Information
-
Patent Grant
-
6495968
-
Patent Number
6,495,968
-
Date Filed
Tuesday, June 26, 200123 years ago
-
Date Issued
Tuesday, December 17, 200221 years ago
-
Inventors
-
Original Assignees
-
Examiners
Agents
-
CPC
-
US Classifications
Field of Search
US
- 345 60
- 345 63
- 345 65
- 345 67
- 345 37
-
International Classifications
-
Abstract
The object is to provide a method for driving a plasma display panel, the method being capable of providing improved display quality. A display cell of the plasma display panel is reset to a light-emitting cell state (or a non-light-emitting cell state) only in the head subfield during the display period of one field. Then, in each subfield, executed is a data write process for applying successively a scanning pulse, for generating a selective erase discharge, to each of the row electrodes in order to change selectively each of the display cells from the light-emitting cell state (non-light-emitting cell state) to the non-light-emitting cell state (light-emitting cell state) in accordance with an input video signal. Also executed in each subfield is a light emission sustain process for applying a train of sustain pulses to each of the row electrodes in conjunction with the scanning pulse, the train of sustain pulses generating a sustain discharge to allow only a display cell in the light-emitting cell state to emit light for the number of times corresponding to a weight of each of the subfields.
Description
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a method for driving a plasma display panel.
2. Description of Related Art
In recent years, display devices have been required to provide reduced thickness as the devices have been increased in size, and accordingly various types of thin display devices have been in practical use. Attention is focused on an AC discharge plasma display panel as one of the thin display devices.
FIG. 1
is a schematic view illustrating the configuration of a plasma display device comprising such a plasma display panel and a drive device.
Referring to
FIG. 1
, the plasma display panel or a PDP
10
comprises m column electrodes D
1
to D
m
, and n row electrodes X
1
to X
n
and n row electrodes Y
1
to Y
n
, each of which intersects the column electrodes. These row electrodes X
1
to X
n
and row electrodes Y
1
to Y
n
allow a pair of row electrode X
i
(1≦i≦n) and row electrode Y
i
(1≦i ≦n) to form the first to nth display line in the PDP
10
. In between a column electrode D and row electrodes X, Y, there is formed a discharge space in which a discharge gas is sealed. There is formed a display cell acting as a pixel at the intersection of each pair of row electrodes and a column electrode, including the discharge space.
With this construction, each display cell emits light through a discharge phenomenon and therefore has only two states, or a “light-emitting” state and a “non-light-emitting” state. Accordingly, the display cell can express the brightness of only two levels of gray scale, or a minimum brightness (“non-light-emitting” state) and a maximum brightness (“light-emitting” state).
In this regard, for the implementation of displaying halftone brightness corresponding to an input video signal, a driver
100
employs a subfield method to perform gray scale drive on the PDP
10
mentioned above.
According to the subfield method, for example, an input video signal is converted into display data of four bits corresponding to each display cell. As shown in
FIG. 2
, one field comprises four subfields SF
1
to SF
4
corresponding to each bit digit of the four bits. Then, in each of the subfields, as described below, a simultaneous reset process Rc, a data write process Wc, a light-emission sustain process Ic, and an erase process E are performed, respectively.
FIG.
3
. is a view illustrating various types of drive pulses that the driver
100
applies to the aforementioned PDP
10
, and the application timing of the drive pulses.
First, in the aforementioned simultaneous reset process Rc, the driver
100
applies a positive reset pulse RP
X
to the row electrodes X
1
to X
n
and a negative reset pulse RP
Y
to the row electrodes Y
1
to Y
n
. The application of these reset pulses RP
X
and RP
Y
will cause all display cells of the PDP
10
to be reset and discharged, allowing a predetermined uniform wall charge to be built in each of the display cells. Immediately thereafter, the driver
100
applies simultaneously an erasing pulse EP to the row electrodes X
1
to X
n
of the PDP
10
. The application of the erasing pulse EP will cause an erase discharge to be generated in all of the display cells, thereby erasing the aforementioned wall charge. This will reset all the display cells to the state in which no light emission (sustain discharge) is allowed (hereinafter referred to as the “non-light-emitting cell” state) in the light-emission sustain process Ic, described later.
Then, in the data write process Wc, the driver
100
separates each bit of the aforementioned display data of four bits corresponding to each of the subfields SF
1
to SF
4
to generate a data pulse having a pulse voltage corresponding to the logic level of the bits. For example, in the data write process Wc of the subfield SF
1
, the driver
100
generates a data pulse having a pulse voltage corresponding to the logic level of the first bit of the aforementioned display data. At this time, the driver
100
generates a high-voltage data pulse with the logic level of the first bit being “1”, and a low-voltage (zero volt) data pulse with the logic level being “0”. Then, as shown in
FIG. 3
, the driver
100
successively applies such data pulses to the column electrodes D
1
to D
m
as a group of data pulses DP
1
to DP
n
for each display line corresponding to each of the first to nth display lines. Furthermore, as shown in
FIG. 3
, the driver
100
generates a negative scanning pulse SP in phase with the application timing of each group of data pulses DP to apply successively the negative scanning pulse SP to the row electrodes Y
1
to Yn. At this time, discharge (selective write discharge) is caused only at the display cells located at the intersections of the display lines to which the scanning pulse SP is applied and the “columns” to which the high-voltage data pulse is applied. After such a selective write discharge has been terminated, wall charges are built up in the display cells and held. This causes the display cells that have been reset to the “non-light-emitting cell” state in the aforementioned simultaneous reset process Rc to change to the state (hereinafter referred to as the “light-emitting cell” state) in which the display cells can emit light (sustain discharge) in the light-emission sustain process Ic, described later. On the other hand, no such a selective write discharge described above is generated in the display cells to which the scanning pulse SP or the low-voltage data pulse has been applied, allowing the state that has been reset in the aforementioned simultaneous reset process Rc or the “non-light-emitting cell” state to be held.
Subsequently, as shown in
FIG. 3
, in the light-emission sustain process Ic, the driver
100
applies the positive sustain pulse IPX and the positive sustain pulse IP
Y
alternately to the row electrodes X
1
to X
n
and the row electrodes Y
1
to Y
n
, respectively. Incidentally, as shown in
FIG. 2
, the number of times (or the duration) of application of the sustain pulses IP
X
and IP
Y
in one subfield is set according to the weight of each subfield. Here, only the display cells in which wall charges are present or only the display cells in the “light-emitting cell” state perform sustain discharge every time the aforementioned sustain pulses IP
X
and IP
Y
are applied thereto in order to sustain the “light-emitting” state involved in the discharge.
Subsequently, in the erase process E, the driver
100
applies simultaneously the negative erasing pulse EP, shown in
FIG. 3
, to each of the row electrodes Y
1
to Y
n
. This allows an erase discharge in all the display cells to be generated, causing all the wall charges remaining in each of the display cells to dissipate.
Execution of the series of these operations in each of the subfields (SF
1
to SF
4
) will allow halftone brightness to be viewed in accordance with the total number of times of light emission carried out in the light-emission sustain process Ic of each subfield. For example, for the four subfields as mentioned above, it is possible to express the range of brightness available to an input video signal with 16 levels of halftone brightness by combining the subfields that are allowed to emit light in the light-emission sustain process Ic. At this time, the greater the number of subfields to be provided by division, the greater the number of steps or the level of gray scale becomes, thereby making it possible to provide a display image of higher quality.
However, since the display period of one field is specified, the number of subfields provided by dividing a field cannot be increased without limitation.
In addition, in the drive shown in
FIGS. 2 and 3
, a light emission pattern for providing display brightness of brightness level “7” shown in
FIG. 4
is inverted with respect to that for providing display brightness of brightness level “8” in one field period. In some cases, this would cause false contours to be viewed in the image.
That is, as shown in
FIG. 4
, the display cells for displaying brightness level “7” are in the “non-light-emitting” state while the display cells for displaying brightness level “8” are emitting light in one field. On the other hand, the display cells for displaying brightness level “8” are in the “non-light-emitting” state while the display cells for displaying brightness level “7” are emitting light in one field.
Thus, looking at the display cells for displaying brightness level “8” immediately before the display cells for displaying brightness level “8” change from the “non-light-emitting” to the “light-emitting” state would cause the viewer to continuously view only the “non-light-emitting” state of both display cells and thereby to recognize dark lines on the boundary thereof. These dark lines, having nothing to do with the display data, would appear as false contours to cause degradation in display quality.
OBJECTS AND SUMMARY OF THE INVENTION
The present invention has been made to solve the aforementioned problems. It is therefore an object of the present invention to provide a method for driving plasma display panels, the method being capable of providing improved display quality.
The present invention provides a method for driving a plasma display panel by allowing a display period of one field of an input video signal to comprise a plurality of subfields for halftone drive, the plasma display panel having a display cell acting as a pixel at each intersection of a plurality of row electrodes acting as a display line and a plurality of column electrodes each intersecting each of said row electrodes. Executed first is a reset process, only in a head subfield during the display period of said one field, for initializing said display cell to a light-emitting cell state. Then, in each of said subfields, executed is a data write process for applying successively a scanning pulse for generating a selective erase discharge to each of said row electrodes in order to change selectively each of said display cells from said light-emitting cell state to a non-light-emitting cell state in accordance with said input video signal. Then, executed is a light emission sustain process for applying a train of scanning pulses to each of the row electrodes immediately after said scanning pulse has been applied thereto, the train of scanning pulses generating a sustain discharge to allow only a display cell in said light-emitting cell state to emit light for the number of times corresponding to a weight of each of said subfields.
Furthermore, the present invention provides a method for driving a plasma display panel by allowing a display period of one field of an input video signal to comprise a plurality of subfields for halftone drive, the plasma display panel having a display cell acting as a pixel at each intersection of a plurality of row electrodes acting as a display line and a plurality of column electrodes each intersecting each of said row electrodes. Executed first is a reset process, only in a head subfield during the display period of said one field, for initializing said display cell to a non-light-emitting cell state. Then, in each of said subfields, executed is a data write process for applying successively a scanning pulse for generating a selective write discharge to each of said row electrodes in order to change selectively each of said display cells from said non-light-emitting cell state to said light-emitting cell state in accordance with said input video signal. Then, executed is a light emission sustain process for applying a train of scanning pulses to each of the row electrodes immediately after said scanning pulse has been applied thereto, the train of scanning pulses generating a sustain discharge to allow only a display cell in said light-emitting cell state to emit light for the number of times corresponding to a weight of each of said subfields.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1
is a schematic view illustrating the configuration of a plasma display device;
FIG. 2
is a view illustrating an example of a light-emission drive format in accordance with a subfield method;
FIG. 3
is a view illustrating various drive pulses to be applied to a PDP
10
and the application timing thereof;
FIG. 4
is a view illustrating an example of a combination of light-emission patterns that causes a false contour;
FIG. 5
is a view illustrating the configuration of a plasma display device for driving a plasma display panel in accordance with a drive method according to the present invention;
FIG. 6
is a view illustrating the internal configuration of a data conversion circuit
30
;
FIG. 7
is a view illustrating the internal configuration of an ABL circuit
31
;
FIG. 8
is a view illustrating the conversion characteristic of a data conversion circuit
312
;
FIG. 9
is a view illustrating the relationship between the brightness mode and the number of times of application of scanning pulses IP in the light-emission sustain process Ic of each of subfields SF
1
to SF
14
;
FIG. 10
is a view illustrating the data conversion characteristic of a first data conversion circuit
32
;
FIG. 11
is a view illustrating a data conversion table in accordance with the data conversion characteristic shown in
FIG. 10
;
FIG. 12
is a view illustrating a data conversion table in accordance with the data conversion characteristic shown in
FIG. 10
;
FIG. 13
is a view illustrating the internal configuration of a multi-level gray scale processing circuit
33
.
FIG. 14
is an explanatory view showing the operation of an error diffusion processing circuit
330
.
FIG. 15
is a view showing the internal configuration of a dither processing circuit
350
.
FIG. 16
is an explanatory view showing the operation of the dither processing circuit
350
.
FIG. 17
is a view showing a conversion table to be used in a second data conversion circuit
34
when a selective erase address method is employed, and a light-emission drive pattern, based on cell drive data GD and provided by the conversion table;
FIG. 18
is a view illustrating a light-emission drive format to be used when the selective erase address method is employed;
FIG. 19
is a view illustrating various drive pulses to be applied to the PDP
10
in accordance with the light-emission drive format shown in FIG.
18
and the application timing thereof;
FIG. 20
is a view illustrating the light-emission drive format to be used when the selective erase address method is employed; and
FIG. 21
is a view showing a conversion table to be used in the second data conversion circuit
34
when a selective write address method is employed, and a light-emission drive pattern, based on cell drive data GD and provided by the conversion table.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Now, the present invention will be explained below with reference to the accompanying drawings in accordance with the embodiments.
FIG. 5
is a view showing the general configuration of a plasma display device for gray scale driving a plasma display panel in accordance with a drive method of the present invention.
As shown in
FIG. 5
, the plasma display device comprises a plasma display panel or a PDP
10
and various types of functional modules for driving the PDP
10
.
The PDP
10
comprises discharge spaces (not shown) in which a discharge gas is sealed, and a front glass substrate (not shown) and a rear glass substrate, which sandwich and thereby define the discharge spaces. The front glass substrate serves as the display screen for use with the PDP
10
, and on the reverse surface thereof, there are formed row electrodes X
1
to X
n
and row electrodes Y
1
to Y
n
, respective pairs of which act as one display line and which are parallel to each other as shown in FIG.
5
. On the other hand, on the rear glass substrate, there are formed m column electrodes D
1
to D
m
in the direction intersecting the aforementioned row electrodes X and Y. A display cell acting as a pixel is formed at the intersection, including the aforementioned discharge space, of each pair of row electrodes and a column electrode.
An A/D converter
1
samples an analog input video signal to convert the video signal into, for example, 8-bit display data PD corresponding to each display cell. Then the resulting data is supplied to a data conversion circuit
30
. The data conversion circuit
30
converts the 8-bit display data PD into 14-bit cell drive data GD, which is in turn supplied to a memory
4
.
FIG. 6
is a view illustrating the internal configuration of the data conversion circuit
30
.
An ABL (automatic brightness control) circuit
31
tunes the brightness level of the display data PD so that the average brightness of the image displayed on the screen of the PDP
10
falls within the predetermined range of brightness. Then, the ABL circuit
31
supplies the brightness tuning display data PDB
L
obtained through the tuning of the brightness level.
FIG. 7
is a view showing the internal configuration of the ABL circuit
31
.
Referring to
FIG. 7
, a data conversion circuit
312
converts the brightness-tuning display data PD
BL
supplied from a level adjusting circuit
310
into the inverse-Gamma-corrected display data PD
r
having the inverse Gamma characteristics (Y=X
2.2
) with the non-linear characteristics as shown in FIG.
8
. Then, the data conversion circuit
312
supplies the inverse-Gamma-corrected display data PDr to an average brightness level detector circuit
311
. That is, from the aforementioned brightness tuning display data PD
BL
, the data conversion circuit
312
restores display data corresponding to the original video signal of which Gamma correction is undone and then outputs the display data as the inverse-Gamma-corrected display data PD
r
. First, the average brightness level detector circuit
311
determines the average brightness of the inverse-Gamma-corrected display data PD
r
and then selects a brightness mode, which is employed for displaying an image at the brightness (the brightness of the whole screen) in response to the average brightness, from the brightness modes 1 to 4, shown in FIG.
9
. Then, the average brightness level detector circuit
311
supplies a brightness mode signal LC indicative of the selected brightness mode to a drive control circuit
2
. In addition, the average brightness level detector circuit
311
supplies average brightness information indicative of the average brightness determined as described above to the aforementioned level adjusting circuit
310
. The level adjusting circuit
310
tunes the brightness level of the display data PD in accordance with the average brightness information to obtain the aforementioned brightness tuning display data PD
BL
, which is in turn supplied to the aforementioned data conversion circuit
312
. Moreover, as shown in
FIG. 6
, the level adjusting circuit
310
supplies the brightness tuning display data PD
BL
to a first data conversion circuit
32
provided in the following stage.
In accordance with the conversion characteristic as shown in
FIG. 10
, the first data conversion circuit
32
suppresses the aforementioned brightness tuning display data PD
BL
to (224/225), which allows for expressing 256 levels of gray scale with 8 bits, and then supplies the resulting data to a multi-level gray scale processing circuit
33
as the brightness suppressing display data PD
P
. More specifically, in accordance with the conversion tables shown in
FIGS. 11 and 12
, which are based on the aforementioned conversion characteristic, the first data conversion circuit
32
converts the brightness tuning display data PD
BL
to the brightness suppressing display data PD
P
. This prevents the occurrence of brightness saturation caused by the multi-gray-scale processing performed by the multi-level gray scale processing circuit
33
and the occurrence of a flat portion in display characteristic (or distortion in level of gray scale), which is caused when a display level of gray scale is not present on bit boundaries.
FIG. 13
is a view showing the internal configuration of the multi-level gray scale processing circuit
33
.
As shown in
FIG. 13
, the multi-level gray scale processing circuit
33
comprises an error diffusion-processing circuit
330
and a dither processing circuit
350
.
A data separation circuit
331
of the error diffusion processing circuit
330
separates the lower 2 bits of the 8-bit brightness suppressing display data PD
P
supplied by the aforementioned first data conversion circuit
32
into error data and the upper 6 bits into main display data. Then, the data separation circuit
331
supplies the main display data to an adder
333
and the aforementioned error data to an adder
332
. The adder
332
supplies, to a delay circuit
336
, the sum obtained by adding the error data, the delay output from a delay circuit
334
, and a multiplication output of a coefficient multiplier
335
. The delay circuit
336
causes the sum supplied by the adder
332
to be delayed by a delay time D of the same length of time as the sampling period of the display data PD. Then, the delay circuit
336
supplies the sum to the aforementioned coefficient multiplier
335
and the delay circuit
337
as a delayed signal AD
1
, respectively. The coefficient multiplier
335
multiplies the aforementioned delayed signal AD
1
by the predetermined coefficient K
1
(for example, “{fraction (7/16)}”) and then supplies the resulting value to the aforementioned adder
332
. The delay circuit
337
causes further the aforementioned delayed signal AD
1
to be delayed by the time (equal to one horizontal scan period—the aforementioned delay time D×4) and then supplies the resulting value to a delay circuit
338
as a delayed signal AD
2
. The delay circuit
338
causes further the delayed signal AD
2
to be delayed by the aforementioned delay time D and then supplies the resulting value to a coefficient multiplier
339
as a delayed signal AD
3
. Moreover, the delay circuit
338
causes further the delayed signal AD
2
to be delayed by the aforementioned delay time D×2 and then supplies the resulting value to a coefficient multiplier
340
as a delayed signal AD
4
. Still moreover, the delay circuit
338
causes the delayed signal AD
2
to be delayed by the aforementioned delay time D×3 and then supplies the resulting value to a coefficient multiplier
341
as a delayed signal AD
5
. The coefficient multiplier
339
multiplies the aforementioned delayed signal AD
3
by the predetermined coefficient K
2
(for example, “{fraction (3/16)}”) and then supplies the resulting value to an adder
342
. The coefficient multiplier
340
multiplies the aforementioned delayed signal AD
4
by the predetermined coefficient K
3
(for example, “{fraction (5/16)}”) and then supplies the resulting value to the adder
342
. The coefficient multiplier
341
multiplies the aforementioned delayed signal AD
5
by the predetermined coefficient K
4
(for example, “{fraction (1/16)}”) and then supplies the resulting value to the adder
342
. The adder
342
supplies, to the aforementioned delay circuit
334
, the sum signal that has been obtained by adding the results of multiplication supplied by the aforementioned respective coefficient multipliers
339
,
340
, and
341
. The delay circuit
334
causes such a sum signal to be delayed by the aforementioned delay time D and then supplies the resulting value signal to the aforementioned adder
332
. The adder
332
adds the aforementioned error data (lower two bits of the brightness suppressing display data PD
P
), the delay output from the delay circuit
334
, and the output of multiplication of the coefficient multiplier
335
. Then, the adder
332
generates a carry-out signal Co of logic “0” in absence of carry as the result of the addition and a carry-out signal Co of logic level “1” in the presence of carry and supplies the signal to the adder
333
. The adder
333
adds the aforementioned main display data (upper 6 bits of the brightness suppressing display data PD
P
) to the aforementioned carry-out signal Co and outputs the resulting value as 6-bit error diffusion processing display data ED.
The operation of the error diffusion processing circuit
330
configured as such is to be explained below.
For example, the error diffusion processing display data ED corresponding to pixel G (j, k) of the PDP
10
shown in
FIG. 14
is determined. In this case, first, the respective pieces of the error data corresponding to pixel G (j, k−1) on the left of the pixel G (j, k), pixel G (j−1, k−1) on the upper left, pixel G (j−1, k) on the immediate above, and pixel G (j−1, k+1) on the upper right, that is:
Error data corresponding to the pixel G (j, k−1), the delayed signal AD
1
;
Error data corresponding to the pixel G (j−1, k+1), the delayed signal AD
3
;
Error data corresponding to the pixel G (j−1, k), the delayed signal AD
4
; and
Error data corresponding to the pixel G (j−1, k−1), the delayed signal AD
5
are assigned the weights of the predetermined coefficients K
1
to K
4
for addition. Subsequently, the result of the addition is added by the error data corresponding to the lower two bits of the brightness suppressing display data PD
P
or pixel G (j, k). Then, the carry-out signal Co of one bit thus obtained is added to the display data corresponding to the upper six bits of the brightness suppressing display data PD
P
or the pixel G (j, k) and the resulting value is employed as the error diffusion processing display data ED.
The error diffusion processing circuit
330
assigns weights (lower two bits of the brightness suppressing display data PD
P
) to and then adds the respective pieces of error data of the surrounding pixels {G (j, k−1), G (j−1, k+1), G (j−1, k), G (j−1, k−1)}, and the resulting value is reflected to the aforementioned display data of the aforementioned pixel G (j, k) (upper six bits of the brightness suppressing display data PD
P
). This operation allows the brightness of the lower 2 bits at the original pixel {G (j, k)} to be expressed by the aforementioned surrounding pixels in an apparent manner. Therefore, this allows the display data of the number of bits less than 8 bits or equal to 6 bits to express the levels of gray scale of brightness equivalent to those expressed by the aforementioned 8-bit display data.
Incidentally, an even addition of these coefficients of error diffusion to respective pixels would cause the noise resulting from error diffusion patterns to be visually noticed in some cases and thus the display quality to be degraded. In this regard, like the case of the dither coefficients to be described later, the coefficients K
1
to K
4
of error diffusion that should be assigned to respective four pixels may be changed at each field.
The dither processing circuit
350
performs the dither processing on the error diffusion processing display data ED supplied by the error diffusion processing circuit
330
. This allows for generating the multi-level gray scale processing display data PD
s
, the number of bits of which is reduced further to 4 bits. Meanwhile, the dither processing circuit
350
maintains the level of gray scale of the same brightness as that of the 6-bit error diffusion processing display data ED. Incidentally, the dither processing allows a plurality of adjacent pixels to express one intermediate display level. For example, suppose that display of gray scale equivalent to 8 bits is performed using the display data of upper 6 bits out of 8-bit display data. In this case, four pixels adjacent to each other on the right and left, and above and below are taken as one set. Four dither coefficients a to d having values different from each other are assigned to respective pieces of the display data corresponding to each of the pixels in the set for addition. The dither processing is to generate four different combinations of intermediate display levels with four pixels. Therefore, even with the number of bits of the display data equal to 6 bits, the brightness levels of gray scale available for display are 4 times or halftone display corresponding to 8 bits becomes available.
However, an even addition of the dither patterns with the coefficients a to d to respective pixels would cause the noise resulting from the dither patterns to be visually noticed and thus the display quality to be degraded.
In this regard, the dither processing circuit
350
changes the dither coefficients a to d that should be assigned to respective four pixels at each field.
FIG. 15
is a view showing the internal configuration of the dither processing circuit
350
.
Referring to
FIG. 15
, a dither coefficient generating circuit
352
generates four dither coefficients a, b, c, and d for each of four pixels adjacent to each other and supplies these coefficients in sequence to an adder
351
.
For example, as shown in
FIG. 16
, four dither coefficients a, b, c, and d are generated corresponding to four pixels, respectively. The four pixels are pixel G (j, k) and pixel G (j, k+1) corresponding to row j, and pixel G (j+1, k) and pixel G (j+1, k+1) corresponding to row (j+1). At this time, the dither coefficient generating circuit
352
changes, for each field as shown in
FIG. 16
, the aforementioned dither coefficients a, b, c, and d that should be assigned to the respective four pixels.
That is, dither coefficients a to d are assigned to the pixels at each field and generated repeatedly in a cyclic manner as shown below and supplied to the adder
351
.
That is, at the starting first field,
pixel G (j, k), dither coefficient a,
pixel G (j k+1), dither coefficient b,
pixel G (j+1, k), dither coefficient c, and
pixel G (j+1, k+1), dither coefficient d;
at the subsequent second field,
pixel G (j, k), dither coefficient b,
pixel G (j, k+1), dither coefficient a,
pixel G (j+1, k), dither coefficient d, and
pixel G (j+1, k+1), dither coefficient c;
at the subsequent third field,
pixel G (j, k), dither coefficient d,
pixel G (j, k+1), dither coefficient c,
pixel G (j+1, k), dither coefficient b, and
pixel G (j+1, k+1), dither coefficient a;
and, at the fourth field,
pixel G (j, k), dither coefficient c,
pixel G (j, k+1), dither coefficient d,
pixel G (j+1, k), dither coefficient a, and
pixel G (j+1, k+1), dither coefficient b;
The dither coefficient generating circuit
352
executes repeatedly the operation of the first to fourth fields mentioned above. That is, upon completion of generating the dither coefficients at the fourth field, the above-mentioned operation is repeated all over again from the aforementioned first field.
The adder
351
adds the dither coefficients a to d which are assigned to respective fields as mentioned above to the error diffusion processing display data ED, respectively. Hereupon, the error diffusion processing display data ED correspond to the aforementioned pixel G (j, k), pixel G (j, k+1), pixel G (j+1, k), and pixel G (j+1, k+1), respectively, which are supplied by the aforementioned error diffusion processing circuit
330
. The adder
351
then supplies the dither additional display data thus obtained to an upper bit extracting circuit
353
.
For example, at the first field shown in
FIG. 16
, each piece of the following data is supplied sequentially as the dither additional display data to the upper bit extracting circuit
353
. That is:
error diffusion processing display data ED corresponding to pixel G (j, k)+dither coefficient a;
error diffusion processing display data ED corresponding to pixel G (j, k+1)+dither coefficient b;
error diffusion processing display data ED corresponding to pixel G (j+1, k)+dither coefficient c; and
error diffusion processing display data ED corresponding to pixel G (j+1, k+1)+dither coefficient d.
The upper bit extracting circuit
353
extracts the bits up to the upper four bits of the dither additional display data to supply the resulting bits to a second data conversion circuit
34
shown in
FIG. 6
as the multi-level gray scale display data PD
s
.
The second data conversion circuit
34
converts the multi-level gray scale display data PD
s
into the cell drive data GD of bit
1
to
14
corresponding to respective subfields SF
1
to SF
14
in accordance with the conversion table shown in FIG.
17
. Incidentally, each of the bits
1
to
14
in the cell drive data GD corresponds to each of the subfields SF
1
to SF
14
, described later. The second data conversion circuit
34
supplies the cell drive data GD to the memory
4
as shown in FIG.
5
.
The memory
4
writes sequentially the aforementioned display drive display data GD in accordance with the write signal supplied by the drive control circuit
2
. The memory
4
performs the following read operation each time the memory
4
has written a screenful of data or (n×m) pieces of data from cell drive data GD
11
corresponding to the first row and column to cell drive data GD
nm
corresponding to the nth row and mth column.
First, the memory
4
interprets the first bit of the cell-drive data GD
11
to GD
nm
as cell-drive data bits DB
1
11
to DD
nm
to read successively the cell-drive data bits DB
1
11
to DB
1
nm
for each display line and supply the bits to an addressing driver
6
. Then, the memory
4
interprets the second bit of the cell-drive data GD
11
to GD
nm
as cell-drive data bits DB
2
11
to DB
2
nm
to read successively the cell-drive data bits DB
2
11
to DB
2
nm
for each display line and supply the bits to the addressing driver
6
. Then, the memory
4
interprets the third bit of the cell-drive data GD
11
to GD
nm
as cell-drive data bits DB
3
11
to DB
3
nm
to read successively the cell-drive data bits DB
3
11
to DB
3
nm
for each display line and supply the bits to the addressing driver
6
. Subsequently, in the similar manner, the memory
4
interprets the fourth, fifth, . . . fourteenth bit of the cell-drive data GD
11
to GD
nm
as cell-drive data bits DB
4
11
to DB
4
nm
, DB
5
11
to DB
5
nm
, . . . DB
14
11
to DB
14
nm
to read successively the cell-drive data bits DB
4
11
to DB
4
nm
, DB
5
11
to DB
5
nm
, . . . DB
14
11
to DB
14
nm
for each display line and supply the bits to the addressing driver
6
.
Incidentally, the memory
4
performs the reading operation of the aforementioned cell-drive data bits DB
1
to DB
14
corresponding to each of the subfields SF
1
to SF
14
, described later. That is, the memory
4
reads cell-drive data bits DB
1
11
to DB
1
nm
in subfield SF
1
, cell-drive data bits DB
2
11
to DB
2
nm
in subfield SF
2
, and cell-drive data bits DB
3
11
to DB
3
nm
in subfield SF
3
.
The drive control circuit
2
generates various timing signals for driving the levels of gray scale of the PDP
10
and supplies the signals to the addressing driver
6
, a first sustain driver
7
, and a second sustain driver
8
in accordance with the light-emission drive format shown in FIG.
18
.
Incidentally, in the light-emission drive format shown in
FIG. 18
, a display period of one field (frame) is divided into
14
subfields SF
1
to SF
14
. Then, the data write process Wc and the light-emission sustain process Ic are performed in each of the subfields. Moreover, the simultaneous reset process Rc is executed only in the head subfield SF
1
and the erase process E is executed only in the last subfield SF
14
.
FIG. 19
is a view illustrating various drive pulses to be applied to the PDP
10
by each of the addressing driver
6
, the first sustain driver
7
, and the second sustain driver
8
in accordance with the various types of timing signals supplied from the drive control circuit
2
, and the application timing thereof. Incidentally,
FIG. 19
shows only the subfields SF
1
, SF
2
and their adjacent subfields, which are extracted from the subfields shown in FIG.
18
.
Throughout all periods, the first sustain driver
7
generates repeatedly the sustain pulse I
X
having a positive voltage Vsus shown in
FIG. 19
at predetermined intervals and applies the sustain pulse IPX to the row electrodes X
1
to X
n
.
Here, only at the head portion of the subfield SF
1
, the second sustain driver
8
generates the reset pulse RP
Y
having a negative voltage −V
rst
at the same timing as that of the aforementioned sustain pulses IP
X
and applies successively the reset pulse RP
Y
to the row electrodes Y
1
to Y
n
as shown in
FIG. 19
(reset process RJ).
According to the aforementioned reset process RJ, a reset discharge is generated in each of the display cells on the display line to which the aforementioned reset pulse RP
Y
is applied. After the termination of the discharge, wall charges are built up in each of the display cells. That is, each display cell is reset by discharge successively at one display line after another to a state in which light emission (sustain discharge) can be executed in the light-emission sustain process Ic, described later.
Then, immediately after the application of each of the aforementioned reset pulses RP
Y
, the second sustain driver
8
generates the scanning pulse SP having a negative voltage −V
OFS
shown in FIG.
19
and applies successively to the row electrodes Y
1
to Y
n
. Incidentally, in the subfields subsequent to the subfield SF
2
, as soon as the last sustain pulse IP
Y
(described later) has been applied to each display line within the subfield immediately before a subfield, the second sustain driver
8
applies the aforementioned scanning pulse SP to the row electrodes Y that are responsible for the display line. Meanwhile, the addressing driver
6
generates a high-voltage data pulse when the aforementioned memory
4
has supplied a cell-drive data bit DB of a logic level of “1”, while generating a low-voltage (zero volt) data pulse when the aforementioned memory
4
has supplied a cell-drive data bit DB of a logic level of “0”. Then, the data pulse is applied successively to the column electrodes D
1
to D
m
on one display line after another at the same timing as that of the aforementioned scanning pulse SP (data write process Wc).
For example, in the subfield SF
1
, the memory
4
supplies the cell-drive data bits DB
1
11
to DB
1
nm
. Thus, in the data write process Wc of the subfield SF
1
, the addressing driver applies each of the group of data pulses DP
1
1
to DP
1
n
, corresponding to the cell-drive data bits DB
1
11
to DB
1
nm
, to the column electrodes D
1
to D
m
successively at the timing of each scanning pulse SP as shown in FIG.
19
. In the subfield SF
2
, the memory
4
supplies the cell-drive data bits DB
2
11
to DB
2
nm
as described above. Thus, in the data write process Wc of the subfield SF
2
, the addressing driver applies each of the group of data pulses DP
2
1
to DP
2
n
, corresponding to the cell-drive data bits DB
2
11
to DB
2
nm
, to the column electrodes D
1
to D
m
successively at the timing of each scanning pulse SP as shown in FIG.
19
. In the subfield SF
3
, the memory
4
supplies the cell-drive data bits DB
3
11
to DB
3
nm
as described above. Thus, in the data write process Wc of the subfield SF
3
, the addressing driver applies each of the group of data pulses DP
3
1
to DP
3
n
, corresponding to the cell-drive data bits DB
3
11
to DB
3
nm
, to the column electrodes D
1
to D
m
successively at the timing of each scanning pulse SP as shown in FIG.
19
.
In the aforementioned data write process Wc, a discharge (selective erase discharge) is caused only at the display cells located at the intersections of the display lines to which the afore scanning pulse SP is applied and the “columns” to which a high-voltage data pulse is applied. The wall charge remaining in the display cells is erased. That is, the display cells in which such a selective erase discharge has been generated change to a state in which light emission (sustain discharge) cannot be performed (hereinafter referred to as the “non-light-emitting cell” state) in the light-emission sustain process Ic, described later. On the other hand, no discharge, as the aforementioned selective erase discharge, is generated in the display cells to which the aforementioned scanning pulse SP and low-voltage data pulse have been applied. Thus, the display cells that have been in the “light-emitting cell” state until the application of the scanning pulse SP remain in the “light-emitting cell” state. On the other hand, the display cells that have been in the “non-light-emitting cell” state remain in the “non-light-emitting cell” state. That is, each display cell is successively selectively erased by discharge on one display line after another in accordance with display data and set to the “light-emitting cell” state or the “non-light-emitting cell” state.
Subsequently, immediately after the application of the aforementioned scanning pulse SP, the second sustain driver
8
generates repeatedly sustain pulses IP
Y
having a positive voltage V
SUS
as shown in
FIG. 19
for each display line and applies the pulses to the row electrodes Y (light-emission sustain process Ic).
Incidentally, the number of times of application of the sustain pulses IP
Y
is set in accordance with the weight assigned to each of the subfields SF
1
to SF
14
and determined in accordance with the brightness mode signal LC supplied from the aforementioned average brightness level detector circuit
311
. For example, for the brightness mode signal LC being indicative of “1” as shown in
FIG. 9
, the sustain pulse IP
Y
is applied in the light-emission sustain process Ic of each of the subfields SF
1
to SF
14
by the following number of times of application. That is,
SF
1
: 1
SF
2
: 3
SF
3
: 5
SF
4
: 8
SF
5
: 10
SF
6
: 13
SF
7
: 16
SF
8
: 19
SF
9
: 22
SF
10
: 25
SF
11
: 28
SF
12
: 32
SF
13
: 35
SF
14
: 39
On the other hand, for the brightness mode signal LC being indicative of mode 4 as shown in
FIG. 9
, the sustain pulse IP
Y
is applied in the light-emission sustain process Ic of each of the subfields SF
1
to SF
14
by the following number of times of application. That is,
SF
1
: 4
SF
2
: 12
SF
3
: 20
SF
4
: 32
SF
5
: 40
SF
6
: 52
SF
7
: 64
SF
8
: 76
SF
9
: 88
SF
10
: 100
SF
11
: 112
SF
12
: 128
SF
13
: 140
SF
14
: 156
In this case, the sustain pulse IP
Y
and sustain pulse IP
X
are applied alternately to avoid overlapping each other.
According to the aforementioned light-emission sustain process Ic, only the display cells in which wall charges remain or in the “light-emitting cell” state perform the sustain discharge each time the aforementioned sustain pulses IP
x
, IP
x
are applied thereto, sustaining the light-emitting state involved in the sustain discharge by the aforementioned number of times (period).
Then, in the last subfield SF
14
, in the order in which the sustain pulse IP
Y
has been applied for the aforementioned number of times of application, the erasing pulse EP having a negative voltage as shown in
FIG. 19
is successively applied to the row electrodes Y
1
to Y
n
(erase process E).
The application of such an erasing pulse EP causes each display cell to be erased by discharge on one display line after another and thereby all wall charges remaining in each display cell will dissipate.
As described above, the plasma display device shown in
FIG. 5
executes the reset process RJ to reset all display cells to the “light-emitting cell” state only in the head subfield SF
1
. Then, in each of the subfields SF
1
to SF
14
, performed are the data write process Wc for changing selectively each display cell to the “non-light-emitting cell” state and the light-emission sustain process Ic for allowing only the display cells in the “light-emitting cell” state to emit light repeatedly.
According to such a drive method, only the display cells that are sustained to the “light-emitting cell” state in the data write process Wc of each of the subfields repeat light emission involved in the sustain discharge for the number of times assigned to the subfield. At this time, whether a display cell changes to the “non-light-emitting cell” state in the data write process Wc of each of the subfields SF
1
to SF
14
depends on the logic level of each of the first to fourteenth bit of the cell drive data GD shown in FIG.
17
.
That is, with the data bit of the cell drive data GD being at logic level “1”, the selective erase discharge is generated in the data write process Wc of the subfield SF (shown in a black circle in
FIG. 17
) corresponding to the bit digit, thereby causing the display cell to change to the “non-light-emitting cell” state. Incidentally, such a discharge for allowing wall charges to be built in a display cell and thereby the display cell to change to the “light-emitting-cell” state is executed only in the reset process RJ of the head subfield SF
1
. Thus, once having changed to the “non-light-emitting cell” state by the aforementioned selective erase discharge, the display cell is sustained at the “non-light-emitting cell” state until the aforementioned reset process RJ is executed again.
On the other hand, with the data bit of the cell drive data GD being at a logic level of “0”, the aforementioned erase discharge is not generated in the data write process Wc of the subfield SF corresponding to the bit digit. Thus, this causes the display cell to be sustained at the state initialized by the reset process RJ or the “light-emitting-cell” state. Thus, light emission involved in the sustain discharge is continually performed in the light-emission sustain process Ic of the subfields SF (shown in white circle in
FIG. 17
) that are present until the aforementioned selective erase discharge is generated in one field period.
Then, various halftone levels of brightness are expressed in a stepwise manner based on the sum of the number of times of light emission that is executed in the light-emission sustain process Ic of each of the subfields SF
1
to SF
14
. At this time, according to the drive method that employs the cell drive data GD of 14 bits having 15 bit patterns as shown in
FIG. 17
, it is made possible to express halftone levels of brightness of 15 types or 15 levels of gray scale, each pattern having the following brightness ratio of light emission. That is, {0, 1, 4, 9, 17, 27, 40, 56, 75, 97, 122, 150, 182, 217, 255}.
Incidentally, the aforementioned display data PD is available for expressing 256 levels of gray scale with 8 bits. In this regard, to implement display of halftone brightness, nearly equal to the 256 levels of gray scale, also by the drive of 16 levels of gray scale as described above, the aforementioned multi-level gray scale processing circuit
33
performs the multi-gray-scale processing such as the error diffusion and dither processing.
Incidentally, according to the drive that employs the cell drive data GD shown in
FIG. 17
, during the display period in one field, there exist the steady state of light emission (shown in white circles in
FIG. 17
) in which the display cell is held at the “light-emitting cell” state and the steady state of no light emission in which the display cell is held at the “non-light-emitting cell” state. In addition, during the display period in one field, the display cell changes once or less from the aforementioned steady state of light emission to the steady state of no light emission, and a display cell that has changed to the steady state of no light emission will never restore to the “light-emitting” state. That is, during one field period, no light emission pattern is adapted to invert between the aforementioned steady state of light emission and the steady state of no light emission.
Thus, in one display screen, upon viewing the screen from one region to another, it does not happen to successively view only the steady state of light emission (or steady state of no light emission) in both regions, thus preventing the occurrence of false contours.
Furthermore, according to the present invention, as shown in
FIGS. 18 and 19
, immediately after data has been written to the display cells on one display line, a sustain discharge is initiated which is responsible for sustaining light emission in the display cells on the display line. That is, after the scanning pulse SP for writing data to each of the display lines has been applied to row electrodes, the application of the sustain pulses IP is initiated to the row electrodes immediately in conjunction with the scanning pulse SP in order to generate the sustain discharge. That is, light emission is sustained in display lines immediately after the completion of writing data.
In the conventional drive method, the sustain light emission is executed simultaneously in all display cells after display data has been written to all display cells on the first to nth display lines. When compared with this conventional drive method, the method according to the present invention can save time spent for the series of aforementioned processes. Thus, it is made possible to increase the levels of gray scale by increasing the number of subfields by making use of the saved time. It is also made possible to improve brightness by increasing the number of times of light emission to be carried out in each light-emission sustain process.
Incidentally, in the aforementioned embodiments, such a case has been described in which what is called the selective erase address method is employed as a method for writing display data. This method allows wall charges to be built in advance in each display cell and then erased selectively in accordance with the display data, thereby writing the display data.
However, the present invention is also applicable to a case in which what is called the selective write address method is employed as a method for writing display data. The selective write address method allows wall charges to be built selectively in each display cell in accordance with the display data.
FIG. 20
is a view illustrating a light-emission drive format to be used in the drive control circuit
2
when such a selective write address method is employed. In addition,
FIG. 21
is a view showing a data conversion table to be used in the second data conversion circuit
34
when the selective write address method is employed, and a light-emission drive pattern based on the cell drive data GD and provided by the data conversion table.
First, in the reset process RJ with the selective write address method being employed, the reset discharge and the erase discharge are continuously generated, thereby causing the wall charges in all display cells to vanish and be thus reset to the “non-light-emitting cell” state. Then, in the data write process Wc with the selective write address method being employed, a discharge (selective write discharge) is generated only in the display cells to which the aforementioned scanning pulse SP and a high-voltage data pulse have been applied simultaneously. At this time, of all display cells, wall charges are built only in the display cells in which the aforementioned selective write discharge has been generated, thus causing the display cells to change to the “light-emitting cell” state. Incidentally, the operation in the light-emission sustain process Ic with the selective write address method being employed is the same as that of the case in which the selective erase address method is employed, and thus not repeatedly explained here.
Accordingly, with the selective write address method being employed, the display cells in which the selective write discharge has been generated in the data write process Wc of the subfields shown by the black circles of
FIG. 21
change to the “light-emitting cells” state. Those display cells sustain discharge continuously in each of the subfields shown by the black circles and each of the subfields (shown by the white circles) that are present subsequently to emit light along with the discharge. That is, like the case where the selective erase address method is employed, no light emission pattern is adapted to invert between the steady state of light emission and the steady state of no light emission during one field period, thus preventing the occurrence of false contours.
As described above, according to the drive method of the present invention, a display cell changes from the steady state of light emission to the steady state of no light emission or from the steady state of no light emission to the steady state of light emission once or less during the display period in one field. Furthermore, once having changed to the steady state of no light emission (or the steady state of light emission), a display cell would not restore to the light-emitting state (or the “non-light-emitting” state). Thus, upon viewing the screen from one region to another, it does not happen to successively view only the steady state of light emission (or the steady state of no light emission) in both regions, thus preventing the occurrence of false contours.
In addition, according to the drive method, it is sufficient to perform only once the reset discharge involving a light emission that has nothing to do with the display image during the display period in one field, thereby making it possible to improve the contrast of the display image.
Furthermore, the present invention is adapted to sustain light emission in the display cells on each display line immediately after data has been written to the display cell on one display line after another. The prior-art drive method is adapted to sustain light emission simultaneously in all display cells after display data has been written to all display cells. When compared with the prior-art drive method, the method according to the present invention can save time spent for each process. Thus, it is made possible to increase the levels of gray scale by increasing the number of subfields by making use of the saved time. It is also made possible to improve brightness by increasing the number of times of light emission to be carried out in each light-emission sustain process.
The present application is based on Japanese Patent Application No. 2000-205329 which is hereby incorported by reference.
Claims
- 1. A method for driving a plasma display panel in which a display period of one field of an input video signal is constitued by a plurality of subfields for a gray scale driving, the plasma display panel having a display cell acting as a pixel at each intersection of a plurality of row electrodes acting as a display line and a plurality of column electrodes each intersecting each of said row electrodes, comprising the steps of:executing a reset process, only in a head subfield during the display period of said one field, for initializing said display cell to a light-emitting cell state, in each of said subfields, executing a data write process for applying successively a scanning pulse for generating a selective erase discharge to each of said row electrodes in order to change selectively each of said display cells from said light-emitting cell state to a non-light-emitting cell state in accordance with said input video signal, and executing a light emission sustain process for applying a train of sustain pulses to each of the row electrodes immediately after said scanning pulse has been applied thereto, the train of sustain pulses generating a sustain discharge to allow only a display cell in said light-emitting cell state to emit light for the number of times corresponding to a weight of each of said subfields.
- 2. The method for driving a plasma display panel according to claim 1, wherein in said data write process, said scanning pulse is applied to said row electrode immediately after the last sustain pulse in said train of sustain pulses has been applied to said row electrode in said light emission sustain process of a subfield immediately before said subfield.
- 3. A method for driving a plasma display panel in which a display period of one field of an input video signal is constitued by a plurality of subfields for gray scale drive, the plasma display panel having a display cell acting as a pixel at each intersection of a plurality of row electrodes acting as a display line and a plurality of column electrodes each intersecting each of said row electrodes, comprising the steps of:executing a reset process, only in a head subfield during the display period of said one field, for initializing said display cell to a non-light-emitting cell state, in each of said subfields, executing a data write process for applying successively a scanning pulse for generating a selective write discharge to each of said row electrodes in order to change selectively each of said display cells from said non-light-emitting cell state to a light-emitting cell state in accordance with said input video signal, and executing a light emission sustain process for applying a train of sustain pulses to each of the row electrodes immediately after said scanning pulse has been applied thereto, the train of sustain pulses generating a sustain discharge to allow only a display cell in said light-emitting cell state to emit light for the number of times corresponding to a weight of each of said subfields.
- 4. The method for driving a plasma display panel according to claim 3, wherein in said data write process, said scanning pulse is applied to said row electrode immediately after the last sustain pulse in said train of sustain pulses has been applied to said row electrode in said light emission sustain process of a subfield immediately before said subfield.
Priority Claims (1)
Number |
Date |
Country |
Kind |
2000-205329 |
Jul 2000 |
JP |
|
US Referenced Citations (2)
Number |
Name |
Date |
Kind |
5818419 |
Tajima et al. |
Oct 1998 |
A |
6256002 |
Shinoda |
Jul 2001 |
B1 |