TW201109786A - Liquid crystal display device - Google Patents

Liquid crystal display device Download PDF

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Publication number
TW201109786A
TW201109786A TW99130153A TW99130153A TW201109786A TW 201109786 A TW201109786 A TW 201109786A TW 99130153 A TW99130153 A TW 99130153A TW 99130153 A TW99130153 A TW 99130153A TW 201109786 A TW201109786 A TW 201109786A
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Taiwan
Prior art keywords
liquid crystal
pixel
region
pixel region
alignment
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TW99130153A
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Chinese (zh)
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TWI354833B (en
Inventor
Norio Koma
Kazuhiro Inoue
Kazuyuki Maeda
Masaaki Koga
Masayuki Kametani
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Sanyo Electric Co
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Priority claimed from JP2004347905A external-priority patent/JP2006011362A/en
Application filed by Sanyo Electric Co filed Critical Sanyo Electric Co
Publication of TW201109786A publication Critical patent/TW201109786A/en
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Publication of TWI354833B publication Critical patent/TWI354833B/en

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Abstract

Provided is a liquid crystal display device comprises a plurality of pixels, and vertical alignment liquid crystal is sealed between a first substrate having a pixel electrode and a second substrate having a common electrode, wherein, each pixel has a shape where the length along the column direction is longer than the length along the row direction; each pixel is divided into a first pixel region and a second pixel region in different area size by a boundary line which is configured to a V-shape along the row direction; one end of the first pixel region is cut into the second pixel region; and a preferential viewing angle of the first pixel region and a preferential viewing angle of the second pixel region are different.

Description

201109786 六、發明說明: 【發明所屬之技術領域】 本發明係有關在具有像素電極之第一基板與具、 電極之第二基板間封入有垂直配向型液晶的液晶颟=通 置。 y、裒 【先前技術】 液晶顯示裝置(以下稱LCD)具備薄型且低消費電 特徵,現在被廣泛運用於電腦顯示器、可攜式資訊機j 之顯示器中。該種LCD,係在一對基板間封入液晶,益等 形成於各個基板之電極控制位於基板間之液晶之^ η藉由 行顯示者,該LCD與CRT(陰極射線管)顯示器、電向而進 (electroluminescence,以下稱£L)顯承毋從 激發光 丨、盗等不同,ώ 原理上不能自身發光,因此為了對觀察者 由於 光源。 考顯-圖像而需要 仍冗,隹牙边又七⑶τ,你徠用通明電極作為形 各基板之電極’而在液晶顯不面板後面及側面 ' ; 以液晶面板控制該光源光之透過量,因此 ’、 4 使疋周圍光線 季乂暗,也可明亮地顯示。但是,由於經常 ^ ’原、點亮進行 顯不,因此會有無法避免由於光源產生 U 之之電力消耗之特 性’或是如同在白天屋外之光線非常強之 . ΤΟ兄下,無法確 保充分之對比度之特性。 另一方面,在反射盤LCD中’將太陽、室内燈等之外 光採用為光源,將入射至液晶面板之這也闲阁μ ^ 〜同圍先,藉由形 成於非觀察面側之基板之反射電極進行反射。然後, 317049D1D1 3 201109786 個像素控制入射至液晶層而由反射電極反射後之光而從液 晶面板射出的射出光量’從而進行顯示。該種反射型LCD 由於採用外光作為光源’因此與穿透型LCD不同,沒有由 於光源之電力消費,而具有非常低之低消費電力,並且當 在屋外等周圍明亮之情況,可獲得充分之對比度,相反地, 在無外光之情況下,具有無法看到顯示之特性。 於此,最近係提出一種在屋外可容易觀視,且在暗處 也可觀察之顯示器’並受到矚目,例如在曰本專利早期公 開平11-101992號公報、日本專利早期公開2003-255399 號公報等所揭示之具備反射功能與光穿透功能之半穿透型 LCD。該穿透型LCD係藉由在一像素區域内設置穿透區域與 反射區域’而謀求同時具有穿透功能及反射功能。 如此,由於能夠同時具有屋外之識認性、以及昏暗情 況下之識認性’因此採用前述之半穿透型LCD作為例如可 攜式之資訊機器等之顯示器係非常有用。 但是’在該可攜式資訊機器等之中,所設想之觀察狀 態有多樣’為了實現即使是多種觀察狀態(特別是各種觀察 角度)都可進行咼品質之顯示,必須擴大視野角度。 此外,由於半穿透性LCD係將一像素分割為穿透區域 與反射區域,從而實現半穿透性,因此1個像素份之穿透 特性、反射特性係低於穿透型LCD或是反射型LCD,因此 為了提咼各個顯示區域(穿透區域、反射區域)之顯示品 質’無論疋哪一區域都必須有更尚的對比度。 但是,關於半穿透型LCD,還僅停留於同時具備穿透 317049D1D1 4 201109786 '功能與反射功能之構造的改良,而尚未為了提高顯示品質 • 而嘗試野角度之擴大、對比度之提高等。 質 【發明内容】 本發明係以實現半穿透型LCD、彩色Lc 質為目的。 不口口 (解決問題的手段) 特徵本發明可實現如前所述之半穿透型LCD,並具備如下 •在一種液晶顯示裝置’具備複數個像素,並 八有像素電極之第—基板與具有共通電極 入有垂直配向型液晶,其中,各像素的形狀= :度^方向長度長;各像素補由沿列方向延伸、f 第㈣面積相異的第—像素區域與 一素區域,前述第一像素區域的端係切入前述第二傻 =域而形成;前述第-區域的優先視角與 _區域的優先視角不同。 木1豕| 在本發明的其他紐巾,係為—種液晶顯 =像素區域的優先視角係垂直於行方向;前述第二: 素區域的優先視角係垂直於列方向。 在本發賴其他紐+,料—_晶顯 第:素區域中,液晶配向方向被分割成為 在前述第二像素區域中,液晶配向方向被分. 成為兩個不同區域。 在本發明的其他態樣中,係為一種液晶顯示裝置,在 317049D1D1 5 201109786 二述第像素區域中,液晶配向方向被控制成朝向垂直於 方向之方向’在前述第二像素區域中,液晶配向方向被 控制成朝向垂直於列方向之方向。 、在本發明的其他態樣令,係為一種液晶顯示裝置,前 述第像素區域的面積比前述第二像素區域的面積小。 在本發明的其他態樣卜係為一種液晶顯示裝置,呈 2複數個像素,並在具有像素電極之第—基板與具有共通 電極之第二基板間,封入有垂直配向型液晶,其令,各像 =的形狀係行方向長度比列方向長度長;各像素係藉由沿 • ^向延伸的分界線而分割成面積相異的第一像素區域與 f-像素區域;在前述第—像素區域中,液晶配向方向被 分割成為四個不同區域’並且,在前述第二像素區域中, 液晶配向方向被分割成為四個不同區域。 、、在本發明的其他態樣中,係為一種液晶顯示裝置,前 述第-像素區域中的四個配向方向與前述第二像素區域中 的四個配向方向相同。 在本發明的其他態樣令’係為一種液晶顯示裝置,前 述第-像素區域的四個區域與前述第二像素區域的四個區 域中的液晶的優先視角相同。 在本發明的其他態樣令,係為一種液晶顯示裝置,前 述第一像素區域的面積比前述第二像素區域的面積小。 【實施方式】 下面使用附圖說明本發明之較佳實施形態(下面稱為 317049D1D1 6 201109786 [實施形態l] 第1圖表示作為本實施形態之半穿透型LCD而使用半 牙透型主動矩陣(Active matrix)LCD時之基本剖面構成。 本實施形態之半穿透型LCD係具有複數像素,且將在相互 的相對面側形成有第i電極200、第2電極32〇之第工及 第2基板以其間夾有液晶層4〇〇之方式予以貼合而構成 者’同時在各像素區域内形成有穿透區域21〇血反射區域 220 〇 ’、 採用具有負介電率異向性之垂直配向型液晶作為液晶 層400,且在第2基板側或第1基板設置有用於將丨個像 素區域内分割為複數配向區域之配向控制部5〇〇(配向分割 P )配向控制部5 0 0係例如由如第1圖所示之向液晶層 4〇〇突出之突起部51〇、傾斜部52〇、以及在第丨圖中由像 素電極200的間隙構成之無電極部等所構成(且體如 所述)。 八 第1及第2基板1〇〇、300使用玻璃等透明基板。在第 1基板100側形成有使用氧化銦錫(ITO,Indiuro Tin de)氧化銦鋅(IZO,Indium Zinc Oxide)等透明導電 ! 生金屬氧化物之在每一像素之個別圖案的像素電極別〇而 作為第1電極、以及與該像素電極200相連接之薄膜電晶 1關元件(未圖示。參閱後述第5圖)。在覆蓋像素電 極200之第1基板100之全面係形成有垂直配向型的配向 膜260。該配向膜26〇例如使用聚醯亞胺等,在本實施形 L中知用無摩擦型(rubbingless),使液晶的初期配向(電 317049D1D1 7 201109786 壓非施加狀態下的配向)垂直於膜的平面方向。再者,藉由 第5圖所示之結構(具體如後面所述),可在1個像素電極 200的形成區域内設置僅由上述透明電極構成之透明區域 210、以及形成有與上述透明電極層疊形成之反射膜或反射 電極之反射區域220。 在與該種第1基板1〇〇之間夾有液晶層400而貼合之 第2基板300中,在與該液晶之相對面側,首先將R、〇、 B彩色濾光層330r ' 330g、330b形成於對應的預定位置。 再者’在各彩色濾光層330r、330g、330b的間隙(像素區 域的間隙)中設置用於防止像素間的漏光之遮光層(在此為 *累色彩色濾光層)330BM。 彩色濾光層330r、330g、330b上形成有由光穿透性材 料構成之間隙調整部340,以使在與各像素的反射區域22〇 目對之區域,其液晶層的厚度(液晶盒間隙)dr與在穿透區 域21〇的液晶層的厚度(液晶盒間隙)dt相比小期望的值 Qr<dt)。該間隙調整部34〇的厚度在入射光通過液晶層 /〇 "人之穿透區域210與通過2次之反射區域220中, 二=對應於為得到最適合的穿透率、反射率而需要之液晶 f度d之不同情形而設定者。因此,例如,決定液晶層 度d ’俾使在未設置間隙調整部34〇之穿透區域21〇 具侍:最,合的穿透率’而在反射區域220中,藉由設置 f有期望厚度之間㈣整部340,從而可得職穿透區域 10小之液晶層的厚度d。 以覆蓋具有上述間隙調整部340之第2基板300之全 8 317049D1D1 201109786 ==成::tr共通的電極(共通電極)32°’而 可使用™、極32G與上述像素電極200相同, 寺透明導電性金屬氧化物形成。 在本貫施形態φ , 部別,作為將^個俊t該共通電極320上’係形成突起 而形成配向方向=區域内躲晶配向方向予以分割 突起部⑽向液晶個區域之配向控制部500。該 性,在此可將絕緣“例:起’可Γ為導電性也可為絕緣 案加以使用。並且1:丙稀酸糸列樹脂等形成期望圖 的穿透區域2心及^部51G分別形成於各像素區域内 Λ及反射區域220。 型之起I 51°及共通電極32°須形成有無摩擦 、 〃為與第1基板偏目m直配向型。 =逑,配向物使液晶配向於與其膜平面方向垂直 ㈣部,位置係形成有反映突起部 」 因此,在突起部510之形成位置,液曰 對於覆錢起部51G之配向膜26之斜面而配向於垂直 。L並以該突起部51〇為界分割液晶之配向方向。並且, ^形心中,使設置於第2基板側之上述間隙調整部 。之側面傾斜為斜錐形,覆蓋間隙調整部340之上方之 260也延續該斜面而形成有斜面。液晶在該斜面也 ::4成與斜面垂直之方向’而間隙調整部34〇之斜面也 作為配向控制部500之用。 在第1圖所示之半穿透型LCD中,在第1基板100之 (光源600側)設置有直線偏光板(第1偏光板)112、以 317049D1D1 9 201109786 及由λ / 4相位差板及λ / 2相位差板之組合構成之廣波長 帶域又/ 4板(第1相位差板)111,由該直線偏光板112與 相位差板111構成廣波長帶域圓偏光板11〇。 在第2基板300之外侧(觀察側)設置具有負的折射率 異向性之相位差板310作為光學補償板,復設置有由又/4 相位板及λ /2相位板之組合構成之廣波長帶域^ /4板(第 2相位差板)111、以及直線偏光板(第2偏光板)112,與第 1基板側相同,由該直線偏光板112與相位差板構成 廣帶域圓偏光板110。在此,該等光學元件之配置關係可 如第1圖之下部之一個例子所示,將第1偏光板之軸配置 為45° ’第1個λ /4板之遲相軸配置為90。,第2個;I /4 板之遲相軸配置為180。’第2偏光板之軸配置為135。。 從光源600射出、且穿透第1基板1〇〇侧之直線偏光 板112而沿該偏光板112之偏光軸方向之直線偏光係藉由 在第1個;1/4板111使其相位差偏離又/4而成為圓偏光。 在此’在本實施形態中,為了至少對波長不同之r、G、β 中任意之成分也確實設為圓偏光,以提高液晶盒中之光之 利用效率(穿透率),而使用λ/4相位板與λ/2相位板雙方 作為廣波長帶域λ/4板ill ^所得到之圓偏光在穿透區域 210穿透像素電極2〇〇而入射至液晶層400。 在本實施形態之半穿透型LCD中,如上所述,使用具 有負介電率異向性(△ ε <0)之垂直配向型液晶於液晶層 400 ’並且使用垂直配向型配向膜“ο。 因此’在電壓非施加狀態下,係分別配向於垂直於配 10 317049D1D1 201109786 向膜26G之平面方向之方向,隨著施加電壓增大,液晶之 長軸方向係以與形成於像素電極2〇〇與共通電極卿之間 之電场垂直(平行於基板之平面方向)的方式傾斜 。在未向 液晶層400施加電壓時,在液晶層400中偏光狀態不會變 化而直接以圓偏光到達第2基板綱,在第2個入/4板 111消除圓偏光而成為直線偏I此時,因係將第2偏光 板112配置成使其與來自》2個λ/4板111之直線偏光之 方向垂直’故該直線偏光不能穿透與第i偏光板ιΐ2為垂 ♦直之方向之穿透軸(偏光軸)之第2偏光板112,使顯示變 為黑色。 向液晶層400施加電壓後,液晶層400使入射之圓偏 光產生相位差’例如成為逆轉之圓偏光、橢圓偏光、直線 偏光,藉由在第2個;1/4板lu對於所得到之光進一步偏 移;1/4相位,從而成為直線偏光(平行於第2偏光板之穿 透軸)、橢圓偏光、圓偏光,這些偏光具有沿第2偏光板 ❿112之偏光軸之成分,對應該成分之光從該第2偏光板112 向觀察側射出,作為顯示(白色或中間色調)而被識認。 再者,相位差板310為負延遲器(negauVe retarder), 能夠提升從斜向觀視LCD時的光學特性,而提高視角。再 者,也可取代該負延遲器(310)與上述λ/4板111而使用 具有該雙方功能之一片2軸相位差板,由此可實現LCD之 薄型化及穿透率之提高。 在本實施形態中,如上所述,藉由間隙調整部340, 將實質上控制光之穿透率之液晶層400之厚度(液晶盒間 317049D1D1 11 201109786 隙)d設為在穿透區域210與反射區域220不同之期望之間 隙。主要的原因是因為,在穿透區域210係對從設置於LCD 背面側(在第1圖中為第1基板1〇〇側)之光源穿透液 晶層400而從第2基板300侧向外部射出之光量(穿透率) 進行控制,從而進行顯示,而在反射區域220係將從LCD 之觀察側向液晶層400入射之光藉由設置於像素電極200 之形成區域内之反射膜予以反射,並再次穿透液晶層400 從第2基板側向觀察側射出之光量(LCD之反射率)進行控 制’從而進行顯示,光之液晶層之穿透次數不同。即,因 在反射區域220 ’光係穿透液晶層400兩次,故其液晶盒 間隙dr必須設定成比穿透區域210之液晶盒間隙dt小。 在本實施形態中’如第1圖所示,藉由將期望厚度之間p+、 調整部340僅設置於各區域之反射區域220,從而達成上 述dr<dt。間隙5周整部340只要具有光穿透性且可形成期 望厚度外,沒有其他特殊限定’例如可採用也作為平挺化 絕緣層等使用之丙稀酸系列樹脂等。 在如上所述間隙調整部340之側面作為配向控制部 500之一部分(傾斜部520)使用時,必須至少其斜錐角相對 於基板平面不刻90度。原因係為如果斜錐角在90度以上, 液晶之配向就會在該間隙調整部340之側面產生混亂,並 且形成於間隙調整部340上之共通電極32〇、配向膜26〇 之覆蓋也會變得不充分。此外,間隙調整部340之側面對 顯示本身沒有作用’如果斜錐角過小的話,就會使間隙調 整部340之側面面積增大’致使像素之開口率、尤其是期 317049D1D1 12 201109786 •望更加提高亮度之反射區域之p和率下降。由此 整部340之側面之斜錐w好為錢上層之第謂、 配向膜;260之覆蓋性下降,且可進行液晶之配向分割,並 率下降Μ之角度。具體地說較宜為30度至8°度 斜錐角之間_部 隙調啓山 饮先釗之上述丙稀酸樹脂。然後,間 合開始劑' I聚:整劑加入丙稀酸樹脂中之聚 置特性等加以調整,有r合製造條件、曝光裝 調整部340之側面為順斜錐成2 =順斜錐角。為使間隙 如,亦可_由除如此調整含有材料外,例 ^ ^ fl〇W> 錢:調整部⑽之表面附近之 氧氣較少,因此X合 也,因離表面較遠之基板側 故顯影時易於去除^抑制效果而持續聚合引起之硬化, 寬度越窄之Μ斜錐。旦化絕緣層38之表面側,形成越向上 曝光時之朵夕Μ 裝置等_,利:、也利用曝光裝置,例如在近接曝光 間隙調整部形成區域==果而在間隙調整部340以 切體流動中二去=形柄錐。 ,仏·。束後,藉由例如以80。(:至]80 317049DID1 13 201109786 °C之溫度、進行烘烤1至2〇min(例如以12(TC、8min),從 而使間隙5周整部340之上面及側面熔融,使表面平滑化, 同時,藉由側表面依存於熔化材料自身所具有之表面張力 之形狀變化’而形成順斜錐。 在此,用於間隙調整部等之有機材料,係公知有表示 對曝光光源之g線(436nm)、h線(405)nm、i線(248nm)之 靈敏度等之材料,對i線具有靈敏度之有機材料其斜錐角 般多在90度以上(逆斜錐)。因此,在本實施形態中,間 隙调整部之材料採用對g線、h線具有靈敏度,容易形成 順斜錐之丙稀酸系列樹脂。 在本實施形態中,在一像素區域内,在穿透區域21〇 與反射區域220改變液晶層之厚度d,同時,分別在波長 不同之R、G、B用像素改變該液晶層之厚度d(但,也可根 據LCD之特性在R、G、B設定共通之間隙)。在第j圖之例 子中’藉由分別形成於第2基板300側之R、G、B之彩色 濾光層330r、330g、330b之厚度分別予以改變,而得以實 現將R、G、B全部之間隙d。不限於改變彩色濾光層之厚 度之構成,也可在穿透區域210亦設置上述間隙調整部 340’在每一 R、G、B之穿透區域21〇與反射區域22〇改變 該間隙調整部340之厚度。並且,在全部R、G、B中,即 使不使液晶層之厚度d互不相同,也可依據LCD之特性, 例如使G用與B用為相同液晶層厚度,而僅R用與其他2 色不同之厚度’也可僅改變B用的d。 第2圖係顯示為使R、G、B用像素為不同之間隙之其 317049D1D1 14 201109786 他構成(在第2圖中,料rt 在第2圖之構成中,^與第1圖相同之構成不再贅述)。 而在第1基板刚側將开,2基板側不改變R、G、B之間隙, 絕緣層38之厚产以^成於像素電極2〇0下層之平坦化 之厚度之方法有例如、B減。改變平故絕緣層38 -或複數個半曝光遮I使用對應於目標厚度之開口量之單 料予以曝光,而不㈣/將含有感光材料之平坦化絕緣材 R後音且古尤^ 追加特別之製程即可形成在每一 R、G、BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a liquid crystal 颟=interval in which a vertical alignment type liquid crystal is sealed between a first substrate having a pixel electrode and a second substrate having an electrode and an electrode. Y, 裒 [Prior Art] Liquid crystal display devices (hereinafter referred to as LCDs) have thin and low power consumption characteristics, and are now widely used in displays for computer monitors and portable information devices. The LCD is formed by encapsulating liquid crystal between a pair of substrates, and the electrodes formed on the respective substrates control the liquid crystal between the substrates by the line display, the LCD and the CRT (cathode ray tube) display, and the electric direction. Electroluminescence (hereinafter referred to as £L) is different from excitation, thief, etc., and in principle, it cannot emit light by itself, so it is used for the observer due to the light source. It takes a lot of time to test the image, and it is still seven (3) τ. You use the bright electrode as the electrode of each substrate 'on the back and side of the liquid crystal display panel'; the liquid crystal panel controls the light transmission of the light source. Therefore, ', 4 makes the light around the 乂 dark, and can also be displayed brightly. However, since it is often [original, lighting, etc., there is a danger that the power consumption of the U due to the light source cannot be avoided" or that the light outside the house is very strong during the daytime. The characteristics of contrast. On the other hand, in the reflective disk LCD, 'the outside light such as the sun or the indoor lamp is used as the light source, and the light incident on the liquid crystal panel is also vacant, and the substrate is formed on the non-observation side. The reflective electrode reflects. Then, 317049D1D1 3 201109786 pixels control the amount of emitted light that is incident on the liquid crystal layer and reflected by the reflective electrode and emitted from the liquid crystal panel. This kind of reflective LCD uses external light as a light source'. Therefore, unlike a transmissive LCD, it has no low power consumption due to power consumption of the light source, and can be obtained when it is bright around the house. Contrast, on the contrary, has the property of not being able to see the display in the absence of external light. Herein, a display which can be easily viewed outside the house and which can be observed in a dark place has recently been proposed, and has been attracting attention, for example, Japanese Patent Laid-Open No. Hei 11-101992, Japanese Patent Laid-Open Publication No. 2003-255399 A transflective LCD having a reflective function and a light penetrating function disclosed in the publication. The transmissive LCD achieves both a penetrating function and a reflecting function by providing a transmissive region and a reflective region ′ in a pixel region. In this way, it is useful to use the above-described transflective LCD as a display system such as a portable information device, since it can have both the visibility of the outside and the visibility in the dark. However, in the portable information device or the like, the assumed observation state is various. In order to realize the display of the 咼 quality even in various observation states (especially various observation angles), it is necessary to enlarge the viewing angle. In addition, since the semi-transparent LCD system divides a pixel into a transmissive area and a reflective area to achieve semi-transparency, the penetration characteristics and reflection characteristics of one pixel are lower than that of the transmissive LCD or reflection. In order to improve the display quality of each display area (transparent area, reflective area), it is necessary to have a higher contrast regardless of the area. However, with respect to the transflective LCD, it is only possible to improve the structure of the function and reflection function of the 317049D1D1 4 201109786, and it is not yet necessary to increase the display angle and improve the contrast. SUMMARY OF THE INVENTION The present invention is directed to achieving a transflective LCD and a color Lc. BACKGROUND OF THE INVENTION The present invention can realize a semi-transmissive LCD as described above, and has the following structure: a liquid crystal display device having a plurality of pixels and having a plurality of pixel electrodes The common electrode has a vertical alignment type liquid crystal in which the shape of each pixel is longer than: the length of the direction is long; each pixel is complemented by a first pixel region and a single region extending in the column direction, and f (4) is different in area The end of the first pixel region is formed by cutting into the second silly= domain; the priority viewing angle of the first region is different from the priority viewing angle of the _region. In the other inventions of the present invention, the priority viewing angle of the pixel region is perpendicular to the row direction; the preferential viewing angle of the second region is perpendicular to the column direction. In the other luminescence, the liquid crystal alignment direction is divided into two in the second pixel region, and the liquid crystal alignment direction is divided into two different regions. In another aspect of the present invention, in a liquid crystal display device, in a pixel region of 317049D1D1 5 201109786, the liquid crystal alignment direction is controlled to be in a direction perpendicular to the direction 'in the foregoing second pixel region, liquid crystal alignment The direction is controlled to be oriented in a direction perpendicular to the column direction. According to still another aspect of the present invention, in a liquid crystal display device, an area of the pixel region is smaller than an area of the second pixel region. In another aspect of the present invention, a liquid crystal display device has two or more pixels, and a vertical alignment type liquid crystal is sealed between a first substrate having a pixel electrode and a second substrate having a common electrode. The shape of each image = the length of the row direction is longer than the length of the column direction; each pixel is divided into a first pixel region and an f-pixel region having different areas by a boundary line extending along the ^ ^ direction; In the region, the liquid crystal alignment direction is divided into four different regions', and in the second pixel region, the liquid crystal alignment direction is divided into four different regions. Further, in another aspect of the invention, a liquid crystal display device is characterized in that four alignment directions in the first pixel region are the same as four alignment directions in the second pixel region. The other aspect of the present invention is a liquid crystal display device in which the four regions of the first-pixel region and the liquid crystal regions of the four regions of the second pixel region have the same preferential viewing angle. In another aspect of the invention, a liquid crystal display device is characterized in that an area of the first pixel region is smaller than an area of the second pixel region. [Embodiment] Hereinafter, a preferred embodiment of the present invention will be described with reference to the drawings (hereinafter referred to as 317049D1D1 6 201109786 [Embodiment 1]. FIG. 1 shows a semi-transmissive active matrix as a semi-transmissive LCD of the present embodiment. (Active matrix) The basic cross-sectional structure of the LCD. The semi-transmissive LCD of the present embodiment has a plurality of pixels, and the first and second electrodes 32 and 32 are formed on the opposite surface sides of each other. 2 The substrate is bonded so as to sandwich the liquid crystal layer 4 其 therebetween. At the same time, a transparent region 21 is formed in each pixel region, and a blood-reflecting region 220 〇 ' is formed, and a negative dielectric anisotropy is used. The vertical alignment type liquid crystal is used as the liquid crystal layer 400, and the alignment control unit 5 (the alignment division P) alignment control unit 50 for dividing the plurality of pixel regions into the plurality of alignment regions is provided on the second substrate side or the first substrate. 0 is constituted, for example, by a projection 51 〇〇 protruding from the liquid crystal layer 4 as shown in FIG. 1 , an inclined portion 52 〇 , and an electrodeless portion composed of a gap of the pixel electrode 200 in the second diagram ( And as described A transparent substrate such as glass is used for the first and second substrates 1 and 300. On the first substrate 100 side, indium tin oxide (ITO, Indium Zinc Oxide) or the like is used. Transparent conductive! The raw metal oxide is a first electrode and a thin film transistor 1 connected to the pixel electrode 200 (not shown.) A vertical alignment type alignment film 260 is formed on the entire first substrate 100 covering the pixel electrode 200. The alignment film 26 is made of, for example, polyimide or the like, and the frictionless type is used in the present embodiment L. (rubbingless), the initial alignment of the liquid crystal (electrical 317049D1D1 7 201109786 alignment in the non-applied state) is perpendicular to the plane direction of the film. Furthermore, by the structure shown in FIG. 5 (specifically as described later), A transparent region 210 composed only of the transparent electrode and a reflective region 220 formed with a reflective film or a reflective electrode formed by laminating the transparent electrode are provided in a formation region of one pixel electrode 200. In the second substrate 300 in which the liquid crystal layer 400 is sandwiched between the first and second substrates 300, the R, 〇, and B color filter layers 330r' 330g and 330b are first formed in the corresponding predetermined surface on the side opposite to the liquid crystal. Further, 'a light-shielding layer (here, a *-color color filter layer) 330BM for preventing light leakage between pixels is provided in a gap (a gap of a pixel region) of each of the color filter layers 330r, 330g, and 330b. The color filter layers 330r, 330g, and 330b are formed with a gap adjusting portion 340 made of a light-transmitting material so that the thickness of the liquid crystal layer (the cell gap) in the region facing the reflective region 22 of each pixel The dr is smaller than the thickness (cell gap) dt of the liquid crystal layer in the penetration region 21A by a desired value Qr < dt). The gap adjusting portion 34 has a thickness in which the incident light passes through the liquid crystal layer/〇" human penetration region 210 and passes through the secondary reflection region 220, and the second corresponds to obtaining the most suitable transmittance and reflectance. The required liquid crystal f degree d is set differently. Therefore, for example, it is determined that the liquid crystal layer degree d '俾 is such that the penetration area 21 of the gap adjustment portion 34 is not provided: the most suitable transmittance" and in the reflection area 220, there is an expectation by setting f Between the thicknesses (4) the entire portion 340, so that the thickness d of the liquid crystal layer of the small penetration region 10 can be obtained. It is possible to use TM and pole 32G in the same manner as the above-described pixel electrode 200 to cover the entire electrode of the second substrate 300 having the gap adjusting portion 340, which is the same as the above-mentioned pixel electrode 200. A conductive metal oxide is formed. In the present embodiment, the φ and the portion are arranged to form a protrusion on the common electrode 320 to form an alignment direction=the direction in which the alignment direction is in the region, and the alignment control unit 500 is divided into the liquid crystal regions. . In this case, the insulation "Example: From" can be used as the conductivity or the insulation case. And 1: the acrylic acid matrix resin and the like can form the desired region of the penetration region 2 and the portion 51G respectively The Λ and the reflective region 220 are formed in each of the pixel regions. The type I 51° and the common electrode 32° must be formed with or without friction, and the 〃 is aligned with the first substrate. The alignment is such that the alignment aligns the liquid crystal to the liquid crystal. The position is perpendicular to the plane direction of the film (four), and the position is formed to reflect the protrusion. Therefore, at the position where the protrusion 510 is formed, the liquid helium is aligned perpendicular to the slope of the alignment film 26 of the money-raising portion 51G. L divides the alignment direction of the liquid crystal by the protrusion 51〇. Further, in the centroid, the gap adjusting portion provided on the second substrate side is provided. The side surface is inclined to a tapered shape, and the upper portion 260 covering the gap adjusting portion 340 also continues the inclined surface to form a slope. The liquid crystal is also ::4 in the direction perpendicular to the inclined surface, and the slope of the gap adjusting portion 34 is also used as the alignment control unit 500. In the transflective LCD shown in Fig. 1, a linear polarizing plate (first polarizing plate) 112, 317049D1D1 9 201109786, and a λ / 4 phase difference plate are provided on the first substrate 100 (on the side of the light source 600). The wide-wavelength band and the four-plate (first phase difference plate) 111 which are combined with the λ / 2 phase difference plate constitute a wide-wavelength-region circular polarizing plate 11 from the linear polarizing plate 112 and the phase difference plate 111. A phase difference plate 310 having a negative refractive index anisotropy is provided on the outer side (observation side) of the second substrate 300 as an optical compensation plate, and a wide combination of a /4 phase plate and a λ/2 phase plate is repeatedly provided. The wavelength band ^ / 4 plate (second phase difference plate) 111 and the linear polarizing plate (second polarizing plate) 112 are the same as the first substrate side, and the linear polarizing plate 112 and the phase difference plate constitute a wide band circle. The polarizing plate 110. Here, the arrangement relationship of the optical elements can be as shown in an example of the lower part of Fig. 1, and the axis of the first polarizing plate is arranged at 45°. The retardation axis of the first λ /4 plate is arranged at 90. , the second; the I/4 board has a slow phase axis configuration of 180. The axis of the second polarizing plate is 135. . The linear polarizing plate 112 that is emitted from the light source 600 and penetrates the linear polarizing plate 112 on the side of the first substrate 1 and in the direction of the polarization axis of the polarizing plate 112 is made to have a phase difference in the first 1/4 plate 111. It deviates from /4 and becomes circularly polarized. Here, in the present embodiment, in order to improve the utilization efficiency (penetration ratio) of light in the liquid crystal cell, at least for any of r, G, and β having different wavelengths, it is possible to use λ. The circularly polarized light obtained by both the /4 phase plate and the λ/2 phase plate as the wide-wavelength band λ/4 plate ill ^ is incident on the liquid crystal layer 400 through the pixel electrode 2 in the penetration region 210. In the transflective LCD of the present embodiment, as described above, a vertical alignment type liquid crystal having a negative dielectric anisotropy (? ε < 0) is used in the liquid crystal layer 400' and a vertical alignment type alignment film is used. Therefore, in the non-applied state of the voltage, the direction is perpendicular to the direction of the plane of the film 26G perpendicular to the distribution of 10 317049D1D1 201109786, and as the applied voltage increases, the long axis direction of the liquid crystal is formed and formed on the pixel electrode 2 The electric field between the crucible and the common electrode is inclined perpendicularly to the plane direction of the substrate. When no voltage is applied to the liquid crystal layer 400, the polarization state does not change in the liquid crystal layer 400 and directly reaches the circularly polarized light. In the second substrate, when the second input/fourth plate 111 eliminates the circularly polarized light and becomes a linear deviation I, the second polarizing plate 112 is disposed so as to be linearly polarized from the two λ/4 plates 111. The direction of the vertical direction is such that the linearly polarized light cannot penetrate the second polarizing plate 112 which is perpendicular to the transmission axis (polarization axis) of the i-th polarizing plate ι 2, and the display becomes black. After the voltage is applied to the liquid crystal layer 400 , the liquid crystal layer 400 makes in The circularly polarized light produces a phase difference, for example, a reversed circular polarization, an elliptically polarized light, or a linearly polarized light, which is further shifted by the second 1/4 plate lu for the obtained light; 1/4 phase, thereby becoming a linearly polarized light (parallel to the transmission axis of the second polarizing plate), elliptically polarized light, and circularly polarized light, the polarized light has a component along the polarization axis of the second polarizing plate ❿112, and light corresponding to the component is emitted from the second polarizing plate 112 toward the observation side. Further, the phase difference plate 310 is a negative retarder (negauVe retarder), which can improve the optical characteristics when viewing the LCD from an oblique direction, and improve the viewing angle. Instead of the negative retarder (310) and the λ/4 plate 111, a two-axis phase difference plate having one of the two functions can be used, whereby the thickness of the LCD can be reduced and the transmittance can be improved. As described above, the thickness of the liquid crystal layer 400 (the liquid crystal cell 317049D1D1 11 201109786 gap) d which substantially controls the transmittance of light is set to be different between the penetration region 210 and the reflection region 220 by the gap adjustment portion 340. Between expectations The main reason is that the light-transmitting region 210 penetrates the liquid crystal layer 400 from the light source provided on the back surface side of the LCD (the first substrate 1 side in FIG. 1) from the second substrate 300 side. The amount of light (transmission rate) emitted to the outside is controlled to be displayed, and in the reflection region 220, the light incident from the observation side of the LCD toward the liquid crystal layer 400 is reflected by the reflection film provided in the formation region of the pixel electrode 200. The amount of light (the reflectance of the LCD) emitted from the second substrate side toward the observation side is controlled to be reflected and reflected again, and the number of times of penetration of the liquid crystal layer is different. That is, since the light system penetrates the liquid crystal layer 400 twice in the reflective region 220', the cell gap dr must be set smaller than the cell gap dt of the penetrating region 210. In the present embodiment, as shown in Fig. 1, the above-mentioned dr < dt is achieved by providing p + between the desired thicknesses and the adjustment portion 340 only in the reflection regions 220 of the respective regions. The entire circumference 340 of the gap 5 is not particularly limited as long as it has light transmittance and can be formed into a desired thickness. For example, an acrylic resin or the like which is also used as a flattened insulating layer or the like can be used. When the side surface of the gap adjusting portion 340 is used as a portion (inclined portion 520) of the alignment control portion 500 as described above, at least the taper angle must be not 90 degrees with respect to the plane of the substrate. The reason is that if the taper angle is 90 degrees or more, the alignment of the liquid crystal is disturbed on the side surface of the gap adjusting portion 340, and the common electrode 32A and the alignment film 26 formed on the gap adjusting portion 340 are also covered. Become inadequate. In addition, the side surface of the gap adjusting portion 340 has no effect on the display itself. If the taper angle is too small, the side surface area of the gap adjusting portion 340 is increased, so that the aperture ratio of the pixel, especially the period 317049D1D1 12 201109786, is expected to be improved. The p-sum rate of the reflective area of the brightness decreases. Therefore, the tapered cone w on the side of the whole portion 340 is better as the upper layer of the upper layer of the money, and the coverage of the 260 is lowered, and the alignment of the liquid crystal can be performed, and the angle of the liquid crystal is lowered. Specifically, it is preferably 30 degrees to 8 degrees. Between the angles of the taper cones, the above-mentioned acrylic resin is used. Then, the intermixing initiator 'I poly: the polymerization agent is added to the acrylic resin to adjust the polymerization characteristics, etc., and the manufacturing conditions of the r-integration, the side of the exposure device adjusting portion 340 is a straight cone 2 = a straight taper angle . In order to make the gap, for example, the material may be adjusted in addition to this, the example: ^^ fl〇W> money: the oxygen near the surface of the adjusting portion (10) is less, so the X is also due to the side of the substrate far from the surface. It is easy to remove the suppressing effect during development and continues to harden by polymerization, and the narrower the width of the skewed cone. On the surface side of the insulating layer 38, the more the device is formed, the more the device is used, and the exposure device is used, for example, in the proximity exposure gap adjusting portion forming region == fruit, and the gap adjusting portion 340 is cut. In the body flow, two go = handle shank. , 仏·. After the beam, for example by 80. (: to 80 317049DID1 13 201109786 °C temperature, baking 1 to 2 〇 min (for example, 12 (TC, 8 min), so that the upper side and the side of the entire circumference 340 of the gap 5 fused, smoothing the surface, At the same time, a tapered cone is formed by the side surface depending on the shape change of the surface tension of the molten material itself. Here, the organic material used for the gap adjusting portion or the like is known to have a g line indicating the exposure light source ( Materials such as 436 nm), h line (405) nm, and i line (248 nm) sensitivity, the organic material having sensitivity to the i line has a taper angle as much as 90 degrees or more (reverse taper). Therefore, in this embodiment In the form, the material of the gap adjusting portion has a sensitivity to the g-line and the h-line, and it is easy to form a slant-cone acrylic resin. In the present embodiment, in the pixel region, the penetration region 21 is reflected and reflected. The region 220 changes the thickness d of the liquid crystal layer, and simultaneously changes the thickness d of the liquid crystal layer for pixels of R, G, and B having different wavelengths (however, the common gap can be set in R, G, and B according to the characteristics of the LCD) In the example of figure j, by forming separately The thicknesses of the color filter layers 330r, 330g, and 330b of the R, G, and B sides on the second substrate 300 side are respectively changed, thereby achieving the gap d of all of R, G, and B. It is not limited to changing the thickness of the color filter layer. In the configuration, the gap adjusting portion 340' may also be provided in the penetration region 210 to change the thickness of the gap adjusting portion 340 in the penetration region 21〇 and the reflection region 22 of each of the R, G, and B. In R, G, and B, even if the thickness d of the liquid crystal layer is not different from each other, depending on the characteristics of the LCD, for example, G and B are used for the same liquid crystal layer thickness, and only R is different from the other two colors. 'It is also possible to change only the d for B. The second figure shows that the pixels for R, G, and B have different gaps. 317049D1D1 14 201109786 He is composed (in the second figure, the composition of rt is shown in Fig. 2) The structure similar to that of Fig. 1 will not be described again. However, the first substrate is opened, the gap between R, G, and B is not changed on the substrate side, and the thickness of the insulating layer 38 is formed on the pixel electrode. The method of flattening the thickness of the lower layer of 2〇0 is, for example, B minus. Changing the insulating layer 38 - or a plurality of half exposures Target opening amount corresponding to the thickness of a single material to be exposed, without (iv) / the material comprising the planarizing insulating and sound of the photosensitive material R ancient particular ^ the addition of a special process can be formed in each of the R, G,

^ 5厚度之平坦化絕緣層38。再者,在第2 中,反射區域在平扫彳有在第2圖 %在仪化絕緣層38之上形成 化絕緣層38之表面之 凸該千坦 絕緣層38上之反射層::使域中形成於平坦化 ' 44延,·貝此形狀,而在反射層44之声 面形成凹凸:從而使向液晶層人射之人射光散亂,提高^ 射區域之顯示品質。並且,也可利用用於在上述R、G、Β 將平坦化絕緣層38形成為不同厚度之半曝光,不追加製程 地一同形成,在平坦化絕緣層38之反射區域之該凹凸、以 及為連接像素電極200與TFT而貫穿平坦化絕緣層38 之接觸孔。 S " 其次’對本實施形態之半穿透型LCD之各像素之具體 結構加以說明。第3圖為本實施形態之半穿透型LCD之美 本平面構成之一例,第4圖為沿第3圖之A — A,線之基本 剖面結構,第5圖為沿第3圖之B — B’線之基本剖面結構, 第6圖表示第3圖之像素電極200及與其相連之薄膜電晶 體等之具體構成。 在第3圖所示之平面構成中’每一像素之個別圖案之 317049D1D1 15 201109786 像素電極2GG在畫面之垂直掃描方向(第3圖之上下方向) 具有細長之六角形圖案,在含有在長度方向之2個上邊而 以圖中斜線所包圍之四角形(在圖中為菱形或正方形)之區 域中,如第6圖所示’選擇性地形成有反射膜,而設置有 反射區域220。並且,六角形像素電極2〇〇之其餘之約略 箭羽形狀區域係成為穿透區域21〇。 如從第4圖也可理解,為使在反射區域22〇之液晶層 之厚度(液晶盒間隙)dr比在穿透區域21〇之間隙dt小, 而將間隙調整層340形成於第2基板300上,在第4圖之 例子中係形成於共通電極320上。 該間隙調整層340之像素内之端部係配置於沿著與上 述六角形之像素電極200之2個上邊大致線對稱之四角形 反射區域220之下側2邊之位置。並且,以連接四角形反 射區域220之水平掃描方向(圖中之左右方向)相對之頂點 間而將該反射區域220於水平掃描方向分割為上下之方 式’在第2基板300(具體地說在第4圖中為間隙調整部340) 上形成有截面為三角形之突起部51 Or。 並且,雖然第4圖中省略,但如第1圖及第2圖所示, 在包括有突起部510及間隙調整部340之第2基板300之 全部表面覆蓋垂直配向膜260。當然,包括第1基板1〇〇 側之像素電極200之全部表面側也與第1圖、第2圖相同 形成有垂直配向膜260。因此,在未於像素電極2〇〇與共 通電極320之間施加電壓之狀態下’液晶之長軸方向(液晶 指向(director))410係相對於垂直配向膜260之平面方向 317049D1D1 16 201109786 而垂直地配向。由此,在第2基板300側,在突起部51〇 及間隙調整部340之斜面上,液晶指向41〇係相對於延續 這些斜面而形成於與液晶之相對面側之配向膜26〇之斜面 而垂直配向。因此,如第3圖及第4圖所示,以將反射區 域220分割為上下之位置之突起部51〇r為界,形成液晶之 配向角(配向方位)互相相差18〇。之區域。 、其人如第3圖及第5圖所示,在箭羽形狀之穿透區 域210中’在垂直掃描方向將細長六角形像素電極㈣沿 垂直掃描方向左右(水平掃描方向)等分之位置(相當於箭 羽之甲。之σ卩刀)’在第2基板_側(具體地說為共通電 極320之上)形成有截面為三角形之突起部51〇^雖在第5 圖中與第4圖同樣予以省略,但在第2基板300側及第】 土板1GG側之任—者均在與液晶之接觸面形成如第1圖及 第2圖所示之垂直配向膜26〇,在穿透區域2ι〇中亦以形 成於第2基板_上之突起部51()t為界,將液晶指向彻 之配向方向(配向方位)分割成互相相差180。之方向。 1匕夕:在本實施形態中’不僅使用上述突起、斜面, 非電極區域53。作為配向控制物,在第3圖至 =圖之例子中,將配置於第1基板_側之像素電極200 :二:=部分作為用於配向控制之無電極部530使用。 通電極 電場下,如第Γ = Γ時之弱咖 無電極部之端部(亦即,電極之端部):朝==、= 317049D1D1 17 201109786 變寬的方式傾斜。然後,具有負介電率異向性之液晶之短 軸係沿著該傾斜之電力線進行配向,因此,液晶分子從初 期之垂直配向狀態所隨著向液晶之施加電壓之上升傾斜之 方向係由傾斜電場決定。 在第3圖所示之六角形像素電極2〇〇中具有該像素電 極200之端部’亦即至少具有六邊之無電極部530。因此, 液晶指向410由於上述突起部510(51〇r、51〇t)及斜面 520,以及像素電極2〇〇周圍之無電極部53〇之作用,在一 像素區域内,在反射區域220至少形成兩個配向區域,在 穿透區域210形成與上述反射區域220之兩個區域中之任 一者都不同之配向方位之兩個配向區域,亦即,總共形成 四個具有不同配向方向之區域。 /、中更準確地說’液晶指向410係被控制成,使其 平面成分(配向方位角)相對於上述突起部51〇之延伸方向 及電極(無電極部)之邊緣之延伸方向垂直。因此,即使在 上述四個配向區域中’在其—個區域内液晶之配向方位角 亦不完全相同。例如,在第3圖中,在穿透區域210之垂 直掃播方向之中間位置,液晶指向410係相對於沿該垂直 掃描方向延伸之突起部51〇t及像素電極2〇〇邊緣而配向為 垂直之方向。但是在穿透區域21〇之例如與反射區域挪 之又界,利用間隙調整部34〇之傾斜部(突起部)52〇係與 域210之突起部51〇t以大於9〇度之角度交叉而 ^著罪近利用間隙調整部34〇之傾斜部52〇,該交叉附近 之液晶之配向方位角係從與突起部510之延伸方向垂直之 317049D1D1 18 201109786 方向,變化成與該傾斜部520之延伸方向垂直之方向。但 是,在一配向區域内,如後所述,以使液晶之配向方位角 之依據位置之變化程度(或最大角度)變小的方式,設定配 向控制部500之延伸方向,因而可防止在一配向區域之不 定位置產生液晶之配向方位角不同之區域之交界(向錯線 (disciination line))。 下面,說明本實施形態之配向控制部500之延伸方向 及液晶之配向方位角在一像素區域内之各位置之關係。 因為液晶分子沒有長軸方向之上下特性差,因此由穿 透區域210之突起部510t控制之液晶之配向方位角以及由 與該突起部510t交叉之間隙調整部340之傾斜部520控制 之液晶之配向方位角之角度差比90度小,在第3圖之例子 中,突起部510與利用間隙調整部340之傾斜部520之交 叉角度約為135度,對此,液晶之配向方位角之差為45度。 再者,在此係以突起部510t與間隙調整部340交叉為例進 行了說明,但也有物理地未交叉的情形,而在本說明書中, 所謂交叉係指各自之延伸線交叉,此外,當設置於各自不 同之基板時,係指各自之延長線之向同一基板平面之投影 線交叉。 另外,利用間隙調整部340之傾斜部520與穿透區域 210之像素電極200之邊之交叉角度(但,因為實際上傾斜 部520及像素電極200並不形成於同一基板上,故此時係 分別朝同一基板平面之投影線的交叉角度),在第3圖之例 子中,為約45度。由傾斜部52控制之液晶之配向方位角 19 317049D1D1 201109786 與由像素電極200之邊緣控制之液晶之配向方位角之角度 仍然在90度以下,於此係為比45度小之角度。 穿透區域210之下端附近之突起部510t與像素電極 200之邊緣朝基板平面之投影線上之交叉角度在此為45 度,因為和上述同樣液晶分子沒有上下之特性差,故在該 交叉附件之液晶之配向方位角之差比90度小,在此,為 45度以下。 在穿透區域210中還具有像素電極200之邊彼此交叉 之區域。在第3圖之例子中,係指沿垂直掃描方向延伸之 邊,與從與上述突起部510交叉之頂點朝向沿該垂直掃描 方向之邊延伸之邊,兩邊之交叉角度比90度大,在此為 135度。而該交叉部之液晶之配向方位角之差仍然因液晶 分子沒有上下特性差,故在此也比90度小,為45度。 同樣,在反射區域220中,在配向控制部500朝基板 平面之投影線(包括延長線)與其他配向控制部500朝同一 基板平面之投影線(包括延長線)交叉之區域,係以使液晶 之配向方位角之差比90度小之方式設置配向控制部500。 即,首先,反射區域220内之將配向方向上下分割之突起 部510 r係與利用在像素電極2 0 0之端部交叉之間隙調整部 340之傾斜部520以小於90度之角度交叉,該交叉區域之 液晶之配向方位角之角度差係控制在比90度小之45度以 下。 該突起部510r與反射區域220之像素電極200之邊緣 之交叉角度(朝基板平面之投影線之交叉角度)也同樣控制 20 317049D1D1 201109786 成小於90度,該等交叉部之液晶之配向方位角之角度差也 與上述相同控制在比90度小之45度以下。 如上所述,當配向控制部500朝基板平面上之投影線 彼此間交叉時,係以使由該等配向控制部500控制之液晶 之配向方位角之差未滿90度之方式而決定配向控制部 500(突起部510、傾斜部520、無電極部(在第3圖之例子 中,為像素電極200之形狀)530)。由此,可確實防止在由 配向控制部500分割之一區域内之不定位置產生向錯線。 • 再者,在反射區域220之像素電極200之邊彼此間交 叉之位置(在第3圖中為位於像素電極200之垂直掃描方向 之最上部之頂點附近)及利用間隙調整部340之傾斜部520 彼此間之交叉部(V字之接頭附近),在第3圖之例子中, 其交叉角度皆為90度。當然,將該交叉角度設為小於90 度或者大於90度從上述觀點而言更好,但因為與穿透區域 210相比較,菱形反射區域220之面積本身較小,故可防 φ 止在不定位置產生向錯線。 反射區域220内之液晶因為強烈地接受利用突起部 51 Or、傾斜部420及像素電極200之邊之配向控制,故在 連接上述反射區域220之電極200之邊之交點與利用間隙 調整部340之斜面部520之交點之菱形反射區域220之斜 線上,不存在物理性之配向控制部5 0 0。但是,從相鄰之 配向控制部500接受到相等之控制,以及相對於突起部 51 Or之延伸方向而被控制成垂直方向之液晶之連續體性雙 方之影響,該位置之液晶指向410之平面分量如第3圖所 21 317049D1D1 201109786 示’成為沿垂直掃描方向之方向。然後,隨著從該位置向 像素電極之水平掃描方向之端部靠近,液晶受到像素電極 2〇〇之邊(530)及間隙調整部340之斜面52〇之延伸方向與 突起部510r之影響,而被控制成朝向從與該等延伸方向垂 直之方向偏離少許之角度(未滿90度,在第3圖之例子中 為小於45度)。因此,即使在反射區域22〇内也可防止在 不定位置產生向錯線。 其次,如第6圖所示,對像素電極2〇〇及與該像素電 極連接之薄膜電晶體TFT之構成及製造方法加以說明。在 本實施形態中’如上所述,係為各像素具有薄膜電晶體之 所謂主動矩陣型LCD,而如第6圖所示,形成於第丄基板 1〇0側之像素電極200與基板1〇〇之間係形成有該薄膜電 晶體TFT。另外由於係為了儘量在一像素區域内高效率地 配置穿透區域210及反射區域220,尤其是不使穿透區域 之開口率降低,因此係將在穿透型lcd中一般亦形成 於遮光區域之TFT配置於即使設置有該TFT也不會對開口 率產生影響之反射區域220。 在本實施形態中,係採用頂閘極型作為TFT,另外, 使用將非結晶石夕(a — S i)用雷射退火而多結晶化得到之多 結晶矽(p〜Si)作為主動層20。當然,TFT不限定於頂閘極 t P Si ’也可為底閘極型,主動層也可採用。TFT 主動層2〇之源極’>及極區域20s、20d所摻雜之雜質可為 ^導電型、P導電型中之任意一種,但在本實施形態中,係 採用摻雜有磷等η導電型雜質的n —oh型之奸丁。 317049D1D1 22 201109786^ 5 thickness of the planarization insulating layer 38. Furthermore, in the second embodiment, the reflective region has a reflective layer on the surface of the insulating layer 38 formed on the surface of the insulating layer 38 on the flat surface of the second insulating layer 38. The domain is formed in a flattened shape of "44", and the shape of the surface of the reflective layer 44 is formed by unevenness: the light emitted to the liquid crystal layer is scattered, and the display quality of the area is improved. Further, it is also possible to form the semi-exposure in which the planarizing insulating layer 38 is formed to have different thicknesses in the above-mentioned R, G, and ,, and to form the same in the reflective region of the planarizing insulating layer 38 without adding a process. The pixel electrode 200 and the TFT are connected to penetrate the contact hole of the planarization insulating layer 38. S " Next, the specific structure of each pixel of the transflective LCD of the present embodiment will be described. Fig. 3 is a view showing an example of a planar structure of a transflective LCD of the present embodiment, Fig. 4 is a cross-sectional view taken along line A-A of Fig. 3, and Fig. 5 is a B along the third drawing. The basic cross-sectional structure of the B' line, and Fig. 6 shows the specific configuration of the pixel electrode 200 of Fig. 3 and a thin film transistor connected thereto. In the plane configuration shown in Fig. 3, the individual pattern of each pixel is 317049D1D1 15 201109786. The pixel electrode 2GG has an elongated hexagonal pattern in the vertical scanning direction of the screen (the lower direction in Fig. 3), and is contained in the longitudinal direction. In the region of the square shape (diamond or square in the figure) surrounded by oblique lines in the figure, as shown in Fig. 6, a reflection film is selectively formed, and a reflection region 220 is provided. Further, the remaining area of the hexagonal pixel electrode 2 is approximately the shape of the penetrating region 21A. As can be understood from Fig. 4, the gap adjusting layer 340 is formed on the second substrate so that the thickness (cell gap) dr of the liquid crystal layer in the reflective region 22 is smaller than the gap dt in the transmissive region 21A. 300 is formed on the common electrode 320 in the example of Fig. 4. The end portion in the pixel of the gap adjusting layer 340 is disposed at a position along the lower side of the quadrangular reflecting region 220 which is substantially line symmetrical with the two upper sides of the hexagonal pixel electrode 200. Further, in the horizontal scanning direction (the horizontal direction in the drawing) of the quadrangular reflection region 220, the reflection region 220 is divided into the upper and lower sides in the horizontal scanning direction in the horizontal scanning direction (in the second substrate 300 (specifically, 4 is a gap adjusting portion 340) in which a projection portion 51 Or having a triangular cross section is formed. Further, although not shown in Fig. 4, as shown in Figs. 1 and 2, the vertical alignment film 260 is covered on the entire surface of the second substrate 300 including the protrusion portion 510 and the gap adjusting portion 340. Of course, the vertical alignment film 260 is formed on the entire surface side of the pixel electrode 200 including the first substrate 1 side as in the first and second drawings. Therefore, in a state where a voltage is not applied between the pixel electrode 2A and the common electrode 320, the long axis direction (liquid crystal director) 410 of the liquid crystal is perpendicular to the plane direction 317049D1D1 16 201109786 of the vertical alignment film 260. Ground alignment. Thereby, on the side of the second substrate 300, on the inclined surface of the protrusion portion 51 and the gap adjusting portion 340, the liquid crystal is directed toward the inclined surface of the alignment film 26 which is formed on the side opposite to the liquid crystal with respect to the slanting surface. Vertical alignment. Therefore, as shown in Figs. 3 and 4, the alignment angles 51 of the liquid crystals are aligned with the projections 51〇r which divide the reflection region 220 into the upper and lower positions, and the alignment angles (alignment directions) of the liquid crystals are different from each other by 18 〇. The area. As shown in FIG. 3 and FIG. 5, in the penetrating region 210 of the arrow feather shape, the position of the elongated hexagonal pixel electrode (four) is equally divided in the vertical scanning direction (horizontal scanning direction) in the vertical scanning direction. (corresponding to the arrowhead of the arrow feather.) The protrusion on the second substrate_ side (specifically, on the common electrode 320) is formed in a triangular shape with a triangular cross section 51〇, although in the fifth figure and the 4, the same is omitted, but the vertical alignment film 26〇 shown in FIGS. 1 and 2 is formed on the contact surface with the liquid crystal on both the second substrate 300 side and the first earth plate 1GG side. The penetration region 2 is also defined by the protrusions 51()t formed on the second substrate_, and the liquid crystals are directed to the alignment direction (orthogonal orientation) to be 180. The direction. In the case of the present embodiment, not only the above-mentioned projections and slopes but also the non-electrode region 53 are used. As an alignment control, in the example of Fig. 3 to Fig., the pixel electrode 200 disposed on the first substrate_ side is used as the electrodeless portion 530 for alignment control. Under the electric field, as in the case of Γ = Γ, the end of the electrodeless part (ie, the end of the electrode): tilted toward the way of ==, = 317049D1D1 17 201109786 widening. Then, the short axis of the liquid crystal having the negative dielectric anisotropy is aligned along the oblique power line. Therefore, the direction in which the liquid crystal molecules are tilted from the initial vertical alignment state with the rise of the applied voltage to the liquid crystal is The tilting electric field is determined. The hexagonal pixel electrode 2A shown in Fig. 3 has an end portion of the pixel electrode 200, i.e., an electrodeless portion 530 having at least six sides. Therefore, the liquid crystal pointing 410 is at least in the reflective region 220 due to the action of the protrusions 510 (51〇r, 51〇t) and the slope 520, and the electrodeless portion 53〇 around the pixel electrode 2〇〇. Two alignment regions are formed, and two alignment regions of the alignment orientation different from any of the two regions of the reflection region 220 are formed in the penetration region 210, that is, a total of four regions having different alignment directions are formed. . More specifically, the liquid crystal pointing 410 is controlled so that the plane component (alignment azimuth angle) is perpendicular to the extending direction of the projection portion 51 and the extending direction of the edge of the electrode (electrodeless portion). Therefore, even in the above four alignment regions, the alignment azimuths of the liquid crystals in their respective regions are not completely the same. For example, in FIG. 3, in the middle of the vertical scanning direction of the penetration region 210, the liquid crystal pointing 410 is aligned with respect to the protrusion 51 〇t and the edge of the pixel electrode 2 延伸 extending in the vertical scanning direction. The direction of the vertical. However, in the penetration region 21, for example, the reflection region is shifted, and the inclined portion (projection portion) 52 of the gap adjustment portion 34 is overlapped with the projection portion 51〇t of the field 210 at an angle of more than 9 degrees. And the sin is close to the inclined portion 52A of the gap adjusting portion 34, and the alignment azimuth of the liquid crystal in the vicinity of the intersection is changed from the direction of the 317049D1D1 18 201109786 perpendicular to the extending direction of the protruding portion 510 to the inclined portion 520 The direction of extension is perpendicular to the direction. However, in an alignment region, as will be described later, the direction in which the alignment direction of the liquid crystal is changed (or the maximum angle) is set to be smaller, thereby setting the direction in which the alignment control unit 500 extends. The indefinite position of the alignment region produces a boundary (disciination line) of a region in which the alignment angles of the liquid crystals are different. Next, the relationship between the extending direction of the alignment control unit 500 and the alignment azimuth of the liquid crystal in each pixel position in the pixel region will be described. Since the liquid crystal molecules have no characteristic difference in the direction of the major axis, the alignment azimuth of the liquid crystal controlled by the protrusion 510t of the penetration region 210 and the liquid crystal controlled by the inclined portion 520 of the gap adjusting portion 340 crossing the protrusion 510t The angular difference of the azimuth angle is smaller than 90 degrees. In the example of FIG. 3, the angle of intersection between the protrusion 510 and the inclined portion 520 of the gap adjusting portion 340 is about 135 degrees. For this, the difference in alignment angle of the liquid crystal It is 45 degrees. In this case, the protrusion 510t and the gap adjustment unit 340 are described as an example. However, there is a case where the intersection is not physically crossed. In the present specification, the intersection means that the respective extension lines intersect, and further, when When disposed on different substrates, it means that the extension lines of the respective extension lines cross the projection line of the same substrate plane. In addition, the angle of intersection between the inclined portion 520 of the gap adjusting portion 340 and the side of the pixel electrode 200 of the penetrating region 210 is used (however, since the inclined portion 520 and the pixel electrode 200 are not formed on the same substrate, respectively, The angle of intersection of the projection lines toward the same substrate plane is about 45 degrees in the example of Fig. 3. The alignment azimuth of the liquid crystal controlled by the inclined portion 52 19 317049D1D1 201109786 The angle of the azimuth angle with the liquid crystal controlled by the edge of the pixel electrode 200 is still 90 degrees or less, which is an angle smaller than 45 degrees. The angle of intersection of the protrusion 510t near the lower end of the penetration region 210 and the edge of the pixel electrode 200 toward the substrate plane is 45 degrees here, because the same liquid crystal molecules have no upper and lower characteristics difference as described above, so in the cross-attachment The difference in the azimuth angle of the liquid crystal is smaller than 90 degrees, and here, it is 45 degrees or less. There is also a region in the penetration region 210 where the sides of the pixel electrode 200 cross each other. In the example of Fig. 3, the side extending in the vertical scanning direction is the side extending from the vertex crossing the protrusion 510 toward the side along the vertical scanning direction, and the angle of intersection between the two sides is larger than 90 degrees. This is 135 degrees. The difference in the azimuth angle of the liquid crystal at the intersection is still due to the fact that the liquid crystal molecules have no difference in upper and lower characteristics, and therefore are also smaller than 90 degrees and are 45 degrees. Similarly, in the reflection region 220, the projection line (including the extension line) of the alignment control unit 500 toward the substrate plane and the other alignment control unit 500 intersect the projection line (including the extension line) of the same substrate plane to make the liquid crystal The alignment control unit 500 is provided such that the difference in the azimuth angle is smaller than 90 degrees. In other words, first, the projections 510 r that are vertically divided in the alignment direction in the reflection region 220 are intersected with the inclined portion 520 of the gap adjustment portion 340 that intersects the end portion of the pixel electrode 2000 at an angle of less than 90 degrees. The angular difference of the alignment azimuth of the liquid crystal in the intersecting region is controlled to be less than 45 degrees below 90 degrees. The angle of intersection of the protrusion 510r with the edge of the pixel electrode 200 of the reflective region 220 (the angle of intersection of the projection line toward the plane of the substrate) also controls 20 317049D1D1 201109786 to be less than 90 degrees, and the alignment azimuth of the liquid crystal of the intersections The angular difference is also controlled to be less than 45 degrees less than 90 degrees as described above. As described above, when the alignment control unit 500 intersects the projection lines on the plane of the substrate, the alignment control is determined such that the difference in the azimuth angles of the liquid crystals controlled by the alignment control unit 500 is less than 90 degrees. The portion 500 (the protrusion portion 510, the inclined portion 520, and the electrodeless portion (in the example of Fig. 3, the shape of the pixel electrode 200) 530). Thereby, it is possible to surely prevent the occurrence of the disclination line at an indefinite position in one of the areas divided by the alignment control unit 500. Further, at a position where the sides of the pixel electrode 200 of the reflection region 220 intersect each other (in the vicinity of the apex of the uppermost portion in the vertical scanning direction of the pixel electrode 200 in FIG. 3) and the inclined portion by the gap adjusting portion 340 520 The intersection between each other (near the V-joint), in the example of Figure 3, the angle of intersection is 90 degrees. Of course, it is better to set the crossing angle to be less than 90 degrees or more than 90 degrees from the above viewpoint, but since the area of the diamond-shaped reflecting area 220 is small as compared with the penetrating area 210, it is possible to prevent φ from being indefinite The position produces a disclination line. Since the liquid crystal in the reflection region 220 strongly receives the alignment control by the side of the protrusion 51 Or, the inclined portion 420, and the pixel electrode 200, the intersection of the side of the electrode 200 connected to the reflection region 220 and the gap adjusting portion 340 are used. There is no physical alignment control unit 500 on the oblique line of the rhombic reflection region 220 at the intersection of the inclined surface 520. However, the adjacent alignment control unit 500 receives the equal control and the influence of the continuous body of the liquid crystal controlled in the vertical direction with respect to the extending direction of the protrusion 51 Or, and the liquid crystal of the position points to the plane of 410. The component is shown in Fig. 3, 21 317049D1D1 201109786, indicating 'being in the direction of the vertical scanning direction. Then, as the end portion of the pixel electrode in the horizontal scanning direction approaches from the position, the liquid crystal is affected by the edge of the pixel electrode 2 (530) and the extending direction of the slope 52 〇 of the gap adjusting portion 340 and the protrusion 510r. It is controlled to be slightly offset from the direction perpendicular to the extending direction (less than 90 degrees, and less than 45 degrees in the example of Fig. 3). Therefore, it is possible to prevent the occurrence of the disclination line at an indefinite position even in the reflection area 22A. Next, as shown in Fig. 6, a configuration and a manufacturing method of the pixel electrode 2A and the thin film transistor TFT connected to the pixel electrode will be described. In the present embodiment, as described above, a so-called active matrix type LCD in which each pixel has a thin film transistor is formed, and as shown in Fig. 6, the pixel electrode 200 and the substrate 1 formed on the side of the second substrate 1? The thin film transistor TFT is formed between the turns. In addition, in order to efficiently arrange the penetration region 210 and the reflection region 220 in a pixel region as much as possible, in particular, the aperture ratio of the penetration region is not lowered, so that it is generally formed in the light-shielding region in the penetration type lcd. The TFT is disposed in the reflective region 220 which does not affect the aperture ratio even if the TFT is provided. In the present embodiment, a top gate type is used as the TFT, and a polycrystalline germanium (p to Si) obtained by multi-crystallization of amorphous austenite (a-S i) by laser annealing is used as an active layer. 20. Of course, the TFT is not limited to the top gate t P Si ' or the bottom gate type, and the active layer can also be used. The source of the TFT active layer 2' and the impurity doped with the polar regions 20s and 20d may be any of a conductive type and a P conductive type. However, in the present embodiment, phosphorus is doped. The n-oh type of η conductivity type impurity. 317049D1D1 22 201109786

TFT之主動層20由閘極絕緣膜3〇予以覆蓋,閘極絕 緣膜30上形成有由Cr、Mo等高熔點金屬材料構成、並兼 作閘極線之閘極電極32。且,該閘極電極32形成後,將 该閘極電極32作為遮罩而在主動層2〇中形成將上述雜質 予以摻雜之源極及汲極區域2〇s、2〇d,以及形成不摻雜雜 資之通道區域20c。其次’覆蓋該全部之TFTii〇而形成層 間絕緣膜34,在該層間絕緣膜34形成接觸孔後,形成電 極材料,透過該接觸孔而分別將源極電極4〇連接於上述p Si主動層20之源極區域2〇s,並將汲極電極連接於 及極區域謝。再者’在本實施形態中,汲極電極36兼作 ^各TFT11G供給與顯示内容相應之資料信號之信號線。另 一方面’源㈣極40如後所述,與作為像素電極之第1電 極200相連接。再者’汲極電極%及源極電極4〇均使用 南導電性之例如A1等。 …源極電極40及及極電極36形成後,覆蓋基板全面而 =成由丙稀酸樹脂等樹脂材料構成之平垣化絕緣膜38。其 在該平丨―化絕緣膜38之源極電極4G之形成區域形成 孔ϋ在該接觸孔中形成連接用金屬層^,而連接源 40與該金屬層42。源極電極4〇使用Μ等時,藉 ::層4:採用Mo等金屬材料,而使源極電極4。與該金 U Γ成為良好的歐姆接觸。再者,也可省略源極 接觸層42係與TFTll°切主動層2°相 =觸’而W金屬可與如献半導體材料之間確立歐姆接 317049D1D1 23 201109786 進打連接用金屬層42之層4 •圖鈴後,首先在基板 全面藉由蒸鐘、崎等層疊反射層用A卜Nd合金、Al等 反射特性較好之反射材料層。層疊之該反射材料層從TFT 之源極區域附近(金屬層42之形成區域)進賴刻去除,俾 不妨礙金屬層42及後面形成之像素電極2〇〇與tft之接 觸’且同時進行⑽j去除俾不殘存於穿透區域別,而將 如上述第3圖所示之外形在各像素之反射區域220形成菱 形圖案之反射層44。再者,為了防止向TFT(尤其是通道區 域20c)照射光而產生洩漏電流之情形,且為了儘量擴大可 反射區域(即顯示區域),而在本實施形態中,如第丨圖所 示,將反射層44也積極形成於TFT11〇之通道上方區域。 在進行該種反射層44之圖案化時,由上述M〇等構成 之金屬層42具有足夠之厚度(例如:0.2以哟,且對蝕刻液 具有足夠之耐性。因此,將金屬層42上之反射層44進行 触刻去除後’該金屬層42也可未完全被去除而殘存於接觸 孔内。另外,在很多情況中,源極電極40等係由與反射層 44相同之材料(A1等)構成,故當不存在上述金屬層42時, 源極電極40會被反射層44之餘刻液浸餘而產生斷線等。 但’本實施形態藉由設置金屬層42,而可耐受反射層44 之圖案化’並可維持與源極電極40之良好的電性連接。 在反射層44之圖案化後,藉由濺鍍層疊透明導電層而 將含有反射層44之基板全部表面予以覆蓋。在此,如上所 述,由A1等構成之反射層44之表面此時以絕緣性之自然 氧化膜覆蓋,而等高熔點金屬即使暴露於濺鍍環境中其 317049D1D1 24 201109786 '表面也不會氧化。因此,在接觸區域露出之金屬層42可與 ' 層疊於該金屬層42上之像素電極用透明導電層之間有歐 姆接觸。再者,透明導電層在成膜後,係獨立於每一像素, 且在一像素區域内共通於反射區域與穿透區域,並例如如 上述第3圖所示,圖案化成細長之六角形形狀,由此得到 像素電極200。另外,該像素電極200進行圖案化後,覆 蓋基板全部表面而形成由聚醯亞胺等構成之配向膜260, 從而完成第1基板側。然後,在第2基板300上形成如第 • 1圖及第2圖所示之R、G、B之彩色濾光層、共通電極320、 間隙調整部340及突起部510(510r、510t)、以及覆蓋該 等元件而形成之配向膜260,再將第2基板300與該第1 基板100以一定間隔分離並在基板之周邊部分貼合,且在 基板間封入液晶’從而得到LCD。 再者,在第1圖及第2圖之例子中,形成於第2基板 300側之共通電極320係形成於間隙調整部340之上層, ^ 在該共通電極320之期望位置則形成有突起部510。相對 於此,如第4圖所示,共通電極320亦可如第4圖所示般 形成於間隙調整部340之下方(實際上,為形成於第2基板 300上之彩色濾光層與間隙調整部340之間)。間隙調整部 340非常厚時,如第4圖所示,在間隙調整部340下方形 成共通電極320後,對液晶層410所施加之實效電壓變得 較低,但在將十分高之電壓施加於共通電極320與像素電 極200之間的情形中,或是間隙調整部340不太厚的情況 中,也可採用第4圖所示之構成。 25 317049D1D1 201109786 下面對本實施形態之半穿透型LCD之各像素之結構之 其他例子加以說明。第7圖為其他例子之半穿透型lcd之 基本平面構成,第8圖為沿第7圖之c — c,線之基本剖面 結構。再者,沿第7圖之D-D,線之基本剖面結構與上述 第5圖所示之基本剖面結構相同。 與上述第3圖所*之結財同之點在於,首先像素電 極240之形狀在第7圖中之例子中為長方形,且在穿透區 域210及反射區域220之各四角形之區域内,在相當於其 四角形斜邊之位置形成有略χ字狀之突起部_、作 為配向控制部500。藉由該種配向控制部5〇〇,在穿透區域 210及反射區域220内以各突起部51〇t、51〇r為境界,分 別形成液晶之配向方向不同之4個區域,從而進一步擴大 視角。 、 另外,在一像素區域内之穿透區域21〇之交界,如上 所述,在第2基板300側構成利用間隙調整部34〇之斜面 部520之配向控制部500,同時將與該斜面部52〇並列、 向水平掃描方向延伸之無電極部(狹縫:窗咖s)53〇形成 於像素電極200。因此’在穿透區域21〇與反射區域22〇 之父界區域中,在第2電極侧係藉由間隙調整部34〇之斜 面(傾斜部5 2 0 )將液晶之初期配向控制為與該斜面垂直之 方向,同時在第1基板側係藉由無電極部53〇s之如第8圖 所示之弱電場之傾斜,將液晶之配向控制為以該無電極部 530s為交界之不同之方向角。因此,可更加確實地進行在 穿透區域210與反射電極220之交界附近之液晶之配向分 3I7049D1D1 26 201109786 .割。 如上所述’由像素電極200之邊緣、上述突起部51〇 及無電極部530s等構成之配向控制部5〇〇之各圖案及配向 分割數量也與上述第3圖所示之形態有所不同,但在第7 圖所示之形態中’由某配向控制部5〇〇控制之液晶之配向 方位角亦與由具有與該配向控制部500朝基板平面上之投 影線相交之投影線之其他配向控制部500所控制之液晶之 配向方位角之角度差在無論在哪個交點都未滿9〇度。因此, ®可確實防止在所分割之各配向區域内在不定位置產生向錯 線。另外,藉由採用上述第3圖及該第7圖所示之配向控 制部500之圖案’可透過最小限度之配向控制部5〇〇之形 成達成最大限度之配向分割數量及;實進行配向分割。本 貫施形態中採用之垂直配向型液晶中,為在電壓非施加狀. 態(亦即垂直配向狀態)下顯示為黑色,而不僅像素電極2〇〇 之間隙正上方,還有在其他配向控制部5〇〇(突起部51〇、 鲁傾斜部520及狹縫530s)之正上方位置,即使在共通電極 320與像素電極200之間施加充分之電壓之狀態,液晶之 配向狀態亦幾乎不會從垂直配向狀態改變,而不影響顯 示。因此’無用之配向控制部5〇〇之配置會使[CD之開口 率下降。但,如果為上面說明之第3圖、第7圖所示之設 計’就可將開口率抑制在最小限度,且可擴大視角並提高 顯示品質。 第9圖及第ίο ®分別表示上述第3圖所示構成之其他 變形例。 27 317049D1D1 201109786 首先’在第9圖中,將全部像素電極25〇形成為箭羽 形狀,其中反射區域220之形狀、構成與第3圖相同,但 不同點在於’在其餘之穿透區域加之圖案係為配置成橫 方向之鼓型或略沙漏形狀’或M字上下相反聯結之形狀。、 該突起部51Gt朝平面上之投影線與朝同—平面上之投影 線相交之透明區域210之像素電極25〇之2邊均以比9〇度 大之角度(在此為135度)交叉。如上所述,因為液晶分子 在長軸方向上下沒有特性差,故該交又區域之液晶之配向 方位角之歧差仍然不到9〇度4外,分職與上述突起 部510t之交又位置朝沿著垂直掃描方向延伸之像素電極 250之2邊之下端延伸之像素電極25〇之下部之2邊,與 沿該垂直掃財向之像素f極25Q之邊之交叉角度不到9〇 度’在該區域中’液晶之配向S位角之最大差也不到90度 (在第9圖之例子中,比45度小)。因此,在穿透區域21〇 内之2個配向區域内也可防止在不定位置產生向錯線。 在第10圖中,像素電極252之形狀為箭羽形狀,穿透 區域210之形狀(箭羽形狀)及構成與第3圖相同,但箭羽 形狀之像素電極252之其餘之反射區域220之形狀,以及 用以分割該區域内之液晶之配向之突起部510r之形成位 置有所不同。即,在第1〇圖之例子中,反射區域220也為 長度較短之箭羽形狀,在反射區域220與穿透區域210之 交界係由間隙調整部340之V字狀傾斜部520進行配向分 割,在連接該V字狀之頂點與反射區域220内之像素電極 252之相同V字狀之頂點之沿垂直掃描方向之線上’在第2 28 317049D1D1 201109786 基板側(間隙調整部上)形成突起部51 〇r,以該突起部51 〇r 為交界使反射區域220在水平掃描方向形成有左右2個之 配向區域。在該種構成中,無論由哪個配向控制部5〇〇控 制之液晶之配向方位角與由具有與該配向控制部5〇〇朝基 板平面之投影線交叉之投影線之其他配向控制部5〇〇所控 制之液晶之配向方位角之角度差係滿足未滿9〇度之關 係,故可進行良好之配向分割。 其次,對本實施形態之垂直配向型半穿透LCD之驅動 電壓與穿透率及其波長之依存性加以說明。 第11圖表示向液晶施加之施加電壓(v)與穿透率(任 意單位)之關係,而係為以— 表示之垂直 配向液晶盒之光學特性,換言之,為改變液晶盒之結構時 之施加電壓與穿透率之關係。其中,在第u圖中,紂為 55〇nm(綠色)。在上述⑴式中,(del —n)為液晶層之複折 射(即折射率異向性)(Δη),d為液晶層之厚度(液晶盒間 隙為人射光之波長。在搭載於_關器等例如手 機上之小型LCD等中,係期望更加降低電力消耗、並降低 驅動電壓等,而從第U圖可知,在例如上述⑴之值為u 之液晶盒中,用以實現最大穿透率之施加電壓係⑽左右即 :,如果增大其值為U、12 _,可使驅動㈣為未滿 3V。透過調整d值而使用同樣之液晶材料、同—光源時, 也可進行非常低之電壓驅動,d值如第i _、第2圖等所 不,可由_調整部34〇、彩色濾、光層咖 層38之厚料明整。 317049D1D1 29 201109786 △另外,攸式(〇具有“Wl”成分理解可知,在本實施 態之LCD中,其穿透特性具有波長依存性。第12圖中,在 將R、G、B之各像素之全部液晶層之厚度(液晶盒間隙^ 設為一定時,相對於施加電壓之穿透率特性對於 R(630nm)、G(550nm)、B(460nm)光之相異點。相對此,第 13圖表示如第!圖所示藉由在每一 r、g、b改變例如彩色 濾光層330r、330g、330b(可由間隙調整部34〇之厚度予 以調整)之厚度而調整了液晶盒間隙d之值之LCD施加ς壓 與穿透率之關係。由第13圖可知,藉由將晶盒間隙㈣只、 G、Β分別設定為期望之值,而可對R、G、Β任意光對於所 對應之各像素之施加電壓之穿透率特性均相同。因此,採 用該種構成,可知可藉由如上述第u圖所示之不到…之 施加電壓’且可將R、G、B以同一振幅之顯示信號驅動。 另外,第14圖及第15圖表示色度(CIEiX —γ座標) 之施加電壓依存性。其中第14圖為如第12圖所示,使液 晶盒間隙在R、G、Β相同時之LCD中,將施加於液晶之電 壓設定為1.5V、2.0V、2. 3V、2. 6V、3. 0V時之色度之變化, 第15圖為如第13圖所示,在R、G、B分別調整液晶盒間 隙而對於施加電壓之穿透率變化之色度依存性之内之LCD 中,將施加於液晶之電壓同樣設為15V、2.〇v、2.3V、2 6V、 3. 0V時之色度之變化。由第14圖與第15圖之比較可知, 藉由在R、G、Β分別調整液晶盒間隙,可改善改變色度之 施加電壓依存性,亦即施加電壓時之色度偏離,而在各種 電壓範圍内驅動時均可實現色度偏離較小之LCD。 30 317049D1D1 201109786 [實施形態2] 接著’說明本發明之實施形態2,即謀求在色彩顯示 中提高顯示品質之態樣。以下,以垂直配向型液晶顯示裝 置之色彩顯示為例進行說明。 垂直配向型液晶顯示裝置,具有廣視角特性,以及高 對比度特性’並具有不需要配向膜的磨擦處理之優點。 在相關垂直配向型液晶顯示裝置中,由於液晶具有負 介電率異向性之特性,因此構成液晶之液晶分子具有朝向 與電場方向垂直之方向之特性。這種液晶顯示裝置係採用 垂直配向膜作為控制液晶之初期配向之配向膜,並使用例 如聚醯亞胺(p〇lyimide)、聚醯胺(p〇lyamide)等有機材料 作為該垂直配向膜之材料。在垂直配向型液晶顯示裝置 中,在沒有施加於液晶之電場時,液晶分子係藉由垂直配 向膜而被控制成朝向垂直配向膜所形成之基板之法線方 向。而當在像素電極與共通電極間施加電壓,從而產生基 φ板之法線方向之電場時,有這些電場控制之區域的液晶分 子則倒向垂直於電場之方向。 藉此,傳送至液晶中之入射光之相位會發生變化。當 將夾住液晶之基板間之距離⑽隙)#做d、將液晶之折射 率當做Δη、將光波長當做λ,則傳送至液晶中之入射光之 相位,化為Δικί/λ。接著,藉由使穿透過液晶之光通過貼 附於則述基板之偏光板,可使入射光之穿透率變化,而可 獲得所希望之液晶顯示。在這種情況中,例如,係設定前 述偏向偏光板,俾在無電壓施加時進行黑顯示,並在電壓 317049D1D1 31 201109786 施加時,以一定電壓(白電壓White)使入射光之穿透率為 最大。 有關該種垂直配向型液晶顯示裝置,最近亦正開發復 具有RGB3原色之像素之全彩之垂直配向型液晶顯示裝置。 但是,全彩垂直配向型液晶顯示裝置中,由於通過依 RGB3原色各像素不同之顏色之彩色濾光層之光的波長入, 係根據各像素不同而不同,因此無法以一定電壓使穿透率 為最大。亦即,如第17C圖所示,依各RGB像素,V-Τ特 性(穿透率對液晶施加電壓之特性)係不同。V--T特性中, 穿透率T隨著液晶施加電壓v的增加而增加,若超出最大 值,則轉向減少。一般在RGB中,係配合以最低電壓而穿 透率T變高之B(藍),而設定白電壓Vwhite作為液晶施加 電壓V。 在施加該白電壓Vwhite時,由於G(綠)與R(紅)沒有 達到10(U之穿透率,因此產生白色會被識認為偏藍之問 題。因此,使β像素之液晶施加電壓(驅動電壓)變高,雖 可文α此種色偏之問題,但將產生液晶顯示裝置之消費電 力增大的問題。 第16圖係有關本發明之實施形態2之垂直配向型液晶 顯不裝置之剖面圖。其中,與前述實施形態i(特別是第1 圖)^通構成者係附上相同符號,並省略說明。本實施形態 2與月ij述實施形態i相㈤’係以在作為腳3原色之顯示用 ^各個相應像素内,具備穿透區域以及反射區域,而無論 周圍%境是明亮或昏暗都方便觀察之半穿透型lCD為例進 32 317049D1D1 201109786 .行說明’然而也適用於具備RGB3原色之像素之穿透型lCD 或反射型LCD。 在第破螭基板1〇〇上,在RGB3原色之各像素内,分 別形成有液晶驅動用m20,並形成有覆蓋這些液晶驅動 用TFT20之層間絕緣膜(在其上形成平坦化絕緣膜則更 佳)34。該層間絕緣膜34上之各像素區域内,形成有像素 電極200在牙透區域係由ITO構成之透明電極21〇形成 像素電極2〇〇,在反射區域則由例如紹等具良好反射特性 •之材料構成之反射電極220形成像素電極2〇〇。 在B像素中,反射電極220(bhf、透過形成於層間絕緣 膜34之接觸孔與液晶驅動用TFT2〇i源極或汲極相連接, 反射電極220並與透明電極210接觸並電性連接。同樣, 在G像素、R像素中,反射電極220亦分別透過形成於層 間絕緣膜34之接觸孔而連接於液晶驅動用TFT20之源極或 汲極,反射電極220並與透明電極210接觸並電性連接。 鳙當反射電極220與透明電極210之直接接觸有困難之情 況,如前述對第6圖所做之說明,較宜將反射電極220實 際上與TFT20絕緣’並直接覆蓋反射電極220而在1像素 區域全體形成由透明導電性金屬氧化物構成之透明電極 210,透明電極210係透過接觸孔與TFT20連接。 形成由例如聚醯亞胺、聚醯胺等有機材料構成之第一 垂直配向膜262’覆蓋各像素之透明電極210、反射電極 220。 此外’與前述第一玻璃基板100相對之第二玻璃基板 33 317049D1D1 201109786 300係配置成與基板loo平行。在第二玻璃基板3〇〇之與 第一玻璃基板100之相對面,對應於RGB3原色之各像素, 而將來自第二基板300側或來自如第1圖所示之配置於第 一基板100側之光源、或是來自第二基板3〇〇側之外光之 光源之入射至液晶層400,並射向第二玻璃基板200的入 射光進行過濾。且形成有使藍色光透過之B色濾光層 332b、使綠色光透過之G色濾光層332g、以及使紅色光透 過之R色濾光層332r。 並且’在各像素之各反射區域中,對應B色濾光層332b 之反射區域之區域係形成有由感光性樹脂形成之突出部 340b ’對應G色遽光層332g之反射區域之區域係形成有由 感光性樹脂形成之突出部340g、對應R色濾光層332r之 反射區域之區域係形成有感光性樹脂形成之突出部340r。 這些突起部340(340b、340g、340r)係為在實施形態1中 亦有說明之在反射區域與穿透區域中,用於調整所要求之 間隙之間隙調整層(間隙調整用突出部),藉由將該間隙調 整層340選擇性地設置於反射區域,使反射區域之第一坡 璃基板100與第二玻璃基板300之相向距離(間隙)比透明 區域更小,使反射特性良好(在反射區域之顯示特性)。此 外,在本例中,在R、G、B之各像素中,突出部340之厚 度係設為共通。 再者,覆蓋分別設置有突出部340之B色濾光層332b、 G色濾光層332g以及R色濾光層332r,而形成由ΠΟ構成 之透明共通電極320,再覆蓋該共通電極320而形成由例 34 317049D1D1 201109786 如聚醯亞胺、聚醯胺等有機係材料構成之第2垂直配向膜 264。然後,在第一玻璃基板1〇〇與第二玻璃基板300間之 空間,封入具有負介電率異向性之液晶400。 第一玻璃基板100之背面(光之射出面)係貼附有作為 相位差板之λ /4板111以及偏光板112。同樣,在第二玻 璃基板200之背面(光射出面)係貼附有作為位差板之;1/4 板111以及偏光板112。藉此,設定成:依據像素電極以 及共通電極214之電壓設定,在液晶400無電壓施加時, • 朝液晶層400射入之入射光不會從第二玻璃基板300側向 外部射出通過,從而實現黑顯示;而當電壓施加於液晶層 400時,對應該電壓之來自第二玻璃基板300侧而向外部 射出之光會增加,亦即入射光於液晶層之穿透率會增加。 在本實施形態2中,其特徵為Β、G、R之各彩色濾光 層之332b、332g、332r之厚度設定。當使Β色濾光層332b 之厚度為D-blue、G色濾光層332g之厚度為D-green、R Φ 色滤光層332r之厚度為D-red時。 則滿足D-blue2 D-green〉D-red之關係式。在RGB之 各像素之穿透區域中,間隙(夾於兩基板間之液晶厚度)與 各彩色濾光層之大小關係成為相反關係。即,當使B像素 之透明區域之間隙為G-b 1 ue (T)、G像素之透明區域之間隙 為G-green(T)、R像素之透明區域之間隙為G-red(T)時, 其關係為 G_red(T)2G_green(T)>G-blue(T)。這樣,將 B 色濾光層201、G色濾光層202、R色濾光層203之厚度設 定成各不相同’使各像素之間隙(也稱為液晶盒間隙)不 35 317049D1D1 201109786 同 可使RGB之各像素的ν—τ特性均一化。 所 -接著,有關職之各像素之ν_τ特性,根據第 不之實驗結果進行說明。第17Α至17c圖中,橫 於液晶300之電壓,縱軸為入射光之穿透率。 為施加 首先,如第17C圖所示’在卜以此邛一灯洗耵叻 情況(所有彩色濾光層厚度相同之情況),各RGB之^如之 性大大不同,如第17A圖所示,若設定為D_Mue〉D〜〜了特 D-red,則B、R像素之ν-τ特性接近G像素之v〜t :eer〇 並且,藉由B色濾光層332b ' G色濾光層332g、以及 濾光層332r之厚度設定,將RGB之各間隙执^色 G-red(T)=4. 8 // m、G-green⑺=4. M m、G_M此定為 // m,從而可使RGB之V-T特性為大致相同。藉此,)==3· 3 擇適當的白電壓White(例如,使穿透率為最大曰之電厂I由選 可在低電壓驅動下,獲得無色偏之顯示。 墼v), ^reen) 而R像 # ’與第I% 獲 此外,如第17B圖所示,若設定為D_Mue=D〜 D-red,則B、G像素之V-T特性與第1孔圖相同, 素之V-T特性係接近G像素之v-T特性。這 圖之V-T#性相比,由於在R像素可藉由更低之電: 得高穿透率,這樣可改善色偏問題。 k 另一方面,在反射區域中,設有各RGB像素之严、 整層(突起部)340r、340g、340b,而前述B、G、R 4隙調 濾光層332b、332g、332r係同時存在於穿透區域以色 區域。因此藉由如前所述地分別設定這些色滹、光声此射 332g、332r之厚度,使反射區域之間隙大小關係^與穿透 317049D1D1 36 201109786 區域之關係成為相同之關係。亦即,若使反射區域之B像 素間隙為G-blue(R)、G像素之間隙為G_green(R)、R像素 之間隙為G-red(R) ’而突起部211、212、213之高度為相 同的話,則成為 G-red(R)>G-green(R)gG-blue(R)之關 係。於是,根據本實施形態2,RGB之各像素之V-R特性(反 射率對液晶施加電壓特性)也更均一,因而同樣可獲得在低 電壓驅動下之無色偏顯示。 其次,說明有關前述r、G、B之各色濾光層332r、332g、 _ 332b之形成方法。各色濾光層基本上係將包含該色顏料之 感光性樹脂旋轉塗布(spin coat)於第二玻璃基板300上, 並藉由曝光以及顯影,將圖形留在所定區域即可。但是, 本實施形態2中,由於各色濾光層厚度並非完全相同,如 果厚的色濾光層’例如B色濾光層332b先形成,則第二玻 璃基板300表面之凹凸會變大,而使其他彩色濾光層,例 如R色濾光層332r的形成產生困難。 φ 於此’首先形成最薄之R色濾光層332r,之後以G色 遽光層332g、B色濾光層332b之順序形成,這種製造步驟 較容易實現,且較為理想。在B色濾光層332b與G色濾光 層332g厚度相同之情況下,該厚度相同之2種色濾光層, 其形成順序任意。 [實施形態3] 接著’參照圖進行有關本發明之實施形態3的說明。 第18圖係有關本實施形態3之垂直配向型液晶顯示裝置之 概略剖面構造示意圖。有關與前述實施形態2共通之構成 37 317049D1D1 201109786 係附上相同符號,並省略說明。 在實施形態3中’在R、G、B之各像素,為了將各個 間隙G設為最適當之不同厚度,除了形成於第二玻璃基板 300側之R、G、B之色攄光層330r、330g、330b、以及用 於調整穿透區域與反射區域之間隙差之突起部340(340r、 340g、340b)外,還具備用於調整R、G、B用之間隙差之調 整層(間隙層)350。具體而言,在液晶盒間隙G係要求比R 像素區域更小之B、G像素區域中,將各個感光性樹脂層 350b、350g選擇性的形成於B色濾光層330b上、以及G 色濾光層330g上,而作為調整層350。於此,使B色濾光 層330b上之感光性樹脂350b之厚度為tl,G色濾光層330g 上之感光性樹脂350g之厚度為t2。此外,如果使B像素 之穿透區域之間隙(兩基板間之液晶厚度)為G-blue(T), 則設定為tigt2。若使G像素之穿透區域之間隙為 G-green(T) ’ R像素之穿透區域之間隙為G_red(T),則滿 足: G-red(T)>G-green(T)2G-blue(T)之關係。 此外,在本實施形態3中,如第18圖所示,使在各 色濾光層330r、330g、330b之厚度分別相同,且突出部 340r、340g、340b之厚度也分別相等之情況下,在>^42 時’液晶盒間隙滿足G-green=G-blue。 這樣,在必要色區域選擇性形成感光性樹脂層35〇, 將各像素之間隙(又稱為液晶盒間隙)依R、G、B分別設為 不同之最適合之值,可使RGB之各像素之ν_τ特性均一化。 317049D1D1 38 201109786 其次根據第19A圖至第19C圖所示之實驗結果,對有The active layer 20 of the TFT is covered by a gate insulating film 3, and a gate electrode 32 made of a high-melting-point metal material such as Cr or Mo and serving as a gate line is formed on the gate insulating film 30. After the gate electrode 32 is formed, the gate electrode 32 is used as a mask to form source and drain regions 2〇s, 2〇d for doping the impurities in the active layer 2, and to form The channel area 20c is not doped with impurities. Next, an interlayer insulating film 34 is formed by covering the entire TFT 〇, and after the interlayer insulating film 34 is formed with a contact hole, an electrode material is formed, and the source electrode 4 分别 is connected to the p Si active layer 20 through the contact hole. The source region is 2〇s, and the drain electrode is connected to the pole region. Further, in the present embodiment, the gate electrode 36 serves as a signal line for supplying a data signal corresponding to the display content to each of the TFTs 11G. On the other hand, the source (four) electrode 40 is connected to the first electrode 200 as a pixel electrode as will be described later. Further, both the gate electrode % and the source electrode 4 are made of a south conductivity such as A1 or the like. After the source electrode 40 and the electrode electrode 36 are formed, the substrate is entirely covered and becomes a flat insulating film 38 made of a resin material such as an acrylic resin. A hole is formed in a region where the source electrode 4G of the flat insulating film 38 is formed, and a metal layer for connection is formed in the contact hole, and the source 40 and the metal layer 42 are connected. When the source electrode 4 is made of germanium or the like, the layer 4 is made of a metal material such as Mo. It becomes a good ohmic contact with the gold U Γ. Furthermore, it is also possible to omit the source contact layer 42 and the TFT 11° active layer 2° phase-touch' and the W metal can establish an ohmic connection with the semiconductor material 317049D1D1 23 201109786 into the layer of the connection metal layer 42 4 • After the bell is applied, the reflective material layer having a good reflection characteristic such as Ab Nd alloy or Al is used for the laminated reflection layer in the entire substrate. The layer of the reflective material layer is removed from the vicinity of the source region of the TFT (the region in which the metal layer 42 is formed), and does not interfere with the contact between the metal layer 42 and the pixel electrode 2 后面 and tft formed later and simultaneously (10) The removal 俾 does not remain in the penetration region, and a reflective layer 44 of a diamond pattern is formed in the reflection region 220 of each pixel as shown in FIG. 3 described above. Further, in order to prevent leakage current from being generated by irradiating light to the TFT (especially, the channel region 20c), and in order to maximize the reflectable region (i.e., display region), in the present embodiment, as shown in FIG. The reflective layer 44 is also actively formed in the region above the channel of the TFT 11 . When the patterning of the reflective layer 44 is performed, the metal layer 42 composed of the above M〇 or the like has a sufficient thickness (for example, 0.2 Å, and has sufficient resistance to the etching liquid. Therefore, the metal layer 42 is formed thereon. After the reflective layer 44 is subjected to etch removal, the metal layer 42 may not be completely removed and remain in the contact hole. Further, in many cases, the source electrode 40 or the like is made of the same material as the reflective layer 44 (A1, etc.) In the case where the metal layer 42 is not present, the source electrode 40 is immersed in the remaining layer of the reflective layer 44 to cause disconnection or the like. However, the present embodiment can be tolerated by providing the metal layer 42. The patterning of the reflective layer 44 can maintain a good electrical connection with the source electrode 40. After the patterning of the reflective layer 44, the entire surface of the substrate containing the reflective layer 44 is coated by sputtering a transparent conductive layer. Here, as described above, the surface of the reflective layer 44 composed of A1 or the like is covered with an insulating natural oxide film at this time, and the surface of the isothermal melting point metal is not exposed even in the sputtering environment, 317049D1D1 24 201109786 ' Will oxidize. Therefore, The exposed metal layer 42 of the contact region may have an ohmic contact with the transparent conductive layer for the pixel electrode laminated on the metal layer 42. Further, after the film is formed, the transparent conductive layer is independent of each pixel, and The pixel region 200 is formed by patterning into an elongated hexagonal shape, as shown in FIG. 3, for example, in a pixel region. The pixel electrode 200 is patterned and covered. An alignment film 260 made of polyimide or the like is formed on the entire surface of the substrate to complete the first substrate side. Then, R, G, and B as shown in Fig. 1 and Fig. 2 are formed on the second substrate 300. The color filter layer, the common electrode 320, the gap adjusting portion 340, the protrusions 510 (510r, 510t), and the alignment film 260 formed by covering the elements, and the second substrate 300 and the first substrate 100 are fixed. The spacers are separated and bonded to the peripheral portion of the substrate, and the liquid crystal is sealed between the substrates to obtain an LCD. Further, in the examples of FIGS. 1 and 2, the common electrode 320 formed on the second substrate 300 side is formed. In the gap adjustment unit 340 The layer Φ is formed at a desired position of the common electrode 320. On the other hand, as shown in FIG. 4, the common electrode 320 may be formed below the gap adjusting portion 340 as shown in FIG. 4 ( Actually, between the color filter layer formed on the second substrate 300 and the gap adjusting portion 340. When the gap adjusting portion 340 is very thick, as shown in FIG. 4, the common electrode 320 is formed under the gap adjusting portion 340. Thereafter, the effective voltage applied to the liquid crystal layer 410 becomes lower, but in the case where a very high voltage is applied between the common electrode 320 and the pixel electrode 200, or in the case where the gap adjusting portion 340 is not too thick The composition shown in Fig. 4 can also be used. 25 317049D1D1 201109786 Next, another example of the configuration of each pixel of the transflective LCD of the present embodiment will be described. Fig. 7 is a basic plan configuration of a semi-transmissive type lcd of another example, and Fig. 8 is a basic sectional structure of the line along c-c of Fig. 7. Further, along D-D of Fig. 7, the basic cross-sectional structure of the line is the same as that of the basic cross-sectional structure shown in Fig. 5. The same as the above-mentioned FIG. 3 is that the shape of the pixel electrode 240 is rectangular in the example of FIG. 7, and in the area of each of the penetrating region 210 and the reflecting region 220, A projection portion _ which is a slightly U-shaped portion is formed at a position corresponding to the quadrangular oblique side thereof, and serves as an alignment control portion 500. According to the alignment control unit 5, in the penetration region 210 and the reflection region 220, the projections 51〇t and 51〇r are used as the boundary, and four regions in which the alignment directions of the liquid crystals are different are formed, thereby further expanding. Perspective. Further, as described above, the alignment control unit 500 of the inclined surface portion 520 by the gap adjustment portion 34 is formed on the second substrate 300 side at the boundary between the penetration regions 21A in the pixel region, and the oblique portion is simultaneously formed 52 〇 and an electrodeless portion (slit: window s) 53 extending in the horizontal scanning direction is formed on the pixel electrode 200. Therefore, in the parent region of the penetration region 21A and the reflection region 22A, the initial alignment of the liquid crystal is controlled by the slope of the gap adjustment portion 34 (the inclined portion 5 2 0) on the second electrode side. In the direction perpendicular to the inclined surface, the alignment of the liquid crystal is controlled to be different from the boundary of the electrodeless portion 530s by the inclination of the weak electric field as shown in FIG. 8 on the first substrate side by the electrodeless portion 53〇s. Direction angle. Therefore, the alignment of the liquid crystal in the vicinity of the boundary between the penetrating region 210 and the reflective electrode 220 can be more surely performed. 3I7049D1D1 26 201109786 . As described above, the number of patterns and the number of divisions of the alignment control unit 5 formed by the edge of the pixel electrode 200, the protrusion portion 51A, and the electrodeless portion 530s are different from those in the third embodiment. However, in the form shown in Fig. 7, the alignment azimuth of the liquid crystal controlled by the alignment control unit 5 is also the other than the projection line having the projection line with the alignment control unit 500 on the substrate plane. The angular difference of the alignment azimuth of the liquid crystal controlled by the alignment control unit 500 is less than 9 degrees at any intersection. Therefore, ® can surely prevent the occurrence of a misalignment at an indefinite position in each of the divided alignment regions. In addition, by using the pattern ' of the alignment control unit 500 shown in the third figure and the seventh figure, the minimum number of alignment divisions can be achieved through the formation of the minimum alignment control unit 5; . In the vertical alignment type liquid crystal used in the present embodiment, it is displayed in black in a voltage non-applied state (ie, a vertical alignment state), and not only in the gap between the pixel electrodes 2, but also in other alignments. The position directly above the control unit 5 (the protrusion 51 〇, the slanted portion 520, and the slit 530 s) is almost in a state where a sufficient voltage is applied between the common electrode 320 and the pixel electrode 200, and the liquid crystal alignment state is hardly observed. Will change from the vertical alignment state without affecting the display. Therefore, the arrangement of the useless alignment control unit 5 causes [the aperture ratio of the CD to decrease. However, in the case of the design shown in Figs. 3 and 7 described above, the aperture ratio can be minimized, and the viewing angle can be enlarged and the display quality can be improved. Fig. 9 and Fig. ○ show other modifications of the configuration shown in Fig. 3, respectively. 27 317049D1D1 201109786 Firstly, in Fig. 9, all the pixel electrodes 25A are formed into an arrow shape, wherein the shape and configuration of the reflection area 220 are the same as those of the third figure, but the difference is that 'the pattern is added to the remaining penetration area. It is a drum type or a slightly hourglass shape that is arranged in the horizontal direction or a shape in which the M characters are connected in the upper and lower directions. The projection line of the protrusion 51Gt on the plane intersects the two sides of the pixel electrode 25 of the transparent region 210 intersecting the projection line on the same plane at an angle greater than 9 degrees (here, 135 degrees) . As described above, since the liquid crystal molecules have no characteristic difference in the long-axis direction, the difference in the alignment azimuth angle of the liquid crystal in the cross-region is still less than 9 4 4, and the position of the division and the protrusion 510t is at the same position. The angle between the two sides of the lower portion of the pixel electrode 25A extending toward the lower end of the two sides of the pixel electrode 250 extending in the vertical scanning direction and the side of the pixel f-pole 25Q along the vertical scanning direction is less than 9 degrees. The maximum difference in the alignment S-bit angle of the liquid crystal in this region is also less than 90 degrees (in the example of Fig. 9, it is smaller than 45 degrees). Therefore, it is possible to prevent the occurrence of the disclination line at the indefinite position in the two alignment regions in the penetration region 21A. In FIG. 10, the shape of the pixel electrode 252 is an arrow feather shape, and the shape of the penetration region 210 (arrow shape) and the configuration are the same as those of the third figure, but the remaining reflection regions 220 of the pixel electrode 252 of the arrow feather shape are The shape, and the position at which the protrusions 510r for dividing the alignment of the liquid crystals in the region are formed are different. That is, in the example of the first diagram, the reflection region 220 is also in the shape of an arrow with a short length, and the boundary between the reflection region 220 and the penetration region 210 is aligned by the V-shaped inclined portion 520 of the gap adjustment portion 340. The segmentation is formed on the substrate side (the gap adjustment portion) on the second 28 317 049 D1D1 201109786 substrate side on the line connecting the apex of the V-shaped vertices and the apex of the same V-shaped apex of the pixel electrode 252 in the reflection region 220 along the vertical scanning direction. The portion 51 〇r has the projection portion 51 〇r as a boundary, and the reflection region 220 is formed with two right and left alignment regions in the horizontal scanning direction. In this configuration, the alignment azimuth of the liquid crystal controlled by which alignment control unit 5 is the other alignment control unit 5 that is a projection line that intersects the projection line of the alignment control unit 5 toward the substrate plane. The angular difference of the alignment azimuth of the liquid crystal controlled by 〇 satisfies the relationship of less than 9 degrees, so that good alignment can be performed. Next, the dependence of the driving voltage, the transmittance, and the wavelength of the vertical alignment type transflective LCD of the present embodiment will be described. Figure 11 is a view showing the relationship between the applied voltage (v) and the transmittance (arbitrary unit) applied to the liquid crystal, and is an optical characteristic of the vertical alignment liquid crystal cell indicated by - in other words, when the structure of the liquid crystal cell is changed. The relationship between voltage and penetration. Among them, in the u-th picture, 纣 is 55〇nm (green). In the above formula (1), (del - n) is a birefringence (i.e., refractive index anisotropy) (Δη) of the liquid crystal layer, and d is a thickness of the liquid crystal layer (the cell gap is a wavelength of human light). In a small LCD such as a mobile phone, etc., it is desirable to further reduce power consumption and lower the driving voltage, etc., and it can be seen from the U-picture that, for example, in the liquid crystal cell having the value of (1) above, the maximum penetration is achieved. The applied voltage is about (10): if the value is U, 12 _, the drive (4) can be less than 3 V. When the same liquid crystal material and the same light source are used to adjust the d value, it can be performed very much. Low voltage drive, d value such as the i-th, the second figure, etc., can be made by the thickening of the _ adjustment part 34 〇, color filter, light layer coffee layer 38. 317049D1D1 29 201109786 △ In addition, 攸 type (〇 It is understood from the understanding of the "Wl" component that in the LCD of the present embodiment, the penetration characteristics have wavelength dependence. In Fig. 12, the thickness of all liquid crystal layers of each pixel of R, G, and B (cell gap) ^ When set to a certain value, the transmittance characteristic with respect to the applied voltage is for R (630nm) ), the difference between G (550 nm) and B (460 nm) light. In contrast, Fig. 13 shows that, for example, the color filter layers 330r, 330g are changed at each r, g, b as shown in Fig. The relationship between the applied pressure and the transmittance of the LCD is adjusted by the thickness of the liquid crystal cell gap d by the thickness of the 330b (adjustable by the thickness of the gap adjusting portion 34). As can be seen from Fig. 13, by the cell gap (four) , G, and Β are respectively set to the desired values, and the transmittance characteristics of the applied voltages of the R, G, and Β arbitrary lights for the corresponding pixels are the same. Therefore, by adopting such a configuration, it can be known that The above-mentioned FIG. 5 is less than the applied voltage ' and can drive R, G, and B with display signals of the same amplitude. In addition, FIGS. 14 and 15 show the application of chromaticity (CIEiX - γ coordinate). The voltage dependence is set to 1.5V, 2.0V, 2. 3V, and the voltage applied to the liquid crystal is set to be the same as in the case of R, G, and Β. 2. The change of chromaticity at 6V, 3.0V, Fig. 15 is the adjustment of the cell gap in R, G, B as shown in Fig. 13 In the LCD in which the chromaticity dependence of the change in the transmittance of the voltage is changed, the voltage applied to the liquid crystal is also set to change in chromaticity at 15 V, 2. 〇 v, 2.3 V, 2 6 V, and 3. 0 V. As can be seen from the comparison between Fig. 14 and Fig. 15, by adjusting the cell gaps in R, G, and Β, the voltage dependence of the chromaticity change, that is, the chromaticity deviation when the voltage is applied, can be improved. In the case of driving in the voltage range, an LCD having a small chromaticity deviation can be realized. 30 317049D1D1 201109786 [Embodiment 2] Next, a second embodiment of the present invention will be described, that is, an aspect in which display quality is improved in color display. Hereinafter, the color display of the vertical alignment type liquid crystal display device will be described as an example. The vertical alignment type liquid crystal display device has a wide viewing angle characteristic and a high contrast characteristic' and has an advantage of eliminating the need for the rubbing treatment of the alignment film. In the related vertical alignment type liquid crystal display device, since the liquid crystal has a characteristic of negative dielectric anisotropy, the liquid crystal molecules constituting the liquid crystal have a characteristic of being oriented perpendicular to the direction of the electric field. The liquid crystal display device uses a vertical alignment film as an alignment film for controlling the initial alignment of the liquid crystal, and uses an organic material such as p〇lyimide or p〇lyamide as the vertical alignment film. material. In the vertical alignment type liquid crystal display device, when no electric field is applied to the liquid crystal, the liquid crystal molecules are controlled to face the normal direction of the substrate formed by the vertical alignment film by the vertical alignment film. When a voltage is applied between the pixel electrode and the common electrode to generate an electric field in the normal direction of the substrate φ, the liquid crystal molecules in the regions controlled by these electric fields are reversed in the direction perpendicular to the electric field. Thereby, the phase of the incident light transmitted to the liquid crystal changes. When the distance (10) between the substrates sandwiching the liquid crystal is made to d, the refractive index of the liquid crystal is regarded as Δη, and the wavelength of light is regarded as λ, the phase of the incident light transmitted to the liquid crystal is converted into Δικί/λ. Then, by passing the light that has passed through the liquid crystal through the polarizing plate attached to the substrate, the transmittance of the incident light can be changed, and a desired liquid crystal display can be obtained. In this case, for example, the polarizing plate is set, the black display is performed when no voltage is applied, and the transmittance of the incident light is made with a certain voltage (white voltage White) when the voltage is applied at 317049D1D1 31 201109786. maximum. With regard to such a vertical alignment type liquid crystal display device, a full-color vertical alignment type liquid crystal display device having pixels of RGB3 primary colors has recently been developed. However, in the full-color vertical alignment type liquid crystal display device, since the wavelength of light passing through the color filter layers of different colors of the respective pixels of the RGB3 primary color differs depending on each pixel, the transmittance cannot be made with a certain voltage. For the biggest. That is, as shown in Fig. 17C, the V-Τ characteristics (the characteristics of the transmittance applied to the liquid crystal) differ depending on the RGB pixels. In the V--T characteristic, the transmittance T increases as the liquid crystal applied voltage v increases, and if the maximum value is exceeded, the steering decreases. Generally, in RGB, B (blue) having a high transmittance T is obtained at the lowest voltage, and white voltage Vwhite is set as the liquid crystal application voltage V. When the white voltage Vwhite is applied, since G (green) and R (red) do not reach 10 (the transmittance of U, white is generated as a problem of being bluish blue. Therefore, the liquid crystal of the β pixel is applied with a voltage ( The drive voltage is high, and although the color shift of the liquid crystal display device is problematic, the power consumption of the liquid crystal display device is increased. Fig. 16 is a vertical alignment type liquid crystal display device according to the second embodiment of the present invention. In the above-mentioned embodiment i (particularly in the first drawing), the same reference numerals will be given to the same components, and the description will be omitted. This embodiment 2 and the month ij describe the embodiment i (five)' The display of the primary color of the foot 3 uses the penetration area and the reflection area in each corresponding pixel, and the semi-transparent type lCD which is convenient to observe regardless of the surrounding % environment is an example of 32 317049D1D1 201109786. Applicable to a penetrating type lCD or a reflective LCD having pixels of RGB3 primary colors. On the first broken substrate 1a, liquid crystal driving m20 is formed in each pixel of the RGB3 primary color, and is formed to cover these liquid crystal driving An interlayer insulating film of the TFT 20 (more preferably, a planarizing insulating film is formed thereon) 34. In each pixel region of the interlayer insulating film 34, a transparent electrode 21 in which the pixel electrode 200 is made of ITO in the tooth-permeable region is formed. The pixel electrode 2 is formed, and in the reflective region, the pixel electrode 2 is formed by the reflective electrode 220 made of a material having good reflection characteristics, for example. In the B pixel, the reflective electrode 220 (bhf, transmission is formed in the interlayer insulation) The contact hole of the film 34 is connected to the source or the drain of the liquid crystal driving TFT2〇i, and the reflective electrode 220 is in contact with and electrically connected to the transparent electrode 210. Similarly, in the G pixel and the R pixel, the reflective electrode 220 is also transmitted through The contact hole formed in the interlayer insulating film 34 is connected to the source or the drain of the liquid crystal driving TFT 20, and the reflective electrode 220 is in contact with and electrically connected to the transparent electrode 210. When the reflective electrode 220 is in direct contact with the transparent electrode 210, In the case of difficulty, as described above for the description of FIG. 6, it is preferable to insulate the reflective electrode 220 from the TFT 20 and directly cover the reflective electrode 220 to form a transparent portion in the entire 1-pixel region. The transparent electrode 210 is made of an electric metal oxide, and the transparent electrode 210 is connected to the TFT 20 through the contact hole. The first vertical alignment film 262' made of an organic material such as polyimide or polyimide is formed to cover the transparent of each pixel. The electrode 210 and the reflective electrode 220. The second glass substrate 33 317049D1D1 201109786 300 opposite to the first glass substrate 100 is disposed in parallel with the substrate loo. The second glass substrate 3 and the first glass substrate 100 are disposed. The opposite surface corresponds to each of the pixels of the RGB3 primary color, and is from the side of the second substrate 300 or from the light source disposed on the side of the first substrate 100 as shown in FIG. 1 or from the side of the second substrate 3 The light source of the light is incident on the liquid crystal layer 400, and the incident light that is incident on the second glass substrate 200 is filtered. Further, a B color filter layer 332b for transmitting blue light, a G color filter layer 332g for transmitting green light, and an R color filter layer 332r for transmitting red light are formed. Further, in each of the reflection regions of the respective pixels, a region corresponding to the reflection region of the B color filter layer 332b is formed with a projection portion 340b formed of a photosensitive resin, and a region corresponding to the reflection region of the G color calender layer 332g is formed. A protruding portion 340g formed of a photosensitive resin and a protruding portion 340r formed of a photosensitive resin are formed in a region corresponding to the reflective region of the R color filter layer 332r. The protrusions 340 (340b, 340g, and 340r) are the gap adjustment layers (gap adjustment protrusions) for adjusting the required gap in the reflection area and the penetration area, as described in the first embodiment. By selectively providing the gap adjusting layer 340 in the reflective region, the opposing distance (gap) of the first glass substrate 100 and the second glass substrate 300 in the reflective region is made smaller than that of the transparent region, so that the reflection characteristics are good (in Display characteristics of the reflective area). Further, in this example, in each of the pixels of R, G, and B, the thickness of the protruding portion 340 is made common. Furthermore, the B color filter layer 332b, the G color filter layer 332g, and the R color filter layer 332r, respectively provided with the protrusions 340, are formed to form a transparent common electrode 320 composed of germanium, and then cover the common electrode 320. A second vertical alignment film 264 composed of an organic material such as polyimine or polyamine is formed in Example 34 317049D1D1 201109786. Then, a liquid crystal 400 having a negative dielectric anisotropy is sealed in a space between the first glass substrate 1A and the second glass substrate 300. A λ /4 plate 111 as a phase difference plate and a polarizing plate 112 are attached to the back surface (light emitting surface) of the first glass substrate 100. Similarly, a 1/4 plate 111 and a polarizing plate 112 are attached to the back surface (light emitting surface) of the second glass substrate 200 as a difference plate. Therefore, according to the voltage setting of the pixel electrode and the common electrode 214, when the liquid crystal 400 is not applied with voltage, the incident light incident on the liquid crystal layer 400 is not emitted from the second glass substrate 300 side to the outside, thereby When the voltage is applied to the liquid crystal layer 400, the light that is emitted to the outside from the side of the second glass substrate 300 corresponding to the voltage increases, that is, the transmittance of the incident light to the liquid crystal layer increases. In the second embodiment, the thickness of each of the color filter layers 332b, 332g, and 332r of Β, G, and R is set. When the thickness of the 滤 color filter layer 332b is D-blue, the thickness of the G color filter layer 332g is D-green, and the thickness of the R Φ color filter layer 332r is D-red. Then it satisfies the relationship of D-blue2 D-green>D-red. In the penetration region of each pixel of RGB, the relationship between the gap (the thickness of the liquid crystal sandwiched between the two substrates) and the color filter layers is inversely related. That is, when the gap between the transparent regions of the B pixels is Gb 1 ue (T), the gap between the transparent regions of the G pixels is G-green (T), and the gap between the transparent regions of the R pixels is G-red (T), The relationship is G_red(T)2G_green(T)>G-blue(T). Thus, the thicknesses of the B color filter layer 201, the G color filter layer 202, and the R color filter layer 203 are set to be different. [The gap between the pixels (also referred to as the cell gap) is not 35 317049D1D1 201109786 The ν-τ characteristics of each pixel of RGB are made uniform. - Next, the ν_τ characteristics of each pixel of the relevant position are described based on the experimental results. In the graphs 17 to 17c, the voltage is perpendicular to the liquid crystal 300, and the vertical axis is the transmittance of incident light. For the first application, as shown in Fig. 17C, the condition of each RGB is greatly different, as shown in Fig. 17A. If D_Mue>D~~ special D-red is set, the ν-τ characteristic of the B and R pixels is close to v~t of the G pixel: eer〇, and the color filter is filtered by the B color filter layer 332b′ The thickness of the layer 332g and the filter layer 332r are set, and the respective RGB gaps are G-red(T)=4. 8 // m, G-green(7)=4. M m, G_M is determined as // m Thus, the VT characteristics of RGB can be made substantially the same. By this,) ==3· 3 Select the appropriate white voltage White (for example, the power plant I with the highest penetration rate can be selected to drive at a low voltage to obtain a display without color shift. 墼v), ^reen And R like #' and the first I% are added. As shown in Fig. 17B, if D_Mue=D~D-red is set, the VT characteristics of the B and G pixels are the same as those of the first hole pattern, and the VT characteristic of the prime. It is close to the vT characteristic of G pixels. Compared with the V-T# property of this figure, since the R pixel can be used with lower power: high transmittance, the color shift problem can be improved. k On the other hand, in the reflection region, strict layers (projections) 340r, 340g, and 340b of the respective RGB pixels are provided, and the B, G, and R 4 filter layers 332b, 332g, and 332r are simultaneously Exist in the colored area of the penetrating area. Therefore, by setting the thicknesses of these pupils, photoacoustic projections 332g, and 332r as described above, the relationship between the gap size relationship of the reflection regions and the region of the penetration 317049D1D1 36 201109786 is the same. That is, if the B pixel gap of the reflection area is G-blue (R), the G pixel gap is G_green (R), and the R pixel gap is G-red (R) ', and the protrusions 211, 212, 213 When the height is the same, the relationship is G-red(R)>G-green(R)gG-blue(R). Therefore, according to the second embodiment, the V-R characteristics of each pixel of RGB (the reflectance is applied to the liquid crystal voltage characteristic) are more uniform, and thus the colorless display under low voltage driving can be obtained in the same manner. Next, a method of forming the respective color filter layers 332r, 332g, and 332b of the above r, G, and B will be described. Each of the color filter layers basically spin-coats the photosensitive resin containing the color pigment on the second glass substrate 300, and the pattern is left in a predetermined area by exposure and development. However, in the second embodiment, since the thicknesses of the respective color filter layers are not completely the same, if the thick color filter layer 'for example, the B color filter layer 332b is formed first, the unevenness on the surface of the second glass substrate 300 becomes large. It is difficult to form other color filter layers such as the R color filter layer 332r. φ is formed by forming the thinnest R color filter layer 332r first, and then forming it in the order of the G color light-emitting layer 332g and the B color filter layer 332b. This manufacturing step is relatively easy to implement and is preferable. When the B color filter layer 332b and the G color filter layer 332g have the same thickness, the two color filter layers having the same thickness are formed in any order. [Embodiment 3] Next, a description will be given of Embodiment 3 of the present invention with reference to the drawings. Figure 18 is a schematic cross-sectional structural view showing a vertical alignment type liquid crystal display device of the third embodiment. The configuration common to the above-described second embodiment is the same as the reference numeral 37 317049D1D1 201109786, and the description thereof is omitted. In the third embodiment, in each of the pixels of R, G, and B, in order to set the respective gaps G to the optimum thickness, the color light-emitting layer 330r of R, G, and B formed on the side of the second glass substrate 300 is provided. And 330g, 330b, and protrusions 340 (340r, 340g, 340b) for adjusting the gap difference between the penetration area and the reflection area, and an adjustment layer (gap) for adjusting the gap difference between R, G, and B Layer) 350. Specifically, in the B and G pixel regions where the cell gap G is required to be smaller than the R pixel region, each of the photosensitive resin layers 350b and 350g is selectively formed on the B color filter layer 330b, and the G color. The filter layer 330g is used as the adjustment layer 350. Here, the thickness of the photosensitive resin 350b on the B color filter layer 330b is t1, and the thickness of the photosensitive resin 350g on the G color filter layer 330g is t2. Further, if the gap of the penetration region of the B pixel (the liquid crystal thickness between the two substrates) is G-blue (T), it is set to tigt2. If the gap between the penetration areas of the G pixels is G-green(T)', the gap between the penetration areas of the R pixels is G_red(T), then: G-red(T)>G-green(T)2G -blue(T) relationship. Further, in the third embodiment, as shown in Fig. 18, when the thicknesses of the respective color filter layers 330r, 330g, and 330b are the same, and the thicknesses of the protruding portions 340r, 340g, and 340b are also equal, >^42' The cell gap meets G-green=G-blue. Thus, the photosensitive resin layer 35 is selectively formed in the necessary color regions, and the gaps (also referred to as cell gaps) of the respective pixels are set to the most suitable values according to R, G, and B, respectively. The ν_τ characteristics of the pixels are uniform. 317049D1D1 38 201109786 Secondly, according to the experimental results shown in Figures 19A to 19C,

關RGB之各像素之ν-Τ特性進行說明。在第19A圖至第19C 圖中,検輛係施加於液晶400之電壓,縱軸係入射光之穿 透率。 首先’如苐 19C 圖所示,在 G-red(T)=G-green(T)= G-blue(T)之情況(不設感光性樹脂層25〇g、25〇t)之情況) 中’各RGB之V-τ特性係大不相同。相對此,如第IgA圖 所示,若設定為The ν-Τ characteristic of each pixel of RGB is described. In Figs. 19A to 19C, the 系 is applied to the voltage of the liquid crystal 400, and the vertical axis is the transmittance of incident light. First, as shown in Fig. 19C, in the case of G-red (T) = G-green (T) = G-blue (T) (when the photosensitive resin layer 25 〇 g, 25 〇 t is not provided) The V-τ characteristics of each RGB are very different. In contrast, as shown in the IgA diagram, if set to

_ G-red(T)>G-green(T)>G-blue(T),則 B、R 像素之 V-T 特性係接近G像素之特性(無修正情況下,R、g、β之各特 性係分別如第19Α圖中的()所示)。更具體而言,藉由將 RGB 之各間隙設定為 G-red=4. 8 # m、G-greenM. 0 y m、 G-blue=3.3//m’可使RGB之V~T特性大致相同。這樣,藉 由選擇適當白電壓Vwhite(例如,穿透率成為最大之電壓 V),則可在低電壓驅動下,獲得無色偏之顯示。 • 此外,如第i9B圖所示,若設定為G-red(T)>G-green (T)=G-blue(T),則B、G像素之v-τ特性與第i9C圖相同, 而R像素之V-T特性係接近G像素之ν-τ特性。這樣,與 第19C 特性相比,在R像素中,由於可在更低電 壓V下獲得高穿透率,因此可改善色偏問題。 另一方面’在反射區域中,RGB之各像素設有突起部 340,由於係將該突起部340之厚度依卜〇、8而設定成相 等’反射區域之間隙大小關係亦為與穿透區域之前述關係 相同之關係。亦即,使反射區域之B像素之間隙為 317049D1D1 39 201109786 G-blue(R)、G像素之間隙為 Gneen(:R)、 G-i⑻的話,則成為:_η⑻㈠象素之間隙為 G-red^>G-green⑻乂 ^⑻之關係。 於疋’根據本實施形態’由於RGB之各像素之 性(反射率對液晶施加電壓特 ⑲ ' 壓驅動下,獲得無色偏之顯示。)更為均问樣可在低電 【圖式簡單說明】 半穿 透LCD之其他概略剖之垂直配向型半穿 態1之更具體之半穿透_ G-red(T)>G-green(T)>G-blue(T), the VT characteristics of B and R pixels are close to the characteristics of G pixels (R, g, β without correction) Each characteristic is as shown in () of Figure 19). More specifically, by setting the gaps of RGB to G-red=4.8. 8 # m, G-greenM. 0 ym, G-blue=3.3//m', the V~T characteristics of RGB are substantially the same. . Thus, by selecting the appropriate white voltage Vwhite (e.g., the voltage V at which the transmittance becomes maximum), the display without color shift can be obtained under low voltage driving. • In addition, as shown in the figure i9B, if G-red(T)>G-green (T)=G-blue(T) is set, the v-τ characteristics of the B and G pixels are the same as those of the i9C picture. The VT characteristic of the R pixel is close to the ν-τ characteristic of the G pixel. Thus, in the R pixel, since the high transmittance can be obtained at a lower voltage V than in the 19th characteristic, the color shift problem can be improved. On the other hand, in the reflective region, each of the RGB pixels is provided with a protrusion 340, and the thickness of the protrusion 340 is set to be equal to the gap size of the reflection region. The aforementioned relationship is the same. In other words, if the gap between the B pixels of the reflection region is 317049D1D1 39 201109786 G-blue(R), and the gap between the G pixels is Gneen (: R) or G-i (8), the gap between the pixels is: _η (8) (1) The gap between the pixels is G-red ^>G-green(8)乂^(8) relationship. According to the present embodiment, the performance of each pixel of RGB (the reflectance is applied to the liquid crystal by a voltage of 19', and the display of the colorless offset is obtained.) 】 More specific semi-transparent of the other vertical cross-section of the semi-transparent LCD

線之位置之半穿透型LCD 線之位置之半穿透型LCD 第4圖沿著第3圖之 之概略剖面構成的示意圖。 第5圖沿著第3圖之 之概略剖面構成的示意圖。 第6圖係表示第3圖所 及與其連接之TFT構成之概略過LCD之像素電極以 半^ 7圖係有關本發明之實施形態,並與第3圖不同之 、LCD之概略平面構成示意圖。 第8圖係沿著第7圖之c_c,線之位置之半穿透型^⑶ 既略剖面構成的示意圖。 第9圖係表示第3圖之半穿透型lcd之變形例之概略 40 317049D1D1 201109786 平面構成的示意圖。 第10圖係表示第3圖之半穿透型LCD之其他變形例之 概略平面構成的示意圖。 第11圖係本實施形態1之垂直配向型半穿透型[CD之 相對於施加電壓之穿透率特性與單元構造之關係之示意 圖。 第12圖係本實施形態1之垂直配向型半穿透型lcj)之 相對於施加電壓之穿透率特性之波長依存性之示意圖。 第13圖係本實施形態1之垂直配向型半穿透型[CD 中,在以R、G、B調整液晶盒間隙後,相對於施加電壓之 穿透率特性之波長依存性之示意圖。 第14圖係表示本實施形態丨之垂直配向型半穿透型 LCD之色度之相對於施加電壓之依存性之色度座標。 第15圖係表示本實施形態丨之垂直配向型半穿透型 LCD中,在以R、G、B調整液晶盒間隙後,色度之相對於 鲁施加電壓之依存性之色度座標。 第16圖係有關本發明之第2實施形態之垂直配向型液 晶顯示裝置之剖面圖。 第ΠΑ、17B、17C圖係表示各RGB像素之ν_τ特性與 液晶盒間隙關係之示意圖。 第18圖係有關本發明之實施形態3之垂直配向型液晶 顯不裝置之剖面圖。 第19Α、19Β、19C圖係表示RGB像素之ν_τ特性與液 晶盒間隙關係之示意圖。 317049D1D1 41 201109786 【主要元件符號說明】 20 主動層 30 32 閘極電極 34 36 汲極電極 38 40 源極電極 42 44 反射層 100 110 圓偏光板 111 112 偏光板 200 210 透明電極 220 260 配向膜 300 310 相位差板 320 330、330r、330g、330b 彩色濾光層 330BM 黑色遮光層 340 400 液晶層 410 500(530)配向控制部 510 520 傾斜部 600 閘極絕緣膜 層間絕緣膜 平坦化絕緣膜 金屬層 第一玻璃基板 λ /4板 第二玻璃基板 反射電極 鲁 第二玻璃基板 透明共通電極 間隙調整部 液晶指向 510t、510r 突起部 光源 42 317049D1D1 rs)The semi-transmissive LCD at the position of the semi-transmissive LCD line at the position of the line Fig. 4 is a schematic view taken along the schematic cross section of Fig. 3. Fig. 5 is a schematic view showing a schematic cross section of Fig. 3. Fig. 6 is a schematic plan view showing the schematic configuration of the LCD in the embodiment of the present invention, which is a schematic diagram of the pixel electrode of the LCD, which is composed of the TFT connected to the third embodiment, and which is different from the third embodiment. Fig. 8 is a schematic view showing a configuration of a semi-transparent type (3) along the c_c of Fig. 7, the position of the line. Fig. 9 is a schematic view showing a modification of the semi-transmissive type lcd of Fig. 3 317049D1D1 201109786. Fig. 10 is a view showing a schematic plan configuration of another modification of the transflective LCD of Fig. 3. Fig. 11 is a schematic view showing the relationship between the transmittance characteristics of the vertical alignment type semi-transmissive type [CD] with respect to the applied voltage and the cell structure. Fig. 12 is a view showing the wavelength dependence of the transmittance characteristics of the vertical alignment type semi-transmissive type lcj) of the first embodiment with respect to the applied voltage. Fig. 13 is a view showing the wavelength dependency of the transmittance characteristic with respect to the applied voltage after the liquid crystal cell gap is adjusted by R, G, and B in the vertical alignment type semi-transmissive type of the first embodiment. Fig. 14 is a view showing the chromaticity coordinates of the dependence of the chromaticity of the vertical alignment type transflective LCD of the present embodiment on the applied voltage. Fig. 15 is a view showing the chromaticity coordinates of the dependence of the chromaticity on the applied voltage after the liquid crystal cell gap is adjusted by R, G, and B in the vertical alignment type transflective LCD of the present embodiment. Figure 16 is a cross-sectional view showing a vertical alignment type liquid crystal display device according to a second embodiment of the present invention. The figures 17, 17B, and 17C show the relationship between the ν_τ characteristics of each RGB pixel and the gap of the liquid crystal cell. Figure 18 is a cross-sectional view showing a vertical alignment type liquid crystal display device according to Embodiment 3 of the present invention. The 19th, 19th, and 19thth drawings show the relationship between the ν_τ characteristic of the RGB pixel and the gap of the liquid crystal cell. 317049D1D1 41 201109786 [Description of main components] 20 Active layer 30 32 Gate electrode 34 36 Gate electrode 38 40 Source electrode 42 44 Reflecting layer 100 110 Circular polarizing plate 111 112 Polarizing plate 200 210 Transparent electrode 220 260 Alignment film 300 310 Phase difference plate 320 330, 330r, 330g, 330b Color filter layer 330BM Black light shielding layer 340 400 Liquid crystal layer 410 500 (530) Alignment control portion 510 520 Inclined portion 600 Gate insulating film Interlayer insulating film Flattening insulating film Metal layer A glass substrate λ / 4 plate second glass substrate reflective electrode Lu second glass substrate transparent common electrode gap adjustment portion liquid crystal pointing 510t, 510r protrusion light source 42 317049D1D1 rs)

Claims (1)

201109786 七、申請專利範圍: L -種液晶顯示裝置’係具 電極之第m 料並在具有像素 垂直配向型液晶ϊ =共通電極之第二基板間,封入有 2素的卿行方向長度比列方向長度長; 繞而八β素係猎由沿列方向延伸、彎曲成ν字狀的分界 :相_相賤第—像素區域與第二像素區域; 則述第-像素區域的端係切入前述第區 而形成; 前述第-區域的優先視角與前述第二像素區域的 優先視角不同。 2· ^申請專利範圍第1項之液晶顯示裝置,其中,前述第 一像素區域的優先視角係垂直於行方向;前述第二像素 區域的優先視角係垂直於列方向。 .如申1專利範圍第1項之液晶顯示裝置,其中,在前述 Φ 第像素區域中,液晶配向方向被分割成為兩個不同區 域,並且,在前述第二像素區域中,液晶配向方向被分 割成為兩個不同區域。 4. 如申請專利範圍第3項之液晶顯示裝置,其中,在前述 第一像素區域中,液晶配向方向被控制成朝向垂直於行 方向之方向,在前述第二像素區域中,液晶配向方向被 控制成朝向垂直於列方向之方向。 5. 如申請專利範圍第2項或第3項之液晶顯示裝置,其 中’前述第一像素區域的面積比前述第二像素區域的面 43 317049D1D1 201109786 積小。 ^液痛不裝置,係具備複數個像素,並在具有像素 ::之第-基板與具有共通電極之第二基板間,封入有 垂直配向型液晶,其中, 各像素的形狀係行方向長度比财向長度長; 各像素係藉由沿列方向延伸的分界線而分割成面 積相異的第-像素區域與第二像素區域; 在前述第-像素區域中,液晶配向方向被分割成為 四個不同區域’並且’在前述第二像素區域t,液晶配 向方向被分割成為四個不同區域。 7.如申5月專利範圍第6項之液晶顯示裂置,其中,前述第 -像素區域t的四個配向方向與前述第二像素區域中 的四個配向方向相同。 8·如申請專利範圍第6項之液晶顯示農置,其中,前述第 i素區域的四個區域與前述第二像素區域的四個區 域中的液晶的優先視角相同。 9.如申請專利範圍第6至8項中任一項之液晶顯示裂置, 其中’前述第-像素區域的面積比前述第二像素區域的 面積小。 317049D1D1 44201109786 VII. Patent application scope: L-type liquid crystal display device's the mth material of the electrode and the second substrate with the pixel vertical alignment type liquid crystal ϊ = common electrode, sealed with a length of 2 The length of the direction is long; the occlusion of the octagonal system is defined by a boundary extending in the column direction and bent into a ν-shape: a phase _ phase-pixel region and a second pixel region; Formed by the first region; the priority viewing angle of the aforementioned first region is different from the priority viewing angle of the second pixel region. The liquid crystal display device of claim 1, wherein the preferential viewing angle of the first pixel region is perpendicular to the row direction; and the preferential viewing angle of the second pixel region is perpendicular to the column direction. The liquid crystal display device of claim 1, wherein in the Φ pixel region, the liquid crystal alignment direction is divided into two different regions, and in the second pixel region, the liquid crystal alignment direction is divided. Become two different areas. 4. The liquid crystal display device of claim 3, wherein, in the first pixel region, the liquid crystal alignment direction is controlled to be oriented in a direction perpendicular to the row direction, and in the second pixel region, the liquid crystal alignment direction is Control is oriented in a direction perpendicular to the column direction. 5. The liquid crystal display device of claim 2, wherein the area of the first pixel region is smaller than the surface of the second pixel region 43 317049D1D1 201109786. ^The liquid pain is not installed, and has a plurality of pixels, and a vertical alignment type liquid crystal is enclosed between the first substrate having the pixel:: and the second substrate having the common electrode, wherein the shape of each pixel is in the direction-to-direction ratio The length of the financial direction is long; each pixel is divided into a first-pixel area and a second pixel area having different areas by a boundary line extending in the column direction; in the first-pixel area, the liquid crystal alignment direction is divided into four The different regions 'and' in the aforementioned second pixel region t, the liquid crystal alignment direction is divided into four different regions. 7. The liquid crystal display cleaving according to item 6 of the patent scope of the fifth aspect, wherein the four alignment directions of the first pixel region t are the same as the four alignment directions of the second pixel region. 8. The liquid crystal display farm according to claim 6, wherein the four regions of the first pixel region and the liquid crystal regions of the four regions of the second pixel region have the same preferential viewing angle. 9. The liquid crystal display cleaving according to any one of claims 6 to 8, wherein the area of the aforementioned first-pixel region is smaller than the area of the second pixel region. 317049D1D1 44
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