TW202306195A - Led epitaxy structure and manufacturing method thereof, and led device - Google Patents

Led epitaxy structure and manufacturing method thereof, and led device Download PDF

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TW202306195A
TW202306195A TW111119258A TW111119258A TW202306195A TW 202306195 A TW202306195 A TW 202306195A TW 111119258 A TW111119258 A TW 111119258A TW 111119258 A TW111119258 A TW 111119258A TW 202306195 A TW202306195 A TW 202306195A
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TWI827064B (en
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馮中山
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大陸商重慶康佳光電技術研究院有限公司
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Abstract

An LED epitaxial structure (100), comprising an n-type semiconductor layer (20), a multi-quantum well active layer (30), and a p-type semiconductor layer (40) which are stacked sequentially. The multi-quantum well active layer (30) comprises at least three barrier layers (31) and at least two potential well layers (32), and the barrier layers (31) and the potential well layers (32) are stacked alternately, wherein the barrier layer (31) comprises a first barrier sub-layer (311), a second barrier sub-layer (312), and a third barrier sub-layer (313) which are stacked sequentially, and the second barrier sub-layer (312) comprises an AlyGa1-yAs oxide layer (3121). Also disclosed are an LED device and a method for manufacturing an LED epitaxial structure.

Description

LED外延結構及其製造方法、LED器件LED epitaxial structure and manufacturing method thereof, LED device

本發明涉及半導體發光技術領域,尤其涉及一種LED外延結構及其製造方法、LED器件。The invention relates to the technical field of semiconductor light emitting, in particular to an LED epitaxial structure, a manufacturing method thereof, and an LED device.

LED器件由於其功耗低、體積小、壽命長、驅動電壓低、堅固耐用以及單色性佳等優點,廣泛應用於顯示技術、信號燈、車用內外指示燈、交通燈、手機、電子儀錶、戶內外顯示、資訊處理、通訊等領域。Due to the advantages of low power consumption, small size, long life, low driving voltage, durability and good monochromaticity, LED devices are widely used in display technology, signal lights, automotive interior and exterior lights, traffic lights, mobile phones, electronic instruments, Indoor and outdoor display, information processing, communication and other fields.

紅光LED器件的外延結構包括多量子阱有源層,目前,多數多量子阱有源層的勢壘層為(Al xGa 1-x) 0.5In 0.5P層,x取值範圍為0.5≤x≤1.0,隨著x增加,即(Al xGa 1-x) 0.5In 0.5P中Al的含量升高,勢壘層中的氧、碳等雜質將顯著增加,導致非輻射複合概率增大,降低多量子阱有源層的發光效率;此外,即使x取值為1.0,(Al xGa 1-x) 0.5In 0.5P的禁帶寬度也約為2.26eV,勢壘層和勢阱層的能級差較小,對躍遷勢壘層的電子阻擋有限,導致紅光LED器件存在發光效率衰減嚴重,耐反向偏壓低,抗靜電能力差等問題。 The epitaxial structure of red LED devices includes multi-quantum well active layers. At present, the barrier layer of most multi-quantum well active layers is (Al x Ga 1-x ) 0.5 In 0.5 P layer, and the range of x is 0.5≤ x≤1.0, as x increases, that is, the content of Al in (Al x Ga 1-x ) 0.5 In 0.5 P increases, impurities such as oxygen and carbon in the barrier layer will increase significantly, resulting in an increase in the probability of non-radiative recombination , reducing the luminous efficiency of the multi-quantum well active layer; in addition, even if the value of x is 1.0, the forbidden band width of (Al x Ga 1-x ) 0.5 In 0.5 P is about 2.26eV, and the barrier layer and potential well layer The energy level difference is small, and the electronic barrier to the transition barrier layer is limited, which leads to serious attenuation of luminous efficiency, low reverse bias resistance, and poor antistatic ability in red LED devices.

鑒於上述現有技術的不足,本申請的目的在於提供一種LED外延結構、LED器件及LED外延結構的製造方法,旨在提升勢壘層的等效禁帶寬度,而有效提升勢壘層和勢阱層的能級差,增強勢壘層對電子的限制以及加強多量子阱有源層的量子化效應,從而提高LED器件的內量子效率、出光效率、耐反向偏壓性能以及抗靜電能力等。In view of the deficiencies in the prior art above, the purpose of this application is to provide a method for manufacturing an LED epitaxial structure, an LED device, and an LED epitaxial structure, aiming at increasing the equivalent band gap of the barrier layer, and effectively improving the barrier layer and the potential well. The energy level difference of the layer enhances the confinement of electrons by the barrier layer and strengthens the quantization effect of the multi-quantum well active layer, thereby improving the internal quantum efficiency, light extraction efficiency, reverse bias resistance and antistatic ability of LED devices, etc. .

一種LED外延結構,所述LED外延結構包括:依次層疊設置的n型半導體層、多量子阱有源層及p型半導體層,所述多量子阱有源層包括至少三層勢壘層和至少二層勢阱層,所述勢壘層和所述勢阱層交替層疊設置,其中,所述勢壘層包括依次層疊設置的勢壘第一子層、勢壘第二子層及勢壘第三子層,所述勢壘第二子層包括Al yGa 1-yAs的氧化物層。 An LED epitaxial structure, the LED epitaxial structure includes: an n-type semiconductor layer, a multi-quantum well active layer and a p-type semiconductor layer stacked in sequence, the multi-quantum well active layer includes at least three barrier layers and at least Two layers of potential well layers, the potential barrier layers and the potential well layers are alternately stacked, wherein the potential barrier layer includes the first sublayer of the potential barrier, the second sublayer of the potential barrier and the second sublayer of the potential barrier that are sequentially stacked. Three sublayers, the second sublayer of the potential barrier includes an oxide layer of AlyGa1 -yAs .

上述LED外延結構,設置的多量子阱有源層的勢壘層包括Al yGa 1-yAs的氧化物層,所述Al yGa 1-yAs的氧化物為寬禁帶材料,使得所述勢壘層與所述勢阱層之間的能級差更大,可有效增強勢壘層對電子的限制以及增強多量子阱有源層的量子化效應,從而有效提升LED器件的出光效率、內量子效率、耐反向偏壓性能以及抗靜電能力等。 In the above-mentioned LED epitaxial structure, the barrier layer of the multi-quantum well active layer includes an oxide layer of AlyGa1 -yAs , and the oxide of AlyGa1 -yAs is a wide bandgap material, so that the The energy level difference between the barrier layer and the potential well layer is larger, which can effectively enhance the confinement of electrons by the barrier layer and enhance the quantization effect of the multi-quantum well active layer, thereby effectively improving the light extraction efficiency of the LED device , internal quantum efficiency, reverse bias resistance and antistatic ability.

可選地,所述Al yGa 1-yAs的氧化物中y的取值範圍為0.8≤y≤1.0。 Optionally, the range of y in the AlyGa 1-y As oxide is 0.8≤y≤1.0.

可選地,所述Al yGa 1-yAs的氧化物層的厚度範圍為0.5nm-3nm。 Optionally, the thickness of the AlyGa1 -yAs oxide layer ranges from 0.5nm to 3nm.

可選地,所述勢壘第一子層和勢壘第三子層均包括(Al xGa 1-x) 0.5In 0.5P層。 Optionally, both the first barrier sublayer and the third barrier sublayer include (Al x Ga 1-x ) 0.5 In 0.5 P layers.

可選地,所述(Al xGa 1-x) 0.5In 0.5P中x的取值範圍為0.5≤x≤0.8。 Optionally, the value range of x in (Al x Ga 1-x ) 0.5 In 0.5 P is 0.5≤x≤0.8.

可選地,所述(Al xGa 1-x) 0.5In 0.5P層的厚度範圍為1nm-6nm。 Optionally, the (Al x Ga 1-x ) 0.5 In 0.5 P layer has a thickness ranging from 1 nm to 6 nm.

可選地,所述勢阱層包括(Al mGa 1-m) 0.5In 0.5P層。 Optionally, the potential well layer includes a (Al m Ga 1-m ) 0.5 In 0.5 P layer.

可選地,所述(Al mGa 1-m) 0.5In 0.5P層的厚度範圍為3nm-10nm。 Optionally, the (Al m Ga 1-m ) 0.5 In 0.5 P layer has a thickness ranging from 3 nm to 10 nm.

可選地,所述多量子阱有源層包括3至21層所述勢壘層和2至20層所述勢阱層,其中,所述勢壘層的層數比所述勢阱層的層數多一層。Optionally, the multi-quantum well active layer includes 3 to 21 layers of the potential barrier layer and 2 to 20 layers of the potential well layer, wherein the number of layers of the potential barrier layer is greater than that of the potential well layer One more layer.

基於同樣的發明構思,本申請還提供一種LED器件,所述LED器件包括n電極、p電極以及前述的LED外延結構,所述n電極與所述n型半導體層電連接,所述p電極與所述p型半導體層電連接。Based on the same inventive concept, the present application also provides an LED device, which includes an n-electrode, a p-electrode and the aforementioned LED epitaxial structure, the n-electrode is electrically connected to the n-type semiconductor layer, and the p-electrode is connected to the n-type semiconductor layer. The p-type semiconductor layers are electrically connected.

基於同樣的發明構思,本申請還提供一種LED外延結構的製造方法,所述LED外延結構的製造方法包括以下步驟:提供襯底;在所述襯底上形成n型半導體層;在所述n型半導體層背離所述襯底的一側形成多量子阱有源層;在所述多量子阱有源層背離所述n型半導體層的一側形成p型半導體層;其中,形成所述多量子阱有源層包括在所述n型半導體層背離所述襯底的一側形成勢壘層,在所述勢壘層背離所述n型半導體層的一側形成勢阱層,以及重複交替形成所述勢壘層和所述勢阱層而形成至少三層勢壘層和至少二層勢阱層,所述勢壘層包括依次層疊形成的勢壘第一子層、勢壘第二子層及勢壘第三子層,所述勢壘第二子層包括Al yGa 1-yAs的氧化物層。 Based on the same inventive concept, the present application also provides a method for manufacturing an LED epitaxial structure. The method for manufacturing an LED epitaxial structure includes the following steps: providing a substrate; forming an n-type semiconductor layer on the substrate; A multi-quantum well active layer is formed on the side of the multi-quantum well active layer away from the substrate; a p-type semiconductor layer is formed on the side of the multi-quantum well active layer away from the n-type semiconductor layer; wherein, the multi-quantum well active layer is formed on the side away from the n-type semiconductor layer; The quantum well active layer includes forming a potential barrier layer on the side of the n-type semiconductor layer away from the substrate, forming a potential well layer on the side of the barrier layer away from the n-type semiconductor layer, and repeating alternately Forming the barrier layer and the potential well layer to form at least three barrier layers and at least two potential well layers, the barrier layer includes the first sub-layer of the potential barrier and the second sub-layer of the potential barrier formed sequentially. layer and a third sublayer of the barrier, the second sublayer of the barrier includes an oxide layer of AlyGa1 -yAs .

上述LED外延結構的製造方法,形成的所述多量子阱有源層的勢壘層包括Al yGa 1-yAs的氧化物層,所述Al yGa 1-yAs的氧化物為寬禁帶材料,使得所述勢壘層與所述勢阱層之間的能級差更大,可有效增強勢壘層對電子的限制以及增強多量子阱有源層的量子化效應,從而有效提升LED器件的內量子效率、出光效率、耐反向偏壓性能以及抗靜電能力等。 In the manufacturing method of the above-mentioned LED epitaxial structure, the barrier layer of the multi-quantum well active layer formed includes an oxide layer of AlyGa1 - yAs, and the oxide layer of AlyGa1 -yAs is a wide range of band material, so that the energy level difference between the barrier layer and the potential well layer is larger, which can effectively enhance the confinement of electrons by the barrier layer and enhance the quantization effect of the multi-quantum well active layer, thereby effectively improving The internal quantum efficiency, light extraction efficiency, reverse bias resistance performance and antistatic ability of LED devices.

可選地,所述勢壘第一子層和勢壘第三子層均包括(Al xGa 1-x) 0.5In 0.5P層,所述在所述n型半導體層背離所述襯底的一側形成勢壘層,包括:通入磷烷和第一比例的三甲基鎵、三甲基鋁、三甲基銦,以在所述n型半導體層背離所述襯底的一側形成(Al xGa 1-x) 0.5In 0.5P層;通入砷烷、三甲基鎵和三甲基鋁,以在所述(Al xGa 1-x) 0.5In 0.5P層背離所述n型半導體層的一側形成Al yGa 1-yAs層;通入磷烷和第一比例的三甲基鎵、三甲基鋁、三甲基銦,以在所述Al yGa 1-yAs層上形成(Al xGa 1-x) 0.5In 0.5P層;對所述Al yGa 1-yAs層進行氧化處理,以氧化所述Al yGa 1-yAs層而形成Al yGa 1-yAs的氧化物層。 Optionally, both the first barrier sublayer and the third barrier sublayer include a (Al x Ga 1-x ) 0.5 In 0.5 P layer, and the A barrier layer is formed on one side, including: passing through phosphine and a first proportion of trimethylgallium, trimethylaluminum, and trimethylindium, so as to be formed on the side of the n-type semiconductor layer away from the substrate (Al x Ga 1-x ) 0.5 In 0.5 P layer; arsine , trimethylgallium and trimethylaluminum are introduced to deviate from the n A layer of A y Ga 1-y As is formed on one side of the type semiconductor layer; phosphine and a first ratio of trimethylgallium, trimethylaluminum, and trimethylindium are introduced to form an AlyGa 1-y As layer on the AlyGa 1-y forming (Al x Ga 1-x ) 0.5 In 0.5 P layer on the As layer; performing oxidation treatment on the Aly Ga 1-y As layer to oxidize the Aly Ga 1-y As layer to form A y Ga Oxide layer of 1-y As.

可選地,所述在所述勢壘層背離所述n型半導體層的一側形成勢阱層,包括:通入磷烷和第二比例的三甲基鎵、三甲基鋁、三甲基銦,以在所述勢壘層背離所述n型半導體層的一側形成(Al mGa 1-m) 0.5In 0.5P層。 Optionally, the formation of a potential well layer on the side of the barrier layer away from the n-type semiconductor layer includes: introducing phosphine and a second proportion of trimethylgallium, trimethylaluminum, trimethyl Indium-based, to form a (Al m Ga 1-m ) 0.5 In 0.5 P layer on the side of the barrier layer away from the n-type semiconductor layer.

為了便於理解本申請,下面將參照相關附圖對本申請進行更全面的描述。附圖中給出了本申請的較佳實施方式。但是,本申請可以以許多不同的形式來實現,並不限於本文所描述的實施方式。相反地,提供這些實施方式的目的是使對本申請的公開內容理解的更加透徹全面。In order to facilitate the understanding of the present application, the present application will be described more fully below with reference to the relevant drawings. Preferred embodiments of the application are shown in the accompanying drawings. However, the present application can be embodied in many different forms and is not limited to the embodiments described herein. On the contrary, the purpose of providing these embodiments is to make the disclosure of the application more thorough and comprehensive.

除非另有定義,本文所使用的所有的技術和科學術語與屬於本申請的技術領域的技術人員通常理解的含義相同。本文中在本申請的說明書中所使用的術語只是為了描述具體的實施方式的目的,不是旨在於限制本申請。Unless otherwise defined, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the technical field to which this application belongs. The terminology used herein in the description of the application is only for the purpose of describing specific embodiments, and is not intended to limit the application.

本申請的描述中,術語“第一”、“第二”、“第三”等是用於區別不同物件,而不是用於描述特定順序,另外,術語“上”、“內”、“外”等指示的方位或者位置關係為基於附圖所示的方位或位置關係,僅是為了便於描述本申請和簡化描述,而不是指示或者暗示所指的裝置或者元件必須具有特定的方位、以特定的方位構造和操作,因此不能理解為對本申請的限制。In the description of the present application, the terms "first", "second", "third", etc. are used to distinguish different items, rather than to describe a specific order. In addition, the terms "upper", "inner", "outer ” and other indicated orientations or positional relationships are based on the orientations or positional relationships shown in the drawings, which are only for the convenience of describing the application and simplifying the description, rather than indicating or implying that the referred device or element must have a specific orientation, use a specific configuration and operation, and therefore should not be construed as limiting the application.

需要說明的是,本申請實施例中所提供的圖示僅以示意方式說明本申請的基本構想,雖圖示中僅顯示與本申請中有關的組件而非按照實際實施時的元件數目、形狀及尺寸繪製,其實際實施時各元件的型態、數量及比例可為一種隨意的改變,且其元件佈局形態也可能更複雜。It should be noted that the diagrams provided in the embodiments of the application are only schematically illustrating the basic idea of the application, although the diagrams only show components related to the application rather than the number and shape of elements in actual implementation and dimensional drawing, the shape, quantity and proportion of each component can be changed arbitrarily during actual implementation, and the layout of the components may also be more complicated.

請參閱圖1,圖1為本申請實施例提供的LED外延結構100的截面結構示意圖。如圖1所示,LED外延結構100包括依次層疊設置的n型半導體層20、多量子阱有源層30和p型半導體層40,所述多量子阱有源層30包括至少三層勢壘層31和至少二層勢阱層32,所述勢壘層31和所述勢阱層32交替層疊設置,其中,所述勢壘層31包括依次層疊設置的勢壘第一子層311、勢壘第二子層312以及勢壘第三子層313,所述勢壘第二子層312包括Al yGa 1-yAs的氧化物層3121。在本實施方式中,勢壘第一子層311相較於勢壘第三子層313靠近n型半導體層20設置。 Please refer to FIG. 1 . FIG. 1 is a schematic cross-sectional structure diagram of an LED epitaxial structure 100 provided by an embodiment of the present application. As shown in FIG. 1 , the LED epitaxial structure 100 includes an n-type semiconductor layer 20, a multi-quantum well active layer 30 and a p-type semiconductor layer 40 stacked in sequence, and the multi-quantum well active layer 30 includes at least three layers of barriers. Layer 31 and at least two layers of potential well layers 32, the barrier layers 31 and the potential well layers 32 are alternately stacked, wherein the barrier layer 31 includes the first sub-layer 311 of the potential barrier, the potential The barrier second sublayer 312 and the barrier third sublayer 313, the barrier second sublayer 312 includes an oxide layer 3121 of AlyGa1 -yAs . In this embodiment, the first barrier sublayer 311 is arranged closer to the n-type semiconductor layer 20 than the third barrier sublayer 313 .

本申請實施例提供的LED外延結構100,設置的多量子阱有源層30的勢壘層31包括Al yGa 1-yAs的氧化物層3121,Al yGa 1-yAs的氧化物為寬禁帶材料,使得勢壘層31與勢阱層32之間的能級差較大,可有效增強勢壘層31對電子的限制以及增強多量子阱有源層的量子化效應,從而有效提升LED器件的發光效率、耐反向偏壓性能以及抗靜電能力。 In the LED epitaxial structure 100 provided in the embodiment of the present application, the barrier layer 31 of the multi-quantum well active layer 30 includes an oxide layer 3121 of AlyGa1 -yAs , and the oxide layer of AlyGa1 -yAs is The wide bandgap material makes the energy level difference between the barrier layer 31 and the potential well layer 32 larger, which can effectively enhance the confinement of the barrier layer 31 to electrons and enhance the quantization effect of the multi-quantum well active layer, thereby effectively Improve the luminous efficiency, reverse bias resistance performance and antistatic ability of LED devices.

其中,Al yGa 1-yAs的氧化物中y的取值範圍為0.8≤y≤1.0。 Wherein, the value range of y in the oxide of Al y Ga 1-y As is 0.8≤y≤1.0.

其中,Al yGa 1-yAs的氧化物層3121的厚度範圍為0.5nm-3nm,Al yGa 1-yAs的氧化物層3121的厚度為Al yGa 1-yAs的氧化物層3121在平行於層疊方向上的尺寸。當Al yGa 1-yAs的氧化物層3121的厚度超過3nm時,勢壘層31會嚴重阻擋載流子的躍遷,而影響載流子之間的輻射複合;當Al yGa 1-yAs的氧化物層3121的厚度低於0.5nm時,勢壘層31對電子的限制作用有限。在一些實施例中,Al yGa 1-yAs的氧化物為非主動摻雜的Al yGa 1-yAs的氧化物,非主動摻雜的Al yGa 1-yAs的氧化物對載流子的吸收較弱,可提高發光效率。 Wherein, the thickness range of the oxide layer 3121 of AlyGa1 -yAs is 0.5nm-3nm, and the thickness of the oxide layer 3121 of AlyGa1 - yAs is the oxide layer 3121 of AlyGa1 -yAs Dimensions parallel to the lamination direction. When the thickness of the oxide layer 3121 of AlyGa 1-y As exceeds 3nm, the barrier layer 31 will seriously block the transition of carriers and affect the radiative recombination between carriers; when AlyGa 1-y When the thickness of the As oxide layer 3121 is less than 0.5 nm, the restriction effect of the barrier layer 31 on electrons is limited. In some embodiments, the oxide of AlyGa 1-y As is an oxide of non-actively doped AlyGa 1-y As, and the oxide of non-actively doped AlyGa 1-yAs supports The absorption of the carrier is weak, which can improve the luminous efficiency.

其中,勢壘第一子層311和勢壘第三子層313均包括(Al xGa 1-x) 0.5In 0.5P層3111,x的取值範圍為0.5≤x≤0.8,(Al xGa 1-x) 0.5In 0.5P層3111的厚度範圍為1nm-6nm,(Al xGa 1-x) 0.5In 0.5P層3111的厚度為(Al xGa 1-x) 0.5In 0.5P層3111在平行於層疊方向上的尺寸。當(Al xGa 1-x) 0.5In 0.5P層3111的厚度超過6nm時,勢壘層31會嚴重阻擋載流子的躍遷,而影響載流子之間的輻射複合;當(Al xGa 1-x) 0.5In 0.5P層3111的厚度低於1nm時,勢壘層31對電子的限制作用有限。在一些實施例中,(Al xGa 1-x) 0.5In 0.5P為非主動摻雜的(Al xGa 1-x) 0.5In 0.5P,非主動摻雜的(Al xGa 1-x) 0.5In 0.5P對載流子的吸收較弱,可提高發光效率。 Wherein, both the first barrier sublayer 311 and the third barrier sublayer 313 include (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111, and the range of x is 0.5≤x≤0.8, (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 has a thickness ranging from 1 nm to 6 nm, and the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 has a thickness of (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 in Dimensions parallel to the lamination direction. When the thickness of the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 exceeds 6 nm, the barrier layer 31 will seriously block the transition of carriers and affect the radiative recombination between carriers; when (Al x Ga 1-x ) When the thickness of the 0.5 In 0.5 P layer 3111 is less than 1 nm, the barrier layer 31 has a limited effect on electron confinement. In some embodiments, (Al x Ga 1-x ) 0.5 In 0.5 P is non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P, non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P has weak carrier absorption, which can improve the luminous efficiency.

其中,勢阱層32包括(Al mGa 1-m) 0.5In 0.5P層321,(Al mGa 1-m) 0.5In 0.5P層321的厚度範圍為3nm-10nm,(Al mGa 1-m) 0.5In 0.5P層321的厚度為(Al mGa 1-m) 0.5In 0.5P層321在平行於層疊方向上的尺寸。當(Al mGa 1-m) 0.5In 0.5P層321的厚度超過10nm時,多量子阱有源層30的波函數重疊較小,阻擋載流子的遷移,而降低內量子阱效率;當(Al mGa 1-m) 0.5In 0.5P層321的厚度低於3nm時,載流子容易溢出勢阱層32,而降低輻射複合效率。其中,m的取值可根據LED器件發出的光的波長設定,波長越長,m取值越小。在一些實施例中,(Al mGa 1-m) 0.5In 0.5P為非主動摻雜的(Al mGa 1-m) 0.5In 0.5P,非主動摻雜的(Al mGa 1-m) 0.5In 0.5P對載流子、光子的吸收較弱,可提高發光效率。 Wherein, the potential well layer 32 includes (Al m Ga 1-m ) 0.5 In 0.5 P layer 321, the thickness range of (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 is 3 nm-10 nm, (Al m Ga 1- The thickness of the m ) 0.5 In 0.5 P layer 321 is the dimension of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 parallel to the stacking direction. When the thickness of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 exceeds 10 nm, the wave function overlap of the multi-quantum well active layer 30 is small, which blocks the migration of carriers and reduces the efficiency of the internal quantum well; when When the thickness of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 is less than 3 nm, the carriers are likely to overflow the potential well layer 32 , thereby reducing the radiation recombination efficiency. Wherein, the value of m can be set according to the wavelength of light emitted by the LED device, and the longer the wavelength, the smaller the value of m. In some embodiments, (Al m Ga 1-m ) 0.5 In 0.5 P is non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P, non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P has weak absorption of carriers and photons, which can improve the luminous efficiency.

其中,多量子阱有源層30包括3至21層勢壘層31和2至20層勢阱層32,其中,勢壘層31的層數比勢阱層32的層數多一層。每層勢壘層31與鄰近的一層勢阱層32形成一個多量子阱週期,前述的多量子阱有源層30包括2至20個多量子阱週期。多量子阱週期數目一般不超過20,當多量子阱週期數目過多,多量子阱有源層30整體過厚,會增加載流子在多量子阱有源層30中的的非輻射複合,而影響發光效率;當多量子阱週期數目過少,多量子阱有源層30的勢壘層31及LED器件的電子阻擋層無法將多數電子限制在多量子阱有源層30中,使得電子溢出導致發光效率降低。Wherein, the multi-quantum well active layer 30 includes 3 to 21 barrier layers 31 and 2 to 20 potential well layers 32 , wherein the number of barrier layers 31 is one more than the number of potential well layers 32 . Each barrier layer 31 and an adjacent potential well layer 32 form a multi-quantum well period, and the aforementioned multi-quantum well active layer 30 includes 2 to 20 multi-quantum well periods. The number of multi-quantum well periods is generally no more than 20. When the number of multi-quantum well periods is too large, the overall thickness of the multi-quantum well active layer 30 will increase the non-radiative recombination of carriers in the multi-quantum well active layer 30, and Affect luminous efficiency; when the number of multi-quantum well periods is too small, the barrier layer 31 of the multi-quantum well active layer 30 and the electron blocking layer of the LED device cannot confine most electrons in the multi-quantum well active layer 30, causing electron overflow to cause Luminous efficiency decreases.

其中,Al yGa 1-yAs的氧化物包括氧化鋁和氧化鎵,氧化鋁的禁帶帶隙較寬,能夠有效提升勢壘層31與勢阱層32的能級差,而增強勢壘層31對電子的限制效果。 Among them, the oxides of Al y Ga 1-y As include aluminum oxide and gallium oxide, and aluminum oxide has a wide bandgap, which can effectively increase the energy level difference between the barrier layer 31 and the potential well layer 32, and enhance the potential barrier Confinement effect of layer 31 on electrons.

請參閱圖2,圖2為本申請另一實施例提供的LED外延結構100的截面結構示意圖。如圖2所示,在一些實施例中,LED外延結構100的n型半導體層20包括依次層疊設置的緩衝層21、n型歐姆接觸層22、n型電流擴展層23、n型限制層24及n型波導層25,其中,緩衝層21相較於n型波導層25遠離多量子阱有源層30設置。Please refer to FIG. 2 . FIG. 2 is a schematic cross-sectional structure diagram of an LED epitaxial structure 100 provided in another embodiment of the present application. As shown in FIG. 2 , in some embodiments, the n-type semiconductor layer 20 of the LED epitaxial structure 100 includes a buffer layer 21 , an n-type ohmic contact layer 22 , an n-type current spreading layer 23 , and an n-type confinement layer 24 which are sequentially stacked. And the n-type waveguide layer 25 , wherein the buffer layer 21 is arranged farther away from the multi-quantum well active layer 30 than the n-type waveguide layer 25 .

其中,緩衝層21可為GaAs層,用於隔離和阻擋雜質進入n型歐姆接觸層22。Wherein, the buffer layer 21 may be a GaAs layer, which is used to isolate and block impurities from entering the n-type ohmic contact layer 22 .

其中,n型歐姆接觸層22可為(Al aGa 1-a) 0.5In 0.5P層,a的取值範圍為0.3≤a≤0.6,用於與n電極形成歐姆接觸。 Wherein, the n-type ohmic contact layer 22 can be an (Al a Ga 1-a ) 0.5 In 0.5 P layer, and the range of a is 0.3≤a≤0.6, which is used to form an ohmic contact with the n-electrode.

其中,n型電流擴展層23可為(Al bGa 1-b) 0.5In 0.5P層,b的取值範圍為0.5≤b≤1.0,在電流流經n型電流擴展層23擴展至多量子阱有源層30時,n型電流擴展層23能夠使得到達多量子阱有源層30的電流密度是均勻的,均勻的電流分佈可提高發光效率。 Wherein, the n-type current spreading layer 23 can be an (Al b Ga 1-b ) 0.5 In 0.5 P layer, and the value range of b is 0.5≤b≤1.0. In the active layer 30, the n-type current spreading layer 23 can make the current density reaching the multi-quantum well active layer 30 uniform, and the uniform current distribution can improve the luminous efficiency.

其中,n型限制層24可為AlInP層,n型限制層24的禁帶寬度大於多量子阱有源層30,可將空穴限制在多量子阱有源層30中,提高電子擴展的均勻性,使得電子與空穴在多量子阱有源層30中輻射複合。Wherein, the n-type confinement layer 24 can be an AlInP layer, and the band gap of the n-type confinement layer 24 is greater than the multi-quantum well active layer 30, holes can be confined in the multi-quantum well active layer 30, and the uniformity of electron expansion can be improved. properties, so that electrons and holes radiatively recombine in the MQW active layer 30 .

其中,n型波導層25可為(Al cGa 1-c) 0.5In 0.5P層,c的取值範圍為0.5≤c≤1.0。n型波導層25的折射率低於多量子阱有源層30,使得多量子阱有源層30發出的光束在n型波導層25與多量子阱有源層30的交界處發生全反射,而使得光束能集中出射,而提升光提取效率。 Wherein, the n-type waveguide layer 25 may be an (Al c Ga 1-c ) 0.5 In 0.5 P layer, and the range of c is 0.5≤c≤1.0. The refractive index of the n-type waveguide layer 25 is lower than that of the multi-quantum well active layer 30, so that the light beam emitted by the multi-quantum well active layer 30 is totally reflected at the junction of the n-type waveguide layer 25 and the multi-quantum well active layer 30, Therefore, the light beam can be emitted in a concentrated manner, thereby improving the light extraction efficiency.

在一些實施例中,p型半導體層40包括依次層疊設置於多量子阱有源層30背離n型半導體層20的一側的p型波導層41、p型限制層42、過渡層43、p型電流擴展層44以及p型歐姆接觸層45。In some embodiments, the p-type semiconductor layer 40 includes a p-type waveguide layer 41, a p-type confinement layer 42, a transition layer 43, a p type current spreading layer 44 and p-type ohmic contact layer 45.

其中,p型波導層41可為(Al dGa 1-d) 0.5In 0.5P層,d的取值範圍為0.5≤d≤1.0,p型波導層41的折射率低於多量子阱有源層30,使得多量子阱有源層30發出的光束在p型波導層41與多量子阱有源層30的交界處發生全反射,而使得光束能集中出射,而提升光提取效率。 Wherein, the p-type waveguide layer 41 can be (Al d Ga 1-d ) 0.5 In 0.5 P layer, the value range of d is 0.5≤d≤1.0, and the refractive index of the p-type waveguide layer 41 is lower than that of the multiple quantum well active layer 30, so that the light beam emitted by the multi-quantum well active layer 30 is totally reflected at the junction of the p-type waveguide layer 41 and the multi-quantum well active layer 30, so that the light beam can be emitted concentratedly, thereby improving the light extraction efficiency.

其中,p型限制層42可為AlInP層,p型限制層42的禁帶寬度大於多量子阱有源層30,可將電子限制在多量子阱有源層30中,使得電子與空穴在多量子阱有源層30中輻射複合。Wherein, the p-type confinement layer 42 can be an AlInP layer, and the band gap of the p-type confinement layer 42 is greater than the multi-quantum well active layer 30, and electrons can be confined in the multi-quantum well active layer 30, so that electrons and holes are Radiative recombination in the multiple quantum well active layer 30 .

其中,p型電流擴展層44可為GaP層,用於與p電極形成歐姆接觸。Wherein, the p-type current spreading layer 44 may be a GaP layer for forming an ohmic contact with the p-electrode.

其中,過渡層43可為(Al eGa 1-e) 0.5In 0.5P層,設置於p型限制層42與p型電流擴展層44之間,起晶格過渡作用,能夠減小p型限制層42與p型電流擴展層44之間的晶格失配,而減小p型電流擴展層44的缺陷密度。 Wherein, the transition layer 43 can be an (Al e Ga 1-e ) 0.5 In 0.5 P layer, which is arranged between the p-type confinement layer 42 and the p-type current spreading layer 44, and acts as a lattice transition to reduce the p-type confinement layer. The lattice mismatch between the layer 42 and the p-type current spreading layer 44 reduces the defect density of the p-type current spreading layer 44 .

其中,p型歐姆接觸層45可為GaP層,用於與p電極形成歐姆接觸。Wherein, the p-type ohmic contact layer 45 may be a GaP layer for forming an ohmic contact with the p-electrode.

綜上,本申請實施例提供的LED外延結構,設置的多量子阱有源層30的勢壘層31包括Al yGa 1-yAs的氧化物層3121,Al yGa 1-yAs的氧化物為寬禁帶材料,使得勢壘層31與勢阱層32之間的能級差更大,可有效增強勢壘層31對電子的限制以及增強多量子阱有源層30的量子化效應,從而有效提升LED器件的內量子效率、出光效率、耐反向偏壓性能以及抗靜電能力等。 To sum up, in the LED epitaxial structure provided by the embodiment of the present application, the barrier layer 31 of the multi-quantum well active layer 30 includes the oxide layer 3121 of AlyGa 1-y As, and the oxide layer 3121 of AlyGa 1-y As The substance is a wide bandgap material, so that the energy level difference between the potential barrier layer 31 and the potential well layer 32 is larger, which can effectively enhance the confinement of the barrier layer 31 to electrons and enhance the quantization effect of the multi-quantum well active layer 30 , so as to effectively improve the internal quantum efficiency, light extraction efficiency, reverse bias resistance performance and antistatic ability of LED devices.

本申請實施例還提供一種LED器件,該LED器件包括前述的任一實施例提供的LED外延結構,其中LED器件還包括n電極和p電極,n電極與n型半導體層20電連接,p電極與p型半導體層40電連接。The embodiment of the present application also provides an LED device, the LED device includes the LED epitaxial structure provided by any of the foregoing embodiments, wherein the LED device further includes an n-electrode and a p-electrode, the n-electrode is electrically connected to the n-type semiconductor layer 20, and the p-electrode It is electrically connected to the p-type semiconductor layer 40 .

其中,在一些實施例中,n型半導體層20包括n型歐姆接觸層22,n電極與n型歐姆接觸層22電連接;p型半導體層40包括p型歐姆接觸層45,p電極與p型歐姆接觸層45電連接。Wherein, in some embodiments, the n-type semiconductor layer 20 includes an n-type ohmic contact layer 22, and the n-electrode is electrically connected to the n-type ohmic contact layer 22; the p-type semiconductor layer 40 includes a p-type ohmic contact layer 45, and the p-electrode is electrically connected to the p-type semiconductor layer 45. Type ohmic contact layer 45 is electrically connected.

請一併參閱1至圖3,圖3為本申請實施例提供的LED外延結構的製造方法的流程圖,LED外延結構的製造方法用於製造前述的任一實施例提供的LED外延結構。如圖3所示,LED外延結構的製造方法包括以下步驟:Please refer to FIG. 1 to FIG. 3 together. FIG. 3 is a flowchart of a method for manufacturing an LED epitaxial structure provided in an embodiment of the present application. The method for manufacturing an LED epitaxial structure is used to manufacture an LED epitaxial structure provided in any of the foregoing embodiments. As shown in Figure 3, the manufacturing method of the LED epitaxial structure includes the following steps:

S101:提供襯底。S101: Provide a substrate.

S102:在襯底上形成n型半導體層20。S102: forming an n-type semiconductor layer 20 on the substrate.

S103:在n型半導體層20背離襯底的一側形成多量子阱有源層30,其中,形成多量子阱有源層30包括在n型半導體層20背離襯底的一側形成勢壘層31,在勢壘層31背離n型半導體層20的一側形成勢阱層32,以及重複交替形成勢壘層31和勢阱層32而形成至少三層勢壘層31和至少二層勢阱層32,勢壘層31包括依次層疊形成的勢壘第一子層311、勢壘第二子層312及勢壘第三子層313,勢壘第二子層312包括Al yGa 1-yAs的氧化物層3121。 S103: Forming the multi-quantum well active layer 30 on the side of the n-type semiconductor layer 20 away from the substrate, wherein forming the multi-quantum well active layer 30 includes forming a barrier layer on the side of the n-type semiconductor layer 20 away from the substrate 31, forming a potential well layer 32 on the side of the barrier layer 31 away from the n-type semiconductor layer 20, and repeatedly forming the potential barrier layer 31 and the potential well layer 32 alternately to form at least three barrier layers 31 and at least two layers of potential wells Layer 32, the barrier layer 31 includes the first barrier sublayer 311, the second barrier sublayer 312 and the third barrier sublayer 313 formed sequentially, the second barrier sublayer 312 includes Al y Ga 1-y As oxide layer 3121 .

S104:在多量子阱有源層30背離n型半導體層20的一側形成p型半導體層40。S104: forming a p-type semiconductor layer 40 on a side of the multi-quantum well active layer 30 away from the n-type semiconductor layer 20 .

本申請實施例提供的LED外延結構的製造方法,形成的多量子阱有源層30的勢壘層31包括Al yGa 1-yAs的氧化物層3121,Al yGa 1-yAs的氧化物為寬禁帶材料,使得勢壘層31與勢阱層32之間的能級差更大,可有效增強勢壘層31對電子的限制以及增強多量子阱有源層30的量子化效應,從而有效提升LED器件的內量子效率、出光效率、耐反向偏壓性能以及抗靜電能力等。 In the manufacturing method of the LED epitaxial structure provided in the embodiment of the present application, the barrier layer 31 of the multi-quantum well active layer 30 formed includes the oxide layer 3121 of AlyGa 1-y As, and the oxide layer 3121 of AlyGa 1-y As The substance is a wide bandgap material, so that the energy level difference between the potential barrier layer 31 and the potential well layer 32 is larger, which can effectively enhance the confinement of the barrier layer 31 to electrons and enhance the quantization effect of the multi-quantum well active layer 30 , so as to effectively improve the internal quantum efficiency, light extraction efficiency, reverse bias resistance performance and antistatic ability of LED devices.

其中,襯底的材料可為GaAs,為其它膜層提供支撐。Wherein, the material of the substrate may be GaAs, which provides support for other film layers.

其中,Al yGa 1-yAs的氧化物中y的取值範圍為0.8≤y≤1.0。 Wherein, the value range of y in the oxide of Al y Ga 1-y As is 0.8≤y≤1.0.

其中,Al yGa 1-yAs的氧化物層3121的厚度範圍為0.5nm-3nm,Al yGa 1-yAs的氧化物層3121的厚度為Al yGa 1-yAs的氧化物層3121在平行於層疊方向上的尺寸。當Al yGa 1-yAs的氧化物層3121的厚度超過3nm時,勢壘層31會嚴重阻擋載流子的躍遷,而影響載流子之間的輻射複合。在一些實施例中,Al yGa 1-yAs的氧化物為非主動摻雜的Al yGa 1-yAs的氧化物,非主動摻雜的Al yGa 1-yAs的氧化物對載流子的吸收較弱,可提高發光效率。 Wherein, the thickness range of the oxide layer 3121 of AlyGa1 -yAs is 0.5nm-3nm, and the thickness of the oxide layer 3121 of AlyGa1 - yAs is the oxide layer 3121 of AlyGa1 -yAs Dimensions parallel to the lamination direction. When the thickness of the oxide layer 3121 of AlyGa1 -yAs exceeds 3nm, the barrier layer 31 will seriously block the transition of carriers and affect the radiative recombination between carriers. In some embodiments, the oxide of AlyGa 1-y As is an oxide of non-actively doped AlyGa 1-y As, and the oxide of non-actively doped AlyGa 1-yAs supports The absorption of the carrier is weak, which can improve the luminous efficiency.

其中,勢壘第一子層311和勢壘第三子層313均包括(Al xGa 1-x) 0.5In 0.5P層3111,x的取值範圍為0.5≤x≤0.8,(Al xGa 1-x) 0.5In 0.5P層3111的厚度範圍為1nm-6nm,(Al xGa 1-x) 0.5In 0.5P層3111的厚度為(Al xGa 1-x) 0.5In 0.5P層3111在平行於層疊方向上的尺寸。當(Al xGa 1-x) 0.5In 0.5P層3111的厚度超過6nm時,勢壘層31會嚴重阻擋載流子的躍遷,而影響載流子之間的輻射複合;當(Al xGa 1-x) 0.5In 0.5P層3111的厚度低於1nm時,勢壘層31對電子的限制作用有限。在一些實施例中,(Al xGa 1-x) 0.5In 0.5P為非主動摻雜的(Al xGa 1-x) 0.5In 0.5P,非主動摻雜的(Al xGa 1-x) 0.5In 0.5P對載流子的吸收較弱,可提高發光效率。 Wherein, both the first barrier sublayer 311 and the third barrier sublayer 313 include (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111, and the range of x is 0.5≤x≤0.8, (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 has a thickness ranging from 1 nm to 6 nm, and the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 has a thickness of (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 in Dimensions parallel to the stacking direction. When the thickness of the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 exceeds 6 nm, the barrier layer 31 will seriously block the transition of carriers and affect the radiative recombination between carriers; when (Al x Ga 1-x ) When the thickness of the 0.5 In 0.5 P layer 3111 is less than 1 nm, the barrier layer 31 has a limited effect on electron confinement. In some embodiments, (Al x Ga 1-x ) 0.5 In 0.5 P is non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P, non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P has weak carrier absorption, which can improve the luminous efficiency.

其中,勢阱層32包括(Al mGa 1-m) 0.5In 0.5P層321,(Al mGa 1-m) 0.5In 0.5P層321的厚度範圍為3nm-10nm,(Al mGa 1-m) 0.5In 0.5P層321的厚度為(Al mGa 1-m) 0.5In 0.5P層321在平行於層疊方向上的尺寸。當(Al mGa 1-m) 0.5In 0.5P層321的厚度超過10nm時,多量子阱有源層30的波函數重疊較小,阻擋載流子的遷移,而降低內量子阱效率;當(Al mGa 1-m) 0.5In 0.5P層321的厚度低於3nm時,載流子容易溢出勢阱層32,而降低輻射複合效率。其中,m的取值可根據LED器件發出的光的波長設定,波長越長,m取值越小。在一些實施例中,(Al mGa 1-m) 0.5In 0.5P為非主動摻雜的(Al mGa 1-m) 0.5In 0.5P,非主動摻雜的(Al mGa 1-m) 0.5In 0.5P對載流子、光子的吸收較弱,可提高發光效率。 Wherein, the potential well layer 32 includes (Al m Ga 1-m ) 0.5 In 0.5 P layer 321, the thickness range of (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 is 3 nm-10 nm, (Al m Ga 1- The thickness of the m ) 0.5 In 0.5 P layer 321 is the dimension of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 parallel to the stacking direction. When the thickness of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 exceeds 10 nm, the wave function overlap of the multi-quantum well active layer 30 is small, which blocks the migration of carriers and reduces the efficiency of the internal quantum well; when When the thickness of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 is less than 3 nm, the carriers are likely to overflow the potential well layer 32 , thereby reducing the radiation recombination efficiency. Wherein, the value of m can be set according to the wavelength of light emitted by the LED device, and the longer the wavelength, the smaller the value of m. In some embodiments, (Al m Ga 1-m ) 0.5 In 0.5 P is non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P, non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P has weak absorption of carriers and photons, which can improve the luminous efficiency.

其中,多量子阱有源層30包括3至21層勢壘層31和2至20層勢阱層32,其中,勢壘層31的層數比勢阱層32的層數多一層。每層勢壘層31與鄰近的一層勢阱層32形成一個多量子阱週期,前述的多量子阱有源層30包括2至20個多量子阱週期。多量子阱週期數目一般不超過20,當多量子阱週期數目過多,多量子阱有源層30整體過厚,會增加載流子在多量子阱有源層30中的的非輻射複合,而影響發光效率;當多量子阱週期數目過少,多量子阱有源層30的勢壘層31及LED器件的電子阻擋層無法將多數電子限制在多量子阱有源層30中,使得電子溢出至p型半導體層40導致發光效率降低。Wherein, the MQW active layer 30 includes 3 to 21 barrier layers 31 and 2 to 20 potential well layers 32 , wherein the number of barrier layers 31 is one more than the number of potential well layers 32 . Each barrier layer 31 and an adjacent potential well layer 32 form a multi-quantum well period, and the aforementioned multi-quantum well active layer 30 includes 2 to 20 multi-quantum well periods. The number of multi-quantum well periods generally does not exceed 20. When the number of multi-quantum well periods is too large, the overall thickness of the multi-quantum well active layer 30 will increase the non-radiative recombination of carriers in the multi-quantum well active layer 30, and Affect luminous efficiency; when the number of MQW periods is too small, the barrier layer 31 of the MQW active layer 30 and the electron blocking layer of the LED device cannot confine most electrons in the MQW active layer 30, so that electrons overflow to The p-type semiconductor layer 40 causes reduction in luminous efficiency.

請一併參閱圖1與圖4,圖4為本申請實施例提供的勢壘層31的形成方法的流程圖。如圖4所示,勢壘第一子層311和勢壘第三子層313均包括(Al xGa 1-x) 0.5In 0.5P層3111,在n型半導體層20背離襯底的一側形成勢壘層31,包括以下步驟: Please refer to FIG. 1 and FIG. 4 together. FIG. 4 is a flow chart of the method for forming the barrier layer 31 provided by the embodiment of the present application. As shown in FIG. 4 , both the first barrier sublayer 311 and the third barrier sublayer 313 include an (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111, on the side of the n-type semiconductor layer 20 away from the substrate Forming the barrier layer 31 includes the following steps:

S1031:通入磷烷和第一比例的三甲基鎵、三甲基鋁、三甲基銦,以在n型半導體層20背離襯底的一側形成(Al xGa 1-x) 0.5In 0.5P層3111。 S1031: Passing phosphine and a first ratio of trimethylgallium, trimethylaluminum, and trimethylindium to form (Al x Ga 1-x ) 0.5 In on the side of the n-type semiconductor layer 20 away from the substrate 0.5 P layer 3111.

S1032:通入砷烷、三甲基鎵和三甲基鋁,以在(Al xGa 1-x) 0.5In 0.5P層3111背離n型半導體層20的一側形成Al yGa 1-yAs層。 S1032: Passing arsine, trimethylgallium and trimethylaluminum to form AlyGa1 -yAs on the side of the ( AlxGa1 -x ) 0.5In0.5P layer 3111 away from the n-type semiconductor layer 20 layer.

S1033:通入磷烷和第一比例的三甲基鎵、三甲基鋁、三甲基銦,以在Al yGa 1-yAs層上形成(Al xGa 1-x) 0.5In 0.5P層3111。 S1033: Passing phosphine and the first ratio of trimethylgallium, trimethylaluminum, and trimethylindium to form ( Al x Ga 1-x ) 0.5 In 0.5 P on the AlyGa 1-y As layer Layer 3111.

S1034:對Al yGa 1-yAs層進行氧化處理,以氧化Al yGa 1-yAs層而形成Al yGa 1-yAs的氧化物層3121。 S1034: Perform oxidation treatment on the AlyGa1 -yAs layer to form an AlyGa1 -yAs oxide layer 3121 by oxidizing the AlyGa1 -yAs layer.

其中,砷烷、三甲基鎵和三甲基鋁發生熱分解反應生成Al yGa 1-yAs,通過氧化Al yGa 1-yAs而生成Al yGa 1-yAs的氧化物。其中,Al yGa 1-yAs的氧化物包括氧化鋁和氧化鎵,氧化鋁的禁帶帶隙較寬,能夠有效提升勢壘層31與勢阱層32的能級差,而增強勢壘層31對電子的限制效果。並且,載流子通過Al yGa 1-yAs的氧化物層3121時主要通過隧道躍遷,可以遮罩缺陷導電,並且可以減小電流瞬態增加,從而提升LED器件的耐反向偏壓性能和抗靜電性能等。 Among them, arsine, trimethylgallium and trimethylaluminum undergo a thermal decomposition reaction to generate AlyGa 1-y As, and the oxide of AlyGa 1-y As is generated by oxidizing AlyGa 1-y As. Among them, the oxides of Al y Ga 1-y As include aluminum oxide and gallium oxide, and aluminum oxide has a wide bandgap, which can effectively increase the energy level difference between the barrier layer 31 and the potential well layer 32, and enhance the potential barrier Confinement effect of layer 31 on electrons. Moreover, when the carriers pass through the oxide layer 3121 of AlyGa1 -yAs , they mainly transition through tunneling, which can shield defects and conduct electricity, and can reduce the transient increase of current, thereby improving the reverse bias resistance performance of LED devices and antistatic properties.

其中,Al yGa 1-yAs的氧化物中y的取值範圍為0.8≤y≤1.0。 Wherein, the value range of y in the oxide of Al y Ga 1-y As is 0.8≤y≤1.0.

其中,Al yGa 1-yAs的氧化物層3121的厚度範圍為0.5nm-3nm,Al yGa 1-yAs的氧化物層3121的厚度為Al yGa 1-yAs的氧化物層3121在平行於層疊方向上的尺寸。當Al yGa 1-yAs的氧化物層3121的厚度超過3nm時,勢壘層31會嚴重阻擋載流子的躍遷,而影響載流子之間的輻射複合。在一些實施例中,Al yGa 1-yAs的氧化物為非主動摻雜的Al yGa 1-yAs的氧化物,非主動摻雜的Al yGa 1-yAs氧化物對載流子的吸收較弱,可提高發光效率。 Wherein, the thickness range of the oxide layer 3121 of AlyGa1 -yAs is 0.5nm-3nm, and the thickness of the oxide layer 3121 of AlyGa1 - yAs is the oxide layer 3121 of AlyGa1 -yAs Dimensions parallel to the lamination direction. When the thickness of the oxide layer 3121 of AlyGa1 -yAs exceeds 3nm, the barrier layer 31 will seriously block the transition of carriers and affect the radiative recombination between carriers. In some embodiments, the oxide of AlyGa 1-y As is an oxide of non-actively doped AlyGa 1-y As, and the oxide of non-actively doped AlyGa 1-yAs has a positive effect on the carrier The absorption of sub-substances is weak, which can improve the luminous efficiency.

其中,(Al xGa 1-x) 0.5In 0.5P中x的取值範圍為0.5≤x≤0.8。 Wherein, the value range of x in (Al x Ga 1-x ) 0.5 In 0.5 P is 0.5≤x≤0.8.

其中,(Al xGa 1-x) 0.5In 0.5P層3111的厚度範圍為1nm-6nm,(Al xGa 1-x) 0.5In 0.5P層3111的厚度為(Al xGa 1-x) 0.5In 0.5P層3111在平行於層疊方向上的尺寸。當(Al xGa 1-x) 0.5In 0.5P層3111的厚度超過6nm時,勢壘層31會嚴重阻擋載流子的躍遷,而影響載流子之間的輻射複合;當(Al xGa 1-x) 0.5In 0.5P層3111的厚度低於3nm時,勢壘層31對電子的限制作用有限。 Wherein, the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 has a thickness ranging from 1 nm to 6 nm, and the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 has a thickness of (Al x Ga 1-x ) 0.5 The dimensions of the In 0.5 P layer 3111 parallel to the stacking direction. When the thickness of the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 exceeds 6 nm, the barrier layer 31 will seriously block the transition of carriers and affect the radiative recombination between carriers; when (Al x Ga 1-x ) When the thickness of the 0.5 In 0.5 P layer 3111 is less than 3 nm, the restriction effect of the barrier layer 31 on electrons is limited.

其中,形成Al yGa 1-yAs層的條件包括:溫度為650℃-700℃、壓力為50mbar-80mbar以及Ⅴ/Ⅲ為50-100,其中,Ⅴ/Ⅲ為Ⅴ族源與Ⅲ族源的氣體流量之比,Ⅴ族源包括砷烷,Ⅲ族源包括三甲基鎵和三甲基鋁中的至少一種。在此工藝條件下,有利於形成厚度均一的Al yGa 1-yAs層。在一些實施例中,Al yGa 1-yAs層為非主動摻雜的Al yGa 1-yAs層,砷烷、三甲基鎵和三甲基鋁發生熱分解反應會生成Al yGa 1-yAs以及副產物碳,而通過控制溫度、壓力以及Ⅴ/Ⅲ等工藝條件,可使得副產物中的碳進入Al yGa 1-yAs而形成非主動摻雜的Al yGa 1-yAs。非主動摻雜的Al yGa 1-yAs被氧化處理後形成非主動摻雜的Al yGa 1-yAs的氧化物,非主動摻雜的Al yGa 1-yAs的氧化物對載流子的吸收較弱,可提高發光效率。 Among them, the conditions for forming the AlyGa 1-y As layer include: the temperature is 650°C-700°C, the pressure is 50mbar-80mbar, and V/III is 50-100, wherein, V/III is the source of Group V and the source of Group III The ratio of the gas flow rate, the group V source includes arsine, and the group III source includes at least one of trimethylgallium and trimethylaluminum. Under this process condition, it is beneficial to form an AlyGa1 -yAs layer with uniform thickness. In some embodiments, the AlyGa 1-y As layer is a non-actively doped AlyGa 1-y As layer, and the thermal decomposition reaction of arsine, trimethylgallium and trimethylaluminum will generate AlyGa 1-y As and by-product carbon, and by controlling the process conditions such as temperature, pressure and Ⅴ/Ⅲ, the carbon in the by-product can enter AlyGa 1-yAs to form non-actively doped AlyGa 1- y As. The non-actively doped AlyGa 1-y As is oxidized to form the non-actively doped AlyGa 1-yAs oxide, and the non-actively doped AlyGa 1-yAs oxide supports The absorption of the carrier is weak, which can improve the luminous efficiency.

其中,形成(Al xGa 1-x) 0.5In 0.5P層3111的條件包括:溫度為680℃-730℃,壓力為50mbar-80mbar。在此工藝條件下,有利於形成厚度均一的(Al xGa 1-x) 0.5In 0.5P層3111。在一些實施例中,(Al xGa 1-x) 0.5In 0.5P層3111為非主動摻雜的(Al xGa 1-x) 0.5In 0.5P層,磷烷、三甲基鎵、三甲基鋁和三甲基銦發生熱分解反應會生成(Al xGa 1-x) 0.5In 0.5P以及副產物碳,而通過控制溫度、壓力以及Ⅴ/Ⅲ等工藝條件,可使得副產物中的碳進入(Al xGa 1-x) 0.5In 0.5P而形成非主動摻雜的(Al xGa 1-x) 0.5In 0.5P。非主動摻雜的(Al xGa 1-x) 0.5In 0.5P對載流子的吸收較弱,可提高發光效率。 Wherein, the conditions for forming the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 include: a temperature of 680°C-730°C, and a pressure of 50mbar-80mbar. Under this process condition, it is favorable to form the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 with uniform thickness. In some embodiments, the (Al x Ga 1-x ) 0.5 In 0.5 P layer 3111 is a non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P layer, phosphine, trimethylgallium, trimethylgallium (Al x Ga 1-x ) 0.5 In 0.5 P and the by-product carbon will be generated by the thermal decomposition reaction of base aluminum and trimethyl indium, and by controlling the process conditions such as temperature, pressure and Ⅴ/Ⅲ, the by-product can be made Carbon enters (Al x Ga 1-x ) 0.5 In 0.5 P to form non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P. Non-actively doped (Al x Ga 1-x ) 0.5 In 0.5 P has weak carrier absorption and can improve luminous efficiency.

其中,對Al yGa 1-yAs層進行氧化處理,具體的,通入氧氣或水蒸氣與氮氣的混合氣,控制氧化溫度為400℃-500℃,氧氣、水蒸氣的氣體流量為5sccm-20sccm,而對Al yGa 1-yAs層進行氧化處理。其中,氧化處理溫度低於400℃時,氧化速率低,Al yGa 1-yAs的氧化物的形成速率低,造成LED器件的生產效率低;氧化處理溫度高於500℃時,會破壞LED器件的結構。在400℃-500℃以及有氧的條件下,Al yGa 1-yAs中的Al、Ga極易被氧化而生成氧化鋁和氧化鎵。 Among them, the Al y Ga 1-y As layer is oxidized, specifically, a mixed gas of oxygen or water vapor and nitrogen is introduced, the oxidation temperature is controlled at 400°C-500°C, and the gas flow rate of oxygen and water vapor is 5 sccm- 20sccm, while the AlyGa1 -yAs layer is oxidized. Among them, when the oxidation treatment temperature is lower than 400°C, the oxidation rate is low, and the formation rate of the oxide of AlyGa 1-y As is low, resulting in low production efficiency of LED devices; when the oxidation treatment temperature is higher than 500°C, the LED will be destroyed. The structure of the device. Under the conditions of 400°C-500°C and oxygen, Al and Ga in AlyGa 1-yAs are easily oxidized to form alumina and gallium oxide.

在一些實施例中,前述的在勢壘層31背離n型半導體層20的一側形成勢阱層32,包括:通入磷烷和第二比例的三甲基鎵、三甲基鋁、三甲基銦,以在勢壘層31背離n型半導體層20的一側形成(Al mGa 1-m) 0.5In 0.5P層321。 In some embodiments, the aforementioned formation of the potential well layer 32 on the side of the barrier layer 31 away from the n-type semiconductor layer 20 includes: introducing phosphine and a second ratio of trimethylgallium, trimethylaluminum, trimethylgallium, and trimethylgallium. methyl indium, to form a (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 on the side of the barrier layer 31 away from the n-type semiconductor layer 20 .

其中,(Al mGa 1-m) 0.5In 0.5P層321的厚度範圍為3nm-10nm,(Al mGa 1-m) 0.5In 0.5P層321的厚度為(Al mGa 1-m) 0.5In 0.5P層321在平行於層疊方向上的尺寸。當(Al mGa 1-m) 0.5In 0.5P層321的厚度超過10nm時,多量子阱有源層30的波函數重疊較小,阻擋載流子的遷移,而降低內量子阱效率;當(Al mGa 1-m) 0.5In 0.5P層321的厚度低於3nm時,載流子容易溢出勢阱層32,而降低輻射複合效率。 Wherein, the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 has a thickness ranging from 3 nm to 10 nm, and the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 has a thickness of (Al m Ga 1-m ) 0.5 The dimensions of the In 0.5 P layer 321 parallel to the stacking direction. When the thickness of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 exceeds 10 nm, the wave function overlap of the multi-quantum well active layer 30 is small, which blocks the migration of carriers and reduces the efficiency of the internal quantum well; when When the thickness of the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 is less than 3 nm, the carriers are likely to overflow the potential well layer 32 , thereby reducing the radiation recombination efficiency.

其中,形成(Al mGa 1-m) 0.5In 0.5P層321的條件包括:溫度為680℃-730℃,壓力為50mbar-80mbar及Ⅴ/Ⅲ為100-200。在此工藝條件下,有利於形成厚度均一的(Al mGa 1-m) 0.5In 0.5P層321。在一些實施例中,(Al mGa 1-m) 0.5In 0.5P層321為非主動摻雜的(Al mGa 1-m) 0.5In 0.5P層,磷烷、三甲基鎵、三甲基鋁和三甲基銦發生熱分解反應會生成(Al mGa 1-m) 0.5In 0.5P以及副產物碳,而通過控制溫度、壓力以及Ⅴ/Ⅲ等工藝條件,可使得副產物中的碳進入(Al mGa 1-m) 0.5In 0.5P而形成非主動摻雜的(Al mGa 1-m) 0.5In 0.5P。非主動摻雜的(Al mGa 1-m) 0.5In 0.5P對載流子、光子的吸收較弱,可提高發光效率。 Wherein, the conditions for forming the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 include: the temperature is 680° C.-730° C., the pressure is 50 mbar-80 mbar and V/III is 100-200. Under this process condition, it is favorable to form the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 with a uniform thickness. In some embodiments, the (Al m Ga 1-m ) 0.5 In 0.5 P layer 321 is a non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P layer, phosphine, trimethylgallium, trimethylgallium (Al m Ga 1-m ) 0.5 In 0.5 P and the by-product carbon will be generated by the thermal decomposition reaction of base aluminum and trimethyl indium, and by controlling the temperature, pressure and Ⅴ/Ⅲ process conditions, the by-products can be made Carbon enters (Al m Ga 1-m ) 0.5 In 0.5 P to form non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P. Non-actively doped (Al m Ga 1-m ) 0.5 In 0.5 P has weak absorption of carriers and photons, which can improve luminous efficiency.

請一併參閱圖2與圖5,圖5為圖3中步驟S102的子流程圖。如圖5所示,在一些實施例中,在襯底上形成n型半導體層20,包括以下步驟:Please refer to FIG. 2 and FIG. 5 together. FIG. 5 is a subflow chart of step S102 in FIG. 3 . As shown in FIG. 5, in some embodiments, forming an n-type semiconductor layer 20 on a substrate includes the following steps:

S1021:在襯底上形成緩衝層21。S1021: Form a buffer layer 21 on the substrate.

S1022:在緩衝層21背離襯底的一側形成n型歐姆接觸層22。S1022: Form an n-type ohmic contact layer 22 on a side of the buffer layer 21 away from the substrate.

S1023:在n型歐姆接觸層22背離緩衝層21的一側形成n型電流擴展層23。S1023: Form an n-type current spreading layer 23 on a side of the n-type ohmic contact layer 22 away from the buffer layer 21 .

S1024:在n型電流擴展層23背離n型歐姆接觸層22的一側形成n型限制層24。S1024: Form an n-type confinement layer 24 on a side of the n-type current spreading layer 23 away from the n-type ohmic contact layer 22 .

S1025:在n型限制層24背離n型電流擴展層23的一側形成n型波導層25。S1025: Form an n-type waveguide layer 25 on a side of the n-type confinement layer 24 away from the n-type current spreading layer 23 .

其中,可通過MOCVD、PVD等工藝形成緩衝層21、n型歐姆接觸層22、n型電流擴展層23、n型限制層24以及n型波導層25。Among them, the buffer layer 21 , n-type ohmic contact layer 22 , n-type current spreading layer 23 , n-type confinement layer 24 and n-type waveguide layer 25 can be formed by MOCVD, PVD and other processes.

其中,緩衝層21可為GaAs層,用於隔離和阻擋襯底表面的缺陷和雜質進入n型歐姆接觸層22。Wherein, the buffer layer 21 may be a GaAs layer, which is used to isolate and block defects and impurities on the substrate surface from entering the n-type ohmic contact layer 22 .

其中,n型歐姆接觸層22可為(Al aGa 1-a) 0.5In 0.5P層,a的取值範圍為0.3≤a≤0.6,用於與n電極形成歐姆接觸。 Wherein, the n-type ohmic contact layer 22 can be an (Al a Ga 1-a ) 0.5 In 0.5 P layer, and the range of a is 0.3≤a≤0.6, which is used to form an ohmic contact with the n-electrode.

其中,n型電流擴展層23可為(Al bGa 1-b) 0.5In 0.5P層,b的取值範圍為0.5≤b≤1.0,在電流流經n型電流擴展層23擴展至多量子阱有源層30時,n型電流擴展層23能夠使得到達多量子阱有源層30的電流密度是均勻的,均勻的電流分佈可提高發光效率。 Wherein, the n-type current spreading layer 23 can be an (Al b Ga 1-b ) 0.5 In 0.5 P layer, and the value range of b is 0.5≤b≤1.0. In the active layer 30, the n-type current spreading layer 23 can make the current density reaching the multi-quantum well active layer 30 uniform, and the uniform current distribution can improve the luminous efficiency.

其中,n型限制層24可為AlInP層,n型限制層24的禁帶寬度大於多量子阱有源層30,可將空穴限制在多量子阱有源層30中,提高電子擴展的均勻性,使得電子與空穴在多量子阱有源層30中輻射複合。Wherein, the n-type confinement layer 24 can be an AlInP layer, and the band gap of the n-type confinement layer 24 is greater than the multi-quantum well active layer 30, holes can be confined in the multi-quantum well active layer 30, and the uniformity of electron expansion can be improved. properties, so that electrons and holes radiatively recombine in the MQW active layer 30 .

其中,n型波導層25可為(Al cGa 1-c) 0.5In 0.5P層,c的取值範圍為0.5≤c≤1.0。n型波導層25的折射率低於多量子阱有源層30,使得多量子阱有源層30發出的光束在n型波導層25與多量子阱有源層30的交界處發生全反射,而使得光束能集中出射,而提升光提取效率。 Wherein, the n-type waveguide layer 25 may be an (Al c Ga 1-c ) 0.5 In 0.5 P layer, and the range of c is 0.5≤c≤1.0. The refractive index of the n-type waveguide layer 25 is lower than that of the multi-quantum well active layer 30, so that the light beam emitted by the multi-quantum well active layer 30 is totally reflected at the junction of the n-type waveguide layer 25 and the multi-quantum well active layer 30, Therefore, the light beam can be emitted in a concentrated manner, thereby improving the light extraction efficiency.

請一併參閱圖2與圖6,圖6為圖3中步驟S104的子流程圖。如圖6所示,在一些實施例中,在多量子阱有源層30背離n型半導體層20的一側形成p型半導體層40,包括以下步驟:Please refer to FIG. 2 and FIG. 6 together. FIG. 6 is a subflow chart of step S104 in FIG. 3 . As shown in FIG. 6, in some embodiments, forming a p-type semiconductor layer 40 on the side of the multi-quantum well active layer 30 away from the n-type semiconductor layer 20 includes the following steps:

S1041:在多量子阱有源層30背離n型半導體層20的一側形成p型波導層41。S1041: Form a p-type waveguide layer 41 on a side of the multi-quantum well active layer 30 away from the n-type semiconductor layer 20 .

S1042:在p型波導層41背離多量子阱有源層30的一側形成p型限制層42。S1042: Form a p-type confinement layer 42 on a side of the p-type waveguide layer 41 away from the MQW active layer 30 .

S1043:在p型限制層42背離p型波導層41的一側形成過渡層43。S1043: Form a transition layer 43 on a side of the p-type confinement layer 42 away from the p-type waveguide layer 41 .

S1044:在過渡層43背離p型限制層42的一側形成p型電流擴展層44。S1044: Form a p-type current spreading layer 44 on a side of the transition layer 43 away from the p-type confinement layer 42 .

S1045:在p型電流擴展層44的背離過渡層43的一側形成p型歐姆接觸層45。S1045 : Form a p-type ohmic contact layer 45 on a side of the p-type current spreading layer 44 away from the transition layer 43 .

其中,可通過MOCVD、PVD等工藝形成p型波導層41、p型限制層42、過渡層43、P型電流擴展層44以及p型歐姆接觸層45。Among them, the p-type waveguide layer 41 , p-type confinement layer 42 , transition layer 43 , p-type current spreading layer 44 and p-type ohmic contact layer 45 can be formed by MOCVD, PVD and other processes.

其中,p型波導層41可為(Al dGa 1-d) 0.5In 0.5P層,d的取值範圍為0.5≤d≤1.0,p型波導子層41的折射率低於多量子阱有源層30,使得多量子阱有源層30發出的光束在p型波導層41與多量子阱有源層30的交界處發生全反射,而使得光束能集中出射,而提升光提取效率。 Wherein, the p-type waveguide layer 41 can be (Al d Ga 1-d ) 0.5 In 0.5 P layer, the value range of d is 0.5≤d≤1.0, and the refractive index of the p-type waveguide sublayer 41 is lower than that of multiple quantum wells The source layer 30 makes the light beam emitted by the multi-quantum well active layer 30 undergo total reflection at the junction of the p-type waveguide layer 41 and the multi-quantum well active layer 30, so that the light beam can be emitted concentratedly, thereby improving the light extraction efficiency.

其中,p型限制層42可為AlInP層,p型限制層42的禁帶寬度大於多量子阱有源層30,可將電子限制在多量子阱有源層30中,使得電子與空穴在多量子阱有源層30中輻射複合。Wherein, the p-type confinement layer 42 can be an AlInP layer, and the band gap of the p-type confinement layer 42 is greater than the multi-quantum well active layer 30, and electrons can be confined in the multi-quantum well active layer 30, so that electrons and holes are Radiative recombination in the multiple quantum well active layer 30 .

其中,p型電流擴展層44可為GaP層,用於與p電極形成歐姆接觸。Wherein, the p-type current spreading layer 44 may be a GaP layer for forming an ohmic contact with the p-electrode.

其中,過渡層43可為(Al eGa 1-e) 0.5In 0.5P層,設置於p型限制層42與p型電流擴展層44之間,起晶格過渡作用,能夠減小p型限制層42與p型電流擴展層44之間的晶格失配,而減小p型電流擴展層44的缺陷密度。 Wherein, the transition layer 43 can be an (Al e Ga 1-e ) 0.5 In 0.5 P layer, which is arranged between the p-type confinement layer 42 and the p-type current spreading layer 44, and acts as a lattice transition to reduce the p-type confinement layer. The lattice mismatch between the layer 42 and the p-type current spreading layer 44 reduces the defect density of the p-type current spreading layer 44 .

其中,p型歐姆接觸層45可為GaP層,用於與p電極形成歐姆接觸。Wherein, the p-type ohmic contact layer 45 may be a GaP layer for forming an ohmic contact with the p-electrode.

綜上,本申請實施例提供的LED外延結構的製造方法,形成的多量子阱有源層30包括Al yGa 1-yAs的氧化物層3121,Al yGa 1-yAs的氧化物中的氧化鋁為寬禁帶材料,使得勢壘層31與勢阱層32之間的能級差更大,可有效增強勢壘層31對電子的限制以及增強多量子阱有源層30的量子化效應,從而有效提升LED器件的內量子效率、出光效率、耐反向偏壓性能以及抗靜電能力等。 To sum up, in the manufacturing method of the LED epitaxial structure provided by the embodiment of the present application, the formed multi-quantum well active layer 30 includes the oxide layer 3121 of AlyGa 1-y As, and the oxide layer 3121 of AlyGa 1-y As Aluminum oxide is a wide bandgap material, so that the energy level difference between the barrier layer 31 and the potential well layer 32 is larger, which can effectively enhance the confinement of electrons by the barrier layer 31 and enhance the quantum of the multi-quantum well active layer 30. The chemical effect can effectively improve the internal quantum efficiency, light extraction efficiency, reverse bias resistance performance and antistatic ability of LED devices.

上述實施例提供的LED外延結構的製造方法與前述的LED外延結構相互對應,相關之處可以相互參照。The manufacturing method of the LED epitaxial structure provided in the foregoing embodiments corresponds to the above-mentioned LED epitaxial structure, and reference may be made to each other for relevant parts.

需要說明的是,對於前述的各方法實施例,為了簡單描述,故將其都表述為一系列的動作組合,但是本領域技術人員應該知悉,本申請並不受所描述的動作順序的限制,因為依據本申請,某些步驟可以採用其他順序或者同時進行。It should be noted that for the foregoing method embodiments, for the sake of simple description, they are expressed as a series of action combinations, but those skilled in the art should know that the present application is not limited by the described action sequence. Depending on the application, certain steps may be performed in other orders or simultaneously.

在上述實施例中,對各個實施例的描述都各有側重,某個實施例中沒有詳述的部分,可以參見其它實施例的相關描述。In the above-mentioned embodiments, the descriptions of each embodiment have their own emphases, and for parts not described in detail in a certain embodiment, reference may be made to relevant descriptions of other embodiments.

應當理解的是,本發明的應用不限於上述的舉例,對本領域普通技術人員來說,可以根據上述說明加以改進或變換,所有這些改進和變換都應屬於本發明所附權利要求的保護範圍。It should be understood that the application of the present invention is not limited to the above examples, and those skilled in the art can make improvements or changes according to the above descriptions, and all these improvements and changes should belong to the scope of protection of the appended claims of the present invention.

20:n型半導體層 21:緩衝層 22:n型歐姆接觸層 23:n型電流擴展層 24:n型限制層 25:n型波導層 30:多量子阱有源層 31:勢壘層 32:勢阱層 40:p型半導體層 41:p型波導層 42:p型限制層 43:過渡層 44:p型電流擴展層 45:p型歐姆接觸層 100:LED外延結構 311:勢壘第一子層 312:勢壘第二子層 313:勢壘第三子層 3121:Al yGa 1:yAs的氧化物層 3111:(Al xGa 1:x) 0.5In 0.5P層 321:(Al mGa 1:m) 0.5In 0.5P層 20: n-type semiconductor layer 21: buffer layer 22: n-type ohmic contact layer 23: n-type current spreading layer 24: n-type confinement layer 25: n-type waveguide layer 30: multiple quantum well active layer 31: barrier layer 32 : potential well layer 40: p-type semiconductor layer 41: p-type waveguide layer 42: p-type confinement layer 43: transition layer 44: p-type current spreading layer 45: p-type ohmic contact layer 100: LED epitaxial structure 311: potential barrier First sublayer 312: potential barrier second sublayer 313: potential barrier third sublayer 3121: Al y Ga 1: y As oxide layer 3111: (Al x Ga 1: x ) 0.5 In 0.5 P layer 321: ( Al m Ga 1:m ) 0.5 In 0.5 P layer

為了更清楚地說明本申請實施例中的技術方案,下面將對實施例中所需要使用的附圖作簡單地介紹,顯而易見地,下面描述中的附圖是本申請的一些實施例,對於本領域普通技術人員來講,在不付出創造性勞動的前提下,還可以根據這些附圖獲得其他的附圖。In order to more clearly illustrate the technical solutions in the embodiments of the present application, the drawings that need to be used in the embodiments will be briefly introduced below. Obviously, the drawings in the following description are some embodiments of the present application. Those of ordinary skill in the art can also obtain other drawings based on these drawings without any creative effort.

圖1為本申請實施例提供的LED外延結構的截面結構示意圖。FIG. 1 is a schematic cross-sectional structure diagram of an LED epitaxial structure provided by an embodiment of the present application.

圖2為本申請另一實施例提供的LED外延結構的截面結構示意圖。FIG. 2 is a schematic cross-sectional structure diagram of an LED epitaxial structure provided by another embodiment of the present application.

圖3為本申請實施例提供的LED外延結構的製造方法的流程圖。FIG. 3 is a flowchart of a method for manufacturing an LED epitaxial structure provided by an embodiment of the present application.

圖4為本申請實施例提供的勢壘層的形成方法的流程圖。FIG. 4 is a flowchart of a method for forming a barrier layer provided by an embodiment of the present application.

圖5為圖3中步驟S102的子流程圖。FIG. 5 is a sub-flow chart of step S102 in FIG. 3 .

圖6為圖3中步驟S104的子流程圖。FIG. 6 is a sub-flow chart of step S104 in FIG. 3 .

20:n型半導體層 20: n-type semiconductor layer

30:多量子阱有源層 30: Multi-quantum well active layer

31:勢壘層 31: Barrier layer

32:勢阱層 32: Potential well layer

40:p型半導體層 40: p-type semiconductor layer

100:LED外延結構 100: LED epitaxial structure

311:勢壘第一子層 311: The first sublayer of the potential barrier

312:勢壘第二子層 312: The second sublayer of the potential barrier

313:勢壘第三子層 313: The third sublayer of the potential barrier

3121:AlyGa1:yAs的氧化物層 3121: Al y Ga 1: y As oxide layer

3111:(AlxGa1:x)0.5In0.5P層 3111: (Al x Ga 1: x ) 0.5 In 0.5 P layer

321:(AlmGa1:m)0.5In0.5P層 321: (Al m Ga 1: m ) 0.5 In 0.5 P layer

Claims (13)

一種LED外延結構,所述LED外延結構包括依次層疊設置的n型半導體層、多量子阱有源層及p型半導體層,其特徵在於,所述多量子阱有源層包括至少三層勢壘層和至少二層勢阱層,所述勢壘層和所述勢阱層交替層疊設置,其中,所述勢壘層包括依次層疊設置的勢壘第一子層、勢壘第二子層以及勢壘第三子層,所述勢壘第二子層包括Al yGa 1-yAs的氧化物層。 An LED epitaxial structure, the LED epitaxial structure includes an n-type semiconductor layer, a multi-quantum well active layer and a p-type semiconductor layer stacked in sequence, wherein the multi-quantum well active layer includes at least three layers of barriers layer and at least two layers of potential well layers, the barrier layers and the potential well layers are alternately stacked, wherein the barrier layer includes the first sublayer of the potential barrier, the second sublayer of the potential barrier and the The third sublayer of the potential barrier, the second sublayer of the potential barrier includes an oxide layer of AlyGa1 -yAs . 如請求項1所述之LED外延結構,其特徵在於,所述Al yGa 1-yAs的氧化物中y的取值範圍為0.8≤y≤1.0。 The LED epitaxial structure according to Claim 1, characterized in that the range of y in the AlyGa 1-y As oxide is 0.8≤y≤1.0. 如請求項1所述之LED外延結構,其特徵在於,所述Al yGa 1-yAs的氧化物層的厚度範圍為0.5nm-3nm。 The LED epitaxial structure according to Claim 1, wherein the thickness of the AlyGa 1-y As oxide layer is in the range of 0.5nm-3nm. 如請求項1所述之LED外延結構,其特徵在於,所述勢壘第一子層和勢壘第三子層均包括(Al xGa 1-x) 0.5In 0.5P層。 The LED epitaxial structure according to Claim 1, wherein the first barrier sublayer and the third barrier sublayer both comprise (Al x Ga 1-x ) 0.5 In 0.5 P layers. 如請求項4所述之LED外延結構,其特徵在於,所述(Al xGa 1-x) 0.5In 0.5P中x的取值範圍為0.5≤x≤0.8。 The LED epitaxial structure according to Claim 4, wherein the value range of x in (Al x Ga 1-x ) 0.5 In 0.5 P is 0.5≤x≤0.8. 如請求項4所述之LED外延結構,其特徵在於,所述(Al xGa 1-x) 0.5In 0.5P層的厚度範圍為1nm-6nm。 The LED epitaxial structure according to Claim 4, wherein the thickness of the (Al x Ga 1-x ) 0.5 In 0.5 P layer is in the range of 1nm-6nm. 如請求項1所述之LED外延結構,其特徵在於,所述勢阱層包括(Al mGa 1-m) 0.5In 0.5P層。 The LED epitaxial structure according to claim 1, wherein the potential well layer comprises (Al m Ga 1-m ) 0.5 In 0.5 P layer. 如請求項7所述之LED外延結構,其特徵在於,所述(Al mGa 1-m) 0.5In 0.5P層的厚度範圍為3nm-10nm。 The LED epitaxial structure according to Claim 7, characterized in that the (Al m Ga 1-m ) 0.5 In 0.5 P layer has a thickness ranging from 3nm to 10nm. 如請求項1所述之LED外延結構,其特徵在於,所述多量子阱有源層包括3至21層勢壘層和2至20層勢阱層,其中,勢壘層的層數比勢阱層的層數多一層。The LED epitaxial structure according to Claim 1, wherein the multi-quantum well active layer includes 3 to 21 barrier layers and 2 to 20 potential well layers, wherein the ratio of the number of barrier layers to the potential The number of well layers is one more. 一種LED器件,其特徵在於,所述LED器件包括n電極、p電極以及如請求項1-9任一項所述的LED外延結構,所述n電極與所述n型半導體層電連接,所述p電極與所述p型半導體層電連接。An LED device, characterized in that the LED device includes an n-electrode, a p-electrode, and the LED epitaxial structure according to any one of claims 1-9, the n-electrode is electrically connected to the n-type semiconductor layer, and the The p-electrode is electrically connected to the p-type semiconductor layer. 一種LED外延結構的製造方法,其特徵在於,所述LED外延結構的製造方法包括以下步驟: 提供襯底; 在所述襯底上形成n型半導體層; 在所述n型半導體層背離所述襯底的一側形成多量子阱有源層; 在所述多量子阱有源層背離所述n型半導體層的一側形成p型半導體層; 其中,形成所述多量子阱有源層包括在所述n型半導體層背離所述襯底的一側形成勢壘層,在所述勢壘層背離所述n型半導體層的一側形成勢阱層,以及重複交替形成所述勢壘層和所述勢阱層而形成至少三層勢壘層和至少二層勢阱層,所述勢壘層包括依次層疊形成的勢壘第一子層、勢壘第二子層以及勢壘第三子層,所述勢壘第二子層包括Al yGa 1-yAs的氧化物層。 A method for manufacturing an LED epitaxial structure, characterized in that the method for manufacturing an LED epitaxial structure includes the following steps: providing a substrate; forming an n-type semiconductor layer on the substrate; A multi-quantum well active layer is formed on one side of the substrate; a p-type semiconductor layer is formed on the side of the multi-quantum well active layer away from the n-type semiconductor layer; wherein, forming the multi-quantum well active layer includes Forming a barrier layer on the side of the n-type semiconductor layer away from the substrate, forming a potential well layer on the side of the barrier layer away from the n-type semiconductor layer, and repeatedly forming the barrier layers alternately and the potential well layer to form at least three barrier layers and at least two potential well layers, the barrier layer includes the first sublayer of the potential barrier, the second sublayer of the potential barrier and the third A sublayer, the barrier second sublayer includes an oxide layer of AlyGa1 -yAs . 如請求項11所述之LED外延結構的製造方法,其特徵在於,所述勢壘第一子層和勢壘第三子層均包括(Al xGa 1-x) 0.5In 0.5P層,所述在所述n型半導體層背離所述襯底的一側形成勢壘層,包括: 通入磷烷和第一比例的三甲基鎵、三甲基鋁、三甲基銦,以在所述n型半導體層背離所述襯底的一側形成(Al xGa 1-x) 0.5In 0.5P層; 通入砷烷、三甲基鎵和三甲基鋁,以在所述(Al xGa 1-x) 0.5In 0.5P層背離所述n型半導體層的一側形成Al yGa 1-yAs層; 通入磷烷和第一比例的三甲基鎵、三甲基鋁、三甲基銦,以在所述Al yGa 1-yAs層上形成(Al xGa 1-x) 0.5In 0.5P層; 對所述Al yGa 1-yAs層進行氧化處理,以氧化所述Al yGa 1-yAs層而形成Al yGa 1-yAs的氧化物層。 The method for manufacturing an LED epitaxial structure according to Claim 11, wherein the first sublayer of the potential barrier and the third sublayer of the potential barrier both include (Al x Ga 1-x ) 0.5 In 0.5 P layers, so The formation of a barrier layer on the side of the n-type semiconductor layer away from the substrate includes: introducing phosphine and a first proportion of trimethylgallium, trimethylaluminum, and trimethylindium, so that the Form (Al x Ga 1-x ) 0.5 In 0.5 P layer on the side of the n-type semiconductor layer away from the substrate ; Ga 1-x ) 0.5 In 0.5 P layer forms an AlyGa 1-y As layer on the side away from the n-type semiconductor layer; feeds phosphine and a first proportion of trimethylgallium, trimethylaluminum, trimethyl methyl indium to form a (Al x Ga 1- x ) 0.5 In 0.5 P layer on the AlyGa 1-y As layer; performing oxidation treatment on the AlyGa 1-y As layer to oxidize the The above-mentioned AlyGa1 -yAs layer is formed to form an AlyGa1 -yAs oxide layer. 如請求項11所述之LED外延結構的製造方法,其特徵在於,所述在所述勢壘層背離所述n型半導體層的一側形成勢阱層,包括: 通入磷烷和第二比例的三甲基鎵、三甲基鋁、三甲基銦,以在所述勢壘層背離所述n型半導體層的一側形成(Al mGa 1-m) 0.5In 0.5P層。 The method for manufacturing an LED epitaxial structure according to Claim 11, wherein the formation of a potential well layer on the side of the barrier layer away from the n-type semiconductor layer includes: introducing phosphine and a second Trimethylgallium, trimethylaluminum, and trimethylindium in proportion to form a (Al m Ga 1-m ) 0.5 In 0.5 P layer on the side of the barrier layer away from the n-type semiconductor layer.
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