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NSR database version of May 21, 2024.

Search: Author = Y.Suzuki

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2024SU08      Phys.Rev. C 109, 044316 (2024)

Y.Suzuki, W.Horiuchi, M.Kimura

Isospin-forbidden electric dipole transition of the 9.64 MeV state of 12C

doi: 10.1103/PhysRevC.109.044316
Citations: PlumX Metrics


2023AB32      Phys.Rev. D 108, 092009 (2023)

K.Abe, N.Akhlaq, R.Akutsu, A.Ali, S.Alonso Monsalve, C.Alt, C.Andreopoulos, M.Antonova, S.Aoki, T.Arihara, Y.Asada, Y.Ashida, E.T.Atkin, M.Barbi, G.J.Barker, G.Barr, D.Barrow, M.Batkiewicz-Kwasniak, V.Berardi, L.Berns, S.Bhadra, A.Blanchet, A.Blondel, S.Bolognesi, T.Bonus, S.Bordoni, S.B.Boyd, A.Bravar, C.Bronner, S.Bron, A.Bubak, M.Buizza Avanzini, J.A.Caballero, N.F.Calabria, S.Cao, D.Carabadjac, A.J.Carter, S.L.Cartwright, M.P.Casado, M.G.Catanesi, A.Cervera, J.Chakrani, D.Cherdack, P.S.Chong, G.Christodoulou, A.Chvirova, M.Cicerchia, J.Coleman, G.Collazuol, L.Cook, A.Cudd, C.Dalmazzone, T.Daret, Yu.I.Davydov, A.De Roeck, G.De Rosa, T.Dealtry, C.C.Delogu, C.Densham, A.Dergacheva, F.Di Lodovico, S.Dolan, D.Douqa, T.A.Doyle, O.Drapier, J.Dumarchez, P.Dunne, K.Dygnarowicz, A.Eguchi, S.Emery-Schrenk, G.Erofeev, A.Ershova, G.Eurin, D.Fedorova, S.Fedotov, M.Feltre, A.J.Finch, G.A.Fiorentini Aguirre, G.Fiorillo, M.D.Fitton, J.M.Franco Patino, M.Friend, Y.Fujii, Y.Fukuda, Y.Furui, L.Giannessi, C.Giganti, V.Glagolev, M.Gonin, J.Gonzalez Rosa, E.A.G.Goodman, A.Gorin, M.Grassi, M.Guigue, D.R.Hadley, J.T.Haigh, P.Hamacher-Baumann, D.A.Harris, M.Hartz, T.Hasegawa, S.Hassani, N.C.Hastings, Y.Hayato, D.Henaff, M.Hogan, J.Holeczek, A.Holin, T.Holvey, N.T.Hong Van, T.Honjo, A.K.Ichikawa, M.Ikeda, T.Ishida, M.Ishitsuka, H.T.Israel, A.Izmaylov, M.Jakkapu, B.Jamieson, S.J.Jenkins, C.Jesus-Valls, J.J.Jiang, J.Y.Ji, P.Jonsson, S.Joshi, C.K.Jung, P.B.Jurj, M.Kabirnezhad, A.C.Kaboth, T.Kajita, H.Kakuno, J.Kameda, S.P.Kasetti, Y.Kataoka, T.Katori, M.Kawaue, E.Kearns, M.Khabibullin, A.Khotjantsev, T.Kikawa, S.King, V.Kiseeva, J.Kisiel, H.Kobayashi, T.Kobayashi, L.Koch, S.Kodama, A.Konaka, L.L.Kormos, Y.Koshio, T.Koto, K.Kowalik, Y.Kudenko, Y.Kudo, S.Kuribayashi, R.Kurjata, T.Kutter, M.Kuze, M.La Commara, L.Labarga, K.Lachner, J.Lagoda, S.M.Lakshmi, M.Lamers James, M.Lamoureux, A.Langella, J.-F.Laporte, D.Last, N.Latham, M.Laveder, L.Lavitola, M.Lawe, Y.Lee, C.Lin, S.-K.Lin, R.P.Litchfield, S.L.Liu, W.Li, A.Longhin, K.R.Long, A.Lopez Moreno, L.Ludovici, X.Lu, T.Lux, L.N.Machado, L.Magaletti, K.Mahn, M.Malek, M.Mandal, S.Manly, A.D.Marino, L.Marti-Magro, D.G.R.Martin, M.Martini, J.F.Martin, T.Maruyama, T.Matsubara, V.Matveev, C.Mauger, K.Mavrokoridis, E.Mazzucato, N.McCauley, J.McElwee, K.S.McFarland, C.McGrew, J.McKean, A.Mefodiev, G.D.Megias, P.Mehta, L.Mellet, C.Metelko, M.Mezzetto, E.Miller, A.Minamino, O.Mineev, S.Mine, M.Miura, L.Molina Bueno, S.Moriyama, S.Moriyama, P.Morrison, Th.A.Mueller, D.Munford, L.Munteanu, K.Nagai, Y.Nagai, T.Nakadaira, K.Nakagiri, M.Nakahata, Y.Nakajima, A.Nakamura, H.Nakamura, K.Nakamura, K.D.Nakamura, Y.Nakano, S.Nakayama, T.Nakaya, K.Nakayoshi, C.E.R.Naseby, T.V.Ngoc, V.Q.Nguyen, K.Niewczas, S.Nishimori, Y.Nishimura, K.Nishizaki, T.Nosek, F.Nova, P.Novella, J.C.Nugent, H.M.O'Keeffe, L.O'Sullivan, T.Odagawa, W.Okinaga, K.Okumura, T.Okusawa, N.Ospina, Y.Oyama, V.Palladino, V.Paolone, M.Pari, J.Parlone, J.Pasternak, M.Pavin, D.Payne, G.C.Penn, D.Pershey, L.Pickering, C.Pidcott, G.Pintaudi, C.Pistillo, B.Popov, K.Porwit, M.Posiadala-Zezula, Y.S.Prabhu, F.Pupilli, B.Quilain, T.Radermacher, E.Radicioni, B.Radics, M.A.Ramirez, P.N.Ratoff, M.Reh, C.Riccio, E.Rondio, S.Roth, N.Roy, A.Rubbia, A.C.Ruggeri, C.A.Ruggles, A.Rychter, K.Sakashita, F.Sanchez, C.M.Schloesser, K.Scholberg, M.Scott, Y.Seiya, T.Sekiguchi, H.Sekiya, D.Sgalaberna, A.Shaikhiev, F.Shaker, M.Shiozawa, W.Shorrock, A.Shvartsman, N.Skrobova, K.Skwarczynski, D.Smyczek, M.Smy, J.T.Sobczyk, H.Sobel, F.J.P.Soler, Y.Sonoda, A.J.Speers, R.Spina, I.A.Suslov, S.Suvorov, A.Suzuki, S.Y.Suzuki, Y.Suzuki, M.Tada, S.Tairafune, S.Takayasu, A.Takeda, Y.Takeuchi, K.Takifuji, H.K.Tanaka, M.Tani, A.Teklu, V.V.Tereshchenko, N.Thamm, L.F.Thompson, W.Toki, C.Touramanis, T.Towstego, K.M.Tsui, T.Tsukamoto, M.Tzanov, Y.Uchida, M.Vagins, D.Vargas, M.Varghese, G.Vasseur, C.Vilela, E.Villa, W.G.S.Vinning, U.Virginet, T.Vladisavljevic, T.Wachala, J.G.Walsh, Y.Wang, L.Wan, D.Wark, M.O.Wascko, A.Weber, R.Wendell, M.J.Wilking, C.Wilkinson, J.R.Wilson, K.Wood, C.Wret, J.Xia, Y.-h.Xu, K.Yamamoto, T.Yamamoto, C.Yanagisawa, G.Yang, T.Yano, K.Yasutome, N.Yershov, U.Yevarouskaya, M.Yokoyama, Y.Yoshimoto, N.Yoshimura, M.Yu, R.Zaki, A.Zalewska, J.Zalipska, K.Zaremba, G.Zarnecki, X.Zhao, T.Zhu, M.Ziembicki, E.D.Zimmerman, M.Zito, S.Zsoldos

Measurements of the νμ and ν-barμ-induced coherent charged pion production cross sections on 12C by the T2K experiment

NUCLEAR REACTIONS 12C(ν, μ-), (ν-bar, μ+), E ∼ 0.8 GeV; measured reaction products; deduced coherent charged pion production σ in the Tokai-to-Kamioka experiment.

doi: 10.1103/PhysRevD.108.092009
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2023TA04      Phys.Rev. C 107, 024314 (2023)

R.Takatsu, Y.Suzuki, W.Horiuchi, M.Kimura

Microscopic study of the deformed neutron halo of 31Ne

NUCLEAR STRUCTURE 30,31Ne; calculated levels, J, p, S(n), point-proton and neutron distribution radii, quadrupole moments of protons and neutrons. 31Ne; calculated neutron single-particle energies, occupation numbers from the five most weakly bound neutrons, spectroscopic factor of ground and excited states, widths of the resonances 30Ne+n. Antisymmetrized molecular dynamics plus resonating group method (AMD+RGM) combined with analytical continuation of the coupling constant (ACCC) to improve the description of resonance states. Showed that 31Ne is a deformed halo nucleus in which the rotational excitation of the core is coupled with a deformed neutron halo. Comparison to experimental data and calculations performed with antisymmetrized molecular dynamics plus generator coordinate method (AMD+GCM).

doi: 10.1103/PhysRevC.107.024314
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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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Data from this article have been entered in the XUNDL database. For more information, click here.


2022HO03      Phys.Rev. C 105, 024310 (2022)

W.Horiuchi, Y.Suzuki, M.A.Shalchi, L.Tomio

Possible halo structure of 62, 72Ca by forbidden-state-free locally peaked Gaussians

NUCLEAR STRUCTURE 62Ca; calculated levels, J, π, rms radii, occupation probabilities. 72Ca; calculated levels, J, π, energy of the ground state, neutron rms radii, occupation probabilities. Developed forbidden-state-free locally peaked Gaussian method to describe core+n+n and core+n systems.

doi: 10.1103/PhysRevC.105.024310
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2022KI01      Phys.Rev. C 105, 014311 (2022)

M.Kimura, Y.Suzuki, T.Baba, Y.Taniguchi

Description of isospin mixing by a generator coordinate method

NUCLEAR STRUCTURE 14C, 14N; calculated energy curves as functions of quadrupole deformation parameter β. 14N; calculated levels, J, π, isospin T=1 components. 14N; calculated B(M1), B(E1), B(E2), magnetic dipole moments, electric quadrupole moments, spectroscopic factors, and overlap functions for low-lying, low-spin positive- and negative-parity states. Generator coordinate method (GCM) by applying the Fermi transition operator to the wave functions of isobars, for describing isospin mixing. Comparison with experimental data.

doi: 10.1103/PhysRevC.105.014311
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2022MO36      Prog.Theor.Exp.Phys. 2022, 113D01 (2022)

H.Motoki, Y.Suzuki, T.Kawai, M.Kimura

Cluster formation in neutron-rich Be and B isotopes

NUCLEAR STRUCTURE 10,12,14Be, 11,13,15,17,19B; calculated quadrupole deformation parameters, the RMS proton, neutron, and matter distribution radii of the Be and B isotopes and the principal neutron quantum numbers, magnetic moments of the B isotopes within the approximated shell model(SM) and molecular orbital (MO) configurations. Comparison with available data.

doi: 10.1093/ptep/ptac145
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2022SU12      Prog.Theor.Exp.Phys. 2022, 063D02 (2022)

Y.Suzuki, W.Horiuchi, M.Kimura

Erosion of N = 28 shell closure: Shape coexistence and monopole transition

NUCLEAR STRUCTURE 40Mg, 42Si, 44S; calculated energy levels, J, π, potential energy surfaces, B(E2) using the theoretical framework of antisymmetrized molecular dynamics with the Gogny D1S density functional; deduced different aspects of shape coexistence.

doi: 10.1093/ptep/ptac071
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2021SU08      Few-Body Systems 62, 2 (2021), Erratum Few-Body Systems 64, 73 (2023)

Y.Suzuki

Calculable Microscopic Theory for 12C(α, γ)16O Cross Section near Gamow Window

NUCLEAR REACTIONS 12C(α, γ), E not given; calculated σ, 3 α-particle and 4 α-particle configurations.

doi: 10.1007/s00601-020-01582-0
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2021SU18      Phys.Rev. C 104, 024327 (2021)

Y.Suzuki, M.Kimura

Triaxial deformation and the disappearance of the N=28 shell gap

NUCLEAR STRUCTURE 38,40,42Mg, 40,42,44Si, 42,44,46S, 44,46,48Ar; calculated potential energy surfaces, squared GCM amplitudes and occupation numbers for ground states in (β, γ) plane, energies, spins, B(E2) and quadrupole moments of low-lying positive-parity levels for N=26, 28 and 30 isotones. 42Mg, 44Si, 46S, 48Ar; calculated proton and neutron single-particle levels as function of β and γ deformation parameters for N=30 isotones; investigated nature and cause of the nuclear deformations and its relation to the disappearance of the neutron magic number N=28 in vicinity of 42Si. Antisymmetrized molecular dynamics (AMD) calculations with Gogny D1S density functional. Comparison with experimental data.

doi: 10.1103/PhysRevC.104.024327
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2021ZH31      Eur.Phys.J. A 57, 157 (2021)

Q.Zhao, Y.Suzuki, J.He, B.Zhou, M.Kimura

α clustering and neutron-skin thickness of carbon isotopes

NUCLEAR STRUCTURE 10,12,14Be, 12,14,16,18C; analyzed available data; calculated point proton and neutron density distributions of the ground states, α spectroscopic factors as function of the neutron skin thickness.

doi: 10.1140/epja/s10050-021-00465-0
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2020HO20      Phys.Rev. C 102, 054601 (2020)

W.Horiuchi, Y.Suzuki, T.Uesaka, M.Miwa

Total reaction cross section on a deuteron target and the eclipse effect of the constituent neutron and proton

NUCLEAR REACTIONS 2H(12C, X), (16O, X), (40Ca, X), E=50, 40-1000 MeV/nucleon; 2H(16O, X), (30Ne, X), (40Ca, X), (60Ca, X), E=40-1000 MeV/nucleon; 2H(34Ca, X), (36Ca, X), (38Ca, X), (40Ca, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (58Ca, X), (60Ca, X), (62Ca, X), (64Ca, X), (66Ca, X), (68Ca, X), (70Ca, X), (48Ni, X), (50Ni, X), (52Ni, X), (54Ni, X), (56Ni, X), (58Ni, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), (72Ni, X), (74Ni, X), (76Ni, X), (78Ni, X), (80Ni, X), (82Ni, X), (84Ni, X), (86Ni, X), E=100, 200, 550, 800 MeV/nucleon; calculated total reaction σ(E) for σd, σp and σn scattered by a deuteron target using the Glauber model, taking into account eclipse effect by the neutron and the proton in the deuteron. Comparison with available experimental data. Relevance to extraction of the nucleus-neutron interaction, and nuclear size properties.

doi: 10.1103/PhysRevC.102.054601
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2020SU03      Phys.Rev. C 101, 014002 (2020)

Y.Suzuki

Adiabatic hyperspherical potentials with localized correlated Gaussians

doi: 10.1103/PhysRevC.101.014002
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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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2017HO17      Phys.Rev. C 96, 024605 (2017)

W.Horiuchi, S.Hatakeyama, S.Ebata, Y.Suzuki

Low-lying electric-dipole strengths of Ca, Ni, and Sn isotopes imprinted on total reaction cross sections

NUCLEAR REACTIONS 40Ca, 120Sn, 208Pb(100Sn, X), (102Sn, X), (104Sn, X), (106Sn, X), (108Sn, X), (110Sn, X), (112Sn, X), (114Sn, X), (116Sn, X), (118Sn, X), (120Sn, X), (122Sn, X), (124Sn, X), (126Sn, X), (128Sn, X), (130Sn, X), (132Sn, X), (134Sn, X), (136Sn, X), (138Sn, X), (140Sn, X), E=100, 200, 550, 1000 MeV/nucleon; calculated total reaction σ(E), nuclear breakup σ(E), and Coulomb breakup σ(E), percentages of the Coulomb breakup cross sections with electric multipoles E1, E2, and E3, contributions of the electric-multipole strengths of 134Sn to the Coulomb breakup cross section by 208Pb target, comparison of the electric-dipole (E1) contributions of 100,110,120,132,134Sn isotopes to the Coulomb breakup cross sections by 208Pb target. 208Pb(40Ca, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (58Ca, X), (60Ca, X), (56Ni, X), (58Ni, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), (72Ni, X), (74Ni, X), (76Ni, X), (78Ni, X), (80Ni, X), (82Ni, X), (84Ni, X), E=100, 200, 550, 1000 MeV/nucleon; calculated total reaction σ(E), nuclear breakup σ(E), and Coulomb breakup σ(E). Hartree-Fock+BCS and the canonical-basis-time-dependent-Hartree-Fock-Bogoliubov methods using SkM*, SLy4, and SkI3 Skyrme-type effective interactions, with nuclear and Coulomb breakup processes described within the Glauber mode.

doi: 10.1103/PhysRevC.96.024605
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2017NA08      Rep.Prog.Phys. 80, 056301 (2017)

S.X.Nakamura, H.Kamano, Y.Hayato, M.Hirai, W.Horiuchi, S.Kumano, T.Murata, K.Saito, M.Sakuda, T.Sato, Y.Suzuki

Towards a unified model of neutrino-nucleus reactions for neutrino oscillation experiments

doi: 10.1088/1361-6633/aa5e6c
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2017SE26      J.Radioanal.Nucl.Chem. 311, 1361 (2017)

S.Sekimoto, K.Tatenuma, Y.Suzuki, A.Tsuguchi, A.Tanaka, T.Tadokoro, Y.Kani, Y.Morikawa, A.Yamamoto, T.Ohtsuki

Separation and purification of 99mTc from 99Mo produced by electron linear accelerator

NUCLEAR REACTIONS 100Mo(γ, n), E=21, 25.5, 32, 35, 41 MeV; measured reaction product, Eγ, Iγ; deduced yields. Comparison with the PHITS code.

doi: 10.1007/s10967-016-4959-2
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2017SU12      Phys.Rev. C 95, 044320 (2017)

Y.Suzuki, W.Horiuchi

Correlated-Gaussian approach to linear-chain states: Case of α particles

NUCLEAR STRUCTURE 16O; calculated energies of linear chain (LC) configurations of positive parity as function of angular momentum, dependence of contributions of kinetic energy, nuclear potential, and Coulomb potential to the lowest energy linear chain (LC) states of four α particles, excitation energies of 4α LC states as a function of L(L+1); deduced possible chain states for Jπ=0+, 2+, 4+ and 6+ with the bandhead energy about 33 MeV, no chain states found with J=8 or J>8. Correlated Gaussians approach in variation-after projection calculations.

doi: 10.1103/PhysRevC.95.044320
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2016HO05      Phys.Rev. C 93, 044611 (2016)

W.Horiuchi, S.Hatakeyama, S.Ebata, Y.Suzuki

Extracting nuclear sizes of medium to heavy nuclei from total reaction cross sections

NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Sn; calculated neutron and proton rms radii. 40,42,44,46,48,50,52,54,56,58,60Ca, 56,58,60,62,64,66,68,70,72,74,76,78,80,82,84Ni, 80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122Zr, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140Sn, 156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196Yb, 190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated matter radius of even-even nuclei using SkM*, SLy4, and SkI3 interactions. HF+BCS and HF theory with different interactions.

NUCLEAR REACTIONS 1,2H, 4He, 12C(40Ca, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (58Ca, X), (60Ca, X), (56Ni, X), (58Ni, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), (72Ni, X), (74Ni, X), (76Ni, X), (78Ni, X), (80Ni, X), (82Ni, X), (84Ni, X), (80Zr, X), (82Zr, X), (84Zr, X), (86Zr, X), (88Zr, X), (90Zr, X), (92Zr, X), (94Zr, X), (96Zr, X), (98Zr, X), (100Zr, X), (102Zr, X), (104Zr, X), (106Zr, X), (108Zr, X), (110Zr, X), (112Zr, X), (114Zr, X), (116Zr, X), (118Zr, X), (120Zr, X), (122Zr, X), (100Sn, X), (102Sn, X), (104Sn, X), (106Sn, X), (108Sn, X), (110Sn, X), (112Sn, X), (114Sn, X), (116Sn, X), (118Sn, X), (120Sn, X), (122Sn, X), (124Sn, X), (126Sn, X), (128Sn, X), (130Sn, X), (132Sn, X), (134Sn, X), (136Sn, X), (138Sn, X), (140Sn, X), (156Yb, X), (158Yb, X), (160Yb, X), (162Yb, X), (164Yb, X), (166Yb, X), (168Yb, X), (170Yb, X), (172Yb, X), (174Yb, X), (176Yb, X), (178Yb, X), (180Yb, X), (182Yb, X), (184Yb, X), (186Yb, X), (188Yb, X), (190Yb, X), (192Yb, X), (194Yb, X), (196Yb, X), (190Pb, X), (192Pb, X), (194Pb, X), (196Pb, X), (198Pb, X), (200Pb, X), (202Pb, X), (204Pb, X), (206Pb, X), (208Pb, X), (210Pb, X), (212Pb, X), (214Pb, X), E=1000 MeV, also 200 MeV for proton target; calculated Coulomb breakup cross sections by equivalent-photon method (EPM) with projectile density from SkM*, SLy4, and SkI3 Skyrme interactions, total reaction and Coulomb breakup probabilities, reaction radii versus point matter rms radii. Glauber model with densities from Skyrme-Hartree-Fock+BCS model. 12C(208Pb, 12C), E=200, 1000 MeV; 1H(208Pb, p), E=45-1000 MeV; calculated elastic σ(θ, E) using SkM* interaction, and compared with experimental data. 1H(40Ca, X), (58Ni, X), (90Zr, X), (120Sn, X), (208Pb, X), E=40-1000 MeV; calculated total reaction σ(E) and compared with experimental data.

doi: 10.1103/PhysRevC.93.044611
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2016KA37      Phys.Rev.Lett. 117, 102501 (2016)

R.Kanungo, W.Horiuchi, G.Hagen, G.R.Jansen, P.Navratil, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, M.Kimura, 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, Y.Suzuki, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Proton Distribution Radii of 12-19C Illuminate Features of Neutron Halos

NUCLEAR REACTIONS Be(20Ne, X), (40Ar, X)12C/13C/14C/15/16C/17C/18C/19C, E=1 GeV/nucleon; measured reaction products; deduced σ, root-mean-square proton and matter radii, neutron skin thickness. Comparison with ab initio calculations.

doi: 10.1103/PhysRevLett.117.102501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2311. Data from this article have been entered in the XUNDL database. For more information, click here.


2016NA31      Phys.Rev. C 94, 035803 (2016)

C.Nakamoto, Y.Suzuki

Quark-Pauli effects in three octet-baryons

doi: 10.1103/PhysRevC.94.035803
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2016SU16      Phys.Rev. C 94, 011602 (2016)

Y.Suzuki, W.Horiuchi, S.Terashima, R.Kanungo, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knoebel, 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, I.Tanihata, J.Vargas, H.Weick, J.S.Winfield

Parameter-free calculation of charge-changing cross sections at high energy

NUCLEAR REACTIONS 12C(12C, X), E=937, 943 MeV/nucleon; 12C(13C, X), E=828 MeV/nucleon; 12C(14C, X), E=900 MeV/nucleon; 1H(12C, X), E=926 MeV/nucleon; 1H(13C, X), E=815 MeV/nucleon; 1H(14C, X), E=889 MeV/nucleon; 1H(15C, X), E=896 MeV/nucleon; 1H(16C, X), E=897 MeV/nucleon; 1H(17C, X), E=970 MeV/nucleon; 1H(18C, X), (19C, X), E=886 MeV/nucleon; calculated charge-changing σ (CCCS), proton, neutron, and matter radii using Glauber and eikonal formalism and approximations. Comparison with recent new high-energy data measured at the FRS-GSI facility.

doi: 10.1103/PhysRevC.94.011602
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2016SU20      Phys.Rev. C 94, 024343 (2016)

Y.Suzuki, H.Nakada, S.Miyahara

Effects of a realistic tensor force on nuclear quadrupole deformation near the "shore" of the island of inversion

NUCLEAR STRUCTURE 30Ne, 32,40Mg, 34,42Si, 44S; calculated intrinsic mass quadrupole moment, deformation parameter β, and energies at the lowest and second lowest minima, proton and neutron single-particle levels; deduced effects of the tensor force on deformation. Constrained Hartree-Fock calculations assuming axial symmetry with M3Y-type semirealistic interaction containing a realistic tensor force. Comparison with available experimental results.

doi: 10.1103/PhysRevC.94.024343
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2016SU25      Phys.Rev. C 94, 054607 (2016)

H.Suno, Y.Suzuki, P.Descouvemont

Precise calculation of the triple-α reaction rates using the transmission-free complex absorbing potential method

NUCLEAR REACTIONS 12C(γ, 3α); calculated photodissociation σ(Eγ) as function of 3α energy, energy-averaged triple-α reaction rate as a function of temperature T=0.01 to 1 GK, adjusted and 3α-model triple-α reaction rates as functions of temperature T=1-10 GK. Solution of Schrodinger equation for three α particles using the modified Smith-Whitten hyperspherical coordinates and a complex absorbing potential. Comparison with CDCC and HHR theoretical approaches, and with the rates in NACRE database.

NUCLEAR STRUCTURE 12C; calculated energies, rms radii, B(E2), E0 strengths for the first two 0+ and first 2+ states using angular-momentum-independent α-α potential and three-body potentials to reproduce the energies of both the Hoyle state and the first 2+ state. Comparison with other theoretical calculations, and with experimental values.

doi: 10.1103/PhysRevC.94.054607
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2015SU03      Phys.Rev. C 91, 014004 (2015)

H.Suno, Y.Suzuki, P.Descouvemont

Triple-α continuum structure and Hoyle resonance of 12C using the hyperspherical slow variable discretization

NUCLEAR STRUCTURE 12C; calculated levels, J, π, bound and continuum energy spectra, energy of the second 0+ (Hoyle) state, ten lowest adiabatic hyperspherical potential curves, and contour plots of the 2D probability density functions of the three-α system for Jπ=0+ and 2+. Calculations based on 3α-particle model, the three particles interacting through both short-range and Coulomb potentials. 8Be; calculated resonance parameters with Legendre polynomial basis.

doi: 10.1103/PhysRevC.91.014004
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2014ES07      Phys.Rev.Lett. 113, 132501 (2014)

A.Estrade, R.Kanungo, W.Horiuchi, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, M.Kimura, 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, Y.Suzuki, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Proton Radii of 12-17B Define a Thick Neutron Surface in 17B

NUCLEAR REACTIONS C(10B, X), (11B, X), (12B, X), (13B, X), (14B, X), (15B, X), (16B, X), (17B, X), E ∼ 900 MeV/nucleon; measured reaction products. 10,11,12,13,14,15,16,17B; deduced charge-changing σ, proton and matter radii, neutron skin. Glauber model analysis.

doi: 10.1103/PhysRevLett.113.132501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0749. Data from this article have been entered in the XUNDL database. For more information, click here.


2014HO01      Phys.Rev. C 89, 011304 (2014)

W.Horiuchi, Y.Suzuki

Correlated-basis description of α-cluster and delocalized 0+ states in 16O

NUCLEAR STRUCTURE 16O, 16C; calculated energies of ground states and first excited 0+ state of 16O, density distributions, particle distances, 12C+α spectroscopic amplitudes, and probability distributions of harmonic-oscillator quanta. Role of core-nucleon and nucleon-nucleon potentials. Five-body approach of 12C plus four nucleons with multiparticle-multihole excitations, shape coexistence, and 12C+α clustering. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.011304
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2014HO02      Phys.Rev. C 89, 011601 (2014)

W.Horiuchi, Y.Suzuki, T.Inakura

Probing neutron-skin thickness with total reaction cross sections

NUCLEAR REACTIONS 1H, 12C(14O, X), (16O, X), (18O, X), (20O, X), (22O, X), (24O, X), (18Ne, X), (20Ne, X), (22Ne, X), (24Ne, X), (26Ne, X), (28Ne, X), (30Ne, X), (32Ne, X), (34Ne, X), (20Mg, X), (22Mg, X), (24Mg, X), (26Mg, X), (28Mg, X), (30Mg, X), (32Mg, X), (34Mg, X), (36Mg, X), (38Mg, X), (40Mg, X), (22Si, X), (24Si, X), (26Si, X), (28Si, X), (30Si, X), (32Si, X), (34Si, X), (36Si, X), (38Si, X), (40Si, X), (42Si, X), (44Si, X), (46Si, X), (26S, X), (28S, X), (30S, X), (32S, X), (34S, X), (36S, X), (38S, X), (40S, X), (42S, X), (44S, X), (46S, X), (48S, X), (50S, X), (34Ca, X), (36Ca, X), (38Ca, X), (40Ca, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), (50Ca, X), (52Ca, X), (54Ca, X), (56Ca, X), (58Ca, X), (60Ca, X), (62Ca, X), (64Ca, X), (66Ca, X), (68Ca, X), (70Ca, X), (48Ni, X), (50Ni, X), (52Ni, X), (54Ni, X), (56Ni, X), (58Ni, X), (60Ni, X), (62Ni, X), (64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), (72Ni, X), (74Ni, X), (76Ni, X), (78Ni, X), (80Ni, X), (82Ni, X), (84Ni, X), (86Ni, X), E=100, 120, 140, 160, 200, 300, 425, 550, 800, 1000 MeV; analyzed total reaction σ(E) in the Glauber model with Skyrme-Hartree-Fock method applied to generate the densities; deduced universal expression relating the reaction radius to the point matter rms radius and neutron skin thickness.

doi: 10.1103/PhysRevC.89.011601
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2014HO15      Phys.Rev. C 90, 034001 (2014)

W.Horiuchi, Y.Suzuki

Harmonic-oscillator excitations of precise few-body wave functions

NUCLEAR STRUCTURE 2H, 3H, 4He; calculated occupation probability distributions of the number of total harmonic-oscillator (HO) quanta in correlated Gaussian (CG) basis for ground state and excited states of 4He, ground-state energies, and rms matter radii of two- to four-nucleon systems with different MN, ATS3, G3RS+3NF, and AV8'+3NF potential models. Discussed cluster structure.

doi: 10.1103/PhysRevC.90.034001
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2014IN03      Phys.Rev. C 89, 064316 (2014)

T.Inakura, W.Horiuchi, Y.Suzuki, T.Nakatsukasa

Mean-field analysis of ground-state and low-lying electric dipole strength in 22C

NUCLEAR STRUCTURE 22C; calculated ground-state properties, neutron single-particle energies, rms matter radius, S(2n) using various Skyrme interactions, E1 strength distributions, neutron Fermi level dependence of low-lying E1 strength, dipole and neutron transition densities. Mean-field approach with Skyrme energy density functionals, and random-phase approximation for E1 strength. Importance of core excitations with the 1d5/2 orbit.

doi: 10.1103/PhysRevC.89.064316
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2014MI10      Phys.Rev. C 89, 064303 (2014)

D.Mikami, W.Horiuchi, Y.Suzuki

Electric dipole response of 6He: Halo-neutron and core excitations

NUCLEAR STRUCTURE 4,6He; calculated B(E1), E1 transition density, binding energy, S(2n), rms radii, proton, neutron density distributions, energy convergence, isoscalar and non-isoscalar compressional B(E1) from pigmy to giant dipole resonance energies. Investigation of neutron-halo and core excitations. Full microscopic six-body calculation with wavefunctions for ground and excited states expressed as superposition of explicitly correlated Gaussians. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.064303
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2014TE06      Prog.Theor.Exp.Phys. 2014, 101D02 (2014)

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

Proton radius of 14Be from measurement of charge-changing cross sections

NUCLEAR REACTIONS C(7Be, np), (9Be, np), (10Be, np), (11Be, np), (12Be, np), (14Be, np), E=90 MeV/nucleon; measured reaction products; deduced σ, proton and nucleon rms radii. Comparison with Glauber model calculations.

doi: 10.1093/ptep/ptu134
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2350.


2013HO06      Phys.Rev. C 87, 034001 (2013)

W.Horiuchi, Y.Suzuki

Spin-dipole strength functions of 4He with realistic nuclear forces

NUCLEAR STRUCTURE 4He; calculated isoscalar and isovector reduced transition probabilities, spin-dipole (SD) strength functions for discretized continuum 0-, 1- and 2- states, energy-weighted sum rules of SD strength functions. 4H, 4He, 4Li; calculated negative-parity levels, resonances, J, π, isospin, widths. Correlated Gaussians with complex scaling method. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.034001
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2012AR10      Prog.Theor.Phys.(Kyoto), Suppl. 196, 483 (2012)

K.Arai, S.Aoyama, Y.Suzuki, P.Descouvemont, D.Baye

Tensor Force Manifestations in Ab Initio Study of the 2H(d, γ)4He, 2H(d, p)3H, and 2H(d, n)3He Reactions

NUCLEAR REACTIONS 2H(d, γ)4He, 2H(d, p)3H, 2H(d, n)3He, E(cm)<10 MeV; calculated S-factors. Extended microscopic cluster model with realistic nucleon-nucleon interaction, comparison with available data.

doi: 10.1143/PTPS.196.483
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2012HO10      Phys.Rev. C 85, 054002 (2012)

W.Horiuchi, Y.Suzuki, K.Arai

Ab initio study of the photoabsorption of 4He

NUCLEAR REACTIONS 4He(γ, p), (γ, n), E<40 MeV; calculated photoabsorption cross section, E1 transition strength. Ab initio calculation with realistic nuclear forces and explicitly correlated Gaussian functions using complex scaling and microscopic R-matrix methods. Importance of 3H+p and 3He+n cluster configurations. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.054002
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2012HO19      Phys.Rev. C 86, 024614 (2012)

W.Horiuchi, T.Inakura, T.Nakatsukasa, Y.Suzuki

Glauber-model analysis of total reaction cross sections for Ne, Mg, Si, and S isotopes with Skyrme-Hartree-Fock densities

NUCLEAR REACTIONS 12C(17Ne, X), (18Ne, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), (33Ne, X), (34Ne, X), (20Mg, X), (21Mg, X), (22Mg, X), (23Mg, X), (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), (24Si, X), (25Si, X), (26Si, X), (27Si, X), (28Si, X), (29Si, X), (30Si, X), (31Si, X), (32Si, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (37Si, X), (38Si, X), (39Si, X), (40Si, X), (41Si, X), (42Si, X), (43Si, X), (44Si, X), (45Si, X), (46Si, X), (26S, X), (27S, X), (28S, X), (29S, X), (30S, X), (31S, X), (32S, X), (33S, X), (34S, X), (35S, X), (36S, X), (37S, X), (38S, X), (39S, X), (40S, X), (41S, X), (42S, X), (43S, X), (44S, X), (45S, X), (46S, X), (47S, X), (48S, X), (49S, X), (50S, X), E=240 MeV/nucleon; 12C(13O, X), (14O, X), (15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), (17Ne, X), (18Ne, X), (19Ne, X), (20Ne, X), (21Ne, X), (22Ne, X), (23Ne, X), (24Ne, X), (25Ne, X), (26Ne, X), (27Ne, X), (28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), (33Ne, X), (34Ne, X), (20Mg, X), (21Mg, X), (22Mg, X), (23Mg, X), (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=1000 MeV/nucleon; calculated total reaction σ. Glauber model for high-energy nucleus-nucleus collisions with SkM* interaction. Comparison with experimental data. Role of nuclear deformation in determining the matter radius.

NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32,33,34Ne, 22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38Mg, 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46Si, 26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50S; calculated point matter, neutron and proton radii, neutron Fermi energy for Ne isotopes, quadrupole deformation parameter. Skyrme-Hartree-Fock calculation SkM* and SLy4 interactions.

doi: 10.1103/PhysRevC.86.024614
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2012HO22      Prog.Theor.Phys.(Kyoto), Suppl. 196, 125 (2012)

W.Horiuchi, Y.Suzuki, K.Arai

Nuclear Reactions with a Realistic Nuclear Interaction Using a Square Integrable Basis

doi: 10.1143/PTPS.196.125
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2012KA33      Phys.Rev. C 86, 044601 (2012)

K.Kaki, Y.Suzuki, R.B.Wiringa

Polarized proton+4, 6, 8He elastic scattering with breakup effects in the eikonal approximation

NUCLEAR REACTIONS 4,6,8He(polarized p, p), E=71, 300, 500 MeV; calculated rms radii, density distribution, optical potential, σ(θ), analyzing powers. Glauber model. Pauli-blocking effect. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044601
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2012SU26      Eur.Phys.J.Plus 127, 111 (2012)

Y.Suzuki, K.Inoue

Kamioka Underground Observatories

doi: 10.1140/epjp/i2012-12111-2
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2011AO01      Int.J.Mod.Phys. E20, 775 (2011)

S.Aoyama, K.Arai, P.Descouvemont, Y.Suzuki, D.Baye

Extended microscopic cluster model study of four nucleon scattering

doi: 10.1142/S0218301311018654
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2011AR12      Phys.Rev.Lett. 107, 132502 (2011)

K.Arai, S.Aoyama, Y.Suzuki, P.Descouvemont, D.Baye

Tensor Force Manifestations in Ab Initio Study of the 2H(d, γ)4He, 2H(d, p)3H, and 2H(d, n)3He Reactions

NUCLEAR REACTIONS 2H(d, γ), (d, p), (d, n), E(cm)<10 MeV; calculated wave functions, phase shifts, σ, S-factors. Multichannel microscopic cluster model, ab initio calculations, comparison with experimental data.

doi: 10.1103/PhysRevLett.107.132501
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2011FE08      Phys.Rev. C 84, 054003 (2011)

H.Feldmeier, W.Horiuchi, T.Neff, Y.Suzuki

Universality of short-range nucleon-nucleon correlations

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated Argonne v8' potential contours, one-body point densities, two-body density contours in coordinate and momentum space, three-body correlations in the unitary correlation operator method (UCOM) approach. Correlated Gaussian basis approach for the Argonne v8' interaction.

doi: 10.1103/PhysRevC.84.054003
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2011HO09      Int.J.Mod.Phys. E20, 781 (2011)

W.Horiuchi, Y.Suzuki, T.Sato

Electro-weak transitions of 4He using realistic nuclear interactions

doi: 10.1142/S0218301311018666
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2011KA01      Phys.Rev. C 83, 021302 (2011)

R.Kanungo, A.Prochazka, W.Horiuchi, C.Nociforo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, Y.Suzuki, I.Szarka, I.Tanihata, Y.Utsuno, H.Weick, M.Winkler

Matter radii of 32-35Mg

NUCLEAR REACTIONS C, H(32Mg, X), (33Mg, X)(34Mg, X)(35Mg, X), E=900 MeV/nucleon, [secondary Mg beams from Be(48Ca, X) primary reaction]; measured interaction cross sections by detecting unreacted Mg particles by Bρ-ΔE-TOF method. 32,33,34,35Mg; deduced matter radii by Glauber model analysis. Comparison with HF and RMF predictions. Neutron skin thickness.

doi: 10.1103/PhysRevC.83.021302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0643. Data from this article have been entered in the XUNDL database. For more information, click here.


2011KA36      Phys.Rev. C 84, 061304 (2011)

R.Kanungo, A.Prochazka, M.Uchida, W.Horiuchi, G.Hagen, T.Papenbrock, C.Nociforo, T.Aumann, D.Boutin, D.Cortina-Gil, B.Davids, M.Diakaki, F.Farinon, H.Geissel, R.Gernhauser, J.Gerl, R.Janik, O.Jensen, B.Jonson, B.Kindler, R.Knobel, R.Krucken, M.Lantz, H.Lenske, Y.Litvinov, B.Lommel, K.Mahata, P.Maierbeck, A.Musumarra, T.Nilsson, C.Perro, C.Scheidenberger, B.Sitar, P.Strmen, B.Sun, Y.Suzuki, I.Szarka, I.Tanihata, H.Weick, M.Winkler

Exploring the anomaly in the interaction cross section and matter radius of 23O

NUCLEAR REACTIONS C(22O, X), (23O, X), [22O, 23O secondary beams from 9Be(48Ca, X), E=1 GeV/nucleon primary reaction], E=900 MeV/nucleon; measured energy loss, time of flight, magnetic rigidity. 22,23O; deduced interaction cross section, matter radii, neutron skin thickness. Glauber model analysis. Comparison with ab initio coupled-cluster theory.

doi: 10.1103/PhysRevC.84.061304
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0806. Data from this article have been entered in the XUNDL database. For more information, click here.


2011PI10      Nucl.Phys. A865, 43 (2011)

E.C.Pinilla, D.Baye, P.Descouvemont, W.Horiuchi, Y.Suzuki

Tests of the discretized-continuum method in three-body dipole strengths

NUCLEAR STRUCTURE 6He; calculated B(E1), halo structure. α+n+n model, R-matrix, discrete-continuum method, pseudostate method.

doi: 10.1016/j.nuclphysa.2011.06.030
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2011SU13      Int.J.Mod.Phys. E20, 753 (2011)

Y.Suzuki

Recent developments in nuclear cluster physics

doi: 10.1142/S0218301311018617
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2010AR02      Phys.Rev. C 81, 037301 (2010)

K.Arai, S.Aoyama, Y.Suzuki

Microscopic cluster model study of 3He+p scattering

NUCLEAR REACTIONS 3He(p, p), E(cm)=0-10 MeV; calculated scattering phase shifts using microscopic cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.037301
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2010HO03      Phys.Rev. C 81, 024606 (2010)

W.Horiuchi, Y.Suzuki, P.Capel, D.Baye

Probing the weakly-bound neutron orbit of 31Ne with total reaction and one-neutron removal cross sections

NUCLEAR REACTIONS 12C, 208Pb(31Ne, 30Ne), E=40-1000 MeV/nucleon; calculated total σ and one-neutron removal σ, matter density, E1 strengths, parallel-momentum distribution for the elastic breakup of 31Ne using Glauber and eikonal models.

NUCLEAR STRUCTURE 31Ne; calculated single-particle energies and discussed halo structure in the context of one-neutron removal reactions on 31Ne.

doi: 10.1103/PhysRevC.81.024606
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2010KO41      Nucl.Phys. A835, 358c (2010)

M.Kohno, Y.Fujiwara, Y.Suzuki

Quark-model predictions for the ΞN interaction and the implications for Ξ hypernuclei

NUCLEAR REACTIONS 12C(K-, K+), E at 1.8 GeV/c; calculated Ξ- hypernucleus production σ(E, θ). Comparison with data.

doi: 10.1016/j.nuclphysa.2010.01.218
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2010SU22      Nucl.Phys. A838, 20 (2010)

Y.Suzuki, D.Baye, A.Kievsky

Solving a coupled-channels scattering problem by adding confining potentials

NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-200 MeV; calculated phase shifts using coupled-channels Green function and Runge-Kutta methods.

doi: 10.1016/j.nuclphysa.2010.03.002
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2010SU23      Phys.Rev. C 82, 041303 (2010)

Y.Suzuki, S.Ohkubo

Enhanced E1 transitions and α+208Pb(3-) clustering in 212Po

NUCLEAR STRUCTURE 212Po; calculated levels, J, π, bands, B(E1) and B(E2) transition rates using coupled-channel α+208Pb cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.041303
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2009AB07      J.Phys.Soc.Jpn. 78, 044201 (2009)

B.Abu-Ibrahim, S.Iwasaki, W.Horiuchi, A.Kohama, Y.Suzuki

Elastic and Total Reaction Cross Sections of Oxygen Isotopes in Glauber Theory

NUCLEAR REACTIONS 16O(p, p), E=317, 1000 MeV; 20,21,23O(p, p), E=300 MeV; calculated σ(θ). 12C(15O, X), (16O, X), (17O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E=1 GeV/nucleon; calculated total reaction cross sections.

doi: 10.1143/JPSJ.78.044201
Citations: PlumX Metrics


2009BA07      Phys.Rev. C 79, 024607 (2009)

D.Baye, P.Capel, P.Descouvemont, Y.Suzuki

Four-body calculation of 6He breakup with the Coulomb-corrected eikonal method

NUCLEAR REACTIONS 208Pb(6He, X), E=70, 240 MeV/nucleon; calculated E1 strength functions, total and partial cross section using Coulomb corrected eikonal method and breakup of 6He halo nucleus treated as 3 body α+n+n model. $Comparison with experimental data.

doi: 10.1103/PhysRevC.79.024607
Citations: PlumX Metrics


2009SU01      Nucl.Phys. A818, 188 (2009)

Y.Suzuki, W.Horiuchi

Significance and properties of internucleon correlation functions

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated internucleon correlation functions, related features and their relation to ground state energies.

doi: 10.1016/j.nuclphysa.2008.12.009
Citations: PlumX Metrics


2009SU05      Nucl.Phys. A823, 1 (2009)

Y.Suzuki, W.Horiuchi, K.Arai

Phase-shift calculation using continuum-discretized states

NUCLEAR REACTIONS 1n(p, p), E≈0.5-100 MeV; 4He(n, n), E≈0.2-15 MeV; calculated phase shifts from the spectroscopic amplitude solved with Green's function. Comparison with other models and various potentials.

doi: 10.1016/j.nuclphysa.2009.03.004
Citations: PlumX Metrics


2008AB07      Phys.Rev. C 77, 034607 (2008); Publshiers note Phys.Rev. C 81, 019901 (2010)

B.Abu-Ibrahim, W.Horiuchi, A.Kohama, Y.Suzuki

Reaction cross sections of carbon isotopes incident on a proton

NUCLEAR REACTIONS 1H(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), (22C, X), E=40, 100, 200, 300, 425, 550, 650, 800 MeV/nucleon; calculated reaction σ, density distributions using Glauber model. Comparison with experimental data.

doi: 10.1103/PhysRevC.77.034607
Citations: PlumX Metrics


2008CA26      Phys.Rev. C 78, 054602 (2008)

P.Capel, D.Baye, Y.Suzuki

Coulomb-corrected eikonal description of the breakup of halo nuclei

NUCLEAR REACTIONS 12C, 208Pb(11Be, X), E=67, 69 MeV/nucleon; calculated σ. Coulomb-corrected eikonal approximation.

doi: 10.1103/PhysRevC.78.054602
Citations: PlumX Metrics


2008CA30      Int.J.Mod.Phys. E17, 2315 (2008)

P.Capel, G.Goldstein, D.Baye, Y.Suzuki

Breakup of halo nuclei within a Dynamical Eikonal Approximation

NUCLEAR REACTIONS C, Pb(11Be, X), E=67, 69 MeV; calculated break-up σ, σ(E), σ(p). Coulomb Corrected Eikonal (CCE) model.

doi: 10.1142/S0218301308011537
Citations: PlumX Metrics


2008FU02      Phys.Rev. C 77, 027001 (2008)

Y.Fujiwara, Y.Suzuki, M.Kohno, K.Miyagawa

Addendum to triton and hypertriton binding energies calculated from SU6 quark-model baryon-baryon interactions

NUCLEAR STRUCTURE 3H; calculated binding energies for nucleus and hypernucleus using SU6 model.

doi: 10.1103/PhysRevC.77.027001
Citations: PlumX Metrics


2008FU12      Prog.Theor.Phys.(Kyoto) 120, 289 (2008)

Y.Fujiwara, M.Kohno, Y.Suzuki

nα Resonating-Group Calculation with a Quark-Model G-Matrix NN Interaction

doi: 10.1143/PTP.120.289
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2008HO08      Phys.Rev. C 78, 034305 (2008)

W.Horiuchi, Y.Suzuki

Inversion doublets of 3N + N cluster structure in excited states of 4He

NUCLEAR STRUCTURE 4He; calculated levels, J, π. Comparison with experimental data.

doi: 10.1103/PhysRevC.78.034305
Citations: PlumX Metrics


2008SU01      Phys.Lett. B 659, 160 (2008)

Y.Suzuki, H.Matsumura, M.Orabi, Y.Fujiwara, P.Descouvemont, M.Theeten, D.Baye

Local versus nonlocal αα interactions in a 3α description of 12C

NUCLEAR STRUCTURE 12C; calculated ground and excited 0+ states energies, radii. α-cluster model with non-local forces.

doi: 10.1016/j.physletb.2007.10.033
Citations: PlumX Metrics


2007FU02      Nucl.Phys. A784, 161 (2007)

Y.Fujiwara, M.Kohno, Y.Suzuki

Λα, Σα and Ξα potentials derived from the SU6 quark-model baryon-baryon interaction

NUCLEAR STRUCTURE 5He; calculated hyperon-nucleus potentials, hypernucleus bound state energies.

doi: 10.1016/j.nuclphysa.2006.12.005
Citations: PlumX Metrics


2007FU03      Prog.Part.Nucl.Phys. 58, 439 (2007)

Y.Fujiwara, Y.Suzuki, C.Nakamoto

Baryon-baryon interactions in the SU6 quark model and their applications to light nuclear systems

doi: 10.1016/j.ppnp.2006.08.001
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2007HO09      Phys.Rev. C 75, 044607 (2007); Erratum Phys.Rev. C 76, 039903 (2007)

W.Horiuchi, Y.Suzuki, B.Abu-Ibrahim, A.Kohama

Systematic analysis of reaction cross sections of carbon isotopes

NUCLEAR REACTIONS 12C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), (22C, X), E=40-1000 MeV/nucleon; calculated reaction σ. Glauber approximation, eikonal model, comparison with data.

doi: 10.1103/PhysRevC.75.044607
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2007HO15      Phys.Rev. C 76, 024311 (2007)

W.Horiuchi, Y.Suzuki

Momentum distribution and correlation of two-nucleon relative motion in 6He and 6Li

doi: 10.1103/PhysRevC.76.024311
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2007MA62      Nucl.Phys. A790, 534c (2007)

H.Matsumura, Y.Suzuki

Decay width of the Θ+(1540) in 5-quark dynamical calculation

doi: 10.1016/j.nuclphysa.2007.03.089
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2007SU12      Nucl.Phys. A790, 223c (2007)

Y.Suzuki, Y.Fujiwara, W.Horiuchi, H.Matsumura, M.Orabi

Dynamics of macroscopic and microscopic three-body systems

NUCLEAR STRUCTURE 3H; calculated binding energies. Quark-model interactions. Comparison with data.

doi: 10.1016/j.nuclphysa.2007.03.039
Citations: PlumX Metrics


2007TH16      Phys.Rev. C 76, 054003 (2007)

M.Theeten, H.Matsumura, M.Orabi, D.Baye, P.Descouvemont, Y.Fujiwara, Y.Suzuki

Three-body model of light nuclei with microscopic nonlocal interactions

NUCLEAR STRUCTURE 6He, 9Be, 12C; calculated potential functions, phase shifts, charge densities, neutron densities. Compared to experimental energies.

doi: 10.1103/PhysRevC.76.054003
Citations: PlumX Metrics


2006HO01      Phys.Rev. C 73, 037304 (2006); Erratum Phys.Rev. C 74, 019901 (2006)

W.Horiuchi, Y.Suzuki

Structure of and E2 transition in 16C in a 14C + n + n model

NUCLEAR STRUCTURE 16C; calculated levels, J, π, transition B(E2). Three-body model.

doi: 10.1103/PhysRevC.73.037304
Citations: PlumX Metrics


2006HO15      Phys.Rev. C 74, 034311 (2006)

W.Horiuchi, Y.Suzuki

22C: An s-wave two-neutron halo nucleus

NUCLEAR STRUCTURE 22C; calculated binding energy, density distributions, radii, halo features. Borromean three-body model.

NUCLEAR REACTIONS 12C(12C, X), (20C, X), (22C, X), E=10-1000 MeV/nucleon; calculated reaction σ.

doi: 10.1103/PhysRevC.74.034311
Citations: PlumX Metrics


2006MA30      Nucl.Phys. A722, 55 (2006)

H.Matsumura, Y.Suzuki

Structure and decay width of the Θ+(1540) in a one-gluon exchange model

doi: 10.1016/j.nuclphysa.2006.03.006
Citations: PlumX Metrics


2006MA52      Nucl.Phys. A776, 1 (2006)

H.Matsumura, M.Orabi, Y.Suzuki, Y.Fujiwara

Removal of forbidden states in a three-α system

NUCLEAR STRUCTURE 12C; calculated ground and excited 0+ states energies, radii. α-cluster model.

doi: 10.1016/j.nuclphysa.2006.07.002
Citations: PlumX Metrics


2005FU05      Nucl.Phys. A754, 43c (2005)

Y.Fujiwara, C.Nakamoto, M.Kohno, Y.Suzuki, K.Miyagawa

Interactions between octet baryons in the SU6 quark model and their applications to light hypernuclei

NUCLEAR STRUCTURE 3H, 6He, 9Be; calculated hypernucleus ground and excited states energies. Three-cluster Fadeev formalism.

doi: 10.1016/j.nuclphysa.2005.02.001
Citations: PlumX Metrics


2005SU03      Prog.Theor.Phys.(Kyoto) 113, 87 (2005)

Y.Suzuki, H.Matsumura

Effective Interaction for the Jastrow Model Wave Function with the Transcorrelated Method

doi: 10.1143/PTP.113.87
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2004AB12      Nucl.Phys. A738, 440 (2004)

B.Abu-Ibrahim, Y.Suzuki

Breakup effects in 6He + 12C elastic scattering

NUCLEAR REACTIONS 12C(6He, 6He), E=40 MeV/nucleon; calculated σ(θ); deduced breakup channel contribution.

doi: 10.1016/j.nuclphysa.2004.04.082
Citations: PlumX Metrics


2004AB13      Phys.Rev. C 70, 011603 (2004)

B.Abu-Ibrahim, Y.Suzuki

Dynamic polarization potentials for the halo nucleus 6He in medium-energy elastic scattering

NUCLEAR REACTIONS 12C(6He, 6He), E=40-800 MeV; calculated reaction σ, σ(θ), dynamic polarization potentials.

doi: 10.1103/PhysRevC.70.011603
Citations: PlumX Metrics


2004AB29      Prog.Theor.Phys.(Kyoto) 112, 1013 (2004); Addendum Prog.Theor.Phys.(Kyoto) 114, 901 (2005)

B.Abu-Ibrahim, Y.Suzuki

Breakup of One-Neutron Halo Nuclei within Eikonal Model

NUCLEAR REACTIONS 12C, 208Pb(11Be, n10Be), (19C, n18C), E=68, 520 MeV/nucleon; calculated elastic and inelastic breakup probabilities, σ(E). Eikonal model, comparison with data.

doi: 10.1143/PTP.112.1013
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2004FU05      Phys.Rev. C 69, 037002 (2004)

Y.Fujiwara, Y.Suzuki, M.Kohno

Case of almost redundant components in 3α Faddeev equations

doi: 10.1103/PhysRevC.69.037002
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2004FU10      Nucl.Phys. A737, 243 (2004)

Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, C.Nakamoto

A Realistic Baryon-Baryon Interaction in the SU6 Quark Model and its Applications to Few-Baryon Systems

doi: 10.1016/j.nuclphysa.2004.03.083
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2004FU11      Few-Body Systems 34, 237 (2004)

Y.Fujiwara, M.Kohno, Y.Suzuki

Solving Three-Cluster OCM Equations in the Faddeev Formalism

NUCLEAR STRUCTURE 12C; calculated 3α cluster states energies, related features. Orthogonality condition models, Faddeev formalism.

doi: 10.1007/s00601-004-0021-y
Citations: PlumX Metrics


2004FU14      Nucl.Phys. A738, 382 (2004)

Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki

Faddeev Calculation of the Hypertriton in the Quark-Model NN and YN Interactions

NUCLEAR STRUCTURE 3H; calculated hypernucleus wave function, binding energy. Three-cluster Fadeev formalism.

doi: 10.1016/j.nuclphysa.2004.04.066
Citations: PlumX Metrics


2004FU15      Nucl.Phys. A738, 495 (2004)

Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, D.Baye, J.-M.Sparenberg

A Consistent 3α and 2αΛ Faddeev Calculation using the 2α RGM Kernel

doi: 10.1016/j.nuclphysa.2004.04.095
Citations: PlumX Metrics


2004FU18      Phys.Rev. C 70, 024001 (2004)

Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki

Faddeev calculation of the hypertriton using the SU6 quark-model nucleon-nucleon and hyperon-nucleon interactions

NUCLEAR STRUCTURE 3H; calculated hypertriton binding energy, wave function, related features. Three-cluster Faddeev formalism.

doi: 10.1103/PhysRevC.70.024001
Citations: PlumX Metrics


2004FU19      Phys.Rev. C 70, 024002 (2004)

Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, D.Baye, J.-M.Sparenberg

Faddeev calculation of 3α and ααΛ systems using αα resonating-group method kernels

NUCLEAR STRUCTURE 12C; calculated 3α-cluster states energies. 9Be; calculated hypernucleus ground and excited states energies. Faddeev calculations, two-cluster resonating-group method kernels.

doi: 10.1103/PhysRevC.70.024002
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2004FU22      Phys.Rev. C 70, 037001 (2004)

Y.Fujiwara, M.Kohno, K.Miyagawa, Y.Suzuki, J.-M.Sparenberg

Faddeev calculation of 6ΛΛHe using SU6 quark-model baryon-baryon interactions

NUCLEAR STRUCTURE 6He; calculated two-Λ hypernucleus binding energy. Faddeev formalism, two-cluster resonating-group method.

doi: 10.1103/PhysRevC.70.037001
Citations: PlumX Metrics


2004FU26      Phys.Rev. C 70, 047002 (2004)

Y.Fujiwara, M.Kohno, K.Miyagawa, Y.Suzuki

Spin-orbit splitting of 9ΛBe excited states studied with the SU6 quark-model baryon-baryon interactions

NUCLEAR STRUCTURE 9Be; calculated hypernucleus excited states energies, spin-orbit splitting.

doi: 10.1103/PhysRevC.70.047002
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2004FU31      Prog.Theor.Phys.(Kyoto), Suppl. 156, 17 (2004)

Y.Fujiwara, C.Nakamoto, Y.Suzuki, M.Kohno, K.Miyagawa

Quark-Model Baryon-Baryon Interaction and Its Applications to Hypernuclei

NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, radii. 3H, 6He, 9Be; calculated hypernucleus ground and excited states energies. Quark-model baryon-baryon interaction.

doi: 10.1143/PTPS.156.17
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2004LO12      Acta Phys.Hung.N.S. 19, 305 (2004)

R.G.Lovas, K.Varga, Y.Suzuki

Description of Nuclei in Terms of Their Substructures

NUCLEAR STRUCTURE 6,11Li; calculated binding energies, radii, quadrupole moments, μ. Cluster models.

NUCLEAR REACTIONS 12C(11Li, X), E=800 MeV/nucleon; calculated reaction σ.

doi: 10.1556/APH.19.2004.3-4.27
Citations: PlumX Metrics


2004MA54      Nucl.Phys. A739, 238 (2004)

H.Matsumura, Y.Suzuki

A microscopic analysis of the amount of α-condensation in 12C

NUCLEAR STRUCTURE 12C; calculated α-cluster states energies, wave functions, degree of α-condensation. Microscopic cluster model.

doi: 10.1016/j.nuclphysa.2004.04.104
Citations: PlumX Metrics


2004SU26      Phys.Rev. C 70, 051302 (2004)

Y.Suzuki, H.Matsumura, B.Abu-Ibrahim

Structure of 15, 16C and phenomenology of the hindered E2 transition in 16C

NUCLEAR STRUCTURE 15,16C; calculated levels, J, π, radii. 15,16C, 17F, 18Ne, 17,18O; analyzed transitions B(E2); deduced polarization charge.

NUCLEAR REACTIONS 12C(16C, 15CX), E=83 MeV/nucleon; calculated fragment parallel momentum distribution. Comparison with data.

doi: 10.1103/PhysRevC.70.051302
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2003AB05      Comput.Phys.Commun. 151, 369 (2003)

B.Abu-Ibrahim, Y.Ogawa, Y.Suzuki, I.Tanihata

Cross section calculations in Glauber model: I. Core plus one-nucleon case

NUCLEAR REACTIONS 12C(12C, X), (13C, X), E=100-1000 MeV/nucleon; calculated total reaction σ. 12C(19C, n18C), E=100-1000 MeV/nucleon; calculated elastic and inelastic neutron-removal σ. 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ). 9Be(11Be, 10BeX), E=63 MeV/nucleon; 12C(8B, 7BeX), E=1.44 GeV/nucleon; calculated fragment longitudinal momentum distribution. Glauber model, comparisons with data.

doi: 10.1016/S0010-4655(02)00734-8
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2003AB26      Nucl.Phys. A728, 118 (2003); Erratum Nucl.Phys. A732, 218 (2004)

B.Abu-Ibrahim, Y.Suzuki

The optical potential of 6He in the eikonal approximation

NUCLEAR REACTIONS 12C(6He, 6He), E=40, 70, 200, 800 MeV/nucleon; 12C(α, α), E=40 MeV/nucleon; calculated σ(θ), phase shifts, optical potential, role of breakup channel. Eikonal approximation.

doi: 10.1016/j.nuclphysa.2003.08.025
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2003FU12      Nucl.Phys. A721, 983c (2003)

Y.Fujiwara, K.Miyagawa, Y.Suzuki, M.Kohno, H.Nemura

Three-Nucleon Bound State in the SU6 Quark Model for the Baryon-Baryon Interaction

doi: 10.1016/S0375-9474(03)01265-X
Citations: PlumX Metrics


2003NE22      Mod.Phys.Lett. A 18, 139 (2003)

H.Nemura, Y.Akaishi, Y.Suzuki

Ab initio calculation of 5ΛHe with explicit Σ admixture

NUCLEAR STRUCTURE 3,4H, 4,5He; calculated hyperon binding energies, Σ hyperon admixture.

doi: 10.1142/S0217732303010120
Citations: PlumX Metrics


2003SU14      Nucl.Phys. A718, 83c (2003)

Y.Suzuki, and the Super-Kamiokande Collaboration

Neutrinos in Super-Kamiokande

doi: 10.1016/S0375-9474(03)00683-3
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2002FU01      Phys.Rev. C65, 014002 (2002)

Y.Fujiwara, T.Fujita, M.Kohno, C.Nakamoto, Y.Suzuki

Resonating-Group Study of Baryon-Baryon Interactions for the Complete Baryon Octet: NN interaction

NUCLEAR REACTIONS 1H(n, X), (p, X), E ≤ 800 MeV; calculated phase shifts. Unified framework of resonating-group method for baryon-baryon interactions.

NUCLEAR STRUCTURE 2H; calculated binding energy, radius, μ, quadrupole moment. Unified framework of resonating-group method for baryon-baryon interactions.

doi: 10.1103/PhysRevC.65.014002
Citations: PlumX Metrics


2002FU12      Prog.Theor.Phys.(Kyoto) 107, 745 (2002)

Y.Fujiwara, H.Nemura, Y.Suzuki, K.Miyagawa, M.Kohno

Three-Cluster Equation Using the Two-Cluster RGM Kernel

doi: 10.1143/PTP.107.745
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2002FU13      Phys.Rev. C66, 021001 (2002)

Y.Fujiwara, K.Miyagawa, M.Kohno, Y.Suzuki, H.Nemura

Triton binding energy calculated from the SU6 quark-model nucleon-nucleon interaction

NUCLEAR STRUCTURE 2,3H, 3He; calculated binding energies, radii. Fadeev approach, quark-model interaction.

doi: 10.1103/PhysRevC.66.021001
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