Color cathode ray tube

Abstract: A color cathode ray tube (1) includes a vacuum envelope (2) having, a faceplate (5), an optical filter (9) formed on an outer surface of the faceplate (5), and a phosphor screen (8) formed on an inner surface of the faceplate (5) and essentially consisting of red, blue, and green emitting phosphors, wherein the red emitting phosphor essentially consists of a Y₂O₃:Eu phosphor, an Eu activation amount thereof being not less than 3.0 mol% and not more than 9.0 mol% with respect to a Y₂O₃ amount as a base material, and light filtering means provided in front of the faceplate for selectively transmitting light, having the maximum absorption wavelength in wavelength range of 575 ± 20 nm in connection with wavelength range from 400nm to 650 nm and being satisfied with the following relationship: T min ≦ T₅₅₀ ≦ T₅₃₀, 1 ≦ T₄₅₀/T₅₃₀ ≦ 2, 1 ≦ T₆₁₅/T₅₃₀ ≦ 2, 0.7 ≦ T₄₅₀/T₆₁₅ ≦ 1.43, T₆₁₅/T₅₈₀₋₆₀₀ ≧ 1.1, wherein T₄₅₀, T₅₃₀, T₅₅₀, T₆₁₅, T min and T₅₈₀₋₆₀₀ represent the transmissivities for lights of wavelength of 450 nm, 530 nm, 550 nm, 615 nm, the said maximum absorption wavelength in wavelength range of 575 ± 20 nm and the maximum absorption wavelength in wavelength range of 580 nm to 600 nm, respectively.

Description: The present invention relates to a color cathode ray tube and, more particularly, to a color cathode ray tube having a thin film having light selectivity, the optical filter being formed on the front surface of a faceplate of the color cathode ray tube. In a color cathode ray tube, electron beams from an electron gun assembly arranged in a neck of an envelope are bombarded on a dot- or stripe-like red, green, and blue emitting phosphor layers regularly formed on the inner surface of the glass faceplate, thereby displaying characters and/or images. A red emitting phosphor in this color cathode ray tube generally consists of europium-activated yttrium oxide (Y₂O₃:Eu) or europium-activated yttrium oxysulfide (Y₂O₂S:Eu). Although the Y₂O₂S:Eu phosphor can provide redness to some extent by color correction using an Eu activator concentration, sufficient brightness as a red pixel of a color cathode ray tube cannot be obtained. Since the Y₂O₂S:Eu phosphor does not have satisfactory temperature characteristics, its brightness is lowered with an increase in temperature of a faceplate upon electron beam radiation. In order to explain this relationship, a relationship between the electron beam radiation time and the brightness of the red emitting phosphor is plotted in a graph of Fig. 1. As shown in Fig. 1, when an electron beam of 10.4 µs/cm² impinges on the Y₂O₂S:Eu phosphor, the brightness of the phosphor is lowered by about 8% in 120 sec. After a lapse of 120 sec. or more, the brightness is gradually lowered. The Y₂O₂S:Eu phosphor does not have satisfactory current - brightness characteristics. That is, when a current density is increased, a decrease in brightness tends to be increased. In particular, a red emitting phosphor has a higher current ratio than that of a blue or green emitting phosphor. Therefore, when the current - brightness characteristics of the red emitting phosphor are not sufficient, a serious problem is posed. To the contrary, the Y₂O₃:Eu phosphor has a very high emission brightness level as compared with the Y₂O₂S:Eu phosphor and satisfactory temperature characteristics, as shown in Fig. 1. Fig. 2 is a graph showing a relationship between the current density and the relative brightness of the Y₂O₃:Eu phosphor for various Eu activation amounts when the brightness of the Y₂O₂S:Eu phosphor is given as 100%. As is apparent from Fig. 2, the relative brightness of the Y₂O₃:Eu phosphor as a function of an increase in current density is higher than that of the Y₂O₂S:Eu phosphor. Judging from this, it is understood that the Y₂O₃:Eu phosphor has satisfactory current - brightness characteristics. As shown in Fig. 2, even if an activation amount of Eu in the Y₂O₃:Eu phosphor is increased, brightness saturation rarely occurs. For this reason, the Y₂O₃:Eu phosphor has a higher brightness level in a large-current range, thus providing satisfactory phosphor properties. When an Eu activation amount is 4.5 mol% with respect to the base material, a practical color purity of a color cathode ray tube can be obtained. In this case, the Y₂O₃:Eu phosphor has a higher emission brightness level than that of the Y₂O₂S:Eu phosphor by +30%. The Eu concentration is represented by an average molecular weight of the phosphor itself, i.e., {(number of moles of Eu₂O₃ contained in 1 mol) × 100} when it is figured out as an average molecular weight of a compound obtained by partially substituting Y of Y₂O₃ with Eu. Along with the recent development of a larger color cathode ray tube, performance of an electron gun assembly for emitting electron beams, and particularly its focusing capacity has been improved. It is expected that the performance of the Y₂O₃:Eu phosphor on the phosphor screen can be improved by suppression of brightness saturation, and that the capability of the high-performance electron gun assembly can be maximized. However, even if an Eu activation amount of the Y₂O₃:Eu phosphor is increased, a sufficient color purity cannot be obtained as compared with the Y₂O₂S:Eu phosphor. Figs. 3a and 3b show the chromaticity coordinate values ( y and x values) and the Eu activation amount of the Y₂O₃:Eu phosphor, respectively. Ranges indicated by a hatched region in Figs. 3a and 3b, i.e., ranges of x = 0.620 or more and y = 0.345 or less, are practical chromaticity ranges of the Y₂O₂S:Eu phosphor. The corresponding Eu activation amount falls within the range of 3.0 mol% to 4.4 mol% with respect to the base material. As compared with the chromaticity ranges of the Y₂O₂S:Eu phosphor, the chromaticity coordinate values of the Y2O3:Eu phosphor are x = 0.628 and y = 0.347, which are not practical. Even if an Eu activation amount is increased, changes in chromaticity are decreased with an increase in Eu concentration. Therefore, the y value as the chromaticity coordinate value does not reach the range represented by the hatched region. It is impossible to maintain image quality of the Y₂O₃:Eu phosphor to be equal to that of Y₂O₂S:Eu phosphor. A red emitting phosphor ideally has satisfactory brightness characteristics as those of the Y₂O₃:Eu phosphor and a satisfactory color purity as that of the Y₂O₂S:Eu phosphor at a low Eu activation amount. In recent years, in order to improve color purity of a red emission component, suppress degradation of image brightness, and improve contrast, a color cathode ray tube having a neodium oxide (Nd₂O₃)-containing glass plate to obtain a selective light-absorbing property formed on the front surface of a faceplate is proposed (Published Unexamined Japanese Patent Application Nos. 57-134848, 57-134849, and 57-134850). This glass plate has a narrow main absorption band in a range of 560 to 615 nm and a sub absorption band in a range of 490 to 545 nm due to light-absorbing properties inherent to neodium oxide. Therefore, red and blue color purity values of an image can be advantageously increased. Although this glass plate has the selective light-absorbing properties, the contrast cannot be greatly improved. A method of evaluating an effect of contrast improvement using BCP (Brightness Contrast Performance) is available. This BCP is defined as BCP = ΔB/ΔRf where ΔB is the brightness decrease rate and ΔRf is the rate of decrease in reflectance of ambient light. The BCP represents a contrast improvement ratio when a system using a neutral filter is assumed as a reference. When a neodium oxide filter having selective light-absorbing properties is evaluated by using the BCP, the BCP falls within the range of 1 ≦ BCP ≦ 1.05. It is therefore understood that the contrast is not sufficiently improved. Since the glass plate containing neodium oxide has a narrow region having a width of 5 to 10 nm in the main absorption band of 560 to 570 nm in a wavelength range of 560 to 615nm, the color (body color) of the glass plate itself is changed by ambient light. In particular, the body color of the glass plate under an incandescent lamp becomes reddish. For this reason, a low-brightness portion such as a black or shadow portion in an image becomes reddish, readability is degraded, and image quality is degraded. In addition, since neodium is an expensive material, the resultant glass plate becomes expensive. It is an object of the present invention to provide a color cathode ray tube having satisfactory red emission pixels, and satisfactory brightness, color purity, and contrast characteristics. A color cathode ray tube according to the present invention comprises: an envelope including a faceplate with an inner and outer surfaces and a side wall portion, a neck and a cone connecting the faceplate to the neck; an electron gun provided inside the neck for emitting at least one electron beam; a phosphor screen provided on the inner surface of the faceplate and consisting essentially of red, blue, and green emitting phosphors, the red emitting phosphor comprising a Y₂O₃:Eu phosphor, and an Eu amount thereof being not less than 3.0 mol% and not more than 9.0 mol% with respect to a Y₂O₃ amount as a base material; and light filtering means provided in front of the faceplate for selectively transmitting light, having the maximum absorption wavelength in wavelength region of 575 ± 20 nm with respect to the wavelength range of 400nm to 650 nm and satisfying the following relationship: T min ≦ T₅₅₀ ≦ T₅₃₀ 1 ≦ T₄₅₀/T₅₃₀ ≦ 2 1 ≦ T₆₁₅/T₅₃₀ ≦ 2 0.7 ≦ T₄₅₀/T₆₁₅ ≦ 1.43 T₆₁₅/T₅₈₀₋₆₀₀ ≧ 1.1 wherein T₄₅₀, T₅₃₀, T₅₅₀, T₆₁₅, T min and T₅₈₀₋₆₀₀ represent the transmissivities for light of wavelength of 450 nm, 530 nm, 550 nm, 615 nm, the maximum absorption wavelength in wavelength region of 575 ± 20 nm, and the maximum absorption wavelength in wavelength range of 580 nm to 600 nm, respectively. According to the present invention, an optical filter having a predetermined selective light-absorbing property is combined with a Y₂O₃:Eu phosphor to obtain a color cathode ray tube exhibiting satisfactory color purity and brightness and having good red pixels. A color cathode ray tube having a high contrast level and being capable of absorbing ambient light can be obtained by using this optical filter. This invention can be more fully understood from the following detailed description when taken in conjunction with the accompanying drawings, in which: Fig. 1 is a graph showing a relationship between the electron beam radiation time and the brightness of a general red emitting phosphor; Fig. 2 is a graph showing current - brightness characteristics of Y₂O₃:Eu phosphor materials having different Eu activation amounts; Figs. 3A and 3B are graphs showing relationships between the Eu activation amounts of the Y₂O₃:Eu phosphor and the chromaticity coordinate values ( y and x values), respectively; Fig. 4 is a partially cutaway view showing a cathode ray tube according to the present invention; Fig. 5 is a graph showing a spectral distribution of light from a fluorescent lamp; Fig. 6 is a graph showing a spectral distribution of light from an incandescent lamp; Fig. 7 is a graph showing spectral distributions of light components from a Y₂O₃:Eu red emitting phosphor, a general blue emitting phosphor, and a general green emitting phosphor; Fig. 8 is a graph showing selective light-absorbing characteristics of an optical filter used in the present invention; Figs. 9A and 9B are graphs showing relationships between the chromaticity coordinate values and the Eu amounts of a cathode ray tube using the optical filter having the characteristics shown in Fig. 8, respectively; Fig. 10 is a graph showing light-absorbing characteristics of an optical filter according to an embodiment of the present invention; and Fig. 11 is a graph showing brightness comparison between the present invention and Y₂O₂S:Eu. The present invention will be described in detail with reference to the accompanying drawings. Fig. 4 is a partially cutaway side view showing a cathode ray tube according to the present invention. A cathode ray tube 1 has a glass vacuum tight envelope 2 having an evacuated interior. The vacuum envelope 2 has a neck 3 and a cone 4 continuous with the neck 3. The vacuum envelope 2 has a faceplate 5 tightly bonded to the cone 4 by fritted glass. A metal tension band 6 is wound around the outer circumferential wall of the faceplate 5 to prevent explosion. An electron gun assembly 7 is arranged in the neck 3 to emit electron beams. More specifically, the electron gun assembly 7 is arranged inside the faceplate 5. A phosphor screen 8 consisting of stripe-like phosphor layers for emitting red, green, and blue light components upon excitation by the electron beams emitted by the electron gun assembly 7 and of stripe-like black light-absorbing layers arranged between the phosphor layers is formed on the inner surface of the faceplate 5. A shadow mask (not shown) having apertures in its entire surface is arranged to closely oppose the phosphor screen 8. A deflection unit (not shown) is mounted on the outer surface of the cone 4 to deflect electron beams so as to scan the phosphor screen 8 with these beams. Light filtering means 9 having a predetermined selective light-absorbing property is formed on the outer surface of the faceplate 5 in the cathode ray tube 1. An optical filter may be used as the light filtering means. A Y₂O₃:Eu phosphor having a predetermined Eu activation amount is used as a red emitting phosphor in the phosphor screen 8. Light filtering means provided in front of the faceplate for selectively transmitting light, having the maximum absorption wavelength in wavelength region of 575 ± 20 nm with respect to the wavelength range of 400nm to 650 nm and satisfying the following relationship: T min ≦ T₅₅₀ ≦ T₅₃₀ 1 ≦ T₄₅₀/T₅₃₀ ≦ 2 1 ≦ T₆₁₅/T₅₃₀ ≦ 2 0.7 ≦ T₄₅₀/T₆₁₅ ≦ 1.43 T₆₁₅/T₅₈₀₋₆₀₀ ≧ 1.1 wherein T₄₅₀, T₅₃₀, T₅₅₀, T₆₁₅, T min and T₅₈₀₋₆₀₀ represent the transmissivities for light of wavelength of 450 nm, 530 nm, 550 nm, 615 nm, the said maximum absorption wavelength in wavelength region of 575 ± 20 nm, and the maximum absorption wavelength in wavelength range of 580 nm to 600 nm, respectively. The relationship between the transmissivities will be described below. Fig. 5 shows a curve 501 representing a spectral distribution of light from a fluorescent lamp, a spectral luminous efficacy curve 502, and a curve 503 representing the product of the spectral distribution curve 501 and the spectral luminous efficacy curve 502. As is apparent from this graph, it is assumed that ambient light can be most efficiently absorbed by shielding light near the maximum value of the curve 503, i.e., light in the range of 575 ± 20 nm. In this case, however, a decrease in brightness must be minimized. It is important to determine the characteristics of this optical filter in such a manner that the filter has a minimum luminous efficacy value, exhibits a maximum transmissivity and a maximum ambient light absorbance near 450 nm and 615 nm corresponding to a high emission energy of the phosphor, exhibits a minimum transmissivity near 575 nm corresponding to a low emission energy of the phosphor, and exhibits a medium transmissivity near 530 nm serving as an emission peak for a green emitting phosphor. In addition, as the characteristics of the optical filter having the above transmissivities, between 575 nm and 530 nm, the transmissivity near 550 nm is smaller than that at 530 nm because an ambient light energy is higher and the emission energy of the green emitting phosphor is lower near 550 nm than those near 530 nm. More specifically, if a filter satisfying conditions T min ≦ T₅₅₀ ≦ T₅₃₀ and T₅₃₀ ≦ T₆₁₅ (where T₄₅₀, T₅₃₀, T₅₅₀, T₆₁₅, and T min are the transmissivities for the wavelengths of 450 nm, 530 nm, 550 nm, and 615 nm, and the maximum light-absorbing wavelength, respectively), maximum efficiency in improving the image contrast can be achieved. Control of the body color of the optical filter was confirmed to be improved to a practical level by causing the transmissivities at the respective wavelengths described above to satisfy equations (1) to (3) below: T₄₅₀/T₅₃₀ = 1 - 2 T₆₁₅/T₅₃₀ = 1 - 2 T₄₅₀/T₆₁₅ = 0.7 - 1.43 In the above equations, when a value calculated by equation (1) exceeds 2 or a value calculated by equation (3) exceeds 1.43, a bluish body color is undesirably obtained. When a value calculated by equation (2) exceeds 2 or a value calculated by equation (3) is smaller than 0.7, a reddish body color is undesirably obtained, resulting in an impractical application. In addition, when values calculated by equations (1) and (2) are smaller than 1, the contrast improvement is suppressed, and the BCP value is decreased, resulting in an impractical application. When this optical filter is used, the BCP value falls within the range of 1.05 to 1.50, thus obtaining excellent contrast characteristics although this value is slightly changed depending on the emission spectrum of a phosphor used, a concentration of a filter material for the optical filter, and the like. When light from an incandescent lamp is replaced with ambient light, the body color of this optical filter becomes often reddish. However, this can be corrected to such a degree that the optical filter can be practically applied. Fig. 6 is a graph showing a spectral distribution curve 601 representing a spectral distribution obtained when light from an incandescent lamp is replaced with ambient light, a spectral luminous efficacy curve 602, and a curve 603 representing the product of the spectral distribution curve 601 and the spectral luminous efficacy curve 602. As is apparent from the curve 601, light from the incandescent lamp has a higher relative intensity with an increase in wavelength. For this reason, the body color of the cathode ray tube having such a selective light-absorbing filter may often be reddish even in the cathode ray tube of the present invention. In this case, the transmissivity of the optical filter in the range of 650 to 700 nm providing a more reddish component can be smaller than that at 615 nm having a higher emission energy of a red emitting phosphor. Judging from this, the body color can be corrected without impairing the BCP improvement effect, thereby obtaining a cathode ray tube having a small body color change caused by ambient light. As described above, since the optical filter used in the present invention has transmissivities satisfying a predetermined relationship, it can selectively absorb ambient light such as natural light or light from a fluorescent lamp. Red and blue color purity values of the image can be increased while a decrease in brightness is minimized. Utilizing the above-described characteristics of the optical filter, the present inventors established a method of correcting color purity to obtain a satisfactory color tone without degrading the high brightness of the Y₂O₃:Eu phosphor by combining the Y₂O₃:Eu phosphor having a high brightness but unsatisfactory color purity and the optical filter under a condition for efficiently improving the color purity. Fig. 7 shows a curve 701 representing an emission spectrum of a typical blue emitting phosphor ( znS:Ag,Cℓ phosphor), a curve 702 representing an emission spectrum of a green emitting phosphor (znS:Au,Aℓ phosphor), and a curve 703 representing an emission spectrum of a red emitting phosphor (Y₂O₃:Eu phosphor). The present inventors found that the color purity could be improved by absorbing a larger amount of light corresponding to a short-wavelength subpeak, i.e., light in the range of 580 nm to 600 nm than an amount of light corresponding to the main peak (615 nm) of the Y₂O₃:Eu phosphor represented by the curve 703 in Fig. 7. The present inventors confirmed that when the transmissivity for 580 to 600 nm and a transmissivity for light of the maximum absorption wavelength in range of 615 nm as a characteristic of the optical filter used in the present invention satisfied the following condition: T₆₁₅/T₅₈₀₋₆₀₀ ≧ 1.1 the chromaticity could be corrected in the same manner as in Y₂O₃S:Eu while the brightness was kept high. When a value satisfying condition (4) is smaller than 0.1, the color tone cannot be satisfactorily corrected. An effect of the present invention can be obtained when an Eu activation amount falls within the range of 3.0 mol% (inclusive) to 9.0 mol% (inclusive) with respect to the base material, as will be described below. Color cathode ray tubes having Eu activation amounts of 3.0 mol%, 5.0 mol%, 7.0 mol%, 9.0 mol%, and 10.0 mol% were prepared, and optical filters A, B, C, D, and E having light-absorbing characteristics represented by curves A, B, C, D, and E in Fig. 8 were formed on the front surfaces of the faceplates, respectively. The chromaticity coordinate values of the resultant color cathode ray tubes were measured, and the relationships between the chromaticity coordinate values and the Eu activation amounts, as shown in Figs. 9a and 9b, were obtained. Curves L, a , b , c , d , and e respectively show CIE chromaticity values ( y and x values) obtained when a filter is not used, the filter A is used, the filter B is used, the filter C is used, the filter D is used, and the filter E is used. A hatched region (practical ranges : y ≦ 0.345 and x ≧ 0.620) represents a practical region of Y₂O₂S:Eu. As shown in Figs. 9a and 9b, when the Eu activation amount is increased, a change in chromaticity is reduced. The chromaticity coordinate values cannot fall within the hatched region without filters. According to the present invention, expensive Eu need not be used in a large amount. The Eu activation amount preferably falls within the range of 3.0 to 5.5 mol%. The body color was evaluated as follows. The body color was evaluated by a human visual sense in accordance with whether an observer can recognize displayed black as natural black without adding any other color tone to black when a black image is displayed on each color cathode ray tube. More specifically, a 50 mm x 50 mm black pattern was displayed at a central portion of each cathode ray tube, and a background of this pattern was displayed in white. The faceplate was illuminated with an incandescent lamp obliquely at a 45° position from the faceplate surface so as to obtain a brightness of 500 luxes. Under these conditions, the tone colors (red, blue, green and the like) of black portions were evaluated. When the black image is observed as black without any other color tone, this result is evaluated as o ○ . When the black image is observed as black with some color tones, which does not pose any practical problem, the result is evaluated as o. When the black image is observed as black with relatively strong tone colors except for the black tone color, which poses a practical problem, the result is evaluated as Δ. When the black image cannot be observed as black due to strong color tones, the result is evaluated as x. Test results are summarized as follows: When the Eu activation amount is 3.0 mol%, the chromaticity coordinate values fall within the hatched region by using the filter B. As shown in Table 1, the body color of the filter B is evaluated as o and presents no problem. However, when the Eu activation amount is less than 3.0 mol%, the chromaticity coordinate values cannot fall within the hatched region even if the filter B is used. Even if chromaticity adjustment is performed by using the filter A or a filter having a higher density, the body color of the filter A becomes strongly reddish, thus posing a practical problem. At this time, when the density of the filter is increased, the above tendency is accelerated, resulting in an impractical application. Therefore, the Eu activation amount is preferably 3.0 mol% or more to obtain a better effect. When the Eu activation amount is 5.5 mol%, the chromaticity coordinate values fall within the hatched region by using the filter E, as shown in Fig. 9a. It is therefore found that an optical filter to be used in the present invention must have a chromaticity correction capacity equal to or higher than that of the filter E. The chromaticity correction capacity is determined depending on whether the subpeak components, i.e., yellow components near 580 nm to 600 nm are absorbed more than the main peak components in Y₂O₃:Eu. When the filter E is used, T₆₁₅/T₅₈₀₋₆₀₀ = 1.1 is given. When a value satisfying condition (4) is less than 1.1, Y₂O₃:Eu cannot be corrected to the practical range of Y₂O₂S:Eu. When the Eu concentration is increased, the brightness is decreased in Y₂O₃:Eu. When the Eu concentration is increased or decreased, the color purity and brightness of the Y₂O₂S:Eu phosphor similarly change. More specifically, when the Eu concentration is decreased, the color purity value is decreased, while the brightness is improved. An Eu amount required to satisfy color purity to fall within the range of x ≧ 0.620 and y ≦ 0.345 by using Y₂O₂S:Eu and the filter B was 3.2 mol%. The corresponding chromaticity coordinates were given as (x, y) = (0.623, 0.345). Fig. 11 shows a curve obtained by changing the Eu concentration of Y₂O₃:Eu and comparing the brightness values when Y₂O₂S:Eu was Eu = 3.2 mol% and the filter B was used. When the Eu concentrations were 3.0 and 3.5 mol%, the filter B was used. When the Eu concentration was 4.0 mol%, the filter C was used. When the Eu concentrations were 4.5 and 5.0 mol%, the filter D was used. When the Eu concentration was 5.5 mol% or more, the filter E was used. As is apparent from the graph in Fig. 11, when the Eu concentration is 9 mol% or more, the brightness is impaired to an impractical value. Therefore, the Eu concentration is preferably less than 9 mol%. Therefore, the Eu concentration falls within the range of 3.0 mol% (inclusive) to 9 mol% (inclusive). According to the present invention, an optical filter satisfying equations (1) to (3) and condition (4) is combined with a Y₂O₃:Eu phosphor having an Eu activation amount of 3.0 mol% (inclusive) to 9.0 mol% (inclusive) to efficiently obtain a low-cost color cathode ray tube which causes less changes in body color upon changes in ambient light and has excellent red pixels, a high contrast level, a high brightness level, and a high color purity level. A cathode ray tube according to the present invention is prepared as follows. Appropriate dyes and pigments which can provide the selective light-transmitting property described above are mixed in an alcohol solution containing ethyl silicate as a major constituent. The resultant mixture is directly applied to the faceplate by spin coating or spray coating to form an optical filter layer. Alternatively, dyes and pigments could be mixed in an acrylic resin or the like to prepare a filter plate, and this filter plate is mounted on the faceplate of the cathode ray tube. In the case of a "telepanel" type cathode ray tube, these dyes may be mixed in an adhesive resin used for adhering this telepanel serving as a color filter to the faceplate. Examples of the dye used for such an optical filter are acid rhodamine B, rhodamine B, and KAYANALMILLING RED 6B (tradename) available from NIPPON KAYAKU CO., LTD. Examples of the dye added to correct a body color are KAYASET BLUE K-FL having a peak at 675 nm, and a near-infrared absorbent. In addition, an organic pigment using a lake of a pigment such as the dyes described above, or an inorganic pigment such as a mixture of cobalt aluminate and cadmium red can be used. An example of the blue emitting phosphor used in the cathode ray tube of the present invention is ZnS:Ag,Cℓ, and the example of the red emitting phosphor is Y₂O₃:Eu. Example 1 Green pixels consisting of a ZnS:Cu,Aℓ phosphor, blue pixels consisting of a ZnS:Ag,Aℓ phosphor, and red pixels consisting of a Y₂O₃:Eu phosphor having an Eu activation amount of 3.5 mol% with respect to the base material were used to form an emission screen on the inner surface of a faceplate by a known photographic printing method, and a color cathode ray tube was assembled with the emission screen. An alcohol coating solution having the following composition was prepared. The resultant solution was applied to the front surface of the faceplate of the above color cathode ray tube by spin coating and was dried to form an optical filter layer. The transmissivity of this optical filter layer is shown in Fig. 10. An image displayed on this color cathode ray tube was evaluated. The red emission brightness level was increased by 50% as compared with a color cathode ray tube using Y₂O₂S:Eu with an Eu activation amount of 4.5 mol% with respect to the base material. The chromaticity coordinate values fell within the practical range of the Y₂O₂S:Eu phosphor. T₅₈₀₋₆₀₀ = 45%, and T₆₁₅ = 98%, thus satisfying condition T₆₁₅/T₅₈₀₋₆₀₀ ≧ 1.1. In addition absorption peak appeared at 575 nm; T min = 42%, T₄₅₀ = 100%; T₅₃₀ = 72%; T₅₅₀ = 68%; and T₆₁₅ = 98%. The test results satisfy the following conditions: T min ≦ T₅₅₀ ≦ T₅₃₀ 1 ≦ T₄₅₀/T₅₃₀ ≦ 2 1 ≦ T₆₁₅/T₅₃₀ ≦ 2 0.7 ≦ T₄₅₀/T₆₁₅ ≦ 1.43 The BCP value was 1.25, thus providing a sufficiently high contrast level. In Example 1, the optical filter layer is formed on the front surface of the faceplate of the normal cathode ray tube. However, in a "telepanel" cathode ray tube on which a telepanel serving as a color filter is mounted on the front surface of its faceplate, even if a dye such as acid rhodamine B was mixed in an adhesive resin for mounting the telepanel, the same effect as in Example 1 was obtained.

Claims: A color cathode ray tube (1) comprising: an envelope (2) including a faceplate (5) with an inner and outer surfaces and a side wall portion, a neck (3) and a cone (4) connecting the faceplate (5) to the neck (3); an electron gun (7) provided inside the neck (3) for emitting at least one electron beam; a phosphor screen (8) provided on the inner surface of the faceplate (5) and consisting essentially of red, blue, and green emitting phosphors; light filtering means (9) provided in front of the faceplate for selectively transmitting light, characterized in that the red emitting phosphor comprises a Y₂O₃:Eu phosphor, and an Eu amount thereof being not less than 3.0 mol% and not more than 9.0 mol% with respect to a Y₂O₃ amount as a base material; and the light filtering means have the maximum light absorption wavelength in wavelength region of 575 ± 20 nm with respect to the wavelength range from 400nm to 650 nm and satisfy the following relationship: T min ≦ T₅₅₀ ≦ T₅₃₀ 1 ≦ T₄₅₀/T₅₃₀ ≦ 2 1 ≦ T₆₁₅/T₅₃₀ ≦ 2 0.7 ≦ T₄₅₀/T₆₁₅ ≦ 1.43 T₆₁₅/T₅₈₀₋₆₀₀ ≧ 1.1 wherein T₄₅₀, T₅₃₀, T₅₅₀, T₆₁₅, T min and T₅₈₀₋₆₀₀ represent the transmissivities for lights of wavelength of 450 nm, 530 nm, 550 nm, 615 nm, the maximum absorption wavelength in wavelength region of 575 ± 20 nm, and the maximum absorption wavelength in wavelength range of 580 nm to 600 nm, respectively. A cathode ray tube (1) according to claim 1, characterized in that the Eu amount of the Y₂O₃:Eu phosphor is not less than 3.0 mol% and not more than 5.5 mol% with respect to the amount of the base material. A cathode ray tube (1) according to claim 1, characterized in that the light filtering means (9) contains SiO₂ as a major constituent and a colorant. A cathode ray tube (1) according to claim 1, characterized in that the light filtering means (9) contains an acrylic resin as a major constituent and a colorant. A cathode ray tube (1) according to claim 3 or 4, characterized in that the colorant is at least one material selected from the group consisting of a dye, an organic pigment, and an inorganic pigment. A cathode ray tube (1) according to claim 3 or 4, characterized in that the colorant is at least one dye selected from the group consisting of acid rhodamine B and rhodamine B. A cathode ray tube (1) according to claim 4, characterized in that the colorant is at least one organic pigment selected from the group consisting of lakes of the dyes acid rhodamine B and rhodamine B. A cathode ray tube (1) according to claim 4, characterized in that the colorant is an inorganic pigment consisting essentially of a mixture of cobalt aluminate and cadmium red. A cathode ray tube (1) according to claim 1, characterized in that the light filtering means (9) consists essentially of a glass layer formed by using a metal alcoholate containing Si.

Inventors: ITOU TAKEO C O INTELLECTUAL PR, MATSUDA HIDEMI C O INTELLECTUA, TANAKA HAJIME C O INTELLECTUAL, ITOU, TAKEO, C/O INTELLECTUAL PROPERTY DIV., MATSUDA, HIDEMI, C/O INTELLECTUAL PROPERTY DIV., TANAKA, HAJIME, C/O INTELLECTUAL PROPERTY DIV.
Applicants: TOSHIBA KK, KABUSHIKI KAISHA TOSHIBA
Application year: 1990
Main classification: H01J29
IPC codes: H01J29