U.S. patent number 3,609,369 [Application Number 04/719,887] was granted by the patent office on 1971-09-28 for neutron generator with radiation acceleration.
This patent grant is currently assigned to Instituttul de Fizica Atomica (IFA). Invention is credited to Petrica Croitoru.
United States Patent |
3,609,369 |
Croitoru |
September 28, 1971 |
NEUTRON GENERATOR WITH RADIATION ACCELERATION
Abstract
Method of and apparatus for generating high neutron flux at a
sample zone maintained at atmospheric pressure and surrounded by an
annular evacuated generator housing along whose inner peripheral
wall is provided a neutron emitter target. An annular array of
ion-particle sources or an annular ion source surrounds the annular
target to direct radial charged-particle beams thereagainst. The
acceleration may be effected by radially spaced accelerator plates
disposed between the source and the target within the chamber or by
radio waves supplied to the chamber; the latter is then constituted
as a coaxial resonant cavity.
Inventors: |
Croitoru; Petrica (Bucharest,
RU) |
Assignee: |
Instituttul de Fizica Atomica
(IFA) (Bucharest, RU)
|
Family
ID: |
20086587 |
Appl.
No.: |
04/719,887 |
Filed: |
April 9, 1968 |
Foreign Application Priority Data
Current U.S.
Class: |
376/108; 250/398;
376/107; 376/151; 376/342 |
Current CPC
Class: |
H05H
9/00 (20130101); H05H 3/06 (20130101); B07B
13/00 (20130101); H05H 7/18 (20130101); H05H
7/00 (20130101) |
Current International
Class: |
B07B
13/00 (20060101); H05H 3/00 (20060101); H05H
7/14 (20060101); H05H 7/00 (20060101); H05H
9/00 (20060101); H05H 3/06 (20060101); H05H
7/18 (20060101); G21g 003/04 () |
Field of
Search: |
;250/845,16S,16T,51
;313/61 |
References Cited
[Referenced By]
U.S. Patent Documents
Primary Examiner: Lindquist; William F.
Assistant Examiner: Frome; Morton J.
Claims
I claim:
1. A high-intensity neutron generator comprising an annular
evacuated housing having an annular inner wall adapted to surround
a sample at ambient pressure; an annular neutron-emissive target
activatable by accelerated charged particles disposed along said
wall for subjecting said sample to high-intensity neutron flux; a
plurality of charged-particle sources spaced radially from said
target for radially directing charged-particle beams substantially
uniformly against said target and across the evacuated space
between said source and said target; and particle-accelerator means
for radially accelerating the particles of said beam, said
particle-accelerator means including radially spaced generally
annular electrodes disposed in said space around said target and
provided with openings passing said beam and means for applying an
accelerating field across said electrode.
2. The generator defined in claim 1, further comprising
continuously operable pumping means connected with said housing for
maintaining said space under reduced pressure.
3. The generator defined in claim 1, further comprising a gettering
means in said housing for maintaining said space at a reduced
pressure.
4. The generator defined in claim 1 wherein said source is an
annular ionized-particle source directing charged particles against
said target generally uniformly therealong.
5. The generator defined in claim 1 wherein said charged-particle
source includes a plurality of angularly spaced ionized particle
sources trained on said target for producing overlapping
charged-particle beams impinging thereagainst.
6. The generator defined in claim 1 wherein said source includes a
plurality of axially spaced ionzied-particle sources training
coplanar axially overlapping beams against said target.
7. The generator defined in claim 1 wherein said
particle-accelerating means includes means for sustaining a
particle-accelerating radiofrequency field in said space.
8. The generator defined in claim 1 wherein said target is
generally cylindrical.
9. A high-intensity neutron generator comprising an annular
evacuated housing having an annular inner wall adapted to surround
a sample at ambient pressure; an annular neutron-emissive target
activatable by accelerated charged particles disposed along said
wall for subjecting said sample to high-intensity neutron flux; at
least one annular charged-particle source spaced radially from said
target for radially directing at least one charged-particle beam
substantially uniformly against said target and across the
evacuated space between said source and said target, said annular
ionized-particle source directing charged particles against said
target generally uniformly therealong; and particle-accelerator
means for radially accelerating the particles of said beam.
Description
My present invention relates to a method of generating neutrons at
high intensity and of irradiating a sample with high-intensity
neutrons, and to an apparatus capable of producing high-intensity
neutron fluxes in a sample-accommodating region.
In general, neutron generators and apparatus for the production of
a neutron flux, referred to generally in the art as "neutron
sources," comprise a mass of materials capable of undergoing
nuclear reaction and transformation to yield neutrons. Such neutron
sources may make use of a particle-generating substance capable of
radioactive decay to yield bombarding particles, e.g. particles
(.sub.2 He.sup.4), which impinge upon a target (e.g. lithium,
beryllium,...) to yield neutrons for irradiating a specimen or
sample. Typical .alpha.-particle sources are radium, plutonium, and
the like. In these systems, the bombarding source is intimately
combined with the target material, e.g. as an alloy.
In the other E.G. type of neutron generator, usually referred to as
an e.g. or C.W. generator, a high or low energy, linear or
nonlinear direct charged-particle accelerator is used for neutron
production. The accelerated charged-particle beam is allowed to
impinge on a suitable target such that a neutron flux is produced
by the resulting nuclear reactions. Thus the neutrons may result
from nuclear reactions between a beam of deuterons (D or .sub.1
H.sup.2 ion), tritons (T or .sub.1 H.sup.3 ion), or a mixture of
these charged particles, which are accelerated to high-energy in an
electric field via an electrostatic high-voltage accelerator (E.G.)
or a Cockroft-Walton high-voltage accelerator (C.W.) and are
focused on a target which may contain tritium or deuterium or
mixtures thereof, beryllium, and like materials known to have a
high neutron yield when bombarded with the high-energy-charged
particles. A typical reaction is that of the deuteron undergoing
nuclear transformation with a tritium nucleus to form an
.alpha.-particle and a neutron D+ .sub.1 H.sup.3 .sub.2 He.sup.4
+.sub.0 n.sup.1). Such neutron generators may be of a variety of
different constructions although, in general, a single linear beam
source directs its beam upon a stationary or rotating target disk.
In these systems, at the sample level, the neutron flux (in terms
of the number of neutrons/cm..sup.2) is much lower than the
specific rate or rating of the target. It is possible to reduce the
difference between the neutron flux at the sample level and the
specific rate of the target by using large-diameter targets
although this increase is accompanied by difficulties in obtaining
high-intensity beams of large aperture and constant density at the
target.
It is, therefore, the principal object of the present invention to
provide an improved method of increasing the neutron flux intensity
at the sample irradiation zone in a neutron generator using a
charged-particle accelerator as previously described.
A further object of this invention is to provide an improved
neutron generator with direct charged-particle acceleration,
adapted to provide high neutron flux and neutron irradiation of
high intensity at the sample irradiation zone.
Still another object of this invention is to provide a neutron
generator of the character described, in the form of a neutron tube
with high neutron flux in the sample zone.
Yet a further object of this invention is to provide an improved
neutron generator using charged-particle acceleration in a
radiofrequency field having intensive neutron flux in a sample
zone.
I have found that these objects and other which will become
apparent hereinafter, can be attained by providing an annular
target capable of undergoing nuclear interaction with an
accelerator-particle beam which closely surrounds an axis of
symmetry and may extend along that axis in the form of a tube or
cylinder while a charged-particle (i.e. ion) beam is directed at
this target from at least one, but preferably a plurality of,
charged-particle injectors or sources while radially effective
accelerator means is provided in the common continuously evacuated
envelope housing the target for radial acceleration of the incident
ion beam toward the cylindrical target. The region surrounded by
the target constitutes the sample irradiation zone and may be
unevacuated (i.e. at atmospheric pressure) while the target may
contain deuterium, tritium, beryllium or other neutron emitters
undergoing neutron production upon interaction with the ion beams.
The sample is thus located within the axial limits of the
cylindrical target and in the interior thereof so that, at the
sample level, the neutron flux will generally be equal to the
specific rate of the target. According to a further feature of this
invention, the impinging charged-particle beams are directed from a
number of sources against the cylindrical target, the source being
angularly spaced around the axis of the target and, therefore, its
cylindrical periphery; angular equispacing is preferred.
Furthermore, the angularly equispaced, radially directed and
preferably divergent charged-particle beams impinge upon mutually
overlapping zones of the target and thus ensure a substantially
uniform radiation intensity.
Still another feature of this invention resides in the use,
independently of but possibly in combination with the preceding
feature, of a plurality of axially offset beams of charged
particles which impinge upon axially overlapping zones of the
cylindrical target. Advantageously, the axially overlapping zones
may derive from charged-particle beams whose axes lie in a common
axial plane of the cylindrical target but converge with respect to
one another at the target so that, for example, a central beam is
directed normal to the surface of the target in each of the axial
planes while at least a pair of outer beams are oriented toward one
another and thus converge toward the normal to the surface
corresponding to the axis of the central beam.
The term "cylindrical" used with reference to the target, is
intended to refer also to prismatic configurations having axial
symmetry. Thus, the target may be a right-circular cylinder or a
body of revolution produced by a line generatrix rotated about the
axis of the device along a closed path which may be noncircular.
With the use of a prismatic target, the generatrix will be rotated
about the axis along a polygonal path with angularly adjoining
sides, thereby imparting a transverse cross section to the target
corresponding to the polygon. The charged-particle sources are
preferably located equidistantly from the surface of the target as
measured along the axis of the respective beam, while the
particle-accelerator means comprises a plurality of electrodes
forming acceleration gaps which also are equidistant from the
target surface at each acceleration region.
According to still another feature of this invention, an annular
ion source is provided (as distinct from a plurality of
charged-particle sources equispaced around the surface of the
target) and its ion particles are directly and radially accelerated
in the direction of the target by continuous or pulsed electric
field or by a radio frequency field of a coaxial cavity
resonator.
The above and other objects, features and advantages of the present
invention will become more readily apparent from the following
description, reference being made to the accompanying drawing in
which:
FIG. 1-A is an axial cross-sectional view, partly in diagrammatic
form of a neutron-irradiating generator, according to the present
invention;
FIG. 1-B is a transverse cross-sectional view through another
arrangement of this character;
FIG. 1-C is an axial cross-sectional view through a system
embodying principles of both these systems;
FIG. 2 is a diagrammatic cross-sectional view of a neutron tube
capable of generating high-intensity neutron flux; and
FIG. 3 is a longitudinal section, partly in diagrammatic form,
through a neutron generator using a resonant coaxial cavity and a
radiofrequency electric field as the acceleration means.
In FIG. 1, I show a neutron generator which comprises an envelope 1
having an inner tubular core 1a receiving the specimen I to be
irradiated and centered upon the axis of symmetry A of the neutron
generator. The tubular core 1a and the outer housing wall 1b form a
vacuum tight enclosure with a pair of electrically insulating
thermal disks 2 which is subjected to continuous evacuation and
suction by the pumping system represented at P. The pumping system
may be any of those described at pages 843-856 of the "Concise
Encyclopedia of Nuclear Energy," Interscience Publishers, New York,
1962. Within the accelerator chamber and coaxially therewith, I
provide a cylindrical target 7 containing deuterium, tritium,
beryllium or like material capable of generating neutrons upon
radiation with an accelerated charged-particle beam.
In a number of axial planes, I provide along the outer wall 1b of
the housing 1, a number of ion sources S.sub.1, S.sub.2, S.sub.3,
these sources generating annular beams F.sub.1, F.sub.2 and
F.sub.3, respectively, in the form of inwardly diverging sheetlike
distributions of charged particles. Instead of the single
annular-ion source at each of a plurality of axially spaced
locations, duoplasmatron or Penning ion sources may be used. When
the annular sources (centered on the axis A and axially spaced
therealong) are employed, they may be of the type described in
"Journal de Physique et Radium," vol. 12 (1951), p. 563.
Three such beams are shown in FIG. 1-A including a central beam
lying in the radial plane R.sub.p and a pair of inwardly directed
beams whose axes are represented at R.sub.p ' and R.sub.p ",
respectively. The beams diverge toward the target 7 and overlap
upon impingement thereagainst.
The radial accelerator means of this system includes a plurality of
inwardly concave generally coaxial accelerator electrodes 3, 4, 5
and 6 which are provided with circular slits 3', 3", 3'", etc.
permitting passage of the beams F.sub.1, F.sub.2 and F.sub.3,
respectively. A pulsed or continuous electrostatic accelerator
source (E.G. as described in my concurrently filed copending
application Ser. No. 719,963, now Pat. No. 3,551,728, entitled
"HIGH-INTENSITY LINEAR ACCELERATORS" or as described in the
"Concise Encyclopedia of Nuclear Energy" mentioned earlier), is
represented at E and is connected to the electrodes 3,4,5,6 to
apply a continuous or pulsed electrostatic field across the gaps
3a, 4a, 5a between the pairs of the electrodes, thereby
accelerating the charged-particle beams F.sub.1, F.sub.2, F.sub.3
in the direction of the target 7. The charged particles, preferably
high-energy deuterons and tritons as indicated earlier, undergo
nuclear reaction with the target 7 with generally radial inward
emission of neutrons as represented by the arrows n, thereby
subjecting the sample I to a high-energy neutron flux.
In the embodiment illustrated in FIG. 1-B the cylindrical housing 8
is hermetically sealed and has a tubular core 8a carrying the
neutron-emitting target 13 in the form of a cylinder. The sample I
is received within the cylinder for neutron irradiation in the
direction of arrows n. In this embodiment, however, a plurality of
duoplasmatron or Penning-type ion sources S.sub.4, S.sub.5, S.sub.6
etc. are disposed in a common radial plane and are angularly
equispaced along the outer wall of housing 8 to direct beams
F.sub.4, F.sub.5 and F.sub.6 etc. of charged particles radially
inwardly along the respective radii R.sub.4, R.sub.5 and R.sub.6 of
the target 13. These beams F.sub.4, F.sub.5, F.sub.6 ... diverge
inwardly and overlap along the angular zones of the target against
which they impinge. In this embodiment, the electrodes 9, 10, 11
and 12 are radially spaced but coaxially disposed within the
chamber 8c of the housing 8, which is evacuated by the continuous
pumping system P. The electrodes 9- 12 are provided with angularly
equispaced slits 9a, 9b, 9c ... extending along generatrices and
parallel to the axis of the device. The slits associated with each
beam are radially aligned as represented for the slits 9a, 10a, 11a
and 12a for the beam F.sub.4. The slits increase progressively in
angular width to ensure the divergence of the beams. The
electrostatic field source E' is connected to each of the
electrodes to sustain an accelerating potential difference across
the gaps 9', 10' and 11' as described in the aforementioned
copending application and in connection with FIG. 1-A.
Since the housing 8 is hermetically sealed and of generally
toroidal shape, the sample I is located at the high-flux zone and
is at atmospheric pressure.
In FIG. 1-C, I show an arrangement in which the housing 31
approaches a torus in configuration and is evacuated by the
continuously operating pump 32. A cylindrical neutron-emitting
target 33 is disposed along the core 34 of the toroid in which the
sample I is positioned at atmospheric pressure. In each of the
radial planes R.sub.p, R.sub.p ' and R.sub.p " of the device,
oriented as in FIG. 1-A, a plurality of ion sources S.sub.7,
S.sub.8, etc. are angularly equispaced from one another about the
axis A. The corresponding sources S.sub.7, S.sub.7 ' and S.sub.7 "
are located in common axial planes of the device represented, for
example, by the plane of the paper in FIG. 1-C. The accelerator
electrodes conform to coaxial spherical segments as shown for the
electrodes 35, 36, 37 and 38 which are provided with the slits 35a,
36a, 37a and 38a in this Figure. The continuous or pulsed
electrostatic field source E" is connected to these electrodes as
previously described.
In FIG. 2, I show a neutron-generating tube in which a tubular
glass envelope 14, which is sealed after evacuation, is provided
with a pressure-regulating getter 15, heated via leads 15' and 15"
by an electric current supplied from the exterior. In another leg
of the annular housing, I provide a mechanical/electrical
transducer 16 serving as a pressure gauge and designed to indicate
the pressure within the tube 14 via a meter 16a connected to the
leads of the gauge period. Within the tube 14, whose inner
relatively thin wall 19 receives a cylindrical deposit of the
target material 18 (a tritium or deuterium/tritium substance of
conventional composition), I provide a ring-shaped ion source 17
including radially spaced accelerator electrodes as described in
connection with FIGS. 1-A and 1-B previously. Again, a well 19a is
provided within the housing at atmospheric pressure for receiving
the sample.
The embodiment of FIG. 3 comprises a ring-shaped ion source S whose
charged particles are accelerated radially toward a target 21
sealed within an annular zone of the cavity resonator 20 which is
supplied, e.g. as described in the aforementioned copending
application, with radiofrequency waves adapted to accelerate the
charged particles. Within the ring formed by the target and the
angular cavity resonator, the sample may be disposed at atmospheric
pressure. The pumping system P operates continuously to evacuate
the system. In all of the aforementioned devices, the neutron flux
at the sample zone is generally equal to the specific rate of the
target.
The invention described and illustrated is believed to admit of
many modifications within the ability of persons skilled in the
art, all such modifications being considered within the spirit and
scope of the appended claims.
* * * * *