TWI303401B - Driving method for liquid crystal display - Google Patents
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- TWI303401B TWI303401B TW94126856A TW94126856A TWI303401B TW I303401 B TWI303401 B TW I303401B TW 94126856 A TW94126856 A TW 94126856A TW 94126856 A TW94126856 A TW 94126856A TW I303401 B TWI303401 B TW I303401B
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- 239000004973 liquid crystal related substance Substances 0.000 title claims description 27
- 238000000034 method Methods 0.000 title claims description 14
- 239000010409 thin film Substances 0.000 claims description 42
- 229910052736 halogen Inorganic materials 0.000 claims description 4
- 150000002367 halogens Chemical class 0.000 claims description 4
- 230000005611 electricity Effects 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 17
- 239000003990 capacitor Substances 0.000 description 13
- 230000000694 effects Effects 0.000 description 9
- 101100102598 Mus musculus Vgll2 gene Proteins 0.000 description 3
- 102100023478 Transcription cofactor vestigial-like protein 1 Human genes 0.000 description 3
- 101710176146 Transcription cofactor vestigial-like protein 1 Proteins 0.000 description 3
- 102100023477 Transcription cofactor vestigial-like protein 2 Human genes 0.000 description 3
- RGCKGOZRHPZPFP-UHFFFAOYSA-N alizarin Chemical compound C1=CC=C2C(=O)C3=C(O)C(O)=CC=C3C(=O)C2=C1 RGCKGOZRHPZPFP-UHFFFAOYSA-N 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 230000003111 delayed effect Effects 0.000 description 2
- 239000010408 film Substances 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 230000000630 rising effect Effects 0.000 description 2
- 235000003140 Panax quinquefolius Nutrition 0.000 description 1
- 240000005373 Panax quinquefolius Species 0.000 description 1
- 206010036790 Productive cough Diseases 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 210000004027 cell Anatomy 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 210000002858 crystal cell Anatomy 0.000 description 1
- 210000003298 dental enamel Anatomy 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 238000010422 painting Methods 0.000 description 1
- 230000003071 parasitic effect Effects 0.000 description 1
- 210000003802 sputum Anatomy 0.000 description 1
- 208000024794 sputum Diseases 0.000 description 1
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Description
.1303401.1303401
三達編號:TW2121PA 、九、發明說明: 、 【發明所屬之技術領域】 • 本發明是有關於一種液晶顯示器’且特別是有關於一種掃 描訊號之電壓波形。 【先前技術】 隨著液晶顯示面板的尺寸不斷地增加,傳輸於掃^線上之 掃描訊號受到的電阻-電容效應也隨著增加。這意味著,離掃^ _ 訊號輸入處較遠之畫素,其接受到掃描訊號之波形將失真的更 為嚴重。掃描訊號之波形失真會造成畫素内作為開關用之薄膜 電晶體,其導通的時間變短。另外,隨著解析度提高,平均於 每個畫素的充電時間也將減少。所以薄膜電晶體之導通時間變 短將使得此晝素内的液晶電容CL及儲存電容cs沒有足夠的充 電時間(chargingtime)儲存預定的電荷量,以致於液晶分子無 法產生預定的旋轉角度,進而使得所顯示晝面無法達成預定之 • 亮度,降低了整體的影像品質。 • 【發明内容】 有鑑於此,本發明的目的就是在提供一種液晶顯示器之驅 動方法’改善因掃描訊號之波形失真所造成離婦描訊號輸入處 較遠之畫素,其充電時間不足之問題,讓液晶顯示器所顯示之 畫面,左右兩邊之亮度更為均勻。 根據本發明的目的,提出—種液晶顯示器之驅動方法。液 曰曰顯不盗包括MxN個晝素(μ為掃描線數,N為資料線數)、掃 描線與資料驅動電路。MxN個畫素係均包括薄膜電晶體。ΜχΝ 個薄膜電晶體之閉極係均與掃描線電性連接。驅動方法欽述如 .1303401Sanda number: TW2121PA, IX. Description of the invention: [Technical field of the invention] The present invention relates to a liquid crystal display and particularly relates to a voltage waveform of a scanning signal. [Prior Art] As the size of the liquid crystal display panel continues to increase, the resistance-capacitance effect of the scanning signal transmitted on the scanning line also increases. This means that the waveform that is farther away from the input of the _ signal will be more distorted by the waveform that receives the scanned signal. The distortion of the waveform of the scanning signal causes a thin film transistor to be used as a switch in the pixel, and the conduction time is shortened. In addition, as the resolution increases, the charging time on average for each pixel will also decrease. Therefore, the on-time of the thin film transistor is shortened, so that the liquid crystal capacitor CL and the storage capacitor cs in the pixel do not have sufficient charging time to store a predetermined amount of charge, so that the liquid crystal molecules cannot generate a predetermined rotation angle, thereby making The displayed side cannot achieve the desired brightness and reduces the overall image quality. SUMMARY OF THE INVENTION In view of the above, the object of the present invention is to provide a driving method for a liquid crystal display 'improving a pixel that is far away from the input of the female signal due to waveform distortion of the scanning signal, and the charging time is insufficient. Let the LCD display display the brightness of the left and right sides more evenly. According to an object of the present invention, a driving method of a liquid crystal display is proposed. The liquid sputum includes MxN elements (μ is the number of scanning lines, N is the number of data lines), scanning lines and data driving circuits. Each of the MxN pixel systems includes a thin film transistor. The closed poles of each of the thin film transistors are electrically connected to the scanning lines. The driving method is described as .1303401
三達編號:TW2121PA '=二輸出掃描訊號至-掃描線上’此掃描訊號具有連續之第一 =堅位準、第二電壓位準與第三電壓位準。N個薄膜電晶體之 •虽接收到知描訊錢,據以導通。於N個薄膜電晶體導通期 N個畫素接收資料驅動電路所輸出之畫素電壓。 、其中,第-電壓位準係由N個薄膜電晶體之漏電量來決定 並用以使N個薄膜電晶體截止。第二電壓位準係用以使n個薄 膜電晶體導通。第三電壓位準與第二電壓位準間之電壓差係大 於第電壓位準與第二電壓位準間之電壓差。 _ $讓本發明之上述目的、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: 【實施方式】 明參妝第1圖,其為晝素電路之一例之示意圖。畫素,〇〇 包括一個作為開關用之薄膜電晶體(丁_ F丨·丨m Transistor)Tsw、液晶電容CL與储存電容cs。薄膜電晶體Tsw 例如為NM〇S,其閘極G係與掃描線SL耦接,其汲極〇與資 _ 料線DL耦接,而其源極s係經由液晶電容CL及儲存電容cS 稱接至共同電極電麼Vcom。 請參照第2圖,其為液晶顯示器之一例之架構示意圖。液 晶顯示顯示器200包括畫素陣列202、掃描驅動電路2〇4與資 料驅動私路206。晝素陣列202係由N個上述書素 、 100(1)〜100(N)所組成,N係為正整數。顯示畫面時,掃描驅動 %路204會輸出知^田訊號SS至掃描線SL上,以使n個書素 100中之薄膜電晶體TSW導通。掃描驅動電路2〇4所輸出之掃 描訊號ss之波形為脈衝方波,其具有高電壓位準Vgh與低電 壓位準Vgl。高電壓位準vgh用以使薄膜電晶體Tsw的導通, 6 1303401 、 ·Sanda number: TW2121PA '= two output scan signal to - scan line' This scan signal has a continuous first = firm level, second voltage level and third voltage level. N thin film transistors • Although they receive the money, they are turned on. During the N film transistor turn-on period, the N pixels receive the pixel voltage output by the data driving circuit. Wherein, the first voltage level is determined by the leakage current of the N thin film transistors and is used to turn off the N thin film transistors. The second voltage level is used to turn on the n thin film transistors. The voltage difference between the third voltage level and the second voltage level is greater than the voltage difference between the first voltage level and the second voltage level. The above-mentioned objects, features, and advantages of the present invention will become more apparent and obvious. The following detailed description of the preferred embodiments, together with the accompanying drawings, will be described in detail as follows: It is a schematic diagram of an example of a halogen circuit. The pixel, 包括 includes a thin film transistor (Tinger Transm Transistor) Tsw, a liquid crystal capacitor CL and a storage capacitor cs. The thin film transistor Tsw is, for example, NM〇S, the gate G is coupled to the scan line SL, the drain electrode is coupled to the resource line DL, and the source s is coupled via the liquid crystal capacitor CL and the storage capacitor cS. Connect to the common electrode power Vcom. Please refer to FIG. 2, which is a schematic diagram of an example of a liquid crystal display. The liquid crystal display display 200 includes a pixel array 202, a scan driving circuit 2〇4, and a data driving private path 206. The halogen array 202 is composed of N pieces of the above-mentioned cells, 100(1) to 100(N), and N is a positive integer. When the screen is displayed, the scan driver % channel 204 outputs the sense signal SS to the scan line SL to turn on the thin film transistors TSW in the n books 100. The waveform of the scan signal ss outputted by the scan driving circuit 2〇4 is a pulse square wave having a high voltage level Vgh and a low voltage level Vgl. The high voltage level vgh is used to turn on the thin film transistor Tsw, 6 1303401,
三達編號:TW2121PA 而低%壓位準Vgl由薄膜電晶體Tsw之漏電量來決定,其用以 ^ 使薄膜電晶體Tsw截止。藉由控制高電壓位準Vgh之致能時間 . 便能控制薄膜電晶體Tsw導通時間。 於薄膜電晶體Tsw導通期間,資料驅動電路206輸出多 筆畫素電壓VP(1)〜VP(N)至對應的資料線dl(1)〜DL(N)上。多 筆畫素電壓VP(1)〜VP(N)便透過對應導通之薄膜電晶體Tsw 輸入至對應的液晶電容CL及儲存電容cs中,以驅動液晶分子 方疋轉。所以薄膜電晶體Tsw的導通時間便會影響到畫素電壓vp 鲁對液日曰電谷CL及儲存電容CS之充電時間(chargjng time)。 而薄膜電晶體Tsw的導通時間,會受到高電壓位準Vgh 之致能時間與掃描訊號SS之波形所影響。以掃描訊號ss之波 形來看,其波形為脈衝方波。脈衝方波的上升時間與下降時間 會影響到薄膜電晶體Tsw的導通與截止時間點。當不同的上升 . 時間與下降時間,會對應影響到薄膜電晶體Tsw導通的時間長 短。 而脈衝方波的上升時間與下降時間會因掃描線上之電阻_ 電容(RC)效應,發生延遲。進一步來說,畫素100具有液晶電 谷CL與儲存電容CS,且掃描線SL與各極板間或導線間亦具 有各種產生寄生電容之條件,例如掃描線SL與共同電極板間, 所以掃描線SL上具有RC效應在或稱負載效應。因為掃描線 SL之RC效應,掃描訊號SS之脈衝方波隨著傳輸於掃描線SL 之距離增加,其波形失真之現象也隨之增加。最終,造成同一 列上左右兩邊之晝素,例如畫素1〇〇(1)與1〇〇(N),因所接收到 之掃描訊號SS之波形失真程度不同,而使得對應的薄膜電晶 體Tsw有著不同導通與截止時間。 凊參照第3圖,其為傳輸於掃描線上之掃描訊號之波形示 7 1303401 麝Sanda number: TW2121PA and the low % pressure level Vgl is determined by the leakage current of the thin film transistor Tsw, which is used to turn off the thin film transistor Tsw. The thin film transistor Tsw turn-on time can be controlled by controlling the enable time of the high voltage level Vgh. During the on-time of the thin film transistor Tsw, the data driving circuit 206 outputs a plurality of pixel voltages VP(1) to VP(N) to the corresponding data lines dl(1) to DL(N). The multi-pixel voltages VP(1) to VP(N) are input to the corresponding liquid crystal capacitors CL and storage capacitors cs through the correspondingly-transferred thin film transistors Tsw to drive the liquid crystal molecules to rotate. Therefore, the on-time of the thin film transistor Tsw affects the charging time (chargjng time) of the pixel voltage vp Lu to the liquid day and valley CL and the storage capacitor CS. The on-time of the thin film transistor Tsw is affected by the enable time of the high voltage level Vgh and the waveform of the scan signal SS. In the waveform of the scanning signal ss, the waveform is a pulse square wave. The rise and fall times of the pulsed square wave affect the conduction and cut-off time points of the thin film transistor Tsw. When different rises. Time and fall time, it will affect the length of time that the thin film transistor Tsw is turned on. The rise and fall times of the pulsed square wave are delayed by the resistance-capacitance (RC) effect on the scan line. Further, the pixel 100 has a liquid crystal cell CL and a storage capacitor CS, and the scanning line SL and each of the plates or between the wires also have various conditions for generating parasitic capacitance, such as between the scanning line SL and the common electrode plate, so scanning The line SL has an RC effect or a load effect. Because of the RC effect of the scan line SL, the pulse square wave of the scan signal SS increases as the distance transmitted to the scan line SL increases, and the waveform distortion phenomenon also increases. Eventually, the pixels on the left and right sides of the same column, such as pixels 1〇〇(1) and 1〇〇(N), are different in waveform distortion due to the received scanning signal SS, so that the corresponding thin film transistor is made. Tsw has different conduction and deadlines.凊 Refer to Figure 3, which is the waveform of the scanning signal transmitted on the scanning line. 7 1303401 麝
三達編號:TW2121PA 思® 〇 @所綠之液晶顯示顯示器2⑽之架構為例,剛輸 U掃描線SL上之掃描訊號%之波形近似於理想方波,但隨 著傳輸的距離i日加’於離掃描訊號輸人處較遠之晝素,例如畫 =100(N) _所接到之掃描訊號沾之波形發生嚴重的波形失 ”。波形失真之問題,將造成晝素1〇_之薄膜電晶體b導 通時間變短,使得其所對應的液晶電容以及儲存⑽For the example of the architecture of the LCD display 2 (10) of the TW2121PA, the waveform of the scanning signal on the SL scan line SL is similar to the ideal square wave, but with the distance of the transmission i In the case of a pixel farther away from the input of the scanning signal, for example, the waveform of the scanned signal received by the picture =100(N) _ is severely lost. The problem of waveform distortion will cause the pixel to be 〇_〇 Thin film transistor b conduction time becomes shorter, so that its corresponding liquid crystal capacitor and storage (10)
足夠的充電時間儲存預定的電荷量,以致於無法達到預定的顯 丁儿度“、:旦素100⑴,因其所接收到之掃描訊號%之波形 近似於理想方波,故有足夠的充電時間儲存預定的電荷量。所 以最、,s每成同一列上之左右兩邊之晝素畫素100(1)與畫素 1〇〇(N),所產生之發光亮度不均勻。 故,本發明提供-種液晶顯示器之驅動方法,用於解決因 負載效應太大而造成充電時間不足之問題,讓液晶顯示器所顯 示之畫面能正確顯示所需之亮度。 本毛明所提出之掃描訊號,藉由增加使薄膜電晶體導通之 包壓位準與使薄膜電晶體截止之電壓位準間之電壓差,例如上 述掃描訊號SS由高電壓位準Vgh切換為低電壓位準Vg|間之 電壓差,使得掃描訊號所呈現之電壓波形巾,電壓之下降時間 (falling time)或上升時間(ns丨’叫丨丨叫更快,以增加掃描訊號維 持於致能之時間。 第一實施例 一立請參照第4圖,其為本發明第一實施例之掃描訊號之波形 不忍圖。掃描訊號SS’例如應用於液晶顯示器2〇〇並由上述之 掃描驅動電路204所輸出。掃描訊號ss,具有連續之第一電壓 位準VgM、第二電壓位準Vgh與第三電壓位準劝丨2。第一電 8 1303401Sufficient charging time to store a predetermined amount of charge, so that the predetermined degree of singularity ", s: 100 (1) is not obtained, because the waveform of the received scanning signal % approximates the ideal square wave, so there is enough charging time The predetermined amount of charge is stored. Therefore, the illuminance brightness of the enamel pixels 100(1) and the pixels 1〇〇(N) on the left and right sides of the same column is not uniform. Therefore, the present invention is not uniform. Providing a driving method for a liquid crystal display for solving the problem of insufficient charging time due to a large load effect, so that the screen displayed by the liquid crystal display can correctly display the required brightness. The scanning signal proposed by the present invention is borrowed. The voltage difference between the voltage level at which the thin film transistor is turned on and the voltage level at which the thin film transistor is turned off, for example, the voltage difference between the high voltage level Vgh and the low voltage level Vg| In order to make the voltage waveform of the scanning signal appear, the falling time or the rising time of the voltage (ns丨' is called faster, to increase the scanning signal to maintain the time of enabling. For the first embodiment, please refer to FIG. 4, which is a waveform diagram of the scanning signal according to the first embodiment of the present invention. The scanning signal SS' is applied to, for example, the liquid crystal display 2 and output by the scanning driving circuit 204 described above. The signal ss has a continuous first voltage level VgM, a second voltage level Vgh and a third voltage level. 2: The first power 8 1303401
三達編號·· TW2121PA ,準Vgl1係由畫素100中之薄膜電晶體Tsw之漏電量來決 定,如為·6伏特。第二電壓位準Vgh係用以使薄膜電晶體丁^ ‘導通’例如為+23伏特。第三電壓位準Vg|2與第二電壓位準間 Vgh之電壓差係大於第—電壓位準Vg|1與第二電壓位準⑽ 間之電壓差,例如第三電壓位準Vg丨2係比第一電壓位準 為低’為-1 7伏特。 藉由將第三電壓位準Vgl2定義的比漏電流量來決定之第 一電壓位準Vgl1更低,讓掃描訊號ss,由高電壓位準Vgh切換 參為低電壓位準Vgl2時,電壓下降時間更快,即更快的電壓下降 斜率,代表到達薄膜電晶體Tsw之臨界電壓之時間點可以提前。 請參照第5A圖,其為本發明較實施例之掃描訊號與傳統 掃描訊號之波形示意圖。比較傳統掃描訊號ss與掃描訊號ss, 之波形。當控制信號〇E致能時(時間TS1),代表著掃描訊號 SS與知描訊號SS’要轉為非致能。如第5A圖所示,當掃描訊 號SS與掃描訊號ss,發生波形失真時,由於掃描訊號ss,之低 電壓位準Vgl2比起掃描訊號SS之低電壓位準VgM更低,所 以掃描訊號ss,下降達到一特定電壓位準,例如臨界電壓Vt, •之時間點T1,比起掃描訊號ss達到臨界電壓ντ之時間點T2 更早。這意味著,可以將掃描訊號SS,的截止時間點延後,即 將控制信號ΟΕ致能時間點延後以增加上述晝素1 〇〇之充電時 間〇 请參照第5 Β圖’其為本發明較實施例之掃描訊號與傳統 掃描訊號之波形示意圖。由於掃描訊號SS’有著較快的電壓下 降斜率,所以新的控制信號〇Ε’可以比上述控制信號〇Ε致能 時間點更晚,即時間點TS2,使得掃描訊號SS,維持在第二電 壓位準Vgh之時間更長,即讓薄膜電晶體Tsw導通之時間更 9 1303401Sanda number · TW2121PA, quasi-Vgl1 is determined by the leakage current of the thin film transistor Tsw in the pixel 100, such as 6 volts. The second voltage level Vgh is used to make the thin film transistor 'on', for example, +23 volts. The voltage difference between the third voltage level Vg|2 and the second voltage level Vgh is greater than the voltage difference between the first voltage level Vg|1 and the second voltage level (10), for example, the third voltage level Vg 丨 2 It is lower than the first voltage level '-1 to 17 volts. The first voltage level Vgl1 is determined by lowering the amount of leakage current defined by the third voltage level Vgl2, so that the scanning signal ss is switched from the high voltage level Vgh to the low voltage level Vgl2, and the voltage falling time is A faster, ie faster, voltage drop slope, which represents the point in time at which the threshold voltage of the thin film transistor Tsw is reached, can be advanced. Please refer to FIG. 5A, which is a waveform diagram of a scan signal and a conventional scan signal according to a comparative embodiment of the present invention. Compare the waveform of the conventional scanning signal ss with the scanning signal ss. When the control signal 〇E is enabled (time TS1), it means that the scan signal SS and the known signal SS' are turned into non-enabling. As shown in FIG. 5A, when the waveform signal SS and the scanning signal ss are distorted, since the scanning signal ss, the low voltage level Vgl2 is lower than the low voltage level VgM of the scanning signal SS, the scanning signal ss The falling reaches a certain voltage level, for example, the threshold voltage Vt, • the time point T1 is earlier than the time point T2 at which the scanning signal ss reaches the threshold voltage ντ. This means that the cut-off time point of the scan signal SS can be postponed, that is, the control signal is delayed by the time point to increase the charging time of the above-mentioned pixel 1 〇, please refer to FIG. 5 A waveform diagram of a scan signal and a conventional scan signal of the embodiment. Since the scanning signal SS' has a relatively fast voltage drop slope, the new control signal 〇Ε' can be later than the above-mentioned control signal 〇Ε enabling time point, that is, the time point TS2, so that the scanning signal SS is maintained at the second voltage. The time of Vgh is longer, that is, the time for turning on the thin film transistor Tsw is more 9 1303401
三達編號:TW2121PA 長。如此,當掃描訊號SS,隨著掃描線SL上之%效應的增加, 而產生波料失真時’藉由增加特在第二電壓㈣㈣之時 :,使得離掃描訊號SS,輸入處較遠之畫素,例如書素1〇_, 其充電時間將比傳統的掃描訊號ss驅動下更久。-如此,將可 大幅改善因負載效應太大而造成充電時間不^之問題。 第二實施例 B月參第6A圖’其為本發明第二實施例之掃描訊號之波 形不意圖。同樣地,掃描訊號ss,,應用於液晶顯示器2〇〇並由 上述之掃描驅動電路2G4所輸出。掃描訊號ss,,具有連續之第 -電壓位準Vg丨1、第二電壓位準㈣與第三電壓位準vgh2。 如同上述,第-電壓位準Vgl1係由晝素⑽中之薄臈電晶體 Tsw之漏電量來決定’例如為_6伏特,第二電壓位準物係 用以使薄膜電晶體Tsw導通’例如為+23伏特。而本實施例不 同於第一實施例之地方在於,第三電壓位準Vgh2係比第二電 壓位準Vgh1為高,例如為+4〇伏特。 一 進一步來說,於薄膜電晶體Tsw導通期間,藉由提高第二 電壓位準Vgh1為第三電壓位準Vgh2,以增加掃描訊號:s"- 變化於高電壓位準與低電壓位準間之電壓差,即第三電壓位準Sanda number: TW2121PA long. Thus, when the scanning signal SS is generated as the % effect on the scanning line SL increases, and the wave distortion occurs, 'by increasing the second voltage (4) (4): so that the scanning signal SS is farther away from the input. A pixel, such as a stencil, will take longer to charge than the traditional scan signal ss. - This will greatly improve the charging time caused by the load effect being too large. SECOND EMBODIMENT B. FIG. 6A is a waveform inconsistency of a scanning signal according to a second embodiment of the present invention. Similarly, the scanning signal ss is applied to the liquid crystal display 2 and outputted by the above-described scanning drive circuit 2G4. The scanning signal ss has a continuous first-voltage level Vg 丨1, a second voltage level (four) and a third voltage level vgh2. As described above, the first voltage level Vgl1 is determined by the leakage current of the thin germanium transistor Tsw in the halogen (10), for example, _6 volts, and the second voltage level is used to turn on the thin film transistor Tsw. It is +23 volts. The present embodiment differs from the first embodiment in that the third voltage level Vgh2 is higher than the second voltage level Vgh1, for example, +4 volts. Further, during the turn-on of the thin film transistor Tsw, the scan signal is increased by increasing the second voltage level Vgh1 to the third voltage level Vgh2: s"- varies between the high voltage level and the low voltage level Voltage difference, that is, the third voltage level
Vgh2與第一電壓位準VgM間之電壓差’讓電壓下降之時間更 快。同樣地,電壓下降之時間更快,除了可增加充電時間^, 更讓薄膜電晶體Tsw截止的更快而避免接收到下一鍪查 ,,.. 罕旦言電壓 的情況。 此外,本實施例中不限只能減少電壓下降之時間,亦可、咸 少電壓上升之時間以增加畫素的充電時間。請參照第固 其為本發明第二實施例之另一掃描訊號之波形示意圖。掃描訊 1.303401The voltage difference between Vgh2 and the first voltage level VgM makes the voltage drop faster. Similarly, the voltage drop time is faster, in addition to increasing the charging time ^, so that the thin film transistor Tsw cuts off faster and avoids receiving the next check, .... In addition, in this embodiment, it is not limited to reducing the time for voltage drop, and the time during which the voltage rises is less, so as to increase the charging time of the pixels. Please refer to the waveform diagram of another scanning signal according to the second embodiment of the present invention. Scanning 1.303401
二達編號:TW2121PA ** - 唬SS改具有連續之第_電壓位準VgM、第三電壓位準Vgh2 與第二電壓位準Vgh1。第三電壓位準vgh2係提前在第二電壓 • 位準Vgh1前呈現’以增加掃描訊號SS"變化於低電壓位準與 回電壓位準間之電壓差。如此即可讓薄膜電晶體Tsw導通之時 間點更為提前’以改善因負載效應太大而造成充電時間不足之 問題。 第三實施例 掃描訊號中,增加薄膜電晶體導通與截止間之電壓差,不 限=由回電壓位準轉換為低電壓位準或由低電壓位準轉換為高 f壓位準時,更可同時增加電壓上升與下降之電壓差。請參照 第7圖,其為本發明第三實施例之掃描訊號之波形示意圖。同 樣地,掃描訊號SS,,,亦應用於液晶顯示器2〇〇並由上述之掃描 驅動電路204所輸出。掃描訊號ss,,,包括連續之第—電壓位準 Vgii、第四電壓位準Vgh2、第二電壓位準ν_與第三電壓位 準刈丨2。同樣地與第-、二實施例相同,第-電壓位準Vgl1 用以使薄膜電晶體截止,例如為_6伏特,而第二電壓位準 用以使薄膜電晶體導通’例如為+23伏特。第三電壓位準華 =第^施丫列,其係比第一電壓位準_為低,例如為·Η :二 =_低電壓位準間之電壓差外,更增加了由 低電壓位準轉換向電壓位準間之電壓差。 如同上述所述之原理,第三實施例讓掃描簡s =與下降時間更快,使得畫素之充電時間可以增加。因此升 本1明所提出之掃描訊號’並不限於是由高電逐位準轉換低電 1303401Erda number: TW2121PA ** - 唬SS change has a continuous _voltage level VgM, a third voltage level Vgh2 and a second voltage level Vgh1. The third voltage level vgh2 is advanced in advance of the second voltage level Vgh1 to increase the voltage difference between the low voltage level and the return voltage level. In this way, the film transistor Tsw can be turned on at a later time to improve the problem of insufficient charging time due to a large load effect. In the scanning signal of the third embodiment, the voltage difference between the on and off of the thin film transistor is increased, and the voltage difference between the on-voltage level and the low-voltage level is changed to the high-f voltage level. At the same time, increase the voltage difference between voltage rise and fall. Please refer to FIG. 7, which is a waveform diagram of a scan signal according to a third embodiment of the present invention. Similarly, the scanning signal SS, is also applied to the liquid crystal display 2 and output by the above-described scanning driving circuit 204. The scan signal ss,, includes a continuous first-voltage level Vgii, a fourth voltage level Vgh2, a second voltage level ν_, and a third voltage level 刈丨2. Similarly, in the same manner as in the first and second embodiments, the first voltage level Vgl1 is used to turn off the thin film transistor, for example, _6 volts, and the second voltage level is used to turn on the thin film transistor, for example, +23 volts. The third voltage level is the second voltage level, which is lower than the first voltage level _, for example, the voltage difference between the low voltage level and the second voltage level is increased by the low voltage level. The voltage difference between the quasi-conversion and voltage levels. As with the principle described above, the third embodiment makes the scan simple s = faster than the fall time, so that the charging time of the pixels can be increased. Therefore, the scanning signal proposed by Sheng 1 is not limited to the conversion of low power by high-voltage leveling. 1303401
三達編號·· TW2121PA 壓位準間之電屢差或低電慶位準轉換高電麼位準間之電麗差, 只要能使掃描訊號之上升時間與下降時間更快即可達到改盖查 素之充電時間。 D旦 除此之一外第4、6或7圖所示之掃描訊號,不限制應用 ^第1圖所示之畫素結構,亦可使用於其他具有作為開關用之 缚臈電晶體之畫素結構。本發明上述實施例所揭露之液晶顯示 器之驅動方法’藉由增加掃描訊號之高電壓位準與低電壓位準达达号·· TW2121PA The voltage difference between the voltage level and the low level of the electric level can be changed as long as the rising time and the falling time of the scanning signal can be changed. Check the charging time. D. In addition to this one, the scanning signal shown in Fig. 4, 6 or 7 does not limit the pixel structure shown in Fig. 1, and can also be used in other paintings having a binding transistor as a switch. Prime structure. The driving method of the liquid crystal display disclosed in the above embodiments of the present invention is as follows: increasing the high voltage level and the low voltage level of the scanning signal
,之電麼差’以使得掃描訊號之上升時間與下降時間比起傳統 掃描訊號更快’讓掃描訊號之波形失真後,仍然比起傳統的作 法有更多的充電時間。 I、上所述,雖然本發明已以一較佳實施例揭露如上 然其 並非用=限定本發明,任何熟習此技藝者,在不脫離本發明之 :神#範圍内’當可作各種之更動與潤飾,因此本發明之保讀 範圍當視後附之巾請專利範圍所界定者為準。The power difference is 'so that the rise and fall times of the scan signal are faster than the conventional scan signal'. After the waveform of the scan signal is distorted, it still has more charging time than the conventional method. In the above, although the present invention has been disclosed in a preferred embodiment as above, it is not intended to limit the present invention, and anyone skilled in the art can make various kinds without departing from the scope of the invention: The scope of the reading of the present invention is determined by the scope of the patent application.
12 130340112 1303401
三達編號:TW2〗21PA 、【圖式簡單說明】 第1圖為畫素電路之一例之示意圖。 第2圖為液晶顯示器之一例之架構示意圖。 第3圖為傳輸於掃描線上之掃描訊號之波形示意圖。 第4圖為本發明第—實施例之掃描訊號之波形示意圖。 第5A圖為本發明較實施例之掃描訊號與傳統掃描訊號之 波形示意圖。 第5B圖為本發明較實施例之掃描訊號與傳統掃描訊號之 I 波形示意圖。 第6A圖為本發明第二實施例之掃描訊號之波形示意圖。 第6B圖為本發明第二實施例之掃描訊號之波形示意圖。 第7圖為本發明第三實施例之掃描訊號之波形示意圖。 【主要元件符號說明】 1〇〇 :晝素 200 :液晶顯示器 > 2〇2 :畫素陣列 204 :掃描驅動電路 2〇6 :資料驅動電路 SL :掃描線 DL :資料線 Tsw :薄膜電晶體 cs :液晶電容 CL :健存電容 13Sanda number: TW2〗 21PA, [Simple description of the diagram] Figure 1 is a schematic diagram of an example of a pixel circuit. Figure 2 is a schematic diagram showing the structure of an example of a liquid crystal display. Figure 3 is a waveform diagram of the scanning signal transmitted on the scanning line. Fig. 4 is a waveform diagram showing the scanning signal of the first embodiment of the present invention. Fig. 5A is a waveform diagram showing the scanning signal and the conventional scanning signal of the embodiment of the present invention. FIG. 5B is a schematic diagram showing the waveforms of the scan signal and the conventional scan signal according to the embodiment of the present invention. FIG. 6A is a schematic diagram showing the waveform of the scanning signal according to the second embodiment of the present invention. FIG. 6B is a schematic diagram showing the waveform of the scanning signal according to the second embodiment of the present invention. Figure 7 is a waveform diagram of a scanning signal according to a third embodiment of the present invention. [Main component symbol description] 1〇〇: Alizarin 200: Liquid crystal display> 2〇2: pixel array 204: scan drive circuit 2〇6: data drive circuit SL: scan line DL: data line Tsw: thin film transistor Cs : liquid crystal capacitor CL : storage capacitor 13
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Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN101916540A (en) * | 2010-08-10 | 2010-12-15 | 友达光电股份有限公司 | Clock pulse signal generating method |
| TWI398840B (en) * | 2009-10-12 | 2013-06-11 | Au Optronics Corp | Organic light emitting display having a power saving mechanism |
| TWI408657B (en) * | 2009-01-16 | 2013-09-11 | Innolux Corp | Liquid crystal display device |
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| TWI408657B (en) * | 2009-01-16 | 2013-09-11 | Innolux Corp | Liquid crystal display device |
| TWI398840B (en) * | 2009-10-12 | 2013-06-11 | Au Optronics Corp | Organic light emitting display having a power saving mechanism |
| CN101916540A (en) * | 2010-08-10 | 2010-12-15 | 友达光电股份有限公司 | Clock pulse signal generating method |
| CN101916540B (en) * | 2010-08-10 | 2012-08-29 | 友达光电股份有限公司 | Clock pulse signal generation method |
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