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Charge Radii Measurements of Exotic Tin Isotopes in the Proximity of N=50 and N=82

F. P. Gustafsson1,2,*, L. V. Rodríguez3,2,4,†, R. F. Garcia Ruiz5,6,2,‡, T. Miyagi7,8,9,3, S. W. Bai10, D. L. Balabanski11, C. L. Binnersley6, M. L. Bissell6, K. Blaum3 et al.

B. Cheal12, T. E. Cocolios1, G. J. Farooq-Smith1, K. T. Flanagan6,13, S. Franchoo4, A. Galindo-Uribarri14,15, G. Georgiev4, W. Gins1, C. Gorges8, R. P. de Groote1, H. Heylen2, J. D. Holt16,17, A. Kanellakopoulos1, J. Karthein5,§, S. Kaufmann8, Á. Koszorús1, K. König8, V. Lagaki2,18, S. Lechner2,19, B. Maass8, S. Malbrunot-Ettenauer2, W. Nazarewicz20, R. Neugart21,3, G. Neyens1,2, W. Nörtershäuser8, T. Otsuka22,1,23,24,25, P.-G. Reinhard26, N. Rondelez1, E. Romero-Romero14,15, C. M. Ricketts6, S. Sailer27, R. Sánchez28, S. Schmidt8, A. Schwenk8,9,3, S. R. Stroberg16,29,30, N. Shimizu7, Y. Tsunoda22, A. R. Vernon5, L. Wehner21, S. G. Wilkins5, C. Wraith12, L. Xie6, Z. Y. Xu1, X. F. Yang10, and D. T. Yordanov3,4,2

  • 1Instituut voor Kern- en Stralingsfysica, KU Leuven, 3001 Leuven, Belgium
  • 2CERN, 1211 Geneva 23, Switzerland
  • 3Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
  • 4IJCLab, Université Paris-Saclay, CNRS/IN2P3, 91405 Orsay, France
  • 5Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
  • 6School of Physics and Astronomy, The University of Manchester, Manchester, M13 9PL, United Kingdom
  • 7Center for Computational Sciences, University of Tsukuba, 1-1-1 Tennodai, Tsukuba, Ibaraki 305-8577, Japan
  • 8Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
  • 9ExtreMe Matter Institute, GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
  • 10School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
  • 11ELI-NP, Horia Hulubei National Institute for R&D in Physics and Nuclear Engineering, 077125 Magurele, Romania
  • 12Oliver Lodge Laboratory, Oxford Street, University of Liverpool, Liverpool L69 7ZE, United Kingdom
  • 13Photon Science Institute, Alan Turing Building, The University of Manchester, Manchester, M13 9PY, United Kingdom
  • 14Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 15Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
  • 16TRIUMF, Vancouver, British Columbia V6T 2A3, Canada
  • 17Department of Physics, McGill University, Montréal, Quebec H3A 2T8, Canada
  • 18Institut für Physik, Universität Greifswald, 17487 Greifswald, Germany
  • 19Technische Universität Wien, Karlsplatz 13, 1040 Wien, Austria
  • 20Facility for Rare Isotope Beams and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan, USA
  • 21Institut für Kernchemie, Universität Mainz, 55128 Mainz, Germany
  • 22Center for Nuclear Study, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
  • 23Department of Physics, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
  • 24RIKEN Nishina Center, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan
  • 25National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
  • 26Institut für Theoretische Physik, Friedrich-Alexander-Universität, Erlangen/Nürnberg, Germany
  • 27Technische Universität München, 80333 Munich, Germany
  • 28GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
  • 29Department of Physics, University of Washington, Seattle, Washington, USA
  • 30Physics Division, Argonne National Laboratory, Lemont, Illinois, USA

  • *Contact author: fredrik.parnefjord.gustafsson@cern.ch
  • †Contact author: liss.vazquez.rodriguez@cern.ch
  • ‡Contact author: rgarciar@mit.edu
  • §Present Address: Texas A&M University, Cyclotron Institute/Department of Physics and Astronomy, College Station, Texas 77840, USA.

Phys. Rev. Lett. 135, 222501 – Published 25 November, 2025

DOI: https://doi.org/10.1103/wbdx-k3cd

Abstract

We report nuclear charge radii for the isotopes Sn104–134, measured using two different collinear laser spectroscopy techniques at ISOLDE-CERN. These measurements clarify the archlike trend in charge radii along the isotopic chain and reveal an odd-even staggering that is more pronounced near the N=50 and N=82 shell closures. The observed local trends are well described by both nuclear density functional theory and valence space in-medium similarity renormalization group calculations. Both theories predict appreciable contributions from beyond-mean-field correlations to the charge radii of the neutron-deficient tin isotopes. The models, however, fall short of reproducing the magnitude of the known B(E2) transition probabilities, highlighting the remaining challenges in achieving a unified description of both ground-state properties and collective phenomena.

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