TW201616044A - Optical component and illumination apparatus having the optical component - Google Patents

Optical component and illumination apparatus having the optical component Download PDF

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TW201616044A
TW201616044A TW103137423A TW103137423A TW201616044A TW 201616044 A TW201616044 A TW 201616044A TW 103137423 A TW103137423 A TW 103137423A TW 103137423 A TW103137423 A TW 103137423A TW 201616044 A TW201616044 A TW 201616044A
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light
concave
region
microstructures
optical component
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TW103137423A
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TWI548838B (en
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魏志銘
張秦溢
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東莞雷笛克光學有限公司
揚州雷笛克光學有限公司
雷笛克光學股份有限公司
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Abstract

An optical component and illumination apparatus having the optical component are described. The optical component includes a main body, an incident surface and light-emitting surface. The main body forms a recess space in the bottom portion of the main body. The incident surface is defined by the recess space for being issued by an incident light and includes an annular region having at least a plurality of micro-structures thereon wherein each of the micro-structures includes a camber surface. The light-emitting surface is formed on the outer surface of the main body wherein a bottom edge of the outer surface is adjacent to an outer edge of the bottom portion of the main body. The present invention is capable of eliminating the yellow ring effect, increasing the light utilization rate and solving the problem of central light spot.

Description

光學元件及具有該光學元件之照明裝置 Optical element and illuminating device having the same

本發明係有關於一種光學元件及具有該光學元件之照明裝置,特別是指入光表面設有微結構的光學元件及具有該光學元件之照明裝置。 The present invention relates to an optical element and an illumination device having the same, and in particular to an optical element having a microstructure on a light incident surface and an illumination device having the same.

隨著發光二極體(light-emitted diode,LED)電視的背光模組不斷朝向大尺寸、重量輕、厚度薄以及高性能等等的各種需求,如何進一步提升這些設計需求已成為近年來LED電視背光模組發展的新趨勢。目前,當LED背光模組使用的發光二極體含有螢光粉時以及因為LED很接近擴散板,在光線通過背光透鏡而容易於擴散板產生不均勻的成像並且產生黃圈現象,影響電視的顯示品質。 With the backlight module of light-emitted diode (LED) TV constantly facing various demands of large size, light weight, thin thickness and high performance, how to further enhance these design requirements has become LED TV in recent years. A new trend in the development of backlight modules. At present, when the LEDs used in the LED backlight module contain phosphor powder and because the LEDs are very close to the diffusion plate, the light passes through the backlight lens, which is easy to produce uneven imaging of the diffusion plate and cause a yellow circle phenomenon, which affects the television. Display quality.

如第1圖所示,在習知技術之背光透鏡100中,為解決上述的問題,發光孔102是由單一曲面104來改變LED 106光線的反射以及折射,通常下半段103的發光孔102係為直升(陡升)形狀(即斜率較大),使偏黃的光線105往背光透鏡100的兩側而向目標投射區域之外的方向打出去,以減少黃圈的問題;雖然上述方式可解決一部分黃圈的效應,但偏黃的光線105往外投射時將會造成一部分光線的浪費。再者,背光模組大都排列多個LED, 同時需要搭配多個背光透鏡100,因此,這些被直接打出去偏黃的光線105可能影響其他背光透鏡的目標投射區域的光斑,從而可能造成其光斑的色度不均勻。此外,下半段103的發光孔102係為直升狀態,一部分的光線打到發光孔102的側壁反射之後,直接朝向發光孔102的頂部110穿過去而造成成像的光斑會有中心亮點,必須額外將出光表面的中心作成凹面108來避免中心亮點,需要較高的成本以及較複雜的製程步驟。 As shown in FIG. 1, in the backlight lens 100 of the prior art, in order to solve the above problem, the illuminating aperture 102 changes the reflection and refraction of the light of the LED 106 by a single curved surface 104, usually the illuminating aperture 102 of the lower half 103. The shape is a straight (sudden) shape (ie, the slope is large), and the yellowish light 105 is directed toward the sides of the backlight lens 100 to the direction outside the target projection area to reduce the problem of the yellow circle; The way to solve the effect of a part of the yellow circle, but the yellowish light 105 will cause a part of the light to be thrown when it is projected outward. Furthermore, the backlight modules are mostly arranged with a plurality of LEDs. At the same time, a plurality of backlight lenses 100 need to be matched. Therefore, the light rays 105 that are directly yellowed out may affect the spot of the target projection area of the other backlight lenses, which may cause unevenness of the chromaticity of the spot. In addition, the illuminating hole 102 of the lower half 103 is in a straight state, and a part of the light is reflected by the side wall of the illuminating hole 102, and directly passes toward the top 110 of the illuminating hole 102, so that the image spot has a central bright spot, and must be The center of the light-emitting surface is additionally made into a concave surface 108 to avoid the central bright spot, which requires high cost and complicated process steps.

因此需要發展一種新式的光學元件以及照明裝置以解決上述問題。 Therefore, there is a need to develop a new type of optical component and illumination device to solve the above problems.

本發明之一目的在於提供一種光學元件及具有此光學元件之照明裝置,藉由至少在入光表面的環形上設有複數個具有弧面的微結構,以減少黃圈現象、提升光線利用率並且解決光學元件造成中心亮點的問題。 An object of the present invention is to provide an optical component and an illumination device having the same, which are provided with a plurality of microstructures having a curved surface at least on the ring of the light-incident surface to reduce the yellow circle phenomenon and improve light utilization efficiency. And solve the problem that the optical component causes the central highlight.

為達成上述目的,本發明之一較佳實施例提供一種光學元件,包括:本體,該本體的底部形成一凹型空間;入光表面,係由該本體的該凹型空間所定義,以供一光線入射,並且該入光表面具有一環形區域,其中該入光表面至少在該環形區域上設有複數個微結構,每一該些微結構具有一弧面;以及出光表面,形成於該本體的外表面,其中該外表面的底緣鄰接該本體的底部的外緣。 In order to achieve the above object, a preferred embodiment of the present invention provides an optical component comprising: a body, a bottom portion of the body forming a concave space; and a light incident surface defined by the concave space of the body for providing a light Injecting, and the light incident surface has an annular region, wherein the light incident surface is provided with at least a plurality of microstructures on the annular region, each of the microstructures having a curved surface; and a light emitting surface formed outside the body a surface, wherein a bottom edge of the outer surface abuts an outer edge of the bottom of the body.

在一實施例中,每一該些微結構係由該本體朝向該凹型空間凹陷或是凸出而形成。 In one embodiment, each of the microstructures is formed by the body being recessed or convex toward the concave space.

在一實施例中,每一該些微結構的該弧面係由每一該些微結 構在該本體與該凹型空間之間的交界面所定義,並且在該交界面處的任一該些微結構的弧面高度表示為H,在該交界面處的任一該些微結構的弧面寬度表示為W,其中0.01毫米≦H≦0.2毫米,且0.01毫米≦W≦0.8毫米。 In an embodiment, the arc of each of the microstructures is formed by each of the microjunctions Constructed at the interface between the body and the concave space, and the arcuate height of any of the microstructures at the interface is denoted H, and the curved surface of any of the microstructures at the interface The width is expressed as W, where 0.01 mm ≦ H ≦ 0.2 mm, and 0.01 mm ≦ W ≦ 0.8 mm.

在一實施例中,每一該些微結構的該弧面係由每一該些微結構在該本體與該凹型空間之間的交界面所定義,並且在該交界面的任一該些微結構的弧面高度H除以該任一該些微結構的弧面寬度W的比值表示為R,其中0.003≦R≦1.2。 In one embodiment, the arc of each of the microstructures is defined by an interface of each of the microstructures between the body and the concave space, and any of the microstructured arcs at the interface The ratio of the face height H divided by the arcuate width W of any of the microstructures is expressed as R, where 0.003 ≦ R ≦ 1.2.

在一實施例中,該些微結構從該凹型空間觀之係為複數個同心圓形狀。 In one embodiment, the microstructures are a plurality of concentric circles from the concave space.

在一實施例中,該些微結構係為格紋狀。 In one embodiment, the microstructures are latticed.

在一實施例中,該些微結構在該入光表面上係為規則排列或是不規則排列。 In an embodiment, the microstructures are regularly arranged or irregularly arranged on the light incident surface.

在一實施例中,該凹型空間具有一開口,以通過該開口口緣的平面定義為基準面,相對於該基準面位在同一高度位置的任一該些微結構具有相同的幾何結構。 In one embodiment, the concave space has an opening defined by the plane of the opening rim as a reference plane, and any of the microstructures at the same height position relative to the reference plane has the same geometry.

在一實施例中,該凹型空間具有一開口,以該開口口緣的幾何中心定義為基準點,以通過該開口口緣的平面定義為基準面,以通過該基準點並垂直該基準面的直線定義為基準軸,以通過該基準軸的一平面定義為截面,在該截面上以該基準軸劃分該入光表面形成一第一區域及一第二區域,在該第一區域中具有該些微結構分布之處形成一微結構分布區段,該微結構分布區段的兩端中較接近該基準軸的一端定義為該第一端點,該第一端點與該基準點的連線與該基準面形成該些微結構的分布角度 θ,其中,20度≦θ≦90度。 In an embodiment, the concave space has an opening defined by a geometric center of the opening edge as a reference plane through a plane of the opening edge to pass the reference point and perpendicular to the reference surface A straight line is defined as a reference axis, and a plane passing through the reference axis is defined as a cross section, and the light incident surface is divided by the reference axis to form a first area and a second area, and the first area is included in the first area The microstructures are distributed to form a microstructure distribution section, and an end of the two ends of the microstructure distribution section that is closer to the reference axis is defined as the first endpoint, and the first endpoint is connected to the reference point. Forming the distribution angle of the microstructures with the reference plane θ, where 20 degrees ≦ θ ≦ 90 degrees.

在一實施例中,20度≦θ≦60度。 In one embodiment, 20 degrees ≦ θ ≦ 60 degrees.

在一實施例中,該微結構分布區段的兩端中較遠離該基準軸的一端定義為一第二端點,該第二端點沿著該基準軸的方向至該基準面的距離定義為HL,其中0毫米≦HL≦5毫米。 In one embodiment, an end of the two ends of the microstructure distribution section that is further away from the reference axis is defined as a second end point, and the distance of the second end point along the direction of the reference axis to the reference plane is defined. For H L , where 0 mm ≦ H L ≦ 5 mm.

在一實施例中,該凹型空間具有一開口,以該開口口緣的幾何中心定義為基準點,以通過該開口口緣的平面定義為基準面,以通過該基準點並垂直該基準面的直線定義為基準軸,以通過該基準軸的一平面定義為截面,在該截面上以該基準軸劃分該入光表面形成一第一區域及一第二區域,在該第一區域中具有該些微結構分布之處形成一微結構分布區段,該微結構分布區段首末兩端的連線與該基準面形成該些微結構的傾斜角度α,其中10度≦α≦80度。 In an embodiment, the concave space has an opening defined by a geometric center of the opening edge as a reference plane through a plane of the opening edge to pass the reference point and perpendicular to the reference surface A straight line is defined as a reference axis, and a plane passing through the reference axis is defined as a cross section, and the light incident surface is divided by the reference axis to form a first area and a second area, and the first area is included in the first area The microstructures are distributed to form a microstructure distribution section, and the line connecting the first and last ends of the microstructure distribution section forms an inclination angle α of the microstructures with the reference plane, wherein 10 degrees ≦α≦80 degrees.

在一實施例中,30度≦α≦60度。 In one embodiment, 30 degrees ≦ α ≦ 60 degrees.

在一實施例中,該凹型空間具有一開口,以該開口口緣的幾何中心定義為基準點,以通過該開口口緣的平面定義為基準面,以通過該基準點並垂直該基準面的直線定義為基準軸,該出表面在該基準軸與該出光表面相交處具有一平坦部。 In an embodiment, the concave space has an opening defined by a geometric center of the opening edge as a reference plane through a plane of the opening edge to pass the reference point and perpendicular to the reference surface The straight line is defined as a reference axis having a flat portion at the intersection of the reference axis and the light exiting surface.

在一實施例中,該平坦部為光滑表面。 In an embodiment, the flat portion is a smooth surface.

在一實施例中,該入光表面具有鄰接該環形區域的一凹形區域,且該環形區域與該凹形區域的交接處形成轉折,該環形區域較該凹形區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 In one embodiment, the light incident surface has a concave region adjacent to the annular region, and the intersection of the annular region and the concave region forms a turn, the annular region being closer to the bottom of the body than the concave region. The concave region is formed by the body recess.

在一實施例中,該凹形區域在與該環形區域的該交接處形成 一第一開口,且該環形區域較遠離該凹形區域處形成一第二開口,其中該環形區域的該第二開口大於該凹形區域的該第一開口。 In an embodiment, the concave region is formed at the intersection with the annular region a first opening, and the annular region forms a second opening away from the concave region, wherein the second opening of the annular region is larger than the first opening of the concave region.

在一實施例中,該入光表面具有鄰接該環形區域的一凹形區域,且該凹形區域為光滑表面,該環形區域較該凹形區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 In one embodiment, the light incident surface has a concave region adjacent to the annular region, and the concave region is a smooth surface, and the annular region is closer to the bottom of the body than the concave region, the concave region is The body is formed by being recessed.

在一實施例中,該入光表面具有鄰接該環形區域的一凹形區域,且該凹形區域為霧化表面,該環形區域較該凹形區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 In an embodiment, the light incident surface has a concave area adjacent to the annular area, and the concave area is an atomizing surface, and the annular area is closer to the bottom of the body than the concave area, and the concave area is Formed by the body recess.

在一實施例中,該凹型空間具有一開口,以通過該開口口緣的平面定義為基準面,該凹型空間的開口口緣的直徑為DI,該入光表面的高度為HI,其中0.2≦HI/DI≦3,該入光表面的高度HI為該入光表面上任一點沿著垂直該基準面的方向至該基準面的距離的最大值。 In an embodiment, the concave space has an opening defined by a plane defined by the opening edge as a reference surface, the opening edge of the concave space has a diameter D I , and the height of the light incident surface is H I , wherein 0.2 ≦ H I / D I ≦ 3, the height H I of the light incident surface is the maximum value of the distance from any point on the light incident surface along the direction perpendicular to the reference surface to the reference surface.

在一實施例中,該凹型空間具有一開口,以通過該開口口緣的平面定義為基準面,該凹型空間的開口口緣的直徑為DI,該入光表面的高度為HI,其中0.2≦HI/DI≦3,該入光表面的高度HI為該入光表面上任一點沿著垂直該基準面的方向至該基準面的距離的最大值。 In an embodiment, the concave space has an opening defined by a plane defined by the opening edge as a reference surface, the opening edge of the concave space has a diameter D I , and the height of the light incident surface is H I , wherein 0.2 ≦ H I / D I ≦ 3, the height H I of the light incident surface is the maximum value of the distance from any point on the light incident surface along the direction perpendicular to the reference surface to the reference surface.

在一實施例中,其中0.2≦HI/DI≦0.8。 In one embodiment, wherein 0.2 ≦H I /D I ≦ 0.8.

在一實施例中,該本體的底部具有一底面,該底面係自該入光表面的底緣向外延伸且與該出光表面直接或間接連接,該底面外緣的直徑為DO,該出光表面的高度為HO,其中0.2≦HO/DO≦0.8,該出光表面的高度HO為該出光表面上任一點沿著垂直該基準面的方向至該基準面的距離的最大值。 In one embodiment, the bottom of the body has a bottom surface extending outward from the bottom edge of the light incident surface and directly or indirectly connected to the light exit surface, the outer edge of the bottom surface having a diameter D O , the light output The height of the surface is H O , where 0.2 ≦ H O /D O ≦ 0.8, and the height H O of the light-emitting surface is the maximum value of the distance from any point on the light-emitting surface along the direction perpendicular to the reference surface to the reference surface.

在一實施例中,該凹型空間具有一開口,以通過該開口口緣的平面為基準面,該凹型空間的該開口口緣為非圓形,以該開口口緣上相距最遠的兩點的連線的方向為一第一方向,在該第一方向上該開口口緣兩側距離的最大值為第一方向寬度D1,以垂直該第一方向為一第二方向,在該第二方向上該開口口緣兩側距離的最大值為該開口口緣的第二方向寬度D2,該入光表面的高度為HI,其中0.2≦HI/D1≦3,0.2≦HI/D2≦3,該入光表面的高度HI為該入光表面上任一點沿著垂直該基準面的方向至該基準面的距離的最大值。 In an embodiment, the concave space has an opening such that a plane passing through the opening edge is a reference surface, and the opening edge of the concave space is non-circular, with two points farthest from the opening edge The direction of the connection is a first direction, and the maximum distance of the two sides of the opening edge in the first direction is a first direction width D 1 , and the first direction is a second direction perpendicular to the first direction. The maximum distance between the two sides of the opening edge in the two directions is the width D 2 of the opening edge in the second direction, and the height of the light incident surface is H I , where 0.2 ≦H I /D 1 ≦3, 0.2≦H I / D 2 ≦ 3, the height H I of the light incident surface is the maximum value of the distance from any point on the light incident surface along the direction perpendicular to the reference plane to the reference plane.

在一實施例中,該本體的該外表面包含一反射面,該反射面的底緣與該本體的底部的外緣鄰接,且該反射面的頂緣與該出光表面的外緣直接或間接連接。 In an embodiment, the outer surface of the body comprises a reflecting surface, the bottom edge of the reflecting surface is adjacent to the outer edge of the bottom of the body, and the top edge of the reflecting surface is directly or indirectly connected to the outer edge of the light emitting surface. connection.

在一實施例中,該入光表面具有鄰接該環形區域的一凹形區域、一凸形區域或一平坦區域三者之一,該環形區域較該凹形區域、該凸形區域或該平坦區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 In one embodiment, the light incident surface has one of a concave region, a convex region or a flat region adjacent to the annular region, the annular region being more planar than the concave region, the convex region or the flat region The region is adjacent to the bottom of the body, and the concave region is formed by the body recess.

在一實施例中,該本體的材質係為透明材質。 In an embodiment, the material of the body is a transparent material.

在一實施例中,這種照明裝置包括光學元件以及發光二極體,該發光二極體的發光面朝向該光學元件的該入光表面。在一實施例中,該發光二極體係為多晶發光二極體。 In an embodiment, the illumination device comprises an optical component and a light emitting diode, the light emitting surface of the light emitting diode facing the light incident surface of the optical component. In one embodiment, the light emitting diode system is a polycrystalline light emitting diode.

在一實施例中,這種照明裝置包括光學元件、光源以及一擴散板,該擴散板設於該光學元件的該出光表面的外側,以供從該出光表面射出的光線射入。 In one embodiment, the illumination device includes an optical component, a light source, and a diffuser plate disposed outside the light exiting surface of the optical component for light incident from the light exiting surface to be incident.

基於上述,藉由本發明之光學元件及具有此光學元件之照明裝置的設計,可產生以下功效: Based on the above, by the design of the optical element of the present invention and the illumination device having the same, the following effects can be produced:

1.發光二極體發出的光線可被入光表面上的微結構打散,並重新混和,從而減少黃圈現象。 1. The light emitted by the light-emitting diode can be broken up by the microstructure on the light-emitting surface and re-mixed, thereby reducing the yellow circle phenomenon.

2.本發明是透過微結構來將偏黃的光打散並混光,這些偏黃的光線仍可往目標投射區域投射而不會浪費,因此本發明除可減少黃圈現象之外,還可提高光線利用率。 2. The present invention disperses and mixes the yellowish light through the microstructure, and the yellowish light can still be projected to the target projection area without wasting, so the present invention can reduce the yellow circle phenomenon in addition to the present invention. Improve light utilization.

3.當本發明的光學元件應用在背光模組而排列多個時,可避免將這些偏黃的光直接往外投射而影響其他光學元件的目標投射區域的光斑。這些偏黃的光直接往外投射可能影響其他光學元件的目標投射區域的光斑,從而可能造成其光斑的色度不均勻的問題。 3. When the optical element of the present invention is applied to a plurality of backlight modules, it is possible to avoid directing these yellowish lights directly to affect the spot of the target projection area of the other optical elements. These yellowish light directly projects light spots that may affect the target projection area of other optical components, which may cause problems in the chromaticity of the spot.

4.藉由這些微結構可將從發光二極體兩側發出的光線打散而較不易直接往出光表面的頂部中央處穿過,而可減少中心亮點的問題。 4. By these microstructures, the light emitted from both sides of the light-emitting diode can be dissipated and it is less easy to directly pass through the center of the top of the light-emitting surface, thereby reducing the problem of the central bright spot.

20‧‧‧照明裝置 20‧‧‧Lighting device

100‧‧‧背光透鏡 100‧‧‧Backlight lens

102‧‧‧發光孔 102‧‧‧Lighting holes

103‧‧‧下半段 The lower half of 103‧‧

104‧‧‧單一曲面 104‧‧‧Single surface

105‧‧‧光線 105‧‧‧Light

106‧‧‧LED 106‧‧‧LED

108‧‧‧凹面 108‧‧‧ concave

110‧‧‧頂部 110‧‧‧ top

200a、200b、200c、200d‧‧‧光學元件 200a, 200b, 200c, 200d‧‧‧ optical components

202‧‧‧本體 202‧‧‧Ontology

204‧‧‧入光表面 204‧‧‧ light surface

206‧‧‧出光表面 206‧‧‧Lighting surface

208‧‧‧底面 208‧‧‧ bottom

210‧‧‧凹型空間 210‧‧‧ concave space

212‧‧‧微結構 212‧‧‧Microstructure

213‧‧‧交界面 213‧‧‧ interface

214‧‧‧弧面 214‧‧‧ curved surface

215‧‧‧轉折 215‧‧‧ turning

216‧‧‧外表面 216‧‧‧ outer surface

217‧‧‧台階面 217‧‧‧step surface

218‧‧‧台階面 218‧‧‧step surface

220‧‧‧開口 220‧‧‧ openings

222‧‧‧開口口緣 222‧‧‧Open mouth

224‧‧‧微結構分布區段 224‧‧‧Microstructure distribution section

226‧‧‧平坦部 226‧‧‧ Flat

228‧‧‧環形區域 228‧‧‧ring area

230‧‧‧凹形區域 230‧‧‧ concave area

232‧‧‧第一開口 232‧‧‧first opening

234‧‧‧第二開口 234‧‧‧second opening

236‧‧‧凸形區域 236‧‧‧ convex area

238‧‧‧平坦區域 238‧‧‧flat area

302‧‧‧光源 302‧‧‧Light source

302a‧‧‧發光二極體 302a‧‧‧Lighting diode

304‧‧‧擴散板 304‧‧‧Diffuser

306‧‧‧電路板 306‧‧‧Circuit board

400‧‧‧反射面 400‧‧‧reflecting surface

61‧‧‧第一方向 61‧‧‧First direction

62‧‧‧第二方向 62‧‧‧second direction

A‧‧‧基準軸 A‧‧‧reference axis

B‧‧‧基準面 B‧‧‧ datum

D1‧‧‧第一方向寬度 D 1 ‧‧‧first direction width

DI‧‧‧直徑 D I ‧‧‧diameter

D2‧‧‧第二方向寬度 D 2 ‧‧‧second direction width

DO‧‧‧直徑 D O ‧‧‧diameter

H‧‧‧弧面高度 H‧‧‧Arc height

HI‧‧‧高度 H I ‧‧‧ Height

HL‧‧‧距離 H L ‧‧‧Distance

HO‧‧‧高度 H O ‧‧‧ Height

HP‧‧‧距離 H P ‧‧‧Distance

Lw1‧‧‧光線 Lw1‧‧‧Light

Lw2‧‧‧光線 Lw2‧‧‧Light

Lw3‧‧‧光線 Lw3‧‧‧Light

Ly‧‧‧光線 Ly‧‧‧Light

Ly1‧‧‧光線 Ly1‧‧‧Light

Ly2‧‧‧光線 Ly2‧‧‧Light

Ly3‧‧‧光線 Ly3‧‧‧Light

O‧‧‧基準點 O‧‧‧ benchmark

P1‧‧‧第一端點 P1‧‧‧ first endpoint

P2‧‧‧第二端點 P2‧‧‧ second endpoint

P3‧‧‧交點 P3‧‧‧ intersection

R1‧‧‧第一區域 R1‧‧‧ first area

R2‧‧‧第二區域 R2‧‧‧ second area

S‧‧‧截面 S‧‧‧ section

W‧‧‧弧面寬度 W‧‧‧Arc width

α‧‧‧傾斜角度 ‧‧‧‧ tilt angle

β‧‧‧夾角 ‧‧‧‧角角

θ‧‧‧分布角度 Θ‧‧‧ distribution angle

為了更清楚地說明本發明實施例中的技術方案,下面將對實施例描述中所需要使用的圖式作簡單地介紹,顯而易見地,下面描述中的圖式僅僅是本發明的一些實施例,對於本發明所屬技術領域中具有通常知識者來講,還可以根據這些圖式獲得其他的圖式。 In order to more clearly illustrate the technical solutions in the embodiments of the present invention, the drawings used in the description of the embodiments will be briefly described below. It is obvious that the drawings in the following description are only some embodiments of the present invention. Other figures may also be obtained from these figures for those of ordinary skill in the art to which the invention pertains.

第1圖是習知技術的背光透鏡的剖視圖。 Fig. 1 is a cross-sectional view of a backlight lens of the prior art.

第2圖是繪示本發明一實施例的照明裝置的剖視圖。 Fig. 2 is a cross-sectional view showing a lighting device in accordance with an embodiment of the present invention.

第3圖是繪示第2圖中的光學元件的立體示意圖。 Fig. 3 is a perspective view showing the optical element in Fig. 2.

第4圖是繪示第2圖中的光學元件的局部立體視圖。 Fig. 4 is a partial perspective view showing the optical element of Fig. 2.

第5圖是繪示第2圖的局部放大圖。 Fig. 5 is a partially enlarged view showing Fig. 2;

第6圖是繪示第2圖中的光學元件的仰視圖。 Fig. 6 is a bottom view showing the optical element in Fig. 2.

第7A圖是繪示本發明一實施例的光路示意圖。 FIG. 7A is a schematic view showing an optical path according to an embodiment of the present invention.

第7B圖是繪示第7A圖的局部放大圖。 Fig. 7B is a partially enlarged view showing Fig. 7A.

第8圖是繪示本發明次一實施例的光學元件的剖視圖。 Figure 8 is a cross-sectional view showing an optical element according to a second embodiment of the present invention.

第9圖是繪示本發明又一實施例的光學元件的剖視圖。 Figure 9 is a cross-sectional view showing an optical element according to still another embodiment of the present invention.

第10圖是繪示本發明另一實施例的光學元件的剖視圖。 Figure 10 is a cross-sectional view showing an optical element according to another embodiment of the present invention.

第11圖是繪示第10圖中的光學元件的設計參數示意圖。 Figure 11 is a schematic view showing the design parameters of the optical element in Figure 10.

第12圖是第10圖中的光學元件的配光曲線圖。 Fig. 12 is a light distribution graph of the optical element in Fig. 10.

第13圖是第10圖中的光學元件的照度圖。 Fig. 13 is an illuminance diagram of the optical element in Fig. 10.

第14圖是繪示本發明又一實施例的光學元件的剖視圖。 Figure 14 is a cross-sectional view showing an optical element according to still another embodiment of the present invention.

第15圖是繪示第14圖中的光學元件的凹型空間開口口緣示意圖。 Fig. 15 is a schematic view showing the concave opening of the optical element in Fig. 14.

第16圖是繪示本發明再一實施例的光學元件的剖視圖。 Figure 16 is a cross-sectional view showing an optical element according to still another embodiment of the present invention.

第17圖是繪示本發明次一實施例的光學元件的剖視圖。 Figure 17 is a cross-sectional view showing an optical element according to a second embodiment of the present invention.

第18圖是繪示本發明另一實施例的光學元件的剖視圖。 Figure 18 is a cross-sectional view showing an optical element according to another embodiment of the present invention.

下面將結合本發明實施例中的圖式,對本發明實施例中的技術方案進行清楚、完整地描述,然而所描述的實施例僅僅是本發明一部分實施例,而不是全部的實施例。此外,為了便於說明或理解本發明,本文中類似或相同的元件在不同圖式或不同實施例中是使用相同或類似的元件符號。 The technical solutions in the embodiments of the present invention are clearly and completely described in the following with reference to the drawings in the embodiments of the present invention. However, the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. In addition, the same or similar elements are used in the different drawings or in different embodiments for the purpose of illustration or understanding of the invention.

請參照第2圖至第4圖所示,其中第2圖是本發明一實施例的照明裝置20的剖視圖。第3圖是繪示第2圖中的光學元件200a的立體示意圖。第4圖是繪示第2圖中的光學元件200a的局部立體側視圖。如第2至第4圖所示,在一實施例中,照明裝置20包括光學元件200a以及光源302,其中光學元件200a又常被稱為透鏡,光源302例如為發光二極體302a,光學元件200a包括本體202、入光表面204以及出光表面206,發光二極體302a的發光面朝向光學元件200a的入光表面204,且在此實施例中發光二極體302a所發出的光線在中央偏白色,在左右兩側的光線則偏黃色。在一實施例中,本體202的材質係為透明材質。本體202的材質例如是選自於聚甲基丙烯酸甲酯(polymethyl methacrylate,PMMA)、聚碳酸酯(polycarbonate,PC)、矽膠(silicone)以及玻璃(glass)所組成的群組。自本體202的底部形成一凹型空間210,在一實施例中此凹型空間210類似吊鐘的形狀。入光表面204係由本體202的凹型空間210所定義。換句話說,從本體202的底部形成了凹型空間210,凹型空間210的內壁面形成了入光表面204。入光表面204可供光線入射,並且入光表面204具有環形區域228,其中入光表面204至少在環形區域228上設有複數個微結構212,每一微結構212具有一弧面214,在一實施例中,弧面214為圓弧的一部分。換句話說,入光表面204除了在環形區域228上可設有複數個微結構212外,還可以在其他的區域設置微結構,例如第8圖所示的入光表面204。如第2圖所示,出光表面206形成於本體202的外表面216,其中外表面216的底緣鄰接本體202的底部的外緣。在此實施例中,外表面216還包含與出光表面206相接的一台階面217。此外,本發明光學元件的入光表面204與出光表面206尚有其他態樣,於後說明。 Referring to FIGS. 2 to 4, FIG. 2 is a cross-sectional view of the illumination device 20 according to an embodiment of the present invention. Fig. 3 is a schematic perspective view showing the optical element 200a in Fig. 2. Fig. 4 is a partial perspective side view showing the optical element 200a in Fig. 2. As shown in FIGS. 2 through 4, in an embodiment, the illumination device 20 includes an optical element 200a and a light source 302, wherein the optical element 200a is often referred to as a lens, and the light source 302 is, for example, a light emitting diode 302a, an optical element. 200a includes a body 202, a light incident surface 204, and a light exit surface 206. The light emitting surface of the light emitting diode 302a faces the light incident surface 204 of the optical element 200a, and in this embodiment, the light emitted by the light emitting diode 302a is centered. White, the light on the left and right sides is yellowish. In an embodiment, the material of the body 202 is a transparent material. The material of the body 202 is, for example, a group selected from the group consisting of polymethyl methacrylate (PMMA), polycarbonate (PC), silicone, and glass. A concave space 210 is formed from the bottom of the body 202, which in an embodiment is similar to the shape of a bell. The light incident surface 204 is defined by the concave space 210 of the body 202. In other words, a concave space 210 is formed from the bottom of the body 202, and an inner wall surface of the concave space 210 forms the light incident surface 204. The light incident surface 204 is incident on the light, and the light incident surface 204 has an annular region 228, wherein the light incident surface 204 is provided with a plurality of microstructures 212 at least on the annular region 228, each microstructure 212 having a curved surface 214, In one embodiment, the curved surface 214 is part of a circular arc. In other words, the light incident surface 204 may be provided with a plurality of microstructures 212 in the annular region 228, and may be provided with microstructures in other regions, such as the light incident surface 204 shown in FIG. As shown in FIG. 2, the light exit surface 206 is formed on the outer surface 216 of the body 202 with the bottom edge of the outer surface 216 abutting the outer edge of the bottom of the body 202. In this embodiment, the outer surface 216 also includes a stepped surface 217 that interfaces with the light exit surface 206. In addition, the light incident surface 204 and the light exit surface 206 of the optical component of the present invention have other aspects, which will be described later.

請參照第2圖、第4圖和第5圖所示,其中第5圖是繪示第2圖的局部放大圖。如圖所示,在一實施例中,每一微結構212可由本體202朝向凹型空間210凹陷或是凸出而形成。在第2圖所示的實施例中,微結構212係由本體202朝向凹型空間210凹陷而形成。每一微結構212的弧面214係由每一微結構212在本體202與凹型空間210之間的交界面213所定義,並且在交界面213處的任一微結構212的弧面高度表示為H,在交界面213處的任一微結構212的弧面寬度表示為W,H與W可為任意的尺寸,其中較佳為0.01毫米≦H≦0.2毫米。在一較佳實施例中,0.01毫米≦W≦0.8毫米。在另一較佳實施例中,在交界面213的任一微結構212的弧面高度H除以任一微結構212的弧面寬度W的比值表示為R,其中較佳為0.003≦R≦1.2。 Please refer to FIG. 2, FIG. 4 and FIG. 5, wherein FIG. 5 is a partial enlarged view of FIG. As shown, in one embodiment, each microstructure 212 can be formed by the body 202 being recessed or convex toward the concave space 210. In the embodiment illustrated in FIG. 2, the microstructures 212 are formed by the body 202 being recessed toward the concave space 210. The arcuate surface 214 of each microstructure 212 is defined by the interface 213 of each microstructure 212 between the body 202 and the concave space 210, and the arc height of any of the microstructures 212 at the interface 213 is expressed as H, the arcuate width of any of the microstructures 212 at the interface 213 is expressed as W, and H and W can be any size, with 0.01 mm ≦ H ≦ 0.2 mm being preferred. In a preferred embodiment, 0.01 mm ≦ W ≦ 0.8 mm. In another preferred embodiment, the ratio of the arcuate height H of any of the microstructures 212 of the interface 213 divided by the arcuate width W of any of the microstructures 212 is expressed as R, of which 0.003≦R≦ is preferred. 1.2.

請參照第2圖和第6圖所示,其中第6圖是繪示第2圖中的光學元件200a的仰視圖,如第6圖所示,這些微結構212從凹型空間210觀之可為複數個同心圓形狀。此外,這些微結構212可例如是格紋狀,格紋狀可例如是第2圖所示的四邊形格紋狀,但不限於此,也可為三邊形格紋狀、五邊形格紋狀、六邊形格紋狀或其他多邊形。這些微結構212在入光表面204上可例如是第2圖所示的規則排列,但不限於此,也可是不規則排列,規則排列的好處在於較易產生出均勻的光斑。微結構212可例如是第2圖所示的凹透鏡微結構,但也可是凸透鏡微結構所組成。此外如第2圖所示,在一實施例中,凹型空間210具有一開口220,以通過開口口緣222的平面定義為基準面B,相對於基準面B位在同一高度位置的任一微結構212具有相同的幾何形狀。 Please refer to FIG. 2 and FIG. 6 , wherein FIG. 6 is a bottom view of the optical element 200 a in FIG. 2 . As shown in FIG. 6 , the microstructures 212 can be viewed from the concave space 210 . A plurality of concentric shapes. In addition, the microstructures 212 may be, for example, a lattice shape, and the lattice shape may be, for example, a quadrangular lattice shape as shown in FIG. 2, but is not limited thereto, and may also be a triangular lattice shape or a pentagon lattice pattern. Shape, hexagonal pattern or other polygons. The microstructures 212 may be arranged on the light incident surface 204, for example, as shown in FIG. 2, but are not limited thereto, and may be irregularly arranged. The advantage of the regular arrangement is that a uniform spot is more likely to be generated. The microstructure 212 can be, for example, a concave lens microstructure as shown in FIG. 2, but can also be composed of a convex lens microstructure. In addition, as shown in FIG. 2, in an embodiment, the concave space 210 has an opening 220 defined by the plane of the opening lip 222 as the reference plane B, and any position at the same height position relative to the reference plane B. Structure 212 has the same geometry.

需要說明的是,雖然習知的霧化表面也具有微結構,但與本 發明的微結構212不同。本發明的微結構212具有弧面214,且此弧面214是可用肉眼或是放大鏡等器具明確辨識出來。此外本發明的微結構212是可在設計初期控制幾何結構,如第5圖所示,在此實施例中,此弧面214是圓弧的一部分,且在設計時即可用繪圖軟體精確地繪製其曲率半徑、弧面高度、寬度或是相鄰微結構212之間的距離或是複數個同心圓形狀、格紋狀、等佈列方式,而這些幾何結構都會影響光線的折射或反射等作用,此外亦可利用光學模擬軟體進行模擬以便掌握光學效果。但霧化表面的微結構是無法用肉眼或是放大鏡等器具明確辨識出具有弧面的,霧化表面的微結構是一種粗糙化的表面,雖可用加工方式控制其粗糙化的程度,但卻無法在設計初期即用繪圖軟體精準的決定每一個微結構的幾何形狀,因此在光學設計上也比較不方便。此外,一般而言,光滑表面因未設有微結構雖然效率高但是無法將光打散(均勻化),相對地,本發明的入光表面204的微結構212和習知的霧化表面都可將光打散從而達到均勻化的功效,然而本發明的微結構212更可因具有弧面214而可用繪圖軟體精確地控制其幾何結構,所以相較習知的光滑表面以及霧化表面較便於在均勻化的需求和光效率的需求之間取得平衡,以滿足設計目標。 It should be noted that although the conventional atomizing surface also has a microstructure, The microstructures 212 of the invention are different. The microstructure 212 of the present invention has a curved surface 214, and the curved surface 214 can be clearly identified by an instrument such as a naked eye or a magnifying glass. In addition, the microstructure 212 of the present invention is capable of controlling the geometry at the beginning of the design, as shown in FIG. 5. In this embodiment, the curved surface 214 is a part of a circular arc and can be accurately drawn by the drawing software at the time of design. The radius of curvature, the height of the arc, the width or the distance between adjacent microstructures 212 or a plurality of concentric shapes, lattices, and the like, and these geometric structures may affect the refraction or reflection of light. In addition, optical simulation software can be used to simulate the optical effects. However, the microstructure of the atomized surface cannot be clearly identified by a naked eye or a magnifying glass. The microstructure of the atomized surface is a roughened surface. Although it can be controlled by processing to reduce the degree of roughening, It is impossible to determine the geometry of each microstructure accurately with the drawing software at the beginning of the design, so it is also inconvenient in optical design. In addition, in general, a smooth surface is not efficient because it is not provided with a microstructure, but the light is not dissipated (homogenized). In contrast, the microstructure 212 of the light incident surface 204 of the present invention and the conventional atomizing surface are both The light can be broken up to achieve the effect of homogenization. However, the microstructure 212 of the present invention can be precisely controlled by the drawing software by having the curved surface 214, so that compared with the conventional smooth surface and the atomized surface, It is easy to balance the need for homogenization with the need for light efficiency to meet design goals.

此外,本發明所指的微結構是一種相對的概念,亦即本發明的微結構212與本體202相比是微小的,具體來說,如第2圖和第5圖所示,微結構212的弧面寬度W與本體202的底面208外緣的直徑DO的比值W/DO是介於0.0001和0.14之間。 In addition, the microstructure referred to in the present invention is a relative concept, that is, the microstructure 212 of the present invention is minute compared to the body 202. Specifically, as shown in FIGS. 2 and 5, the microstructure 212 The ratio W/D O of the arcuate width W to the diameter D O of the outer edge of the bottom surface 208 of the body 202 is between 0.0001 and 0.14.

參考第2圖、第7A圖和第7B圖所示,其中第7A圖是繪示本發明一實施例的光路示意圖,第7B圖是繪示第7A圖的局部放大圖。在此實 施例中,入光表面204、出光表面206和發光二極體302a所發出的光相對基準軸A大致呈左右對稱,故第7A圖和第7B圖僅繪示基準軸A的左側區域(亦即第一區域R1)的光路示意。如第7A圖和第7B圖所示,藉由入光表面204在環形區域228上至少設有複數個微結構212,每一微結構212具有一弧面214,發光二極體302a發出的光線可被這些微結構212打散,並且重新混合光線,藉此可達到光線均勻化的功效,具體來說,這些微結構212可將從發光二極體302a由兩側發出而偏黃的光線Ly打散,然後被打散的偏黃光線Ly1、Ly2、Ly3可分別和從發光二極體302a靠近中央所發出偏白的光線Lw1、Lw2、Lw3在擴散板304處混合而被中和,從而減少黃圈現象。這種減少黃圈現象的做法與習知不同,習知的背光透鏡是透過發光孔的下半段為直升狀而把偏黃的光直接往目標投射區域以外的方向投射而浪費掉,但本發明的做法是透過微結構212來將偏黃的光Ly打散後經混光,這些偏黃的光Ly1、Ly2、Ly3仍可往目標投射區域投射而不會浪費,因此本發明除可減少黃圈現象之外還可提高光線利用率。因此,當本發明的光學元件200a應用在背光模組而排列多個時,可避免將這些偏黃的光直接往外投射而影響其他光學元件的目標投射區域的光斑(這些偏黃的光直接往外投射可能影響其他光學元件的目標投射區域的光斑,從而造成其光斑的色度不均勻的問題)。此外,藉由這些微結構212可將從發光二極體302a兩側發出的光線打散而較不易直接往出光面頂部中央處穿過,而可改善中心亮點的問題。相對地,習知技術的背光透鏡因其發光孔下半部為直升狀態,所以較易將光反射而從出光面頂部中央處穿過,而造成中心亮點。 Referring to FIG. 2, FIG. 7A and FIG. 7B, FIG. 7A is a schematic view showing an optical path according to an embodiment of the present invention, and FIG. 7B is a partially enlarged view showing FIG. 7A. In this In the embodiment, the light emitted from the light-incident surface 204, the light-emitting surface 206, and the light-emitting diode 302a is substantially bilaterally symmetric with respect to the reference axis A. Therefore, FIGS. 7A and 7B only show the left side region of the reference axis A (also That is, the optical path of the first region R1) is indicated. As shown in FIG. 7A and FIG. 7B, at least a plurality of microstructures 212 are disposed on the annular region 228 by the light incident surface 204. Each of the microstructures 212 has a curved surface 214 and the light emitted by the LEDs 302a. The microstructures 212 can be broken up and the light can be re-mixed, thereby achieving the effect of uniformizing the light. Specifically, the microstructures 212 can emit yellow light from both sides of the light-emitting diode 302a. The yellowish light rays Ly1, Ly2, and Ly3 which are scattered and then scattered are mixed with the white light Lw1, Lw2, and Lw3 emitted from the center of the light emitting diode 302a at the diffusion plate 304, respectively, to be neutralized, thereby Reduce the yellow circle phenomenon. This method of reducing the yellow circle phenomenon is different from the conventional method. The conventional backlight lens is used to project the yellow light directly in the direction other than the target projection area through the lower half of the light-emitting hole, and is wasted, but The method of the present invention is to disperse the yellowish light Ly through the microstructure 212 and then mix the light, and the yellowish lights Ly1, Ly2, Ly3 can still be projected to the target projection area without wasting, so the present invention can be omitted. In addition to reducing the yellow circle phenomenon, it can also improve light utilization. Therefore, when the optical element 200a of the present invention is applied to a plurality of backlight modules, it is possible to avoid directing these yellowish lights directly to affect the spot of the target projection area of other optical elements (the yellowish lights are directly outward). Projecting a spot that may affect the target projection area of other optical components, causing a problem of uneven chromaticity of its spot). In addition, by using the microstructures 212, the light emitted from both sides of the light-emitting diode 302a can be dissipated and it is less easy to directly pass through the center of the top of the light-emitting surface, thereby improving the problem of the central bright spot. In contrast, the backlight lens of the prior art has a state in which the lower half of the light-emitting aperture is in a straight state, so that it is easier to reflect light and pass through the center of the top of the light-emitting surface to cause a central bright spot.

如第2圖所示,在一實施例中,凹型空間210具有一開口220, 以開口口緣222的幾何中心定義為基準點O,以通過開口口緣222的平面定義為基準面B,以通過基準點O並垂直基準面B的直線定義為基準軸A,以通過基準軸A的一平面定義為截面S,在截面S上以基準軸A劃分入光表面204形成第一區域R1及第二區域R2。如第2圖和第6圖所示,在此實施例中,光學元件200a的開口口緣222為圓形,基準點O即為圓心,基準軸A即為入光表面204和出光表面206的對稱軸,且這些微結構212是圍繞基準軸A一圈而分布在入光表面204的環形區域228上,此外基準軸A貫穿出光表面206的中心。另外,發光二極體302a的底面與本體202的底面208齊平。 As shown in FIG. 2, in an embodiment, the concave space 210 has an opening 220. The geometric center of the opening rim 222 is defined as the reference point O, and the plane passing through the opening rim 222 is defined as the reference plane B, and the straight line passing through the reference point O and the vertical reference plane B is defined as the reference axis A to pass the reference axis. A plane of A is defined as a section S, which is divided into a light surface 204 by a reference axis A on the section S to form a first region R1 and a second region R2. As shown in FIG. 2 and FIG. 6, in this embodiment, the opening edge 222 of the optical element 200a is circular, the reference point O is the center of the circle, and the reference axis A is the light incident surface 204 and the light exit surface 206. The axes of symmetry, and the microstructures 212 are distributed around the reference axis A on the annular region 228 of the light incident surface 204, and further the reference axis A extends through the center of the light exit surface 206. In addition, the bottom surface of the light-emitting diode 302a is flush with the bottom surface 208 of the body 202.

如第2圖和第5圖所示,在一實施例中,在第一區域R1中具有這些微結構212分布之處形成一微結構分布區段224,微結構分布區段224的兩端中較接近基準軸A的一端定義為第一端點P1,第一端點P1與基準點O的連線與基準面B形成這些微結構212的分布角度θ,在一實施例中,20度≦θ≦90度。在一較佳實施例中,20度≦θ≦60度,在第2圖的最佳實施例中,θ=42度。在本發明的光學元件200a中,適當地調整分布角度θ可有效消除黃圈現象。如第7A圖和第7B圖的光路示意圖所示,由於發光二極體302a在兩側所發光的光偏黃中央偏白,其中兩側偏黃的光線Ly造成黃圈現象,本發明的這些微結構212主要是針對這些偏黃的光線Ly,將其打散而起均勻化的作用,但在某些條件下,若微結構212的分布角度θ太大的話,則會打散中央偏白的光線Lw1、Lw2、Lw3,可能使中央的光效率降低,因此,在光學設計時會特別控制分布角度θ的大小。 As shown in FIGS. 2 and 5, in an embodiment, a microstructure distribution section 224 is formed in the first region R1 having the distribution of the microstructures 212, and both ends of the microstructure distribution section 224 are formed. An end closer to the reference axis A is defined as a first end point P1, and a line connecting the first end point P1 and the reference point O forms a distribution angle θ of the microstructures 212 with the reference plane B. In one embodiment, 20 degrees ≦ θ ≦ 90 degrees. In a preferred embodiment, 20 degrees ≦ θ ≦ 60 degrees, and in the preferred embodiment of Fig. 2, θ = 42 degrees. In the optical element 200a of the present invention, appropriately adjusting the distribution angle θ can effectively eliminate the yellow circle phenomenon. As shown in the optical path diagrams of FIGS. 7A and 7B, since the light-emitting diode 302a is whitened at the center of the yellow light emitted from both sides, the yellow light on both sides causes a yellow circle phenomenon, and the present invention The microstructure 212 is mainly for the yellowish light Ly, which is broken up to homogenize, but under certain conditions, if the distribution angle θ of the microstructure 212 is too large, the central whitening will be broken. The light rays Lw1, Lw2, and Lw3 may lower the light efficiency at the center, and therefore, the size of the distribution angle θ is particularly controlled in optical design.

如第2圖所示,在一實施例中,微結構分布區段224的兩端中較遠離基準軸A的一端定義為第二端點P2,第二端點P2沿著基準軸A的方向 至基準面B的距離定義為HL,其中0毫米≦HL≦5毫米。在第2圖的實施例中,HL約為0.65毫米,且發光二極體302的厚度約等於HL。換句話說,發光二極體302a可容納於凹型空間210中,且入光表面204在臨近發光二極體302a左右兩側的部分是光滑表面,但不以此限,亦可為霧化表面。 As shown in FIG. 2, in one embodiment, one of the two ends of the microstructure distribution section 224 that is further away from the reference axis A is defined as the second end point P2, and the second end point P2 is along the direction of the reference axis A. The distance to the reference plane B is defined as H L , where 0 mm ≦ H L ≦ 5 mm. In the embodiment of Fig. 2, H L is about 0.65 mm, and the thickness of the light-emitting diode 302 is approximately equal to H L . In other words, the light emitting diode 302a can be accommodated in the concave space 210, and the portion of the light incident surface 204 adjacent to the left and right sides of the light emitting diode 302a is a smooth surface, but not limited thereto, and can also be an atomizing surface. .

如第2圖和第5圖所示,在一實施例中,在第一區域R1中具有這些微結構212分布之處形成一微結構分布區段224,微結構分布區段224首末兩端的連線與基準面B形成這些微結構212的傾斜角度α,亦即微結構分布區段224首末兩端的連線與基準面B所形成的夾角為傾斜角度α,在一實施例中,10度≦α≦80度。請一併參考第8圖所示,若傾斜角度α增加至大於80度時,被微結構212打散的光線Ly1、Ly2、Ly3會往遠離基準軸A的方向偏移,而往兩側散出,成為雜散光而降低光線利用率。在一實施例中,30度≦α≦60度,由於從發光二極體302a左右兩側所發出的光線Ly偏黃,傾斜角度α在30度到60度的範圍內時,這些微結構212可對偏黃的光線Ly起較直接的作用,也就是說,在光學設計上,要讓發光二極體302a左右兩側所發出偏黃的光線和較接近中央發出偏白的光線相互混和,會較為簡便,從而利於減少黃圈現象。在第2圖的較佳實施例中,這些微結構212的傾斜角度α約為44度。 As shown in FIGS. 2 and 5, in an embodiment, a microstructure distribution section 224 is formed in the first region R1 with the distribution of the microstructures 212, and the microstructure distribution section 224 is at the ends of the first and second ends. The line and the reference plane B form the inclination angle α of the microstructures 212, that is, the angle formed by the line connecting the ends of the microstructure distribution section 224 and the reference plane B is an inclination angle α. In an embodiment, 10 Degree ≦α≦80 degrees. Referring to FIG. 8 together, if the tilt angle α is increased to more than 80 degrees, the rays Ly1, Ly2, and Ly3 scattered by the microstructure 212 are shifted away from the reference axis A, and are scattered to the sides. Out, become stray light and reduce light utilization. In one embodiment, 30 degrees ≦α ≦ 60 degrees, since the light rays Ly from the left and right sides of the light-emitting diode 302a are yellowish, and the tilt angle α is in the range of 30 degrees to 60 degrees, the microstructures 212 It can play a relatively direct role in the yellowish light Ly, that is to say, in the optical design, the yellowish light emitted from the left and right sides of the light emitting diode 302a and the light emitted closer to the center are mixed with each other. It will be easier, which will help reduce the yellow circle phenomenon. In the preferred embodiment of Fig. 2, the microstructures 212 have an angle of inclination a of about 44 degrees.

如第2圖和第4圖所示,在此實施例中,入光表面204具有位在下半部的環形區域228以及鄰接環形區域228並位於上半部的凹形區域230,環形區域228較凹形區域230接近本體202的底部,凹形區域230係由本體202凹陷而形成,換句話說,凹型空間210係由環形區域228以及凹形區域230所圍繞。在一實施例中,環形區域228與凹形區域230的交接處形成轉折 215,但也可不形成轉折,如第9圖所示的實施例。如第2圖和第4圖所示,具體來說,凹形區域230在與環形區域228的交接處形成第一開口232,且環形區域228較遠離凹形區域230處形成第二開口234,其中環形區域228的第二開口234大於凹形區域230的第一開口232。環形區域228與凹形區域230的交接處形成轉折215的好處在於,可使入光表面206有兩個區段可以分別去設計,而可針對兩個部份的光,分別做更有彈性的調整,進而便於讓這兩個部份的光做混光,以符合設計目標。環形區域228的第二開口234大於凹形區域230的第一開口232可使這些微結構212的傾斜角度α較容易設計成30度≦α≦60度。如第2圖和第4圖所示,在此實施例中,凹形區域230為光滑表面,然而,凹形區域230亦可為霧化表面,詳見以下的說明。 As shown in Figures 2 and 4, in this embodiment, the light incident surface 204 has an annular region 228 positioned in the lower half and a concave region 230 adjacent the annular region 228 and located in the upper half, the annular region 228 being more The concave region 230 is adjacent to the bottom of the body 202, and the concave region 230 is formed by the recess of the body 202. In other words, the concave space 210 is surrounded by the annular region 228 and the concave region 230. In an embodiment, the intersection of the annular region 228 and the concave region 230 forms a turning point. 215, but it is also possible to form a transition, as in the embodiment shown in FIG. As shown in FIGS. 2 and 4, in particular, the concave region 230 forms a first opening 232 at the intersection with the annular region 228, and the annular region 228 forms a second opening 234 away from the concave region 230. The second opening 234 of the annular region 228 is larger than the first opening 232 of the concave region 230. The advantage of forming the turn 215 at the intersection of the annular region 228 and the concave region 230 is that the two regions of the light incident surface 206 can be separately designed, and the two portions can be made more flexible for the two portions. Adjustments, which in turn allow the two parts of the light to be mixed to meet the design goals. The second opening 234 of the annular region 228 is larger than the first opening 232 of the concave region 230. The tilt angle a of the microstructures 212 can be easily designed to be 30 degrees ≦α ≦ 60 degrees. As shown in Figures 2 and 4, in this embodiment, the concave region 230 is a smooth surface, however, the concave region 230 may also be an atomizing surface as described below.

請參照第10圖所示,第10圖是繪示本發明另一實施例的光學元件200b的剖視圖,入光表面204具有環形區域228以及鄰接環形區域228的凹形區域230,且環形區域228設有這些微結構212,凹形區域230為霧化表面,環形區域228較凹形區域230接近本體202的底部,凹形區域230係由本體202凹陷而形成,且在此實施例中,環形區域228上的微結構212亦有作霧化處理。入光表面204不限於此,亦可如第8圖所示在環形區域228和凹形區域230都設有複數個微結構212。如第2圖所示,在一實施例中,凹型空間210的開口口緣222的直徑為DI,入光表面204的高度為HI,其中0.2≦HI/DI≦3,入光表面204的高度HI為入光表面204上任一點沿著垂直基準面B的方向至基準面B的距離的最大值。在一實施例中,0.2≦HI/DI≦0.8,具體來說在第2圖的實施例中HI/DI約為0.56,在第10圖的實施例中HI/DI約為0.69。HI/DI的比值會影響凹型空間210的形狀,當HI/DI大於1時,凹型空間210會趨於尖 聳,當HI/DI小於1時,凹型空間210會趨於扁平。習知技術的背光透鏡其HI/DI大都大於1,而趨於尖聳,這可便於將其發光孔下半段設計成直升狀態,但在本發明第2圖和第10圖所示的實施例中卻將HI/DI設計成小於1而可使環形區域228的傾斜程度較為和緩,減小這些微結構212的傾斜角度α,從而可避免光往兩側直接散出,進而可增加光線利用率。 Referring to FIG. 10, FIG. 10 is a cross-sectional view of an optical element 200b having an annular region 228 and a concave region 230 adjoining the annular region 228, and an annular region 228, in accordance with another embodiment of the present invention. These microstructures 212 are provided, the concave region 230 being an atomizing surface, the annular region 228 being closer to the bottom of the body 202 than the concave region 230, and the concave region 230 being formed by the body 202 being recessed, and in this embodiment, a ring The microstructures 212 on the region 228 are also atomized. The light incident surface 204 is not limited thereto, and a plurality of microstructures 212 may be provided in both the annular region 228 and the concave region 230 as shown in FIG. As shown in FIG. 2, in an embodiment, the opening edge 222 of the concave space 210 has a diameter D I , and the height of the light incident surface 204 is H I , wherein 0.2 ≦H I /D I ≦3, into the light. The height H I of the surface 204 is the maximum value of the distance from the point of the vertical reference plane B to the reference plane B at any point on the light incident surface 204. In one embodiment, 0.2 ≦H I /D I ≦ 0.8, specifically H I /D I is about 0.56 in the embodiment of Fig. 2, and in the embodiment of Fig. 10, H I /D I is about It is 0.69. The ratio of H I /D I affects the shape of the concave space 210. When H I /D I is greater than 1, the concave space 210 tends to be sharp, and when H I /D I is less than 1, the concave space 210 tends to Flat. The backlight lens of the prior art has a larger H I /D I than 1 and tends to be pointed, which facilitates designing the lower half of its illuminating aperture to a straight state, but in the second and tenth embodiments of the present invention. In the illustrated embodiment, H I /D I is designed to be less than one, so that the inclination of the annular region 228 is relatively gentle, and the inclination angle α of the microstructures 212 is reduced, so that the light can be prevented from being directly discharged to both sides. In turn, the light utilization rate can be increased.

如第2圖和第4圖所示,在一實施例中,本體202的底部具有一底面208,底面208係自入光表面204的底緣向外延伸且與出光表面206直接或間接連接,在第2圖至第4圖中所示的實施例中,底面208是透過一台階面217而與出光表面206間接連接,換句話說,在此實施例中,外表面216包含了出光表面206以及台階面217,也可以說本體202是由外表面216、底面208以及入光表面204所包圍。在第2圖的實施例中台階面217具有接近垂直的轉折。如第2圖所示,底面208外緣的直徑為DO,出光表面206的高度為HO,其中0.2≦HO/DO≦0.8,出光表面206的高度HO為出光表面206上任一點沿著垂直基準面B的方向至基準面B的距離的最大值。如第2圖所示,此類光學元件200a為扁平狀,較適合背光模組、廣告看板、平板燈和路燈等需要大發光角度的應用領域。 As shown in FIG. 2 and FIG. 4, in an embodiment, the bottom of the body 202 has a bottom surface 208 extending outward from the bottom edge of the light incident surface 204 and directly or indirectly connected to the light exit surface 206. In the embodiment illustrated in Figures 2 through 4, the bottom surface 208 is indirectly coupled to the light exit surface 206 through a stepped surface 217. In other words, in this embodiment, the outer surface 216 includes a light exit surface 206. And the step surface 217, it can also be said that the body 202 is surrounded by the outer surface 216, the bottom surface 208 and the light incident surface 204. In the embodiment of Fig. 2, the stepped surface 217 has a nearly vertical transition. As shown in FIG. 2, the outer edge of the bottom surface 208 has a diameter D O , the height of the light-emitting surface 206 is H O , where 0.2 ≦ H O /D O ≦ 0.8, and the height H O of the light-emitting surface 206 is any point on the light-emitting surface 206. The maximum value of the distance along the direction of the vertical reference plane B to the reference plane B. As shown in FIG. 2, such an optical element 200a is flat, and is suitable for applications such as backlight modules, advertising billboards, flat lamps, and street lamps that require a large illumination angle.

如第2圖所示,在一實施例中,出光表面206在基準軸A與出光表面206的相交處具有一平坦部226。在一實施例中,以基準點O至出光表面206的平坦部226上任一點的連線與基準軸A所形成的夾角β表示為平坦部226的涵蓋角度,其中0度≦β≦20度。在一實施例中,出光表面206的平坦部226與入光表面204相對應。由於入光表面204在至少環形區域228設有複數個微結構212,而可減少中心亮點,因此出光表面206可具有平坦部226而 不需要形成凹面,從而可有效簡化光學元件200a之製程並降低生產成本。在一實施例中,平坦部226可例如是光滑表面,更進一步的,如第2圖所示的實施例,出光表面206可例如是光滑表面,而使整個出光表面206都未設置任何的微結構,如此這可進一步的簡化製程。 As shown in FIG. 2, in one embodiment, the light exit surface 206 has a flat portion 226 at the intersection of the reference axis A and the light exit surface 206. In one embodiment, the angle β formed by the line connecting the reference point O to any point on the flat portion 226 of the light-emitting surface 206 to the reference axis A is expressed as the coverage angle of the flat portion 226, where 0 degrees ≦ β ≦ 20 degrees. In an embodiment, the flat portion 226 of the light exit surface 206 corresponds to the light incident surface 204. Since the light incident surface 204 is provided with at least a plurality of microstructures 212 in at least the annular region 228, the central bright spot can be reduced, so that the light exit surface 206 can have a flat portion 226 It is not necessary to form a concave surface, so that the manufacturing process of the optical element 200a can be effectively simplified and the production cost can be reduced. In an embodiment, the flat portion 226 can be, for example, a smooth surface. Further, as in the embodiment shown in FIG. 2, the light-emitting surface 206 can be, for example, a smooth surface, such that the entire light-emitting surface 206 is not provided with any micro-- Structure, this will further simplify the process.

請再參照第10圖所示,第10圖所示的光學元件200b與第2圖所示的光學元件200a主要差異在於,光學元件200b的環形區域228和凹形區域230都有霧化處理,但光學元件200a則無,此外光學元件200b的凹型空間210較為尖聳,光學元件200a的則較為扁平。以下詳列第10圖的光學元件200b的設計參數,由於光學元件200b和光學元件200a的設計參數定義方式相同,故請一併參見第2圖和第5圖,光學元件200b的微結構212弧面寬度W約為0.30毫米、微結構212弧面高度H約為0.04毫米、微結構212弧面的曲率半徑約為0.31(在此實施例各微結構212弧面的曲率半徑均同,但不在此限,也可不同)、這些微結構212的分布角度θ約為42度、這些微結構212的傾斜角度α約為47度、HL約為0.56毫米、凹型空間210的開口口緣222直徑DI約為5.76毫米,入光表面204的高度HI約為3.96毫米、底面208外緣的直徑DO約為21.06毫米,出光表面206的高度HO約為5.34毫米,以上設計參數皆符合前述的相關數值範圍。此外光學元件200b的出光表面206在與基準軸A的相交處也具有一平坦部226,微結構212也排列為複數個同心圓狀。 Referring again to FIG. 10, the optical component 200b shown in FIG. 10 is mainly different from the optical component 200a shown in FIG. 2 in that the annular region 228 and the concave region 230 of the optical component 200b are atomized. However, the optical element 200a is absent, and the concave space 210 of the optical element 200b is relatively pointed, and the optical element 200a is relatively flat. The design parameters of the optical element 200b of FIG. 10 are detailed below. Since the design parameters of the optical element 200b and the optical element 200a are defined in the same manner, please refer to FIG. 2 and FIG. 5 together, and the microstructure of the optical element 200b is 212 arc. The width W of the surface is about 0.30 mm, the height H of the microstructure 212 is about 0.04 mm, and the radius of curvature of the curved surface of the microstructure 212 is about 0.31 (in this embodiment, the curvature radius of each of the microstructures 212 is the same, but not This limit may also be different. The distribution angle θ of the microstructures 212 is about 42 degrees, the inclination angle α of the microstructures 212 is about 47 degrees, the H L is about 0.56 mm, and the opening edge 222 of the concave space 210 is diameter. D I is about 5.76 mm, the height H I of the light-incident surface 204 is about 3.96 mm, the diameter D O of the outer edge of the bottom surface 208 is about 21.06 mm, and the height H O of the light-emitting surface 206 is about 5.34 mm. The aforementioned range of relevant values. In addition, the light-emitting surface 206 of the optical element 200b also has a flat portion 226 at the intersection with the reference axis A, and the microstructures 212 are also arranged in a plurality of concentric circles.

請參照第10圖和第11圖所示,其中第11圖是繪示第10圖的光學元件200b的設計參數示意圖。在第10圖的實施例中,入光表面204和出光表面206均是以基準軸A為旋轉對稱軸形成旋轉對稱,同時也以基準軸A為對稱軸形成左右對稱,以基準面B和截面S所相交的一直線為一直角座標系 的X軸,以基準軸A為此直角座標系的Y軸,且第二區域R2為此直角座標系的第一象限,第一區域R1為此直角座標系的第二象限,其中第一象限的X坐標和Y坐標均為正值,第二象限的X坐標為負值,Y坐標為正值,在入光表面204上包含具有下列座標的點:(0,3.96)、(0.48,3.86)、(0.99,3.48)、(1.48,2.85)、(1.74,2.21)、(1.84,1.63)、(2.12,1.43)、(2.35,1.22)、(2.55,0.99)、(2.73,0.74)、(2.84,0.56);在出光表面206上包含具有下列座標的點:(0,5.34)、(-3.22,5.18)、(-4.42,4.90)、(-5.56,4.42)、(-6.62,3.73)、(-7.54,2.86)、(-8.14,2.13)、(-8.61,1.30)。 Please refer to FIG. 10 and FIG. 11, wherein FIG. 11 is a schematic diagram showing design parameters of the optical element 200b of FIG. In the embodiment of FIG. 10, both the light incident surface 204 and the light exiting surface 206 form a rotational symmetry with the reference axis A as a rotational symmetry axis, and also form a left-right symmetry with the reference axis A as the symmetry axis, with the reference plane B and the cross section. The straight line intersecting with S is the constant angle coordinate system The X axis, the reference axis A is the Y axis of the rectangular coordinate system, and the second region R2 is the first quadrant of the rectangular coordinate system, and the first region R1 is the second quadrant of the rectangular coordinate system, wherein the first quadrant The X coordinate and the Y coordinate are both positive values, the X coordinate of the second quadrant is a negative value, and the Y coordinate is a positive value, and the points having the following coordinates are included on the light incident surface 204: (0, 3.96), (0.48, 3.86) ), (0.99, 3.48), (1.48, 2.85), (1.74, 2.21), (1.84, 1.63), (2.12, 1.43), (2.35, 1.22), (2.55, 0.99), (2.73, 0.74), (2.84, 0.56); points on the light-emitting surface 206 containing the following coordinates: (0, 5.34), (-3.22, 5.18), (-4.42, 4.90), (-5.56, 4.42), (-6.62, 3.73) ), (-7.54, 2.86), (-8.14, 2.13), (-8.61, 1.30).

請參照第12圖和第13圖所示,其中第12圖是第10圖的光學元件200b的配光曲線圖,第13圖是第10圖的光學元件200b的照度圖。藉由第12圖之配光曲線圖,可知本發明的光學元件200b的發光角度可符合背光模組、廣告看板或平板燈等需要大發光角度的應用領域。透過第13圖之照度圖,可知本發明的光學元件200b可產生照度分布均勻的光。 Referring to Fig. 12 and Fig. 13, Fig. 12 is a light distribution graph of the optical element 200b of Fig. 10, and Fig. 13 is an illuminance diagram of the optical element 200b of Fig. 10. According to the light distribution graph of FIG. 12, it can be seen that the light-emitting angle of the optical element 200b of the present invention can conform to an application field requiring a large light-emitting angle such as a backlight module, an advertising billboard, or a panel light. As is apparent from the illuminance map of Fig. 13, it is understood that the optical element 200b of the present invention can generate light having a uniform illuminance distribution.

如第2圖所示,在一實施例中,照明裝置包括光學元件200a、發光二極體302a以及電路板306,發光二極體302a的發光面朝向光學元件200a的入光表面204。光學元件200a和發光二極體302a均可設置於電路板306的頂面上,也可以說光學元件200a的底面208、發光二極體302a的底面和電路板的頂面均與基準面B齊平。基準軸A通過發光二極體302a底面的幾何中心並且與該發光二極體302a的底面垂直。發光二極體302a可為單晶或多晶發光二極體。值得一提的是,由於高亮度的需求越來越普遍,因此市場上採用多晶發光二極體也越來越多,但採用多晶發光二極體時,晶片成像的問題會更容易發生,也更為嚴重,然而,本發明在入光表面204的環形區域228 設有微結構212而可將發光二極體302a的光線打散而均勻化,除了可減少黃圈現象外,也可有效減少晶片成像的問題。 As shown in FIG. 2, in an embodiment, the illumination device includes an optical element 200a, a light emitting diode 302a, and a circuit board 306. The light emitting surface of the light emitting diode 302a faces the light incident surface 204 of the optical element 200a. The optical element 200a and the light emitting diode 302a may be disposed on the top surface of the circuit board 306. It may be said that the bottom surface 208 of the optical element 200a, the bottom surface of the light emitting diode 302a, and the top surface of the circuit board are all flush with the reference plane B. level. The reference axis A passes through the geometric center of the bottom surface of the light-emitting diode 302a and is perpendicular to the bottom surface of the light-emitting diode 302a. The light emitting diode 302a may be a single crystal or a polycrystalline light emitting diode. It is worth mentioning that due to the increasing popularity of high-brightness requirements, there are more and more polycrystalline LEDs on the market, but when using polycrystalline LEDs, wafer imaging problems are more likely to occur. Also more serious, however, the present invention is in the annular region 228 of the light incident surface 204. The microstructure 212 is provided to disperse and homogenize the light of the LED 230a. In addition to reducing the yellow circle phenomenon, the problem of wafer imaging can be effectively reduced.

在一實施例中,照明裝置20包括光學元件200a、光源302以及擴散板304,擴散板304設於光學元件200a的出光表面206的外側,以供從出光表面206射出的光線射入。擴散板302與基準軸A的交點P3至該基準面B的距離為HP,其中15毫米≦HP≦500毫米,在此實施例中,HP=45毫米。此照明裝置20可用應用於背光模組、廣告看板或平板燈等領域,亦即在此類應用領域中,此照明裝置20可作為背光源。值得一提的是,在此類應用領域中,除了在亮度和色度上需要均勻之外,薄型化也是市場的趨勢,因此也需要大發光角度,而本發明入光表面204因具有微結構212而可把光打散,所以恰好可符合這些需求。 In one embodiment, the illumination device 20 includes an optical element 200a, a light source 302, and a diffuser plate 304 disposed outside the light exit surface 206 of the optical element 200a for light incident from the light exit surface 206 to be incident. The distance from the intersection P3 of the diffuser plate 302 to the reference axis A to the reference plane B is H P , where 15 mm ≦ H P ≦ 500 mm, in this embodiment, H P = 45 mm. The illuminating device 20 can be applied to the fields of a backlight module, an advertising kanban or a flat panel lamp, that is, in such an application field, the illuminating device 20 can be used as a backlight. It is worth mentioning that in such applications, in addition to the need for uniformity in brightness and chromaticity, thinning is also a market trend, so a large illuminating angle is also required, and the light incident surface 204 of the present invention has a microstructure. 212 can break up the light, so it just meets these needs.

請參照第14圖和第15圖所示,其中第14圖是繪示本發明又一實施例的光學元件200c的剖視圖,第15圖是繪示第14圖中的光學元件200c的凹型空間210開口口緣222示意圖。在第14圖所示的實施例中,基準軸A、基準面B以及入光表面204高度HI的定義方式和第2圖所示的實施例相仿。亦即,光學元件200c的凹型空間210具有一開口220,以開口口緣222的幾何中心定義為基準點O,以通過開口口緣222的平面定義為基準面B,以通過基準點O並垂直基準面B的直線定義為基準軸A,入光表面204的高度HI為入光表面204上任一點沿著垂直基準面B的方向至基準面B的距離的最大值。如圖所示,第14圖的光學元件200c類似第2圖的光學元件200a,但光學元件200c的出光表面206非對稱於基準軸A,此外光學元件200c的凹型空間210的開口口緣222為非圓形,而可如第15圖所示的橢圓形。此類的光學元件200c可應用 於路燈,所以常稱為路燈透鏡。更具體來說,以開口口緣222上相距最遠的兩點的連線的方向為一第一方向61,在第一方向61上開口口緣222兩側距離的最大值為第一方向寬度D1,以垂直第一方向為一第二方向62,在第二方向62上開口口緣222兩側距離的最大值為開口口緣222的第二方向寬度D2,其中0.2≦HI/D1≦3,0.2≦HI/D2≦3。請參照第16圖所示,其是繪示本發明再一實施例的光學元件200d的剖視圖。第16圖的光學元件200d的入光表面204和第2圖的光學元件200a的入光表面204類似,光學元件200d和200a的差異在於,光學元件200d的出光表面208為平坦狀,此外,光學元件200d的外表面216還包含一反射面400,反射面400的底緣與本體202的底部的外緣鄰接,且反射面400的頂緣與出光表面206的外緣可直接或間接連接,在第16圖的實施例中,反射面400的頂緣是透過一台階面218而與出光表面206間接連接,且台階面218形成接近直角的轉折。在此實施例中,光學元件200d呈杯狀,在一實施例中,反射面400d可例如為全反射面或塗佈反射層,而可將光線反射至出光表面206。光學元件200d可讓光線集中,而可應用於杯燈、投射燈,因此又常稱為杯燈透鏡。 Referring to FIG. 14 and FIG. 15, FIG. 14 is a cross-sectional view showing an optical element 200c according to still another embodiment of the present invention, and FIG. 15 is a view showing a concave space 210 of the optical element 200c in FIG. A schematic view of the opening rim 222. In the embodiment shown in Fig. 14, the definitions of the heights H I of the reference axis A, the reference plane B, and the light incident surface 204 are similar to those of the embodiment shown in Fig. 2. That is, the concave space 210 of the optical element 200c has an opening 220 defined by the geometric center of the opening rim 222 as a reference point O to be defined as a reference plane B through the plane of the opening rim 222 to pass the reference point O and be vertical The straight line of the reference plane B is defined as the reference axis A, and the height H I of the light incident surface 204 is the maximum value of the distance from the direction of the vertical reference plane B to the reference plane B at any point on the light incident surface 204. As shown in the figure, the optical element 200c of FIG. 14 is similar to the optical element 200a of FIG. 2, but the light-emitting surface 206 of the optical element 200c is asymmetric with respect to the reference axis A, and the opening edge 222 of the concave space 210 of the optical element 200c is Non-circular, but elliptical as shown in Figure 15. Such an optical element 200c can be applied to a street light, so it is often referred to as a street light lens. More specifically, the direction of the line connecting the two points farthest apart on the opening edge 222 is a first direction 61, and the maximum distance between the sides of the opening edge 222 in the first direction 61 is the width of the first direction. D 1 , the first direction is a second direction 62, and the maximum distance between the sides of the opening 222 in the second direction 62 is the width D 2 of the opening 222 in the second direction, wherein 0.2 ≦H I / D 1 ≦ 3, 0.2 ≦ H I / D 2 ≦ 3. Referring to Fig. 16, there is shown a cross-sectional view of an optical element 200d according to still another embodiment of the present invention. The light incident surface 204 of the optical element 200d of Fig. 16 is similar to the light incident surface 204 of the optical element 200a of Fig. 2, and the difference between the optical elements 200d and 200a is that the light exit surface 208 of the optical element 200d is flat, and further, optical The outer surface 216 of the component 200d further includes a reflective surface 400. The bottom edge of the reflective surface 400 is adjacent to the outer edge of the bottom of the body 202, and the top edge of the reflective surface 400 is directly or indirectly connected to the outer edge of the light exit surface 206. In the embodiment of Fig. 16, the top edge of the reflective surface 400 is indirectly connected to the light exit surface 206 through a stepped surface 218, and the stepped surface 218 forms a near right angle turn. In this embodiment, the optical element 200d has a cup shape. In an embodiment, the reflective surface 400d can be, for example, a total reflection surface or a reflective layer, and the light can be reflected to the light exit surface 206. The optical element 200d allows light to be concentrated, and can be applied to a cup lamp or a projection lamp, and is therefore often referred to as a cup lamp lens.

入光表面204還有其他的實施態樣,請一併參照第17圖和第18圖所示,如圖所示,入光表面204具有一環形區域228以及鄰接環形區域228的一凹形區域230、凸形區域236或平坦區域238三者之一,且環形區域228設有這些微結構212,環形區域228較凹形區域230、凸形區域或平坦區域接近本體202的底部,凹形區域230係由本體202凹陷而形成。換句話說,入光表面204的環形區域228不限於和凹形區域223鄰接,也可和凸形區域236(如第17圖所示)或平坦區域238(如第18圖所示)鄰接。 There are other embodiments of the light incident surface 204. Referring to Figures 17 and 18 together, as shown, the light incident surface 204 has an annular region 228 and a concave region adjacent the annular region 228. 230, one of the convex region 236 or the flat region 238, and the annular region 228 is provided with the microstructures 212, the annular region 228 is closer to the bottom of the body 202 than the concave region 230, the convex region or the flat region, the concave region The 230 series is formed by recessing the body 202. In other words, the annular region 228 of the light incident surface 204 is not limited to being contiguous with the concave region 223, but may be contiguous with the convex region 236 (as shown in Figure 17) or the flat region 238 (shown in Figure 18).

簡單來說,本發明提供一種光學元件及具有此光學元件的照明裝置,藉由至少在入光表面的環形區域上設有複數個具有弧面的微結構,以消除黃圈現象、提高光線利用率並且解決中心亮點的問題。 Briefly, the present invention provides an optical component and an illumination device having the same, which is provided with a plurality of microstructures having a curved surface at least on an annular region of the light incident surface to eliminate yellow circles and improve light utilization. Rate and solve the problem of the center highlights.

雖然本發明已用較佳實施例揭露如上,然其並非用以限定本發明,本發明所屬技術領域中具有通常知識者,在不脫離本發明之精神與範圍內,當可作各種之更動與潤飾,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。 While the invention has been described above in terms of the preferred embodiments, the invention is not intended to limit the scope of the invention, and the invention may be practiced without departing from the spirit and scope of the invention. The scope of protection of the present invention is therefore defined by the scope of the appended claims.

20‧‧‧照明裝置 20‧‧‧Lighting device

200a‧‧‧光學元件 200a‧‧‧Optical components

202‧‧‧本體 202‧‧‧Ontology

204‧‧‧入光表面 204‧‧‧ light surface

206‧‧‧出光表面 206‧‧‧Lighting surface

208‧‧‧底部 208‧‧‧ bottom

210‧‧‧凹型空間 210‧‧‧ concave space

212‧‧‧微結構 212‧‧‧Microstructure

214‧‧‧弧面 214‧‧‧ curved surface

215‧‧‧轉折 215‧‧‧ turning

216‧‧‧外表面 216‧‧‧ outer surface

217‧‧‧台階面 217‧‧‧step surface

220‧‧‧開口 220‧‧‧ openings

222‧‧‧開口口緣 222‧‧‧Open mouth

226‧‧‧平坦部 226‧‧‧ Flat

228‧‧‧環形區域 228‧‧‧ring area

230‧‧‧凹形區域 230‧‧‧ concave area

232‧‧‧第一開口 232‧‧‧first opening

234‧‧‧第二開口 234‧‧‧second opening

302‧‧‧光源 302‧‧‧Light source

302a‧‧‧發光二極體 302a‧‧‧Lighting diode

304‧‧‧擴散板 304‧‧‧Diffuser

306‧‧‧電路板 306‧‧‧Circuit board

A‧‧‧基準軸 A‧‧‧reference axis

B‧‧‧基準面 B‧‧‧ datum

DI‧‧‧直徑 D I ‧‧‧diameter

DO‧‧‧直徑 D O ‧‧‧diameter

HI‧‧‧高度 H I ‧‧‧ Height

HL‧‧‧距離 H L ‧‧‧Distance

HO‧‧‧高度 H O ‧‧‧ Height

HP‧‧‧距離 H P ‧‧‧Distance

O‧‧‧基準點 O‧‧‧ benchmark

P1‧‧‧第一端點 P1‧‧‧ first endpoint

P2‧‧‧第二端點 P2‧‧‧ second endpoint

P3‧‧‧交點 P3‧‧‧ intersection

R1‧‧‧第一區域 R1‧‧‧ first area

R2‧‧‧第二區域 R2‧‧‧ second area

S‧‧‧截面 S‧‧‧ section

β‧‧‧夾角 ‧‧‧‧角角

θ‧‧‧分布角度 Θ‧‧‧ distribution angle

Claims (29)

一種光學元件,包括:一本體,自該本體的底部形成一凹型空間;一入光表面,係由該本體的該凹型空間所定義,以供一光線入射,並且該入光表面具有一環形區域,其中該入光表面至少在該環形區域上設有複數個微結構,每一該些微結構具有一弧面;以及一出光表面,形成於該本體的外表面,其中該外表面的底緣鄰接該本體的底部的外緣。 An optical component comprising: a body defining a concave space from a bottom of the body; a light incident surface defined by the concave space of the body for incident light, and the light incident surface having an annular region Wherein the light incident surface is provided with a plurality of microstructures at least on the annular region, each of the microstructures having a curved surface; and a light exiting surface formed on an outer surface of the body, wherein a bottom edge of the outer surface is adjacent The outer edge of the bottom of the body. 如申請專利範圍第1項所述的光學元件,其中每一該些微結構係由該本體朝向該凹型空間凹陷或是凸出而形成。 The optical component of claim 1, wherein each of the microstructures is formed by the body being recessed or convex toward the concave space. 如申請專利範圍第2項所述的光學元件,其中每一該些微結構的該弧面係由每一該些微結構在該本體與該凹型空間之間的交界面所定義,並且在該交界面處的任一該些微結構的弧面高度表示為H,在該交界面處的任一該些微結構的弧面寬度表示為W,其中0.01毫米≦H≦0.2毫米,且0.01毫米≦W≦0.8毫米。 The optical component of claim 2, wherein the arcuate surface of each of the microstructures is defined by an interface of each of the microstructures between the body and the concave space, and at the interface The arcuate height of any of the microstructures is represented as H, and the arcuate width of any of the microstructures at the interface is expressed as W, where 0.01 mm ≦H ≦ 0.2 mm, and 0.01 mm ≦ W ≦ 0.8 Millimeter. 如申請專利範圍第2項所述的光學元件,其中每一該些微結構的該弧面係由每一該些微結構在該本體與該凹型空間之間的交界面所定義,並且在該交界面的任一該些微結構的弧面高度H除以該任一該些微結構的弧面寬度W的比值表示為R,其中0.003≦R≦1.2。 The optical component of claim 2, wherein the arcuate surface of each of the microstructures is defined by an interface of each of the microstructures between the body and the concave space, and at the interface The ratio of the arcuate height H of any of the microstructures divided by the arcuate width W of any of the microstructures is expressed as R, where 0.003 ≦ R ≦ 1.2. 如申請專利範圍第1項所述的光學元件,其中該些微結構從該凹型空間觀之係為複數個同心圓形狀。 The optical component of claim 1, wherein the microstructures have a plurality of concentric shapes from the concave space. 如申請專利範圍第1項所述的光學元件,其中該些微結構係為格紋 狀。 The optical component of claim 1, wherein the microstructures are plaid shape. 如申請專利範圍第1項所述的光學元件,其中該些微結構在該入光表面上係為規則排列或是不規則排列。 The optical component of claim 1, wherein the microstructures are regularly arranged or irregularly arranged on the light incident surface. 如申請專利範圍第1項所述的光學元件,其中該凹型空間具有一開口,以通過該開口口緣的平面定義為基準面,相對於該基準面位在同一高度位置的任一該些微結構具有相同的幾何結構。 The optical component of claim 1, wherein the concave space has an opening defined by a plane of the opening rim as a reference plane, and any of the microstructures at the same height position relative to the reference plane Have the same geometry. 如申請專利範圍第1項所述的光學元件,其中該凹型空間具有一開口,以該開口口緣的幾何中心定義為基準點,以通過該開口口緣的平面定義為基準面,以通過該基準點並垂直該基準面的直線定義為基準軸,以通過該基準軸的一平面定義為截面,在該截面上以該基準軸劃分該入光表面形成一第一區域及一第二區域,在該第一區域中具有該些微結構分布之處形成一微結構分布區段,該微結構分布區段的兩端中較接近該基準軸的一端定義為該第一端點,該第一端點與該基準點的連線與該基準面形成該些微結構的分布角度θ,其中20度≦θ≦90度。 The optical element according to claim 1, wherein the concave space has an opening, and a geometric center of the opening edge is defined as a reference point, and a plane passing through the opening edge is defined as a reference surface to pass the A straight line of the reference point and perpendicular to the reference plane is defined as a reference axis, and a plane passing through the reference axis is defined as a section, and the light incident surface is divided by the reference axis to form a first area and a second area. Forming a microstructure distribution section in the first region having the microstructure distribution, an end of the two ends of the microstructure distribution section being closer to the reference axis is defined as the first end point, the first end A line connecting the point to the reference point forms a distribution angle θ of the microstructures with the reference plane, wherein 20 degrees ≦ θ ≦ 90 degrees. 如申請專利範圍第9項所述的光學元件,其中20度≦θ≦60度。 The optical component of claim 9, wherein 20 degrees ≦ θ ≦ 60 degrees. 如申請專利範圍第9項所述的光學元件,其中該微結構分布區段的兩端中較遠離該基準軸的一端定義為一第二端點,該第二端點沿著該基準軸的方向至該基準面的距離定義為HL,其中0毫米≦HL≦5毫米。 The optical component of claim 9, wherein an end of the two ends of the microstructure distribution section that is further away from the reference axis is defined as a second end point along the reference axis The distance from the direction to the reference plane is defined as H L , where 0 mm ≦ H L ≦ 5 mm. 如申請專利範圍第1項所述的光學元件,其中該凹型空間具有一開口,以該開口口緣的幾何中心定義為基準點,以通過該開口口緣的平面定義為基準面,以通過該基準點並垂直該基準面的直線定義為基準軸,以通過該基準軸的一平面定義為截面,在該截面上以該基準軸劃分該入光表面 形成一第一區域及一第二區域,在該第一區域中具有該些微結構分布之處形成一微結構分布區段,該微結構分布區段首末兩端的連線與該基準面形成該些微結構的傾斜角度α,其中10度≦α≦80度。 The optical element according to claim 1, wherein the concave space has an opening, and a geometric center of the opening edge is defined as a reference point, and a plane passing through the opening edge is defined as a reference surface to pass the A straight line of the reference point and perpendicular to the reference plane is defined as a reference axis, and a plane passing through the reference axis is defined as a section on which the light incident surface is divided by the reference axis Forming a first region and a second region, and forming a microstructure distribution portion in the first region having the microstructure distribution, the connection between the first and last ends of the microstructure distribution segment and the reference surface forming the The tilt angle α of some microstructures, where 10 degrees ≦α≦80 degrees. 如申請專利範圍第12項所述的光學元件,其中30度≦α≦60度。 The optical component of claim 12, wherein 30 degrees ≦α ≦ 60 degrees. 如申請專利範圍第1項所述的光學元件,其中該凹型空間具有一開口,以該開口口緣的幾何中心定義為基準點,以通過該開口口緣的平面定義為基準面,以通過該基準點並垂直該基準面的直線定義為基準軸,該出光表面在該基準軸與該出光表面相交處具有一平坦部。 The optical element according to claim 1, wherein the concave space has an opening, and a geometric center of the opening edge is defined as a reference point, and a plane passing through the opening edge is defined as a reference surface to pass the A straight line of the reference point and perpendicular to the reference plane is defined as a reference axis, and the light exiting surface has a flat portion at a position where the reference axis intersects the light exiting surface. 如申請專利範圍第14項所述的光學元件,其中該平坦部為光滑表面。 The optical component of claim 14, wherein the flat portion is a smooth surface. 如申請專利範圍第1項所述的光學元件,其中該入光表面具有鄰接該環形區域的一凹形區域,且該環形區域與該凹形區域的交接處形成轉折,該環形區域較該凹形區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 The optical component of claim 1, wherein the light incident surface has a concave region adjacent to the annular region, and the intersection of the annular region and the concave region forms a turn, the annular region being smaller than the concave portion The shaped region is adjacent to the bottom of the body, and the concave region is formed by the recess of the body. 如申請專利範圍第16項所述的光學元件,其中該凹形區域在與該環形區域的該交接處形成一第一開口,且該環形區域較遠離該凹形區域處形成一第二開口,其中該環形區域的該第二開口大於該凹形區域的該第一開口。 The optical component of claim 16, wherein the concave region forms a first opening at the intersection with the annular region, and the annular region forms a second opening away from the concave region. Wherein the second opening of the annular region is larger than the first opening of the concave region. 如申請專利範圍第1~15項中任一項所述的光學元件,其中該入光表面具有鄰接該環形區域的一凹形區域,且該凹形區域為光滑表面,該環形區域較該凹形區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 The optical element according to any one of claims 1 to 15, wherein the light incident surface has a concave area adjacent to the annular area, and the concave area is a smooth surface, and the annular area is smaller than the concave area The shaped region is adjacent to the bottom of the body, and the concave region is formed by the recess of the body. 如申請專利範圍第1~15項中任一項所述的光學元件,其中該入光表面具有鄰接該環形區域的一凹形區域,且該凹形區域為霧化表面,該環形區域較該凹形區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 The optical element according to any one of claims 1 to 15, wherein the light incident surface has a concave area adjacent to the annular area, and the concave area is an atomizing surface, and the annular area is The concave region is adjacent to the bottom of the body, and the concave region is formed by the recess of the body. 如申請專利範圍第1~6項中任一項所述的光學元件,其中該凹型空間具有一開口,以通過該開口口緣的平面定義為基準面,該凹型空間的開口口緣的直徑為DI,該入光表面的高度為HI,其中0.2≦HI/DI≦3,該入光表面的高度HI為該入光表面上任一點沿著垂直該基準面的方向至該基準面的距離的最大值。 The optical element according to any one of claims 1 to 6, wherein the concave space has an opening defined by a plane of the opening edge as a reference surface, and a diameter of an opening edge of the concave space is D I , the height of the light incident surface is H I , wherein 0.2 ≦H I /D I ≦3, the height H I of the light incident surface is any point on the light incident surface along the direction perpendicular to the reference plane to the reference The maximum distance of the face. 如申請專利範圍第20項所述的光學元件,其中0.2≦HI/DI≦0.8。 The optical component of claim 20, wherein 0.2 ≦H I /D I ≦0.8. 如申請專利範圍第21項所述的光學元件,其中該本體的底部具有一底面,該底面係自該入光表面的底緣向外延伸且與該出光表面直接或間接連接,該底面外緣的直徑為DO,該出光表面的高度為HO,其中0.2≦HO/DO≦0.8,該出光表面的高度HO為該出光表面上任一點沿著垂直該基準面的方向至該基準面的距離的最大值。 The optical component of claim 21, wherein the bottom of the body has a bottom surface extending outward from a bottom edge of the light incident surface and directly or indirectly connected to the light exit surface, the bottom edge of the bottom surface diameter D O, that the height of the light surface is H O, wherein 0.2 ≦ H O / D O ≦ 0.8, the light exit surface of the height H O that light exit surfaces of any point on the direction of the reference surface along a perpendicular to the reference The maximum distance of the face. 如申請專利範圍第1~6項中任一項所述的光學元件,其中該凹型空間具有一開口,以通過該開口口緣的平面為基準面,該凹型空間的該開口口緣為非圓形,以該開口口緣上相距最遠的兩點的連線的方向為一第一方向,在該第一方向上該開口口緣兩側距離的最大值為第一方向寬度D1,以垂直該第一方向為一第二方向,在該第二方向上該開口口緣兩側距離的最大值為該開口口緣的第二方向寬度D2,該入光表面的高度為HI,其中0.2≦HI/D1≦3,0.2≦HI/D2≦3,該入光表面的高度HI為該入光表面上任一點 沿著垂直該基準面的方向至該基準面的距離的最大值。 The optical element according to any one of claims 1 to 6, wherein the concave space has an opening so that a plane passing through the opening edge is a reference surface, and the opening edge of the concave space is non-circular The direction of the line connecting the two points farthest apart on the opening edge is a first direction, and the maximum distance of the two sides of the opening edge in the first direction is the first direction width D 1 , The first direction is a second direction, and the maximum distance between the two sides of the opening edge is the width D 2 of the opening edge, and the height of the light incident surface is H I , wherein 0.2 ≦ H I / D 1 ≦ 3,0.2 ≦ H I / D 2 ≦ 3, the height H of the light-incident surface for the light incident surface I took a little distance of the reference surface of the reference surface in a direction perpendicular to The maximum value. 如申請專利範圍第1~15項中任一項所述的光學元件,其中該本體的該外表面包含一反射面,該反射面的底緣與該本體的底部的外緣鄰接,且該反射面的頂緣與該出光表面的外緣直接或間接連接。 The optical element according to any one of claims 1 to 15, wherein the outer surface of the body comprises a reflecting surface, a bottom edge of the reflecting surface is adjacent to an outer edge of the bottom of the body, and the reflection The top edge of the face is directly or indirectly connected to the outer edge of the light exiting surface. 如申請專利範圍第1~15項中任一項所述的光學元件,其中該入光表面具有鄰接該環形區域的一凹形區域、一凸形區域或一平坦區域三者之一,該環形區域較該凹形區域、該凸形區域或該平坦區域接近該本體的底部,該凹形區域係由該本體凹陷而形成。 The optical element according to any one of claims 1 to 15, wherein the light incident surface has one of a concave area, a convex area or a flat area adjacent to the annular area, the ring The region is closer to the bottom of the body than the concave region, the convex region or the flat region, and the concave region is formed by the recess of the body. 如申請專利範圍第1~17項中任一項所述的光學元件,其中該本體的材質係為透明材質。 The optical element according to any one of claims 1 to 17, wherein the material of the body is a transparent material. 一種照明裝置,包括:一如申請專利範圍第1~15項中任一項所述的光學元件;以及一發光二極體,該發光二極體的發光面朝向該光學元件的該入光表面。 An illuminating device, comprising: the optical element according to any one of claims 1 to 15; and a light emitting diode, the light emitting surface of the light emitting diode facing the light incident surface of the optical element . 如申請專利範圍第27項所述的照明裝置,其中該發光二極體係為多晶發光二極體。 The illuminating device of claim 27, wherein the illuminating diode system is a polycrystalline luminescent diode. 一種照明裝置,包括:一如申請專利範圍第22項所述的光學元件;一光源;以及一擴散板,設於該光學元件的該出光表面的外側,以供從該出光表面射出的光線射入。 An illuminating device comprising: the optical component according to claim 22; a light source; and a diffusing plate disposed outside the light emitting surface of the optical component for emitting light emitted from the light emitting surface In.
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