The present invention relates to a display apparatus having thin film type electron emitting elements, for example, each constituted by an upper electrode, an electron acceleration layer and a lower electrode.
For example, JP-A-8-248921 discloses a display apparatus using a matrix type display panel where electron emitting elements serving as pixels are arrayed in a matrix. In JP-A-8-248921, surface conduction type electron emitting elements are used as the electron emitting elements. A plurality of electron emitting elements are arrayed in a matrix so as to be located in intersection portions between a plurality of row electrodes (scan lines) extending in a row direction (horizontal direction on screen) and a plurality of column electrodes (data lines) extending in a column direction (vertically on screen), so as to form a display panel. A scan signal (scan pulse) is applied to the scan lines so as to select electron emitting elements by row (in this sense, the scan signal will be also referred to as “selection signal”). At the same time, a driving signal based on a vide signal is supplied to electron emitting elements of the selected row so as to allow the electron emitting elements to emit electrons. The electrons are brought into collision against phosphors disposed oppositely to the electron emitting elements so that the phosphors emit light. The operation to select a scan line and the operation to supply a driving signal based on a video signal in sync with the selection operation are performed sequentially on all the scan lines by scan line. Thus, a video image of one frame (or one field) is formed. As the method for supplying a driving signal, for example, there has been known a method in which a driving signal is supplied to each scan line sequentially from the scan line on the top of a screen of the display panel toward the scan line at the bottom of the screen. Various electron emitting elements have been proposed as well as the aforementioned surface conduction type electron emitting elements. One of them is a thin film type electron emitting element. In the thin film type electron emitting element, for example, a thin film has a three-layer structure composed of an upper electrode, an insulating layer and a lower layer, and a predetermined voltage is applied between the upper electrode and the lower electrode so as to emit electrons into a vacuum from the surface of the upper electrode, as disclosed in Paragraph 0003 of JP-A-11-095716. The electron emitting element may be regarded as an electron emitting element having an upper electrode, a lower electrode and an electron acceleration layer disposed therebetween. Here, the insulating layer in JP-A-11-095716 corresponds to the electron acceleration layer.
Other examples of thin film type electron emitting elements include MIM (Metal-Insulator-Metal) type electron emitting elements using metal as upper and lower electrodes, MIS (Metal-Insulator-Semiconductor) type electron emitting elements using semiconductor as at least one of electrodes, electron emitting elements using a laminated film of insulator and semiconductor in place of the insulating layer, that is, having a four-layer structure of an upper electrode, an insulating layer, a semiconductor layer and a lower electrode as a whole, etc.
These thin film type electron emitting elements have the property of easily accumulating charges in the insulating layer or a layer taking the place of the insulating layer.
Therefore, the aforementioned JP-A-11-095716 discloses the following method for elongating the lives of thin film type electron emitting elements in a display apparatus using a matrix type display panel where the electron emitting elements serving as pixels are arrayed in a matrix. That is, a signal (hereinafter referred to as “reverse-polarity signal”) whose polarity is reverse to the polarity of a scan signal (scan pulse) for applying a voltage in a direction (polarity) to allow a scan line to emit electrons is applied, for example, in a vertical non-display interval (also referred to as “vertical blanking interval”, and hereinafter often referred to as “non-display interval” simply) so as to prevent trapped electrons from being accumulated into an impurity level or a defect level in each insulating layer and reduce the deterioration of each electron emitting element. Thus, the life of the electron emitting element can be elongated.
According to the aforementioned technique disclosed in JP-A-11-095716, a reverse bias voltage is applied to each electron emitting element of the display apparatus in order to prevent charges from being accumulated in the insulating layer (or a layer taking the place of the insulating layer). There is, however, no consideration about the fact that a reverse bias voltage applied to one electron emitting element differs from that applied to another electron emitting element due to the resistance of the scan line.
The present invention was developed in consideration of the aforementioned problem. An object of the invention is to provide a display apparatus in which the life of the display screen can be elongated.
In order to attain the object, a display apparatus according to the invention includes a plurality of scan lines, a scan line driving circuit connected to at least left or right ends of the plurality of scan lines so as to apply a scan voltage to the plurality of scan lines, a plurality of data lines, a data line driving circuit connected to the plurality of data lines so as to apply a driving voltage to the plurality of data lines in accordance with an inputted video signal, electron emitting elements connected to intersection portions between the plurality of scan lines and the plurality of data lines respectively so as to emit electrons in accordance with a potential difference between the scan voltage and the driving voltage, and a control module, wherein the control module controls the scan line driving circuit and/or the data line driving circuit so as to apply a reverse-polarity voltage to the electron emitting elements in accordance with the electron emitting elements, the reverse-polarity voltage having reverse polarity to the voltage applied to the electron emitting elements. With this configuration, the reverse-polarity voltage can be applied all over the screen.
These and other features, objects and advantages of the present invention will become more apparent from the following description when taken in conjunction with the accompanying drawings wherein:
Several embodiments of the present invention will be described below with reference to the drawings. Constituents having similar functions are referenced correspondingly among the drawings, and in order to avoid redundancy, parts described once will not be. described repeatedly.
Taking into consideration the fact that a reverse bias voltage applied to one electron emitting element differs from that applied to another electron emitting element due to the resistance of a scan line, this embodiment is to control the reverse bias voltage applied to each electron emitting element. To this end, first, description will be made on the influence of the resistance of the scan line with reference to
As shown in
First, description will be made on the display panel 1, the scan drivers 2 and 3 and the data drivers 4 and 5 serving as driving circuits of the display panel 1, and the high voltage generating circuit 6.
The display panel 1 is a video display panel based on a passive matrix system. The display panel 1 has a back substrate (not shown) and a front substrate (not shown) opposed to each other. On the back substrate, a plurality of data lines 32 and 33 extending in a column direction (Y-direction which is a vertical direction of the screen) are arrayed in a row direction (X-direction which is a horizontal direction of the screen) and a plurality of scan lines 31 extending in the row direction (X-direction) are arrayed in the column direction (Y-direction). Thin film type electron emitting elements (“thin film type” will be omitted as long as misunderstanding will not be caused) la are disposed in a matrix in intersection portions between the data lines and the scan lines respectively. On the front substrate, phosphors (not shown) are disposed oppositely to the electron emitting elements respectively.
The scan drivers 2 and 3 are connected to each scan line 31 of the display panel 1. The reason why the scan drivers 2 and 3 are disposed on the left and right sides of the display panel 1 is to reduce the luminance gradient caused by a voltage drop caused by the resistance belonging to the scan lines. In this system, identical scan signals are supplied to one and the same scan line 31 from its left and right sides. In this manner, this embodiment is arranged using two scan drivers, that is, the scan drivers 2 and 3. To simplify the system, the scan lines 31 may be driven by one of the left and right scan drivers. The scan drivers 2 and 3 apply selection signals to the scan lines sequentially from one scan line to the next so as to select a plurality of electron emitting elements 1a by row (one or two rows). Thus, the scan drivers 2 and 3 perform a selection operation (scan) over the rows in turn. The selection operation of the scan drivers 2 and 3 is executed based on a scan control signal Sscan which is a timing signal from the timing controller 7.
In
The data drivers 4 and 5 supply driving signals to a plurality of electron emitting elements of the selected row through the data lines 32 and 33 in accordance with video data from the timing controller 7, respectively. The data drivers 4 and 5 hold data of one row of the display panel 1, that is, video data of one line from the timing controller 7 for one horizontal interval based on a timing signal from the timing controller 7. After one horizontal interval, the data are rewritten by data for the next row. Driving signals are supplied from the data driver 4 in a display interval of the upper region of the screen, and from the data driver 5 in a display interval of the lower region of the screen.
The high voltage generating circuit 6 supplies a high voltage to the front substrate through an anode line 34 of the display panel 1. On the front substrate, phosphors are disposed correspondingly to the electron emitting elements respectively.
The operation of the embodiment will be described below.
A selection signal (scan signal) outputted from the scan drivers 2 and 3 is applied to the scan lines 31. In a plurality of electron emitting elements 1a on one row (line) selected by the selection signal (scan signal), electrons are released. The amount of the electrons depends on the potential difference between the selection signal (scan signal) and a driving signal applied to the data lines 32 (33) by the data driver 4 (5). The voltage level of the selection signal applied for selecting the scan line 31 is constant regardless of the layout of the electron emitting elements. Thus, the amount of electrons released from each electron emitting element changes in accordance with the voltage level of the driving signal. That is, the amount of the electrons depends on the voltage level of a video signal on which the driving signal is based. On the other hand, an acceleration voltage (e.g. 7 kV) from the high voltage generating circuit 6 is applied to the anode line 34 of the display panel 1. For this reason, the electrons released from the electron emitting elements 1a are accelerated toward the front substrate due to the acceleration voltage, and collide with the phosphors disposed on the front substrate of the display panel 1. The phosphors are excited by the collision of the accelerated electrons. Thus, the phosphors emit light. In this manner, an image of the selected horizontal line is displayed. Further, the scan drivers 2 and 3 select the next scan line, and perform similar operation. Finally, all the scan lines of one screen are selected so that an image of one frame can be formed on the display screen of the display panel 1.
Next, description will be made on the operation of the video signal processing circuit 9, the compensation data generating circuit 8 and the timing controller 7.
A video signal inputted to a video signal terminal 10 is first inputted to the video signal processing circuit 9. The video signal processing circuit 9 performs format conversion upon the inputted video signal as to the number of pixels of the signal, the frequencies of sync signals, etc. so that the video signal can be displayed on the display panel 1 where the electron emitting elements are disposed in a matrix.
The video signal having a format converted by the video signal processing circuit 9 is inputted to the timing controller 7. The timing controller 7 generates a scan control signal Sscan based on the sync signals (horizontal sync signal and vertical sync signal) of the inputted video signal. The scan control signal Sscan is a timing signal for controlling the scan drivers 2 and 3 so that the scan drivers 2 and 3 can select and scan one of the scan lines of the display panel 1 each time. The scan control signal Sscan is outputted to the scan drivers 2 and 3. Thus, the scan drivers 2 and 3 sort the data of the inputted video signal in sync with the timing signal, and output the sorted data signal to the data drivers 4 and 5. Due to this operation, video data can be displayed on the display panel 1 in sync with the inputted video signal. In this embodiment, the screen of the display panel 1 is divided into two, i.e. the upper region and the lower region. For this reason, pixel data have to be sorted to display on the screen divided into the upper and lower regions. This sorting is performed by the timing controller 7.
The timing controller 7 also has a reverse-polarity signal generating function to generate a reverse-polarity signal. The reverse-polarity signal serves to apply a reverse bias voltage to electron emitting elements in order to prevent charges from being accumulated in the insulating layer (or a layer taking the place of the insulating layer) forming each thin film type electron emitting element.
In this embodiment, the timing controller 7 generates a signal (scan control signal Sscan) having a predetermined voltage value to be applied to each scan line of the display panel 1 in a display interval, and a signal (reverse-polarity signal) having a predetermined voltage value to be applied to all the scan lines in a vertical non-display interval. In the display interval, the scan drivers 2 and 3 switch the scan control signal Sscan from the timing controller 7 so as to apply the scan control signal Sscan to each scan line sequentially. In the vertical non-display interval, the scan drivers 2 and 3 apply the reverse-polarity signal to all the scan lines. It is a matter of course that a signal from the timing controller 7 may be controlled to a predetermined voltage value by the scan drivers 2 and 3.
Next, description will be made on the detailed operation of the timing controller 7 according to the present invention. As described previously, the timing controller 7 generates the scan control signal Sscan having a predetermined voltage value with polarity to allow electron emitting elements to emit electrons, so that the scan drivers 2 and 3 can select and scan the electron emitting elements in a row (line) each time in the display interval. The scan drivers 2 and 3 switch the scan control signal Sscan so as to apply the scan control signal Sscan to each scan line sequentially as a selection signal (scan signal). Thus, the scan drivers 2 and 3 select a row (line). The timing controller 7 generates a reverse-polarity signal such that the driving voltage for the electron emitting elements has a reverse direction to its regular direction in the vertical non-display interval. When the scan drivers 2 and 3 receive the input of the reverse-polarity signal, the scan drivers 2 and 3 apply the reverse-polarity signal to all the scan lines simultaneously. Since the driving voltage applied to the electron emitting elements has a reverse direction to its regular direction, electrons accumulated in the electron emitting elements are released. Thus, the electron emitting elements are prevented from accumulating electrons continuously, so that the lives of the electron emitting elements can be elongated.
The compensation data generating circuit 8 is a circuit which generates a data line voltage for compensating the voltage applied to each electron emitting element so as to solve a problem that the voltage of the reverse-polarity signal drops down in each electron emitting element terminal due to the resistance of the scan line. As shown in
When the electron emitting elements are driven by the scan drivers 2 and 3 as in this embodiment, there occurs a maximum voltage drop in the center portion of the screen. When the electron emitting elements are driven by one scan driver 2 or 3, there occurs a maximum voltage drop in an end portion of the screen on the opposite side of an end portion where the scan driver supplies a scan line signal. Also in this case, the compensation data generating circuit 8 generates a compensation value corresponding to a horizontal position of the screen corresponding to each data line.
The compensation data generating circuit 8 generates compensation data for the data lines, and outputs the compensation data to the timing controller 7 in a period designated by a vertical blanking interval gate 81. The timing controller 7 sends the value of the output of the compensation data generating circuit 8 to the data drivers 4 and 5 in a vertical blanking interval. The data drivers 4 and 5 then output compensation data in accordance with a display position in the vertical blanking interval. On the other hand, the scan drivers 2 and 3 output a reverse-polarity signal in this interval. A differential voltage between the reverse-polarity signal outputted from the scan drivers 2 and 3 and the compensation data outputted from the data drivers 4 and 5 is applied to each electron emitting element. Thus, a predetermined reverse-polarity voltage is applied to each electron emitting element in spite of the wiring resistance. It is therefore possible to improve the lives of the electron emitting elements uniformly all over the screen.
The operation of the compensation data generating circuit 8 will be described in detail with reference to
In
The electron emitting elements p11, p21 and p31 on the left end of the display screen are located just closely to the output of the scan driver 2. The reverse-polarity signal supplied to the electron emitting elements p11, p21 and p31 is hardly affected by the resistance of the scan lines. In this case, it is hardly necessary to compensate the voltage drop of the reverse-polarity signal caused by the resistance of the scan lines. Therefore, compensation in the period of the reverse-polarity signal does not have to be performed upon the electron emitting elements p11, p21 and p31. The waveform of the data signal d1 shows the waveform in this case. In the non-display interval of the data signal d1, the compensation value of the reverse-polarity signal is zero as described above. In the same manner, the electron emitting elements p13, p23 and p33 on the right end of the display screen are located just closely to the output of the scan driver 3 so that the reverse-polarity signal supplied to the electron emitting elements p13, p23 and p33 is hardly affected by the resistance of the scan lines. In this case, it is hardly necessary to compensate the voltage drop of the reverse-polarity signal caused by the resistance of the scan lines. Therefore, compensation in the period of the reverse-polarity signal does not have to be performed upon the electron emitting elements p13, p23 and p33. The waveform of the data signal d3 shows the waveform in this case. In the non-display interval of the data signal d3, the compensation value of the reverse-polarity signal is zero as described above.
On the other hand, the electron emitting elements p12, p22 and p32 located in the center of the display screen are disposed at distances from the scan drivers 2 and 3. The reverse-polarity signal supplied to the electron emitting elements p12, p22 and p32 is greatly affected by the resistance of the scan lines. In this case, it is therefore necessary to compensate the voltage drop of the reverse-polarity signal caused by the resistance of the scan lines. Compensation in the period of the reverse-polarity signal is performed upon the electron emitting elements p12, p22 and p32. The compensation value may be determined in accordance with the resistance value of the scan lines. The waveform of the data signal d2 shows the waveform in this case. In the non-display interval of the data signal d2, the compensation value of the reverse-polarity signal is set as described above. The value is vc.
It is a matter of course that the vertical non-display interval TVOFF and the reverse-polarity signal period TER are set to have optimum values in accordance with a pulse amplitude value VA of the reverse-polarity signal. For example, a table of vertical non-display intervals TVOFF and reverse-polarity signal periods TER corresponding to a plurality of pulse amplitude values of the reverse-polarity signal is prepared in advance. When a pulse amplitude value of the reverse-polarity signal is designated by a not-shown input unit or on a menu screen, an optimum vertical non-display interval TVOFF and an optimum reverse-polarity signal period TER can be set.
According to this embodiment, as described above, the voltage of the reverse-polarity pulse signal to be supplied can be made substantially uniform over the electron emitting elements. It is therefore possible to cancel the nonuniformity of deterioration over the electron emitting elements caused by the resistance of the scan lines. In addition, charges accumulated in the insulating layer of each electron emitting element can be released sufficiently regardless of the position where the electron emitting element is arranged. It is therefore possible to elongate the lives of the electron emitting elements uniformly over the display screen.
Next, a second embodiment for compensation of the value of a reverse-polarity signal will be described with reference to
In
In
On the other hand, description will be made on the data signals. The electron emitting elements p11, p21 and p31 on the left end of the display screen are located just closely to the output of the scan driver 2. The reverse-polarity signal supplied to the electron emitting elements p11, p21 and p31 is hardly affected by the resistance of the scan lines. For the electron emitting elements p11, p21 and p31, therefore, it is not necessary to compensate the voltage drop of the reverse-polarity signal caused by the resistance of the scan lines. Therefore, compensation in the period of the reverse-voltage signal may be low for the electron emitting elements p11, p21 and p31. The waveform of the data signal d1 shows the waveform in this case. In the non-display interval of the data signal d1, the compensation value of the reverse-polarity signal is vr1. In the same manner, the electron emitting elements p13, p23 and p33 on the right end of the display screen are located just closely to the output of the scan driver 3 so that the reverse-polarity signal supplied to the electron emitting elements p13, p23 and p33 is hardly affected by the resistance of the scan lines. In this case, therefore, it is hardly necessary to compensate the voltage drop of the reverse-polarity signal caused by the resistance of the scan lines. Therefore, compensation in the period of the reverse-voltage signal may be low for the electron emitting elements p13, p23 and p33. The waveform of the data signal d3 shows the waveform in this case. In the non-display interval of the data signal d3, the compensation value of the reverse-polarity signal is vr3.
On the other hand, the electron emitting elements p12, p22 and p32 located in the center of the display screen are disposed at distances from the scan drivers 2 and 3. The reverse-polarity signal supplied to the electron emitting elements p12, p22 and p32 is greatly affected by the resistance of the scan lines. In this case, it is therefore necessary to greatly compensate the voltage drop of the reverse-polarity signal caused by the resistance of the scan lines. Compensation in the period of the reverse-voltage signal is performed upon the electron emitting elements p12, p22 and p32. The compensation value may be determined in accordance with the resistance value of the scan lines. The waveform of the data signal d2 shows the waveform in this case. In the non-display interval of the data signal d2, the compensation value of the reverse-polarity signal is set as described above. The value is vr2.
Next, a third embodiment for compensation of the value of a reverse-polarity signal will be described with reference to
In
Further another embodiment will be described with reference to
In
Further another embodiment will be described with reference to
In
While we have shown and described several embodiments in accordance with our invention, it should be understood that disclosed embodiments are susceptible of changes and modifications without departing from the scope of the invention. Therefor, we do not intend to be bound by the details shown and described herein but intend to cover all such changes and modifications a fall within the ambit of the appended claims.
Number | Date | Country | Kind |
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2005-313690 | Oct 2005 | JP | national |