JP2018194566A - Diffusion lens and light emitting device - Google Patents

Diffusion lens and light emitting device Download PDF

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JP2018194566A
JP2018194566A JP2015195121A JP2015195121A JP2018194566A JP 2018194566 A JP2018194566 A JP 2018194566A JP 2015195121 A JP2015195121 A JP 2015195121A JP 2015195121 A JP2015195121 A JP 2015195121A JP 2018194566 A JP2018194566 A JP 2018194566A
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light
lens
back surface
central axis
emitting device
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松本 浩一
Koichi Matsumoto
浩一 松本
北村 英二
Eiji Kitamura
英二 北村
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Ip Labo
Ip Labo Corp
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Ip Labo
Ip Labo Corp
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Priority to JP2015195121A priority Critical patent/JP2018194566A/en
Priority to PCT/JP2016/077424 priority patent/WO2017057051A1/en
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F21LIGHTING
    • F21VFUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
    • F21V5/00Refractors for light sources
    • F21V5/04Refractors for light sources of lens shape
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/18Optical objectives specially designed for the purposes specified below with lenses having one or more non-spherical faces, e.g. for reducing geometrical aberration
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B3/00Simple or compound lenses
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/85Packages
    • H10H20/855Optical field-shaping means, e.g. lenses

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Planar Illumination Modules (AREA)
  • Lenses (AREA)
  • Led Device Packages (AREA)

Abstract

To provide a diffusion lens having high degree of freedom in designing of surface shape, which is easily designed and formed and capable of suppressing brightness unevenness.SOLUTION: Disclosed lens 4 has a circular shape in plan view, and each of a surface 6 and a rear face 8 is formed generally symmetrically with respect to the central axis X passing through the center of the circular shape. In a central area of the rear face 8, a concave incident part 9 is formed so that light from an LED 2, which is disposed so that the central axis X coincides with the optical axis, enters. The rear face 8 is formed in a taper which is inclined upward at a predetermined angle when viewed from the incident part 9 side.SELECTED DRAWING: Figure 4

Description

本発明は、画像表示装置のバックライトに用いられる発光ダイオード(LED)等の光を拡散させる拡散レンズと、この拡散レンズを備える発光装置に関する。   The present invention relates to a diffusing lens for diffusing light such as a light emitting diode (LED) used for a backlight of an image display device, and a light emitting device including the diffusing lens.

LED等の発光素子では、その光軸付近に光量が集中する特性があり、例えば液晶テレビ等の画像表示装置のバックライトに用いられるLEDについては、輝度ムラを抑制するために、その発光を拡散させる拡散レンズが使用されている。   A light emitting element such as an LED has a characteristic that the amount of light is concentrated in the vicinity of the optical axis. For example, an LED used for a backlight of an image display device such as a liquid crystal television diffuses light emission in order to suppress luminance unevenness. A diffusing lens is used.

このような拡散レンズとして、従来、特許文献1に記載された発光装置のレンズが知られている。同文献に記載されたレンズは、裏面側に配置されたLEDの発光を拡散させるもので、その表面(出射面)の中心部に、光軸を法線とする平面に対して傾斜の緩い透過屈折面と傾斜の急な反射面が交互に階段状に形成された第1の領域が設けられ、この第1の領域の外周に、連続した曲面で形成された第2の領域が設けられている。そして、第1の領域において、反射面により光線の一部が反射されることによって、光軸付近に強度の高い出射光が集中することによる輝度ムラの発生が抑制されている。   As such a diffusing lens, a lens of a light emitting device described in Patent Document 1 is conventionally known. The lens described in this document diffuses the light emission of the LED arranged on the back side, and is transmitted at a slant with respect to a plane whose normal is the optical axis at the center of the front surface (outgoing surface). A first region in which a refracting surface and a steep reflecting surface are alternately formed in a staircase shape is provided, and a second region formed by a continuous curved surface is provided on the outer periphery of the first region. Yes. Then, in the first region, a part of the light beam is reflected by the reflecting surface, thereby suppressing the occurrence of luminance unevenness due to the concentrated emitted light having a high intensity near the optical axis.

特開2011−34770号公報JP 2011-34770 A

しかしながら、特許文献1に記載された拡散レンズでは、特に第1の領域の形状が複雑であることから、その設計と成形が容易ではなく製造コストが嵩み、また、第1の領域の成形に伴いレンズの表面側に凹みができることから、レンズの表面形状の設計の自由度が失われるという問題があった。   However, in the diffusing lens described in Patent Document 1, since the shape of the first region is particularly complicated, the design and molding thereof is not easy and the manufacturing cost is high, and the molding of the first region is also difficult. Along with this, there is a problem in that the degree of freedom in designing the surface shape of the lens is lost because a dent is formed on the surface side of the lens.

本発明は、上記の事情に鑑みてなされたもので、表面形状の設計の自由度が高く、設計及び成形が容易で輝度ムラを抑制することができる拡散レンズと、このような拡散レンズを備える発光装置を提供することを課題としている。   The present invention has been made in view of the above circumstances, and includes a diffusing lens that has a high degree of freedom in designing a surface shape, can be easily designed and molded, and can suppress luminance unevenness, and such a diffusing lens. An object is to provide a light-emitting device.

上記課題を解決するために、本発明に係る拡散レンズは、平面視円形状を呈し、該円形の中心を通る中心軸に対して表面及び裏面のそれぞれが略対称に形成され、前記裏面の中心部には、前記中心軸と光軸が合致するように配置される光源からの光が入射する凹状の入射部が設けられ、前記裏面は、前記入射部の側から見て所定の角度で上方に傾斜したテーパー状に形成されていることを特徴とする。   In order to solve the above problems, a diffusing lens according to the present invention has a circular shape in plan view, and each of a front surface and a back surface is formed substantially symmetrically with respect to a central axis passing through the center of the circle, and the center of the back surface The portion is provided with a concave incident portion on which light from a light source arranged so that the central axis and the optical axis coincide with each other, and the back surface is upward at a predetermined angle when viewed from the incident portion side. It is characterized by being formed in a tapered shape.

また、本発明に係る発光装置は、光源と、該光源の発光を拡散させる拡散レンズとを備え、前記拡散レンズは、平面視円形状を呈し、該円形の中心を通る中心軸に対して表面及び裏面のそれぞれが略対称に形成され、前記裏面の中心部には、前記中心軸と光軸が合致するように配置される前記光源からの光が入射する凹状の入射部が設けられ、前記裏面は、前記入射部の側から見て所定の角度で上方に傾斜したテーパー状に形成されていることを特徴とする。   The light-emitting device according to the present invention includes a light source and a diffusion lens that diffuses light emitted from the light source, and the diffusion lens has a circular shape in plan view and has a surface with respect to a central axis passing through the center of the circle. Each of the back surface and the back surface is formed substantially symmetrically, and a concave incident portion on which light from the light source is disposed so that the central axis and the optical axis coincide with each other is provided at a center portion of the back surface, The back surface is formed in a tapered shape inclined upward at a predetermined angle when viewed from the incident portion side.

本発明に係る拡散レンズ及び発光装置においては、拡散レンズの裏面が入射部の側から見て所定の角度で上方に傾斜したテーパー状に形成されていることにより、光源が光軸付近に光量が集中する特性を有する場合であっても光軸付近のピーク光量が減少し、その分、光軸から離れたところの光量が増大して輝度ムラが抑制される。すなわち、この効果は、拡散レンズの表面を複雑な形状に加工することなく裏面を所定の角度でテーパー状に形成するだけで得られるから、本発明によれば、拡散レンズを、表面形状の設計の自由度が高く、設計及び成形が容易で輝度ムラを抑制可能なものとすることができる。   In the diffusing lens and the light emitting device according to the present invention, the back surface of the diffusing lens is formed in a tapered shape inclined upward at a predetermined angle when viewed from the incident portion side, so that the light source has a light amount near the optical axis. Even in the case of a concentration characteristic, the peak light quantity near the optical axis is reduced, and the light quantity away from the optical axis is increased correspondingly to suppress luminance unevenness. In other words, this effect can be obtained simply by forming the back surface into a tapered shape at a predetermined angle without processing the surface of the diffusion lens into a complicated shape. The degree of freedom is high, design and molding are easy, and luminance unevenness can be suppressed.

また、裏面がテーパー状に形成されることにより、入射部付近に籠りがちな光源の熱が裏面の下方空間から放散されやすくなり、放熱効果を向上させることができる。   Further, since the back surface is formed in a tapered shape, the heat of the light source which tends to be scattered near the incident portion is easily dissipated from the lower space on the back surface, and the heat dissipation effect can be improved.

前記所定の角度は、前記中心軸を法線とする平面に対して2.5度以上6度以下であることが望ましく、これにより、ピーク光量を大幅に減少させて輝度ムラを効果的に抑制することができる。   The predetermined angle is preferably 2.5 degrees or more and 6 degrees or less with respect to a plane having the central axis as a normal line, and thereby, the peak light amount is greatly reduced and luminance unevenness is effectively suppressed. can do.

本発明によれば、拡散レンズを、表面形状の設計の自由度が高く、設計及び成形が容易で輝度ムラを抑制可能なものとすることができる。   According to the present invention, the diffusing lens can have a high degree of freedom in designing the surface shape, can be easily designed and molded, and can suppress uneven brightness.

発明を実施するための形態に係る発光装置の断面図である。It is sectional drawing of the light-emitting device which concerns on the form for inventing. 図1の発光装置のレンズの表面側を示す斜視図である。It is a perspective view which shows the surface side of the lens of the light-emitting device of FIG. 図1の発光装置のレンズの裏面側を示す斜視図である。It is a perspective view which shows the back surface side of the lens of the light-emitting device of FIG. 図1の発光装置において、LEDの出射光の経路を例示する説明図である。FIG. 2 is an explanatory diagram illustrating a path of emitted light from an LED in the light emitting device of FIG. 1. 図1の発光装置において、レンズの裏面の傾斜角度を変化させたときのピーク光量の変化を示す説明図である。In the light-emitting device of FIG. 1, it is explanatory drawing which shows the change of the peak light quantity when changing the inclination-angle of the back surface of a lens. 図1の発光装置について、(a)はレンズの裏面の傾斜角度が0度のときの照射面における照度分布を示す説明図、(b)はレンズの裏面の傾斜角度が4.5度のときの照射面における照度分布を示す説明図である。1A is an explanatory diagram showing the illuminance distribution on the irradiated surface when the tilt angle of the back surface of the lens is 0 degree, and FIG. 1B is a diagram when the tilt angle of the back surface of the lens is 4.5 degrees. It is explanatory drawing which shows the illumination intensity distribution in the irradiation surface. 図1の発光装置について、レンズの裏面の傾斜角度が0度と3度のときの照射面における光線分布を示す説明図である。FIG. 2 is an explanatory diagram showing the light distribution on the irradiated surface when the inclination angle of the back surface of the lens is 0 degree and 3 degrees for the light emitting device of FIG. 1. 発明を実施するための形態に係る他の発光装置において、LEDの出射光の経路を例示する説明図である。It is explanatory drawing which illustrates the path | route of the emitted light of LED in the other light-emitting device which concerns on the form for inventing. 図8の発光装置について、レンズの裏面の傾斜角度が0度と3度のときの照射面における光線分布を示す説明図である。FIG. 9 is an explanatory diagram showing a light distribution on the irradiated surface when the inclination angle of the back surface of the lens is 0 degree and 3 degrees for the light emitting device of FIG. 8. 発明を実施するための形態に係るさらに他の発光装置において、LEDの出射光の経路を例示する説明図である。It is explanatory drawing which illustrates the path | route of the emitted light of LED in the further another light-emitting device based on the form for inventing. 図10の発光装置について、レンズの裏面の傾斜角度が0度と3度のときの照射面における光線分布を示す説明図である。FIG. 11 is an explanatory diagram showing a light distribution on the irradiated surface when the inclination angle of the rear surface of the lens is 0 degree and 3 degrees for the light emitting device of FIG. 10.

本発明を実施するための形態について、図面を用いて説明する。   Embodiments for carrying out the present invention will be described with reference to the drawings.

図1は、本形態に係る拡散レンズを備えた発光装置を示す。この発光装置1は、液晶テレビ等の画像表示装置のバックライトに使用することが可能で、LED2と、基板3と、レンズ4とを有する。   FIG. 1 shows a light emitting device including a diffusing lens according to this embodiment. The light emitting device 1 can be used as a backlight of an image display device such as a liquid crystal television, and includes an LED 2, a substrate 3, and a lens 4.

LED2は、図示を略す電源に駆動されて白色の光を出射する。   The LED 2 is driven by a power supply (not shown) and emits white light.

基板3は、平面視長方形状を呈し、その上面5には反射コーティングが施されるとともに、長手方向に沿ってLED2が複数設けられている。LED2は、光軸が基板3の法線と平行するように基板3に固着され、上方に向けて(基板3と反対側に向けて)発光する。   The substrate 3 has a rectangular shape in plan view, and the upper surface 5 is provided with a reflective coating, and a plurality of LEDs 2 are provided along the longitudinal direction. The LED 2 is fixed to the substrate 3 so that its optical axis is parallel to the normal line of the substrate 3, and emits light upward (toward the side opposite to the substrate 3).

レンズ4は、ここでは透過率95パーセント以上、屈折率約1.5のPMMA樹脂により一体成形され、図2に示すように、平面視円形を呈する。この円形の中心を通る中心軸XがLED2の光軸と合致するように、レンズ4はLED2の上方に設けられている。   Here, the lens 4 is integrally formed of PMMA resin having a transmittance of 95% or more and a refractive index of about 1.5, and has a circular shape in plan view as shown in FIG. The lens 4 is provided above the LED 2 so that the central axis X passing through the center of the circle coincides with the optical axis of the LED 2.

レンズ4の表面6は、頂部に凸部7が形成されたドーム状を呈し、中心軸Xを含む任意の断面における表面6の形状は、中心軸Xに対して略対称である。   The surface 6 of the lens 4 has a dome shape with a convex portion 7 formed on the top, and the shape of the surface 6 in any cross section including the central axis X is substantially symmetric with respect to the central axis X.

レンズの裏面8の中心部には、LED2からの光が入射する凹状の入射部9が設けられ、中心軸Xを含む任意の断面における入射部9の形状は、中心軸Xに対して略対称である。   A concave incident portion 9 into which light from the LED 2 is incident is provided at the center of the back surface 8 of the lens, and the shape of the incident portion 9 in an arbitrary cross section including the central axis X is substantially symmetric with respect to the central axis X. It is.

また、裏面8は、入射部9の側から見て所定の角度θ(図1参照)で上方に傾斜したテーパー状に形成され、中心軸Xを含む任意の断面における裏面8の形状も、中心軸Xに対して略対称である。   Further, the back surface 8 is formed in a tapered shape inclined upward at a predetermined angle θ (see FIG. 1) when viewed from the incident portion 9 side, and the shape of the back surface 8 in an arbitrary cross section including the central axis X is also the center. It is substantially symmetric with respect to the axis X.

図3に示すように、入射部9の外側には、底面視円形の3つの脚部10が中心軸Xから等距離に位置するように、かつ、互いに等距離で離間するように形成され、レンズ4は、脚部10により、基板3上に固定される。   As shown in FIG. 3, on the outer side of the incident portion 9, three leg portions 10 having a circular shape in a bottom view are formed so as to be located at an equal distance from the central axis X and to be separated from each other at an equal distance, The lens 4 is fixed on the substrate 3 by the legs 10.

この発光装置1では、図4に示すように、LED2からの光はレンズ4の入射部9に入射して屈折し、その一部が表面6で反射され、残部が表面6を透過して出射する。表面6で反射された光は、その一部が裏面8を透過して残部が裏面8で反射され、裏面8を透過した光は、基板3の上面5で反射され、裏面8からレンズ4に再度入射する。裏面8で反射された光や上面5で反射された光も、最終的には表面6を透過して出射し、照明に供する。   In this light emitting device 1, as shown in FIG. 4, the light from the LED 2 enters and refracts the incident part 9 of the lens 4, a part of which is reflected by the surface 6, and the remaining part is transmitted through the surface 6 and emitted. To do. A part of the light reflected by the front surface 6 is transmitted through the back surface 8 and the remaining part is reflected by the back surface 8, and the light transmitted through the back surface 8 is reflected by the top surface 5 of the substrate 3 and passes from the back surface 8 to the lens 4. Incident again. The light reflected by the back surface 8 and the light reflected by the upper surface 5 are finally transmitted through the front surface 6 and emitted for illumination.

このとき、裏面8が入射部9の側から見て所定の角度で上方に傾斜したテーパー状に形成されていることにより、LED2の光軸付近(レンズ4の中心軸X付近)のピーク光量が減少し、その分、光軸から離れたところの光量が増大する。図5に示すように、テーパー面(裏面8)と中心軸Xを法線とする平面とのなす傾斜角度を0.5度ずつ変化させると、ピーク光量は4.5度付近で最小値となり、とりわけ傾斜角度が2.5度以上6度以下である場合には、裏面がテーパー状でない場合に比べてピーク光量が5パーセント以上カットされ、図6に示すように、ピーク光量に起因する輝点(図6(a)における中心の白い点)が観察されなくなる。   At this time, the back surface 8 is formed in a taper shape that is inclined upward at a predetermined angle when viewed from the incident portion 9 side, so that the peak light amount in the vicinity of the optical axis of the LED 2 (near the central axis X of the lens 4) is increased. The amount of light decreases and the amount of light away from the optical axis increases accordingly. As shown in FIG. 5, when the inclination angle between the tapered surface (rear surface 8) and the plane having the central axis X as a normal line is changed by 0.5 degrees, the peak light amount becomes the minimum value near 4.5 degrees. In particular, when the tilt angle is 2.5 degrees or more and 6 degrees or less, the peak light amount is cut by 5% or more as compared with the case where the back surface is not tapered, and as shown in FIG. A point (a central white point in FIG. 6A) is not observed.

傾斜角度を0度、3度としたときの照射面における光線分布を見ても、図7に示すように、3度のときの照射範囲(分布範囲)L1の方が7度のときの照射範囲L2よりも広範で、光量が分散していることがわかる。   Even if the light ray distribution on the irradiation surface when the inclination angle is 0 degree and 3 degrees is seen, as shown in FIG. 7, the irradiation range (distribution range) L1 at 3 degrees is 7 degrees. It can be seen that the light quantity is wider than the range L2.

要するに、本形態では、レンズ4の裏面8が入射部9の側から見て所定の角度(傾斜角度)で上方に傾斜したテーパー状に形成されていることにより、LED2の光軸付近のピーク光量が減少し、その分、光軸から離れたところの光量が増大して輝度ムラが抑制される。この効果は、レンズ4の表面を複雑な形状に加工することなく裏面8を所定の角度でテーパー状に形成するだけで得られるから、本実施例によれば、レンズ4を、表面形状の設計の自由度が高く、設計及び成形が容易で輝度ムラを抑制可能なものとすることができる。   In short, in this embodiment, the back surface 8 of the lens 4 is formed in a tapered shape that is inclined upward at a predetermined angle (inclination angle) when viewed from the incident portion 9 side, so that the peak light amount near the optical axis of the LED 2 is obtained. Decreases, and accordingly, the amount of light away from the optical axis increases to suppress uneven brightness. This effect can be obtained simply by forming the back surface 8 into a tapered shape at a predetermined angle without processing the surface of the lens 4 into a complicated shape. According to this embodiment, the lens 4 is designed to have a surface shape design. The degree of freedom is high, design and molding are easy, and luminance unevenness can be suppressed.

また、裏面8がテーパー状に形成されることにより、入射部9付近に籠りがちなLED2の熱が裏面8の下方空間(裏面8と基板3の上面5との間の空間)から放散されやすくなり、放熱効果を向上させることができる。   Further, since the back surface 8 is formed in a taper shape, the heat of the LED 2 that tends to be scattered near the incident portion 9 is easily dissipated from the lower space of the back surface 8 (the space between the back surface 8 and the upper surface 5 of the substrate 3). Thus, the heat dissipation effect can be improved.

上記所定の角度は、2.5度以上6度以下であることが望ましく、これにより、ピーク光量を大幅に減少させて輝度ムラを効果的に抑制することができる。   The predetermined angle is desirably 2.5 degrees or more and 6 degrees or less, and thereby, the peak light quantity can be significantly reduced and luminance unevenness can be effectively suppressed.

図8は、本発明に係る拡散レンズを備えた発光装置の他の例を示す。この発光装置11は、表面6の頂部に凸部7が形成されていない点以外は、実施例1に係る発光装置1と同様であり、図7に対応する光線分布は、図9に示すようになる。   FIG. 8 shows another example of a light emitting device including a diffusing lens according to the present invention. This light-emitting device 11 is the same as the light-emitting device 1 according to Example 1 except that the convex portion 7 is not formed on the top of the surface 6, and the light distribution corresponding to FIG. 7 is as shown in FIG. become.

図10は、本発明に係る拡散レンズを備えた発光装置のさらに他の例を示す。この発光装置12は、表面6の頂部に凸部7が形成されずに凹部13が形成されている点以外は、実施例1に係る発光装置1と同様であり、図7に対応する光線分布は、図11に示すようになる。   FIG. 10 shows still another example of the light emitting device including the diffusing lens according to the present invention. The light emitting device 12 is the same as the light emitting device 1 according to Example 1 except that the convex portion 7 is not formed at the top of the surface 6 but the concave portion 13 is formed, and the light distribution corresponding to FIG. Is as shown in FIG.

以上、本発明を実施するための形態について例示したが、本発明の実施形態は上述したものに限られず、発明の趣旨を逸脱しない範囲で適宜変更等してもよい。   As mentioned above, although the form for implementing this invention was illustrated, embodiment of this invention is not restricted to what was mentioned above, You may change suitably etc. in the range which does not deviate from the meaning of invention.

例えば、上記形態ではLED2は白色の光を出射するとしたが、赤色や緑色、青色等の光を出射するものでもよい。   For example, in the above embodiment, the LED 2 emits white light, but may emit light of red, green, blue, or the like.

また、レンズ4もPMMA樹脂により一体成形したものでなくてもよく、ABS(アクリロニトリル・ブタジエン・スチレン共重合体)、PC(ポリカーボネート)その他の透明材料を用いてもかまわない。   Further, the lens 4 may not be integrally formed of PMMA resin, and ABS (acrylonitrile / butadiene / styrene copolymer), PC (polycarbonate) or other transparent materials may be used.

さらに、レンズの表面形状も実施例1乃至3に示したものに限られず、平面視形状が円形ではない方形、楕円形等のレンズに対して裏面をテーパー状とすることも考えられる。   Further, the surface shape of the lens is not limited to those shown in the first to third embodiments, and it is also conceivable that the back surface is tapered with respect to a square or elliptical lens whose shape in plan view is not circular.

本発明は、大画面の画像表示装置のバックライトを少ない発光素子で構成する場合等に好適に利用可能である。   The present invention can be suitably used when, for example, a backlight of a large screen image display apparatus is configured with a small number of light emitting elements.

1,11,12 発光装置
2 LED(光源)
3 基板
4 レンズ(拡散レンズ)
6 表面
8 裏面
9 入射部
X 中心軸
1, 11, 12 Light-emitting device 2 LED (light source)
3 Substrate 4 Lens (Diffusion lens)
6 Front surface 8 Back surface 9 Incident part X Central axis

Claims (4)

平面視円形状を呈し、該円形の中心を通る中心軸に対して表面及び裏面のそれぞれが略対称に形成され、
前記裏面の中心部には、前記中心軸と光軸が合致するように配置される光源からの光が入射する凹状の入射部が設けられ、
前記裏面は、前記入射部の側から見て所定の角度で上方に傾斜したテーパー状に形成されていることを特徴とする拡散レンズ。
It has a circular shape in plan view, and each of the front surface and the back surface is formed substantially symmetrically with respect to the central axis passing through the center of the circle.
A concave incident portion into which light from a light source arranged so that the central axis and the optical axis coincide with each other is provided at the center of the back surface,
The diffusing lens is characterized in that the back surface is formed in a tapered shape inclined upward at a predetermined angle when viewed from the incident portion side.
前記所定の角度は、前記中心軸を法線とする平面に対して2.5度以上6度以下であることを特徴とする請求項1に記載の拡散レンズ。   The diffusing lens according to claim 1, wherein the predetermined angle is 2.5 degrees or more and 6 degrees or less with respect to a plane having the central axis as a normal line. 光源と、該光源の発光を拡散させる拡散レンズとを備え、
前記拡散レンズは、平面視円形状を呈し、該円形の中心を通る中心軸に対して表面及び裏面のそれぞれが略対称に形成され、
前記裏面の中心部には、前記中心軸と光軸が合致するように配置される前記光源からの光が入射する凹状の入射部が設けられ、
前記裏面は、前記入射部の側から見て所定の角度で上方に傾斜したテーパー状に形成されていることを特徴とする発光装置。
A light source, and a diffusion lens that diffuses the light emitted from the light source,
The diffuser lens has a circular shape in plan view, and each of the front and back surfaces is formed substantially symmetrically with respect to a central axis passing through the center of the circle.
A concave incident portion into which light from the light source is arranged so that the central axis and the optical axis coincide with each other is provided at the center of the back surface,
The light-emitting device, wherein the back surface is formed in a tapered shape inclined upward at a predetermined angle when viewed from the incident portion side.
前記所定の角度は、前記中心軸を法線とする平面に対して2.5度以上6度以下であることを特徴とする請求項3に記載の発光装置。   The light emitting device according to claim 3, wherein the predetermined angle is 2.5 degrees or more and 6 degrees or less with respect to a plane having the central axis as a normal line.
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