COMPARISON OF RADIOACTIVE ION-BEAM INTENSITIES PRODUCED BY MEANS OF THICK TARGETS BOMBARDED WITH NEUTRONS, PROTONS AND HEAVY-IONS

Citation
Hl. Ravn et al., COMPARISON OF RADIOACTIVE ION-BEAM INTENSITIES PRODUCED BY MEANS OF THICK TARGETS BOMBARDED WITH NEUTRONS, PROTONS AND HEAVY-IONS, Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms, 88(4), 1994, pp. 441-461
Citations number
52
Categorie Soggetti
Physics, Nuclear","Nuclear Sciences & Tecnology","Instument & Instrumentation
ISSN journal
0168583X
Volume
88
Issue
4
Year of publication
1994
Pages
441 - 461
Database
ISI
SICI code
0168-583X(1994)88:4<441:CORIIP>2.0.ZU;2-E
Abstract
Target and ion-source techniques which allow rapid separation of therm alized radioactive nuclei from 1-500 g/cm2 thick irradiated target mat erial and continuously convert them into a mono-isotopic ion beam have been proven to be a powerful method of radiochemical separation. Thes e techniques combine nuclear reactions with high-temperature chemistry , metallurgy, solid-state diffusion, and ionization phenomena. Develop ed at the many mass separators on-line to various accelerators or reac tors they are today widely used to produce low-energy (10-60 keV) radi oactive ion-beams for physics experiments. Since some years they have reached a stage of development that allows the production of high-inte nsity beams of up to 10(12) ions/s of radioactive isotopes of most ele ments in the periodic system. Such on-line mass separators seem to be excellent injectors to a second accelerator which accelerates up to 20 MeV/u. This paper discusses the radioactive beam intensities that may be injected into proposed or working European radioactive ion-beam fa cilities which make use of such injectors. First a short introduction is given to the technique of on-line mass separation. This is followed by a detailed discussion of the three factors that determine the prod uction rates in the target, i.e. reaction cross-sections, primary beam properties, and target thicknesses, and by a discussion of the more d ecisive factors that control the efficiency with which the radioactive nuclei produced in the target can be transformed into an injection io n-beam of typically 10-60 keV energy. Throughout the discussion the in fluence of new developments is assessed. Finally, selected examples of realistic beam intensities are given, which are used for intercompari son of the different production methods used by the various European p rojects.