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Electromagnetic fission of238U at 600 and 1000 MeV per nucleon
Authors:Th Rubehn  W F J Müller  R Bassini  M Begemann-Blaich  Th Blaich  A Ferrero  C Groß  G Imme  I Iori  G J Kunde  W D Kunze  V Lindenstruth  U Lynen  T Möhlenkamp  L G Moretto  B Ocker  J Pochodzalla  G Raciti  S Reito  H Sann  A Schüttauf  W Seidel  V Serfling  W Trautmann  A Trzcinski  G Verde  A Wörner  E Zude  B Zwieglinski
Institution:1. Gesellschaft für Schwerionenforschung, D-64220, Darmstadt, Germany
2. Dipartimento di Fisica, Università di Milano I.N.F.N., I-20133, Milano, Italy
3. Institut für Kernchemie, Universit?t Mainz, D-55099, Mainz, Germany
4. Dipartimento di Fisica dell' Università and I.N.F.N., I-95129, Catania, Italy
7. Forschungszentrum Rossendorf, D-01314, Dresden, Germany
8. Lawrence Berkeley Laboratory, 94720, Berkeley, CA, USA
9. Institut für Kernphysik, Universit?t Frankfurt, D-60486, Frankfurt, Germany
10. Soltan Institute for Nuclear Studies, 00-681, Warsaw, Hoza 69, Poland
Abstract:Electromagnetic fission of238U projectiles at E/A =600 and 1000 MeV was studied with the ALADIN spectrometer at the heavy-ion synchrotron SIS. Seven different targets (Be, C, Al, Cu, In, Au and U) were used. By considering only those fission events where the two charges added up to 92, most of the nuclear interactions were excluded. The nuclear contributions to the measured fission cross sections were determined by extrapolating from beryllium to the heavier targets with the concept of factorization. The obtained cross sections for electromagnetic fission are well reproduced by extended Weizsäcker-Williams calculations which include E1 and E2 excitations. The asymmetry of the fission fragments' charge distribution gives evidence for the excitation of the double giant-dipole resonance in uranium.Communicated by V. Metag
Keywords:PACS" target="_blank">PACS  25  75  +r  25  85  -w  27  90  +b
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