128 im f.doc/006 九、發明說明: 【發明所屬之技術領域】 本發明是有關於一種顯示晝素的補償電路及驅動方法並 顯示裝置,且特別是有關於一種主動式矩陣有機發光顯示 晝素的補償電路及驅動方法並顯示裝置。 【先前技術】 目前有機發光顯示器技術依驅動方式可分為被動式 (passive matrix)與主動式(active matrix)驅動兩種。被動驅 動的方法為掃描線依序開啟時,逐列在開啟時間依各個資 料線不同電流值而點亮陣列的發光二極體。因此每個二極 體皆是操作在短脈衝的模式下,且每個時間點僅有一條掃 描線會被點亮,此表示欲達到顯示器的平均亮度,每一發 光二極體均需以高脈衝操作(>1〇〇〇〇 Nits),所以需更高的 二極體操作電壓與電流。但這樣也將會造成材料壽命及效 率的大幅下降。而且,此問題隨著顯示器的尺寸與解析度 增加,將會更為嚴重。因此,可使用主動驅動方法來解決 被動驅動方法的缺失,也就是在每個發光二極體的畫素内 加上電晶體的開關與驅動電路。 因有機發光二極體是一種電流驅動元件,故一般畫素 結構至=需兩顆電晶體,圖1A所示為一般主動驅動式有機 發光顯示H的晝素架構,該畫素架構主要包含_個切換薄 膜電晶體(Switch TFT)l〇〇、- >[固驅動薄膜冑晶體(Drive 丁?丁)1〇2和一個電容儲存器(別〇1#咽(;叩触〇1>)1〇4。切換薄 膜電晶體100的功能在於作為影像資料進入儲存電容104 I281H. doc/006 的開關及定址之用,儲存電容104提供電位來打開驅動薄 膜電晶體102,並由電源電壓位準Vdd提供電流,用以驅 動有機發光二極體元件106,同時藉由調變不同電流值進 而控制顯示器的灰階。 但是’低溫多晶矽之驅動薄膜電晶體的臨界電 v (閾值電壓)及載子遷移率(yn or Vp)會因雷射社晶製 而造成變異’以及晝素結構的位置差異而不 有ηχη個晝素結構之顯示裝置,而不同位置# 皆有不同的臨界電壓:如νΛ(1,υ、vth(1,njV^(^、128 im f.doc/006 IX. Description of the Invention: [Technical Field] The present invention relates to a compensation circuit and a driving method for displaying a pixel, and a display device, and more particularly to an active matrix organic light emitting display The compensation circuit and the driving method of the halogen are displayed. [Prior Art] At present, the organic light-emitting display technology can be classified into a passive matrix and an active matrix driving according to a driving method. The passive driving method is to illuminate the LEDs of the array according to different current values of the respective data lines at the turn-on time when the scan lines are sequentially turned on. Therefore, each diode is operated in a short pulse mode, and only one scan line is lit at each time point, which means that to achieve the average brightness of the display, each light-emitting diode needs to be high. Pulse operation (>1〇〇〇〇Nits) requires higher diode operating voltage and current. However, this will also result in a significant drop in material life and efficiency. Moreover, this problem will become more serious as the size and resolution of the display increase. Therefore, the active driving method can be used to solve the lack of the passive driving method, that is, the switching and driving circuit of the transistor is added to the pixels of each of the light-emitting diodes. Since the organic light emitting diode is a current driving element, the general pixel structure to = two transistors is required, and FIG. 1A shows the pixel structure of the general active driving organic light emitting display H. The pixel structure mainly includes _ Switched TFTs (Switch TFT) l〇〇, - > [Solid Drive Thin Films (Drive Ding) 1〇2 and a Capacitor Reservoir (Do not 〇1# 咽(;叩触〇1>) 1〇4. The function of switching thin film transistor 100 is to enter the storage capacitor 104 I281H.doc/006 as the image data for the switching and addressing. The storage capacitor 104 provides the potential to open the driving thin film transistor 102 and is regulated by the power supply voltage. Vdd provides current for driving the organic light-emitting diode element 106 while controlling the gray scale of the display by modulating different current values. However, the critical electric frequency (threshold voltage) and carrier of the low-temperature polycrystalline silicon driven thin film transistor The mobility (yn or Vp) will cause variation due to the crystal structure of the laser company, and the position difference of the structure of the alizarin without the display device of the ηχη 昼 结构 structure, and the different positions # have different threshold voltages: such as νΛ (1, υ, vt h(1,njV^(^,
Vth(n,n)…·等。圖1C繪示,位置的不同對驅動薄’曰 之臨界電壓所造成的變化。所以可得vth =(^電=體 有機發光二極體的電流為Ud = f= 极加KlriJ2,所以與有機發光二極體的位置有關。 輝度咖/心又與WK成正比 為申數),因此可知,在不同的晝素結構位^ 臨界電壓會導致輝度不均及灰階不準確等問題。 、 請參看圖2,%示沒有補償電路的—個晝素結構的驅動 觀結果。關巾資料雜人賴值為·4V,當臨界電壓分 別為-IV、-2V、以及_3V時,模擬結果的電流值,也皆不 相同,因此會造成晝面品質的不穩定。 為了改善此種因雷射結晶製程及空間差異所導致的變 ίΞΪ禮許ίίί及研究單位紛紛提出用電路補償方式的 畫素結構、參看圖从〜犯。—般其晝素結構内是採 6顆1晶体來加以改善上述之變異’但是因為此種補償電路 至少需要4、顆電晶體才可以實現,因此開口率較低,而且 有工作比難以調整等缺失,待需解決。 — 【發明内容】 本發明的目的就是在提供一種顯示晝素的補償電路及 驅動方法並顯示裝置。僅使用三個電晶體,就改善了因臨 界電壓變異而造成的輝度不均及灰階不準確的問題,且具 有比習知更高的開口率及易於調整工作比等優點。 本發明提出一種顯示晝素的補償電路,此補償電路包 括有三個電晶體、一個電容、以及一個發光二極體。三個 電晶體皆具有閘極、第一及第二源/汲極。其中第一電晶體 的第一源/汲極麵接於資料線,閘極則麵接於掃猫線。第二 電晶體之閘極與第二源/汲極耦接,並耦接於第一電晶體之 第一源//及極,而弟二電晶體之第一源/没極則麵接於資料 線。第三電晶體之第二源/汲極耦接於電源電壓位準,其閘 極則輕接於第二電晶體之第二源/汲極。另外,電容具有二 端,其中一端耦接於第二電晶體之閘極,另一端則耦接於 第三電晶體之第二源/汲極。以及一個發光二極體,具有p 端以及N端,其中P端耦接於第三電晶體之第一源/汲極, N端則接地。 上述之補償電路中,電晶體可以使用薄膜電晶體;發 光二極體可以使用有機發光二極體。 從另一觀點來看,本發明亦提供一種顯示裝置,此顯 示裝置包括有多數個補償電路,其中每一補償電路至少更 包括有三個電晶體、一個電容、以及一個發光二極體。三 個電晶體皆具有閘極、第一及第二源/汲極。其中第一電晶 體的第一源/汲極耦接於資料線,閘極則耦接於掃瞄線。第 doc/006 1281139 13349twfj 一電晶體之閘極與第二源/ 曰體 之第二源/汲極,而第二電’並输於第一電晶 線。第三電晶體之第二源汲極聰接於資料 極二電·第有閉 :二其:趙以 P滅以;5龍甘t 以及—個發光二極體,具有 W以及N知,其tP端轉接於第三電晶體之第 有 Μ此顯Ϊ裝置還包括資料線驅動電路、 -個第n以及中資料線驅動電路输於上述之每 動電路,則11垃於第一電晶體之第一源/沒極,而間極驅 相接於上述之第—電晶體之閘極 號選擇性地使該些電晶料通。 心輸出k 上述_示裝置,在—實施财,電 =每一個晝素架構所使用的發光二極體為有= 從另一觀點看,本發明亦提供一種電路驅動方法,此 驅動方法適用於上述之補償電路,首先使電源電壓 0 ’接著使資料線之電壓值小於第二電晶體之臨界電壓值: Ξ==線之電壓以打開第一電晶體,再改變掃崎 電堡以關閉第-電晶體’之後改變資料線至顯示影 需的電麗’以及改變電源電壓位準為工作電位, 流驅動發光二極體。 捉供電 本發明之補償電路為電壓驅動電路,且可以改盖 因臨界電壓變異而造成的輝度不均勻及灰階不準^等^ 1281 f.doc/006 失:使得顯示器畫面品質可以更為均勻。除此之外,更有 較咼的開口率、以及易於調整工作比等優點。 為讓本發明之上述和其他目的、舰和優點能更明顯 下文特舉_較佳實施例,並配合所附圖式,作詳細 說明如下。 【實施方式】 睛參照圖4A,其緣示依照本發明一較佳實施例的由3 個電晶體所實現的補償電路I其中,η、Τ2、Τ3為三個 電晶體,400為電容,402為有機發光二極體(〇rganiciight diode以下稱咖)。DAT為資料線,sct為掃 須注意的是,在本實施例中係採?型電晶體為例, 然熟習該撤術者魏轉核制时Vth(n,n)...·etc. Figure 1C illustrates the change in threshold voltage caused by the difference in position. Therefore, vth = (^ electric = body organic light-emitting diode current Ud = f = extremely KlriJ2, so it is related to the position of the organic light-emitting diode. The brightness coffee / heart is proportional to WK is the application) Therefore, it can be seen that the threshold voltage in different pixel structure levels causes uneven brightness and inaccurate gray levels. Please refer to Figure 2, where % shows the driving view result of a monolithic structure without a compensation circuit. When the threshold voltage is -IV, -2V, and _3V, the current values of the simulation results are also different, so the quality of the kneading surface is unstable. In order to improve the laser crystallization process and space differences caused by the changes, the research unit has proposed the pixel structure of the circuit compensation method, see the picture from ~ guilty. In the general structure, six crystals are used to improve the above variation. However, since the compensation circuit requires at least 4 transistors, the aperture ratio is low, and the working ratio is difficult to adjust. Missing, pending resolution. SUMMARY OF THE INVENTION An object of the present invention is to provide a compensation circuit and a driving method for displaying a pixel and a display device. The use of only three transistors improves the unevenness of the luminance and the inaccuracy of the gray scale due to the critical voltage variation, and has the advantages of a higher aperture ratio and easier adjustment of the work ratio. The present invention provides a compensation circuit for displaying a halogen, the compensation circuit comprising three transistors, a capacitor, and a light emitting diode. Each of the three transistors has a gate, first and second source/drain. The first source/drain surface of the first transistor is connected to the data line, and the gate is connected to the sweeping cat line. The gate of the second transistor is coupled to the second source/drain and coupled to the first source//pole of the first transistor, and the first source/no pole of the second transistor is surface-connected Information line. The second source/drain of the third transistor is coupled to the power supply voltage level, and the gate is lightly coupled to the second source/drain of the second transistor. In addition, the capacitor has two ends, one end of which is coupled to the gate of the second transistor, and the other end of which is coupled to the second source/drain of the third transistor. And a light emitting diode having a p terminal and an N terminal, wherein the P terminal is coupled to the first source/drain of the third transistor, and the N terminal is grounded. In the above compensation circuit, a thin film transistor can be used for the transistor; an organic light emitting diode can be used for the light emitting diode. From another point of view, the present invention also provides a display device comprising a plurality of compensation circuits, wherein each compensation circuit further comprises at least three transistors, a capacitor, and a light-emitting diode. Each of the three transistors has a gate, first and second source/drain. The first source/drain of the first transistor is coupled to the data line, and the gate is coupled to the scan line. The doc/006 1281139 13349 twfj is a gate of the transistor and a second source/drain of the second source/body, and the second electric is coupled to the first transistor. The second source of the third transistor is the same as that of the data pole. The second is closed: two of them: Zhao to P; 5, Long Gan and a light-emitting diode, with W and N, The tP terminal is switched to the third transistor. The display device further includes a data line driving circuit, and the nth and middle data line driving circuits are respectively connected to each of the moving circuits, and the first transistor is disposed on the first transistor. The first source/no pole, and the gate of the first transistor connected to the above-mentioned transistor-selectively selectively pass the electro-ceramic materials. Heart output k The above-mentioned device shows that the light-emitting diode used in each pixel structure is present. From another point of view, the present invention also provides a circuit driving method, which is applicable to The compensation circuit described above first makes the power supply voltage 0' and then causes the voltage value of the data line to be smaller than the threshold voltage value of the second transistor: Ξ== the voltage of the line to open the first transistor, and then change the sweeping power to close the first - After changing the data line to the display device, and changing the power supply voltage level to the operating potential, the current drives the light-emitting diode. The power supply circuit of the present invention is a voltage driving circuit, and can change the brightness unevenness caused by the threshold voltage variation and the gray level is not allowed. ^1281 f.doc/006 Loss: the display picture quality can be more uniform . In addition, it has the advantages of a relatively low aperture ratio and easy adjustment of the work ratio. The above and other objects, advantages, and advantages of the present invention will become more apparent from the following detailed description of the preferred embodiments. [Embodiment] Referring to FIG. 4A, there is shown a compensation circuit 1 implemented by three transistors according to a preferred embodiment of the present invention, wherein η, Τ2, Τ3 are three transistors, 400 is a capacitor, 402 It is an organic light-emitting diode (〇rganiciight diode hereinafter referred to as coffee). DAT is the data line, and sct is the sweep. Note that in this embodiment, it is adopted? For example, a type of transistor is familiar to the
電晶體之肢。 I 朽三個電晶體T1、T2^3分別具有閘 木、第-及第-源/錄。第—電晶體η的第 接於資料線DAT ’閘極則_於掃瞒線SCT '二 :2之間極與第二源,難_,綱於第-電晶:τΓ! ^二臟極,而第二電晶體Τ2之第一源__接於資 位。/門:電上體Τ3之第二源/沒極耦接於電源電壓 位準vdd,其__接於第二電晶體τ 另外,電容400具有二端,其中 第:=〜 之閘極,另—端_接於第三電晶體T3之及體極 =發光二極體402,具有ρ端以及Ν端’ρ 於第三電晶體Τ3之第-源級極,Ν端則接地。 1281 LI- 請對照圖5之時脈圖。在第一階段,即重置階段時, 電源電壓位準由Vdd降至為〇,資料線DAt的電壓值降為 -Vdn’且此電壓值-Vdn低於-VthT2(電晶體T2的臨界電壓)。 再者,掃瞄線SCT則降至比資料線DAT之電壓值還低至 少-VthT1(電晶體T1的臨界電壓)的電壓。在此狀況下,原 本圖4A所示之電路將等效如圖4B所示。其中,由於T1 電晶體此時將導通,所以在理想假設狀態下,&點電壓值Va 應等同於資料線DAT的電壓而為_Vdn。 在圖5的第二階段,即程式化階段時,資料線dAt的 電壓值由-Vdn回覆至原本顯示時所需的電壓vdata,且掃 瞄線sct的電位亦拉高以使電晶體T1關閉。在此狀況下, 原本圖4A所示之電路將等效如圖4C所示。其中,電晶體 T1被關閉,而原本電壓值為^^如的a點,則因為電晶體打 被導通而逐漸升高,這種電壓升高的過程將一直持續到a 點的電壓值與Vdata間相差為-vthT2(電晶體T2的臨界電 壓)’並因此導致電晶體T2被關閉時才會停止。因此,在 程式化階段結束後,a點的電壓值將為Vdata-|Vtj^卜 接下來,在圖5的第三階段,即發光階段中,電源電 壓位準由〇回復為Vdd>0,且其他條件不變。在此狀況下, 原本圖4A所示之電路將等效如圖4D所示。其中,電晶體 T2保持斷路,而a點的電壓值(即為T3的閘極電壓值) 由於電容400的推升效應所致,將同步上升約vdd。換句 話說,此時a點的電壓值Va=Vdd+Vdata_|VthT2丨,流經有 機發光二極體的電流ioled的值可由下式推得· 128 魏 _ ioled^ |(|^h|^3|)2 = I [(Vdd - Fa)^\VthT3\J == 營[㈣-(⑸心胸α - —n 1))一—n |]2 其中,由於業界一般預設:在同一晝素中的電晶體因 距離極小,所以臨界電壓值幾乎相等。故可得VthT2 = Vth^, 則上式中iQled=警[―Kcfeta]2。 由上述運算實證中可以得知,此補償電路為一種電壓 驅動電路,流經有機發光二極體的電流只與資料線的輸入 電壓值Vdata有關,與有機發光二極體所在的晝素位置The limb of the transistor. I The three transistors T1 and T2^3 have sluice, first- and first-source/record respectively. The first - transistor η is connected to the data line DAT 'gate _ on the broom line SCT 'two: 2 between the pole and the second source, difficult _, the first-electro-crystal: τ Γ! ^ two dirty And the first source __ of the second transistor Τ2 is connected to the position. / gate: the second source/no pole of the electrical upper body 3 is coupled to the power supply voltage level vdd, and the __ is connected to the second transistor τ. In addition, the capacitor 400 has two ends, wherein the gate of the first:=~ The other end is connected to the third transistor T3 and the body pole = the light emitting diode 402, having a p-terminal and a terminal end 'p to the first-source level of the third transistor Τ3, and the terminal is grounded. 1281 LI- Please refer to the clock map of Figure 5. In the first phase, the reset phase, the power supply voltage level is reduced from Vdd to 〇, the voltage value of the data line DAt is reduced to -Vdn' and the voltage value -Vdn is lower than -VthT2 (the threshold voltage of the transistor T2) ). Furthermore, the scan line SCT is reduced to a voltage which is at least -VthT1 (the threshold voltage of the transistor T1) lower than the voltage value of the data line DAT. In this case, the circuit shown in Fig. 4A will be equivalent as shown in Fig. 4B. Among them, since the T1 transistor will be turned on at this time, in the ideal hypothesis state, the & point voltage value Va should be equal to the voltage of the data line DAT and be _Vdn. In the second phase of FIG. 5, that is, during the stylization phase, the voltage value of the data line dAt is returned from -Vdn to the voltage vdata required for the original display, and the potential of the scan line sct is also pulled high to turn off the transistor T1. . In this case, the circuit shown in Fig. 4A will be equivalent as shown in Fig. 4C. Among them, the transistor T1 is turned off, and the original voltage value is a point of ^^, because the transistor is gradually turned on due to conduction, the voltage rise process will continue until the voltage value of point a and Vdata The phase difference is -vthT2 (the threshold voltage of the transistor T2)' and thus causes the transistor T2 to be stopped when it is turned off. Therefore, after the end of the stylization phase, the voltage value at point a will be Vdata-|Vtj^. Next, in the third phase of Figure 5, the illuminating phase, the power supply voltage level is restored by 〇 to Vdd> And other conditions remain unchanged. In this case, the circuit shown in Fig. 4A will be equivalent as shown in Fig. 4D. Among them, the transistor T2 is kept open, and the voltage value at point a (i.e., the gate voltage value of T3) is synchronously increased by about vdd due to the push-up effect of the capacitor 400. In other words, at this time, the voltage value of point a is Va=Vdd+Vdata_|VthT2丨, and the value of the current ioled flowing through the organic light-emitting diode can be obtained by the following formula: 128 Wei_ioled^ |(|^h|^ 3|)2 = I [(Vdd - Fa)^\VthT3\J == Camp [(4)-((5) Cardiac α - -n 1)) 1-n |]2 Among them, due to the industry's general presupposition: in the same 昼Since the transistors in the prime are extremely small, the threshold voltages are almost equal. Therefore, VthT2 = Vth^ can be obtained, then iQled=[[Kcfeta]2 in the above formula. It can be known from the above calculation that the compensation circuit is a voltage driving circuit, and the current flowing through the organic light emitting diode is only related to the input voltage value Vdata of the data line, and the position of the pixel where the organic light emitting diode is located.
Vth(x,y;)無關。因此,可以改善因著vth臨界電壓值空間 變化,而導致的輝度不均、以及灰階不準確的問題。 本發明亦提供一種顯示裝置,請參照圖4E,至少包括 多數個上述之補償電路、一個資料線驅動電路41〇、以及 一個閘極驅動電路412。其中資料線驅動電路41〇耦接於们 及Τ2的第一源/汲極,閘極驅動電路412耦接於T1的閘極, 用以輸出信號選擇性地導通電晶體。透過應用上述補償電 路使本發明之顯示裝置,亦有本發明之補償電路所具有 之功效及優點。 ^ 往參K if ^算n外’*亦可透過模擬看出此結果。 圖v f示時間對電壓的模擬結果圖。在Vth(x,y;) has nothing to do. Therefore, the problem of uneven luminance and inaccurate gray scale due to spatial variation of the vth threshold voltage value can be improved. The present invention also provides a display device. Referring to Figure 4E, at least a plurality of the above-described compensation circuits, a data line drive circuit 41A, and a gate drive circuit 412 are included. The data line driving circuit 41 is coupled to the first source/drain of the Τ2, and the gate driving circuit 412 is coupled to the gate of the T1 for outputting a signal to selectively conduct the crystal. The display device of the present invention also has the functions and advantages of the compensation circuit of the present invention by applying the above compensation circuit. ^ To the parameter K if ^ calculate n outside '* can also see the result through simulation. Figure v f shows the simulation results of time vs. voltage. in
Si s? f f VthT2 V^-2V 以及-3V時’ Va鋪擬結果分別為_5V、祝、 則所”之·a皆為.而[屬十因此,當Vdata 保持^疋時,I。丨^也會穩定,使得輝度 定的晝面。圖7繪示有補償電路的電流穩 與圖2相對照,可看出,當Vth分jam莫擬結果’ 時’所得到的電流值皆趨近於;又因及二 Τ2/(Τ1+Τ2),T1 ; I28iy^doc/006 得以調整。 習知中電子遷移率的變異問題,可以透過較高的 率來改善,而開口率與補償電路的大小成反比,也就 當我們使用越少的元件來實現補償電路,便可以得1古 的開口率來改善電子遷移率的問題。 又向 綜上所述,本發明之補償電路,因只用三個電晶體 實現,因此除了改善無補償電路時,輝度不均、灰階進 碟等問題之外,相較於習知的補償電路,又有更高’ 率可提高電子遷移率、降低成本、以及具有可 二 比之優點。 作 雖然本發明已以較佳實施例揭露如上,然其並 限定本發明’任何熟習此㈣者,在不麟本㈣之精神 31當可Γ許之更動與潤飾,因此本發明之保護 耗圍备視伽之申料利細所界定者為準。 【圖式簡單說明】 口:C知絲式有機發光_器的晝素架構圖。 圖1B疋習知主動式有機發光顯示器圖。 P補 圖3A〜3D是習知補償電路圖。 是本發明之補償電路及其等效電路圖。 圖4E疋本發明之顯示裝置圖。 圖5是本發明之時脈圖。 圖6是本發明之電麼時間模擬結果圖。 圖7是本發明之電流時間模擬結果圖。 12 128 im f.doc/006 【主要元件符號說明】 100、102 :電晶體 104 :電容 106 :有機發光二極體 400 :電容 402 :發光二極體 410 :資料線驅動電路 412 :閘極驅動電路 ΤΙ、T2、T3 :電晶體Si s? ff VthT2 V^-2V and -3V 'Va paving results are _5V, wish, then," a is all. And [is ten, therefore, when Vdata keeps ^疋, I.丨^ will also be stable, making the brightness of the face. Figure 7 shows the current stability of the compensation circuit compared with Figure 2, it can be seen that when Vth points jam, the result of the current results are close. And; because of 2Τ(/1Τ2), T1; I28iy^doc/006 can be adjusted. The variation of electron mobility in the conventional case can be improved by a higher rate, and the aperture ratio and compensation circuit Inversely proportional to the size, when we use fewer components to implement the compensation circuit, we can get an aperture ratio to improve the electron mobility. In summary, the compensation circuit of the present invention is only used. Three transistors are implemented, so in addition to improving the uncompensated circuit, the uneven brightness, gray scale into the disk and other issues, compared with the conventional compensation circuit, there is a higher rate to improve the electron mobility and reduce the cost. And having the advantage of being comparable to the above. Although the invention has been disclosed above in the preferred embodiment, It also stipulates that any of the inventions of the present invention may be modified and retouched in the spirit of the present invention. Therefore, the protection of the present invention is defined by the definition of the application. [Simple diagram of the diagram] Port: C. The structure of the organic light-emitting device. Figure 1B shows the active organic light-emitting display. Figure 3A to 3D are conventional compensation circuit diagrams. Fig. 4 is a timing diagram of the present invention. Fig. 5 is a timing diagram of the present invention. Fig. 7 is a graph showing the simulation results of the present invention. Fig. 12 128 im f.doc/006 [Description of main component symbols] 100, 102: Transistor 104: Capacitor 106: Organic light emitting diode 400: Capacitor 402: Light emitting diode 410: Data line driving circuit 412: Gate drive circuit ΤΙ, T2, T3: transistor
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