TWI301257B - Improved passive matrix electrophoretic display driving scheme - Google Patents
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1301257 玖、發明說明: 【發明所屬之技術領域】 本發明一般係關於電泳顯示器。更明確地說,本發明 係揭示一種被動矩陣電泳顯示器的改進驅動機制。 【先前技術】 電泳顯示器(EPD)係一基於懸浮在溶劑中之帶電顏料 粒子之電泳現象的非發射式裝置。最先被提出的時間在 1 969年。該顯示器通常包括兩塊具電極且位置彼此相向的 板子,兩者係以分隔體分離。該等電極中其中一者、通常係 透明的。於該等兩塊板子間封住一由一有色溶劑及複數個 帶電顏料粒子所組成之懸浮液。當於該等兩塊板子間賦加 一電壓差時,該等顏料粒子便會遷徙至其中一側,然後便 可依據該電壓差的極性看見顏料的顏色或溶劑的顏色。 有數種不同種類的EPD。於分割型EPD(參見Hopper 及 V.Novotny 於 IEEE Trans· Electr· Dev.,第 ED 26 冊, 第8號,第1148-1152頁(1979年)中所發表的文章)中,在 該等兩塊板子間會有複數個分割部,用以將該空間分割成 複數個小型的單元,以避免粒子發生不必要的移動,例如 沉澱。微囊封型EPD(如美國專利案第5,961,8〇4號及美國 專利案第53930,026號所述)實質上具有二維的微囊封排列 ’每個囊封之中皆具有一電泳組成物,其係由一介電流體 及含複數個帶電顏料粒子之懸浮液(視覺效果上與該介電溶 劑成對比)所組成。另一種類型EPD(參見美國專利案第 3,612,758號)則會具有電泳單元,其係由複數條平行直線 1301257 儲存體所構成。該等通道狀的電泳單元會被透明導體覆蓋 住並且與其產生電接觸。於該等透明導體之上則有一層透 明玻璃’吾人從透明破璃側處來觀看該面板。 於下面同在審查中的申請案中則揭示一種改進之epd 技術’本文以引用的方式將其全部併人:薦年3月3號 提出申請之關專利中請案序號第G9/5i8,488號、2〇〇1年 1月11號提出中睛之美國專利中請案序號第⑽/759,212號 2000年6月28號提出申請之美國專利申請案序號第 〇9/6〇M54號、以及_年2月15號提出申請之美國專 利申》月案序號第G9/784,972號。該改進之EpD包括封閉單 兀其係由形狀、大小及孔徑比經過良好界定之微杯狀體 所構成’ ϋ且充滿懸浮在介電溶劑中之帶電顏料粒子。 可以利用-被動矩陣系統來驅動卿。就一典型的被 動矩陣系統來說,於該顯示器之頂端(觀看表面)上具有行 電極且於該等單元之底端具有列電極(或者兩種排列方式倒 置亦可)。該等列電極及該等行電極彼此垂直1不過,就利 用-被動矩陣系統來驅動的EPD而言,有兩種相關的已知 問題:串訊及交叉偏壓。當一單元之相鄰單元的電場對該 單元中之該等粒子提供偏壓時,便會發生串訊。圖丨即為 一範例。單元A的偏壓電壓會將該等正電粒子朝該單元的 底部驅動。因為單兀B不具任何偏壓電壓,所以單元B中 的該等正電粒子原本預期應該會停留在該單元的頂端,不 過,如馬單元八與8彼此非常靠近的話,單元3的頂端電 極電壓(30V)及單元A的底部電極電壓(〇v)則會產生串訊 1301257 電場,該電場便合i白伯s Ώ丄 曰、使早7G Β中的部份粒子向下移動。放 寬相鄰單元間的距離可能便會消除此項問冑;不過,該距 離亦可能會降低該顯示器的解析度。 如果某一單亓且, 干凡具有非吊尚的臨界電壓的話,那麼便可 ㈣串^題。本發明内文中的臨界電·“義成可被施 加至單7L之最大偏屢電壓,但卻不會於該單元相反側上 的兩個電極間造成斗 成粒子移動。如果該等單元具有非常高的 臨界電壓的話,那麼便可減低串訊效應,卻又不會犧牲該 顯示器的解析度。 又 堃亦為被動矩陣顯示器熟知的一項問題。被才 力至卩電極上的電壓不僅會提供掃描列上該單元的驅童 偏壓’還會影響同_行上非掃描單S的偏壓。此非預㈣ 壓可能會迫使—非掃描單元的該等粒子遷徙至反向電極< 此非預期的粒子遷徙會造成可見的光學密度變化,並且11301257 发明, DESCRIPTION OF THE INVENTION: TECHNICAL FIELD OF THE INVENTION The present invention generally relates to electrophoretic displays. More specifically, the present invention discloses an improved driving mechanism for a passive matrix electrophoretic display. [Prior Art] An electrophoretic display (EPD) is a non-emissive device based on electrophoresis of charged pigment particles suspended in a solvent. The first time was raised in 1 969. The display typically includes two plates with electrodes and facing each other, the two being separated by a separator. One of the electrodes is typically transparent. A suspension of a colored solvent and a plurality of charged pigment particles is sealed between the two plates. When a voltage difference is applied between the two boards, the pigment particles migrate to one side, and then the color of the pigment or the color of the solvent can be seen depending on the polarity of the voltage difference. There are several different types of EPD. In the split type EPD (see article published by Hopper and V. Novotny in IEEE Trans. Electr. Dev., ed. 26, No. 8, pp. 1148-1152 (1979)), in these two There will be a plurality of divisions between the plates to divide the space into a plurality of small units to avoid unnecessary movement of particles, such as precipitation. The microencapsulated EPD (as described in U.S. Patent Nos. 5,961,8, 4 and U.S. Patent No. 5,539,026) has substantially two-dimensional microencapsulated arrays. The composition consists of a dielectric fluid and a suspension comprising a plurality of charged pigment particles (visually in contrast to the dielectric solvent). Another type of EPD (see U.S. Patent No. 3,612,758) will have an electrophoresis unit consisting of a plurality of parallel lines 1301257 storage. The channel-like electrophoretic cells are covered by and in electrical contact with the transparent conductor. Above the transparent conductors there is a layer of transparent glass, which is viewed from the side of the transparent glass. In the following application in the review, an improved epd technique is disclosed. 'This article refers to all of them in the manner cited: the patent number of the application filed on March 3, the number of the application number G9/5i8, 488 No. 〇9/6〇M54, filed in the U.S. Patent Application Serial No. (10)/759,212, filed Jun. 28, 2000, filed on Jan. _ The US patent application filed on February 15th of the year is No. G9/784,972. The improved EpD comprises a closed unit which is composed of a well-defined microcup having a shape, size and pore size and filled with charged pigment particles suspended in a dielectric solvent. A passive matrix system can be used to drive the Qing. In the case of a typical passive matrix system, there are row electrodes on the top (viewing surface) of the display and column electrodes at the bottom of the cells (or both arrangements can be inverted). The column electrodes and the row electrodes are perpendicular to each other. However, in the case of an EPD driven by a passive matrix system, there are two related known problems: crosstalk and cross bias. Crosstalk occurs when the electric field of adjacent cells of a cell provides a bias to the particles in the cell. Figure 丨 is an example. The bias voltage of cell A drives the positively charged particles toward the bottom of the cell. Since the single 兀B does not have any bias voltage, the positively charged particles in unit B should originally be expected to stay at the top of the unit, but the front electrode voltage of unit 3 is such that horse units 8 and 8 are very close to each other. (30V) and the bottom electrode voltage (〇v) of unit A will generate a crosstalk 1301257 electric field, which will make i Baibo s Ώ丄曰, and move some of the particles in the early 7G 向下 down. Relaxing the distance between adjacent units may eliminate this problem; however, this distance may also reduce the resolution of the display. If there is a single 亓, and if there is a non-hanging threshold voltage, then (4) string questions. The critical electric energy in the context of the present invention can be applied to the maximum partial voltage of a single 7L, but does not cause the particles to move between the two electrodes on the opposite side of the unit. If the units are very high The threshold voltage can reduce the crosstalk effect without sacrificing the resolution of the display. It is also a well-known problem for passive matrix displays. The voltage on the electrode is not only provided for scanning. The driver's bias voltage on the cell will also affect the bias of the non-scanning single S on the same row. This non-pre-four voltage may force the non-scanning cells to migrate to the opposite electrode. Expected particle migration causes visible optical density changes, and 1
降低該顯示器的對比度。 E ;年9月12曰提出申請的美國專利申請案第 0/322,635唬(法律檔案編號第26822_〇〇42號)中便說明一 種解決串訊及交又偏壓等問題的EPD,其名稱為「__ 有閘控%極之改良電泳顯示器(An Impr〇VedReduce the contrast of the display. E; the name of the EPD that solves the problems of crosstalk, crossover and bias, etc., is described in U.S. Patent Application Serial No. 0/322,635, filed on Sep. 12, 2009. "__ Improved electrophoretic display with gated % pole (An Impr〇Ved)
Electrophoretic Display with Gating Electrodes)」,基於所 f目的,本文以引用的方式將其併入。不過,即使一顯示 。。中所運用的單元呈現出先前段落中所參考之申請案中所 述之界效應’不過如果使用不對的被動矩陣驅動機制的 話,其仍然可能會有影像品質不佳及/或顯示效能不彰的問 1301257 題。這係因為呈現臨界效應(也就是,即使於交叉偏壓條件 下’非掃描列中仍然不會發生明顯的粒子遷徙,只要該交 又偏塵不超過臨界值即可)的某一單元仍然可能會因特定條 件下的交又偏壓而造成影像品質不佳,舉例來說,該等特 定條件為長時間施加該單元之標稱臨界電壓以下的直流 (DC)電壓,或是於該單元之初始狀態在該標稱臨界電壓以 下的交又偏壓條件下會發生非預期的特殊遷徙時施加該臨 界電壓或該標稱臨界電壓以下的電壓。再次聲明,特殊實 例或特殊組條件中某一單元的真實臨界電壓不僅取決該單 元的結構與材料,還會取決於下面的額外因素··該電壓的 施加日守間長度以及該單元的初始狀態。一單元可能會針對 第週期=τ中所施加的電壓呈現出第一臨界值vth=A,針 對另一兩倍週期(2T)中所施加的電壓呈現出弟二、較低的 臣品界值Vth=B。 所以’吾人需要一種被動矩陣驅動機制,其必須能解 決父又偏麼的問題並且還會考量到於該驅動機制下會受到 影響之特殊條件下能後夠影響該等EpD單元將會呈現之臨 界電壓Vth的各種變數。 和由被動矩陣驅動的EPD有關的另一項問題係反向偏 壓。舉例來說:當特殊單元上的偏壓電壓因含有該EpD媒 體層的材料及結構在内的固有電容中的已儲存電荷的關係 而產生提昇或降低的快速變化時,便會出現反向偏壓。舉 例來說,於上述申請案中所述的微杯式EpD中,該密封及 黏著層、該電泳分散劑、該微杯、以及任何其它絕緣層或 10 1301257 材料各具有一與其相關的固有電容(以及電阻)。當有一偏 壓電壓施加於一單元上時(例如用以將其驅動至不同的顯示 狀心)名些電谷便會被充電,並且會於偏壓電壓發生變化 時出現-反向偏壓。於特定環境下,此反向偏壓會藉由讓 又ρ θ單元中之帶電顏料粒子遷徙遠離其被驅動的位置而 影響顯示品質。 圖2 Α顯不的係一典型的EpD單元2〇〇,其包括大量 的電冰分散劑,言亥分散冑包括分散在一 #色介電溶劑2〇6 中的複數個帶電顏料粒子204。該分散劑係内含於一頂端 的Ί緣材料層208及-底部的絕緣材料層21()之中。於其 中-貫施例中,該絕緣材料可能包括一非導電聚合物。於 上述同在審查中之專利申請案中的單元中,此絕緣層可能 包括一密封及/或料層或是該微杯結構。該分散劑及相關 的黏著材料係位於一上方電極212及-下方電極214之間 「圖2A中顯示出三個點,其標示為「A」、%以及 「C」,點A係位於絕緣層2〇8的頂端,點b係位於絕緣 層208㈤底部(也就是,位於分散劑逝的頂端),而點〔 則係位於絕緣層21〇的底部。圖2β顯示的係圖2a之單元 00中"於點A與點C之間部份的等效電路。圖2B中, 電容器C1及雷阻R 7上± ϋ R1代表的係上方絕緣層—208的固有電 容及電阻。同樣地,電容器C2及電阻器尺2代表的係下方 絕緣層2 1 〇的固有雷交只@。 及電阻。分散劑202同樣會具有與 其相關的電容以及電阻。 ^ 1301257 如圖2A及2B所示,如果施加驅動電壓Vd至該上方 電極212並且將該下方電極214固定在接地電位的話,那 麼跨越該分散劑本身施加的電壓剛開始將會非常接近Vd, 不過’隨著電容器C1與C2被充電,該電壓便會略微下降 。圖3顯示的係隨著電容器C1與C2被充電,跨越該分散 劑施加的電壓的下降情形,以及如果跨越該單元200所施 的電壓驟然大1提昇而發生改變時(例如從驅動電壓Vd 轉k成零伏特)可能發生的誘發反向偏壓效應。於點a處 ,所施加的電壓可能係一正方形波形,剛開始會迅速上升 至Vd,保持於該位準,然後便快速地下降且停留在零值處 (士圖3中的虛線所示)。不過,當點a處所施加的電壓降 為零時,該分散劑實際上會受到一誘發反向偏壓的影響, 電容C1及C2會於此時放電,致使會至少以暫態方式(參 見圖3中標示為「反向偏壓」的點)於該分散劑上施加一負 电%。一旦該等電容被放電後,被施加至該分散劑上的電 壓(也就是’點B處)便會設回零值。視該等條件及單元設 計而定’該暫態誘發反向偏壓可能會造成影像品質不良, 例如藉由讓帶電顏料粒子遷徙遠離其被驅動的位置來顯示 預期的影像。 如上述,當長時間施加該單元之臨界電壓以下的偏壓 電壓而未予以中斷時,便會發生雷同的問題。此一未中斷 電C有日守亦稱為「直流」電壓或成份。於此等條件下,即 使該偏壓電壓低於該臨界電壓,帶電粒子仍然可能會遷徙 至非預期的位置,這係因為對長時間施加的偏壓電壓而言 ’該有效臨界電壓較低的關係。 12 1301257 ,里所以^吾人需要一種供被動矩陣EPD使用的驅動機制 可緩解反向偏壓及非預期之DC偏壓電壓效應等問 題。 【發明内容】 本發明提供一種減輕被動矩陣電泳顯示器中之誘發反 :偏Μ效應的系統與方法。於驅動循環前執行中間偏壓階 段’選擇該中間偏壓階段的該等偏壓條件,致使可將從該 驅動循環前的偏壓條件轉變成該驅動循環期間使用的偏壓 條件之過程分為至少兩道步驟。本發明料在每條已掃描 列的驅動階段後及下一條欲掃描列的驅動階段前插入一沉 ;#““又。本發明揭示於掃描前加入一前置驅動階段,用以 減㈣發反向偏壓效應。本發明揭^__㈣器及和該驅 動器相關的電極間加入一同線電阻器。本發明還揭示藉由 下面方法於一電泳顯示器中來顯示影像:t先將電泳單元 陣列驅動至白色顯示狀態,錢將背景區驅動至背景顯示 狀態。此外,本發明還揭示於掃描每列後插入一平衡階段 ’以便將非掃描列中的顯示元素還原成相同的初始狀態。 【實施方式】 應該瞭解的係,可以各種方式來實現本發明,其包含 一種方法,一種设備,一種系統;或是一種電腦可讀取媒 體,例如電腦可讀取儲存媒體;或是一種電腦網路,其中 <透過光學或電子通信鏈路來傳送程式指令。應該注意的 係,方;本發明的範臀内可改變本文所揭示之方法的步驟順 序。 13 1% 1301257Electrophoretic Display with Gating Electrodes), based on the purpose of which it is incorporated herein by reference. However, even one shows. . The unit used in the application presents the boundary effect described in the application referenced in the previous paragraph. However, if the passive matrix driving mechanism is used incorrectly, it may still have poor image quality and/or poor display performance. Question 1301257. This is because of the critical effect (that is, even in the case of cross-bias conditions, there is still no significant particle migration in the non-scanning column, as long as the intersection does not exceed the critical value) Image quality may be poor due to bias and bias under certain conditions. For example, the specific conditions are the direct current (DC) voltage below the nominal threshold voltage of the unit, or the unit. The initial state is a voltage applied below the nominal threshold voltage when an unexpected special migration occurs under an alternating bias condition below the nominal threshold voltage. Again, the true threshold voltage of a particular instance or special group of conditions depends not only on the structure and material of the unit, but also on the additional factors below. • The length of the application of the voltage and the initial state of the unit. . A unit may exhibit a first critical value vth=A for the voltage applied in the second period = τ, and a lower second value for the voltage applied in another double period (2T). Vth=B. So 'we need a passive matrix drive mechanism, which must solve the problem of the parent and the partiality. It will also consider the critical conditions that the EpD unit will present after the special conditions that will be affected by the drive mechanism. Various variables of voltage Vth. Another problem associated with EPD driven by passive matrix is reverse bias. For example, when the bias voltage on a particular cell changes rapidly or decreases due to the stored charge in the inherent capacitance of the material and structure of the EpD dielectric layer, a reverse bias occurs. Pressure. For example, in the microcup EpD described in the above application, the sealing and adhesive layer, the electrophoretic dispersant, the microcup, and any other insulating layer or 10 1301257 material each have an inherent capacitance associated therewith. (and resistance). When a bias voltage is applied to a cell (e.g., to drive it to a different display center), the name of the valley is charged and a reverse bias occurs when the bias voltage changes. Under certain circumstances, this reverse bias affects display quality by allowing the charged pigment particles in the ρ θ unit to migrate away from their driven position. Figure 2 shows a typical EpD unit 2, which comprises a large amount of electro-ice dispersant, and a plurality of charged pigment particles 204 dispersed in a #色 dielectric solvent 2〇6. The dispersant is contained in a top edge of the rim material layer 208 and a bottom insulating material layer 21 (). In these embodiments, the insulating material may comprise a non-conductive polymer. In the unit of the above-mentioned patent application under review, the insulating layer may comprise a sealing and/or layer or the microcup structure. The dispersant and associated adhesive material are located between an upper electrode 212 and a lower electrode 214. "Three points are shown in FIG. 2A, which are labeled as "A", %, and "C", and point A is located in the insulating layer. At the top of 2〇8, point b is at the bottom of insulating layer 208(5) (i.e., at the top of the dispersant), and the point is at the bottom of insulating layer 21〇. Fig. 2β shows the equivalent circuit of the portion between the point A and the point C in the unit 00 of Fig. 2a. In Fig. 2B, the capacitor C1 and the lightning resistance R 7 are ± ϋ R1 representing the inherent capacitance and resistance of the insulating layer 208 above. Similarly, the capacitor C2 and the resistor scale 2 represent the intrinsic lightning cross of the insulating layer 2 1 下方 below the @. And resistance. Dispersant 202 will also have its associated capacitance and electrical resistance. ^ 1301257 As shown in FIGS. 2A and 2B, if the driving voltage Vd is applied to the upper electrode 212 and the lower electrode 214 is fixed at the ground potential, the voltage applied across the dispersing agent itself will initially be very close to Vd, but 'As capacitors C1 and C2 are charged, this voltage will drop slightly. Figure 3 shows the drop in voltage applied across the dispersant as capacitors C1 and C2 are charged, and if the voltage applied across the cell 200 suddenly changes by one (e.g., from drive voltage Vd) k to zero volts can occur to induce a reverse bias effect. At point a, the applied voltage may be a square waveform that will initially rise to Vd, remain at that level, and then quickly fall and stay at zero (shown by the dashed line in Figure 3) . However, when the voltage drop applied at point a is zero, the dispersant is actually affected by an induced reverse bias, and capacitors C1 and C2 will discharge at this time, causing at least transient mode (see figure). The point labeled "Reverse Bias" in 3) applies a negative power % to the dispersant. Once the capacitors are discharged, the voltage applied to the dispersant (i.e., at point B) is set back to zero. Depending on these conditions and the design of the unit, the transient induced reverse bias may cause poor image quality, for example by allowing the charged pigment particles to migrate away from their driven position to display the desired image. As described above, when the bias voltage below the threshold voltage of the cell is applied for a long time without being interrupted, a similar problem occurs. This uninterrupted power C is also known as the "DC" voltage or component. Under these conditions, even if the bias voltage is lower than the threshold voltage, the charged particles may migrate to an unintended position because the effective threshold voltage is lower for the bias voltage applied for a long time. relationship. 12 1301257, so we need a driving mechanism for the passive matrix EPD to alleviate the problems of reverse bias and unintended DC bias voltage effects. SUMMARY OF THE INVENTION The present invention provides a system and method for mitigating the induced inverse: bias effect in a passive matrix electrophoretic display. Performing the intermediate bias phase prior to the drive cycle 'selecting the bias conditions of the intermediate bias phase, such that the process from the bias condition before the drive cycle to the bias condition used during the drive cycle can be divided into At least two steps. The invention feeds a sink after the drive phase of each scanned column and before the drive phase of the next column to be scanned; #"" again. The present invention discloses the addition of a pre-drive phase prior to scanning to reduce (4) the reverse bias effect. The in-line resistor is added between the __(4) device and the electrode associated with the driver. The present invention also discloses displaying an image in an electrophoretic display by the following method: t first driving the electrophoretic cell array to a white display state, and driving the background region to the background display state. Furthermore, the present invention also discloses inserting an equilibration phase ' after scanning each column to restore the display elements in the non-scan columns to the same initial state. [Embodiment] It should be understood that the present invention can be implemented in various ways, including a method, a device, a system, or a computer readable medium such as a computer readable storage medium, or a computer Network, where < transmits program instructions over an optical or electronic communication link. It should be noted that the steps of the method disclosed herein may be altered within the scope of the invention. 13 1% 1301257
下文將配合圖解本發明原理之圖式以範例來詳細地說 明本發明之一個以上較佳實施例。雖然配合此等實施例來 δ兒明本發明,不過,應該瞭解的係,本發明並不受限於任 何實施例。相反地,本發明的範疇僅受限於申請專利範圍 ,而且本發明涵蓋各種替代例、修正例、以及等效例。為 達不範目的,於下面的說明中會提出各種明確細節,以便 ^透澈地瞭解本發明。或許可根據申請專利範圍可實施本 發明,而不需要任何該等明確細節。為求清楚起見,和本 發明相關的技術領域中所熟知的技術内容將不作詳細說明 ’以免對本發明造成不必要的混淆。 &為解決交叉偏壓問題而施加至掃描列、非掃描列、 以及行電極之電壓之推導結果 合1本揭示之内文中的「臨界電壓(vth)」一詞係定義成不 會造成一單元中的粒子產生移動的最大偏壓電壓。本揭示 之内文中的「驅動電壓(Vd)」一詞係定義成用以改變一單DETAILED DESCRIPTION OF THE INVENTION One or more preferred embodiments of the present invention will be described in detail by way of example with reference to the drawings. While the invention has been described in connection with the embodiments, it should be understood that the invention is not limited to any embodiment. On the contrary, the scope of the invention is limited only by the scope of the claims, and the invention is intended to cover various alternatives, modifications, and equivalents. In the following description, various specific details are set forth in order to provide a clear understanding of the invention. The invention may be practiced according to the scope of the patent application without any such express details. For the sake of clarity, the technical contents well-known in the technical fields related to the present invention will not be described in detail so as not to obscure the present invention. & Derivation of the voltage applied to the scan column, the non-scan column, and the row electrode to solve the cross-bias problem. The term "threshold voltage (vth)" in the context of this disclosure is defined as not causing a The particles in the cell produce a moving maximum bias voltage. The term "drive voltage (Vd)" in the context of this disclosure is defined to change a single
=之顏色狀態(例如藉由將該單元中之該等粒子從—電極處 〔、近〇初始位置驅動至相反電極處或附近的末端位置)所 :加的偏壓電壓。某-特殊應用中所使用的驅動電壓vd 頊足以於该應用的必要效能參數内造成該單元之顏色狀 、毛生改變,包含此等參數(例如狀態轉換完成所花費之時 間)所測得者。 、、 被動矩陣顯示器中之「掃描」列係該顯示器中目前正 或再新的某一列。「非掃描」列係目前並未被更新 或再新的某-列。本揭示之内文中的「正偏壓」係定義成 14 1301257 傾向於讓正電粒子& μ u,, k 子向上遷徙(也就是,下方電極的電位高於 上方電極)的偏壓。因此 、 U此,正偏壓傾向於將正電粒子 表面驅動,例如用以將一 。本揭干早70切換至白色或「開啟」狀態 子== 負偏磨」係定義成傾向於讓正電粒 :向下遷徒(也就是’下方電極的電位低於上方電極)的偏 端二:型:皮動矩陣來說,該等列電極可能係位於頂 叮。μ電極可能係位於底部且垂直該 可倒置排列亦然。圖以及心至㈣所示的係—2χ2 ^ ^ ^ P# 〇 @ 4Α ^ ^ ^ # ^ ^ f 谰HI。仏固丄 巾〜zxz被動矩陣之俯= color state (e.g., by applying the particles in the cell from the -electrode [, near the initial position of the crucible to the end position at or near the opposite electrode): the applied bias voltage. The driving voltage vd 某 used in a particular application is sufficient to cause the color and the change of the unit within the necessary performance parameters of the application, including those measured by the parameters (such as the time taken for the state transition to complete). . The "Scan" column in the passive matrix display is a column currently being updated or renewed in the display. The "Non-Scan" column is a column that is not currently updated or renewed. The "positive bias" in the context of the present disclosure is defined as the bias of 14 1301257 which tends to cause the positively charged particles & μ u,, k to migrate upward (i.e., the potential of the lower electrode is higher than the upper electrode). Therefore, U, the positive bias tends to drive the surface of the positively charged particles, for example to be used. This is done as early as 70 switching to white or "on" state == negative eccentricity is defined as the tendency to let positive particles: move downwards (that is, the potential of the lower electrode is lower than the upper electrode) Two: Type: For the skin matrix, the column electrodes may be located at the top. The μ electrode may be located at the bottom and perpendicular to the invertible arrangement. Figure and heart to (4) shown in the series -2χ2 ^ ^ ^ P# 〇 @ 4Α ^ ^ ^ # ^ ^ f 谰HI.仏固丄 towel~zxz passive matrix
奋,,電壓A會驅動頂端的非掃描列,而電壓B 則會驅動底部的掃描列。 电U 剛開始,如圖4B」至4B_4所示,單元以及Z 中的粒子係位於該等單元的頂 付於兮梦一 幻貝知而早凡X中的粒子則係 ::…的底部。假設此處欲調整的係掃描列Β,致 二的粒子移動至底部電極,同時讓單元Ζ中的粒 :二持在其目:的頂端電極位置處。當然,即使出現交又 偏>£狀況’非掃描列之單元中 早7°巾的粒子亦應該㈣會維持在 ”初始的位置處-頂端電極處的w以及底部電極處的X。 因為單元W及X係位於非掃描列中,所以其目標便 係即Μ叉偏壓狀況影響該列,亦可確保該等粒子維 在目前的電極位置處。於縿此土 冑於省些兩種情況·中,該單元的臨界 電壓都係一非常重要的因素。除非該臨界„大於或等於 可能會出現的交又偏屋電壓,不然,當出現此交又偏歷時 15 1301257 該些單元中的該等粒子便將會移動,從而降低對比度。 為於特定時間週期内將單元γ中的該等粒子從頂端電 極驅動至底部電極’必須施加一驅動電壓vd。特殊應中所 使用的驅動電麼可能係取決於數種因素,其包含但不“必僅 限於單元幾何、單元設計、陣列設計及佈置、以及所使用 的材料與溶劑。為移動單元γ中的該等粒子而不會影響單 兀W、x及Ζ中的該等粒子,用於改變單元丫之狀態所施 加的驅動電壓Vd的強度以及施加方式必須讓其餘單元受 到偏壓作用的大小不會大於該等單元的臨界電壓Vth。 為決定在該些條件下避免於圖4A至4B-4中所示之基 本被動矩陣中發生非故意的狀態改變所需要的最小臨界電 壓,必須滿足下面的不等式: A-C<Vth D-A<Vth B-C>Vd B-D<Vth 將含有Vth在内的三個不等式相加後便可解出此等式 糸統’付出不等式(A-C)+(D-A) + (B-D)<Vth+Vth+Vth,簡 化後變成B-C<3 Vth或是3 Vth>B-C。將此不等式與剩餘的 不等式B-C〉Vd結合後便可得出3Vth〉B-C>Vd的結果,得 出3Vth>Vd或是Vth>l/3Vd。也就是,對圖4A至4B.4所 示的被動矩陣而言,該等單元的臨界電壓必須大於或等於 用來改變該些單元之狀態而欲施加之驅動電壓的三分之— ,以便發生預期的狀態改變,方能避免因交叉偏壓該些單 16 1301257 元的狀悲而造成的變化,從而發生非預期的狀態改變。 進一步麥考圖4A至4B-4,如果施加驅動電壓Vd至 掃描列B的活,那麼解出上面不等式便會指出必須確保下 面狀況Ή頁施加驅動偏壓電壓給欲進行冑式化的單元而 且不會施加高於臨界電壓的電壓給其它單元(也就是,該掃 !田列中的非紅式化單凡以及非掃描列中的所有單元"被施 加至該非掃描列Α的電壓應該等於l/3Vd,被施加至和欲 進行程式化(也就是,改變顯示狀態)之掃描列中之一單元 相關聯的行電極(例如行電極C)的電壓應該為〇伏,被施 =至和不欲進行程式化(也就是,保持初始或重置狀態)之 掃描列中之一單元相關聯的行電極的電壓應該等於2/3vd 。舉例來祝’於其中-實施例中,為達成可接受效能所需 要的驅動電壓為30V。如果圖4A至4B_4中所示之被動矩 陣顳示器中的驅動電壓Vd=3〇v的話,那麼若欲藉由施加 30V的驅動電壓至單元γ以保持單元w、χ以及z之初始 狀態且同時改變單元γ之狀態所需要的最小臨界電壓便會 係Vth=10V。假設B=30V,那麼上面等式的解便係a=i〇v 、O0V以及D=2〇V。參考圖4Α至4β·4,吾人便能夠看 見,於該些條件下,被施加至單元w、x以及ζ中每一者 處之偏壓實際上便會小於或等於最小臨界電壓Vth=1〇v。 從圖中顯示出,此解可使用於任何尺寸的被動矩陣,而且 不限於圖4A中所示之2X2陣列。 於其中一貫施例中,一被動矩陣電泳顯示器包括一利 用捲對捲㈣i-to-roU)製程所製成的顯示媒體。含有該顯示 17 1301257 媒體之顯示元素包括 中所述的微杯式EPD單 方式所併人之專利申請案 封該等微杯 70於其中一實施例中可個別地密 的住-二’致使可將整片或整捲的顯示媒體切割成任何 ,、思於其中—實施例中,可提供—連接子/轉接子 :亥顯不媒體之該等列電極及/或行電極連接至-驅 /路,例如驅動器積體電路(1C)。舉例來說,於LCD技 *中,可利用「扇出」及/或「扇入」方式來將行電極及/ 或:電極連接至-驅動IC’其連接子(黏接觸點)的寬度 1不及&顯不$的寬度° ® 4C所示的係使用於行電極 d」方式。遠等行電極440包括一筆直部份442, 該料係為於該等列電#构之上。該等行電極進一步包 羽°卩知446,其能夠讓該等行電極44〇與驅動器積 體=路(1C) 448產生電連接。於LCD技術中,藉由於該顯 不器之玻璃基板上形成電極扇入/扇出部份便可實現圖4C 中所示之方式。 上述之扇入/扇出方式可供一被動矩陣EpD來使用, 不過,吾人必須事先知道該顯示器的形狀,以便能夠於該 基板上形成該等電極的扇入或扇出部份。圖4D所示的係 一替代方式,其中提供一連接子/轉接子,用以讓一任意形 狀顯不器能夠被連接至一驅動器1C。於圖4D所示之圖解 範例中,已經從僅具有筆直列或行(也就是,沒有任何的扇 入部份或扇出部份)之整片或整捲EPD顯示器中切割出一 四列乘四行的區段460。該等行電極462會透過一連接子/ 轉接子464被電連接至行驅動器ic 466,其方式係藉由於 18 1301257 468中將和該連接子/轉接子偏相關 认甘”動益IC 466相關聯之相應的複數 调黏接觸點。於直中一普 例中,可利用導電黏著劑(例如 =或銀質糊狀劑)將該行驅動器IC4_接至該連接子/ 妾子464。5亥連接子/轉接子464的結構非常類似圖化 所不之扇入部份446。相同地,該等列電極Μ會透過連 接子/轉接子474被電連接至列驅動器Ic 476。藉由提供各 種化狀”尺寸之扇人/扇出連接子/轉接子,那麼透過支援 從整捲或整片顯示媒體中切割下來之任意形狀顯示器的連 接但部不必改變或客製化該製程,便可實現利用捲對捲製 私所形成之EPD媒體的最大彈性,而且不會增加該製程的 複雜度及無彈性。 I加入中間階段、沉澱階段、及/或前置驅動階段以減 輕反向偏塵效應 本章節中所述的被動矩陣驅動技術假設一包括一由電 泳單元所組成之陣列的被動矩陣電泳顯示器含有一電泳分 放劑,该分散劑包括分散在一有色介電溶劑中的正電顏料 粒子。於其中一實施例中,該等帶電顏料粒子為白色,而 該介電溶劑則為黑色或適合作為背景色之特定其它對比色 。於本文所述之範例中,單元臨界電壓Vth係假設為丨〇v ,而單元驅動電壓Vd則假設為30V。於本文所述之範例 t,該EPD係假設為於該EPD之觀看表面側上之該顯示 器的上層(位於該EPD單元陣列之上)中包括一行電極陣列 ’以及於该顯示器中和該觀看表面相反的側上之該顯示器 19 1301257 的下層(位於該EPD單元陣列之下)中包括一列電極陣列。 於該些範例所述之卿巾,會將和—像素相關聯之單元中 的該等白色顏料粒子驅動至該觀看表面,用以於該像素中 顯示白色的顏色,必且可取而代之地於該等單元之底部處 被驅動(或是維持不變),用以於該像素中顯示黑色的顏色 (或是其它背景顏色)(而且於特定實施例中,必要時,可部 份被驅動至該頂端或底部表面,用以於該像素中顯示一灰 階顏色)。 熟習本技術的人士將會發現,本文所述的技術亦可使 用於具有其它類型的單元、不同的電泳分散劑(無任何限制 ’吾人亦可具有負電顏料粒子)、不同顏色、不同電極排列 等的其它被動矩P車EPD,必要時可輕易地計算出本文所述 之電壓的極性變化及/或強度變化,以便達成本文所述之結 果。 圖5所示的係本章節所述之圖解範例中所使用的組態 與情況。圖中所不的係一 3χ3的被動矩陣EpD陣列5〇〇(舉 例來說,其可能係一更大型陣列的一部份)。於圖5中,該 陣列500包括複數個列電極5〇2、5〇4以及5〇6,其亦分別 被標不為Rl、R2以及R3。該陣列5〇〇進一步包括複數個 订電極508、510以及512,其亦分別被標示為C1、C2以 及C3。某一列電極及某一行電極的每個交點皆具有一和其 相關聯的電泳顧示元素,例如第一列5〇2及第一行5〇8之 交點處的元素514。於下面的討論中,可以一組笛卡兒座 標來確認對應的列編號與行編號以表示一顯示元素(元素 20 1301257 514),例如元素514可表示為(R1、C1),因為其係位於列 R1及行C1之中。 士圖5所示之3x3陣列500的狀態係假設如下:該陣 列中的全部九個顯示元素已經被重置為黑色/背景狀態,其 中忒等白色帶電顏料粒子已經被驅動到該等顯示元素的底 部(非觀看側);而且為達本目的,此處考慮的係經由連續 掃描列Rl、R2以及R3後僅有第一行中的元素(R1、ci)以 及(R3、Cl)會被切換成白色狀態(帶電顏料粒子會被驅動到 頂端,也就是觀看表面),而元素(R2、叫則會維持其初始 的、黑色狀態(底部處的粒子)。下面的段落說明的係各種 驅動機制,其可用於將該等第一行(C1)的元素從該等單元 被重置為全黑的初始狀態驅動成圖5所示的最終狀態。 圖6所示的係一基本被動矩陣EpD的驅動機制。對一 :本被動矩陣EPD而言’該掃描列中欲被切換的該等像素 久处;最同的驅動能量下,該驅動能量和驅動電壓及 衝寬度的乘積成正比。該掃描列中的該等非切換像素以 及2掃描列中的該等像素通常會受到最大驅動能量的三分 的作用(參見上面章節A中的討論)。所以,只要含有 乂等像素之EPD單元的臨界效應大於最大驅動能量的三分 之一,那麼該交叉偏壓效應理論上便將不會對影像品質造 參考圖6,標示為602的區域包括一重置循環,其中 所2的單70都會被驅動至初始的黑色/背景狀態,於該初始 狀怨中,該等帶電顏料粒子都係處於該等單元的底部。如 21 1301257 圖6所示,於第一區間中全部三列都會被設在3〇伏處, 而該等行電極(行C1)則會被固定在〇伏處;其後跟隨的係 一實質相等的第二區間,該等列電極會於該第二區間期間 被固疋在0伏處,而該等行電極則會被設在3 0伏處;其 後跟隨的則係反覆第一區間與第二區間。於其中一實施例 中僉終區間(於該區間中,該等行電極(位於頂端,也就是 該顯示器的觀看表面)會被驅動至3〇伏,而該等列電極則 S被固疋在〇伏處)會導致該等正電顏料粒子被驅動至遠離 該等行電極且靠近該等列電極的位置(也就是,被驅動至該 等單元的底部)。如上所述,此範例以及本文所述之其它範 例中所述的電壓都僅係供作解釋用途,而且所使用之電壓 的極性與大小將會隨著特殊設計而改變。 進一步參考圖6,於第一列掃描區間604期間會掃描 第一列R1,於第二列掃描區間6〇6期間會掃描第二列R2 ,以及於第三列掃描區間608期間會掃描第三列R3。如圖 6所示,s某一列正在被掃描時,其便會被設在驅動電壓 Vd=3〇V處’而所有其它列則會被設在l/3Vd=10V處。® 6顯示出之電壓係於列R1至R3的驅動期間被施加至該等 仃电極C1,以達成如圖5所示之該等行c1單元的最終狀 怨。單7L (Rl、C1)以及(R3、C1)都會被驅動至白色狀態(帶 電粒子被驅動到頂端)。就此而言,於列R1及R3的掃描 期間(區間604及608),行電極C1會被固定在〇v處,所 造成的結果係,該等單元(R1、C1)以及(R3、C1)的頂端以 及該些單元的底部之間的電位降大小會係完整的Vd=3〇v 22 1301257 ,致使該些單元中的帶電粒子會於其個別列的掃描期間被 驅動至靠近該顯示器之觀看表面側上之頂端(也就是,行) 電極的新位置(請注意,頂端與底部等用語都係隨意指定的 。如本文所使用般,「頂端」所指的係該顯示器之觀看表 面。不過’於某些設計中,此處卻可能係該顯示元素的實 體「底部」,例如於微杯設計中即為如此,其中該等微杯 的「底部」會構成該觀看表面,而該等微杯的密封「頂端 」則會構成與該觀看表面相反的表面)。相反地,單元(R2 、ci)係維持其初始的、黑色/背景狀態。就此而言,於列 R2的掃描期間,行電極C1會被設為2〇v,致使跨越單元 (R2、C1)的電位差僅為1〇v(也就是,驅動電壓Vd的m) ,並且等於(也就是,不大於)公稱臨界電壓Vth,所造成 的結果係’料帶電粒子會維持在初始狀態+,該初始狀 悲係於重置循環602期間被重置的狀態。 雖然圖6所示之被動矩陣驅動機制理論上應該係有效 的,不過,因為其會如上面章節A中所述般地考量臨界電 i Vth及驅動電壓Vd間的算術推導關係,所以,圖6所 丁之機制並無法解決非切換像素中之反向偏壓的問題。圖 7所示的係-被動矩陣EPD驅動機制,其中已經加入一中 間P白I又’用來減起非切換像素中的反向偏壓。目7中所示 之機制係攸和圖6所示相同的重置循環6〇2開始。於該重 置循%之後及驅動循j裒7〇4之前則已經加入_中間階段 2其中β驅動循環和圖6之區間6〇4-6〇8相同。於該中 ’戸白丰又702期間,該等行電極(例如行電極ci)會被驅動至 23 1301257 20V,而該等列電極則會被驅動至1 〇v。加入此一中間階 段便可將從重置循環轉換成驅動循環的過程分為兩道步驟 ,從而便可減輕反向偏壓效應。舉例來說,吾人可以比較 圖6及7中所示之個別機制下被施加至像素(R2、C1)的電 Μ。於圖6之機制下,(R2、C1)於該重置循環的最終區間 期間會受到30V負偏壓(行C1電壓比列R2電壓高30V)的 作用,隨後則會受到10V正偏壓(於區間604期間,R2處 之電壓=iov,ci處之電壓=〇v)的作用。淨轉換為40ν。 相較之下,於圖7之機制下,此轉換會分為兩道步驟,第 -人的20V轉換係從該重置循環的最終區間進入該中間階 段702(從該重置循環終點處之R2-C1=-30V變成該中間階 段中之R2-C1=-10V);第二次的20V轉換則係從該中間階 段702進入該驅動循環704的第一部份,其對應的係圖6 的區間604(從該中間階段中之R2_cl=_1〇v變成該驅動循 環之初始部份處之R2_C1 = 10Vp將此轉換分為兩道較小步 驟便可減輕該反向偏壓效應。 圖8中所示的被動矩陣EPD驅動機制可進一步改進圖 7所示之機制。圖8中所示的機制係從圖7的中間階段 702開始,並且假設於該中間階段7〇2之前已經完成二: 重置循環(例如重置循環602,圖8中並未顯示該循環)。 於該中間階段702後面的驅動循環中,則已經於掃 之後以及掃描下-列之前加入—「沉澱」階段。因此,第 一列R1掃描區間802之後便係沉澱階段8〇4,於該階段中 會將所有的列電極及行電極設為0伏,以便讓該等::顏 24 1301257 料粒子沉澱且集結在一起,並且於掃描下列之前讓該等 EPD單元結構之固有電容進行放電。同樣地,第二列R2 掃描區間806之後便係沉澱階段808,而且第三列R3掃描 區間8 1 〇之後便係沉澱階段812。於掃描下列之前讓該等 固有電容進行放電便可減輕該反向偏壓效應。此外,導入 一沉澱階段可分解被施加至該等單元的DC成份,此作法 相當有利,因為如上述,即使施加一小於或等於該公稱臨 界龟壓Vth的DC成份一段長時間而未予以中斷便可能會 對影像品質造成負面影響。最後,於其中一實施例中,因 為该等粒子之間及/或該等粒子和該介電溶劑之間及/或 EPD結構與材料的物理、化學、及/或電氣相互作用的關係 ,該沉澱階段可讓該等帶電粒子更緊密地集結在一起,從 而讓該等單元更完整且強烈地呈現出本文所述之電壓特徵 〇 圖9 A所示的係一被動矩陣EPd驅動機制,其中已經 於圖8所示之機制中在掃描每列前後加入額外的中間階段 。可於重置之後施加第一類型之初始中間階段902。如圖 9A所示,於其中一實施例中,該第一類型中間階段9〇2與 圖7之中間階段702相同(也就是,有複數行在2〇v處且 有複數列在10V處)。於圖9 A所示之機制中,該第一類型 中間階段902的之後係第一列ri掃描階段904 ,揍著,其 後面係第二類型中間階段906(於其中一實施例中,如圖 9A所示,其包括將該等列電極設為1〇v且將該等行電極 設為0V),其後面則係沉澱階段908,於該階段中會將所 25 1301257 有的列電極及行電極皆設為0V。接著便可針對第二列R2( 階段910至916)以及第三列R3(階段918至924)反覆進行 上面針對第一列R1所述之四個階段循環(階段9〇2至9〇8) 0 於其中一實施例中,在圖9A所示之機制中導入該等 額外的中間階段會使得每個像素先受到一負偏壓電壓(第一 類型中間階段)作用,然後再受到一大小相等而極性相反之 負偏壓電壓(第二類型中間階段)作用,以交錯的方式進行 便可降低因長期施加相同的交叉偏壓電壓未予以中斷所造 成的粒子遷徙現象。如圖8所示之機制,該沉澱階段可讓 該等粒子沉澱且集結在一起。此外.,於掃描後加入該等第 二類型中間階段則可降低一機制中(例如圖8中所示之機制 ,也就是,於掃描後加入一沉澱階段的機制)在掃描後所發 生之偏壓電壓下降的現象,從而可進一步降低誘發反向偏 壓效應。 圖9B所示的係一被動矩陣EPE)驅動機制,其中已經 修正圖6所示之驅動循環(區間6〇扣6〇8),使其在掃描每一 列之如包含一前置驅動脈衝。如果和該像素相關聯的資料 係為欲施加該驅動偏壓電壓來改變該電極之顯示狀態的話 ’那麼於圖9B中所示之驅動波形及下面更完全的說明中 便會使用一反向驅動脈衝(本文稱為前置驅動脈衝)先於該 電極的一方向來驅動該掃描列中複數個像素的該等粒子, 該方向與該掃描列中之該等粒子在掃描期間被驅動的方向 相反。在該前置驅動脈衝已經充電該像素而倒置其極性之 26 用以將談等粒子驅動 1301257 後’接著便會施加該正向驅動脈衝, 至指定的電極。 於圖9B戶斤示的示範驅動波形中,在每個掃描循環之 前便有-個此類前置驅動脈衝。於圖9β ^的範例中, 吾人假設該等像素含有正電白色_粒子懸浮在黑色的介 電溶劑中,其重置狀態為黑色顯示狀態,於該狀態中,該 等帶電粒子已經被驅動至該列(底部)電極處或其附近的位 置,而欲寫入的資料則係行C1中列R1與R3中的像素會 被寫入成白色顯示狀態(行(頂端)電極C1處或其附近的粒 子),而列R2中的像素則會維持在黑色顯示狀態。當定址 某一列(例如R1)時,該掃描列中之該等像素便會於前置驅 動階段942期間被首先重置為黑色顯示狀態,於該階段期 間’下個欲被掃描的列(即R1)會被設為〇V,而非掃描列 R2與R3以及行電極(例如行電極ci)則會被設為3〇v,導 致會有一反向驅動(即重置)偏壓條件被施加至列R1的該等 像素,但卻沒有任何偏壓會被施加至非掃描列中的像素。 接著列R1便會於列R1掃描階段944期間被設為30V。於 列R1掃描階段944期間,行電極C1會被設為〇V,導致 行C1列R1中相關聯的像素會依照與該像素相關聯的顯示 資料被驅動至白色顯示狀態。於列R1掃描階段944期間 ’非掃描列R2及R3會被設為10V,以避免此等非掃描列 中之像素的顯示狀態因交又偏壓的關係而發生改變。掃描 列R1之後便是列R2的前置驅動階段946,於該階段中, 列R2會被設為〇v,而列R1與R3以及行電極(例如C1)則Excuse, voltage A drives the non-scanning column at the top, while voltage B drives the scanning column at the bottom. At the beginning of the electric U, as shown in Figs. 4B" to 4B_4, the cells in the cell and Z are located at the bottom of the cells that are in the vicinity of the nightmare. Assuming that the system to be adjusted here scans the column, the particles of the second are moved to the bottom electrode, while the particles in the cell are held at the top electrode position of the target. Of course, even if there is a cross-cutting > £ condition, the particles of the 7° early in the non-scanning column should (4) be maintained at the “initial position—w at the top electrode and X at the bottom electrode. The W and X systems are located in the non-scanning column, so the target is that the yoke bias condition affects the column, and it is also ensured that the particle granules are at the current electrode position. In the middle, the critical voltage of the unit is a very important factor. Unless the critical value is greater than or equal to the crossover voltage that may occur, otherwise, when the intersection occurs and the bias is 15 1301257, the unit The particles will move and the contrast will be reduced. A driving voltage vd must be applied in order to drive the particles in the cell γ from the top electrode to the bottom electrode ' during a specific time period. The driving power used in a particular application may depend on several factors, including but not necessarily limited to cell geometry, cell design, array design and placement, and materials and solvents used. The particles do not affect the particles in the single 兀W, x and Ζ, the intensity of the driving voltage Vd applied to change the state of the unit 以及 and the manner in which the application must be biased by the remaining units Greater than the threshold voltage Vth of the cells. To determine the minimum threshold voltage required to avoid unintentional state changes in the basic passive matrix shown in Figures 4A through 4B-4 under these conditions, the following inequality must be satisfied. : A-C<Vth D-A<Vth B-C>Vd B-D<Vth Adding three inequalities including Vth to solve this equation's paying inequality (AC)+( DA) + (BD) <Vth+Vth+Vth, which becomes simplification and becomes B-C<3 Vth or 3 Vth> BC. Combining this inequality with the remaining inequality BC>Vd gives 3Vth>B- The result of C>Vd is 3Vth>Vd or Vth>l/3Vd. For the passive matrix shown in Figures 4A to 4B.4, the threshold voltage of the cells must be greater than or equal to three-thirds of the driving voltage to be applied to change the state of the cells, so that the expected The state changes to avoid the change caused by the cross-biasing of the single 16 1301257 yuan, resulting in an unexpected state change. Further McCaw charts 4A to 4B-4, if the driving voltage Vd is applied to the scanning column B's activity, then the above inequality will be pointed out that it is necessary to ensure that the following conditions apply the driving bias voltage to the unit to be clamped and that no voltage higher than the threshold voltage is applied to the other unit (ie, the sweep) The non-redformed and non-scanned cells in the field column are applied to the non-scanning column and the voltage applied to the non-scanning column should be equal to l/3Vd, applied to and intended to be programmed (ie, changed display) The voltage of the row electrode (eg, row electrode C) associated with one of the scan columns of the state column should be 〇V, applied to and not programmed (ie, remain in the initial or reset state) The voltage of the row electrode associated with one of the cells in the scan column should be equal to 2/3 vd. For example, in the embodiment - the drive voltage required to achieve acceptable performance is 30 V. If shown in Figures 4A through 4B_4 If the driving voltage Vd=3〇v in the passive matrix display is shown, then if the driving voltage of 30V is applied to the cell γ to maintain the initial state of the cells w, χ, and z and simultaneously change the state of the cell γ. The minimum threshold voltage required is Vth = 10 V. Assuming B = 30 V, then the solutions of the above equation are a = i 〇 v , O 0 V and D = 2 〇 V. Referring to Figures 4A to 4β·4, it can be seen that under these conditions, the bias applied to each of the cells w, x and ζ is actually less than or equal to the minimum threshold voltage Vth = 1 〇 v. It is shown from the figure that this solution can be used for passive matrices of any size and is not limited to the 2X2 array shown in Figure 4A. In a consistent embodiment, a passive matrix electrophoretic display includes a display medium made using a roll-to-roll (iv) i-to-roU process. The display element containing the display 17 1301257 medium includes the micro-cup EPD single-mode patent application described in the above-mentioned patent application. The micro-cups 70 can be individually densely-occupied in one embodiment. Cutting the entire or full-volume display medium into any, and thinking about it - in the embodiment, it can be provided - the connector / the adapter: the column electrodes and / or row electrodes connected to the - drive / Road, such as the driver integrated circuit (1C). For example, in LCD technology*, the "fan-out" and/or "fan-in" method can be used to connect the row electrode and/or the electrode to the width of the connector IC (the contact point of the drive IC). Less than & not visible $ width ° ® 4C is used in the row electrode d" mode. The far row electrode 440 includes a straight portion 442 that is above the array. The row electrodes further enclose 446, which enables the row electrodes 44A to be electrically connected to the driver integrated circuit (1C) 448. In the LCD technology, the manner shown in Fig. 4C can be realized by forming an electrode fan-in/fan-out portion on the glass substrate of the display. The above fan-in/fan-out mode can be used for a passive matrix EpD. However, the shape of the display must be known in advance so that the fan-in or fan-out portions of the electrodes can be formed on the substrate. An alternative to that shown in Figure 4D is the provision of a connector/condulator for enabling an arbitrary shape display to be coupled to a driver 1C. In the illustrated example shown in FIG. 4D, a four-column multiplication has been cut from a full-piece or full-volume EPD display having only straight columns or rows (ie, without any fan-in or fan-out portions). A four-row section 460. The row electrodes 462 are electrically connected to the row driver ic 466 through a connector/switch 464 by way of a partial correlation with the connector/transformer in 18 1301257 468. 466 associated with a plurality of viscous contact points. In a straightforward example, the row driver IC4_ can be connected to the connector/tweezer 464 using a conductive adhesive (eg, = or a silver paste). The structure of the 5H connector/switch 464 is very similar to the fan-in portion 446 of the figure. Similarly, the column electrodes are electrically connected to the column driver Ic 476 through the connector/transfer 474. By providing a variety of sized "fans / fan-out connectors / adapters", the connection of any shape display that is cut from the entire roll or the entire display medium is supported, but does not have to be changed or customized. The process can achieve maximum flexibility in the use of roll-to-roll private EPD media without increasing the complexity and inelasticity of the process. I join the intermediate stage, the precipitation stage, and/or the pre-drive stage to mitigate the reverse dust effect. The passive matrix drive technique described in this section assumes that a passive matrix electrophoretic display comprising an array of electrophoretic cells contains a An electrophoretic dispensing agent comprising positively charged pigment particles dispersed in a colored dielectric solvent. In one embodiment, the charged pigment particles are white and the dielectric solvent is black or a particular other contrasting color suitable as the background color. In the example described herein, the cell threshold voltage Vth is assumed to be 丨〇v, and the cell driving voltage Vd is assumed to be 30V. In the example t described herein, the EPD is assumed to include a row of electrode arrays in the upper layer of the display (on the EPD cell array) on the viewing surface side of the EPD, and in the display and the viewing surface The lower layer of the display 19 1301257 (located under the EPD cell array) on the opposite side includes a column of electrode arrays. The scented towels of the examples will drive the white pigment particles in the unit associated with the pixel to the viewing surface for displaying the white color in the pixel, and may instead The bottom of the cell is driven (or remains unchanged) to display a black color (or other background color) in the pixel (and in certain embodiments, if necessary, may be partially driven to the The top or bottom surface is used to display a grayscale color in the pixel). Those skilled in the art will recognize that the techniques described herein can also be used with other types of units, different electrophoretic dispersants (without any limitation 'we can also have negatively charged pigment particles), different colors, different electrode arrangements, etc. Other passive moment P-car EPDs, if necessary, can easily calculate the polarity change and/or intensity variation of the voltages described herein to achieve the results described herein. Figure 5 shows the configuration and conditions used in the graphical examples described in this section. What is not shown in the figure is a 3χ3 passive matrix EpD array 5〇〇 (which may be part of a larger array, for example). In Fig. 5, the array 500 includes a plurality of column electrodes 5〇2, 5〇4, and 5〇6, which are also labeled R1, R2, and R3, respectively. The array 5 further includes a plurality of set electrodes 508, 510, and 512, which are also labeled C1, C2, and C3, respectively. Each intersection of a column of electrodes and a row of electrodes has an electrophoretic element associated with it, such as element 514 at the intersection of the first column 5〇2 and the first row 5〇8. In the following discussion, a set of Cartesian coordinates can be used to confirm the corresponding column number and row number to represent a display element (element 20 1301257 514), for example element 514 can be represented as (R1, C1) because it is located Column R1 and row C1. The state of the 3x3 array 500 shown in Figure 5 is assumed to be as follows: all nine display elements in the array have been reset to a black/background state in which white charged pigment particles have been driven to the display elements. Bottom (non-viewing side); and for this purpose, the elements considered here (R1, ci) and (R3, Cl) are switched after successive scans of columns R1, R2 and R3. In a white state (charged pigment particles are driven to the top, that is, viewing the surface), while elements (R2, will maintain their initial, black state (particles at the bottom). The following paragraphs illustrate various driving mechanisms , which can be used to drive the elements of the first row (C1) from the initial state in which the cells are reset to all black to the final state shown in Figure 5. Figure 6 shows a basic passive matrix EpD Driving mechanism. For one: the passive matrix EPD, 'the pixels in the scan column to be switched are long; the same driving energy, the driving energy is proportional to the product of the driving voltage and the punch width. The scan In the column Such non-switched pixels and the pixels in the 2 scan columns are typically subjected to a three-point maximum drive energy (see discussion in Section A above). Therefore, as long as the EPD unit containing 乂 pixels has a critical effect greater than the maximum drive One-third of the energy, then the cross-bias effect will theoretically not refer to Figure 6 for image quality. The area labeled 602 includes a reset cycle in which the single 70 of the 2 is driven to the initial Black/background state, in the initial complaint, the charged pigment particles are at the bottom of the unit. As shown in Fig. 6 of 21 1301257, all three columns in the first interval are set at 3 volts. And the row electrodes (row C1) are fixed at the squat; followed by a substantially equal second interval, the column electrodes being solidified at 0 volts during the second interval And the row electrodes are set at 30 volts; followed by the first interval and the second interval. In one embodiment, the final interval (in the interval, the row electrodes) (located at the top, that is, the display The viewing surface of the device will be driven to 3 volts, and the column electrodes S will be fixed at the undulations) causing the positively charged pigment particles to be driven away from the row electrodes and close to the column electrodes The position (i.e., driven to the bottom of the cells). As noted above, the voltages described in this example and other examples described herein are for illustrative purposes only, and the polarity of the voltage used is The size will vary with the particular design. Further referring to Figure 6, the first column R1 will be scanned during the first column scan interval 604, and the second column R2 will be scanned during the second column scan interval 6〇6, and The third column R3 is scanned during the three-column scanning interval 608. As shown in Fig. 6, when a column of s is being scanned, it is set at the driving voltage Vd=3〇V and all other columns are set. At l/3Vd=10V. The voltages shown by ® 6 are applied to the electrodes C1 during the driving of columns R1 to R3 to achieve the final grievance of the row c1 units as shown in FIG. Single 7L (Rl, C1) and (R3, C1) are driven to a white state (charged particles are driven to the top). In this regard, during the scanning periods (intervals 604 and 608) of the columns R1 and R3, the row electrode C1 is fixed at 〇v, resulting in the units (R1, C1) and (R3, C1). The magnitude of the potential drop between the top end and the bottom of the cells will be complete Vd = 3 〇 v 22 1301257, causing charged particles in the cells to be driven close to the display during scanning of their individual columns. The top position on the surface side (ie, the row) The new position of the electrode (note that the terms top and bottom are arbitrarily specified. As used herein, "top" refers to the viewing surface of the display. 'In some designs, it may be the "bottom" of the display element, as in the microcup design, where the "bottom" of the microcups will constitute the viewing surface, and the micro The seal "top" of the cup will form the opposite surface to the viewing surface). Conversely, the cell (R2, ci) maintains its original, black/background state. In this regard, during the scanning of the column R2, the row electrode C1 is set to 2 〇 v, so that the potential difference across the cells (R2, C1) is only 1 〇 v (that is, m of the driving voltage Vd), and is equal to (ie, no greater than) the nominal threshold voltage Vth, the result of which is that the charged particles will remain in the initial state +, which is in a state of being reset during the reset cycle 602. Although the passive matrix driving mechanism shown in FIG. 6 should be theoretically effective, since it will consider the arithmetic derivation relationship between the critical electric power i Vth and the driving voltage Vd as described in the above section A, FIG. 6 The mechanism does not solve the problem of reverse bias in non-switching pixels. The system-passive matrix EPD driving mechanism shown in Fig. 7 in which an intermediate P white I has been added to reduce the reverse bias in the non-switching pixels. The mechanism shown in Figure 7 begins with the same reset cycle 6〇2 shown in Figure 6. After the reset cycle % and before the drive cycle j裒7〇4, the intermediate phase 2 has been added, wherein the β drive cycle is the same as the interval 6〇4-6〇8 of FIG. During the period of 戸白丰和702, the row electrodes (e.g., row electrodes ci) are driven to 23 1301257 20V, and the column electrodes are driven to 1 〇v. By adding this intermediate stage, the process of converting the reset cycle to the drive cycle can be divided into two steps, thereby reducing the reverse bias effect. For example, we can compare the electrodes applied to the pixels (R2, C1) under the individual mechanisms shown in Figures 6 and 7. Under the mechanism of Figure 6, (R2, C1) will be subjected to a 30V negative bias during the final interval of the reset cycle (the line C1 voltage is 30V higher than the column R2 voltage), and then subjected to a 10V positive bias ( During interval 604, the voltage at R2 = iov, the voltage at ci = 〇v). The net conversion is 40ν. In contrast, under the mechanism of Figure 7, this conversion is divided into two steps, the first-person 20V transition from the final interval of the reset cycle to the intermediate phase 702 (from the end of the reset cycle) R2-C1=-30V becomes R2-C1=-10V in the intermediate stage; the second 20V transition enters the first part of the drive cycle 704 from the intermediate stage 702, which corresponds to Figure 6 The interval 604 (from R2_cl=_1〇v in the intermediate stage to R2_C1 = 10Vp at the initial portion of the drive cycle) divides the transition into two smaller steps to mitigate the reverse bias effect. The passive matrix EPD driving mechanism shown in the figure can further improve the mechanism shown in Figure 7. The mechanism shown in Figure 8 begins with the intermediate stage 702 of Figure 7, and assumes that two have been completed before the intermediate stage 7〇2: The reset cycle (eg, reset cycle 602, which is not shown in Figure 8). In the drive cycle following the intermediate phase 702, the "precipitation" phase has been added after the sweep and before the scan-column. The first column R1 scan interval 802 is followed by the precipitation stage 8〇4, at this stage All of the column and row electrodes are set to 0 volts to allow the particles to be deposited and brought together, and the inherent capacitance of the EPD cell structures is discharged before scanning. The second column R2 scan interval 806 is followed by a precipitation phase 808, and the third column R3 scan interval 8 1 〇 is followed by a precipitation phase 812. This inversion can be mitigated by discharging the inherent capacitance before scanning the following. In addition, the introduction of a precipitation stage can decompose the DC component applied to the cells, which is advantageous because, as described above, even if a DC component less than or equal to the nominal critical turtle pressure Vth is applied for a long period of time Uninterrupted may have a negative impact on image quality. Finally, in one embodiment, due to the physics between the particles and/or between the particles and the dielectric solvent and/or the EPD structure and materials Relationship between chemical, and/or electrical interactions, which allows the charged particles to be more closely packed together, making the units more complete and strong The passive-element EPd driving mechanism shown in Figure 9A is presented in a violent manner, and an additional intermediate stage has been added before and after scanning each column in the mechanism shown in Figure 8. An initial intermediate stage 902 of the first type is then applied. As shown in Figure 9A, in one embodiment, the first type intermediate stage 9〇2 is the same as the intermediate stage 702 of Figure 7 (i.e., there are multiple lines in 2) 〇v and plural are listed at 10V. In the mechanism shown in Fig. 9A, the first type intermediate stage 902 is followed by the first column ri scanning stage 904, squatting, followed by the second type intermediate Stage 906 (in one embodiment, as shown in Figure 9A, which includes setting the column electrodes to 1 〇v and setting the row electrodes to 0V), followed by a precipitation stage 908, at which stage The column electrodes and row electrodes of the 25 1301257 are set to 0V. The four phase cycles (stages 9〇2 to 9〇8) described above for the first column R1 can then be repeated for the second column R2 (stages 910 to 916) and the third column R3 (stages 918 to 924). In one of the embodiments, the introduction of the additional intermediate stages in the mechanism illustrated in Figure 9A causes each pixel to be subjected to a negative bias voltage (intermediate phase of the first type) and then to an equal magnitude. Negative bias voltages of opposite polarity (intermediate phase 2 of the second type) act in a staggered manner to reduce particle migration caused by long-term application of the same cross-bias voltage without interruption. As shown in the mechanism of Figure 8, the precipitation stage allows the particles to precipitate and build together. In addition, the addition of the second type of intermediate stages after scanning can reduce the bias in a mechanism (such as the mechanism shown in Figure 8, that is, the mechanism of adding a precipitation stage after scanning). The phenomenon that the voltage is lowered, thereby further reducing the induced reverse bias effect. The passive matrix EPE driving mechanism shown in Fig. 9B has been modified in the driving cycle shown in Fig. 6 (interval 6 〇 6 〇 8) so as to include a pre-drive pulse in scanning each column. If the data associated with the pixel is to apply the drive bias voltage to change the display state of the electrode, then a drive is used in the drive waveform shown in Figure 9B and a more complete description below. A pulse (referred to herein as a pre-driver pulse) drives the particles of the plurality of pixels in the scan column prior to the direction of the electrode, the direction being opposite to the direction in which the particles in the scan column are driven during scanning . After the pre-drive pulse has charged the pixel and inverted its polarity 26 to drive the particles to 1301257, then the forward drive pulse is applied to the designated electrode. In the exemplary drive waveform shown in Figure 9B, there is one such pre-driver pulse before each scan cycle. In the example of Fig. 9β, we assume that the pixels contain positively charged white particles suspended in a black dielectric solvent whose reset state is a black display state in which the charged particles have been driven to The position at or near the column (bottom) electrode, and the data to be written is that the pixels in the columns R1 and R3 in the row C1 are written in a white display state (at or near the row (top) electrode C1) The particles in column R2 will remain in the black display state. When a column (eg, R1) is addressed, the pixels in the scan column are first reset to a black display state during the pre-drive phase 942, during which the next column to be scanned (ie, R1) will be set to 〇V, while the non-scan columns R2 and R3 and the row electrodes (eg row electrode ci) will be set to 3〇v, resulting in a reverse drive (ie reset) bias condition being applied. The pixels to column R1, but without any bias, are applied to the pixels in the non-scanning column. Column R1 is then set to 30V during column R1 scan phase 944. During column R1 scan phase 944, row electrode C1 is set to 〇V, causing the associated pixel in row C1 column R1 to be driven to a white display state in accordance with the display data associated with that pixel. During the column R1 scan phase 944, the non-scan columns R2 and R3 are set to 10V to prevent the display state of the pixels in these non-scan columns from changing due to the biased relationship. Scan column R1 is followed by a pre-drive phase 946 of column R2, in which column R2 is set to 〇v, while columns R1 and R3 and row electrodes (e.g., C1) are
27 1301257 會被設為30V,使得會有一反向驅動偏壓條件被施加至列 R2的像素,將其驅動至黑色顯示狀態,同時會有一零偏壓 被施加至非掃描列中的像素。於列R2掃描階段948斯間 ,列電極R2會被設為30V,列電極R1及R3會被設為 1 0V ’維持該等非掃描列中之像素的顯示狀態,而且行電 極C1則會被設為20V,使得和列R2及行C1相關聯的像 素會雒持其黑色顯示狀態(依照上述的情況)。列R3前置驅 動階段950及掃描階段952與列R1對應的階段942及944 雷同,並且會導致和列r3及行C1相關聯的像素被驅動至 白色顯示狀態。 圖9C所示的係利用包含圖9B所示之前置驅動階段能 夠達成的誘發反向偏壓。實線所示的係前置驅動階段96〇 及驅動Ρό段962期間被施加至一像素的驅動電壓(偏壓), 虛線所示的則係該像素之帶電粒子上的有效偏壓。轉換期 間的反向偏壓效應會因下面兩項因素而降低:第一,該像 素上的反向電荷會抵消部份反向偏壓。第二,轉換中的電 壓較高(前置驅動階段期間的偏壓為_3〇ν,並且會於驅動期 間擺動至+30V),所以會更緊密地驅動及集結該等粒子, 使得該等粒子受到該反向偏壓效應的影響程度較低。 ^藉由將背景區域驅動至背景顏色來顯示影以女 效能 氏 於特定的被動矩陣EPD _,將帶電粒子從該等㈣ 單元之底部驅動至該等單元之頂端(觀看側)所 可能會比於反向方向中(也就是,從頂銼谷产* 们子間 π甲(也就疋,從頂端至底部)來驅動該 28 1301257 等粒子所需要的時間還長。舉例來說,於含有微杯電泳顯 , :單元的EPD中,於特定實施例中,基於下面的理由,將 、 π電顏料粒子驅動至該等微杯之非觀看側的時間可能會小 於將该等帶電顏料粒子從該非觀看側驅動至該觀看側所需 要的日守間,該等理由包含,但不限於:該等微杯的形狀; 省’I電溶劑及/或帶電顏料粒子的特徵及/或其間的動力特 性;及/或用於形成和該微杯相關聯之一種以上特徵的材料 〇 圖1 〇 Α及10Β所示的係一實施例中用來於一被動矩陣春 EPD上顯不一預期影像所使用的方式,其中帶電粒子被驅 離忒觀看表面的速度快於其從該非觀看側被驅動至該觀看 表面的速度。圖10A所示的係一欲於其上一圓形影像的被 動矩陣電泳顯示器1〇〇〇,該顯示器1〇〇〇中心處之虛線 1002係界定該虛線1〇〇2内部的影像區1〇〇4,以及該圓外 面的背景區1006,例如依照被提供給該顯示器1〇〇〇的影 像資料及/或相關的電路及/或處理元件。用於顯示此影像 的典型方式係先將所有的像素重置成黑色/背景狀態(將帶 ® 電粒子驅動至該等單元的非觀看側),然後再藉由將此等單 兀中之帶電粒子驅動至該觀看表面以便將該影像區(例如圓 10A之影像區10〇4)中之該等單元驅動至白色狀態。 圖10A中所示的起點並不會將所有的像素驅動至黑色/ 背景顏色狀態,取而代之的係,所有的像素都已被驅動至 一初始狀態,於該初始狀態中,該等帶電顏料粒子都係為 於該觀看表面處(有時候稱為「開啟」狀態)。從此狀態開 29 1301257 始’藉由將此等單元中的該等帶電顏料粒子驅離該觀看表 面,該背景區1006中的該等單元便會被驅動至黑色/背景 狀態,進而於該影像區1〇〇4中留下一由虛線1〇〇2所界定 之圓形的白色影像,如圖1 〇B所示。 雖然圖10A及10B中所示之圖解範例說明的係白色帶 電顏料粒子以及一具有黑色或其它背景顏色之溶劑,不過 ,於使用不同及/或多重顏色(例如用於提供一彩色顯示器) 之顏料粒子及/或溶劑的顯示器中亦可採用相同的技術。確 切地說,該項技術的優點係可使用於「向下」驅動(也就是 ,驅動至該顯示器之非觀看表面)帶電粒子所花費之時間少 於「向上」驅動(也就是,從底部或非觀看表面驅動至頂端 或觀看表面)帶電粒子所花費之時間的任何Epd中。 I使用一同線電阻器及/或短脈衝寬度來減低誘發反向 偏壓效應 上面章節B中所述之被動矩陣EPD驅動機制係藉由將 大電壓轉換分成兩道步驟來減低誘發反向偏壓效應;及/或 藉由包含一沉澱階段,讓造成該誘發反向偏壓效應的電容 可於該階段其間進行放電。吾人已經發現,若合適的話, 於上層或下層絕緣結構之前(也就是,於和該些結構相關聯 之電谷及電阻之前)加入一同線(串聯)電阻器便可進一步減 低該誘發反向偏壓效應,而不必讓與該單元相關聯之電容 在下個電壓轉換之前都變成完全充電狀態。圖UA所示的 係已經加入一同線電阻器之EPD單元的等效電路11〇〇。 比較圖11A與圖2B,兩者的等效電路皆相同,不過 1301257 ’圖UA中已經於和該EPD單元之上層絕緣結構相關聯 之電容及電阻之前加入一同線電阻器丨丨⑽。於其中一實施 例中,每個列電極、每個行電極、或兩種電極皆係透過: 同線電阻器被連接至該相關的驅動電路。於其中一實施例 中,該同線電阻器會有一離散部份位於該EpD電極基板之 上、或是位於上述的連接子/轉接子之上、或是位於二驅動 器1C電路板之上。於一實施例中,該同線電阻器可實施 於驅動器1C中,例如作為厚膜電阻器或薄膜電阻器。 圖11B所示的係一 4χ4陣列(或是某一陣列的一部份) ,其中已經於該等列電極與行電極以及其個別的驅動器之 間加入同線電阻器。該陣列111〇包括複數個行電極HP 以及複數個列電極1114。該等複數個行電極1112中每一 者皆會透過複數個行電極同線電阻器丨丨丨6中相對應的其 中一者被連接至其相關聯的行驅動器(圖中未顯示)。同樣 地,該等複數個列電極1114中每一者皆會透過複數個列 電極同線電阻器1118中相對應的其中一者被連接至其相 關聯的列驅動器(圖中未顯示p如上述,於替代的實施例 中,則僅有該等列電極或該等行電極可能會透過一同線電 阻益被連接至其個別的驅動器。 圖HC所示的係其中一實施例中所使用的替代排列, 於該替代排列中會提供一開關,以便能夠於驅動斯間從該 電路中移除該同線電阻器。圖nc所示的係一陣列114〇, 其包括列電極1142、1144、1146以及1148。和列電極 1142相關聯的係一同線電阻器1152與一開關1154。和列 31 130125727 1301257 will be set to 30V so that a reverse drive bias condition is applied to the pixels of column R2, driving it to the black display state, while a zero bias is applied to the pixels in the non-scan column. During the column R2 scanning phase 948, the column electrode R2 will be set to 30V, the column electrodes R1 and R3 will be set to 10 V 'to maintain the display state of the pixels in the non-scan columns, and the row electrode C1 will be Set to 20V so that the pixels associated with column R2 and row C1 will maintain their black display state (as per the above). Column R3 pre-driver stage 950 and scan stage 952 are identical to stages 942 and 944 corresponding to column R1 and cause the pixels associated with column r3 and row C1 to be driven to a white display state. The phase shown in Fig. 9C utilizes an induced reverse bias that can be achieved by including the pre-drive phase shown in Figure 9B. The solid line shows the driving voltage (bias) applied to one pixel during the pre-drive phase 96 〇 and the drive segment 962, and the effective bias on the charged particles of the pixel as indicated by the dashed line. The reverse bias effect during the transition is reduced by two factors: first, the reverse charge on the pixel cancels out some of the reverse bias. Second, the voltage during the conversion is high (the bias voltage during the pre-drive phase is _3 〇 ν and will swing to +30 V during the drive), so the particles will be driven and assembled more tightly, making these Particles are less affected by this reverse bias effect. ^ By driving the background area to the background color to display the effect of the female effect on the specific passive matrix EPD _, driving charged particles from the bottom of the (four) unit to the top (viewing side) of the units may be better than In the reverse direction (that is, it takes a long time to drive the particles such as 28 1301257 from the top 锉 * 们 们 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 28 28 28 28 28 28 28 28 28 28 28 28 28 Microcup electrophoresis, in the EPD of the unit, in a particular embodiment, the time for driving the π-electro-pigment particles to the non-viewing side of the microcups may be less than the charged pigment particles in the following reasons The non-viewing side is driven to the daytime waiting space required for the viewing side, and the reasons include, but are not limited to, the shape of the microcups; the characteristics of the 'I-electrolyte and/or charged pigment particles and/or the power between them Characteristics; and/or materials used to form one or more of the features associated with the microcups are shown in FIGS. 1A and 10B for use in a passive matrix spring EPD to display an expected image Way of use The charged particles are driven away from the viewing surface faster than they are driven from the non-viewing side to the viewing surface. Figure 10A shows a passive matrix electrophoretic display that is intended for its upper circular image. The dotted line 1002 at the center of the display 1 defines an image area 1〇〇4 inside the dotted line 1〇〇2, and a background area 1006 outside the circle, for example, according to being provided to the display 1〇〇〇 Image data and/or associated circuitry and/or processing components. The typical way to display this image is to first reset all pixels to a black/background state (with the ® particles driven to the non-viewing side of the unit) And then driving the charged particles in the unit to the viewing surface to drive the cells in the image area (e.g., image area 10〇4 of circle 10A) to a white state. The starting point of the display does not drive all pixels to the black/background color state. Instead, all pixels have been driven to an initial state in which the charged pigment particles are Viewing the surface (sometimes referred to as the "on" state). From this state, starting at 29 1301257, by driving the charged pigment particles in the cells away from the viewing surface, the cells in the background region 1006 Will be driven to the black/background state, leaving a circular white image defined by the dashed line 1〇〇2 in the image area 1〇〇4, as shown in Figure 〇B. Although Figures 10A and 10B The illustrated graphical examples illustrate white charged pigment particles and a solvent having a black or other background color, however, pigment particles and/or solvents used in different and/or multiple colors (eg, to provide a color display). The same technique can be used in the display. Rather, the advantage of this technique is that it takes less time to charge the particles for "downward" driving (ie, driving to the non-viewing surface of the display). Any Epd that drives up (ie, from the bottom or non-viewing surface to the top or viewing surface) the time it takes to charge the particles. I use a common line resistor and / or short pulse width to reduce the induced reverse bias effect. The passive matrix EPD driving mechanism described in Section B above reduces the induced reverse bias by dividing the large voltage conversion into two steps. The effect; and/or by including a precipitation stage, the capacitance causing the induced reverse bias effect can be discharged during this phase. We have found that, if appropriate, the in-line (series) resistor can be added to the upper or lower insulating structure (i.e., before the valleys and resistors associated with the structures) to further reduce the induced reverse bias. The voltage effect does not have to cause the capacitor associated with the cell to become fully charged before the next voltage transition. The system shown in Figure UA has been added to the equivalent circuit 11 of the EPD unit of the same line resistor. Comparing Fig. 11A with Fig. 2B, the equivalent circuits of the two are the same, but in the 1301257' UA, a line resistor 丨丨(10) has been added before the capacitance and resistance associated with the upper insulating structure of the EPD unit. In one embodiment, each column electrode, each row electrode, or both electrodes are permeable: a line-of-line resistor is coupled to the associated drive circuit. In one embodiment, the in-line resistor has a discrete portion located on the EpD electrode substrate, above the connector/switch, or on the second driver 1C board. In one embodiment, the in-line resistor can be implemented in driver 1C, for example as a thick film resistor or a thin film resistor. The array shown in Figure 11B is a 4 χ 4 array (or part of an array) in which in-line resistors have been added between the column electrodes and the row electrodes and their individual drivers. The array 111A includes a plurality of row electrodes HP and a plurality of column electrodes 1114. Each of the plurality of row electrodes 1112 is coupled to its associated row driver (not shown) through a corresponding one of the plurality of row electrode in-line resistors 丨丨丨6. Similarly, each of the plurality of column electrodes 1114 is coupled to its associated column driver through one of a plurality of column electrode in-line resistors 1118 (p is not shown) In an alternative embodiment, only the column electrodes or the row electrodes may be connected to their individual drivers through a common line resistor. Figure HC shows an alternative used in one embodiment. Arranging, in the alternative arrangement, a switch is provided to enable removal of the in-line resistor from the circuit between the drivers. Figure nc shows an array 114〇 comprising column electrodes 1142, 1144, 1146 And 1148. The in-line resistor 1152 and a switch 1154 associated with the column electrode 1142. and the column 31 1301257
電極1144相關聯的係一同線電阻器U56與一開關1158。 和列電極1146相關聯的係一同線電阻器1160與一開關 1162。和列電極1148相關聯的係一同線電阻器1164與一 開關1166。該等開關1154、1158、1162以及1166中每一 者皆具有兩個位置,於第一位置中,會於該驅動器至該電 極的路徑中納入該相關聯的同線電阻器;於第二位置中, 則會旁通該同線電阻器。圖中的開關n54、n62以及 1166係位於第一位置中;而圖中的開關n58則係於第二 位置中。於其中一實施例中,和一列電極相關聯的開關在 該相關列的驅動期間係位於第二(旁通)位置,使得不會於 該驅動器至該電極的路徑中納入該同線電阻器,因此讓電 阻器並不會出現而對跨越施加於該電泳分散劑之上的偏壓 電壓造成負面影響(也就是,減低該偏壓電壓);亦即,藉 由如果於該電路中納入該同線電阻器,所造成跨越該同線 電阻器所發生的電壓降。於其中一實施例中,當完成一特 殊列的掃描時,與該列相關聯的開關便會從第二位置改變 成第一位置,從而將該同線電阻器重新插入至該驅動器至 5亥電極的路梭中。此組態可運用同線電阻器的優點來降低 反向偏壓,但卻不會在該相關的電極被驅動時因納入該同 線電阻器而造成效能下降。當然,視特殊的被動矩陣EPD 的設計而定,亦可同時以行電極使用此組態(或是以行電極 取代而使用此組態)。The electrode 1144 is associated with a line-of-line resistor U56 and a switch 1158. Associated with column electrode 1146 is a line-of-line resistor 1160 and a switch 1162. Associated with column electrode 1148 is a line-of-line resistor 1164 and a switch 1166. Each of the switches 1154, 1158, 1162, and 1166 has two positions in which the associated in-line resistor is included in the path of the driver to the electrode; in the second position The same line resistor is bypassed. The switches n54, n62 and 1166 in the figure are in the first position; the switch n58 in the figure is in the second position. In one embodiment, the switch associated with a column of electrodes is in a second (bypass) position during actuation of the associated column such that the in-line resistor is not included in the path of the driver to the electrode, Therefore, the resistor does not appear to have a negative influence on the bias voltage applied across the electrophoretic dispersant (ie, the bias voltage is reduced); that is, by including the same in the circuit A line resistor that causes a voltage drop across the same-line resistor. In one embodiment, when a special column scan is completed, the switch associated with the column is changed from the second position to the first position, thereby reinserting the in-line resistor to the driver to 5 The electrode is in the road shuttle. This configuration can take advantage of the same-line resistors to reduce the reverse bias, but does not cause a drop in performance when the associated electrode is driven due to the inclusion of the same-line resistor. Of course, depending on the design of the particular passive matrix EPD, this configuration can also be used with row electrodes (or with row electrodes instead).
圖12所繪製的係圖11A中點A與點B的電壓與時間 的關係圖,其對應的係圖2A中所示之EPD單元中的點A 32 1301257 與點B。比較圖12與圖3,吾人便能發現,增加該同線電 阻益1102會減慢圖ha中所示之等效電路的電容ci與 C2的充電速度,因而會產生所減低的反向偏壓效應。不過 ’因為此外加的同線電阻器的關係,亦會因為跨越該同線 電阻器之電壓降的結果而減低電泳分散劑上的有效偏壓。 所以’必須最佳化該同線電阻器數值的選擇結果,使得該 數值夠高’足以降低該反向偏壓;但卻亦足夠低,能夠將 違有效偏壓保持在可接受的程度。該同線電阻器的電阻值 係取決於該顧示器的像素大小以及同列或同行上的像素數 罝。該分散劑與該等絕緣層的電氣特徵亦會影響該同線電 阻裔之阻值的選擇結果。於其中一實施例中,其數值係落 在百萬歐姆範圍中。 藉由阻止該等EPD單元結構之固有電容完全充電以減 低該反向偏壓效應所能採取的另一項措施則係縮減用來進 行驅動的脈衝寬度。圖13所示的係利用一較短脈衝寬度 便月b夠達成的降低反向偏壓的圖式。上方的電壓時間關係 圖1302繪製的係圖3中所示之關係圖的再生圖。下方的 電壓時間關係圖1304繪製的係利用一較短脈衝寬度的效 應示意圖’遠較短脈衝寬度在於降低該反向偏壓效應,但 卻不會允許於下個電壓轉換前與單元結構相關聯的電容(例 如圖11A的電谷C1與C2)被完全充電。於其中一實施例 中,可能必須使用更多數量的該等較短循環,以便依照該 影像資料將欲被切換的該等EPD單元驅動至新的狀態^該 脈衝寬度必須夠長,足以至少部份誘使該等粒子以該預期 33 1301257 的方向移動,不過還必須夠短,以減低反向偏壓。所以, 於其中一實施例中,該脈衝寬度的最佳值會與下面的因素 有關:粒子的移動率以及EPD的電氣特徵。 1加入一平衡階段用以將非掃描列中的單元還原成相 同的掃描初始狀態 如上述,在一組既定的條件下,能夠影響一 EPD單元 之實際臨界電壓的因素中其中一者便係該EPD單元的初始 狀態,尤其是該單元内之該等帶電顏料粒子的狀態。舉例 來說,如果該等帶電顏料粒子已經充份地沉澱且密集地集 結在該單元的底部,曝露出該介電溶劑的顏色,那麼實際 的臨界電壓將會大於該等帶電顏料粒子未充份沉澱且密集 集結實的臨界電壓。於後者的條件下,讓至少部份該等帶 電粒子朝上方(觀看)表面移動所需要的電壓便可能會低於 前者情形下所需要的電壓。 交叉偏壓效應能夠於對一列進行掃描前讓該列中部份 單元轉換至不同於同列中其它單元的初始狀態。如上述, 於掃描其它列時,可施加電壓至經選定的行電極,以便依 照設計結果讓與此等經選定之行電極相關聯之掃描中之個 別列單元改變或維持其狀態。即使被施加至此等單元的電 壓係該單元之公稱臨界電壓或以下,該些電壓仍然能夠讓 正好位於相同行中之非掃描列中的單元對其初始狀態作某 種程度的改變。也就是,即使交又偏壓電壓小於公稱臨界 電壓,該等受到此交叉偏壓電壓作用的單元仍然可能會部 份改變其初始狀態。舉例來說,在掃描前先將所有單=重 34 1301257 置成黑色/背景狀態(帶電顏料粒子位於該等單元之底部或 非觀看側之上)的實施例中,非掃描列中受到交又偏壓作用 的單元中的該等帶電顏料粒子的集結情形可能較不緊密, 而且可能會有部份粒子開始朝觀看表面移動。於後續的掃 描期間,此等初始狀態的變化可能會響應掃描期間所施加 之驅動電壓而造成非預期的變化,因而可能會造成不均句 的影像。 本發明揭示使用一平衡階段將非掃描列中的單元還原 成相同的初始狀態。圖14A所示的係一示範被動矩陣EpD 於掃描第一列R1時的圖式,該示範被動矩陣EpD包括一 3x3的EPD單元陣列(或包括一個或多個EpD單元的像素) 。於圖14A所示的範例中,藉由施加2〇v給行c i與Q 的行電極,同時施加掃描電壓Vd==3〇v給列R1,便可讓該 列之第單元與第一單元(也就是,單元(Rl、C1)與(R1、 C2))維持在初始的黑色/背景狀態(假設該範例中所有的單 元於進行掃描前都會被重置成該初始狀態)。於掃描期間將 仃C3的行電極固定在(^,使得跨越該單元所施加的驅動 電壓vd=30v,便可將列R1中之第三單元(單元(ri、c3)) 驅動至白色狀態。於如圖14A所示之列R1的掃描期間, 該等非掃描列中第三行C3中的單元(也就是,單元(R2、 C3)與(R3、C3))都會受到1〇v的正交叉偏塵(下方列電極電 壓比上方行電極電壓高出1〇v)的作用。如上述,此交又偏 壓(吾。人假設其低於該等單元的公稱臨界電壓)可能足以讓 .亥些單兀t #至少部份粒子以觀看表面的#向而遷徙,或 35 1301257 疋至v使其集結在一起的情形變得比較不緊密。請注意, 4非掃描列中的剩餘單元會受到10V的負交又偏壓(上方/ 订電極電壓比下方/列電極電壓高出10V)的作用,並不必 矛J用下文所述之平衡階段來抵消該交叉偏壓,因為其會傾 向於將該等粒子維持在該等EPD單元底部中其已被重置的 位置處。 圖所示的係其中一實施例中所使用的平衡階段, 用以將非掃描列中的單元還原成相同的掃描初始狀態。於 圖14B所示的平衡階段中,會於掃描列ri斯間施加一負 偏壓電壓給受到正交又偏壓作用的單元。如圖14B所示, 於其中一實施例中,藉由將於掃描列R1期間的非掃描列( 也就疋,列R2與R3)設為ον,同時施加1 〇γ給於掃描列 R1期間被设為0V的行(也就是,和列ri中於掃描列R1 期間從黑色/背景被切換成白色之單元相關聯的行)的行電 極’便可達成此目的。和於掃描列R 1期間被開啟之單元 無關聯的行(此情況中為行C1與C2)則會被設為〇v,其結 果係不會施加任何偏壓給列R2與R3中在掃描列尺丨期間 沒有受到一正交叉偏壓影響的單元,也就是,單元(R2、 Cl)、(R2、C2)、(R3、Cl)以及(R3、C2)。先前掃描過的 列R1會設為10V,以便確保沒有任何負交叉偏壓被施加 至該些單元’以確保該列中於掃描期間被開啟之該等單元 會保持完全開啟狀態(也就是’粒子位於觀看表面處),以 維持影像品質。被施加至列R1中該等未切換單元之丨〇v 的生成正偏壓會小於或等於臨界電壓Vth,而且被施加的 36 1301257 日守間不會太長以致於對影像品質造成負面影響。於其中一 實施例中’於下個掃描循環之前的重置循環期間,該些單 70將會連同所有其它單元都完全被重置成黑色/背景狀態。 圖14C所示的係掃描第二列R2的圖式。於圖中所示 的範例中’藉由施加ov給相關行C1,同時施加驅動電壓 Vd=30V給列R2,便可將該列中的第一單元(R2、ei)切換 成白色狀態。藉由施加2〇v給行C2與C3可讓列R2的剩 餘單元維持在黑色/背景狀態中。於圖丨所示的列r2的 掃描循環期間,列R3中的第一單元(也就是,單元(R3、 Cl))會受到lov的正交叉偏壓作用。圖14D所示的係其中 一實施例中所使用的平衡階段,用以抵消非掃描列R3中 單元上的正交又偏壓效應。如圖14B所示,非掃描列R3 會被設為ον,同時和於掃描列R2期間受到該正交叉偏壓 作用之單元相關聯的行(此情況中為行C1)係被設為請, 而剩餘的㈣缝設為0V。如此便會導致有—負偏職施 加至單元(R3、C1),從而將該單元重置為和單元(们、c2) 2 (R3、C3)於掃描列R3之前相同的初始狀態。於其中一 只也例中#圖14D所不,先前已經過掃描之列(例如列 R1)上的正父叉偏壓效應並不會被圖14D中所示的平衡階 段抵消’因為該列已經過掃描且該列中的單元將會於重置 循環期間被重置為共同的初始狀態,只要所有的列都已經 過知描且該顯不錢已經備妥可以顯示下個影像資料訊框 即會出現此動作。於其中一實施例中,如圖14D所示:所 有先前已經過掃描之列都祐母盔,叱上 J丨被认為10ν,以便確保該些列中 37 1301257 的單元會維持在0V偏壓處或10V正偏壓處,以便藉由避 免先前被切換成白色狀態或「開啟」狀態之單元中的帶電 粒子於該平衡階段期間遷徙遠離觀看表面,因而得以維持 影像品質。 ' 為達清楚瞭解的目的,雖然已經於前面對本發明作特 定的詳細說明,不過,吾人將會發現,亦可於申請專利範 圍的範疇内對其進行特定變化與修正。應該注意的係,有 許多替代方式來實現本發明的方法與設備。據此,該等實 施例係用於解釋而不在於限制,而且本發明並不僅限於本 文提出的細節,而可於申請專利範圍的範疇與等效範圍内 對其進行修正。 【圖式簡單說明】 (一)圖式部分 配合圖式閱讀詳細說明將會更容易瞭解本發明,其中 相同的元件符號表示的係相同的結構元件,而且其中:/、 圖1所示的係串訊現象。 圖2A所示的係一典型的電泳顯示器單元2⑼。 圖2B所示的係圖2A之單元2〇〇中介於點a與點c 之間部份的等效電路。 3所示的係誘發反向偏壓效應。 4A以及4別至你4所示的係一 2χ2的被動矩陣。 圖 圖 圖4C所示的係使用於行電極的「扇入」方式。 將 圖4D所不的係—連接子/轉接子,其係被配置成用以 任意形狀顯示器連接至一驅動器積體電路。 38 1301257 圖5所示的係用來說明其中一實施例中所使用之被動 矩陣驅動機制的組態與情況。 圖ό所示的係一基本被動矩陣電泳顯示器的驅動機制 圖7所示的係一被動矩陣電泳顯示器驅動機制,其中 已經加入一中間階段’用來減輕非切換像素中的反向偏壓。 圖8所示的係一被動矩陣電泳顯示器驅動機制,其可 進一步改進圖7所示之機制。 圖9Α所示的係一被動矩陣電泳顯示器驅動機制,其 中已經於圖8所不之機制中在掃描每列前後加入複數個中 間階段。 圖9B所示的係一示範驅動波形,其中此前置驅動脈 衝係位於每個掃描循環的前方。 圖9C所示的係利用包含圖9B所示之前置驅動脈衝能 夠達成降低之反向偏壓。 圖10A所示的係一欲於其上顯示一圓形影像的被動矩 陣電泳顯示器1000。 圖10B所示的係正被驅動 中的單元。 至黑色/背景狀態的背景區域 圖11A所示的係已經加入 單元的等效電路1100。 一同線電阻器之電泳顯示器 間 圖1 1B所示的係一 其中已經於該等列電 加入同線電阻器。 4X4陣列(其為某一陣列的一部份) 極與行電極以及其個別的驅動器之 39 1301257 圖11C所示的係其中一實施例中所使用的替代排列, 於该替代排列中會提供一開關,以便能夠於驅動期間從該 電路中移除該同線電阻器。 圖12所繪製的係圖11A中點A與點B的電壓與時間 的關係圖’其對應的係圖2A中所示之電泳顯示器單元中 的點A與點B 〇 圖13所示的係利用一較短脈衝寬度便能夠達成的降低 反向偏壓的圖式。 圖14A所不的係一示範被動矩陣電泳顯示器於掃描第 列R1時的圖式’該示範被動矩陣電泳顯示器包括一 3x3 的電泳顯不器單元陣列(或包括一個或更多之電泳顯示器單 元之像素)。 θ 14B所示的係其中一實施例中所使用的平衡階段, 用以將非掃㈣中的單元還原成相同的掃描初始狀態。 圖14C所示的係掃描第二列汉2的圖式。 圖14D所不的係其中一實施例中所使用的平衡階段, 用以抵消非掃播列]^ 2由tm _ 评彻幻尺3中早兀上的正交叉偏壓效應。 (二)元件代表符號 200 電泳顯示器單元 202 分散劑 204 帶電顧料粒子 206 有色介電溶劑 208 絕緣材料層 210 絕緣材料層 1301257 212 上方電極 214 下方電極 Cl 電容器 C2 電容器 R1 電阻器 R2 電阻器 440 行電極 442 筆直部份 444 列電極 446 扇入部份 448 驅動器積體電路 460 區段 462 行電極 464 連接子/轉接子 466 行驅動器積體電路 468 重疊區 472 列電極 474 連接子/轉接子 476 列驅動器積體電路 500 被動矩陣電泳顯示器陣列 502 列電極 5 04 列電極 506 列電極 508 行電極 41 1301257 510 行電極 512 行電極 514 電泳顯示元素 1000 被動矩陣電泳顯示器 1004 影像區 1006 背景區 1100 電泳顯示器單元 1102 同線電阻器 1110 陣列 1112 行電極 1114 列電極 1116 同線電阻器 1118 同線電阻器 1140 陣列 1142 列電極 1144 列電極 1146 列電極 1148 列電極 1152 電阻器 1154 開關 1156 電阻器 1158 開關 1160 電阻器 1162 開關 42 1301257 1164 電阻器 1166 開關Figure 12 is a graph of voltage versus time for point A and point B in Figure 11A, corresponding to point A 32 1301257 and point B in the EPD unit shown in Figure 2A. Comparing Fig. 12 with Fig. 3, we can find that increasing the same line resistance benefit 1102 will slow down the charging speeds of the capacitances ci and C2 of the equivalent circuit shown in Fig. ha, thus producing a reduced reverse bias. effect. However, because of the addition of the same-line resistor, the effective bias voltage on the electrophoretic dispersant is also reduced as a result of the voltage drop across the in-line resistor. Therefore, the selection of the value of the in-line resistor must be optimized such that the value is high enough to reduce the reverse bias; but low enough to maintain the off-duty bias to an acceptable level. The resistance value of the in-line resistor depends on the pixel size of the detector and the number of pixels in the same column or in the same row. The electrical characteristics of the dispersant and the insulating layers also affect the selection of the resistance of the in-line resistor. In one of the embodiments, the values fall within the range of one million ohms. Another measure that can be taken by preventing the inherent capacitance of the EPD cell structures from being fully charged to reduce the reverse bias effect is to reduce the pulse width used to drive. Figure 13 shows a pattern of reduced reverse bias that is achieved with a short pulse width. The voltage time relationship above is shown in Fig. 1302 as a regenerative map of the relationship diagram shown in Fig. 3. The voltage vs. relationship below is plotted in Figure 1304 using a shorter pulse width effect. The far shorter pulse width is to reduce the reverse bias effect, but it does not allow the cell structure to be associated before the next voltage conversion. The capacitance (e.g., the valleys C1 and C2 of Figure 11A) is fully charged. In one embodiment, it may be necessary to use a greater number of such shorter cycles in order to drive the EPD units to be switched to a new state in accordance with the image data. The pulse width must be long enough for at least The particles are induced to move in the direction of the expected 33 1301257, but must also be short enough to reduce the reverse bias. Therefore, in one of the embodiments, the optimum value of the pulse width is related to the following factors: the mobility of the particles and the electrical characteristics of the EPD. 1 adding an equilibration phase for restoring cells in the non-scanning column to the same initial state of scanning as described above, under one set of established conditions, one of the factors that can affect the actual threshold voltage of an EPD cell is The initial state of the EPD unit, especially the state of the charged pigment particles within the unit. For example, if the charged pigment particles have been sufficiently precipitated and densely packed at the bottom of the unit to expose the color of the dielectric solvent, the actual threshold voltage will be greater than the charged pigment particles are not sufficient. Precipitating and densely set the critical voltage. Under the latter conditions, the voltage required to move at least some of the charged particles toward the upper (viewing) surface may be lower than the voltage required in the former case. The cross-bias effect can cause some of the cells in the column to transition to an initial state different from other cells in the same column before scanning a column. As described above, when scanning other columns, a voltage can be applied to the selected row electrodes to change or maintain the state of the individual columns in the scan associated with the selected row electrodes, depending on the design. Even if the voltage applied to the cells is at or below the nominal threshold voltage of the cell, the voltages can cause some of the cells in the non-scanning columns that are in the same row to change their initial state to some extent. That is, even if the bias voltage is less than the nominal threshold voltage, the cells subjected to the cross-bias voltage may still partially change their initial state. For example, in an embodiment where all single = weights 34 1301257 are placed in a black/background state (charged pigment particles are located on the bottom or non-viewing side of the cells) prior to scanning, the non-scanning columns are subject to The agglomeration of the charged pigment particles in the biasing unit may be less tight and there may be some particles that begin to move toward the viewing surface. During subsequent scans, changes in these initial states may cause unintended changes in response to the drive voltage applied during the scan, which may result in an image of the uneven sentence. The present invention discloses the use of a balancing phase to restore cells in a non-scanning column to the same initial state. Figure 14A shows a schematic diagram of a passive matrix EpD for scanning a first column R1 comprising a 3x3 array of EPD cells (or pixels comprising one or more EpD cells). In the example shown in FIG. 14A, by applying 2〇v to the row electrodes of ci and Q, and simultaneously applying the scan voltage Vd==3〇v to the column R1, the first unit and the first unit of the column can be made. (That is, the cells (Rl, C1) and (R1, C2)) are maintained in the initial black/background state (assuming all cells in this example are reset to this initial state before being scanned). The third cell (cell (ri, c3)) in column R1 can be driven to a white state by fixing the row electrode of 仃C3 to (^ such that the driving voltage vd=30v applied across the cell during scanning. During the scanning of column R1 as shown in FIG. 14A, the cells in the third row C3 of the non-scanning columns (that is, the cells (R2, C3) and (R3, C3)) are subjected to a positive 1〇v. Cross-dust (the lower column electrode voltage is 1〇v higher than the upper row electrode voltage). As mentioned above, this crossover bias (I assume that it is lower than the nominal threshold voltage of these cells) may be sufficient. Some of the 兀 # # # 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少 至少It is subjected to a negative bias of 10V and a bias voltage (the upper/set electrode voltage is 10V higher than the lower/column voltage), and it is not necessary to use the balance phase described below to offset the cross bias because it tends to The particles are maintained at the bottom of the EPD unit where they have been reset. Shown is the balancing phase used in one of the embodiments to restore the cells in the non-scanning column to the same initial scanning state. In the balancing phase shown in Figure 14B, the scanning column ri is applied. A negative bias voltage is applied to the quadrature and biased cells. As shown in Figure 14B, in one embodiment, by non-scanning columns during the scan column R1 (i.e., columns R2 and R3) ) is set to ον, and 1 〇 γ is applied to the row set to 0 V during the scan column R1 (that is, the row associated with the cell in which the black/background is switched to white during the scan column R1 in the column ri) This can be achieved by the row electrode '. The row unrelated to the cell that was turned on during scan column R 1 (in this case, rows C1 and C2) will be set to 〇v, and the result will not be applied. The bias voltage is given to the cells in columns R2 and R3 that are not affected by a positive crossover bias during scanning of the scale, that is, cells (R2, Cl), (R2, C2), (R3, Cl), and (R3, C2). The previously scanned column R1 will be set to 10V to ensure that no negative cross bias is applied. The units 'to ensure that the cells in the column that are turned on during the scan remain fully open (ie, 'the particles are at the viewing surface) to maintain image quality. The unswitched cells are applied to column R1 The generated positive bias of v is less than or equal to the threshold voltage Vth, and the applied 36 1301257 day guard is not too long to negatively affect the image quality. In one embodiment, the next scan is performed. During the reset cycle before the cycle, the sheets 70 will be completely reset to the black/background state along with all other cells. The diagram shown in Figure 14C scans the pattern of the second column R2. In the example, by applying ov to the relevant row C1 while applying the driving voltage Vd=30V to the column R2, the first cell (R2, ei) in the column can be switched to a white state. The remaining cells of column R2 can be maintained in the black/background state by applying 2 〇 v to rows C2 and C3. During the scan cycle of column r2 shown in Figure ,, the first cell in column R3 (i.e., cell (R3, Cl)) is subjected to the positive cross bias of lov. Figure 14D shows the balancing phase used in one of the embodiments to counteract the quadrature and biasing effects on the cells in the non-scanning column R3. As shown in FIG. 14B, the non-scanning column R3 is set to ον, and the row associated with the cell subjected to the positive cross-biasing during the scanning of the column R2 (in this case, the row C1) is set as the request, The remaining (four) seams are set to 0V. This causes a negative bias to be applied to the unit (R3, C1), thereby resetting the unit to the same initial state as the unit (1, c2) 2 (R3, C3) before scanning column R3. In one of the examples, the positive parent fork bias effect on the previously scanned column (e.g., column R1) is not offset by the balancing phase shown in Figure 14D because the column has been After scanning and the cells in the column will be reset to the common initial state during the reset cycle, as long as all the columns have been known and the money is ready, the next image data frame can be displayed. This action will occur. In one of the embodiments, as shown in Fig. 14D: all the previously scanned arrays are wooed, and the upper J 丨 is considered to be 10 ν to ensure that the cells of the 37 1301257 in the columns are maintained at 0 V bias. At or a positive bias of 10V, image quality is maintained by avoiding the migration of charged particles in the cells previously switched to the white or "on" state away from the viewing surface during the balancing phase. For the purpose of achieving a clear understanding, although the present invention has been specifically described in detail above, it will be appreciated that certain changes and modifications may be made within the scope of the patent application. It should be noted that there are many alternative ways of implementing the methods and apparatus of the present invention. Accordingly, the present invention is to be construed as illustrative and not restrictive, and the invention is not limited to the details disclosed herein. BRIEF DESCRIPTION OF THE DRAWINGS The present invention will be more readily understood from the following detailed description of the drawings, wherein the same reference numerals represent the same structural elements, and wherein: Crosstalk phenomenon. Figure 2A shows a typical electrophoretic display unit 2 (9). 2B is an equivalent circuit of a portion between the point a and the point c in the unit 2A of FIG. 2A. The system shown in 3 induces a reverse bias effect. 4A and 4 are the passive matrix of 2χ2 shown in your 4th. Figure 4C shows the "fan-in" method used for row electrodes. The connector/connector, which is not shown in Figure 4D, is configured to be connected to a driver integrated circuit for any shape display. 38 1301257 Figure 5 is a diagram showing the configuration and situation of the passive matrix drive mechanism used in one of the embodiments. Figure 1 shows the driving mechanism of a basic passive matrix electrophoretic display. Figure 7 shows a passive matrix electrophoretic display driving mechanism in which an intermediate stage has been added to mitigate the reverse bias in non-switching pixels. Fig. 8 shows a passive matrix electrophoretic display driving mechanism which can further improve the mechanism shown in Fig. 7. Figure 9A shows a passive matrix electrophoretic display drive mechanism in which a plurality of intermediate stages have been added before and after scanning each column in the mechanism of Figure 8. Figure 9B shows an exemplary drive waveform in which the pre-drive pulse is located in front of each scan cycle. The reverse bias voltage can be achieved by using the pre-drive pulse shown in Fig. 9B as shown in Fig. 9C. Figure 10A shows a passive matrix electrophoretic display 1000 on which a circular image is to be displayed. The unit shown in Fig. 10B is being driven. Background area to black/background state The system shown in Fig. 11A has been added to the equivalent circuit 1100 of the unit. The electrophoretic display between the same line resistors is shown in Figure 1 1B. One of the lines has been added to the same line resistor. 4X4 array (which is part of an array) pole and row electrodes and its individual drivers 39 1301257 Figure 11C is an alternative arrangement used in one of the embodiments, in which an alternative arrangement would be provided A switch is provided to be able to remove the in-line resistor from the circuit during driving. FIG. 12 is a diagram showing the relationship between voltage A and point B in FIG. 11A in FIG. 11A. FIG. 2 corresponds to the point A and the point B in the electrophoretic display unit shown in FIG. 2A. A pattern of reduced reverse bias that can be achieved with a shorter pulse width. 14A is a diagram of an exemplary passive matrix electrophoretic display when scanning the column R1. The exemplary passive matrix electrophoretic display includes a 3×3 array of electrophoretic display units (or one or more electrophoretic display units). Pixel). θ 14B is an equilibrium phase used in one of the embodiments to restore cells in the non-sweep (four) to the same initial state of scanning. The diagram shown in Fig. 14C scans the pattern of the second column Han-2. Figure 14D is a phase of the balance used in one of the embodiments to counteract the non-scanning sequence of the positive cross-bias effect on the early 由3 by tm_. (2) Component Representation Symbol 200 Electrophoretic Display Unit 202 Dispersant 204 Charged Particles 206 Colored Dielectric Solvent 208 Insulation Material Layer 210 Insulation Material Layer 1301257 212 Upper Electrode 214 Lower Electrode Cl Capacitor C2 Capacitor R1 Resistor R2 Resistor 440 Row Electrode 442 straight portion 444 column electrode 446 fan-in portion 448 driver integrated circuit 460 segment 462 row electrode 464 connector/conductor 466 row driver integrated circuit 468 overlap region 472 column electrode 474 connector/conduit 476 column driver integrated circuit 500 passive matrix electrophoretic display array 502 column electrode 5 04 column electrode 506 column electrode 508 row electrode 41 1301257 510 row electrode 512 row electrode 514 electrophoretic display element 1000 passive matrix electrophoretic display 1004 image area 1006 background area 1100 electrophoresis Display unit 1102 Same-line resistor 1110 Array 1112 Row electrode 1114 Column electrode 1116 Same-line resistor 1118 Same-line resistor 1140 Array 1142 Column electrode 1144 Column electrode 1146 Column electrode 1148 Column electrode 1152 Resistor 1154 Switch 1156 Resistor 1158 Switch 1160 Resistor 1162 Switch 42 1301257 1164 Resistor 1166 Switch
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CN103229096A (en) * | 2010-07-14 | 2013-07-31 | 三菱铅笔株式会社 | Electromigration display device and drive method thereof |
TWI406232B (en) * | 2009-09-04 | 2013-08-21 | Chunghwa Picture Tubes Ltd | Electrophoretic display |
CN104050932A (en) * | 2013-03-13 | 2014-09-17 | 达意科技股份有限公司 | Electrophoretic display device for reducing passive matrix coupling effect and method thereof |
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TWI406217B (en) * | 2008-12-29 | 2013-08-21 | Prime View Int Co Ltd | Displaying method for electrophoretic display and corresponding electrophoretic display |
TWI550580B (en) * | 2012-09-26 | 2016-09-21 | 達意科技股份有限公司 | Electro-phoretic display and driving method thereof |
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Publication number | Priority date | Publication date | Assignee | Title |
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TWI406232B (en) * | 2009-09-04 | 2013-08-21 | Chunghwa Picture Tubes Ltd | Electrophoretic display |
CN103229096A (en) * | 2010-07-14 | 2013-07-31 | 三菱铅笔株式会社 | Electromigration display device and drive method thereof |
CN104050932A (en) * | 2013-03-13 | 2014-09-17 | 达意科技股份有限公司 | Electrophoretic display device for reducing passive matrix coupling effect and method thereof |
TWI502573B (en) * | 2013-03-13 | 2015-10-01 | Sipix Technology Inc | Electrophoretic display capable of reducing passive matrix coupling effect and method thereof |
US9262973B2 (en) | 2013-03-13 | 2016-02-16 | Sipix Technology, Inc. | Electrophoretic display capable of reducing passive matrix coupling effect and method thereof |
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