Abstract:
A pixel region is surrounded in any adjacent scan lines and any adjacent data lines. Two thin film transistor (TFT) groups that are controlled by different scan lines are located in each pixel region. The two data lines respectively send different polarity data to the pixel region through the two TFT groups. At least one capacitor is used to couple with the two TFT groups for providing a coupling effect to make sure the voltage in the two connection points simultaneously goes up and down.

Description:
CROSS-REFERENCE TO RELATED APPLICATIONS  
       [0001]     This application is a continuation-in-part of U.S. application Ser. No. 10/790,824, filed on Mar. 3, 2004, hereby incorporated by reference as it fully set forth herein. The present application also claims priority from, Taiwan Application Serial Number 93120035, filed Jul. 2, 2004, the disclosure of which is hereby incorporated by reference herein in its entirety. 
     
    
     FIELD OF THE INVENTION  
       [0002]     The present invention relates to a driving circuit, and more particularly, to a driving circuit of a liquid crystal display.  
       BACKGROUND OF THE INVENTION  
       [0003]     User demand for entertainment equipment is particularly high as a result of the rapid development of multimedia applications. Conventionally, the cathode ray tube (CRT) display, which is a type of monitor, is commonly used. However, the cathode ray tube display does not meet the needs of multimedia technology because of the large volume thereof. Therefore, many flat panel display techniques such as liquid crystal display (LCD) have been recently developed.  
         [0004]     Conventional LCD panels have narrow view angles so the normal images displayed by them only can be viewed directly in front of the display area. If the display area is watched from an oblique view angle, color distortion occurs in what is viewed, and gray inversion may even occur. That is, what appears black is actually white and what appears white is actually black. Therefore, how to widen the view angle is an important subject for the LCD manufacturers.  
         [0005]     Among various methods for widening the view angle, an LC vertical alignment (VA) technique is still one of the most popular techniques in the current LCD market. However, because liquid crystal molecules are aligned in the same direction (mono-domain vertical alignment), a normal image cannot be seen from a view angle perpendicular to or symmetric to the direction. No matter whether the liquid crystal molecules are realigned in a different direction after the electrical field existing therein changes, the view angle is also limited to the parallel direction of the liquid crystal molecules. Therefore, a multi-domain VA (MVA) technique has been put forth to improve the drawback of the prior art. However, according to MVA technology, additional ridges or bumps are required on the color filter to control the alignment of the tilt direction of liquid crystal molecules and automatically align tilt direction according to their region to which they belong. But because the existence of the bumps results in a need for precise alignment between a color filter and an active matrix substrate, and an additional over-coating must be formed on the color filter, the yield of this LCD panel is reduced and the cost thereof is increased. Therefore, bias-bending vertical alignment (BBVA) technology has been developed to solve the foregoing problem.  
         [0006]      FIG. 1  is a schematic, cross-sectional diagram of a conventional LCD display panel of the bias-bending vertical alignment (BBVA) type. The LCD panel  100  comprises an upper transparent substrate  102 , a lower transparent substrate  104  and a liquid crystal molecule layer  106  between the upper and lower substrates  102  and  104 . A common electrode  108  is located over the upper transparent substrate  102 . Pixel electrodes  1   10  are located over the lower transparent substrate  104 . A main electric field exists between the common electrode  108  and the pixel electrode  110  to make liquid crystal molecules  116  have oblique positions. A control electrode  112  is formed on the lower substrate  104 . An insulation layer  114  is interposed between the control electrode  112  and the pixel electrode  110 . During operation, a bias voltage is generated first between the control electrode  112  and the common electrode  108 . The bias voltage causes the corresponding liquid crystal molecule to be in a saturation state. Then, when another voltage is applied to the pixel electrode  110 , the adjacent liquid crystal molecules are sequentially arranged in a predetermined orientation.  
         [0007]      FIG. 2  is a conventional equivalent circuit diagram of a pixel region implanting BBVA technology. Three thin film transistors are located in each pixel region. The thin film transistors  202  and  204  serve as switches of the pixel electrode voltage (V pixel ). The thin film transistor  206  serve as a switch of the control electrode voltage (V CE ). The three thin film transistors  202 ,  204  and  206  are controlled by the signals from the adjacent scan lines G n-1  and G n .  
         [0008]     When the scan line G n-1  is scanned, the thin film transistors  204  and  206  are on and the thin film transistor  202  is off. At this time, the control electrode voltage (V CE ) and the pixel voltage (V pixel ) are written into the data lines D m-1  and D m  through the thin film transistors  204  and  206 , respectively. Therefore, a voltage difference is built between the control electrode voltage (V CE ) and the pixel voltage (V pixel ). Next, when the scan line G n  is scanned, the thin film transistor  202  is on and the thin film transistors  204  and  206  are off. At this time, the voltage signal transmitted in the data line D m  is written into the pixel region through the thin film transistor  202 . The control electrode voltage (V CE ) is raised or dropped to a specific voltage by the pixel voltage (V pixel ) through a coupling effect generated by a capacitor C 2 .  
         [0009]     However, three thin film transistors are used in the conventional circuit structure designed for BBVA technology, which reduces the aperture ratio. If one of the thin film transistors is damaged, the pixel is considered to be malfunctioning. On the other hand, too many thin film transistors connected to a same scanning line result in a severe RC delay on the scan signal.  
       SUMMARY OF THE INVENTION  
       [0010]     The main purpose of the present invention is to provide a pixel structure of a liquid crystal display implementing the BBVA driving type. According to this structure, the number of the required thin film transistors in a pixel region can be reduced. Therefore, the aperture ratio of the pixel region can be raised and the RC delay phenomenon can be reduced.  
         [0011]     Another purpose of the present invention is to provide a pixel structure of a liquid crystal display implementing the BBVA driving type. According to this structure, it is not necessary to redesign the driving circuit. Therefore, the convenience in use can be improved.  
         [0012]     Yet another purpose of the present invention is to provide a pixel structure of a liquid crystal display in which additional ridges or bumps are not required to change the orientation of the liquid crystal molecules. Therefore, the manufacturing cost can be reduced. The range of the permitted error in the alignment process can be raised to improve the manufacturing yield.  
         [0013]     According to the above purposes of the present invention, a pixel region is surrounded in any adjacent scan lines and any adjacent data lines. Two thin film transistor (TFT) groups controlled by different scan lines are located in each pixel region. The two data lines respectively send different polarity data to the pixel region through the two TFT groups. At least one capacitor is used to couple with the two TFT groups for providing a coupling effect to make sure the voltage in the two connection points simultaneously goes up and down.  
         [0014]     The present invention also provides an operating waveform of this pixel structure. According to the operating waveform, the adjacent scan lines can be maintained at a “high” level together at a specific time to conduct the two thin film transistor groups connected to the adjacent scan lines. At this time, different polarity date signals transmitted in the data lines are written into the control electrode voltage and the pixel electrode voltage through the two thin film transistor groups. Therefore, a voltage difference exists between the control electrode voltage and the pixel electrode voltage.  
       BRIEF DESCRIPTION OF THE DRAWINGS  
       [0015]     The foregoing aspects and many of the attendant advantages of this invention will become more readily appreciated as the same becomes better understood by reference to the following detailed description, when taken in conjunction with the accompanying drawings, wherein:  
         [0016]      FIG. 1  is a schematic, cross-sectional diagram of a conventional liquid crystal display implementing bias-bending vertical alignment (BBVA);  
         [0017]      FIG. 2  illustrates an equivalent circuit diagram of a pixel of a conventional liquid crystal display implementing bias-bending vertical alignment (BBVA);  
         [0018]      FIG. 3  illustrates an equivalent circuit diagram for driving a liquid crystal display implementing bias-bending vertical alignment (BBVA) according to the first embodiment of the present invention;  
         [0019]      FIG. 4  is a waveform diagram of driving signals applied to the pixel in  FIG. 3 ;  
         [0020]      FIG. 5  illustrates an equivalent circuit diagram for driving a liquid crystal display implementing a bias-bending vertical alignment (BBVA) type according to the second embodiment of the present invention;  
         [0021]      FIG. 6A  illustrates a comparison diagram of the control electrode voltage variation (ΔV CE ) in the pixel regions depicted in  FIG. 3  and  FIG. 5  when the scan signals do not select the pixel regions;  
         [0022]      FIG. 6B  illustrates a comparison diagram of the pixel electrode voltage variation (ΔV pixel ) in the pixel regions depicted in  FIG. 3  and  FIG. 5  when the scan signals do not select the pixel regions;  
         [0023]      FIG. 7  illustrates an equivalent circuit diagram for driving a liquid crystal display implementing bias-bending vertical alignment (BBVA) according to the third embodiment of the present invention;  
         [0024]      FIG. 8A  illustrates a comparison diagram of the control electrode voltage variation (ΔV CE ) in the pixel regions depicted in  FIG. 5  and  FIG. 7  when the scan signals do not select the pixel regions; and  
         [0025]      FIG. 8B  illustrates a comparison diagram of the pixel electrode voltage variation (ΔV pixel ) in the pixel regions depicted in  FIG. 5  and  FIG. 7  when the scan signals do not select the pixel regions. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT  
       [0026]      FIG. 3  illustrates an equivalent circuit diagram for driving a liquid crystal display implementing bias-bending vertical alignment (BBVA) according to the first embodiment of the present invention. Only four adjacent pixels are shown in  FIG. 3 , which are formed by scan lines G n-2 , G n-1  and G n  arranged in parallel to each other and crossing data lines D m-2 , D m-1  and D m  arranged in parallel to each other. Each pixel region includes a first thin film transistor T 1 , a second thin film transistor T 2 , a control electrode E CE  with control electrode voltage V CE  and a pixel electrode E pixel  with pixel electrode voltage V pixel .  
         [0027]     In this pixel region surrounded by the adjacent scan lines G n-1  and G n  and the adjacent data lines D m-1  and D m , the gate electrode of the first thin film transistor T 1  is connected to the scan line G n . The source electrode and the drain electrode of the first thin film transistor T 1  are respectively connected to the data line D m  and the pixel electrode E pixel . The gate electrode of the second thin film transistor T 2  is connected to the scan line G n-1 . The source electrode and the drain electrode of the second thin film transistor T 2  are respectively connected to the data line D m-1  and the control electrode E CE . In the pixel configuration of the presented invention, a liquid crystal capacitor C 1  exists between the pixel electrode E pixel  and a common electrode  300 , a capacitor C 2  exists between the control electrode E CE  and the pixel electrode E pixel  and a bias voltage capacitor C 3  is formed between the control electrode E CE  and the common electrode  300 .  
         [0028]      FIG. 4  is a waveform diagram of driving signals applied to the pixel in  FIG. 3 . A dot-inversion driving method is applied to the driving circuit. Accordingly, the polarity states of the adjacent data lines are inversed as shown in  FIG. 4 . The voltage signal V Dm-1  and the voltage signal V Dm  with the reversed polarity states are respectively applied to the data lines D m-1  and D m . The voltage signal V Gn-1  and the voltage signal V Gn  are applied to the scan lines G n  and G n-1 . The driving method of the present invention is to extend the turning on time of the thin film transistors located in the adjacent pixel regions. In other words, the driving signals transmitted by the adjacent scan lines are in the “high” state together during a specific time period. Therefore, the first thin film transistor T 1  and the second thin film transistor T 2  are “on” together during the specific time period.  
         [0029]     The operation method is described in the following when the waveform depicted in  FIG. 4  is applied to the pixel region surrounded by the adjacent scan lines G n-1  and G n  and the adjacent data lines D m-1  and D m . The voltage signal V Dm-1  and the voltage signal V Dm  with the reversed polarity states are respectively applied to the data lines D m-1  and D m . The common electrode voltage is represented by the V com .  
         [0030]     Reference is made to  FIG. 3  and  FIG. 4  together. In the negative time frame period A, at time t 1 , the voltage signal V Gn-1  of the scan line G n-1  is in a “high” state so as to turn on the thin film transistor T 2 . The voltage signal V Gn  of the scan line G n  is in a “low” state so as to turn off the thin film transistor T 1 . At this time, the positive polarity voltage signal V Dm-1  transmitted by the data line D m-1  is written into the control electrode E CE  through the thin film transistor T 2 .  
         [0031]     At time t 2 , the driving signals V Gn-1  and V Gn  respectively transmitted by the adjacent scan lines G n-1  and G Gn  both are in “high” states so as to turn on the thin film transistor T 1  and the thin film transistor T 2 . At this time, the negative polarity voltage signal V Dm-1  transmitted by the data line D m-1  is written into the control electrode E CE  through the thin film transistor T 2 . The positive polarity voltage signal V Dm  transmitted by the data line D m  is written into the pixel electrode E pixel  through the thin film transistor T 1 . Since the written polarity states are inversed, a significant voltage difference exists between the pixel electrode E pixel  and the control electrode E CE . The significant voltage difference is provided to the liquid crystal molecule layer to change their orientations.  
         [0032]     At time t 3 , the voltage signal V Gn-1  of the scan line G n-1  is in a “low” state so as to turn off the thin film transistor T 2 . The voltage signal V Gn  of the scan line G n  is in a “high” state so that the thin film transistor T 1  remains on. At this time, the negative polarity voltage signal V Dm  transmitted by the data line D m  is written into the pixel electrode E pixel  through the thin film transistor T 1 . Since the thin film transistor T 2  is off state, the control electrode E CE  is in a “floating” state. Therefore, the voltage of the control electrode E CE  is further dropped down by the coupling effect of the capacitor C 2  between the control electrode E CE  and the pixel electrode E pixel .  
         [0033]     According to the operating method in the negative time frame, the value of the voltage difference between the control electrode E CE  and the pixel electrode E pixel  is determined at the moment time t 2  ends. At this moment, the voltage polarity of the pixel electrode E pixel  is positive and the voltage polarity of the control electrode E CE  is negative, which is exactly inversed. On the other hand, when time t 2  ends, the voltage difference between the control electrode E CE  and the pixel electrode E pixel  is further dropped down because of the coupling effect of the capacitor C 2 , which provides a larger bias voltage to the liquid crystal molecule to change their orientations.  
         [0034]     Similarly, in the positive time frame period B, at time t 4 , the voltage signal V Gn-1  of the scan line G n-1  is in a “high” state so as to turn on the thin film transistor T 2 . The voltage signal V Gn  of the scan line G n  is in a “low” state so as to turn off the thin film transistor T 1 . At this time, the negative polarity voltage signal V Dm-1  transmitted by the data line D m-1  is written into the control electrode E CE  through the thin film transistor T 2 .  
         [0035]     At time t 5 , the driving signals V Gn-1  and V Gn  respectively transmitted by the adjacent scan lines G n-1  and G Gn  both are in “high” states so as to turn on the thin film transistor T 1  and the thin film transistor T 2 . At this time, the positive polarity voltage signal V Dm-1  transmitted by the data line D m-1  is written into the control electrode E CE  through the thin film transistor T 2 . The negative polarity voltage signal V Dm  transmitted by the data line D m  is written into the pixel electrode E pixel  through the thin film transistor T 1 . Since the written polarity states are inversed, a significant voltage difference exists between the pixel electrode E pixel  and the control electrode E CE . The significant voltage difference is provided to the liquid crystal molecule layer to change their orientations.  
         [0036]     At time t 6 , the voltage signal V Gn-1  of the scan line G n-1  is in a “low” state so as to turn off the thin film transistor T 2 . The voltage signal V Gn  of the scan line G n  is in a “high” state so that the thin film transistor T 1  remains on. At this time, the positive polarity voltage signal V Dm  transmitted by the data line D m  is written into the pixel electrode E pixel  through the thin film transistor T 1 . Since the thin film transistor T 2  is off, the control electrode E CE  is in a “floating” state. Therefore, the voltage of the control electrode E CE  is further raised up by the coupling effect of the capacitor C 2  between the control electrode E CE  and the pixel electrode E pixel .  
         [0037]     According to the operating method in the positive time frame, the value of the voltage difference between the control electrode E CE  and the pixel electrode E pixel  is determined in the moment while time t 5  is over. At this moment, the voltage polarity of the pixel electrode E pixel  is negative and the voltage polarity of the control electrode E CE  is positive, which is exactly inversed. On the other hand, when time t 5  ends, the voltage difference between the control electrode E CE  and the pixel electrode E pixel  is further raised up because of the coupling effect of the capacitor C 2 , which can provide a larger bias voltage to the liquid crystal molecule to change their orientations.  
         [0038]     In other words, according to the operating method used in the positive time frame of the present invention, the voltage relationship between the control electrode E CE  and the pixel electrode E pixel  is that the pixel electrode voltage V pixel  is larger than common electrode voltage V com  and the control electrode voltage V CE  is larger than the pixel electrode voltage V pixel . Therefore, the following is the relationship between the three voltages, V pixel , V com  and V CE : 
 
V CE &gt;V pixel &gt;V com  
 
         [0039]     According to the operating method used in the negative time frame of the present invention, the pixel electrode voltage V pixel  is less than common electrode voltage V com  and the control electrode voltage V CE  is less than the pixel electrode voltage V pixel . Therefore, the following is the relationship between the three voltages, V pixel , V com  and V CE : 
 
V com &gt;V pixel &gt;V CE  
 
         [0040]     When the thin film transistor T 2  is off, the control electrode E CE  is in a “floating” state. At this time, the voltage of the control electrode E CE  is further raised up or pulled down by the coupling effect of the capacitor C 2  between the control electrode E CE  and the pixel electrode E pixel . Such situation could result in too great a voltage difference being applied to the source electrode and the drain electrode when the thin film transistor T 2  is off. This too-great voltage difference would then cause a leakage current in the thin film transistor T 2  to pull down the voltage of the control electrode E CE  that is in a “floating” state. Before this pixel region is scanned by the scan signal again, when the thin film transistor T 1  and the thin film transistor T 2  are both off, at this time, both the control electrode E CE  and the pixel electrode E pixel  are in “floating” states. Therefore, the voltage decrease of the control electrode E CE  pulls down the voltage of the pixel electrode E pixel  because of the coupling effect of the capacitor C 2  between the control electrode E CE  and the pixel electrode E pixel , which causes a flicker phenomenon in the display.  
         [0041]      FIG. 5  illustrates an equivalent circuit diagram for driving a liquid crystal display implementing a bias-bending vertical alignment (BBVA) type according to the second embodiment of the present invention. For avoiding a leakage current generated in the thin film transistor T 2  because of too great voltage difference being applied to the source and drain electrode, two thin film transistors T 2 ′ and T 2 ″ arranged in series are used in the second embodiment to replace the thin film transistor T 2  in the first embodiment. According to the structure of the second embodiment, the voltage originally applied to the source and drain electrode of the thin film transistor T 2  can be spread to the two thin film transistors T 2 ′ and T 2 ″ arranged in series. Therefore, the cross voltage in the source and drain electrode of each thin film transistor is reduced so as to reduce the leakage current. The smaller leakage current smoothes the voltage change of the control electrode E CE  that is in “floating” state. Of course, the voltage change of the pixel electrode E pixel  because of the coupling effect generated by the capacitor C 2  also can be smoothed. Therefore, the flicker phenomenon can be reduced. It is noted that the first embodiment and the second embodiment have the same operating method and the operating waveform diagram.  
         [0042]      FIG. 6A  illustrates a comparison diagram of the control electrode voltage variation (ΔV CE ) in the pixel regions depicted in  FIG. 3  and  FIG. 5  when the scan signals do not select the pixel regions. According to this diagram, when the control electrode voltage V CE  is applied to the source and drain electrode of the thin film transistor T 2  illustrated in  FIG. 3 , the voltage variation (ΔV CE ) of the control electrode (E CE ) is 1.72 volts during the positive polarity period of the dot inversion driving method. The voltage variation (ΔV CE ) of the control electrode (E CE ) is 1.41 volts during the negative polarity period of the dot inversion driving method. On the other hand, when the control electrode voltage V CE  is applied to the source and drain electrode of the in-series thin film transistors T 2 ′ and T 2 ″ illustrated in  FIG. 5 , the voltage variation (ΔV CE ) of the control electrode (E CE ) is  1 . 08  volts during the positive polarity period of the dot inversion driving method. On the other hand, the voltage variation (ΔV CE ) of the control electrode (E CE ) is 0.81 volts during the negative polarity period of the dot inversion driving method.  
         [0043]      FIG. 6B  illustrates a comparison diagram of the pixel electrode voltage variation (ΔV pixel ) in the pixel regions depicted in  FIG. 3  and  FIG. 5  when the scan signals do not select the pixel regions. According to this diagram, when the control electrode voltage V CE  is applied to the source and drain electrode of the thin film transistor T 2  illustrated in  FIG. 3 , the pixel electrode voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔE pixel ) is 0.821 volts during the positive polarity period of the dot inversion driving method. The pixel electrode voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (Δ pixel ) is 0.757 volts during the negative polarity period of the dot inversion driving method. On the other hand, when the control electrode voltage V CE  is applied to the source and drain electrode of the in-series thin film transistors T 2 ′ and T 2 ″ illustrated in  FIG. 5 , the pixel electrode voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔV CE ) is 0.5912 volts during the positive polarity period of the dot inversion driving method. On the other hand, the pixel electrode voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔV CE ) is 0.5273 volts during the negative polarity period of the dot inversion driving method.  
         [0044]     According to the comparison diagrams illustrated in  FIG. 6A  and  FIG. 6B , the leakage current in a pixel region is obviously improved by using in-series thin film transistors T 2 ′ and T 2 ″ to replace the thin film transistor T 2  to reduce the cross voltage connected to the source and drain electrode. Therefore, the voltage variations ΔE pixel  and ΔV pixel  is improved so as to reduce the flicker phenomenon.  
         [0045]      FIG. 7  illustrates an equivalent circuit diagram for driving a liquid crystal display implementing a bias-bending vertical alignment (BBVA) type according to the third embodiment of the present invention. Typically, a parasitic capacitor C gd  exists between the gate electrode and the drain electrode in a thin film transistor. A parasitic capacitor C gs  exists between the gate electrode and the source electrode in a thin film transistor. Therefore, when using in-series thin film transistors T 2 ′ and T 2 ″ with a common connection V m  (illustrated in  FIG. 5 ) to replace the thin film transistor T 2  (illustrated in  FIG. 3 ), parasitic capacitors C gs  and C gd  exist between the gate electrode, the drain electrode, the source electrode and the common connection V m .  
         [0046]     When the scan signal applied to the scan line G n-1  is switched from a “high” level to a “low” level, the voltage in the common connection V m  is pull down again due to the parasitic capacitors C gs  and C gd . At this time, the voltage difference of the drain electrode and the source electrode of the thin film transistor T 2 ′ is enlarged to generate a leakage current. Therefore, for further reducing the leakage current phenomenon, an additional capacitor C 4  is cross-connected to the source electrode and the drain electrode of the thin film transistor T 2 ′ in the third embodiment. It is noted that the first embodiment and the third embodiment have the same operating method and the operating waveform diagram.  
         [0047]     By using the capacitor C 4 , when the scan signal applied to the scan line G n-1  is switched from a “high” level to a “low” level, the control electrode voltage V CE  restrains the voltage in the common connection V m  to be pulled down again due to the coupling effect of the capacitor C 4 . Therefore, the voltage difference of the drain electrode and the source electrode of the thin film transistor T 2 ′ is not enlarged so that the leakage current phenomenon can be reduced.  
         [0048]      FIG. 8A  illustrates a comparison diagram of the control electrode voltage variation (ΔV CE ) in the pixel regions depicted in  FIG. 5  and FIG.  7  when the scan signals do not select the pixel regions. According to this diagram, when an additional capacitor is not used to cross-connect the source electrode and the drain electrode of the thin film transistor T 2 ′ illustrated in  FIG. 5 , the voltage variation (ΔV CE ) of the control electrode (E CE ) is 1.08 volts during the positive polarity period of the dot inversion driving method. The voltage variation (ΔV CE ) of the control electrode (E CE ) is 0.81 volts during the negative polarity period of the dot inversion driving method. On the other hand, when an additional capacitor is used to cross-connect the source electrode and the drain electrode of the thin film transistor T 2 ′ illustrated in  FIG. 7 , the voltage variation (ΔV CE ) of the control electrode (E CE ) is 0.68 volts during the positive polarity period of the dot inversion driving method. On the other hand, the voltage variation (ΔV CE ) of the control electrode (E CE ) is 0.99 volts during the negative polarity period of the dot inversion driving method.  
         [0049]     On the other hand,  FIG. 8B  illustrates a comparison diagram of the pixel electrode voltage variation (ΔV pixel ) in the pixel regions depicted in  FIG. 5  and  FIG. 7  when the scan signals do not select the pixel regions. When an additional capacitor is not used to cross-connect the source electrode and the drain electrode of the thin film transistor T 2 ′ illustrated in  FIG. 5 , the pixel voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔV CE ) is 0.5912 volts during the positive polarity period of the dot inversion driving method. The pixel voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔV CE ) is 0.5273 volts during the negative polarity period of the dot inversion driving method. On the other hand, when an additional capacitor is used to cross-connect the source electrode and the drain electrode of the thin film transistor T 2 ′ illustrated in  FIG. 7 , the pixel voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔV CE ) is 0.42 volts during the positive polarity period of the dot inversion driving method. On the other hand, the pixel voltage variation (ΔV pixel ) resulting from the control electrode voltage variation (ΔV CE ) is 0.595 volts during the negative polarity period of the dot inversion driving method.  
         [0050]     According to the comparison diagrams illustrated in  FIG. 8A  and  FIG. 8B , the leakage current in a pixel region is obviously improved by using an additional capacitor to cross-connect the source electrode and the drain electrode of the thin film transistor T 2 ′. Therefore, the voltage variations ΔE pixel  and ΔV pixel  is improved so as to reduce the flicker phenomenon As a whole, there are two thin film transistor groups in each pixel region according to the present invention. The two thin film transistor groups are controlled by different scan lines and receive the data signals from different data lines. At least one capacitor is used to couple the two thin film transistor groups. When operating, adjacent scan lines are kept in a “high” level in a specific scan time to turn on the two thin film transistor groups together. Different polarity signals are respectively transmitted to this pixel region through the two thin film transistor groups to form a voltage difference between the control electrode and pixel electrode. A multiple domain effect results. In other words, additional ridges or bumps are not required in the liquid crystal display to change the orientation of the liquid crystal molecules. Therefore, the manufacturing cost can be reduced. The range of the permitted error in the alignment process can be broadened to improve the manufacturing yield.  
         [0051]     On the other hand, the number of the required thin film transistors in a pixel region can be reduced. Therefore, the aperture ratio of the pixel region can be raised and the RC delay phenomenon can be reduced.  
         [0052]     As is understood by a person skilled in the art, the foregoing preferred embodiments of the present invention are illustrative of the present invention rather than limiting of the present invention. It is intended that this description cover various modifications and similar arrangements included within the spirit and scope of the appended claims, the scope of which should be accorded the broadest interpretation so as to encompass all such modifications and similar structure.