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NSR database version of April 11, 2024.

Search: Author = N.Itaco

Found 85 matches.

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2024CO01      Phys.Rev. C 109, 014301 (2024)

L.Coraggio, N.Itaco, G.De Gregorio, A.Gargano, Z.H.Cheng, Y.Z.Ma, F.R.Xu, M.Viviani

The renormalization of the shell-model Gamow-Teller operator starting from effective field theory for nuclear systems

doi: 10.1103/PhysRevC.109.014301
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2022CO04      Phys.Rev. C 105, 034312 (2022)

L.Coraggio, N.Itaco, G.De Gregorio, A.Gargano, R.Mancino, F.Nowacki

Shell-model calculation of 100Mo double -β decay

NUCLEAR STRUCTURE 100Mo; calculated neutron effective single-particle, proton and neutron single-particle energy spacings, running sum of B(GT) strength up to 3 MeV. 100Mo, 100Ru; calculated levels, J, π, B(E2). Effective shell-model Hamiltonian with realistic nucleon-nucleon potential. Comparison to experimental data.

RADIOACTIVITY 100Mo(2β-); calculated nuclear matrix elements for double β-decay and neutrinoless double β-decay to yrare and yrast 0+ states in 100Ru. Effective shell-model Hamiltonian with realistic nucleon-nucleon potential and decay operators derived within the many-body perturbation theory. Comparison to available experimental data and other theoretical predictions.

doi: 10.1103/PhysRevC.105.034312
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2021CO14      Phys.Rev. C 104, 054304 (2021)

L.Coraggio, G.De Gregorio, A.Gargano, N.Itaco, T.Fukui, Y.Z.Ma, F.R.Xu

Shell-model study of titanium isotopic chain with chiral two- and three-body forces

NUCLEAR STRUCTURE 42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72Ti; calculated S(2n) and compared with AME2020 values, energies of the first 2+ states and compared with experimental values, effective single-particle energies (ESPEs), neutron-neutron monopole matrix elements. Shell-model calculations with an effective Hamiltonian from many-body perturbation theory using 40Ca as a closed core, and three-body contributions through density-dependent two-body matrix elements (TBME) derived within a microscopic approach from chiral forces.

doi: 10.1103/PhysRevC.104.054304
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2021FU11      Few-Body Systems 62, 64 (2021)

T.Fukui, L.Coraggio, G.De Gregorio, A.Gargano, N.Itaco, Y.Ma, F.Xu

Realistic Shell Model with Chiral Interaction and Its Application to Drip-Line Predictions

NUCLEAR STRUCTURE 10B, 42,44,46,48,50,52,54,56,58,60,62,64,66,68,70Ca; calculated energy levels, J, π, two-neutron separation energy. Comparison with experimental data.

doi: 10.1007/s00601-021-01655-8
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2021UR02      Phys.Atomic Nuclei 84, 250 (2021)

B.A.Urazbekov, A.S.Denikin, N.Itaco, D.Janseitov

Application of the 2α+n Three-Body Cluster Model of the 9Be Nucleus in the Reaction 9Be(3He, 3He)9Be

NUCLEAR REACTIONS 9Be(3He, 3He), E=30-60 MeV; calculated σ(θ); deduced optical model parameters. Comparison with experimental data.

doi: 10.1134/S1063778821030145
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2020CO05      Phys.Rev. C 101, 044315 (2020)

L.Coraggio, A.Gargano, N.Itaco, R.Mancino, F.Nowacki

Calculation of the neutrinoless double-β decay matrix element within the realistic shell model

RADIOACTIVITY 48Ca, 76Ge, 82Se, 130Te, 136Xe(2β-); calculated nuclear matrix element, and neutron pair contributions to nuclear matrix element of 0νββ decay using shell model with realistic nucleon-nucleon potential. Comparison with other theoretical calculations.

doi: 10.1103/PhysRevC.101.044315
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2020CO10      Phys.Rev. C 102, 054326 (2020)

L.Coraggio, G.De Gregorio, A.Gargano, N.Itaco, T.Fukui, Y.Z.Ma, F.R.Xu

Shell-model study of calcium isotopes toward their drip line

NUCLEAR STRUCTURE 50Ca; calculated low-lying levels, J, π. 42,44,46,48,50,52,54,56,58,60,62,64,66,68,70Ca; calculated S(2n), energies of first 2+ states. 49Ca; calculated negative-parity, low-spin energy levels. Shell model calculations with two- and three-nucleon potentials derived within the chiral perturbation theory. Calculated two-body matrix elements given in Supplemental material. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.054326
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2020CO16      Universe 6, 233 (2020)

L.Coraggio, N.Itaco, G.De Gregorio, A.Gargano, R.Mancino, S.Pastore

Present Status of Nuclear Shell-Model Calculations of 0νββ Decay Matrix Elements

doi: 10.3390/universe6120233
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2020GO06      Phys.Rev. C 102, 014323 (2020)

A.Gottardo, G.de Angelis, P.Doornenbal, L.Coraggio, A.Gargano, N.Itaco, K.Kaneko, P.Van Isacker, T.Furumoto, G.Benzoni, J.Lee, H.Liu, M.Matsushita, D.Mengoni, V.Modamio-Hoybjor, S.Momiyama, T.Motobayashi, D.R.Napoli, M.Niikura, E.Sahin, Y.Shiga, H.Sakurai, R.Taniuchi, S.Takeuchi, H.Wang, J.J.Valiente-Dobon, R.Avigo, H.Baba, N.Blasi, F.L.Bello Garrote, F.Browne, F.C.L.Crespi, S.Ceruti, R.Daido, M.-C.Delattre, D.Fang, Zs.Dombradi, T.Isobe, I.Kuti, G.Lorusso, K.Matsui, B.Melon, T.Miyazaki, S.Nishimura, R.Orlandi, Z.Patel, S.Rice, L.Sinclair, P.A.Soderstrom, D.Sohler, T.Sumikama, J.Taprogge, Zs.Vajta, H.Watanabe, O.Wieland, J.Wu, Z.Y.Xu, M.Yalcinkaya, R.Yokoyama

Transition strengths in the neutron-rich 73, 74, 75Ni isotopes

NUCLEAR REACTIONS Pb(73Ni, 73Ni'), (74Ni, 74Ni'), (75Ni, 75Ni'), E=215 MeV/nucleon, [secondary cocktail beam from 9Be(238U, F), E=345 MeV/nucleon, and separated by A/Q using the BigRIPS fragment separator at RIBF-RIKEN facility]; measured reaction products identified by the ZeroDegree spectrometer, Eγ, Iγ, (scattered Ni nuclei)γ-coin using the WAS3Abi-EURICA setup with the DALI2 NaI(Tl) array for γ detection. 73,74,75Ni; deduced levels, J, π, B(E2) from Coulomb excitation cross sections. Comparison with large-scale shell model calculations.

doi: 10.1103/PhysRevC.102.014323
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2020GR01      Phys.Rev.Lett. 124, 032502 (2020)

T.J.Gray, J.M.Allmond, A.E.Stuchbery, C.-H.Yu, C.Baktash, A.Gargano, A.Galindo-Uribarri, D.C.Radford, J.C.Batchelder, J.R.Beene, C.R.Bingham, L.Coraggio, A.Covello, M.Danchev, C.J.Gross, P.A.Hausladen, N.Itaco, W.Krolas, J.F.Liang, E.Padilla-Rodal, J.Pavan, D.W.Stracener, R.L.Varner

Early Signal of Emerging Nuclear Collectivity in Neutron-Rich 129Sb

NUCLEAR REACTIONS 50Ti(129Sb, 129Sb'), E=400 MeV; measured reaction products, Eγ, Iγ. 129Sb; deduced γ-ray energies, J, π, B(E2). Comparison with shell model calculations.

doi: 10.1103/PhysRevLett.124.032502
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2020MA33      Phys.Lett. B 808, 135673 (2020)

Y.Z.Ma, F.R.Xu, N.Michel, S.Zhang, J.G.Li, B.S.Hu, L.Coraggio, N.Itaco, A.Gargano

Continuum and three-nucleon force in Borromean system: The 17Ne case

NUCLEAR STRUCTURE 17Ne; analyzed available data; calculated energy levels, J, π, proton-proton and proton-neutron correlation densities.

doi: 10.1016/j.physletb.2020.135673
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2019CO07      Phys.Rev. C 100, 014316 (2019)

L.Coraggio, L.De Angelis, T.Fukui, A.Gargano, N.Itaco, F.Nowacki

Renormalization of the Gamow-Teller operator within the realistic shell model

NUCLEAR STRUCTURE 48Ca, 48Ti, 76Ge, 76,82Se, 82Kr, 130Te, 130,136Xe, 136Ba; calculated levels, B(E2), B(M1), B(GT) strengths, magnetic dipole moments using realistic shell model. Comparison with experimental data.

RADIOACTIVITY 48Ca, 76Ge, 82Se, 82Kr, 130Te, 136Xe(2β-); calculated nuclear matrix elements for 2νββ decay mode.

doi: 10.1103/PhysRevC.100.014316
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2019KA04      Phys.Rev. C 99, 014301 (2019)

L.Kaya, A.Vogt, P.Reiter, C.Muller-Gatermann, A.Gargano, L.Coraggio, N.Itaco, A.Blazhev, K.Arnswald, D.Bazzacco, B.Birkenbach, A.Bracco, B.Bruyneel, L.Corradi, F.C.L.Crespi, G.de Angelis, M.Droste, J.Eberth, E.Farnea, E.Fioretto, C.Fransen, A.Gadea, A.Giaz, A.Gorgen, A.Gottardo, K.Hadynska-Klek, H.Hess, R.Hetzenegger, R.Hirsch, P.R.John, J.Jolie, A.Jungclaus, W.Korten, S.Leoni, L.Lewandowski, S.Lunardi, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, D.Napoli, Zs.Podolyak, G.Pollarolo, F.Recchia, D.Rosiak, N.Saed-Samii, E.Sahin, M.Siciliano, F.Scarlassara, M.Seidlitz, P.-A.Soderstrom, A.M.Stefanini, O.Stezowski, S.Szilner, B.Szpak, C.Ur, J.J.Valiente-Dobon, M.Weinert, K.Wolf, K.O.Zell

Identification of high-spin proton configurations in 136Ba and 137Ba

NUCLEAR REACTIONS 238U(136Xe, 136Ba), E=6.84 MeV/nucleon; measured Eγ, Iγ, charged particles, and (charged particles)γ- and γγ-coin using the AGATA array for γ detection and the PRISMA spectrometer for charged particles at PIAVE+ALPI accelerator complex of INFN-LNL-Legnaro. 130Te(9Be, X)136Ba, E=40, 43 MeV; 130Te(11B, X)136Ba/137Ba, E not given; measured Eγ, Iγ, γγ-coin, γγ(θ) using 11 HPGe detectors and HORUS array of 14 HPGe detectors at the FN Tandem accelerator of University of Cologne. 136,137Ba; deduced high-spin levels, J, π, multipolarities, mixing ratios. Comparison with shell model predictions using GCN50:82, PQM130, realistic SM and SN100PN interactions. Systematics of high-spin levels in 134,135Xe, 136,137Ba, 138,139Ce, 140Nd.

NUCLEAR STRUCTURE 136,137Ba; calculated levels, J, π, wave functions, neutron occupation numbers using shell model with several interactions. Comparison with experimental data. 134Xe, 136Ba, 138Ce; calculated average neutron occupation numbers of the gdsh model space for observed high-spin states using the GCN50:82 and SN100PN interactions. 134Xe, 136Ba; calculated decomposition of the total angular momentum of selected states.

doi: 10.1103/PhysRevC.99.014301
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2019KA36      Phys.Rev. C 100, 024323 (2019)

L.Kaya, A.Vogt, P.Reiter, M.Siciliano, N.Shimizu, Y.Utsuno, H.-K.Wang, A.Gargano, L.Coraggio, N.Itaco, K.Arnswald, D.Bazzacco, B.Birkenbach, A.Blazhev, A.Bracco, B.Bruyneel, L.Corradi, F.C.L.Crespi, G.de Angelis, M.Droste, J.Eberth, A.Esmaylzadeh, E.Farnea, E.Fioretto, C.Fransen, A.Gadea, A.Giaz, A.Gorgen, A.Gottardo, K.Hadynska-Klek, H.Hess, R.Hirsch, P.R.John, J.Jolie, A.Jungclaus, V.Karayonchev, L.Kornwebel, W.Korten, S.Leoni, L.Lewandowski, S.Lunardi, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, C.Muller-Gatermann, D.Napoli, Zs.Podolyak, G.Pollarolo, F.Recchia, J.-M.Regis, N.Saed-Samii, E.Sahin, F.Scarlassara, K.Schomacker, M.Seidlitz, B.Siebeck, P.-A.Soderstrom, A.M.Stefanini, O.Stezowski, S.Szilner, B.Szpak, E.Teruya, C.Ur, J.J.Valiente-Dobon, K.Wolf, K.Yanase, N.Yoshinaga, K.O.Zell

Isomer spectroscopy in 133Ba and high-spin structure of 134Ba

NUCLEAR REACTIONS 124Sn(13C, X)133Ba/134Ba, E=55 MeV from FN tandem accelerator at Cologne; 208Pb(136Xe, X)134Ba, E=6.84 MeV/nucleon from PIAVE+ALPI accelerator complex at LNL-Legnaro; measured Eγ, Iγ, γγ-coin, γγ(θ), half-lives of isomers by γγ(t) using eight HPGe and 12 LaBr3(ce) detectors at Cologne, and magnetic spectrometer PRISMA with AGATA array at Legnaro. 133,134Ba; deduced high-spin levels, isomers, J, π, multipolarities, alignments, bands, backbending, configurations, B(E1), B(E2). Comparison with shell-model calculations for 134Ba, and with previous experimental results. Systematics of positive- and negative-parity yrast states in N=78 nuclei: 130Te, 132Xe, 134Ba, 136Ce, 138Nd, 140Sm, 142Gd, and Z=56 nuclei: 126,128,130,132,134,136,138Ba.

NUCLEAR STRUCTURE 134Ba; calculated levels, J, π using GCN50:82, SN100PN, SNV, PQM130, and realistic SM interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.024323
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2019MA65      Phys.Rev. C 100, 034324 (2019)

Y.Z.Ma, L.Coraggio, L.De Angelis, T.Fukui, A.Gargano, N.Itaco, F.R.Xu

Contribution of chiral three-body forces to the monopole component of the effective shell-model Hamiltonian

NUCLEAR STRUCTURE 41,42Ca, 41Sc; calculated low-lying levels, J, π, single-particle spectra for 41Ca and 41Sc. 40,42,44,46,48,50,52,54,56,58,60Ca, 48,50,52,54,56,58,60,62,64,66,68Ni; calculated neutron and proton effective single-particle energies (ESPEs), energies of 2+ levels, S(2n). 42,44,46,48,50,52,54,56,58,60,62Ti, 44,46,48,50,52,54,56,58,60,62,64Cr, 46,48,50,52,54,56,58,60,62,64,66Fe; calculated energies of 2+ levels, S(2n). 46Ar, 48Ca, 50Ti, 52Cr, 54Fe, 56Ni; calculated energies of 2+ levels, B(E2) for the first 2+ levels. Realistic shell-model calculations for fp-shell even-even nuclei (Z=20-28, N=20-40) starting from chiral two-nucleon (2NF) and three-nucleon (3NF) forces, within the many-body perturbation theory. Comparison with experimental data. Discussed the role of the monopole component of the effective shell-model Hamiltonian.

doi: 10.1103/PhysRevC.100.034324
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2019UR03      J.Phys.(London) G46, 105110 (2019)

B.A.Urazbekov, A.S.Denikin, S.M.Lukyanov, N.Itaco, D.M.Janseitov, K.Mendibayev, V.Burjan, V.Kroha, J.Mrazek, W.H.Trzaska, M.N.Harakeh, D.Etasse, I.Stefan, D.Verney, T.Issatayev, Y.E.Penionzhkevich, K.A.Kuterbekov, T.Zholdybayev

Clusterization and strong coupled-channels effects in deuteron interaction with 9Be nuclei

NUCLEAR REACTIONS 9Be(d, d), (d, d'), (d, p), (d, t), (d, α), E=19.5, 35 MeV; measured reaction products, Ep, Ip, Eα, Iα; deduced σ(θ), deformation parameter, spectroscopic amplitudes using the optical model and the coupled-channel approach.

doi: 10.1088/1361-6471/ab37a6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0962. Data from this article have been entered in the XUNDL database. For more information, click here.


2018FU14      Phys.Rev. C 98, 044305 (2018)

T.Fukui, L.De Angelis, Y.Z.Ma, L.Coraggio, A.Gargano, N.Itaco, F.R.Xu

Realistic shell-model calculations for p-shell nuclei including contributions of a chiral three-body force

NUCLEAR STRUCTURE 6,8Li, 8Be, 8,10,11B, 12,13C, 16O, 20Ne, 24Mg; calculated levels, g.s. energies, proton and neutron effective single-particle energies of N=Z nuclei with and without next-to-next-to leading order three-body potential using chiral perturbation theory and realistic shell-model (RCM) Hamiltonian. Comparison with experimental values, and with no-core shell-model calculations.

doi: 10.1103/PhysRevC.98.044305
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2018KA27      Phys.Rev. C 98, 014309 (2018)

L.Kaya, A.Vogt, P.Reiter, M.Siciliano, B.Birkenbach, A.Blazhev, L.Coraggio, E.Teruya, N.Yoshinaga, K.Higashiyama, K.Arnswald, D.Bazzacco, A.Bracco, B.Bruyneel, L.Corradi, F.C.L.Crespi, G.de Angelis, J.Eberth, E.Farnea, E.Fioretto, C.Fransen, B.Fu, A.Gadea, A.Gargano, A.Giaz, A.Gorgen, A.Gottardo, K.Hadynska-Klek, H.Hess, R.Hetzenegger, R.Hirsch, N.Itaco, P.R.John, J.Jolie, A.Jungclaus, W.Korten, S.Leoni, L.Lewandowski, S.Lunardi, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, C.Muller-Gatermann, D.Napoli, Zs.Podolyak, G.Pollarolo, A.Pullia, M.Queiser, F.Recchia, D.Rosiak, N.Saed-Samii, E.Sahin, F.Scarlassara, D.Schneiders, M.Seidlitz, B.Siebeck, J.F.Smith, P.-A.Soderstrom, A.M.Stefanini, T.Steinbach, O.Stezowski, S.Szilner, B.Szpak, C.Ur, J.J.Valiente-Dobon, K.Wolf, K.O.Zell

High-spin structure in the transitional nucleus 131Xe: Competitive neutron and proton alignment in the vicinity of the N=82 shell closure

NUCLEAR REACTIONS 208Pb(136Xe, X), E=6.84 MeV/nucleon; 238U(136Xe, X), E=7.35 MeV/nucleon; measured projectile-like reaction fragments using PRISMA magnetic spectrometer, Eγ, Iγ, γγ- and (131Xe)γ-coin using AGATA demonstrator array for γ detection at LNL-Legnaro. 124Sn(11B, 3np), E=54 MeV; measured Eγ, Iγ, γγ and pγ-coin, γγ(θ) using HORUS array at Cologne for γ detection and annular double-sided silicon strip detector (DSSSD) for particles. 131Xe; deduced levels, J, π, high-spin states. Comparison with shell-model calculations using several different interactions; discussed systematics of high-spin states in Z=54 nuclei of 123,125,127,129,131Xe, and N=77 nuclei of 127Sn, 129Te131Xe, 133Ba, 135Ce, 137Nd, 139Sm, 141Gd; compiled experimental total aligned angular momentum versus rotational frequency plots for yrast bands in A=117-132 Xe isotopes.

NUCLEAR STRUCTURE 131Xe; calculated levels, J, π, contribution of proton and neutron configurations for selected states, proton and neutron occupation numbers in h11/2 orbital, total aligned angular momenta as function of rotational frequency, and B(E2) using shell-model calculations with PQM130, SN100PN, GCN50:82, realistic SM, and SN100-KTH interactions. 129Xe; calculated proton and neutron occupation numbers in h11/2 orbital, total aligned angular momenta as function rotational frequency using shell model. Comparison with experimental data.

doi: 10.1103/PhysRevC.98.014309
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2018KA47      Phys.Rev. C 98, 054312 (2018)

L.Kaya, A.Vogt, P.Reiter, C.Muller-Gatermann, M.Siciliano, L.Coraggio, N.Itaco, A.Gargano, K.Arnswald, D.Bazzacco, B.Birkenbach, A.Blazhev, A.Bracco, B.Bruyneel, L.Corradi, F.C.L.Crespi, G.de Angelis, M.Droste, J.Eberth, E.Farnea, E.Fioretto, C.Fransen, A.Gadea, A.Giaz, A.Gorgen, A.Gottardo, K.Hadynska-Klek, H.Hess, R.Hetzenegger, R.Hirsch, P.R.John, J.Jolie, A.Jungclaus, W.Korten, S.Leoni, L.Lewandowski, S.Lunardi, R.Menegazzo, D.Mengoni, C.Michelagnoli, T.Mijatovic, G.Montagnoli, D.Montanari, D.Napoli, Zs.Podolyak, G.Pollarolo, F.Recchia, D.Rosiak, N.Saed-Samii, E.Sahin, F.Scarlassara, M.Seidlitz, P.-A.Soderstrom, A.M.Stefanini, O.Stezowski, S.Szilner, B.Szpak, C.Ur, J.J.Valiente-Dobon, M.Weinert, K.Wolf, K.O.Zell

Millisecond 23/2+ isomers in the N=79 isotones 133Xe and 135Ba

NUCLEAR REACTIONS 208Pb(136Xe, X)135Ba/133Xe/132Xe/136Ba, E=6.84 MeV/nucleon; measured Eγ, Iγ, γγ-coin, (particle)γ-coin using the Advanced GAmma Tracking Array (AGATA) for γ detection and the PRISMA magnetic spectrometer for particle identification at the PIAVE+ALPI accelerator complex of LNL-Legnaro. 130Te(9Be, X)132Xe/133Xe/135Ba/136Ba, E=40 MeV; measured Eγ, Iγ, γγ-coin, off-beam γγ(θ), half-lives of isomers using the HORUS array for γ detection at the FN tandem accelerator of the University of Cologne. 132,133Xe, 135,136Ba; deduced high-spin levels, isomers, J, π, total conversion coefficients, multipolarities, mixing ratios, configurations, B(M2), B(E3). 214Po; deduced mixing ratio for a transition from γγ(θ) measurement. Comparison with previous experimental data, and with large-scale shell model calculations using the SM, GCN50:82, SN100PN and SN100-KTH interactions. Systematics of levels, J, π, transition probabilities and isomers in N=79 isotones of 129Sn, 131Te, 133Xe, 135Ba, 137Ce, 139Nd, 141Sm, 143Gd.

NUCLEAR STRUCTURE 133Xe, 135Ba; calculated levels, J, π, configurations using large-scale shell model with SM, GCN50:82, SN100PN and SN100-KTH interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.98.054312
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2018MO33      Phys.Lett. B 781, 706 (2018)

A.I.Morales, G.Benzoni, H.Watanabe, G.de Angelis, S.Nishimura, L.Coraggio, A.Gargano, N.Itaco, T.Otsuka, Y.Tsunoda, P.Van Isacker, F.Browne, R.Daido, P.Doornenbal, Y.Fang, G.Lorusso, Z.Patel, S.Rice, L.Sinclair, P.-A.Soderstrom, T.Sumikama, J.J.Valiente-Dobon, J.Wu, Z.Y.Xu, A.Yagi, R.Yokoyama, H.Baba, R.Avigo, F.L.Bello Garrote, N.Blasi, A.Bracco, A.M.Bruce, F.Camera, S.Ceruti, F.C.L.Crespi, M.-C.Delattre, Zs.Dombradi, A.Gottardo, T.Isobe, I.Kojouharov, N.Kurz, I.Kuti, S.Lalkovski, K.Matsui, B.Melon, D.Mengoni, T.Miyazaki, V.Modamio-Hoybjor, S.Momiyama, D.R.Napoli, M.Niikura, R.Orlandi, Zs.Podolyak, P.H.Regan, H.Sakurai, E.Sahin, D.Sohler, H.Schaffner, R.Taniuchi, J.Taprogge, Zs.Vajta, O.Wieland, M.Yalcinkaya

Is seniority a partial dynamic symmetry in the first νg9/2 shell?

RADIOACTIVITY 72,74Co(β-) [from 9Be(238U, X), E=345 MeV/nucleon]; measured reaction products, Eγ, Iγ; deduced γ-ray energies, levels, isomeric states, seniority scheme, B(E2), the disappearance of the seniority isomerism. Comparison with available data. The MCSM calculations. The first in-flight β-delayed fast-timing study. The RIBF facility in RIKEN within the EURICA collaboration.

doi: 10.1016/j.physletb.2018.04.049
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2018RE09      Phys.Rev. C 98, 014328 (2018)

W.Reviol, D.G.Sarantites, J.M.Elson, J.E.Kinnison, A.Gargano, R.V.F.Janssens, J.M.Allmond, A.D.Ayangeakaa, S.Bottoni, M.P.Carpenter, H.M.David, A.Galindo-Uribarri, N.Itaco, T.Lauritsen, E.Padilla-Rodal, S.Zhu

Low-spin structure of the N=82 nucleus 137Cs

NUCLEAR REACTIONS 10B(136Xe, 9Be), E=560 MeV; measured Eγ, Iγ, particle spectra, γγ- and (9Be)γ-coin, γ(θ) using Gammasphere array for γ detection and Phoswich Wall array for charged particle detection at ATLAS-ANL. 137Cs; deduced levels, J, π, multipolarities, configurations. Comparison of level spectra with shell-model calculations. Systematics of level energies in N=82 133Sb, 135I, and 137Cs isotones.

doi: 10.1103/PhysRevC.98.014328
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2017AL06      Phys.Rev.Lett. 118, 092503 (2017)

J.M.Allmond, A.E.Stuchbery, C.Baktash, A.Gargano, A.Galindo-Uribarri, D.C.Radford, C.R.Bingham, B.A.Brown, L.Coraggio, A.Covello, M.Danchev, C.J.Gross, P.A.Hausladen, N.Itaco, K.Lagergren, E.Padilla-Rodal, J.Pavan, M.A.Riley, N.J.Stone, D.W.Stracener, R.L.Varner, C.-H.Yu

Electromagnetic Moments of Radioactive 136Te and the Emergence of Collectivity 2p (+) 2n Outside of Double-Magic 132Sn

NUCLEAR REACTIONS Ti(136Te, 136Te'), E=410 MeV; measured reaction products, Eγ, Iγ. 136Te; deduced energy levels, J, π, B(E2) values. Comparison with experimental data and theoretical calculations.

doi: 10.1103/PhysRevLett.118.092503
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2017AR09      Phys.Lett. B 772, 599 (2017)

K.Arnswald, T.Braunroth, M.Seidlitz, L.Coraggio, P.Reiter, B.Birkenbach, A.Blazhev, A.Dewald, C.Fransen, B.Fu, A.Gargano, H.Hess, R.Hirsch, N.Itaco, S.M.Lenzi, L.Lewandowski, J.Litzinger, C.Muller-Gatermann, M.Queiser, D.Rosiak, D.Schneiders, B.Siebeck, T.Steinbach, A.Vogt, K.Wolf, K.O.Zell

Enhanced collectivity along the N = Z line: Lifetime measurements in 44Ti, 48Cr, and 52Fe

NUCLEAR REACTIONS Mg(23Na, xnp)44Ti, 40Ca(10B, np)48Cr, 27Al(28Si, 2np)52Fe, E=62, 26, 86 MeV; measured reaction products, Eγ, Iγ. 44Ti, 48,50Cr, 52Fe; deduced γ-ray energies, level T1/2, B(E2). Recoil distance Doppler-shift method, comparison with available data.

doi: 10.1016/j.physletb.2017.07.032
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2017CO03      Int.J.Mod.Phys. E26, 1740006 (2017)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Core polarization and modern realistic shell-model Hamiltonians

NUCLEAR STRUCTURE 6Li, 6He; calculated energy levels, J, π. Comparison with available data.

doi: 10.1142/S0218301317400067
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2017CO08      Phys.Rev. C 95, 064324 (2017)

L.Coraggio, L.De Angelis, T.Fukui, A.Gargano, N.Itaco

Calculation of Gamow-Teller and two-neutrino double-β decay properties for 130Te and 136Xe with a realistic nucleon-nucleon potential

RADIOACTIVITY 130Te, 136Xe(2β-); calculated nuclear matrix elements (NMEs) and Gamow-Teller (GT) strengths for 2νββ decay. Comparison with experimental values.

NUCLEAR STRUCTURE 130Te, 130,136Xe, 136Ba; calculated levels, J, π, B(E2) for yrast states up to 6+ using the shell model, and compared with experimental data.

doi: 10.1103/PhysRevC.95.064324
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2017GA19      Phys.Scr. 92, 094003 (2017)

A.Gargano, L.Coraggio, N.Itaco

Effectively-truncated large-scale shell-model calculations and nuclei around 100Sn

doi: 10.1088/1402-4896/aa7d6d
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2017JU02      Phys.Lett. B 772, 483 (2017)

A.Jungclaus, H.Grawe, S.Nishimura, P.Doornenbal, G.Lorusso, G.S.Simpson, P.-A.Soderstrom, T.Sumikama, J.Taprogge, Z.Y.Xu, H.Baba, F.Browne, N.Fukuda, R.Gernhauser, G.Gey, N.Inabe, T.Isobe, H.S.Jung, D.Kameda, G.D.Kim, Y.-K.Kim, I.Kojouharov, T.Kubo, N.Kurz, Y.K.Kwon, Z.Li, H.Sakurai, H.Schaffner, Y.Shimizu, K.Steiger, H.Suzuki, H.Takeda, Zs.Vajta, H.Watanabe, J.Wu, A.Yagi, K.Yoshinaga, G.Benzoni, S.Bonig, K.Y.Chae, L.Coraggio, J.-M.Daugas, F.Drouet, A.Gadea, A.Gargano, S.Ilieva, N.Itaco, F.G.Kondev, T.Kroll, G.J.Lane, A.Montaner-Piza, K.Moschner, D.Mucher, F.Naqvi, M.Niikura, H.Nishibata, A.Odahara, R.Orlandi, Z.Patel, Zs.Podolyak, A.Wendt

Observation of a γ decaying millisecond isomeric state in 128Cd80

NUCLEAR REACTIONS 9Be(238U, X)128Cd, E=345 MeV/nucleon; measured reaction products, Eγ, Iγ. 129Cd, 129In; deduced γ-ray energies, J, π, level T1/2, B(E3). Comparison with theoretical calculations.

doi: 10.1016/j.physletb.2017.07.006
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2016CO10      Phys.Rev. C 93, 064328 (2016)

L.Coraggio, A.Gargano, N.Itaco

Double-step truncation procedure for large-scale shell-model calculations

NUCLEAR STRUCTURE 90,92,94,96,98Zr, 92,94,96,98,100Mo, 94,96,98,100,102Ru, 96,98,100,102,104Pd, 98,100,102,104,106Cd, 100,102,104,106,108Sn; calculated energies and B(E2) for first 2+ states, effective single-particle energies (ESPEs). Large-scale shell-model calculations. Investigated dependence of shell-model results on different truncation schemes of the original model space. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.064328
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2016JU02      Phys.Rev. C 93, 041301 (2016)

A.Jungclaus, A.Gargano, H.Grawe, J.Taprogge, S.Nishimura, P.Doornenbal, G.Lorusso, Y.Shimizu, G.S.Simpson, P.-A.Soderstrom, T.Sumikama, Z.Y.Xu, H.Baba, F.Browne, N.Fukuda, R.Gernhauser, G.Gey, N.Inabe, T.Isobe, H.S.Jung, D.Kameda, G.D.Kim, Y.-K.Kim, I.Kojouharov, T.Kubo, N.Kurz, Y.K.Kwon, Z.Li, H.Sakurai, H.Schaffner, K.Steiger, H.Suzuki, H.Takeda, Zs.Vajta, H.Watanabe, J.Wu, A.Yagi, K.Yoshinaga, S.Bonig, L.Coraggio, J.-M.Daugas, F.Drouet, A.Gadea, S.Ilieva, N.Itaco, T.Kroll, A.Montaner-Piza, K.Moschner, D.Mucher, H.Nishibata, A.Odahara, R.Orlandi, A.Wendt

First observation of γ rays emitted from excited states south-east of 132Sn: The π g-19/2 (X) νf7/2 multiplet of 132In83

RADIOACTIVITY 133Cd(β-), (β-n)[from 9Be(238U, F), E=345 MeV/nucleon using BigRIPS fragment separator and ZeroDegree spectrometer at RIBF-RIKEN facility]; measured Eγ, Iγ, (133Cd ions)γ-coin using WAS3ABi detection system of DSSSDs for β rays and ions, and 12 large-volume Ge cluster detectors for gamma rays. 132In; deduced levels, J, π. Shell-model calculations.

NUCLEAR REACTIONS 9Be(238U, F)129Cd47+/130Cd47+/132Cd48+/133Cd48+, E=345 MeV/nucleon; measured partial particle identification plot of Z=45-51 isotopes and mass-to-charge ratio A/q using BigRIPS fragment separator and ZeroDegree spectrometer at RIBF-RIKEN facility.

doi: 10.1103/PhysRevC.93.041301
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2016JU03      Phys.Rev. C 94, 024303 (2016)

A.Jungclaus, H.Grawe, S.Nishimura, P.Doornenbal, G.Lorusso, G.S.Simpson, P.-A.Soderstrom, T.Sumikama, J.Taprogge, Z.Y.Xu, H.Baba, F.Browne, N.Fukuda, R.Gernhauser, G.Gey, N.Inabe, T.Isobe, H.S.Jung, D.Kameda, G.D.Kim, Y.-K.Kim, I.Kojouharov, T.Kubo, N.Kurz, Y.K.Kwon, Z.Li, H.Sakurai, H.Schaffner, Y.Shimizu, K.Steiger, H.Suzuki, H.Takeda, Zs.Vajta, H.Watanabe, J.Wu, A.Yagi, K.Yoshinaga, G.Benzoni, S.Bonig, K.Y.Chae, L.Coraggio, J.-M.Daugas, F.Drouet, A.Gadea, A.Gargano, S.Ilieva, N.Itaco, F.G.Kondev, T.Kroll, G.J.Lane, A.Montaner-Piza, K.Moschner, D.Mucher, F.Naqvi, M.Niikura, H.Nishibata, A.Odahara, R.Orlandi, Z.Patel, Zs.Podolyak, A.Wendt

β decay of semi-magic 130Cd: Revision and extension of the level scheme of 130In

RADIOACTIVITY 130Cd(β-)[from 9Be(238U, F), E=345 MeV/nucleon, using BigRIPS separator and ZeroDegree spectrometer (ZDS) at RIBF-RIKEN facility]; Measured Eγ, Iγ, γγ-, βγ-coin, isomer half-life by γγ(t) using WAS3ABi array for β and ion detection, and EURICA array of 12 large-volume HPGe clusters for γ detection. 130In; deduced levels, J, π, β feedings, logft, high-lying core-excited states, configurations. Comparison with previous experimental results, ENSDF evaluation, and shell-model calculations.

doi: 10.1103/PhysRevC.94.024303
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2016RE15      Phys.Rev. C 94, 034309 (2016)

W.Reviol, D.G.Sarantites, J.M.Elson, J.E.Kinnison, A.Gargano, S.Bottoni, R.V.F.Janssens, J.M.Allmond, A.D.Ayangeakaa, M.P.Carpenter, H.M.David, A.Galindo-Uribarri, N.Itaco, T.Lauritsen, E.Padilla-Rodal, S.Zhu

One-neutron transfer study of 137Xe and systematics of 13/2+1 and 13/2+2 levels in N=83 nuclei

NUCLEAR REACTIONS 13C(136Xe, 12C)137Xe, 9Be(136Xe, 8Be)137Xe, E=560 MeV; measured particle spectra, Eγ, Iγ, γ(θ), (particle)γ-, (particle)γγ-coin using Phoswich Wall and Digital Gammasphere arrays at ATLAS-ANL facility. 137Xe; deduced levels, J, π, multipolarity, relative yields. One-neutron transfer reactions. Comparison with systematics of first and second 13/2+ states in N=83 isotones, and with shell-model calculations. 135,137Xe, 137Cs, 139,140Ba, 142Ce; observed γ rays from contaminants.

doi: 10.1103/PhysRevC.94.034309
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2016TA22      Eur.Phys.J. A 52, 347 (2016), Erratum Eur.Phys.J. A 52, 375 (2016)

J.Taprogge, A.Jungclaus, H.Grawe, I.N.Borzov, S.Nishimura, P.Doornenbal, G.Lorusso, G.S.Simpson, P.-A.Soderstrom, T.Sumikama, Z.Y.Xu, H.Baba, F.Browne, N.Fukuda, R.Gernhauser, G.Gey, N.Inabe, T.Isobe, H.S.Jung, D.Kameda, G.D.Kim, Y.-K.Kim, I.Kojouharov, T.Kubo, N.Kurz, Y.K.Kwon, Z.Li, H.Sakurai, H.Schaffner, Y.Shimizu, K.Steiger, H.Suzuki, H.Takeda, Zs.Vajta, H.Watanabe, J.Wu, A.Yagi, K.Yoshinaga, G.Benzoni, S.Bonig, K.Y.Chae, L.Coraggio, J.-M.Daugas, F.Drouet, A.Gadea, A.Gargano, S.Ilieva, N.Itaco, F.G.Kondev, T.Kroll, G.J.Lane, A.Montaner-Piza, K.Moschner, D.Mucher, F.Naqvi, M.Niikura, H.Nishibata, A.Odahara, R.Orlandi, Z.Patel, Zs.Podolyak, A.Wendt

Proton-hole and core-excited states in the semi-magic nucleus 131In82

RADIOACTIVITY 131Cd(β-)[from 238U on 9Be at 345 MeV/nucleon]; measured Eγ, Iγ using EURICA array (84 Ge crystals around Si detectors), β-decay using WAS3ABi detector (8 DSSD's of 40x60 strips each), βγ-coin, other reaction products; deduced γ spectrum in prompt coincidence with first β decay, γ transitions, relative intensities, 131In level scheme, β feeding intensities (for transitions to excited states in 131In), excitation energies of several core-excited configurations; calculated log ft, β decay strength for GT allowed and first-forbidden β decay branches, excitation energies of core-excited configurations using shell model and QRPA.

doi: 10.1140/epja/i2016-16347-y
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2015BE32      Phys.Lett. B 751, 107 (2015)

G.Benzoni, A.I.Morales, H.Watanabe, S.Nishimura, L.Coraggio, N.Itaco, A.Gargano, F.Browne, R.Daido, P.Doornenbal, Y.Fang, G.Lorusso, Z.Patel, S.Rice, L.Sinclair, P.-A.Soderstrom, T.Sumikama, J.Wu, Z.Y.Xu, R.Yokoyama, H.Baba, R.Avigo, F.L.Bello Garrote, N.Blasi, A.Bracco, F.Camera, S.Ceruti, F.C.L.Crespi, G.de Angelis, M.-C.Delattre, Zs.Dombradi, A.Gottardo, T.Isobe, I.Kuti, K.Matsui, B.Melon, D.Mengoni, T.Miyazaki, V.Modamio-Hoybjor

Decay properties of 68, 69, 70Mn: Probing collectivity up to N = 44 in Fe isotopic chain

RADIOACTIVITY 68,69,70Mn(β-), (β-n) [from Be(238U, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ, Eβ, Iβ; deduced γ-ray energies, T1/2, β-delayed neutron emission probabilities. Comparison with FRDM + QRPA and KTUY + GT2 calculations.

doi: 10.1016/j.physletb.2015.10.025
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2015CO06      Phys.Rev. C 91, 041301 (2015)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Shell-model study of quadrupole collectivity in light tin isotopes

NUCLEAR STRUCTURE 100,102,104,106,108,110Sn; calculated two-body matrix elements, single-particle energies, and effective charges for electric quadrupole transition operators, energies and B(E2) of first 2+ states, proton occupation numbers for ground and first 2+ states, levels, J and π for 102Sn. Z=38, 40, 42, 44, 46, 48, 50; calculated neutron and proton effective single-particle energies as function of atomic number. Shell-model calculations using realistic NN potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.041301
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2015KA06      Phys.Rev. C 91, 024318 (2015)

S.Kaim, C.M.Petrache, A.Gargano, N.Itaco, T.Zerrouki, R.Leguillon, A.Astier, I.Deloncle, T.Konstantinopoulos, J.M.Regis, D.Wilmsen, B.Melon, A.Nannini, C.Ducoin, D.Guinet, T.Bhattacharjee

High-spin spectroscopy of 139Ce

NUCLEAR REACTIONS 130Te(14C, 5n), E=82 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(θ)(anisotropy ratio) using ORGAM array at IPN-Orsay tandem accelerator facility. 139Ce; deduced high-spin levels, J, π, multipolarity, magnetic-dipole rotational band, configuration, B(M1)/B(E2). Comparison with Tilted-axis (TAC) and cranked Nilsson Strutinsky (CNS) calculations. 139,140Ce; calculated levels, J, π using shell model with OSLO code; comparison with experimental data.

doi: 10.1103/PhysRevC.91.024318
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2015SA22      Phys.Rev. C 91, 054311 (2015)

F.Sammarruca, L.Coraggio, J.W.Holt, N.Itaco, R.Machleidt, L.E.Marcucci

Toward order-by-order calculations of the nuclear and neutron matter equations of state in chiral effective field theory

doi: 10.1103/PhysRevC.91.054311
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2014CO04      Phys.Rev. C 89, 024319 (2014)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Realistic shell-model calculations for isotopic chains "north-east" of 48Ca in the (N, Z) plane

NUCLEAR STRUCTURE 50,52,54,56,58,60,62,64,66,68,70,72Ca, 50,52,54,56,58,60,62Ti, 52,54,56,58,60,62,64Cr, 54,56,58,60,62,64,66Fe, 56,58,60,62,64,66,68,70,72,74,76,78Ni; calculated energies and B(E2) values of first 2+ states using realistic shell-model calculations with two different model spaces. Discussed role of 1d5/2 neutron orbital on yrast quadrupole excitations. Comparison with experimental data taken from ENSDF and XUNDL databases.

doi: 10.1103/PhysRevC.89.024319
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2014CO09      Phys.Rev. C 89, 044321 (2014)

L.Coraggio, J.W.Holt, N.Itaco, R.Machleidt, L.E.Marcucci, F.Sammarruca

Nuclear-matter equation of state with consistent two- and three-body perturbative chiral interactions

NUCLEAR STRUCTURE 3H, 3He; calculated neutron-proton phase shifts, binding energy, Gamow-Teller transition matrix element, nuclear matter energy per particle. Equation of state (EOS) for two- and three-body perturbative chiral interactions in the framework of the perturbative Goldstone expansion and regulator functions. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.044321
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2014CO13      Nucl.Phys. A928, 43 (2014)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

From Kuo-Brown to today's realistic shell-model calculations

NUCLEAR STRUCTURE 18O, 18F; calculated levels, J, π. 17O; calculated energy spacings. Nuclear shell model with effective interaction from Hamada-Johnston NN potential. Compared with earlier calculations and data.

doi: 10.1016/j.nuclphysa.2014.03.018
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2014MA85      Phys.Rev.Lett. 113, 182501 (2014)

T.Marchi, G.de Angelis, J.J.Valiente-Dobon, V.M.Bader, T.Baugher, D.Bazin, J.Berryman, A.Bonaccorso, R.Clark, L.Coraggio, H.L.Crawford, M.Doncel, E.Farnea, A.Gade, A.Gadea, A.Gargano, T.Glasmacher, A.Gottardo, F.Gramegna, N.Itaco, P.R.John, R.Kumar, S.M.Lenzi, S.Lunardi, S.McDaniel, C.Michelagnoli, D.Mengoni, V.Modamio, D.R.Napoli, B.Quintana, A.Ratkiewicz, F.Recchia, E.Sahin, R.Stroberg, D.Weisshaar, K.Wimmer, R.Winkler

Quadrupole Transition Strength in the 74Ni Nucleus and Core Polarization Effects in the Neutron-Rich Ni Isotopes

NUCLEAR REACTIONS 197Au(74Ni, 74Ni'), E=95.8 MeV/nucleon; measured reaction products, Eγ, Iγ. 74Ni; deduced energy levels, B(E2). Comparison with shell model calculations.

doi: 10.1103/PhysRevLett.113.182501
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2013CO02      Phys.Rev. C 87, 014322 (2013)

L.Coraggio, J.W.Holt, N.Itaco, R.Machleidt, F.Sammarruca

Reduced regulator dependence of neutron-matter predictions with perturbative chiral interactions

doi: 10.1103/PhysRevC.87.014322
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2013CO03      Phys.Rev. C 87, 021301 (2013)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Shell-model study of single-neutron strength fragmentation in 137Xe

NUCLEAR REACTIONS 136Xe(d, p), E not given; calculated spectroscopic factors using Shell-model. Comparison with experimental data.

NUCLEAR STRUCTURE 137Xe; calculated levels, J, π, spectroscopic factors. Shell-model calculations using CD-Bonn NN potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.021301
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2013CO06      Phys.Rev. C 87, 034309 (2013)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Evolution of single-particle states beyond 132Sn

NUCLEAR STRUCTURE 133Sn, 135Te, 137Xe, 133,135,137Sb; calculated levels, J, π, spectroscopic factors, single-particle energies, summed single-proton strengths, effective single-particle energies (ESPE). Shell-model calculations using a realistic two-body effective interaction based on CD-Bonn nucleon-nucleon potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.034309
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2013CO22      Phys.Rev. C 88, 041304 (2013)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Behavior of odd-even mass staggering around 132Sn

NUCLEAR STRUCTURE 134,135Sn, 134,135,136Sb, 134,135,136,137Te, 136,137,138Xe; calculated binding energies. 131,133Sn, 133,135Te, 135,137Xe; calculated odd-even staggering around N=82. Shell model calculations with realistic low-momentum two-body effective interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.041304
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2012CO07      Phys.Rev. C 85, 034335 (2012)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

g9/2 nuclei and neutron-proton interaction

NUCLEAR STRUCTURE 90Nb, 98In; calculated proton-neutron multiplets, proton-proton, neutron-neutron, and proton-neutron matrix elements. 92Pd, 96,98Cd, 97Ag, 96Pd; calculated yrast levels, J, π, yrast state overlap, isoscalar and isovector pair contribution to the energy level spacings. Shell model calculations using two-body effective interaction from the CD-Bonn potential. Role of isoscalar spin-aligned coupling. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.034335
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2012SA51      Phys.Rev. C 86, 054317 (2012)

F.Sammarruca, B.Chen, L.Coraggio, N.Itaco, R.Machleidt

Dirac-Brueckner-Hartree-Fock versus chiral effective field theory

doi: 10.1103/PhysRevC.86.054317
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2011CO18      J.Phys.:Conf.Ser. 312, 092021 (2011)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Fully microscopic shell-model calculations with realistic effective hamiltonians

NUCLEAR STRUCTURE 16,18,20,22,24C, 18,20,22,24,26,28O, 42,44,46,48,50,52,54,56Ca; calculated binding energy, mass excess, yrast 2+ state energy. 42,44,46,48,50,52,54,56Ti; calculated yrast 2+ state energy, B(E2). 134Sn, 136Te, 138Xe, 140Ba, 142Ce, 144Nd, 146Sm, 148Gd, 150Dy, 152Er, 154Yb; calculated ground state energy, mass excess. 134Te; calculated levels, J, π. Realistic shell model within fully microscopic approach; compared with available data.

doi: 10.1088/1742-6596/312/9/092021
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2010CO05      Phys.Rev. C 81, 064303 (2010)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Shell-model calculations for neutron-rich carbon isotopes with a chiral nucleon-nucleon potential

NUCLEAR STRUCTURE 16,18,20,22C; calculated level energies, B(E2), M1 transition matrix elements, two-body matrix elements, location of the neutron drip line. 17,19C; calculated low-energy levels. Shell model with a realistic effective Hamiltonian derived from the chiral N3LOW nucleon-nucleon potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.064303
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2010CO17      J.Phys.:Conf.Ser. 205, 012004 (2010)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Realistic low-momentum effective interactions and nuclear structure near double closed shells

NUCLEAR STRUCTURE 136Sn, 134,136Sb, 136I, 212Pb, 210,212Bi, 212At; calculated low-lying levels, J, π using shell model with realistic low-momentum effective interactions derived from CD-Bonn potential. Compared with data.

doi: 10.1088/1742-6596/205/1/012004
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2010LI03      Phys.Rev. C 81, 014316 (2010)

S.H.Liu, J.H.Hamilton, A.V.Ramayya, A.Covello, A.Gargano, N.Itaco, N.J.Stone, A.V.Daniel, J.K.Hwang, Y.X.Luo, J.O.Rasmussen, G.M.Ter-Akopian, S.J.Zhu, W.C.Ma

g-factor and spin-parity assignments of excited states in the N=83 isotones 135Te, 136I, 137Xe, and 138Cs

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin, γγ(θ) using Gammasphere array. 135Te, 136I, 137Xe, 138Cs; deduced levels, J, π. Comparison with shell model calculations.

NUCLEAR MOMENTS 137Xe; measured g factor of a 15/2- state using integral perturbed angular correlation (IPAC) technique.

doi: 10.1103/PhysRevC.81.014316
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2010LI24      Nucl.Phys. A834, 78c (2010)

S.H.Liu, J.H.Hamilton, A.V.Ramayya, A.Covello, A.Gargano, N.Itaco, Y.X.Luo, J.O.Rasmussen, J.K.Hwang, A.V.Daniel, G.M.Ter-Akopian, S.J.Zhu, W.C.Ma

High spin structure of the neutron-rich 139, 142Cs nuclei

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ(θ), γγ-coin. 139,142Cs; deduced high-spin states, levels, J, π, bands, ICC, δ. 139Cs calculated levels, J, π, δ using shell model.

doi: 10.1016/j.nuclphysa.2010.01.023
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2009CO04      Acta Phys.Pol. B40, 401 (2009)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Two-Valence-Particle Nuclei in the 132Sn and 208Pb Regions

NUCLEAR STRUCTURE 134Sn, 134Te, 134Sb; calculated energies, Jπ. shell model.


2009CO15      Phys.Rev. C 80, 021305 (2009)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Similarity of nuclear structure in the 132Sn and 208Pb regions: Proton-neutron multiplets

NUCLEAR STRUCTURE 132Sn, 136I, 134,136Sb, 208Pb, 210,212Bi, 212At; calculated energies of proton-neutron multiplets and diagonal matrix elements for proton-neutron configurations using large-scale shell model calculations and interactions derived from CD-Bonn nucleon-nucleon potentials. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.021305
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2009CO19      Phys.Rev. C 80, 044311 (2009)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Spectroscopic study of neutron-rich calcium isotopes with a realistic shell-model interaction

NUCLEAR STRUCTURE 49,50,51,52,53,54,55Ca, 56Ca; calculated levels, J, π, and neutron-neutron two-body matrix elements using shell-model with a realistic effective interaction from the CD-Bonn nucleon-nucleon potential. 42,44,46,48,50,52,54,56Ca; calculated ground-state energies per valence neutron and effective single-particle energies. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.044311
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2009CO20      Phys.Rev. C 80, 044320 (2009)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Shell-model study of the N = 82 isotonic chain with a realistic effective Hamiltonian

NUCLEAR STRUCTURE 133Sb, 134Te, 135I, 136Xe, 137Cs, 138Ba, 139La, 140Ce, 141Pr, 142Nd, 143Pm, 144Sm, 145Eu, 146Gd, 147Tb, 148Dy, 149Ho, 150Er, 152Yb, 154Hf; calculated single-particle energies, levels, J, π and B(E2) of N=82 nuclei using shell-model within the framework of time-dependent degenerate perturbation theory. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.044320
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2009CO23      Phys.Rev. C 80, 061303 (2009)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Shell-model interpretation of high-spin states in 134I

NUCLEAR STRUCTURE 134I; calculated levels, J, π using shell-model and CD-Bonn nucleon-nucleon potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.061303
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2009LI42      Phys.Rev. C 80, 044314 (2009)

S.H.Liu, J.H.Hamilton, A.V.Ramayya, A.Covello, A.Gargano, N.Itaco, Y.X.Luo, J.O.Rasmussen, J.K.Hwang, A.V.Daniel, G.M.Ter-Akopian, S.J.Zhu, W.C.Ma

High spin structure of the neutron-rich nuclei 137I and 139Cs

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin, and γγ(θ) using Gammasphere array. 137I, 139Cs; deduced levels, J, π, bands, multipolarities and mixing ratios. 108,109,110Tc, 111,113Rh; measured Eγ, γγ-coin. Comparison with shell-model calculations. A=133-141(odd), Z=55; N=84, Sb, I, Cs, La; A=132-140(even), Z=52, 54, 56; systematics of low-lying states.

doi: 10.1103/PhysRevC.80.044314
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2008CO08      Nucl.Phys. A805, 424c (2008)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Shell-model studies on exotic nuclei around 132Sn

NUCLEAR STRUCTURE 134Te, 134Sn, 134,135Sb; calculated energy levels, J, π using a realistic shell model with two approaches.

doi: 10.1016/j.nuclphysa.2008.02.264
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2007CO04      Phys.Rev. C 75, 024311 (2007)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, D.R.Entem, T.T.S.Kuo, R.Machleidt

Low-momentum nucleon-nucleon interactions and shell-model calculations

NUCLEAR STRUCTURE 18,20,22,24,26O; calculated ground and excited states energies. Low-momentum potential.

doi: 10.1103/PhysRevC.75.024311
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2007CO13      Prog.Part.Nucl.Phys. 59, 401 (2007)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Structure of exotic nuclei around double shell closures

doi: 10.1016/j.ppnp.2007.01.001
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2007CO15      Phys.Rev. C 75, 057303 (2007)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Ground-state energy of 40Ca with the CD-Bonn nucleon-nucleon potential

NUCLEAR STRUCTURE 40Ca; calculated ground state energy within the framework of the Goldstone expansion using the CD-Bonn nucleon-nucleon potential.

doi: 10.1103/PhysRevC.75.057303
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2007CO28      Phys.Rev. C 76, 061303 (2007)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Long standing problem of 210Bi and the realistic proton-neutron effective interaction

NUCLEAR STRUCTURE 210Bi; calculated single particle energies, level energies, J. Comparisons with experimental data and with proton-neutron multiplets in 132Sn, 208Pb. Shell-model calculations.

doi: 10.1103/PhysRevC.76.061303
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2007CO29      Eur.Phys.J. Special Topics 150, 93 (2007)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Shell-model structure of exotic nuclei beyond 132Sn

NUCLEAR STRUCTURE 134,136Sn, 135Sb; calculated level energies, J, π using the shell model with a realistic effective interaction derived from the CD-Bonn nucleon-nucleon potential.

doi: 10.1140/epjst/e2007-00275-7
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2006CO01      Phys.Rev. C 73, 014304 (2006)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Nuclear structure calculations with low-momentum potentials in a model space truncation approach

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies. Goldstone expansion.

doi: 10.1103/PhysRevC.73.014304
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2006CO07      Phys.Rev. C 73, 031302 (2006)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Proton-neutron multiplets in exotic 134Sb: Testing the shell-model effective interaction

NUCLEAR STRUCTURE 134Sb; calculated level energies, configurations. Shell-model effective interaction, comparison with data.

doi: 10.1103/PhysRevC.73.031302
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2005CO01      Phys.Rev. C 71, 014307 (2005)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, R.Machleidt

Nuclear structure calculations and modern nucleon-nucleon potentials

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energies, radii. Several nucleon-nucleon potentials compared.

doi: 10.1103/PhysRevC.71.014307
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2005CO09      Phys.Lett. B 616, 43 (2005)

L.Coraggio, N.Itaco

Self-consistent nuclear shell-model calculation starting from a realistic N N potential

NUCLEAR STRUCTURE 6He, 6,7,8Li, 7,8Be, 8B; calculated ground and excited states energies, μ, quadrupole moments, B(E2), B(M1). Self-consistent shell model approach, comparison with data.

doi: 10.1016/j.physletb.2005.04.060
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2005CO23      Phys.Rev. C 72, 057302 (2005); Erratum Phys.Rev. C 73, 069901 (2006)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Shell-model structure of exotic 135Sb

NUCLEAR STRUCTURE 135Sb; calculated levels, J, π, B(M1). Shell model, realistic effective interaction, comparison with data.

doi: 10.1103/PhysRevC.72.057302
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2004CO15      Phys.Rev. C 70, 034310 (2004)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Structure of particle-hole nuclei around 100Sn

NUCLEAR STRUCTURE 98Ag, 100,102In; calculated level energies for particle-hole multiplets. Shell model, comparison with data.

doi: 10.1103/PhysRevC.70.034310
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2004CO19      Yad.Fiz. 67, 1637 (2004); Phys.Atomic Nuclei 67, 1611 (2004)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Proton-Neutron Interaction near Closed Shells

NUCLEAR STRUCTURE 208,210Bi, 132,134Sb, 98Ag, 102In; calculated particle-hole and particle-particle multiplet energies, proton-neutron interaction effects.

doi: 10.1134/1.1802346
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2003CO17      Phys.Rev. C 68, 034320 (2003)

L.Coraggio, N.Itaco, A.Covello, A.Gargano, T.T.S.Kuo

Ground-state properties of closed-shell nuclei with low-momentum realistic interactions

NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energies, radii, single-particle energies and occupation probabilities. Low-momentum nucleon-nucleon potential.

doi: 10.1103/PhysRevC.68.034320
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2003CO24      Acta Phys.Pol. B34, 2257 (2003)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Particle-hole multiplets near closed shells

NUCLEAR STRUCTURE 98Ag, 102In, 130,132Sb; calculated particle-hole multiplets energy vs spin. Shell model, comparison with data.


2003HW01      Phys.Rev. C 67, 014317 (2003), Erratum Phys.Rev. C 106, 049903 (2022)

J.K.Hwang, A.V.Ramayya, J.H.Hamilton, Y.X.Luo, J.O.Rasmussen, C.J.Beyer, P.M.Gore, S.C.Wu, I.Y.Lee, C.M.Folden III, P.Fallon, P.Zielinski, K.E.Gregorich, A.O.Macchiavelli, M.A.Stoyer, S.J.Asztalos, T.N.Ginter, R.Donangelo, L.Coraggio, A.Covello, A.Gargano, N.Itaco

High spin states in 93Sr

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 93Sr deduced high-spin levels, J, π, configurations. Gammasphere array, comparisons with model predictions.

NUCLEAR STRUCTURE 90,92,93,94Sr; calculated levels, J, π. Shell model.

doi: 10.1103/PhysRevC.67.014317
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2002BO18      Phys.Rev. C65, 051301 (2002)

S.Bogner, T.T.S.Kuo, L.Coraggio, A.Covello, N.Itaco

Low Momentum Nucleon-Nucleon Potential and Shell Model Effective Interactions

NUCLEAR STRUCTURE 18O, 134Te, 135I; calculated levels, J, π. Shell model, renormalization group - effective field theory approach. Comparison with data.

doi: 10.1103/PhysRevC.65.051301
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2002CO07      Phys.Rev. C65, 044320 (2002)

A.Covello, A.Gargano, N.Itaco

Neutron-Proton Interaction in Rare-Earth Nuclei: Role of tensor force

NUCLEAR STRUCTURE 174Lu, 180,182Ta, 188Re; calculated levels, J, π, configurations; deduced role of tensor force. Particle-rotor model.

doi: 10.1103/PhysRevC.65.044320
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2002CO12      Phys.Rev. C65, 051306 (2002)

L.Coraggio, A.Covello, A.Gargano, N.Itaco

Structure of Sn Isotopes Beyond N = 82

NUCLEAR STRUCTURE 134,135Sn; calculated levels, J, π. 134Sn calculated transitions B(E2). Shell model, realistic effective interaction, comparison with data.

doi: 10.1103/PhysRevC.65.051306
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2002CO20      Phys.Rev. C66, 021303 (2002)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, D.R.Entem, R.Machleidt

Microscopic nuclear structure based upon a chiral NN potential

NUCLEAR STRUCTURE 18O, 134Te, 210Po; calculated levels, J, π, binding energies. Shell model, chiral effective field theory, comparison with data.

doi: 10.1103/PhysRevC.66.021303
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2002CO27      Phys.Rev. C 66, 064311 (2002)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Realistic shell-model calculations for proton particle-neutron hole nuclei around 132Sn

NUCLEAR STRUCTURE 130,131,132Sb, 133Te; calculated levels, J, π, configurations. Shell model, realistic effective interaction, comparison with data.

doi: 10.1103/PhysRevC.66.064311
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2001CO07      Acta Phys.Pol. B32, 871 (2001)

A.Covello, L.Coraggio, A.Gargano, N.Itaco

Present Status of Realistic Shell-Model Calculations

NUCLEAR STRUCTURE 130Sn, 134Te, 206Pb calculated levels, J, π. 210Po calculated levels J, π, μ, quadrupole moments, transitions B(E2). 98Cd, 102,130Sn, 134Te, 206Pb, 210Po calculated ground-state binding energies. Shell model, comparisons with data.


2001CO21      J.Phys.(London) G27, 2351 (2001)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Two-Frequency Shell-Model Calculations for p-Shell Nuclei

NUCLEAR STRUCTURE 6,7,8,9He, 6,7,8,9Li, 6,7,8,9Be, 7,8,9B, 8,9C; calculated ground-state binding energies. 6,7,8Li, 7Be, 8B; calculated levels, J, π, B(E2), B(M1), μ, quadrupole moments. Two-frequency shell model approach, comparisons with data.

doi: 10.1088/0954-3899/27/11/313
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2001IT06      Acta Phys.Pol. B32, 2479 (2001)

N.Itaco, A.Covello, A.Gargano

Effects of Neutron-Proton Interaction in Doubly Odd Deformed Nuclei

NUCLEAR STRUCTURE 176Lu, 182Ta, 188Re; calculated levels, J, π, neutron-proton interaction effects. Particle-rotor model.


2000CO26      J.Phys.(London) G26, 1697 (2000)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Realistic Shell-Model Calculations for Proton-Rich N = 50 Isotones

NUCLEAR STRUCTURE 96Pd, 97Ag, 98Cd; calculated levels, J, π. Shell model, realistic effective interaction, comparison with data.

doi: 10.1088/0954-3899/26/11/305
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1999CO30      Phys.Rev. C60, 064306 (1999)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Bonn Potential and Shell-Model Calculations for N = 126 Isotones

NUCLEAR STRUCTURE 210Po, 211At, 212Rn; calculated levels, J, π, μ, quadrupole moments, B(λ). Shell model, comparisons with data.

doi: 10.1103/PhysRevC.60.064306
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1998CO34      Phys.Rev. C58, 3346 (1998)

L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo

Bonn Potential and Shell-Model Calculations for 206, 205, 204Pb

NUCLEAR STRUCTURE 204,205,206Pb; calculated levels, J, π. Shell model, realistic effective interaction. Comparison with data.

doi: 10.1103/PhysRevC.58.3346
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1997CO28      Phys.Rev. C56, 3092 (1997)

A.Covello, A.Gargano, N.Itaco

Tensor Force in Doubly Odd Deformed Nuclei

NUCLEAR STRUCTURE 176Lu; calculated levels, configurations; deduced space exchange, tensor forces role. Particle-rotor model.

doi: 10.1103/PhysRevC.56.3092
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