NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments

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,...

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Main Authors: Dickel T., Mardor I., Wilsenach H., Ashkenazy J., Plaß W. R., Scheidenberger C., Yavor M. I.
Format: Article
Language:English
Published: EDP Sciences 2022-01-01
Series:EPJ Web of Conferences
Online Access:https://www.epj-conferences.org/articles/epjconf/pdf/2022/04/epjconf_nic16th2022_11021.pdf
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author Dickel T.
Mardor I.
Wilsenach H.
Ashkenazy J.
Plaß W. R.
Scheidenberger C.
Yavor M. I.
author_facet Dickel T.
Mardor I.
Wilsenach H.
Ashkenazy J.
Plaß W. R.
Scheidenberger C.
Yavor M. I.
author_sort Dickel T.
collection DOAJ
description 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.
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spelling doaj.art-c0ef3551d08945a389d8299e1ff048902022-12-21T18:35:37ZengEDP SciencesEPJ Web of Conferences2100-014X2022-01-012601102110.1051/epjconf/202226011021epjconf_nic16th2022_11021NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragmentsDickel T.0Mardor I.1Wilsenach H.2Ashkenazy J.3Plaß W. R.4Scheidenberger C.5Yavor M. I.6GSI Helmholtzzentrum für Schwerionenforschung GmbHSoreq Nuclear Research CenterJustus-Liebig-Universität GießenSoreq Nuclear Research CenterGSI Helmholtzzentrum für Schwerionenforschung GmbHGSI Helmholtzzentrum für Schwerionenforschung GmbHInstitute for Analytical Instrumentation of the Russian Academy of SciencesWe 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.https://www.epj-conferences.org/articles/epjconf/pdf/2022/04/epjconf_nic16th2022_11021.pdf
spellingShingle Dickel T.
Mardor I.
Wilsenach H.
Ashkenazy J.
Plaß W. R.
Scheidenberger C.
Yavor M. I.
NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
EPJ Web of Conferences
title NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
title_full NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
title_fullStr NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
title_full_unstemmed NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
title_short NG-TRAP: Measuring neutron capture cross-sections of short-lived fission fragments
title_sort ng trap measuring neutron capture cross sections of short lived fission fragments
url https://www.epj-conferences.org/articles/epjconf/pdf/2022/04/epjconf_nic16th2022_11021.pdf
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