Title: The perspectives of nuclear astrophysics at fragmentation facilities
1The perspectives of nuclear astrophysics at
fragmentation facilities
Klaus Sümmerer, GSI Darmstadt
- Nuclear physics input to astrophysics e.g.
- Nuclear structure Masses, decay half lives,
level properties, GT strengths, shell closures
etc. - Reaction rates for capture reactions
- Isospin and density dependence of the nuclear
equation of state
- Contributions from fragmentation-type facilities
- Spectroscopy of stopped fragments
- Unique storage-ring experiments
- Break-up reactions of unstable nuclei
2Nuclear-structure information from fragmentation
facilities
- Experiments with stopped fragments
- Combines production/separation at high energy
with experiments at low energy - High energy ? thick degrader ? high isotopic
purity - Complementary to ISOL
- Access to refractory elements not available from
ISOL - Access to very short half lives
- Future (GSI/RIA) Access to N126 r-process
waiting-point nuclei and fissile nuclei below 238U
3Super-FRS low-energy branch
4Predicted production rates at Super-FRS
5Storage-ring experiments
- Mass/half life measurements at storage rings
- Mass measurements over large areas of the
nuclear chart - Resolution of isomers
- Access to very short half lives (TOF method)
- Half life measurements for ionized species (e.g.
BBD)
- Scattering and transfer reactions at internal
target - (p,n) to measure GT strengths
- (?, ?) to measure giant monopole resonance
(?EOS of asymmetric nuclear matter)
6Super-FRS Ring branch
- Mass and half life measurements
- Scattering and transfer ?Electron scattering
Short half lives, stochastic cooling
Long half lives, electron cooling, nuclear
reactions
H.Weick, H.Simon et al.
7Excitation of Giant Monopole Resonances to
determine the nuclear compressibility of
asymmetric nuclear matter
- GMR excitations in (?, ?) reactions
- measure near ?cm0 degree
- E? ? 1 MeV
- possible only in storage ring!
- wide range of A/Z
- E.g. 104-132Sn
E/A400 MeV, 1014 He atoms/cm2
8Reaction-rate measurements at fragmentation
facilities
Measure rad.capture reaction (p/n, ?) via
Coul.diss. (?,p/n)
- Advantages of inverse measurements
- Access to short-lived species
- Thick targets ? access to rare species
- Coincident detection of fast particles ? low
background
- Disadvantages of inverse measurements
- Connects only ground states
- Different sensitivity to multipolarities
- Small Q-values
- Recent examples
- 7Be(p,?)8B (GSI)
- 8B(p,?)9C (RIKEN)
- 14C(n,?)15C (GSI)