TW200525847A - Gallium nitride vertical light emitting diode structure and method of separating a substrate and a thin film in the structure - Google Patents

Gallium nitride vertical light emitting diode structure and method of separating a substrate and a thin film in the structure Download PDF

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TW200525847A
TW200525847A TW93101293A TW93101293A TW200525847A TW 200525847 A TW200525847 A TW 200525847A TW 93101293 A TW93101293 A TW 93101293A TW 93101293 A TW93101293 A TW 93101293A TW 200525847 A TW200525847 A TW 200525847A
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substrate
thin film
film layer
layer
gallium nitride
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TW93101293A
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TWI232016B (en
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Schang-Jing Hon
Mu-Jen Lai
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Super Nova Optoelectronics Corp
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Abstract

A GaN vertical light emitting device structure and a method of separating a substrate and a thin film thereon in the GaN vertical light emitting device (LED). The structure comprises a metal reflector for reflecting a light. The method comprises the steps: providing a laser array over the substrate wherein a laser light emitted by the laser array may at least partially be transparent to the substrate and its energy may be absorbed by the thin film; irradiating the thin film through the substrate; and then separating the substrate and the thin film.

Description

【先前技術】 半導體發光二極體(led)之發展已有數十年歷史, 發光效率之提升與否一直為LED能否進—步用於民生ς 之關鍵,因此多年來LED的發展方向大致皆在於發光效率、 之提升上。然於發光效率提升之路上,散熱問題一直 大限制因素;亦即,當發光效率不斷上升之際,若光所: 之熱無法有效排除,lew乃將陷於無法正常工作之境。 此,多年來LED之研發實以提升發光效率及排除熱為主。 在LED發展史中,所提出之排熱技術良多,如以金 材電路基板取代傳統導熱性不佳之印刷電路板,俾使晶 :^熱得在LED結構外藉金屬排除。LED結構内之排熱^亦 得提升之,如藍寶石上雖適於成長氮化鎵(。幻系“以吉 ,,、但其為導熱性不佳之非導體材料,因此—般常先藉由 ,、成長GaN系LED結構,之後再將其脫離該LED結構,並在 :後貼附以另一導熱性較佳之基材,纟示意說明於第一 A 及第一 B圖中。由於上述藍寶石基材功能僅在形成多層 巧於其上,t各多層薄膜皆形成後需予移除,故在此稱 ^,過渡基材。第一 A圖中,所示者為一垂直發光元件結 ,其正處於未完成製造階段中。圖中,首先先以一過 200525847 五、發明說明(2) 渡基材1 6當作基板生成薄膜結構層,薄膜結構包含^型氮 化鎵系層1 5、主動層1 4、ρ型氮化鎵系層丨3及金屬基材 11,其一端更有Ρ型電極17形成於該金屬基材丨丨上,因過 渡基材1 6之存在係欲使後續製程有一支撐體,故可於此垂 直發光元件結構完成後移除之,如第一 Β圖所示。之後, 將整個垂直發光元件結構1 0加以1 8 〇度翻轉即可得如第一 Β 圖之結構,第一 Β圖其中,過渡基材16,先予去除,之後一 η型電極18’再製作於η型氮化鎵系層15,上,如此便完成整 個垂直發光元件結構1 0 ’之製造。 再請參閱第一 Β圖,此時整個垂直發光元件結構丨〇,之 上下側得分別貼附以金屬電極1 7 ’( ρ型電極)及1 8,( η型 電極),由於整個垂直發光元件結構丨〇,之各層無側向結 構,故稱作垂直結構L E D。如此形成之結構不僅得改善上 述排熱問題,其發光面積亦較傳統者為大,因其二電極皆 不設於結構側向上;因此,側向出射光面積不需減小,且 因透明形式形成於led結構兩側上而得讓光線穿透。 如第一 C圖所示,其為第一 a圖至第一B圖移除過渡基材 後之氮化鎵系垂直發光元件結構10,,。主動層14"所發之 光有一部份往p型氮化鎵系層1 3”行進,另有一部份往\型 氮化鎵系層1 5,’(如圖中箭頭所示),若η型電極1 8,,一側為 所欲之光出射處,則往Ρ型電極1 7π之光形同浪費。 關於上述垂直結構之過渡基材與上方薄膜層間之分 離’現已有數種技術被提出,如先以藍寶石作為基材(過 渡基材)而進行結構各層之形成,該過渡基材與其上方之ρ[Previous technology] The development of semiconductor light-emitting diodes (LEDs) has a history of decades. The improvement of luminous efficiency has always been the key to whether LEDs can be used—the key to further use in people's livelihood. Therefore, the development direction of LEDs over the years is roughly All are in the improvement of luminous efficiency. However, on the way of improving the luminous efficiency, the heat dissipation problem has been a major limiting factor; that is, when the luminous efficiency is continuously increasing, if the heat of the light source cannot be effectively eliminated, lew will be trapped in a situation where it cannot work normally. Therefore, the research and development of LED for many years has been focused on improving luminous efficiency and eliminating heat. In the history of LED development, there are many proposed heat removal technologies, such as replacing traditional printed circuit boards with poor thermal conductivity with gold circuit boards, so that the crystals can be removed from the LED structure by metal. The heat dissipation in the LED structure must also be improved. For example, although sapphire is suitable for growing gallium nitride (. The magic system "Yi," but it is a non-conductive material with poor thermal conductivity, so-often by first To grow a GaN-based LED structure, detach it from the LED structure, and attach another substrate with better thermal conductivity at the back, which is illustrated schematically in the first A and B diagrams. Because of the above sapphire The function of the substrate is only after the formation of multiple layers, and each multilayer film needs to be removed after it is formed, so it is called ^, the transition substrate. In the first A diagram, the one shown is a vertical light-emitting element junction. It is in the unfinished manufacturing stage. In the figure, first use 200525847. V. Description of Invention (2) Substrate 16 is used as a substrate to generate a thin film structure layer. The thin film structure includes a ^ -type gallium nitride system layer 1 5 , Active layer 14, 4, p-type gallium nitride-based layer 3, and metal substrate 11, one end of which has a P-type electrode 17 formed on the metal substrate, because the existence of the transition substrate 16 is to be used The subsequent process has a support, so it can be removed after the vertical light emitting element structure is completed, such as the first B After that, the entire vertical light-emitting element structure 10 is turned by 180 ° to obtain a structure like the first B picture, in which the transition substrate 16 is removed first, and then an n-type The electrode 18 'is then fabricated on the n-type gallium nitride-based layer 15, so that the fabrication of the entire vertical light emitting element structure 10' is completed. Referring again to the first B figure, the entire vertical light emitting element structure at this time 丨 〇, The upper and lower sides must be attached with metal electrodes 17 '(ρ-type electrodes) and 18, (n-type electrodes). Since the entire vertical light-emitting element structure has no lateral structure, it is called a vertical structure LED. The structure thus formed not only improves the above-mentioned heat removal problem, but also has a larger light emitting area than the traditional ones, because neither of the two electrodes is arranged on the side of the structure; therefore, the area of lateral light emission does not need to be reduced, and due to the transparent form It is formed on both sides of the LED structure to allow light to penetrate. As shown in FIG. 1C, it is a first a to a B diagram of the gallium nitride-based vertical light emitting element structure 10 after the transition substrate is removed, ,. Active layer 14 " part of the light emitted The p-type gallium nitride-based layer 1 3 ″ travels, and another part goes to the \ -type gallium nitride-based layer 15 ′, (as shown by the arrow in the figure). If the n-type electrode 18, one side is as desired Where the light exits, the light towards the P-shaped electrode 17 7 is equally wasteful. Regarding the separation between the above-mentioned vertical structure transition substrate and the upper film layer, several technologies have been proposed, such as using sapphire as the substrate (transition Substrate) to form layers of the structure, the transition substrate and the ρ above

第7頁 200525847 五、發明說明(3) 型半導體材料層或η型半導體材料層間製作以一脆性結 構,並藉力使之分離。亦有習用技術以雷射光提供能量而 分離過渡基材與其上方之薄膜,此時該上方薄膜得吸收該 雷射光能量,並因融解而與過渡基材分離’如美國早期公 開專利申請案US20030150843。在該申請案中(請參閱第二 圖),一線狀雷射光2 3對過渡基材2 2上薄膜層2 1進行掃 描,薄膜層2 1吸收雷射光2 3能量後便可因其與基材之接面 2 5處融解而與過渡基材2 2分離,其中過渡基材2 2與薄膜層 2 1在掃描時之移動方向如圖中所示,S為一次掃描時之掃 描區,Μ為一次掃描之掃描寬度,t為薄膜層2 1之厚度,其 中掃描寬度Μ之值近乎等於或小於厚度t值。 然而,該篇申請案仍有其技術上之缺點。例如,整層 薄膜在線狀光源掃描過後,薄膜上各處之融解程度已不相 同;因此,在將過渡基材2 2脫離之時,過渡基材2 2與薄膜 層2 1間之各處受剝離力不夠均勻。再者,線狀雷射掃描進 行時有熱應力問題的存在,該不均勻熱應力亦使剝離效果 不盡理想,且有膜層破裂之虞。 鑑於習用氮化鎵系垂直結構發光二極體(LED)元件結構及 其製造方法上的缺點,一種在製造時能避免上述問題之氮 化鎵系垂直發光二極體(LED)之結構及該結構上一基材與 一薄膜分離之方法確有提出的必要。 【發明内容】 鑑於上述問題,本發明之主要目的即在於降低垂直發Page 7 200525847 V. Description of the invention (3) Type semiconductor material layer or n-type semiconductor material layer is fabricated with a brittle structure and separated by force. There are also conventional techniques that use laser light to provide energy to separate the transition substrate from the film above it. At this time, the upper film must absorb the laser light energy and be separated from the transition substrate due to melting ', such as in the early US patent application US20030150843. In this application (please refer to the second figure), a linear laser light 2 3 scans the thin film layer 2 1 on the transition substrate 2 2, and the thin film layer 2 1 can absorb the laser light 2 3 energy and then it can communicate with the substrate. The interface 25 of the material melts and separates from the transition substrate 22, where the transition direction of the transition substrate 22 and the film layer 21 during scanning is shown in the figure, S is the scanning area during one scan, and M Is the scanning width of one scan, and t is the thickness of the thin film layer 21, where the value of the scanning width M is approximately equal to or less than the thickness t. However, this application still has its technical disadvantages. For example, after the entire layer of film is scanned by the linear light source, the degree of melting on the film is not the same; therefore, when the transition substrate 22 is detached, the transition substrate 22 and the film layer 21 are affected by each other. The peeling force is not uniform enough. Furthermore, there is a problem of thermal stress during the linear laser scanning. This uneven thermal stress also makes the peeling effect unsatisfactory, and there is a possibility that the film layer is broken. In view of the shortcomings of the conventional GaN-based vertical structure light-emitting diode (LED) element structure and its manufacturing method, a GaN-based vertical light-emitting diode (LED) structure and the It is necessary to put forward a method for separating a substrate from a film on the structure. SUMMARY OF THE INVENTION In view of the above problems, the main purpose of the present invention is to reduce vertical hair.

200525847 五、發明說明(4) 光二極體結構製造時一薄膜與一過渡基材間加以雷射分離 的不均勻熱應力及融解程度問題。 ' 為達上,目的,本發明之第一態樣在於以一雷射陣列作為 融解能置源’且該雷射陣列照射範圍大小與待融解分開之 薄膜與過渡基材間接觸面近乎相等。 當該雷射陣列之電源一經開啟,陣列中各雷射能量同時為 薄膜面所吸收,薄膜面各處融解程度相當而均勻與過渡基 材分離,且薄膜面不存在熱應力問題而更得均勻脫離與過 渡基材間之貼附。 此外,由於雷射陣列對整個薄膜的照射時間較短,因 此製程時間得以縮短。 本發明之第二態樣為具較佳發光效率之氮化鎵系垂直發光 二極體元件結構,一金屬反射層提供其中以行光反射,以 得較大之光輸出效率。 針對垂直發光二極體(LED)結構,本發明提出一種有 效之製造方法。利用該方法,垂直結構中以藍寶石為材料 之過渡基材與其上方薄膜層間得較均勻分離,且能減少製 請參閱第三圖所示之製程示意圖3〇。圖中,所示結構 34包含過渡基材31及上方之一薄膜層32,其中薄膜結‘之 細節並未顯示圖中,其應包含有n型氮化鎵系層、主動 層、P型氮化鎵系層及金屬基材等,更包括一端之?型電200525847 V. Description of the invention (4) The problem of uneven thermal stress and melting degree of laser separation between a film and a transition substrate during the manufacture of a photodiode structure. In order to achieve the objective, the first aspect of the present invention is to use a laser array as the melting energy source ', and the size of the irradiation range of the laser array is almost equal to the contact surface between the film to be melted and the transition substrate. Once the power of the laser array is turned on, the laser energy in the array is absorbed by the film surface at the same time, the melting degree of the film surface is equivalent and separated from the transition substrate uniformly, and the film surface is more uniform without thermal stress. Adhesion between release and transition substrate. In addition, because the laser array has a shorter irradiation time on the entire film, the process time can be shortened. A second aspect of the present invention is a gallium nitride-based vertical light-emitting diode element structure with better luminous efficiency, and a metal reflective layer provides reflection of traveling light therein to obtain greater light output efficiency. Aiming at the vertical light emitting diode (LED) structure, the present invention proposes an effective manufacturing method. With this method, the sapphire-based transition substrate in the vertical structure is more uniformly separated from the film layer above it, and the manufacturing process can be reduced. Please refer to the process schematic diagram 3 shown in the third figure. In the figure, the structure 34 shown includes a transition substrate 31 and a thin film layer 32 above. The details of the thin film junction are not shown in the figure. It should include an n-type GaN-based layer, an active layer, and a P-type nitrogen. Gallium-based layers and metal substrates, including one end? Type

surface

第9頁 200525847Page 9 200525847

極。該兩材料3 1,3 2需加以分離,分離之方式為過渡基材 3 1上方提供以一雷射陣列3 3,並藉由雷射陣列提供能量; 由於雷射陣列佈於整個薄膜層3 2之上方,故結構3 4不需移 動即可使整個薄膜層3 2受到照射。在此當予指出,圖式中 雷射陣列33雖以ΐχ 3雷射陣列33為之,但其形式實可為任 意適合得均勻投射於接面3 5上者,如lx η陣列、3χ η陣列 等。 當雷射陣列3 3之電源一開啟,雷射陣列3 3便發射出能 量。由於雷射陣列3 3之提供係用於使過渡基材3 1及薄膜層 32間接面35融解,因此雷射陣列之雷射光的波長選擇以使 該雷射光能為該接面3 5吸收並融解、且能穿透基材為原 則,如當該薄膜層32為^型氮化鎵(GaN)系層時,雷射光 波長為約3 2 7奈米。 為使過渡基材3 1與薄膜層3 2間接面3 5得均勻吸收雷射 陣列3 3發出之能量,雷射陣列之設計當以能使整個接面3 5 之能量吸收圖案為均勻為原則。 、在一實施例中,過渡基材3丨與雷射陣列3 3之間得加以 一光拇面(數道狹縫之組合,未示於圖中),藉以使雷射光 源變成長條狀。當長條狀雷射光投射於過渡基材3 1上後, 薄膜層3 2上能量吸收模型應以如第四圖所示者為原則。 如第四圖所示’薄膜層42接面45上有數道能量吸收圖案, 即1st’ 2nd...... ·,nth。該等條狀能量吸收圖案 ^St’ fnd ··· ·,nth係由其上方之光柵面之諸縫隙所形成, 八中每道條狀區域1st,2nd...... ·,nth緊密相接,每一區pole. The two materials 3 1, 3 2 need to be separated. The separation method is to provide a laser array 3 3 above the transition substrate 31 and to provide energy through the laser array. Since the laser array is disposed on the entire thin film layer 3 Above 2, the structure 3 4 can irradiate the entire thin film layer 32 without moving. It should be pointed out here that although the laser array 33 in the figure is a ΐχ 3 laser array 33, its form can be any suitable for uniformly projecting on the interface 35, such as the lx η array, 3χ η Array, etc. When the power of the laser array 33 is turned on, the laser array 33 emits energy. Since the laser array 33 is provided to melt the transition substrate 31 and the indirect surface 35 of the thin film layer 32, the wavelength of the laser light of the laser array is selected so that the laser light can be absorbed by the interface 3 5 and The principle of melting is that it can penetrate the substrate. For example, when the thin film layer 32 is a GaN-type layer, the laser light wavelength is about 3 2 7 nm. In order to make the transition substrate 3 1 and the film layer 3 2 indirectly face 3 5 evenly absorb the energy emitted by the laser array 3 3, the design of the laser array should be based on the principle that the energy absorption pattern of the entire interface 3 5 is uniform. . In one embodiment, a light thumb surface (a combination of several slits, not shown in the figure) must be added between the transition substrate 3 and the laser array 33, so that the laser light source becomes a long strip. . After the long laser light is projected on the transition substrate 31, the energy absorption model on the thin film layer 32 should be based on the principle shown in the fourth figure. As shown in the fourth figure, there are several energy absorption patterns on the interface 45 of the thin film layer 42, namely, 1st '2nd ... ·, nth. The strip energy absorption patterns ^ St 'fnd ····, nth is formed by the gaps of the grating surface above it, and each stripe area in the eighth is 1st, 2nd ... ·, nth is close Docking, each zone

200525847 五、發明說明(6) 域1st,2nd…….,nth内能量吸收強度近乎均勻相等,且各 區域1st,2nd...... .,nt h之吸收能量強度亦近乎均勻相等。 在此另當提出的是,該光柵面得以其它光學零件代替,只 要能使投射於薄膜4 2上之雷射光均勻分佈即可。 第五圖所示為另一能量吸收強度分佈模型實施例,薄 膜層5 2上有複數道吸收圖案,該吸收圖案與第四圖者不 同,此時亦得令薄膜層5 2表面均勻吸收能量而均勻與過渡 基材分離,當然任何其它能使薄膜層5 2表面均勻吸收之強 度吸收模型實施例皆可為之。 欲達成均勻分佈的能量吸收強度均勻分佈模型,雷射 光需再加以處理方能達成,如上述之加入光栅面;此外, 雷射光之其它特性亦得因加調整而更均勻分佈,如調整各 雷射光之投射焦聚等。總之,最後的薄膜吸收雷射光強度 分佈模型以儘量近乎第六圖所示者為原則,其中第六圖表 示薄膜接面之X軸與y軸上各點之吸收能量強度相同。 相較於習用技術,由於本發明投射於薄膜接面之能量 分佈均勻,因此整個薄膜接面上無不均勻熱應力問題,亦 無分離前雷射照射完成時間點不同引發之分離不均勻問 題,因此本發明提出之雷射陣列能量源設計堪為一足以有 效解決習用技術缺點之發明。再者,由於薄膜面上的雷射 照射不需如習用技術般以掃描方式為之,而係一次對整個 薄膜面進行照射,因此製程時間得以大大縮短。 第七圖所示為本發明之氮化鎵系垂直二極體元件結構 7 0,該結構包括有多層薄膜結構與p型電極7 7、η型電極200525847 V. Description of the invention (6) The energy absorption intensity in the domains 1st, 2nd ... ,, nth is almost uniform, and the energy absorption intensity in each region 1st, 2nd, ..., nt h is also nearly uniform. It is also proposed here that the grating surface can be replaced by other optical components, as long as the laser light projected on the film 42 can be uniformly distributed. The fifth figure shows another embodiment of the energy absorption intensity distribution model. There are multiple absorption patterns on the thin film layer 52. The absorption pattern is different from that in the fourth figure. At this time, the surface of the thin film layer 52 can also absorb energy uniformly. And it is uniformly separated from the transition substrate, of course, any other embodiment of the intensity absorption model capable of uniformly absorbing the surface of the film layer 52 can be used. To achieve a uniformly distributed energy absorption intensity uniform distribution model, the laser light needs to be processed before it can be achieved, as described above, the grating surface is added; in addition, other characteristics of the laser light must be more uniformly distributed due to adjustments, such as adjusting each laser Focusing of the projection of light. In short, the final film absorption laser light intensity distribution model is based on the principle as close to that shown in the sixth figure, where the sixth chart shows that the X-axis and y-axis of the film interface have the same absorbed energy intensity at each point. Compared with the conventional technology, because the energy projected on the film interface of the present invention is uniform, there is no problem of uneven thermal stress on the entire film interface, and there is no problem of non-uniform separation caused by different completion time points of laser irradiation before separation. Therefore, the laser array energy source design proposed by the present invention can be an invention that can effectively solve the shortcomings of conventional technology. In addition, since the laser irradiation on the thin film surface does not need to be scanned in a conventional manner as in conventional technology, and the entire thin film surface is irradiated at one time, the process time can be greatly shortened. The seventh figure shows a gallium nitride-based vertical diode device structure 70 of the present invention, which includes a multilayer thin film structure and a p-type electrode 7 7. An n-type electrode

200525847 五、發明說明(7) 78,其中一金屬反射層7 2製作於其中。當主動層7 4發光 時’部份光往ρ型氮化蘇系層7 3行進,金屬反射層7 2對遠 部份光加以反射,使反射光往η型氮化鎵系層7 5—側往結 構7 0外出射,因此發光效率受到提升。此外,該結構7 0之 η型氮化鎵系層7 5與該ρ型氮化鎵系層7 3之位置可互換,構 成本發明之另一實施例(未顯示)。至於金屬反射層7 2之材 料’其可選為與金屬基材7 1貼附匹配度隹、且反射能力佳 者’其中銅鎢合金(CuW)可為金屬基材,此時銀(Ag)、鋁 (A1)、铑(Rh)可為金屬反射層72材料。 ^ 本發明之基本實施例已詳述於上,熟習該項技術者得 藉由對上述實施例之閱讀及了解而推衍出各種不同實施 例#例如,雷射陣列的大小及所發出的雷射光束數量得加 3它Ϊ:接面之強度吸收分佈模型可加改變、光栅面得 改i等I零件替代、雷射光源與薄膜材料之組合亦得做 …之,凡得藉由本發明之發明說Μ ^ 1 ^ 實施例皆厪μ 士 a 0 '明輕易推導出之 白屬於本發明之精神範圍,而該等 申请專利範圍一節中。 祝W疋義於後述200525847 V. Description of the invention (7) 78, in which a metal reflective layer 72 is made. When the active layer 74 emits light, 'part of the light travels toward the p-type nitride nitride system layer 73, and the metal reflective layer 72 reflects the far part of the light, so that the reflected light is directed to the n-type gallium nitride-based layer 7 5— The lateral structure 70 emits light, so the luminous efficiency is improved. In addition, the positions of the n-type gallium nitride-based layer 75 of the structure 70 and the p-type gallium nitride-based layer 73 are interchangeable, and constitute another embodiment (not shown) of the present invention. As for the material of the metal reflective layer 7 2, it can be selected to match the metal substrate 7 1 with a good matching degree, and the reflection ability is good. Among them, copper tungsten alloy (CuW) can be a metal substrate, and silver (Ag) at this time , Aluminum (A1), and rhodium (Rh) can be the material of the metal reflective layer 72. ^ The basic embodiment of the present invention has been described in detail above. Those skilled in the art can derive various embodiments by reading and understanding the above embodiments # For example, the size of the laser array and the emitted laser The number of beams can be increased by 3: the intensity absorption distribution model of the interface can be changed, the grating surface must be changed, such as I parts, and the combination of the laser light source and the thin film material can be made ... The invention says that M ^ 1 ^ The examples are all μ a a 0 ′ The white that is easily deduced belongs to the spirit scope of the present invention, and the scope of these patent applications is in the section. I wish W Yi Yi to be described later

200525847 圖式簡單說明 第1 A及1 B圖為一基材與一薄膜層加以分離之習用製程示意 圖; 第一 C圖為習用技術之垂直發光二極體結構示意圖; 第二圖為習用技術對一基材與一薄膜層加以分離之製程示 意圖; 第三圖為本發明中一以雷射陣列分離薄膜與基材之製程實 施例示意圖; 第四圖為本發明中一薄膜層上吸收能量強度之分佈模型實 施例示意圖; 第五圖為本發明中另一薄膜層上吸收能量強度之分佈模型 實施例示意圖; 第六圖為本發明中薄膜接面各點上理想吸收能量強度之分 佈模型示意圖;及 第七圖為本發明之氮化鎵系垂直發光二極體結構之示意 圖。 10 垂直發光元件結構 11 過渡基材 13 p型氮化銶系層 14 主動層 1 5 η型氮化鎵系層 16 金屬基材 I 0 ’,1 0 ’ ’ 垂直發光元件結構 II ’,1 Γ ’ 過渡基材200525847 Brief description of the drawings. Figures 1 A and 1 B are schematic diagrams of a conventional process for separating a substrate from a thin film layer. Figure 1 C is a schematic diagram of a vertical light emitting diode structure of a conventional technique. A schematic diagram of a process for separating a substrate and a thin film layer; the third diagram is a schematic diagram of an embodiment of a process for separating a film and a substrate with a laser array in the present invention; the fourth diagram is the intensity of energy absorbed on a thin film layer in the present invention A schematic diagram of an embodiment of a distribution model; the fifth diagram is a schematic diagram of an embodiment of a distribution model of absorbed energy intensity on another thin film layer in the present invention; the sixth diagram is a schematic diagram of a distribution model of ideal absorbed energy intensity at each point of the film junction in the present invention And FIG. 7 is a schematic diagram of a gallium nitride-based vertical light-emitting diode structure of the present invention. 10 Vertical light-emitting element structure 11 Transition substrate 13 p-type hafnium nitride-based layer 14 Active layer 1 5 n-type gallium nitride-based layer 16 Metal substrate I 0 ', 1 0' 'Vertical light-emitting element structure II', 1 Γ '' Transition substrate

第13頁 200525847Page 13 200525847

第14頁 圖式簡單說明 13, ,1 3 ’ ’ p型氮化鎵系層 14, ,14’ ’ 主動層 15, ,1 5 ’ ’ η型氮化鎵系層 16, ,16’ ’ 金屬基材 17, 1 7 ’,1 7 ’ ’ ρ型電極 18, ,1 8 ’ ’ η型電極 21 薄膜層 22 過渡基材 23 雷射光 25 接面 31 過渡基材 32 薄膜 33 雷射矩陣光源 35 基材與薄膜層之接面 42 薄膜 45 基材與薄膜間接面 52 薄膜 55 基材與薄膜間接面 70 氮化鎵系垂直發光二極體結構 71 金屬基材 72 金屬反射層 73 Ρ型氮化鎵系層 74 主動層 75 η型氮化鎵系層 200525847 圖式簡單說明 77 p型電極 7 8 η型電極 mil 第15頁Schematic illustrations on page 14, 13, 13, 3 '' p-type GaN-based layer 14, 14, 14 '' active layer 15, 1, 15''n-type gallium nitride-based layer 16, 16, 16 '' metal Substrate 17, 1 7 ', 1 7' 'ρ-type electrode 18, 1 8' 'η-type electrode 21 Thin film layer 22 Transition substrate 23 Laser light 25 Junction 31 Transition substrate 32 Film 33 Laser matrix light source 35 Interface between substrate and film layer 42 film 45 substrate and film indirect surface 52 film 55 substrate and film indirect surface 70 gallium nitride-based vertical light-emitting diode structure 71 metal substrate 72 metal reflective layer 73 p-type nitride Gallium-based layer 74 Active layer 75 η-type GaN-based layer 200525847 Brief description of the diagram 77 p-type electrode 7 8 η-type electrode mil Page 15

Claims (1)

200525847 六、申請專利範圍 1· 一種分離一氮化鎵系垂直發光二極體元件中一藍寶石美 材及一晶體薄膜層之方法’其中該晶體薄祺層貼附於二 藍寶石基材之上,該方法至少包含下列步驟· 提供一雷射陣列於該藍寶石基材之上方,且該雷射陣 列發出之雷射光得至少部份穿透該藍寶石基材二:能為 該晶體薄膜層吸收者; % ^ 以該雷射陣列透過該藍寶石基材而照射該晶體薄膜 層;及 日日/ 、 分開該藍寶石基材與該晶體薄膜層。 2.如申請專利範圍第1項所述之分離一氮化鎵系垂直發光 二極體元件中一藍寶石基材及一晶體薄膜層之方法,其 中該雷射光之波長約為3 2 7奈米。 ’、 3·如申請專利範圍第1項所述之分離一氮化鎵系垂直發光 二極體元件中一藍寶石基材及一晶體薄膜層之方法",其 中該照射晶體薄膜層係照射在該藍寶石基材與該晶體& 膜層之接面上。 ' / 4 ·如申請專利範圍第1項所述之分離一氮化鎵系垂直發光 二極體元件中一藍寶石基材及一晶體薄膜層之方法,其 中該雷射陣列為任意陣列形式之雷射光。 5 · —種分離一基材與一薄膜層之方法,其中該薄膜位於該 基材之上方’該方法至少包含下列步驟: 提供一雷射陣列於該基材之上方,且該雷射陣列發出之 雷射光得至少部份穿透該基材、且能為該薄膜層吸收; 以該雷射陣列透過該基材照射該薄膜層;200525847 VI. Scope of patent application 1. A method for separating a sapphire material and a crystalline thin film layer in a gallium nitride-based vertical light-emitting diode element, wherein the thin crystal layer is attached to a sapphire substrate, The method includes at least the following steps. A laser array is provided above the sapphire substrate, and the laser light emitted by the laser array at least partially penetrates the sapphire substrate 2. It can absorb the crystal thin film layer; % ^ Irradiating the crystalline film layer through the sapphire substrate with the laser array; and separating the sapphire substrate and the crystalline film layer from each other. 2. The method for separating a sapphire substrate and a crystalline thin film layer in a gallium nitride-based vertical light emitting diode device as described in item 1 of the scope of patent application, wherein the wavelength of the laser light is about 3 2 7 nm . ', 3. The method for separating a sapphire substrate and a crystalline thin film layer in a gallium nitride-based vertical light emitting diode element as described in item 1 of the scope of the patent application, wherein the irradiated crystalline thin film layer is irradiated on The interface between the sapphire substrate and the crystal & film layer. '/ 4 · The method for separating a sapphire substrate and a crystalline thin film layer in a gallium nitride-based vertical light-emitting diode device as described in item 1 of the scope of patent application, wherein the laser array is a laser in an arbitrary array form Shoot light. 5 · A method of separating a substrate from a thin film layer, wherein the film is above the substrate 'The method includes at least the following steps: A laser array is provided above the substrate, and the laser array emits The laser light at least partially penetrates the substrate and can be absorbed by the thin film layer; the laser array irradiates the thin film layer through the substrate; 第16頁 200525847 六、申請專利範圍 分開該基材與該薄膜層。 6. 如申請專利範圍第5項所述之分離一基材與一薄膜層之 方法,其中該薄膜層之吸收係為該基材與該與該薄膜層 之接面上的吸收。 7. 如申請專利範圍第5項所述之分離一基材與一薄膜層之 方法,其中該雷射陣列為任意陣列形式之雷射光。 8. —種氮化鎵系垂直發光元件結構,其包含: 一金屬基材; 一金屬反射層,位於該金屬基材上; 一 P型氮化鎵層,位於該金屬反射層上; 一主動層,位於該p型氮化鎵系層上;及 一 η型氮化鎵系層,位於該主動層上, 其中該ρ型氮化鎵系層與該η型氮化鎵層之位置可互 換。 9 .如申請專利範圍第8項所述之氮化鎵系垂直發光元件結 構,其中該金屬基材至少為CuW,而該金屬反射層至少 為 Ag, A1 and Rh〇Page 16 200525847 6. Scope of patent application Separate the substrate from the film layer. 6. The method for separating a substrate and a thin film layer as described in item 5 of the scope of the patent application, wherein the absorption of the thin film layer is the absorption of the substrate and the interface with the thin film layer. 7. The method for separating a substrate and a thin film layer as described in item 5 of the scope of patent application, wherein the laser array is laser light in an arbitrary array form. 8. A gallium nitride-based vertical light emitting element structure, comprising: a metal substrate; a metal reflective layer on the metal substrate; a P-type gallium nitride layer on the metal reflective layer; an active Layer on the p-type gallium nitride-based layer; and an n-type gallium nitride-based layer on the active layer, wherein the positions of the p-type gallium nitride-based layer and the n-type gallium nitride layer are interchangeable . 9. The gallium nitride-based vertical light-emitting device structure according to item 8 of the scope of patent application, wherein the metal substrate is at least CuW, and the metal reflective layer is at least Ag, A1 and Rh. 第17頁Page 17
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