Patent Number: 
Section: claims

1. A target for implementing a process for producing actinium-225 and radium isotopes, the target comprising a thorium metal sample enclosed in a hermetic shell, the sample being in the form of at least one bulk thorium metal monoliths that is 2 to 30 mm thick, the hermetic shell having walls with a wall thickness on a beam inlet and outlet side in a range of 50 to 300 μm, the walls of the shell being diffusion-welded to the sample so as to provide a contact between the sample and the shell that enables improved cooling of the target with a flow of water around the walls than if the walls were not diffusion-welded to the sample, the target further comprising an electron-beam, laser, or argon-arc weld seam sealing the walls to the sample at a periphery of the target, the hermetic shell being arranged and constructed with a material that does not react either (a) with thorium under thermal and radiation loads resulting from an irradiation of the sample with protons at an energy above 40 MeV while the target is being cooled with the water flow or (b) with radiolytic water from the water flow when the target is cooled with the water flow during the irradiation, said material being selected from the group consisting of metallic niobium, nickelated molybdenum, and high-alloy austenitic steel. 2. The target according to claim 1, wherein the hermetic shell is made of hot-rolled molybdenum comprising, on top of the hermetic shell made of hot-rolled molybdenum, a protective layer of metallic nickel having a thickness within a range from 40 to 90 μm. 3. The target process according to claim 1, wherein the material is metallic niobium. 4. The target process according to claim 1, wherein the material is high-alloy austenitic steel. 5. The target process according to claim 1, wherein the material is hot-rolled molybdenum. 6. A system comprising(i) the target according to claim 1;(ii) a proton beam source for generating proton beams at an energy above 40 MeV, said proton beam source being positioned for irradiating the target; and(iii) a water flow source that provides a flow of water for cooling the target while it is being irradiated by protons from the proton beam source,wherein the target is constructed and arranged such that, when the thorium monolith is irradiated with proton beams from the proton beam source at an energy above 40 MeV and the irradiated thorium is withdrawn from the shell, a yield of at least 93% of actinium can be recovered from the thorium by a chemical process comprising dissolving the thorium in nitric acid under heating, extracting with tributyl phosphate and separating by chromatography.