Background of the Invention
1. Field of the Invention
This invention relates to a color picture tube with a magnetic focusing device which provides an improved circularity of an electron beam spot.
2. Cross-Reference to Related Application
In a focusing device for focusing electron beams in a color picture tube with electron guns for red, blue and green arranged in a row, which is disclosed in U.S. application Ser. No. 917,179 filed by one of the present applicants on June 20, 1978 and assigned to the same assignee, a color picture tube is provided at the neck portion with a couple of magnetic members having through-holes permitting the electron beams to pass therethrough and disposed separately in the tube axial direction, and a magnetizing means for magnetizing the respective magnetic members, thereby to form focusing magnetic lenses in spaces between pairs of through-holes in which the paired holes are opposite to each other.
The magnetic focusing device will further be described with reference to FIG. 1 and FIGS. 2a and 2b. FIG. 1 shows a longitudinal sectional view of an inline type three-gun color picture tube with the magnetic focusing device, FIG. 2a shows an enlarged sectional view of a neck portion of the tube shown in FIG. 1, and FIG. 2b shows an enlarged cross sectional view taken along line IIa--IIb of FIG. 1. In the figures, reference numerals 1, 2 and 3 designate electron guns for red, green and blue for emitting red, green and blue electron beams 91 to 93, respectively; 4 a glass tube portion of a cathode ray tube; 5 a tubular permanent magnet disposed around the glass tube portion 4; 6 and 7 magnetic members of high permeability with through-holes 61 to 63 and 71 to 73 through which the electron beams 91, 92 and 93 pass; 8 a fluorescent screen. A magnetic flux emanating from the N pole of the tubular permanent magnet 5 enters the tubular part 74 of the magnetic member 7, emanates from the holes 71, 72 and 73 toward the holes 61, 62 and 63 of the magnetic member 6, enters again the magnetic member 6, emanating from the tubular part 64 of the magnetic member 6, and returns to the S pole of the tubular permanent magnet 5. Therefore, the periphery of each of holes 71 to 73 is magnetized in an S pole while the periphery of each of holes 61 to 63 is magnetized in an N pole. As a result, focusing magnetic fields are formed between the respective pairs of the holes 61 and 71, 62 and 72, and 63 and 73, respectively.
With this magnetic focusing device, the magnetic field component in the direction (X direction) in which the electron guns are arranged, is weaker than that in the direction (Y direction) orthogonal to the X direction. Therefore, the focusing magnetic lenses formed are not symmetrical with respect to the tube axis. In the case of the focusing magnetic lens for the central electron beam 92, the magnetic flux in the X direction which passes through the magnetic member 7 to reach the hole 72 is partly emitted from the adjacent holes 71 and 73, with the result that the magnetic field in the X direction is weaker than that in the Y direction, by about 10% which is confirmed by our experiment. Accordingly, the focusings of the electron beams 91, 92 and 93 in the X direction are different from those in the Y direction, so that the beam spots of those beams are each not circular and are flatly deformed in the Y direction to have an elliptical shape in the X direction. When the electron beam passes through the focusing magnetic field, there is generated a rotational force rotating about its center of the beam traveling path. By the rotational force generated, the beam spot flatly deformed rotates and then impinges upon the fluorescent screen.
When the spot is flatly deformed, the resolution in the widened direction of the beam spot is considerably deteriorated and further the adjacent focusings are adversely affected to a great extent.
Summary of the Invention
Accordingly, an object of the invention is to provide a color picture tube with a magnetic focusing device which minimizes the deterioration of the resolution due to the flat deformation of the beam spot.
To achieve the above object, a magnetic flux concentration means are provided near the through-holes of the magnetic members. The through-holes are aligned in a given direction. The magnetic field in the direction of the hole alignment, which is weakened due to the presence of the holes, is intensified by the magnetic flux concentration means, so that the weakened magnetic field is compensated and focusing magnetic fields symmetrical with the axes thereof are obtained.
Brief Description of the Drawings
FIG. 1 shows a longitudinal sectional view of an in-line type three-gun color picture tube with a magnetic focusing device.
FIG. 2a shows an enlarged sectional view of a neck portion of the color picture tube shown in FIG. 1.
FIG. 2b shows an enlarged cross sectional view taken along line IIb--IIb of FIG. 1.
FIG. 3a shows an enlarged sectional view of a neck portion of a color picture tube with a magnetic focusing device which is an embodiment according to the invention.
FIG. 3b shows an enlarged cross sectional view taken along line IIIb--IIIb of FIG. 3a.
FIG. 4 shows an enlarged cross sectional view of a neck portion of a color picture tube with a magnetic focusing device which is another embodiment according to the invention.
Description of the Preferred Embodiments
In FIGS. 3a to 3b, reference numerals 21 to 24 designate magnetic pieces disposed on the peripheries of the through-holes and on and along an alignment of the holes 61 to 63; 25 to 28 magnetic pieces disposed on the peripheries of small holes 71 to 73 on and along an alignment of the holes 71 to 73. The magnetic pieces 21 to 24 and 25 to 28 are fixed to magnetic members 6 and 7, respectively, by an adhesive agent or the like. The magnetic pieces 21 to 24 and 25 to 28 disposed on the alignments of the through-holes 61 to 63 and 71 to 73, concentrate the magnetic flux in the alignment direction, so that the magnetic field in the alignment direction is intensified as compared with the case where the magnetic pieces 21 to 24 and 25 to 28 are not provided. When those magnetic pieces 21 to 24 and 25 to 28 are not used, the X directional components of focusing magnetic fields formed between the respective pairs of the through-holes 61 and 71, 62 and 72, and 63 and 73 are weaker than the Y directional components thereof. For this, these focusing magnetic fields are not symmetrical with respect to their axes. On the other hand, when the magnetic pieces 21 to 28 are used as in this embodiment, the X directional components of the magnetic field, which is weakened when those pieces are not used, is intensified and the weakened magnetic field is compensated. As a result, the focusing magnetic fields formed between the respective pairs of the through-holes 61 and 71, 62 and 72, and 63 and 73 are symmetrical with respect to the axes thereof to prevent the electron beams passing therethrough from being flatly deformed in the cross section. The magnetic pieces added may be disposed not only between the through-holes but also on the upper side, in the X direction, of the through-holes 61 and 71 or on the lower side, in the direction of the through-holes 63 and 73. As shown in FIG. 4, further, rectangular magnetic pieces 34 and 36 may be placed between the through-holes 71 and 72, and 72 and 73. In that case, the magnetic piece 34 serves as those pieces 27 and 28 in FIGS. 3a and 3b. Moreover, in place of using the magnetic pieces 21 to 28, 34 and 36, the upper and lower edges (Y direction) of each of the through-holes 71, 72 and 73 are cut away to be thinner in the thickness so that the focusing magnetic field in the Y direction is not more intensified than that in the X direction.