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Sommer F, König K, Rossi DM, Everett N, Garand D, de Groote RP, Holt JD, Imgram P, Incorvati A, Kalman C, Klose A, Lantis J, Liu Y, Miller AJ, Minamisono K, Miyagi T, Nazarewicz W, Nörtershäuser W, Pineda SV, Powel R, Reinhard PG, Renth L, Romero-Romero E, Roth R, Schwenk A, Sumithrarachchi C, Teigelhöfer A. Charge Radii of ^{55,56}Ni Reveal a Surprisingly Similar Behavior at N=28 in Ca and Ni Isotopes. PHYSICAL REVIEW LETTERS 2022; 129:132501. [PMID: 36206412 DOI: 10.1103/physrevlett.129.132501] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/28/2022] [Revised: 06/17/2022] [Accepted: 08/09/2022] [Indexed: 06/16/2023]
Abstract
Nuclear charge radii of ^{55,56}Ni were measured by collinear laser spectroscopy. The obtained information completes the behavior of the charge radii at the shell closure of the doubly magic nucleus ^{56}Ni. The trend of charge radii across the shell closures in calcium and nickel is surprisingly similar despite the fact that the ^{56}Ni core is supposed to be much softer than the ^{48}Ca core. The very low magnetic moment μ(^{55}Ni)=-1.108(20) μ_{N} indicates the impact of M1 excitations between spin-orbit partners across the N,Z=28 shell gaps. Our charge-radii results are compared to ab initio and nuclear density functional theory calculations, showing good agreement within theoretical uncertainties.
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Affiliation(s)
- Felix Sommer
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - Kristian König
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - Dominic M Rossi
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstr. 1, 64291 Darmstadt, Germany
| | - Nathan Everett
- 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
| | - David Garand
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
| | - Ruben P de Groote
- Department of Physics, University of Jyväskylä, Survontie 9, Jyväskylä FI-40014, Finland
| | - Jason D Holt
- TRIUMF 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, Canada
- Department of Physics, McGill University, Montréal, Québec H3A 2T8, Canada
| | - Phillip Imgram
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - Anthony Incorvati
- 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
| | - Colton Kalman
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
| | - Andrew Klose
- Department of Chemistry, Augustana University, Sioux Falls, South Dakota 57197, USA
| | - Jeremy Lantis
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
| | - Yuan Liu
- Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - Andrew J Miller
- 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
| | - Kei Minamisono
- 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
| | - Takayuki Miyagi
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
- TRIUMF 4004 Wesbrook Mall, Vancouver, British Columbia V6T 2A3, Canada
- ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, D-64291 Darmstadt, Germany
| | - Witold Nazarewicz
- Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
- Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA
| | - Wilfried Nörtershäuser
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
- Helmholtz Research Academy Hesse for FAIR, Campus Darmstadt, 64289 Darmstadt, Germany
| | - Skyy V Pineda
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
- Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA
| | - Robert Powel
- 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
| | - Paul-Gerhard Reinhard
- Institut für Theoretische Physik II, Universität Erlangen-Nürnberg, 91058 Erlangen, Germany
| | - Laura Renth
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
| | - Elisa Romero-Romero
- Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
- Department of Physics and Astronomy, University of Tennessee, Knoxville, Knoxville, Tennessee 37996, USA
| | - Robert Roth
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
- Helmholtz Research Academy Hesse for FAIR, Campus Darmstadt, 64289 Darmstadt, Germany
| | - Achim Schwenk
- Institut für Kernphysik, Technische Universität Darmstadt, 64289 Darmstadt, Germany
- ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung GmbH, D-64291 Darmstadt, Germany
- Max-Planck-Institut für Kernphysik, D-69117 Heidelberg, Germany
| | - Chandana Sumithrarachchi
- National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
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Monrozeau C, Khan E, Blumenfeld Y, Demonchy CE, Mittig W, Roussel-Chomaz P, Beaumel D, Caamaño M, Cortina-Gil D, Ebran JP, Frascaria N, Garg U, Gelin M, Gillibert A, Gupta D, Keeley N, Maréchal F, Obertelli A, Scarpaci JA. First measurement of the giant monopole and quadrupole resonances in a short-lived nucleus: 56Ni. PHYSICAL REVIEW LETTERS 2008; 100:042501. [PMID: 18352262 DOI: 10.1103/physrevlett.100.042501] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/19/2007] [Indexed: 05/26/2023]
Abstract
The isoscalar giant monopole resonance (GMR) and giant quadrupole resonance (GQR) have been measured in the 56Ni unstable nucleus by inducing the 56Ni(d,d') reaction at 50A MeV in the Maya active target at the GANIL facility. The GMR and GQR centroids are measured at 19.3+/-0.5 MeV and 16.2+/-0.5 MeV, respectively. The corresponding angular distributions are extracted from 3 degrees to 7 degrees . A multipole decomposition analysis using distorted wave Born approximation with random phase approximation transition densities shows that both the GMR and the GQR exhaust a large fraction of the energy-weighted sum rule. The demonstration of this new method opens a broad range of giant resonance studies at intermediate-energy radioactive beam facilities.
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Affiliation(s)
- C Monrozeau
- Institut de Physique Nucléaire IN2P3/CNRS, Université Paris Sud, 91406 Orsay Cedex, France
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5
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Becheva E, Blumenfeld Y, Khan E, Beaumel D, Daugas JM, Delaunay F, Demonchy CE, Drouart A, Fallot M, Gillibert A, Giot L, Grasso M, Keeley N, Kemper KW, Khoa DT, Lapoux V, Lima V, Musumarra A, Nalpas L, Pollacco EC, Roig O, Roussel-Chomaz P, Sauvestre JE, Scarpaci JA, Skaza F, Than HS. N = 14 shell closure in 22O viewed through a neutron sensitive probe. PHYSICAL REVIEW LETTERS 2006; 96:012501. [PMID: 16486448 DOI: 10.1103/physrevlett.96.012501] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/28/2005] [Indexed: 05/06/2023]
Abstract
To investigate the behavior of the N = 14 neutron gap far from stability with a neutron-sensitive probe, proton elastic and 2(1)+ inelastic scattering angular distributions for the neutron-rich nucleus 22O were measured using the MUr à STrip detector array at the Grand Accélérateur National d'Ions Lourds facility. A deformation parameter beta(p,p') = 0.26 +/- 0.04 is obtained for the 2(1)+ state, much lower than in 20O, showing a weak neutron contribution to this state. A microscopic analysis was performed using matter and transition densities generated by continuum Skyrme-Hartree-Fock-Bogoliubov and quasiparticle random phase approximation calculations, respectively. The ratio of neutron to proton contributions to the 2(1)+ state is found close to the N/Z ratio, demonstrating a strong N = 14 shell closure in the vicinity of the neutron drip line.
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Affiliation(s)
- E Becheva
- Institut de Physique Nucléaire, IN2P3-CNRS, 91406 Orsay, France
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6
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Sorlin O, Leenhardt S, Donzaud C, Duprat J, Azaiez F, Nowacki F, Grawe H, Dombrádi Z, Amorini F, Astier A, Baiborodin D, Belleguic M, Borcea C, Bourgeois C, Cullen DM, Dlouhy Z, Dragulescu E, Górska M, Grévy S, Guillemaud-Mueller D, Hagemann G, Herskind B, Kiener J, Lemmon R, Lewitowicz M, Lukyanov SM, Mayet P, de Oliveira Santos F, Pantalica D, Penionzhkevich YE, Pougheon F, Poves A, Redon N, Saint-Laurent MG, Scarpaci JA, Sletten G, Stanoiu M, Tarasov O, Theisen C. (68)(28)Ni(40): Magicity versus superfluidity. PHYSICAL REVIEW LETTERS 2002; 88:092501. [PMID: 11863997 DOI: 10.1103/physrevlett.88.092501] [Citation(s) in RCA: 6] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/21/2000] [Revised: 11/15/2001] [Indexed: 05/23/2023]
Abstract
The neutron-rich (66,68)Ni have been produced at GANIL via interactions of a 65.9A MeV 70Zn beam with a 58Ni target. Their reduced transition probability B(E2;0(+)(1)-->2+) has been measured for the first time by Coulomb excitation in a (208)Pb target at intermediate energy. The B(E2) value for (68)Ni(40) is unexpectedly small. An analysis in terms of large scale shell model calculations stresses the importance of proton core excitations to reproduce the B(E2) values and indicates the erosion of the N = 40 harmonic-oscillator subshell by neutron-pair scattering.
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Affiliation(s)
- O Sorlin
- Institut de Physique Nucléaire, IN2P3-CNRS, F-91406 Orsay Cedex, France
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10
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Lipoglavsek M, Cederkäll J, Palacz M, Persson J, Atac-under-dot A, Blomqvist J, Fahlander C, Grawe H, Johnson A, Kerek A, Klamra W, Kownacki J, Likar A, Norlin L, Nyberg J, Schubart R, Seweryniak D, Bednarczyk P, Dombrádi Z, Foltescu D, Jerrestam D, Juutinen S, Mäkelä E, Perez G, Roth HA, Shizuma T, Skeppstedt Ö, Sletten G, Törmänen S, Vass T. Stability of 10050Sn50 deduced from excited states in 9948Cd51. PHYSICAL REVIEW LETTERS 1996; 76:888-891. [PMID: 10061577 DOI: 10.1103/physrevlett.76.888] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.0] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/23/2023]
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