This application claims priority to and the benefit of Korean Patent Application No. 10-2004-0038164, filed on May 28, 2004, which is hereby incorporated by reference for all purposes as if fully set forth herein.
1. Field of the Invention
The present invention relates to a plasma display panel (PDP) that displays images.
2. Discussion of the Background
Generally, a PDP displays images by gas discharge. More specifically, the gas discharge creates plasma, which emits vacuum ultraviolet (VUV) rays that excite phosphors, and the phosphors emit red (R), green (G), and blue (B) visible rays to form an image. The PDP's screen may be larger than 60 inches, and it may be formed 10 cm or less thick. Additionally, since the PDP is a self-emissive display device, it may have high color reproducibility and no distortion caused by viewing angle. Further, since the PDP may be manufactured easier than a liquid crystal display (LCD) panel, it may have higher productivity and lower manufacturing costs. Thus, the PDP has drawn attention as a next-generation flat panel display.
Generally, in an alternating current (AC) PDP, address electrodes are formed on a rear substrate in one direction, and a dielectric layer is formed covering the address electrodes. Then, strip-shaped barrier ribs are formed on the dielectric layer in parallel with, and between, the address electrodes, and red (R), green (G), and blue (B) phosphor layers are formed between the barrier ribs, respectively.
Further, display electrode pairs, such as a sustain electrode and a scan electrode, are formed on a surface of the front substrate facing the rear substrate and in a direction substantially perpendicular to the address electrodes. Each display electrode may include a transparent electrode for generating a surface discharge and a bus electrode for applying a discharge voltage. A dielectric layer covers the display electrodes and a protective layer, which may be made of magnesium oxide (MgO), covers the dielectric layer.
A discharge cell is formed at each intersection of an address electrode and a display electrode pair.
In this way, millions of discharge cells may be arranged in a matrix in the PDP, and a memory characteristic may be used to simultaneously drive the discharge cells in the AC PDP.
More specifically, a potential difference, which is referred to as a firing voltage Vf, higher than a predetermined voltage is needed to generate a discharge between the sustain electrode and the scan electrode of a display electrode pair. In this case, when an address voltage is applied between the scan electrode and the address electrode, an address discharge starts, thereby generating plasma in the discharge cells. Then, electrons and ions in the plasma move to electrodes having different polarities, respectively, which causes the flow of current.
As noted above, since dielectric layers are formed on the AC PDP's electrodes, most of the space charges accumulate on the dielectric layers having different polarities. Therefore, a net space potential between the scan electrode and the address electrode may become lower than an address voltage Va that is first applied, which causes a low discharge voltage. As a result, the address discharge stops. At that time, a relatively small number of electrons may be accumulated on the sustain electrode, and a relatively large number of ions may be accumulated on the scan electrode. The charges accumulated on the dielectric layer that covers the scan electrode and the sustain electrode are referred to as wall charges (Qw), and a space voltage formed between the scan electrode and the sustain electrode by these wall charges is referred to as a wall voltage (Vw).
When applying a predetermined voltage Vs (discharge sustain voltage) between the sustain electrode and the scan electrode, if a voltage obtained by adding the discharge sustain voltage Vs and the wall voltage Vw (Vs+Vw) is higher than the firing voltage Vf, a discharge occurs in the corresponding discharge cell. Then, the generated VUV rays excite the phosphor layers, and visible rays are emitted from the transparent front substrate to display images.
However, in such a PDP, in order to improve brightness, the amount of emitted secondary electrons may be increased when ions collide with each other in the discharge cells. Accordingly, various techniques using carbon nanotubes have been developed for this purpose.
The present invention provides a PDP and a method of manufacturing the same that may have improved brightness, low-voltage driving, and high efficiency by increasing the amount of emitted secondary electrons in discharge cells using a carbon nanotube.
Additional features of the invention will be set forth in the description which follows, and in part will be apparent from the description, or may be learned by practice of the invention.
The present invention discloses a PDP including a first substrate, a second substrate, barrier ribs formed between the first substrate and the second substrate to partition discharge cells, address electrodes formed corresponding to the discharge cells, respectively, display electrodes formed on the first substrate in a direction substantially perpendicular to the address electrodes, a dielectric layer that substantially covers the display electrodes, and a carbon nanotube layer formed in the dielectric layer.
The present invention also discloses a method of manufacturing a PDP including forming display electrodes on a first substrate, forming a first dielectric layer to cover the display electrodes, forming a carbon nanotube layer on the first dielectric layer, and forming a second dielectric layer to substantially cover the carbon nanotube layer.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory and are intended to provide further explanation of the invention as claimed.
The accompanying drawings, which are included to provide a further understanding of the invention and are incorporated in and constitute a part of this specification, illustrate embodiments of the invention and together with the description serve to explain the principles of the invention.
Hereinafter, exemplary embodiments of the invention will be described with reference to the accompanying drawings.
Referring to
Display electrodes 9 and 11 may be formed on the front substrate 1 and extending in the x-axis direction of
The barrier ribs 5 may be arranged parallel to each other at predetermined intervals between the front substrate 1 and the rear substrate 3, thereby partitioning the discharge cells 7R, 7G, and 7B required for plasma discharge. While
Accordingly, a closed partition structure may be utilized in which the discharge cells 7R, 7G, and 7B are independently partitioned by the barrier ribs 5 formed parallel to the address electrodes 13 and barrier ribs (not shown) formed in a direction (the x-axis direction of
The address electrodes 13 may be formed on the rear substrate 3, as shown in
The display electrodes 9 and 11 may be formed of a sustain electrode and a scan electrode 9 and 11 corresponding to both sides of each discharge cell 7R, 7G, and 7B. Additionally, as
Further, as
The transparent electrodes 9a and 11a may be formed in a strip type extending in a direction (the x-axis direction of
The bus electrodes 9b and 11b may compensate for the transparent electrodes' high resistance to enhance the electrical conductivity of the transparent electrodes 9a and 11a. Thus, the bus electrodes 9b and 11b may be made of a metallic material having high electrical conductivity, such as, for example, aluminum. The bus electrodes 9b and 11b may be respectively laminated on the transparent electrodes 9a and 11a to extend in the direction (the x-axis direction of
Further, the bus electrodes 9b and 11b may be made of an opaque material, and when the barrier ribs are formed in a closed structure, the bus electrodes may be arranged to correspond to the barrier ribs. Additionally, the bus electrodes 9b and 11b may be formed narrower than the barrier rib 5 so as to minimally shield visible rays emitted from the discharge cells 7R, 7G, and 7B.
A dielectric layer 17 may cover the display electrodes 9 and 11, and a protective layer 19, which may be an MgO layer, covers the dielectric layer 17, thereby forming a laminated structure that stores wall charges. The dielectric layer 17 may be made of a transparent dielectric material to improve the transmittance of visible rays. The protective layer 19 prevents the dielectric layer 17 from damage due to collision with ions, and it facilitates emission of secondary electrons during gas discharge.
The dielectric layer 17 will now be described with reference to
The pattern of the carbon nanotube layer 21 may be obtained by patterning the dielectric layer 17.
In this case, the dielectric layer 17 may include a first dielectric layer 17a and a second dielectric layer 17b, and the carbon nanotube layer 21 may be interposed therebetween. Hence, the first dielectric layer 17a may be formed on the display electrodes 9 and 11, and the carbon nanotube layer 21 may be formed on the first dielectric layer 17a. The second dielectric layer 17b may then be formed on the carbon nanotube layer 21 and patterned such that a portion of the carbon nanotube layer 21 is exposed. Accordingly, the carbon nanotube layer 21 may be formed covering the first dielectric layer 17a, and the second dielectric layer 17b having an opening pattern may be formed on the carbon nanotube layer 21.
Consequently, according to the pattern of the second dielectric layer 17b, the carbon nanotube layer 21 includes portions 21a that are covered with the second dielectric layer 17b and portions 21b that are exposed by the opening pattern of the second dielectric layer 17b. The exposed portions 21b may be formed so as to correspond to edge portions of the display electrodes 9 and 11 that are located closer to the center of the discharge cell 7G in order to increase the amount of emitted secondary electrons and to perform low-voltage driving. More specifically, the exposed portions 21b of the carbon nanotube layer 21 may correspond to edges of the transparent electrodes 9a and 11a.
Further, the first dielectric layer 17a may be formed about 10 to 20 μm thick. Then, the carbon nanotube layer 21 may be formed thereon, and the second dielectric layer 17b may be formed on the carbon nanotube layer 21. The second dielectric layer 17b may then be patterned. Here, the thickness of the dielectric layer 17 differs in the patterned portions and non-patterned portions, which may have the same effect as that obtained when the carbon nanotube layer 21 is patterned.
Since the portions 21b of the carbon nanotube layer 21 exposed by the opening pattern of the second dielectric layer 17b are not covered by the second dielectric layer 17b, the portions 21b may have carbon nanotubes that are more upright than that of the portions 21a that are covered with the second dielectric layer 17b. However, since the protective layer 19 may cover the exposed portions 21b, the uprightness of the carbon nanotube may not cause a problem. That is, the protective layer 19 covers the second dielectric layer 17b and the portions 21b of the carbon nanotube layer 21 exposed by the second dielectric layer 17b opening pattern.
Referring again to
Since the processes described above may be performed by a well-known method, a detailed description thereof will be omitted.
Further, since the transparent electrodes 9a and 11a and the bus electrodes 9b and 11b may be formed using a well-known method, a detailed description thereof will be omitted.
Hence, a process of patterning the carbon nanotube layer 21 on the dielectric layer 17 will be described herein.
Referring to
Then, the carbon nanotube layer 21 may be formed on the first dielectric layer 17a (see
The second dielectric layer 17b may then be formed on the carbon nanotube layer 21 (see
For example, the second dielectric layer 17b may be patterned by a printing method using a screen mask 23 or by an exposure/development method. When using the exposure/development method, the second dielectric layer 17b or the dielectric layer 17 may be made of a photosensitive dielectric material.
After patterning the second dielectric layer 17b, a protective layer 19, which may be made of MgO, for example, may be formed thereon (see
As described above, according to a PDP of exemplary embodiments of the invention, a first dielectric layer and a carbon nanotube layer may be formed on display electrodes on a first substrate, and a second dielectric layer may be formed on the carbon nanotube layer with an opening pattern corresponding to the display electrodes. The carbon nanotube layer may increase the amount of emitted secondary electrons in the discharge cells, resulting in improved discharge efficiency (the ratio of power consumption to brightness). Consequently, it may be possible to improve brightness and achieve low-voltage driving.
It will be apparent to those skilled in the art that various modifications and variation can be made in the present invention without departing from the spirit or scope of the invention. Thus, it is intended that the present invention cover the modifications and variations of this invention provided they come within the scope of the appended claims and their equivalents.
Number | Date | Country | Kind |
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10-2004-0038164 | May 2004 | KR | national |