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EP 0 517 320 B1 |
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EUROPEAN PATENT SPECIFICATION |
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Mention of the grant of the patent: |
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16.10.1996 Bulletin 1996/42 |
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Date of filing: 02.06.1992 |
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International Patent Classification (IPC)6: H01J 29/56 |
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Colour display tube with coma correction
Farbbildröhre mit Coma-Korrektur
Tube d'affichage en couleurs avec correction de coma
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Designated Contracting States: |
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DE FR GB IT |
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Priority: |
05.06.1991 EP 91201380
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Date of publication of application: |
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09.12.1992 Bulletin 1992/50 |
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Proprietor: Philips Electronics N.V. |
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5621 BA Eindhoven (NL) |
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Inventor: |
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- Sluyterman, Albertus Aemilius Seyno
NL-5656 AA Eindhoven (NL)
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Representative: Koppen, Jan et al |
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INTERNATIONAAL OCTROOIBUREAU B.V.,
Prof. Holstlaan 6 5656 AA Eindhoven 5656 AA Eindhoven (NL) |
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References cited: :
EP-A- 0 241 057 US-A- 4 455 542 US-A- 4 874 983
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US-A- 3 725 831 US-A- 4 524 340
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Note: Within nine months from the publication of the mention of the grant of the European
patent, any person may give notice to the European Patent Office of opposition to
the European patent
granted. Notice of opposition shall be filed in a written reasoned statement. It shall
not be deemed to
have been filed until the opposition fee has been paid. (Art. 99(1) European Patent
Convention).
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[0001] The invention relates to a colour display tube comprising an electron gun of the
"in-line" type for generating three electron beams whose axes are coplanar, a deflection
unit comprising a first and a second deflection rail for generating a first and a
second deflection field for deflecting the electron beams in the operating display
tube across said display screen in two mutually perpendicular directions, the direction
of the first deflection field being parallel to said plane, and convergence correction
means which, during deflection, keep the electron beams converged on a display screen
arranged on a wall of the envelope and having a short display screen axis and a long
display screen axis.
[0002] Various types of deflection units may be used for deflecting the electron beams in
colour display tubes. In tubes having an "in-line" electron gun system these deflection
units are generally self-convergent. In conventional deflection units having field
deflection coils of the saddle type and field deflection coils of the toroidal type
the winding technique used does not permit of rendering the unit entirely self-convergent.
Usually such a winding distribution is chosen that a certain convergence error remains,
which error is commonly referred to as coma. This coma error becomes manifest, for
example, in a larger raster (horizontal and vertical) for the outer beams with respect
to the central beam. The horizontal and vertical deflection of the central beam is
smaller than that of the outer beams. As described,
inter alia, in United States Patent 4,196,370, this can be corrected by providing elements (referred
to as field shapers) of a material (for example of mu-metal) having a high magnetic
permeability around the outer beams at the end of the gun. The peripheral field at
the arc of the outer electron beams is shielded to some extent by these elements,
so that these beams are deflected to a lesser extent and the coma error is reduced.
[0003] Various problems then present themselves. A first problem is that the shielding means
around the outer electron beams detrimentally influence the spot shape of these beams.
Another problem is that the correction of the field coma (Y coma) is anisotropic.
In other words, the correction in the corners is less than the correction at the end
of the field axis (the field axis is the display screen axis which is parallel to
the field deflection direction). This is caused by the positive "lens" action of the
line deflection coil (approximately quadratically with the line deflection) for vertical
beam displacements. (The field deflection coil has a corresponding lens action, but
it does not contribute to the relevant anisotropic effect.)
[0004] It is,
inter alia, an object of the invention to provide a solution to the above-mentioned problems.
To this end, a colour display tube of the type described in the opening paragraph
is characterized in that the convergence correction means efect a first, or field
deflection field which is characterized in that an electron beam entering the field
deflection field first passes an area with a barrel-shaped delection field component
and next an adjoining area with a pincushion-shaped deflection field component.
[0005] Such a distribution of field components, whose effect will be elucidated, may be
realised in different manners. If the strength of the barrel-shaped field component
is to be adjusted independently of the strength of the pincushion-shaped field component,
it will be, for example adventageous to use an embodiment which is characterized in
that convergence correction means comprise a first coma corrector which is positioned
at the gun side of the first deflection coil and provides the pincushion-shaped field
component, and a second coma corrector which, viewed in the direction of propagation
of electrons, is positioned upstream of the first coma corrector and provides the
barrelshaped field component.
[0006] The invention is based,
inter alia, on the recognition that the problem of the anisotropic Y coma (referred to as "green
doop") can be reduced by making suitable use of the Z dependence of the anisotropic
Y coma.
[0007] This dependence implies that as the coma correction takes place at a larger distance
(in the Z direction) from the "lens" formed by the line deflection coil, the action
of said "lens" becomes more effective so that the coma correction acquires a stronger
anisotropic character. The invention utilizes this aspect in that a pincushion-shaped
component is realised at the entrance side of the field deflection field, so that
coma is corrected, and in that barrel-shaped component is realised upstream of said
area, so that the anisotropic character of the correction will be less anisotropic.
[0008] Field coma errors at the end of the vertical axis and in the corners can be corrected
effectively and to an approximately equal extent by effecting particularly a pincushion-shaped
component which has a strength which is sufficient to correct the field coma in the
corners, but which is more pincushion-shaped than is necessary for coma correction
at the ends of the vertical axis, and by effecting a barrel-shaped vertical deflection
field component at a location located closer to the electron gun or around the electron
gun, which field component corrects the overcompensation at the ends of the vertical
axis.
[0009] By influencing the shape of the deflection field, rather than partly shielding the
side beams from the deflection field, it is achieved that the spots of the side beams
are not influenced detrimentally. An additional advantage is that the deflection unit
can be moved in the axial direction, for example, for colour purity adjustment without
this influencing the convergence.
[0010] The display tube according to the invention is very suitable for use with a field
deflection coil of the toroidal type, particularly when the display tube should be
free from raster correction.
[0011] These and other aspects of the invention will be elucidated with reference to the
embodiments described hereinafter.
Fig. 1 is a longitudinal section of a display tube according to the invention with
field coma correctors 14 and 14';
Fig. 2a shows the field coma in a conventional display system without coma correction;
Fig. 2b shows the field coma in a conventional display system with coma correction;
Fig. 2c shows the field coma in a display system according to the invention with coma
corrector 14' only; and
Fig. 2d shows the field coma in a display system according to the invention with coma
corrector 14 only;
Fig. 2e shows the field coma in a display system according to the invention with complete
coma correction;
Figs. 3,4,5 show three examples of embodiments of coma correctors for a colour display
tube according to the invention;
Figs. 6a, 6b and Fig. 7 show two modifications of coma correction elements which can
be used within the scope of the invention.
[0012] Fig. 1 is a longitudinal section of a display tube according to the invention. It
is a colour display tube of the "in-line" type. In a glass envelope 1, which is composed
of a display window 2, a cone 3 and a neck 4, said neck accommodates an integrated
electron gun system 5 which generates three electron beams 6, 7 and 8 whose axes are
coplanar prior to deflection. The axis of the central ("green") electron beam 7 coincides
with the tube axis 9. The display window 2 has a large number of phosphor element
triplets on its inner side. The elements may be rows or dots. Each triplet comprises
an element of a blue-luminescing phosphor, an element of a green-luminescing phosphor
and an element of a red-luminescing phosphor. All triplets combined constitute the
display screen 10. The phosphor rows are substantially perpendicular to said plane
through the beam axes. A shadow mask 11 having a very large number of elongate apertures
12 for passing the electron beams 6, 7 and 8 each impinging upon phosphor elements
of one colour only is arranged in front of the display screen. The three coplanar
electron beams are deflected by a system 13 of deflection coils, which is not completely
self converging because of the fact that a field coma error occurs, which system comprises
a line deflection coil 16, a yoke ring 15 and a field deflection coil 16'.
[0013] Coma correction coil 14' produces a (positive) six-pole field by which a pincushion-shaped
field distribution is effected so that the green beam is deflected in the direction
of deflection of the field deflection coil to a greater extent than the side beams.
Correction coil 14 produces a (negative) six-pole field by which a barrel-shaped field
distribution is effected, so that the green beam is deflected in the direction of
deflection of the vertical deflection coil to a lesser extent than the side beams.
[0014] A problem to be solved is that of the "green droop". Green droop means that the field
coma is corrected at the end of the vertical axis but is insufficiently corrected
in the corners. Fig. 2a shows a situation where the field coma correction is insufficient,
Fig. 2b shows the green droop situation. This problem becomes worse as the axial distance
between the location of coma correction and the centre of the line deflection coil
increases. Use can be made of the axial dependence of the green droop for solving
the problem of the green droop. The problem can be solved by overcorrecting the field
coma at the entrance side of the field deflection field (see Fig. 2c) and by performing
an opposite correction at a location "upstream" (see Fig. 2d), which opposite correction
is, however less effective in the corners. The overall result is a uniform coma correction
along the entire edge of the display screen (see Fig. 2e). This idea, using shielding
means ("corretion rings") is described in PHN 11.418 (European Patent Application
no. 205222).
[0015] The method described in this Application is based on coma correction by means of
field-shielding components arranged around the paths of individual electron beams.
The drawback of coma correction by partially shielding the beams is that the spot
shape of the side beams is detrimentally influenced.
[0016] The invention provides,
inter alia, a solution for correcting field coma and preventing the green droop, while the spot
shape of the side beames is minimally influenced. Moreover, in the proposed solution
the deflection unit can be moved in the axial direction, for example, for colour purity
adjustment without any convergence side effects.
[0017] Figure 3, 4 and 5 show modifications of embodiments of coma correctors 14' each comprising
one or more magnetic cores with such a coil arrangement that a positive six-pole field
is generated upon energization. Figures 3, 4 and 5 show, in this order, increasingly
simplified embodiments (i.e. magnetic cores provided with fewer coils). The (overcompensated)
coma correction can also be performed by means of coma correction means of the type
used in the Philips colour display tube systems 30AX, 45AX or as described in PHN
10.667 (USP 4,524,340) or PHN 12.132 (USP 4,874,983).
[0018] The corrector 14 which works in the opposite way and this enlarges the original coma
error to some extent may comprise correctors of the type shown in Figs. 3, 4 and 5,
with such an energization of the coils that the field direction is opposite to that
shown in Figures 3, 4 and 5. This means that a negative sixpole field is generated.
[0019] It is alternatively possible to generate a negative sixpole field by arranging two
plate-shaped magnetic elements 17, 17' at the gun-sided end of the field deflection
coil in the way as shown in Figs. 6a and 6b. This construction resembles an astigmatic
error corrector, but is arranged at the gun side of the deflection coil. The difference
with an astigmatic error corrector is that there is not yet sufficient predeflection,
so that there is no or little effect on astigmatism. Viewed in the direction of the
screen, the elements 17, 17' will be followed by the conventional astigmatic error
correction means.
[0020] When using a saddle-shaped or mussel-shaped field deflection coil it is possible
to perform the same effect as the correction means 14 and 14' by arranging four U-shaped
correctors 18, 19, 20, 21 in the manner shown in Fig. 7. A field similar to that of
Fig. 5 is then produced at the screen side of the U-shaped correctors and a field
opposite thereto is produced at the gun side. The extent to which the limbs of the
U-shaped correctors extend towards as the neck glass determines the strength of the
correction.
1. A colour display tube comprising an electron gun (5) for generating three electron
beams (6, 7, 8) whose axes are coplanar, a deflection unit (13) comprising a first
and a second deflection coil for generating a field and a line deflection field (16',
16) for deflecting the electron beams in the operating display tube across said display
screen (10) in two mutually perpendicular directions (x, y), the direction of the
field deflection field being parallel to said beam axes plane and convergence correction
means (14, 14') which, during deflection, keep the electron beams converged on a display
screen arranged on a wall of the envelope and having a short display screen axis and
a long display screen axis, characterized in that the convergence correction means
help to form a field deflection field having a distribution such that the electron
beams entering the field deflection field first pass an area with a barrel-shaped
deflection field component and next pass an area with a pincushion-shaped deflection
field component.
2. A colour display tube as claimed in claim 1, characterized in that the convergence
correction means comprise a first coma corrector (14') which is positioned at the
gun side of the field deflection coil and provides the pincushion-shaped field component,
and a second coma corrector (14) which, when viewed in the direction of propagation
of the electrons, is positioned upstream of the first coma corrector and provides
the barrel-shaped field component.
3. A colour display tube as claimed in Claim 2, characterized in that the first coma
corrector (14') overcompensates coma at the ends of the short display screen axis
and in that the second coma corrector (14) corrects the overcompensation produced
by the first coma corrector.
4. A colour display tube as claimed in Claim 2, characterized in that the first coma
corrector (14') comprises a system of coils wound on at least one magnetic core, which
system, when energized, generates a magnetic six-pole field.
5. A colour display tube as claimed in Claim 2, characterized in that the second coma
corrector (14) comprises a system of coils wound on at least one magnetic core, which
system, when energized, generates a magnetic six-pole field.
6. A colour display tube as claimed in Claim 2, characterized in that at least one of
the coma correctors comprises at least two plate-shaped magnetic elements (17, 17')
arranged in the field deflection field so as to realise a six-pole field component.
1. Farbbildröhre mit einem Elektronenstrahlerzeugungssystem (5) zum Erzeugen von drei
Elektronenstrahlen (6, 7, 8), deren Achsen koplanar sind, mit einer Ablenkeinheit
(13) mit einer ersten und einer zweiten Ablenkspule zum Erzeugen eines Bild- und eines
Zeilen-Ablenkfeldes (16, 16') zum Ablenken der Elektronenstrahlen im Betrieb der Wiedergaberöhre
über den genannten Wiedergabeschirm (10) in zwei senkrecht aufeinander stehenden Richtungen
(x, y), wobei die Richtung des Bild-Ablenkfeldes sich parallel zu der genannten Ebene
der Strahlenachsen erstreckt und mit Konvergenzkorrekturmitteln (14, 14'), die während
der Ablenkung die Elektronenstrahlen auf einen an einer Wand der Hülle vorgesehenen
Wiedergabeschirm konvergiert halten, und wobei der Schirm eine kurze und eine lange
Achse aufweist, dadurch gekennzeichnet, daß die Konvergenzkorrekturmittel dazu beitragen ein Bild-Ablenkfeld herbeiführen,
das eine derartige verteilung aufweist, daß die in das Bildablenkfeld eintreffenden
Elektronenstrahlen zunächst durch ein Gebiet mit einem tonnenförmigen Ablenkfeldanteil
hindurchgehen und danach durch ein Gebiet mit einem kissenförmigen Ablenkfeldanteil.
2. Farbwiedergaberöhre nach Anspruch 1, dadurch gekennzeichnet, daß die Konvergenzkorrekturmittel eine erste Koma-Korrekturstufe (14') aufweisen,
die an der Elektronenstrahlerzeugungssystemseite der BildAblenkspule vorgesehen ist
und den kissenförmigen Bildfeldanteil schafft, und eine zweite Koma-Korrekturstufe
(14), die, in der Fortpflanzungsrichtung der Elektronen gesehen, stromaufwärts der
ersten Koma-Korrekturstufe vorgesehen ist und den tonnenförmigen Bildfeldanteil schafft.
3. Farbwiedergaberöhre nach Anspruch 2, dadurch gekennzeichnet, daß die erste Koma-Korrekturstufe (14') an den Enden der kurzen Wiedergabeschirmachse
die Koma überkompensiert und daß die zweite Koma-Korrekturstufe (14) die von der ersten
Koma-Korrekturstufe erzeugte Überkompensation korrigiert.
4. Farbwiedergaberöhre nach Anspruch 2, dadurch gekennzeichnet, daß die erste Koma-Korrekturstufe (14') ein auf wenigstens einem Kern gewickeltes
Spulensystem aufweist, das bei Erregung ein Sechspol-Magnetfeld erzeugt.
5. Farbwiedergaberöhre nach Anspruch 2, dadurch gekennzeichnet, daß die zweite Koma-Korrekturstufe (14) ein auf wenigstens einem Magnetkern gewickeltes
Spulensystem aufweist, das bei Erregung ein Sechspol-Magnetfeld erzeugt.
6. Farbwiedergaberöhre nach Anspruch 2, dadurch gekennzeichnet, daß wenigstens eine der Koma-Korrekturstufen wenigstens zwei plattenförmige Magnetelemente
(17, 17') aufweist, die derart in dem Bildablenkfeld vorgesehen sind, daß ein Sechspolfeldanteil
verwirklicht wird.
1. Tube d'affichage en couleurs comprenant un canon électronique (5) pour générer trois
faisceaux d'électrons (6, 7, 8) dont les axes sont coplanaires, une unité de déviation
(13) comprenant une première et une deuxième bobines de déviation pour générer un
champ de déviation verticale (16) et un champ de déviation horizontale (16') afin
de dévier les faisceaux d'électrons dans le tube d'affichage en service, en travers
de l'écran d'affichage (10) dans deux directions mutuellement perpendiculaires (x,
y), la direction du champ de déviation verticale étant parallèle au plan desdits axes
de faisceaux, et des moyens de correction de convergence (14, 14') qui, pendant la
déviation, maintiennent les faisceaux d'électrons en convergence sur un écran d'affichage
agencé sur une paroi de l'enveloppe et ayant un axe d'écran court et un axe d'écran
long, caractérisé en ce que les moyens de correction de convergence aident à former
un champ de déviation verticale ayant une distribution telle que les faisceaux d'électrons
pénétrant dans le champ de déviation verticale passent d'abord par une zone ayant
une composante de champ de déviation en forme de tonneau, puis par une zone ayant
une composante de champ de déviation en forme de coussin.
2. Tube d'affichage en couleurs selon la revendication 1, caractérisé en ce que les moyens
de correction de convergence comprennent un premier correcteur de coma (14') qui est
disposé du côté canon de la bobine de déviation verticale et fournit la composante
de champ en forme de coussin, et un deuxième correcteur de coma (14) qui, vu dans
la direction de propagation des électrons, est positionné en amont du premier correcteur
de coma et fournit la composante de champ en forme de tonneau.
3. Tube d'affichage en couleurs selon la revendication 2, caractérisé en ce que le premier
correcteur de coma (14') surcompense le coma aux extrémités de l'axe court de l'écran
d'affichage et en ce que le deuxième correcteur de coma (14) corrige la surcompensation
produite par le premier correcteur de coma.
4. Tube d'affichage en couleurs selon la revendication 2, caractérisé en ce que le premier
correcteur de coma (14') comprend un système de bobines enroulées sur au moins un
noyau magnétique, ledit système, lorsqu'il est excité, générant un champ hexapolaire
magnétique.
5. Tube d'affichage en couleurs selon la revendication 2, caractérisé en ce que le deuxième
correcteur de coma (14) comprend un système de bobines enroulées sur au moins un noyau
magnétique, ledit système, lorsqu'il est excité, générant un champ hexapolaire magnétique.
6. Tube d'affichage en couleurs selon la revendication 2, caractérisé en ce qu'au moins
un des correcteurs de coma comprend au moins deux éléments magnétiques (17, 17') en
forme de plaques agencés dans le champ de déviation verticale de manière à réaliser
une composante de champ hexapolaire.