TW455704B - Polarized-light pipe and polarized-light source - Google Patents
Polarized-light pipe and polarized-light source Download PDFInfo
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4 5 5 7 〇 4 ~ 幽_年月日 條正 五、發明說明⑴ ' -- 1明之背熹 k發明之頜迠 本發明係關於一種可將自其側面接收到之入射光轉變為 具有均勻亮度之線性偏光,其接著再在控制之下在振盪表 面上自其兩表面發射,以致其適用於形成供液晶顯示裝置 用之背光的偏光管及平面偏光源。 本申請案係以日本專利申請案No. Hei. 1卜1 31 429、 U-131430、Π-138102、1 卜166727、1卜1 74 368 及 11-197083為基礎’將其併入本文為參考資料。 k 相關技藝之說明 關於可使用作為供液晶裝置用之背光的側光型光管,迄 今為止已知一種包含由設於光透射樹脂板上之反射點等等 所製成之光發射構件的裝置,其中此光透射樹脂板具有使 由全反射所產生之透射光1經由散射等等而自板之兩表面 之其中一者發射的配置。然而,前述的發射光係具有極少 或沒有極化的自然光,因此,在液晶顯示之前必需透過極 化板將其轉變為線性偏光。因此,前述的裝置有極化板造 成吸收損耗’而使光的百分利用率無法超過5 0 %之缺點。 在前述的情況之下,提出一種除了前述的配置之外,尚 包括具有利用布汝士特(Brewster)角以產生線性偏光之偏 光分離板與相差板結合之偏光轉化構件的系統 (JP-A-6-18873 C此處所使用之術語「jp-Aj係指「未經審 查已公告的日本專利申請案」)、JP-A-6-160840、 JP-A-6-265892 、JP-A-7-72475 、JP-A-7-261122 、4 5 5 7 〇4 ~ You _ _ month month day article five, description of the invention ⑴--1 Ming of the back 熹 k invention of the jaw 迠 The present invention relates to a kind of incident light received from its side can be transformed into a uniform The linearly polarized light is then emitted from its two surfaces on an oscillating surface under control, so that it is suitable for forming polarizing tubes and planar polarized light sources for backlights for liquid crystal display devices. This application is based on Japanese Patent Application Nos. Hei. 1 and 1 31 1 429, U-131430, Π-138102, 1 and 1 166727, 1 and 1 74 368, and 11-197083, which are incorporated herein by reference data. k Description of Related Art Regarding an edge-light type light pipe that can be used as a backlight for a liquid crystal device, a device including a light-emitting member made of a reflection point provided on a light-transmitting resin plate, etc. has been hitherto known The light transmitting resin plate has a configuration in which the transmitted light 1 generated by total reflection is emitted from one of the two surfaces of the plate through scattering or the like. However, the aforementioned emitted light has natural light with little or no polarization, so it is necessary to convert it into linearly polarized light through a polarizing plate before the liquid crystal display. Therefore, the aforementioned device has the disadvantage that the polarizing plate causes absorption loss' and the percentage utilization of light cannot exceed 50%. Under the foregoing circumstances, a system (JP-A) including a polarization conversion member having a combination of a polarization separation plate using a Brewster angle to generate linearly polarized light and a phase difference plate is proposed in addition to the foregoing configuration (JP-A -6-18873 C The term "jp-Aj" as used herein means "an unexamined and published Japanese patent application"), JP-A-6-160840, JP-A-6-265892, JP-A- 7-72475, JP-A-7-261122,
89109116.ptc 第5頁 455704 _案號891 (mm_年月 日 倏色 五、發明說明(2) ' -- JP-A-7-270 792 ^ JP-A-9-54556 ' JP-A - 9- 1 05933, JP-A-9-138406 、JP-a-9-152604 、JP-A-9-293406 、 JP-A-9-326205、JP-a-1〇_78581)。然而,此一背光無法 提供足夠的極化’且幾乎無法控制極化方向。因此,·>此一 背光幾乎無法作實際利用。 發明之概述 本發明之一目的在於提供一種偏光管,其包括有—光透 射樹脂板及層合於光透射樹脂板之一面或兩面上之偏光散 射板的。此偏光散射板具有分散於其中之微小雙折射晶 域,以展現歸因於極化方向的散射各向異性。 根據本發明,在前述的配置中,當在侧面接收自然光 時’可自兩表面有效率地發射線性偏光,而無需形成特殊 的光發射構件,諸如在光透射樹脂板上之反射點。此外, 當線性偏光通過額外使用之偏光散射板的光學軸時,可得 到具有對應於振盈方向的線性偏光。因此,可經由控制偏 光散射板之光學軸而任意改變線性偏光之振盪方向。更甚 者,可自此一具有設置於另一表面上之單向反射層之偏光 管的一個表面發射偏光,以增進每個表面的發射效率,而 使其可提供具有優異擴散性質的線性偏光。經由將液體顯 示元件設置於偏光管上,以使兩元件之光學轴彼此平行之 此一配置,可達到接近一般值兩倍的亮度。 在前述說明中,經於光管之側面接收的入射光經由光管 内部透射,同時由於與空氣之折射率的差異而重複全反 射,然後再進入偏光散射板中。在被偏光散射板接收之入 89109116.ptc 第6頁 455704 ___89109116-年月 g_____ 五、發明說明⑶ ~ 射光的成份中’具有平行於顯現與微小晶域之折射率之最 大差異(Δηΐ)之軸向(Δηΐ方向)的振盪平面的線性偏光被 選擇性地強烈散射。在小於全反射角之角度下反射之一部 分的線性偏光成份被光管發射。在此配置十,光映於單向 反射層側上’然後再供給至相對侧内(沒有單面反射層之 光管的另一表面)。因此’光集中發射於光管的另一側 上。因此’線性偏光可透過光擴散層自光管的一表面擴 散’而不會使極化度大大地退化,然後再以良好的均勻度 發射。 另一方面,在Δηΐ方向之大角度下散射之光,滿足關於 Anl方向之條件但尚未被散射之光,及具有除方向外 之振盪方向的光被限制於其所透射的光管中,同時龙重複 全反射。此等成份以此方式等待由於偏光散射板所造成之 雙折射相的差異而被退極化,及滿足關於△ n〗方向之條 件,而將其發射出去之機會。經由重複此程序,而可有效 率地自光管發射具有預定振盪平面的線性偏光。 前述的偏光散射板以包括一其中分散有微小晶域之透明 薄膜’此微小晶域包括在低於構成透明薄膜之基材之聚合 物之玻璃轉移溫度的溫度下展現出向列,且具有5〇 X:以上 之玻璃轉移溫度的液晶聚合物較佳。 在此配置中,可製得具有優異耐熱性的偏光管β如此製 得的偏光管極不易發生變形及功能退化,即使當其於光源 的長時間操作後受到溫度上升時亦然。因此,本發明之偏 光管的耐用性,尤其係熱安定性優異。89109116.ptc Page 5 455704 _Case No. 891 (mm_year, month, day, time, date, fifth, description of the invention (2) '-JP-A-7-270 792 ^ JP-A-9-54556' JP-A- 9- 1 05933, JP-A-9-138406, JP-a-9-152604, JP-A-9-293406, JP-A-9-326205, JP-a-10_78581). However, this backlight cannot provide sufficient polarization 'and it is almost impossible to control the polarization direction. Therefore, > This backlight can hardly be practically used. SUMMARY OF THE INVENTION An object of the present invention is to provide a polarizer including a light transmitting resin plate and a polarizing light diffusing plate laminated on one or both sides of the light transmitting resin plate. This polarizing light scattering plate has minute birefringent crystal domains dispersed therein to exhibit scattering anisotropy due to the direction of polarization. According to the present invention, in the foregoing configuration, when natural light is received at the side, linearly polarized light can be efficiently emitted from both surfaces without forming a special light emitting member such as a reflection point on a light transmitting resin plate. In addition, when linearly polarized light passes through the optical axis of a polarizing light scattering plate additionally used, linearly polarized light having a direction corresponding to the vibration direction can be obtained. Therefore, the direction of oscillation of the linearly polarized light can be arbitrarily changed by controlling the optical axis of the polarized light scattering plate. Furthermore, polarized light can be emitted from one surface of a polarizer having a one-way reflective layer provided on the other surface to enhance the emission efficiency of each surface, so that it can provide linearly polarized light with excellent diffusion properties. . By arranging the liquid display element on the polarizer so that the optical axes of the two elements are parallel to each other, a brightness close to twice the normal value can be achieved. In the foregoing description, the incident light received through the side of the light pipe is transmitted through the inside of the light pipe, and at the same time, the total reflection is repeated due to the difference in refractive index with the air, and then it enters the polarized light scattering plate. 89109116.ptc received by the polarized light scattering plate Page 6 455704 ___ 89109116-year month g_____ V. Description of the invention ⑶ ~ The component of the emitted light 'has an axis parallel to the largest difference (Δηΐ) between the refractive index of the manifestation and the small crystal domain The linearly polarized light in the (Δηΐ direction) oscillation plane is selectively strongly scattered. A part of the linearly polarized light reflected at an angle smaller than the total reflection angle is emitted by the light pipe. In this configuration, the light is reflected on the side of the one-way reflection layer 'and then supplied to the opposite side (the other surface of the light pipe without the one-side reflection layer). Therefore, the 'light is concentratedly emitted on the other side of the light pipe. Therefore, 'linearly polarized light can be diffused from one surface of the light pipe through the light diffusion layer' without greatly degrading polarization, and then emitted with good uniformity. On the other hand, light scattered at a large angle in the Δηΐ direction meets the conditions of the Anl direction but has not yet been scattered, and light with an oscillation direction other than the direction is restricted to the light pipe that it transmits. Dragon repeats total reflection. In this way, these components wait for an opportunity to be depolarized due to the difference in the birefringent phase caused by the polarized light scattering plate, and to satisfy the conditions regarding the direction of Δ n and to emit them. By repeating this procedure, linearly polarized light having a predetermined oscillation plane can be efficiently emitted from the light pipe. The aforementioned polarizing light scattering plate includes a transparent film in which minute crystal domains are dispersed. This minute crystal domain includes nematics at a temperature lower than the glass transition temperature of the polymer constituting the substrate of the transparent film, and has a temperature of 50%. X: A liquid crystal polymer having a glass transition temperature above is preferred. In this configuration, a polarizer β having excellent heat resistance can be obtained. The polarizer thus produced is extremely unlikely to be deformed and deteriorated in function, even when it is subjected to temperature rise after long-term operation of the light source. Therefore, the polarizer of the present invention is excellent in durability, especially in thermal stability.
89109116.ptc 第7頁 45 57 0489109116.ptc Page 7 45 57 04
本發明更提供一種偏光管,苴台^ e 丹包括具有於其之一表面上 設置之單向反射層及於另一表面μ #堪―r · 衣甶上設置之至少一個極化錐 持透鏡片之前述偏光散射板作為層合物…種平面偏光 源,其包括於偏光管之至少一側面上設置之光源。 極化維持透鏡片控制發射光的路#,而得㈣前方之方向 性優異的線性偏光。經由將液晶元件設置於極化維持透鏡 片上’可得到一般值之1.5倍以上的亮度。 本發明更提供一種偏光管,其包括具有雙折射光透射樹 脂板,及於其之一或兩表面上設置之具有分散於其中之微 小雙折射晶域’且視極化方向而顯現散射之各向異性之偏 光散射板之層合物’該層合物包括於其之一表面上設置的 單向反射層;及一種平面偏光源,其包括於偏光管之至少 一側面上設置之光源。在此配置中,先透射樹脂板利用其 雙折射有效率地消除極化’因此而提高前述發射的機會, 而使其可提高亮度。 本發明更提供一種偏光管’其包括光透射樹脂板,及以 光路徑插置於其間’而部分設成與其之一或兩表面緊密接 觸之具有分散於其中之微小雙折射晶域,且視極化方向而 顯現散射之各向異性之偏光散射板;及一種平面偏光源, 其包括於偏光管之至少一側面上設置之光源。 根據本發明,光管可於其側面接收自然光,然後再自其 之兩表面以良好的亮度均勻度有效率地發射線性偏光。 更詳細說明,經於光透射樹脂板之側面接收的入射光被 樹脂板的内部透射,同時由於與空氣之折射率的差異而重The present invention further provides a polarizing tube, which includes a unidirectional reflective layer provided on one surface thereof and at least one polarizing cone-shaped lens provided on the other surface μ # CAN―r. The aforementioned polarizing light scattering plate of the sheet is a laminate ... a kind of planar polarizing light source, which includes a light source provided on at least one side surface of the polarizing tube. The polarization maintaining lens sheet controls the path # of the emitted light, and achieves linearly polarized light with excellent directivity in the front direction. By placing the liquid crystal element on the polarization maintaining lens sheet ', a brightness of 1.5 times or more of the normal value can be obtained. The present invention further provides a polarizer including a birefringent light-transmitting resin plate, and micro-birefringent crystal domains dispersed therein disposed on one or both surfaces thereof, each of which exhibits scattering depending on a polarization direction. A laminate of an anisotropic polarized light scattering plate. The laminate includes a one-way reflective layer provided on one surface thereof; and a planar polarized light source including a light source provided on at least one side surface of a polarizer. In this configuration, the first transmissive resin plate uses its birefringence to effectively eliminate polarization ', thereby increasing the opportunity for the aforementioned emission, so that it can increase brightness. The present invention further provides a polarizing tube which includes a light transmitting resin plate and a light path interposed therebetween, and is partially disposed in close contact with one or both surfaces thereof, and has micro-birefringent crystal domains dispersed therein. An anisotropic polarized light scattering plate showing polarization in the direction of polarization; and a planar polarized light source including a light source disposed on at least one side of a polarizer. According to the present invention, the light pipe can receive natural light on its side, and then efficiently emit linearly polarized light from both surfaces with good brightness uniformity. In more detail, the incident light received through the side of the light-transmitting resin plate is transmitted by the inside of the resin plate, and at the same time is heavy due to the difference in refractive index with the air.
89109116.ptc 第 8 頁 455704 ___89IQ9116___车月曰_ 五、發明說明(5) 複全反射’然後經由光路徑經歷散射而進入偏光散射板, 其接著再自光管發射。因此,入射光之量,及因而亮度, 可藉由與先路徑接觸之面積而作控制。 本發明之特色及優點當可由以下結合附圖說明之較佳具 體例的詳細說明而更加明白。 較佳具體例之明 根據本發明之偏光管包括光透射樹脂板及具有分散於其 中之微小雙折射晶域,且視極化方向而顯現散射之各向異 性’並層合於光透射樹脂板之一或兩個表面上之偏光散射 板。圖1及2顯示偏光管之一具體例。元件編號〗係指示光 透射樹脂板’元件編號3係指示偏光散射板,及元件編號2 係指示非必需的黏著劑層。 偏光散射板3包括其中分散有包含液晶聚合物之微小晶 域之透明薄膜,此液晶聚合物在低於構成薄膜之聚合物 (基材聚合物)之玻璃轉移溫度的溫度下展現出向列,且具 有5 0 °C以上之玻璃轉移溫度。 ” 作為層合物之偏光管可更句乜於甘 ^ __ , 叉巴栝於其之一表面上設置的簞 面反射層’及於另一表面上姐罢 # @ t m 衣面上°又置之至少一個極化維持光擴 散層。此配置之一呈體如丨千认阳„ υ '、筱例不於圖3 »元件編號4係指示層厶 物(偏光散射板),元件編號6 # _ 層σ 诉指不單向反射層, 編號7係指示光擴散層。圖3說 兀件 光源的一具體例。元件編號5係指示光源。 +面偏 前述層合物可更包括於其之£ . ' 、来μ , # , ' <方一表面上設置的極卟杖 透名兄片。在圖4,元件編號8係指示透鏡片。 ,准持89109116.ptc Page 8 455704 ___89IQ9116___ Che Yueyue_ V. Description of the invention (5) Complex total reflection ’then undergoes scattering through the light path and enters the polarized light scattering plate, which is then emitted from the light pipe. Therefore, the amount of incident light, and thus the brightness, can be controlled by the area in contact with the anterior path. The features and advantages of the present invention will be more clearly understood from the following detailed description of preferred specific examples described in conjunction with the accompanying drawings. The description of a preferred specific example A polarizer according to the present invention includes a light-transmitting resin plate and a micro-birefringent crystal domain dispersed therein, and exhibits anisotropy of scattering depending on the polarization direction, and is laminated on the light-transmitting resin plate. A polarizing light scattering plate on one or both surfaces. Figures 1 and 2 show a specific example of a polarizer. The element number is a light transmitting resin plate, and the element number 3 is a polarizing light scattering plate, and the element number 2 is a non-essential adhesive layer. The polarizing light scattering plate 3 includes a transparent film in which minute crystal domains including a liquid crystal polymer are dispersed, the liquid crystal polymer exhibiting nematicity at a temperature lower than the glass transition temperature of the polymer (substrate polymer) constituting the film, and Has a glass transition temperature above 50 ° C. ”As a laminated polarizer, you can say more about Gan ^ __, and you can use a reflective surface on one surface of it, and on the other surface. # @ Tm 衣 面 ° 又 置At least one polarization maintains a light diffusion layer. One of the configurations is like Qian Qianyang „υ ', Xiao example is not as shown in FIG. 3» Element No. 4 is an indicator layer (polarizing light scattering plate), and element number 6 # _ Layer σ refers to a non-unidirectional reflective layer, and the number 7 indicates a light diffusion layer. Fig. 3 illustrates a specific example of the element light source. Element number 5 indicates the light source. + 面面 The aforementioned laminate may further include £. ', 来 μ, #,' < Porous porcine rods on the surface of the side. In FIG. 4, the element number 8 indicates a lens sheet. , Hold
W326\2d-\90-〇3\891091!6.ptc 4 5 5 7 891〇9116 五、發明說明(6) 曰W326 \ 2d- \ 90-〇3 \ 891091! 6.ptc 4 5 5 7 891〇9116 V. Description of the invention (6)
板之 根據本發明之偏光管可更包括經部分A + & , A 或兩個表面緊密接觸’並在其間插置光路徑之= 散射板。此配置之一具體例示於阁β _ ^ ^ ^ 你丹間插置光路徑之前述 的偏光散射板。此配置之一具體例示於囷6 ^元件編 $ 指示光透射樹脂板,元件編號9係指示去故’ 1务、 不九路徑,及元件編 號3係指示偏光散射板。此等組件形成為具有最少所 元之偏光管的層合物4。圖6說明包含前述偏光管之 光源的一具體例。 關於光透射樹脂板,可使用由對來自光源之光之預定波 長顯現透明度之適當材料所形成的任何扁平材料。舉例來 說,對於可見光範圍,可使用由丙烯酸系樹脂、聚碳酸酯 樹脂、苯乙烯系樹脂、去甲為烯基樹脂、環氧樹脂等等製 成之扁平材料較佳。由透光率的觀點來看,由具有儘可能 小之折射率之樹脂製成的扁平材料為較佳。此外,將耐用 性列入考慮,由具有優異耐熱性之樹脂製成的扁平材料為 較佳。 關於光透射樹脂板’可使用展現平面内雙折射的材料, 以消除由光管之内部所透射之光的極化,而增加自偏光散 射板發射之機會,因此而增進亮度。為有效地消除極化, 使用以平面内之平均相差計算,具有5 0毫微米以上之歸因 於雙折射之相差的材料較佳,6〇毫微米以上更佳,7〇毫微 米以上為特佳。此外’為防止不均句的亮度,使用具有儘 可能小之不均勻相差的材料較佳。 古雙折射光透射樹脂板之形成可利用任何適當方法完成’ 諸如包括在板的形成過種中利用應變等等發展定向雙折射Plate The polarizing tube according to the present invention may further include a diffusing plate via a portion A + & A or both surfaces in close contact 'with an optical path interposed therebetween. One specific example of this configuration is shown in the above-mentioned polarized light scattering plate in which the light path is interposed between β and ^. One specific example of this configuration is shown in 囷 6 ^ element series $ indicates a light-transmitting resin plate, element number 9 indicates the direction of failure, and the path number is 3, and element number 3 indicates a polarized light scattering plate. These components are formed as a laminate 4 having a polarizer with a minimum of elements. Fig. 6 illustrates a specific example of a light source including the aforementioned polarizer. As for the light transmitting resin plate, any flat material formed of a suitable material that exhibits transparency to a predetermined wavelength of light from a light source can be used. For example, for the visible light range, a flat material made of an acrylic resin, a polycarbonate resin, a styrene resin, a norbornene-based resin, an epoxy resin, or the like can be preferably used. From the viewpoint of light transmittance, a flat material made of a resin having a refractive index as small as possible is preferable. Further, in consideration of durability, a flat material made of a resin having excellent heat resistance is preferable. Regarding the light-transmitting resin plate ', a material exhibiting birefringence in a plane can be used to eliminate polarization of light transmitted through the inside of the light pipe and increase the chance of emission from the self-polarizing light-diffusing plate, thereby improving brightness. In order to effectively eliminate the polarization, a material with a phase difference due to birefringence of more than 50 nm, which is calculated based on the average phase difference in the plane, is preferably more than 60 nm, and more preferably 70 nm or more. good. In addition, in order to prevent the brightness of the uneven sentence, it is preferable to use a material having as small unevenness as possible. The formation of ancient birefringent light-transmitting resin plates can be accomplished by any suitable method, such as including the development of directional birefringence, including the use of strain in the formation of plates, and the like.
第10頁 ^ 4557 04Page 10 ^ 4557 04
修正 _銮號 89109114 五、發明說明(7) 之方法,包括拉伸 場或磁場的作用下 的觀點來看,此等 發展定向雙折射之 脂、聚碳酸酯樹脂 之方法,包括輥壓之 使樹脂定向之方法。 方法中之特佳方法為 方法。由此觀點來看 等等為較佳。 方法’及包括在電 由大量製造樹脂板 包括利用應變等等 ’使用丙烯酸系樹 為維持發射光之期望的極化性質,使用具有儘可能小之 平面内相差的樹脂板為較佳。由此觀點來看,使用極不 由於在板之形成過程中之應變等等而產生定向雙折射之材 料,尤其係聚曱基丙稀酸甲酿或去甲范烯基樹脂為較佳。 此一樹脂可適當地形成為板。 光透射樹脂板之形狀可根據液晶單元之尺寸 '光源之特 性、發射光之亮度的均勻程度等等適當地決定,因此並無 特殊之限制。由可成形性等等的觀點來看,使用扁平或楔 形板為較佳。光透射樹脂板之厚度可根據光源及液晶單元 之尺寸適當地決定,因此並無特殊之限制。然而,為降低 光&之厚度及重量,光透射樹脂板以儘可能薄較佳,明確 言之為10毫米以下,尤其係自0.5至5毫米。 光透射樹脂板之形成可利用任何適當的方法完成,諸如 注塑法、、鑄塑法、擠塑法、流鑄法、輥塗法、壓鑄法及反 應左塑法(RIM)。為形成光透射樹脂板,可將適當的添加 劑’諸如變色抑制劑、氧化抑制剤、紫外光吸收劑及離模 劑’加至材料中。 另一方面’可使用包含分散於其中之微小雙折射晶域的 任何適當材料作為偏光散射板,以視極化方向而展現散射Modification _ 銮 89109114 V. Description of the invention (7), including the viewpoint of the action of a tensile field or a magnetic field, these methods of developing directional birefringent grease, polycarbonate resin, including rolling Resin orientation method. A particularly preferred method is the method. From this point of view, etc. is better. The method 'and the production of a resin plate including a large amount of electricity, including the use of strain, etc.' Using an acrylic tree In order to maintain the desired polarization properties of the emitted light, it is preferable to use a resin plate having a phase difference as small as possible. From this point of view, it is preferable to use a material that does not cause directional birefringence due to strain or the like during the formation of the plate, especially a polyacrylic acrylic or methylphenidyl resin. This resin can be suitably formed into a board. The shape of the light-transmitting resin plate can be appropriately determined according to the size of the liquid crystal cell, the characteristics of the light source, the uniformity of the brightness of the emitted light, and the like, so there is no particular limitation. From the viewpoint of formability and the like, it is preferable to use a flat or wedge-shaped plate. The thickness of the light-transmitting resin plate can be appropriately determined according to the size of the light source and the liquid crystal cell, so there is no particular limitation. However, in order to reduce the thickness and weight of light, it is preferable that the light transmitting resin plate be as thin as possible, specifically, 10 mm or less, especially from 0.5 to 5 mm. The formation of the light-transmitting resin sheet can be performed by any appropriate method, such as injection molding, casting, extrusion, flow casting, roll coating, die casting, and reaction left plastic (RIM). To form a light-transmitting resin plate, appropriate additives such as a discoloration inhibitor, an oxidation-inhibiting hafnium, an ultraviolet light absorber, and a release agent 'can be added to the material. On the other hand ’, any suitable material containing tiny birefringent crystal domains dispersed therein can be used as a polarizing light scattering plate to show scattering depending on the direction of polarization
89109116.ptc 第11頁 4557 04 — ___89109116.__±——^-§ 修正__ 五、發明說明(8) 之各向異性。偏光散射板之一例子為其中分散有微小雙折 射晶域之透明薄膜。 舉例來說,可使用包含其中分散有包含液晶聚合物之微 小晶域之透明薄膜,且視極化方向而顯現散射之各向異性 的材料,此液晶聚合物在低於構成薄膜之聚合物之玻璃轉 移溫度的溫度下展現出向列’且具有50 t以上之玻璃轉移 溫度。在此配置中,可製得耐熱性優異的偏光散射板,而 使其可形成熱安定性優異的偏光管。 前述顯現散射之各向異性之偏光散射板的形成可利用任 何適當方法完成,諸如包括利用拉伸等等使具有優異透明 度之一或多種適當材料諸如聚合物及液晶接受適當定向之 方法,在此一組合中,形成具有不同雙折射之區域,而製 得定向薄膜。 前述組合之例子包括聚合 物及各向異性聚合物之組合 由微小晶域之分散分佈的觀 組合較佳。微小晶域之分散 性作控制。相分離可利用任 用溶劑溶解不相容材料之方 及炼融於推合物中之方法。 物及液晶之組合,等向性聚合 ’及各向異性聚合物之組合。 點來看’使用會造成相分離的 分佈可利用待結合材料之相容 何適當方法完成,諸如包括利 法,及包括將不相容材料加熱 在經由拉伸而於前述 ί物及液晶之組合及等向性聚合物及各向異性聚 Ϊ性ί =在任意溫度及拉伸比下拉伸iUt 、° 組口’則可經由適當地控制拉伸條件,而;89109116.ptc Page 11 4557 04 — ___ 89109116 .__ ± —— ^-§ Amendment __ 5. Anisotropy of invention description (8). An example of a polarizing light-scattering plate is a transparent film in which minute birefringent crystal domains are dispersed. For example, a material including a transparent film in which minute crystal domains including a liquid crystal polymer are dispersed and exhibiting anisotropy of scattering depending on the polarization direction can be used. This liquid crystal polymer is lower than the polymer constituting the film. The glass transition temperature exhibits nematic 'and has a glass transition temperature of 50 t or more. In this configuration, a polarizing plate having excellent heat resistance can be obtained, and a polarizing tube having excellent thermal stability can be formed. The formation of the aforementioned anisotropic polarizing light scattering plate which can exhibit scattering can be accomplished by any suitable method, such as a method in which one or more appropriate materials having excellent transparency such as polymer and liquid crystal are subjected to proper orientation using stretching or the like, and here In one combination, regions having different birefringences are formed, and an oriented film is prepared. Examples of the foregoing combination include a combination of a polymer and an anisotropic polymer, and a combination of dispersive distribution of minute crystal domains is preferable. The dispersion of the tiny crystal domains is controlled. Phase separation can be achieved by dissolving incompatible materials with any solvent and melting in the inferred material. A combination of a polymer and a liquid crystal, a combination of anisotropic polymerization and an anisotropic polymer. Point to point 'The use of the distribution that will cause phase separation can be accomplished using any suitable method of compatibility of the materials to be bonded, such as including liquefaction, and including heating incompatible materials to a combination of the foregoing materials and liquid crystals by stretching. And isotropic polymers and anisotropic polymers ί = stretching iUt, ° at any temperature and stretching ratio can be through appropriate control of the stretching conditions, and;
455704455704
成期望的偏 中之折射率 負各向異性 合物之組合 物及負各向 光散射板。 的變化,而 聚合物皆可 ,負各向異 異性聚合物 各向異性聚 分類為正或 使用。可使 性聚合物之 之組合》 合物可根據 負。在本發 用任何的正 组合及正各 在杈伸方向 明中,正及 各向異性聚 向異性聚合 前述聚合物之例子包括酯基聚合物諸如聚對笨二甲酸 二酯及聚萘二甲酸乙二酯,苯乙烯基聚合物諸如聚笨乙^ 及丙烯腈-苯乙烯共聚物(AS聚合物),烯烴聚合物諸如聚 乙烯、聚丙烯、具有環或去甲;fg烯結構之聚烯烴及乙稀— 丙婦共聚物’丙烯酸系聚合物諸如聚曱基丙烯酸曱酷、纖 維素基聚合物諸如二醋酸纖維素及三醋酸纖維素,及醯胺 基聚合物諸如耐綸及芳族聚醯胺。 前述透明聚合物之其他例子包括熱固性或紫外光固化聚 ^物諸如碳酸酯基聚合物、氣乙烯基聚合物、醯亞胺基聚 合物、颯基聚合物、聚醚颯、聚醚醚酮、聚亞笨基硫醚、 $稀醇基聚合物、偏二氯乙稀基聚合物、乙烯縮丁齡基聚 合物、丙烯酸酯基聚合物 '聚甲醛、聚矽氧基聚合物、胺 ^甲酸醋基聚合物、醚基聚合物、乙酸乙烯酯基聚合物、 剛述聚合物之摻混物、酚聚合物、三聚氰胺基聚合物、丙 歸酸系聚合物、胺基甲酸酯基聚合物、胺基甲酸酯丙烯基 聚合物、環氣基聚合物、及聚矽氧基聚合物。 尤其’在期望波長範圍諸如可見光範圍中之透明度優異 的聚合物為較佳。為製得熱安定性優異的偏光散射板,使 用具有80 t以上之載荷下撓曲溫度,及丨丨〇 Ό以上之玻璃A combination of negative refractive index and a desired anisotropic composition and a negative isotropic light scattering plate. While the polymer can be changed, the negative anisotropic polymer is classified as positive or used as anisotropic polymer. The combination of functional polymers can be negative. In any positive combination and positive directions used in the present invention, positive and anisotropic polyanisotropic polymerization. Examples of the foregoing polymers include ester-based polymers such as polyethylene terephthalate and polynaphthalate. Ethylene glycol, styrene-based polymers such as polystyrene and acrylonitrile-styrene copolymers (AS polymers), olefin polymers such as polyethylene, polypropylene, polyolefins with cyclic or nor methylene; fg olefin structures And ethylene-acrylic copolymers' acrylic polymers such as polyacrylic acrylic polymers, cellulose-based polymers such as cellulose diacetate and cellulose triacetate, and amine-based polymers such as nylon and aromatic polymers Lamine. Other examples of the aforementioned transparent polymers include thermosetting or UV-curable polymers such as carbonate-based polymers, vinyl-based polymers, ammonium-based polymers, amidine-based polymers, polyethers, polyetheretherketones, Polybenzylene sulfide, dilute alcohol-based polymer, vinylidene chloride-based polymer, ethylene butylene-based polymer, acrylate-based polymer 'polyoxymethylene, polysiloxy polymer, amine formic acid Acetate-based polymers, ether-based polymers, vinyl acetate-based polymers, blends of polymers just described, phenol polymers, melamine-based polymers, propionic acid-based polymers, urethane-based polymers , Urethane propylene-based polymers, ring gas-based polymers, and polysiloxy polymers. In particular, a polymer excellent in transparency in a desired wavelength range such as a visible light range is preferred. In order to obtain a polarizing light scattering plate with excellent thermal stability, a glass having a deflection temperature under a load of 80 t or more and a temperature of 丨 丨 〇 Ό is used.
4557 04 η 修正 曰 _案號 89109116 五、發明說明(10) 轉移溫度的聚合物為較佳’玻璃轉移溫度為1151 佳,1 2 D C以上為特佳。載荷下挽曲:w声4557 04 η Amendment _ Case No. 89109116 V. Description of the invention (10) Polymers with a transition temperature are preferred 'The glass transition temperature is preferably 1151, and above 1 2 D C is particularly preferred. Elbow under load: w sound
If 79Π7J产视曲恤度之測ϊ係根據J IS K 7207進仃。更洋細說明,使加熱槽中之熱傳介質在2。〔 /分鐘之速率下加熱’同時使在加熱槽中之具有"毫米高 度的試樣受到I 8. 5公斤力/平方公分之彎曲應力。將:樣 之撓曲達到0, 32毫米之熱傳介質的溫度定義為栽荷下撓曲 溫度。 液晶之例子包括在室溫或高溫下展現向列或距列的低分 子液晶或可交聯液晶單體,諸如氣基聯苯基化合物氰 基環己烧基化合物、氰苯基醋基化合物、$甲酸苯基醋基 化合物、苯基嘧啶基化合物及其混合物,及在室溫 下展現出向列或距列的液晶聚合物。一般先使前述的可交 聯液晶單體進行定向’隨後再利用適當的方式諸如埶 交聯,而成為聚合物。 為製得耐熱性、耐用性等等優異之偏光散射板,將具有 50 C以上之破璃轉移溫度,以8〇 t以上更佳,12〇 t以上 特佳之聚合物與可交聯液晶單體或液晶聚合物結合使用較 佳。關於液晶聚合物,其可為任何適當材料諸如主鏈型化 合物及側鏈型化合物。液晶聚合物之種類並無特殊之限 制。 利用液晶聚合物形成偏光散射板,可藉由包括將一或多 種聚合物與一或多種供形成微小晶域用之液晶聚合物混 合,形,具有液晶聚合物以微小區域之形態分散於其中之 聚合物薄膜,然後再使聚合物薄膜接受適當的定向,而形If 79Π7J produces visual music shirt, the measurement is based on J IS K 7207. More detailed explanation, make the heat transfer medium in the heating tank at 2. [Heating at a rate per minute 'while subjecting the specimen having a height of " mm in the heating bath to a bending stress of 8.5 kgf / cm2. The temperature of the heat transfer medium whose deflection reaches 0,32 mm is defined as the deflection temperature under load. Examples of liquid crystals include low-molecular liquid crystals or crosslinkable liquid crystal monomers that exhibit nematic or pitch at room temperature or high temperature, such as cyanobiphenyl compounds, cyanocyclohexyl compounds, cyanophenylacetate compounds, A formic acid phenylacetate compound, a phenylpyrimidinyl compound, and a mixture thereof, and a liquid crystal polymer exhibiting nematic or pitch at room temperature. Generally, the aforementioned crosslinkable liquid crystal monomer is first aligned 'and then crosslinked by a suitable method such as fluorene to form a polymer. In order to obtain a polarizing light scattering plate with excellent heat resistance, durability, etc., it will have a glass breaking temperature of 50 C or more, more preferably 80t or more, and particularly good polymer and crosslinkable liquid crystal monomers of 120t or more. Or a combination of liquid crystal polymers is preferred. As for the liquid crystal polymer, it may be any appropriate material such as a main chain type compound and a side chain type compound. The type of the liquid crystal polymer is not particularly limited. The liquid crystal polymer is used to form a polarized light scattering plate, and the liquid crystal polymer can be formed by mixing one or more polymers with one or more liquid crystal polymers for forming minute crystal domains, and the liquid crystal polymer is dispersed in the form of minute regions. Polymer film, and then subject the polymer film to the proper orientation and shape
89109116.ptc 第14頁 455704 _案號89109116_年月 p 修正__ 五、發明說明(11) 成具有不同雙折射之區域的方法完成。 由藉由定向而控制前述折射率差Δηΐ及An2之容易度的 觀點來看,可使用具有50 °C之玻璃轉移溫度,且在低於構 成薄膜之聚合物之玻璃轉移溫度的溫度下展現出向列之材 料作為供形成微小晶域用之液晶聚合物。此處所使用之液 晶聚合物的種類並無特殊之限制。可使用展現此種性質之 主鏈型或側鏈型的適當液晶聚合物。 前述液晶聚合物之特定例子包括具有由以下通式所表示 之單體單元的側鏈液晶聚合物。側鏈型液晶聚合物可為適 胃的熱塑性聚合物,諸如具有此一單體單元之均聚物及共 % 尤其,單晶域定向性優異的此一熱塑性聚合物為較 佳。89109116.ptc Page 14 455704 _Case No. 89109116_year p Modification __ 5. Description of the invention (11) The method of forming regions with different birefringence is completed. From the viewpoint of controlling the ease of the aforementioned refractive index difference Δηΐ and An2 by orientation, it is possible to use a glass transition temperature having a temperature of 50 ° C and exhibit the orientation at a temperature lower than the glass transition temperature of the polymer constituting the film The listed materials are used as liquid crystal polymers for forming minute crystal domains. The type of liquid crystal polymer used here is not particularly limited. Appropriate liquid crystal polymers of a main chain type or a side chain type which exhibit such properties can be used. Specific examples of the aforementioned liquid crystal polymer include a side chain liquid crystal polymer having a monomer unit represented by the following general formula. The side chain liquid crystal polymer may be a stomach-friendly thermoplastic polymer, such as a homopolymer having a single monomer unit and a total%. In particular, this thermoplastic polymer having excellent single crystal domain orientation is preferred.
在前述通式中,X代表形成液晶聚合物之主鏈的架構基 3 ’其可利用適當的連接鏈諸如直键、分支鏈及環鏈形 臂。架構基團之例子包括聚丙烯酸醋、聚曱基丙烯酸酯、 鹵丙烯酸酯 '聚氰基丙烯酸酯、聚丙烯醯胺、 =丙烯腈、聚甲基丙烯腈、聚醯胺、聚酯、聚胺基甲酸 θ聚驗、聚醮亞胺、及聚環己烷。 性代表自主鍵分支之隔離基團。由偏光散射板之可成形 绪士對折射率之控制容易度的觀點來看。隔離基困之In the foregoing general formula, X represents a structural group 3 'which forms the main chain of the liquid crystal polymer, which can utilize appropriate linking chains such as straight bonds, branched chains, and ring-shaped arms. Examples of structural groups include polyacrylic acid, polyacrylic acid acrylate, haloacrylate 'polycyanoacrylate, polyacrylamide, acrylonitrile, polymethacrylonitrile, polyacrylamide, polyester, polyamine Carboxylic acid theta polymer test, polyimide, and polycyclohexane. Sex represents an isolating group branched by an autonomous bond. From the viewpoint of the ease of controlling the refractive index from the formability of polarized light scattering plates. Segregated base
第15頁 4 5 5 7 0 4 案號 89109116 月 修正 五、發明説明(12) 例子包括伸乙基、伸丙基、伸丁基、伸戊基、伸己基、伸 辛基、伸癸基、伸十一基、伸十二基、伸十八基、乙氧伸 乙基、及甲氧伸丁基。 另一方面,Z代表賦予液晶定向性(向列定向性)的介原 (mesogen)基團。以下將列示介原基團之例子。 C,H· —(〇^-,Page 15 4 5 5 7 0 4 Case No. 89109116 Amendment V. Description of the Invention (12) Examples include ethylene, propyl, butyl, pentyl, hexyl, octyl, decyl, Undecyl, dodecyl, octadecyl, ethoxyethyl, and methoxybutyl. On the other hand, Z represents a mesogen group that imparts liquid crystal alignment (nematic alignment). Examples of mesogen groups are listed below. C, H ·-(〇 ^-,
-(O^co.^o^c^c^o)- —〇c〇-^(〇y~ —c = c— A -^(〇)-CH = N—(〇)- A . 乂~^-(〇)^csc"^qV- a c o.-(O ^ co. ^ O ^ c ^ c ^ o)-—〇c〇-^ (〇y ~ —c = c— A-^ (〇) -CH = N— (〇)-A. 乂 ~ ^-(〇) ^ csc " ^ qV- ac o.
-C〇M 在先前的化合物中’端基取代基a可為適當的基團,諸 如氰基、烷基、烯基、烷氧基、氧烷基及一或多個氫原子 為氟或氣取代之産烧基、自燒氧基及齒稀基。 隔離基團Y及介原基團Z可經由醚鍵,即-〇-,而彼此連 接。介原基團Z中之苯基可有一或多個氫原子被鹵素取 代。所使用的齒素為氯或氟較佳。 利用前述的可向列定向液晶聚合物形成偏光散射板可藉 由例如包括將供形成聚合物薄膜用之聚合物與液晶聚合物 混合,形成具有液晶聚合物以微小區域之形態分散於其中-COM In the previous compounds, the 'end group substituent a may be a suitable group such as cyano, alkyl, alkenyl, alkoxy, oxyalkyl and one or more hydrogen atoms are fluorine or gas. Substituted alkanoyl, self-oxygenated and dilute oxo groups. The spacer group Y and the mesogen group Z may be connected to each other via an ether bond, that is, -0-. The phenyl group in the mesogen group Z may be substituted with one or more hydrogen atoms by a halogen. The dentition used is preferably chlorine or fluorine. The formation of the polarized light scattering plate using the aforementioned nematic liquid crystal polymer can include, for example, mixing a polymer for forming a polymer film with a liquid crystal polymer to form a liquid crystal polymer dispersed therein in a microscopic region.
89109116.ptc 第16頁 4557 04 ___案號 891091H____^^__ 五、發明說明(13) 之聚合物薄膜,使聚合物薄膜進行熱處理’以致使供形成 微小晶域用之液晶聚合物定向於液晶配置_,然後再使聚 合物薄膜冷卻,以使定向固定之方法完成。 尤其,偏光散射板之形成可例如’藉由包括將供形成薄 膜用之一或多種聚合物與在低於前述聚合物之玻璃轉移溫 度的溫度下展現出向列’且具有5 0 °C以上之玻璃轉移溫度 之供形成微小晶域用之一或多種液晶聚合物混合’形成具 有液晶聚合物以微小區域之形態分散於其中之聚合物薄 膜,使聚合物薄膜進行熱處理’以致使供形成微小晶域用 之液晶聚合物定向於向列液晶相中’然後再使聚合物薄膜 冷卻,以使定向固定之方法完成。 為製得耐熱性及耐用性優異之偏光散射板,使用具有60 °C以上之玻璃轉移溫度,以70 °C以上更佳,80 t以上特佳 之液晶聚合物較佳。由形成具有顆粒直徑分佈之優異均勻 度之微小晶域的容易度、熱安定性、形成為薄膜的可成形 性、及定向容易度的觀點來看,需要具有8以上之聚合度 的液晶聚合物’以1 0以上較佳,自1 5至5,0 〇 〇為特佳。 由在如此製得之偏光管中之微小晶域之分散分佈的觀點 來看’將供形成薄膜用之聚合物及供形成微小晶域用之液 晶聚合物以可發生相分離之组合使用較佳。微小晶域之分 散分佈可利用由此一组合所達到的相容性作控制。相分離 例如,可利用任何適當方法,諸如包括利用溶劑溶解不相 谷材料之方法’及包括將不相容材料加熱及熔融於摻合物 中之方法而達成。89109116.ptc Page 16 4557 04 ___Case No. 891091H ____ ^^ __ V. The polymer film of (13), heat treatment of the polymer film ', so that the liquid crystal polymer used to form microcrystalline domains is oriented to the liquid crystal Configure _ and then cool the polymer film to complete the orientation fixation method. In particular, the formation of the polarizing light scattering plate can be, for example, 'by including one or more polymers for forming a thin film and exhibiting a nematic at a temperature lower than the glass transition temperature of the aforementioned polymer' and having a temperature of 50 ° C or more One or more liquid crystal polymers for forming microcrystalline domains at the glass transition temperature are mixed to form a polymer film having liquid crystal polymers dispersed in the form of microdomains, and the polymer film is subjected to heat treatment, so as to form microcrystals. The liquid crystal polymer used in the domain is oriented in the nematic liquid crystal phase, and then the polymer film is cooled to complete the method of orientation fixation. In order to obtain a polarizing light scattering plate with excellent heat resistance and durability, a glass transition temperature of 60 ° C or higher is used, preferably 70 ° C or higher, and a liquid crystal polymer of 80t or higher is particularly preferred. A liquid crystal polymer having a degree of polymerization of 8 or more is required from the viewpoints of ease of forming minute crystal domains having excellent uniformity of particle diameter distribution, thermal stability, formability into a thin film, and ease of orientation. 'It is preferably 10 or more, and particularly preferably from 15 to 5,000. From the viewpoint of the dispersion distribution of the minute crystal domains in the polarizer thus prepared, it is preferable to use a combination of a polymer for forming a thin film and a liquid crystal polymer for forming a minute crystal domain in such a manner that phase separation can occur. . The dispersion distribution of minute crystal domains can be controlled by using the compatibility achieved by this combination. Phase separation can be achieved, for example, by any suitable method, such as a method including dissolving non-phase valley materials with a solvent 'and a method including heating and melting incompatible materials in the blend.
89l09116.ptc 第17頁 455704 __案號 89109116__年-1_§-ϋ.__ 五、發明說明(14) 其中分散有微小晶域之前述聚合物薄膜(即待定向之薄 膜)的形成,可例如,利用任何適當方法’諸如流延法、 擠塑法、注塑法、輥壓法及流鑄法而完成。或者’前述聚 合物薄膜之形成可利用包括將聚合物以單體之形態散佈, 然後再使材料進行熱處理或照射紫外光線等等而形成薄膜 之方法完成。 為製得微小晶域之分佈均勾度優異之偏光散射板,使用 包括使成膜材料與溶劑之混合物進行流延或流鑄而形成薄 膜之方法為較佳。在此情況中,微小晶域之尺寸及分佈可 利用溶劑之種類、混合物之黏度、混合物-散佈層之乾燥 速率等等作控制。舉例來說’可經由降低混合物之黏度或 提高混合物-散佈層之乾燥速率,而方便地達成微小晶域 之面積的減小。 然而’實際上,由 米較佳,自5微米 佳。在薄膜之形成 的添加劑,諸如分 色有機顏料、阻燃 之一或多種適當方 單軸、雙軸、連續 移溫度或液晶轉移 ,然後再使材料快速 形成過程中流動定 待定向薄膜之厚度可經適當地決定。 定向性的觀點來看,其為自1微米至3毫 至1毫米更佳’自1〇微米至500微米為特 過程中,材料可包含加入於其中之適當 散劑、表面活性劑、紫外光吸收劑、彩 劑 '離模劑及氧化抑制劑。 定向可利用可藉由定向而控制折射率 法完成’諸如拉伸方法或輥壓方法諸如 雙軸或Z—轴方法’包括在不低於玻璃轉 溫度之溫度下對材料施加電場或磁場, 冷卻而使定向固定之方法,包括在薄犋89l09116.ptc Page 17 455704 __Case No. 89109116__year-1_§-ϋ .__ V. Description of the invention (14) The formation of the aforementioned polymer film (ie, the film to be oriented) in which microcrystalline domains are dispersed, can be For example, it is accomplished using any suitable method such as a casting method, an extrusion method, an injection molding method, a roll pressing method, and a casting method. Alternatively, the formation of the aforementioned polymer film can be completed by a method including dispersing the polymer in the form of a monomer, and then subjecting the material to heat treatment or irradiating ultraviolet light to form a film. In order to obtain a polarized light scattering plate having excellent distribution uniformity of minute crystal domains, it is preferable to use a method including casting or casting a mixture of a film-forming material and a solvent to form a thin film. In this case, the size and distribution of the minute crystal domains can be controlled by the type of the solvent, the viscosity of the mixture, the drying rate of the mixture-dispersion layer, and the like. For example, the reduction of the area of the minute crystal domains can be conveniently achieved by reducing the viscosity of the mixture or increasing the drying rate of the mixture-dispersion layer. However, in fact, it is better to be from 5 m, and better to be from 5 m. Additives in film formation, such as color separation organic pigments, flame retardant one or more suitable square uniaxial, biaxial, continuous temperature shift or liquid crystal transfer, and then the material can be flowed during rapid formation. The thickness of the film to be oriented may be Appropriately decided. From the point of view of orientation, it is more preferably from 1 micrometer to 3 millimeters to 1 millimeter. From 10 micrometers to 500 micrometers, in particular, the material may include a suitable powder, a surfactant, and ultraviolet light absorption added thereto Agents, colorants' release agents and oxidation inhibitors. Orientation can be accomplished using an index-controllable refractive index method such as a stretching method or a rolling method such as a biaxial or Z-axis method, including applying an electric or magnetic field to a material at a temperature not lower than the glass transition temperature, and cooling The method of fixing the orientation includes
455704 - --—案號 8910911 fi__年月 a 修正______ 五、發明說明(15) 向之方法,及包括根據等向性聚合物之輕微定向使液晶自 行定向之方法。因此,如此製得之偏光散射板可為拉伸薄 膜或未拉伸薄膜e在製造拉伸薄膜之情況中,亦可使用脆 性聚合物。然而,特別需要伸長性優異的聚合物。 在由前述液晶聚合物製成微小晶域的情況中,可使用包 括將材料加熱至使待以微小晶域之形態分散及分佈於聚合 物4膜中之液晶聚合物顯現期望的液晶相,諸如向列相, 以致其經熔融之溫度,使材料在定向調節力之作用下進行 定向’然後再使材料快速冷卻,以使定向固定之方法。微 小晶域之定向以在儘可能單晶域的狀態中較佳,以抑制光 學性質的分散》 關於定向調節力’可使用可使液晶聚合物定向之適當的 調節力’諸如使用於包括在適當牽引比下拉伸聚合物薄膜 之方法中的拉伸力,在薄膜形成過程中所使用之剪切力, 及電場或磁場。可有一或多個此等調節力作用於聚合物薄 膜上’而將液晶聚合物定向。 因此,在偏光散射板中除微小晶域外之部分,即透明薄 膜之基材(聚合物薄膜部分),可展現雙折射,或可為等向 性。完全展現雙折射的偏光散射板可經由使定向雙折射成 膜聚合物在前述的成膜程序中進行分子定向而製得。若須 要,可使聚合物進行已知的定向,諸如拉伸,以使其成為 雙折射或控制其雙折射。 ^ 在除微小晶域外之區域中為等向性之偏光散射板可經由 使等向性成膜聚合物在不高於聚合物之玻璃轉移溫度的溫455704---- Case number 8910911 fi__year a. Amendment ______ V. Description of the invention (15) The method of orientation, and the method including the orientation of the liquid crystal by the slight orientation of the isotropic polymer. Therefore, the polarizing light scattering plate thus obtained may be a stretched film or an unstretched film. In the case of manufacturing a stretched film, a brittle polymer may also be used. However, a polymer having excellent elongation is particularly required. In the case of making microcrystalline domains from the aforementioned liquid crystal polymer, a liquid crystal polymer including heating the material to disperse and distribute in the form of the microcrystalline domains in the polymer 4 film can be used to develop a desired liquid crystal phase, such as Nematic phase, so that the temperature of its melting, so that the material is oriented under the effect of the orientation adjustment force, and then quickly cooled the material to fix the orientation method. The orientation of the microcrystalline domains is better in the state of the single crystal domains as much as possible to suppress the dispersion of optical properties. "Regarding the orientation adjustment force, 'the appropriate adjustment force which can orient the liquid crystal polymer can be used', such as used in The tensile force in the method of stretching a polymer film under a traction ratio, the shear force used during film formation, and an electric or magnetic field. One or more of these regulatory forces can act on the polymer film ' to orient the liquid crystal polymer. Therefore, the part of the polarized light scattering plate other than the microcrystalline domain, that is, the base material (polymer film part) of the transparent film, may exhibit birefringence or may be isotropic. A polarizing light scattering plate that fully exhibits birefringence can be produced by subjecting an oriented birefringent film-forming polymer to molecular orientation in the aforementioned film-forming procedure. If necessary, the polymer can be subjected to a known orientation, such as stretching, to make it birefringent or to control its birefringence. ^ An isotropic polarized light scattering plate in areas other than microcrystalline domains can be made by isotropic film-forming polymer at a temperature not higher than the glass transition temperature of the polymer.
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度下拉伸而製得。 控制偏光散射板之一較佳具體例,以致在微小晶域與作 為聚合物薄膜部分之其他部分之間的微小晶域之各個光軸 折射率差(即Δηΐ、Δη2及Δη3)中之軸向(Δη1方向)為最 大,Δηΐ為〇.〇3以上,及在垂直於Αη1方向之另兩軸向 (Δη2及Δη3方向)中,Δη2及Δη3各為Δηΐ之50%以下。 △ η 2及△ η 3以彼此相等較佳。 經由使用前述的折射率,△ η丨方向中之線性偏光在小於 全反射角之角度下強烈地散射,而使其可提高自光管發射 之光的量。其他方向中之線性偏光幾乎不會散射,因此其 重複地全反射,而可將其限制於光管中。 在先前的說明中,如成臈聚合物為光學等向性,則在各 個軸向中之微小晶域之折射率與除微小晶域外之部分之折 射率之間的差係指在各個方向中之微小晶域之折射率與聚 合物薄膜之平均折射率之間的差。如成膜聚合物為光學各 向異性,則其係指在主光學軸向中之聚合物薄膜之折射 與主光學軸向中之微小晶域之折射率之間的差,因兩 學方向通常相同。 由前述全反射的觀點來看,Δη1方向中之折射率差 適度地大較佳,自Ο.〇π至1更佳,自0.045至0.5為特佳。 在Δη2及Δη3方向中之折射率差Δη2及_各分別 卢 地小較佳。此等折射率差可經由調整使用材料 ^ = 進行前述定向而控制。 ~ f β 由於前述的△ η 1方向係對應於由光管所發射之線性偏光It is obtained by stretching under the temperature. One of the preferred specific examples of controlling the polarized light scattering plate, so that the axial directions in the refractive index differences (ie, Δηΐ, Δη2, and Δη3) of the respective optical axes of the minute crystal domains between the minute crystal domains and other parts that are part of the polymer film (Δη1 direction) is the largest, Δηΐ is greater than 0.03, and in the other two axes (directions of Δη2 and Δη3) perpendicular to the direction of Δη1, Δη2 and Δη3 are each 50% or less of Δηΐ. It is preferable that Δ η 2 and Δ η 3 are equal to each other. By using the aforementioned refractive index, linearly polarized light in the Δη 丨 direction is strongly scattered at an angle smaller than the total reflection angle, so that it can increase the amount of light emitted from the light pipe. Linearly polarized light in other directions hardly scatters, so it repeats total reflection, but it can be confined to the light pipe. In the previous description, if the fluorene-forming polymer is optically isotropic, the difference between the refractive index of the microcrystalline domain in each axis and the refractive index of the part other than the microcrystalline domain refers to the direction in each direction The difference between the refractive index of a small crystal domain and the average refractive index of a polymer film. If the film-forming polymer is optically anisotropic, it refers to the difference between the refractive index of the polymer film in the main optical axis and the refractive index of the small crystal domain in the main optical axis. the same. From the viewpoint of the aforementioned total reflection, the refractive index difference in the Δη1 direction is moderately large and preferably, more preferably from 0.0π to 1 and particularly preferably from 0.045 to 0.5. The refractive index differences Δη2 and _ in the directions of Δη2 and Δη3 are each preferably small. These refractive index differences can be controlled by adjusting the aforementioned orientation using the material ^ =. ~ f β Since the aforementioned △ η 1 direction corresponds to the linearly polarized light emitted by the light pipe
89109116.ptc 第20頁 -lS_89l〇9]j^ 455704 年 月 修正 曰 五、發明說明(17) 的振蘆平面,因而廿 期望的液晶單元以ΐ行於偏光散射板之表面較佳。視 办〇 哥專而定’平面内的Δηΐ方向可能為適 由散射作用之扭' ^ >1从八也《 \ 呜句度的觀點來看’微小晶域以儘可能均 勻地分散及分佑认& , .3. , , _ ^ 於偏光散射板中較佳。微小晶域’尤其係 為散射方向之△nt + L , ,.e ^ ^ n 1方向的尺寸係與回散射(反射)相關或視 波長而定。 由增進光的百分利用率’防止由於視波長而定之著色, 防止阻礙微小晶域之景多像被看見,防止阻礙清晰的顯示, 成膜性質及薄膜強度的觀點來看,微小晶域之較佳尺寸, 尤其係Δη1方向之較佳長度,係自0. 05至500微米,自0. 1 至250微米更佳,自1至100微米為特佳。雖然微小晶域通 常係以晶域的形態存在於偏光散射板中,但其Δη2方向之 長度並無特殊之限制。 在偏光散射板中之微小晶域的比例可由A η丨方向中之散 射性質而適當地決定。然而,實際上,亦將薄膜強度列入 考慮’其係自0.1至70重量百分比較佳,自〇5至50重量百 分比更佳’自1至30重量百分比為特佳。 偏光散射板可以由顯現雙折射之前述薄膜製成之單層的 形態形成。可將二或多個此一薄膜層合,而形成偏光散射 板。將此等薄膜層合可產生較由增加厚度所產生者大的增 強散射作用。可進行層合’以使薄膜以任意角度設置,諸 如Δηΐ或Δη〗方向。由增進散射作用的觀點來看,進行層 合,以使兩垂直相鄰層之△ η 1方向彼此平行較佳。薄膜的 I麵89109116.ptc Page 20 -lS_89l〇9] j ^ 455704 Rev. Y. 5. Description of the invention (17) The reed plane, so it is better that the liquid crystal cell is expected to run on the surface of the polarized light scattering plate. Depending on the subject, 'the direction of Δηΐ in the plane may be a twist suitable for scattering' ^ > 1 From the point of view of Yaya "\ Woo degree, 'the microcrystalline domains are dispersed and divided as uniformly as possible. It is better to use &, .3.,, _ ^ In the polarized light scattering plate. The microcrystalline domain 'is especially Δnt + L, .e ^ ^ n in the scattering direction. The size is related to backscattering (reflection) or depends on the wavelength. By increasing the percentage utilization of light, it prevents coloring due to the wavelength, prevents multiple images that hinder the microcrystalline domains from being seen, prevents clear display, film-forming properties, and film strength. The preferred size, especially the preferred length in the Δη1 direction, is from 0.05 to 500 microns, more preferably from 0.1 to 250 microns, and particularly preferably from 1 to 100 microns. Although the microcrystalline domains usually exist in the polarized light scattering plate in the form of crystal domains, the length in the Δη2 direction is not particularly limited. The proportion of the minute crystal domains in the polarized light scattering plate can be appropriately determined by the scattering properties in the A η 丨 direction. However, in fact, the strength of the film is also taken into consideration, which is more preferably from 0.1 to 70% by weight, more preferably from 0.05 to 50% by weight, and particularly preferably from 1 to 30% by weight. The polarizing light scattering plate may be formed in the form of a single layer made of the aforementioned thin film exhibiting birefringence. Two or more of these films may be laminated to form a polarized light scattering plate. Laminating these films can produce a stronger scattering effect than that produced by increasing the thickness. Lamination can be performed so that the film is set at any angle, such as in the direction of Δηΐ or Δη. From the viewpoint of enhancing the scattering effect, it is preferable to carry out lamination so that the Δη1 directions of two vertically adjacent layers are parallel to each other. I side of film
89109116.ptc 第21頁 45 57 0 4 -__案號 89109116_年月日 修正 _ 五、發明說明(18) 層合數為2以上的任意數目。 待層合的薄膜可具有相同或不同的△^或^心方向。垂 直相鄰層之△ η 1方向等等係儘可能地彼此平行。然而,可 容許由於工作誤差所致的偏差。當方向等等分散時, 可將Δηΐ方向的值平均 利用黏著劑層以使全反射表面為最外部表面的配置,使 待層合的薄膜彼此黏合。可使用任何適當的黏著劑諸如熱 熔膠及黏性黏著劑作為黏著劑。為抑制反射損耗,使用與 前述薄膜具有儘可能小之折射率差的黏著劑層為較佳。可 將此等薄膜黏合至其本身’或使用供形成微小晶域用之聚 合物。 偏光管以整體或部分具有相差較佳,由於當光被光管之 内部透射時可適當地消除極化,因而由光之百分利用率的 觀點來看有利。由於散射偏光管的滯後軸與線性偏光之極 化轴(振盪平面)基本上係互相垂直,因而據認為由於相差 所致的極化轉變幾乎不會發生,但輕微的散射會造成產生 極化轉變之視角(apparent angle)的變化。 由前述極化轉變的觀點來看,發生5毫微米以上的平面 内相差通常為較佳,儘管其係視散射偏光管之厚度而定。 可利用適當的方法賦予相差,諸如包括使雙折射顆粒加入 至散射偏光管中之方法,包括使雙折射顆粒附著至散射偏 光管之表面的方法,包括使聚合物薄膜成為雙折射之方法 及其組合。 根據本發明之偏光管包括光透射樹脂板與偏光散射板之89109116.ptc Page 21 45 57 0 4 -__ Case No. 89109116_Year Month Day Amendment _ V. Description of the invention (18) The number of layers is any number above 2. The films to be laminated may have the same or different Δ ^ or ^ directions. The Δη1 direction of the vertically adjacent layers and the like are as parallel as possible to each other. However, deviations due to operating errors can be tolerated. When the directions and the like are dispersed, the values in the Δηΐ direction can be averaged to make the total reflection surface be the outermost surface using the adhesive layer, and the films to be laminated are adhered to each other. Any appropriate adhesive such as hot melt adhesive and adhesive can be used as the adhesive. In order to suppress reflection loss, it is preferable to use an adhesive layer having a refractive index difference as small as possible from the film. These films can be adhered to itself 'or a polymer for forming minute crystal domains can be used. It is better for the polarizer to have a phase difference in whole or in part. Since the polarization can be properly eliminated when light is transmitted through the interior of the light pipe, it is advantageous from the viewpoint of the percentage utilization of light. Since the retardation axis of the polarizing tube and the polarization axis (oscillating plane) of linearly polarized light are basically perpendicular to each other, it is thought that the polarization transition due to the phase difference hardly occurs, but a slight scattering will cause a polarization transition. Change in apparent angle. From the viewpoint of the aforementioned polarization transition, an in-plane phase difference of 5 nm or more is generally preferred, although it depends on the thickness of the scattering polarizer. The phase difference can be imparted by an appropriate method, such as a method including adding birefringent particles to the scattering polarizer, a method including attaching the birefringent particles to the surface of the scattering polarizer, a method including making a polymer film birefringent, and combination. A polarizing tube according to the present invention includes a light transmitting resin plate and a polarizing light scattering plate.
89109116.ptc 第22頁 455704 _案號89109116_年月 日 你 五、發明說明(19) 層合物。為形成本發明之偏光管,使光透射樹脂板丨與偏 光散射板3利用具有與兩層儘可能接近之折射率之黏著劑 或其類似物而彼此黏合較佳,以儘可能地抑制被光透射樹 脂板1與偏光散射板3之界面的反射,即促進光在光透射樹 脂板與偏光散射板之間的透射,因此而利用由如圖丨所示 之兩層之緊密層合物製成之光管的兩表面達到全反射。黏 合由防止轴之偏差的觀點來看有效。為形成偏光管,可如 圖2所示將偏光散射板3設於光透射樹脂板1之兩表面上。 為形成光透射樹脂板與偏光散射板之層合物,將光透射 樹脂板與偏光散射板設置成使光透射樹脂板之平均滞後袖 與光學軸(發射偏光之振盪平面)以5度以上之角度相交較 佳’自10至80度更佳,自15至75度為特佳,以有效地消除 透射光之極化。 '” 關於前述的黏合’如同前述層合物型偏光散射板之情 況,可使用適當的黏著劑’諸如透明黏著劑(例如,丙稀 酸系黏著劑、聚矽氧黏著劑、聚酯基黏著劑、聚胺基甲酸 酯基黏著劑、聚醚基黏著劑、橡膠黏著劑)。因此,對於 黏合並無特殊之限制。由防止光學特性改變的觀點來看;, 不需高溫長時間的固化及乾燥程序之黏著劑為較佳。此 外’在加熱或潤濕條件下不易浮動或剝離的黏著劑為 佳。 ^ 由前述的觀點來看,使用包含經由使具有2〇個以下 Γ ^π; 原子之烷基諸如甲基、乙基及丁基之(甲基)丙烯酸燒基醋 與包含改質成份諸如(曱基)丙烯酸及(甲基)丙烯酸經^ ^89109116.ptc Page 22 455704 _Case No. 89109116_Year Month Day You 5. Description of the invention (19) Laminate. In order to form the polarizing tube of the present invention, it is preferable that the light-transmitting resin plate 丨 and the polarizing light-scattering plate 3 are adhered to each other by using an adhesive or the like having a refractive index as close as possible to the two layers, so as to suppress as much as possible The reflection at the interface between the transmissive resin plate 1 and the polarized light scattering plate 3, that is, to promote the transmission of light between the light transmissive resin plate and the polarized light scattering plate. Therefore, it is made of a two-layer compact laminate as shown in Figure 丨. Both surfaces of the light pipe achieve total reflection. Adhesion is effective from the viewpoint of preventing shaft deviation. To form a polarizing tube, a polarizing light scattering plate 3 may be provided on both surfaces of the light transmitting resin plate 1 as shown in FIG. 2. In order to form a laminate of a light-transmitting resin plate and a polarizing light-scattering plate, the light-transmitting resin plate and the polarizing light-scattering plate are set so that the average hysteresis sleeve of the light-transmitting resin plate and the optical axis (oscillation plane that emits polarized light) are at least 5 degrees. The angles intersect better. From 10 to 80 degrees is more preferred, and from 15 to 75 degrees is particularly preferred to effectively eliminate the polarization of transmitted light. "" About the aforementioned adhesion "As in the case of the aforementioned laminated polarizing light scattering plate, an appropriate adhesive such as a transparent adhesive (for example, acrylic adhesive, polysiloxane adhesive, polyester-based adhesive can be used) Agent, polyurethane-based adhesive, polyether-based adhesive, rubber adhesive). Therefore, there is no special restriction on adhesion. From the viewpoint of preventing the change of optical characteristics; Adhesives for curing and drying procedures are preferred. In addition, 'adhesives that do not easily float or peel off under heating or wetting conditions are preferred. ^ From the foregoing point of view, the use of Atomic alkyl groups such as methyl, ethyl and butyl (meth) acrylic acid alkyl vinegar and containing modified ingredients such as (fluorenyl) acrylic acid and (meth) acrylic acid ^ ^
五 '發明說明(20) 之丙烯酸系單體以使所得玻璃轉移溫度為0 °C以下之組合 共聚合而製得之具有重量平均分子量為100, 〇〇〇以上之丙 烯酸系聚合物為基礎聚合物之丙烯酸系黏著劑較佳。此一 丙烯酸系黏著劑亦有透明度、耐天候老化性及耐熱性優異 的優點。 將黏著劑層提供於光透射樹脂板及/或偏光散射板上可 ,用任何適當方法完成。此一方法之例子包括:包括將黏 著劑成份單獨或以摻合物溶解或分散於適當溶劑諸如甲苯 及乙酸乙S旨中,而製備得具有自約1〇至4〇重量百分比之濃 度的黏著劑落液’然後再利用任何適當的散佈方法諸如流 延方法及塗布方法將黏著劑溶液直接提供於光透射樹脂板 或偏光散射板上之方法’及包括以與如前所述之相同方式 將黏著劑層形成於隔離物上’然後再將黏著劑層轉移至光 透射樹脂板或偏光散射板上之方法。所提供的黏著劑層可 為具有不同組合物或種類之層合層。 黏者劑層之厚度可由黏性專等而適當地決定。其—般係 自1至5 0 0微米。黏著劑層可包括填料諸如天然或合成樹 脂、玻璃纖維、玻璃珠、金屬粉末及其他無機粉末,或視 需要而加入於其中之適當的添加劑諸如顏料、著色劑及氧 化抑制劑。此外,黏著劑層可包括加入於其中之微細分割 的顆粒,以展現光擴散性質。 根據本發明之偏光管係用於將於其側面接收到之入射光 轉變為線性偏光’其接著再如前所述地自其之雨表面發 射,因此’其可較佳地用於形成平面偏光源。平面偏光源Fifth invention description (20) The acrylic monomer is polymerized based on a combination copolymerization of the obtained glass transition temperature of 0 ° C or lower, and an acrylic polymer having a weight average molecular weight of 100, 000 or more as a base polymerization. Acrylic adhesives are preferred. This acrylic adhesive also has the advantages of excellent transparency, weather resistance, and heat resistance. The provision of the adhesive layer on the light transmitting resin plate and / or the polarizing light scattering plate may be performed by any appropriate method. Examples of such a method include preparing adhesives having a concentration from about 10 to 40 weight percent by dissolving or dispersing the adhesive ingredients alone or in a blend in an appropriate solvent such as toluene and ethyl acetate. The agent dropping liquid 'then a method of directly supplying the adhesive solution on a light-transmitting resin plate or a polarizing light-scattering plate by any suitable spreading method such as a casting method and a coating method' and includes applying A method of forming an adhesive layer on a spacer, and then transferring the adhesive layer to a light transmitting resin plate or a polarizing light scattering plate. The provided adhesive layer may be a laminated layer having different compositions or kinds. The thickness of the adhesive layer can be appropriately determined by the adhesive property. Its-generally from 1 to 500 microns. The adhesive layer may include fillers such as natural or synthetic resins, glass fibers, glass beads, metal powders, and other inorganic powders, or appropriate additives such as pigments, colorants, and oxidation inhibitors added thereto as necessary. In addition, the adhesive layer may include finely divided particles added thereto to exhibit light diffusion properties. A polarizing tube according to the present invention is used to convert incident light received on its side into linear polarized light, which is then emitted from its rain surface as described above, and therefore, it can be preferably used to form planar polarized light. source. Plane polarized light source
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第24頁 89l〇9lI6.ptc ^ 4557 0 4Page 24 89l〇9lI6.ptc ^ 4557 0 4
之至少一側面上 可經由如圖3所示將光源5設置於偏光管4 而形成。 光源,如 上較佳。 層回轉, 態,而使 置於偏光 極射線管 ’由光發 冷陰極射 兩相對侧 用三個侧 在此配置中,自 並集中於偏光管 其可增進亮度。 管之侧面上之任 、發光二極體之 射效率、降低電 線管為較佳。可 面或三個側面 面的情況中,可 為製得具有優異亮度之平面偏 面反射層6設於偏光管4之一表面 反射層側發射的光可被單向反射 之一表面上,並不改變其極化狀 關於前述的光源,可使用可設 何適當的光源,諸如(冷、熱)陰 線性或平面陣列及白熾燈。尤其 源消耗及降低直徑的觀點來看, 將光源設置於多個側面上,諸如 上,以增進亮度或均勾度。在使 使用U形管。 為形成平面偏光源,若須要,可設置適當的輔助構件諸 如包圍光源5的反射器51,以自光源將散射光引入至偏光 管之側面,如圖3所示。關於此一反射器,一般可使用設 有具高反射比之金屬薄層的樹脂片材或金屬箔。反射器可 延伸至偏光管之下表面,以同樣地作為反射層用。反射器 亦有用作為光源固定構件。 另一方面’由極化維持的觀點來看,前述的單面反射層 6以儘可能地單面反射較佳。由此觀點來看,由金屬製成 的反射表面為特佳。關於此一金屬’可使用任何適當的金 屬諸如銘、銀、鉻、金、銅、錫、鋅、麵、虹、翻及其合 金。At least one side surface can be formed by disposing the light source 5 on the polarizer 4 as shown in FIG. 3. The light source is better as above. The layer is rotated, and placed in a polarized polar tube, which is radiated by a light, a cold cathode, two opposite sides, and three sides. In this configuration, it is concentrated on the polarized tube, which can increase the brightness. Anything on the side of the tube, the radiation efficiency of the light-emitting diode, and the reduction of the tube are better. In the case of two or three side surfaces, a planar polarized reflective layer 6 having excellent brightness can be provided on one surface of the polarizer 4 and the light emitted from the reflective layer side can be unidirectionally reflected on one of the surfaces. Changing its polarization state Regarding the aforementioned light source, any suitable light source can be used, such as (cold, hot) female linear or planar arrays and incandescent lamps. In particular, from the viewpoints of source consumption and reduction in diameter, the light source is arranged on a plurality of sides, such as above, to improve brightness or uniformity. U-shaped tubes are used. To form a planar polarized light source, if necessary, appropriate auxiliary members such as a reflector 51 surrounding the light source 5 can be provided to introduce scattered light from the light source to the side of the polarizer, as shown in FIG. 3. As for this reflector, a resin sheet or a metal foil provided with a thin metal layer having a high reflectance can be generally used. The reflector can be extended to the lower surface of the polarizer to serve as a reflective layer. The reflector is also useful as a light source fixing member. On the other hand, from the viewpoint of polarization maintenance, it is preferable that the aforementioned single-sided reflective layer 6 reflects as much as possible on one side. From this point of view, a reflective surface made of metal is particularly preferred. As this metal ', any appropriate metal such as inscription, silver, chromium, gold, copper, tin, zinc, surface, rainbow, phantom, and alloy thereof can be used.
89109116.ptc 第25頁 45 57 0 4 __案號 891Q911R_年月日_修正 五、發明說明(22) - 反射層6可經由將此一金屬於偏光管上真空蒸發至一小 的厚度’以使其與偏光管保持直接接觸而形成。然而, 空沈積金屬幾乎不會造成全反射。此反射層會造成一些 的吸收。因此,將由全反射造成的重複列入考慮,可&察 吸收損耗。為抑制吸收損耗,配置係使反射器僅疊置於偏 光管上’以致在其間插置空氣層較佳。因此,由此觀點 看,反射器係經由將金屬於支承基材上濺鍍或真空蒸發至 一小的厚度而形成較佳。或者,使用扁平金屬材料^如 屬箔及金屬之輥製片材較佳。關於反射器之支承基材,° 使用適當的材料諸如玻璃板及樹脂片材。尤其,由反射β 比、色澤及可處理性的觀點來看,使用有銀或鋁真空沈 於其上之樹脂片材較佳。可將反射層設置於偏光管$任— 表面。 為形成平面偏光源,可將一或多個適當的光學層,諸如 圖3所示之擴散層7,設置於適當位置。使用於此的光學 並無特殊之限制《舉例來說,可使用適當的材料,諸如用 於形成液晶顯示裝置之光學層。圖5係沒有光擴散層7之 面偏光源的一具體例。 '' 在為層合物之偏光管4之另一表面(即未設有前述單面反 2層之偏光管之表面)上所設置之極化維持光擴散層7係 來使由層合物所發射之光(線性偏光)擴散,同時儘可能地 維持其極化,因此使發射均勻,而使其可增進其之可 度0 此外,亦可視需要設置光擴散層,以經由透過稍後說明89109116.ptc Page 25 45 57 0 4 __Case No. 891Q911R_Year Month Day_Revision V. Description of the invention (22)-The reflective layer 6 can be evaporated to a small thickness by vacuum evaporation of this metal on a polarizer ' It is formed by keeping it in direct contact with the polarizer. However, empty-deposited metals hardly cause total reflection. This reflective layer will cause some absorption. Therefore, taking into account the duplication caused by total reflection, the absorption loss can be observed. In order to suppress absorption loss, the arrangement is such that the reflector is stacked only on the polarizer 'so that an air layer is preferably interposed therebetween. Therefore, from this point of view, the reflector is preferably formed by sputtering or vacuum evaporation of metal to a small thickness on the supporting substrate. Alternatively, flat metal materials such as foils and metal roll sheets are preferred. Regarding the supporting substrate of the reflector, ° Use an appropriate material such as a glass plate and a resin sheet. In particular, from the viewpoint of the reflection β ratio, color, and handleability, it is preferable to use a resin sheet having silver or aluminum vacuum-deposited thereon. The reflective layer can be disposed on the surface of the polarizer. To form a planar polarized light source, one or more appropriate optical layers, such as the diffusion layer 7 shown in Fig. 3, may be provided at appropriate positions. There is no particular limitation on the optics used herein. For example, an appropriate material such as an optical layer for forming a liquid crystal display device may be used. Fig. 5 is a specific example of a surface-biased light source without the light diffusion layer 7. '' The polarization-maintaining light diffusion layer 7 is provided on the other surface of the polarizer 4 that is a laminate (that is, the surface of the polarizer that is not provided with the aforementioned single-sided reverse 2 layer) to make the laminate The emitted light (linearly polarized light) is diffused while maintaining its polarization as much as possible, so that the emission is uniform, so that it can improve its degree of 0. In addition, a light diffusing layer can be provided as needed to explain later
>1 R R7 0 89109116 五、發明說明(23)> 1 R R7 0 89109116 V. Description of the invention (23)
B 修正 之透鏡片上之凹凸形態放籍視力,而增進可見度。 在本發明’為有效率地利用由偏光管所發射之線性偏 光’如將光學層’尤其係極化板’設於偏光管之發射面, 則待設置於極化板與偏光管之間的光學層係可展現優異的 透光率’及儘可能地維持發射光之線性極化(極化度),而 不將其消除之光學層較佳。尤其,光學層以展現8 〇 %以上 之總透光率’ 85%以上更佳’ 90%以上為特佳,及展現5%以 下之洩漏百分比(透射比),2%以下更佳,1 %以下為特佳, 如經由透過設置正交尼科耳稜晶(cr〇ss_Nic〇i)之配置消 除極化所發展。 由於消除極化通常係利用雙折射或多重散射進行,因而 顯現極化維持性質的光學層可經由儘可能地降低雙折射或 降低光線軌道中之平均反射(散射)之數目而產生。由此觀 點來看’光學層以由具有低雙折射之樹脂(具有良好光學 等向性之樹脂),諸如三醋酸纖維素基樹脂、聚甲基丙烯 酸甲酯、聚碳酸酯及去甲莅烯基樹脂形成較佳。可使用— 或多種此等樹脂。 極化維持性質優異的光擴散層可藉由適當的方法而在其 表面上叹有微細粗化結構,該方法諸如包括使透明顆粒分 散於由具有小雙折射之樹脂製成之層令之方法,及包括將 樹脂層之表面粗加工之方法。可使用於此之透明顆粒的例 子〇括了為導電性之材料之微細分割的顆粒,諸如氧化 矽、玻璃、二氧化鈦、氧化锆、氧化錫、氧化銦、氧化鎘 及氧化銻,及由交聯或未交聯聚合物製成之微細分割的顆B The convex and concave shape on the lens is corrected to improve the visibility. In the present invention 'for the efficient use of the linearly polarized light emitted by the polarizer', if the optical layer 'especially a polarizing plate' is provided on the emitting surface of the polarizing tube, it is to be disposed between the polarizing plate and the polarizing tube. An optical layer is an optical layer that can exhibit excellent light transmittance and maintain linear polarization (polarization) of emitted light as much as possible without eliminating it. In particular, the optical layer exhibits a total light transmittance of 80% or more, and more preferably of 85% or more. 90% or more is particularly preferred, and exhibits a leakage percentage (transmittance) of less than 5%, more preferably less than 2%, and 1%. The following is particularly good, as developed by eliminating polarization through the arrangement of crossed Nicol prisms (crOss_Nicoi). Since polarization elimination is usually performed using birefringence or multiple scattering, an optical layer that exhibits polarization-maintaining properties can be produced by minimizing birefringence or reducing the number of average reflections (scattering) in a light track. From this point of view, the optical layer consists of resins with low birefringence (resins with good optical isotropy), such as cellulose triacetate-based resins, polymethyl methacrylate, polycarbonate, and norrene. The base resin is preferably formed. May use-or more of these resins. A light-diffusing layer having excellent polarization maintaining properties can be fine-grained on its surface by an appropriate method such as a method including dispersing transparent particles in a layer made of a resin having small birefringence. , And a method including roughing the surface of the resin layer. Examples of transparent particles that can be used for this include finely divided particles that are conductive materials such as silicon oxide, glass, titanium dioxide, zirconia, tin oxide, indium oxide, cadmium oxide, and antimony oxide, and are crosslinked by Finely divided particles made of or uncrosslinked polymer
第27頁 4557 04 ___案號 89109116__1年 月 日_修正-_ 五、發明說明(24) ~ 粒,該聚合物諸如丙烯酸系聚合物、聚丙烯腈、聚酯、環 氧樹脂、三聚氰胺基樹脂、胺基甲酸酯基樹脂、聚碳醆 酯、聚苯乙烯、聚矽氧基樹脂、苯胍胺、三聚氰胺-苯胍 胺縮合物及苯胍胺-曱醛縮合物。可使用一或多種此等化 合物。 由光之擴散性及擴散均句度的觀點來看,透明顆粒之直 徑係自1至20微米較佳。顆粒可為任意形狀,然而,實際 上’可使用球形顆粒或其二次凝聚體。尤其,由極化維持 性質的觀點來看’使用對樹脂具有自〇. 9至丨.1之折射率' 的透明顆粒較佳。 羊比 其中加入透明顆粒之光擴散層的形成可利用任何適當的 習知方法完成’諸如包括將熔融樹脂溶液與透明顆粒混 合’然後再將混合物擠塑形成月材等等之方法,包括將透 明顆粒加入至樹脂溶液或單體中,將混合物鑄塑成片材, 然後再視需要使片材進行聚合之方法,及包括將其中加 透明顆粒之樹脂溶液塗布至預定表面或極化維持 ^ 之方法。 又艰溥膜 另一方面,在其表面上具有微細粗化結構之光擴散 形成可利用任何適當方法完成,諸如包括經由使用、聱 等擦光或壓花’而將由光學等向性光透射樹脂製成之片' 表面粗加工之方法,及包括形成在前述片材之表面 材 突起物之光透射材料層之方法。然而,並不希望包;有 在氣泡諸如空氣或二氡化鈦顆粒與光透射樹脂之間罝=成 的折射率差之糙度(突起物)之方法,由於其會二二有大 s分匆地消Page 27 4557 04 ___Case No. 89109116__1Year Month _ Amendment-_ V. Description of the invention (24) ~ pellets, the polymer such as acrylic polymer, polyacrylonitrile, polyester, epoxy resin, melamine resin , Urethane-based resin, polycarbamate, polystyrene, polysiloxy resin, benzoguanamine, melamine-benzoguanamine condensate, and benzoguanamine-fluorenal condensate. One or more of these compounds can be used. From the viewpoint of light diffusivity and average diffusivity, the diameter of the transparent particles is preferably from 1 to 20 m. The particles may have any shape, however, in practice, spherical particles or secondary aggregates thereof may be used. In particular, from the viewpoint of the polarization maintaining property, it is preferable to use 'transparent particles having a refractive index of 0.9 to 1 with respect to resin'. The formation of a light diffusing layer with transparent particles added to the sheep can be accomplished by any suitable conventional method, such as including mixing a molten resin solution with transparent particles, and then extruding the mixture to form a moon material. A method for adding particles to a resin solution or a monomer, casting the mixture into a sheet, and then polymerizing the sheet as needed, and a method including coating a resin solution with transparent particles added to a predetermined surface or maintaining polarization ^ method. On the other hand, the film, on the other hand, can be formed by light diffusion with a fine roughened structure on its surface by any suitable method, such as through the use of rubbing, embossing, or embossing. A method of roughening the surface of the manufactured sheet, and a method including forming a light-transmitting material layer of a protrusion on the surface of the aforementioned sheet. However, it is not desirable to wrap; there is a method of roughness (protrusions) of refractive index difference formed between air bubbles such as air or titanium dihalide particles and light transmitting resin, since it will have a large s score. Hastily
4 5 57 0 4 Λ_η 曰 修正 案號 89109116 五、發明說明(25) 除極化。 提到在光擴散層之表面上的微細粗化結構,由光之擴散 性或擴散均勻度的觀點來看,光擴散層之表面糙度以自不 低於入射光之波長至不多於丨〇〇微米,且為非週期1生較 佳。為形成前述加入透明顆粒之類型或粗化表面類型之光 擴散層’由極化維持性質等等的觀點來看,儘可能防止由 光透射樹脂製成之底層受到由於光學彈性或定向所造成之 相差的上升較佳。 可在層合物之發射面上設立一或多個此等光擴散層。若 有二或多個光擴散層可相同或不同。然而,此等光擴散層 以整體具有前述的極化維持性質較佳。如於前述單面反射 層之情沉’將光擴散層設置成具有相對於層合物而形成之 間隙較佳》由全反射的觀點來看,此間隙以充分地較入射 光之波長大較佳c 在圖4之具體例中設於層合物4之另一表面上,亦即沒有 單面反射層之層合物之表面上之極化維持透鏡片8係要控 制來自層合物之散射發射光(線性偏光)之光路徑,同時儘 可能地維持其極化度,因而改良對前方的方向性,而有利 於影像’及因此而使散射發射光之強度波峰出現於前方方 向。 關於透鏡片’可使用可控制於其之一表面接收到之入射 光之光路徑,並將其自另一表面在儘可能垂直於片材表面 之方向(别向)中有效率地發射之任何適當的材料。因此, 透鏡片並無特殊之限制。因此,可使用在習知之側光型光4 5 57 0 4 Λ_η Amendment No. 89109116 V. Description of the invention (25) Depolarization. When referring to the micro-roughened structure on the surface of the light diffusion layer, from the viewpoint of light diffusivity or uniformity of diffusion, the surface roughness of the light diffusion layer ranges from not less than the wavelength of incident light to not more than 丨0 micron, and is preferably non-periodic. In order to form the light-diffusing layer of the type in which the transparent particles are added or the type of the roughened surface, from the viewpoint of polarization maintaining properties, etc., the bottom layer made of the light-transmitting resin is prevented from being caused by optical elasticity or orientation as much as possible. The increase in phase difference is better. One or more of these light diffusion layers may be provided on the emitting surface of the laminate. If there are two or more light diffusion layers, they may be the same or different. However, it is preferable that these light diffusion layers have the aforementioned polarization maintaining properties as a whole. For example, in the case of the aforementioned single-sided reflective layer, it is better to set the light diffusion layer to have a gap with respect to the laminate. From the viewpoint of total reflection, this gap is sufficiently larger than the wavelength of incident light.佳 c The polarization maintaining lens sheet 8 provided on the other surface of the laminate 4 in the specific example of FIG. 4, that is, on the surface of the laminate without a single-sided reflection layer, is to control the The light path of the scattered emitted light (linearly polarized light), while maintaining its polarization as much as possible, thus improving the directivity to the front, which is conducive to the image 'and therefore the intensity peak of the scattered emitted light appears in the forward direction. Regarding the lens sheet, any light path that can control the incident light received on one surface and emit it efficiently from the other surface in a direction (aspect) perpendicular to the surface of the sheet as efficiently as possible Appropriate materials. Therefore, the lens sheet is not particularly limited. Therefore, the conventional side-light type light can be used.
89109116,ptc 第29頁 45 57 Ο δ Λ_η 曰 -修正 __案號 89109116 五、發明說明(26) 管中所使用之具有各種透鏡形式的任何材料,除了極化維 持性質(JP-A-5-1 69 0 1 5 )。 ^ 關於使用於此的透鏡片,可使用具有可防止消除發射光 之極化性質之優異透光率的透鏡片,例如,具有8〇%以上 之總透光率’以85%以上較佳,90%以上為特佳,及5%以下 之汽漏百分比(透射比),2%以下更佳,1%以下為特佳,如 經由透過設置正交尼科耳稜晶之配置消除極化所發展。 由於消除極化係藉由雙折射或多重散射而發生,因而顯 現極化維持性質之前述的透鏡片可經由儘可能地降低雙折 射或降低光線軌道中之平均反射(散射)之數目而產生。更 詳細說明,透鏡片可利用參照光透射樹脂板或散射極化板 而例舉之一或多種聚合物形成,尤其係具有低雙折射之樹 月曰(具有良好光學等向性之樹脂),諸如三醋酸纖維素基樹 脂、聚甲基丙烯酸甲酯、聚碳酸酯及去曱蓓烯基樹脂。 關於透鏡片,可使用具有適當透鏡形態諸如具有許多外 凸類型或折射率分佈型(GI型)區域(其之折射率係利用光 聚合物等等作控制’尤其係形成於視需要可包含具有不同 ,射率之樹脂之透明樹脂基材之表面上或内部之微小透鏡 區域)之透鏡片’具有經由將設於透明樹脂基材中之許多 通孔填補與樹脂具有不同折射率之聚合物而形成之透鏡區 域的透鏡片及具有利用一薄層固定許多球面透鏡之單層 之透鏡片由對利用折射率差之光路徑之控制的觀點來 看’透鏡片為具有在任一或兩表面上(尤其係如圖4所示之 片材8的任一表面)之粗化結構之特殊透鏡結構8 1的形態較89109116, ptc page 29 45 57 Ο δ Λ_η-Correction__ Case No. 89109116 V. Description of the invention (26) Any material used in the tube with various lens forms, except for polarization maintaining properties (JP-A-5 -1 69 0 1 5). ^ As for the lens sheet used here, a lens sheet having excellent light transmittance that can prevent the polarization property of the emitted light from being eliminated can be used, for example, a total light transmittance of 80% or more is preferably 85% or more, Above 90% is particularly good, and the percentage of vapor leakage (transmittance) below 5%, more preferably below 2%, especially below 1%, such as by eliminating the polarization through the configuration of crossed Nicol prisms development of. Since polarization elimination occurs by birefringence or multiple scattering, the aforementioned lens sheet exhibiting polarization maintaining properties can be produced by minimizing birefringence or reducing the number of average reflections (scattering) in the light track. In more detail, the lens sheet can be formed by using one or more polymers exemplified with reference to a light-transmitting resin plate or a scattering polarizing plate, especially a tree with low birefringence (resin with good optical isotropy), Such as cellulose triacetate-based resins, polymethyl methacrylate, polycarbonate, and norberene-based resins. Regarding the lens sheet, it is possible to use a lens having an appropriate lens shape such as a region having many convex types or a refractive index distribution type (GI type) whose refractive index is controlled using a photopolymer or the like, and is formed in particular if necessary. Differently, the lens sheet of the transparent resin substrate of the emissivity resin (the micro lens area on or inside the transparent resin substrate) has a polymer having a refractive index different from that of the resin by filling many through holes provided in the transparent resin substrate. The lens sheet of the formed lens area and the single-layered lens sheet having a single layer holding a plurality of spherical lenses by a thin layer are viewed from the viewpoint of controlling the light path using the refractive index difference. 'The lens sheet is provided on either or both surfaces ( In particular, the shape of the special lens structure 8 1 of the roughened structure of the sheet 8 shown in FIG. 4 is more
89109116.ptc 第30頁 45570489109116.ptc Page 30 455704
形成前述透鏡形態之粗化結構可為任意結構,只要立可 控制由Μ材所透射之光的光路徑,並使透射光朝前方聚集 即可。粗化結構之例子包括線性槽溝或具有三角形截面之 突起物之條紋或格子形的排列,及具有諸如三角錐、四角 錐及多角錐之底部之許多圓錐形微小突起物的點狀排列。 線性或點狀粒化結構可為球面透鏡、非球面透鏡或半柱面 透鏡。因此’可使用適當的透鏡形態。 ^前述具有線性或點狀粗化結構之透鏡月的形成可利用適 4的方法完成,諸如包括將樹脂溶液或樹脂形成單體填充 至用於形成預定粗化結構之模具中,然後再視需要使材料 聚合’以將粗化形態轉移至材料之方法,及包括將樹脂片 材於模具上熱壓’以將粗化形態轉移至樹脂片材之方法。 透鏡片可利用與支承片材相同種類的材料形成,例如,經 由提供具有透鏡形態之支承片材而製得。或者,可將二或 多個不同的樹脂層層合,而形成透鏡片。 可將一或多個透鏡片設於層合物之發射面上。若有之二 或多個透鏡片可相同或不同。然而,此等層以整體保持極 化維持性質較佳。當將透鏡片鄰接於層合物(偏光管)設置 時’係使在其間形成間隙的配置較佳。由全反射的觀點來 看’此間隙以充分地較入射光之波長大較佳。 在透鏡片中之透鏡形態係由線性粗化結構製成的情況 中’由對朝向前方之光路徑之控制的觀點來看,將透鏡形 態之線性方向設置成平行或垂直於偏光散射板之光學軸The roughened structure forming the aforementioned lens form may be any structure as long as the light path of the light transmitted by the M material can be controlled, and the transmitted light can be focused forward. Examples of the roughened structure include a linear groove or a striped or grid-like arrangement of protrusions having a triangular cross-section, and a dot-like arrangement of a plurality of conical minute protrusions such as a triangular pyramid, a quadrangular pyramid, and a polygonal pyramid at the bottom. The linear or dot-like granular structure may be a spherical lens, an aspherical lens, or a semi-cylindrical lens. Therefore, an appropriate lens form can be used. ^ The formation of the aforementioned lens with a linear or dot-like roughened structure can be accomplished by a suitable method, such as filling a resin solution or a resin-forming monomer into a mold for forming a predetermined roughened structure, and then if necessary A method of polymerizing a material 'to transfer a roughened form to a material, and a method including hot pressing a resin sheet on a mold' to transfer a roughened form to a resin sheet. The lens sheet can be formed from the same kind of material as the support sheet, for example, by providing a support sheet having a lens form. Alternatively, two or more different resin layers may be laminated to form a lens sheet. One or more lens sheets may be provided on the emitting surface of the laminate. If there are two or more lens sheets, they may be the same or different. However, it is better for these layers to maintain polarization as a whole to maintain properties. When the lens sheet is provided adjacent to the laminate (polarizing tube), it is preferable to arrange the gap therebetween. From the viewpoint of total reflection, it is better that this gap is sufficiently larger than the wavelength of incident light. In the case where the lens form in the lens sheet is made of a linear roughened structure, 'from the viewpoint of controlling the light path toward the front, the linear direction of the lens form is set to be parallel or perpendicular to the optical of the polarizing diffuser plate. axis
4 5 57 0 4 __案號 89109116__车月日__ 五、發明說明(28) (發射偏光之振盪平面)較佳。在設置二或多個此種透鏡片 之情況中,由對光路徑之控制的觀點來看,係使兩垂直相 鄰層之線性方向彼此相交的配置較佳。 如圖4所示,可將一或多個先前提及的極化維持光擴散 層7隨同用於使發射光(線性偏光)擴散,同時儘可能地維 持其極化’以使發射均勻或放鬆透鏡片之形態之影像,因 而增進可見度之透鏡片8而設置於透鏡片與層合物之間, 或於透鏡片之發射面上,於作為偏光管之層合物4之發射 面上。 可將光擴散層設置為由扁平材料製成的獨立層,或可設 置為與透鏡片成為一體的相關層。在將光擴散層鄰接於層 合物設置之情況中,如同透鏡片之情況,係使在其間形成 間隙的配置較佳β若有之二或多個光擴散層可相同或不 同。然而,此等層以整體保持極化維持性質較佳。 待遠離於偏光管而設置之光學層可視需要利用黏著劑層 或其類似物而黏合至層合物。然而,將具有粗化表面結構 之光學層諸如前述的粗化表面型光擴散層及具有粗化結構 之透鏡片設置成具有間隙較佳。因此,可將光學層諸如 擴散層設置為由扁平材料製成的獨立層,或可設置 他光學層緊密整合的相關層。 %八 在如圖4所示將光擴散層7與透鏡片8結合使用的情兄 中’可將-或多個光擴散層設置於透鏡片與偏光管之 /或在透鏡片之發射面。提到具有包含 透鏡形態之透鏡片,由對朝向前方之光路徑之控制4 5 57 0 4 __Case No. 89109116__Car Moon Day__ V. Description of the invention (28) (oscillating plane that emits polarized light) is better. In the case where two or more such lens sheets are provided, from the viewpoint of controlling the light path, a configuration in which the linear directions of two vertically adjacent layers intersect each other is preferable. As shown in FIG. 4, one or more of the previously mentioned polarization-maintaining light diffusion layers 7 may be used to diffuse the emitted light (linearly polarized light) while maintaining its polarization as much as possible to make the emission uniform or relaxed. The image of the shape of the lens sheet, and thus the lens sheet 8 for improving visibility is disposed between the lens sheet and the laminate, or on the emission surface of the lens sheet, and on the emission surface of the laminate 4 as a polarizer. The light diffusion layer may be provided as a separate layer made of a flat material, or may be provided as a related layer integrated with the lens sheet. In the case where the light diffusing layer is provided adjacent to the laminate, as in the case of a lens sheet, the arrangement forming a gap therebetween is preferably β. If there are two or more light diffusing layers, they may be the same or different. However, it is better for these layers to maintain polarization maintenance properties as a whole. The optical layer to be set away from the polarizer may be bonded to the laminate by using an adhesive layer or the like, if necessary. However, it is preferable that an optical layer having a roughened surface structure such as the aforementioned roughened surface type light diffusion layer and a lens sheet having a roughened structure be provided with a gap. Therefore, an optical layer such as a diffusion layer may be provided as a separate layer made of a flat material, or a related layer in which other optical layers are tightly integrated may be provided. % 八 In the brother who uses the light diffusion layer 7 in combination with the lens sheet 8 as shown in FIG. 4, one or more light diffusion layers may be provided on the lens sheet and the polarizer and / or on the emitting surface of the lens sheet. Mentioned to have a lens sheet containing a lens form, controlled by the path of the light path facing forward
89109116.ptc 第32頁 45570489109116.ptc Page 32 455704
案號 89109116 五、發明說明(29) 來看,係使透鏡形態之線性方向平行或垂直於偏光散射板 之光學軸的配置較佳。當設置二或多個此種透鏡片時,由 對光路徑之控制之效率的觀點來看,係使兩垂直相鄰層之 線性方向彼此相交的配置較佳。 圖6所π之偏光管包括具有藉由光路徑9而與光透射樹脂 板1之一或兩個表面部分保持緊密接觸之偏光散射板3的層 合物4,光路徑9如圖6所示亦作為設於其間之黏著劑層, 以控制自光透射樹脂板於偏光散射板接收到之透射光的 量。 根據前述說明’使用使光透射樹脂板與偏光散射板有間 隙插置於其間之隔離配置使其可滿足關於全反射的條件, 因此而使透射光保持於光透射樹脂板中。此外,透射光可 經由光路徑散射’以致其自光透射樹脂板經由光路徑而引 入至偏光散射板中。在此過程中’經由調整光路徑之配 置,可控制自光透射樹脂板於偏光散射板接收到之光的 量’因此而可使光管上之亮度均勻化。 最終可將光路徑插置於光透射樹脂板與偏光散射板之 間°因此’光路徑可利用任何適當方法形成。舉例來說, 可使光透射樹脂板或偏光散射板之形成伴隨形成在其之一 或兩表面上的粗化結構,而形成與光透射樹脂板或偏光散 射板為一體的粗化結構,因而將光透射樹脂板及偏光散射 板與插置於其間的粗化結構層合。 或者,可將光透射樹脂板及偏光散射板與形成為光路徑 之具有粗化結構之片材的插入物層合。此外,可將光透射Case No. 89109116 V. Description of the Invention (29) From the viewpoint of the configuration, the linear direction of the lens shape is parallel or perpendicular to the optical axis of the polarizing plate. When two or more such lens sheets are provided, from the viewpoint of the efficiency of the control of the light path, a configuration in which the linear directions of two vertically adjacent layers intersect each other is preferable. The polarizing tube shown in FIG. 6 includes a laminate 4 having a polarizing light scattering plate 3 in close contact with one or both surface portions of the light transmitting resin plate 1 through a light path 9. The light path 9 is shown in FIG. 6. It also acts as an adhesive layer interposed therebetween to control the amount of transmitted light received from the light-transmitting resin plate and the polarized light scattering plate. According to the foregoing description ', the use of an isolated configuration with a gap between the light-transmitting resin plate and the polarized light scattering plate interposed therebetween makes it possible to satisfy the condition regarding total reflection, and thus the transmitted light is held in the light-transmitting resin plate. Further, the transmitted light may be scattered via the light path 'so that it is introduced into the polarized light scattering plate from the light transmitting resin plate via the light path. In this process, ‘the amount of light received from the light-transmitting resin plate and the polarizing diffuser plate can be controlled by adjusting the configuration of the light path’, so that the brightness on the light pipe can be made uniform. Finally, the light path can be interposed between the light-transmitting resin plate and the polarizing light scattering plate so that the 'light path can be formed by any appropriate method. For example, the formation of a light-transmitting resin plate or a polarizing light scattering plate may be accompanied by a roughened structure formed on one or both surfaces thereof, thereby forming a roughened structure integral with the light-transmitting resin plate or a polarizing light scattering plate. A light transmitting resin plate and a polarizing light scattering plate are laminated with a roughened structure interposed therebetween. Alternatively, the light-transmitting resin plate and the polarizing light-scattering plate may be laminated with an insert of a sheet having a roughened structure formed as a light path. In addition, light can be transmitted
89109116.ptc 第33頁 4557 04 _案號 8910911ft_年月日_^_ 五、發明說明(30) 樹脂板及偏光散射板與經透過光罩而逐圖型地塗布於光透 射樹脂板或偏光散射板之一或兩表面上之粗化結構之插入 物層合。因此’可將光路徑與光透射樹脂板或偏光散射板 整體形成’或與光透射樹脂板或偏光散射板個別形成。 光路徑可為適當形態,以使光透射樹脂板及偏光散射板 可彼此部分連接,例如,點狀形態或條紋形態。由對於經 由與光透射樹脂板或偏光散射板接觸而控制入射光之量之 能力的觀點來看,將光路徑在其接觸表面上形成為平坦形 態較佳。 在將光路徑設為構成於光透射樹脂板或偏光散射板之表 面上之粗化結構之外凸部分的情況中,由外凸部分之黏著 及藉由在外凸部分之間之内凹部分之全反射的觀點來看, 其具有圖7所示之矩形載面的粗化結構較佳。更詳細說 明’内凹部分91及外凸部分92(光路徑9)具有平坦的表面 93及95。因此’由全反射的觀點來看’光透射樹脂板及偏 光散射板未與光路徑緊密接觸之區域以具有平坦的表面較 佳。 前述的平坦表面可具有由粗加工所產生的微細粗化結 構。然而,由全反射或緊密接觸的觀點來看,平坦表面以 儘可能地光滑較佳。尤其’將在光路徑中作為接觸表面之 平坦表面設置為平坦,以與光透射樹脂板或偏光散射板保 持緊密接觸較佳。 此外*如圖7所示由内凹部分91製成之光路徑的光透射 樹脂板侧以具有截面為連續第一差分曲線及角落部分94具89109116.ptc P.33 4557 04 _Case No. 8910911ft_Year_Year_ ^ V. Description of the invention (30) Resin plates and polarized light scattering plates are coated on a light-transmitting resin plate or polarized light pattern by pattern through a reticle. Laminated inserts of coarse structure on one or both surfaces of the diffuser plate. Therefore, 'the light path may be integrally formed with the light transmitting resin plate or the polarizing light scattering plate' or may be formed separately from the light transmitting resin plate or the polarizing light scattering plate. The light path may be in a suitable form so that the light-transmitting resin plate and the polarizing light-scattering plate may be partially connected to each other, for example, a dot-like shape or a stripe-like shape. From the viewpoint of the ability to control the amount of incident light by contact with a light-transmitting resin plate or a polarizing light scattering plate, it is preferable to form the light path in a flat state on its contact surface. In the case where the light path is set as a convex portion of the roughened structure formed on the surface of the light-transmitting resin plate or the polarizing light scattering plate, it is caused by the adhesion of the convex portions and by the concave portions between the convex portions. From the viewpoint of total reflection, a roughened structure having a rectangular carrier surface as shown in FIG. 7 is preferable. In more detail, the concave portion 91 and the convex portion 92 (light path 9) have flat surfaces 93 and 95. Therefore, "from the viewpoint of total reflection", it is preferable that the light-transmitting resin plate and the polarizing-scattering plate have a flat surface in a region not in close contact with the light path. The aforementioned flat surface may have a fine roughened structure resulting from rough machining. However, from the viewpoint of total reflection or close contact, a flat surface is preferably as smooth as possible. In particular, it is preferable to set the flat surface as the contact surface in the light path to be flat so as to maintain close contact with the light-transmitting resin plate or the polarizing light scattering plate. In addition, as shown in FIG. 7, the light transmission of the light path made of the concave portion 91 is continuous on the resin plate side with a first differential curve having a continuous cross section and 94 corner portions.
89109]16.ptc 第34頁 455704 _案號 89109116___车月日_修正 五、發明說明(31) 有平順曲線較佳。如在光路徑之光透射樹脂板側上之角落 部分具有尖銳的角度,則其會導致產生亮點及亮線。 光路徑之配置可由待被偏光散射板接收之入射光的期望 量而適當地決定。在本發明,當將光源設置於光管之側 面,而形成平面偏光源時,一般會出現亮度朝光源而増加 的趨勢。為使光管之整個發射表面的亮度均勻化,係使光 路徑有分佈密度的變化,尤其係使單位平面面積之光路徑 的分佈密度隨距光源之距離的增加而增加的配置較佳。光 路徑之分佈密度可逐步或連續地變化。 由降低光管之厚度的觀點來看,為在粗化結構中在内凹 部分與外凸部分之間之高度差之光路徑的長度,即在光透 射樹脂板與偏光散射板之間在沒有光路徑之位置之間隙的 厚度,以小為佳。當間隙之厚度大時,有更多光經由此部 分洩漏產生光池’而使光的百分利用率降低。為防止光1 百分利用率降低及確保間隙大於透射光之波長,因而得到 前述的全反射效率,光路徑之長度以自〇 5至1〇〇〇微米 佳,500微米以下更佳,自1至1〇〇微米為特佳。 光透射樹脂板與偏光散射板透過光路徑之部分接觸以經 由將兩組件於其界面處黏合而達成較佳,以儘可能地抑制 被界面反射,因此而促進光被光路徑自光透射樹脂板 至偏光散射板。黏合由防止軸偏差的觀點來看有利。* 關於黏合,如同前述層合型偏光散射板之情況, 任何適當的黏著劑’諸如黏性黏著劑、熱熔膠 :: 化黏著劑及熱固性黏著齊j。使用具有優異透明度及與此等89109] 16.ptc page 34 455704 _ case number 89109116 _ car month day _ amendment V. Description of the invention (31) It is better to have a smooth curve. If the corner portion on the light transmitting resin plate side of the light path has a sharp angle, it may cause bright spots and bright lines. The configuration of the light path can be appropriately determined by the desired amount of incident light to be received by the polarized light scattering plate. In the present invention, when the light source is disposed on the side of the light pipe to form a flat-biased light source, the brightness tends to increase toward the light source. In order to make the brightness of the entire emission surface of the light pipe uniform, the distribution density of the light path is changed, especially the configuration in which the distribution density of the light path per unit plane area increases as the distance from the light source increases. The distribution density of the light path can be changed stepwise or continuously. From the viewpoint of reducing the thickness of the light pipe, it is the length of the light path of the height difference between the concave portion and the convex portion in the roughened structure, that is, between the light transmitting resin plate and the polarizing light scattering plate. The thickness of the gap at the position of the light path is preferably small. When the thickness of the gap is large, more light leaks through this part to generate a light pool ', which reduces the percentage utilization of light. In order to prevent the percentage utilization of light 1 from decreasing and to ensure that the gap is larger than the wavelength of transmitted light, the aforementioned total reflection efficiency is obtained. The length of the light path is preferably from 0.05 to 1,000 microns, and more preferably below 500 microns. Up to 100 microns is particularly preferred. The light-transmitting resin plate is in contact with the part of the polarizing light-scattering plate that passes through the light path to achieve better by bonding the two components at its interface, so as to suppress the reflection from the interface as much as possible, thus promoting the light from the light-transmitting resin plate by the light path To the polarized light scattering plate. Adhesion is advantageous from the viewpoint of preventing shaft deviation. * Regarding the adhesion, as in the case of the aforementioned laminated polarized light scattering plate, any appropriate adhesive agent such as an adhesive agent, a hot-melt adhesive: an adhesive and a thermosetting adhesive are used. Use with excellent transparency and more
455704 曰455704 day
Ji·正 案號89】09Π6 五'發明說明(32) 組件儘可能接近之折射率的黏著劑材 如圖6所又’可使用此一黏著劑於形成4二= 光透射樹脂板1與偏光散射板3彼此黏合。 為形成平面偏光源,可將一哎多彻 ^ ^ ^ w ϋ H 次夕個適當的光學層設置於 任何適S位置,。此先學層並無特殊之限制。舉例來說,可 使用用於形成液晶顯示裝置之任何適當的光學層,諸如 化板二相差板及液晶單元。在此情況,可利用插置於其間 之黏者劑層或其類似物而使前述的透鏡片及光擴散層與上 方的光學層保持緊密接觸 '然而,在具有粗化結構之透鏡 >1或粗化表面型光擴散層之情況中,係設有前述的間隙的 配置較佳。 構成偏光管或平面偏光源之各種層各可包括加入於其中 之紫外光吸收劑’諸如水楊酸酯基化合物、苯酚基化合 物、苯并二咕基化合物、氰基丙烯酸酯基化合物及鎳錯合 物基化合物’以視需要而具有紫外光吸收力。 如前所述’根據本發明之偏光管及平面偏光源可提供其 振盈平面(極化轴)經適當控制之線性偏光,因此而可使用 於利用線性偏光之適當裝置及用途中,如利用其優點而形 成液晶顯示裝置。 實施例1 使200份(以下係以重量計)之“樹脂(51^131^八543八111 CHEMICAL INDUSTRY CO·,LTD.製造)及 800 份之聚碳酸酯 (Pan 1 ite,TEIJIN LTD.製造)之20重量百分比的二氣甲烷 溶液進行流延’而形成厚度8 〇微米之聚合物薄膜’然後使 第36頁 89109116.ptc l 45 5 7 Ο 4 ___案號89109116_车月曰 倏正_ 五、發明說明(33) 其在80 °C之溫度及2. 5之牵引比下拉伸,並快速冷卻,而 製得偏光散射板。 前述的偏光散射板包含以晶域形態分散於由聚碳酸酯製 成之薄膜中之由AS樹脂製成的微小晶域,且展現0. 05之△ nl、0.001之An2及0.001之Δη3之折射率差。在偏光顯微 鏡下根據相差利用顏色測量前述微小晶域之平均直徑。結 果’ Δηΐ方向中之長度約為8微米。 接著將前述的偏光散射板以使其△ η 1方向以4 5度角與側 面相交的配置黏合至丙烯酸系樹脂板(三菱人造絲股份有 限公司(Mitsubishi Rayon Co.,Ltd.)製造)之一表面, 而製得偏光管。然後利用由消光PET基反射片材製成之燈 管反射器將冷陰極射線管固定至偏光管之一側面。將包含 有銀真空蒸發於其上之PET片材之單面反射片材設置於偏 光散射板之下表面,而製得平面偏光源。 比較實施例1 以與實施例1相同之方式製得平面光源,除了使用經由 將包含其中加入鈦白之反射墨水以點狀形態印刷於厚度2 毫米之丙烯酸系樹脂板的一表面上,然後再將由發泡PE? 製成之白色反射板设置於丙稀酸系樹脂板之相同表面上而 製得之光管。 評估試驗1 將於實施例1及比較實施例1中製得之平面(偏)光源各於 前向及於斜向以視覺觀察其亮度。結果,兩光源在前向展 現幾乎相同的亮度β然而,當在斜向觀察時,實施例1之Ji · Zheng Case No. 89] 09Π6 Five 'Description of the Invention (32) The adhesive material with the refractive index as close as possible to the component is shown in Figure 6 again. This adhesive can be used to form 4 2 = light transmitting resin plate 1 and polarized light. The diffusion plates 3 are adhered to each other. In order to form a plane-biased light source, an appropriate optical layer can be set at any suitable position, such as ^ ^ ^ w ϋ H. There are no special restrictions on this level. For example, any suitable optical layer used to form a liquid crystal display device, such as a two-phase plate and a liquid crystal cell, can be used. In this case, an adhesive layer or the like interposed therebetween can be used to keep the aforementioned lens sheet and light diffusion layer in close contact with the optical layer above. However, in a lens having a roughened structure> 1 In the case of roughening the surface-type light diffusion layer, the arrangement in which the aforementioned gap is provided is preferable. The various layers constituting the polarizer or the planar polarized light source may each include an ultraviolet light absorber such as a salicylate-based compound, a phenol-based compound, a benzodiacyl-based compound, a cyanoacrylate-based compound, and a nickel oxide added thereto. The compound-based compound 'has ultraviolet light absorption as needed. As described above, the polarizing tube and the planar polarized light source according to the present invention can provide linearly polarized light whose plane of polarization (polarization axis) is appropriately controlled, and therefore can be used in appropriate devices and applications using linearly polarized light, such as using Due to these advantages, a liquid crystal display device is formed. Example 1 200 parts (hereinafter referred to by weight) of "resin (51 ^ 131 ^ 8,543,111,111 manufactured by Chemical Industry Co., Ltd.)" and 800 parts of polycarbonate ("Pan 1 ite, manufactured by TEIJIN LTD." ) 20% by weight of digas methane solution is cast 'to form a polymer film with a thickness of 80 microns' and then make a page 89109116.ptc l 45 5 7 Ο 4 ___ Case No. 89109116_ _ V. Description of the invention (33) It is stretched at a temperature of 80 ° C and a traction ratio of 2.5 and rapidly cooled to obtain a polarized light scattering plate. The aforementioned polarized light scattering plate includes a crystal domain dispersed in The microcrystalline domains made of AS resin in the film made of polycarbonate exhibit refractive index differences of Δnl of 0.05, An2 of 0.001, and Δη3 of 0.001. The foregoing is measured by color under a polarizing microscope based on the phase difference. The average diameter of the minute crystal domains. As a result, the length in the Δηΐ direction was about 8 microns. Then, the aforementioned polarizing light scattering plate was bonded to the acrylic resin plate in a configuration where the Δ η 1 direction intersected the side surface at a 45 degree angle ( 2. Mitsubishi Rayon Co., Ltd. Rayon Co., Ltd.) to produce a polarized tube. Then, a cold-cathode ray tube was fixed to one side of the polarized tube using a lamp reflector made of a matte PET-based reflective sheet. A single-sided reflective sheet having a PET sheet on which silver was vacuum-evaporated was set on the lower surface of a polarized light scattering plate to obtain a planar polarized light source. Comparative Example 1 A planar light source was prepared in the same manner as in Example 1. In addition to using a reflective ink containing titanium white added to the surface of an acrylic resin plate with a thickness of 2 mm in a dot form, and then a white reflective plate made of foamed PE? Is set in acrylic acid A light pipe made on the same surface of a resin plate. Evaluation Test 1 The planar (biased) light sources prepared in Example 1 and Comparative Example 1 were visually observed for their brightness in the forward direction and in the oblique direction. Results , The two light sources exhibit almost the same brightness β in the forward direction. However, when viewed obliquely, Example 1
455704 __案號89109116_年月曰 條正_ 五、發明說明(34) 平面偏光源較比較實施例1在更寬廣的角度範圍展現優異 的亮度。 另一方面’將在4 5度之方向具有透射軸之極化板設置於 平面(偏)光源上。然後以與前述之相同方式,測量平面 (偏)光源之亮度。結果,比較實施例1之光源由於極化板 之配置而顯現大約減半的亮度,然而,實施例1之平面偏 光源顯現極少的亮度下降,因此而展現大約為比較實施例 1之兩倍的亮度。 實施例2 使950份之具有165 °C之撓曲溫度及182 °C之玻璃轉移溫 度之去甲掊稀基樹脂(Arton,JSR Inc.製造),及50份具 有80 °C之玻璃轉移溫度及自1〇〇 °c至290 °C之向列液晶化溫 度之由以下通式所表示之液晶聚合物之2〇重量百分比的二 氣甲烷溶液進行流延,而形成厚度100微米之聚合物薄 膜’然後使其在1 80 °c之溫度及3之牽引比下拉伸,並快速 冷卻,而製得偏光散射板。 r'C〇,H〇每 CH, 前述的偏光散射板包含以具有幾乎相同形狀之晶域形態 分散於由去曱蓓烯基樹脂製成之透明薄膜中之液晶聚合 物,其拉伸方向為縱向,且展現〇. 23之Δηΐ、0. 029之A n2及0· 0 2 9之Δη3之折射率差。在偏光顯微鏡下根據相差 利用顏色測量前述微小晶域之平均直徑。結果,△ η 1方向455704 __Case No. 89109116_ Years and Months _ V. Description of the invention (34) The planar polarized light source exhibits superior brightness over a wider angle range than Comparative Example 1. On the other hand, a polarizing plate having a transmission axis in a direction of 45 degrees is set on a flat (polarized) light source. Then, in the same manner as described above, the brightness of the planar (biased) light source is measured. As a result, the light source of Comparative Example 1 exhibited approximately half the brightness due to the configuration of the polarizing plate. However, the flat polarized light source of Example 1 exhibited a slight decrease in brightness, and thus exhibited approximately twice the brightness of Comparative Example 1. brightness. Example 2 950 parts of norformamidine-based resin (manufactured by Arton, JSR Inc.) having a deflection temperature of 165 ° C and a glass transition temperature of 182 ° C, and 50 parts of a glass transition temperature of 80 ° C And a nematic liquid crystal temperature of 100 ° C to 290 ° C, a 20 weight percent solution of a gaseous methane solution of a liquid crystal polymer represented by the following formula is cast to form a polymer having a thickness of 100 microns The film was then stretched at a temperature of 1 80 ° C and a draw ratio of 3, and quickly cooled to obtain a polarized light scattering plate. r'C〇, H〇 per CH, the aforementioned polarizing light scattering plate includes a liquid crystal polymer dispersed in a transparent film made of a debenzene-based resin in the form of crystal domains having almost the same shape, and the stretching direction is In the longitudinal direction, refractive index differences of Δηΐ of 0.02, Δ2 of 0.029, and Δη3 of 0.029 are exhibited. The average diameter of the aforementioned minute crystal domains was measured by a phase difference using a color under a polarizing microscope. As a result, △ η 1 direction
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__案號 89109116 五、發明說明(35) 中之長度約為5微米。 接耆將前述的偏光散射板以使其在Δηΐ方向以45度角與 側面相交的配置黏合至丙烯酸系樹脂板(三菱人造絲股份' 有限公司製造)之一表面,而製得偏光管β然後利用由消 光PET基反射片材製成之燈管反射器將冷陰極射線管固定 至偏光管之一側面。將包含有銀真空蒸發於其上之PET片 材之單面反射片材設置於偏光散射板之下表面,而製得平 面偏光源。 比较實施例2 以與實施例2相同之方式製得平面光源,除了使用經由 將包含其中加入鈦白之反射墨水以點狀形態印刷於厚度2 毫米之兩烯酸系樹脂板的一表面上,然後再將由發泡ρΕτ 製成之白色反射板設置於丙烯酸系樹脂板之相同表面上而 製得之光管。 評估試驗2 將於實施例2及比較實施例2中製得之平面(偏)光源各於 前向及於斜向以視覺觀察其亮度。結果,兩光源在前向展 現幾乎相同的亮度。然而’當在斜向觀察0夺,實施例2之 平面偏光源較比較實施例2在更寬廣的角度範圍展現優異 另一方面,將在45度之方 平面(偏)光源上。然後以與 (偏)光源之亮度。結果,比 之配置而顯現大約減半的亮 向具有透射軸之極化板設置於 前述之相同方式,測量平面 較實施例2之光源由於極化板 度’然而,實施例2之平面偏__Case No. 89109116 5. The length in the description of the invention (35) is about 5 microns. Then, the above-mentioned polarizing plate was bonded to a surface of an acrylic resin plate (manufactured by Mitsubishi Rayon Co., Ltd.) at a configuration that intersects the sides at a 45-degree angle in the Δηΐ direction, and a polarizing tube β was produced. A cold-cathode ray tube is fixed to one side of the polarizer using a lamp reflector made of a matte PET-based reflective sheet. A single-sided reflective sheet containing a PET sheet on which silver was vacuum-evaporated was set on the lower surface of a polarizing light-scattering plate to produce a planar polarized light source. Comparative Example 2 A flat light source was prepared in the same manner as in Example 2, except that a reflective ink containing titanium white was added in a dot-like form on one surface of a diene-based resin plate having a thickness of 2 mm, Then, a white reflection plate made of foamed ρΕτ is set on the same surface of an acrylic resin plate to obtain a light pipe. Evaluation Test 2 The brightness of the planar (biased) light source prepared in Example 2 and Comparative Example 2 was observed in the forward direction and the oblique direction, respectively. As a result, both light sources exhibit almost the same brightness in the forward direction. However, when viewed obliquely, the plane-biased light source of Example 2 exhibits a wider range of angles than that of Comparative Example 2. On the other hand, it will be on a 45-degree-square plane (biased) light source. Then the brightness of the (biased) light source. As a result, the brightness is reduced by about half as compared with the configuration. The polarizing plate having a transmission axis is set in the same manner as described above, and the measurement plane is higher than that of the light source of Example 2 due to the polarization degree.
89109116.ptc 第39頁 ^ 45 57 0 4 _89109116_年月 η 彼 χ_ 五、發明說明。6) ' 光源顯現極少的亮度下降’因此而展現大約為比較實施例 2之兩倍的亮度。使實施例2之平面偏光源在8〇充之環境中 靜置100小時,然後再次操作。結果,實施例2之平 源未顯現亮度下降。 如由前述說明所明顯可見,當將根據本發明之平面偏光 源使用作為供液晶顯示裝置用之背光時,可得到非常明亮 的顯示。此外’根據本發明之平面偏光源展現優異的熱安 定性’因此可長時間保持其功能。 實施例3 使950份之具有182 °C之玻璃轉移溫度之去甲為烯基樹脂 (Arton ’ JSR Inc.製造)及50份之由與實施例2中之相同通 式所表示之液晶聚合物之20重量百分比的二氣曱烷溶液進 行流延’而形成厚度1〇〇微米之聚合物薄膜,然後使其在 1 80 °C之溫度及3之牵引比下拉伸,並快速冷卻,而製得偏 光散射板。如此製得之偏光散射板展現與實施例2相同的 折射率差Δηΐ、Δη2及An3,及平均微小區域直徑。 接著將前述的偏光散射板以使其在Δηΐ方向以45度角與 侧面相交的配置黏合至丙烯酸系樹脂板(三菱人造絲股份 有限公司製造)之一表面,而製得層合物。然後將包含有 銀真空蒸發於其上之PET片材之單向反射片材設置於層合 物之下表面。同時並將光擴散板設置於層合物之上表面, 而製得偏光管。然後利用由消光PET基反射片材製成之燈 管反射器將冷陰極射線管固定至偏光管之一側面。 前述的光擴散板係利用包括將30份平均直徑4微米之聚89109116.ptc page 39 ^ 45 57 0 4 _89109116_ year month η χ_ 5. Description of the invention. 6) 'The light source exhibits very little decrease in brightness' and therefore exhibits approximately twice the brightness of Comparative Example 2. The planar polarized light source of Example 2 was allowed to stand for 100 hours in a 80-charge environment, and then operated again. As a result, the flat source of Example 2 did not show a decrease in brightness. As is apparent from the foregoing description, when the planar polarized light source according to the present invention is used as a backlight for a liquid crystal display device, a very bright display can be obtained. In addition, the 'planar polarized light source according to the present invention exhibits excellent thermal stability' and therefore can maintain its function for a long time. Example 3 950 parts of norbornene having a glass transition temperature of 182 ° C were olefin-based resin (manufactured by Arton 'JSR Inc.) and 50 parts of a liquid crystal polymer represented by the same general formula as in Example 2 20% by weight of the dioxane solution is cast to form a polymer film with a thickness of 100 microns, and then it is stretched at a temperature of 1 80 ° C and a draw ratio of 3, and rapidly cooled, and A polarizing light scattering plate was prepared. The thus obtained polarized light scattering plate exhibited the same refractive index differences Δηΐ, Δη2, and An3 as in Example 2, and the average minute region diameter. Next, the aforementioned polarizing light scattering plate was bonded to a surface of an acrylic resin plate (manufactured by Mitsubishi Rayon Co., Ltd.) in a configuration in which the sides intersected with the side surface at a 45-degree angle in the Δηΐ direction to obtain a laminate. A unidirectional reflective sheet containing a PET sheet on which silver was vacuum-evaporated was then placed on the lower surface of the laminate. At the same time, a light diffusing plate was set on the upper surface of the laminate to prepare a polarizer. A cold-cathode ray tube was then fixed to one side of the polarizer using a lamp reflector made of a matting PET-based reflective sheet. The aforementioned light diffusing plate is formed by using
89109116.ptc 第40頁 455704 案號 8910fl11fi 五、發明說明(37) 梦氧顆粒加至7 0份之紫外丼固化環g掏_ ,, ± ^ ^ ^系卜元U化衣氧樹月日,將混合物攪拌 以使其4泡,將材料於80微米厚三醋酸纖 面塗布米之厚度,然後再使經塗 】膜二表 ί耳=公分之累積刺量下照射來自高㈣氣燈之 、固化在光擴散板中,聚發氧顆粒對固化環氧 樹脂之折射率之比為〇.95。在包含光擴散板插置於正交尼 ::ϊ ί之Γ化器之間之配置中,由於消除極化而洩漏之 光的量為入射光總量的〇. 7% ^ 實施例4 以與實施例3相同之方式製得偏光管及平面偏光源 了1用利用包括下列步驟之方法製得之具有微細粗化表面 I。構之材料作為光擴散板:將丨〇份具有平均直徑8微 之氡化矽顆粒、1 00份紫外光固化丙烯胺基甲酸酯 平、 物及3份二苯甲酮與乙酸伸乙酯在高速下攪拌而得具 50重量百分比固體含量之分散物,將分散物塗布至厚度 微米之三醋酸纖維素薄膜之—表面,將經塗布之材料乾 以使塗布薄膜之厚度達到4微米,然後再使經塗布之稱、 =〇毫焦耳/平方公分之累積劑量下照射來自高壓汞装 虱燈之光,以使其固化。 … 光擴散板顯現0. 93之氧化矽顆粒對固化樹脂之折射 比。由於消除極化而洩漏之光的量為入射光總量的丨卟。 如利用表面糙度儀所測得,光擴散板展現丨.5微米之 。 糖度Ra(根據JIS Β 060丨於1〇個點平均得的值)。 也_較f施例Π89109116.ptc Page 40 455704 Case No. 8910fl11fi V. Description of the invention (37) The dream oxygen particles are added to 70 parts of the UV ray curing ring g, ,,, ± ^ ^ ^ is the U-shaped oxygen tree moon day, The mixture was stirred to make it 4 bubbles, and the material was coated with a thickness of rice on a surface of 80 micrometers thick triacetate fiber, and then the coated film was irradiated with a high amount of gas from a high tritium gas lamp, Cured in a light diffusion plate, the ratio of the refractive index of the polyoxygen particles to the cured epoxy resin was 0.95. In a configuration including a light diffusing plate interposed between orthogonal :: ϊ Γ's, the amount of light leaked due to the elimination of polarization is 0.7% of the total amount of incident light ^ Example 4 以A polarizing tube and a planar polarized light source were prepared in the same manner as in Example 3 and had a finely roughened surface I prepared by a method including the following steps. The structure of the material is used as a light diffusion plate: 10 parts of silicon oxide particles having an average diameter of 8 micrometers, 100 parts of UV-curable acrylaminocarbamate, 3 parts of benzophenone and ethyl acetate Stir at a high speed to obtain a dispersion with a solid content of 50% by weight. Apply the dispersion to the surface of a micron-thick cellulose acetate film. Dry the coated material so that the thickness of the coated film reaches 4 microns. Then, the light from the high-pressure mercury-containing lice lamp was irradiated at a cumulative dose of 0 millijoules per square centimeter of the coated name to cure it. … The light diffusion plate shows a refractive index of 0.93 of silica particles to the cured resin. The amount of light leaked due to the elimination of polarization is the porosity of the total amount of incident light. As measured with a surface roughness meter, the light diffusion plate exhibited a thickness of .5 microns. Sugar content Ra (value averaged at 10 points according to JIS B 060). Also _ compared to Example Π
455704 --索號89109116__年月 目 偬t_ 五、發明說明(38) 以與實施例3相同之方式製得平面光源,除了使用經由 將包含其中加入鈦白之反射墨水以點狀形態印刷於厚度2 毫米之丙烯酸系樹脂板的一表面上’然後再將由發泡pET 製成之白色反射板設置於丙烯酸系樹脂板之相同表面上而 製得之光管。 上匕較實施例4 以與實施例4相同之方式製得偏光管及平面偏光源,除 了使用包含聚酯薄膜替代三醋酸纖維素薄膜之光擴散板, 因此而使由於消除極化所致的光洩漏量為入射光納量 5_ 2%。 ' 生較實施例5 以與實施例3相同之方式製得偏光管及平面偏光源,除 了並不設置光擴散板。 迕_估試驗3 將於實施例3及4及比較實施例3至5中製得之平面(偏)光 源各利用亮度計(BM-7 ’T0PC0N C0RP·製造)測量其在前向 在中央部分的亮度及在平面上的亮度均勻度。根據比較實 施例1所測定這些測量值之比例。結果記述於下表。括號 中之數字各係指示當根據比較實施例1將極化板以使透射 軸位在45度角之配置設置於平面光源上時,所測得之亮度 的比例。 455704 __案號891Q911g_年月 q 條正 五、發明說明(39) 實施例3 則方亮度(设置極化板) 110(100) 均勻度 良好 實施例4 90(80) 良好 比較實施例3 100(40) 良好 比較實施例4 90(50) 良好 比較實施例5 60(50) 差 與上表中之比較實施例5的比較顯示配置光擴散板使其 可大大地增進前方亮度以及平面上的亮度均勻度。將實施 例與比較實施例3比較顯示實施例發射線性偏光,且透過 極化板而展現大大增進的亮度。將實施例與比較實施例4 比較顯示如光擴散板消除極化’則無法利用發射線性偏光 的優點。因此,顯然當將根據本發明之平面偏光源使用作 為液晶顯示裝置之背光時’可得到一般值(比較實施例3) 之兩倍以上的亮度,而使其可達成均勻度優異之非常明亮 的顯示。 實施例5 經由將與實施例3之相同方式製得之偏光散射板與使用 於實施例1及3之相同的丙烯酸系樹脂板以與實施例1及3之 相同方式層合’而製得層合物(偏光管)^然後將包含有銀 真空蒸發於其上之PET片材之單向反射片材設置於層合物 之下表面。同時並將光擴散板設置於層合物之上表面,而 製得偏光管。然後利用由消光PET基反射月材製成之燈管 反射器將冷陰極射線管固定至偏光管之一側面。 前述的透鏡片係經由在厚度80微米之三醋酸纖維素樹脂455704-cable number 89109116__ 年月 目 偬 t_ V. Description of the invention (38) A flat light source was prepared in the same manner as in Example 3, except that the reflective ink containing titanium white was used to print it in a dot shape. A light pipe having a thickness of 2 mm on one surface of an acrylic resin plate, and then a white reflecting plate made of foamed pET was placed on the same surface of the acrylic resin plate. The polarizer and the planar polarized light source were prepared in the same manner as in Example 4 except that a light diffusion plate containing a polyester film instead of a cellulose triacetate film was used. The amount of light leakage is 5_ 2% of the incident light. 'Comparative Example 5 A polarizing tube and a planar polarized light source were produced in the same manner as in Example 3, except that a light diffusion plate was not provided.估 _Estimation test 3 The planar (biased) light sources prepared in Examples 3 and 4 and Comparative Examples 3 to 5 were each measured with a luminance meter (BM-7 'T0PC0N C0RP · made) in the forward direction and the center portion. Brightness and uniformity of brightness on the plane. The ratio of these measured values was determined according to Comparative Example 1. The results are described in the following table. Each number in the parentheses indicates the ratio of the measured brightness when a polarizing plate is disposed on a planar light source with a transmission axis at a 45-degree angle according to Comparative Example 1. 455704 __Case No. 891Q911g_ Year and month q Article 5. Explanation of the invention (39) Example 3 Regular brightness (with polarizing plate) 110 (100) Good uniformity Example 4 90 (80) Good comparative example 3 100 (40) Good comparison example 4 90 (50) Good comparison example 5 60 (50) Poor comparison with the comparison example 5 in the table above shows that the configuration of the light diffusion plate can greatly improve the brightness in the front and on the plane Brightness uniformity. Comparing the embodiment with the comparative example 3 shows that the embodiment emits linearly polarized light and shows a greatly improved brightness through the polarizing plate. Comparing the embodiment with the comparative example 4 shows that if the light diffusion plate is depolarized, the advantage of emitting linearly polarized light cannot be used. Therefore, it is apparent that when a planar polarized light source according to the present invention is used as a backlight of a liquid crystal display device, a brightness that is twice or more of a general value (Comparative Example 3) can be obtained, and it can achieve a very bright uniformity excellent display. Example 5 A layer was obtained by laminating a polarizing light scattering plate prepared in the same manner as in Example 3 and an acrylic resin plate used in Examples 1 and 3 in the same manner as in Examples 1 and 3. A composite (polarizing tube) ^ Then a unidirectional reflective sheet containing a PET sheet on which silver was vacuum-evaporated was placed on the lower surface of the laminate. At the same time, a light diffusing plate was set on the upper surface of the laminate to produce a polarizing tube. A cold-cathode ray tube was then fixed to one side of the polarizing tube using a lamp reflector made of a matte PET-based reflective moon. The aforementioned lens sheet is made of cellulose acetate resin with a thickness of 80 microns.
89109116,ptc 第43頁 455704 匕 _ 案號 89109116_年月 a 五、發明說明(40) 薄膜之一表面上提供具有以350微米之間隔,設置之具有 90度之垂直角及80微米高度之三角形截面之由光固化環氧 樹脂製成之線性突起物之條紋排列的透鏡形態而製得。其 之配置係使透鏡形態位於上側,且條紋的方^平行於前述 的△ n2方向。如此製得之透鏡片當設置於正交尼科耳棱晶 之間時如利用積分球(integrating sphere)所測得,展現 入射光之總量之1. 0 %的透射比(以下為由於消除極化所致 之光的洩漏量),因此其之極化維持性質優異β 實施例6 以與實施例1相同之方式製得偏光管及平面偏光源,除 了將利用包括下列步驟之方法製得之光擴散板設置於層合 物與透鏡片之間:將30份具有平均直徑4微米之聚石夕氧顆 粒加至7 0份之紫外光固化環氧樹脂,將混合物攪拌以使其 消泡’將材料於8 〇微米厚三醋酸纖維素薄膜之一表面塗布 至30微米之厚度,然後再使經塗布之材料在ι,〇〇〇毫焦耳 /平方公分之累積劑量下照射來自高壓汞蒸氣燈之光,以 使其固化。前述的光擴散板由於消除極化所致之光的洩漏 量為入射光總量的〇. 7%。 比較實施例fi 以與實施例5相同之方式製得平面光源,除了使用經由 將包含其中加入鈦白之反射墨水以點狀形態印刷於厚度2 毫米之丙烯酸系樹脂板的一表面上,然後再將由發泡PET 製成之白色反射板設置於丙稀酸系樹脂板之相同表面上而 製得之光管。89109116, ptc Page 43 455704 Dagger_ Case No. 89109116_ Month a. V. Description of the invention (40) A triangle with a vertical angle of 90 degrees and a height of 80 micrometers is provided on a surface of the film at a distance of 350 micrometers. The cross-section is made of a stripe-shaped lens configuration of linear protrusions made of light-curing epoxy resin. The configuration is such that the lens shape is located on the upper side, and the square of the stripes is parallel to the aforementioned Δn2 direction. The lens sheet thus prepared, when set between crossed Nicol prisms, as measured using an integrating sphere, exhibits a transmittance of 1.0% of the total amount of incident light (the following is due to elimination The amount of light leakage due to polarization), so its polarization maintenance properties are excellent β Example 6 A polarizing tube and a planar polarized light source were prepared in the same manner as in Example 1, except that a method including the following steps was used The light diffusing plate is placed between the laminate and the lens sheet: 30 parts of polylithium oxide particles having an average diameter of 4 microns are added to 70 parts of a UV-curable epoxy resin, and the mixture is stirred to defoam 'Coat the material on one surface of an 80 micron thick cellulose triacetate film to a thickness of 30 micron, and then irradiate the coated material with a cumulative dose of 100,000 millijoules per square centimeter from high-pressure mercury vapor. The light of the lamp to cure it. 7%。 The aforementioned light diffusion plate due to the elimination of light due to polarization leakage is 0.7% of the total amount of incident light. Comparative Example fi A flat light source was prepared in the same manner as in Example 5, except that a reflective ink containing titanium white was added thereto in a dot-like form on a surface of an acrylic resin plate having a thickness of 2 mm, and then A light pipe made by setting a white reflecting plate made of foamed PET on the same surface of an acrylic resin plate.
89109116.ptc 第44頁 455704 ___案號89109116_ 年月日 修正___ 五、發明說明(41) 比較實施你丨7 以與實施例5相同之方式製得偏光管及平面偏光源,除 了使用包含聚酯薄膜替代三醋酸纖維素薄膜之透鏡片,因 此而使由於消除極化所致的光洩漏量為入射光總量的 6.2%。 評估試驗4 將於實施例5及6及比較實施例6及7中製得之平面(偏)光 源各利用亮度計(BM-7,TOPCON C0RP.製造)測量其在前向 中央部分的亮度,及將具有44%之透射比及99%之極化度之 市售的吸收型極化板以使透射軸位在45度角之配置設置於 平面光源上之在前向中的亮度。根據沒有極化板之比較實 施例6測定此等測量值之比例。結果記述於下表。 前方亮度 未設置極化板 設置極化板 實施例5 95 76 實施例6 98 77 比較實施例6 100 44 比較實施例7 95 48 上表中之結果顯示實施例可發射線性偏光,並透過極化 板而展現大大增進的亮度。此外’將實施例與比較實施例 7比較顯示如光擴散板消除極化,則無法利用發射線性偏 光的優點。因此,顯然當將根據本發明之平面偏光源使用 作為液晶顯示裝置之背光時,可得到一般值(比較實施例 1)之1.5倍以上的亮度,而使其可達成非常明亮的顯示。89109116.ptc Page 44 455704 ___Case No. 89109116_ Year, Month, and Day Amendment ___ V. Description of the Invention (41) Comparative Implementation 丨 7 A polarizer and a planar polarized light source were prepared in the same manner as in Example 5, except that The polyester film replaces the lens sheet of the cellulose triacetate film, so that the amount of light leakage due to the elimination of polarization is 6.2% of the total incident light. Evaluation Test 4 Each of the planar (biased) light sources prepared in Examples 5 and 6 and Comparative Examples 6 and 7 was measured with a luminance meter (BM-7, manufactured by TOPCON CORP.) For the brightness in the forward central portion, And a commercially available absorption-type polarizing plate having a transmittance of 44% and a polarization of 99% so that the transmission axis is positioned at a 45-degree angle is set on a planar light source in a forward direction brightness. The ratio of these measured values was determined according to Comparative Example 6 without a polarizing plate. The results are described in the following table. The front brightness is not provided with a polarizing plate. Example 5 95 76 Example 6 98 77 Comparative Example 6 100 44 Comparative Example 7 95 48 The results in the table above show that the example can emit linearly polarized light and transmit polarization. Board while exhibiting greatly enhanced brightness. In addition, a comparison between the embodiment and the comparative example 7 shows that if the light diffusion plate is depolarized, the advantage of emitting linearly polarized light cannot be used. Therefore, it is apparent that when the planar polarized light source according to the present invention is used as a backlight of a liquid crystal display device, a brightness of 1.5 times or more of a general value (Comparative Example 1) can be obtained, so that it can achieve a very bright display.
S9109116.ptc 第45頁 455704 ''-----塞號 89109116· _年月 η_修正__ 五、發明說明(42) 在包含加入於其中之光擴散板之實施例6中,在透鏡片上 之線性圖型的影像被放鬆,而増進可見度。 實施例7 將如於實施例3中所製得之相同的偏光散射板利用丙烯 酸系黏著劑層以使其在△ η 1方向以4 5度角與側面相交之配 置黏合至厚度2毫米之市售聚碳酸酯板之一表面,而製得 層合物。將包含有銀真空蒸發於其上之ρΕΤ片材之單向反 射片材設置於層合物之下表面,而製得偏光管。然後利用 由/肖光PET基反射片材製成之燈管反射器將冷陰極射線管 固定至廣合物之一側面。在前述聚碳酸酯板之平面中的平 均相差為80毫微米’及平均延遲轴係平行於其側面(〇度方 向)〇 上匕較實施你丨8 以與實施例7相同之方式製得平面光源,除了使用經由 將包含其中加入鈥白之反射墨水以點狀形態印刷於厚度2 毫米之丙稀酸系樹脂板的一表面上,然後再將由發泡ΡΕτ 製成之白色反射板設置於丙烯酸系樹脂板之相同表面上而 製得之光管。 选較實施例9 以與實施例7相同之方式製得偏光管及平面偏光源,除 了使用丙烯酸系樹脂板(平面内平均相差:5毫微米以下) 替代聚碳酸酯板》 估試驗5 將市售的吸收型極化板以使透射柏位在45度角之配置,S9109116.ptc Page 45 455704 '' ---- Serial No. 89109116 · _ Year Month η_ Correction __ V. Description of the Invention (42) In Embodiment 6, which includes a light diffusion plate incorporated therein, the lens The image of the linear pattern on the film is relaxed and the visibility is enhanced. Example 7 The same polarizing light-scattering plate as prepared in Example 3 was adhered to a city with a thickness of 2 mm by using an acrylic adhesive layer so that it intersects the side at a 45 degree angle in the direction of Δη1. One of the surfaces of the polycarbonate sheet was sold to produce a laminate. A unidirectional reflective sheet containing a pETE sheet on which silver was vacuum-evaporated was set on the lower surface of the laminate to produce a polarizing tube. Then, a cold-cathode ray tube was fixed to one side of the broad compound using a lamp reflector made of / Xiaoguang PET-based reflective sheet. The average phase difference in the plane of the aforementioned polycarbonate plate is 80 nm 'and the average retardation axis is parallel to its side (0 degree direction). The upper surface is implemented in the same manner as in Example 7 to obtain a plane. The light source was printed on a surface of an acrylic resin plate having a thickness of 2 mm in a dot shape by using a reflection ink containing “white” added thereto, and then a white reflection plate made of foamed PET was set on acrylic It is a light pipe made on the same surface of a resin plate. Comparative Example 9 A polarizer and a planar polarized light source were prepared in the same manner as in Example 7, except that an acrylic resin plate (average difference in the plane: 5 nm or less) was used instead of the polycarbonate plate. Evaluation Test 5 The absorbing polarizing plate is sold so that the transmission position is arranged at a 45-degree angle.
455704 _索號89109116_年月 日 搞:ιΤ 五、發明說明(43) ' '-- 設置於在實施例7及比較實施例8及9中製犋夕亚二,&、 τ农付 < 十面(偏)光 源上。各以視覺測量此等配置在前向令之亮度。梦果,真 度依實施例1、比較實施例9及比較實施例8之次序1咸小’ /U 亦以視覺明確地觀察亮度差。在比較實施例9與比較實施 例8之間的亮度差明顯地大於在實施例7與比較實施例g之 間的亮度差。 如可於前述說明所見’當未設置極化板時,實施例7及 比較實施例8及9於前向以視覺觀察得之亮度幾乎相同,因 此’幾乎無法作區別。可以看到在具有極化板之配置中在 實施例7與比較實施例8之間的亮度差使其可透過實施例7 中之極化板而大大地增進線性偏光之亮度。如前所述,當 將根據本發明之平面偏光源使用作為液晶顯示裝置之背光 時,亮度可大大地增進’而使其可達成非常明亮的顯示。 實施例8 將熱熔樹脂(Evaf lex ’ Du P〇nt製造)之甲苯溶液透過其 中形成有直徑1毫米之許多通孔的型板圖案,塗布於如實 施例3中製得之相同偏光散射板的一表面上,然後乾燥而 形成在其光源側上稀少及在其相對側上密集之具有1 〇微米 南度的光路徑。 然後將前述的偏光散射板以使其在A n 1方向與其侧面相 交之配置使光路徑插置於其間而熱壓於厚度2毫米之丙烯 酸系樹脂板(三菱人造絲股份有限公司製造)的一表面上, 其中光源係以45度角設置’而製得偏光管。將包含有銀真 空蒸發於其上之PET片材之單面反射片材設置於偏光管之455704 _ 索 号 89109116_ Engagement: ιΤ V. Description of the invention (43) ''-It is provided in Example 7 and Comparative Examples 8 and 9 which are manufactured in Xixia Second, &, τ 农 付 & lt On ten-sided (biased) light source. The brightness of these arrangements in the forward order was measured visually. In Mengguo, the accuracy is in accordance with the order 1 of Example 1, Comparative Example 9, and Comparative Example 8 and the brightness difference is small. The difference in brightness between Comparative Example 9 and Comparative Example 8 is significantly larger than the difference in brightness between Example 7 and Comparative Example g. As can be seen from the foregoing description, when the polarizing plate is not provided, the brightness of Example 7 and Comparative Examples 8 and 9 which are visually observed in the forward direction are almost the same, and therefore, it is hardly distinguishable. It can be seen that the brightness difference between Example 7 and Comparative Example 8 in a configuration with a polarizing plate allows it to pass through the polarizing plate in Example 7 and greatly enhance the brightness of linearly polarized light. As described above, when the planar polarized light source according to the present invention is used as a backlight of a liquid crystal display device, the brightness can be greatly improved 'so that it can achieve a very bright display. Example 8 A toluene solution of a hot-melt resin (manufactured by Evaflex 'Du Pont) was passed through a pattern pattern having a plurality of through holes having a diameter of 1 mm, and applied to the same polarized light scattering plate prepared in Example 3. On one surface, it is then dried to form a light path with 10 microns south that is scarce on its light source side and dense on its opposite side. Then, the aforementioned polarizing light scattering plate was arranged so that it intersects its side in the direction of A n 1 so that the light path is interposed therebetween and heat-pressed onto a part of an acrylic resin plate (made by Mitsubishi Rayon Co., Ltd.) having a thickness of 2 mm. On the surface, the light source is arranged at a 45 degree angle to make a polarizing tube. A single-sided reflective sheet containing a PET sheet on which silver vacuum evaporates is set on a polarizer.
89109116.pic 第47頁 ^557 04- _案號891(1fl11fi_年月曰_____ 五、發明說明¢44) 下表面。同時接著利用由消光PET基反射片材製成之燈管 反射器將冷陰極射線管固定至偏光管之一侧面,而製得平 面偏光源。 比較實施例1 0 以與實施例8相同之方式製得平面光源,除了使用經由 將包含其中加入鈦白之反射墨水以點狀形態印刷於厚度2 毫米之丙烯酸系樹脂板的一表面上,然後再將由發泡PET 製成之白色反射板設置於丙烯酸系樹脂板之相同表面上而 製得之光管。 比較實施例11 以與實施例8相同之方式製得偏光管及平面偏光源,除 了將熱熔膠塗布至偏光散射板之一表面的全部之上,然後 使偏光散射板完全黏合至丙烯酸系樹脂板,並使熱熔膠層 插置於其間。 評估試驗6 將具有44%之透射比及99%之極化度之市售的吸收型極化 板以使透射軸位在45度角之配置設置在於實施例8及比較 實施例1 0及1 1中製得之平面(偏)光源上。各以視覺測量此 等配置之亮度β結果,與比較實施例丨0的比較顯示實施例 8及比較實施例11透過極化板而顯現大大增進的亮度,因 此而可自平面光源發射線性偏光。 另一方面,比較實施例11在朝向光源處較亮,及隨距光 源之距離的增加而較不亮,其顯現大的亮度變化。然而, 實施例8在其之整個表面上未顯現亮度的視覺差異,因89109116.pic Page 47 ^ 557 04- _Case No. 891 (1fl11fi_year month _____ V. Description of the invention ¢ 44) The lower surface. At the same time, a cold-cathode ray tube is fixed to one side of the polarizing tube using a lamp reflector made of a matting PET-based reflective sheet, thereby producing a planar polarized light source. Comparative Example 10 A flat light source was prepared in the same manner as in Example 8, except that a reflective ink containing titanium white was added thereto in a dot-like form on a surface of an acrylic resin plate having a thickness of 2 mm, and then Then, a white reflective plate made of foamed PET is set on the same surface of an acrylic resin plate to obtain a light pipe. Comparative Example 11 A polarizing tube and a planar polarized light source were prepared in the same manner as in Example 8, except that hot-melt adhesive was applied to the entire surface of one surface of the polarizing light scattering plate, and then the polarizing light scattering plate was completely bonded to the acrylic resin Board, with a hot melt adhesive layer in between. Evaluation Test 6 A commercially available absorptive polarizing plate having a transmittance of 44% and a polarization degree of 99% so that the transmission axis is positioned at a 45-degree angle is set in Example 8 and Comparative Examples 10 and 1 On the flat (biased) light source prepared in 1. The results of visually measuring the brightness β of each of these configurations, compared with Comparative Example 丨 0, show that Example 8 and Comparative Example 11 show greatly improved brightness through the polarizing plate, and therefore, linearly polarized light can be emitted from a planar light source. On the other hand, Comparative Example 11 is brighter toward the light source and less bright as the distance from the light source increases, which shows a large change in brightness. However, Example 8 did not show a visual difference in brightness over its entire surface, because
89109116.ptc 第48頁 d557 〇J^ 891〇9116 年 修正 五、發明說明(45) 此,其之亮度均勻度優異。如前所述,當將根據本發明之 平面偏光源使用作為液晶顯示裝置之背光時,光的百分利 用率可大大地增進,而使其可達成具有優異亮度均勻度及 良好可見度之明亮的顯示。 雖然本發明已就具有特定特異性程度之其較佳形式作說 明,但應明瞭本較佳形式之揭示内容可不脫離如於後文提 出專利申請之本發明之精神及範圍,而就其構造細節及其 各部分之組合及配置作變化。 元件編號說明 1 光 透 射 樹 脂 板 2 黏 著 劑 層 3 偏 光 散 射 板 4 層 合 物 5 光 源 6 單 面 反 射 層 7 擴 散 層 8 透 鏡 片 9 光 路 徑 51 反 射 器 81 特 殊 透 鏡 結 構 91 内 凹 部 分 92 外 凸 部 分 93 平 坦 表 面 94 角 落 部 分 95 平 坦 表 面89109116.ptc Page 48 d557 〇J ^ 891〇 9116 Amended 5. Description of the invention (45) Therefore, its brightness uniformity is excellent. As mentioned above, when the planar polarized light source according to the present invention is used as a backlight of a liquid crystal display device, the percentage utilization of light can be greatly improved, so that it can achieve a bright, excellent brightness uniformity and good visibility. display. Although the present invention has been described in terms of its preferred form with a specific degree of specificity, it should be understood that the disclosure of this preferred form can be made without departing from the spirit and scope of the present invention, such as the one filed in the following patent application, as to its structural details And the combination and configuration of its various parts. Description of component number 1 Light transmitting resin plate 2 Adhesive layer 3 Polarizing light scattering plate 4 Laminate 5 Light source 6 Single-sided reflective layer 7 Diffusion layer 8 Lens sheet 9 Light path 51 Reflector 81 Special lens structure 91 Concave portion 92 Outward convex Part 93 flat surface 94 corner part 95 flat surface
89109116.ptc 第49頁 455704 _案號89109116_年月曰 修正_ 圖式簡單說明 在附圖中: 圖1係根據本發明之偏光管之一具體例的剖面圖; 圖2係根據本發明之偏光管之另一具體例的剖面圖; 圖3係根據本發明之平面偏光源之一具體例的剖面圖; 圖4係根據本發明之平面偏光源之另一具體例的剖面 圖; 圖5係根據本發明之平面偏光源之再一具體例的剖面 圖; 圖6係根據本發明之平面偏光源之又再一具體例的剖面 圖;及 圖7係說明光路徑之截面形狀的圖示。89109116.ptc Page 49 455704 _Case No. 89109116_ Year Month Revision _ The drawing is briefly illustrated in the drawings: FIG. 1 is a cross-sectional view of a specific example of a polarizer according to the present invention; FIG. 2 is a cross-sectional view according to the present invention; Sectional view of another specific example of a polarizer; FIG. 3 is a sectional view of a specific example of a planar polarized light source according to the present invention; FIG. 4 is a sectional view of another specific example of a planar polarized light source according to the present invention; FIG. 6 is a sectional view of still another specific example of the planar polarized light source according to the present invention; FIG. 6 is a sectional view of still another specific example of the planar polarized light source according to the present invention; and FIG. 7 is a diagram illustrating a cross-sectional shape of a light path .
89109116.ptc 第50頁89109116.ptc Page 50
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Application Number | Priority Date | Filing Date | Title |
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JP13142999A JP3514660B2 (en) | 1999-05-12 | 1999-05-12 | Polarized light guide plate and polarized plane light source |
JP13143099A JP3422473B2 (en) | 1999-05-12 | 1999-05-12 | Polarized light guide plate and polarized plane light source |
JP13810299A JP3422474B2 (en) | 1999-05-19 | 1999-05-19 | Polarized light guide plate and polarized plane light source |
JP16672799A JP3422475B2 (en) | 1999-06-14 | 1999-06-14 | Polarized light guide plate and polarized plane light source |
JP17436899A JP3422476B2 (en) | 1999-06-21 | 1999-06-21 | Polarized light guide plate and polarized plane light source |
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