Abstract:
A light-emitting display device with low power consumption and its driving method. In the driving method of a light-emitting display wherein light-emitting elements are connected to the intersections of positive electrode lines and negative electrode lines arranged in a matrix, either one of the positive electrode lines or the negative electrode lines are employed as scan lines with the other employed as drive lines; while scanning the scan lines, drive sources are connected to desired drive lines in synchronization with the scan, whereby allowing the light-emitting elements connected to the intersections of the scan lines and drive lines to emit light, a first reset voltage is applied to all of the scan lines and a second relet voltage that is greater than the first reset voltage is applied to all of the drive lines during a reset period after a scan period for scanning an arbitrary scan line is completed and before scanning the following scan line is started.

Description:
BACKGROUND OF THE INVENTION  
         [0001]    1. Field of the Invention  
           [0002]    The present invention relates to a light-emitting display device that employs light-emitting elements such as organic EL (electroluminescent) elements and a driving method therefor.  
           [0003]    2. Description of Related Art  
           [0004]    In recent years, organic EL elements that are self-light-emitting elements employing organic compounds have been extensively studied, and dot matrix displays employing an organic EL element have been developed as well.  
           [0005]    [0005]FIG. 1 shows an equivalent circuit of an organic EL element. FIG. 2A shows the current luminance properties of the organic EL element, FIG. 2B shows the voltage-current properties of the organic EL element, and FIG. 2C shows the voltage luminance properties.  
           [0006]    As shown in FIG. 1, the organic EL element can be represented by a light-emitting element E having diode properties, and the parasitic capacitance C connected in parallel to the light-emitting element E and the resistance R connected in series with the light-emitting element E.  
           [0007]    As shown in FIGS. 2A through 2C, the organic EL element emits light with luminance in proportion to current. In the case where the driving voltage is less than the predetermined light emission specifying voltage Vth, it allows current to hardly flow, resulting in practically no emission.  
           [0008]    [0008]FIG. 3 shows a driving method of a prior art light-emitting element.  
           [0009]    The driving method shown in FIG. 3 is called the passive matrix driving method, in which the positive electrode lines Al through A 4  and the negative electrode lines B 1  through Bn (n is a natural number. Four positive electrode lines are used for ease of explanation) are arranged in a matrix (grid). To each intersection of the positive electrode lines and the negative electrode lines arranged in a matrix, light-emitting elements E 11  through E 4 n are connected. Either one of the positive electrode lines or the negative electrode lines are selected for scanning at constant intervals of time and other lines are driven by the constant-current sources  21  through  24 , whereby light-emitting elements at arbitrary intersections are allowed for emitting light in synchronization with the scanning.  
           [0010]    A voltage source may be used for the driving source, however, a current source may be preferably used to provide better reproducibility of luminance. This is because current luminance properties are more stable against changes in environmental temperature than voltage luminance properties, and current luminance properties of light-emitting elements have a linear proportionality.  
           [0011]    In the case of FIG. 3, the driving source employs constant-current sources with the amount of constant current sufficient for the desired instantaneous luminance. Therefore, when the instantaneous luminance of light-emitting elements is desired to be equal to Lx, as shown in FIGS. 2A through 2C, the amount of constant current of a driving source is to be set to Ix. Also the voltage across both ends of the light-emitting element (hereinafter designated the light emission specifying voltage) becomes V x  when light is emitted with desired instantaneous luminance (hereinafter designated a steady state of light emission).  
           [0012]    There are two driving methods by means of said driving sources, namely, scanning negative electrode lines and driving positive electrode lines, and scanning positive electrode lines and driving negative electrode lines. FIG. 3 shows the method of scanning negative electrode lines and driving positive electrode lines. The negative electrode line scan circuit,  1 , is connected to the negative electrode lines B 1  through Bn. The positive electrode line drive circuit  2  that comprises the current sources  21  through  24  and the drive switches  31  through  34  are also connected to the positive electrode lines A 3  through A 4 .  
           [0013]    The negative electrode line scan circuit  1  performs scanning while sequentially switching the scan switches  11  through  1 n over to the ground terminal sides at constant intervals of time, thereby providing negative electrode lines B 1  through Bn with ground potential (0V) in sequence. Furthermore, the positive electrode line drive circuit  2  controls the on and off of the drive switches  31  through  34  in synchronization with the switch scanning of said negative electrode line scan circuit  1 . This allows the positive electrode lines A 1  through A 4  to be connected with the constant-current sources  21  through  24  to supply driving current to light-emitting elements located at desired intersections. These negative electrode line scan circuit  1  and the positive electrode line drive circuit  2  are drive-controlled by means of a control circuit that is not shown.  
           [0014]    For example, a case where the light-emitting elements E 11  and E 21  are lit is taken as an example. As shown in the drawing, when the scan switch  11  of the negative electrode line scan circuit  1  is switched to the ground side with the ground potential applied to the first negative electrode line B 1 , the drive switches  31  and  32  of the positive electrode line drive circuit  2  are preferably switched over to the sides of the constant-current sources to connect the constant-current sources  21  and  22  to the positive electrode lines A 1  and A 2 . By repeating the scanning and driving at a high speed, control is performed in a manner such that light-emitting elements at arbitrary positions are lit as if each light-emitting element emits light at the same time.  
           [0015]    Other negative electrode lines B 2  through Bn except for negative electrode line B 1  that is being scanned are connected with the constant voltage sources  42  through  4 n to apply a reverse bias voltage V1 that has the same potential as the light emission specifying voltage V x . This prevents the light-emitting elements E 12  through E 1 n and E 22  through E 2 n, connected to the positive electrode lines A 1  and A 2 , emitting light accidentally.  
           [0016]    The reverse bias voltage sources  41  through  4 n, which provide the reverse bias voltage V1, are provided so that light-emitting elements connected to the intersections of the positive electrode lines A 1  and A 2  to be driven and the negative electrode lines B 2  through Bn not to be scanned (E 12  through E 1 n and E 22  through E 2 n in the case of FIG. 3) do not emit light accidentally. Accordingly, the voltage applied thereto is preferably set in a manner such that the voltage across both ends of the light-emitting element is equal to or less than the light emission threshold voltage Vth. However, the reverse bias voltage V1 is best set to the light emission specifying voltage V x  for the reason mentioned below. That is, letting V1=V x  causes the voltage across both ends of the light-emitting element to become 0, and thus the current supplied by the drive source flows only into the light-emitting elements that are emitting light, thereby reproducing a desired luminance in accuracy.  
           [0017]    As mentioned above referring to FIG. 3, the state of charge of each parasitic capacitance of each light-emitting element is as follows. The light-emitting elements E 11  and E 21  connected to the intersections of the positive electrode lines A 1  and A 2  to be driven and the negative electrode line B 1  to be scanned are forward charged. The light-emitting elements E 11  through E 1 n and E 22  through E 2 n connected to the intersections of the positive electrode lines A 1  and A 2  to be driven and the negative electrode lines B 2 , B 3 , and B 4 , which are not scanned, are not charged. The light-emitting elements E 31  and E 41  connected to the intersections of the positive electrode lines A 3  and A 4  not to be driven and the negative electrode line B 1  to be scanned are not charged. The light-emitting elements E 32  through E 3 n and E 42  through E 4 n, connected to the intersections of the positive electrode lines A 3  and A 4 , which are not driven, and the negative electrode lines B 2 , B 3 , and B 4 , which are not scanned, are reverse charged. (In the drawing, each light-emitting element E is represented by the symbol of a capacitor, a light-emitting element that is lit is represented by the symbol of a diode, and a capacitor that is charged is shaded.)  
           [0018]    This driving method, however, had the following problem caused by parasitic capacitance C in the equivalent circuit of a light-emitting element shown in FIG. 1. The problem will be explained below.  
           [0019]    In FIGS. 7A and 7B, the light-emitting elements E 11  through E 1 n connected to said positive electrode line A 1  in FIG. 3 are extracted with each of the light-emitting elements E 11  through E 1 n shown only by said parasitic capacitance C. In a case where the positive electrode line A 1  is not driven at the time of scanning the negative electrode line B 1 , the parasitic capacitors C 12  through Cln of the light-emitting elements E 12  through E 1 n other than the parasitic capacitor C 11  of the light-emitting element E 11  connected to the negative electrode line B 1  which is currently scanned, are charged by the reverse bias voltage V1 applied to each of the negative electrode lines B 2  through Bn which are charged in the direction as shown in FIG. 7A.  
           [0020]    When the scanning position is shifted from the negative electrode line B 1  to the following negative electrode line B 2 , the positive electrode line A 1  is driven to cause, for example, the light-emitting element E 12  to emit light providing the circuit status as shown in FIG. 7B. At the instant circuits are switched over like this, not only is the parasitic capacitor of the light-emitting element E 12  that is to be lit charged but also other parasitic capacitors of the light-emitting elements E 13  through E 1 n connected to other negative electrode lines B 3  through Bn are charged by letting current flow therein in the direction shown with the arrows.  
           [0021]    As mentioned in the foregoing, a light-emitting element is not allowed to emit light with a desired luminance unless the voltage across both ends thereof reaches the light emission specifying voltage V x . According to the prior art driving method, as shown in FIGS. 7A and 7B in the foregoing, when the positive electrode line A 1  is driven to allow the light-emitting element E 12  connected to the negative electrode line B 2  to emit light, which causes not only the parasitic capacitor of the light-emitting element E 12  that to be lit but also other light-emitting elements E 13  through E 1 n that are connected to the positive electrode line A 1  to be charged. Thus, until the parasitic capacitors of all these light-emitting elements have been completely charged, the voltage across both ends of the light-emitting element E 12  connected to the negative electrode line B 2  is not allowed to reach the light emission specifying voltage V x .  
           [0022]    Accordingly, in the prior art driving method, there was a problem in that the rate of rise was slow until light emission was fired and a high-speed scanning could not be performed.  
           [0023]    Said problem would exert adverse effects with the increasing number of light-emitting elements. Especially, in the case of employing organic EL elements as light-emitting elements, the effect of said problem would be brought to the fore since organic EL elements have a large parasitic capacitance C due to the surface light emission scheme thereof.  
           [0024]    A driving method for solving the aforementioned problem is disclosed in Japanese Patent Kokai No. Hei 9-232074.  
           [0025]    The driving method disclosed in said publication will be explained referring to FIG. 3 through FIG. 6. FIG. 3 is a view for explaining the state of light emission A, FIG. 4 is a view for explaining the state of reset, FIG. 5 is view for explaining the transition to the state of light emission B, and FIG. 6 is a view for explaining the state of light emission B.  
           [0026]    For explanation, taken as an example is the case of shifting from a state where the light-emitting elements E 11  and E 12  are lit at the time of scanning the negative electrode line B 1 , through the reset period shown in FIG. 4, and then to a state where the light-emitting elements E 22  and E 32  are lit at the time of scanning the negative electrode line B 2  as shown in FIG. 5 and FIG. 6.  
           [0027]    The point in said publication is that, in the case of allowing the light-emitting elements E 22  and E 32  to emit light following the light-emitting elements E 11  and E 21 , a reset period is provided for resetting the voltages across both ends of all light-emitting elements E 11  through E 4 n to 0 potential while scanning is switched from the negative electrode line B 1  over to the negative electrode line B 2  to allow charge accumulated in parasitic capacitors C to be discharged.  
           [0028]    That is, as shown in FIG. 4, all scan switches  11  through  1 n connected to the negative electrode lines are connected to the ground side, and all drive switches  31  through  34  connected to the positive electrode lines are connected to the ground side, and thus the charge accumulated in the parasitic capacitors of all light-emitting elements E 11  through E 4 n are discharged.  
           [0029]    Once all light-emitting elements have been completely reset, scanning is shifted to the negative electrode line B 2  to address the light-emitting elements E 22  and E 32  as shown in FIG. 5.  
           [0030]    That is, the negative electrode line B 2  is connected to the ground potential, the negative electrode lines B 1  and B 3  through Bn are also connected with the reverse bias voltage sources  41  and  43  through  4 n, the positive electrode lines A 2  and A 3  to which the light-emitting elements E 22  and E 32  are connected are connected to the constant-current sources  22  and  23 , and the remaining positive electrode lines A 1  and A 4  are connected to the ground potential.  
           [0031]    As mentioned above, at the instant the scan switches  11  through in and drive switches  31  through  34  are switched over, the potential of the positive electrode lines A 2  and A 3  becomes approximately equal to V1 (more precisely n−1/n·V1), and the voltage across both ends of the light-emitting elements E 22  and E 32  becomes a forward bias voltage approximately equal to the light emission specifying voltage V x . Hence, the light-emitting elements E 22  and E 32  are quickly charged by the current from a plurality of routes shown with arrows in FIG. 5, and then are allowed to shift to a steady state of light emission shown in FIG. 6 instantaneously. In FIG. 6, the driving current supplied by the constant-current sources  22  and  23  flows only into the light-emitting elements E 22  and E 32  respectively, so that the light-emitting elements E 22  and E 32  are allowed to emit light with a desired instantaneous luminance Lx.  
         OBJECTS AND SUMMARY OF THE INVENTION  
         [0032]    In the conventional driving method mentioned above, the problem relating to the rate in rise of light emission was eliminated. However, there still was a problem that power consumption increases since the charge accumulated in light-emitting elements is to be discharged completely each time scanning is shifted. Furthermore, the possibility of losing the display quality of images is developed due to the provision of the non-light emission period of a reset period at each time of scanning.  
           [0033]    An object of the present invention is to provide a light-emitting display device with low power consumption and the driving method therefor. Another object is to improve display quality.  
           [0034]    According to a first aspect of the present invention, in the driving method of a light-emitting display wherein light-emitting elements are connected to the intersections of positive electrode lines and negative electrode lines arranged in a matrix, either one of the positive electrode lines or the negative electrode lines are employed as scan lines with the other employed as drive lines; while scanning the scan lines, drive sources are connected to desired drive lines in synchronization with the scanning, whereby allowing the light-emitting elements connected to the intersections of the scan lines and drive lines to emit light,  
           [0035]    during a reset period after a scan period for scanning an arbitrary scan line is complete and before scanning the following scan line is started, a first reset voltage is applied to all of the scan lines and a second reset voltage that is greater than the first reset voltage is applied to all of the drive lines.  
           [0036]    According to another aspect of the present invention, the difference between the second reset voltage and the first voltage is set to be lower than the light emission threshold voltage of the light-emitting element.  
           [0037]    According to still another aspect of the present invention, the drive lines are connectable to either the drive source or a second reset voltage source for providing the second reset voltage, and the scan lines are connectable to either a first reset voltage source for providing the first reset voltage or a reverse bias voltage source for providing a predetermined reverse bias voltage.  
           [0038]    According to still another aspect of the present invention, the first reset voltage source provides the ground potential.  
           [0039]    According to still another aspect of the present invention, the reverse bias voltage source is almost the same as the voltage value determined by subtracting the second reset voltage from the light emission specifying voltage of a light-emitting element.  
           [0040]    According to still another aspect of the present invention, during the reset period, all of the drive lines are connected to the second reset voltage source and all of the scan lines are connected to the first reset voltage source.  
           [0041]    According to still another aspect of the present invention, during the scan period, scan lines to be scanned are connected to the first reset voltage source, scan lines not to be scanned are connected to the reverse bias voltage source, drive lines to be driven are connected to the drive sources, and drive lines not to be driven are connected to the second reset voltage source.  
           [0042]    According to still another aspect of the present invention, the drive lines are connectable to either one of the drive sources, the second reset voltage source for providing the second reset voltage, or grounding means for providing the ground potential, the scan lines are connectable to either the first reset voltage source for providing the first reset voltage or the reverse bias voltage source for providing a predetermined reverse bias voltage.  
           [0043]    According to still another aspect of the present invention, the first reset voltage source provides the ground potential.  
           [0044]    According to still another aspect of the present invention, the reverse bias voltage source has almost the same voltage as the light emission specifying voltage of light-emitting elements.  
           [0045]    According to still another aspect of the present invention, during the reset period, all of the drive lines are connected to the second reset voltage source and all of the scan lines are connected to the first reset voltage source.  
           [0046]    According to still another aspect of the present invention, during the scan period, scan lines to be scanned are connected to the first reset voltage source, scan lines not to be scanned are connected to the reverse bias voltage source, drive lines to be driven are connected to the drive sources, and drive lines not to be driven are connected to the grounding means.  
           [0047]    According to still another aspect of the present invention, the light-emitting elements are organic EL elements.  
           [0048]    According to still another aspect of the present invention, the drive sources are constant-current sources.  
           [0049]    According to still another aspect of the present invention, in a light-emitting display device in which light-emitting elements are connected to intersections of positive electrode lines and negative electrode lines arranged in a matrix, either one of the positive electrode lines or the negative electrode lines are employed as scan lines with the other employed as drive lines, a scan period during which drive sources are connected to desired drive lines while scanning the scan lines in synchronization with the scan and thus the light-emitting elements connected to the intersections of the scan lines and drive lines are lit, and a reset period for providing reset voltage for light-emitting elements are alternately repeated for display by light emission, the light-emitting display device comprises: scan switch means for enabling either of grounding means for providing a ground potential or a reverse bias voltage source for providing a predetermined reverse bias voltage to connect to each of the scan lines; drive switch means for enabling either of the drive source or reset voltage sources for providing the reset voltage to connect to each of the drive lines; and control means for controlling the switching of the scan switch means and the drive switch means in accordance with light emission data being inputted.  
           [0050]    According to still another aspect of the present invention, the reset voltage is set to be lower than the light emission threshold voltage of the light-emitting elements.  
           [0051]    According to still another aspect of the present invention, the reverse bias voltage source has almost the same voltage as the voltage determined by subtracting the reset voltage from the light emission specifying voltage of light-emitting elements.  
           [0052]    According to still another aspect of the present invention, during the reset period, all of the scan switch means are connected to the grounding means and the drive switch means are connected to the reset voltage source.  
           [0053]    According to still another aspect of the present invention, during the scan period, the scan switch means to be scanned are connected to the grounding means, the scan switch means not to be scanned are connected to the reverse bias voltage sources, the drive switch means to be driven are connected to the drive sources, and the drive switch means not to be driven are connected to the reset voltage sources.  
           [0054]    According to still another aspect of the present invention, the drive switch means allow for selectively connecting to either one of the drive sources, the reset voltage sources, or grounding means for providing the ground potential.  
           [0055]    According to still another aspect of the present invention, the voltage of the reverse bias voltage source is set to be almost the same as the light emission specifying voltage of the light-emitting elements.  
           [0056]    According to still another aspect of the present invention, during the reset period, all of scan switch means are connected to the grounding means and the drive switch means are connected to the reset voltage sources.  
           [0057]    According to still another aspect of the present invention, during the scan period, the scan switch means to be scanned are connected to the grounding means, the scan switch means not to be scanned are connected to the reverse bias voltage sources, the drive switch means to be driven are connected to the drive sources, and the drive switch means not to be driven are connected to the grounding means.  
           [0058]    According to still another aspect of the present invention, the light-emitting elements are organic EL elements.  
           [0059]    According to still another aspect of the present invention, the drive sources are constant-current sources. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0060]    [0060]FIG. 1 is a view showing an equivalent circuit of an organic EL element,  
         [0061]    [0061]FIGS. 2A through 2C are views for explaining the relationship between the light emission luminance, drive voltage, and drive current of an organic EL element,  
         [0062]    [0062]FIG. 3 is a view showing a configuration of the prior art under light emission status A,  
         [0063]    [0063]FIG. 4 is a view showing a configuration of the prior art under reset status,  
         [0064]    [0064]FIG. 5 is a view showing a configuration of the prior art at the time of switchover to light emission status B,  
         [0065]    [0065]FIG. 6 is a view showing a configuration of a prior art under light emission status B,  
         [0066]    [0066]FIGS. 7A and 7B are views for explaining the status of charging and discharging according to the prior art,  
         [0067]    [0067]FIG. 8 is a view showing a configuration of the first embodiment of the present invention under light emission status A,  
         [0068]    [0068]FIG. 9 is a view showing a configuration of the first embodiment of the present invention under reset status,  
         [0069]    [0069]FIG. 10 is a view showing a configuration of the first embodiment of the present invention at the time of switchover to light emission status B,  
         [0070]    [0070]FIG. 11 is a view showing a configuration of the first embodiment of the present invention under light emission status B,  
         [0071]    [0071]FIG. 12 is a view showing a configuration of the second embodiment of the present invention under light emission status A,  
         [0072]    [0072]FIG. 13 is a view showing a configuration of the second embodiment of the present invention under reset status,  
         [0073]    [0073]FIG. 14 a view showing a configuration of the second embodiment of the present invention at the time of switchover to light emission status B,  
         [0074]    [0074]FIG. 15 is a view showing a configuration of the second embodiment of the present invention under light emission status B,  
         [0075]    [0075]FIG. 16 is a view for explaining the operation of a light-emitting element of the second embodiment, and  
         [0076]    [0076]FIG. 17 is a diagram showing an example of the structure of the light emission control circuit  3 . 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0077]    Referring to FIG. 8 through FIG. 11, an embodiment of the present invention will be explained. In the embodiment to be explained below, it is to be understood that light-emitting elements are to be emitted at the same instantaneous luminance L x  as that of the prior art, and the constant current I x  of a constant-current source and the light emission specifying voltage V x  are to be set to the same value as that of the prior art.  
         [0078]    [0078]FIG. 8 through FIG. 11 are views showing the configuration of a first embodiment of the present invention, FIG. 8 shows the light emission status A, FIG. 9 shows the reset status, FIG. 10 shows the time of switchover to the light emission status B, and FIG. 11 shows the light emission status B.  
         [0079]    Referring to FIG. 8 through FIG. 11, A 1  through A 4  are positive electrode lines (it is to be understood that there are more than four lines normally, however, there are provided only four lines for convenience of explanation), and B 1  through Bn are negative electrode lines (n is a natural number). E 11  through E 4 n are light-emitting elements, such as organic EL (electroluminescent) elements, connected to each intersection.  1  is the negative electrode line scan circuit,  2  is the positive electrode line drive circuit, and  3  is the light emission control circuit to which light emission data is supplied. The light emission control circuit  3  may be a control circuit of a known structure that provides driving signals of the negative electrode scan circuit  1  and the positive electrode line drive circuit  2 . For instance, a one-chip microcomputer  30  having a ROM, a RAM, and an I/O port may be used in the light emission control circuit  3  as shown in FIG. 17. In such a case, the microcomputer  30  previously stores a program for producing driving signals of the negative electrode line scan circuit  1  and the positive electrode line drive circuit  2  which will be describe below in synchronism with the incoming light emission data.  
         [0080]    As shown in FIG. 8, the negative electrode scan circuit  1  is provided with scan switches  11  through In for scanning each negative electrode line B 1  through Bn in sequence. One terminal of each scan switch  11  through In is connected to reverse bias voltage sources  41  through  4 n for providing reverse bias voltages with the other terminals connected to the ground potential (0V), respectively.  
         [0081]    The reverse bias voltage sources  41  through  4 n were intended to apply V1 as the reverse bias voltage, the same voltage as the light emission specifying voltage V x  in the prior art. However, the present embodiment employs V1−V2, which is a voltage lower than that of the prior art, as the reverse bias voltage. V2 will be explained later.  
         [0082]    The positive electrode drive circuit  2  is provided with the constant-current sources  21  through  24  as drive sources, the reset voltage sources  51  through  54  for providing reset voltage V2, and the drive switches  31  through  34  for selecting each positive electrode line A 1  through A 4 . Turning on an arbitrary drive switch to the constant-current source side allows for connecting the current sources  21  through  24  to the corresponding positive electrode lines.  
         [0083]    Positive electrode lines that are not driven during scan are connected to the reset voltage sources  51  through  54 . As mentioned later, the reset voltage sources  51  through  54  are connected with the positive electrode lines A 1  through A 4  during reset, thereby applying the reset voltage V2 to all light-emitting elements E 11  to E 4 n in the forward direction.  
         [0084]    The reset voltage V2 is made lower than the light-emitting threshold voltage V TH  of light-emitting elements, thereby preventing light-emitting elements from emitting light during reset. As mentioned, the positive electrode line drive circuit  2  is different from the prior art in the points that the positive electrode line drive circuit  2  is provided with the reset voltage sources  51  through  54  for providing the reset voltage V2, and positive electrode lines that are not driven are connected to the reset voltage sources  51  through  54 .  
         [0085]    The light emission control circuit  3  controls turning on and off of the scan switches  11  through ln and the drive switches  31  through  34 .  
         [0086]    Referring to FIG. 8 through FIG. 11, the light emission operation of the first embodiment will be explained below.  
         [0087]    Like the prior art example, the operation to be described below is an example in which negative electrode line B 1  is scanned to cause light-emitting elements E 11  and E 21  to emit light and then light-emitting elements E 22  and E 32  to emit light by scanning the negative electrode line B 2 .  
         [0088]    First, referring to FIG. 8, the scan switch  11  is switched to the ground and the negative electrode line B 1  is scanned. To other negative electrode lines B 2  through Bn, the scan switches  12  through  1 n allow the reverse bias voltage sources  41  through  4 n to apply V1−V2. Furthermore, the positive electrode lines A 1  and A 2  are connected with the constant-current sources  21  and  22  by means of the drive switches  31  and  32 . In addition, other positive electrode lines A 3  and A 4  are connected with the reset voltage sources  53  and  54 , and the reset voltage V2 is applied thereto.  
         [0089]    Therefore, as shown with arrows in FIG. 8, drive current flows only into the light-emitting elements E 11  and E 21  from the constant-current sources  21  and  22  to cause only the light-emitting elements E 11  and E 21  to emit light under a steady state of light emission.  
         [0090]    As shown in FIG. 8, a voltage of V2 is applied to light-emitting elements E 31 , E 41 , E 12 -E 1 n, and E 22 -E 2 n. Since V2 is lower than the light-emitting threshold voltage, current scarcely flows through these light-emitting elements and hence, practically no light emission is provided. Moreover, −(V1−2V2) of reverse-directional voltage is applied to the light-emitting elements E 32 -E 3 n and E 42 -E 4 n, and these light-emitting elements are not allowed to emit light.  
         [0091]    When scanning is shifted from the light-emitting state shown in FIG. 8 to the state, shown in FIG. 11, in which the light-emitting elements E 22  and E 32  emit light, the reset control is performed as shown in FIG. 9.  
         [0092]    That is, before scanning is shifted from the negative electrode line B 1  of FIG. 8 to the negative electrode line B 2  of FIG. 11, all drive switches  31  through  34  are switched over to the reset voltage sources  51  through  54  and as well all scan switches  11  through  1 n are switched over to 0V for reset as shown in FIG. 9. When the reset has been performed, a voltage of V2 is applied to all light-emitting elements E 11  through E 4 n. Therefore, light-emitting elements with a voltage different from V2 applied thereto are charged or discharged as shown with the arrows in FIG. 9. Consequently, parasitic capacitors of all light-emitting elements E 11  through E 4 n are charged so as to make the voltage across both ends V2.  
         [0093]    As mentioned in the foregoing, as shown in FIG. 10 after the reset control has been performed, the scan switch  12  corresponding to the negative electrode line B 2  is not switched over but made 0V, the scan switches  11 , and  13  through In corresponding to other negative electrode lines B 1 , and B 3  through Bn are switched over to the reverse bias voltage sources  41 , and  43  through  4 n to scan the negative electrode line B 2 . Simultaneously, the drive switches  32  and  33  are switched over to the constant-current sources  22  and  23 , and the drive switches  31  and  34  are switched over to the reset voltage sources  51  and  54 .  
         [0094]    As mentioned above, at the instant of switching of the scan switches  11  through In and the drive switches  31  through  34 , the potential of the positive electrode lines A 2  and A 3  becomes approximately V1 (precisely speaking, (n−1/n)_EV1) due to the applied voltage V1−V2 by means of the reverse bias voltage sources  41 , and  43  through  4 n and the voltage across both ends V2 due to a charged charge of the light-emitting elements E 21 , E 23  through E 2 n, E 31 , and E 33  through E 3 n, the voltage across both ends of the light-emitting elements E 22  and E 32  is a forward-biased voltage approximately equal to the light emission specifying voltage V x . That is, the voltage of the reverse bias voltage sources  41  through  4 n is set to V1−V2 in response to the reset voltage V2 to be applied to the reset voltage sources  51  through  54 , thereby allowing both ends of light-emitting elements E 22  and E 32  to be roughly equal to the light emission specifying voltage V x . This allows the light-emitting elements E 22  and E 32  to quickly be charged by current flowing from a plurality of routes shown with arrows in FIG. 10, and thus allowing for shifting instantaneously to a steady state of light emission shown in FIG. 11.  
         [0095]    Furthermore, a reverse-directional voltage of −(V1−2V2) is applied to light-emitting elements E 11 , and E 13  through E 1 n, E 41 , and E 43  through E 4 n which are charged as shown with arrows in FIG. 10 in response to the difference between the voltage and voltage V2 at the time of reset, which has been explained referring to FIG. 9.  
         [0096]    Furthermore, since the voltage applied to the light-emitting elements E 12  and E 42  is V2, no current flows therethrough. In addition, even when the light-emitting elements E 21 , and E 23  through E 2 n, E 31 , and E 33  through E 3 n are brought into a steady state of light emission as shown in FIG. 11, the voltage across both ends still remains V2, and hence, no current flows in from the constant-current sources  32  and  33 . As mentioned in the foregoing, at a steady state of light emission shown in FIG. 11, the drive current supplied by the constant-current sources  32  and  33  flows into the light-emitting elements E 22  and E 32 , and hence the light-emitting elements E 21  and E 32  emit light at the desired instantaneous luminance Lx.  
         [0097]    Power consumption of the present embodiment will be explained referring to Tables 1 and 2.  
         [0098]    Table 1 shows, in comparison to an example of the prior art, the voltages applied to each light-emitting element at steady states of light emission of the light-emitting elements E 11  and E 21  (FIG. 8 and FIG. 3), and at the reset state (FIG. 9 and FIG. 4). On the other hand, Table 2 shows, in comparison to an example of the prior art, the voltages applied to each light-emitting element at steady states of light emission of the light-emitting elements E 22  and E 32  (FIG. 10 and FIG. 5), and at the reset state (FIG. 9 and FIG. 4).  
                                                                           TABLE 1                           Light-   Prior art   First embodiment            emitting   Voltage   Difference   Voltage   Difference            element   Drive   Reset   in voltage   Drive   Reset   in voltage               E11, E21    V1   0   −V1   V1   V2   −(V1 − V2)       E31, E41   0   0   0   V2   V2   0       E12, E13,   0   0   0   V2   V2   0       E1n,       E22, E23,       E2n       E32, E33,   −V1   0    V1   −(V1 − 2V2)   V2   V1 − V2       E3n                  
 
         [0099]    [0099]                                                                           TABLE 2                           Light-   Prior art   First embodiment            emitting   Voltage   Difference   Voltage   Difference            element   Reset   Drive   in voltage   Reset   Drive   in voltage               E22, E32   0    V1    V1   V2   V1   V1 − V2       E12, E42   0   0   0   V2   V2   0       E11, E13,   0   −V1   −V1   V2   −(V1 − 2V2)   −(V1 − V2)       E1n,       E41, E43,       E2n       E21, E23,   0   0   0    V2   V2   0       E2n,       E31, E33,       E3n                    
         [0100]    At the time of switching, a potential corresponding to the difference in voltage of Tables 1 and 2 is produced across both ends of light-emitting elements to charge and discharge the parasitic capacitors.  
         [0101]    As shown in Tables 1 and 2, the difference in voltage was V1 in the example of the prior art, whereas the difference in voltage is V1−V2 according to the first embodiment, and thus the difference in voltage is made lower. Moreover, a voltage of −V1 according to the example of the prior art has been also reduced to a lower difference in voltage of −(V1−V2 ) according to the first embodiment.  
         [0102]    Since the charge to be charged or discharged to and from the parasitic capacitance of light-emitting elements is proportional to the difference in voltage, the drive power for the first embodiment can be considerably reduced compared with the example of the prior art.  
         [0103]    Referring to FIG. 12 through FIG. 15, a second embodiment of the present invention will be explained. FIG. 12 through FIG. 15 are views showing the configuration of the second embodiment of the present invention. FIG. 12 shows the light emission status A, FIG. 13 shows the reset status, FIG. 14 shows the time of switchover to the light emission status B, and FIG. 15 shows the light emission status B.  
         [0104]    What is different between the second and the first embodiments is as follows. In the first embodiment, the scan switches  11  through in are constructed so as to perform switching between the ground voltage and the reverse bias voltage sources  41  through  4 n having a voltage of V1−V2 . On the other hand, in the second embodiment, switching is performed between the ground voltage and the reverse bias voltage sources  41  through  4 n having a voltage of V1.  
         [0105]    Furthermore, in the first embodiment the drive switches  31  through  34  are intended so as to perform switching between the constant-current sources  21  through  24  and the reset voltage source V2, whereas in the second embodiment the drive switches  31  through  34  are intended to perform switching between any of the constant-current sources  21  through  24 , reset voltage sources  51  through  54  having a voltage of V2, and the ground voltage.  
         [0106]    Referring to FIG. 12 through FIG. 15, the operation of light emission of the second embodiment will be explained below.  
         [0107]    Like the first embodiment, an example will be explained in which, after the negative electrode line B 1  is scanned to cause the light-emitting elements E 11  and E 21  to emit light, the scan is shifted to the negative electrode line B 2  to cause the light-emitting elements E 22  and E 32  to emit light.  
         [0108]    First in FIG. 12, the scan switch  11  is switched over to the 0V side and then the negative electrode line B 1  is scanned. To other negative electrode lines B 2  through Bn, the reverse bias voltage source V1 is applied by the reverse bias voltage sources  42  through  4 n. Furthermore, to the positive electrode lines A 1  and A 2 , the drive switches  31  and  32  connect the constant-current sources  21  and  22 . To other positive electrode lines A 3  through A 4  are supplied with a voltage of 0V.  
         [0109]    Therefore, in the case of FIG. 12, only the light-emitting elements E 11  and E 21  allow drive current to flow therein as shown with the arrows from the constant-current sources  21  and  22 , and thus only the light-emitting elements E 11  and E 21  are emitting light at a steady state of light emission. On the other hand, other light-emitting elements are at the same charged status as the prior art.  
         [0110]    At the time scan is shifted from the light-emitting state shown in FIG. 12 to the light-emitting state of the light-emitting elements E 22  and E 32  shown in FIG. 15, the reset control shown in FIG. 13 is performed.  
         [0111]    That is, before scan is shifted from the negative electrode line B 1  shown in FIG. 12 to the negative electrode line B 2  shown in FIG. 15, first as shown in FIG. 13, all drive switches  31  through  34  are switched over to the side of reset voltage sources  51  through  54 , and, as well, all scan switches  11  through  14  are switched over to the side of 0V to perform reset. Consequently, electric charge is Charged into the parasitic capacitors of all light-emitting elements E 11  through E 4 n to raise the voltages across both ends thereof to V2.  
         [0112]    As mentioned above, after the reset control has been performed, as shown in FIG. 14, the scan switches  12  corresponding to the negative electrode line B 2  are not switched over but remain at the side of 0V. The scan switches  11  and  13  through in corresponding to other negative electrode lines B 1  and B 3  through Bn are switched over to the side of the reverse bias voltage sources  41  and  43  through  4 n to scan the negative electrode line B 2 . Simultaneously, the drive switches  32  and  33  are switched over to the constant-current sources  22  and  23  and, as well, the drive switches  31  through  34  are switched over to the ground side.  
         [0113]    At the instant the switches  11  through in and  31  through  34  have been switched over as mentioned above, the potentials of the positive electrode lines A 2  and A 3  become approximately V1+V2 due to a voltage V1 of the reverse bias voltage sources  41  and  43  through  4 n, and a voltage of V2 caused by the charged charge of the light-emitting elements E 21 , E 23  through E 2 n, E 31 , and E 33  through E 3 n across both ends thereof. The voltage across both ends of the light-emitting elements E 22  and E 32  is a forward bias voltage of approximately V1+V2, which is greater than the light emission specifying voltage V x  .  
         [0114]    This allows the light-emitting elements E 22  and E 32  to be quickly charged by the currents from a plurality of routes shown with arrows in FIG. 14 to emit light with instantaneous luminance greater than the instantaneous luminance L x  under a steady state of light emission and then to be shifted to a steady state of light emission shown in FIG. 15.  
         [0115]    [0115]FIG. 16 shows the transition state of the voltage across both ends of the light-emitting elements E 22  and E 32  until the light-emitting elements E 22  and E 32  shown in FIG. 14 are shifted to a steady state of light emission. As shown in the figure, the voltage across both ends of the light-emitting elements E 22  and E 32  becomes approximately V1+V2 immediately after the scanning of negative electrode line B 2  has been initiated and soon converges to the light emission specifying voltage V1 (=V x ) to fall in a steady state of light emission.  
         [0116]    As mentioned above, the light-emitting elements E 22  and E 32  emit light with instantaneous luminance greater than the instantaneous luminance L x  under a steady state of light emission only immediately after the scanning of negative electrode line B 2  has been initiated. The excessive luminance supplements the non-light-emission period resulting from the reset immediately before, thus allowing for displaying images without reducing the luminance.  
         [0117]    Explanation has been made for the embodiments of the present invention in the foregoing, however, the present invention is not limited to a light-emitting display device that employs organic EL elements, but is also applicable to elements if the element has the properties of capacitance and the diode like organic EL elements.  
         [0118]    As explained above, during the period of reset, the present invention allows all scan lines to be given a first reset voltage and, as well, all drive lines to be given a second reset voltage that is greater than the first reset voltage. For this reason, a light-emitting display device can be provided which allows for realizing high performance such as a reduction in power consumption while a rise in light emission made quick at the time of switching of the scanning like in the prior art reset drive method.