Electron gun for cathode ray tube

An electron gun includes a cathode adapted to emit thermal electrons, a first electrode and a second electrode adapted to form a triode portion together with the cathode, a plurality of focusing electrodes, each of said plurality of focusing electrodes being perforated by a plurality of beam passage apertures and an anode electrode, wherein a pitch between ones of said plurality of beam passage apertures of a one of said plurality of focusing electrodes arranged closest to the second electrode is smaller than a pitch between ones of said plurality of the beam passage apertures of a remaining of said plurality of focusing electrodes.

CLAIM OF PRIORITY

This application makes reference to, incorporates the same herein, and claims all benefits accruing under 35 U.S.C. §119 from an application for ELECTRON GUN FOR CATHODE RAY TUBE, earlier filed in the Korean Intellectual Property Office on 11 Mar. 2005 and there duly assigned Ser. No. 10-2005-0020518.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an electron gun for a cathode ray tube display (CRT), and in particular, to an electron gun for a CRT that enhances the focusing characteristics by improving the image spreading of red, green and blue colors.

2. Description of Related Art

Generally, a CRT includes an electron gun for emitting electron beams, a deflection yoke for deflecting the electron beams, a shadow mask for color-selecting the electron beams, and a panel having a phosphor layer on an inner side. The electron beams emitted from the electron gun are deflected by the deflection magnetic field of the deflection yoke, and the deflected electron beams pass through the color-selecting shadow mask, followed by colliding with green, blue and red phosphors of the phosphor layer to emit light to display the desired images.

The electron gun for a CRT includes a cathode for emitting thermal electrons, a heater installed at the cathode to heat the cathode and emit thermal electrons, and a plurality of electrodes for focusing and accelerating the thermal electrons emitted from the cathode. The electrodes include first and second electrodes forming a triode portion together with the cathode, a plurality of focusing electrodes having focusing voltages applied thereto, and an anode electrode receiving a high anode voltage. The cathode, the first electrode, the second electrode, the focusing electrodes and the anode electrode are partitioned into three domains corresponding to the red, green and blue phosphors.

With the in line electron gun where the three domains are linearly arranged, the white balance image spreading occurs to a large extent due to the arrangement structure thereof, and the left and right difference occurs to a significantly extent with the electron beams placed at the left and the right sides corresponding to the red and the blue colors. For instance, for the electron beams corresponding to the red color, a relatively small beam is formed at the left side of the screen, and a relatively large beam is formed at the right screen side. Furthermore, for the electron beams corresponding to the blue color, a relatively large beam is formed at the left screen side, and a relatively small beam is formed at the right screen side. Accordingly, in the case of a white state where all the electron gun portions corresponding to the red, green and blue colors are operated, the peripheral beam focusing is deteriorated compared to that with one electron gun portion.

With the widening of the deflection angle to slim the CRT (the maximum deflection angle reaching up to 110° or more), the electron beams corresponding to the red color at the center of the screen represent the left sided image spreading, and the electron beams corresponding to the blue color represent the right sided image spreading, thereby differing from the CRT with the maximum deflection angle of 102-106°.

The electron beams corresponding to the red color at the first quadrant (the right upper side) of the screen represent the right sided image spreading, and the electron beams corresponding to the blue color represent the left sided image spreading. That is, in the case of a CRT having a widened deflection angle, the image spreading of the electron beams at the center and at the periphery of the screen is directed opposite to that of earlier CRTs. What is therefore needed is a new design for an electron gun that is better suited for the newer svelte, flat panel wide screen high deflection angle CRTs where less image spreading is produced and a higher quality image is produced.

SUMMARY OF THE INVENTION

It is therefore an object of the present invention to provide an improved design for an electron gun that is suited for high deflection angle CRTs.

It is further an object of the present invention to provide a CRT employing the novel electron gun.

It is also an object of the present invention to provide an electron gun for a CRT which improves the image spreading deviation at the periphery of a high deflection angle CRT screen.

It is yet an object of the present invention to provide a high deflection angle CRT with improved image spreading deviation at the periphery of the screen.

These and other objects may be achieved by an electron gun for a CRT that includes a cathode adapted to emit thermal electrons, a first electrode and a second electrode adapted to form a triode portion together with the cathode, a plurality of focusing electrodes, each of said plurality of focusing electrodes being perforated by a plurality of beam passage apertures and an anode electrode, wherein a pitch between ones of said plurality of beam passage apertures of a one of said plurality of focusing electrodes arranged closest to the second electrode is smaller than a pitch between ones of said plurality of the beam passage apertures of a remaining of said plurality of focusing electrodes.

The pitch between ones of the plurality of beam passage apertures perforating the one of said plurality of focusing electrodes arranged closest to the second electrode can be between 5.55 mm and 5.59 mm. A pitch between ones of said plurality of beam passage apertures perforating the remaining of said focusing electrodes can be 5.60 mm. The pitch between ones of the plurality of beam passage apertures perforating the one of said plurality of focusing electrodes arranged closest to the second electrode can be established by controlling the location of the beam passage apertures placed at the left and the right sides of the focusing electrode. The pitch of the beam passage apertures of the one of the plurality of focusing electrodes arranged closest to the second electrode can be varied by differentiating a size of a beam passage aperture placed at the center of the one of the plurality of focusing electrodes arranged closest to the second electrode from a size of the beam passage apertures arranged at the left and the right sides of the one of the plurality of focusing electrodes arranged closest to the second electrode.

A shape of the beam passage apertures arranged in the one of the plurality of focusing electrodes arranged closest to the second electrode can be one of a rectangle, an oval and a track elongated vertical to an arrangement of the beam passage apertures. A shape of the beam passage apertures arranged in the one of the plurality of focusing electrodes arranged closest to the second electrode can have a circular center and two sides extended from the circular center vertical to an arrangement of the beam passage apertures and communicated with the circular center. The extended sides of the beam passage apertures can have a shape selected from the group consisting of a rectangle, a semi-circle, and an oval.

According to another aspect of the present invention, there is provided a cathode ray tube display (CRT) that includes a panel, a funnel and a neck connected to each other to form a vacuum vessel, a phosphor layer arranged on an inner surface of the panel and having a pattern, an electron gun arranged within the neck and adapted to emit and focus electron beams, a deflection yoke arranged around an outer circumference of the funnel and adapted to deflect the electron beams emitted from the electron gun and a shadow mask arranged within the panel and adapted to color-selectively pass the electron beams emitted from the electron gun so that the electron beams land on relevant phosphors of the phosphor layer, the electron gun being as stated above.

DETAILED DESCRIPTION OF THE INVENTION

With the widening of the deflection angle to slim the CRT up to 110° or more as shown inFIG. 8, the electron beams corresponding to the red color at the center of the screen represent the left sided image spreading, and the electron beams corresponding to the blue color represent the right sided image spreading, thereby differing from the CRT with the maximum deflection angle of 102-106°. As shown inFIG. 9, the electron beams corresponding to the red color at the first quadrant (the right upper side) of the screen represent the right sided image spreading, and the electron beams corresponding to the blue color represent the left sided image spreading. That is, in the case of a CRT with widened deflection angle, the image spreading of the electron beams at the center and at the periphery of the screen is directed opposite to that with the conventional CRT.

Turning now toFIG. 1,FIG. 1is a view of a CRT according to an embodiment of the present invention. The CRT ofFIG. 1includes a panel12, a funnel14and a neck16serially connected to each other to form a vacuum vessel. A phosphor layer13is formed on the inner surface of the panel12with a pattern of red, blue and green phosphors. An electron gun20is installed in the neck16to emit and focus electron beams. A deflection yoke15is mounted around the outer circumference of the funnel14to deflect the electron beams emitted from the electron gun20. A shadow mask18is installed within the panel12to color-selectively pass the electron beams emitted from the electron gun20, allowing them to land on the phosphors of the phosphor layer13.

The phosphor layer13is a circular or a rectangular dot or stripe-pattern of red R, green G and blue B phosphors on the inner surface of the panel12with a black matrix BM in between. The shadow mask18is fitted to the panel12via a frame17so that it is spaced apart from the phosphor layer13by a distance. A plurality of beam passage apertures19are formed in the shadow mask18and have a pattern allowing for the passage of the electron beams. In order to make the CRT slim, the deflection angle of the deflection yoke15is widened so that the maximum value thereof reaches 110° or more (compared to a CRT with a maximum deflection angle of 102-106°). Other structural components of the CRT are the same as those related to the common one, and detailed explanation thereof will be omitted.

With the above structured CRT, the electron beams emitted from the electron gun20are deflected by the deflection magnetic field produced by the deflection yoke15. The electron beams pass through the beam passage apertures19of the color selecting shadow mask18, and collide against the green, blue and red phosphors of the phosphor layer13so that the phosphors are excited and emit light, thus displaying the desired screen images.

As shown inFIGS. 2 and 3, in an electron gun20for a CRT according to an embodiment of the present invention, the electron gun20includes a cathode22for emitting thermal electrons, first and second electrodes24and26forming a triode portion together with the cathode22, a plurality of focusing electrodes30, and an anode electrode28. The first and the second electrodes24and26, the plurality of focusing electrodes30and the anode electrode28are fixed to a bead glass21. The focusing electrodes30can include from2to8individual electrodes.

As shown inFIG. 4, the pitch S between the beam passage apertures31perforating the first focusing electrode32(the focusing electrode closest to the second electrode26) is smaller than the pitch S between the beam passage apertures31perforating the other focusing electrodes34,36and38. The pitch S between the beam passage apertures31of the first focusing electrode32is established to satisfy the condition 5.55 mm≦S≦5.59 mm.

The pitch S between the beam passage apertures31refers to the distance between a center line of the beam passage aperture31going through the center of the focusing electrode32and the center lines of the beam passage apertures31located at the left and the right sides of the focusing electrode32. The beam passage apertures31placed at the left and the right sides of the focusing electrode32are shaped symmetrical to each other left and right with respect to the center line of the beam passage aperture31going through the center of the focusing electrode32. Regarding the focusing electrodes34,36and38other than the first focusing electrode32, the pitch S between the beam passage apertures31is established to be 5.60 mm.

In order to provide for a slim CRT, the deflection angle is widened to at least 110° so that the distance between the electron gun20and the phosphor layer13of the panel12(the tube length) becomes shortened. Accordingly, the electron beams are shaped at the center and at the periphery of the screen opposite to each other, and the focusing of the electron beams at the center of the screen is freely achieved by the shortened tube length. Consequently, it becomes possible to reduce the pitch S between the beam passage apertures31of the first focusing electrode32, thus improving the image spreading of the electron beams at the periphery of the screen.

The pitch S between the beam passage apertures31of the first focusing electrode32is established by controlling the location of the beam passage apertures31placed at the left and the right sides of the first focusing electrode32. Furthermore, the pitch S between the beam passage apertures31may be varied by differing the sizes of the beam passage apertures31located at the left and the right sides of the first focusing electrode32from the size of the beam passage aperture31placed at the center of the first focusing electrode32. As shown inFIG. 4, the beam passage aperture31formed in the first focusing electrode32have a rectangle shape, but could instead have an oval or a track shape that is elongated in the vertical direction to the arrangement of the beam passage apertures31.

As shown inFIG. 5, the beam passage aperture31formed in the first focusing electrode32can have a circular center34and two sides33extending from the circular center34vertically to the arrangement of the beam passage apertures31, so that they are communicated with the circular center34. The extended sides33can instead take on other shapes, such as rectangular, semi-circular or oval.

When the pitch S and shape of the beam passage apertures31of the first focusing electrode32are designed as above, the result is the electron beams ofFIGS. 6 and 7. InFIGS. 6 and 7, the electron beams corresponding to the red color at the center of the screen is increased in the left image spreading, and the electron beam corresponding to the blue color is increased in the right image spreading. By contrast, as known from the comparison between the structures shown inFIGS. 7 and 9, with the electron beams in the first quadrant (the right upper side) of the screen, the electron beam corresponding to the red color is decreased in the left image spreading, and the electron beam corresponding to the blue color is decreased in the right image spreading, thus reducing the difference between the red and the blue colors.

With the usage of the electron guns20where the pitch S of the beam passage apertures31of the first focusing electrode32was varied to be 5.57 mm, 5.58 mm, 5.60 mm, 5.63 mm and 5.65 mm, the image spreading of the electron beams corresponding to the red color at the center and in the first and second quadrants of the screen was measured on the left and right sides thereof around the central point, and listed in Table 1.

As illustrated in Table 1, as the pitch S of the beam passage apertures31of the first focusing electrode32is decreased, the left and right difference in the first and the second quadrants of the screen is significantly reduced. This can also be seen by comparing the photographs ofFIGS. 9 and 7. In the electron beam image shown inFIG. 9, when the pitch S of the beam passage apertures31is established to be 5.63 mm, the left and the right sizes (roughly indicated by the red oval) largely differ from each other. By contrast, in the electron beam image shown inFIG. 7, when the pitch S of the beam passage apertures31is established to be 5.57 mm, the left and the right sizes (roughly indicated by the red oval) are similar to each other.

When the above structured electron gun is applied to the CRT where the deflection angle is increased to a maximum value of 110° or more to obtain a svelte device (compared to the maximum deflection angle of 102-106° for a CRT), the obtainable effect becomes further enhanced.

With the electron gun for a CRT according to the present invention, the pitch of the beam passage apertures of the first focusing electrode is established to be smaller than that of other focusing electrodes so that the beam spreading at the periphery of the screen can be improved. Accordingly, the electron beams corresponding to the red and the blue colors are minimized in the deviation of beam spreading, and the focusing is improved, thereby enhancing the display image quality.