U.S. patent number 3,883,761 [Application Number 05/313,451] was granted by the patent office on 1975-05-13 for electrostatic extraction method and apparatus for cyclotrons.
This patent grant is currently assigned to The Cyclotron Corporation. Invention is credited to George O. Hendry.
United States Patent |
3,883,761 |
Hendry |
May 13, 1975 |
Electrostatic extraction method and apparatus for cyclotrons
Abstract
A method and apparatus for electrostatically extracting high
beam currents at improved energy from small diameter, high magnetic
field cyclotrons by deflecting particles from their trajectory
within an electrostatic field traversing an extraction channel
wherein magnetic material immediately adjacent to the inside of at
least a portion of the channel first reduces the fringe field and
then reverses its normal gradient to assist in extraction and to
focus the extracted beam radially with respect to the center of the
cyclotron.
Inventors: |
Hendry; George O. (Napa,
CA) |
Assignee: |
The Cyclotron Corporation
(Berkeley, CA)
|
Family
ID: |
23215733 |
Appl.
No.: |
05/313,451 |
Filed: |
December 8, 1972 |
Current U.S.
Class: |
313/62;
315/502 |
Current CPC
Class: |
H05H
13/00 (20130101); H05H 7/10 (20130101) |
Current International
Class: |
H05H
7/10 (20060101); H05H 7/00 (20060101); H05H
13/00 (20060101); H05l 013/08 () |
Field of
Search: |
;313/62 ;328/234
;250/49.5ME |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lawrence; James W.
Assistant Examiner: Anderson; B. C.
Claims
I claim:
1. Improved apparatus for electrostatically deflecting a beam of
charged particles at an extraction radius in the fringe magnetic
field of an isochronous cyclotron comprising
means defining an electrostatic field across a deflection channel
at the extraction radius, the location of said field increasing in
radius with respect to the center of the cyclotron; and
magnetic material positioned inside and adjacent to at least a
portion of said channel to reduce the cyclotron fringe field at the
channel and to focus the beam of charged particles radially with
respect to the center of the cyclotron, by concentrating the lines
of magnetic force of said fringe field inwardly of but immediately
adjacent to said channel to reduce said fringe field and then to
reverse the normally decreasing field gradient in said channel.
2. The apparatus of claim 1 wherein the means defining an
electrostatic field includes a thin curved septum and a curved
deflector electrode which define between them a shaped deflection
channel with a high electric field gradient across it and the
magnetic material is positioned along inside of at least a portion
of said septum.
3. An improved method for electrostatically deflecting a beam of
charged particles at an extraction radius in the fringe magnetic
field of an isochronous cyclotron comprising the steps of
defining an electrostatic field within a channel at the extraction
radius which increases in radius with respect to the center of the
cyclotron; and
placing a magnetic member along at least a portion of said channel
to concentrate the lines of magnetic force of said fringe field
inwardly of but immediately adjacent to said channel to reduce said
fringe field and then to reverse the normally decreasing field
gradient in said channel.
Description
This invention relates generally to beam extraction from cyclotrons
and more particularly to a method and means for extracting a
high-energy high quality beam from small diameter isochronous
cyclotrons.
One object of this invention is to increase the amount and quality
of beam current available from a small diameter, high magnetic
field isochronous cyclotron.
Another object of this invention is to provide a method and means
for enabling electrostatic deflection of a beam of higher energy
particles from an isochronous cyclotron of any fixed diameter.
Other objects and advantages of this invention will become apparent
from a consideration of the following description in connection
with the accompanying drawings wherein
FIG. 1 is a partially schematic cross-sectional view of a typical
isochronous cyclotron at its median plane;
FIG. 2 is a plan view of the electrostatic deflection assembly of
this invention;
FIG. 3 is a cross-sectional view of a portion of the electrostatic
deflection assembly taken along line 3--3 of FIG. 2; and
FIG. 4 is a curve plotting fringe magnetic field strength (B) of
the cyclotron against radius in the region of the extraction
radius.
This invention relates to electrostatic extraction methods and
apparatus, for example, like those known for isochronous cyclotrons
generally disclosed in U.S. Pat. No. 3,582,700 entitled Cyclotron
Beam Extraction System and in copending application Ser. No.
118,751 entitled Improved Cyclotron Beam Extraction filed on Feb.
25, 1971 by George O. Hendry and Dale K. Wells, now U.S. Pat. No.
3,725,709. The external beam current of the isochronous cyclotrons
therein described for a fixed cyclotron diameter can be produced at
higher energy, increased in amount and improved in quality by the
present invention wherein magnetic material is placed along at
least a portion of the electrostatic deflection channel. The
magnetic material concentrates the lines of magnetic force of the
fringe field of the cyclotron, first to reduce that field at the
electrostatic deflection channel and thereby assist in deflection
and second to reverse the fringe field gradient so that it tends to
focus the extracted beam of particles radially with respect to the
center of the cyclotron.
FIG. 1 illustrates the orientation of the electrostatic deflection
assembly of this invention with respect to the other components of
a typical small isochronous cyclotron at its median plane. A main
d-c electromagnet defines a magnetic guide field for the particles
orbiting within the evacuated region of the cyclotron. The main d-c
magnet includes a lower yoke slab 2, a pair of interconnecting iron
legs 3 and two cylindrical iron pole bases 4, the lower one of
which is shown in FIG. 1. In the described embodiment the lower
pole tip is warp plate 6b that, with sidewalls and with a similar
upper warp plate, forms a vacuum tank within which charged
particles are accelerated in the machine.
Three shaped hill pieces 9 mount on each of the warp plates in
corresponding locations to produce the azimuthally varying field
necessary for isochronous operation. A pair of hollow 120.degree.
dees within the vacuum tank provides a radio frequency accelerating
field and an ion source supplies ions for acceleration in the
central region of the cyclotron between the two dees all as is more
fully described in U.S. Pat. No. 3,582,700.
In the described embodiment the extraction system includes
electrostatic deflection means 30 and a magnetic channel 31 which
receives and radially focuses a beam of ions deflected by the
electrostatic deflection means. Also a preseptum unit 50 mounts
adjacent to the electrostatic deflection means 30 at the extraction
radius and precedes it with respect to the path of orbiting
particles as is more fully described in copending application Ser.
No. 118,751 now U.S. Pat. No. 3,725,709.
FIGS. 2-3 show the improved electrostatic deflection assembly of
this invention in detail. It includes a thin curved tungsten septum
35 maintained at ground potential and a curved deflector electrode
36 which is held at a high negative potential (for positively
charged, accelerated particles). The septum 35 and deflector
electrode 36 define between them a shaped electrostatic deflection
channel 37 with a high electric field gradient which is located so
it increases in radius with respect to the center of the cyclotron.
When traversed by the orbiting particles segregated by the
preseptum 50, the electrostatic field forces the particles to move
to a larger radius where they no longer are held in a circular path
by the main magnet.
The septum and deflector electrode are carefully shaped and located
so that the segregated beam remains centered in the channel as it
moves to greater radius. Both mount upon a water cooled
non-magnetic base plate 38 on one of the hill pieces 9 as shown in
FIG. 1. The septum 35 clamps to the base plate 38 and an upper
cooling plate 39. A pair of alumina insulators 46 cantilevered from
brackets 47 support the hollow copper deflector electrode 36 from
base plate 38. Electrode 36 is cooled by water coolant supplied to
its interior through hollow electrical conductor 48a and returned
through conductor 48b. The same conductors 48a, 48b provide high
negative potential to the electrode from its power supply.
After leaving the electrostatic channel 37 the beam of extracted
particles follows a path of increasing radius and is focused
radially by magnetic channel 31.
While output beam currents in the order of 50 microamperes of 22
MeV protons can be obtained in a 30 inch cyclotron with the
described electrostatic deflection means alone, an improvement in
external beam energy for the same cyclotron diameter in the order
of 50 microamperes at 30 MeV protons can be obtained by placement
of magnetic material inside at least a portion of the electrostatic
deflection channel 37. As is more particularly shown in Figs. 2 and
3, this magnetic material can be in the form of an iron bar 60
clamped to septum 35 at its terminal end from which the extracted
beam leaves channel 37. In the described embodiment, for example,
iron bar 60 is secured to the septum 35 by a pair of clamps 61 to
which it is held by cap screws 62.
The presence of the magnetic material concentrates the lines of
force of the fringe magnetic field of the machine through it, first
to reduce the fringe field just radially beyond it and to assist
the electrostatic deflection and second to reverse the gradient of
the fringe field and focus the extracted particles radially with
respect to the center of the cyclotron.
For example, in FIG. 4 the curve 70 shown in solid lines depicts
the normal fringe magnetic field (B) plotted against the machine
radius in the region of the extraction radius. At the entrance to
the electrostatic channel 37, the electric field across it normally
reduces the net fringe field as shown in the vertical portion 71 of
the curve 70. The net field then has a normally reducing gradient
as at 72 of the same slope as the fringe field would have without
the effect of the uniform electrostatic field. At the terminal end
of the channel the electrostatic field no longer has any effect and
the net fringe field returns verticallly at 73 to its normal value
along curve 74.
With the magnetic material of this invention in place, however, the
normal fringe field in the region of the extraction radius is
modified as shown in hidden lines in FIG. 4. The net field
increases as at 80, then drops vertically along 71 to a value 81
less than that normally reached without the iron in place. Then,
the normally decreasing gradient through the channel at 72 is
reversed so that, as one moves radially, the net field has an
increasing gradient as at 82 to the end of the channel where the
curve resumes the same shape 73 as in normal operation.
The specific iron placement of this invention is shown for
illustrative purposes only. The iron bar may vary in size or shape
or may extend further along the septum. In practice it has been
found that the iron should extend as far as possible along the
channel to produce the effects described, but should not be so long
as to have the internally orbiting particles impinge upon it which
are not segregated by the septum and preseptum and directed through
the electrostatic channel. Those and various other modifications
will be apparent to those skilled in the art within the scope of
the invention defined in the following claims.
* * * * *