TW201037230A - Lighting apparatus and display apparatus - Google Patents

Lighting apparatus and display apparatus Download PDF

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TW201037230A
TW201037230A TW99101215A TW99101215A TW201037230A TW 201037230 A TW201037230 A TW 201037230A TW 99101215 A TW99101215 A TW 99101215A TW 99101215 A TW99101215 A TW 99101215A TW 201037230 A TW201037230 A TW 201037230A
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Taiwan
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light
grating
convex
reflecting surface
reflection
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TW99101215A
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Chinese (zh)
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TWI375774B (en
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Yuuichi Suzuki
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Yuuichi Suzuki
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Priority claimed from JP2009030382A external-priority patent/JP4399678B1/en
Priority claimed from JP2010006184A external-priority patent/JP4681075B1/en
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Abstract

Color mixture by dispersion has difficult radiation angle control and low efficiency, therefore it realizes the lighting apparatus and the display apparatus which mix colors with control of radiation angle and in high efficiency. It sets up one diagonal of a lozenge-shaped refraction plane on base plane, and contacts each other in adjacent side of lozenge-shaped refraction plane in upward of base plane, and adjacent side of a lozenge-shaped refraction plane in the lower part, namely it becomes trigonal pyramid refraction grating with bump and hollow, and the grating inclination angle γ between normal line of a lozenge-shaped refraction plane and base plane, which is set by difference with incident angle α to refraction plane and refraction angle β. By the above structure, parallel light from light source of three directions enters into only each refraction plane of facing toward light source, and be refracted in a perpendicular direction of base plane, and be radiated in the same direction with mixing. The liquid crystal display apparatus which used the above, parallel light enters into the side of the light-guide plate which has trigonal pyramid refraction grating 4 in radiation surface and convex mirror 5 in base surface, three colors of parallel light expand flux of light by convex mirror, and reflect to trigonal pyramid refraction grating, and irradiate to the pixel which is consisted of lozenge-shaped sub-pixel.

Description

201037230 mirror 5 in base surface, three colors of parallel light expand flux of light by convex mirror, and reflect to trigonal pyramid refraction grating, and irradiate to the pixel which is consisted of > lozenge-shaped sub-pixel. 四、 指定代表圖·· (一) 本案指定代表圖為:第(20 )圖。 * (二) 本代表圖之元件符號簡單說明: 5A、5C:凸反射面 u 15A:折射面 24 :導光板 27A、27C:次像素 . 2 8 :液晶夾持基板 4 8 :偏光板 五、 本案若有化學式時,請揭示最能顯示發明特 ^徵的化學式: •六、發明說明: .【發明所屬之技術領域】 本發明是關於藉由構成格子狀的反射元件或折射元件 控制來自發光元件的光的射出方向,並改善混色特性之照 明裝置(llghting apparatus)及顯示裝置(display apparatus) ° 3 201037230 【先前技術】 半導體發光元件(semiconductor light emitting .ele«ient)因小型、高效率、長壽命、低電壓動作、高速響 •應等的優良的特徵而被廣泛地使用於各種顯示裝置、照明 裝置等。 • 液晶顯示裝置即使是由紅、綠、藍的3原色發光元件 .產生的不連續的光譜(spectrum)’因藉由3色的控制信號 顯示其中間色’故可利用使用3色的發光元件的3原色光。 ❹將3色的發光元件配設於圓錐内面並拉長後方散射的混色 距離之提案(圖40’專利文獻1)會使伴隨多重反射的吸收 増加並使效率降低。雖然有將3色的發光元件收納於同一 封裝(package) ’使接近發光元件的部分的反射鏡的斜度陡 • 峭’並緩和各發光元件與反射鏡的距離與角度的差異之提 •案(圖41,專利文獻2 ),但只能一部分得到均勻的混色。 很難使3色的發光元件在同一封裝内充份地混色,基於元 件的電源電壓不同等的理由,以下的螢光白色發光二極體 〇 (fluorescent white light emitting diode)常被使用。 . 將藍色發光二極體的藍色光照射到黃色螢光體,利用 補色的螢光白色發光二極體的光譜是由尖銳的藍色與平緩 • 的黃色域的兩個峰值(peak)構成(專利文獻3)。為紅色域 , 非常少,綠色也具有大的谷值(valley)之藍色強烈的光譜 特性。但是,因螢光白色發光二極體與3原色的混色比較 可簡單地製造,故當作行動電話等的液晶顯示裝置的背光 (back 1 ight)、LED燈泡等被利用。 4 201037230 由於半導體發光兀件的發光欵率的提高,比螢光燈小 型的發光二極體被應用於照明。因發光二極體其容許溫度 *上升比其他的光源小’得到大的光束需要多數個晶粒(ch i p ) 而價格高,故被重視效率成為藍色強烈的光譜。以藍色發 光二極體激發(excite)發光效率函數(ph〇t〇pic lumin〇us • efficiency function)最局的黃綠色附近的螢光體,將利 •用補色的螢光白色光使用於一般照明的情形,紅色域或谷 底波段的被照射體與連續光谱的白色光比較變暗。有混合 〇紅色螢光體等的方法或將釔的一部分置換成釓並移動 (shift)到長波長側’—邊改善現色性(c〇1〇r rendering),一邊提高效率之提案(專利文獻3)。 在來自白色光背光光源以彩色濾光片(c〇1〇r f i丨ter) ^刀解成3色時,2/3的光量藉由彩色濾光片吸收,效率降 低。不使用彩色濾光片而是使用3原色發光元件並加法混 色(additive mixture)的方法有在導光板配設與像素數相 同個數的45。的溝,重疊3層在溝的界面全反射於液晶面 0板方向的導光板之提案(圖42,專利文獻4)。 . 在複數個棒狀導光體的界面配設遮光層,遮蔽複數色 發光一極體的顏色區別的光並傳播於棒狀導光體内,不使 彩色濾光片將3色光供給至液晶條紋的方法被提出(圖 • 43,專利文獻5 )。 在液晶面板的3邊設置3色的光源,在導光板配設四 錐成矩陣狀’並藉由四角錐的斜度面照射到液晶面板的 定的像素之液晶顯示裝置被提出(圖44,專利文獻6)。 5 201037230 有使3原色的平行光傳播於配置凸反射面成梯田狀的 導光板並擴大光束於像素方向並反射,以反射/透射元件將 • 各色的反射光分配成條紋之提案(圖45,專利文獻7)。 . 因在頂角與谷角具有90。的角度的棱鏡(prism)的底 面由兩方向入射兩色的光’入射到入射角大的斜度面的光 • 將折射光混色並射出於同一方向,入射到入射角大的斜度 • 面的光變成臨界角以上並全反射,故返回到他方的光源。 為了活用返回的光線,使用帶通鏡(bandpass mirror)由其 ❹他的光源側射出的構造被提出(圖4 6,專利文獻8 )。 攝影用光源常被使用3波長冷陰極管(cold cathode tube),惟因各色的螢光材料為線光譜(Ηη6 Spectrum), 故波長特性的凹凸大,無法進行正確的色彩再現(c〇l〇r reproduction)。有因發光二極體的發光強度(iumin〇us intensity)成為尖峰(peak)的約半值的半值寬度(half value width)為20nm〜60nm,故使用6色〜9色涵蓋可見光 域之提案(專利文獻7)。 〇 顯示有透過將7種類的發光元件排列於基板中央附 • 近’封入比焦平面(focal plane)淺的位置的透鏡(iens) 内,以焦平面的散射材層混色,以各色的半峰值波長 • (half-peak wavelength)連接並形成白色光,以線光源轉 .換元件轉換當作掃描器(scanner)光源的應用。 〔專利文獻1〕日本國特開2 0 0 5-3 535 0 6號公報 〔專利文獻2〕日本國特開2004-87935號公報 〔專利文獻3〕日本國特許3246386號公報 6 201037230 〔專利文獻4〕日本國特開平6_59252號公報 〔專利文獻5〕曰本國特開平2 _丨丨丨9 2 2號公報 .〔專利文獻6〕日本國特開2006-323221號公報 〔專利文獻7〕日本國特許4114173號公報 〔專利文獻8〕日本國特開2008 — 218154號公報 馬 .【發明内容】 因藉由將3色的發光元件配置於同一封裝,使發光元 〇件附近的反射鏡的斜度陡峭等的構造混色的專利文獻1的 k案為自各發光元件到反射鏡的距離與角度不同,故產生 依照晶粒的排列的色斑。因利用正反射進行的混色很困 難’故藉由圓錐内面的散射層使其後方散射,長長地取散 ’射距離等的混色,故反射光返回到光源側,在多重反射時 被吸收,效率降低。 利用將藍色發光二極體的藍色光照射到黃色螢光體的 補色的白色發光二極體具有尖銳的光譜的藍色光與平緩的 〇黃色光的光譜,紅色域與青綠色域不足(專利文獻3)。隨 • 著螢光體的配合比率增大’藍色光的尖峰降低,螢光的尖 峰增大,螢光不照到行進方向的螢光體而透過的話就呈黃 . 色光’若照到別的黃色螢光體,則因螢光體為有色不透明, - 對螢光波長螢光轉換率低,故被吸收。若補償吸收提高螢 光體配合比率’則效率更降低。螢光白色發光二極體為使 效率優先,藍光光譜大的青白的光,平均現色評價數約 的現色性低的照明。 7 201037230 為了改善現色性’混合寬的波段的螢光體時需以依照 轉換效率(conversion efficiency )與發光效率函數的營 '光體的配合比率混合。因在發光效率函數、轉換效率 、 卞低的 .紅色等中’長波長螢光體的量增加,由長波長螢光體發出 的光在短波長螢光體中只被吸收不會被進行螢光轉換,故 -產生更增加螢光體的必要。黃色螢光照到黃色螢光體的機 .率與紅色螢光照到紅色螢光體的機率也增大,效率降低 因此,混合分散複數種的螢光體實現連續光譜的白色光有 〇效率降低的問題。 不使用彩色濾光片而是使用3原色發光元件並加法混 色的方法,在導光板配設與像素數相同個數的45。的溝此 重疊3層在溝的界面全反射於液晶面板方向的導光板之專 .利文獻4的提案因配設與次像素(subpixel)數相同個數的 -45°的斜度,故需晝面寬的1/3的厚度,在畫面寬3〇〇職 中每一層導光板需ΙΟΟπππ厚,由於加工條紋數的溝的工時 (man-hours)而變的昂貴。 在複數個棒狀導光 別 日 处暇颂色區 的光並傳播於棒狀導光體内,不使用彩色濾光片將 光供給至液晶條级之專利讀5的提案很難綑紫被 理的次像素寬的線狀導光構件而製造,若積層配設 的透光片,則片厚的公差累計,與液晶的像素尺寸 因擴散光傳播於以各遮光層隔開的透光材内,* 。 膜的情形為每次反射就被吸收而越遠越暗。 、、、一 在導光板配設多數個由四角錐構成的反射體,將來自 8 201037230 3方向的3原色光反射於像素並混色之專利文獻6的提案 被跟前的四角錐遮蔽,僅得到倒v型的反射光,若照射斜 •斜的平行光到四角錐,則也照到側面,故成為散射光人射 . 到其他的像素而變的不鮮明。 藉由配置凸反射面成梯田狀的導光板與反射/透射元 .件分配成條紋之專利文獻7的提案因使用構造不同的兩種 •類的導光元件’故需正確的對準。 交通號言志燈(trafflc light)的發光二極體因透鏡的 Ο指向性(directivity)宽,舍站,、自恶,|_ ,上 會破浪費地放射到上空等消耗電 流多’可看到交叉的道路側的㈣,故有許多三叉路等需 要遮光板的狀況。因有接受太陽光,非點亮的兩燈也變亮 的疑似點亮現象,故配設有遮蔽太陽光的遮光板。 . 目專利文獻8為以—方的傾斜折射面折射並朝底面的 -鉛直方向射出的構造,入射到成對的他方的折射面的光其 入射角為臨界角以上’故全反射並返回到他方的光源側。 藉由帶通鏡再反射全反射光並利用的話雖然可損失, 〇但是複雜且昂貴。 ' 若使薄長方形反射面的長轴方向正交於來自光源的平 行光的行進方向並配置於基準面上,使薄長方形反射面的 .短轴方向交互具有±30。的斜度並排列成三角波狀,則形成 有三角波狀反射光柵(refleetiQngrating)4。顯示三角波 狀反射光柵與在對稱位置配設平行光光源於在薄長方形反 射面的短軸方向斜上方30。的方向的構造於圖工。 因各個平行光光源與三角波狀光柵的成對的反射面平 9 201037230 行,故無法入射於配置於成對的平行光光源側的反射面, 來自距水平面30。上方的平行光光源 一 叉万的平仃光沿著 •二肖波狀反射鏡的光源方向反射面入#。若對向於反射面 •的光源的平行光入射到反射面,則由雙方入射的 到鉛直上方。 . 若設三角波狀光栅的斜度及傾斜光的斜度角度為“, •斜度面的法線與鉛直方向所構成的角度為石,則如公式 1 ’斜度α、石為30。。 [公式1 ] 2α+]3 = α + 20 = 9Ο° ·_·α = β = 3 0〇 來自左右平行光光源的反射光都成為依照光源侧的反 .射面的梳子形,來自左右的平行光為交互排列成梳子形的 -反射光。若作成無法以肉眼辨識光柵間距(pi tch)的尺寸的 條紋並使左右的平行光光源成別色的兩色,則被進行併設 加法混色。 〇 為了使射出光成擴散光或收斂光,可並用透鏡、反射 ,鏡等並控制放射角(radiation angle),惟即使不根據透鏡 也fb错由將光柵反射面製作成曲面而控制放射角。顯示以 •凸反射面5形成反射光柵並擴大光束的狀態的側視圖於圖 2。若成對的曲面的放射角方向不相等,則因看的方向而成 為僅一方的成分而產生色斑。在圖2中,光柵的谷部中的 左側光源光的反射光與光柵的頂部中的右側光源光的反射 光成平行,光柵的頂部中的左側光源光的反射光與光栅的 201037230 谷部中的右側光源光的反射光也成平行。即使是擴散光也 透過在該範圍内左右的光成對平行地射出而被均等混合。 • 顯示為了決定距鉛直方向的放射角7的入射光的斜度α、 * 頂部斜度α、谷部斜度点的關係於公式2與圖3。 [公式2 ] % 召=45。一α/2 + γ/2 n 在放射角r=6。中,α=28。 ,/5=34。,在放射角r 〇-30中,α=20° ,冷=50° 。照明裝置除了該放射角7外 也需加上由發光元件尺寸產生的誤差角度0。 若在拋物面鏡6的焦點設置發光元件1,則可得到平 行光’但因發光二極體的晶粒尺寸為各邊約2 5 〇 μ m,故由 於配設於拋物面鏡的焦點的發光元件的尺寸,由中心部與 '周邊部發出的光產生光程差,具有距圖4所示的平行光的 誤差。距由外周部發出的平行光的誤差角度Θ是藉由發光 元件的中心到外周部的長度r、拋物面鏡的座標m (X,y )、 〇焦距p以公式3表示’為了減小誤差角度0需加大焦距。 [公式3 ] e^tan"1 {(p-x) / (y-r)} - t a n"1 {(p-x) /y} ’ 顯示為了使用三角波狀光柵混合3色,在傾斜反射面 - 的底部設有透光性的開口部的構造於圖5。為了不使傾斜 光照到開口部’需藉由公式4使反射面的斜度0 s成為3 5. 3 [公式4 ] 201037230 t a η θ r= t a n (tc/2 — 2 · Θβ) 〇 t ( 2 ^ Θ β)201037230 mirror 5 in base surface, three colors of parallel light expand flux of light by convex mirror, and reflect to trigonal pyramid refraction grating, and irradiate to the pixel which is consist of > lozenge-shaped sub-pixel. Figure·· (1) The representative representative of the case is: (20). * (2) A brief description of the symbol of the representative figure: 5A, 5C: convex reflecting surface u 15A: refractive surface 24: light guide plate 27A, 27C: sub-pixel. 2 8 : liquid crystal holding substrate 4 8 : polarizing plate 5 If there is a chemical formula in this case, please disclose the chemical formula that best shows the characteristics of the invention: • Sixth, the invention description: [Technical field of the invention] The present invention relates to controlling the light emission from the reflective element or the refractive element constituting the lattice shape A llghting apparatus and a display apparatus for improving the color-emitting direction of a component, and a display apparatus. 3 3, 2010, 372. [Prior Art] A semiconductor light emitting device (semiconductor light emitting .ele«ient) is small, high-efficiency, It is widely used in various display devices, illumination devices, and the like because of its excellent characteristics such as long life, low voltage operation, high speed response, and the like. • The liquid crystal display device uses a three-color light-emitting element even if it is a discontinuous spectrum generated by three primary color light-emitting elements of red, green, and blue, because the intermediate color is displayed by the three-color control signal. 3 primary colors of light. In the case where the three-color light-emitting elements are disposed on the inner surface of the cone and the color mixture distance of the back scattering is elongated (Fig. 40' Patent Document 1), the absorption accompanying the multiple reflection is increased and the efficiency is lowered. Although it is possible to store the three-color light-emitting elements in the same package, the slope of the mirror close to the light-emitting element is steep and steep, and the difference between the distance and angle of each light-emitting element and the mirror is relaxed. (Fig. 41, Patent Document 2), but only a part of them can be uniformly mixed. It is difficult to sufficiently mix the three color light-emitting elements in the same package, and the following fluorescent white light emitting diodes are often used for reasons such as the difference in the power supply voltage of the elements. The blue light of the blue light-emitting diode is irradiated to the yellow phosphor, and the spectrum of the fluorescent white light-emitting diode using the complementary color is composed of two peaks of a sharp blue and a gentle yellow field. (Patent Document 3). It is a red domain, very few, and green also has a strong blue spectral characteristic of large valleys. However, since the fluorescent white light-emitting diode can be easily manufactured in comparison with the color mixture of the three primary colors, it is used as a backlight (backlight) of a liquid crystal display device such as a mobile phone or the like, and an LED bulb or the like. 4 201037230 Due to the increase in the luminous efficiency of semiconductor light-emitting devices, light-emitting diodes smaller than fluorescent lamps are used for illumination. Since the allowable temperature of the light-emitting diode is *the rise is smaller than that of other light sources. A large beam requires a large number of crystal grains (ch i p ) and is expensive, so that the efficiency is considered to be a strong blue spectrum. The fluorescent body near the yellow-green color with the excite luminous efficiency function (ph〇t〇pic lumin〇us • efficiency function) of the blue light-emitting diode is used to supplement the fluorescent white light with complementary color. In the case of general illumination, the illuminated body of the red or valley band is darker than the white light of the continuous spectrum. A method of mixing a magenta phosphor or the like, or replacing a part of the crucible with a crucible and shifting it to the long wavelength side to improve the color rendering property (c〇1〇r rendering) Document 3). When the color filter (c〇1〇r f i丨ter) is cut into three colors from the white light backlight source, 2/3 of the light amount is absorbed by the color filter, and the efficiency is lowered. Instead of using a color filter, a method of using three primary color light-emitting elements and adding additive mixture is provided in the light guide plate with the same number of pixels as 45. The groove is a proposal of superimposing three layers of the light guide plate on the liquid crystal surface in the direction of the 0-plate at the interface of the groove (Fig. 42, Patent Document 4). A light shielding layer is disposed at an interface of the plurality of rod-shaped light guides to shield the light of the color difference of the plurality of light-emitting ones and propagate in the rod-shaped light guide body, so that the color filter does not supply the three colors of light to the liquid crystal A method of streaking is proposed (Fig. 43, Patent Document 5). A liquid crystal display device in which a three-color light source is provided on three sides of a liquid crystal panel, and a four-cone is arranged in a matrix shape on the light guide plate, and a predetermined pixel of the liquid crystal panel is irradiated by a sloped surface of the quadrangular pyramid is proposed (FIG. 44, Patent Document 6). 5 201037230 There is a proposal to spread parallel light of three primary colors to a light guide plate in which a convex reflecting surface is arranged in a terrace shape, and to expand and reflect the light beam in the pixel direction, and to distribute the reflected light of each color into stripes by the reflection/transmission element (Fig. 45, Patent Document 7). Because there are 90 in the apex angle and the valley angle. The bottom surface of the prism is incident on both sides of the light of two colors incident in two directions. The light incident on the slope of the incident angle is large. The refracted light is mixed and emitted in the same direction, and is incident on the slope of the incident angle. The light becomes above the critical angle and is totally reflected, so it returns to the other source. In order to utilize the returned light, a configuration in which a bandpass mirror is used to emit light from the side of the light source is proposed (Fig. 4, Patent Document 8). A three-wavelength cold cathode tube is often used as a light source for photography. However, since the fluorescent material of each color is a line spectrum (Ηη6 Spectrum), the unevenness of the wavelength characteristics is large, and accurate color reproduction cannot be performed (c〇l〇). r reproduction). The half value of the iumin〇us intensity of the light-emitting diode becomes a half value of the peak, and the half value width is 20 nm to 60 nm. Therefore, the use of 6 colors to 9 colors covers the visible light region. (Patent Document 7). 〇In the lens (iens) in which seven kinds of light-emitting elements are arranged in the center of the substrate and enclosed in a shallower focal plane, the color of the scattering layer in the focal plane is mixed, and the half-peak of each color is displayed. The wavelength of (half-peak wavelength) is connected to and forms white light, which is used as a light source for converters. [Patent Document 1] Japanese Patent Laid-Open Publication No. JP-A-2004-87935 (Patent Document 3) Japanese Patent No. 3246386 No. 6 201037230 [Patent Literature Japanese Patent Laid-Open No. Hei. No. Hei. No. 2006-323221 (Patent Document 6) Japanese Patent Publication No. 2006-323221 (Patent Document 7) Japanese Patent Laid-Open No. Hei. No. 2008-218154. [Summary of the Invention] Since the light-emitting elements of three colors are arranged in the same package, the inclination of the mirror in the vicinity of the light-emitting element element is obtained. The k case of Patent Document 1 in which structural color mixing such as steepness is different from the distance from the respective light-emitting elements to the mirror, and thus a color unevenness according to the arrangement of the crystal grains is generated. It is difficult to mix colors by regular reflection. Therefore, the scattering layer on the inner surface of the cone is used to scatter back, and the color mixture such as the distance of the emission is longly dispersed. Therefore, the reflected light returns to the light source side and is absorbed during multiple reflection. Reduced efficiency. A white light-emitting diode that illuminates a complementary color of a blue light-emitting diode to a yellow phosphor has a sharp spectrum of blue light and a gentle yellow-yellow spectrum, and the red and cyan domains are insufficient (patent Document 3). With the increase of the blending ratio of the phosphor, the peak of the blue light is lowered, the peak of the fluorescent light is increased, and the fluorescent light is yellow when it passes through the fluorescent body in the traveling direction. In the case of a yellow phosphor, the phosphor is colored and opaque, and the fluorescence conversion rate to the fluorescent wavelength is low, so it is absorbed. If the compensation absorption increases the phosphor blending ratio, the efficiency is further lowered. The fluorescent white light-emitting diode is a light-lighting illumination with a light-emitting blue light having a large blue light spectrum and an average color rendering. 7 201037230 In order to improve the color rendering, the phosphor of a wide-band mixture is mixed with a blending ratio of the luminous efficiency in accordance with the conversion efficiency and the luminous efficiency function. Since the amount of the long-wavelength phosphor increases in the luminous efficiency function, the conversion efficiency, the degraded red color, etc., the light emitted by the long-wavelength phosphor is absorbed only in the short-wavelength phosphor and is not subjected to the firefly. Light conversion, so - the need to increase the amount of phosphors. The yellow fluorescent light is illuminated to the yellow phosphor. The rate and the red fluorescent light are also increased to the red fluorescent body, and the efficiency is lowered. Therefore, mixing and dispersing a plurality of kinds of phosphors realizes a continuous spectrum of white light with reduced efficiency. problem. Instead of using a color filter, a method of using three primary color light-emitting elements and adding color mixing is used, and the light guide plate is provided with the same number of pixels as 45. The groove is superimposed on the light guide plate in which the interface of the groove is totally reflected in the direction of the liquid crystal panel. The proposal of Document 4 is to provide a slope of -45° which is the same as the number of subpixels. The thickness of 1/3 of the width of the face is required to be ΙΟΟπππ thick in each of the three layers of the screen width, which is expensive due to the man-hours of the groove in which the number of stripes is processed. In the case of a plurality of rod-shaped light guides, the light in the bleed area is propagated in the rod-shaped light guide body, and the patent reading 5 which does not use the color filter to supply light to the liquid crystal strip level is difficult to bind the purple quilt. It is manufactured by a linear light guide member having a wide sub-pixel width. When the light-transmissive sheet is laminated, the tolerance of the sheet thickness is integrated, and the pixel size of the liquid crystal is transmitted by the diffused light to the light-transmitting material separated by the respective light-shielding layers. Inside,* . The case of the film is that each reflection is absorbed and the farther and darker. In the light guide plate, a plurality of reflectors composed of a quadrangular pyramid are disposed, and the proposal of the patent document 6 in which the three primary colors of light from the direction of the 3, 2010, 372, 30 are reflected and mixed with the color is masked by the square pyramid, and only the inverted When the reflected light of the v-type illuminates the oblique and oblique parallel light to the quadrangular pyramid, it also shines on the side surface, so that it becomes a scattered light person. It becomes unclear to other pixels. Patent Document 7 in which a light-conducting plate having a convex reflecting surface and a reflecting/transmissive element are arranged in a stripe shape is proposed to be correctly aligned by using two types of light guiding elements of different configurations. The light-emitting diode of the traffic light (trafflc light) is wide because of the directivity of the lens, the station is stationed, and the self-destructive, |_, the waste current is radiated to the sky and the current consumption is large. In the case of (4) on the side of the intersection, there are many conditions such as a three-way road that requires a visor. Because of the acceptance of the sun, the two lights that are not lit are also lit up, so there is a visor that shields the sun. Patent Document 8 is a structure in which a slanted refracting surface is refracted toward the bottom surface in a vertical direction, and light incident on a pair of other refracting surfaces has an incident angle of a critical angle or more, so total reflection and return to Other side of the light source. By using a band-pass mirror to reflect the total reflected light and using it, it can be lost, but it is complicated and expensive. When the long-axis direction of the thin rectangular reflecting surface is orthogonal to the traveling direction of the parallel light from the light source and is arranged on the reference surface, the short-axis direction interaction of the thin rectangular reflecting surface is ±30. The slopes are arranged in a triangular wave shape, and a triangular wave-shaped reflection grating 4 is formed. The triangular wave-shaped reflection grating is arranged to be disposed at a symmetrical position with a parallel light source 30 obliquely above the short axis direction of the thin rectangular reflecting surface. The direction of the construction is in the drawing. Since the pair of reflecting surfaces of the parallel light source and the triangular wave grating are horizontally 9 201037230, they cannot enter the reflecting surface disposed on the side of the pair of parallel light sources, and are located from the horizontal plane 30. The parallel light source above is a flat light that is reflected by the light source in the direction of the light source of the two chord mirrors. When the parallel light of the light source directed to the reflecting surface is incident on the reflecting surface, it is incident on both sides vertically. If the slope of the triangular wave grating and the slope angle of the oblique light are ", • the angle formed by the normal of the slope plane and the vertical direction is stone, then the slope 1 and the stone are 30 as in Equation 1. [Formula 1] 2α+]3 = α + 20 = 9Ο° ·_·α = β = 3 0 The reflected light from the left and right parallel light sources becomes the comb shape according to the opposite side of the light source side, from the left and right The parallel light is a reflected light that is alternately arranged in a comb shape. If a stripe of a size that cannot recognize the grating pitch (pi tch) is visually recognized and the left and right parallel light sources are made into two colors of different colors, additive color mixing is performed. In order to make the emitted light into diffused light or convergent light, a radiation angle can be controlled by using a lens, a reflection, a mirror, or the like in combination, but the radiation angle can be controlled by making the grating reflection surface a curved surface without depending on the lens. A side view showing a state in which the reflection grating is formed by the convex reflection surface 5 and the light beam is enlarged is shown in Fig. 2. When the radiation angle directions of the pair of curved surfaces are not equal, the color direction is caused by only one component due to the direction of the viewing. In Figure 2, in the valley of the grating The reflected light of the left side source light is parallel to the reflected light of the right side source light in the top of the grating, and the reflected light of the left side source light in the top of the grating is also parallel to the reflected light of the right side source light in the valley of the 201037230. Even if the diffused light is emitted in parallel through the light in the range, the light is uniformly mixed in pairs. • The inclination α of the incident light to determine the radiation angle 7 from the vertical direction is displayed, and the top slope α and the valley are displayed. The slope point is related to Equation 2 and Figure 3. [Formula 2] % Call = 45. One α/2 + γ/2 n In the radiation angle r = 6, α = 28, /5 = 34. In the radiation angle r 〇-30, α=20°, cold=50°. In addition to the radiation angle 7, the illumination device needs to add an error angle of 0 caused by the size of the light-emitting element. If the focus is set at the focus of the parabolic mirror 6 In the case of the element 1, the parallel light can be obtained. However, since the crystal grain size of the light-emitting diode is about 25 μm on each side, the size of the light-emitting element disposed at the focus of the parabolic mirror is from the center portion and the periphery. The light emitted by the portion produces an optical path difference with an error from the parallel light shown in Figure 4. The error angle 平行 of the parallel light emitted from the periphery is the length r from the center to the outer circumference of the light-emitting element, the coordinates m (X, y) of the parabolic mirror, and the focal length p of the 以 are expressed by the formula 3 'in order to reduce the error angle 0 Increase the focal length. [Equation 3] e^tan"1 {(px) / (yr)} - ta n"1 {(px) /y} ' Displayed in order to mix 3 colors with a triangular wavy grating, on a tilted reflective surface - The structure in which the translucent opening is provided at the bottom is shown in Fig. 5. In order not to incline the light to the opening portion, the inclination 0 s of the reflecting surface is required to be 3 5. 3 [Formula 4] 201037230 ta η θ r= tan (tc/2 — 2 · Θβ) 〇t ( 2 ^ Θ β)

—__G ° t a θ s" 1 2 c 〇 t Θ S =t a n0s/2 ** t a ϊι 2 0g= 1/2 6s=tan-1 ·=3:5_26。 (1/2/-2) =19.47* • 目入射&的斜度^有19.5° ’故轉換成平行光的光 ,源部的厚度方向的尺寸變大,適合前方的光源部的尺寸不 會影響的投影機(projector)等。 〇 與藉由來自左右平行光光源的反射光交互排列成梳子 形的反射光進行併設加法混色者一樣’若藉由斜度為3〇。 的二角錐反射面將3方向的平行光反射到錯直方向,則會 以正三角形配置的三角排列(delta arrange)混合並射 出。照射到二角錐反射面的光源如圖6所示由於是配置於 ' 3方向,朝基準面向下30。照射的配置,故各反射面無來 自對向的光源以外的入射’為不會被跟前的三角錐遮蔽的 構造。由於是與三角波狀光栅同一的斜度面,在基準面錯 ¢)直方向以3色的混色光當作平行光射出,故可當作3原色 . 顯示裝置的光源等利用。若以凸型與凹型構成三角錐,則 上下的三角形連結’朝3方向的斜度面的形狀如圖2所示 • 為組合菱形者。圖6是以虛線表示三角錐的基準面,以〇 • 表示凸型三角錐的頂部,以•表示凹型三角錐的谷部。 三角波狀光柵也能以折射面構成,顯示藉由由兩個方 向入射並構成三角波狀的面折射,以平行光射出的狀態於 圖7。設折射光栅(refractive grating)構成物質的折射 12 201037230 率為n2 ’周圍介質(medium)的折射率為,由右侧光源以 入射角α入射到折射光柵的右側斜度面的光藉由公式5〇) •的司乃耳定律(Snell ’ s law)以折射角彡折射。因平行地 . 入射到三角波狀折射光栅的斜度面角度對令心線以7成對 的折射面,右側光源光只入射到右側斜度面,因斜度面與 *入射光對稱’故左側光源光也一樣。藉由如公式5(2)所示 .以石與α的差設定三角波狀折射光栅的斜度面角度r ,雙 方的折射光平行地射出到中心線。因若以角度δ由左右對 〇稱地入射到折射光栅的水平面’則以角度α入射到折射 面,故會混色並以平行光射出。 [公式5 ] (1) (2) (3) n2 s i η α = η i s i η j3 7 = /3-α n2s iny = nlS ΐηδ 丙烯酸曱酯 顯不代表的透光高分子的聚曱基 (polymethylmethacrylate:PMMA)與 聚 (p〇lyCarb〇nate:PC)中的 α 、 0 r 、占的 碳 酸 酯 例子。—__G ° t a θ s" 1 2 c 〇 t Θ S = t a n0s/2 ** t a ϊι 2 0g= 1/2 6s=tan-1 ·=3:5_26. (1/2/-2) =19.47* • The inclination of the incident angle &amp is 19.5°. Therefore, the light converted into parallel light has a larger size in the thickness direction of the source portion, and the size of the light source unit suitable for the front is not Projectors that will be affected, etc.进行 It is the same as the reflected light that is alternately arranged in a comb shape by the reflected light from the left and right parallel light sources, and is set to be the same as if the slope is 3〇. The dichroic reflecting surface reflects the parallel light in the three directions to the wrong direction, and then mixes and emits in a delta arrangement of equilateral triangles. The light source that is incident on the cube-cone reflecting surface is disposed in the '3 direction as shown in Fig. 6 and faces downward 30 toward the reference surface. Since the arrangement of the illumination is such that the incident surface other than the opposite light source is not shielded by the triangular pyramid. Since the gradient plane is the same as the triangular wavy grating, and the mixed color light of three colors is emitted as parallel light in the straight direction in the reference plane, it can be used as the three primary colors. The light source of the display device or the like is used. If the triangular pyramid is formed by a convex shape and a concave shape, the shape of the inclined surface in the three directions of the upper and lower triangular joints is as shown in Fig. 2 • It is a combination diamond. Fig. 6 is a datum line showing the reference surface of the triangular pyramid, and 〇 • indicates the top of the convex triangular pyramid, and • indicates the valley of the concave triangular pyramid. The triangular wavy grating can also be formed by a refracting surface, and is shown in Fig. 7 in a state in which the plane light is incident by two directions and forms a triangular wave. Refractive grating (refractive grating) constitutes the refraction of the material 12 201037230 is n2 'the refractive index of the surrounding medium (medium) is the light incident on the right oblique plane of the refractive grating by the right side light source at the incident angle α by the formula 5 〇) • Snell's law is refracted by the refraction angle 彡. In parallel, the angle of the oblique plane incident on the triangular wave-shaped refractive grating is 7 pairs of refractive surfaces of the core line, and the right side light source is incident only on the right inclined surface, because the sloped surface is symmetric with the *incident light, so the left side The light source is the same. By setting the slope angle r of the triangular wave-shaped refractive grating with the difference between the stone and α as shown in the formula 5 (2), the refracted light of both directions is emitted in parallel to the center line. If the angle δ is incident on the horizontal plane of the refractive grating by the right and left symmetry, it is incident on the refractive surface at an angle α, so that it is mixed and emitted as parallel light. [Formula 5] (1) (2) (3) n2 si η α = η isi η j3 7 = /3-α n2s iny = nlS ΐηδ Polymethylmethacrylate of light-transmitting polymer not represented by decyl acrylate :PMMA) and α, 0 r in poly(p〇lyCarb〇nate: PC), examples of carbonates.

折射先栅並使射出方向一致,則如圖 8所示可將來自3方6从上 則如圖 万向的先混色。三角錐的3 度都是對中心線為r ,氺A 〇 斜度面角 來自3方向的平行光斑底 入射角為(5。因藉由麻;4二6 ''底面構成的 由底面折射的光僅入射到行進方向的 201037230 面並平行於其他的兩面,故不入射。® 8為在來 右側的光源Α的平行光Α藉由底面折射後,以入 射到一角錐的左側的折射面並折射後射出於鉛直 .來自配置於左邊裏面的光源、B❸平行光B藉由 後藉由二角錐的右側的折射面折射後射出於鉛 •在來自配置於左手前側的光源c的平行光c藉由 •後,藉由二角錐的裏面側的折射面折射後射出 向。裏+面側的折射面在圖8中成陰影。 〇 若在基準面上排列複數個三角錐於同一方向 -角錐折射面將3方向的平行光折射混合並射出 向而准在基準面上會產生朝與前述三角錐的方 向的一角形的空間。即使在該空間上配設凸的三 ‘、、、法使折射光射出於鉛直方向’在該空間配設比 •陷的凹型三角冑’若以前述凸型三角錐與凹型三 的話則上下的二角形連結,傾斜的折射面的形 所不為組合菱形者。亦即為如下的構造:藉由將菱 〇的-方的對角線設於基準面i,接觸排列比基準 .角線還上側的菱形折射面的接鄰的邊,在比基準 成凸型的三角錐折射光柵’接觸排列比對角線還 ;折射面的接鄰的邊,形成比基準面凹陷的凹型 •折射光柵,以朝折射面的入射角與折射角的差分 定菱形折射面與基準面的法線構成的斜度角,以 周圍介質大的物質構成三角錐折射光柵’並由高 射出到低折射率側。來自3方向的平行光光源的 自配置於 射角α入 方向,在 底面折射 直方向, 底面折射 於鉛直方 ,則藉由 於鉛直方 向相反方 角錐,也 基準面四 角錐構成 狀如圖9 形折射面 面上的對 面還上形 下侧的菱 的三角錐 的角度設 折射率比 折射率側 平行光各 201037230 I僅入射到對向於光源的側的折射面’並折射於基準面的 鉛直上方,可使其與射出方向一致而漏合。 • ® 9是以虛線表不三角錐的底面,以。表示凸型三角 •錐的頂部’以♦表示凹型三角雜的谷部。折射面的形狀為 菱形’惟由於是組合凸型三角錐與凹型三角錐的構造,故 .擬稱為二角錐折射光柵4。若以凸型三角錐與凹型二角錐 •構成’則可不浪費地將平行光照射到對向於平行光的菱形。 照射到三角錐折射面的光源如圖8所示由於是配置於 〇 3方肖’朝基準面以仰角以上述占的角度照射的配置,故 為各折射面無來自對向的光源以外的入射,不會被跟前的 三角錐遮蔽的構造。因在基準面的垂直方向以3色的混色 光當作平行光射出,故可利用於3原色顯示裝置的光源等。 :射到折射光栅的光為平行光的情形需為了在顯示裝 y面配設複數個平行光光源的大的空間,針 造,明二 錐折射光栅並薄型化的構 …。右在導光板的射出面側形 G在導光板的底面形成凸反射面5 斤=:4, •傾斜的平行光入射到凸反射面5將由導先板側面對底面By refracting the first grid and making the directions of the shots uniform, as shown in Fig. 8, the first color mixture from the three sides can be seen from the top. The 3 degrees of the triangular cone are the center line r, and the 氺A 〇 slope angle is from the 3 direction of the parallel spot bottom incident angle (5. Because of the bottom surface of the light; 4 2 6 '' bottom surface It is incident only on the 201037230 plane of the traveling direction and parallel to the other two sides, so it is not incident. The 8 is the parallel pupil of the light source 右侧 on the right side, and is refracted by the bottom surface, and is incident on the refractive surface of the left side of the corner cone and refracted. The rear shot is straight. The light source from the left side is arranged, and the B parallel light B is refracted by the refractive surface on the right side of the pyramid and then emitted from the lead. The parallel light c from the light source c disposed on the front side of the left hand is used. • After that, the refracting surface on the inner side of the pyramid is refracted and then emitted. The refracting surface on the inner + side is shaded in Fig. 8. 〇 If a plurality of triangular pyramids are arranged on the reference plane in the same direction - the pyramidal refractive surface The three directions of parallel light are refracted and mixed to emit a space which is oriented toward the reference plane in a direction perpendicular to the direction of the triangular pyramid. Even if the space is provided with a convex three', Shot in the vertical direction' In the space, the concave triangular ridges of the concave-shaped triangular ridges are connected to each other by the upper and lower ridges, and the shape of the inclined refracting surfaces is not the combination of the diamonds. : By setting the diagonal of the square of the diamond to the reference plane i, the contact is arranged adjacent to the adjacent side of the rhombic refractive surface on the upper side of the reference angle, and the triangular pyramidal refractive grating is convex toward the reference. The contact arrangement is more than the diagonal line; the adjacent side of the refractive surface forms a concave/refractive grating recessed from the reference surface, and the difference between the incident angle of the refractive surface and the angle of refraction and the normal of the reference surface The slope angle is such that the material having a large surrounding medium constitutes a triangular pyramidal refractive grating 'and is emitted from the high to the low refractive index side. The parallel light source from the three directions is self-disposed in the direction of the angle of incidence α, and is refracted in the straight direction at the bottom surface. The bottom surface is refracted to the vertical direction, and the angle of the reference square pyramid is also formed by the angle of the triangular pyramid which is opposite to the upper side of the refractory surface on the refracting surface of the 9-shaped refractive surface. Each side of the rate side parallel light 201037230 I is incident only on the refracting surface of the side opposite to the light source and is refracted vertically above the reference plane to make it coincide with the exit direction. • ® 9 is a triangular cone with a dotted line. The bottom surface of the convex triangle is the top of the cone. The y indicates the valley of the concave triangular polygon. The shape of the refractive surface is a diamond shape. However, since it is a combination of a convex triangular pyramid and a concave triangular pyramid, it is called It is a two-cone refractive index 4. If it is formed by a convex triangular pyramid and a concave double pyramid, it can illuminate the parallel light to the diamond that opposes the parallel light without waste. The light source that illuminates the refractive surface of the triangular cone is as shown in Fig. 8. Since it is arranged in the 〇3 square ′′, the illuminating surface is irradiated at the angle of the elevation at the elevation angle. Therefore, the refracting surface has no structure other than the incident light source, and is not shielded by the triangular pyramid. Since the mixed color light of three colors is emitted as parallel light in the vertical direction of the reference surface, it can be used for a light source of the three primary color display devices. : In the case where the light incident on the refracting grating is parallel light, it is necessary to arrange a large space of a plurality of parallel light sources on the display y-plane, a needle-forming, and a thin-conical refracting grating. Right on the exit surface side of the light guide plate G forms a convex reflection surface on the bottom surface of the light guide plate 5 kg =: 4, • oblique parallel light incident on the convex reflection surface 5 will be from the side of the guide plate to the bottom surface

^ ^ 匕 凸反射面5,則會反射並擴大光走0S 射到三角錐折射光柵 穴九束照 •並反射,藉由-自雜凸反射面擴大光束 次像素27的:折射光柵折射並擴大成被照射面中的 .射射部的寬度w的樣子於圖10。由沿著凸: 射面的圓周的曲面 街,口耆凸反 率。到被照射面的^ #大成次像素寬w為光束擴大 和,若設次像導光板厚與液晶夹持基板厚的 、的通射部的寬度為w,·沿著導光板凸面傾 201037230 斜部的圓周的 J碑面長度為d,則凸反射面的曲率半徑r以 公式6表示。 • [公式6 ] • r = 2.t.d/(w_d//v-2) 對入射光的底面的斜度“是由段差s與像素寬X以 . 公式7求出。 ^ [公式7 ] 0i =t an-1 (s/x) O 右由3方向將3色的入射光入射到凸反射面,則各自 擴大光束並反射,被照射到三角錐折射光栅的菱形折射 ==射到次像素。因藉由菱形折射面折射並射出於 •=角二故正交於菱形折射面的基準面的對角線的長 折射光栅的上方的次像素寬W同等。因组合菱 -形的次像素形狀,故像素的形狀為6角形。 , 段差為io"m’像素寬為4〇〇//m時,θ 土成 因可平緩成圖5中的1 9. 5。的丨/ n A i . 可炉。蕻由鴒, 1 / 1 3 ’故光源部的薄型化為 〇 了此。藉由4型化使導光板 耔沾厶i J 了利用由凸反射面進 •仃的全反射,故無須鏡面形.。鹿—— 现 顯不母一像音宮35? 4/La 於兩方向的光源的凸反射面 、-6又子向 的構造於圖U。因擴大主I邱^ ^ 匕 convex reflecting surface 5, then reflects and enlarges the light travel 0S to the triangular cone refracting grating. The nine beams are reflected and reflected, and the beam sub-pixel 27 is enlarged by the self-heavy convex reflecting surface: the refractive grating is refracted and enlarged The appearance of the width w of the incident portion in the illuminated surface is shown in FIG. By the curved surface along the convex: the circumference of the surface, the mouth is convex and inverse. The width of the sub-pixel to the illuminated surface is the beam expansion. If the thickness of the light-emitting portion is thicker than that of the liquid crystal-holding substrate, the width of the light-emitting portion is w, and the convex surface of the light guide plate is tilted toward 201037230. The length of the J-surface of the circumference of the portion is d, and the radius of curvature r of the convex reflecting surface is expressed by Formula 6. • [Formula 6] • r = 2.td/(w_d//v-2) The slope of the bottom surface of the incident light “is determined by the step s and the pixel width X. Equation 7. ^ [Formula 7] 0i =t an-1 (s/x) O Right-incident three-color incident light is incident on the convex reflecting surface by the three directions, and each beam is enlarged and reflected, and is irradiated to the diamond-shaped refractive index of the triangular-cone refractive grating == to the sub-pixel The sub-pixel width W above the long-refractive grating orthogonal to the diagonal of the reference plane of the rhombic refractive surface is equalized by the rhombic refractive surface and is emitted by the ?= angle 2. The combined sub-pixel of the rhombic shape The shape is such that the shape of the pixel is hexagonal. When the step is io"m', the pixel width is 4 〇〇//m, and the θ soil can be flattened to 9.5/n A i in Fig. 5. The furnace can be used. 蕻1鸰, 1 / 1 3 'The thinning of the light source unit is the same. The 4th type makes the light guide plate 耔 厶 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 利用 全 全 全 全 全 全 全There is no need for a mirror shape. Deer - It is not like a mother-in-law 35? 4/La The convex reflection surface of the light source in two directions, the structure of the -6 and the sub-direction is shown in Figure U.

• /刀,故Θ i比1. 43。還大而被g ' 要°P 皮顯不。圖12是以兩片導朵柘 .構成,各導光板都以對向於 導先板 成。藉由使別色光透射於凸反 構 反射面間距間的水平面,使3 色以上的混色為可能’圖1 2是 m . 疋顯不藉由錯開配置同一形狀 導光板,混合4色的狀態。π 心狀 从在導光板射出面配設凸折射 201037230 面並恢復成平行光的情形顯示。 圖13是顯示供給3色至液晶顯示裝置的次像素並混色 '的狀態之圖。在圖12與圖13中雖然是使用兩片導光板, •惟若統合該等要素’則如圖14所示能以—片導光板實現3 色條:。由於是-片構成的導光板,&無須像素的對準, •可提高生產性,可減去一半材料費。擴大圖14的主要部分 、 於圖1 5而說明。 入射到Μ 3個次像素構成像素的第—個次像素m的 〇細線的光越過右端的凸反射自5的上端並入射到中央的石 反射面5A。藉由凸反射面全反射,擴大光束並照射到次像 素寬。虛線的光入射到左側的凸反射面並擴大光束入射到 第二個次像素,第3色的光由導光板的下部入射。突出於 導光板的下部的入射部構成垂直於入射光線的面,將突起 .部的後面作成凸反射面5C ’擴大光束並照射到第3個像 素。若形成對稱於5C面的反射面,則4色顯示也可能。 A了使擴大光束的擴散光不入射到構成三角錐的其他 〇 、 冑平行於其他的兩面或成為其他的兩面的陰影而 •不入射。以該條件混色的光根據公式5⑴的司乃耳定律擴 大光束並射出。圖16的光線A平行地行進於構成三角錐的 .其他的兩面的稜並在基準面射出於錯直方向。成為將凸反 .射面中的反射造成的光束擴大光轉換成平行光的凸折射 配設於與三角錐折射光柵之間的兩層構造,惟也能使入射 到二角錐折射光柵的角度一定。為擴散光的放射角越大, '線C D的射出光越由鉛直方向傾斜的射出a。若入 17 201037230 射到構成三角錐的其他的兩面’則如光線E般全反射並射 出到與公式2不同的方向。 圖17、圖18是顯示三角錐折射光栅中的兩面的剖面 之圖。圖17是顯示II由一⑯㈣凸反射面反射並照射到一 列的次像素的列的狀態,也可以如圖18所示由一個圓筒凸 反射面照射到複數個次像素的列。次像素列的數目不限於 整數’若來自下一個凸反射面的光連續的肖,則使用尾數 也可能。#以導光板底面的圓筒凸反射面比像素數少的列• / knife, so Θ i is 1. 43. It is still big and is not seen by g'. Fig. 12 is composed of two conductive sheets, each of which is oriented opposite to the leading sheet. By allowing the color light to be transmitted through the horizontal plane between the pitches of the convex reflective surfaces, it is possible to mix colors of three or more colors. Fig. 12 is m. The state in which four colors are mixed without disposing the same shape of the light guide plate. π heart shape is displayed from the case where the surface of the light guide plate is provided with a convex refraction 201037230 and restored to parallel light. Fig. 13 is a view showing a state in which three colors are supplied to the sub-pixels of the liquid crystal display device and the color mixture is mixed. In Fig. 12 and Fig. 13, although two light guide plates are used, if only these elements are integrated, a three-color strip can be realized by a sheet light guide as shown in Fig. 14. Since it is a light guide plate composed of a sheet, & does not require pixel alignment, • can improve productivity, and can reduce the material cost by half. The main part of Fig. 14 is enlarged and explained in Fig. 15. The light incident on the thin line of the first sub-pixel m of the sub-pixels of the three sub-pixels is reflected from the upper end of the convex portion of the fifth end and incident on the central stone reflecting surface 5A. The total reflection of the convex reflecting surface enlarges the light beam and illuminates the sub-pixel width. The dotted light is incident on the convex reflecting surface on the left side and the enlarged light beam is incident on the second sub-pixel, and the light of the third color is incident on the lower portion of the light guiding plate. The incident portion protruding from the lower portion of the light guide plate constitutes a surface perpendicular to the incident light, and the rear surface of the projection portion is formed as a convex reflection surface 5C' to expand the light beam and to illuminate the third pixel. If a reflecting surface symmetrical to the 5C plane is formed, a 4-color display is also possible. A. The diffused light of the enlarged beam is not incident on the other 〇 and 胄 which form the triangular pyramid, and is parallel to the other two faces or the shadows of the other two faces. The light mixed under this condition expands the beam according to the Sner's law of Equation 5(1) and emits it. The ray A of Fig. 16 travels in parallel to the other ribs constituting the triangular pyramid and is incident on the reference plane in the wrong direction. It is a two-layer structure in which a convex refraction of a beam-expanded light caused by reflection in a convex surface is converted into parallel light and a triangular-concave-refracting grating, but also an angle of incidence to the dichroic refractive grating is constant. . The larger the radiation angle of the diffused light is, the more the emitted light of the line C D is emitted obliquely from the vertical direction. If 17 201037230 is incident on the other two sides constituting the triangular pyramid, it is totally reflected as the light E and is emitted in a direction different from the formula 2. 17 and 18 are views showing a cross section of both faces in a triangular pyramidal refractive grating. Fig. 17 is a view showing a state in which II is reflected by a 16 (four) convex reflecting surface and irradiated to a column of sub-pixels of one column, and as shown in Fig. 18, a cylindrical convex reflecting surface is irradiated to a column of a plurality of sub-pixels. The number of sub-pixel columns is not limited to the integer '. If the light from the next convex reflecting surface is continuous, it is also possible to use the mantissa. #The column with a convex convex surface on the bottom surface of the light guide plate is smaller than the number of pixels

數構成,由一個圓筒凸反射面照射到複數個次像素的列, 則凸反射面的尺寸比照射到一列的次像素的列時大可削 減圓筒凸反射面的列數’故幸月3方向的凸反射面的成型變 的容易。 _ 因隨著增加分配於複數個次像素列的數目,如圖16 •的光線B、C、D般傾斜,故為了使射出方向成鉛直方向需 根據公式5(1 )補正射出面的斜度,或者抑制在不入射到接 鄰的其他顏色的次像素的放射角。圖16的光線B、c、D 〇被谷部遮蔽並在頂部附近產生死角部分並減少光量 (quantity of light)’抑制在不產生亮度不均(brightness unevenness)的影響的放射角較佳。減少導光板厚的情形也 . 如光線B、C、D般傾斜,故一樣。 纟於圖17、圖18僅顯示兩方向成分,故以俯視圖顯 示3方向成分為圖19。說明藉由朝導光板底面的3方向的 凸反射面將來自3方向的平行光全反射於三角錐折射光柵 方向的機制(mechanism)。圖19的B-B,中的剖面是配設 201037230 於圖17、圖18的底面之朝兩方向的三角柱狀 延伸於® 19的橫方向之以3们組構成的線是 .向於導光板側面的上邊與下邊的兩邊而配設的 •面接觸頂稜形成三角柱狀。將為了使照射於圖 的平行光B反射於菱形的折射光柵方向的圓筒 ,列於導光板的底面,使照射於圖的右上方向的 •射於菱形的㈣光柵方向㈣筒凸反射面接觸 藉由接觸該頂稜的圓筒凸反射面反射照射於圖 〇的平行光B與照射於圖的右上方向的平行光c 角錐折射光柵,且入射到次像素B、c。 藉由菱形的折射光柵將來自朝左方向的平 的光轉換方向成鉛直方向並照射到排列於上下 •素A。 • 將反射來自在圖19中配設於右邊的光源a 個凸反射面配設於位於兩個三角柱狀凸反射 部。因來自配設於圖1 9的上邊與下邊的光源 〇入射到位於三角柱狀凸反射面的陰影的谷部 5A ’故僅將光源A的光照射到次像素A。 顯示沿著該谷部的剖面A-A’於圖20。藉1 ' 反射面5A擴大光束並反射的光僅入射到三角 . 射面15A並入射到次像素27A。顯示於凸反射 凸反射面5C不是存在於同一個剖面上,而是有 直方向,透視顯示。來自配設於圖19的上邊輿 B、C的光藉由凸反射面5C與更存在於其背面 凸反射面。 使平行於對 圓筒凸反射 的右下方向 凸反射面排 平行光C反 並形成稜, 的右下方向 並入射到三 行光光源 A 方向的次像 的光的複數 面之間的谷 s、c的光不 的凸反射面 台圖20的& 錐光柵的折 每5A之上的 在於紙面垂 下邊的光源 側的凸反射 19 201037230 面5B擴大光束並反射,各自入射到三角錐光栅的折射面 15C與15B並入射到次像素27C與27B。因凸反射面5B、 折射面15B、次像素27B位於背面側,故未圖示,朝3方 向的凸反射面的導光板底面將來自3方向的平行光全反射 於三角錐折射光栅方向。 ' 形成凸反射面A成圓筒的情形,因若來自右邊的光反 •射’則三角柱狀凸反射面的上部成為死角不被照明,故也 在凸反射面A的長軸方向形成曲面,控制長軸方向的放射 〇角ε並照射到三角柱狀凸反射面的上部的像素。凸反射面 的長轴方向的曲率半徑R是設凸反射面的長軸方向的長度 為L,以公式8表示。 [公式8 ] . 尺-L// ( 2 . s i η (ε /2)} 因照射比正交於三角柱狀凸反射面的方向的凸反射面 的長轴方向長度長的範圍,故可照射到前述三角柱狀凸反 射面的上部的像素。 〇 藉由圖19的底面的凸反射面反射的3方向的光入射到 .配設於導光板的上側面的三角錐折射光柵的a、B、c面 因三角錐折射光柵為組合3個菱形面的構造,故在導光板 -的上方配置具有菱形的次像素的液晶面板。圖21是以菱, 形成3色的次像素並三角排列’自6角 形 a ^ l稠1成的液 曰日‘,,、’、裂置之俯視圖。在圖2 1中為了說明的方便起 當大地擴大次像素的尺寸而顯示。 相 將3色的光源A、B、C配置於周邊部並由1 9n。 屯1 zu 不同 20 201037230 的方向照射。雖缺、Γ η ^ …、 、Β的排列為任意,但因配置於右 邊的光源Α的數目最少, _ > 故配置向焭度的元件為上策。在 右邊排列照射於朝左方向 十灯九先源A’在圖21的上邊 與左邊上㈣列照射於圖的右下方向的平行光光源B,在 下邊與左:下側排列照射於圖的右上方向的平行光光源 、,㈣素將3方向的光混色並進行彩色顯示。 因通過二角錐折射光栅照射3色光到次像素,故不使 用彩色濾光片可進行液晶顯示裝置的彩色顯示,由於凸反 Ο 射面與三角錐折射光柵是由同—構件構成的導光板,故可 與液晶面板的像素對進卄;佳#必A _ 對羊並進盯彩色顯不。由於是將菱形次 像素排列成點對㈣6㈣像素,故併設加法混色佳,比 由條紋構成的正方形像素平滑。 ’ 目彩色濾、光片吸收該色以外,故透射率(transraission ' faCt〇r)為33%以下,若包含偏光板的吸收等,則液晶顯示 裝置全體的效率為8%以下,惟因本案發明不使用彩色遽光 片,故效率變成3倍,與白色發光二極體比較為約1/3的 〇 RGB發光二極體數。因此,不僅削減彩色濾光片的製造程 •序,也能削減發光二極體與電源部的成本。 在顯示裝置中能以3原色的混色再現,惟在照明装 -置、攝影裝置等中若缺乏光源的波長特性,則無法進行正 確的色彩再現。利用將藍色發光二極體的藍色光照射到黃 色螢光體的補色的白色發光二極體具有尖銳的藍光光譜與 平緩的黃光光5普,在青綠色域具有大的谷值。混合複數個 螢光體並使螢光白色發光二極體寬頻化時,藉由多量地混 21 201037230 合螢光體’使螢光藉由其他的替来賴明此 j赏尤體吸收’效率更降低。 因此’不是混合螢光體,而是芸鏟士 __ 疋右藉由二角錐折射光柵或三The number structure is such that a cylindrical convex reflecting surface is irradiated to a plurality of sub-pixel columns, and the size of the convex reflecting surface is larger than the number of columns of the cylindrical convex reflecting surface when irradiated to the columns of the sub-pixels of one column. The formation of the convex reflecting surface in the three directions becomes easy. _ Since the number of sub-pixel columns allocated is increased, as shown by the light rays B, C, and D in Fig. 16, the slope of the exit surface is corrected according to the formula 5(1) in order to make the emission direction vertical. Or suppressing the radiation angle of sub-pixels that are not incident on other colors adjacent to each other. The ray B, c, D 图 of Fig. 16 is shielded by the valley portion and produces a dead angle portion near the top portion and reduces the amount of light. The radiation angle which suppresses the influence of the brightness unevenness is preferable. The case of reducing the thickness of the light guide plate is also the same as the light B, C, and D. In Fig. 17 and Fig. 18, only the two-direction components are shown. Therefore, the three-direction component is shown in Fig. 19 in a plan view. A mechanism in which the parallel light from the three directions is totally reflected in the direction of the triangular pyramidal refractive grating by the convex reflecting surface in the three directions of the bottom surface of the light guide plate will be described. In the BB of Fig. 19, the cross section of the lining of the bottom surface of the lining of the lining of the lining of the lining of the lining of the lining of the lining of the lining of the lining of the lining of The top surface of the upper and lower sides is connected to the top edge to form a triangular column shape. A cylinder for reflecting the parallel light B irradiated in the figure in the direction of the rhombic refractive grating is arranged on the bottom surface of the light guide plate so as to be in contact with the diamond in the upper right direction of the figure (the fourth) of the grating direction The parallel light B irradiated to the figure and the parallel light c which is irradiated in the upper right direction of the figure are reflected by the cylindrical convex reflecting surface contacting the top edge, and are incident on the sub-pixels B and c. The flat light from the leftward direction is converted into a vertical direction by a diamond-shaped refractive grating and irradiated to the upper and lower sides. • The reflection from the light source a convex reflecting surface disposed on the right side in Fig. 19 is disposed in the two triangular columnar convex reflecting portions. Since the light source 配 disposed on the upper side and the lower side of Fig. 19 is incident on the valley portion 5A' of the shadow located on the triangular columnar convex reflecting surface, only the light of the light source A is irradiated to the sub-pixel A. A section A-A' along the valley portion is shown in Fig. 20. The light beam is enlarged by the 1' reflecting surface 5A and reflected light is incident only on the triangle. The emitting surface 15A is incident on the sub-pixel 27A. Displayed on the convex reflection convex reflection surface 5C does not exist on the same cross section, but has a straight direction and a perspective display. The light from the upper side B, C disposed in Fig. 19 is further present on the back surface of the convex reflecting surface by the convex reflecting surface 5C. Aligning the parallel light C parallel to the convex reflection surface in the lower right direction of the convex reflection of the cylindrical convex portion, and forming a valley in the lower right direction and incident on the complex surface of the light of the secondary image in the direction of the three rows of light sources A The convex reflection surface of the light of c is smaller than the convex reflection of the light source side on the lower side of the paper surface on the lower side of the 5A of the cone grating 19 201037230. The surface 5B enlarges the light beam and reflects it, and each of them is incident on the triangular pyramid grating. The refractive surfaces 15C and 15B are incident on the sub-pixels 27C and 27B. Since the convex reflecting surface 5B, the refracting surface 15B, and the sub-pixel 27B are located on the back side, the bottom surface of the light guide plate of the convex reflecting surface in the three directions totally reflects the parallel light from the three directions in the direction of the triangular pyramidal refractive grating. When the convex reflection surface A is formed into a cylinder, if the light from the right side is reversed, the upper portion of the triangular prism-shaped convex reflection surface is not illuminated, so that a curved surface is formed in the longitudinal direction of the convex reflection surface A. The radiation pupil angle ε in the long axis direction is controlled and irradiated to the pixels above the triangular columnar convex reflecting surface. The radius of curvature R of the convex reflecting surface in the long-axis direction is such that the length of the convex reflecting surface in the long-axis direction is L, which is expressed by Formula 8. [Formula 8]. Ruler-L// (2. si η (ε /2)} The irradiation length is longer than the length of the convex reflection surface of the convex reflection surface orthogonal to the direction of the triangular columnar convex reflection surface, so that it can be irradiated The pixel in the upper portion of the triangular columnar convex reflecting surface. The light in the three directions reflected by the convex reflecting surface of the bottom surface of FIG. 19 is incident on the a and B of the triangular pyramidal refractive grating disposed on the upper side surface of the light guide plate. Since the c-plane triangular pyramidal refractive grating has a structure in which three diamond-shaped surfaces are combined, a liquid crystal panel having a diamond-shaped sub-pixel is disposed above the light guide plate. FIG. 21 is a sub-pixel of three colors and is triangularly arranged. 6-shaped a ^ l thick 1% of the liquid 曰 ',,, ', and the top view of the rupture. In Figure 21 for the convenience of explanation, when the size of the sub-pixel is enlarged greatly, the three-color source A , B, C are arranged in the peripheral part and are illuminated by 1 9n. 屯1 zu is different from 20 201037230. Although the arrangement of the missing, Γ η ^ ..., Β is arbitrary, the number of light sources 配置 disposed on the right side is the least. _ > Therefore, it is best to configure the components to the width. Arrange the light on the right to the left. The ten-light source A' is a parallel light source B that is irradiated in the lower right direction of the figure on the upper side and the upper (four) column on the upper side of FIG. 21, and the parallel light source that is irradiated in the upper-right direction of the figure on the lower side and the lower side: (4) The color in the three directions is mixed and displayed in color. Since the dichroic refractive grating is used to illuminate the three colors of light to the sub-pixels, the color display of the liquid crystal display device can be performed without using the color filter, due to the convex anti-reflection surface and the triangle The cone-refracting grating is a light-guiding plate composed of the same member, so that it can be aligned with the pixel of the liquid crystal panel; the good #必A _ is to be displayed in the color of the sheep. Since the diamond-shaped sub-pixels are arranged in a point pair (four) 6 (four) pixels, Therefore, it is preferable that the additive color mixture is better than the square pixels formed by the stripes. The transmission of the transurassion faCt〇r is 33% or less, and the absorption of the polarizing plate is included. The efficiency of the entire liquid crystal display device is 8% or less. However, since the color light-receiving sheet is not used in the present invention, the efficiency is three times, and the number of 〇RGB light-emitting diodes is about 1/3 as compared with the white light-emitting diode. because In addition, it is possible to reduce the cost of the light-emitting diode and the power supply unit by reducing the manufacturing process of the color filter. The display device can be reproduced in a mixed color of three primary colors, but in a lighting device, a photographing device, or the like. The lack of the wavelength characteristics of the light source makes it impossible to perform correct color reproduction. The white light-emitting diode that uses the blue light of the blue light-emitting diode to illuminate the complementary color of the yellow phosphor has a sharp blue spectrum and a gentle yellow light. It has a large valley value in the cyan field. When a plurality of phosphors are mixed and the fluorescent white light-emitting diode is wide-banded, the amount of fluorescence is reduced by a large amount of 21 201037230. Come to Lai Ming this j-reward to absorb the 'efficiency is even lower. So 'not a hybrid phosphor, but a shovel __ 疋 right by a two-cone refractive grating or three

• 角錐反射光桃混色’則不伴隨效查胳·姑站、± E 吸欵羊降低使波長特性寬頻化。 令第一發光元件為青紫色發妙 • 巴赞九一極體,若以由黃色螢 光體產生的波高值為青紫色光油古柏认奶 丄 ^ %及回值的約一半的雙峰特性 • (dual-peak charac ter i s t i c<^ 八私 n 舰 1 csv刀散螢光體,則為在藍色〜 綠色具有谷值’紅色域降低的特性。 令以第一發光元件的谷庙油且政 履波長發先的青綠色發光二極 Λ體為第二發光元件,若以由糌6技丨L €) 田燈色螢光體產生的波高值為青 綠色光波高值的約一半的雙峰牲地 叉▼特性分散螢光體,則為在綠 色〜黃色具有谷值的特性。 令以第一發光元件的谷麻、士 Ε於 底波長發光的綠色發光二極體 ' 為第三發光元件’若以由撥甶技Α 田後色螢光體產生的波高值為綠色 光波高值的約一半的雙峰Μ ,14八 文辛特性分散螢光體,則為在黃色~ 橙色具有谷值的特性。 若使用三角錐折射糸; 耵九柵加法混色第一〜第三發光二極 Ο體光,則第一發光二極體的公念r , … 姐的合底區域藉由第二、第三發光 二極體的激發光補足。第一〜笛一& 弟二發光二極體的螢光光譜藉 由加法混色遍及黃色〜紅色域, ^ ’皮兩值大致與激發光相等, . 可得到平缓的連續光譜的蒂# 曰Θ愛7b。以螢光體得到寬頻特性的 方法其效率降低,惟可藉由左 • 稽田在谷底區域設有別的激發波長 並進行利用三角錐折射光输准〜 一 元樹進仃的混色,高效率地實現連 續波長。顯示由拋物面鐘禮土、从 兄構成的剖面圖於圖22,顯示將折 射光柵的斜度面作成凹面,ώ 由導光板構成的剖面圖於圖 22 201037230 23。顯示以三角錐混色裝置將不同的激發波長的 發光二極體混色之合成前與合成後的波長特性於 ' 因在照明裝置中往往比平行光還擴大放射 用,故可藉由負焦距光學系統將被混色的平行光 還擴大放射角。由於若放射方向不同,則成為僅 •分,故藉由使各光源光其放射角與方向都一致, -勻的混色光。圖24是在折射光柵的射出部配設凹 (concave lens array)之圖 〇 0 可藉由將折射光柵的斜度面作成凹面擴大放 其顯示於圖25。可藉由使對向的折射光柵斜度面 射出光的放射角一致,照射均勻的混色光。為了 對向的折射光柵斜度面’需以折射光栅谷部中的 .度入射。因此,因不入射到折射光栅的頂部,故 作成尖銳,也可使其平坦而容易成型。 也可將折射光柵的斜度面作成凸面,在通過 大放射角。即使折射光柵的斜度面為平面,入射 ◎是平行光,而是於擴散光時,在射出折射光柵後肩 •不將折射光柵的基準面作成平面而是作成凹面, 光入射到折射光栅,射出擴散光。 • 若令光源部為來自一點的擴散光,則入射到 -的基準面的角度因位置而不同,惟若令成來自複 擴散光’則可使入射到基準面的角度一致。 因在聚光燈(spot light )、號誌燈(traffic 中照射範圍或觀察可能範圍的放射角θ比公式6 螢光轉換 圖30。 角而被使 比平行光 一方的成 可照射均 透鏡陣列 射角,將 的凹面的 不入射到 切線的斜 頂部無需 焦點後擴 光也不會 f擴散光。 可使擴散 折射光柵 數個點的 light)等 、圖1 0的 201037230 顯不面中的寬度w還容易利用,故若以凸反射面的曲率半 、Γ /〇者圓周的曲面長度d、放射角0表示的話,則能以 a式9表示也能以公式1〇近似。其中放射角如圖11所 .示為對中心線對稱的角度。 [公式9 ] θ = ά - 36〇° / (2πΓ) [公式1 0 ] 0 = s i n_1 (d/r)• The pyramidal reflection of the peach-paste color is not accompanied by the effect of the skeletal and ± E sucking sheep to reduce the wavelength characteristics. Let the first illuminating element be blue-purple. • Bazin's nine-pole, if the wave height produced by the yellow phosphor is blue-purple varnish, the cypress recognizes the milk 丄 ^ % and about half of the double value of the return value. Features • (dual-peak charac ter isti c<^ eight private n ship 1 csv knife scattered fluorescent body, then in the blue ~ green with a valley 'red field' reduced characteristics. Let the first light-emitting element of the valley temple The cyan-green light-emitting diode of the oil and the political wavelength is the second light-emitting element. If the wave height of the field-light phosphor is 约6, the wave height is about half of the value of the blue-green light wave. The characteristics of the bimodal Boundary fork ▼ characteristic dispersion of the phosphor are in the shade of green to yellow. The green light-emitting diode 'which is the third light-emitting element' that emits light at the bottom wavelength of the first light-emitting element is used as the third light-emitting element. Approximately half of the value of the double-peak Μ, 14 octa- octane characteristic dispersion of the phosphor, is a characteristic of the valley in yellow to orange. If a triangular cone refraction 使用 is used; the 耵九 grid addition color mixing the first to third illuminating dipole Ο body light, then the first illuminating diode of the first illuminating dipole, ... the sister's bottom area by the second and third illuminating The excitation light of the diode complements the light. The fluorescence spectrum of the first ~ flute one & two light-emitting diodes is added by the additive color throughout the yellow ~ red domain, ^ 'the two values of the skin are roughly equal to the excitation light, and a flat continuous spectrum can be obtained. Love 7b. The method of obtaining broad-band characteristics of the phosphor is reduced in efficiency, but it is possible to provide a different excitation wavelength in the valley region by left-handed field and perform color mixing using the triangular cone refracting light to the mono-tree tree, and efficiently Achieve continuous wavelengths. A cross-sectional view showing the parabolic clock and the brother is shown in Fig. 22, showing that the slope of the refractive grating is concave, and the cross-sectional view of the light guide is shown in Fig. 22 201037230. It is shown that the pre-synthesis and post-synthesis wavelength characteristics of the dither mixing of different excitation wavelengths by the triangular cone color mixing device are used for the purpose of expanding the radiation by the parallel light, so the negative focal length optical system can be used. The parallel light to be mixed is also enlarged to the radiation angle. If the radiation direction is different, it is only a minute, so that the light source angle and the direction of the respective light sources are uniform, and the mixed color light is uniform. Fig. 24 is a diagram in which a concave lens array is disposed in an emitting portion of a refractive grating. 〇 0 can be enlarged by a concave surface of a refractive grating, and is shown in Fig. 25. The uniform mixed color light can be irradiated by making the radiation angles of the light emitted from the oblique surface of the opposing refractive grating uniform. In order to oppose the refractive grating slope plane, it is required to be incident at a degree in the valley of the refractive grating. Therefore, since it is not incident on the top of the refractive grating, it can be made sharp, and it can be made flat and easily molded. It is also possible to make the slope of the refractive grating convex, and to pass through a large radiation angle. Even if the slope of the refractive grating is a plane, the incident ◎ is parallel light, but when the light is diffused, after the refractive grating is emitted, the shoulder is not formed into a plane but a concave surface, and the light is incident on the refractive grating. The diffused light is emitted. • When the light source unit is diffused from a point, the angle of the reference plane incident on - differs depending on the position, but if it is from the complex diffused light, the angle of incidence on the reference plane can be made uniform. Because of the spot light, the illumination range (the illumination range of the illumination range or the observed range of the radiation angle θ is greater than the angle of the fluorescence conversion diagram of Equation 6), the angle of the parallel lens is illuminable to the uniform lens array angle. The concave top of the concave surface is not incident on the oblique top of the tangential line, and the light is diffused without the focus, and the light is not diffused. The light of the diffusion refraction grating can be several points, and the width w of the 201037230 of FIG. Since it is easy to use, if it is represented by the curvature half of the convex reflection surface, the curved surface length d of the Γ / 〇 circumference, and the radiation angle 0, it can be approximated by Formula 1 表示. The radiation angle is shown in Fig. 11 and is shown as an angle symmetrical to the center line. [Formula 9] θ = ά - 36〇° / (2πΓ) [Formula 1 0 ] 0 = s i n_1 (d/r)

、圖11疋顯示以放射角0將來自兩方向的平行光混色 並射出於同一方向的狀態。若為放射角相等且方向一致無 法辨識光柵的尺寸,則均勾地進行加法混色。 為了以個別發光元件得到連續光譜,發光二極體的發 光強度成為尖峰的約半值的波長寬為2〇 nm~6〇nm,故若以 各色的半值波長連接並使用6色~9色,則可涵蓋可見光域 並實現連續光譜的白色光。更由於入射到三角錐折射光柵 的3個光源使用由折射光柵或反射光柵產生的混色光,可 〇在合6色或9色。因不是由散射產生的混色’故可照射放 •射角窄的白色光。若混合6色,則如圖31所示可合成連續 光謂·的白色光’顯示其構造的主要部分透視圖的例子於圖 • 26’顯示剖面圖的例子於圖27〜圖29。 因射出面的折射光栅可將複數條光入射到一個光柵斜 度面’故圖28與圖27比較變成一半的折射光栅數。圖29 疋利用導光板底面的凸反射光栅的光束擴大功能’刪除圖 27的導光板射出面的凹折射面之圖。 24 201037230 【發明的功效】 • 為了解決產生因複數個發光元件與反射鏡的距離 度的非對稱性造成的色斑,藉由使用防止別的光源光 的反射光柵或折射光柵並混合,以同一放射角射出, * 止色斑。 藉由將反射光柵作成凸反射面,可減小入射光 度’使光源部薄型化。 ^ 因可藉由使凸反射面光栅朝3方向的構造或使三 折射光栅與凸反射面光柵朝3方向的構造,以一片導 實現3色條紋,故無須對準,生產性提高,可削減彩 光片製程與發光二極體等的材料費。 - 為了解決螢光白色發光二極體的光譜是由尖銳的 與平緩的黃色域的兩個尖峰構成,可藉由使用混色裝 用複數個激發光,高效率地實現連續光譜。 可比以多成分系混合螢光體並使光譜寬頻化的方 0高效率地得到連續光譜的白色光。 【實施方式】 [實施例1 ] 針對藉由使用三角錐折射光栅,由菱形次像素構 液晶顯示裝置說明。顯示在液晶顯示裝置的導光板的 配置3種類的凸反射光柵,在導光板侧面配置3種類 源之俯視圖於圖1 9,顯示由菱形次像素構成的液晶顯 與角 混入 可防 的斜 角錐 光板 色濾 藍色 置利 法還 成的 底面 的光 示裝 25 201037230 置的俯視圖於圖21。對角1117m(46型)、Fig. 11A shows a state in which parallel light from both directions is mixed at a radiation angle of 0 and is emitted in the same direction. If the radiation angles are equal and the directions are the same and the size of the grating cannot be recognized, the additive color mixing is performed. In order to obtain a continuous spectrum of individual light-emitting elements, the light-emitting intensity of the light-emitting diode has a wavelength of about half a value of a peak of 2 〇 nm to 6 〇 nm, so that the color is connected at a half-value wavelength of each color and 6 to 9 colors are used. , can cover the visible light region and achieve a continuous spectrum of white light. Furthermore, since the three light sources incident on the triangular pyramidal refractive grating use the mixed color light generated by the refractive grating or the reflective grating, they can be combined in 6 colors or 9 colors. Since it is not a color mixture caused by scattering, white light having a narrow emission angle can be irradiated. If six colors are mixed, white light of continuous light can be synthesized as shown in Fig. 31. An example of a principal part perspective view showing the structure is shown in Fig. 26 to Fig. 29 for an example of a sectional view. The refractive grating of the exit surface can inject a plurality of lights onto a grating slope surface, so that FIG. 28 is compared with FIG. 27 to become a half of the number of refractive gratings. Fig. 29 is a view showing the concave-convex surface of the light-emitting plate exit surface of Fig. 27 by the beam expanding function of the convex reflection grating on the bottom surface of the light guide plate. 24 201037230 [Effects of the Invention] • In order to solve the problem of unevenness caused by the asymmetry of the distance between the plurality of light-emitting elements and the mirror, by using a reflection grating or a refractive grating that prevents light of other light sources and mixing, the same The radiation angle is emitted, * stop the stain. By making the reflection grating a convex reflection surface, the incident illuminance can be made small, and the light source portion can be made thinner. ^ By making the convex reflection grating in the three-direction structure or the three-refracting grating and the convex reflection grating in the three-direction structure, the three-color stripe is realized by one guide, so that alignment is not required, productivity is improved, and reduction can be achieved. Material costs for color film processing and light-emitting diodes. - In order to solve the problem that the spectrum of the fluorescent white light-emitting diode is composed of two sharp peaks of a sharp and gentle yellow domain, a continuous spectrum can be efficiently realized by using a plurality of excitation lights using a color mixture. It is possible to obtain a continuous spectrum of white light with high efficiency by mixing the phosphors in a multi-component manner and widening the spectrum. [Embodiment] [Embodiment 1] A description will be given of a liquid crystal display device using a diamond-shaped sub-pixel structure by using a triangular pyramidal refractive grating. Three types of convex reflection gratings are arranged on the light guide plate of the liquid crystal display device, and three types of sources are arranged on the side surface of the light guide plate. Fig. 1 is a view showing the liquid crystal display and the corner mixed with the rhombic sub-pixels. The optical display of the bottom surface of the blue filter is also shown in Fig. 21. Diagonal 1117m (type 46),

High Definiti〇n:Full HD)(1920xl080)時,| .1〇18龍、縱573mm、像素間距53〇"m、次像章 306 " m。 導光板的底面是配置朝3方向的3種類的 .以圓筒凸反射面B將照射到圖的右下方向的平 .到斜上方,並以入射角α入射到菱形的折射光 前述圓筒凸反射面Β接觸並形成稜的圓筒凸反 〇射到圖的右上方向的平行光C反射到斜上方, α入射到菱形的折射光柵β。以圓筒凸反射面 左方向的平行光光源Α的光反射到斜上方’並 入射到菱形的折射光柵。 - 以三角錐折射光栅的折射面A、B、C轉換 方向並照射到次像素A、B、C。因導光板的凸 比像素尺寸小,故擴大成像素尺寸,惟因導光 故凸反射面的曲率半徑為一定。若設導光板厚 〇凸反射面的段差s為l〇"m,則曲率半徑!>為 位於略鉛直方向的液晶的次像素反射來自光 線,無須藉由傾斜成全反射臨界角以上而形成 .削減製造費用。 將發光二極體偏移(offset)配置於在光源 鏡的焦點不遮蔽拋物面鏡的反射光的位置。藉 配置540個發光強度240mcd的發光二極體,在 配置540個發光強度I40mcd的發光二極體 高畫質(Full ^面尺寸為橫 ^的菱形邊長 丨凸反射面。 行光B反射 >柵B。以與 射面C將照 並以入射角 A將來自朝 以入射角α 方向成鉛直 反射面段差 板厚一定, t 為 1Omm , 1 5 9 // m。朝 源的平行光 反射層,可 部的拋物面 由在光源 A .光源B與g ,在透光率 26 201037230 (light transmittance)40%時得到亮度 263cd/m2。此時的 功率消耗(power consumption)約130W,為白色發光二極 體與彩色濾光片的情形的約1 / 3的功率消耗。 透明材料可為聚甲基丙烯酸甲酯、脂環族丙烯酸樹脂 (all cyclic acrylic resin)、環烯烴樹脂(CyCi〇〇iefin * resin)、聚碳酸酯、光硬化丙烯酸樹脂(photocurable .acrylic res in)等,可藉由射出壓縮成型等成型。因光硬 化丙烯酸樹脂為低黏度的單體(m〇n〇mer),將低聚物 〇 (oligomer)聚合成起始材料(startingmateriai),故精密 的成型為可能。 [實施例二] 顯示混合成配置反射面成格子狀的3色條紋的液晶顯 -示裝置的照明裝置於圖14’顯示主要部分於圖15。對角 .510·(20.1 型)、XGA( 1 024x768 )時晝面尺寸為橫 4〇8_、 縱306龍、像素間距399 /ira、次像素間距^3"^。 朝3方向的3種類的凸反射面為以像素間距均等地配 〇置1 024段的構造。因導光板的凸反射面段差比像素尺寸 •小,故擴大成像素尺寸,惟因導光板厚一$,故凸反射面 的曲率半徑為一定。若設導光板 ^ 极序t為10mm,凸反射面的 - 段差s為ΙΟμπι,則曲率半徑上 位r為159“ m。朝位於略鉛直 方向的液晶的次像素反射來自光源的 τ〜十仃尤線,無領Μ由 傾斜成全反射臨界角以上而形成反射 乂夂射層,可削減製造費用。 將發光二極體偏移配置於在光泝 兀*碌0卩的拋物面鏡的焦點 不遮蔽拋物面鏡的反射光的位置。藉 ‘…, 稭由配置128個各色的 27 201037230 發光強度250mcd的發光二極體,在透光率4〇%時得到亮度 307cd/m2 。 -[實施例三] 將兩色的平行光入射到在雙方向具有凸反射面的光柵 的導光板並混色的實施例是針對使用紅色發光二極體與綠 •色發光一極體合成黃色的號諸燈說明。以實施例四說明依 •照折射光柵的例子’以實施例五說明依照反射光柵的例 子。雖然被稱為藍信號,但正確為綠色。色盲對策是以帶 〇藍色的綠色顯示。黃色jg號是以帶橙色的橙黃色顯示。圖 32為將綠色與紅色的平行光入射到在雙方向具有凸反射 面的光栅’在黃色信號時將綠色與紅色混色並以黃橙色顯 示的號誌燈之剖面圖。顯示俯視圖於圖3 2。 導光板的底面為朝以圖11顯示的雙方向的凸反射面 -形成三角柱。因到號諸燈顯示面的距離為約5m以上,故在 凸反射面的寬度為5mm以下無法辨識光栅,在紅色光與綠 色光由凸反射光栅於同一方向以同一放射角射出時,被加 ◎法混色不產生色斑。 顯示面周圍的兩個光源部是由配設於各9 6個的橢圓 鏡的焦點後’以拋物面鏡形成平行光並入射到一方的凸反 射面的構造構成,在一方的光源部配設綠色發光二極體, 在他方的光源部配設紅色發光二極體。以成對的凸反射面 於同一方向以同一放射角反射,以導光板表面的凹折射面 擴大光束成必要的放射角。習知的照射到上空或交叉的道 路的指向性其消耗電流變成浪費’惟若令上下方向的放射 28 201037230 範圍為水平面以下’令左右方向的放射角為土45。的範圍, 則可削減消耗電流成約1/4。因此,即使在一個顯示面一 • 半一半配設紅與綠的元件也能得到必要的光量。 - 若使用5〇〇nm以下的青綠色發光二極體並與紅色發光 一極體混色,則色度座標上的直線接近白色域並成為淡黃 •色,故若使用5〇〇ηπι以上的綠色發光二極體與610nm以上 .的紅色發光二極體,則混色直線沿著成馬蹄形的色度座標 的右側緣面,故可將濃的黃色混色。 在習知的3燈 變亮,亮度差降低 的混色中因顯示面 減黃色的發光元件 • 數的降低削減號誌 故不僅可看到交又 雖然消耗電流變多 低消耗電流,可藉 〇發光效率的提高顯 . 著’若削減元件數 減困難。但是,因 •全體被均勻地顯示 率削減發光元件數 [實施例四] 〇 的疑似點 為1燈, ,可更藉 燈的成本 的道路側 ’但若令 由元件數 著,惟習 ,則更成 以無法辨 。因此, 亮現象, 故不發生 由由指向 。習知的 的信號, 成必要的 的降低削 知的顯示 為粗輪的 識凸反射 可依照指 在利用折 疑似點亮 性的控制 號誌燈因 也能放射 指向性範 減製造成 面因發光 顯示,故 光柵的寬 向性的控 免的兩燈也 射光栅進行 現象,可削 造成的元件 指向性寬, 到上空,故 圍,則可降 本。近年來 元件的點顯 元件數的削 度顯示,故 制與發光效 ’十對與實施例三的不同點,却hb姑山> 益土 ” 說月藉由折射光柵將紅色 發光二極體與青綠色發光二 ®骽合成黃色的號誌燈。若作 29 201037230 成圖34所示的單元(unit)的直徑25mm,則可在圖35所示 的直徑30〇mm的顯示面排列約12〇單元。若配設8對折射 '光柵’則成為在單侧面1. 5mm寬的梳子形,在紅或綠顯示 •時由光柵的單侧面射出成梳子形。在紅色光與綠色光由寬 1. 5mm的折射光栅射出時’無法藉由到號誌燈顯示面的距 .離辨識光柵’也藉由放射方向的一致不產生色斑。在必要 .的^日向性範圍射出擴散光的手段(means)為圖34所示的凹 透鏡陣列。凹透鏡陣列具有兼具防塵、防水的防護罩(h〇〇d) ^的功能。 [實施例五] 針對與實施例三的不同點’說明藉由反射光栅將紅色 發光二極體與青綠色發光二極體合成黃色的號誌燈。若將 • 圖2所示的單元的反射光栅面作成19mm四角形,則可在圖 36所示的直徑300mm的顯示面排列約120單元。若配設8 對反射光柵,則成為在單側面1. 5mm寬的凸反射面,在紅 或綠顯示時由光栅的單側面射出成梳子形。在紅色光與綠 ❹色光由寬1. 5 mm的反射光柵射出時’無法藉由到號誌燈顯 示面的距離辨識光栅’也藉由放射方向的一致不產生色斑。 反射光柵藉由彎曲反射面擴大指向性’具有發光元件 尺寸加原來的放射角的指向性’可彎曲反射光柵的設置面 並可設定指向性。因此’可藉由反射光栅的彎曲設置面設 定成依照道路狀況的指向性。指向性的控制具有自由度比 導光板的凸反射面及/或導光板的折射面寬的特徵。因反射 光栅形為光源部排列的構造,故反射面的佔積率(sPace 30 201037230 factor)為60%。在使用砲彈型發光二極體 的顯示面’發光元件的點引人注目者為根 • 計,僅尖端附近發光,故輝亮部分所佔 .ratio)為約50%。因此,為與以往同等以 積率。 •[實施例六] . 使用由凸反射面構成的反射光栅,放 交方向有差的實施例是針對車輛用前照燈 〇使用黃色螢光體於藍色發光二極體的螢: 體’與使用橙色螢光體於青綠色發光二極 光二極體混色,並滿足可見光域的白色光 角等,則也能應用於聚光燈等。 ' 設車輛用前照燈的上下方向的放射角 由光源尺寸造成的誤差角度約4° ,則正 放射角7為6 ° 。由公式2傾斜光與頂部的 谷部的斜度沒為34° 。若設平行於反射光 ¢)角為20° ,設反射光栅薄長方形的長度為 8曲率半徑為40mm。顯示4對的凸反射面 圖於圖37,顯示車輛用前照燈的前視圖於 - 源部的一方為使用黃色螢光體於藍色發光 色發光二極體,他方為使用橙色螢光體於 體的螢光白色發光二極體。 在橢圓鏡的一方的焦點配設發光元件 配設螢光體。由接受激發光的螢光體發出 的習知的號誌燈 據透鏡形狀的設 的面積比(area 上的輝亮部的佔 射角在光栅的正 說明。光源為將 先白色發光二極 體的螢光白色發 源。若變更放射 為10° ,若扣除 交於反射光柵的 1斜度α為28° , 栅的方向的放射 1 4 m m,貝丨J由公式 光栅構成的剖面 圖38。左右的光 二極體的螢光白 青綠色發光二極 ’在他方的焦點 螢光至後方與前 3 1 201037230 方的拋物面鏡,來自後方的拋物面鏡的平行光藉由平面鏡 轉換方向並照射平行光於反射光柵方向。 • 若使40mA的正向電流(forward current )流到發光元 -件’則成為由2光源構成的1單元、〇. 28W,使用該單元橫 向11列’縱向8列合計88單元,得到轉換效率601m/W、 .14801m的光束。尺寸為橫向縱向170mm。顯示混色 的光譜於圖39。 交錯光束(beam)時若點亮下5列,則成為9201m,如 〇圖38所示若在單元的配置配設截止線(cutoff iine),則 可增加給予對向車的防眩效果。截止線斜的反射光柵是組 合橢圓鏡與雙曲線鏡並作成梯形狀的反射光栅。圖38是正 面看左側行駛車輛的情形之圖,顯示將上3段熄燈,交錯 光束的狀態。反射光栅若利用鋁等的金屬鏡面,則可兼用 散熱板。由上述構成造成的行駛光束時的全損失成為 24. 6W。在反射光栅陣列的周圍設有30mm寬的安裝空間時 的散熱板尺寸為橫向220m、縱向230m。若在該散熱板的後 ◎方配設導管(duct),以風速U=1 0m/s(36km/h)以上的行駛 風或強制對流冷卻,則由公式9,溫度上升為約2 5 °C。因 可由散熱板熱傳導到導管的壁面全體並可利用於散熱,故 • 可使溫度上升比約2 5 °C還降低。因公式9使用散熱板溫度 中的空氣的物性值,故需要重複計算,使用收斂條件附近 的50°C中的物性值 卜然托數(Prandtl number)Pr:0.71 熱導率(thermal conductivity) λ :0. ] 32 201037230 動力黏度(dynamic viscosity)^ :1.86x10_5 [m2/s] 雷諾數(Reynolds number)Re、那塞特數(Nusselt • number)Nu、平均熱傳遞率(average heat transfer rate) • a、溫度上升T可由公式ii求出。 設散熱板的縱尺寸L、橫尺寸w,設外部的空氣溫度為 .2 0 〇C。 [公式11 ]High Definiti〇n: Full HD) (1920xl080), | .1〇18 dragon, vertical 573mm, pixel spacing 53〇"m, sub-chapter 306 " m. The bottom surface of the light guide plate is arranged in three directions in the three directions. The cylindrical convex reflection surface B is irradiated to the lower right direction of the figure, and is obliquely upward, and is incident on the rhombic refracted light at the incident angle α. The convex light C of the convex reflecting surface Β contacting and forming the ribs is reflected obliquely upward to the upper right direction of the figure, and α is incident on the diamond-shaped refractive grating β. The light of the parallel light source Α in the left direction of the cylindrical convex reflecting surface is reflected obliquely upward' and incident on the diamond-shaped refractive grating. - The refractive surfaces A, B, and C of the triangular pyramidal refractive grating are converted in the direction and irradiated to the sub-pixels A, B, and C. Since the convexity of the light guide plate is small, the pixel size is enlarged, but the curvature radius of the convex reflection surface is constant due to the light guide. If the step s of the thickness of the light guide plate and the convex reflection surface is l〇"m, the radius of curvature! > The sub-pixels of the liquid crystal located in the direction perpendicular to the vertical direction are reflected from the light line, and are formed without being inclined to a critical angle of total reflection or more. The manufacturing cost is reduced. The light-emitting diode offset is placed at a position where the focus of the light source mirror does not obscure the reflected light of the parabolic mirror. By illuminating 540 light-emitting diodes with a luminous intensity of 240mcd, 540 light-emitting diodes with a luminous intensity of I40mcd are arranged with high image quality (Full-face size is a horizontally-shaped diamond-shaped side long convex reflection surface. Row light B reflection> Grid B. With the incident surface C, the incident angle A will be from the direction of the incident angle α to the vertical reflection surface, the thickness of the plate is constant, t is 1Omm, 1 5 9 // m. Parallel light reflection towards the source The layer, the paraboloid of the part can be obtained by the light source A. The light source B and g, and the brightness is 263 cd/m2 at a transmittance of 40 201037230 (light transmittance) 40. The power consumption at this time is about 130 W, which is white light. About 1/3 of the power consumption of the case of a diode and a color filter. The transparent material may be polymethyl methacrylate, all cyclic acrylic resin, or cyclic olefin resin (CyCi〇〇iefin) * resin), polycarbonate, photocurable acrylic resin (photocurable.acrylic res in), etc., can be formed by injection compression molding, etc. Since photohardenable acrylic resin is a low-viscosity monomer (m〇n〇mer), Oligomer polygomer As a starting material, starting molding is possible. [Embodiment 2] An illuminating device which displays a liquid crystal display device which is mixed into a three-color stripe in which a reflecting surface is arranged in a lattice shape is mainly shown in Fig. 14'. Figure 15. Diagonal 510·(20.1 type), XGA (1 024x768), the facet size is 4〇8_, 306 vertical, pixel spacing 399 /ira, sub-pixel spacing ^3"^. The three types of convex reflecting surfaces have a structure in which the number of pixels is evenly spaced by 1,024 segments. Since the convex reflecting surface difference of the light guide plate is smaller than the pixel size, it is enlarged into a pixel size, because the light guide plate has a thickness of $, The radius of curvature of the convex reflecting surface is constant. If the polar sequence t of the light guide plate is 10 mm and the difference s of the convex reflecting surface is ΙΟμπι, the upper radius r of the curvature radius is 159" m. The sub-pixel of the liquid crystal is located in the direction perpendicular to the vertical direction. Reflecting the τ~10 仃 线 line from the light source, the 乂夂 Μ Μ Μ Μ Μ Μ Μ Μ Μ 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 形成 可 可 可 可 可 可 可 可 可 可 可 可 可 可The focus of the parabolic mirror does not obscure the parabola The position of the reflected light of the mirror. By [..., the straw is configured with 128 colors of 27 201037230 light-emitting diodes of 250mcd, and the brightness is 307cd/m2 when the light transmittance is 4〇%. - [Example 3] An embodiment in which two colors of parallel light are incident on a light guide plate of a grating having a convex reflection surface in both directions and color mixing is described for a lamp in which a red light emitting diode and a green color light emitting body are used to synthesize yellow. An example of the refracting grating according to the fourth embodiment will be described by way of the fifth embodiment. Although called the blue signal, it is correct green. The color blindness strategy is shown in green with an indigo color. The yellow jg number is shown in orange-orange with orange. Fig. 32 is a cross-sectional view of a light lamp in which green and red parallel light is incident on a grating having a convex reflecting surface in both directions, and green and red are mixed in a yellow signal and displayed in yellow-orange. The top view is shown in Figure 3 2. The bottom surface of the light guide plate is a convex reflecting surface in the two directions shown in Fig. 11 - forming a triangular prism. Since the distance between the display surfaces of the lamps is about 5 m or more, the grating cannot be recognized when the width of the convex reflection surface is 5 mm or less, and is applied when the red light and the green light are emitted by the convex reflection grating at the same radiation angle in the same direction. ◎ The method of mixing colors does not produce stains. The two light source sections around the display surface are configured by a focus of each of the eleven elliptical mirrors, and are configured by a parabolic mirror to form parallel light and incident on one of the convex reflecting surfaces, and are disposed in one of the light source portions. The light-emitting diode is provided with a red light-emitting diode in the other light source portion. The pair of convex reflecting surfaces are reflected at the same radiation angle in the same direction, and the concave refractive surface of the surface of the light guide plate is enlarged to form a necessary radiation angle. The directionality of the conventionally irradiated road or the crossing path is a waste of the current consumption. However, if the radiation in the up and down direction is 28 201037230, the range is below the horizontal plane, and the radiation angle in the left and right direction is the soil 45. The range can be reduced by about 1/4 of the current consumption. Therefore, the necessary amount of light can be obtained even if one or half of the display surface is provided with red and green components. - If a cyan LED of 5 〇〇 nm or less is used and mixed with a red illuminator, the line on the chromaticity coordinates is close to the white field and becomes yellowish, so if 5 〇〇ηπι or more is used, The green light-emitting diode and the red light-emitting diode of 610 nm or more, the color mixture straight line follows the right side edge of the horseshoe-shaped chromaticity coordinate, so that the thick yellow color can be mixed. In the conventional color mixing, the color difference is reduced, and the number of light-emitting elements that are reduced by yellow on the display surface is reduced by the number. Therefore, not only can the intersection be seen, but also the current consumption is reduced, and the current consumption can be reduced. The improvement in efficiency is obvious. 'If the number of components is reduced, it will be difficult. However, since the number of light-emitting elements is reduced by the number of light-emitting elements (the fourth embodiment), the number of suspected points is one light, and the road side of the cost of the light can be used more. It is even more indistinguishable. Therefore, the phenomenon of lighting does not occur because of pointing. The conventional signal, which is necessary to reduce the knowledge of the cutting, is the convex reflection of the coarse wheel, which can be used to produce the surface illuminance according to the control of the ignoring light. The display shows that the two lamps of the wide-direction control of the grating also emit the grating, and the directionality of the components that can be cut can be wide, and the space can be reduced. In recent years, the taper of the number of components of the component is displayed, so the difference between the system and the luminous effect is 'the difference between the ten and the third embodiment, but the hb Gushan> the beneficial soil. The red light emitting diode is replaced by the refractive grating. A light with a cyan luminescent two 骽 骽 骽 。 。 。 。 。 2010 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 29 〇 unit. If 8 pairs of refractive 'gratings' are provided, it becomes a comb shape of 1. 5mm wide on one side, and is formed into a comb shape by a single side of the grating when it is displayed in red or green. 1. When a 5mm refraction grating is emitted, 'the distance from the surface of the display surface of the illuminator can not be obtained. The color difference is not generated by the uniformity of the radiation direction. The means for emitting the diffused light in the range of the necessary range (means) is a concave lens array as shown in Fig. 34. The concave lens array has a function of a dustproof and waterproof protective cover (H〇〇d) ^ [Embodiment 5] Reflective grating with red LED and cyan LED A yellow light is synthesized. If the reflection grating surface of the unit shown in Fig. 2 is formed into a 19 mm square shape, about 120 units can be arranged on the display surface having a diameter of 300 mm as shown in Fig. 36. If eight pairs of reflection gratings are provided, Then, it is a convex reflecting surface of 1. 5 mm wide on one side, and is formed into a comb shape by a single side of the grating when it is displayed in red or green. When red and green light are emitted by a reflection grating having a width of 1.5 mm, The grating is recognized by the distance to the display surface of the signal light. The color speckle is also produced by the uniformity of the radiation direction. The reflection grating expands the directivity by bending the reflection surface, and has the directivity of the size of the light-emitting element plus the original radiation angle. The setting surface of the curved reflection grating can be set and the directivity can be set. Therefore, the bending setting surface of the reflection grating can be set to the directivity according to the road condition. The directivity control has a degree of freedom than the convex reflection surface of the light guide plate and/or the guide. The characteristic of the refractive surface of the light plate is wide. Since the reflection grating shape is a structure in which the light source portions are arranged, the occupation ratio of the reflection surface (sPace 30 201037230 factor) is 60%. In the case of using a bullet-type light-emitting diode The point of the 'light-emitting element' is noticeable, and only the vicinity of the tip is illuminated, so the bright portion accounts for about 50%. Therefore, it is equivalent to the conventional rate. • [Embodiment 6] Using a reflective grating composed of a convex reflecting surface, the embodiment in which the direction of the delivery is poor is for a vehicle headlamp, a yellow phosphor is used for the blue light emitting diode, and the body is used with an orange phosphor. It can also be applied to spotlights, etc., when it is mixed with cyan-emitting diodes and satisfies the white light angle of the visible light field. ' Let the angle of the vertical direction of the vehicle headlamps be caused by the size of the light source. 4°, the positive radiation angle 7 is 6 °. The slope of the light from Equation 2 and the top of the valley are not 34°. If the angle parallel to the reflected light is 20°, the length of the thin rectangle of the reflective grating is 8 and the radius of curvature is 40 mm. The convex reflection surface of the four pairs is shown in Fig. 37, and the front view of the vehicle headlight is shown on the one side of the source portion. The yellow phosphor is used for the blue light emitting diode, and the other is the orange phosphor. Fluorescent white light-emitting diodes in the body. A phosphor is disposed in a light-emitting element disposed at one of the focal points of the elliptical mirror. The area ratio of the conventional horn light emitted by the phosphor receiving the excitation light according to the shape of the lens (the angle of incidence of the highlight on the area is indicated in the grating. The light source is the white light-emitting diode Fluorescent white source. If the change radiation is 10°, if the slope 1 of the reflection grating is 28°, the radiation in the direction of the grid is 14 mm, and the profile of the shell J is defined by the formula grating. The light-emitting diodes of the fluorescent white-green-green emitting diodes are fluorescent in the other side to the rear with the front 3 1 201037230 square parabolic mirror, the parallel light from the rear parabolic mirror is converted by the plane mirror and illuminates the parallel light Direction of the reflection grating. • If 40 mA forward current flows to the illuminator-piece ', it becomes a unit consisting of 2 light sources, 〇. 28W, using the unit horizontally 11 columns 'longitudinal 8 columns totaling 88 units A light beam with a conversion efficiency of 601 m/W and .14801 m is obtained. The size is 170 mm in the horizontal direction. The spectrum showing the color mixture is shown in Fig. 39. When the light beam is crossed, the next five columns are turned into 9201 m, as shown in Fig. 38. If in the unit The configuration of the cutoff iine can increase the anti-glare effect given to the opposite vehicle. The reflection grating with the cut-off line is a reflection grating combining the elliptical mirror and the hyperbolic mirror and forming a trapezoidal shape. Figure 38 is the front side of the left side. 6W, the total loss of the traveling beam caused by the above-mentioned configuration is 24.6W. The figure of the vehicle is turned off and the light is turned off. When the installation of a 30 mm wide installation space around the reflective grating array, the size of the heat dissipation plate is 220 m in the lateral direction and 230 m in the longitudinal direction. If the duct is disposed behind the heat dissipating plate, the wind speed U = 10 m/s. (36km/h) or more for traveling wind or forced convection cooling, the temperature rises to about 25 °C by Equation 9. Since the heat sink can be thermally conducted to the entire wall surface of the duct and can be used for heat dissipation, the temperature can be increased. It is lower than about 25 ° C. Since Equation 9 uses the physical property value of the air in the temperature of the heat sink, it is necessary to repeat the calculation, and use the physical property value of Prandtl number in the vicinity of the convergence condition (Prandtl number) Pr: 0.71 heat Thermal conductivity λ :0. ] 32 201037230 Dynamic viscosity ^ : 1.86x10_5 [m2/s] Reynolds number Re, Nusselt • number Nu, average heat transfer Average heat transfer rate • a. Temperature rise T can be obtained by Equation ii. Set the longitudinal dimension L and the horizontal dimension w of the heat sink, and set the external air temperature to .20 〇C. [Formula 11]

Re=u·L/vRe=u·L/v

Nu = 〇· 3 3 2 · Pf 诡Nu = 〇· 3 3 2 · Pf 诡

a—Nu·λ/ψ T=P/ (1. 1 0 3 * a · L · w) [實施例七] 藉由圖22、圖23等說明使用三角錐折射光柵,在3 .方向使用3種類的螢光轉換發光二極體的照明裝置的實施 .例。第一螢光轉換發光二極體A為激發波長44〇ηιη、榮光 波長 5 5 0 n m。第二#来μ掐义义也 _ ^ 禾®尤轉換發先二極體Β為激發波長 仍.螢光波長590.第三榮光轉換發光二極體c為教 〇發波長51〇,螢光波長59〇。因圖23為第一榮光轉換 發光二極體A與第二螢光轉換發._ w ?兴赞九一極體B之間的剖面 圖,故第三螢光轉換發光二極體(:未顯示。a—Nu·λ/ψ T=P/ (1. 1 0 3 * a · L · w) [Embodiment 7] A triangular-cone refractive grating is used as illustrated in Fig. 22, Fig. 23, etc., and 3 is used in the direction of 3. An example of the implementation of a lighting device for a fluorescent conversion LED. The first fluorescent conversion light-emitting diode A has an excitation wavelength of 44 〇ηιη and a glory wavelength of 550 nm. The second #来μ掐义义也_ ^ Wo® especially converts the first diode to the excitation wavelength still. The fluorescence wavelength is 590. The third glory conversion light-emitting diode c is the teaching wavelength of 51〇, fluorescent The wavelength is 59 〇. FIG. 23 is a cross-sectional view between the first glory-converted light-emitting diode A and the second fluorescent-converted light, _w? Xingzan, a first-pole body B, so the third fluorescent-converted light-emitting diode (: display.

- 發光元件1 A、1 B各自酎机於缸AL 六“。 配6又於軸外拋物面鏡6的焦點, 在紙面縱深方向各配設6個 拉 .ν 個藉由軸外拋物面鏡6轉換成 千订先,藉由分散配置於導光板24的反 射到三角錐折射光柵1 5。 Κ 為了使放射角成約±10。 , ^ = . 角錐折射光柵的射出面 33 201037230 作成凹折射面。 若使1 oomA的正向電流流到各發光元件,則成為合計 • 18個光源、6· 3W,得到轉換效率8〇lm/w、5〇〇lm的光束。 •扣色的光&如圖22所示為連續光譜的白色光。因可見光域 的包絡線(envel〇pe)近似於55〇〇κ的白色光故適合求高 .的色彩再現性’不包含紅外線避免溫度上升,it免因紫外 .線造成的損傷之用途。 [實施例八] 〇 說明使用三角錐折射光柵,在3方向使用6色的發光 一極體的LED燈泡的實施例。圖26為透視主要部分之斜視 圖。為了照射到三角錐折射光栅的3方向的光源為具有朝 在圖11說明的雙方向的凸反射面的導光板與雙方向的光 源顯不二角錐折射光柵與具有朝雙方向的凸反射面的導 光板的。彳面圖於圖28。具有朝雙方向的凸反射面的導光板 將來自兩方向的平行光擴大光束並反射在藉由導光板射 出面的凸折射面恢復成平行光後入射到三角錐折射光柵。 〇因一角錐折射光柵的射出光為平行光,故配設凹折射面11 • 光束成必要的放射角。放射角窄的情形如圖27所示 以凹折射面構成三角錐折射光柵也可以。混色的光譜如圖 • 31所示為連續光譜的白色光。 【圖式簡單說明】 圖1是顯示三角波狀反射光柵之剖面圖。 圖2是顯示三角波狀凸面反射光柵之側視圖。 34 201037230 圖3是顯示頂部斜度、谷部斜度與放射角之圖。 圖4是顯示由光源尺寸造成的放射角誤差之圖。 圖5是顯示併用反射光栅與透射部的3色條紋顯示裝 _ 置之圖。 圖6是顯示組合凸三角錐反射光栅與凹三角錐反射光 . 柵的構造之俯視圖。 圖7是顯示利用三角波狀折射光柵進行的混色之原理 圖。 ^ 圖8是顯示利用三角錐折射光柵進行的混色的原理之 斜視圖。 圖9是顯示組合凸三角錐折射光柵與凹三角錐折射光 栅的構造之俯視圖。 圖10是顯示利用凸反射面進行的光束擴大之原理圖。 圖11是顯示利用成對的凸反射光栅進行的混色與放 射角之圖。 圖12是顯示併用凸反射面光柵與透射部的多色條紋 ❹的導光板之圖。 圖13是顯示併用凸反射面光栅與透射部的兩層構造 的3色條紋的導光板之圖。 . 圖1 4是顯示將凸反射面光柵配置於導光板底面側的 一片構成的3色條紋的導光板之圖。 圖1 5是顯示一片構成的3色條紋導光板的主要部分擴 大圖。 圖16是顯示擴散光的入射射出角之圖。 35 201037230 圖17是顯示併用凸反射光柵與三角錐折射光柵 晶顯示裝置的導光板之剖面圖。 圖18是顯示由一個凸反射光柵照射到複數個三 •折射光拇的液晶顯示裝置的導光板之剖面圖。 圖19是顯示在導光板的底面配置3種類的凸反 .栅,在導光板側面配置3種類的光源之俯視圖。 ' 圖是顯示併用凸反射光柵與三角錐折射光柵 晶顯示裝置的導光板之剖面圖。 Ο 圖21是顯示由菱形次像素構成的6角形像素的液 示裝置之俯視圖。 圖22是顯示由3種類的螢光轉換發光二極體與三 折射光栅的混色構成的燈之剖面圖。 圖23是顯示藉由3種類的螢光轉換發光二極體與 -的二角錐折射光栅混色的燈之剖面圖。 圖24是顯示藉由凹透鏡使三角錐折射光柵的射 擴散之剖面圖。 Ο 圖25是顯示藉由三角錐折射光柵的凹折射面使 . 光擴散之剖面圖。 圖26是顯示由6種類的發光二極體與三角錐折射 的混色構成的燈之主要部分透視圖。 . 圖27是顯示由6種類的發光二極體與凹面的三角 射光柵的混色構成的燈之剖面圖。 圖28是顯示射出側的三角錐折射光柵為兩色混 射光柵尺寸的兩倍的情形的混色之圖。 的液 角錐 射光 的液 晶顯 角錐 凹面 出光 射出 光柵 錐折 色折 201037230 圖29是顯示以凹面的三角錐折射光栅與導光板底面 的凸反射面擴大光束的燈之剖面圖。 • 圖30是顯示由3種類的螢光白色發光二極體的混色產 生的合成光譜之圖。 圖31是顯示由6種類的發光二極體的混色產生的合成 光譜之圖。 圖32是顯示以凸反射面擴大光束並混色的號誌燈的 實施例之剖面圖。 〇 圖33是顯示以凸反射面擴大光束並混色的號誌燈的 實施例之俯視圖。 圖34是顯示由三角波狀折射面光柵構成的混色裝置 之圖。 圖35是顯示由折射光柵構成的交通號誌燈的顯示面 之圖。 圖36是顯示由反射光柵構成的交通號誌燈的顯示面 之圖。 Q 圖37是顯示凸面光栅單元之剖面圖。 . 圖38是顯示車輛用前照燈之前視圖。 圖39是顯示由2種類的螢光白色發光二極體的混色產 . 生的合成光譜之圖。 圖40是僅顯示由圓錐型散射面產生的習知的混色裝 置中的前方散射光之模式圖。 圖41疋顯示使晶粒附近的反射鏡急遽傾斜,緩和色斑 並混色的封裝的習知例之圖。 37 201037230 圖42是顯示以45。的溝的界面全反射於液晶面 向的無彩色濾光片的習知例之圖。 圖43是顯示藉由條紋寬的積層導光體將3色光供 .液晶條紋的習知例之圖。 圖44是顯示藉由配設於導光板的四角錐的斜度 -射3色光到規定的像素的習知例之圖。 - 圖45是顯示由梯田狀凸反射面導光板與條紋分 件構成的3色液晶顯示裝置的習知例之圖。 〇 圖46是顯示使兩方向的光入射到直角稜鏡,並用 鏡並’在色的習知例之圖。 【主要元件符號說明】 板方 給到 面照 配元 帶通 1:發光元件 4 :三角波狀光柵 5 : 凸反射面 5A、5B、5C:凸反射面 6 :拋物面鏡 8:橢圓鏡 9: 雙曲線鏡 1 〇 :凸折射面 11 :凹折射面 15 :折射光柵 15A ' 15B、15C:折射面 1 8 :透光物質 19:平行光 20 :擴散光 21 .凹面鏡 22:凸面鏡 24 :導光板 2?:次像素 27A 、 27B 、 27C: 次像素 2 8 :液晶失持基板 29 :基板 30 :電路基板 31 :谷部 32 :頂部 33 :空氣層 3 7 :入射面 38 :支撐構件 39 :散射面 40 :焦點 42 :溝 38 201037230 44 : 四角錐 45 :入射光 4 6 :光源 47 : 帶通鏡 4 8 :偏光板 4 9 :棱鏡 • 50 : 基準面 5 1 :死角 ο 〇 39- The light-emitting elements 1 A and 1 B are each driven in the cylinder AL 6. "The 6 is placed in the focus of the off-axis parabolic mirror 6 and 6 pulls are arranged in the depth direction of the paper. ν are converted by the off-axis parabolic mirror 6. Thousands of orders are made by the dispersion of the light guide plate 24 to the triangular pyramidal refraction grating 15. Κ In order to make the radiation angle about ±10, ^ = . The exit surface 33 of the pyramidal refractive grating 33 201037230 is a concave refractive surface. When the forward current of 1 oomA flows to each of the light-emitting elements, it becomes a total of 18 light sources and 6.3 W, and a light beam with a conversion efficiency of 8 〇lm/w and 5 〇〇lm is obtained. 22 shows the white light of the continuous spectrum. Since the envelope of the visible light region (envel〇pe) is similar to the white light of 55 〇〇 κ, it is suitable for high color reproducibility 'excluding infrared rays to avoid temperature rise, it is free of Use of damage by ultraviolet rays. [Embodiment 8] An embodiment of an LED bulb using a six-color light-emitting diode in three directions using a triangular pyramidal refractive grating will be described. Fig. 26 is a perspective view of a main portion in perspective. The light source for the three directions in order to illuminate the triangular cone refractive grating is There are a light guide plate having a convex reflection surface in both directions as illustrated in Fig. 11 and a light guide plate having a birefringent refractive index in a bidirectional direction and a convex reflection surface having a bidirectional direction. Fig. 28 is a plan view. The light guide plate of the convex reflection surface of the two directions expands the parallel light from the two directions and reflects the convex light on the exit surface of the light guide plate to return to the parallel light and then enters the triangular cone refraction grating. Since the emitted light is parallel light, the concave refractive surface 11 is provided. • The light beam has a necessary radiation angle. The radiation angle is narrow as shown in Fig. 27. The concave refractive surface may be a triangular refractive index grating. The spectrum of the mixed color is shown in Fig. 31. Figure 1 is a cross-sectional view showing a triangular wave-shaped reflection grating. Fig. 2 is a side view showing a triangular wave-shaped convex reflection grating. Fig. 4 is a diagram showing the radiation angle error caused by the size of the light source. Fig. 5 is a diagram showing the 3 color stripe display device of the reflection grating and the transmissive portion. Fig. 6 is a plan view showing the structure of a combined convex triangular pyramid reflection grating and concave triangular pyramid reflection light. Fig. 7 is a schematic diagram showing color mixing by a triangular wave refractive grating. ^ Fig. 8 is a view showing a triangular pyramidal refractive grating Fig. 9 is a plan view showing the structure of a combined convex triangular pyramidal refractive grating and a concave triangular pyramidal refractive grating. Fig. 10 is a schematic diagram showing beam expansion by a convex reflecting surface. Fig. 12 is a view showing a light guide plate of a pair of convex reflection gratings. Fig. 12 is a view showing a light guide plate of a multi-color stripe of a convex reflection grating and a transmissive portion. Fig. 13 is a view showing a convex reflection grating and a transmission portion. A two-layered structure of a 3-color striped light guide. Fig. 14 is a view showing a light guide plate of a three-color stripe in which a convex reflection grating is disposed on the bottom surface side of the light guide plate. Fig. 15 is a main portion enlarged view showing a three-color stripe light guide plate of one piece. Fig. 16 is a view showing an incident exit angle of diffused light. 35 201037230 Figure 17 is a cross-sectional view showing a light guide plate using a convex reflection grating and a triangular pyramid refractive grating crystal display device. Figure 18 is a cross-sectional view showing a light guide plate of a liquid crystal display device which is irradiated to a plurality of three-refractive optical arms by a convex reflection grating. Fig. 19 is a plan view showing three types of convex reverse gratings arranged on the bottom surface of the light guide plate and three types of light sources arranged on the side surface of the light guide plate. The figure is a cross-sectional view showing a light guide plate of a convex reflection grating and a triangular pyramid refractive grating crystal display device. Figure 21 is a plan view showing a liquid crystal display device of hexagonal pixels composed of diamond-shaped sub-pixels. Fig. 22 is a cross-sectional view showing a lamp comprising a mixture of three types of fluorescent conversion light-emitting diodes and a three-refracting grating. Figure 23 is a cross-sectional view showing a lamp in which three types of fluorescent conversion LEDs are mixed with a two-cone refractive grating. Figure 24 is a cross-sectional view showing the diffusion of a triangular pyramidal refractive grating by a concave lens. Figure 25 is a cross-sectional view showing light diffusion by a concave refractive surface of a triangular pyramidal refractive grating. Fig. 26 is a perspective view showing a main portion of a lamp comprising a mixture of six types of light-emitting diodes and triangular cones. Fig. 27 is a cross-sectional view showing a lamp comprising a mixture of six types of light-emitting diodes and a concave triangular grating. Fig. 28 is a view showing the color mixture in the case where the triangular pyramidal refractive grating on the exit side is twice the size of the two-color hybrid grating. The liquid pyramid of the liquid cone shows the concave surface of the liquid cone. The light exits the grating. The cone is folded. The color is folded. 201037230 Fig. 29 is a cross-sectional view showing the lamp with a concave triangular pyramidal refractive grating and a convex reflecting surface on the bottom surface of the light guide plate. • Fig. 30 is a view showing a synthesized spectrum produced by color mixing of three types of fluorescent white light-emitting diodes. Fig. 31 is a view showing a synthesized spectrum produced by color mixing of six types of light-emitting diodes. Fig. 32 is a cross-sectional view showing an embodiment of a horn lamp in which a light beam is enlarged by a convex reflecting surface and mixed. Fig. 33 is a plan view showing an embodiment of a lamp which enlarges a light beam by a convex reflecting surface and mixes colors. Figure 34 is a view showing a color mixing device composed of a triangular wave-shaped refractive surface grating. Fig. 35 is a view showing a display surface of a traffic light lamp composed of a refractive grating. Fig. 36 is a view showing a display surface of a traffic light lamp constituted by a reflection grating. Q Figure 37 is a cross-sectional view showing a convex grating unit. Figure 38 is a front view showing a headlight for a vehicle. Fig. 39 is a view showing a synthetic spectrum produced by color mixing of two types of fluorescent white light-emitting diodes. Fig. 40 is a schematic view showing only forward scattered light in a conventional color mixing device produced by a conical scattering surface. Fig. 41 is a view showing a conventional example of a package in which the mirror in the vicinity of the crystal grain is sharply tilted, the stain is moderated, and the color mixture is mixed. 37 201037230 Figure 42 is shown at 45. A diagram of a conventional example in which the interface of the groove is totally reflected by the achromatic filter of the liquid crystal surface. Fig. 43 is a view showing a conventional example in which three color lights are supplied to liquid crystal stripes by a laminated light guide having a wide stripe. Fig. 44 is a view showing a conventional example in which the inclination of the quadrangular pyramid disposed on the light guide plate is applied to a predetermined pixel. - Fig. 45 is a view showing a conventional example of a three-color liquid crystal display device comprising a terrace-like convex reflecting surface light guide plate and stripe members. 〇 Fig. 46 is a view showing a conventional example in which light in both directions is incident on a right angle 稜鏡 and a mirror is used. [Description of main component symbols] Plate-side surface-matching bandpass 1: Light-emitting component 4: Triangle-wave grating 5: Convex reflector surface 5A, 5B, 5C: Convex reflector surface 6: Parabolic mirror 8: Elliptical mirror 9: Double Curved mirror 1 〇: convex refractive surface 11: concave refractive surface 15: refractive grating 15A '15B, 15C: refractive surface 18: light-transmitting substance 19: parallel light 20: diffused light 21. concave mirror 22: convex mirror 24: light guide plate 2 ?: sub-pixels 27A, 27B, 27C: sub-pixels 2 8 : liquid crystal off-board 29 : substrate 30 : circuit substrate 31 : valley 32 : top 33 : air layer 3 7 : incident surface 38 : support member 39 : scattering surface 40: Focus 42: Groove 38 201037230 44 : Quadrilateral cone 45: Incident light 4 6 : Light source 47 : Band-pass lens 4 8 : Polarizer 4 9 : Prism • 50 : Reference plane 5 1 : Dead angle ο 〇 39

Claims (1)

201037230 七、申請專利範圍: 1、—種照明裝置,其特徵為如下的. • 在水平面基板上接觸長方形平面 ^ ' 缸七久射面的長邊’使 •軸方向正交於來自光源的平行光的行進方向 藉由接觸並重複排列長方形平° •邊,形成三角波狀反射光柵, 射面的接鄰的 :由兩個長方形平面反射面相等地對稱配設長方形 面反射面的紐軸方向與水平面構成的斜度, 〇 藉由與長方形平面反射面的短軸方;的斜度相等的 角配設兩個平行光光源於對稱方向,其中 來自對稱方向的平行光光源雙方的平行光各自僅入 到對向於平行光光源的側的反射面並反射到基板平W ’直上方,冑由雙方的平行A光源A射的光都&射到H 方並與射出方向一致而混合。 2、一種照明裝置,其特徵為如下的構造. 在基板的水平面上使菱形反射面的一方的對角線與 〇準面平行,配置菱形反射面於正交於來自3方向 _ 口^的十竹' . 光源的平行光的行進方向, 藉由接觸比菱形平面反射面的水平對角線還上侧的 鄰的邊彼此且排列成三角錐狀,在比水平面叆 吗逖上形成凸 的三角錐反射光柵, 藉由接觸比菱形平面反射面的水平對角線還下側的 鄰的邊彼此且排列成三角錐狀,形成比水平面淨 | w艰凹陷的 型三角錐反射光栅,其中 長 長 平 仰 射 鉛 上 基 光 接 型 接 凹 40 201037230 將位於距水平 曲相專的仰角的來自3方向的平行 源的平行光僅入射到翻—* 町$』朝二角錐反射面的光源的側的反 並反射到基板平面的金L吉μ + .,, W私1上方,使由3方向入射的光 射到錯直上方並與射屮古a • 、耵出方向一致而混合。 3、一種照明驻® 裝置’其特徵為由如下的構造構成: . 在水平面上接觸·&士·:η/ A = 丧觸長方形凸反射面的長邊,將長方 反射面的長轴方向邴罢认七上 , - 门配置於來自光源的平行光的行進方 正交方向, 〇 #由接觸長方形凸反射面的長邊彼此且對稱地排 棱’將其配置複數摘 取4、 及數個形成三角波狀反射光栅, 具有.長方形凸反射面的短軸方向其頂稜部中的 方向切線與水平面構成的斜度α,谷部中的短轴方向 與水平面構成的斜度沒之彎曲, 藉由/、長方开)凸反射面的頂部中的短轴方向切線 度“目等的仰角配設兩個平行光光源於對稱方向, 以距水平面的斜度α入射的平行光藉由凸反射面 〇並以放射角r擴大光束, • 3〇 ~7/3,$=45。~a/2+r/2 設定,其 來自對稱方向的平行光光源雙方的平行光各自僅 •到朝反射光柵的光源的側的反射面,朝水平面的大致 方向反射來自複數光源的光。 4、-種照明裝置,其特徵為如下的構造: 使長方形巴反射面的長邊接觸" 上侧’使長方形凸反射面的長轴方向正交於來自光源 光光 射面 都反 形凸 向的 列成 短軸 切線 的斜 反射 入射 鉛直 面的 的平 201037230 行光的行進方向, 接觸長方形凸反射面的長邊彼此,以像素寬X的間距 • 對稱地配置長方形凸反射面成稜,並形成三角波狀反射光 柵, 藉由液晶次像素的透射部的寬度W、凸反射面到被照 • 射面的距離ΐ、凸反射面的曲面長度d,以r = 2.t.d/(W-d/ ./2) »又疋長方形凸反射面的短轴方向的曲率半徑, 以長方形凸反射面的段差s、像素寬X,以斜度0 〇 i-tan (s/X)將兩個平行光光源配設於對稱方向, 在導光板底部的水平面的下側以像素寬χ的間距配置 長方形凸反射面的三角波狀反射光柵, 配設藉由長方形凸反射面的段差s、像素寬χ,以斜度 θ 1 t^an (s/χ)由水平面下側入射的平行光光源,其中 "吏比水平面還上側的成對的長方形凸反射面反 射的兩色的反射光,盥 一社比水千面還上側的凸反射面的間 距間以比水平面摄e Η的長方形凸反射面反射的別色光透 〇射’並照射到導光板上 上的混色。 液a曰面板像素,進行3色光以 5、一種照明护罢 使長方形凸、,’、特徵為如下的構造: 上,使長方形凸及面的長邊接觸導光板底部的水平面 ' 反射面的長 光的行進方向4 向正交於來自光源的平行 排列成稜, 、y凸反射面的長邊彼此並對稱地 藉由液晶次係ι π 、、透射部的寬度w、凸反射面到被照 201037230 射面的距離t、凸反射面的曲面長度d,以r = 2, 2)設定長方形凸反射面的短轴方向的曲率半 . 以像素寬X的間距配置對稱於長邊彼此接 方形凸反射面並形成三角波狀反射光栅, 藉由長方形凸反射面的段差s、像素寬X .i = t arT1 ( s /X )配設兩個平行光光源於對稱方向 將以像素寬X的間距配置長方形凸反射面 波狀反射光柵的別的導光板配設於該導光板的 ^ 將藉由長方形凸反射面的段差s、像素寬: 〇 iztarT's/X)入射的平行光光源配設於下側的 中 藉由使以上側的導光板的成對的長方形凸 - 的兩色的反射光,與在上側的導光板的凸反射 以下側的導光板的長方形凸反射面反射的別色 照射到導光板上部的液晶面板像素,進行3色 色。 q 6、一種照明裝置’其特徵為如下的構造: 在平面的基準面上排列折射率比周圍介質 複數個二等邊三角柱狀體, 以朝折射面的入射角與折射角的差分的角 邊三角柱狀體的斜度面與基準面的法線構成的 成三角波狀並形成光桃折射面, 在朝平面的基準面的下側的仰角相等的對 平行光光源,其中 • t· d/(W-d/ 徑, 觸的稜的長 ,以斜度Θ , 並形成三角 下侧, ί,以斜度0 導光板,其 反射面反射 面的間距間 光透射,並 光以上的混 大的物質的 度設定二等 角度’排列 稱方向配設 43 201037230 來自 到對向於 . 上方,由 與射出方 將菱 並排列比 邊,形成 接觸 邊’形成 以朝 折射面與 到低折射 來自 的側的折 一致而混 Ο 由基準面的下侧入鼾 ^ # # , 的雙方的平行光各自僅入射 十订先先源的側的批 # . ^ , χ 折射面並折射於基準面的鉛直 雙方的平打光光源入 干四 射的光都折射到鉛直上方並 句一致而混合。 -種照明裝置,其特榭* 、荷欲為以如下的構造. 形折射面的一方的Μ & . Λ m ^ ι- & 、角線配設於基準面上,接觸 巷旱面上的對角镇潘 6 、側的菱形折射面的接鄰的 凸型的二角錐折射光柵, 並排列比對角線還 tb ^ m ^ ^ 側的菱形折射面的接鄰的 比基準面凹陷的凹型 J —用錐折射夯—, 折射面的入射角與折射 、角的差分的角产母定赛形 基準面的法線構成的斜 又°又疋菱 率側,其中 角由两折射率侧射出 3方向的光源的平行光 ^ ^ ^ ^ AL , 目僅入射到對向於光源 射面並折射到基準面的鉛 合。 |上方,並與射出方向 〇 8、一種照明裝置’其特徵為 • I導光板的射出面形成"專利r構‘構成: 折射光拇,在導光板的底面第*項之三角雖 、,二導光板的側面對底面傾斜的平行光入射到凸反射 三角錐折射光柵並照射 平行光照射到由菱形的 以凸反射面擴大光束並反射到 到次像素,將來自3方向的3色的 次像素構成的像素。 44 201037230 9、如申請專利範圍第8項之照明裝置,其中藉由 板底面的圓筒凸反射面以比像素數少的列數構成,由 • 圓筒凸反射面照射到複數個次像素的列,擴大凸反射 . 尺寸,使成型容易。 1 0、如申請專利範圍第8項之照明裝置,其中由 • 的構造構成: • 平行地形成於導光板側面的對向的兩邊,接觸圓 反射面的頂稜並在導光板底面形成三角柱狀, 0 在兩個三角柱狀凸反射面之間,於與三角柱狀凸 面正交的方向配設複數個凸反射面, 由配設於導光板側面的對向的兩邊的兩色的光源 到三角柱狀圓筒凸反射面, 由配設於與三角柱狀凸反射面正交的方向的光源 到與二角柱狀凸反射面正交的方向的凸反射面,其中 將來自3方向的平行光入射到三角錐折射光拇的 的折射面並入射到3個次像素。 〇 11、如申請專利範圍第8項之照明裝置,其中在 •於二角柱狀凸反射面的方向的凸反射面的長軸方向形 面, • #由照射比正交於三角柱狀凸反射面的方向的凸 面的長轴方向長度長的範圍,照射到該三角&狀凸反 的上部的像素。 1 2、如申請專利範圍帛8項之照明裝f,其中由 的構造構成:在由菱形折& 八 乂奸射面構成的二角錐折射光柵 導光 一個 面的 如下 筒凸 反射 照射 照射 對向 正交 成曲 反射 射面 如下 的上 45 201037230 方配置由以3個菱形的次像素構成的6角 晶面板,藉由二角錐折射光栅將以凸反射 • 的光折射並照射到曼形的次像素,其中 以6角形的像素將3方向的光混色並 1 3、如申請專利範圍第3項之照明裝 .水平面上正父於來自光源的平行光的行進 •構造排列長方形凸反射面的長軸方向之反 燈的顯示面’將在一方的拋物面鏡或拋物 〇的焦點配設紅色發光元件,在另外的拋物 似曲率圓鏡的焦點配設綠色發光元件之平 距水平面的仰角相等的對稱方向, 紅信號時點亮紅色發光元件,並以反 ' 紅色顯示, 綠信號時點亮綠色發光元件,並以反 綠色顯示, 藉由黃色信號時點亮紅色發光元件與 〇由雙方將平行光入射到反射光栅並混色, 識0 •1 4、如申請專利範圍第6項之照明裝 的基準面上排列由折射率比周圍介質大的 個二等邊三角柱狀體, 為以如下構件構成的號誌燈的顯示3 入射角與折射角的差分的角度將複數個二 的斜度面與基準面的法線構成的角度排列 形像素構成的液 面反射的3方向 進行彩色顯示。 置,其中藉由在 方向,並以波狀 射光拇構成被諸、 面近似曲率圓鏡 面鏡或拋物面近 行光光源配設於 射光柵反射進行 射光柵反射進行 綠色發光元件, 被當作橙黃色辨 置,其中在平面 物質構成的複數 ':以朝折射面的 等邊三角柱狀體 成三角波狀,構 46 201037230 成由高折射率側射出到低折射率侧的折射面之折射 由在一方的拋物面鏡或拋物面近似㈣圓鏡的焦點 -色發光元件,與在另外的拋物面鏡或抛物面近似曲 的焦點配設綠色發光元件的構造構成的平行光光源 擴大放射角配設於折射光栅的前面的凹折射面, • 於朝平面的基準面的下側的仰角相等的對稱方 該平行光光源, 在為了入射到折射光柵之成對的光源部的焦點 0色發光元件與綠色發光元件, 紅信號時點亮紅色發光元件並以折射光柵折射 色顯示, 綠信號時點亮綠色發光元件並以折射光柵折射 - 色顯示, . 藉由黃色彳§號時點亮紅色發光元件與綠色發光 由雙方將平行光入射到折射光柵並混色,被當作撥 識。 q 1 5、如申請專利範圍第3項之照明裝置,其中 射光栅與具有不同的激發波長的複數個發光元件並 藉由激發波長長的發光元件的波高值補足激發 的側的發光元件的波高值與其螢光波長的中間域, 藉由以反射光柵加上複數個螢光域的波高值, 等地混合激發光的波高值與被加上的螢光域的波高 1 6、如申請專利範圍第6項之照明裝置,其中 射光柵與具有不同的激發波長的複數個發光元件並 光柵; 配設紅 率圓鏡 ;為了 向配設 配設紅 進行紅 進行綠 元件, 黃色辨 使用反 混色, 波長短 大致均 值。 使用折 混色, 47 201037230 藉由激發波長長的發光元件的波高值補足 的侧的發光元件的波高值與其螢光波長的中間 • 藉由以折射光柵加上複數個螢光域的波高 . 等地混合激發光的波高值與被加上的螢光域的 1 7、如申請專利範圍第3項之照明裝置, . 基板的水平面上以三角波狀構造排列長方形凸 . 方形平面反射面形成反射光栅, 於距水平面的仰角相等的對稱方向配設平 0 藉由在散熱基板上將由複數個該反射光柵 單位排列於橫方向,使一部分的反射光柵構成 弯曲成截止線的形狀而構成, 為將橫方向的反射光柵列排列複數個於縱 '車輛用前照燈, 藉由點亮所有的反射光柵列照射行駛光束 將橫方向的反射光柵列排列於縱向的一部分的 錯光束。 Ο 1 8、如申請專利範圍第7項之照明裝置, •光栅谷部中的切線的斜度的凹面構成三角錐折 度面, 擴大折射光柵的射出光的放射角。 1 9、如申請專利範圍第3項之照明裝置, 形凸反射面的長邊接觸水平面,將長軸方向配 源的平行光的行進方向的正交方向’以曲率半 圓周的曲面長度d的凸反射面反射來自兩方向 激發波長短 域, 值,大致均 波尚值。 其中在散熱 反射面或長 行光光源, 構成的構成 單位傾斜, 向而構成的 ,藉由點亮 列,照射交 其中以折射 射光柵的斜 其中使長方 置於來自光 徑r、沿著 的平行光, 48 201037230 以放射角0 =d. 360° /(27rr)朝同一方向混色並射出。201037230 VII. Patent application scope: 1. A kind of lighting device, which is characterized as follows: • Contact the rectangular plane on the horizontal plane ^ 'The long side of the cylinder seven-time surface' makes the axis direction orthogonal to the parallel from the light source The traveling direction of the light is formed by the contact and repeating arrangement of the rectangular flat sides, forming a triangular wave-shaped reflection grating, and the adjacent sides of the emitting surface are: the two axis planes are equally symmetrically arranged with the rectangular axis reflecting surface The slope of the horizontal plane is configured by arranging two parallel light sources in a symmetrical direction by an angle equal to the slope of the short axis of the rectangular plane reflecting surface, wherein the parallel light from both sides of the parallel light source in the symmetrical direction is only The light enters the reflecting surface on the side opposite to the parallel light source and is reflected directly above the substrate plane W', and the light emitted by both parallel A light sources A is incident on the H side and mixed with the emission direction. 2. An illuminating device characterized by the following structure. A diagonal line of a rhomboid reflecting surface is parallel to a quasi-surface in a horizontal plane of the substrate, and a rhomboid reflecting surface is disposed orthogonal to the ten from the 3-direction _ mouth ^ Bamboo'. The direction of travel of the parallel light of the light source is formed by a triangular triangle on the upper side of the horizontal plane by contacting the adjacent sides of the horizontal diagonal of the rhomboid plane reflecting surface and arranging the triangles on the upper side. The cone-reflecting grating is formed by a triangular pyramid shape by contacting the adjacent sides of the horizontal diagonal and the lower side of the rhomboid plane reflecting surface, thereby forming a triangular pyramidal reflection grating which is more concave than the horizontal plane, wherein the long flat Up-and-down lead-based optical connection type recess 40 201037230 Parallel light from a parallel source of 3 directions located at an elevation angle specific to the horizontal curved phase is incident only on the side of the light source facing the dioptric cone reflecting surface The light is reflected back to the plane of the substrate, and the light incident from the three directions is incident above the misalignment and mixed with the direction of the shot a • and the exit. 3. A lighting station device is characterized by the following structure: . Contact on a horizontal surface · & 士:: η / A = long side of the concave convex reflecting surface, the long axis of the rectangular reflecting surface The direction 邴 七 , , - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - 门 门 门 门 门 门 门 门The plurality of triangular wave-shaped reflection gratings have a slope α formed by a tangential line in a vertex portion of the rectangular convex reflecting surface and a horizontal plane, and a slope formed by a short axis direction and a horizontal plane in the valley portion is not bent. By the tangential degree of the short axis direction in the top of the convex reflecting surface by "/, the square opening" "the elevation angle of the eye is arranged in two symmetrical directions in the symmetry direction, and the parallel light incident at a slope α from the horizontal plane is used by The convex reflecting surface 〇 and the beam is enlarged by the radiation angle r, • 3〇~7/3, $=45.~a/2+r/2 is set, and the parallel light from both sides of the parallel light source in the symmetrical direction is only Reflection towards the side of the source of the reflective grating The surface reflects the light from the plurality of light sources in a general direction of the horizontal plane. 4. An illumination device characterized by the following structure: making the long side of the reflective surface of the rectangular bar contact " the upper side making the long axis of the rectangular convex reflecting surface The direction is orthogonal to the direction of travel of the flat 201037230 row light from the obliquely incident incident vertical plane of the short-axis tangent line from the light source light-emitting surface, and the long sides of the rectangular convex reflection surface are in contact with each other, in pixels wide Spacing of X • The rectangular convex reflecting surface is symmetrically arranged to form a triangular wave-shaped reflecting grating, and the width W of the transmitting portion of the liquid crystal sub-pixel, the distance from the convex reflecting surface to the illuminated surface, and the convex reflecting surface The length d of the surface is r = 2.td/(Wd/ ./2) » and the radius of curvature of the short convex axis of the rectangular convex reflecting surface, the step s of the convex convex reflecting surface, the pixel width X, and the slope 0 〇i-tan (s/X) aligns two parallel light sources in a symmetrical direction, and arranges a triangular wave-shaped reflection grating with a rectangular convex reflection surface at a pitch of pixels wide on the lower side of the horizontal plane at the bottom of the light guide plate. By a step s of a rectangular convex reflecting surface, a pixel width χ, a parallel light source incident from the lower side of the horizontal plane with a slope θ 1 t^an (s/χ), wherein the pair is rectangular on the upper side of the horizontal plane The two-color reflected light reflected by the convex reflecting surface is irradiated by a different color light reflected from the rectangular convex reflecting surface of the upper surface than the horizontal convex surface of the water surface. The color mixture on the light board. The liquid a 曰 panel pixel, 3 colors of light to 5, a kind of illumination to protect the rectangle convex, ', characterized by the following structure: The upper side of the rectangular convex surface and the bottom of the light guide plate The traveling direction 4 of the long light of the horizontal plane 'reflecting surface is aligned perpendicular to the parallel line from the light source, and the long sides of the y convex reflecting surface are symmetrically symmetric with each other by the liquid crystal system ι π , the width w of the transmitting portion, The distance from the convex reflecting surface to the surface of the 201037230 emitting surface and the curved surface length d of the convex reflecting surface are set to r = 2, 2). The curvature of the short convex axis of the rectangular convex reflecting surface is set to be half. Long sides to each other The convex reflecting surface forms a triangular wave-shaped reflection grating, and the two parallel light sources are arranged in the symmetry direction by the pixel width X by the step s of the rectangular convex reflecting surface and the pixel width X.i = t arT1 ( s /X ) The other light guide plate of the rectangular convex reflecting surface wave-shaped reflective grating is disposed on the light guide plate, and the parallel light source incident by the step s of the rectangular convex reflecting surface and the pixel width: 〇iztarT's/X) is disposed under In the side, the reflected light of the two sides of the light guide plate on the upper side is irradiated with the other color reflected by the rectangular convex reflection surface of the light guide plate on the lower side of the convex reflection of the upper light guide plate. The liquid crystal panel pixels on the upper portion of the light guide plate are colored in three colors. q 6. An illuminating device' is characterized by the following structure: arranging a plurality of equilateral triangular prisms having a refractive index larger than that of the surrounding medium on a plane reference plane, and a corner of the difference between the incident angle and the refraction angle of the refractive surface The inclined surface of the triangular column and the normal of the reference surface form a triangular wave shape and form a refracting surface of the light peach, and the parallel light source having the same elevation angle on the lower side of the reference plane toward the plane, wherein • t·d/( Wd/ diameter, the length of the touched rib, with a slope Θ, and the lower side of the triangle, ί, with a slope of 0 light guide plate, the light of the reflective surface of the reflective surface is transmitted, and the light above the mixed substance Degree setting second-order angle 'arrangement direction arrangement 43 201037230 From to the opposite direction. Above, the edge is arranged side by side with the injection side, forming the contact edge 'formed to the side of the refractive surface and the side from which the low refraction comes Consistent and confusing The parallel light from both sides of the reference plane into the 鼾^##, each of which is only incident on the side of the ten-first source. # , ^ 折射 The refractive surface is refracted to the flat side of the reference plane. Light The light from the dry light is refracted to the vertical and mixed with the sentence. - The illumination device has the characteristics of *, and the background is the following structure. One of the refracting surfaces is Μ & . Λ m ^ ι - & angle, the corner line is arranged on the reference surface, and the diagonal convex prism 6 on the arid surface of the roadway and the convex pyramidal refraction grating adjacent to the side of the rhombic refractive surface are arranged, and are arranged diagonally tb ^ m ^ ^ The side of the diamond-shaped refractive surface is adjacent to the concave surface of the reference surface concave J—using the cone-concave 夯—, the angle of incidence of the refractive surface and the difference between the angle of refraction and the angle, the normal of the reference plane The slanting and slanting side of the slanting side, wherein the angle is from the two refractive index sides, the parallel light of the light source of the three directions is emitted, and the incident light is incident only on the lead surface opposite to the light source and refracted to the reference surface. Above, and with the direction of exit 〇8, an illuminating device 'characterized by: · The exit surface of the light guide plate is formed." The patented r-structure consists of: refracting the light thumb, the triangle of the bottom surface of the light guide plate, , the side of the two light guide plates are inclined to the bottom of the parallel light incident The convex reflection triangular pyramid refraction grating irradiates parallel light to a pixel formed by a diamond-shaped convex reflection surface and is reflected to the sub-pixel, and a sub-pixel of three colors from three directions is formed. 44 201037230 9. Patent application scope The illuminating device of item 8, wherein the cylindrical convex reflecting surface on the bottom surface of the plate is formed by a number of columns smaller than the number of pixels, and the cylindrical convex reflecting surface is irradiated to the plurality of sub-pixel columns to enlarge the convex reflection. 10. The illuminating device of claim 8 wherein the illuminating device consists of: • a parallel structure formed on opposite sides of the side of the light guide plate, contacting the top edge of the circular reflecting surface and on the light guide plate The bottom surface is formed in a triangular column shape, and 0 is disposed between the two triangular columnar convex reflecting surfaces, and a plurality of convex reflecting surfaces are disposed in a direction orthogonal to the triangular columnar convex surface, and the two sides of the two sides disposed opposite to each other on the side surface of the light guide plate The light source is applied to the triangular prism-shaped convex reflecting surface, and the light is disposed in a direction orthogonal to the triangular columnar convex reflecting surface to a convex reflection in a direction orthogonal to the two-columnar convex reflecting surface Wherein the parallel light incident from a third direction to a triangular pyramid refractive surface refracting the incident thumb three sub-pixels. 〇11. The illuminating device of claim 8, wherein the longitudinal surface of the convex reflecting surface in the direction of the prismatic convex reflecting surface, • is orthogonal to the triangular prismatic reflecting surface by the irradiation ratio The length of the convex surface in the direction of the long axis is long, and the upper pixel of the triangular &amplified convex surface is irradiated. 1 2. For example, the lighting installation f of the patent application scope ,8 is composed of the following structure: the following convex reflection illumination of the surface of the two-cone refractive refracting grating formed by the diamond-shaped folding & A six-angle crystal panel composed of three diamond-shaped sub-pixels is arranged on the upper 45 201037230 side of the orthogonal curved reflection surface as follows, and the convex reflection light is refracted and irradiated to the mann shape by the diopter refractive grating a sub-pixel in which a light of three directions is mixed by a pixel of a hexagonal shape and is illuminated as in the third aspect of the patent application. The horizontal plane is the father of the parallel light from the light source, and the rectangular convex reflecting surface is arranged. The display surface of the backlight in the long-axis direction will be provided with a red light-emitting element at the focus of one of the parabolic mirrors or the parabolic mirror, and the elevation angle of the horizontal horizontal plane of the green light-emitting element is equal to the focus of the other parabolic curvature circular mirror. Symmetrical direction, red signal illuminates red illuminating element, and is displayed in reverse red, green illuminating element in green signal, and displayed in reverse green, by yellow When the signal is illuminated, the red light-emitting element is illuminated and the parallel light is incident on the reflective grating by both parties and mixed, and the color is recognized as 0. 1 4. The reference surface of the illumination device according to the sixth application of the patent scope is arranged by the refractive index larger than the surrounding medium. The second equilateral triangular columnar body is a display of the symbol light of the following components: the angle of the difference between the incident angle and the refraction angle, and the angle between the plurality of sloped surfaces and the normal of the reference plane The three directions of the liquid level reflection are displayed in color. In the direction, and in the direction of the illuminating light, the rounded mirror or the parabolic short-range light source is disposed on the grating to reflect the reflection of the grating, and the green light-emitting element is regarded as orange-yellow In the plural, the complex matter composed of a planar material is formed in a triangular wave shape by an equilateral triangular columnar body toward the refractive surface, and the refractive index of the refractive surface which is emitted from the high refractive index side to the low refractive index side is formed by one of the Parabolic mirror or parabolic approximation (4) Focus of the circular mirror - the color light-emitting element, and a parallel light source with a green light-emitting element disposed at a focal point of another parabolic mirror or a parabolic surface, the radiation source is disposed at the front of the refractive grating Concave refracting surface, symmetrical to the lower side of the reference plane toward the plane, the parallel light source, the focal point 0 color illuminating element and the green illuminating element, red signal for the pair of light source portions incident on the refracting grating Lights up the red illuminating element and displays it in the refracted color of the refracting grating, illuminates the green illuminating element with the green signal and refracts the grating Refraction - Color display, . Lights up the red illuminating element and green illuminates by the yellow 彳 §. Parallel light is incident on the refracting grating and mixed by both sides, and is used as an identification. The illuminating device of claim 3, wherein the grating grating and the plurality of illuminating elements having different excitation wavelengths complement the wave height of the illuminating side of the excitation side by the wave height value of the illuminating element having a long excitation wavelength The intermediate value of the value and the wavelength of the fluorescent light, by adding the wave height value of the plurality of fluorescent domains with the reflection grating, and the wave height of the excitation light and the wave height of the added fluorescent domain are equalized, as in the patent application scope. The illumination device of item 6, wherein the grating is combined with a plurality of light-emitting elements having different excitation wavelengths and gratings; a red-rate circular mirror is arranged; in order to arrange red with red for green components, yellow for anti-mixing, The wavelength is short and roughly average. Using a blend color, 47 201037230 The height of the light-emitting element on the side of the light-emitting element that excites the wavelength of the light-emitting element with a long wavelength is intermediate with the wavelength of the fluorescent light. • By adding the wave height of the plurality of fluorescent domains to the refractive grating. The wave height value of the mixed excitation light and the added fluorescence field are 17. The illumination device of the third aspect of the patent application scope, the rectangular plane is arranged in a triangular wave structure on the horizontal plane of the substrate. The square plane reflection surface forms a reflection grating. A flat 0 is arranged in a symmetrical direction equal to the elevation angle of the horizontal plane. The plurality of reflective grating units are arranged in the horizontal direction on the heat dissipation substrate, and a part of the reflection grating is formed into a shape that is bent into a cutoff line. The reflection grating array is arranged in a plurality of vertical vehicle headlights, and a plurality of reflection grating rows are illuminated to illuminate the traveling beam to align the horizontal reflection grating arrays in a part of the longitudinal light beam. Ο 18. In the illuminating device of claim 7, the concave surface of the tangential line in the grating valley portion constitutes a triangular pyramidal folding surface, and the radiation angle of the emitted light of the refractive grating is enlarged. 1. The illumination device of claim 3, wherein the long side of the convex reflecting surface contacts the horizontal plane, and the orthogonal direction of the traveling direction of the parallel light of the long axis direction is 'the curved surface length d of the curvature half circumference The convex reflecting surface reflects the short-field of the excitation wavelength from both directions, and the value is roughly the average value of the wave. Wherein the heat-dissipating reflecting surface or the long-line light source is formed by tilting the constituent unit, and by illuminating the column, the illuminating grating is irradiated with the oblique direction of the refracting grating, so that the rectangular distance is placed from the optical path r, along Parallel light, 48 201037230 Mix and shoot in the same direction with a radiation angle of 0 = d. 360 ° / (27 rr). 4949
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TWI449864B (en) * 2010-12-06 2014-08-21 Hitachi Appliances Inc Light bulb
TWI556024B (en) * 2011-06-07 2016-11-01 住友化學股份有限公司 Light guide plate, surface light source device, transmission-type image display device
CN107783211A (en) * 2016-08-30 2018-03-09 环视先进数字显示无锡有限公司 Micron LED display module mixed light gratings manufacture method, grating and display module

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JP4507062B2 (en) 2003-11-20 2010-07-21 オムロン株式会社 Surface light source device and equipment using the device
JP4678364B2 (en) 2006-12-05 2011-04-27 スタンレー電気株式会社 Light source device and vehicle headlamp
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JP4114173B1 (en) 2007-05-15 2008-07-09 鈴木 優一 Display device and lighting device

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TWI449864B (en) * 2010-12-06 2014-08-21 Hitachi Appliances Inc Light bulb
TWI556024B (en) * 2011-06-07 2016-11-01 住友化學股份有限公司 Light guide plate, surface light source device, transmission-type image display device
CN107783211A (en) * 2016-08-30 2018-03-09 环视先进数字显示无锡有限公司 Micron LED display module mixed light gratings manufacture method, grating and display module

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