KR100400667B1 - A display apparatus using gas discharge - Google Patents

Abstract

According to the present invention, a barrier rib structure having a predetermined separation height and a separation width includes a filling space having a predetermined size, inert gas is filled in the space, and a voltage having a predetermined size is applied to an electrode exposed in the filling space. The present invention relates to a gas discharge display device composed of cells in which the phosphor emits light due to excitation of the phosphor due to a discharge phenomenon generated between the electrodes. Particularly, a barrier rib to which a phosphor is coated is used. When the phosphor is coated in a "W" shape and a bridge is formed on the existing bulkhead, and the phosphor is coated on the new "H" shaped barrier rib where the address electrode is perforated, infrared (828 nm) or vacuum ultraviolet rays emitted from the PDP cell are formed. (147 nm, 173 nm) and the like concentrated on the center of the cell can be used sufficiently to By increasing the light intensity, thereby increasing the efficiency of the PDP.

Description

A display apparatus using gas discharge

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a display apparatus using gas discharge, and more particularly, to a partition on which a phosphor is applied, and a new partition is formed between the partition and the partition to apply the phosphor in a "W" shape. When a bridge is formed on the partition wall and the phosphor is applied on the new "H" shaped partition wall where the address electrode is drilled, infrared rays (828 nm) or vacuum ultraviolet rays (147 nm, 173 nm) emitted from the PDP cell are placed on the center of the cell. The present invention relates to a gas discharge display device for increasing the efficiency of a plasma display panel (hereinafter referred to as a PDP) by increasing the luminance of emitted light of a fluorescent substance.

In general, PDP is a display device for display developed as an alternative to LCD, and its characteristic is to display characters or graphics using visible light generated by excitation of phosphor by vacuum ultraviolet (VUV) generated by discharging inert gas It is an element to make.

Therefore, it is also referred to as a gas discharge display device, and the basic technical principle thereof is as shown in FIG.

At this time, the PDP is classified into various types according to the electrode structure. The structure of PDP electrode is classified into DC type, AC type, and hybrid type in which DC type and AC type are combined. In addition, it can be classified into a two-electrode structure three-electrode structure according to the number of electrodes installed in the cell. In addition, according to the arrangement of the electrodes forming the discharge, it can be classified into a counter electrode and a surface discharge electrode structure, as shown in Figs.

As shown in FIG. 2, in the case of the counter electrode structure, two sustain electrodes forming a discharge are positioned on the front substrate and the back substrate, respectively, and the discharge is formed on the vertical axis of the panel. In the case of the surface discharge electrode structure, It refers to an electrode structure in which two sustain electrodes forming a discharge are located on the same substrate so that the discharge is formed on one plane of the panel. Finally, the electrode structure of the PDP is classified into a transmissive type and a reflective type structure as shown in FIGS. 4 and 5 by the application position of the phosphor.

The transmissive electrode structure has the advantage of being easy to fabricate but has the disadvantage of large variation due to the printing surface state of the phosphor. The reflective structure has the advantage of increasing the luminance by increasing the coating area of the phosphor, but the phosphor There is a difficulty in the technique of application.

Reflective electrode structure has higher luminance characteristics than transmissive electrode structure, and the problem of phosphor coating is solved by the development of thick film printing technology.

Currently, AC-PDP of the surface discharge-reflective-3 electrode structure of Fujitsu panel shows superior performance compared to other structures, and each company adopts this structure. The panel structure of Fujitsu is shown in FIG. . It has a form of surface discharge by arranging ITO (transparent electrode (Indium Tin Oxide transparent electrode)), which is a transparent conductor, side by side on the front substrate, and has a structure in which a phosphor is coated on the rear substrate by arranging an address electrode and a partition wall in parallel. In particular, the conductivity was improved by adding a Cr-Cu-Cr metal electrode (hereinafter referred to as a metal electrode) on the transparent electrode on the front substrate.

This is to prevent the voltage drop due to the large resistance of the transparent electrode to form a discharge directly to a large panel because the resistance is increased. It is called a discharge holding electrode including such a transparent electrode and a metal electrode.

3 and 4 are cross-sectional views illustrating basic electrode structures of an AC PDP and a DC PDP. In the case of DC type PDP, the electrode is directly exposed to the discharge plasma. In the case of AC type PDP, the electrode is indirectly coupled with the plasma through the dielectric layer. This difference shows a difference in discharge phenomenon, and in the case of AC PDP, the charged particles formed by the discharge are accumulated in the dielectric layer.

In other words, electrons are accumulated in the dielectric layer on the positively charged electrode, and ions are accumulated in the dielectric layer on the negatively charged electrode. The potential formed through this phenomenon is called a wall potential, and since the wall potential is formed to be opposite to the potential applied from the outside, the potential applied to the gas in the cell decreases when the wall potential starts to be formed.

Therefore, when a sufficiently large wall potential is formed, the discharge is erased because the potential applied to the gas decreases below the potential at which discharge can be maintained. However, if the potential of the potential applied to the external electrode is applied after the wall potential is formed, the potential by the wall potential and the externally applied potential are added to the drive by a memory function that can discharge even when a low external potential is applied. Do it.

AC type PDPs have memory functional effects due to wall potentials accumulated in such dielectrics, and dielectrics in cells where discharges were previously formed are more likely than those in cells in which charged particles form wall potentials in dielectrics and do not have wall potentials. It can cause discharge at low voltage. This memory function is very useful for driving a large panel of a PDP, which is a gas discharge display device employing a row driving method.

In addition, the DC-type PDP, unlike the AC-type PDP, does not have a function of forming a wall potential by a dielectric and thus does not have a unique memory function. That is, since the electrode is directly exposed to the discharge region, the charged particles formed by the discharge flow to the external circuit through the electrodes having opposite polarities, and thus cannot be accumulated on the electrode surface. Therefore, in the case of DC type PDP, the charged particle supply effect is used. Use the pulse memory function.

The pulse memory function refers to the principle that when a discharge pulse is applied again before the charged particles and quasi-neutral particles formed in the discharge are attenuated, the discharge is formed under a lower voltage than without these charged particles. Such a memory function is an essential feature that enables driving without deterioration of luminance when driving a large panel by a row driving method, and such a characteristic is also necessary in terms of electrode structure.

As shown in FIG. 7, the basic electrode structure of the DC-type PDP includes the anode electrode 3 and the cathode electrode 4, the partition wall 5, and the phosphor 6 formed on the front substrate 1 and the back substrate 2. )

The anode 3 and the cathode 4 form a current path for forming a discharge, and the partition wall 5 determines the distance between electrodes for forming a discharge, It prevents crosstalk.

The electrode material mainly used in the DC-type PDP has a high secondary electron emission coefficient so as to have a low discharge voltage characteristic, and nickel, which is excellent in sputtering characteristics that can withstand sputtering by ions, is mainly used.

In the case of the AC PDP shown in Fig. 8, the dielectric layer 10 for forming the capacitively coupled discharge comprises a sustain electrode 7 composed of a transparent ITO electrode 7 and a Cr-Cu-Cr metal electrode 8 ( 8) (hereinafter, sustain electrodes 7 and 8) and address electrodes 9 are covered.

In general, the dielectric layer used is a borosilicate series, has a low secondary electron emission coefficient, and has a short lifetime due to sputtering by ions generated during plasma formation. An oxide thin film such as MgO) is used as a protective film (hereinafter referred to as Mgo protective film 11) and coated on the dielectric layer 10.

The magnesium oxide (MgO) exhibits low voltage discharge characteristics because of its good sputter resistance and high secondary electron emission coefficient. However, since the thickness of the MgO protective layer should be thin and the surface characteristics should be excellent, it is difficult to form through thick film printing and is usually manufactured by a thin film process by vacuum deposition.

In the case of the partition 5, a height of about 100 to 200 μm is required to form a discharge distance and a volume. By the thick film printing method and the electrophoresis method, the partition 5 of several tens of micrometers in thickness is formed.

In addition, as a requirement for forming a discharge, an electrode structure having two electrodes or generally three electrodes is mainly used.

In case of DC type PDP, an auxiliary cathode is added to form an auxiliary discharge. In case of an AC type PDP, the sustain electrode (7) (8) and the selective discharge and the sustain discharge are separated to address speed. An address electrode 9 is introduced to improve the efficiency.

Therefore, the electrode structure may be classified into a two-electrode structure and a three-electrode structure according to the number of electrodes. In addition, as described above, the electrode may be classified into a counter electrode structure and a surface discharge electrode structure according to the arrangement of the electrodes forming the discharge. In the case of the counter electrode structure, two sustain electrodes forming the discharge may be respectively formed on the front substrate and the back surface. In the surface discharge type electrode structure, two sustain electrodes are formed on the same substrate so that the discharge is formed on one plane of the panel. Say structure.

8 is a view showing an AC type PDP according to the prior art, and is formed to have a predetermined interval in the horizontal direction on the front substrate 1 and the upper surface of the front substrate 1 made of glass to facilitate light transmission and discharge. In order to maintain the voltage, a sustain electrode (7) (8) consisting of a transparent ITO electrode (7) and a metal electrode (8) of Cr-Cu-Cr, and a front substrate (1) including the sustain electrode (7) (8). Mgo on the dielectric layer is formed on the front surface to protect the dielectric layer 10 and the dielectric layer 10 to protect the sustain electrodes 7 and 8 to extend the lifespan, improve the secondary electron emission effect, and reduce the discharge characteristics. The protective layer 11 is formed and the address electrode 9 is formed to have a predetermined interval in the orthogonal direction to the sustain electrodes 7 and 8 formed on the upper front surface of the back substrate 2, and the dielectric layer 10 is formed thereon. While maintaining the gap between the front substrate (1) and the back substrate (2) between each cell In order to prevent discharge, partition walls 5 are formed parallel to the address electrodes 9 with each lower address electrode 9 therebetween, and red, green and blue (R, G) are formed between the partition walls 5. The phosphor 6 of (B) is applied.

As described above, when the manufacturing of the front substrate 1 and the rear substrate 2 is completed, exhaust holes are formed in the rear substrate 2 to fill a desired discharge gas in a vacuum state, and then the front substrate 1 and After applying the bonding frit to the periphery of the rear substrate 2 and the completion of the bonding, a discharge region is formed between the front substrate 1 and the rear substrate (2). When the above process is completed, the process of injecting the discharge gas according to the desired optical characteristics through the exhaust hole and then sealing is completed the entire process of PDP manufacturing.

On the other hand, the colorization of PDP adopts a method of exciting phosphors like CRT, and CRT uses electro-luminescence which is excited by electrons accelerated to several tens of keV. Emitting light by photo-luminescence, in which a phosphor is excited by ultraviolet rays formed by the film, is adopted.

In particular, 147 nm vacuum ultraviolet rays of Xen gas are mainly used. As described above, a gas discharge display device mainly applied to a PDP uses a penning effect of discharge gas as a core technology for image display. have.

The phenning effect is to promote the ionization reaction through metastable particle species with a very large impact area, which enhances Townsend's “α-process”.

Metastable atoms are long-lived once they have been created, which makes them easier to ionize other species through collisions.

For example, the penning reaction of He + Xe and Ne + Xe is shown in the following formula (1).

In Formula 1, He and Ne are main component gases, Xe is an additive gas, and He ^* and Ne ^* are particles in metastable states or particles in an excited state, respectively.

Particles in these excited states have a relatively long life time and have a large impact cross section, so the probability of collision with other particles is greater.The effect of these neutral excitation species on the addition of He and Ne gas is higher than that of Xe Gas. This is to promote ionization. In addition, the secondary electron emission from the surface of the material in contact with the plasma plays a very important role in determining the discharge characteristics of the PDP.

In particular, the secondary electrons are emitted by the plasma from the electrode covered with the dielectric layer, such as AC-type PDP may be a direct ion impact, the surface reaction of the excitable species, and the reaction by light.

The most important of these is the reaction by ion bombardment. Ne ion with ionization energy of 21.6 eV enters and is neutralized by combining with one electron in the valence band, and the extra energy is applied to the other valence band. Electrons are emitted to the surface.

The kinetic energy of the electron can be obtained by subtracting the bandgap energy of MgO and the surface work-function energy from the energy of the incident ions. Will generate ions and electrons.

Therefore, the energy levels and lifetimes of the resonance and metastable states for various gases are summarized in Table 1 below.

division He Ne Ar Kr Xe Resonancelevel Energy (eV) 21.2 16.6 11.6 9.98 8.4 Lifetime (sec) 0.56 20.7 10.2 4.4 3.8 Metastablelevel Energy (eV) 19.8 16.6 11.5 9.9 8.3 Lifetime (sec) 6 * 10 ⁵ 70.8 1.3 One

Next, VUV will be described in the gas discharge display device. Vacuum Ultraviolet (VUV) refers to UV having a short wavelength of 200 nm or less even in UV. VUV does not pass through these gases if the pressure of the gas is high or contains oxygen, and strong absorption occurs in the gases.

Unlike the CRT, unlike the CRT, since the photo-luminescence of the phosphor is excited by the ultraviolet rays generated by the gas discharge as described above, the wavelength and intensity of the VUV in the PDP are important factors for determining the luminance of the light emitted from the panel. The initial PDP study used Hg, but it was not suitable for practical use due to the problem of increasing the temperature.

Among the various gases, UV emitted in the inert gas Resonance state was found to be most suitable for PDP, and the 147 nm, 152 nmm, and 173 nm resonance and molecular beams emitted from Xe showed the wavelength region where RGB phosphors had the best efficiency. Overlap

However, in the case of He and Ne among inert gases, since the wavelength of light emitted from resonanceI has a short wavelength of 100 nm or less, it is not suitable for use for UV for stimulating a phosphor and emitting visible light.

The physical characteristics of each gas are summarized in the table as shown in Table 2 below.

Ionizationenergies (eV) Metastableenergies (eV) Resonanace state Atomic radius Collision radius with electrons energies (ev) Emission wavelength (nm) Gas used He 24.6 19.8 / 20.7 21.2 59 1.50 7.07 Ne 21.6 16.6 / 16.7 16.7 / 16.8 74/73 1.59 7.94 Ar 15.8 11.5 / 11.7 11.6 / 11.8 107/105 1.91 11.46 Kr 14.0 9.9 / 10.5 10.0 / 10.6 125/117 2.01 12.69 Xe 12.1 8.3 / 9.4 8.4 / 9.6 147/129 2.20 15.21 Hg 10.4 4.7 / 5.4 4.9 / 6.7 253/185 1.41 6.25

Considering the intensity and wavelength of the emitted UV light, Xe gas seems to be suitable. However, in order to use it as a PDP gas, Xe gas should be considered at the same time as the driving voltage or the lifetime of the electrode.

Representative case is to add Xe gas to He or Ne to lower the driving voltage and improve the UV efficiency. The use of He or Ne as the main gas is to take advantage of the fact that the excitation of Xe is efficient and the panning effect with Xe is higher because the electron temperature in these gases is higher than that of pure Xe gas.

In addition, it is mixed with other inert gases such as Ar and Kr to maximize light emission and improve color purity by the penning effect.

As described above, not only the type of gas but also the gas composition, pressure, and the wavelength of light emitted and efficiency vary. Indirectly, the cell structure or the driving circuit affects the optimal discharge gas. It should be selected in combination with the driving circuit.

The theoretical efficiency that can be derived from the PDP principle described above is about 5lm / W. However, the efficiency of PDP currently being commercialized is about 2lm / W, which is lower than that of other displays.

An object of the present invention for solving the above problems is for a partition to which the phosphor is applied to form a new partition between the partition and the partition wall to apply the phosphor in a "W" shape and to form a bridge to the existing partition address When the phosphor is applied onto a new "H" -shaped partition wall where the electrode portion is drilled, infrared (828 nm) or vacuum ultraviolet (147 nm, 173 nm) emitted from the PDP cell can be fully utilized. The present invention provides a gas discharge display device for increasing the efficiency of a plasma display panel (hereinafter referred to as PDP) by increasing light emission luminance of a phosphor.

1 is a schematic diagram showing a light emission principle of a plasma display panel.

2 is a schematic diagram of a counter electrode structure of a PDP.

3 is a schematic diagram of a surface discharge electrode structure of a PDP.

4 is a schematic diagram of a transmissive electrode structure of a PDP.

5 is a reflective electrode structure of a PDP.

6 is a Fujitsu panel electrode structure.

7 is a cross-sectional view showing an electrode structure of a discharge cell of a DC-type PDP.

8 is a sectional view showing the electrode structure of a discharge cell of an AC PDP.

Fig. 9 is a graph showing the three-dimensional measurement results for 828 nm in PDP cells not coated with phosphors.

10 is a graph showing a three-dimensional measurement result in a PDP cell coated with a phosphor.

11A and 11B show a new bulkhead structure of an AC PDP according to the present invention.

12A and 12B show a bridged " H " bulkhead structure of an AC PDP according to the present invention;

<Description of Symbols for Major Parts of Drawings>

1: Front board 2: Back board

3: anode electrode 4: cathode electrode

5: bulkhead 6: phosphor

7, 8: sustain electrode 9: address electrode

10 dielectric layer 11: MgO protective film

A feature of the present invention for achieving the above object is a partition structure having a predetermined separation height and separation width having a filling space of a predetermined size and filled with an inert gas in the space, the electrode exposed in the filling space A gas discharge display device comprising cells in which a phosphor emits light when a voltage of a predetermined size is applied to the electrode, and the phosphor is excited by a discharge phenomenon generated between the electrodes. In the barrier rib structure, a new barrier rib of a certain size is not formed between the barrier ribs and the barrier ribs so that the phosphor is filled in a "W" shape.

As an additional feature of the present invention for achieving the above object, when the partition structure for forming the space filled with the inert gas has a height of 100 to 200㎛ and a width of 50 to 80㎛ the new partition is 10 to 170 height The thickness is 10 to 100 µm.

As another additional feature of the present invention for achieving the above object, the position of the new partition wall is formed at a predetermined position including the center of the cell in the range that does not invade on the address electrode of the electrodes exposed in the filling space, It is spaced apart from any one of 1-250 micrometers from the said address electrode, and is spaced apart from the existing partition by any one of 10-300 micrometers.

Another feature of the present invention for achieving the above object is a partition structure having a predetermined separation height and separation width having a filling space of a predetermined size and filled with an inert gas in the space, and is exposed in the filling space A gas discharge display device comprising a cell in which a phosphor emits light when a predetermined voltage is applied to an electrode, and the phosphor is excited by a discharge phenomenon generated between the electrodes. A gas discharge display device comprising: a space in which the inert gas is filled. In the barrier rib structure, a bridge is formed between the barrier rib and the barrier rib to form an “H” -shaped barrier rib in which an address electrode portion is formed.

As an additional feature of the present invention for achieving the above object, a phosphor is applied to a partition of an "H" shape through which the address electrode portion is drilled through the formation of the bridge, and the address electrode portion is drilled through the formation of the bridge. The bridges facing each other in the H ”-shaped bulkhead are staggered.

In another aspect of the present invention for achieving the above object, when the barrier rib structure forming the space filled with the inert gas has a height of 100 ~ 200㎛ and a width of 50 ~ 80㎛ address to form the bridge The width of the bridge portion is 10 to 200 mu m and the height is 1 to 150 mu m in the "H" -shaped partition wall where the electrode portion is drilled, and the length is in the range which does not invade the address electrode portion.

In another aspect of the present invention for achieving the above object, 1 to 250㎛ of the electrode exposed in the filling space in the "H" -shaped partition wall formed by forming the bridge and the portion of the address electrode is perforated. It is spaced at one interval.

The above object and various advantages of the present invention will become more apparent from the preferred embodiments of the present invention described below with reference to the accompanying drawings by those skilled in the art.

In the case of the conventional structure of the AC-PDP, as described above, the front substrate 1 made of glass and the upper surface of the front substrate 1 are formed to have a predetermined interval in the horizontal direction to facilitate light transmission, and thus discharge voltage. In order to maintain the front surface of the front substrate 1 including the sustain electrode (7) (8) consisting of a transparent ITO electrode (7) and a metal electrode (8) of Cr-Cu-Cr, the sustain electrode (7) Mgo protective film formed on the dielectric layer 10 to protect the sustain electrodes 7 and 8 and the dielectric layer 10 to extend the lifespan, improve the secondary electron emission effect, and reduce the discharge characteristics. (11), an address electrode 9 is positioned on the rear substrate 2 and an upper surface of the rear substrate 2 so as to have a predetermined interval in a direction orthogonal to the sustain electrodes 7 and 8, and the address electrode 9 ) To form a dielectric layer. In addition, in order to maintain a gap between the front substrate 1 and the rear substrate 2 and to prevent mis-discharge between cells, the partition walls 5 parallel to the address electrodes 9 with each address electrode 9 therebetween interposed therebetween. ), And phosphors 6 of red, green, and blue (R, G, B) are applied between the partition walls 5.

As such, when manufacturing of the front substrate 1 and the rear substrate 2 is completed, an exhaust hole is formed in the rear substrate 2 to fill a desired discharge gas in a vacuum state, and a heat sink and a driving circuit are formed on the rear surface of the rear substrate. Is supposed to be located.

Fig. 9 shows the results of three-dimensional experiments on infrared rays (828 nm) emitting vacuum ultraviolet rays (147 nm) in a PDP cell to which no phosphor was applied. Infrared radiation (828 nm) emitted from the PDP cell is concentrated above the center of the cell.

However, in the PDP cell coated with the phosphor of FIG. 10, strong light emission was detected near the partition wall. Therefore, by efficiently using infrared rays (828 nm) concentrated on the center of the cell, vacuum ultraviolet rays (147 nm) emitted from infrared rays (828 nm) will be able to effectively excite the phosphor.

Therefore, in the structure proposed in the present invention, as shown in Figs. 11 and 12, the new barrier rib is formed between the barrier rib and the barrier rib as shown in Figs. To form a new H-shaped partition wall and to apply the phosphor.

At this time, Figure 11 is an illustration of a new partition structure of the AC type PDP according to the present invention, Figure 11a is a side view of the partition structure of the AC type PDP cell according to the present invention, Figure 11b is a view of the AC type PDP cell according to the present invention It is a plan view of a partition wall.

12 is an exemplary view of a bridge-type "H" partition structure of the AC type PDP according to the present invention, Figure 12a is a side view of the partition structure of the AC type PDP cell according to the present invention, Figure 12b is an AC according to the present invention It is a partition plan view of a type PDP cell.

Therefore, in this case, the vacuum ultraviolet rays (147 nm) emitted on the center of the cell efficiently excite the phosphor, thereby increasing the emission luminance of the phosphor, thereby increasing the efficiency of the plasma display panel (PDP).

While the invention has been shown and described in connection with specific embodiments thereof, it is well known in the art that various modifications and changes can be made without departing from the spirit and scope of the invention as indicated by the claims. Anyone who owns it can easily find out.

As described above, according to the present invention, in order to increase the efficiency of low-efficiency PDP, the vacuum ultraviolet ray (147 nm) emitted from the center of the cell efficiently excites the phosphor to increase the emission luminance of the phosphor. When the new barrier rib is formed between the barrier rib and the barrier rib, the phosphor is applied in a "W" shape, and the bridge is formed in the existing barrier rib and the phosphor is applied onto the new "H" shaped barrier rib where the address electrode is perforated. (828 nm), vacuum ultraviolet rays (147 nm, 173 nm), and the like, which are concentrated on the center of the cell, can be sufficiently used to increase the luminescence brightness of the phosphor.

Claims (10)

delete delete delete delete delete A barrier rib structure having a predetermined separation height and a separation width includes a filling space having a predetermined size, inert gas is filled in the space, and a voltage of a predetermined size is applied to the electrodes exposed in the filling space. In a gas discharge display device comprising cells in which the phosphor emits light by being excited by the generated discharge phenomenon: And forming a bridge between the partition walls and the partition walls to form an “H” -shaped partition wall in which an address electrode portion is formed. The method of claim 6, And a phosphor is coated on the “H” -shaped partition wall through which the address electrode portion is formed by forming the bridge. The method of claim 6, And the bridges facing each other in the " H " partition wall where the address electrode portion is drilled through the formation of the bridge, and phosphors are coated on each partition wall. The method of claim 6, When the barrier rib structure forming the space filled with the inert gas has a height of 100 to 200 μm and a width of 50 to 80 μm, the width of the bridge portion is formed in the “H” -shaped barrier rib formed with the bridge to form the bridge. Is 10 to 200 µm, the height is 1 to 150 µm, and the length thereof is within a range that does not involve the address electrode portion. The method of claim 6, A gas discharge display device, wherein the gas is formed at a distance of 1 to 250 μm from an address electrode among the electrodes exposed in the filling space in a “H” -shaped partition wall formed by forming the bridge. .