WO2011114608A1 - 発光装置、面光源および液晶ディスプレイ装置 - Google Patents
発光装置、面光源および液晶ディスプレイ装置 Download PDFInfo
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- WO2011114608A1 WO2011114608A1 PCT/JP2011/000326 JP2011000326W WO2011114608A1 WO 2011114608 A1 WO2011114608 A1 WO 2011114608A1 JP 2011000326 W JP2011000326 W JP 2011000326W WO 2011114608 A1 WO2011114608 A1 WO 2011114608A1
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- light emitting
- light
- light source
- emitting device
- lens
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/08—Anamorphotic objectives
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/1336—Illuminating devices
- G02F1/133602—Direct backlight
- G02F1/133603—Direct backlight with LEDs
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L33/48—Semiconductor devices with at least one potential-jump barrier or surface barrier specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor body packages
- H01L33/58—Optical field-shaping elements
Definitions
- the present invention relates to a light emitting device that spreads the directionality of light from a light source such as a light emitting diode (hereinafter simply referred to as “LED”) with a lens.
- a light source such as a light emitting diode (hereinafter simply referred to as “LED”) with a lens.
- the present invention also relates to a surface light source including a plurality of light emitting devices, and a liquid crystal display device in which the surface light source is disposed behind a liquid crystal panel as a backlight.
- a large number of cold cathode fluorescent lamps are arranged directly under the liquid crystal panel, and these cold cathode fluorescent lamps are used together with members such as a diffusion plate and a reflector.
- LEDs have been used as light sources for backlights. LEDs have been improved in efficiency in recent years, and are expected as light sources with low power consumption, which are replaced with fluorescent lamps. Further, as a light source for a liquid crystal display device, the power consumption of the liquid crystal display device can be reduced by controlling the brightness of the LED according to the image.
- Patent Document 1 proposes a light emitting device that can obtain a uniform surface light source even with a small number of LEDs. Yes.
- the lens used in the light emitting device of Patent Document 1 has a circular shape in a plan view, and has both a concave incident surface, a concave portion near the optical axis, and a convex emission surface on the outer side. It is rotationally symmetric with respect to the optical axis.
- Patent Document 2 discloses a light-emitting device using a lens in which a V-groove extending in a direction perpendicular to the optical axis is formed at the center of the exit surface. According to the lens of this light emitting device, the light from the LED is expanded while maintaining the angular distribution of the normal distribution in the direction (longitudinal direction) in which the V groove extends, but the direction orthogonal to the direction in which the V groove extends ( In the horizontal direction, the angular distribution is greatly depressed near the optical axis and expanded so as to rise steeply on both sides.
- a light emitting device it is desirable to emit light that is symmetric in any direction with respect to the optical axis, that is, light having no anisotropy, even if a light source having an asymmetric light emitting surface is used. Further, from the viewpoint of reducing the backlight height and reducing the cost of the light emitting device, it is desirable to be able to radiate light uniform in the circumferential direction while using a relatively small lens.
- the present invention provides a light emitting device capable of uniformizing and emitting light from a light source having an asymmetric light emitting surface in the circumferential direction while using a relatively small lens. It is an object of the present invention to provide a surface light source including a liquid crystal display device and a liquid crystal display device.
- the present invention provides a light emitting device that emits light around an optical axis, a light source having a light emitting surface extending in a first direction orthogonal to the optical axis, and light from the light source And a lens having a refractive power in a second direction orthogonal to the optical axis and the first direction larger than a refractive power in the first direction.
- the present invention provides a plurality of light emitting devices arranged in a plane and a state in which light emitted from one surface of the plurality of light emitting devices is diffused from the other surface.
- a surface light source comprising: a diffuser plate that radiates at a plurality of light emitting devices, wherein each of the plurality of light emitting devices provides the surface light source.
- the present invention provides a liquid crystal display device comprising a liquid crystal panel and the above surface light source disposed on the back side of the liquid crystal panel.
- the refractive power of the lens in the length direction of the light emitting surface of the light source is larger than the refractive power in the direction perpendicular thereto, the anisotropy of light from the light source is reduced by the lens. Is done. Therefore, according to the present invention, it is possible to radiate light from a light source having an asymmetric light emitting surface in the circumferential direction while using a relatively small lens.
- FIG. 1 is a plan view of a light-emitting device according to Embodiment 1 of the present invention.
- 2A is a cross-sectional view taken along line IIA-IIA in FIG. 1
- FIG. 2B is a cross-sectional view taken along line IIB-IIB in FIG. 3A to 3C are perspective views showing specific examples of the light source.
- Luminance distribution on the light emitting surface of the light source used in the light emitting device of FIG. 5A and 5B are plan views of a light emitting device according to a modification. The figure for demonstrating the light-emitting device of Examples 1-4 FIG.
- FIG. 7A is a graph showing the incident surface shape of the lens used in the light emitting device of Example 1, showing the relationship between R and sagAX, sagAY, and FIG. 7B shows the relationship between R and sagB showing the shape of the exit surface of the lens.
- Graph both Table 1 is graphed
- Illuminance distribution of the light emitting device of Example 1 Illuminance distribution of a light emitting device having the same configuration as in Example 1 except that the entrance surface of the lens is rotationally symmetric.
- FIG. 1 is a graph showing the incident surface shape of the lens used in the light emitting device of Example 1, showing the relationship between R and sagAX, sagAY
- FIG. 7B shows the relationship between R and sagB showing the shape of the exit surface of the lens.
- Graph both Table 1 is graphe
- FIG. 11A is a graph showing the shape of the entrance surface of the lens used in the light emitting device of Example 2, showing the relationship between R and sagAX, sagAY, and FIG. 11B shows the relationship between R and sagB showing the shape of the exit surface of the lens.
- FIG. 13A is a graph showing an incident surface shape of a lens used in the light emitting device of Example 3, and showing a relationship between R, sagAX, and sagAY.
- FIG. 13B shows an outgoing surface shape of the lens, and showing a relationship between R and sagB.
- FIG. 15A is a graph showing an incident surface shape of a lens used in the light emitting device of Example 4, and shows a relationship between R, sagAX, and sagAY, and FIG. 15B shows an emission surface shape of the lens, and showing a relationship between R and sagB.
- Graph Illuminance distribution of the light emitting device of Example 4 For Examples 1 to 4, a graph showing a sag difference curve in the region where the standard distance is 0.5 or more and an approximate straight line of this curve A graph showing that the range defined by the conditional expression and Examples 1 to 4 are within the range 19A is a graph showing the incident surface shape of a lens used in the light emitting device of Reference Example 1, and shows the relationship between R, sagAX, and sagAY.
- FIG. 19B is the illuminance distribution of the light emitting device of Reference Example 1.
- 20A is a graph showing an incident surface shape of a lens used in the light emitting device of Reference Example 2, and shows a relationship between R, sagAX, and sagAY.
- FIG. 20B is an illuminance distribution of the light emitting device of Reference Example 2.
- FIG. 6 is a diagram for explaining a light emitting device according to Example 5; 22A is a graph showing the incident surface shape of the lens used in the light emitting device of Example 5, showing the relationship between R and sagA, and FIG. 22B shows the emission surface shape of the lens, showing the relationship between R and sagBX, sagBY.
- Illuminance distribution of the light emitting device of Example 5 Illuminance distribution of a light emitting device having the same configuration as in Example 5 except that the exit surface of the lens is rotationally symmetric
- Configuration diagram of a surface light source according to Embodiment 2 of the present invention 26 is a partial sectional view of the surface light source of FIG. Illuminance distribution when the light emitting device of Example 1 is used with the surface light source of FIG. Illuminance distribution when a surface light source is composed of only LEDs for confirming the effect of the light emitting device of Example 1.
- the light emitting device 1 emits light in a substantially circular shape with an optical axis A as a center on an irradiated surface, for example, and includes a light source 2 and a lens 3 that radially expands light from the light source 2. Yes. That is, the directionality of light from the light source 2 is widened by the lens 3, thereby illuminating a wide range around the optical axis A on the irradiated surface.
- the illuminance distribution on the surface to be irradiated decreases substantially monotonically as the distance on the optical axis A reaches the maximum.
- the light source 2 has a light emitting surface 21 extending in a first direction orthogonal to the optical axis A. For this reason, anisotropic light is emitted from the light source 2.
- the first direction is referred to as the X direction
- the second direction orthogonal to the first direction and the optical axis A is referred to as the Y direction.
- a chip-like LED which is a light emitting element, is employed as the light source 2, and the light emitting surface 21 is configured by the flat surface of the LED.
- the shape of the light emitting surface 21 is not particularly limited as long as it extends in the X direction.
- the light emitting surface 21 may have a rectangular shape as shown in FIG. 3A, or may have an oval shape as shown in FIG. 3B.
- the light source 2 does not need to be comprised only by LED, for example, as shown to FIG. 3C, it is comprised by LED and the phosphor layer formed in the dome shape on LED, A phosphor layer
- the light emitting surface 21 may be configured by a three-dimensional surface.
- the light emission in the LED is light emission having no directivity, but the refractive index of the light emitting region is 2.0 or more.
- the interface method is affected by the refraction of the interface. The maximum intensity in the line direction and the greater the angle from the normal direction, the smaller the light intensity.
- the LED has directivity, and in order to illuminate a wide range on the irradiated surface, it is necessary to widen the directivity of light from the LED with the lens 3.
- FIG. 4 shows a luminance distribution on a line extending in the X direction through the optical axis A on the light emitting surface 21 of the light source 2 and a luminance distribution on a line extending in the Y direction through the optical axis A.
- the luminance distribution differs between the X direction and the Y direction. Specifically, the luminance distribution in the X direction is wider than the luminance distribution in the Y direction.
- the light source 2 emits light that is asymmetric with respect to the optical axis A, that is, light having anisotropy.
- the lens 3 is made of a transparent material having a predetermined refractive index.
- the refractive index of the transparent material is, for example, about 1.4 to 2.0.
- an epoxy resin, a silicon resin, an acrylic resin, a resin such as polycarbonate, a glass, or a rubber such as silicon rubber can be used.
- an epoxy resin or silicon rubber that has been conventionally used as a sealing resin for LEDs.
- the lens 3 includes an incident surface 31 that allows light from the light source 2 to enter the lens 3, and an output surface 32 that emits light that has entered the lens 3. have.
- the outermost diameter of the emission surface 32 defines the effective diameter of the lens 3.
- the lens 3 has a bottom surface 33 facing the exit surface 32 around the entrance surface 31.
- a ring portion 35 that projects radially outward is provided between the emission surface 32 and the bottom surface 33, and the periphery of the emission surface 32 is an outer surface that is substantially U-shaped in cross section of the ring portion 35.
- the outer peripheral edge of the bottom surface 33 are connected.
- the ring portion 35 can be omitted, and the peripheral edge of the emission surface 32 and the outer peripheral edge of the bottom surface 33 may be connected by an end surface having a linear cross section or an arc shape.
- the incident surface 31 is a continuous concave surface in this embodiment.
- the light source 2 is disposed away from the incident surface 31 of the lens 3.
- the emission surface 32 is a continuous convex surface that is rotationally symmetric with respect to the optical axis A.
- the annular bottom surface 33 surrounding the incident surface 31 is preferably flat.
- the light emitting surface 21 of the light source 2 is at the same position in the optical axis direction in which the flat bottom surface 33 and the optical axis A extend.
- the light from the light source 2 enters the lens 3 from the incident surface 31 and then exits from the exit surface 32 to reach the irradiated surface (not shown).
- the light emitted from the light source 2 is expanded by the refracting action of the entrance surface 31 and the exit surface 32 and reaches a wide range of the illuminated surface.
- the lens 3 also plays a role of uniforming the anisotropic light emitted from the light source 2 in the circumferential direction.
- the lens 3 is configured such that the refractive power in the Y direction is larger than the refractive power in the X direction.
- the incident surface 31 includes an anamorphic curved surface having different curvatures in the X direction and the Y direction, the refractive power in the Y direction is larger than the refractive power in the X direction.
- the entire entrance surface 31 is such a curved surface.
- the incident surface 31 has a vertex Q on the optical axis A.
- the incident surface 31 has a sag amount (the sign is negative from the vertex Q to the light source 2 side, the vertex is the distance along the optical axis A from the vertex Q to the point P on the incident surface 31).
- Sag amount in the X direction at a position separated from the optical axis A by the same distance R in the radial direction (that is, on the same circumference centered on the optical axis A).
- SagAX has a shape larger than the sag amount sagAY in the Y direction.
- the incident surface 31 may extend to the light source 2 side after retreating from the apex Q to the side opposite to the light source 2 so that the sag amount becomes positive in the vicinity of the optical axis A, but the sag amount extends over the entire area. It is preferable to extend only from the apex Q toward the light source 2 so as to be negative.
- the shape of the incident surface 31 is the curvature of the portion intersecting the optical axis A in the cross section in the X direction (1 / curvature radius) Cx. Can be expressed as smaller than the curvature Cy of the portion intersecting the optical axis A in the cross section in the Y direction.
- the anisotropy of light from the light source 2 is reduced by the lens 3. Accordingly, it is possible to radiate light from the light source 2 having an asymmetric light emitting surface 21 in the circumferential direction while using a relatively small lens 3.
- the sag difference sagD obtained by subtracting the sag amount sagAY in the Y direction from the sag amount sagAX in the X direction is preferably increased as the distance from the optical axis A increases. This is because luminance unevenness can be reduced even when a positional deviation in the rotational direction about the optical axis A occurs between the light source 2 and the lens 3.
- the sag difference sagD at that time is preferably increased toward the radially outer side so that the following conditional expression is satisfied.
- F is a light emitting surface length / shortness ratio which is a ratio (L / W) of the length L of the light emitting surface 21 in the X direction to the width W of the light emitting surface 21 in the Y direction
- S is a ratio from the optical axis A.
- the exit surface 32 that is rotationally symmetric with respect to the optical axis A does not necessarily have to be a convex surface as a whole.
- a portion near the optical axis may be a concave surface, and an outer portion thereof may be a convex surface.
- the optical axis vicinity part in the output surface 32 may be flat.
- the entrance surface 31 includes an anamorphic aspherical curved surface.
- the entrance surface 31 and the exit surface are used. It is sufficient that at least one of 32 includes an anamorphic aspherical curved surface.
- the entrance surface 31 may be a continuous concave surface that is rotationally symmetric with respect to the optical axis A, and the exit surface 32 may be a convex surface including an anamorphic aspheric surface.
- the incident surface 31 may be flat, and the light emitting surface 21 of the light source 2 may be optically bonded to the incident surface 31 via a bonding material. Further, when the incident surface 31 is flat, the incident surface 31 may not be rotationally symmetric but may have the same shape as the light emitting surface 21.
- both the entrance surface 31 and the exit surface 32 may include an anamorphic aspheric surface.
- the light emitting element used for the light source 2 is not necessarily an LED, and may be an organic EL, for example.
- Examples 1 to 5 of the light emitting device 1 are shown below as specific numerical examples of the present invention.
- FIG. 6 is a diagram for explaining the light emitting devices of Examples 1 to 4, and FIG. 21 is a diagram for explaining the light emitting device of Example 5.
- the entire surface of the incident surface 31 is an anamorphic curved surface and the lens 3 having a rotationally symmetric exit surface 32 is employed.
- the entire surface of the emission surface 32 is an anamorphic curved surface, and the lens 3 whose entrance surface 31 is rotationally symmetric is employed.
- sagB in FIG. 6 is a sag amount of the emission surface 32 at a position away from the optical axis A by a distance R.
- Q is the vertex on the optical axis A of the exit surface 32
- P is a point on the exit surface 32 at a distance R from the optical axis A
- sagBX is the sag amount (vertex) of the exit surface 32 in the X direction.
- SagBY is a sag amount of the exit surface 32 in the Y direction. The distance along the optical axis A from Q to the point P).
- sagA in FIG. 21 is the sag amount of the incident surface 31 at a position away from the optical axis A by the distance R.
- Example 1 employs a general-purpose LED in which the length of the light emitting surface 21 in the X direction is 2.60 mm and the width of the light emitting surface 21 in the Y direction is 1.00 mm as the light source 2, and the direction of light from the light source 2 This is a design example for the purpose of expanding the performance.
- the effective diameter of the lens 3 is 15 mm. Specific numerical values of Example 1 are shown in Table 1.
- FIG. 7A is a graph of R, sagAX, and sagAY in Table 1
- FIG. 7B is a graph of R and sagB of Table 1.
- FIG. 8 shows the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2 using the light emitting device of Example 1.
- FIG. 9 shows a case where a light emitting device having the same configuration as in Example 1 is used except that the incident surface of the lens is rotationally symmetric, and the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2.
- the illuminance distribution on the irradiated surface obtained by calculation is represented.
- Example 10 shows a light emitting device having the same configuration as in Example 1 except that the entrance surface of the lens is rotationally symmetric and the lens is enlarged to an effective diameter of 20 mm, and is covered at a position 23 mm away from the light emitting surface 21 of the light source 2. It represents the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged.
- the illuminance distribution on the irradiated surface is not so different between the X direction and the Y direction.
- the effective diameter of the lens is reduced to 15 mm, the illuminance distribution on the irradiated surface is greatly shifted between the X direction and the Y direction as shown in FIG.
- Example 1 since the lens 3 having a larger refractive power in the Y direction than that in the X direction is used, even if the effective diameter of the lens 3 is as small as 15 mm as shown in FIG.
- the illuminance distribution on the irradiation surface can be made similar in the X direction and the Y direction.
- Example 2 employs a general-purpose LED in which the length of the light emitting surface 21 in the X direction is 2.20 mm and the width of the light emitting surface 21 in the Y direction is 1.10 mm as the light source 2, and the direction of light from the light source 2 This is a design example for the purpose of expanding the performance.
- the effective diameter of the lens 3 is 15 mm.
- 11A and 11B show the incident surface shape and the output surface shape of the lens 3 used in the light emitting device of Example 2, respectively.
- FIG. 12 shows the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2 using the light emitting device of Example 2.
- the illuminance distribution on the irradiated surface can be made similar in the X direction and the Y direction.
- Example 3 employs a general-purpose LED in which the length of the light emitting surface 21 in the X direction is 2.07 mm and the width of the light emitting surface 21 in the Y direction is 1.17 mm as the light source 2, and the direction of light from the light source 2 This is a design example for the purpose of expanding the performance.
- the effective diameter of the lens 3 is 15 mm.
- 13A and 13B show the incident surface shape and the output surface shape of the lens 3 used in the light emitting device of Example 3, respectively.
- FIG. 14 shows the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2 using the light emitting device of Example 2.
- Example 14 similarly to Example 1, even in Example 3, even if the effective diameter of the lens 3 is as small as 15 mm, the illuminance distribution on the irradiated surface can be made similar in the X direction and the Y direction.
- Example 4 employs a general-purpose LED in which the length of the light emitting surface 21 in the X direction is 1.80 mm and the width of the light emitting surface 21 in the Y direction is 1.35 mm as the light source 2, and the direction of light from the light source 2 This is a design example for the purpose of expanding the performance.
- the effective diameter of the lens 3 is 15 mm.
- 15A and 15B respectively show the incident surface shape and the output surface shape of the lens 3 used in the light emitting device of Example 4.
- FIG. 16 shows the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2 using the light emitting device of Example 4.
- Example 16 similarly to Example 1, even in Example 4, even if the effective diameter of the lens 3 is as small as 15 mm, the illuminance distribution on the irradiated surface can be made similar in the X direction and the Y direction.
- the distance R from the light source A is normalized by the maximum diameter DY of the incident surface 31 in the Y direction, and the sag difference sagD having the standard distance of 0.5 or more is obtained.
- a curve as shown in FIG. 17 can be drawn.
- these curves are approximated to a straight line by the method of least squares, an approximate straight line represented by the equation described in FIG. 17 is obtained.
- the slopes of these approximate lines are plotted in FIG. 18, it can be seen that the above-described conditional expressions are satisfied in Examples 1 to 4.
- Reference Example 1 and Reference Example 2 that do not satisfy the conditional expressions described above are shown in FIG.
- the entire surface of the entrance surface 31 is an anamorphic curved surface, and the lens 3 whose exit surface 32 is rotationally symmetric is employed.
- the anamorphic level is large as shown in FIG. 19A, and in Reference Example 2, the anamorphic level is low as shown in FIG. 20A.
- the light emitting surface length / shortness ratio of the light source 2 is set to 2.0
- Reference Example 2 the light emitting surface length / shortness ratio of the light source 2 is set to 2.8.
- the effective diameter of the lens 3 is 11 mm.
- the illuminance distribution of the light emitting device of Reference Example 1 is as shown in FIG. 19B, and the illuminance distribution of the light emitting device of Reference Example 2 is as shown in FIG. 20B. From these figures, it can be seen that the distribution shape of light on the irradiated surface collapses at an anamorphic level where the above-described conditional expression is not satisfied.
- Example 5 employs a general-purpose LED in which the length of the light emitting surface 21 in the direction is 2.20 mm and the width of the light emitting surface 21 in the Y direction is 1.10 mm as the light source 2, and the directionality of light from the light source 2. This is a design example for the purpose of expanding the range.
- the effective diameter of the lens 3 is 11 mm. Specific numerical values of Example 5 are shown in Table 2.
- FIG. 22A is a graph of R and sagA in Table 2
- FIG. 22B is a graph of R, sagBX and sagBY in Table 2.
- FIG. 23 shows the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2 using the light emitting device of Example 5.
- FIG. 24 shows a case where a light emitting device having the same configuration as in Example 5 is used except that the exit surface of the lens is rotationally symmetric, and the irradiated surface is arranged at a position 23 mm away from the light emitting surface 21 of the light source 2.
- the illuminance distribution on the irradiated surface obtained by calculation is represented.
- Example 25 shows a light emitting device having the same configuration as in Example 5 except that the exit surface of the lens is rotationally symmetric and the lens is enlarged to an effective diameter of 18 mm, and is covered at a position 23 mm away from the light emitting surface 21 of the light source 2. It represents the illuminance distribution on the irradiated surface obtained by calculation when the irradiated surface is arranged.
- Example 5 since the lens 3 having a refractive power in the Y direction larger than that in the X direction is used, even if the effective diameter of the lens 3 is as small as 11 mm as shown in FIG.
- the illuminance distribution on the irradiation surface can be made similar in the X direction and the Y direction.
- FIG. 26 is a configuration diagram of the surface light source 7 according to Embodiment 2 of the present invention.
- the surface light source 7 includes a plurality of light emitting devices 1 described in the first embodiment, which are arranged in a plane, and a diffusion plate 4 arranged so as to cover these light emitting devices 1. Note that the light emitting devices 1 may be arranged in a matrix as shown in FIG. 26, or may be arranged in a staggered manner.
- the surface light source 7 includes a substrate 5 facing the diffusion plate 4 with the light emitting device 1 interposed therebetween.
- a light source 2 of each light emitting device 1 is mounted on the substrate 5.
- the bottom surface 33 of the lens 3 is joined to the substrate 5 via a support 55, and the reflection plate 6 is disposed on the substrate 5 so as to cover the substrate 5 while avoiding the light source 2.
- the bottom surface 33 of the lens 3 is not necessarily bonded to the substrate 5 via the support column 55, and may be directly bonded to the substrate 5.
- the support column 55 may be formed integrally with the lens 3.
- the light emitting device 1 irradiates one surface 4a of the diffusion plate 4 with light. That is, the one surface 4a of the diffusion plate 4 is the irradiated surface described in the first embodiment.
- the diffusing plate 4 radiates light irradiated on the one surface 4a in a state of being diffused from the other surface 4b.
- Each light emitting device 1 irradiates light having a uniform illuminance in a wide range on one surface 4a of the diffusion plate 4, and the light is diffused by the diffusion plate 4 so that there is little luminance unevenness in the surface.
- a surface light source is created.
- the light from the light emitting device 1 is scattered by the diffusion plate 4 and returns to the light emitting device side or passes through the diffusion plate 4.
- the light that returns to the light emitting device side and enters the reflection plate 6 is reflected by the reflection plate 6 and then enters the diffusion plate 4 again.
- Example 1 Five light emitting devices of Example 1 employing the lens 3 whose entire incident surface is an anamorphic curved surface are arranged on a straight line at a pitch of 60 mm and diffused to a position 23 mm away from the light emitting surface 21 of the light source 2.
- the illuminance distribution on the diffusion plate incident surface (one surface on the light emitting device side) obtained by calculation when the plate is arranged is shown. This is because fine waves are seen in the illuminance distribution, but the number of light rays to be evaluated is insufficient in executing the illuminance calculation.
- FIG. 29 shows the illuminance distribution on the entrance surface of the diffuser plate obtained by calculation when only 5 LEDs are arranged on a straight line at a pitch of 60 mm and the diffuser plate is placed 23 mm away from the surface of the LED.
- FIG. 30 is a configuration diagram of a liquid crystal display device according to Embodiment 3 of the present invention.
- This liquid crystal display device includes a liquid crystal panel 8 and the surface light source 7 described in the third embodiment, which is disposed on the back side of the liquid crystal panel 8.
- a plurality of light emitting devices 1 are arranged in a plane, and the light diffusing plate 4 is illuminated by these light emitting devices 1.
- the back surface (one surface) of the diffusion plate 4 is irradiated with light with uniform illuminance, and this light is diffused by the diffusion plate 4 to illuminate the liquid crystal panel 8.
- an optical sheet such as a diffusion sheet or a prism sheet is preferably disposed between the liquid crystal panel 8 and the surface light source 7. In this case, the light transmitted through the diffusion plate 4 is further diffused by the optical sheet to illuminate the liquid crystal panel 8.
Abstract
Description
図1ならびに図2Aおよび2Bに、本発明の実施の形態1に係る発光装置1を示す。この発光装置1は、例えば被照射面に、光軸Aを中心として略円形状に光を放射するものであり、光源2と、光源2からの光を放射状に拡張するレンズ3とを備えている。すなわち、光源2からの光の方向性がレンズ3で広げられ、これにより被照射面における光軸Aを中心とする広い範囲が照明される。被照射面の照度分布は、光軸A上が最大で周囲に行くほど略単調に減少する。
0.12(F-1)2≦S≦3log10F
式中、Fは、Y方向における発光面21の幅Wに対するX方向における発光面21の長さLの比(L/W)である発光面長短比であり、Sは、光軸Aからの距離RをY方向における入射面31の最大径DYで規格化し、この規格距離(R/DY)が0.5以上の領域のサグ差sagDの曲線を最小二乗法にて直線に近似したときの近似直線の傾きである(図17参照)。
なお、光軸Aに対して回転対称な出射面32は、必ずしも全体的に凸面となっている必要はなく、例えば光軸近傍部分が凹面、その外側部分が凸面になっていてもよい。あるいは、出射面32における光軸近傍部分はフラットになっていてもよい。
以下、本発明の具体的な数値例として、発光装置1の実施例1~5を示す。
実施例1は、光源2としてX方向における発光面21の長さが2.60mm、Y方向における発光面21の幅が1.00mmの汎用品のLEDを採用し、光源2からの光の方向性を広げることを目的とした設計例である。実施例1では、レンズ3の有効径が15mmとなっている。実施例1の具体的な数値を表1に示す。
実施例2は、光源2としてX方向における発光面21の長さが2.20mm、Y方向における発光面21の幅が1.10mmの汎用品のLEDを採用し、光源2からの光の方向性を広げることを目的とした設計例である。実施例2では、レンズ3の有効径が15mmとなっている。図11Aおよび11Bは、実施例2の発光装置に用いられるレンズ3の入射面形状および出射面形状をそれぞれ示す。図12は、実施例2の発光装置を用い、光源2の発光面21から23mm離れた位置に被照射面を配置したときの、計算で求めた被照射面での照度分布を表す。
実施例3は、光源2としてX方向における発光面21の長さが2.07mm、Y方向における発光面21の幅が1.17mmの汎用品のLEDを採用し、光源2からの光の方向性を広げることを目的とした設計例である。実施例3では、レンズ3の有効径が15mmとなっている。図13Aおよび13Bは、実施例3の発光装置に用いられるレンズ3の入射面形状および出射面形状をそれぞれ示す。図14は、実施例2の発光装置を用い、光源2の発光面21から23mm離れた位置に被照射面を配置したときの、計算で求めた被照射面での照度分布を表す。
実施例4は、光源2としてX方向における発光面21の長さが1.80mm、Y方向における発光面21の幅が1.35mmの汎用品のLEDを採用し、光源2からの光の方向性を広げることを目的とした設計例である。実施例4では、レンズ3の有効径が15mmとなっている。図15Aおよび15Bは、実施例4の発光装置に用いられるレンズ3の入射面形状および出射面形状をそれぞれ示す。図16は、実施例4の発光装置を用い、光源2の発光面21から23mm離れた位置に被照射面を配置したときの、計算で求めた被照射面での照度分布を表す。
実施例5は、光源2として方向における発光面21の長さが2.20mm、Y方向における発光面21の幅が1.10mmの汎用品のLEDを採用し、光源2からの光の方向性を広げることを目的とした設計例である。実施例5では、レンズ3の有効径が11mmとなっている。実施例5の具体的な数値を表2に示す。
図26は、本発明の実施の形態2に係る面光源7の構成図である。この面光源7は、平面的に配置された、実施の形態1で説明した複数の発光装置1と、これらの発光装置1を覆うように配置された拡散板4とを備えている。なお、発光装置1は、図26に示すようにマトリクス状に配置されていてもよいし、千鳥状に配置されていてもよい。
図30は、本発明の実施の形態3に係る液晶ディスプレイ装置の構成図である。この液晶ディスプレイ装置は、液晶パネル8と、液晶パネル8の裏側に配置された、実施の形態3で説明した面光源7とを備えている。
Claims (11)
- 光軸を中心として光を放射する発光装置であって、
前記光軸と直交する第1方向に延びる発光面を有する光源と、
前記光源からの光を放射状に拡張するレンズであって、前記光軸および前記第1方向と直交する第2方向の屈折力が前記第1方向の屈折力よりも大きなレンズと、
を備える、発光装置。 - 前記レンズは、前記光源からの光を該レンズ内に入射させる入射面と、該レンズ内に入射した光を出射させる出射面とを有し、
前記入射面と前記出射面の少なくとも一方がアナモフィックな非球面の曲面を含む、請求項1に記載の発光装置。 - 前記曲面は、前記光軸上に頂点を有しており、
前記頂点から前記曲面上の点までの前記光軸に沿った距離をサグ量(符号は前記頂点から前記光源側が負、前記頂点から前記光源と反対側が正)としたときに、
前記光軸から径方向に同じ距離だけ離れた位置では、前記第1方向におけるサグ量が前記第2方向におけるサグ量よりも大きい、請求項2に記載の発光装置。 - 前記出射面は、前記曲面を含む凸面であり、前記入射面は、前記光軸に対して回転対称な凹面である、請求項3に記載の発光装置。
- 前記入射面は、前記曲面を含む凹面であり、前記出射面は、前記光軸に対して回転対称な凸面である、請求項3に記載の発光装置。
- 前記第1方向におけるサグ量から前記第2方向におけるサグ量を引いたサグ差は、前記光軸から離れるにつれて大きくなる、請求項5に記載の発光装置。
- 前記第2方向における前記発光面の幅に対する前記第1方向における前記発光面の長さの比である発光面長短比をFとし、
さらに、前記光軸からの距離を前記第2方向における前記曲面の最大径で規格化し、この規格距離が0.5以上の領域の前記サグ差の曲線を最小二乗法にて直線に近似したときの近似直線の傾きをSとしたときに、
次の条件式
0.12(F-1)2≦S≦3log10F
が満たされる、請求項6に記載の発光装置。 - 前記光源は、発光素子と、この発光素子上にドーム状に形成された蛍光体層とを含み、前記蛍光体層の表面で前記発光面が構成されている、請求項1に記載の発光装置。
- 平面的に配置された複数の発光装置と、前記複数の発光装置を覆うように配置され、前記複数の発光装置から一方面に照射された光を他方面から拡散した状態で放射する拡散板と、を備える面光源であって、
前記複数の発光装置のそれぞれは、請求項1に記載の発光装置である、面光源。 - 前記複数の発光装置を挟んで前記拡散板と対向する基板であって前記複数の発光装置のそれぞれの前記光源が実装された基板と、前記光源を避けながら前記基板を覆うように前記基板上に配置された反射板と、をさらに備える、請求項9に記載の面光源。
- 液晶パネルと、前記液晶パネルの裏側に配置された請求項9に記載の面光源と、を備える液晶ディスプレイ装置。
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