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Raeder S, Ackermann D, Backe H, Beerwerth R, Berengut JC, Block M, Borschevsky A, Cheal B, Chhetri P, Düllmann CE, Dzuba VA, Eliav E, Even J, Ferrer R, Flambaum VV, Fritzsche S, Giacoppo F, Götz S, Heßberger FP, Huyse M, Kaldor U, Kaleja O, Khuyagbaatar J, Kunz P, Laatiaoui M, Lautenschläger F, Lauth W, Mistry AK, Minaya Ramirez E, Nazarewicz W, Porsev SG, Safronova MS, Safronova UI, Schuetrumpf B, Van Duppen P, Walther T, Wraith C, Yakushev A. Probing Sizes and Shapes of Nobelium Isotopes by Laser Spectroscopy. PHYSICAL REVIEW LETTERS 2018; 120:232503. [PMID: 29932712 DOI: 10.1103/physrevlett.120.232503] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.8] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/02/2018] [Revised: 04/20/2018] [Indexed: 06/08/2023]
Abstract
Until recently, ground-state nuclear moments of the heaviest nuclei could only be inferred from nuclear spectroscopy, where model assumptions are required. Laser spectroscopy in combination with modern atomic structure calculations is now able to probe these moments directly, in a comprehensive and nuclear-model-independent way. Here we report on unique access to the differential mean-square charge radii of ^{252,253,254}No, and therefore to changes in nuclear size and shape. State-of-the-art nuclear density functional calculations describe well the changes in nuclear charge radii in the region of the heavy actinides, indicating an appreciable central depression in the deformed proton density distribution in ^{252,254}No isotopes. Finally, the hyperfine splitting of ^{253}No was evaluated, enabling a complementary measure of its (quadrupole) deformation, as well as an insight into the neutron single-particle wave function via the nuclear spin and magnetic moment.
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Affiliation(s)
- S Raeder
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - D Ackermann
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- GANIL, CEA/DRF-CNRS/IN2P3, Boulevard Henri Becquerel, BP 55027, F-14076 Caen, France
| | - H Backe
- Institut für Kernphysik, Johannes Gutenberg Universität, 55128 Mainz, Germany
| | - R Beerwerth
- Helmholtz-Institut Jena, 07743 Jena, Germany
- Theoretisch-Physikalisches Institut, Friedrich-Schiller-Universität Jena, 07743 Jena, Germany
| | - J C Berengut
- School of Physics, University of New South Wales, Sydney 2052, Australia
| | - M Block
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Institut für Kernchemie, Johannes Gutenberg Universität, 55128 Mainz, Germany
| | - A Borschevsky
- Van Swinderen Institute, University of Groningen, 9747 AG Groningen, The Netherlands
| | - B Cheal
- Department of Physics, University of Liverpool, L69 7ZE Liverpool, United Kingdom
| | - P Chhetri
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Institut für Angewandte Physik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - Ch E Düllmann
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Institut für Kernchemie, Johannes Gutenberg Universität, 55128 Mainz, Germany
| | - V A Dzuba
- School of Physics, University of New South Wales, Sydney 2052, Australia
| | - E Eliav
- School of Chemistry, Tel Aviv University, 69978 Tel Aviv, Israel
| | - J Even
- KVI-CART, University of Groningen, 9747 AA Groningen, The Netherlands
| | - R Ferrer
- KU Leuven, Instituut voor Kern- en Stralingsfysica, 3001 Leuven, Belgium
| | - V V Flambaum
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- School of Physics, University of New South Wales, Sydney 2052, Australia
| | - S Fritzsche
- Helmholtz-Institut Jena, 07743 Jena, Germany
- Theoretisch-Physikalisches Institut, Friedrich-Schiller-Universität Jena, 07743 Jena, Germany
| | - F Giacoppo
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - S Götz
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- Institut für Kernchemie, Johannes Gutenberg Universität, 55128 Mainz, Germany
| | - F P Heßberger
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - M Huyse
- KU Leuven, Instituut voor Kern- en Stralingsfysica, 3001 Leuven, Belgium
| | - U Kaldor
- School of Chemistry, Tel Aviv University, 69978 Tel Aviv, Israel
| | - O Kaleja
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - J Khuyagbaatar
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - P Kunz
- TRIUMF, 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, Canada
| | - M Laatiaoui
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - F Lautenschläger
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Institut für Angewandte Physik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - W Lauth
- Institut für Kernphysik, Johannes Gutenberg Universität, 55128 Mainz, Germany
| | - A K Mistry
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | | | - W Nazarewicz
- Department of Physics and Astronomy and FRIB Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - S G Porsev
- Department of Physics and Astronomy, University of Delaware, Newark, Delaware 19716, USA
- Petersburg Nuclear Physics Institute of NRC "Kurchatov Institute," Gatchina, Leningrad District 188300, Russia
| | - M S Safronova
- Department of Physics and Astronomy, University of Delaware, Newark, Delaware 19716, USA
- Joint Quantum Institute, NIST and the University of Maryland, College Park, Maryland 20742, USA
| | - U I Safronova
- Physics Department, University of Nevada, Reno, Nevada 89557, USA
| | - B Schuetrumpf
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - P Van Duppen
- KU Leuven, Instituut voor Kern- en Stralingsfysica, 3001 Leuven, Belgium
| | - T Walther
- Institut für Angewandte Physik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - C Wraith
- Department of Physics, University of Liverpool, L69 7ZE Liverpool, United Kingdom
| | - A Yakushev
- Helmholtz-Institut Mainz, 55128 Mainz, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
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Stone JR, Guichon PAM, Reinhard PG, Thomas AW. Finite Nuclei in the Quark-Meson Coupling Model. PHYSICAL REVIEW LETTERS 2016; 116:092501. [PMID: 26991171 DOI: 10.1103/physrevlett.116.092501] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/08/2015] [Indexed: 06/05/2023]
Abstract
We report the first use of the effective quark-meson coupling (QMC) energy density functional (EDF), derived from a quark model of hadron structure, to study a broad range of ground state properties of even-even nuclei across the periodic table in the nonrelativistic Hartree-Fock+BCS framework. The novelty of the QMC model is that the nuclear medium effects are treated through modification of the internal structure of the nucleon. The density dependence is microscopically derived and the spin-orbit term arises naturally. The QMC EDF depends on a single set of four adjustable parameters having a clear physics basis. When applied to diverse ground state data the QMC EDF already produces, in its present simple form, overall agreement with experiment of a quality comparable to a representative Skyrme EDF. There exist, however, multiple Skyrme parameter sets, frequently tailored to describe selected nuclear phenomena. The QMC EDF set of fewer parameters, derived in this work, is not open to such variation, chosen set being applied, without adjustment, to both the properties of finite nuclei and nuclear matter.
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Affiliation(s)
- J R Stone
- Department of Physics, University of Oxford, Oxford OX1 3PU, United Kingdom
- Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
| | - P A M Guichon
- SPhN-IRFU, CEA Saclay, F91191 Gif sur Yvette, France
| | - P G Reinhard
- Institut für Theoretische Physik II, Universität Erlangen, D-91058 Erlangen, Germany
| | - A W Thomas
- ARC Centre of Excellence in Particle Physics at the Terascale and CSSM, Department of Physics, University of Adelaide, SA 5005 Australia
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