This application makes reference to, incorporates the same herein, and claims all benefits accruing under 35 U.S.C. §119 from an application entitled PLASMA DISPLAY PANEL filed with the Korean Industrial Property Office on 19 Apr. 2004 and there duly assigned Serial No. 2004-0026646.
1. Field of the Invention
The present invention relates to a plasma display panel having an improved structure.
2. Description of the Related Art
A plasma display panel (PDP) is a slim and light flat display panel that has a large size, high definition and wide viewing angle. Compared with other flat panel displays, the PDP can be easily manufactured to have a large size and the PDP is thus considered to be next-generation large flat panel display.
The PDP is classified into a DC type, an AC type, and a hybrid type according to the discharge voltage characteristics. Also, the PDP can be classified into an opposite discharge type and a surface discharge type according to the discharge structure.
Turning now to
Another problem with the design of
It is therefore an object of the present invention to provide an improved design for a PDP.
It is further an object of the present invention to provide a design for a PDP that results in improved luminous efficiency.
It is still an object of the present invention to provide a design for a PDP that avoids the problem of image sticking or image burn in when the same image is displayed for a long period of time.
These and other objects can be achieved by a design for a PDP that includes a front substrate, a rear substrate arranged opposite to the front substrate, closed-type front barrier ribs arranged between the front substrate and the rear substrate and made of a dielectric material, the front barrier ribs defining discharge cells together with the front and rear substrates, front and rear discharge electrodes being arranged within the front barrier ribs and surrounding the discharge cells and spaced apart from each other, phosphor layers arranged within the discharge cells, and a discharge gas injected into the discharge cells.
The discharge cell may have a cross section of a circular shape. The front and rear discharge electrodes may include a loop portion having a predetermined width and a circular cross section and surrounding the discharge cell. Also, the front and rear discharge electrodes may include a loop portion having a predetermined width and a polygonal-shaped cross section and surrounding the discharge cell, where the ratio R of the minimum distance to a maximum distance from a symmetry axis of the loop portion of the front discharge electrode or the rear discharge electrode to the front discharge electrode satisfies the inequality 1.0/√{square root over (2)}≦R≦1.0.
The front and rear discharge electrodes may include a rectangular loop portion surrounding the discharge cell, and a ratio of a length of a vertical portion to a length of a horizontal portion in the loop portion may be between 0.9 and 1.5.
According to the present invention, the interference of the electric field occurring in the front and rear discharge electrodes can be minimized, and a uniform discharge can be generated, thus improving the luminous efficiency. Also, since there are no electrons at portions of the front substrate where visible rays emitted from the discharge cell pass, an opening ratio and a transmittance can be remarkably improved. In addition, since the surface discharge occurs in all sides forming the discharge space, the discharge surface can be greatly extended.
Further, since the discharge is generated at the sides of the discharge cell and then spread toward the central portion of the discharge cell, the entire discharge cell can be efficiently used. Accordingly, the PDP can be driven at a low voltage, such that the luminous efficiency is remarkably improved. Furthermore, since the PDP can be driven at a low voltage even when a high-concentration Xe gas is present as discharge gas, the luminous efficiency can be improved.
A more complete appreciation of the invention, and many of the attendant advantages thereof, will be readily apparent as the same becomes better understood by reference to the following detailed description when considered in conjunction with the accompanying drawings in which like reference symbols indicate the same or similar components, wherein:
The PDP 200 according to the first embodiment of the present invention will now be described in conjunction with
In this embodiment, since visible rays generated from the discharge cells 220 are emitted through the front substrate 201 to the outside, the front substrate 201 is formed of a material having good transmittance, such as glass. A front transmittance of visible rays is remarkably improved over the PDP 100 of
In the PDP 200 of
Referring to
Turning now to
The PDP 200 according to the first embodiment of the present invention may instead not include an address electrode 203. When there is no address electrode, the front discharge electrodes are extended along one direction, and the rear discharge electrode is extended in a direction intersecting with the extended direction of the front discharge electrodes. In this case, one of the front and rear discharge electrodes serves as the address electrode and the other serves as the scan electrode and the sustain electrode.
Turning now to
In order to maximize the uniformity of the electric field and the luminous efficiency, it is preferable that the loop portions 211 and 212 of the front and rear discharge electrodes 206 and 207 both have a regular polygonal shape. Furthermore, if the cross sections of the discharge cells 220 and the loop portions of the front and rear discharge electrodes have a form close to a circular shape, the luminous efficiency is even more improved.
That is, in order to improve the luminous efficiency in a discharge cell whose cross section has a the regular polygonal shape, the loop portions of the front and rear discharge electrodes must be formed to have a form closer to a circular shape. Turning to
Likewise,
In general, considering the opening ratio of the PDP, if the loop portion has a regular polygonal shape with four or more edges, the interference of the electric field occurring between the discharge electrodes is small and the opening ratio increases. A ratio R for a square loop is 1/√{square root over (2)}, a ratio of the regular hexagonal loop is √{square root over (3)}/2, and a ratio of the circular loop is 1. Accordingly, as the regular polygonal shape gets closer to that of a circle, the ratio R decreases and the ratio of a circular loop becomes 1. Thus, it is preferable that the ratio R1=(Lmin1/Lmax1) of the front discharge electrode 206 satisfies the inequality 1/√{square root over (2)}≦Lmin1/Lmax1≦1.0. Likewise, it is preferable that the ratio R2=(Lmin2/Lmax2) of the rear discharge electrode 207 satisfies the inequality 1/√{square root over (2)}Lmin1/Lmax1≦1.0. However, considering the process error in the formation of the front and rear discharge electrodes 206 and 207, it is preferable that the ratio R1=(Lmin1/Lmax1) of the front discharge electrode 206 satisfies the inequality 1.1/√{square root over (2)}≦Lmin1/Lmax1≦1.0 and the ratio R2=(Lmin2/Lmax2) of the rear discharge electrode 207 satisfies the inequality 1.1/√{square root over (2)}≦Lmin2/Lmax2≦1.0.
In this embodiment, the loop portion 211 of the front discharge electrode 206, the loop portion 212 of the rear discharge electrode 207, and the discharge cells 220 have the same cross section. However, the present invention is not limited to this. That is, the loop portion 211 of the front discharge electrode 206, the loop portion 212 of the rear discharge electrode 207, and the discharge cells 220 can also have different cross sections. Meanwhile, if the loop portion 211 of the front discharge electrode 206, the loop portion 212 of the rear discharge electrode 207, and the discharge cell 200 each have the same cross section, the uniformity of the discharge is improved so that the luminous efficiency increases.
It is preferable that at least sides of the front barrier ribs 208 are covered with the MgO layer 209 that serves as a protective layer. The MgO layer 209 can be formed by a deposition process at the front barrier ribs, lower surfaces of the front barrier ribs, and/or a lower surface of the front substrate between the discharge cells. Although the MgO layer 209 is not a requisite component, its presence can prevent the barrier ribs 208 from being damaged due to collision with charged particles. Also, the presence of the MgO layer 209 is beneficial for another reason because the MgO layer 209 emits a lot of secondary electrons during the discharge.
The rear substrate 202 supports the address electrodes 203 and the dielectric layer 204 and is made of a material whose main component is a glass. On the rear substrate 202, the address electrodes 203 are arranged. The address electrodes 203 each extend along one row of discharge cells in a direction intersecting the direction the front and rear discharge electrodes 206 and 207 extend. In this embodiment, the address electrodes 203 are formed to be orthogonal to the front and rear discharge electrodes 206 and 207.
The address electrodes 203 initiate an address discharge that makes it easier to initiate a sustain discharge between the front discharge electrode 206 and the rear discharge electrode 207. That is, the address electrode 203 reduces the voltage needed to initiate the sustain discharge. The address discharge occurs between the scan electrode and the address electrode. When the address discharge is finished, positive ions accumulate near the scan electrode and electrons accumulate near the common electrode. Thus, the sustain discharge between the scan electrode and the common electrode can occur more easily than if no charges accumulated.
Since an address discharge occurs most efficiently when the gap between the scan electrode and the address electrode small, the rear discharge electrode 207 is located closer to the address electrode 203 than the front discharge electrode 206. The rear discharge electrode serves as the scan electrode and the front discharge electrode 206 serves as the common electrode. However, even when there is no address electrode 203 present on the rear substrate, the discharge can occur between the front and rear discharge electrodes 206 and 207. Therefore, the present invention is not limited to the structure where address electrodes 203 are present.
The dielectric layer 204 where the address electrode 203 is buried is made of a dielectric material such as PbO, B2O3 and SiO2. Such materials can guide charges and also prevent damage to the address electrode 203 caused by collision of positive ions or electrons during the discharge.
The rear barrier ribs 205 are arranged between the front barrier ribs 208 and the dielectric layer 204 and define a space therebetween. Although the rear barrier ribs 205 define a square matrix shape in the PDP 200 of
Although the phosphor layers 210 illustrated in
The discharge cells 220 are filled with a discharge gas, such as Ne, Xe or a mixture thereof. According to the present invention, the discharge surface can be increased and the discharge area can be extended so that an amount of plasma increases. Therefore, low voltage driving is possible. Since the present invention can achieve low voltage driving even when a high-concentration Xe gas is used as the discharge gas, the luminous efficiency can be remarkably improved. Consequently, the present invention can solve the problem of the PDP 100 of
In the above-described PDP 200, the address discharge is initiated by applying a potential difference between the address electrode 203 and the rear discharge electrode 207. As a result of the address discharge that occurs as a result of this potential difference, the discharge cells 220 for the sustain discharge is selected.
Thereafter, an AC sustain voltage is applied between the front discharge electrode 206 and the rear discharge electrode 207 of the selected discharge cells 220. This causes a sustain discharge to occur therebetween. Due to the sustain discharge, an energy level of the excited discharge gas is lowered and thus ultraviolet rays are emitted. The ultraviolet rays excite the phosphor layer 210 located within the discharge cells 220 and the energy level of the excited phosphor layer 210 is lowered thus emitting visible rays that form an image.
According to the PDP 100 illustrated in
Also, the sustain discharge is formed in a closed curve along the sides of the discharge cells 220 and is gradually spread toward the center of the discharge cells 220. Thus, a volume of space where the sustain discharge occurs is increased compared to the PDP 100 of
As illustrated in
Turning now to
As with the PDP 200 of
Compared with the PDP 200 of
The second modification of
Turning now to
The PDP 300 according to the second embodiment differs from PDP 200 according to the first embodiment in that the discharge cells 320 have a cross section of a rectangular shape instead of a square shape. Referring to
As described in the first embodiment, in order to uniformly produce the discharge in the discharge cells 320 and increase the luminous efficiency, it is preferable that the loop portions 311 of the front discharge electrodes have a shape close to a square. Accordingly, in order to maximize the luminous efficiency in the discharge cells 320 having the cross section of the rectangular shape, a horizontal portion 311a and a vertical portion 311b constituting each loop portion 311 of the front discharge electrode 306 is formed to have a shape close to that of a square. A ratio (N/M) of a length N of the vertical portion 311b to a length M of the horizontal portion 311a in the loop portion 312 of the front discharge electrode 306 can be considered as a design parameter.
It is preferable that a ratio (N/M) of a length N of the vertical portion 311a to a length M of the horizontal portion 311a in the loop portion 311 of the rear discharge electrode 307 is in range from 0.9 to 1.5. Likewise, a ratio (N′/M′) of a length N′ of the vertical portion 312b to a length M′ of the horizontal portion 312b in a loop portion 312 of the rear discharge electrode 307 is also preferably in range of 0.9 to 1.5.
In this second embodiment, although the loop portion 311 of the front discharge electrode 306, the loop portion 312 of the rear discharge electrode 307, and the cross section of the discharge cells 320 are all illustrated as having the same rectangular shape, the present invention is in no way so Limited. That is, the loop portion 311 of the front discharge electrode 306, the loop portion 312 of the rear discharge electrode 307, and the cross section of the discharge cells 320 may be formed to have different shapes and still be within the scope of the present invention.
Meanwhile, if the loop portion 311 of the front discharge electrode 306, the loop portion 312 of the rear discharge electrode 307, and the cross section of the discharge cells 320 have the same cross section, the uniformity of the discharge is improved so that the luminous efficiency is increased. Since a driving method of the PDP 300 is similar to that of the first embodiment, a detailed description thereof will be omitted.
While the present invention has been particularly illustrated and described with reference to exemplary embodiments thereof, it will be understood by those of ordinary skill in the art that various changes in form and details maybe made therein without departing from the spirit and scope of the present invention as defined by the following claims.
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