9–13 Mar 2026
Salle Totem, Le Bachat, Chamrousse, France
Europe/Paris timezone

Session

session 4 (Chair: N. Pillet)

session_04
10 Mar 2026, 10:35
Salle Totem, Le Bachat, Chamrousse, France

Salle Totem, Le Bachat, Chamrousse, France

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  1. Timo Dickel (GSI Helmholtzzentrum für Schwerionenforschung GmbH(GSI))
    10/03/2026, 10:35

    The structure of fission barriers in actinide nuclei is characterized by pronounced multi-humped shapes, which give rise to long-lived isomeric states trapped in secondary minima of the potential-energy surface. These complex barrier profiles emerge from the interplay between macroscopic liquid-drop behavior and microscopic shell effects. In the region around the deformed magic neutron number...

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  2. Mr Henrik Haug (University of Oslo)
    10/03/2026, 11:00

    H. S. Haug1, S. Marin2, N. P. Giha2,3, J. N. Wilson4, I. A. Tolstukhin3, A. Al-Adili1,5, D.Gjestvang1, S. Siem1

    1 Department of Physics, University of Oslo, N-0316 Oslo, Norway
    2 Department of Nuclear Engineering and Radiological Sciences, University of Michigan, Ann Arbor, Michigan 48109, USA
    3 Physics Division, Argonne National Laboratory, Lemont, Illinois 60439, USA
    4 Universit´e...

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  3. Alex Cobo Zarzuelo (GANIL)
    10/03/2026, 11:15

    Since the discovery of fission in 1939, several theoretical models were developed to properly explain the observations [1]. It wasn’t until the introduction of shell effects by Strutinsky [2], that the microscopic - macroscopic models [3] could match the measured yields of heavy actinides like 252Cf or 254Es [4]. The interplay between both quantities prevents, so far, from a fully...

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