TW516013B - Driving method and device of plasma display panel - Google Patents
Driving method and device of plasma display panel Download PDFInfo
- Publication number
- TW516013B TW516013B TW89100333A TW89100333A TW516013B TW 516013 B TW516013 B TW 516013B TW 89100333 A TW89100333 A TW 89100333A TW 89100333 A TW89100333 A TW 89100333A TW 516013 B TW516013 B TW 516013B
- Authority
- TW
- Taiwan
- Prior art keywords
- voltage
- electrode
- waveform
- mentioned
- slope
- Prior art date
Links
Landscapes
- Control Of Indicators Other Than Cathode Ray Tubes (AREA)
- Control Of Gas Discharge Display Tubes (AREA)
Abstract
Description
516013 五、發明說明α) 本發明係有關於一種電漿顯示面板(plasma di spl ay panel,PDP)的驅動方法和裝置,特別是能夠對於電漿顯 示面板,降低其重置期間(reset period)中放電 (discharge)操作所造成的背景閃爍(backglow)現象。 PDP主要是利用電極放電累積電荷的方式進行顯示, 由於具有大螢幕、高容量以及能夠顯示全彩(full — c〇l〇r) 影像’是未來最具潛力的平面顯示器。以下就PDP的基本 原理和操作方式加以說明。 第1圖表示習知技術PDP中單元(cel 1)結構的側視剖面 圖。如圖所示,PDP主要是由兩塊玻璃基板1和7及其上構 件所組成’在玻璃基板1和7之間的空腔(C a V丨t ^ )則填入惰 性氣體’如N e、X e。在玻璃基板1上包括維持電極 (sustain electrodes)X和掃描電極Yi(彼此平行延伸)、 J丨電層3以及保護膜(pr〇tective 。在玻璃基板7上 貝1包括位址電極(address e lectr〇des)Ai和其上的螢光材 料9 _在母個單元的四周則以分隔牆(p & μ丨七丨〇 n w a 1 1 ) 8加 以隔離。因此’在每個單元1 〇中包含三個電極,分別是平 行的維持電極X和掃描電極Yi以及橫跨其上之位址電極Ai 〇 第2圖表示利用第i圖所示之PDP所組成之電漿顯示器 白塊圖。如圖所示,PDP 1〇〇是由彼此平行的掃描電極 口 n以^及維持電極X,以及橫跨其上之位址電極A1〜Am所 ^ Ϊ 1單元1 〇之位置則如圖中所示,而每個單元之間則是 圖中所示之分隔牆8加以隔離。另外,電漿顯示器尚516013 V. Description of the invention α) The present invention relates to a driving method and device for a plasma display panel (PDP), in particular, it can reduce the reset period of the plasma display panel. The background flicker caused by the discharge operation. PDP is mainly used to display the accumulated charge through electrode discharge. Due to its large screen, high capacity and ability to display full-color images, it is the most promising flat display in the future. The basic principles and operation methods of the PDP are explained below. Fig. 1 is a side sectional view showing the structure of a cell (cel 1) in a conventional PDP. As shown in the figure, the PDP is mainly composed of two glass substrates 1 and 7 and their upper components. The cavity (C a V 丨 t ^) between the glass substrates 1 and 7 is filled with an inert gas such as N e, X e. The glass substrate 1 includes sustain electrodes X and scan electrodes Yi (extending in parallel with each other), an electric layer 3, and a protective film. The glass substrate 7 includes an address electrode (address e). lectrdes) Ai and the fluorescent material 9 _ are separated by a dividing wall (p & μ 丨 七 丨 〇nwa 1 1) 8 around the parent unit. Therefore, 'in each unit 10 Contains three electrodes, namely sustain electrode X and scan electrode Yi in parallel and address electrode Ai across it. Figure 2 shows a white block diagram of a plasma display using the PDP shown in Figure i. As shown in the figure, the PDP 100 is formed by the scan electrode port n and the sustain electrode X parallel to each other, and the address electrodes A1 to Am across it. The position of the unit 1 〇 is shown in the figure. And each unit is isolated by the partition wall 8 shown in the figure. In addition, the plasma display is still
516013516013
包括控制電路(contr〇1 cirCUit)11〇、γ掃描驅動器(γ s c a n d r i v e r ) 1 1 2、維持驅動器(χ d r i v e r ) 1 1 4以及位址驅 動态(address driver) 1 16。控制電路i 10根據外部所提供 之時脈信號CLOCK、資料信號DATA、垂直同步信號VSYNC以' 及水平同步信號HSYNC,產生各驅動器所需要之時序資訊 。其中時脈信號CLOCK表示資料傳輸時脈,資料信號data 表示顯示資料,垂直同步信號VSYNC和水平同步信號bHsYNc 則是用以定義單一晝框(frame)和單一掃描線(scanning I inj)之時序。控制電路丨丨〇將顯示資料和時脈送到位址驅 動器11 6 ’並且將相關之晝框控制時序送至γ掃描驅動器 II 2和維持驅動器丨丨4。必須注意的是,顯示相關資料係由 控制電路11〇送至位址驅動器116,並且在y掃描驅動器n2 ,序掃描各掃描電極Y1〜Yrl時,透過位址電極^^111將顯示 資料寫入各單元中。其詳細顯示動作和各電極所需要之控 制信號,則配合第3圖和第4圖說明如下。 工 第3圖表示習知技術驅動pdp顯示一畫框(f rame )之動 作不意圖。如圖所示,每一個畫框分割成8個次圖場 (sub-field)SF1〜SF8。必須注意的是,此處次圖場的意義 與傳統陰極射線管(cathode ray tube,CRT)中的圖場 (field)不同,傳統CRT中的圖場是分別對於奇偶數掃$描線 進行掃描顯示,而PDP之圖場則是對於全部掃描線顯示不 同的灰階位準(gray scale)。每個次圖場由三個操作動作 期間所組成,分別為重置期間(reset peri〇d)R1〜R8、寫 入期間(address period)Al〜A8以及維持時間(sustainIncluding control circuit (contr01 cirCUit) 11, γ scan driver (γ s c a n d r i v e r) 1 1 2, maintain driver (χ d r i v e r) 1 1 4 and address driver dynamic (address driver) 1 16. The control circuit i 10 generates timing information required by each driver according to a clock signal CLOCK, a data signal DATA, a vertical synchronization signal VSYNC, and a horizontal synchronization signal HSYNC provided externally. The clock signal CLOCK indicates the data transmission clock, the data signal data indicates the display data, and the vertical synchronization signal VSYNC and the horizontal synchronization signal bHsYNc are used to define the timing of a single day frame (scanning I inj). The control circuit 丨 丨 sends the display data and clock to the address driver 11 6 ′ and sends the relevant day frame control timing to the γ scan driver II 2 and the sustain driver 丨 4. It must be noted that the display-related data is sent from the control circuit 110 to the address driver 116, and when the y scan driver n2 sequentially scans each scan electrode Y1 ~ Yrl, the display data is written through the address electrode ^^ 111 In each unit. The detailed display of the operation and the control signals required for each electrode are described below with reference to Figures 3 and 4. Figure 3 shows that the conventional technology drives the PD to display a frame (frame). As shown in the figure, each picture frame is divided into 8 sub-fields SF1 to SF8. It must be noted that the meaning of the secondary field here is different from the field in the traditional cathode ray tube (CRT). The field in the traditional CRT is to scan and display the odd and even scan lines. The field of the PDP displays different gray scales for all scan lines. Each sub-field is composed of three operation periods, which are reset period R1 ~ R8, write period (address period) Al ~ A8, and sustain time (sustain
第5頁 五、發明說明(3) 7二31/,8以;置期間是用來清除前-次圖場_ '餘之,、u及在每個單元中留下-定數量之壁電荷( =/二寫人期間則是透過位址放電(3(1(11^33 ^Fge而要顯不之單元中(即呈〇n狀態)累積壁電行 以是在已透過位址放電累積壁電荷的單上 、 電(sustam discharge)進行顯示。其中,重 期間R1〜R8和維持期間S1〜S8是同時處理pDp上的全部單 i而寫^期間A1〜A8則是依序對於各掃描電極Y1〜γη上的各 =寫入動作。另外,顯示亮度是與維持期間W〜S8 士、又、正比。在第3圖的例子中,各次圖場SF卜SF8中維 持期間S1〜S8的長度可以設為1 ·· 2 ·· 4 ·· 8 : 16 · 32 . 64 : 1 28之比例,藉此實現2 56灰階。 · 口第4圖表示習知技術在單一次圖場中各電極上控制信 號之時序圖,其中位址電極4丨上的信號是由位址驅動器 11 6所產生,維持電極χ上的信號是由維持驅動器11 4所產 生,掃描電極Υ1〜γη上的信號是由掃描驅動器丨丨2所產生。 如圖所不,每個次圖場是包含重置期間、寫入期間和維持 期間。以下詳細說明各期間信號波形以及其所造成的動作 在重置期間的時間點a,掃描電極Yi〜Yfl設為〇ν,維持 電極X上則送入電壓值為vs+vw的寫入脈波(write pulse)、 2〇L ’ β其中電壓值VS + VW大於維持電極x和Yi之間的放電啟Page 5 V. Explanation of the invention (3) 7: 2 31 /, 8; The setting period is used to clear the previous-second field _ 'remainder', u, and leave a fixed amount of wall charge in each unit (= / The period of writing people is discharged through the address (3 (1 (11 ^ 33 ^ Fge and the unit to be displayed is in the state of 0n). The wall charges are displayed on a single charge and a single charge (sustam discharge). Among them, the heavy periods R1 to R8 and the sustaining periods S1 to S8 process all the single i on pDp at the same time, and the writing periods A1 to A8 are sequentially performed for each scan. Each of the electrodes Y1 to γη = write operation. In addition, the display brightness is proportional to the sustain period W to S8. In the example in FIG. 3, the sustain periods S1 to S8 in each field SF and SF8. The length can be set to 1 ·· 2 ·· 4 ·· 8: 16 · 32. 64: 1 28 ratio to achieve 2 56 gray levels. · Figure 4 shows the conventional technology in a single field Timing chart of control signals on each electrode, where the signal on the address electrode 4 丨 is generated by the address driver 116, and the signal on the sustain electrode χ is controlled by the sustain driver 11 4 The signals on scan electrodes Υ1 ~ γη are generated by the scan driver 丨 2. As shown in the figure, each sub-field includes a reset period, a write period, and a sustain period. The signal waveforms of each period are described in detail below. And at the time point a during the reset period, the actions caused by the scan electrodes Yi ~ Yfl are set to ν, and the sustain electrodes X send write pulses with a voltage value of vs + vw, 2〇 L 'β where the voltage value VS + VW is greater than the discharge start between the sustain electrodes x and Yi
始電墨(discharge start voltage)。因此,在維持電極X 和掃描電極Yi之間出現全域寫入放電(t〇tal write 516013 五、發明說明(4) diSCharge)W。此放電過程會在維 在掃描電極y i上累積了正電離芊山才上累積負電何, 雷雜、一::丄 子。由於累積的負電荷和正 =子所造成之電場會抵消掉維持電極之 全域寫入放電W的時間很短。 差 □ 接著在時間點b,維持電Μ M ^ ^ # ^ ^(sustaL p^ 6): 值必彡f大;^掃π # . 持電極間電荷所造成之電壓 但乂 /貝大於抑描電極γ i和χ之間 維持電極X和掃描電極Yi之F1 , σ電反。因此在 susta.n d1scharge)S〇rit ft M'^^t(t〇tal ,在維持電極x上會累積正電】電過程相反 積了負電荷。 宅離子,在掃描電極Yi上會累 接著在時間點c,掃描電極 則送入電壓值低於VS的清除 δ又為0V,而維持電極X上 在位址電極Ai上也可以送入/ (eraSe Pulse) 203,同時 是用來中和(neUtralize)部分電的位址^f。/除脈波2〇3 Υιι上留下所需要的壁 電何,取後在知描電極γι〜 能夠以&侗μ t π 電何。此壁電荷讓後續寫入期間中, 月匕刃以較低的電壓值進行寫入動 d门甲 接著開始寫入期間。首本 掃描電如拉至電壓值極X和 於各掃描電極Y1〜Yn送入掃描者攸k間點e開始,依序對 在位址電極Ai上送入電壓值Y皮(SCan pulse)2〇4,同時 線中的單元是設為0N時,則:=址脈波。冑某個掃描 應的顯示資料寫人此單元中5生寫人放電’ &就是將對 516013 五 、發明說明(5) 在f成所有掃描電極Y1〜Yn的掃描後 間。〜各維持電極χ和掃描電極η設為〇、 士持期 錯的方式(¥間點f和時間點g),對維耆u交 Yi送入相同電壓值的維持脈波2〇5。此時° v描電極 入on資料的單元即會顯示亮度。必須說明的是入期間被寫 明之驅=號二形僅為一範例’ *實際應 =說 與此一耗例不同,但是基本原理是一致的。 皮形可能 如前所述’維持期間的長度與示的 假設’個晝框中包含51。次維持放電週期(以 放電)’則在次圖場sn〜SF8中維持 兩: 配置為2、4、8、16、32、64、128、256。因此里,了一以二別 框顯示期間用於維持期間之放電次數為5ΐ〇χ2 = ι〇2〇。: 部分的放電操作是顯示影像的主要部分。 另一方面,實際上在重置期間行了2到3個放電周 期’例如全域寫入放電、全域維持放電以及清除放電,以 便均綱壁電荷:不$,這些重置期間内之放電動作也 會產生壳度,同時會略咼於在維持期間放電動作所產生亮 度。大略來况,重置期間三次放電所產生的亮度大約等於 維持期間五次放電所產生的亮度。因此在pDp上最大亮度 和最小亮度的比率大約為1 0 20:5 x 8 = 26:1 ,其對應於黑色 (black)的亮度。因此,在重置期間放電所產生的亮度是 愈低愈好,如此才能夠改善黑色晝質。黑色晝質是影像顯 示的重要參數之一,因此降低重置期間放電動作所造成之 亮度效應為必須解決的重要課題。Discharge start voltage. Therefore, a global write discharge occurs between the sustain electrode X and the scan electrode Yi (total write 516013 V. Description of the invention (4) diSCharge) W. This discharge process will accumulate a positive ionization on the scan electrode y i and a negative charge will accumulate on the mountain, Lei Za, 1 :: Xunzi. The electric field caused by the accumulated negative charges and positive ions will offset the global write discharge W of the sustain electrodes for a short time. Difference □ Then at time b, maintain the voltage MM ^ ^ # ^ ^ (sustaL p ^ 6): The value must be 彡 f; ^ Scanπ #. Hold the voltage caused by the charge between the electrodes but 乂 / 乂 is larger than the suppression Between the electrodes γ i and χ, F1, σ of the sustain electrode X and the scan electrode Yi are electrically reversed. Therefore, in susta.n d1scharge) Sortrit ft M '^^ t (t〇tal, a positive charge will be accumulated on the sustain electrode x) the negative process will accumulate a negative charge. House ions will be accumulated on the scan electrode Yi At time point c, the scan electrode sends a clear voltage δ lower than VS to 0V, and the sustain electrode X can also send / (eraSe Pulse) 203 on the address electrode Ai, which is also used to neutralize (NeUtralize) The address of part of the electricity ^ f. / In addition to the pulse wave 2 0 3 留下 ιι leaves the required wall electric Ho, after taking out the electrode γι ~ can be & 侗 μ t π electric Ho. This wall The charge allows the moon dagger to write at a lower voltage during the subsequent writing period, and then starts the writing period. The first scanning power is pulled to the voltage value X and sent to each scanning electrode Y1 ~ Yn. Starting from the point e between the scanner and the scanner, a voltage value Y skin (SCan pulse) 204 is sequentially sent to the address electrode Ai, and when the cell in the line is set to 0N, then: = address pulse胄 The display data of a scan should be written by the 5 writers in this unit. '&Amp; It will be on 516013 V. Description of the invention (5) All scans at f After scanning of the electrodes Y1 to Yn. ~ Each sustain electrode χ and scan electrode η are set to 0, and the holding period is wrong (¥ interval f and time g), and the same voltage value is input to Yi The sustaining pulse wave is 205. At this time, the unit where the electrode is turned on will display the brightness. It must be noted that the drive during the entry period = No. The shape is only an example '* Actual should = say and This case is different, but the basic principles are the same. The skin shape may be as described earlier. The length of the sustain period and the hypothesis shown include 51 in the day box. The sustain discharge period (by discharge) is shown in the figure below. In the field sn ~ SF8, two are maintained: the configuration is 2, 4, 8, 16, 32, 64, 128, 256. Therefore, the number of discharges for the sustain period during the display period in a two-frame box is 5ΐ〇χ2 = ι 〇2〇 .: Part of the discharge operation is the main part of the display image. On the other hand, actually, 2 to 3 discharge cycles are performed during the reset period, such as global write discharge, global sustain discharge, and clear discharge, so that Gang wall charge: not $, the discharge action during these reset periods will also produce shell, It will be slightly less than the brightness generated by the discharge during the sustain period. Roughly speaking, the brightness generated by three discharges during the reset period is approximately equal to the brightness generated by five discharges during the sustain period. Therefore, the ratio of the maximum brightness to the minimum brightness on pDp Approximately 1 0 20: 5 x 8 = 26: 1, which corresponds to the brightness of black. Therefore, the lower the brightness generated by the discharge during the reset, the better, so that the black day quality can be improved. Black Day quality is one of the important parameters of image display, so reducing the brightness effect caused by the discharge action during resetting is an important issue that must be resolved.
、參明說明(6) 有鑑於此,本發明的主要目 濟板的驅動方法和裝i 0 ’在於提供-種電漿顯 的放電操作對於影像亮度影響=每一次圖場重置期 根據上述之目的,本發明提出一種 動方法,電漿顯示面板上包含複 、員不面板之驅 #描電極,以及橫跨維持:::平持電極 和掃描電極之間的放::用二透:維持電 麼電荷,全Β皆, 卞座生電漿顯不面板中各單元 …再以較小斜率波形從=電=昇工 #又小斜率波形可以是漸增或漸減的 域寫入腑油上…α ^ ^ ^ 威 換 异 電壓 /从,入,人v J Μ疋斯增或漸減的變速 f·上昇ί第1 =波也可以利用較小斜率波形,由第-電 ΐ多第:電’再利用較大斜率波形,由第二電壓上 并ϋ!以較大斜率波形提昇電壓的部分可以大量 系二以較小斜率波形提昇電壓的部分則可以避 免邊成過強的亮度,影響顯示品質。 避 另,,本發明提出一種電漿顯示面板之驅動裝置,波 s料;ϋ電路二用以接收外部之顯示資料及其相關時序 7 X、驅動哭驅動态,耦接於控制電路,用以驅動位址電極 在重詈I态,、耦接於控制電路,用以驅動維持電極,其中 雷κ 4 ^門送入全域寫入脈波至維持電極,用以透過維梏 各抑—口 ν描電極之間的放電動作產生上述電漿顯示面中 土电何。此全域寫入脈波係以較大斜率波形由第 第9頁 516013 五、發明說明(7) 一電壓上昇至第二電壓,再以較小斜率波形從第二電壓上 昇至第三電壓,或是以較小斜率波形由第一電壓上昇至第 二電壓,再以較大斜率波形由第二電壓上昇至第三電壓; 以及Y掃描驅動器,耦接於控制電路,用以驅動上述掃描 電極。 另外,本發明提出一種電漿顯示面板之驅動裝置,其 不同處在於X驅動器和Y掃描驅動器。X驅動器在重置期間 送入全域寫入脈波之第一成分脈波至上述維持電極,上述 全域寫入脈波之第一成分脈波係以一較大斜率波形由第一 電壓上昇至第二電壓。Y掃描驅動器則在重置期間送入全 域寫入脈波之第二成分脈波至掃描電極,其以一較小斜率 波形下降至第二電壓,藉此維持電極和掃描電極之間的全 域寫入脈波所造成之放電動作,產生電漿顯示面板中各單 元之壁電荷。 圖式之簡單說明: 為使本發明之上述目的、特徵和優點能更明顯易懂, 下文特舉一較佳實施例,並配合所附圖式,作詳細說明如 下: 第1圖表示習知技術電漿顯示面板(PDP)中單元(cell) 結構之側視剖面圖。 第2圖表示利用第1圖所示之電漿顯示面板所組成之電 漿顯示器的方塊圖。 第3圖表示習知技術中驅動電聚顯示面板顯示一晝框(6) In view of this, in view of this, the driving method and device of the main objective board of the present invention is to provide-the effect of a plasma display discharge operation on the brightness of the image = each field reset period according to the above For the purpose of the present invention, the present invention proposes a moving method, and the plasma display panel includes a tracing electrode and a tracing electrode, and maintains between ::: the flat electrode and the scanning electrode. To maintain the electric charge, all B are, all units in the plasma plasma display panel ... then use a smaller slope waveform from = 电 = 升 工 # and a small slope waveform can be written in a gradually increasing or decreasing field. Up ... α ^ ^ ^ Changing the voltage / slave, input, person v J Μ 疋 increases or decreases the speed of the variable speed f. Rising 1 = wave can also use a smaller slope waveform, from the first to the second: Electricity 'reuses the larger slope waveform, which is paralleled by the second voltage! The part that boosts the voltage with the larger slope waveform can be tied to a large number. The part that boosts the voltage with the smaller slope waveform can avoid the edge becoming too bright, which affects Display quality. To avoid another problem, the present invention provides a driving device for a plasma display panel, which can be used as a signal source; circuit two is used to receive external display data and its related timing sequence 7 X, drive driving state, and is coupled to the control circuit for The driving address electrode is in the I state, and is coupled to the control circuit to drive the sustain electrode. The thunder κ 4 ^ gate sends a global write pulse to the sustain electrode, which is used to pass through the gate. The discharge action between the drawing electrodes generates the geoelectricity in the plasma display surface. This global write pulse wave has a larger slope waveform from page 9 516013. 5. Description of the invention (7) A voltage rises to the second voltage, and then rises from the second voltage to the third voltage with a smaller slope waveform, or The waveform is increased from the first voltage to the second voltage with a smaller slope waveform, and then increased from the second voltage to the third voltage with a larger slope waveform; and a Y-scan driver is coupled to the control circuit to drive the scan electrode. In addition, the present invention proposes a driving device for a plasma display panel, which differs in an X driver and a Y scanning driver. The X driver sends the first component pulse of the global write pulse to the sustain electrode during the reset period. The first component pulse of the global write pulse rises from the first voltage to the first voltage with a large slope waveform. Two voltages. The Y scan driver sends the second component pulse of the global write pulse to the scan electrode during the reset period, which drops to a second voltage with a smaller slope waveform, thereby maintaining the global write between the electrode and the scan electrode. The discharge action caused by the incoming pulse wave generates wall charges of each unit in the plasma display panel. Brief description of the drawings: In order to make the above-mentioned objects, features, and advantages of the present invention more comprehensible, a preferred embodiment is given below and described in detail with the accompanying drawings as follows: FIG. 1 shows the conventional knowledge Side sectional view of a cell structure in a technical plasma display panel (PDP). Fig. 2 is a block diagram of a plasma display device using the plasma display panel shown in Fig. 1. FIG. 3 shows driving a polycondensation display panel to display a day frame in the conventional technology.
516013 五、發明說明(8) 之示意圖。 第4圖表示習知技術中在單— ^ ^ # t ^ ^ „ t ^Υ〇 ^ ^ ^ ^ 。 1彡上控制h號之時序圖 第5圖表示本發明第一實施例 ’各電極(包含位址電才紹、維持圖=之重置期間 控制信號之時序圖。 、電極X和知描電極Y i )上 第6圖表示本發明第一實施例 装置的方塊圖。 電水”、、員不面板之驅動 第7圖表示本發明第二實施例中 示意圖。 j干王域寫入脈波之波形 |示本發明第三實施例中在次圖場 間,各電極(包含位址電極A i、維# 置^ 上控制信號之時序圖。 、*持電《和掃描電極Yl) 符號說明: 1、7〜玻璃基板;3〜介電層;5〜保 9 ~螢光材料;a i〜位址電極;X i〜維持電極曰〜/刀隔牆; ;10〜單元;100~電漿顯示面板;11〇〜控制,1〜掃描電極 122〜Y掃描驅動器;114、1241驅動器;路;112、 ;20卜全域寫入脈波;2 02〜全域維持脈位址驅動器 ;204〜掃描脈波;205〜維持脈波;2 a ’ Z〇3〜清除脈波 域寫入脈波;30 0a〜第一成分脈波’;3〜脈波;300〜全 3 0 1、3 0 2〜清除脈波。 第二成分脈波;516013 V. Schematic diagram of invention description (8). FIG. 4 shows the conventional technique in the single — ^ ^ # t ^ ^ ^ t ^ Υ〇 ^ ^ ^ ^. The timing chart for controlling the number h on 1 彡 FIG. 5 shows the first embodiment of the present invention 'each electrode ( The timing diagram of the control signal during the reset period, including the address signal, the maintenance map =, the electrode X, and the scan electrode Y i). Figure 6 shows a block diagram of the device of the first embodiment of the present invention. Fig. 7 is a schematic diagram of the second embodiment of the present invention. The waveform of the writing pulse wave in the j-king domain | shows the timing diagram of the control signals on each electrode (including the address electrode Ai and the dimension # ^) between the sub-picture fields in the third embodiment of the present invention. "And scan electrode Yl) Symbol description: 1, 7 ~ glass substrate; 3 ~ dielectric layer; 5 ~ Paul 9 ~ fluorescent material; ai ~ address electrode; X i ~ sustain electrode ~ / knife partition wall; 10 ~ unit; 100 ~ plasma display panel; 11 ~~ control, 1 ~ scan electrode 122 ~ Y scan driver; 114, 1241 driver; road; 112,; 20b global write pulse; 2 02 ~ global sustain pulse Address driver; 204 ~ scanning pulse wave; 205 ~ sustaining pulse wave; 2 a 'Z〇3 ~ clear pulse wave domain write pulse wave; 30 0a ~ first component pulse wave'; 3 ~ pulse wave; 300 ~ full 3 0 1, 3 0 2 ~ Clear the pulse wave. Second component pulse
5l6〇i35l6〇i3
實施例: 本發明主要係針對習知技術 二不品質所造成影響,提出可以改盖此;J :a1放電操作對於 J置對重置期时全域;二1之驅動方法和 ::增加其累積壁電荷的能力,所造成放電操 產生的亮度。以下配合 /夕其放電過程中 例。 飞咩細說明本發明之各實施 第一實施例: 第5圖表示本實施例中在4^ 包含位址電極Ai、維持電極Xi二::5置期間’各電極 =時序圖。重置期間是同時處理V田〃極γ 1 )上控制信§ 二、產生一定數量之壁電荷,因此以I描線上的單元,隹 係指全部的掃描電極γ。一 下所稱之掃描電極γ !, 为又而吕 5 jh , 別,會在掃描電極Yi送入_、、主 别一二人圖場結束之 圖場中狀態設為。η之單元内=巧’用來清除在前-:大 ,在本次圖場之重置期間之第:栌何。接著如第5圖所示 一全域寫入脈波30 0,讓維持一 1間二維持電極X上送入 差大於兩者間的放電啟始電壓,°#和掃描電極Y i之間的壓 電荷。此全域寫入脈波3 〇 0與羽=由放電產生所需要的壁 兩部分所組成。如圖所示/全白〇技術不同,其波形係由 率波形由第一電壓(0V)提昇2 ^二’脈波300是以較大斜 形由第二電壓逐漸提昇至第二垂二電壓’再以較小斜率波 一電壓。在本實施例中,第二 516013 五、發明說明(10) 電壓可以設為18〇ν,·第三電壓可以設為36〇v。接著如 所不,在掃描電極Yl上依序送入清除脈波3〇1,主、 除脈波302。接著,則進入後續的寫入期間和維持期二 t須說明的是,第5圖中重置期間内各電極控 號 =並非用以限定本發明,對於熟知潜相 二: 者而s ,可以依據其顯示原理而作不同程度之修改。 、=於本實施例主要特徵在於全域寫入脈波3 〇〇,因此 以下詳細說明其波形。全域寫入脈波3〇〇的第一部 據一較大斜率波形,由第一電壓(〇v)提昇至第二 1 作用在於可以累積大量的壁電荷,此亦為此脈波 目、 的。全域寫入脈波300的第二部分則根據一較小斜波 ,從第二電壓提昇至第三電壓’其作用亦為累積壁電/, 不過由於其電壓上昇斜率較小,因此放電效果較習知 。所以:致於”亮。總結而言,利用這種全域寫 入脈波30 0之波形,一方面仍可以累積大量壁電荷, 也不會造成太明亮的背景閃爍。 一疋 第6圖表示本實施例中電漿顯示面板之驅動裝 塊圖’其基本架構與習知技術大致相同。驅動裝置勺括 制電路11 0、位址驅動器11 6、維持驅動器丨24以匕工 $二22。控制電路110接收外部所提供之顯示資料da:和 傳輸日守脈CLOCK,以及垂直同步信號VSYNC和水 HSYNC等時序資料’將其送至各驅動器上。位址驅動/器1 = 則,寫入期間驅動位址電極Ai,將顯示資料寫入各掃° 的單元内。掃描驅動器1 22則負責驅動掃描電極η ;維田持、Example: The present invention is mainly aimed at the impact caused by the inferior quality of the conventional technology 2. It is proposed that it can be changed to cover this; J: a1 discharge operation for the entire range of the reset period; J1 driving method and: increase its accumulation The ability of the wall charges to cause the brightness produced by the discharge operation. The following is an example of the discharge process. A detailed description of each implementation of the present invention is shown in FIG. 1. First embodiment: FIG. 5 shows that in this embodiment, the address electrode Ai and the sustain electrode Xi are included in the 4: 5 period. Each electrode = timing chart. During the reset period, the control letter on the V field electrode γ 1) is processed at the same time. Second, a certain amount of wall charges are generated. Therefore, the unit on the line I indicates that 隹 refers to all the scan electrodes γ. The so-called scan electrode γ! Is again 5 yh, and the state will be set in the field where the scan electrode Yi is fed into _, and the main field is ended. In the unit of η = Qiao 'is used to clear the previous-: big, the :: he in the reset period of this field. Then, as shown in FIG. 5, a global write pulse 30 0 is written, so that the difference between the input voltage of the sustain electrodes X1 and the sustain electrode X is greater than the discharge start voltage between them, and the voltage between ° # and the scan electrode Yi. Charge. This global write pulse 3 0 0 and plume = are composed of two parts of the wall required for discharge generation. As shown in the figure / different technology, its waveform is increased from the first voltage (0V) by the rate waveform. The pulse wave 300 is gradually increased from the second voltage to the second vertical voltage in a large slope. 'Wave a voltage again with a smaller slope. In this embodiment, the second 516013 V. Description of the invention (10) The voltage can be set to 18〇v, and the third voltage can be set to 36Ov. Then, as described above, the scan pulse Y1 is sequentially fed with the clear pulse wave 301, and the main pulse wave 302 is removed. Then, it enters the subsequent writing period and maintenance period t. It should be noted that the electrode control number in the reset period in FIG. 5 is not used to limit the present invention. For the well-known latent phase two: s, you can According to its display principle, it can be modified to different degrees. The main feature of this embodiment is that the global pulse wave 300 is written, so its waveform will be described in detail below. According to a larger slope waveform, the first part of the global writing pulse 300 is increased from the first voltage (0v) to the second 1 The function is to accumulate a large amount of wall charges, which is also the purpose of this pulse wave. . The second part of the global write pulse 300 is based on a small ramp wave, which is raised from the second voltage to the third voltage. Its role is also to accumulate wall voltage /, but because its slope of voltage rise is small, the discharge effect is relatively Learn. So: "Because" is bright. In summary, using this global write pulse waveform of 300, on the one hand, it can still accumulate a lot of wall charges, and it will not cause too bright background flicker. Figure 6 shows this implementation. The driving block diagram of the plasma display panel in the example 'its basic structure is roughly the same as the conventional technology. The driving device includes a control circuit 11 0, an address driver 11 6 and a maintenance driver 丨 24 with a dagger $ 22. Control circuit 110 receives the display data da: provided by the outside, and transmits timing data such as the day guard pulse CLOCK, and the vertical synchronization signal VSYNC and water HSYNC to send it to each driver. Address driver / driver 1 = Then, drive during writing The address electrode Ai writes the display data into each scan unit. The scan driver 1 22 is responsible for driving the scan electrode η;
516013 五、發明說明(11) 驅動器1 2 4則負責驅動維持電極X。 如第5圖所示,維持驅動器】24在 間所送入的全域寫入脈波,是先以,=^圖%的重置期 壓上幵至弟二電壓(0V_>180V),再以較 電 電壓上昇至第三電壓(180V_>360 V),利用二 電極X和掃描電極γ i之間的放電動作, _ 、、、持 壁電荷。 F木產生各早TL中的 、㈣W在第5·圖中所示之全域寫入脈波3〇〇的較小斜率 波形’疋先以相對較大斜率續丨黑卜旦 緩慢上昇,盆波开二ΪΪ :幵’再以相對較小斜率 姓:士:類似二次曲線的形狀(向外凸)。維 合成逼近於此波形。式’可以利用步階電壓來 根據以上所述,本實施例之PDp驅動方法主要是修改 的全域寫入脈波,使其能夠累積大量壁電荷, 在放電時造成過高亮度而影響晝f。*實現上述 ς二”、、入脈波的波形’則只需要修改原來χ驅動器的部分 不丄4吏其月b夠產生所需要的波形,目此額外增加的成本 +两 〇 苐_貫施例: 本只鉍例與第一實施例的基本驅動方式和驅動裝置相 二,i別僅在於全域寫入脈波3 〇 〇的波形。在第一實施例 一垂ΐ域寫入脈波30 0的第一部分是以較大斜率波形由第 ^壓上昇至第二電壓,第二部分則以較小斜率波形上昇516013 V. Description of the invention (11) The driver 1 2 4 is responsible for driving the sustain electrode X. As shown in Fig. 5, the sustaining drive] 24 writes the global pulses sent in between, firstly, the voltage is reset to the second voltage (0V_ > 180V) in the reset period of = ^%, and then The electric voltage rises to a third voltage (180V_ > 360V), and uses a discharge operation between the two electrodes X and the scan electrode γ i to hold wall charges. F wood produces a small slope waveform in each early TL, ㈣W writes the pulse wave 300 in the whole domain shown in Fig. 5; 疋 first continues with a relatively large slope 丨 Habdan slowly rises, and the basin wave Open two ΪΪ: 幵 'and then with a relatively small slope Surname: Shi: Similar to the shape of a quadratic curve (outward convex). The dimensional synthesis approximates this waveform. Formula can use step voltage. According to the above, the PDp driving method of this embodiment is mainly a modified global write pulse, which enables it to accumulate a large amount of wall charges, which causes excessive brightness during discharge and affects day f. * To achieve the above two, the waveform of the incoming pulse 'only needs to modify the part of the original χ driver, which can generate the required waveform, so the additional cost + 20% Example: This example of bismuth is different from the basic driving method and driving device of the first embodiment. The difference is that the waveform of the pulse wave 300 is written in the entire domain. The pulse wave 30 is written in the vertical region of the first embodiment. The first part of 0 rises from the third voltage to the second voltage with a larger slope waveform, and the second part rises with a smaller slope waveform
516013516013
五、發明說明(12) 至第三電壓,且第二部分中電壓上昇斜率則是呈漸減的 態。而在本實施例中則以數個不同的波形說明其變異性厂 皆可以達到本發明之目的。5. Description of the invention (12) to the third voltage, and the slope of the voltage rise in the second part is gradually decreasing. In this embodiment, several different waveforms are used to illustrate that the variability plants can all achieve the purpose of the present invention.
第7a圖表示本實施例中全域寫入脈波3〇〇之第—種轉 異波形。如第7a圖所示,全域寫入波形3〇〇在第一部分^ 以較大斜率波形由第一電壓上昇至第一電壓,在第二77部 '八 以較小斜率波形上昇至第二電壓,其與第一實施例不: 處在於:第二部分中電壓上昇斜率是呈漸增的形態,因 其波形呈現二次曲線向内凹的形狀。此波形之全域寫 波300同樣可以一方面大量累積電荷,另一方面避免在脈 電過程中發出過強的亮度而影響晝質。 I 第7b圖表示本實施例中全域寫入脈波3 〇〇之第二鐵 異波形。與第一實施例不同的是,第7b圖的全域寫文 30 0仍是區分第一部份與第二部分,而是先以較小斜率&形 形上昇,再以較大斜率波形上昇(幾乎垂直之脈衝),/皮 其波形呈現二次曲線向内凹的形狀。此波形之全 U此 波3 0 〇同樣可以一方面大量累積電荷,另一方面避2 ”、、入脈 電過程中發出過強的亮度而影響晝質。 在放 根據以上所述’本發明並不特別限定全域寫入 實際波形,而只要符合以至少兩階段的方式來提的 即可以符合本發明的精神。 电& ’ 第三實施例: 本實施例是以等效波形的觀念來實現第一實施例 參Fig. 7a shows the first variation waveform of the global write pulse 300 in this embodiment. As shown in Figure 7a, the global write waveform 300 rises from the first voltage to the first voltage with a larger slope waveform in the first part, and rises to the second voltage with a smaller slope waveform in the second part 77. It is different from the first embodiment in that the slope of the voltage rise in the second part is gradually increasing, because the waveform shows a shape where the quadratic curve is concave inward. The global write wave 300 of this waveform can also accumulate a large amount of charge on the one hand, and on the other hand, avoid too much brightness during the pulse process to affect the quality of the day. Fig. 7b shows the second iron-differential waveform of the global write pulse 300 in this embodiment. Different from the first embodiment, the global writing 300 in Fig. 7b still distinguishes the first part from the second part, but first rises with a smaller slope & shape, and then rises with a larger slope waveform (Almost vertical pulse), the shape of the waveform is concave in the quadratic curve. The whole of this waveform, this wave of 300, can also accumulate a large amount of charge on the one hand, and avoid 2 ″, which emits too strong brightness during the pulsed electricity process, which affects the quality of the day. It does not specifically limit the actual writing of the global waveform, but it can meet the spirit of the present invention as long as it is mentioned in at least two stages. Electricity & 'Third embodiment: This embodiment is based on the concept of equivalent waveforms. Implementing the first embodiment
516013 五、發明說明(13) 1 第曰—實施例的第5圖,在維持電極X上的全域寫入脈波 相對來說比較複雜,成本也比較高。在本ί:二= ,此全域寫入脈波300的兩個部分,分別由維持驅動器124 描驅動器122產生並送入維持電極χ和掃描電極Yi上, 猎此簡化波形產生電路。 第8圖表示本實施例中在次圖場之重置期間,位 維持電極X和掃描電極Yi上控制信號之時序圖。如 :不,原來的全域寫入脈波3〇 〇係以 成分脈波3〇〇a(第一電I急速 :m的第- 力"三電麈緩慢下降至第四電壓) 中第-成分:波;〇fi電效果與第一實施例相同。其 波形成分,而第-^巧原全域寫入脈波300的較大斜率 ,,. 而弟一成分脈波30〇b等於;f+衫皆& 的較小斜率波形成 寫入脈波300 生第8圖之波形要一 ^ =電路貝作的角度來說,要產 驅動哭1 24 π币西產生第5圖之波形來得容易,不僅雄姓 二軔时124不需要使用到倍 勿+僅維持 動器1 2 2上增加幾個 Ρ寸只需要在掃描驅 具有較高的產業^^:件即可達到波形產生的目的, 本發明雖以齡彳土二 範圍内,當可做些許=,藝者,在不脫離本發明之精神和 圍當視後附之申过皇勺更動與潤飾,因此本發明之保嗖笳 之申5月專利範圍所界定者為準 4粍 第16頁516013 V. Description of the invention (13) 1 The fifth figure of the embodiment, writing the pulse wave on the sustain electrode X in the whole area is relatively complicated and the cost is relatively high. In this case: two =, the two parts of the global write pulse 300 are generated by the sustain driver 124 and the driver 122 and sent to the sustain electrode χ and the scan electrode Yi, respectively. This simplified waveform generating circuit is hunted. FIG. 8 shows a timing chart of the control signals on the bit sustain electrodes X and the scan electrodes Yi during the reset period of the sub-field in this embodiment. For example: No, the original global write pulse 300 is based on the component pulse 300a (the first electric I is rapid: the first-force of the "three-electricity" slowly drops to the fourth voltage)- Composition: wave; ofi electric effect is the same as the first embodiment. Its waveform component, and the larger slope of the-^ Qiaoyuan global writing pulse 300, and the smaller component of the pulse wave 300b is equal to; f + shirt all & the smaller slope wave forms the writing pulse 300 The waveform of Figure 8 needs to be ^ = From the perspective of the circuit, it is easy to produce the driving waveform of Figure 24. It is easy to produce the waveform of Figure 5 not only when the male surname Erji 124 does not need to be used. Only maintaining a few P inches on the actuator 1 2 2 can achieve the purpose of waveform generation only when the scanning drive has a high industry ^^: Although the present invention is within the range of aging soil, it can be done a little =, Artist, without deviating from the spirit and scope of the present invention, the application of the Emperor spoon has been modified and retouched. Therefore, the scope of the May patent for the protection of the present invention shall be as defined in the May 4 patent.
Claims (1)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW89100333A TW516013B (en) | 2000-01-11 | 2000-01-11 | Driving method and device of plasma display panel |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
TW89100333A TW516013B (en) | 2000-01-11 | 2000-01-11 | Driving method and device of plasma display panel |
Publications (1)
Publication Number | Publication Date |
---|---|
TW516013B true TW516013B (en) | 2003-01-01 |
Family
ID=27801155
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
TW89100333A TW516013B (en) | 2000-01-11 | 2000-01-11 | Driving method and device of plasma display panel |
Country Status (1)
Country | Link |
---|---|
TW (1) | TW516013B (en) |
-
2000
- 2000-01-11 TW TW89100333A patent/TW516013B/en not_active IP Right Cessation
Similar Documents
Publication | Publication Date | Title |
---|---|---|
TW519604B (en) | Method for driving a plasma display panel | |
TW418380B (en) | Method for driving a plasma display panel | |
KR100574124B1 (en) | Plasma display panel drive method | |
EP0657861B1 (en) | Driving surface discharge plasma display panels | |
CN100423057C (en) | Plasma display panel driving method | |
US7173578B2 (en) | Method and apparatus for driving a plasma display panel in which reset discharge is selectively performed | |
US6670774B2 (en) | Plasma display panel driving method and apparatus capable of realizing reset stabilization | |
JP2004021181A (en) | Driving method for plasma display panel | |
JP2004206094A (en) | Plasma display panel drive method | |
TW535128B (en) | Plasma display and method for driving the same | |
CN100552759C (en) | Plasma display panel device | |
TWI277928B (en) | Plasma display apparatus | |
JP2001265281A (en) | Display device and its driving method | |
KR100636943B1 (en) | Plasma display panel drive method | |
KR20040010769A (en) | Plasma display panel display and its drive method | |
US6337674B1 (en) | Driving method for an alternating-current plasma display panel device | |
US20070024533A1 (en) | Plasma display and driving method thereof | |
JP3115727B2 (en) | Driving device for plasma display panel | |
TWI248595B (en) | Apparatus and method of driving a plasma display panel | |
JP2000194320A (en) | Plasma display panel device | |
JP2004226792A (en) | Driving method of plasma display panel | |
TWI278809B (en) | Method and apparatus for driving plasma display panel | |
US20060273989A1 (en) | Plasma display device and driving method thereof | |
TW516013B (en) | Driving method and device of plasma display panel | |
TWI322402B (en) | Plasma display apparatus and driving method thereof |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
GD4A | Issue of patent certificate for granted invention patent | ||
MM4A | Annulment or lapse of patent due to non-payment of fees |