TWI424592B - White light semiconductor light-emitting device with filtering layer - Google Patents
White light semiconductor light-emitting device with filtering layer Download PDFInfo
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- 238000005530 etching Methods 0.000 description 1
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- HZXMRANICFIONG-UHFFFAOYSA-N gallium phosphide Chemical compound [Ga]#P HZXMRANICFIONG-UHFFFAOYSA-N 0.000 description 1
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Description
本發明係關於一種白光半導體發光元件(white light semiconductor light-emitting device),特別是關於一種具有濾光層(filtering layer)之高效率白光半導體發光元件。The present invention relates to a white light semiconductor light-emitting device, and more particularly to a high efficiency white light semiconductor light-emitting element having a filtering layer.
半導體發光元件(例如,發光二極體(light-emitting diode,LED))係一類相當重要的固態元件(solid state device),其將電能轉換成光。一典型的半導體發光元件通常包含一層或更多層由半導體材料製成的發光層(light-emitting layer),並且像三明治似地夾在相反摻雜型態的層之間。當一偏壓被施加通過上述摻雜層時,電洞與電子被注入發光層內,電洞與電子在發光層內再結合進而產生光。光從發光層朝全方向發射,並且從半導體發光元件的所有表面發射出去。有用的光通常是朝向該半導體發光元件的出光面所發射的光。Semiconductor light-emitting elements (eg, light-emitting diodes (LEDs)) are a class of relatively important solid state devices that convert electrical energy into light. A typical semiconductor light-emitting element typically comprises one or more layers of light-emitting layers made of a semiconductor material and sandwiched between layers of oppositely doped forms. When a bias voltage is applied through the doped layer, holes and electrons are injected into the light-emitting layer, and holes and electrons are recombined in the light-emitting layer to generate light. Light is emitted from the luminescent layer in all directions and is emitted from all surfaces of the semiconductor light emitting element. Useful light is typically light that is emitted toward the light exiting surface of the semiconductor light emitting element.
傳統LED的一項缺點就是它們不能從它們的發光層產生白光。讓傳統的LED產生白光的方法之一,即是將從不同種LED所發的不同色光混光成白光。例如,從紅光、綠光及藍光LED發光元件所發出的光,或者從藍光及黃光LED件所發出的光,可以被混光進而產生白光。此種方法的缺點之一即是它需要用到多種LED以產生單一顏色的光,明顯地增加了成本。除此之外,不同顏色的光通常係由不同型態的LED所產生,要將這些LED結合成一個元件必須需要複雜的製程來達成。上述完成的元件因為不同的二極體型態必須要不同的控制電壓,也必須需要複雜的控制電路。這些元件的長波長以及穩定性也會由於不同型態LED的不同時效行為而劣化。A disadvantage of conventional LEDs is that they do not produce white light from their luminescent layers. One of the methods for making conventional LEDs produce white light is to mix different colors of light emitted by different kinds of LEDs into white light. For example, light emitted from red, green, and blue LED light-emitting elements, or light emitted from blue and yellow LEDs, can be mixed to produce white light. One of the disadvantages of this approach is that it requires the use of multiple LEDs to produce a single color of light, which adds significant cost. In addition, different colors of light are usually produced by different types of LEDs. To combine these LEDs into one component requires a complicated process to achieve. The above completed components must have different control voltages due to different diode types, and complex control circuits must also be required. The long wavelength and stability of these components can also be degraded by the different ageing behavior of different types of LEDs.
近來,已經藉由用混入透明封裝材料(例如,環氧樹脂或矽膠)內的黃色光螢光粉(phosphor)、高分子(polymer)或染料(dye),等波長轉換材料(wavelength conversion material)環繞,來將從藍光單晶片LED所發出的光轉換成白光。此種方法的相關先前技術請參考美國專利第5,813,753號、美國專利第5,959,316號以及美國專利第6,069,440號。這些環繞的波長轉換材料將LED所發出之部分光的頻率向下轉換(再次發出的光具有較低的頻率),進而改變其顏色。例如,如果一顆氮化物基的藍光LED被黃色螢光粉環繞,其所發出的部分藍光將穿過螢光粉沒被改變,而剩餘的光將被向下轉換成黃光。上述案例中的LED將發出的藍光與由螢光粉轉換成的黃光結合,進而產生白光。此種類型的白光發光二極體製作容易且生產成本也較低,因此目前市面上之白光發光二極體大多為此種類型。此外,已有將螢光粉被覆在發光二極體晶片的出光面上上,已取代將螢光粉混入封裝材料內的技術被提出,相關先前技術請參考美國專利公開號第20080203410號。Recently, a wavelength conversion material such as a yellow light phosphor, a polymer, or a dye mixed in a transparent encapsulating material such as epoxy resin or silicone resin has been used. Surround, to convert light emitted from a blue single-chip LED into white light. For a prior art of such a method, reference is made to U.S. Patent No. 5,813,753, U.S. Patent No. 5,959,316, and U.S. Patent No. 6,069,440. These surrounding wavelength converting materials downconvert the frequency of the portion of light emitted by the LED (the re-emitted light has a lower frequency), which in turn changes its color. For example, if a nitride-based blue LED is surrounded by yellow phosphor, a portion of the blue light it emits will pass through the phosphor without being altered, and the remaining light will be converted down to yellow. In the above case, the LED emits blue light combined with yellow light converted from phosphor powder to produce white light. This type of white light emitting diode is easy to manufacture and has a low production cost, so most of the white light emitting diodes currently on the market are of this type. Further, there has been proposed a technique in which a phosphor powder is coated on a light-emitting surface of a light-emitting diode wafer, and a technique of mixing the phosphor powder into the package material has been proposed. For the related art, please refer to U.S. Patent Publication No. 20080203410.
上述利用晶片本身所發出的藍光與由螢光粉所轉換成的黃光混光成白光的LED,其面臨晶片發出的藍光在晶片的出光面發生全反射(total reflection),而無法發射出去。以往大多利用對LED晶片的出光面施以表面粗化來克服全反射。此種方法的相關先前技術請參考美國專利第6,277,665號、美國專利第6,429,460號以及美國專利第6,441,403號。這些表面粗化的先前技術大多需藉由蝕刻製程來達成,因此,製程上較為耗時,而且LED晶片的出光面的粗糙度較難控制達到全面均勻。此外,由螢光粉所發出的黃光也是朝全方向發射,因此,部分黃光會射入LED晶片而被LED晶片吸收,進而降低LED整體的發光效率。目前尚未見到既可克服藍光LED晶片之出光面對藍光造成的全反射,也可降低黃光被LED晶片吸收的技術被提出。The above-mentioned LED which uses the blue light emitted by the wafer itself and the yellow light converted by the phosphor powder to be white light is subjected to total reflection of the blue light emitted from the wafer on the light-emitting surface of the wafer, and cannot be emitted. In the past, the surface of the LED wafer was roughened to overcome total reflection. For a prior art of such a method, reference is made to U.S. Patent No. 6,277,665, U.S. Patent No. 6,429,460, and U.S. Patent No. 6,441,403. Most of the prior art of surface roughening is achieved by an etching process, and therefore, the process is time consuming, and the roughness of the light emitting surface of the LED wafer is difficult to control to achieve uniformity. In addition, the yellow light emitted by the phosphor powder is also emitted in all directions. Therefore, part of the yellow light is incident on the LED chip and absorbed by the LED chip, thereby reducing the overall luminous efficiency of the LED. At present, no technology has been found which overcomes the total reflection caused by the blue light of the blue LED chip facing the blue light, and also reduces the absorption of the yellow light by the LED wafer.
因此,本發明之主要範疇在於提供一種具有濾光層之白光半導體發光元件,以解決上述問題,進而提升白光半導體發光元件整體的發光效率。Accordingly, it is a primary object of the present invention to provide a white light semiconductor light-emitting element having a filter layer to solve the above problems and further improve the light-emitting efficiency of the white light-emitting semiconductor light-emitting element as a whole.
根據本發明之一較佳具體實施例之白光半導體發光元件,其包含一半導體疊層(semiconductor multi-layer)、一濾光層、一透明封裝材料以及一波長轉換材料。該半導體疊層包含一發光層。該發光層能被一電流激發,以發射一藍光波段的光。該半導體疊層具有一出光面。該濾光層係形成於該半導體疊層之該出光面上。該透明封裝材料係包覆該半導體疊層以及該濾光層。該波長轉換材料係均勻地分佈於該透明封裝材料內或被覆於該濾光層上。該波長轉換材料吸收該藍光波段的光之一部分再行發射一黃光波段的光。特別地,該濾光層能讓該藍光波段的光通過並反射該黃光波段的光。該藍光波段的光與該黃光波段的光進而混成白光。A white light semiconductor light-emitting device according to a preferred embodiment of the present invention comprises a semiconductor multi-layer, a filter layer, a transparent encapsulating material, and a wavelength converting material. The semiconductor stack includes a light emitting layer. The luminescent layer can be excited by a current to emit light in a blue band. The semiconductor stack has a light exit surface. The filter layer is formed on the light exit surface of the semiconductor stack. The transparent encapsulating material encapsulates the semiconductor stack and the filter layer. The wavelength converting material is uniformly distributed in or coated on the transparent encapsulating material. The wavelength converting material absorbs a portion of the light in the blue light band and emits light in a yellow light band. In particular, the filter layer allows light in the blue band to pass through and reflect light in the yellow band. The light in the blue band and the light in the yellow band are further mixed into white light.
於一具體實施例中,該濾光層係由一第一材料層以及一第二材料層交互堆疊成一多層複合材料層。該第一材料層可以由TiO2 、Ti3 O5 、Y2 O3 、HfO2 、Ta2 O5 或ZrO2 所形成。該第二材料層可以由SiO2 、MgF2 、Na3 AF6 或Al2 O3 所形成。In one embodiment, the filter layer is alternately stacked into a multi-layer composite layer by a first material layer and a second material layer. The first material layer may be formed of TiO 2 , Ti 3 O 5 , Y 2 O 3 , HfO 2 , Ta 2 O 5 or ZrO 2 . The second material layer may be formed of SiO 2 , MgF 2 , Na 3 AF 6 or Al 2 O 3 .
關於本發明之優點與精神可以藉由以下的發明詳述及所附圖式得到進一步的瞭解。The advantages and spirit of the present invention will be further understood from the following detailed description of the invention.
請參閱圖一,圖一繪示根據本發明之一較佳體實施例之白光半導體發光元件1之截面視圖。Referring to FIG. 1, FIG. 1 is a cross-sectional view of a white light semiconductor light emitting device 1 according to a preferred embodiment of the present invention.
如圖一所示,該白光半導體發光元件1包含一半導體疊層10、一濾光層12、一透明封裝材料14以及一波長轉換材料16。As shown in FIG. 1 , the white light semiconductor light emitting device 1 includes a semiconductor laminate 10 , a filter layer 12 , a transparent encapsulating material 14 , and a wavelength converting material 16 .
同樣示於圖一,如同典型的半導體發光元件,該白光半導體疊層10包含一基材(substrate)102以及在該基材102上形成的多層磊晶層。實務上,該基材102可以是玻璃(SiO2 )、矽(Si)、鍺(Ge)、氮化鎵(GaN)、砷化鎵(GaAs)、磷化鎵(GaP)、氮化鋁(AlN)、藍寶石(sapphire)、尖晶石(spinnel)、三氧化二鋁(Al2 O3 )、碳化矽(SiC)、氧化鋅(ZnO)、氧化鎂(MgO)、二氧化鋰鋁(LiAlO2 )、二氧化鋰鎵(LiGaO2 )或四氧化鎂二鋁(MgAl2 O4 ),等供磊晶用的基材。Also shown in FIG. 1, like a typical semiconductor light emitting device, the white light semiconductor stack 10 includes a substrate 102 and a plurality of epitaxial layers formed on the substrate 102. In practice, the substrate 102 may be glass (SiO 2 ), germanium (Si), germanium (Ge), gallium nitride (GaN), gallium arsenide (GaAs), gallium phosphide (GaP), aluminum nitride ( AlN), sapphire, spinel, Al 2 O 3 , SiC, zinc oxide, magnesium oxide (MgO), lithium aluminum oxide (LiAlO) 2 ), lithium gallium dioxide (LiGaO 2 ) or magnesium aluminum oxide (MgAl 2 O 4 ), and the like for the substrate for epitaxy.
該半導體疊層10之多層磊晶層包含一發光層104。該發光層104能被一電流激發,以發射一第一光。於一具體實施例中,該發光層104係由一II-VI族化合物或一III-V族化合物所形成。圖一所示案例,該發光層104為GaN基的發光層(GaN-based light-emitting layer),能被一電流激發,以發射藍光波段的光BL。於一具體實施例中,上述藍光波段的光之波長範圍係介於445~475nm。The multilayer epitaxial layer of the semiconductor stack 10 includes a light emitting layer 104. The luminescent layer 104 can be excited by a current to emit a first light. In one embodiment, the light-emitting layer 104 is formed of a II-VI compound or a III-V compound. In the case shown in FIG. 1, the luminescent layer 104 is a GaN-based light-emitting layer that can be excited by a current to emit light BL in the blue band. In a specific embodiment, the wavelength range of the light in the blue light band is between 445 and 475 nm.
如圖一所示,該半導體疊層10具有一出光面108。圖一所示案例,該半導體疊層10並且包含形成在多層磊晶層上之透明導電層106(例如,ITO層或ZnO層)。提供該半導體疊層10之出光面108者即為該透明導電層106。於實際應用中,提供該半導體疊層10之出光面108者也可能是多層磊晶層的頂表面。As shown in FIG. 1, the semiconductor laminate 10 has a light exiting surface 108. In the case shown in FIG. 1, the semiconductor stack 10 includes a transparent conductive layer 106 (eg, an ITO layer or a ZnO layer) formed on a plurality of epitaxial layers. The transparent conductive layer 106 is provided as the light-emitting surface 108 of the semiconductor laminate 10. In practical applications, the light exit surface 108 of the semiconductor stack 10 may also be the top surface of the multilayer epitaxial layer.
同樣示於圖一,該濾光層12係形成於該半導體疊層10之該出光面106上。特別地,該濾光層12之組成與結構係設計成讓射向該濾光層12之藍光波段的光穿透該濾光層12。例如,圖一中標示由該發光層104所發出的藍光波段的光BL係穿透該濾光層12。Also shown in FIG. 1, the filter layer 12 is formed on the light exit surface 106 of the semiconductor stack 10. In particular, the composition and structure of the filter layer 12 are designed such that light directed into the blue light band of the filter layer 12 penetrates the filter layer 12. For example, the light BL of the blue light band emitted by the light-emitting layer 104 in FIG. 1 penetrates the filter layer 12.
如圖一所示,該半導體疊層10並且包含兩個電極19。如同典型的半導體發光元件之封裝,一封裝基板(base)18係先製備。該封裝基板18上提供兩個端子182。該半導體疊層10係固定上該封裝基板18上。該兩電極19係以一打線接合(wire-bonding)的方式分別與該兩端子182做電連接。As shown in FIG. 1, the semiconductor stack 10 comprises two electrodes 19. As with the packaging of a typical semiconductor light emitting device, a package substrate 18 is prepared first. Two terminals 182 are provided on the package substrate 18. The semiconductor laminate 10 is fixed to the package substrate 18. The two electrodes 19 are electrically connected to the two terminals 182 in a wire-bonding manner.
如圖一所示,該透明封裝材料14係包覆該半導體疊層10以及該濾光層12。該波長轉換材料16(例如,螢光粉)係均勻地分佈於該透明封裝材料14內。於圖一中,一螢光粉體16被刻意誇大地描繪,以利說明光轉換的過程。該波長轉換材料16吸收該藍光波段的光之一部分再行發射一黃光波段的光。該藍光波段的光與該黃光波段的光進而混成白光。於一具體實施例,上述黃光波段的光之波長範圍係介於480~700nm。As shown in FIG. 1 , the transparent encapsulating material 14 covers the semiconductor laminate 10 and the filter layer 12 . The wavelength converting material 16 (eg, phosphor) is uniformly distributed within the transparent encapsulating material 14. In Figure 1, a phosphor powder 16 is deliberately exaggerated to illustrate the process of light conversion. The wavelength converting material 16 absorbs a portion of the light in the blue light band and emits light in a yellow light band. The light in the blue band and the light in the yellow band are further mixed into white light. In one embodiment, the wavelength of light in the yellow light band is between 480 and 700 nm.
特別地,該濾光層12之組成與結構係設計成讓射向該濾光層12之黃光波段的光被該濾光層12反射。圖一所示案例,該螢光粉體16為黃色螢光粉,能吸收藍光波段的光BL,再行發射黃光波段的光YL。射向該濾光層12之黃光波段的光YL被該濾光層12反射。藉此,降低黃光波段的光被該半導體疊層10吸收,進而提升該白光半導體發光元件1的整體發光效率。In particular, the composition and structure of the filter layer 12 are designed such that light directed to the yellow light band of the filter layer 12 is reflected by the filter layer 12. In the case shown in Fig. 1, the phosphor powder 16 is a yellow phosphor powder, which can absorb the light BL of the blue light band and emit the light YL of the yellow light band. The light YL that is incident on the yellow light band of the filter layer 12 is reflected by the filter layer 12. Thereby, the light in the yellow light band is absorbed by the semiconductor laminate 10, thereby improving the overall luminous efficiency of the white light semiconductor light emitting element 1.
請再參閱圖一,該濾光層12並且形成在該半導體疊層10之側表面上。藉此,該發光層104發出的藍光波段的光之取出率可以再增加,並且該波長轉換材料16所發出的黃光波段的光被該半導體疊層10吸收的量可以再降低,進而該白光半導體發光元件1的整體發光效率可以再提升。Referring again to FIG. 1, the filter layer 12 is formed on the side surface of the semiconductor laminate 10. Thereby, the light extraction rate of the blue light band emitted by the light emitting layer 104 can be further increased, and the amount of the yellow light band emitted by the wavelength converting material 16 can be further reduced by the semiconductor layer 10, and the white light is further reduced. The overall luminous efficiency of the semiconductor light emitting element 1 can be further improved.
圖一所示之白光半導體發光元件1的另一變異,該波長轉換材料16不是混入透明封裝材料14內,而是被覆於該濾光層12上形成螢光層。同樣地,被覆於該濾光層12上之波長轉換材料16吸收該藍光波段的光之一部分再行發射一黃光波段的光。也同樣地,該濾光層12之組成與結構係設計成讓射向該濾光層12之該黃光波段的光被該濾光層12反射。Another variation of the white light-emitting semiconductor light-emitting element 1 shown in FIG. 1 is that the wavelength-converting material 16 is not mixed into the transparent encapsulating material 14, but is coated on the filter layer 12 to form a phosphor layer. Similarly, the wavelength converting material 16 coated on the filter layer 12 absorbs a portion of the light in the blue light band and emits light in a yellow light band. Similarly, the composition and structure of the filter layer 12 are designed such that light in the yellow wavelength band that is directed toward the filter layer 12 is reflected by the filter layer 12.
請參閱圖二,根據本發明之白光半導體發光元件1係以一覆晶接合(flip-chip bonding)方式讓該兩電極19與該兩端子182直接接合。因此,提供該半導體疊層10之出光面108者是該基材102的底表面。該濾光層12係形成於該基材102的底表面上。同樣地,該波長轉換材料16係均勻地分佈於該透明封裝材料14內或塗佈在該濾光層12上。圖二中元件符號與圖一中元件符號相同者,即為先前已詳述的各個結構,其作用也相同,在此不多做贅述。需強調的是,該濾光層12並且形成在該半導體疊層10之側表面上,進一步提升該白光半導體發光元件1的整體發光效率。Referring to FIG. 2, the white light semiconductor light-emitting device 1 according to the present invention directly bonds the two electrodes 19 to the two terminals 182 by a flip-chip bonding method. Therefore, the light exit surface 108 of the semiconductor laminate 10 is provided as the bottom surface of the substrate 102. The filter layer 12 is formed on the bottom surface of the substrate 102. Similarly, the wavelength converting material 16 is uniformly distributed in or coated on the transparent encapsulating material 14. The component symbols in FIG. 2 are the same as those in FIG. 1, that is, the structures which have been described in detail above, and their functions are also the same, and will not be described here. It is to be emphasized that the filter layer 12 is formed on the side surface of the semiconductor laminate 10 to further enhance the overall luminous efficiency of the white light semiconductor light-emitting element 1.
圖二所示之白光半導體發光元件1的另一變異,該基材102可以被移除。因此,提供該半導體疊層10之出光面108者是多層磊晶層的底表面,並且該濾光層12係形成於該多層磊晶層的底表面上。Another variation of the white light semiconductor light-emitting element 1 shown in Fig. 2, the substrate 102 can be removed. Therefore, the light exiting surface 108 of the semiconductor laminate 10 is provided as a bottom surface of the multilayer epitaxial layer, and the filter layer 12 is formed on the bottom surface of the multilayer epitaxial layer.
於一具體實施例中,該濾光層12即為分佈式布拉格反射鏡(distributed Bragg reflector,DBR)。也就是說,該濾光層12係由具有較高折射率之一第一材料層以及具有較低折射率之一第二材料層交互堆疊成一多層複合材料層。多層複合材料層主要由(0.5H L 0.5H)m 組成,H為1/4λ厚的第一材料層,L為1/4λ厚的第二材料層。該第一材料層可以由TiO2 、Ti3 O5 、Y2 O3 、HfO2 、Ta2 O5 或ZrO2 所形成。該第二材料層可以由SiO2 、MgF2 、Na3 AF6 或Al2 O3 所形成。In a specific embodiment, the filter layer 12 is a distributed Bragg reflector (DBR). That is, the filter layer 12 is alternately stacked into a multilayer composite layer by a first material layer having a higher refractive index and a second material layer having a lower refractive index. The multilayer composite layer consists essentially of (0.5 HL 0.5H) m , H is a 1/4 λ thick first material layer, and L is a 1/4 λ thick second material layer. The first material layer may be formed of TiO 2 , Ti 3 O 5 , Y 2 O 3 , HfO 2 , Ta 2 O 5 or ZrO 2 . The second material layer may be formed of SiO 2 , MgF 2 , Na 3 AF 6 or Al 2 O 3 .
需強調的是,於實際應用上,該濾光層12即做為被覆在該半導體疊層10上的鈍化層(passivation layer),用以保護該半導體疊層10。It should be emphasized that, in practical applications, the filter layer 12 serves as a passivation layer over the semiconductor stack 10 for protecting the semiconductor stack 10.
於一具體實施例中,多層複合材料層形式之濾光層12係藉由一電子束蒸鍍製程所形成。為讓該濾光層12中每一層鍍膜的品質更佳,上述電子束蒸鍍製程可以採用一離子輔助電子束蒸鍍製程(ion-assisted electron-beam evaporation process)。In one embodiment, the filter layer 12 in the form of a multilayer composite layer is formed by an electron beam evaporation process. In order to make the quality of each layer of the filter layer 12 better, the electron beam evaporation process may employ an ion-assisted electron-beam evaporation process.
在此需強調的是,根據本發明之濾光層12其各層鍍膜的厚度除了需根據多層膜等效導納(effective admittance)的理論外,還需考量濾光層12所被覆之材料的折射率,更需考量到鍍膜材料本身的折射率會隨著入射光的波長不同而改變。因此在實務操作上,需先行藉由電腦模擬在特定半導體材料或透明導電材料上形成不同層數、不同鍍膜材料之多層抗反射結構層之整體光譜圖。It should be emphasized here that the thickness of the coating layer of each layer of the filter layer 12 according to the present invention requires consideration of the refraction of the material covered by the filter layer 12 in addition to the theory of the effective admittance of the multilayer film. The rate, more importantly, depends on the refractive index of the coating material itself to vary with the wavelength of the incident light. Therefore, in practical operation, it is necessary to first simulate the overall spectrum of the multilayer anti-reflection structure layer of different layers and different coating materials on a specific semiconductor material or a transparent conductive material by computer simulation.
關於根據本發明之濾光層對入射光之反射率的電腦模擬,請參閱圖三A、圖三B、圖三C、圖三D及圖三E。於該模擬案例中,在ITO層上形成SiO2 與TiO2 交互堆疊成27層之濾光層,濾光層的組成、各層材料的折射率以及各層的膜厚請見圖三A。For a computer simulation of the reflectance of the filter layer to incident light according to the present invention, please refer to FIG. 3A, FIG. 3B, FIG. 3C, FIG. 3D and FIG. In the simulation case, SiO 2 and TiO 2 were alternately stacked on the ITO layer to form a 27-layer filter layer. The composition of the filter layer, the refractive index of each layer of the material, and the film thickness of each layer are shown in FIG.
於該模擬案例中,先行模擬不同波長之入射光以0°、10°以及20°三個不同入射角度從GaN層射向圖三A所示ITO層、濾光層以及環氧樹脂的反射率,其模擬結果如圖三B所示。從圖三B的結果,清楚地顯示截止頻帶隨著入射角的增加而向短波長區域移動,並且在入射角20°以下,濾光層對455nm藍光的反射率可以降到10%以下。In the simulation case, the incident light of different wavelengths is first simulated to emit from the GaN layer to the ITO layer, the filter layer and the epoxy resin shown in FIG. 3A at three different incident angles of 0°, 10° and 20°. The simulation results are shown in Figure 3B. From the results of FIG. 3B, it is clearly shown that the cutoff band shifts toward the short wavelength region as the incident angle increases, and the reflectance of the filter layer to 455 nm blue light can be reduced to less than 10% at an incident angle of 20° or less.
圖三C為模擬由GaN基半導體發光元件所發出波長為455nm藍光之入射光以0°至90°的入射角度射向圖三A所示濾ITO層、濾光層以及環氧樹脂的反射率,由SiO2 鈍化層取代濾光層做相同之模擬的結果一併顯示於圖三C中。從圖三C的結果,雖看出介入濾光層造成全反射的臨界角約為22°,而介入SiO2 鈍化層造成全反射的臨界角約為27°。但是介入濾光層對於GaN基半導體發光元件發出藍光的整體取出率並未小於介入SiO2 鈍化層對於GaN基半導體發光元件發出藍光的整體取出率。Figure 3C is a graph showing the reflectance of the incident light of 455 nm blue light emitted from a GaN-based semiconductor light-emitting element at an incident angle of 0° to 90° toward the filtered ITO layer, the filter layer, and the epoxy resin shown in Fig. 3A. The results of the same simulation in which the filter layer was replaced by the SiO 2 passivation layer are shown in Fig. 3C. From the results of Fig. 3C, it is seen that the critical angle of total reflection caused by the intervening filter layer is about 22°, and the critical angle of total reflection caused by the intervening SiO 2 passivation layer is about 27°. However, the overall extraction rate of the intervening filter layer for emitting blue light to the GaN-based semiconductor light-emitting element is not less than the overall extraction rate of the blue light emitted by the intervening SiO 2 passivation layer for the GaN-based semiconductor light-emitting element.
於該模擬案例中,接著模擬不同波長之入射光以0°、10°、20°、30°、以及40°四個不同入射角度從環氧樹脂射向圖三A所示濾光層、ITO層以及GaN層的反射率,其模擬結果如圖三D所示。從圖三D的結果,清楚地顯示截止頻帶隨著入射角的增加而向短波長區域移動,並且在入射角40°以下,濾光層對570nm黃光的反射率可高達90%以上。In the simulation case, the incident light of different wavelengths is then simulated to be emitted from the epoxy resin to the filter layer shown in FIG. 3A at four different incident angles of 0°, 10°, 20°, 30°, and 40°, and ITO. The reflectance of the layer and the GaN layer is shown in Fig. 3D. From the results of Fig. 3D, it is clearly shown that the cutoff band shifts toward the short wavelength region as the incident angle increases, and the reflectance of the filter layer to 570 nm yellow light can be as high as 90% or more at an incident angle of 40 or less.
圖三E為模擬由螢光粉所發出波長為570nm黃光之入射光以0°至90°的入射角度從環氧樹脂射向圖三A所示濾光層、ITO層以及GaN層的反射率,由SiO2 鈍化層取代濾光層做相同之模擬的結果一併顯示於圖三E中。從圖三E的結果,清楚地顯示介入濾光層對570nm黃光的反射率可高達98%,而介入SiO2 鈍化層對570nm黃光的反射率低於10%。Figure 3E is a graph showing the reflectance of the incident light of 570 nm yellow light emitted by the phosphor from the epoxy resin to the filter layer, the ITO layer and the GaN layer shown in Fig. 3A at an incident angle of 0° to 90°. The result of the same simulation in which the filter layer was replaced by the SiO 2 passivation layer is shown in Fig. 3E. From the results of Figure 3E, it is clearly shown that the reflectance of the intervening filter layer to 570 nm yellow light can be as high as 98%, while the reflectivity of the intervening SiO 2 passivation layer to 570 nm yellow light is less than 10%.
藉由以上較佳具體實施例之詳述,係希望能更加清楚描述本發明之特徵與精神,而並非以上述所揭露的較佳具體實施例來對本發明之範疇加以限制。相反地,其目的是希望能涵蓋各種改變及具相等性的安排於本發明所欲申請之專利範圍的範疇內。因此,本發明所申請之專利範圍的範疇應該根據上述的說明作最寬廣的解釋,以致使其涵蓋所有可能的改變以及具相等性的安排。The features and spirit of the present invention will be more apparent from the detailed description of the preferred embodiments. On the contrary, the intention is to cover various modifications and equivalents within the scope of the invention as claimed. Therefore, the scope of the patented scope of the invention should be construed as broadly construed in the
1...白光半導體發光元件1. . . White light semiconductor light emitting element
10...半導體疊層10. . . Semiconductor stack
102...基材102. . . Substrate
104...發光層104. . . Luminous layer
106‧‧‧透明導電層106‧‧‧Transparent conductive layer
108‧‧‧出光面108‧‧‧Glossy
12‧‧‧濾光層12‧‧‧Filter layer
14‧‧‧透明封裝材料14‧‧‧Transparent packaging materials
16‧‧‧波長轉換材料16‧‧‧ wavelength conversion material
18‧‧‧封裝基板18‧‧‧Package substrate
182‧‧‧端子182‧‧‧ terminals
19‧‧‧電極19‧‧‧Electrode
BL‧‧‧藍光BL‧‧‧Blue
YL‧‧‧黃光YL‧‧‧Yuangguang
圖一係繪示根據本發明之一較佳具體實施例之白光半導體發光元件之截面視圖。BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a cross-sectional view showing a white light semiconductor light emitting device in accordance with a preferred embodiment of the present invention.
圖二係一截面視圖以示意地繪示根據本發明之白光半導體發光元件係以一覆晶接合方式進行封裝。2 is a cross-sectional view to schematically illustrate a white light semiconductor light emitting device according to the present invention packaged in a flip chip bonding manner.
圖三A為根據本發明之濾光層之模擬案例其濾光層的組成、各層材料的折射率以及各層的膜厚。Fig. 3A is a diagram showing the composition of the filter layer, the refractive index of each layer material, and the film thickness of each layer in the simulation case of the filter layer according to the present invention.
圖三B為模擬不同波長之入射光以0°、10°以及20°三個不同入射角度從GaN層射向圖三A所示ITO層、濾光層以及環氧樹脂的反射率。FIG. 3B is a graph showing the reflectance of the incident light of different wavelengths from the GaN layer to the ITO layer, the filter layer, and the epoxy resin shown in FIG. 3A at three different incident angles of 0°, 10°, and 20°.
圖三C為模擬由GaN基半導體發光元件所發出波長為455nm藍光之入射光以0°至90°的入射角度射向圖三A所示濾ITO層、濾光層以及環氧樹脂的反射率。Figure 3C is a graph showing the reflectance of the incident light of 455 nm blue light emitted from a GaN-based semiconductor light-emitting element at an incident angle of 0° to 90° toward the filtered ITO layer, the filter layer, and the epoxy resin shown in Fig. 3A. .
圖三D為模擬不同波長之入射光以0°、10°、20°、30°、以及40°四個不同入射角度從環氧樹脂射向圖三A所示濾光層、ITO層以及GaN層的反射率。Figure 3D is a simulation of different wavelengths of incident light from 0 °, 10 °, 20 °, 30 °, and 40 ° four different angles of incidence from the epoxy resin to the filter layer, ITO layer and GaN shown in Figure A The reflectivity of the layer.
圖三E為模擬由螢光粉所發出波長為570nm黃光之入射光以0°至90°的入射角度從環氧樹脂射向圖三A所示濾光層、ITO層以及GaN層的反射率。Fig. 3E is a graph showing the reflectance of the incident light of the 570 nm yellow light emitted by the phosphor from the epoxy resin toward the filter layer, the ITO layer and the GaN layer shown in Fig. 3A at an incident angle of 0° to 90°.
1...白光半導體發光元件1. . . White light semiconductor light emitting element
10...半導體疊層10. . . Semiconductor stack
102...基材102. . . Substrate
104...發光層104. . . Luminous layer
106...透明導電層106. . . Transparent conductive layer
108...出光面108. . . Glossy surface
12...濾光層12. . . Filter layer
14...透明封裝材料14. . . Transparent packaging material
16...波長轉換材料16. . . Wavelength conversion material
18...封裝基板18. . . Package substrate
182...端子182. . . Terminal
19...電極19. . . electrode
BL...藍光BL. . . Blue light
YL...黃光YL. . . Huang Guang
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| US6155699A (en) * | 1999-03-15 | 2000-12-05 | Agilent Technologies, Inc. | Efficient phosphor-conversion led structure |
| TW200618337A (en) * | 2004-05-26 | 2006-06-01 | Lumileds Lighting Llc | Semiconductor light emitting device including photonic band gap material and luminescent material |
| US7372078B2 (en) * | 2005-11-23 | 2008-05-13 | Samsung Electro-Mechanics Co., Ltd. | Vertical gallium-nitride based light emitting diode |
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| Publication number | Publication date |
|---|---|
| TW201117430A (en) | 2011-05-16 |
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