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NSR database version of April 25, 2024.

Search: Author = L.Grente

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2022CH38      Phys.Rev. C 106, 024618 (2022)

A.Chatillon, J.Taieb, A.Heinz, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Influence of proton and neutron deformed shells on the asymmetric fission of thorium isotopes

NUCLEAR REACTIONS ^{222,223,225,226,229,230}Th, ^{228,229,231,232}Pa, ^234,235,238U, ²³⁸Np(γ, F), E=13-14 MeV; ^219,223,227Ac(γ, F), E ≈ 16 MeV; analyzed elemental, isotonic, and isobaric experimental fission fragment yields in Coulex experiments obtained at R3B/SOFIA setups (2019CH20); deduced average value of the atomic number of the light and heavy fission fragments, centroid positions of the light and heavy peaks of the isotonic yields, average total prompt-neutron multiplicity. Discussed the influence of deformed neutron and proton shells on the fission process.

doi: 10.1103/PhysRevC.106.024618
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2021MA68      Phys.Rev. C 104, 044602 (2021)

J.-F.Martin, J.Taieb, G.Boutoux, A.Chatillon, T.Gorbinet, E.Pellereau, L.Audouin, A.Heinz, H.Alvarez-Pol, Y.Ayyad, G.Belier, J.Benlliure, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, L.Grente, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, C.Nociforo, C.Paradela, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Fission-fragment yields and prompt-neutron multiplicity for Coulomb-induced fission of ^{234, 235}U and ^{237, 238}Np

NUCLEAR REACTIONS ²³⁸U(²³⁴U, F), (²³⁵U, F), (²³⁷Np, F), (²³⁸Np, F), E=555 MeV/nucleon in the center of the target, [secondary ^234,235U, ^237,238Np beams from ⁹Be(²³⁸U, X), E=1 GeV/nucleon primary reaction, followed by separation of reaction products using FRS separator at GSI facility]; measured fission fragments, (fragment)(fragment)-coin, Coulomb excitation induced fission σ(A, Z), electromagnetic-induced fission yields, mass and charge distribution of fission fragments, isotonic, isobaric, and isotopic fission yields produced for Coulomb-induced fission using the Reactions with Relativistic Radioactive Beams/Studies On FIssion with Aladin (R3B/SOFIA) apparatus at GSI facility. ^234,235,238U, ^237,238Np(γ, F), virtual photons from Coulomb excitation; deduced yields Y(A, Z), σ(A, Z), prompt-neutron and total neutron multiplicities ν(A, Z) for A=77-157, Z=28-64, and N=45-97 fragments: ^{77,78,79,80,81,82,83,84}Ge, ^{78,79,80,81,82,83,84,85,86,87}As, ^{80,81,82,83,84,85,86,87,88,89}Se, ^{83,84,85,86,87,88,89,90,91}Br, ^{85,86,87,88,89,90,91,92,93}Kr, ^{87,88,89,90,91,92,93,94,95,96}Rb, ^{90,91,92,93,94,95,96,97,98}Sr, ^{92,93,94,95,96,97,98,99,100,101}Y, ^{95,96,97,98,99,100,101,102,103}Zr, ^{97,98,99,100,101,102,103,104,105,106}Nb, ^{100,101,102,103,104,105,106,107,108}Mo, ^{103,104,105,106,107,108,109,110,111}Tc, ^{102,103,104,105,106,107,108,109,110,111,112,113,114}Ru, ^{108,109,110,111,112,113,114,115,116,117}Rh, ^{110,111,112,113,114,115,116,117,118,119,120}Pd, ^{113,114,115,116,117,118,119,120,121,122}Ag, ^{115,116,117,118,119,120,121,122,123,124,125,126}Cd, ^{118,119,120,121,122,123,124,125,126,127,128,129}In, ^{121,122,123,124,125,126,127,128,129,130,131,132,133}Sn, ^{124,125,126,127,128,129,130,131,132,133,134,135}Sb, ^{127,128,129,130,131,132,133,134,135,136,137}Te, ^{130,131,132,133,134,135,136,137,138,139,140}I, ^{132,133,134,135,136,137,138,139,140,141,142}Xe, ^{135,136,137,138,139,140,141,142,143,144}Cs, ^{137,138,139,140,141,142,143,144,145,146,147}Ba, ^{139,140,141,142,143,144,145,146,147,148,149,150}La, ^{142,143,144,145,146,147,148,149,150,151,152}Ce, ^{144,145,146,147,148,149,150,151,152,153,154}Pr, ^{146,147,148,149,150,151,152,153,154,155,156,157}Nd, ^{151,152,153,154,155,156}, and ¹⁵⁷Pm, average values of atomic, neutron, and mass numbers for the light and heavy fission fragments, proton even-odd staggering, neutron excess of pre-neutron-evaporation fission fragments produced for Coulomb-induced fission. Comparison with previous measurements using (γ, F) and thermal-neutron induced fission. Comparison with theoretical reaction model calculations using GEF-2019V1.1 code, unchanged charge density (UCD) approach, and by fission treated as an adiabatic process in a Fermi gas (FA). Numerical values of yields, cross sections and neutron multiplicities are listed in the Supplemental Material of this work.

doi: 10.1103/PhysRevC.104.044602
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2020CH18      Phys.Rev.Lett. 124, 202502 (2020)

A.Chatillon, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, D.Rossi, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Evidence for a New Compact Symmetric Fission Mode in Light Thorium Isotopes

NUCLEAR REACTIONS ^222,226,230Th(γ, F)¹NN, E not given; measured reaction products, En, In; deduced prompt-neutron emission probability, σ(E), yields.

doi: 10.1103/PhysRevLett.124.202502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0076.

2019CH20      Phys.Rev. C 99, 054628 (2019)

A.Chatillon, J.Taieb, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.T.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, E.Pellereau, S.Pietri, A.Prochazka, J.L.Rodriguez-Sanchez, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Experimental study of nuclear fission along the thorium isotopic chain: From asymmetric to symmetric fission

NUCLEAR REACTIONS ²⁰⁸Pb, ²³⁸U(²¹⁹Ac, F), (²²⁰Ac, F), (²²³Ac, F), (²²⁷Ac, F), (²²¹Th, F), (²²²Th, F), (²²³Th, F), (²²⁵Th, F), (²²⁶Th, F), (²²⁹Th, F), (²³⁰Th, F), (²²⁸Pa, F), (²²⁹Pa, F), (²¹⁹Ac, F), (²²⁰Ac, F), (²²³Ac, F), (²²⁷Ac, F), (²²¹Th, F), (²²²Th, F), (²²³Th, F), (²²⁵Th, F), (²²⁶Th, F), (²²⁹Th, F), (²³⁰Th, F), (²²⁸Pa, F), (²²⁹Pa, F), E=551.7-568.9 MeV/nucleon, [secondary Ac and Th beams from ⁹Be(²³⁸U, X), E=1 GeV/nucleon primary reaction, and using FRS separator at GSI facility for separation of reaction products]; measured fission fragments, (fragment)(fragment)-coin, Coulomb excitation induced fission σ, differential Coulomb excitation σ(θ), electromagnetic-induced fission yields, mass and charge distribution of fission fragments, isotonic and isobaric fission yields using the Reactions with Relativistic Radioactive Beams/Studies On FIssion with Aladin (R3B/SOFIA) apparatus at GSI accelerator facility. Comparison with local even-odd staggering, previous measurements using either the same reaction mechanism and/or thermal-neutron induced fission.

doi: 10.1103/PhysRevC.99.054628
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0074.

2019GO20      Phys.Rev. C 100, 034302 (2019)

A.Goasduff, J.Ljungvall, T.R.Rodriguez, F.L.Bello Garrote, A.Etile, G.Georgiev, F.Giacoppo, L.Grente, M.Klintefjord, A.Kusoglu, I.Matea, S.Roccia, M.-D.Salsac, C.Sotty

B(E2) anomalies in the yrast band of ¹⁷⁰Os

NUCLEAR REACTIONS ¹⁴²Nd(³²S, 4n)¹⁷⁰Os, E=170 MeV; measured Eγ, Iγ, γγ-coin, half-lives of the first 2+ and 4+ levels by recoil-distance Doppler-shift (RDDS) method using the Orsay universal plunger system, enriched target and ORGAM germanium detector array with ten Compton-suppressed HPGe detectors at the ALTO facility of IPN, Orsay. ¹⁷⁰Os; deduced levels, B(E2). Comparison with state-of-the-art beyond-mean-field calculations.

NUCLEAR STRUCTURE ^{162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198}Os; calculated energies of the first 2+ and 4+ levels and their ratios, B(E2) for the first 2+ and 4+ states for ^168,170,172Os, and PN-VAP potential energy surfaces for g.s., first 2+ and 4+ states in ¹⁷⁰Os. Symmetry conserving configuration mixing (SCCM) calculations using the generator coordinate method (GCM) framework with Hartree-Fock-Bogoliubov states from variation after particle number projection (PN-VAP). Comparison with available experimental data.

doi: 10.1103/PhysRevC.100.034302
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Data from this article have been entered in the XUNDL database. For more information, click here.

2018HA16      Eur.Phys.J. A 54, 50 (2018)

T.W.Hagen, A.Gorgen, W.Korten, L.Grente, M.-D.Salsac, F.Farget, T.Braunroth, B.Bruyneel, I.Celikovic, E.Clement, G.de France, O.Delaune, A.Dewald, A.Dijon, M.Hackstein, B.Jacquot, J.Litzinger, J.Ljungvall, C.Louchart, C.Michelagnoli, D.R.Napoli, F.Recchia, W.Rother, E.Sahin, S.Siem, B.Sulignano, Ch.Theisen, J.J.Valiente-Dobon

Lifetimes of excited states in triaxially deformed ¹⁰⁷Tc and ^{109, 111, 113}Rh

NUCLEAR REACTIONS ⁹B(²³⁸U, F), E=6.2 MeV/nucleon; measured reaction products. ¹⁰⁷Tc, ^109,111,113Rh; measured prompt Eγ, Iγ, γγ-coin using EXOGAM Ge detector array, (ion)γ-coin; deduced T_1/2, positive-parity yrast bands using Recoil-Distance Doppler Shift (RDDS) method; calculated yrast bands states T_1/2 using triaxial particle-rotor method; deduced configuration for the strongest positive-parity band in ¹⁰⁷Tc, indicated gradual increase of triaxial deformation with atomic number Z, reaching almost maximum triaxiality for neutron-rich Rh nuclei. T_1/2 compared to data.

doi: 10.1140/epja/i2018-12482-9
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Data from this article have been entered in the XUNDL database. For more information, click here.

2018SI26      Phys.Rev.Lett. 121, 192501 (2018)

P.Singh, W.Korten, T.W.Hagen, A.Gorgen, L.Grente, M.-D.Salsac, F.Farget, E.Clement, G.de France, T.Braunroth, B.Bruyneel, I.Celikovic, O.Delaune, A.Dewald, A.Dijon, J.-P.Delaroche, M.Girod, M.Hackstein, B.Jacquot, J.Libert, J.Litzinger, J.Ljungvall, C.Louchart, A.Gottardo, C.Michelagnoli, C.Muller-Gatermann, D.R.Napoli, T.Otsuka, N.Pillet, F.Recchia, W.Rother, E.Sahin, S.Siem, B.Sulignano, T.Togashi, Y.Tsunoda, Ch.Theisen, J.J.Valiente-Dobon

Evidence for Coexisting Shapes through Lifetime Measurements in ⁹⁸Zr

NUCLEAR REACTIONS ⁹Be(²³⁸U, X)⁹⁸Zr, E=6.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced level lifetimes, B(E2) values. Comparison with available data. Recoil-distance Doppler shift method.

doi: 10.1103/PhysRevLett.121.192501
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Data from this article have been entered in the XUNDL database. For more information, click here.

2017HA12      Phys.Rev. C 95, 034302 (2017)

T.W.Hagen, A.Gorgen, W.Korten, L.Grente, M.-D.Salsac, F.Farget, I.Ragnarsson, T.Braunroth, B.Bruyneel, I.Celikovic, E.Clement, G.de France, O.Delaune, A.Dewald, A.Dijon, M.Hackstein, B.Jacquot, J.Litzinger, J.Ljungvall, C.Louchart, C.Michelagnoli, D.R.Napoli, F.Recchia, W.Rother, E.Sahin, S.Siem, B.Sulignano, Ch.Theisen, J.J.Valiente-Dobon

Evolution of nuclear shapes in odd-mass yttrium and niobium isotopes from lifetime measurements following fission reactions

NUCLEAR REACTIONS ⁹Be(²³⁸U, F)⁹²Y/⁹³Y/⁹⁴Y/⁹⁵Y/⁹⁶Y/⁹⁷Y/⁹⁸Y/⁹⁹Y/¹⁰⁰Y/¹⁰¹Y/¹⁰²Y/¹⁰³Y/⁹⁷Nb/⁹⁸Nb/⁹⁹Nb/¹⁰⁰Nb/¹⁰¹Nb/¹⁰²Nb/¹⁰³Nb/¹⁰⁴Nb/¹⁰⁵Nb/¹⁰⁶Nb/¹⁰⁷Nb/¹⁰⁸Nb, E=6.2 MeV/nucleon; measured energy loss ΔE versus the total energy, mass versus mass-to-charge ratio, mass distributions of fission fragments, Eγ, Iγ, (fission fragment)γ-coin, level half-lives by recoil-distance Doppler-shift (RDDS) method using VAMOS++ spectrometer and EXOGAM array at GANIL facility. ^99,101Y, ^{101,103,105,107}Nb; deduced high-spin levels, J, π, rotational bands, configurations, B(M1), B(E2). Comparison with triaxial particle-rotor calculations.

doi: 10.1103/PhysRevC.95.034302
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Data from this article have been entered in the XUNDL database. For more information, click here.

2017JO07      Phys.Rev. C 95, 064321 (2017)

P.R.John, J.J.Valiente-Dobon, D.Mengoni, V.Modamio, S.Lunardi, D.Bazzacco, A.Gadea, C.Wheldon, T.R.Rodriguez, T.Alexander, G.de Angelis, N.Ashwood, M.Barr, G.Benzoni, B.Birkenbach, P.G.Bizzeti, A.M.Bizzeti-Sona, S.Bottoni, M.Bowry, A.Bracco, F.Browne, M.Bunce, F.Camera, L.Corradi, F.C.L.Crespi, B.Melon, E.Farnea, E.Fioretto, A.Gottardo, L.Grente, H.Hess, Tz.Kokalova, W.Korten, A.Kusoglu, S.Lenzi, S.Leoni, J.Ljungvall, R.Menegazzo, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, D.R.Napoli, Zs.Podolyak, G.Pollarolo, F.Recchia, P.Reiter, O.J.Roberts, E.Sahin, M.-D.Salsac, F.Scarlassara, M.Sferrazza, P.-A.Soderstrom, A.M.Stefanini, S.Szilner, C.A.Ur, A.Vogt, J.Walshe

In-beam γ-ray spectroscopy of the neutron-rich platinum isotope ²⁰⁰Pt toward the N=126 shell gap

NUCLEAR REACTIONS ¹⁹⁸Pt(⁸²Se, ⁸⁰Se)²⁰⁰Pt, E=426 MeV; measured Eγ, Iγ, (⁸⁰Se recoils)γγ-coin using PRISMA spectrometer for ⁸⁰Se recoils and AGATA array for Doppler-corrected γ rays at XTU Tandem-ALPI accelerator of LNL-Legnaro facility. ²⁰⁰Pt; deduced levels, J, π, ground-state band, structure above the 17-ns, 7- isomer. Comparison with theoretical model calculations.

NUCLEAR STRUCTURE ^{190,192,194,196,198,200,202,204}Pt; calculated particle-number-projected potential energy surfaces in (β₂, γ) plane, yrast band excitation energies. Beyond mean-field, symmetry-conserving configuration-mixing (SCCM) calculations based on Gogny D1S energy density functionals. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.064321
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Data from this article have been entered in the XUNDL database. For more information, click here.

2017PE08      Phys.Rev. C 95, 054603 (2017)

E.Pellereau, J.Taieb, A.Chatillon, H.Alvarez-Pol, L.Audouin, Y.Ayyad, G.Belier, J.Benlliure, G.Boutoux, M.Caamano, E.Casarejos, D.Cortina-Gil, A.Ebran, F.Farget, B.Fernandez-Dominguez, T.Gorbinet, L.Grente, A.Heinz, H.Johansson, B.Jurado, A.Kelic-Heil, N.Kurz, B.Laurent, J.-F.Martin, C.Nociforo, C.Paradela, S.Pietri, J.L.Rodriguez-Sanchez, K.-H.Schmidt, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Accurate isotopic fission yields of electromagnetically induced fission of ²³⁸U measured in inverse kinematics at relativistic energies

NUCLEAR REACTIONS ²³⁸U(²³⁸U, F), E=650 MeV/nucleon; measured mass and charge coincidences, elemental, isobaric and isotopic yields and mass distribution of fission fragments of Z=29-62, N=43-95, A=71-156 in ²³⁸U(γ, F) using the SOFIA experimental setup and around the ALADIN magnet at GSI. Comparison with the GEF model calculations, and with ²³⁸U(n, F) data in ENDF-BVII.1 and JEFF.3.1.

doi: 10.1103/PhysRevC.95.054603
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0077.

2016HA04      Acta Phys.Pol. B47, 903 (2016)

T.W.Hagen, L.Grente, A.Gorgen, M.-D.Salsac, W.Korten, F.Farget, T.Braunroth, B.Bruyneel, I.Celikovic, E.Clement, G.de France, O.Delaune, A.Dewald, A.Dijon, M.Hackstein, B.Jacquot, J.Litzinger, J.Ljungvall, C.Louchart, C.Michelagnoli, D.R.Napoli, A.Navin, F.Recchia, M.Rejmund, W.Rother, E.Sahin, S.Siem, B.Sulignano, Ch.Theisen, J.J.Valiente-Dobon

Lifetime Measurements of Excited States in Neutron-rich Fission Fragments

RADIOACTIVITY ²⁴⁷Cm(SF) [ from ⁹Be(²³⁸U, X)²⁴⁷Cm, E=6.2 MeV/nucleon]; measured decay products, Eγ, Iγ. ⁹⁹Y; deduced energy levels, J, π.

doi: 10.5506/APhysPolB.47.903
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2015MA70      Eur.Phys.J. A 51, 174 (2015)

J.-F.Martin, J.Taieb, A.Chatillon, G.Belier, G.Boutoux, A.Ebran, T.Gorbinet, L.Grente, B.Laurent, E.Pellereau, H.Alvarez-Pol, L.Audouin, T.Aumann, Y.Ayyad, J.Benlliure, E.Casarejos, D.Cortina Gil, M.Caamano, F.Farget, B.Fernandez-Dominguez, A.Heinz, B.Jurado, A.Kelic-Heil, N.Kurz, C.Nociforo, C.Paradela, S.Pietri, D.Ramos, J.-L.Rodriguez-Sanchez, C.Rodriguez-Tajes, D.Rossi, K.-H.Schmidt, H.Simon, L.Tassan-Got, J.Vargas, B.Voss, H.Weick

Studies on fission with ALADIN - Precise and simultaneous measurement of fission yields, total kinetic energy and total prompt neutron multiplicity at GSI

doi: 10.1140/epja/i2015-15174-0
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2014JO05      Phys.Rev. C 90, 021301 (2014)

P.R.John, V.Modamio, J.J.Valiente-Dobon, D.Mengoni, S.Lunardi, T.R.Rodriguez, D.Bazzacco, A.Gadea, C.Wheldon, T.Alexander, G.de Angelis, N.Ashwood, M.Barr, G.Benzoni, B.Birkenbach, P.G.Bizzeti, A.M.Bizzeti-Sona, S.Bottoni, M.Bowry, A.Bracco, F.Browne, M.Bunce, F.Camera, B.Cederwall, L.Corradi, F.C.L.Crespi, P.Desesquelles, J.Eberth, E.Farnea, E.Fioretto, A.Gorgen, A.Gottardo, J.Grebosz, L.Grente, H.Hess, A.Jungclaus, Tz.Kokalova, A.Korichi, W.Korten, A.Kusoglu, S.Lenzi, S.Leoni, J.Ljungvall, G.Maron, W.Meczynski, B.Melon, R.Menegazzo, C.Michelagnoli, T.Mijatovic, B.Million, P.Molini, G.Montagnoli, D.Montanari, D.R.Napoli, P.Nolan, C.Oziol, Zs.Podolyak, G.Pollarolo, A.Pullia, B.Quintana, F.Recchia, P.Reiter, O.J.Roberts, D.Rosso, E.Sahin, M.-D.Salsac, F.Scarlassara, M.Sferrazza, J.Simpson, P.-A.Soderstrom, A.M.Stefanini, O.Stezowski, S.Szilner, Ch.Theisen, C.A.Ur, J.Walshe

Shape evolution in the neutron-rich osmium isotopes: Prompt γ-ray spectroscopy of ¹⁹⁶Os

NUCLEAR REACTIONS ¹⁹⁸Pt(⁸²Se, X), E=426 MeV; measured Eγ, Iγ, γγ-, (⁸⁴Kr)γ-coin using PRISMA spectrometer for fragments and AGATA array for γ rays at Tandem-ALPI-LNL accelerator facility. ¹⁹⁶Os; deduced levels, J, π, γ-unstable/triaxial rotor yrast band. Comparison with state-of-the-art beyond-mean-field calculations.

NUCLEAR STRUCTURE ^{188,190,192,194,196,198}Os; calculated particle number projected potential energy surfaces in (β₂, γ) plane, level energies in the yrast bands using Gogny D1S interaction. State-of-the-art beyond-meanfield calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.021301
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Data from this article have been entered in the XUNDL database. For more information, click here.