TWI323818B - Liquid crystal display lighting apparatus - Google Patents

Liquid crystal display lighting apparatus Download PDF

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Publication number
TWI323818B
TWI323818B TW98133842A TW98133842A TWI323818B TW I323818 B TWI323818 B TW I323818B TW 98133842 A TW98133842 A TW 98133842A TW 98133842 A TW98133842 A TW 98133842A TW I323818 B TWI323818 B TW I323818B
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Taiwan
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light
liquid crystal
convex
guide plate
light guide
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TW98133842A
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Chinese (zh)
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TW201113604A (en
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Yuuichi Suzuki
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Yuuichi Suzuki
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Publication of TW201113604A publication Critical patent/TW201113604A/en

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1323818 .【發明所屬之技術領域】 本發明疋關於液晶顯示裝置(liquid crystal display apparatus)及照明裝置(lighting apparatus)。 瓤 【先前技術】 « 液晶顯示裝置的側光型(side light type)背光(back 11 ght)是在導光板的側面設置光源,並以配置多數個於導 光板的反射面側之微小反射材使其反射到液晶側的方式。 籲由於光源為擴散光’故越接近光源,越需要減少放射至液 晶側的機率’如圖3 9所示,在光源的附近白色塗料點的直 徑、密度變小’越遠離光源越大而被設置(專利文獻i)。 但是’由於以光源附近的小的點反射的光其光束密度高, 故容易成為亮點,需併用擴散片。 因不以漫反射(dif f used ref 1 ec t i on )點反射地通過導 光板背後的光越接近光源越多,效率降低顯著,故需再利 用用的反射板。 鲁以漫反射點反射的光在導光板射出面將臨界角以内的 光放射至液晶側’臨界角以上則在反射面側多重反射。被 照射到液晶的臨界角以内的光不是垂直方向,而是成為來 • 自光源側之斜向的光。因斜向的光會使亮度降低,故常採 用在導光板與液晶板之間配設稜鏡片,並轉換成垂直方向 之方法(專利文獻2 )。 由於漫反射方式會伴隨著多重反射,因此也有重複試作 評價使亮度均勻化’開發為沒有效率之問題。為了避免此 4 1323818 .問題’許多使其接近平行光線的提案已出現。 i 在交互連續地配置對入射平行光約45。的金屬蒸鐘反 - 射面與水平面之導光板的背後配設反射板之導光板被提出 •(圖40,專利文獻3)。因光源為擴散光,與距光源的距離 的2次方成反比’光束密度降低’故亮度不均(brightness unevenness)變大,在光源附近仰角成分多,故需再利用透 過水平面的光之反射板。 因上述提案在接近光源的部分仰角光線多,故透過依 籲照距光源的距離,使長邊面在b10。的範圍傾斜,短邊面 在30〜50。的範圍以入射面為基準逐漸增加,改善亮度不 均之導光板被k出’(圖4 1,專利文獻4 )惟距光源的距離 與傾斜之函數未被顯示。 形成越遠離光源反射面積越大的四角錐於底面,配設 以四角錐的反射面當作焦點之透鏡(lens)於導光板射出 面,射出平行光線至液晶側的方式被提出(專利文獻5 )。 因四角錐凹陷,故平行光無法入射,因底面的反射面其面 籲積遠比四角錐還寬’故底面中的反射光照射遠方的透鏡面 並多重反射’以致於效率降低,由於多重反射,故光線追 蹤很困難。 . 在導光板配設多數個環帶狀的微小拋物面反射鏡,剖 面呈鋸齒狀而組合的拋物面菲涅爾反射鏡(Fresnel reflection mirror)被提出(專利文獻 6)。因距點光源的 放射角度之内’可平行光化的光線被局限於拋物面鏡方 向,故併用反射鏡。若來自併用的反射鏡的光線在拋物面 5 1323818 •鏡反射,則有在與平行光錯開的方向反射之問題。在專利 文獻6也提出’以鋸齒狀菲涅爾面反射來自設置於拋物面 鏡的焦線之線狀光源的光之方式,惟因此方式是由拋物面 .鏡反射的平行光與來自光源的直接光混合,拋物面鏡的光 束密度依存性非常大,故亮度的均勻化很困難。 配5又依照距光源的距離使透射率(transmissi〇n factor)直線地降低之傾斜45。的反射面之多重光束分束 器(multiple beam splitter)方式被提出(專利文獻了)。 籲因光源為擴散光’故擴散光透過光源附近的光束分束器 (beam splitter*),且到達遠方的光束分束器者僅為平行光 成分’故即使光束分束器的透射率設定為直線的也會變成 不均勻。顯示有10等份的例子’在寬度3〇〇mni的晝面尺寸 中厚度變成30mm’會影響重量與材料費。為了減少厚度, 更增加分割數在膜厚控制上彳艮困難,藏錄(sputtering)為 多製程,製造成本變高。 在可攜式機器(portable machine)中於配置同心圓狀 •的微小反射材之導光板使用利用白色發光二極體的點光 源’惟因亮點比線光源的情形更顯著,故擴散片被併用β 如圖43所示’因光源的指向性(directivity)範圍外變 • 暗,故增加光源數進行緩和(專利文獻8 )。 正下方照明型(direct light type)之最正統的 (orthodox)的形狀為在箱型的平面反射鏡排列冷陰極管 (Cold Cathode Fluorescent Lamp:CCFL)。因若採用薄型, 則容易出現管照,故藉由離開光源,併用反射鏡形狀與擴 1323818 .散片等可謀求均勻化(專利文獻9)。雖然使用餘弦函數反 射鏡的方式是顯示光束密度均勻的結果(專利文獻1〇)。因 距光源的距離與冷陰極管間距(pitch)的函數’故很難滿足 薄型化與光源數的削減之兩方。 反射鏡的形狀被提出許多的方式,雖然光線轨跡被顯 示’但因多數未被定量地處理,故均勻性不明確。越增加 擴散片的厚度,越能使亮度均勻化,但因吸收而使效率降 低。 φ 許多液晶的彩色顯示是將像素(p i X e 1 ) 3分割’透過利 用紅、綠、藍的顏料被分散之彩色濾光片(color f i Iter) 之加法混色法顯示。彩色濾光片是採用藉由著色材料吸收 不需要的波長成分之方式。染料由於是可溶性,故有分散 佳’透射區域的透射率高之優點,惟在彩色濾光片基板 (substrate)的製程中’透明電極、配向膜(aHgnment fHm) 製程變成高溫’因染料在耐熱性、耐光性上不佳,故顏料 法成為主流。1323818. Field of the Invention The present invention relates to a liquid crystal display apparatus and a lighting apparatus.先前[Prior Art] « The side light type backlight of the liquid crystal display device is provided with a light source on the side surface of the light guide plate, and a small reflective material disposed on the side of the reflection surface of the light guide plate The way it is reflected to the liquid crystal side. Because the light source is diffused light, the closer to the light source, the more it is necessary to reduce the probability of radiation to the liquid crystal side. As shown in Fig. 39, the diameter and density of the white paint spot in the vicinity of the light source become smaller. Setting (Patent Document i). However, since light reflected by a small point near the light source has a high beam density, it tends to be a bright spot, and a diffusion sheet is used in combination. Since the light passing through the back of the light guide plate is not reflected by the diffuse reflection (dif f used ref 1 ec t i on ), the closer the light source is to the light source, the more the efficiency is lowered, so that the reflector used is required. The light reflected by the diffuse reflection point radiates light within the critical angle to the liquid crystal side at the exit surface of the light guide plate, and is multi-reflected on the side of the reflection surface. The light that is irradiated to the critical angle of the liquid crystal is not the vertical direction but is the light that is oblique from the light source side. Since the oblique light causes a decrease in luminance, a method of disposing a cymbal between the light guide plate and the liquid crystal panel and converting it into a vertical direction is often employed (Patent Document 2). Since the diffuse reflection method is accompanied by multiple reflections, there are also repeated trial evaluations to equalize the brightness' development as a problem of inefficiency. In order to avoid this 4 1323818. The problem 'many proposals that make it close to parallel rays have emerged. i is continuously configured to interact with parallel light about 45. The metal vapor clock is reversed - a light guide plate with a reflecting plate disposed behind the light guide plate of the surface and the horizontal surface is proposed (Fig. 40, Patent Document 3). Since the light source is diffused light, and the distance from the light source is inversely proportional to the square of the 'light beam density', the brightness unevenness becomes large, and there are many elevation angle components near the light source. Therefore, it is necessary to reuse the light reflection through the horizontal plane. board. Since the above proposal has a large amount of elevation light in a portion close to the light source, the long side surface is at b10 by urging the distance from the light source. The range is slanted, and the short side is 30 to 50. The range is gradually increased on the basis of the incident surface, and the light guide plate which improves the unevenness of brightness is turned out (Fig. 4, Patent Document 4). The distance and the function of the inclination from the light source are not displayed. A quadrangular pyramid having a larger reflection area from the light source is formed on the bottom surface, and a lens having a reflection surface of a quadrangular pyramid as a focus is disposed on the light-emitting plate exit surface, and a parallel light is emitted to the liquid crystal side (Patent Document 5) ). Because the quadrangular pyramid is recessed, the parallel light cannot be incident, because the reflective surface of the bottom surface is far wider than the quadrangular pyramid. Therefore, the reflected light in the bottom surface illuminates the far lens surface and multiple reflections, so that the efficiency is reduced due to multiple reflections. Therefore, ray tracing is difficult. A parabolic Fresnel reflection mirror in which a plurality of endless belt-shaped micro-parabolic mirrors are arranged in a zigzag shape is proposed (Patent Document 6). The light that can be collimated in the plane of the radiation from the point source is limited to the direction of the parabolic mirror, so a mirror is used in combination. If the light from the combined mirror is on the paraboloid 5 1323818 • Mirror reflection, there is a problem of reflection in the direction of staggered parallel light. Patent Document 6 also proposes a method of reflecting light from a linear light source provided on a focal line of a parabolic mirror by a serrated Fresnel surface, but in this manner, parallel light reflected by a parabolic mirror and direct light from a light source Hybrid, the parabolic mirror has a very large beam density dependence, so uniformizing the brightness is difficult. The distribution 5 further reduces the transmittance (transmissi〇n factor) by a slope 45 in accordance with the distance from the light source. A multiple beam splitter method of the reflecting surface has been proposed (patent literature). Because the light source is diffused light', the diffused light passes through the beam splitter* near the light source, and the beam splitter that reaches the far side is only a parallel light component', even if the transmittance of the beam splitter is set to Straight lines will also become uneven. The example showing 10 aliquots 'the thickness becomes 30 mm in the kneading dimension of the width of 3 〇〇 mni' affects the weight and material cost. In order to reduce the thickness, it is difficult to increase the number of divisions in film thickness control, and the sputtering is a multi-process, and the manufacturing cost becomes high. In a portable machine, a light source using a white light-emitting diode is used for a light guide plate that is arranged in a concentric circular shape. However, since the bright spot is more prominent than the line light source, the diffusion sheet is used in combination. As shown in Fig. 43, 'Because the directivity range of the light source is changed from the outside to the dark, the number of light sources is increased to ease (Patent Document 8). The most orthodox shape of the direct light type is a box-type flat mirror array of cold cathode tubes (CCFLs). In the case of a thin type, it is easy to cause a tube, and it is possible to achieve uniformity by leaving the light source and using a mirror shape and expanding the sheet (Patent Document 9). Although the method of using the cosine function mirror is to show a uniform beam density (Patent Document 1). Due to the distance from the light source and the function of the pitch of the cold cathode tube, it is difficult to satisfy both the reduction in thickness and the reduction in the number of light sources. The shape of the mirror is proposed in a number of ways, although the ray trajectory is shown 'but the majority is not quantified, so the uniformity is not clear. The more the thickness of the diffusion sheet is increased, the more uniform the brightness is, but the efficiency is lowered by absorption. φ The color display of many liquid crystals is an additive color mixing method in which a pixel (p i X e 1 ) 3 is divided into 'color f i Iter' which is dispersed by a pigment of red, green and blue. The color filter is a method of absorbing an unnecessary wavelength component by a coloring material. Since the dye is soluble, it has the advantage of high dispersion in the transmission region, but in the process of the color filter substrate, the 'transparent electrode and the alignment film (aHgnment fHm) process become high temperature. The color and light resistance are not good, so the pigment method has become the mainstream.

使用顏料之著色是白色光照射顏料粒子’依照其反射 光的分光特性而進行。若白色光不射中粒子而貫通,則會 淡色化,若顏料含有率過高,則透射區域的透射率降低而 變暗。為了提高透射率,偻隐姐^ L & 使&絕特性陡峭’需要微粒化、 顏料分散比率與膜厚控制。 藉由彩色遽光片使不需要 收’因即使是透射區域也 transmittance)為 30%以下。 的頻帶(band)之2/3被吸 有吸枚,故透光率(1 ight 3波長冷陰極管的發光光譜 1323818 .(spectrum)也包含許多3波長以外的光譜,若想充分地隔 絕此等光譜’則透射區域的透射率也降低,透光率更下降。 彩色慮光片的透射率為在液晶裝置之中最低,其次由於偏 光板的約45%等,故液晶顯示裝置全體的透射率為8%以下。 • 液晶基板中的彩色濾光片製造法雖然印刷法能以少的 製程製造’但因高解析度化(high res〇iution)困難,故照 相钮刻法(photo etching method)常被採用。但是,因照 相#刻法針對黑色矩陣(b 1 a c k m a t r i X)、紅、綠、藍的4 鲁層進行洗淨(cleaning)、光阻塗佈(resist coating)、曝 光(exposure)、顯影(development)、硬化(curing)的製 程’製私長’需昂貴的裝置’故佔液晶面板(liquidcryStal pane 1 )的價格之比例最昂貴。 因冷陰極放電管其發光效率高等的優點,故常被採用 於背光’惟發光光譜依照螢光材料的波長轉換特性,也包 含許多3原色以外的光譜,在透射率為標準的彩色濾光片 中 N T S C (N a t i ο n a 1 T e 1 e v i s i ο n S y s t e m C 〇 m m i 11 e e :美國國 鲁家電視系統委員會)比約70%。因在電視中色再現性(c〇1〇r reproduction characteristics)的要求強烈,故藉由提高 彩色濾光片的濃度提高NTSC比,惟如此會使透射率降低且 使功率消耗增大。 因冷陰極管需要換流器而有小型化等的問題,故在可 » 攜式用途等中為白色發光二極體被使用。 白色發光二極體為將由藍色發光二極體產生的藍色光 照射到其補色之黃色螢光體,藉由藍與黃色加法混色轉換 8 1323818 成白色光的方式常被使用於白色照明用途等。因液晶顯示 的情形在2色昆色法中紅等的再現性差,故將藍色光照射 到黃色、紅或綠、紅的螢光材之加法混色方式被採用。但 .是,為了以螢光材料比對藍色光進行波長轉換,配合比不 .規則(deviation)使不平衡(unbalance)増大為2倍,即使 經過經時變化也會產生不平衡,故需使發光元件與螢光材 料的經時變化同等。 雖然也有將3色的晶片(chip)放在同一封裝(package) 鲁之加法混色方式,但來自小的封裝的焦點之偏移大,會因 3個晶片的指向性而產生不平衡。 在重視色再現性的用途上,雖然藉由分色棱鏡 (dichroic prism)將紅、綠、藍的發光二極體的光混色之 方法被採用(專利文獻11 ),惟藉由3個獨立的光學系統會 使尺寸變大而昂貴。 液晶投影機也藉由分色稜鏡混色,因照射面積寬敞, 故使用金属_化燈等的高發光強度(lumin〇us intensity) 鲁的白色光源’以分色鏡(dichroicmirror)進行彩色分解的 方法常被採用。 彩色濾光片價格所佔的比例高,光利用效率降低至 .30%以下專的問題’削減區段電極(segment eiectrode)數 成1/3,使TFT基板的製造變的容易之時分割方式被提出。 時分割方式是將畫面的顯示週期16 6mS三分割成 红、綠、藍’每5. 6mS切換而進行視覺上殘留影像混色之 方式。液晶正確地表現色調(t〇ne)、顏色是扣除液晶響應 1323818 的上升期間、下降期間之平坦期間,若平坦期間所佔的比 例低,則亮度與對比均下降。 若以時分割方式播放動畫,則會發生紅、綠、藍的3 .個畫像在觀察者的網膜上偏移而被合成的色分離(color break-up)妨礙。防止此現象的方法是在第4週期插入白、 黑或中間色之方法等被提出(專利文獻i 2、1 3 ),惟在4分 割法中需響應速度為2mS以下。因向列型液晶(nematic liquid crystal)的響應速度為50mS〜lOOmS,故被限制於 籲彎曲配向、鐵電液晶(ferroelectric Hquid cryStal)、 反鐵電液晶(antiferroelectric liquid crystal)等高速 的液晶材料。鐵電液晶為高速響應,另一方面因人字形 (chevron)構造造成的鑛齒形缺陷(zigZag defect)而容易 發生漏光(1 ight leak),使配向控制變的困難。有因碰撞 使層構造容易被破壞’不自我修復等的難點。 藉由於複數個棒狀導光體的界面配設遮光層,在各導 光棒的端面配設彩色濾光片並對向配置白色光源,或對向 鲁配置複數個彩色發光二極體’遮蔽顏色區別的光並傳導於 棒狀導光體内’藉由供給至液晶條紋,液晶面板本身不使 用彩色濾光片的方法被提出(圖45,專利文獻1 5 )。因顯 •不畫面為次像素需無法被明確地目視的尺寸,故通常的條 紋寬度為10〇ym等級(order)’不是棒狀而是在線狀的導 光體覆蓋遮光體後積層線狀體。因擴散光傳導於以各遮光 層隔開的透光材内’故金屬遮光膜的情形為每次反射就被 吸收而越遠越暗。以折射率比透光材低的材料覆蓋的情形 1323818 因臨界角以内的擴散光透過,故會混色。在積層透光片的 製造法中若透光片厚度的公差累計,則不會與液晶的像素 尺寸一致。 • 因背投影機(rear pro jector)若由後方直接投射至榮 、幕’則後方的尺寸變長,故經由反射鏡返回,藉由使投射 透鏡廣角化’可使縱深被縮短化(圖44,專利文獻i 4)。 在橫1 00 0mm、縱56 0mm的螢幕中以反射鏡j片、畫面視角 (angle of view) 60°的廣角透鏡需要約5〇〇mm的縱深。因 _低像差(aberration)廣角透鏡其透鏡片數增加,變成高 價,故有藉由採用反射鏡為凸面鏡縮短縱深之提案等。但 即使採取這種對策,也因縱深約4〇〇mm,故縱深成為利用 上的限制。 〔專利文獻1〕曰本國特開平6- 31 3883號公報 〔專利文獻2〕曰本國特開平5 — i 2 7 1 5 9號公報 〔專利文獻3〕曰本國特開平7— 2〇462號公報 〔專利文獻4〕日本國特開平1〇_ 1〇462 1號公報 籲〔專利文獻5〕日本國特開2〇〇5- Ή928號公報 〔專利文獻6〕日本國特開2〇〇4_ 185〇2〇號公報 〔專利文獻7〕日本國特開2〇〇6_丨1 445號公報 〔專利文獻8〕日本國特開2005- 353506號公報 〔專利文獻9〕日本國特開2〇〇卜1 388〇號公報 〔專利文獻1 〇〕日本國特開2〇〇卜i 74丨2號公報 〔專利文獻11〕日本國特開2〇〇5_ 183〇〇5號公報 〔專利文獻12〕日本國特開2〇〇2_ 1 91 〇55號公報 1323818 〔專利文獻1 3〕日本國特開2 Ο (Π - 2 81 6 2 3號公報 〔專利文獻14〕曰本國特開平6- 1 1 767號公報 〔專利文獻15〕日本國特開平2- 1 1 1 922號公報 【發明内容】 因依照光源至白色塗料點的距離改變白色塗料點的密 度之漫反射方式係接近光源的部分為白色塗料密度低,故 容易成為亮點,產生併用擴散片之需要,會影響光效率、 |價格、厚度。 因接近光源的部分為白色塗料密度低,故需要防止透 射至導光板背後的光的損失之反射板。 因導光板内的漫反射為斜的光,使對比降低,故產生 以棱鏡片將機率中心轉換成垂直方向之需要。 為了進行多重反射而重複試作評價,使亮度被均勻化,開 發為沒有效率。 由於彩色濾光片為吸收不需要的波長,得到3原色之 鲁方式,故透光率為約 30%以下,在液晶裝置之中透射率最 低,液晶裝置全體的透射率變成8%以下。 彩色濾光片中的著色是依照以顏料粒子進行反射,因 成為散射光,故發生由於在垂直配向、彎曲配向中以黑顯 示模式使斜的光照射液晶分子造成漏光,使對比降低。 彩色濾光片是藉由照相蝕刻法等依次印上黑色矩陣、紅、 綠、藍,故製程多,佔液晶顯示裝置的製造成本之比例最 昂貴。 1323818 3波長白色光冷陰極管的發光光譜為波長與3 一致,也包含許多3波長以外的光譜。冷陰極管方 換流器’會影響尺寸、價格、效率。 . 將藍色發光二極體的光照射到紅、綠螢光體之 白色發光二極體係色平衡(color balance)顯著地 材料的配合比影響。 將紅、綠、藍發光二極體放在同一封裝,混合 之簡易的混色方法會依照觀看的方向而使色平衡崩 _使用分色稜鏡取得各元件的平衡之方法為光學系統 雜且昂貴。 交互地使紅、綠、藍的發光二極體點亮之時分 是由將場週期(field period) 16. 6mS三分割後之5 除顯示時間約3mS,變成約2. 6mS以下。 在3分割方式中有發生高速的動晝被錯開成紅 藍而顯示的色分離之問題,雖然4分割方式等被提 在4分割方式中需要約2mS以下的高速響應的液晶 •藉由在複數個棒狀導光體的界面配設遮光層, 色區別的光並傳導於棒狀導光體内,供給至液晶條 晶面板本身不使用彩色濾光片的方法因擴散光傳導 - 遮光層隔開的透光材内,故金屬遮光膜的情形為每 就被吸收而越遠越暗。以折射率比透光材低的材料 十月形因臨界角以内的擴散光透過,故會混色。在積 片的製造法中若透光片厚度的公差累計,則不會與 像素尺寸一致。 原色不 式需要 混色法 被螢光 3色光 潰。 變的複 割方式 6mS扣 、綠、 出,但 〇 遮蔽顏 紋,液 於以各 次反射 覆蓋的 層透光 液晶的 因背投影機若由後方直接投射至螢幕,則後方的尺寸 ^ ^ j ’故經由反射鏡,使用廣角透鏡使縱深被縮短化。在 縱560mm的螢幕中以畫面視角60度的廣角透 , 一 兄 縱深變成約500mm。縱深成為利用上的限制。 爲了防止與其他顏色的光源光混色,藉由平行光轉換 手段將來自光源的光形成平行光,該平行光入射到以像素 間距分散配置有凸反射面5成梯田狀的導光板内。 由側面看入射來自光源的光之梯田狀導光板1之構造 是如圖1,在對向於液晶側的反射面側配置凸反射面5之 梯田狀構造。該凸反射面5是朝位於略垂直方向的液晶的 像素反射來自光源的平行光線,因凸反射面比像素尺寸 小’故為用以擴大成像素尺寸的凸反射面。雖然在光傳導 的導光板内是凸面,但是從導光板外面看則成凹面° s玄凸 反射面5如圖2,若傾斜至臨界角以上,則玎進行全反射。 採用鏡面反射層進行反射也可以,雖然沒有了臨界角的限 制,但因需要蒸鍍製程等,故價格會上昇。 在凸反射面5的光源側中,在與水平面所成的傾斜角 0 d、入射角61 1之間下式的關係成立: [公式1 ] 0d=9〇° -θι 由全反射條件θ 1 > Θ c ’有下式的必要: [公式2 ] 0d <9〇。 因光源不為完全的點光源,具有平行性公差’故0 d f取公差的裕度(allowance)。 顯示平;^止, 中的-欠僮去 反射面擴大光束並擴大到被照射面 •的距^ ^透射部的寬度W的樣子於圖3。到被照射體 二欠像素的^導光板厚度與液晶透明基板厚度的和,若設 圓周之官择* 者導先板凸面傾斜部的 [公式3「為d,則凸反射面的曲率半徑r是以下式表示: r、2 . t . d / (w- d /,2) •是梯田狀構造的導光板,故可藉由依照由位置造成的 心的變化而改變曲率半徑Γ,均勻地照射到像素透射 藉由平行光轉換手段將來自光源的光形成平行光並入 射到導光元件,使傳導於導光板内的平行光以臨界角以上 的入射角入射到設於導光板的底面的反射面並進行全反 射,或者藉由以前述反射面當作鏡面進行反射,依照被照 射尺寸、到被照射體的距離設定反射面的曲率,擴大光束 •並反射於目的方向。如圖4,藉由使用三色的光源斑二層 梯田狀導光板,以次像素寬度的條紋間距錯開照射於同一 像素的三層梯田狀段差部,可不被其他顏色的光源光用的 傾斜反射面阻礙且不配設彩色濾光片於液晶面板而進行彩 色顯示。爲了在導光板内部形成凸反射面而以三層構成, 惟若可藉由擠壓成型(extrusion molding)等在内部形成 凸反射面’則以單一的導光板也能實現同一功能。 凸反射面若直線狀地排列圓筒面,則能在液晶面中以 直線的Yl基# S _ 也处” 員示’但藉由將凸反射面折彎配置成鋸齒狀 月匕實現鋸齒狀條紋。 4 導光板的各凸反射面的曲率半徑是藉由公式3並依照 久 f象春 /4r 曰” ”紋寬度與到液晶面的距離以三層設定,惟因到液 的距離在三層不同,故曲率半徑每—層不同。 ;"'藉由使用二色的點光源與三層梯田狀導光板,以 次像音宮#The coloring of the pigment is carried out by the white light-irradiating pigment particles 'in accordance with the spectral characteristics of the reflected light. When the white light penetrates without passing through the particles, the color is lightened, and if the pigment content is too high, the transmittance of the transmission region is lowered to become dark. In order to increase the transmittance, 偻 姐 ^ ^ L && absolute characteristics steepness 'requires micronization, pigment dispersion ratio and film thickness control. By using a color calender sheet, it is not necessary to receive a light transmittance of 30% or less. 2/3 of the band is absorbed, so the light transmittance (1 ight 3 wavelength cold cathode tube luminescence spectrum 1323818. (spectrum) also contains many spectra outside the 3 wavelengths, if you want to fully isolate this In the equal spectrum, the transmittance of the transmissive region is also lowered, and the transmittance is further decreased. The transmittance of the color filter is the lowest among the liquid crystal devices, and secondly, the transmittance of the entire liquid crystal display device is about 45% of the polarizing plate. The rate is 8% or less. • The color filter manufacturing method in the liquid crystal substrate can be manufactured with a small number of processes, but the high res〇iution is difficult, so the photo etching method It is often used. However, cleaning, photoresist coating, exposure (exposure) for the black matrix (b 1 ackmatri X), red, green, and blue 4 layers ), development, curing process, 'private length' requires expensive equipment', so the proportion of the price of liquid crystal panel (liquidcryStal pane 1) is the most expensive. Because of the high luminous efficiency of cold cathode discharge tube, etc. , Often used in backlights, but the luminescence spectrum according to the wavelength conversion characteristics of the fluorescent material, also contains many spectra other than the three primary colors, in the standard color filter of NTSC (N ati ο na 1 T e 1 evisi ο n S ystem C 〇mmi 11 ee: About 70% of the US National Lu Television Systems Committee. Because of the strong demand for color reproduction (d〇1〇r reproduction characteristics) on television, by increasing the color filter The concentration increases the NTSC ratio, but this reduces the transmittance and increases the power consumption. Since the cold cathode tube requires an inverter and has a problem of miniaturization, it is a white light-emitting diode in a portable type or the like. The white light-emitting diode is a yellow phosphor that illuminates the blue light generated by the blue light-emitting diode to its complementary color, and is converted into white light by blue and yellow additive color mixing. White lighting use, etc. In the case of liquid crystal display, the reproducibility of red or the like is poor in the two-color method, so the additive color mixing method in which blue light is irradiated to yellow, red, green, or red fluorescent materials is However, in order to perform wavelength conversion on the blue light by the fluorescent material, the unbalance is twice as large as the ratio, and even if it changes over time, an imbalance occurs. It is necessary to make the light-emitting element and the fluorescent material change with time. Although there are also three-color chips in the same package, the focus of the small package is large. An imbalance occurs due to the directivity of the three wafers. In the application of color reproducibility, a method of mixing colors of red, green, and blue light-emitting diodes by a dichroic prism is adopted (Patent Document 11), but by three independent Optical systems can make the size larger and more expensive. The liquid crystal projector also uses color separation and color mixing, and because of the large irradiation area, it uses a high-intensity luminescence intensity such as a metal lamp, and a white light source of the color is decomposed by a dichroic mirror. Methods are often used. The ratio of the price of the color filter is high, and the light use efficiency is reduced to less than .30%. The number of segment eiectrode is reduced to 1/3, making it easier to manufacture the TFT substrate. Been proposed. The time division method is a method in which the display period of the screen is divided into 16 6 mS into red, green, and blue, and the visual residual image is mixed every 5.6 mS. The liquid crystal accurately expresses the color tone (t〇ne), and the color is a flat period in which the rising period and the falling period of the liquid crystal response 1323818 are deducted, and if the ratio of the flat period is low, both the brightness and the contrast are lowered. When the animation is played back in a time division manner, three images of red, green, and blue are scattered on the viewer's web and interfered by the resultant color break-up. A method of preventing this phenomenon is to insert a white, black or intermediate color in the fourth cycle (Patent Documents i 2, 1 3), but the response speed is required to be 2 mS or less in the 4-minute cutting method. Since the response speed of nematic liquid crystal is 50 mS to 100 mS, it is limited to high-speed liquid crystal materials such as bend alignment, ferroelectric Hquid cryStal, and antiferroelectric liquid crystal. The ferroelectric liquid crystal has a high-speed response, and on the other hand, due to a zigZag defect caused by a chevron structure, light leakage (1 ight leak) is liable to occur, making alignment control difficult. There is a difficulty in destroying the layer structure due to collisions. By arranging a light-shielding layer at the interface of the plurality of rod-shaped light guides, a color filter is disposed on the end surface of each of the light guide bars, and a white light source is disposed, or a plurality of color light-emitting diodes are disposed in the opposite direction. The light of the color difference is transmitted to the rod-shaped light guide body' by the method of supplying the liquid crystal stripe, and the liquid crystal panel itself does not use the color filter (FIG. 45, Patent Document 15). Since the display screen is a sub-pixel that cannot be clearly viewed, the normal stripe width is 10 〇ym. The order is not a rod shape, but the linear light guide body covers the light-shielding body and the laminated linear body. . Since the diffused light is conducted in the light-transmitting material separated by the respective light-shielding layers, the metal light-shielding film is absorbed for each reflection and is darker and darker. When the material has a lower refractive index than the light-transmissive material, 1323818 is diffused by the diffused light within the critical angle, so it mixes colors. In the manufacturing method of the laminated light-transmissive sheet, if the tolerance of the thickness of the light-transmitting sheet is accumulated, it does not match the pixel size of the liquid crystal. • Since the rear projector (rear pro jector) is directly projected from the rear to the glory and the screen, the size of the rear is longer. Therefore, by returning through the mirror, the depth of the projection lens can be shortened (Fig. 44). , Patent Document i 4). A wide-angle lens with a mirror j-piece and an angle of view of 60° in a screen of 10,000 mm and 560 mm in length requires a depth of about 5 mm. Since the number of lenses of the _ low-abration wide-angle lens increases and becomes high, there is a proposal to shorten the depth by using a mirror as a convex mirror. However, even if this countermeasure is adopted, since the depth is about 4 mm, the depth becomes a limitation in use. [Patent Document 1] 曰 特 6 6 6 6 6 6 6 6 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰 曰[Patent Document 4] Japanese Patent Publication No. 1 〇 〇 〇 1 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利 专利Japanese Patent Laid-Open Publication No. Hei. No. Hei. No. 2005-353506 (Patent Document 9) Japanese Unexamined Patent Publication No. Hei No. Hei. No. s. Japanese Patent Publication No. 2_1 91 〇 55, Bulletin 1323818 [Patent Document 13] Japanese Patent Laid-Open No. 2 Ο (Π - 2 81 6 2 3 (Patent Document 14) 曰 National Special Kaiping 6- 1 1 Japanese Patent Application Laid-Open No. Hei No. Hei-2- 1 1 922 (Invention) Contents are changed according to the distance from the light source to the white paint point. The diffuse reflection mode of the density of the white paint spot is close to the light source. The white paint has a low density, so it is easy to become a bright spot. The need to use a diffuser together will affect the light efficiency, price, and thickness. The part close to the light source is white. Since the density of the paint is low, it is necessary to prevent the reflection of the light transmitted to the back of the light guide plate. Since the diffuse reflection in the light guide plate is oblique light, the contrast is lowered, so that the prism sheet is required to convert the probability center into the vertical direction. In order to perform multiple reflections and repeat the test evaluation, the brightness is uniformized and developed to be inefficient. Since the color filter absorbs unnecessary wavelengths, the three primary colors are obtained, so the light transmittance is about 30% or less. In the liquid crystal device, the transmittance is the lowest, and the transmittance of the entire liquid crystal device is 8% or less. The coloring in the color filter is reflected by the pigment particles, and the scattered light is generated in the vertical alignment and the curved alignment. In the black display mode, the oblique light illuminates the liquid crystal molecules to cause light leakage, which reduces the contrast. The color filter is photographicly etched. The method is printed with black matrix, red, green and blue in turn, so the number of processes is large, and the proportion of the manufacturing cost of the liquid crystal display device is the most expensive. 1323818 The wavelength spectrum of the three-wavelength white light-cooled cathode tube is the same as the wavelength, and also contains many Spectrals other than 3 wavelengths. Cold cathode tube converters will affect size, price, and efficiency. The color of the blue light emitting diode is illuminated by the white light emitting diode of the red and green phosphors. Balance) Significantly affects the mix ratio of materials. The red, green and blue light-emitting diodes are placed in the same package, and the simple color mixing method of mixing will make the color balance collapse according to the direction of viewing. The method of balancing is that the optical system is complicated and expensive. 5米以下以下。 The red, green, and blue light-emitting diodes are illuminate by the field period (field period) 16. 6mS three divided by 5, the display time is about 3mS, and becomes about 2. 6mS or less. In the three-division method, there is a problem that the high-speed motion is shifted into red and blue and the color separation is displayed. In the four-division method, a high-speed response liquid crystal of about 2 mS or less is required in the four-division method. The interface of the rod-shaped light guide body is provided with a light-shielding layer, and the light of the color difference is transmitted to the rod-shaped light guide body, and is supplied to the liquid crystal stripe panel itself without using a color filter due to diffusion light conduction - the light shielding layer is separated In the case of the light-transmitting material that is opened, the case of the metal light-shielding film is that the farther and darker it is absorbed. A material whose refractive index is lower than that of a light-transmitting material is transmitted by diffused light within a critical angle in the form of a moon, so that color is mixed. In the manufacturing method of the sheet, if the tolerance of the thickness of the light-transmissive sheet is accumulated, it does not match the pixel size. The primary color is not required. The color mixing method is broken by the fluorescent 3 color. Changed cutting mode 6mS buckle, green, out, but 〇 masking the lines, liquid in the layer of light-transparent liquid crystal covered by each reflection, if the rear projector directly projects to the screen from the rear, the size of the rear ^ ^ j 'Therefore, the depth is shortened by using a wide-angle lens through a mirror. In the vertical 560mm screen, the wide angle of 60 degrees of the screen is transparent, and the depth of one brother becomes about 500mm. Depth is a limitation in utilization. In order to prevent color mixing with the light source of the other colors, the light from the light source is formed into parallel light by the parallel light conversion means, and the parallel light is incident on the light guide plate in which the convex reflection surface 5 is dispersed and arranged in a terrace shape at a pixel pitch. The structure of the terrace-shaped light guide plate 1 that receives light from the light source as viewed from the side is a terrace-like structure in which the convex reflection surface 5 is disposed on the side of the reflection surface facing the liquid crystal side as shown in Fig. 1 . The convex reflecting surface 5 reflects parallel rays from the light source toward the pixels of the liquid crystal in the slightly perpendicular direction, and is a convex reflecting surface for expanding the pixel size because the convex reflecting surface is smaller than the pixel size. Although it is convex in the light-conducting light guide plate, it is concave as seen from the outside of the light guide plate. The sinusoidal reflection surface 5 is as shown in Fig. 2. If it is inclined to a critical angle or more, the 玎 is totally reflected. It is also possible to use a specular reflection layer for reflection. Although there is no limitation of the critical angle, the price is increased because a vapor deposition process is required. In the light source side of the convex reflecting surface 5, the relationship of the following equation is established between the inclination angle 0d and the incident angle 611 which are formed with the horizontal plane: [Formula 1] 0d=9〇° - θι From the total reflection condition θ 1 > Θ c ' has the following formula: [Formula 2] 0d <9〇. Since the light source is not a complete point source, it has a parallel tolerance, so 0 d f takes the tolerance of the tolerance. The display is flat; in the middle, the child is in the shadow. The reflecting surface enlarges the beam and expands to the surface of the illuminated surface. The width W of the transmitting portion is as shown in Fig. 3. The sum of the thickness of the light guide plate to the thickness of the liquid crystal transparent substrate of the two pixels of the irradiated body, and the radius of curvature of the convex reflecting surface of the convex portion of the convex portion of the circumferential guide It is expressed by the following formula: r, 2 . t . d / (w- d /, 2) • is a light guide plate of a terrace-like structure, so that the radius of curvature Γ can be changed uniformly according to the change of the heart caused by the position, uniformly Irradiation to the pixel transmission, the light from the light source is formed into parallel light by the parallel light conversion means and is incident on the light guiding element, so that the parallel light transmitted in the light guide plate is incident on the bottom surface of the light guide plate at an incident angle above a critical angle. The reflecting surface is totally reflected or reflected by the reflecting surface as a mirror surface, and the curvature of the reflecting surface is set according to the size of the irradiated object and the distance to the irradiated object, and the light beam is enlarged and reflected in the target direction. By using a three-color light source spot two-layer terrace-shaped light guide plate, the three-layer terrace-like step portion irradiated to the same pixel is shifted by the stripe pitch of the sub-pixel width, and can be prevented from being obstructed by the oblique reflection surface for the light source of the other color. Color display is not provided on the liquid crystal panel for color display. In order to form a convex reflection surface inside the light guide plate, it is composed of three layers, but if a convex reflection surface can be formed inside by extrusion molding or the like The same function can be achieved with a single light guide plate. If the convex reflecting surface is arranged linearly in a cylindrical shape, the Y1 base # S _ can be displayed in the liquid crystal surface as a straight line, but by the convex reflecting surface The bend is configured in a zigzag pattern to achieve a zigzag stripe. 4 The radius of curvature of each convex reflecting surface of the light guide plate is set by three layers according to the formula 3 and according to the distance between the width of the spring/4r 曰"" and the liquid crystal surface, but the distance to the liquid is different in three layers. Therefore, the radius of curvature is different for each layer. ;"' by using a two-color point source with three layers of terraced light guides

I見度的條紋間距錯開梯田狀段差部的狀態之斜視圖 於圖 C 」 。照射於同一像素的凸反射面的曲率半徑在三層導 '*不同為短暫地设定液晶面側的曲率半徑之狀態。光 原疋使用一色的發光二極體,配設於軸外拋物面鏡的焦 點。 都作 距、 故爲 軸外拋物面鏡可藉由將導光板的厚度方向、寬度方向 成拋^線而轉換成平行光。目寬度方向以寸藉由焦 光束密度分布、光源的發光強度、指向性等而被設定, 了加大寬度需使抛物面的縱深變長。 藉由以次像素寬度的條紋間距錯開照射於同一像素^ 三層的梯田狀段差部,配設正焦距折射面於各導光板的糸 出面並轉換成平行光’冑凸反射面的曲率半徑各層都庚 一’並:由堆疊三層同一形狀的導光板使平行光入射免 各色的次像素,可進杆必A gAn oblique view of the state in which the stripe pitch of the I-view is shifted from the terraced section is shown in Fig. C". The radius of curvature of the convex reflecting surface that is irradiated on the same pixel is different from the three-layered guide ** in a state in which the radius of curvature of the liquid crystal surface side is temporarily set. The light source uses a one-color LED that is placed at the focal point of the off-axis parabolic mirror. The off-axis parabolic mirror can be converted into parallel light by throwing the thickness direction and the width direction of the light guide plate. The width direction of the mesh is set by the focal beam density distribution, the luminous intensity of the light source, the directivity, etc., and the width is increased to make the depth of the paraboloid longer. By shifting the stripe pitch of the sub-pixel width to the terrace-like step portion of the same pixel, the positive focal length refracting surface is disposed on the exit surface of each light guide plate and converted into a plane of curvature of the parallel light '胄 convex reflecting surface. Du Gengyi' and: by stacking three layers of the same shape of the light guide plate, the parallel light is incident on the sub-pixels of various colors, and the rod can be inserted into the beam.

進仃如色顯不。若在各導光板的射出S 配設正…、距折射面並轉換成平行光,則可使平行光入射到 各色的次像素,如此凸反射面的曲率半徑各層都成同一。 因此’因堆疊三層-種類的形狀的導光板,故模具製造成 本便宜,由於是一種類,故製造性也變佳。 、象素見度的條紋間距錯開三色的光源與梯田狀段 16 1323818 差部的狀態 外拋物面鏡 離在各層不 . 折射面,使 圖6。 因拋物 利用,若光 蔽平行光, I 變成不均勻 (offset)的 鏡近似凹球 阻礙而能傳 藉由在 點配設發光 複數色的發 因拋物 φ 的2次方成 低。 設拋物線為 [公式4 ] . y 2= 4 p X 設拋物矣 [公式5 ] ’以及光源使用三色的發光二極體,配設於轴 的焦點這幾點與前述一樣,惟因到液晶面的距 同’故顯示在導光板的射出面側配設正焦距的 用三層同一構造的梯田狀導光板時的斜視圖於 面鏡可產生平行光’故將點光源配設於焦點而 源位於平行光的射出路徑之中,則光源不僅遮 也將直接光(direct ray)加諸於反射平行光, 。如圖1、圖4等藉由在由平行光的路徑偏移 位置具有焦點的轴外抛物凹面鏡或轴外抛物面 面鏡的焦點配設光源,可使平行光不會被光源 導於導光板。 導光板的厚度方向、寬度方向都在拋物面的焦 二極體,依照液晶條紋的排列順序交互地配置 光二極體’可供給複數色的平行光。 面鏡為光束密度和光源與反射面上的點之距離 反比,故反射光的光束分布是越遠離先軸越降 下式: 上的點(X,y)與焦點(p,〇)間的距離為&,則 1323818 h =V~(x — p) 2+y2 =7 x2— 2 p x + p2+ 4 p x =X + p = y2/ (4 p ) + p 因光束密度和光源與反射面上的點之距離的 2次方成 反比,故若以y的函數表示光束密度I,則 '[公式6 ] \ — \q/ {y2/ (4p) +p) 2 若令p為1,以0到4的範圍圖示y,則如圖7越遠離 I光軸光束密度越減少。 總光束若以0到4的範圍對y積分,則 [公式7 ] /〇4 I ο/7 {γ2/ (4ρ) +ρ) 2 dy = I〇/2p.[y/ (y2/ (4p) +p) + 2tan_i (2y)] 04 =1 . 5 1 · I 〇 顯示積分的曲線於圖8。 若在導光板中利用接近拋物面鏡的光軸之範圍,設定 •導光板反射面積為反函數並進行補正,則可抑制厚度增 加,使光束密度均勻。顯示到X座標的焦點p、y座標的 1.41p之拋物面鏡中的段差的位置函數曲線於圖9,顯示導 光板剖面的包絡線於圖1 0。 雖然拋物面鏡可產生平行光,但光束密度特性為越遠 離光軸光束越降低。為了使拋物面鏡的開口端中的光束密 度均勻,需將集中於光軸附近的光束擴散至週邊側,在開 口端返回成平行光。圖11是顯示其原理之圖,Θ1為比平 1323818 行光還擴大光束之角度,0m為反射鏡的傾斜角。以光束 密度成均勻的狀態當作光線軌跡的解析結果並顯示於圖 16〜18。 為一種對拋物面鏡開口端中的光束進行積分求總光 束,於反射鏡上求在開口端成均等的值,使與該座標連結 的線均勻化用之擴散光線軌跡。 在開口端使該總光束於光軸垂直方向成均勻而進行等 分。將總光束等分之光束係反射鏡上的y座標被由光束密 度分布求出,X座標也被求出。若連結該點與開口端的點, 則可求出擴散角度。在圖11顯示拋物面鏡9的平行光射 出,同樣地,增加(increment)反射鏡的傾斜之角度為來自 平行光的增加(increment)的擴散角之一半。為了求反射鏡 的傾斜,需求拋物面鏡9的切線的斜率(s 1 〇 p e ) m與法線的 斜率-1 / m。 拋物線上的點(X 0,y 0 )的斜率以X進行微分,得到 [公式8 ] 2 · y · dy/dx= 4 p 由切線的方程式,m為 [公式9 ] y — y 〇=dy/dx · (X — X 〇) = 2p /y . (x — x〇) y = 2p /y〇. (x + xo) .·. m = 2 p / y o 因法線與切線正交,故 19 1323818 [公式1 ο ] -l/m = -y〇//2 p 具有德 抛物® 之一, 以均句 増大 的面才| 光還擔 光在 開口蝶 光。對 點的光 大的陆 在維持拋物線的包絡線下增大反射鏡的傾斜θ 細的陡峭傾斜鏡面與緩和傾斜面而連接。藉由分割 鏡的鏡面,使來自用以被均勻的平行光的擴散角声 比拋物線的切線斜率還增大,在反射鏡開口端 t '月匕 的光束密度擴散。 以分割凹面鏡的鏡面並比抛物線的切線斜率還 陡ώ肖傾斜鏡面,與使緩和傾斜面對向於焦點方& 成。使來自配設於凹面鏡的焦點的光源的光比平行 大光束,俾比抛物線的切線斜率還增大的面的反射 面鏡開口端中成為均勻的光束密度,藉由更在前述 配設正焦距折射面,可轉換成光束密度均勻的平行 向於焦點方向的鏡面的反射光藉由再度將返回到焦 照射到凹面鏡,最終會以比拋物線的切線斜率還增 峭傾斜面的反射光被射出。 區別鏡面的傾斜成陡峭緩和並微細化乃因利用成型、 蒸鍍(evaporation)之製造為可能,但研磨困難。因此,顯 示增大傾斜作成連續曲線之方法如下。因若進行連續化, 則座標移動至後方’故必須再度計算光束密度分布、積分 曲線’惟藉由重複計算該光束密度分布、積分曲線,可極 小地收傲誤差。 顯示在反射鏡上的y座標的點中光束擴大之分布狀態 於圖13,以虛線顯示光束密度分布,以實線顯示光束密度 20 1323818 的積分曲線於圖14。 藉由以上的方法求出的曲線為 [公式11 ]The progress is not obvious. When the emission S of each of the light guide plates is arranged in a positive direction and is converted into parallel light from the refracting surface, the parallel light can be incident on the sub-pixels of the respective colors, and the layers of the radii of curvature of the convex reflecting surfaces are all the same. Therefore, since the light guide plate of the three-layer type is stacked, the mold manufacturing cost is inexpensive, and since it is one type, the manufacturability is also improved. The pixel spacing of the pixel is staggered by the three-color source and the terraced section. 16 1323818 The state of the difference is the outer parabolic mirror. The refraction surface is not shown. Figure 6. Due to parabolic use, if the light is blocked by parallel light, I becomes an uneven mirror. The concave sphere is obstructed and can be transmitted by the second power of the parabola φ at the point where the complex color is arranged. Let the parabola be [Equation 4]. y 2= 4 p X Let the parabola [Equation 5] 'and the light source use three-color light-emitting diodes. The points that are placed on the axis are the same as before, but because of the liquid crystal When the distance between the faces is the same as that of the three-layered terrace-shaped light guide plate with the positive focal length disposed on the exit surface side of the light guide plate, the oblique view can be generated in the mirror, so that the point light source is disposed at the focus. The source is located in the exit path of the parallel light, and the light source not only covers but also direct ray to the reflected parallel light. As shown in Fig. 1, Fig. 4, etc., by arranging the light source at the focus of the off-axis parabolic mirror or the off-axis parabolic mirror having the focus at the path offset of the parallel light, the parallel light can be prevented from being guided by the light source to the light guide. The photodiode of the parabolic surface in the thickness direction and the width direction of the light guide plate is alternately arranged in accordance with the arrangement order of the liquid crystal stripes, and the parallel light of the plurality of colors can be supplied. The mirror is inversely proportional to the beam density and the distance between the source and the point on the reflecting surface, so the beam distribution of the reflected light is farther away from the first axis: the distance between the point (X, y) and the focus (p, 〇) For &, then 1323818 h =V~(x - p) 2+y2 =7 x2— 2 px + p2+ 4 px =X + p = y2/ (4 p ) + p due to beam density and light source and reflection surface The distance of the point is inversely proportional to the square of the second power. Therefore, if the beam density I is expressed as a function of y, then [[Formula 6] \ — \q/ {y2/ (4p) +p) 2 If p is 1, The range of 0 to 4 is shown as y, and as shown in Fig. 7, the beam density decreases as it moves away from the I optical axis. If the total beam is integrated over y in the range of 0 to 4, then [Equation 7] /〇4 I ο/7 {γ2/ (4ρ) +ρ) 2 dy = I〇/2p.[y/ (y2/ (4p ) +p) + 2tan_i (2y)] 04 =1 . 5 1 · I 〇 The curve showing the integral is shown in Figure 8. If the range of the optical axis close to the parabolic mirror is used in the light guide plate, and the reflection area of the light guide plate is set to an inverse function and corrected, the thickness can be suppressed and the beam density can be made uniform. The positional function curve of the step difference in the 1.41p parabolic mirror showing the focus p and y coordinates of the X coordinate is shown in Fig. 9, and the envelope of the light guide plate section is shown in Fig. 10. Although a parabolic mirror can produce parallel light, the farther the beam density characteristic is, the lower the beam is from the optical axis. In order to make the beam density in the open end of the parabolic mirror uniform, it is necessary to diffuse the light beam concentrated near the optical axis to the peripheral side and return to parallel light at the open end. Figure 11 is a diagram showing the principle, Θ1 is the angle of the beam that is enlarged by the light of 1323818, and 0m is the inclination angle of the mirror. The state in which the beam density is uniform is taken as the analysis result of the ray trajectory and is shown in Figs. 16 to 18. For the purpose of integrating the beam in the open end of the parabolic mirror, the total beam is obtained, and the mirror is equalized at the open end, so that the line connected to the coordinate is used to spread the trajectory of the ray. The total beam is equally divided in the vertical direction of the optical axis at the open end. The y coordinate on the beam-beam mirror that divides the total beam is obtained from the beam density distribution, and the X coordinate is also found. When the point between the point and the open end is connected, the diffusion angle can be obtained. The parallel light emission of the parabolic mirror 9 is shown in Fig. 11, and likewise, the angle of the inclination of the mirror is increased by one half of the diffusion angle from the increment of the parallel light. In order to find the tilt of the mirror, the slope of the tangent of the parabolic mirror 9 (s 1 〇 p e ) m and the slope of the normal line -1 / m are required. The slope of the point (X 0,y 0 ) on the parabola is differentiated by X to obtain [Equation 8] 2 · y · dy/dx = 4 p Equation by tangent, m is [Formula 9] y — y 〇=dy /dx · (X — X 〇) = 2p /y . (x — x〇) y = 2p /y〇. (x + xo) .·. m = 2 p / yo Since the normal is perpendicular to the tangent, 19 1323818 [Formula 1 ο ] -l/m = -y〇//2 p One of the German parabolic products, with a large face evenly | The light also bears light in the opening butterfly. The light of the point is large. The slope of the mirror is increased under the envelope of the parabola. The steep steep mirror surface is connected to the gently inclined surface. By splitting the mirror surface of the mirror, the slope of the tangential angle from the diffuse angle of the uniform parallel light is increased more than the parabola, and the beam density at the open end of the mirror t'. The mirror surface of the concave mirror is divided and the slope of the tangent of the parabola is steeper than the slope of the mirror, and the gentle tilt is faced to the focus side & The light source from the light source disposed at the focal point of the concave mirror is made to have a uniform beam density in the open end of the reflecting mirror of the surface which is larger than the parallel large beam, and the tangential slope of the 还 is larger than the tangential slope of the parabola. The refracting surface, which is converted into a mirror with a uniform beam density and parallel to the focus direction, is again irradiated to the concave mirror by the returning focus, and finally the reflected light of the inclined surface is increased by the tangential slope of the parabola. It is possible to distinguish between the inclination of the mirror surface and the steepness and the refinement due to the production by molding or evaporation, but the polishing is difficult. Therefore, the method of increasing the inclination to form a continuous curve is as follows. If the coordinates are moved to the rear, the beam density distribution and the integral curve must be calculated again. However, by repeatedly calculating the beam density distribution and the integral curve, the error can be extremely small. The distribution of the beam expansion in the point of the y coordinate displayed on the mirror is shown in Fig. 13, and the beam density distribution is shown by a broken line, and the integral curve of the beam density 20 1323818 is shown by a solid line in Fig. 14. The curve obtained by the above method is [Equation 11]

y2=a . ρ · X— bXC 4. 5 < a < 7 . 5 , o^b , 〇 ^ c a為反射鏡的軸方向長度,因正焦距折射面的傾斜每 '丁寻的影 響而具有寬度。x<2之淺的反射鏡的情形,第2頊认 ^ 的貢獻 小’無須利用第2項的補正,藉由隨著X變長而調整匕 使均勻性變佳。X長的’亦即口徑y大的反射鏡如 圓7因 越遠離光轴光束密度越減少,故如a般不顯著。 顯示比較光束密度均勻化反射鏡的a = 5.8、h〇 υ〜幺.5、 c = 2、p=l中的曲線與拋物線之圖於圖15。 若將該擴散光入射到正焦距折射面,則可返回成平〜 光,據此,可得到光束密度均勻的平行光。顯示用以返了 成平行光的折射面的角度於圖12。 回 藉由正焦距折射面轉換成平杆 率03為 战干仃於先軸用的界面之斜 [公式1 2 ] 03~~9〇° —tan-1 (sin^,/ in 2y γ, ni'<=〇S0,) 對'各擴散角度求03,若形成連 琛、透鏡曲線。顯示入射到導# & 初印曲 Μ ^ τ 九板等的透光物質時,以_Y2=a . ρ · X— bXC 4. 5 < a < 7 . 5 , o^b , 〇 ^ ca is the axial length of the mirror, due to the inclination of the refractive surface of the positive focal length Has a width. In the case of a shallow mirror of x<2, the contribution of the second 顼^ is small.] It is not necessary to use the correction of the second term, and the uniformity is improved by adjusting 匕 as X becomes longer. A mirror having a length X, that is, a mirror having a large aperture y, such as the circle 7, is less marked as far as it is farther from the optical axis. The graph showing the curve and parabola in a = 5.8, h〇 υ~幺.5, c = 2, p=l of the comparative beam density uniformizing mirror is shown in Fig. 15. When the diffused light is incident on the positive focal length refractive surface, it can be returned to flattened light, whereby parallel light having a uniform beam density can be obtained. The angle at which the refractive surface for returning parallel light is displayed is shown in Fig. 12. The back is converted by the positive focal length refracting surface into a flat rod rate 03 for the interface of the warhead to the front axis [Formula 1 2 ] 03~~9〇° —tan-1 (sin^,/ in 2y γ, ni' <=〇S0,) For each of the diffusion angles, 03 is obtained, and a twist and a lens curve are formed. When the light-transmitting substance incident on the #######################

巧將正焦距折射面轉換成平扞 ^ U 16。不僅平行光,也能藉由折射:解析結果的曲線於圖 均勻的擴散光、收斂光。 的曲線轉換成光束密度 藉由平凸透鏡的平面轉換的折射光射The positive focal length refracting surface is converted to a flat 捍 ^ U 16 . Not only parallel light, but also by refracting: the curve of the analytical result is uniformly diffused and convergent in the figure. The curve is converted into a beam density. The refracted light is converted by the plane of the plano-convex lens.

1323818 Μ &光束密度均勻化反射鏡反射的擴散光照射到空 中的清形為折射面變成複數,顯示以平凸透鏡構成的例 於圖17。 [公式1 3 ] 0 2 - S 1 η 1 (η 1 / η 2 · s i η Θ 〗) 藉由折射面轉換成平行於光軸用的界面之斜率03i [公式1 4 ] 〇3=yU (s ίηθ2/ (η,/η,-co s Θ2) 顯不使透鏡厚比折射率丨.55的平凸透鏡還薄的菲涅 透鏡(Fresnel lens)的例子於圖18。 若入射到具有正焦距折射面的導光板’則梯田狀導 板的段差變成一定,包絡線成為直線,故由圖9、圖1〇 補償方法薄型化為可能。 因即使是使光束密度均勻化的反射鏡直接光也會 疊,直接光與距離的2次方成反比’故到照射面的距離 近越不均勻,光束容易集中於光軸附近。因此,如圖 所示,可藉由在光源的前方配設附有開口的遮光體限制 接光,緩和在光源前方因凹面鏡反射光與來自光源的直 光重疊造成的光束集中。可藉由配合凹面鏡反射光的光 密度設定設於遮光體的開口孔的尺寸、密度而使光束均 化。可將光源的前方之附有開口的遮光體取代成凸面鏡 藉由以凸面鏡反射到凹面鏡提高效率。而且,如圖20 示,可藉由將以設於凸面鏡的孔徑部(aperturepart)面 氣 子 爾 光 的 重 越 19 直 接 束 勻 所 積 22 132381¾ 設定透射光量時的孔徑部作成凹透鏡,控制擴散狀態。 構 顯 具 入 成 率 面 導 的 反 開 顯 長 均 板 形 面 〇 光 能 色 層 ® 21〜23是製作成在兩方命具有梯田狀凸反射面的 - ie ^ 個光源供給各色的構造。在以液晶顯示裝置的 - 示面為ΧΥ平面’以紙面橫方向為X軸時’以對yz平面 有傾斜成梯田狀之第一微小傾斜反射面將由導光板側面 射到y轴方向的平行光轉換成X軸方向。具有分散配置 梯田狀的微小段差之傾斜反射面若採用液晶面板側的曲 半徑長’相反側短的凸反射面,則與第二微小傾斜反射 鲁的位置無關’可擴大光束成一定的y方向長度。若將在 光板内被轉換成X方向的光束照射到分散配置成梯田狀 第二微小傾斜反射面’則以凸圓筒全反射面擴大光束並 射到位於略垂直方向的液晶面板。 藉由使用三層導光板’以次像素寬度的條紋間距錯 第二梯田狀段差部,由三個光源照射三色,可進行彩色 示。該凸圓筒全反射面可藉由增加入射側的曲率半徑的 度,減少遠方側的長度,使入射到液晶面板的光束密度 籲勻。雖然在一層導光板與一個發光元件的構成中液晶面 需要彩色濾光片’但三層導光板與三色的發光元件的情 液晶面板不使用彩色濾光片也能進行彩色顯示。因以凸 鏡擴大光束,故無須擴散片’可效率佳地提高正面亮度 藉由使用二層具有第一、第二梯田狀反射面的導 -·板,以次像素寬度的條紋間距錯開第二梯田狀段差部, _以三個光源實現彩色顯示。三層導光板各自具有其他顏 的光源,藉由平行光轉換手段供給平行光。圖Μ是將三 23 1323818 製作於同一導光板時的狀態。在射出面側配設正焦 面,俾不發生到液晶面的距離依存性。 第一凸反射面與前項一樣,液晶面侧的曲率半 縮短底面側並緩和第二梯田狀導光板之上段與下 異。在以液晶顯示裝置的顯示面為xy平面時,以4 面上具有梯田狀的段差的第一梯田狀凸反射面將由 光元件側面入射到y軸方向的平行光線擴大光束於 向並進行方向轉換,被轉換於X方向並擴大光束的 • 在第二梯田狀導光板中越是下段側光束擴大率越高 光,若將凸反射面作成圓筒狀,則在液晶面中越是 被擴大。不是圓筒,而是藉由在軸方向進行當作負 射面的補正,可不依存於位置而入射到液晶像素。 以配置成梯田狀的圓筒狀凸反射面將在長軸方 於棒狀的導光體内部的平行光擴大光束,並在射出 定間距而進行反射’更藉由以沿著射出面配置以焦 與前述凸反射面的焦點共同的正焦距折射面轉換成 參的要素之棒狀的構造,當作線光源射出並入射到導 可藉由圓筒狀的正焦距折射面傳導平行光並照射到 凸反射面。因此’不是在一片導光板具有第一、第 狀反射面的構造,而是成如圖22所示組合兩種類的 由於棒狀導光體的凸反射面、導光板的凸反射面都 狀,故模具製作比前項容易。 ^可藉由將三色的光依顏色區別照射到三片液晶 稿7L件,以二色錯開配置分散配置於三層導光板内 距折射 徑長, 段的差 t yz平 背光導 X軸方 光線為 的入射 下段越 焦距反 向傳導 面側成 點位置 平行光 光板。 圓筒狀 -梯田 構造。 是圓筒 顯示原 的反射 24 1323818 面,以反射面擴大光束到像素寬度並混合三色於透射型 幕,在顯示面合成而進行彩色顯示。液晶投影機是在合 三色後入射到投影透鏡,惟因以三層的反射面擴大投影 •故可不使用交又分色稜鏡(cross dichroic prism)而在 幕上混色合成三色光’故構造簡單且低價格。 於在xy平面上具有梯田狀的段差的略楔形導光板的 射面配設顯示原稿元件,若照射到梯田狀反射面,則藉 凸反射面中的光束擴大功能在位於xy平面的顯示面擴 鲁畫像並使該反射光被反射,可將小的液晶顯示原稿元件 畫像擴大顯示於螢幕。 因以梯田狀導光板的反射面進行畫像擴大,故入射 的液晶顯示元件為細長的形狀。僅將其畫像擴大於段丘 斜方向的情形需厚度方向被壓縮扁平化的晝像。 段丘方向的段差的間距並非被限定於像素寬度,也 藉由以一個反射面投影複數個像素,在螢幕上合成三色 進行彩色顯示。據此,可擴大段差的間距與反射面尺寸 |削減段數。 顯示設第1層為紅[第2層為綠G、帛3層為藍β 以第1段的凸反射面反射12個像素份的狀態的模式圖於 .25。設梯田的段丘方向的12個像素由下側起為a、b、c L。第二段以後省略。 螢 成 j 螢 入 由 大 的 面 傾 能 光 圖 若以第一層的凸反 像素照射到螢幕’ α第二層將綠的像素照射到相同 以第三層將藍的像素照射到相同位置,則在營幕上 的 的 1323818 位置被照射ΑΓ、Ag、Ab ’在螢幕上被混色。同樣地在螢幕 上的B的位置被照射Br、Bg、Bb,在螢幕上被混色。以下 全都一樣》並非能以一段無限制地分配至多數個像素,如 圖2所示與凸面的前面側比較,在後面側中會照射到寬 廣的面積,後面側為每—螢幕上的單位面積的光量降低。 _對於每一段的多數個像素,分配數需以亮度的非線性不顯 著的範圍決定。 為了彳于到對配設於xz平面上的投影顯示元件投影於乂 鲁軸方向的光,第一梯田狀構造的反射鏡是將在以平面上軸 方向為z軸的微小圓筒凸面鏡或微小圓錐凸面鏡於X方向 傾斜成梯田狀而配設。據此,藉由微小圓筒凸面鏡或微小 圓錐凸面鏡將反射中心轉換成X軸方向,擴大光束並反 射。藉由以對X y平面傾斜於z方向而配設的第二梯田狀構 造的反射鏡的圓筒凸面,投影至位於xy平面的垂直方向的 螢幕’可比配設於XZ平面上的投影顯示元件還能擴大顯 示。藉由使用二層在位於X y平面的顯示面擴大晝像並反 鲁射該反射光的導光板’以次像素寬度的條紋間距錯開第_ 梯田狀段差部,以三個光源將顯示元件畫像擴大顯示於榮 幕,可比配設於X Z平面上的投影顯示元件還能擴大顯示。 導光板的透明物質係聚甲基丙烯酸甲酯(P〇lymethyl methacrylic acid:PMMA)樹脂、脂環埃丙稀酸樹脂 _ (alicyclic acrylic resin) ' 環烯烴樹脂(cycl〇〇lefin resin)、聚碳酸酯(polycarbonate: PC)、空氣等較適合。 使用螢幕大畫面顯示的情形,若將透光物質製作成高分子 26 1323818 材料,則會影響重量、價格、成型畸變等。在反射面形成 蒸鍍膜等的鏡面因需透過三層導光板,故需限定於凸反射 面,需罩幕(masking)、餘刻(etching)製程等。 透明物質使用空氣,爲形成凸反射面以逯光物質並以 凸反射面的入射側當作對平行光垂直的面,將平行光入射1323818 Μ & Beam Density Homogenization The diffused light reflected by the mirror is illuminating into the air, and the refracting surface becomes a complex number, and the display is formed by a plano-convex lens. [Formula 1 3 ] 0 2 - S 1 η 1 (η 1 / η 2 · si η Θ 〗) The slope of the interface for conversion to the plane parallel to the optical axis by the refractive index 03i [Equation 1 4 ] 〇 3 = yU ( s ίηθ2/ (η, /η, -co s Θ2) An example of a Fresnel lens which is not thinner than a plano-convex lens having a lens thickness of 丨55 is shown in Fig. 18. If it is incident on a positive focal length In the light guide plate of the refracting surface, the step difference of the terrace-shaped guide plate becomes constant, and the envelope becomes a straight line, so that the compensation method of FIG. 9 and FIG. 1 can be made thinner, because even the mirror which makes the beam density uniform is directly light. Stacking, the direct light is inversely proportional to the square of the distance. Therefore, the distance to the illuminated surface is more uneven, and the beam is easily concentrated near the optical axis. Therefore, as shown in the figure, it can be attached in front of the light source. The light-shielding body having an opening restricts the light-collecting, and mitigates the concentration of the light beam caused by the overlap of the reflected light of the concave mirror and the direct light from the light source in front of the light source. The size of the opening hole provided in the light-shielding body can be set by the optical density of the light reflected by the concave mirror, Density and homogenization of the beam. An opening can be attached to the front of the light source. The light-shielding body is replaced by a convex mirror to improve the efficiency by reflecting the convex mirror to the concave mirror. Moreover, as shown in Fig. 20, the weight of the surface of the aperture portion provided on the convex mirror can be directly concentrated. 22 1323813⁄4 When the amount of transmitted light is set, the aperture portion is made into a concave lens to control the diffusion state. The reverse-opening and uniform-plate-shaped surface of the surface-conducting surface is formed. The 21~23 is made in both directions. The structure of the terrace-like convex reflecting surface - ie ^ light source is supplied to each color. When the liquid crystal display device - the display surface is the ΧΥ plane ' when the paper surface is the X-axis direction, the first direction is inclined to the yz plane. The micro-inclined reflecting surface converts the parallel light that is incident on the y-axis direction from the side of the light guide plate into the X-axis direction. The inclined reflecting surface having a small step difference in a distributed arrangement of the terraces has a curved radius of the liquid crystal panel side and a short convex reflection on the opposite side. The surface is independent of the position of the second tiny oblique reflection Lu. The enlarged beam can be a certain length in the y direction. If the beam is converted into the X direction in the light panel The second micro-inclined reflecting surface that is dispersed and arranged in a terrace shape expands the light beam by the convex full reflection surface and is incident on the liquid crystal panel located in a slightly vertical direction. The stripe pitch of the sub-pixel width is used by using the three-layer light guide plate. The second terrace-like section is illuminated by three light sources and can be colored. The convex full-reflection surface can reduce the length of the far side by increasing the radius of curvature of the incident side, so that the liquid crystal is incident on the liquid crystal. The beam density of the panel is uniform. Although the liquid crystal surface requires a color filter in the structure of one light guide plate and one light-emitting element, the liquid crystal panel of the three-layer light guide plate and the three-color light-emitting element can be used without using a color filter. Perform color display. Since the beam is enlarged by the convex mirror, the diffusion sheet can be used to improve the front brightness efficiently. By using two layers of the first and second terrace-shaped reflecting surfaces, the stripe pitch of the sub-pixel width is shifted by the second. The terraced section is poorly colored, _ with three light sources for color display. The three-layer light guide plates each have a light source of another color, and the parallel light is supplied by the parallel light conversion means. Figure 状态 is the state when three 23 1323818 are made on the same light guide plate. A positive focal plane is disposed on the exit surface side, and the distance dependence on the liquid crystal surface does not occur. The first convex reflecting surface is the same as the above, and the curvature on the liquid crystal side is shortened by half on the bottom side and the upper portion of the second terrace-shaped light guiding plate is lowered. When the display surface of the liquid crystal display device is the xy plane, the first terrace-like convex reflecting surface having a stepped-like step on the four sides expands the beam of the parallel light incident on the y-axis direction from the side surface of the optical element. In the second terrace-shaped light guide plate, the higher the light beam expansion ratio is, the higher the light beam expansion rate is. In the second terrace-shaped light guide plate, the convex reflection surface is formed into a cylindrical shape, and the liquid crystal surface is enlarged. Instead of a cylinder, it is corrected as a negative surface in the axial direction, and can be incident on the liquid crystal pixel without depending on the position. The cylindrical convex reflecting surface arranged in a terrace shape enlarges the parallel light of the long light axis inside the rod-shaped light guiding body, and reflects at a predetermined pitch, and is further disposed by being arranged along the emitting surface. A positive focal length refractive surface common to the focal point of the convex reflecting surface is converted into a rod-like structure of the reference element, and is emitted as a line light source and incident on the conductive surface. The parallel light is radiated by the cylindrical positive focal length refractive surface and irradiated To the convex reflective surface. Therefore, instead of the structure in which one of the light guide plates has the first and first reflecting surfaces, the two types of convex reflecting surfaces of the rod-shaped light guiding body and the convex reflecting surface of the light guiding plate are combined as shown in FIG. Therefore, the mold making is easier than the previous one. ^ By illuminating the three colors of the light to the three liquid crystal drafts 7L, the two-color staggered arrangement is dispersed in the three-layer light guide plate from the refraction path length, and the difference of the segments is yz. The light is incident on the lower part of the focal point and the opposite side of the opposite conduction side is parallel to the light plate. Cylindrical - terraced structure. It is a cylinder that displays the original reflection 24 1323818 surface, expands the beam to the pixel width with a reflecting surface, and mixes the three colors into the transmissive screen, and synthesizes it on the display surface for color display. The liquid crystal projector is incident on the projection lens after combining three colors. However, since the projection is enlarged by the three-layer reflection surface, it is possible to mix and match the three-color light on the screen without using cross dichroic prism. Simple and low price. The surface of the slightly wedge-shaped light guide plate having a terrace-like step on the xy plane is provided with a display original element. When the terrace-shaped reflecting surface is irradiated, the beam expanding function in the convex reflecting surface is expanded on the display surface located on the xy plane. The Lu image and the reflected light are reflected, and the small liquid crystal display original element image can be enlarged and displayed on the screen. Since the image is enlarged by the reflecting surface of the terrace-shaped light guiding plate, the incident liquid crystal display element has an elongated shape. In the case where only the image is enlarged in the oblique direction of the segmental hill, the image in which the thickness direction is compressed and flattened is required. The pitch of the step difference in the segment direction is not limited to the pixel width, and a plurality of pixels are projected on one reflecting surface to synthesize three colors on the screen for color display. According to this, the pitch of the step and the size of the reflecting surface can be enlarged. The display shows a state in which the first layer is red [the second layer is green G, and the third layer is blue β, and the convex reflection surface of the first segment is reflected by 12 pixels. The 12 pixels in the direction of the segment of the terrace are a, b, and c L from the lower side. The second paragraph will be omitted later. The fluorescing j is illuminated by a large facet energy image. If the first layer of convex anti-pixels is illuminated to the screen 'α, the second layer illuminates the green pixels to the same level, and the third layer illuminates the blue pixels to the same position. Then, at the 1323818 position on the camp, it is illuminated, Ag, Ab' is mixed on the screen. Similarly, the positions of B on the screen are irradiated with Br, Bg, and Bb, and are mixed on the screen. The following are all the same. It is not possible to distribute to a large number of pixels in an unrestricted manner. As shown in Fig. 2, compared with the front side of the convex surface, a wide area is illuminated in the rear side, and the rear side is the unit area on each screen. The amount of light is reduced. For a large number of pixels in each segment, the number of allocations is determined by the range in which the nonlinearity of the luminance is not significant. In order to project light projected on the xz plane by the projection display element disposed on the xz plane, the first terrace-like mirror is a micro-cylindrical mirror or a tiny z-axis in the plane axis direction. The conical convex mirror is arranged in a terrace shape in the X direction. According to this, the reflection center is converted into the X-axis direction by a micro cylindrical convex mirror or a micro conical convex mirror, and the beam is enlarged and reflected. By projecting a cylindrical convex surface of a second terrace-shaped mirror disposed obliquely to the z-direction with respect to the X y plane, a projection screen that is projected to a vertical direction on the xy plane can be disposed on the XZ plane Can also expand the display. The display element is imaged by three light sources by using two layers of the light guide plate that enlarges the image on the display surface of the X y plane and back-reflects the reflected light by the stripe pitch of the sub-pixel width. The enlarged display is displayed on the screen, and the projection display element disposed on the XZ plane can be enlarged. The transparent material of the light guide plate is P〇lymethyl methacrylic acid (PMMA) resin, alicyclic acrylic resin cycline-lefin resin, polycarbonate Polyester (PC), air, etc. are suitable. In the case of using a large screen display, if the light-transmitting material is made into a polymer 26 1323818 material, weight, price, molding distortion, and the like are affected. The mirror surface on which the vapor deposition film or the like is formed on the reflecting surface is required to pass through the three-layer light guide plate, so it is limited to the convex reflecting surface, and a masking process or an etching process is required. The transparent substance uses air to form a convex reflecting surface with a light-emitting substance and the incident side of the convex reflecting surface as a plane perpendicular to the parallel light, and the parallel light is incident.

到全反射凸反射面,對將該反射光擴大光束於射出側的光 線略垂直的面若以透光物質構成的話,則也能取代鏡面利 用全反射。因射出側擴大光束,故平面的情形為略垂直的 射出面,稱此為梯田狀全反射面板。藉由該構成,因透光 層的大部分為空氣,為構成全反射面用的透明高分子層, ^可實現輕里化與削減成本。若使梯田狀全反射面板非常 專貝J剛陡降低,爲了不損及光學特性需要支樓。在圖2 7、 圖2 8顯示配設兼作維如,f 表(frame)的支撐基板21於背面的例 加大梯田狀全反射而Q 士 对面板3 9本身的厚度並提高剛性也可 方 取马略楔形,若使三層導光板的 互配置欢則如圖5所示變成堆疊厚的部分之構造。 立配置略楔形墓本4 j丨刀 的導光板厚度薄到約厚的部分’則如圖29所示可使 性提高,&可減少::3。因藉由交互配置使導光板 增大。 夕早0厚度並可抑制三層構造造成的 顯示透明物質為 奇才又衫機的例子於圖 機構在圖中省略。 ^氣層’及使用梯 3〇。楔形地支撐梯 田狀食反射面板的 田狀食反射面板的 27 1323818 以橫100〇mm、縱560mm的晝面尺寸,設擴大率為 倍,縱深為被攝顯示元件的短邊尺寸變成11· 2mm。使用三 層梯田狀導光板,其他能以到螢幕為止的空間為約, •除了框體的厚度外,能以縱深約80_構成背投影機。 .丨正下方照明型液晶顯示裝置薄型化,則因光束與距 光源的距離的2次方成反比,故容易發生管照。藉由^傾 斜的反射面將由正下方入射的A方向#換成+面方向,^ 傾斜反射面將傳導於平面方向的光反射到液晶面板可得 _到均勻的照明。為了將行進方向轉換成直角’反射面的傾 斜度為45 ,所以導光板厚度需要凹面鏡22的寬度,伸 如圖32所示,藉由將傾斜面分散配置成梯田狀並導二水: 面,也能適用於比凹面鏡寬度還薄的導光板。因—使水平 面透明’就會朝上部透射損失,故如圖3 3藉由將水平面作 成反射鏡並返回到光源,再利用光源前方的凹面鏡2 8的反 射光,可防止水平面透明的情形之朝上部的損失。 因返回到光源的反射鏡藉由蒸鍍等形成,故需製程的 鲁追加’惟右如圖34形成返回反射元件(retroreflection element ),則可於樹脂成型時形成,故低價格化為可能。 返回反射元件有角隅棱鏡(corner cube)或直角棱鏡,惟因 在傾斜反射面的延長上,故直角稜鏡較容易。 在正下方照明型液晶顯示裝置中,藉由傾斜的反射面 ‘ 使由正下方入射到導光板的光方向轉換成平面方向並反射 的情形,因反射面上部未被照明,故變成配設光源於端部 之一方向的傳導。配設光源於端部以外,為了反射於對向 28 1323818 的兩方向’需對被反射面包圍的三角柱部分曰 77的攸晶像素進 行照明。如圆33、圖34所示,將朝水平方&以p >卞万向的反射面29 分散成梯田狀的情形可藉由朝上部的孔似^ , 几 ^ 比(aperture ratio)的設定使三角柱部分及其他的導本 π汔板面的亮度一 致。孔徑比小的情形可藉由將孔徑部作虑自 凡貝焦距折射面, 擴大光束於三角柱上部的液晶。由轉換於次伞士二 a 丁不句的45。 之傾斜反射面、擴大光束之凹面、反射於异调 %你万向的反射 鏡構成。 配設光源於端部以外,為了反射於對向的兩方向,如 圖3 6需對被反射面包圍的三角柱部分的液晶像素進行照 明。因在三層導光板中光源部成障礙’所以需在三角柱間 授受其他顏色的光(圖38)。以藍色用導光板18内的三角 柱分割成導光板平面方向、正上方方向及接鄰三角柱方向 的三方向。顯示該等狀態於圖37的A。 緑色用導光板1G内的三角柱也分割成導光板平面方 向、正上方方向及接鄰三角柱方向的三方向,惟在傾斜反 射面30的臨界角以内入射來自藍色三角柱的藍色光。藍色 光不僅照射綠色光三角柱上部’也需傳導至接鄰的紅色光 二角柱。顯示録色三角柱與導光板1R的界面狀態於圖37 疋顯不以臨界角以内的光透過傾斜反射面的狀 態。 爲了屯成全反射面,紅色光二角柱成兩層’顯示於圖 37 的 c 〇 29 【發明的功效】 因本發明使用三層以梯田狀導光板將平行光方向轉換 的構成’並錯開次像素寬度照射到液晶層,故無彩色濾光 •片造成的損失,可提高作爲液晶裝置的透射效率3倍。因 藉由梯田狀導光板的段差設定補償由平行光轉換元件產生 的光束密度分布’故亮度均勻的照明為可能。 因梯田狀導光板將平行光擴大光束於目的方向並全反 射’故與散射方式比較損失少’設計效率的提高、構件成 φ本的削減為可能。 以液晶投影機進行彩色顯示的情形是藉由交又分色稜 鏡混色,故構造複雜且昂貴,但因在螢幕上被混色,故構 造簡單且低價格。 【實施方式】 [實施例1 ] 顯示以對角510mm(2〇. 1型)、XGA(l〇24x768)、側光的 •例子於圖5或圖6。 圖面尺寸為橫408_、縱306mm、像素間距399;czra、次 像素間距1 33 // ra。為將來自光源的光轉換成平行光而供 • 給’配設傾斜於梯田狀剖面的導光板之凸反射面。 對向於液晶側的反射面側是以均等間距配置384個圓 筒凸反射面之梯田狀構造。因導光板的梯田狀段差比像素 尺寸小,故用以擴大成像素尺寸的凸反射面是朝位於略垂 直方向的液晶的像素反射來自光源的平行光線,該凸反射 30 1323818 面無需藉由傾斜於全反射臨界角以上而形成反射 費用削減為可能。因拋物面鏡的光束密度具有距 離依存性’故加大距光軸遠的導光板底面側的段 度均勻化。 光源為在於梯田狀導光板光源部的厚度方向 向共通的拋物面鏡的焦點,依紅、綠、藍的順序 各色64個的發光二極體。發光二極體如圖4是偏身 至不遮蔽拋物面鏡9的反射光之位置。在該實施 配置發光強度25 Omcd的發光二極體各色64個於 透光率40%時得到亮度307cd/m2。 [實施例2 ] 如圖21,為將光源部與導光板一體成型,在 的軸外焦點配設白色發光二極體,供給平行光。 由導光板側面傳導至紙面縱深方向,藉由第一梯 射面擴大光束,反射到第二梯田狀凸反射面方向 第二梯田狀反射面為止的距離在上段與下段不同 凸反射面大致在下段側減小曲率半徑,將擴大角 凸反射面是對入射光設定為臨界角以上並利用全 因第二凸反射面為圓筒狀反射面,在下段與 晶面板的距離不同’故大致在上段減小曲率半徑 因在凸反射面擴大光束,故無須擴散片。因射出 性窄的光束擴大光’故無須稜鏡片。因利用全反 無須反射板。 [實施例3 ] 層,製造 光軸的距 差,使亮 與寬度方 交互配置 ^(offset) 例中藉由 兩側,在 拋物面鏡 平行光是 田狀凸反 。由於到 ,故第一 度擴大。 反射。 上段至液 ^該方式 光為指向 射,故也 以JO丄8 顯不交互配置略楔形導井 板的配置方A vi 的厚的部分,使三層導光 置方向一致的情形的全 刀 的例子於圄9η . 的導光板厚度薄到約2/3 丁於圖29。因梯田狀導光柘 板的配置方a 板為略横形,若使三層導光 方向一致,則如圖5 造,惟如圖Μ娇_ 下變成堆疊厚的部分的構 口 ^所不’若父互配罟响以 分,則鱼圖q u 置略楔形導光板的厚的部 5比較可使全體的導 光板的單層的厚度如圖i。所示為A厚度薄到約2小導 光學特性與實施例i 一樣。.2mm’故變成8.4_。 [實施例4 ] 示配置具有於導光板入 的晝像之細县“,一、对面厚度方向破壓縮爲平化 光板内的反稭由分散配置於導 反射面中的光束擴大功能,由細長的 顯示元件擔夬5丨丄 > 的形狀的液晶 擴大到大晝面的液晶顯示裝置 5l〇m m c ?n 1 , J于如下。對角 0· 1 型)、XGA ( 1 024x768 )畫面尺 mm、縱 了為撗 4〇8 mm、像素間距399μιη。於縱 的擴大率下汸曰3 縱方向在50倍 展日日顯示元件的像素尺寸變成縱8 " 顯示尺寸相同為^ 啖8以m,橫與 』馮399"m。入射面的液晶顯示 的形狀,壤土4 α不疋件為細長 先板厚度為單層6ππη,故若積層三層 置方向,則藤 增於父互配 〜导先板厚度變成12_。 L貫施例5] 顯不透明物質為空氣層,及 背投影機的例早μ 全反射面板的 J例子於圖30。楔形地支撐梯田狀全 機構在圖中省欢 王反射面板的 ,略。以橫1 0 0 0mm、縱5 6 0_的書 擴大率為50位 思面尺寸,設 u倍’縱深為被攝顯示元件的銪边α 墁尺寸變成 32 1323818 11. 2mm。使用三層該梯田肤導朵 仰街狀导九板,其他能以到螢幕為止 的空間為約30πππ’除了梅的戸痒认 ί框體的;度外,能以縱深約 構成背投影機。 _ 透明物質使用空氣,& ^爲形成凸反射面以透光物質並以 凸反射面的入射側當作對平行光垂直的面,將平行光入射 到全反射凸反射面’對將該反射光擴大光束於射出側的光 線略垂直的面是以透光物質構成。藉由該構成,因透光層 的大部分為空氣,為構成全反射面用的透明高分子層,故When the surface of the total reflection convex reflection surface which is slightly perpendicular to the light beam which expands the reflected light on the emission side is formed of a light-transmitting material, total reflection can be used instead of the mirror surface. Since the beam is enlarged on the exit side, the plane is a slightly vertical exit surface, which is called a terrace-like total reflection panel. According to this configuration, since most of the light-transmitting layer is air and is a transparent polymer layer for forming a total reflection surface, it is possible to achieve lighter weight and cost. If the terrace-like total reflection panel is very steep, the branch is required to be damaged without impairing the optical characteristics. In Fig. 27 and Fig. 28, it is shown that the support substrate 21 which serves as the frame and the frame f is arranged on the back surface, and the thickness of the panel itself is increased and the rigidity is increased. Take the Marten wedge shape, if the mutual arrangement of the three-layer light guide plate is as shown in FIG. 5, it becomes a structure in which a thick portion is stacked. The thickness of the light guide plate of the slightly wedged tomb 4 j knives is thin to about thick, and the sufficiency is improved as shown in Fig. 29, and the reduction can be reduced to: 3. The light guide plate is enlarged by the interactive configuration. The thickness of the eve is 0 and can suppress the display of the transparent substance caused by the three-layer structure. The example of the genius and the machine is omitted in the figure. ^ Gas layer' and use ladder 3〇. 27 1323818, which supports the field-reflecting panel of the terraced food-reflecting panel in a wedge shape, has a width of 100 mm and a length of 560 mm, and the magnification is doubled, and the depth of the display element is 11 2 mm. . A three-layer terrace-shaped light guide plate is used, and the other space can be approximated to the screen. • In addition to the thickness of the frame, the rear projector can be formed in a depth of about 80 mm. When the under-lighting type liquid crystal display device is made thinner, since the light beam is inversely proportional to the distance from the light source, the tube photoshoot is likely to occur. By the inclined surface of the tilting, the A direction # incident from the lower side is changed to the + surface direction, and the inclined reflecting surface reflects the light conducted in the plane direction to the liquid crystal panel to obtain uniform illumination. In order to convert the traveling direction into a right angle, the inclination of the reflecting surface is 45, the thickness of the light guide plate needs the width of the concave mirror 22, as shown in Fig. 32, by dispersing the inclined surface into a terrace shape and guiding the water: surface, It can also be applied to a light guide plate that is thinner than the width of the concave mirror. Because the water level is transparent, it will transmit loss to the upper part. Therefore, by using the horizontal plane as a mirror and returning to the light source, and using the reflected light from the concave mirror 28 in front of the light source, the horizontal plane can be prevented from being transparent. The loss of the upper part. Since the mirror returned to the light source is formed by vapor deposition or the like, the addition of the process is required. However, if a retroreflection element is formed as shown in Fig. 34, it can be formed at the time of resin molding, which makes it possible to reduce the price. The returning reflection element has a corner cube or a right-angle prism, but because of the extension of the inclined reflecting surface, the right angle 稜鏡 is easier. In the case of the direct illumination type liquid crystal display device, the light direction incident on the light guide plate from the direct downward direction is converted into a planar direction by the inclined reflection surface ′, and the reflection surface is not illuminated, so that the light source is provided with the light source. Conduction in one direction of the end. The light source is disposed outside the end portion, and the twin crystal pixel of the triangular prism portion 曰 77 surrounded by the reflecting surface is illuminated for reflection in two directions of the opposite direction 13 1323818. As shown in the circle 33 and FIG. 34, the horizontal surface & the p > gimbal reflective surface 29 is dispersed into a terrace shape, and the hole toward the upper portion can be approximated by an aperture ratio. Set the brightness of the triangular prism portion and other guide π 汔 plate surfaces to match. In the case where the aperture ratio is small, the liquid crystal on the upper portion of the triangular prism can be enlarged by taking the aperture portion into consideration of the refracting surface. Converted from the second umbrella to a second. The inclined reflecting surface, the concave surface of the enlarged beam, and the reflection are reflected in the mirror. In addition to the end portion, in order to reflect the two directions in the opposite direction, as shown in Fig. 36, the liquid crystal pixels of the triangular prism portion surrounded by the reflecting surface are illuminated. Since the light source portion is obstructed in the three-layer light guide plate, it is necessary to impart light of other colors between the triangular columns (Fig. 38). The triangular column in the blue light guide plate 18 is divided into three directions of the light guide plate plane direction, the direct upper direction, and the adjacent triangular prism direction. These states are shown in A of FIG. The triangular prism in the green light guide plate 1G is also divided into three directions of the plane direction of the light guide plate, the direction directly above, and the direction of the adjacent triangular prism, but the blue light from the blue triangular prism is incident inside the critical angle of the inclined reflection surface 30. The blue light not only illuminates the upper part of the green light triangle column but also needs to be transmitted to the adjacent red light column. The state of the interface between the color-recording triangular prism and the light guide plate 1R is shown in Fig. 37, and the light within the critical angle is transmitted through the oblique reflecting surface. In order to form a total reflection surface, the red light prism column is formed into two layers 'c 〇 29 shown in FIG. 37. [Effect of the invention] Since the present invention uses three layers to convert the parallel light direction by the terrace-shaped light guide plate, and staggers the sub-pixel width. Since it is irradiated to the liquid crystal layer, the loss due to the colorless filter and the sheet can be improved by three times as the transmission efficiency of the liquid crystal device. Since the beam density distribution generated by the parallel light conversion elements is compensated by the step difference setting of the terrace-shaped light guide plate, illumination with uniform brightness is possible. Since the terrace-shaped light guide plate expands the parallel light in the direction of the target and totally reflects the light, the loss is less compared with the scattering method, and the design efficiency is improved, and the reduction of the member is possible. The case where the color display is performed by the liquid crystal projector is mixed by the cross-separating prism, so that the structure is complicated and expensive, but because it is mixed on the screen, the construction is simple and the price is low. [Embodiment] [Embodiment 1] An example in which a diagonal of 510 mm (2〇.1 type), XGA (10〇24x768), and side light is shown in Fig. 5 or Fig. 6 is shown. The picture size is 408_ horizontal, 306mm vertical, pixel spacing 399; czra, sub-pixel spacing 1 33 // ra. In order to convert the light from the light source into parallel light, a convex reflecting surface of the light guide plate inclined to the terrace-like cross section is provided. On the side of the reflecting surface facing the liquid crystal side, a terrace-like structure in which 384 cylindrical convex reflecting surfaces are arranged at equal intervals is provided. Since the terrace section difference of the light guide plate is smaller than the pixel size, the convex reflection surface for expanding into the pixel size reflects the parallel light from the light source toward the pixel of the liquid crystal located in the slightly vertical direction, and the convex reflection 30 1323818 surface does not need to be tilted. It is possible to reduce the reflection cost by forming the critical angle above the total reflection. Since the beam density of the parabolic mirror has a distance dependence, the segment on the bottom surface side of the light guide plate farther from the optical axis is made uniform. The light source is a focus of a parabolic mirror that is common to the thickness direction of the light source portion of the terrace-shaped light guide plate, and 64 light-emitting diodes of each color in the order of red, green, and blue. The light-emitting diode is as shown in Fig. 4 at a position that is deflected to the point where the reflected light of the parabolic mirror 9 is not shielded. In this embodiment, 64 light-emitting diodes each having a luminous intensity of 25 Omcd were arranged at a light transmittance of 40% to obtain a luminance of 307 cd/m2. [Embodiment 2] As shown in Fig. 21, in order to integrally form a light source unit and a light guide plate, a white light-emitting diode is disposed at an off-axis focus, and parallel light is supplied. Conducting from the side of the light guide plate to the depth direction of the paper surface, expanding the light beam by the first stepped surface, and reflecting the distance to the second terrace-like reflecting surface in the direction of the second terrace-like convex reflecting surface is different from the convex reflecting surface in the upper and lower portions. The side reduces the radius of curvature, and the enlarged convex reflecting surface is set to a critical angle or more for the incident light and the second convex reflecting surface is a cylindrical reflecting surface, and the distance from the crystal panel is different in the lower stage. Reducing the radius of curvature Because the beam is enlarged on the convex reflecting surface, there is no need for a diffusion sheet. Since the beam with a narrow emission expands the light, there is no need for a slap. Due to the use of all-reflection, there is no need for a reflector. [Embodiment 3] Layer, the distance of the optical axis is made, and the light and width sides are alternately arranged. ^(offset) In the example, the parallax parallel light is the field convex back by both sides. Because of it, it expanded for the first time. reflection. The upper part to the liquid ^ This way the light is directed, so the thick part of the arrangement side A vi of the slightly wedge-shaped guide plate is also arranged with JO丄8, so that the three layers of light guiding directions are the same. For example, the thickness of the light guide plate at 圄9η. is as thin as about 2/3. Because the configuration of the terrace-shaped light guide plate is slightly horizontal, if the three layers of light guide directions are the same, as shown in Figure 5, but as shown in Fig. 5, the structure becomes a thick part of the stack. If the father is matched with each other, the thick portion 5 of the wedge-shaped light guide plate can be compared to the thickness of the single layer of the entire light guide plate as shown in FIG. It is shown that the thickness of A is as thin as about 2 and the optical characteristics are the same as in the embodiment i. .2mm' becomes 8.4_. [Embodiment 4] It is shown that a fine county having an image of a light guide plate is disposed. "I. The opposite side of the thickness direction is broken into a flat beam. The anti-straw in the flattened light plate is dispersed and disposed in the light-conducting surface. The liquid crystal display device of the shape of the display element of 5夬> is enlarged to the large-surface liquid crystal display device 5l〇mmc?n 1 , J is as follows. Diagonal 0·1 type), XGA (1 024x768) picture size mm The vertical length is 〇4〇8 mm, and the pixel pitch is 399μιη. In the vertical expansion ratio 汸曰3, the vertical direction is displayed on the 50th day of the day. The pixel size of the display element becomes vertical 8 " The display size is the same as ^ 啖8 to m , horizontal and "Feng 399 " m. The shape of the liquid crystal display on the incident surface, the loam 4 α is not a piece of the thickness of the slender first plate is a single layer 6ππη, so if the three layers are stacked, the vine is added to the parent. The thickness of the first plate becomes 12_. L. Example 5] The opaque substance is the air layer, and the example of the back projector is an example of the full-reflection panel of Fig. 30. The wedge-shaped support of the terrace-like mechanism is shown in the figure. Reflective panel, slightly. Expanded with a book of 1 0 0 0 mm and 5 6 0_ For 50 face sizes, set u times 'depth to the edge of the displayed display element α 墁 size becomes 32 1323818 11. 2mm. Use three layers of the terraced skin guide to the street-shaped guide nine-plate, the other can be used to the screen The space so far is about 30πππ' except for the itching of the frame of the plum; in addition, it can form the rear projector in depth. _ The transparent substance uses air, & ^ is to form a convex reflecting surface to transmit light and to The incident side of the convex reflecting surface is a plane perpendicular to the parallel light, and the parallel light is incident on the total reflection convex reflecting surface. The surface which is slightly perpendicular to the light beam which expands the reflected light on the emitting side is composed of a light transmitting material. In this configuration, since most of the light-transmitting layer is air, it is a transparent polymer layer for forming a total reflection surface.

可實現輕里化與削減成本。若使梯田狀全反射面板非常 薄,則剛性降低,爲了不損及光學特性需要支撐,顯示配 及兼作框架的支撐基板2 1於背面的例子。 [實施例6 ] 顯示使用三色的冷陰極管’藉由傾斜的反射面將由正 下方入射的光方向轉換成平面方向,藉由傾斜反射面將傳 導於平面方向的光反射到液晶面板的例子於圖35。光源部 使用將光束密度轉換成均勻的平行光之凹面鏡,將由正下 方方向轉換成導光板平面方向的傾斜面分散配置成梯田 狀’並可藉由返回反射元件使水平面部比凹面鏡的孔徑寬 度還薄。被照射於傾斜反射面以外的光藉由返回反射元件 返回到光源,藉由再利用光束密度均勻化反射鏡中的光源 前方的凹面鏡28的反射光,最終可射出到導光板的平面方 向。分散配置於傾斜反射面的水平面部分若如圖34形成返 回反射元件’則可於樹脂成型時形成’故低價格化為可能。 因返回反射元件在傾斜反射面的延長上,故作成直角稜鏡 33 並槔回到光源, 4行再反射並射 出到導光板的平面方向。 【圖式簡單說明】Lightweight and cost-cutting can be achieved. When the terrace-like total reflection panel is made very thin, the rigidity is lowered, and support is required in order not to impair the optical characteristics, and an example in which the support substrate 21 which also serves as a frame is displayed on the back surface is shown. [Embodiment 6] A cold cathode tube using three colors is shown. The direction of light incident directly from below is converted into a planar direction by a tilted reflecting surface, and the light transmitted in the planar direction is reflected to the liquid crystal panel by the inclined reflecting surface. Figure 35. The light source portion uses a concave mirror that converts the beam density into uniform parallel light, and the inclined surface that is converted from the direct downward direction into the plane direction of the light guide plate is dispersedly arranged in a terrace shape and can return the horizontal surface to the aperture width of the concave mirror by the return reflecting member. thin. The light irradiated on the outside of the inclined reflecting surface is returned to the light source by the returning reflection element, and the reflected light of the concave mirror 28 in front of the light source in the mirror is made uniform by the beam density, and finally emitted to the plane direction of the light guide plate. When the horizontal portion which is disposed on the inclined reflecting surface is formed as shown in Fig. 34, it can be formed at the time of resin molding, so that it is possible to reduce the price. Since the returning reflection element is extended on the inclined reflecting surface, it is formed at a right angle 稜鏡 33 and returned to the light source, and the four rows are reflected again and emitted to the plane direction of the light guiding plate. [Simple description of the map]

’照射到次像素寬度的狀態之圖。 圖2是顯示藉由梯田狀導光板的 傾斜的凸反射面將平 行光擴大光束並全反射的狀態之圖β 圖3是顯示藉由凸反射面擴大光束並照射到次像素寬 度的角度與尺寸的關係之圖。 圖4是顯示使用三層梯田狀導光板將三色的平行光錯 開次像素寬度並照射到液晶層的狀態之圖。 圖5是顯示寬度與深度方向都配置抛物面鏡於三層導 光板的狀態之斜視圖。 圖6是顯示在導光板的各層的射出部配置正焦距折射 面並照射平行光至次像素的狀態之圖。 圖7是以y為正的範圍顯示拋物面鏡的光束密度分布 之圖。 圖8是以y為正的範圍顯示對拋物面鏡的光束密度積 分的分布之圖。 圖9是顯示用以使由拋物面鏡反射的平行光光束密度 均勻化之導光板的段差分布之圖。 34 1323818 圖ίο是顯示用以使光束密度均勻化之導光板的厚度分 布之圖。 圖11是顯示用以使拋物面鏡的光束密度均勻化的傾斜 反射光及反射面的斜率之圖。 圖12是顯示藉由折射面將用以使拋物面鏡的光束密度 均勻化的傾斜反射光轉換成平行光的角度狀態之圖。 圖1 3是顯示用以使光束密度均勻化的傾斜反射光的傾 斜分布之圖。 圖14是顯示由光束密度均勻化反射鏡反射的光束密度 分布及光束密度的積分之圖。 圖15是以y為正的範圍顯示光束密度均勻化反射鏡、 拋物面鏡的曲線之圖。 圖16是顯示由光束密度均勻化反射鏡與平凸透鏡反射 的光束密度均勻的平行光之圖。 圖17是顯示由光束密度均勻化反射鏡與正焦距折射面 反射的光束密度均勻的平行光之圖。 圖18是顯示由光束密度均勻化反射鏡與菲涅爾透鏡反 射的光束密度均勻的平行光之圖。 圖19是顯示以凹面鏡反射光源前方的直接光,當作光 束密度均勻化凹面鏡反射’照射由前方凹面鏡孔徑部透射 的透射光的狀態之圖。 圖2 0是顯示藉由透鏡擴散照射由前方凹面鏡孔徑部透 射的透射光的狀態之圖。 圖21是顯示以一個光源照明各層,以第一梯田狀反射 35 〜οίδ 面將縱深方向的光線轉換成第二梯田狀反射面 —梯田狀反射面照射到液晶面板的構成之圖。 圖22是顯示以正焦距折射面將以第—梯田 換縱/衣方向的光線後的光束擴大光轉換成平行 第一梯田狀反射面方向的構成之圖。 圓2 3是顯示以一個光源照明各層’略楔形 的導光板形狀之圖。 圖24是顯示在導光板的入射部配設細長 ’照射平行光並以導光板擴大顯示的狀態之 圖25是顯示將平行光照射到投射原稿元件 田狀反射面將縱深方向的光線轉換成第二梯田 向’以第二梯田狀反射面將複數個像素照射到 的液晶顯示裝置之圖。 圖26是顯不將第二梯田狀反射面的縱深方 狀’抑制以第一梯田狀反射面轉換縱深方向的 束擴大光其反射光的光束擴大的狀態之圖。 圖27是顯示令透光層為空氣並構成背投影 體形成轉換縱深方向光線的第一梯田狀反射面 視圖》 圖28是顯示由令透光層的大部分為空氣並 成第一梯田狀反射面之二層的梯田狀反射面構 機之側視圖。 圖29是顯示各層交互配置略楔形的導光板 化的構成之圖。 方向,以第 狀反射面轉 光並傳導於 地構成各層 液晶顯示元 圖。 ’以第一梯 狀反射面方 螢幕而混色 向作成凹面 光線後的光 機,以板狀 的狀態之俯 以板狀體形 成的背投影 形狀而薄型 36 1323818 圖30是顯示令透光層的大部分為空氣並以板狀體形成 第二梯田狀反射面,厚的部分交叉而配置三層的梯田狀反 射面的背投影機之側視圖。 圖31是顯示使用三層梯田狀導光板,由三色的冷陰極 管構成的側光構成之圖。 圖32是顯示以傾斜的反射面將由正下方型背光產生的 光束密度均勻的平行光轉換成平行於導光板的方向的狀態 之圖。 圖3 3是顯示藉由分散配置傾斜面成梯田狀,將水平面 作成反射鏡並返回到光源後再反射,防止朝水平面上部的 損失的狀態之圖。 圖3 4是顯示令返回到光源的部分為返回反射元件並返 回到光源的狀態之圖。 圖35是顯示使用三層梯田狀導光板,配置三色的冷陰 極管於端部之正下方型背光的構成之圖。 圖36是以一層的導光板顯示將朝水平方向的反射面分 散成梯田狀,以朝上部的孔徑比的設定使三角柱部分和其 他的導光板面的亮度一致的原理之圖。 圖37是顯示使用三層梯田狀導光板,由用以配光給由 三色的冷陰極管構成的正下方型背光的三角柱部分的最下 層的三角柱傳導至上層三角柱的原理之圖。 圖38是顯示使用三層梯田狀導光板,用以配光給由三 色的冷陰極管構成的正下方型背光的三角柱部分的構成之 圖0 37 1323818 圖39是顯示由漫反射點構成的習知的導光板的構成之 圖。 圖40是顯示以傾斜的反射面反射來自冷陰極管的擴散 光之習知的導光板的構成之圖。 圖41是顯示採用光源附近的斜率為参,垆士 ^ + τ勺貝顆大m方的段 差之習知的導光板的構成之圖。 圖42是顯示由正下方型背光的波型反射鏡構习 的習知 的反射鏡的構造之圖。 φ 圖43是顯示習知的可攜式機器用側光的構造與* 均之圖。 。元線不 圖44是顯示習知的背投影機的構造之圖。 圖45是顯示積層以條紋寬度具有遮光層的導光體, 使用彩色濾光片的習知的導光板的構造之圖。 【主要元件符號說明】 I :梯田狀導光板 _ 2 :次像素 3 :空隙 5 :凸反射面 .7 :點光源 8 :線光源 9 :抛物面鏡 II :凹透鏡 1 2 .偏光板 1323818 1 3 :透明基板 1 4 .液晶層 1 5 :平行光 2 0 :配線基板 22:光束均勻化凹面鏡 23 :正焦距折射面 24 :凸面鏡 2 5 :狹縫 27 :棒狀導光體 28 :凹面鏡 29 :反射面 30 :三角柱 31 :反射鏡 33 :全反射光 34:返回反射元件 36 :負焦距折射面 3 7 :低折射率層 39 :透光物質 40 :焦點 4 3 ·液晶面板 51 :螢幕 5 2 .投射原柄 56 :投射裝置 58 :擴散材料層 39 1323818 60 :擴散材料 61 :稜鏡 62 :漫反射點層 66 :遮光體 40A diagram of a state in which the sub-pixel width is irradiated. 2 is a view showing a state in which a parallel light is enlarged and totally reflected by a convex convex reflecting surface of a terrace-shaped light guiding plate. FIG. 3 is a view showing an angle and a size of a sub-pixel width by expanding a light beam by a convex reflecting surface. Diagram of the relationship. Fig. 4 is a view showing a state in which three-color parallel light is shifted by a sub-pixel width and irradiated to a liquid crystal layer by using a three-layer terrace-shaped light guide plate. Fig. 5 is a perspective view showing a state in which a parabolic mirror is disposed on a three-layer light guide plate in both the width and the depth direction. Fig. 6 is a view showing a state in which a positive focal length refractive surface is disposed on an emitting portion of each layer of the light guiding plate and parallel light is irradiated to the sub-pixel. Fig. 7 is a view showing a beam density distribution of a parabolic mirror in a range in which y is positive. Fig. 8 is a graph showing the distribution of the beam density distribution to the parabolic mirror in a range in which y is positive. Fig. 9 is a view showing a step distribution of a light guide plate for homogenizing the density of parallel light beams reflected by a parabolic mirror. 34 1323818 Figure ίο is a diagram showing the thickness distribution of a light guide plate for homogenizing the beam density. Fig. 11 is a view showing the slope of the oblique reflected light and the reflecting surface for making the beam density of the parabolic mirror uniform. Fig. 12 is a view showing an angular state in which obliquely reflected light for homogenizing a beam density of a parabolic mirror is converted into parallel light by a refractive surface. Fig. 13 is a diagram showing the oblique distribution of obliquely reflected light for equalizing the beam density. Fig. 14 is a graph showing the integration of the beam density distribution and the beam density reflected by the beam density uniformizing mirror. Fig. 15 is a view showing a curve in which the beam density is uniformized by a mirror or a parabolic mirror in a range in which y is positive. Fig. 16 is a view showing parallel light having a uniform beam density reflected by a beam density uniformizing mirror and a plano-convex lens. Fig. 17 is a view showing parallel light having a uniform beam density reflected by a beam density uniformizing mirror and a positive focal length refractive surface. Fig. 18 is a view showing parallel light having a uniform beam density reflected by a beam density uniformizing mirror and a Fresnel lens. Fig. 19 is a view showing a state in which direct light in front of a light source is reflected by a concave mirror, and the transmitted light transmitted from the front concave mirror aperture portion is irradiated as a uniformity of the beam density. Fig. 20 is a view showing a state in which the transmitted light transmitted from the front concave mirror aperture portion is diffused by the lens diffusion. Fig. 21 is a view showing a configuration in which the respective layers are illuminated by one light source, and the light in the depth direction is converted into the second terrace-like reflecting surface by the first terrace-like reflection 35 - o δ δ surface - the terrace-like reflecting surface is irradiated onto the liquid crystal panel. Fig. 22 is a view showing a configuration in which the beam-expanded light after the light in the direction of the first-treading direction/clothing direction is converted into the direction parallel to the first terrace-like reflecting surface by the positive focal length refractive surface. The circle 2 3 is a view showing the shape of the light guide plate in which the respective layers are slightly wedge-shaped by one light source. FIG. 24 is a view showing a state in which an elongated 'illuminated parallel light is disposed on the incident portion of the light guide plate and enlarged by the light guide plate. FIG. 25 is a view showing that the parallel light is irradiated onto the field-shaped reflecting surface of the projected original element to convert the light in the depth direction into the first direction. The two terraces are diagrams of a liquid crystal display device that irradiates a plurality of pixels with a second terrace-like reflecting surface. Fig. 26 is a view showing a state in which the depth direction of the second terrace-shaped reflecting surface is suppressed from being expanded by the beam-expanding light in the depth direction of the first terrace-like reflecting surface. Figure 27 is a view showing a first terrace-like reflecting surface in which the light-transmitting layer is made air and the rear-projection body is formed to convert the light in the depth direction. Figure 28 is a view showing that the light-transmitting layer is mostly air and is formed into a first terrace-like reflection. Side view of a two-story terrace-like reflecting surface structure machine. Fig. 29 is a view showing the configuration of a light guide plate in which the layers are alternately arranged in a slightly wedge shape. The direction is converted by the first reflecting surface and transmitted to the ground to form a liquid crystal display element. 'A light machine that produces a concave ray with a first step-like reflective surface screen, and a thin-shaped shape formed by a plate-like state in a plate-like state. 36 1323818 FIG. 30 shows the light-transmitting layer. A side view of a rear projector in which a plurality of terrace-like reflecting surfaces are formed by forming a second terrace-like reflecting surface with a thick portion and a three-layered terrace-like reflecting surface. Fig. 31 is a view showing the configuration of side light composed of three color cold cathode tubes using a three-layer terrace-shaped light guide plate. Fig. 32 is a view showing a state in which parallel light having a uniform beam density generated by a direct type backlight is converted into a direction parallel to the light guide plate with an inclined reflecting surface. Fig. 3 is a view showing a state in which the inclined surface is dispersed in a terrace shape, the horizontal plane is made into a mirror, and returned to the light source and then reflected to prevent loss to the horizontal surface portion. Fig. 34 is a diagram showing a state in which the portion returned to the light source is a returning reflection element and returned to the light source. Fig. 35 is a view showing the configuration of a direct-back type backlight in which three-color cold cathode tubes are disposed at the ends using a three-layer terrace-shaped light guide plate. Fig. 36 is a view showing a principle in which the light guide plate of one layer is used to disperse the reflection surface in the horizontal direction into a terrace shape, and the brightness of the triangular prism portion and the other light guide plate surfaces are aligned with the setting of the aperture ratio toward the upper portion. Fig. 37 is a view showing the principle of conducting the lowermost triangular prism of the triangular prism portion for distributing the light to the direct-down type backlight composed of the three-color cold cathode tube to the upper triangular prism using a three-layer terrace-shaped light guide plate. Figure 38 is a view showing the constitution of a triangular-column portion using a three-layer terrace-shaped light guide plate for distributing light to a direct-down type backlight composed of three-color cold cathode tubes. Figure 39 is a view showing a diffuse reflection point. A diagram of the composition of a conventional light guide plate. Fig. 40 is a view showing the configuration of a conventional light guide plate for reflecting diffused light from a cold cathode tube by a slanted reflecting surface. Fig. 41 is a view showing the configuration of a conventional light guide plate using a slope in the vicinity of a light source as a parameter, and a step of a large m-square of a gentleman's ^ + τ spoon. Fig. 42 is a view showing the configuration of a conventional mirror constructed by a wave mirror of a direct type backlight. φ Fig. 43 is a view showing the construction and the uniform view of the side light for a portable portable machine. . Yuan Line FIG. 44 is a diagram showing the construction of a conventional rear projector. Fig. 45 is a view showing a structure of a conventional light guide plate in which a light guide having a light shielding layer in a stripe width is laminated and a color filter is used. [Description of main component symbols] I: terraced light guide plate _ 2 : sub-pixel 3 : gap 5 : convex reflection surface . 7 : point light source 8 : line light source 9 : parabolic mirror II : concave lens 1 2 . polarizing plate 1323818 1 3 : Transparent substrate 14 4. Liquid crystal layer 15: Parallel light 2 0: Wiring substrate 22: Beam uniformization Concave mirror 23: Positive focal length refractive surface 24: Convex mirror 2 5: Slit 27: Rod-shaped light guide 28: Concave mirror 29: Reflection Face 30: triangular prism 31: mirror 33: total reflection light 34: return reflection element 36: negative focal length refractive surface 3 7 : low refractive index layer 39: light transmissive substance 40: focus 4 3 · liquid crystal panel 51: screen 5 2 . Projection original handle 56: Projection device 58: diffusion material layer 39 1323818 60: diffusion material 61: 稜鏡 62: diffuse reflection point layer 66: light shielding body 40

Claims (1)

七、申請專利範圍: 1、一種液晶顯示照明裝置,其特徵為: 以像素間距將如下設定的凸反射面分散配設於導 . 的底面成梯田狀:依照被照射尺寸w、到被照射面的 t、凸反射面的傾斜寬度d,曲率半徑r為 r = 2 · t · d/(W-d/^ 2) 以藉由以臨界角以上將來自光源的光藉由平行 換手段轉換成平行光並傳導於導光板内的平行光入射 _凸反射面,進行全反射或鏡面反射,擴大光束並反射 照射面之導光板當作構成要素, 藉由使用三色的光源與三層該導光板,將顏色區 光入射到各導光板,以各三層次像素寬度錯開配置導 的傾斜的凸反射面的段差部,使由配置於下層側的導 的凸反射面反射的反射光透過配置於上層側的導光板 反射面的間距間’將來自二色的光源的光照射到顯示 由三個次像素構成的同一像素並進行彩色顯示。 馨 2、如申請專利範圍第1項之液晶顯示照明裝置 中以像素間距分散配設正焦距折射面於導光板的射出 以像素間距分散配置凸反射面於導光板的底面成梯田 依照次像素寬度W、凸反射面至導光板射出面的厚度 反射面寬度d,以r = 2 · 11 · d/(W-d// 2)設定凸反射面 率半徑r, 各層都同一地設定曲率半徑的分布並堆疊三層同 狀的導光板, 光板 距離 光轉 到該 到被 別的 光板 光板 的凸 面的 ,其 面, 狀, :、凸 的曲 一形 41 1323818 、;射出面的正焦距折射面將以臨界角以 該凸反射面並擴大杏击.隹,从认 上入射到 配置於下^ 轉換成平行光,使由 配置於下層侧的導光板的凸反射面反射的 於上層側的導^ 先透過配置 α導先板的凸反射面的間距間, 入射到由三個々榇本姐A L 巴的千仃光 3、如申It像素構成的同—像素並進行彩色顯示。 申…範圍第丨項之液晶顯示照 在以液日曰_示裝置的顯示面當作xy平面時, ,、中 第梯田狀凸反射面為略楔形的梯田 的,配設於正交導先板最厚 曲率半徑,缩乂 的^平面上’增加液晶面板側的 置的凸反:相反側地構成具有梯田狀的段差並分散配 第二梯田狀凸反射面是_晶顯 光板最厚的囟下°卩的梯田狀導 到被昭射面的距: 被配設’以依照被照射尺寸與 破…射面的距離的曲率構成 置的凸反射面, 田狀的1 又差並分散配 以第—梯田狀凸反射面將平 yz平面的y軸方向且由側面人//梯田狀導先板最厚的 J且田彳則面入射的平^ 軸方向並進行方向轉換, …先線擴大光束於X 將被轉換於χ + t + 射面,浐大光击 …擴大先束之光線照射到第二凸反 ::擴大先束於位於略垂直方向的液晶面板並反射,夢 層該導光板將顏色區別的光入射到各導光板,以 射J各導先板以 差部,使由配置於 第二梯田狀凸反射面的段 '田θ&置於下層側的道 4c k 光透過位於三層導光板的上…的凸反射面反射的反射 導先板的上層側的導光板的凸反射面的間 42 距間,以三色 素並進行砮S 自三個光源的光照射到顯示面的同 廷盯知色顯示。 4、如申請直 寻利範圍第1項之液晶顯示照明梦罢 在以液晶顯示萝契 、乃裝置, 、置的顯示面當作xy平面時, 第一梯田壯 n 正交於顯 凸反射面為梯田狀導光板最厚的,配 縮短相反側地椹Γ平面上’增加液晶面板側的曲率半 面, 稱成具有梯田狀的段差並分散配置的凸 第二梯田壯π 凸反射面是以液晶顯不面下部的梯田 光板最厚的χ 、 y干面為基準而被配設,以依照被照射尺 到被照射面的花抓 的距離的曲率具備具有梯田狀的段差並分 置的凸反射面, I轴方向以凸反射面當作負焦距反射面而構成, 弟 梯田狀凸反射面將平行於梯田狀導光板最 yz平面的y軸方向且由側面入射的平行光線擴大光束 轴方向並進行方向轉換的光線越遠離液晶面板側光束 率越高’故藉由形成負焦距反射面於軸方向’與第二 狀凸反射面的X座標無關地控制光束擴大率於液晶像 度而入射於第二梯田狀凸反射面。 5、如申請專利範圍第1項之液晶顯示照明裝置 中以分散配置成梯田狀的凸反射面將在長軸方向傳導 狀的導光體内部的平行光擴大光束’在射出面側成定 而反射於導光棒狀體的側面,更沿著射出面配置以焦 置與該凸反射面共同的正焦距折射面轉換成平行光 一像 其中 設於 徑, 反射 狀導 寸與 散配 厚的 於X 擴大 梯田 素寬 ,其 於棒 間距 點位 的要 43 1323818 素,由棒狀體的側面射出平行光並入射到導光板。 6、 如申請專利範圍第1項之液晶顯示照明裝置,其 中藉由將三色的光依顏色區別照射到三片液晶顯示原稿元 件,以三色錯開配置分散配置於三層導光板内的反射面, 以傾斜的反射面不阻礙行進方向而光束擴大成像素寬度並 在營幕合成三色,進行彩色顯示。 7、 如申請專利範圍第1項之液晶顯示照明裝置,其 中藉由於在X y平面上分散配置反射面成梯田狀的略楔形 導光板的入射面配設顯不原私元件,將顯不原稿元件投影 光照射到梯田狀反射面,在位於xy平面的顯示面擴大晝像 並反射該反射光,可擴大顯示顯示元件畫像於螢幕。 8、 如申請專利範圍第1項之液晶顯示照明裝置,其 中配置具有垂直方向被壓縮扁平化的畫像的細長的形狀的 液晶顯示元件於導光板入射面,藉由分散配置於導光板内 的反射面中的光束擴大功能,由細長的形狀的液晶顯示元 件擴大到畫面尺寸。 9、 如申請專利範圍第1項之液晶顯示照明裝置,其 中透過藉由以每一梯田狀反射面的一反射面投影複數個像 素削減分散配置成梯田狀的段數並擴大反射面尺寸,使模 具製作容易。 1 0、如申請專利範圍第1項之液晶顯示照明裝置,其 中在以顯示面為xy平面,以顯示透射光方向為z軸,配設 投影顯示元件於xz平面,照射平行光於y軸方向的配置 t,藉由一邊以在yz平面上具有梯田狀的段差之第一梯田 44 昭 .射 反 狀 彩 其 尚 的 出 其 體 其 由 之 面 出 其 板 導 形 狀凸反射鏡擴大查德於 &士丄 射 :a象於x軸方向’ -邊進行方向轉換, 面,〇平面上具有梯田狀的段差之第二梯田狀凸反 射,層在位於〇平面的顯示面擴大畫像並反射該 Λ 光板以次像素寬度的條紋間距錯開第二梯田 又差π ’ u二個光源將顯示元件畫像擴大於螢幕並進行 色顯示。 11、如申請專利範圍第1項之液晶顯示昭明裝置, :透明物質使用空氣’以爲形成全反射面而使用的透明 魯刀子材料中的梯田狀反射面的入射側當作對平行光垂直 面,並將平打光入射到全反射面,以透光物質構成以射 侧的面當作對擴大光束的反射光線略垂直的面。 1 2、如申請專利範圍第1項之液晶顯示照明裝置, 中藉由交互堆疊配置略楔形導光板的厚的部分,可使全 的導光板厚度變薄。 1 3、如申請專利範圍第1項之液晶顯示照明裝置, 中在將線光源光進行平行光轉換’藉由傾斜的反射面將 _導光板正下方入射的平行光轉換成平面方向並進行反射 正下方照明型液晶顯示裝置中’藉由將45。的傾斜反射 分割成梯田狀並插入水平部’使導光板厚度比光源的射 寬度還薄。 1 4、如申請專利範圍第1項之液晶顯示照明裝置, 中在設於導光板的正下方方向的光源的孔徑寬度比導光 厚度寬,以4 5。的傾斜反射面將來自該光源的光反射到 光板的平面方向之導光板中’以反射鏡或返回反射元件 45 θ,,倾斜反射部的寬度比導光板厚度寬而分散插入的平 Ρ刀並返回到光源,再度以平行光照射到傾斜反射面。 15如申睛專利範圍第1項之液晶顯示照明裝置,其 .中在正下方照明型液晶顯示裝置的導光板配設三角柱狀的 傾斜反射面,以該三角柱狀的傾斜反射面上部的面積與無 三角柱狀的傾斜反射面的部分的導光板面積的比設定傾斜 的反射面與水平面中的透過孔徑部之面積比,藉由控制反 射到導光板的平面方向的成分與透射到傾斜面的正上方部 鲁的成分,使形成於正下方照明型液晶顯示裝置的三角柱狀 的傾斜反射面上部與其他的導光板面的亮度一致。 1 6、如申請專利範圍第1項之液晶顯示照明裝置,其 中以三角柱狀的傾斜反射面將來自正下方照明的三色的光 源的平行光反射於平面方向,藉由以配設於傾斜反射面的 透射部使入射至二角柱上部及接鄰的三角柱在臨界角以 内,也能照明接鄰的三角柱的上部。 1 7、如申請專利範圍第1項之液晶顯示照明裝置,其 籲中在使凹面鏡的鏡面比拋物線的切線斜率還増大並使來自 光源的光比平行光還擴大光束’俾在凹面鏡開口端中成爲 均勻的光束密度之凹面鏡中’以分割鏡面且比拋物線的切 線斜率還增大的陡Λ肖傾斜鏡面與對向於焦點方向的緩和傾 斜面構成,對向於焦點方向的鏡面的反射光再库收、G ^ π度將返回焦 點的光照射到凹面鏡’並以比拋物線的切線铒.玄#以L t w牛還增大的 陡峭傾斜面的反射光射出。 46VII. Patent application scope: 1. A liquid crystal display illumination device, characterized in that: the convex reflection surface set as follows is dispersed and arranged on the bottom surface of the guide to form a terrace shape according to the pixel pitch: according to the irradiated size w, to the illuminated surface t, the oblique width d of the convex reflecting surface, the radius of curvature r is r = 2 · t · d / (Wd / ^ 2) to convert the light from the light source into parallel light by means of parallel switching by a critical angle or more And conducting the parallel light incident_convex reflective surface in the light guide plate, performing total reflection or specular reflection, expanding the light beam and reflecting the light guide plate of the illumination surface as a constituent element, by using a three-color light source and three layers of the light guide plate, The color zone light is incident on each of the light guide plates, and the stepped portion of the inclined convex reflection surface is arranged so as to be shifted by the three-layer pixel width, and the reflected light reflected by the convex reflection surface disposed on the lower layer side is transmitted through the upper layer side. The distance between the reflecting surfaces of the light guide plates is such that light from two light sources is illuminated to display the same pixel composed of three sub-pixels and displayed in color. In the liquid crystal display illumination device of claim 1, the positive focal length refractive surface is dispersed at a pixel pitch, and the light-emitting plate is dispersed at a pixel pitch to form a convex reflecting surface on the bottom surface of the light guide plate in a terraced manner according to the sub-pixel width. W, the thickness of the convex reflecting surface to the thickness of the light-emitting surface of the light-reflecting surface d, set the convex reflecting surface radius r with r = 2 · 11 · d / (Wd / / 2), and each layer sets the distribution of the radius of curvature Stacking three layers of the same light guide plate, the light plate is separated from the light to the convex surface of the other light plate, and its surface is shaped like: convex curved shape 41 1323818; the positive focal length refractive surface of the exit surface will be The critical angle is increased by the convex reflecting surface and the apricot hitting, and the upper side is guided by the convex reflecting surface of the light guide plate disposed on the lower layer side. By arranging the pitches of the convex reflecting surfaces of the α-leading plates, they are incident on the same pixels composed of three 仃 姐 AL AL 、 、 、 、 、 、 It In the liquid crystal display of the third item of the application range, when the display surface of the liquid display device is used as the xy plane, the middle terrace-shaped convex reflection surface is a slightly wedge-shaped terrace, and is disposed in the orthogonal guide. The thickest radius of curvature of the plate, on the ^ plane of the shrinkage, increases the convex back of the liquid crystal panel side: the opposite side forms a terrace-like step difference and is dispersed with the second terrace-like convex reflecting surface is the thickest of the crystal light-emitting plate距 卩 卩 卩 卩 梯 梯 梯 : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : In the y-axis direction of the plane yz plane, and the direction of the plane axis of the surface of the J-field 最 最 最 最 最 最 , , , , , , , , , , , , , Enlarging the beam on X will be converted to χ + t + plane, 浐大光击...Expanding the first beam of light to the second convex inverse:: Expanding the beam to the liquid crystal panel in the slightly vertical direction and reflecting, the dream layer The light guide plate injects light of different colors into each of the light guide plates to shoot each The first plate is a difference portion, so that the track 4c k placed on the lower layer side of the segment θ & disposed on the second terrace-like convex reflecting surface transmits the reflection of the convex reflecting surface reflected on the upper surface of the three-layer light guiding plate. The distance between the convex reflection surfaces of the light guide plate on the upper layer side of the plate is displayed by the three colors and the light from the three light sources is irradiated onto the display surface. 4. If the liquid crystal display illumination of the first item of the application for the direct search is in the liquid crystal display, the display surface of the display is used as the xy plane, the first terraced n is orthogonal to the convex reflection surface. The thickest of the terrace-shaped light guide plate, with the shortening of the opposite side of the mantle plane, 'increasing the curvature half of the liquid crystal panel side, which is called a terrace-like step and dispersed arrangement of the convex second terraced π-convex reflective surface is liquid crystal The thickest χ and y dry surfaces of the terraced light panel in the lower part of the surface are arranged as reference, and the convex reflection having the terrace-like step and the division is provided in accordance with the curvature of the distance from the illuminated ruler to the flowered surface of the illuminated surface. In the I-axis direction, the convex reflection surface is formed as a negative focal length reflection surface, and the terrace-like convex reflection surface is parallel to the y-axis direction of the most yz plane of the terrace-shaped light guide plate, and the parallel rays incident from the side surface are enlarged in the beam axis direction and The farther the light beam for direction conversion is, the higher the beam rate is from the side of the liquid crystal panel. Therefore, the beam expansion ratio is controlled by the X coordinate of the second convex surface of the second convex reflecting surface by forming the negative focal length reflecting surface in the axial direction. Degree incident on the second convex terraced reflecting surface. 5. In the liquid crystal display illuminating device of the first aspect of the invention, the parallel light-expanding light beam in the light guide body in the long-axis direction is formed on the emission surface side by a convex reflection surface which is arranged in a terrace shape. Reflected on the side surface of the light guiding rod, and disposed along the emitting surface, the positive focal length refractive surface common to the convex reflecting surface is converted into parallel light, and the image is disposed in the diameter, and the reflective guide and the bulk are thicker. X enlarges the terrace width, which is 43 1323818 at the point of the rod spacing, and emits parallel light from the side of the rod and enters the light guide plate. 6. The liquid crystal display illumination device of claim 1, wherein the three-color light is differently illuminated by light to three liquid crystal display original elements, and the three-color staggered arrangement is dispersed and disposed in the three-layer light guide plate. In the face, the inclined reflecting surface does not hinder the traveling direction, the light beam is expanded into a pixel width, and three colors are synthesized in the camp to perform color display. 7. The liquid crystal display illumination device of claim 1, wherein the original surface of the slightly wedge-shaped light guide plate which is arranged in a terrace shape by dispersing the reflective surface on the X y plane is provided with a display element The element projection light is irradiated onto the terrace-shaped reflecting surface, and the image is enlarged on the display surface located on the xy plane, and the reflected light is reflected, thereby expanding the display element image on the screen. 8. The liquid crystal display illuminating device according to claim 1, wherein the liquid crystal display element having an elongated shape in which the image is compressed and flattened in the vertical direction is disposed on the light incident surface of the light guide plate, and the reflection is dispersed in the light guide plate. The beam expanding function in the face is expanded by the elongated liquid crystal display element to the screen size. 9. The liquid crystal display illuminating device of claim 1, wherein the number of segments arranged in a terrace shape and the size of the reflecting surface are reduced by projecting a plurality of pixels on a reflecting surface of each of the terrace-shaped reflecting surfaces. Mold making is easy. The liquid crystal display illumination device of claim 1, wherein the display surface is an xy plane, the direction of the transmitted light is z-axis, the projection display element is disposed on the xz plane, and the parallel light is irradiated in the y-axis direction. The configuration t, by the side of the first terraced field with a terrace-like step in the yz plane, the singularity of the singularity of the surface of the slab & 丄 丄 : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : The light plate is shifted by the stripe pitch of the sub-pixel width by the second terrace and the difference is π'. The two light sources expand the display element image on the screen and display the color. 11. The liquid crystal display illumination device of claim 1 is as follows: the transparent substance uses air 'the incident side of the terrace-shaped reflecting surface in the transparent knive material used for forming the total reflection surface is regarded as the vertical plane of the parallel light, and The flat light is incident on the total reflection surface, and the light-transmitting material is formed on the side of the radiation side as a plane which is slightly perpendicular to the reflected light of the enlarged light beam. 1. In the liquid crystal display lighting device of claim 1, in which the thick portion of the slightly wedge-shaped light guide plate is alternately stacked, the thickness of the entire light guide plate can be made thin. 1 3. In the liquid crystal display illumination device of claim 1, in which the line source light is converted into parallel light, the parallel light incident directly under the light guide plate is converted into a plane direction and reflected by the inclined reflection surface. In the under-lighting type liquid crystal display device, 'by 45. The oblique reflection is divided into a terrace shape and inserted into the horizontal portion' so that the thickness of the light guide plate is thinner than the radiation width of the light source. In the liquid crystal display illumination device of claim 1, the aperture width of the light source disposed directly under the light guide plate is wider than the light guide thickness by 45. The inclined reflecting surface reflects the light from the light source into the light guide plate in the plane direction of the light plate' by the mirror or the return reflecting element 45 θ, and the width of the inclined reflecting portion is wider than the thickness of the light guiding plate to disperse the inserted flat boring tool and Return to the light source and illuminate the oblique reflection surface again with parallel light. [15] The liquid crystal display illumination device of claim 1, wherein the light guide plate of the direct illumination type liquid crystal display device is provided with a triangular columnar inclined reflection surface, and the area of the triangular columnar inclined reflection surface portion is The ratio of the area of the light guide plate of the portion of the inclined reflecting surface without the triangular column is set to the area ratio of the reflecting surface of the inclined surface to the transparent opening portion in the horizontal plane, by controlling the component reflected in the plane direction of the light guiding plate and the positively transmitted to the inclined surface The component of the upper portion is such that the triangular prism-shaped oblique reflecting surface portion formed in the direct-lit illuminating liquid crystal display device matches the brightness of the other light guiding plate surface. The liquid crystal display lighting device of claim 1, wherein the parallel light of the three-color light source illuminated directly below is reflected in a plane direction by a triangular prism-shaped inclined reflecting surface, and is disposed in the oblique reflection The transmissive portion of the surface allows the entrance to the upper portion of the gusset and the adjacent triangular prism to be within the critical angle, and can also illuminate the upper portion of the adjacent triangular prism. 1. The liquid crystal display illumination device of claim 1, wherein the mirror surface of the concave mirror is larger than the tangential slope of the parabola and the light from the light source is further enlarged than the parallel light '俾 in the open end of the concave mirror In a concave mirror that becomes a uniform beam density, a steeply inclined mirror surface that splits the mirror surface and increases in slope of the tangent to the parabola, and a gently inclined surface that opposes the focus direction, and the reflected light of the mirror surface that faces the focus direction The collection, G ^ π degree, illuminates the light returning to the concave mirror' and emits the reflected light of the steep inclined surface which is larger than the tangential line of the parabola. 46
TW98133842A 2009-10-06 2009-10-06 Liquid crystal display lighting apparatus TWI323818B (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111273486A (en) * 2020-03-25 2020-06-12 京东方科技集团股份有限公司 Light collimation device, backlight module and display panel

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111273486A (en) * 2020-03-25 2020-06-12 京东方科技集团股份有限公司 Light collimation device, backlight module and display panel
US11215874B2 (en) 2020-03-25 2022-01-04 Boe Technology Group Co., Ltd. Light collimation device, backlight module and display panel
CN111273486B (en) * 2020-03-25 2022-05-13 京东方科技集团股份有限公司 Light collimation device, backlight module and display panel

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