U.S. patent number 3,906,280 [Application Number 05/372,582] was granted by the patent office on 1975-09-16 for electron beam producing system for very high acceleration voltages and beam powers.
This patent grant is currently assigned to Max-Planck-Gesellschaft zur Forderung der Wissenschaften e.V.. Invention is credited to Claus Andelfinger, Walter Dommaschk, Werner Ott, Manfred Ulrich, German Weber.
United States Patent |
3,906,280 |
Andelfinger , et
al. |
September 16, 1975 |
Electron beam producing system for very high acceleration voltages
and beam powers
Abstract
An electron beam producing system for acceleration voltages in
the order of agnitude of megavolts and beam powers in the order of
magnitude of gigawatts, comprises a tubular housing of insulating
material, in which adjacent to its one closed end a field emission
cathode with a large surface area is arranged while at its other
end, from which the electron beam emerges, an annular anode is
arranged. A device serves for collimating the electrons emitted by
the cathode to form a collimated electron beam. The device for
collimating the electron consists of annular electrodes, which
respectively comprise a part adjacent to their center opening and
an outer part which is held on the housing and has a radial
electrical passage extending towards the outside of the housing.
The inner part of the electrode lying closest to the cathode has at
least approximately the shape of a frusto-conical surface which
tapers towards the cathode; in that the inner part of the remaining
electrodes is flat or at least approximately frusto-conical and
respectively lies in an equipotential surface of an electric field,
which collimates the electrons, emitted by the cathode, to form a
parallel beam. The housing is surrounded by a coaxial insulating
casing with a clearance. The intermediate space between the outer
surface of the housing and the casing is surrounded with an
electrically conducting liquid with a relatively high specific
resistance and at the axial ends has a respective connection
electrode, which makes contact with the liquid, for the operating
voltage and that the outer parts of the electrodes are so shaped
that the radial passages end at those sites of the liquid filled
intermediate space at which the fraction, provided for the relevant
electrode, of the operating voltage obtains when the operating
voltage is applied to the connection electrodes.
Inventors: |
Andelfinger; Claus (Haar,
DT), Dommaschk; Walter (Garching, DT), Ott;
Werner (Garching, DT), Ulrich; Manfred (Garching,
DT), Weber; German (Munich, DT) |
Assignee: |
Max-Planck-Gesellschaft zur
Forderung der Wissenschaften e.V. (Gottingen,
DT)
|
Family
ID: |
6631106 |
Appl.
No.: |
05/372,582 |
Filed: |
June 22, 1973 |
Foreign Application Priority Data
|
|
|
|
|
Jun 22, 1972 [DT] |
|
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7223397 |
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Current U.S.
Class: |
313/449; 313/336;
313/452; 313/351 |
Current CPC
Class: |
H01J
5/06 (20130101); H01J 3/02 (20130101) |
Current International
Class: |
H01J
3/02 (20060101); H01J 5/06 (20060101); H01J
3/00 (20060101); H01J 5/02 (20060101); H01J
029/46 () |
Field of
Search: |
;313/63,82R,82BF,336,351,446,448,449,452,454 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Mullins; James B.
Attorney, Agent or Firm: Spencer & Kaye
Claims
We claim:
1. An electron beam producing system for acceleration voltages in
the order of magnitude of megavolts and beam powers in the order of
magnitude of gigawatts, comprising a tubular housing of insulating
material, in which adjacent to its one closed end a field emission
cathode with a large surface area is arranged while at its other
end, from which the electron beam emerges, an annular anode is
arranged, and with a device for collimating the electrons emitted
by the cathode to form a collimated electron beam, characterized in
that: the device for collimating the electron includes annular
electrodes, which respectively comprise a part adjacent to their
center opening and an outer part which is held on the housing and
has a radial electrical passage extending towards the outside of
the housing; the inner part of the electrode lying closest to the
cathode has at least approximately the shape of a frusto-conical
surface which tapers towards the cathode; the inner part of the
remaining electrodes is flat and lies in an equipotential surface
of an electric field, which collimates the electrons, emitted by
the cathode, to form a parallel beam; the housing is surrounded by
a coaxial insulating casing with a clearance; in that the
intermediate space between the outer surface of the housing and the
casing is surrounded with an electrically conducting liquid with a
relatively high specific resistance and at the axial ends has a
respective connection electrode, which makes contact with the
liquid, for the operating voltage and that the outer parts of the
electrodes are so shaped that the radial passages end at those
sites of the liquid filled intermediate space at which the
fraction, provided for the relevant electrode, of the operating
voltage obtains when the operating voltage is applied to the
connection electrodes.
2. An electron beam producing system in accordance with claim 1,
characterized in that the outer part of the annular electrodes is
furthermore so curved that stray electrons are caught by the
electrodes before reaching the inner wall of the housing.
3. An electron beam producing system in accordance with claim 1,
characterized in that the housing includes tubular parts, between
which annular electrode holding means of a conducting material are
arranged, which form the passages.
4. An electron beam producing system in accordance with claim 3,
characterized in that the inner wall of the housing has ribs
extending in the peripheral direction.
5. An electron beam producing system in accordance with claim 1,
characterized in that the opening of the electrode closest to the
cathode is covered by a wire fabric.
6. An electron beam producing system in accordance with claim 1,
characterized in that the opening of the electrode furthest removed
from the cathode is covered with a wire fabric.
7. An electron beam producing system in accordance with claim 1,
characterized in that the emission surface of the cathode is
surrounded by an annular conductor part.
8. An electron beam producing system in accordance with claim 7,
characterized in that the zone, adjacent to the emission surface,
of the annular conductor part as seen from the adjacent annular
electrode is concave.
9. An electron beam producing system in accordance with claim 7,
characterized in that the radially outer part of the surface,
adjacent to the emission surface, of the annular conductor part as
seen from the adjacent annular electrode is convex.
10. An electron beam producing system in accordance with claim 1,
characterized in that the cathode is axially adjustable with
respect to the annular electrode adjacent to it.
11. An electron beam producing system in accordance with claim 1,
characterized in that the emitting part of the cathode includes a
stack of razor blades.
12. An electron beam producing system in accordance with claim 1,
characterized in that the emitting part of the cathode consists of
a stack of needles.
13. An electron beam producing system for acceleration voltages in
the order of magnitude of megavolts and beam powers in the order of
magnitude of gigawatts, comprising a tubular housing of insulating
material, in which adjacent to its one closed end a field emission
cathode with a large surface area is arranged while at its other
end, from which the electron beam emerges, an annular anode is
arranged, and with a device for collimating the electrons emitted
by the cathode to form a collimated electron beam, characterized in
that: the device for collimating the electron includes annular
electrodes, which respectively comprise a part adjacent to their
center opening and an outer part which is held on the housing and
has a radial electrical passage extending towards the outside of
the housing; the inner part of the electrode lying closest to the
cathode has at least approximately the shape of a frusto-conical
surface which tapers towards the cathode; the inner part of the
remaining electrodes is at least approximately frusto-conical and
lies in an equipotential surface of an electric field, which
collimates the electrons, emitted by the cathode, to form a
parallel beam; the housing is surrounded by a coaxial insulating
casing with a clearance; the intermediate space between the outer
surface of the housing and the casing is surrounded with an
electrically conducting liquid with a relatively high specific
resistance and at the axial ends has a respective connection
electrode, which makes contact with the liquid, for the operating
voltage and that the outer parts of the electrodes are so shaped
that the radial passages end at those sites of the liquid filled
intermediate space at which the fraction, provided for the relevant
electrode, of the operating voltage obtains when the operating
voltage is applied to the connection electrodes.
Description
BACKGROUND OF INVENTION
1. Field to which Invention Relates
The present invention relates to an electron beam producing system
for acceleration voltages in the order of magnitude of megavolts
and beam powers in the order of magnitude of gigawatts, comprising
a tubular housing of insulating material, in which adjacent to its
one closed end a field emission cathode with a large surface area
is arranged while at its other end, from which the electron beam
emerges, an annular anode is arranged, and with a device for
collimating the electrons emitted by the cathode to form a
collimated electron beam.
2. The Prior Art
For a number of physical experiments and devices extremely
energy-rich high current electron beams are required. For example,
a prior art plasma ring accelerator requires a relative electron
beam of some hundreds of amps with an emittance of approximately 1
rad mm.
Electron beam producing systems for very high acceleration voltages
and beam powers have already been proposed. A prior art electron
beam producing system of this type consists of a sealed by fusion
tube, in which a vacuum of 10.sup.-.sup.9 torr obtains. The tube
contains a relatively large surface area field emission cathode,
that is to say a cold cathode. The ray emergence is through a
Lenard window in the form of titanium foil with a thickness of 25
microns. However, such a window leads to an impairment in the ray
quality to a substantial extent and furthermore limits the length
of life of the tube to a few shots.
The above problems can be avoided with an open electron beam
producing system, that is to say with an electron beam producing
system, which at the beam outlet opening is not provided with a
vacuum-tight window, and instead is connected with the vacuum space
of the adjacent device or load for the electron beam. In this case
the electron beam producing system must be operated with pressure
in order of magnitude of 10.sup.-.sup.6 torr, something which in
the prior art involved extraordinary difficulties as regards
resistance to arcing. The required resistance to high voltages
could admittedly be ensured with the known constructions in the
condition free of current, that is to say without the electron
beam, comparatively easily. However, as soon as the electron beam
which has a very high current and is very rich in energy, is caused
to flow arcing repeatedly occurs despite careful adjustment of the
device for collimating, consisting of a magnet coil, the electrons
emitted by the cathode.
SUMMARY OF INVENTION
One aim of the present invention is therefore that of creating an
electron beam producing system of the above-mentioned type which
can be reliably operated with an open electron beam outlet opening
without arcing occurring and which produces a substantially
mono-energetic electron beam which is highly collimated.
In order to achieve these and other aims the present invention
consists in an electron beam producing system of the
above-mentioned type which is characterized in that the device for
collimating the electron consists of annular electrodes, which
respectively comprise a part adjacent to their center opening and
an outer part which is held on the housing and has a radial
electrical passage extending towards the outside of the housing; in
that the inner part of the electrode lying closest to the cathode
has at least approximately the shape of a frusto-conical surface
which tapers towards the cathode (that is to say it is convex with
respect to the cathode); in that the inner part of the remaining
electrodes is flat or at least approximately frusto-conical and
respectively lies in an equipotential surface of an electric field,
which collimates the electrons, emitted by the cathode, to form a
parallel beam; in that the housing is surrounded by a coaxial
insulating casing with a clearance; in that the intermediate space
between the outer surface of the housing and the casing is
surrounded with an electrically conducting liquid with a relatively
high specific resistance and at the axial ends has a respective
connection electrode, which makes contact with the liquid, for the
operating voltage and that the outer parts of the electrodes are so
shaped that the radial passages end at those sites of the liquid
filled intermediate space at which the fraction, provided for the
relevant electrode, of the operating voltage obtains when the
operating voltage is applied to the connection electrodes.
The present electron beam producing system thus operates with an
electrostatic collimating of the electron beam and the annular
electrodes producing the collimating field simultaneously ensure
that the stray electrons do not reach the inner wall of the tubular
housing and cannot at this position free adsorbed material, always
present in the case of the relatively high working pressures, so as
to lead to arcing.
In the case of one embodiment of the invention the electron current
available was 300 A, that is to say approximately 4 to 4 times
greater than in the case of prior art electron beam producing
systems and could be focussed with an admittance of 1.3 rad mm. At
the same time the total extraneous emission (X-ray emission) only
amounted to approximately one fifth of that involved in the case of
commercial prior art tubes.
The reproducibility of the electron energy amounted to 0.15 % in
the case of series of shots occurring directly one after the other.
Even in the case of shots made as intervals of several weeks the
variations lay below 1 %. The present electron beam producing
system can furthermore readily be matched to suit any desired
initial resistance of the high voltage source by changing the
specific resistance of the electrically conducting liquid
(preferably water with small amounts of added salts, as for example
copper sulfate).
The present electron beam producing system is furthermore capable
of withstanding the voltage and resistant to arcing when a strong
electron beam is flowing.
Further developments of the invention are defined in the
subclaims.
LIST OF SEVERAL VIEWS OF DRAWINGS
The principle of the invention will now be explained in detail with
reference to embodiments referring to the drawings.
FIG. 1 shows a sectional view of a half of an electron beam
producing system in accordance with an embodiment of the
invention.
FIGS. 2 to 5 show field line diagrams, from which the shape of the
inner parts, bringing about the collimation of the electron beam,
of the annular electrodes of further embodiments of the invention
is shown.
DESCRIPTION OF PREFERRED EMBODIMENTS
FIG. 1 shows a half of an electron beam producing system in
accordance with the invention in section. The electron beam
producing system is substantially radially symmetrical with
reference to a center axis 10. It is designed for an operating
voltage of 2 megavolts.
The electron beam producing system which is shown comprises a
tubular housing 12, which is mainly made of annular parts 12a -12e,
which can be made of epoxy resin or ceramic material and in order
to increase the voltage resistance have a ribbed inner wall 14
extending in the peripheral direction. Between the annular parts of
the housing annular electrode holding means 16a-16d are arranged.
The end surfaces of the annular pieces 12a-12e and of the annular
electrode holding means 16a-16d have annular grooves in which the
sealing rings are located. The sealing rings ensure that there is a
vacuum-tight connection.
The one end of the housing 12 is closed by means of a disc-shaped
end plate 18, which has an axial hole, through which a preferably
axially sliding cathode connection and holding conductor 20 is
passed in a vacuum-tight manner. On the other end of the annular
housing there is an attachment flange 22, which consists of metal,
and which forms a beam outlet opening 24.
The arrangement described is held together by means of a casing 26
consisting of acrylic resin and which at one end has a flange 28
which projects inwards and at the other end has a flange 30 which
projects outwards. The flange 30 is connected by screw means with
the attachment flange 22. Between the flange 28 and the end plate
18 there is a sealing and intermediate ring 32.
On the cathode connection conductor 20 a cathode 34 is attached,
whose active part 36 consists of a razor blade stack or a stack of
needles, whose cutting edges or tips form an emission surface 38,
whose diameter can for example amount to 1 to 5 cm. To the outside
a conductor part 40 is connected with the emission surface 38 of
the cathode. The surface, adjacent to the beam exit opening 24, of
the conductor part 40 adjacent to the emission surface 38 is
firstly somewhat concave towards the outlet opening 24 and then
forms an annular bead which is convex towards the surface. On the
radially outer end of the conductor part 40 there is an anti-corona
ring 42. On the electrode holding means 16a-16d there are
respectively ring disc electrodes 44a-44d and a further electrode
44e is connected with the attachment flange 22. The electrodes each
have a center opening, through which the collimated electron beam
running along the axis 10 passes. Following the center opening they
have an inner part 44a'-44e', which is respectively so shaped that
it runs into an equipotential surface of an electric field, which
collimates the electrons which are emitted by the emission surface
38 of the cathode and accelerated towards the outlet opening 24 to
form a substantially parallel beam. The beam has in this case no
so-called intersection point in contrast to beam producing systems
as are used for example in television picture tubes.
Adjoining the inner part 44a'-44e' of the electrodes there is a
respective outer part 44a"-44e", which fulfills two functions.
Firstly it serves to prevent the impingement of electrons which
have been dispersed from the beam on the inner wall 14 of the
tubular housing as far as this is possible, and secondly it
constitutes a mechanical holding means and the electrical
connection for the annular electrode holding means 16a-16d,
consisting of metal, and, respectively, the attachment flange 24.
The axial length of the annular pieces 12a-12e of the housing and
thus the position of the annular electrode holding means 16 are so
selected that the annular electrode holding means are located at a
position, corresponding to the operating voltage provided of the
relevant electrode, along the housing. The annular electrode
holding means and the attachment flange 22 are thus connected
electrically with a liquid 46 with a comparatively high specific
resistance, for example a copper sulfate solution, which occupies
the intermediate space between the outer wall of the tubular
housing 12 and the casing 26 and provides a voltage divider for the
operating voltage. The operating voltage is applied between the
attachment flange 22 consisting of metal and the end plate 18, also
consisting of metal, and also the cathode connection conductor
20.
Preferably the center opening of the first electrode 44a closest to
the cathode is covered over by wire fabric 48. Also the center
opening of the last electrode 44e at the other end of the housing,
that is to say the anode, can be covered with wire fabric 50.
The various electrodes have the following shape in the case of the
embodiment shown in FIG. 1.
The inner part 44a' of the first electrode 44a which as seen from
the cathode is comparatively close (for example 10 to 20 mm with a
distance of 24 cm between the electrodes 44a and 44e) is convex
towards the cathode and can as a first approximation be denoted as
frusto-conical with a taper towards the cathode. The part 44a"
adjacent to this is arranged to bulge outwards towards the last
electrode (anode) 44e convexly.
The second electrode 44b has an inner part 44b' which is
substantially frusto-conical and is concave towards the cathode,
and an outer part 44b" which is convex towards the cathode and is
substantially frusto-conical. The two next electrodes 44c and 44d
are apart from the angle, which the inner and the outer parts make
with the axis 10, similarly shaped to the second electrode 44b. In
the case of the last electrode (anode) 44e on the other hand both
the inner and also the outer parts 44e' and 44e" are convex towards
the cathode, though they form different angles with respect to the
axis, as will be gathered from FIG. 1.
The field which is produced by the electrode arrangements
described, and of which the further equipotential surfaces lying
between the electrodes are shown in broken lines, bringing about a
satisfactory collimation of the electrons emitted from the cathode
34 and the shape of the outer parts of the electrodes ensures that
practically no stray electrodes can strike the inner wall of the
housing 12 and cause arcing on the wall.
By adjusting the distance between the emission surface 38 of the
cathode 34 from the wire fabric 48 of the first electrode 44a
("take-up grid") it is possible to set an emission current
resulting for a predetermined operating voltage.
Preferred dimensions and operational voltages are shown in FIG. 1.
In this respect it was assumed that in operation the connection
flange 22 lies at ground potential and the cathode lies at -2 MV.
The internal diameter of the annular housing 12 amounts for example
to approximately 28 cm and is therefore comparatively large having
regard to prior art tubes. The diameter of the electron beam which
is collimated lies in the order of magnitude of 20 mm.
FIG. 2 shows in an extremely simplified form a further embodiment
of the invention. In this case only the axis 10, the radial limit
52 of the electron beam, the inner parts of the various electrodes,
the wire fabric 48 and 50 and then the inner parts of the
electrodes are shown in broken lines while the further course of
the ideal equipotential surfaces corresponding respectively to the
electrodes are shown. The course of the electrodes can depart from
this ideal course at a reasonable distance from the limit 52 of the
electron beam in order to fulfill the above-mentioned conditions,
which are to be set as regards the outer parts of the electrodes.
Since the voltage drop at the liquid 46 operating as a voltage
divider, is linear, the loci of the annular electrode holding means
of the individual electrodes are fixed. In the case of FIG. 2 (and
the following figures) the voltage values are with respect to the
cathode.
In FIGS. 3 to 5 only the equipotential surfaces with the associated
voltage values are shown, in which case it is assumed that the beam
passage openings of the first electrode (draw-off electrode) and
the last electrode (anode) are provided with wire fabric (like the
wire fabric 48 and 50 in FIG. 1). The inner parts of the electrodes
of the corresponding embodiments of the invention then have
substantially the same shape as the relevant equipotential
surfaces. Naturally it is not necessary for an electrode to be
provided for each of the equipotential surfaces represented.
In the case of the field distributions in accordance with FIGS. 3
and 4 it is possible to provide, besides annular disc-shaped
electrodes as explained with reference to FIG. 1, bead-shaped
electrodes as well, which have, for example, the form of
equipotential surfaces 54 and 56.
The saddle potential obtained in the field distribution in
accordance with FIG. 3 can instead of the bead-shaped electrodes
corresponding to the equipotential surfaces 54 and 56, also be
produced by a single bead-shaped electrode 58 (which would then lie
at approximately 1.95 MV) or an annular disc-shaped electrode 44f,
or by an annular bead electrode 60 (potential 1.95 MV) shaped in
cross-section like a pear which is flattened at the bottom.
In the absence of anything to the contrary the beam current I
amounts respectively to 1000A.
* * * * *