3–7 Oct 2022
Science Culture Center, IBS
Asia/Seoul timezone

High-resolution mass measurements for the verification of particle identification at in-flight separators

3 Oct 2022, 21:42
8m
S236 (Science Culture Center, IBS)

S236

Science Culture Center, IBS

55 EXPO-ro, Yuseong-gu, Daejeon
Poster Session Poster Session

Speaker

Christine Hornung (GSI Helmholtzzentrum für Schwerionenforschung)

Description

Nowadays, many experiments in the field of nuclear structure, fundamental interactions and nuclear astrophysics require the use of exotic nuclei. These rare isotopes can be produced with modern powerful accelerator facilities at several laboratories worldwide. These laboratories solve the problem of the inherent small production cross sections via high primary beam intensities and high energies. However, the successful production of exotic nuclei is only the first necessary step, the separation from the primary beam and from the abundant contaminants and the particle identification, by measurements of their properties are of equal importance.

At the FRS facility at GSI, exotic ions are produced, separated and identified in-flight. The Particle IDentification (PID) by proton number (Z) and mass number (A) can be performed with the FRS and its particle detectors applying the B$\rho$-$\Delta$E-TOF method. At relativistic velocities, the verification of the selected bare ions can be easily performed with particle detectors via velocity (TOF), energy-deposition ($\Delta$E) and magnetic rigidity (B$\rho$) measurements in coincidence. Still the separation and identification requires an elaborated absolute calibration. At lower velocities (300~MeV/u), the heaviest fragments emerge from the target in different ionic charge states which makes an unambiguous PID very difficult.

Therefore, the fragment identification in-flight by the B$\rho$-$\Delta$E-TOF method at these velocities can be verified by accurate high-resolution mass measurements. Note that each isotope has a unique signature in terms of the measured binding energy (mass excess). At the final focal plane of the FRS, the FRS Ion Catcher (FRS-IC) setup is installed where the ions-of-interest are stopped in a gas cell to perform accurate mass measurements. The mass measurements of the ions are performed with a multi-reflection time-of-flight mass spectrometer (MR-TOF-MS). In this way, the FRS-IC can provide an unambiguous isotope identification via high-resolution mass measurement. This method has been successfully applied with the combination of the FRS-IC and the in-flight separator FRS. The method is fast, sensitive and universal. A verification of the FRS PID by the MR-TOF-MS at the FRS-IC was proven in several experiment with $^{107}$Ag, $^{124}$Xe, $^{208}$Pb and $^{238}$U primary beams.

Primary authors

Christine Hornung (GSI Helmholtzzentrum für Schwerionenforschung) Timo Dickel (GSI Helmholtzzentrum für Schwerionenforschung GmbH; JLU Gießen, Germany) Daler Amanbayev (Justus-Liebig-Universität Gießen, II. Physikalisches Institut, Gießen, Germany) Samuel Ayet San Andres (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany, Justus-Liebig-Universität Gießen, II. Physikalisches Institut, Gießen, Germany) Sönke Beck (Justus-Liebig-Universität Gießen, II. Physikalisches Institut, Gießen, Germany) Julian Bergmann (Justus-Liebig-Universität Gießen, II. Physikalisches Institut, Gießen, Germany) Hans Geissel (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany; JLU Gießen, Germany) Emma Haettner (GSI Helmholtzzentrum für Schwerionenforschung GmbH) Jan-Paul Hucka (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany, Institut für Kernphysik, Technische Universität Darmstadt, D-64289 Darmstadt, Germany) Gabriella Kripko-Koncz (Justus-Liebig-Universität Gießen, II. Physikalisches Institut, Gießen, Germany) Israel Mardor (Tel Aviv University, 6997801 Tel Aviv, Israel, Soreq Nuclear Research Center, 81800 Yavne, Israel) Ali Mollaebrahimi (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany, Nuclear Energy Group, ESRIG, University of Groningen, 9747 AA Groningen, The Netherlands) Ivan Mukha (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany) Stephane Pietri (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany) Wolfgang Plass (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany; JLU Gießen, Germany) Sivaji Purushothaman (GSI Helmholtzzentrum für Schwerionenforschung GmbH) Moritz Pascal Reiter (Justus-Liebig-Universität Gießen, II. Physikalisches Institut, Gießen, Germany, University of Edinburgh, EH8 9AB Edinburgh, United Kingdom) Heidi Rösch (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany, Institut für Kernphysik, Technische Universität Darmstadt, D-64289 Darmstadt, Germany) Christoph Scheidenberger (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany; JLU Gießen, Germany) Yoshiki Tanaka (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany) Helmut Weick (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany) Jianwei Zhao (GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany)

Presentation materials

There are no materials yet.