CATHODE RAY TUBE INCLUDING A MAGNETIC FOCUSING LENS

Abstract: Monochrome cathode ray tube including a magnetic focusing device (26) provided with means for generating a static magnetic focusing field. These means surround the neck (23) of the cathode ray tube (20) without contacting this neck and a system of correction coils (27,28,29) for generating an additional focusing field and 2-, 4- and/or 6-pole fields is provided coaxially between these means and the neck of the tube.

Description: The invention relates to a monochrome cathode ray tube provided at one end with an electron gun and at the end located oppositely thereto with a display screen having a phosphor layer, a deflection unit provided around the neck of the display tube and a magnetic focusing device provided around the neck of the display tube between the electron gun and the deflection unit, which device has means for generating a static magnetic field. When focusing electrons in a cathode ray tube, two types of lenses are used, viz. electrostatic or magnetic lenses. To achieve a good definition it is desirable to achieve a very good extent of focusing (= small electron spot or high resolution). Magnetic lenses can generally be provided outside the neck of the tube, in contrast to electrostatic lenses which are present in the neck of the tube. Therefore the diameter of the magnetic lenses may be larger, which yields a better lens quality: the spherical aberration decreases with an increasing lens diameter. A smaller spherical aberration leads to a smaller spot on the screen, which is required for high-resolution guns. Consequently, a magnetic focusing lens is preferably used for high-resolution (projection) television tubes. When magnetic focusing lenses are used, a distinction can be made between two types, viz. electromagnetic and magnetostatic lenses. In an electromagnetic lens a field is generated by a coil which is partially enclosed by a yoke. In a permanent magnetic lens the field is generated by a permanent magnetic material with or without a yoke (DE-PS 891 119). The electron beam is also moved across the screen by a deflection coil, whilst the intensity of the beam is modulated for obtaining a picture. The large beam aperture angle which occurs at a large intensity of the electron beam results in the electron spot on the screen being not only enlarged but also distorted during deflection of the beam by the deflection coil. As a result of this deflection defocusing an elliptical spot having a diameter which is larger than that in the centre of the display screen is produced on the edge of the screen. In some uses of cathode ray tubes, such as projection television tubes or so-called data-graphics display tubes such a distortion cannot be tolerated. It is an object of the invention to provide a cathode ray tube of the type having a magnetic focusing lens in such a manner that a high resolution is accompanied by a minimum power dissipation in the driver amplifier(s). This object is solved in a cathode ray tube according to the invention in that the means for generating a static magnetic dipole field directly adjoin the deflection unit and surround the neck of the cathode ray tube in a spaced relationship, and in that a system of correction coils for generating 2-, ­ 4- and/or 6-pole fields is provided coaxially between these means and the neck of the tube. The invention is based on the following recognition. - For an optimum resolution the distance between focusing lens and display screen should be maintained as small as possible. If this is done, typically a small circular spot in the centre of the picture is always obtained. A static focusing lens is only required for the centre of the picture (an efficient embodiment is, for example, a focusing lens with permanent magnetic material). - Although the spot in the centre of the picture is then circular and small, the spot size increases towards the edge of the picture and becomes elliptical. This decrease in resolution can be reduced by modulating the focusing field synchronously with the picture scan by 3-4% using a (rapid) focusing coil (at a low impedance). The largest resolution and the smallest power dissipation in the driver amplifier occurs if the dynamic focusing coil is placed in the same position as the static focusing lens (as close as possible to the display screen). The remaining spot growth towards the edge of the picture can be eliminated by modulating 2 quadrupole fields synchronously with the picture scan. The highest resolution and the smallest power dissipation again occurs in the driver amplifiers of the (rapid) quadrupole coils (at a low impedance) if these quadrupoles are positioned as close as possible to the display screen, thus also in the same position as the static focusing lens. According to the invention, to realize this a magnetic focusing lens having an (en)large(d) diameter is used within which the required correction coils are provided coaxially. For an efficient drive of a (rapid) raster correction or convergence coil (having a low impendance) this coil must also be positioned as close as possible to the display screen, hence within the magnetic focusing lens. A first embodiment of the invention is therefore characterized in that the system of correction coils generates two dipole fields for correcting the geometry of the raster formed on the display screen. More particularly a cathode ray tube according to the invention is characterized in that the system of correction coils generates two 4-pole fields for correcting astigmatic errors, and in that the system of correction coils generates two 4-pole fields and two 6-pole fields for correcting higher order spot distortions. The two latter embodiments may or may not be combined with the first-mentioned embodiment. A further embodiment of the invention is characterized in that the system of correction coils includes a dynamic focusing coil. An embodiment of the invention will be described in greater detail with reference to the drawing. In this drawing: Figure 1 is a broken-up elevational view of a cathode ray tube including a system of correction coils according to the invention. As explained above, the invention provides for the increase of the inner diameter of the focusing lens and positioning a system of correction coils between the focusing lens and the neck of the tube. This embodiment is shown in Figure 1. An electron beam 22 is generated by an electron gun 21 in a cathode ray tube (20). A deflection yoke 24 with which the electron beam 22 is moved across a phosphor screen 25 is provided around the neck 23 of the tube 20. A (static) magnetic focusing coil 26 having an enlarged inner diameter is provided directly behind the deflection yoke 24 around the neck 23 of the tube. The magnetic focusing coil 26 is thus positioned as close as possible to the phosphor screen 25 for the purpose of a maximum possible resolution. A (dynamically controlled) multipole coil 27 is positioned coaxially within the focusing coil 26, with which a magnetic 4-pole field can be generated for correcting deflection astigmatism. Furthermore a dynamically controlled magnetic focusing coil 28 and a (dynamically controlled) convergence coil 29 are provided coaxially within the static focusing coil 26. Two dipole fields can be generated with the convergence coil 29 in order to correct the geometry of the raster and to make the red, green and blue images accurately coincide in projection television. According to the invention the multipole correction coil is provided at the area where the beam diameter in the tube is largest. At this large beam diameter the sensitivity of the multipole coil is also highest. This is the case at the area of the magnetic lens. The fact that it is desirable to place th focusing coil as close as possible to the screen in connection with the resolution of the tube also plays a role. The invention is based on the following recognitions: i) when positioning the convergence coil behind the focusing lens (so near the electron gun) the deflection sensitivity of this convergence coil is impractically low because the operation of the magnetic focusing lens is based on the rotating "compression" of the electron beam towards the centre line of the lens and because the magnetic field of the convergence coil is partly shielded from the electron beam by the metal of the electron gun. In addition the electron beam will traverse the focusing lens in a more excentric way so that the rotation of the geometrical corrections becomes larger and more astigmatism is introduced. ii) When the picture distance is reduced and the focusing distance is increased the enlargement of a picture and hence the minimum achievable picture size decreases in a reproducing system. iii) When the inner diameter of a magnetic focusing lens is increased, the spherical aberration of this lens decreases. The increase in spherical aberration which is to be expected upon an increase of the focusing distance due to an enlargement of the effective diameter of the electron beam to be focused at the area of the focusing lens can be amply eliminated thereby. iv) In the case of mutually perpendicular orientations of coils the mutual inductance is low. v) Providing copper in a magnetic field will affect this field to a negligible extent because copper is diamagnetic and has a magnetic permeability which deviates only by 0.001% from the magnetic permeability of vacuum. vi) Interactions between the magnetic focusing field on the one hand and deflection and convergence fields on the other hand primarily become manifest at large inner diameters of the magnetic focusing lens as a rotation of the picture on the phosphor screen and as a rotation of the geometrical corrections provided. These rotations can be eliminated by opposite and equally large rotations of deflection and convergence coil. The following advantages are obtained with the proposed integration of multipole correction coil and focusing coil: i) A compact electron-optical system has been obtained around the cathode ray tube with which the maximum achievable resolution has increased by approximately 15% while maintaining the possibility of dynamic focusing and accurate dynamic convergence. ii) Due to the compactness of the proposed electron-optical system the length of the neck of the cathode ray tube may be reduced so that again a gain in resolution can be made. A short cathode ray tube is also of great importance for constructing small projection television sets for consumer uses. The invention can be used in the field of monochromatic, high-resolution cathode ray tubes which, as one possibility, can be built in a projection television set.

Claims: 1. A monochrome cathode ray tube provided at one end with an electron gun and at the end located oppositely thereto with a display screen, a deflection unit provided around the neck of the display tube and a magnetic focusing device provided around the neck of a display tube between the electron gun and the deflection unit, which device has means for generating a static magnetic field, characterized in that the means for generating a static magnetic dipole field directly adjoin the deflection unit and surround the neck of the cathode ray tube in a spaced relationship, and in that a system of correction coils for generating 2-, 4- and/or 6-­ pole fields is provided coaxially between these means and the neck of the tube. 2. A cathode ray tube as claimed in Claim 1, characterized in that the system of correction coils generates two dipole fields for correcting the geometry of the raster formed on the display screen. 3. A cathode ray tube as claimed in Claim 1 or 2, characterized in that the system of correction coils generates two 4-pole fields for correcting astigmatic errors. 4. A cathode ray tube as claimed in Claim 1 or 2, characterized in that the system of correction coils generates two 4-pole fields and two 6-pole fields for correcting higher order spot distortions. 5. A cathode ray tube as claimed in Claim 1, 2, 3 or 4, characterized in that the system of correction coils includes a dynamic focusing coil.

Inventors: DUWAER, ARNE LEX, VAN ALPHEN, WILLEM MEIJNDERT
Applicants: N.V. PHILIPS' GLOEILAMPENFABRIEKEN
Application year: 1987
Main classification: H01J29
IPC codes: H01J31, H01J29