30 August 2026 to 6 September 2026
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High-spin structure and shape evolution in neutron-rich 192Re

Not scheduled
20m

Speaker

Arunita Mukherjee (Institute for Basic Science)

Description

The nuclei in the south of 208Pb, which is so called “blank spot” in the nuclear chart, remain experimentally less explored than other neutron-rich regions because of the difficulty in producing and identifying these nuclei with sufficient yield. In particular, the Re isotopes with Z=75 provide a sensitive testing ground for studying the evolution of nuclear shape. With increasing neutron number, these nuclei are expected to evolve from well-deformed prolate structures toward non-axial and oblate configurations. Previous studies of neighboring Re isotopes have revealed rotational structures, quasiparticle excitations, and long-lived isomeric states, indicating strong competition between intrinsic configurations and collective deformation [1,2]. The nucleus 192Re, with N=117, is especially important because it lies close to the predicted prolate-oblate transitional region [3]. However, prior to the present study, no spectroscopic information was available on its high-spin structure and the known data were mainly restricted to the low-spin isomeric state [4].
Recent developments in multi-nucleon transfer reactions with heavy-ion beams have opened new possibilities for accessing neutron-rich nuclei around A≈190, which are difficult to populate by conventional fusion-evaporation, fission, or fragmentation techniques [5]. In the present work, excited states in 192Re were populated using a multi-nucleon transfer reaction induced by a 136Xe beam at 7 MeV/nucleon incident on a 198Pt target at GANIL. Prompt and delayed γ rays from 192Re were measured using the AGATA tracking array and the second arm CATLIFE spectrometer [6] coupled to EXOGAM HPGe detectors, while projectile-like fragments were identified event-by-event with the VAMOS++ spectrometer. The 192Re reaction channel was selected using projectile-fragment identification, kinematic correlations, total kinetic energy loss selection, and confirmed with known isomer decay.
Using prompt-delayed and prompt-prompt γ-γ coincidence techniques, excited states above the known isomeric structure of 192Re were established for the first time, making it the most neutron-rich rhenium nucleus for which the excited states above an isomer have been measured . The resulting level structure provides the first experimental information on the high-spin excitation pattern of this nucleus. The observed sequence suggests the development of collective behavior above the isomeric state, while comparison with lighter neighboring odd-odd Re isotopes indicates changes in the underlying intrinsic configuration with increasing neutron number. The theoretical calculation using cranking-relativistic DFT using PC-PK1 covariant density functional and shell model-like approach was carried out to interpret the experimental result. These results extend the spectroscopy of 192Re into the high-spin regime and provide new constraints on the evolution of deformation and quasiparticle structure in neutron-rich Re isotopes below 208Pb.
References
[1] D. A. Matters et al., Phys. Rev. C 96, 014318 (2017).
[2] S. J. Steer et al., Phys. Rev. C 84, 044313 (2011).
[3] K. Sahrma et al., Phys. Rev. C 111, L031301 (2025).
[4] H. Watanabe et al., Phys. Lett. B 814, 136088 (2021).
[5] Y. X. Watanabe et al., Phys. Rev. Lett. 115, 172503 (2015).
[6] Y. Son et al., Nucl. Instr. And Meth. B 540, 234 (2023).

Authors

Arunita Mukherjee (Institute for Basic Science) Dr Y. H. Kim (Center for Exotic Nuclear Studies, Institute for Basic Science, Daejeon 34126, Republic of Korea) Dr Y. Cho (Department of Physics and Astronomy, Seoul National University, Seoul 08826, Republic of Korea) Dr N. Alahari (GANIL, France) Dr A. Lemasson (GANIL,France) Dr A. N. Andreyev (School of Physics, Engineering and Technology, University of York, Heslington, York, North Yorkshire YO10 5DD, United Kingdom) A. Utepov (GANIL, France) C. Foug´eres (GANIL, France) C. H. Kim (Department of Physics, Sungkyunkwan University, Suwon 16419, Korea) Dr D. Ackermann (GANIL, France) Dr D. Ramos (GANIL, France) D. T. Kattikat Melcom (LP2I Bordeaux, UMR5797, Universit´e de Bordeaux, CNRS, F-33170, Gradignan, France) Dr E. Clement (GANIL, France) F Recchia (University of Padua, Via 8 Febbraio, 1848, 2, 35122 Padua, Italy) F. Didierjean (University of Strasbourg, CNRS/IPHC UMR7178, F-67000 Strasbourg, France) Dr G. de Angelis (NFN Laboratori Nazionali di Legnaro, IT-35020 Legnaro, Italy) G. de France (GANIL, France) G. Fremont (GANIL, France) G. M Gu (Department of Physics, Sungkyunkwan University, Suwon 16419, Korea) Dr G. Mukherjee (Variable Energy Cyclotron Centre, 1/AF, Bidhannagar, Kolkata, West Bengal 700064, India) H. Miyatake (Wako Nuclear Science Center, IPNS, High Energy Accelerator Research Organization (KEK), Wako, Saitama 351-0198, Japan) I. Tsekhanovich (LP2I Bordeaux, UMR5797, Universit´e de Bordeaux, CNRS, F-33170, Gradignan, France) J. C. Thomas (GANIL, France) Dr J. Dudouet (Universit´e Lyon, Universit´e Claude Bernard Lyon 1, CNRS/IN2P3, IP2I Lyon, UMR 5822, F-69622 Villeurbanne, France) J. Goupil, (GANIL, France) J. Ha (CENS, IBS) Dr J. Meng (State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China) J. Park (Department of Physics, Hope College, Michigan 49423, United States) K. Chae (Department of Physics, Sungkyunkwan University, Suwon 16419, Korea) K. I. Hahn (CENS, IBS) K. Rezynkina (stituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy) M. Mukai (Wako Nuclear Science Center, IPNS, High Energy Accelerator Research Organization (KEK), Wako, Saitama 351-0198, Japan) Dr M. Rejmund (GANIL, France) M.J. Kim (Department of Physics, Sungkyunkwan University, Suwon 16419, Korea) P. Marini (LP2I Bordeaux, UMR5797, Universit´e de Bordeaux, CNRS, F-33170, Gradignan, France) P. Schury (RIKEN Nishina Center, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan) Dr R. Banik (nstitute of Engineering & Management, Kolkata 700091, India) R.M. P´erez-Vidal (nstituto de F´ısica Corpuscular, CSIC-Universidad de Valencia, Valencia E-46980, Spain) Dr S. Bae (CENS, IBS) Dr S. Bhattacharya (Variable Energy Cyclotron Centre, 1/AF, Bidhannagar, Kolkata, West Bengal 700064, India) Dr S. Bhattacharyya (Variable Energy Cyclotron Centre, 1/AF, Bidhannagar, Kolkata, West Bengal 700064, India) Dr S. Choi (nstitute for Nuclear and Particle Astrophysics, Seoul National University, Seoul 08826, Republic of Korea) S. H. Kim (Department of Physics, Sungkyunkwan University, Suwon 16419, Korea) S. Jeong (Wako Nuclear Science Center, IPNS, High Energy Accelerator Research Organization (KEK), Wako, Saitama 351-0198, Japan) T Otsuka (Department of Physics, University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-0033, Japan) T. Niwase (Wako Nuclear Science Center, IPNS, High Energy Accelerator Research Organization (KEK), Wako, Saitama 351-0198, Japan) W. Korten (CEA/DRF/IRFU, 17 rue des Martyrs 38054 Grenoble Cedex 9 France) Y. Hirayama (Wako Nuclear Science Center, IPNS, High Energy Accelerator Research Organization (KEK), Wako, Saitama 351-0198, Japan) Mr Y. Son (nstitute for Nuclear and Particle Astrophysics, Seoul National University, Seoul 08826, Republic of Korea) Dr Y.P. Wang (State Key Laboratory of Nuclear Physics and Technology, School of Physics, Peking University, Beijing 100871, China) Y.X. Watanabe (Wako Nuclear Science Center, IPNS, High Energy Accelerator Research Organization (KEK), Wako, Saitama 351-0198, Japan)

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