001     357443
005     20250208100459.0
024 7 _ |a 10.18429/JACOW-IPAC2024-TUPS13
|2 doi
024 7 _ |a 10.15120/GSI-2025-00400
|2 datacite_doi
037 _ _ |a GSI-2025-00400
041 _ _ |a English
100 1 _ |a Bozyk, Lars
|0 P:(DE-Ds200)OR2146
|b 0
|e Corresponding author
111 2 _ |a 15th International Particle Accelerator Conference
|g IPAC2024
|c Nashville
|d 2024-05-19 - 2024-05-24
|w USA
245 _ _ |a SIS18 Operation with $U^{28+}$
260 _ _ |c 2024
|b JACoW Publishing
300 _ _ |a 1661-1664 pages1.5 MB
336 7 _ |a CONFERENCE_PAPER
|2 ORCID
336 7 _ |a Conference Paper
|0 33
|2 EndNote
336 7 _ |a INPROCEEDINGS
|2 BibTeX
336 7 _ |a conferenceObject
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336 7 _ |a Output Types/Conference Paper
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336 7 _ |a Contribution to a conference proceedings
|b contrib
|m contrib
|0 PUB:(DE-HGF)8
|s 1738928850_2659993
|2 PUB:(DE-HGF)
500 _ _ |a Published by JACoW Publishing under the terms of the Creative Commons Attribution 4.0 license.
520 _ _ |a In SIS18 U²⁸⁺ is used to reach highest heavy ion beam intensities for FAIR-operation. The medium charge state avoids losses during stripping processes and shifts the space charge limit to higher number of particles. Nevertheless, these ions are subjected to ionization loss in collisions with residual gas particles. Via ion impact induced gas desorption a feedback between vacuum quality and beam emerges, yielding in a beam intensity limitation. The installation of a charge exchange collimator is one of the several upgrade measures which have been performed to shift this limit. They are equipped with a current measurement system to detect charge exchanged ions, which is routinely used during machine experiments. In this proceeding we present different beam based measurements showing dynamic vacuum effects. The non-linear dependence of the extraction intensity on the number of injected particles, ramp rate, and brake-time for vacuum relaxation will be shown. Stored heavy ion beams were used for charge exchange current measurements. They allow conclusions on the vacuum conditions and are presented as well.
536 _ _ |a 6G14 - GSI-MU Ion Facilities (POF4-6G14)
|0 G:(DE-HGF)POF4-6G14
|c POF4-6G14
|f POF IV
|x 0
588 _ _ |a Dataset connected to DataCite
650 _ 7 |a Accelerator Physics
|2 Other
650 _ 7 |a mc4-hadron-accelerators - MC4: Hadron Accelerators
|2 Other
650 _ 7 |a MC4.A04 - MC4.A04 Circular Accelerators
|2 Other
693 _ _ |a Facility_outside_beam_time_program
|e Experiment at GSI without experiment proposal number ( - ; Facility_outside_beam_time_program )
|1 EXP:(DE-Ds200)Facility_outside_beam_time_program-20200803
|0 EXP:(DE-Ds200)Experiment_without_proposal_number-20200803
|5 EXP:(DE-Ds200)Experiment_without_proposal_number-20200803
|x 0
700 1 _ |a Spiller, Peter
|0 P:(DE-Ds200)OR1222
|b 1
700 1 _ |a Pilat, Fulvia
|b 2
|e Editor
700 1 _ |a Fischer, Wolfram
|b 3
|e Editor
700 1 _ |a Saethre, Robert
|b 4
|e Editor
700 1 _ |a Anisimov, Petr
|b 5
|e Editor
700 1 _ |a Andrian, Ivan
|b 6
|e Editor
773 _ _ |a 10.18429/JACOW-IPAC2024-TUPS13
856 4 _ |y OpenAccess
|u https://repository.gsi.de/record/357443/files/TUPS13.pdf
856 4 _ |y OpenAccess
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|u https://repository.gsi.de/record/357443/files/TUPS13.pdf?subformat=pdfa
909 C O |o oai:repository.gsi.de:357443
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910 1 _ |a GSI Helmholtzzentrum für Schwerionenforschung GmbH
|0 I:(DE-Ds200)20121206GSI
|k GSI
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|6 P:(DE-Ds200)OR2146
910 1 _ |a GSI Helmholtzzentrum für Schwerionenforschung GmbH
|0 I:(DE-Ds200)20121206GSI
|k GSI
|b 1
|6 P:(DE-Ds200)OR1222
913 1 _ |a DE-HGF
|b Forschungsbereich Materie
|l Großgeräte: Materie
|1 G:(DE-HGF)POF4-6G0
|0 G:(DE-HGF)POF4-6G14
|3 G:(DE-HGF)POF4
|2 G:(DE-HGF)POF4-600
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|v GSI-MU Ion Facilities
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914 1 _ |y 2024
915 _ _ |a OpenAccess
|0 StatID:(DE-HGF)0510
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915 _ _ |a Creative Commons Attribution CC BY 4.0
|0 LIC:(DE-HGF)CCBY4
|2 HGFVOC
920 1 _ |0 I:(DE-Ds200)SYS-20121002OR231
|k SYS
|l System Design SIS 100 / SIS 18
|x 0
980 _ _ |a contrib
980 _ _ |a VDB
980 _ _ |a UNRESTRICTED
980 _ _ |a I:(DE-Ds200)SYS-20121002OR231
980 1 _ |a FullTexts


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