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Three–dimensional simulations of a solid graphite target for high intensity fast extracted uranium beams for the Super–FRS

Published online by Cambridge University Press:  08 January 2009

N.A. Tahir ,
A. Matveichev ,
V. Kim ,
A. Ostrik ,
A. Shutov ,
V. Sultanov ,
I.V. Lomonosov ,
A.R. Piriz  and
D.H.H. Hoffmann
N.A. Tahir*
Affiliation:
Gesellschaft für Schwerionenforschung Darmstadt, Darmstadt, Germany
A. Matveichev
Affiliation:
Institute of Problems of Chemical Physics, Chernogolovka, Russia
V. Kim
Affiliation:
Institute of Problems of Chemical Physics, Chernogolovka, Russia
A. Ostrik
Affiliation:
Institute of Problems of Chemical Physics, Chernogolovka, Russia
A. Shutov
Affiliation:
Institute of Problems of Chemical Physics, Chernogolovka, Russia
V. Sultanov
Affiliation:
Institute of Problems of Chemical Physics, Chernogolovka, Russia
I.V. Lomonosov
Affiliation:
Institute of Problems of Chemical Physics, Chernogolovka, Russia
A.R. Piriz
Affiliation:
E.T.S.I. Industriales, Universidad de Castilla-La Mancha, Ciudad Real, Spain
D.H.H. Hoffmann
Affiliation:
Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany
*
Address correspondence and reprint requests to: N.A. Tahir: Gesellschaft für Schwerionenforschung Darmstadt Planckstrasse 1, 64291 Darmstadt, Germany. E-mail: n.tahir@gsi.de
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Abstract

This paper presents three–dimensional numerical simulations of thermodynamic and hydrodynamic response of a wheel shaped solid graphite production target for the super conducting fragment separator (Super–FRS) that is irradiated with a fast extracted high intensity uranium beam. These fragment separator experiments will be carried out at the future Facility for Antiprotons and Ion Research (FAIR), at Darmstadt. Previously, we reported simulation results that were carried out using two–dimensional computer codes which showed that one can use a solid graphite target for the Super-FRS for the highest intensity (5 × 1011 ions per spill) of the fast extracted uranium beam. Present results, however, have shown that due to three–dimensional effects the maximum intensity that can be used with such a target is 3 × 1011 ions per spill. A detailed comparison between two–dimensional and three–dimensional results is presented in this paper.

Keywords

Elastic plastic behaviorFAIRFragment separatorHigh energy density physicsIntense heavy ion beamsRadioactive beams

Information

Type
Research Article
Information
Laser and Particle Beams , Volume 27 , Issue 1 , March 2009 , pp. 9 - 17
Copyright
Copyright © Cambridge University Press 2009

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References

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