TW201301563A - Optical semiconductor device and manufacturing method of optical semiconductor device - Google Patents

Optical semiconductor device and manufacturing method of optical semiconductor device Download PDF

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TW201301563A
TW201301563A TW101110651A TW101110651A TW201301563A TW 201301563 A TW201301563 A TW 201301563A TW 101110651 A TW101110651 A TW 101110651A TW 101110651 A TW101110651 A TW 101110651A TW 201301563 A TW201301563 A TW 201301563A
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electrode
plating
current
optical semiconductor
semiconductor layer
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TW101110651A
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TWI459595B (en
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Keiichi Sawai
Fujio Agoh
Yuji Watanabe
Katsuji Kawakami
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Sharp Kk
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L2224/00Indexing scheme for arrangements for connecting or disconnecting semiconductor or solid-state bodies and methods related thereto as covered by H01L24/00
    • H01L2224/01Means for bonding being attached to, or being formed on, the surface to be connected, e.g. chip-to-package, die-attach, "first-level" interconnects; Manufacturing methods related thereto
    • H01L2224/10Bump connectors; Manufacturing methods related thereto
    • H01L2224/11Manufacturing methods

Abstract

An optical semiconductor device 10 comprises a first semiconductor layer 12 comprising a first conductive-type semiconductor; a second semiconductor layer 13 comprising a second conductive-type semiconductor and formed on a portion of an upper surface of the first semiconductor layer 12; a first electrode 14a formed on the other portion of the upper surface of the first semiconductor layer 12; a second electrode 14b formed on an upper surface of the second semiconductor layer 13 and having an upper surface arranged at a position higher than an upper surface of the first electrode 14a; a first connecting electrode 52 formed on the upper surface of the first electrode 14a; a second connecting electrode 51 formed on an upper surface of the second electrode; and a protective film 51 covering the surface of the first semiconductor layer 12 and that of the second semiconductor layer 13, and having an opening portion 21 for exposing a portion of the surface of the first semiconductor layer 12.

Description

光半導體元件及光半導體元件之製造方法 Optical semiconductor element and method of manufacturing optical semiconductor element

本發明係關於一種適用於倒裝片安裝之具有連接電極之光半導體元件、及該光半導體元件之製造方法。 The present invention relates to an optical semiconductor element having a connection electrode suitable for flip chip mounting, and a method of manufacturing the same.

發光二極體(LED)係以實現白色化及發光效率之急劇上升等之技術性發展為背景,而被普遍廣泛使用。例如,可舉出普通家庭用之照明及汽車用之頭燈等。 Light-emitting diodes (LEDs) are widely used in the background of technical development such as whitening and a sharp increase in luminous efficiency. For example, lighting for general household use, headlights for automobiles, and the like can be cited.

從發光效率、製造效率及製造成本等的觀點來看,成為現在主流之LED之結構為以下結構。於絕緣性透明基板(藍寶石基板等)上積層n型及p型之氮化鎵系化合物半導體。其後,藉由蝕刻p型層之一部份,將n型層及p型層之表面以具有階差之狀態形成。於n型層及p型層之表面形成電極,進行倒裝片安裝。自LED放射之光透過絕緣性透明基板而照射。 From the viewpoints of luminous efficiency, manufacturing efficiency, manufacturing cost, and the like, the structure of the LED which is currently in the mainstream is the following structure. An n-type and p-type gallium nitride-based compound semiconductor is laminated on an insulating transparent substrate (such as a sapphire substrate). Thereafter, the surface of the n-type layer and the p-type layer is formed in a state having a step by etching one of the p-type layers. An electrode is formed on the surface of the n-type layer and the p-type layer, and flip-chip mounting is performed. The light emitted from the LED is irradiated through the insulating transparent substrate.

對於LED來說,p極及n極之導通狀態均勻對於降低消耗電力及提高耐久性很重要。因此,安裝有倒裝片之LED中,連接電極之形成技術係重要技術。專利文件1中,揭示有一種利用真空鍍膜法與脫膜,於具有階差之LED晶片上形成電極之技術。專利文件2中,揭示有一種利用無電解電鍍,於具有階差之光半導體元件上形成電極之技術。 For the LED, the conduction state of the p-pole and the n-pole is uniform, which is important for reducing power consumption and improving durability. Therefore, in the LED mounted with the flip chip, the formation technique of the connection electrode is an important technique. Patent Document 1 discloses a technique for forming an electrode on an LED chip having a step by vacuum deposition and stripping. Patent Document 2 discloses a technique for forming an electrode on an optical semiconductor element having a step by electroless plating.

[先前技術文獻] [Previous Technical Literature] [專利文獻] [Patent Literature]

[專利文獻1]日本公開專利公報「日本特開平9-232632號 公報(1997年9月5日公開)」 [Patent Document 1] Japanese Laid-Open Patent Publication No. 9-232632 Gazette (public on September 5, 1997)

[專利文獻2]日本公開專利公報「日本特開2004-103975號公報(2004年4月2日公開)」 [Patent Document 2] Japanese Laid-Open Patent Publication No. 2004-103975 (published on April 2, 2004)

[專利文獻3]日本公開專利公報「日本特開平10-64953號公報(1998年3月6日公開)」 [Patent Document 3] Japanese Laid-Open Patent Publication No. 10-64953 (published on March 6, 1998)

然而,專利文獻1及2因形成有相同膜厚之電極,故無法消除LED及光半導體元件具有之階差。因此,實施形成膜厚較厚之電極而在安裝倒裝片時壓壞電極,或使用較上述階差更大之焊球而吸收階差等的方法。該等方法中,雖可吸收上述階差而安裝倒裝片,但不能使導通狀態均勻。 However, in Patent Documents 1 and 2, since the electrodes having the same film thickness are formed, the step difference between the LED and the optical semiconductor element cannot be eliminated. Therefore, a method of forming an electrode having a thick film thickness, crushing the electrode when the flip chip is mounted, or using a solder ball having a larger step than the above to absorb a step or the like is performed. In these methods, the flip chip is mounted while absorbing the above-described step, but the conduction state cannot be made uniform.

另一方面,專利文獻3中揭示有一種利用進行電鍍時,於形成的電鍍層之厚度與開口徑之間有相互關係之技術。在表面高度不同之半導體基板上,藉由使支柱形成部之開口徑變化,而形成高度不同之支柱。據此,抵消半導體基板表面上之階差而安裝倒裝片。但,該技術雖可吸收半導體基板表面上之階差,卻因吸收半導體基板表面上之階差而約束了導電性支柱(連接電極)。 On the other hand, Patent Document 3 discloses a technique in which a relationship between a thickness of a plating layer formed and an opening diameter is used when plating is performed. On the semiconductor substrate having different surface heights, the pillars having different heights are formed by changing the opening diameter of the pillar forming portion. According to this, the flip chip is mounted by offsetting the step on the surface of the semiconductor substrate. However, this technique can absorb the step on the surface of the semiconductor substrate, but constrains the conductive pillar (connecting electrode) by absorbing the step on the surface of the semiconductor substrate.

本發明係鑒於上述問題而完成者,其目的在於提供一種具有適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極之光半導體元件。又,本發明之另一目的在於提供一種可不使各連接電極之尺寸受到約束地形成適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極之光 半導體元件之製造方法。 The present invention has been made in view of the above problems, and an object thereof is to provide an optical semiconductor element having a first connection electrode and a second connection electrode which are suitable for flip chip mounting without stepping therebetween. Further, another object of the present invention is to provide a light for forming a first connection electrode and a second connection electrode which are suitable for flip chip mounting without stepping on each other without restricting the size of each connection electrode. A method of manufacturing a semiconductor element.

為解決上述問題,本發明之一態樣之光半導體元件之特徵為包含:第1半導體層,其包含第1導電型之半導體;第2半導體層,其包含第2導電型之半導體,且形成於上述第1半導體層之上表面的一部份;第1電極,其形成於上述第1半導體層之上表面的另一部份;第2電極,其形成於上述第2半導體層之上表面,且具有位於較上述第1電極之上表面更高之位置的上表面;第1連接電極,其形成於上述第1電極之上表面;第2連接電極,其形成於上述第2電極之上表面;及保護膜,其係覆蓋於上述第1半導體層之表面及上述第2半導體層之表面的絕緣性保護膜,且具有使上述第1半導體層之表面之一部份露出的開口部。 In order to solve the above problems, an optical semiconductor device according to an aspect of the present invention includes a first semiconductor layer including a semiconductor of a first conductivity type, and a second semiconductor layer including a semiconductor of a second conductivity type and formed. a portion of the upper surface of the first semiconductor layer; a first electrode formed on the upper surface of the first semiconductor layer; and a second electrode formed on the upper surface of the second semiconductor layer And having an upper surface located higher than the upper surface of the first electrode; a first connection electrode formed on the upper surface of the first electrode; and a second connection electrode formed on the second electrode And a protective film covering the surface of the first semiconductor layer and the insulating film of the surface of the second semiconductor layer, and having an opening that exposes a part of the surface of the first semiconductor layer.

為解決上述問題,本發明之一態樣之光半導體元件之製造方法之特徵為包含:於光半導體基板之上表面的整面上,形成導電性之電流薄膜之步驟,該光半導體基板包含:基板;形成於該基板之上表面且包含第1導電型之半導體之第1半導體層;包含第2導電型之半導體,且形成於上述第1半導體層之上表面的一部份之第2半導體層;形成於上述第1半導體層之上表面的另一部份之第1電極;形成於上述第2半導體層之上表 面,且具有位於較上述第1電極之上表面更高之位置的上表面之第2電極;及覆蓋於上述第1半導體層之表面及上述第2半導體層之表面的絕緣性保護膜,且具有使上述第1半導體層之表面之一部份露出的開口部之保護膜;及形成上述電流薄膜後,藉由電鍍上述光半導體基板而於上述第1電極之上表面形成第1連接電極,且於上述第2電極之上表面形成第2連接電極之步驟。 In order to solve the above problems, a method of fabricating an optical semiconductor device according to an aspect of the present invention includes the steps of forming a conductive current film on an entire surface of an upper surface of an optical semiconductor substrate, the optical semiconductor substrate comprising: a substrate; a first semiconductor layer including a semiconductor of a first conductivity type formed on an upper surface of the substrate; and a second semiconductor including a semiconductor of a second conductivity type and formed on a surface of the upper surface of the first semiconductor layer a first electrode formed on the other surface of the upper surface of the first semiconductor layer; formed on the second semiconductor layer a second electrode having an upper surface located higher than the upper surface of the first electrode; and an insulating protective film covering the surface of the first semiconductor layer and the surface of the second semiconductor layer, and a protective film having an opening for exposing a portion of the surface of the first semiconductor layer; and after forming the current film, the first connection electrode is formed on the upper surface of the first electrode by plating the optical semiconductor substrate. And forming a second connection electrode on the upper surface of the second electrode.

根據上述構成,本發明之一態樣之光半導體元件中,保護膜覆蓋第1半導體層之表面及第2半導體層之表面。又,保護膜具有使第1半導體層之表面之一部份露出的開口部。 According to the above configuration, in the optical semiconductor device according to the aspect of the invention, the protective film covers the surface of the first semiconductor layer and the surface of the second semiconductor layer. Further, the protective film has an opening that exposes a part of the surface of the first semiconductor layer.

製造該構成之光半導體元件時,藉由使用電鍍而形成第1連接電極及第2連接電極。具體而言,於光半導體基板之上表面之整面上形成電流薄膜,隨後形成在第1及第2電極上開口的光阻圖案,然後於光半導體元件施加電鍍電流。 When the optical semiconductor element of this configuration is manufactured, the first connection electrode and the second connection electrode are formed by using electroplating. Specifically, a current film is formed on the entire surface of the upper surface of the optical semiconductor substrate, and then a photoresist pattern opened on the first and second electrodes is formed, and then a plating current is applied to the optical semiconductor element.

該處,第1電極與電流薄膜係直接導通。又,第1電極與導通之第1半導體層通過保護膜之開口部,而與電流薄膜導通。據此,自第1電極向電流薄膜及第1半導體層雙方流通有電鍍電流。 At this point, the first electrode and the current film are directly turned on. Further, the first electrode and the conductive first semiconductor layer pass through the opening of the protective film to be electrically connected to the current film. As a result, a plating current flows from both the first electrode to the current film and the first semiconductor layer.

另一方面,第2電極雖與電流薄膜直接導通,但與第2電極導通之第2半導體層未在電流薄膜上導通。據此,自第2電極僅於電流薄膜上流通有電鍍電流。 On the other hand, although the second electrode is directly electrically connected to the current film, the second semiconductor layer that is electrically connected to the second electrode is not electrically connected to the current film. Accordingly, a plating current flows only from the second electrode to the current film.

如上所述,在電鍍光半導體基板時,流通之電鍍電流為第1電極側>第2電極側。其結果,藉由控制光半導體元件 中流通之電鍍電流之參數,可形成吸收第1電極及第2電極之階差的相互間無階差之第1連接電極及第2連接電極。此時,只要控制電鍍電流之參數即可,故第1連接電極及第2連接電極之尺寸無任何約束。 As described above, when the optical semiconductor substrate is plated, the plating current flowing therethrough is the first electrode side > the second electrode side. As a result, by controlling the optical semiconductor component The parameters of the plating current flowing therethrough form a first connection electrode and a second connection electrode which absorb the step difference between the first electrode and the second electrode and have no step difference therebetween. In this case, as long as the parameters of the plating current are controlled, the dimensions of the first connection electrode and the second connection electrode are not restricted.

因此,根據本發明之一態樣之光半導體元件之製造方法,可不使各連接電極之尺寸受到約束地形成適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極。又,根據本發明之一態樣之光半導體元件,可實現具有適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極之光半導體元件。 Therefore, according to the method of manufacturing an optical semiconductor device according to an aspect of the present invention, the first connection electrode and the second connection electrode which are suitable for flip chip mounting without stepping therebetween can be formed without constraining the size of each connection electrode. . Further, according to the optical semiconductor device of one aspect of the present invention, it is possible to realize an optical semiconductor element having a first connection electrode and a second connection electrode which are suitable for flip chip mounting without stepping therebetween.

本發明之其他目的、特徵、及優點,可通過以下所示之記載充分理解。又,本發明之優勢,可通過參照附加圖式之說明而明瞭。 Other objects, features, and advantages of the present invention will be apparent from the description appended claims. Further, the advantages of the present invention can be understood by referring to the description of the additional drawings.

本發明係提供一種光半導體元件之製造方法,可不使各連接電極之尺寸受到約束地形成適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極。又,根據本發明之一態樣之光半導體元件,可實現具有適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極之光半導體元件。 The present invention provides a method of manufacturing an optical semiconductor device, which is capable of forming a first connection electrode and a second connection electrode which are suitable for flip chip mounting without stepping, without restricting the size of each connection electrode. Further, according to the optical semiconductor device of one aspect of the present invention, it is possible to realize an optical semiconductor element having a first connection electrode and a second connection electrode which are suitable for flip chip mounting without stepping therebetween.

以下,茲參照圖1~圖8詳細說明本發明之一實施形態。 Hereinafter, an embodiment of the present invention will be described in detail with reference to Figs. 1 to 8 .

[實施形態1] [Embodiment 1] (光半導體元件10之構成) (Configuration of Optical Semiconductor Element 10)

一面參照圖1一面說明本發明之一實施形態之光半導體元件10。 An optical semiconductor device 10 according to an embodiment of the present invention will be described with reference to Fig. 1 .

圖1係顯示本發明之一實施形態之光半導體元件10之構成之簡略圖。光半導體元件10於絕緣性透明基板11之上表面形成有第1導電型半導體層12。且,第1導電型半導體層12之上表面之一部份上形成有第2導電型半導體層13。本實施形態中,作為絕緣性透明基板11係使用藍寶石基板11。本實施形態中,第1導電型半導體層12及第2導電型半導體層13係以包含n型及p型之氮化鎵系化合物半導體而說明。因此,第1導電型半導體層12為n型層12,第2導電型半導體層13為p型層13。本實施形態中,將於藍寶石基板11上形成包含氮化鎵系化合物半導體之n型層及p型層之光半導體基板稱為p-n接面晶圓。 Fig. 1 is a schematic view showing the configuration of an optical semiconductor device 10 according to an embodiment of the present invention. The optical semiconductor element 10 is formed with a first conductive semiconductor layer 12 on the upper surface of the insulating transparent substrate 11. Further, a second conductive semiconductor layer 13 is formed on one surface of the upper surface of the first conductive semiconductor layer 12. In the present embodiment, the sapphire substrate 11 is used as the insulating transparent substrate 11. In the present embodiment, the first conductive semiconductor layer 12 and the second conductive semiconductor layer 13 are described as including a n-type and p-type gallium nitride-based compound semiconductor. Therefore, the first conductive semiconductor layer 12 is the n-type layer 12, and the second conductive semiconductor layer 13 is the p-type layer 13. In the present embodiment, an optical semiconductor substrate in which an n-type layer and a p-type layer including a gallium nitride-based compound semiconductor are formed on a sapphire substrate 11 is referred to as a p-n junction wafer.

n型層12及p型層13之上表面之一部份上,設置有於n型層12之上表面之一部份具有開口部21之絕緣性之保護膜15。又,n型層12中與開口部21對應之區域形成有凹槽22(參照圖1)。 A part of the upper surface of the n-type layer 12 and the p-type layer 13 is provided with an insulating protective film 15 having an opening portion 21 in a portion of the upper surface of the n-type layer 12. Further, a groove 22 is formed in a region of the n-type layer 12 corresponding to the opening portion 21 (see FIG. 1).

n型層12之上表面之一部份及p型層13之上表面之一部份上,設置有n極電極(第1電極)14a及p極電極(第2電極)14b。n極電極14a及p極電極14b包含相同之金屬,具有相同之厚度。由於n型層12之上表面形成有p型層13,故n型層12及p型層13之上表面具有階差。因此,n極電極14a及p極電極14b之上表面亦有階差。 An n-electrode (first electrode) 14a and a p-electrode (second electrode) 14b are provided on a portion of the upper surface of the n-type layer 12 and a portion of the upper surface of the p-type layer 13. The n-electrode electrode 14a and the p-pole electrode 14b comprise the same metal and have the same thickness. Since the p-type layer 13 is formed on the upper surface of the n-type layer 12, the upper surface of the n-type layer 12 and the p-type layer 13 has a step. Therefore, the upper surfaces of the n-electrode electrode 14a and the p-pole electrode 14b also have a step.

製作光半導體元件10之過程中,於包含n極電極14a及p 極電極14b之上表面之上述p-n接面晶圓之整面上,設置有包含二層之電流薄膜33(參照圖2之(b)~(f))。電流薄膜33具有導電性,利用電鍍形成凸塊時,作為用以通過電鍍電流之導電層工作。電流薄膜33包含下層電流薄膜31及上層電流薄膜32。 In the process of fabricating the optical semiconductor device 10, the n-pole electrodes 14a and p are included A current film 33 including two layers is provided on the entire surface of the p-n junction wafer on the upper surface of the electrode electrode 14b (see FIGS. 2(b) to (f)). The current film 33 has electrical conductivity, and when a bump is formed by plating, it functions as a conductive layer for plating current. The current film 33 includes a lower current film 31 and an upper current film 32.

電鍍電流經由電流薄膜33而流經n極電極14a及p極電極14b,n極電極14a及p極電極14b之上,利用電鍍而形成n極凸塊52(第1連接電極)及p極凸塊51(第2連接電極)。n極凸塊52及p極凸塊51分別以不同之厚度形成。n極凸塊52之厚度比p極凸塊51之厚度更厚地形成,消除n型層12及p型層13之上表面具有之階差。因此,n極凸塊52及p極凸塊51之上表面以相同高度形成。 The plating current flows through the n-electrode 14a and the p-electrode 14b, the n-electrode 14a, and the p-electrode 14b via the current film 33, and the n-pole bump 52 (first connection electrode) and the p-pole convex are formed by plating. Block 51 (second connecting electrode). The n-pole bumps 52 and the p-pole bumps 51 are respectively formed with different thicknesses. The thickness of the n-pole bump 52 is formed thicker than the thickness of the p-pole bump 51, eliminating the step difference between the upper surface of the n-type layer 12 and the p-type layer 13. Therefore, the upper surfaces of the n-pole bump 52 and the p-pole bump 51 are formed at the same height.

由於n極凸塊52及p極凸塊51之上表面係以相同之高度形成,故本發明之一實施形態之光半導體元件10可適宜地安裝倒裝片。其後會詳細敍述,但n極凸塊52及p極凸塊51之厚度可不依存於n極電極14a及p極電極14b之面積而得以控制。因此,光半導體元件10,可不約束n極電極14a及p極電極14b之上形成之n極凸塊52及p極凸塊51之尺寸地吸收半導體基板表面上之階差。 Since the upper surfaces of the n-pole bumps 52 and the p-pole bumps 51 are formed at the same height, the optical semiconductor device 10 according to an embodiment of the present invention can be suitably mounted with a flip chip. Although the details will be described later, the thickness of the n-pole bump 52 and the p-pole bump 51 can be controlled independently of the area of the n-pole electrode 14a and the p-pole electrode 14b. Therefore, the optical semiconductor element 10 can absorb the step on the surface of the semiconductor substrate without restricting the size of the n-pole bump 52 and the p-pole bump 51 formed on the n-electrode electrode 14a and the p-pole electrode 14b.

另,本實施形態中,雖作為第1導電型半導體層係使用n型層,作為第2導電型半導體層係使用p型層,但亦可為相反之構成。即,作為第1導電型半導體層使用p型層,作為第2導電型半導體層使用n型層亦可。 In the present embodiment, an n-type layer is used as the first conductive type semiconductor layer, and a p-type layer is used as the second conductive type semiconductor layer. However, the configuration may be reversed. In other words, a p-type layer is used as the first conductive semiconductor layer, and an n-type layer may be used as the second conductive semiconductor layer.

(光半導體元件10之製作方法) (Method of Manufacturing Optical Semiconductor Element 10) (1)電流薄膜之形成 (1) Formation of current film

茲一面參照圖2一面說明光半導體元件10之製作方法。光半導體元件10之製作中,使用藍寶石基板11上形成包含氮化鎵系化合物半導體之n型層及p型層之上述p-n接面晶圓。選擇性蝕刻上述p-n接面晶圓之p型層13而使n型層12露出。該步驟中,使用與先前相同之周知之技術即可。另,上述p-n接面晶圓上形成有複數個光半導體元件10,而圖2中圖示有該等複數個光半導體元件10中的1個。 A method of fabricating the optical semiconductor device 10 will be described with reference to FIG. In the fabrication of the optical semiconductor device 10, the p-n junction wafer including the n-type layer and the p-type layer of the gallium nitride-based compound semiconductor is formed on the sapphire substrate 11. The p-type layer 13 of the p-n junction wafer is selectively etched to expose the n-type layer 12. In this step, the same well-known technique as before can be used. Further, a plurality of optical semiconductor elements 10 are formed on the p-n junction wafer, and one of the plurality of optical semiconductor elements 10 is illustrated in FIG.

於露出之n型層12之上表面與未被蝕刻而剩餘的p型層13之上表面形成包含鎳及金之積層結構之n極電極14a及p極電極14b。作為n極電極14a及p極電極14b,藉由使用包含鎳及金之積層結構,可在n型層12與n極電極14a之接觸界面、及p型層13與p極電極14b之接觸界面中得到良好的歐姆特性。包含Ni(鎳)及Au(金)之積層結構之形成中,使用濺鍍法、真空鍍膜法等之技術即可。電極形成等步驟之圖案化中,例如使用光微影法即可。 An n-electrode 14a and a p-electrode 14b including a laminated structure of nickel and gold are formed on the upper surface of the exposed n-type layer 12 and the upper surface of the p-type layer 13 which is not etched. As the n-electrode electrode 14a and the p-electrode electrode 14b, a contact interface between the n-type layer 12 and the n-pole electrode 14a and a contact interface between the p-type layer 13 and the p-electrode electrode 14b can be used by using a laminated structure including nickel and gold. Good ohmic properties are obtained. In the formation of a laminated structure including Ni (nickel) and Au (gold), a technique such as a sputtering method or a vacuum coating method may be used. In the patterning of steps such as electrode formation, for example, photolithography may be used.

形成n極電極14a及p極電極14b後,於n型層12及p型層13之上表面形成作為絕緣性之保護膜15之SiO2(二氧化矽)。形成保護膜15後,自n極電極14a及p極電極14b之一部份及開口部21中除去保護膜15。進而僅選擇性蝕刻n型層12,而於開口部21對應之區域形成凹槽22。該狀態顯示於圖2(a)。 After the n-electrode electrode 14a and the p-pole electrode 14b are formed, SiO 2 (cerium oxide) as an insulating protective film 15 is formed on the upper surfaces of the n-type layer 12 and the p-type layer 13. After the protective film 15 is formed, the protective film 15 is removed from a portion of the n-electrode electrode 14a and the p-electrode electrode 14b and the opening portion 21. Further, only the n-type layer 12 is selectively etched, and the groove 22 is formed in a region corresponding to the opening portion 21. This state is shown in Fig. 2(a).

開口部21及凹槽22之形狀,更好的是,自上面觀察光半導體元件10時,係以開口部21及凹槽22包圍光半導體元件 10之周圍,分離各個光半導體元件10之形狀形成。 The shape of the opening portion 21 and the recess 22 is more preferably such that the optical semiconductor element 10 is surrounded by the opening portion 21 and the recess 22 when the optical semiconductor element 10 is viewed from above. Around the periphery of 10, the shape of each of the optical semiconductor elements 10 is separated.

形成具有開口部21之保護膜15及凹槽22後,形成用以流通電鍍電流之電流薄膜33。如圖2之(b)所示,電流薄膜33包含下層電流薄膜31及上層電流薄膜32。作為構成下層電流薄膜31之材料,例如TiW較適宜。藉由將TiW設為下層電流薄膜31,可抑制n型層12與上層電流薄膜32之間之原子的擴散。同樣的,亦可抑制n極電極14a及p極電極14b與上層電流薄膜32之間之原子的擴散。TiW可利用例如濺鍍法而堆積。 After the protective film 15 having the opening portion 21 and the recess 22 are formed, a current film 33 for circulating a plating current is formed. As shown in FIG. 2(b), the current film 33 includes a lower current film 31 and an upper current film 32. As a material constituting the lower current film 31, for example, TiW is suitable. By making TiW the lower layer current film 31, diffusion of atoms between the n-type layer 12 and the upper layer current film 32 can be suppressed. Similarly, the diffusion of atoms between the n-electrode electrode 14a and the p-electrode electrode 14b and the upper layer current film 32 can be suppressed. TiW can be deposited by, for example, sputtering.

構成上層電流薄膜32之材料使用與形成凸塊之電鍍金屬相同之金屬。藉由對上層電流薄膜32使用與形成凸塊之電鍍金屬相同之金屬,可提高介隔電流薄膜之n極電極14a及p極電極14b與凸塊之密著性,亦可提高光半導體元件10之耐久性。本實施形態中,因使用Au作為構成凸塊之材料,故亦使用Au作為構成上層電流薄膜32之材料。上層電流薄膜32可利用例如濺鍍法堆積。 The material constituting the upper current film 32 is made of the same metal as the plating metal forming the bump. By using the same metal as the plating metal forming the bumps for the upper current film 32, the adhesion between the n-electrode electrode 14a and the p-electrode electrode 14b of the current-intercepting film and the bump can be improved, and the optical semiconductor element 10 can be improved. Durability. In the present embodiment, since Au is used as the material constituting the bump, Au is also used as the material constituting the upper layer current film 32. The upper current film 32 can be deposited by, for example, sputtering.

形成電流薄膜33時,在形成有保護膜15、n極電極14a及p極電極14b之區域中,電流薄膜33與n型層12不直接接觸(參照圖2之(b))。另一方面,藉由設置有開口部21,電流薄膜33亦形成於開口部21及凹槽22之內側。藉由將電流薄膜33形成至開口部21及凹槽22之內側,使電流薄膜33與n型層12直接接觸,成為電性導通之狀態。詳如後述,藉由在開口部21使電流薄膜33與n型層12導通,可利用電鍍而於n極電極14a及p極電極14b之上形成厚度不同之凸塊。 When the current film 33 is formed, the current film 33 and the n-type layer 12 are not in direct contact with each other in the region where the protective film 15, the n-electrode 14a, and the p-electrode 14b are formed (see FIG. 2(b)). On the other hand, the current film 33 is also formed inside the opening portion 21 and the recess 22 by providing the opening portion 21. By forming the current film 33 to the inside of the opening 21 and the recess 22, the current film 33 is brought into direct contact with the n-type layer 12, and is electrically connected. As will be described later, by forming the current film 33 and the n-type layer 12 in the opening portion 21, bumps having different thicknesses can be formed on the n-electrode electrode 14a and the p-pole electrode 14b by electroplating.

在形成電流薄膜33之元件上,利用例如旋塗法而塗佈光阻41(參照圖2之(c))。其後,使用光微影法,於與n極電極14a及p極電極14b對應之位置上,形成作為光阻41之開口部之凸塊形成圖案42(參照圖2之(d))。 On the element forming the current film 33, the photoresist 41 is applied by, for example, spin coating (see (c) of Fig. 2). Thereafter, a bump forming pattern 42 as an opening portion of the photoresist 41 is formed at a position corresponding to the n-electrode electrode 14a and the p-pole electrode 14b by photolithography (see (d) of FIG. 2).

(2)利用電鍍之凸塊形成 (2) Using electroplated bump formation

形成凸塊形成圖案42後,利用電鍍形成n極凸塊52及p極凸塊51。光半導體元件10之製作中,使用p-n接面晶圓。於上述p-n接面晶圓之上表面形成之電流薄膜33不僅形成於光半導體元件10之製作區域,亦形成至上述p-n接面晶圓之外周部。藉由將外部電源之陰極30連接於上述p-n接面晶圓之外周部之電流薄膜33,而將電流薄膜33作為電鍍之一個電極。 After the bump formation pattern 42 is formed, the n-pole bump 52 and the p-pole bump 51 are formed by plating. In the fabrication of the optical semiconductor device 10, a p-n junction wafer is used. The current film 33 formed on the upper surface of the p-n junction wafer is formed not only in the fabrication region of the optical semiconductor device 10 but also on the outer peripheral portion of the p-n junction wafer. The current film 33 is used as one of the electroplated electrodes by connecting the cathode 30 of the external power source to the current film 33 on the outer peripheral portion of the p-n junction wafer.

於包含與電鍍之金屬相同之材料或適宜之材料之陽極板81上連接外部電源之陽極80,藉此作為電鍍之另一個電極。本實施形態中,使用Pt(白金)之板作為陽極板81。 An anode 80 of an external power source is connected to the anode plate 81 containing the same material as the plated metal or a suitable material, thereby serving as the other electrode for electroplating. In the present embodiment, a plate of Pt (platinum) is used as the anode plate 81.

將連接有陰極30之上述p-n接面晶圓及連接有陽極80之陽極板81浸漬於電鍍液中,自外部電源流通電鍍電流。本實施形態中,為形成包含金之凸塊,而使用金電鍍液。電鍍液之溫度及電鍍液所含之金屬離子濃度等物理條件係以不在電鍍過程中變動之方式予以管理。 The p-n junction wafer to which the cathode 30 is connected and the anode plate 81 to which the anode 80 is connected are immersed in the plating solution, and a plating current flows from the external power source. In the present embodiment, a gold plating solution is used to form a bump including gold. Physical conditions such as the temperature of the plating solution and the concentration of metal ions contained in the plating solution are managed in such a manner that they do not change during the plating process.

利用電鍍而形成之膜之電鍍率依存於電鍍之區域中流通之電鍍電流之電流值(更精確為電流密度)。此處,對於n極電極14a及p極電極14b中流通之電流值之大小關係加以說明。 The plating rate of the film formed by electroplating depends on the current value (more precisely, the current density) of the plating current flowing in the area of the plating. Here, the magnitude relationship between the current values flowing through the n-electrode electrode 14a and the p-pole electrode 14b will be described.

自陰極30至開口部21之電流路徑對n極電極14a與p極電極14b為共用。因此,n極電極14a及p極電極14b中流通之電流值依存於自開口部21至n極電極14a之電流路徑及自開口部21至p極電極14b之電流路徑。 The current path from the cathode 30 to the opening 21 is common to the n-electrode 14a and the p-electrode 14b. Therefore, the current values flowing through the n-electrode electrode 14a and the p-electrode electrode 14b depend on the current path from the opening portion 21 to the n-pole electrode 14a and the current path from the opening portion 21 to the p-electrode electrode 14b.

於開口部21與n極電極14a之間形成之電流路徑中,經由開口部21及凹槽22,使電流薄膜33及n型層12導通。且,亦導通n型層12之上表面與n極電極14a。因此,陰極30與n極電極14a之間之電流電路包含電流薄膜33與n型層12之並聯電路(參照圖3)。 In the current path formed between the opening 21 and the n-electrode 14a, the current film 33 and the n-type layer 12 are electrically connected via the opening 21 and the groove 22. Further, the upper surface of the n-type layer 12 and the n-electrode electrode 14a are also turned on. Therefore, the current circuit between the cathode 30 and the n-electrode 14a includes a parallel circuit of the current film 33 and the n-type layer 12 (refer to FIG. 3).

另一方面,p極電極14b與n型層12之間,存在有p型層13(參照圖1)。n型層12與p型層13之接觸界面上形成有p-n接面層。當電鍍之時,n極電極14a及p極電極14b之間產生之電位差,與上述p-n接面層之勢壘高度相比極小。因此,介隔p型層13,n型層12與p極電極14b未導通。因此,開口部21與p極電極14b之間形成之電流路徑為僅根據電流薄膜33之串聯電路(參照圖3)。 On the other hand, a p-type layer 13 exists between the p-electrode electrode 14b and the n-type layer 12 (see FIG. 1). A p-n junction layer is formed on the contact interface between the n-type layer 12 and the p-type layer 13. When electroplating, the potential difference generated between the n-electrode electrode 14a and the p-electrode electrode 14b is extremely small compared to the barrier height of the p-n junction layer. Therefore, the n-type layer 12 and the p-electrode electrode 14b are not electrically connected to each other through the p-type layer 13. Therefore, the current path formed between the opening portion 21 and the p-electrode electrode 14b is a series circuit based only on the current film 33 (refer to FIG. 3).

比較僅根據電流薄膜33之串聯電路之電阻值與包含電流薄膜33及n型層12之並聯電路之電阻值之大小關係之情形,包含電流薄膜33及n型層12之並聯電路之電阻值較小。因此,自開口部21至n極電極14a之電阻值,小於自開口部21至p極電極14b之電阻值。因此,陰極30與n極電極14a之間之電阻值,小於陰極30與p極電極14b之間之電阻值。 Comparing only the magnitude relationship between the resistance value of the series circuit of the current film 33 and the resistance value of the parallel circuit including the current film 33 and the n-type layer 12, the resistance value of the parallel circuit including the current film 33 and the n-type layer 12 is compared. small. Therefore, the resistance value from the opening portion 21 to the n-pole electrode 14a is smaller than the resistance value from the opening portion 21 to the p-pole electrode 14b. Therefore, the resistance value between the cathode 30 and the n-electrode 14a is smaller than the resistance between the cathode 30 and the p-electrode 14b.

因電阻值與電流值成反比之關係,故n極電極14a與電鍍 液之間,較p極電極14b與電鍍液之間流通有較大之電鍍電流。其結果,n極電極14a上,形成有較p極凸塊51厚度更厚之n極凸塊52(參照圖2之(e))。 Since the resistance value is inversely proportional to the current value, the n-pole electrode 14a and plating Between the liquids, a larger plating current flows between the p-electrode electrode 14b and the plating solution. As a result, an n-pole bump 52 having a thicker thickness than the p-pole bump 51 is formed on the n-electrode electrode 14a (see FIG. 2(e)).

p極凸塊51及n極凸塊52之厚度,係為消除因n型層12之上表面形成有p型層13所引起之階差而形成。其結果,p極凸塊51及n極凸塊52之上表面形成為相同之高度。關於p極凸塊51及n極凸塊52之厚度之控制方法請容後述。 The thickness of the p-pole bump 51 and the n-pole bump 52 is formed by eliminating the step caused by the p-type layer 13 formed on the upper surface of the n-type layer 12. As a result, the upper surfaces of the p-pole bumps 51 and the n-pole bumps 52 are formed to have the same height. The method of controlling the thickness of the p-pole bump 51 and the n-pole bump 52 will be described later.

本實施形態中,使用Au作為n極凸塊52及p極凸塊51之材料。然而,作為Au以外之材料,亦可將Ag(銀)、Pt(白金)、Cu(銅)、Pd(鈀)、Ni(鎳)、焊錫、及包含該等之合金作為n極凸塊52及p極凸塊51之材料任意使用。更好的是,構成n極凸塊52及p極凸塊51之材料與構成上層電流薄膜32之材料相同。因此,Ag、Pt、Cu、Pd、Ni、焊錫、及包含該等之合金亦可作為上層電流薄膜32之材料使用。 In the present embodiment, Au is used as the material of the n-pole bump 52 and the p-pole bump 51. However, as a material other than Au, Ag (silver), Pt (platinum), Cu (copper), Pd (palladium), Ni (nickel), solder, and an alloy containing the same may be used as the n-pole bump 52. The material of the p-pole bump 51 is used arbitrarily. More preferably, the material constituting the n-pole bump 52 and the p-pole bump 51 is the same as the material constituting the upper layer current film 32. Therefore, Ag, Pt, Cu, Pd, Ni, solder, and an alloy containing the same may be used as the material of the upper layer current film 32.

藉由使用Au、Ag、Pt、Cu、Pd、Ni、焊錫、及包含該等之合金作為n極凸塊52及p極凸塊51之材料,將光半導體元件10進行倒裝片安裝時,可得到良好之歐姆特性。 When the optical semiconductor element 10 is flip-chip mounted by using Au, Ag, Pt, Cu, Pd, Ni, solder, and the alloy containing the same as the material of the n-pole bump 52 and the p-pole bump 51, Good ohmic properties are obtained.

形成n極凸塊52及p極凸塊51之後,使用有機溶劑除去光阻41(參照圖2之(f))。其結果,於p極電極14b上介隔電流薄膜33而形成p極凸塊51,於n極電極14a上介隔電流薄膜33而形成n極凸塊52。 After the n-pole bump 52 and the p-pole bump 51 are formed, the photoresist 41 is removed using an organic solvent (see (f) of FIG. 2). As a result, the p-electrode 33 is interposed on the p-electrode 14b to form the p-pole bump 51, and the current film 33 is interposed on the n-electrode 14a to form the n-pole bump 52.

其後,藉由自處於圖2之(f)之狀態之元件中除去電流薄膜33,完成圖2(g)所示之光半導體元件10。為除去電流薄膜33,可將處於圖2之(f)之狀態之元件浸漬於可蝕刻構成 下層電流薄膜31及上層電流薄膜32之金屬之蝕刻液中。 Thereafter, the optical semiconductor element 10 shown in Fig. 2(g) is completed by removing the current film 33 from the element in the state of (f) of Fig. 2 . In order to remove the current film 33, the element in the state of (f) of FIG. 2 can be immersed in an etchable composition. The metal current etching solution of the lower current film 31 and the upper current film 32.

最後,藉由分割上述p-n接面晶圓,自上述p-n接面晶圓擷取各個光半導體元件10。藉由使光半導體元件10具有凹槽22,可在將上述p-n接面晶圓以特定大小分割時,不於n型層12上產生缺陷地進行分割。 Finally, each of the optical semiconductor elements 10 is drawn from the p-n junction wafer by dividing the p-n junction wafer. By providing the optical semiconductor element 10 with the recess 22, when the p-n junction wafer is divided by a specific size, the division can be performed without causing defects on the n-type layer 12.

利用上述之製作方法,可提供p極凸塊51及n極凸塊52之上表面形成為相同之高度之適於倒裝片安裝之光半導體元件10。p極凸塊51及n極凸塊52之厚度係根據p極電極14b及n極電極14a中流通之電鍍電流之電流值而控制。因而,本發明之一實施形態之光半導體元件之製造方法中,p極凸塊51及n極凸塊52之尺寸不受約束。 According to the above manufacturing method, the optical semiconductor element 10 suitable for flip chip mounting in which the upper surfaces of the p-pole bumps 51 and the n-pole bumps 52 are formed to have the same height can be provided. The thicknesses of the p-pole bumps 51 and the n-pole bumps 52 are controlled based on the current values of the plating currents flowing through the p-electrode electrodes 14b and the n-electrode electrodes 14a. Therefore, in the method of manufacturing an optical semiconductor device according to an embodiment of the present invention, the size of the p-pole bump 51 and the n-pole bump 52 is not restricted.

(凸塊之厚度控制方法) (Bump thickness control method)

茲一面參照圖1~7一面說明控制p極凸塊51及n極凸塊52之厚度之方法 A method of controlling the thickness of the p-pole bump 51 and the n-pole bump 52 will be described with reference to FIGS. 1-7.

(1)電鍍電流電路 (1) Electroplating current circuit

光半導體元件10之製作中,使用p-n接面晶圓。將連接有陰極30之上述p-n接面晶圓及連接有陽極80之陽極板81浸漬於電鍍液中,藉由自外部電源流通電鍍電流而實施電鍍。此時之電鍍電流電路之等價電路顯示於圖3。 In the fabrication of the optical semiconductor device 10, a p-n junction wafer is used. The p-n junction wafer to which the cathode 30 is connected and the anode plate 81 to which the anode 80 is connected are immersed in a plating solution, and plating is performed by circulating a plating current from an external power source. The equivalent circuit of the plating current circuit at this time is shown in FIG.

設置於上述p-n接面晶圓上之電流薄膜33與陰極30實際上係連接在相同部位。然而,電流薄膜33係設置於上述p-n接面晶圓之全區域,故著眼於1組n極電極14a及p極電極14b之情形,n極電極14a及p極電極14b與陰極30之電流路徑係無數地存在。本實施形態中,為簡單說明,以對應圖 2所示之剖面圖之形式而圖示圖3。圖2之(d)之狀態之元件中,電鍍電流係自n極電極14a及p極電極14b向電流薄膜33之左右兩端流通。為顯示此點,圖3中將2個陰極30描繪於開口部21之外側。 The current film 33 and the cathode 30 provided on the p-n junction wafer are actually connected to the same portion. However, since the current film 33 is provided over the entire area of the pn junction wafer, the current path of the n-pole electrode 14a and the p-pole electrode 14b and the cathode 30 is focused on the case of one set of the n-electrode electrode 14a and the p-pole electrode 14b. There are countless places. In the present embodiment, for the sake of simplicity, Figure 3 is shown in the form of a cross-sectional view shown in Fig. 2. In the element of the state of (d) of FIG. 2, the plating current flows from the n-electrode electrode 14a and the p-electrode electrode 14b to the left and right ends of the current film 33. To show this, in FIG. 3, two cathodes 30 are drawn on the outer side of the opening 21.

陽極80與陽極板81實際上亦係連接在相同部位。然而,為成為與陰極30相對應之形式,以使陽極80亦存在於陽極板81之兩端之方式圖示(參照圖3)。 The anode 80 and the anode plate 81 are actually connected to the same portion. However, in order to be in a form corresponding to the cathode 30, the anode 80 is also present on both ends of the anode plate 81 (see FIG. 3).

陰極30在上述p-n接面晶圓之外周部連接於電流薄膜33上。上述p-n接面晶圓上為可製作複數個光半導體元件10而配置有圖案。因此,於上述p-n接面晶圓上,設置有複數個開口部21及凹槽22,且在各個開口部21及凹槽22中電流薄膜33與n型層12導通。因此,自陰極30至開口部21之電流路徑包含電流薄膜33及n型層12。然而,為簡化說明,省略自陰極30至開口部21之電流路徑,而以無電阻成份者顯示於圖3。另,為簡化說明,凹槽22亦未於圖3中圖示。 The cathode 30 is connected to the current film 33 at the outer periphery of the p-n junction wafer. A pattern is formed on the p-n junction wafer in which a plurality of optical semiconductor elements 10 can be formed. Therefore, a plurality of openings 21 and recesses 22 are provided on the p-n junction wafer, and the current film 33 and the n-type layer 12 are electrically connected to the respective openings 21 and 22. Therefore, the current path from the cathode 30 to the opening portion 21 includes the current film 33 and the n-type layer 12. However, for simplification of explanation, the current path from the cathode 30 to the opening portion 21 is omitted, and is shown in Fig. 3 as a non-resistance component. In addition, the recess 22 is also not illustrated in FIG. 3 for simplicity of explanation.

n極電極14a及p極電極14b與陽極板81係經由電鍍液而導通。圖3中,電鍍液之電阻值為RbathThe n-electrode electrode 14a and the p-pole electrode 14b and the anode plate 81 are electrically connected via a plating solution. In Fig. 3, the resistance value of the plating solution is R bath .

圖3中顯示之2個開口部21係與圖2之(d)之2個開口部21相對應。圖2之(d)中,於2個開口部21及凹槽22之間設置有電流薄膜33,電流薄膜33之中途存在有n極電極14a及p極電極14b。即,2個開口部21及凹槽22與n極電極14a、p極電極14b,分別係介隔電流薄膜33而導通。圖3中之14a及14b係表示n極電極14a及p極電極14b,Rcf表示電流薄膜33 之電阻值。 The two opening portions 21 shown in Fig. 3 correspond to the two opening portions 21 of Fig. 2(d). In (d) of FIG. 2, a current film 33 is provided between the two openings 21 and the grooves 22, and an n-pole electrode 14a and a p-pole electrode 14b are present in the middle of the current film 33. In other words, the two openings 21 and the recesses 22, the n-electrode electrode 14a, and the p-electrode 14b are electrically connected to each other via the current film 33. 14a and 14b in Fig. 3 show an n-electrode electrode 14a and a p-electrode electrode 14b, and Rcf represents a resistance value of the current film 33.

電鍍電流流通電流薄膜33之同時,亦經由開口部21及凹槽22流通於n型層12。開口部21中於電流薄膜33及n型層12接觸之界面上,存在有連接電阻Rop。開口部21及凹槽22之表面積越大,則電流薄膜33及n型層12之接觸面積越增大,故Rop越小。圖3中,R1為n型層12之電阻值。藉由使電鍍電流流通於電流薄膜33及n型層12,而於n極電極14a與開口部21之間形成並聯電路(參照圖3)。另一方面,p極電極14b與開口部21僅介隔電流薄膜33而導通。 The plating current flows through the current film 33, and also flows through the opening portion 21 and the groove 22 to the n-type layer 12. In the opening portion 21, at the interface where the current film 33 and the n-type layer 12 are in contact, there is a connection resistance R op . The larger the surface area of the opening portion 21 and the recess 22, the larger the contact area between the current film 33 and the n-type layer 12 is, so the smaller the R op is . In Fig. 3, R 1 is the resistance value of the n-type layer 12. By causing a plating current to flow through the current film 33 and the n-type layer 12, a parallel circuit is formed between the n-electrode electrode 14a and the opening portion 21 (see FIG. 3). On the other hand, the p-electrode electrode 14b and the opening portion 21 are electrically connected only by the current film 33.

n極電極14a與開口部21之間形成有包含Rcf、R1及Rop之並聯電路,p極電極14b與開口部21之間形成有僅包含Rcf之串聯電路。因此,n極電極14a與開口部21之間之電阻值小於p極電極14b與開口部21之間之電阻值。 A parallel circuit including R cf , R 1 , and R op is formed between the n-electrode 14 a and the opening 21 , and a series circuit including only R cf is formed between the p-electrode 14 b and the opening 21 . Therefore, the resistance value between the n-electrode electrode 14a and the opening portion 21 is smaller than the resistance value between the p-electrode electrode 14b and the opening portion 21.

n極電極14a中流通有較p極電極14b大之電鍍電流,其結果,n極電極14a之電鍍率較p極電極14b之電鍍率高。其結果,n極凸塊52之厚度亦較p極凸塊51之厚度厚。本實施形態中,將n極電極14a之電鍍率與p極電極14b之電鍍率之比稱為電鍍率比。 A plating current larger than that of the p-electrode 14b flows through the n-electrode electrode 14a, and as a result, the plating rate of the n-electrode electrode 14a is higher than that of the p-electrode electrode 14b. As a result, the thickness of the n-pole bumps 52 is also thicker than the thickness of the p-pole bumps 51. In the present embodiment, the ratio of the plating rate of the n-electrode electrode 14a to the plating rate of the p-electrode electrode 14b is referred to as a plating ratio.

(2)電鍍率比之控制 (2) Electroplating rate ratio control

藉由對n極電極14a與開口部21間之電阻值、與p極電極14b與開口部21間之電阻值賦與差,而對n極電極14a及p極電極14b中流通之電鍍電流賦與差。如此,藉由控制n極電極14a與開口部21間之電阻值、與p極電極14b與開口部21間之電阻值,而可控制n極電極14a及p極電極14b之電鍍 率。n極電極14a與開口部21間之電阻值及p極電極14b與開口部21間之電阻值之電阻值差,更好為n極電極14a與開口部21間之電阻值之10%左右。其結果,可有效地控制n極電極14a之電鍍率與p極電極14b之電鍍率之比率。 By applying a difference between the resistance value between the n-electrode electrode 14a and the opening portion 21 and the resistance value between the p-electrode electrode 14b and the opening portion 21, the plating current flowing through the n-electrode electrode 14a and the p-electrode electrode 14b is given. And poor. Thus, by controlling the resistance between the n-electrode 14a and the opening 21 and the resistance between the p-electrode 14b and the opening 21, the plating of the n-electrode 14a and the p-electrode 14b can be controlled. rate. The resistance value between the n-electrode electrode 14a and the opening portion 21 and the resistance value of the resistance value between the p-electrode electrode 14b and the opening portion 21 are preferably about 10% of the resistance value between the n-electrode electrode 14a and the opening portion 21. As a result, the ratio of the plating rate of the n-electrode electrode 14a to the plating rate of the p-electrode electrode 14b can be effectively controlled.

光半導體元件10之製作中所用之p-n接面晶圓之n型層12之薄片電阻為1~20 Ω/□。因此,電流薄膜33之薄片電阻較好為10 mΩ/□~1000 mΩ/□之範圍內,進而,更好為50 mΩ/□至200 mΩ/□。電流薄膜33之薄片電阻依存於電流薄膜33之膜厚。若增加該膜厚則薄片電阻會變小,若減小該膜厚則薄片電阻會變大。 The sheet resistance of the n-type layer 12 of the p-n junction wafer used in the fabrication of the optical semiconductor device 10 is 1 to 20 Ω/□. Therefore, the sheet resistance of the current film 33 is preferably in the range of 10 mΩ/□ to 1000 mΩ/□, and more preferably 50 mΩ/□ to 200 mΩ/□. The sheet resistance of the current film 33 depends on the film thickness of the current film 33. When the film thickness is increased, the sheet resistance becomes small, and if the film thickness is decreased, the sheet resistance becomes large.

如此,可將電流薄膜33之膜厚作為參數而控制電流薄膜33之薄片電阻。藉由設定電流薄膜33之薄片電阻為上述之範圍,可設定n極電極14a與開口部21間之電阻值及p極電極14b與開口部21間之電阻值之電阻值的差為10%左右。 Thus, the sheet resistance of the current film 33 can be controlled by using the film thickness of the current film 33 as a parameter. By setting the sheet resistance of the current film 33 to the above range, the difference between the resistance value between the n-electrode electrode 14a and the opening portion 21 and the resistance value between the p-electrode electrode 14b and the opening portion 21 can be set to about 10%. .

電流薄膜33之薄片電阻較小之情形下,電鍍電流大多流通於電流薄膜33。因此,流通於n極電極14a與p極電極14b之各個電鍍電流之差變小,電鍍率比變為近於1之值。電流薄膜33之薄片電阻較大之情形下,流通於n型層12之電鍍電流增加,流通於n極電極14a與p極電極14b之各個電鍍電流之差變大。因此,電鍍率比變為大於1之值。如此,藉由變換電流薄膜33之膜厚,可變化電鍍率比。因此,藉由設電流薄膜33之膜厚為適宜之值,可形成相互間無階差之p極凸塊51及n極凸塊52。 When the sheet resistance of the current film 33 is small, the plating current mostly flows through the current film 33. Therefore, the difference between the plating currents flowing through the n-electrode electrode 14a and the p-electrode electrode 14b becomes small, and the plating ratio becomes a value close to 1. When the sheet resistance of the current film 33 is large, the plating current flowing through the n-type layer 12 increases, and the difference between the plating currents flowing through the n-electrode electrode 14a and the p-electrode electrode 14b becomes large. Therefore, the plating ratio becomes a value larger than 1. Thus, by changing the film thickness of the current film 33, the plating rate ratio can be changed. Therefore, by setting the film thickness of the current film 33 to an appropriate value, the p-pole bumps 51 and the n-pole bumps 52 having no step difference therebetween can be formed.

作為對n極電極14a與開口部21間之電阻值、p極電極14b 與開口部21間之電阻值賦與差之其他方法,亦可變化電流薄膜33及n型層12之連接電阻Rop。即使Rcf與R1相同之情形,只要Rop變大,n極電極14a與開口部21間之電阻值就變大。相反,若Rop變小,則n極電極14a與開口部21間之電阻值亦變小。另一方面,即使Rop變化,p極電極14b與開口部21間之電阻值仍不變。Rop係依存於開口部21及凹槽22之表面積,故藉由使該表面積變化,可變化n極電極14a與開口部21間之電阻值、及p極電極14b與開口部21間之電阻值之比。換而言之,藉由將開口部21之圖案尺寸設計成任意之大小,可控制電鍍率比(參照圖6)。圖6之開口部之面積比率係相對n型層12所形成之區域之面積,開口部21之表面積所占之比例。 As another method of imparting a difference between the resistance value between the n-electrode electrode 14a and the opening portion 21 and the resistance value between the p-electrode electrode 14b and the opening portion 21, the connection resistance Rop of the current film 33 and the n-type layer 12 may be changed. . Even when R cf is the same as R 1 , as long as R op becomes large, the resistance value between the n-electrode electrode 14a and the opening portion 21 becomes large. On the contrary, when R op becomes small, the resistance value between the n-electrode electrode 14a and the opening portion 21 also becomes small. On the other hand, even if R op changes, the resistance value between the p-electrode electrode 14b and the opening portion 21 does not change. R op depends on the surface area of the opening 21 and the recess 22, so that the resistance between the n-electrode 14a and the opening 21 and the resistance between the p-electrode 14b and the opening 21 can be changed by changing the surface area. The ratio of values. In other words, by designing the pattern size of the opening portion 21 to an arbitrary size, the plating ratio can be controlled (refer to FIG. 6). The area ratio of the opening portion of Fig. 6 is the ratio of the area of the area formed by the n-type layer 12 to the surface area of the opening portion 21.

如上所述,開口部21之表面積較好為可利用電鍍形成相互間無階差之p極凸塊51及n極凸塊52之表面積。根據該構成,製造光半導體元件10時,可確實地形成相互間無階差之p極凸塊51及n極凸塊52。 As described above, the surface area of the opening portion 21 is preferably a surface area of the p-pole bump 51 and the n-pole bump 52 which can be formed by plating without stepping therebetween. According to this configuration, when the optical semiconductor element 10 is manufactured, the p-pole bumps 51 and the n-pole bumps 52 having no step difference therebetween can be surely formed.

又。凹槽22之表面積較好為可利用電鍍形成相互間無階差之p極凸塊51及n極凸塊52之表面積。根據該構成,製造光半導體元件10時,可確實地形成相互間無階差之p極凸塊51及n極凸塊52。 also. The surface area of the recess 22 is preferably a surface area of the p-pole bump 51 and the n-pole bump 52 which can be formed by electroplating without stepping between them. According to this configuration, when the optical semiconductor element 10 is manufactured, the p-pole bumps 51 and the n-pole bumps 52 having no step difference therebetween can be surely formed.

如上所述,藉由控制n極電極14a及p極電極14b中流通之電鍍電流,可使n極凸塊52及p極凸塊51之電鍍率比變化。然而,為了消除n型層12及p型層13之階差,要將n極凸塊52及p極凸塊51之上表面設為相同之高度,要求更精密之 電鍍率比之控制。 As described above, by controlling the plating current flowing through the n-electrode electrode 14a and the p-electrode electrode 14b, the plating ratio of the n-pole bump 52 and the p-pole bump 51 can be changed. However, in order to eliminate the step difference between the n-type layer 12 and the p-type layer 13, the upper surfaces of the n-pole bump 52 and the p-pole bump 51 are set to the same height, which requires more precision. The plating rate is controlled.

為更精密地控制電鍍率比,本申請案之一實施形態之光半導體元件之製造方法中,將電鍍電流之驅動波形作為脈衝波形。藉由使脈衝波形之脈衝週期變化,可控制電鍍率比。 In order to control the plating ratio more precisely, in the method of manufacturing an optical semiconductor device according to an embodiment of the present application, a driving waveform of a plating current is used as a pulse waveform. The plating ratio can be controlled by changing the pulse period of the pulse waveform.

設n極電極14a及p極電極14b之上表面之階差為D,所期望之p極凸塊51之高度為H。設n極電極14a之電鍍率相對p極電極14b之電鍍率之比為電鍍率比R。此時,為將p極凸塊51及n極凸塊52之上表面形成為相同高度所需之電鍍率比R以下式表示。 The step of the upper surface of the n-electrode electrode 14a and the p-pole electrode 14b is D, and the height of the desired p-pole bump 51 is H. The ratio of the plating rate of the n-electrode electrode 14a to the plating rate of the p-electrode electrode 14b is set to be the plating ratio R. At this time, the plating ratio R is required to form the upper surfaces of the p-pole bumps 51 and the n-pole bumps 52 at the same height.

R=(H+D)/H電鍍率比之脈衝週期依存性,只要例如如圖4所示之圖般預先測定即可。使用預先測定之電鍍率比之脈衝週期依存性,在光半導體元件10之凸塊形成時選擇與所需之R相對應之電鍍電流之脈衝週期。藉由使用如此選定之脈衝週期而形成凸塊,可得到以相同高度形成p極凸塊51及n極凸塊52之上表面之光半導體元件10。 The R=(H+D)/H plating ratio is proportional to the pulse period dependency, and may be measured in advance, for example, as shown in FIG. The pulse period of the plating current corresponding to the desired R is selected at the time of bump formation of the optical semiconductor element 10 using the pre-measured plating ratio as compared with the pulse period dependency. By forming the bumps using the pulse period thus selected, the optical semiconductor element 10 in which the upper surfaces of the p-pole bumps 51 and the n-pole bumps 52 are formed at the same height can be obtained.

藉由使電鍍電流之驅動波形為脈衝波形,除了可實現電鍍率比之精密控制以外,還可防止形成之凸塊成為所謂燒焦電鍍之異常之電鍍狀態。圖5顯示p極凸塊51及n極凸塊152。其顯示p極凸塊51表示正常形成之凸塊,n極凸塊152表示成為所謂燒焦電鍍之狀態之凸塊之例。燒焦電鍍係因長時間流通大電流之電鍍電流而形成之電鍍中易產生之異常。本實施形態之光半導體元件之製造方法中,於n極電 極14a中流通有較p極電極14b更大之電流。於n極電極14a中流通有大電鍍電流之狀態中,將驅動波形作為直流波形之情形下,形成之凸塊有可能成為燒焦電鍍。藉由使電鍍電流之驅動波形為脈衝波形,可排除該可能性。 By making the driving waveform of the plating current into a pulse waveform, in addition to the precise control of the plating rate ratio, it is possible to prevent the formed bump from becoming an abnormal plating state of so-called burnt plating. FIG. 5 shows a p-pole bump 51 and an n-pole bump 152. It is shown that the p-pole bumps 51 represent the bumps formed normally, and the n-pole bumps 152 represent the examples of the bumps in the state of the so-called burnt plating. The scorch plating is an abnormality that is easily generated in electroplating due to a plating current of a large current flowing for a long period of time. In the method of manufacturing an optical semiconductor device according to the embodiment, the n-pole is electrically A larger current is flown through the pole 14a than the p-pole electrode 14b. In the state where a large plating current flows in the n-electrode electrode 14a, in the case where the driving waveform is a DC waveform, the bump formed may be burnt-plated. This possibility can be eliminated by making the driving waveform of the plating current a pulse waveform.

(3)脈衝週期 (3) Pulse period

本發明之一實施形態之光半導體元件之製造方法中,更好的是,電鍍電流之驅動波形為脈衝波形,脈衝週期為0.1秒至100秒之範圍。自圖4所示之電鍍率比之脈衝週期依存性可知,脈衝週期為0.1秒至100秒之範圍中電鍍率比顯現對脈衝週期較大之依存性。因此,藉由將電鍍電流之脈衝週期設定為0.1秒至100秒之範圍內,可得到所期望之電鍍率比。 In the method of manufacturing an optical semiconductor device according to an embodiment of the present invention, it is more preferable that the driving waveform of the plating current is a pulse waveform, and the pulse period is in the range of 0.1 second to 100 seconds. The plating rate shown in Fig. 4 is more dependent on the pulse period dependency, and the plating ratio is in the range of 0.1 second to 100 seconds, and the plating ratio is more dependent on the pulse period. Therefore, by setting the pulse period of the plating current to be in the range of 0.1 second to 100 seconds, the desired plating ratio can be obtained.

施加電鍍電流之後立即於n極電極14a及p極電極14b之表面形成電雙層。自電鍍電流之施加之後立即成為對電雙層充電電鍍電流(非法拉第電流)充電之過渡狀態,約30秒後電鍍電流之電流值收斂到特定值。藉由利用該電鍍狀態之過渡狀態,在本發明之一實施形態之光半導體元件之製造方法中控制電鍍率比。藉由使電鍍電流為脈衝波形,可反複利用電鍍電流之過渡狀態。因此,可確實地控制電鍍率比。 Immediately after the plating current is applied, an electric double layer is formed on the surfaces of the n-electrode electrode 14a and the p-pole electrode 14b. Immediately after the application of the plating current, it becomes a transition state for charging the electric double layer charging plating current (illegal pulling current), and the current value of the plating current converges to a specific value after about 30 seconds. The plating ratio is controlled in the method of manufacturing an optical semiconductor device according to an embodiment of the present invention by utilizing the transition state of the plating state. By making the plating current a pulse waveform, the transition state of the plating current can be repeatedly used. Therefore, the plating ratio can be surely controlled.

(4)工作週期比 (4) Work cycle ratio

本發明之一實施形態之光半導體元件之製造方法,更好的是,脈衝週期之工作週期比為80%以上,或,脈衝週期之電鍍電流之停止時間為2秒以下。製造光半導體元件 時,從產出效能之觀點來看,利用電鍍而形成凸塊所需之時間(作為電鍍時間)越短越好。基於縮短電鍍時間之觀點,較好為使用直流波形之電鍍(作為直流電鍍),但不能控制電鍍率比。再者,有可能因電鍍電流穩定流通而導致燒焦電鍍。電鍍使用脈衝波形之電鍍電流,設定脈衝波形之工作週期比為80%以上,藉此,除可控制電鍍率比以外,還可將電鍍時間之增加相對直流電鍍之情形控制在20%以內。為提高產出,雖希望提高工作週期比,但設定近於100%之值會提高產生燒焦電鍍之可能性。工作週期比之上限值為小於100%之值,且,為可排除產生燒焦電鍍之可能性之值。 In the method of manufacturing an optical semiconductor device according to an embodiment of the present invention, it is more preferable that the duty cycle ratio of the pulse period is 80% or more, or the stop time of the plating current of the pulse period is 2 seconds or less. Manufacturing optical semiconductor components At the time of output efficiency, the time required for forming bumps by electroplating (as plating time) is as short as possible. From the viewpoint of shortening the plating time, it is preferred to use a DC waveform plating (as a DC plating), but it is not possible to control the plating ratio. Furthermore, there is a possibility that the plating current is stably circulated to cause burnt plating. The electroplating current of the pulse waveform is used for electroplating, and the duty cycle ratio of the pulse waveform is set to be 80% or more. Therefore, in addition to controlling the plating ratio, the increase of the plating time can be controlled within 20% with respect to the DC plating. In order to increase the output, although it is desirable to increase the duty cycle ratio, setting a value close to 100% will increase the possibility of causing burnt plating. The duty cycle is less than 100% of the upper limit value, and is a value that excludes the possibility of causing burnt plating.

又,藉由使脈衝波形之一週期之電鍍電流之停止時間為2秒以下,可控制電鍍率比而將產出之降低控制為最小限,且可防止燒焦電鍍之形成。電鍍電流之停止時間之下限值為大於0秒之值,且,為可排除產生燒焦電鍍之可能性之值。 Further, by setting the stop time of the plating current for one cycle of the pulse waveform to 2 seconds or less, the plating rate ratio can be controlled to minimize the decrease in output, and the formation of scorch plating can be prevented. The lower limit of the stop time of the plating current is a value greater than 0 seconds, and is a value excluding the possibility of causing burnt plating.

(5)電鍍電流密度 (5) Electroplating current density

本發明之一實施形態之光半導體元件之製造方法,藉由使具有脈衝波形之電鍍電流之電流密度可變,而變化電鍍率比。換而言之,作為用以控制電鍍率比之參數,可使用電鍍電流之電流密度。 In the method of manufacturing an optical semiconductor device according to an embodiment of the present invention, the plating ratio is changed by changing the current density of the plating current having a pulse waveform. In other words, as a parameter for controlling the plating rate ratio, the current density of the plating current can be used.

可產生良好之電鍍之電流密度之範圍,係依存於電鍍所使用之電鍍液之種類,及以電鍍液之pH、溫度、有無攪拌為代表之電鍍液條件而變化。然而,藉由使電流密度變 化,在控制電鍍平比之情形下,電流密度只要為滿足後述之臨界電流密度之下限值至上限值之範圍之範圍即可。換而言之,電流密度之範圍為臨界電流密度之下限值至上限值之範圍以內即可。 The range of current density at which good plating can be produced varies depending on the type of plating solution used for electroplating, and the plating solution conditions represented by the pH, temperature, and presence or absence of stirring of the plating solution. However, by making the current density change In the case of controlling the plating ratio, the current density may be in a range that satisfies the range from the lower limit value to the upper limit value of the critical current density described later. In other words, the range of the current density is within the range from the lower limit of the critical current density to the upper limit.

臨界電流密度係指利用電鍍而產生覆蓋膜時,產生正常之覆蓋膜之電流密度的上限及下限。電鍍時之電流密度低於臨界電流密度之下限時會產生光澤電鍍,另一方面,高於臨界電流密度之上限時會產生燒焦電鍍(表面之變色、色斑)。光澤電鍍及燒焦電鍍均不佳故避免為好。 The critical current density refers to an upper limit and a lower limit of the current density at which a normal coating film is produced when a coating film is formed by electroplating. Gloss plating is produced when the current density at the time of electroplating is lower than the lower limit of the critical current density, and on the other hand, scorch plating (discoloration of the surface, stain) occurs when the upper limit of the critical current density is exceeded. Gloss plating and charring plating are not good, so avoid it.

藉由使電鍍時之電流密度大於臨界電密度之下限值,可於作為被電鍍面之n極電極14a及p極電極14b上正常地產生電鍍。又,藉由使電流密度小於臨界電密度之上限值,可防止被稱為燒焦電鍍之異常的電鍍狀態之產生。藉此,可形成正常形狀之p極凸塊51及n極凸塊52。又,藉由在臨界電流密度之下限值至上限值之範圍中設電流密度為適宜之值,可形成相互間無階差之p極凸塊51及n極凸塊52。 By making the current density at the time of plating larger than the lower limit of the critical electric density, plating can be normally performed on the n-electrode electrode 14a and the p-electrode electrode 14b as the surface to be plated. Further, by making the current density smaller than the upper limit of the critical electric density, it is possible to prevent the occurrence of an abnormal plating state called scorch plating. Thereby, the p-pole bumps 51 and the n-pole bumps 52 of a normal shape can be formed. Further, by setting the current density to a suitable value in the range from the lower limit value of the critical current density to the upper limit value, the p-pole bump 51 and the n-pole bump 52 having no step difference therebetween can be formed.

[實施例1] [Example 1]

本發明之一實施形態之光半導體元件10之製造方法中,電鍍率比之脈衝週期依存性之測定結果顯示於圖4。光半導體元件10之製造方法係以圖2所示之製造方法為標準。經過圖2之(a)~(d)之步驟後,利用電鍍形成凸塊(參照圖2之(e))。其凸塊形成之時,使作為脈衝波形之電鍍電流之脈衝頻率在0.1秒至1000秒之範圍內變化,將n極凸塊52之厚度與p極凸塊51之厚度之比作為電鍍率比顯示於圖4。 In the method of manufacturing the optical semiconductor device 10 according to the embodiment of the present invention, the measurement results of the plating rate ratio and the pulse period dependency are shown in Fig. 4 . The manufacturing method of the optical semiconductor element 10 is based on the manufacturing method shown in FIG. After the steps (a) to (d) of Fig. 2, bumps are formed by electroplating (refer to Fig. 2 (e)). When the bump is formed, the pulse frequency of the plating current as the pulse waveform is varied in the range of 0.1 second to 1000 seconds, and the ratio of the thickness of the n-pole bump 52 to the thickness of the p-pole bump 51 is used as the plating ratio. Shown in Figure 4.

圖4中用空心圓表示實測值。波狀線係作為擬合實測值之結果而得到之曲線。將利用直流電鍍所得到的電鍍率比以實線圖示。 The measured values are indicated by open circles in Fig. 4. The wavy line is obtained as a result of fitting the measured values. The plating ratio obtained by direct current plating is shown by a solid line.

自圖4之結果可知,在電鍍電流之脈衝週期為0.1秒至100秒之範圍內,電鍍率比會自約1.00至1.25之間大幅變化。因此,藉由自0.1秒至100秒之範圍中選擇電鍍電流之脈衝週期,可得到適宜之電鍍率比。 As can be seen from the results of Fig. 4, the plating ratio is greatly changed from about 1.00 to 1.25 in the range of the pulse period of the plating current from 0.1 second to 100 seconds. Therefore, by selecting the pulse period of the plating current from the range of 0.1 second to 100 seconds, a suitable plating ratio can be obtained.

為決定電鍍電流之脈衝週期,首先,根據n極電極14a與p極電極14b之階差、及欲形成之p極凸塊51之厚度決定必要之電鍍率比。其後,自圖4中讀取上述必要之電鍍率比相對應之脈衝週期即可。 In order to determine the pulse period of the plating current, first, the necessary plating ratio is determined according to the step difference between the n-electrode electrode 14a and the p-electrode electrode 14b and the thickness of the p-pole bump 51 to be formed. Thereafter, the above-mentioned necessary plating ratio is read from the corresponding pulse period in FIG.

[實施例2] [Embodiment 2]

本發明之一實施形態之光半導體元件10之製造方法中,將測定開口部21之面積比率與電鍍率比之關係之實驗結果顯示於圖6中。本實施例之電鍍條件如下。 In the method of manufacturing the optical semiconductor device 10 according to the embodiment of the present invention, an experimental result of measuring the relationship between the area ratio of the opening portion 21 and the plating ratio is shown in Fig. 6 . The plating conditions of this embodiment are as follows.

.電鍍液:EEJA製非氰基型金電鍍液 . Plating solution: non-cyano type gold plating solution made of EEJA

.電鍍浴溫度:52℃ . Electroplating bath temperature: 52 ° C

.電鍍電流密度:直流6 mA/cm2 . Plating current density: DC 6 mA/cm 2

.被電鍍物:光半導體元件製作用晶圓(6寸) . Electroplated material: wafer for optical semiconductor device fabrication (6 inch)

上述條件下,使用無開口部21之晶圓(開口比率0%)及形成有開口部21之晶圓(開口比率6%),進行電鍍。其結果,如圖6所示,得到開口部21之面積比率為0%(開口比率0%)之情形時電鍍率比為約1.00,開口部21之面積比率為6%(開口比率6%)之情形時電鍍率比為約1.30之結果。如此 可知,藉由變化開口部21之面積比率,可控制電鍍率比。 Under the above conditions, the wafer was formed using the wafer having no opening 21 (opening ratio: 0%) and the wafer on which the opening 21 was formed (opening ratio: 6%). As a result, as shown in FIG. 6, when the area ratio of the opening portion 21 is 0% (opening ratio 0%), the plating ratio is about 1.00, and the area ratio of the opening portion 21 is 6% (opening ratio 6%). In the case of the case, the plating ratio is about 1.30. in this way It can be seen that the plating ratio can be controlled by changing the area ratio of the opening portion 21.

[實施例3] [Example 3]

本發明之一實施形態之光半導體元件10之製造方法中,將測定電鍍率比之電流密度依存性之結果顯示於圖7中。本實施例之電鍍條件如下。 In the method of manufacturing the optical semiconductor device 10 according to the embodiment of the present invention, the result of measuring the plating ratio to the current density dependency is shown in Fig. 7 . The plating conditions of this embodiment are as follows.

.電鍍液:EEJA製非氰基型金電鍍液 . Plating solution: non-cyano type gold plating solution made of EEJA

.電鍍浴溫度:52℃ . Electroplating bath temperature: 52 ° C

.脈衝週期:1秒 . Pulse period: 1 second

.工作週期比:80% . Work cycle ratio: 80%

.被電鍍物:光半導體元件製作用晶圓(6寸) . Electroplated material: wafer for optical semiconductor device fabrication (6 inch)

.電鍍電流:在3.5 mA/cm2至11 mA/cm2之範圍內可變 . Plating current: variable from 3.5 mA/cm 2 to 11 mA/cm 2

上述電鍍條件之臨界電流密度之範圍為2 mA/cm2至8 mA/cm2。使電鍍電流之電流密度在3.5 mA/cm2至11 mA/cm2之範圍內變化而進行電鍍。在超過臨界電流密度之範圍之條件下仍進行電鍍係為確認電流密度對所形成之凸塊的影響。實驗之結果,所得到之電鍍率比大約在1.45至1.10之範圍內變化,電鍍率比與電流密度之間存在明確之負相關關係(圖7)。又,可知在臨界電流密度之範圍內,藉由變化電鍍電流之電流密度,可得到期望之電鍍率比。 The critical current density of the above plating conditions ranges from 2 mA/cm 2 to 8 mA/cm 2 . Electroplating was performed by changing the current density of the plating current in the range of 3.5 mA/cm 2 to 11 mA/cm 2 . Electroplating is still performed under conditions exceeding the critical current density to confirm the influence of current density on the formed bumps. As a result of the experiment, the resulting electroplating rate was varied from about 1.45 to 1.10, and there was a clear negative correlation between the electroplating ratio and the current density (Fig. 7). Further, it can be seen that a desired plating ratio can be obtained by varying the current density of the plating current within the range of the critical current density.

[實施例4] [Example 4]

本發明之一實施形態之光半導體元件10之製造方法中,測定電流薄膜33之薄片電阻與電鍍率比之關係之實驗結果,顯示於圖8。本實施例之電鍍條件如下。 In the method for producing an optical semiconductor device 10 according to an embodiment of the present invention, an experimental result of measuring the relationship between the sheet resistance of the current film 33 and the plating ratio is shown in FIG. The plating conditions of this embodiment are as follows.

.電鍍液:EEJA製非氰基型金電鍍液 . Plating solution: non-cyano type gold plating solution made of EEJA

.電鍍浴溫度:50℃ . Electroplating bath temperature: 50 ° C

.電鍍電流密度:直流6 mA/cm2 . Plating current density: DC 6 mA/cm 2

.被電鍍物:光半導體元件製作用晶圓(6寸) . Electroplated material: wafer for optical semiconductor device fabrication (6 inch)

上述條件下,變化各種電流薄膜33之薄片電阻之值,測定電鍍率比。變化薄片電阻之值時,變化電流薄膜33之膜厚。實驗之結果,得到薄片電阻為10 mΩ/□以上之情形,薄片電阻越高電鍍率比更高之結果。即,發現薄片電阻與電鍍率比為正相關關係。如此,可知藉由變化電流薄膜33之薄片電阻,可控制電鍍率比。另,薄片電阻為200 mΩ/□以上之情形,導致n極產生燒焦電鍍之結果。 Under the above conditions, the values of the sheet resistances of the various current films 33 were varied, and the plating ratio was measured. When the value of the sheet resistance is changed, the film thickness of the current film 33 is changed. As a result of the experiment, a sheet resistance of 10 mΩ/□ or more was obtained, and the higher the sheet resistance, the higher the plating ratio. That is, it was found that the sheet resistance and the plating ratio were positively correlated. Thus, it can be seen that the plating ratio can be controlled by varying the sheet resistance of the current film 33. In addition, the sheet resistance is 200 mΩ/□ or more, resulting in the result of burnt plating of the n-pole.

[實施形態2] [Embodiment 2]

參照圖9及圖10說明本發明之一實施形態之光半導體元件60。另,與實施形態1相同之構件附註相同之材料序號,省略其說明。 An optical semiconductor device 60 according to an embodiment of the present invention will be described with reference to Figs. 9 and 10 . The same components as those in the first embodiment are denoted by the same reference numerals, and their description will be omitted.

(光半導體元件60) (Opto Semiconductor Element 60)

光半導體元件60係實施形態1之光半導體元件10之變化例。光半導體元件10與光半導體元件60相比較之不同點在於光半導體元件60具有之n型層62(第1導電型半導體層)及光半導體元件10具有之n型層12之形狀(參照圖9)。光半導體元件60具有之n型層62於與保護膜15所具有之開口部21相對應之區域中不具有特別結構。即,在與開口部21相對應之區域中,n型層62之上表面為平面。 The optical semiconductor element 60 is a modification of the optical semiconductor element 10 of the first embodiment. The optical semiconductor element 10 is different from the optical semiconductor element 60 in that the optical semiconductor element 60 has an n-type layer 62 (first conductive type semiconductor layer) and an optical semiconductor element 10 having an n-type layer 12 shape (refer to FIG. 9). ). The n-type layer 62 of the optical semiconductor element 60 does not have a special structure in a region corresponding to the opening portion 21 of the protective film 15. That is, in the region corresponding to the opening portion 21, the upper surface of the n-type layer 62 is a flat surface.

n型層之形狀以外之構成,在光半導體元件10及光半導體元件60中共通。 The configuration other than the shape of the n-type layer is common to the optical semiconductor element 10 and the optical semiconductor element 60.

n極凸塊52之厚度較p極凸塊51之厚度更厚地形成,而消除n型層12及p型層13之上表面具有之階差。由於n極凸塊52及p極凸塊51之上表面形成為相同高度,故本發明之一實施形態之光半導體元件60可適宜地安裝倒裝片。 The thickness of the n-pole bump 52 is formed thicker than the thickness of the p-pole bump 51, and the step on the upper surface of the n-type layer 12 and the p-type layer 13 is eliminated. Since the upper surfaces of the n-pole bumps 52 and the p-pole bumps 51 are formed at the same height, the optical semiconductor element 60 of one embodiment of the present invention can be suitably mounted with a flip chip.

(光半導體元件60之製作方法) (Method of Manufacturing Optical Semiconductor Element 60)

一面參照圖10一面說明光半導體元件60之製作方法。關於製作方法,光半導體元件60與光半導體元件10相同。 A method of fabricating the optical semiconductor element 60 will be described with reference to FIG. Regarding the manufacturing method, the optical semiconductor element 60 is the same as the optical semiconductor element 10.

自藍寶石基板11上堆積有n型層62及p型層13之p-n接面晶圓,保留p型層13之一部份而選擇性地蝕刻n型層62。於n型層62及p型層13之上表面上形成n極電極14a及p極電極14b,於n型層62之上表面之一部份上形成具有開口部21之保護膜15(參照圖10(a))。此時,n型層62不具有凹槽,n型層62之上表面為平面。 A p-n junction wafer in which an n-type layer 62 and a p-type layer 13 are deposited from the sapphire substrate 11 is left, and one portion of the p-type layer 13 is left to selectively etch the n-type layer 62. An n-electrode electrode 14a and a p-pole electrode 14b are formed on the upper surface of the n-type layer 62 and the p-type layer 13, and a protective film 15 having an opening portion 21 is formed on a portion of the upper surface of the n-type layer 62 (refer to the figure). 10(a)). At this time, the n-type layer 62 does not have a groove, and the upper surface of the n-type layer 62 is a flat surface.

然後,依序形成下層電流薄膜31及上層電流薄膜32,作為電流薄膜33(圖10之(b))。 Then, the lower current film 31 and the upper current film 32 are sequentially formed as the current film 33 ((b) of FIG. 10).

形成電流薄膜33後,依序進行以下步驟。塗佈光阻41(參照圖10之(c))。利用光微影法形成凸塊形成圖案42(圖10之(d))。藉由使用脈衝波形之驅動電流之電鍍而形成p極凸塊51及n極凸塊52(參照圖10之(e))。使用有機溶劑除去光阻41(參照圖10之(f))。將不需要之部份之電流薄膜33經蝕刻而除去(參照圖10之(g))。藉由以上步驟完成光半導體元件60。 After the current film 33 is formed, the following steps are sequentially performed. The photoresist 41 is applied (refer to (c) of FIG. 10). The bump forming pattern 42 is formed by photolithography ((d) of FIG. 10). The p-pole bumps 51 and the n-pole bumps 52 are formed by plating using a driving current of a pulse waveform (refer to (e) of FIG. 10). The photoresist 41 is removed using an organic solvent (refer to (f) of FIG. 10). The unnecessary portion of the current film 33 is removed by etching (refer to (g) of FIG. 10). The optical semiconductor element 60 is completed by the above steps.

形成電流薄膜33之後,即使n型層62之上表面為平面,仍經由開口部21使電流薄膜33與n型層62接觸而導通。因 此,自開口部21至n極電極14a之電流路徑為包含電流薄膜33與n型層62之並聯電路。另一方面,自開口部21至p極電極14b之電流路徑僅為電流薄膜33。 After the current film 33 is formed, even if the upper surface of the n-type layer 62 is flat, the current film 33 is brought into contact with the n-type layer 62 via the opening portion 21 to be electrically connected. because Thus, the current path from the opening portion 21 to the n-pole electrode 14a is a parallel circuit including the current film 33 and the n-type layer 62. On the other hand, the current path from the opening portion 21 to the p-pole electrode 14b is only the current film 33.

因此,開口部21至n極電極14a之電阻值小於開口部21至p極電極14b之電阻值。因n極電極14a中流通有較p極電極14b更大之電鍍電流,故n極電極14a之電鍍率高於p極電極14b之電鍍率。 Therefore, the resistance value of the opening portion 21 to the n-pole electrode 14a is smaller than the resistance value of the opening portion 21 to the p-pole electrode 14b. Since a plating current larger than that of the p-electrode 14b flows through the n-electrode electrode 14a, the plating rate of the n-electrode electrode 14a is higher than that of the p-electrode electrode 14b.

電鍍之驅動波形使用脈衝波形,變化脈衝週期,藉此可控制n極電極14a之電鍍率與p極電極14b之電鍍率之電鍍率比。因此,光半導體元件60為不約束n極凸塊52及p極凸塊51之尺寸,可吸收半導體基板表面上之階差,且適於倒裝片安裝之光半導體元件。 The driving waveform of the plating uses a pulse waveform to change the pulse period, whereby the plating ratio of the plating rate of the n-electrode electrode 14a and the plating rate of the p-electrode electrode 14b can be controlled. Therefore, the optical semiconductor element 60 is a size that does not constrain the size of the n-pole bump 52 and the p-pole bump 51, absorbs the step on the surface of the semiconductor substrate, and is suitable for flip-chip mounted optical semiconductor elements.

(總結) (to sum up)

本發明之一態樣之光半導體元件,為解決上述問題,其特徵為包含:第1半導體層,其包含第1導電型之半導體;第2半導體層,其包含第2導電型之半導體,且形成於上述第1半導體層之上表面的一部份;第1電極,其形成於上述第1半導體層之上表面的另一部份;第2電極,其形成於上述第2半導體層之上表面,且具有位於較上述第1電極之上表面更高之位置的上表面;第1連接電極,其形成於上述第1電極之上表面;第2連接電極,其形成於上述第2電極之上表面;及 保護膜,其係覆蓋於上述第1半導體層之表面及上述第2半導體層之表面的絕緣性保護膜,且具有使上述第1半導體層之表面之一部份露出的開口部。 In order to solve the above problems, an optical semiconductor device according to an aspect of the present invention includes a first semiconductor layer including a semiconductor of a first conductivity type, and a second semiconductor layer including a semiconductor of a second conductivity type, and a portion formed on an upper surface of the first semiconductor layer; a first electrode formed on the upper surface of the first semiconductor layer; and a second electrode formed on the second semiconductor layer a surface having an upper surface located higher than a surface of the first electrode; a first connection electrode formed on an upper surface of the first electrode; and a second connection electrode formed on the second electrode Upper surface; and The protective film covers an insulating protective film covering the surface of the first semiconductor layer and the surface of the second semiconductor layer, and has an opening that exposes a part of the surface of the first semiconductor layer.

本發明之一態樣之光半導體元件之製造方法,為解決上述問題,其特徵為包含:於光半導體基板之上表面的整面上,形成導電性之電流薄膜之步驟,該光半導體基板包含:基板;形成於該基板之上表面且包含第1導電型之半導體之第1半導體層;包含第2導電型之半導體,且形成於上述第1半導體層之上表面的一部份之第2半導體層;形成於上述第1半導體層之上表面的另一部份之第1電極;形成於上述第2半導體層之上表面,且具有位於較上述第1電極之上表面更高之位置的上表面之第2電極;及覆蓋於上述第1半導體層之表面及上述第2半導體層之表面的絕緣性保護膜,且具有使上述第1半導體層之表面之一部份露出的開口部之保護膜;及形成上述電流薄膜後,藉由電鍍上述光半導體基板而於上述第1電極之上表面形成第1連接電極,且於上述第2電極之上表面形成第2連接電極之步驟。 In order to solve the above problems, a method for manufacturing an optical semiconductor device according to an aspect of the present invention includes the step of forming a conductive current film on an entire surface of an upper surface of an optical semiconductor substrate, the optical semiconductor substrate including a substrate; a first semiconductor layer including a semiconductor of a first conductivity type formed on an upper surface of the substrate; and a second semiconductor layer including a semiconductor of a second conductivity type and formed on a surface of the upper surface of the first semiconductor layer a semiconductor layer; a first electrode formed on the other surface of the upper surface of the first semiconductor layer; formed on the upper surface of the second semiconductor layer and having a higher position than the upper surface of the first electrode a second electrode on the upper surface; and an insulating protective film covering the surface of the first semiconductor layer and the surface of the second semiconductor layer, and having an opening for exposing a part of the surface of the first semiconductor layer a protective film; and after forming the current film, forming a first connection electrode on the upper surface of the first electrode by plating the photo-semiconductor substrate, and forming a surface on the upper surface of the second electrode The second step of connecting the electrodes.

根據上述構成,本發明之一態樣之光半導體元件中,保護膜覆蓋於第1半導體層之表面與第2半導體層之表面。又,保護膜具有使第1半導體層之表面之一部份露出之開口部。 According to the above configuration, in the optical semiconductor device according to the aspect of the invention, the protective film covers the surface of the first semiconductor layer and the surface of the second semiconductor layer. Further, the protective film has an opening that exposes a part of the surface of the first semiconductor layer.

製造該構成之光半導體元件之時,藉由使用電鍍,而形成第1連接電極及第2連接電極。具體而言,於光半導體基 板之上表面之整面上形成電流薄膜,隨後形成將第1及第2電極上開口之光阻圖案,然後於光半導體元件上施加電鍍電流。 When the optical semiconductor element of this configuration is manufactured, the first connection electrode and the second connection electrode are formed by using electroplating. Specifically, in the optical semiconductor base A current film is formed on the entire surface of the upper surface of the board, and then a photoresist pattern opening the first and second electrodes is formed, and then a plating current is applied to the optical semiconductor element.

此處,第1電極與電流薄膜係直接導通。又,與第1電極導通之第1半導體層係通過保護膜之開口部而與電流薄膜導通。據此可知,自第1電極向電流薄膜及第1半導體層雙方流通有電鍍電流。 Here, the first electrode and the current film are directly electrically connected. Further, the first semiconductor layer that is electrically connected to the first electrode is electrically connected to the current film through the opening of the protective film. From this, it is understood that a plating current flows from both the first electrode to the current film and the first semiconductor layer.

另一方面,第2電極係與電流薄膜直接導通,但與第2電極導通之第2半導體層未與電流薄膜導通。因此,僅是自第2電極向電流薄膜流通有電鍍電流。 On the other hand, the second electrode is directly electrically connected to the current film, but the second semiconductor layer that is electrically connected to the second electrode is not electrically connected to the current film. Therefore, only the plating current flows from the second electrode to the current film.

如以上所述,電鍍光半導體基板時,流通之電鍍電流係第1電極側>第2電極側。其結果,藉由控制光半導體元件中流通之電鍍電流之參數,可形成吸收第1電極與第2電極之階差之相互間無階差之第1連接電極及第2連接電極。此時,只要控制電鍍電流之參數即可,故第1連接電極及第2連接電極之尺寸不受任何約束。 As described above, when the optical semiconductor substrate is plated, the plating current flowing through the first electrode side is the second electrode side. As a result, by controlling the parameters of the plating current flowing through the optical semiconductor element, the first connection electrode and the second connection electrode which absorb the step difference between the first electrode and the second electrode without forming a step can be formed. In this case, as long as the parameters of the plating current are controlled, the dimensions of the first connection electrode and the second connection electrode are not subject to any restriction.

因此,根據本發明之一態樣之光半導體元件之製造方法,可不使各連接電極之尺寸受到約束地形成適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極。又,根據本發明之一態樣之光半導體元件,可實現具有適於倒裝片安裝之相互間無階差之第1連接電極及第2連接電極之光半導體元件。 Therefore, according to the method of manufacturing an optical semiconductor device according to an aspect of the present invention, the first connection electrode and the second connection electrode which are suitable for flip chip mounting without stepping therebetween can be formed without constraining the size of each connection electrode. . Further, according to the optical semiconductor device of one aspect of the present invention, it is possible to realize an optical semiconductor element having a first connection electrode and a second connection electrode which are suitable for flip chip mounting without stepping therebetween.

又,本發明之一態樣之光半導體元件,進而,較好的是,上述開口部之表面積為可利用電鍍形成相互 間無階差之第1連接電極及第2連接電極之表面積。 Further, in an optical semiconductor device according to an aspect of the present invention, it is preferable that a surface area of the opening portion is formed by plating. The surface area of the first connection electrode and the second connection electrode without step difference therebetween.

根據上述之構成,在製造本發明之一態樣之光半導體元件時,可確實地形成相互間無階差之第1連接電極及第2連接電極。 According to the above configuration, when the optical semiconductor element of one aspect of the present invention is manufactured, the first connection electrode and the second connection electrode which are free from each other can be reliably formed.

又,本發明之一態樣之光半導體元件,進而,較好的是,與上述第1半導體層之上述開口部對應之位置上形成有凹槽。 Further, in an optical semiconductor device according to an aspect of the invention, it is preferable that a groove is formed at a position corresponding to the opening of the first semiconductor layer.

根據上述之構成,藉由於凹槽處切分光半導體元件,可不於第1半導體層上產生缺陷地將光半導體元件分割成特定之大小。 According to the above configuration, since the optical semiconductor element is cut by the recess, the optical semiconductor element can be divided into a specific size without causing defects on the first semiconductor layer.

又,本發明之一態樣之光半導體元件,進而,較好的是,上述凹槽之表面積為可利用電鍍形成相互間無階差之上述第1連接電極及第2連接電極之表面積。 Further, in the optical semiconductor device according to an aspect of the invention, it is preferable that the surface area of the groove is such that the surface areas of the first connection electrode and the second connection electrode which are formed without any step difference by plating are formed.

根據上述構成,在製造本發明之一態樣之光半導體元件時,可確實地形成相互間無階差之第1連接電極及第2連接電極。 According to the above configuration, when the optical semiconductor element of one aspect of the present invention is manufactured, the first connection electrode and the second connection electrode having no step difference therebetween can be reliably formed.

又,本發明之一態樣之光半導體元件之製造方法,進而,較好的是,藉由流通脈衝波形之電鍍電流,而電鍍光半導體元件。 Further, in the method of manufacturing an optical semiconductor device according to an aspect of the present invention, it is preferable that the optical semiconductor element is plated by a plating current of a pulse waveform.

根據上述構成,藉由控制電鍍電流之各種參數,可高效地控制第1電極之電鍍率與第2電極之電鍍率之比率。 According to the above configuration, by controlling various parameters of the plating current, the ratio of the plating rate of the first electrode to the plating rate of the second electrode can be efficiently controlled.

又,本發明之一態樣之光半導體元件之製造方法,進而, 較好的是,上述脈衝波形之週期係在0.1~100秒之範圍內。 Moreover, a method of manufacturing an optical semiconductor device according to an aspect of the present invention is further Preferably, the period of the pulse waveform is in the range of 0.1 to 100 seconds.

根據上述之構成,可高效地控制第1電極之電鍍率與第2電極之電鍍率之比率。其理由如下。當於光半導體基板上施加電鍍電流時,電鍍液電阻之過渡性變化於30秒內收斂。因此,若脈衝波形在0.1~100秒之範圍內,則可得到脈衝波形可變之效果。 According to the above configuration, the ratio of the plating rate of the first electrode to the plating rate of the second electrode can be efficiently controlled. The reason is as follows. When a plating current is applied to the optical semiconductor substrate, the transitional change in the plating solution resistance converges within 30 seconds. Therefore, if the pulse waveform is in the range of 0.1 to 100 seconds, the effect of the pulse waveform being variable can be obtained.

又,本發明之一態樣之光半導體元件之製造方法,進而,較好的是,上述脈衝波形之工作週期比為80%以上。 Further, in the method of manufacturing an optical semiconductor device according to one aspect of the invention, it is preferable that the duty cycle ratio of the pulse waveform is 80% or more.

根據上述之構成,可高效地控制第1電極之電鍍率與第2電極之電鍍率之比率。 According to the above configuration, the ratio of the plating rate of the first electrode to the plating rate of the second electrode can be efficiently controlled.

又,本發明之一態樣之光半導體元件之製造方法,進而,較好的是,上述脈衝波形之每一週期之電流之停止時間為2秒以下。 Further, in the method of manufacturing an optical semiconductor device according to an aspect of the invention, it is preferable that a current stop time of each of the pulse waveforms is 2 seconds or shorter.

根據上述之構成,可高效地控制第1電極之電鍍率與第2電極之電鍍率之比率。 According to the above configuration, the ratio of the plating rate of the first electrode to the plating rate of the second electrode can be efficiently controlled.

又,本發明之一態樣之光半導體元件之製造方法,進而,較好的是,上述電流薄膜之薄片電阻在10~1000 mΩ/□之範圍內。 Further, in the method of manufacturing an optical semiconductor device according to an aspect of the invention, it is preferable that the sheet resistance of the current film is in the range of 10 to 1000 mΩ/□.

根據上述之構成,電流薄膜之薄片電阻在10~1000 mΩ/□之範圍內。此處,光半導體基板之第1半導體層之薄片 電阻係在1~20 mΩ/□之範圍內。因此,可使第1電極側中流通電鍍電流之路徑之合成電阻、與第2電極側中流通電鍍電流之路徑之合成電阻之差為第1電極側之該合成電阻之10%。其結果,可高效地控制第1電極之電鍍率與第2電極之電鍍率之比率。 According to the above configuration, the sheet resistance of the current film is in the range of 10 to 1000 mΩ/□. Here, the sheet of the first semiconductor layer of the optical semiconductor substrate The resistance is in the range of 1 to 20 mΩ/□. Therefore, the difference between the combined resistance of the path through which the plating current flows in the first electrode side and the path of the plating current flowing through the second electrode side can be made 10% of the combined resistance on the first electrode side. As a result, the ratio of the plating rate of the first electrode to the plating rate of the second electrode can be efficiently controlled.

又,本發明之一態樣之光半導體元件之製造方法,進而,較好的是,利用上述脈衝波形之電鍍電流而實施電鍍之表面上該電鍍電流之電流密度,為滿足自臨界電流密度之下限值至上限值之範圍之範圍。 Further, in the method of manufacturing an optical semiconductor device according to an aspect of the present invention, it is preferable that the current density of the plating current on the surface of the plating is performed by the plating current of the pulse waveform to satisfy the self-critical current density. The range from the lower limit to the upper limit.

根據上述之構成,可形成正常形狀之第1連接電極及第2連接電極。又,藉由在該範圍中使電流密度變化,可變化電鍍率比。因此,藉由設電流密度為適當之值,可形成相互間無階差之第1連接電極與第2連接電極。 According to the above configuration, the first connection electrode and the second connection electrode of the normal shape can be formed. Further, by changing the current density in this range, the plating ratio can be changed. Therefore, by setting the current density to an appropriate value, the first connection electrode and the second connection electrode having no step difference therebetween can be formed.

又,本發明之一態樣之光半導體元件之製造方法,進而,較好的是,根據形成上述電流薄膜之步驟中所形成之上述電流薄膜之膜厚,而決定形成上述連續電極之步驟中之上述第1電極與上述第2電極之電鍍率比。 Further, in the method of manufacturing an optical semiconductor device according to an aspect of the present invention, it is preferable that the step of forming the continuous electrode is performed in accordance with a film thickness of the current film formed in the step of forming the current film. The ratio of the plating rate of the first electrode to the second electrode is higher.

根據上述之構成,藉由變化電流薄膜之膜厚,可變化電鍍率比。因此,藉由設電流薄膜之膜厚為適當之值,可形成相互間無階差之第1連接電極與第2連接電極。 According to the above configuration, the plating ratio can be changed by changing the film thickness of the current film. Therefore, by setting the film thickness of the current film to an appropriate value, the first connection electrode and the second connection electrode having no step difference therebetween can be formed.

又,本發明之一態樣之光半導體元件之製造方法,進而, 較好的是,電鍍上述光半導體元件時,使用自金、銀、白金、銅、鈀、鎳、焊錫、及該等之合金中任意選擇之金屬。 Moreover, a method of manufacturing an optical semiconductor device according to an aspect of the present invention is further Preferably, when the optical semiconductor element is plated, a metal selected from gold, silver, platinum, copper, palladium, nickel, solder, and the like is used.

根據上述之構成,可製造歐姆特性更好且適於倒裝片安裝之具有第1連接電極及第2連接電極之光半導體元件。 According to the above configuration, it is possible to manufacture an optical semiconductor element having the first connection electrode and the second connection electrode which are more excellent in ohmic characteristics and suitable for flip chip mounting.

本發明不限定於上述之各實施形態者,在技術方案所示之範圍中可有各種變更,將不同之實施形態中分別揭示之技術手段適宜組合而得到之實施形態亦包含於本發明之技術範圍。 The present invention is not limited to the embodiments described above, and various modifications can be made without departing from the scope of the invention. The embodiments obtained by appropriately combining the technical means disclosed in the different embodiments are also included in the technology of the present invention. range.

[產業上之可利用性] [Industrial availability]

本發明作為發光二極體(LED)等之光半導體元件,可廣泛利用。又,亦可作為製造該種光半導體元件之方法利用。 The present invention can be widely used as an optical semiconductor element such as a light emitting diode (LED). Moreover, it can also be utilized as a method of manufacturing such an optical semiconductor element.

10‧‧‧光半導體元件 10‧‧‧Optical semiconductor components

11‧‧‧藍寶石基板(絕緣性透明基板) 11‧‧‧Sapphire substrate (insulating transparent substrate)

12‧‧‧n型層(第1導電型半導體層) 12‧‧‧n type layer (first conductivity type semiconductor layer)

13‧‧‧p型層(第2導電型半導體層) 13‧‧‧p-type layer (second conductivity type semiconductor layer)

14a‧‧‧n極電極(第1電極) 14a‧‧‧n pole electrode (first electrode)

14b‧‧‧p極電極(第2電極) 14b‧‧‧p pole electrode (2nd electrode)

15‧‧‧保護膜 15‧‧‧Protective film

21‧‧‧開口部 21‧‧‧ openings

22‧‧‧凹槽 22‧‧‧ Groove

30‧‧‧陰極 30‧‧‧ cathode

31‧‧‧下層電流薄膜 31‧‧‧Under current film

32‧‧‧上層電流薄膜 32‧‧‧Upper current film

33‧‧‧電流薄膜 33‧‧‧current film

41‧‧‧光阻 41‧‧‧Light resistance

42‧‧‧凸塊形成圖案 42‧‧‧Bump formation pattern

51‧‧‧p極凸塊(第2連接電極) 51‧‧‧p pole bump (2nd connecting electrode)

52‧‧‧n極凸塊(第1連接電極) 52‧‧‧n pole bump (first connecting electrode)

60‧‧‧光半導體元件 60‧‧‧Optical semiconductor components

62‧‧‧n型層(第1導電型半導體層) 62‧‧‧n type layer (first conductivity type semiconductor layer)

80‧‧‧陽極 80‧‧‧Anode

81‧‧‧陽極板 81‧‧‧Anode plate

152‧‧‧n極凸塊 152‧‧‧n pole bump

圖1係顯示本發明之一實施形態之光半導體元件之簡略剖面圖。 BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic cross-sectional view showing an optical semiconductor device according to an embodiment of the present invention.

圖2(a)~(g)係顯示本發明之一實施形態之光半導體元件之製造方法之簡略剖面圖。 2(a) to 2(g) are schematic cross-sectional views showing a method of manufacturing an optical semiconductor device according to an embodiment of the present invention.

圖3係顯示本發明之一實施形態之光半導體元件之製造方法中,利用電鍍形成凸塊時之電鍍電流電路之等價電路之圖。且Rcf表示電流薄膜之電阻值,R1表示第1導電型半導體層之電阻值,Rop表示開口部之電流薄膜與第1導電型半導體層之連接電阻,且Rbath表示電鍍液之電阻值。 Fig. 3 is a view showing an equivalent circuit of a plating current circuit when a bump is formed by plating in a method of manufacturing an optical semiconductor device according to an embodiment of the present invention. R cf represents the resistance value of the current film, R 1 represents the resistance value of the first conductivity type semiconductor layer, R op represents the connection resistance of the current film of the opening portion and the first conductivity type semiconductor layer, and R bath represents the resistance of the plating solution. value.

圖4係顯示n極之電鍍率與p極之電鍍率之比之脈衝週期 依存性之圖。空心圓係顯示實測值。波狀線係作為擬合實測值之結果得到的曲線。實線係顯示使用直流之電鍍電流之情形所得到的電鍍率比。 Figure 4 shows the pulse period of the ratio of the plating rate of the n-pole to the plating rate of the p-pole. A map of dependence. The open circle shows the measured value. The wavy line is a curve obtained as a result of fitting the measured values. The solid line shows the plating ratio obtained by using the plating current of DC.

圖5係顯示利用直流電鍍所形成之凸塊之形狀的剖面圖。 Fig. 5 is a cross-sectional view showing the shape of a bump formed by direct current plating.

圖6係顯示本發明之一實施形態之電鍍率比之開口部之面積比依存性之圖。 Fig. 6 is a graph showing the ratio of the plating ratio to the area ratio of the opening in an embodiment of the present invention.

圖7係顯示本發明之一實施形態之電鍍率比之電流密度依存性之圖。 Fig. 7 is a graph showing the dependence of the plating rate ratio on the current density in an embodiment of the present invention.

圖8係顯示本發明之一實施形態之測定電流薄膜33之薄片電阻與電鍍率比之關係之實驗結果之圖。 Fig. 8 is a graph showing the results of an experiment for measuring the relationship between the sheet resistance of the current film 33 and the plating ratio in an embodiment of the present invention.

圖9係顯示本發明之一實施形態之光半導體元件之簡略剖面圖。 Fig. 9 is a schematic cross-sectional view showing an optical semiconductor device according to an embodiment of the present invention.

圖10(a)~(g)係顯示本發明之另一實施形態之光半導體元件之製作方法之簡略剖面圖。 Figs. 10(a) through 10(g) are schematic cross sectional views showing a method of fabricating an optical semiconductor device according to another embodiment of the present invention.

10‧‧‧光半導體元件 10‧‧‧Optical semiconductor components

11‧‧‧藍寶石基板 11‧‧‧Sapphire substrate

12‧‧‧n型層 12‧‧‧n-type layer

13‧‧‧p型層 13‧‧‧p-type layer

14a‧‧‧n極電極 14a‧‧‧ pole electrode

14b‧‧‧p極電極 14b‧‧‧p pole electrode

15‧‧‧保護膜 15‧‧‧Protective film

21‧‧‧開口部 21‧‧‧ openings

22‧‧‧凹槽 22‧‧‧ Groove

31‧‧‧下層電流薄膜 31‧‧‧Under current film

32‧‧‧上層電流薄膜 32‧‧‧Upper current film

33‧‧‧電流薄膜 33‧‧‧current film

51‧‧‧p極凸塊 51‧‧‧p pole bump

52‧‧‧n極凸塊 52‧‧‧n pole bump

Claims (13)

一種光半導體元件,其特徵為包含:第1半導體層,其包含第1導電型之半導體;第2半導體層,其包含第2導電型之半導體,且形成於上述第1半導體層之上表面的一部份;第1電極,其形成於上述第1半導體層之上表面的另一部份;第2電極,其形成於上述第2半導體層之上表面,且具有位於較上述第1電極之上表面更高之位置的上表面;第1連接電極,其形成於上述第1電極之上表面;第2連接電極,其形成於上述第2電極之上表面;及保護膜,其係覆蓋於上述第1半導體層之表面及上述第2半導體層之表面的絕緣性保護膜,且具有使上述第1半導體層之表面之一部份露出的開口部。 An optical semiconductor device comprising: a first semiconductor layer including a semiconductor of a first conductivity type; and a second semiconductor layer comprising a semiconductor of a second conductivity type formed on an upper surface of the first semiconductor layer a first electrode formed on the upper surface of the upper surface of the first semiconductor layer; and a second electrode formed on the upper surface of the second semiconductor layer and having a position higher than the first electrode An upper surface having a higher upper surface; a first connection electrode formed on the upper surface of the first electrode; a second connection electrode formed on an upper surface of the second electrode; and a protective film covering the surface The insulating protective film on the surface of the first semiconductor layer and the surface of the second semiconductor layer has an opening that exposes a part of the surface of the first semiconductor layer. 如請求項1之光半導體元件,其中上述開口部之表面積為可利用電鍍而形成相互間無階差之上述第1連接電極及第2連接電極之表面積。 The optical semiconductor device according to claim 1, wherein the surface area of the opening portion is a surface area of the first connection electrode and the second connection electrode which are formed by plating to form a step difference between the first connection electrode and the second connection electrode. 如請求項1之光半導體元件,其中於與上述第1半導體層之上述開口部對應的位置上形成有凹槽。 An optical semiconductor device according to claim 1, wherein a groove is formed at a position corresponding to the opening of the first semiconductor layer. 如請求項3之光半導體元件,其中上述凹槽之表面積為可利用電鍍而形成相互間無階差之上述第1連接電極及第2連接電極之表面積。 The optical semiconductor device according to claim 3, wherein the surface area of the recess is a surface area of the first connection electrode and the second connection electrode which are formed by electroplating to have no step difference therebetween. 一種光半導體元件之製造方法,其特徵為包含:於光半導體基板之上表面的整面上,形成導電性之電 流薄膜之步驟,該光半導體基板包含:基板;形成於該基板之上表面且包含第1導電型之半導體之第1半導體層;包含第2導電型之半導體,且形成於上述第1半導體層之上表面的一部份之第2半導體層;形成於上述第1半導體層之上表面的另一部份之第1電極;形成於上述第2半導體層之上表面,且具有位於較上述第1電極之上表面更高之位置的上表面之第2電極;及覆蓋於上述第1半導體層之表面及上述第2半導體層之表面的絕緣性保護膜,且具有使上述第1半導體層之表面之一部份露出的開口部之保護膜;及形成上述電流薄膜後,藉由電鍍上述光半導體基板而於上述第1電極之上表面形成第1連接電極,且於上述第2電極之上表面形成第2連接電極之步驟。 A method of fabricating an optical semiconductor device, comprising: forming a conductive electric current on an entire surface of an upper surface of an optical semiconductor substrate a step of flowing a thin film comprising: a substrate; a first semiconductor layer including a semiconductor of a first conductivity type formed on an upper surface of the substrate; and a semiconductor including a second conductivity type formed on the first semiconductor layer a second semiconductor layer on a portion of the upper surface; a first electrode formed on the other surface of the upper surface of the first semiconductor layer; formed on the upper surface of the second semiconductor layer; a second electrode on the upper surface of the upper surface of the electrode, and an insulating protective film covering the surface of the first semiconductor layer and the surface of the second semiconductor layer, and having the first semiconductor layer a protective film for the exposed portion of the surface; and after forming the current film, the first connection electrode is formed on the upper surface of the first electrode by plating the photo-semiconductor substrate, and above the second electrode The step of forming the second connection electrode on the surface. 如請求項5之光半導體元件之製造方法,其中藉由流通脈衝波形之電鍍電流,而電鍍光半導體元件。 A method of manufacturing an optical semiconductor device according to claim 5, wherein the optical semiconductor element is plated by circulating a plating current of a pulse waveform. 如請求項6之光半導體元件之製造方法,其中上述脈衝波形之週期為0.1~100秒之範圍內。 The method of manufacturing an optical semiconductor device according to claim 6, wherein the period of the pulse waveform is in a range of 0.1 to 100 seconds. 如請求項6之光半導體元件之製造方法,其中上述脈衝波形之工作週期比為80%以上。 A method of manufacturing an optical semiconductor device according to claim 6, wherein a duty cycle ratio of said pulse waveform is 80% or more. 如請求項6之光半導體元件之製造方法,其中上述脈衝波形之每一週期之電流之停止時間為2秒以下。 The method of manufacturing an optical semiconductor device according to claim 6, wherein the current of each of the pulse waveforms has a stop time of 2 seconds or less. 如請求項6之光半導體元件之製造方法,其中上述電流薄膜之薄片電阻為10~1000 mΩ/□之範圍內。 The method of producing an optical semiconductor device according to claim 6, wherein the sheet resistance of the current film is in the range of 10 to 1000 mΩ/□. 如請求項6之光半導體元件之製造方法,其中利用上述 脈衝波形之電鍍電流而電鍍之表面之該電鍍電流之電流密度,為滿足自臨界電流密度之下限值至上限值之範圍之範圍。 A method of manufacturing an optical semiconductor component according to claim 6, wherein the above The current density of the plating current on the surface of the electroplated current of the pulse waveform is a range satisfying the range from the lower limit value to the upper limit value of the self-critical current density. 如請求項5之光半導體元件之製造方法,其中根據形成上述電流薄膜之步驟中形成之上述電流薄膜之膜厚,決定形成上述連接電極之步驟中之上述第1電極與上述第2電極之電鍍率比。 The method of manufacturing an optical semiconductor device according to claim 5, wherein the plating of the first electrode and the second electrode in the step of forming the connection electrode is determined according to a film thickness of the current film formed in the step of forming the current film Rate ratio. 如請求項5之光半導體元件之製造方法,其中在電鍍上述光半導體元件時,使用自金、銀、白金、銅、鈀、鎳、焊錫、及該等之合金中任意選擇之金屬。 A method of producing an optical semiconductor device according to claim 5, wherein a metal selected from the group consisting of gold, silver, platinum, copper, palladium, nickel, solder, and the like is used for plating the above-mentioned optical semiconductor element.
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