NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = Y.Suzuki Found 203 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
2021SU08 Few-Body Systems 62, 2 (2021), Erratum Few-Body Systems 64, 73 (2023) 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
2021SU18 Phys.Rev. C 104, 024327 (2021) 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
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
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
2020SU03 Phys.Rev. C 101, 014002 (2020) Adiabatic hyperspherical potentials with localized correlated Gaussians
doi: 10.1103/PhysRevC.101.014002
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
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
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
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
2017SU12 Phys.Rev. C 95, 044320 (2017) 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
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
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
2016NA31 Phys.Rev. C 94, 035803 (2016) Quark-Pauli effects in three octet-baryons
doi: 10.1103/PhysRevC.94.035803
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
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
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
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
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
2014HO01 Phys.Rev. C 89, 011304 (2014) 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
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
2014HO15 Phys.Rev. C 90, 034001 (2014) 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
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
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
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
2013HO06 Phys.Rev. C 87, 034001 (2013) 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
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
2012HO10 Phys.Rev. C 85, 054002 (2012) 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
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
2012HO22 Prog.Theor.Phys.(Kyoto), Suppl. 196, 125 (2012) Nuclear Reactions with a Realistic Nuclear Interaction Using a Square Integrable Basis
doi: 10.1143/PTPS.196.125
2012KA33 Phys.Rev. C 86, 044601 (2012) 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
2012SU26 Eur.Phys.J.Plus 127, 111 (2012) Kamioka Underground Observatories
doi: 10.1140/epjp/i2012-12111-2
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
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
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
2011HO09 Int.J.Mod.Phys. E20, 781 (2011) Electro-weak transitions of 4He using realistic nuclear interactions
doi: 10.1142/S0218301311018666
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
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
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
2011SU13 Int.J.Mod.Phys. E20, 753 (2011) Recent developments in nuclear cluster physics
doi: 10.1142/S0218301311018617
2010AR02 Phys.Rev. C 81, 037301 (2010) 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
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
2010KO41 Nucl.Phys. A835, 358c (2010) 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
2010SU22 Nucl.Phys. A838, 20 (2010) 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
2010SU23 Phys.Rev. C 82, 041303 (2010) 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
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
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
2009SU01 Nucl.Phys. A818, 188 (2009) 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
2009SU05 Nucl.Phys. A823, 1 (2009) 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
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
2008CA26 Phys.Rev. C 78, 054602 (2008) 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
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
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
2008FU12 Prog.Theor.Phys.(Kyoto) 120, 289 (2008) nα Resonating-Group Calculation with a Quark-Model G-Matrix NN Interaction
doi: 10.1143/PTP.120.289
2008HO08 Phys.Rev. C 78, 034305 (2008) 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
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
2007FU02 Nucl.Phys. A784, 161 (2007) 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
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
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
2007HO15 Phys.Rev. C 76, 024311 (2007) Momentum distribution and correlation of two-nucleon relative motion in 6He and 6Li
doi: 10.1103/PhysRevC.76.024311
2007MA62 Nucl.Phys. A790, 534c (2007) Decay width of the Θ+(1540) in 5-quark dynamical calculation
doi: 10.1016/j.nuclphysa.2007.03.089
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
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
2006HO01 Phys.Rev. C 73, 037304 (2006); Erratum Phys.Rev. C 74, 019901 (2006) 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
2006HO15 Phys.Rev. C 74, 034311 (2006) 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
2006MA30 Nucl.Phys. A722, 55 (2006) Structure and decay width of the Θ+(1540) in a one-gluon exchange model
doi: 10.1016/j.nuclphysa.2006.03.006
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
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
2005SU03 Prog.Theor.Phys.(Kyoto) 113, 87 (2005) Effective Interaction for the Jastrow Model Wave Function with the Transcorrelated Method
doi: 10.1143/PTP.113.87
2004AB12 Nucl.Phys. A738, 440 (2004) 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
2004AB13 Phys.Rev. C 70, 011603 (2004) 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
2004AB29 Prog.Theor.Phys.(Kyoto) 112, 1013 (2004); Addendum Prog.Theor.Phys.(Kyoto) 114, 901 (2005) 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
2004FU05 Phys.Rev. C 69, 037002 (2004) Case of almost redundant components in 3α Faddeev equations
doi: 10.1103/PhysRevC.69.037002
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
2004FU11 Few-Body Systems 34, 237 (2004) 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
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
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
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
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
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
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
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
2004LO12 Acta Phys.Hung.N.S. 19, 305 (2004) 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
2004MA54 Nucl.Phys. A739, 238 (2004) 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
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
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
2003AB26 Nucl.Phys. A728, 118 (2003); Erratum Nucl.Phys. A732, 218 (2004) 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
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
2003NE22 Mod.Phys.Lett. A 18, 139 (2003) 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
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
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
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
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
2002NE11 Phys.Rev.Lett. 89, 142504 (2002) Ab initio Approach to s-Shell Hypernuclei Λ3H, Λ4H, Λ4He, and Λ5He with a ΛN-ΣN Interaction NUCLEAR STRUCTURE 3,4H, 4,5He; calculated hypernucleus binding energies, wave functions, role of Σ admixture.
doi: 10.1103/PhysRevLett.89.142504
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