Container, method for obtaining same and target assembly for the production of radioisotopes using such a container
10854349 ยท 2020-12-01
Assignee
Inventors
Cpc classification
C25D1/003
CHEMISTRY; METALLURGY
International classification
Abstract
The invention relates to a container (100, 901, 902, 903, 904, 905, 906, 907, 908, 909, 910) for the production of radioisotopes by irradiation of a precursor material formed by a one-piece metal casing, the wall of said casing including one thin portion (130) having a thickness of between 5 and 100 m, the remainder having a thickness greater than 100 m. The invention also relates to a method for obtaining the container and to a target assembly using same.
Claims
1. A container for producing radioisotopes by irradiation of a precursor material, the container comprising: a metal jacket of integral construction, the metal jacket having a symmetry of revolution about an axis, and having from top to bottom (i) an upper portion being open and having a conical shape, the opening of the cone being oriented upwards, (ii) a first cylindrical portion connected to the upper portion, (iii) a thin wall cylindrical section connected to the first cylindrical portion, (iv) a second cylindrical portion connected to the thin wall cylindrical section, and (v) a dome connected to the second cylindrical portion, the thin wall cylindrical section having a first thickness between 5 m and 100 m, the first and second cylindrical section and the dome having a second thickness larger than 100 m.
2. The container as claimed in claim 1, wherein thin wall cylindrical section has an outside diameter between 4 mm and 100 mm.
3. The container as claimed in claim 1, wherein the container is at least partially made from at least one of nickel, titanium, niobium, tantalum, iron, chromium, cobalt or a stainless steel.
4. A method for obtaining a container as claimed in claim 1, the method comprising: providing a matrix; electrodepositing on the matrix a thickness of a metallic material, until a first thickness between 5 m and 100 m is obtained; masking a fraction of a surface of the matrix; electrodepositing on an unmasked section until a thickness larger than 100 m is obtained; removing the matrix; and obtaining the container as claimed in claim 1.
5. The method as claimed in claim 4, wherein the matrix is removed by dissolution.
6. A target assembly for producing radioisotopes, including: a container as claimed in claim 1; a holding tube including at one end a threaded portion; and a ring including a suitable interior thread, the holding tube and the ring being configured to encase the container.
7. The target assembly as claimed in claim 6, wherein the container has an end having a conical shape, a base of the cone being oriented toward an exterior of the container, the holding tube has a conical end congruent with the end of the container, and the ring has a conical end congruent with the end of the container.
8. The target assembly as claimed in claim 6, wherein the holding tube and the container are mounted so as to be able to rotate about an axis, and the target assembly includes a motor arranged to make the holding tube and the container rotate.
9. The target assembly as claimed claim 6, further including a cooling tube placed inside the container and arranged to allow a cooling liquid to flow.
10. The target assembly as claimed in claim 9, wherein the cooling tube includes a cooling head that has a recess on a portion of a periphery of the cooling head, the recess to give incident beam a longer path in a precursor liquid.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION OF THE INVENTION
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(11) The obtainment of a container 100 according to the invention, in particular when the thin fraction 130 is very thin, presents many difficulties. The applicant has developed a manufacturing method by virtue of which the shape shown, or other shapes, may be produced easily. This method is based on electroforming: A matrix having the shape of the interior of the container 100 is produced. This matrix may for example be made of aluminum; A metal layer is deposited by electrodeposition on all the exterior surface of the matrix, until the thickness desired for the thin portion has been obtained; A fraction of the height of the matrix is masked by applying an insulating layer, a lacquer or a plastic tape for example; the electrodeposition is continued until the thickness desired for the non-thinned portions has been obtained; the matrix is removed, for example in a caustic solution.
The thickness of the deposit is determined by the magnitude of the current and the duration of application thereof. The following metals may be used: nickel, titanium, niobium and tantalum, and alloys may also be obtained such as stainless steel, Havar (cobalt-based alloy), Invar or Kovar. In the case of a rotating target, the point of penetration of the beam into the container is a hotspot that is in continuous motion. This spot is a source of thermal expansion/contraction that may lead to fatigue of the metal. The choice of a material with a low thermal expansion coefficient, such as Invar and Kovar, may then be advantageous. It is also possible to deposit different alloys or metals in successive electrodeposition steps so as to obtain a first layer in one material, and one or more other layers in other materials. It is thus possible to choose the constituent material of the thin fraction for its resistance to the beam, or to make the layer making contact with the precursor material from a material having a chemical compatibility with the precursor material. Niobium may advantageously be used for the first layer forming the internal wall of the container i.e. the wall making contact with the precursor material. Specifically, it is known that the use of niobium does not lead to contamination of the produced radioisotope by undesired radioisotopes.
(12) The choice of the thickness of the thin portion 130 is an important element of the invention. In the table below, the residual energy that a beam of protons having an energy of 7, 10, 15, 20 and 30 MeV, respectively, has after passage through a nickel sheet of various thicknesses has been indicated. It may be seen that when the sheet has a thickness of 5 m, the energy loss of the protons is negligible i.e. less than 3% at 7 MeV and less than 0.2% at 30 MeV. In contrast, at 100 m and low energy, the loss in the sheet is substantial. It is then necessary to make recourse to a higher energy and therefore a more expensive accelerator. It is known that the production yield of .sup.18F from H.sub.2.sup.18O by (p,n) reaction is practically zero when the protons have an energy below 3 MeV. To obtain a yield higher than 60 mCi/A, it is necessary to use protons of 6 MeV at least. The thickness values indicated in bold in the table below are therefore maximum preferred thicknesses, depending on the energy of the available beam. If a yield even higher than 60 mCi/A is desired, it is necessary to further decrease the thickness of the thin fraction.
(13) TABLE-US-00001 NICKEL Sheet Incident E <MeV> thickness 7 10 15 20 30 <m> Transmitted E <MeV> 5 6.84 9.87 14.91 19.92 29.94 10 6.67 9.74 14.81 19.85 29.89 20 6.32 9.48 14.62 19.70 29.78 40 5.59 8.95 14.24 19.39 29.55 60 4.77 8.38 13.85 19.07 29.33 80 3.86 7.80 13.43 18.76 29.10 100 2.75 7.16 13.01 18.44 28.86 200 Stopped 3.00 10.79 16.75 27.72
The choice of a thinner wall, for example of thickness smaller than or equal to 100 m, allows the production of heat as the beam passes through to be limited. The above table may be used to guide the choice of the thickness when the chosen material is nickel. Other metals, such as niobium, titanium or Havar, have a slightly higher transparency and will give better results.
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(16) Independently of whether the target of the invention is used as an internal or external target, it is advantageous to be able to make it rotate. It is possible to either successively give thereto various orientations, for example to rotate it by 10 each time it is used, or preferably, to continuously rotate the container 100 during the irradiation. It is thus possible to ensure that all the periphery of the thin wall fraction is passed through by the beam, thereby ensuring a better distribution of the production of heat over a larger area. Furthermore, in the case of a liquid target, the rotation induces stirring of the precursor material, thereby improving the cooling by convection.
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(18) Certain radioisotope precursors, such as H.sub.2.sup.18O, are precious and expensive. Moreover, it is sometimes advantageous to be able to synthesize radiochemicals from a concentrated product. It is therefore advantageous to minimize the amount used. To this end, a preferred embodiment of the invention has been designed, in which embodiment (shown in
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(20) The container 901, which has symmetry of revolution, is cylindrical and has an upper end of conical shape, is one of the preferred embodiments of the invention. The container 902, which has a symmetry of revolution, has two open ends, both of which are of conical shape. The containers 903 and 904 are similar to the container 901, except that they have an open end with a flat edge and an open end with a cylindrical edge, respectively. The container 905 is similar to the container 901, except that it has a barrel shape.
(21) The container 906 is similar to the container 901, except that it has a one-sheet-hyperboloid shape.
(22) The container 907 is similar to the container 901, except that it has a thin wall in the closed end. It thus allows an axial penetration of the beam.
(23) The container 908, in contrast to the other containers shown, does not have symmetry of revolution, but a square or rectangular cross section, the thin wall possibly extending over a portion of two or three faces. This container is also shown in semi-isometric perspective. The container 910 is similar to the container 901, except that it has a larger diameter (for example 50 mm) and a flat bottom.
(24) The container 909 is similar to the container 910, except that the thin portion is arranged in a ring on the flat bottom and allows an axial penetration of the beam. This container may advantageously be used in an external target, in which the incident beam is parallel to the axis of rotation, as shown by the arrow X.
(25) In case of use as an external target, the targets 901 to 907 may be placed such that the beam penetrates into the target radially.
Advantages of the Invention
(26) The container 100 according to the invention has the advantage of being of integral construction, i.e. of not requiring assembling means or working, mounting or demounting means. The thin fraction 130 of the container 100 forms as it were a window integrated into the container 100. The target and the container 100 according to the invention may be easily demounted and remounted. The operator may act rapidly and may therefore limit his exposure to radiation. The container of the invention requires little material. It is therefore inexpensive and creates little waste when it must be scrapped. The target assembly according to the invention may if needs be serve as a beam stop, for example during the setup of an accelerator.
(27) The present invention has been described with reference to specific embodiments, which have been given purely by way a of illustration and which must not be considered to be limiting. Generally, it will appear obvious to those skilled in the art that the present invention is not limited to the examples illustrated and/or described above. The presence of reference numbers in the drawings must not be considered to be limiting, including when these numbers are indicated in the claims. The use of the verbs comprise, contain, include, or any other variant, and their conjugations, in no way excludes the presence of elements other than those mentioned. The use of the indefinite article a, an or the definite article the to introduce an element does not exclude the presence of a plurality of these elements. The use of the words top/bottom lower/upper is to be understood as being relative to the orientation of the components shown in the drawings. Although the examples described relate to the production of .sup.18F by irradiation by a beam of protons of a target material containing .sup.18O-enriched water, the invention may be applied to other liquid precursors, such as ordinary water H.sub.2.sup.16O, which produces .sup.13N during irradiation with protons, or gaseous precursors, such as .sup.14N.sub.2 to obtain .sup.11C. It is also possible to apply the invention to pulverulent precursor materials or to powders in suspension in a liquid and forming slurries. Lastly, the invention is also applicable to the case of a precursor material such as .sup.11B.sub.2O.sub.3, which produces .sup.11C by (p,n) reaction and forms .sup.11CO.sub.2 that may be collected. Other particles such as deuterons and alpha particles may be used. Likewise, the target according to the invention may be used with the chamber of the container at atmospheric pressure, or with the chamber placed under pressure.