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NSR database version of March 18, 2024.

Search: Author = T.Suzuki

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2023LO09      Phys.Lett. B 845, 138149 (2023)

J.Lois-Fuentes, B.Fernandez-Dominguez, X.Pereira-Lopez, F.Delaunay, W.N.Catford, A.Matta, N.A.Orr, T.Duguet, T.Otsuka, V.Soma, O.Sorlin, T.Suzuki, N.L.Achouri, M.Assie, S.Bailey, B.Bastin, Y.Blumenfeld, R.Borcea, M.Caamano, L.Caceres, E.Clement, A.Corsi, N.Curtis, Q.Deshayes, F.Farget, M.Fisichella, G.de France, S.Franchoo, M.Freer, J.Gibelin, A.Gillibert, G.F.Grinyer, F.Hammache, O.Kamalou, A.Knapton, Tz.Kokalova, V.Lapoux, B.Le Crom, S.Leblond, F.M.Marques, P.Morfouace, J.Pancin, L.Perrot, J.Piot, E.Pollacco, D.Ramos, D.Regueira-Castro, C.Rodriguez-Tajes, T.Roger, F.Rotaru, M.Senoville, N.de Sereville, R.Smith, M.Stanoiu, I.Stefan, C.Stodel, D.Suzuki, J.C.Thomas, N.Timofeyuk, M.Vandebrouck, J.Walshe, C.Wheldon

Cross-shell states in 15C: A test for p-sd interactions

NUCLEAR REACTIONS 2H(16C, t), E=17.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ), level energies, J, π, experimental level scheme, single-particle strength, normalised spectroscopic factors. Comparison with the ab initio self-consistent Green's function method employing the NNLOsat interaction. TIARA Silicon array, three MUST2 telescopes, GANIL.

doi: 10.1016/j.physletb.2023.138149
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2023SA08      Nucl.Phys. A1032, 122618 (2023)

S.Sahoo, P.C.Srivastava, T.Suzuki

Study of structure and radii for 20-31Na isotopes using microscopic interactions

NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31Na; calculated ground state energies, energy levels, J, π, B(E2), charge and natter radii, neutron skin using different microscopic effective interactions. Comparison with available data.

doi: 10.1016/j.nuclphysa.2023.122618
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2023SU08      Phys.Rev. C 108, 014611 (2023)

T.Suzuki, N.Shimizu

Neutrino-induced neutral- and charged-current reactions on 40Ar

NUCLEAR REACTIONS 40Ar(ν, e), E=10-130 MeV; calculated σ(E), cumulative sum of the GT strength. 40Ar(ν, ν'), E=10-130 MeV; calculated neutral-current reaction σ(E) for the 1+ multipole, dependence of the σ(E) on the quenching factor. Calculations using shell model for Gamow-Teller transitions and random-phase approximation (RPA) for forbidden transitions.

NUCLEAR STRUCTURE 40Ar; calculated B(M1) and B(GT) values.

doi: 10.1103/PhysRevC.108.014611
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2023SU10      Nucl.Phys. A1038, 122719 (2023)

T.Suzuki, K.Nakazato, M.Sakuda

Neutrino-induced reactions on 18O and implications of 18O mixture in water Cherenkov detectors on supernova neutrino events

NUCLEAR REACTIONS 16,18O(ν, e-), (ν-bar, e+), (ν, ν'), E<80MeV; calculated σ; deduced contributions from Gamow-Teller transitions. Comparison with available data.

doi: 10.1016/j.nuclphysa.2023.122719
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2022AB17      Phys.Lett. B 833, 137355 (2022)

K.Abe, K.Hiraide, K.Ichimura, N.Kato, Y.Kishimoto, K.Kobayashi, M.Kobayashi, S.Moriyama, M.Nakahata, K.Sato, H.Sekiya, T.Suzuki, A.Takeda, S.Tasaka, M.Yamashita, B.S.Yang, N.Y.Kim, Y.D.Kim, Y.H.Kim, R.Ishii, Y.Itow, K.Kanzawa, K.Masuda, K.Martens, A.Mason, Y.Suzuki, K.Miuchi, Y.Takeuchi, K.B.Lee, M.K.Lee, Y.Fukuda, H.Ogawa, K.Nishijima, K.Fushimi, B.D.Xu, S.Nakamura, for the XMASS Collaboration

Search for neutrinoless quadruple beta decay of 136Xe in XMASS-I

RADIOACTIVITY 136Xe(4β-); measured decay products, Eβ, Iβ, Eγ, Iγ; deduced T1/2 lower limit. The liquid-xenon detector XMASS-I.

doi: 10.1016/j.physletb.2022.137355
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2022FU05      Few-Body Systems 63, 37 (2022)

M.Fukutome, M.Fukuda, M.Tanaka, D.Nishimura, M.Takechi, T.Ohtsubo, M.Mihara, K.Matsuta, T.Suzuki, T.Yamaguchi, T.Izumikawa, S.Sato, S.Fukuda, A.Kitagawa, H.Takahashi, Y.Kimura, S.Sugawara, K.Takatsu, G.Takayama

One-Neutron Removal Cross Sections for 16N Isomeric State

NUCLEAR REACTIONS 9Be(18O, X)16N, E=160 MeV/nucleon; 9Be(15N, X)16N, E=169 MeV/nucleon; measured reaction products; deduced one-neutron σ with different isomeric ratios. Comparison with theoretical calculations. The HIMAC synchrotron accelerator facility of the National Institute of Radiological Sciences.

doi: 10.1007/s00601-021-01721-1
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2022KA35      Phys.Rev.Lett. 129, 142502 (2022)

S.Kaur, R.Kanungo, W.Horiuchi, G.Hagen, J.D.Holt, B.S.Hu, T.Miyagi, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, S.Bagchi, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knobel, J.Kurcewicz, Y.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, T.Otsuka, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Proton Distribution Radii of 16-24O: Signatures of New Shell Closures and Neutron Skin

NUCLEAR REACTIONS 12C(16O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E<1 GeV/nucleon; measured reaction products. 16,18,20,21,22,23,24O; deduced charge changing σ, root mean square proton and matter radii, neutron skin thickness, shell closure. Comparison with with ab initio calculations employing the chiral NNLO sat interaction, shell model predictions. The fragment separator FRS at GSI.

doi: 10.1103/PhysRevLett.129.142502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8052. Data from this article have been entered in the XUNDL database. For more information, click here.


2022KU07      Prog.Theor.Exp.Phys. 2022, 023D03 (2022)

H.Kurasawa, T.Suzuki

The mean-square radius of the neutron distribution in the relativistic and non-relativistic mean-field models

NUCLEAR STRUCTURE 48Ca, 208Pb; calculated root msr of the point neutron and proton distributions with NL3, effective masses, the densities for neutrons and protons, neutron skin.

doi: 10.1093/ptep/ptac008
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2022LE07      Phys.Lett. B 829, 137057 (2022)

B.Le Crom, M.Assie, Y.Blumenfeld, J.Guillot, H.Sagawa, T.Suzuki, M.Honma, N.L.Achouri, B.Bastin, R.Borcea, W.N.Catford, E.Clement, L.Caceres, M.Caamano, A.Corsi, G.De France, F.Delaunay, N.De Sereville, B.Fernandez-Dominguez, M.Fisichella, S.Franchoo, A.Georgiadou, J.Gibelin, A.Gillibert, F.Hammache, O.Kamalou, A.Knapton, V.Lapoux, S.Leblond, A.O.Macchiavelli, F.M.Marques, A.Matta, L.Menager, P.Morfouace, N.A.Orr, J.Pancin, X.Pereira-Lopez, L.Perrot, J.Piot, E.Pollacco, D.Ramos, T.Roger, F.Rotaru, A.M.Sanchez-Benitez, M.Senoville, O.Sorlin, M.Stanoiu, I.Stefan, C.Stodel, D.Suzuki, J.-C.Thomas, M.Vandebrouck

Neutron-proton pairing in the N=Z radioactive fp-shell nuclei 56Ni and 52Fe probed by pair transfer

NUCLEAR REACTIONS 1H(56Ni, 3He)54Co, E=30.5 MeV/nucleon; 1H(52Fe, 3He)50Mn, E=31.2 MeV/nucleon; measured reaction products; deduced yields, σ(θ), partial level schemes, J, π, isovector and isoscalar components of neutron-proton pairing. Comparison with with second-order distorted-wave Born approximation (DWBA) calculations. GANIL/LISE facility, MUST2 telescopes.

doi: 10.1016/j.physletb.2022.137057
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022SA22      Phys.Lett. B 829, 137072 (2022)

H.Sagawa, S.Yoshida, T.Naito, T.Uesaka, J.Zenihiro, J.Tanaka, T.Suzuki

Isovector density and isospin impurity in 40Ca

NUCLEAR STRUCTURE 40Ca; calculated proton and neutron densities with modified occupation probabilities of orbits around the Fermi energy, isospin impurity; deduced isoscalar (IS) and isovector (IV) densities. Comparison with theoretical densities calculated by Skyrme Hatree-Fock (HF) models.

doi: 10.1016/j.physletb.2022.137072
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2022SH35      Phys.Rev. C 106, 024333 (2022)

S.Sharma, P.C.Srivastava, A.Kumar, T.Suzuki

Shell-model description for the properties of the forbidden β- decay in the region "northeast" of 208Pb

RADIOACTIVITY 210,211,212,213,214,215Pb, 210,211,212,213,214,214m,215Bi(β-); calculated logft for forbidden nonunique and forbidden unique β-decay, T1/2, Q, shape factors. Shell-model calculation using the KHPE interaction in valence shells 82-126 for protons and 126-184 for neutrons without any truncation. Comparison to experimental data.

NUCLEAR STRUCTURE 214Po; calculated levels J, π. Shell model calculations.

doi: 10.1103/PhysRevC.106.024333
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2022SU11      Prog.Theor.Exp.Phys. 2022, 063D01 (2022)

T.Suzuki

The relationship of the neutron skin thickness to the symmetry energy and its slope

NUCLEAR STRUCTURE 208Pb; calculated neutron skin thickness using the relational formula is derived on the basis of the Hugenholtz-Van Hove theorem in the mean-field (MF) approximation for nuclear matter.

doi: 10.1093/ptep/ptac083
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2022SU25      Prog.Part.Nucl.Phys. 126, 103974 (2022)

T.Suzuki

Nuclear weak rates and nuclear weak processes in stars

NUCLEAR REACTIONS 20Ne, 56Ni, 31Al, 78Ni(e-, ν), E<1 MeV; calculate total capture rates, shape factors, averaged neutrino energy and averaged energy production, explosion-collapse bifurcation diagram, GT strengths, electron-capture rates using with GXPF1J, KBF and KB3G interactions as a function of temperature at densities. Comparison with available data.

doi: 10.1016/j.ppnp.2022.103974
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2022TA12      Phys.Rev. C 106, 014617 (2022)

M.Tanaka, M.Takechi, A.Homma, A.Prochazka, M.Fukuda, D.Nishimura, T.Suzuki, T.Moriguchi, D.S.Ahn, A.Aimaganbetov, M.Amano, H.Arakawa, S.Bagchi, K.-H.Behr, N.Burtebayev, K.Chikaato, H.Du, T.Fujii, N.Fukuda, H.Geissel, T.Hori, S.Hoshino, R.Igosawa, A.Ikeda, N.Inabe, K.Inomata, K.Itahashi, T.Izumikawa, D.Kamioka, N.Kanda, I.Kato, I.Kenzhina, Z.Korkulu, Y.Kuk, K.Kusaka, K.Matsuta, M.Mihara, E.Miyata, D.Nagae, S.Nakamura, M.Nassurlla, K.Nishimuro, K.Nishizuka, K.Ohnishi, M.Ohtake, T.Ohtsubo, S.Omika, H.J.Ong, A.Ozawa, H.Sakurai, C.Scheidenberger, Y.Shimizu, T.Sugihara, T.Sumikama, H.Suzuki, S.Suzuki, H.Takeda, Y.Tanaka, Y.K.Tanaka, I.Tanihata, T.Wada, K.Wakayama, S.Yagi, T.Yamaguchi, R.Yanagihara, Y.Yanagisawa, K.Yoshida, T.K.Zholdybayev

Charge-changing cross sections for 42-51Ca and effect of charged-particle evaporation induced by neutron-removal reactions

NUCLEAR REACTIONS 12C(42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=280 MeV/nucleon; measured reaction products; deduced charge-exchange σ. Comparison to Glauber-like model calculations. Observed significant decrease of charge-exchange cross-section with increase of point-proton radius and attributed this effect to attributed to the charged-particle evaporation induced by the neutron-removal reaction. Used the conclusions of the present work to re-analyze charge-exchange σ for Be, B, C, N, O, F, Si, Ti, Ca, Fe isotopes. BigRIPS fragment separator at RI Beam Factory (RIBF).

doi: 10.1103/PhysRevC.106.014617
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2733.


2022YU06      Phys.Rev. C 106, 044314 (2022)

C.Yuan, M.Liu, N.Shimizu, Z.Podolyak, T.Suzuki, T.Otsuka, Z.Liu

Shell-model study on spectroscopic properties in the region "south" of 208Pb

NUCLEAR STRUCTURE 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213Tl, 198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217Pb, 198,199,200,201,202,203,204,205,206,207,208,209,210,211Hg, 198,199,200,201,202,203,204,205,206,207,208,209Au, 198,199,200,201,202,203,204,205,206,207Pt, 198,199,200,201,202,203,204Ir, 198,199,200,201,202,203Os, 198,199,200,201,202Re, 197,198,199,200,201W; calculated levels J, π, configurations, T1/2, effective single-particle energies, B(E2), binding energies, S(n), proton and neutron E2 transition matrix elements, electric quadrupole moments, magnetic dipole moments. Large-scale shell-model calculations with combined KHHE (with adjustment of its proton-proton part) and KHPE Hamiltonians and the monopole-based universal interaction. Comparison to experimental results and AME2020 data.

doi: 10.1103/PhysRevC.106.044314
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2021CH17      Phys.Rev. C 103, L031302 (2021)

J.Chen, S.M.Wang, H.T.Fortune, J.L.Lou, Y.L.Ye, Z.H.Li, N.Michel, J.G.Li, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, D.Y.Pang, F.R.Xu, W.Zuo, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, H.J.Ong, E.Ideguchi, Y.Ayyad, K.Hatanaka, D.T.Tran, D.Bazin, J.Lee, Y.N.Zhang, J.Wu, H.N.Liu, C.Wen, T.Yamamoto, M.Tanaka, T.Suzuki

Observation of the near-threshold intruder 0- resonance in 12Be

NUCLEAR REACTIONS 2H(11Be, p)12Be, E=26.9 MeV/nucleon; measured E(p), I(p), σ(θ) using two parallel-plate avalanche counters (PPACs), and a set of annular double-sided silicon detectors (ADSSDs) at the RCNP, Osaka University. 12Be; deduced missing-mass spectra of 12Be unbound states, levels, J, π, a 0- resonance just above S(n), decay width. DWBA analysis. Comparison with Gamow coupled-channel and Gamow shell-model calculations.

doi: 10.1103/PhysRevC.103.L031302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2690. Data from this article have been entered in the XUNDL database. For more information, click here.


2021CH26      Phys.Rev. C 103, 064325 (2021)

P.Choudhary, A.Kumar, P.C.Srivastava, T.Suzuki

Structure of 46, 47Ca from the β- decay of 46, 47K in the framework of the nuclear shell model

NUCLEAR STRUCTURE 46,47Ca, 46,47K; calculated levels, J, π, B(E2), electric quadrupole and magnetic dipole moments, configurations using shell-model in sd-pf-valence space with the SDPF-MU interaction. Comparison with experimental data.

RADIOACTIVITY 46,47K(β-); calculated logft values for various transitions and compared with recent experimental data from GRIFFIN spectrometer at the TRIUMF-ISAC facility. Shell model calculations.

doi: 10.1103/PhysRevC.103.064325
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2021KU01      Prog.Theor.Exp.Phys. 2021, 013D02 (2021)

H.Kurasawa, T.Suda, T.Suzuki

The mean square radius of the neutron distribution and the skin thickness derived from electron scattering

NUCLEAR REACTIONS 40,48Ca, 208Pb(e-, e-'), E not given; analyzed available data; calculated the second-order moment of the nuclear charge density, mean square radius of the point proton distribution, the fourth-order momentum, mean square radius of the point neutron distribution; deduced the skin thickness.

doi: 10.1093/ptep/ptaa177
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2021SA05      Phys.Rev. C 103, 014308 (2021)

M.Sasano, H.Sagawa, T.Suzuki, M.Honma

Energy-weighted sum rule for Gamow-Teller giant resonances in high-spin isomeric states of N = Z nuclei

NUCLEAR STRUCTURE 52mFe, 94mAg; calculated energies of Gamow-Teller (GT) giant resonances and isoscalar M1 transitions in N=Z nuclei, (12+) and (21+) isomeric high-spin state of 52Fe and 94Ag, respectively; extracted energy-weighted sum rules (EWSR). Comparison with large-scale shell-model calculations. Relevance to evaluation of short-range part of the spin residual interaction, to describe the onset of the pion condensation in nuclear matter.

doi: 10.1103/PhysRevC.103.014308
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2021SU17      Few-Body Systems 62, 32 (2021)

T.Suzuki, T.Otsuka

Structure of Two-Neutron Halo in Light Exotic Nuclei

NUCLEAR STRUCTURE 22C, 29F, 18O, 17,19B; calculated rms radii, energy levels, J, π; deduced two-neutron halo with a three-body model using the neutron-neutron interaction fixed at the low-energy scattering limit. Comparison with experimental values.

doi: 10.1007/s00601-021-01612-5
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2021ZI01      Phys.Rev. C 104, L041301 (2021)

S.Ziliani, M.Ciemala, F.C.L.Crespi, S.Leoni, B.Fornal, T.Suzuki, T.Otsuka, A.Maj, P.Bednarczyk, G.Benzoni, A.Bracco, C.Boiano, S.Bottoni, S.Brambilla, M.Bast, M.Beckers, T.Braunroth, F.Camera, N.Cieplicka-Orynczak, E.Clement, S.Coelli, O.Dorvaux, S.Erturk, G.de France, C.Fransen, A.Goldkuhle, J.Grebosz, M.N.Harakeh, L.W.Iskra, B.Jacquot, A.Karpov, M.Kicinska-Habior, Y.Kim, M.Kmiecik, A.Lemasson, S.M.Lenzi, M.Lewitowicz, H.Li, I.Matea, K.Mazurek, C.Michelagnoli, M.Matejska-Minda, B.Million, C.Muller-Gatermann, V.Nanal, P.Napiorkowski, D.R.Napoli, R.Palit, M.Rejmund, Ch.Schmitt, M.Stanoiu, I.Stefan, E.Vardaci, B.Wasilewska, O.Wieland, M.Zieblinski, M.Zielinska

Complete set of bound negative-parity states in the neutron-rich nucleus 18N

NUCLEAR REACTIONS 181Ta(18O, X)18N, E=126 MeV; measured reaction products, A/Q versus ion charge Q identification plot using VAMOS++ spectrometer at GANIL accelerator facility, Doppler-corrected Eγ, Iγ, γγ-coin using the γ-tracking array AGATA. 18N; deduced levels, J, π, configurations. Comparison with shell-model calculations using YSOX interactions, and with previous experimental data.

NUCLEAR STRUCTURE 16,18N; calculated levels, J, π using shell-model with YSOX interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.L041301
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2020BA27      Phys.Rev.Lett. 124, 222504 (2020)

S.Bagchi, R.Kanungo, Y.K.Tanaka, H.Geissel, P.Doornenbal, W.Horiuchi, G.Hagen, T.Suzuki, N.Tsunoda, D.S.Ahn, H.Baba, K.Behr, F.Browne, S.Chen, M.L.Cortes, A.Estrade, N.Fukuda, M.Holl, K.Itahashi, N.Iwasa, G.R.Jansen, W.G.Jiang, S.Kaur, A.O.Macchiavelli, S.Y.Matsumoto, S.S.Momiyama, I.Murray, T.Nakamura, S.J.Novario, H.J.Ong, T.Otsuka, T.Papenbrock, S.Paschalis, A.Prochazka, C.Scheidenberger, P.Schrock, Y.Shimizu, D.Steppenbeck, H.Sakurai, D.Suzuki, H.Suzuki, M.Takechi, H.Takeda, S.Takeuchi, R.Taniuchi, K.Wimmer, K.Yoshida

Two-Neutron Halo is Unveiled in 29F

NUCLEAR REACTIONS C(29F, X), E=255 MeV/nucleon; C(27F, X), E=250 MeV/nucleon; measured reaction products, En, In. 27,29F; deduced two-neutron Borromean halo. Comparison with theoretical calculations.

doi: 10.1103/PhysRevLett.124.222504
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2672. Data from this article have been entered in the XUNDL database. For more information, click here.


2020KU10      Prog.Theor.Exp.Phys. 2020, 033D01 (2020)

A.Kumar, P.C .Srivastava, T.Suzuki

Shell model results for nuclear β--decay properties of sd-shell nuclei

RADIOACTIVITY 15,20,21,22,24O, 20,21,22,23,26F, 23,24,25,26,27,28Ne, 24,25,26,27,28,29,30Na, 27,28,29,30,32Mg, 28,29,30,32,33Al, 31,32,33,34Si, 32,33,34P(β-); calculated M(GT) matrix elements, log ft, T1/2 using the framework of the nuclear shell model using the valence space Hamiltonians derived from modern ab initio methods, such as in-medium similarity renormalization group and coupled-cluster theory. Comparison with available data.

doi: 10.1093/ptep/ptaa012
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2020MO05      Nucl.Phys. A994, 121663 (2020)

T.Moriguchi, M.Amano, A.Ozawa, W.Horiuchi, Y.Abe, T.Fujii, R.Kagesawa, D.Kamioka, A.Kitagawa, M.Mukai, D.Nagae, M.Sakaue, S.Sato, S.Suzuki, T.Suzuki, T.Yamaguchi, K.Yokota

Energy dependence of total reaction cross sections for 17Ne on a proton target

doi: 10.1016/j.nuclphysa.2019.121663
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2669.


2020OT02      Rev.Mod.Phys. 92, 015002 (2020)

T.Otsuka, A.Gade, O.Sorlin, T.Suzuki, Y.Utsuno

Evolution of shell structure in exotic nuclei

NUCLEAR STRUCTURE Z=8-126; analyzed available data; deduced changes in magic numbers for hort-lived, so-called exotic nuclei or rare isotopes, characterized by a large N=Z asymmetry and located far from the valley of β stability on the nuclear chart.

doi: 10.1103/RevModPhys.92.015002
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2020PE15      Phys.Lett. B 811, 135939 (2020)

X.Pereira-Lopez, B.Fernandez-Dominguez, F.Delaunay, N.L.Achouri, N.A.Orr, W.N.Catford, M.Assie, S.Bailey, B.Bastin, Y.Blumenfeld, R.Borcea, M.Caamano, L.Caceres, E.Clement, A.Corsi, N.Curtis, Q.Deshayes, F.Farget, M.Fisichella, G.de France, S.Franchoo, M.Freer, J.Gibelin, A.Gillibert, G.F.Grinyer, F.Hammache, O.Kamalou, A.Knapton, T.Kokalova, V.Lapoux, J.A.Lay, B.Le Crom, S.Leblond, J.Lois-Fuentes, F.M.Marques, A.Matta, P.Morfouace, A.M.Moro, T.Otsuka, J.Pancin, L.Perrot, J.Piot, E.Pollacco, D.Ramos, C.Rodriguez-Tajes, T.Roger, F.Rotaru, M.Senoville, N.de Sereville, R.Smith, O.Sorlin, M.Stanoiu, I.Stefan, C.Stodel, D.Suzuki, T.Suzuki, J.C.Thomas, N.Timofeyuk, M.Vandebrouck, J.Walshe, C.Wheldon

Low-lying single-particle structure of 17C and the N=14 sub-shell closure

NUCLEAR REACTIONS 2H(16C, p)17C, E=17.2 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ), γ-ray energies, J, π, level scheme, spectroscopic factors. Comparison with shell model and particle-core model calculations.

doi: 10.1016/j.physletb.2020.135939
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8032. Data from this article have been entered in the XUNDL database. For more information, click here.


2020TA05      Phys.Rev.Lett. 124, 102501 (2020)

M.Tanaka, M.Takechi, A.Homma, M.Fukuda, D.Nishimura, T.Suzuki, Y.Tanaka, T.Moriguchi, D.S.Ahn, A.Aimaganbetov, M.Amano, H.Arakawa, S.Bagchi, K.-H.Behr, N.Burtebayev, K.Chikaato, H.Du, S.Ebata, T.Fujii, N.Fukuda, H.Geissel, T.Hori, W.Horiuchi, S.Hoshino, R.Igosawa, A.Ikeda, N.Inabe, K.Inomata, K.Itahashi, T.Izumikawa, D.Kamioka, N.Kanda, I.Kato, I.Kenzhina, Z.Korkulu, Y.Kuk, K.Kusaka, K.Matsuta, M.Mihara, E.Miyata, D.Nagae, S.Nakamura, M.Nassurlla, K.Nishimuro, K.Nishizuka, K.Ohnishi, M.Ohtake, T.Ohtsubo, S.Omika, H.J.Ong, A.Ozawa, A.Prochazka, H.Sakurai, C.Scheidenberger, Y.Shimizu, T.Sugihara, T.Sumikama, H.Suzuki, S.Suzuki, H.Takeda, Y.K.Tanaka, I.Tanihata, T.Wada, K.Wakayama, S.Yagi, T.Yamaguchi, R.Yanagihara, Y.Yanagisawa, K.Yoshida, T.K.Zholdybayev

Swelling of Doubly Magic 48Ca Core in Ca Isotopes beyond N=28

NUCLEAR REACTIONS C(42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=280 MeV/nucleon; measured reaction products. 42,43,44,45,46,47,48,49,50,51Ca; deduced neutron number dependence in root-mean-square matter radii, novel growth in neutron skin thickness. Comparison with mean field calculations.

doi: 10.1103/PhysRevLett.124.102501
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2020TS03      Nature(London) 587, 66 (2020)

N.Tsunoda, T.Otsuka, K.Takayanagi, N.Shimizu, T.Suzuki, Y.Utsuno, S.Yoshida, H.Ueno

The impact of nuclear shape on the emergence of the neutron dripline

NUCLEAR STRUCTURE 22,24,26,28,30,32,34,36Ne, 24,26,28,30,32,34,36,38,40,42Mg, 23,25,27,29,31,33,35,37Na, 19,21,23,25,27,29F; analyzed available data; calculated 2+ and 4+ energies using configuration interaction, ground-state energies, dripline, magic numbers, J, π and energy levels using nucleon-nucleon interactions, nuclear shapes. Comparison with ENSDF library, available data; deduced mechanism for the formation of the neutron dripline.

doi: 10.1038/s41586-020-2848-x
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2019AJ01      Phys.Lett. B 789, 620 (2019)

S.Ajimura, H.Asano, G.Beer, C.Berucci, H.Bhang, M.Bragadireanu, P.Buehler, L.Busso, M.Cargnelli, S.Choi, C.Curceanu, S.Enomoto, H.Fujioka, Y.Fujiwara, T.Fukuda, C.Guaraldo, T.Hashimoto, R.S.Hayano, T.Hiraiwa, M.Iio, M.Iliescu, K.Inoue, Y.Ishiguro, T.Ishikawa, S.Ishimoto, K.Itahashi, M.Iwasaki, K.Kanno, K.Kato, Y.Kato, S.Kawasaki, P.Kienle, H.Kou, Y.Ma, J.Marton, Y.Matsuda, Y.Mizoi, O.Morra, T.Nagae, H.Noumi, H.Ohnishi, S.Okada, H.Outa, K.Piscicchia, Y.Sada, A.Sakaguchi, F.Sakuma, M.Sato, A.Scordo, M.Sekimoto, H.Shi, K.Shirotori, D.Sirghi, F.Sirghi, K.Suzuki, S.Suzuki, T.Suzuki, K.Tanida, H.Tatsuno, M.Tokuda, D.Tomono, A.Toyoda, K.Tsukada, O.Vazquez Doce, E.Widmann, T.Yamaga, T.Yamazaki, Q.Zhang, J.Zmeskal

"K-pp", a K-bar-meson nuclear bound state, observed in 3He(K-, Λp)n reactions

NUCLEAR REACTIONS 3He(K-, Λp), E ∼ 1 GeV; measured reaction products; deduced a distinct peak in the Λp invariant mass spectrum.

doi: 10.1016/j.physletb.2018.12.058
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2019BA11      Phys.Lett. B 790, 251 (2019)

S.Bagchi, R.Kanungo, W.Horiuchi, G.Hagen, T.D.Morris, S.R.Stroberg, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, S.Kaur, R.Knobel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, Y.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Neutron skin and signature of the N = 14 shell gap found from measured proton radii of 17-22N

NUCLEAR REACTIONS C(14N, X), (15N, X), (17N, X), (18N, X), (19N, X), (20N, X), (21N, X), (22N, X), E=851-932 MeV/nucleon; measured reaction products. 14,15,17,18,19,20,21,22N; deduced σ, root mean square point proton and matter radii, unconventional shell gap at N = 14 arising from the attractive proton–neutron tensor interaction. Comparison with ab initio calculations.

doi: 10.1016/j.physletb.2019.01.024
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2019BU28      Acta Phys.Pol. B50, 703 (2019)

N.Burtebayev, Zh.K.Kerimkulov, M.Nassurlla, J.T.Burtebayeva, M.Nassurlla, S.B.Sakuta, T.Suzuki, K.Rusek, A.Trzcinska, M.Wolinska-Cichocka

Study of the 7Li(d, t)6Li Reaction at the Energy of 14.5 MeV

NUCLEAR REACTIONS 7Li(d, t), E=14.5 MeV; measured reaction products; deduced elastic and inelastic σ(θ). Comparison with coupled reaction channels (CRC) calculations.

doi: 10.5506/aphyspolb.50.703
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2019FU06      Phys.Rev. C 100, 034618 (2019)

H.Fujita, Y.Fujita, Y.Utsuno, K.Yoshida, T.Adachi, A.Algora, M.Csatlos, J.M.Deaven, E.Estevez Aguado, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, R.Hutton, D.Ishikawa, A.Krasznahorkay, H.Matsubara, F.Molina, H.Okamura, H.J.Ong, G.Perdikakis, B.Rubio, C.Scholl, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, R.G.T.Zegers, J.Zenihiro

Experimental study of Gamow-Teller transitions via the high-energy-resolution 18O(3He, t)18F reaction: Identification of the low-energy "super"-Gamow-Teller state

NUCLEAR REACTIONS 18O(3He, t)18F, E=140 MeV/nucleon; measured E(t), I(t), angular distribution of tritons using Grand Raiden magnetic spectrometer at RCNP facility. 18F; deduced levels, J, π, L-transfers, widths, B(GT) Gamow-Teller strengths, low-energy super Gamow-Teller (LeSGT) state. DWBA analysis. Comparison with previous experimental and evaluated data, and with shell-model calculations using USDA, USDB and modified-PSDWBT interactions, and quasiparticle-random-phase approximation (QRPA) calculations.

doi: 10.1103/PhysRevC.100.034618
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2019KU20      Prog.Theor.Exp.Phys. 2019, 113D01 (2019)

H.Kurasawa, T.Suzuki

The nth-order moment of the nuclear charge density and contribution from the neutrons

NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated mean square radius of the charge distribution, fourth-order moment of the charge distribution.

doi: 10.1093/ptep/ptz121
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2019OZ03      Phys.Lett. B 797, 134800 (2019)

F.C.Ozturk, B.Akkus, D.Atanasov, H.Beyer, F.Bosch, D.Boutin, C.Brandau, P.Buhler, R.B.Cakirli, R.J.Chen, W.D.Chen, X.C.Chen, I.Dillmann, C.Dimopoulou, W.Enders, H.G.Essel, T.Faestermann, O.Forstner, B.S.Gao, H.Geissel, R.Gernhauser, R.E.Grisenti, A.Gumberidze, S.Hagmann, T.Heftrich, M.Heil, M.O.Herdrich, P.-M.Hillenbrand, T.Izumikawa, P.Kienle, C.Klaushofer, C.Kleffner, C.Kozhuharov, R.K.Knobel, O.Kovalenko, S.Kreim, T.Kuhl, C.Lederer-Woods, M.Lestinsky, S.A.Litvinov, Yu.A.Litvinov, Z.Liu, X.W.Ma, L.Maier, B.Mei, H.Miura, I.Mukha, A.Najafi, D.Nagae, T.Nishimura, C.Nociforo, F.Nolden, T.Ohtsubo, Y.Oktem, S.Omika, A.Ozawa, N.Petridis, J.Piotrowski, R.Reifarth, J.Rossbach, R.Sanchez, M.S.Sanjari, C.Scheidenberger, R.S.Sidhu, H.Simon, U.Spillmann, M.Steck, Th.Stohlker, B.H.Sun, L.A.Susam, F.Suzaki, T.Suzuki, S.Yu.Torilov, C.Trageser, M.Trassinelli, S.Trotsenko, X.L.Tu, P.M.Walker, M.Wang, G.Weber, H.Weick, N.Winckler, D.F.A.Winters, P.J.Woods, T.Yamaguchi, X.D.Xu, X.L.Yan, J.C.Yang, Y.J.Yuan, Y.H.Zhang, X.H.Zhou

New test of modulated electron capture decay of hydrogen-like 142Pm ions: Precision measurement of purely exponential decay

RADIOACTIVITY 142Pm(EC); measured decay products; deduced T1/2.

doi: 10.1016/j.physletb.2019.134800
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Data from this article have been entered in the XUNDL database. For more information, click here.


2019RE08      Phys.Rev. C 100, 024615 (2019)

M.S.Reen, I.Ou, T.Sudo, D.Fukuda, T.Mori, A.Ali, Y.Koshio, M.Sakuda, A.Tamii, N.Aoi, M.Yosoi, E.Ideguchi, T.Suzuki, T.Yamamoto, C.Iwamoto, T.Kawabata, S.Adachi, M.Tsumura, M.Murata, T.Furuno, H.Akimune, T.Yano, T.Suzuki, R.Dhir

Measurement of γ rays from giant resonances excited by the 12C(p, p') reaction at 392 MeV and 0 degrees

NUCLEAR REACTIONS 12C(p, p')12C, E=392 MeV; measured Eγ, Iγ, Ep, Ip, pγ-coin, σ(θ) from 0-3.5° using magnetic spectrometer Grand Raiden and NaI(Tl) detectors at the Research Center for Nuclear Physics (RCNP), Osaka University, Japan; deduced differential cross section, γ-ray emission probability; cross section decomposed into spin-flip and non-spin-flip components. Angular distributions compared with DWBA calculations. 12C; deduced levels, resonances in the 16-32 MeV range, J, π, widths, σ, γ-ray spectra from giant resonances in 12C. 11B, 11C; deduced levels, J, π, γ-ray energies and emission probabilities in daughter nuclei 11B and 11C populated from the decay of 12C resonances. Comparison of the measured γ-ray emission probabilities with statistical model calculation based on the Hauser-Feshbach formalism.

doi: 10.1103/PhysRevC.100.024615
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2019SA23      Hyperfine Interactions 240, 37 (2019)

A.Saxena, A.Kumar, V.Kumar, P.C.Srivastava, T.Suzuki

Ab initio description of collectivity for sd shell nuclei

NUCLEAR STRUCTURE 20Ne, 24,32Mg, 34Si; calculated energy levels, J, π, B(E2) values. Comparison with experimental data.

doi: 10.1007/s10751-019-1582-y
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2019SU05      Astropart.Phys. 110, 1 (2019)

T.Suzuki, K.Abe, K.Hiraide, K.Ichimura, Y.Kishimoto, K.Kobayashi, M.Kobayashi, S.Moriyama, M.Nakahata, H.Ogawa, K.Sato, H.Sekiya, A.Takeda, S.Tasaka, M.Yamashita, B.S.Yang, N.Y.Kim, Y.D.Kim, Y.Itow, K.Kanzawa, K.Masuda, K.Martens, Y.Suzuki, B.D.Xu, K.Miuchi, N.Oka, Y.Takeuchi, Y.H.Kim, K.B.Lee, M.K.Lee, Y.Fukuda, M.Miyasaka, K.Nishijima, K.Fushimi, G.Kanzaki, S.Nakamura, for the XMASS Collaboration

Search for WIMP-129Xe inelastic scattering with particle identification in XMASS-I

doi: 10.1016/j.astropartphys.2019.02.007
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2019SU18      Astrophys.J. 881, 64 (2019)

T.Suzuki, S.Zha, S.-C.Leung, K.Nomoto

Electron-capture Rates in 20Ne for a Forbidden Transition to the Ground State of 20F Relevant to the Final Evolution of High-density O-Ne-Mg Cores

RADIOACTIVITY 20Ne(EC); analyzed available data; deduced evaluated capture rates.

doi: 10.3847/1538-4357/ab2b93
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2019SU19      Astrophys.J. 881, 64 (2019)

T.Suzuki, S.Zha, S.-C.Leung, K.Nomoto

Electron-capture Rates in 20Ne for a Forbidden Transition to the Ground State of 20F Relevant to the Final Evolution of High-density O-Ne-Mg Cores

RADIOACTIVITY 20Ne(EC); calculated electron capture rates, σ. Comparison with available data.

doi: 10.3847/1538-4357/ab2b93
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2019SU21      J.Phys.(London) G46, 075103 (2019)

T.Suzuki, A.B.Balantekin, T.Kajino, S.Chiba

Neutrino-13C cross sections at supernova neutrino energies

NUCLEAR REACTIONS 13C(ν, E), (ν, ν), E<50 MeV; calculated σ. Comparison with available data.

doi: 10.1088/1361-6471/ab1c11
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2018CH31      Phys.Lett. B 781, 412 (2018)

J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, D.Y.Pang, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, F.R.Xu, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki

A new measurement of the intruder configuration in 12Be

NUCLEAR REACTIONS 11Be(d, p), E=26.9 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), low-lying isomeric 0+ states, J, π, spectroscopic factors. Comparison with available data.

doi: 10.1016/j.physletb.2018.04.016
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2604. Data from this article have been entered in the XUNDL database. For more information, click here.


2018CH38      Phys.Rev. C 98, 014616 (2018)

J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, D.Y.Pang, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, F.R.Xu, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, G.Li, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki

Low-lying states in 12Be using one-neutron transfer reaction

NUCLEAR REACTIONS 1,2H(11Be, 11Be), (11Be, p), E=26.9 MeV/nucleon; measured recoils, Ep, Ip, p(θ), Eγ and Iγ from decay of recoils, (recoil)p-coin, differential σ(θ) for low-lying 0+, 2+ and 1- states in 12Be, half-life of excited 0+ isomer by decay-tagging method using (CH2)n and (CD2)n targets, annular silicon detectors (ADSSD) for protons, detector telescopes for charged particle detection, and scintillation detectors for γ detection, and isomer-tagging method at RCNP-Osaka. DWBA analysis of σ(θ) data. 12Be; deduced levels, J, π, spectroscopic factors, single-particle components in the g.s. and excited 0+ state. Comparison with shell-model calculations, and with previous experimental results. 11,12Be; calculated B(E2), B(E1), S(n) and S(2n) from shell-model, and compared with experimental data in literature.

doi: 10.1103/PhysRevC.98.014616
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2018JI04      Chin.Phys.Lett. 35, 082501 (2018)

Y.Jiang, J.-L.Lou, Y.-L.Ye, D.-Y.Pang, J.Chen, Z.-H.Li, Y.-C.Ge, Q.-T.Li, J.Li, W.Jiang, Y.-Le.Sun, H.-L.Zang, Y.Zhang, W.Liu, Y.-D.Chen, G.Li, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.-N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, T.T.Nguyen

A New Measurement of 11Be(p, d) Transfer Reaction

NUCLEAR REACTIONS 1H(11Be, d), E=26.9 MeV/nucleon; measured reaction products. 10Be; deduced Q-value spectrum, σ(θ), spectroscopic factors to 0+ and 2+. Comparison with theoretical calculations.

doi: 10.1088/0256-307X/35/8/082501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0092. Data from this article have been entered in the XUNDL database. For more information, click here.


2018LI32      Phys.Rev. C 98, 014311 (2018)

H.Z.Liang, H.Sagawa, M.Sasano, T.Suzuki, M.Honma

Gamow-Teller transitions from high-spin isomers in N = Z nuclei

RADIOACTIVITY 52Fe, 94Ag(β-); calculated Gamow-Teller transition strength distributions from 12+ isomeric state and g.s. in 52Fe and 21+ isomeric state and g.s. in 94Ag using sum-rule approach and shell model calculations; deduced stronger Gamow-Teller strengths from the high-spin states as compared to those from the low-spin ground states.

doi: 10.1103/PhysRevC.98.014311
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2018SA10      Phys.Rev. C 97, 024310 (2018)

A.Saxena, P.C.Srivastava, T.Suzuki

Ab initio calculations of Gamow-Teller strengths in the sd shell

NUCLEAR REACTIONS 20Ne(n, p), E*<10 MeV; 23Ne(3He, t), E*<12 MeV; 23Na(n, p), E*<4 MeV; 24Mg(t, 3He), (d, 2He), E*<7 MeV; 24Mg(3He, t), (p, n), E*<7 MeV; 25Mg(3He, t), E*<6 MeV; 26Mg(t, 3He), (d, 2He), E*<5 MeV; 26Mg(3He, t), (p, n), E*<18 MeV; 27Mg(3He, t), E*<10 MeV; 28Si(3He, t), (p, n), E*<12 MeV; 31P(n, p), E*<5 MeV; 32S(d, 2He), E*<8 MeV; calculated Gamow-Teller transition-strength distributions B(GT) using shell model and ab initio effective interactions: coupled-cluster effective interaction (CCEI), in-medium similarity renormalization group (IM-SRG), and phenomenological USDB effective interaction. Comparison with experimental data. 23Na(e-, ν)23Ne, 25Mg(e-, ν)25Na, T9=8.6-9.6; calculated electron-capture rates at high densities and high temperatures using shell-model and different effective interactions CCEI, IM-SRG, USDB, USDB*.

RADIOACTIVITY 26Si(β+); calculated Gamow-Teller transition-strength distribution B(GT) using shell model and ab initio effective interactions: CCEI, IM-SRG, and USDB. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.024310
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2018SA18      Phys.Rev. C 97, 054333 (2018)

H.Sagawa, T.Suzuki

Isoscalar and isovector spin response in sd-shell nuclei

NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated isoscalar (IS) and isovector (IV) differential B(M1)(E), summed IS and IV B(M1) strengths, and proton-neutron spin-spin correlations by shell model calculations using USDB effective interaction with and without IS spin-triplet pairing matrices and effective IV spin operator. 12C; IS and IV 1+ states, and B(M1) used as reference. A=19, 21, 23, 25, 27, 29, 31, 33, 35, 37; calculated effect of effective spin operators and enhanced IS pairing on β-decay rates between mirror nuclei with T=1/2 and Tz=+1/2 and -1/2, and IS magnetic moments in sd-shell mirror nuclei using shell-model and USDB and USDB** interactions with the bare spin g factor, as well as with USDBqGT and USDB**qGT with Towner's effective Gamow-Teller operator. Comparison with experimental values.

doi: 10.1103/PhysRevC.97.054333
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2018SU20      Phys.Rev. C 98, 034613 (2018)

T.Suzuki, S.Chiba, T.Yoshida, K.Takahashi, H.Umeda

Neutrino-nucleus reactions on 16O based on new shell-model Hamiltonians

NUCLEAR REACTIONS 16O(ν, e-)16F, 16O(ν-bar, e+)16N, 16O(ν, ν'), 16O(ν, e-p)15O, 16O(ν, e-np)14O, 16O(ν, e-pp)14N, 16O(ν, e-3He)13N, 16O(ν, e-α)12N, 16O(ν, e-p3He)12C, 16O(ν, e-pα)11C, 16O(ν-bar, e+n)15N, 16O(ν-bar, e+np)14C, 16O(ν-bar, e+nn)14N, 16O(ν-bar, e+t)13C, 16O(ν-bar, e+α)12B, 16O(ν-bar, e+nα)11B, 16O(ν, ν'n)15O, 16O(ν, ν'p)15N, 16O(ν, ν'np)14N, 16O(ν, ν'pp)14C, 16O(ν, ν't)13N, 16O(ν, ν'3He)13C, 16O(ν, ν'α)12C, 16O(ν, ν'nα)11C, 16O(ν, ν'pα)11B, E=0-100 MeV; calculated 16O spin-dipole strength, total σ(E), partial σ(E) from each multipole of excited product nucleus or single- and multi-particle emission channels using shell-model with new Hamiltonian SFO-tls, and branching ratios for various channels from Hauser-Feshbach statistical model. Comparison with other theoretical predictions. Discussed production yields of 6,7Li, 7,9Be, 10,11B, 11C from supernova simulations using theoretical reaction cross sections. Discussed effects of multiparticle emission channels on nucleosynthesis in core-collapse supernova explosion. Relevance to supernova (SN) neutrino detection at the Super-Kamiokande.

doi: 10.1103/PhysRevC.98.034613
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2017DU04      Acta Phys.Pol. B48, 473 (2017)

H.Du, M.Fukuda, D.Nishimura, M.Takechi, T.Suzuki, Y.Tanaka, I.Kato, M.Tanaka, K.Abe, T.Izumikawa, H.Oikawa, T.Ohtsubo, J.Ohno, Y.Kanke, H.Kikuchi, A.Kitagawa, S.Sato, U.Sayama, J.Shimaya, S.Suzuki, Y.Takeuchi, T.Takemoto, N.Tadano, R.Tamura, J.Nagumo, K.Nishizuka, S.Fukuda, K.Hori, S.Matsunaga, A.Mizukami, M.Mihara, E.Miyata, D.Murooka, S.Yamaoka, T.Yamaguchi

Nuclear Structure of 15, 16C via Reaction Cross-section Measurements

NUCLEAR REACTIONS 1H, 9Be, 12C, 27Al(15C, x), (16C, x), E=40-140 MeV/nucleon; measured outgoing particles using ΔE-E counter telescope; deduced reaction σ, mass and charge density of 14,15,16C vs radius, mass and charge radii using the data supplemented by published data at different eneegies. Compared with data on radii (both experimental and calculations) from other groups.

doi: 10.5506/APhysPolB.48.473
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2720.


2017MI04      Acta Phys.Pol. B48, 409 (2017)

E.Miyata, M.Takechi, T.Ohtsubo, M.Fukuda, D.Nishimura, K.Abe, K.Aoki, A.Ikeda, T.Izumikawa, H.Oikawa, K.Ohnishi, S.Ohmika, I.Kato, Y.Kanke, N.Kanda, R.Kanbe, H.Kikuchi, A.Kitagawa, S.Sato, H.Shimamura, J.Shimaya, S.Suzuki, T.Suzuki, R.Takagaki, H.Takahashi, Y.Takei, Y.Takeuchi, T.Takenouchi, N.Tadano, M.Tanaka, Y.Tanaka, K.Chikaato, H.Du, J.Nagumo, K.Nishizuka, T.Nishimura, S.Fukuda, M.Machida, A.Mizukami, M.Mihara, J.Muraoka, S.Yagi, S.Yamaoka, T.Yamaguchi, K.Yokoyama

Development of High Resolution TOF Detector for RI Beams Using Cherenkov Radiation

doi: 10.5506/APhysPolB.48.409
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2017SA16      Nucl.Phys. A961, 142 (2017)

K.Sawahata, A.Ozawa, Y.Saito, Y.Abe, Y.Ichikawa, N.Inaba, Y.Ishibashi, A.Kitagawa, S.Matsunaga, T.Moriguchi, D.Nagae, S.Okada, S.Sato, S.Suzuki, T.Suzuki, Y.Takeuchi, T.Yamaguchi, J.Zenihiro

Investigations of charge-changing processes for light proton-rich nuclei on carbon and solid-hydrogen targets

NUCLEAR REACTIONS 1H, 12C(25Si, x), (26Si, x), (27Si, x), (28Si, x), (33Cl, x), (34Ar, x), (35Ar, x), (36Ar, x), E≈300 MeV/nucleon; measured charge-changing reaction products; deduced total charge-changing σ, partial charge-changing σ; calculated total charge-changing σ, partial charge-changing σ. 1H, 25,26,27Si, 33Cl; calculated, estimated nuclear proton RMS radii using total charge-changing σ and Glauber model with correction factor. 33Cl; calculated, estimated proton skin thickness.

doi: 10.1016/j.nuclphysa.2017.02.012
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2017TA06      Acta Phys.Pol. B48, 461 (2017)

M.Tanaka, M.Fukuda, D.Nishimura, M.Takechi, S.Suzuki, H.Du, Y.Tanaka, K.Aoki, S.Fukuda, A.Honma, T.Izumikawa, Y.Kamisho, N.Kanda, I.Kato, Y.Kanke, A.Kitagawa, J.Kohno, M.Machida, K.Matsuta, M.Mihara, E.Miyata, Y.Morita, J.Muraoka, D.Murooka, T.Nagai, M.Nagashima, K.Ohnishi, J.Ohno, T.Ohtsubo, H.Oikawa, S.Sato, H.Shimamura, T.Sugihara, T.Suzuki, N.Tadano, R.Takagaki, Y.Takei, A.Takenouchi, S.Yagi, T.Yamaguchi, S.Yamaki, S.Yamaoka

Reaction Cross Sections for 13-15B and One-neutron Halo in 14B

NUCLEAR REACTIONS 1H, 9Be, 12C, 27Al(13B, x), (14B, x), (15B, x), E=50-130 MeV/nucleon; measured reaction products; deduced reaction σ; calculated σ using Glauber-type approach; deduced nuclear matter density distribution, matter and charge radii for 13,15B and one-neutron halo 14B. Cross sections compared also with asymptotical σ at relativistic energy; nuclear radii with both calculations and data for B isotopes published in literature.

doi: 10.5506/APhysPolB.48.461
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2017TS01      Phys.Rev. C 95, 021304 (2017)

N.Tsunoda, T.Otsuka, N.Shimizu, M.Hjorth-Jensen, K.Takayanagi, T.Suzuki

Exotic neutron-rich medium-mass nuclei with realistic nuclear forces

NUCLEAR STRUCTURE 20,22,24,26,28,30,32Ne, 24,26,28,30,32,34Mg, 28,30,32,34,36Si; calculated energies of the first 2+ and 4+ states, B(E2), expectation values of the number of the particle-hole excitations in the ground states of Mg isotopes. 31,32Mg; calculated levels, J, π. 28O, 30Ne, 32Mg, 34Si, 36S, 38Ar, 40Ca; calculated effective neutron single-particle energies (ESPEs) of N=20 isotones. Extended Kuo-Krenciglowa (EKK) theory of effective nucleon-nucleon interaction for exotic nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.021304
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2016CH12      Phys.Rev. C 93, 034623 (2016)

J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, Y.C.Ge, Q.T.Li, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, E.Ideguchi, H.J.Ong, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, N.T.Tho, J.Rangel, A.M.Moro, D.Y.Pang, J.Lee, J.Wu, H.N.Liu, C.Wen

Elastic scattering and breakup of 11Be on protons at 26.9A MeV

NUCLEAR REACTIONS 1H(11B, 11B), (11B, X), E=26.9 MeV/nucleon, [11B beam from 9Be(13C, X), E=60 MeV/nucleon]; measured 10,11Be, recoiled protons and deuterons, (10,11Be)p-coin, σ(θ) for elastic and breakup reactions using charged particle telescopes and annular silicon detectors at RCNP-Osaka accelerator facility. 11Be; deduced excitation energy spectrum for the ground state and the excited states. Analysis using Chapel Hill 89 (CH89) and Koning-Delaroche (KD) global optical model potentials (OMPs) for elastic scattering, and extended continuum-discretized coupled-channels (XCDCC) formalism for elastic scattering and breakup data.

doi: 10.1103/PhysRevC.93.034623
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2016CH51      Phys.Rev. C 94, 064620 (2016)

J.Chen, J.L.Lou, Y.L.Ye, J.Rangel, A.M.Moro, D.Y.Pang, Z.H.Li, Y.C.Ge, Q.T.Li, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, T.D.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, T.T.Nguyen

Elastic scattering and breakup of 11Be on deuterons at 26.9A MeV

NUCLEAR REACTIONS 2H(11Be, 11Be), (11Be, X), E=26.9 MeV/nucleon, [secondary 11Be beam from 9Be(13C, X), E=60 MeV/nucleon using EN-course beam line at RCNP-Osaka]; measured projectile-like isotopes and recoil light particles, (deuterons)(11Be)- and (deuterons)(10Be)-coin, angular distributions and angular correlations, elastic σ(θ) and breakup σ(θ) using TELE0 and TELE1 telescopes of double-sided silicon strip detector; deduced excitation energy spectrum for the ground state and unbound excited states of 11Be. Comparison of experimental cross sections with optical model calculations, and with continuum-discretized coupled-channels (XCDCC) formalism.

doi: 10.1103/PhysRevC.94.064620
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2016EN04      Phys.Rev. C 93, 064312 (2016)

J.P.Entwisle, B.P.Kay, A.Tamii, S.Adachi, N.Aoi, J.A.Clark, S.J.Freeman, H.Fujita, Y.Fujita, T.Furuno, T.Hashimoto, C.R.Hoffman, E.Ideguchi, T.Ito, C.Iwamoto, T.Kawabata, B.Liu, M.Miura, H.J.Ong, J.P.Schiffer, D.K.Sharp, G.Susoy, T.Suzuki, S.V.Szwec, M.Takaki, M.Tsumura, T.Yamamoto

Change of nuclear configurations in the neutrinoless double-β decay of 130Te → 130Xe and 136Xe → 136Ba

NUCLEAR REACTIONS 128,130Te, 130,132,134,136Xe, 136,138Ba(d, 3He), E=101 MeV; measured Ed, Id, σ(θ) using Grand Raiden (GR) spectrometer at RCNP-Osaka cyclotron facility. 127,129Sb, 129,131,133,135I, 135,137Cs; deduced levels, L-transfers, spectroscopic factors. DWBA and optical model analysis. 128,130Te, 130,132,134,136Xe, 136,138Ba; deduced ground state proton occupancies. Comparison with shell-model and interacting boson-model calculations.

RADIOACTIVITY 130Te, 136Xe(2β-); deduced change in the configuration of valence protons between the initial and final states in the 0νββ decay mode from measurements of the cross sections in (d, 3He) reaction, nuclear matrix elements.

doi: 10.1103/PhysRevC.93.064312
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2016GA23      Phys.Rev. C 93, 064326 (2016)

E.Ganioglu, H.Fujita, B.Rubio, Y.Fujita, T.Adachi, A.Algora, M.Csatlos, J.M.Deaven, E.Estevez Aguado, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, M.Honma, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, T.Otsuka, G.Perdikakis, C.Scholl, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, R.G.T.Zegers, J.Zenihiro

High-resolution study of Gamow-Teller transitions in the 48Ti(3He, t)48V reaction

NUCLEAR REACTIONS 48Ti(3He, t), E=140 MeV/nucleon; measured E(t), I(t), σ(θ) using Grand Raiden spectrometer at RCNP-Osaka cyclotron facility. 48V; deduced levels, L-transfers, Tz=+2 to +1 Gamow-Teller transitions, Gamow-Teller B(GT) strengths. DWBA analysis. Comparisons with shell-model calculations using GXPF1J interaction, and with B(GT) results from 47Ti(3He, t)47V reaction. Predictions for β spectrum of mirror decay 48Fe to 48Mn.

doi: 10.1103/PhysRevC.93.064326
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2016KN02      Phys.Lett. B 754, 288 (2016)

R.Knobel, M.Diwisch, F.Bosch, D.Boutin, L.Chen, C.Dimopoulou, A.Dolinskii, B.Franczak, B.Franzke, H.Geissel, M.Hausmann, C.Kozhuharov, J.Kurcewicz, S.A.Litvinov, G.Martinez-Pinedo, M.Matos, M.Mazzocco, G.Munzenberg, S.Nakajima, C.Nociforo, F.Nolden, T.Ohtsubo, A.Ozawa, Z.Patyk, W.R.Plass, C.Scheidenberger, J.Stadlmann, M.Steck, B.Sun, T.Suzuki, P.M.Walker, H.Weick, M.-R.Wu, M.Winkler, T.Yamaguchi

First direct mass measurements of stored neutron-rich 129, 130, 131Cd isotopes with FRS-ESR

ATOMIC MASSES 129,130,131Cd; measured mean velocity of the stored fragments; deduced mass excess values of cadmium isotopes and uncertainties. Comparison with AME 2012 evaluation.

doi: 10.1016/j.physletb.2016.01.039
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2016KN03      Eur.Phys.J. A 52, 138 (2016)

R.Knobel, M.Diwisch, H.Geissel, Yu.A.Litvinov, Z.Patyk, W.R.Plass, C.Scheidenberger, B.Sun, H.Weick, F.Bosch, D.Boutin, L.Chen, C.Dimopoulou, A.Dolinskii, B.Franczak, B.Franzke, M.Hausmann, C.Kozhuharov, J.Kurcewicz, S.A.Litvinov, M.Matos, M.Mazzocco, G.Munzenberg, S.Nakajima, C.Nociforo, F.Nolden, T.Ohtsubo, A.Ozawa, J.Stadlmann, M.Steck, T.Suzuki, P.M.Walker, M.Winkler, T.Yamaguchi

New results from isochronous mass measurements of neutron-rich uranium fission fragments with the FRS-ESR-facility at GSI

NUCLEAR REACTIONS 9Be(238U, x), E=410-415 Mev/nucleon; measured reaction products; deduced mass excess for Z=28-62. Compared to AME2012 and other data.

ATOMIC MASSES 68Ge, 91Se, 94Br, 105Y, 106,107Zr, 110Nb, 113Mo, 114,115Tc, 118Ru, 121Rh, 123,124Pd, 126Ag, 138Sb, 141,143I, 149,150Ba, 150,151La, 154Ce, 93Br, 109Nb, 117Ru, 125Ag, 137Sb, 140I; measured correlation between the spread of the revolution time and the number of turns recorded in the ring; deduced mass-excess values.

doi: 10.1140/epja/i2016-16138-6
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2016NI07      Phys.Lett. B 756, 273 (2016)

N.Nishimura, Z.Podolyak, D.-L.Fang, T.Suzuki

Impact of the first-forbidden β decay on the production of A ∼ 195 r-process peak

NUCLEAR STRUCTURE A=175-210; calculated isotopic abundances, β-decay rates; deduced effects of first-forbidden transitions in β-decays on the production of the r-process A ∼ 195 peak. Comparison with available data.

doi: 10.1016/j.physletb.2016.03.025
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2016OR03      Phys.Rev. C 93, 044336 (2016)

S.E.A.Orrigo, B.Rubio, Y.Fujita, W.Gelletly, J.Agramunt, A.Algora, P.Ascher, B.Bilgier, B.Blank, L.Caceres, R.B.Cakirli, E.Ganioglu, M.Gerbaux, J.Giovinazzo, S.Grevy, O.Kamalou, H.C.Kozer, L.Kucuk, T.Kurtukian-Nieto, F.Molina, L.Popescu, A.M.Rogers, G.Susoy, C.Stodel, T.Suzuki, A.Tamii, J.C.Thomas

β decay of the exotic Tz = - 2 nuclei 48Fe, 52Ni, and 56Zn

RADIOACTIVITY 48Fe, 52Ni, 56Zn(EC), (β+), (β+p)[from Ni(58Ni, X), E=74.5 MeV/nucleon using LISE3 separator at GANIL]; measured decay products, Eγ, Iγ, Ep, Ip, pγ-coin, half-life of decays of 48Fe, 52Ni, 56Zn from time correlations between protons and implants using DSSSDs and four EXOGAM Ge clovers; deduced total proton branching ratios. 47Cr, 48Mn, 51Fe, 52Co, 55Ni, 56Cu; deduced energy levels, J, π, isospin (T), T=2 IAS, beta and proton branching ratios, Fermi B(F) and Gamow Teller B(GT) transition strengths using comparison with mirror states, mass excesses for T=2 multiplet by isobaric mass multiplet equation (IMME). Comparison with previous available experimental data, and mass evaluations.

NUCLEAR REACTIONS Ni(58Ni, X)56Zn/57Zn/55Cu/56Cu/52Ni/53Ni/54Ni/55Ni/50Co/51Co/52Co/53Co/48Fe/49Fe/50Fe/51Fe/47Mn/48Mn/49Mn/45Cr/46Cr/47Cr/48Cr/44V/45V/46V, E=74.5 MeV/nucleon; measured ΔE versus TOF isotopic identification plot for Tz=-2, -3/2, -1 and -1/2 nuclei using LISE3 separator at GANIL.

doi: 10.1103/PhysRevC.93.044336
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2016OR08      Phys.Rev. C 94, 044315 (2016)

S.E.A.Orrigo, B.Rubio, W.Gelletly, B.Blank, Y.Fujita, J.Giovinazzo, J.Agramunt, A.Algora, P.Ascher, B.Bilgier, L.Caceres, R.B.Cakirli, G.de France, E.Ganioglu, M.Gerbaux, S.Grevy, O.Kamalou, H.C.Kozer, L.Kucuk, T.Kurtukian-Nieto, F.Molina, L.Popescu, A.M.Rogers, G.Susoy, C.Stodel, T.Suzuki, A.Tamii, J.C.Thomas

Observation of the 2+ isomer in 52Co

RADIOACTIVITY 52Ni, 52mCo, 52Co(EC), (β+)[from Ni(58Ni, X), E=74.5 MeV/nucleon using LISE3 separator at GANIL]; measured yields of reaction products with Tz=-1/2, -1, -3/2 and -2 by ΔE-E and TOF techniques, β particle and protons, Eγ, Iγ, half-lives of the ground state and isomer of 52Co from (fragment)γ-correlated decay curves. 52Co, 52Fe; deduced levels, J, π, IAS in 52Fe, β feedings, Fermi and Gamow-Teller transition strengths B(F) and B(GT). Relevance of 52Co nucleus for the rp-process.

doi: 10.1103/PhysRevC.94.044315
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2016SA45      Phys.Rev. C 94, 041303 (2016)

H.Sagawa, T.Suzuki, M.Sasano

Effect of isoscalar spin-triplet pairings on spin-isospin responses in sd-shell nuclei

NUCLEAR STRUCTURE 24Mg, 28Si, 32S, 36Ar; calculated isoscalar (IS) and isovector (IV) spin-M1 transition strengths, accumulative sums of the IS- and IV-spin-M1 strengths, proton-neutron spin-spin correlation. Shell-model calculations with USDB interactions in full sd-shell model space for even-even N=Z sd-shell nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.94.041303
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2016SU03      Phys.Lett. B 753, 199 (2016)

T.Suzuki, T.Otsuka, C.Yuan, N.Alahari

Two-neutron "halo" from the low-energy limit of neutron-neutron interaction: Applications to drip-line nuclei 22C and 24O

NUCLEAR STRUCTURE 22C, 23,24O; analyzed available data; calculated density distributions for a neutron, radial wave function of halo neutron, RMS radius of the halo neutron, two-neutron separation energy. The neutron-neutron (nn) interaction fixed at the low-energy nn scattering limit.

doi: 10.1016/j.physletb.2015.12.001
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2015FA03      Phys.Rev. C 91, 014614 (2015)

G.W.Fan, M.Fukuda, D.Nishimura, X.L.Cai, S.Fukuda, I.Hachiuma, C.Ichikawa, T.Izumikawa, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, Y.Ohkuma, T.Ohtsubo, Z.z.Ren, S.Sato, Z.Q.Sheng, M.Sugiyama, S.Suzuki, T.Suzuki, M.Takechi, T.Yamaguchi, W.Xu

Density distribution of 8Li and 8B and capture reaction at low energy

NUCLEAR REACTIONS 9Be, 12C, 27Al(8Li, X), E=30-110 MeV, [8Li secondary beam produced in 9Be(13C, X), E=130 MeV/nucleon primary reaction]; measured reaction products, reaction σ(E) at HIMAC synchrotron and fragment-separator facility of NIRS, Japan; deduced density distributions of 8B and 8Li using modified Glauber model, halo structure of 8B. 7Li(n, γ)8Li, E=0.01 eV-1 MeV; 7Be(p, γ)8B, E=0-0.5 MeV; calculated capture σ(E) for (n, γ) and S(E) factor for (p, γ) reactions using density distributions determined in present work, comparison with experimental data.

doi: 10.1103/PhysRevC.91.014614
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2015FR02      Phys.Rev. C 91, 034608 (2015); Erratum Phys.Rev. C 100, 049901 (2019)

D.Frekers, T.Adachi, H.Akimune, M.Alanssari, B.A.Brown, B.T.Cleveland, H.Ejiri, H.Fujita, Y.Fujita, M.Fujiwara, V.N.Gavrin, M.N.Harakeh, K.Hatanaka, M.Holl, C.Iwamoto, A.Lennarz, A.Okamoto, H.Okamura, T.Suzuki, A.Tamii

Precision evaluation of the 71Ga (νe, e-) solar neutrino capture rate from the (3He, t) charge-exchange reaction

NUCLEAR REACTIONS 71Ga(3He, t)71Ge, E=420 MeV; measured triton spectra, σ(θ) using Grand Raiden spectrometer at RCNP-Osaka facility. 71Ge; deduced levels, J, π, IAS, Gamow-Teller B(GT) transition strengths from analysis based on theoretical form factors and one-body transition densities from the shell-model code NUSHELLX with the GXPF1a interaction in full fp-model space. DWBA analysis of σ(θ) data. 71Ga(ν, e-); deduced solar neutrino capture rates as function of excitation energy in 71Ge from B(GT) values.

doi: 10.1103/PhysRevC.91.034608
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2015FU08      Phys.Rev. C 91, 064316 (2015)

Y.Fujita, H.Fujita, T.Adachi, G.Susoy, A.Algora, C.L.Bai, G.Colo, M.Csatlos, J.M.Deaven, E.Estevez Aguado, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, M.Honma, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Nakada, H.Okamura, H.J.Ong, T.Otsuka, G.Perdikakis, B.Rubio, H.Sagawa, P.Sarriguren, C.Scholl, Y.Shimbara, E.J.Stephenson, T.Suzuki, A.Tamii, J.H.Thies, K.Yoshida, R.G.T.Zegers, J.Zenihiro

High-resolution study of Gamow-Teller excitations in the 42Ca (3He, t) 42Sc reaction and the observation of a "low-energy super-Gamow-Teller state"

NUCLEAR REACTIONS 42Ca(3He, t), E=140 MeV/nucleon; measured triton spectra, σ(θ) using Grand Raiden spectrometer at RCNP facility. 42Sc; deduced levels, J, π, IAS, isospin of excited GT states, L-transfers, B(GT), configurations. Comparison of B(GT) values with those for 44,48Sc, and from 42Ti β+ decay to 42Sc. Isospin assignments made in comparison with results from 42Ca(p, p') reaction. Comparison with shell-model calculations using GXPF1J interaction. 12N, 16F, 40,44Sc; observed peaks from contaminants in the target material, and appropriate corrections applied to triton spectra for 42Sc.

doi: 10.1103/PhysRevC.91.064316
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2015HA21      Phys.Rev. C 92, 031305 (2015)

T.Hashimoto, A.M.Krumbholz, P.-G.Reinhard, A.Tamii, P.von Neumann-Cosel, T.Adachi, N.Aoi, C.A.Bertulani, H.Fujita, Y.Fujita, E.Ganioglu, K.Hatanaka, E.Ideguchi, C.Iwamoto, T.Kawabata, N.T.Khai, A.Krugmann, D.Martin, H.Matsubara, K.Miki, R.Neveling, H.Okamura, H.J.Ong, I.Poltoratska, V.Yu.Ponomarev, A.Richter, H.Sakaguchi, Y.Shimbara, Y.Shimizu, J.Simonis, F.D.Smit, G.Susoy, T.Suzuki, J.H.Thies, M.Yosoi, J.Zenihiro

Dipole polarizability of 120Sn and nuclear energy density functionals

NUCLEAR REACTIONS 120Sn(polarized p, p'), E=295 MeV; measured scattered proton spectra, p(θ) using Grand Raiden spectrometer at RCNP-Osaka; analyzed polarization transfer observables; deduced ISGQR excitation, B(E1), precise electric dipole polarizability αD, nuclear symmetry energy and its density dependence. Comparison with other experimental data. Comparison with model calculations based on Skyrme interactions and on relativistic Hamiltonians.

doi: 10.1103/PhysRevC.92.031305
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2015HO11      Prog.Theor.Exp.Phys. 2015, 081D01 (2015)

K.Hosomi, Y.Ma, S.Ajimura, K.Aoki, S.Dairaku, Y.Fu, H.Fujioka, K.Futatsukawa, W.Imoto, Y.Kakiguchi, M.Kawai, S.Kinoshita, T.Koike, N.Maruyama, M.Mimori, S.Minami, Y.Miura, K.Miwa, Y.Miyagi, T.Nagae, D.Nakajima, H.Noumi, K.Shirotori, T.Suzuki, T.Takahashi, T.N.Takahashi, H.Tamura, K.Tanida, N.Terada, A.Toyoda, K.Tsukada, M.Ukai, S.Zhou

Precise determination of Λ12C level structure by γ-ray spectroscopy

NUCLEAR REACTIONS 12C(π+, K+), E=12 GeV; measured reaction products, Eγ, Iγ; deduced the level structure of the 12C hypernucleus, J, π, the spacing of the ground-state doublet. Comparison with available data.

doi: 10.1093/ptep/ptv113
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2015KA15      Phys.Rev.Lett. 114, 192502 (2015)

R.Kanungo, A.Sanetullaev, J.Tanaka, S.Ishimoto, G.Hagen, T.Myo, T.Suzuki, C.Andreoiu, P.Bender, A.A.Chen, B.Davids, J.Fallis, J.P.Fortin, N.Galinski, A.T.Gallant, P.E.Garrett, G.Hackman, B.Hadinia, G.Jansen, M.Keefe, R.Krucken, J.Lighthall, E.McNeice, D.Miller, T.Otsuka, J.Purcell, J.S.Randhawa, T.Roger, A.Rojas, H.Savajols, A.Shotter, I.Tanihata, I.J.Thompson, C.Unsworth, P.Voss, Z.Wang

Evidence of Soft Dipole Resonance in 11Li with Isoscalar Character

NUCLEAR REACTIONS 2H(11Li, X)7Li/8Li/9Li/10Li/11Li, E=5.5 MeV/nucleon; measured reaction products. 11Li; deduced yields, σ(θ), excitation energy, soft dipole resonance. Comparison with ab initio calculations in the coupled cluster framework.

doi: 10.1103/PhysRevLett.114.192502
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2015KR05      Phys.Lett. B 744, 7 (2015)

A.M.Krumbholz, P.von Neumann-Cosel, T.Hashimoto, A.Tamii, T.Adachi, C.A.Bertulani, H.Fujita, Y.Fujita, E.Ganioglu, K.Hatanaka, C.Iwamoto, T.Kawabata, N.T.Khai, A.Krugmann, D.Martin, H.Matsubara, R.Neveling, H.Okamura, H.J.Ong, I.Poltoratska, V.Yu.Ponomarev, A.Richter, H.Sakaguchi, Y.Shimbara, Y.Shimizu, J.Simonis, F.D.Smit, G.Susoy, J.H.Thies, T.Suzuki, M.Yosoi, J.Zenihiro

Low-energy electric dipole response in 120Sn

NUCLEAR REACTIONS 120Sn(p, p'), E=295 MeV; measured reaction products, Ep, Ip; deduced σ, σ(θ, E), B(E1). Comparison with available data.

doi: 10.1016/j.physletb.2015.03.023
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2015NI05      Phys.Rev. C 91, 054305 (2015), Erratum Phys.Rev. C 95, 029902 (2017)

H.Nishibata, R.Leguillon, A.Odahara, T.Shimoda, C.M.Petrache, Y.Ito, J.Takatsu, K.Tajiri, N.Hamatani, R.Yokoyama, E.Ideguchi, H.Watanabe, Y.Wakabayashi, K.Yoshinaga, T.Suzuki, S.Nishimura, D.Beaumel, G.Lehaut, D.Guinet, P.Desesquelles, D.Curien, K.Higashiyama, N.Yoshinaga

High-spin states in 136La and possible structure change in the N=79 region

NUCLEAR REACTIONS 124Sn(17N, 5n), E=5.2 MeV/nucleon, [17N secondary beam from 9Be(18O, 17N), E=9.3 MeV/nucleon primary reaction]; measured Eγ, Iγ, γγ-coin, isomer half-life by γ(t) at RCNP-Osaka facility. 136La; deduced high-spin levels, J, π, isomer, bands, configuration, B(M1), B(E2). Comparison with pair-truncated shell model (PTSM) calculations, and cranked Nilsson-Strutinsky (CNS) model. Systematics of band structures in 130,132,134,136La and N=79 isotones 134Cs, 136La, 138Pr, 140Pm.

doi: 10.1103/PhysRevC.91.054305
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2015OR02      Acta Phys.Pol. B46, 709 (2015)

S.E.A.Orrigo, B.Rubio, Y.Fujita, B.Blank, W.Gelletly, J.Agramunt, A.Algora, P.Ascher, B.Bilgier, L.Caceres, R.B.Cakirli, H.Fujita, E.Ganioglu, M.Gerbaux, J.Giovinazzo, S.Grevy, O.Kamalou, H.C.Kozer, L.Kucuk, T.Kurtukian-Nieto, F.Molina, L.Popescu, A.M.Rogers, G.Susoy, C.Stodel, T.Suzuki, A.Tamii, J.C.Thomas

β-delayed γ-proton Decay in 56Zn: Analysis of the Charged-particle Spectrum

RADIOACTIVITY 56Zn(ECp) [from Ni(56Ni, X)56Zn, E=74.5 MeV/nucleon]; measured decay products, Ep, Ip; deduced the charged particle spectrum.

doi: 10.5506/APhysPolB.46.709
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2015WH02      Phys.Rev. C 91, 041303 (2015)

K.Whitmore, D.Smalley, H.Iwasaki, T.Suzuki, V.M.Bader, D.Bazin, J.S.Berryman, B.A.Brown, C.M.Campbell, P.Fallon, A.Gade, C.Langer, A.Lemasson, C.Loelius, A.O.Macchiavelli, C.Morse, T.Otsuka, J.Parker, F.Recchia, S.R.Stroberg, D.Weisshaar, K.Wimmer

Magnetic response of the halo nucleus 19C studied via lifetime measurement

NUCLEAR REACTIONS 9Be, Ta(20N, 19C), E=74 MeV/nucleon, [secondary 20N beam from 9Be(22Ne, X), E=120 MeV/nucleon primary reaction]; measured reaction products using A1900 separator, Eγ, Iγ, (particle)γ-, γγ-coin, half-life of the first excited state from line-shape and recoil-distance methods using GRETINA array at NSCL-MSU facility. 19C; deduced levels, J, π, B(M1), configuration. One-neutron halo nucleus populated in one-proton knockout reaction. Comparison with shell-model calculations using several different interactions.

doi: 10.1103/PhysRevC.91.041303
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2014AD13      Phys.Rev. C 89, 065209 (2014)

O.Adriani, E.Berti, L.Bonechi, M.Bongi, G.Castellini, R.D'Alessandro, M.Del Prete, M.Haguenauer, Y.Itow, K.Kasahara, K.Kawade, Y.Makino, K.Masuda, E.Matsubayashi, H.Menjo, G.Mitsuka, Y.Muraki, P.Papini, A.-L.Perrot, D.Pfeiffer, S.Ricciarini, T.Sako, N.Sakurai, T.Suzuki, T.Tamura, A.Tiberio, S.Torii, A.Tricomi, W.C.Turner

Transverse-momentum distribution and nuclear modification factor for neutral pions in the forward-rapidity region in proton-lead collisions at √ sNN = 5.02 TeV

doi: 10.1103/PhysRevC.89.065209
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2014AS03      Physics of Part.and Nuclei 45, 199 (2014)

K.Asahi, Y.Ichikawa, M.Chikamori, Y.Ohtomo, E.Hikota, T.Suzuki, T.Inoue, T.Furukawa, A.Yoshimi, K.Suzuki, T.Nanao, H.Miyatake, M.Tsuchiya, N.Yoshida, H.Shirai, T.Ino, H.Ueno, Y.Matsuo, T.Fukuyama

Search for electric dipole moment in 129Xe atom using a nuclear spin oscillator

ATOMIC PHYSICS 129Xe; analyzed experimental sensitivity for electric dipole moment measurements.

doi: 10.1134/S1063779614010080
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2014BU01      Phys.Rev.Lett. 112, 042502 (2014)

G.Burgunder, O.Sorlin, F.Nowacki, S.Giron, F.Hammache, M.Moukaddam, N.de Sereville, D.Beaumel, L.Caceres, E.clement, G.Duchene, J.P.Ebran, B.Fernandez-Dominguez, F.Flavigny, S.Franchoo, J.Gibelin, A.Gillibert, S.Grevy, J.Guillot, A.Lepailleur, I.Matea, A.Matta, L.Nalpas, A.Obertelli, T.Otsuka, J.Pancin, A.Poves, R.Raabe, J.A.Scarpaci, I.Stefan, C.Stodel, T.Suzuki, J.C.Thomas

Experimental Study of the Two-Body Spin-Orbit Force in Nuclei

NUCLEAR REACTIONS 2H(34Si, p), E=20.5 MeV/nucleon; 2H(36S, p), E=19 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), level energies, spectroscopic factors, reduction of spin-orbit splitting, two-body spin-orbit interaction. Comparison with strength calculations for N3LO and KLS nucleon-nucleon forces.

doi: 10.1103/PhysRevLett.112.042502
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2014FA18      Phys.Rev. C 90, 044321 (2014)

G.W.Fan, M.Fukuda, D.Nishimura, X.L.Cai, S.Fukuda, I.Hachiuma, C.Ichikawa, T.Izumikawa, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, Y.Ohkuma, T.Ohtsubo, Z.Ren, S.Sato, Z.Q.Shen, M.Sugiyama, S.Suzuki, T.Suzuki, M.Takechi, T.Yamaguchi, B.J.Xu, W.Xu

Structure of 8Li from a reaction cross-section measurement

NUCLEAR REACTIONS 1H, 9Be, 12C, 27Al(8Li, 8Li'), E=30-110 MeV/nucleon, [secondary 8Li beam from 9Be(13C, X), E=130 MeV/nucleon primary reaction]; measured particle spectra by Bρ-ΔE-TOF technique, reaction σ(E) at HIMAC synchrotron and NIRS fragment-separator facility in Japan. 8Li; deduced density distribution, matter radius, tendency for 8Li as a skin nucleus. Modified Glauber model analysis of experimental data. Comparison with previous experimental results and with calculations based on harmonic oscillator (HO)+Yukawa and HO+single-particle model (SPM) functions.

doi: 10.1103/PhysRevC.90.044321
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2014FU02      Phys.Rev.Lett. 112, 112502 (2014)

Y.Fujita, H.Fujita, T.Adachi, C.L.Bai, A.Algora, G.P.A.Berg, P.von Brentano, G.Colo, M.Csatlos, J.M.Deaven, E.Estevez Aguado, C.Fransen, D.De Frenne, K.Fujita, E.Ganioglu, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, M.Honma, D.Ishikawa, E.Jacobs, A.Krasznahorkay, H.Matsubara, K.Matsuyanagi, R.Meharchand, F.Molina, K.Muto, K.Nakanishi, A.Negret, H.Okamura, H.J.Ong, T.Otsuka, N.Pietralla, G.Perdikakis, L.Popescu, B.Rubio, H.Sagawa, P.Sarriguren, C.Scholl, Y.Shimbara, Y.Shimizu, G.Susoy, T.Suzuki, Y.Tameshige, A.Tamii, J.H.Thies, M.Uchida, T.Wakasa, M.Yosoi, R.G.T.Zegers, K.O.Zell, J.Zenihiro

Observation of Low- and High-Energy Gamow-Teller Phonon Excitations in Nuclei

NUCLEAR REACTIONS 42Ca, 46Ti, 50Cr, 54Fe(3He, t), E=140 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced cumulative-sum strengths of the experimental B(GT) values in the final nuclei, two kinds of GT phonon states. GXPF1J, quasi particle random phase approximation (QRPA) framework based on a self-consistent Hartree-Fock mean field with Skyrme interaction calculations, comparison with available data.

doi: 10.1103/PhysRevLett.112.112502
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2014KA27      Phys.Rev. C 89, 064313 (2014)

M.Karakoc, R.G.T.Zegers, B.A.Brown, Y.Fujita, T.Adachi, I.Boztosun, H.Fujita, M.Csatlos, J.M.Deaven, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, G.Perdikakis, C.Scholl, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, J.Zenihiro

Gamow-Teller transitions in the A=40 isoquintet of relevance for neutrino captures in 40Ar

NUCLEAR REACTIONS 40Ar(3He, t), E=140 MeV/nucleon; measured triton spectra, σ using Grand-Raiden spectrometer at RCNP facility. 40K; deduced levels, J, π, B(GT) DWBA analysis. Main focus on 1+ states at 2290 and 2730 keV. Other details to appear in a future publication. 40Ar(p, n)40K; 40Ti(β+), (EC); analyzed previous experimental results, and compared Gamow-Teller B(GT) strengths in all three studies. Comparison with shell-model calculations in the sd-pf shell with a new interaction (WBMB-C) to study differences between structure of transitions from 40Ar and 40Ti. Discussed ratio of the cross sections for low-lying 1+ states populated in 40Ar(p, n) and 40Ar(3He, t) reactions. Relevance of 40Ar in the use of liquid argon as a medium for neutrino detection.

doi: 10.1103/PhysRevC.89.064313
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2014MA72      Few-Body Systems 55, 729 (2014)

Y.Maeda, T.Saito, H.Miyasako, T.Uesaka, S.Ota, S.Kawase, T.Kikuchi, H.Tokieda, T.Kawabata, K.Yako, T.Wakasa, S.Sakaguchi, R.Chen, H.Sakaguchi, T.Shima, T.Suzuki, A.Tamii

Measurement of the 2H(p, n) Breakup Reaction at 170 MeV and the Three-Nucleon Force Effects

NUCLEAR REACTIONS 2H(p, 2p), E=170 MeV; measured reaction products, Ep, Ip; deduced σ(θ, E), analyzing powers. Comparison with available data.

doi: 10.1007/s00601-014-0868-5
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2014MO19      Nucl.Phys. A929, 83 (2014)

T.Moriguchi, A.Ozawa, S.Ishimoto, Y.Abe, M.Fukuda, I.Hachiuma, Y.Ishibashi, Y.Ito, T.Kuboki, M.Lantz, D.Nagae, K.Namihira, D.Nishimura, T.Ohtsubo, H.Ooishi, T.Suda, H.Suzuki, T.Suzuki, M.Takechi, K.Tanaka, T.YamaguchI

Density distribution of 14Be from reaction cross-section measurements

NUCLEAR REACTIONS 1H, 12C(14Be, x), E=46, 79 MeV/nucleon; measured reaction products; deduced reaction σ. 14Be deduced using also data at other energies, mass density distribution, radius; calculated σ.

doi: 10.1016/j.nuclphysa.2014.06.003
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2014OR03      Acta Phys.Pol. B45, 355 (2014)

S.E.A.Orrigo, B.Rubio, J.Agramunt, A.Algora, F.Molina, Y.Fujita, B.Blank, P.Ascher, M.Gerbaux, J.Giovinazzo, S.Grevy, T.Kurtukian-Nieto, W.Gelletly, B.Bilgier, R.B.Cakirli, E.Ganioglu, H.C.Kozer, L.Kucuk, G.Susoy, L.Caceres, O.Kamalou, C.Stodel, J.C.Thomas, H.Fujita, T.Suzuki, A.Tamii, L.Popescu, A.M.Rogers

Beta Decay of the Exotic Tz = -2, 56Zn Nucleus and Half-life of Various Proton-rich Tz = -1 Nuclei

RADIOACTIVITY 56Zn(β+p); measured decay products, Eπ, Iπ, Eγ, Iγ; deduced level scheme, J, π, Fermi strength.

doi: 10.5506/APhysPolB.45.355
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2014OR04      Phys.Rev.Lett. 112, 222501 (2014)

S.E.A.Orrigo, B.Rubio, Y.Fujita, B.Blank, W.Gelletly, J.Agramunt, A.Algora, P.Ascher, B.Bilgier, L.Caceres, R.B.Cakirli, H.Fujita, E.Ganioglu, M.Gerbaux, J.Giovinazzo, S.Grevy, O.Kamalou, H.C.Kozer, L.Kucuk, T.Kurtukian-Nieto, F.Molina, L.Popescu, A.M.Rogers, G.Susoy, C.Stodel, T.Suzuki, A.Tamii, J.C.Thomas

Observation of the β-Delayed γ-Proton Decay of 56Zn and its Impact on the Gamow-Teller Strength Evaluation

RADIOACTIVITY 56Zn(EC), (ECp) [from Ni(58Ni, X)56Zn, E=74.5 MeV/nucleon]; measured decay products, Eγ, Iγ, Ep, Ip; deduced γ and proton energies, intensities, Fermi and Gamow-Teller transition strengths, B(F), B(GT). Comparison with available data.

doi: 10.1103/PhysRevLett.112.222501
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2014OZ02      Phys.Rev. C 89, 044602 (2014)

A.Ozawa, T.Moriguchi, T.Ohtsubo, N.Aoi, D.Q.Fang, N.Fukuda, M.Fukuda, H.Geissel, I.Hachiuma, N.Inabe, Y.Ishibashi, S.Ishimoto, Y.Ito, T.Izumikawa, D.Kameda, T.Kubo, T.Kuboki, K.Kusaka, M.Lantz, Y.G.Ma, M.Mihara, Y.Miyashita, S.Momota, D.Nagae, K.Namihira, D.Nishimura, H.Ooishi, Y.Ohkuma, T.Ohnishi, M.Ohtake, K.Ogawa, Y.Shimbara, T.Suda, T.Sumikama, H.Suzuki, S.Suzuki, T.Suzuki, M.Takechi, H.Takeda, K.Tanaka, R.Watanabe, M.Winkler, T.Yamaguchi, Y.Yanagisawa, Y.Yasuda, K.Yoshinaga, A.Yoshida, K.Yoshida

Charge-changing cross sections of 30Ne, 32, 33Na with a proton target

NUCLEAR REACTIONS 1H(30Ne, X), (32Na, X), (33Na, X), [secondary 30Ne, 32,33Na beams from 9Be(48Ca, X)30Ne/31Ne/31Na/32Na/33Na, E=345 MeV/nucleon primary reaction], E≈240 MeV/nucleon; measured particle spectra, charge-changing, partial charge-changing and charge-pickup σ using Big-RIPS and ZDS spectrometers at RIBF-RIKEN facility; deduced rms proton and matter radii, neutron skin thickness. 30Ne, 32Na; deduced neutron skin thickness, rms proton radii. Glauber-model analysis. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.89.044602
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2014RU08      Nucl.Data Sheets 120, 37 (2014)

B.Rubio, S.E.A.Orrigo, L.Kucuk, A.Montaner-Piza, Y.Fujita, H.Fujita, B.Blank, W.Gelletly, T.Adachi, J.Agramunt, A.Algora, P.Ascher, B.Bilgier, L.Caceres, R.B.Cakirli, G.de France, E.Ganioglu, M.Gerbaux, J.Giovinazzo, S.Grevy, O.Kamalou, H.C.Kozer, T.Kurtukian-Nieto, F.M.Marques, F.Molina, Y.Oktem, F.de Oliveira Santos, L.Perrot, L.Popescu, R.Raabe, A.M.Rogers, P.C.Srivastava, G.Susoy, T.Suzuki, A.Tamii, J.C.Thomas

Beta Decay Study of the Tz = -256Zn Nucleus and the Determination of the Half-Lives of a Few fp-shell Nuclei

RADIOACTIVITY 56,58,59Zn, 53Co(EC), (β+p), 55Ni(EC); measured decay products, Ep, Ip.; deduced energy levels, J, π, total proton branching ratios, β-delayed γ-emission.

doi: 10.1016/j.nds.2014.06.135
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2014SA46      Phys.Lett. B 736, 137 (2014)

A.Sanetullaev, M.B.Tsang, W.G.Lynch, Jenny Lee, D.Bazin, K.P.Chan, D.Coupland, V.Henzl, D.Henzlova, M.Kilburn, A.M.Rogers, Z.Y.Sun, M.Youngs, R.J.Charity, L.G.Sobotka, M.Famiano, S.Hudan, D.Shapira, W.A.Peters, C.Barbieri, M.Hjorth-Jensen, M.Horoi, T.Otsuka, T.Suzuki, Y.Utsuno

Neutron spectroscopic factors of 55Ni hole-states from image transfer reactions

NUCLEAR REACTIONS 1H(56Ni, d), E=37 MeV/nucleon; measured reaction products; deduced spectroscopic factors, J, π, σ(θ). Comparison with shell model calculations.

doi: 10.1016/j.physletb.2014.07.003
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2014SH01      Hyperfine Interactions 225, 183 (2014)

T.Shimoda, K.Tajiri, K.Kura, A.Odahara, M.Suga, Y.Hirayama, N.Imai, H.Miyatake, M.Pearson, C.D.P.Levy, K.P.Jackson, R.Legillon, C.Petrache, T.Fukuchi, N.Hamatani, T.Hori, M.Kazato, Y.Kenmoku, T.Masue, H.Nishibata, T.Suzuki, A.Takashima, R.Yokoyama

Nuclear structure explored by β-delayed decay spectroscopy of spin-polarized radioactive nuclei at TRIUMF ISAC-1

RADIOACTIVITY 29,30Na(β-); measured decay products, Eγ, Iγ; deduced energy levels, J, π. Comparison with available data.

doi: 10.1007/s10751-013-0895-5
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2014TA32      Phys.Rev. C 90, 061305 (2014)

M.Takechi, S.Suzuki, D.Nishimura, M.Fukuda, T.Ohtsubo, M.Nagashima, T.Suzuki, T.Yamaguchi, A.Ozawa, T.Moriguchi, H.Ohishi, T.Sumikama, H.Geissel, N.Aoi, R.-J.Chen, D.-Q.Fang, N.Fukuda, S.Fukuoka, H.Furuki, N.Inabe, Y.Ishibashi, T.Itoh, T.Izumikawa, D.Kameda, T.Kubo, M.Lantz, C.S.Lee, Y.-G.Ma, K.Matsuta, M.Mihara, S.Momota, D.Nagae, R.Nishikiori, T.Niwa, T.Ohnishi, K.Okumura, M.Ohtake, T.Ogura, H.Sakurai, K.Sato, Y.Shimbara, H.Suzuki, H.Takeda, S.Takeuchi, K.Tanaka, M.Tanaka, H.Uenishi, M.Winkler, Y.Yanagisawa, S.Watanabe, K.Minomo, S.Tagami, M.Shimada, M.Kimura, T.Matsumoto, Y.R.Shimizu, M.Yahiro

Evidence of halo structure in 37Mg observed via reaction cross sections and intruder orbitals beyond the island of inversion

NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon, [secondary Mg beams from 9Be(48Ca, X), E=345 MeV/nucleon primary reaction]; measured spectra and TOF of outgoing particles, precise reaction σ using BigRIPS spectrometer at RIBF-RIKEN facility. Comparison with theoretical deformation parameter β2 versus mass plot using double-folding model (DFM) calculation combined with antisymmetrized molecular dynamics (AMD) calculation. 37Mg; deduced deformed halo effect from observed enhanced cross section, comparison with DFM calculation based on the deformed Woods-Saxon (DWS) model; collapse of N=28 magic shell for neutrons.

doi: 10.1103/PhysRevC.90.061305
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2014WA14      Phys.Rev. C 89, 044610 (2014)

S.Watanabe, K.Minomo, M.Shimada, S.Tagami, M.Kimura, M.Takechi, M.Fukuda, D.Nishimura, T.Suzuki, T.Matsumoto, Y.R.Shimizu, M.Yahiro

Ground-state properties of neutron-rich Mg isotopes

NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon; calculated reaction σ; deduced rms matter radii from reaction cross sections. Antisymmetrized molecular dynamics (AMD) with folding model and deformed Woods-Saxon model. Comparison with experimental data, and with other theoretical calculations.

NUCLEAR STRUCTURE 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated ground state binding J, π, S(n), S(2n) for 40Mg, β and γ deformation parameters, proton, neutron and matter radii, neutron skin thickness. 37Mg; calculated levels, J, π, neutron single-particle energies. Antisymmetrized molecular dynamics (AMD) with folding model and deformed Woods-Saxon model. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.044610
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2014YA28      Phys.Rev. A 90, 052516 (2014)

X.Yang, T.Furukawa, T.Wakui, T.Fujita, K.Imamura, Y.Mitsuya, M.Hayasaka, Y.Ichikawa, Y.Ishibashi, H.Shirai, T.Suzuki, Y.Ebara, A.Hatakeyama, M.Wada, T.Sonoda, Y.Ito, T.Kobayashi, S.Nishimura, Mizuki Kurata-Nishimura, Y.Kondo, K.-I.Yoneda, S.Kubono, Y.Ohshiro, H.Ueno, T.Shinozuka, T.Shimoda, K.Asahi, Y.Matsuo

Laser-radio-frequency double-resonance spectroscopy of 84-87Rb isotopes trapped in superfluid helium

NUCLEAR MOMENTS 84,85,86,87Rb; measured laser-radio-frequency double-resonance spectra; deduced nuclear spin values with reasonable accuracy.

doi: 10.1103/PhysRevA.90.052516
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2014YU02      Phys.Rev. C 89, 044327 (2014)

C.Yuan, C.Qi, F.Xu, T.Suzuki, T.Otsuka

Mirror energy difference and the structure of loosely bound proton-rich nuclei around A =20

NUCLEAR STRUCTURE 18O, 18Ne; 19O, 19Na; 21O, 21Al; 22F, 22Al; 23Ne, 23Al;, 24Na, 24Al; calculated levels, J, π of loosely bound proton-rich mirror nuclei. 18Ne, 19Na, 20Mg, 21,22,23,24Al, 22,23,24Si; calculated binding energies. 22,23,24Al, 22,23,24Si; calculated low lying levels, J, π. 18Ne, 19Na, 23,24Al; calculated mirror energy differences (MEDs). Shell model Hamiltonian (USD, USDA, USDB) in Woods-Saxon basis. Comparison with experimental data.

RADIOACTIVITY 24Ne(β-), 24Si(β+); calculated B(GT+)/B(GT-) ratios for mirror nuclei. Shell model Hamiltonian (USD, USDA, USDB) in Woods-Saxon basis. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.044327
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2013AT02      Phys.Scr. T156, 014026 (2013)

D.R.Atanasov, D.Balabanski, L.Batist, K.Blaum, F.Bosch, D.Boutin, C.Brandau, C.Dimopoulou, H.G.Essel, T.Faestermann, H.Geissel, S.Hagmann, R.Hess, P.-M.Hillenbrand, P.Kienle, R.Knobel, C.Kozhuharov, J.Kurcewicz, M.Lestinsky, S.A.Litvinov, Yu A.Litvinov, X.Ma, R.Martin, M.Mazzocco, G.Munzenberg, F.Nolden, T.Ohtsubo, Z.Patyk, M.S.Sanjari, C.Scheidenberger, D.Shubina, U.Spillmann, M.Steck, Th.Stohlker, B.Sun, T.Suzuki, S.Torilov, M.Trassinelli, S.Trotsenko, X.Tu, I.I.Tupitsyn, H.Weick, N.Winckler, M.Winkler, D.F.A.Winters, N.Winters, H.Xu, T.Yamaguchi, X.Yan, Y.Yuan, Y.Zhang

Half-life measurements of highly charged radionuclides

doi: 10.1088/0031-8949/2013/T156/014026
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2013FA05      Phys.Rev. C 88, 024314 (2013)

D.-L.Fang, B.A.Brown, T.Suzuki

β-decay properties for neutron-rich Kr-Tc isotopes from deformed pn-quasiparticle random-phase approximation calculations with realistic forces

RADIOACTIVITY 96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111Kr, 97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112Rb, 98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113Sr, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114Y, 104,105,106,107,108,109,110,111,112,113,114,115Zr, 105,106,107,108,109,110,111,112,113,114,115,116Nb, 107,108,109,110,111,112,113,114,115,116,117Mo, 108,109,110,111,112,113,114,115,116,117,118Tc(β-), (β-n); calculated half-lives, delayed neutron emission probabilities Pn. 98,100Y, 100Nb, 108Tc; calculated low-spin low-lying levels, J, π; and compared with experimental values. Deformed quasiparticle random-phase approximation (pn-QRPA) method with realistic CD-Bonn forces, including Gamow-Teller and first-forbidden β transitions. Comparison of half-life and Pn values with available data from RIKEN facility. Implications for r-process elemental abundances.

doi: 10.1103/PhysRevC.88.024314
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2013FA08      Phys.Rev. C 88, 034304 (2013)

D.-L.Fang, B.A.Brown, T.Suzuki

Investigating β-decay properties of spherical nuclei along the possible r-process path

RADIOACTIVITY 118,120,122,124,126,128,130,132Cd, 136,138,140Xe, 139Cs, 203,205Au, 207Tl(β-); 124Mo, 125Tc, 126Ru, 127Rh, 128Pd, 129Ag, 130Cd, 131In, 190Gd, 191Tb, 192Dy, 193Ho, 194Er, 195Tm, 196Yb, 197Lu, 198Hf, 199Ta, 113,115,117As, 114,116,118Se, 115,117,119Br, 116,118,120Kr, 117,119,121Rb, 118,120,122Sr, 119,121,123Y, 120,122,124Zr, 121,123,125Nb, 122,124,126Mo, 123,125,127Tc, 124,126,128Ru, 125,127,129Rh, 126,128,130Pd, 127,129,131Ag, 128,130,132Cd, 129,131,133In, 130,132,134Sn, 131,133,135Sb, 174,176Sn, 175,177Sb, 176,178Te, 177,179I, 178,180Xe, 179,181Cs, 180,182,184Ba, 181,183,185La, 182,184,186Ce, 183,185,187Pr, 184,186,188Nd, 185,187,189Pm, 186,188,190Sm, 187,189,191Eu, 188,190,192Gd, 189,191,193Tb, 190,192,194Dy, 191,193,195Ho, 192,194,196Er, 193,195,197Tm, 194,196,198Yb, 195,197,199Lu, 196,198,200Hf, 197,199,201Ta, 198,200,202W, 199,201,203Re, 200,202,204Os, 201,203,205Ir, 202,204,206Pt, 203,205,207Au, 206,208Hg, 207,209Tl(β-), (β-n); calculated Q values, half-life, delayed neutron emission probability Pn, logft, first-forbidden to total ratio. Spherical QRPA + real forces (FRDM+GTF, FRDM+Real, HFB21+Real) using different mass models. Comparison with experimental data. Relevance to r-process path.

NUCLEAR STRUCTURE 118,120,122,124,126,128,130,132Cd, 136,138,140Xe, 139Cs, 203,205Au, 207Tl; calculated levels, J, π. Spherical QRPA + real forces. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.034304
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2013FU08      Phys.Rev. C 88, 014308 (2013)

Y.Fujita, T.Adachi, H.Fujita, A.Algora, B.Blank, M.Csatlos, J.M.Deaven, E.Estevez Aguado, E.Ganioglu, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, M.Honma, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, T.Otsuka, G.Perdikakis, B.Rubio, C.Scholl, Y.Shimbara, E.J.Stephenson, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, R.G.T.Zegers, J.Zenihiro

High-resolution study of TZ = +2 → +1 Gamow-Teller transitions in the 44Ca(3He, t)44Sc reaction

NUCLEAR REACTIONS 44Ca(3He, t), E=140 MeV/nucleon; measured triton spectra, σ(θ) using Grand Raiden magnetic spectrometer at RCNP facility. 44Sc; deduced levels, IAS, L transfers, J, π, B(GT) strengths, Ikeda sum rule for B(GT). Comparison with data from 44Ca(p, p'), E=200 MeV reaction populating T=1 states in 44Ca. Comparison with shell-model calculations using GXPF1J effective interaction. Discussed double isobaric analog state in 44Ca, and analog states in A=44 system of 44K, 44Ca, 44Sc, 44Ti, 44V, 44Cr nuclei.

RADIOACTIVITY 44Cr(β+), (β+p); deduced half-life of 44Cr, and β+ spectrum based on B(GT) from 44Ca(3He, t) reaction; compared β+ spectrum with measured delayed-proton spectrum.

doi: 10.1103/PhysRevC.88.014308
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2013FU15      Phys.Rev. C 88, 054329 (2013)

H.Fujita, Y.Fujita, T.Adachi, H.Akimune, N.T.Botha, K.Hatanaka, H.Matsubara, K.Nakanishi, R.Neveling, A.Okamoto, Y.Sakemi, T.Shima, Y.Shimizu, F.D.Smit, T.Suzuki, A.Tamii, M.Yosoi

Isospin mixing of the isobaric analog state studied in a high-resolution 56Fe(3He, t)56Co reaction

NUCLEAR REACTIONS 56Fe(3He, t), E=100, 140 MeV/nucleon; measured E(t) I(t), σ(θ) using Grand Raiden magnetic spectrometer at RCNP facility. 56Co; deduced levels, IAS, L-transfer, J, π, isospin, Fermi and Gamow-Teller transitions, isospin mixing matrix element and isospin impurity. DWBA analysis. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.88.054329
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2013GA04      Phys.Rev. C 87, 014321 (2013)

E.Ganioglu, H.Fujita, Y.Fujita, T.Adachi, A.Algora, M.Csatlos, J.M.Deaven, E.Estevez Aguado, C.J.Guess, J.Gulyas, K.Hatanaka, K.Hirota, M.Honma, D.Ishikawa, A.Krasznahorkay, H.Matsubara, R.Meharchand, F.Molina, H.Okamura, H.J.Ong, T.Otsuka, G.Perdikakis, B.Rubio, C.Scholl, Y.Shimbara, G.Susoy, T.Suzuki, A.Tamii, J.H.Thies, R.G.T.Zegers, J.Zenihiro

High-resolution study of Gamow-Teller transitions in the 47Ti(3He, t)47V reaction

NUCLEAR REACTIONS 47Ti(3He, t), E=140 MeV/nucleon; measured E(t), I(t), σ(θ) using Grand Raiden magnetic spectrometer at the RCNP, Osaka. 47V; deduced levels, IAS, L-transfer, J, π, Gamow-Teller strengths. DWBA analysis. Comparison with shell-model calculations using the GXPF1 interaction.

doi: 10.1103/PhysRevC.87.014321
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2013Ho17      Nucl.Phys. A914, 184c (2013)

K.Hosomi, S.Ajimura, K.Aoki, M.Dairaku, Y.Y.Fu, H.Fujioka, T.Fukuda, K.Futatsukawa, W.Imoto, Y.Kakiguchi, M.Kawai, S.Kinoshita, T.Koike, Y.Ma, N.Maruyamai, M.Mimori, S.Minami, Y.Miura, K.Miwa, Y.Miyagi, T.Nagae, D.Nakajima, H.Noumi, K.Shirotori, T.Suzuki, T.Takahashi, T.N.Takahashi, H.Tamura, K.Tanida, N.Terada, A.Toyoda, K.Tsukada, M.Ukai, S.H.Zhou

Gamma-ray spectroscopy of 12ΛC via the (π+, K+) reaction

NUCLEAR REACTIONS 12C(π+, K+), E not given; measured E(kaon), I(kaon), Eγ, Iγ. 12C deduced Λ hypernucleus γ transitions.

doi: 10.1016/j.nuclphysa.2013.04.007
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2013LE27      Phys.Rev. C 88, 044309 (2013)

R.Leguillon, H.Nishibata, Y.Ito, C.M.Petrache, A.Odahara, T.Shimoda, N.Hamatani, K.Tajiri, J.Takatsu, R.Yokoyama, E.Ideguchi, H.Watanabe, Y.Wakabayashi, K.Yoshinaga, T.Suzuki, S.Nishimura, D.Beaumel, G.Lehaut, D.Guinet, P.Desesquelles, D.Curien, A.Astier, T.Konstantinopoulos, T.Zerrouki

Spectroscopy of 135La

NUCLEAR REACTIONS 124Sn(17N, 6n), [17N secondary beam from 9Be(18O, 17N)10B, E=9.2 MeV/nucleon primary reaction], E not given; measured Eγ, Iγ, γγ-coin, isomer half-lives by γγ(t) using array of 12 HPGe detectors at RCNP, Osaka facility. 135La; deduced levels, J, π, bands, configuration. Comparison with previous experimental results. Systematics of low-lying states in 127,129,131,133,135,137,139La. Comparison of low-lying states in 135La with N=78 isotones 134Ba and 136Ce.

doi: 10.1103/PhysRevC.88.044309
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2013MO21      Phys.Rev. C 88, 024610 (2013)

T.Moriguchi, A.Ozawa, S.Ishimoto, Y.Abe, M.Fukuda, I.Hachiuma, Y.Ishibashi, Y.Ito, T.Kuboki, M.Lantz, D.Nagae, K.Namihira, D.Nishimura, T.Ohtsubo, H.Ooishi, T.Suda, H.Suzuki, T.Suzuki, M.Takechi, K.Tanaka, T.Yamaguchi

Density distributions of 11Li deduced from reaction cross-section measurements

NUCLEAR REACTIONS 1H, 12C(11Li, X), E=31, 41 MeV/nucleon; measured particle spectra, time-of-flight, reaction σ(E) using RIPS at RIKEN facility. 11Li; deduced neutron, proton, and matter density distributions, root-mean-square (rms) radii. Glauber model calculations based on the optical limit approximation. Comparison with previous data for 6,7,8,9,11Li. Discussed disappearance of N=8 shell gap.

doi: 10.1103/PhysRevC.88.024610
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