Solution target for cyclotron production of radiometals
US-2017221594-A1 · Aug 3, 2017 · US
US10242760B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10242760-B2 |
| Application number | US-201514949583-A |
| Country | US |
| Kind code | B2 |
| Filing date | Nov 23, 2015 |
| Priority date | Dec 7, 2009 |
| Publication date | Mar 26, 2019 |
| Grant date | Mar 26, 2019 |
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Accelerator based systems are disclosed for the generation of isotopes, such as molybdenum-98 (“99Mo”) and metastable technetium-99 (“99mTc”) from molybdenum-98 (“98Mo”). Multilayer targets are disclosed for use in the system and other systems to generate 99mTc and 98Mo, and other isotopes. In one example a multilayer target comprises a first, inner target of 98Mo surrounded, at least in part, by a separate, second outer layer of 98Mo. In another example, a first target layer of molybdenum-100 is surrounded, at least in part, by a second target layer of 98Mo. In another example, a first inner target comprises a Bremsstrahlung target material surrounded, at least in part, by a second target layer of molybdenum-100, surrounded, at least in part, by a third target layer of 98Mo.
Opening claim text (preview).
I claim: 1. A system for generating isotopes, comprising: an accelerator; a source of charged particles coupled to the accelerator to inject charged particles into the accelerator; a target positioned in the path of the accelerated charged particles, the target comprising: a first, inner target material comprising a first isotope of molybdenum; and a second, outer target material comprising a second isotope of molybdenum, the second outer target material at least partially surrounding the first, inner target material, the second, outer target material defining a passage for accelerated charged particles to the first, inner target material. 2. The system of claim 1 , wherein the first isotope and the second isotope are different isotopes of molybdenum. 3. The system of claim 2 , wherein the first, inner target material and the second, outer target material are separated by a gap. 4. The system of claim 1 , wherein the first isotope and the second isotope each comprise molybdenum-98. 5. The system of claim 2 , wherein the first isotope comprises molybdenum-100 and the second isotope comprises molybdenum-98. 6. The system of claim 1 , wherein the target further comprises a layer of hydrogenous material between the first, inner target material and the second, outer target material. 7. The system of claim 1 , wherein: the first inner target material comprises a Bremsstrahlung material; the second target material comprises molybdenum 100; and the target further comprises third target material comprising molybdenum-98 at least partially surrounding the second target material. 8. The system of claim 1 , further comprising: a target assembly containing the target; a target chamber containing the target assembly; and a drift tube coupling an output of the accelerator to the target chamber, defining the path from the accelerator to the target. 9. The system of claim 8 , further comprising: electromagnetic coils adjacent to the drift tube, to selectively deflect the accelerated charged particle beam onto at least two locations on the target. 10. The system of claim 1 , wherein the accelerator is chosen from the group consisting of a cyclotron, a radio frequency quadrupole accelerator, and a linear accelerator. 11. The system of claim 1 , further comprising: means for rotating the target. 12. The system of claim 1 , wherein the source of charged particles comprises a source of deuterons. 13. The system of claim 12 , wherein: the accelerated charged particles comprise accelerated deuterons; the first, inner target material comprises molybdenum-98, wherein bombardment of the first, inner target material by the accelerated deuterons during operation generates molybdenum-99 and metastable technetium-99, and releases neutrons; and the second, outer target material comprises molybdenum-98, wherein impact of the second, outer target material by the released neutrons generates molybdenum-99 and metastable technetium-99. 14. The system of claim 13 , wherein the target further comprises: a layer of hydrogenous material between the first, inner target material and the second, outer target material. 15. The system of claim 14 , wherein the target defines a gap region between the first, inner target material and the layer of hydrogenous material. 16. The system of claim 1 , wherein the source of charged particles comprises a source of electrons. 17. The system of claim 1 , further comprising: an electromagnetic coil adjacent to the path of the accelerated charged particles; the electromagnetic coil being configured to selectively, sequentially deflect the accelerated charged particles to impact the first, inner target material at respective different locations. 18. The system of claim 1 , wherein the first, inner target material is at an oblique angle with respect to a direction of the accelerated charged particles.
by bombardment with electrically charged particles (irradiation devices G21K5/00) · CPC title
by electromagnetic irradiation, e.g. with gamma or X-rays (applications of radiation G21H5/00; irradiation devices G21K5/00) · CPC title
Recovery of specific isotopes from irradiated targets · CPC title
by neutron irradiation · CPC title
Molybdenum · CPC title
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