Method for driving plasma display panel

Computer graphics processing and selective visual display system – Plural physical display element control system – Display elements arranged in matrix

Reexamination Certificate

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Details

C345S067000

Reexamination Certificate

active

06559817

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a method for driving a plasma display panel, and more particularly, to a method for driving a three-electrode surface-discharge plasma display panel.
2. Description of the Related Art
FIG. 1
shows a structure of a general three-electrode surface-discharge plasma display panel,
FIG. 2
shows an electrode line pattern of the panel shown in
FIG. 1
, and
FIG. 3
shows an example of a pixel of the panel shown in FIG.
1
. Referring to the drawings, address electrode lines A
1
, A
2
, . . . , A
m−1
and A
m
, dielectric layers
11
and
15
, Y electrode lines Y
1
, . . . , and Y
n
, X electrode lines X
1
, . . . , and X
n
, phosphors
16
, partition walls
17
and a MgO protective film
12
are provided between front and rear glass substrates
10
and
13
of a general surface-discharge plasma display panel
1
.
The address electrode lines A
1
, A
2
, . . . , A
m−1
and A
m
are coated over the front surface of the rear glass substrate
13
in a predetermined pattern. The lower dielectric layer
15
entirely coats the front surface of the address electrode lines A
1
, A
2
, . . . , A
m−1
and A
m
. The partition walls
17
on the front surface of the lower dielectric layer
15
are parallel to the address electrode lines A
1
, A
2
, . . . , A
m−1
and A
m
. The partition walls
17
define discharge areas of the respective pixels and prevent optical crosstalk among pixels. The phosphors
17
coat the partition walls
17
.
The X electrode lines X
1
, . . . and X
n
and the Y electrode lines Y
1
, . . . and Y
n
are arranged on the rear surface of the front glass substrate
10
and are orthogonal to the address electrode lines A
1
, A
2
, . . . , A
m−1
and A
m
in a predetermined pattern. The respective intersections define corresponding pixels. The X electrode lines X
1
, . . . and X
n
and the Y electrode lines Y
1
, . . . and Y
n
each comprise conductive indium tin oxide (ITO) electrode lines (X
na
and Y
na
of
FIG. 3
) and metal bus electrode lines (X
nb
and Y
nb
of FIG.
3
). The upper dielectric layer
11
entirely coats the rear surface of the X electrode lines X
1
, . . . and X
n
and the Y electrode lines Y
1
, . . . and Y
n
. The MgO protective film
12
for protecting the panel
1
against strong electrical fields entirely coats over the rear surface of the upper dielectric layer
11
. A gas for forming a plasma is hermetically sealed in a discharge space
14
.
The above-described plasma display panel is basically driven such that a reset step, an address step and a sustain-discharge step are sequentially performed in a unit subfield. In the reset step, wall charges remaining in the previous subfield are erased and space charges are evenly formed. In the address step, the wall charges are formed in a selected pixel area. Also, in the sustain-discharge step, light is produced at the pixel at which the wall charges are formed in the address step. In other words, if alternating pulses of a relatively high voltage are applied between the X electrode lines X
1
, . . . and X
n
and the Y electrode lines Y
1
, . . . and Y
n
, a surface discharge occurs at the pixels at which the wall charges are formed. Here, plasma is formed at the gas layer of the discharge space
14
and the phosphors
142
are excited by ultraviolet rays and thus emit light.
FIG. 4
shows the structure of a unit display period based on a driving method of a general plasma display panel. Here, a unit display period represents a frame in a progressive scanning method, and a field in the case of an interlaced scanning method. The driving method shown in
FIG. 4
is generally referred to as a multiple address overlapping display driving method. According to this driving method, pulses for a display discharge are consistently applied to all X electrode lines X
1
, . . . and X
n
and all Y electrode lines Y
1
, . . . and Y
n
, and pulses for resetting or addressing are applied between the respective pulses for a display discharge. Here, the pulses for resetting or addressing are applied to the Y electrode lines corresponding to a plurality of subfields SF
1
, . . . and SF
8
set as driving periods for the purpose of displaying gray scales in a time-divisional manner.
Thus, compared to an address-display separation driving method, the multiple address overlapping display driving method has an enhanced display luminance. Here, the address-display separation driving method refers to a method in which, within a unit subfield, reset and address steps are performed for all Y electrode lines Y
1
, . . . and Y
n
, during a certain period and a display discharge step is then performed.
Referring to
FIG. 4
, a unit field or frame is divided into 8 subfields SF
1
, . . . and SF
8
for achieving a time-divisional gray scale display. Also, in each subfield, reset, address and sustain-discharge steps are performed, and the time allocated to each sub-field is determined by the display discharge time corresponding to gray scales. For example, in the case of displaying 256 gray scales with 8-bit image data in units of frames, assuming that a unit frame, generally {fraction (1/60)} sec consists of 256 unit times, the first subfield SF
1
driven by the image data of the least significant bit has 1 (2°) unit time, the second subfield SF
2
2 (2
1
) unit times, the third subfield SF
3
4 (2
2
) unit times, the fourth subfield SF
4
8 (2
3
) unit times, the fifth subfield SF
5
16 (2
4
) unit times, the sixth subfield SF
6
32 (2
5
) unit times, the seventh subfield SF
7
64 (2
6
) unit times, and the eighth subfield SF
8
driven by the image data of the most significant bit 128 (2
7
) unit time, respectively. In other words, since the sum of the unit times allocated to the respective subfields is 255 unit times, it is possible to achieve 255 gray scale display, and 256 gray scale display inclusive of one gray scale in which a no display discharge occurs at any subfield.
If an address step is performed for a Y electrode line and then a display discharge step is performed in the first subfield SF
1
, an address step is performed for the corresponding Y electrode line at the second subfield SF
2
. The same procedure is applied to subsequent subfields SF
3
, . . . and SF
8
. For example, if an address step is performed for a corresponding Y electrode line and then a display discharge step is performed in the seventh subfield SF
7
, an address step is performed for the corresponding Y electrode line at the eighth subfield SF
8
. Although the time for a unit subfield equals the time for a unit field or frame, the respective unit subfields are overlapped on the basis of driven Y electrode lines Y
1
, . . . and Y
480
to form a unit field or frame. Thus, since all subfields SF
1
, . . . and SF
8
exist at every timing, time slots for addressing, depending on the number of subfields, are set between the respective display discharge pulses for the purpose of performing the respective address steps.
As one of the above-described multiple address overlapping display driving methods, a driving method in which address steps are performed in the order of Y electrode lines corresponding to the respective subfields between pulses for each. display discharge, is generally used. In this driving method, conventionally, a constant voltage of pulses of display data signals are applied to the address electrode lines selected in accordance with the respective Y electrode lines scanned in the order of the respective subfields. However, since the scanning timings for the respective subfields are different, the standby times required for wall charges which have been formed on the respective Y electrode lines waiting for the pulses for the first display discharge, are different. As the standby time becomes longer, many more of the wall charges which have been formed at the pixels to be displayed are removed. Therefore, according to the conventional driving method, it is quite highly probable that only pixels to be displayed at subfields h

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