TW202046514A - Light emitting element and method of manufacturing light emitting element - Google Patents

Light emitting element and method of manufacturing light emitting element Download PDF

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TW202046514A
TW202046514A TW109111436A TW109111436A TW202046514A TW 202046514 A TW202046514 A TW 202046514A TW 109111436 A TW109111436 A TW 109111436A TW 109111436 A TW109111436 A TW 109111436A TW 202046514 A TW202046514 A TW 202046514A
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石崎順也
山田雅人
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日商信越半導體股份有限公司
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Abstract

The present invention is a light emitting element having a light emitting part in which an N-type cladding layer, an active layer, and a P-type cladding layer are formed in this order, wherein the active layer includes a P-type dopant of which the concentration gradually decreases from the P-type cladding layer side to the N-type cladding layer side, and in the active layer, the average concentration of the P-type dopant in a region from the P-type cladding layer to a position corresponding to 1/3 of the thickness of the active layer is 1.0 * 1016 atoms/cm3 or more and 3.0 * 1017 atoms/cm3 or less. Accordingly, provided are: the light emitting element which has excellent luminance characteristics with respect to the environmental temperature and which suppresses the deterioration of life characteristics; and a method of manufacturing the same.

Description

發光元件及發光元件之製造方法Light-emitting element and manufacturing method of light-emitting element

本發明係關於一種發光元件及發光元件之製造方法,尤其關於一種相應於環境溫度的輝度特性良好且抑制壽命特性惡化之發光元件及發光元件之製造方法。The present invention relates to a light-emitting element and a method for manufacturing a light-emitting element, and more particularly to a light-emitting element and a method for manufacturing a light-emitting element that have good luminance characteristics corresponding to ambient temperature and suppress deterioration in lifetime characteristics.

AlGaInP系材料具有氮化物以外的III-V族化合物半導體混晶中最大的直接躍遷型能隙,作為550~650nm帶(綠色~紅色波段)的可見光發光裝置之材料而受到矚目。此種具有由擁有較大直接躍遷型能隙之AlGaInP所構成的活性層之AlGaInP系發光元件,能達到比使用GaP、GaAsP等間接躍遷型的材料構成者更高輝度的發光(例如專利文獻1)。AlGaInP-based materials have the largest direct transition type energy gap in III-V compound semiconductor mixed crystals other than nitrides, and are attracting attention as materials for visible light emitting devices in the 550-650 nm band (green-red band). Such an AlGaInP-based light-emitting element having an active layer composed of AlGaInP with a large direct transition type energy gap can achieve higher brightness than those composed of indirect transition type materials such as GaP and GaAsP (for example, Patent Document 1 ).

圖4係顯示習知AlGaInP系發光元件的一例之概略剖面圖。 此發光元件310於GaAs出發基板300上具有:厚度0.1~1.0μm的GaAs緩衝層;例如厚度1.0μm的AlInP蝕刻終止層302;例如厚度1.0μm的N型AlGaInP護套層303;例如厚度0.9μm的AlGaInP活性層304;例如厚度1.0μm的P型AlGaInP護套層305;緩和與電流傳播層之晶格錯合的P型InGaP緩衝層306;將施加至元件的電流加以傳播且擴散、具有光萃取功能之例如厚度5.0μm的P型GaP電流傳播層307。亦可無須GaAs緩衝層。另,在圖4中省略發光元件的電極等。4 is a schematic cross-sectional view showing an example of a conventional AlGaInP-based light-emitting device. The light-emitting element 310 has on the GaAs starting substrate 300: a GaAs buffer layer with a thickness of 0.1 to 1.0 μm; for example, an AlInP etching stop layer 302 with a thickness of 1.0 μm; for example, an N-type AlGaInP sheath layer 303 with a thickness of 1.0 μm; for example, a thickness of 0.9 μm The AlGaInP active layer 304; for example, the P-type AlGaInP sheath layer 305 with a thickness of 1.0 μm; the P-type InGaP buffer layer 306 that eases the lattice misalignment with the current propagation layer; the current applied to the element is propagated and diffused to have light The extraction function is, for example, a P-type GaP current propagation layer 307 with a thickness of 5.0 μm. The GaAs buffer layer may not be required. Note that the electrodes of the light-emitting element and the like are omitted in FIG. 4.

在此,就N型摻雜物而言,例如將Si、S、Se等摻雜至N型護套層303。又,就P型摻雜物而言,將Zn、Mg、Te等摻雜至P型護套層305及P型緩衝層306及P型電流傳播層307。Here, as for the N-type dopant, for example, Si, S, Se, etc. are doped into the N-type sheath layer 303. In addition, for P-type dopants, Zn, Mg, Te, etc. are doped into the P-type sheath layer 305, the P-type buffer layer 306, and the P-type current propagation layer 307.

N型護套層303係以1層以上之組成及摻雜水準的磊晶層所構成,P型護套層305係以1層以上之組成及摻雜水準的磊晶層所構成。活性層304係均一組成的表體型活性層,或由發光復合層與具有大於該發光復合層之組成的能帶隙組成之障壁層所多重接合的多重接合型活性層所構成。The N-type sheath layer 303 is composed of an epitaxial layer with more than one composition and doping level, and the P-type sheath layer 305 is composed of an epitaxial layer with more than one composition and doping level. The active layer 304 is a uniformly composed surface-type active layer, or a multiple junction type active layer in which a light-emitting composite layer and a barrier layer having an energy band gap larger than the composition of the light-emitting composite layer are multiple-joined.

此外,以磊晶成長來形成發光元件(例如AlGaInP系發光元件)的發光部之際,為了迴避壽命特性之惡化,必須將殘留在活性層中,又或於壽命試驗中擴散、泳動的摻雜物之濃度設計成極小。然而,使活性層中的摻雜物濃度極小雖能改善壽命特性,但另一方面,相應於環境溫度的輝度變化有變大的傾向。 又,為了改善相應於環境溫度的輝度特性,已知將摻雜物過度置入活性層中為有效。然而,過度投入活性層中的摻雜物雖能改善輝度特性,但成為差排、缺陷發生源,使壽命特性顯著惡化。In addition, when forming the light-emitting portion of a light-emitting element (such as an AlGaInP-based light-emitting element) by epitaxial growth, in order to avoid deterioration of life characteristics, it is necessary to remain in the active layer, or to diffuse or migrate during the life test. The concentration of the material is designed to be extremely small. However, making the concentration of the dopant in the active layer extremely small can improve the life characteristics, but on the other hand, the change in brightness corresponding to the ambient temperature tends to become larger. In addition, in order to improve the brightness characteristics corresponding to the ambient temperature, it is known that excessive placement of dopants in the active layer is effective. However, the dopants that are excessively added to the active layer can improve the brightness characteristics, but become a source of dislocations and defects, and significantly deteriorate the lifetime characteristics.

所以,相應於環境溫度的輝度特性良好之發光元件為壽命特性差,另一方面,壽命特性良好的發光元件則相應於環境溫度的輝度特性差,期望實現兩個特性良好的發光元件。 [先前技術文獻] [專利文獻]Therefore, a light-emitting element with good luminance characteristics corresponding to ambient temperature has poor lifetime characteristics. On the other hand, a light-emitting element with good lifetime characteristics has poor luminance characteristics corresponding to ambient temperature. It is desired to realize two light-emitting elements with good characteristics. [Prior Technical Literature] [Patent Literature]

[專利文獻1]日本特開2005-150645號公報[Patent Document 1] Japanese Patent Application Publication No. 2005-150645

[發明所欲解決之問題][The problem to be solved by the invention]

本發明有鑒於上述課題而成,目的在於提供一種發光元件及其製造方法,其相應於環境溫度的輝度特性良好,且抑制壽命特性之惡化。 [解決問題之方式]The present invention has been made in view of the above-mentioned problems, and an object thereof is to provide a light-emitting element and a method of manufacturing the same, which have good luminance characteristics corresponding to ambient temperature and suppress deterioration of lifetime characteristics. [The way to solve the problem]

為達成上述目的,本發明提供一種發光元件,包含依序形成有N型護套層、活性層及P型護套層的發光部,其特徵在於, 前述活性層包含:P型摻雜物,其濃度自前述P型護套層側往前述N型護套層側漸減; 且在前述活性層中,自前述P型護套層起算到前述活性層的1/3厚度大小之位置為止的區域之平均前述P型摻雜物濃度為1.0×1016 atoms/cm3 以上,且為3.0×1017 atoms/cm3 以下。In order to achieve the above object, the present invention provides a light-emitting element including a light-emitting portion in which an N-type sheath layer, an active layer, and a P-type sheath layer are sequentially formed, wherein the active layer includes: P-type dopants, Its concentration gradually decreases from the P-type sheath layer side to the N-type sheath layer side; and in the active layer, the area from the P-type sheath layer to the position of 1/3 of the thickness of the active layer The average P-type dopant concentration is 1.0×10 16 atoms/cm 3 or more and 3.0×10 17 atoms/cm 3 or less.

在此種活性層中,只要自P型護套層起算到活性層的1/3厚度大小之位置為止的區域之平均P型摻雜物濃度為1.0×1016 atoms/cm3 以上,則能提昇光輸出並且提昇相應於環境溫度的輝度特性。 又,自P型護套層起算到活性層的1/3厚度大小之位置為止的區域之平均P型摻雜物濃度為3.0×1017 atoms/cm3 以下,且在活性層中係自P型護套層側往N型護套層側漸減的P型摻雜物濃度曲線,能藉以抑制壽命特性之惡化。In such an active layer, as long as the average P-type dopant concentration in the region from the P-type sheath layer to the position of 1/3 of the thickness of the active layer is 1.0×10 16 atoms/cm 3 or more, it can Increase the light output and increase the brightness characteristics corresponding to the ambient temperature. In addition, the average P-type dopant concentration in the region from the P-type sheath layer to the position of 1/3 of the thickness of the active layer is 3.0×10 17 atoms/cm 3 or less, and the active layer is derived from P The P-type dopant concentration curve that gradually decreases from the side of the N-type sheath layer to the side of the N-type sheath layer can suppress the deterioration of the life characteristics.

又,前述發光部可定為由AlGaInP系的化合物半導體所構成。In addition, the aforementioned light-emitting portion can be determined to be composed of an AlGaInP-based compound semiconductor.

本發明尤其能適合用於發光部係由AlGaInP系的化合物半導體所構成的發光元件。In particular, the present invention can be suitably used for a light-emitting element in which the light-emitting portion is composed of an AlGaInP-based compound semiconductor.

又,可定為在前述活性層中,自前述P型護套層起算前述活性層的1/3厚度大小之位置到2/3厚度大小之位置為止的區域之平均前述P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。In addition, it can be determined as the average P-type dopant concentration in the active layer from the position of the P-type sheath layer from the position of 1/3 of the thickness of the active layer to the position of 2/3 of the thickness of the active layer It is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less.

只要如此P型摻雜物濃度在上述區域係上述數值範圍,能更加確實抑制壽命特性惡化。As long as the P-type dopant concentration is within the above-mentioned numerical range in the above-mentioned region, the deterioration of the lifetime characteristics can be suppressed more reliably.

此時,可定為在前述活性層中,自前述P型護套層起算前述活性層的2/3厚度大小之位置到N型護套層為止的區域之平均前述P型摻雜物濃度為0.3×1016 atoms/cm3 以下。At this time, it can be determined that in the active layer, the average P-type dopant concentration in the region from the position of 2/3 of the thickness of the active layer from the P-type sheath layer to the N-type sheath layer is 0.3×10 16 atoms/cm 3 or less.

只要如此P型摻雜物濃度在上述區域係上述數值範圍,能更加進一步確實抑制壽命特性惡化。As long as the P-type dopant concentration is within the above-mentioned numerical range in the above-mentioned region, the deterioration of the lifetime characteristics can be further reliably suppressed.

又,本發明提供一種發光元件之製造方法,該發光元件具有N型護套層、活性層與P型護套層依此順序形成的發光部,其特徵在於: 在前述活性層中,P型摻雜物濃度自前述P型護套層側往前述N型護套層側漸減,且將前述P型摻雜物摻雜成如下來製造: 在前述活性層中,自前述P型護套層起算到前述活性層的1/3厚度大小之位置為止的區域之平均前述P型摻雜物濃度為1.0×1016 atoms/cm3 以上,且為3.0×1017 atoms/cm3 以下。In addition, the present invention provides a method of manufacturing a light-emitting element, the light-emitting element having a light-emitting portion formed in this order of an N-type sheath layer, an active layer, and a P-type sheath layer, characterized in that: in the active layer, the P-type The dopant concentration gradually decreases from the P-type sheath layer side to the N-type sheath layer side, and the P-type dopant is doped as follows to manufacture: In the active layer, from the P-type sheath layer The average P-type dopant concentration in the region from the position of 1/3 of the thickness of the active layer is 1.0×10 16 atoms/cm 3 or more and 3.0×10 17 atoms/cm 3 or less.

只要如此製造成在活性層中,自P型護套層起算到活性層的1/3厚度大小之位置為止的區域之平均P型摻雜物濃度為1.0×1016 atoms/cm3 以上,則提昇光輸出並提昇相應於環境溫度的輝度特性。 又,使自P型護套層起算到活性層的1/3厚度大小之位置為止的區域之平均P型摻雜物濃度為3.0×1017 atoms/cm3 以下,且定為在活性層中自P型護套層側往N型護套層側漸減的P型摻雜物濃度曲線,可藉以抑制壽命特性惡化。As long as it is manufactured so that the average P-type dopant concentration in the active layer from the P-type sheath layer to the position of 1/3 the thickness of the active layer is 1.0×10 16 atoms/cm 3 or more, then Increase the light output and improve the brightness characteristics corresponding to the ambient temperature. In addition, the average P-type dopant concentration in the region from the P-type sheath layer to the position where the thickness of the active layer is 1/3 of the thickness of the active layer is 3.0×10 17 atoms/cm 3 or less, and is defined as being in the active layer The P-type dopant concentration curve gradually decreasing from the P-type sheath layer side to the N-type sheath layer side can suppress the deterioration of life characteristics.

此時,前述發光部可定為由AlGaInP系的化合物半導體所構成。In this case, the aforementioned light-emitting portion can be determined to be composed of an AlGaInP-based compound semiconductor.

本發明尤其能適合用於製造發光部係由AlGaInP系的化合物半導體所構成的發光元件。In particular, the present invention can be suitably used to manufacture a light-emitting element in which the light-emitting portion is composed of an AlGaInP-based compound semiconductor.

又,將前述P型摻雜物摻雜至前述活性層時,可摻雜成如下: 在前述活性層中,自前述P型護套層起算前述活性層的1/3厚度大小之位置到2/3厚度大小之位置為止的區域之平均前述P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。In addition, when the P-type dopant is doped into the active layer, it can be doped as follows: In the active layer, from the P-type sheath layer, the thickness of the active layer is 1/3 to 2 The average P-type dopant concentration in the region up to the position having the thickness of /3 is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less.

只要如此定為P型摻雜物濃度在上述區域係上述數值範圍,能更加確實地抑制壽命特性惡化。As long as the P-type dopant concentration is determined to be in the above-mentioned numerical range in the above-mentioned region, deterioration of the lifetime characteristics can be suppressed more reliably.

此時,將前述P型摻雜物摻雜至前述活性層時,可摻雜成如下: 在前述活性層中,自前述P型護套層起算前述活性層的2/3厚度大小之位置到N型護套層為止的區域之平均前述P型摻雜物濃度為0.3×1016 atoms/cm3 以下。At this time, when the aforementioned P-type dopant is doped into the aforementioned active layer, it can be doped as follows: In the aforementioned active layer, from the aforementioned P-type sheath layer to a position of 2/3 of the thickness of the aforementioned active layer The average P-type dopant concentration in the region up to the N-type sheath layer is 0.3×10 16 atoms/cm 3 or less.

只要如此將P型摻雜物濃度定為在上述區域係上述數值範圍,則能更加進一步確實地抑制壽命特性惡化。As long as the P-type dopant concentration is set within the above-mentioned numerical range in the above-mentioned region, the deterioration of the lifetime characteristics can be further reliably suppressed.

又,可將前述P型摻雜物針對前述活性層之摻雜,藉由如下方式進行: 一邊形成前述活性層一邊氣體摻雜。 或,可將前述P型摻雜物針對前述活性層的摻雜,藉由如下方式進行: 形成前述活性層之後,形成已摻雜前述P型摻雜物的前述P型護套層再施加熱處理,使已摻雜至前述P型護套層的前述P型摻雜物擴散至前述活性層。In addition, the aforementioned P-type dopant can be doped to the aforementioned active layer by the following method: Gas doping is performed while forming the aforementioned active layer. Or, the aforementioned P-type dopant can be doped to the aforementioned active layer by the following method: After the active layer is formed, the P-type sheath layer doped with the P-type dopant is formed and heat treatment is applied to diffuse the P-type dopant that has been doped into the P-type sheath layer to the active layer. .

如此藉由利用氣體摻雜或熱處理的摻雜,能簡便地以上述濃度曲線摻雜至上述各區域。 [發明之效果]In this way, by doping by gas doping or heat treatment, it is possible to easily dope to the above-mentioned regions with the above-mentioned concentration curve. [Effects of Invention]

如上所述,只要是本發明之發光元件及發光元件之製造方法,即能提昇光輸出並且相應於環境溫度的輝度特性良好,且抑制壽命特性之惡化。As described above, as long as the light-emitting element and the method of manufacturing the light-emitting element of the present invention can increase the light output, the brightness characteristics corresponding to the ambient temperature are good, and the deterioration of the lifetime characteristics is suppressed.

[實施發明之較佳形態][Preferable form for implementing invention]

如上所述,吾人期望開發出壽命特性及相應於環境溫度的輝度特性兩者良好的發光元件(尤其是AlGaInP系LED)。本案發明人針對此課題反覆特意探討而得知,在具有至少N型護套層、活性層與P型護套層依此順序形成的發光部之發光元件中,改變相應於環境溫度的輝度特性之巨大要因係活性層區域之中的P型載子富含區域的載子之舉動,因此,靠近P型護套層的活性層區域,具體而言為活性層全厚的1/3厚度,將靠近P型護套層的區域定為P型活性層區域,將該P型活性層區域之P型摻雜物濃度定為1.0×1016 atoms/cm3 以上3×1017 atoms/cm3 以下,並再為了防止過度擴散至活性層中,而於磊晶成長時,將P型摻雜物雜質以呈自P型護套層側起朝向N型護套層側而往活性層中漸減的濃度曲線的方式摻雜至活性層中,能製造出相應於環境溫度的輝度特性與壽命特性兩種特性良好的發光元件,再加上進一步探討而完成本發明。As described above, we hope to develop light-emitting elements (especially AlGaInP-based LEDs) that have good lifetime characteristics and brightness characteristics corresponding to ambient temperature. The inventor of the present case has deliberately discussed this subject repeatedly and learned that in a light-emitting element having a light-emitting portion formed in this order at least an N-type sheath layer, an active layer, and a P-type sheath layer, the brightness characteristics corresponding to the ambient temperature are changed The huge reason is due to the behavior of the carriers in the P-type carrier-rich region in the active layer region. Therefore, the active layer region near the P-type sheath layer is specifically 1/3 of the full thickness of the active layer. The region close to the P-type sheath layer is designated as the P-type active layer region, and the P-type dopant concentration in the P-type active layer region is determined to be 1.0×10 16 atoms/cm 3 or more and 3×10 17 atoms/cm 3 In the following, in order to prevent excessive diffusion into the active layer, during epitaxial growth, the P-type dopant impurities are gradually reduced from the side of the P-type sheath layer to the side of the N-type sheath layer. The method of doping into the active layer by the concentration curve of, can produce a light-emitting element with good characteristics of brightness and lifetime characteristics corresponding to the ambient temperature, and further studies have completed the present invention.

以下針對本發明,參照圖式進一步詳細說明實施形態,但本發明不限定於此。 (第一實施形態) 本發明之發光元件的第一實施形態顯示於圖1。如圖1所示,第一實施形態的發光元件110於GaAs出發基板100上具有:厚度0.1~1.0μm的GaAs緩衝層,例如厚度1.0μm的AlInP蝕刻終止層102;例如厚度1.0μm的N型AlGaInP護套層103;例如厚度0.9μm的AlGaInP活性層104;例如厚度1.0μm的P型AlGaInP護套層105;將與電流傳播層之晶格錯合加以緩和的P型InGaP緩衝層106;及施加至元件的電流加以傳播且擴散、具有光萃取功能之例如厚度5.0μm的P型GaP電流傳播層107。 亦可沒有GaAs緩衝層。另,在圖1中省略發光元件之電極等。Hereinafter, the embodiments of the present invention will be described in further detail with reference to the drawings, but the present invention is not limited to this. (First Embodiment) The first embodiment of the light-emitting device of the present invention is shown in FIG. 1. As shown in FIG. 1, the light-emitting element 110 of the first embodiment has a GaAs buffer layer with a thickness of 0.1 to 1.0 μm, such as an AlInP etching stop layer 102 with a thickness of 1.0 μm, on a GaAs starting substrate 100; AlGaInP sheath layer 103; for example, an AlGaInP active layer 104 with a thickness of 0.9 μm; for example, a P-type AlGaInP sheath layer 105 with a thickness of 1.0 μm; a P-type InGaP buffer layer 106 that relaxes lattice misalignment with the current propagation layer; and The current applied to the element propagates and diffuses, and has a light extraction function, for example, a P-type GaP current propagation layer 107 having a thickness of 5.0 μm. There may be no GaAs buffer layer. In addition, the electrodes of the light-emitting element and the like are omitted in FIG. 1.

在此,將Si、S、Se之中1種以上摻雜至N型護套層103作為N型摻雜物,將Zn、Mg、Te之中1種以上摻雜至P型護套層105、P型緩衝層106及P型電流傳播層107作為P型摻雜物。Here, one or more of Si, S, and Se is doped into the N-type sheath layer 103 as an N-type dopant, and one or more kinds of Zn, Mg, and Te are doped into the P-type sheath layer 105 , P-type buffer layer 106 and P-type current propagation layer 107 are used as P-type dopants.

N型護套層103以1層以上之組成及摻雜水準的磊晶層所構成,P型護套層105以1層以上之組成及摻雜水準的磊晶層所構成。The N-type sheath layer 103 is composed of an epitaxial layer with more than one composition and doping level, and the P-type sheath layer 105 is composed of an epitaxial layer with more than one composition and doping level.

活性層104由均一組成的表體型活性層而成。 活性層104自P型護套層105起朝向N型護套層103以例如平緩傾斜或階梯狀的方式摻雜有濃度漸減的P型摻雜物(傾斜摻雜)。以下顯示摻雜有Zn與Mg兩種作為P型摻雜物之例,但本發明不限定於此,例如可僅摻雜Zn,亦可摻雜3種以上。 又,就本發明更佳例而言,舉發光部(N型護套層、活性層、P型護套層)由AlGaInP系化合物半導體所構成者來說明,但不限定於此。The active layer 104 is composed of a surface body type active layer of uniform composition. The active layer 104 is doped with P-type dopants (inclined doping) of decreasing concentration from the P-type sheath layer 105 toward the N-type sheath layer 103 in a gentle or stepwise manner, for example. The following shows an example of doping two kinds of Zn and Mg as P-type dopants, but the present invention is not limited to this, for example, only Zn may be doped, or three or more kinds may be doped. Furthermore, in a more preferable example of the present invention, the light-emitting portion (N-type sheath layer, active layer, P-type sheath layer) is described as being composed of AlGaInP-based compound semiconductors, but it is not limited to this.

圖2顯示活性層中的平均P型摻雜物之濃度的說明圖。 在此,將自P型護套層105起朝向N型護套層103的方向定義為活性層104的深度方向,將活性層104與P型護套層105之界面定為深度位置的基準。上述傾斜摻雜的濃度曲線,自P型護套層105起算到深度1/3位置為止的區域(亦即,自P型護套層105起算到活性層104的1/3厚度大小之位置為止的區域)之平均P型摻雜物濃度成為1.0×1016 atoms/cm3 以上3×1017 atoms/cm3 以下。具體而言,就P型摻雜物而言,Zn的平均濃度設計為例如5×1016 atoms/cm3 ,Mg的平均濃度設計為例如1×1016 atoms/cm3 (平均濃度的合計值:6×1016 atoms/cm3 )。 另,在上述深度1/3位置為止的區域中,若所摻雜的P型摻雜物之種類為1種,則該1種本身的平均濃度落在上述濃度範圍即可,又,若為兩種以上,則各自之平均濃度相加的合計值落在上述濃度範圍即可。Fig. 2 shows an explanatory diagram of the average P-type dopant concentration in the active layer. Here, the direction from the P-type sheath layer 105 to the N-type sheath layer 103 is defined as the depth direction of the active layer 104, and the interface between the active layer 104 and the P-type sheath layer 105 is defined as the reference of the depth position. The above-mentioned oblique doping concentration curve is calculated from the P-type sheath layer 105 to the depth 1/3 position (that is, from the P-type sheath layer 105 to the 1/3 thickness of the active layer 104) The average P-type dopant concentration is 1.0×10 16 atoms/cm 3 or more and 3×10 17 atoms/cm 3 or less. Specifically, for P-type dopants, the average concentration of Zn is designed to be, for example, 5×10 16 atoms/cm 3 , and the average concentration of Mg is designed to, for example, 1×10 16 atoms/cm 3 (the total value of the average concentration : 6×10 16 atoms/cm 3 ). In addition, in the region up to 1/3 of the depth, if the type of P-type dopant to be doped is one type, the average concentration of the one type itself may fall within the above-mentioned concentration range, and if it is If there are more than two types, the sum of their average concentrations should fall within the above-mentioned concentration range.

如上所述,只要係P型摻雜物的傾斜摻雜,且深度1/3的位置為止的區域之平均濃度為3.0×1017 atoms/cm3 以下,則能抑制壽命特性惡化。而且,因為深度1/3的位置為止的區域之平均濃度為1.0×1016 atoms/cm3 以上,所以能提昇光輸出,並能提昇相應於環境溫度的輝度特性。如此,在活性層104中P型摻雜物的濃度曲線滿足上述條件之情形,能兼顧習知品無法達成的、提昇相應於環境溫度的輝度特性及抑制壽命特性惡化。As described above, as long as the P-type dopant is obliquely doped and the average concentration of the region up to the depth 1/3 is 3.0×10 17 atoms/cm 3 or less, the deterioration of the lifetime characteristics can be suppressed. In addition, since the average concentration of the region up to the depth 1/3 is 1.0×10 16 atoms/cm 3 or more, the light output can be improved, and the brightness characteristic corresponding to the ambient temperature can be improved. In this way, when the concentration curve of the P-type dopant in the active layer 104 satisfies the above-mentioned conditions, it is possible to balance the improvement of the brightness characteristics corresponding to the ambient temperature and the suppression of the deterioration of the lifetime characteristics that cannot be achieved by conventional products.

以下說明針對上述本發明之效果調查的實驗。 (實驗) 於[001]方向傾斜15度的GaAs基板上,以有機金屬氣相磊晶法(MOVPE)法,形成下述各層依序逐次疊層的發光元件用晶圓:1.0μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的蝕刻終止層;1.0μm厚的N型護套層;0.9μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的活性層;由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的1.0μm厚之P型護套層;由Gay In1 y P(0.0≦y≦1.0)所構成的中間組成層(緩衝層);具有0.5μm以上厚度的GaP電流擴散層(電流傳播層)。再者,形成電極並進行晶片切割,再進行打線接合而製造出發光元件。The following describes an experiment for investigating the effect of the above-mentioned present invention. (Experiment) On a GaAs substrate with a 15-degree tilt in the [001] direction, the following layers are sequentially stacked using the metal-organic vapor phase epitaxy (MOVPE) method to form a light-emitting element wafer: 1.0μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) an etching stop layer; 1.0μm thick N-type sheath layer; 0.9μm thick layer ( Active layer composed of Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6); consisting of (Al x Ga 1 x ) y In 1 y P(0≦ x ≦ 1,0.4 ≦ y ≦ 0.6) P -type layer of 1.0μm thickness of the sheath is formed; a Ga y in 1 - y P ( 0.0 ≦ y ≦ 1.0) consisting of an intermediate layer (buffer layer) is formed; a GaP current spreading layer (current spreading layer) with a thickness of 0.5μm or more. Furthermore, electrodes are formed, wafer dicing is performed, and wire bonding is performed to manufacture a light-emitting element.

另,活性層由均一組成的(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)層所構成。 再者,活性層以濃度自P型護套層起朝向N型護套層而漸減的方式摻雜有P型摻雜物。此際,藉由改變自活性層的P型護套層起算到深度1/3位置為止的區域之平均濃度,製造出該區域之平均濃度不同的複數發光元件。 並且,在各發光元件中,針對在0℃與60℃下的相對光輸出比、及壽命特性進行實驗。將其結果顯示於表1。In addition, the active layer is composed of a uniformly composed (Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6) layer. Furthermore, the active layer is doped with P-type dopants in a manner that the concentration gradually decreases from the P-type sheath layer toward the N-type sheath layer. At this time, by changing the average concentration of the region from the P-type sheath layer of the active layer to the depth 1/3 position, a plurality of light-emitting elements with different average concentrations in the region are manufactured. In addition, in each light-emitting element, experiments were performed on the relative light output ratio at 0°C and 60°C and lifetime characteristics. The results are shown in Table 1.

【表1】 平均濃度 (atoms/cm3 ) 相對光輸出比 (0℃vs60℃) 壽命特性 (%) 3.00×1015 0.8 93 6.00×1015 0.8 92 1.00×1016 0.86 91 3.00×1016 0.86 87 6.00×1016 0.87 85 1.00×1017 0.89 83 3.00×1017 0.9 81 6.00×1017 0.9 61 【Table 1】 Average concentration (atoms/cm 3 ) Relative light output ratio (0℃vs60℃) Life characteristics (%) 3.00×10 15 0.8 93 6.00×10 15 0.8 92 1.00×10 16 0.86 91 3.00×10 16 0.86 87 6.00×10 16 0.87 85 1.00×10 17 0.89 83 3.00×10 17 0.9 81 6.00×10 17 0.9 61

如表1所示,得知只要在傾斜摻雜的活性層中,自P型護套層起算到深度1/3的位置為止的區域之平均濃度為1.0×1016 atoms/cm3 以上,則相對光輸出比為0.86以上,該比更進一步靠近1,而能減少相應於環境溫度的輸出變化。又,得知只要在3.0×1017 atoms/cm3 以下,則能使壽命特性在81%以上,而能抑制其惡化。 由此等結果得知,為了兼顧良好的相應於環境溫度的輝度特性及良好的壽命特性,必須在傾斜摻雜的活性層之上述區域中定為1.0×1016 atoms/cm3 以上,且為3.0×1017 atoms/cm3 以下的濃度範圍。As shown in Table 1, it is known that as long as the average concentration of the area from the P-type sheath layer to the depth 1/3 of the active layer is 1.0×10 16 atoms/cm 3 or more in the obliquely doped active layer, then The relative light output ratio is 0.86 or higher, which is closer to 1, and can reduce the output change corresponding to the ambient temperature. In addition, it is found that as long as it is 3.0×10 17 atoms/cm 3 or less, the lifetime characteristic can be 81% or more, and the deterioration can be suppressed. From these results, it is known that in order to have both good brightness characteristics corresponding to ambient temperature and good lifetime characteristics, it is necessary to set 1.0×10 16 atoms/cm 3 or more in the above-mentioned region of the obliquely doped active layer. The concentration range is 3.0×10 17 atoms/cm 3 or less.

又,在圖1的第一實施形態中,更宜為自P型護套層105起算深度1/3的位置到深度2/3的位置之區域(亦即,自P型護套層105起算活性層104的1/3厚度大小之位置到2/3厚度大小之位置為止的區域)之平均P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。具體而言,Zn的平均濃度設計為例如2×1016 atoms/cm3 ,Mg的平均濃度設計為例如0.5×1016 atoms/cm3 (平均濃度的合計值:2.5×1016 atoms/cm3 )。 只要在如上所述的濃度範圍,能更加確實地抑制壽命特性惡化。Moreover, in the first embodiment of FIG. 1, it is more preferable to be a region from a position of 1/3 of the depth of the P-type sheath layer 105 to a position of 2/3 of the depth of the P-type sheath layer 105 (that is, from the P-type sheath layer 105) The active layer 104 has an average P-type dopant concentration of 0.3×10 16 atoms/cm 3 or more, and 3.0×10 16 atoms/ cm 3 or less. Specifically, the average concentration of Zn is designed to be, for example, 2×10 16 atoms/cm 3 , and the average concentration of Mg is designed to, for example, 0.5×10 16 atoms/cm 3 (the total value of the average concentration: 2.5×10 16 atoms/cm 3 ). As long as it is in the above-mentioned concentration range, deterioration of life characteristics can be suppressed more reliably.

再者,自P型護套層105起算深度2/3的位置到N型護套層103之側的區域(亦即,自P型護套層105起算活性層104的2/3厚度大小之位置到N型護套層103為止的區域)的平均P型摻雜物濃度(具體而言為Zn與Mg的平均濃度之合計值)宜為0.3×1016 atoms/cm3 以下。另,下限值不特別限定,但可定為例如0atoms/cm3 以上。 只要在如上所述的濃度範圍,則能進一步確實地抑制壽命特性惡化。Furthermore, the area from the depth of 2/3 of the P-type sheath layer 105 to the side of the N-type sheath layer 103 (that is, the thickness of 2/3 of the active layer 104 from the P-type sheath layer 105) The average P-type dopant concentration (specifically, the sum of the average concentrations of Zn and Mg) of the region from the position to the N-type sheath layer 103 is preferably 0.3×10 16 atoms/cm 3 or less. In addition, the lower limit is not particularly limited, but can be set to, for example, 0 atoms/cm 3 or more. As long as the concentration is in the above-mentioned concentration range, the deterioration of the lifetime characteristics can be further reliably suppressed.

(第二實施形態) 本發明之發光元件的第二實施形態顯示於圖3。如圖3所示,第二實施形態的發光元件210於GaAs出發基板200上具有:例如厚度0.5μm的GaAs緩衝層;例如厚度1.0μm的AlInP蝕刻終止層202;例如厚度1.0μm的N型AlGaInP護套層203;例如厚度0.48μm的AlGaInP活性層204;例如厚度1.0μm的P型AlGaInP護套層205;將與電流傳播層之晶格錯合加以緩和的P型InGaP緩衝層206;以及將施加至元件的電流加以傳播且擴散、具有光萃取功能之例如厚度5.0μm的P型GaP電流傳播層207。 亦可沒有GaAs緩衝層。另,在圖3中省略發光元件的電極等。(Second Embodiment) The second embodiment of the light-emitting device of the present invention is shown in FIG. 3. As shown in FIG. 3, the light-emitting element 210 of the second embodiment has on the GaAs starting substrate 200: for example, a GaAs buffer layer with a thickness of 0.5 μm; for example, an AlInP etching stop layer 202 with a thickness of 1.0 μm; for example, an N-type AlGaInP with a thickness of 1.0 μm The sheath layer 203; for example, the AlGaInP active layer 204 with a thickness of 0.48 μm; for example, the P-type AlGaInP sheath layer 205 with a thickness of 1.0 μm; the P-type InGaP buffer layer 206 that relaxes the lattice misalignment with the current propagation layer; and The current applied to the element propagates and diffuses, and has a light extraction function, for example, a P-type GaP current propagation layer 207 with a thickness of 5.0 μm. There may be no GaAs buffer layer. In addition, the electrodes of the light-emitting element and the like are omitted in FIG. 3.

將Si、S、Se之中1種以上摻雜至N型護套層203作為N型摻雜物,將Zn、Mg、Te之中1種以上摻雜至P型護套層205、P型緩衝層206及P型電流傳播層207作為P型摻雜物。Doping more than one of Si, S, and Se into the N-type sheath layer 203 as an N-type dopant, and doping more than one of Zn, Mg, and Te into the P-type sheath layer 205 and P-type The buffer layer 206 and the P-type current propagation layer 207 serve as P-type dopants.

N型護套層203係以1層以上之組成及摻雜水準的磊晶層所構成,P型護套層205係以1層以上之組成及摻雜水準的磊晶層所構成。The N-type sheath layer 203 is composed of an epitaxial layer with more than one composition and doping level, and the P-type sheath layer 205 is composed of an epitaxial layer with more than one composition and doping level.

在第二實施形態的發光元件210中,活性層204係由將AlGaInP所構成的發光復合層與具有大於發光復合層之組成的能帶隙之組成的障壁層加以多重接合的多重接合型活性層所構成。障壁層具有比起發光復合層之AlGaInP更高的Al組成。又,障壁層的厚度可設定為比起波函數重疊的德布羅伊波長更薄的厚度,亦可設定為更厚的厚度。例如可定為發光復合層的厚度8nm,障壁層的厚度8nm,且為30對的活性層構造。In the light-emitting element 210 of the second embodiment, the active layer 204 is a multiple junction type active layer in which a light-emitting composite layer composed of AlGaInP and a barrier layer having an energy band gap larger than the composition of the light-emitting composite layer are multiple-joined Constituted. The barrier layer has a higher Al composition than the AlGaInP of the light-emitting composite layer. In addition, the thickness of the barrier layer may be set to be thinner than the De Broglie wavelength where the wave function overlaps, or may be set to be thicker. For example, the thickness of the light-emitting composite layer is 8 nm, the thickness of the barrier layer is 8 nm, and the active layer structure is 30 pairs.

活性層204自P型護套層205起朝向N型護套層203以例如平緩傾斜或階梯狀的方式摻雜有濃度漸減的P型摻雜物(傾斜摻雜)。以下顯示摻雜有Zn與Mg兩種作為P型摻雜物之例,但與第一實施形態同樣,並不限定於此。The active layer 204 is doped with P-type dopants (inclined doping) of decreasing concentration from the P-type sheath layer 205 toward the N-type sheath layer 203 in a gentle or stepwise manner, for example. The following shows an example in which two kinds of Zn and Mg are doped as P-type dopants, but it is the same as in the first embodiment, and is not limited to this.

上述傾斜摻雜的濃度曲線,自P型護套層205起算到深度1/3的位置為止的區域之平均P型摻雜物濃度為1.0×1016 atoms/cm3 以上3×1017 atoms/cm3 以下。具體而言,就P型摻雜物而言,Zn的平均濃度設計為例如5×1016 atoms/cm3 ,Mg的平均濃度設計為例如1×1016 atoms/cm3 (平均濃度的合計值:6×1016 atoms/cm3 )。 只要為如此,則能兼顧良好的相應於環境溫度的輝度特性及良好的壽命特性。In the above-mentioned oblique doping concentration curve, the average P-type dopant concentration in the region from the P-type sheath layer 205 to the depth 1/3 position is 1.0×10 16 atoms/cm 3 or more and 3×10 17 atoms/ cm 3 or less. Specifically, for P-type dopants, the average concentration of Zn is designed to be, for example, 5×10 16 atoms/cm 3 , and the average concentration of Mg is designed to, for example, 1×10 16 atoms/cm 3 (the total value of the average concentration : 6×10 16 atoms/cm 3 ). As long as this is the case, it is possible to achieve both good luminance characteristics corresponding to ambient temperature and good lifetime characteristics.

又,自P型護套層205起算深度1/3的位置到深度2/3的位置之區域的平均P型摻雜物濃度宜為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。具體而言,Zn的平均濃度設計為例如2×1016 atoms/cm3 ,Mg的平均濃度設計為例如0.5×1016 atoms/cm3 (平均濃度的合計值:2.5×1016 atoms/cm3 )。 再者,自P型護套層205起算深度2/3的位置到N型護套層203之側的區域之平均P型摻雜物濃度(具體而言為Zn與Mg之平均濃度的合計值)宜為0.3×1016 atoms/cm3 以下。另,下限值不特別限定,可定為例如0atoms/cm3 以上。 只要上述各區域在此等濃度範圍,則能進一步確實地抑制壽命特性惡化。In addition, the average P-type dopant concentration in the region from the position 1/3 of the depth to the position 2/3 of the depth from the P-type sheath layer 205 is preferably 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less. Specifically, the average concentration of Zn is designed to be, for example, 2×10 16 atoms/cm 3 , and the average concentration of Mg is designed to, for example, 0.5×10 16 atoms/cm 3 (the total value of the average concentration: 2.5×10 16 atoms/cm 3 ). Furthermore, the average P-type dopant concentration in the region from the depth 2/3 of the P-type sheath layer 205 to the side of the N-type sheath layer 203 (specifically, the sum of the average concentrations of Zn and Mg) ) Is preferably 0.3×10 16 atoms/cm 3 or less. In addition, the lower limit is not particularly limited, and can be set to, for example, 0 atoms/cm 3 or more. As long as the above-mentioned regions are within these concentration ranges, the deterioration of the lifetime characteristics can be further reliably suppressed.

其次說明本發明之發光元件之製造方法。另,在此以製造圖1之發光元件110之情形為例說明。又,就針對活性層的摻雜方法而言舉利用氣體摻雜之方法(第一製造方法)與利用熱處理之摻雜方法(第二製造方法)為例說明,但針對活性層之摻雜方法不限定於此。 (第一製造方法) 首先,說明利用氣體摻雜進行針對活性層的摻雜之例。 準備GaAs出發基板100作為成長用基板,清洗之後,放入MOVPE(Metal Organic Vapor Phase Epitaxy,金屬有機氣相磊晶)爐,於GaAs出發基板100上磊晶成長出AlInP蝕刻終止層102、N型AlGaInP護套層103、AlGaInP活性層104、P型AlGaInP護套層105、及P型InGaP緩衝層106。Next, the manufacturing method of the light-emitting element of the present invention will be explained. In addition, the case of manufacturing the light-emitting element 110 of FIG. 1 is taken as an example for description. Also, regarding the doping method of the active layer, the method using gas doping (the first manufacturing method) and the doping method using heat treatment (the second manufacturing method) are described as examples, but the doping method of the active layer is Not limited to this. (First manufacturing method) First, an example of doping to the active layer by gas doping will be described. The GaAs starting substrate 100 is prepared as a growth substrate. After cleaning, it is placed in a MOVPE (Metal Organic Vapor Phase Epitaxy) furnace to epitaxially grow AlInP etching stop layer 102 and N-type on the GaAs starting substrate 100 The AlGaInP sheath layer 103, the AlGaInP active layer 104, the P-type AlGaInP sheath layer 105, and the P-type InGaP buffer layer 106.

另,上述各層之磊晶成長可藉由公知的MOVPE法來進行。作為Al、Ga、In、P的各成分源之原料氣體,雖不限定於此,但可使用例如下述者。 ・Al源氣體:三甲基鋁(TMAl),三乙基鋁(TEAl)等。 ・Ga源氣體:三甲基鎵(TMGa),三乙基鎵(TEGa)等。 ・In源氣體:三甲基銦(TMIn),三乙基銦(TEIn)等。 ・P源氣體:三甲基磷(TMP),三乙基磷(TEP),磷化氫(PH3)等。In addition, the epitaxial growth of the above-mentioned layers can be performed by the well-known MOVPE method. Although not limited to this as the source gas of the component sources of Al, Ga, In, and P, for example, the following can be used. ・Al source gas: trimethyl aluminum (TMAl), triethyl aluminum (TEAl), etc. ・Ga source gas: Trimethylgallium (TMGa), Triethylgallium (TEGa), etc. ・In source gas: trimethyl indium (TMIn), triethyl indium (TEIn), etc. ・P source gas: trimethylphosphorus (TMP), triethylphosphorus (TEP), phosphine (PH3), etc.

又,就針對各層的摻雜物之摻雜而言,可藉由氣體摻雜來進行。可使活性層等各層一邊磊晶成長並且一邊進行氣體摻雜。就摻雜物氣體而言,可使例如下述者。 (P型摻雜物) ・Zn源:二甲基鋅(DMZn),二乙基鋅(DEZn)等。 ・Mg源:雙(環戊二烯)鎂(Cp2 Mg)等。 ・Te源:二甲基碲(DMTe),二乙基碲(DETe)等 (N型摻雜物) ・Si源:甲矽烷等矽氫化物等。 ・S源:硫化氫(H2 S)等。 ・Se源:硒化氫等。In addition, the doping of dopants for each layer can be performed by gas doping. The active layer and other layers can be grown epitaxially and gas doped. As for the dopant gas, for example, the following can be used. (P-type dopant) ・Zn source: dimethyl zinc (DMZn), diethyl zinc (DEZn), etc.・Mg source: Bis (cyclopentadiene) magnesium (Cp 2 Mg), etc.・Te source: dimethyl tellurium (DMTe), diethyl tellurium (DETe), etc. (N-type dopants) ・Si source: silicon hydride such as silane, etc.・S source: hydrogen sulfide (H 2 S), etc.・Se source: hydrogen selenide, etc.

另,在此氣體摻雜之際,關於活性層104中的P型摻雜物而言,定為如圖2所示的傾斜摻雜之濃度曲線。亦即,在活性層104中,以P型摻雜物之濃度自P型護套層105之側往N型護套層103之側漸減的方式進行傾斜摻雜。並且摻雜成如下:自P型護套層105起算到深度1/3的位置為止的區域之平均P型摻雜物濃度為1.0×1016 atoms/cm3 以上,且為3.0×1017 atoms/cm3 以下。 可藉由例如質量流量控制器等來控制摻雜物氣體的流量,而簡便地以如上所述的濃度曲線進行氣體摻雜。 由於磊晶成長中的熱效果,而多少容易成為比起所欲的濃度曲線更偏移至熱平衡側的濃度曲線。關於此點,只要考慮到該偏移而適當調整流量等來進行氣體摻雜,成為所欲的濃度曲線即可。 並且,只要在活性層中P型摻雜物為此種濃度曲線,則能如前所述,達到兼顧提昇相應於環境溫度的輝度特性及抑制壽命特性惡化。In addition, during this gas doping, the P-type dopant in the active layer 104 is set as the concentration curve of the inclined doping as shown in FIG. 2. That is, the active layer 104 is doped obliquely in such a way that the concentration of the P-type dopant gradually decreases from the side of the P-type sheath layer 105 to the side of the N-type sheath layer 103. And the doping is as follows: the average P-type dopant concentration in the region from the P-type sheath layer 105 to the depth 1/3 position is 1.0×10 16 atoms/cm 3 or more and 3.0×10 17 atoms /cm 3 or less. The flow rate of the dopant gas can be controlled by, for example, a mass flow controller, and the gas doping can be easily performed with the concentration curve described above. Due to the thermal effect during epitaxial growth, it is more likely to become a concentration curve that shifts to the thermal equilibrium side than the desired concentration curve. In this regard, it is only necessary to appropriately adjust the flow rate and the like in consideration of the deviation to perform gas doping to achieve a desired concentration curve. Moreover, as long as the P-type dopant in the active layer has such a concentration curve, as described above, it is possible to achieve both the improvement of the brightness characteristic corresponding to the ambient temperature and the suppression of the deterioration of the lifetime characteristic.

又,將P型摻雜物摻雜至活性層104時,宜摻雜成如下:在活性層104中,自P型護套層105起算深度1/3的位置到深度2/3的位置之區域的平均P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。 再者,宜摻雜成如下:在活性層104中,自P型護套層105起算深度2/3的位置到N型護套層103之側的區域之平均P型摻雜物濃度為0.3×1016 atoms/cm3 以下。另,下限值不特別限定,可定為例如0atoms/cm3 以上。 只要上述各區域在此等濃度範圍,則能更進一步確實地抑制壽命特性惡化。In addition, when the P-type dopant is doped into the active layer 104, it is preferable to dope as follows: In the active layer 104, from the position of the depth 1/3 of the P-type sheath layer 105 to the position of 2/3 of the depth The average P-type dopant concentration of the region is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less. Furthermore, the doping is preferably as follows: In the active layer 104, the average P-type dopant concentration in the region from the position of 2/3 of the depth of the P-type sheath layer 105 to the side of the N-type sheath layer 103 is 0.3 ×10 16 atoms/cm 3 or less. In addition, the lower limit is not particularly limited, and can be set to, for example, 0 atoms/cm 3 or more. As long as the above-mentioned regions are within these concentration ranges, the deterioration of the lifetime characteristics can be further reliably suppressed.

此後,以HVPE法(氫化物氣相磊晶法:Hydride Vapor Phase Epitaxy法)來氣相成長P型GaP電流傳播層107。 HVPE法,具體而言例如藉由將金屬Ga加熱保持在既定溫度,並且將氯化氫導入至該金屬Ga上,藉由下述(1)式的反應來產生GaCl,並與載子氣體即H2 氣體共同供給至基板上。 Ga(液體)+HCl(氣體)→GaCl(氣體)+1/2H2 (氣體)…(1) 成長溫度可設定在例如640℃以上860℃以下。又,將V族元素P,例如PH3 ,與載子氣體即H2 共同供給至基板上。再者,可將例如Zn以二甲基鋅(DMZn)的形式供給作為P型摻雜物,藉由如下述(2)式的反應來形成電流傳播層107。 GaCl(氣體)+PH3 (氣體) →GaP(固體)+HCl(氣體)+H2 (氣體)…(2)Thereafter, the P-type GaP current propagation layer 107 was vapor-grown by the HVPE method (Hydride Vapor Phase Epitaxy method). In the HVPE method, specifically, for example, by heating metal Ga to maintain a predetermined temperature, and introducing hydrogen chloride to the metal Ga, GaCl is generated by the reaction of the following formula (1), and it interacts with carrier gas, which is H 2 The gas is supplied to the substrate together. Ga (liquid) + HCl (gas) → GaCl (gas) + 1/2H 2 (gas)... (1) The growth temperature can be set at 640°C or higher and 860°C or lower. In addition, the group V element P, such as PH 3 , is supplied to the substrate together with H 2 which is a carrier gas. Furthermore, for example, Zn can be supplied as a P-type dopant in the form of dimethyl zinc (DMZn), and the current propagation layer 107 can be formed by the reaction shown in the following formula (2). GaCl (gas) + PH 3 (gas) → GaP (solid) + HCl (gas) + H 2 (gas)...(2)

(第二製造方法:利用熱處理之摻雜) 其次說明利用熱處理來進行針對活性層的摻雜之例。 基本上與第一製造方法同樣進行,自出發基板100的準備起進行至緩衝層106的形成。其中,考慮到將P型摻雜物藉由熱處理自P型護套層105往活性層104擴散來進行摻雜,在活性層104的磊晶成長時定為無摻雜。又,在P型護套層105中亦可用較第一製造方法之情形更加高濃度先摻雜好P型摻雜物。(Second manufacturing method: doping by heat treatment) Next, an example of doping to the active layer by heat treatment will be described. Basically, it is performed in the same manner as the first manufacturing method, starting from the preparation of the starting substrate 100 to the formation of the buffer layer 106. Among them, considering that the P-type dopant is diffused from the P-type sheath layer 105 to the active layer 104 by heat treatment for doping, the active layer 104 is determined to be undoped during epitaxial growth. In addition, the P-type sheath layer 105 can also be doped with P-type dopants at a higher concentration than in the first manufacturing method.

更具體而言,P型護套層105的P型摻雜物濃度,將例如Zn、Mg定為P型摻雜物之情形,可將Zn的濃度定為1.0×1016 ~3.0×1018 atoms/cm3 ,Mg的濃度定為1.0×1016 ~5.0×1017 atoms/cm3 的濃度範圍。只要在此種濃度範圍,能更加確實地在下一程序即熱處理程序定為如圖2所示的傾斜摻雜之濃度曲線。More specifically, the P-type dopant concentration of the P-type sheath layer 105, for example, when Zn and Mg are set as P-type dopants, the concentration of Zn can be set to 1.0×10 16 to 3.0×10 18 The concentration of atoms/cm 3 and Mg is set to a concentration range of 1.0×10 16 to 5.0×10 17 atoms/cm 3 . As long as it is in this concentration range, the next procedure, the heat treatment procedure, can be set as the inclined doping concentration curve shown in FIG. 2 more reliably.

如上所述形成出至少P型護套層105為止的各層後(在此例中連緩衝層106都形成完畢),在MOVPE爐內,例如PH3 爐氛下,施加700℃以上、3小時以上的熱處理。在此定為在700℃(與磊晶成長時相同程度的溫度)下8小時的熱處理。藉由此種熱處理,能簡便地定為如圖2所示的傾斜摻雜之濃度曲線。藉由施加熱處理,使摻雜物自P型護套層105依循擴散式而擴散至活性層104內,形成朝向N型護套層103漸減的濃度曲線。After forming at least the layers up to the P-type sheath layer 105 as described above (in this example, even the buffer layer 106 is formed), in a MOVPE furnace, for example, in a PH 3 furnace atmosphere, apply 700°C or more for 3 hours or more Heat treatment. Here, the heat treatment is set at 700°C (the same temperature as during epitaxial growth) for 8 hours. By this heat treatment, it can be easily determined as the inclined doping concentration curve shown in FIG. 2. By applying heat treatment, the dopant diffuses from the P-type sheath layer 105 into the active layer 104 according to the diffusion method, forming a concentration curve that gradually decreases toward the N-type sheath layer 103.

另,熱處理的溫度、時間不特別限定,可適當決定來獲得期望的傾斜摻雜之濃度曲線。又,只要如上所述在PH3 爐氛下進行,則能有效地避免P(磷)自磊晶層表面脫離而較佳。In addition, the temperature and time of the heat treatment are not particularly limited, and can be appropriately determined to obtain a desired gradient doping concentration profile. Moreover, as long as it is carried out in a PH 3 furnace atmosphere as described above, it is preferable to effectively prevent P (phosphorus) from detaching from the surface of the epitaxial layer.

其後,與第一製造方法同樣進行,以HVPE法形成電流傳播層107。 另,在上述例中,係於形成緩衝層106後進行熱處理,但亦可不在該時序進行熱處理,取而代之在形成電流傳播層107後施加熱處理(在HVPE爐、PH3 爐氛下,700℃以上、3小時以上,尤其在700℃下8小時),在活性層104中形成傾斜摻雜之濃度曲線。 [實施例]Thereafter, in the same manner as in the first manufacturing method, the current propagation layer 107 is formed by the HVPE method. In addition, in the above example, the heat treatment is performed after the buffer layer 106 is formed. However, the heat treatment may not be performed at this timing. Instead, heat treatment is applied after the current propagation layer 107 is formed (in an HVPE furnace, PH 3 furnace atmosphere, 700°C or higher , 3 hours or more, especially 8 hours at 700°C), a gradient doping concentration curve is formed in the active layer 104. [Example]

以下顯示本發明的實施例及比較例來更加具體地說明本發明,但本發明並非限定於此。 (實施例1) 如下進行而藉由本發明之製造方法來製造出本發明之發光元件。 於[001]方向傾斜15度的GaAs基板上,以有機金屬氣相磊晶法(MOVPE)法,形成下述各層依序逐次疊層的發光元件用晶圓:1.0μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的蝕刻終止層;1.0μm厚的N型護套層;0.9μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的活性層;由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的1.0μm厚的P型護套層;由Gay In1 y P(0.0≦y≦1.0)所構成的中間組成層(緩衝層);具有0.5μm以上厚度的GaP電流擴散層(電流傳播層)。Examples and comparative examples of the present invention are shown below to explain the present invention more specifically, but the present invention is not limited thereto. (Example 1) The light-emitting element of the present invention was manufactured by the manufacturing method of the present invention as follows. On a GaAs substrate with a 15-degree tilt in the [001] direction, a metal-organic vapor phase epitaxy (MOVPE) method was used to form a light-emitting element wafer with the following layers sequentially stacked: 1.0μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an etching stop layer; 1.0μm thick N-type sheath layer; 0.9μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an active layer; composed of (Al x Ga 1 x ) y In 1 y P (0≦x≦1 , 0.4 ≦ y P-type layer 1.0μm thick sheath constituted ≦ 0.6); a Ga y in 1 - y P ( 0.0 ≦ y ≦ 1.0) consisting of an intermediate layer (buffer layer) is formed; having more than 0.5μm Thickness of GaP current spreading layer (current spreading layer).

活性層由均一組成的(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)層所構成。 活性層以濃度自P型護套層朝向N型護套層漸減的方式摻雜P型摻雜物(Zn及Mg兩種)。具體而言,形成活性層並且流通DEZn、Cp2 Mg而進行氣體摻雜。 濃度曲線,在與P型護套層之界面中,作為P型摻雜物的Zn之濃度為5×1016 atoms/cm3 ,作為P型摻雜物的Mg之濃度為1×1016 atoms/cm3 。 並且,自P型護套層起算深度0.3μm的位置(活性層全厚0.9μm的1/3)為止的區域之Zn平均濃度為2×1016 atoms/cm3 ,Mg平均濃度為0.5×1016 atoms/cm3 (平均濃度的合計值:2.5×1016 atoms/cm3 )。 又,自深度0.3μm的位置到深度0.6μm的位置(自全厚0.9μm的1/3至2/3)為止的區域之中的Zn平均濃度為0.5×1016 atoms/cm3 ,Mg平均濃度為0.2×1016 atoms/cm3 (平均濃度的合計值:0.7×1016 atoms/cm3 )。 其後深度(自深度2/3的位置到N型護套層為止)的Mg及Zn各自之平均濃度之合計值為0.3×1016 atoms/cm3 以下。 將電極形成在如此製造的晶圓並進行晶片切割,再進行打線接合來製造出發光元件。The active layer is composed of a uniformly composed (Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6) layer. The active layer is doped with P-type dopants (both Zn and Mg) in a manner that the concentration gradually decreases from the P-type sheath layer to the N-type sheath layer. Specifically, an active layer is formed and DEZn and Cp 2 Mg are flowed to perform gas doping. Concentration curve. In the interface with the P-type sheath layer, the concentration of Zn as the P-type dopant is 5×10 16 atoms/cm 3 , and the concentration of Mg as the P-type dopant is 1×10 16 atoms /cm 3 . In addition, the average Zn concentration in the area from the P-type sheath layer to a depth of 0.3 μm (1/3 of the total thickness of the active layer 0.9 μm) is 2×10 16 atoms/cm 3 , and the average Mg concentration is 0.5×10 16 atoms/cm 3 (Total average concentration: 2.5×10 16 atoms/cm 3 ). In addition, the average concentration of Zn in the region from the position with a depth of 0.3 μm to the position with a depth of 0.6 μm (from 1/3 to 2/3 of the total thickness of 0.9 μm) is 0.5×10 16 atoms/cm 3 , and the average Mg concentration The concentration is 0.2×10 16 atoms/cm 3 (total value of average concentration: 0.7×10 16 atoms/cm 3 ). The sum of the average concentrations of Mg and Zn in the subsequent depth (from the position of the depth 2/3 to the N-type sheath layer) is 0.3×10 16 atoms/cm 3 or less. The electrodes are formed on the wafer thus manufactured, the wafer is diced, and then wire bonding is performed to manufacture a light-emitting element.

(實施例2) 如下進行而藉由本發明之製造方法來製造本發明之發光元件。 於[001]方向傾斜15度的GaAs基板上,以有機金屬氣相磊晶法(MOVPE)法,形成下述各層依序逐次疊層的發光元件用晶圓:1.0μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的蝕刻終止層;1.0μm厚的N型護套層;0.48μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的活性層;由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的1.0μm厚的P型護套層;由Gay In1 y P(0.0≦y≦1.0)所構成的中間組成層(緩衝層);具有0.5μm以上厚度的GaP電流擴散層(電流傳播層)。(Example 2) The light-emitting element of the present invention was manufactured by the manufacturing method of the present invention as follows. On a GaAs substrate with a 15-degree tilt in the [001] direction, a metal-organic vapor phase epitaxy (MOVPE) method was used to form a light-emitting element wafer with the following layers sequentially stacked: 1.0μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an etching stop layer; 1.0μm thick N-type sheath layer; 0.48μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an active layer; composed of (Al x Ga 1 x ) y In 1 y P (0≦x≦1 , 0.4 ≦ y P-type layer 1.0μm thick sheath constituted ≦ 0.6); a Ga y in 1 - y P ( 0.0 ≦ y ≦ 1.0) consisting of an intermediate layer (buffer layer) is formed; having more than 0.5μm Thickness of GaP current spreading layer (current spreading layer).

活性層由下述各者交互疊層的多重障壁型活性層所構成:由第一組成的(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)層所構成的發光復合層;以及由第二組成的(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)層所構成的障壁層。 第一組成的Al比率設定為較第二組成的Al比率更少的比率。The active layer is composed of the following multiple barrier active layers alternately laminated: the first composition (Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6 ) A light-emitting composite layer composed of a layer; and a barrier layer composed of a second composition (Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6) layer. The Al ratio of the first composition is set to a lower ratio than the Al ratio of the second composition.

活性層以濃度自P型護套層朝向N型護套層漸減的方式摻雜P型摻雜物(Zn及Mg兩種)。具體而言,形成活性層並且流通DEZn、Cp2 Mg而進行氣體摻雜。 濃度曲線,在與P型護套層之界面中,作為P型摻雜物的Zn之濃度為5×1016 atoms/cm3 ,作為P型摻雜物的Mg之濃度為1×1016 atoms/cm3 。 並且,自P型護套層起算深度0.16μm的位置(活性層全厚0.48μm的1/3)為止的區域之Zn的平均濃度為2×1016 atoms/cm3 ,Mg平均濃度為0.5×1016 atoms/cm3 (平均濃度的合計值:2.5×1016 atoms/cm3 )。 又,自深度0.16μm的位置到深度0.32μm的位置(自全厚0.48μm的1/3至2/3)為止的區域之中的Zn平均濃度為0.5×1016 atoms/cm3 ,Mg平均濃度為0.2×1016 atoms/cm3 (平均濃度的合計值:0.7×1016 atoms/cm3 )。 其後深度(自深度2/3的位置到N型護套層為止)的Mg及Zn各者之平均濃度的合計值為0.3×1016 atoms/cm3 以下。 將電極形成在如此製造的晶圓並進行晶片切割,再進行打線接合來製造出發光元件。The active layer is doped with P-type dopants (both Zn and Mg) in a manner that the concentration gradually decreases from the P-type sheath layer to the N-type sheath layer. Specifically, an active layer is formed and DEZn and Cp 2 Mg are flowed to perform gas doping. Concentration curve. In the interface with the P-type sheath layer, the concentration of Zn as the P-type dopant is 5×10 16 atoms/cm 3 , and the concentration of Mg as the P-type dopant is 1×10 16 atoms /cm 3 . In addition, the average concentration of Zn in the region from the P-type sheath layer to a depth of 0.16 μm (1/3 of the total thickness of the active layer 0.48 μm) is 2×10 16 atoms/cm 3 , and the average concentration of Mg is 0.5× 10 16 atoms/cm 3 (Total average concentration: 2.5×10 16 atoms/cm 3 ). In addition, the average concentration of Zn in the region from the position with a depth of 0.16 μm to the position with a depth of 0.32 μm (from 1/3 to 2/3 of the total thickness of 0.48 μm) is 0.5×10 16 atoms/cm 3 , and Mg averages The concentration is 0.2×10 16 atoms/cm 3 (total value of average concentration: 0.7×10 16 atoms/cm 3 ). The total value of the average concentration of each of Mg and Zn in the subsequent depth (from the depth 2/3 position to the N-type sheath layer) is 0.3×10 16 atoms/cm 3 or less. The electrodes are formed on the wafer thus manufactured, the wafer is diced, and then wire bonding is performed to manufacture a light-emitting element.

(比較例1) 如下進行而製造出發光元件。 於[001]方向傾斜15度的GaAs基板上,以有機金屬氣相磊晶法(MOVPE)法,形成下述各層依序逐次疊層的發光元件用晶圓:1.0μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的蝕刻終止層;1.0μm厚的N型護套層;0.9μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的活性層;由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的1.0μm厚的P型護套層;由Gay In1 y P(0.0≦y≦1.0)所構成的中間組成層(緩衝層);具有0.5μm以上厚度的GaP電流擴散層(電流傳播層)。(Comparative Example 1) The light-emitting element was manufactured as follows. On a GaAs substrate with a 15-degree tilt in the [001] direction, a metal-organic vapor phase epitaxy (MOVPE) method was used to form a light-emitting element wafer with the following layers sequentially stacked: 1.0μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an etching stop layer; 1.0μm thick N-type sheath layer; 0.9μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an active layer; composed of (Al x Ga 1 x ) y In 1 y P (0≦x≦1 , 0.4 ≦ y P-type layer 1.0μm thick sheath constituted ≦ 0.6); a Ga y in 1 - y P ( 0.0 ≦ y ≦ 1.0) consisting of an intermediate layer (buffer layer) is formed; having more than 0.5μm Thickness of GaP current spreading layer (current spreading layer).

活性層由均一組成的(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)層所構成,且藉由氣體摻雜(使用DEZn、Cp2 Mg)定為活性層的Mg及Zn各自之濃度的合計值為0.3×1016 atoms/cm3 以下。 將電極形成在如此製造的晶圓並進行晶片切割,再進行打線接合來製造出發光元件。The active layer is composed of a uniformly composed (Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6) layer, and is doped by gas (using DEZn, Cp 2 Mg ) The total value of the respective concentrations of Mg and Zn in the active layer is set to 0.3×10 16 atoms/cm 3 or less. The electrodes are formed on the wafer thus manufactured, the wafer is diced, and then wire bonding is performed to manufacture a light-emitting element.

(比較例2) 如下進行而製造出發光元件。 於[001]方向傾斜15度的GaAs基板上,以有機金屬氣相磊晶法(MOVPE)法,形成下述各層依序逐次疊層的發光元件用晶圓:1.0μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的蝕刻終止層;1.0μm厚的N型護套層;0.9μm厚的由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的活性層;由(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)所構成的1.0μm厚的P型護套層;由Gay In1 y P(0.0≦y≦1.0)所構成的中間組成層(緩衝層);具有0.5μm以上厚度的GaP電流擴散層(電流傳播層)。(Comparative Example 2) The light-emitting element was manufactured as follows. On a GaAs substrate with a 15-degree tilt in the [001] direction, a metal-organic vapor phase epitaxy (MOVPE) method was used to form a light-emitting element wafer with the following layers sequentially stacked: 1.0μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an etching stop layer; 1.0μm thick N-type sheath layer; 0.9μm thick (Al x Ga 1 x ) y In 1 y P (0≦x≦1, 0.4≦y≦0.6) composed of an active layer; composed of (Al x Ga 1 x ) y In 1 y P (0≦x≦1 , 0.4 ≦ y P-type layer 1.0μm thick sheath constituted ≦ 0.6); a Ga y in 1 - y P ( 0.0 ≦ y ≦ 1.0) consisting of an intermediate layer (buffer layer) is formed; having more than 0.5μm Thickness of GaP current spreading layer (current spreading layer).

活性層由均一組成的(Alx Ga1 xy In1 y P(0≦x≦1,0.4≦y≦0.6)層所構成,又,藉由氣體摻雜(使用DEZn、Cp2 Mg)將活性層的Zn的濃度固定為5×1016 atoms/cm3 ,Mg的濃度固定為1×1016 atoms/cm3 (濃度的合計值:6×1016 atoms/cm3 )。 將電極形成在如此製造的晶圓並進行晶片切割,再進行打線接合來製造出發光元件。The active layer is composed of a uniformly composed (Al x Ga 1 - x ) y In 1 - y P (0≦x≦1, 0.4≦y≦0.6) layer, and is doped by gas (using DEZn, Cp 2 Mg) The concentration of Zn in the active layer is fixed to 5×10 16 atoms/cm 3 , and the concentration of Mg is fixed to 1×10 16 atoms/cm 3 (total concentration value: 6×10 16 atoms/cm 3 ). The electrodes are formed on the wafer thus manufactured, the wafer is diced, and then wire bonding is performed to manufacture a light-emitting element.

表2針對實施例1、實施例2、比較例1、比較例2的發光元件顯示環境溫度不同(0℃vs60℃)所致的光輸出比及壽命特性。 如表2所示,關於實施例1、2,環境溫度不同所致的光輸出比係0.86以上,且,壽命特性係87,此等兩者係良好的值。 另一方面,比較例1因為活性層幾乎不存在有摻雜物,所以壽命特性良好,但環境溫度不同所致的光輸出比為0.8,環境溫度所致的輝度變化較大。又,比較例2在環境溫度不同所致的光輸出比為良好,但由於活性層的摻雜物並未漸減而定為固定,壽命特性為60%而有所惡化。Table 2 shows the light output ratio and lifetime characteristics of the light-emitting elements of Example 1, Example 2, Comparative Example 1, and Comparative Example 2 due to different ambient temperatures (0° C. vs. 60° C.). As shown in Table 2, regarding Examples 1 and 2, the light output ratio due to the difference in ambient temperature is 0.86 or more, and the lifetime characteristic is 87, both of which are good values. On the other hand, in Comparative Example 1, since there are almost no dopants in the active layer, the lifetime characteristics are good, but the light output ratio due to different environmental temperatures is 0.8, and the brightness change due to the environmental temperature is large. In addition, in Comparative Example 2, the light output ratio due to the difference in ambient temperature was good, but the dopant of the active layer did not gradually decrease but was fixed, and the lifetime characteristic was 60% and deteriorated.

【表2】   相對光輸出比 (0℃vs60℃) 壽命特性 (%) 實施例1 0.86 87 實施例2 0.87 87 比較例1 0.8 89 比較例2 0.87 60 【Table 2】 Relative light output ratio (0℃vs60℃) Life characteristics (%) Example 1 0.86 87 Example 2 0.87 87 Comparative example 1 0.8 89 Comparative example 2 0.87 60

又,本案發明人已確認,在利用氣體摻雜之實施例1、2以外,形成出至少P型護套層為止的各層後,施加熱處理使P型摻雜物自P型護套層擴散至活性層,能製造出具有與實施例1、2同等的傾斜摻雜之濃度曲線,且具有同等的光輸出比及壽命特性之發光元件。In addition, the inventor of the present case has confirmed that, in addition to Examples 1 and 2 using gas doping, after forming at least the P-type sheath layer, heat treatment is applied to diffuse the P-type dopant from the P-type sheath layer to The active layer can produce a light-emitting element having the same gradient doping concentration profile as in Examples 1 and 2, and having the same light output ratio and lifetime characteristics.

另,本發明不限定於上述實施形態。上述實施形態係例示,與本發明之申請專利範圍記載之技術思想具有實質上同一構成、發揮同樣作用效果者均包含於本發明之技術範圍。In addition, this invention is not limited to the said embodiment. The above-mentioned embodiments are exemplified, and the technical ideas described in the scope of the patent application of the present invention have substantially the same constitution and exert the same effects are included in the technical scope of the present invention.

100:GaAs出發基板 102:AlInP蝕刻終止層 103:N型AlGaInP護套層 104:AlGaInP活性層 105:P型AlGaInP護套層 106:P型InGaP緩衝層 107:P型GaP電流傳播層 110:發光元件 200:GaAs出發基板 202:AlInP蝕刻終止層 203:N型AlGaInP護套層 204:AlGaInP活性層 205:P型AlGaInP護套層 206:P型InGaP緩衝層 207:P型GaP電流傳播層 210:發光元件 300:GaAs出發基板 302:AlInP蝕刻終止層 303:N型AlGaInP護套層 304:AlGaInP活性層 305:P型AlGaInP護套層 306:P型InGaP緩衝層 307:P型GaP電流傳播層 310:發光元件100: GaAs starting substrate 102: AlInP etching stop layer 103: N-type AlGaInP sheath layer 104: AlGaInP active layer 105: P-type AlGaInP sheath layer 106: P-type InGaP buffer layer 107: P-type GaP current propagation layer 110: Light-emitting element 200: GaAs starting substrate 202: AlInP etching stop layer 203: N-type AlGaInP sheath layer 204: AlGaInP active layer 205: P-type AlGaInP sheath layer 206: P-type InGaP buffer layer 207: P-type GaP current propagation layer 210: light-emitting element 300: GaAs starting substrate 302: AlInP etching stop layer 303: N-type AlGaInP sheath layer 304: AlGaInP active layer 305: P-type AlGaInP sheath layer 306: P-type InGaP buffer layer 307: P-type GaP current propagation layer 310: Light-emitting element

圖1係顯示本發明之發光元件的一例之概略圖。 圖2係顯示活性層中之平均P型摻雜物濃度之說明圖。 圖3係顯示本發明之發光元件其它例之概略圖。 圖4係顯示習知發光元件的一例之概略圖。Fig. 1 is a schematic diagram showing an example of the light-emitting device of the present invention. Fig. 2 is an explanatory diagram showing the average P-type dopant concentration in the active layer. Fig. 3 is a schematic diagram showing another example of the light-emitting device of the present invention. Fig. 4 is a schematic diagram showing an example of a conventional light-emitting device.

103:N型AlGaInP護套層 103: N-type AlGaInP sheath layer

104:AlGaInP活性層 104: AlGaInP active layer

105:P型AlGaInP護套層 105: P-type AlGaInP sheath layer

Claims (13)

一種發光元件,包含依序形成有N型護套層、活性層及P型護套層的發光部,其特徵在於, 該活性層包含:P型摻雜物,其濃度自該P型護套層側往該N型護套層側漸減; 且在該活性層中,自該P型護套層起算到該活性層的1/3厚度大小之位置為止的區域的平均之該P型摻雜物濃度為1.0×1016 atoms/cm3 以上,且為3.0×1017 atoms/cm3 以下。A light-emitting element includes a light-emitting part having an N-type sheath layer, an active layer, and a P-type sheath layer sequentially formed, wherein the active layer includes: P-type dopants whose concentration is derived from the P-type sheath The layer side gradually decreases toward the N-type sheath layer side; and in the active layer, the average P-type doping in the region from the P-type sheath layer to the position of 1/3 of the thickness of the active layer The substance concentration is 1.0×10 16 atoms/cm 3 or more and 3.0×10 17 atoms/cm 3 or less. 如請求項1之發光元件,其中, 該發光部係由AlGaInP系的化合物半導體所構成。Such as the light-emitting element of claim 1, wherein The light-emitting part is composed of an AlGaInP-based compound semiconductor. 如請求項1之發光元件,其中, 在該活性層中,自該P型護套層起算該活性層的1/3厚度大小之位置到2/3厚度大小之位置為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。The light-emitting element of claim 1, wherein, in the active layer, the average value of the area from the position of 1/3 of the thickness of the active layer to the position of 2/3 of the thickness of the active layer from the P-type sheath layer is the P The concentration of the type dopant is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less. 如請求項2之發光元件,其中, 在該活性層中,自該P型護套層起算該活性層的1/3厚度大小之位置到2/3厚度大小之位置為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。The light-emitting element of claim 2, wherein, in the active layer, the average value of the area from the position of 1/3 of the thickness of the active layer to the position of 2/3 of the thickness of the active layer is the P The concentration of the type dopant is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less. 如請求項3或請求項4之發光元件,其中, 在該活性層中,自該P型護套層起算該活性層的2/3厚度大小之位置到N型護套層為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以下。Such as the light-emitting element of claim 3 or claim 4, wherein, in the active layer, the average of the area from the position of 2/3 of the thickness of the active layer to the N-type sheath layer from the P-type sheath layer The P-type dopant concentration is 0.3×10 16 atoms/cm 3 or less. 一種發光元件之製造方法,該發光元件包含依序形成有N型護套層、活性層及P型護套層的發光部,其特徵為摻雜P型摻雜物而製造該發光元件成如下情況: 在該活性層中,該P型摻雜物濃度自該P型護套層側往該N型護套層側漸減, 且在該活性層中,自該P型護套層起算到該活性層的1/3厚度大小之位置為止的區域之平均該P型摻雜物濃度為1.0×1016 atoms/cm3 以上,且為3.0×1017 atoms/cm3 以下。A method for manufacturing a light-emitting element, the light-emitting element includes a light-emitting portion formed with an N-type sheath layer, an active layer, and a P-type sheath layer in sequence, characterized by doping with P-type dopants to manufacture the light-emitting element as follows Situation: In the active layer, the P-type dopant concentration gradually decreases from the P-type sheath layer side to the N-type sheath layer side, and in the active layer, from the P-type sheath layer to the The average P-type dopant concentration in the region up to the position 1/3 of the thickness of the active layer is 1.0×10 16 atoms/cm 3 or more and 3.0×10 17 atoms/cm 3 or less. 如請求項6之發光元件之製造方法,其中, 該發光部係由AlGaInP系的化合物半導體所構成。Such as the method of manufacturing a light-emitting element of claim 6, wherein: The light-emitting part is composed of an AlGaInP-based compound semiconductor. 如請求項6之發光元件之製造方法,其中, 將該P型摻雜物摻雜於該活性層時,係摻雜成如下情況: 在該活性層中,自該P型護套層起算該活性層的1/3厚度大小之位置到2/3厚度大小之位置為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。The method of manufacturing a light-emitting element of claim 6, wherein when the P-type dopant is doped in the active layer, the doping is as follows: In the active layer, the P-type sheath layer The average P-type dopant concentration in the region from the position of 1/3 thickness of the active layer to the position of 2/3 thickness is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less. 如請求項7之發光元件之製造方法,其中, 將該P型摻雜物摻雜至該活性層時,係摻雜成如下情況: 在該活性層中,自該P型護套層起算該活性層的1/3厚度大小之位置到2/3厚度大小之位置為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以上,且為3.0×1016 atoms/cm3 以下。The method for manufacturing a light-emitting element of claim 7, wherein when the P-type dopant is doped into the active layer, the doping is as follows: In the active layer, the P-type sheath layer The average P-type dopant concentration in the region from the position of 1/3 thickness of the active layer to the position of 2/3 thickness is 0.3×10 16 atoms/cm 3 or more and 3.0×10 16 atoms/cm 3 or less. 如請求項8之發光元件之製造方法,其中, 將該P型摻雜物摻雜至該活性層時,係摻雜成如下情況: 在該活性層中,自該P型護套層起算該活性層的2/3厚度大小之位置到N型護套層為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以下。The method for manufacturing a light-emitting element according to claim 8, wherein, when the P-type dopant is doped into the active layer, the doping is as follows: In the active layer, the P-type sheath layer The average P-type dopant concentration in the region from the position of 2/3 of the thickness of the active layer to the N-type sheath layer is 0.3×10 16 atoms/cm 3 or less. 如請求項9之發光元件之製造方法,其中, 將該P型摻雜物摻雜至該活性層時,係摻雜成如下情況: 在該活性層中,自該P型護套層起算該活性層的2/3厚度大小之位置到N型護套層為止的區域之平均該P型摻雜物濃度為0.3×1016 atoms/cm3 以下。The method for manufacturing a light-emitting element according to claim 9, wherein when the P-type dopant is doped into the active layer, the doping is as follows: In the active layer, the P-type sheath layer The average P-type dopant concentration in the region from the position of 2/3 of the thickness of the active layer to the N-type sheath layer is 0.3×10 16 atoms/cm 3 or less. 如請求項6至請求項11其中任一項之發光元件之製造方法,其中, 該P型摻雜物之摻雜至該活性層係藉由如下方式進行: 一邊形成該活性層並且一邊進行氣體摻雜。Such as the method of manufacturing a light-emitting element of any one of claim 6 to claim 11, wherein: The doping of the P-type dopant to the active layer is performed in the following manner: Gas doping is performed while forming the active layer. 如請求項6至請求項11其中任一項之發光元件之製造方法,其中, 該P型摻雜物之摻雜至該活性層係藉由如下方式進行: 於形成該活性層之後,形成已摻雜該P型摻雜物的該P型護套層,然後再施加熱處理,使已摻雜至該P型護套層的該P型摻雜物擴散至該活性層。Such as the method of manufacturing a light-emitting element of any one of claim 6 to claim 11, wherein: The doping of the P-type dopant to the active layer is performed in the following manner: After the active layer is formed, the P-type sheath layer doped with the P-type dopant is formed, and then heat treatment is applied to diffuse the P-type dopant that has been doped into the P-type sheath layer to The active layer.
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