Cathode-ray tube having an asymmetric slot formed in a screen grid electrode of an inline electron gun

An inline electron gun for a cathode-ray tube includes a plurality of cathodes, a control grid, a screen grid and a main focus lens arranged successively in alignment with the cathodes for focusing a plurality of electron beams along beam paths onto a screen. The screen grid has a functional grid area with a given thickness. A recessed portion is formed within the functional grid area. A plurality of apertures are formed within the recessed portion of the screen grid. The recessed portion is surrounded by a peripheral rim which is in proximity to the outer apertures thereby affecting the electrostatic field in the vicinity of the outer electron beam paths.

BACKGROUND OF THE INVENTION 
This invention relates to cathode-ray tubes, and particularly to color 
cathode-ray tubes of the type useful in home television receivers and 
color display tubes, and to inline electron guns therefore having a high 
degree of insensitivity to deflection defocusing of the electron beams. 
An inline electron gun is one designed to generate at least two, and 
preferably three, electron beams in a common plane and to direct the beams 
along convergent paths to a small spot on the screen. In one type of 
inline electron gun, such as that shown in U.S. Pat. No. 3,772,554, issued 
to R. H. Hughes on Nov. 13, 1973, the main electrostatic focusing lenses 
for focusing the electron beams are formed between two electrodes referred 
to as the first and second accelerating and focusing electrodes. These 
electrodes include two cup-shaped members having the bottoms of the 
members facing each other. Three apertures are included in each cup bottom 
to permit passage of three electron beams and to form three separate main 
focus lenses, one for each electron beam. In such electron guns, static 
convergence of the outer beams with respect to the center beam is usually 
attained by offsetting the outer apertures in the second focusing 
electrode with respect to the outer apertures in the first focusing 
electrode. 
An inline electron gun wherein two electrostatic focusing lenses are 
utilized to form an effective larger main focus lens is described in a 
copending U.S. patent application Ser. No. 485,860, filed on Apr. 18, 
1983, entitled, "Color Picture Tube Having An Improved Inline Electron 
Gun", by D. J. Bechis, et al., and assigned to the same assignee as the 
present invention. In the Bechis et al. copending patent application, the 
third and fifth electrodes from the cathode are electrically 
interconnected and the fourth and sixth electrodes are electrically 
interconnected. Facing portions of the fifth and sixth electrodes each 
include a peripheral rim and three separate inline apertures therein set 
back from the rim. The peripheral rims are elongated in the inline 
direction of the inline apertures and form an astigmatic focus field. This 
field may be matched to an astigmatic beam forming region formed by the 
first and second electrodes from the cathode. 
It has been noted that the horizontal beam landing locations of the outer 
electron beams, in color picture tubes having the above-described electron 
guns, change with changes in the focus voltage applied to the electron 
guns. It therefore is desirable to improve such inline electron guns to 
eliminate, or at least reduce, this horizontal convergence sensitivity to 
focus voltage changes. 
Copending U.S. patent application Ser. No. 461,584, filed on Jan. 27, 1983 
by H. Y. Chen and assigned to the assignee of the present invention, 
discloses a screen grid structure shown in FIG. 3 of the copending 
application for reducing the horizontal convergence sensitivity of the 
inline electron gun to focus voltage changes. The screen grid structure 
disclosed in the copending Chen patent application utilizes a pair of 
reconvergence slots formed in the first accelerating and focusing 
electrode side of the screen grid electrode. The reconvergence slots are 
formed closely to and inwardly from the outer apertures in the screen grid 
electrode and cause a refraction of the electrostatic beam path between 
the screen grid electrode and the first accelerating and focusing 
electrode to compensate for the offset refraction within the main lens of 
the electron gun. 
An alternative screen grid structure for reducing the sensitivity of the 
inline electron gun to focus voltage changes is also disclosed in 
copending U.S. patent application Ser. No. 492,044 entitled, "Cathode Ray 
Tube Having Asymmetric Slots Formed In A Screen Grid Electrode Of An 
Inline Electron Gun", filed on May 6, 1983, by H. Y. Chen and assigned to 
the assignee of the present invention. In the alternative screen grid 
structure, asymmetric depressions are formed about the outer apertures in 
the first accelerating and focusing electrode side of the screen grid 
electrode. In one embodiment, the depressions are transverse slots which 
also reduce vertical flare which appears on the screen of the tube as an 
undesirable low intensity tail or smear extending from a desirable intense 
core of the electron beam. Flare is common in tubes having a deflection 
angle in excess of 90 degrees. 
While the screen grid structures described in the Chen copending patent 
applications are satisfactory for reducing the horizontal sensitivity of 
the outer beams with respect to focus voltage changes, a simpler structure 
that can be easily and inexpensively produced is desired. 
SUMMARY OF THE INVENTION 
An inline electron gun for a cathode-ray tube includes a plurality of 
cathodes, a control grid, a screen grid, and electron lens means arranged 
successively in alignment with the cathodes for focusing a plurality of 
electron beams along beam paths onto a screen. The screen grid has a 
functional grid area with a given thickness. A recessed portion is formed 
within the functional grid area. A plurality of apertures are formed 
within the recessed portion of the screen grid. The recessed portion is 
surrounded by a peripheral rim which is in proximity to the outer 
apertures thereby affecting the electrostatic field in the vicinity of the 
outer electron beam paths.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
FIG. 1 is a plan view of a rectangular color cathode-ray tube 10 having a 
glass envelope 11 comprising a rectangular faceplate panel or cap 12 and a 
tubular neck 14 connected by a rectangular funnel 16. The panel comprises 
a viewing faceplate 18 and peripheral flange or sidewall 20 which is 
sealed to the funnel 16. A mosaic three-color phosphor screen 22 is 
carried by the inner surface of the faceplate 18. The screen 22 is 
preferably a line screen with the phosphor lines extending substantially 
perpendicular to the high frequency raster line scan of the tube (normal 
to the plane of FIG. 1). Alternately, the screen could be a dot screen as 
is known in the art. A multiapertured color selection electrode or shadow 
mask 24 is removably mounted, by conventional means, in predetermined 
spaced relation to the screen 22. An improved inline electron gun 26, 
shown schematically by dotted lines in FIG. 1, is centrally mounted within 
the neck 14 to generate and direct three electron beams 28 along spaced 
coplanar convergent paths through the mask 24 to the screen 22. 
The tube of FIG. 1 is designed to be used with an external magnetic 
deflection yoke, such as the yoke 30 schematically shown surrounding the 
neck 14 and funnel 16 in the neighborhood of their junction. When 
activated, the yoke 30 subjects the three beams 28 to vertical and 
horizontal magnetic flux which cause the beams to scan horizontally and 
vertically, respectively, in a rectangular raster over the screen 22. The 
initial plane of deflection (at zero deflection) is shown by the line P--P 
in FIG. 1 at about the middle of the yoke 30. For simplicity, the actual 
curvature of the deflected beam paths in the deflection zone is not shown 
in FIG. 1. A readjustment or change in focus voltage from the optimum 
focus voltage changes the focus voltage to ultor voltage ratio of the 
electron gun and results in a change in the relative strength or focal 
length of the main electrostatic focus lenses with a resulting 
misconvergence of the outer beams relative to the center beam. 
The details of the improved electron gun 26 are shown in FIG. 2. The gun 
comprises two glass support rods 32 on which various electrodes are 
mounted. These electrodes include three equally spaced coplanar cathodes 
34 (one for each beam), a beam forming region comprising a control grid 
electrode 36 (G1) and a screen grid electrode 38 (G2), and a main lens 
assembly comprising a first focusing electrode 40 (G3), a second focusing 
electrode 42 (G4), a third focusing electrode 44 (G5), and a fourth 
focusing electrode 46 (G6), spaced along the glass rods 32 in the order 
named. A shielding cup 48 is attached to the G6 electrode 46. All of the 
electrodes have three inline apertures in them to permit passage of three 
coplanar electron beams. The G1 grid 36 and the G2 grid 38 are parallel 
plate members that can include embossing therein which add strength to the 
members and can influence the behavior of the electron beams. In addition 
to three inline apertures 50, the G1 grid 36 may also include three slots 
52 superposed on the apertures, on the side of the grid 36 facing the G2 
grid 38. The purpose of the slots 52 will be disclosed hereinafter. The 
elongated dimension of the slots 52 extends in a direction perpendicular 
to the inline direction of the apertures. The construction of the main 
lens assembly is disclosed in the above-referenced Bechis et al. copending 
patent application, incorporated by reference herein for the purpose of 
disclosure. 
The facing closed ends of the G5 electrode 44 and the G6 electrode 46, as 
shown in FIG. 2, have large recesses 54 and 56, respectively, therein. The 
recesses 54 and 56 set back the portion of the closed end of the G5 
electrode 44 that contains three apertures 58 from the portion of the 
closed end of the G6 electrode 46 that contains three apertures 60. The 
remaining portions of the closed ends of the G5 electrode 44 and the G6 
electrode 46 form rims 62 and 64, respectively, that extend peripherally 
around the recesses 54 and 56. The rims 62 and 64 are the closest portions 
of the two electrodes 44 and 46 to each other. 
The G4 electrode 42 is electrically connected by a lead 66 to the G6 
electrode 46 and the G3 electrode 40 is electrically connected by a lead 
68 to the G5 electrode 44, as shown in FIG. 2. Separate leads (not shown) 
connect the G3 electrode 40, the G2 grid electrode 38, the G1 grid 
electrode 36, the cathodes 34 and the cathode heaters to a base 100 (shown 
in FIG. 1) of the tube 10 so that these components can be electrically 
excited. Electrical excitation of the G6 electrode 46 is obtained by a 
contact between the shield cup 48 and an internal conductive coating in 
the tube which is connected to an anode button (not shown) extending 
through the funnel 16. 
FIGS. 2, 3, 4 and 5 illustrate in detail a portion of the beam forming 
region of the electron gun 26. The G2 electrode 38 has a functional grid 
area 70 with three apertures 72 formed therethrough and aligned with the 
apertures 50 in the G1 electrode 36. A pair of securing members 74 extend 
from opposite sides of the functional grid area 70 to attach the electrode 
38 to the glass support rods 32. The functional grid area 70 includes a 
transversely disposed recessed portion 76 through which the apertures 72 
are formed. A peripheral rim 78 surrounds the apertures 50 and extends 
between the recessed portion 76 and the functional grid area 70 of the G2 
electrode 38. The recessed portion 76 and the peripheral rim 78 are 
symmetric with respect to the center aperture 72 but asymmetric with 
respect to the two outer apertures 72. 
In the preferred embodiment, the apertures 72 have a diameter of 0.64 mm 
(25 mils) and are laterally spaced apart a distance of 5.08 mm (200 mils) 
center-to-center. The recessed portion 76 has an overall lateral 
dimension, or length, of about 12.50 mm (492 mils) and a maximum 
transverse dimension, or width, of about 3.81 mm (150 mils). The maximum 
width of the recessed portion 76 extends laterally outwardly about 3.94 mm 
(155 mils) from opposite sides of the center aperture 72 to form a 
substantially rectangularly-shaped central part. The ends of the recessed 
portion 76 form an angle, .theta., of about 30.degree. with the horizontal 
and are thus substantially triangularly shaped with the apex of each of 
the triangularly-shaped end parts being smoothly curved and having a 
radius of about 1.168 mm (46 mils) measured from the center of the outer 
apertures. The G2 electrode 38 has a thickness of about 0.71 mm (28 mils) 
and the recessed portion 76 has a depth of about 0.15 mm (6 mils). The 
peripheral rim 78 has a shape which forms an angle, .phi., of about 
63.degree. with a surface of the electrode. 
As shown in FIG. 5, electrostatic equipotential field lines 80 extend 
between the G2 electrode 38 and the G3 electrode 40 of the electron gun 
26. The asymmetric shape and the depth of the recessed portion 76 of 
electrode 38 as well as the proximity of the peripheral rim 78 to the 
outer apertures 72 affect the electrostatic field in the vicinity of outer 
electron beams by tilting the field lines 80 within the recessed portion 
76 thereby causing the outer electron beams to horizontally converge 
toward the center electron beam passing through the center aperture (not 
shown). The three electron beams are unperturbed in the vertical direction 
because of the vertical symmetry of the recessed portion 76 and the 
substantially greater spacing between the apertures 72 and the peripheral 
rim 78 in the vertical direction. Thus, the recessed portion 76 affects 
only the horizontal convergence of the outer electron beams for changes in 
focus voltage. The strength of the aforementioned effect is governed by 
the depth of the recess and the radius of the triangular end parts 
thereof. The greater the radius, the farther removed from the outer 
apertures 72 is the peripheral rim 78, and the deeper the recess must be 
to affect the paths of the electron beams. In tubes having deflection 
angles of not greater than 90.degree., vertical flare is not a problem. 
However, in tubes having deflection angles in excess of 90.degree., the 
addition of the slots 52 superposed on the apertures 50 of the G1 
electrode 36 facing the G2 electrode 38 will reduce vertical flare. Such a 
structure is disclosed in the above-referenced Bechis, et al. copending 
patent application. 
A second embodiment of the present novel G2 electrode 138 is shown in the 
inline bipotential electron gun 126 of FIG. 6. The electron gun 126 
comprises two glass support rods 132 (one shown) on which various 
electrodes are mounted. These electrodes include three equally spaced 
coplanar cathode assemblies 134 (one for each beam), a control grid 
electrode 136 (G1), a screen grid electrode 138 (G2), a first accelerating 
and focusing electrode 140 (G3), and a second accelerating and focusing 
electrode 142 (G4), spaced along the glass rods 132 in the order named. 
All of the post-cathode electrodes have at least three inline apertures in 
them to permit passage of three coplanar electron beams. The main 
electrostatic focusing lens in the gun 126 is formed between the G3 
electrode 140 and the G4 electrode 142. The G3 electrode 140 is formed 
with two cup-shaped elements 144 and 146, the open ends of which are 
attached to each other. The G4 electrode 142 also is cup-shaped, but has 
its open end closed with a shield cup 148. The portion of the G4 electrode 
142 facing the G3 electrode 140 includes three inline apertures 150, the 
outer two of which are slightly offset outwardly from corresponding 
apertures 152 in the G3 electrode 140. The purpose of this offset is to 
cause the outer electron beams to converge with the center electron beam. 
However, misconvergence can occur if the focus voltage on the G3 electrode 
140 is changed significantly from the optimum focus voltage utilized 
during the attachment of the yoke (not shown). The side of the G3 
electrode 140 facing the G2 electrode 138 includes three apertures 154 
which are aligned with apertures 156 in the G1 electrode 136 and with 
apertures 158 in the G2 electrode 138. 
In the alternative embodiment of electron gun 126, the apertures 158 of the 
G2 electrode 138 have a diameter of about 0.64 mm (25 mils) and are 
laterally spaced apart a distance of 6.60 mm (260 mils) center-to-center. 
The G2 electrode 138 is similar to the above-described G2 electrode 38 
except that the length and width of the recessed portion 176 are scaled-up 
to correspond to the larger lateral spacing between the electron beam 
apertures in the bipotential electron gun 126.