Patent Grant
7876047
1. Field of the Invention
The present invention relates to a plasma display panel. More particularly, the present invention relates to a plasma display panel that may improve discharge uniformity by varying a permittivity of a dielectric layer according to a size of a discharge gap.
2. Description of the Related Art
A plasma display panel may generally use vacuum ultraviolet (VUV) rays emitted from plasma generated by gas discharge so as to excite a phosphor material. The excited phosphor material may generate red (R), green (G), and blue (B) visible light beams, so that an image may be displayed.
In an AC type plasma display panel, address electrodes may be formed on a rear substrate. The address electrodes may be covered with a dielectric layer. Barrier ribs may respectively be arranged in a stripe pattern between the address electrodes on the dielectric layer. R, G, and B phosphor layers may be in the barrier ribs. A front substrate may face the rear substrate. Display electrodes constructed with pairs of sustain electrodes and scan electrodes may be on the front substrate in a direction crossing the address electrodes. The display electrodes may be covered with a dielectric layer and an MgO protective layer. Discharge cells may be at a portion where the address electrodes on the rear substrate cross the display electrodes on the front substrate. Millions or more of unit discharge cells may be arranged in the plasma display panel in a matrix pattern.
Memory characteristics may be used to drive the discharge cells of the plasma display panel. Specifically, in order for a discharge to occur between the sustain electrodes and the scan electrodes constituting the display electrodes, an electric potential difference over a predetermined voltage may be required. A threshold voltage thereof may be a firing voltage Vf. When a scan voltage and an address voltage are respectively supplied to the scan electrodes and the address electrodes, a discharge may initially occur to produce plasma in the discharge cells. Electrons and ions of the plasma may be transferred towards an electrode having an opposite polarity.
Each electrode of the plasma display panel may be coated with a dielectric layer. Most of transferred space charges may be accumulated on the dielectric layer having an opposite polarity. Therefore, a net space voltage between the scan electrodes and the address electrodes may become lower than an initially provided address voltage Va. As a result, a discharge may diminish, and an address discharge may disappear. In this case, the amount of electrons accumulated in the sustain electrodes may be relatively small, while the amount of ions accumulated in the scan electrodes may be relatively large. Charges accumulated on the dielectric layer covering the sustain electrodes and the scan electrodes may be wall charges Qw. A space voltage produced between the sustain electrodes and the scan electrodes by the wall charges Qw may be a wall voltage Vw.
When a discharge sustain voltage Vs is supplied to the sustain electrodes and the scan electrodes, if a sum voltage Vs+Vw of the discharge sustain voltage Vs and the wall voltage Vw is greater than the firing voltage Vf, a sustain discharge may occur in the discharge cells. As a result, a VUV ray may be generated to excite a corresponding phosphor layer. Accordingly, a visible light beam may be emitted through the transparent front substrate.
When the address discharge does not occur between the scan electrodes and the address electrodes (that is, when the address voltage Va is not provided), the wall charges Qw may not accumulate between the sustain electrodes and the scan electrodes. As a result, the wall voltage Vw may not exist between the sustain electrodes and the scan electrodes. In this case, only the discharge sustain voltage Vs supplied to the sustain electrodes and the scan electrodes may be produced in the discharge cells. Since the discharge sustain voltage Vs may be lower than the firing voltage Vf, a discharge may not occur in a gas space between the sustain electrodes and the scan electrodes.
In the plasma display panel driven in the aforementioned manner, a discharge gap may be formed between a transparent electrode of the sustain electrode and a transparent electrode of the scan electrode.
Referring to
The transparent electrodes may be formed by using various methods, e.g., an etching method. However, it may be difficult to form the transparent electrodes to have uniform sizes due to manufacturing errors. In this case, the transparent electrodes of the plasma display panel may have irregular sizes, and thus a discharge gap also may become irregular. As a result, there may be problems arising from a firing voltage becomes irregular.
The above information disclosed in this Background section is only for enhancement of understanding of the background of the invention and therefore it may contain information that does not form the prior art that is already known in this country to a person of ordinary skill in the art.
It is therefore a feature of an embodiment of the present invention to provide a plasma display apparatus having electrodes covered by a dielectric layer which substantially overcomes one or more of the problems due to the limitations and disadvantages of the related art.
At least one of the above and other features and advantages of the present invention may be realized by providing a plasma display panel, which may include a first substrate, a second substrate facing the first substrate, barrier ribs between the first and second substrates, the barrier ribs defining discharge cells, address electrodes corresponding to the discharge cells, the address electrode extending in a first direction, first and second electrodes which extend in a second direction crossing the first direction, the first electrodes and second electrodes being on any one of the first substrate or the second substrate corresponding to the discharge cells, the first electrodes and the second electrodes being spaced apart from each other to form discharge gaps having distances, and a dielectric layer covering the first and second electrodes, where the dielectric layer may have varying permittivities depending on the respective distances of the discharge gaps.
The discharge gap may have at least two different distances. The dielectric layer may have at least two permittivities. The discharge gap may include a first discharge gap having a first distance, and a second discharge gap having a second distance that is less than the first distance, where the permittivity of the dielectric layer corresponding to the first discharge gap may be higher than the permittivity of the dielectric layer corresponding to the second discharge gap. The first and second electrodes may include bus electrodes extending in the second direction at both edges of the discharge cells, and transparent electrodes protruding towards respective centers of the discharge cells in the first direction, where the discharge gaps may be formed between the transparent electrodes of the first electrodes and the transparent electrodes of the second electrodes.
The first substrate or the second substrate may be in a shape of a rectangle, and the distances of the discharge gaps and the permittivities of the dielectric layer may become larger from one long side of the rectangle to the other long side of the rectangle. The first substrate or the second substrate may be formed in a shape of a rectangle, and the distances of the discharge gaps and the permittivities of the dielectric layer may become larger from one short side of the rectangle to the other short side of the rectangle. The dielectric layer may be constructed with a sheet having at least two permittivities. The discharge gaps may include a first discharge gap having a first distance, and a second discharge gap having a second distance that is less than the first distance, where a thickness of the dielectric layer corresponding to the first discharge gap may be greater than a thickness of the dielectric layer corresponding to the second discharge gap. The discharge gaps may include a first discharge gap having a first distance, and a second discharge gap having a second distance that is less than the first distance, where the dielectric layer may be covered with a protective layer, and a partial pressure of the protective layer corresponding to the first discharge gap may be lower than a partial pressure of the protective layer corresponding to the second discharge gap.
At least one of the above and other features and advantages of the present invention may be realized by providing a method of manufacturing a plasma display panel, which may include facing a first substrate and a second substrate, forming barrier ribs between the first substrate and the second substrate, the barrier ribs defining discharge cells, extending address electrodes in a first direction to correspond to the discharge cells, extending first electrodes and second electrodes in a second direction crossing the first direction, the first electrodes and second electrodes being on any one of the first substrate and the second substrate corresponding to the discharge cells, the first electrodes and the second electrodes being spaced apart from each other to form discharge gaps having distances, and covering the first electrodes and the second electrodes with a dielectric layer, where the dielectric layer may have varying permittivities depending on respective distances of the discharge gaps.
The above and other features and advantages of the present invention will become more apparent to those of ordinary skill in the art by describing in detail exemplary embodiments thereof with reference to the attached drawings, in which:
Korean Patent Application No. 10-2006-0028288, filed on Mar. 29, 2006, in the Korean Intellectual Property Office, and entitled: “Plasma Display Panel,” is incorporated by reference herein in its entirety.
The present invention will now be described more fully hereinafter with reference to the accompanying drawings, in which exemplary embodiments of the invention are illustrated. The invention may, however, be embodied in different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the invention to those skilled in the art.
In the drawing figures, the dimensions of layers and regions may be exaggerated for clarity of illustration. It will also be understood that when a layer or element is referred to as being “on” another layer or substrate, it can be directly on the other layer or substrate, or intervening layers may also be present. Further, it will be understood that when a layer is referred to as being “under” another layer, it can be directly under, and one or more intervening layers may also be present. In addition, it will also be understood that when a layer is referred to as being “between” two layers, it can be the only layer between the two layers, or one or more intervening layers may also be present. Like reference numerals refer to like elements throughout.
Referring to
The barrier ribs 16 may be between the rear substrate 10 and the front substrate 20 to define multiple discharge cells 17. The discharge cells 17 may be filled with a discharge gas, e.g., a gas mixture containing neon (Ne) and xenon (Xe), so that vacuum ultraviolet (VUV) rays may be generated via a gas discharge. Each discharge cell 17 may include a phosphor layer 19 which absorbs the VUV rays to emit a visible light beam.
In order to form an image by the gas discharge, the plasma display panel may include address electrodes 11 disposed between the rear substrate 10 and the front substrate 20 and corresponding to the respective discharge cells 17. The plasma display panel may also include first electrodes 31 (hereinafter, referred to sustain electrodes) and second electrodes 32 (hereinafter, referred to scan electrodes).
The address electrodes 11 may be on the upper surface of the rear substrate 10 and may extend in a first direction (the y-axis direction of the figure) to sequentially correspond to the adjacent discharge cells 17. The address electrodes 11 may be parallel with each other and correspond to the adjacent discharge cells 17 in a second direction (the x-axis direction in the figure) crossing the first direction.
The address electrodes 11 may be covered with a dielectric layer 13 that may cover the upper surface of the rear substrate 10. The dielectric layer 13 may prevent the address electrodes 11 from being directly bombarded with positive ions or electrons during a discharge, thereby protecting the address electrodes 11 against damage. Further, the dielectric layer 13 may form and accumulate wall charges. The address electrodes 11 on the rear substrate 10 may not interfere when the visible beam is transmitted forward. Thus, the address electrodes 11 may be made of an opaque material, e.g., a metallic material having an excellent conductivity.
The barrier ribs 16 may be on the dielectric layer 13 of the rear substrate 10 so as to define the discharge cells 17. The barrier ribs 16 may include first barrier members 16a extending in the first direction and second barrier members 16b extending in the second direction, so as to form the discharge cells 17 in a matrix pattern.
If the barrier ribs 16 include only the first barrier members 16a extending in the first direction so as to be parallel to the second direction, the discharge cells 17 may be formed in a stripe pattern.
The phosphor layers 19 may be respectively formed in the discharge cells 17. In order to form the phosphor layers 19, a photoconductive phosphorous paste may be coated on lateral surfaces of the barrier ribs 16 and the surface of the dielectric layer 13. The photoconductive phosphorous paste may then undergo drying, light exposure, development, and annealing processes.
For the discharge cells 17 arranged in the first direction, the phosphor layers 19 may have the same color. On the other hand, for the discharge cells 17 repeatedly arranged in the second direction, red (R), green (G), and blue (B) phosphor layers 19 may be repeatedly formed.
The sustain electrodes 31 and the scan electrodes 32 may be on the lower surface of the front substrate 20 and may correspond to the respective discharge cells 17, thereby forming a surface discharge structure. The sustain electrodes 31 and the scan electrodes 32 may extend in the second direction crossing the first direction.
The sustain electrodes 31 and the scan electrodes 32 may cross the address electrodes 11, may face each other to correspond to the discharge cells 17, and may be covered with a dielectric layer 40. The dielectric layer 40 may protect the sustain electrodes 31 and the scan electrodes 32 against a gas discharge. Further, the dielectric layer 40 may form and accumulate wall charges during the discharge.
The dielectric layer 40 may be covered with a protective layer 23. The protective layer 23 may be made of a transparent material, e.g., MgO, which may protect the dielectric layer 40, thereby increasing a secondary electron emission coefficient during a discharge.
The sustain electrodes 31 and the scan electrodes 32 respectively may include transparent electrodes 31a and 32a generating a discharge, and bus electrodes 31b and 32b respectively supplying a voltage signal to the transparent electrodes 31a and 32a.
The transparent electrodes 31a and 32a may produce a surface discharge inside the discharge cells 17. In order to ensure good aperture ratios for the discharge cells 17, the transparent electrodes 31a and 32a may be made of a transparent material, e.g., indium tin oxide (ITO), indium zinc oxide (IZO), etc. The bus electrodes 31b and 32b may be made of a metal material having excellent conductivity so that high electric resistances of the transparent electrodes 31a and 32a may be compensated.
Referring to
The bus electrodes 31b and 32b may be respectively arranged on the transparent electrodes 31a and 32a and extend in the second direction from the edge portions of the discharge cells 17. When voltage signals are supplied to the bus electrodes 31b and 32b, the voltage signals may be respectively supplied to the transparent electrodes 31a and 32a connected to the bus electrodes 31b and 32b, respectively.
When the plasma display panel is driven, a reset discharge may occur during a rest period in response to a reset pulse supplied to the sustain electrodes 31. An address discharge may occur during an address period in response to a scan pulse supplied to the scan electrodes 32 and an address pulse supplied to the address electrodes 11. A sustain discharge may occur during a sustain period in response to a sustain pulse supplied to the sustain electrodes 31 and the scan electrodes 32.
The sustain electrodes 31 and the scan electrodes 32 may function as electrodes for providing the sustain pulse required for the sustain discharge. The scan electrodes 32 may function as electrodes for providing the reset pulse and the scan pulse. The address electrodes 11 may function as electrodes for providing the address pulse. The sustain electrodes 31, the scan electrodes 32, and the address electrodes 11 may function in a different manner according to a voltage waveform supplied to each electrode. Thus, these electrodes are not limited to the aforementioned functions.
In the plasma display panel, the discharge cells 17 to be turned on may be selected when the address discharge occurs due to an interaction between the address electrodes 11 and the scan electrodes 32. Further, the discharge cells 17 may be driven from those selected when the sustain discharge occurs due to an interaction between the sustain electrodes 31 and the scan electrodes 32. As a result, an image may be formed.
The permittivity of the dielectric layer 40 covering the sustain electrodes 31 and the scan electrodes 32 may vary depending on a size, i.e., distance, of the discharge gap G. For example, for a discharge gap G having a size of about 70 μm, about 75 μm, about 80 μm, and about 85 μm, the permittivity of the dielectric layer 40 may be about 12.3, about 12.8, about 13.3, and about 13.6, respectively. If the relationship is considered to be linear, multiplying the discharge gap by about 0.168 will yield the approximate permittivity.
Widening the distance of the discharge gap G may increase a firing voltage Vf. Narrowing the distance of the discharge gap G may lower the firing voltage Vf. Furthermore, lowering the permittivity of the dielectric layer 40 may raise the firing voltage Vf. Raising the permittivity of the dielectric layer 40 may lower the firing voltage Vf.
In the present invention, since the permittivity of the dielectric layer 40 may increase as the distance of the discharge gap G is widened, the raising of the firing voltage Vf caused by the increase of the distance of the discharge gap G, and the falling of the firing voltage Vf caused by the increase of the permittivity of the dielectric layer 40, may compensate each other.
Also, since the permittivity of the dielectric layer 40 may decrease as the distance of the discharge gap G is narrowed, the falling of the firing voltage Vf caused by the reduction of the discharge G and the raising of the firing voltage Vf caused by the reduction of the permittivity of the dielectric layer 40 may compensate each other.
According to the present invention, since the permittivity of the dielectric layer 40 may change along with the change of the discharge gap G, the firing voltage Vf may be uniformly maintained. As a result, the plasma display panel may have improved discharge uniformity.
The magnitude of the firing voltage Vf may be related to the thickness of the dielectric layer 40. When the thickness of the dielectric layer 40 is increased by about 1 μm, the firing voltage Vf may be increased by about 3V. Therefore, the firing voltage Vf may be uniformly maintained by controlling not only the permittivity of the dielectric layer 40, but also the thickness of the dielectric layer 40. That is, the firing voltage Vf may be high when the discharge gap G is wide. In this case, the firing voltage Vf may be decreased by reducing the thickness of the dielectric layer 40. As a result, the firing voltage Vf may be uniformly maintained. Of course, the same may be applied when the discharge gap G is narrow.
Increasing the partial pressure of the protective layer 23 covering the dielectric layer 40 may raise the firing voltage Vf. When the partial pressure is about 1.26×10−7 Torr, the firing voltage Vf may be about 248V. However, when the partial pressure is about 7.73×10−7 Torr, the firing voltage Vf may be about 256V, i.e., increased by about 8V. Moreover, if a grain size of the protective layer 23 is large, its partial pressure may be increased. Therefore, increasing the grain size may raise the firing voltage Vf. Accordingly, when the discharge gap G is wide, the firing voltage Vf may be high, and the firing voltage Vf may be uniformly maintained by using the protective layer 23 having a low partial pressure. On the contrary, when the discharge gap G is narrow, the same may be achieved in an opposite manner.
The discharge gaps G may be formed between the transparent electrodes 31a of the sustain electrodes 31 and the transparent electrodes 32a of the scan electrodes 32.
The transparent electrodes 31a and 32a may be formed in the respective discharge cells 17 to have two different sizes instead of having the same size. The transparent electrodes 31a and 32a may have different sizes for the respective discharge cells 17. Likewise, the permittivity of the dielectric layer 40 may be different in each discharge cell 17.
As described above, according to the present invention, in order to uniformly maintain the firing voltage Vf, the permittivity of the dielectric layer 40 may vary depending on the size of the discharge gap G.
Referring to
The transparent electrodes 131a and 132a forming the short gap SG may generate a sustain discharge at a low firing voltage Vf. The dielectric layer 40 having the low permittivity P1 may slightly reduce the firing voltage Vf.
Referring to
The transparent electrodes 231a and 232a forming the long gap LG may generate a sustain discharge at a high firing voltage Vf. Therefore, the dielectric layer 40 having high permittivity P2 may significantly reduce the firing voltage Vf.
Herein, the short gap SG, the long gap LG, the low permittivity P1, and the high permittivity P2 may be all relative values.
Referring to
Besides the rectangular sheet, the dielectric layer 40 may be constructed using a paste or other equivalents. In the present invention, an integral type sheet may be attached by using, e.g., a tape, etc.
The dielectric layer 40 may have a permittivity distribution in which the permittivity becomes higher from the first long side 21a to the second long side 22a. In this case, the discharge gap G has a pattern in which the discharge gap G may become wider from the first long side 21a where the short gap SG is formed to the second long side 22a where the long gap LG is formed.
Referring to
Referring to
When comparing
Exemplary embodiments of the present invention have been disclosed herein, and although specific terms are employed, they are used and are to be interpreted in a generic and descriptive sense only and not for purpose of limitation. Accordingly, it will be understood by those of ordinary skill in the art that various changes in form and details may be made without departing from the spirit and scope of the present invention as set forth in the following claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10-2006-0028288 | Mar 2006 | KR | national |
| Number | Name | Date | Kind |
|---|---|---|---|
| 6788004 | Aoki et al. | Sep 2004 | B1 |
| 7071621 | Namiki et al. | Jul 2006 | B1 |
| 20050280369 | Hashikawa | Dec 2005 | A1 |
| Number | Date | Country |
|---|---|---|
| 1 345 457 | Apr 2002 | CN |
| 2000-306515 | Nov 2000 | JP |
| 10-2002-0062003 | Jul 2002 | KR |
| 10-2005-0029073 | Mar 2005 | KR |
| Number | Date | Country | |
|---|---|---|---|
| 20070228966 A1 | Oct 2007 | US |
