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High-Precision Spectroscopy of
Zanon, I; Clément, E; Goasduff, A; Menéndez, J; Miyagi, T; Assié, M; Ciemala, M; Flavigny, F; Lemasson, A; Matta, A; Ramos, D; Rejmund, M; Achouri, L; Ackermann, D; Barrientos, D; Beaumel, D; Benzoni, G; Boston, A J; Boston, H C; Bottoni, S; Bracco, A; Brugnara, D; de France, G; de Sereville, N; Delaunay, F; Desesquelles, P; Didierjean, F; Domingo-Prato, C; Dudouet, J; Eberth, J; Fernández, D; Fougères, C; Gadea, A; Galtarossa, F; Girard-Alcindor, V; Gonzales, V; Gottardo, A; Hammache, F; Harkness-Brennan, L J; Hess, H; Judson, D S; Jungclaus, A; Kaskas, A; Kim, Y H; Kusoglu, A; Labiche, M; Leblond, S; Lenain, C; Lenzi, S M; Leoni, S.
Afiliación
  • Zanon I; INFN Laboratori Nazionali di Legnaro, Legnaro, Italy.
  • Clément E; Dipartimento di Fisica e Scienze della Terra, Università di Ferrara, Ferrara, Italy.
  • Goasduff A; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Menéndez J; INFN Laboratori Nazionali di Legnaro, Legnaro, Italy.
  • Miyagi T; Department of Quantum Physics and Astrophysics and Institute of Cosmos Sciences, University of Barcelona, Spain.
  • Assié M; Department of Physics, Technische Universität Darmstadt, Darmstadt, Germany.
  • Ciemala M; ExtreMe Matter Institute, GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.
  • Flavigny F; Max-Planck-Institut für Kernphysik, Heidelberg, Germany.
  • Lemasson A; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Matta A; IFJ PAN, Krakow, Poland.
  • Ramos D; Université de Caen Normandie, ENSICAEN, CNRS/IN2P3, LPC Caen UMR6534, F-14000 Caen, France.
  • Rejmund M; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Achouri L; Université de Caen Normandie, ENSICAEN, CNRS/IN2P3, LPC Caen UMR6534, F-14000 Caen, France.
  • Ackermann D; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Barrientos D; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Beaumel D; Université de Caen Normandie, ENSICAEN, CNRS/IN2P3, LPC Caen UMR6534, F-14000 Caen, France.
  • Benzoni G; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Boston AJ; CERN, CH-1211 Geneva 23, Switzerland.
  • Boston HC; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Bottoni S; INFN Sezione di Milano, I-20133 Milano, Italy.
  • Bracco A; Oliver Lodge Laboratory, The University of Liverpool, Liverpool, United Kingdom.
  • Brugnara D; Oliver Lodge Laboratory, The University of Liverpool, Liverpool, United Kingdom.
  • de France G; INFN Sezione di Milano, I-20133 Milano, Italy.
  • de Sereville N; Dipartimento di Fisica, Università di Milano, Milano, Italy.
  • Delaunay F; INFN Sezione di Milano, I-20133 Milano, Italy.
  • Desesquelles P; Dipartimento di Fisica, Università di Milano, Milano, Italy.
  • Didierjean F; INFN Laboratori Nazionali di Legnaro, Legnaro, Italy.
  • Domingo-Prato C; Dipartimento di Fisica, Università di Padova, Padova, Italy.
  • Dudouet J; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Eberth J; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Fernández D; Université de Caen Normandie, ENSICAEN, CNRS/IN2P3, LPC Caen UMR6534, F-14000 Caen, France.
  • Fougères C; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Gadea A; Université de Strasbourg, IPHC, Strasbourg, France.
  • Galtarossa F; Instituto de Fisica Corpuscolar, CSIC-Universidad de Valencia, E-46071 Valencia, Spain.
  • Girard-Alcindor V; Université de Lyon, Université Lyon-1, CNRS/IN2P3, UMR5822, IP2I, F-69622 Villeurbanne Cedex, France.
  • Gonzales V; Institut für Kernphysik, Universität zu Köln, Zülpicher Strasse 77, D-50937 Köln, Germany.
  • Gottardo A; IGFAE and Department de Física de Partículas, Universidade of Santiago de Compostela, Santiago de Compostela, Spain.
  • Hammache F; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Harkness-Brennan LJ; Instituto de Fisica Corpuscolar, CSIC-Universidad de Valencia, E-46071 Valencia, Spain.
  • Hess H; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Judson DS; Grand Accélérateur National d'Ions Lourds (GANIL), CEA/DRF-CNRS/IN2P3, Caen, France.
  • Jungclaus A; Departamento de Ingeniería Electrónica, Universitat de Valencia, Burjassot, Valencia, Spain.
  • Kaskas A; INFN Laboratori Nazionali di Legnaro, Legnaro, Italy.
  • Kim YH; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Kusoglu A; Oliver Lodge Laboratory, The University of Liverpool, Liverpool, United Kingdom.
  • Labiche M; Institut für Kernphysik, Universität zu Köln, Zülpicher Strasse 77, D-50937 Köln, Germany.
  • Leblond S; Oliver Lodge Laboratory, The University of Liverpool, Liverpool, United Kingdom.
  • Lenain C; Instituto de Estructura de la Materia, CSIC, Madrid, E-28006 Madrid, Spain.
  • Lenzi SM; Department of Physics, Faculty of Science, Ankara University, 06100 Besevler - Ankara, Turkey.
  • Leoni S; Institue Laue-Langevin, Grenoble, France.
Phys Rev Lett ; 131(26): 262501, 2023 Dec 29.
Article en En | MEDLINE | ID: mdl-38215380
ABSTRACT
The excited states of unstable ^{20}O were investigated via γ-ray spectroscopy following the ^{19}O(d,p)^{20}O reaction at 8 AMeV. By exploiting the Doppler shift attenuation method, the lifetimes of the 2_{2}^{+} and 3_{1}^{+} states were firmly established. From the γ-ray branching and E2/M1 mixing ratios for transitions deexciting the 2_{2}^{+} and 3_{1}^{+} states, the B(E2) and B(M1) were determined. Various chiral effective field theory Hamiltonians, describing the nuclear properties beyond ground states, along with a standard USDB interaction, were compared with the experimentally obtained data. Such a comparison for a large set of γ-ray transition probabilities with the valence space in medium similarity renormalization group ab initio calculations was performed for the first time in a nucleus far from stability. It was shown that the ab initio approaches using chiral effective field theory forces are challenged by detailed high-precision spectroscopic properties of nuclei. The reduced transition probabilities were found to be a very constraining test of the performance of the ab initio models.

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2023 Tipo del documento: Article País de afiliación: Italia Pais de publicación: Estados Unidos

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Phys Rev Lett Año: 2023 Tipo del documento: Article País de afiliación: Italia Pais de publicación: Estados Unidos