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Study of radiative-capture reactions at LUNA and in DresdenNuclear reactions power our sun, and they create the chemical elements that are necessary for human life. In order to correctly understand the nuclear processes in stars, both astronomical observations and nuclear data are necessary. Recent investments in satellite-based astronomy and in neutrino observatories have enabled a breakthrough in the precision of the observations. This calls for new nuclear data of similar precision. Radiative-capture reactions of importance for astrophysics are studied in precision experiments: in Dresden using ion beams at the surface of the Earth, in the Felsenkeller shallow underground counting facility, and at LUNA deep underground in the Gran Sasso laboratory in Italy. We are currently discussing whether to upgrade the Felsenkeller laboratory by installing an accelerator of 2-3 MV accelerating potential. News21 June 2010: Experiment on 40Ca(α,γ)44Ti started: Physics, experiment, ELOG. 28-30 April 2010: Workshop in Dresden on underground accelerators. More details here. See also article in Physik-Journal, June 2010. 7 December 2009: Michael Anders joined the group as new PhD student on LUNA. August 2009: Our research is included in FZD-Journal (only German). 6 April 2009: The Gran Sasso laboratory was not harmed by the earthquake in L'Aquila on 6 April 2009. We call for solidarity towards the earthquake victims, e.g. here. The 2H(α,γ)6Li reaction: Nucleosynthesis in the Big BangPhD project M. Anders (2009-2012) Motivation: This reaction controls the production of 6Li in big-bang nucleosynthesis. In very old stars, lithium-6 is found in quantities greatly exceeding the value predicted by standard big-bang nucleosynthesis calculations. Experiment: The first experiment studying this reaction directly at big-bang energies is in preparation at LUNA. Further details can be found here. The 14N(p,γ)15O reaction: The Bethe-Weizsäcker cycle of hydrogen burningPhD project M. Marta (2007-2010), Masters project E. Trompler (2008-2009, thesis) Motivation: This reaction controls the rate of the carbon-nitrogen-oxygen (CNO) cycle, first proposed in 1938 by Bethe and Weizsäcker. The CNO rate affects low-energy solar neutrinos (under study at the SNO+ detector in Canada and at the Borexino detector in Italy), carbon stars and last not least the age of our universe. It has attracted recent interest because of its contribution to directly measure the content of carbon and nitrogen in the solar core. Experiment at the FZD ion beam facility: An experiment at E = 0.6 - 2 MeV, complementary to the previous lower-energy study at LUNA, has been performed in Dresden (2008 and 2009). Improved data on resonance strengths in the 14N(p,γ)15O and 15N(p,αγ)12C are now available. The off-resonance data are still under analysis.
Experiment at LUNA: The LUNA study of this reaction showed that the CNO rate was only half the previously accepted value:
Experiment at Agata demonstrator Legnaro/Italy: The lifetime of the exited state at 6.79 MeV in 15O is to be studied by the Doppler shift attenuation method. The 40Ca(α,γ)44Ti reaction: Nucleosynthesis in supernovaeMasters project K. Schmidt (2010-2011) Motivation: The radioactive nucleus 44Ti (halflife 59 years) is created in supernovae. Gamma-rays from the decay of 44Ti have been observed in satellite-based observatories. Together with precise nuclear data, the observations can be used to calibrate supernova models. Experiment at FZD ion-beam facility and Felsenkeller: A study of resonance strengths in the 44Ti-producing reaction 40Ca(α,γ)44Ti is running on for 21.-30. June 2010. More info on the science here; more info on technical details here (local access). The 15N(p,γ)16O reaction - CNO cycles II and IIIMotivation: This reaction lies at the branching point between CNO cycles I and II, controlling the amount of nucleosynthetic material passed to the higher CNO and subsequent NeNa and MgAl cycles. Experiment at LUNA: The cross section has been measured with nitrogen targets of natural isotopic composition (0.37% 15N), see below paper. Further experiments with enriched 15N targets, using first a HPGe and then a 4π BGO summing detector, are presently under analysis.
The 3He(α,γ)7Be reaction - thermometer of the center of the SunMotivation: The flux of solar 8B neutrinos has been measured with 3.5% precision (2006) by the SuperKamiokande neutrino detector in Japan. The uncertainty in the predicted 8B neutrino flux is dominated by the 3He(α,γ)7Be reaction. Experiment at LUNA: The 3He(α,γ)7Be reaction has been studied experimentally with a systematic uncertainty as low as 3.0%, decisively improving the precision of the prediction:
γ-ray background measurements at LUNALUNA = Laboratory Underground for Nuclear Astrophysics
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