Energy recovery circuit for 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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C345S211000, C315S169300

Reexamination Certificate

active

06657604

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates in general to a technology for plasma display panel, and more particularly to an energy recovery circuit for a plasma display panel.
2. Description of the Related Art
A PDP device, which displays images by accumulating charges by electrode discharge, is an attention-getting flat display since it can have a large screen size display a full-color image.
FIG. 1
is a cross-sectional diagram of a conventional PDP cell, in which the PDP is triple-electrode type. As shown in the drawing, the PDP is basically constituted by two glass substrates
1
and
7
. Inert gas such as Ne, Xe is filled in the cavity formed between the glass substrates
1
and
7
. Two electrodes including a sustain electrode X and a sustain electrode Yi are disposed parallel to each other on the glass substrate
1
. A dielectric layer
3
and a protective film
5
are formed covering the sustain electrode X and the sustain electrode Yi. Address electrodes Ai, which are perpendicular to the sustain electrode X and the sustain electrode Yi, are disposed on the glass substrate
7
. Partition wall
8
is used to isolate each PDP cell. Fluorescent material is placed between the partition walls to luminesce during the discharge process.
FIG. 2
is a block diagram of a conventional PDP device. As shown in the drawing, the PDP
100
is driven by the sustain electrodes Y
1
~Yn and sustain electrode X parallel to each other and the address electrodes A
1
~Am across thereon. The reference numeral
10
indicates the display unit of the PDP
100
. Partition wall
8
is used to isolate each display unit
10
.
Besides the PDP
100
, the PDP device includes the control circuit
110
, the Y scan driver
112
, the X common driver
114
and the address driver
116
. The control circuit
110
can generate the timing information necessary for every driver according to the external clock signal CLOCK, the video data signal DATA, the vertical synchronous signal VSYNC and the horizontal synchronous signal HSYNC. The clock signal CLOCK represents the data-transmitting clock. The video data signal DATA represents the display data. The vertical synchronous signal VSYNC and the horizontal synchronous signal HSYNC are used to define the timing of a single frame and a single scanning line. The control circuit
110
generates every clock and data to be displayed, which are sent to the corresponding drivers to generate the signals needed to drive the electrodes.
FIG. 3
is diagram of driving the PDP to display a frame in the prior art. A frame is normally divided into several sub-fields. For instance, the frame of
FIG. 3
is divided into 8 sub-fields SF
1
~SF
8
. Each sub-field is used to display the corresponding gray scales on all scanning lines. For example, 8 sub-fields can be used when 256 levels of gray scales corresponding to 8 bits are to be displayed. Each sub-field is constituted by three operating periods, i.e., the reset periods R
1
~R
8
, the address periods A
1
~A
8
and the sustain periods S
1
~S
8
. The residual charge left from the last field display is cleaned in the reset period. The wall charge is accumulated in the display cell through address discharge in the address period. The accumulated wall charge is sustained to maintain the display status in the sustain period. All display units on the PDP are simultaneously processed in the reset period R
1
~R
8
and the sustain period S
1
~S
8
. However, address operation is sequentially performed for the display units on the sustain electrodes Y
1
~Yn in the address periods A
1
~A
8
.
FIG. 4
is the timing diagram of the control signals of the sustain electrodes X and Yi on a single sub-field of
FIG. 3
such as SF
1
. After finishing the reset operation of all scanning lines, the address period starts. In the address period, i.e., A
1
, the X common driver
114
controls the sustain electrode X to output the voltage Vs. The scanning lines corresponding to the electrodes Y
1
, Y
2
, Y
3
, . . . , Yn sequentially output the address pulses AP including display data to the address electrodes A
1
, A
2
, . . . , Am through the address driver
116
. Therefore, a transient discharge occurs on the display unit
10
corresponding to the data to be displayed, and the wall charge is accumulated in the display unit
10
. After processing all of the scanning lines, the “data to be displayed” can be stored in the corresponding display unit
10
in the form of accumulated wall charge.
After finishing the address period, the sustain period (i.e., S
1
) starts. In the sustain period, the Y scan driver
112
and the X common driver
114
alternately send the sustain pulses to all of the sustain electrodes Yi and the common sustain electrode X. As shown in
FIG. 4
, a sustain pulse Xsus having a voltage level Vs is sent to the sustain electrode X. This action will be repeated during the sustain period of the sub-field. Moreover, this action involves all of the display units
10
, but only the display units
10
that have accumulated wall charges through the address discharge during the address period keep luminescing during the sustain period.
Accordingly, the X common driver
114
periodically generates a sustain pulse Xsus during the sustain period. Normally, the sustain pulse Xsus is a signal of high frequency and high voltage, thus causing a considerable power consumption. There are many energy-recovery structures designed for this driving circuit currently.
FIG. 5
is a circuit diagram of a prior-art energy-recovery structure for PDP driving circuit. As shown in the drawing, Cp indicates the capacitor-like load corresponding to the display units
10
of the PDP
100
. The capacitor Cp has one end connected to the Y scan driver
112
. The X common driver
114
includes the MOS transistors T
1
, T
2
, T
3
and T
4
, the inductance element
61
and the capacitor C
3
. The capacitor C
3
is an element storing and releasing energy. The transistors T
3
and T
4
are alternatively opened to raise up or pull down the voltage of the sustain electrode X. The operation is briefly described below.
When the voltage of the sustain electrode X changes from 0 volts to Vs, i.e., the rising edge of the sustain pulse Xsus, the voltage of the capacitor C
3
maintains at Vs/2, and the voltage of the coil is 0 volts. At this time, the transistor T
3
is turned on, and the voltage Vs/2 of the capacitor is applied to one end of the coil
61
. Thus a current occurs on the coil
61
and the voltage of the sustain electrode X on the other end of the coil rises up. Since a counter electromotive force exists on the coil
61
, the voltage of the sustain electrode X, i.e., the other end of the coil, can theoretically be raised to Vs. However, the voltage cannot rise up to Vs in practice due to loss. The voltage of the sustain electrode X is raised to Vs by turning the transistor T
1
on if the voltage of the sustain electrode X is a little lower than Vs. That the voltage of the sustain electrode X suddenly rises to Vs will cause the problem of electromagnetic interference.
On the other hand, when the voltage of the sustain electrode X changes from Vs to 0 volts, i.e., the falling edge of the sustain pulse Xsus, the voltage of the coil is Vs. At this time, the transistor T
4
is turned on, and the voltage Vs/2 of the capacitor C
3
is applied to one end of the coil
61
. Thus a reverse current occurs on the coil
61
, and the voltage of the sustain electrode X on the other end of the coil
61
falls down to 0 volts. However, the voltage of the sustain electrode X does not fall to 0 volts in practice due to loss. The voltage of the sustain electrode X can fall down to 0 volts by turning the transistor T
2
on if the voltage of the sustain electrode X is a little higher than 0 volts. That the voltage of the sustain electrode X suddenly falls to 0 volts will also cause the problem of electromagnetic interference.
In order to improve on the drawbacks for the above energy-recovery structure, U.S. Pat. Nos. 5,438,290 and 5,828,353 disclose us

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