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Zhang S, Cheng Z, Li J, Xu Z, Xu F. 含手征三体力的第一性原理Gamow壳模型计算<sup>14</sup>O同中子素. CHINESE SCIENCE BULLETIN-CHINESE 2022. [DOI: 10.1360/tb-2022-0432] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/09/2022]
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2
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Jin Y, Niu CY, Brown KW, Li ZH, Hua H, Anthony AK, Barney J, Charity RJ, Crosby J, Dell'Aquila D, Elson JM, Estee J, Ghazali M, Jhang G, Li JG, Lynch WG, Michel N, Sobotka LG, Sweany S, Teh FCE, Thomas A, Tsang CY, Tsang MB, Wang SM, Wu HY, Yuan CX, Zhu K. First Observation of the Four-Proton Unbound Nucleus ^{18}Mg. PHYSICAL REVIEW LETTERS 2021; 127:262502. [PMID: 35029460 DOI: 10.1103/physrevlett.127.262502] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/30/2021] [Revised: 10/18/2021] [Accepted: 11/16/2021] [Indexed: 06/14/2023]
Abstract
^{18}Mg was observed, for the first time, by the invariant-mass reconstruction of ^{14}O+4p events. The ground-state decay energy and width are E_{T}=4.865(34) MeV and Γ=115(100) keV, respectively. The observed momentum correlations between the five particles are consistent with two sequential steps of prompt 2p decay passing through the ground state of ^{16}Ne. The invariant-mass spectrum also provides evidence for an excited state at an excitation energy of 1.84(14) MeV, which is likely the first excited 2^{+} state. As this energy exceeds that for the 2^{+} state in ^{20}Mg, this observation provides an argument for the demise of the N=8 shell closure in nuclei far from stability. However, in open systems this classical argument for shell strength is compromised by Thomas-Ehrman shifts.
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Affiliation(s)
- Y Jin
- School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
| | - C Y Niu
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - K W Brown
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
| | - Z H Li
- School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
| | - H Hua
- School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
| | - A K Anthony
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - J Barney
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - R J Charity
- Department of Chemistry, Washington University, St. Louis, Missouri 63130, USA
| | - J Crosby
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - D Dell'Aquila
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - J M Elson
- Department of Chemistry, Washington University, St. Louis, Missouri 63130, USA
| | - J Estee
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - M Ghazali
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - G Jhang
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - J G Li
- School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China
| | - W G Lynch
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - N Michel
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, China
| | - L G Sobotka
- Department of Chemistry, Washington University, St. Louis, Missouri 63130, USA
- Department of Physics, Washington University, St. Louis, Missouri 63130, USA
| | - S Sweany
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - F C E Teh
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - A Thomas
- Department of Chemistry, Washington University, St. Louis, Missouri 63130, USA
| | - C Y Tsang
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - M B Tsang
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - S M Wang
- Institute of Modern Physics, Fudan University, Shanghai 200433, China
- FRIB Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - H Y Wu
- School of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China
| | - C X Yuan
- Sino-French Institute of Nuclear Engineering and Technology, Sun Yat-Sen University, Zhuhai 519082, China
| | - K Zhu
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
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Kostyleva D, Mukha I, Acosta L, Casarejos E, Chudoba V, Ciemny AA, Dominik W, Dueñas JA, Dunin V, Espino JM, Estradé A, Farinon F, Fomichev A, Geissel H, Gorshkov A, Grigorenko LV, Janas Z, Kamiński G, Kiselev O, Knöbel R, Krupko S, Kuich M, Litvinov YA, Marquinez-Durán G, Martel I, Mazzocchi C, Nociforo C, Ordúz AK, Pfützner M, Pietri S, Pomorski M, Prochazka A, Rymzhanova S, Sánchez-Benítez AM, Scheidenberger C, Simon H, Sitar B, Slepnev R, Stanoiu M, Strmen P, Szarka I, Takechi M, Tanaka YK, Weick H, Winkler M, Winfield JS, Xu X, Zhukov MV. Towards the Limits of Existence of Nuclear Structure: Observation and First Spectroscopy of the Isotope ^{31}K by Measuring Its Three-Proton Decay. PHYSICAL REVIEW LETTERS 2019; 123:092502. [PMID: 31524489 DOI: 10.1103/physrevlett.123.092502] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/22/2019] [Revised: 06/28/2019] [Indexed: 06/10/2023]
Abstract
The most remote isotope from the proton dripline (by 4 atomic mass units) has been observed: ^{31}K. It is unbound with respect to three-proton (3p) emission, and its decays have been detected in flight by measuring the trajectories of all decay products using microstrip detectors. The 3p emission processes have been studied by the means of angular correlations of ^{28}S+3p and the respective decay vertices. The energies of the previously unknown ground and excited states of ^{31}K have been determined. This provides its 3p separation energy value S_{3p} of -4.6(2) MeV. Upper half-life limits of 10 ps of the observed ^{31}K states have been derived from distributions of the measured decay vertices.
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Affiliation(s)
- D Kostyleva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - I Mukha
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - L Acosta
- INFN, Laboratori Nazionali del Sud, Via S. Sofía, 95123 Catania, Italy
- Instituto de Física, Universidad Nacional Autónoma de México, México, Distrito Federal 01000, Mexico
| | | | - V Chudoba
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
- Institute of Physics, Silesian University Opava, 74601 Opava, Czech Republic
| | - A A Ciemny
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - W Dominik
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - J A Dueñas
- Departamento de Ingenieria Electrica y Centro de Estudios Avanzados en Fisica, Matemáticas y Computación, Universidad de Huelva, 21071 Huelva, Spain
| | - V Dunin
- Veksler and Baldin Laboratory of High Energy Physics, JINR, 141980 Dubna, Russia
| | - J M Espino
- Department of Atomic, Molecular and Nuclear Physics, University of Seville, 41012 Seville, Spain
| | - A Estradé
- University of Edinburgh, EH1 1HT Edinburgh, United Kingdom
| | - F Farinon
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - A Fomichev
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - H Geissel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - A Gorshkov
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - L V Grigorenko
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
- National Research Nuclear University "MEPhI," 115409 Moscow, Russia
- National Research Centre "Kurchatov Institute," Kurchatov square 1, 123182 Moscow, Russia
| | - Z Janas
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - G Kamiński
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
- Heavy Ion Laboratory, University of Warsaw, 02-093 Warszawa, Poland
| | - O Kiselev
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - R Knöbel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - S Krupko
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - M Kuich
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
- Faculty of Physics, Warsaw University of Technology, 00-662 Warszawa, Poland
| | - Yu A Litvinov
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - G Marquinez-Durán
- Department of Applied Physics, University of Huelva, 21071 Huelva, Spain
| | - I Martel
- Department of Physics, University of Liverpool, Liverpool L69 9ZE, United Kingdom
| | - C Mazzocchi
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - C Nociforo
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - A K Ordúz
- Grand Accélérateur National d'Ions Lourds - GANIL, Bd Henri Becquerel, 14076 Caen, France
| | - M Pfützner
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - S Pietri
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - M Pomorski
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - A Prochazka
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - S Rymzhanova
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - A M Sánchez-Benítez
- Centro de Estudios Avanzados en Física, Matemáticas y Computación (CEAFMC), Department of Integrated Sciences, University of Huelva, 21071 Huelva, Spain
| | - C Scheidenberger
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - H Simon
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - B Sitar
- Faculty of Mathematics and Physics, Comenius University, 84248 Bratislava, Slovakia
| | - R Slepnev
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - M Stanoiu
- IFIN-HH, Post Office Box MG-6, 077125 Bucharest, Romania
| | - P Strmen
- Faculty of Mathematics and Physics, Comenius University, 84248 Bratislava, Slovakia
| | - I Szarka
- Faculty of Mathematics and Physics, Comenius University, 84248 Bratislava, Slovakia
| | - M Takechi
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - Y K Tanaka
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- University of Tokyo, 113-0033 Tokyo, Japan
| | - H Weick
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - M Winkler
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - J S Winfield
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
| | - X Xu
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291 Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China
| | - M V Zhukov
- Department of Physics, Chalmers University of Technology, S-41296 Göteborg, Sweden
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Wang SM, Nazarewicz W. Puzzling Two-Proton Decay of ^{67}Kr. PHYSICAL REVIEW LETTERS 2018; 120:212502. [PMID: 29883183 DOI: 10.1103/physrevlett.120.212502] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/20/2018] [Revised: 04/20/2018] [Indexed: 06/08/2023]
Abstract
Ground-state two-proton (2p) radioactivity is a rare decay mode found in a few very proton-rich isotopes. The 2p decay lifetime and properties of emitted protons carry invaluable information on nuclear structure in the presence of a low-lying proton continuum. The recently measured 2p decay of ^{67}Kr turned out to be unexpectedly fast. Since ^{67}Kr is expected to be a deformed system, we investigate the impact of deformation effects on the 2p radioactivity. We apply the recently developed Gamow coupled-channel framework, which allows for a precise description of three-body systems in the presence of rotational and vibrational couplings. This is the first application of a three-body approach to a two-nucleon decay from a deformed nucleus. We show that deformation couplings significantly increase the 2p decay width of ^{67}Kr; this finding explains the puzzling experimental data. The calculated angular proton-proton correlations reflect a competition between 1p and 2p decay modes in this nucleus.
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Affiliation(s)
- S M Wang
- FRIB/NSCL Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - W Nazarewicz
- Department of Physics and Astronomy and FRIB Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
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5
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Mukha I, Grigorenko LV, Xu X, Acosta L, Casarejos E, Ciemny AA, Dominik W, Duénas-Díaz J, Dunin V, Espino JM, Estradé A, Farinon F, Fomichev A, Geissel H, Golubkova TA, Gorshkov A, Janas Z, Kamiński G, Kiselev O, Knöbel R, Krupko S, Kuich M, Litvinov YA, Marquinez-Durán G, Martel I, Mazzocchi C, Nociforo C, Ordúz AK, Pfützner M, Pietri S, Pomorski M, Prochazka A, Rymzhanova S, Sánchez-Benítez AM, Scheidenberger C, Sharov P, Simon H, Sitar B, Slepnev R, Stanoiu M, Strmen P, Szarka I, Takechi M, Tanaka YK, Weick H, Winkler M, Winfield JS, Zhukov MV. Observation and Spectroscopy of New Proton-Unbound Isotopes ³⁰Ar and ²⁹Cl: An Interplay of Prompt Two-Proton and Sequential Decay. PHYSICAL REVIEW LETTERS 2015; 115:202501. [PMID: 26613434 DOI: 10.1103/physrevlett.115.202501] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/06/2015] [Indexed: 06/05/2023]
Abstract
Previously unknown isotopes (30)Ar and (29)Cl have been identified by measurement of the trajectories of their in-flight decay products (28)S+p+p and (28)S+p, respectively. The analysis of angular correlations of the fragments provided information on decay energies and the structure of the parent states. The ground states of (30)Ar and (29)Cl were found at 2.25(-0.10)(+0.15) and 1.8±0.1 MeV above the two- and one-proton thresholds, respectively. The lowest states in (30)Ar and (29)Cl point to a violation of isobaric symmetry in the structure of these unbound nuclei. The two-proton decay has been identified in a transition region between simultaneous two-proton and sequential proton emissions from the (30)Ar ground state, which is characterized by an interplay of three-body and two-body decay mechanisms. The first hint of a fine structure of the two-proton decay of (30)Ar*(2(+)) has been obtained by detecting two decay branches into the ground and first-excited states of the (28)S fragment.
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Affiliation(s)
- I Mukha
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- National Research Centre "Kurchatov Institute," Kurchatov square 1, 123182 Moscow, Russia
| | - L V Grigorenko
- National Research Centre "Kurchatov Institute," Kurchatov square 1, 123182 Moscow, Russia
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
- National Research Nuclear University "MEPhI," 115409 Moscow, Russia
| | - X Xu
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- II.Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
- School of Physics and Nuclear Energy Engineering, Beihang University, 100191 Beijing, China
| | - L Acosta
- INFN, Laboratori Nazionali del Sud, Via S. Sofía, 95123 Catania, Italy
- Instituto de Física, Universidad Nacional Autónoma de México, México, D.F. 01000, Mexico
| | | | - A A Ciemny
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - W Dominik
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - J Duénas-Díaz
- Department of Applied Physics, University of Huelva, 21071 Huelva, Spain
| | - V Dunin
- Veksler and Baldin Laboratory of High Energy Physics, JINR, 141980 Dubna, Russia
| | - J M Espino
- Department of Atomic, Molecular and Nuclear Physics, University of Seville, 41012 Seville, Spain
| | - A Estradé
- University of Edinburgh, EH1 1HT Edinburgh, United Kingdom
| | - F Farinon
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - A Fomichev
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - H Geissel
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- II.Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - T A Golubkova
- Advanced Educational and Scientific Center, Moscow State University, 121357 Moscow, Russia
| | - A Gorshkov
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - Z Janas
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - G Kamiński
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
- Institute of Nuclear Physics PAN, 31-342 Kraków, Poland
| | - O Kiselev
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - R Knöbel
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- II.Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - S Krupko
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - M Kuich
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
- Faculty of Physics, Warsaw University of Technology, 00-662 Warszawa, Poland
| | - Yu A Litvinov
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - G Marquinez-Durán
- Department of Applied Physics, University of Huelva, 21071 Huelva, Spain
| | - I Martel
- Department of Applied Physics, University of Huelva, 21071 Huelva, Spain
| | - C Mazzocchi
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - C Nociforo
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - A K Ordúz
- Department of Applied Physics, University of Huelva, 21071 Huelva, Spain
| | - M Pfützner
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - S Pietri
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - M Pomorski
- Faculty of Physics, University of Warsaw, 02-093 Warszawa, Poland
| | - A Prochazka
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - S Rymzhanova
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | | | - C Scheidenberger
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- II.Physikalisches Institut, Justus-Liebig-Universität, 35392 Gießen, Germany
| | - P Sharov
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - H Simon
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - B Sitar
- Faculty of Mathematics and Physics, Comenius University, 84248 Bratislava, Slovakia
| | - R Slepnev
- Flerov Laboratory of Nuclear Reactions, JINR, 141980 Dubna, Russia
| | - M Stanoiu
- IFIN-HH, Post Office Box MG-6, Bucharest, Romania
| | - P Strmen
- Faculty of Mathematics and Physics, Comenius University, 84248 Bratislava, Slovakia
| | - I Szarka
- Faculty of Mathematics and Physics, Comenius University, 84248 Bratislava, Slovakia
| | - M Takechi
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - Y K Tanaka
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
- University of Tokyo, 113-0033 Tokyo, Japan
| | - H Weick
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - M Winkler
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - J S Winfield
- GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
| | - M V Zhukov
- Fundamental Physics, Chalmers University of Technology, S-41296 Göteborg, Sweden
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Scheidenberger C, Gales S, Geissel H, Simon H, Tanihata I, Winkler M. Unique separator-spectrometer experiments at the frontiers of nuclear physics: the Super-FRS scientific program. EPJ WEB OF CONFERENCES 2014. [DOI: 10.1051/epjconf/20146611034] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/14/2022] Open
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7
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Grigorenko LV, Mukha IG, Zhukov MV. Lifetime and fragment correlations for the two-neutron decay of 26O ground state. PHYSICAL REVIEW LETTERS 2013; 111:042501. [PMID: 23931359 DOI: 10.1103/physrevlett.111.042501] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/16/2013] [Indexed: 06/02/2023]
Abstract
The structure and decay of 26O are investigated in a three-body 24O+n+n model suitable for studies of the long-lived (including radioactivity time scale) states. We have found extremely strong effects of the subbarrier configuration mixing on the decay width of true 2n emitters due to core recoil and neutron-neutron final state interaction. This effect far exceeds the analogous effect in the true 2p emitters. Our calculations provide reasonably narrow boundaries for the lifetime vs decay energy dependence for the true 2n emission. An upper limit of ∼1 keV for the decay energy of the unbound 26O is inferred based on the recent experimental lifetime value.
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Affiliation(s)
- L V Grigorenko
- Flerov Laboratory of Nuclear Reactions, JINR, Dubna RU-141980, Russia
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8
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Olsen E, Pfützner M, Birge N, Brown M, Nazarewicz W, Perhac A. Landscape of two-proton radioactivity. PHYSICAL REVIEW LETTERS 2013; 110:222501. [PMID: 23767715 DOI: 10.1103/physrevlett.110.222501] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/04/2013] [Indexed: 06/02/2023]
Abstract
Ground-state two-proton (2p) radioactivity is a decay mode found in isotopes of elements with even atomic numbers located beyond the two-proton drip line. So far, this exotic process has been experimentally observed in a few light- and medium-mass nuclides with Z≤30. In this study, using state-of-the-art nuclear density functional theory, we globally analyze 2p radioactivity and for the first time identify 2p-decay candidates in elements heavier than strontium. We predict a few cases where the competition between 2p emission and α decay may be observed. In nuclei above lead, the α-decay mode is found to be dominating and no measurable candidates for the 2p radioactivity are expected.
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Affiliation(s)
- E Olsen
- Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
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9
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Kohley Z, Baumann T, Bazin D, Christian G, DeYoung PA, Finck JE, Frank N, Jones M, Lunderberg E, Luther B, Mosby S, Nagi T, Smith JK, Snyder J, Spyrou A, Thoennessen M. Study of two-neutron radioactivity in the decay of 26O. PHYSICAL REVIEW LETTERS 2013; 110:152501. [PMID: 25167255 DOI: 10.1103/physrevlett.110.152501] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/10/2012] [Indexed: 06/03/2023]
Abstract
A new technique was developed to measure the lifetimes of neutron unbound nuclei in the picosecond range. The decay of 26O→24O+n+n was examined as it had been predicted to have an appreciable lifetime due to the unique structure of the neutron-rich oxygen isotopes. The half-life of 26O was extracted as 4.5(-1.5)(+1.1)(stat)±3(syst) ps. This corresponds to 26O having a finite lifetime at an 82% confidence level and, thus, suggests the possibility of two-neutron radioactivity.
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Affiliation(s)
- Z Kohley
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
| | - T Baumann
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - D Bazin
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - G Christian
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - P A DeYoung
- Department of Physics, Hope College, Holland, Michigan 49423, USA
| | - J E Finck
- Department of Physics, Central Michigan University, Mount Pleasant, Michigan 48859, USA
| | - N Frank
- Department of Physics and Astronomy, Augustana College, Rock Island, Illinois 61201, USA
| | - M Jones
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - E Lunderberg
- Department of Physics, Hope College, Holland, Michigan 49423, USA
| | - B Luther
- Department of Physics, Concordia College, Moorhead, Minnesota 56562, USA
| | - S Mosby
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - T Nagi
- Department of Physics, Hope College, Holland, Michigan 49423, USA
| | - J K Smith
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - J Snyder
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - A Spyrou
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
| | - M Thoennessen
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
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10
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Raciti G, Cardella G, De Napoli M, Rapisarda E, Amorini F, Sfienti C. Experimental evidence of (2)He decay from (18)Ne excited states. PHYSICAL REVIEW LETTERS 2008; 100:192503. [PMID: 18518446 DOI: 10.1103/physrevlett.100.192503] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/21/2007] [Indexed: 05/26/2023]
Abstract
Two-proton decay from (18)Ne excited states has been studied by complete kinematical reconstruction of the decay products. The (18)Ne nucleus has been produced as a radioactive beam by (20)Ne primary projectile fragmentation at 45 AMeV incident energy on a Be target. The (18)Ne at 33 AMeV incident energy has been excited via Coulomb excitation on a (nat)Pb target. The obtained results unambiguously show that the 6.15 MeV (18)Ne state two-proton decay proceeds through a (2)He diproton resonance (31%) and democratic or virtual sequential decay (69%). The quoted branching ratio has been deduced from relative angle and momentum correlations of the emitted proton pairs.
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Affiliation(s)
- G Raciti
- Dipartimento di Fisica e Astronomia, Università di Catania, Catania, Italy.
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