https://doi.org/10.1051/epjconf/202226011021
NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
1 GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
2 Justus-Liebig-Universität Gießen, 35392 Gießen, Germany
3 Soreq Nuclear Research Center, Yavne 81800, Israel
4 Tel Aviv University, Tel Aviv 69978, Israel
5 Helmholtz Forschungsakademie Hessen für FAIR (HFHF), GSI Helmholtzzentrum für Schwerionen forschung, Campus Gießen, 35392 Gießen, Germany
6 Institute for Analytical Instrumentation of the Russian Academy of Sciences, 190103 St. Petersburg, Russia
* e-mail: t.dickel@gsi.de
Published online: 24 February 2022
We lack significant nuclear physics input to understand the rapid-neutron capture (r-)process fully. The r-process is the source of half the elements heavier than iron and the only way to produce the long-lived actinides we find on earth. This process’s key nuclear physics inputs are nuclear masses, cross-sections of (n,γ) and (γ,n), and decay half-lives and branching ratios of neutron-rich isotopes. However, there is currently no method to directly measure neutron-induced reaction rates on short-lived nuclides, so there is no experimental data for the primary nuclear reaction that drives the r-process. We show here a conceptual design of a novel approach to access this information experimentally. The idea is to form a target of short-lived isotopes by confining them as ions in a radio-frequency (RF) trap. Next, they are irradiated with an intense neutron flux, and the reaction products are identified by mass spectrometry. The chosen method is a two-stage process in the presence of high neutron fluxes. The first process is neutron-induced fission in a thin actinide foil to create fission fragments. These fragments are slowed down in a cryogenic stopping cell before being filtered through a radio frequency quadrupole (RFQ) system. The RFQ system selects fission fragments of a specific atomic mass number A and confines them to a small volume in an RF trap, where they are irradiated for a second time in a controlled manner. The resultant A+1 isotopes are mass-selectively transported to a multiple-reflection time-of-flight mass spectrometer, where the reaction products are identified and counted.
© The Authors, published by EDP Sciences, 2022
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