Plasma display, driving apparatus for a plasma display panel and driving method thereof

Abstract

A plasma display panel driving method for a display panel having a plurality of electrodes forming cells, including a first electrode group arranged on a permeable substrate and being capable of being driven in common, a second electrode group arranged in parallel with the first electrode group on the permeable substrate and being capable of being driven independently, a third electrode group arranged perpendicular to the first and second electrode groups on another substrate and being capable of being driven independently. The driving method supplying a voltage with a fast rising leading edge so as to immediately produce a maximum electric discharge one time per a sub-field in a cell in which an electric discharge was performed beforehand and supplying another voltage without causing any electric discharge under a first condition.

Description

BACKGROUND OF THE INVENTION

The invention relates to plasma display, driving apparatus for a plasma display panel and driving method thereof for use, for example, as a display apparatus for a personal computer or workstation, a flat type wall hanging television receiver, or for a display apparatus for advertising and information. This invention is preferably applicable to AC type plasma display devices.

In plasma display, one field is divided into several sub-fields, and each pixel (cell) emits light by exciting a phosphor using ultraviolet rays that are generated by a electric discharge carried out in the cell. The cell that emits light is selected by an address electric discharge between two set of electrodes which are provided perpendicular to each other on a front side glass substrate and a back side glass substrate, respectively, and are capable of being driven independently.

A first example of a plasma display device is disclosed, for example, in Japanese Patent Application Laid-Open No. 1994/186927. In this first example, the condition of electrically charged particles in all cells is equalized for surely prohibiting the lighting of some cells which are not intended to emit light, and two sets of light emitting discharges, that is, a full writing electric discharge and a full erasing electric discharge in each sub-field are carried out so as to be able to use a low voltage for an address electric discharge. Therefore, the contrast is deteriorated because light emitting occurs on the full panel when black is displayed.

A second example is disclosed, for example, in Japanese Patent Application Laid-Open No. 1995/49663. In the second example, a plurality of sub-fields having the same brightness gradations are arranged to form a sub-field block, and several blocks are provided. In sub-field blocks, a preliminary discharge, including a full writing electric discharge and a fine line erasing electric discharge, is performed in one sub-field, and a writing electric discharge and a erasing electric discharge for a pixel is carried out one time. Therefore, deterioration of the panel is reduced and the contrast of the display is improved. The second example discloses one solution to improve the contrast, but no means is disclosed to improve the contrast in an arrangement in which plural sub-fields having different brightness gradations are provided for forming one sub-field block.

About 3 μsec to 4 μsec is needed to write one line of plasma panel, and an ordinary television display has 480 lines. The writing period of a screen is 1.44 msec, if the writing period of one line is 3 sec, so that 1.44 msec×9≈=13 msec is needed for one field. However, the period of one field is 16.7 msec. The sustaining period is 16.7 msec minus a writing period and preliminary discharge period, and so this period is not long enough. Further, if a display has 760 lines per screen, like a high definition display, or if a display has 8 sub-fields for providing 256 gradations, the period for writing will not be sufficient.

SUMMARY OF THE INVENTION

It is an object of the present invention to improve contrast in a display.

It is another object of the present invention to improve contrast in a display by reducing a full erasing electric discharge and full writing electric discharge.

It is still another object of the invention to improve contrast in a display by reducing a preliminary discharge without changing the number of sub-fields.

According to a feature of the present invention, to achieve the above objects, a plasma display and a plasma display driving system include a first electrode group, which is arranged on a permeable substrate and in which the electrodes are capable of being driven in common, a second electrode group, which is arranged in parallel with the first electrode group on the permeable substrate and in which the electrodes are capable of being driven independently, a third electrode group, which is arranged perpendicular to the first and second electrode groups on the other substrate and in which the electrodes are capable of being driven independently, and a plasma panel, and wherein the driving system comprises means for performing at least one electric discharge for equalizing electrically charged particles in a cell in which another electrically charged particle is produced beforehand.

According to another feature of the present invention, to achieve the above objects, a plasma display, and a plasma display panel driving system and circuit include a first electrode group in which the electrodes are driven in common, a second electrode group in which the electrodes are driven independently, a third electrode group for producing an address electric discharge, means for erasing and polarizing electrically charged particles by a fine line erasing pulse after a sustaining period and for supplying an equalizing pulse to one electrode of the one of the first and second electrode groups to which the last fine line erasing pulse was supplied and for supplying a regulating pulse to an electrode of the other of the first and the second electrode groups after the equalizing pulse has been supplied, thereby controlling the electrically charged particles without fully erasing the electric discharge and fully writing an electric discharge, while improving the contrast without a light emitting discharge in the case of a black display.

According to still another feature of the present invention, to achieve the above objects, a plasma display and a plasma display panel driving system and circuit include means for forming a field block from a plurality of sub-fields and for performing a full writing electric discharge and a fine line erasing electric discharge in a first sub-field of the field block for decreasing the number of electric discharges, means for gathering positive electrically charged particles in the vicinity of an address electrode by the full writing electric discharge and fine line erasing electric discharge, thereby decreasing the voltage level of an address pulse, and means for reproducing the condition of electrically charged particles to the same condition as after performing full writing electric discharge and fine line erasing electric discharge are performed by utilizing a sustaining electric discharge in a cell in which the address electric discharge occurred, thereby reducing the voltage of a address electric discharge in the next field, without the full writing electric discharge and the fine line electric discharge. In a cell having no address electric discharge, the condition of electrically charged particles after the full writing electric discharge and fine line erasing electric discharge are performed is maintained during one field, so that it is sufficient to perform full writing electric discharge and fine line electric discharge only one time.

These and other objects, features and advantages of the present invention will become more apparent from the following description when taken in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a exploded perspective view illustrating a plasma display panel of the present invention.

FIG. 2 is a sectional view of a plasma display panel as seen in the direction of arrow A in FIG. 1 .

FIG. 3 is a sectional view of a plasma display panel as seen in the direction of arrow B in FIG. 1 .

FIG. 4 is a diagram which illustrates electrodes and circuits connected to the electrodes of the plasma display panel of FIG. 1 .

FIG. 5 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the first embodiment of the present invention.

FIG. 5 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the first embodiment of the present invention.

FIG. 5 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the first embodiment of the present invention.

FIG. 5 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the first embodiment of the present invention.

FIG. 5 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the first embodiment of the present invention.

FIG. 6 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell is illustrated immediately after power is supplied and then equalizing pulse and a protecting pulse are supplied.

FIG. 7 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after performing an address electric discharge is illustrated.

FIG. 8 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a fine line erasing pulse is illustrated.

FIG. 9 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying an equalizing pulse in a second field is illustrated.

FIG. 10 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a regulating pulse in a second field is illustrated.

FIG. 11 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 11 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the second embodiment of the present invention.

FIG. 11 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the second embodiment of the present invention.

FIG. 11 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the second embodiment of the present invention.

FIG. 11 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the second embodiment of the present invention.

FIG. 12 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 12 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the third embodiment of the present invention.

FIG. 12 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the third embodiment of the present invention.

FIG. 12 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the third embodiment of the present invention.

FIG. 12 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the third embodiment of the present invention.

FIG. 13 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the invention.

FIG. 13 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the fourth embodiment of the present invention.

FIG. 13 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the fourth embodiment of the present invention.

FIG. 13 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the fourth embodiment of the present invention.

FIG. 13 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the fourth embodiment of the present invention.

FIG. 14 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the invention.

FIG. 14 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the fifth embodiment of the present invention.

FIG. 14 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the fifth embodiment of the present invention.

FIG. 14 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the fifth embodiment of the present invention.

FIG. 14 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the fifth embodiment of the present invention.

FIG. 15 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 15 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the sixth embodiment of the present invention.

FIG. 15 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the sixth embodiment of the present invention.

FIG. 15 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the sixth embodiment of the present invention.

FIG. 15 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the sixth embodiment of the present invention.

FIG. 16 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the invention.

FIG. 16 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the seventh embodiment of the present invention.

FIG. 16 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the seventh embodiment of the present invention.

FIG. 16 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the seventh embodiment of the present invention.

FIG. 16 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the seventh embodiment of the present invention.

FIG. 17 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 17 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the eighth embodiment of the present invention.

FIG. 17 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the eighth embodiment of the present invention.

FIG. 17 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the eight embodiment of the present invention.

FIG. 17 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the eight embodiment of the present invention.

FIG. 18 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 18 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the ninth embodiment of the present invention.

FIG. 18 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the ninth embodiment of the present invention.

FIG. 18 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the ninth embodiment of the present invention.

FIG. 18 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the ninth embodiment of the present invention.

FIG. 19 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell is illustrated immediately after power is supplied and then an equalizing pulse and a regulating pulse are supplied in accordance with the ninth embodiment.

FIG. 20 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after performing an address electric discharge is illustrated in accordance with ninth embodiment of the present invention.

FIG. 21 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a fine line erasing pulse is illustrated in accordance with the ninth embodiment of the present invention.

FIG. 22 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying an equalizing pulse in a second field is illustrated in accordance with the ninth embodiment of the present invention.

FIG. 23 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a regulating pulse in a second field is illustrated in accordance with the ninth embodiment of the present invention.

FIG. 24 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 24 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the tenth embodiment of the present invention.

FIG. 24 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the tenth embodiment of the present invention.

FIG. 24 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the tenth embodiment of the present invention.

FIG. 24 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the tenth embodiment of the present invention.

FIG. 25 ( a ) is a t time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 25 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the eleventh embodiment of the present invention.

FIG. 25 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the eleventh embodiment of the present invention.

FIG. 25 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the eleventh embodiment of the present invention.

FIG. 25 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the eleventh embodiment of the present invention.

FIG. 26 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 26 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the twelfth embodiment of the present invention.

FIG. 26 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the twelfth embodiment of the present invention.

FIG. 26 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the twelfth embodiment of the present invention.

FIG. 26 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the twelfth embodiment of the present invention.

FIG. 27 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention.

FIG. 27 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the thirteenth embodiment of the present invention.

FIG. 27 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the thirteenth embodiment of the present invention.

FIG. 27 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the thirteenth embodiment of the present invention.

FIG. 27 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the thirteenth embodiment of the present invention.

FIG. 28 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with a second embodiment of the present invention.

FIG. 28 ( b ) is a waveform diagram which illustrates a driving wave-form supplied to a common X electrode in accordance with the fourteenth embodiment of the present invention.

FIG. 28 ( c ) is a waveform diagram which illustrates a driving wave-form supplied to an address A electrode in accordance with the fourteenth embodiment of the present invention.

FIG. 28 ( d ) is a waveform diagram which illustrates a driving wave-form supplied to a first independent Y electrode in accordance with the fourteenth embodiment of the present invention.

FIG. 28 ( e ) is a waveform diagram which illustrates a driving wave-form supplied to a second independent Y electrode in accordance with the fourteenth embodiment of the present invention.

FIG. 28 ( f ) is a waveform diagram which illustrates a driving wave-form supplied to a third independent Y electrode in accordance with the fourteenth embodiment of the present invention.

FIG. 28 ( g ) is a waveform diagram which illustrates a driving wave-form supplied to a fourth independent Y electrode in accordance with the fourteenth embodiment of the present invention.

FIG. 29 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying sustaining pulses is illustrated in accordance with a embodiment shown in FIGS. 28 ( a )- 28 ( g ) of the present invention.

FIG. 30 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell during discharging by a selection electric discharge pulse is illustrated in accordance with the embodiment shown in FIGS. 28 ( a )- 28 ( g ) of the present invention.

FIG. 31 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell during the supplying of an electrically charged particle control pulse is illustrated in accordance with the embodiment shown in FIGS. 28 ( a )- 28 ( g ) of the present invention.

FIG. 32 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a fine line erasing pulse is illustrated in accordance with the embodiment shown in FIG. 28 ( a )-FIG. 28 ( g ) of the present invention.

FIG. 33 is a time chart of sub-fields illustrating a driving method in accordance with the fifteenth embodiment of the present invention.

FIG. 34 is a time chart of sub-fields illustrating a driving method in accordance with the sixteenth embodiment of the present invention.

FIG. 35 is a time chart of sub-fields illustrating a driving method in accordance with the seventeenth embodiment of the present invention.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The preferred embodiments of the present invention will be described with reference to the drawings hereinafter.

FIG. 1 illustrates an exploded perspective view of a plasma display panel relating to the first embodiment of the present invention.

A transparent common X electrode 22 and a transparent independent Y electrode 23 are provided under a front glass substrate 21 , and a X bus electrode 24 and a Y bus electrode 25 are laminated on the electrodes 21 and 22 , respectively. A dielectric layer 26 and a protecting layer 27 , such as acid magnesium (MgO), are provided on these electrodes 22 , 23 , 24 and 25 . An address A electrode 29 provided on a back glass substrate 28 is arranged perpendicular to the common X electrode 22 and the independent Y electrode 23 on the front glass substrate 21 . The address A electrode 29 is covered by a dielectric layer 30 , and a partition wall 31 arranged parallel to the address A electrode 29 is provided on the electrode 29 . A phosphor 32 is coated on the partition wall 31 and the address A electrode 29 .

FIG. 2 is a sectional view of a plasma display panel as seen in the direction of arrow A in FIG. 1 . The address A electrode 29 is centered with respect to the two partition walls. A discharge gas, such as a neon gas or a xenon gas, is filled in a space 33 that is provided between the front glass substrate 21 and the back glass substrate 38 .

FIG. 3 is a sectional view of a plasma display panel as seen in the direction of arrow B in FIG. 1. A border of each cell is shown by a dotted line, and the common X electrode 22 and the independent Y electrode 23 are arranged alternatively.

In an AC type plasma display panel, the electrically charged particles on the dielectric layer in the vicinity of the common X electrode 22 and the independent Y electrode 23 are divided into positive electrically charged particles and negative electrically charged particles for forming an electric field, so that a discharge is generated by means of an electric field.

FIG. 4 illustrates electrodes and circuits connected to the electrodes of the plasma display panel of FIG. 1 . The common X electrode 22 is connected to an output terminal or several terminals of a X electrode driving circuit 35 that generates a driving pulse for supplying a voltage to the common X electrode 22 . Each independent Y electrode 23 is connected to respective output terminals of a Y electrode driving circuit 36 . Each address A electrode 29 is connected to respective output terminals of an A electrode driving circuit 37 .

FIGS. 5 ( a ) to 5 ( e ) illustrate a first driving system in accordance with a first embodiment of the present invention. FIG. 5 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the invention, wherein reference numeral 1 denotes one field, the horizontal axis illustrates time and the vertical axis illustrates a line of the cell. The one field is divided into eight sub-fields, that is, a first sub-field 2 to an eighth sub-field 9 . An electrically charged particle equalizing period 2 a - 9 a , an address period 2 b - 9 b and a sustaining period 2 c - 9 c are arranged in order in each sub-field. Numbers of electric discharges are allotted for each sub-field, and display on gradations are determined by the total numbers of the discharges. The order for arranging the sub-fields having predetermined numbers of discharges is free, but in the embodiment, the sub-fields are arranged in order from a sub-field having a fewer number of electric discharges.

FIGS. 5 ( b )-FIG. 5 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and the second independent Y electrodes, respectively. A pulse waveform 10 illustrates a part of the driving wave-form supplied to the common X electrode 22 in one field. A pulse wave-form 11 illustrates a part of the driving wave-form supplied to the one of the address A electrodes 29 .

Pulse wave-forms 12 and 13 illustrate parts of a driving wave-form supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 10 , which is supplied to the common X electrode 22 during a first sub-field includes a regulating pulse 40 lasting from a first part of the electrically charged particle equalizing period 2 a through the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c . In this embodiment, the voltage of the regulating pulse 40 is lower than the voltage of the sustaining pulses 41 . The pulse wave-form 11 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b , which address pulse 42 corresponds to the cell which is to emit light. The address pulse 42 is not supplied when there is no cell to be illuminated. That is, the address pulses 42 are supplied to the cells to be illuminated, and the address pulse 42 is not supplied to the other cells which are not to be illuminated. The pulse wave-forms 12 and 13 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes electrically charged particle equalizing pulses 43 a , 43 b , - - - in the electrically charged particle equalizing period 2 a of the first sub-field, scan pulses 44 a , 44 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c . In the embodiment, the voltage of the scan pulses 44 a , 44 b , - - - is lower than the voltage of the sustaining pulses 45 a , 45 b , - - - . The fine line erasing pulses 46 a , 46 b , - - - and the equalizing pulses 43 a , 43 b , - - - are supplied to the same electrodes. Further, it is preferable to select the pulse width of the fine line erasing pulses 46 a , 46 b , - - - between 0.5 μsec-2 μsec.

The actions in the panel will be explained hereinafter.

In this embodiment, electric discharges in all cells are performed between the independent Y electrodes 23 and the common X electrodes 22 by supplying the equalizing pulses 43 a , 43 b , - - - to the independent Y electrodes 23 , whereby negative electrically charged particles are formed on the dielectric layer 26 in the vicinity of the independent Y electrode 23 during the equalizing period 2 a occurring immediately after the power is supplied to the display. The electric discharge generated by the equalizing pulses 43 a , 43 b , - - - occurs only one time, and the discharge is not generated after this. That is, the discharge occurs only one time other than when the space 33 of the cell becomes in an abnormal condition. The regulating pulse 40 is supplied to the common X electrode 22 within the time between 0.3 μsec-2 μsec from the rising edge of the equalizing pulses 43 a , 43 b , - - - . The negative electrically charged particles are formed in the vicinity of the common X electrode 22 , and the positive electrically charged particles are formed in the vicinity of the address A electrode 29 .

The reason the time between the rising edge of the equalizing pulses 43 a , 43 b , - - - and the rising edge of the regulating pulse 40 is determined as described the above is that too many negative electrically charged particles are gathered in the vicinity of the independent Y electrode 23 and the negative electrically charged particles gather at the common X electrode 22 when the time between edges of both pulses 43 a , 43 b , - - - and 40 is selected to be too long. When the time is too short, on the other hand, the negative electrically charged particles are not gathered on the independent Y electrode 23 and also the positive electrically charged particles are not gathered on the address A electrode 22 .

The main purpose for supplying the regulating pulse 40 is to attract the negative electrically charged particles toward the common X electrode 22 and to form positive electrically charged particles on the address A electrode 29 . Another purpose is to assist the electric discharges between the common X electrode 22 and the independent Y electrode 23 when the address electric discharge is performed between the address A electrode 29 and the independent Y electrode 23 .

An address electric discharge is performed in the cell which is formed at the cross point of the first line of the independent Y electrode 23 and one of the address A electrodes 22 when the scan pulse 44 a is supplied to the first line of the independent Y electrode 23 and the address pulse 42 is supplied to one of the address A electrodes 29 at the same time, with the result that the positive electrically charged particles are gathered on the independent Y electrode 23 . On the other hand, no discharge occurs when the address pulse 42 , which corresponds to the scan pulse 44 b , is not supplied to the second line of the independent Y electrode 23 ; therefore, no electrically charged particle is gathered on the independent Y electrode 23 . The address pulses 42 are supplied to the address A electrodes 29 which correspond to the cell to be illuminated, and select all the cells at the cross points of all address A electrodes 29 , and the scan pulses 44 a or 44 b are supplied to the independent Y electrodes 23 , so that the electric discharges are performed between the address A electrode 29 and the independent Y electrodes 23 .

Next, in the sustaining period 2 c , the electric discharges for emitting light are performed by the sustaining pulses 41 , 45 a , 45 b , - - - between the common X electrode 22 and the independent Y electrodes 23 in the cell in which the positive electrically charged particles are gathered on the independent Y electrodes 23 side by the electric discharges performed during the address period 2 b . After that, electric discharges occur between the independent Y electrodes 23 and the common X electrode 22 by supplying the fine line erasing pulses 46 a , 46 b , - - - to the independent Y electrodes 23 , whereby the electrically charged particles in the cells are erased, so that all electrically charged particles generated for emitting light in the cell are erased. The pulse width of the fine line erasing pulses 46 a , 46 b , - - - is a little longer than the electric discharge duration time, therefore, the negative electrically charged particles are gathered on the dielectric layer in the vicinity of the independent Y electrodes 23 . In the cells in which no electric discharge has occurred, the erasing discharges are not performed because no electrically charged particle is in the cell. Therefore, the negative electrically charged particles formed in the vicinity of the independent Y electrodes 23 are kept unchanged.

In this situation, no electric discharge occurs when supplying the equalizing pulses 43 a , 43 b , - - - to the independent Y electrodes 23 because the negative electrically charged particles in the cell negate the voltage of the equalizing pulses 43 a , 43 b , - - - and sufficient electric fields needed for the electric discharge are not formed. After that, no electric discharge is performed through all sub-fields even if the equalizing pulses are supplied. Therefore, the electric discharges are not performed, except for the first sub-field immediately after the power is turned on, therefore no light emitting occurs in the black display.

Further, for the linearity of display gradations determined by the numbers of sustaining pulses, one electric discharge will have less influence than two electric discharges. According to the present invention, the equalization of electrically charged particles is effected by one electric discharge in the cell in which the sustaining electric discharge is performed, therefore, the influence on the linearity for display gradations is very small.

The same driving method is performed during the second sub-field 3 to the eighth sub-field 9 , and so a screen of one field is formed.

FIG. 6 - FIG. 10 are sectional views of the plasma display panel in which the condition of the electrically charged particles in the cell during a sustaining electric discharge are illustrated from the first sub-field after the power is supplied to the second sub-field until the equalizing pulses and the regulating pulse are supplied. In these figures, reference numeral 60 denotes a positive electrically charged particles, and reference numeral 61 denotes negative electrically charged particles. Further the condition of electrically charged particles is illustrated in a cell at a center position in FIG. 6 -FIG. 10 .

FIG. 6 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell is illustrated immediately after power is supplied and then an equalizing pulse and a regulating pulse are supplied. The figure illustrates the condition of electrically charged particles in the first sub-field after power is supplied at first and then the equalizing pulses 43 a , 43 b are supplied to the independent Y electrodes 23 and finally the regulating pulse 40 is supplied. The electric discharges in all cells occur between the common X electrode 22 and the independent Y electrodes 23 by supplying the equalizing pulses 43 a , 43 b , - - - to the independent Y electrodes 23 , whereby the negative electrically charged particles 61 are gathered on the dielectric layer in the vicinity of the independent Y electrodes 23 a and the common X electrode 22 and the positive electrically charged particles 60 are gathered on the address A electrodes 29 side.

FIG. 7 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after performing an address electric discharge is illustrated. In FIG. 7 , the condition of electric discharges is illustrated after the address pulse 42 is supplied to the address A electrode 29 and address electric discharges occur between the address A electrode 29 and the independent Y electrodes 23 . The positive electrically charged particles 60 are gathered on the dielectric layer in the vicinity of the independent Y electrode 23 because the voltage of the independent Y electrode 23 is lower than the voltages of the address A electrode 29 and the common X electrode 22 . The condition of the electrically charged particles is shown in FIG. 7 . The electric discharge occurs between the independent Y electrode 23 and the common X electrode 22 by the positive electrically charged particles 60 and the first pulse of the sustaining pulses 45 a , 45 b , - - - supplied to the independent Y electrode 23 . This is a sustain discharge. This time, the negative electrically charged particles 61 are gathered around the independent Y electrode 23 and the positive charges 60 are gathered around the common X electrode 22 by the electric discharge generated by the sustaining pulses 45 a , 45 b . As a result, sustaining electric discharges occur between the independent Y electrode 23 and the common X electrode 22 by the first pulse of sustaining pulses 41 . These electric discharges are repeated during the sustaining period 2 c.

FIG. 8 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a fine erase pulse is illustrated. In FIG. 8 , the condition of the electric discharge after the last sustaining pulses 41 is supplied to the common X electrode 22 and then the fine line erasing pulses 46 a , 46 b , - - - are supplied is illustrated.

The condition of the electrically charged particles after the discharges have occurred due to the final sustaining pulses 41 is the same as the condition shown in FIG. 7 .

The pulse width of the fine line erasing pulses 46 a , 46 b , - - - is longer than the discharge duration time, so that negative electrically charged particles 61 which move so quickly are gathered on the dielectric layer in the vicinity of the independent Y electrode 23 . As a result, separation of the electrically charged particles is performed. The positive electrically charged particles that move slowly in space float in the cell. The negative charges float in the discharge space for a while.

FIG. 9 is a sectional view of a plasma display panel in which a condition of the electrically charged particles in a cell after supplying an equalizing pulse in a second field is illustrated. In FIG. 9 , a condition of the electric discharge after the equalizing pulses 43 a , 43 b , - - - in the second sub-field are supplied is illustrated. The voltage of the equalizing pulses 43 a , 43 b , - - - is canceled by the negative charges and does not reach the discharge voltage, so that no discharge is performed. The voltage of the independent Y electrode 23 is higher than the voltage of the other electrodes, so the negative charges are attracted toward the independent Y electrode 23 .

FIG. 10 is a sectional view of a plasma display panel in which a condition of the electrically charged particles in a cell after supplying a regulating pulse in a second field is illustrated.

Referring to the drawing, the condition of the electrically charged particles after the regulating pulse 40 is supplied to the common X electrode 22 is illustrated. The negative electrically charged particles are gathered on the dielectric layer in the vicinity of the common X electrode 22 and the positive charges are gathered at the address A electrode 29 . By this, the same driving as the first sub-field is performed without electric discharge by the equalizing pulses 43 a , 43 b , - - - . In this case, the voltage of the equalizing pulses 43 a , 43 b , - - - is reduced by the negative electrically charged particles at the independent Y electrode 23 , so that an electric discharge between the independent Y electrode 23 and the common X electrode 22 is not performed.

The driving of the panel is capable of being performed without using the full writing electric discharge and fine line erasing electric discharge for each sub-field. As a result, unnecessary light emitting is erased for displaying a black brightness, so that the contrast is improved.

A second embodiment of the present invention will be described hereinafter. FIGS. 11 ( a ) to 11 ( e ) illustrate a driving method in accordance with a second embodiment of the present invention. FIG. 11 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis shows time and the vertical axis shows lines of cells.

FIG. 11 ( b )-FIG. 11 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 70 illustrates a part of the driving wave-form supplied to the common X electrode 22 in one field. A pulse wave-form 71 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 72 and 73 illustrate parts of a driving wave-form supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 70 , which is supplied to the common X electrode 22 during the first sub-field, includes a regulating pulse 40 lasting from a first part the electrically charged particle equalizing period 2 a through the address period 2 b and the sustaining pulses 41 and a fine line erasing pulse 74 in the sustaining period 2 c . The pulse waveform 71 which is supplied to one of the address A electrodes 29 illustrates the address pulse 42 in the address period 2 b which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse waveforms 71 and 72 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes an electrically charged particle equalizing pulse 43 a 43 b , - - - in the equalizing period 2 a of the first sub-field, scan pulses 44 a , 44 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and first fine line erasing pulses 75 a , 75 b , - - - in the sustaining period 2 c.

Under these circumstances, the pulse width of the first fine line erasing pulses 75 a , 75 b , - - - is the same as or shorter than the pulse width of the second fine line erasing pulse 74 . The number of the fine line erasing pulses is an even number as shown in FIG. 11 ( c ), that is, the first and the second fine line erasing pulses 75 a , 75 b and 74 , the first fine line erasing pulses 75 a , 75 b , - - - which are the last erasing pulses, and the equalizing pulses 43 a , 43 b , - - - are supplied to the same electrodes, that is, the independent Y electrode 23 . The second fine line erasing pulse 74 is supplied to the other electrode, that is, the common X electrode 22 .

In the embodiment, the last sustaining pulse is supplied to the independent Y electrode 23 . A condition of electrically charged particles after supplying the first fine line erasing pulses 75 a , 75 b , - - - is almost the same as the condition shown in FIG. 8 in accordance with the first embodiment. The condition of the electric discharges in the other sub-fields 3 - 9 are the same condition. Further, the erasing and polarizing of the electrically charged particles are performed by these fine line erasing pulses, so that these erasing pulses may be designated as a polarization pulse group. In this embodiment, by using the first and the second fine line erasing pulses 75 a , 75 b and 74 , the erasing and polarization are effectively performed, and the electric discharging time during the address discharging time is maintained constant.

A third embodiment of the present invention will be described hereinafter. FIGS. 12 ( a ) to 12 ( e ) illustrate a driving method in accordance with the third embodiment of the present invention. FIG. 12 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells.

FIG. 12 ( b )-FIG. 12 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and the second independent Y electrodes, respectively.

A pulse wave-form 80 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 81 illustrates a part of the driving wave-form supplied to the one of the address A electrodes 29 . Pulse wave-forms 82 and 83 illustrate parts of the driving wave-forms supplied, for example to first and second independent Y electrodes 23 .

The pulse wave-form 80 , which is supplied to the common X electrode 22 during the first sub-field, includes a regulating pulse 40 lasting from a first part of the electrically charged particle equalizing period 2 a through the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c and second fine line erasing pulse 84 . The pulse wave-form 81 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 82 and 83 which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 includes electrically charged particle equalizing pulses 43 a 43 b , - - - in the equalizing period 2 a of the first sub-field, scan pulses 44 a , 44 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and third fine line erasing pulses 85 a , 85 b , - - - and first fine line erasing pulses 86 a , 86 b , - - - in the sustaining period 2 c .

Under these circumstances, the pulse width of the second fine line erasing pulses 84 is the same as or shorter than the pulse width of a third fine line erasing pulses 85 a , 85 b , - - - . The pulse width of the first fine line erasing pulses 86 a , 86 b , - - - is also the same as or shorter than the pulse width of the second fine line erasing pulse 84 .

If the numbers of the fine line erasing pulses are an odd number, as shown in FIG. 12 ( d ), that is, the first to the third fine line erasing pulses, the first fine line erasing pulses 86 a , 86 b , - - - which are the last supplied erasing pulses and the equalizing pulses 43 a , 43 b , - - - are supplied to the same electrodes, that is, the independent Y electrode 23 . The third fine line erasing pulse 85 , which is first supplied fine line erasing pulse, is supplied to the same electrode to which the first supplied fine line erasing pulses 86 a and 86 b are supplied, that is, the independent Y electrode 23 . Therefore, the last sustaining pulse is supplied to the common X electrode 22 . A condition of the electrically charged particles after supplying the first fine line erasing pulses 86 a , 86 b , - - - is almost the same condition as shown in FIG. 8 in accordance with the first embodiment. The condition of the electric discharges in the other sub-fields 3 - 9 is the same condition. In this embodiment, by using the first, the second and the third fine line erasing pulses 86 a , 86 b , 84 , 85 a and 85 b , the erasing and polarization are more effectively performed, and the electric discharging time during address discharging time is maintained constant. According to an experiment performed by the present inventors, it was found that it is effective for erasing to use up to three fine line erasing pulses, but using more than four fine line erasing pulses is not so effective.

A fourth embodiment of the present invention will be described hereinafter. FIGS. 13 ( a ) to 13 ( e ) illustrate a driving method in accordance with a fourth embodiment of the present invention. FIG. 13 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells.

FIG. 13 ( b )-FIG. 13 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 90 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 91 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 92 and 93 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 90 , which is supplied to the common X electrode 22 during the first sub-field, includes a regulating pulse 94 lasting from a first part of the electrically charged particle equalizing period 2 a to the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c.

The voltage of the regulating pulse 94 and the voltage of the sustaining pulses 41 are the same, and thereby the driving circuit is simplified because the same power is used. The pulse wave-form 91 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be emitted. The pulse wave-forms 92 and 93 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes electrically charged particle equalizing pulses 43 a 43 b , - - - in the electric charge particle equalizing period 2 a of the first sub-field, scan pulses 44 a , 44 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c . A condition of electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition. In this embodiment, the voltage of the regulating pulse 94 supplied to the common X electrode 22 and the voltage of the sustaining pulses are the same, therefore simplifying the driving circuit construction.

A fifth embodiment of the present invention will be described hereinafter. FIGS. 14 ( a ) to 14 ( e ) illustrate a driving method in accordance with the fifth embodiment of the present invention. FIG. 14 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 14 ( b )-FIG. 14 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 100 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 101 illustrates a part of the driving wave-form supplied to the one of the address A electrodes 29 . Pulse wave-forms 102 and 103 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 100 , which is supplied to the common X electrode 22 during the first sub-field, includes a regulating pulse 94 lasting from a first part of the electrically charged particle equalizing period 2 a through the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c . The voltage of the regulating pulse 94 and the voltage of the sustaining pulses 41 are the same as the fourth embodiment shown in FIG. 13 ( d ), thereby the driving circuit is simplified because the same power is used. The pulse wave-form 101 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 102 and 103 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes electrically charged particle equalizing pulses 43 a 43 b , - - - in the equalizing period 2 a of the first sub-field, scan pulses 104 a , 104 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c . The voltage of the independent Y electrode 23 during the address period 2 c and the voltage of the sustaining pulses 45 a , 45 b , - - - are the same, thereby the driving circuit is simplified because the same power is used. A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of the electrically charged particles in accordance with the first embodiment. The condition of the electrically charged particles in the other sub-fields 3 - 9 is the same condition.

A sixth embodiment of the present invention will be described hereinafter. FIGS. 15 ( a ) to 15 ( e ) illustrate a driving method in accordance with a sixth embodiment of the present invention. FIG. 15 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and vertical axis illustrates a line of cells. FIG. 15 ( b )-FIG. 15 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and first and second independent Y electrodes, respectively.

A pulse wave-form 110 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 111 illustrates a part of the driving wave-form supplied to the one of the address A electrodes 29 . Pulse wave-forms 112 and 113 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 110 , which is supplied to the common X electrode 22 during the first sub-field, includes a first regulating pulse 114 in the electrically charged particle equalizing period 2 a , a second regulating pulse 115 in the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c . In this embodiment, the regulating pulse supplied to the common X electrode 22 is divided into a first regulating pulse 114 in the equalizing period 2 a and a second regulation pulse 115 in the address period 2 b . The pulse wave-form 111 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 112 and 113 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes electrically charged particle equalizing pulses 43 a 43 b , - - - in the equalizing period 2 a of the first sub-field, scan pulses 116 a , 116 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c . A condition of electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition. As seen FIGS. 15 ( b ) and 15 ( d ), the rising edge of the first regulating pulse slightly later than that of the equalizing pulse 43 a , thereby preventing electric discharging by mistake between the common X electrode 22 and the independent Y electrode. Further, a rising edge of the second regulating pulse 115 and a rising edge of the scan pulses 116 a , 116 b is effected at the same time, thereby preventing electric discharge by mistake between the common X electrode 22 and the independent Y electrode 23 .

The first regulating pulse 114 supplied to the common X electrode 22 and the sustaining pulses 41 may use the same voltage.

A seventh embodiment of the present invention will be described hereinafter. FIGS. 16 ( a ) to 16 ( e ) illustrate a driving method in accordance with a seventh embodiment of the present invention. FIG. 16 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 16 ( b )-FIG. 16 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrode, respectively.

A pulse wave-form 130 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 131 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 132 and 133 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 130 , which is supplied to the common X electrode 22 during the first sub-field, includes a first regulating pulse 134 in the electrically charged particle equalizing period 2 a , a second regulating pulse 135 in the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c . The pulse wave-form 131 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b of the first sub-field which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 132 and 133 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes electrically charged particle equalizing pulses 136 a , 136 b , - - - in the equalizing period 2 a of the first sub-field, scan pulses 137 a , 137 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c .

A falling edge of the equalizing pulse 136 a , 136 b , - - - becomes zero voltage within a time less than 1 μs in accordance with the present embodiment, which is different from the above mentioned embodiment. As the voltage of the second regulating pulse 135 and the scan pulses 137 a , 137 b , the same voltage as the sustaining pulses 41 , 45 a , 45 b , - - - is employed. A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition.

In this embodiment, the edge of the first regulating pulse 134 rises after the edge of the equalizing pulse rises, as shown in FIG. 16 ( d ), thereby preventing electric discharge by mistake between the common X electrode 22 and the independent Y electrode.

An eighth embodiment of the present invention will be described hereinafter. FIGS. 17 ( a ) to 17 ( e ) illustrate a driving method in accordance with an eighth embodiment of the present invention. FIG. 17 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 17 ( b )-FIG. 17 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 140 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 141 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 142 and 143 illustrate part of the driving wave-form supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 140 , which is supplied to the common X electrode 22 during the first sub-field, includes a first regulating pulse 144 in the electrically charged particle equalizing period 2 a , a second regulating pulse 145 in the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c.

According to the present embodiment, the voltage of the first regulating pulse 144 is set higher than the voltage of the sustaining pulses 41 . The pulse wave-form 141 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b of the first sub-field which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 142 and 143 which are supplied to the first electrode of the independent electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes electrically charged particle equalizing pulses 136 a 136 b , - - - in the equalizing period 2 a of the first sub-field, scan pulses 137 a , 137 b , - - - in the address period 2 b , sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c .

The voltage of the second regulating pulse 135 and the scan pulses 137 a , 137 b , - - - can be set to the same voltage as the sustaining pulses 41 , 45 a , 45 b , - - - . A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same.

According to the present embodiment, the voltage of the first regulating pulse 144 is higher than that of the sustaining pulses 41 . By using a higher voltage for the first regulating pulse 144 , a lot of negative electrically charged particles can be collected, and as a result, a lot of positive electrically charged particles are collected on the address electrode 29 side, thereby address discharging is performed very easily.

A ninth embodiment of the present invention will be described hereinafter. FIGS. 18 ( a ) to 18 ( e ) illustrate a driving method in accordance with a ninth embodiment of the present invention. FIG. 18 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 18 ( b )-FIG. 18 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 150 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 151 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 152 and 153 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 150 , which is supplied to the common X electrode 22 during the first sub-field, includes an equalizing pulse 153 in the equalizing period 2 a , a regulating pulse 154 in the address period 2 b and the sustaining pulses 41 and a fine line erasing pulse 155 in the sustaining period 2 c.

According to the present embodiment, only one fine line erasing pulse 155 is provided. The equalizing pulse 153 is supplied to the electrode to which the fine line erasing pulse 155 is supplied, such as in the case of the fifth embodiment.

In case two or three fine line erasing pulses are provided, as shown in the second and the third embodiment (see FIGS. 11 ( b ), 11 ( d ) and FIGS. 12 ( b ), 12 ( d ), the equalizing pulses are supplied to the electrode to which the last fine line erasing 20 pulse is supplied.

The pulse wave-form 151 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b of the first sub-field which corresponds to the light emitting cell. The address pulse 42 is not supplied 25 when there is no cell to be illuminated. The pulse wave-forms 152 and 153 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , include first regulating pulses 156 a , 156 b , - - - in the electrically charged particle equalizing period 2 a of the first sub-field, scan pulses 137 a , 137 b , - - - in the address period 2 b , and sustaining pulses 45 a , 45 b , - - - in the sustaining period 2 c.

In this embodiment, the first regulating pulses 156 a , 156 b , - - - are supplied within 0.3 μsec to 2 μsec from the rising edge of the equalizing pulse 153 .

The voltage of the second regulating pulse 154 and the scan pulses 137 a , 137 b , - - - can be set to the same voltage as that of the sustaining pulses 41 , 45 a , 45 b , - - - as shown in the fifth embodiment (see FIG. 14 ( b )). A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of the electrically charged particles in accordance with the first embodiment. The condition of electric discharge in the other sub-fields 3 - 9 is the same.

According to the present embodiment, the first regulating pulses 156 a , 156 b , - - - are similar to the equalizing pulses 43 a , 43 b , - - - as shown in FIG. 15 ( d ) and FIG. 15 ( e ), but an equalizing pulse according to the present invention is a pulse that rises first during the electrically charged particle equalizing period. The reason for providing a 0.3 μsec to 2 μsec period between the rising edge of the equalizing pulse 153 and the rising edge of the first regulating pulses 156 a , 156 b , - - - has already been explained.

FIG. 19 to FIG. 23 are sectional views of the plasma display panel in accordance with the ninth embodiment in which the condition of electrically charged particles in the cell for effecting an electric discharge for light emission are illustrated from the first sub-field after the power is supplied to the second sub-field until the equalizing pulses and the regulating pulses are supplied. In these drawings, reference numeral 60 denotes a positive electrically charged particle, and reference numeral 61 denotes a negative electrically charged particle. Further, the condition of the electrically charged particles is illustrated in a cell at a center position in FIG. 19 through FIG. 23 .

FIG. 19 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell is illustrated immediately after power is supplied and then an equalizing pulse and regulating pulses are supplied. The figure illustrate the condition of electrically charged particles in a first sub-field after power is supplied at first and then the equalizing pulse 153 is supplied to the common X electrode 22 and finally the first regulating pulses 156 a , 156 b , - - - are supplied. The electric discharge occurs between the common X electrode 22 and the independent Y electrodes 23 by supplying the equalizing pulse 153 to the independent Y electrodes 23 in all cells, so that the negative electrically charged particles 61 are gathered on the dielectric layer in the vicinity of the independent Y electrodes 23 and the common X electrode 22 , and the positive electrically charged particles 60 are gathered on the address A electrode 29 side.

FIG. 20 is a sectional view of a plasma display panel in accordance with the ninth embodiment in which a condition of the electrically charged particles in a cell after performing an address electric discharge is illustrated. In FIG. 20 , the condition of the electric discharge is illustrated after the address pulse 42 is supplied to the address A electrode 29 and address electric discharges are performed between the address A electrode 29 and the independent Y electrodes 23 . The positive electrically charged particles 60 are gathered on the dielectric layer in the vicinity of the independent Y electrode 23 because the voltage of the independent Y electrode 23 is lower than the voltages of the address A electrode 29 and the common X electrode 22 . The negative electrically charged particles 61 are gathered on the other electrode side.

The condition of the electrically charged particles is shown in FIG. 20 . The sustaining electric discharge is produced between the independent Y electrode 23 and the common X electrode 22 by the positive electrically charged particles 60 and the first pulse of the sustaining pulses 45 a , 45 b , - - - supplied to the independent Y electrode 23 . This is a sustain discharge.

FIG. 21 is a sectional view of a plasma display panel in which a condition of electrically charged particles in a cell after supplying a fine line erasing pulse is illustrated. In FIG. 21 , the condition of the electric discharge after the last sustaining pulses 45 a , 45 b , - - - are supplied to the independent Y electrode and then the fine line erasing pulses 155 are supplied to the common X electrode 22 is illustrated.

The pulse width of the fine line erasing pulse 155 is longer than the discharge duration time, so that negative electrically charged particles 61 , which move so quickly, are gathered on the dielectric layer in the vicinity of the common X electrode 22 . The positive electrically charged particles that move slowly in space float in the cell. The negative charges float in the discharge space for a while.

FIG. 22 is a sectional view of a plasma display panel in accordance with the ninth embodiment in which a condition of electrically charged particles in a cell after supplying an equalizing pulse in a second sub-field is illustrated. FIG. 22 illustrates a condition of the electric discharge after the equalizing pulse 153 in the second sub-field is supplied. The voltage of the equalizing pulse 153 is canceled by the negative charged particles 61 and does not reach the discharge voltage, so that no electric discharge occurs.

FIG. 23 is a sectional view of a plasma display panel in which a condition of electric charges in a cell after supplying a regulating pulse in a second sub-field is illustrated. In the figure, the condition of electrically charged particles after the first regulating pulses 156 a , 156 b , - - - are supplied to the independent Y electrodes 23 is illustrated. The negative electrically charged particles 61 are gathered on the dielectric layer in the vicinity of the common X electrode 22 and the independent Y electrodes 23 , and the positive electrically charged particles 60 are gathered on the address A electrode 29 side. By this, the same driving as the first sub-field is performed without electric discharge by the equalizing pulses 153 .

A tenth embodiment of the present invention will be described hereinafter. FIGS. 24 ( a ) to 24 ( e ) illustrate a driving method in accordance with a tenth embodiment of the present invention. FIG. 24 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 18 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 24 ( b )-FIG. 24 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 160 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 161 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 162 and 163 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 160 , which is supplied to the common X electrode 22 during the first sub-field, includes an equalizing pulse 164 in the equalizing period 2 a , a regulating pulse 165 , which continues from the equalizing pulse 164 in the equalizing period 2 a and continues through the address period 2 b , and the sustaining pulses 41 and a fine line erasing pulse 155 in the sustaining period 2 c.

According to the present embodiment, only one fine line erasing pulse is provided. The equalizing pulse 164 is supplied to the electrode to which the fine line erasing pulse 155 is supplied as in the first embodiment. In case two or three fine line erasing pulses are provided, as in the second embodiment and the third embodiment (see FIGS. 11 ( b ), 11 ( d ) and FIGS. 12 ( b ), 12 ( d )), the equalizing pulse is supplied to the electrode to which the last fine line erasing pulse is supplied. The pulse wave-form 161 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b of the first sub-field which corresponds to the light emitting cell. The address pulses 42 are not supplied when there is no cell to be illuminated. The pulse wave-forms 162 and 163 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , includes first regulating pulses 156 a , 156 b , - - - in the electrically charged particle equalizing period 2 a of the first sub-field, scan pulses 137 a , 137 b , - - - in the address period 2 b , and sustaining pulses 45 a , 45 b , - - - in the sustaining period 2 c . In this embodiment, the first regulating pulses 156 a , 156 b , - - - are supplied within 0.3 μsec to 2 μsec from the rising edge of the equalizing pulse 164 . The voltage of the regulating pulse 165 and the scan pulses 137 a , 137 b , - - - can be set to the same voltage as the sustaining pulses 41 , 45 a , 45 b , - - - as shown in the ninth embodiment (see FIG. 18 ( b )). The other sub-fields 3 - 9 are constructed the same as the first sub-field.

A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition.

According to the present embodiment, the reason for setting the voltage of the equalizing pulse 164 at a higher voltage is to collect the negative electrically charged particles on the common X electrode side, and to collect lots of positive electrically charged particles on the address A electrode 29 side. Further, the reason for setting the voltage of the regulating pulse 165 in the address period 2 b is to protect an electric discharge from taking place by mistake between the common X electrode 22 and the independent Y electrode 23 .

An eleventh embodiment of the present invention will be described hereinafter. FIGS. 25 ( a ) to 25 ( d ) illustrate a driving system in accordance with an eleventh embodiment of the present invention. FIG. 25 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates line of cells. FIG. 25 ( b )-FIG. 25 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 170 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 171 illustrates a part of the driving wave-form supplied to the one of the address A electrodes 29 . Pulse wave-forms 172 and 173 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 170 , which is supplied to the common X electrode 22 during the first sub-field, includes a regulating pulse 40 in the period continuing from the first part of the equalizing period 2 a through the address period 2 b and the sustaining pulses 41 in the sustaining period 2 c . The pulse wave-form 171 , which is supplied to one of the address A electrodes 29 , includes a voltage holding pulse 174 whose voltage is determined so that a discharge is not produced by the scan pulses 44 a , 44 b , - - - and the address pulse 42 in the first address period 2 b which corresponds to the light emitting cell and between the address electrode 29 and the independent Y electrode 23 . The address pulse 42 is not supplied when there is no cell to be illuminated. According to the present embodiment, the voltage needed for the address electric discharging to occur is the sum of the voltage of the voltage holding pulse 174 and the voltage of the address pulse 175 , thereby making it possible to reduce the voltage of the address pulse 175 . The address pulse 175 is not supplied when there is no cell to be illuminated. The pulse wave-forms 172 and 173 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , include equalizing pulses 43 a , 43 b , - - - in the electrically charged particle equalizing period 2 a of the first sub-field, scan pulses 44 a , 44 b , - - - in the address period 2 b , and sustaining pulses 45 a , 45 b , - - - in the sustaining period 2 c . The voltage of the regulating pulse 40 and the scan pulses 44 a , 44 b , - - - can be determined to be the same voltage as sustaining pulses 41 , 45 a , 45 b , - - - .

A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition.

A twelfth embodiment of the present invention will be described hereinafter. FIGS. 26 ( a ) to 26 ( e ) illustrate a driving method in accordance with a twelfth embodiment of the present invention. FIG. 26 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 5 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 26 ( b )-FIG. 26 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 180 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 181 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 182 and 183 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The pulse wave-form 180 , which is supplied to the common X electrode 22 during the first sub-field includes a regulating pulse 184 in the equalizing period 2 a and sustaining pulses 41 in the sustaining period 2 c . The pulse wave-form 181 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b of the first address period which corresponds to the light emitting cell. The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 182 and 183 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , include equalizing pulses 43 a , 43 b , - - - in the electric charging equalizing period 2 a of the first sub-field, sustaining pulses 185 a , 185 b , - - - in the address period 2 b , and sustaining pulses 45 a , 45 b , - - - and fine line erasing pulses 46 a , 46 b , - - - in the sustaining period 2 c . The voltage level of the regulating pulse 184 can be the same as the voltage of the sustaining pulses 41 .

A condition of the electrically charged particles after supplying the fine line erasing pulses 46 a , 46 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition. According to the present embodiment, the voltage of the scan pulses 185 a , 185 b , - - - is a minus voltage and the voltage of the address pulses 42 is a plus voltage, therefore the voltage differences become so large that the electric discharge is performed surely.

A thirteenth embodiment of the present invention will be described hereinafter. FIGS. 27 ( a ) to 27 ( e ) illustrate a driving method in accordance with a thirteenth embodiment of the present invention. FIG. 27 ( a ) is a time chart illustrating an arrangement of sub-fields in one field in accordance with the present invention. The figure illustrates a division of one field into several sub-fields, similar to the case of FIG. 18 ( a ). The horizontal axis illustrates time and the vertical axis illustrates a line of cells. FIG. 27 ( b )-FIG. 27 ( e ) illustrate wave-forms of pulses supplied to the common X electrode, the address A electrode, and the first and second independent Y electrodes, respectively.

A pulse wave-form 190 illustrates a part of the driving wave-form supplied to the common X electrode 22 in the first sub-field. A pulse wave-form 191 illustrates a part of the driving wave-form supplied to one of the address A electrodes 29 . Pulse wave-forms 192 and 193 illustrate parts of the driving wave-forms supplied, for example, to first and second independent Y electrodes 23 .

The wave-form 190 , which is supplied to the common X electrode 22 during the eighth sub-field, and the field blank period 9 d thereafter includes a regulating pulse 40 from the first part of the electric charge particle equalizing period 2 a through the address period 2 b , sustaining pulses 41 and a full writing pulse 194 in the sustaining period 2 c . In this embodiment, the voltage of the full writing pulse 194 is high enough to produce a discharge regardless of whether a sustaining discharge occurs or not. As a result, the electrically charged particles in all cells are equalized. The field blank period 9 d can be provided between the sub-fields. And also, the field blank period 9 d can be provided several times in one field. The pulse waveform 191 , which is supplied to one of the address A electrodes 29 , includes the address pulse 42 in the address period 2 b . The address pulse 42 is not supplied when there is no cell to be illuminated. The pulse wave-forms 192 and 193 , which are supplied to the first electrode of the independent Y electrodes 23 and adjacent second electrode of the independent Y electrodes 23 , include the equalizing pulses 43 a , 43 b , - - - in the electric charging equalizing period 2 a , the scan pulses 44 a , 44 b , - - - in the address period 2 b , the sustaining pulses 45 a , 45 b , - - - in the sustaining period 2 c , and fine line erasing pulses 195 a , 195 b , - - - in the field blank period 9 d . The voltage level of the regulating pulse 40 and the scan pulses 44 a , 44 b , - - - can be the same as the voltage of the sustaining pulses 41 . A condition of the electrically charged particles after supplying the fine line erasing pulses 195 a , 195 b , - - - is almost the same condition as shown in FIG. 8 , which illustrates the condition of electrically charged particles in accordance with the first embodiment. The condition of the electric discharge in the other sub-fields 3 - 9 is the same condition.

According to the present embodiment, no electrically charged particle remain in the cells when a black portion continues across several sub-fields, and so the address electric discharges are not performed well in the coming address period. To prevent this situation, discharges are forced by the field full writing pulse 194 between the common X electrode 22 and the independent Y electrode 23 .

As explained above, the plasma display driving system in accordance with the first through the twelfth embodiments can drive the panel without using the full writing electric discharge and erasing discharge for all the cells for equalizing the electrically charged particles.

Still other embodiments of the present invention will be explained hereinafter.

FIGS. 28 ( a ) to 28 ( g ) illustrate a driving method for a plasma display panel in accordance with a fourteenth embodiment of the present invention. FIG. 28 ( a ) is a time chart illustrating an arrangement of sub-fields in the first sub-field. The horizontal axis illustrates time, and the vertical axis illustrates a line of cells. FIG. 28 ( b )-FIG. 28 ( g ) are wave-forms illustrating pulse wave-forms supplied to a common X electrode, an address A electrode and four independent Y electrodes, respectively. In the figure, reference numeral 201 denotes a field, reference numerals 202 - 209 denote sub-fields, reference numerals 202 a - 209 a denote address periods, reference numerals 202 b - 209 b denote sustaining periods, reference numerals 210 - 213 denote field blocks, and reference numerals 210 a - 213 a denote full writing periods. A wave-form 220 is a driving wave-form supplied to the common X electrode. A wave-form 221 is a driving wave-form supplied to the address A electrode 29 . The wave-forms 222 - 225 are driving wave-forms supplied to first, second, third and fourth electrodes of the independent Y electrodes 23 , respectively.

In FIG. 28 ( a ), one field period 201 is divided into eight sub-fields 202 - 209 , and one field block is formed by two successive sub-fields, therefore one field period 201 is constructed of four field blocks.

In each field block, the full writing periods 210 a , 211 a , 212 a and 213 a , which are arranged as the first period of sub-fields, are provided in each first sub-field 202 , 204 , 206 and 208 of the field blocks 210 - 213 , and following the writing period 210 a - 213 a , the address periods 202 a , 204 a , 206 a and 208 a and sustaining periods 202 b , 204 b , 206 b and 208 b are provided, respectively. In the second sub-fields 203 , 205 , 207 and 209 , which follow the first sub-fields 202 - 208 , the address periods 203 a , 205 a , 207 a and 209 a are provided first, and then the sustaining periods 203 b , 205 b , 207 b and 209 b are provided, respectively.

The numbers of light emissions are allotted for each sustaining period 202 b - 209 b , and display graduations are effected by the combinations of the numbers of the light emissions. The numbers of light emissions and the order of the sub-fields are optional. In this embodiment, the numbers of light emissions of the sustaining periods 202 b , 204 b , 206 b , 208 b , 203 b , 205 b , 207 b and 209 b are arranged in this order from few numbers. The sustaining periods 202 b , 204 b , 206 b and 208 b just before the sub-fields 203 , 205 , 207 and 209 in which a full writing erase period is not provided have fewer numbers of light emissions.

FIG. 28 ( b ) illustrates the field block 210 , and the other field blocks are constructed similarly. The driving wave-form 220 supplied to the common X electrode 22 includes in the first sub-field 202 a full writing pulse 240 and a polarizing pulse 241 in the first full writing erasing period 210 a , a high pulse 242 in the succeeding address period 202 a and sustaining pulses 243 and an electrically charged particle control pulse 244 and a fine line erasing pulse 245 in the succeeding sustaining period 202 b , and further includes in the succeeding sub-field a high pulse 246 and sustaining pulses 247 .

The voltage level of the electrically charged particle control pulse 244 and the fine line erasing pulse 245 is the same as or less than the voltage level of the sustaining pulses 243 . Next to the sustaining pulses 247 is the field block 211 . The voltage of the full writing pulse 240 is stepped up a level. The voltage is usually determined to be about 300 volts, and the reason for stepping up the level thereof is to allow the circuit to be constructed simply, therefore the stepping up the voltage of the full writing pulse 240 is not always necessary.

The driving wave-form 221 supplied to the address A electrode 29 shown in FIG. 28 ( c ) includes, in the first sub-field, a plurality of the address pulses 248 a , 248 b , - - - which relates to the cells to be illuminated in the address period 202 a , and, in the succeeding sub-field 203 , a plurality of address pulses 249 a , 249 b , - - - in the address period 203 a.

FIG. 28 ( d )- 28 ( g ) show wave-forms 222 , 223 , 224 and 225 supplied to four independent Y electrodes 23 whose electrodes 23 are arranged side by side, and these waveforms include, in the first sub-field 202 , scan pulses 250 a , 250 b , 250 c , 250 d , - - - in the address period 202 a , sustaining pulses 251 a , 251 b , 251 c , 251 d , - - - , selection electric discharge pulses 252 a , 252 b , 252 c , 252 d - - - , fine line erasing pulses 253 a , 253 b , 253 c , 253 d , - - - in the sustaining period, 222 b and, in the succeeding sub-field 203 , scan pulses 254 a , 254 b , 254 c , 254 d , - - - , in the address period 203 a , and sustaining pulses 255 a , 255 b , 255 c , 255 d , - - - in the sustaining period 203 b.

The voltage level of the selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - is almost the same as the voltage level of the electrically charged particle control pulse 244 , which rises with a time lag from the rising edge of the selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - , the delay time t 1 being 0.1 μsec-1.5 μsec. The electrically charged particle control pulse 244 falls earlier than the selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - . The time t 2 is about 0.1 μsec-1.0 μsec. The reason for setting the time lag from the rising edge of the selection electric discharge pulses 252 a - 252 d to the rising edge of the electrically charged particle control pulse 244 as above mentioned is that, if the time longer than that is set, a lot of negative electrically charged particles gather on the independent Y electrode 23 side, and a few negative electrically charged particles gather on the common X electrode 22 side. Further, the reason for starting the selection electric discharge pulses 252 a - 252 d a little earlier than the electrically charged particle control pulse 244 is to produce an electric discharge by generating a selection electric discharge between the common X electrode 22 and independent Y electrode 23 . The reason for ending the electrically charged particle control pulse 244 is to defends the electric charge between the common X electrode 22 and the independent Y electrode 23 when the selection electric discharge pulses 252 a - 252 d fall.

The selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - , the fine line erasing pulses 253 a , 253 b , 253 c , 253 d , - - - and the electrically charged particle control pulse 244 are not provided in the succeeded sub-field 203 of the field block 210 of FIG. 28 ( a ).

The sustaining pulses of the sub-field 203 terminate with the sustaining pulses 255 a , 255 b , 255 c , 255 d , - - - supplied to the independent Y electrodes 23 . The same driving wave-forms are used in the other field blocks 211 - 213 , but the numbers of the sustaining pulses are different. The selection electric discharge pulses, the electrically charged particle control pulse and the fine line erasing pulses are provided in the first sub-field 204 , 206 , 208 of the field blocks 210 - 213 .

The operation of this embodiment will be explained with reference to FIG. 29 -FIG. 32 . The electric discharges occur in all the cells in response to the full writing pulse 240 supplied to the common X electrode 22 in the field block 210 of FIG. 28 ( a )-FIG. 28 ( b ), and so the electrically charged particles are formed. Under these circumstances, the negative electrically charged particles 61 are gathered on the address A electrode 29 side. The electric discharge for polarization occurs in response to the polarization pulse 241 , and electrically charged particles on the common X electrode 22 side and the independent Y electrode 23 side are polarized.

The scan pulses 250 a of the wave-form 222 are supplied to the first line of the independent Y electrode 23 , and at the same time, the address pulses 248 a are supplied to a predetermined address A electrode 29 in the succeeded address period 202 a , thereby generating a full writing electric discharge and forming electrically charged particles in the cell positioned at the cross point of the first line of the independent Y electrode 23 and the address A electrode 29 , so that positive electrically charged particles are gathered on the independent Y electrode 23 side in the cell.

In a similar way, when the scan pulses 250 c of the driving wave-form 224 are supplied to the third independent Y electrode 23 and the address pulse 248 b is supplied to a predetermined address A electrode 29 , thereby generating a full writing electric discharge and forming electrically charged particles in the cell positioned at the cross point of the third line of the independent Y electrode 23 and the address A electrode 29 , positive electrically charged particles 60 are gathered on the independent Y electrode 23 side in the cell.

The address pulses which correspond to the scan pulses 250 b , 250 d of the driving wave-form 223 , 225 supplied to the second and the fourth independent Y electrodes 23 are not supplied when the predetermined cells are not illuminated, therefore, writing electric discharges do not occur and electrically charged particles are not formed on the independent Y electrode 23 side.

The sustaining discharge or light emitting discharge in the sustaining period 202 b occurs in response to the sustaining pulses 234 of the driving wave-form 220 and the sustaining pulses 251 a , 251 b , 251 c , 251 d , - - - , of the driving wave-forms 222 , 223 , 224 , 225 in the cell in which the positive electrically charged particles are gathered on the independent Y electrode 23 side.

The optional or selecting electric discharges occur in response to the selection electric discharge pulses 252 a , 252 b , 252 c and 252 d in the cell in which a sufficient number of electrically charged particles are formed by the electric discharge for light emission. The positive electrically charged particles 60 are gathered on the address A electrode 29 side by supplying electrically charged particle control pulse 244 to the common X electrode 22 before the electric discharges by the selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - , cease.

After that, the erasing electric discharge is caused by the fine line erasing pulse 245 of the waveform 220 supplied to the common X electrode 22 and the fine line erasing pulses 253 a , 253 b , 253 c , 253 d , - - - , of the wave-form 222 supplied to the independent Y electrode 23 , so that the electrically charged particles on the common X electrode 22 side and on the independent Y electrode 23 side are mainly erased. Thereby, the condition of the electrically charged particles in all cells in which electric discharges are produced is almost the same as the condition of the electrically charged particles after the full writing erasing period 210 a is finished.

On the other hand, the writing electric discharges or the address electric discharges are not generated in the cells in which the electric discharges for light emission are not produced, and the condition of electrically charged particles is the same condition after the full writing erasing period 210 a is finished.

As explained above, the electrically charged particles in all cells at a point of time after the final erasing pulses 245 , 253 a , 253 b , 253 c , 253 d , - - - , are supplied in the first sub-field 202 can be made to have the same condition after the full writing erasing period 210 a is finished. By this, in the succeeding sub-field, address electric discharges in all of the cells can be produced without providing a full writing erasing period.

The same functions are repeated in the field blocks 211 - 213 , whereby a screen of one field is formed.

FIG. 29 - FIG. 32 are sectional views of a plasma display panel illustrating a condition of the electrically charged particles in a cell in which a sustaining discharge is performed. The condition of the electrically charged particles in the drawings is illustrated in a center cell of three cells.

FIG. 29 is a sectional view of the plasma display panel in which a condition of the electrically charged particles in a cell after supplying sustaining pulses is illustrated in accordance with the embodiment shown in FIG. 28 ( a )- 28 ( g ) of the present invention. The negative electrically charged particles 61 are gathered on the dielectric layer 26 of the common X electrode 22 side and the positive electrically charged particles 60 are gathered on the dielectric layer 26 of the independent Y electrode 23 side after a final pulse of the sustaining pulses 243 is supplied to the common X electrode 22 .

FIG. 30 is a sectional view of the plasma display panel in which a condition of the electrically charged particles in a cell during discharging by a selection electric discharge pulse is illustrated. Electric discharges are caused by the voltage of the selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - and the voltage of positive electrically charged particles gathered on the dielectric layer at the independent Y electrode 23 , and these discharges are produced 20 between the independent Y electrode 23 and the common X electrode 22 when selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - , are supplied to the independent Y electrode. Thereby, many positive and negative electrically charged-particles are generated in the discharging space.

FIG. 31 is a sectional view of the plasma display panel in which a condition of the electrically charged particles in a cell when electric charge particle control pulse is supplied is illustrated. The positive electrically charged particles are gathered on the address A electrode 29 when the electrically charged particle control pulse 244 is supplied to the common X electrode 22 , because the voltages of the common X electrode 22 and the independent Y electrode 23 are almost the same and these voltages are higher than the voltage of address A electrode 29 . Erasing of electrically charged particles by the erase pulse is still needed because there still remains electrically charged particles on the common X electrode 22 side, on the independent Y electrode 23 side and in the discharging space, which are not neutralized and not erased.

FIG. 32 is a sectional view of the plasma display panel in which a condition of the electrically charged particles in a cell after supplying a fine line erasing pulse is illustrated. The positive electrically charged particles 60 are gathered on the address A electrode 29 side and the negative electrically charged particles 61 are gathered on the common X electrode 22 side and the independent Y electrode 23 side. The condition of the electrically charged particles is the same after the full writing erase period 210 a is finished.

A condition of the electrically charged particles after the full writing erasing period 210 a is finished is maintained in the sustaining period 202 b because address electric discharges are not generated in the cells in which no sustaining electric discharge is performed. Also, no electric discharge is performed by the selection electric discharge pulses 252 a , 252 b , 252 c , 252 d , - - - , and there is no change in the condition of the electrically charged particles even if the electrically charged particle control pulse 244 and erasing pulse are supplied. Therefore, the condition of the electrically charged particles in all cells is almost same as the condition after the full writing erasing period 210 a and the address electric discharge or a writing electric discharge is produced in the next sub-field 203 , thereby increasing the contrast by double.

By increasing the voltage of the address pulses 248 a and 248 b in the sub-fields 203 , 205 , 207 , 209 in which the full writing erasing period is not carried out, compared with the voltage of the address pulses 248 a and 248 b in the other sub-fields 202 , 204 , 206 and 208 , the address electric discharges are caused surely even in a cell in which sustaining electric discharges are not performed, because the positive electrically charged particles 60 on the address A electrode 29 side are reduced gradually by neutralization.

FIG. 33 is a time chart of sub-fields illustrating a driving method in accordance with a fifteenth embodiment of the present invention. Referring to the drawing, the horizontal axis illustrates time, and the vertical axis illustrates lines of cells. Reference numeral 270 denotes one field period, 271 - 276 denote sub-fields, 271 a - 276 a denote address periods, 271 b - 276 b denote sustaining periods, 277 and 278 denote field blocks, and 277 a and 278 a denote full writing erasing periods.

One field period 270 is divided into six sub-fields 271 - 276 , and the consecutive first three sub-fields 271 - 273 form the field block 277 , while the succeeding consecutive three sub-fields 274 - 276 form the other field block 278 .

In the first period of the field blocks 277 and 278 , full writing erasing periods 277 a and 278 a are arranged, respectively. In each sub-field 271 - 276 , the address periods 271 a - 276 a and the sustaining periods 271 b - 276 b are provided, but the full writing erasing periods 277 a and 278 a are not provided. That is, the full writing erasing periods 277 a and 278 a are arranged at the first part of the first sub-fields 271 and 274 of the field blocks 277 and 278 , respectively. The numbers of light emissions are allotted for the sustaining periods 271 b - 276 b , and gradations of display are produced by combining the numbers of light emissions. According to this fifteenth embodiment, the numbers of the light emissions are increased in the order of the sub-fields 271 , 272 , 273 .

Referring to FIGS. 28 ( b ) to 28 ( g ), the selection electric discharge pulses 252 a - 252 d , the electrically charged particle control pulse 244 and fine line erasing pulses 245 , 253 a - 253 b , which are used in the fourteenth embodiment, are provided in the first two sub-fields 271 , 272 , 274 , 275 of the field blocks 277 and 278 , and these pulses are not provided in the other (last) sub-field. Further, these selection electric discharge pulses, the electrically charged particle control pulse and the fine line erasing pulses are arranged in the last part of the sustaining period 271 b , 272 b , 274 b and 275 b , thereby the condition of electrically charged particles in all cells after the sustaining periods 271 b , 272 b , 274 b and 275 b are finished is maintained in the same condition after the full writing erasing period 277 a is finished, so that the full writing erasing period 210 a can be deleted in the sub-fields 272 , 273 , 275 and 276 , although it is provided in the first sub-fields 271 and 274 , and the address electric discharges are produced in the address periods 272 a , 273 a , 275 a and 276 a without supplying the selection electric discharge pulses 252 a - 252 d and electrically charged particle control pulse 244 in the last sub-field. Therefore, the contrast is multiplied by three.

FIG. 34 is a time chart of sub-fields illustrating a driving method in accordance with a sixteenth embodiment of the present invention. Referring to the drawing, the horizontal axis illustrates time, and the vertical axis illustrates a line of cells. Reference numeral 280 denotes one field period, 281 - 286 denote sub-fields, 281 a - 288 a denote address periods, 281 b - 288 b denote sustaining periods, 289 and 290 denote field blocks, and 289 a and 290 a denote full writing erasing periods.

One field period 280 is divided into eight sub-fields 281 - 288 , and the consecutive first four sub-fields 281 - 284 form the field block 289 , while the succeeding consecutive four sub-fields 285 - 288 form the other field block 290 .

The first period of these field blocks 289 and 290 include the full writing erasing periods 289 a and 290 a , respectively, and the address periods 281 a - 288 a and the sustaining periods 281 b - 288 b are arranged in each sub-field 281 - 288 , respectively. That is, the full writing erasing periods 289 a and 290 a are arranged at the first part of the first sub-fields 281 and 285 of the field blocks 289 and 290 , respectively. The numbers of the light emissions are allotted for the sustaining periods 281 b - 288 b , and gradations of display are performed by combining the numbers of the light emissions. According to the sixteenth embodiment, the numbers of the light emissions are increased in order of the sub-fields 281 , 282 , 283 , - - - .

Referring to FIGS. 28 ( b ) to 28 ( g ), the selection electric discharge pulses 252 a - 252 d , the electrically charged particle control pulse 244 and the fine line erasing pulses 245 , 253 a - 253 b , which are used in the fourteenth embodiment, are provided in the sustaining periods 281 b , 282 b , 283 b , 285 b , 286 b and 287 b of the first three sub-fields 281 , 282 , 284 , 285 , 286 and 287 b in the field blocks 287 and 290 , and these pulses are not provided in the other (last) sub-field.

The condition of the electrically charged particles in all cells after the sustaining periods 281 b , 282 b and 283 b of the sub-fields 281 , 282 and 283 in the field block 289 and sustaining periods 285 b , 286 b and 287 b of the sub-fields 285 , 286 and 287 in the field block 290 are finished is maintained in the same condition after the full writing erasing period 289 a is finished, so that the full writing erasing periods 210 a can be deleted in the three sub-fields 282 , 283 , 284 , 286 , 287 and 288 , although they are retained in the first sub-fields 281 and 285 , and the address electric discharges are produced in the address periods 282 a , 283 a , 284 a , 286 a , 287 a and 288 a without supplying the selection electric discharge pulses 252 a - 252 d and the electrically charged particle control pulse 244 in the last sub-field. Therefore, the contrast is multiplied by four.

FIG. 35 is a time chart of sub-fields illustrating a driving method in accordance with a seventeenth embodiment of the present invention. Referring to the drawing, the horizontal axis illustrates time, and the vertical axis illustrates a line of cells. Reference numeral 300 denotes one field period, 301 - 308 denote sub-fields, 301 a - 308 a denote address periods, 301 b - 308 b denote sustaining periods, 309 denotes a field block, and 309 a denotes a full writing erasing period.

One field period 300 is divided into eight sub-fields 301 - 308 , and the field block 309 is formed by all the sub-fields 301 - 308 in the one field. The first period of this field block 309 includes the full writing erasing period 309 a . The address periods 301 a - 308 a and the following sustaining periods 301 b - 308 b are arranged in each sub-field 301 - 308 , respectively. That is, the full writing erasing period 309 a are arranged at the first part of the first sub-field 301 . The numbers of the light emissions are allotted for the sustaining periods 301 b - 308 b and gradations of display are performed by combining the numbers of the light emissions.

Referring to FIGS. 28 ( b ) to 28 ( g ), the selection electric discharge pulses 252 a - 252 d , the electrically charged particle control pulses 244 and the fine line erasing pulses 245 , 253 a - 253 b , which are used in the fourteenth embodiment, are provided in the sustaining periods 301 b - 307 b of the first seven sub-fields 301 - 307 , and the full writing erasing period 309 a is arranged only in the first sub-field 301 . The address electric discharges in the address periods 302 a - 308 a are possible, even if the full writing erasing periods 309 a in the sub-fields 302 - 308 which follow the first sub-field 301 are deleted. Thereby the contrast is multiplied by eight.

According to the invention, by deleting the full writing erasing period in some sub-fields, the contrast is improved. The practical contrast of a cathode ray tube display is, for example, 150:1, and in the plasma display according to the embodiments shown in FIG. 33 or FIG. 34 , a corresponding contrast is accomplished.

The numbers of sub-fields in one field and the numbers of the sub-fields in one field block are optional and not limited to the above mentioned embodiments, and so any combination will be applicable.

According to the present invention, full writing electric discharge and erasing electric discharge are deleted or reduced, thereby improving the contrast of the display.

According to the present invention, a full writing erasing period can be arranged one time per several sub-fields, thereby improving the contrast.

While we have shown and described several embodiments in accordance with the present invention, it is understood that the invention is not limited thereto, but is susceptible of numerous changes and modifications as known to those skilled in the art, and we therefore do not wish to be limited to the details shown and described herein, but intend to cover all such changes and modifications as are encompassed by the scope of the appended claims.

Claims

1. A plasma display panel driving method for a display panel having a plurality of electrodes forming cells, including a first electrode group arranged on a permeable substrate and being capable of being driven in common, a second electrode group arranged in parallel with said first electrode group on said permeable substrate and being capable of being driven independently, a third electrode group arranged perpendicular to said first and second electrode groups on another substrate and being capable of being driven independently, said driving method comprising the steps of:supplying a voltage with a fast rising leading edge so as to immediately produce a maximum electric discharge one time per a sub-field in a cell in which an electric discharge was performed beforehand; and supplying another voltage having a voltage value larger than a voltage value of said voltage with said fast rising leading edge without causing any electric discharge under a first condition.

2. A plasma display panel driving method according to claim 1, further comprising the steps of producing an electric discharge between said first electrode group and said second electrode group by supplying said another voltage under a second condition to said one of said first and second electrode groups one time immediately after power is supplied to said display panel other than when an abnormal state occurs in said cell, and gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering electrically charged particles having the other polarity in the vicinity of said third electrode group by supplying a pulse after said another pulse is supplied.

3. A plasma display panel driving method according to claim 1, wherein said another voltage has a fast rising leading edge.

4. A plasma display panel driving apparatus for a display panel having a plurality of cells, comprising:a first electrode group arranged on a permeable substrate and being capable of being driven in common; a second electrode group arranged in parallel with said first electrode group on said permeable substrate and being capable of being driven independently; a third electrode group arranged perpendicular to said first and second electrode groups on another substrate and being capable of being driven independently; and a circuit for supplying a voltage with a fast rising leading edge so as to immediately produce a maximum electric discharge one time per a sub-field in a cell in which an electric discharge was performed beforehand and for supplying another voltage having a voltage value larger than a voltage value of said voltage with said fast rising leading edge without causing any electric discharge under a first condition.

5. A plasma display panel driving apparatus according to claim 4, wherein said circuit further supplies said another voltage under a second condition to one of said first and second electrode groups for producing an electric discharge between said first electrode group and said second electrode group one time immediately after power is supplied to said display panel other than when an abnormal state occurs in said cell, and another circuit for supplying a pulse after said another pulse is supplied for gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering electrically charged particles having the other polarity in the vicinity of said third electrode group.

6. A plasma display panel driving apparatus according to claim 4, wherein said another voltage has a fast rising leading edge.

7. A plasma display having a plurality of cells, comprising:a first electrode group arranged on a permeable substrate and being capable of being driven in common; a second electrode group arranged in parallel with said first electrode group on said permeable substrate and being capable of being driven independently; and a third electrode group arranged perpendicular to said first and second electrode groups on another substrate and being capable of being driven independently; a circuit for supplying a voltage with a fast rising edge so as to immediately produce a maximum electric discharge one time per a sub-field in a cell to which the electric discharge was performed beforehand and for supplying another voltage having a voltage value larger than a voltage value of said voltage with said fast rising leading edge without causing any electric discharge under a first condition, thereby improving linearity of display gradation.

8. A plasma display according to claim 7, further comprising wherein said circuit further supplies said another voltage under a second condition to one of said first and second electrode groups for producing an electric discharge between said first electrode group and said second electrode group one time immediately after power is supplied to said display panel other than when an abnormal state occurs in said cell, and another circuit for supplying a pulse after said another pulse is supplied for gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering electrically charged particles having the other polarity in the vicinity of said third electrode group.

9. A plasma display according to claim 7, wherein said another voltage has a fast rising leading edge.

10. A plasma display panel driving method for a display panel having a plurality of electrodes forming cells, including first electrode group arranged on a first substrate and being capable of being driven in common, a second electrode group arranged in parallel with said first electrode group on said first substrate and being capable of being driven independently, a third electrode group arranged perpendicular to said first and second electrode groups on a second substrate and being capable of being driven independently, said driving method comprising the steps of:generating a sustaining electric discharge by supplying a sustaining pulse to said first and said second electrode groups; polarizing electrically charged particles in a cell by supplying a fine line erasing pulse having a fast rising edge to one of said first and said second electrode groups so as to immediately produce a maximum electric discharge; gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups, gathering said electrically charged particles having the other polarity in the vicinity of said third electrode group by supplying an equalizing pulse having a voltage value larger than a voltage value of said fine line erasing pulse to said one of electrode groups, and by supplying a regulating pulse rising later than said equalizing pulse to the other electrode group of said first and said second electrode groups without producing an electric discharge under a first condition.

11. A plasma display panel driving method according to the claim 10, further comprising the steps of producing an electric discharge between said first electrode group and said second electrode group by supplying said equalizing pulse to said one of the electrode groups after supplying power, and gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering electrically charged particles having the other polarity in the vicinity of said third electrode group by supplying said regulating pulse after said equalizing pulse is supplied.

12. A plasma display panel driving method according to claim 10, further comprising the steps of producing an address electric discharge between said second electrode group and said third electric group after gathering electrically charged particles having one of the polarities in the vicinity of the said first and said second electrode groups and gathering electrically charged particles having the other polarity in the vicinity of said third electrode group, and performing a sustaining electric discharge.

13. A plasma display panel driving method according to claim 10, further comprising the step of supplying said regulating pulse to said other electrode group within 0.3 μsec-2 μsec after supplying said equalizing pulse to said one of said electrode groups.

14. A plasma display panel driving method according to claim 10, further comprising the steps of supplying said equalizing pulse to said second electrode group, and maintaining the supply of said regulating pulse to said first electrode group until selecting cells to be illuminated for gathering electrically charged particles to a predetermined electrode group.

15. A plasma display panel driving method according to claim 10, further comprising the step of supplying said equalizing pulse to said one electrode group, and setting the falling edge of said equalizing pulse to a time more than 1 μsec.

16. A plasma display panel driving method according to claim 10, wherein said equalizing pulse has a fast rising leading edge.

17. A plasma display panel driving circuit comprising:a first electrode group arranged on a first substrate and driven in common; a second electrode group arranged parallel to said first electrode group on said first substrate and controlled independently; a third electrode group arranged perpendicular to said first and second electrode groups on a second substrate facing said first substrate and controlled independently; a first driving circuit connected to said first electrode group for supplying a first driving pulse; a second driving circuit connected to said second electrode group for supplying a second driving pulse; and a third driving circuit connected to said third electrode group for supplying an address driving pulse; wherein said second driving circuit supplies a fine line erasing pulse having a fast rising leading edge to said second electrode group after sustaining discharging so as to immediately produce a maximum electric discharge, said second driving circuit further supplies an equalizing pulse having a voltage value larger than a voltage value of said fine line erasing pulse to said second electrode group and said first driving circuit supplies a regulating pulse which is delayed from the rising edge of said equalizing pulse to the other electrode group of said first and said second electrode groups, gathers electrically charged particles having one of opposite polarities in the vicinity of said first and said second electrode groups and gathers electrically charged particles having the other polarity in the vicinity of said third electrode group.

18. A plasma display panel driving circuit according to claim 17, wherein said regulating pulse is supplied to said other electrode group within 0.3 μsec-2 μsec after supplying said equalizing pulse to said one of said electrode groups.

19. A plasma display panel driving circuit according to claim 17, wherein said equalizing pulse is supplied from said second driving circuit to said second electrode group, and said regulating pulse is supplied from said first driving circuit to said first electrode group during the addressing of cells to be illuminated.

20. A plasma display panel driving circuit according to claim 17, wherein said equalizing pulse has a fast rising leading edge.

21. A plasma display comprising:a first electrode group arranged on a first substrate and driven in common; a second electrode group arranged parallel to said first electrode group on said first substrate and controlled independently; a third electrode group arranged perpendicular to said first and second electrode groups on a second substrate facing said first substrate and controlled independently; a plurality of cells constructed at the cross points of said first and said second and said third electrode groups; a first circuit for generating a discharge using a fine line erasing pulse having a fast rising leading edge supplied to one of the electrodes of said first and said second electrode groups after a sustaining discharge so as to immediately produce a maximum electric discharge for erasing and polarizing electrically charged particles generated in cells in which said sustaining discharge was generated and for supplying an equalizing pulse having a voltage value larger than a voltage value of said fine line erasing pulse; and a second circuit for supplying a regulating pulse so as to gather electrically charged particles having one of opposite polarities in the vicinity of said first and said second electrode groups and to gather electrically charged particles having the other one of the polarities in the vicinity of said third electrode group by supplying said equalizing pulse to said one of the electrodes and by supplying said regulating pulse to the other of said first and said second electrode groups so as to be able to produce a discharge for addressing which determines light emitting cells by said third electrode group.

22. A plasma display according to claim 21, wherein said regulating pulse is supplied to said other electrode group within 0.3 μsec-2 μsec after supplying said equalizing pulse to said one of said electrode groups for collecting electrically charged particles having one of said polarities in the vicinity of said first and said second electrode groups and electrically charged particles having the other one of said polarities in the vicinity of said third electrode group.

23. A plasma display according to claim 21, wherein said equalizing pulse has a fast rising leading edge.

24. A plasma display panel driving method for a display panel having a plurality of electrodes forming cells, including a first electrode group arranged on a first substrate and being capable of being driven in common, a second electrode group arranged in parallel with said first electrode group on said first substrate and being capable of being driven independently, a third electrode group arranged perpendicular to said first and second electrode groups on a second substrate and being capable of being driven independently, said driving method comprising the steps of:supplying an equalizing pulse under one condition for producing an electric discharge one time in cells other than when an abnormal state occurs in said cells after supplying power for generating electrically charged particles; gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering said electrically charged particles having the other polarity in the vicinity of said third electrode group by supplying a regulating pulse; producing address electric discharge by supplying an address pulse to said third electrode group for selecting cells to be illuminated; generating a sustaining electric discharge by supplying a sustaining pulse to said first and said second electrode groups, polarizing electrically charged particles in a cell by supplying a fine line erasing pulse having a voltage value smaller than a voltage value of said equalizing pulse and having a fast rising leading edge to one of said first and said second electrode groups one time per a sub-field so as to immediately produce a maximum electric discharge; and gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering said electrically charged particles having the other polarity in the vicinity of said third electrode group by supplying said equalizing pulse under another condition to said one of electrode groups and by supplying said regulating pulse rising later than said equalizing pulse to the other electrode group of said first and said second electrode groups without producing an electric discharge.

25. A plasma display panel driving method according to claim 24, wherein said equalizing pulse has a fast rising leading edge.

26. A plasma display panel driving circuit comprising:a first electrode group arranged on a first substrate and driven in common; a second electrode group arranged parallel to said first electrode group on said first substrate and controlled independently; a third electrode group arranged perpendicular to said first and second electrode groups an a second substrate facing said first substrate and controlled independently; a first driving circuit connected to said first electrode group for supplying a first driving pulse; a second driving circuit connected to said second electrode group for supplying a second driving pulse; and a third driving circuit connected to said third electrode group for supplying an address driving pulse; wherein said second driving circuit is arranged for supplying an equalizing pulse under one condition for producing an electric discharge one time in cells other than when an abnormal state occurs in said cells after supplying power for generating electrically charged particles; said first driving circuit is arranged for supplying a regulating pulse for gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering said electrically charged particles having the other polarity in the vicinity of said third electrode group; said third driving circuit is arranged for supplying an address pulse to said third electrode group for producing address electric discharge to select cells to be illuminated; said first driving circuit is arranged for supplying a sustain pulse to said first electrode group and said second driving circuit is arranged for supplying a sustain pulse to said second electrode group for generating sustain discharge; said second driving circuit is arranged for supplying a fine line erasing pulse having a voltage value smaller than a voltage value of said equalizing pulse and having a fast rising leading edge to one of said first and second electrode groups after sustaining discharging so as to immediately produce a maximum electric discharge; and said second driving circuit is arranged for supplying said equalizing pulse under another condition to said one electrode group without discharging, and said first driving circuit is arranged for supplying said regulating pulse which is delayed from the rising edge of said equalizing pulse to the other electrode group of said first and said second electrode groups for gathering electrically charged particles having one of opposite polarities in the vicinity of said first and said second electrode groups and for gathering electrically charged particles having the other polarity in the vicinity of said third electrode group.

27. A plasma display panel driving circuit according to claim 26, wherein said equalizing pulse has a fast rising leading edge.

28. A plasma display comprising:a first electrode group arranged on a first substrate and driven in common; a second electrode group arranged parallel to said first electrode group on said first substrate and controlled independently; a third electrode group arranged perpendicular to said first and second electrode groups on a second substrate provided faced on said first substrate and controlled independently; a plurality of cells constructed at the cross points of said first and said second and said third electrode groups; a first circuit arrangement for supplying an equalizing pulse under one condition for producing an electric discharge one time in cells other than when an abnormal state occurs in said cells after supplying power for generating electrically charged particles; a second circuit arrangement for supplying a regulating pulse for gathering electrically charged particles having one of the polarities in the vicinity of said first and said second electrode groups and gathering said electrically charged particles having the other polarity in the vicinity of said third electrode group; and a third circuit arrangement for supplying an address pulse to said third electrode group for producing address electric discharge to select cells to be illuminated; said first circuit arrangement is arranged for supplying a sustain pulse to said second electrode group and said second circuit arrangement is arranged for supplying a sustain pulse to said first electrode group for generating sustain discharge; said first circuit arrangement is arranged for supplying a fine line erasing pulse to one of said first and second electrode groups after sustaining discharging; and said first circuit arrangement is arranged for generating a discharge using said fine line erasing pulse having a voltage value smaller than a voltage value of said equalizing pulse and having a fast rising leading edge supplied to one of the electrodes of said first and said second electrode groups after a sustaining discharge so as to immediately produce a maximum electric discharge for erasing and polarizing electrically charged particles in cells in which said sustaining discharge was generated; and said first and second circuit arrangements are arranged for gathering electrically charged particles having one of polarities in the vicinity of said first and said second electrode groups and for gathering electrically charged particles having the other one of the polarities in the vicinity of said third electrode group by supplying said equalizing pulse under another condition to said one of the electrodes without electric discharging and by supplying a regulating pulse to the other of said first and said second electrode groups so as to be able to produce a discharge for addressing which determines light emitting cells by said third electrode group.

29. A plasma display according to claim 28, wherein said equalizing pulse has a fast rising leading edge.