Bochum 1998 – wissenschaftliches Programm
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HK: Hadronen und Kerne
HK 39: Nuclear Astrophysics III
HK 39.3: Gruppenbericht
Dienstag, 17. März 1998, 17:30–18:00, E
Investigation of the reactions 19F(p,αγ)16O and 19F(p,γ)20Ne relevant for the recycling/breakout of the CNO cycles 1.0mm♣ — •J.W. Hammer1, R. Ott1, G. Bulski2, M. Jaeger1, A. Mayer1, R. Kunz1, R. Morlock1, G. Staudt3, K. Spyrou4, Ch. Chronidou4, S. Harissopulos4, T. Paradellis4, H. Schulte5, and C. Rolfs5 — 1Inst. f"ur Strahlenphysik, Univ. Stuttgart, D–70550 Stuttgart — 2Fa. DANET GmbH., Waldburgstraße 17–19, D–70563 Stuttgart — 3Physikal. Inst., Univ. Tübingen, D–72076 Tübingen — 4Inst. of Nuclear Physics, N.C.S.R. “Demokritos”, Gr–15310 Athens — 5Inst. für Experimentalphysik 3, Univ. Bochum, D–44780 Bochum
Hydrogen burning stars of the second or third generation with masses
larger than the sun, produce energy faster by the standard CNO cycle which
has four reaction loops. At the outer loop 19F can react into two
directions, one branch is recycling via 19F(p,αγ)16O
and the other is a breakout via 19F(p,γ)20Ne into the
NeNa-cycle with no return. The reaction rates at burning temperatures are
uncertain because of the lack of reliable data of both branches at low
energies.
Now new data are available measured in some experimental approaches with
quite different concepts. In a first set of experiments angular
distributions and excitation functions of all subbranches pα0,
pα1, pα2, pα3, pα4; pαγ2,
pαγ3, pαγ4; pγ0 and pγ1 have been
measured in inverse kinematics using a 19Fx+ beam (x=1-4). There
was no possibility to construct a pure fluorine target. In a second set,
using solid state targets, several particle detectors and two high
resolution γ-detectors at 0∘ and 90∘, excitation
functions of the subbranches pα0, pαγ2,
pαγ3, pαγ4, pγ0 and pγ1 were
observed. The aim of these two sets of experiments was to get as far as
possible the complete differential information for the reaction in order
to describe the reaction mechanism by the R-matrix formalism.
The concept of the third set of experiments was to avoid the problems of a
differential measurement by measuring the total γ-transition-rate in
4π without discrimination of subchannels. The γ-detection was
performed by using large 4π-NaJ-detectors which were summing up the
cascade transitions with high efficiency.
The experiments on both reactions have been performed at the
Dynamitron accelerators of Bochum and Stuttgart and at the tandem
of Demokritos, Athens.
The data have been analyzed and a good agreement is observed between the
different results. The actual situation concerning cross sections,
resonances, S-factors and reaction rates will be presented.
1.0mm♣ Work supported
by Deutsche Forschungsgemeinschaft (DFG) HA 962, Bonn