1992
DOI: 10.1016/0168-9002(92)90190-f
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Preliminary measurements of SIS 18 beam parameters

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Cited by 15 publications
(12 citation statements)
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“…The experiment requires the use of a heavy-ion accelerator to provide the relativistic primary beam and a high-resolution magnetic spectrometer to avoid any ambiguity when identifying the projectile residues produced in the reaction. The SchwerIonen Synchrotron (SIS) [14] coupled with the Fragment Separator (FRS) [15] facility at GSI is best suited for this kind of experiment. 208 Pb beams are extracted from the ion source, preaccelerated, and then injected into the Universal Linear Accelerator (UNILAC), which accelerates primary beams up to 12 A MeV.…”
Section: Methodsmentioning
confidence: 99%
“…The experiment requires the use of a heavy-ion accelerator to provide the relativistic primary beam and a high-resolution magnetic spectrometer to avoid any ambiguity when identifying the projectile residues produced in the reaction. The SchwerIonen Synchrotron (SIS) [14] coupled with the Fragment Separator (FRS) [15] facility at GSI is best suited for this kind of experiment. 208 Pb beams are extracted from the ion source, preaccelerated, and then injected into the Universal Linear Accelerator (UNILAC), which accelerates primary beams up to 12 A MeV.…”
Section: Methodsmentioning
confidence: 99%
“…In the present experiment, a 238 U primary beam was accelerated in the heavy-ion synchrotron SIS [27,28] up to an energy of 1A GeV. The intensity, of the order of 10 7 ions/s, was continuously measured during the experiment with the secondary-electron monitor SEE-TRAM [29,30].…”
Section: A Experimental Setupmentioning
confidence: 99%
“…The [26] nuclei 54 Ni, 50 Fe, 46 Cr and 42 Ti were produced by the fragmentation of a 58 Ni beam at 680 MeV per nucleon on a 400 mg/cm 2 Be target in separate runs optimised to transport and implant the nucleus of interest. The SIS-18 synchrotron [1] delivered the 58 Ni primary beam with a spill structure of 10 s ON and 3 s OFF and an average intensity of 2×10 9 particles per spill. The ions were selected by the FRS [2] and then implanted in one DSSSD of an array of six, each with 16 X and 16 Y strips and thickness of 1 mm.…”
Section: Introduction Experiments and Resultsmentioning
confidence: 99%