U.S. patent number 3,710,163 [Application Number 05/111,838] was granted by the patent office on 1973-01-09 for method for the acceleration of ions in linear accelerators and a linear accelerator for the realization of this method.
Invention is credited to Vasily Alexeevich Bomko, Anatoly Vasilievich Pipa, Evgeny Ivanovich Revutsky, Boris Ivanovich Rudiak.
United States Patent |
3,710,163 |
Bomko , et al. |
January 9, 1973 |
METHOD FOR THE ACCELERATION OF IONS IN LINEAR ACCELERATORS AND A
LINEAR ACCELERATOR FOR THE REALIZATION OF THIS METHOD
Abstract
The present invention relates to methods for acceleration of
ions in linear accelerator and to a linear accelerator realizing
this method. The method for the acceleration of ions in linear
accelerators consisting of a cavity resonator 1 and drift tubes 2
employing a standing r.f. electromagnetic wave, according to the
invention, is characterized in that the resonator is excited in the
E.sub.011 mode enabling the energy of the accelerated-ion beam to
be controlled continuously by establishing a region with a uniform
distrubution of the accelerating field and by varying the extent of
that tregion. This method can be realized by a linear accelerator
comprising a cavity resonator 1 with drift tubes 2; tuners 3
arranged on the side wall of the resonator 1; an additional tuning
means made in the form of a conducting post 4 installed in an end
wall of the resonator 1 near its side wall parallel with the axis
of the resonator and capable of being moved along that axis.
Inventors: |
Bomko; Vasily Alexeevich
(Kharkov, SU), Revutsky; Evgeny Ivanovich (Kharkov,
SU), Rudiak; Boris Ivanovich (Kharkov, SU),
Pipa; Anatoly Vasilievich (Kharkov, SU) |
Family
ID: |
22340704 |
Appl.
No.: |
05/111,838 |
Filed: |
February 2, 1971 |
Current U.S.
Class: |
313/360.1;
315/5.41; 315/505 |
Current CPC
Class: |
H05H
9/04 (20130101); H05H 7/18 (20130101) |
Current International
Class: |
H05H
7/18 (20060101); H05H 7/14 (20060101); H05H
9/04 (20060101); H05H 9/00 (20060101); H05h () |
Field of
Search: |
;313/63 ;315/5.41,5.42
;328/233 |
References Cited
[Referenced By]
U.S. Patent Documents
|
|
|
2867748 |
January 1959 |
Van Atta et al. |
|
Primary Examiner: Lake; Roy
Assistant Examiner: Mullins; James B.
Claims
What is claimed is :
1. A method for the acceleration of ions in linear accelerators of
the cavity resonator type with drift tubes, employing a standing
r.f. electromagnetic wave in the E.sub.011 mode, enabling the
energy of the accelerated-ion beam to be controlled continuously by
establishing a region with a uniform distribution of the
accelerating field and by varying the extent of that region.
2. A linear accelerator to realize the method for the acceleration
of ions, comprising a cavity resonator with drift tubes; tuners
arranged on the side wall of said resonator; an additional tuning
means ensuring control of the extent of the region with a uniform
distribution of the accelerating field and made in the form of a
conducting post installed in an end wall of said resonator, near
its side wall parallel with the axis of said resonator and capable
of being moved along that axis.
Description
The present invention relates to accelerators, and more
specifically to methods for the acceleration of ions in linear
accelerators and to linear accelerators for their realization.
In the prior art, there is a method for the acceleration of ions in
linear accelerators which are cylindrical cavity resonators with
drift tubes. This method is based on the excitation of an r.f.
electromagnetic standing wave in the E.sub.010 mode, in which case
the electric field is uniformly distributed along the axis of the
resonator. In this case, because of the requirement for
synchronism, acceleration can be effected only at a single value of
the accelerating field strength.
A disadvantage of this method is that the accelerated-particle beam
at the output from the accelerator can only have one value of
energy for which the accelerator has been designed. On the other
hand, most research and development programmes may be markedly
extended, if the energy of the accelerated particles can be
adjusted within broad limits.
Intermediate energies have been obtained on the heavy-ion linear
accelerators at Berkeley, U.S.A., and Manchester, Great Britain, by
varyin the tilt of the accelerating field excited in the E.sub.010
mode.
Among the disadvantages of this method are the impossibility of
continuously controlling the energy of the accelerated particles,
more than a two-fold loss of beam intensity, increased energy
spread, and impaired stability of accelerator operation.
Another method for obtaining accelerated particles with
intermediate energies is based on the use of a chain of single
resonators uncoupled for the r.f. supply. By cutting off the r.f.
supply to a certain number of the final resonators, it is possible
to obtain beams with the energy attained at the excited
resonators.
Among the disadvantages of this method are the difficulty of
feeding the chain of uncoupled resonators with r.f. power in phase,
the complex design and the low efficiency of the accelerator
because of considerable additional losses of r.f. power on the many
end walls in the chain of resonators.
Neither of these methods offers a means for the continuous control
of the energy of accelerated particles.
An object of the present invention is to avoid the above-mentioned
disadvantages.
The present invention is aimed at providing a method for the
acceleration of ions in linear accelerators ensuring the continuous
control of the energy of accelerated particles without any
impairment in the quality of the beam, owing to a change in the
mode of excitation, and at developing a linear-accelerator which
realizes this method in the simples and most efficient way.
The present invention resides in that in the method disclosed
herein ions are accelerated by an r.f. field excited in the
E.sub.011 mode, enabling the energy of the accelerated particles to
be controlled continuously by establishing region in which the
accelerating field strength is distributed uniformly and by varying
the extent of this uniform region, while the linear accelerator
intended to realize this method, consisting of a cavity resonator
with drift tubes and with tuners arranged on its side wall, has an
additional tuning means made in the form of a conducting post
installed in an end wall of the resonator near its side wall in
parallel with the axis of the resonator and capable of being moved
along this axis.
The fundamentally new method for the acceleration of particles
disclosed herein enables the energy of the accelerated particles to
be controlled continuously within broad limits (from one-third to
the maximum energy of the accelerator) without any loss in the
intensity of the accelerated beam. This acceleration method, in
conjunction with the additional tuning means made in the form of a
conducting post installed in an end wall of the resonator near its
side wall in parallel with the axis of the resonator and capable of
being moved along this axis, when used in a linear accelerator
intended to realize this method, ensures high monochromaticity and
stability of the characteristics of the beam with time without
posing stringent requirements for the accuracy of the elements of
the accelerating structure.
It is important that any linear accelerator can be switched over to
controlled beam energy operation with ease and with only minor
changes in its construction.
The additional tuning means for beam-energy control disclosed
herein is very simple in design. The principle underlying the
method for energy control and the construction of the tuning
element make it possible to accomplish this control automatically
to a pre-determined program.
A further advantage of the acceleration method disclosed herein is
that it can be realized on the prior-art linear accelerators
without major changes in construction and, as a consequence,
without additional capital outlays.
The invention will be more fully understood from the following
description of preferred embodiments when read in connection with
the accompanying drawings wherein:
FIG. 1 is a plot showing the distribution of the accelerating field
along the resonator excited in the E.sub.011 mode;
FIG. 2 shows the construction of a linear accelerator according to
the invention;
FIG. 3 is a plot showing the frequency of the E.sub.011 mode and
the frequencies of the nearby modes as functions of the length of
the post immersed into the resonator;
FIG. 4 shows the spectra of some of the intermediate beam energies
obtained in an experiment on a linear accelerator designed for a
maximum proton energy of 9 MeV.
The method for the acceleration of ions disclosed herein consists
in that acceleration is accomplished by an r.f. field excited in
the E.sub.011 mode, by establishing a region in which the
accelerated field is distributed uniformly and the extent of which
can be controlled at will. Ordinarily, when the E.sub.011 mode is
excited in the resonator of a linear accelerator with drift tubes
all cells of which are tuned to resonate at the same frequency, the
distribution of the r.f. electric field along its axis obeys the
cosine law (curve a in FIG. 1).
The region in which the accelerating field is distributed uniformly
and the extent of which can be controlled at will is realized in
the linear accelerator of FIG. 2 which is a cylindrical cavity
resonator 1 with drift tubes 2, tuners 3 arranged on its side wall,
and an additional tuning means made in the form of a conducting
post 4 installed on an end wall of the resonator near its side wall
so that it can be moved along the axis of the resonator. By varying
the length to which the post 4 is immersed into the resonator, one
can shift the node of the electric field along the axis of the
resonator and, as a result, reduce the field strength represented
by the right-hand branch of curve b in FIG. 1, which by varying the
depth of immersion into the resonator for the tuners 3, one can
produce a region with a uniform distribution and a steep downward
jump of the accelerating field.
If the extent of the region with the uniform distribution and an
ideally steep downward jump of the accelerating field is changed,
the energy of the accelerated particles will also change in a jamp,
in step with the change of energy across one accelerating period.
In practice, the downward jump is gradual rather than abrupt.
Therefore, it is possible, by varying the slope of the jump, to
control energy continuously within the limits corresponding to the
change of energy across one accelerating period.
In the limiting case, by adjusting the depth of immersion into the
resonator for the tuning post 4 and the tuners 3, it is an easy
matter to obtain a uniform distribution for the accelerating field
strength along the entire resonator owing to the said deformation
of the field excited in the E.sub.011 mode.
Within certain limits, regions with a uniform distribution of field
strength in the resonator excited in the E.sub.011 mode can be
controlled solely by means of the tuners 3. However, in this case,
the control is more difficult, since it involves a considerable
increase in the size of the tuning means. Besides there remains the
right-hand branch of the field (represented by curve c in FIG. 1)
which results in an increased energy spread of the beam of
accelerated particles.
In actual operation of the accelerator, the continuous control of
the energy of accelerated ions is accomplished by moving the post 4
and the tuners 3 to a pre-determined program under which the length
of post 4 immersed into the resonator and the depth of immersion
into the resonator for the tuners 3 are calibrated in advance
according to the required energy of the accelerated particles. This
control, can be accomplished automatically. Furthermore, the length
of the post 4 immersed into the resonator 1 and the depth of
immersion for the tuners 3 can be varied from the outside, without
any impairment of the vacuum in the resonator.
The stability of the characteristics of the accelerated beam in the
face of changes in the energy of the accelerated particles is
ensured by increasing the separation between the resonant frequency
f.sub.011 of the resonator, corresponding to the E.sub.011 mode,
and the frequencies f.sub.010 and f.sub.012 (FIG. 3) of the nearby
modes, as the length 1 of the post 4 immersed into the resonator 1
(FIG. 2) is increased. The stability of the accelerating field is
enhanced accordingly.
As an example of an embodiment of the acceleration method disclosed
herein, we may quote the results obtained on a linear proton
accelerator with a maximum design energy of 9 MeV. This accelerator
operated in an experimental program, with the continuous control of
the energy of accelerated particles. Energy control was
accomplished remotely. Some of the spectra of the beams accelerated
under conditions of continuous energy control are shown in FIG. 4.
The energy of accelerated particles is laid off as abscissa and the
relative intensity of the beams at the output of the accelerator is
laid off as ordinate.
The slight decrease in beam intensity with decreasing energy of the
accelerated particles seen in the spectra of FIG. 4 does not steam
from the essence of the acceleration method disclosed herein, but
is due to the type of beam focusing used in acceleration. In the
case on hand, use was made of grid focusing, with the result that
for some length of the accelerator where the accelerating field was
not applied the beam was not focused either, and some of the
accelerated particles were lost. No loss of beam intensity occurs
when the accelerated beam is focused by quadrupole magnetic lenses
installed in the drift tubes.
* * * * *