TWI676302B - Surface light source structure of light emitting diode - Google Patents

Surface light source structure of light emitting diode Download PDF

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Publication number
TWI676302B
TWI676302B TW107144754A TW107144754A TWI676302B TW I676302 B TWI676302 B TW I676302B TW 107144754 A TW107144754 A TW 107144754A TW 107144754 A TW107144754 A TW 107144754A TW I676302 B TWI676302 B TW I676302B
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Taiwan
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light
isolation
emitting diode
light emitting
layer
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TW107144754A
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Chinese (zh)
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TW202023071A (en
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黃文孝
Wen Hsiao Huang
林榮松
Jung Sung Lin
黃達人
Ta Jen Huang
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大陸商業成科技(成都)有限公司
Interface Technology (Chengdu) Co., Ltd.
大陸商業成光電(深圳)有限公司
Interface Optoelectronics (Shenzhen) Co., Ltd.
英特盛科技股份有限公司
General Interface Solution Limited
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21KNON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
    • F21K9/00Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
    • F21K9/20Light sources comprising attachment means
    • F21K9/23Retrofit light sources for lighting devices with a single fitting for each light source, e.g. for substitution of incandescent lamps with bayonet or threaded fittings
    • F21K9/238Arrangement or mounting of circuit elements integrated in the light source
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21KNON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
    • F21K9/00Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
    • F21K9/60Optical arrangements integrated in the light source, e.g. for improving the colour rendering index or the light extraction
    • F21K9/64Optical arrangements integrated in the light source, e.g. for improving the colour rendering index or the light extraction using wavelength conversion means distinct or spaced from the light-generating element, e.g. a remote phosphor layer
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21KNON-ELECTRIC LIGHT SOURCES USING LUMINESCENCE; LIGHT SOURCES USING ELECTROCHEMILUMINESCENCE; LIGHT SOURCES USING CHARGES OF COMBUSTIBLE MATERIAL; LIGHT SOURCES USING SEMICONDUCTOR DEVICES AS LIGHT-GENERATING ELEMENTS; LIGHT SOURCES NOT OTHERWISE PROVIDED FOR
    • F21K9/00Light sources using semiconductor devices as light-generating elements, e.g. using light-emitting diodes [LED] or lasers
    • F21K9/60Optical arrangements integrated in the light source, e.g. for improving the colour rendering index or the light extraction
    • F21K9/69Details of refractors forming part of the light source
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21YINDEXING SCHEME ASSOCIATED WITH SUBCLASSES F21K, F21L, F21S and F21V, RELATING TO THE FORM OR THE KIND OF THE LIGHT SOURCES OR OF THE COLOUR OF THE LIGHT EMITTED
    • F21Y2115/00Light-generating elements of semiconductor light sources
    • F21Y2115/10Light-emitting diodes [LED]

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Optics & Photonics (AREA)
  • General Engineering & Computer Science (AREA)
  • Led Device Packages (AREA)

Abstract

本發明揭露一種發光二極體面光源結構,其包含:一電路板、一發光二極體陣列,設置於該電路板上,具有複數個發光二極體單元、一第一隔離層,完整覆蓋該發光二極體陣列,並具有一第一隔離高度及一第一隔離厚度、一發光轉換層,完整覆蓋該第一隔離層,並具有一發光轉換層高度及一發光轉換層厚度,以及一第二隔離層,完整覆蓋該發光轉換層,並具有一第二隔離高度、一第二隔離厚度及一表面微結構。The invention discloses a light emitting diode surface light source structure, which includes: a circuit board and a light emitting diode array, which are arranged on the circuit board, have a plurality of light emitting diode units, and a first isolation layer, and completely cover the light emitting diode unit. The light-emitting diode array has a first isolation height and a first isolation thickness, a light-emitting conversion layer that completely covers the first isolation layer, and has a light-emitting conversion layer height and a light-emitting conversion layer thickness, and a first Two isolation layers completely cover the light-emitting conversion layer, and have a second isolation height, a second isolation thickness, and a surface microstructure.

Description

發光二極體面光源結構Light emitting diode decent light source structure

本發明涉及一種直下式發光二極體面光源結構。The invention relates to a direct type light emitting diode surface light source structure.

發光二極體面光源結構根據發光二極體光源位置可分成側光式與直下式兩種,前者多適用於小型顯示面板中,例如:監視器或筆記型電腦,後者多適用於大型顯示面板中,例如:液晶螢幕。本發明主要揭露一種適用於直下式的發光二極體面光源結構,然而,現今直下式發光二極體面光源結構,主要分為塗佈封裝及薄膜封裝兩種封裝型式,下文中將針對此兩種封裝形式進行優缺點比較。The structure of the light emitting diode surface light source can be divided into two types of edge light type and direct type according to the position of the light emitting diode light source. The former is mostly suitable for small display panels, such as monitors or notebook computers, and the latter is mostly suitable for large display panels. , For example: LCD screen. The present invention mainly discloses a light-emitting diode decent light source structure suitable for a direct-type light-emitting diode. However, the current direct-type light-emitting diode decent-light source structure is mainly divided into two types of packaging: coating package and thin-film packaging. Compare the advantages and disadvantages of the package.

習知的發光二極體面光源塗佈封裝,首先先將發光二極體陣列設置於電路板上,接著將發光轉換層塗佈並完全覆蓋發光二極體陣列,其中該發光轉換層的材料可選自釔鋁石榴石 (YAG)、矽酸鹽或氟化物螢光粉等螢光材料,此種封裝方式封裝過程簡單,且封裝成本與光轉換效率都高於薄膜封裝方式,但搭配液晶螢幕使用時,其NTSC色域覆蓋率僅達80~85%。In the conventional light emitting diode surface light source coating and packaging, first, the light emitting diode array is first set on a circuit board, and then the light emitting conversion layer is coated and completely covers the light emitting diode array. The material of the light emitting conversion layer can be It is selected from fluorescent materials such as yttrium aluminum garnet (YAG), silicate or fluoride phosphor. This packaging method has a simple packaging process, and the packaging cost and light conversion efficiency are higher than the thin film packaging method, but with a liquid crystal screen When used, its NTSC color gamut coverage is only 80 ~ 85%.

習知的發光二極體面光源薄膜封裝,首先將發光二極體陣列設置於電路板上,接著將事先製程好的發光轉換層薄膜覆蓋於發光二極體陣列上,其中發光轉換層薄膜可使用如上所述的螢光材料,亦可使用量子點螢光材料,當使用量子點螢光材料時,因量子點螢光材料容易受溫度與濕度的影像進而喪失轉換功效,故需在發光轉換層薄膜周圍再製程一隔離層以保護量子點螢光材料不受損壞,此種封裝方式,因量子點螢光材料可提供較窄頻的原色光(R/G/B),故搭配液晶螢幕使用時,其NTSC色域覆蓋率可達100%以上,但在此面光源的邊緣處卻呈現漏光現象,需而外在此面光源機構上增加遮光機構,因此可知薄膜封裝方式容易造成能量的浪費。In the conventional light emitting diode surface light source film packaging, the light emitting diode array is first set on a circuit board, and then the light emitting conversion layer film prepared in advance is covered on the light emitting diode array, and the light emitting conversion layer film can be used. The fluorescent material described above can also be a quantum dot fluorescent material. When a quantum dot fluorescent material is used, the quantum dot fluorescent material is easily affected by the temperature and humidity images and thus loses the conversion effect. An isolation layer is manufactured around the film to protect the quantum dot fluorescent material from damage. This packaging method, because the quantum dot fluorescent material can provide a narrower band of primary color light (R / G / B), so it is used with the LCD screen At this time, its NTSC color gamut coverage can reach more than 100%, but light leakage occurs at the edge of the surface light source. It is necessary to add a light shielding mechanism to the surface light source mechanism, so it can be seen that the thin film packaging method is likely to cause waste of energy. .

因此,欲解決上述現今發光二極體之封裝方式的問題與缺失,本發明提出一種新的結構設計,利用次毫米發光二極體(Mini LED)在超低電流(小於0.1mA)驅動,發光二極體陣列產生極低的熱特性,進一步提出此結構設計,但本發明不應僅限於此,亦可適用於發光二極體、次毫米發光二極體(Mini LED)或微型發光二極體(Micro LED)。Therefore, in order to solve the above-mentioned problems and shortcomings of the packaging methods of light-emitting diodes, the present invention proposes a new structural design that uses sub-millimeter light-emitting diodes (Mini LEDs) to drive and emit light at ultra-low current (less than 0.1 mA). Diode arrays generate extremely low thermal characteristics, and this structure design is further proposed, but the invention should not be limited to this, but can also be applied to light-emitting diodes, sub-millimeter light-emitting diodes (Mini LEDs), or miniature light-emitting diodes. Body (Micro LED).

本發明提出 一種發光二極體面光源結構,其包含:電路板、發光二極體陣列,設置於該電路板上,具有複數個發光二極體單元、第一隔離層,完整覆蓋發光二極體陣列,並具有第一隔離高度及第一隔離厚度、發光轉換層,完整覆蓋第一隔離層,並具有發光轉換層高度及發光轉換層厚度,以及第二隔離層,完整覆蓋發光轉換層,並具有第二隔離高度、第二隔離厚度及表面微結構。The invention provides a light emitting diode surface light source structure, which includes a circuit board and a light emitting diode array. The light emitting diode unit is provided on the circuit board and has a plurality of light emitting diode units and a first isolation layer, which completely cover the light emitting diode. An array, having a first isolation height, a first isolation thickness, and a light-emitting conversion layer, completely covering the first isolation layer, and having a light-emitting conversion layer height and a light-emitting conversion layer thickness, and a second isolation layer, completely covering the light-emitting conversion layer, and It has a second isolation height, a second isolation thickness and a surface microstructure.

其中第一隔離高度、第二隔離高度及發光轉換層高度的高度定義為與電路板垂直的方向,而第一隔離厚度、第二隔離厚度及發光轉換層厚度的厚度定義為與電路板水平的方向。The height of the first isolation height, the second isolation height, and the light-emitting conversion layer height is defined as a direction perpendicular to the circuit board, and the thicknesses of the first isolation thickness, the second isolation thickness, and the light-emitting conversion layer thickness are defined as being horizontal to the circuit board. direction.

較佳者,第一隔離厚度需大於或等於第一隔離高度。Preferably, the first isolation thickness needs to be greater than or equal to the first isolation height.

較佳者,第二隔離厚度需大於或等於第二隔離高度。Preferably, the second isolation thickness needs to be greater than or equal to the second isolation height.

較佳者,發光轉換層厚度大約等(≒)於該發光轉換層高度。Preferably, the thickness of the light-emitting conversion layer is approximately equal to (i) the height of the light-emitting conversion layer.

較佳者,表面微結構為棱鏡、透鏡或錐體結構等,透過此微結構透過光折射原理可進一步將發散的角度較大的光,修正其光路徑俾使收斂聚集,進而獲得光強度更高的光源。Preferably, the surface microstructure is a prism, lens, or cone structure, etc. Through this microstructure, the principle of light refraction can further diverge light with a larger divergence angle, correct its light path, and converge to converge, thereby obtaining more light intensity. High light source.

較佳者,發光轉換層的折射率為n qPreferably, the refractive index of the light-emitting conversion layer is n q .

較佳者,第一隔離層與第二隔離層可由至少一層子隔離層堆疊形成,然而,該子隔離層由內而外其折射率依序為n 1、n 2、n 3、…、n N,其中N為自然數,應符合1 ≦ n 1≦ n 2≦ n 3≦ … ≦n N≦ n qPreferably, the first isolation layer and the second isolation layer may be formed by stacking at least one sub-isolation layer. However, the refractive index of the sub-isolation layer is n 1 , n 2 , n 3 , ..., n from the inside to the outside. N , where N is a natural number, and should meet 1 ≦ n 1 ≦ n 2 ≦ n 3 ≦… ≦ n N ≦ n q .

透過上述結構設計可更充分利用發光二極體的光能並提升光的轉換率,且減少漏光現象避免光能量的浪費。Through the above structural design, the light energy of the light emitting diode can be more fully used and the light conversion rate can be improved, and the light leakage phenomenon can be reduced to avoid waste of light energy.

為達成上述目的及功效,本發明所採用之技術手段及構造,茲繪圖就本發明實施例詳加說明其特徵與功能,可誇大塗層和範圍的尺寸,俾利完全了解 ,但應理解的是,該等內容不夠成本發明的限定。In order to achieve the above-mentioned objects and effects, the technical means and structure adopted in the present invention, the features and functions of the embodiments of the present invention are described in detail in the drawings, and the size of the coating and range can be exaggerated. Yes, such content is not sufficient to qualify the invention.

參考圖1,為根據本發明實施例發光二極體面光源結構的示意圖,發光二極體面光源結構可依序包含電路板100、發光二極體陣列110、第一隔離層130a、發光轉換層 120及第二隔離層130b。發光二極體陣列110設置於電路板100之上,電路板100與第一隔離層130a之間,且被第一隔離層130a完全包覆;發光轉換層120設置於第一隔離層130a之上,第一隔離層130a與第二隔離層130b之間,其中第二隔離層130b設置於發光轉換層120上並完全覆蓋發光轉換層120,藉由將發光轉換層120夾於第一隔離層130a與第二隔離層130b之間以保護發光轉換層120免受溫溼度的影響。Referring to FIG. 1, a schematic diagram of a light emitting diode surface light source structure according to an embodiment of the present invention. The light emitting diode surface light source structure may include a circuit board 100, a light emitting diode array 110, a first isolation layer 130a, and a light emitting conversion layer 120 in this order. And the second isolation layer 130b. The light emitting diode array 110 is disposed on the circuit board 100, between the circuit board 100 and the first isolation layer 130a, and is completely covered by the first isolation layer 130a. The light emitting conversion layer 120 is disposed on the first isolation layer 130a. Between the first isolation layer 130a and the second isolation layer 130b, wherein the second isolation layer 130b is disposed on the light-emitting conversion layer 120 and completely covers the light-emitting conversion layer 120, and the light-emitting conversion layer 120 is sandwiched between the first isolation layer 130a And the second isolation layer 130b to protect the light emitting conversion layer 120 from the influence of temperature and humidity.

本發明可設置為一板體例如平面板體或可撓式板體等,本實施例以平面式結構做詳細說明,但不等於限制本發明精神與範疇。首先將發光二極體陣列110均勻設置於電路板100上,接著將第一隔離層130a塗佈並堆疊於發光二極體陣列110上且完全覆蓋,此第一隔離層130a具有第一隔離高度h a與第一隔離厚度s a,接著將發光轉換層120均勻塗佈並堆疊至第一隔離層130a上且完全覆蓋,此發光轉換層120具有發光轉換層高度h q與發光轉換層厚度s q,其中發光轉換層 120可選自釔鋁石榴石 (YAG)、矽酸鹽、氟化物螢光粉,或量子點螢光粉等螢光材料,最後將第二隔離層130b均勻塗佈並堆疊至發光轉換層120上且完全覆蓋,此第二隔離層130b具有第二隔離高度h b與第二隔離厚度s b,其中第一隔離層130a及第二隔離層130b可使用透明或高霧度(Haze)的材料。如上文所述,其製成方式可以狹縫塗佈、線棒塗佈、浸泡塗佈或旋轉塗佈等方式成形。 The present invention may be provided as a plate body such as a flat plate body or a flexible plate body. The embodiment is described in detail with a flat structure, but it does not limit the spirit and scope of the invention. Firstly, the light emitting diode array 110 is uniformly disposed on the circuit board 100, and then a first isolation layer 130a is coated and stacked on the light emitting diode array 110 and completely covered. The first isolation layer 130a has a first isolation height. h a and the first isolation thickness s a , and then the light-emitting conversion layer 120 is uniformly coated and stacked on the first isolation layer 130 a and completely covered. The light-emitting conversion layer 120 has a light-emitting conversion layer height h q and a light-emitting conversion layer thickness s. q , wherein the light emitting conversion layer 120 may be selected from fluorescent materials such as yttrium aluminum garnet (YAG), silicate, fluoride phosphor, or quantum dot phosphor, and finally the second isolation layer 130b is uniformly coated and stack 120 to the luminescence conversion layer and completely covers, the second spacer a second spacer layer 130b having a height h b of the second spacer thickness s b, wherein the first release layer 130a and the second spacer layer 130b may be transparent or high haze Haze material. As mentioned above, it can be made by slit coating, wire rod coating, dip coating or spin coating.

第一隔離高度h a定義為從電路板100表面到第一隔離層130a與發光轉換層120接觸面的垂直高度,發光轉換層高度h q定義為從第一隔離層130a與發光轉換層120接觸面到發光轉換層120與第二隔離層130b接觸面的垂直高度,而第二隔離高度h b定義為發光轉換層120與第二隔離層130b接觸面到第二隔離層130b的頂表面的垂直高度。 The first isolation height h a is defined as the vertical height from the surface of the circuit board 100 to the contact surface between the first isolation layer 130 a and the light-emitting conversion layer 120, and the light-emitting conversion layer height h q is defined as the contact from the first isolation layer 130 a to the light-emitting conversion layer 120. surface to the contact surface 130b of the vertical height of the second spacer layer 120 and the luminescence conversion layer, and a second spacer height h b is defined as the luminescence conversion layer 120 and the contact surface of the second spacer layer 130b to a top surface of the second spacer layer 130b are perpendicular height.

第一隔離厚度s a定義為從邊緣的發光二極體陣列110邊緣側到第一隔離層130a與發光轉換層120接觸面的水平厚度,發光轉換層厚度s q定義為從第一隔離層130a與發光轉換層120接觸面到發光轉換層120與第二隔離層130b接觸面的水平厚度,而第二隔離厚度s b定義為發光轉換層120與第二隔離層130b接觸面到第二隔離層130b的邊緣側的水平厚度。 The first isolation thickness s a is defined as the horizontal thickness from the edge of the edge of the light emitting diode array 110 to the contact surface between the first isolation layer 130 a and the light emitting conversion layer 120, and the light emission conversion layer thickness s q is defined as being from the first isolation layer 130 a and the contact surface 120 to the light emitting luminescence conversion layer 120 and the conversion layer 130b in contact with the horizontal surface of the second spacer layer thickness, the second thickness of the barrier is defined as s b luminescence conversion layer 120 and the contact surface of the second spacer layer 130b to the second spacer layer The horizontal thickness of the edge side of 130b.

第一隔離厚度s a需大於或等於第一隔離高度h a,且第二隔離厚度s b需大於或等於第二隔離高度h b,其主要目的為防止面光源的邊緣聚光或過亮。發光轉換層厚度s q需大約等於(≒)發光轉換層高度h q,為防止發光轉換層120受溫度與濕度的影響,第一隔離高度h a與第二隔離高度h b需大於30µm才具有隔離效果,然而第一隔離層130a與第二隔離層130b的高度(h a、h b)或厚度(s a、s b)其越薄穿透率越佳。 The first isolation thickness s a must be greater than or equal to the first isolation height h a , and the second isolation thickness s b must be greater than or equal to the second isolation height h b . Its main purpose is to prevent the edge of the surface light source from condensing or being too bright. The thickness of the light-emitting conversion layer s q needs to be approximately equal to (≒) the height of the light-emitting conversion layer h q . In order to prevent the light-emitting conversion layer 120 from being affected by temperature and humidity, the first isolation height h a and the second isolation height h b must be greater than 30 μm. Isolation effect, however, the thinner the first isolation layer 130a and the second isolation layer 130b are (h a , h b ) or thickness (s a , s b ), the thinner the better the transmittance.

參考圖2(a) 、圖2(b)與圖2(c),為本發明另一實施例發光二極體面光源結構之表面微結構240的示意圖。承如上述實施例之特徵,本實施例進一步在第二隔離層230b的頂表面上加工為至少一表面突出物,表面突出物可為如:棱鏡、透鏡或錐體等表面微結構240,或上述結構之組合,藉由此表面微結構240,以修正光路徑俾使光收斂聚集的效果,進而獲得光強度更高的光源,其中本發明的表面微結構240其排列方式可為規則排列或 隨機亂數排列。應理解的是,本發明實施例的圖示僅為使所屬領域具通常知識者能更加清楚明白本發明的精神與範疇,不應僅限於此。Referring to FIG. 2 (a), FIG. 2 (b), and FIG. 2 (c), it is a schematic diagram of a surface microstructure 240 of a light emitting diode planar light source structure according to another embodiment of the present invention. Following the features of the above embodiment, this embodiment further processes at least one surface protrusion on the top surface of the second isolation layer 230b. The surface protrusion may be a surface microstructure 240 such as a prism, a lens, or a cone, or The combination of the above structures uses the surface microstructures 240 to modify the effect of the light path and converge the light, thereby obtaining a light source with higher light intensity. The surface microstructures 240 of the present invention can be arranged regularly or Random random numbers. It should be understood that the illustrations of the embodiments of the present invention are only for those skilled in the art to understand the spirit and scope of the present invention more clearly, and should not be limited to this.

本發明提出另一實施例,依據菲涅耳方程式(fresnel equation)當光入射角趨近於零時,其光的穿透率符合4n 1n 2/( n 1+n 2) 2×100%,例如:光從空氣(折射率為1)中入射至玻璃(折射率約為1.5),根據菲涅耳方程式4×1×1.5/(1+1.5) 2×100%=96%可得其穿透率為96%,倘若在玻璃外層塗佈一折射率為1.2的薄膜,根據菲涅耳方程式4×1×1.2/(1+1.2) 2×4×1.2×1.5/(1.2+1.5) 2×100%≒98%可獲的最終穿透率為98%,故由此可知,塗佈一薄膜於外層可有效提升穿透率的效果。 The present invention proposes another embodiment. According to the Fresnel equation, when the incident angle of light approaches zero, the light transmittance thereof conforms to 4n 1 n 2 / (n 1 + n 2 ) 2 × 100%. For example: light enters glass (refractive index is about 1.5) from air (refractive index is 1), according to Fresnel equation 4 × 1 × 1.5 / (1 + 1.5) 2 × 100% = 96% The transmittance is 96%. If a thin film with a refractive index of 1.2 is applied to the outer layer of glass, according to the Fresnel equation 4 × 1 × 1.2 / (1 + 1.2) 2 × 4 × 1.2 × 1.5 / (1.2 + 1.5) The final transmittance obtained from 2 × 100% to 98% is 98%, so it can be known that coating a thin film on the outer layer can effectively improve the transmittance effect.

綜合上述,為提升光轉換效率,提升光穿透率為必要的課題,進一步參考圖3,為本發明另一實施例發光二極體面光源結構之示意圖,承如上述實施例之特徵,本實施例的第一隔離層330a及第二隔離層330b可進一步由至少一子隔離層堆疊形成。由圖所示,第一隔離層330a包含至少一第一子隔離層且由內而外為依序為331a、332a…、33Na,而第二隔離層330b包含至少一第二子隔離層且由內而外為依序為331b、332b…、33Nb,其中N為自然數。To sum up, in order to improve the light conversion efficiency and the problem of improving the light transmittance, further reference is made to FIG. 3, which is a schematic diagram of a light emitting diode decent light source structure according to another embodiment of the present invention. The first isolation layer 330a and the second isolation layer 330b may be further formed by stacking at least one sub-isolation layer. As shown in the figure, the first isolation layer 330a includes at least one first sub-isolation layer and is 331a, 332a ..., 33Na in order from the inside to the outside, and the second isolation layer 330b includes at least one second sub-isolation layer and is formed from the inside. The outer numbers are 331b, 332b ..., 33Nb in order, where N is a natural number.

為提升光轉換效率,當發光轉換層320其折射率為n q時,第一子隔離層331a、332a…、33Na與第二子隔離層331b、332b…、33Nb其折射率依序為n 1、n 2、n 3、…、n N,其中N為自然數,且折射率必須符合1≦n 1≦ n 2≦ n 3≦ … ≦n N≦ n q。藉由此結構設計,可使得較多光能量穿透發光轉換層320進而提升發光二極體面光源的發光效率。 In order to improve the light conversion efficiency, when the refractive index of the light-emitting conversion layer 320 is nq , the refractive indices of the first sub-isolation layers 331a, 332a ..., 33Na and the second sub-isolation layers 331b, 332b ..., 33Nb are sequentially n 1 , N 2 , n 3 , ..., n N , where N is a natural number, and the refractive index must conform to 1 ≦ n 1 ≦ n 2 ≦ n 3 ≦… ≦ n N ≦ n q . With this structure design, more light energy can be transmitted through the light-emitting conversion layer 320 and the light-emitting efficiency of the light-emitting diode surface light source is improved.

透過上述之詳細說明,即可充分顯示本發明之目的及功效,以上所述僅為清楚說明本發明的精神與範疇,並非限制本發明,因此本領域具通常知識者應理解的是凡運用到本發明說明書及圖示內容所做出等同替換和顯而易見的變化,均包含在本發明的保護範圍內。Through the above detailed description, the object and effect of the present invention can be fully displayed. The above is only for clearly explaining the spirit and scope of the present invention, and does not limit the present invention. Therefore, those with ordinary knowledge in the art should understand that Equivalent substitutions and obvious changes made in the description and illustrated contents of the present invention are included in the protection scope of the present invention.

100、200、300‧‧‧電路板100, 200, 300‧‧‧ circuit boards

110、210、310‧‧‧發光二極體陣列110, 210, 310‧‧‧‧ Light Emitting Diode Array

120、220、320‧‧‧發光轉換層120, 220, 320‧‧‧‧ Luminous Conversion Layer

130a、230a、330a‧‧‧第一隔離層130a, 230a, 330a ‧‧‧ the first isolation layer

130b、230b、330a‧‧‧第二隔離層130b, 230b, 330a‧‧‧Second isolation layer

240‧‧‧表面微結構240‧‧‧ surface microstructure

331a、…、33Na‧‧‧第一子隔離層331a, ..., 33Na‧‧‧The first sub-isolation layer

331b、…、33Nb‧‧‧第二子隔離層331b, ..., 33Nb‧‧‧Second Sub-Isolation Layer

圖1,為本發明實施例發光二極體面光源結構的示意圖。FIG. 1 is a schematic diagram of a light emitting diode surface light source structure according to an embodiment of the present invention.

圖2(a) 、圖2(b)與圖2(c),為本發明另一實施例發光二極體面光源結構之表面微結構的示意圖。FIG. 2 (a), FIG. 2 (b), and FIG. 2 (c) are schematic diagrams of surface microstructures of a light emitting diode planar light source structure according to another embodiment of the present invention.

圖3,為本發明另一實施例發光二極體面光源結構之示意圖。FIG. 3 is a schematic diagram showing a structure of a light emitting diode surface light source according to another embodiment of the present invention.

Claims (9)

一種發光二極體面光源結構,其包含:一電路板;一發光二極體陣列,設置於該電路板上,具有複數個發光二極體單元;一第一隔離層,完整覆蓋該發光二極體陣列,並具有一第一隔離高度及一第一隔離厚度,其中該第一隔離厚度需大於或等於該第一隔離高度;一發光轉換層,完整覆蓋該第一隔離層,並具有一發光轉換層高度及一發光轉換層厚度;以及一第二隔離層,完整覆蓋該發光轉換層,並具有一第二隔離高度、一第二隔離厚度及一表面微結構。A light emitting diode surface light source structure includes: a circuit board; a light emitting diode array disposed on the circuit board and having a plurality of light emitting diode units; a first isolation layer completely covering the light emitting diode A body array having a first isolation height and a first isolation thickness, wherein the first isolation thickness needs to be greater than or equal to the first isolation height; a light-emitting conversion layer that completely covers the first isolation layer and has a light emission The height of the conversion layer and the thickness of a light-emitting conversion layer; and a second isolation layer that completely covers the light-emitting conversion layer, and has a second isolation height, a second isolation thickness, and a surface microstructure. 如申請專利範圍第1項所述之發光二極體面光源結構,其中該第一隔離高度、該第二隔離高度及該發光轉換層高度的高度定義為與該電路板垂直的方向,且該第一隔離厚度、該第二隔離厚度及該發光轉換層厚度的厚度定義為與該電路板水平的方向。The light emitting diode surface light source structure described in item 1 of the scope of the patent application, wherein the height of the first isolation height, the second isolation height, and the height of the light-emitting conversion layer is defined as a direction perpendicular to the circuit board, and the first A thickness of an isolation thickness, the second isolation thickness, and the thickness of the light-emitting conversion layer is defined as a direction horizontal to the circuit board. 如申請專利範圍第2項所述之發光二極體面光源結構,其中該第二隔離厚度需大於或等於該第二隔離高度。According to the light emitting diode decent light source structure described in item 2 of the scope of the patent application, the second isolation thickness needs to be greater than or equal to the second isolation height. 如申請專利範圍第2項所述之發光二極體面光源結構,其中該發光轉換層厚度等於該發光轉換層高度。The light emitting diode surface light source structure described in item 2 of the scope of the patent application, wherein the thickness of the light emitting conversion layer is equal to the height of the light emitting conversion layer. 如申請專利範圍第1項所述之發光二極體面光源結構,其中該表面微結構為表面突出物,用以修正光路徑俾使光收斂聚集的效果。According to the light emitting diode surface light source structure described in item 1 of the scope of the patent application, wherein the surface microstructure is a surface protrusion, which is used to modify the effect of the light path and converge the light. 如申請專利範圍第1項所述之發光二極體面光源結構,其中該發光轉換層的折射率為nqAccording to the light emitting diode surface light source structure described in item 1 of the patent application scope, wherein the refractive index of the light emitting conversion layer is n q . 如申請專利範圍第2項所述之發光二極體面光源結構,其中該第一隔離層由至少一第一子隔離層堆疊形成。The light emitting diode surface light source structure described in item 2 of the patent application scope, wherein the first isolation layer is formed by stacking at least one first sub-isolation layer. 如申請專利範圍第2項所述之發光二極體面光源結構,其中該第二隔離層由至少一第二子隔離層堆疊形成。According to the light emitting diode decent light source structure described in item 2 of the patent application scope, wherein the second isolation layer is formed by stacking at least one second sub-isolation layer. 如申請專利範圍第8項或第9項所述之發光二極體面光源結構,其中該子隔離層由內而外其折射率依序為n1、n2、n3、...、nN,其中N為自然數,且符合1≦n1≦n2≦n3≦...≦nN≦nqAccording to the light emitting diode surface light source structure described in item 8 or item 9 of the scope of patent application, wherein the sub-isolation layer has an index of refraction in order from n 1 , n 2 , n 3 , ..., n N , where N is a natural number, and conforms to 1 ≦ n 1 ≦ n 2 ≦ n 3 ≦ ... ≦ n N ≦ n q .
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