Peter Egelhof GSI Darmstadt, Germany 8th. International ... - Bulgaria

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II. Experimental TechniquesThe Present <strong>GSI</strong> Accelerator Facilities:UNILAC: universal linear acceleratorall ions ( 1 H ... 238 U)E = 3 - 20 MeV/uSIS:ESR:FRS:heavy ion synchrotronE = 100 - 2000 MeV/u0 50mexperimental storage ringbeam cooling⇒ excellent beam qualitiesUNILACfragment separatorprojectile fragmentation, fission⇒ secondary radioactive beamswith energies E ≥ 100 – 1000 MeV/utransfer channelexperimental hall(3 – 20 MeV/u)experimental hall(up to 2000 MeV/u)SISFRSESR
The Present Radioactive Beam Facility at <strong>GSI</strong>FRS: In-Flight Separator & High-Resolution SpectrometerSecondary Beam Branches3SIS121. Decay Spectroscopy, Reactions,High-Resolution Particle-γ Measurements2. Masses, Lifetimes, Isomeric Beams,Direct Reactions3. Reactions Studies (Complete Kinematics)Active Target IKAR
Page 1 and 2: Nuclear Structure Studies on Exotic
Page 3 and 4: I. Introductionmethods of nuclear s
Page 5 and 6: Introduction: Phenomena and Burning
Page 9 and 10: Halo-Nuclei - a New Phenomenonof th
Page 11 and 12: The Radial Shape of Nuclei: from St
Page 15 and 16: The Collective Response of the Nucl
Page 17 and 18: The Collective Response of the Nucl
Page 19 and 20: The Radial Shape of Nuclei: from St
Page 21 and 22: New Magic Number N = 16N=20 shell g
Page 27: Light-Ion Induced Direct Reactions
Page 31 and 32: Production of Radioactive Beams at
Page 33 and 34: Why Fast Radioactive Beams?Producti
Page 35 and 36: II. Experimental TechniquesExperime
Page 37 and 38: Application of Active TargetsConcep
Page 39 and 40: The Experimental Storage Ring ESR a

Peter Egelhof GSI Darmstadt, Germany 8th. International ... - Bulgaria

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