Physics Letters B (Apr 2023)
Studying Gamow-Teller transitions and the assignment of isomeric and ground states at N = 50
- Ali Mollaebrahimi,
- Christine Hornung,
- Timo Dickel,
- Daler Amanbayev,
- Gabriella Kripko-Koncz,
- Wolfgang R. Plaß,
- Samuel Ayet San Andrés,
- Sönke Beck,
- Andrey Blazhev,
- Julian Bergmann,
- Hans Geissel,
- Magdalena Górska,
- Hubert Grawe,
- Florian Greiner,
- Emma Haettner,
- Nasser Kalantar-Nayestanaki,
- Ivan Miskun,
- Frédéric Nowacki,
- Christoph Scheidenberger,
- Soumya Bagchi,
- Dimiter L. Balabanski,
- Ziga Brencic,
- Olga Charviakova,
- Paul Constantin,
- Masoumeh Dehghan,
- Jens Ebert,
- Lizzy Gröf,
- Oscar Hall,
- Muhsin N. Harakeh,
- Satbir Kaur,
- Anu Kankainen,
- Ronja Knöbel,
- Daria A. Kostyleva,
- Natalia Kurkova,
- Natalia Kuzminchuk,
- Israel Mardor,
- Dragos Nichita,
- Jan-Hendrik Otto,
- Zygmunt Patyk,
- Stephane Pietri,
- Sivaji Purushothaman,
- Moritz Pascal Reiter,
- Ann-Kathrin Rink,
- Heidi Roesch,
- Anamaria Spătaru,
- Goran Stanic,
- Alexandru State,
- Yoshiki K. Tanaka,
- Matjaz Vencelj,
- Helmut Weick,
- John S. Winfield,
- Michael I. Yavor,
- Jianwei Zhao
Affiliations
- Ali Mollaebrahimi
- Nuclear Energy Group, ESRIG, University of Groningen, Zernikelaan 25, 9747 AA, Groningen, the Netherlands; II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany; Corresponding author at: II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany.
- Christine Hornung
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Timo Dickel
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Daler Amanbayev
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Gabriella Kripko-Koncz
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Wolfgang R. Plaß
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Samuel Ayet San Andrés
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Sönke Beck
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Andrey Blazhev
- Institut für Kernphysik, Universität zu Köln, Universitätsstraße 16, Köln, D-50937, Germany
- Julian Bergmann
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Hans Geissel
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Magdalena Górska
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Hubert Grawe
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Florian Greiner
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Emma Haettner
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Nasser Kalantar-Nayestanaki
- Nuclear Energy Group, ESRIG, University of Groningen, Zernikelaan 25, 9747 AA, Groningen, the Netherlands
- Ivan Miskun
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Frédéric Nowacki
- Université de Strasbourg, CNRS, IPHC UMR, Strasbourg, 7178, F-67000, France
- Christoph Scheidenberger
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany; Helmholtz Research Academy Hesse for FAIR (HFHF), GSI Helmholtz Center for Heavy Ion Research, Gießen, 35392, Germany
- Soumya Bagchi
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany; Indian Institute of Technology (Indian School of Mines), Jharkhand, Dhanbad, 826004, India; Saint Mary's University, 923 Robie St, Halifax, NS B3H 3C3, Canada
- Dimiter L. Balabanski
- Extreme Light Infrastructure-Nuclear Physics (ELI-NP), Strada Reactorului 30, Bucharest-Măgurele, 077125, Romania
- Ziga Brencic
- Jozef Stefan Institute, Jamova cesta 39, Ljubljana, SI-1000 Ljubljana, Slovenia
- Olga Charviakova
- National Centre for Nuclear Research, Pasteur 7, Warszawa, 02-093, Poland
- Paul Constantin
- Extreme Light Infrastructure-Nuclear Physics (ELI-NP), Strada Reactorului 30, Bucharest-Măgurele, 077125, Romania
- Masoumeh Dehghan
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Jens Ebert
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Lizzy Gröf
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Oscar Hall
- University of Edinburgh, Edinburgh, EH9 3FD, United Kingdom
- Muhsin N. Harakeh
- Nuclear Energy Group, ESRIG, University of Groningen, Zernikelaan 25, 9747 AA, Groningen, the Netherlands
- Satbir Kaur
- Saint Mary's University, 923 Robie St, Halifax, NS B3H 3C3, Canada
- Anu Kankainen
- University of Jyväskylä, Seminaarinkatu 15, Jyväskylä, 40014, Finland; Helsinki Institute of Physics, Helsinki, 00014, Finland
- Ronja Knöbel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Daria A. Kostyleva
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany; GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Natalia Kurkova
- Flerov Laboratory of Nuclear Reactions, JINR, Dubna, 141980, Russia
- Natalia Kuzminchuk
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Israel Mardor
- Tel Aviv University, Tel Aviv, 6997801, Israel; Soreq Nuclear Research Center, Yavne, 81800, Israel
- Dragos Nichita
- Extreme Light Infrastructure-Nuclear Physics (ELI-NP), Strada Reactorului 30, Bucharest-Măgurele, 077125, Romania; Doctoral School in Engineering and Applications of Lasers and Accelerators, University Polytechnica of Bucharest, Bucharest, 060811, Romania
- Jan-Hendrik Otto
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Zygmunt Patyk
- National Centre for Nuclear Research, Pasteur 7, Warszawa, 02-093, Poland
- Stephane Pietri
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Sivaji Purushothaman
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Moritz Pascal Reiter
- University of Edinburgh, Edinburgh, EH9 3FD, United Kingdom
- Ann-Kathrin Rink
- II. Physikalisches Institut, Justus-Liebig-Universität, Heinrich-Buff-Ring 16, Gießen, 35392, Germany
- Heidi Roesch
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany; Technische Universität Darmstadt, Karolinenpl. 5, Darmstadt, D-64289, Germany
- Anamaria Spătaru
- Extreme Light Infrastructure-Nuclear Physics (ELI-NP), Strada Reactorului 30, Bucharest-Măgurele, 077125, Romania; Doctoral School in Engineering and Applications of Lasers and Accelerators, University Polytechnica of Bucharest, Bucharest, 060811, Romania
- Goran Stanic
- Johannes Gutenberg-Universität Mainz, Mainz, 55099, Germany
- Alexandru State
- Extreme Light Infrastructure-Nuclear Physics (ELI-NP), Strada Reactorului 30, Bucharest-Măgurele, 077125, Romania; Doctoral School in Engineering and Applications of Lasers and Accelerators, University Polytechnica of Bucharest, Bucharest, 060811, Romania
- Yoshiki K. Tanaka
- High Energy Nuclear Physics Laboratory, RIKEN, 2-1 Hirosawa, Wako, Saitama, 351-0198, Japan
- Matjaz Vencelj
- Jozef Stefan Institute, Jamova cesta 39, Ljubljana, SI-1000 Ljubljana, Slovenia
- Helmut Weick
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- John S. Winfield
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Michael I. Yavor
- Institute for Analytical Instrumentation, RAS, Petersburg, 190103, Russia
- Jianwei Zhao
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstraße 1, Darmstadt, 64291, Germany
- Journal volume & issue
-
Vol. 839
p. 137833
Abstract
Direct mass measurements of neutron-deficient nuclides around the N=50 shell closure below 100Sn were performed at the FRS Ion Catcher (FRS-IC) at GSI, Germany. The nuclei were produced by projectile fragmentation of 124Xe, separated in the fragment separator FRS and delivered to the FRS-IC. The masses of 14 ground states and two isomers were measured with relative mass uncertainties down to 1×10−7 using the multiple-reflection time-of-flight mass spectrometer of the FRS-IC, including the first direct mass measurements of 98Cd and 97Rh. A new QEC=5437±67 keV was obtained for 98Cd, resulting in a summed Gamow-Teller (GT) strength for the five observed transitions (0+⟶1+) as B(GT)=2.94−0.28+0.32. Investigation of this result in state-of-the-art shell model approaches accounting for the first time experimentally observed spectrum of GT transitions points to a perfect agreement for N=50 isotones. The excitation energy of the long-lived isomeric state in 94Rh was determined for the first time to be 293±21 keV. This, together with the shell model calculations, allows the level ordering in 94Rh to be understood.