KR100615258B1 - Plasma display panel - Google Patents

Abstract

SUMMARY OF THE INVENTION An object of the present invention is to improve the discharge efficiency, brightness, and lifetime of a panel in a plasma display panel having a three-electrode surface discharge structure, wherein the distance between the scan electrode and the sustain electrode is longer than the distance between the scan electrode and the address electrode. It is done.

In order to achieve the above object, the present invention, the front substrate and the rear substrate disposed in parallel to the front substrate; Barrier ribs disposed between the front substrate and the rear substrate and defining discharge cells generating discharge; Scan electrode lines and sustain electrode lines disposed in a front dielectric layer formed on a front substrate in a rear substrate direction and extending in one direction in which discharge cells extend; Address electrode lines disposed in the rear dielectric layer formed on the rear substrate in the front substrate direction and extending to cross the direction in which the scan electrode lines and the sustain electrode lines extend; A phosphor layer disposed in the discharge cells and positioned above the address electrode lines; And a discharge gas in the discharge cells; wherein the distance between the scan electrode lines and the sustain electrode lines that partition the discharge cells is longer than the distance between the address electrode lines and the scan electrode lines, and is reset. Driven by a drive signal having a section, an address section, and a sustain discharge section,

In the sustain discharge period, the first sustain pulse and the second sustain pulse having the rising slope reaching the first voltage and the falling slope reaching the ground voltage are alternately applied to the scan electrode lines and the sustain electrode lines, respectively. And a section in which the first voltage is applied in the first sustain pulse and the second sustain pulse overlap each other in time, and a short pulse is applied to the address electrode lines.

Description

Plasma display panel {Plasma display panel}

1 is a timing diagram for explaining an example of a conventional driving signal.

FIG. 2 is a timing diagram for describing in detail the driving signal of the sustain discharge period of FIG. 1.

3 is an exploded perspective view showing the plasma display panel of the present invention.

4 is a plan view of the plasma display panel of FIG. 3 taken along line II-II.

5 is a view schematically illustrating an electrode arrangement of the plasma display panel of FIG. 3.

FIG. 6 is a block diagram schematically illustrating an apparatus for driving a plasma display panel for driving the plasma display panel of FIG. 3.

FIG. 7 illustrates an address-display separation driving method for Y electrode lines as an example of a driving method for driving the plasma display panel of FIG. 3.

FIG. 8 is a timing diagram for describing the first embodiment as a drive signal of the plasma display panel of FIG. 3.

FIG. 9 is a timing diagram for describing in detail the driving signal of the sustain discharge period of FIG. 8.

FIG. 10 is a timing diagram for describing a second embodiment as a drive signal of the plasma display panel of FIG. 3.

FIG. 11 is a timing diagram for describing the driving signal of the sustain discharge period of FIG. 10 in detail.

FIG. 12 is a timing diagram for describing a third embodiment as a drive signal of the plasma display panel of FIG. 3.

FIG. 13 is a timing diagram for describing the driving signal of the sustain discharge period of FIG. 12 in detail.

A1 to A6 of FIG. 14 show the drive signal of FIG. 1 and b1 to b6 show the voltage distribution, electron density, and ultraviolet ray of 147 nm in the discharge cell during the sustain discharge when the drive signal of FIG. 8 is applied to the plasma display panel of FIG. Distribution, 173 nm ultraviolet distribution, xenon (Xe) ion distribution, and neon (Ne) ion distribution, respectively.

Explanation of symbols on the main parts of the drawings

1 ... plasma display panel, 110 ... front panel,

111 front panel, 112 scanning electrode,

113 holding electrode, 115 front dielectric layer,

116 front shield, 120 rear panel,

121 back panel, 122 address electrode,

123 rear dielectric layer, 124 bulkhead,

125 phosphor layer, 128 rear shield,

Ce ...

Y1, ..., Yn ... scanning electrode lines,

X1, ..., Xn ... holding electrode lines,

A1, A2, ..., Am ... address electrode lines,

Vs ... first voltage, Vset ... second voltage,

Vset + Vs ... third voltage, Vnf ... fourth voltage,

Vb ... fifth voltage, Vsch ... sixth voltage,

Vscl ... 7th voltage, Va ... 8th voltage,

400 image processing unit, 402 logic control unit,

404 ... Y drive, 406 ... address drive,

408 ... X driver, Vs1 ... short pulse voltage of Fig. 8,

Vs2 ... short pulse voltage of FIG. 10, Vs3 ... short pulse voltage of FIG.

The present invention relates to a plasma display panel, and more particularly, to a plasma display panel having a three-electrode surface discharge structure, wherein a distance between a scan electrode and a sustain electrode is longer than a distance between a scan electrode and an address electrode.

Japanese Laid-Open Patent Publication No. 1999-120924 discloses a structure of a conventional plasma display panel. That is, between the front and rear substrates of a conventional plasma display panel, address electrode lines, dielectric layers, scan electrode lines, sustain electrode lines, phosphor layers, barrier ribs, and magnesium monoxide (MgO) protective layers are provided.

The address electrode lines are formed in a predetermined pattern on the front side of the back substrate. The back dielectric layer is applied to the front of the address electrode lines. In the front of the rear dielectric layer, barrier ribs are formed in a direction parallel to the address electrode lines. These partitions partition the discharge area of each discharge cell and serve to prevent optical interference between the discharge cells. The phosphor layer is applied in front of the rear dielectric layer on the address electrode lines between the partition walls, and a red light emitting phosphor layer, a green light emitting phosphor layer, and a blue light emitting phosphor layer are sequentially disposed.

The sustain electrode lines and the scan electrode lines are formed in a constant pattern on the rear side of the front substrate so as to be orthogonal to the address electrode lines. Each intersection sets a corresponding display cell. Each sustain electrode line and each scan electrode line may be formed by combining a transparent electrode line of a transparent conductive material such as indium tin oxide (ITO) and a metal electrode (bus electrode) line for increasing conductivity. The front dielectric layer is formed by coating the entire surface behind the sustain electrode lines and the scan electrode lines. A protective layer for protecting the panel from a strong electric field, for example, a magnesium monoxide (MgO) layer is formed by applying the entire surface to the rear of the front dielectric layer layer. The plasma forming gas is sealed in the discharge space.

The driving signal of FIG. 1 is used as a driving signal for driving a conventional plasma display panel. That is, one subfield SF has a reset period PR, an address period PA, and a sustain discharge period PS, and address electrode lines A1, A2, ..., Am, and sustain electrode line. Driving signals are applied to the fields X1, ..., Xn and the scan electrode lines Y1, ..., Yn, respectively.

First, the reset period PR applies a reset pulse to all the scan electrode lines Y1,..., And Yn to perform reset discharge, thereby initializing the wall charge state of all the discharge cells. The reset period PR is carried out before entering the address period PA, which is carried out over the entire screen, thus making it possible to create a fairly even and evenly distributed wall charge arrangement. To this end, as shown in FIG. 1, the ground voltage Vg is first applied to the scan electrode lines Y1,..., And Yn, and then the sustain discharge voltage Vs is applied, and the sustain discharge voltage Vs is applied. The rising ramp signal is applied to reach the highest rising voltage (Vset + Vs), which is increased by the rising voltage (Vset), and then rapidly falls to the sustaining discharge voltage (Vs), and falls from the sustaining discharge voltage (Vs). Is applied to reach the lowest falling voltage (Vnf). The ground voltage Vg is applied to the address electrode lines A1, A2, ..., Am during the reset period PR, and the falling ramp signal is applied to the sustain electrode lines X1, ..., Xn. The bias voltage Vb is continuously applied from time to time.

Next, in the address period PA, in order to select a cell to be turned on, a bias voltage Vb is applied to the sustain electrode lines X1, ..., Xn, and the scan electrode lines Y1,. The scan high voltage Vsch is applied to Yn, and the scan pulses having the scan low voltage Vscl are sequentially applied to the scan electrode lines Y1, ..., Yn. A display data signal having an address voltage Va is applied to the address electrode lines A1, A2, ..., Am. As the scan pulse and the display data signal are applied, address discharge is performed in the selected discharge cell.

Next, in the sustain discharge period PS, the sustain electrode lines X1,..., Xn and the scan electrode lines Y1, so that the sustain discharge is performed in the cell to be turned on selected in the address period PA. ..., and a sustain pulse having a sustain discharge voltage Vs is applied alternately. The sustain pulse has a rising slope and reaches a sustain discharge voltage, and has a falling slope and reaches a ground voltage. 2, the sustain pulse applied to the scan electrode Y has a rising slope from time ta to tb and finally reaches the sustain discharge voltage Vs, and the sustain discharge continues from time tb to tc. Maintain the voltage (Vs). It has a falling slope from time tc to td, and finally reaches ground voltage Vg, and continues to have ground voltage from time td to tg. The sustain pulse applied to the sustain electrode X is applied with a ground voltage from time ta to td, has a rising slope from time td to te, and finally reaches the sustain discharge voltage Vs, from time te to tf. The sustain discharge voltage Vs is continuously applied, has a falling slope to tg at a time tf, and finally reaches the ground voltage Vg. As shown in FIG. 2, a sustain pulse in which no section having a common sustain discharge voltage Vs is present is alternately applied to the scan electrode Y and the sustain electrode X. The sustain discharge is performed by the wall charge accumulated in the discharge cell selected by the address discharge and the applied sustain discharge voltage Vs. Plasma is formed from the plasma forming gas of the discharge cells which perform the sustain discharge, and the phosphors of the discharge cells are excited by ultraviolet radiation from the plasma to generate light.

The conventional plasma display panel described above has a three-electrode surface discharge structure, in which the scan electrodes Y and the sustain electrodes X are arranged side by side behind the front substrate. Therefore, during sustain discharge during the driving of the panel by applying the driving signals as shown in FIGS. 1 and 2, the ion particles are accelerated by the electric field formed by the potential applied to the scan electrode Y and the sustain electrode X. Even if the discharge gas collides with the discharge gas, the movement path of the ion particles accelerated by the electric field is limited to a certain range at the rear of the front substrate, so that the collision probability with the discharge gas is extremely low, and the discharge cell is discharged. As a result, the plasma display panel has a problem of low discharge efficiency and poor luminance.

In order to solve the above problems, a plasma display panel having a three-electrode surface discharge structure and having a distance between a scan electrode and a sustain electrode longer than a distance between a scan electrode and an address electrode is provided. The purpose is to improve the life of the panel.

In order to achieve the above object, the present invention, the front substrate and the rear substrate disposed in parallel to the front substrate; Barrier ribs disposed between the front substrate and the rear substrate and defining discharge cells generating discharge; Scan electrode lines and sustain electrode lines disposed in a front dielectric layer formed on a front substrate in a rear substrate direction and extending in one direction in which discharge cells extend; Address electrode lines disposed in a rear dielectric layer formed on a rear substrate in a front substrate direction and extending to cross a direction in which the scan electrode lines and the sustain electrode lines extend; A phosphor layer disposed in the discharge cells and positioned above the address electrode lines; And a discharge gas in the discharge cells; wherein the distance between the scan electrode lines and the sustain electrode lines that partition the discharge cells is longer than the distance between the address electrode lines and the scan electrode lines, and is reset. Driven by a drive signal having a section, an address section, and a sustain discharge section,

In the sustain discharge period, the first sustain pulse and the second sustain pulse having the rising slope reaching the first voltage and the falling slope reaching the ground voltage are alternately applied to the scan electrode lines and the sustain electrode lines, respectively. And a section in which the first voltage is applied in the first sustain pulse and the second sustain pulse overlap each other in time, and a short pulse is applied to the address electrode lines.

According to another aspect of the present invention, the plasma display panel,

In the reset period, the rising ramp signal is applied to the scan electrode lines at the first voltage to finally reach the third voltage which is increased by the second voltage, and the falling ramp signal is applied at the first voltage to finally the fourth voltage. A voltage is reached, a fifth voltage is applied from the falling ramp signal to the sustain electrode lines, and a ground voltage is applied to the address electrode lines;

In the address period, scan pulses having a seventh voltage are sequentially applied to sixth voltages to scan electrode lines, and display data signals having an eighth voltage are applied to address electrodes according to scan pulses. The fifth voltage may be continuously applied to the scan electrode lines.

According to another feature of the invention, the pulse width of the short pulse may be less than half of the pulse width of the first sustain pulse and the second sustain pulse.

According to another feature of the invention, the short pulse has a ninth voltage less than or equal to the magnitude of the eighth voltage, the ninth voltage is the moment when the first sustain pulse and the second sustain pulse reaches the first voltage; Can be applied to.

According to another feature of the invention, the short pulse has a tenth voltage less than or equal to the magnitude of the eighth voltage, the tenth voltage may be applied at the moment the first sustain pulse reaches the first voltage. .

According to another feature of the present invention, the short pulse has an eleventh voltage less than or equal to the magnitude of the eighth voltage, and the eleventh voltage may be applied at the moment when the second sustain pulse reaches the first voltage. .

Hereinafter, with reference to the accompanying drawings will be described in detail an embodiment of the present invention.

3 is an exploded perspective view showing the plasma display panel of the present invention.

4 is a plan view of the plasma display panel of FIG. 3 taken along line II-II.

A description with reference to FIGS. 3 to 4 is as follows.

The plasma display panel 1 of FIG. 3 includes a front panel 110 and a rear panel 120, the front panel 110 having a front substrate 111, and the rear panel 120 having a rear substrate 121. ). The plasma display panel 1 is disposed between the front substrate 111 and the rear substrate 121, and partition walls 124 defining discharge cells Ce, which are spaces for generating discharge and generating light, for realizing an image. ).

The front panel 110 is disposed on the rear of the front substrate 111, that is, the rear surface of the front substrate, and includes a front dielectric layer disposed to cover the scan electrode lines 112 and the sustain electrode lines 113, which will be described later. 115). The scan electrode lines 112 and the sustain electrode lines 113 are bus electrodes 112a and 113a made of a metallic material to increase conductivity, and transparent electrodes 112b and 113b made of a transparent conductive material such as indium tin oxide (ITO). ). The scan electrode lines 112 and the sustain electrode lines 113 extend in one direction in which the discharge cells Ce extend.

The front passivation layer 116 for protecting the front dielectric layer 115 is preferably provided on the rear surface of the front dielectric layer 115.

The rear panel 120 may include the rear substrate 121 and a rear dielectric layer 123 formed on the rear substrate 121 in the direction of the front substrate 121. In the rear dielectric layer 123, address electrode lines 122 extend in a direction orthogonal to a direction in which the scan electrode lines 112 and the sustain electrode line 113 extend.

In addition, the rear panel 120 has partition walls 124 partitioning discharge cells on the rear dielectric layer 123, and the phosphor layer 125 disposed in a space defined by the partition walls 124. ). In order to protect the phosphor layer 125, it is preferable to provide a rear protective foil 128 on the entire surface of the phosphor layer 125.

The front panel 110 and the rear panel 120 are preferably coupled and sealed by a coupling member such as a frit (not shown), and need not necessarily be coupled by a coupling member such as frit, When the discharge gas in the discharge cells (Ce) is in a vacuum state, it may be combined at a pressure according to the vacuum state. On the other hand, the discharge cells (Ce) is made of any one or two or more of the mixed gas of neon (Ne), helium (He), or argon (Ar) including xenon (Xe) gas before and after 10%. The discharge gas is charged. On the other hand, it is also possible to make the content ratio of xenon (Xe) gas in the discharge gas to 10% or more.

The front substrate 111 and the rear substrate 121 are generally formed of glass, and the front substrate is preferably formed of a material having high light transmittance. On the other hand, the rear substrate 121 does not necessarily need to transmit light, and a wider selection range of materials than the front substrate 111 does not necessarily require a material having a high light transmittance such as glass. Rather, it may be more desirable to use a variety of materials that have high light reflectance or that can reduce reactive power.

In order to improve the brightness of the plasma display panel, a reflective layer (not shown) is disposed on the top surface of the rear substrate 121 or the top surface of the rear dielectric layer 123 or includes a light reflective material in the rear dielectric layer 123. The visible light generated by the phosphor may be efficiently reflected forward.

Since the transparent electrodes 112b and 113b of the scan electrode lines 112 and the sustain electrode lines 113 are disposed on the rear surface of the front substrate 111, the transparent electrodes 112b and 113b easily transmit visible light generated from the phosphor layer 125. You should be able to. As a material of the transparent electrode 112 having a good light transmittance, a material such as ITO, SnO 2, or ZnO may be used, and ITO is preferably used. On the other hand, since the light transmittance does not have to be considered in the address electrode lines 122, it is preferable that Ag, Cu, Cr, etc. having a wide selection range of electrode materials and high electrical conductivity are used. A front passivation layer 116 may be formed on the rear surface of the front dielectric layer 115, and the front passivation layer 116 may protect the front dielectric layer 115 and emit secondary electrons so that the discharge may occur easily. I can help.

The distance between the scan electrode line 112 and the sustain electrode line 113 in the discharge cell Ce (hereinafter referred to as d1) is the scan electrode line 112 or the sustain electrode line 113 in the discharge cell ce. ) And a distance between the address electrode and the address electrode (hereinafter referred to as d2). It is preferable to make d1 into 100 micrometers or more.

Meanwhile, the partition walls 124 disposed between the front substrate 111 and the rear substrate 121 are formed to define discharge cells Ce together with the front substrate 111 and the rear substrate 121. In FIG. 3, the partition walls 124 divide the discharge cells Ce into a matrix, but are not limited thereto, and may be partitioned into various shapes such as a honeycomb form and a delta form. In addition, although the cross section of the discharge cell Ce is illustrated in FIG. 4 as being rectangular, the present invention is not limited thereto and may be a polygon such as a triangle, a pentagon, or a circle, an ellipse, or the like.

The barrier ribs 124 may be formed on the rear dielectric layer 123, and may be formed of a glass component including elements such as Pb, B, Si, Al, and O, and the like, as necessary. Fillers such as, ZrO 2, TiO 2, and Al 2 O 3 and pigments such as Cr, Cu, Co, Fe, TiO 2 may be included. The partition walls 124 secure a space in which the phosphor layer 125 may be applied, and together with the front partition walls 115, the partition walls 124 may be formed of discharge gas charged inside the front panel 110 and the rear panel 120. It supports the pressure generated due to the vacuum state (for example 0.5 atm), secures the space of the discharge cell (Ce), and serves to prevent cross talk between the discharge cells (Ce). Can be. A red, green, or blue light emitting phosphor layer 125 may be disposed in a space defined by the partitions 124, and the phosphor layer 125 is partitioned by the partitions 124.

The phosphor layer 125 is a phosphor paste in which any one of a phosphor, a solvent, and a binder of a red light emitting phosphor, a green light emitting phosphor, and a blue light emitting phosphor is mixed is applied to the front and rear partitions 124 of the rear dielectric layer 123. After forming and drying and firing. Examples of the red light emitting phosphor include Y (V, P) O 4: Eu, and examples of the green light emitting phosphor include ZnSi 4 4: Mn, YBO 3: Tb, and the blue light emitting phosphor include BAM: Eu.

A rear passivation layer 128 made of MgO or the like may be formed on the entire surface of the phosphor layer 125. The rear passivation layer 128 prevents the phosphor layer from deteriorating due to collision of discharge particles when discharge occurs in the discharge cell Ce, and emits secondary electrons so that the discharge can easily occur. I can help.

5 is a view schematically illustrating an electrode arrangement of the plasma display panel of FIG. 3.

Referring to FIGS. 3 to 5, the scan electrode lines Y1,..., Yn and the sustain electrode lines X1,..., Xn are arranged in parallel in parallel. That is, scan electrode lines Y1,..., Yn and sustain electrode lines X1,..., Xn are disposed in the front dielectric layers 115. Address electrode lines A1, A2, ..., Am are disposed so as to be orthogonal to the scan electrode lines Y1, ..., Yn and sustain electrode lines X1, ..., Xn. In the region where the scan electrode lines Y1, ..., Yn and the sustain electrode lines X1, ..., Xn intersect with the address electrode lines A1, A2, ..., Am. The discharge cells Ce are partitioned.

FIG. 6 is a block diagram schematically illustrating an apparatus for driving a plasma display panel for driving the plasma display panel of FIG. 3.

Referring to FIGS. 5 and 6, the driving apparatus of the plasma display panel includes an image processor 400, a logic controller 402, a Y driver 404, an address driver 406, an X driver 408, and a plasma. The display panel 1 is provided.

The image processor 400 receives an external video signal such as a PC signal, a DVD signal, a video signal, or a TV signal from the outside, converts an analog signal into a digital signal, and processes the digital signal into an internal video signal. The internal video signals are 8-bit red (R), green (G), and blue (B) image data, clock signals, and vertical and horizontal sync signals, respectively.

The logic controller 402 receives an internal image signal from the image processor 400 and undergoes a gamma correction, an automatic power control (APC) step, and the like, such as an address driving control signal SA, a Y driving control signal SY, and Outputs the X drive control signal SX.

The Y driver 404 receives the Y drive control signal SY from the logic controller 402, and has an erase pulse having an erase voltage for initialization discharge in the reset period (PR of FIG. 8), and an address period (FIG. 8). And a scan signal having a negative scan low voltage (Vscl in FIG. 8) sequentially along the vertical direction of the panel 1 while a positive scan high voltage (Vsch in FIG. 8) is applied to PA). The sustain pulses having the positive sustain discharge voltage (Vs in FIG. 8) and the ground voltage (Vg in FIG. 8) in the PS of FIG. 8 are connected to the scan electrode lines Y1, ..., of the plasma display panel 1. Yn).

The address driver 406 receives the address drive control signal SA from the logic controller 402 and has an address voltage (Va in FIG. 8) in a cell to be turned on among all cells in the address period (PA in FIG. 8). The display data signal is output to the address electrode lines of the plasma display panel 1. Also in connection with the present invention, a short pulse is applied in the sustain discharge period (Vs in FIG. 8). The voltage of the short pulse may be less than or equal to the address voltage Va of FIG. 8.

The X driving unit 408 receives the X driving control signal SX from the logic control unit 402, and the bias voltage (Vb of FIG. 8) in the reset period (PR of FIG. 8) and the address period (PA of FIG. 8). And a sustain pulse having a positive sustain discharge voltage (Vs in FIG. 8) and a ground voltage (Vg in FIG. 8) in the sustain discharge period (PS in FIG. 8). , ..., Xn).

FIG. 7 illustrates an address-display separation driving method for Y electrode lines as an example of a driving method for driving the plasma display panel of FIG. 3.

5 and 7, a unit frame may be divided into a predetermined number, for example, eight subfields SF1,..., SF8 to realize time division gray scale display. Further, each subfield SF1, ... SF8 is divided into a reset section (not shown), an address section A1, ..., A8, and a sustain discharge section S1, ..., S8. .

In each address section A1, ..., A8, a display data signal is applied to the address electrode lines A1, A2, ..., Am and at the same time, the scan electrode lines Y1, ..., Yn Are sequentially applied.

In each sustain discharge section S1, ..., S8, sustain pulses are alternately applied to the scan electrode lines Y1, ..., Yn and sustain electrode lines X1, ..., Xn. , Sustain discharge occurs in the discharge cells in which wall charges are formed in the address periods A1, ..., A8.

The luminance of the plasma display panel is proportional to the number of sustain discharge pulses in the sustain discharge sections S1, ..., S8 occupied in the unit frame. When one frame forming one image is represented by eight subfields and 256 gradations, each subfield is kept different at a ratio of 1, 2, 4, 8, 16, 32, 64, and 128 in turn. The number of pulses can be assigned. In order to obtain luminance of 133 gradations, cells may be addressed and sustained and discharged during the subfield 1 period, the subfield 3 period, and the subfield 8 period.

The number of sustain discharges allocated to each subfield may be variably determined according to weights of the subfields according to the APC (Automatic Power Control) step. The number of sustain discharges allocated to each subfield can be variously modified in consideration of gamma characteristics and panel characteristics. For example, the gray level assigned to subfield 4 may be lowered from 8 to 6, and the gray level assigned to subfield 6 may be increased from 32 to 34. In addition, the number of subfields forming one frame can be variously modified according to design specifications.

FIG. 8 is a timing diagram for describing the first embodiment as a drive signal of the plasma display panel of FIG. 3.

FIG. 9 is a timing diagram for describing in detail the driving signal of the sustain discharge period of FIG. 8.

Referring to FIGS. 3, 8, and 9, first, the subfield SF includes a reset period PR, an address period PA, and a sustain discharge period PS.

In the reset period PR, the ground voltage Vg is first applied to the scan electrode lines Y1, ..., Yn. Next, the sustain discharge voltage Vs, which is the first voltage, is rapidly applied, and the rising ramp signal is applied from the first voltage Vs, and the highest rise is the third voltage that is raised by the rising voltage Vset, which is the second voltage. The voltage Vset + Vs is reached. The weak discharge occurs due to the application of the rising ramp signal having an inclined slope, and the negative discharge starts to accumulate in the vicinity of the scan electrode lines Y1,..., And Yn. Next, after rapidly falling to the first voltage Vs, a falling ramp signal is applied to reach the fourth falling voltage Vnf. A weak discharge is generated by applying a falling ramp signal having a steep slope, and a portion of the negative charges accumulated near the scan electrode lines Y1, ..., Yn is emitted while the weak discharge is generated. As a result, a negative amount of negative charge suitable for generating an address discharge remains in the vicinity of the scan electrode lines Y1, ..., and Yn. Since the falling ramp signal is applied to the scan electrode lines Y1,..., And Yn, a bias voltage Vb, which is a fifth voltage, is applied to the sustain electrode lines X1,..., Xn. The ground voltage Vg is applied to the address electrode lines A1, A2, ..., Am during the reset period PR.

Next, in order to select a cell to be turned on in the address period PA, a scan high voltage Vsch, which is a sixth voltage, is first applied to the scan electrode lines Y1,. A scan pulse having a scan low voltage Vscl, which is a seventh voltage, is applied to each line. A display data signal having an address voltage Va, which is an eighth voltage, is applied to the address electrode lines A1, A2, ..., Am in accordance with the scan pulse. The fifth voltage Vb is continuously applied to the sustain electrode lines X1,..., And Xn. The address discharge is performed by the eighth voltage Va, the seventh voltage Vscl, the wall voltage caused by the negative charge near the scan electrode Y, and the wall voltage caused by the positive charge near the address electrode A. After the address discharge is performed, positive charges are accumulated near the scan electrode Y, and negative charges are accumulated near the sustain electrode X.

In the sustain discharge period PS, the first sustain pulse and the second sustain pulse having the rising slope reaching the first voltage Vs and having the falling slope reaching the ground voltage Vg are respectively the scan electrode lines. (Y1, ..., Yn) and sustain electrode lines (X1, ..., Xn) are alternately applied to each other, and have the first voltage (Vs) at the first sustain pulse and the second sustain pulse. The sections overlap in time.

A short pulse is applied to the address electrode lines A1, A2, ..., Am, and the short pulse is for improving discharge efficiency during sustain discharge, and the first voltage is applied to the first sustain pulse and the second sustain pulse. It is preferable that a short pulse is applied at the instant (Vs) is applied. In addition, the pulse width of the short pulse may be less than half of the pulse widths of the first sustain pulse and the second sustain pulse. The short pulse may have a ninth voltage Vs1, and the magnitude of the ninth voltage Vs1 may be smaller than or equal to the magnitude of the eighth voltage Va.

The structure of the plasma display panel in Fig. 3 is characterized in that the distance d1 between the sustain electrode and the scan electrode in the discharge cell is longer than the distance d2 between the scan electrode or the sustain electrode and the address electrode. For example, d1 may be 200 μm or more. When d1> d2, the discharge volume becomes large at the time of discharge, and the brightness improves. However, if the distance of d1 is too large, the sustain discharge can be performed only by increasing the voltage applied to the sustain electrode and the voltage applied to the scan electrode, and the high voltage must be supplied from the power supply device, thereby increasing the manufacturing cost of the plasma display panel. Will be higher. Therefore, it is preferable to make d1 more than 100 micrometers. In addition, in order to solve the above problems, first, there is a period in which the first voltage is overlapped in the first sustain pulse applied to the scan electrode and the second sustain pulse applied to the sustain electrode during sustain discharge. It is preferable to apply a short pulse to the electrode.

The first sustain pulse and the second sustain pulse of FIG. 8 are overlapping waveforms in which sections in which the first voltage is applied overlap each other. Referring to FIG. 9 in detail, from time t1 to t2, the first sustain pulse applied to the scan electrode lines Y1, ..., Yn has a rising slope and finally at the first voltage Vs. To reach. At this time, the second sustain pulse applied to the sustain electrode lines X1,..., Xn has a ground voltage Vg. From time t2 to t4, the first sustain pulse continues to have the first voltage Vs. On the other hand, the second sustain pulse continues to have the ground voltage Vg from time t2 to t3, has a rising slope from time t3 to t4, and finally reaches the first voltage Vs. As a result, the first sustain pulse and the second sustain pulse overlap the first voltage Vs at time t4. Then from time t4 to t5, the first sustain pulse has a falling slope and finally reaches the ground voltage Vg. From time t4 to t7, the second sustain pulse has a first voltage Vs. From time t5 to t6, the first sustain pulse has a ground voltage Vg. From time t6 to t7, the first holding pulse has a rising slope, finally reaching the first voltage, and repeating the above process. From time t7 to t8, the second holding pulse has a falling slope, finally reaching the ground voltage, and continuing the ground voltage from time t8 to t9. The rising and falling slopes are typically used for energy charging and recovery.

 The overlapping waveform in the sustain discharge period PS is such that a section having the first voltage Vs overlaps each other in the first sustain pulse applied to the scan electrode Y and the second sustain pulse applied to the sustain electrode X. 9 is not limited to overlapping at time t4 as shown in FIG. 9, and may overlap for more time. The longer the overlapping section, the shorter the period between the first sustain pulse and the second sustain pulse, and the shorter the interval between the sustain discharges. In other words, when the discharge frequency is increased, the space charge can be well utilized in sustain discharge, and the luminous efficiency can be improved.

In the case where the first sustain pulse has the first voltage Vs, the first positive voltage Vs applied to the scan electrode Y, the ground voltage Vg applied to the sustain electrode X, and the scan As the sustain discharge is performed due to the wall voltage due to the positive charge accumulated near the electrode Y and the wall voltage due to the negative charge accumulated near the sustain electrode X, a negative charge is accumulated near the scan electrode Y, and the sustain electrode A positive charge builds up near (X). At the moment when the first sustain pulse reaches the first voltage Vs, a short pulse is applied to the address electrode A, whereby a part of the negative charge accumulated on the scan electrode Y is located near the address electrode A. FIG. Move to. As the discharge volume is increased to the vicinity of the address electrode A due to the application of the short pulse to the address electrode A, the sustain discharge is smoothly performed, thereby increasing the discharge efficiency and improving the luminance. In addition, since the discharge volume is increased, ion sputtering by the charged particles of the discharge gas in the phosphor is reduced as compared with the conventional, thereby improving the life of the plasma display panel.

Next, when the second sustain pulse has the first voltage, the first positive voltage Vs applied to the sustain electrode X, the ground voltage Vg applied to the scan electrode Y, and the sustain voltage are applied. As the sustain discharge is performed due to the wall voltage due to the positive charge accumulated near the electrode X and the wall voltage due to the negative charge accumulated near the scan electrode Y, a positive charge is accumulated near the scan electrode Y, and the sustain electrode A negative charge builds up near (X). At the moment when the second sustain pulse reaches the first voltage Vs, a short pulse is applied to the address electrode A. FIG. As the discharge volume is increased to the vicinity of the address electrode A due to the application of the short pulse to the address electrode A, the sustain discharge is smoothly performed, thereby increasing the discharge efficiency and improving the brightness and the life of the panel.

 The above steps are repeated continuously, which causes the sustain discharge to continue.

However, the pulse width of the applied short pulse is half of the pulse width of the first sustain pulse and the second sustain pulse so that a large amount of negative charges are not taken from the scan electrode Y or the sustain electrode X due to the application of the short pulse. The smaller one is preferable, and the ninth voltage Vs1 of the short pulse is preferably smaller than the eighth voltage Va. However, in consideration of an increase in manufacturing cost caused by supplying various powers from the power supply device, the ninth voltage Vs1 may be equal to the magnitude of the eighth voltage Va.

FIG. 10 is a timing diagram for describing a second embodiment as a drive signal of the plasma display panel of FIG. 3.

FIG. 11 is a timing diagram for describing the driving signal of the sustain discharge period of FIG. 10 in detail.

Referring to FIGS. 3, 11, and 12, first, the subfield SF includes a reset period PR, an address period PA, and a sustain discharge period PS.

The driving signals in the reset period PR and the address period Pa are the same as in FIG.

In the sustain discharge period PS, the first sustain pulse and the second sustain pulse having the rising slope reaching the first voltage Vs and having the falling slope reaching the ground voltage Vg are respectively the scan electrode lines. (Y1, ..., Yn) and the sustain electrode lines (X1, ..., Xn) are alternately applied to each other, and the first voltage (Vs) in the first sustain pulse and the second sustain pulse The sections with overlap in time.

A short pulse is applied to the address electrode lines A1, A2, ..., Am, and the short pulse is for improving the discharge efficiency during sustain discharge, and the first voltage Vs is applied from the first sustain pulse. It is preferable that a short pulse is applied at the moment. In addition, the pulse width of the short pulse may be less than half of the pulse width of the first sustain pulse. In addition, the short pulse may have a tenth voltage Vs2, and the magnitude of the tenth voltage Vs2 may be smaller than or equal to the magnitude of the eighth voltage Va.

The first sustain pulse and the second sustain pulse of FIG. 10 are overlapping waveforms in which sections in which the first voltage is applied overlap each other. Referring to FIG. 11 in detail, from time t11 to t12, the first sustain pulse applied to the scan electrode lines Y1, ..., Yn has a rising slope and finally at the first voltage Vs. To reach. At this time, the second sustain pulse applied to the sustain electrode lines X1,..., Xn has a ground voltage Vg. From time t12 to t14, the first sustain pulse continues to have the first voltage Vs. On the other hand, the second sustain pulse continues to have the ground voltage Vg from time t12 to t13, and has a rising slope from time t13 to t14 and finally reaches the first voltage Vs. As a result, the first sustain pulse and the second sustain pulse overlap the first voltage Vs at time t14. Next, from time t14 to t15, the first sustain pulse has a falling slope and finally reaches the ground voltage Vg. From time t14 to t17, the second sustain pulse has a first voltage Vs. From time t15 to t16, the first sustain pulse has a ground voltage Vg. From time t16 to t17, the first holding pulse has a rising slope, finally reaching the first voltage, and repeating the above process. From time t17 to t18, the second holding pulse has a falling slope, finally reaching the ground voltage, and continuing the ground voltage from time t18 to t19. The rising and falling slopes are typically used for energy charging and recovery.

The overlapping waveform in the sustain discharge period PS is such that a section having the first voltage Vs overlaps each other in the first sustain pulse applied to the scan electrode Y and the second sustain pulse applied to the sustain electrode X. It is not limited to overlapping at time t14 as shown in FIG. 11, and may overlap for more time. The longer the overlapping section, the shorter the period between the first sustain pulse and the second sustain pulse, and the shorter the interval between the sustain discharges. In other words, when the discharge frequency is increased, the space charge can be well utilized in sustain discharge, and the luminous efficiency can be improved.

In the case where the first sustain pulse has the first voltage Vs, the first positive voltage Vs applied to the scan electrode Y, the ground voltage Vg applied to the sustain electrode X, and the scan As the sustain discharge is performed due to the wall voltage due to the positive charge accumulated near the electrode Y and the wall voltage due to the negative charge accumulated near the sustain electrode X, a negative charge is accumulated near the scan electrode Y, and the sustain electrode A positive charge builds up near (X). On the other hand, a short pulse is applied to the address electrode A at the moment when the first sustain pulse reaches the first voltage Vs. Negative charges accumulated near the scan electrode Y move near the address electrode A due to the short pulse, thereby increasing the discharge volume and improving luminance and panel life. However, the pulse width of the applied short pulse is preferably less than half of the pulse width of the first sustain pulse so that a large amount of negative charges are not drawn from the scan electrode Y due to the application of the short pulse. The tenth voltage Vs2 is preferably smaller than the eighth voltage Va. However, in consideration of an increase in manufacturing cost caused by supplying various powers from the power supply device, the tenth voltage Vs2 may be equal to the magnitude of the eighth voltage Va.

Next, when the second sustain pulse has the first voltage, the first positive voltage Vs applied to the sustain electrode X, the ground voltage Vg applied to the scan electrode Y, and the sustain voltage are applied. As the sustain discharge is performed due to the wall voltage due to the positive charge accumulated near the electrode X and the wall voltage due to the negative charge accumulated near the scan electrode Y, a positive charge is accumulated near the scan electrode Y, and the sustain electrode A negative charge builds up near (X).

The above steps are repeated continuously, which causes the sustain discharge to continue.

FIG. 12 is a timing diagram for describing a third embodiment as a drive signal of the plasma display panel of FIG. 3.

FIG. 13 is a timing diagram for describing the driving signal of the sustain discharge period of FIG. 12 in detail.

This will be described with reference to FIGS. 3, 12, and 13.

The driving signals in the reset period PR and the address period Pa are the same as in FIG.

In the sustain discharge period PS, the first sustain pulse and the second sustain pulse having the rising slope reaching the first voltage Vs and having the falling slope reaching the ground voltage Vg are respectively the scan electrode lines. (Y1, ..., Yn) and the sustain electrode lines (X1, ..., Xn) are alternately applied to each other, and the first voltage (Vs) in the first sustain pulse and the second sustain pulse The sections with overlap in time.

A short pulse is applied to the address electrode lines A1, A2, ..., Am, and the short pulse is for improving the discharge efficiency during sustain discharge, and the first voltage Vs is applied to the second sustain pulse. It is preferable that a short pulse is applied at the moment. In addition, the pulse width of the short pulse may be less than half of the pulse width of the second sustain pulse. In addition, the short pulse may have an eleventh voltage Vs3, and the magnitude of the eleventh voltage Vs3 may be smaller than or equal to the magnitude of the eighth voltage Va.

The first sustain pulse and the second sustain pulse of FIG. 12 are overlapping waveforms in which sections to which the first voltage is applied overlap each other. Referring to FIG. 13, from time t21 to t22, the first sustain pulse applied to the scan electrode lines Y1,..., And Yn has a rising slope and finally reaches the first voltage Vs. To reach. At this time, the second sustain pulse applied to the sustain electrode lines X1,..., Xn has a ground voltage Vg. From time t22 to t24, the first sustain pulse continues to have the first voltage Vs. On the other hand, the second sustain pulse continues to have the ground voltage Vg from time t22 to t23, has a rising slope from time t23 to t24, and finally reaches the first voltage Vs. As a result, the first sustain pulse and the second sustain pulse overlap the first voltage Vs at time t24. Then from time t24 to t25 the first sustain pulse has a falling slope and finally reaches ground voltage Vg. From time t24 to t27, the second sustain pulse has a first voltage Vs. From time t25 to t26, the first sustain pulse has a ground voltage Vg. From time t26 to t27, the first holding pulse has a rising slope, finally reaching the first voltage, and repeating the above process. From time t27 to t28, the second holding pulse has a falling slope and finally reaches ground voltage, and the ground voltage continues from time t28 to t29. The rising and falling slopes are typically used for energy charging and recovery.

The overlapping waveform in the sustain discharge period PS is such that a section having the first voltage Vs overlaps each other in the first sustain pulse applied to the scan electrode Y and the second sustain pulse applied to the sustain electrode X. It is not limited to overlapping at time t24 as shown in FIG. 13, and may overlap for more time. The longer the overlapping section, the shorter the period between the first sustain pulse and the second sustain pulse, and the shorter the interval between the sustain discharges. In other words, when the discharge frequency is increased, the space charge can be well utilized in sustain discharge, and the luminous efficiency can be improved.

In the case where the first sustain pulse has the first voltage Vs, the first positive voltage Vs applied to the scan electrode Y, the ground voltage Vg applied to the sustain electrode X, and the scan As the sustain discharge is performed due to the wall voltage due to the positive charge accumulated near the electrode Y and the wall voltage due to the negative charge accumulated near the sustain electrode X, a negative charge is accumulated near the scan electrode Y, and the sustain electrode A positive charge builds up near (X).

Next, when the second sustain pulse has the first voltage, the first positive voltage Vs applied to the sustain electrode X, the ground voltage Vg applied to the scan electrode Y, and the sustain voltage are applied. As the sustain discharge is performed due to the wall voltage due to the positive charge accumulated near the electrode X and the wall voltage due to the negative charge accumulated near the scan electrode Y, a positive charge is accumulated near the scan electrode Y, and the sustain electrode A negative charge builds up near (X). On the other hand, a short pulse is applied to the address electrode A when the second sustain pulse reaches the first voltage Vs. The negative charge accumulated near the sustain electrode X is moved to the vicinity of the address electrode A by the short pulse, thereby increasing the discharge volume and improving luminance and panel life. However, the pulse width of the applied short pulse is preferably less than half of the pulse width of the second sustain pulse so that a large amount of negative charges are not drawn from the sustain electrode X due to the application of the short pulse. The eleventh voltage Vs3 is preferably smaller than the eighth voltage Va. However, in consideration of an increase in manufacturing cost caused by supplying various powers from the power supply device, the eleventh voltage Vs3 may be equal to the magnitude of the eighth voltage Va.

The above steps are repeated continuously, which causes the sustain discharge to continue.

14A to 14A of FIGS. 14A and 6B show the potential distribution inside the discharge cell, the electron density, and the ultraviolet ray of 147 nm during the sustain discharge when the drive signal of FIG. 1 is applied and the drive signal of FIG. 8 is applied to the plasma display panel of FIG. Distribution, 173 nm ultraviolet distribution, xenon (Xe) ion distribution, and neon (Ne) ion distribution, respectively.

First, when comparing a1 and b1, it can be seen that b1 is uniformly enlarged in the sustain electrode and the scan electrode due to the application of the overlapping waveform and the short pulse. Next, when comparing a2 and b2, due to the application of the overlapping waveform and the short pulse, the distribution of electron density is partially distributed near the address electrode, unlike a2, which is distributed only around the sustain electrode and the scan electrode. It can be seen that. Next, comparing a3 and b3, it can be seen that b3 has an enlarged distribution of 147 nm ultraviolet rays inside the discharge cell due to the application of an overlapping waveform and a short pulse. Next, comparing a4 and b4, it can be seen that b4 has an enlarged ultraviolet distribution of 173 nm inside the discharge cell due to the application of the overlapping waveform and the short pulse. Comparing a5 and b5, it can be seen that b5 has an enlarged xenon ion distribution inside the discharge cell due to the application of an overlapping waveform and a short pulse. Comparing a6 and b6, it can be seen that b6 has an enlarged neon (Ne) ion distribution in the discharge cell due to the application of the overlapping waveform and the short pulse.

According to the present invention as described above, the following effects can be obtained.

First, in the plasma display panel, the distance between the sustain electrode and the scan electrode is longer than the distance between the scan electrode or the sustain electrode and the address electrode in the three-electrode surface discharge structure, and, in theory, the discharge volume is increased to improve luminance.

Second, in order to solve the disadvantage that a high voltage is required in the discharge generated in the structure of the plasma display panel, the first voltage Vs at the first sustain pulse applied to the scan electrode and the second sustain pulse applied to the sustain electrode during sustain discharge. By overlapping the sections where) is applied, the discharge cycle is faster, the brightness and discharge efficiency of the panel are improved, and the sustain discharge time can be shortened. You may.

Third, by attracting negative charge near the address electrode by applying a short pulse having a positive voltage to the address electrode at the moment when the first voltage Vs is applied from the first sustain pulse or the second sustain pulse during sustain discharge, The discharge volume is improved by increasing the electron density inside the discharge cell, expanding the ultraviolet distribution at 147nm and 173nm, and expanding the Xen and Ne ion distribution, and improving the efficiency of ion particles. Ion sputtering can be reduced, thereby improving the life of the panel.

Although the present invention has been described with reference to the embodiments shown in the drawings, this is merely exemplary, and it will be understood by those skilled in the art that various modifications and equivalent other embodiments are possible. Therefore, the true technical protection scope of the present invention will be defined by the technical spirit of the appended claims.

Claims (6)

A rear substrate disposed in parallel with the front substrate and the front substrate; Barrier ribs disposed between the front substrate and the rear substrate and defining discharge cells generating discharge; Scan electrode lines and sustain electrode lines disposed in the front dielectric layer formed on the front substrate in the rear substrate direction and extending in one direction in which the discharge cells extend; Address electrode lines disposed on a rear dielectric layer formed on the rear substrate in a direction toward the front substrate and extending to cross a direction in which the scan electrode lines and the sustain electrode lines extend; A phosphor layer disposed in the discharge cells and positioned above the address electrode lines; And a discharge gas in the discharge cells, wherein a distance between the scan electrode lines and the sustain electrode lines that divide the discharge cells is longer than a distance between the address electrode lines and the scan electrode lines. Formed, Driven by a drive signal having a reset section, an address section, and a sustain discharge section, In the sustain discharge period, the first sustain pulse and the second sustain pulse having the rising slope reaching the first voltage and having the falling slope reaching the ground voltage are respectively applied to the scan electrode lines and the sustain electrode lines. Alternately applied, a section in which the first voltage is applied in the first sustain pulse and the second sustain pulse overlap each other in time, and a short pulse is applied to the address electrode lines; . The method of claim 1, In the reset period, a rising ramp signal is applied to the scan electrode lines at the first voltage to reach a third voltage which is finally increased by a second voltage, and a falling ramp signal is finally applied at the first voltage. Reaches a fourth voltage, a fifth voltage is applied from the falling ramp signal to the sustain electrode lines, and a ground voltage is applied to the address electrode lines; In the address period, a scan pulse having a seventh voltage is sequentially applied to the scan electrode lines while a sixth voltage is applied, and a display data signal having an eighth voltage is applied to the address electrodes according to the scan pulse. And the fifth voltage is continuously applied to the scan electrode lines. The method of claim 2, And the pulse width of the short pulse is less than half of the pulse widths of the first sustain pulse and the second sustain pulse. The method of claim 3, wherein the short pulse, And a ninth voltage less than or equal to the magnitude of the eighth voltage, wherein the ninth voltage is applied when the first sustain pulse and the second sustain pulse reach the first voltage. . The method of claim 3, wherein the short pulse, And a tenth voltage less than or equal to the magnitude of the eighth voltage, wherein the tenth voltage is applied at the moment when the first sustain pulse reaches the first voltage. The method of claim 3, wherein the short pulse, And an eleventh voltage less than or equal to the magnitude of the eighth voltage, wherein the eleventh voltage is applied when the second sustain pulse reaches the first voltage.

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