暫時下降後(降溫步驟),再次提高溫度,形成第2積層體11。於降溫步驟中,較佳降低至較形成第2積層體11之溫度更低之溫度(例如500℃以下),更佳降低至室溫以上且100℃以下。「降溫步驟之溫度」意指基板3之溫度、及成膜裝置或成長裝置內之溫度中較高者之溫度。又,於降溫步驟後,較佳將第1積層體6暴露於大氣中。作為將第1積層體6暴露於大氣之方法,例舉例如自第1結晶成長裝置內取出第1積層體6後放入第2結晶成長裝置內之方法。再次提高溫度後,藉由例如MOCVD法等,於n型調變摻雜層9上依序形成V凹坑產生層10、多層構造體121及超晶格層122。 After the first layered body 6 is formed, the temperature is temporarily lowered (the temperature lowering step), and the temperature is raised again to form the second layered body 11. In the temperature lowering step, it is preferably lowered to a temperature lower than the temperature at which the second layered body 11 is formed (for example, 500 ° C or lower), and more preferably lowered to room temperature or higher and 100 ° C or lower. The "temperature of the cooling step" means the temperature of the substrate 3 and the temperature of the higher of the temperature in the film forming apparatus or the growth apparatus. Further, after the cooling step, the first layered body 6 is preferably exposed to the atmosphere. As a method of exposing the first layered body 6 to the atmosphere, for example, a method of taking out the first layered body 6 from the first crystal growth apparatus and putting it into the second crystal growth apparatus is exemplified. After the temperature is raised again, the V-pit generation layer 10, the multilayer structure 121, and the superlattice layer 122 are sequentially formed on the n-type modulation doped layer 9 by, for example, MOCVD.

V凹坑產生層10之成長溫度較佳低於第1積層體6之形成溫度,低於例如n型接觸層8或n型調變摻雜層9之成長溫度(形成第1n型氮化物半導體層之溫度)。如圖5(a)所示,發光層14係於低於第1積層體6之形成溫度之溫度形成。因此,若V凹坑產生層10之成長溫度低於n型接觸層8或n型調變摻雜層9之成長溫度(形成第1n型氮化物半導體層之溫度),則可縮短第2積層體11之形成後之降溫步驟所需之時間,因而可維持較高之處理量。又,與V凹坑產生層10之成長溫度為高溫之情形相比,附著於形成V凹坑產生層10之裝置之腔室之附著物量減少。藉此,維護用以形成第2積層體11之成膜裝置之頻率降低。基於該等原因,氮化物半導體發光元件1之生產性變高。基於維持較高之MQW發光層14之發光效率之觀點,V凹坑產生層10之成長溫度更佳為700℃以上,進而較佳在750℃以上。 The growth temperature of the V-pit generation layer 10 is preferably lower than the formation temperature of the first laminate body 6, lower than, for example, the growth temperature of the n-type contact layer 8 or the n-type modulation doping layer 9 (formation of the first n-type nitride semiconductor) The temperature of the layer). As shown in FIG. 5(a), the light-emitting layer 14 is formed at a temperature lower than the formation temperature of the first layered body 6. Therefore, if the growth temperature of the V-pit generation layer 10 is lower than the growth temperature of the n-type contact layer 8 or the n-type modulation doping layer 9 (the temperature at which the first n-type nitride semiconductor layer is formed), the second laminate can be shortened. The time required for the cooling step after the formation of the body 11 is such that a higher throughput can be maintained. Further, the amount of adhering matter adhering to the chamber of the apparatus for forming the V-pit generation layer 10 is reduced as compared with the case where the growth temperature of the V-pit generation layer 10 is high. Thereby, the frequency of the film forming apparatus for forming the second layered body 11 is lowered. For these reasons, the productivity of the nitride semiconductor light-emitting element 1 becomes high. The growth temperature of the V-pit generation layer 10 is more preferably 700 ° C or higher, and further preferably 750 ° C or higher, from the viewpoint of maintaining the luminous efficiency of the higher MQW light-emitting layer 14 .

亦可較n型調變摻雜層9提高n型摻雜物濃度且形成V凹坑產生層10。藉此,V凹坑產生層10之V凹坑形成效果增大。 It is also possible to increase the n-type dopant concentration and form the V-pit generation layer 10 than the n-type modulation doped layer 9. Thereby, the V-pit forming effect of the V-pit generation layer 10 is increased.

多層構造體121之成長溫度較佳為V凹坑產生層10之成長溫度以下,更佳與V凹坑產生層10之成長溫度相同。若多層構造體121之成 長溫度為V凹坑產生層10之成長溫度以下,則可增大V凹坑15之大小,因而ESD所引起之不良率變低。為了有效獲得該效果,多層構造體121之成長溫度更佳為600℃以上。 The growth temperature of the multilayer structure 121 is preferably not higher than the growth temperature of the V-pit generation layer 10, and more preferably the same as the growth temperature of the V-pit generation layer 10. If the multilayer structure 121 is formed When the long temperature is below the growth temperature of the V-pit generation layer 10, the size of the V-pit 15 can be increased, and the defective rate caused by ESD becomes low. In order to effectively obtain this effect, the growth temperature of the multilayer structure 121 is more preferably 600 ° C or higher.

超晶格層122之成長溫度較佳為V凹坑產生層10之成長溫度以下,更佳與V凹坑產生層10之成長溫度相同。若超晶格層122之成長溫度為V凹坑產生層10之成長溫度以下,則可進而縮短第2積層體11之形成後之降溫步驟所需之時間,因而可進而維持較高之處理量。又,維護用以形成超晶格層122之成膜裝置之頻率進而降低。基於該等原因,氮化物半導體發光元件1之生產性進而變高。除此之外,因可增大V凹坑15之大小,故ESD所引起之不良率變低。為了有效獲得該效果,超晶格層122之成長溫度更佳為600℃以上。 The growth temperature of the superlattice layer 122 is preferably lower than the growth temperature of the V-pit generation layer 10, and more preferably the same as the growth temperature of the V-pit generation layer 10. If the growth temperature of the superlattice layer 122 is less than the growth temperature of the V-pit layer 10, the time required for the temperature-lowering step after the formation of the second layered body 11 can be further shortened, thereby maintaining a higher throughput. . Moreover, the frequency of maintaining the film forming apparatus for forming the superlattice layer 122 is further reduced. For these reasons, the productivity of the nitride semiconductor light-emitting element 1 is further increased. In addition, since the size of the V-pit 15 can be increased, the defective rate caused by the ESD becomes low. In order to effectively obtain this effect, the growth temperature of the superlattice layer 122 is more preferably 600 ° C or higher.

繼而,於第2積層體11上依序形成發光層14、p型氮化物半導體層16、17、18。發光層14之形成方法並未特別限定,作為MQW構造之形成方法,可不特別限定地使用周知之方法。p型氮化物半導體層16、17、18之形成方法並未特別限定,作為p型氮化物半導體層之形成方法,可不特別限定地使用周知之方法。 Then, the light-emitting layer 14 and the p-type nitride semiconductor layers 16, 17, and 18 are sequentially formed on the second layered body 11. The method of forming the light-emitting layer 14 is not particularly limited. As a method of forming the MQW structure, a well-known method can be used without particular limitation. The method of forming the p-type nitride semiconductor layers 16, 17, and 18 is not particularly limited, and a known method can be used as the method of forming the p-type nitride semiconductor layer.

繼而,以露出n型接觸層8之一部分之方式,蝕刻p型氮化物半導體層16、17、18、發光層14、第2積層體11、n型調變摻雜層9及n型接觸層8。於藉由該蝕刻而露出之n型接觸層8之上表面上形成n側電極21。又,於p型氮化物半導體層18之上表面上依序積層透明電極23與p側電極25。其後,以覆蓋透明電極23與藉由上述蝕刻而露出之各層之側面之方式,形成透明保護膜27。藉此,獲得如圖1所示之氮化物半導體發光元件1。 Then, the p-type nitride semiconductor layers 16, 17, 18, the light-emitting layer 14, the second laminate 11, the n-type modulation doping layer 9, and the n-type contact layer are etched so as to expose a portion of the n-type contact layer 8. 8. An n-side electrode 21 is formed on the upper surface of the n-type contact layer 8 exposed by the etching. Further, the transparent electrode 23 and the p-side electrode 25 are sequentially laminated on the upper surface of the p-type nitride semiconductor layer 18. Thereafter, the transparent protective film 27 is formed so as to cover the transparent electrode 23 and the side faces of the respective layers exposed by the above etching. Thereby, the nitride semiconductor light-emitting element 1 shown in FIG. 1 is obtained.

另,亦可去除基板3。去除基板3之時序並未特別限定,可例如在形成第1積層體6之步驟後去除基板3。 Alternatively, the substrate 3 can be removed. The timing at which the substrate 3 is removed is not particularly limited, and the substrate 3 can be removed, for example, after the step of forming the first layered body 6.

亦可於第1結晶成長裝置內形成基底層7與n型接觸層8,且於第2 結晶成長裝置內形成n型調變摻雜層9與第2積層體11。然而,若於第1結晶成長裝置內形成基底層7、n型接觸層8及n型調變摻雜層9且於第2結晶成長裝置內形成第2積層體11,則可進而縮短第2積層體11之形成後之降溫步驟所需之時間。 The underlayer 7 and the n-type contact layer 8 may be formed in the first crystal growth apparatus, and may be in the second The n-type modulation doped layer 9 and the second layered body 11 are formed in the crystal growth apparatus. However, when the underlayer 7, the n-type contact layer 8, and the n-type modulation doped layer 9 are formed in the first crystal growth apparatus, and the second layered body 11 is formed in the second crystal growth apparatus, the second layer can be further shortened. The time required for the temperature-lowering step after the formation of the layered body 11.

如上說明,如圖1所示之氮化物半導體發光元件1係包含:包含1層以上之第1n型氮化物半導體層8、9之第1積層體6、包含與第1積層體6之第1面61相接之第2n型氮化物半導體層10之第2積層體11、設於第2積層體11上之發光層14、及設於發光層14上之p型氮化物半導體層16、17、18。第2n型氮化物半導體層10係於比形成第1n型氮化物半導體層之溫度(例如n型接觸層8或n型調變摻雜層9之成長溫度)低之溫度形成。藉此,如圖1所示之氮化物半導體發光元件1之生產性變高。 As described above, the nitride semiconductor light-emitting device 1 shown in FIG. 1 includes the first layered body 6 including the first n-type nitride semiconductor layers 8 and 9 of one or more layers, and the first layer 6 including the first layered body 6. The second layered body 11 of the second n-type nitride semiconductor layer 10 in contact with the surface 61, the light-emitting layer 14 provided on the second layered body 11, and the p-type nitride semiconductor layers 16 and 17 provided on the light-emitting layer 14. 18. The second n-type nitride semiconductor layer 10 is formed at a temperature lower than a temperature at which the first n-type nitride semiconductor layer is formed (for example, a growth temperature of the n-type contact layer 8 or the n-type modulation doping layer 9). Thereby, the productivity of the nitride semiconductor light-emitting element 1 shown in FIG. 1 becomes high.

第2積層體11較佳於第2n型氮化物半導體層10與發光層14之間,進而包含1層以上之第3n型氮化物半導體層121、122。第3n型氮化物半導體層121、122較佳於第2n型氮化物半導體層10之形成溫度以下之溫度形成。藉此,如圖1所示之氮化物半導體發光元件1之生產性進而變高。 The second layered body 11 is preferably provided between the second n-type nitride semiconductor layer 10 and the light-emitting layer 14, and further includes one or more third n-type nitride semiconductor layers 121 and 122. The third n-type nitride semiconductor layers 121 and 122 are preferably formed at a temperature lower than the formation temperature of the second n-type nitride semiconductor layer 10. Thereby, the productivity of the nitride semiconductor light-emitting element 1 shown in FIG. 1 is further increased.

構成第1積層體6之第1面61之半導體層較佳為非摻雜層。該情形時,第2n型氮化物半導體層10較佳為摻雜層。 The semiconductor layer constituting the first surface 61 of the first layered body 6 is preferably an undoped layer. In this case, the second n-type nitride semiconductor layer 10 is preferably a doped layer.

構成第1積層體6之第1面61之半導體層較佳為摻雜層。該情形時,第2n型氮化物半導體層10較佳為非摻雜層。 The semiconductor layer constituting the first surface 61 of the first layered body 6 is preferably a doped layer. In this case, the second n-type nitride semiconductor layer 10 is preferably an undoped layer.

本發明之氮化物半導體發光元件1之製造方法係至少包含:形成包含1層以上之第1n型氮化物半導體層8、9之第1積層體6之步驟、形成包含與第1積層體6之第1面61相接之第2n型氮化物半導體層10之第2積層體11之步驟、於第2積層體11上形成發光層14之步驟、及於發光層14上形成p型氮化物半導體層16、17、18之步驟。在形成第1積層體6之步驟後且形成第2積層體11之步驟前,進而包含降溫至較形成第2 積層體11之溫度更低之溫度之降溫步驟。藉此,可提高圖1所示之氮化物半導體發光元件1之生產性。 The method for producing the nitride semiconductor light-emitting device 1 of the present invention includes at least a step of forming the first layered body 6 including the first n-type nitride semiconductor layers 8 and 9 of one or more layers, and forming and including the first layered body 6. a step of forming the second layered body 11 of the second n-type nitride semiconductor layer 10 in contact with the first surface 61, a step of forming the light-emitting layer 14 on the second layered body 11, and forming a p-type nitride semiconductor on the light-emitting layer 14 The steps of layers 16, 17, 18. After the step of forming the first layered body 6 and before the step of forming the second layered body 11, the temperature is further lowered to form the second The step of lowering the temperature of the laminate 11 at a lower temperature. Thereby, the productivity of the nitride semiconductor light-emitting element 1 shown in Fig. 1 can be improved.

在形成第1積層體之步驟後且形成第2積層體之步驟前,較佳進而進行將第1積層體暴露於大氣之步驟。藉此,可進而提高圖1所示之氮化物半導體發光元件1之生產性。 It is preferable to further expose the first layered body to the atmosphere before the step of forming the first layered body and before the step of forming the second layered body. Thereby, the productivity of the nitride semiconductor light-emitting element 1 shown in FIG. 1 can be further improved.

[實施例] [Examples]

以下,例舉實施例更詳細地說明本發明,但本發明並未限定於此。 Hereinafter, the present invention will be described in more detail by way of examples, but the invention is not limited thereto.

<實施例1> <Example 1>

首先,準備包含100mm徑之藍寶石基板之晶圓。於晶圓之上表面,形成有凸部3a與凹部3b交替形成之凹凸形狀。 First, a wafer containing a 100 mm diameter sapphire substrate is prepared. On the upper surface of the wafer, a concavo-convex shape in which the convex portion 3a and the concave portion 3b are alternately formed is formed.

顯示對於晶圓之凹凸形狀之形成方法。首先,將規定有圖4所示之凸部3a之平面配置之遮罩設於晶圓上。其次,使用該遮罩乾蝕刻晶圓之上表面。經乾蝕刻之部分成為凹部3b,藉此,於晶圓之上表面上形成具有圖4所示之平面配置之凹部3b。藉此,凸部3a排列於晶圓之上表面之a(sub)軸方向(<11-20>方向),且分別配置於對於晶圓之上表面之a(sub)軸方向成+60°之傾斜之方向與對於晶圓之上表面之a(sub)軸方向成-60°之傾斜之方向(均為u方向)。凸部3a係於晶圓之上表面中,分別配置於圖4中以虛線顯示之假想三角形3t之頂點,且沿假想三角形3t之3邊之各邊方向週期性配置。 A method of forming the uneven shape of the wafer is displayed. First, a mask in which the planes of the convex portions 3a shown in Fig. 4 are arranged is placed on the wafer. Second, the mask is used to dry etch the upper surface of the wafer. The portion that is dry etched becomes the concave portion 3b, whereby the concave portion 3b having the planar arrangement shown in Fig. 4 is formed on the upper surface of the wafer. Thereby, the convex portions 3a are arranged in the a (sub)axis direction (<11-20> direction) of the upper surface of the wafer, and are respectively disposed at +60° to the a (sub) axis direction of the upper surface of the wafer. The direction of the tilt is in the direction of the inclination of -60° to the a(sub)axis direction of the upper surface of the wafer (both in the u direction). The convex portions 3a are arranged on the upper surface of the wafer, and are respectively arranged at the vertices of the imaginary triangles 3t shown by broken lines in FIG. 4, and are arranged periodically along the respective sides of the three sides of the imaginary triangle 3t.

晶圓之上表面中的凸部3a之形狀為圓形,該圓之直徑為1.2μm左右。鄰接之凸部3a之頂點之間隔(圖4所示之假想三角形3t之1邊)為2μm,凸部3a之高度為0.6μm左右。凸部3a具有圖1所示之側面視形狀,其前端帶圓。凹部3b具有圖1所示之側面視形狀。 The shape of the convex portion 3a in the upper surface of the wafer is circular, and the diameter of the circle is about 1.2 μm. The interval between the apexes of the adjacent convex portions 3a (one side of the imaginary triangle 3t shown in Fig. 4) is 2 μm, and the height of the convex portion 3a is about 0.6 μm. The convex portion 3a has a side view shape as shown in Fig. 1, and its front end is rounded. The recess 3b has a side view shape as shown in FIG.

凸部3a及凹部3b形成後,對晶圓之上表面進行RCA洗淨。將RCA洗淨後之晶圓放入腔室內,將N2、O2、及Ar導入該腔室內,並將腔 室內之晶圓加熱至650℃。藉由在N2、O2、及Ar之混合環境氣體下濺鍍Al靶材之反應性濺鍍法,而於形成有凸部3a及凹部3b之晶圓之上表面上形成包含AlON結晶之緩衝層5(厚度25nm)。形成之緩衝層5係包含於晶圓之上表面之法線方向伸長之柱狀結晶之集合體,即結晶粒之整齊柱狀結晶之集合體。 After the convex portion 3a and the concave portion 3b are formed, the upper surface of the wafer is subjected to RCA cleaning. The RCA-cleaned wafer was placed in a chamber, N 2 , O 2 , and Ar were introduced into the chamber, and the wafer in the chamber was heated to 650 ° C. The AlON crystal is formed on the upper surface of the wafer on which the convex portion 3a and the recess 3b are formed by a reactive sputtering method in which an Al target is sputtered under a mixed atmosphere of N 2 , O 2 , and Ar. Buffer layer 5 (thickness 25 nm). The buffer layer 5 formed is an aggregate of columnar crystals elongated in the normal direction on the upper surface of the wafer, that is, an aggregate of uniform crystal grains of crystal grains.

將已形成緩衝層5之晶圓放入第1MOCVD裝置內。於500Torr之壓力下,且990℃之溫度下,藉由MOCVD法使包含非摻雜GaN之第1基底層71結晶成長。又,於200Torr之壓力下,且1080℃之溫度下,藉由MOCVD法使包含非摻雜GaN之第2基底層75結晶成長。基底層7之厚度為4μm。其後,藉由MOCVD法使Si摻雜n型GaN層(n型接觸層8)結晶成長。n型接觸層8之厚度為3μm,n型接觸層8之n型摻雜物濃度為1×1019cm-3The wafer in which the buffer layer 5 has been formed is placed in the first MOCVD apparatus. The first underlayer 71 containing undoped GaN was crystal grown by MOCVD under a pressure of 500 Torr and a temperature of 990 °C. Further, the second underlayer 75 containing undoped GaN was crystal grown by MOCVD under a pressure of 200 Torr and a temperature of 1080 °C. The thickness of the base layer 7 was 4 μm. Thereafter, the Si-doped n-type GaN layer (n-type contact layer 8) is crystal grown by MOCVD. The n-type contact layer 8 has a thickness of 3 μm, and the n-type contact layer 8 has an n-type dopant concentration of 1 × 10 19 cm -3 .

將晶圓溫度設定成1081℃,且於n型接觸層8上藉由MOCVD法依序結晶成長厚度50nm之包含Si摻雜n型GaN之氮化物半導體層(n+層9A、n型摻雜物濃度:i×1019cm-3)、厚度87nm之包含非摻雜GaN之氮化物半導體層(n-層9B)、厚度50nm之包含Si摻雜n型GaN之氮化物半導體層(n+層9A、n型摻雜物濃度:1×1019cm-3)、及厚度87nm之包含非摻雜GaN之氮化物半導體層(n-層9B)。藉此,形成n型調變摻雜層9。 The wafer temperature was set to 1081 ° C, and a nitride semiconductor layer containing Si-doped n-type GaN having a thickness of 50 nm was grown on the n-type contact layer 8 by MOCVD (n + layer 9A, n-type doping) Material concentration: i × 10 19 cm -3 ), a nitride semiconductor layer (n - layer 9B) containing undoped GaN having a thickness of 87 nm, and a nitride semiconductor layer containing Si-doped n-type GaN having a thickness of 50 nm (n + Layer 9A, n-type dopant concentration: 1 × 10 19 cm -3 ), and a nitride semiconductor layer (n - layer 9B) containing undoped GaN having a thickness of 87 nm. Thereby, the n-type modulation doping layer 9 is formed.

形成n型調變摻雜層9後,晶圓溫度降低至80℃。在將晶圓自第1MOCVD裝置內暫時取出至大氣中後,放入第2MOCVD裝置內。將晶圓之溫度設定成801℃,且藉由MOCVD法結晶成長厚度25nm之Si摻雜GaN層(V凹坑產生層10)。經結晶成長之Si摻雜GaN層與n型調變摻雜層9之最上層相接,其n型摻雜物濃度為1×1019cm-3After the n-type modulation doping layer 9 is formed, the wafer temperature is lowered to 80 °C. After the wafer was temporarily taken out from the first MOCVD apparatus to the atmosphere, it was placed in a second MOCVD apparatus. The temperature of the wafer was set to 801 ° C, and a Si-doped GaN layer (V-pit generation layer 10) having a thickness of 25 nm was grown by MOCVD. The crystal-grown Si-doped GaN layer is in contact with the uppermost layer of the n-type modulation doped layer 9, and has an n-type dopant concentration of 1 × 10 19 cm -3 .

在將晶圓溫度保持於801℃之狀態下,使多層構造體121結晶成長。將厚度7nm之Si摻雜InGaN層、厚度30nm之Si摻雜GaN層、厚度 7nm之Si摻雜InGaN層、及厚度20nm之Si摻雜GaN層每2層交替積層。於構成多層構造體121之層之任一者中,亦將n型摻雜物濃度設為7×1017cm-3。將InGaN層之In組成比設為與後續成長之超晶格層122之窄帶隙層122B之In組成比相同。 The multilayer structure 121 is crystal grown in a state where the wafer temperature is maintained at 801 °C. A Si-doped InGaN layer having a thickness of 7 nm, a Si-doped GaN layer having a thickness of 30 nm, a Si-doped InGaN layer having a thickness of 7 nm, and a Si-doped GaN layer having a thickness of 20 nm were alternately laminated in two layers. In any of the layers constituting the multilayer structure 121, the n-type dopant concentration was also set to 7 × 10 17 cm -3 . The In composition ratio of the InGaN layer is set to be the same as the In composition ratio of the narrow band gap layer 122B of the subsequently grown superlattice layer 122.

在將晶圓之溫度保持於801℃之狀態下,使超晶格層122結晶成長。使包含Si摻雜GaN之寬帶隙層122A與包含Si摻雜InGaN之窄帶隙層122B交替成長20週期。各寬帶隙層122A之厚度為2.05nm。各窄帶隙層122B之厚度為2.05nm。各寬帶隙層122A之n型摻雜物濃度於寬帶隙層122A中位於發光層14側之5層中為1×1019cm-3,在較該5層更靠向第1積層體6側之層中為0cm-3(非摻雜)。各窄帶隙層122B之n型摻雜物濃度於窄帶隙層122B中位於發光層14側之5層中為1×1019cm-3,在較該5層更靠向第1積層體6側之層中為0cm-3(非摻雜)。發光層14之井層14W以藉由光致發光發出之光之波長成375nm之方式調整TMI(三甲基銦)之流量,因而各窄帶隙層122B之組成為InyGa1-yN(y=0.04)。 The superlattice layer 122 is crystal grown while maintaining the temperature of the wafer at 801 °C. The wide band gap layer 122A containing Si-doped GaN and the narrow band gap layer 122B containing Si-doped InGaN were alternately grown for 20 cycles. Each of the wide band gap layers 122A has a thickness of 2.05 nm. Each of the narrow band gap layers 122B has a thickness of 2.05 nm. The n-type dopant concentration of each of the wide band gap layers 122A is 1 × 10 19 cm -3 in 5 layers on the side of the light-emitting layer 14 in the wide-band gap layer 122A, and is closer to the side of the first layered body 6 than the 5 layers. The layer is 0 cm -3 (non-doped). The n-type dopant concentration of each of the narrow band gap layers 122B is 1 × 10 19 cm -3 in the five layers on the side of the light-emitting layer 14 in the narrow band gap layer 122B, and is closer to the side of the first layered body 6 than the five layers. The layer is 0 cm -3 (non-doped). The well layer 14W of the light-emitting layer 14 adjusts the flow rate of TMI (trimethyl indium) in such a manner that the wavelength of light emitted by photoluminescence becomes 375 nm, and thus the composition of each narrow band gap layer 122B is In y Ga 1-y N ( y=0.04).

將晶圓之溫度降至672℃,使發光層14結晶成長。使障壁層14A與包含InGaN之井層14W交替結晶成長,且使井層14W結晶成長8層。各障壁層14A之厚度為4.2nm。最初之障壁層14AZ及障壁層14A7之n型摻雜物濃度為4.3×1018cm-3,其他之障壁層14A6、14A5、...、14A1為非摻雜。 The temperature of the wafer was lowered to 672 ° C to crystallize the light-emitting layer 14 . The barrier layer 14A and the well layer 14W containing InGaN are alternately crystal grown, and the well layer 14W is crystal grown to have 8 layers. Each of the barrier layers 14A has a thickness of 4.2 nm. The initial barrier layer 14AZ and the barrier layer 14A7 have an n-type dopant concentration of 4.3 × 10 18 cm -3 , and the other barrier layers 14A6, 14A5, ..., 14A1 are undoped.

此處,最初之障壁層14AZ之厚度較佳大於障壁層14A7之厚度,亦可為例如5.05nm。藉此,可於超晶格層122中最靠近發光層14側形成窄帶隙層122B,且可維持未包含於超晶格層122之組數之寬帶隙層122A之作用。亦可將最初之障壁層14AZ之n型摻雜物濃度於最初之障壁層14AZ之上部(自最初之障壁層14AZ與井層14W8之界面離開1.55nm之區域)中設為1×1019cm-3,於最初之障壁層14AZ之下部(最初之障壁層14AZ之上部以外之部分)設為4.3×1818cm-3Here, the thickness of the first barrier layer 14AZ is preferably larger than the thickness of the barrier layer 14A7, and may be, for example, 5.05 nm. Thereby, the narrow band gap layer 122B can be formed closest to the light-emitting layer 14 side in the superlattice layer 122, and the wide band gap layer 122A not included in the number of superlattice layers 122 can be maintained. The n-type dopant concentration of the first barrier layer 14AZ may also be set to 1×10 19 cm in the upper portion of the first barrier layer 14AZ (from the region where the barrier layer 14AZ and the well layer 14W8 are separated by 1.55 nm). -3 , the portion below the first barrier layer 14AZ (the portion other than the upper portion of the first barrier layer 14AZ) is set to 4.3 × 18 18 cm -3 .

亦可僅於障壁層14A7之下部(自井層14W8與障壁層14A7之界面離開3.5nm之區域)摻雜n型摻雜物,且將障壁層14A7之上部(障壁層14A7之下部以外之部分)設為非摻雜。如此,藉由將障壁層14A7之上部設為非摻雜,可防止井層14W7之注入載子與n型摻雜之障壁層部分直接接觸。 Alternatively, the n-type dopant may be doped only in the lower portion of the barrier layer 14A7 (a region away from the interface of the well layer 14W8 and the barrier layer 14A7 by 3.5 nm), and the upper portion of the barrier layer 14A7 (the portion other than the lower portion of the barrier layer 14A7) ) set to non-doped. Thus, by making the upper portion of the barrier layer 14A7 non-doped, it is possible to prevent the injection carrier of the well layer 14W7 from coming into direct contact with the n-type doped barrier layer portion.

井層14W係使用氮氣作為載子氣體進行結晶成長之非摻雜InxGa1-xN層(x=0.20)。各井層14W之厚度為2.7nm。井層14W以使由光致發光發出之光之波長成為448nm之方式調整TMI之流量,且設定井層14W中的In之組成x。 The well layer 14W is a non-doped In x Ga 1-x N layer (x = 0.20) in which crystal growth is performed using nitrogen gas as a carrier gas. The thickness of each well layer 14W is 2.7 nm. The well layer 14W adjusts the flow rate of the TMI so that the wavelength of the light emitted by the photoluminescence becomes 448 nm, and sets the composition x of In in the well layer 14W.

於最上層之井層14W1上,使包含非摻雜之GaN之最後之障壁層14A0(厚度10nm)結晶成長。 On the uppermost well layer 14W1, the last barrier layer 14A0 (thickness 10 nm) containing undoped GaN was crystal grown.

將晶圓之溫度提高至1000℃,且於最後之障壁層14A0之上表面上,使p型Al0.18Ga0.82N層(p型氮化物半導體層16)、p型GaN層(p型氮化物半導體層17)及p型接觸層(p型氮化物半導體層18)依序結晶成長。 The temperature of the wafer is raised to 1000 ° C, and on the upper surface of the last barrier layer 14A0, a p-type Al 0.18 Ga 0.82 N layer (p-type nitride semiconductor layer 16), a p-type GaN layer (p-type nitride) is used. The semiconductor layer 17) and the p-type contact layer (p-type nitride semiconductor layer 18) are sequentially crystal grown.

於上述各層之結晶成長中,作為Ga之原料氣體係使用TMG(三甲基鎵),作為Al之原料氣體係使用TMA(三甲基鋁),作為In之原料氣體係使用TMI(三甲基銦),作為N之原料氣體係使用NH3。又,作為n型摻雜物的Si之原料氣體係使用SiH4,作為p型摻雜物的Mg之原料氣體係使用Cp2Mg。然而,原料氣體並未限定於上述氣體,只要為作為MOCVD用原料氣體而使用之氣體,則可無限定地使用。例如,可使用TEG(三乙基鎵)作為Ga之原料氣體,可使用TEA(三乙基鋁)作為Al之原料氣體,可使用TEI(三乙基銦)作為In之原料氣體,可使用DMHy(二甲基肼)等之有機氮化合物作為N之原料氣體,可使用Si2H6或有機Si等作為Si之原料氣體。 In the crystal growth of each of the above layers, TMG (trimethylgallium) is used as the raw material gas system of Ga, TMA (trimethylaluminum) is used as the raw material gas system of Al, and TMI (trimethylmethyl) is used as the raw material gas system of In. Indium), NH 3 is used as a raw material gas system for N. Further, SiH 4 is used as the raw material gas system of Si as the n-type dopant, and Cp 2 Mg is used as the raw material gas system of Mg as the p-type dopant. However, the material gas is not limited to the above gas, and may be used without limitation as long as it is a gas used as a material gas for MOCVD. For example, TEG (triethylgallium) can be used as a raw material gas of Ga, TEA (triethylaluminum) can be used as a raw material gas of Al, and TEI (triethylindium) can be used as a raw material gas of In, and DMHy can be used. As the raw material gas of N, an organic nitrogen compound such as (dimethyl hydrazine) can be used as a raw material gas of Si by using Si 2 H 6 or organic Si.

自第2MOCVD裝置內取出晶圓。其後,以露出n型接觸層8之一部分之方式,蝕刻p型接觸層(p型氮化物半導體層18)、p型GaN層(p型 氮化物半導體層17)、p型Al0.18Ga0.82N層(p型氮化物半導體層16)、發光層14、超晶格層122、多層構造體121、Si摻雜GaN層(V凹坑產生層10)、n型調變摻雜層9及n型接觸層8。於藉由該蝕刻露出之n型接觸層8之上表面上,形成包含Au之n側電極21。於p型接觸層18之上表面上,依序形成包含ITO之透明電極23與包含Au之p側電極25。以主要覆蓋透明電極23及因上述蝕刻而露出之各層之側面之方式,形成包含SiO2之透明保護膜27。其後,將晶圓分割成620×680μm尺寸之晶片。藉此獲得實施例1之氮化物半導體發光元件。 The wafer is taken out from the second MOCVD apparatus. Thereafter, the p-type contact layer (p-type nitride semiconductor layer 18), the p-type GaN layer (p-type nitride semiconductor layer 17), and p-type Al 0.18 Ga 0.82 are etched so as to expose a portion of the n-type contact layer 8. N-layer (p-type nitride semiconductor layer 16), light-emitting layer 14, superlattice layer 122, multilayer structure 121, Si-doped GaN layer (V-pit generation layer 10), n-type modulation doped layer 9 and N-type contact layer 8. On the upper surface of the n-type contact layer 8 exposed by the etching, an n-side electrode 21 containing Au is formed. On the upper surface of the p-type contact layer 18, a transparent electrode 23 containing ITO and a p-side electrode 25 containing Au are sequentially formed. A transparent protective film 27 containing SiO 2 is formed so as to mainly cover the transparent electrode 23 and the side faces of the respective layers exposed by the etching. Thereafter, the wafer was divided into wafers having a size of 620 × 680 μm. Thereby, the nitride semiconductor light-emitting element of Example 1 was obtained.

於本實施例中,Si摻雜GaN層(V凹坑產生層10)之形成以後之降溫步驟所需之時間縮短,藉此,可維持較高處理量。又,維護第2MOCVD裝置之頻率降低。 In the present embodiment, the time required for the temperature lowering step after the formation of the Si-doped GaN layer (V-pit generation layer 10) is shortened, whereby a high throughput can be maintained. Moreover, the frequency of maintaining the second MOCVD apparatus is lowered.

<實施例2> <Example 2>

與實施例1相同,於第1MOCVD裝置內形成基底層7與n型接觸層8後,將晶圓之溫度設定成1081℃且形成n型調變摻雜層9。於n型接觸層8上藉由MOCVD法依序結晶成長厚度50nm之包含Si摻雜n型GaN之氮化物半導體層(n+層9A,n型摻雜物濃度:1×1019cm-3)、厚度87nm之包含非摻雜GaN之氮化物半導體層(n-層9B)、及厚度50nm之包含Si摻雜n型GaN之氮化物半導體層(n+層9A,n型摻雜物濃度:1×1019cm-3)。 In the same manner as in the first embodiment, after the underlayer 7 and the n-type contact layer 8 were formed in the first MOCVD apparatus, the temperature of the wafer was set to 1081 ° C to form an n-type modulation doped layer 9. A nitride semiconductor layer containing Si-doped n-type GaN having a thickness of 50 nm is grown on the n-type contact layer 8 by MOCVD (n + layer 9A, n-type dopant concentration: 1 × 10 19 cm -3 ) a nitride semiconductor layer (n - layer 9B) containing undoped GaN having a thickness of 87 nm, and a nitride semiconductor layer containing Si-doped n-type GaN having a thickness of 50 nm (n + layer 9A, n-type dopant concentration) : 1 × 10 19 cm -3 ).

其次,將晶圓自第1MOCVD裝置內取出,放入第2MOCVD裝置內。將晶圓之溫度設定成801℃,且藉由MOCVD法結晶成長厚度10nm之非摻雜GaN層(n-層9BL)。其後,在將晶圓溫度保持於801℃之狀態下再與實施例1同樣,於第2MOCVD裝置內形成Si摻雜GaN層(V凹坑產生層10)、多層構造體121及超晶格層122。如此製造本實施例之氮化物半導體發光元件。於本實施例中,n-層9BL之形成以後之降溫步驟所需之時間亦縮短。 Next, the wafer was taken out from the first MOCVD apparatus and placed in the second MOCVD apparatus. The temperature of the wafer was set to 801 ° C, and an undoped GaN layer (n - layer 9BL) having a thickness of 10 nm was grown by MOCVD. Then, in the same manner as in the first embodiment, a Si-doped GaN layer (V-pit generation layer 10), a multilayer structure 121, and a superlattice are formed in the second MOCVD apparatus while maintaining the wafer temperature at 801 °C. Layer 122. The nitride semiconductor light-emitting element of the present embodiment was fabricated in this manner. In the present embodiment, the time required for the temperature lowering step after the formation of the n - layer 9BL is also shortened.

<實施例3> <Example 3>

除了將晶圓之溫度設為750℃使V凹坑產生層10、多層構造體121、及超晶格層122結晶成長外,根據上述實施例1所記述之方法製造本實施例之氮化物半導體發光元件。於本實施例中,Si摻雜GaN層(V凹坑產生層10)之形成以後之降溫步驟所需要之時間亦縮短。又,可維持較高之MQW發光層14之發光效率。 The nitride semiconductor of the present embodiment was fabricated according to the method described in the above first embodiment, except that the V-pit generation layer 10, the multilayer structure 121, and the superlattice layer 122 were crystallized by setting the temperature of the wafer to 750 °C. Light-emitting element. In the present embodiment, the time required for the temperature lowering step after the formation of the Si-doped GaN layer (V-pit generation layer 10) is also shortened. Moreover, the luminous efficiency of the higher MQW light-emitting layer 14 can be maintained.

<實施例4> <Example 4>

除了將晶圓之溫度設為750℃使多層構造體121及超晶格層122結晶成長外,根據上述實施例1所記述之方法製造本實施例之氮化物半導體發光元件。於本實施例中,Si摻雜GaN層(V凹坑產生層10)之形成以後之降溫步驟所需要之時間亦縮短。又,V凹坑15之大小變大。 The nitride semiconductor light-emitting device of the present example was produced by the method described in the above first embodiment except that the multilayer structure 121 and the superlattice layer 122 were crystallized by setting the temperature of the wafer to 750 °C. In the present embodiment, the time required for the temperature lowering step after the formation of the Si-doped GaN layer (V-pit generation layer 10) is also shortened. Further, the size of the V-pit 15 becomes large.

<實施例5> <Example 5>

除了將晶圓之溫度設為700℃使超晶格層122結晶成長外,根據上述實施例4所記述之方法製造本實施例之氮化物半導體發光元件。於本實施例中,Si摻雜GaN層(V凹坑產生層10)之形成以後之降溫步驟所需要之時間亦縮短。又,V凹坑15之大小變大。 The nitride semiconductor light-emitting device of the present example was produced by the method described in the above Example 4 except that the temperature of the wafer was set to 700 ° C to crystallize the superlattice layer 122. In the present embodiment, the time required for the temperature lowering step after the formation of the Si-doped GaN layer (V-pit generation layer 10) is also shortened. Further, the size of the V-pit 15 becomes large.

<實施例6> <Example 6>

於實施例6中除了第1積層體採用包含基板、緩衝層、基底層及n型接觸層之構成,第2積層體採用包含低摻雜n型氮化物半導體層、非摻雜氮化物半導體層及n型氮化物半導體層之構成,發光層之障壁層之組成採用AlGaN外,根據上述實施例1所記述之方法,製造氮化物半導體發光元件。即,於本實施例中,低摻雜n型氮化物半導體層相當於申請專利範圍中的「第2n型氮化物半導體層」。 In the sixth embodiment, the first laminate is composed of a substrate, a buffer layer, a base layer, and an n-type contact layer, and the second laminate includes a low-doped n-type nitride semiconductor layer and an undoped nitride semiconductor layer. In the configuration of the n-type nitride semiconductor layer, the composition of the barrier layer of the light-emitting layer was made of AlGaN, and a nitride semiconductor light-emitting device was produced according to the method described in the first embodiment. That is, in the present embodiment, the low-doped n-type nitride semiconductor layer corresponds to the "second n-type nitride semiconductor layer" in the patent application.

圖6係本實施例之氮化物半導體發光元件1之概略剖面圖。圖7係示意性顯示本實施例之氮化物半導體發光元件1之n型接觸層8至p型氮化物半導體層16中的帶隙能量Eg大小之能量圖。於圖6及圖7中,於包 含與上述實施例1相同組成之層,附註有與圖1中的符號相同之符號。又,於圖7中,於摻雜有n型摻雜物之層之右側附註小點且記述為「n」。 Fig. 6 is a schematic cross-sectional view showing the nitride semiconductor light-emitting device 1 of the present embodiment. Fig. 7 is an energy diagram schematically showing the magnitude of the band gap energy Eg in the n-type contact layer 8 to the p-type nitride semiconductor layer 16 of the nitride semiconductor light-emitting element 1 of the present embodiment. In Figure 6 and Figure 7, in the package The layer having the same composition as that of the above-described embodiment 1 is denoted by the same reference numeral as the symbol in Fig. 1. Further, in FIG. 7, a small dot is indicated on the right side of the layer doped with the n-type dopant and described as "n".

將形成有緩衝層5之晶圓放入第1MOCVD裝置內。於500Torr之壓力、990℃之溫度下,藉由MOCVD法結晶成長包含非摻雜GaN之第1基底層71。又,於200Torr之壓力、1080℃之溫度下,藉由MOCVD法結晶成長包含非摻雜GaN之第2基底層75。基底層7之厚度為3μm。其後,於1100℃之溫度下,藉由MOCVD法結晶成長Si摻雜n型GaN層(n型接觸層8)。n型接觸層8之厚度為4μm,n型接觸層8之n型摻雜物濃度為1×1019cm-3The wafer in which the buffer layer 5 is formed is placed in the first MOCVD apparatus. The first underlayer 71 containing undoped GaN was grown by MOCVD at a pressure of 500 Torr and a temperature of 990 °C. Further, the second underlayer 75 containing undoped GaN was grown by MOCVD at a pressure of 200 Torr and a temperature of 1080 °C. The thickness of the base layer 7 was 3 μm. Thereafter, a Si-doped n-type GaN layer (n-type contact layer 8) was grown by MOCVD at a temperature of 1,100 °C. The n-type contact layer 8 has a thickness of 4 μm, and the n-type contact layer 8 has an n-type dopant concentration of 1 × 10 19 cm -3 .

在形成n型接觸層8後,將晶圓溫度降低至500℃以下(若可能,則降至100℃以下)。在將晶圓自第1MOCVD裝置內暫時取出至大氣中後,放入第2MOCVD裝置內。將晶圓之溫度設定為870℃,藉由MOCVD法結晶成長厚度74nm之Si摻雜GaN層(低摻雜n型氮化物半導體層10A)。經結晶成長之低摻雜n型氮化物半導體層10A與n型接觸層8之最上層(第1積層體6之第1面61)相接,其n型摻雜物濃度為7×1017cm-3After the formation of the n-type contact layer 8, the wafer temperature is lowered to below 500 ° C (down to 100 ° C if possible). After the wafer was temporarily taken out from the first MOCVD apparatus to the atmosphere, it was placed in a second MOCVD apparatus. The temperature of the wafer was set to 870 ° C, and a Si-doped GaN layer (low-doped n-type nitride semiconductor layer 10A) having a thickness of 74 nm was grown by MOCVD. The crystallized low-doped n-type nitride semiconductor layer 10A is in contact with the uppermost layer of the n-type contact layer 8 (the first surface 61 of the first layered body 6), and has an n-type dopant concentration of 7 × 10 17 . Cm -3 .

在將晶圓溫度保持為870℃之狀態下,結晶成長厚度63.5nm之非摻雜GaN層(非摻雜氮化物半導體層123)。 The undoped GaN layer (undoped nitride semiconductor layer 123) having a thickness of 63.5 nm was grown in a state where the wafer temperature was maintained at 870 °C.

在將晶圓溫度保持為870℃之狀態下,結晶成長厚度20.5nm之Si摻雜AlGaN層(n型氮化物半導體層124)。經結晶成長之n型氮化物半導體層124係與發光層14相接之層,其n型摻雜物濃度係1×1019cm-3A Si-doped AlGaN layer (n-type nitride semiconductor layer 124) having a thickness of 20.5 nm was grown in a state where the wafer temperature was maintained at 870 °C. Through crystal growth of the contact layer 14 of n-type nitride-based semiconductor layer 124 and the light emitting layer, an n-type dopant concentration which is based 1 × 10 19 cm -3.

於本實施例中,將形成低摻雜n型氮化物半導體層10A、非摻雜氮化物半導體層123及n型氮化物半導體層124時之晶圓之溫度固定為870℃。然而,形成該等層時之晶圓之溫度只要於850~950℃之溫度範圍內則各可任意設定。例如,自提高第2積層體11之表面平坦性之觀 點而言,亦可將形成低摻雜n型氮化物半導體層10A及非摻雜氮化物半導體層123時之晶圓之溫度設為870℃,且將形成n型氮化物半導體層124時之晶圓之溫度設為900℃。又可將形成3層時之晶圓之溫度分別設定成不同之溫度。 In the present embodiment, the temperature of the wafer when the low-doped n-type nitride semiconductor layer 10A, the undoped nitride semiconductor layer 123, and the n-type nitride semiconductor layer 124 are formed is fixed at 870 °C. However, the temperature of the wafer when the layers are formed can be arbitrarily set as long as it is in the temperature range of 850 to 950 °C. For example, from the viewpoint of improving the surface flatness of the second layered body 11 In addition, the temperature of the wafer when the low-doped n-type nitride semiconductor layer 10A and the undoped nitride semiconductor layer 123 are formed may be 870 ° C, and the n-type nitride semiconductor layer 124 will be formed. The temperature of the wafer was set to 900 °C. Further, the temperatures of the wafers at the time of forming the three layers can be set to different temperatures.

<比較例1> <Comparative Example 1>

除了自第1MOCVD裝置內取出晶圓放入第2MOCVD裝置內後,將晶圓之溫度設為1100℃使n型調變摻雜層9結晶成長外,根據上述實施例1所記述之方法製造本比較例之氮化物半導體發光元件。於本比較例中,超晶格層122之形成後之降溫步驟所需要之時間變得比上述實施例1長。又,維護第2MOCVD裝置之頻率變得較上述實施例1高。 After the wafer was taken out from the first MOCVD apparatus and placed in the second MOCVD apparatus, the temperature of the wafer was set to 1,100 ° C, and the n-type modulation doping layer 9 was crystal grown. The method described in the above Example 1 was used. A nitride semiconductor light-emitting device of a comparative example. In the present comparative example, the time required for the temperature lowering step after the formation of the superlattice layer 122 becomes longer than that of the above-described first embodiment. Moreover, the frequency of maintaining the second MOCVD apparatus is higher than that of the first embodiment.

雖已對本發明之實施形態加以說明,但應認為本次揭示之實施形態之全部點僅為例示而非限制性者。本發明之範圍係由申請專利範圍表示,意欲包含與申請專利範圍等效及範圍內之所有變更。 The embodiments of the present invention have been described by way of example only. The scope of the present invention is defined by the scope of the claims, and is intended to be

1‧‧‧氮化物半導體發光元件 1‧‧‧Nitride semiconductor light-emitting elements

3‧‧‧基板 3‧‧‧Substrate

3a‧‧‧凸部 3a‧‧‧ convex

3b‧‧‧凹部 3b‧‧‧ recess

5‧‧‧緩衝層 5‧‧‧buffer layer

6‧‧‧第1積層體 6‧‧‧1st laminate

7‧‧‧基底層 7‧‧‧ basal layer

8‧‧‧n型接觸層 8‧‧‧n type contact layer

8A‧‧‧n型接觸層 8A‧‧‧n type contact layer

8B‧‧‧n型接觸層 8B‧‧‧n type contact layer

9‧‧‧n型調變摻雜層 9‧‧‧n type modulation doping layer

10‧‧‧V凹坑產生層 10‧‧‧V pit generation layer

11‧‧‧第2積層體 11‧‧‧2nd layered body

14‧‧‧發光層 14‧‧‧Lighting layer

15‧‧‧V凹坑 15‧‧‧V pit

16‧‧‧p型氮化物半導體層 16‧‧‧p-type nitride semiconductor layer

17‧‧‧p型氮化物半導體層 17‧‧‧p-type nitride semiconductor layer

18‧‧‧p型氮化物半導體層 18‧‧‧p-type nitride semiconductor layer

21‧‧‧n側電極 21‧‧‧n side electrode

23‧‧‧透明電極 23‧‧‧Transparent electrode

25‧‧‧p側電極 25‧‧‧p side electrode

27‧‧‧透明保護膜 27‧‧‧Transparent protective film

30‧‧‧台面部 30‧‧‧Face

61‧‧‧第1面 61‧‧‧1st

71‧‧‧第1基底層 71‧‧‧1st basal layer

71a‧‧‧傾斜晶面 71a‧‧‧Sloping facets

71b‧‧‧上表面 71b‧‧‧ upper surface

75‧‧‧第2基底層 75‧‧‧2nd basal layer

75b‧‧‧上表面 75b‧‧‧ upper surface

121‧‧‧多層構造體 121‧‧‧Multilayer structure

122‧‧‧超晶格層 122‧‧‧Superlattice layer

Claims (6)

一種氮化物半導體發光元件,其包含:第1積層體,其包含1層以上之第1n型氮化物半導體層;第2積層體,其包含與上述第1積層體之第1面相接之第2n型氮化物半導體層;發光層,其設於上述第2積層體上;及p型氮化物半導體層,其設於上述發光層上;且上述第2n型氮化物半導體層係以較形成上述第1n型氮化物半導體層之溫度更低之溫度形成。 A nitride semiconductor light-emitting device comprising: a first layered body including one or more first n-type nitride semiconductor layers; and a second layered body including a first surface of the first layered body a 2n-type nitride semiconductor layer; a light-emitting layer provided on the second layered body; and a p-type nitride semiconductor layer provided on the light-emitting layer; wherein the second n-type nitride semiconductor layer is formed The temperature of the first n-type nitride semiconductor layer is formed at a lower temperature. 如請求項1之氮化物半導體發光元件,其中上述第2積層體係於上述第2n型氮化物半導體層與上述發光層之間,進而包含1層以上之第3n型氮化物半導體層;且上述第3n型氮化物半導體層係以上述第2n型氮化物半導體層之形成溫度以下之溫度形成。 The nitride semiconductor light-emitting device according to claim 1, wherein the second build-up system further includes one or more third n-type nitride semiconductor layers between the second n-type nitride semiconductor layer and the light-emitting layer; The 3n-type nitride semiconductor layer is formed at a temperature equal to or lower than the formation temperature of the second n-type nitride semiconductor layer. 如請求項1或2之氮化物半導體發光元件,其中構成上述第1積層體之上述第1面之半導體層為非摻雜層;且上述第2n型氮化物半導體層係摻雜層。 The nitride semiconductor light-emitting device according to claim 1 or 2, wherein the semiconductor layer constituting the first surface of the first layered body is an undoped layer; and the second n-type nitride semiconductor layer is a doped layer. 如請求項1或2之氮化物半導體發光元件,其中構成上述第1積層體之上述第1面之半導體層為摻雜層;且上述第2n型氮化物半導體層為非摻雜層。 The nitride semiconductor light-emitting device according to claim 1 or 2, wherein the semiconductor layer constituting the first surface of the first layered body is a doped layer; and the second n-type nitride semiconductor layer is an undoped layer. 一種氮化物半導體發光元件之製造方法,其至少包含:形成包含1層以上之第1n型氮化物半導體層之第1積層體之步驟;形成包含與上述第1積層體之第1面相接之第2n型氮化物半導體層之第2積層體之步驟; 於上述第2積層體上形成發光層之步驟;及於上述發光層上形成p型氮化物半導體層之步驟;且以較形成上述第1n型氮化物半導體層之溫度更低之溫度,形成上述第2n型氮化物半導體層;在形成上述第1積層體之步驟後且形成上述第2積層體之步驟前,進而包含降溫至較形成上述第2積層體之溫度更低之溫度之降溫步驟。 A method for producing a nitride semiconductor light-emitting device, comprising: a step of forming a first layered body including a first n-type nitride semiconductor layer of one or more layers; and forming a first surface of the first layered body a step of forming a second layered body of the second n-type nitride semiconductor layer; a step of forming a light-emitting layer on the second layered body; and a step of forming a p-type nitride semiconductor layer on the light-emitting layer; and forming the above temperature at a temperature lower than a temperature at which the first n-type nitride semiconductor layer is formed The second n-type nitride semiconductor layer further includes a temperature lowering step of lowering the temperature to a temperature lower than a temperature at which the second layered body is formed, after the step of forming the first layered body and forming the second layered body. 如請求項5之氮化物半導體發光元件之製造方法,其中在上述降溫步驟後且形成上述第2積層體之步驟前,進而包含將上述第1積層體暴露於大氣中之步驟。 The method for producing a nitride semiconductor light-emitting device according to claim 5, further comprising the step of exposing the first layered body to the atmosphere before the step of forming the second layered body after the step of lowering the temperature.
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