Cathode ray tube having apertured shadow mask

Information

  • Patent Grant
  • 6566795
  • Patent Number
    6,566,795
  • Date Filed
    Tuesday, January 2, 2001
    23 years ago
  • Date Issued
    Tuesday, May 20, 2003
    21 years ago
Abstract
A cathode ray tube capable of reducing the doming amount and suppressing the occurrence of moire stripes at the same time, which also can prevent the so-called persimmon stone phenomenon from occurring, is provided. In the apertures, the protruding portions that are protruding from end faces in the horizontal direction of the apertures to the inside of the apertures are formed. The protruding portion in the aperture located on the right side of the phosphor surface from the vertical center line of the shadow mask is protruding in the direction toward the peripheral portion on the right side, while the protruding portion in the aperture located on the left side of the phosphor surface is protruding toward the peripheral portion on the left side. Accordingly, the doming amount can be reduced and the occurrence of moire stripes can be suppressed at the same time, while the persimmon stone phenomenon in which the beam spot of an electron beam on the phosphor surface is cut partially can be prevented from occurring.
Description




FIELD OF THE INVENTION




The present invention relates to a shadow mask type cathode ray tube, which is used for a television receiver, a computer display, and the like.




BACKGROUND OF THE INVENTION





FIG. 4

is a cross-sectional view showing one example of a conventional color cathode ray tube. The color cathode ray tube


1


shown in

FIG. 4

includes a substantially rectangular-shaped face panel


2


having a phosphor screen


2




a


on its inner face, a funnel


3


connected to the rear side of the face panel


2


, an electron gun


4


contained in a neck portion


3




a


of the funnel


3


, a shadow mask


6


facing the phosphor screen


2




a


inside the face panel


2


, and a mask frame


7


for fixing the shadow mask


6


. Furthermore, in order to deflect and scan electron beams, a deflection yoke


5


is provided on the outer periphery of the funnel


3


.




The shadow mask


6


plays a role of selecting colors with respect to three electron beams emitted from the electron gun


4


. “A” shows a track of the electron beams. The shadow mask is provided with a number of apertures formed by etching, through which electron beams pass.




In a color cathode ray tube, due to the thermal expansion caused by the impact of the emitted electron beams, the electron beam through aperture is shifted. Consequently, a doming phenomenon occurs. That is, the electron beams passing through the apertures fail to hit a predetermined phosphor correctly, thus causing unevenness in colors. Therefore, a tension force to absorb the thermal expansion due to the temperature increase of the shadow mask is applied in advance, and then the shadow mask is stretched and held to the mask frame. When the shadow mask is stretched and held as mentioned above, even if the temperature of the shadow mask is raised, it is possible to reduce the amount of displacement between an aperture of the shadow mask and phosphor strips of the phosphor screen.





FIG. 5

is a plan view showing an example of a shadow mask


35


to which a tension force is applied mainly in the vertical direction (vertical direction of the screen). Apertures


36


are formed at constant pitches. Reference numeral


37


is referred to as a bridge, which is a portion between respective apertures


36


. The bridge width has an effect on the mechanical strength of the shadow mask. More specifically, the bridge with a narrow width has a weak tension force particularly in the horizontal direction. If the bridge width is increased in order to improve the mechanical strength, the open area of the aperture is reduced, thus deteriorating the luminance intensity.




Furthermore, the vertical pitch of the bridge is related to the doming amount of the shadow mask. The shadow mask is stretched mainly in the vertical direction. Therefore, the thermal expansion in the vertical direction is absorbed by the tension force, while the thermal expansion in the horizontal direction is transmitted in the horizontal direction through the bridges. The doming amount can be reduced by increasing the vertical pitch of the bridge. Therefore, when the vertical pitch of the bridge is increased, the doming amount can be reduced. In this case, however, moire stripes easily occur, thus causing the deterioration of the image quality. The moire stripe means a mutual interference stripe between scanning lines (luminescent lines) of the electron beams arranged at constant intervals and the regular pattern of the electron beam through apertures of the shadow mask.




Furthermore, when the vertical pitch of the bridge is increased, the bridges themselves may appear as dots on the screen, or may be recognized as a pattern in which the bridges are piled up (a brick-like pattern).




On the contrary, when the vertical pitch of the bridge is reduced, moire stripes are suppressed sufficiently and the bridges themselves are not noticeable, but the doming amount is increased.




To solve this problem, as shown in

FIG. 6A

, for example, a shadow mask


40


is proposed in which protruding portions


42




a


,


42




b


protruding in different directions are formed in an aperture


41


. By forming the protruding portions


42




a


,


42




b


, the vertical pitch of the bridge is maintained at a large value, while the occurrence of moire stripes can be suppressed in the same manner as the vertical pitch of the bridge is reduced. In other words, it is possible to reduce the doming amount of the shadow mask to which a tension force is applied mainly in the vertical direction and also to suppress the occurrence of moire stripes at the same time.




Furthermore, a shadow mask provided with slot-shaped apertures shows a so-called “persimmon stone phenomenon”, which is characterized as follows. By taking the vertical center line of the shadow mask as the border, electron beams entering obliquely into apertures located on the right side of the phosphor screen


2




a


(

FIG. 4

) are cut in the vicinity of upper right and lower right corners of the apertures, and electron beams entering obliquely into apertures located on the left side are cut in the vicinity of upper left and lower left corners of the apertures.





FIG. 7A

is a horizontal cross-sectional view showing the vicinity of upper and lower corners of an aperture located on the right side of the phosphor screen by taking the vertical center line of the shadow mask as the border.

FIG. 7A

shows a state in which a portion of an electron beam ray


51


passing through an aperture


50


is cut by an ascending portion


52


of the aperture


50


. In this way, when the electron beam is cut in the vicinity of the upper right and lower right corners of the aperture, as illustrated in

FIG. 7B

, the shape of a beam spot


53


that originally is intended to be of a substantially slot shape is formed into the shape of a persimmon stone. Shaded portions


54




a


and


54




b


are portions where the electron beam ray was cut.




In order to prevent this persimmon stone phenomenon in the vicinity of the upper and lower corners of the apertures, various shapes of apertures are proposed. For example, JP1(1989)-320738A discloses a method for preventing this persimmon stone phenomenon by increasing a width of an open portion (i.e. W in

FIG. 7A

) in the vicinity of upper right and lower right corners of apertures located on the right side of a shadow mask from the vertical center line. Furthermore, JP63(1988)-119139A discloses another method for preventing electron beams from being cut, as shown in

FIG. 7C

, by widening upper and lower end portions a, b of an aperture


55


.




Although the shadow mask


40


shown in

FIG. 6A

can suppress the occurrence of moire stripes with the protruding portions


42




a


,


42




b


by shielding the electron beam in the same manner as the vertical pitch of the bridge is reduced, this shadow mask still suffered from this persimmon stone phenomenon. In other words, as illustrated in

FIG. 6B

, the electron beam is cut in base portions C with regard to the aperture


41


located on the right side of the shadow mask from the vertical center line, and the electron beam is cut in base portions D with regard to the aperture


41


located on the left side from the vertical center line of the shadow mask.




Furthermore, the apertures proposed by JP1(1989)-320738A and JP63(1988)-119139A both try to prevent this persimmon stone phenomenon by changing the aperture shape, but there is a limitation to solve the above problem with the shape.




SUMMARY OF THE INVENTION




It is an object of the present invention to solve the conventional problems described above by providing a cathode ray tube capable of reducing the doming amount and suppressing the occurrence of moire stripes at the same time, and which can prevent the so-called persimmon stone phenomenon from occurring.




To achieve the above object, a cathode ray tube of the present invention includes a shadow mask made of a flat plate provided with a number of apertures, wherein protruding portions protruding in the horizontal direction from an end of the aperture that is closer to the vertical center line of the shadow mask are formed at least in the apertures positioned in the vicinity of both right and left edges of the shadow mask. According to the configuration described above, while the cathode ray tube can reduce the doming amount and suppress the occurrence of moire stripes at the same time, the persimmon stone phenomenon in which the beam spot of an electron beam on the phosphor surface is cut partially can be prevented from occurring.




In the cathode ray tube described above, it is preferable that an end of the aperture that is farther from the vertical center line has dented portions in areas opposing tips of the protruding portions. According to this configuration, the dented portions are formed so that the protruding portions can be lengthened and the area of the aperture can be enlarged at the same time. Thus, the occurrence of moire stripes and the persimmon stone phenomenon can be suppressed even more surely.




Furthermore, it is preferable that the protruding portions are formed almost on the entire shadow mask.




Furthermore, it is preferable that the shadow mask is stretched and held in a state in which a tension force is applied in the vertical direction.




Furthermore, it is preferable that the shadow mask is formed into a curved shape.











BRIEF DESCRIPTION OF THE DRAWINGS





FIG. 1

is a perspective view showing a color-selecting electrode of one embodiment of to the present invention.





FIG. 2A

is a plan view showing a shadow mask of one embodiment of the present invention.





FIG. 2B

is an enlarged view of FIG.


2


A.





FIG. 3

is an enlarged view of a shadow mask in another embodiment according to the present invention.





FIG. 4

is a cross-sectional view showing an example of a color cathode ray tube.





FIG. 5

is a plan view showing an example of a conventional shadow mask.





FIG. 6A

is a plan view showing another example of a conventional shadow mask.





FIG. 6B

is an enlarged view of FIG.


6


A.





FIG. 7A

is a horizontal cross-sectional view showing upper and lower areas of an aperture in a conventional shadow mask.





FIG. 7B

is a plan view showing an example of a conventional beam spot shape.





FIG. 7C

is a plan view showing an example of a conventional aperture shape.











DETAILED DESCRIPTION OF THE INVENTION




Hereinafter, the present invention will be described by way of an embodiment with reference to drawings. Since the construction of the color cathode ray tube described with reference to

FIG. 4

is the same as that in this embodiment, the explanations thereof are not repeated herein.





FIG. 1

is a perspective view showing a color-selecting electrode of one embodiment. A mask frame


10


is a rectangular frame and is made of a pair of long frame supports


11


, facing each other, fixed to a pair of short frames made of elastic members


12


. On the shadow mask


13


, apertures


14


, through which electron beams pass, are formed by etching.




In this drawing, a tension method is employed, and the shadow mask


13


is stretched and held between the supports


11


with a tension force applied mainly in the direction illustrated by arrow Y. The aperture


14


is provided with protruding portions


23


,


24


to be explained later in

FIG. 2A

, which are not shown in this drawing.





FIG. 2A

is a plan view showing one embodiment of a shadow mask.

FIG. 2B

is an enlarged view of one portion in FIG.


2


A. In the shadow mask


20


shown in

FIG. 2

, the vertical direction of the drawing is the vertical direction of the screen, and the horizontal direction is the horizontal direction of the screen. A vertical center line


25


shows the vertical center line of the shadow mask


20


. By taking the vertical center line


25


as the border, the protruding portion


23


is formed in an aperture


21


arranged in an area on the right side of the phosphor screen surface


2




a


(

FIG. 4

) (hereinafter referred to as “the right area”), while the protruding portion


24


is formed in an aperture


22


arranged in an area on the left side of the phosphor screen surface


2




a


(hereinafter referred to as “the left area”). The apertures


21


,


22


neighboring in the vertical direction are linked by a bridge


26


.




The protruding portions


23


,


24


respectively are protruding from one end of the horizontal direction of the apertures


21


,


22


. Both the protruding portions


23


and


24


are protruding in the horizontal directions away from the vertical center line


25


in the apertures


21


,


22


, that is, in the directions toward the right and left peripheries of the shadow mask. More specifically, a base


23




a


of the protruding portion


23


in the right area is formed along an end face


21




a


that is closer to the vertical center line


25


of the aperture


21


. A first opening


27


is formed between the protruding portions


23


neighboring in the vertical direction, and a second opening


28


is formed between a tip


23




b


of the protruding portion


23


and an end face


21




b


of the aperture


21


.




In the left area, the protruding portion


24


is protruding in the opposite direction, and a base


24




a


of the protruding portion


24


in the left area is formed along an end face


22




a


that is closer to the vertical center line


25


of the aperture


22


. A first opening


29


is formed between the protruding portions


24


neighboring in the vertical direction, and a second opening


30


is formed between a tip


24




b


of the protruding portion


24


and an end face


22




b


of the aperture


22


.




By forming such protruding portions


23


,


24


, electron beams can be shielded, so that the same effect can be obtained as the vertical pitch of the bridge


26


being reduced, and the occurrence of moire stripes can be suppressed. In addition, the protruding portions


23


,


24


do not cover up the apertures


21


,


22


completely in the horizontal direction. The tips


23




b


,


24




b


and the end faces


21




b


,


22




b


are separated because the second openings


28


,


30


are formed. Therefore, the thermal expansion in the horizontal direction is not transmitted between the tips


23




b


,


24




b


and the end faces


21




b


,


22




b


, and the doming can be prevented. In other words, according to this embodiment, it is possible to reduce the doming amount of the shadow mask to which a tension force is applied mainly in the vertical direction and also to suppress the occurrence of moire stripes at the same time.




Furthermore, the first opening


27


is formed in a plurality in one aperture


21


in the right area, and each of the first opening


27


functions as one aperture. In other words, it is equivalent to the state in which a plurality of apertures whose vertical pitch is reduced is formed in one aperture


21


.




In this embodiment, the second openings


28


respectively are formed in the upper right portion and in the lower right portion of the first opening


27


. Therefore, the corner portions C as illustrated in

FIG. 6B

are not formed along the end face


21




b


on the right side of the aperture


21


in this drawing.




In other words, the aperture is enlarged in the vicinity of the upper right and lower right corners of the first opening


27


by the second openings


28


, which is equivalent to the state in which a plurality of apertures having enlarged upper right and lower right corners are formed in one aperture


21


.




Thus, electron beams can be prevented from being cut in area portions A of the first opening


27


, and the so-called persimmon stone phenomenon in which the beam spot of an electron beam on the phosphor surface is cut partially can be prevented from occurring.




This means that the left area also has the same configuration except that the left-right relationship is now opposite. Accordingly, the first opening


29


is formed in a plurality in one aperture


22


, and the second openings


30


are formed in the upper left portion and in the lower left portion of the first opening


29


. Therefore, the corner portions D as illustrated in

FIG. 6B

are not formed along the end face


22




b


on the left side of the aperture


22


in this drawing. As a result, electron beams can be prevented from being cut in area portions B of the first opening


29


, and the persimmon stone phenomenon can be prevented from occurring.




According to this embodiment, while the doming amount and the occurrence of moire stripes of the shadow mask can be suppressed at the same time, the persimmon stone phenomenon can be prevented from occurring in which the beam spot of an electron beam on the phosphor surface is cut in the upper and lower corners of one side.




Here, the persimmon stone phenomenon described above is likely to occur in the peripheral portions or in the corners of the shadow mask on the right and left sides where the incident angle of the electron beam is enlarged. Therefore, when the apertures provided with the protruding portions arranged in the manner described above are formed at least in the vicinity of both right and left edges, the effect of preventing the electron beams from being cut can be obtained.




Further, since the incident angle of the electron beam is enlarged also in the vicinity of both upper and lower edges of the shadow mask, it is preferable that the apertures provided with the protruding portions are formed at least in the vicinity of both the right and left edges and both the upper and lower edges of the shadow mask.




Specifically, it is preferable that the apertures with the protruding portions are formed at least in the areas whose lengths in the horizontal direction measured from both the right and left edges of the perforated area of the shadow mask are approximately one third the total length of the perforated area in the horizontal direction, respectively, and in the areas whose lengths in the vertical direction measured from both the upper and lower edges of the perforated area are approximately one tenth the total length of the perforated area in the vertical direction, respectively.





FIG. 3

is an enlarged view of a shadow mask in another embodiment. In this embodiment, a dented portion


32


is formed in an aperture


33


, so that a tip


31




a


of a protruding portion


31


can be lengthened to surely shield the electron beam in the width of the phosphor with the protruding portion


31


. Here, it is not appropriate simply to lengthen the protruding portion without providing the dented portion, because if so, the distance between the tip of the protruding portion and the end face of the aperture is reduced further, which then is difficult to manufacture. In the present embodiment, the dented portion


32


is formed, so that the distance between the tip of the protruding portion and the end face of the aperture can be secured while the protruding portion can be lengthened at the same time. This configuration does not cause any particular manufacturing problems.




Furthermore, in the area where the dented portion


32


is formed, the width of the aperture


33


is wider than in other portions. Therefore, even if electron beams are cut in areas where the horizontal cross section of the aperture


33


has an ascending form, the luminous intensity is not reduced. As a result, the occurrence of moire stripes and the persimmon stone phenomenon can be suppressed even more surely.




The above embodiment was described on the assumption that the shadow mask is stretched and held. However, even if the shadow mask is not stretched and held, the same effect can be obtained with regard to the prevention of electron beams from being cut as described above. Therefore, the present embodiment also is effective for a shadow mask that has a curved surface formed by press molding, which is not stretched and held.




Furthermore, the shape of the protruding portion in the planar direction was illustrated as a rectangular shape in this example, but it is not limited thereto. It is also possible to form the aperture and the protruding portion to have round corners. Alternatively, the protruding portion may be formed so as to protrude gradually from the base to the tip. This kind of gradually protruding shape can be formed easily by the etching method used mainly for the production of shadow masks, so that it is practical.




According to the cathode ray tube of the present invention described above, the protruding portions protruding to the inside of the aperture are formed in the shadow mask, and the protruding portions are protruding in the horizontal directions away from the vertical center line of the shadow mask. As a result, the doming amount can be reduced and the occurrence of moire stripes can be suppressed at the same time. In addition, the persimmon stone phenomenon in which the beam spot of an electron beam on the phosphor surface is cut partially can be prevented from occurring.




The invention may be embodied in other forms without departing from the spirit or essential characteristics thereof. The embodiments disclosed in this application are to be considered in all respects as illustrative and not limiting. The scope of the invention is indicated by the appended claims rather than by the foregoing description, and all changes which come within the meaning and range of equivalency of the claims are intended to be embraced therein.



Claims
  • 1. A cathode ray tube comprising a shadow mask made of a flat plate provided with a number of apertures,wherein protruding portions protruding in the horizontal direction from an end of the aperture that is close to the vertical center line of the shadow mask are formed at least in the apertures positioned in the vicinity of both right and left edges of the show mask, and adjacent protruding portions protrude in a same direction and the aperture does not include a protruding portion at an end of the aperture that opposes a tip of each of the protruding portions.
  • 2. The cathode ray tube according to claim 1, wherein an end of the aperture that is farther from the vertical center line has dented portions in areas opposing tips of the protruding portions.
  • 3. The cathode ray tube according to claim 1, wherein the protruding portions are formed substantially on the entire shadow mask.
  • 4. The cathode ray tube according to claim 1, wherein the shadow mask is stretched and held in a state in which a tension force is applied in the vertical direction.
  • 5. The cathode ray tube according to claim 1, wherein the shadow mask is formed into a curved shape.
Priority Claims (1)
Number Date Country Kind
2000-004982 Jan 2000 JP
US Referenced Citations (6)
Number Name Date Kind
4926089 Moore May 1990 A
5280215 Ohtake et al. Jan 1994 A
5583391 Moore Dec 1996 A
5631520 Inoue et al. May 1997 A
5856725 Ueda Jan 1999 A
6124668 Shoda Sep 2000 A
Foreign Referenced Citations (7)
Number Date Country
0 487 106 May 1992 EP
2 801 136 May 2001 FR
2 351 600 Jan 2001 GB
63-119139 May 1988 JP
1-320738 Nov 1989 JP
1-320738 Dec 1989 JP
9-265916 Oct 1997 JP
Non-Patent Literature Citations (1)
Entry
Dec. 21, 2001 EPO Search Report