Patent Application
20070029925
The present invention relates to a high-strength glass member which is drastically improved in shatter resistance and finds useful application to various kinds of structural members, glass products and other products utilizing glass which are required to maintain shatter resistance even if reduced in size and weight.
Glass is utilized for a very wide variety of articles ranging from tableware, window glass and its sort which are found close to us, to electronic devices such as displays and storages and transportation means such as various kinds of vehicles and aircraft. It has been the general concept that glass is fragile and easily broken, and realization of unbreakable glass has been but a fantasy. As means for strengthening glass, there have been known several methods such as chemical strengthening, air blast cooling and crystallization. Nevertheless, even with the glass which has had such strengthening treatments, or so-called strengthened glass, the improvement of strength is limited to approximately double to thrice the strength of the non-treated glass (ordinary glass). In this field of industry, development of high-strength glass having four or more times higher strength than ordinary glass is being pushed ahead for application to flat panel displays (FPD).
It is considered that shatter (break) of glass occurs as the innumerable microcracks existing in the glass surface are forced to grow up to the greater cracks when a bending stress is exerted thereto. It is impossible to eliminate such microcracks from the glass surface. Therefore, it has been tried to obtain so-called strengthened glass by subjecting ordinary glass to the various strengthening treatments such as mentioned above.
As an example of glass strengthening treatments, Patent Document 1 discloses a chemical strengthening treatment in which a rare earth oxide (such as La2O3, Y2O3 or CeO2) is incorporated in ordinary glass in an amount of 1% by weight or less. Also, Patent Document 2 discloses a method in which ultra-shortwave laser is applied to ordinary glass to form a heterogeneous phase in the surface portion of this glass to thereby inhibit growth of the cracks.
Air blast cooling is a treatment in which cold air is blown against the heated glass surface to form a compression strengthened layer on this glass surface to thereby prevent formation of cracks. This treatment is principally targeted at the large-sized plate glass, 4 mm or greater in thickness, which is mostly used for vehicles or building materials. The crystallization method features forming the crystal grains with a size of 100 nm or greater in the inside of amorphous glass to suppress the growth of the microcracks to the larger cracks in the glass surface by the presence of the crystal grains, thereby to strengthen the whole body of glass.
Patent Document 1: JP-A-2001-302278
Patent Document 2: JP-A-2003-286048
In the chemical strengthening method which is a conventional concept of means for strengthening glass, the glass surface is subjected to alkali ion exchange in a heated and melted nitrate for replacing Li ions in the surface portion of ordinary glass with Na ions, and the Na ions in the surface portion of ordinary glass with K ions, to form a compression strengthened layer on the glass surface. “Unbreakable glass” is required to have strength which is about 10 times that of ordinary glass as a result of the strengthening treatments. The strength enhancing effect by the conventional chemical treatments, however, is limited to about double or thrice higher strength than ordinary glass and far from being capable of providing “unbreakable glass”. Further, such strengthened glass involves the problem of low heat resistance (drop of strength on heating). Also, strength of the “strengthened glass” obtained by the conventional crystallization treatment is only about double that of ordinary glass, and such “strengthened glass” is low in transparency. As viewed above, it has been hardly possible to realize unbreakable glass with the prior art technology.
An object of the present invention is to provide a high-strength glass which is applicable to the scheme for size and weight reduction. The high-strength glass according to the present invention is capable of realizing enhancement of strength by about 6 to 10 times over the ordinary glass and finds its useful application to a wide variety of articles such as mentioned above including substrates for FPD, various kinds of glass-utilizing products, building materials, etc.
In order to attain the above object, the present invention features forming, at a surface portion of a glass member containing at least a rare earth element, a strengthened layer comprising a layer of a heterogeneous phase containing at least the said rare earth element. The “surface portion” of glass referred to in this invention signifies the portion of the glass in the very shallow region from the outermost surface of the glass, which will be further explained in the section of Examples.
The said rare earth element is at least one element selected from the group consisting of Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb and Lu, preferably from the group consisting of Eu, Gd, Dy, Tm, Yb and Lu, more preferably it is Gd.
In the present invention, said heterogeneous phase is formed by irradiation with ultra-short pulse laser so that it will exist in the region within the depth of 300 μm from the outermost surface on one side, preferably on both sides, of said glass.
In the present invention, a rare earth element is contained in the glass in an amount of 1 to 10% by weight, preferably 2 to 7% by weight, calculated as an oxide thereof Ln2O3 (Ln: rare earth element).
In the present invention, a high-density heterogeneous phase containing a rare earth element is formed at the surface portion of the glass by applying ultra-short pulse laser, for example femtosecond laser, to the surface portion of the glass containing a rare earth element. This high-density heterogeneous phase containing a rare earth element functions to check growth of the microcracks to the larger cracks when a bending stress is exerted to the glass. Since formation of this heterogeneous phase does not depend on alkali ion exchange in the surface portion of the glass such as practiced in the chemical strengthening treatment, there is no need of incorporating an alkali in the glass to be strengthened.
In the portion irradiated with femtosecond laser, the particles containing a rare earth element are caused to separate out in the surface portion of the glass to form a high-density heterogeneous phase, which strengthens the glass surface and inhibits the microcracks from growing up to the larger cracks. By containing a rare earth element in the glass, it becomes possible to form a high-density and high-crystallinity heterogeneous phase.
As the rare earth element, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb or Lu, preferably Eu, Gd, Dy, Tm, Yb or Lu, more preferably Gd is used. The glass containing Eu, Gd, Dy, Tm, Yb or Lu has high light transmittance in the visible light region. Particularly, when Gd is contained, it is possible to satisfy, at remarkably high levels, both requirements for enhancement of strength and good light transmittance in the visible light region.
In the present invention, ultra-short pulse laser is applied to a prescribed depth of the surface portion of the glass to form a heterogeneous phase. Since irradiation with ultra-short pulse laser such as femtosecond laser gives no thermal influence to the glass, such as often observed in ordinary laser irradiation, there is no fear that a strain be built up in the glass after laser irradiation.
A high glass strengthening effect can be obtained by forming a heterogeneous phase in the glass region which is within 300 μm in depth from the outermost surface of the glass. This is because at a depth exceeding 300 μm, the effect of inhibiting growth of the already existing microcracks in the glass surface to the larger cracks is lessened, and there rather is produced a tendency to lower strength of the glass. Even higher strengthening can be realized by forming the heterogeneous phase on both sides of the glass.
When the content of Ln2O3 is less than 1% by weight, its strength enhancing effect is small. When its content exceeds 10% by weight, the treated glass tends to devitrify (crystallize). In view of this, the preferred range of content of Ln2O3 is 2 to 7% by weight.
The scope of use of the present invention is not limited to the structural components of the display devices and the glass structural members of electronic devices such as substrates of magnetic discs; the invention can be also applied widely to the other objectives such as structural materials and window glass (including 2-layer glass and laminated glass) of buildings, substrates for solar batteries, structural members and window glass of vehicles, aircraft, spacecraft, etc., for which high strength and reduction of size and weight are essential requirements.
Other objects, features and advantages of the invention will become apparent from the following description of the embodiments of the invention taken in conjunction with the accompanying drawings.
HIG: high strength glass, HSL: high-density heterogeneous phase layer, MC: microcrack, UIG: ultra-high strength glass, ODG: ordinary glass, OIG: strengthened glass obtained by forming a high-density heterogeneous phase layer on ordinary glass, PNL1: back panel, PNL2: front panel, SUB1: back substrate, SUB2: front substrate, s (s1, s2, . . . sm): scanning signal lines, d (d1, d2, d3, . . . ): picture signal lines, ELS: electron source, ELC: connecting electrode, AD: anode, BM: black matrix, PH (PH(R), PH(G), PH(B)): phosphor layer, SDR: scanning signal line drive circuit, DDR: picture signal line drive circuit, SPC: spacer.
The best mode for carrying out the present invention is described below.
On the other hand, according to the conventional strengthening means shown in
The rare earth oxide added in the glass in the present invention is an oxide (Ln2O3) of Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb or Lu, preferably an oxide (Ln2O3) of at least one element selected from Eu, Gd, Dy, Tm, Yb and Lu, more preferably an oxide of Gd. By incorporating such a rare earth oxide in the glass, high strengthening of the whole glass can be realized, and further by forming a heterogeneous phase region HGL on both surfaces, it is possible to obtain a glass with extremely high strength.
The high-strength glass HIG which has been strengthened in its whole body by the addition of a rare earth oxide Ln2O3 is irradiated with femtosecond laser to form a heterogeneous phase region HGL on the glass surface, providing an ultra-high strength glass UIG which is proof against break caused by the microcracks.
The above-mentioned average flexural strength test of the glass according to the present invention is explained here. In this average flexural strength test, the test pieces were made from the glass block described below and the method explained with reference to
(1) Making of Glass Block
The melt was cast into a mold to make a glass block, and it was overheated at 600° C. for one hour, then gradually cooled at a cooling rate of 1° C./min and straightened.
The composition of the glass to which no rare earth oxide was added (indicated by “No addition” in the drawing) was 63 wt % SiO2, 15 wt % Al2O3, 8 wt % B2O3, 3 wt % MgO, 4 wt % CaO and 7 wt % SrO.
As indicated by an oval in
Further, by incorporating at least one element selected from the group consisting of Al element, B element and alkali earth metal elements in the oxide-based glass, the following effects can be obtained. That is, Al element (Al2O3) is effective for preventing devitrification and improving chemical stability, and B element (B2O3) is helpful for lowering glass making temperature and improving vitrification stability, while an alkali earth metal oxide (R′O) contributes to the improvement of Young's modulus.
In case a rare earth element is contained in an amount of 1 to 10% by weight, preferably 2 to 7% by weight calculated as an oxide thereof Ln2O3 (Ln: rare earth element) based on the whole oxide-based glass, if the amount of Ln2O3 contained in the oxide-based glass is less than 1% by weight, its effect of enhancing glass strength is unsatisfactorily small, but if its amount exceeds 10% by weight, it tends to cause devitrification (crystallization) of glass. Therefore, the amount of this element contained in the glass should be in the range of 1 to 10% by weight, preferably 2 to 7% by weight.
(2) Preparation of Test Pieces
The test pieces, each measuring 3 mm in thickness (t), 4 mm in width (a) and 40 mm in length (h), were made from the glass block made in (1) according to JIS R1601. Ten test pieces were prepared for each of the tests before and after laser irradiation.
(3) Conditions for Forming Heterogeneous Phase
Ultra-short pulse laser (YAG laser excited sapphire laser) was used under the following conditions: pulse width=200 femtoseconds; frequency=1 kHz; wavelength=780 nm; laser irradiated section=region to a depth of about 100 μm from the test piece surface; irradiated area=4×40 mm on both sides of the glass.
(4) Flexural Strength Test (3-Point Bending Test) Conditions
Three-point bending strength ν (MPa) was calculated from the following equation:
σ=(3s·w/2a·t2) (1)
wherein s: span of the lower portion; w: breaking load;
a: width of the test piece; t: thickness of the test piece.
The heterogeneous phase was found formed in the region to a depth of about 180 μm from the outermost surface of the glass. This region corresponds to the area where femtosecond laser was concentrated. Also, this heterogeneous phase was composed of a particulate precipitate, and it had high density and appeared to be crystallized.
(1) Making of Glass Block
The melt was cast into a mold to make a glass block, and it was overheated at 550° C. for one hour, then gradually cooled at a cooling rate of 1° C./min and straightened.
(2) Preparation of Test Pieces
The test pieces measuring 3 mm in thickness (t), 4 mm in width (a) and 40 mm in length (h) were made from the glass block made obtained in (1) according to JIS R1601. There were prepared 10 test pieces for each of the tests before and after laser irradiation.
(3) Conditions for Forming Heterogeneous Phase
Ultra-short pulse laser (YAG laser excited sapphire laser) was used under the following conditions: pulse width=200 femtoseconds; frequency=1 kHz; wavelength=780 nm; laser irradiated section: region to a depth of about 50 μm from the test piece surface; irradiated area: 4×40 mm on both sides of the glass.
In
When the content of Gd2O3 was 0 to 0.5% by weight, a high-density amorphous heterogeneous phase separated out. When the content of Gd2O3 was 1 to 3% by weight, a high-density Gd element-containing heterogeneous phase having a tendency to crystallize separated out. When the content of Gd2O3 was 5 to 10% by weight, a high-density Gd element-containing heterogeneous phase having crystallizability separated out. When the content of Gd2O3 was 15% by weight or higher, the formed phase had already a tendency to devitrify (crystallize), and there was observed no remarkable influence by laser irradiation.
The melt was cast into a mold to make a glass block, overheated at 600° C. for one hour, then gradually cooled at a cooling rate of 1° C./min and straightened.
As the test pieces for the flexural strength test, those measuring 3 mm in thickness (t), 4 mm in width (a) and 40 mm in length (h) were made from the said glass block according to JIS R1601. There were prepared 10 test pieces for each of the tests before and after laser irradiation.
For forming the heterogeneous phase, ultra-short pulse laser, viz. YAG laser excited sapphire laser, was used under the following conditions: pulse width=200 femtoseconds; frequency=1 kHz; wavelength=780 nm; laser irradiated section: region to the depth of about 200 μm from the test piece surface; irradiated area: 4×40 mm on both sides.
A 3-point bending test was conducted for determining the flexural strength. The 3-point bending strength C (MPa) was calculated from the following equation:
σ=(3s·w/2a·t2)
From observation by an electron microscope, it was found that in the ultra-high strength glass UIG obtained by irradiating the rare earth element-containing glass with femtosecond laser, a heterogeneous phase HGL was formed to the depth of 100-300 μm, the region where femtosecond laser was concentrated, from the outermost surface of said glass UIG.
Next, heat resistance of the glass according to the present invention is explained. In the glass which has undergone the chemical strengthening treatment (alkali ion exchange in the glass surface) which is one of the conventional means for strengthening glass surface, the alkali ions are diffused to the surface on heating to reduce strength. Such reduction of strength on heating can be prevented by the surface strengthening treatment comprising femtosecond laser irradiation according to the present invention. This technique is particularly useful for the structural members of the devices which require a heat treatment in their production process, such as flat panel displays (FPD) and magnetic discs.
In the heat resistance improvement test, there were used the glass samples of the following compositions:
The melt was cast into a mold to make a glass block, and it was overheated at 600° C. for one hour, then gradually cooled at a cooling rate of 1° C./min and straightened.
The size of the test pieces was 3 mm in thickness (t), 4 mm in width (a) and 40 mm in length (h). As means for strengthening the test pieces, a heterogeneous phase containing a rare earth element was formed on glass A in the same way as illustrated in
The heat treatment of the test pieces was conducted at 100° C., 150° C., 200° C., 250° C., 300° C., 350° C., 400° C. and 450° C. for 10 minutes for each temperature. There were prepared 5 test pieces for the test at each of the above temperatures. The flexural strength test conditions were the same as illustrated in
In contrast, in “Comparative Example h”, a sharp drop of strength occurs at 300° C. or above. This is because the alkali ions which have undergone ion exchange in the heat treatment are diffused to the surface. Also, in “Comparative Example g”, there takes place a drop of strength at 200° C. or above. This is because the heterogeneous phase is faded out by the heat treatment.
A steel ball drop test on the glass according to the present invention is explained below. The compositions of the glass samples used for this test were as follows.
The melt was cast into a mold to make a 150 mm×150 mm×150 mm cubic glass block, and it was heated at 550-600° C. for 2 hours, then gradually cooled at a cooling rate of 1° C./min and straightened.
The 150 mm×150 mm×2.5 mm test pieces were prepared from this glass block and subjected to the following strengthening treatments.
An impact test was conducted on the above glass samples according to JIS C8917. In the test, a steel ball of 450 g in mass was dropped to each test piece from the heights of 25 cm, 50 cm, 75 cm, 100 cm and 125 cm. 3 test pieces were used in the drop test for each height. The results of the tests are shown in Table 2. In Table 2, ◯ indicates no test piece fractured, Δ indicates part of the test pieces fractured, and × indicates all of the test pieces fractured.
As seen from Table 2, the test pieces of rare earth element-containing glass subjected to the chemical strengthening treatment comprising formation of a heterogeneous phase according to the present invention (Examples s and t) suffered no fracture by drop of the steel ball from the heights of up to 75 cm, with only one test piece being fractured by drop of the steel ball from the height of 100 cm in Example s. In Comparative Examples i to m, all of the test pieces were fractured by the drop of the steel ball from the height of 75 cm. This indicates that the rare earth element-containing glass having a heterogeneous phase formed in its surface according to the present invention has far higher strength than the glass samples of the Comparative Examples.
As viewed above, the glass member according to the present invention has required strength even if small in thickness, and when it has a large thickness, its safety and reliability are appreciably increased. Thus, the scope of use of the present invention is not limited to the electronic devices such as panel glass for FPD and solar batteries; the invention can be applied as well to the fields of buildings, vehicles, aircraft, spacecraft, etc.
Here, the results of the tests on impact fracture resistance of the laminated glass (glass laminates) according to the present invention are explained. The compositions of the test pieces and the glass materials are the same as used in the impact fracture tests on the single-layer glass (glass C) described above, but the amount of the materials melted was about 17 kg and the melting conditions were 1,500° C. and 6 hours (of which 3.5 hours was used for stirring and homogenization of glass). The melt was cast into a mold to make an approximately 150 mm×150 mm×220 mm glass block, and it was heated at 550° C. for 3 hours, then gradually cooled a cooling rate of 1° C./min and straightened.
The following 3 different test pieces were cut out from the said glass block and subjected to optical polishing:
Test piece for single layer glass: 150 mm×150 mm×3.0 mm
Test piece for 2-layer glass: 150 mm×150 mm×1.5 mm
Test piece for 3-layer glass: 150 m×150 mm×1.0 mm
The chemical strengthening treatment was the same as conducted on said glass C, that is, a heterogeneous phase containing a rare earth element was formed.
After forming a chemically strengthened layer, a synthetic resin EVA (ethylene-vinyl acetate copolymer) was sandwiched between the test pieces for 2-layer glass and pressed together to make 2-layer laminated glass, and this glass was presented here as “Example v”. EVA was also sandwiched between the respective test pieces for 3-layer glass and pressed together to make 3-layer laminated glass, which was presented as “Example x”. The attached layer thickness was about 0.3 mm. The test piece for single-layer glass is intended for comparison with laminated glass, and it is designed so that the overall thickness of glass exclusive of the resin will be equal to the glass thickness of 2-layer laminated glass (1.5 mm+1.5 mm=3.0 mm) and the glass thickness of 3-layer laminated glass (1.0 mm+1.0 mm+1.0 mm=3.0 mm). This single-layer glass is presented as “Example u”.
Table 3 shows the results of the impact facture test by drop of a steel ball on the 2-layer and 3-layer glass laminates, along with the test results on the test piece for single-layer glass with the same thickness. The mass of the steel ball used was 1.0 kg. This test was also a test according to JIS C8917 in which, with the layout described above, a steel ball of 1.0 kg in mass was dropped onto the test piece from the heights of 25 cm, 50 cm, 75 cm, 100 cm, 125 cm and 150 cm. Three test pieces were used in the drop test for each height. In Table 3, ◯ indicates no test piece fractured, Δ indicates part of the test pieces fractured, and × indicates all of the test pieces fractured.
As seen from the results shown in Table 3, the laminated glass made by using the rare earth element-containing glass having a heterogeneous phase formed in its surface according to the present invention (Examples v and x) is appreciably strengthened in comparison with the single-layer glass (Example u) of the same thickness, and even if such laminated glass is fractured, there takes place no scattering of its fragments.
The present invention described above may be summarized as follows.
In the present invention, a high-density heterogeneous phase containing a rare earth element is formed in the surface portion of the glass by applying ultra-short pulse laser, such as femtosecond laser, to the surface portion of the glass containing a rare earth element. This high-density heterogeneous phase containing a rare earth element prevents the microcracks from growing to the larger cracks when a flexural stress is exerted to the glass. Since formation of this heterogeneous phase does not depend on alkali ion exchange in the glass surface portion as conducted in the chemical strengthening treatment, there is no need of containing an alkali in the glass to be strengthened.
In the femtosecond laser irradiated portion, the particles containing a rare earth element separate out uniformly in the glass surface portion to form a high-density heterogeneous phase, which strengthens the glass surface and prevents growth of the microcracks to the larger cracks. Incorporation of a rare earth element in the glass enables formation of a heterogeneous phase with high density and high crystallinity.
As the rare earth element, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb and Lu can be used, of which Eu, Gd, Dy, Tm, Yb and Lu are preferred, with Gd being the most preferred. The glass containing Eu, Gd, Dy, Tm, Yb or Lu has high light transmittance in the visible light region, and by containing Gd in particular, it is possible to satisfy, quite remarkably, both requirements for enhancement of strength and good light transmittance in the visible light region.
Irradiation with ultra-short pulse laser such as femtosecond laser used in the present invention, unlike ordinary laser irradiation, gives no thermal influence to the glass, so that no strain is left in the glass after laser irradiation. Also, since a heterogeneous phase is formed to a depth within 300 μm from the outermost surface of the glass, a high strengthening effect can be obtained. Further, by forming the heterogeneous phase on both front and back sides of the glass, a higher degree of strengthening can be realized.
When the content of Ln2O3 is less than 1% by weight, its strength enhancing effect is small. When its content exceeds 10% by weight, the treated glass tends to devitrify (crystallize). In view of this, the preferred range of content of Ln2O3 is 2 to 7% by weight.
The scope of use of the glass member according to the present invention is not limited to the structural components of the display devices such as FPD and the glass structural members of electronic devices such as substrates of magnetic discs; the glass of this invention can be also applied widely to the other objectives such as structural materials and window glass (including 2-layer glass and laminated glass) of buildings, substrates for solar batteries, structural members and window glass of vehicles, aircraft, spacecraft, etc., for which high strength as well as reduction of size and weight are required.
In the following, an example of flat panel display (FPD) which is one of the most promising fields of application of the glass of the present invention is explained.
As one of the self-emission type FPD having an electron source arranged as a matrix, there are known field emission displays (FED) and electron emission displays utilizing the cold cathodes capable of integration with low power. For these cold cathodes, there are used, for instance, spindt-type electron source, surface conduction type electron source, carbon nanotube type electron source, metal-insulator-metal (MIM) laminate type, metal-insulator-semiconductor (MIS) laminate type, and metal-insulator-semiconductor-metal type thin-film electron sources.
Self-emission type FPD has a display panel comprising a back panel provided with electron sources such as mentioned above, a front panel provided with phosphor layers and an anode issuing an accelerating voltage for bombarding the electrons emitted from the electron sources, and a sealing frame for sealing the inside space between the two opposing panels in a prescribed evacuated state. The back panel has the said electron sources formed on a back substrate, and the front panel has the phosphor layers formed on a front substrate and an anode issuing an accelerating voltage for forming an electric field for bombarding the electrons emitted from the electron sources against the phosphor layers. A drive circuit is combined with this display panel. Usually, the back panel, front panel and sealing frame are made of glass. By using the said glass of the present invention for these parts, it is possible to realize an FPD which is small in size and weight and resistant to breakage.
Each electron source makes a pair with a corresponding phosphor layer to constitute a unit picture element. Usually, one pixel (color pixel) is composed of unit picture elements of three colors, viz. red (R), green (G) and blue (B). In the case of color pixel, the unit picture element is also called sub-pixel.
The front and back panels are separated by a member called spacer to keep a prescribed space between them. This spacer is a plate-like member made of an insulating material such as glass or ceramic or a material having a certain degree of conductivity, and it is provided for each group of pixels at a position where it will not hinder the movement of the pixels. By using the glass of the present invention for this spacer, it is possible to realize a thin, light-weight and breakage-resistant FPD.
The front substrate SUB2 of the front panel is made of the glass according to the present invention. An anode electrode AD is provided on the inner surface of the substrate, and phosphor layers PH (PH(R), PH(G), PH(B)) are formed on said anode electrode AD. With this arrangement, the phosphor layers PH (PH(R), PH(G), PH(B)) are comparted by a light shielding layer (black matrix) BM. The anode electrode AD is shown as a solid electrode, but it may be constituted as stripe electrodes arranged to cross the scanning signal lines s (s1, s2, s3, . . . sm) and divided for each row of pixels. The electrons emitted from the electron sources ELS are accelerated and bombarded against the phosphor layers PH (PH(R), PH(G), PH(B)) constituting the corresponding sub-pixels. Consequently, the said phosphor layers PH emit light with a prescribed color and it is mixed with the color of the light emitted from the phosphor of the other sub-pixels to constitute a color pixel of a prescribed color.
The front panel PNL2 and the back panel PNL1 are opposed to each other, and in order to keep a prescribed space between them, the rib-like spacers SPC of approximately 80 μm in width and approximately 2.5 mm in height are provided above and in the extending direction of the scanning signal wiring and secured in position by using fritted glass or other means. A glass-made sealing frame MFL is provided at the peripheral edges of both panels and fixed in position by fritted glass (not shown) so that the internal space held by both panels will be isolated from the outside.
For fixing the spacers with fritted glass, they are heated at 400-450° C., and then the system is evacuated to about 1 μPa through an evacuating tube 303 and then sealed. In operation, a voltage of about 5-10 kV is applied to the anode AD on the front panel PNL2.
It should be further understood by those skilled in the art that although the foregoing description has been made on embodiments of the invention, the invention is not limited thereto and various changes and modifications may be made without departing from the spirit of the invention and the scope of the appended claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2004-272244 | Sep 2004 | JP | national |
This application is a continuation application of U.S. application Ser. No. 11/224,096, filed Sep. 13, 2005, the contents of which are incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| Parent | 11224096 | Sep 2005 | US |
| Child | 11580126 | Oct 2006 | US |
