TWI318325B - Line-at-a-time electronic driving method and micro-electromechanical systems device - Google Patents

Line-at-a-time electronic driving method and micro-electromechanical systems device Download PDF

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TWI318325B
TWI318325B TW95139009A TW95139009A TWI318325B TW I318325 B TWI318325 B TW I318325B TW 95139009 A TW95139009 A TW 95139009A TW 95139009 A TW95139009 A TW 95139009A TW I318325 B TWI318325 B TW I318325B
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mirror surface
film
mirror
light
substrate
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TW95139009A
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Chinese (zh)
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W Miles Mark
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Qualcomm Mems Technologies Inc
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1318325 九、發明說明: 【發明所屬之技術領域】 本發明係有關於一種干涉調制器。 【先前技術】 調制::r=IMods)藉由操作微機械元件之光學特性 性πΓ-制各種技術改變微機械元件之光學特 成。千+哨& 文叮又爻此兀件的光學特性而完 成干涉調制器提供本身許多應- 言+笪央输止挪 攸十面顯不姦、光舉 冲异先纖先學調制器至〜 使用不同的干Μ 每些不同的應用可以 Ν的十涉调制器設計。 【發明内容】 又叩5 於—形態中,本私昍+ 器為主的顯示器,* "之特徵係以干涉調制 ° ’其將抗反射鍍膜或微劊、生 一般而言,认 1 •輔助光源。1318325 IX. Description of the Invention: TECHNICAL FIELD OF THE INVENTION The present invention relates to an interferometric modulator. [Prior Art] Modulation::r=IMods) The optical characteristics of the micromechanical element are changed by operating the optical characteristics of the micromechanical element. Thousands of whistle & 叮 叮 爻 叮 叮 叮 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉 干涉~ Use different cognac Each of the different applications can be designed with a sinister modulator. [Summary of the Invention] 叩5 In the form, the display of the private 昍+ device, * " is characterized by interferometric modulation ° 'which will be anti-reflective coating or micro-刽, in general, recognize 1 • Auxiliary light source.

於—形態中,對於干爷 陣列或其它為機楠_ ^ 5周制器之矩陣驅動 巧機蜮兀件’本發明之特徵 期 一般而言,扒 又為鬲效率驅動系統。 其提供更好的靈活性 特徵為一彩色系統, —.hn. 7|χ ITI7 = ) JU.In the form, for the dry array or other matrix-driven device for the machine, the characteristic period of the present invention is generally a 鬲 efficiency driving system. It provides better flexibility as a color system, —.hn. 7|χ ITI7 = ) JU.

;一形態中,本發明之M 其底色可重新配署 寺徵為—電子設備, 能。 属不形態及/或應用功 之特徵為—干涉調制 減少干涉調制器的運 一般而言,於 器设计’其自干涉 轉狀態。 一形態中,本發明 5周制器的光學作用In one form, the background color of the M of the present invention can be re-assigned to the temple as an electronic device, capable. It is characterized by non-morphological and/or applied work—interference modulation reduces the operation of the interferometric modulator. In general, the device design 'has its self-interference state. In one form, the optical function of the 5-week device of the present invention

1077A-4732A-PF 6 1318325 ι而。,於一形態中,本發明之^ ^ ^ ^ ^ ^ ^ 驅動裝置的干涉調制器設計。 a為具有選擇的 一般而言,於一形態中,本 器哎千、、n心 个'"之特徵為-干涉調制 态次干涉調制|g陣列,其被製造 換陣列,曰/々、/ 、 微機電切換器或切 、 或以微機電為基礎的邏輯連接使用。 器 般而言,於一形態中,本發明 甘π、+ 4 d惑特被為一干涉調制 °以應用於光學切換以及光學調制。 I又而言’於一形態中,本 器 私73乏特徵為一干涉調制 /、組成2-D及3 —D光電結構。 種應:般而言’於一形態中,本發明之特徵為調制光的各 ^而言’於—形態中,本發明之特徵為-種微機電 製仏以及根據連續網狀供給程序的封裝方法。 …般而言,於一形態中,本發明之特徵為,於沉積的 薄膜中,干涉調制器當作測試結構用以計算剩餘應力。 【實施方式】 抗反射鍍膜 一種之前描述的干涉調制器設計(於1995年η月6日 申請的美國專利申諳牵筮Q 「c 4 η 〒月業弟08/554, 630號之感應吸收器設 計’在此當作參考)之功效為黑狀態,其中可以將照射於其 表面上的"_7%的光吸收。這有助於反射式顯示器。於此 種。又汁中此種干涉凋制器於未啟動狀態反射既定顏色的 光’並且於啟動狀態吸收光。1077A-4732A-PF 6 1318325 ι and. In one form, the interferometric modulator design of the ^^^^^^^ driving device of the present invention. a is a selection in general, in one form, the device is characterized by a thousand and n-characteristics - interferometric modulation state interferometric modulation | g array, which is manufactured by changing arrays, 曰 / 々, / , MEMS switch or cut, or MEMS based logic connection. In general, in one embodiment, the present invention is applied to optical switching and optical modulation as an interferometric modulation. In addition, in one form, the device is characterized by an interferometric modulation/, consisting of 2-D and 3-D photoelectric structures. Generally speaking, in a form, the invention is characterized in that each of the modulated light is in a form, and the invention is characterized by a microelectromechanical system and a package according to a continuous mesh supply program. method. In general, in one aspect, the invention is characterized in that in the deposited film, the interferometric modulator acts as a test structure for calculating the residual stress. [Embodiment] Anti-reflection coating A previously described interferometric modulator design (in U.S. Patent Application No. 2, filed on November 6, 1995, "C 4 η 〒月业弟08/554, No. 630" The design 'as a reference here' is a black state in which light of "_ 7% is absorbed on its surface. This contributes to the reflective display. This kind of interference in the juice The controller reflects light of a given color in an unactivated state and absorbs light in an activated state.

1077A-4732A-PF 1318325 因為干涉調制器陣列形成於一基底上,吸收能力將藉 由基底本質的反射而降低。於玻璃基底的範例中’反射量 一般約為4%,超過了可見光的頻譜。因此,儘管干涉調制 器結構具有吸收光的能力,黑狀態只能儘可能的黑暗,來 自基底的正面反射還是存在。 一種改善以干涉調制器為基礎的顯示器之整體性能的 方法,係藉由利用抗反射鍍膜(AR c〇atings)。此種鍍膜可1077A-4732A-PF 1318325 Because the interferometric modulator array is formed on a substrate, the absorptive capacity is reduced by the intrinsic reflection of the substrate. In the example of a glass substrate, the amount of reflection is typically about 4%, exceeding the spectrum of visible light. Thus, although the interferometric modulator structure has the ability to absorb light, the black state can only be as dark as possible, and the frontal reflection from the substrate still exists. One method of improving the overall performance of an interferometric modulator-based display is by using anti-reflective coatings. This coating can be

包括-層或更多層的介電膜,其沉積於基底表面上並且被 設計用來減少基底的反射。目前已知有許多種可能的關於 這種薄膜之設計與製造的方法。—種簡單的薄膜設計係氣 化鎂之單一鑛膜’其近似於四分之一波長的厚度。另一種 方法係將氟化㈣四分之—波薄膜沉積於玻璃i,接著日 一層四分之一波薄膜的氣化鎂,另-種方法係於兩者之: 加入一層硫化鋅薄膜。 制顯示器,以便改善顯示系統的效能。於第u圖中= 鍍膜100,如上所述的可包括一層或 竹 於玻璃基底1G6上的玻璃層1()2之表 Β,〉儿積於黏接 藉由將更多光導入玻璃層1〇2中:此AR鍍膜_ 反射的免度。結果為當干涉調 面 時,可以使更多入射光入射干涉 ”乍為吸收模式 獲得更黑的顯示狀態。此AR鍍臈!P列上,且仍然可 上具有干涉調制器陣列的表面上。’、可直接沉積於表面A dielectric film comprising - or more layers deposited on the surface of the substrate and designed to reduce reflection of the substrate. There are many possible ways to design and manufacture such films. A simple film design is a single film of magnesia, which is approximately one quarter wavelength thick. Another method is to deposit a fluorinated (tetra) quarter-wave film on the glass i, followed by a quarter-wave film of magnesium carbide, and another method is to add a zinc sulfide film. Display to improve the performance of the display system. In the figure u, the coating 100, as described above, may include a layer or a surface of the glass layer 1() 2 on the glass substrate 1G6, which is deposited by bonding more light into the glass layer 1 〇 2: This AR coating _ reflection relief. The result is that when interfering with the facet, more incident light incidents can be made to interfere with the absorption mode to achieve a darker display state. This AR is plated on the !P column and still on the surface with the interferometric modulator array. ', can be deposited directly on the surface

1077A-4732A-PF 1318325 * 整合性糸 第1A圖亦顯示輔助光如何照射於一顯示器上。於此範 例中,顯Μ鏡用弧光燈陣列1 〇 4製造於玻璃層丄〇 2中。弧 光燈係光源的效率提供者。根據史實,弧光燈已經利用— 般燈泡的製造技術製造。此種燈的典型樣式已於美國專利 第4, 987, 496號中說明。製造—玻璃器皿,並且分別製造 的電極被包圍於玻璃器皿中。填充適當的氣體後,玻璃器 #皿被密封起來。雖然此燈泡可製造的很小,其製造方法可 能不適合製造大量的燈泡陣列。 用於製造微機電結構的技術可應用於製造顯微放電或 弧光燈。因為此種、'微型燈"的顯微大小,施加的電壓與 電流明顯的小於提供給以傳統方式製造的弧光燈的電壓盘 電流。於第U圖中的範例,可以製造陣列,藉由燈發射的 先113藉由本體的反射器& lu指引向干涉調制器陣列 108,其描述如下。 • 帛2圖對於此種燈做了詳細的描述,對於應用於平面 顯示器做了最佳化的製造。流程描述如下。如步^所示, 利用濕或乾化學㈣,㈣—玻璃層綱以便形成反射器 T狀物加。碗狀物的深度舆形狀藉由對於每—個光源需 ^面積與免度而決淺的碗狀物可產生寬廣的反射光 束分布,同時拋物狀可將反射光平行化。碗狀物的直徑變 =約自p1G微米至數百微米。此尺寸係藉由顯示器面積量 陳列^觀貝者的觀點可欣然的接受。亦必須考慮微型燈 1、密度。利用一般的沉積技術,例如滅鍍,以及標準1077A-4732A-PF 1318325 * Integration 糸 Figure 1A also shows how the auxiliary light is illuminated on a display. In this example, the illuminating mirror is fabricated in the glass layer 丄〇 2 using an arc lamp array 1 〇 4 . The efficiency of the arc lamp is the source of the light source. According to historical facts, arc lamps have been manufactured using the same bulb manufacturing technology. A typical style of such a lamp is described in U.S. Patent No. 4,987,496. Manufactured - glassware, and separately fabricated electrodes are enclosed in glassware. After filling the appropriate gas, the glassware is sealed. Although this bulb can be made very small, its manufacturing method may not be suitable for manufacturing a large number of bulb arrays. Techniques for fabricating microelectromechanical structures can be applied to the fabrication of microdischarge or arc lamps. Because of the microscopic size of such a 'micro lamp', the applied voltage and current are significantly less than the voltage plate current supplied to the arc lamp manufactured in the conventional manner. In the example of Figure U, an array can be fabricated, with the first 113 emitted by the lamp directed to the interferometric modulator array 108 by the reflector & lu of the body, as described below. • The 帛2 diagram provides a detailed description of the lamp and is optimized for use in flat panel displays. The process is described below. As shown in step ^, wet or dry chemistry (4), (4) - glass layer is used to form the reflector T. The depth 舆 shape of the bowl produces a broad reflected beam distribution by a shallower bowl for each light source and a parabolic shape, while the parabolic shape parallelizes the reflected light. The diameter of the bowl is changed from about p1G to several hundred microns. This size is readily accepted by the display area of the display area. Microlights must also be considered. 1. Density. Utilize general deposition techniques such as deplating, and standards

1077A-4732A-PF 1318325 二:影技術’沉積-反射器/複金屬I 2。4及犧牲層 形成既定圖案。此反射器/複金屬層可為一堆積薄 膜’其包括銘U射器)及複金屬,例如碘化 碘化銦。此禎Λ厲 f 灵金屬,並非必要的,可增加產生 此犧牲層可以是一層,例如石夕。 的特1 生 個八F1的堂^儿積電極層2〇6且形成既定圖案,以便形成兩 =開的電極。此材料可以是耐高溫金屬,例如鶴;並且 。有充分提供機械切的厚度,約為數千個埃單位。缺後 ;!^202 +者於玻璃板’例如基底(如帛1Α圖所示)上而密封,盆中 反射器面向該板。氣體,例如氤器,用以回填上述空:, =封燈泡步驟中形成,麗力大約為—大氣壓。這可以於 已事先充滿氣氣的密閉腔室中,執行密封步驟。 對於·^ @泡的電極施加充分的電壓將造成放電,於 兩電極末端之間的氣體,並且 、 哭?, 耵的先205朝向运離反射 二204的方向。假若閘間隔大約為數百個微米或更少,電 降低至數時伏特。假若電極材料沉積著少量的壓力, =2:將於碗狀物内決定電極的位置。於此範例中, 會造志雷炻田移除日守,應剩餘多少壓力, +成電極位私,那就決定了厚度以便補償位移。— s ,厚度將只是碗狀物深度的一 又 個微米。 ’大約為數個至數十 再一次參考第1A圖,顯示#、、儿— ^ . , 先/σ者路杈113行進。因此 先朝向干涉調制器陣列發射’在那极作用且依序藉由心 10 1318325 傷 沿著路徑110朝向介面107及觀察者111反射。 亦可以製造不具有反射器層的燈,因此其將全方位 射光。 具有或不具有反射器的燈可應用於需要顯微光源或顯 微,源陣列的地方。這可以包括投影顯示器、發射平面顯 不器的被光或内部(居家、房屋)的傳統光源或外部(汽車、 閃光燈)光源。1077A-4732A-PF 1318325 II: Shadow Technology 'Deposition-reflector/composite metal I 2. 4 and sacrificial layer form a defined pattern. The reflector/composite metal layer can be a stacked film 'which includes an ejector" and a complex metal such as iodide iodide. This is a strong metal, not necessary, can be increased. This sacrificial layer can be a layer, such as Shi Xi. The special electrode 1 has an electrode layer 2〇6 and forms a predetermined pattern to form two=open electrodes. This material can be a high temperature resistant metal such as a crane; and. There is a full thickness of mechanical cut, which is about several thousand angstroms. After the absence; !^202 + is sealed on a glass plate, such as a substrate (as shown in Figure 1), with the reflector in the basin facing the plate. A gas, such as a sputum, is used to backfill the above air:, = formed in the step of sealing the bulb, and the Lili is approximately - atmospheric pressure. This can be done in a sealed chamber that has been previously filled with air. Applying a sufficient voltage to the electrode of the ^^ bubble will cause a discharge, gas between the ends of the two electrodes, and crying? The first 205 of the crucible faces away from the direction of the reflection 204. If the gate interval is approximately a few hundred microns or less, the electricity is reduced to several volts. If the electrode material deposits a small amount of pressure, =2: the position of the electrode will be determined in the bowl. In this example, I will create a mine to remove the day guard, how much pressure should be left, and the electrode is private, then the thickness is determined to compensate for the displacement. — s , the thickness will be only a few microns deep in the depth of the bowl. ‘About several to tens of times. Referring again to Figure 1A, showing #,, 儿—^., first/σ path 113. Therefore, it is first directed toward the interferometric modulator array to act at that pole and is sequentially reflected by the heart 10 1318325 along the path 110 toward the interface 107 and the viewer 111. It is also possible to manufacture a lamp without a reflector layer so that it will illuminate in all directions. Lamps with or without reflectors can be used where micro light sources or subtle, source arrays are required. This may include a projection display, a light source that emits a flat panel display or a conventional light source for the interior (home, house) or an external (car, flash) light source.

參考第1B圖,顯示可選擇的輔助光方法。光導ιΐ8包 括-玻璃或塑膠層’其黏著於基们12。可包括任意種: 的發射源的光源U6,例如螢光燈、LED陣列或上述微型产 陣列,岐於光導的對立侧。光122使用—準直器12〇耗 合入光導’因此大部份的光經由内全反射捕捉於光導内。 散射塾鍍上—材料或薄膜堆積126,形成朝向基底⑴的 一反射表面以及朝向觀察者128的吸收表面。 當捕捉於光導内的光入射於散射塾上時,不再遵守内 全反㈣條件且某部份的光於全方位㈣。可垂直進入附 近介I的散射光,就是朝向觀察I 128的,由於 賴126而被反射進入基底Π2。類似上述的微型燈泡, 散社墊可以製作成陣列狀,每一 丨早列的尺寸如同顯示的部 位使得直視時幾乎無法查覺。當其尺寸相當小,約為十 個微米時,可提供充分的辅 ' 列1 U τ ^ . ,因為加上干涉調制器陣 下方’本身的光效率。散射墊的形狀 矩形或任意形狀’其可以降低觀察者的察覺。Referring to Figure 1B, an alternative auxiliary light method is shown. The light guide ι 8 includes a glass or plastic layer that adheres to the base 12 . Light source U6, such as a fluorescent lamp, an array of LEDs, or the above-described micro-production array, may be included in any of the following sources: on the opposite side of the light guide. The light 122 is collimated into the light guide using the collimator 12 so that most of the light is captured within the light guide via total internal reflection. The scattering iridium is plated - a material or film stack 126, forming a reflective surface facing the substrate (1) and an absorbing surface facing the viewer 128. When light trapped in the light guide is incident on the scattering ridge, the internal all-inverse (four) condition is no longer observed and some portion of the light is in all directions (four). The scattered light of the nearby medium I can be vertically entered, that is, toward the observation I 128, which is reflected into the substrate Π 2 due to the 134. Similar to the above-mentioned miniature light bulbs, the loose mats can be made in an array, and each of the early rows is as large as the displayed portion, making it almost impossible to detect when looking directly. When the size is quite small, about ten microns, a sufficient auxiliary 'column 1 U τ ^ . can be provided because of the light efficiency of the 'under the interferometric modulator array' itself. The shape of the scattering pad is rectangular or of any shape 'which reduces the perception of the viewer.

1077A-4732A-PF 11 1318325 _ 於陣列中的定址元件 為了啟動干涉調制器陣列,及為了顯示而協調的方 式,於陣列的行與列施加一連續的電壓,其中一般稱為、、時 間線方式。此基礎的觀念係對於特別行施加充分的電壓, 因此施加於被選擇的列的電壓造成,於被選擇的行上的單 元根據列電壓啟動或取消。臨界值以及施加的電壓必須 為〃有位於被選擇的行上面的單元受到施加的列電壓的 影響。藉由依序選擇包括於整個顯示器上的行,整個陣列 可以於一個週期時間内被定址。 一簡單完成的範例以顯示於第3圖中。磁滞曲線3〇〇 係反射式干涉調制器之電性反應之理想化表示。x軸表亍 施加的電壓,且y軸表示反射光的振幅。干涉調制器顯示 磁滯係因為,當增加電壓超過拉回臨界值時’啟動干涉調 :器::構且成為高吸收。當施加的電壓減少時,施加Π1077A-4732A-PF 11 1318325 _ Addressing elements in the array In order to activate the interferometric modulator array and coordinate for display, a continuous voltage is applied to the rows and columns of the array, generally referred to as the timeline . The underlying concept is to apply a sufficient voltage to a particular row, so that the voltage applied to the selected column causes the cells on the selected row to be initiated or cancelled according to the column voltage. The threshold and the applied voltage must be such that the cell above the selected row is affected by the applied column voltage. By sequentially selecting the rows included on the entire display, the entire array can be addressed in one cycle time. A simple completed example is shown in Figure 3. Hysteresis curve 3 is an idealized representation of the electrical response of a reflective interferometric modulator. The x-axis represents the applied voltage and the y-axis represents the amplitude of the reflected light. The interferometric modulator displays the hysteresis because, when the voltage is increased beyond the pullback threshold, the interferometer is activated and becomes highly absorbed. When the applied voltage is reduced, apply Π

拉回釋放臨界值,以便使結構恢復成未啟動狀態。 拉口與釋放臨界值之問Ml g1 和可… 磁滞窗。此磁滯效應, :::::統,已揭露於1 996年1…曰申請的美 丨申㉖案第08/744,253號,並且在此當作參考。任何 守』,磁滯窗可藉由維持一 干涉調制器吏用,以便使 對應於必續施也^ 成任何狀態。電壓¥。"與Von φ /、動或釋放干涉調制器結構的電壓。Μ 用電子設備藉由施加電&陣列利 驅動器。干涉調制器利用拉回臨界ΤΗ特:::為列與行 釋放臨界值為3伏_ ^ 伙特而製造,並且 伏特。對於如此的裳置,關於ν_,ν_Pull back the release threshold to return the structure to an unactivated state. Pull the mouth with the release threshold and ask for the Ml g1 and the... hysteresis window. This hysteresis effect, :::::, has been disclosed in the U.S. Patent Application Serial No. 08/744,253, the entire disclosure of which is hereby incorporated by reference. Any of the guards, the hysteresis window can be used by maintaining an interferometric modulator so that it corresponds to any state. Voltage ¥. " with Von φ /, moving or releasing the voltage of the interferometric modulator structure. Μ Using an electronic device by applying an electric & array driver. The interferometric modulator utilizes the pull back threshold::: is manufactured for column and row release thresholds of 3 volts _ ^ 特 , and volts. For such a skirt, about ν_, ν_

1077A-4732A-PF 12 1318325 的叙值分別為4· 5伏特、〇伏特及9伏特。 、? 圖中時間圖3 〇 2說明波形種類,可用以施加 ,動干"調制器陣列,顯示-磁滯曲線類曲線3 0 0。 、而要五種電壓,兩列電壓及三行電壓。被選擇的電壓, V。。"為兩倍的^值,並且為零伏特。行電壓被 广,因此Vs_與^之間的差額等於L,並且與 額等=的差額等於V°f”相反地,Vsein與L。11之間的差 ^ ’並且^⑴與Vc。丨。之間的差額等於V。"。 疋址發生於二選—的畫面0與i中。於一般的定址次 :關於行。的資料於畫面0期間被載入 i康:料::為二進位的-或零,導致施加一。的電 壓值。當資料結束時 u 1動态〇施加具有vse丨F0值的選擇 的脈衝。廷導致於列上 分紈私^ 〇 〃、有Vc。10的任何干涉調制器造成開 始啟動’並且於列上且右v — 〃、有的任何干涉調制器釋放。關 於下一仃的資料被载入列,並且_ _ 行,並且依序實施直到顯、、衝施加於該 且主J顯不态的最末一行。接 行〇開始定址,鋏而此日车6 丧考丹-人從 …、而此時,定址出現晝面i。 晝面之間的差異與資料及 & λλ泰 汉幻電壓之間的轉換相似,二 進位的零現在藉由VcQifl 、 v 、 乂及行選擇脈衝現在為 km。利用此技術,施加於 巧 每-畫面變化。這是肴用的”牲、歹’的整體電壓極性隨 一如田&心 0,特別對於以微機電為主的顯 不益,因為允許對於任何此值 ^ , 當只有施加單-極性電屡。於7曰長補知’廷會出現於 偏移干涉調制器或其它微機 H頁者的 挪电褒置的電性曲線。The values of 1077A-4732A-PF 12 1318325 are 4.5 volts, volts and 9 volts, respectively. Fig. 3 shows the type of waveform, which can be used to apply, dry "modulator array, display-hysteresis curve 3 0 0. There are five voltages, two columns of voltages and three rows of voltages. The voltage selected, V. . " is twice the value of ^ and is zero volts. The line voltage is wide, so the difference between Vs_ and ^ is equal to L, and the difference from the amount such as = is equal to V°f", the difference between Vsein and L.11 is ^' and ^(1) and Vc. The difference between the two is equal to V. " The address occurs in the screens 0 and i of the second choice. In general address: the line is loaded during the screen 0 i: material:: The binary - or zero, results in the application of a voltage value of 1. When the data is finished, u 1 dynamically applies a selected pulse with a value of vse F0. The result is that the column is separated from the other, with Vc. Any interfering modulator of 10 causes the start-up and is released on the column and right v-〃, any interfering modulator is released. The data about the next frame is loaded into the column, and the __ line is executed and sequentially executed until the display The rushing is applied to the last line of the main J. The 〇 〇 定 定 定 接 接 接 接 接 接 接 接 接 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 6 - - - - - - - - - - The difference between the data and the & λλ Thai Han magic voltage is similar, the binary zero is now by VcQifl, v, 乂The selection pulse is now km. Using this technique, it is applied to every screen-variation. This is the overall voltage polarity of the "Essence, 歹" used with the same as the field & heart 0, especially for MEMS-based display Not helpful, because for any such value ^, when only a single-polarity is applied. At 7 曰 补 ’ ’ 廷 廷 廷 廷 廷 廷 廷 廷 廷 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移 偏移

1077A-4732A-PF 13 1318325 彩色顯 能裳置H /八周制器係一具有各種可能的光學響應的多功 ;;;能的、二彩色顯示圖像可具有不同的特性。-#丨具有一部份的干涉調制器設計,相同 =制器可以獲得彩色狀態、黑色狀態及白色狀態。 此可月&性可用ιν # β, &侍彩色的圖像,可以、、底色+顏料。用 =係因為,此方法類似緣畫上色,其藉由增加顏料: 白底色以便雜溫兩通 而要的色彩而產生。利用此方法,特別的 得=光譜中的顏色,並且藉由控制顏料加入底 、刀與3里獲得需要的飽和度。此方法可構成具有彩 邑、…、色及白色像素的顯示器。 =第4A圖所示像素_包括五個次像素單元術、 6、彻,每-次像素可分別反射紅色、綠色、藍色 及白色。所有的次像素可以產生黑狀態。每—次 利用脈衝寬度調制而完成,相關技術已揭露於美 〇 ' 5, 835,255號。同時適當的選擇相關次像素大 Π導致像素整體具有非常大程度的控制亮度與L ^列如’藉由減少白色次像素之總亮度,可獲 地餘和色彩。相反地1由減少彩色次像素之亮度,J 由同時將其與白色次像素最大化,可獲得明顯的黑與二 式。中間的所有變化可輕易地獲得。 使—用者控制的彩色圖偉_ 如上所述的彩色圖像, s 4疫 口课,就解析度、灰階程度以及清晰1077A-4732A-PF 13 1318325 Color-capable H/eight-week system is a multi-function with various possible optical responses;;; two-color display images can have different characteristics. -#丨 has a part of the interferometric modulator design, the same = the device can get the color state, black state and white state. This can be used for the month & ιν #β, & color image, can, background color + pigment. With the = system, this method is similar to the coloring of the edge, which is produced by adding the color of the pigment: white background to the mixed temperature. Using this method, the color in the spectrum is specifically obtained, and the desired saturation is obtained by controlling the addition of the pigment to the bottom, the knife and the 3rd. This method can constitute a display with color, ..., color and white pixels. = The pixel _ shown in Fig. 4A includes five sub-pixel units, 6, and the per-pixel can reflect red, green, blue, and white, respectively. All sub-pixels can produce a black state. Each time is completed using pulse width modulation, and the related art has been disclosed in the United States '5, 835, 255. At the same time, the appropriate selection of the relevant sub-pixels causes the pixel as a whole to have a very large degree of control brightness and L^column, such as by reducing the total brightness of the white sub-pixels, to obtain the balance and color. Conversely, by reducing the brightness of the color sub-pixels, and by maximizing them with the white sub-pixels at the same time, significant black and two modes can be obtained. All changes in the middle can be easily obtained. Color image of user-controlled _ color image as described above, s 4 epidemic class, resolution, grayscale degree and clarity

1077A-4732A-PF 14 1318325 Μ 度而言,如同以干涉調制器為主的顯示器之本質特性 供更玻活的顯示性能。為 在此乾圍内,可有效的提供使用者 超越一般特性的顯示控制的產品。或者,關於顯示的 功此係自動地適應不同觀賞需要。 、 例如,假如一此文耷,口 要#用字,使用者可能想 要使用黑白換式的產品。然而,另一種狀況,使用者可能 想要觀看南品質的彩色靜態影像,或者於另一種模, 觀看動態晝面。這類的每一個模式,於提供的干涉調制器 顯㈣態範圍内,盡可能地需要特別屬性的交換。交換包 括,假若需要高解析度的晝面,需要低更新率;假若 要黑與白,有能力獲得高度灰階。 為了給予使用者此種彈性的兩 裡坪阻的而求,控制器硬體可重新 配置至某種程度。根據事實,任何顯干A ώ w 1 顯不只具有某種波段寬 度;基本上係受像素單元之響應時間限制,並且因此決定 於既定時間内可被顯示的資訊量。 可以提供此種彈性的一顯示架構已說明於第4B圖 中。於此方塊圖中’利用各種IC技術之—執行控制器邏輯 操作412,包括可程式的邏輯元件以及場可程式間極陣列 (FPGAs)’提供改變元件的功能或出貨後可重新設^。這類 的元件,一般用於特別的應用’例如數位信號處理或影像 壓縮,料這類的處理可提供高品質,於產品設計階段加 入使用迫類的元件同時提供了彈性。 此控制器412對於定址顯示418提供信號及資料至驅 動電子轉4U與416。習知的控制係根據ΐ(:或應用特性1077A-4732A-PF 14 1318325 In terms of temperature, it is like the nature of an interferometer-based display for more vivid display performance. For this purpose, it is possible to effectively provide users with display control that exceeds the general characteristics. Alternatively, the display is automatically adapted to different viewing needs. For example, if the text is used, the user may want to use a black-and-white model. However, in another situation, the user may want to view a south-quality color still image, or in another mode, watch the dynamic face. Each of these modes requires the exchange of special attributes as much as possible within the range of the provided interferometric modulators. Exchanging, if a high-resolution face is required, requires a low update rate; if it is black and white, it has the ability to achieve a high gray level. In order to give the user the flexibility of two inches, the controller hardware can be reconfigured to some extent. According to the fact, any significant A ώ w 1 shows not only a certain band width; it is basically limited by the response time of the pixel unit, and therefore determines the amount of information that can be displayed in a given time. A display architecture that can provide such flexibility has been illustrated in Figure 4B. In this block diagram, 'execution of controller logic operations 412, including programmable logic elements and field programmable inter-array arrays (FPGAs)', provides the ability to change components or can be re-set after shipment. Components of this type are typically used for special applications such as digital signal processing or image compression. This type of processing provides high quality and adds flexibility to the use of compelling components during the product design phase. The controller 412 provides signals and data to the drive electronics 4U and 416 for the address display 418. The conventional control system is based on ΐ (: or application characteristics)

1077A-4732A-PF 15 1318325 4 積體電路(ASICs),於製造期間藉 訂程式〃。於此範例中,逐侔=广效有效地、'制 心你的%序表示,句杯批1077A-4732A-PF 15 1318325 4 Integrated Circuits (ASICs), which are borrowed during manufacturing. In this example, 侔 侔 = 广 有效 广 广 广 广 广 广 你 你 你 你 你 你 你 你 你 你 你

::Γ之更内高广層的邏輯元件(邏輯問極及邏輯模組娜配 :)内广片佈局。藉由使用場可程式元件,例如PLAS 二:,於硬體應用型式或硬體應用中,不同的顯示 设疋可自一元件410,像是印愔舻七 财I w^ 體或白知具有記憶體的:: Γ 更 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高 高By using field programmable components, such as PLAS II: in hardware applications or hardware applications, different display settings can be from a component 410, such as the Indiana IW^ or Baizhi. Memory

載人顯示控制元件。記憶體可以為刪0MS型 式或其它可程式的儲存元件;並且微處理器可採用簡易的 微控制器型式,其功能係用以自記憶體將大量應用載入 FPGA’除了處理器處理產品的一般功能之外。此方法之優 點在於’ m為具有相關簡易的電路圖’與其結合可以獲得 寬廣的各種不同顯示功能設定以及混合的顯示掃描率。 例如,螢幕之一部份可能以低階解析度顯示文字晝 面,同時另一個提供高品質的接收電子郵件顯示。這可以 於顯不器之整體頻帶寬度範圍内,藉由對於顯示器的不同 區域變化掃描的顯示率而完成。低階解析度文字區域可以 快速掃描,並且只有扭當於一個或兩個的—或兩個位元之 灰階浪度。高解析度電子郵件區域可以快速地掃描,並且 相當於二個或四個的三或四個位元之灰階。Manned display control elements. The memory can be deleted from the 0MS type or other programmable storage elements; and the microprocessor can be used in a simple microcontroller type, the function is to load a large number of applications from the memory into the FPGA 'except the processor processing products Beyond the function. The advantage of this method is that 'm is a circuit diagram with a related ease' combined with it to achieve a wide variety of different display function settings and mixed display scan rates. For example, one part of the screen may display text in low-level resolution while the other provides high-quality receiving email display. This can be done over the overall bandwidth of the display by varying the display rate of the scan for different areas of the display. The low-order resolution text area can be scanned quickly and only if it is one or two—or two bits of grayscale volatility. High-resolution email areas can be scanned quickly and are equivalent to two or four three- or four-bit grayscales.

此構想廣義的包括,不只是顯示控制器的功能,更包 括整體產品的功能。第4C圖顯示,般可攜式電子產品41 8 之°又疋’其具有可程式的邏輯元件或於其核心420的同等 1077Α-4732A-PF 16 1318325 4 物。於許多顯示中心 ^ , v R ^ 個人電子產,例如PDAs(個人數位 .τςΓ . φ ^事本’中央處理器係-不同版本的 = 其使用更少的指令組。當處理器係更 ΓΓ 本時’提升更多個人電腦之功能,其仍然 為一般功能的處理器,耗費許多能量執行重複的工作,例 如擷取來自記憶體的指令。This concept broadly includes, not only, the functionality of the display controller, but also the functionality of the overall product. Figure 4C shows that the portable electronic product 41 8 has a programmable logic element or an equivalent 1077Α-4732A-PF 16 1318325 4 at its core 420. In many display centers ^, v R ^ personal electronics, such as PDAs (personal digits. τςΓ. φ ^books' central processor system - different versions = it uses fewer instruction sets. When the processor is more ΓΓ At the time of 'improving the functionality of more personal computers, it is still a general-purpose processor that consumes a lot of energy to perform repetitive tasks, such as capturing instructions from memory.

於個人電腦_,能量消耗量並不是問題,並且使用者 -般想要執行許多複雜的應用軟體。此相對觀點對於一般 ㈤中心個人電子產品而言是正確的。需要消耗低能量, f且提供相當少量的相對簡易的程式。此種制度有利於執 仃特別功旎的程式’例如包括網路瀏覽器、行事曆、繪圖 程式、電活/定址資料庫以及手寫/語音辨識,當作一硬體 應用。因此當使用者需要執行—特別功能模式,例如一程 f ’核心處理器隨著硬體應用更改設定,並且使用者與產 動因此此硬體應用的處理器,顯示於其内部邏輯 #作與連結中的各種場可程式閘陣列具有&困難應用(即 程式),當載入一個新的硬體應用就重新配置與寫入。此元 件的許多供應者亦提供應用發展系統’其允許特定程式語 5 ( —硬體敘述語言),以便被減少成邏輯表示,其製造了 適當的處理器。許多的功能亦進行簡化處理或減少更高階 程式語言成為此種型式。實現此處理器的一種方法已於For personal computers, energy consumption is not an issue, and users want to perform many complex applications. This relative view is correct for general (5) central personal electronic products. It requires low energy consumption and provides a relatively small amount of relatively simple program. Such a system facilitates the execution of special programs such as web browsers, calendars, drawing programs, live/addressed databases, and handwriting/voice recognition as a hardware application. Therefore, when the user needs to perform a special function mode, for example, a pass f 'core processor changes settings with the hardware application, and the user and the processor that is the hardware application are displayed in the internal logic # The various field programmable gate arrays in the link have & difficult applications (ie, programs) that are reconfigured and written when a new hardware application is loaded. Many providers of this component also provide application development systems that allow specific programming language 5 (-hardware narration language) to be reduced to a logical representation that creates the appropriate processor. Many of the functions are also simplified or reduced to higher-level programming languages. One way to implement this processor is

Kouichi Nagami 等人的於 1 998 年於 Proc. IEEE Workshop on FPGA based Custom Computing Mechines 之論文Kouichi Nagami et al., Proc. IEEE Workshop on FPGA based Custom Computing Mechines, 1998

Plastic Cell Architecture : Towards Reconfigurab 1 ePlastic Cell Architecture : Towards Reconfigurab 1 e

1077A-4732A-PF 17 1318325 虡1077A-4732A-PF 17 1318325 虡

Computing for General_purp〇se/’ 揭露。 再_人參考第4C圖’此硬體應用處理器420顯示於一 堆的I/O το件與電腦週邊產品之中央,其將根據目前載入 的硬體應用之功能及特性而使用、修飾或不理會。此硬體 應用可自存在於產品内的記憶體422或經由RF或IR介面 ,:外部資源載入’就是可自網路、蜂巢式網路或其它 電子裝置汲取具有特別硬體應用的應用内容。硬體應用之 另一種例子,關於音響介面432係包括聲音識別或語音合 成規則系統’關於手寫輪入426包括手寫辨識規則系統以 及關於影像輸人裝f 43〇包括影像壓縮與處理模式。此類 的產品可藉由其主要部位之功效執行大量的㈣,顯示器 當:主要使用者介面以及可更改設定核心處理器。藉由與 目前產品之數百毫瓦特比較,關於這類元件之整體功率總 合大約為數十毫瓦特等級。 從光學觀點鮮叙機雷翻赴 於1 996年12 $ 19曰申請的美國專利申請案第 〇8觸,947號,以及於1 998年4月4日巾請的美國專利 申請案第隨56,975號,在此提供參考,其已揭露干涉調 驗計’提議自其光學功能退轉干涉調制器之機電功 此。另一種方法,可藉由第5A圖與帛5β圖所描述的完成。 計利用靜電力量改變干涉空穴的幾何。電極502係製 造上,並且藉由絕緣薄膜5〇4與膜狀物/鏡面 “生阻隔。電極502之功能只有當作電極使用,並未Computing for General_purp〇se/’ exposes. Referring to FIG. 4C, the hardware application processor 420 is displayed in the middle of a stack of I/Os and computer peripheral products, which will be used and modified according to the functions and characteristics of the currently loaded hardware applications. Or ignore it. This hardware application can be self-existing in the memory 422 in the product or via the RF or IR interface: external resource loading 'is to extract application content with special hardware applications from the network, cellular network or other electronic devices . Another example of a hardware application is that the audio interface 432 includes a voice recognition or speech synthesis rule system. The handwriting wheel entry 426 includes a handwriting recognition rule system and an image compression and processing mode. Such products can perform a large number of (4) functions by their main parts, and the display is: the main user interface and the settable core processor can be changed. By combining hundreds of milliwatts of current products, the overall power mix for such components is on the order of tens of milliwatts. From the optical point of view, the singularity of the U.S. Patent Application No. 触8, No. 947, and the U.S. Patent Application No. 56,975, filed on April 4, 998. Reference is provided herein, which has disclosed that the interference calibrator's proposed electromechanical work from its optical function to reverse the interferometric modulator. Another method can be accomplished by the description of Figure 5A and Figure 5β. The use of electrostatic forces changes the geometry of the interfering holes. The electrode 502 is fabricated and is "blocked" by the insulating film 5〇4 and the film/mirror. The function of the electrode 502 is only used as an electrode, and

J077A-4732A-PF 18 1318325 m 當作鏡面使用。 光學空穴505形成於薄膜/鏡面506與第二鏡面5〇8之 間。關於第二鏡自508的支撐物係一透明的上部構造川, 其可以為-厚沉積有機物,例如、聚硫亞氨或—盈機 材料。於製造期間藉由犧牲層決定,未施加電塵時,如第 =圖所示’相對於第二鏡面508,薄膜/鏡面邮維持一既 疋位置。數千埃的厚度適用於大約四伏特的啟動電屢。假 若第二鏡面以適當的材料製造,例如鉻,且鏡面/薄膜以反 射材料製造’例如紹;則此結構將反射可被觀察者512感 知的既定頻率光川。此外,假若鉻大約4〇埃,薄到半透 明,以及鋁相當的薄,至少5〇〇 ^ 3υυ埃且不透光,則此結構可 具有寬廣的各式光響應。第5(:圖 口兴乐圖,分別顯示黑 白及Μ的響應’皆藉由空穴長度及構成層的厚度決定。 第5Β圖顯示於主電極502及薄膜鏡面5〇6之間施加電 壓的結果。垂直的設置此薄膜/鏡面,因此改變光學空穴的 =及干涉調制器之光學特性。第5C圖顯卜種反射光 子響應,可具有兩種狀態,當裝 ,9t ^ 田哀置70全啟動時說明黑狀態 以置未啟動時係白狀態。第5D圖顯禾具有色彩峰 值挪、527及529的光學響應,分別相當於藍色、綠色及 :色:因此裝置的機電操作狀態可與其光學性能分開地控 二鏡面的材料;因為其不且;;::’可選擇不包含第 有干涉§周制器之光學功能。此 ^可利用表面微機械之步驟與技術製造 於1996年7月31a由匕揭路 申印的美國專利申請案第08/688,71 0J077A-4732A-PF 18 1318325 m Used as a mirror. An optical cavity 505 is formed between the film/mirror 506 and the second mirror 5〇8. The support for the second mirror from 508 is a transparent superstructure, which may be a thick deposit of organic matter, such as polysulfide or a slewing material. The film/mirror is maintained at an adjacent position relative to the second mirror 508 as determined by the sacrificial layer during the manufacturing process by the sacrificial layer. The thickness of several thousand angstroms is suitable for starting power of approximately four volts. If the second mirror is made of a suitable material, such as chrome, and the mirror/film is made of a reflective material, the structure will reflect a given frequency of light that can be perceived by the observer 512. In addition, if the chromium is about 4 angstroms, thin to semi-transparent, and aluminum is relatively thin, at least 5 〇〇 ^ 3 angstroms and opaque, the structure can have a wide variety of photoresponses. The fifth (: 口口兴乐图, respectively showing the response of black and white and Μ) is determined by the length of the hole and the thickness of the constituent layer. Figure 5 shows the application of voltage between the main electrode 502 and the film mirror 5〇6. As a result, the film/mirror is vertically disposed, thus changing the optical hole = and the optical characteristics of the interferometric modulator. Figure 5C shows the reflected photon response, which can have two states, when loaded, 9t ^ Tian Ai 70 The black state is fully activated to set the white state when it is not activated. The 5D figure shows the optical response of color peak shift, 527 and 529, which are equivalent to blue, green and color: respectively, so the electromechanical operation state of the device can be The material of the two mirrors is controlled separately from its optical properties; because it does not;;::' can choose not to include the optical function of the first interference § circumstance. This can be fabricated in 1996 using the steps and techniques of surface micromechanics. U.S. Patent Application Serial No. 08/688, 71 0, issued July 31, 31

1077A-4732A-PF 19 1318325 號,並在此列入參考。 於另一個範例中,顯示於第6A圖中,關於干涉調制器 之支撐物結構設置於適當位置,以便藉由薄膜/鏡面 -608而隱藏。於此方法,不起作用的區域數量有效地降低, 因為觀察者只看見藉由薄膜/鏡面覆蓋的區域以及鄰接的 干涉調制器之間的最小間隔。此不像第5A圖中,從彩色觀 點,薄膜支撐物為透明且構成不起作用的結構。第6β圖, φ 於啟動狀態中揭露相同的結構。 於第7A圖_,揭露應用於一干涉調制器結構的另—種 幾何配置。此設計相似於揭露於美國專利案第5,638,〇84 號。此設計係利用透明的塑膠薄膜,其係各向異性地伸張, 因此自然地以捲曲狀態存在。施加電壓使薄膜平坦化,當 作微機電遮光器。 w 此裝置的功能可藉由使其干涉而改善。於第u圖中 的干涉調制器變化,其中薄膜堆積7〇4為介電…導電層/ •絕緣層,係1 996年7月31日申請美國專利申請案第 08/688’ 710號揭露的感應式吸收干涉調制器設計之主要部 份’在此列入參考。 於鋁薄膜702及堆積層704之間施加的電壓造成薄膜 702相對於堆積層呈現平坦狀。於製造時,鋁亦包括 其它反射的金屬(銀、銅、鎳)’或於介電材料或於有機材 料内層鍍上反射金屬,設置於一薄犧牲層上,犧牲層可利 用濕蝕刻或氣體相位移除技術被移除。鋁薄膜7〇2 半 以機械方式藉由—支撐調整片716固定於基底,其係直^1077A-4732A-PF 19 1318325 and is incorporated herein by reference. In another example, shown in Figure 6A, the support structure for the interferometric modulator is placed in position to be hidden by the film/mirror-608. In this way, the number of inactive regions is effectively reduced because the viewer only sees the area covered by the film/mirror and the minimum spacing between adjacent interferometric modulators. This is not the case in Fig. 5A. From the viewpoint of color, the film support is transparent and constitutes a structure that does not function. In the 6th figure, φ exposes the same structure in the startup state. In Figure 7A, another geometric configuration applied to an interferometric modulator structure is disclosed. This design is similar to that disclosed in U.S. Patent No. 5,638, No. 84. This design utilizes a transparent plastic film that stretches anisotropically and thus naturally exists in a curled state. A voltage is applied to flatten the film as a microelectromechanical shutter. w The function of this device can be improved by interfering with it. The variation of the interferometric modulator in Fig. u, wherein the film stack 7 〇 4 is a dielectric ... conductive layer / • insulating layer, which is disclosed in U.S. Patent Application Serial No. 08/688, filed on Jul. 31, 1976. The main part of the design of inductive absorption interferometric modulators is listed here. The voltage applied between the aluminum film 702 and the buildup layer 704 causes the film 702 to assume a flat shape relative to the buildup layer. At the time of manufacture, aluminum also includes other reflective metals (silver, copper, nickel)' or is plated with a reflective material in a dielectric material or an inner layer of an organic material, disposed on a thin sacrificial layer, which may utilize wet etching or gas The phase removal technique was removed. The aluminum film 7〇2 half is mechanically fixed to the substrate by the support tab 716, which is straightened ^

1077A-4732A-PF 20 1318325 * /儿積於光學堆積層704上。因為如此,入射於調整片及堆 •積層上的區域的光被吸收,使得此機械方式不起作用的區 域於光學方面不起作用。於此範例及其他干涉調制器設計 . 令,此技術消除分散的黑色遮蔽物。 w 入射光706不是完全被吸收,就是根據堆積層的間隔 使部份頻率的光708被反射。此光學作用就是於1 996年7 月31日申請的美國專利申請案第〇8/688,71 〇號所揭露的 •感應式吸收的干涉調制器,在此列入參考。 .第7β圖顯示當未施加電壓時的裝置狀況。於薄膜中的 殘留應力造成其捲曲成緊密的捲區狀。剩餘應力可藉由於 薄膜上方沉積一薄材料層718而產生,其具有相當高的殘 留,力。鉻係一使用範例,其中薄膜厚度減少至數百埃可 獲得高應力。隨著薄膜不再遮擋其光路徑,可允許光束 通過堆積層704且貫穿此平板71〇。平板71〇可存在於不 是高度吸收就是高度反射(既定色彩或白光)的狀態。關於 使用於反射式顯示n中的調制器’光學堆積層7Q4可設計 成,當襄置啟動時,可反射既定色彩(假若平板71〇係吸收) 或者吸收(假若平板710為反射狀態)。 兹A式啟動 如第8A圖所示,另一種干涉調制器幾何結構係以旋轉 Μ啟I利用於1 996年7月31日中請的美國專利申請 案第08/688, 71 0號中揭露地步驟且在此列入參考,電極 8〇2、約1_埃厚度的銘薄膜形成於基底上。設置支1077A-4732A-PF 20 1318325 * / is accumulated on the optical buildup layer 704. Because of this, the light incident on the area of the tab and the stack is absorbed, so that this mechanically inactive area does not function optically. This example and other interferometric modulator designs. This technique eliminates scattered black masks. w The incident light 706 is not completely absorbed, or a portion of the frequency of light 708 is reflected according to the spacing of the deposited layers. This optical effect is an inductively absorbing interferometric modulator as disclosed in U.S. Patent Application Serial No. 8/688,71, filed on Jan. 31, s. The 7th figure shows the condition of the device when no voltage is applied. The residual stress in the film causes it to curl into a tight roll shape. The residual stress can be generated by depositing a thin layer of material 718 over the film, which has a relatively high residual force. An example of the use of chromium, in which the film thickness is reduced to hundreds of angstroms to obtain high stress. As the film no longer obscures its light path, the beam can be allowed to pass through the buildup layer 704 and through the plate 71. The flat plate 71 can exist in a state of not being highly absorbed or highly reflective (constant color or white light). Regarding the modulator used in the reflective display n, the optical buildup layer 7Q4 can be designed to reflect a predetermined color (if the plate 71 is absorbed) or absorbed (if the plate 710 is in a reflective state) when the device is activated. A type A start is shown in Fig. 8A, and another type of interferometric modulator structure is disclosed in U.S. Patent Application Serial No. 08/688, No. 71, the entire disclosure of which is incorporated herein by reference. The ground step and incorporated herein by reference, the electrode 8 〇 2, about 1 angstrom thickness of the film is formed on the substrate. Setting up

1077A-4732A-PF 21 1318325 撐棒808及旋轉樞紐81。、支撐遮光器8i2及其上的反射 薄膜813。支揮遮光器可為—㈣膜’其具有數千埃厚度。 .其χ-γ尺寸為數十至數百微米。此薄膜可為干涉式且設計 •成用以反射既定色彩。在此當作參考的1 996年7月31日 申請的美國專財請㈣G8觸,m號揭露了,感應吸收 型式的固定干涉堆疊層。其亦可包括浸泡彩色染料的聚合 物,或者為銘或銀以便提供寬波段反射。設計電極及 •遮光器812,因此於兩者之間施加電壓(例如1 0伏特)將造 成遮光器812以旋轉樞紐軸部份或完全旋轉。一個遮光器 818顯示於轉動狀態,一般而言,對於一已知的像素,所 有的遮光器將-起藉由位於共同匯流排電極8〇4的信號而 驅動。此遮光器將經歷機電磁滞現象,假若設計旋轉樞紐 與電極距離使得電極的靜電吸引力,於旋轉期間超過旋轉 樞紐的彈簧張力。遮光器將因此具有兩個電機穩定狀態。 於穿透模式的操作中,遮光器不是遮擋入射光就是允 籲3午其通過。第8A圖說明反射模式,其中入射光822被反射 回觀察者820。於此模式之一個狀態中,假若遮光器是金 屬製造,遮光器將反射白光,或假若遮光器鍍上干涉薄膜 或染料,遮光器將反射既定色彩或一組色彩。關於干涉堆 積層之描述的厚度及產生的顏色,亦已揭露於1 996年7月 31日申請的美國專利申請案第08/688, 71 0號,並且在此 列入參考。於另一個狀態中,允許光通過並且被基底8〇〇 吸收’假如遮光器的對立面鍍上吸收薄膜或薄膜722。此 薄膜可包括另一種染料浸泡有機薄膜,或設計用來吸收的1077A-4732A-PF 21 1318325 Strut 808 and rotating joint 81. The shutter 8i2 and the reflective film 813 thereon are supported. The fulcrum shutter can be - (iv) film 'having a thickness of several thousand angstroms. Its χ-γ size is tens to hundreds of microns. The film can be interferometric and designed to reflect a given color. As for reference, July 31, 1996, the application for the US special account (4) G8 touch, m revealed, the induction absorption type of fixed interference stacking layer. It may also include a polymer immersed in a color dye, or inscription or silver to provide wide band reflection. The electrodes and the shutter 812 are designed such that applying a voltage between them (e.g., 10 volts) will cause the shutter 812 to partially or fully rotate the rotating hinge shaft. A shutter 818 is shown in a rotated state. Generally, for a known pixel, all of the shutters will be driven by signals located at the common bus bar electrodes 8〇4. This shutter will experience electromagnetic hysteresis, if the distance between the rotating hub and the electrode is designed such that the electrostatic attraction of the electrode exceeds the spring tension of the rotating hub during rotation. The shutter will therefore have two motor steady states. In the operation of the penetrating mode, the shutter does not block the incident light or allows it to pass through at 3 o'clock. Figure 8A illustrates a reflection mode in which incident light 822 is reflected back to viewer 820. In one state of this mode, if the shutter is made of metal, the shutter will reflect white light, or if the shutter is coated with an interference film or dye, the shutter will reflect a given color or a set of colors. The thickness of the description of the interference stack and the resulting color are also disclosed in U.S. Patent Application Serial No. 08/688, the entire disclosure of which is incorporated herein by reference. In another state, light is allowed to pass through and is absorbed by the substrate 8' if the opposite side of the shutter is plated with an absorbent film or film 722. The film may comprise another dye soaked organic film or designed to be absorbed

1077A-4732A-PF 22 1318325 感應吸收堆積層。相反地,遮光器將高度地吸收,就是 呈現黑色,並且基底800鍍上高反射薄膜824,或者沿著 上所述的彩色反射薄膜線選擇性地鍍上具有染料薄膜戋 干涉薄膜以便反射色彩。 '一 凌置的操作可進一步藉由加入輔助電極814而改善, 2對於遮光器提供額外的力矩,當充電至―電位,於輔助 电才° 814與遮光益812之間感應產生靜電吸引力。輔助電 極814包括導體814與支摔結構816的結合體。電極包括 透明V體’例如IT〇 ’其大約為數千埃厚度。所有的結 構與相關電極皆利用材料以機械製造,其沉㈣―單一基 底之表面上’例如一單石面板;並且因此輕易地製造及由 於良好的控制電極間隔距離可讀實地啟動。例如,假若電 2 =㈣立基底上’裝置基底與對立基底兩者的表面變 化可結合成產生至多數個 ^ ^ ^ r- 被未的偏差。如此,需要影響既 广電整可藉由數十伏特而改變。單石的結構隨著 基底表面準確地變化’並且產生微量變化。 第8β圖顯示關於旋轉調制器的製造流程,步驟!至7。 於步驟1中,基底83G已經鑛上電極832及絕緣體834。 一般的電極及絕緣體材料為銘及二氧切,每一個厚度八 別為一千埃。這些於步驟2 又刀 ―材料,例如數個;^㈣u 間隔836係 圖案;接著於步驟4令铲上耘早"… 匕積且形成 ⑽。這約為埃厚度㈣人;^疋轉框组/遮光器材料 中,材料838已經形成:宰二、或鈦/鶴合金。於步驟5 成圖案以便形成匯流排電極844、支1077A-4732A-PF 22 1318325 Inductive absorption stack. Conversely, the shutter will be highly absorbed, i.e., appear black, and the substrate 800 is plated with a highly reflective film 824 or selectively coated with a dye film 干涉 interference film along the colored reflective film lines described above to reflect color. The operation of a ping can be further improved by the addition of the auxiliary electrode 814. 2 provides an additional torque to the shutter, and when charged to the "potential," an electrostatic attraction is induced between the auxiliary Δ814 and the shading 812. Auxiliary electrode 814 includes a combination of conductor 814 and breakout structure 816. The electrode comprises a transparent V body 'e.g. IT 〇 ' which is approximately several thousand angstroms thick. All of the structures and associated electrodes are mechanically fabricated from materials, which are on the surface of a single substrate, such as a single stone panel; and are therefore easily fabricated and readable and readable by good control electrode spacing distances. For example, if the surface change of both the device substrate and the counter substrate on the substrate 2 = (d), the substrate can be combined to produce a deviation of a majority of ^ ^ ^ r-. In this way, the need to influence the wide range of electricity can be changed by tens of volts. The structure of the monolith varies exactly with the surface of the substrate' and produces a slight change. The 8th figure shows the manufacturing process, steps for the rotary modulator! To 7. In step 1, the substrate 83G has the upper electrode 832 and the insulator 834. The general electrode and insulator materials are Ming and Dioxo, each of which is one thousand angstroms in thickness. These are in step 2 - the material - for example, several; ^ (four) u interval 836 system pattern; then in step 4, the shovel is smashed early "... hoarding and forming (10). This is about angstrom thickness (four) person; ^ 疋 turn frame group / shutter material, material 838 has been formed: slaughter two, or titanium / crane alloy. Patterned in step 5 to form bus bar electrodes 844, branches

1077A-4732A-PF 23 1318325 _ 撐柱840及遮光器842。於步驟6中,遮光反射器846已 I被>儿積且形成圖案。於步驟7 +,犧牲間隔已被蝕刻移 除產生&整的結構。步冑7亦揭示結構的上視圖,詳細顯 示包括支撐柱848、扭力臂85〇及遮光器852的旋轉樞紐。 切換元# 關於干涉調制器’其係二位元裝置,π需要少量電壓 籲即可以驅動顯不。驅動電子元件不需要產生類比訊號,可 獲得灰階操作。 因此,電子元件可利用於1 996年12月19日申請的美 國專利申請案第08/769, 947號建議的裝置而執行使用,該 篇申明案在此列入參考。此外,驅動電子元件及邏輯功能 可利用微機電的切換元件而執行使用。 第9Α圖至第9Ε圖說明此觀念。第9Α圖係一基礎切換 鬼圖/…、有輸入端9 〇 0,藉由施加一控制信號9 〇 2 •而連結至輸出端904。第肿圖說明一行驅動器如何執行使 用。用於如上所述的定址結構的行驅動器需要輸出三種電 壓值。施加適當的控制信號至行驅動器,允許一輸入電壓 值選擇提供給輸出端903。輸入電壓為Vccn、Vc。,。及Vhs, 於圖中對應於906、908及910。相同地,關於顯示於第9C 圖中的列驅動器,適當的控制信號造成選擇—個或其它電 壓值,傳輸至輸出端92〇。此輪入電壓為Vsein、Vs⑴。及接 地’對應於圖中的914、916及918。第9D圖說明邏輯裝 置932如何使用,於此範例中,一 MND閘極利用基礎切換1077A-4732A-PF 23 1318325 _ struts 840 and shutters 842. In step 6, the shading reflector 846 has been <> and patterned. In step 7 +, the sacrificial interval has been etched away to produce & the entire structure. Step 7 also reveals a top view of the structure showing in detail the pivotal hub including support post 848, torsion arm 85〇 and shutter 852. Switching element # About the interferometric modulator' is a two-bit device, π requires a small amount of voltage to drive the display. The drive electronics do not need to generate analog signals to achieve grayscale operation. Thus, the use of electronic components can be carried out using the apparatus proposed in U.S. Patent Application Serial No. 08/769,947, filed on Dec. 19, 1996, which is incorporated herein by reference. In addition, the drive electronics and logic functions can be implemented using MEMS switching elements. Figures 9 through 9 illustrate this concept. The ninth diagram is a basic switching ghost diagram/... with an input 9 〇 0 coupled to the output 904 by applying a control signal 9 〇 2 •. The first swollen map shows how a row of drives performs. A row driver for the addressing structure as described above needs to output three voltage values. Applying an appropriate control signal to the row driver allows an input voltage value selection to be provided to output 903. The input voltage is Vccn, Vc. ,. And Vhs, corresponding to 906, 908 and 910 in the figure. Similarly, with respect to the column drivers shown in Figure 9C, the appropriate control signals cause a selected one or other voltage value to be transmitted to output 92. This wheeling voltage is Vsein, Vs (1). And ground' corresponds to 914, 916 and 918 in the figure. Figure 9D illustrates how the logic device 932 is used. In this example, an MND gate utilizes a basic switch.

1077A-4732A-PF 24 1318325 鬼—934 936、938及940。所有的元件可以此方法配置 :結合’其提供於第卯圖中顯示的顯示次系統之製造。此 人系、為包括控制邏輯926、行驅動器924、列驅動器以 及,.、,員不陣列93〇,並且使用如第3圖所描述的定址結構。 此切換兀件之製造,例如微機電元件,可利用一單一 人驟製k整個顯示系統。此切換製造步驟成為干涉調制器 製造步驟之次步驟’並且說明於第Ϊ0Α圖令。 一 j驟1顯不起始平台之上視圖與側視圖。箭號1 〇〇4表 一、 方向。基底已沉積犧牲間隔1002,2000埃 厚度的石夕層;並且於其表面形成圖案。於步驟2中,一社 ㈣料’數微米厚的紹合金,已經沉積並且曝光形成源極 杯1010、汲極1 008及閘極結構1〇〇6。數百埃的不可侵蝕 金屬’例如金、銥或麵可鏟於此結構材料上’以便於切換 期間保持低接觸阻抗。於源極101。内蝕刻形成一凹槽 1〇12’以便幫助源極桿於平行基底地平面移動。比較上視 :與正面圖,立體圖顯示了步驟3與4的差異。箭號1016 表不正面之方向。於步驟3中’犧牲材料已經被蝕刻移除, 留下完整的源極桿1010且可自由移動。 *於源極柃及閘極結構之間施加電壓時,源極桿1010 偏轉向閘極1。。6直到與汲極1〇。8接觸,因此於源極與汲 極之間產生電性接觸。啟動模式平行於基底表面,因此允 許製造步驟適用於主干涉調制器製造步驟。此方法需要更 多步驟,超過用以製造垂直於基底表面方向啟動的切換器。 第10B圖與第1〇c圖說明關於平面微機電切換器的另1077A-4732A-PF 24 1318325 Ghosts - 934 936, 938 and 940. All of the components can be configured in this manner: in conjunction with the manufacture of the display subsystem shown in the figure. This person is included in the control logic 926, the row driver 924, the column driver, and the array, and uses the addressing structure as described in FIG. The manufacture of this switching element, such as a microelectromechanical component, can utilize a single person to make the entire display system. This switching manufacturing step becomes the second step of the interferometric modulator manufacturing step' and is illustrated in Figure 。. A j-jumping 1 shows the top view and side view of the starting platform. Arrow 1 〇〇 4 Table 1. Direction. The substrate has been deposited with a sacrificial interval of 1002, 2000 angstrom thickness; and a pattern is formed on the surface thereof. In step 2, a semiconductor material having a thickness of several micrometers has been deposited and exposed to form a source cup 1010, a drain 1 008, and a gate structure 1〇〇6. A few hundred angstroms of non-erodable metal 'such as gold, tantalum or face can be shoveled on this structural material' to maintain low contact resistance during switching. At source 101. The inner etch forms a recess 1 〇 12' to assist in moving the source rod in a plane parallel to the substrate. Compare top view: With the front view, the perspective view shows the difference between steps 3 and 4. Arrow 1016 is not in the right direction. In step 3 the 'sacrificial material has been etched away, leaving the complete source rod 1010 and free to move. * When a voltage is applied between the source and gate structures, the source rod 1010 is deflected toward the gate 1. . 6 until 1 with the bungee. 8 contact, thus making electrical contact between the source and the drain. The startup mode is parallel to the substrate surface, thus allowing the fabrication steps to be applied to the main interferometric modulator fabrication steps. This method requires more steps than to make a switch that is activated perpendicular to the surface of the substrate. Figure 10B and Figure 1c illustrate additional aspects of a planar MEMS switch

1077A-4732A-PF 25 1318325 外兩種設計。於第⑽圖中的切換器不同於1以於汲極 1024與源極1 026之間接觸的切換桿】〇28。於第⑽圖中 =切換Μ ’必須流通源極桿至沒極的電流將影響切換臨 界值,使電路設計複雜化。 此不疋具有切換器1 020的範 例。於弟1 〇C圖中的切換哭掘兩g 刀換态揭路另—種改善。於此範例中, 絕緣器1 040將切換桿1 〇42盥技總與! Λ0n ^ 〇 W興接觸桿1038電性絕緣。此絕 緣器可為S i 〇2,其可利用pi 认4 洲已知技術沉積與曝光形成圖索。 於包括此切換器之電路中,剎 ” f利用此切換器消除必須將邏輯 h遽與切換驅動電壓電性絕緣的需要。 科 光雷結_ -般而言,干涉調制器之特 的 能,且藉由與本身或1它雪i u -有有皿的先學功 方X”匕電子、機構或井 動裝置而可移動。 #飞光予裝置有關的啟 產生了干涉堆疊的薄膜群έ日投抑 .,^ ^ ^ ^ 腰群組係早石結構的次階層,為 田夕 ❺光電結構。概括地,定義 結構幾何社i盖;5甘4 ΒΒ 光電、,,口構’由於 筹成仏.、。構及其相關變化,可以改 … 結構可與光於沿著一 'Μ丁進。此 丨口 2夕個軸方向作用。 如同光電頻帶差距結構(P 夕維的、、-。構亦 k 136 或光電晶體。Jnh„ n J〇annopoulos 等人撰 John J). J Photonic Crystal 週期性的光電結構。 Qstals說明了 一維的PBG可出現於一 1 6圖顯示一介電法布 、璺、型式令。例如,第 -派洛濾波器型式 其製造方法。薄膜ϊβ1/( ^式的干涉調制器及 寻膘堆積1614與1618 例如間隔的矽層盥1077A-4732A-PF 25 1318325 Two designs. The switch in the (10) diagram is different from the switch lever 〇 28 which is in contact with the drain 1024 and the source 1 026. In Figure (10) = Switching Μ ‘The flow of the source rod to the immersive current will affect the switching threshold and complicate the circuit design. This does not have an example of switch 1 020. In the picture of Yu Di 1 〇 C, the switch is crying and digging two g knives to change the way and to improve the other. In this example, the insulator 1 040 will switch the lever 1 〇 42 to the total! Λ0n ^ 〇 W Xing contact rod 1038 is electrically insulated. The insulator can be S i 〇 2, which can be formed by depositing and exposing a known technique using pi. In the circuit including the switch, the switch uses the switch to eliminate the need to electrically insulate the logic h遽 from the switching drive voltage. Keko Ray Knot _ In general, the special energy of the interferometric modulator, And it can be moved by itself, or by its own snow iu - there is a pre-skilled X" electronic, mechanical or well-moving device. #飞光予装置 Related to the generation of interference film stacks of the day of the day. ^ ^ ^ ^ waist group is the sub-hierarchy of the early stone structure, which is the Tian Xi ❺ photoelectric structure. In summary, the definition of the structure of the geometry of the i cover; 5 Gan 4 ΒΒ photoelectric,,, mouth structure ' due to the preparation of 仏. The structure and its related changes can be changed... The structure can be compared with the light along a 'Ding Ding. This 丨口2 acts in the direction of the axis. Like the photoelectric band gap structure (P eve, , -. also k 136 or photoelectric crystal. Jnh „ n J〇annopoulos et al. John J). J Photonic Crystal periodic photoelectric structure. Qstals illustrates one-dimensional PBG It can be seen in Fig. 16 to show a dielectric method, 璺, type, etc. For example, the method of manufacturing the first-Pylo filter type. Film ϊβ1/(^-type interferometric modulator and seek stacking 1614 and 1618 Interval layer

1077A-4732A-PF 26 1318325 « 氧化石夕層’每一個是四 以便形成具有中心 的長厚’製造於-基底上’ 言,堆叠孫連續於叉…涉調制器結構。-般而 於2方向具有週期性的光學二由:材折射率變化, 交替的高、低折射率層。二:可::當它們是具有間隔 於沿著單-轴,例如、/可考慮為一維的,因為對 最大。 Z軸方向行進的光波,《性功效係 第11A圖與第j 1B圖^ 於第11A圖中,微環狀共㈣…電、4的型式。 許多已知㈣” D 可利用已知的技術使用 對於波長為! 55微”:氧化组及二氧切的合金。 J丄·心儆木靶圍改良的# 般尺寸為… 本質上為圓來、皮1^上(例如玻璃,仍有許多可選擇^結構 折射率及尺寸"及…行進於 可以當作頻率選擇3 "類的共振器,假若設計正確, 此範例中,此傳=行=將寬頻帶傳播輕合進人。於 ΧΥ平面中。此裝置的 ;如圖所標示的符號1101的 造的法布里維類似物將會是利用單-鏡面層製 f置"持^ 。由於單一邊界層(鏡面層),沒有 哀置此維持一咼階光學 光電結構。 n然而’可以視作寬頻效用的 於第11B圖中顯不更多的傳統 向,列陣歹"106呈現—调,… 於X方向與Y方 圖所標示的符號u〇3的二變 十面範圍内’行進通過此介質1077A-4732A-PF 26 1318325 «The oxidized stone layers are each four so as to form a long thick layer with a center made on the substrate, and the stacked sun is continuous with the fork...in the modulator structure. Generally, there are periodic optical two-direction changes in the two directions: a refractive index change of the material, alternating high and low refractive index layers. Two: Yes:: When they are spaced apart along a single-axis, for example, / can be considered as one-dimensional, because the pair is the largest. The light wave traveling in the Z-axis direction, "Sexual effect system" Figure 11A and Figure j 1B Figure ^ In Figure 11A, the micro-ring is a total of (four) ... electricity, 4 type. Many known (four)" D can be used with known techniques for wavelengths of ! 55 micro": oxidized and oxydiminated alloys. The general size of J丄·心儆木靶围改良 is... It is essentially round, leather 1^ (for example, glass, there are still many choices ^ structural refractive index and size " and... travel can be used as frequency Select the 3 " class of resonators, if the design is correct, in this example, this pass = line = spread the broadband transmission into the human. In the plane of the plane. This device; as shown in the symbol 1101 Fabriavi analogs will be constructed using a single-mirror layer. Because of the single boundary layer (mirror layer), there is no stagnation to maintain a one-step optical optoelectronic structure. However, 'can be regarded as broadband The utility of the utility in Figure 11B shows no more traditional directions, arrays 歹 " 106 presentation - tune, ... in the X direction and the Y square map marked by the symbol u 〇 3 within the range of two changes This medium

1077A-4732A-PF 27 1318325 的電磁傳播係最顯著的被影響。 *因為其週期的自然特性,第ιΐβ圖的陣列共同#用一 維薄膜堆積層的属地 、同使用 檟層的屬性,除了其更高階的維度 内,沿著通過瘅刻从甘& — π +面 逋過陣列的某些座標軸,此陣列係 率係於圓柱材料盥用,惠4丨生,折射 材科與周邊材料之間變化,週邊材 氣。利用應用於薄膜埵籍#斗★ 4 叙為工 專膜堆積§又计之相同原則的變化,適舍嗖 計此陣列,允許萝诰夫銥円燃儿λ 遇* 口又 段通過读^ 的光學共振器,(鏡面、波 U波盗、邊緣遽波器),作用於面中行進的傳 :。=第11Β圖範例中顯示的陣列11G6包括圓柱形式的一 圓i二陷:°8,其不同於尺寸及/或折射率。例如,此 圓柱的直徑略微地大於或小於其它圓柱(例如直徑差異四 分之-波長),或其差異為材料(例如空氣 陣列的整個尺寸藉由弁學备M今、_ 乳化石夕) 精由先子糸統或凡件之尺寸決定,盆必須 巧妙地處理。依據其需要的特性’此缺陷亦可以一列或多 列m現。此結構類似於第6i圖_的介電法布里—派洛 慮波益’但只作用於二維範圍中。於此範例中,缺陷類似 於孔穴1616。剩餘圓柱類似於鄰近的二維堆積。 第11B圖結構的相關維度藉由列χ間隔sx、列y間隔 sy(兩者可視作晶格)、圓柱直徑d及陣列高度h表示。類 似四分之一波長堆疊,—維♦吾 μ 维田里、圓柱直徑及間隔為四分 之-波長等級。高度h經由需要行進模式而決定,對於單 一模式行進具有猶微大於半波長。關於作用於光的結構尺 寸之等“已知mlQhnD.。卿-等人證明The electromagnetic propagation system of 1077A-4732A-PF 27 1318325 is most significantly affected. *Because of the natural nature of its period, the array of the ιΐβ map is common with the properties of the one-dimensional film-stacked layer, the same as the properties of the layer used, except for its higher-order dimensions, along with the engraving from Gan & + Faces over some coordinate axes of the array. This array rate is used for cylindrical materials, Hui 4, and the change between the refractive material and the surrounding materials, and the surrounding material. The use of the same principle applied to the film 埵 # 斗 4 4 4 4 为 工 工 工 工 工 工 工 工 工 工 工 工 § § § § § § § § § § § § § § § § § § § § § 工 工 工 § Optical resonator, (mirror surface, wave U wave thief, edge chopper), acting on the surface of the transmission: = Array 11G6 shown in the example of Figure 11 includes a cylindrical one-circle: two, which is different from the size and/or refractive index. For example, the diameter of the cylinder is slightly larger or smaller than other cylinders (for example, the difference in diameter by a quarter-wavelength), or the difference is the material (for example, the entire size of the air array by 弁学备M, _ emulsified stone eve) Determined by the size of the scorpion or the size of the piece, the basin must be handled skillfully. According to its required characteristics, this defect can also be listed in one or more columns. This structure is similar to the dielectric Fabry-Perot wave effect of Figure 6i, but acts only in the two-dimensional range. In this example, the defect is similar to the aperture 1616. The remaining cylinders are similar to adjacent two-dimensional stacks. The relevant dimensions of the structure of Fig. 11B are represented by the column spacing sx, the column y spacing sy (both can be regarded as a crystal lattice), the cylinder diameter d, and the array height h. Similar to a quarter-wavelength stack, the dimension, the diameter of the cylinder, and the spacing are four-wavelength. The height h is determined by the need for a travel mode and is more than half a wavelength for a single mode travel. About the size of the structure acting on the light, "known as mlQhnD.. Qing - et al.

於教科書 Photonic Crystals,,中。 1077A-4732A-PF 28 1318325 ::結構亦利用相同的材料及用以製造共振器⑽ 的技術製造。例如,矽的單一 早/專膜可利用習知技術沉積於 璃土底上並且形成圖案,接著利用易反應的離子蝕刻製 造好外觀比例的圓柱。例如, /皮長1. 5 5 /z m,圓柱的直徑 與間隔分別為〇· 5# m及〇.丨# m。 光電結構亦可以於限制的幾何下導引傳播。因此,於 應用方面相當有用,當尺寸限制得相當嚴謹時,可以引導 且/或選擇既定光頻率或光波段。亦可以製造波導,其傳送 先於π平面中行進’強迫光於小於光波長的空間中9〇度 轉折。這可以藉由產生直線行型式的圓柱缺陷而完成,可 以當波導使用。 於第12圖中說明二維結構。三維週期結構⑵2作用 於XY、YZ&XZ平面中行進的傳播。藉由適當的結構設計 及選擇構成材料可獲得各種光學響應。應用這些相同的設 。十規則’然而’在此應用三維的。缺陷以點、線或區域型 式相對於點及線出現,其與周邊介f不同於尺寸及/或折射 率。於第12圖中’缺陷12〇4係_單—點元件,但是亦可 能為線型或線與點元件或區域的結合。例如,可以製造一 '線型’’ 婉蜒,,缺陷點陣列,其依據任意的三為:伊 通過PBG,並且當作用以使光於其中傳輸的一緊密束縛波 導。缺陷一般位於其内,但是為了說明的緣故顯示於表面。 此結構之相關尺寸皆說明於圖式中。PBG之直徑、間隔及 材料係完全相關的,然而亦可利用上述設計規則。 製造三維的PBGs係更複雜。關於製造—維或二維特徵 1077A-4732A-PF 29 1318325In the textbook Photonic Crystals,, in. 1077A-4732A-PF 28 1318325 :: The structure is also fabricated using the same materials and techniques used to fabricate the resonator (10). For example, a single early/special film of tantalum can be deposited on a glass substrate and patterned using conventional techniques, followed by the use of reactive ion etching to produce a cylinder of apparent proportion. For example, / leather length is 1. 5 5 /z m, and the diameter and spacing of the cylinder are 〇·5# m and 〇.丨# m, respectively. The optoelectronic structure can also be guided to propagate under a limited geometry. Therefore, it is quite useful in terms of application, and when the size is constrained to be quite strict, it is possible to guide and/or select a predetermined optical frequency or optical band. It is also possible to fabricate a waveguide whose propagation precedes the travel in the π plane to force the light to turn at a 9 degree turn in a space smaller than the wavelength of the light. This can be done by creating a linear row of cylindrical defects that can be used as a waveguide. The two-dimensional structure is illustrated in Fig. 12. The three-dimensional periodic structure (2) 2 acts on the propagation of travel in the XY, YZ & XZ planes. Various optical responses can be obtained by appropriate structural design and selection of constituent materials. Apply these same settings. The ten rule 'however' applies three-dimensionality here. Defects occur in point, line or area form with respect to points and lines, which differ from the peripheral dimension by size and/or refractive index. In Fig. 12, the 'defective 12〇4 series_single-point element, but may be a combination of a line type or a line and a point element or a region. For example, a 'line type' 婉蜒, an array of defect points can be fabricated, which is based on any three: I pass PBG and act as a tightly bound waveguide for transmitting light therein. Defects are generally located therein, but are shown on the surface for illustrative purposes. The relevant dimensions of this structure are illustrated in the drawings. The diameter, spacing and material of the PBG are completely relevant, however the above design rules can also be utilized. Making three-dimensional PBGs is more complicated. About Manufacturing - Dimensional or 2D Features 1077A-4732A-PF 29 1318325

的習知裝置,假若應用於三維中,將加入更多的沉積、顯 衫及蝕刻循環以便獲得三維的結構。對於製造週期性二維 結構之製造技術包括:全像顯影,其中一光感應材料以一 標準波曝光並且於材料㈣疊此波成折射率變化的型式; 自我組織的有機材料或自我結合的材料根據其固有的黏著 性及某些異量分子聚合材料之方向特性,⑥沉積材料期間 產生圓柱陣列或球狀結構;可加入陶瓷方法,提供球狀結 構控制尺寸成液體懸浮…但固化、組織此結構並且可: 由溶解或咼溫而移除;上述方法的結合等等。 異量分子聚合技術及自我結合技術特別令人關注,因 為兩者為低溫的並且需要少量或不需要曝光顯影。—般而 言’此技術包括高分子溶解’例如多苯基奎寧塊多聚笨乙 烤(PPQmPSn)溶解於:硫化碳中。將溶液塗佈於基底^且使 ’合d揮發後,產生氣體充滿聚合物球體内的緊密六角型排 列。此技術可重複多次,以便產生許多層;可藉由運用高 分子單元On與η)之重複單元數目,控制陣列之週期。使用 微米大小’包括金屬、氧化物半導體的勝狀體,具有減少 陣列週期之功效,進一步可增.加高分子的折射率。 經由直接將材料運用次微米等級的聚焦離子束或原子 力顯微鏡等工具,i生缺陷。之前的可用於非常小的選擇 區域内,移除或加入材料;#用以改變材料的光學特性。 材料移除產生於當具有能量的粒子束’例如使用聚焦離子 束工具’於其路徑上喷除材料。材料加入發生於當聚焦離 子光束穿透-易揮發的、含有氣體的金屬,例如六氣化嫣Conventional devices, if applied in three dimensions, will incorporate more deposition, embroidering, and etching cycles to achieve a three-dimensional structure. Manufacturing techniques for fabricating periodic two-dimensional structures include: holographic development in which a photo-sensitive material is exposed to a standard wave and the material (four) is superimposed into a pattern of refractive index changes; self-organizing organic materials or self-bonding materials According to its inherent adhesion and the directional characteristics of some heterogeneous molecular polymeric materials, a cylindrical array or a spherical structure is produced during the deposition of the material; a ceramic method can be added to provide a spherical structure to control the size into a liquid suspension... but solidify, organize this The structure can be: removed by dissolution or enthalpy; a combination of the above methods, and the like. Heterogeneous molecular polymerization techniques and self-binding techniques are of particular interest because both are low temperature and require little or no exposure development. As a general rule, this technique involves the dissolution of a polymer such as polyphenyl quinine block polystyrene (PPQmPSn) dissolved in: carbon sulfide. The solution is applied to the substrate and the resulting mixture is volatilized to produce a tight hexagonal arrangement in which the gas fills the polymer sphere. This technique can be repeated multiple times to produce a number of layers; the period of the array can be controlled by applying the number of repeating units of the high molecular units On and η). The use of a micron size, including a metal or an oxide semiconductor, has the effect of reducing the array period, and further increases the refractive index of the polymer. Defects are generated by directly applying materials to sub-micron-scale focused ion beams or atomic force microscopes. Previously available for very small selections, removing or adding materials; # to change the optical properties of the material. Material removal results from the ejection of material from the particle beam with energy ', for example, using a focused ion beam tool' Material addition occurs when the focused ion beam penetrates - a volatile, gas-containing metal, such as six gas enthalpy

1077A-4732A-PF 30 1318325 (鶴導體)或四氟切(絕緣的二氧化石夕)。氣體減緩速度, 且組成物沉積於離子束接觸基底處。 ,另一種方法包括使用稱之為微電極沉積技術,且盆已 洋細敘述於美國專利㈣5,641,391 ^於此方法中了 利用一單一微觀電極,定羞 各種材料與基底的次微米 又之二維特徵。利用此方法沉積的金屬、、缺陷 :氧化,以便形成m陣列圍繞的介電缺陷 使用上述技術製造。 係 存在表面上的特微為,7甘 μ— 以其他材料圖案之形式,例如 面士製造PBG陣列;於缺陷形成期間,於pBG範 底狀兄乍產生缺陷的樣板。這特別係有關於對於基 ==的PBG方法,主要地自我組合方法。根據方法 種此方法可促進或抑制PBG之''成長〃於被晶 =度圍,的局部區域。於此方法中,缺陷、、晶種的圖 案可以被製造;之後’於形成 圍内形成PBG。 纟PBG期間,於缺陷產生的範 類的=已知為干涉調制器的裝置之種類藉由將更多種 構加入調制器本身,而變得更多。任何光 附近的有為靜#裝置,可藉由改變其幾何及/或改變其 附近的結構而變成動態。 器(於第16圖中所干)’勺括: 法布里-派洛遽波 電鏡面,每-個為-維的光 電、,'D構,可藉由靜電地改變空穴寬度而調整。 苐13圖顯示加入二維沾^ 個範例。於第13A圖中 調制器設計的兩 A圖中,一部份切除的圖案揭露一自我支1077A-4732A-PF 30 1318325 (Heavy conductor) or PTFE (insulated carbon dioxide eve). The gas slows down and the composition deposits at the ion beam contacting the substrate. Another method involves the use of a technique called microelectrode deposition, and the basin has been described in detail in U.S. Patent No. 5,641,391. In this method, a single microscopic electrode is used to shame the submicron of various materials and substrates. The two-dimensional feature. Metals deposited by this method, defects: oxidation, to form dielectric defects surrounded by m-arrays, are fabricated using the techniques described above. There are special features on the surface, 7 g - in the form of other material patterns, such as the PBG array made by the pastry; during the formation of the defect, the pBG paradigm produces defects in the template. This is especially relevant for PBG methods for base ==, mainly self-combining methods. According to the method, this method can promote or inhibit the growth of the PBG from the local area surrounded by the crystal. In this method, a pattern of defects, seed crystals can be fabricated; then PBG is formed in the formation. During the 纟PBG, the type of device that is known to be an interfering modulator in the class of defect generation becomes more by adding more species to the modulator itself. Any static device near the light can become dynamic by changing its geometry and/or changing the structure in its vicinity. The device (made in Figure 16)'s scoop: Fabry-Pylowave's electro-mirror surface, each --dimensional photoelectric, 'D-structure, can be adjusted by electrostatically changing the hole width . The 苐13 image shows an example of adding a two-dimensional smear. In the two A diagrams of the modulator design in Fig. 13A, a partially cut pattern reveals a self-support

1077A-4732A-PF 31 1318325 °的薄膜1 304,其被製造且固定於面對基底側上,並且具 微環狀共振器1306。橫臥於基底1303内部的波導1301 1 302係平的且平行,並且可利用已知技術製造。於 • 1 Ο Λ .. t 鱼圖中,干涉調制器顯示處於未被驅動狀態,於微環狀 與基底之間具有一有限的空氣間隔。製造微環狀,因此其 位置與此對波導重疊且對齊。微環狀的尺寸與上述範例相 同。1J面圖1 305顯示波導之尺寸,為w=1 " m、h=〇· 瓜 •及^lGGnm。於未被驅動狀態中,光13()8未分布的傳導於 ‘ 1 302内,並且輸出光束131〇之光譜完全相同於入射 光束1 308。驅動干涉調制器以便強迫微環狀緊密的與基底 及波導接觸’改變裝置的光學特性。於波導i3Q2中行進的 =可藉由消逝現象_人微環狀。此微環狀,假若大小適當, 當作一光學共振器’將挑選的頻率自波導1302耦出且引入 波導1301。此顯示於第13B圖中,其中光束1312顯示行 ,於與光束1308方向相反的方向。這類的裝置可當作頻率 • j擇切換器使用;藉由施加電壓,或其它需要將此結構與 橫躺的波導緊密接觸的驅動襄置,可將特殊的波長自波導 挑選出來。此幾何結構的靜電描述已說明於B. E. Little 等人發表的論文、、Vertically c〇upled1077A-4732A-PF 31 1318325 ° film 1 304, which is fabricated and fixed on the side facing the substrate, and has a micro-ring resonator 1306. The waveguides 1301 1 302 lying across the interior of the substrate 1303 are flat and parallel and can be fabricated using known techniques. In the 1 Ο Λ .. t fish diagram, the interferometric modulator shows an undriven state with a limited air gap between the microring and the substrate. The microring is fabricated so that its position overlaps and aligns with the pair of waveguides. The size of the microring is the same as the above example. Figure 1 305 shows the dimensions of the waveguide, which is w = 1 " m, h = 〇 · melon • and ^lGGnm. In the undriven state, light 13()8 is undistributed within '1 302, and the output beam 131〇 has the same spectrum as incident beam 1 308. The interferometric modulator is driven to force the micro-rings to closely contact the substrate and the waveguide to alter the optical properties of the device. The travel in the waveguide i3Q2 can be made by the evanescent phenomenon _ human micro-ring. This micro-ring, if properly sized, acts as an optical resonator' to couple the selected frequency out of the waveguide 1302 and into the waveguide 1301. This is shown in Figure 13B, where beam 1312 shows the line in the opposite direction to beam 1308. Such devices can be used as a frequency switch; special wavelengths can be selected from the waveguide by applying a voltage, or other drive device that requires the structure to be in intimate contact with the lying waveguide. The electrostatic description of this geometry has been described in the paper by B. E. Little et al., Vertically c〇upled

Resonator Channel Dropping Filter^ , iEEE Photonics Technology Letters,vol, n,n〇. 2,1 999。 於第13C圖中說明另一範例。於此範例中,一對波導 1 332及聰以及共振器1314以圓柱形式製造於基底上。 PBG係相同的圓柱陣列,藉由移除兩行(每一波導一個)定Resonator Channel Dropping Filter^ , iEEE Photonics Technology Letters, vol, n, n〇. 2,1 999. Another example is illustrated in Figure 13C. In this example, a pair of waveguides 1 332 and Cong and resonators 1314 are fabricated in a cylindrical shape on a substrate. PBG is the same cylindrical array, by removing two rows (one for each waveguide)

1077A-4732A-PF 32 1318325 義波導,並且藉由移除兩列定義共振器。上 細的波導1330與〗332及ηΐ4 + α 口扠仏更詳 汉,、振态1 314之結構。尺寸係盥 要的波長以及使用的材料有關。對於155^波長,'圓 的直徑與間隔分別為〇.5"…心高以決定行進模 式,其將被支撐且猶微大於半波長,假若只有單 播。 於薄膜1315之内表面上製造兩個獨立的圓柱1川, 其朝向下方;並且如同基底上的圓柱,具有相同的尺寸以 及相同的材料(或光學特性相同的)。共振器與圓柱被設計 ^彼此相配;於共振器中對應出現—圓柱,其中適當的於 溥膜上設置圓柱。 當干涉調制器處於未被驅動狀態,具有—有限的垂直 、,氣間1 312 ’其位於pBG及薄膜圓柱之間至少數百奈 米’並且因此不再發生光學交互作用。於共振器中出現的 圓柱如同缺陷作用,於波導133G及1332之間產生耗合。 於此狀態中’裝置如同帛13B圖中顯示的作用,並且:著 波導行進的光選擇頻率,現在注入波導1 332中,並且盘光 1 329之相反方向行進。 ” 驅動干涉調制器與PBG接觸,然而,將圓柱適當的放 置於、振器改變其特性。共振器之缺陷藉由配置薄膜圓柱 而消除。利用行進時未干涉的光i 328,於此狀態中的裝置 如同第13A圖中顯示的作用。 此幾何結構之靜電說明已發表於H_ A. Haus之論文 nnel drop filters in photonic crystals^ , Optics1077A-4732A-PF 32 1318325 A waveguide, and the resonator is defined by removing two columns. The upper fine waveguide 1330 is more detailed with the 332 and η ΐ 4 + α 口 , , and the structure of the vibration state 1 314 . The size is related to the desired wavelength and the materials used. For the 155^ wavelength, the diameter and spacing of the circle are 〇.5"...heart height to determine the travel mode, which will be supported and slightly larger than half a wavelength, if only unicast. Two separate cylinders are fabricated on the inner surface of the film 1315, which face downward; and, like the cylinders on the substrate, have the same dimensions and the same material (or optical properties are the same). The resonator and the cylinder are designed to match each other; in the resonator, a cylinder is formed correspondingly, and a cylinder is suitably disposed on the diaphragm. When the interferometric modulator is in an undriven state, with a finite vertical, the air gap 1 312 ' is at least a few hundred nanometers between the pBG and the film cylinder' and thus no optical interaction occurs. The cylinder appearing in the resonator acts as a defect, creating a trade-off between the waveguides 133G and 1332. In this state the device acts as shown in Figure 13B, and: the light selection frequency at which the waveguide travels is now injected into the waveguide 1 332 and the opposite direction of the disk light 1 329 travels. The drive interferometer is in contact with the PBG, however, the cylinder is properly placed in the vibrator to change its characteristics. The defect of the resonator is eliminated by arranging the thin film cylinder. Using the light i 328 that does not interfere during travel, in this state The device is shown in Figure 13A. The static description of this geometry has been published in H_A. Haus's paper nnel drop filters in photonic crystals^ , Optics

1077A-4732A-PF 33 13183251077A-4732A-PF 33 1318325

Express, vol. no. 1, 1998。 先學切換器 :第14A圖中,根據感應吸收器的裝置包括 接㈣膜刚,位純十至數百㈣平方上,料支 堆積層1402上’此材料堆積層包括金屬與氧化物的电人^ 二=2底上形成既定圖案。於感應吸收調制器:使 用的薄膜適合此目的,已揭露於1 996年7月31日申= =國專利中請案第〇8/688, 71 G號,並且在此列人參考。於 土底上的薄膜亦包括-透明導體’例> IT0。此結構可於 其下面加上一金屬薄膜,例如鉬或鎢,數百埃的厚度。 ,:吏用此材料’因此於未驅動狀態,此裝置反射特定的 波長範圍’當薄膜被驅動與之接觸時,變得極力吸收光。 側視圖1410顯示此裝置之一圖視,從基底之側面查看。光 束1408以某一任意角度於基底内傳播並且入射顯示處於 未驅動狀態的干涉調制器1權。假設光的頻率與處於未驅 動狀態的干涉調制器之反射範圍一致時,光以一互補角度 反射並且遠離。側視圖,1414,顯示處於驅動狀態的相同 干涉調制器。因為裝置現在極力吸收光,入射於其上的光 不再被反射,並且藉由干涉調制器堆疊的材料吸收。 因此’於此配置中,製造可當作光學切換器的干涉調 制斋,對於行進於基底内的光切換。以機器製作基底,以 便形成非常光滑、非常平坦(於注重的光的i /丨〇波長範 圍)’並且較光的波長還長數倍(至少數百微米)。這允許基Express, vol. no. 1, 1998. First learn the switch: In Figure 14A, the device according to the inductive absorber comprises a (four) film just, the position is purely ten to several hundred (four) squares, and the material is deposited on the layer 1402. The material stack includes metal and oxide. People ^ 2 = 2 forms a predetermined pattern on the bottom. Inductive Absorption Modulators: The films used are suitable for this purpose and have been disclosed in July 31, 1996, in the National Patent Application No. 8/688, 71 G, and are hereby incorporated by reference. The film on the soil floor also includes - a transparent conductor 'example> IT0. The structure may be followed by a metal film such as molybdenum or tungsten, a thickness of several hundred angstroms. ,: This material is used. Therefore, in the undriven state, the device reflects a specific wavelength range. When the film is driven in contact with it, it becomes extremely absorbed. Side view 1410 shows a view of one of the devices, viewed from the side of the substrate. Light beam 1408 propagates within the substrate at an arbitrary angle and is incident to exhibit an interferometric modulator 1 in an undriven state. Assuming that the frequency of the light coincides with the range of reflection of the interferometric modulator in the undriven state, the light is reflected at a complementary angle and away. Side view, 1414, shows the same interferometric modulator in the driven state. Because the device now absorbs light as much as possible, the light incident thereon is no longer reflected and is absorbed by the material of the interferometric modulator stack. Thus, in this configuration, interference can be fabricated that acts as an optical switcher for switching light traveling within the substrate. The substrate is machined to form a very smooth, very flat (i/丨〇 wavelength range of focused light)' and is several times longer (at least hundreds of microns) than the wavelength of light. This allows the base

1077A-4732A-PF 34 1318325 底當作基底/波導使用,光束於並 二_ T y 〇〒以某一方向行進,— 平行於基底,但是從-表面至另-表面經過多-欠; 射。於此結構中的光波經常當作基底導向波。 反 第14 B圖顯示此發明之 1例月之變化。形成既定圖案的薄膜 1420,不再是矩形而是―端 寻膜1077A-4732A-PF 34 1318325 The bottom is used as a substrate/waveguide, and the beam travels in a certain direction, and parallel to the substrate, but from the surface to the other surface through multiple-undershoot; Light waves in this structure are often used as substrate guiding waves. The reverse Fig. 14B shows the change of the month of the invention. The film 1420 forming a predetermined pattern is no longer a rectangle but an end film.

^ 變夂虽結構的機様强I 常數沿著此長度維持不變減幾構弹簧 茭成〆電極面積。因此, 物之尖端施加靜電的力量大 " ^ 尔較小的。假若逐漸拗知φ 壓,將首先於較寬端驅動薄膜 θ電 从卜 导膜接者當電壓增加時,脾、、κ 者箭號1428方向啟動。 冬/t3 對於入射光,干涉續制哭a 八周制益畲作-吸收區域操作,复中 根據施加電壓值決定面積 /、中 ^ _ 檟側視圖1434顯示當沒有施加電 昼時,於基底上傳播先击的έ士审,, 电 束的結果。對應的反射區域1429, 即入射光束的立體圖顯示 |ν’剌态’顯不光束於及鼾 域重疊蹤跡1431。因兔敕伽广α 射^ 因為整個區域1429不會吸收,光束143〇 自干涉調制器1428及鼾忐止Α , 0汉射成先束1432的形式。 於側視圖1436中,施加—暫丰 J 暫Bf罨壓值,並且反射走 1 440已經衰減至某箱铲择m a、 汉对尤末 ” 王又’因為被顯示的反射區域1437 部份吸收。圖式1438鱼U9〇 # _ 興1 429顯示完整作用的結果以及光 束完全衷減。 因此,藉由使用一錐狀結構,可以製造可調制光學衰 減器’其反應直接與施加電壓值有關。 /另-種光學切換器說明於第15Α圖中。支撐結構测 係利用金屬製造,例士貉主 數千埃厚度的鋁’以此方法其與一 鏡面1 5 0 2電性連技^ π , 鏡面1502存在於透明的光學支座^ Although the structure of the machine is strong, the I constant decreases along this length to reduce the area of the electrode. Therefore, the power of the tip of the object to apply static electricity is large and small. If the φ pressure is gradually known, the film will be driven first at the wider end. When the voltage is increased, the spleen, κ, arrow 1428 direction is activated. Winter/t3 For incident light, the interference continues to cry a eight-week system-absorption area operation, the intermediate area is determined according to the applied voltage value, and the middle ^ _ 槚 side view 1434 shows that when no electricity is applied, it propagates on the substrate. The first attack on the gentleman, the result of the electric beam. The corresponding reflective area 1429, i.e., the perspective view of the incident beam, shows that the |ν' 剌 state does not show the beam and the 重叠 domain overlap trace 1431. Because of the gamma gamma of the rabbit, since the entire region 1429 does not absorb, the beam 143 〇 is from the interferometric modulator 1428 and the 汉 Α Α , 0 汉 is in the form of the first beam 1432 . In the side view 1436, the value of the temporary Bf is applied, and the reflection 1 440 has been attenuated to a certain box to select ma, and the Han to the end of the "wang" because the reflected area 1437 is partially absorbed. Figure 1438 Fish U9〇# _ 兴1 429 shows the result of the complete action and the beam is completely reduced. Therefore, by using a tapered structure, a modulatable optical attenuator can be fabricated whose response is directly related to the applied voltage value. Another type of optical switch is described in Figure 15. The support structure is made of metal, which is a kind of aluminum with a thickness of several thousand angstroms. In this way, it is electrically connected with a mirror of 1 502. Mirror 1502 is present in a transparent optical mount

1077A-4732A-PF 35 1318325 .礞 1501,其黏接於支撐物1 500。鏡面15〇2可包括一單一金 屬薄膜或金屬氧化物以及半導體薄膜。 以支架係利用材料製造,材料具有等於或大於基底的折 _射率。這可為Si02(相同的折射率)或可變化折射率的高分 子聚合物。支架係按規定尺寸製造,因此鏡面係以45度角 支撐。利用類黃光微影技術,其根據連續隨其光學密^變 化特徵的光罩,可完成支架之製造。於一特定的表面上, 籲藉由適當的變化密度,並利用此光罩曝光,可於光阻中形 成三維的形狀。經由反應離子蝕刻,此形狀可轉換至其他 材料。整個結構懸浮於導體15〇3上,其已經形成既定的圖 案以便於其下面的基底1 504上提供一不會遮住光的窗 1505。換句話說,一塊導體15〇3已經被蝕刻移除,因此窗 1 5 05包括裸露的玻璃。此切換類似干涉調制器,可以啟動 以便驅使整個結構與基底/波導接觸。側視圖1512,顯示 光子特性。光束151 〇於基底内,與法線夾45度角傳播, #防止其行進超越基底的邊界。這是因為45度角係已知的臨 界角,根據完全内反射理論(TIR),允許光束於基底與外部 介質之間的介面,以少量或無損失的反射。 TIR理論係根據Snell定理,但是有一基本需要,就 是基底外的介質之折射率小於基底的折射率。於側面圖 1512中,裝置顯示此切換器15〇6處於未被驅動狀態,並 且光束1510以楊通無阻的方式行進。當切換器啟動 並與基底接觸時,如側視圖1514所示,改變光束路徑。因 為支架具有大於或等於基底的折射率,故光束不再於介面1077A-4732A-PF 35 1318325 .礞 1501, which is bonded to the support 1500. The mirror 15 〇 2 may comprise a single metal film or metal oxide and a semiconductor film. The stent is made of a material having a refractive index equal to or greater than the substrate. This can be a SiO 2 (same refractive index) or a high refractive index polymer with a variable refractive index. The brackets are manufactured to the specified dimensions, so the mirrors are supported at a 45 degree angle. With the yellow-like lithography technique, the fabrication of the stent can be accomplished according to a reticle that continuously changes its optical characteristics. On a particular surface, a three-dimensional shape can be formed in the photoresist by appropriate density of change and exposure using the reticle. This shape can be converted to other materials via reactive ion etching. The entire structure is suspended on conductor 15A, which has formed a predetermined pattern to provide a window 1505 on the underlying substrate 1 504 that does not block light. In other words, a piece of conductor 15〇3 has been removed by etching, so window 15 5 05 includes bare glass. This switching is similar to an interferometric modulator that can be activated to drive the entire structure into contact with the substrate/waveguide. Side view 1512 shows photon characteristics. The beam 151 is placed in the substrate and propagates at a 45 degree angle to the normal, preventing it from traveling beyond the boundary of the substrate. This is because the 45 degree angle is known as the critical angle, which allows for a small or no loss of reflection of the beam between the substrate and the external medium according to the Total Internal Reflection Theory (TIR). The TIR theory is based on the Snell theorem, but there is a basic need that the refractive index of the medium outside the substrate is less than the refractive index of the substrate. In side view 1512, the device shows that the switch 15〇6 is in an undriven state and that the beam 1510 travels in an unimpeded manner. When the switch is activated and in contact with the substrate, as shown in side view 1514, the beam path is changed. Since the stent has a refractive index greater than or equal to the substrate, the beam is no longer at the interface

1077A-4732A^PF 36 1318325 發生TIR。光束離開基底進入光學支架,並在那裡藉由鏡 面反射。處於45度的鏡面反射光束,使其以垂直於基底平 面行進。結果,光可以穿透基底介面,因為其不再滿足Ur; 並且可藉由一光纖耦合器152〇捕捉,光纖耦合器已經設置 於基底/波導之對立面上。-相似的觀念已揭露於X. Zhou 等人於 1 998 年,SIDDigest,νο1. χχιχ 的論文、1077A-4732A^PF 36 1318325 TIR occurs. The beam exits the substrate and enters the optical support where it is mirrored. A specularly reflected beam at 45 degrees is allowed to travel perpendicular to the plane of the substrate. As a result, light can penetrate the substrate interface because it no longer satisfies Ur; and can be captured by a fiber coupler 152, the fiber coupler has been placed on the opposite side of the substrate/waveguide. - A similar concept has been revealed in X. Zhou et al. in 998, SIDDigest, νο1. χχιχ's paper,

Panel Display Using Electromechanical Spatial Modulat㈣,。此特別的裝置設計於發光顯示器應用。此 鏡面亦可加入反射光栅,可利用習知曝光技術钮刻支架之 表面。然而,此方法顯示與波長有關,並且由於多階繞射 造成損耗,這並不是薄膜鏡面的緣故。此外,另 結構可替代鏡面,如同盆屬性盥 干 J /、屬性與紐處。此可分類成折射、 反射及繞射;並且可包括微透鏡(穿透及反射)、凹面鏡或 凸面鏡、繞射光學元件、全像光學元件、棱鏡及任㈣它 形式的光學元件,並且可利用微製造技術產生。於使用另 一種光學元件的範例中,彡靼 光學種類無關。 支*及角度給予的光學可能與微 干涉調制器之變化當作光的解麵合切換器使用。假若 正確,寬波段發光或特定頻率可任意的自基底/ 波導輕出。侧視圖1 526顯示更多複雜的改良,其中一額外 的固定鏡面,以央角4 5# 的相對側卜l 又“於具有解耦合切換器之基底 的相對側上。此鏡面與切換考兀问 由卜m 吳益不问,其不可以被啟動。藉 離兩種結構上的鏡面角度,已經有效率地搞合 離開基底的光1522藉由切換器15G6,可再藉由軸合鏡Panel Display Using Electromechanical Spatial Modulat (4). This particular device is designed for illuminating display applications. The mirror can also be incorporated with a reflective grating that can be engraved on the surface of the stent using conventional exposure techniques. However, this method shows wavelength dependence and loss due to multi-order diffraction, which is not the result of a film mirror. In addition, another structure can replace the mirror, like the basin property 盥 dry J /, attributes and links. This can be classified into refraction, reflection, and diffraction; and can include microlenses (penetration and reflection), concave or convex mirrors, diffractive optical elements, holographic optical elements, prisms, and any of the optical elements in its form, and can be utilized Microfabrication technology is produced. In the case of using another optical component, the optical type is independent. The optics imparted by the * and angle may be used as a light-combining switcher with changes in the micro-interferometer modulator. If correct, wide-band illumination or a specific frequency can be arbitrarily removed from the substrate/waveguide. Side view 1 526 shows a more complex improvement in which an additional fixed mirror, on the opposite side of the central angle 4 5#, is again "on the opposite side of the base with the decoupled switcher. This mirror and switching test Qi Wu Wu Yi does not ask, it can not be activated. By the two mirror angles of the structure, the light 1522 that has been separated from the base has been efficiently engaged by the switch 15G6, and can be used by the mirror

1077A-4732A-PF 37 1318325 礴 面測再I禺合回基底。然而,於χγ平面_藉由製造且有 不同定位方向的再裁合鏡面;於基底/波導内,鏡W體 可再次導引光至任何新方向。此 ° , 扪種、,,°構的結合體將參考 當作一方向切換器使用。S知人 一 优用再耦合鏡面亦可用來耦合任何 光,使光以垂直於表面方向傳播進入基底中。 第15Β圖顯示一種使用方向性切換器之陣列。俯峨基 底1535,線性陣歹〇 536係一光纖搞合器陣列,並引 以垂直於ΧΥ平面之角度進入基底。一再•合鏡面陣列(未 顯示)直接設置於與光纖相合器陣列相對之位置,以 輕合入平行於光束刪的基底中。於基底之表面MM上, 製造了方向性切換器陣列,其中⑽係其中一個。以特殊 方法設置切換器、,因此自任—輸人光_合器Η%麵合進 入基底的光,可引導至任一輸出光纖搞合器1 532。利用此 方法之裝置可當作一 Ν χ Ν的光學切換器使用,其可以切 換任一不同的輸入至任一不同的輸出。 可調制滤波恶 >考第1 6圖’顯不一可調制法布里一派洛濾波器形式 勺干涉㈣器。於此範例中,沉積—導電接觸塾⑽2,並 且沿著介面鏡面1 604與1 608及犧牲層1 606形成圖案。這 匕括發;#膜’其厚度為半波長之某些倍數。鏡面可包括 ㈣堆疊’例% Ti〇2(高折射率)與_(低折射率),具有 又替的π低折射率’並且其中—層亦可為空氣。沉積絕 緣層161G ’並且形成圖案,使得第二接觸墊只接觸1077A-4732A-PF 37 1318325 面 The surface is measured and returned to the substrate. However, in the χ γ plane _ the mirror surface is fabricated by having different orientation directions; in the substrate/waveguide, the mirror W body can redirect the light to any new direction again. This combination of °, 扪, ,, ° configurations uses the reference as a directional switcher. S knowing that a re-coupled mirror can also be used to couple any light, allowing light to propagate into the substrate perpendicular to the surface. Figure 15 shows an array using a directional switch. The base 1535, the linear array 536 is an array of fiber optic adapters that enter the substrate at an angle perpendicular to the plane of the pupil. A repeating mirror array (not shown) is placed directly opposite the fiber optic coupler array to lightly fit into the substrate parallel to the beam. On the surface MM of the substrate, a directional switcher array is fabricated, wherein (10) is one of them. The switch is set up in a special way, so that the light that enters the substrate can be directed to any of the output fiber combiners 1 532. The device using this method can be used as an optical switcher that can switch any different input to any different output. Can be modulated and filtered evil > test No. 1 6 '' can be modulated by Fabry-Perot filter form scoop interference (four). In this example, the conductive-contact 塾(10) 2 is deposited and patterned along the interface mirrors 1 604 and 1 608 and the sacrificial layer 1 606. This includes the hair; #膜' has a thickness that is a multiple of a half wavelength. The mirror may comprise (iv) a stack of '% Ti〇2 (high refractive index) and _ (low refractive index), with a further π low refractive index' and wherein the layer may also be air. The insulating layer 161G' is deposited and patterned such that the second contact pad only contacts

1077A-4732A-PF 38 1318325 鏡面。形成圖案的鏡面16 1614’藉由支撐物1615連接 體…鏡面 '島〃 互作用之光束大小而決定。—=尺寸主要藉由將交 級。犧牲層i 6 0 6係部份被化學餘又刻為數十至數百微米等 架以便提供機構穩定性,大概為十微米平I下適:大小的支 之頂層與鏡面胸之底層輕 _ 。假讀面1608 1 602盥161…-雜以便導電,則接觸墊1077A-4732A-PF 38 1318325 Mirror surface. The patterned mirror 16 1614' is determined by the size of the beam of the mirror 16's interaction of the support 1615. —= Size is mainly due to the level of the intersection. The sacrificial layer i 6 0 6 part is chemically engraved into tens to hundreds of micrometers to provide mechanical stability, which is about ten micrometers flat I. The top layer of the size of the branch and the bottom of the mirror chest are light _ . False reading surface 1608 1 602盥161...-hetery for conduction, then contact pad

可門啟此㈣ 電壓將造成鏡面島離開。因此, 可開啟此結構之光學響應。 第ΠΑ圖顯示此可調制濾'波器之應用。基底_之上 表面上已經製造可調制渡“ 17G4、鏡面m 鑛膜1712。一鏡面1717已經製造於基底之下表面上,= 如形成-金屬,像是至少10。厚度之黃金。固定於基底 之上表面上的是一光學超結構17〇6,其内表面具有至少 95%反射率,例如藉由一額外的反射金薄膜,並且支撐一傾 斜的鏡面1710。於此裝置中,光束17〇2以大於臨界角度 之某角度於基底内行進,關於玻璃基底及空氣介質的臨界 角度為41度。因此,需要將鏡面1716保持固定於基底/ 波導範圍内。此配置結構於角度選擇方面提供光的傳播更 多的彈性。 光束1702入射於法布里-派洛1704上,當反射剩餘光 束1 709時,使既定頻率的光! 7〇8通過。穿透的頻率入射 反射超結構1 706上並且自其反射,接著再藉由鏡面1716 反射至傾斜的鏡面1 7〗0上。鏡面1 71 0適當傾斜,使得光 相對於基底以垂直角度導引朝向抗反射鍍膜1712,接著通The door can be opened (4) The voltage will cause the mirror island to leave. Therefore, the optical response of this structure can be turned on. The figure below shows the application of this modulatable filter. A substrate can be fabricated on the upper surface of the "17G4, mirror m mineral film 1712. A mirror 1717 has been fabricated on the lower surface of the substrate, = as formed - metal, like at least 10. thickness of gold. Fixed to the substrate On the upper surface is an optical superstructure 17〇6 having an inner surface having at least 95% reflectivity, for example by an additional reflective gold film, and supporting a slanted mirror surface 1710. In this device, the beam 17〇 2 Traveling within the substrate at an angle greater than the critical angle, the critical angle for the glass substrate and the air medium is 41 degrees. Therefore, the mirror 1716 needs to remain fixed within the substrate/waveguide range. This configuration provides light in terms of angle selection. The propagation of the beam is more flexible. The beam 1702 is incident on the Fabry-Pylo 1704, and when the remaining beam 1 709 is reflected, the light of a given frequency is passed through! 7〇8. The penetrating frequency is incident on the superstructure 1706. And reflected from it, and then reflected by the mirror surface 1716 onto the inclined mirror surface 177. The mirror surface 710 is appropriately tilted so that the light is directed toward the anti-reflection coating 171 at a vertical angle with respect to the substrate. 2, then pass

1077A-4732A-PF 39 1318325 過且進入外部介面。 使用。 彳正體而"當作波長選擇渡波器 超結構可利用許多技術製造。盆 量微機械形成精密深度的空穴,例;基底之=石夕厚,大 :微米。完成空穴飯刻之後製造傾斜的鏡面 件黏合於某麻 ^ m 並且整個組 之—種於基底例如破璃,利用許多石夕/破璃黏合技術當中 J 17:圖係更多的詳盡的變化。於此範例 用一第二可調制煻油 U、工災 道。換句节爷、’ ° 以便提供額外的頻率選擇通 兩個分開的頻率現在可個別的選擇。亦加 入感測器⑽,並提供高度功能整合。 以才加 第17C圖係顯示加入積體電路。光束175〇已經輕 入基底1 770内’並且入射可調制濾波 器不同於第m圖及第17β圖,” ::波 °兄 ®上製造的再耦合鏡面1 756。鏡面之角度使得 藉由遽波器Π52選擇的頻率,以光束之樣式以= 角度直接耦合入基底中。包含於光束175。内的剩餘頻率傳 播直到其照射傾斜的再轉合鏡面m〇,其呈現垂直於行進 光束Π56之表面。因此光束再追溯原來路徑離開裝置,至 光學連接的其他裝置而使用。光束1 758入射於可檢測及解 #此光束内之貧訊的iCi 764上。此IC可為Fp以樣式,戋 具有積體電路之其切化鎵裝置,其具有直接 搞合攜帶資料的光的益處。例如’一高頻寬的光學互相聯 繫可藉由雙方向光路徑1772功能,形成於ICS1 764及1 7621077A-4732A-PF 39 1318325 and enter the external interface. use.彳正体和“; as a wavelength selective ferrite superstructure can be manufactured using many technologies. The basin micromachines form holes of precise depth, for example; the base = shi shi thick, large: micron. After the completion of the hole meal, the slanted mirror member is bonded to a certain numb and the whole group is planted on the substrate such as broken glass, and many of the lithography/glass reinforced techniques are used. . In this example, a second modulating eucalyptus U and a work-stricken road are used. In other words, in order to provide additional frequency selection, two separate frequencies are now available individually. A sensor (10) is also added and provides a high degree of functional integration. Adding the 17C chart shows the addition of the integrated circuit. The beam 175 〇 has been lightly plunged into the substrate 1 770 'and the incident modulatable filter is different from the mth and 17th spectrograms,": the recoupling mirror 1 756 made on the wave. The angle of the mirror is made by 遽The frequency selected by the wave stop 52 is directly coupled into the substrate at the angle of the beam at an angle of =. The remaining frequency contained in the beam 175 propagates until it illuminates the tilted re-converted mirror m〇, which is perpendicular to the traveling beam Π56. The surface is thus traced back to the original path and used by other devices that are optically connected. The beam 1 758 is incident on the iCi 764 that can detect and resolve the poor signal in this beam. This IC can be Fp-styled. A gallium-cutting device having an integrated circuit having the benefit of directly engaging light carrying data. For example, 'a high-frequency wide optical interconnection can be formed by ICS1 764 and 1 762 by a bidirectional optical path 1772 function.

1077A-4732A-PF 40 1318325 。此藉由鏡面1766與再耦合鏡面1768之結合體形成。 假右具有像是垂直空穴表面發射雷射(vcsels)或光發射二 極體LEDs的元件’藉由任-ICs發射光。藉由任何光學感 應元件並根據用以製造IC的半導體技術製造的元件特性 檢測光。入射於ic上的光,亦可藉由已經於IC表面製造 的干涉調制器,暴露於基底行進光束而調制入射I c上的 光。 導的光聲混和器 第18A圖與第18B圖係說明具有使用基底/波導之TIR 變化形式之兩通道光學混合器。第18A圖顯示裝置之概要 圖式。包含多種波長的光具有兩種特定的波長18〇丨及 1 8 03,破劃分且導引朝向兩個獨立的可變衰減器“Μ。接 著,它們輸出至許多可能的通道18〇7或進入一光學停止器1077A-4732A-PF 40 1318325. This is formed by a combination of mirror 1766 and re-coupling mirror 1768. The false right has elements such as vertical hole surface emitting lasers (vcsels) or light emitting diode LEDs that emit light by any-ICs. Light is detected by any optical sensing element and according to the characteristics of the element fabricated by the semiconductor technology used to fabricate the IC. Light incident on the ic can also modulate light incident on Ic by exposure to a substrate traveling beam that has been fabricated on the surface of the IC. Guided Photoacoustic Mixer Figures 18A and 18B illustrate a two-channel optical mixer with a TIR variation using a substrate/waveguide. Figure 18A shows a schematic diagram of the device. Lights containing multiple wavelengths have two specific wavelengths 18〇丨 and 18 03, broken and directed towards two independent variable attenuators “Μ. Then they are output to many possible channels 18〇7 or into Optical stop

第18B圖揭露另一種結構。此輸入光藉由光纖輕合器 18〇〇、抗反射鍍膜1 802被導引入裝置,並且利用再耦=鏡 面1 806耦合進入基底。此再耦合鏡面引導光入射可調制濾 波器1808’劃分出頻率λ1(光束1815)並且未被選擇的: 率引導朝向第二可調制濾波器18〇9,其劃分出頻率又2(光 束1817),剩餘頻率的光束1819進一步經由行進。、八 著藉由可調制濾波器〗808傳輸的光束i 815之路徑,此一 再次經由鏡面1810反射通過—抗反射鍍膜而被導弓丨二^ 底/波導,並且再耦合入基底。再耦合鏡面181丨導弓丨Figure 18B reveals another structure. This input light is guided into the device by the fiber optic light coupler 18, anti-reflective coating 1 802, and coupled into the substrate using re-coupling = mirror 1 806. This re-coupling mirror directs the light incident modulatable filter 1808' to divide the frequency λ1 (light beam 1815) and is unselected: the rate is directed towards the second modulatable filter 18〇9, which divides the frequency by 2 (light beam 1817) The remaining frequency beam 1819 is further traveled. The path of the beam i 815 transmitted by the modulatable filter 808 is again reflected through the mirror 1810 through the anti-reflective coating to be guided and coupled to the substrate. Re-coupling mirror 181

1077A-4732A-PF 41 1318325 T朝向衰減器1812,接著沿著與光束1817平行的路徑, 繼續藉由第二可調制濾波器18〇9選擇。此兩光束藉由光束 位置改變器1 816之功能而位置移動。 盘此結構如同再耗合鏡面,產生相同的結果,除了鏡面 與基底之表面平行。因為鏡面係以一固定距離懸浮在基底 表面之上,於相對基底分界面上入射點的位置朝向右邊移 動。位移係直接藉由位置改變器之高度而決定。包含未被 選擇波長的光束1819亦藉由位置改變器1818之功能而移 動。結果是三個所有光束等分地被分開,當其入射解麵合 切換益1 820及1824陣列。此等當做選擇性地引導引導光 束進入兩個光結合g 1 828之一,或進入感測器/吸收器 1830。光結合器可利用各種技術製造。高分子薄膜曝光形 成圓柱樣式的圖案’利用反應性離子㈣其頂部形成一透 鏡:吸收器/感測器包括固定於基底上的一半導體元件,提 供當作混合器的輸出功率量測。光學超結構1829支撐外部 光學元件,並且對於混合器提供一密閉封裝。 此平面干涉調制器與基底波導之結合,提供—種容易 製造的、設定的以及_合至外部的光學元件,目為裝置存 在於波導及/或超結構上,並且可以對於在波導内及在波導 與超結構之間傳播的光作用。因為所有的元件以平面方式 製U藉由於大面積上大量製造可達到相當經濟效益,並 且不同部分可㈣且精準地對其與較。此外,因為所有 的活動元件於垂直於基底之方向顯示啟動,與更加精心製 作的非平面鏡面及光束比較,其係相當簡單而製造與驅The 1077A-4732A-PF 41 1318325 T faces the attenuator 1812 and continues along the path parallel to the beam 1817, continuing to be selected by the second modulatable filter 18〇9. The two beams are moved in position by the function of the beam position changer 1 816. The disc is like a mirror that again consumes the same result, except that the mirror is parallel to the surface of the substrate. Since the mirror is suspended above the surface of the substrate at a fixed distance, the position of the incident point on the interface opposite the substrate moves toward the right. The displacement is determined directly by the height of the position changer. Light beam 1819 containing unselected wavelengths is also moved by the function of position changer 1818. The result is that all three beams are equally divided, and when they are incident, they are switched to the 1 820 and 1824 arrays. These are optionally directed to direct the beam into one of the two light combinations g 1 828 or into the sensor/sink 1830. Optical combiners can be fabricated using a variety of techniques. The polymer film is exposed to form a cylindrical pattern. The top of the substrate is formed by a reactive ion (4). The absorber/sensor includes a semiconductor element mounted on the substrate to provide an output power measurement as a mixer. The optical superstructure 1829 supports the external optics and provides a hermetic package for the mixer. The combination of the planar interferometric modulator and the substrate waveguide provides an easy-to-manufacture, set-up, and external-to-external optical component that is present on the waveguide and/or superstructure and that can be used within the waveguide and The effect of light propagating between the waveguide and the superstructure. Since all the components are made in a planar manner, it can be quite economical due to mass production on a large area, and different parts can be (4) accurately compared. In addition, because all of the moving elements are activated in a direction perpendicular to the substrate, they are relatively simple to manufacture and drive compared to more elaborate non-planar mirrors and beams.

1077A-4732A-PF 42 1318325 動。’舌動電子7L件可固定於超結構或基底/波導兩者之一, 以便增加功忐。或者,活動元件可製造成超結構之一部份, 特別假右其係一半導體,例如石夕或石申化鎵。 印刷製造方法 因為其為平面’且因為許多層不具有需要特殊基底的 半V1電子特性,干涉調制器,如同許多微機電結構,可 才木用製。e技術之優點,像是類似於印刷工業。此類的方法 一般包括彈性的且Μ $ + & 耵且紙張或塑膠之連續平板樣式的、基底夕。 參考網印餹人太、、土 ',八—般包括一基底材料的連續滾筒, 基底材料饋入_揸虫τ n 、、 串一,每一個選擇性地於基底鍍上染 料以便連續地製造完成一彩色圖案影像。由於可以高速製 造此產品,此種步驟相當重要。 ▲二二圖儀用以說明-連串應用於單-干涉調制器製 =構:網::此延伸而製造干涉調制器陣列或其它微機電 、乡口構。網印來源j 9〇〇伤 來自滾筒的-塊材料上、二 例如透明塑膠的滾筒。 -單-二:表示區域包括,為了說明,只有 早 裝置。净雕圖幸I目 圖案。可,由呈古 於塑膠板内壓印出-凹陷 ^ S ”有蝕刻形成於表面上的適當突出ffi索& 金屬磁帶而完成。 、田大出圖案的一 金屬磁帶係固定於— 板,使塑膠變形而形成凹陷圖宰丄用充份的歷力壓印薄 膜器聰利用已知薄: 圖式1 906已說明之。錢 J用已知4獏沉積方法,例 _層。結果為包括氧化物、金屬、氧1077A-4732A-PF 42 1318325 Moving. The tongue-wound electronics 7L can be attached to either the superstructure or the substrate/waveguide to increase the power. Alternatively, the movable element can be fabricated as part of a superstructure, in particular a right-handed semiconductor, such as a stone or a stone. The printing manufacturing method is because it is a plane' and because many layers do not have the semi-V1 electronic characteristics requiring a special substrate, the interferometric modulator, like many microelectromechanical structures, can be used. The advantages of e-technology, like the printing industry. Such methods generally include a flexible and Μ $ + & and a continuous flat plate of paper or plastic. The reference screen printing 太人太,,土', generally includes a continuous roller of a base material, the base material is fed into the locust τ n , and the string one, each of which is selectively plated with a dye for continuous manufacture. Complete a color pattern image. This step is important because it can be manufactured at high speed. ▲Two-two diagram instrument used to illustrate - serial application to single-interference modulator system = structure: network:: This extension to create an array of interferometric modulators or other micro-electromechanical, township structure. Screen printing source j 9 bruises from the drum - on the block material, two, such as a transparent plastic roller. - Single-two: indicates that the area is included, for the sake of explanation, only the early device. The net carving is fortunate to the I mesh pattern. Alternatively, the embossing of the plastic plate is formed by embossing the embossed metal film on the surface. The metal tape of the pattern is fixed to the plate. Deformation of the plastic to form a concave pattern. The use of a sufficient lithographic embossing film using a known thin film: Figure 1 906 has been described. Money J uses a known 4 貘 deposition method, Example _ layer. The results include Oxide, metal, oxygen

1077A-4732A-PF 43 1318325 膜的四層薄膜的堆疊1910 調制器設計。一h lqi9 v 料相當於感應吸收干涉 装置1 912分配、固化日祖# 便對於這些層形成圖崇且對於光阻曝光,以 成圓案。只要形成了圖 貫施薄膜蝕刻。或者,刹田ρ ά + 於衣置1914中 於此範例中,於整個材料上掃描的雷射,允圖案。 料至大::乎Γ 率足夠可以汽化需要的材 大'為微未等級。調整雷射的頻率,如此口右… 上的材料作用,並沒右4 Α έ 戈此/、有和基底 工/又有和基底本身作用。因 基底輕微地受熱。 马π化太快, 於此4置範例中’所有的薄膜利用相 刻。如1 91 8所示,應用與署 的圖案而蝕 係另一種沉籍駐’、 使光阻被韌離。裝置1920 g' ° 、置,其沉積將成為干涉調制写之处m > 關於此層1922可使用鈕利盗之L構層。 具有極微小的應力,並 有制枓,顯不 藉0· β V 了利用各種PVD及PECVD技術沉 積H刀別利用裝置1 924、1926與1928 成既定圖案、蝕刻且剝離光 ^ " _除。假若此層為秒,關:此置目^ 钕刻劑,XeF2,而完成。社、T利用亂體相位 成此干涉調制器。 果為自我支撐薄膜結構腕形 封裝此完成裝置係# A mω ^ 板之卜U L 定弹性薄板1 933於基底薄 膜裝置聰鍍上密封的物V::其已利用鍍 t 1q,7 溥膜,例如金屬。兩薄板利用固定 #置1 937結合,以便完成封裝元件1 940。1077A-4732A-PF 43 1318325 Film stacking of four layers of film 1910 modulator design. A h lqi9 v material is equivalent to the inductive absorption interference device 1 912 distribution, solidification of the ancestor # will be formed for these layers and for the photoresist exposure, in order to round the case. As long as a thin film etching is formed. Alternatively, the brake field ρ ά + in the garment 1914. In this example, the laser scanned over the entire material allows the pattern. Expected to be large:: The rate is enough to vaporize the required material. Adjust the frequency of the laser, so the right side of the material... does not have the right 4 Α 戈 戈 戈 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 、 The substrate is slightly heated. The horse is too fast, and in this 4th example, all the films use the phase. As shown in 1 91 8 , the application of the pattern and the system's pattern eclipse another kind of sinking station, so that the photoresist is toughened. The device 1920 g' °, set, its deposition will become the location of the interferometric modulation m > About this layer 1922 can use the L-layer of the button. It has extremely small stress and has a system of enthalpy. It does not use 0·β V. It uses various PVD and PECVD techniques to deposit H-knife. It uses the devices 1 924, 1926 and 1928 to form a pattern, etch and strip light ^ " . If this layer is seconds, off: this is set to ^ 钕 engraving agent, XeF2, and completed. The Society and T use the chaotic phase to form this interferometric modulator. The result is a self-supporting film structure wrist-shaped package. This complete device is # A mω ^ plate-shaped UL-shaped elastic sheet 1 933 is sealed on the base film device C-plate: it has been plated with t 1q, 7 溥 film, For example metal. The two sheets are bonded using a fixed #1 937 to complete the package component 1 940.

1077A-4732A-PF 1318325 應力量测 殘餘應力係設計與製造微機電結構之一因素。於干涉 凋制益及其它結構中,其中於製造過程期間,結構構件已 經機械式地鬆開,殘餘應力決定構件的幾何形狀。 此干涉調制器,如一干涉元件,對於可移動構件之最 終幾何形狀之變化係敏感的。反射的,或於其它設計中為 穿透的色彩係空穴之空氣間隙之直接作用。結果,沿著空 φ 穴長度變化此距離,可導致不可接受的色彩變化。另一方 面,此特性可用以決定結構本身的殘餘應力,及於構件的 形變程度。任何材料的已知形變狀態提供測量材料中的殘 餘應力。電腦模擬程式及演算規則可利用關於形變狀態的 二維資料而決定。因此’干涉調制器可提供關於此估算的 裝置。 第20A圖與第2〇B圖顯示干涉調制器如何被應用於此 方法的範例。分別自側面及底部(透視基底)顯示干涉調制 鲁器2000與2002。分別為雙懸臂樑及單懸臂標形式。於此 範例中,結構材料不具有殘餘應力,並且兩構件顯示不具 有形變。當自底部透視基底,此裝置顯示均勻的色彩,其 藉由形成於其上的間隔層厚度決定。干涉調制器⑽4與 2006顯示具有應力梯度,因為於上面較下面更具有壓縮 力。結果此結構薄膜顯示變形,並且底部圖式顯示其造成 的色彩自然變化。例如’假若色彩區域2Qi6為綠色,而色 彩區域2014為藍色,這是因為其靠近基底。相反地,色彩 區域2018(顯示位於雙懸臂樑)為紅色時,這是因為遠離基1077A-4732A-PF 1318325 Strength measurement Residual stress is one of the factors in the design and manufacture of microelectromechanical structures. In interference with other structures, where the structural members have been mechanically loosened during the manufacturing process, the residual stress determines the geometry of the member. This interferometric modulator, such as an interference element, is sensitive to changes in the final geometry of the movable member. The direct effect of the air gap that is reflected, or otherwise penetrated by the color cavity. As a result, varying this distance along the length of the void φ can result in unacceptable color variations. On the other hand, this property can be used to determine the residual stress of the structure itself and the degree of deformation of the component. The known deformation state of any material provides a measure of the residual stress in the material. Computer simulation programs and calculation rules can be determined using two-dimensional data on the deformation state. Thus an 'interferometric modulator' can provide a means for this estimation. Figures 20A and 2B show how an interferometric modulator can be applied to an example of this method. The interferometric modulations 2000 and 2002 are shown from the side and bottom (perspective base), respectively. They are in the form of double cantilever beams and single cantilever. In this example, the structural material does not have residual stress and the two members show no deformation. When the substrate is viewed from the bottom, the device exhibits a uniform color which is determined by the thickness of the spacer layer formed thereon. The interferometric modulators (10) 4 and 2006 show a stress gradient because they have a compressive force above them. As a result, the structural film showed deformation, and the bottom pattern showed a natural change in color caused by it. For example, 'If the color area 2Qi6 is green and the color area 2014 is blue, it is because it is close to the substrate. Conversely, when the color area 2018 (the display is located in the double cantilever beam) is red, this is because the distance is far from the base.

1077A-4732A-PF 45 1318325 二步調制器2°°8及2010顯示處於-狀態,其中上面 較下面顯示更高張力應力的應力梯度。結構構件適當的變 /且改變色區域。於此範例中,當區域為 區域2020為紅色。 守 妯仕:第2〇B圊中’顯示一系統,其可用以快速地且精確 估异沉積薄膜之殘餘應力狀態。晶圓2〇3〇包 器結構陣列,其包括可變化長度與寬度的單一懸臂襟= 及又懸臂標薄膜。結構薄膜係選自機械及殘留應力已詳细 ;:的材料製造。許多材料皆可以,然受限於反射條件的 相當少,於此範例中的干涉調制器並未應用於顯示 目的。好的替代材料可包括晶體形式的材料(矽、 ::製造觀點為相容的,顯示某種程度的反射並且其機械特 之特徵為具有尚度精確性。製造且釋放此種 ''判試处 ^ ’因此其係獨立運作的。假若材料沒有應力,那麼: 構將顯示沒有色彩變化。然事實並非如此,因此色彩 狀態或色彩圖像可藉由使用高解析度攝像裝置2。34記 錄,可經由光學系統獲得高放大倍率的影像。 此攝像裝置與-電腦系統2G36連接,於其上存在硬體 並且可以記錄與處理影像資料。此硬體簡易地包括容易獲 :的南速處理板’以便於高速率執行數值計算。軟體可包 收集顏色資訊且計算表面變形的大量例行程序。核心程 ^利用變形資料,決定橫跨薄膜厚度的均勻應力與應力 梯度之最佳組合,可以產生所有種類。 使用的-種模式係產生一大堆、'未摻雜、測試晶片,1077A-4732A-PF 45 1318325 The two-step modulator 2°°8 and 2010 show a state in which the stress gradient of higher tensile stress is shown above. The structural member is appropriately changed and the color region is changed. In this example, when the area is area 2020 is red.守妯仕:第2〇B圊' shows a system that can be used to quickly and accurately estimate the residual stress state of a deposited film. The wafer 2 〇 3 〇 package structure array includes a single cantilever 襟 = and cantilevered film of varying length and width. The structural film is selected from the group consisting of mechanical and residual stresses. Many materials are possible, but limited by the few reflective conditions, the interferometric modulator in this example is not used for display purposes. Good alternative materials may include materials in crystalline form (矽, :: manufacturing viewpoint is compatible, exhibiting some degree of reflection and its mechanical characteristics are characterized by a degree of precision. Manufacturing and releasing such a 'question' ^^ Therefore it works independently. If the material is not stressed, then: the structure will show no color change. However, this is not the case, so the color state or color image can be recorded by using the high-resolution camera 2.34, High-magnification images can be obtained via the optical system. This camera is connected to the computer system 2G36, which has hardware and can record and process image data. This hardware easily includes the easy-to-obtain: South-speed processing board' In order to perform numerical calculations at a high rate, the software can collect a large number of routines for collecting color information and calculating surface deformation. The core process uses the deformation data to determine the optimal combination of uniform stress and stress gradient across the thickness of the film, which can generate all The type of pattern used produces a large number of 'undoped, test wafers,

1077A-4732A-PF 46 1318325 其具有未沉積應力狀態之詳細記錄,被收藏以方便使用。 當有需要測定沉積薄膜之殘餘應力時,選擇一測試晶片且 薄膜沉積於其頂端。沉積薄膜改變結構的幾何及其彩色影 像。利用常駐於電腦系統内的軟體,可比對測試晶片之前 後兩個彩色影像且精確地估算沉積薄膜内的殘餘應力。亦 可設計於沉積完成後,啟動測試結構。啟動新沉積的薄膜 期間觀察其作用,可提供更多有關殘餘應力狀態的資料,、 如同於整個啟動過程内的薄膜變化特性。 當沉積薄膜時,此技術可被用於測定薄膜應力。適者 :::變沉積系統,產生一光路徑使得影像系統可即時觀; 影像之變化。這形成-即時回饋系統,用 體可參考測試3曰此:法控制殘餘應力。軟體與硬 可別忒曰曰片的週期,並且當成長薄膜時, 裝置操控器改變條件。關於量測殘餘庫力馨"’ 其它技術,不論是.右…二餘應力’整個系統優於 且複雜的干、η 有依賴電子機械啟動,或者利用昂貴 且複雜的干涉錢量測製造結構㈣形量。 驅動電子至报大的裝置陣列 别者㈣供 福性。後者於觀察下受限於薄膜的位移之不精 雜的外部光學與硬體。 、性,以及需要複 不連續薄膜 另一種具有令人關注特性 為非同質的。這此舊腔了 糸種溥膜’其結構 _ <二4臈可以數種型 類成不連續薄膜。第2 現,並且應將其歸 兒明一種不連續薄骐。基底2!001077A-4732A-PF 46 1318325 It has a detailed record of the undeposited stress state and is conveniently stored for use. When it is necessary to determine the residual stress of the deposited film, a test wafer is selected and a film is deposited on top of it. The deposited film changes the geometry of the structure and its color image. Using software resident in the computer system, the two color images before and after the test wafer can be compared and the residual stress in the deposited film can be accurately estimated. It can also be designed to start the test structure after the deposition is completed. Observing its effect during the initiation of a newly deposited film provides more information about the state of the residual stress, as is the film's changing characteristics throughout the startup process. This technique can be used to determine film stress when depositing a film. The fittest ::: The deposition system creates a light path that allows the image system to be instantly viewed; the image changes. This forms an instant feedback system that can be used to refer to the test 3: This method controls the residual stress. Soft and hard can be different from the cycle of the cymbal, and when the film is grown, the device manipulator changes conditions. Regarding the measurement of residual Ku Lixin's 'other technologies, whether it is right or two stresses' the whole system is superior and complex dry, η has dependence on electromechanical start-up, or uses expensive and complicated interference money to measure the manufacturing structure. (4) Shape. Drive the electronics to the large array of devices. (4) For blessing. The latter is observed by the unconventional external optics and hardware that are limited by the displacement of the film. , sex, and the need for complex discontinuous films. Another feature of interest is non-homogenous. In this old cavity, the ruthenium film's structure _ < two 4 臈 can be several types of discontinuous films. The second is, and should be, a non-continuous thin enamel. Base 2!00

1077A-4732A-PF 47 1318325 可為-金屬、介電或半導體,其具有餘刻至其表面的不佳 輪廓、,輪廓包括各個結構外觀且應具有一高度⑴〇,為 光波長之某些分,係利用黃光微影及化學姓刻技術 而被钮刻,以便獲得近似於藉由2m(三角形)、21〇6(圓 ^)及2108(錐形)描述的高度。任何個別高度之基底有 ^直徑亦相當於圖案高度等級。當每—輪_微不同時, 二-有相同的特性’例如當一光束自入射處橫越進入基 底’折射率逐漸自入射介質變化至薄膜基底21〇〇。與多層 薄膜結合的鍵膜比較,此種結構當作較佳的抗反射鍍膜使 :’因t其與角度量測無關。因此,對於更大的入射角度, 〃、維持高度地抗反射。 第21B圖揭露一種鍍膜212〇,其已沉積於基底㈣ :’可4金屬、介電質或半導體。於此範例中,薄 早期階段形成’大約小於1_埃厚度。於大多數沉 期間,薄膜經歷-階段式結晶過程,形成材料的區 連大’直到彼此結合成-體,並且於某些點形成-連續相。圖2124顯示此薄膜之上視圖。於較早階 的薄膜光學特性與連續薄膜不相同。對於金屬而言,薄膜 更容易較連續相同特性者顯示出更高的損耗。 、 f 2!C圖說明不連㈣膜的第三種型式。於 中,相㈣已經於基底2132上沉積至—厚戶,至小」 可將其視為連續。利用與上述自我結合方法㈣的 ㈣宰於材财形成一、、次波長,(就是直徑小於波長)孔 。於此範例中’高分子可當作將敍刻圖案移轉至底 1077A-4732A、pp 48 1318325 # 卜材料的光罩 " 1又W挪別子匕洞。因 為材料是連續的,但是被穿孔,並不與第21β圖的較早階 段薄膜相同。相反地,其光學特性不同於未钱刻薄膜,直 中入射光束經歷更小的損耗,並且根據表面顯示穿透的峰 值。此外,孔洞的幾何結構,如同入射角度與入射介面之 折射率’可操控穿透光的光譜特性。2⑶顯示此薄膜之上 視圖。此類的薄媒已於Tae JinKiffl的論文''CO* — opt-al transmission through metals perforated with =™e_h〇learraysW月。同時,其屬於 結構,不同於PBG^ 取 所有二種不連續薄膜可庙 立+ 寻膘了應用於干涉調制器結構中。这 思味’其可應用於干涉綱在 A A 周制為結構之靜態且/或可移動部位 中的一種或多種的材料薄^ *是根據個別薄膜的二::的三種獨特的特性,主 組合。其可與干心=二代替變化厚度的薄膜 用。於很簡單的範例中,此等薄學j機械7^件結合應 表面導電或光學干涉變化,導致並直:::學特性可經由 靠近其它薄膜。這可藉由直接改變薄:的、導它, 由改變其周圍介質的折射率而 、 ,且/或藉 益中,利用此更簡單的 個干"調制 複雜的光學變化。 t間易的製造㈣,獲得更 雖然本發明已以較佳實施 限定本發明,任何熟習此項技蔽者^上’、然其並非用以 神和範圍内,當可作 " 在不脫離本發明之精 作更動與潤飾,因此本發明之保護範圍1077A-4732A-PF 47 1318325 can be - metal, dielectric or semiconductor with a poor profile engraved to its surface, the profile including the appearance of each structure and should have a height (1) 〇, which is a fraction of the wavelength of light It is engraved with yellow lithography and chemical surrogate techniques to obtain a height similar to that described by 2m (triangle), 21〇6 (circle ^), and 2108 (taper). The base of any individual height has a diameter which is also equivalent to the height level of the pattern. When each-wheel is slightly different, the second-having the same characteristic 'e.g., when a light beam traverses from the incident into the substrate', the refractive index gradually changes from the incident medium to the film substrate 21A. Compared with the bonding film of the multilayer film, this structure is regarded as a preferred anti-reflection coating: 'Because t is independent of the angle measurement. Therefore, for a larger angle of incidence, 〃, maintain a high degree of anti-reflection. Figure 21B illustrates a coating 212 that has been deposited on a substrate (4): '4 metal, dielectric or semiconductor. In this example, the early stages of thin formation 'are less than about 1 angstrom thick. During most of the sinking, the film undergoes a -stage crystallization process, forming regions of the material that are large until they are combined into a body and form a continuous phase at some point. Figure 2124 shows a top view of the film. The optical properties of the film at an earlier stage are not the same as those of the continuous film. For metals, the film is more prone to exhibit higher losses than the same continuous characteristics. , f 2! C diagram illustrates the third type of film without (4). In the middle, the phase (4) has been deposited on the substrate 2132 to a thicker household, which is considered to be continuous. Using the above-mentioned self-binding method (4), (4) slaughtering the material to form the first and second wavelengths (that is, the diameter is smaller than the wavelength). In this example, the polymer can be used as a mask to transfer the pattern to the bottom 1077A-4732A, pp 48 1318325 # 卜 material. Since the material is continuous but perforated, it is not the same as the earlier stage film of the 21β chart. Conversely, its optical properties are different from those of the unfilled film, and the straight-injected beam experiences less loss and shows the peak of the penetration according to the surface. In addition, the geometry of the hole, like the angle of incidence of the incident angle to the incident interface, manipulates the spectral properties of the transmitted light. 2(3) shows the top view of this film. Such thin media has been published in Tae JinKiffl's paper ''CO*- opt-al transmission through metals perforated with =TMe_h〇learraysW month. At the same time, it belongs to the structure, which is different from PBG^. All two kinds of discontinuous films can be applied to the interferometric modulator structure. This is considered to be applicable to the material of one or more of the static and/or movable parts of the structure in the AA system. * According to the three unique characteristics of the individual film:: the main combination . It can be used with a dry heart = two instead of a film of varying thickness. In a very simple example, these thin-film joints should be surface-conducting or optically interfering, resulting in a straight-through::: learning properties can be passed close to other films. This can be done by directly changing the thinness, guiding it, by changing the refractive index of the surrounding medium, and/or by taking advantage of this simpler " modulation of complex optical changes. Manufacture of t-easy (4), although the invention has been defined by the preferred embodiment, any skilled person is skilled in the art, but it is not used within the scope of God and can be used as The invention is improved and retouched, so the scope of protection of the present invention

1077A-4732A-PF 49 1318325 當視後附之申請專利範圍所界定者為準。 【圖式簡單說明】 第1A圖係一顯示器基板之剖面圖式,其具有抗反射鍍 膜及結合—體的辅助光;第則揭露另-種關於輔助光的 結構; 第2圖詳細顯示微機械弧光燈源的製造流程; ”第3圖說明顯示器内的干涉調制器陣列的偏壓中心的 驅動結構; 第4Α圖係一圖式’其根據 '、基底+顏『觀念說明彩 色顯不器的結構;第4Β圖揭露一糸#的 底声可舌站、 口询路序、統的方塊圖式,其提供 -色τ重新刀配顯示中心產品;第4c圖說 於-般用途的顯示中心產品; 述觀心應用 示自:運涉調制器幾何圖式,於未啟動狀態中顯 :峨電運作中減少光學作用;第㈤圖係 訪於啟動狀態;第5C圖係一圖式, 干"調制 於黑與白的狀態的運作⑽圖係I::干設計 狀態的運作; ’ $許多色彩 第6A圖顯示干涉調制器的圖式,相同地 =少光學作用,不過支撐結構被隱藏; :運作 同的設計處於啟動狀態; 口係顯示相 第7A圖說明使用非等向性應力構件的 於-狀態中;…顯示相同的干涉調制器處二:制器處 中; 、另·'狀態1077A-4732A-PF 49 1318325 The date defined in the attached patent application shall prevail. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1A is a cross-sectional view of a display substrate having an anti-reflection coating and a combined-body auxiliary light; the first discloses another structure for auxiliary light; and FIG. 2 shows the micro-mechanical in detail. The manufacturing process of the arc lamp source; "Fig. 3 illustrates the driving structure of the bias center of the interferometric modulator array in the display; the fourth figure is a figure based on the 'base + face' concept to illustrate the color display The structure; the fourth picture reveals the bottom sound of a 糸# can be tongue station, the interrogation path sequence, the unified block diagram, which provides - color τ re-tooling display center product; Figure 4c shows the general purpose display center product; The application of the mind is shown in: the geometric pattern of the modulator, which is displayed in the unactivated state: the optical effect is reduced in the operation of the 峨; the (5) is accessed in the startup state; the 5C is a pattern, dry " Operation in the black and white state (10) Figure I:: Operation of the dry design state; '$ Many colors Figure 6A shows the pattern of the interferometric modulator, the same = less optical effect, but the support structure is hidden; Operating the same design office Activated state; display system with a first opening 7A in FIG instructions anisotropic stress member in - state; ... interferometric modulator display the same at two: in the system device; and the other · 'state

1077A-4732A-PF 50 1318325 第8A圖說明干涉調制哭 制益’其藉由旋轉啟動;第犯圖 揭硌旋轉式干涉調制器設計的製造流程; 第9A圖係一微機電開關 a ]關的方塊圖式;第9B圖係根據 微機電開關的列驅動器的方堍 去 鬼圖式’苐9C圖係根據微機電 ΜΛΜη μ Λ ’第9D圖係根據微機電開關的 NAND閘之方塊圖式;第9 圖係顯示具有利用邏輯與驅動 "件之微機電的顯示系統的方塊圖式; 第10A圖係一圖式,盆想带 ,α /、揭路—微機電開關的結構、製 造與操作;第1 〇Β、1 〇C圖$昍; 表 第11Α圖係一圖式,里觀_ r .. . ^ . ,、顯不依據2-β光電結構的微型 把例,第11Β圖係週期性的9 n 期性的2 — D光電結構的圖式; 第1 2圖係一圖式,复掘带 ,、揭路—3-D光電結構的範例; 弟13A圖係一圖式,並约拍点 結構的干涉調制器;第13B、: f於未啟動狀態具有微型 動狀態1 UC圖係顯干呈=相同的干涉調制器處於啟 涉調制器; H、有週期性的2-D光電結構的干 第i4A圖係說明干涉調制器設計,其當作 使用;第14B圖係顯示此種 予開關 -X. °十的各種變化,當作一弁4¾ 衮減器使用; 田F光學 第15A圖係—干涉調制器設計的圖式 學開關或一光學退耦考.第 ,、b為—光 ,, 。,弟15B圖說明此等干涉調制3! θ 如何結合而當作—ΝΧΝ光學開關使用; 巧〜 第1 6圖顯示可铜在丨丨工、土 Α ^ ^ 制干^调制器結構的製造流程; 第1 7 A圖說明可,細工、土 1 凋制干涉调制器結構如何可應用於波1077A-4732A-PF 50 1318325 Figure 8A illustrates the interferometric modulation crying benefit 'which is initiated by rotation; the first is to illustrate the manufacturing process of the rotary interferometric modulator design; the 9A is a microelectromechanical switch a ] off Block diagram; Figure 9B is based on the square drive of the MEMS switch. The 苐9C diagram is based on the micro-electromechanical ΜΛΜμ μ Λ '9D diagram according to the NAND gate block diagram of the MEMS switch; Figure 9 shows a block diagram of a display system with logic and drive &MEMS; Figure 10A is a diagram, a basin, a /, Jielu - MEMS switch structure, manufacturing and Operation; the first 〇Β, 1 〇C diagram $昍; Table 11 Α diagram is a diagram, the view _ r .. . ^ . , , the micro-handle based on the 2-β photoelectric structure, the 11th A pattern of periodic 9 n-phase 2-D photoelectric structures; Figure 12 is a diagram of a pattern, a dig-removal zone, and an unvehicle-3-D photoelectric structure; And about the structure of the interferometric modulator; 13B, : f in the unactivated state has a micro-motion state 1 UC diagram is dry = the same interferometric modulator is in the open modulator; H, the dry i4A diagram with periodic 2-D optoelectronic structure illustrates the interferometric modulator design, which is used; 14B shows the pre-switch - Various changes of X. °10, used as a 43⁄4 reducer; Field F optics 15A - the graphical switch of the interferometric modulator design or an optical decoupling test. The first, b is - light, , . Figure 15B shows how these interferometric modulations 3! θ are combined and used as ΝΧΝ optical switches; 巧 ~ Figure 16 shows the manufacturing process of copper in the completion, soil ^ ^ dry ^ modulator structure Figure 1 7 A illustrates how the fine-grained, soil-induced interferometric modulator structure can be applied to waves.

1〇77A-4732A-PF 1318325 長選擇開關丨第1 7B圖進一步說明波長選 久TC k擇開關如何可廍 用於固態元件;第17C圖說明凸塊連 ,ω 逆、,σ 7Μ牛如何積體化; 第Α圖係一兩通道等化器/混合器的概要圖式;第 18Β圖係說明等化器’混合器如何使用干涉調制器; 第1 9圖係一圖式’其說明—連續 口 硬、,貝的網狀基礎的製造流 程; 第2 0 A、2 Ο Β圖說明干涉調制刺分处& 利益利忒結構如何使用於應 力量測;以及 第21A圖至第21C圖描述。 【主要元件符號說明】 100~AR 鍍膜; 102〜玻璃層; 104〜弧光燈陣列; 106〜玻璃基底; 10 7 ~介面; 108〜干涉調制器陣列 109〜入射光; 11 0〜光路徑; 111~反射器層; 112〜基底; 114 ~干涉調制器陣列; 116〜光源; 118~光導; 120〜準直器; 122~光線; 12 6〜薄膜堆積; 128~觀察者; 2 0 0〜玻璃層; 201〜反射器碗狀物; 202〜犧牲層; 204~反射器/複金屬層 y 205〜光線; 206〜沉積電極層; 300〜磁滯曲線; 3〇2〜時間圖; 1077A-4732A-PF 52 1318325 400~像素; 404~綠色; 408〜白色; 412〜執行控制器; 418~可攜式電子產品; 422〜記憶體; 426~手寫輸入; 432〜音響介面; 5 0 2〜電極棒, 505〜光學空穴; 508〜第二鏡面; 511〜既定頻率光; 521〜黑狀態; 527〜綠色峰值; 6 0 6〜干涉調制器; 7 0 2〜鋁薄膜; 70 6〜入射光; 71 0〜平板; 71 8〜薄材料層; 8 0 2〜電極; 8 0 8 ~支撐棒; 812〜支撐遮光器; 816〜支撐結構; 820〜觀察者; 402〜紅色; 406〜藍色; 410~元件; 414、416〜驅動電子電路 420〜核心處理器; 424〜RF或IR介面; 430~影像輸入裝置; 5 0 0〜基底; 504〜絕緣薄膜; 506〜膜狀物/鏡面; 510〜透明上部構造; 512〜觀察者; 525〜藍色峰值; 529〜紅色峰值; 608〜薄膜/鏡面; 7 0 4〜堆積層; 708〜部份頻率的光; 716〜支撐調整片; 8 0 0〜基底; 804〜共同匯流排電極; 81 0〜旋轉樞紐; 81 4〜輔助電極; 81 8〜遮光器; 8 3 0〜基底;1〇77A-4732A-PF 1318325 Long selection switch 丨1 7B further explains how the wavelength selection TC k switch can be used for solid-state components; Figure 17C illustrates the bump connection, ω inverse, σ 7 Μ The first diagram is a schematic diagram of a two-channel equalizer/mixer; the 18th diagram illustrates how the equalizer 'mixer uses an interferometric modulator; the nineteenth diagram is a diagram' The manufacturing process of the continuous port hard, and the mesh foundation of the shell; the 2 0 A, 2 Β diagram illustrates how the interference modulation point & benefit structure is used for stress measurement; and 21A to 21C description. [Main component symbol description] 100~AR coating; 102~glass layer; 104~arc array; 106~glass substrate; 10 7 ~ interface; 108~interferometric modulator array 109~incident light; 11 0~light path; ~ reflector layer; 112 ~ substrate; 114 ~ interferometric modulator array; 116 ~ light source; 118 ~ light guide; 120 ~ collimator; 122 ~ light; 12 6 ~ film stack; 128 ~ observer; 2 0 0 ~ glass Layer; 201 ~ reflector bowl; 202 ~ sacrificial layer; 204 ~ reflector / complex metal layer y 205 ~ light; 206 ~ deposited electrode layer; 300 ~ hysteresis curve; 3 〇 2 ~ time chart; 1077A-4732A -PF 52 1318325 400~pixel; 404~green; 408~white; 412~execution controller; 418~portable electronic product; 422~memory; 426~handwriting input; 432~audio interface; 5 0 2~electrode Rod, 505~ optical cavity; 508~second mirror; 511~determined frequency light; 521~black state; 527~green peak; 6 0 6~interferometric modulator; 7 0 2~aluminum film; 70 6~incident light ; 71 0~ flat; 71 8~ thin material layer; 8 0 2~ electrode; 8 0 8 ~ support rod; 812 ~ support shutter; 816 ~ support structure; 820 ~ observer; 402 ~ red; 406 ~ blue; 410 ~ components; 414, 416 ~ drive electronic circuit 420 ~ core processor; ~ RF or IR interface; 430 ~ image input device; 5 0 0 ~ substrate; 504 ~ insulating film; 506 ~ film / mirror; 510 ~ transparent upper structure; 512 ~ observer; 525 ~ blue peak; Red peak; 608~ film/mirror; 7 0 4~ stacked layer; 708~ part of the frequency of light; 716~ support tab; 8 0 0~ substrate; 804~ common bus electrode; 81 0~ rotary hub; 4 ~ auxiliary electrode; 81 8 ~ shutter; 8 3 0 ~ base;

1077A-4732A-PF 1318325 832 ' 834、836〜犧牲隔間; 838〜柱子/旋轉枢紐/遮光器材料;1077A-4732A-PF 1318325 832 '834,836~sacrificial compartment; 838~column/rotary hub/shader material;

840〜支擇柱; 844〜匯流排電極; 848〜支禮柱; 852〜遮光器; 902〜控制信號; 906〜輸入電壓veQll ; 910〜輸入電壓Vbias ; 916~輸入電壓VselFQ ; 920〜輸出端; 9 2 6〜控制邏輯; 9 3 0〜顯示陣列; 842~遮光器; 846〜遮光反射器; 8 5 0 ~扭力臂; 900〜輸入端; 904〜輸出端; 908〜輸入電壓Vw。; 914〜輸入電壓yselF1 ; 918 ~接地; 924〜行驅動器; 928〜列驅動器; 932〜邏輯裝置;840 ~ support column; 844 ~ bus bar electrode; 848 ~ branch column; 852 ~ shutter; 902 ~ control signal; 906 ~ input voltage veQll; 910 ~ input voltage Vbias; 916 ~ input voltage VselFQ; 920 ~ output ; 9 2 6 ~ control logic; 9 3 0 ~ display array; 842 ~ shutter; 846 ~ shading reflector; 8 5 0 ~ torque arm; 900 ~ input; 904 ~ output; 908 ~ input voltage Vw. ; 914 ~ input voltage yselF1; 918 ~ ground; 924 ~ row driver; 928 ~ column driver; 932 ~ logic device;

9 4 0 ~基礎切換方塊; 1002〜犧牲間 10 0 6〜閘極結. 101 0 ~源極桿 1016〜箭號; 934 、 936 、 938 、 1〇〇〇~基底; 1 004〜箭號; 1 0 0 8 ~没極結構; 1012〜凹槽; 10 2 4 ~汲極; I 0 2 8〜切換桿; 10 4 0 ~絕緣器; 1100〜基底; 1102〜微環狀共振器; II 0 8〜缺陷; 1026〜源極; 1 038〜接觸桿; 1042〜切換桿; 1101、1103〜XYZ 座標 11 0 6〜陣列; 1 200〜基底;9 4 0 ~ basic switching block; 1002 ~ sacrificial interval 10 0 6 ~ gate junction. 101 0 ~ source pole 1016 ~ arrow; 934, 936, 938, 1〇〇〇 ~ base; 1 004 ~ arrow; 1 0 0 8 ~ no pole structure; 1012 ~ groove; 10 2 4 ~ drain; I 0 2 8 ~ switching rod; 10 4 0 ~ insulator; 1100 ~ substrate; 1102 ~ micro ring resonator; II 0 8~defect; 1026~source; 1 038~contact rod; 1042~switching rod; 1101, 1103~XYZ coordinates 11 0 6~ array; 1 200~ substrate;

1077A-4732A-PF 54 1318325 1202〜三維週期結構;1 204~缺陷; 1301〜波導; 1 303〜基底; 1 3 0 5 ~剖面圖; 1 308〜光束; 1311〜圓柱; 1314〜共振器; 1 326、1 328〜未干涉的光 1 329〜光; 1400〜鋁薄膜; 1 406〜干涉調制器; 141 0 ~側視圖; 1420〜薄膜; 1429〜反射區域; 1431〜重疊蹤跡; 14 3 4 ~側視圖; 1437〜反射區域; 1440〜反射光束; 1501~透明光學支座; 1 503~導體; 1 505〜窗; 1510~光束; 151 4〜側視圖; 1 522〜光束;1077A-4732A-PF 54 1318325 1202~3D periodic structure; 1 204~ defect; 1301~waveguide; 1 303~substrate; 1 3 0 5 ~ sectional view; 1 308~beam; 1311~column; 1314~resonator; 326, 1 328~ uninterfered light 1 329~ light; 1400~aluminum film; 1 406~interferometric modulator; 141 0 ~ side view; 1420~ film; 1429~reflection area; 1431~overlap trace; 14 3 4 ~ Side view; 1437~reflection area; 1440~reflected beam; 1501~transparent optical support; 1 503~conductor; 1 505~window; 1510~beam; 151 4~side view; 1 522~beam;

1 302~波導; 13〇4~薄膜; 1 306~微環狀共振器; 1310〜輸出光束; 1312〜有限的垂直空氣間隔; 1315〜薄膜; j 1 330、1 332〜波導; 1402~材料堆積層; 1 408〜光束; 1414 ~側視圖; 1428〜箭號; 1 430〜光束; 1 432〜光束; 1 436〜側視圖; 1438〜完全吸收狀態; 1500〜支撐結構; 1 5 0 2〜鏡面; 1 504〜基底; 1 5 0 6〜切換器; 151 2〜側視圖; 1 5 2 0 ~光纖搞合器; 1 526〜侧視圖; 1077A-4732A-PF 55 13183251 302 ~ waveguide; 13 〇 4 ~ film; 1 306 ~ micro ring resonator; 1310 ~ output beam; 1312 ~ limited vertical air gap; 1315 ~ film; j 1 330, 1 332 ~ waveguide; 1402 ~ material accumulation Layer; 1 408 ~ beam; 1414 ~ side view; 1428 ~ arrow; 1 430 ~ beam; 1 432 ~ beam; 1 436 ~ side view; 1438 ~ fully absorbed state; 1500 ~ support structure; 1 5 0 2 ~ mirror ; 1 504 ~ substrate; 1 5 0 6 ~ switcher; 151 2 ~ side view; 1 5 2 0 ~ fiber optic adapter; 1 526 ~ side view; 1077A-4732A-PF 55 1318325

1 528〜再耦合鏡面; 1531〜方向性切換器陣列 1 532〜輸出光纖耦合器; 1 5 3 5〜基底; 1 602~導電接觸墊; 1 6 0 6〜犧牲層; 1610〜絕緣層; 1614〜薄膜堆積; 1616〜中心孔穴; 1 702〜光束; 1 706〜光學超結構; 1 709~光束; 1712〜抗反射鍍膜; 1716〜鏡面; 1 738〜感測器; 1 7 5 Q ~光束; 1756〜再耦合鏡面; 1 760〜再耦合鏡面; 1764~ICs ; 1 768~再耦合鏡面; 1 772〜雙方向光路徑; 1 8 01〜光; 1803~光; 1806〜再搞合鏡面; 1 530〜光束; 1 536〜線性陣列; 1 604~鏡面; 1 608〜鏡面; 1612〜第二接觸墊; 1615〜支撐物; 1618〜薄膜堆積; 1 704〜可調制濾波器; 1 708〜光; 1710~鏡面; 1714〜基底; 1717〜鏡面; 1739〜第二可調制濾波器 1 752〜可調制濾波器; 1 758〜光束; 1762~ICs ; 1 76 6 ~鏡面; 1 770〜基底; 1800~光纖搞合器; 1 802〜抗反射鍍膜; 1 805〜可變衰減器; 1 807〜通道; 1077A-4732A-PF 56 13183251 528~recoupling mirror; 1531~directional switcher array 1 532~output fiber coupler; 1 5 3 5~substrate; 1 602~conductive contact pad; 1 6 0 6~ sacrificial layer; 1610~insulation layer; 1614 ~ film stacking; 1616 ~ center hole; 1 702 ~ beam; 1 706 ~ optical superstructure; 1 709 ~ beam; 1712 ~ anti-reflective coating; 1716 ~ mirror; 1 738 ~ sensor; 1 7 5 Q ~ beam; 1756~re-coupling mirror; 1 760~re-coupling mirror; 1764~ICs; 1 768~re-coupling mirror; 1 772~bidirectional light path; 1 8 01~ light; 1803~ light; 1806~ re-engaged mirror; 530~beam; 1 536~ linear array; 1 604~mirror; 1 608~mirror; 1612~second contact pad; 1615~support; 1618~film stack; 1 704~ modulatable filter; 1 708~ light; 1710~mirror; 1714~substrate; 1717~mirror; 1739~second modulatable filter 1 752~ modulatable filter; 1 758~beam; 1762~ICs; 1 76 6 ~mirror; 1 770~substrate; 1800~ Fiber optic adapter; 1 802 ~ anti-reflective coating; 1 805 ~ variable attenuator; 1 807~ Tao; 1077A-4732A-PF 56 1318325

1 808〜可調制濾波器; 1810~鏡面; 1812〜衰減器; 1815〜光束; 1817〜光束; 1819〜光束; 1 824〜解辆合切換器; 1 829〜光學超結構; 1 9 0 0〜網印來源; 1 906〜圖式; 1910〜薄膜的堆疊; 1914〜裝置; 1918~圖式; 1 922〜干涉調制器之結構 1 924〜裝置; 1 928〜裝置; 1 932〜自我支撐薄膜結構 1 933〜彈性薄板; 1 936~連續滚筒; 20 00〜干涉調制器; 2004〜干涉調制器; 2008〜干涉調制器; 2014〜色彩區域; 2018〜色彩區域; 1 80 9〜第二可調制濾波器; 1811〜再相|合鏡面; 1813〜光學停止器; 1816~光束位置改變器; 1818〜位置改變器; 1820〜解耦合切換器; 1 828〜光結合器; 1 830~感測器/吸收器; 1 904〜浮雕圖案工具; 1908〜鍍膜器; 1912~裝置; 1916〜裝置; 1 920~裝置; 層; 1926~裝置; 1 930~裝置; , 1 934〜鍍膜裝置; 1 940〜封裝元件; 2002〜干涉調制器; 20 06 ~干涉調制器; 2010〜干涉調制器; 2016〜色彩區域; 2020〜區域; 1077A-4732A-PF 57 1318325 2022 〜 區域, 203(l· ~晶圓, 2034- 攝像裝置; 2036 〜電腦系統; 2100 〜 基底; 2104- 、三角形; 2106 〜 圓柱形; 2108- 錐形; 2110- 高度; 2120- 、鍍膜; 2122- 基底; 2124· …薄膜; 2130- 薄膜; 2132- '基底; 2136 〜 薄膜。 1077A-4732A-PF 581 808~ modulatable filter; 1810~mirror; 1812~attenuator; 1815~beam; 1817~beam; 1819~beam; 1 824~ solution hybrid switch; 1 829~ optical superstructure; 1 9 0 0~ Screen printing source; 1 906~ pattern; 1910~ film stacking; 1914~ device; 1918~ pattern; 1 922~ interferometric modulator structure 1 924~ device; 1 928~ device; 1 932~ self-supporting film structure 1 933~elastic sheet; 1 936~continuous roller; 20 00~interferometric modulator; 2004~interferometric modulator; 2008~interferometric modulator; 2014~color area; 2018~color area; 1 80 9~second modulatable filter 1811~re-phase|closed mirror; 1813~optical stop; 1816~beam position changer; 1818~position changer; 1820~decoupled switcher; 1 828~optical coupler; 1 830~sensor/ Absorber; 1 904~embossed pattern tool; 1908~ coater; 1912~ device; 1916~ device; 1 920~ device; layer; 1926~ device; 1 930~ device; , 1 934~ coating device; Component; 2002~ interferometric modulator; 20 06 ~ dry </ br> </ br> </ br> </ br> </ br> </ br> </ br> Substrate; 2104-, triangle; 2106~cylindrical; 2108-conical; 2110-height; 2120-, coating; 2122- substrate; 2124·...film; 2130-film; 2132- 'substrate; 2136~ film. 1077A- 4732A-PF 58

Claims (1)

修正曰期:98.9.9 13185¾139。。9號中文_專利範圍修正本 十、申請專利範圍: i.一種微機電系統裝置之製造方法,—包括一.一 ‘··一:一 提供一可撓式基底;以及 於上述可撓式基底上設置一或多層薄膜,其中上述薄 膜包括: —第一鏡面,至少用以部分地反射入射光; 一第二鏡面,至少用以部分地反射入射光,其中上述 第一鏡面係設置於上述可撓式基底與上述第二鏡面之間, 並且上述第一、第二鏡面中之一者係相對於另一鏡面於一 第一位置以及一第二位置間移動,上述第一位置係與上述 另—鏡面相距一第一距離,而上述第二位置係與上述另— 鏡面相距一第二距離。 2.如申請專利範圍第丨項所述之微機電系統装置之製 &amp;方法’其中上述可撓式基底包括一連續平板。 3·如申s青專利範圍第2項所述之微機電系統裝置之製 &amp;方法,其中上述可撓式基底包括一塑膠材質之連續平板。 4·如申請專利範圍第2項所述之微機電系統裝置之製 造方法,其中上述可撓式基底包括一紙類材質之連續平板。 5.如申請專利範爵第丨項所述之微機電系統裝置之製 造方法,其中上述薄膜包括一氧化層、一金屬層以及—犧 牲層》 6_如申請專利範圍第1項所述之微機電系統裝置之製 方法,其中上述第一鏡面允許部分入射光通過,並且於 上述第二鏡面係不透光。。 1077A-4732A-PF3 59 1318325 (f年(月1f 曰修(更)正本I Μ----- ..._________ 如申請專利範圍第1項所述之微機電系統裝置之製 造方法’其中上述可撓式基底上之上述薄膜包括一氧化層 並且上述氧化層係設置於上述第一鏡面與第二鏡面之間。 8.如申請專利範圍第1項所述之微機電系統裝置之製 方法’更包括藉由接合(b〇n(jing) —可撓式平板至上述可 挽式基底’對上述微機電系統裝置進行封裝。 9·如申請專利範圍第8項所述之微機電系統裝置之製 造方法’其中上述可撓式平板係包括一可撓式材質之連續 滾筒。 10·如申請專利範圍第8項所述之微機電系統裝置之 製造方法’其中上述可撓式平板係由一密封薄膜所覆蓋。 U.如申請專利範圍第10項所述之微機電系統裝置之 製造方法’其中上述密封薄膜由金屬所構成。 12. 如申請專利範圍第1項所述之微機電系統裝置之 製造方法,其中上述微機電系統裝置係為一干涉調製器。 13. 如申請專利範圍第1項所述之微機電系統裝置,其 中上述第二鏡面允許部分入射光通過,並且於上述第一鏡 面係不透光。 .14: 一羞癥81—系統裝ϊ「 ------------- 可挽式基底;以及 —第一鏡面,至少用以部分地反射入射光; —第二鏡面’至少用以部分地反射入射光,其中上述 第一鏡面係設置於上述可撓式基底與上述第二鏡面之間, 並且上述第一、第二鏡面中之一者係相對於另—鏡面於— 1077A-4732A-PF3 60 1318325 ;::置…第二位置間移歴1襲i上述 &amp;面相5巨—第一距_,而1述第二位置係貞上述另一 鏡面相距一第二距離。 盆5’如申請專利範圍第14項所述之微機電系統裝置, '、 迷微機電系統裝置係為一干涉調製器。 16 λ .申請專利範圍第14項所述之微機電系統裝置, 其中上、 ^ 鏡面允許部分入射光通過,並且於上述第二 鏡面於上说贫 Λ* 处第一、第二位置間之移動量,係用以調節由上 述第一、筮_ &amp; 弟一鏡面所反射之光所導致干涉。 17. 如申請專利範圍第14項所述之微機電系統裝置, 其中上述可撓式基底由塑膠或紙類材料所構成。 18. 如申請專利範圍第14項所述之微機電系統裝置, 更包括一氧化層設置於上述第一鏡面與上述第二鏡面之 間。 19. 如申請專利範圍第14項所述之微機電系統裝置, 更包括一可撓式平板,接合(bonding)至上述可撓式基底以 便封裝住上述微機電系統裝置進行。 20. 如申請專利範圍第i 9項所述之微機電系統裝置, 其中上述W式平板係包栝一可撓式材質之連續滚筒。 21. 如申請專利範圍第19項所述之微機電系統裝置, 其中上述可撓式平板係由一密封薄膜所覆蓋》 22. 如申請專利範圍第21項所述之微機電系統裝置, 其中上述密封薄膜由金屬所構成。 23·如申請專利範圍第14項所述之微機電系統裝置’ 1077A-4732A-PF3 61 1318325 月f日修(更)正本 其中上述第一鏡面允許部分入射光通過,並且於上述第二 鏡面於上述第一、第二位置間之移動量,係用以調節由上 述第一、第二鏡面所反射之光所導致干涉。 1077A-4732A-PF3 62 1318325 4' 七、指定代表圖: (一)本案指定代砉!St &amp; ._ '表圖為:第(1B)圖。 (一)本代表圖之开杜# t %件付號簡單說明: 112〜基底; 114〜干v調制器陣列 116〜光源; uo〜準直器; 1 2 6〜薄膜堆積 118〜光導; 12 2〜光線; 128~觀察。 八、本案若有化學式時,請揭示最能顯示發明特徵的化 學式Revised deadline: 98.9.9 131853⁄4139. . No. 9 Chinese _ Patent Scope Amendment 10, Patent Application Range: i. A method of manufacturing a microelectromechanical system device, comprising: a one-to-one: providing a flexible substrate; and the above flexible substrate Providing one or more layers of the film, wherein the film comprises: a first mirror surface for at least partially reflecting incident light; and a second mirror surface for at least partially reflecting incident light, wherein the first mirror surface is disposed on the Between the flexible substrate and the second mirror surface, and one of the first and second mirror surfaces is moved relative to the other mirror surface between a first position and a second position, the first position is different from the other - the mirrors are separated by a first distance and the second position is at a second distance from the other mirror surface. 2. The method of &lt;RTI ID=0.0&gt;&gt;&gt; 3. The method of manufacturing a microelectromechanical system device according to claim 2, wherein the flexible substrate comprises a continuous plate of plastic material. 4. The method of fabricating a MEMS device according to claim 2, wherein the flexible substrate comprises a continuous sheet of paper material. 5. The method of fabricating a microelectromechanical system device as claimed in claim 1, wherein the film comprises an oxide layer, a metal layer, and a sacrificial layer. 6_ as described in claim 1 A method of fabricating an electromechanical system device, wherein the first mirror surface allows a portion of incident light to pass therethrough and is opaque to the second mirror surface. . 1077A-4732A-PF3 59 1318325 (Fin year 1f 曰修(更)本本本 I Μ----- ..._________ The manufacturing method of the MEMS device as described in claim 1] The film on the flexible substrate comprises an oxide layer and the oxide layer is disposed between the first mirror surface and the second mirror surface. 8. The method for manufacturing a microelectromechanical system device according to claim 1 Furthermore, the MEMS device is packaged by bonding (b〇n (jing)-flexible plate to the above-mentioned liftable substrate.] 9. The MEMS device according to claim 8 The manufacturing method of the above-mentioned flexible flat plate comprises a continuous roller of a flexible material. The manufacturing method of the MEMS device according to claim 8 wherein the flexible flat plate is sealed by a seal. U. The method of manufacturing a MEMS device according to claim 10, wherein the sealing film is made of a metal. 12. The MEMS device of claim 1The manufacturing method, wherein the MEMS device is an interferometric modulator, the MEMS device of claim 1, wherein the second mirror surface allows a portion of the incident light to pass through, and the first mirror surface It is opaque. .14: A shame 81—system mounting “------------- a liftable substrate; and—a first mirror that at least partially reflects incident light; a second mirror surface at least partially for reflecting incident light, wherein the first mirror surface is disposed between the flexible substrate and the second mirror surface, and one of the first and second mirror surfaces is opposite to Another - mirror surface - 1077A-4732A-PF3 60 1318325 ;:: set ... between the second position moved 1 attack i face &face; 5 giant - first distance _, and the second position is the other mirror A second distance from the basin 5', as in the MEMS device described in claim 14, ', the micro-electromechanical system device is an interferometric modulator. 16 λ. Electromechanical system device, where upper, ^ mirror permitting The incident light passes through, and the amount of movement between the first and second positions at the second mirror surface is said to be used to adjust the light reflected by the mirror surface of the first, 筮 _ &amp; 17. The MEMS device of claim 14, wherein the flexible substrate is made of a plastic or paper material. 18. The MEMS as described in claim 14. The device further includes an oxide layer disposed between the first mirror surface and the second mirror surface. 19. The MEMS device of claim 14, further comprising a flexible flat panel, bonding To the above flexible substrate for encapsulation of the above MEMS device. 20. The MEMS device of claim i, wherein the W-type plate is a continuous roller of a flexible material. 21. The MEMS device of claim 19, wherein the flexible slab is covered by a sealing film, 22. The MEMS device of claim 21, wherein The sealing film is made of metal. 23) The MEMS device as described in claim 14 of the patent application '1077A-4732A-PF3 61 1318325 </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> </ RTI> wherein the first mirror surface allows partial incident light to pass through, and the second mirror surface The amount of movement between the first and second positions is used to adjust the interference caused by the light reflected by the first and second mirror surfaces. 1077A-4732A-PF3 62 1318325 4' VII. Designated representative map: (1) The designated case for this case! The St &amp; ._ 'table chart is: (1B). (1) The representative figure of the opening Du # t % piece payment number simple description: 112 ~ base; 114 ~ dry v modulator array 116 ~ light source; uo ~ collimator; 1 2 6 ~ film stack 118 ~ light guide; 2 ~ light; 128 ~ observation. 8. If there is a chemical formula in this case, please reveal the chemical formula that best shows the characteristics of the invention. 1077A-4732A-PF 51077A-4732A-PF 5
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