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TWI394293B - Light emitting diode - Google Patents

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TWI394293B
TWI394293B TW96117736A TW96117736A TWI394293B TW I394293 B TWI394293 B TW I394293B TW 96117736 A TW96117736 A TW 96117736A TW 96117736 A TW96117736 A TW 96117736A TW I394293 B TWI394293 B TW I394293B
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semiconductor layer
layer
crystal structure
photonic crystal
light
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TW96117736A
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TW200847463A (en
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Zhen-Feng Xu
Guo-Fan Jin
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Hon Hai Prec Ind Co Ltd
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Description

發光二極體 Light-emitting diode

本發明涉及一種發光二極體,尤其涉及具有較高光提取效率之發光二極體。 The present invention relates to a light-emitting diode, and more particularly to a light-emitting diode having higher light extraction efficiency.

由氮化鎵基(GaN)半導體材料製成之高效藍光、綠光及白光發光二極體(LED)具有壽命長、節能、綠色環保等顯著特點,已被廣泛應用於大螢幕彩色顯示、汽車照明、交通訊號、多媒體顯示及光通訊等領域,特別於照明領域具有廣闊之發展潛力。先前之LED通常包括N型半導體層、P型半導體層、設置於N型半導體層與P型半導體層之間之活性層、設置於P型半導體層上之正極(通常為透明電極)以及設置於N型半導體層上之負極。LED處於工作狀態時,於P型半導體層與N型半導體層上分別施加正、負電壓,這樣,存在於P型半導體層中之空穴與存在於N型半導體層中之電子相互靠近而進入到活性層中;並於活性層中發生複合而產生光波,該光波透過透明電極從LED中發射出。然而,先前之LED提取效率(提取效率通常指活性層中所產生之光波從LED內部釋放出之效率)較低,這主要係由於全反射現象與材料對光波之吸收引起的。全反射現象之產生係由於半導體之折射率大於空氣之折射率。來自活性層之光波於半導體與空氣之介面處發生全反射,從而大部分光波被限制於LED之內部,直至被LED內之材料完全吸收。 High-efficiency blue, green and white light-emitting diodes (LEDs) made of gallium nitride-based (GaN) semiconductor materials have longevity, energy saving, green environmental protection, etc., and have been widely used in large-screen color displays and automobiles. In the fields of lighting, traffic signal, multimedia display and optical communication, it has broad development potential especially in the field of lighting. The prior LED generally includes an N-type semiconductor layer, a P-type semiconductor layer, an active layer disposed between the N-type semiconductor layer and the P-type semiconductor layer, a positive electrode (usually a transparent electrode) disposed on the P-type semiconductor layer, and A negative electrode on the N-type semiconductor layer. When the LED is in operation, positive and negative voltages are applied to the P-type semiconductor layer and the N-type semiconductor layer, respectively, so that holes existing in the P-type semiconductor layer and electrons existing in the N-type semiconductor layer are adjacent to each other. Into the active layer; and recombination occurs in the active layer to generate light waves, which are emitted from the LED through the transparent electrode. However, previous LED extraction efficiencies (extraction efficiency generally refers to the efficiency with which light waves generated in the active layer are released from the interior of the LED) are low due to total reflection and material absorption of light waves. The total reflection phenomenon occurs because the refractive index of the semiconductor is greater than the refractive index of the air. The light from the active layer is totally reflected at the interface between the semiconductor and the air, so that most of the light is confined to the inside of the LED until it is completely absorbed by the material inside the LED.

有鑒於此,提供一種具有較高提取效率之LED實屬必要。 In view of this, it is necessary to provide an LED with high extraction efficiency.

以下以實施例說明一種發光二極體。 Hereinafter, a light-emitting diode will be described by way of examples.

一種發光二極體,其包括一基底、反射層、有源層、透明電極、第一光子晶體結構以及第二光子晶體結構。所述反射層形成於上述基底上,所述有源層形成於上述反射層上,且所述透明電極形成於上述有源層上。所述透明電極包括一上表面及一下表面,該透明電極之下表面與上述有源層相結合。所述第一光子晶體結構設置於上述透明電極之上表面,且所述第二光子晶體結構形成於上述有源層中。 A light emitting diode includes a substrate, a reflective layer, an active layer, a transparent electrode, a first photonic crystal structure, and a second photonic crystal structure. The reflective layer is formed on the substrate, the active layer is formed on the reflective layer, and the transparent electrode is formed on the active layer. The transparent electrode includes an upper surface and a lower surface, and the lower surface of the transparent electrode is combined with the active layer. The first photonic crystal structure is disposed on an upper surface of the transparent electrode, and the second photonic crystal structure is formed in the active layer.

一種發光二極體,其包括基底、反射層、第一半導體層、活性層、第二半導體層、透明電極、第一光子晶體結構以及第二光子晶體結構。所述反射層設置於上述基底上,所述第一半導體層設置於上述反射層上,所述第二半導體層設置於上述第一半導體層上,所述活性層設置於上述第一半導體層與第二半導體層之間,所述透明電極設置於上述第二半導體層上。所述活性層包括一底面與上述第一半導體層相結合,所述第二光子晶體結構形成於上述活性層之底面。所述透明電極包括一上表面及一下表面,該透明電極之下表面與上述第二半導體層相結合,所述第一光子晶體結構設置於上述透明電極之上表面。 A light emitting diode comprising a substrate, a reflective layer, a first semiconductor layer, an active layer, a second semiconductor layer, a transparent electrode, a first photonic crystal structure, and a second photonic crystal structure. The reflective layer is disposed on the substrate, the first semiconductor layer is disposed on the reflective layer, the second semiconductor layer is disposed on the first semiconductor layer, and the active layer is disposed on the first semiconductor layer The transparent electrode is disposed on the second semiconductor layer between the second semiconductor layers. The active layer includes a bottom surface coupled to the first semiconductor layer, and the second photonic crystal structure is formed on a bottom surface of the active layer. The transparent electrode includes an upper surface and a lower surface, the lower surface of the transparent electrode is combined with the second semiconductor layer, and the first photonic crystal structure is disposed on the upper surface of the transparent electrode.

與先前技術相比,上述發光二極體具有第一光子晶體結構與第二光子晶體結構,發光二極體工作過程產生光波,對於入射角較小之光波,第一光子晶體結構可將其衍 射至發光二極體之外部空間;而入射角較大之光波會被反射回有源層中,第二光子晶體結構可將其衍射為入射角較小之光波而再經第一光子晶體結構衍射至發光二極體之外部空間。這樣,第二光子晶體結構結合第一光子晶體結構對光波進行衍射,從而使光波較快出射至外部空間,這樣可減少反射光在有源層中進行多次反射,因而避免有源層材料以及反射層材料等對光波之吸收,從而使得發光二極體具有較高之光提取效率。 Compared with the prior art, the light-emitting diode has a first photonic crystal structure and a second photonic crystal structure, and the light-emitting diode generates light waves during operation, and the first photonic crystal structure can be used for light waves with a small incident angle. The light is incident on the outer space of the light-emitting diode; and the light wave with a larger incident angle is reflected back into the active layer, and the second photonic crystal structure can diffract it into a light wave with a smaller incident angle and then pass through the first photonic crystal structure. Diffraction to the outer space of the light-emitting diode. In this way, the second photonic crystal structure is combined with the first photonic crystal structure to diffract the light wave, so that the light wave is emitted to the external space relatively quickly, thereby reducing the multiple reflection of the reflected light in the active layer, thereby avoiding the active layer material and The absorption of the light wave by the material of the reflective layer, etc., so that the light-emitting diode has a higher light extraction efficiency.

下面將結合附圖及實施例對本技術方案之發光二極體作進一步之詳細說明。 The illuminating diode of the present technical solution will be further described in detail below with reference to the accompanying drawings and embodiments.

請參閱圖1,本技術方案實施例提供一種發光二極體100,其包括基底110、反射層120以及形成於反射層120上之發光二極體基體10。所述發光二極體基體10包括有源層11以及形成於有源層11上之透明電極160。所述有源層11包括第一半導體層130、活性層140以及第二半導體層150。該第一半導體層130、活性層140以及第二半導體層150依次形成於反射層120上。 Referring to FIG. 1 , an embodiment of the present invention provides a light emitting diode 100 including a substrate 110 , a reflective layer 120 , and a light emitting diode substrate 10 formed on the reflective layer 120 . The light emitting diode body 10 includes an active layer 11 and a transparent electrode 160 formed on the active layer 11. The active layer 11 includes a first semiconductor layer 130, an active layer 140, and a second semiconductor layer 150. The first semiconductor layer 130, the active layer 140, and the second semiconductor layer 150 are sequentially formed on the reflective layer 120.

所述透明電極160具有一上表面161及一下表面162,該下表面162與上述第二半導體層150相結合,該上表面161上形成有一第一光子晶體結構170。 The transparent electrode 160 has an upper surface 161 and a lower surface 162. The lower surface 162 is combined with the second semiconductor layer 150. A first photonic crystal structure 170 is formed on the upper surface 161.

所述有源層11中形成有一第二光子晶體結構180,可選地,該第二光子晶體結構180可形成於活性層140與第一半導體層130之介面處,具體可形成於活性層140之下表面(活性層140與第一半導體層130接觸之表面)上,亦可形成 於第一半導體層130之上表面(第一半導體層130與活性層140接觸之表面)上。另外,第二光子晶體結構180亦可形成在第一半導體層130之底面(第一半導體層130靠近反射層120之表面)。本實施例中,第二光子晶體結構180形成在第一半導體層130之底面上,即,有源層11之底面上。 A second photonic crystal structure 180 is formed in the active layer 11. Optionally, the second photonic crystal structure 180 may be formed at the interface between the active layer 140 and the first semiconductor layer 130, and may be formed on the active layer 140. The lower surface (the surface of the active layer 140 in contact with the first semiconductor layer 130) may also be formed On the upper surface of the first semiconductor layer 130 (the surface on which the first semiconductor layer 130 is in contact with the active layer 140). In addition, the second photonic crystal structure 180 may also be formed on the bottom surface of the first semiconductor layer 130 (the surface of the first semiconductor layer 130 near the reflective layer 120). In this embodiment, the second photonic crystal structure 180 is formed on the bottom surface of the first semiconductor layer 130, that is, on the bottom surface of the active layer 11.

優選地,所述第一半導體層130與反射層120之間可設置一黏結層190,用於將底面具有第二光子晶體結構180之有源層11與反射層120結合起來。 Preferably, a bonding layer 190 may be disposed between the first semiconductor layer 130 and the reflective layer 120 for combining the active layer 11 having the second photonic crystal structure 180 on the bottom surface and the reflective layer 120.

如圖2所示,光子晶體之結構特徵通常可通過以下三個參數來表徵,即,晶格常數(a)、孔徑(d)、孔深(h)。所述a係指光子晶體結構中相鄰孔之中心距。第一光子晶體結構170與第二光子晶體結構180之a、d、h取值範圍相同,即,a大約為0.5~2.0微米,d大約為0.5a~0.9a,h大於零且小於或等於0.5微米。當第一光子晶體結構170與第二光子晶體結構180之a、d、h均相同時,第一光子晶體結構170與第二光子晶體結構180之結構相同。當然,第一光子晶體結構170與第二光子晶體結構180之結構亦可不同,即兩者之a、d、h之取值不同。 As shown in FIG. 2, the structural features of the photonic crystal can generally be characterized by the following three parameters, namely, lattice constant (a), aperture (d), and hole depth (h). The a is the center distance of adjacent holes in the photonic crystal structure. The first photonic crystal structure 170 and the second photonic crystal structure 180 have the same range of a, d, and h, that is, a is about 0.5 to 2.0 micrometers, d is about 0.5a to 0.9a, and h is greater than zero and less than or equal to 0.5 micron. When the first photonic crystal structure 170 is the same as a, d, and h of the second photonic crystal structure 180, the first photonic crystal structure 170 is identical in structure to the second photonic crystal structure 180. Of course, the structures of the first photonic crystal structure 170 and the second photonic crystal structure 180 may also be different, that is, the values of a, d, and h of the two are different.

基底110之材料為藍寶石,還可為砷化鎵、磷化銦、矽、碳化矽、氮化矽等材料。反射層120由金屬材料形成,例如金屬銀或鋁。第一半導體層130為N型半導體層,其材料為N型氮化鎵(GaN),亦可為N型砷化鎵或N型磷化銅。活性層140之材料為氮化銦鎵(InGaN)。第二半導體層150為P型半導體層,其材料為P型GaN,還可為P型砷化鎵或P型磷化銅。透明電極層160之材料為氧化銦錫(ITO )。黏結層190可為環氧樹脂膠黏劑、紫外固化膠等。 The material of the substrate 110 is sapphire, and may also be a material such as gallium arsenide, indium phosphide, antimony, antimony carbide or tantalum nitride. The reflective layer 120 is formed of a metallic material such as metallic silver or aluminum. The first semiconductor layer 130 is an N-type semiconductor layer made of N-type gallium nitride (GaN) or N-type gallium arsenide or N-type phosphide. The material of the active layer 140 is indium gallium nitride (InGaN). The second semiconductor layer 150 is a P-type semiconductor layer made of P-type GaN, and may also be P-type gallium arsenide or P-type phosphide. The material of the transparent electrode layer 160 is indium tin oxide (ITO) ). The bonding layer 190 may be an epoxy resin adhesive, an ultraviolet curing adhesive, or the like.

下面對上述發光二極體100之製作方法進行詳細描述。第一步,提供一形成於基底110上之發光二極體基體10。所述發光二極體基體10包括第一半導體層130、活性層140、第二半導體層150以及透明電極160。且活性層140設置於第一半導體層130與第二半導體層150之間,透明電極160形成在第二半導體層150上。 The method of fabricating the above-described light emitting diode 100 will be described in detail below. In a first step, a light-emitting diode substrate 10 formed on a substrate 110 is provided. The light emitting diode substrate 10 includes a first semiconductor layer 130, an active layer 140, a second semiconductor layer 150, and a transparent electrode 160. The active layer 140 is disposed between the first semiconductor layer 130 and the second semiconductor layer 150, and the transparent electrode 160 is formed on the second semiconductor layer 150.

發光二極體基體10為先前技術中最簡易之發光二極體結構,其通常通過一系列之物理或化學沈積法形成於基底110上。本實施例中基底110為藍寶石材質,第一半導體層130為N型氮化鎵材質,第二半導體層150為P型氮化鎵材質,活性層140為氮化銦鎵材質,透明電極160為氧化銦錫材質。 The light-emitting diode substrate 10 is the simplest light-emitting diode structure of the prior art and is typically formed on the substrate 110 by a series of physical or chemical deposition methods. In the embodiment, the substrate 110 is made of sapphire, the first semiconductor layer 130 is made of N-type gallium nitride, the second semiconductor layer 150 is made of P-type gallium nitride, the active layer 140 is made of indium gallium nitride, and the transparent electrode 160 is Indium tin oxide material.

第二步,將基底110與發光二極體基體10進行分離。利用先前技術手段如雷射剝離等方法將基底110與發光二極體基體10沿基底110與第一半導體層130之介面分開。這樣便得到單獨之基底110,以及由第一半導體層130、活性層140、第二半導體層150以及透明電極160所組成之發光二極體基體10。 In the second step, the substrate 110 is separated from the light-emitting diode substrate 10. The substrate 110 and the light-emitting diode substrate 10 are separated along the interface of the substrate 110 and the first semiconductor layer 130 by a prior art method such as laser lift-off. Thus, a separate substrate 110, and a light-emitting diode substrate 10 composed of the first semiconductor layer 130, the active layer 140, the second semiconductor layer 150, and the transparent electrode 160 are obtained.

第三步,於第一半導體層130上製作第二光子晶體結構180。 In the third step, a second photonic crystal structure 180 is formed on the first semiconductor layer 130.

首先,具體製作前依次用丙酮、異丙醇、去離子水並結合超聲波對發光二極體基體10之第一半導體層130進行清洗,然後用氮氣吹幹。 First, the first semiconductor layer 130 of the light-emitting diode substrate 10 was washed with acetone, isopropyl alcohol, deionized water and ultrasonic waves in advance before the specific production, and then blown dry with nitrogen.

其次,利用電漿輔助化學氣相沈積法在第一半導體層130上形成一層抗蝕刻能力較強之薄膜,如二氧化矽薄膜。由於後續待形成之電子阻劑抗蝕刻能力不佳,因而此步驟所形成之二氧化矽薄膜可在電漿刻蝕過程中保護第一半導體層130不被破壞。 Next, a film having a strong etching resistance such as a hafnium oxide film is formed on the first semiconductor layer 130 by plasma-assisted chemical vapor deposition. Since the subsequent electronic resist to be formed has poor etching resistance, the ruthenium dioxide film formed in this step can protect the first semiconductor layer 130 from being damaged during the plasma etching process.

再次,在二氧化矽薄膜上形成電子阻劑層,如聚甲基丙烯酸甲酯(PMMA)。在形成PMMA層之前,需要對完成第二步後所得到結構,特別係二氧化矽薄膜層之表面進行清洗,並用氮氣吹幹。由於二氧化矽層表面存在水分會影響PMMA與二氧化矽層的結合效果,因此,為確保二氧化矽層表面無水可對其進行低溫加熱。然後,利用旋轉塗覆法在二氧化矽層上形成PMMA層。最後,利用電子束微影技術將第二光子晶體結構180之預設圖案形成在PMMA層上。 Again, an electron resistive layer, such as polymethyl methacrylate (PMMA), is formed on the hafnium oxide film. Before the formation of the PMMA layer, it is necessary to clean the surface obtained after the completion of the second step, in particular, the surface of the ruthenium oxide film layer, and blow dry with nitrogen. Since the presence of moisture on the surface of the cerium oxide layer affects the bonding effect of the PMMA layer and the cerium oxide layer, it can be heated at a low temperature to ensure that the surface of the cerium oxide layer is anhydrous. Then, a PMMA layer was formed on the ceria layer by a spin coating method. Finally, a predetermined pattern of the second photonic crystal structure 180 is formed on the PMMA layer by electron beam lithography.

再次,以活性離子反應法結合幹刻蝕之方式將PMMA之圖案轉移到二氧化矽層中。刻蝕深度為二氧化矽層之厚度,以使圖案露出第一半導體層130之表面。隨後,依次用丙酮、異丙醇、去離子水並結合超聲波清洗一段時間,如約5分鐘,然後利用紫外光臭氧清洗機清洗除去PMMA層。 Again, the pattern of PMMA is transferred to the cerium oxide layer by reactive ion reaction in combination with dry etching. The etching depth is the thickness of the hafnium oxide layer to expose the pattern to the surface of the first semiconductor layer 130. Subsequently, it is washed successively with acetone, isopropanol, deionized water and ultrasonic waves for a period of time, such as about 5 minutes, and then the PMMA layer is removed by washing with an ultraviolet ozone cleaner.

最後,以活性離子反應法刻蝕第一半導體層130將二氧化矽層中之圖案轉移到第一半導體層130中。活性離子反應中,可使用三氯化硼(BCl3)氣體,待第一半導體層130被蝕刻形成圖案後,然後利用氫氟酸與去離子水除去二氧化矽層,從而在第一半導體層130上得到所需之第二光子 晶體結構180。 Finally, the first semiconductor layer 130 is etched by active ion reaction to transfer the pattern in the ceria layer to the first semiconductor layer 130. In the active ion reaction, boron trichloride (BCl 3 ) gas may be used. After the first semiconductor layer 130 is etched into a pattern, the cerium oxide layer is removed by using hydrofluoric acid and deionized water, thereby forming the first semiconductor layer. A desired second photonic crystal structure 180 is obtained at 130.

第四步,同上述在第一半導體層130上製作第二光子晶體結構180類似之方法,在透明電極160上製作第一光子晶體結構170。 In the fourth step, a first photonic crystal structure 170 is formed on the transparent electrode 160 in a manner similar to the above method of fabricating the second photonic crystal structure 180 on the first semiconductor layer 130.

第五步,在基底110之表面利用物理或化學氣相沈積法形成金屬反射層120。 In the fifth step, the metal reflective layer 120 is formed on the surface of the substrate 110 by physical or chemical vapor deposition.

第六步,將上述具有金屬反射層120之基底110及具有第一光子晶體結構170與第二光子晶體結構180之發光二極體基體10組裝起來,使得第一半導體層130與金屬反射層120通過黏膠層190結合於一起,從而得到本技術方案所述之發光二極體100。具體組裝方法可採用膠黏型材料將兩者膠合起來,或採用習知、可行之方法。 In the sixth step, the substrate 110 having the metal reflective layer 120 and the LED substrate 10 having the first photonic crystal structure 170 and the second photonic crystal structure 180 are assembled such that the first semiconductor layer 130 and the metal reflective layer 120 are disposed. The phosphor layers 190 are bonded together to obtain the light-emitting diode 100 of the present technical solution. The specific assembly method can be glued with an adhesive material, or a conventional and feasible method can be used.

上述製備之發光二極體100工作時,可在基底110上設置一負電極,並分別在透明電極160(通常為正極)與基底110之負電極上施加正電壓與負電壓,這樣在電場作用下,第二半導體層150中之空穴載流子會向第一半導體層130移動,同時第一半導體層130中之電子載流體會向第二半導體層150移動,這樣,空穴載流子與電子載流子在活性層140中將會發生複合並釋放出能量,而該釋放出之能量將會以光能之形式釋放出來,即,產生光波。所產生之光波會經透明電極160從發光二極體100內部發射出來。 When the light-emitting diode 100 prepared above is in operation, a negative electrode may be disposed on the substrate 110, and a positive voltage and a negative voltage are applied to the negative electrode of the transparent electrode 160 (usually the positive electrode) and the substrate 110, respectively, so that under the electric field The hole carriers in the second semiconductor layer 150 move toward the first semiconductor layer 130 while the electron carrier fluid in the first semiconductor layer 130 moves toward the second semiconductor layer 150, so that the hole carriers are The electron carriers will recombine in the active layer 140 and release energy, and the released energy will be released in the form of light energy, that is, light waves are generated. The generated light wave is emitted from the inside of the light emitting diode 100 through the transparent electrode 160.

活性層140中產生之光波會以不同角度入射至透明電極160中,對於形成在透明電極160上之第一光子晶體結構 170來說,其會對入射角較小之光波產生較好之衍射作用,即,入射角較小之光波經第一光子晶體結構170衍射後可進入外部自由空間中。而入射角較大之光波會在透明電極160與第二半導體層150之介面發生反射,重新回到有源層11中。當回到有源層11中之反射光入射至第二光子晶體結構180時,第二光子晶體結構180會將反射光衍射為入射角較小之光波至反射層120,此入射角較小之光波經反射層120反射後重新到達第二光子晶體結構180,然後再由第二光子晶體結構180衍射到透明電極160。此過程可將入射角較大之光波變為符合第一光子晶體結構170衍射條件之入射角較小之光波而到達透明電極160中,然後經第一光子晶體結構170之再次衍射而進入發光二極體100之外部空間中。本實施例中,設置在有源層11中之第二光子晶體結構180結合設置在透明電極160上之第一光子晶體結構170對光波之衍射作用,可大大減少反射光在有源層11中進行反射的次數,因而避免有源層11材料以及反射層120材料等對光波之吸收,從而使得本實施例之發光二極體100具有較高之光提取效率。 The light waves generated in the active layer 140 are incident into the transparent electrode 160 at different angles for the first photonic crystal structure formed on the transparent electrode 160. In 170, it produces a better diffractive effect on a light wave having a smaller incident angle, that is, a light wave having a smaller incident angle is diffracted by the first photonic crystal structure 170 and can enter the external free space. The light wave having a large incident angle is reflected by the interface between the transparent electrode 160 and the second semiconductor layer 150, and is returned to the active layer 11. When the reflected light returning to the active layer 11 is incident on the second photonic crystal structure 180, the second photonic crystal structure 180 diffracts the reflected light into a light wave having a smaller incident angle to the reflective layer 120, and the incident angle is smaller. The light wave is reflected by the reflective layer 120 and then reaches the second photonic crystal structure 180, and then diffracted by the second photonic crystal structure 180 to the transparent electrode 160. In this process, the light wave having a larger incident angle is converted into a light wave having a smaller incident angle according to the diffraction condition of the first photonic crystal structure 170, and reaches the transparent electrode 160, and then diffracted by the first photonic crystal structure 170 to enter the light-emitting diode. In the outer space of the polar body 100. In this embodiment, the second photonic crystal structure 180 disposed in the active layer 11 combines the diffracting effect of the first photonic crystal structure 170 disposed on the transparent electrode 160 on the optical wave, and the reflected light is greatly reduced in the active layer 11. The number of times of reflection is performed, thereby avoiding absorption of light waves by the material of the active layer 11 and the material of the reflective layer 120, so that the light-emitting diode 100 of the present embodiment has higher light extraction efficiency.

下面通過實驗對上述實施例之發光二極體100之發光效果進行驗證。以波長450奈米之氮化鎵材料作為發光二極體100之有源層11材料,建立發光二極體100模型:反射層120、黏膠層190、有源層11、透明電極160之平均厚度依次為0.1微米、0.1微米、2.5微米、0.3微米;透明電極160與黏膠層190之折射率分別為2.0與1.5左右;有源層11與反射層120之複折射率分別為2.5+i0.02與 0.1+i5.6;第一光子晶體結構170與第二光子晶體結構180具有相同之a與d,具體地,a等於0.8微米,d等於0.8a;第一光子晶體結構170之孔深計為h1,且h1等於0.2微米;第二光子晶體結構180之孔深計為h2,且h2從零微米變化至0.5微米。 The illuminating effect of the light-emitting diode 100 of the above embodiment was verified by experiments. A gallium nitride material having a wavelength of 450 nm is used as the active layer 11 material of the light-emitting diode 100, and a model of the light-emitting diode 100 is established: an average of the reflective layer 120, the adhesive layer 190, the active layer 11, and the transparent electrode 160. The thicknesses are 0.1 micron, 0.1 micron, 2.5 micron, and 0.3 micron in order; the refractive indices of the transparent electrode 160 and the adhesive layer 190 are about 2.0 and 1.5, respectively; and the complex refractive indices of the active layer 11 and the reflective layer 120 are 2.5+i0, respectively. .02 and 0.1+i5.6; the first photonic crystal structure 170 and the second photonic crystal structure 180 have the same a and d, specifically, a is equal to 0.8 micron and d is equal to 0.8a; the aperture of the first photonic crystal structure 170 The depth is calculated as h 1 and h 1 is equal to 0.2 μm; the depth of the second photonic crystal structure 180 is h 2 , and h 2 is varied from zero micron to 0.5 μm.

根據上述發光二極體100之參數,利用時域有限差分法對發光二極體100之發光效率進行類比計算,各種參數結構之歸一化發光效率隨時間之變化如圖3所示,圖3中之橫坐標表示模擬時間;縱坐標表示隨第二光子晶體結構180孔深之變化,發光二極體100之發光效率與未設置第一光子晶體結構170及第二光子晶體結構之發光二極體發光效率之比值之變化。如圖3所示,曲線A表示當發光二極體100未設置第一光子晶體結構170及第二光子晶體結構時,此時之發光二極體稱作M-LED,其發光效率歸一化為1,作為參考曲線;當h2取零微米時,即,發光二極體100僅設置第一光子晶體結構170,此時之發光二極體通常稱作SPC-LED,從圖3可看出SPC-LED之發光效率約為M-LED之兩倍多;當h2等於0.3微米時,發光二極體100之發光效率為M-LED發光效率之3.2倍。因此,試驗結果表明,本實施例之發光二極體100相對於無光子晶體結構之發光二極體來說具有較高之光提取效率,較具有一個光子晶體結構之發光二極體來說,可進一步提高光提取效率。 According to the parameters of the above-mentioned light-emitting diode 100, the luminous efficiency of the light-emitting diode 100 is analogically calculated by the finite-difference time-domain method, and the normalized luminous efficiency of various parameter structures changes with time as shown in FIG. 3, FIG. 3 The abscissa of the middle represents the simulation time; the ordinate represents the change of the hole depth of the second photonic crystal structure 180, the luminous efficiency of the light emitting diode 100 and the light emitting diode of the first photonic crystal structure 170 and the second photonic crystal structure are not provided. The change in the ratio of bulk luminescence efficiency. As shown in FIG. 3, the curve A indicates that when the first photonic crystal structure 170 and the second photonic crystal structure are not disposed in the light emitting diode 100, the light emitting diode is called M-LED at this time, and the luminous efficiency is normalized. 1 is used as a reference curve; when h 2 is taken to be zero micrometers, that is, the light-emitting diode 100 is only provided with the first photonic crystal structure 170, and the light-emitting diode is usually referred to as SPC-LED, which can be seen from FIG. The luminous efficiency of the SPC-LED is about twice that of the M-LED; when h 2 is equal to 0.3 micron, the luminous efficiency of the LED 100 is 3.2 times that of the M-LED. Therefore, the test results show that the light-emitting diode 100 of the present embodiment has higher light extraction efficiency than the light-emitting diode having no photonic crystal structure, and can be further improved than the light-emitting diode having a photonic crystal structure. Improve light extraction efficiency.

綜上所述,本發明確已符合發明專利之要件,遂依法提出專利申請。惟,以上所述者僅為本發明之較佳實施例 ,自不能以此限制本案之申請專利範圍第。舉凡熟悉本案技藝之人士援依本發明之精神所作之等效修飾或變化,皆應涵蓋於以下申請專利範圍第內。 In summary, the present invention has indeed met the requirements of the invention patent, and has filed a patent application according to law. However, the above is only a preferred embodiment of the present invention. It is not possible to limit the scope of the patent application in this case. Equivalent modifications or variations made by persons skilled in the art in light of the spirit of the present invention are intended to be included in the scope of the following claims.

100‧‧‧發光二極體 100‧‧‧Lighting diode

110‧‧‧基底 110‧‧‧Base

120‧‧‧反射層 120‧‧‧reflective layer

130‧‧‧第一半導體層 130‧‧‧First semiconductor layer

140‧‧‧活性層 140‧‧‧Active layer

150‧‧‧第二半導體 150‧‧‧Second Semiconductor

11‧‧‧有源層 11‧‧‧Active layer

160‧‧‧透明電極 160‧‧‧Transparent electrode

170‧‧‧第一光子晶體結構 170‧‧‧First photonic crystal structure

180‧‧‧第二光子晶體結構 180‧‧‧Second photonic crystal structure

10‧‧‧發光二極體基體 10‧‧‧Light-emitting diode substrate

190‧‧‧黏結層 190‧‧‧bonded layer

161‧‧‧上表面 161‧‧‧ upper surface

162‧‧‧下表面 162‧‧‧ lower surface

圖1係本技術方案實施例發光二極體之剖面示意圖。 1 is a schematic cross-sectional view of a light emitting diode according to an embodiment of the present technical solution.

圖2係本技術方案實施例發光二極體之立體示意圖。 2 is a schematic perspective view of a light emitting diode according to an embodiment of the present technical solution.

圖3係利用時域有限差分法對上述實施例之發光二極體進行模擬計算所得到發光效率隨時間變化之曲線。 FIG. 3 is a graph showing the luminous efficiency as a function of time in the simulation calculation of the light-emitting diode of the above embodiment by the finite difference time domain method.

100‧‧‧發光二極體 100‧‧‧Lighting diode

110‧‧‧基底 110‧‧‧Base

120‧‧‧反射層 120‧‧‧reflective layer

130‧‧‧第一半導體層 130‧‧‧First semiconductor layer

140‧‧‧活性層 140‧‧‧Active layer

150‧‧‧第二半導體 150‧‧‧Second Semiconductor

11‧‧‧有源層 11‧‧‧Active layer

160‧‧‧透明電極 160‧‧‧Transparent electrode

170‧‧‧第一光子晶體結構 170‧‧‧First photonic crystal structure

180‧‧‧第二光子晶體結構 180‧‧‧Second photonic crystal structure

10‧‧‧發光二極體基體 10‧‧‧Light-emitting diode substrate

190‧‧‧黏結層 190‧‧‧bonded layer

161‧‧‧上表面 161‧‧‧ upper surface

162‧‧‧下表面 162‧‧‧ lower surface

Claims (9)

一種發光二極體,其包括:一基底;一反射層設置於上述基底上;一第一半導體層設置於上述反射層上;一第二半導體層設置於上述第一半導體層上;一活性層設置於上述第一半導體層與第二半導體層之間,該活性層包括一底面與上述第一半導體層相結合;以及一透明電極設置於上述第二半導體層上,該透明電極包括一上表面及一下表面,該透明電極之下表面與上述第二半導體層相結合;其改進在於,所述發光二極體進一步包括第一光子晶體結構與第二光子晶體結構,該第一光子晶體結構設置於上述透明電極之上表面,該第二光子晶體結構僅形成於上述活性層之底面第一半導體層的底面。 A light emitting diode comprising: a substrate; a reflective layer disposed on the substrate; a first semiconductor layer disposed on the reflective layer; a second semiconductor layer disposed on the first semiconductor layer; an active layer And disposed between the first semiconductor layer and the second semiconductor layer, the active layer includes a bottom surface coupled to the first semiconductor layer; and a transparent electrode disposed on the second semiconductor layer, the transparent electrode including an upper surface And a lower surface, the lower surface of the transparent electrode is combined with the second semiconductor layer; and the improvement is that the light emitting diode further comprises a first photonic crystal structure and a second photonic crystal structure, the first photonic crystal structure is disposed On the upper surface of the transparent electrode, the second photonic crystal structure is formed only on the bottom surface of the first semiconductor layer on the bottom surface of the active layer. 如申請專利範圍第1項所述之發光二極體,其中,所述第一光子晶體結構之晶格常數為0.5~2.0微米,孔徑為0.5~0.9倍之晶格常數,孔深小於或等於0.5微米。 The light-emitting diode according to claim 1, wherein the first photonic crystal structure has a lattice constant of 0.5 to 2.0 μm, a pore size of 0.5 to 0.9 times a lattice constant, and a pore depth of less than or equal to 0.5 micron. 如申請專利範圍第2項所述之發光二極體,其中,所述第二光子晶體結構之晶格常數為0.5~2.0微米,孔徑為0.5~0.9倍之晶格常數,孔深小於或等於0.5微米。 The light-emitting diode according to claim 2, wherein the second photonic crystal structure has a lattice constant of 0.5 to 2.0 μm, a pore size of 0.5 to 0.9 times a lattice constant, and a pore depth of less than or equal to 0.5 micron. 如申請專利範圍第3項所述之發光二極體,其中,所述第一光子晶體結構之晶格常數、孔徑以及孔深等於第二光子晶體結構之晶格常數、孔徑以及孔深。 The light-emitting diode according to claim 3, wherein a lattice constant, a pore diameter, and a hole depth of the first photonic crystal structure are equal to a lattice constant, a pore diameter, and a hole depth of the second photonic crystal structure. 如申請專利範圍第1項所述之發光二極體,其中,所述發 光二極體進一步包括一黏結層,該黏結層形成於所述第一半導體層與所述反射層之間。 The light-emitting diode according to claim 1, wherein the hair The photodiode further includes a bonding layer formed between the first semiconductor layer and the reflective layer. 一種發光二極體,其包括:一基底;一反射層形成於上述基底上;一有源層形成於上述反射層上;以及一透明電極形成於上述有源層上,該透明電極包括一上表面及一下表面,該透明電極之下表面與上述有源層相結合;所述有源層包括一第一半導體層、一第二半導體層及形成於第一半導體層與第二半導體層之間之活性層,所述活性層具有一下底面與所述第一半導體層相接觸,所述第一半導體層具有一上底面與所述活性層的下底面相結合;其改進在於,所述發光二極體進一步包括第一光子晶體結構與第二光子晶體結構,該第一光子晶體結構設置於上述透明電極之上表面,該第二光子晶體結構形成於上述有源層中第一半導體層與活性層的介面處。 A light emitting diode comprising: a substrate; a reflective layer formed on the substrate; an active layer formed on the reflective layer; and a transparent electrode formed on the active layer, the transparent electrode including an upper surface a surface and a lower surface, the lower surface of the transparent electrode is combined with the active layer; the active layer includes a first semiconductor layer, a second semiconductor layer, and is formed between the first semiconductor layer and the second semiconductor layer An active layer having a lower bottom surface in contact with the first semiconductor layer, the first semiconductor layer having an upper bottom surface combined with a lower bottom surface of the active layer; The pole body further includes a first photonic crystal structure disposed on an upper surface of the transparent electrode, and a second photonic crystal structure formed on the first semiconductor layer and active in the active layer At the interface of the layer. 如申請專利範圍第6項所述之發光二極體,其中,所述第二光子晶體結構形成於活性層之下底面。 The light-emitting diode according to claim 6, wherein the second photonic crystal structure is formed on a bottom surface of the active layer. 如申請專利範圍第6項所述之發光二極體,其中,所述第二光子晶體結構形成於第一半導體層之上底面。 The light-emitting diode according to claim 6, wherein the second photonic crystal structure is formed on a bottom surface of the first semiconductor layer. 如申請專利範圍第6項所述之發光二極體,其中,所述發光二極體進一步包括一黏結層,該黏結層形成於第一半導體層與反射層之間。 The light-emitting diode of claim 6, wherein the light-emitting diode further comprises a bonding layer formed between the first semiconductor layer and the reflective layer.
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Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW200603436A (en) * 2004-03-19 2006-01-16 Lumileds Lighting Llc Photonic crystal light emitting device
US20060027888A1 (en) * 2004-07-08 2006-02-09 Ikuo Yoshihara Solid-state image pickup device and manufacturing method thereof

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW200603436A (en) * 2004-03-19 2006-01-16 Lumileds Lighting Llc Photonic crystal light emitting device
US20060027888A1 (en) * 2004-07-08 2006-02-09 Ikuo Yoshihara Solid-state image pickup device and manufacturing method thereof

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