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Smooth trends in fermium charge radii and the impact of shell effects

Author

Listed:
  • Jessica Warbinek

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz
    CERN)

  • Elisabeth Rickert

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Sebastian Raeder

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz)

  • Thomas Albrecht-Schönzart

    (Colorado School of Mines)

  • Brankica Andelic

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz
    University of Groningen)

  • Julian Auler

    (Johannes Gutenberg-Universität Mainz)

  • Benjamin Bally

    (Université Paris-Saclay)

  • Michael Bender

    (CNRS/IN2P3, IP2I, UMR 5822)

  • Sebastian Berndt

    (Johannes Gutenberg-Universität Mainz)

  • Michael Block

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Alexandre Brizard

    (GANIL)

  • Pierre Chauveau

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz)

  • Bradley Cheal

    (University of Liverpool)

  • Premaditya Chhetri

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz
    KU Leuven)

  • Arno Claessens

    (KU Leuven)

  • Antoine de Roubin

    (KU Leuven)

  • Charlie Devlin

    (University of Liverpool)

  • Holger Dorrer

    (Johannes Gutenberg-Universität Mainz)

  • Christoph E. Düllmann

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Julie Ezold

    (Oak Ridge National Laboratory)

  • Rafael Ferrer

    (KU Leuven)

  • Vadim Gadelshin

    (Johannes Gutenberg-Universität Mainz)

  • Alyssa Gaiser

    (Michigan State University
    Michigan State University)

  • Francesca Giacoppo

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz)

  • Stephane Goriely

    (Université Libre de Bruxelles)

  • Manuel J. Gutiérrez

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz)

  • Ashley Harvey

    (Oak Ridge National Laboratory)

  • Raphael Hasse

    (Johannes Gutenberg-Universität Mainz)

  • Reinhard Heinke

    (Johannes Gutenberg-Universität Mainz)

  • Fritz-Peter Heßberger

    (GSI Helmholtzzentrum für Schwerionenforschung)

  • Stephane Hilaire

    (CEA, DAM, DIF
    CEA LMCE)

  • Magdalena Kaja

    (Johannes Gutenberg-Universität Mainz)

  • Oliver Kaleja

    (GSI Helmholtzzentrum für Schwerionenforschung
    Universität Greifswald)

  • Tom Kieck

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • EunKang Kim

    (Johannes Gutenberg-Universität Mainz)

  • Nina Kneip

    (Johannes Gutenberg-Universität Mainz)

  • Ulli Köster

    (Institut Laue-Langevin)

  • Sandro Kraemer

    (KU Leuven)

  • Mustapha Laatiaoui

    (Johannes Gutenberg-Universität Mainz)

  • Jeremy Lantis

    (Johannes Gutenberg-Universität Mainz)

  • Nathalie Lecesne

    (GANIL)

  • Andrea Tzeitel Loria Basto

    (Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Andrew Kishor Mistry

    (GSI Helmholtzzentrum für Schwerionenforschung
    GSI Helmholtzzentrum für Schwerionenforschung
    TU Darmstadt)

  • Christoph Mokry

    (Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Iain Moore

    (University of Jyväskylä)

  • Tobias Murböck

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz)

  • Danny Münzberg

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Witold Nazarewicz

    (Michigan State University
    Michigan State University)

  • Thorben Niemeyer

    (Johannes Gutenberg-Universität Mainz)

  • Steven Nothhelfer

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Sophie Péru

    (CEA, DAM, DIF
    CEA LMCE)

  • Andrea Raggio

    (University of Jyväskylä)

  • Paul-Gerhard Reinhard

    (Universität Erlangen)

  • Dennis Renisch

    (Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Emmanuel Rey-Herme

    (Université Paris-Saclay)

  • Jekabs Romans

    (KU Leuven)

  • Elisa Romero Romero

    (Johannes Gutenberg-Universität Mainz)

  • Jörg Runke

    (GSI Helmholtzzentrum für Schwerionenforschung
    Johannes Gutenberg-Universität Mainz)

  • Wouter Ryssens

    (Université Libre de Bruxelles)

  • Hervé Savajols

    (GANIL)

  • Fabian Schneider

    (Johannes Gutenberg-Universität Mainz)

  • Joseph Sperling

    (Colorado School of Mines)

  • Matou Stemmler

    (Johannes Gutenberg-Universität Mainz)

  • Dominik Studer

    (GSI Helmholtzzentrum für Schwerionenforschung
    Helmholtz-Institut Mainz
    Johannes Gutenberg-Universität Mainz)

  • Petra Thörle-Pospiech

    (Johannes Gutenberg-Universität Mainz
    Helmholtz-Institut Mainz)

  • Norbert Trautmann

    (Johannes Gutenberg-Universität Mainz)

  • Mitzi Urquiza-González

    (HÜBNER
    University of Gothenburg)

  • Kenneth van Beek

    (TU Darmstadt)

  • Shelley Van Cleve

    (Oak Ridge National Laboratory)

  • Piet Van Duppen

    (KU Leuven)

  • Marine Vandebrouck

    (Université Paris-Saclay)

  • Elise Verstraelen

    (KU Leuven)

  • Thomas Walther

    (TU Darmstadt)

  • Felix Weber

    (Johannes Gutenberg-Universität Mainz)

  • Klaus Wendt

    (Johannes Gutenberg-Universität Mainz)

Abstract

The quantum-mechanical nuclear-shell structure determines the stability and limits of the existence of the heaviest nuclides with large proton numbers Z ≳ 100 (refs. 1–3). Shell effects also affect the sizes and shapes of atomic nuclei, as shown by laser spectroscopy studies in lighter nuclides4. However, experimental information on the charge radii and the nuclear moments of the heavy actinide elements, which link the heaviest naturally abundant nuclides with artificially produced superheavy elements, is sparse5. Here we present laser spectroscopy measurements along the fermium (Z = 100) isotopic chain and an extension of data in the nobelium isotopic chain (Z = 102) across a key region. Multiple production schemes and different advanced techniques were applied to determine the isotope shifts in atomic transitions, from which changes in the nuclear mean-square charge radii were extracted. A range of nuclear models based on energy density functionals reproduce well the observed smooth evolution of the nuclear size. Both the remarkable consistency of model prediction and the similarity of predictions for different isotopes suggest a transition to a regime in which shell effects have a diminished effect on the size compared with lighter nuclei.

Suggested Citation

  • Jessica Warbinek & Elisabeth Rickert & Sebastian Raeder & Thomas Albrecht-Schönzart & Brankica Andelic & Julian Auler & Benjamin Bally & Michael Bender & Sebastian Berndt & Michael Block & Alexandre B, 2024. "Smooth trends in fermium charge radii and the impact of shell effects," Nature, Nature, vol. 634(8036), pages 1075-1079, October.
  • Handle: RePEc:nat:nature:v:634:y:2024:i:8036:d:10.1038_s41586-024-08062-z
    DOI: 10.1038/s41586-024-08062-z
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