TW201029233A - Semiconductor light emitting element and method for manufacturing same - Google Patents

Semiconductor light emitting element and method for manufacturing same Download PDF

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Publication number
TW201029233A
TW201029233A TW98140795A TW98140795A TW201029233A TW 201029233 A TW201029233 A TW 201029233A TW 98140795 A TW98140795 A TW 98140795A TW 98140795 A TW98140795 A TW 98140795A TW 201029233 A TW201029233 A TW 201029233A
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Taiwan
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layer
refractive index
substrate
gan
semiconductor light
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TW98140795A
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Chinese (zh)
Inventor
Kazuyuki Tadatomo
Narihito Okada
Yoshimi Watabe
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Univ Yamaguchi
Choshu Industry Co Ltd
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Publication of TW201029233A publication Critical patent/TW201029233A/en

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/005Processes
    • H01L33/0062Processes for devices with an active region comprising only III-V compounds
    • H01L33/0066Processes for devices with an active region comprising only III-V compounds with a substrate not being a III-V compound
    • H01L33/007Processes for devices with an active region comprising only III-V compounds with a substrate not being a III-V compound comprising nitride compounds
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L33/02Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies
    • H01L33/12Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor bodies with a stress relaxation structure, e.g. buffer layer

Abstract

A semiconductor light emitting element (10) includes: a substrate (11) having a surface which enables GaN crystal growth; a mask layer (12) having a surface which is arranged to cover the surface of the substrate (11) but has an opening (12a) where the surface of the substrate (11) is partially exposed and which disables GaN crystal growth; and a GaN layer (13) arranged to cover the mask layer (12) and the surface of the substrate (11) exposed through the opening (12a) of the mask layer (12). The mask layer (12) has a refraction index greater than that of SiO2 and smaller than that of the GaN layer (13).

Description

201029233 六、發明說明: 【發明所屬之技術領域】 本發明係有關半導體發光元件及其製造方法。 【先前技術】 作為發光二極體(LED)或半導體雷射(LD)等半導體發 光元件,具有在基板上設置GaN等半導體層的結構之元件 已經量產化。 非專利文獻1中公開了如下技術:在藍寶石基板上設 置以Si〇2%&gt;成之光罩層,在該光罩層使藍寶石基板露出地 來形成條紋狀溝,經由以從溝所露出的藍寳石基板為起點 使才于GaN結晶成長將能夠降低差排(disi〇cati〇n)缺陷,並 且,經由此將能夠提高發光輸出功率(外部量子效率)。 非專利文獻 1 ·· K.Hoshino,T.Murata,M.Araki,and K.Tadatomo,phys.stat.sol.(c)5,No.9,3060-3062(2008) 【發明内容】 本發明之半導體發光元件包括:基板、其具有GaN結 晶能夠成長的表面,光罩層、其被設成覆蓋上述基板的表 面而形成有使得該基板的表面部分露出的開口並具有GaN 結晶無法成長的表面,以及GaN層、其覆蓋上述光罩層和 從該光罩層的開口露出的上述基板的表面;上述光罩層之 折射率(refractive index)大於Si〇2之折射率且小於上述GaN 層之折射率。 本發明的半導體發光元件之製造方法,係一種製造如 下半導體發光兀件之方法,該半導體發光元件包括:基板、 其具有GaN結晶能夠唪長之表面,光罩層、其被設成覆蓋 上述基板的表面而形成有使得該基板的表面部分露出的開 3/22 201029233 口並具有GaN的結絲法成長之表面,以及⑽層、其覆 蓋上述光單層及從該光罩層的開口露出、 面;根據αω法沉積形成光!l層賴’使得光罩層之折= 率大於Si〇2之折射率且小於GaN層之折射率。 在半導體發光元件,由於起因於元件内外的折射率差 異所造成的全反射角之限制’發出的光之大部分被封閉於 元件内部。制是在1化物料體發光元件的情況,基板(譬 如在藍寶石基板、對波長410nm的光之折射率為!㈣與在 其上成長之GaN層(對波長稱nm的光之折射率為2 5句的 折射率差異所造成的全反射角之限制,發出的光之大部分❹ 被封閉於折射率高的GaN層。根據本發明,由於在光罩層 形成了開口使得GaN層的在基板-侧的界面具有凹凸在 ⑽相人㈣其細触紐麵反㈣在界面反射, 其結果,其光的-部分從全反射角⑽al灿㈣⑽妨㈣的 限制解放,而不會被封閉於GaN層、進而也不會被封閉於 几件内部而提高了出射到元件外部的概率,將能夠實現高 。並且’可以經由使得光單層的折射率大於叫 斤射率且小於GaN層的折射率能夠實現高取光率。在高折❹ 射率的GaN層令傳播(propagati〇n)的光,於光罩層一部分反 ^而-部分折射入射到光罩層内。入射到光罩層内的光在 土板界面反射或是折射出到基板—側。此一反射和折射的 比率依存於光罩層的折射率。光罩層的折射率小於基板的 =射,時’人射光罩層内之光被封閉在光罩層内的比例 南,若是與基板的折射率變得相同,入射到光罩層内之光 . 將會效率良好地出射到基板一側,出到元件外部。若是光 罩層的折射率大於基板的折射率,職GaN層的折射率差 4/22 201029233 異將變小,反射或折射光罩層本身的光之效果將變小。並 且:若是與GaN層的折射率變得相同,對於光而言將不會 感受到光罩層,而成為與平坦基板時同樣的取 【實施方式】 以下,按照附圖詳細說明該實施方式。 (半導體發光元件) 圖1示出本實施方式之半導體發光元件1〇。 實施方式1 +之相關半導體發光元件10,基板11的表 ❹ 自為光罩層12所覆蓋,並且在其上依序堆#有u_GaN層 13(故意未添加雜質的層)、n型GaN | 14、多重量子井層 15、p型AlGaN層16、以及卩型祕層17的各半導體層, 在結構上於p型GaN層π上面設有p型電極19、並在以 I虫刻露出的η型GaN層14上面設有n型電極18,而孽如 作為發光二極體等來使用。 作為基板1卜關舉㈣如典_藍寶石基板(Αΐ2〇3 金剛石(C〇mndUm)結構的單結晶基板),其他還能夠舉出 ^ Zn〇基板、SlC基板等。基板1卜譬如在發光元件的狀態 被形成為矩形,縱橫分別為細〜誦^,厚度為5〇〜3〇〇 // m。 基板11的表面被構成為GaN的結晶能夠成長。藍寶石 基板的情況時,其表面可以是a面印㈣丨面〉、。面&lt;{_} 面&gt;、m面〈{l-ioow〉、或是^面^卜卿面〉,並且也可 以疋其他面方位的結晶面。並且,a面、c面、和瓜面的面 方位互相垂直。 基板11之折射率宜為大於Si02之折射率並小於後述 的u-GaN層13之折射率,具體而言,宜為M5〜2.54, L45 5/22 201029233 〜2·2則更為理想。於此,在本中請案之“折射率,,為相對 於波長405nm至41〇nm的光之值β藍寶石基板的折射率為 1.76 〇 作為光罩層12之構成材料,能夠舉出譬如:GaN的結 晶無法成長的氮氧化石夕(Si〇XNY:〇&lt;x&lt;2,〇&lt;Y&lt;4/3)、氧化= (:l〇i、氧化矽鋁(A1Si〇)、氤化硼_ ’氮化硼矽_Ν) 為理想罩層丨2之厚度宜為G.1〜5.G//m,G.2〜3,()_則更 n罩層12形成有使基板u的表面部分露出之開口 為ri2a,譬如能夠舉出溝、孔等。開口❿能 又置為複數個’具體而言,譬如使其為溝隔著間隔平行 之結構,或是使其為_成為縱橫的格子結構, 孔離触地複舰設之賴。域為使溝隔著間 伸方向可,並且,溝的延 伸方向可从基板11的表_任-财向。 :2的表面被構成為⑽的結晶無法成長。 13祕Ί玄,2的折射率大於⑽折射率並小於u_⑽層 13的折射率。具體而古,也 σ先罩層12的折射率大於1.45並 小於2.54, 1.45〜2.2則更為理想。 卫 並且^層Γ的折射率,可以是小於基板11的折射率, 11的折射ΐ相ΐ於基板11的折射率’進而也可以是與基板 m 的折射率也可以是在厚度 罩—層12的折射率在厚度方向的從』 p 土 侧連續性階段性地逐漸變小來變化之 201029233 變大來《Nb之2 t 難料触性地逐蠏 變大來之、、,。構,並且,鮮層12崎射率 上具有1個乃至複數的峰值變化之結構。 ^ u GaN層13的構成材料是無推雜 :„一__被構成為使得基板:= -aN心曰曰能夠成長,另一方面使得光翠層u的表面201029233 6. Description of the Invention: TECHNICAL FIELD OF THE INVENTION The present invention relates to a semiconductor light-emitting element and a method of fabricating the same. [Prior Art] As a semiconductor light-emitting device such as a light-emitting diode (LED) or a semiconductor laser (LD), an element having a structure in which a semiconductor layer such as GaN is provided on a substrate has been mass-produced. Non-Patent Document 1 discloses a technique in which a mask layer made of Si〇2% is provided on a sapphire substrate, and a sapphire substrate is exposed in the mask layer to form a stripe-shaped groove, which is exposed from the groove. The sapphire substrate is a starting point for crystal growth of GaN, which is capable of reducing the defect (disi〇cati〇n), and by this, the light-emitting output power (external quantum efficiency) can be improved. Non-Patent Document 1 · K. Hoshino, T. Murata, M. Araki, and K. Tadatomo, phys. stat. sol. (c) 5, No. 9, 3060-3062 (2008) [Invention] The semiconductor light-emitting device includes a substrate having a surface on which GaN crystal can grow, a photomask layer provided to cover a surface of the substrate, and an opening in which a surface portion of the substrate is exposed and having a surface in which GaN crystal cannot grow And a GaN layer covering the surface of the photomask layer and the substrate exposed from the opening of the photomask layer; the refractive index of the photomask layer is greater than the refractive index of Si〇2 and smaller than the GaN layer Refractive index. A method of manufacturing a semiconductor light-emitting device according to the present invention is a method of manufacturing a semiconductor light-emitting device comprising: a substrate having a surface on which a GaN crystal can be elongated, and a photomask layer provided to cover the substrate a surface on which a surface portion of the substrate is exposed, a surface of the opening 3/22 201029233 having a GaN wire growth method, and a (10) layer covering the light monolayer and exposing from the opening of the photomask layer, Surface; deposited according to the αω method to form light! The layer layer is such that the refractive index of the photomask layer is greater than the refractive index of Si〇2 and smaller than the refractive index of the GaN layer. In the semiconductor light-emitting element, most of the light emitted by the limitation of the total reflection angle due to the difference in refractive index between the inside and the outside of the element is enclosed inside the element. In the case of a material light-emitting element, the substrate (for example, a sapphire substrate, a refractive index for light having a wavelength of 410 nm is (4) and a GaN layer grown thereon (refractive index of light for a wavelength of nm is 2) The limitation of the total reflection angle caused by the difference in refractive index of the five sentences, most of the emitted light is blocked by the GaN layer having a high refractive index. According to the present invention, the GaN layer is formed on the substrate by forming an opening in the photomask layer. - The side interface has a bump at (10) phase (4) its fine touch button reverse (four) at the interface reflection, and as a result, its light-portion is liberated from the limit of total reflection angle (10)alcan(4)(10)(4) without being enclosed in GaN The layer, and thus the number of layers, which are not enclosed in several parts, increases the probability of exiting to the outside of the component, and can be made high. And can be made such that the refractive index of the optical single layer is greater than the refractive index and smaller than the refractive index of the GaN layer. A high light extraction rate can be achieved. The GaN layer at a high refractive index causes propagtiated light to be partially refracted into the reticle layer and incident on the reticle layer. Light reflects or refracts at the interface of the soil Substrate-side. The ratio of this reflection and refraction depends on the refractive index of the mask layer. The refractive index of the mask layer is smaller than that of the substrate, and the ratio of the light in the human mask layer is enclosed in the mask layer. In the south, if the refractive index of the substrate becomes the same, the light incident into the mask layer will be efficiently emitted to the side of the substrate and out to the outside of the device. If the refractive index of the mask layer is greater than the refractive index of the substrate, The refractive index difference of the GaN layer is 4/22 201029233. The effect will be smaller, and the effect of reflecting or refracting the light of the mask layer itself will be smaller. And if the refractive index of the GaN layer becomes the same, it will not be for light. The present embodiment will be described in detail with reference to the accompanying drawings. (Semiconductor Light Emitting Element) FIG. 1 shows a semiconductor light emitting element 1A of the present embodiment. Embodiment 1 + related semiconductor light-emitting element 10, the surface of the substrate 11 is covered by the photomask layer 12, and sequentially stacked thereon with a u_GaN layer 13 (deliberately no impurity-added layer), n-type GaN | 14. Multiple quantum well layers 15, p Each of the semiconductor layers of the AlGaN layer 16 and the germanium type secret layer 17 is provided with a p-type electrode 19 on the p-type GaN layer π and an n-type on the n-type GaN layer 14 exposed by the insect. The electrode 18 is used as a light-emitting diode, etc. As the substrate 1 (4) 如 _ sapphire substrate (a single crystal substrate of a 〇 2 〇 3 diamond (C〇mndUm) structure), the other can also be Zn 〇 A substrate, an S1C substrate, etc. The substrate 1 is formed into a rectangular shape in a state of a light-emitting element, and has a thickness of 5 Å to 3 Å/m, respectively, in a vertical and horizontal direction. The surface of the substrate 11 is formed into a crystal of GaN. In the case of a sapphire substrate, the surface of the sapphire substrate can be a faceted (four) faceted surface. The face &lt;{_} face&gt;, the m-face <{l-ioow>, or the ^ face^b-face>, and may also be a crystal face of other face orientations. Further, the plane faces of the a face, the c face, and the melon face are perpendicular to each other. The refractive index of the substrate 11 is preferably larger than the refractive index of SiO 2 and smaller than the refractive index of the u-GaN layer 13 to be described later. Specifically, it is preferably M5 to 2.54, and L45 5/22 201029233 to 2·2 is more preferable. Here, the "refractive index" of the present invention is a value of light of 407 nm to 41 〇 nm with respect to the wavelength of the sapphire substrate of 1.76 〇 as a constituent material of the mask layer 12, for example, Nitrous oxide which cannot grow crystals of GaN (Si〇XNY: 〇&lt;x&lt;2, 〇&lt;Y&lt;4/3), oxidation = (:l〇i, yttrium aluminum oxide (A1Si〇), bismuth Boron _ 'boron nitride 矽 Ν 为) is the ideal cover layer 丨 2 thickness is preferably G.1~5.G / / m, G. 2 ~ 3, () _ then n cover layer 12 is formed with the substrate The opening of the surface portion of u is ri2a, for example, a groove, a hole, etc. The opening ❿ can be set to a plurality of 'specifically, for example, it is a structure in which the grooves are parallel to each other, or is made _ It is a lattice structure of vertical and horizontal, and the hole is located away from the ground. The domain is such that the groove is interposed between the grooves, and the direction of the groove can be extended from the surface of the substrate 11. The crystal composed of (10) cannot grow. 13 The refractive index of 2 is greater than (10) and less than the refractive index of layer u of (10) layer 13. Specifically, the refractive index of σ first layer 12 is greater than 1.45 and less than 2.54, 1.45. ~2 .2 is more desirable. The refractive index of the layer may be smaller than the refractive index of the substrate 11, the refractive index of 11 is opposite to the refractive index of the substrate 11 and may also be the refractive index with the substrate m. In the thick cover-layer 12, the refractive index in the thickness direction gradually decreases from the s-p soil side gradually, and the change becomes 201029233, and the Nb 2 t is unpredictable. And, the structure of the fresh layer 12 has a structure of peak change of one or even plural. ^ u The constituent material of the GaN layer 13 is non-inductive: „一__ is configured such that the substrate:= -aN heart can grow, on the other hand, make the surface of the light layer u

=的結晶無法成長’因此,u伽層13是一層以從^ ^2的開口 12a露出之基板㈣表面為起點⑽結晶成 :所形成。u-GaN々13的厚度譬如為2〜2〇_。…⑽ 二13的婦枝2.54。再者,為結晶成長起點的基板^ 的表面和u-GaN層13之間設置厚度為2〇〜3〇nm左 GaN的低溫緩衝層。 如上述般,若是根據光罩層12及u_GaN層13之結構, 在光罩層12所形成之開口 12a的部分GaN在基板U表面 的法線方向上結晶成長而形成層,另一方面,開口以以 外的光罩層12的部分,經由GaN在橫方向結晶成長凝結而 形成覆蓋該部分的層。經由此’在⑴⑽層13的表面所呈 現的差排缺陷密度將會降低,而能夠提高外部量子效率。 並且,一般地,在半導體發光元件,由於元件内外折 射率的差異所造成的全反射角的限制,發光的大部分的光 被封閉於元件⑽’制是在譬如具有藍賨石基板和在其 上成長之GaN層的氮化物半導體發光元件之情況下,起因 ,折射率的差異所造成的全反射角的限制,使得發光的大 4分的光被封閉在〇aN層。然而,如上所述,若是根據光 罩層12及u-GaN層13之結構,由於在光罩層12形成了開 7/22 201029233 口 12a’u-GaN層13的在基板11 —側的界面具有凹凸,在 u-GaN層13料面入射的光於種種的反射角反射,其結 果’其光的-部分從全反射角的限制中解放,提高了不被 封閉於GaN層内部、進而不被封閉於元件而出射到内部元 件外部的概率’而能夠獲得高的取光率。並且,光罩層12 的折射率大於Si〇2折射率並小於〜⑽層13的折射率, 將能夠獲得更為顯著的效果。 具艚而言,在本實施方式的半導體發光元件1〇,如果The crystal of = cannot grow. Therefore, the u-gayer layer 13 is formed by crystallizing from the surface (10) of the substrate (4) exposed from the opening 12a of the ^2. The thickness of the u-GaN germanium 13 is, for example, 2 to 2 Å. ...(10) Two women's branches of 2.5. Further, a low temperature buffer layer having a thickness of 2 〇 to 3 〇 nm left GaN is provided between the surface of the substrate ^ which is the starting point of the crystal growth and the u-GaN layer 13. As described above, according to the configuration of the mask layer 12 and the u_GaN layer 13, a portion of the GaN in the opening 12a formed in the mask layer 12 crystallizes in the normal direction of the surface of the substrate U to form a layer, and on the other hand, the opening is formed. The portion of the mask layer 12 other than the layer is crystallized and grown in the lateral direction via GaN to form a layer covering the portion. The difference in the defect density exhibited by the surface of the (1) (10) layer 13 by this will be lowered, and the external quantum efficiency can be improved. Moreover, in general, in a semiconductor light-emitting element, due to the limitation of the total reflection angle caused by the difference in refractive index between the inside and the outside of the element, most of the light of the light is enclosed in the element (10)', for example, having a bluestone substrate and In the case of the nitride semiconductor light-emitting element of the grown GaN layer, the cause of the total reflection angle caused by the difference in refractive index is limited, so that the light of the light-emitting 4 minute is enclosed in the 〇aN layer. However, as described above, according to the structure of the photomask layer 12 and the u-GaN layer 13, the interface on the substrate 11 side of the 12a'u-GaN layer 13 is formed in the photomask layer 12 by the opening 7/22 201029233. With irregularities, the light incident on the material plane of the u-GaN layer 13 is reflected by various reflection angles, and as a result, the portion of the light is liberated from the limitation of the total reflection angle, and is improved not to be enclosed inside the GaN layer, and thus not A high rate of light extraction can be obtained by the probability of being enclosed by the element and emerging outside the internal element. Further, the refractive index of the photomask layer 12 is larger than the refractive index of Si〇2 and smaller than the refractive index of the layer (~10), and a more remarkable effect can be obtained. In the case of the semiconductor light-emitting device 1 of the present embodiment,

將基板11為藍寶石基板而設置了魏切的光罩層12,在 向發光中心波長為4G5nm的發Μ件中輸人2()mA的電流 時的輸出功率為加〜29.0mW而外部量子效率為似〜 47.4%。再者’在平坦的藍寶石基板上不設置光罩層而設置 u·㈣層的同等半導體發光元件中,輸出功率為2〇.7禮而 子效率為33跳,在平坦的藍寶石基板上設置Si02 在其上設置u_⑽層的同等半導體發光元件,輸 出功率為23.5mW而外部量子效率為38 4%。The substrate 11 is a sapphire substrate, and the mask layer 12 of the Weiche is provided. When a current of 2 (? mA) is input to a hairpin having an emission center wavelength of 4 G5 nm, the output power is ~29.0 mW and the external quantum efficiency is increased. Like ~ 47.4%. Furthermore, in an equivalent semiconductor light-emitting device in which a u·(four) layer is provided without a photomask layer on a flat sapphire substrate, the output power is 2 〇.7 and the sub-efficiency is 33 hops, and SiO 2 is provided on a flat sapphire substrate. An equivalent semiconductor light-emitting device having a u_(10) layer provided thereon has an output of 23.5 mW and an external quantum efficiency of 38 4%.

n^GaN層Μ的構成材料為摻雜了 n型雜質(d〇pant) 之GaN。作為n型雜質’能夠舉出譬如Si、Ge等。n型雜 質的濃度譬如為1.0Χ10Π〜2〇xl〇17/cm3。&quot;祕層Μ, == 一層構成,也可以是用η型雜質的種類和濃度 不相同的複數層加以構成。n型⑽们4厚度譬 〜 10/zm。 重ί子井層15具有井層15M°障壁層15b的交替堆 曼結構。井層15a和障壁層15b的層數譬如是5〜15層。 =井層以的構成材料,能舉出譬如城祕㈣邏 等。井層15a的厚度譬如是1〜2〇nm。 8/22 201029233 作為障壁層15b的構成材料,能舉出譬如、 InGaN(大於井層的帶隙)等。障壁層i5b的厚^譬如是5〜 20nm ° p型AlGaN層16的構成材料為摻雜了 p型雜質之The constituent material of the n^GaN layer is GaN doped with an n-type impurity (d〇pant). Examples of the n-type impurity 'e" include Si, Ge, and the like. The concentration of the n-type impurity is, for example, 1.0 Χ 10 Π 2 〇 x 〇 17 / cm 3 . &quot;secret layer Μ, == One layer composition, or it may be composed of a plurality of layers of different types and concentrations of η-type impurities. n type (10) 4 thickness 譬 ~ 10 / zm. The heavy well layer 15 has an alternating stack structure of the 15M° barrier layer 15b of the well layer. The number of layers of the well layer 15a and the barrier layer 15b is, for example, 5 to 15 layers. = The composition of the well layer can be exemplified by the city secret (four) logic. The thickness of the well layer 15a is, for example, 1 to 2 〇 nm. 8/22 201029233 As a constituent material of the barrier layer 15b, for example, InGaN (greater than the band gap of the well layer) can be cited. The thickness of the barrier layer i5b is 5 to 20 nm. The constituent material of the p-type AlGaN layer 16 is doped with p-type impurities.

AlGaN。A1N的混晶比從〇.〇5〜0.3來適當選擇。作為p型 雜質,能舉出譬如Mg、Cd等。p型時由於為受體能階高, 雜質濃度和自由空穴濃度相差很大。因此,有關p型以用 空穴效應測量的自由空穴濃度為評價指標。自由空穴濃 ❹ 度,譬如是〜5xl017/cm3。p型AlGaN層16的厚 度譬如是10〜30mn。 p型GaN層17的構成材料為摻雜了 p型雜質的(}必。 作為P型雜質,與ρ型GaN同樣,能夠舉出譬如]^^、(::(1 等。用空穴效應測量的自由空穴濃度,譬如是2 〇χι〇ΐ7〜 10xl017/cm3。P型GaN層17也可以是用單一層構成,並 且,也可以用P型雜質的種類和濃度不相同的複數層加以 構成。p型GaN層17的厚度譬如是50〜2〇〇nm。 Φ 作為11型電極18的構成電極材料,能夠舉出譬如AlGaN. The mixed crystal ratio of A1N is appropriately selected from 〇.〇5 to 0.3. As the p-type impurity, for example, Mg, Cd or the like can be mentioned. In the p-type, since the acceptor level is high, the impurity concentration and the free hole concentration differ greatly. Therefore, the free hole concentration measured by the cavitation with respect to the p-type is used as an evaluation index. The free hole concentration is, for example, ~5xl017/cm3. The thickness of the p-type AlGaN layer 16 is, for example, 10 to 30 nm. The constituent material of the p-type GaN layer 17 is doped with a p-type impurity. As a p-type impurity, as in the case of the p-type GaN, for example, ^^, (:: 1, etc., a hole effect is used. The measured free hole concentration is, for example, 2 〇χι〇ΐ7 to 10xl017/cm3. The P-type GaN layer 17 may be formed of a single layer, and may also be formed of a plurality of layers of different types and concentrations of P-type impurities. The thickness of the p-type GaN layer 17 is, for example, 50 to 2 〇〇 nm. Φ As the constituent electrode material of the 11-type electrode 18, for example,

Ti/Al ' Ti/Al/Mo/Au、Hf/Au等的堆疊結構或是合金等。η 型電極18的厚度譬如是Ti/Al(10nm/500nm)。 作為p型電極19,能夠舉出譬如pd/pt/Au、Ni/Au、 Pd/Mo/Au等的堆疊結構或者合金等、或是IT〇(氧化銦錫) 等氧化物系之透明導電材料。ρ型電極19的厚度譬如是ΙΤ〇 時為10〜200mn。在ρ型電極上需有打線(wireb〇nding)用的 銲墊電極,大多數的情況用與n型電極同樣的材料系統製 造。 (半導體發光元件之製造方法) 9/22 201029233 其次’按照圖2⑻〜(f)來說明有關本實施方式之相關 半導體發光元件10之製造方法。以下本實施方式之相關半 導體發光元件10之製造方法中,以如下為例子:在藍寶石 晶圓1Γ(基板11)上面設置氮氧化矽的光罩層12,而且在其 上依序形成u-GaN層13、η型GaN層14(摻Si)、為發光層 的多重量子井層15(井層15a:InGaN、障壁層i5b:GaN)、p 型AlGaN層16(摻Mg)、以及p型GaN層17(摻Mg)的各半 導體層之後,在η型GaN層14及p型GaN層17上面各自 形成η型電極18和p型電極19。 &lt;準備藍寶石晶圓&gt; 準備藍寶石晶圓11,。藍寶石晶圓11,,雖然根據其直徑 有所不同其厚度為0.3〜3.0mm、並且直徑為50〜300mm。 再者,在直徑50mm的藍寶石晶圓11'的情況時,在1張藍 寶石晶圓1Γ上面能製造出5000〜12000個半導體發光元件 10。 &lt;形成光罩層&gt; 作為形成光罩層12之方法,能夠舉出電漿CVD法、 常壓CVD法、濺射法等。 以下’說明有關利用了電漿CVD法的光罩層12之形 成方法。 形成光罩層12所使用的電漿CVD裝置,在不鏽鋼製 真空容器上方設置構成高頻電極的反應氣體供給部,並 且,在該真空容器内下方構成相對電極的晶圓臺並在晶圓 臺安裝加熱器。反應氣體供給部和晶圓臺之間的間隔譬如 是2.0〜3.0cm。並且,電漿CVD裝置構成為使得設定在晶 圓臺上的藍寶石晶圓11'上面經由反應氣體來沉積形成光罩 10/22 201029233 層12。 使用上述電漿CVD裝置,使藍寶石晶圓11,為表面朝 上地設定在晶圓臺之後,將藍寶石晶圓ir的溫度加熱到 300〜400°C並且使反應容器内的放電壓力為2〇〜3〇〇Pa,作 為反應谷器内的反應氣體’各自供給碎曱烧、A stacked structure of Ti/Al 'Ti/Al/Mo/Au, Hf/Au, or the like. The thickness of the n-type electrode 18 is, for example, Ti/Al (10 nm/500 nm). Examples of the p-type electrode 19 include a stacked structure such as pd/pt/Au, Ni/Au, Pd/Mo/Au, an alloy, or the like, or an oxide-based transparent conductive material such as IT〇 (indium tin oxide). . The thickness of the p-type electrode 19 is, for example, 10 to 200 nm. A pad electrode for wireb〇nding is required on the p-type electrode, and most of the cases are fabricated using the same material system as the n-type electrode. (Manufacturing method of semiconductor light-emitting device) 9/22 201029233 Next, a method of manufacturing the semiconductor light-emitting device 10 according to the present embodiment will be described with reference to Figs. 2(8) to (f). In the following method for manufacturing the semiconductor light-emitting device 10 according to the present embodiment, a photomask layer 12 of ruthenium oxynitride is provided on the sapphire wafer 1 (substrate 11), and u-GaN is sequentially formed thereon. Layer 13, n-type GaN layer 14 (doped with Si), multiple quantum well layers 15 of light-emitting layer (well layer 15a: InGaN, barrier layer i5b: GaN), p-type AlGaN layer 16 (doped with Mg), and p-type GaN After each of the semiconductor layers of the layer 17 (doped with Mg), an n-type electrode 18 and a p-type electrode 19 are formed on the n-type GaN layer 14 and the p-type GaN layer 17, respectively. &lt;Preparation of sapphire wafer&gt; Preparation of sapphire wafer 11 . The sapphire wafer 11, although it differs in diameter, has a thickness of 0.3 to 3.0 mm and a diameter of 50 to 300 mm. Further, in the case of a sapphire wafer 11' having a diameter of 50 mm, 5000 to 12,000 semiconductor light-emitting elements 10 can be produced on one sapphire wafer. &lt;Formation of Photomask Layer&gt; Examples of the method of forming the mask layer 12 include a plasma CVD method, a normal pressure CVD method, a sputtering method, and the like. The following describes the method of forming the photomask layer 12 using the plasma CVD method. In the plasma CVD apparatus used for forming the mask layer 12, a reaction gas supply unit constituting a high-frequency electrode is disposed above the stainless steel vacuum container, and a wafer stage of the opposite electrode is formed inside the vacuum container and is on the wafer stage. Install the heater. The interval between the reaction gas supply portion and the wafer stage is, for example, 2.0 to 3.0 cm. Further, the plasma CVD apparatus is constructed such that the layer 10 of the reticle 10/22 201029233 is deposited on the sapphire wafer 11' set on the wafer stage via the reaction gas. Using the above plasma CVD apparatus, the sapphire wafer 11 is set to face up after the wafer stage, and the temperature of the sapphire wafer ir is heated to 300 to 400 ° C and the discharge pressure in the reaction vessel is 2 〇. ~3〇〇Pa, as the reaction gas in the reaction cell, each is supplied with shredded pork,

SiH4)、氨(NH3)、氮(N2)、笑氣(N20)、和氫(H2),使其供 給流量各自為 1 〜1 〇mL/min(sccm)、0.5 〜1 OmL/min、1 〜SiH4), ammonia (NH3), nitrogen (N2), nitrous oxide (N20), and hydrogen (H2) are supplied at a flow rate of 1 to 1 〇mL/min (sccm), 0.5 to 1 OmL/min, and 1 ~

100mL/min、10〜5000mL/min、和 10〜5〇〇〇mL/min。再者, 使放電頻率為l〇〇kHz〜100MHz,高頻電力為1〇〜i〇〇w。 此時,如圖2⑻所示,在藍寶石晶圓1Γ上面,覆蓋其 表面地沉積氮氧化矽薄膜來形成光罩層12。 所形成的光罩層12之折射率,能夠經由向反應容器内 供給的反應氣體之組成或成膜條件之設定來加以控制。譬 =,旎夠經由提高矽甲烷的供給流量的比例來提高折射 率,另一方面,能夠經由提高笑氣的供給流量的比例、或 者經由增大高頻電力來降低折射率。因此,要使光罩層12 的折射率在厚度方向有所變化,在成顯_變更反應氣體 組成和成膜條件即可。 _再者,由於反應氣體中所含的氫將使得在光罩層12含 氫原子’在含過_氫原子時,由於加熱處理時的氮原子 ^離f對光罩層12產生裂縫(咖k)或是產生泡狀的缺 熱損傷顯著,而對光罩層12的性質―y)帶來 Z 、、;而,如上述般經由使用與矽甲烷相同乃至少許的 氣將能夠降低光罩層12的氫原子含有量。 =’如圖2(b)所示’在光罩層12形成開口 I2a。作 成先罩層12的開口 12a之方法,能夠舉出譬如反應性 11/22 201029233 離子蝕刻法(Reactive Ion Etching:RIE)等乾蝕刻法或是使用 氟酸系蝕刻液的濕蝕刻法等。 &lt;半導體層之形成&gt; 作為以下的各半導體層之形成方法,能夠舉出有機金 屬氣相蟲晶法(Metal Organic Vapor Phase Epitaxy:MOVPE)、分子磊晶法(M〇iecuiar Beam Epitaxy.MBE)、氫化物氣相遙晶法(Hydride Vapor Phase Epitaxy.’HVPE)等,這當中有機金屬氣相成長法最為一般。 以下,說明有關利用了有機金屬氣相成長法的各半導體層 之形成方法。 在形成各半導體層所使用的MOVPE裝置,能夠各自 以電子控制的晶圓搬送系、晶圓加熱系、氣體供給系、和 氣體排氣系來構成。晶圓加熱系、熱電偶及電阻加熱,在 其上設置之碳製或是SiC製的加熱臺並且,MOVPE裝置, 在晶圓加熱系中,搬送的石英盤(tray)的加熱臺上面設定的 藍寶石晶圓11’上面根據反應氣體使半導體層結晶成長。 -u-GaN層之形成- 使用上述MOVPE裝置,使得設有光罩層12的藍寶石 晶圓1Γ的光罩層12表面朝上地來設定在石英盤上後,並 將藍寶石晶圓1Γ加熱到1050〜115(TC並使反應容器内的壓 力為10k〜lOOkPa,並向設置在反應容器内的流路内作為載 子氣體使H2流通,將其狀態保持數分鐘將藍寶石晶圓u· 熱洗(thermal cleaning)。 接著,使藍寶石晶圓11,的溫度為1050〜1150〇c並且使 ,應容器内的壓力為10k〜l〇〇kpa,並向反應容器内將載子 氣體H2以l〇L/min左右的流量使之流通,於此作為反應氣 12/22 201029233 體,供給V族元素供給源_3)、和ΠΙ族元素供給源(TMG) 使其各自流量為G.ML/—、和5G〜。 S &quot;此時’從光罩層12的表面雖然不會產生結晶成長,但 是從在光罩層12形成的開口 12a露出之藍寶石晶圓11,表面 為起點’在其上使無摻雜的GaN結晶成長,如圖2⑹所示, . 來在光罩層12上面形成u-GaN層13。再者,在光罩層12 形成之開口 12a的部分,GaN於藍寶石晶圓^,表面的法線 方向上結阳成長形成層,另一方面,開口 12a之外的光罩 ® I 12的部分,經由GaN在橫方向結晶成長聚結(coalescence) 來形成覆蓋該部分的層。 再者,如果在形成u_GaN層13之前形成低溫緩衝層 時,使藍寶石晶圓11’的溫度為4〇〇〜5〇〇〇c來使GaN結晶 成長。 -η型GaN層之形成- 使反應容器内的壓力為l〇k〜i〇〇kpa,並且向反應容器 内以5〜15L/min(以下使氣體流量為基準狀態(0〇c、1氣壓) Φ 之值)的流量使載子氣體H2流通,並且作為反應氣體,供 給V族元素供給源(NH3)、III族元素供給源i(TMG)、和η 型摻雜元素供給源(SiH4)、使其流量各自為o.i〜5L/min、 5〇〜150#mol/min、*l〜5xl〇-3;czmol/min。 此時,如圖2(d)所示,接著u-GaN層13使η型GaN 結晶成長形成η型GaN層14。 _多重量子井層之形成-100 mL/min, 10 to 5000 mL/min, and 10 to 5 mL/min. Furthermore, the discharge frequency is from 1 kHz to 100 MHz, and the high frequency power is from 1 〇 to i 〇〇 w. At this time, as shown in Fig. 2 (8), a ruthenium oxynitride film is deposited on the surface of the sapphire wafer to form a mask layer 12. The refractive index of the formed photomask layer 12 can be controlled via the composition of the reaction gas supplied to the reaction vessel or the setting of the film formation conditions.譬 =, the refractive index is increased by increasing the ratio of the supply flow rate of the methane, and on the other hand, the refractive index can be lowered by increasing the ratio of the supply flow rate of the laughing gas or by increasing the high-frequency power. Therefore, in order to change the refractive index of the photomask layer 12 in the thickness direction, it is sufficient to change the composition of the reaction gas and the film formation conditions. Further, since the hydrogen contained in the reaction gas will cause the hydrogen atom in the photomask layer 12 to contain a hydrogen atom, a crack occurs in the photomask layer 12 due to the nitrogen atom from the heat treatment. k) or the bubble-like heat loss damage is significant, and brings the Z to the property y) of the mask layer 12; and, as described above, the mask can be reduced by using the same or a little gas as the methane. The hydrogen atom content of the layer 12 is. = ' As shown in Fig. 2(b), an opening I2a is formed in the photomask layer 12. The method of forming the opening 12a of the cap layer 12 may be, for example, a dry etching method such as reactivity 11/22 201029233 ion etching (Reactive Ion Etching: RIE) or a wet etching method using a hydrofluoric acid etching solution. &lt;Formation of Semiconductor Layer&gt; Examples of the method for forming each of the following semiconductor layers include Metal Organic Vapor Phase Epitaxy (MOVPE) and Molecular Epitaxy (M〇iecuiar Beam Epitaxy. MBE). ), Hydride Vapor Phase Epitaxy. 'HVPE, etc., among which organometallic vapor phase growth is the most common. Hereinafter, a method of forming each semiconductor layer using the organometallic vapor phase growth method will be described. The MOVPE devices used to form the respective semiconductor layers can be configured by an electronically controlled wafer transfer system, a wafer heating system, a gas supply system, and a gas exhaust system. Wafer heating system, thermocouple and resistance heating, carbon or SiC heating table provided thereon, and MOVPE device, set in the wafer heating system, on the heating table of the quartz disk (tray) The semiconductor layer is crystal grown on the sapphire wafer 11' according to the reaction gas. Formation of a -u-GaN layer - Using the MOVPE device described above, the mask layer 12 of the sapphire wafer 1 provided with the mask layer 12 is placed on the quartz disk with the surface facing up, and the sapphire wafer is heated to 1 1050 to 115 (TC and the pressure in the reaction vessel is 10k to 100 kPa, and H2 is supplied as a carrier gas in the flow path provided in the reaction container, and the state is kept for several minutes to heat the sapphire wafer u· (thermal cleaning) Next, the temperature of the sapphire wafer 11 is 1050 to 1150 〇c, and the pressure in the container is 10k~l〇〇kpa, and the carrier gas H2 is taken into the reaction vessel. The flow rate around L/min is circulated, and as the reaction gas 12/22 201029233, the V element supply source _3) and the steroid element supply source (TMG) are supplied so that their respective flows are G.ML/- , and 5G ~. S &quot; At this time, although the crystal growth does not occur from the surface of the photomask layer 12, the surface of the sapphire wafer 11 exposed from the opening 12a formed in the photomask layer 12 is the starting point 'on which is undoped The GaN crystal grows, and as shown in Fig. 2 (6), a u-GaN layer 13 is formed on the mask layer 12. Further, in a portion of the opening 12a where the mask layer 12 is formed, GaN is grown in a sapphire wafer in the normal direction of the surface, and on the other hand, a portion of the mask® I 12 outside the opening 12a is formed. The layer covering the portion is formed by crystal growth and crystallization in the lateral direction via GaN. Further, when the low temperature buffer layer is formed before the formation of the u_GaN layer 13, the temperature of the sapphire wafer 11' is made 4 〇〇 to 5 〇〇〇 c to crystallize the GaN. - Formation of n-type GaN layer - The pressure in the reaction vessel is l〇k~i〇〇kpa, and is 5 to 15 L/min in the reaction vessel (hereinafter, the gas flow rate is used as a reference state (0 〇 c, 1 gas pressure) The flow rate of the value of Φ causes the carrier gas H2 to flow, and supplies the group V element supply source (NH3), the group III element supply source i (TMG), and the n-type doping element supply source (SiH4) as a reaction gas. The flow rates were respectively oi~5L/min, 5〇~150#mol/min, *l~5xl〇-3; czmol/min. At this time, as shown in FIG. 2(d), the u-GaN layer 13 then crystallizes the n-type GaN to form the n-type GaN layer 14. _The formation of multiple quantum well layers -

使藍寶石晶圓ir的溫度為8〇o°c左右並使反應容器内 的壓力為l〇k〜lOOkPa,並且,向反應容器内以5〜15L/min 的流量使載子氣體N2流通,於此作為反應氣體,供給V 13/22 201029233 族元素供給源(NH3)、III族元素供給源KTMG)、和m族 元素供給源2(TMI),使其流量各自為〇」〜5L/min、5〜15 &quot;mol/min、和 2〜30&quot;mol/min。此時,接著 n 型 GaN 層 14使得InGaN結晶成長形成井層i5a。 接著,使得v族元素供給源(NH3)、和ΙΠ族元素供給 源(TMG)的供給流量各自為和$〜丨 mol/min。此時,接著InGaN的井層15a,使⑽結晶成長 形成障壁層15b。 並且,交替重複與上述同樣的操作,如圖2(e)所示,經 由交替形成井層15a和障壁層15b來構成多重量子井層 15。再者,多重量子井層15的發光波長依存於井層15a的 井寬度(井層的厚度)和InN混晶比,InN混晶比愈高發光 波長將變成長波長。InN混晶比根據TMI的莫耳流量/(TMG 的莫耳流量+TMI的莫耳流量)成長溫度決定。 -P型AlGaN層及GaN層之形成- 使藍寶石晶圓1Γ的溫度為1000〜ll〇〇t並使反應容器 内的壓力為l〇k〜100kPa,向反應容器内以5〜15L/min的 流量使載子氣體H2流通,作為反應氣體,供給v族元素 供給源(NH3)、III族元素供給源l(TMG)、ΠΙ族元素供給源 3(TMA)、和p型摻雜元素供給源(Cp2Mg),使其各自的供 給流篁為 0.1 〜5L/min、50 〜150 // mol/min、2 〜80 // mol/min、和 〇.〇3〜30//mol/min 〇 此時,如圖2(f)所示,接著多重量子井層15,使AlGaN 結晶成長形成p型AlGaN層16。 接著,作為反應氣體,供給V族元素供給源(NH3)、III 族元素供給源l(TMG)、和p型摻雜元素供給源(Cp2Mg), 14/22 201029233 使其各自的供給流置為〇 1〜5L/min、%〜i5〇&quot;mol/min、 和 0.03〜30^m〇i/min。 此時,如圖2(f)所示,接著p型A1GaN層16,使p型 GaN結晶成長形成P型GaN層π。 &lt;電極之形成&gt; 經由使得堆疊形成的半導體層的藍寶石晶圓 1Γ部分地 反應性離子侧來露出n型⑽層14之後,根據真空蒸 鑛減射 CVD(Chemical Vapor Deposition)等方法來在 η 型⑽層14上面形成η型電極18並在ρ型GaN層17上 面形成p型電極19。 一並且,經由切開藍寶石晶圓u,分割成各個的半導體發 光元件10。 【實施例】 (測試評價1) 除了在藍寶;5基板上形成平行延長的複數的溝(相當於 =成上述實施方式的光罩層之開口部)之後設置〜⑽層這 點之外,在與上述實施方式同樣結構的半導體發光元 ^外部量子效率為43%。再者,此—半導體發光元件, 上述實把方式的半導體發光元件中,相當於光罩層的折 射率與藍寶石基板的折射率為相同之情況。 除了在平坦的藍寶石基板上不言免置光罩層而設置 u GaN層點之外、與上述實施方式同樣結構的半導體 發光元件,外部量子效率為33 8%。再者,此一半導體發 光凡件,在上述實施方式的半導體發光元件中,相 罩層的折射率與u_GaN層的折射率為囉情況。w ' 除了設置在平坦的藍寶石基板上形成平行延長的複數 15/22 201029233 而在其上設置一層這-部量子效率為=式同樣結構的彻發光元件,外 率為與合之模擬’當光革層的折射 時、外部量:!:ί ,當光罩層的折射率為”6 ㈣番名量率為43.2’當光罩層的折射率為1.88時、 : 效率為42.8,當光罩層的折射率為2 〇1時The temperature of the sapphire wafer ir is about 8 〇 o ° c and the pressure in the reaction vessel is l〇k to 100 kPa, and the carrier gas N2 is caused to flow in the reaction vessel at a flow rate of 5 to 15 L/min. As a reaction gas, V 13/22 201029233 group element supply source (NH3), group III element supply source KTMG), and m group element supply source 2 (TMI) are supplied, and the flow rates thereof are each 〇" to 5 L/min, 5~15 &quot;mol/min, and 2~30&quot;mol/min. At this time, the n-type GaN layer 14 is followed to crystallize the InGaN crystal to form the well layer i5a. Next, the supply flow rates of the group v element supply source (NH3) and the lanthanum element supply source (TMG) are each made equal to $~丨 mol/min. At this time, the well layer 15a of InGaN is grown to form (10) crystals to form the barrier layer 15b. Further, the same operation as described above is alternately repeated, and as shown in Fig. 2(e), the multiple quantum well layers 15 are formed by alternately forming the well layer 15a and the barrier layer 15b. Furthermore, the emission wavelength of the multiple quantum well layer 15 depends on the well width (thickness of the well layer) and the InN mixed crystal ratio of the well layer 15a, and the higher the InN mixed crystal ratio, the longer the wavelength becomes. The InN mixed crystal ratio is determined according to the MMI flow rate of TMI / (mole flow of TMG + molar flow of TMI). -P-type AlGaN layer and GaN layer formation - the temperature of the sapphire wafer 1 为 1000 〇〇 〇〇 并使 并使 并使 并使 并使 并使 并使 并使 并使 并使 并使 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应 反应The flow rate causes the carrier gas H2 to flow, and supplies a group V element supply source (NH3), a group III element supply source 1 (TMG), a steroid element supply source 3 (TMA), and a p-type doping element supply source as a reaction gas. (Cp2Mg), so that their respective supply flow is 0.1 to 5 L/min, 50 to 150 //mol/min, 2 to 80 //mol/min, and 〇.〇3 to 30//mol/min. At the same time, as shown in FIG. 2(f), the multi-quantum well layer 15 is followed to crystallize the AlGaN crystal to form the p-type AlGaN layer 16. Next, as a reaction gas, a group V element supply source (NH3), a group III element supply source 1 (TMG), and a p type doping element supply source (Cp2Mg) are supplied, 14/22 201029233, and their respective supply flows are set to 〇1~5L/min, %~i5〇&quot;mol/min, and 0.03~30^m〇i/min. At this time, as shown in FIG. 2(f), the p-type GaN layer 16 is subsequently grown to form a p-type GaN layer π. &lt;Formation of Electrodes&gt; After the n-type (10) layer 14 is exposed by partially displacing the ionic surface of the sapphire wafer of the semiconductor layer formed by stacking, according to a method such as vacuum vapor deposition CVD (Chemical Vapor Deposition) An n-type electrode 18 is formed on the n-type (10) layer 14 and a p-type electrode 19 is formed on the p-type GaN layer 17. One is divided into individual semiconductor light-emitting elements 10 by cutting the sapphire wafer u. [Examples] (Test evaluation 1) Except that a plurality of grooves extending in parallel (corresponding to the opening of the mask layer of the above-described embodiment) were formed on the sapphire; 5 substrate, and then the layer (~) was provided. The external quantum efficiency of the semiconductor light-emitting device having the same structure as that of the above embodiment was 43%. Further, in the above-described semiconductor light-emitting device, the semiconductor light-emitting device of the above-described embodiment has a case where the refractive index of the photomask layer is the same as the refractive index of the sapphire substrate. The external quantum efficiency of the semiconductor light-emitting device having the same configuration as that of the above embodiment except that the u GaN layer was provided on the flat sapphire substrate without the mask layer was provided, the external quantum efficiency was 33 8%. Further, in the semiconductor light-emitting device of the above-described embodiment, the refractive index of the phase mask layer and the refractive index of the u-GaN layer are in the case of the semiconductor light-emitting device. w 'In addition to the parallel embossed plural 15/22 201029233 formed on a flat sapphire substrate, a layer of this light-emitting component with the same quantum efficiency is the same structure, and the external ratio is simulated. The refractive index of the leather layer, the external amount:!: ί, when the refractive index of the mask layer is "6 (four), the nominal rate is 43.2', when the refractive index of the mask layer is 1.88, the efficiency is 42.8, when the mask When the refractive index of the layer is 2 〇1

量钱率為42.卜當光罩層的折射率為221時、外部量; 效率為41.0 ’當料層的折射率為2.35時、外部量子效率 為37.8 ’以及、當光罩層的折射率為2 54時、外 率為 33.8。 ha 圖3不出基於以上結果的光罩層之折射率和外 效率之關係。 .根據圖3,能夠得知:經由使得光罩層的折射率大於 Si02的折射率並小於GaN層的折射率,外部量子效率變高。 (測試評價2)The amount of money is 42. When the refractive index of the mask layer is 221, the external amount; the efficiency is 41.0 'when the refractive index of the layer is 2.35, the external quantum efficiency is 37.8 ', and when the refractive index of the mask layer The rate was 23.8 and the rate was 33.8. Ha Figure 3 shows the relationship between the refractive index and the external efficiency of the mask layer based on the above results. According to Fig. 3, it can be seen that the external quantum efficiency is increased by making the refractive index of the photomask layer larger than the refractive index of SiO 2 and smaller than the refractive index of the GaN layer. (Test Evaluation 2)

使用電漿CVD裝置(反應氣體供給部和晶圓臺之間的 間隔:25mm)’在晶圓臺上設定藍寶石晶圓之後,將藍寶石 晶圓的溫度加熱到350X:並使得反應容器内的放電壓力為 lOOPa’向反應容器内供給矽甲烷、氨、和氮作為反應氣體, 使其流量各自為5mL/min、2mL/min、和50mL/min ,來在 藍寶石晶圓上沉積形成薄膜。並且,使放電頻率為 13.56MHz,使高頻電力為50W。 有關沉積形成之薄膜,使用傅立葉變換型紅外光譜光 度計(Nanometrics Inc製、型號:QS1200)來分析紅外線吸收 16/22 201029233 光譜,得知其為氮化石夕。並且,有關此一氮化石夕薄膜,使 用橢圓偏振光儀(EllipSometer)(堀場製作所製、商品名 稱:UVISEL/M200-VIS-AG-200S)所測量的折射率為 2 其次,除了作為反應氣體供給笑氣這一點以外與上述 _地沉積形賴氧切薄膜1㈣氣的供給流量複數 · :欠來沉獅簡膜。並且’有·氮氧切_測量其折 射率。 圖4示出笑氣的供給流量與沉積形成的氮氧化石夕薄膜 φ 的折射率之關係。 ' 根據圖4,得知:若是笑氣的供給流量在0〜6mL/min 的範圍增加,氮氧化石夕薄膜的折射率將從2〇降低到i6左 右。並且,可以得知:笑氣的供給流量約3mL/min時,氮 氧化矽薄膜的折射率與藍寶石同樣的為17。 (測試評價3) 使用與測試評價2相同的電漿CVD裝置,在晶圓臺上 設定了藍寶石晶圓之後,將藍寶石晶圓的溫度加熱到35〇 • °C並使得反應容器内的放電壓力為l〇〇Pa,作為反應氣體, 向反應容器内供給石夕曱烧、氮和笑氣使其各自流量為 5mL/min、2mL/min、50mL/min、和 3mL/min,在藍寶石晶 圓上沉積形成氮氧化矽薄膜。並且,使得放電頻率為 13.56MHz,高頻電力為50W。 . 其次,除了反應氣體供給氫這一點之外與上述同樣地 侃錄㈣薄膜。經由複數錢賊的供給流量來沉積 形成薄膜。 並且,有關各成膜之氮氧化石夕的薄膜,使用平整度測 量儀(flatness tester) (NIDEK 公司製、型號:FT_9〇〇)測量了内 17/22 201029233 部應力。 圖5不出氫的供給流量和氤氡化矽薄膜的内部應力之 關係。 根據圖5,能夠得知:隨著氩供給流量變多,在壓縮應 力變大的方向内部應力變化,並且,氫的供給流量在 20mL/min附近内部應力急遽地從拉伸侧變為壓縮側。因 此,能夠認為:經由操縱氫的供給流量能控制氤氧化矽薄 膜的内部應力。 再者,有關薄膜的内部應力,有著一個問題是:若是 大的拉伸應力產生作用加熱處理時薄膜熱膨脹容易產生破 裂,另一方面,有著一個問題是:若是大的壓縮應力起作 用時加熱處理時氫等脫掉而容易產生表面形態的不均。 (測試評價4) 除了作為反應氣體把氮的一部分或整個置換為惰性氣 體的氬這一點之外、與在測試評價2的使反應氣體為矽甲 烷、氨和氮同樣地來在藍寶石晶圓上沉積形成氮氧化矽薄 膜。經由複數次改變氬的置換量來沉積形成薄膜。 並且,有關各形成的氮氧化石夕薄膜測量其内部應力。 其如果得知··隨著氬的置換量變多,在壓縮應^變大 的方向上内部應力變化,在把全部的氮的全部置換為氬時 將為108Pa程度之壓縮應力。因此,能夠認為:根據操縱 置換氮的一部分的惰性氣體之置換量將能夠控制氮氧化矽 的薄膜的内部應力。 (測試評價5) 〆除了改變放電頻率這-點、與在測試評價2的使反應 氣體為矽甲烷、氨、和氮的情況同樣地來在藍寶石晶圓上 18/22 201029233 形成氮氧化矽薄膜。經由複數次改變放電頻率來沉積形成 薄膜。Using a plasma CVD apparatus (interval between the reaction gas supply unit and the wafer stage: 25 mm) 'After setting the sapphire wafer on the wafer stage, the temperature of the sapphire wafer is heated to 350X: and the discharge in the reaction vessel is made. Methane, ammonia, and nitrogen were supplied as reaction gases to the reaction vessel at a pressure of 100 Pa', and the flow rates were 5 mL/min, 2 mL/min, and 50 mL/min, respectively, to deposit a film on the sapphire wafer. Further, the discharge frequency was 13.56 MHz, and the high frequency power was 50 W. For the film formed by deposition, a spectrum of infrared absorption 16/22 201029233 was analyzed using a Fourier transform infrared spectrophotometer (manufactured by Nanometrics Inc., model: QS1200), and it was found to be a nitride. Further, regarding this nitriding film, the refractive index measured by an EllipSometer (manufactured by Horiba, Ltd., trade name: UVISEL/M200-VIS-AG-200S) is 2, followed by supply as a reaction gas. Laughing this point is not the same as the above-mentioned _ ground deposition type lysate film 1 (four) gas supply flow plural number: owe to the lion. And 'there is a nitroxene _ measuring its refractive index. Fig. 4 shows the relationship between the supply flow rate of the laughing gas and the refractive index of the nitrous oxide film φ formed by the deposition. According to Fig. 4, it is found that if the supply flow rate of laughing gas increases in the range of 0 to 6 mL/min, the refractive index of the nitrous oxide film will decrease from 2 到 to about i6. Further, it can be seen that when the supply flow rate of the laughing gas is about 3 mL/min, the refractive index of the yttrium oxynitride film is 17 as in the case of sapphire. (Test Evaluation 3) Using the same plasma CVD apparatus as Test Evaluation 2, after the sapphire wafer was set on the wafer stage, the temperature of the sapphire wafer was heated to 35 〇 ° ° C and the discharge pressure in the reaction vessel was made. As a reaction gas, as a reaction gas, the reaction vessel was supplied with Shixia, Nitrogen and Naughty gas at respective flow rates of 5 mL/min, 2 mL/min, 50 mL/min, and 3 mL/min on the sapphire wafer. A film of arsenic oxynitride is formed on the upper layer. Further, the discharge frequency was 13.56 MHz, and the high frequency power was 50 W. Next, in the same manner as described above, the film was recorded in the same manner as described above except that the reaction gas was supplied with hydrogen. A film is deposited by the supply flow of a plurality of money thieves. Further, the inner 17/22 201029233 stress was measured using a flatness tester (manufactured by NIDEK Co., Ltd., model: FT_9〇〇) for each of the film-formed nitrous oxide films. Fig. 5 shows the relationship between the supply flow rate of hydrogen and the internal stress of the antimony telluride film. According to FIG. 5, it can be seen that as the argon supply flow rate increases, the internal stress changes in the direction in which the compressive stress increases, and the internal pressure of the hydrogen supply flow rate is approximately 20 mL/min, and the internal stress is rapidly changed from the tensile side to the compression side. . Therefore, it can be considered that the internal stress of the tantalum oxide thin film can be controlled by manipulating the supply flow rate of hydrogen. Furthermore, there is a problem with the internal stress of the film: if the large tensile stress acts to heat the film, the thermal expansion of the film is liable to cause cracking. On the other hand, there is a problem that if a large compressive stress acts, heat treatment When hydrogen or the like is removed, unevenness in surface morphology is likely to occur. (Test Evaluation 4) In addition to the argon which replaced a part or the whole of the nitrogen as an inert gas as a reaction gas, the reaction gas was the same as the methane, ammonia and nitrogen in the test evaluation 2 on the sapphire wafer. The deposition forms a thin film of cerium oxynitride. The film formation is deposited by changing the amount of substitution of argon several times. Further, the internal stress of each of the formed nitrous oxide films was measured. When it is known that the amount of substitution of argon increases, the internal stress changes in the direction in which the compression is large, and when all of the nitrogen is replaced by argon, it is a compressive stress of about 108 Pa. Therefore, it can be considered that the internal stress of the film of yttrium oxynitride can be controlled by the amount of substitution of the inert gas which manipulates a part of the replacement nitrogen. (Test Evaluation 5) In addition to changing the discharge frequency, the yttrium oxynitride film was formed on the sapphire wafer 18/22 201029233 in the same manner as in the test evaluation 2, the reaction gas was 矽methane, ammonia, and nitrogen. . A thin film is deposited by changing the discharge frequency a plurality of times.

並且,有關各形成之氮氧化矽薄膜,測量其内部應力。 其結果,能夠得知:使放電頻率為低時,在離子電漿 頻率附近中内部應力急遽低從拉伸侧變化為壓縮側,在 4MHz時成為ixl〇8Pa以下的壓縮應力。因此,能夠認為: 經由操作放電頻率能夠控制氮氧化矽薄膜的内部應力。 【產業利用之可能性】Further, the internal stress of each of the formed yttria thin films was measured. As a result, when the discharge frequency is low, the internal stress is rapidly lowered from the tensile side to the compression side in the vicinity of the ion plasma frequency, and becomes a compressive stress of ixl 〇 8 Pa or less at 4 MHz. Therefore, it can be considered that the internal stress of the yttrium oxynitride film can be controlled by operating the discharge frequency. [Possibility of industrial use]

【圖=:】半導想發光元件及其製造方法極為有用[图 =:] Semi-conductive light-emitting elements and their manufacturing methods are extremely useful

圖1為實施方式的半導體發光元件之斷面圖。 =為實财式神導體發光元件製造方法之說 圖3為光罩層的折射率和外部量子效率 係圖圖4衫㈣供給流量魏氧切 為氫的供給流量與氮氧化砂薄勒部應力 圖 圖 之關係 【主要元件符號說明】 10 半導體發光元件 11 基板 12 光罩層 12a 開口 13 u-GaN 層 14 n型GaN層 15 多重量子井層 15a 井層 19/22 201029233 15b障壁層 16 p 型 AlGaN 層 17 p型GaN層 18 n型電極 19 ρ型電極1 is a cross-sectional view showing a semiconductor light emitting device of an embodiment. Fig. 3 is a diagram showing the manufacturing method of the refractive index and the external quantum efficiency of the photomask layer. Fig. 4 (4) Supply flow rate Wei oxygen is the supply flow rate of hydrogen and the nitrogen oxide sand Diagram relationship [Main component symbol description] 10 Semiconductor light-emitting element 11 Substrate 12 Photomask layer 12a Opening 13 u-GaN layer 14 n-type GaN layer 15 Multiple quantum well layer 15a Well layer 19/22 201029233 15b barrier layer 16 p type AlGaN layer 17 p-type GaN layer 18 n-type electrode 19 p-type electrode

20/2220/22

Claims (1)

201029233 七、申請專利範圍·· L種半導體發光元件,其令: 該半導體發光元件包括: 基板、具有GaN的結晶能夠成長之表面, 某杯的if被°又為覆蓋上述基板之表面而形成有使得該 表Ϊ 2部分露出之開口並具有GaN的結晶無法成長之 ❹ ❿ 露出蓋上述光罩層及從該_的開口 GaN=?折射率大於_之折射率且小於上述 2如申請專利範圍第i項所記載之半導體發光元件,其 中.上述光罩層的折射率大於Μ1 2並小於2 Μ。 、 件,=申項所記載之半賴發光元 千具中.上述先罩層以氮氧化矽形成。 發光利範㈣1至3項之任1所記載之半導體 =讀,其中:上述光罩層之折射率在厚度方向產生變 21/22 1 . 如t料職_ 4摘記狀半物發光元件,盆 中·上述光罩層之折射率從厚度方向上的上述⑽層一侧 朝向上述基板一侧逐漸變小地產生變化。 2 . 如申請專利範圍第!至1項之任— 發光元件,其中:上述基板為藍f石基板。㉙之+導體 7. —種半導體發光元件之製造方法,其中. 該半導體發光元件包括: 基板、具有GaN的結晶能夠成長之表面, 201029233 光單層、被設為覆蓋上述基板之表面而形成有使得該 基板的表面部分露出之開口並具有GaN的結晶無法成長之 表面,以及 GaN層、被設為覆蓋上述光罩層及從該光罩層的開口 露出的上述基板之表面; 以CVD法沉積形成光罩層使得該光罩層之折射率大於 Si〇2之折射率且小於上述GaN層之折射率。201029233 VII. Patent application scope · L semiconductor light-emitting device, the semiconductor light-emitting device includes: a substrate, a surface on which crystals having GaN can grow, and a if of the cup is formed to cover the surface of the substrate Opening the surface of the surface of the surface 2 and having crystals of GaN that cannot grow ❹ exposing the photomask layer and the opening GaN=? refractive index of the opening from the opening is greater than _ and less than the above 2 The semiconductor light-emitting device according to Item 1, wherein the photomask layer has a refractive index greater than Μ1 2 and less than 2 Μ. , the piece, = the semi-luminous illuminating element described in the application. The first cover layer is formed by yttrium oxynitride. The semiconductor = read as described in any one of items 1 to 3, wherein the refractive index of the photomask layer is changed by 21/22 1 in the thickness direction. For example, t material _ 4 unmarked half-element light-emitting element, in the basin The refractive index of the mask layer changes gradually from the (10) layer side in the thickness direction toward the substrate side. 2. If you apply for a patent scope! To one of the light-emitting elements, wherein the substrate is a blue f-stone substrate. A method of manufacturing a semiconductor light-emitting device, wherein: the semiconductor light-emitting device comprises: a substrate, a surface capable of growing crystals having GaN, and a light single layer of 201029233, which is formed to cover a surface of the substrate a surface in which a surface portion of the substrate is exposed and having a surface in which crystallization of GaN cannot grow, and a surface of the GaN layer covered with the photomask layer and exposed from the opening of the photomask layer; deposited by CVD The photomask layer is formed such that the refractive index of the photomask layer is greater than the refractive index of Si〇2 and smaller than the refractive index of the GaN layer.
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