High-resolution experiments on nuclear reactions and their implications for astrophysics and nuclear technology Karl-Heinz Schmidt for CHARMS.

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Presentation transcript:

High-resolution experiments on nuclear reactions and their implications for astrophysics and nuclear technology Karl-Heinz Schmidt for CHARMS

SIS + FRS  Unique combination world-wide Availability of relativistic HI beams and high-resolution magnetic spectrometer

High-resolution magnetic spectrometer FRS M.V. Ricciardi, PhD thesis 238 U+Ti at 1 A GeV Z /  Z  200 A /  A  400  (  )/   5·10 -4

Engagement of the CHARMS group Status on May 2005 –10 scientists (1 Senior scientist, 6 Postdocs, 3 PhD) –Basic research: Momentum dependence of nuclear mean field Thermal instabilities of nuclear matter Nuclear dissipation Very asymmetric fission Structure effects in fission and fragmentation Nuclide production in fragmentation and fission –Applications: Nuclear astrophysics Spin, alignment and polarisation in fragmentation Transmutation of nuclear waste Nuclear safety Production of secondary beams

Spectator response to the participant blast - A measure of the momentum dependence of the nuclear mean field Momentum dependence of nuclear mean field Shi, Danielewicz and Lacey, Phys. Rev. C 64 (2001)

New FRS results Momentum dependence of nuclear mean field The data give an early signature (the acceleration of the spectator is acquired during contact with the fireball). Valuable basis for general verification of transport calculations. M.V. Ricciardi et al., PRL 90 (2003)

Major difficulties Not many data available on nuclide distributions (radiochemical methods). Difficulties in obtaining information on the dynamics of the reaction. Theoretical models facing problems in reproducing measured data IAEA - CRP F ( ) - Importance of calculating fission-fragment yields recognised but severe difficulties in modelling nuclide-distribution. Models should have predictive power (physics basis required). Nuclide production in fragmentation and fission

Measured nuclide production in fragmentation and fission Excellent basis for model development  GSI code ABLA Data available at:

GSI code ABLA - Examples high-energy reactions

GSI code ABLA - Examples low-energy reactions Excitation function and A- and Z- distributions:

Comparison between experimental data and different model calculations D. Ridikas, Fission05, Cadarache, 2005 Best results  GSI code ABLA!

r-process nucleosynthesis and fission Application I - Nuclear astrophysics Fission plays an important role in the r-process which is responsible not only for the yields of transuranium isotopes, but may have a strong influence on the formation of the majority of heavy nuclei due to fission recycling.

r-process nucleosynthesis and fission Application I - Nuclear astrophysics Uranium - Previous status: Large uncertainties on fission barriers  No calculations on nuclide distribution (only symmetric fission assumed) - Our contribution: Careful analysis of macroscopic fission barriers (A. Kelić and K.-H. Schmidt, proceedings of Fission05, Cadarache, 2005) Modelling of nuclide distribution in fission (A. Kelić, N. Zinner, E. Kolbe, K. Langanke and K.-H. Schmidt, accepted in PLB )

Nuclear Waste Application II - Nuclear-waste transmutation Fission products: 129 I (15.7 ·10 6 y), 107 Pd (6.5·10 6 y), 135 Cs (2·10 6 y), 93 Zr (1.5·10 6 y)... Heavy nuclei: 239 Pu (2.4 ·10 4 y), 237 Np (2.1·10 6 y), 241 Am (432.6 y), 242 Am (141 y)...

Accelerator-driven systems Application II - Nuclear-waste transmutation Needed: High-energy data and models of proton-induced reactions. Damage to window and construction materials due to irradiation, yields of spallation neutrons, production of radioactive nuclei...

Non-destructive characterisation of weapon grade materials or nuclear waste D. Ridikas et al Detection sensitivity. 0.1 g of nuclear material per ton of container Needed: delayed-neutron yields, fission fragments A and Z distributions. Application III - Nuclear safety

Projects with external financing From 2004: Humboldt foundation  Fundamental research; 1 fellowship on nuclear dissipation. IP_EUROTRANS  EU-FP6 Technical application - Transmutation of nuclear waste; 32 research institutes + 17 universities; 2 EURATOM fellowship + 1 financed by the project. EURISOL_DS  EU-FP6 Technical application - Production of secondary beams; 20 participants + 20 contributors; 1 fellowship; task leader - Calculations of Beam Intensities. NUMADE  EU-FP6 Technical application - Nuclear safety; 14 partners (research centers, universities, industry); 1 fellowship; task leader - Basic Physics Experiments on Photofission : FP4 – Mobility fellows (3 fellowships); FP5 - HINDAS (4 fellowships), EURISOL_R&D (1 fellowship); Humboldt foundation (1 fellowship) In total: 15 fellowships with external financing.

Collaboration GSI: Antoine Bacquias, Lydie Giot, Vladimir Henzl, Daniela Henzlova, Aleksandra Kelić, Strahinja Lukić, Pavel Nadtochy, Radek Pleskač, Maria Valentina Ricciardi, Karl-Heinz Schmidt, Orlin Yordanov / Peter Armbruster, Karlheinz Langanke Univ. Santiago de Compostela, Spain: Jose Benlliure, Jorge Pereira, Enrique Casarejos, Manuel Fernandez, Teresa Kurtukian IPN Orsay, France: Charles-Olivier Bacri, Monique Bernas, Laurent Tassan-Got, Laurent Audouin, Claude Stéphan DAPNIA/SPhN, CEA Saclay, France: Alain Boudard, Sylvie Leray, Claude Volant, Carmen Villagrasa, Beatriz Fernandez, Jean-Eric Ducret DEN/DM2S/SERMA/LENR, CEA Saclay, France: Julien Taïeb IPNL, France: Christelle Schmitt CENBG, France: Beatriz Jurado GANIL, France: Fanny Rejmund, Paolo Napolitani, David Boilley FZ Rossendorf, Germany: Arnd Junghans, Andreas Wagner Nuclear Physics Institute, Czech Republic: Andrej Kugler, Vladimir Wagner, Antonin Krasa Yale University, USA: Andreas Heinz MSU, USA: Pawel Danielewicz, L. Shi CUPP Project, Finland: Timo Enqvist University of Helsinki, Finland: Kerttuli Helariutta IPPE-Obninsk, Russia: Anatoly Ignatyuk Institute for Nuclear Research, Russia: Alexandre Botvina etc.