Comparison of radioactive ion-beam intensities produced by means of thick targets bombarded with neutrons, protons and heavy ions
References (52)
Nucl. Instr. and Meth. B
(1992)- et al.
Nucl. Instr. and Meth. B
(1992) - et al.
Nucl. Instr. and Meth.
(1971) Nucl. Instr. and Meth. B
(1992)- et al.
Nucl. Instr. and Meth. B
(1987) - et al.
Nucl. Instr. and Meth.
(1981) - et al.
Nucl. Instr. and Meth. B
(1992) Nucl. Instr. and Meth. B
(1992)Phys. Rep.
(1979)Nucl. Instr. and Meth. A
(1990)
Nucl. Instr. and Meth.
Nucl. Instr. and Meth. B
Nucl. Instr. and Meth.
Nucl. Instr. and Meth. B
Nucl. Instr. and Meth. B
Nucl. Instr. and Meth. B
Nucl. Instr. and Meth.
Nucl. Instr. and Meth. B
Nucl. Instr. and Meth. B
Nucl. Instr. and Meth. B
Nucl. Phys. A
Nucl. Instr. and Meth. B
Cited by (47)
High intensity targets for ISOL, historical and practical perspectives
2008, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :In the 1980s, some astrophysical reaction studies were already being performed with radioactive beams produced by projectile fragmentation [4–7], however, the existing facilities could not meet the intensity requirements of many potential experiments. The requirement for higher intensity radioactive beams soon resulted in a proliferation of workshops [8–11], design studies [12,13] and facility proposals [14,15] based on using intense primary beams irradiating thick ISOL targets to produce intense RIB that could subsequently be accelerated using a second dedicated accelerator. The first 2-accelerator facility to produce RIB with high intensities for astrophysics studies was the Louvain-la-Neuve laboratory which, in 1990, used a 100 μA, 30 MeV proton beam from a cyclotron to produce 13N through the 13C(p,n)13N reaction on an enriched target [16].
RIB production by photofission in the framework of the ALTO project: First experimental measurements and Monte-Carlo simulations
2008, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsHigh-accuracy mass spectrometry with stored ions
2006, Physics ReportsReview of ISOL target-ion-source systems
2003, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Reason for the suppression of SbS+ must thus be instability of the molecular ions. This explanation is analogous to the one [3] for the surprising mobility of halogenes, which is most likely due to molecules formed with the omni-present alkali impurities. Also here the respective alkali-halogenide ions are not observed, although the neutral molecules are known to have a sufficient thermal stability [50].
An ISOL test-bench at China Institute of Atomic Energy
2003, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsYield calculations for a facility for short-lived nuclear beams
2002, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment