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| 001 | 200609 | ||
| 005 | 20230317222215.0 | ||
| 024 | 7 | _ | |a 10.15120/GSI-2016-03764 |2 datacite_doi |
| 037 | _ | _ | |a GSI-2016-03764 |
| 041 | _ | _ | |a English |
| 088 | 1 | _ | |a Report |
| 088 | _ | _ | |a Report |2 Other |
| 100 | 1 | _ | |a Appel, S. |0 P:(DE-Ds200)OR0031 |b 0 |e Corresponding author |u gsi |
| 245 | _ | _ | |a Measurement of UNILAC and SIS18 proton performance |
| 260 | _ | _ | |c 2016 |
| 300 | _ | _ | |a 3 Seiten |
| 336 | 7 | _ | |a report |2 DRIVER |
| 336 | 7 | _ | |a REPORT |2 ORCID |
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| 336 | 7 | _ | |a Output Types/Report |2 DataCite |
| 336 | 7 | _ | |a Report |b report |m report |0 PUB:(DE-HGF)29 |s 1484134549_22242 |2 PUB:(DE-HGF) |
| 336 | 7 | _ | |a TECHREPORT |2 BibTeX |
| 520 | _ | _ | |a On July 16th 2016 the UNILAC and SIS18 proton performance has been measured. Due to scheduled maintenance works of the UNILAC's rf-system, the post-stripper energy was restricted to 5.9~MeV and accordingly the beam quality suffered considerably from the interruption of the periodic focusing system. This limitation will not be any longer in future beam times. Six single-gap resonators were used for acceleration to 10.7~MeV. After an optimization of the multi-turn injection $\pmb{1.2\cdot10^{11}}$ protons were extracted form the SIS18. |
| 536 | _ | _ | |a 631 - Accelerator R & D (POF3-631) |0 G:(DE-HGF)POF3-631 |c POF3-631 |f POF III |x 0 |
| 536 | _ | _ | |a GSI Machine UNILAC (GSILSFUNILAC) |0 G:(DE-Ds200)GSILSFUNILAC |c GSILSFUNILAC |x 1 |
| 536 | _ | _ | |a GSI Machine SIS18 (GSILSFSIS18) |0 G:(DE-Ds200)GSILSFSIS18 |c GSILSFSIS18 |x 2 |
| 700 | 1 | _ | |a Groening, L. |0 P:(DE-Ds200)OR0383 |b 1 |u gsi |
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| 700 | 1 | _ | |a Mickat, S. |0 P:(DE-Ds200)OR2389 |b 6 |u gsi |
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