U.S. patent number 3,793,550 [Application Number 05/235,763] was granted by the patent office on 1974-02-19 for electrode configuration for particle acceleration tube.
This patent grant is currently assigned to Radiation Dynamics, Inc.. Invention is credited to Chester C. Thompson, Jr..
United States Patent |
3,793,550 |
Thompson, Jr. |
February 19, 1974 |
ELECTRODE CONFIGURATION FOR PARTICLE ACCELERATION TUBE
Abstract
In a high vacuum particle acceleration tube of the type in which
a series of spaced apertured electrodes define the acceleration
path, the apertured electrodes are provided with circular
depressions of asymmetric V-shaped cross-section. The asymmetry is
such that adjacent electrodes are closer to one another on the
radially inward side of the V than on the radially outward side.
Thus, arcing, if it occurs, is directed inwardly of the V and metal
vapor is not deposited on the insulator. In addition, the
V-configured recess acts to intercept high energy particles which
are scattered out of the main beam, thereby protecting the glass
insulators at the electrode periphery from radiation damage.
Inventors: |
Thompson, Jr.; Chester C.
(Roslyn Heights, NY) |
Assignee: |
Radiation Dynamics, Inc.
(Westbury, NY)
|
Family
ID: |
22886810 |
Appl.
No.: |
05/235,763 |
Filed: |
March 17, 1972 |
Current U.S.
Class: |
313/360.1;
315/506; 315/507 |
Current CPC
Class: |
H01J
5/06 (20130101); H05H 5/02 (20130101) |
Current International
Class: |
H01J
5/06 (20060101); H01J 5/02 (20060101); H05H
5/00 (20060101); H05H 5/02 (20060101); H05h
005/06 () |
Field of
Search: |
;313/63 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lake; Roy
Assistant Examiner: Hostetter; Darwin R.
Attorney, Agent or Firm: Rose & Edell
Claims
I claim:
1. A high-vacuum particle accelerator tube of the type in which
successive apertured electrodes are spaced by insulators at their
peripheries and have their apertures aligned to define a path for
an accelerated particle beam along the length of the tube, said
tube being characterized in that each electrode includes a
continuous recess disposed about said aperture, the recesses of
suscessive electrodes being aligned in a direction parallel to the
alignment of said apertures, said recess having an asymmetrical
cross-section configured such that the closest points between
successive electrodes are located along the side of the recesses of
those electrodes which is closest to said apertures.
2. The combination according to claim 1 wherein said recess
includes an apex about which said recess is asymmetrical,
successive electrodes being positioned such that the apex of the
recess of each electrode extends a short distance into the recess
of the next successive electrode.
3. The combination according to claim 2 wherein said recess has an
asymmetrical V cross-section, the leg of the V closest to said
aperture being shorter than the leg disposed more remote from said
aperture, said closest leg subtending a smaller angle with said
particle beam path than said remote leg.
4. The combination according to claim 1 wherein said recess has an
asymmetrical V cross-section, the leg of the V closest to said
aperture being shorter than the leg disposed more remote from said
aperture, said closest leg subtending a smaller angle with said
particle beam path than said remote leg.
5. A device for accelerating ions injected thereinto in a
downstream direction, said device comprising an acceleration tube
having a series of alternating insulating rings and apertured
electrodes, and means for applying successive voltage increments
across adjacent electrodes to provide a substantially uniform
electric field in said acceleration tube, wherein said apertured
electrodes include a flat upstream surface in which a continuing
downstream-directed recess is formed concentrically about the
electrode aperture, the recesses of said electrodes being aligned
in a downstream direction, each recess having an asymmetric
cross-sectional configuration about an apex such that the side of
said recess between said apex and said aperture is closer to the
next downstream electrode than is the side of said recess remote
from said aperture.
6. The device according to claim 5 wherein the apex of each
electrode recess extends a short distance into the recess region of
the next downstream electrode.
7. The device according to claim 6 wherein the cross-section of
said recess is in the form of a V which is asymmetric about the
apex, the side of the V closest to the aperture being shorter than
the side remote from said aperture.
8. A device for accelerating charged particles comprising:
an acceleration tube having an upstream end and a downstream end
and comprising a multiplicity of alternating apertured electrodes
and insulating rings, the apertures of said electrodes being
axially aligned to define a path for said charged particles
therethrough between the upstream and downstream ends of said
tube;
means for applying successive voltage increments across adjacent
electrodes to provide an electric field between the upstream and
downstream ends of said tube; and
means for injecting a beam of said charged particles into said tube
at the upstream end thereof and directed generally toward the
downstream end thereof;
wherein each electrode includes a continuous recess disposed
concentrically about said aperture and having an asymmetric
V-configured cross-section, the apices of the recesses in
successive electrodes being aligned along the length of the
tube.
9. The device according to claim 8 wherein said tube is part of a
tandem-type accelerator further comprising an electron stripper
element disposed at the downstream end of said tube and toward
which said beam is focused.
Description
BACKGROUND OF THE INVENTION
The present invention relates to high vacuum particle acceleration
tubes and, more particularly, to improvements in such tubes whereby
damage due to arcing is minimized.
High vacuum particle accelerators generally include a series of
apertured electrodes positioned between anode and cathode to define
a path for the accelerated particle beam. These apertured
electrodes are connected to progressively increasing potentials and
spaced by a series of insulating rings made from glass or the like.
Inadvertent arcing within the tube is a fact of life the tube
desgner must live with. Such arcing may be initiated by a stray
particle escaping from the beam and striking an electrode,
resulting in secondary emission from the electrode and arcing
between adjacent electrodes. Alternatively, the arcing may result
from the presence of one or more stray gas molecules finding their
way into the evacuated tube. The component most subject to
permanent damage by such arcing is the insulating spacer ring
between electrodes. Specifically, when an arc occurs between two
adjacent electrodes it tends to pit, burn, or otherwise damage the
insulator.
In the prior art it is known to configure each apertured electrode
with a circular recess disposed about the aperture and having a
symmetrical V configuration. An example of such electrodes may be
seen in U.S. Pat. No. 3,458,743, particularly in FIG. 4. Such
electrodes, because of the recesses, tend to interrupt the radial
path between the tube axis and the insulating rings. Thus, stray
beam particles are intercepted by the electrodes and are not
permitted to cause direct radiation damage to the insulators.
However, since the V-shaped recesses in the electrodes are
symmetrical, arcing between successive electrodes is just as likely
to occur between the outer legs of the V as between the similarly
spaced inner legs. Consequently, arcing proximate the insulators is
not significantly minimized by the recess.
It is therefore an object of the present invention to provide an
electrode structure in a high vacuum particle accelerator tube
which substantially reduces the possibility of damage to the
insulating rings.
It is still another object of the present invention to provide an
electrode structure for a tube of the type described whereby damage
to the insulator rings both by arcing and direct impingement by
stray beam particles is substantially eliminated.
SUMMARY OF THE INVENTION
According to the present invention, the V cross-section of the
electrode recess is asymmetrical such that the radially inward legs
of successive V's are closer to one another than the radially
outward legs. Arcing, if it occurs, will therefore tend to remain
inward of the apex of the V, substantially reducing the possibility
of arcing damage to the insulators.
BRIEF DESCRIPTION OF DRAWINGS
The above and still further objects, features and advantages of the
present invention will become apparent upon consideration of the
following detailed description of one specific embodiment thereof,
especially when taken in conjunction with the accompanying
drawings, wherein:
FIG. 1 is a diagrammatic illustration of a particle accelerator of
the type in which the present invention may be utilized;
FIG. 2 is a plan view in partial section of a portion of one of the
accelerator tubes of FIG. 1; and
FIG. 3 is a detailed plan view in section of the configuration of
two successively disposed electrodes of the present invention.
DESCRIPTION OF THE PREFERRED EMBODIMENT
Referring now specifically to FIG. 1 of the accompanying drawing
there is illustrated a tandem-type particle accelerator 10 having a
grounded casing 11. A high voltage terminal 13 is supported
substantially at the longitudinal center of casing 11. High voltage
is applied across terminal 13 and casing 11, plus to minus
respectively, from a high voltage supply 14, for example of the
type disclosed in U.S. Pat. No. 3,178,604. Evacuated acceleration
tubes 15 and 17 are supported within casing 11, extending
longitudinally therein from respective casing ends to high voltage
terminal 13. Tubes 15 and 17 are aligned with one another and with
a stripper element 19 located within terminal 13. Negative ions are
emitted from an ion source 21 and injected in a beam into
acceleration tube 15 within which they are accelerated toward high
voltage terminal 13. Electrons are removed from the negative ions
in stripper element 19, and the positive ions thus formed are
accelerated through tube 17 to the other end of accelerator 10.
By way of example only, stripper element 19 may be of the type
disclosed in the article "A High Efficiency Ion Optical System For
Tandem Accelerators" by Brooks, et al, appearing in the June, 1965
issue of I.E.E.E. Transactions On Nuclear Science, pages 313
through 316; however any conventional electron stripping unit may
be employed.
Referring now to FIG. 2 of the accompanying drawings there is
illustrated a partial section of the upstream end of acceleration
tube 15 of FIG. 1. By "upstream end" is meant the end through which
the ion beam enters tube 15. As illustrated, tube 15 comprises a
series of alternating apertured electrodes 23 and insulating rings
25. The apertures 27 in the electrodes are axially aligned to
define a path for the ion beam through tube 15. The extreme
upstream electrode is at casing potential (ground).
The terminal voltage V.sub.t applied between terminal 13 and casing
11 is subdivided by a resistor column or string 29. Successive
electrodes 23 are connected to successive points along resistor
string 29 to define a uniform electric field along the length of
tube 15.
Each electrode 23 takes the form of a disk having a central
circular aperture 27 and a circular recess 28 disposed
concentrically about the aperture. As is the case with aperture 27,
the recess 28 of successive disks are aligned throughout the length
of tube 15. The cross-section of recess is V-shaped, the V being
asymmetrical. Specifically, and reference made to FIG. 3, inner leg
31 of each V, which is closer to the tube axis than outer leg 32,
is shorter than outer leg 32. In addition, inner leg 31 subtends a
smaller angle with tube axis A-A than does outer leg 32.
Still referring to FIG. 3, the apex 34 of the V-configured recess
28 extends a very short distance into the recess region of the next
electrode. That is, the apex 34 of the V extends slightly beyond
the plane of the unrecessed upstream surface 33 of the next
downstream electrode 23. By this feature the recesses block the
radial path between tube axis A-A and insulators 25, thereby
intercepting stray particles which escape from the beam and
preventing their impingement against the insulators.
The asymmetry of recesses 28 results in the spacing between inner
legs 31 of successive electrodes being the shortest distance
between these electrodes. Thus arcing, if it occurs at all, tends
to occur between legs 31. Importantly, this arcing path is radially
inward of apex 34 and not at all proximate insulators 25.
Consequently, the possibility of insulator damage, such as pitting,
deposition of metal vapors, etc. due to arcing is significantly
minimized.
While the preferred embodiment has been described as utilized in a
tandem accelerator, tandem operation is obviously not necessary for
the asymmetrical recess to have utility. Nor is the polarity of the
accelerated particle limiting. The important point is that the
asymmetry of the electrode recess acts, in a high vacuum
accelerator tube, to restrict the arcing between successive
electrodes to a region close to the tube axis, thereby protecting
the insulators from arc damage.
While I have described and illustrated one specific embodiment of
my invention, it will be clear that variations of the details of
construction which are specifically illustrated and described may
be resorted to without departing from the true spirit and scope of
the invention as defined in the appended claims.
* * * * *