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TWI333573B - Liquid crystal display - Google Patents

Liquid crystal display Download PDF

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Publication number
TWI333573B
TWI333573B TW95121088A TW95121088A TWI333573B TW I333573 B TWI333573 B TW I333573B TW 95121088 A TW95121088 A TW 95121088A TW 95121088 A TW95121088 A TW 95121088A TW I333573 B TWI333573 B TW I333573B
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Taiwan
Prior art keywords
refractive index
high refractive
index block
block
liquid crystal
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TW95121088A
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Chinese (zh)
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TW200801683A (en
Inventor
Pei Hsun Wu
Yingche Lan
Chihhaw Wang
Szu Han Li
Keng Ju Liu
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Au Optronics Corp
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Priority to TW95121088A priority Critical patent/TWI333573B/en
Priority to US11/785,976 priority patent/US8009251B2/en
Priority to KR1020070046794A priority patent/KR100857958B1/en
Publication of TW200801683A publication Critical patent/TW200801683A/en
Application granted granted Critical
Publication of TWI333573B publication Critical patent/TWI333573B/en
Priority to US13/192,776 priority patent/US8879028B2/en

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Description

1333573 九、發明說明: 【發明所屬之技術領域】 本發明是有關於一種液晶顯示器’且特別是有關於一 種高亮度之液晶顯示器。 【先前技術】1333573 IX. Description of the Invention: [Technical Field] The present invention relates to a liquid crystal display and particularly relates to a high brightness liquid crystal display. [Prior Art]

近年來光電相關技術不斷推陳出新,加上數位化時代 的到來’進而推動了液晶顯示器市場的蓬勃發展。液晶顯 示器(Liquid Crystal Displayer ; LCD)具有高畫質、體積小、 重量輕、低電壓驅動、低消耗功率及應用範圍廣等優點, 因此被廣泛地應用於可攜式電視、行動電話、筆記型電腦 以及桌上型顯示器等消費性電子或電腦產品,並逐漸取代 陰極射線管(Cathode Ray Tube ; CRT)成為顯示器的主流。In recent years, optoelectronic related technologies have been continuously introduced, and the arrival of the digital era has promoted the vigorous development of the liquid crystal display market. Liquid crystal display (LCD) is widely used in portable TVs, mobile phones, and notebooks because of its high image quality, small size, light weight, low voltage drive, low power consumption, and wide application range. Consumer electronics or computer products such as computers and desktop displays have gradually replaced cathode ray tubes (CRTs) as the mainstream of displays.

有繁於液晶本身並不會發光,因此需要使用背光模組 來供應光源,才能達到顯示效果。傳統的液晶顯示器大部 分為背光(Back-light)型液晶顯示器,主要包括前端的液晶 顯示面板以及後端的背光模組。 液晶顯示器的亮度是設計上重要的考量項目之一,傳 統上’提高液晶顯示器之亮度的方法不外乎是増加開口率 或是在背光模組中使用增亮膜。然而,若利用增加開口率 的方式來提高液晶顯示器的亮度時,不僅會提高製程的難 度,同時也會有增加成本負擔之問題。但是,若在背光模 組中使用多張光學膜片來提高亮度時,又會衍生出其他的 問題。例如,當光線在傳遞㈣程中,光線不僅會被這些 光學膜片部分吸收而降低了光線的使用率之外,更會因:The LCD itself does not emit light, so it is necessary to use a backlight module to supply the light source in order to achieve the display effect. Conventional liquid crystal displays are mostly classified into back-light type liquid crystal displays, which mainly include a liquid crystal display panel at the front end and a backlight module at the rear end. The brightness of liquid crystal displays is one of the important considerations in design. Traditionally, the method of increasing the brightness of liquid crystal displays is to increase the aperture ratio or use a brightness enhancement film in the backlight module. However, if the brightness of the liquid crystal display is increased by increasing the aperture ratio, not only the difficulty of the process will be increased, but also the cost burden will be increased. However, if multiple optical films are used in the backlight module to increase the brightness, other problems arise. For example, when light is transmitted (four), the light is not only absorbed by the optical film but reduces the use of light, but also because:

1333573 用多張光學膜片而造成材料與組裝成本的負擔。再者,這 些光學膜片更可能會在進行信賴性測試時,造成光學臈片 之間的括擦毁損,進而增加成本的負擔。此外,倘若這些 光學膜片配置不當時,則容易產生干涉條紋,發生疊紋效 應(moire effect) ’而造成視覺上的缺陷。1333573 The burden of material and assembly costs with multiple optical diaphragms. Moreover, these optical films are more likely to cause damage between the optical cymbals when performing the reliability test, thereby increasing the cost burden. Further, if these optical films are not properly arranged, interference fringes are likely to occur, and a moire effect is caused to cause visual defects.

有鑑於此,美國專利第6,421,1〇5號提出一種改善上述 缺點之方法,其係於液晶顯示面板中之上玻璃基板的表面 上製作微透鏡(micro lens)陣列,利用微透鏡的曲面結構來 提南液晶顯示器之亮度。然而’此方法之最大難處在於, 由於微透鏡之尺寸大小係微米級以下之尺寸,且其表面結 構為曲面結構,所以在製作上不容易控制。再者,因受限 於微透鏡之尺寸大小與結構,所以無法再藉由增加微透鏡 之曲面結構的曲度來更加增強液晶顯示器之亮度。 因此,如何在降低成本負擔的情況下,且能同時不增 加製程控制的難度’進而提高液晶顯示器的亮度,為目前 研發的重點之一。In view of the above, a method for improving the above disadvantages is proposed in U.S. Patent No. 6,421,1,5, which is to form a microlens array on the surface of a glass substrate in a liquid crystal display panel, using a curved surface structure of the microlens. To bring the brightness of the LCD screen. However, the biggest difficulty of this method is that since the size of the microlens is a size below the micrometer level and the surface structure is a curved surface structure, it is not easy to control in fabrication. Moreover, due to the size and structure of the microlens, it is no longer possible to increase the brightness of the liquid crystal display by increasing the curvature of the curved structure of the microlens. Therefore, how to reduce the cost burden and not increase the difficulty of process control at the same time, thereby increasing the brightness of the liquid crystal display, is one of the current research and development priorities.

【發明内容】 因此本發明的目的就是在提供—種液晶顯示器足以 產生下述目的其中至少其一。 本發明的目的就是在提供—種液晶顯示器,可用以減 少因遮光區而產生之光損耗,進而提高液晶顯示器之亮度。 本發明的另-目的是在提供—種液晶顯示器,可有效 地降低暗態漏光的現象’以增加液晶顯示器之對比。 本發明的又-目的是在提供—種液晶顯示器,可以減SUMMARY OF THE INVENTION It is therefore an object of the present invention to provide a liquid crystal display sufficient to produce at least one of the following objectives. SUMMARY OF THE INVENTION It is an object of the present invention to provide a liquid crystal display which can be used to reduce the loss of light due to a light-shielding region and thereby increase the brightness of the liquid crystal display. Another object of the present invention is to provide a liquid crystal display which can effectively reduce the phenomenon of light leakage in the dark state to increase the contrast of the liquid crystal display. Still another object of the present invention is to provide a liquid crystal display which can be reduced

1333573 少增亮膜之使用數量,進而降低成本負擔。 根據本發明之上述目的之中至少其一,提出一種液晶 顯不器。上述之液晶顯示器包含背光源、高分子膜層以及 液晶顯示面板,且高分子膜層係位於液晶顯示面板之下、 背光源之上。其中,高分子膜層具有複數個聚光陣列,每 一聚光陣列包含複數個高折射率區塊。其中一最寬的高折 射率區塊置於中央,其餘高折射率區塊係對稱分列於最寬 的咼折射率區塊兩側。且位於對稱位置之兩高折射率區塊 具有相同的寬度,高折射率區塊兩兩之間為一低折射率區 塊所分斷。液晶顯示面板具有複數個可透光區與複數個遮 光區,每一個聚光陣列係搭配一可透光區而設置,可透光 區係位於高分子膜層中之聚光陣列之上方。 其中’當光線穿過高分子膜層中之每一個聚光陣列且 到達聚光陣列中之高折射率區塊與低折射率區塊之介面上 時’高折射率區塊與低折射率區塊之介面上會形成反射現 象’並且通過聚光陣列之光線會產生聚光的效果,使得光 線集中於液晶顯示面板之可透光區中,進而提高液晶顯示 器之壳度。因此,高分子膜層不僅是一具有聚光效果之聚 光膜層’更可以將高分子膜層中之聚光陣列視為一具有集 中光%功能之凸透鏡。 依照本發明一較佳實施例,位於最寬的高折射率區塊 一側之高折射率區塊的寬度朝向遠離最寬的高折射率區塊 的方向逐漸縮減。且在本發明之較佳實施例中,聚光陣列 較佳係具有5個高折射率區塊,其排列方式由左至右依序 為第三高折射率區塊、第二高折射率區塊、第一高折射率 1333573 區塊、第二高折射率區塊以及第三高折射率區塊。其中, 第一高折射率區塊之寬度係大於第二高折射率區塊,第二 高折射率區塊之寬度係大於第三高折射率區塊。 因此,本發明係利用光線在不同折射率的介質之介面 上需滿足折射定律(Snell’s Law),讓入射光通過不同折射 率的介質之介面上時,產生反射現象而將光線反射至液晶 顯示面板之可透光區中,以減少因經過遮光區之光線損 耗,進而增加光線的使用_。再者,由於本發明之聚光陣 列中之高折射率區塊之尺寸係微奈米級以下,又加上高折 射率區塊之排列方式,所以當光線通過本發明之聚光陣列 的結構時,可以使光線產生聚光的功能,以進一步提高液 晶顯不is的免度。 除此之外,應用本發明之方法可以有效地降低暗態漏 光的現象,以增加液晶顯示器之對比。且本發明之方法不 僅可以減少增亮膜之使用數量,更可以降低成本負擔。本 發明之方法更可以讓穿過低折射率區塊之光線,在不同折 射率的介質之介面上產生折射的效果,使得光線更有效地 集中於可透光區,以更進一步地提高液晶顯示器的亮度。 【實施方式】 請參照第1A圖,其繪示依照本發明一較佳實施例的一 種液晶顯示器的剖面結構示意圖。在第i A圖中液晶顯示 器100依序包含背光源1〇2、高分子膜層1〇8、第一偏光板 104、第一透明基板106、液晶層11〇、彩色濾光片ιΐ2、第 二透明基板114以及第二偏光板116。其中,高分子膜層 1333573 108具有複數個聚光陣列103 ’且聚光陣列i〇3係由複數個 尚折射率區塊105與複數個低折射率區塊1〇7所組成。上 述之彩色濾光片112更包含可透光區112a與遮光區U2b, 聚光陣列103係搭配可透光區112a而設置,且可透光區 112a係位於高分子膜層1〇8中之聚光陣列1〇3之上方。可 透光區112a彳占據彩色滤光片112之表面積較佳係等於聚光 陣列103佔據高分子膜層1〇8之表面積。 凊參照第1B圖’係為第1A圖之高分子膜層中之一聚 光陣列的局部放大示意圖。在第1B圖中,聚光陣列1〇3係 由複數個局折射率區塊105與複數個低折射率區塊IQ?所 組成,且聚光陣列103中之高折射率區塊1〇5與低折射率 區塊1〇7係交錯設置。其中,上述之高折射率區塊1〇5更 包含第一高折射率區塊l〇5a、第二高折射率區塊1〇5b以及 第三高折射率區塊105c,且第一高折射率區塊、第二 南折射率區塊l〇5b以及第三高折射率區塊1〇5c皆具有相 同之折射率。第一高折射率區塊105a、第二高折射率區塊 l〇5b與第三高折射率區塊1〇5c之寬度依序為l丨、[2、與1333573 Less increase in the use of bright film, which in turn reduces the cost burden. According to at least one of the above objects of the present invention, a liquid crystal display device is proposed. The liquid crystal display comprises a backlight, a polymer film layer and a liquid crystal display panel, and the polymer film layer is located under the liquid crystal display panel and above the backlight. Wherein, the polymer film layer has a plurality of concentrating arrays, and each concentrating array comprises a plurality of high refractive index blocks. One of the widest high-refractive-rate blocks is centered, and the remaining high-refractive-index blocks are symmetrically placed on either side of the widest 咼-refractive-index block. And the two high refractive index blocks located at the symmetrical position have the same width, and the high refractive index block is separated by a low refractive index block between the two. The liquid crystal display panel has a plurality of light transmissive regions and a plurality of light shielding regions, each of which is disposed with a light transmissive region, and the light transmissive region is located above the light collecting array in the polymer film layer. Wherein 'high refractive index block and low refractive index area when light passes through each of the concentrating arrays of the polymer film layer and reaches the interface of the high refractive index block and the low refractive index block in the concentrating array A reflection phenomenon is formed on the interface of the block, and the light passing through the concentrating array generates a condensing effect, so that the light is concentrated in the permeable region of the liquid crystal display panel, thereby improving the shell of the liquid crystal display. Therefore, the polymer film layer is not only a light-concentrating film layer having a light collecting effect, but also the light-converging array in the polymer film layer can be regarded as a convex lens having a function of collecting light %. In accordance with a preferred embodiment of the present invention, the width of the high refractive index block on one side of the widest high refractive index block tapers away from the widest high refractive index block. In a preferred embodiment of the present invention, the concentrating array preferably has five high refractive index blocks arranged in order from left to right into a third high refractive index block and a second high refractive index region. a block, a first high refractive index 1333573 block, a second high refractive index block, and a third high refractive index block. The width of the first high refractive index block is greater than the second high refractive index block, and the width of the second high refractive index block is greater than the third high refractive index block. Therefore, the present invention utilizes light to meet the law of refraction (Snell's Law) at the interface of media of different refractive indices, so that when the incident light passes through the interface of the medium of different refractive index, a reflection phenomenon is generated to reflect the light to the liquid crystal display panel. In the permeable area, the use of light due to the loss of light passing through the opaque area is reduced, thereby increasing the use of light. Furthermore, since the size of the high refractive index block in the concentrating array of the present invention is below the micro-nano level, and the arrangement of the high refractive index block is added, when the light passes through the structure of the concentrating array of the present invention In time, the light can be made to collect light to further improve the liquid crystal display. In addition, the method of the present invention can effectively reduce the phenomenon of dark state light leakage to increase the contrast of the liquid crystal display. Moreover, the method of the present invention can not only reduce the number of use of the brightness enhancement film, but also reduce the cost burden. The method of the invention can make the light passing through the low refractive index block have a refraction effect on the interface of the medium with different refractive indexes, so that the light is more effectively concentrated in the light transmissive area, thereby further improving the liquid crystal display. Brightness. [Embodiment] Please refer to FIG. 1A, which is a cross-sectional structural view of a liquid crystal display according to a preferred embodiment of the present invention. In the figure iA, the liquid crystal display 100 sequentially includes a backlight 1〇2, a polymer film layer 1〇8, a first polarizing plate 104, a first transparent substrate 106, a liquid crystal layer 11〇, a color filter ι 2, and a The second transparent substrate 114 and the second polarizing plate 116. The polymer film layer 1333573 108 has a plurality of concentrating arrays 103 ′ and the concentrating array i 〇 3 is composed of a plurality of still refractive index blocks 105 and a plurality of low refractive index blocks 1 〇 7 . The color filter 112 further includes a light-transmitting region 112a and a light-shielding region U2b, and the light-concentrating array 103 is disposed in the light-transmitting region 112a, and the light-transmitting region 112a is located in the polymer film layer 1〇8. Above the concentrating array 1〇3. The surface area of the light-transmitting region 112a 彳 occupies the color filter 112 is preferably equal to the surface area of the concentrating array 103 occupying the polymer film layer 1 〇 8.凊 Referring to Fig. 1B' is a partially enlarged schematic view showing a concentrating array of one of the polymer film layers of Fig. 1A. In FIG. 1B, the concentrating array 1〇3 is composed of a plurality of local refractive index blocks 105 and a plurality of low refractive index blocks IQ?, and the high refractive index block 1〇5 in the concentrating array 103 Interlaced with the low refractive index block 1〇7. Wherein, the high refractive index block 〇5 further includes a first high refractive index block 〇5a, a second high refractive index block 〇5b, and a third high refractive index block 105c, and the first high refractive index The rate block, the second south refractive index block l〇5b, and the third high refractive index block 1〇5c all have the same refractive index. The widths of the first high refractive index block 105a, the second high refractive index block l〇5b and the third high refractive index block 1〇5c are sequentially l丨, [2, and

La,且第一高折射率區塊105a之寬度Li係大於第二高折射 率區塊105b之寬度L2,第二高折射率區塊1〇外之寬度L2 係大於第三高折射率區塊1〇5c寬度Ls。在本發明之較佳實 施例中,第—高折射率區塊1〇5a、第二高折射率區塊祕 與第三高折射率區塊敝之寬度比例較佳為9 : 4M,但 並不以此為限。 一請再參照第⑺圖,上述之第二高折射率區塊職與 第二南折射率區塊1G5e係依序對稱分列於第—高折射率區La, and the width Li of the first high refractive index block 105a is greater than the width L2 of the second high refractive index block 105b, and the width L2 of the second high refractive index block 1 is larger than the third high refractive index block. 1〇5c width Ls. In a preferred embodiment of the present invention, the width ratio of the first high refractive index block 1〇5a, the second high refractive index block secret and the third high refractive index block 敝 is preferably 9:4M, but Not limited to this. Referring again to the figure (7), the second high refractive index block and the second south refractive index block 1G5e are sequentially symmetrically arranged in the first high refractive index region.

10 1333573 塊l〇5a之兩側,也就是說聚光陣列1〇3中之高折射率區塊 105之排列方式由左至右依序為第三高折射率區塊l〇5c、 第二馬折射率區塊l〇5b、第一高折射率區塊i〇5a、第二高 折射率區塊105b以及第三高折射率區塊105c。 高分子膜層108之較佳材質係一高分子材料,且其較 佳厚度係介於5em至300//m之間。高折射率區塊ι〇5之 較佳折射率係介於1.4至1.8之間’低折射率區塊之折 射率較佳約介於1.2至1.55之間。此外,在本發明之一較 佳實施例中,第一偏光板104之折射率較佳係大於高分子 媒層108中之高折射率區塊1〇5之折射率,以更進一步提 高光線的使用率,但並不用以限定本發明之範園。 在本發明之另一較佳實施例中,如第2圖所示,也可 以將高分子膜層108設置於第一透明基板丨〇6之下、第一 偏光板104之上’但並不用以限定本發明之範圍。由於高 分子膜層108之較佳材質以及聚光陣列1〇3中之高折射率 區塊105與低折射率區塊107之排列方式皆如同上述之較 佳實施例之高分子膜層1 〇8,故不在此多加贅述。 请參照第3 A圖,其繪·示依照本發明再一較佳實施例的 一種液晶顯示器的剖面結構示意圖。在第3 A圖中,液晶顯 示器300依序包含背光源302、第一偏光板304、第一透明 基板306、聚光陣列303、液晶層310、彩色濾光片312、 第二透明基板314以及第二偏光板316。其中,聚光陣列 303係由複數個高折射率區塊3〇5a、3〇51)、3〇5c所組成, 高折射率區塊305係設置於第一透明基板3〇6之一表面内 且鄰近第一偏光板304之一面。上述之彩色滤光片312更 11 1333573 包含可透光區312a與遮光區312b,每一個聚光陣列303 係搭配一可透光區312a而設置,且可透光區312a係位於 聚光陣列303之上方。 請參照第3B圖,係為第3A圖中第一透明基板上之一 聚光陣列之局部放大示意圖。在第3B圖中,聚光陣列303 中之南折射率區塊305更包含第一高折射率區塊305a、第 二尚折射率區塊305b以及第三高折射率區塊305c。第一高 折射率區塊305a、第二高折射率區塊3〇5b與第三高折射率 區塊305c之寬度依序為ρ^Ρ2、與P3,且第一高折射率區 塊305a之寬度Pl係大於第二高折射率區塊3〇5b之寬度 P2,第二高折射率區塊3〇5b之寬度Pa係大於第三高折射率 區塊305c寬度Pa。第二高折射率區塊3〇5b與第三高折射 率區塊305c係對稱分列於第一高折射率區塊3〇5a之兩 側,也就是說聚光陣列303中之高折射率區塊3〇5之排列 方式由左至右依序為第三高折射率區塊3〇5c、第二高折射 率區塊305b、第一高折射率區塊3〇5a、第二高折射率區塊 3〇5b以及第三高折射率區塊3〇5c。 ^上述之高折射率區塊305之較佳為一高分子材料,且 南折射,區塊3G5之折射率係大於第—透明基板襄之折 、率尚折射率區塊305之折射率較佳約介於14至i 8之 間,且第一透明基板306之折射率較佳約介於i 2至丨Μ 之間。上述之咼折射率區塊3〇5之厚度較佳係介於5#爪至 3〇〇^rn之間,但並不用以限定本發明之範圍。 或者如第4Α圖所不,其係繪示本發明一較佳實施例 ;第透明基板内之-聚光陣列之局部放大俯視圖更10 1333573 The two sides of the block l〇5a, that is, the arrangement of the high refractive index block 105 in the concentrating array 1〇3 is sequentially arranged from left to right into a third high refractive index block l〇5c, second The horse refractive index block l〇5b, the first high refractive index block i〇5a, the second high refractive index block 105b, and the third high refractive index block 105c. The preferred material of the polymer film layer 108 is a polymer material, and the preferred thickness thereof is between 5 em and 300 / / m. The preferred refractive index of the high refractive index block ι 5 is between 1.4 and 1.8. The refractive index of the low refractive index block is preferably between about 1.2 and 1.55. In addition, in a preferred embodiment of the present invention, the refractive index of the first polarizing plate 104 is preferably greater than the refractive index of the high refractive index block 1〇5 in the polymer dielectric layer 108 to further improve the light. The usage rate is not intended to limit the scope of the invention. In another preferred embodiment of the present invention, as shown in FIG. 2, the polymer film layer 108 may be disposed under the first transparent substrate 丨〇6 and above the first polarizing plate 104. To limit the scope of the invention. The preferred material of the polymer film layer 108 and the high refractive index block 105 and the low refractive index block 107 in the concentrating array 1〇3 are arranged in the same manner as the polymer film layer 1 of the above preferred embodiment. 8, so I will not repeat them here. Referring to FIG. 3A, there is shown a cross-sectional structural view of a liquid crystal display according to still another preferred embodiment of the present invention. In FIG. 3A, the liquid crystal display 300 sequentially includes a backlight 302, a first polarizing plate 304, a first transparent substrate 306, a concentrating array 303, a liquid crystal layer 310, a color filter 312, a second transparent substrate 314, and The second polarizing plate 316. The concentrating array 303 is composed of a plurality of high refractive index blocks 3〇5a, 3〇51), 3〇5c, and the high refractive index block 305 is disposed on one surface of the first transparent substrate 3〇6. And adjacent to one side of the first polarizing plate 304. The color filter 312 further includes a light-permeable region 312a and a light-shielding region 312b. Each of the light-concentrating arrays 303 is disposed with a light-transmitting region 312a, and the light-transmitting region 312a is located in the light-concentrating array 303. Above. Please refer to FIG. 3B, which is a partially enlarged schematic view of a concentrating array on the first transparent substrate in FIG. 3A. In Fig. 3B, the south refractive index block 305 in the concentrating array 303 further includes a first high refractive index block 305a, a second still refractive index block 305b, and a third high refractive index block 305c. The widths of the first high refractive index block 305a, the second high refractive index block 3〇5b and the third high refractive index block 305c are sequentially ρ^Ρ2, and P3, and the first high refractive index block 305a The width P1 is greater than the width P2 of the second high refractive index block 3〇5b, and the width Pa of the second high refractive index block 3〇5b is greater than the width Pa of the third high refractive index block 305c. The second high refractive index block 3〇5b and the third high refractive index block 305c are symmetrically arranged on both sides of the first high refractive index block 3〇5a, that is, the high refractive index in the concentrating array 303 The arrangement of the blocks 3〇5 is from the left to the right, the third high refractive index block 3〇5c, the second high refractive index block 305b, the first high refractive index block 3〇5a, and the second high refractive index. The rate block 3〇5b and the third high refractive index block 3〇5c. Preferably, the high refractive index block 305 is a polymer material and is refracted south. The refractive index of the block 3G5 is larger than that of the first transparent substrate, and the refractive index of the refractive index block 305 is better. It is between about 14 and i8, and the refractive index of the first transparent substrate 306 is preferably between about i 2 and 丨Μ. The thickness of the above-mentioned 咼 refractive index block 3〇5 is preferably between 5# claws and 3〇〇^rn, but is not intended to limit the scope of the invention. Or, as shown in FIG. 4, which is a preferred embodiment of the present invention; a partially enlarged top view of the concentrating array in the transparent substrate is further

12 1333573 可以選擇性地於第一透明基板406之一表面内設置複數個 具有十字型排列的高折射率區塊405之聚光陣列403。其 中’聚光陣列403係由複數個高折射率區塊405所組成, 且這些高折射率區塊405之排列方式係呈十字型排列。高 折射率區塊405更包含第一、第二、第三、第四以及第五12 1333573 A plurality of concentrating arrays 403 having a cross-arranged high refractive index block 405 may be selectively disposed in a surface of one of the first transparent substrates 406. The 'concentrating array 403' is composed of a plurality of high refractive index blocks 405, and the arrangement of the high refractive index blocks 405 is arranged in a cross shape. The high refractive index block 405 further includes first, second, third, fourth, and fifth

高折射率區塊405a、…、405e ’第一高折射率區塊405a係 位於聚光陣列403之中央,第二高折射率區塊4〇5b與第三 高折射率區塊405c係依序沿著X方向對稱排列於第一高折 射率區塊405a之兩侧,而第四高折射率區塊4〇5d與第五 间折射率區塊405e係依序沿著γ方向對稱排列於第一高折 射率區塊405a之兩側。每一個聚光陣列4〇3係搭配液晶顯 不器中之一可透光區(未繪示)而設置,且可透光區係設置於 聚光陣列403之上方。The high refractive index block 405a, ..., 405e 'the first high refractive index block 405a is located at the center of the concentrating array 403, and the second high refractive index block 4 〇 5b and the third high refractive index block 405c are sequentially Arranged symmetrically on both sides of the first high refractive index block 405a along the X direction, and the fourth high refractive index block 4〇5d and the fifth intermediate refractive index block 405e are sequentially arranged symmetrically along the γ direction. A side of a high refractive index block 405a. Each of the concentrating arrays 4 〇 3 is disposed in a light transmissive area (not shown) of the liquid crystal display, and the light permeable area is disposed above the concentrating array 403 .

在第4A圖中,上述之第一高折射率區塊4〇5&之長度 與寬度分別為h,與k!。其中,沿著χ方向對稱排列之第二 同折射率區塊405b與第三高折射率區塊4〇5c之長度皆為 h」’其係與第一高折射率區塊4〇5&之長度h相當,而第二 同折射率區塊4G5b與第三高折射率區塊4()5e之寬度分別 為k2與k3。其中,第一高折射率區塊4〇5a之寬度、係大 於第二高折射率區塊4〇5b之寬度k2,第二高折㈣區塊 4〇5b之寬度k2係大於第三高折射率區塊4〇5c之寬度匕。 沿著Y方向對稱排列之第四高折射率區塊觀與第五高折 射率區塊405e之宽唐皆& , 為ki’其係與第一高折射率區塊 術之寬度k丨相當,而第四高折射料塊4㈣與第五高 折射率區塊她之長度分别為…。其中,第一高折 13 丄川573 射率區塊405a之長度hi係大於第四高折射率區塊钧“之 長度hz’第四高折射率區塊4〇5d之長度h〗係大於第五高 折射率區塊405e之長度h3。 除此之外,如第4B圖,其係繪示本發明一較佳實施例 之於第一透明基板與第二透明基板内分別設置聚光陣列與 發散光陣列之局部放大俯面示意圖,更可以於第一透明基 板406之一表面内設置複數個具有十字型排列的高折射率 區塊405之聚光陣列403,且同時於第二透明基板414之一 表面内設置具有十字型排列的低折射率區塊415之發散光 陣列413,以更進一步提高液晶顯示器之亮度與視角。其 中,發散光陣列413中之複數個低折射率區塊415的排列 較佳係對應於聚光陣列403中之高折射率區塊4〇5的排 列,而發散光陣列413中之低折射率區塊415之尺寸大小 較佳係與聚光陣列403中之高折射率區塊4〇5之尺寸大小 相當。上述之高折射率區塊405之折射率係大於第一透明 基板406之折射率,而低折射率區塊415之折射率係小於 第二透明基板414之折射率。 在本發明之更一較佳實施例中’如第5圖所示,更可 以選擇性地搭配可透光區512a設置具有低折射率區塊5〇7 之聚光陣列503’且於遮光區512b之下方設置低折射率區 塊507,但並不用以限定本發明之範圍。其中,聚光陣列 503中之低折射率區塊507之排列方式係自聚光陣列503 之中央往左右兩旁對稱排列’且每一低折射率區塊507間 之間距X!、X2、X3係不相同’也就是說間距Χι係大於間 距X2,間距X2係大於間距X3。 1333573 本發明係例用光線在不同折射率的介質之介面上需滿 足折射定律(Snell’s Law) ’讓入射光通過不同折射率的介 質之介面上時,產生反射現象而將光線反射至液晶顯示面 板之可透光區中,進而提高光線的使用率。請參照第6與7 圖’係為第3A圖中第一透明基板上之聚光陣列中之一高折 射率區塊的局部放大示意圖。在第6圖中,高折射率區塊 305之折射率係為m,第一透明基板306之折射率為n2, 南折射率區塊305與第一透明基板306之接觸介面係為接 觸面307,且入射角為0,,折射角為其中,高折射率 區塊305之折射率ηι大於第一透明基板3〇6之折射率〜。 因此’根據折射定律(Snell’s Law) ( 1 ): ηι X sin0 ! = n2 X sin 6> 2 ( \ ) 當入射光301由高折射率區塊305(密介質)進入第一透明基 板306 (疏介質)時,折射角Θ2會大於入射角01。若當折射 角6»2等於90°時,折射後的光線3〇9會發生於接觸面3〇7 上。此時,入射角0丨則稱為全反射之臨界角。所以折 射定律公式(1)可改寫成: Θ c= sin'^ n2/ n〇 ( 2) 所以由第(2)式可知,當入射角大於全反射的臨界角 0C時,則會發生全反射的現象,如第7圖所示,於接觸面 3〇7上產生反射之光線309。 再者,由於本發明之聚光陣列中之高折射率區塊之尺 寸係微奈米級以下,又加上聚光陣列中之高折射率區塊之 排列方式,所以當光線通過本發明之聚光陣列的結構時, 可以使光線產生聚光的功能,以進一步提高液晶顯示器之In Fig. 4A, the length and width of the above-mentioned first high refractive index block 4〇5& are h, and k!, respectively. The lengths of the second high refractive index block 405b and the third high refractive index block 4〇5c symmetrically arranged along the χ direction are both h′′ and the first high refractive index block 4〇5& The length h is equivalent, and the widths of the second same refractive index block 4G5b and the third high refractive index block 4() 5e are k2 and k3, respectively. Wherein, the width of the first high refractive index block 4〇5a is greater than the width k2 of the second high refractive index block 4〇5b, and the width k2 of the second high folding (four) block 4〇5b is greater than the third high refractive index. The width of the block 4〇5c is 匕. The fourth high refractive index block symmetrically arranged along the Y direction and the width of the fifth high refractive index block 405e are both ki's and the width of the first high refractive index block is equal to k宽度And the fourth high refractive block 4 (four) and the fifth high refractive index block her length are respectively .... Wherein, the length of the first high-definition 13 丄川 573 irradiance block 405a is greater than the length of the fourth high-refractive-index block 钧 "the length hz' of the fourth high-refractive-index block 4 〇 5d is greater than the The length h3 of the five high refractive index block 405e. In addition, as shown in FIG. 4B, the concentrating array is respectively disposed in the first transparent substrate and the second transparent substrate according to a preferred embodiment of the present invention. A partially enlarged plan view of the divergent light array may further include a plurality of concentrating arrays 403 having a cross-type array of high refractive index blocks 405 in one surface of the first transparent substrate 406, and simultaneously on the second transparent substrate 414. One of the surfaces is provided with a divergent light array 413 having a cross-shaped array of low refractive index blocks 415 to further improve the brightness and viewing angle of the liquid crystal display. Among the plurality of low refractive index blocks 415 in the divergent light array 413 Preferably, the arrangement corresponds to the arrangement of the high refractive index blocks 4〇5 in the concentrating array 403, and the size of the low refractive index block 415 in the divergent light array 413 is preferably higher than that in the concentrating array 403. Size of the refractive index block 4〇5 The refractive index of the high refractive index block 405 is greater than the refractive index of the first transparent substrate 406, and the refractive index of the low refractive index block 415 is smaller than the refractive index of the second transparent substrate 414. In a preferred embodiment, as shown in FIG. 5, a concentrating array 503' having a low refractive index block 5〇7 may be selectively disposed in combination with the light transmissive region 512a and disposed below the light shielding region 512b. The refractive index block 507 is not limited to the scope of the present invention, wherein the low refractive index block 507 in the concentrating array 503 is arranged symmetrically from the center of the concentrating array 503 to the left and right sides and each The distance between the low refractive index blocks 507 is different from X!, X2, and X3', that is, the pitch Χι is greater than the pitch X2, and the pitch X2 is greater than the pitch X3. 1333573 The present invention uses light in different refractive index media. The interface needs to meet the law of refraction (Snell's Law). When the incident light passes through the interface of the medium with different refractive indices, the reflection phenomenon is generated to reflect the light into the light transmissive area of the liquid crystal display panel, thereby improving the light utilization rate. Please refer to FIGS. 6 and 7 for a partial enlarged view of a high refractive index block in the concentrating array on the first transparent substrate in FIG. 3A. In FIG. 6, the refraction of the high refractive index block 305 The rate is m, the refractive index of the first transparent substrate 306 is n2, the contact interface between the south refractive index block 305 and the first transparent substrate 306 is the contact surface 307, and the incident angle is 0, and the refraction angle is high therein. The refractive index η of the refractive index block 305 is larger than the refractive index of the first transparent substrate 3〇6. Therefore, 'According to the law of refraction (Snell's Law) (1): ηι X sin0 ! = n2 X sin 6> 2 ( \ ) When the incident light 301 enters the first transparent substrate 306 (saturated medium) by the high refractive index block 305 (density medium), the refraction angle Θ2 is greater than the incident angle 01. If the refraction angle 6»2 is equal to 90°, the refracted light 3〇9 will occur on the contact surface 3〇7. At this time, the incident angle 0 丨 is called the critical angle of total reflection. Therefore, the formula of refraction law (1) can be rewritten as: Θ c= sin'^ n2/ n〇( 2) Therefore, it can be known from equation (2) that when the incident angle is greater than the critical angle of total reflection 0C, total reflection occurs. The phenomenon, as shown in Fig. 7, produces a reflected ray 309 on the contact surface 3〇7. Furthermore, since the size of the high refractive index block in the concentrating array of the present invention is below the micro-nano level, and the arrangement of the high-refractive-index blocks in the concentrating array is added, when the light passes through the present invention When the structure of the concentrating array is configured, the light can be concentrated to improve the liquid crystal display.

15 1333573 亮度。請再參照第3B圖,聚光陣列303中之高折射率區塊 305之尺寸大小係微奈米級以下。第二高折射率區塊3〇讣 與第三高折射率區塊305c係依序對稱分列於第一高折射率 區塊305a之兩側’且位於對稱位置之兩兩第二高折射率區 塊305b與兩兩第三高折射率區塊3〇5c分別具有相同寬度 P2與P3。第一高折射率區塊的寬度Pl係大於第二高折射率 區塊的寬度P2’第二高折射率區塊的寬度P2係大於第三高 折射率區塊的寬度P3。所以,當光線301通過聚光陣列3〇3 時’不僅於接觸面307上產生反射的光線309,更可以使反 射後的光線309產生聚光的功能’以更進一步提高液晶顯 示器之亮度。因此,可以將聚光陣列303視為一種具有聚 光功能之凸透鏡。 請再參照第3 A圖,並同時參照第3B圖。首先,背光 源302投射出的光線會進入第一偏光板3〇4。接著,入射光 301經過聚光陣列303之後,會在接觸面307上產生反射之 光線309 ’且反射光線309會產生聚光的效果。隨後,光線 309會穿過第一透明基板306,並依序進入液晶層31〇與彩 色濾光片312中之可透光區312a、第二透明基板314以及 第二偏光板316。 更具體地說,本發明係利用光線在不同折射率的介質 之介面上需滿足折射定律(Snell’s Law),讓入射光通過不 同折射率的介質之介面上時,產生反射現象而將光線反射 至液bb顯不面板之可透光區312a中,以減少因經過彩色遽 光片312之遮光區312b之光線損耗,進而增加光線的使用 率’且同時提尚液晶顯示器的亮度。再者,由於本發明之 16 聚光陣列303中之高折射率區塊3()5之尺寸係微奈米級以 下’又加上聚光陣列中之第二高折射率區塊 305b與第三高 折射率區塊305c係對稱分列於第一高折射率區塊觀之 兩側,所以當光線301通過聚光陣列3()3 _,可以讓光線 309產生聚光的功能’以進一步提高液晶顯示胃则的亮 度。 除此之外,如第3A圖所示,本發明之方法更可以讓穿 過折射率較低的第一透明基板3〇6之入射光3〇la,在不同 折射率的介質之介面上產生折射的效果,使得光線3〇9a更 有效地集中於可透光區312a,以更進-步地提高液晶顯示 器的亮度。 以下將針對本發明較佳實施例中之高折射率區塊之製 造方法做一詳細說明,但此製造方法並不用以限定本發明 之範圍》 製作方法一 清參照第8 A圖至第8D圖,係繪示依據本發明之一較 佳實施例之於透明基板上製作高分子膜層之製程步驟的結 構不意圖。在第8A圖中’提供一透明基板6〇2。接著,在 第8B圖中’形成一高分子膜層604於透明基板6〇2之上。 上述形成高分子膜層604之方法較佳為旋塗法,但並不用 以限定本發明之範圍。 隨後’於第8C圖中’利用光罩606與紫外光608對高 分子膜層604進行曝光,以形成如第8D圖所示之聚光陣列 6〇3 〇其中,聚光陣列603係由複數個高折射率區塊6〇5與 1333573 複數個低折射率區塊607所組成。其中,上述之高分子膜 層604係藉由控制曝光時間與曝光強度而得到不同折射率 之高折射率區塊605與低折射率區塊607。如此一來,即可 於透明基板上完成聚光陣列之製作。 或者,在本發明之另一較佳實施例中,更可以於偏光 . 板上形成高分子膜層,使得偏光板上具有高折射率區塊與 . 低折射率區塊,但並不用以限定本發明之範圍。 • 製作方法二 明參照第9Α圖至第9Ε圖,係繪示依據本發明之另一 較佳實施例之於透明基板上製作聚光陣列之製程步驟的結 構示意圖。在第9Α圖中,提供一透明基板7〇2,並於透明 基板702上形成一光阻層7〇4。接著,在第9Β圖中,對光 , 阻層704進行一微影製程,以形成圖案化光阻7〇6。在第 9C圖中,蝕刻未為圖案化光阻7〇6覆蓋之透明基板7〇2, 以於透明基板702上形成具有不同寬度之凹槽7〇8。其中, • 凹槽708係搭配彩色濾光片之可透光區(未繪示)而設置。隨 後,移除圖案化光阻706。 在第9D圖中,利用旋塗法形成一高分子材料71〇於凹 槽708之内與透明基板7〇2之上。其中,高分子材料71〇 ^ 之折射率係大於透明基板702之折射率。接著,再利用紫 外光線照射高分子材料71〇,以硬化高分子材料71〇。在第 ·· 9Ε圖中,進行一蝕刻製程與研磨製程,以於透明基板7〇2 之表面上形成一平整的表面,同時形成聚光陣列7⑽。其 中,聚光陣列703係由第一、第二與第三高折射率區塊 18 1333573 705a、705b與705c所組成。如此一來,即可於透明基板上 完成聚光陣列703之製作。 或者’如第9F圖所示,更可以依需求於透明基板702 上形成複數個低折射率區塊7〇7之聚光陣列703,但並不用 以限定本發明之範圍。其中,低折射率區塊707間之間距 係不相同。 製作方法三 φ 請參照第1圖至第i〇d圖,係繪示依據本發明之再 一較佳實施例之於透明基板上製作高折射率區塊之製程步 驟的結構示意圖。在第l〇A圖中,於透明基板802上形成 一光阻層(未繪示),接著對光阻層進行一微影製程,以形成 • 圖案化光阻804。在第10B圖中,蝕刻未為圖案化光阻8〇4 . 覆蓋之透明基板802’以於透明基板802上形成具有不同寬 度之凹槽806。其中,凹槽806係搭配彩色濾光片之可透光 區(未繪示)而設置。隨後,移除圖案化光阻8〇4。 φ 在第10C圖中,於偏光板808上塗佈一層黏著層810。 其中,上述之黏著層810之材料較佳為一高分子材料,黏 著層810之厚度較佳係介於2〇 “出至” 之間。且上 述之黏著層810之折射率係大於透明基板8〇2之折射率。 然後,如第10D圖所示,透過黏著層81〇將偏光板8〇8與 透明基板802黏貼在一起。如此一來,即可於透明基板8〇2 * 上完成聚光陣列803之製作。其中,聚光陣歹"03係由第 一、第二與第三高折射率區塊8〇5a、8〇5b與8〇5c所組成。 或者,更可以依需求於透明基板上形成複數個低折射15 1333573 Brightness. Referring again to FIG. 3B, the size of the high refractive index block 305 in the concentrating array 303 is below the micron level. The second high refractive index block 3〇讣 and the third high refractive index block 305c are sequentially symmetrically arranged on both sides of the first high refractive index block 305a and are located at two positions of the second high refractive index at the symmetrical position. The block 305b and the two second higher refractive index blocks 3〇5c have the same widths P2 and P3, respectively. The width P1 of the first high refractive index block is greater than the width P2' of the second high refractive index block. The width P2 of the second high refractive index block is greater than the width P3 of the third high refractive index block. Therefore, when the light ray 301 passes through the concentrating array 3 〇 3, not only the reflected light 309 is generated on the contact surface 307, but also the reflected light 309 is caused to condense the light □ to further increase the brightness of the liquid crystal display. Therefore, the concentrating array 303 can be regarded as a convex lens having a condensing function. Please refer to Figure 3A again, and refer to Figure 3B at the same time. First, the light projected by the backlight 302 enters the first polarizing plate 3〇4. Then, after the incident light 301 passes through the concentrating array 303, a reflected ray 309' is generated on the contact surface 307 and the reflected ray 309 produces a condensing effect. Then, the light 309 passes through the first transparent substrate 306, and sequentially enters the liquid permeable layer 312a, the second transparent substrate 314, and the second polarizing plate 316 in the liquid crystal layer 31 and the color filter 312. More specifically, the present invention utilizes light to meet the law of refraction (Snell's Law) at the interface of media of different refractive indices, so that when the incident light passes through the interface of the medium of different refractive index, a reflection phenomenon is generated to reflect the light to The liquid bb is not visible in the opaque region 312a of the panel to reduce the light loss caused by the light-shielding region 312b passing through the color light-receiving sheet 312, thereby increasing the light usage rate and at the same time improving the brightness of the liquid crystal display. Furthermore, since the size of the high refractive index block 3 () 5 in the 16 concentrating array 303 of the present invention is below the micron level, plus the second high refractive index block 305b and the first in the concentrating array. The three high refractive index blocks 305c are symmetrically arranged on both sides of the first high refractive index block view, so when the light ray 301 passes through the concentrating array 3() 3 _, the light 309 can be made to condense the function 'to further Improve the brightness of the liquid crystal display stomach. In addition, as shown in FIG. 3A, the method of the present invention allows the incident light 3〇la passing through the first transparent substrate 3〇6 having a lower refractive index to be generated on the interface of the medium having different refractive indexes. The effect of refraction causes the light rays 3〇9a to concentrate more effectively on the light-permeable region 312a to further increase the brightness of the liquid crystal display. Hereinafter, the manufacturing method of the high refractive index block in the preferred embodiment of the present invention will be described in detail, but the manufacturing method is not intended to limit the scope of the present invention. The manufacturing method is clear with reference to FIGS. 8A to 8D. The structure of the process for fabricating a polymer film layer on a transparent substrate according to a preferred embodiment of the present invention is not intended. A transparent substrate 6〇2 is provided in Fig. 8A. Next, a polymer film layer 604 is formed on the transparent substrate 6〇2 in Fig. 8B. The above method of forming the polymer film layer 604 is preferably a spin coating method, but is not intended to limit the scope of the invention. Subsequently, the polymer film layer 604 is exposed by the photomask 606 and the ultraviolet light 608 in FIG. 8C to form a concentrating array 6〇3 as shown in FIG. 8D, wherein the concentrating array 603 is composed of plural The high refractive index blocks 6〇5 and 1333573 are composed of a plurality of low refractive index blocks 607. The polymer film layer 604 described above obtains the high refractive index block 605 and the low refractive index block 607 having different refractive indexes by controlling the exposure time and the exposure intensity. In this way, the fabrication of the concentrating array can be completed on the transparent substrate. Alternatively, in another preferred embodiment of the present invention, the polymer film layer may be formed on the polarizing plate such that the polarizing plate has a high refractive index block and a low refractive index block, but is not limited thereto. The scope of the invention. • Manufacturing Method 2 Referring to Figures 9 through 9, there is shown a schematic view of a process for fabricating a concentrating array on a transparent substrate in accordance with another preferred embodiment of the present invention. In Fig. 9, a transparent substrate 7〇2 is provided, and a photoresist layer 7〇4 is formed on the transparent substrate 702. Next, in the ninth drawing, the light and resist layer 704 is subjected to a lithography process to form a patterned photoresist 7〇6. In Fig. 9C, the transparent substrate 7〇2 not covered by the patterned photoresist 7〇6 is etched to form grooves 7〇8 having different widths on the transparent substrate 702. Wherein, the groove 708 is provided with a light transmissive area (not shown) of the color filter. The patterned photoresist 706 is then removed. In Fig. 9D, a polymer material 71 is formed by spin coating in the recess 708 and over the transparent substrate 7〇2. The refractive index of the polymer material 71 〇 ^ is greater than the refractive index of the transparent substrate 702. Next, the polymer material 71 is irradiated with ultraviolet light to harden the polymer material 71. In the drawing, an etching process and a polishing process are performed to form a flat surface on the surface of the transparent substrate 7〇2 while forming the concentrating array 7 (10). The concentrating array 703 is composed of first, second and third high refractive index blocks 18 1333573 705a, 705b and 705c. In this way, the fabrication of the concentrating array 703 can be completed on the transparent substrate. Alternatively, as shown in Fig. 9F, a plurality of concentrating arrays 703 of low refractive index blocks 7 〇 7 may be formed on the transparent substrate 702 as needed, but are not intended to limit the scope of the invention. Among them, the distance between the low refractive index blocks 707 is different. Manufacturing Method 3 φ Referring to FIGS. 1 to 1D, a schematic structural view of a process for fabricating a high refractive index block on a transparent substrate according to still another preferred embodiment of the present invention is shown. In FIG. 1A, a photoresist layer (not shown) is formed on the transparent substrate 802, and then the photoresist layer is subjected to a lithography process to form a patterned photoresist 804. In Fig. 10B, the etching is not a patterned photoresist 8〇4. The covered transparent substrate 802' is such that grooves 806 having different widths are formed on the transparent substrate 802. The groove 806 is provided with a light transmissive area (not shown) of the color filter. Subsequently, the patterned photoresist 8 〇 4 is removed. φ In the 10Cth view, an adhesive layer 810 is coated on the polarizing plate 808. The material of the adhesive layer 810 is preferably a polymer material, and the thickness of the adhesive layer 810 is preferably between 2" and "out". The refractive index of the adhesive layer 810 is greater than the refractive index of the transparent substrate 8〇2. Then, as shown in Fig. 10D, the polarizing plate 8A8 is adhered to the transparent substrate 802 through the adhesive layer 81. In this way, the fabrication of the concentrating array 803 can be completed on the transparent substrate 8〇2*. Among them, the concentrating array "03 is composed of the first, second and third high refractive index blocks 8〇5a, 8〇5b and 8〇5c. Alternatively, a plurality of low refractions can be formed on the transparent substrate as needed.

1333573 率區塊之聚光陣列,但並不用以限定本發明之範圍。其中, 低折射率區塊間之間距係不相同。 由上述本發明之較佳實施例可知,應用本發明具有下 列優點。本發明之液晶顯示器不僅可以減少因經過遮光區 而產生之之光損耗,更可以集中光場分布,進而提高液晶 . 顯示器之亮度。再者,本發明之方法可以讓光線產生聚光 •的功能,以進一步提高液晶顯示器的亮度。且應用本發明 之方法可以有效地降低暗態漏光的現象,以增加液晶顯示 • 器之對比。除此之外,本發明之方法不僅可以減少增亮膜 之使用數量,更可以降低成本。本發明之方法更可以讓穿 過低折射率區塊之光線,在不同折射率的介質之介面上產 生折射的效果,使得光線更有效地集中於可透光區,以更 • 進一步地提高液晶顯示器的亮度。 ·· 雖然本發明已以一較佳實施例揭露如上,然其並非用 以限定本發明,任何熟習此技藝者,在不脫離本發明之精 神和範圍内,當可作各種之更動與潤飾,因此本發明之保 # 護範圍當視後附之申請專利範圍所界定者為準。 【圖式簡單說明】 為讓本發明之上述和其他目的、特徵、優點與實施例 能更明顯易懂’所附圖式之詳細說明如下: 第1Α圖、第2圖及第3Α圖,其繪示依照本發明一較 ' 佳實施例的一種液晶顯示器的剖面結構示意圖。 第圖,係為第1A圖之高分子膜層中之聚光陣列的 局部放大示意圖。 20 1333573 第3B圖,係為第3A圖之第一透明基板上之聚光陣列 之局部放大示意圖。 第4A圖係繪示依照本發明一較佳實施例之於第一透 明基板内之聚光陣列的局部放大俯視圖。 第4B圖,係繪示本發明一較佳實施例之於第一透明基 板與第二透明基板内分別設置聚光陣列與發散光陣列之局 部放大俯面示意圖。 第5圖,係繪示依照本發明一較佳實施例的一種液晶 顯不的剔面結構示意圖。 第6與7圖,係為第3A圖中第一透明基板上之聚光陣 列中之一高折射率區塊的局部放大示意圖。 第8 A圖至第8D圖,係繪示依據本發明之一較佳實施 例之於透明基板上製作高分子膜層之製程步驟的結構示意 圖。 第9A圖至第9E圖’係繪示依據本發明之另一較佳實 施例之於透明基板上製作聚光陣列之製程步驟的結構示意 圖。 第9F圖’係繪示依據本發明之—較佳實施例之於透明 基板上製作聚光陣列之結構示意圖。 第10A圖至第10D圖’係繪示依據本發明之再一較佳 實施例之於透明基板上製作高折射率區塊之製程步驟的結 構示意圖。 【主要元件符號說明】 100、300、500 :液晶顯示器 103、303、403、503、603、 21 1333573 102、302、502 :背光源 104、304、504:第一偏光板 106、306、406、506 :第一透 明基板 108 :高分子膜層 110、310、510 :液晶層 112a、312a、512a :可透光區 114、314、414、514 :第二透 明基板 105b、305b、405b、705b、 805b :第二高折射率區塊 301、301a :入射光 307 :接觸面 405d :第四高折射率區塊 413 :發散光陣列 415b :第二低折射率區塊 415d:第四低折射率區塊 602、702、802 :透明基板 608 :紫外光線 704 :光阻層 708、806 :凹槽 808 ·偏光板 hi、h2、h3 :長度 川、L2、L3 :寬度 Xl、X2、X3 :間距 Θ i :入射角 703、803 :聚光陣列 105、305、405 ' 605 :高折射 率區塊 107 、 415 、 507 、 607 、 707 : 低折射率區塊 112、312、512 ·•彩色濾光片 112b、312b、512b :遮光區 116、316、516:第二偏光板 105a、305a、405a、705a、 805a :第一高折射率區塊 105c、305c、405c、705c、 805c :第三高折射率區塊 309、309a :光線 405e:第五高折射率區塊 415a:第一低折射率區塊 415c:第三低折射率區塊 415e:第五低折射率區塊 604 :高分子膜層 606 :光罩 706、804 :圖案化光阻層 710 :高分子材料 810 :黏著層 ki、k2、k3 :寬度 p!、p2、P3 :寬度 ηι、n2 :折射率 0 2 :折射角1333573 A concentrating array of rate blocks, but is not intended to limit the scope of the invention. Among them, the distance between the low refractive index blocks is different. It will be apparent from the above-described preferred embodiments of the present invention that the application of the present invention has the following advantages. The liquid crystal display of the invention not only can reduce the light loss caused by passing through the light shielding area, but also can concentrate the light field distribution, thereby improving the brightness of the liquid crystal display. Furthermore, the method of the present invention allows the light to produce a condensing function to further increase the brightness of the liquid crystal display. Moreover, the method of the present invention can effectively reduce the phenomenon of dark state light leakage to increase the contrast of the liquid crystal display device. In addition to this, the method of the present invention can not only reduce the number of use of the brightness enhancing film, but also reduce the cost. The method of the invention can make the light passing through the low refractive index block have a refraction effect on the interface of the medium with different refractive indexes, so that the light is more effectively concentrated in the light transmissive area, so as to further improve the liquid crystal. The brightness of the display. The present invention has been described above in terms of a preferred embodiment, and is not intended to limit the invention, and various modifications and changes may be made without departing from the spirit and scope of the invention. Therefore, the scope of protection of the present invention is subject to the definition of the scope of the patent application. BRIEF DESCRIPTION OF THE DRAWINGS The above and other objects, features, advantages and embodiments of the present invention will become more <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; </ RTI> <RTIgt; A schematic cross-sectional view of a liquid crystal display according to a preferred embodiment of the present invention is shown. The figure is a partially enlarged schematic view of a concentrating array in the polymer film layer of Fig. 1A. 20 1333573 Figure 3B is a partially enlarged schematic view of the concentrating array on the first transparent substrate of Figure 3A. Figure 4A is a partially enlarged plan view showing a concentrating array in a first transparent substrate in accordance with a preferred embodiment of the present invention. FIG. 4B is a partially enlarged plan view showing a concentrating array and a diverging light array respectively disposed in the first transparent substrate and the second transparent substrate according to a preferred embodiment of the present invention. Figure 5 is a schematic view showing the structure of a liquid crystal display in accordance with a preferred embodiment of the present invention. Figures 6 and 7 are partial enlarged views of one of the high refractive index blocks in the concentrating array on the first transparent substrate in Fig. 3A. 8A to 8D are schematic structural views showing a process of fabricating a polymer film layer on a transparent substrate in accordance with a preferred embodiment of the present invention. 9A to 9E are schematic structural views showing a process of fabricating a concentrating array on a transparent substrate in accordance with another preferred embodiment of the present invention. Figure 9F is a schematic view showing the structure of a concentrating array formed on a transparent substrate in accordance with a preferred embodiment of the present invention. 10A to 10D are schematic views showing the steps of a process for fabricating a high refractive index block on a transparent substrate in accordance with still another preferred embodiment of the present invention. [Description of main component symbols] 100, 300, 500: liquid crystal display 103, 303, 403, 503, 603, 21 1333573 102, 302, 502: backlights 104, 304, 504: first polarizing plates 106, 306, 406, 506: first transparent substrate 108: polymer film layer 110, 310, 510: liquid crystal layer 112a, 312a, 512a: light transmissive regions 114, 314, 414, 514: second transparent substrate 105b, 305b, 405b, 705b, 805b: second high refractive index block 301, 301a: incident light 307: contact surface 405d: fourth high refractive index block 413: divergent light array 415b: second low refractive index block 415d: fourth low refractive index region Blocks 602, 702, 802: transparent substrate 608: ultraviolet light 704: photoresist layer 708, 806: groove 808 · polarizing plate hi, h2, h3: length, L2, L3: width Xl, X2, X3: pitch Θ i: incident angles 703, 803: concentrating arrays 105, 305, 405 '605: high refractive index blocks 107, 415, 507, 607, 707: low refractive index blocks 112, 312, 512 · color filters 112b, 312b, 512b: light shielding regions 116, 316, 516: second polarizing plates 105a, 305a, 405a, 705a, 805a: first high refractive index region 105c, 305c, 405c, 705c, 805c: third high refractive index block 309, 309a: light 405e: fifth high refractive index block 415a: first low refractive index block 415c: third low refractive index block 415e : fifth low refractive index block 604: polymer film layer 606: photomask 706, 804: patterned photoresist layer 710: polymer material 810: adhesive layer ki, k2, k3: width p!, p2, P3: Width ηι, n2 : refractive index 0 2 : refraction angle

Claims (1)

1333573 2〇fe 7f 13日|銳翁正本 十、申請專利範圍: -- h 一種尚亮度之液晶顯示器,該液晶顯示器包含: 一背光源; —第一偏光板,設置於該背光源之上; 一第一透明基板,設置於該第一偏光板之上; 複數個聚光陣列,設置於該第一透明基板之一表面内 φ 且鄰近該第一偏光板之一面,每一該些聚光陣列包括: 一第一高折射率區塊;以及 複數個第二咼折射率區塊’對稱分列於該第一高 折射率區塊兩側且位於對稱位置之兩該些第二高折射 率區塊具有相同的寬度,該第一高折射率區塊與該些 第二高折射率區塊兩兩之間為一低折射率區塊,該第 一尚折射率區塊與該些第二高折射率區塊之折射率係 大於該低折射率區塊之折射率,且該第一高折射率區 •塊的寬度大於該些第二高折射率區塊,位於該第一高 折射率區塊一側之該些第二高折射率區塊的寬度朝向 遠離該第一尚折射率區塊的方向逐漸縮減; 一第二透明基板,設置於該第一透明基板之上,具複 數個可透光區對應於該些聚光陣列配置; 一液晶層,設置於該第一透明基板與該第二透明基板 之間;以及 一第二偏光板’設置於該第二透明基板之上。 23 [SI 2010年7月13曰修正替換頁 古 &amp;專利範圍第1項所述之液晶顯示器,其中該第 ^折射率區塊與該些第二高折射率區塊之材質係一高分 一 ^ .如申凊專利範圍第1項所述之液晶顯示器,其中該第 ^折射率區塊與該些第二高折射率區塊之折射率係介於 M至1.8之間。 、 4·如申請專利範圍第1項所述之液晶顯示器,其中該低 折射率區塊之折射率係介於1.2至1.55之間。 _ 一5·如申請專利範圍第1項所述之液晶顯示器,其中該第 尚折射率區塊與該些第二高折射率區塊之厚度係介於$ V m至3〇〇以m之間。 6.—種液晶顯示器,該液晶顯示器包含: 一背光源; 问分子膜層,設置於該背光源之上,該高分子膜層 具有複數個聚光陣列,每一該些聚光陣列包含: 一第一高折射率區塊;以及 複數個第二南折射率區塊,對稱分列於該第一高 折射率區塊兩側且位於對稱位置之兩該些第二高折射 率區塊具有相同的寬度’該第一高折射率區塊:該些 第二高折射率區塊兩兩之間為一低折射率區塊,該第 Γ5] 24 1333573 2010年7月丨3曰修正替換頁 同折射率區塊與該些第二高折射率區塊之折射率係 大於該低折射率區塊之折射率,且該第一高折射率區 塊的寬度大於該些第二高折射率區塊,位於該第一高 f射率區塊-側之該些第二高折射率區塊的寬度朝向 遠離該第一高折射率區塊的方向逐漸縮減;以及 一液晶顯示面板,設置於該高分子膜層之上,該液晶 =示面板具有複數個可透錢且該些可透光區係位於該高 分子膜層中之該些聚光陣列之上方。 7·如申請專利範圍第6項所述之液晶顯示器其中該第 —高折射率區塊與該些第二高折射率區塊之折射率係於 1.4至1.8之間。 8.如申請專利範圍第6項所述之液晶顯示器其中該低 折射率區塊之折射率係介於1.2至1.55之間。 X _ 9_如申請專利範圍第6項所述之液晶顯示器,其中該高 分子膜層之厚度係介於至3〇〇/zm之間。 X间 1〇*種用於一液晶顯示器之一聚光膜層,其特徵在 於:該聚光膜層具有複數個聚光陣列,每—該些聚光陣列 包含複數個高折射率區塊且其中—最寬的高折射率區塊置 於中央其餘該些南折射率區塊係對稱分列於該最寬的高 折射率區塊兩側且位於對稱位置之兩該些高折射率區塊具 有相同的寬度’該些高折射率區塊兩兩之間為一低折射率 LSI 25 1333573 2010年7月丨3曰修正替換頁 區塊,該些高折射率區塊之折射率係大於該低折射率區塊 之折射率’位於該最寬的高折射率區塊一側之該些高折射 率區塊的寬度朝向遠離該最寬的高折射率區塊的方向逐漸 縮減’該些聚光陣列係對應該液晶顯示器中複數個可透光 區而配置。 11.如申請專利範圍第10項所述之聚光膜層,其中該聚 光膜層之材質係一高分子材質。 12_如申請專利範圍第10項所述之聚光膜層,其中該些 冋折射率區塊之折射率係於1.4至1.8之間。 13·如申請專利範圍第10項所述之聚光膜層,其中該低 折射率區塊之折射率係介於 1.2至1.55之間。 14·如申請專利範圍第10項所述之聚光膜層’其中該聚 光膜層之厚度係介於5从m至300# m之間。 m 261333573 2〇fe 7f 13th | Rui Weng Zheng Ben 10, the scope of application for patents: -- h A liquid crystal display of still brightness, the liquid crystal display comprises: a backlight; - a first polarizing plate, disposed above the backlight; a first transparent substrate disposed on the first polarizing plate; a plurality of concentrating arrays disposed in a surface of the first transparent substrate φ and adjacent to one surface of the first polarizing plate, each of the concentrating lights The array includes: a first high refractive index block; and a plurality of second yttrium refractive index blocks symmetrically disposed on the two sides of the first high refractive index block and at the symmetrical positions The blocks have the same width, and the first high refractive index block and the second high refractive index blocks are a low refractive index block, and the first still refractive index block and the second The refractive index of the high refractive index block is greater than the refractive index of the low refractive index block, and the width of the first high refractive index block is larger than the second high refractive index block, and the first high refractive index is located The second high refractive index blocks on one side of the block The second transparent substrate is disposed on the first transparent substrate, and has a plurality of light transmissive regions corresponding to the concentrating arrays; The layer is disposed between the first transparent substrate and the second transparent substrate; and a second polarizing plate is disposed on the second transparent substrate. 23 [SI] The liquid crystal display of the first aspect of the invention, wherein the second refractive index block and the second high refractive index block are one high score. The liquid crystal display of claim 1, wherein the refractive index of the second refractive index block and the second high refractive index block are between M and 1.8. 4. The liquid crystal display of claim 1, wherein the low refractive index block has a refractive index of between 1.2 and 1.55. The liquid crystal display of claim 1, wherein the thickness of the first refractive index block and the second high refractive index block are between $Vm and 3〇〇m between. 6. A liquid crystal display, comprising: a backlight; a molecular film layer disposed on the backlight, the polymer film layer having a plurality of concentrating arrays, each of the concentrating arrays comprising: a first high refractive index block; and a plurality of second south refractive index blocks, the two second high refractive index blocks symmetrically arranged on both sides of the first high refractive index block and located at a symmetrical position The same width 'the first high refractive index block: the second high refractive index block is a low refractive index block between the two, the second ] 5] 24 1333573 July 2010 丨 3 曰 corrected replacement page The refractive index of the same refractive index block and the second high refractive index block is greater than the refractive index of the low refractive index block, and the width of the first high refractive index block is larger than the second high refractive index regions a block, the width of the second high refractive index blocks located on the first high-amplitude block-side is gradually reduced toward a direction away from the first high-refractive-index block; and a liquid crystal display panel disposed at the Above the polymer film layer, the liquid crystal = display panel has a plurality Permeable costly and the plurality of light transmitting regions positioned above the plurality of lines converging arrays of the high molecular film layers. 7. The liquid crystal display of claim 6, wherein the refractive index of the first high refractive index block and the second high refractive index block is between 1.4 and 1.8. 8. The liquid crystal display of claim 6, wherein the low refractive index block has a refractive index of between 1.2 and 1.55. The liquid crystal display of claim 6, wherein the high molecular layer has a thickness of between 3 Å/zm. A concentrating film layer for use in a liquid crystal display, characterized in that the concentrating film layer has a plurality of concentrating arrays, each of the concentrating arrays comprising a plurality of high refractive index blocks and Wherein, the widest high-refractive-index block is placed in the center, and the other of the south-refractive-index blocks are symmetrically arranged on the two sides of the widest high-refractive-index block and located at two positions in the symmetric position. Having the same width 'the high refractive index blocks between the two are a low refractive index LSI 25 1333573 July 2010 丨 3 曰 modified replacement page block, the refractive index of the high refractive index block is greater than The refractive index of the low refractive index block is located on the side of the widest high refractive index block, and the widths of the high refractive index blocks are gradually reduced toward the direction away from the widest high refractive index block. The light array is configured corresponding to a plurality of light transmissive regions in the liquid crystal display. 11. The concentrating film layer of claim 10, wherein the material of the concentrating film layer is a polymer material. The concentrating film layer of claim 10, wherein the refractive index of the bismuth refractive index block is between 1.4 and 1.8. 13. The concentrating film layer of claim 10, wherein the low refractive index block has a refractive index between 1.2 and 1.55. 14. The concentrating film layer as described in claim 10, wherein the thickness of the concentrating film layer is between 5 and 300 m. m 26
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TW95121088A TWI333573B (en) 2006-06-13 2006-06-13 Liquid crystal display
US11/785,976 US8009251B2 (en) 2006-06-13 2007-04-23 High brightness liquid crystal display
KR1020070046794A KR100857958B1 (en) 2006-06-13 2007-05-14 Liquid crystal display
US13/192,776 US8879028B2 (en) 2006-06-13 2011-07-28 High brightness liquid crystal display

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