JP4388056B2 - AC type plasma display panel - Google Patents

Description

  The present invention relates to an AC type plasma display panel used for image display such as a television receiver and an advertisement display panel.

  FIG. 11 is a partially cutaway perspective view showing a schematic configuration of a conventional AC type plasma display panel (hereinafter simply referred to as “panel”). FIG. 12 is a cross-sectional view seen from the direction of the arrow in the BB line of FIG.

  As shown in FIG. 11, in a conventional AC type plasma display panel 80, a front substrate 82 and a rear substrate 83 are arranged to face each other across a discharge space. On the surface substrate 82, a plurality of stripe-shaped scanning electrodes 86 and sustaining electrodes 87 are arranged in parallel with each other, and these are covered with a dielectric layer 84 and a protective film 85. On the back substrate 83, a plurality of stripe-shaped address electrodes 88 are formed substantially in parallel in a direction orthogonal to the scan electrodes 86 and the sustain electrodes 87. A stripe-shaped partition wall 89 is arranged between the address electrodes 88. A phosphor 90 is formed between the partition walls 89 so as to cover the address electrodes 88. Each space surrounded by the front substrate 82, the rear substrate 83, and the barrier ribs 89 forms a discharge cell 91. The space in the discharge cell 91 is filled with a gas that emits ultraviolet rays by discharge.

  As shown in FIG. 12, the phosphor 90 is composed of three colors, a blue phosphor 90b, a green phosphor 90g, and a red phosphor 90r, and these three color phosphors are sequentially formed in each discharge cell one color at a time. ing. As a result, the discharge cell with the blue phosphor 90b is replaced with the blue discharge cell 91b, the discharge cell with the green phosphor 90g is replaced with the green discharge cell 91g, and the discharge cell with the red phosphor 90r is attached. Each of the red discharge cells 91r is configured.

  Next, a method for displaying image data on the conventional panel 80 will be described.

  In driving the panel 80, one field period is divided into subfields having a light emission period weight based on the binary system, and gradation display is performed by a combination of subfields to emit light. For example, when one field is divided into eight subfields, 256 gradation display can be performed. The subfield includes an initialization period, an address period, and a sustain period.

  In order to display image data, different signal waveforms are applied to the electrodes in the initialization period, the address period, and the sustain period.

  In the initialization period, for example, a positive pulse voltage with respect to the address electrode 88 is applied to all the scan electrodes 86, and wall charges are accumulated on the protective film 85 and the phosphor 90.

  In the address period, a positive pulse (write voltage) is applied to the address electrode 88 while the scan electrode 86 is sequentially scanned by applying a negative pulse to the scan electrode 86. At this time, discharge (writing discharge) occurs in the discharge cell 91 at the intersection of the scan electrode 86 and the address electrode 88, and charged particles are generated. Such an operation is called a write operation.

  In the subsequent sustain period, an alternating voltage sufficient to maintain the discharge is applied between the scan electrode 86 and the sustain electrode 87 for a certain period. As a result, the discharge plasma generated at the intersection of the scan electrode 86 and the address electrode 88 excites the phosphor 90 while applying this AC voltage between the scan electrode 86 and the sustain electrode 87. . Where light emission is not desired, a pulse need not be applied to the scan electrode 86 in the address period.

  In such a conventional panel, in order to obtain the same white color as the chromaticity coordinates of the standard white light source, the width of the discharge cells 91 of each of the three colors (that is, the interval between the barrier ribs 89 on both sides constituting the discharge cell 91) is They are different from each other (Japanese Patent Laid-Open No. 9-115466). Specifically, the discharge cell 91b having the blue phosphor 90b has the widest width, and the green discharge cell 91g and the red discharge cell 91r are configured to be narrower than the blue discharge cell 91b. ing. This is due to the following reason. That is, since the luminous efficiency of the blue phosphor 90b is lower than that of the green phosphor 90g and the red phosphor 90r, when all of the blue, green, and red discharge cells have the same width, the discharge cells of the respective colors are the largest. When an input signal is input, desired chromaticity and color temperature cannot be obtained because the chromaticity obtained by combining the three colors deviates from the white region or the color temperature is low. Therefore, by adjusting the widths of the discharge cells 91 for the three colors as described above, adjustment is made so that a desired white color is obtained when the maximum input signal is input to the discharge cells of the respective colors.

  However, the above structure has a problem that the discharge start voltage of the blue discharge cell 91b is different from the discharge start voltages of the other two-color discharge cells 91g and 91r. FIG. 13 shows, for each discharge cell of each color, the write voltage (complete lighting write voltage) necessary for stably performing the write discharge when the voltage applied to the scan electrode 86 is constant in the write operation in the address period. ing. As described above, in the conventional panel, the value of the write voltage required for each color discharge cell is different. Due to this, as is apparent from the figure, the completely lit write voltage varies greatly depending on the discharge cells of the respective colors. Therefore, when the same write voltage is applied to all the discharge cells, the write discharge becomes unstable, or erroneous discharge or discharge flickering occurs, resulting in a problem that correct display cannot be performed.

  In order to perform a stable write operation, it is necessary to change the write voltage applied to the address electrode 88 for each color of the discharge cell in accordance with the full lighting write voltage of the discharge cell of each color. However, this complicates voltage control and makes the device expensive.

  The present invention solves the above-described problems, and even when the discharge cells of blue, green, and red have different widths, the writing discharge is stable, and there is no erroneous discharge or discharge flickering. The purpose is to provide a panel.

  In order to achieve the above object, the present invention has the following configuration.

The AC type plasma display panel of the present invention has a plurality of discharge cells in which two substrates are opposed to each other with a partition wall interposed between the two substrates and the partition wall, and each of the discharge cells has a fluorescent light. The width of the discharge cell in which the phosphor of at least one color among the plurality of colors is formed is different from the width of the discharge cell in which the phosphor of the other color is formed, and initialization prior to the address period A voltage waveform having a voltage change rate of 10 V / μs or less during the period is applied so that the residual voltage in each discharge cell substantially coincides with the discharge start voltage of each discharge cell at the end of the initialization period. It is structured. According to this configuration, it is possible to make the complete lighting write voltage of the discharge cells of each color substantially uniform. In the present invention, the “completely lit write voltage” means a write voltage necessary for causing a write discharge to all desired discharge cells in a write operation in an address period prior to the sustain operation.

  According to the present invention, when the width of the discharge cell is different for each color, an AC type plasma display panel with high display quality is obtained, in which the writing discharge is stable, there is no erroneous discharge or discharge flicker, and the display can be stably performed correctly. It is done. In addition, since the width of the discharge cell can be arbitrarily changed for each color, an AC type plasma display panel having desired chromaticity and color temperature and improved white display quality can be obtained.

(Embodiment 1)
Hereinafter, Embodiment 1 of the present invention will be described with reference to the drawings.

  FIG. 1 is a partially cutaway perspective view of an AC type plasma display panel (hereinafter simply referred to as “panel”) according to Embodiment 1 of the present invention. FIG. 2 is a cross-sectional view as seen from the direction of the arrow in the AA line of FIG.

  As shown in FIG. 1, in the panel 10 of this embodiment, the front substrate 2 and the rear substrate 3 are arranged to face each other with a discharge space interposed therebetween. On the surface substrate 2 made of a transparent material such as glass, a plurality of stripe-shaped scanning electrodes 6 and sustaining electrodes 7 are arranged in parallel with each other, and these are covered with the dielectric layer 4 and the protective film 5. It has been broken. Between the front substrate 2 and the rear substrate 3, stripe-shaped (band-shaped) partition walls 13 are provided in a direction orthogonal to the scan electrodes 6 and the sustain electrodes 7. As shown in FIG. 2, a blue discharge cell 14b, a green discharge cell 14g, and a red discharge cell 14r are sequentially formed in a region surrounded by the front substrate 2, the rear substrate 3, and the partition wall 13.

  Between the adjacent barrier ribs 13, parallel to the barrier ribs 13, striped address electrodes 15b, 15g, 15r are provided corresponding to the discharge cells 14b, 14g, 14r of the respective colors, and these address electrodes 15b, 15g are respectively provided. , 15r, and blue phosphor 16b, green phosphor 16g, and red phosphor 16r are formed from the side of the partition 13 on both sides. The discharge cells 14b, 14g, and 14r are filled with a mixed gas of at least one of helium, neon, and argon and xenon.

  The address electrode 15b formed in the blue discharge cell 14b is the blue address electrode 15b, the address electrode 15g formed in the green discharge cell 14g is the green address electrode 15g, and the address is formed in the red discharge cell 14r. The electrode 15r is called a red address electrode 15r.

  As shown in FIG. 2, the interval between the barrier ribs 13 constituting the blue discharge cell 14b, that is, the blue discharge cell width is Wb, and the interval between the barrier ribs 13 constituting the green discharge cell 14g, ie, the green discharge cell width is set. Wg is set such that Wb> Wg> Wr, where Wr is the interval between the barrier ribs 13 constituting the red discharge cell 14r, that is, the red discharge cell width. Further, when the width of the blue address electrode 15b is Db, the width of the green address electrode 15g is Dg, and the width of the red address electrode 15r is Dr, Db> Dg> Dr is set. The address electrodes 15b, 15g, and 15r for each color are arranged so as to be positioned approximately at the center of the discharge cells 14b, 14g, and 14r for each color.

  Next, the operation of the discharge light emission display of the panel according to the present embodiment will be described with reference to FIGS.

  First, in the write operation, when a positive write pulse voltage (write voltage) is applied to the address electrodes 15b, 15g, and 15r and a negative scan pulse voltage is applied to the scan electrode 6, write discharge occurs in the discharge cells 14b, 14g, and 14r. And positive charges are accumulated on the surface of the protective film 5 on the scan electrodes 6.

  Thereafter, in the sustain operation, first, a negative sustain pulse voltage is applied to sustain electrode 7, and then a negative sustain pulse voltage is alternately applied to scan electrode 6 and sustain electrode 7, whereby sustain discharge is sustained. Is done. Finally, the sustain discharge is stopped by applying a negative erase pulse voltage to the sustain electrode 7.

  As a specific example of the panel 10 of the present embodiment, the discharge cell widths of blue, green and red are Wb1 = 0.37 mm, Wg1 = 0.28 mm, Wr1 = 0.19 mm, and the width of the partition wall 13 is 0.08 mm. Db1 = 0.222 mm, Dg1 = 0.168 mm, and Dr1 = 0.114 mm so that the blue, green, and red address electrode widths are proportional to the discharge cell widths of the respective colors. During the display operation, the charge amounts formed on the surface of the protective film 5 in the blue, green and red discharge cells are Qb1, Qg1 and Qr1, respectively.

  As can be seen from FIG. 1, the volume ratio of the discharge space of each of the blue, green, and red discharge cells can be approximately the ratio of the discharge cell width of each color, so that the volume ratio is Wb1: Wg1: Wr1. = 5: 4: 3. Further, during the display operation, the ratio Qb1: Qg1: Qr1 of the amount of charge formed on the surface of the protective film 5 in the blue, green and red discharge cells substantially coincides with the ratio Db1: Dg1: Dr1 of the address electrode width. Qb1: Qg1: Qr1 = 5: 4: 3. Therefore, charge amounts Qb1, Qg1, and Qr1 substantially equal to the volume ratio of the discharge space of each color discharge cell are obtained on the surface of the protective film 5 in the blue, green, and red discharge cells 14b, 14g, and 14r, respectively. As a result, it is possible to obtain a panel with less display errors and good display characteristics.

  For example, as a comparative example, the discharge cell widths of blue, green, and red are set to Wb2 = 0.37 mm, Wg2 = 0.28 mm, and Wr2 = 0.19 mm, respectively, as in the specific example panel of this embodiment. The discharge electrode address electrode widths are all made the same so that Db2 = Dg2 = Dr2 = 0.18 mm. In this panel, the ratio Qb2: Qg2: Qr2 of the amount of charge formed on the surface of the protective film 5 in the blue, green and red discharge cells during the display operation is the ratio Db2: Dg2: Dr2 of the address electrode width. . That is, since Qb2: Qg2: Qr2 = 1: 1: 1, the charge accumulated on the surface of the protective film 5 in each color discharge cell is not proportional to the ratio of the volume of the discharge space of the corresponding discharge cell. . In this case, the discharge becomes unstable in the blue discharge cell 14b which is the widest discharge cell, causing erroneous discharge and discharge flicker.

  Next, FIG. 3 shows the measurement results of the write voltage (complete lighting write voltage) that can stably perform the write discharge in the write operation for the panel of the specific example and the comparative example of the embodiment described above. In FIG. 3, the results measured with the panels of the specific example and comparative example of the present embodiment are represented by solid lines and broken lines, respectively. In the following description, the full lighting write voltages of the blue, green, and red discharge cells are Vbd, Vgd, and Vrd, respectively.

  As shown in FIG. 3, in the panel of the comparative example, the full lighting write voltages of the blue, green and red discharge cells are Vbd> Vgd> Vrd, and it can be seen that the difference between the respective voltage values is large. In order to stably perform the discharge display operation of such a panel, the write voltage is set to be equal to or higher than the full lighting write voltage Vbd of the highest blue discharge cell among the full lighting write voltages of the discharge cells of each color. There is a need. In this case, since a voltage higher than Vrd by 10 V or more is applied to the red discharge cell having the lowest fully lit write voltage, the discharge becomes unstable, causing flickering or erroneous write operation. .

  On the other hand, in the panel of the specific example of the present embodiment, as shown in FIG. 3, the full lighting write voltages Vbd, Vgd, and Vrd of the discharge cells of the respective colors have almost the same value. It is possible to eliminate the occurrence of flickering of display light emission and erroneous writing operation.

  Therefore, during the display operation, the address electrodes 15b, 15g, and 15r for the respective colors are accumulated so that the amount of charge corresponding to the volume of the discharge space of the blue, green, and red discharge cells is accumulated on the surface of the protective film 5 in the discharge cells of the respective colors. By appropriately setting the width, a panel capable of performing stable display discharge without erroneous discharge or discharge flickering can be obtained.

  In the present embodiment, the case where the discharge cell width of each color is Wb> Wg> Wr has been described. However, even if the relationship between the discharge cell widths of each color is other than this, the address electrode By setting the width in proportion to the width of the discharge cell in which the address electrode is formed, a panel capable of performing stable display discharge without erroneous discharge or discharge flicker can be obtained. In the present embodiment, the discharge electrode of each color is described in which the address electrode width is set to be proportional to the discharge cell width. However, the address electrode width is simply set in the order of the discharge cell width. Even in such a panel, a panel capable of performing stable display discharge without erroneous discharge or discharge flicker can be obtained.

(Embodiment 2)
The second embodiment of the present invention will be described below with reference to the drawings.

  FIG. 4 is a cross-sectional view in the thickness direction of an AC type plasma display panel (hereinafter simply referred to as “panel”) according to Embodiment 2 of the present invention.

  As shown in FIG. 4, in the panel 20 of this embodiment, the front substrate 2 and the rear substrate 3 are provided to face each other with a predetermined gap, and a gas that emits ultraviolet rays by discharge in the gap. For example, neon and xenon are encapsulated. On the surface substrate 2, a display electrode group composed of a strip-shaped scan electrode 6 and a sustain electrode 7 is formed substantially in parallel, and a dielectric layer 4 is formed so as to cover them. Although not shown, a protective layer may be provided on the dielectric layer 4 as in the first embodiment. Address electrodes 15 are formed on the back substrate 3 in a direction orthogonal to the scan electrodes 6 and the sustain electrodes 7. A plurality of strip-shaped partition walls 13 are provided in parallel with the address electrodes 15 between the front substrate 2 and the rear substrate 3.

  Between the adjacent barrier ribs 13, the phosphors 16 of the blue phosphor 16b, the green phosphor 16g, and the red phosphor 16r are sequentially attached to the back substrate 3 so as to cover the address electrodes 15 one by one. A discharge cell 14 is formed in a region surrounded by the front substrate 2, the rear substrate 3, and the barrier rib 13, and the discharge cell provided with the blue phosphor 16b is replaced with the blue discharge cell 14b and the green phosphor 16g. The discharge cell provided with is the green discharge cell 14g, and the discharge cell provided with the red phosphor 16r is the red discharge cell 14r.

  Next, a driving method of the panel 20 for displaying image data on the panel 20 of the present embodiment will be described with reference to FIG.

  As a method of driving the panel 20, one field period is divided into subfields having a light emission period weight based on the binary system, and gradation display is performed by a combination of subfields to emit light, as in the conventional case. The subfield includes an initialization period, an address period, and a sustain period.

  FIG. 5 shows voltage waveforms applied to the electrodes. As shown in FIG. 5, during the initialization period, a voltage (gradient voltage) having a waveform that gradually rises with respect to the sustain electrode 7 and the address electrode 15 and then gradually falls is applied to all the scan electrodes 6. As a result, wall charges are accumulated on the dielectric layer 6 and the phosphor 16.

  In the address period, a positive pulse corresponding to display data is applied to the address electrode 15, and a negative pulse is sequentially applied to the scan electrode 6. At this time, an address discharge (address discharge) occurs in the discharge cell 14 at the intersection of the address electrode 15 and the scan electrode 6 to generate charged particles. A positive pulse is not applied to the address electrode 15 corresponding to the discharge cell 14 that does not perform display.

  In the subsequent sustain period, a discharge in which a write discharge (address discharge) is generated by applying an alternating voltage large enough to maintain the discharge for a certain period between the scan electrode 6 and the sustain electrode 7. A discharge plasma is generated in the cell 14. The discharge plasma generated in this way causes the phosphor 16 to excite and emit light, thereby displaying the panel.

In the present embodiment, BaMgAl ₁₀ O ₁₇ ; Eu is used as the blue phosphor 16b, Zn ₂ SiO ₄ ; Mn is used as the green phosphor 16g, and (Y ₂ Gd) BO ₃ ; Eu is used as the red phosphor 16r. Yes. In addition, the width Wb of the blue discharge cell 14b is 0.37 mm, the width Wg of the green discharge cell 14g is 0.28 mm, the width Wr of the red discharge cell 14r is 0.19 mm, and the width of the partition wall 13 is 0.08 mm. The total width of these three-color discharge cells is 1.08 mm. In this case, the chromaticity of white light emission, which combines the light emission of the three-color phosphors, is located on a black body radiation locus of approximately 10,000K. High-quality white display was achieved.

  Next, a change in wall voltage of a certain discharge cell from the initialization period to the address period will be described with reference to FIGS. In FIG. 6A, the solid line indicates the relative potential Ve (V) of the scan electrode 6 with respect to the sustain electrode 7, and the broken line indicates the wall voltage Vw (V) accumulated on the dielectric layer 4. The voltage applied to the discharge space is the difference Ve−Vw between Ve and Vw. FIG. 6B shows the current Is flowing in the discharge space.

  During time t1 to t3, which is the first half of the initialization period, a ramp voltage that gently rises from 0 to Vc (V) is applied to the scan electrode 6 as shown in FIG. 5, and the discharge space as shown in FIG. Discharge occurs at a time t2 when the voltage Ve-Vw applied to is equal to or higher than the discharge start voltage Vf (V), and the wall voltage Vw increases as the relative potential Ve increases. Next, at time t3, the potential of the sustain electrode 7 is raised to Vs (V). As a result, the relative potential Ve decreases, and the voltage Ve−Vw applied to the discharge space becomes less than the discharge start voltage Vf, so that the discharge is stopped. Thereafter, a ramp voltage is applied to the scan electrode 6 so that the potential of the scan electrode 6 gradually falls from Vc to zero. With the application of such a ramp voltage, the relative potential Ve decreases, and the discharge starts again at time t4 when the absolute value of the voltage Ve−Vw applied to the discharge space becomes equal to or higher than the discharge start voltage Vf. The wall voltage Vw gradually decreases due to the discharge starting from time t4, and the discharge stops at time t5 when the voltage applied to the scan electrode 6 becomes zero. At this time, the discharge space is stabilized in a state where the residual voltage Vg = Vw−Ve is applied.

  Since the current Is (A) that flows when discharge occurs in the initialization period is proportional to dVe / dt, the current Is can be reduced by sufficiently reducing the rate of change of the voltage applied to the scan electrode 6, that is, dVe / dt. It can be suppressed to a very low value. The wall voltage Vw is generated by the formation of wall charges on the dielectric layer 4 by discharge. Therefore, when a gentle gradient voltage is applied, the wall charges start to be formed when the voltage Ve−Vw applied to the discharge space exceeds the discharge start voltage Vf, while being substantially proportional to the increase in the voltage applied to the scan electrode 6. It will increase. Thereafter, when the voltage applied to the scan electrode 6 is gradually lowered, the wall charge starts to decrease from the time when the absolute value of the voltage Ve−Vw applied to the discharge space exceeds the discharge start voltage Vf, and is applied to the scan electrode 6. The voltage decreases almost in proportion to the voltage drop. As a result, at time t5, the residual voltage Vg and the discharge start voltage Vf are equal. After time t5, charged particles remaining in the discharge space are accumulated as wall charges, so the residual voltage Vg may change slightly. However, since the current Is is a very low value, the change is slight. The relationship of Vg≈Vf is maintained after time t5.

  FIG. 7 shows in detail the relationship between the relative potential Ve and the residual voltage Vg when a ramp voltage is applied to the scan electrodes. FIG. 7 shows the walls of the blue, red and green discharge cells when the discharge start voltage Vfb of the blue discharge cells is different from the discharge start voltages Vfr and Vfg of the red and green discharge cells as in the present embodiment. Changes in the voltages Vwb, Vwr and Vwg are indicated by dotted lines. The solid line indicates the relative potential Ve of the scan electrode 6 with respect to the sustain electrode 7 when a ramp voltage is applied to the scan electrode 6. Since the blue discharge cell has a high discharge start voltage Vfb, the discharge starts after the red and green discharge cells as shown in FIG. 7, but the timing at which the discharge stops is the same in the three-color discharge cells (FIG. 6). Therefore, the residual voltage Vgb of the blue discharge cell is the highest, and Vgb≈Vfb. Similarly, the residual voltages Vgr and Vgg of the red and green discharge cells are Vgr≈Vfr and Vgg≈Vfg. The same applies when the voltage applied to the scan electrode 6 is gradually lowered. After the discharge of the red and green discharge cells starts, the discharge of the blue discharge cells starts. Since the same applies to the discharge cells of three colors (time t5 in FIG. 6), the residual voltage Vgb of the blue discharge cell is the highest, and Vgb≈Vfb. Similarly, the residual voltages Vgr and Vgg of the red and green discharge cells are Vgr≈Vfr and Vgg≈Vfg.

  From the above, the voltage applied to the discharge space of each color discharge cell at the end of the initialization period (which corresponds to the residual voltage) is substantially equal to the discharge start voltage of the discharge cell. I understand. Therefore, when the address period starts, the potential of the scan electrode 6 is once raised to the bias potential VB (V) at time t6 as shown in FIG. 5 to prevent the occurrence of erroneous discharge. Thereafter, the scan pulse is applied to the scan electrode 6 by sequentially returning the potential of the scan electrode 6 to 0 (V) in accordance with the timing at which a positive pulse (write voltage) is applied to the address electrode 15. (Write operation). At this time, since the wall voltage accumulated in the dielectric layer 4 is maintained as it is, by returning the potential of the scan electrode 6 to 0 (V), each discharge cell is substantially equal to the discharge start voltage of the discharge cell. Voltage will be applied. Therefore, by applying a pulse having a constant value to the address electrode 15 in accordance with this, the write discharge can be similarly started in the discharge cells of the respective colors.

  FIG. 8 shows a result of measuring a writing voltage (complete lighting writing voltage) that can stably perform writing discharge during the writing operation using the panel of the present embodiment. Here, Vs = 190 (V), Vc = 450 (V), VB = 100 (V), t5−t1 = 1 (ms), Vc / (t5−t3) = 0.7 (V / μs) did. According to the present embodiment, since the full lighting write voltage of the discharge cells of each color is almost the same value, the write operation is uniform among the discharge cells of each color, and the flickering of display light emission or the erroneous write operation is performed. Occurrence can be eliminated. As a result, it can be seen that a stable write operation (address operation) can be performed.

  Further, as can be seen from FIG. 8, in the panel of the present embodiment, the minimum voltage required for writing in the discharge cells of each color is less than 40V, and in contrast to the conventional panel requiring nearly 100V. Therefore, a low-cost IC can be used for the write pulse generation circuit.

  For comparison, the relationship between the relative potential Ve of the scan electrode 6 to the sustain electrode 7 and the wall voltage Vw when a wall charge is formed by applying a pulse voltage to the scan electrode 6 in the initialization period as in the conventional panel. Is shown in FIG. Moreover, the electric current which flows into the discharge space at that time is shown in FIG.9 (b). When a pulse voltage that rises sharply is applied to the scan electrode 6, the discharge starts instantaneously and a large current flows. Therefore, the wall voltage Vw accumulated in the dielectric layer 4 also rises rapidly, attenuates the voltage applied to the discharge space, and the discharge current flows in a pulse manner and stops. Since many charged particles remain in the space even after the discharge current is stopped, wall charges are finally formed until the voltage Ve−Vw applied to the discharge space becomes zero.

  Therefore, the wall voltage formed in the initialization period in the conventional panel is a value determined by the magnitude of the initialization pulse and is independent of the discharge start voltage of the discharge cell. For this reason, as shown in FIG. 13, the completely lit write voltage varies greatly depending on the discharge cells of each color, and in order to perform a stable write operation, a write voltage (address voltage) Va required in the address period. Must be changed in accordance with the discharge start voltage of each color discharge cell.

  According to the results of experiments conducted on various panel design values by the present inventors, the effect as shown in the present embodiment was confirmed if the gradient of the ramp voltage during the initialization period was 10 V / μs or less. Thus, by applying a voltage waveform that gradually rises or falls during the initialization period, the panel having the configuration of this embodiment can be driven stably.

  As for the lower limit of the gradient of the ramp voltage in the initialization period, a stable address operation can be obtained as long as it does not become 0. However, when displaying 256 gradations, the time for one field is about 16 ms. The practical range of the gradient is limited to 0.5 V / μs or more.

  As described above, in the present embodiment, the quality of white display is improved, and a stable writing operation can be performed even if the writing voltage (address voltage) in the address period is constant for the discharge cells of all colors. As a result, an AC type plasma display panel that realizes stable display can be obtained.

  Next, another embodiment different from the above will be described with reference to FIG.

  An AC plasma display panel according to the present embodiment (hereinafter simply referred to as “panel”) has the same configuration as the panel of the above-described embodiment shown in FIG. The present embodiment is different from the above-described embodiment in that the ramp voltage is applied after the potential of the scan electrode 6 is sharply raised to a certain value in the initialization period.

  As can be seen from FIG. 6, the voltage Ve-Vw applied to the discharge space at time t2 reaches the discharge start voltage Vf, the discharge starts, and the wall voltage starts to be formed. In other words, the period until discharge starts (time until time t2) is redundant. Therefore, in the present embodiment, as shown in FIG. 10, the scan electrode 6 has a steep waveform so that the relative potential Ve of the scan electrode 6 with respect to the sustain electrode 7 rises steeply to a value slightly lower than the discharge start voltage. Then, a ramp voltage having a gentle gradient is applied.

  As a result, the time of the initialization period is shortened, and it is possible to increase the luminance of light emission by increasing the time allocated to the sustain period.

  As described above, in the present embodiment, the quality of white display is improved, and a stable writing operation can be performed even if the writing voltage (address voltage) in the address period is constant for the discharge cells of all colors. As a result, it is possible to obtain an AC plasma display panel that can realize stable display and further increase the luminance of light emission.

  In the above embodiment, the case where the width of the blue discharge cell is wider than the width of the discharge cells of other colors has been described. However, depending on the chromaticity of the white display to be obtained, the above embodiment is different from the above embodiment. The widths of the discharge cells may be changed at different ratios. In some cases, the width of the discharge cell may be different from that of the above embodiment depending on the characteristics of the phosphor used.

  Further, in the above embodiment, in the initialization period, a voltage waveform having a slope that gently rises with respect to the sustain electrodes and the address electrodes and then gently declines is applied to all the scan electrodes. As described above, when a voltage waveform having a slope that gently rises with respect to the scan electrode and the address electrode and then gently falls is applied to all the sustain electrodes, or after that, the scan electrode is applied to all the address electrodes. The same effect can be obtained even when a voltage waveform having an inclined portion that rises gently with respect to the sustain electrode and then gradually falls is applied.

  Furthermore, the voltage waveform during the initialization period has been described as a waveform that rises slowly and then falls. However, the residual voltage Vg of each discharge cell at the end of the initialization period is also different from the waveform in the above embodiment. A similar effect can be obtained by setting the ramp voltage waveform so as to substantially match the discharge start voltage Vf of the discharge cell.

  In the above embodiment, a panel in which a plurality of strip-shaped partition walls are arranged substantially in parallel between the front substrate and the rear substrate is illustrated, but the panel of the present invention is not limited to such a configuration. For example, it may be a panel in which a plurality of substantially parallel strip-shaped partition walls are arranged so as to intersect in the vertical direction and the horizontal direction (that is, in a substantially lattice shape). In this case, the address electrodes are formed substantially parallel to either the vertical or horizontal partition walls, and the sustain electrodes and the scan electrodes are formed in a direction orthogonal to the address electrodes. In this case, the width of the discharge cell is the same width as the address electrode.

  The embodiments described above are intended to clarify the technical contents of the present invention, and the present invention is not construed as being limited to such specific examples. Various changes can be made within the spirit and scope of the present invention, and the present invention should be interpreted broadly.

  According to the present invention, when the width of the discharge cell is different for each color, an AC type plasma display panel with high display quality is obtained, in which the writing discharge is stable, there is no erroneous discharge or discharge flicker, and the display can be stably performed correctly. It is done.

It is a partial notch perspective view of the AC type plasma display panel of Embodiment 1 of this invention. It is sectional drawing seen from the arrow direction in the AA of FIG. It is the figure which showed the full lighting write voltage of the plasma display panel of Embodiment 1, and the plasma display panel of a comparative example according to the discharge cell of each color. It is sectional drawing of the AC type plasma display panel of Embodiment 2 of this invention. It is a figure which shows the drive voltage waveform of the AC type plasma display panel of Embodiment 2. FIG. It is a figure for demonstrating the change of the wall voltage of a certain discharge cell in Embodiment 2. FIG. FIG. 11 is a diagram for explaining a change in wall voltage of each color discharge cell in the initialization period of the second embodiment. It is the figure which showed the complete lighting write voltage of the plasma display panel of Embodiment 2 according to the discharge cell of each color. It is a figure which shows the change of the wall voltage in the initialization period of the conventional AC type plasma display panel. It is a figure which shows the drive voltage waveform of the AC type plasma display panel which concerns on another example of Embodiment 2 of this invention. It is a partial notch perspective view of the conventional AC type plasma display panel. It is sectional drawing seen from the arrow direction in the BB line of FIG. It is the figure which showed the full lighting write voltage of the conventional plasma display panel according to the discharge cell of each color.

Explanation of symbols

2 Surface substrate 3 Back substrate 6 Scan electrode 7 Sustain electrode 13 Partition wall 14, 14b, 14g, 14r Discharge cell 15, 15b, 15g, 15r Address electrode 16 Phosphor 16r Red phosphor 16g Green phosphor 16b Blue phosphor

Claims (4)

Two substrates are arranged opposite to each other with a partition wall interposed therebetween, and there are a plurality of discharge cells surrounded by the two substrates and the partition wall, and a phosphor is formed in each of the discharge cells. Among them, the width of the discharge cell in which the phosphor of at least one color is formed is different from the width of the discharge cell in which the phosphor of the other color is formed , and the voltage change rate is 10 V / μs or less in the initialization period preceding the address period. The AC waveform is configured such that a residual voltage in each discharge cell substantially coincides with a discharge start voltage of each discharge cell at the end of the initialization period. Plasma display panel. 2. The AC plasma display panel according to claim 1, wherein in the initialization period, a discharge is generated while the voltage waveform is applied, and a current having a substantially constant magnitude flows . An address electrode is formed on one of the two substrates, a sustain electrode and a scan electrode are formed on the other substrate in a direction perpendicular to the address electrode, and the voltage waveform is 3. The AC plasma display panel according to claim 1, wherein the plasma display panel is applied to the scan electrodes. 3. The AC type plasma display panel according to claim 1, wherein the portion where the voltage change rate of the voltage waveform is 10 V / μs or less has a portion where the voltage rises and a portion where the voltage falls.

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