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Fragmentation in Proton-Nucleus Reactions from 100 to 1400 MeV

Jäderström, Henrik, 1979- (författare)
Uppsala universitet,Kärn- och partikelfysik
Wesretberg, Lars (preses)
Murin, Yuri (preses)
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Aleklett, Kjell, professor (preses)
Uppsala universitet,Kärn- och partikelfysik
Simon, Haik, Dr. (opponent)
GSI, Gesellschaft für Schwerionenforschung mbH, Darmstadt
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 (creator_code:org_t)
ISBN 9789155471156
Uppsala : Acta Universitatis Upsaliensis, 2008
Engelska 73 s.
Serie: Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology, 1651-6214 ; 402
  • Doktorsavhandling (övrigt vetenskapligt/konstnärligt)
Abstract Ämnesord
Stäng  
  • The heaviest fragments, recoils, have been studied in proton and deuteron induced 28Si reactions and proton-20Ne reactions at 100-300 MeV per nucleon. Inclusive charge and angular distributions and coincidences between He nuclei and recoils have been compared to two theoretical models, Dubna Cascade Model and JAERI Quantum Molecular Dynamics. The overall agreement was good for the reactions with 28Si, however the angular distributions of He fragments could not be reproduced. For the 20Ne reactions the recoil angular distributions were only reproduced for large angles. There was a significant underestimation at small angles and low recoil charge. α-clustering in the bombarding nucleus is a possible explanation for the deviations. In the 100 MeV per nucleon reactions all assumptions of the models may not be valid and the agreement was worst for these reactions. In proton-natXe reactions intermediate mass fragments have been studied from 200 to 1400 MeV. Slow ramping was used to scan the energy. Charge distributions and a caloric curve have been compared to Cascade Fragmentation Evaporation Model. Charge distributions showed good agreement for fragments with Z<8 but the heavier fragments were underestimated.

Nyckelord

Nuclear physics
proton
deuteron
20Ne
28Si
Xe
nuclear reactions
inverse kinematics
recoils
intermediate mass fragments
angular distribution
DCM model
JQMD model
CFEM model
single event upset
Kärnfysik

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