TWI343505B - 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 PDFInfo
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1343505 (一) 本案指定代表圖為:第(1B)圖。 (二) 本代表圖之元件符號簡單說明: 112〜基底; 114〜干涉調制器陣列; 116〜光源; 118〜光導; 120〜準直器; ^ 122〜光線; 126〜薄膜堆積; 128-觀察。 五、 本案若有化學式時,請揭*最能顯示發明特徵的化 益。 工、· 六、 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】 干涉調制器(丨Mods)藉由操作微機械元件之光學特性 調制入射光。藉由利用各種技術改變微機械元件之光學特 性而完成。藉由利用各種技術改變此元件的光學特性而完 成。干涉調制器提供本身許多應用,從平面顯示器、光學 計算光纖光學調制器至投影顯示器。這些不同的應用可以 1077A-4732AA-PF 3 1343505 使用不同的干涉調制器設計。 【發明内容】 一般而言,於一形態中,本發明之特徵係以干涉調制 器為主的顯示器,其將抗反射鍍膜或微製造輔助光源。 一般而言,於一形態中,對於干涉調制器之矩陣驅動 陣列或其它為機械元件,本發明之特徵為高效率驅動系統。 一般而言,於一形態中,本發明之特徵為一彩色系統, 其提供更好的靈活性。 一般而言,於一形態中,本發明之特徵為一電子設備, 其底色可重新配置以便提供不同的顯示形態及/或應用功 能。 一般而言’於一形態中,本發明 < 个货a之特徵為一干涉調制 轉自干涉調制器的光學作用減少干涉調制器的運 驅動’於_形態中’本發明之特徵為具有選擇的 駆動裝置的干涉調制器設計。 一般而言’於一形態中,本發明 器或干涉 特微為一干涉調制 換陣列,且η 具被以且與微機電切換器或切 或以微機電為基礎的邏輯連接使用。 般而έ,於一形態中,本發明之 器,其可以庫 将微為一干涉調制 應用於光學切換以及光學調制。 一般而t,如 ° 於一形態中,本發明之特糌& 器,其組成2 η «。 今徵為一干涉調制 战及3-D光電結構。 r 43505 一般而言,於一形態中,本發明之 種應用。 待徵為 調制光的各 -般而言’於—形態中,本發明 芻i生以;^擗姑、#砝咖, #信文為—種微機電 基la以及根據連續網狀供給程序的封裝方法 -般而言,於-形態中,本發 .. 付信文為,接66 薄膜令,干涉調制器當作測試結構用以計算剩餘應: 【實施方式】 抗反射鍍膜 一種之前描述的干涉調制器設計(於1 995年丨丨月6日 的美國專射請案帛〇8/554,63(^之感應吸收器設 申請 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# 99. 7%的光吸收。4有助於反射式顯示器。於此 種設計中,此種干涉調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。1343505 (I) The representative representative of the case is: (1B). (b) A brief description of the symbol of the representative figure: 112~substrate; 114~interferometric modulator array; 116~light source; 118~lightguide; 120~collimator; ^122~light; 126~film stack; 128-observation . 5. If there is a chemical formula in this case, please disclose the benefits that best show the characteristics of the invention. TECHNICAL FIELD OF THE INVENTION: 1. Technical Field of the Invention The present invention relates to an interference modulator. [Prior Art] An interferometric modulator (丨Mods) modulates incident light by operating the optical characteristics of the micromechanical element. This is accomplished by using various techniques to alter the optical characteristics of the micromechanical components. This is accomplished by varying the optical properties of the component using various techniques. Interferometric modulators offer many applications in their own right, from flat panel displays to optical computing fiber optic modulators to projection displays. These different applications can be designed with different interferometric modulators for the 1077A-4732AA-PF 3 1343505. SUMMARY OF THE INVENTION Generally, in one aspect, the invention features an interferometric modulator-based display that will be an anti-reflective coating or a micro-fabricated auxiliary light source. In general, in one aspect, for a matrix driven array of interferometric modulators or other mechanical components, the invention features a high efficiency drive system. In general, in one form, the invention features a color system that provides greater flexibility. In general, in one aspect, the invention features an electronic device whose background color can be reconfigured to provide different display modalities and/or application functions. Generally, in one form, the present invention is characterized in that an interference modulation is transferred from an interferometric modulator to reduce the operation of the interferometric modulator. In the present invention, the invention is characterized by having a choice. The interferometric modulator design of the swaying device. Generally, in one aspect, the inventive device or interferometer is an interferometric modulation array, and η is used with and in conjunction with a microelectromechanical switch or a micro-electromechanical based logic connection. As a general matter, in one form, the apparatus of the present invention can apply micro-interference modulation to optical switching as well as optical modulation. In general, t, such as °, in a form, the special device of the present invention, which consists of 2 η «. This is an interference modulation warfare and 3-D photoelectric structure. r 43505 In general, in one form, the application of the invention. In the general form of the modulated light, the present invention is in the form, the invention is 生isheng; ^擗gu, #砝咖,#信文为—the microelectromechanical base la and according to the continuous mesh supply procedure Packaging method - in general, in the form, the present invention: the payment of the letter is 66, the film is used, the interferometric modulator is used as the test structure to calculate the remaining should be: [Embodiment] Anti-reflective coating is a previously described The design of the interferometric modulator (in the United States, on the 6th of January, 1995, the special shot request 帛〇 8/554, 63 (the induction absorber design application, here for reference) is black, in which It is possible to absorb #99.7% of the light absorbed on its surface. 4 contributes to the reflective display. In this design, the interferometric modulator reflects light of a given color in an unactivated state and absorbs in an activated state. Light.
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’係藉由利用抗反射鑛膜(ARcoatings)。此種錢膜可 包括一層或更多層的介電骐,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 1077A-4732AA-PF 5 13435〇5 廷種薄膜之設計與製造的一 杰 種簡早的缚膜設計係氟 化鎂之早一鍍膜,其近似 w刀您及長的厚度。另一種 方法係將氟化鋁的四分之—油壤 β /皮/専膜/儿積於破璃上,接著是 —層四分之一波薄膜的氟仆 虱化鎂另一種方法係於兩者之間 加入一層硫化鋅薄膜。 第1Α圖說明一種方沐 甘士 adm 裡万去,其中AR鍍膜應用於干涉儀調 制顯示器,以便改盖§音;么a k , kBecause the interferometric modulator array is formed on a substrate, the absorptive capacity will be reduced by the intrinsic reflection of the substrate. In the case of a glass substrate, the amount of reflection is typically about 4%, which exceeds 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 utilizing anti-reflective mineral film (ARcoatings). Such a film of money may include one or more layers of dielectric germanium deposited on the surface of the substrate and designed to reduce reflection from the substrate. There are many possible examples of the design and manufacture of 1077A-4732AA-PF 5 13435〇5 film, which is a kind of early and late film design. It is an early coating of magnesium fluoride. Long thickness. Another method is to divide the aluminum fluoride into four parts - oily soil β / skin / enamel film / children on the broken glass, followed by a layer of quarter-wave film of fluorescein magnesium. A layer of zinc sulfide film is added between the two. The first picture shows a Fang Mu Gans adm Riwan, where the AR coating is applied to the interferometer modulation display to change the § sound; a k , k
不糸統的效能。於第1A圖中,AR 鍵膜100,如上所述的可句 一 匕括層或更夕層’沉積於黏接 於玻璃基底106上的玻璃層1〇2之表面上。此AR鍍膜_ 藉由將更多光導入玻璃層1〇2中而降低入射光ι〇9從表面 反射的亮度。這結果為當干涉調制器被操作為吸收模式 時,可以使更多入射光入射干涉調制器陣列上且仍然可 獲得更黑的顯示狀態。此AR鍍膜⑽亦可直接沉積於表面 上具有干涉調制器陣列的表面上。 整合性光 第1A圖亦顯示輔助光如何照射於一顯示器上。於此範 例中,顯微鏡用弧光燈陣列1〇4製造於玻璃層1〇2中。弧 光燈係光源的效率提供者。根據史實,弧光燈已經利用一 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。製造一玻璃器血,並且分別製造 的電極被包圍於玻螭器孤中。填充適當的氣體後,玻璃器 m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Unsound performance. In Fig. 1A, the AR key film 100, as described above, is deposited on the surface of the glass layer 1 2 adhered to the glass substrate 106. This AR coating _ reduces the brightness of the incident light ι 9 reflected from the surface by introducing more light into the glass layer 1〇2. The result is that when the interferometric modulator is operated in the absorption mode, more incident light can be incident on the interferometric modulator array and a darker display state can still be obtained. The AR coating (10) can also be deposited directly onto the surface of the surface having an array of interferometric modulators. Integrated Light Figure 1A also shows how the auxiliary light is illuminated on a display. In this example, a microscope arc lamp array 1〇4 is fabricated in the glass layer 1〇2. The efficiency of the arc lamp is the source of the light source. According to historical facts, arc lamps have been manufactured using the manufacturing technology of general light bulbs. A typical style of such a lamp is described in U.S. Patent No. 4,987,496. A glass of blood is produced and the separately fabricated electrodes are enclosed in a glass borer. After filling the appropriate gas, the glass m 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 fabricate microdischarges or
1077A-4732AA-PF 6 505 : 因為此種微型燈〃的顯微大小,施加的電壓與 ^ "員的小於提供給以傳統方式製造的弧光燈的電壓與 電μ於第1A圖中的範例,可以製造陣列,藉由燈發射的 光Π3藉由本體的反射器層lu指引向干涉調制器陣列 108’其描述如下。 第2圖對於此種燈做了詳細的描述,對於應用於平面 ’示器做了最佳化的製造。流程描述如下。如步驟^所示, 利用濕或乾化學蝕刻’蝕刻一破璃層2〇。以便形成反射器 碗狀物201。碗狀物的深度與形狀藉由對於每一個光源需 求的面積與受度而決定。淺的碗狀物可產生寬廣的反射光 束刀布同時抛物狀可將反射光平行化。碗狀物的直徑變 化,約自10微米至數百微米。此尺寸係藉由顯示器面積量 決疋從觀貝者的觀點可欣然的接受。亦必須考慮微型燈 陣列的密度。利用一般的沉積技術,例如濺鍍以及標準 的黃光顯影技術,沉積一反射器/複金屬層204及犧牲層 202且形成既定圖案。此反射器/複金屬層可為一堆積薄 膜,其包括鋁(反射器)及複金屬,例如碘化鉈 '碘化奸及 碘化銦。此複金屬,並非必要的,可增加產生的光的特性。 此犧牲層可以是一層,例如石夕。 接著’沉積電極層206且形成既定圖案,以便形成兩 個分開的電極。此材料可以是耐高溫金屬,例如鶴;並且 具有充分提供機械支撐的厚度’約為數千個埃單位。然後 犧牲層202利用乾蝕刻技術移除。整組(例如燈泡陣列)以 黏著於玻璃板,例如基底(如第1A圖所示)上而密封,其中 1077A-4732AA-PF 7 1343505 反射器面向該板。氣體’例如氙器,用以回填上述空穴, 於岔封燈泡步驟中形成’壓力大約為一大氣壓。這可以於 已事先充滿氙氣的密閉腔室中’執行密封步驟。 對於每一燈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,並且發射的光2〇5朝向遠離反射 器204的方向。假若閘間隔大約為數百個微米或更少,電 壓可降低至數時伏特。假若電極材料沉積著少量的壓力, 犧牲層202將於碗狀物内決定電極的位置。於此範例中, 選擇的厚度係用以提供放電。當移除時,應剩餘多少壓力, 會造成電極位移,那就決定了厚度以便補償位移。一般而 s,厚度將只是碗狀物深度的一點點,大約為數個至數十 個微米。 再一次參考第1A圖,顯示光沿著路徑113行進。因此 光朝向干涉調制器陣列發射,在那裡作用且依序藉由陣列 沿著路徑110朝向介面107及觀察者⑴反射。 因此其將全方位發 亦可以製造不具有反射器層的燈 射光。 具有或不具有反射器 w + ^ A J ^丑j悠用於而要顯微光源或擇 微光源陣列的地方D P可L7 4θ . k可以包括投影顯示器、發射平面農 示器的被光或内部(居突 ’、 丨1居豕、房屋)的傳統光源或外部(汽車 閃光燈)光源。 「I W飞早 參考第1 β圖,顯 括一玻璃或塑膠層, 的發射源的光源】】6 , 示可選擇的輔助光方法。光導118包 其點著於“ 112。可包括任意種類 例如螢光燈、LED陣列或上述微型燈1077A-4732AA-PF 6 505 : Because of the microscopic size of such a miniature lamp cymbal, the applied voltage is less than the voltage and electricity supplied to the conventionally manufactured arc lamp in the example of Figure 1A. An array can be fabricated by which the diaphragm 3 emitted by the lamp is directed to the interferometric modulator array 108' by the reflector layer lu of the body as described below. Figure 2 shows a detailed description of such a lamp, which is optimized for use in a flat panel. The process is described below. As shown in step ^, a frit layer 2 is etched by wet or dry chemical etching. In order to form the reflector bowl 201. The depth and shape of the bowl is determined by the area and tolerance required for each source. Shallow bowls produce a wide range of reflected light. The knives are parabolic and parallel to the reflected light. The diameter of the bowl varies from about 10 microns to hundreds of microns. This size is readily accepted by the viewer's point of view by the amount of display area. The density of the micro lamp array must also be considered. A reflector/composite metal layer 204 and sacrificial layer 202 are deposited and formed into a predetermined pattern using conventional deposition techniques, such as sputtering and standard yellow light development techniques. The reflector/composite metal layer can be a stack of thin films comprising aluminum (reflector) and a complex metal such as cesium iodide 'iodine rape and indium iodide. This complex metal is not necessary to increase the characteristics of the light produced. This sacrificial layer can be a layer, such as Shi Xi. The electrode layer 206 is then deposited and formed into a predetermined pattern to form two separate electrodes. This material may be a high temperature resistant metal such as a crane; and has a thickness sufficient to provide mechanical support 's of thousands of angstrom units. The sacrificial layer 202 is then removed using dry etching techniques. The entire set (e.g., the array of bulbs) is sealed by adhering to a glass sheet, such as a substrate (as shown in Figure 1A), with the 1077A-4732AA-PF 7 1343505 reflector facing the panel. A gas, such as a crucible, is used to backfill the voids and form a pressure of about one atmosphere during the step of sealing the bulb. This can be performed in a closed chamber that has been previously filled with helium. Applying a sufficient voltage to the electrodes of each bulb will cause a discharge, a gas between the ends of the two electrodes, and the emitted light 2〇5 will face away from the reflector 204. If the gate interval is approximately a few hundred microns or less, the voltage can be reduced to several volts. If the electrode material is deposited with a small amount of pressure, the sacrificial layer 202 will determine the position of the electrode within the bowl. In this example, the thickness selected is used to provide a discharge. When removed, how much pressure should be left, causing electrode displacement, which determines the thickness to compensate for the displacement. Generally, s, the thickness will be only a little bit of the depth of the bowl, about several to tens of microns. Referring again to Figure 1A, light is shown traveling along path 113. The light is therefore emitted towards the interferometric modulator array where it acts and is sequentially reflected by the array along path 110 towards interface 107 and observer (1). Therefore, it is possible to manufacture a lamp that does not have a reflector layer in all directions. With or without a reflector w + ^ AJ ^ ug j used for a micro light source or a micro light source array where the DP can be L7 4θ . k can include the projection display, the emission plane of the light or the interior of the plane ( A traditional light source or an external (automobile flash) light source of Judu', 丨1 residence, house. "I W flying early refers to the first β-graph, which shows a source of light from a source of glass or plastic.] 6 shows an alternative auxiliary light method. The light guide 118 is dotted with "112. Can include any type such as fluorescent lamps, LED arrays or the above miniature lamps
1077A-4732AA-PF 343505 陣列,固定於光導的對立侧。光122使用一準直器i2〇耦 合入光導,因此大部份的光經由内全反射捕捉於光導内。 散射墊鍍上一材料或薄膜堆積126,形成朝向基底ιΐ2的 一反射表面以及朝向觀察者的吸收表面。 當捕捉於光導内的光入射於散射墊上時,不再遵守内 全反射的條件且某部份的光於全方位散射。可垂直進入附 、 近介質的散射光,就是朝向觀察者128的,由於存在反射 •鍍膜I26而被反射進入基底112。類似上述的微型燈泡, 散社塾可以製作成陣列狀,每一陣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,可提供充分的輔助光,因為加上干涉調制器陣 列114下方,本身的光效率。散射墊的形狀可以為圓形、 矩形或任意形狀’其可以降低觀察者的察覺。 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 鲁式’於陣列的行與列施加—連續的電壓其中—般稱為、 間線々方式。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,只有位於被選擇的行丨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。磁滯曲線3〇〇 係反射式干涉調制器之電性反應之理想化表示。χ軸表示1077A-4732AA-PF 343505 Array, fixed to the opposite side of the light guide. Light 122 is coupled into the light guide using a collimator i2, such that most of the light is captured within the light guide via total internal reflection. The diffuser pad is plated with a material or film stack 126 that forms a reflective surface toward the substrate ι2 and an absorbing surface toward the viewer. When light trapped in the light guide is incident on the scattering pad, the condition of total internal reflection is no longer observed and some portion of the light is scattered in all directions. The scattered light that can enter the near and near media vertically, is toward the viewer 128, and is reflected into the substrate 112 due to the presence of the reflective coating I26. Similar to the above-mentioned miniature light bulbs, the dispersions can be made in an array, and each array is as large as the displayed portion, making it almost impossible to detect when looking directly. When the size is relatively small, about ten microns, sufficient auxiliary light can be provided because of the inherent light efficiency of the interferometric modulator array 114. The shape of the scattering pad can be circular, rectangular or of any shape' which can reduce the perception of the viewer. Addressing Elements in the Array In order to activate the array of interferometric modulators, and to coordinate the display, the equations are applied to the rows and columns of the array—continuous voltages are commonly referred to as inter-line modes. 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 only the cells located below the selected row are 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. χ axis representation
1077A-4732AA-PF ^^505 包加的電壓,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 制器結構且成為高吸收。當施加的電壓減少時,施加的電 壓必須小於釋放臨界值κ更使結構恢復成未啟動狀態。 拉回與釋放臨界值之間的差異產生磁滯窗。此磁滞效應, 和可選擇定址系統,已揭露於1 996年1 U 5日申請的美 國專利申清案第08/744 253號,並且在此當作參考。任何 時刻’磁滯窗可藉由維持-偏壓電壓V»,as而使用,以便使 ,調制器可以被驅動或釋放成任何狀態。電壓V。"與 對應於必須驅動或釋放干涉調制器結構的電壓。此陣列利 用電:設備藉由施加電壓於行與列而驅動,已知為列與行 驅動盗。干涉調制器利用拉回臨界值6伏特而製造,並且 釋放臨界值J Α 值為3伙特。對於如此的裝置,關於 的一般值分別為“伏特、。伏特及9伏特。 =3圖中’日夺間圖3〇2說明波形種類,可用以施加 =干涉調制器陣列’顯示一磁滞曲線類曲線_。 :::要五種電壓’兩列電塵及三行《。被選擇的電壓, 選擇,因ΓΓ 。1。為零伏特。行電壓被 w㈣與Vet)10之間的差額等於^,並且V盥 V-之間的差額等於L。相反地 se,F"' 額等於I,並且v ^ v '、I。丨丨之間的差1077A-4732AA-PF ^^505 The applied voltage, and the y-axis represents the amplitude of the reflected light. The interferometric modulator exhibits a hysteresis because, when the applied voltage exceeds the pullback threshold, the interferometric modulator structure is activated and becomes highly absorbed. When the applied voltage is reduced, the applied voltage must be less than the release threshold κ to return the structure to the unactivated state. The difference between the pullback and the release threshold creates a hysteresis window. This hysteresis effect, and the optional addressing system, are disclosed in U.S. Patent Application Serial No. 08/744,253, filed on Jan. The hysteresis window can be used at any time by the sustain-bias voltage V», as so that the modulator can be driven or released in any state. Voltage V. " and corresponds to the voltage that must drive or release the interferometric modulator structure. This array utilizes power: the device is driven by applying voltage to the rows and columns, known as column and row drive theft. The interferometric modulator is fabricated using a pull back threshold of 6 volts and has a release threshold J Α of 3 tex. For such a device, the general values are "volts, volts, and 9 volts. =3" in the graph, the graph is shown in Fig. 3〇2, and the waveform type can be used to display a hysteresis curve. Class curve _. ::: Five voltages are required for 'two columns of dust and three rows.' The selected voltage, select, because 。 1. 1. Zero volts. The difference between the line voltage is w (four) and Vet) 10 is equal to ^, and the difference between V盥V- is equal to L. Conversely, se, F"' is equal to I, and the difference between v ^ v ', I.
Vsem與L。1。之間的差額等於v。"。 定址發生;-,5g ,, ^ 序中,關於“: 與…於—般的定址次 ..^ 丁的貝料於畫面0期間被載入列驅動考,ρ 據資料分別A 和動态,根 進位的一或零,導致施加^或V。。,。的電Vsem and L. 1. The difference between them is equal to v. ". Addressing occurs; -, 5g,, ^ In the order, about ": and ... in the general address of the order.. ^ Ding's shell material is loaded into the column driver test during the picture 0, ρ data separately A and dynamic, One or zero of the root carry, resulting in the application of ^ or V.
1077A-4732AA-PF »1343505 壓值备貝料結束時,行驅動器〇施加具有Vseir。值的選擇 的脈衝。這導致於列上具有v_的任何干涉調制器造成開 始啟動’並且於列上具有Ve。"的任何干涉調制器釋放。關 於下-行的資料被載入列,並且一選擇的脈衝施加於該 二,並且依序實施直到顯w的最末—行。接著再一次從 玎〇開始定址,然而此時,定址出現畫面i。 畫面之間的差異與資料及列電壓之間的轉換相似,二 進位的零現在藉由v_表示,以及行選擇脈衝現在為 v-n。利用此技術,施加於顯示器陣列的整體電壓極性隨 每一晝面變化。這是有用的,特別對於以微機電為主的顯 示器,因為允許對於任何DC值電荷增長補償,這會出現於 當只有施加單-極性電壓。於結構内的電荷增長可顯著的 偏移干涉調制器或其它微機電裝置的電性曲線。 彩色顯示圖像 ▲因為干涉調制器係一具有各種可能的光學響應的多功 能裝置’-些不同的彩色顯示圖像可具有不同的特性。一 種可能的結構開發出具有二部份的干㈣μ設計,相同 的干涉調制器可以獲得彩色狀態、黑色狀態及白色狀態。 此可能性可用以擔俱必& Μ ® /备 -r* ^ 又件Φ色的圖像,可以、底色+顏料,,。用 此術語係因為,此方法類似繪畫上色’其藉由增加顏料至 白底色以便獲得需要的色彩而產生。利用此方法,特別的 繪畫可獲得任何光言並φ & Λ 的顏色’並且藉由控制顏料加入底 色的成刀與3置獲得需要的飽和度。此方法可構成具有彩 色、黑色及白色像素的顯示器。1077A-4732AA-PF »1343505 At the end of the pressure reserve, the row driver 〇 is applied with Vseir. The pulse of the choice of value. This results in any interferometric modulator with v_ on the column causing the start-up' and having Ve on the column. " Any interfering modulator release. The data for the lower-row is loaded into the column, and a selected pulse is applied to the second, and is implemented sequentially until the last-line of the display w. Then, the address is started again from 玎〇, but at this time, the screen i appears. The difference between the pictures is similar to the conversion between the data and the column voltage. The binary zero is now represented by v_ and the row select pulse is now v-n. With this technique, the overall voltage polarity applied to the display array varies with each face. This is useful, especially for MEMS-based displays, because it allows compensation for any DC value charge growth, which occurs when only a single-polar voltage is applied. The increase in charge within the structure can significantly shift the electrical curve of the interferometric modulator or other microelectromechanical device. Color display image ▲Because the interferometric modulator is a multi-function device with various possible optical responses' - different color display images may have different characteristics. One possible structure develops a two-part dry (four) μ design, and the same interferometric modulator can achieve a color state, a black state, and a white state. This possibility can be used to take care of & Μ ® /preparation -r* ^ and Φ color image, can, background color + pigment,,. This term is used because this method is similar to painting coloring, which is produced by adding a pigment to a white background to obtain the desired color. With this method, a special painting can obtain any utterance and φ & Λ color' and obtain the desired saturation by controlling the addition of the pigment to the background. This method can constitute a display with color, black and white pixels.
1077A-4732AA-PF 11 1343505 如第4A圖所示,一像素4〇〇包括五個次像素單元4〇2、 404、406、408 ’每一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。每一次像素的亮 度控制可利用脈衝寬度調制而完成,相關技術已揭露於^ 國專利第5’ 835’ 255號。同時適當的選擇相關次像素大 小,這導致像素整體具有非常大程度的控制亮度與飽和 度。例如’藉由減少白色次像素之總亮度,可獲得相举言 地飽和色彩。相反地,#由減Μ色次像素之亮度,= 由同時將其與白色次像素最大化可獲得明顯的黑與白^ 式。中間的所有變化可輕易地獲得。 /、果 使用者控制的彩色圖像 如上所述的彩色圖像,就解析度、灰階程度以及清1 度而言’如同以干涉調制器為主的顯示器之本質特性二 供更靈活的顯不性能。在此範圍内,可有效的提供使用 具f超越一般特性的顯示控制的產品。或者,關於顯示丨 功旎係自動地適應不同觀賞需要。 …、 例如’假如一些文章,只要觀看文字使用者可⑸ 要使用黑白模式的產品〇然而,另— b Λ 想要觀看高品質的彩色靜離 / ,使用者可倉 觀看動態書面。=Γ:Γ或者於另一種模式下, —w 込類的母一個模式,於裎视从工,土 顯示形態範圍内,翥可w 、鍉供的干涉調制器 …固内i可迠地需要特別屬性的交換 ,假右需要高解析度的畫面,需要、又、已 要黑與白’有能力獲得高度灰階。-…假若只需 為了給予使用者此種译性的需求,控制器硬趙可重新1077A-4732AA-PF 11 1343505 As shown in FIG. 4A, a pixel 4 〇〇 includes five sub-pixel units 4 〇 2, 404, 406, 408 ′ each of which can reflect red 'green, blue, and white, respectively. All sub-pixels can produce a black state. The brightness control of each pixel can be accomplished by pulse width modulation, and the related art has been disclosed in Japanese Patent No. 5' 835' 255. At the same time, the relevant sub-pixel size is appropriately selected, which results in a very large degree of control of brightness and saturation of the pixel as a whole. For example, by reducing the total brightness of white sub-pixels, a saturated color can be obtained. Conversely, # is reduced by the brightness of the sub-pixels, = by simultaneously maximizing it with the white sub-pixels to obtain significant black and white. All changes in the middle can be easily obtained. /, color image controlled by the user as described above, in terms of resolution, grayscale degree, and clearness, 'as in the nature of the display based on the interferometric modulator, the second is more flexible. No performance. Within this range, it is possible to effectively provide a product using display control with f beyond the general characteristics. Or, the display system automatically adapts to different viewing needs. ..., for example, 'If you have some articles, you can use the black and white mode of the product if you want to watch the text. (5) If you want to watch high-quality color silence / , you can watch the dynamic writing. =Γ:Γ, or in another mode, the parent mode of the -w 込 class, in the range of the sinister work, the soil display form, the interference modulator of the w , 鍉 固 固 固 固The exchange of special attributes, false right requires a high-resolution picture, needs, and has to be black and white 'has the ability to obtain a high gray level. -... If it is only necessary to give the user the need for such translation, the controller can be restarted.
1077A-4 732AA-PP1077A-4 732AA-PP
12 1343505 具有某種波段寬 ’並且因此決定 配置至某種程度。根據事實,任何顯示只 度,基本上係受像素單元之響應時間限制 於既定時間内可被顯示的資訊量。12 1343505 has a certain band width ‘and therefore determines the configuration to some extent. According to the fact, any display degree is basically limited by the response time of the pixel unit to the amount of information that can be displayed in a given time.
可以提供此種彈性的一顯示架構已說明於第仙圖 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問極陣列 (FPGAs),提供改變元件的功能或出貨後可重新設定。這類 的元件’-般用於特別的應帛’例如數位信號處理或影像 壓縮,對於這類的處理可提供高品質,於產品設計階段加 入使用這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 動電子電路414與416。習知的控制係根據1(:或應用特性 積體電路(ASICs),於製造期間藉由其設計功效有效地 '制 訂程式〜於此範例中’逐條的程序表示,包括數種基本 的及更高階層的邏輯元件(邏輯閘極及邏輯模組或閘極配 件)之内部晶片佈局。藉由使用場可程式元件,例如 或FPG As,,於硬體應用型式或硬體應用中,不同的顯示 設定可自一元件410 ’像是記憶體或一習知具有記憶體的 微處理器,載入顯示控制元件。記憶體可以為EEpR〇Ms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,因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。A display architecture that can provide such flexibility has been described in the figure. In this block diagram, the executor controller logic operations 412, including programmable logic components and field programmable arrays (FPGAs), utilizing various IC techniques, provide the functionality to change components or can be reset after shipment. Such components are typically used for special applications such as digital signal processing or image compression, which provide high quality for such processing, and the use of such components during the product design phase while providing flexibility. The controller 412 provides signals and data to the drive electronics 414 and 416 for the address display 418. The conventional control system is based on 1 (or application-specific integrated circuits (ASICs), which effectively validate the program during manufacturing by its design function. - In this example, the program description includes several basic and Internal wafer layout of higher-level logic components (logic gates and logic blocks or gate components). By using field programmable components, such as FPG As, in hardware applications or hardware applications, The display setting can be loaded from the display control component from a component 410' such as a memory or a conventional microprocessor having a memory. The memory can be an EEpR〇Ms type or other programmable storage element; and the micro-processing The device can be implemented in a simple microcontroller type, and its function is to load a large number of applications from the memory into the FPGA in addition to the general functions of the processor processing products. The advantage of this method is that it has a simple and easy circuit diagram combined with it. A wide variety of display function settings and mixed display scan rates are available.
1077A-4732AA-PF ^43505 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 於顯示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,並且只有相當於一個或兩個的—或兩個位元之 灰階濃度。高解析度電子郵件區域可以快速地掃描,並且 相S於二個或四個的三或四個位元之灰階。 可更改設定電子產品 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圖顯示一般可攜式電子產品418 之設定,其具有可程式的邏輯元件或於其核心420的同等 物。於許多顯示中心個人電子產品,例如pDAs(個人數位 助理)以及電子萬用記事本,中央處理ϋ係-不同版本的 RISC處理器,其使用更少的指令組。當Risc處理器係更 有效率的CPU版本時,提升更多個人電腦之功能,其仍然 為-般功能的處理器’㈣許多能量執行重複的工作,例 如擷取來自記憶體的指令。 於個人電腦中,能量消耗量並不是問題,並且使用者 一般想要執行許多複雜的應用軟體。此相對觀點對於-般 顯示中心個人電子產σ _^β 电卞座。口而έ疋正確的。需要消耗低能量, 並且提供相當少量的相對簡易的程式。此種制度有利於執 行特別功能的程式,例如包括網路瀏覽器、行事曆、繪圖 程式 '電話/定址資料庫以及手寫/語音辨識當作一石更體 應用。因此當使用者需要執行―❹卜力能模式,例如 1077Α-4732ΑΑ-ΡΓ 14 [1343505 式’核心處理器隨著硬體應用更改設定,並且使用者與產 品互動。因此,此硬體應用的處理器,顯示於其内部邏輯 操作與連結中的各種場可程式閘陣列具有此困難應用(即 程式)’當载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 言(一硬體敘述語言),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 K〇uichi Nagaini 等人的於 1 998 年於 Proc. IEEE Workshop on FPGA based Custom Computing Mechines 之論文1077A-4732AA-PF ^43505 For example, 'one part of the screen may display text side with low-level resolution' while the other provides high-quality receiving e-mail display. This can be done over the entire 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 has only one or two—or two bits of grayscale density. High-resolution email areas can be scanned quickly, and the phase S is in two or four three- or four-bit grayscales. Changeable settings electronics This concept broadly includes, not only, the functionality of the display controller, but also the functionality of the overall product. Figure 4C shows a setup of a general portable electronic product 418 having programmable logic elements or equivalents to its core 420. In many display center personal electronic products, such as pDAs (personal digital assistants) and electronic universal notebooks, the central processing system - different versions of RISC processors, using fewer instruction sets. When the Risc processor is a more efficient CPU version, it boosts the functionality of more PCs, which still perform a repetitive work for the general-purpose processor's (4) many functions, such as fetching instructions from memory. In personal computers, energy consumption is not an issue, and users generally want to implement many complex application software. This relative view is for the general display of the center personal electronics σ _^β 卞 。. The mouth is right and wrong. It requires low energy consumption and provides a relatively small amount of relatively simple programs. Such a system facilitates programs that perform special functions, such as web browsers, calendars, drawing programs, 'telephone/addressing databases, and handwriting/speech recognition as a stone-like application. Therefore, when the user needs to perform the "power" mode, for example, 1077Α-4732ΑΑ-ΡΓ 14 [1343505] core processor changes the settings with the hardware application, and the user interacts with the product. Therefore, the processor of this hardware application, the various field programmable gate arrays displayed in its internal logic operations and connections have this difficult application (ie program) 'reconfigure and write when loading a new hardware application. . Many providers of this component also provide an application development system that allows for a specific programming language (a hardware narrative 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 in the paper by K〇uichi Nagaini et al., Proc. IEEE Workshop on FPGA based Custom Computing Mechines, 1998.
Plastic Cell Architecture: Towards Reconfigurab1e Computing f0r GenerabPurp〇se,,揭露。 再一次參考第4C圖,此硬體應用處理器420顯示於一 堆的I/O元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或介面 424自外部資源載入,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,關於手寫輸人426包括手寫辨識規則系統以 及關於〜像輸入裝置43〇包括影像壓縮與處理模式。此類 的產。口可藉由其主要部位之功效執行大量的功能,顯示器 田作主要使用者介面以及可更改設定核心處理器。藉由與 目刖產°°之數百毫瓦特比較,關於這類元件之整體功率總Plastic Cell Architecture: Towards Reconfigurab1e Computing f0r GenerabPurp〇se,, expose. Referring again to FIG. 4C, the hardware application processor 420 is displayed in the center of a stack of I/O components and computer peripheral products that will be used, modified, or not depending on the functionality and characteristics of the currently loaded hardware application. The Council. The hardware application can be loaded from external memory in the memory 422 present in the product or via RF or interface 424, i.e., application content with a particular hardware application can be retrieved from a networked cellular network or other electronic device. Another example of a hardware application is that the audio interface 432 includes a voice recognition or voice synthesis rule system, the handwriting input 426 includes a handwriting recognition rule system, and the image input device 43 includes an image compression and processing mode. The production of this type. The port can perform a large number of functions by the function of its main part, the display field is the main user interface and the core processor can be changed. By comparing the total power of such components with the hundreds of milliwatts of the production
1077A-4732AA-PF 15 1343505 合大約為數十毫瓦特等級。 伙光學觀點解麵機電觀點 於1 996年12月19日申臂 _,947號,以及於年“ *、國專:申請案第 申請案第09/056’975號’在此提供參考,心 ^|| 51 ^Λ. ,θ ^ , 、匕揭路干涉調 制器6又汁,鍉礒自其光學功能 Λ, 〇 .接士,1 祸干涉調制器之機電功 月另—種方法’可籍由第5Α圖與第5β圖所描述的完成。 此言又計利用靜電力量改變干涉空 的幾何。電極502係製 :、二〇上’並且藉由絕緣薄膜5〇4與膜狀物/鏡面 _電性阻隔。電極502之功能只有當作電極使用,並未 當作鏡面使用。 光學空穴505形成於薄膜/鏡面5〇6與第二鏡面5〇8之 間。關於第二鏡面508的支撑物係-透明的上部構造510, 其可以為一厚沉積有機物,例如SU8、聚硫亞氨或一無機 材料。於製造期間藉由犧牲層決定’未施加電壓時,如'第 5—A圖所示’相對於第二鏡面5()8,薄膜/鏡面咖維持一既 定位置。數千埃的厚度適用於大約四伏特的啟動電壓。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it ’例Μ呂;則此結構將反射可被觀察者512感 知的既定頻率光511。此外’假若鉻大約4〇 土矣薄到半透 明’以及鋁相當的薄’至少5〇〇埃且不透光,則此結構可 具有寬廣的各式光響應。第5C圖與第5D圖,分別顯示專 白及彩色的響應,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5〇2及薄膜鏡面5〇6之間施加電1077A-4732AA-PF 15 1343505 The combination is on the order of tens of milliwatts. The optical point of view of the optical point of view on December 19, 996, the application of the arm _, 947, and the year "*, national special: application No. 09/056 '975" is hereby provided, reference ^|| 51 ^Λ. , θ ^ , , 匕 路 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 干涉 干涉This is done by the description of Fig. 5 and Fig. 5β. This statement also uses the electrostatic force to change the geometry of the interference space. The electrode 502 is made of: 〇 on the top and through the insulating film 5〇4 and the film/ Mirror_Electrical barrier. The function of the electrode 502 is only used as an electrode and is not used as a mirror. The optical cavity 505 is formed between the film/mirror 5〇6 and the second mirror 5〇8. Regarding the second mirror 508 The support system - a transparent superstructure 510, which may be a thick deposition of organic matter, such as SU8, polythionimide or an inorganic material. Determined by the sacrificial layer during fabrication, when no voltage is applied, such as '5th As shown in Figure A, the film/mirror is maintained at a predetermined position relative to the second mirror 5 () 8. The thickness of several thousand angstroms is suitable. For a starting voltage 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 the given frequency that can be perceived by the observer 512. Light 511. In addition, if the chrome is about 4 矣 thin to translucent and the aluminum is relatively thin 'at least 5 angstroms and opaque, the structure can have a wide variety of photoresponses. 5C and The 5D image shows the response of the white and the color, respectively, determined by the length of the hole and the thickness of the constituent layer. Figure 5 shows the application of electricity between the main electrode 5〇2 and the film mirror 5〇6.
1077A-4732AA-PF 16 1343505 座的結果。垂直的設晋士董胺 罝此/專膜/鏡面,因此改變光學空六 長度以及干涉調制器之氺Μ 先學特性。第5c®顯示-種反射光 學響應,可具有兩藉#能 ^ ^ 狀〜、,备裝置完全啟動時說明黑狀態 521,g裝置未啟動時係白#能 时保白狀態。第5D圖顯示具有色彩峰 值525、527及529的光學響應,分別相#於藍& in 紅色。因此裝置的機電操作狀態可與其光學性能分開地控 制。主電極的材料與配置,其影響機電,可選擇不包含第 二鏡面的材料;因為其不具有干涉調制器之光學功能。此 設計可利用表面微機械之步驟與技術製造,例如,已揭露 於1 996年7月31日中請的美國專利中請案第08/688,川 號,並在此列入參考。 ’ 於另-個範例中’顯示於第6A圖中,關於干涉調制器 606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6b圖, 於啟動狀態申揭露相同的結構。 於第7A圖中,揭露應用於—干涉調制器結構的另一種 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。 此裝置的功能可藉由使其干涉而改善。於第7A圖中的 1077A-4732AA-PF 17 B43505 干涉調制器變化,其中薄膜堆積7〇4為介電層/導電層人絕 緣層,係1 996年7月31曰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7〇2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進一步 以機械方式藉由一支撐調整片716固定於基底,其係直接 沉積於光學堆積層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 中’此技術消除分散的黑色遮蔽物。 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08/688,71 0號所揭露的 感應式吸收的干涉調制器,在此列入參考。 第Μ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& 718而產生,其具有相當高的殘 留應力。鉻係一使用範例,#中薄膜厚度減少至數百埃可 獲付间應力。隨著薄膜不再遮擋其光路徑,可允許光束7〇 6 通過隹積f 704且貫穿此平板71〇。平板71Q可存在於不1077A-4732AA-PF 16 1343505 The result of the seat. The vertical setting of Jinshi Dong amine 罝 this / film / mirror surface, thus changing the optical empty length and the interferometric modulator 氺Μ learning characteristics. The 5c® display - a kind of reflected optical response, can have two borrowing #能^^~, and the black state 521 is indicated when the device is fully started, and the white state is white when the device is not activated. Figure 5D shows the optical response with color peaks 525, 527, and 529, respectively, in #蓝& in red. Thus the electromechanical operating state of the device can be controlled separately from its optical performance. The material and configuration of the main electrode, which affects electromechanical, may be selected from materials that do not include a second mirror; since it does not have the optical function of an interferometric modulator. This design can be made using the steps and techniques of surface micromechanics, for example, as disclosed in U.S. Patent Application Serial No. 08/688, filed on Jul. 31, 196, which is incorporated herein by reference. In another example, shown in Figure 6A, the support structure for the interferometric modulator 606 is placed in position to be hidden by the film/mirror 608. In this way, the number of inactive areas is effectively reduced because the observer 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. Figure 6b shows the same structure in the startup state. In Figure 7A, another geometric configuration applied to the interferometric modulator structure is disclosed. This design is similar to that disclosed in U.S. Patent Nos. 5,638, 〇84. This design utilizes a transparent plastic film that stretches anisotropically and thus naturally exists in a curled state. A voltage is applied to planarize the film as a microelectromechanical shutter. The function of this device can be improved by interfering with it. 1077A-4732AA-PF 17 B43505 Interferometric Modulator Change in Figure 7A, in which the film stack 7〇4 is the dielectric layer/conductive layer human insulating layer, July 07, 996, filed in US Patent Application No. 08 /688' The main part of the design of the inductive absorption interferometric modulator disclosed in 710 is hereby incorporated by reference. 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, the aluminum 7〇2 also includes other reflective metals (silver 'copper, nickel), or is plated with a reflective metal in the dielectric material or in the inner layer of the organic material, and is disposed on a thin sacrificial layer, and the sacrificial layer can be wetted. Etching or gas phase removal techniques are removed. The aluminum film 7〇2 is further mechanically fixed to the substrate by a support tab 716 which is deposited directly onto the optical buildup layer 704. Because of this, the light incident on the area of the tab and the buildup layer is absorbed, so that this mechanically inactive area does not function optically. In this example and other interferometric modulator designs, this technique eliminates scattered black masks. 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. 08/688,71, the entire disclosure of which is incorporated herein by reference. The 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 material & 718 over the film, which has a relatively high residual stress. In the case of chrome-based use, the thickness of the film in # is reduced to several hundred angstroms to obtain the inter-stress. As the film no longer obscures its light path, the beam 7 〇 6 is allowed to pass through the hoarding f 704 and through the plate 71 〇. Tablet 71Q can exist in no
1077A-4732AA-PF 18 1343505 是高度吸收就是高度反射(既定色彩或白光)的狀態。關於 使用於反射式顯示器中的調制器,光學堆積層704可設計 成,當裝置啟動時,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)。 旋轉式啟動 如第8A囷所示,另一種干涉調制器幾何結構係以旋轉 方式啟動。利用於1 996年7月31曰申請的美國專利申請 案第08/688, 71 0號中揭露地步驟且在此列入參考,電極 802、約1〇〇〇埃厚度的鋁薄膜形成於基底8〇〇上。設置支 撐棒808及旋轉樞紐810、支撐遮光器812及其上的反射 薄膜813。支撐遮光器可為一鋁薄膜,其具有數千埃厚度。 其X-Y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1996年7月曰 申請的美國專利申請案第〇8/688 71〇號揭露了感應吸收 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’或者為鋁或銀以便提供寬波段反射。設計電極2及 遮光器812,因此於兩者之間施加電壓(例如1〇伏特)將造 成遮光器812以旋轉樞紐轴部份或完全旋轉。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 有的遮光器將一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滯現象,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 框紐的彈簧張力。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1077A-4732AA-PF 18 1343505 is a state of high absorption or highly reflective (established color or white light). With respect to the modulators used in reflective displays, the optical buildup layer 704 can be designed to reflect a given color (if the plate 71 is absorbing) or absorbed (if the plate 710 is in a reflective state) when the device is activated. Rotary Startup As shown in Figure 8A, another interferometric modulator geometry is activated in a rotary manner. The electrode 802, an aluminum film having a thickness of about 1 angstrom, is formed on the substrate, as disclosed in U.S. Patent Application Serial No. 08/688,70, the entire disclosure of which is incorporated herein by reference. 8 〇〇. A support rod 808 and a rotary joint 810, a support shutter 812 and a reflective film 813 thereon are disposed. The support shutter can be an aluminum film having a thickness of several thousand angstroms. Its X-Y size is from tens to hundreds of microns. The film can be interferometric and designed to reflect a given color. A fixed interference stacked layer of inductively absorbing type is disclosed in U.S. Patent Application Serial No. 8/688,71, filed on Jan. s. It may also include a polymer immersed in a color dye' or aluminum or silver to provide broadband reflection. The electrode 2 and the shutter 812 are designed such that applying a voltage (e.g., 1 volt) between the two 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 together 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 so that the electrostatic attraction of the electrode exceeds the spring tension of the rotating frame 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.
1077A-4 7 32AA-PF 19 »43505 許其通過。第8A圖說明反射模式,其中入射光822被反射 回嬈察者820。於此模式之一個狀態中,假若遮光器是金 屬装造,遮光器將反射白光,或假若遮光器鍍上干涉薄膜 或柒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1996年7月 31日申請的美國專利申請案第〇8/688 71 〇號,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。此 4膜可包括另一種染料浸泡有機薄膜,或設計用來吸收的 一感應吸收堆積層。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 如上所述的彩色反射薄膜線選擇性地鍍上具有染料薄膜或 干涉薄膜以便反射色彩。 裝置的操作可進一步藉由加入輔助電極814而改善, 其對於遮光器提供額外的力矩,當充電至一電位於輔助 電極814與遮光器812之間感應產生靜電吸引力。輔助電 極814包括導體814與支撐結構816的結合體。電極包括 —透明導體,例如ΙΤ0,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,其沉積於一單—茂 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確實地啟動。例如,假若電 極叹置於對立基底上,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微米的偏差。如此,需要影響既 疋改變處的電壓可藉由數十伏特而改變。單石的結構隨著 1077A-4732AA-PF 20 1343505 基底表面準確地變化,並且產生微量變化。 第8B圖顯示關於旋轉調制器的製造流程,步驟丨至7。 於^驟1中,基底830已經鍍上電極832及絕緣體834。 般的電極及絕緣體材料為鋁及二氧化矽,每一個厚度分 別為一千埃。這些於步驟2中形成圖案。犧牲間隔836係1077A-4 7 32AA-PF 19 »43505 Xu Qi passed. Figure 8A illustrates a reflection mode in which incident light 822 is reflected back to observer 820. In one state of this mode, if the shutter is metal fabricated, the shutter will reflect white light, or if the shutter is plated with an interference film or a skimmer, it 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. 8/688, filed on Jan. 31, 1996, 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 absorbing film or film. The 4 film may comprise another dye soaked organic film or an inductively absorbing buildup layer designed to absorb. Conversely, the shutter will be highly absorbing, i.e., appear black, and the substrate 800 is plated with a highly reflective film 824 or selectively coated with a dye film or interference film along the color reflective film lines as described above to reflect color. The operation of the apparatus can be further improved by the addition of the auxiliary electrode 814, which provides additional torque to the shutter, which induces electrostatic attraction when charged to an electrical source between the auxiliary electrode 814 and the shutter 812. Auxiliary electrode 814 includes a combination of conductor 814 and support structure 816. The electrode comprises a transparent conductor, such as ΙΤ0, which is approximately several thousand angstroms thick. All of the structures and associated electrodes are mechanically fabricated from materials that are deposited on a single-bottomed surface, such as a monolithic panel; and are therefore easily fabricated and can be reliably activated due to good control electrode spacing. For example, if the electrodes are placed on opposing substrates, surface variations of both the device substrate and the opposing substrate can be combined to produce a deviation of a majority of microns. Thus, the voltage that needs to affect the change can be varied by tens of volts. The structure of the monolith varies exactly with the surface of the 1077A-4732AA-PF 20 1343505 substrate and produces minor changes. Figure 8B shows the manufacturing flow for the rotary modulator, steps 丨7. In step 1, the substrate 830 has been plated with an electrode 832 and an insulator 834. The electrodes and insulator materials are aluminum and ruthenium dioxide, each having a thickness of one thousand angstroms. These are patterned in step 2. Sacrificial interval 836
一材料,例如數個微米厚度的矽,於步驟3中沉積且形成 圖案;接著於步驟4中鍍上柱子/旋轉樞紐/遮光器材料 838這、々為1〇〇〇埃厚度的紹合金或鈦/鶴合金。於步驟5 中,材料838已經形成圖案以便形成匯流排電極844、支 撐柱840及遮光器842。於步驟6中,遮光反射器846已 經被沉積且形成圖案。於步驟”,犧牲間隔已被蝕刻移 除產生完整的結構。步冑7亦揭示結構的上視圖,詳細顯 不包括支撐柱848、扭力臂850及遮光器852的旋轉枢紐。 切換元件 關於干涉調制器,其係二位元裝置,只需要少量電壓 • #可以驅動顯示。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 篇申凊案在此列入參考。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 方塊圖,其具有一輸入端9〇〇,藉由施加一控制信號9〇2 而連結至輸出端904。第9Β圖說明一行驅動器如何執行使A material, such as a plurality of microns of germanium, is deposited and patterned in step 3; then in step 4 is plated with a pillar/rotary hub/shader material 838, a tantalum of 1 angstrom thickness or Titanium / crane alloy. In step 5, material 838 has been patterned to form bus bar electrodes 844, support posts 840, and shutters 842. In step 6, the shading reflector 846 has been deposited and patterned. In the step ", the sacrificial interval has been etched away to produce a complete structure. Step 7 also reveals a top view of the structure, detailing the rotation hub of the support post 848, the torsion arm 850 and the shutter 852. The modulator, which is a two-bit device, requires only a small amount of voltage • # can drive the display. The driver electronics do not need to generate analog signals to obtain gray-scale operation. Therefore, the electronic components can be used on December 19, 1996. U.S. Patent Application Serial No. 08/769,947, the entire disclosure of which is incorporated herein by reference. Figure 9 illustrates this concept. Figure 9 is a basic switching block diagram having an input terminal 9〇〇 coupled to output 904 by applying a control signal 9〇2. Figure 9 illustrates how a row of drivers performs Make
1077A-4732AA-PF 21 1343505 用。用於如上所述的定址結才冓的行驅動$需要冑出三種電 壓值。施加適當的控制信號至行驅動器,允許—輸入電壓 值選擇提供給輸出端9G3。輸人電壓為^_及Vb,as, 於圖中對應於906、刪及910。相同地,關於顯示於第% 圖中的列ϋ動|§,適當的控制信號造成選擇一個或其它電 壓值’傳輸至輸出端92〇。此輸入電壓為及接 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,—N励開極利用基礎切換 方塊934、936、938及94〇。所有的元件可以此方法配置 與結合,其提供於第9 E圖中顯示的顯示次系統之製造。此 次系統包括控制邏輯926、行驅動胃924、列驅動^⑽以 及顯不陣列930,並且使用如第3圖所描述的定址結構。 此切換元件之製造,例如微機電元件,可利用—單一 步驟製造整個顯示系統。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i〇A圖令。 -步驟1顯示起始平台之上視圖與側視圖。箭號_4表 θ Η見之方向。基底】剛已沉積犧牲間隔1⑽2,㈣〇埃 0又的夕層,並且於其表面形成圖案。於步驟2中一結 ,材枓’數微米厚的銘合金,已經沉積並且曝光形成源極 10汲極1 008及間極結構1〇〇6。數百埃的不可侵蝕 金屬,例如金 '銥或鉑可鍍於此結構材料上以便於切換 期間保持低接觸阻抗。於源極剛内鞋刻形成一、凹槽 2’以便幫助源極桿於平行基底地平面移動。比較上視 圆與正面圖,也驊阁 圖立體圖顯不了步驟3與4的差異。箭號】〇】61077A-4732AA-PF 21 1343505 used. The row drive $ used for addressing as described above requires three voltage values to be extracted. Applying the appropriate control signal to the row driver allows the input-to-input voltage selection to be provided to output 9G3. The input voltage is ^_ and Vb, as, corresponding to 906, deleted and 910 in the figure. Similarly, with respect to the column flips shown in the % graph, the appropriate control signal causes selection of one or other voltage value 'transmission to output 92'. This input voltage is the sum ground ’ corresponding to 914, 916 and 918 in the figure. Figure 9D illustrates how the logic device 932 is used. In this example, the -N excitation opens using the base switching blocks 934, 936, 938, and 94. All of the components can be configured and combined in this manner, which is provided in the fabrication of the display subsystem shown in Figure 9E. This system includes control logic 926, row driven stomach 924, column driver (10), and display array 930, and uses the addressing structure as described in FIG. The manufacture of this switching element, such as a microelectromechanical component, can be used to manufacture the entire display system in a single step. This switching manufacturing step becomes the second step of the interferometric modulator manufacturing step and is illustrated in Figure IX. - Step 1 shows the top view and side view of the starting platform. Arrow _4 table θ See the direction. Substrate] A sacrificial interval of 1 (10) 2, (4) 〇 0 0 has been deposited, and a pattern is formed on the surface. At the end of step 2, the material 数's several micrometers thick alloy has been deposited and exposed to form the source 10 drain 1 008 and the interpole structure 1 〇〇 6. An impervious metal of hundreds of angstroms, such as gold '铱 or platinum, can be plated onto this structural material to maintain low contact resistance during switching. A groove 2' is formed in the source shoe to facilitate the movement of the source rod in the plane of the parallel substrate. Comparing the upper circle with the front view, the perspective view also shows the difference between steps 3 and 4. Arrow number】〇】6
1077A-4732AA-PF 表不正面之方向„於步驟3中,犧牲材 留下6敕ΛΑ、 Ύ 〇、,·生被姓刻移除, 疋整的源極桿1 010且可自由移動。 偏轉極桿及閉極結構之間施加電料’源極桿10】〇 極之門二⑽6直到與沒極剛8接觸,因此於源極與沒 心=生電性接觸。啟動模式平行於基底表面,因此允 ;步:: 驟適用於主干涉調制器製造步驟。此方法需要更 ,。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10c圖說明關於平面微機電切㈣的另 丄兩種設計。於第⑽圖中的切換器不同於,用以於汲極 ,、源極·之間接觸的切換桿m卜於第则中 的切換器中’必須流通源極桿 取地 % 7炫枰至,及極的電流將影響切換臨 1 ’使電路設計複雜化。此不是具有切換器1〇2〇的範 ’。於第10C圖中的切換器揭露另一種改善。於此範例中, 絕U)40將切換桿1 042與接觸桿觀電性絕緣。此絕 緣器可為Si〇2,其可利玥p & 已知技術沉積與曝光形成圖案。 \括此切換器之電路中,利用此切換器消除必須將邏輯 信號與切換驅動電壓電性絕緣的需要。 多維光電結構 a 一般而言,干涉調制器之特微元件具有有益的光學功 月匕’且藉由與本身或盆夕雷ijL· /、匕電子、機構或光學裝置有關的啟 動裝置而可移動。 產生了干涉堆疊的溥膜群組係單石結構的次階層,在 此當作多維的光電結構。概括地,定義一光電結構,由於 結構幾何結構及其相關變化,可以改善電磁波的行進。此1077A-4732AA-PF indicates the direction of the front side. In step 3, the sacrificial material leaves 6敕ΛΑ, Ύ 〇, and is removed by the surname. The adjusted source pole is 1 010 and can move freely. The electrode 'source pole 10' is applied between the pole and the closed pole structure. The gate 2 (10) 6 of the drain pole is not in contact with the poleless ring 8, so the source is in contact with the centerless. The starting mode is parallel to the surface of the substrate. Therefore, the steps are: Applicable to the main interferometric modulator manufacturing step. This method needs to be used to manufacture a switch that is activated perpendicular to the surface of the substrate. Figures 10B and 10c illustrate the planar microelectromechanical cutting (d) The other two designs. The switch in (10) is different from the switch used in the switch between the drain and the source, and the source must be circulated. The rod takes the ground to 7%, and the current of the pole will affect the switching of 1' to complicate the circuit design. This is not the norm with the switch 1〇2〇. The switch in Figure 10C reveals another improvement. In this example, the U)40 electrically insulates the switching lever 1042 from the contact rod. The edge can be Si〇2, which can be used to form a pattern by depositing and exposing with known techniques. In the circuit of the switch, the switch is used to eliminate the necessity of electrically isolating the logic signal from the switching drive voltage. Needed. Multi-Dimensional Optoelectronic Structure a In general, the ultra-micro-element of an interferometric modulator has a beneficial optical power function and is activated by itself or with a starter associated with the ray, the electron, the mechanism or the optical device. Movable. The sub-layer of the monolithic structure of the interference film stack is generated as a multi-dimensional optoelectronic structure. In general, a photoelectric structure is defined, which can improve electromagnetic waves due to structural geometry and related changes. Travel. This
1077A'4732AA-PF 23 結構可與光於沿著— 如η*㈣”方向作用。多維的結構亦 如同光電頻f差距处槿(ρβΓ, 、·Ό構(PBG s)或光電晶體。John D. Joannopoulos等人撰寫的v · Ή…丄· 撰罵的Ph〇t〇nlc Crystals"說明了 週期性的光電結構。 一維的PBG可出現於一續 、核隹叠的型式中。例如,第 16圖顯不一介電法右 苴製 各濾波器型式的干涉調制器及 ,、1坆方法。4骐堆積1614盥 — ” U18,例如間隔的矽層與 氧化石夕層’母一個是分 .. 疋四刀之一波長厚,製造於一基底上, 以便形成具有中心孔穴1 从工土 土 &上 涉調制器結構。-般而 5 堆疊係連續於X盥γ太A , ^ ^ β ,由於材料之折射率變化, 於Ζ方向具有週期性 交替的古„ 的先子效β,只要當它們是具有間隔 父替的同、低折射率層。此 於产荖 考慮為一維的,因為對 最;:早—轴’例如2轴方向行進的光波,週期性功效係 二广圖與第11Β圖說明兩種二維光 於第UA圖中,微環狀共 1式 畔多P 4 益1102可利用已知的技術使用 許夕已知的材料製造,例如五 jw. ,.λ E ^ , —氧化石夕的合金。 h波長為1.55微米範圍改良的裝置,一 ㈣,^1.0^,以及 Γ=1〇^。 ' 於一基底1100上(例如玻螭, f ± a m ^ ·* ii· ^ 許^可選擇),結構 '為圓先波導,其折射率及尺寸 其内的丨汉11决疋仃進於 丹内的先的頻率及模式。 可以含柞相玄 、類的、振盗,假若設計正確, Τ以田作頻率選擇光 <«•益Mb 以便將寬頻帶傳播耦合進入。於 此輕例令,此傳播一 4 ^ 々、 傳播I仃進於如圖所標示的符號"Ο!的The structure of 1077A'4732AA-PF 23 can interact with light in the direction of - such as η * (four). The multidimensional structure is also like the difference of the photoelectric frequency f (ρβΓ, Ό structure (PBG s) or photoelectric crystal. John D Joannopoulos et al., written by Ph.t〇nlc Crystals", explains the periodic optoelectronic structure. One-dimensional PBG can appear in a continuous, nuclear-folding pattern. For example, Figure 16 shows the different types of interferometric modulators of the filter type and the 1坆 method. 4骐 stacked 1614盥—” U18, for example, the interstitial layer and the oxidized stone layer are the same. .. One of the four knives is thicker in wavelength and is fabricated on a substrate to form a central cavity with a central cavity 1 and a modulator structure. -5 stacked lines are continuous with X盥γ too A , ^ ^ β, due to the change in the refractive index of the material, has a periodic alternating ancient primal effect β in the Ζ direction, as long as they are the same, low refractive index layer with the spacing of the parent. This is considered to be one-dimensional in calving. Because of the most;: early-axis', for example, the light wave traveling in the 2-axis direction, periodic effect The two-dimensional map and the eleventh-first graph illustrate two kinds of two-dimensional light in the UA diagram, and the micro-rings have a total of one type and more P 4 benefits 1102 can be fabricated using known techniques using materials known by Xu Xi, such as five jw , .λ E ^ , —Oxide oxide alloy. Improved device with h wavelength in the range of 1.55 μm, one (four), ^1.0^, and Γ=1〇^. 'On a substrate 1100 (eg glass, f ± am ^ · * ii· ^ Xu ^ can be selected), the structure 'is a circular first waveguide, its refractive index and size within the Aohan 11 decided to enter the first frequency and mode of Dane. , class, and theft, if the design is correct, 选择 选择 田 田 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择 选择As indicated by the symbol "Ο!
1077A-4732AA-PF 24 1343505 平面中。此褒置的一維類似物將會是利 造的法右田4 ^早一鏡面層製 -派洛濾波器。由於單一邊界層( ^ 裝置能維持—高階光學 a ,沒有 门μ尤千週期,然而,可以視 光電結構。 兄頻效用的 方 如 質 ;弟UB圖中顯示更多的傳統PBG。於 向’列陣列11。6呈現-週期變化的折射率:向_與隹 圖斛护-以狀 版右仃進;!1077A-4732AA-PF 24 1343505 In the plane. The one-dimensional analog of this device will be the manufactured Fukuda 4^ early-mirror-Pylo filter. Due to the single boundary layer (^ device can maintain - high-order optics a, no gate μ is more than a thousand cycles, however, the photoelectric structure can be considered. The side of the brother frequency effect is qualitative; the younger PBG is shown in the UB diagram. The column array 11.6 exhibits a refractive index that changes periodically: toward _ and 隹 斛 - - to the right side of the shape;
:仏不的符號U03的XY平面範圍内,行進通過此/ 、電磁傳播係最顯著的被影響。 ★因為其週期的自然特性,帛11B圖的陣列共同使用— 維4膜堆積層的属性,除了其更高階的維 人 π ΛΥ平面 内,沿著通過陣列的某些座標軸,此陣列係週期性·,折射 率係於圓柱材料與周邊材料之間變化,週邊材料—般為允 氣。利用應用於薄膜堆積設計之相同原則的變化,適:< 計此陣列,允許製造大範圍變化的光學共振器,(鏡面、波 段通過濾波器、邊緣濾波器),作用於χγ平面中行進的傳 播。於第11Β圖範例中顯示的陣列丨丨〇6包括圓桎形式的一 畸點或缺陷1108,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 刀之波長)’或其差異為材料(例如空氣相對二氧化石夕) 陣列的整個尺寸藉由光學系統或元件之尺寸決定,其必須 巧妙地處理。依據其需要的特性,此缺陷亦可以—列戍多 列形式出現。此結構類似於第61圖中的介電法布里派、各 濾波器’但只作用於二維範圍中。於此範例中,缺陷類似 於孔穴1 61 6。剩餘圓柱類似於鄰近的二維堆積。 l〇77A-4732AA-PF 25 I3435U5 第圖結構的相關維度藉由列χ間隔 -(兩者可視作晶格)、圓柱直心 ]:間: 似四分之一波异地r 』门又h表不。類 # 、$ ’ —維當量、®柱直徑及間隔為四分 之 波長等級0文)# U I工 …經由需要行進模式而決定,對於單 一核式仃進具有務料女 平 寸之算… 關於作用於光的結構尺 、 ’、 且藉由John D. Joannopoulos等人證明 於教科書、Ph〇tonicCrystais,中。 。且月 此種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1的單—薄膜可利用習知技術沉積於 玻璃基底上並且形成圖帛,接著利用易反應的離子敍刻梦 造好外觀比例的圓柱。例如’波長155/zm,圓柱的直徑 與間隔分別為〇. 5 // m及〇. 1 // 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 光於XY平面中行進,強迫光於小於光波長的空間中度 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圖中說明三維結構。三維週期結構1 2 0 2作用 於XY、YZ及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 計規則,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,其與周邊介質不同於尺寸及/或折射 率。於第12圖中’缺陷1 204係一單一點元件,但是亦可 1077A-4732AA—PF 26 1343505 能為線型或線與點元件或區域的結合。例如,可以製造_ 、線型、'碗蜓,缺陷點陣列’其依據任意的三為路徑 =過PBG’並且當作用以使光於其中傳輸的—緊密束缚波 導。缺陷-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。咖之直徑'間隔及 材枓係完全相關的,然而亦可利用上述設計規則。 製造三維的ms係更複雜。關於製造一維或二維特徵 的習知裝置,假若應用於三維中,將加入更多的沉積、藥 影及姓刻循環以便獲得三維的結構。對於製造週期性三維 結構之製造技術包括:全像顯影,其中—光感應材料以— 標準波曝光並且於材料内摺φ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㈣有的黏著 及某二異里刀子聚合材料之方向特性,於沉積材料期間 產生圓柱陣列或球狀結構,可加入陶竟方法,提供球狀結 構控制尺寸成液體懸浮,一但固化、組織此結構並且可藉 由溶解或高溫而移除;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苯乙 WPPQmPSr〇轉碳中1溶液塗佈於基底上且使 溶劑揮發後,產生氣體充滿聚合物球體内的緊密六角型拼 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Μη)之重複單元數目,控制陣列之週期。使用 微米大小,包括金屬、氧化物半導體的夥狀體,具有減少: In the XY plane of the symbol U03, the most significant influence is caused by the travel of this / and the electromagnetic propagation system. ★ Because of the natural nature of the period, the array of 帛11B is used together—the properties of the 44 film stack, except for its higher-order π ΛΥ plane, along the coordinate axes of the array, the array is periodic. The refractive index is changed between the cylindrical material and the surrounding material, and the surrounding material is generally a gas. Using the same principles applied to the thin film stacking design, it is appropriate to: < Measure the array, allowing the fabrication of a wide range of optical resonators (mirror, band pass filter, edge filter) acting in the χγ plane propagation. The array 丨丨〇6 shown in the example of Fig. 11 includes a distortion or defect 1108 in the form of a circle which is different from the size and/or refractive index. For example, the diameter of the cylinder is slightly larger or smaller than the other cylinders (eg, the diameter of the four-knife difference in diameter) or its difference is the material (eg, air versus dioxide). The entire size of the array is determined by the size of the optical system or component. , it must be handled skillfully. Depending on the characteristics required, this defect can also occur in multiple columns. This structure is similar to the dielectric Fabry, filter ’ in Fig. 61 but acts only in the two-dimensional range. In this example, the defect is similar to the hole 1 61 6 . The remaining cylinders are similar to adjacent two-dimensional stacks. l〇77A-4732AA-PF 25 I3435U5 The relevant dimensions of the structure of the figure are shown by the column spacing - (both can be regarded as a crystal lattice), the cylinder is straight]: between: a quarter wave is different from the ground r 』 . Class #, $ ' - Dimensional Equivalent, ® Column Diameter and Interval is a quarter-wavelength level 0)) The UI work... is determined by the need for the travel mode, and for the single-core expansion, there is a calculation of the female level... The structural rule acting on light, ', and proved by John D. Joannopoulos et al. in textbooks, Ph〇tonic Crystais. . And this structure is also manufactured using the same materials and techniques used to fabricate the resonator (10). A mono-film of, for example, 1 can be deposited on a glass substrate using conventional techniques and formed into a pattern, and then a column of the appearance ratio can be created using a reactive ion. For example, 'wavelength 155/zm, the diameter and spacing of the cylinder are 〇. 5 // m and 〇. 1 // m. 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 that transmits light traveling in the XY plane, forcing the light to moderately transition in a space less 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 three-dimensional structure is illustrated in Fig. 12. The three-dimensional periodic structure 1 2 0 2 acts on the propagation of travel in the XY, YZ and XZ planes. Various optical responses can be obtained by appropriate structural design and selection of constituent materials. Apply these same design rules, however, apply 3D here. Defects occur in points, lines or regions relative to points and lines, which differ from the surrounding medium in size and/or refractive index. In Fig. 12, the defect 1 204 is a single point element, but it is also possible that 1077A-4732AA-PF 26 1343505 can be a line or a combination of line and point elements or regions. For example, _, line type, 'bowl 蜓, array of defect points' can be made which is based on any three paths = over PBG' and acts as a tightly bound waveguide for transmitting light therein. Defects are generally located within them, but are shown on the surface for illustrative purposes. The relevant dimensions of this structure are illustrated in the drawings. The diameter of the coffee's spacing is completely related to the material, but the above design rules can also be used. Making a three-dimensional ms system is more complicated. Conventional devices for making one-dimensional or two-dimensional features, if applied to three-dimensional, will add more deposition, artifacts, and surname cycles to obtain a three-dimensional structure. Manufacturing techniques for fabricating periodic three-dimensional structures include: holographic development, in which a light-sensitive material is exposed to a standard wave and folded into a material to form a refractive index change pattern; a self-organizing organic material or a self-bonding material According to (4) some adhesion and the directional characteristics of a certain dissimilar kiln polymeric material, a cylindrical array or a spherical structure is generated during the deposition of the material, and the ceramic method can be added to provide a spherical structure to control the size into a liquid suspension, once cured, organized This structure can also be removed by dissolution or high temperature; a combination of the above methods and the like. Heterogeneous molecular polymerization techniques and self-binding techniques are of particular concern because both are low temperature and require little or no exposure to development. [This technique includes polymer dissolution, such as polyphenylquinic block polyphenylene. After the B solution of the WPPQmPSr 〇 carbon is coated on the substrate and the solvent is volatilized, a tight hexagonal arrangement in which the gas is filled in the polymer sphere is generated. This technique can be repeated multiple times to produce a number of layers; the period of the array can be controlled by the number of repeating units using the high molecular unit Μη). Use micron size, including metal, oxide semiconductor, with reduced
1077A-4732AA-PF 27 陣列週期之功效,進—步 _ /』日加间分子的折射率。 經由直接將材料運用次微米等級的聚 力顯微鏡等工具,產生缺陷。束2原子 j J用於非常小的選擇 &域内,移除或加入材料; 次用以改變材料的光學特性。 產生於當具有能量的粒子束’例如使用聚焦離子 ΐ…:上嘴除材料。材料加入發生於當聚焦離 一易揮發的、含有氣體的金屬,例如六氟化鎢 (鶴導體)或四氟切(絕緣的二氧切)。氣體減緩速度, 且組成物沉積於離子束接觸基底處。 另種方法包括使用稱之為微電極沉積㈣ 詳細㈣於美國專利案第5,641 391號。於此方法中:可 利用一單一微觀電極,定義 解析度之三維特徵。利用=;材底的次微米 利用此方法沉積的金屬、缺陷〃大體 被氧化’以便形成m陣列圍繞的介電缺陷,PBG陣列係 使用上述技術製造。 存在表面上的特徵為 v甘 马以其他材料圖案之形式,例如 於基底表面上製造PBG陣列;於缺陷形成期間,於pBG範 圍内亦可以當作產生缺陷的樣板。這特別係有關於對於基 底狀況敏感的m方法,主要地自我組合方法。根據方法 的:殊性質’此方法可促進或抑制PBG之、'成長々於被晶 種兩度圍繞的局部區域。於此方法中,缺陷 ''晶種、圖 案可以被製造…美,於形成PBG期間,於缺陷產 圍内形成PBG。 因此’已知為干涉調制器的裝置之種類藉由將更多種1077A-4732AA-PF 27 The effect of the array period, the step-by-step _ / 』 the refractive index of the molecule between the days. Defects are created by direct application of materials to tools such as submicron grade condensers. Beam 2 atoms j J is used for very small selections within the & domain, where materials are removed or added; and times are used to alter the optical properties of the material. It is produced when a particle beam having energy is used, for example, using a focused ion ΐ...: upper mouth to remove material. Material addition occurs when focusing on a volatile, gas-containing metal such as tungsten hexafluoride (helicopter conductor) or tetrafluoroethylene (insulated dioxane). The gas slows down and the composition deposits at the ion beam contacting the substrate. Another method includes the use of what is called microelectrode deposition (4). Details (4) U.S. Patent No. 5,641,391. In this method, a single microscopic electrode can be used to define the three-dimensional features of the resolution. Using the sub-micron of the substrate, the metal deposited by this method, the defect 〃 is generally oxidized' to form a dielectric defect surrounded by the m array, and the PBG array is fabricated using the above technique. There are features on the surface that v-Gamma is in the form of other material patterns, such as PBG arrays on the surface of the substrate; during the formation of defects, it can also be used as a template for defects in the pBG range. This is especially relevant for the m method, which is sensitive to the condition of the substrate, mainly the self-assembly method. According to the method: the nature of this method can promote or inhibit the PBG's 'growth' from the local area surrounded by the seed crystal twice. In this method, the defect ''seed, pattern can be made...before, during the formation of PBG, PBG is formed within the defect area. Therefore, the type of device known as an interferometric modulator is more
1077A-4732AA-PF 28 ,維先電結構加入調制器本身’而變得更多。任何光 =構,固有為靜態裝置,可藉由改變其幾何及/或改變其 =㈣心。㈣地’微機構法布里〜派洛遽波 :(於第16圖中所示)’包括兩個鏡面,每一個為一雉的光 L告構,可藉由靜電地改變空穴寬度而調整。 第13圖顯示加入二維的、土… 」之干涉調制器設計的兩 ^例。於第13A圖令,一部份切除的圖案揭露一自我支 樓的薄膜1 304’其被製造且固定於面對基底側上,並且具 有—微環狀共振器13〇6。橫臥於基底13〇3内部的波導ι3〇ι 及1302係平的且平行,並且可利用已知技術製造。於第 W圖中,干涉調制器顯示處於未被驅動狀態,於微環狀 。土底之間具#冑限的空氣間隔。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。剖面圖1 305顯示波導之尺寸,$ w=Umm 及t = i〇〇nm。於未被驅動狀態中,光13〇8未分布的傳導於 波導1302内,並且輸出光束131〇之光譜完全相同於入射 光束1308。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13〇2中行進的 光可藉由消逝現象耦入微環狀。此微環狀,假若大小適當, &作一光學共振器,將挑選的頻率自波導〗3〇2耦出且引入 波導1301。此顯示於第13B圖中,其中光束1312顯示行 進於與光束1 308方向相反的方向。這類的裝置可當作頻率 選擇切換器使用;藉由施加電壓,或其它需要將此結構與 k躺的波導緊密接觸的驅動裝置,可將特殊的波長自波導 1077Α-4732ΑΑ-ΡΓ 29 1343505 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 Coupled Microring1077A-4732AA-PF 28, the first electrical structure is added to the modulator itself' and becomes more. Any light = structure, inherently a static device, can be changed by changing its geometry and/or changing its = (4) heart. (4) The ground's micro-fabric Fabri-Pylopo: (shown in Figure 16) 'contains two mirrors, each of which is a glimpse of light, which can be electrostatically changed by the hole width. Adjustment. Figure 13 shows two examples of the addition of a two-dimensional, earth-like interferometric modulator design. In Fig. 13A, a partially cut-away pattern reveals a self-supporting film 1 304' which is fabricated and fixed on the side facing the substrate and has a micro-ring resonator 13〇6. The waveguides ι3〇ι and 1302 lying inside the substrate 13〇3 are flat and parallel, and can be fabricated using known techniques. In Figure W, the interferometric modulator is shown in an undriven state, in a micro-ring. There is an air gap between the soil bottoms. 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. Section 1 305 shows the dimensions of the waveguide, $ w = Umm and t = i 〇〇 nm. In the undriven state, light 13〇8 is undistributed within waveguide 1302, and the output beam 131〇 has a spectrum identical to incident beam 1308. The interferometric modulator is driven to force the micro-rings to closely contact the substrate and the waveguide, changing the optical properties of the device. Light traveling in the waveguide 13〇2 can be coupled into the microring by an evanescent phenomenon. This micro-ring, if properly sized, is an optical resonator that couples the selected frequency from the waveguide 〇3〇2 and introduces it into the waveguide 1301. This is shown in Figure 13B, where beam 1312 is shown traveling in the opposite direction of beam 1 308. This type of device can be used as a frequency selective switch; a special wavelength can be selected from the waveguide 1077Α-4732ΑΑ-ΡΓ 29 1343505 by applying a voltage or other driving device that requires the structure to be in close contact with the lying waveguide. come out. The electrostatic description of this geometry has been described in a paper by B. E Little et al., Vertically Coupled Microring
Resonator Channel Dropping Filter" , IEEE Photonics Technology Letters, vol· 11, no· 2, 1999。 於第1 3 C圖中說明另一範例。於此範例中,一對波導 1332及1330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—個)定 義波導,並且藉由移除兩列定義共振器。上視圖提供更詳 細的波導1 330與1332及共振器1314之結構。尺寸係與重 要的波長以及使用的材料有關。對於1. 55 " m波長,圓柱 的直徑與間隔分別為〇. 5 // m及1 // m。高度h決定行進模 式,其將被支撐且稍微大於半波長,假若只有單一模式傳 播。 於薄膜1315之内表面上製造兩個獨立的圓柱i3u, 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 成彼此相配;於共振器中對應出現一圓柱’其中適當的於 薄膜上設置圓柱。 當干涉調制器處於未被驅動狀態,具有—有限的垂直 空氣間隔1312,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1330及1332之間產生耦合。 於此狀態中’裝置如同第13B圖中顯示的作用,並且沿著 波導行進的光選擇頻率’現在注入波導丨332中,並且與光 1077A-4732AA-PF 30 1343505 1329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 置於共振器改變其特性。共振器之缺陷藉由配置薄獏圓柱 而消除。利用行進時未干涉的光1 328,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 Channel drop filters in photonic crystals" , OpticsResonator Channel Dropping Filter" , IEEE Photonics Technology Letters, vol· 11, no. 2, 1999. Another example is illustrated in Figure 13C. In this example, a pair of waveguides 1332 and 1330 and a resonator 1314 are fabricated in a cylindrical shape on a substrate. The PBG is the same cylindrical array, the waveguide is defined by removing two rows (each waveguide), and the resonator is defined by removing two columns. The top view provides a more detailed structure of the waveguides 1 330 and 1332 and the resonator 1314. The size is related to the important wavelength and the materials used. For the 1.55 " m wavelength, the diameter and spacing of the cylinder are 〇. 5 // m and 1 // m, respectively. The height h determines the travel mode, which will be supported and slightly larger than half a wavelength, if only a single mode is propagated. Two separate cylinders i3u are formed 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 the same optical properties). The resonator and the cylinder are designed to match each other; a cylinder is correspondingly present in the resonator, wherein a cylinder is suitably disposed on the film. When the interferometric modulator is in an undriven state, it has a finite vertical air gap 1312 that is at least a few hundred nanometers between the PBG and the thin film cylinder, and thus no optical interaction occurs. The cylinder appearing in the resonator acts as a defect, creating a coupling between the waveguides 1330 and 1332. In this state, the device acts as shown in Fig. 13B, and the light selection frequency ' traveling along the waveguide is now injected into the waveguide 332 and travels in the opposite direction to the light 1077A-4732AA-PF 30 1343505 1329. The interferometric modulator is driven into contact with the PBG, however, placing the cylinder properly in the resonator changes its characteristics. The defects of the resonator are eliminated by arranging the thin cylinder. With the light 1 328 that does not interfere when traveling, the device in this state acts as shown in Figure 13A. A description of the static electricity of this geometry has been published in the paper by H A. Haus. Channel drop filters in photonic crystals" , Optics
Express, vol. 3, no, i, i998 〇 光學切換器 於第14A圖中,根據感應吸收器的裝置包括—自我支 撐鋁薄膜1400,位於數十至數百微米平方上,懸浮於材料 堆積層1402上,此材料堆積層包括金屬與氧化物的組合物 的且於透明基底上形成既定圖案。於感應吸收調制器中使 用的薄膜適合此目的,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Express, vol. 3, no, i, i998 〇 Optical Switcher In Figure 14A, the device according to the inductive absorber includes a self-supporting aluminum film 1400, located on the tens to hundreds of micrometers square, suspended in the material accumulation layer. At 1402, the buildup layer of material comprises a combination of a metal and an oxide and forms a predetermined pattern on the transparent substrate. </ RTI> <RTIgt; to
基底上的薄膜亦包括一透明導體,例如IT〇。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。 使用此材料,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 W某-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1406。假設光的頻率與處於未駆 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。侧視圖’ 1414,顯示處於驅動狀態的相^ 31The film on the substrate also includes a transparent conductor such as IT〇. The structure may be followed by a metal film such as molybdenum or tungsten, a thickness of several hundred angstroms. This material is used so that in the undriven state, the device reflects a specific range of wavelengths and becomes as strong as possible when the film is driven into contact therewith. Side view 1410 shows a view of one of the devices, viewed from the side of the substrate. Beam 1408 is propagated within the substrate at any angle and is incident on an interferometric modulator 1406 that is shown in an undriven state. Assuming that the frequency of the light coincides with the range of reflection of the interferometric modulator in an untwisted state, the light is reflected at a complementary angle and away. Side view '1414, showing the phase in the drive state ^ 31
1077A-4732AA-PF1077A-4732AA-PF
JKJJ 干涉調制器。因為裝置現在極力 不再被反射’並且藉由干涉調制器堆疊的:::二的光 制号,對;配置中’製造可當作光學切換器的干涉調 對於仃切基底㈣光 ::成非常光滑、非常平坦(於注重的光…:長: 並且較先的波長還長數倍(至少數百微米 底當作基底/波導使用,光束於其中以某-方向行進,= 而言,平行於基底,但是從一表面至另—表面經過多次反 射。於此結構中的光波經常當作基底導向波。 第14B圖顯示此發明之一變化。形成既定圖案的薄膜 ^20’不再是矩形而是—端逐潮變尖。當結構的機構彈箬 常數沿著此長度維持不變,減少電極面積,於錐形 物之尖端施加靜電的力量大小係較小的。假若逐漸增加電 壓將首先於較寬端驅動薄膜,接著當電壓增加時,將沿 著箭號1428方向啟動。 對於入射光,+涉調制器當作一吸收區域操作其中 根據把加電壓值決定面積Q側視圖1434顯示當沒有施加電 壓時’於基底上傳播光束的結果。對應的反射區域1429, 即入射光束的立體圖顯示干涉調制器,顯示光束於反射區 戍重疊蹤跡143卜因為整個區域1429不會吸收,光束143〇 自干涉調制器丨428反射成光束1432的形式。 於側視圖1 436中,施加一暫時電壓值,並且反射光束 1440已經衰減至某種程度,因為被顯示的反射區域丨437 P伤吸收。圖式1438與1429顯示完整作用的結果以及光JKJJ Interferometric Modulator. Because the device is now no longer being reflected too much' and by interfering with the modulator's stack of ::: two light gauges, pairs; in the configuration 'manufacturing can be used as an optical switcher's interference modulation for the chopped base (four) light:: Very smooth, very flat (focus on light...: long: and the previous wavelength is still several times longer (at least hundreds of micrometers are used as the substrate/waveguide, where the beam travels in a certain direction, = parallel On the substrate, but from multiple reflections from one surface to the other surface. The light waves in this structure are often used as the substrate guiding waves. Figure 14B shows a variation of the invention. The film forming the predetermined pattern ^20' is no longer The rectangle is—the end of the tide is sharp. When the mechanical constant of the structure is kept constant along this length, the electrode area is reduced, and the force of applying static electricity to the tip of the cone is small. If the voltage is gradually increased The film is first driven at the wider end, and then when the voltage is increased, it will be activated in the direction of arrow 1428. For incident light, the + modulator acts as an absorption region where the area Q is determined according to the applied voltage value. 4 shows the result of propagating the beam on the substrate when no voltage is applied. The corresponding reflection region 1429, ie the perspective view of the incident beam, shows the interferometric modulator, showing that the beam overlaps the trace 143 in the reflection region because the entire region 1429 does not absorb, The beam 143 is reflected from the interferometric modulator 428 into the form of a beam 1432. In side view 1 436, a temporary voltage value is applied and the reflected beam 1440 has decayed to some extent because the displayed reflective region 丨437 P is injured. Absorption. Figures 1438 and 1429 show the results of the full effect and light
1077A-4 732AA-PP 束完全衰減。 ^ τίκ J M眾造可調制光學衰 囚此’藉由使用 減器,其反應直接與施加電壓值有關 ::種光學切換器說明於第15A圖中。支擇結構测 :利用金屬製造’例如數千埃厚度的#,以此方…一 鏡面職電性連接。鏡面1502存在於透明的光以座The 1077A-4 732AA-PP beam is fully attenuated. ^ τίκ J M can be modulated by optical attenuation. By using a reducer, the response is directly related to the applied voltage value. :: The optical switch is illustrated in Figure 15A. Selective structure measurement: using metal to make ', for example, thousands of angstroms of thickness #, in this way... a mirrored electrical connection. Mirror 1502 exists in transparent light
? ’其黏接於支撐物1 500。鏡® 1502可包括一單一金 屬薄膜或金屬氧化物以及半導體薄膜。?' It is bonded to the support 1500. Mirror® 1502 can include a single metal film or metal oxide and a semiconductor film.
支架係利用材料製造,材料具有等於或大於基底的折 射率。廷可為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度變 化特徵的光罩,可完成支架之製》。於一特定的表面上, 藉由適當的變化密纟’並制此光罩曝光,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 1 505。換句話說,一塊導體15〇3已經被蝕刻移除因此窗 1 5 0 5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 其光學特性。光束1510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。 1077A-4732AA'PF 33 1343505 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1 506處於未被驅動狀態,並 且光束1510以暢通無阻的方式行進。當切換器15〇6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 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TIR ; 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。一相似的觀念已揭露於X. Zhou 等人於 1 998 年,siDDigest,vol. XXIX 的論文 1avegUideThe stent is made of a material having a refractive index equal to or greater than the substrate. Ting can be a SiO 2 (same refractive index) or a high refractive index polymer having a variable refractive index. The brackets are manufactured to the specified dimensions, so the mirrors are supported at a 45 degree angle. Utilizing a yellow-like lithography technique, which can be completed according to a reticle that continuously changes its optical density. On a particular surface, a three-dimensional shape can be formed in the photoresist by appropriately varying the density and making the reticle exposure. 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 1 505 on the underlying substrate 1 504 that does not block light. In other words, a piece of conductor 15〇3 has been etched away so window 155 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 its optical properties. The beam 1510 is within the substrate and propagates at a 45 degree angle to the normal to prevent 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). 1077A-4732AA'PF 33 1343505 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. The device in side view 1512 shows that the switch 1 506 is in an undriven state and the beam 1510 travels in an unobstructed manner. When the switch 15〇6 is activated and in contact with the substrate, the beam path is changed as shown in side view 1514. Since the stent has a refractive index greater than or equal to the substrate, the beam no longer undergoes a TIR at the interface. 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. The result 'light can penetrate the substrate interface because it no longer satisfies TIR; 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., 1 998, siDDigest, vol. XXIX, paper 1avegUide
Panel Display Using Electromechanical SpatialPanel Display Using Electromechanical Spatial
Modulators々。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柵,可利用習知曝光技術蝕刻支架之 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,另一種光學 結構可替代鏡面,如同其屬性與短處。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、稜鏡及任何其它 形式的光學元件,並且可利用微製造技術產生。於使用另 一種光學件的範例中,支架及角度給予的光學可能與微 光學種類無關。 干以調制裔之變化當作光的解耦合切換器使用^假若Modulators々. This particular device is designed for illuminating display applications. The mirror can also be incorporated with a reflective grating that can be etched using conventional exposure techniques. However, this method shows wavelength dependence, and the loss due to multi-order diffraction is not the result of the film mirror. In addition, another optical structure can replace the mirror as its properties and shortcomings. 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, germanium, and any other form of optical element, and can be utilized Microfabrication technology is produced. In an example where another optic is used, the optics imparted by the stent and angle may be independent of the type of micro-optics. Use the decoupling switcher that uses the change of the genus as the light.
1077A-4732AA-PF 34 1343505 面设计 /6¾ 5 Φ 'rK ίΠ- 、'皮導Μ ^ 特定頻率可任意的自基底/ 波糊。側視圖㈣顯示更多複雜的改良,其中—額外 的固定鏡面,以失角45度製 的相對傾“山 A1"於具有解輕合切換器之基底 . 鏡面與切換器不同’其不可以被啟動。藉 由小心選擇於兩種結構上的鏡面, 錐I麻丄 又已、有效率地耗合 離開基底的光1522藉由切換琴15〇6, γ s ~ 面再輕合回美“ 6可再錯由再輕合鏡 π柄口回暴底。然而,於χγ ^ n e. ^ 、λΥ十面中错由製造具有 不冋疋位方向的再耦合鏡 ~r s a 1 , 於綦底Λ皮導内,鏡面結合體 可再•人導引光至任何新方向。 沾 ^ 此兩種^構的結合體將參考 虽作一方向切換器使用。 再耦口鏡面亦可用來耦合任何 以垂直於表面方向傳播進入基底中。 第15Β圖顯示一種使用古―& 麻… 使用方向性切換器之陣列。俯瞰基 底1 535,線性陣列j 536係一 ..^ . γν ^ 先纖耦3益陣列,其引導光 乂垂直於_χ γ平面之角唐^隹 ι _ 土底。一再耦合鏡面陣列(耒 :示)直接設置於與光纖耗合器陣列相對之位置,以便將光 ^合入平行於光束測的基底卜㈣底之表面聰上, 製造了方向性切換器陣列,其, 31係其中一個。以特殊 方法設置切換器’因此自任一铨 輸入先纖耦合器1 536耦合進 入基底的光,可引導至任一鉍山,λ 輸出光纖耦合器1 532。利用此1077A-4732AA-PF 34 1343505 Surface design /63⁄4 5 Φ 'rK ίΠ- , '皮导Μ ^ Specific frequency can be arbitrary from the substrate / wave paste. The side view (4) shows more complicated improvements, in which - the additional fixed mirror, the opposite tilt of the 45 degree system "mountain A1" on the base with the decoupling switcher. The mirror is different from the switcher" it can not be By carefully selecting the mirrors on the two structures, the cone I paralyzed and efficiently dissipates the light 1522 leaving the substrate by switching the piano 15〇6, and the γ s ~ surface is again lighted back to the United States. Can be mistaken by the re-lighting mirror π handle mouth back to the bottom. However, in the χγ^ n e. ^, λΥ 面 面 由 由 由 由 由 rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs rs Any new direction. The combination of the two structures will be used as a direction switcher. The re-coupling mirror can also be used to couple anything that propagates into the substrate perpendicular to the surface. Figure 15 shows an array using an ancient- & hemp... directional switcher. Overlooking the base 1 535, the linear array j 536 is a .. ^ . γν ^ first fiber coupled to the 3 y array, which guides the pupil perpendicular to the corner of the _χ γ plane Tang ^ 隹 ι _ soil bottom. A re-coupling mirror array (耒: shown) is directly disposed at a position opposite to the fiber consumable array, so that the light is merged into the surface parallel to the bottom surface of the beam, and a directional switcher array is fabricated. It is one of the 31 series. The switch is set in a special manner so that light from any of the input fiber couplers 1 536 coupled into the substrate can be directed to either of the mountains, λ output fiber coupler 1 532. Use this
方法之裝置可當作一 Ν X 的先學切換器使用,其可以切 換任一不同的輸入至任一不同的輸出。 可調制濾波器 參考第】6圖,顯示_可难糸丨土 + J调制法布里-派洛濾波器形式 的干涉調制器。於此範例中, ,儿積一導電接觸墊1 602,並The device of the method can be used as a learning switch for X, which can switch any different input to any different output. Modulable Filter Refer to Figure 6 for an interferometric modulator in the form of a _ 糸丨 糸丨 + + J modulation Fabry-Perot filter. In this example, a conductive contact pad 1 602 is accumulated, and
i〇77A-4732AA-PF 35 以 3505 且沿著介面鏡面1604與刪及犧牲層赚形成圖案。這 包括一石夕薄膜,其厚度為半波長之某些倍數。鏡面可包括 ㈣堆叠’例如Τ1〇2(高折射率)與⑽(低折射率),且有 Γ的高、低折射率’並且其中-層亦可為空氣。沉積絕 緣屬wo,並且形成圖案,使得第二接觸墊i6i2只接觸 鏡面刪。形錢案的鏡面删大體留τ_鏡面Ύ ㈣,藉由支撐物1615連接1的橫向尺寸主要藉由將交 互作用之光束大小而決定。—般約為數十至數百微米等 級。犧牲層16G6係部份被化學㈣,而留下適當大小的支 架以便提供機構敎性’大概為十微米平方。假㈣面刪 之頂層與鏡面1 604之底層輕微地摻雜以便導電,則接觸墊 1 602與1612之間施加的電壓將造成鏡面島離開。因此, 可開啟此結構之光學響應。 第i7A圖顯示此可調制濾波器之應用。基底1714之上 表面上已經製造可調制濾波器17G4、鏡面1716及抗反射 鍍膜m2。—鏡面1717已經製造於基底之下表面上,例 如形成-金属’像是至少1GGnni厚度之黃金。固定於基底 之上表面上的是一光學超結構1 706,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。The i〇77A-4732AA-PF 35 is patterned with 3505 along the interface mirror 1604 and the sacrificial layer. This includes a stone film having a thickness that is a multiple of a half wavelength. The mirror may include (iv) a stack 'e.g., Τ1〇2 (high refractive index) and (10) (low refractive index), and has a high and low refractive index ' of germanium and the layer may also be air. The deposition insulation is wo and is patterned such that the second contact pad i6i2 is only in contact with the mirror. The mirror of the money case is deleted from the mirror Ύ (4), and the lateral dimension of the connection 1 by the support 1615 is mainly determined by the beam size of the interaction. Generally, it is about tens to hundreds of micrometers. The sacrificial layer 16G6 is partially chemically quarantined, leaving a suitably sized support to provide mechanical flexibility of approximately ten micrometers squared. The dummy (four) face-cut top layer and the bottom layer of mirror 1 604 are slightly doped to conduct electricity, and the voltage applied between contact pads 1 602 and 1612 will cause the mirror island to exit. Therefore, the optical response of this structure can be turned on. Figure i7A shows the application of this tunable filter. A modulatable filter 17G4, a mirror surface 1716, and an anti-reflection coating m2 have been fabricated on the upper surface of the substrate 1714. - Mirror 1717 has been fabricated on the underlying surface of the substrate, e.g., forming a -metal' image of gold at least 1 GGnni thickness. Mounted on the upper surface of the substrate is an optical superstructure 1706 having an inner surface having a reflectivity of at least 95%, such as by an additional reflective gold film, and supporting a tilted mirror surface 1710. In this device, the beam 17 〇 2 travels within the substrate at an angle greater than the critical angle, with a critical angle of .41 degrees with respect to the glass substrate and the air medium. Therefore, it is necessary to keep the mirror 1716 fixed within the substrate/waveguide range. This configuration provides more flexibility in the propagation of light in terms of angle selection.
1077A-4732AA-PF 36 丄叫505 光束1702入射於法布里—派洛17〇4上,當反射剩餘光 束I?09時,使既定頻率的光1708通過。穿透的頻率入射 反射超結肖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171G上。鏡面Π10適當傾斜,使得光 相對於基底以垂直角度導引朝向抗反射链膜1712,接著通 進入外°卩"面。此裝置整體而言當作波長選擇濾波器 使用。 〜 • $結構刊料多技術製H包括對厚板大 量微機械形成精密深度的空穴,例如基底之厚度且至少數 百微米。完成空穴钱刻之後製造傾斜的鏡面並且整個組 件黏合於基底,例如玻璃,利用許多矽/玻璃黏合技術當中 第1 7B圖係更多的詳盡的變化。於此範例中,已經 用-第二可調制遽波器1 739以便提供額外的頻率選擇通1077A-4732AA-PF 36 Howling 505 Beam 1702 is incident on Fabry-Pylo 17〇4, and when the remaining beam I?09 is reflected, light 1708 of a given frequency is passed. The transmitted frequency is incident on and reflected from the super-junction 1706 and then reflected by the mirror 1716 onto the inclined mirror 171G. The mirror Π 10 is suitably tilted such that light is directed at a vertical angle relative to the substrate toward the anti-reflective chain film 1712 and then into the outer surface. This device is used as a wavelength selective filter as a whole. ~ • $Structural Multi-Tech H includes the formation of precise depths of holes for a large number of micromachines, such as the thickness of the substrate and at least several hundred microns. After completing the hole engraving, the slanted mirror is fabricated and the entire assembly is bonded to the substrate, such as glass, using a number of 矽/glass bonding techniques in which the more detailed changes are made in Figure 17B. In this example, the second modulatable chopper 1 739 has been used to provide additional frequency selective
道。換句話說’兩個分開的頻率現在可個別的選擇。亦加 入感測器1 738,並提供高度功能整合。 入其麻咖 工不已經耦合進 入基底1 7 7 0内’並且入射可 町J满制濾波态1 752上。此凃.士 器不同於第17Α圖及第j 7R _ ^ ^ 匕濾波 闽夂第1 7B ®,其中它包括於可 器鏡面之表面上製造的爯刼人# 移動濾波 藉由濾波器1 752選擇的噸i 角度使侍 角度直接耦合入基底t。包含 粟式Μ垂直 匕δ於先束175〇内的 播直到其照射傾斜的再耦人Ρ 餘頻率傳 的再耦。鏡面1 760,其呈 光束1 756之表面。因此弁击生直於仃進 此先束再追溯原來路徑離開裝置,至Road. In other words, 'two separate frequencies are now individually selectable. Sensor 1 738 is also added and provides a high degree of functional integration. The mascots have not been coupled into the base 1 7 7 ' and are incident on the 1 752 filter state. This coating is different from the 17th and 7th 7th _ ^ ^ 匕 filter 闽夂 1 7B ® , which includes the 爯刼 制造 制造 # # # # # # # # # # # # # # # # # # # # # # # # # # # # The selected ton i angle directly couples the wait angle into the base t. It includes the recoupling of the re-coupling frequency of the Μ 于 vertical 匕 δ in the first 175 直到 until the illumination is tilted. Mirror 1 760, which is the surface of beam 1 756. Therefore, the sniper is born straight ahead of this, and then traces the original path away from the device, to
1077A-4732AA-PF 37 ^43505 光學連接的其他裝置而使用。光束1 758入射於可檢測及解 譯此光束内之資訊的IC1 764上。此IC可為FPGA樣式,或 具有積體電路之其它矽、矽/鍺或砷化鎵裝置,其具有直接 耦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控1 772功能,形成於iCsl764& 1762 之間。此藉由鏡面1 766與再耦合鏡面1 768之結合體形成。 假若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,藉由任一 ICs發射光。藉由任何光學感 應兀件,並根據用以製造1C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,暴露於基底行進光東而調制入射I c上的 光。 使用基底波導的光學混和器 ^第18A圖與第18B圖係說明具有使用基底/波導之τα 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。&含多種;皮長的《具有兩種肖定的〉皮& Μ。及 1 803,被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—光學停止器 第⑽圖揭露另一種結構。此輸入光藉由 刪、抗反射链膜麗被導引入裝置,並且利用再Μ鏡 面1806耦合進入基底。此再耦合鏡面引導光 波器,劃分出頻讀光束竭並且未被 率引導朝向第二可調㈣波器·,其割=的頻 」刀出頰率;I 2(光1077A-4732AA-PF 37 ^43505 Use with other devices for optical connection. Beam 1 758 is incident on IC1 764 which can detect and interpret information within the beam. This IC can be an FPGA style, or other 矽, 矽/锗 or gallium arsenide device with integrated circuitry that has the benefit of directly coupling light carrying data. For example, a high frequency wide optical interconnect can be formed between iCsl764 & 1762 by a two-way optical path control 1772 function. This is formed by a combination of mirror 1 766 and re-coupling mirror 1 768. If there are elements such as vertical hole surface emitting lasers (VCSELS) or light emitting diode LEDs, light is emitted by either ICs. Light is detected by any optical sensing element and according to the characteristics of the element fabricated by the semiconductor technology used to manufacture 1C. The light incident on the ic can also modulate the light incident on Ic by exposure to the substrate traveling light by an interferometric modulator already fabricated on the surface of Ic. Optical Mixer Using Substrate Waveguides Figures 18A and 18B illustrate a two-channel optical mixer having a τα variation using a substrate/waveguide. Figure 18A shows a schematic diagram of the device. & contains a variety; leather long "with two stereotypes" skin & Μ. And 1 803, divided and directed toward two independent variable attenuators "Μ. Then, they are output to a number of possible channels 18〇7 or enter-optical stop. Figure 10 (10) reveals another structure. This input light The device is guided into the substrate by the occlusion, anti-reflection chain, and coupled into the substrate by means of a re-mirror mirror 1806. This re-coupling mirror guides the optical wave, dividing the frequency reading beam and not guiding the direction toward the second adjustable (four) Wave, · its cutting = frequency" knife cheek rate; I 2 (light
1077A-4732AA-PF 38 1343505 束1 81 7),剩餘頻率的光束! 8丨9進一步經由τ丨R行進。沿 著藉由可調制濾波器1808傳輸的光束1815之路徑,此光 再··人經由鏡面1810反射通過一抗反射鍍膜而被導引回基 底/波導,並且再耦合入基底。再耦合鏡面1811導引光束 1817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1816之功能而位置移動。 此結構如同再耦合鏡面,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,當其入射解耦合 切換器1820及1824陣列。此等當做選擇性地引導引導光 束進入兩個光結合器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,利用反應性離子蝕刻其頂部形成一透 鏡。吸收器/感測器包括固定於基底上的一半導體元件,提 供當作混合益的輸出功率量測。光學超結構丨829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’提供一種容易 製造的、設定的以及耗合至外部的光學元件因為裝置存 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1077A-4732AA-PF 38 1343505 Beam 1 81 7), beam of residual frequency! 8丨9 further travels via τ丨R. Along the path of the beam 1815 transmitted by the modulatable filter 1808, the light is reflected back through the mirror 1810 through an anti-reflective coating to the substrate/waveguide and recoupled into the substrate. The re-coupling mirror 1811 directs the beam 1817 toward the attenuator 1812 and then continues along the path parallel to the beam 1817 to continue selection by the second modulatable filter 18〇9. The two beams are moved in position by the function of the beam position changer 1816. This structure acts as a recoupling mirror, producing 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, as they are incident decoupled from the array of switches 1820 and 1824. These are optionally directed to direct the light beam into one of the two optical combiners 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, and a top mirror is formed by reactive ion etching. The absorber/sensor includes a semiconductor component mounted to the substrate to provide an output power measurement as a benefit. The optical superstructure 829 supports the external optical components and provides a hermetic package for the mixer. The combination of this planar interferometric modulator and the substrate waveguide provides an optical component that is easy to manufacture, set, and external to the external because the device is present on the waveguide and/or superstructure and can be used in the waveguide and in the waveguide and super The role of light propagating between structures. Because all the components are in a flat manner
1077A-4732AA-PF 39 »Φ3505 製造’藉由於大面積上大量製造可達到相當經濟效益,並 且不同部分可輕易且精準地對其與固定。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 動。活動電子元件可固定於超結構或基底/波導兩者之一, 以便増加功能。或者,活動元件可製造成超結構之一部份, 特別假若其係一半導體,例如矽或砷化鎵。 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 半導體電子特性,干涉調制器,如同許多微機電結構,可 採用I 技術之優點,像是類似於印刷工業。此類的方法 一般包括彈性的且紙張或塑膠之連續平板樣式的、、基底夕。 參考網印饋入方法’其一般包括一基底材料的連續滾筒, 基底材料饋入一連串工具,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。 第1 9圖係用以說明一連串應用於單一干涉調制器製 ,並且藉由此延伸而製造干涉調制器陣列或其它微機電 結構。網印來源19〇〇係基底材料,例如透明塑膠的滚筒。 來自/袞筒#塊材料上的表示區域包括,為了說明,只有 單裝置。/予雕圖案工具1 904於塑膠板内壓印出—凹陷 圖案。可藉由具有姓刻带屮± ^成於表面上的適當突出圓案的一 金屬磁帶而完成。 金屬磁帶係固定於一辛结 、/衰简,利用充份的壓力壓印薄1077A-4732AA-PF 39 »Φ3505 Manufacturing' is economically efficient thanks to large-scale manufacturing on a large scale, and different parts can be easily and accurately fixed and fixed. 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. The active electronic component can be attached to either the superstructure or the substrate/waveguide for added functionality. Alternatively, the moving element can be fabricated as part of a superstructure, especially if it is a semiconductor such as germanium or gallium arsenide. Print manufacturing methods Because they are planar' and because many layers do not have the semiconductor electronic properties that require special substrates, interferometric modulators, like many microelectromechanical structures, can take advantage of I technology, like the printing industry. Such methods generally include a flexible, continuous sheet-like pattern of paper or plastic. The reference screen printing method </ RTI> generally comprises a continuous roll of substrate material fed into a series of tools, each selectively coated with a dye to continuously produce a color pattern image. This step is important because it can be manufactured at high speed. Figure 19 is intended to illustrate a series of applications to a single interferometric modulator and by virtue of this extension to fabricate an interferometric modulator array or other microelectromechanical structure. Screen printing source 19 基底 base material, such as a transparent plastic roller. The representation area from the block material includes, for illustration, only a single device. / Pre-engraving tool 1 904 is stamped in a plastic plate - a recessed pattern. This can be done by a metal tape having a suitable protruding case with a surname 刻 ± ^ formed on the surface. The metal tape is fixed to a sinusoidal knot, / simplification, and is embossed with sufficient pressure.
1077A-4732AA-PF 40 1343505 板’使塑勝變形而形成凹陷圖案。 』圖式1906已說明之。鋰 膜Is 1 9 0 8利用已知薄膜沉積方法 薄u u屏 ^ 彳如濺鍍或蒸鍍,沉積 4材枓層。結果為包括氧化物、 ^ L 〇 复屬、氧化物及一犧牲薄 膜的四層溥膜的堆疊1910。這些材钮 ^ ,,, ^ ^ τ科相當於感應吸收干涉 調制Is s又计。一裝置丨9丨2分配、 固化且對於光阻曝光,以 便對於這些層形成圖案。只要 战了圖案,於裝置〗914中 貫施薄膜蝕刻。或者,利用已知 射熔融方法完成圖案。 於此蛇例中,於整個材料上掃摇 7由射,允許隨者基底移 動而同時進灯。雷射的頻率與功率足夠可以汽化需要的材 科至大小為微米等級。調整雷射的頻帛,如此只有和基底 上的材料作用,並沒有和美麻〜 ' 男和基底本身作用。因為汽化太快, 基底輕微地受熱。 於此裝置範例中,所古认w ^ 斤有的濤膜利用相同的圖案而蝕 刻。如1 91 8所示,應用奘罟]Q丨β 浐置1 9 1 6使光阻被剝離。裝置丨92〇 係另一種沉積裝置,其沉藉腺士氣工a 丹,儿積將成為干涉調制器之結構層。 關於此層1 9 2 2可使用铉。u_ u M a 便用叙。此材料亦可包括有機材料,顯示 ’、有極微J的應力,並且可利用各種pvD及Μ㈣技術沉 積。此層分別利用裝置1 924、1 926與咖,大體被曝光 成既定圖案m剝離光阻。裝置193G係用來將犧牲層 姓刻移除。假若此層為石夕,關於此目的則可利用氣體相位 姓刻劑,而完成。結果為自我支撐薄膜結構1 932形 成此干涉調制器。 封裝此疋成裝置係藉由固定彈性薄板1 933於基底薄 板之上表面。此亦可藉由連續滾筒i 936提供其已利用鍍1077A-4732AA-PF 40 1343505 The plate 'deforms the plastic to form a concave pattern. Figure 1906 has been described. The lithium film Is 1 9 0 8 is deposited by a known thin film deposition method, such as sputtering or evaporation, to deposit a 4-layer layer. The result is a stack 1910 of four ruthenium films comprising oxide, ^ L 〇 complex, oxide and a sacrificial film. These material buttons ^ , , , ^ ^ τ are equivalent to the inductive absorption interference modulation Is s. A device 分配9丨2 is dispensed, cured and exposed to photoresist to pattern these layers. As long as the pattern is combated, a thin film etch is applied in device 914. Alternatively, the pattern is completed using a known shot melting method. In this case, the 7-shot is swept across the material, allowing the substrate to move while entering the lamp. The frequency and power of the laser is sufficient to vaporize the required material to a micron size. Adjusting the frequency of the laser, so only with the material on the substrate, does not work with the melon ~ 'male and the substrate itself. Because the vaporization is too fast, the substrate is slightly heated. In the example of this device, the Tao film that has been recognized by the ancients is etched using the same pattern. As shown in 1 91, the photoresist is stripped by applying 奘罟]Q丨β to 1 916. The device 丨92 is another deposition device that sinks the gazette gas, and the product will become the structural layer of the interferometric modulator. About this layer 1 9 2 2 can be used. U_ u M a will be used. This material can also include organic materials that exhibit ', have very slight J stress, and can be deposited using a variety of pvD and Μ (4) techniques. This layer is exposed to a predetermined pattern m stripping photoresist by means of devices 1 924, 1 926 and coffee, respectively. Device 193G is used to remove the sacrificial layer surname. If this layer is Shi Xi, this purpose can be accomplished by using the gas phase surname. The result is that the self-supporting film structure 1 932 forms this interferometric modulator. The encapsulation device is packaged by securing the elastic sheet 1 933 to the upper surface of the substrate sheet. This can also be provided by continuous roller i 936.
1077A-4732AA-PF ^43505 膜裝置1 934鍍上密封的薄膜,例如金屬β兩薄板利用固定 裝置1937結合,以便完成封裝元件194〇。 應力量測 殘餘應力係設計與製造微機電結構之一因专。 ^ 於干涉 調制器及其它結構中,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 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熊的 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m圖與第20Β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 器2000與2002。分別為雙懸臂樑及單懸臂樑形式。於此 乾例中’結構材料不具有殘餘應力,並且兩構件顯示不具 有形變° #自底部透視基底,此裝置顯示均句的色彩,其 藉由形成於其上的間隔層厚度決^。干涉調制H 2_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2〇16為綠色,而色1077A-4732AA-PF ^43505 Membrane device 1 934 is plated with a sealed film, such as a metal beta, which is bonded by a fixture 1937 to complete the packaged component 194. The force should be measured by the residual stress system to design and manufacture one of the micro-electromechanical structures. In interferometric modulators and other structures in which the structural members have been mechanically loosened during the manufacturing process, the residual stress determines the geometry of the members. 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 cavity 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 deformed bears. Therefore, the interferometric modulator can provide a means for this estimation. "" Figure m and Figure 20 show examples of how an interferometric modulator can be applied to this method. Interferometric modulators 2000 and 2002 are shown from the side and bottom (perspective substrate), respectively. They are in the form of double cantilever beams and single cantilever beams. In this example, the structural material does not have residual stress, and the two members show no deformation. From the bottom perspective substrate, the device displays the color of the uniform sentence, which is determined by the thickness of the spacer layer formed thereon. The interferometric modulations H 2_ and 2006 show a stress gradient 'because there is more compressive force than above. 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 2〇16 is green, and the color
1077A-4732AA-PF 42 1343505 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 底。干涉調制器2008及2010顯示處於一狀態,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 形’且改變彩色區域。於此範例中,當區域2〇22為藍色時, 區域2020為紅色。1077A-4732AA-PF 42 1343505 The color area 2014 is blue because it is close to the base. Conversely, when the color area 2018 (the display is located in the double cantilever beam) is red, this is because it is far from the base. Interferometric modulators 2008 and 2010 are shown in a state in which the stress gradient of higher tensile stress is shown above. The structural member is suitably deformed' and the colored area is changed. In this example, when region 2〇22 is blue, region 2020 is red.
於第20B圖中,顯示一系統,其可用以快速地且精確 地估算沉積薄膜之殘餘應力狀態。晶圓2〇3〇包括干涉調制 器結構陣列,其包括可變化長度與寬度的單一懸臂樑薄膜 及雙懸臂樑薄膜。結構薄膜係選自機械及殘留應力已詳細 拖述的材料製造。許多材料皆可以,然受限於反射條件的 材料便相當少,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、鋁鍺),In Fig. 20B, a system is shown which can be used to quickly and accurately estimate the residual stress state of the deposited film. The wafer 2〇3〇 includes an array of interferometric modulator structures including a single cantilever beam film and a double cantilever film of variable length and width. The structural film is selected from materials that have been detailed in mechanical and residual stresses. Many materials are possible, but the material limited by the reflection conditions is quite small. The interferometric modulator in this example is not used for display purposes. Good alternative materials can include materials in the form of crystals (矽, aluminum 锗),
從製造觀點目容的’顯示某種程度的反射並且其機械特 性之特徵為具有尚度精確性^製造且釋放此種、、測試結 構’因此其係獨立運作的。假若材料沒有應力,那麼結 構將顯示沒有色彩變化。然而,”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2〇34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2036連接,於其上存在硬體 ,且^記錄與處理影像資料。此硬體簡易地包括容易獲 V的门速處理;便於高速率執行數值計算。軟體可包 括收集顏色資訊且計 序將利用變形資料, 算表面變形的大量例行程序。核心程 決定橫跨薄膜厚度的均勻應力與應力From the point of view of manufacturing, the 'shows a certain degree of reflection and its mechanical characteristics are characterized by a degree of precision that is manufactured and released, and the test structure' thus operates independently. If the material is not stressed, the structure will show no color change. However, "not so, the color state or color image can be recorded by using the high-resolution camera device 2, 34, and a high-magnification image can be obtained via the optical system. This camera device is connected to the computer system 2036. There is hardware on it, and ^ record and process image data. This hardware simply includes the door speed processing that is easy to obtain V; it is convenient to perform numerical calculation at a high rate. The software can include collecting color information and the order will use the deformation data to calculate the surface. A large number of routines for deformation. The core process determines the uniform stress and stress across the thickness of the film.
1077A-4732AA-PF 43 1343505 梯度之最佳組合,可以產生所有種類。 使用的一種模式係產生一大堆、、未摻雜〃的測試晶片, 其具有未沉積應力狀態之詳細記錄,被收藏以方便使用。 虽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 期間觀察其作肖’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。適當 地改變沉積系、統’產生—光路徑使得影像系統可即時觀察 結構及追縱色彩影像之變化。這形成一即時回饋系統用 以控制沉積參數,以便以此方法控制殘餘應力。軟體與硬 體可參考測試晶片的週期,並且當成長薄膜時,允許沉 裝置操控器改變條件。關於量測殘餘應力,敕;積 王调糸蛛優於 其它技術’不論是只有依賴電子機械啟動,或卜 且複雜的干涉系統量測製造結構的變形量。^ 叩貝 驅動電子至很大的裝置陣列,以及電子 垅又提供 久电于式1剛位移之x姓 確性。後者於觀察下受限於薄膜的光學特性、 不精 雜的外部光學與硬體。 及需要複 不連續薄膜 另一種具有令人關注特性的材料係— 其結構 將其歸 為非同質的。這些薄膜可以數種型式中 、35規,並且應 1077A-4732AA-PF ΑΔ 1343505 類成不連續薄臈。第21A圖說明一種不連續薄膜。基底2100 可為一金屬、介電或半導體,其具有蝕刻至其表面的不佳 輪廊。此輪廓包括各個結構外觀且應具有一高度2丨丨〇,為 相干光波長之某些部分,係利用黃光微影及化學蝕刻技術 而被钱刻’以便獲得近似於藉由2104(三角形)、2106(圓 柱形)及2108(錐形)描述的高度。任何個別高度之基底有 效直徑亦相當於圖案高度等級。當每一輪廓稍微不同時, _ 其仍具有相同的特性,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2100。與多層 溥膜結合的鍍膜比較,此種結構當作較佳的抗反射鍍膜使 用,因為其與角度量測無關。因此,對於更大的入射角度, 其維持高度地抗反射。 第21B圖揭露一種鍍膜212〇,其已沉積於基底2122 上,並且可為一金屬、介電質或半導體。於此範例中,薄 膜已於早期階段形成,大約小於丨〇〇〇埃厚度。於大多數沉 籲積步驟期間,薄膜經歷一階段式結晶過程,形成材料的區 域逐漸長大,直到彼此結合成一體,並且於某些點形成— 連續4膜。圖21 24顯示此薄膜之上視圖。於較早階段形成 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。 第21C圖說明不連續薄膜的第三種型式。於此範例 中,溥膜2130已經於基底2132上沉積至一厚度,至少一 千埃’可將其視為連續。利用與上述自我結合方法相同的 技術’於材料中形成—、、次波長',(就是直徑小於波長)孔 1077A-4732AA-PF 45 1343505 洞圖案。於此範例中,高分子可當作將蝕刻圖案移轉至底 下材料的光罩’並且利用活性離子钱刻技術姓刻孔洞。因 為材料是連續的,但是被穿孔,並不與第21 b圖的較早階 段薄膜相同。相反地’其光學特性不同於未蝕刻薄膜,其 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。2136顯示此薄膜之上 視圖。此類的薄膜已於Tae Jin Kim的論文'c〇ntr〇1 〇f optical transmission through metals perforated with subwavelength hole arrays中說明。同時,其屬於一般 結構,不同於PBGs。 所有二種不連續薄胺άΓ庙田私工:土^„ Al ,1077A-4732AA-PF 43 1343505 The best combination of gradients can produce all kinds. One mode used is to produce a large, undoped test wafer with a detailed record of the undeposited stress state, which is conveniently stored for use. While it is desirable to determine the residual stress of the deposited film, a test wafer is selected and the film is deposited on top of it. The deposited film changes the geometry of the structure and its color image. Using software that resides 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 the film during the initiation of the newly deposited film provides more information about the residual stress state, as is the film variation characteristics throughout the startup process. This technique can be used to determine film stress when depositing a film. Appropriately changing the sedimentary system, the generation-light path allows the imaging system to instantly observe the structure and track changes in color images. This forms an instant feedback system for controlling the deposition parameters in order to control the residual stress in this way. The software and hardware can refer to the period of the test wafer, and when the film is grown, the sink device controller is allowed to change conditions. Regarding the measurement of residual stress, 敕; 王 糸 is superior to other techniques', whether it is only relying on electromechanical activation, or a complex interference system to measure the deformation of the manufacturing structure. ^ Mussels drive electrons to a large array of devices, and the electrons provide the x-positiveness of the long-term displacement of Equation 1. The latter is limited by the optical properties of the film, uncomplicated external optics and hardware. And the need for a discontinuous film. Another material with interesting properties - its structure is classified as non-homogenous. These films are available in several versions, 35 gauges, and should be classified as discontinuous thin rafts at 1077A-4732AA-PF ΑΔ 1343505. Figure 21A illustrates a discontinuous film. Substrate 2100 can be a metal, dielectric or semiconductor having a poor corridor etched to its surface. This profile includes the appearance of each structure and should have a height of 2 丨丨〇, which is part of the wavelength of the coherent light, which is etched by the use of yellow lithography and chemical etching techniques to obtain an approximation by 2104 (triangle), 2106. The height described by (cylindrical) and 2108 (tapered). The effective diameter of the substrate at any individual height is also equivalent to the height level of the pattern. When each profile is slightly different, it still has the same characteristics, such as when a beam traverses into the substrate from the entrance, the refractive index gradually changes from the incident medium to the film substrate 2100. This structure is used as a preferred anti-reflective coating as compared to a multilayer enamel film because it is independent of angular measurement. Therefore, it maintains a high degree of anti-reflection for a larger angle of incidence. Figure 21B illustrates a coating 212 that has been deposited on substrate 2122 and can be a metal, dielectric or semiconductor. In this example, the film has been formed at an early stage, approximately less than the thickness of the 丨〇〇〇. During most of the deposition steps, the film undergoes a one-stage crystallization process, and the regions forming the material gradually grow until they are integrated into one another and form a continuous film at some point. Figure 21 24 shows a top view of the film. The optical properties of the film formed 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. Figure 21C illustrates a third version of the discontinuous film. In this example, the ruthenium film 2130 has been deposited to a thickness on the substrate 2132, which may be considered continuous as at least one thousand angstroms. The hole 1077A-4732AA-PF 45 1343505 hole pattern is formed in the material by the same technique as the self-binding method described above. In this example, the polymer can be used as a reticle that shifts the etched pattern to the underlying material and utilizes the active ion engraving technique to name the hole. Since the material is continuous but perforated, it is not the same as the earlier stage film of Figure 21b. Conversely, its optical properties are different from those of an unetched film, where the incident beam experiences less loss and exhibits a peak of penetration depending on the surface. In addition, the geometry of the hole, like the angle of incidence and the refractive index of the incident interface, manipulates the spectral properties of the transmitted light. 2136 shows the top view of this film. Such films have been described in Tae Jin Kim's paper 'c〇ntr〇1 〇f optical transmission through metals perforated with subwavelength hole arrays. At the same time, it is a general structure, unlike PBGs. All two kinds of discontinuous thin amines, Miao Tian private workers: soil ^„ Al,
1077Λ-47 32AA-PF 露如上’然其並非用以 ,在不脫離本發明之精 46 备.,圍内*可作更動與潤飾,因此本發明之保護範圍 田視後附之中請專利範s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 处堪〜^的輔助光;第1B圖揭露另一種關於輔助光的 、,口 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4A圖係一圖式,盆班诚νκ . ,^ ^ 式根據基底+顏料"觀念說明彩 巴..肩不器的結構;第4 R圄掘咖 么 ,A ¥ 4B圖揭路一系統的方塊圖式,其提# 底色可重新分配顯 捉供 於-般用途的顯示二第C圖說明上述觀念應用 示自:干涉調制器幾何圖式’於未啟動狀態中顯 丁自微機電運作中減少光學作 器於啟動狀態;第5C圖關顯不干涉調制 於里斑白的狀“ ’、®式,顯不此干涉調制器設計 狀:的::…運作;…係一圖式,顯示許多色彩 第示干涉調制器的圖式,相同 中減少光學作用,不過支樓結構„藏;㈣圖== 同的設計處於啟動狀態; 4^49 第U圖說明使用非等向性 於一狀皞中.笙馎仟的干涉调制器處 、", 圖顯示相同的干涉調制器處於另—狀離1077Λ-47 32AA-PF is exposed as above. However, it is not used. It can be used for modification and retouching without departing from the essence of the present invention. Therefore, the scope of protection of the present invention is attached to the patent field. The one defined by s shall prevail. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1A is a cross-sectional view of a display substrate having auxiliary light for anti-reflection plating; FIG. 1B discloses another configuration for auxiliary light; FIG. 2 is a detailed view The manufacturing process of the micro-mechanical arc lamp source; Figure 3 illustrates the driving structure of the bias center of the interferometric modulator array in the display; Figure 4A is a figure, the Banban Cheng νκ . , ^ ^ type according to the base + pigment " The concept illustrates the structure of the color bar.. Should not be the structure of the shoulder; the 4th R 圄 咖 么 , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , Figure 2 shows the application of the above concept. The interferometric modulator geometry diagram reduces the optical actuator in the startup state in the unactivated state. The 5C diagram shows the non-interference modulation in the white spot. “ ',®, does not interfere with the design of the modulator: ::...Operation;... is a diagram showing many colors showing the pattern of the interferometric modulator, which reduces the optical effect, but the structure of the branch (4) Figure == The same design is in the startup ; FIG. 4 ^ 49 U of instructions in an anisotropic shape Hao the interferometric modulator at a thousand Sheng Bo, ", the same figure shows the interferometric modulator is in another - from the shape.
1077A-4732AA-PF 47 T343505 中; 第8A圖說明干涉調制器,i藉 '、稭由靛轉啟動;第8B圖 揭露旋轉式干涉調制器設計的製造流程; 第9A圖係一微機電開關的方塊圖式;第9B圖係根據 微機電開關的列驅動器的方塊圖式;第9c圖係根據微機電 開關的行驅動器的方塊圖式;第⑽圏係根據微機電開關的 麵問之方塊圖式;第9£圖係顯示具有利用邏輯與驅動 器元件之微機電的顯示系統的方塊圖式; 第10A圖係一圖式,其揭露 询路微機電開關的結構、製 造與操作;第1 OB、1 〇ς圖% Μ β啕樘可選擇的開關設計; 第11Α圖係一圖式,其顯示依據2_d光電結構的微型 範例;第11B圖係週期性的2咄光電結構的圖式; 第12圖係一圖式,jl据+ 0 圃式其揭路一3-D光電結構的範例; 第1 3A圖係一圖式,宜^ ,、"兄月處於未啟動狀態具有微型 結構的干涉調制器;第nR阁 圖係相同的干涉調制器處於啟 動狀態;第1 3C圖係s目干呈古.田《 糸員不具有週期性& 2-D光電結構的干 涉調制器; 第14A圖係說明干涉調制器設計,其當作一光學開關 使用;第14β圖係顯示此種設計的各種變化,當作—光學 衰減器使用; 干 第1 5 Α圖係一千味^因生丨 干ν凋制态设計的圖式,其功能為— 學開關或一光學退無哭.笛 口 ,第15 Β圖說明此等干涉調制器 如何結合而當作-刚光學開關使用; 〇 第1 6圖顯不可胡法丨不,半 。周制干涉調制器結構的製造流程; 1077A-4732AA-PF· A8 1343505 第1 7A圖說明可調制干涉調制器結構如何可鹿 長選擇開關;第ΠΒ圖進—步說明波長選擇開關:付可: 用於固態元件4 m圖說明凸塊連結元件如何積體化;〜 第18A圖係一兩通道等化器/混合器的概要圖式;第 18B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’其說明一連續的 網狀基礎的製造流 程; 第20A、20B圖說明干涉調制器測試結構如何使用於應 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; 1 02〜玻璃層; 104-弧光燈陣列; 106〜玻璃基底; 1 0 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; 1 2 2〜光線; 1 2 6〜薄膜堆積; 128〜觀察者; 200〜玻璃層; 20卜反射器碗狀物; 202〜犧牲層; 204~反射器/複金屬層 2 0 5〜光線; 206~沉積電極層; 1077A-4732AA-PF 49 1743505 300〜磁滯曲線; 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; 5 2 7 ~綠色峰值; 606〜干涉調制器; 702~鋁薄膜; 706〜入射光; 710〜平板; 718〜薄材料層; 8 0 2〜電極; 808〜支撐棒; 812〜支撐遮光器; 816〜支撐結構;1077A-4732AA-PF 47 T343505; Figure 8A illustrates the interferometric modulator, i borrowed ', straw turned from 靛 turn; 8B shows the manufacturing flow of the rotary interferometric modulator design; Figure 9A shows a microelectromechanical switch Block diagram; Fig. 9B is a block diagram of a column driver according to a microelectromechanical switch; Fig. 9c is a block diagram of a row driver according to a microelectromechanical switch; and (10) is a block diagram according to a face of a microelectromechanical switch Figure 9 shows a block diagram of a display system with MEMS utilizing logic and driver components; Figure 10A is a diagram that discloses the structure, fabrication, and operation of an interrogation MEMS switch; 1 〇ς % 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 ; ; ; ; ; ; ; ; 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘 啕樘12 is a picture, jl according to + 0 其 其 揭 揭 一 3- 3- 3- 3- 3- 3- 3- 3- 3- ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; Interferometric modulator; the same interference modulation of the nRth map The device is in a startup state; the 1st 3C system is the same as the interferometric modulator of the periodicity & 2-D photoelectric structure; the 14A is a description of the interferometric modulator design, which is regarded as a The optical switch is used; the 14th figure shows various changes of this design, and is used as an optical attenuator; the dry 15th 系 is a pattern of one thousand flavors, which is designed by the dry ν 制The function is - learning switch or an optical retreat without crying. The mouthpiece, the 15th figure shows how these interferometric modulators are combined and used as a --------------------------------------- Manufacturing process of the peripheral interferometric modulator structure; 1077A-4732AA-PF· A8 1343505 Figure 1 7A illustrates how the modulatable interferometric modulator structure can be selected as a deer length switch; the second figure shows the wavelength selection switch: 4 m for the solid-state component shows how the bump-bonding element is integrated; ~ Figure 18A is a schematic diagram of a two-channel equalizer/mixer; Figure 18B shows how the equalizer/mixer uses interference Modulator; Fig. 19 is a diagram illustrating the manufacturing flow of a continuous mesh base; Figs. 20A, 20B illustrate how the interferometric modulator test structure is used for stress measurement; and 21A to 21C description. [Main component symbol description] 100~AR coating; 1 02~glass layer; 104-arc array; 106~glass substrate; 1 0 7~interface; 108~interferometric modulator array; 109~ incident light; 11 0~ light Path; 111~reflector layer; 112~substrate; 114~interferometric modulator array; 116~light source; 118~ light guide; 120~collimator; 1 2 2~ light; 1 2 6~film stack; 128~observer 200~glass layer; 20b reflector bowl; 202~ sacrificial layer; 204~ reflector/composite metal layer 2 0 5~ light; 206~ deposited electrode layer; 1077A-4732AA-PF 49 1743505 300~ hysteresis Curve; 400~pixel; 404~green; 408~white; 412~ executive controller; 418~ portable electronic product 422~memory; 426~ handwriting input; 432~audio interface; 5 0 2~electrode rod; ~ optical hole; 508 ~ second mirror; 511 ~ predetermined frequency light; 521 ~ black state; 5 2 7 ~ green peak; 606 ~ interferometric modulator; 702 ~ aluminum film; 706 ~ incident light; 710 ~ plate; ~ thin material layer; 8 0 2 ~ electrode; 808 ~ support rod ; 812 ~ support shutter; 816 ~ support structure;
1077A-4732AA-PF 302〜時間圖; 4 0 2〜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; 500~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; 5 2 9〜紅色峰值; 608〜薄膜/鏡面; 7 〇 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; 814~輔助電極; 81 8 ~遮光器; 50 1343505 820〜觀察者; 830〜基底; 832、834、836〜犧牲隔間; 838〜柱子/旋轉樞紐/遮光器材料;1077A-4732AA-PF 302~time diagram; 4 0 2~red; 406~blue; 410~ component; 414, 416~ drive electronic circuit; 420~ core processor; 424~RF or IR interface; 430~ image Input device; 500~ substrate; 504~ insulating film; 506~ film/mirror; 510~transparent upper structure; 512~observer; 525~blue peak; 5 2 9~red peak; 608~film/mirror; 7 〇 4 ~ stacked layer; 708 ~ part of the frequency of light; 716 ~ support adjustment piece; 8 0 0 ~ substrate; 804 ~ common bus electrode; 81 0 ~ rotating hub; 814 ~ auxiliary electrode; 81 8 ~ shutter 50 1343505 820 ~ observer; 830 ~ substrate; 832, 834, 836 ~ sacrificial compartment; 838 ~ pillar / rotating hub / shutter material;
840〜支撐柱; 844〜匯流排電極; 848〜支撐柱; 852〜遮光器; 902〜控制信號; 906〜輸入電壓Vc〇n ; 91 0〜輸入電壓Vb,as : 91 6〜輸入電壓VselFO ; 920〜輸出端; 926〜控制邏輯; 9 3 0〜顯示陣列; 934 、 936 、 938 、 940 1 000〜基底; 1 004〜箭號; 1 008〜汲極結構: 1 012 ~凹槽; 10 24〜汲極; 842〜遮光器; 846〜遮光反射器 8 5 0 ~扭力臂; 900〜輸入端; 9〇4~輪出端; 908〜輸入電壓ve〇i〇 ; 91 4〜輸入電壓vsem ; 91 8 ~接地; 924〜行驅動器; 9 2 8〜列驅動器; 932〜邏輯裝置; 基礎切換方塊; 1 0 0 2〜犧牲間隔; 1 0 0 6〜閘極結構; 1010〜源極桿; 1 〇 16〜箭號: 1026〜源極; 1 0 2 8 ~切換桿; 1 〇 4 0〜絕緣器: 1100〜基底; 1102〜微環狀共振器;840 ~ support column; 844 ~ bus bar electrode; 848 ~ support column; 852 ~ shutter; 902 ~ control signal; 906 ~ input voltage Vc 〇 n; 91 0 ~ input voltage Vb, as: 91 6 ~ input voltage VselFO; 920~output; 926~ control logic; 9 3 0~ display array; 934, 936, 938, 940 1 000~ base; 1 004~arrow; 1 008~汲 structure: 1 012 ~ groove; 10 24 ~ bungee; 842 ~ shutter; 846 ~ shading reflector 8 5 0 ~ torque arm; 900 ~ input; 9 〇 4 ~ wheel end; 908 ~ input voltage ve〇i〇; 91 4 ~ input voltage vsem; 91 8 ~ grounding; 924~ row driver; 9 2 8~ column driver; 932~ logic device; basic switching block; 1 0 0 2~ sacrificial interval; 1 0 0 6~ gate structure; 1010~source pole; 〇16~arrow: 1026~source; 1 0 2 8 ~ switching lever; 1 〇4 0~ insulator: 1100~ base; 1102~ micro ring resonator;
1077A-4732AA-PF 1 038〜接觸桿; I 0 4 2〜切換桿; 1101、1103〜XYZ 座標; II 0 6〜陣列; 1343505 1108〜缺陷; 1 200〜基底; 1 202〜三維週期結構; 1 204〜缺陷; 1301~波導; 1 302~波導; 1 3 0 3 ~基底; 1 304〜薄膜; 1 3 0 5〜剖面圖; 1 306〜微環狀共振器; 1 3 0 8〜光束; 1310〜輸出光束; 1311〜圓柱; 1 31 2〜有限的垂直空氣間隔; 1314〜共振器; 1315〜薄膜; 1326、1 328〜未干涉的光; 1329〜光; 1 330、1 332〜波導; 1400〜鋁薄膜; 1 402〜材料堆積層; 1 406〜干涉調制器; 1 408~光束; 141 0〜側視圖; 1 4 1 4 ~側視圖; 1420〜薄膜; 1428~箭號; 1429〜反射區域; 1430〜光束; 1431〜重疊蹤跡; 1432〜光束; 1434〜側視圖; 1 436〜側視圖; 1 437〜反射區域; 1 438〜完全吸收狀態; 1 440〜反射光束; 1 5 00〜支撐結構; 1501〜透明光學支座; 1502〜鏡面; 1 503〜導體; 1 504〜基底; 1 5 0 5〜窗; 1 506〜切換器; 1 51 0 ~光束; 1512〜側視圖; 1514〜側視圖; 1520〜光纖耦合器; 1077A-4732AA-PF 52 1343505 1 522〜光束; 1 526〜側視圖; 1528〜再麵合鏡面; 1530~光束; 1531〜方向性切換器陣列; 1532〜輸出光纖耦合器; 1 536〜線性陣列; 1 535〜基底; 1 602〜導電接觸墊; 1 606〜犧牲層; 1610〜絕緣層; 1614〜薄膜堆積; 1 61 6〜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; 1 750〜光束; 1756〜再搞合鏡面; 1760〜再麵合鏡面; 1764~ICs ; 1768~再輕合鏡面; 1 772〜雙方向光路徑; 180卜光; 1 803〜光; 1 604〜鏡面; 1 6 0 8〜鏡面; 1612〜第二接觸墊; 1615〜支撐物; 161 8〜薄膜堆積; 1 704〜可調制濾波器; 1 708〜光; 1 71 0 ~鏡面; 1714〜基底; 1717〜鏡面; 1 739〜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~光纖麵合器; 1 802〜抗反射鍍膜; 1 805〜可變衰減器; 1077A-4732AA-PF 53 T343505 1 806〜再耦合鏡面; 1 808~可調制濾波器; 1810〜鏡面; 1812〜衰減器; 1815〜光束; 1817〜光束; 1 81 9〜光束; 1 824〜解耦合切換器; 1 829〜光學超結構; 1 900 ~網印來源; 1 906〜圖式; 1 91 0〜薄膜的堆疊; 1914〜裝置; 1918〜圖式; 1 922〜干涉調制器之結 1 924〜裝置; 1 928〜裝置; 1 932〜自我支撐薄膜結 1 933〜彈性薄板; 1 936〜連續滾筒; 2000〜干涉調制器; 2004〜干涉調制器; 2008〜干涉調制器; 2014~色彩區域;1077A-4732AA-PF 1 038~contact rod; I 0 4 2~switching rod; 1101, 1103~XYZ coordinates; II 0 6~ array; 1343505 1108~ defect; 1 200~ substrate; 1 202~3D periodic structure; 204~defect; 1301~waveguide; 1 302~waveguide; 1 3 0 3 ~substrate; 1 304~film; 1 3 0 5~profile; 1 306~microring resonator; 1 3 0 8~beam; 1310 ~ output beam; 1311 ~ cylinder; 1 31 2 ~ limited vertical air gap; 1314 ~ resonator; 1315 ~ film; 1326, 1 328 ~ uninterfered light; 1329 ~ light; 1 330, 1 332 ~ waveguide; ~ aluminum film; 1 402 ~ material stack; 1 406 ~ interferometric modulator; 1 408 ~ beam; 141 0 ~ side view; 1 4 1 4 ~ side view; 1420 ~ film; 1428 ~ arrow; 1429 ~ reflection area ; 1430 ~ beam; 1431 ~ overlap trace; 1432 ~ beam; 1434 ~ side view; 1 436 ~ side view; 1 437 ~ reflection area; 1 438 ~ fully absorbed state; 1 440 ~ reflected beam; 1 5 00 ~ support structure 1501~transparent optical support; 1502~mirror; 1 503~conductor 1 504~substrate; 1 5 0 5~window; 1 506~switcher; 1 51 0 ~beam; 1512~side view; 1514~side view; 1520~fiber coupler; 1077A-4732AA-PF 52 1343505 1 522~ Beam; 1 526~side view; 1528~reface mirror; 1530~beam; 1531~directional switcher array; 1532~output fiber coupler; 1 536~ linear array; 1 535~ substrate; 1 602~ conductive contact Pad; 1 606~ sacrificial layer; 1610~ insulating layer; 1614~ film stacking; 1 61 6~ center hole; 1 702~ beam; 1 706~ optical superstructure; 1 709-beam; 1712~ anti-reflective coating; Mirror surface; 1 738~ sensor; 1 750~ beam; 1756~ re-mirror; 1760~ re-surface mirror; 1764~ICs; 1768~ re-light mirror; 1 772~ bidirectional light path; ; 1 803 ~ light; 1 604 ~ mirror; 1 6 0 8 ~ mirror; 1612 ~ second contact pad; 1615 ~ support; 161 8 ~ film stack; 1 704 ~ modulate filter; 1 708 ~ light; 71 0 ~ mirror surface; 1714 ~ base; 1717 ~ mirror; 1 739 ~ second modulatable filter 1 752~ modulatable filter; 1 758~beam; 1762~ICs; 1 76 6~mirror; 1 770~ substrate; 1800~ fiber optic coupler; 1 802~ anti-reflective coating; 1 805~variable attenuator 1077A-4732AA-PF 53 T343505 1 806~ re-coupling mirror; 1 808~ modulatable filter; 1810~mirror; 1812~ attenuator; 1815~beam; 1817~beam; 1 81 9~beam; 1 824~ solution Coupling switch; 1 829~ optical superstructure; 1 900 ~ screen printing source; 1 906~ pattern; 1 91 0~ film stack; 1914~ device; 1918~ pattern; 1 922~ interferometric modulator knot 1 924~ device; 1 928~ device; 1 932~ self-supporting film junction 1 933~ elastic sheet; 1 936~ continuous roller; 2000~ interferometric modulator; 2004~ interferometric modulator; 2008~ interferometric modulator; ;
1077A-4732AA-PF 1 807~通道; 1 809~第二可調制濾波器; 1811〜再耦合鏡面; 1813~光學停止器; 1816〜光束位置改變器; 1818〜位置改變器; 1 820〜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; 1 908〜鍍膜器; 1912~裝置; 1916〜裝置; 1 920~裝置; 構層, 1 926〜裝置; 1 930〜裝置; 構; 1 934~鍍膜裝置; 1 940〜封裝元件; 2002~干涉調制器; 2006~干涉調制器; 2 01 0〜干涉調制器; 2 01 6〜色彩區域; 13435.051077A-4732AA-PF 1 807~ channel; 1 809~ second modulatable filter; 1811~recoupling mirror; 1813~ optical stop; 1816~beam position changer; 1818~position changer; 1 820~decoupling Switcher; 1 828~ optical combiner; 1 830~sensor/absorber; 1 904~embossed pattern tool; 1 908~ coater; 1912~ device; 1916~ device; 1 920~ device; 926~ device; 1 930~ device; structure; 1 934~ coating device; 1 940~ package component; 2002~ interferometric modulator; 2006~ interferometric modulator; 2 01 0~ interferometric modulator; 2 01 6~ color area; 13435.05
2018~色彩區域; 2022〜區域; 2034~攝像裝置; 2100~基底; 2106〜圓柱形; 2110〜高度; 2122〜基底; 2130~薄膜; 2136〜薄膜。 2020〜區域; 2 0 3 0〜晶圓, 2036〜電腦系統 2104〜三角形; 2108〜錐形; 2120~鏟膜; 2124〜薄膜; 2132〜基底;2018~ color area; 2022~ area; 2034~ camera unit; 2100~ substrate; 2106~cylindrical; 2110~height; 2122~ substrate; 2130~ film; 2136~ film. 2020~ area; 2 0 3 0~ wafer, 2036~ computer system 2104~ triangle; 2108~ cone; 2120~ shovel; 2124~ film; 2132~ substrate;
1077A-4732AA-PF1 551077A-4732AA-PF1 55
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