NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = Y.Ogawa Found 33 matches. 2013ON02 Phys.Lett. B 725, 277 (2013) H.J.Ong, I.Tanihata, A.Tamii, T.Myo, K.Ogata, M.Fukuda, K.Hirota, K.Ikeda, D.Ishikawa, T.Kawabata, H.Matsubara, K.Matsuta, M.Mihara, T.Naito, D.Nishimura, Y.Ogawa, H.Okamura, A.Ozawa, D.Y.Pang, H.Sakaguchi, K.Sekiguchi, T.Suzuki, M.Taniguchi, M.Takashina, H.Toki, Y.Yasuda, M.Yosoi, J.Zenihiro Probing effect of tensor interactions in 16O via (p, d) reaction NUCLEAR REACTIONS 16O(p, d), E=198, 295, 392 MeV; measured reaction products; deduced σ(θ), tensor interaction in one-nucleon transfer reactions.
doi: 10.1016/j.physletb.2013.07.038
2012OG08 J.Phys.:Conf.Ser. 381, 012111 (2012) Extended Brueckner-Hartree-Fock theory with pionic correlation in finite nuclei
doi: 10.1088/1742-6596/381/1/012111
2011OG05 Nucl.Phys. A860, 22 (2011) Relativistic chiral mean field model for finite nuclei NUCLEAR STRUCTURE 12C, 16O; calculated mass excess, pion energy using RCMF (Relativistic Chiral Mean Field) with pionic correlations.
doi: 10.1016/j.nuclphysa.2011.04.015
2009HU02 Phys.Rev. C 79, 024305 (2009) J.Hu, Y.Ogawa, H.Toki, A.Hosaka, H.Shen Extended relativistic chiral mean field model for nuclear matter
doi: 10.1103/PhysRevC.79.024305
2008TA26 Nucl.Phys. A811, 306 (2008) S.Tamenaga, H.Toki, A.Haga, Y.Ogawa Spontaneous chiral symmetry breaking in the massless linear sigma model by fermion and boson loop corrections NUCLEAR STRUCTURE 16O; calculated baryon density using the (massless) chiral sigma models.
doi: 10.1016/j.nuclphysa.2008.07.015
2007OG03 Phys.Rev. C 76, 014305 (2007) Relativistic chiral mean-field model with parity and charge projection for finite nuclei NUCLEAR STRUCTURE A=12, 16, 28, 0, 56; calculated ground state properties using the CPPCMF chiral mean field model.
doi: 10.1103/PhysRevC.76.014305
2007TO12 Prog.Part.Nucl.Phys. 59, 209 (2007) H.Toki, Y.Ogawa, S.Tamenaga, A.Haga Relativistic chiral mean field model for finite nuclei
doi: 10.1016/j.ppnp.2006.12.011
2006OG02 Phys.Rev. C 73, 034301 (2006) Y.Ogawa, H.Toki, S.Tamenaga, S.Sugimoto, K.Ikeda Charge and parity projected relativistic mean field model with pion for finite nuclei NUCLEAR STRUCTURE 4He; calculated ground-state energy, matter density distribution, dependence on meson-nucleon potential. Charge and parity projected relativistic mean field model.
doi: 10.1103/PhysRevC.73.034301
2004OG04 Prog.Theor.Phys.(Kyoto) 111, 75 (2004) Y.Ogawa, H.Toki, S.Tamenaga, H.Shen, A.Hosaka, S.Sugimoto, K.Ikeda Chiral Sigma Model with Pion Mean Field in Finite Nuclei NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn, 64Ge, 68Se; calculated single-particle level energies, pion mean-field features.
doi: 10.1143/PTP.111.75
2004TO13 Nucl.Phys. A738, 87 (2004) H.Toki, Y.Ogawa, S.Tamenaga, S.Sugimoto, K.Ikeda Chiral Symmetry and Finite Pion Mean Field in Nuclei NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn, 64Ge, 68Se; calculated proton single-particle levels, binding energy per nucleon; deduced role of chiral symmetry. Chiral sigma model with finite pion mean field.
doi: 10.1016/j.nuclphysa.2004.04.016
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
2003KA43 Phys.Lett. B 571, 21 (2003) R.Kanungo, M.Chiba, S.Adhikari, D.Fang, N.Iwasa, K.Kimura, K.Maeda, S.Nishimura, Y.Ogawa, T.Ohnishi, A.Ozawa, C.Samanta, T.Suda, T.Suzuki, Q.Wang, C.Wu, Y.Yamaguchi, K.Yamada, A.Yoshida, T.Zheng, I.Tanihata Possibility of a two-proton halo in 17Ne NUCLEAR REACTIONS 9Be(17Ne, X), E=66 MeV/nucleon; measured particle spectra, longitudinal momentum distribution, two-proton removal σ. 17Ne deduced two-proton halo features.
doi: 10.1016/j.physletb.2003.07.050
2002KA34 Nucl.Phys. A701, 378c (2002) R.Kanungo, I.Tanihata, Y.Ogawa, H.Toki, A.Ozawa Halo Structure in 19C NUCLEAR REACTIONS 12C(19C, X), E=910, 960 MeV/nucleon; analyzed interaction σ, longitudinal momentum distributions following breakup. 19C deduced halo features.
doi: 10.1016/S0375-9474(01)01614-1
2002SU12 Phys.Rev.Lett. 89, 012501 (2002) T.Suzuki, Y.Ogawa, M.Chiba, M.Fukuda, N.Iwasa, T.Izumikawa, R.Kanungo, Y.Kawamura, A.Ozawa, T.Suda, I.Tanihata, S.Watanabe, T.Yamaguchi, Y.Yamaguchi Momentum Distribution of 15B Fragments from the Breakup of 17B NUCLEAR REACTIONS 9Be(17B, 15BX), E=70 MeV/nucleon; measured fragment longitudinal momentum distribution, two-neutron removal σ. 17B deduced halo structure. Glauber-type analysis.
doi: 10.1103/PhysRevLett.89.012501
2001AR22 Prog.Theor.Phys.(Kyoto), Suppl. 142, 97 (2001) K.Arai, Y.Ogawa, Y.Suzuki, K.Varga Microscopic Multicluster Description of Light Exotic Nuclei with Stochastic Variational Method on Correlated Gaussians NUCLEAR STRUCTURE 6,8He, 6Li; calculated ground-state energies, matter density distributions, two-neutron removal amplitudes. 7Be, 7,8,9Li, 8B, 9C; calculated radii, μ, quadrupole moments, density distributions. 9,10Be, 9B calculated levels, J, π. 8,9Be, 9B; calculated resonance energies, widths. Microscopic multicluster model, comparisons with data. NUCLEAR REACTIONS 6He(p, p), E=717 MeV; calculated σ(θ). Microscopic multicluster model, comparisons with data.
doi: 10.1143/PTPS.142.97
2001OG10 Prog.Theor.Phys.(Kyoto), Suppl. 142, 157 (2001) Y.Ogawa, T.Kido, K.Yabana, Y.Suzuki Microscopic Theories for the Reactions in Halo Nuclei NUCLEAR REACTIONS 1H, Be, C, 27Al, Cu, Pb(11Li, X), E=800 MeV/nucleon; calculated interaction σ, two-neutron removal σ. 12C(11Li, 9Li), E=800 MeV/nucleon; C(8B, 7BeX), E=1471 MeV/nucleon; calculated fragment longitudinal momentum distributions. 12C(11Li, X), E=10-200 MeV/nucleon; calculated reaction σ, breakup σ. Comparisons with data.
doi: 10.1143/PTPS.142.157
2001OZ03 Nucl.Phys. A691, 599 (2001) A.Ozawa, O.Bochkarev, L.Chulkov, D.Cortina, H.Geissel, M.Hellstrom, M.Ivanov, R.Janik, K.Kimura, T.Kobayashi, A.A.Korsheninnikov, G.Munzenberg, F.Nickel, Y.Ogawa, A.A.Ogloblin, M.Pfutzner, V.Pribora, H.Simon, B.Sitar, P.Strmen, K.Summerer, T.Suzuki, I.Tanihata, M.Winkler, K.Yoshida Measurements of Interaction Cross Sections for Light Neutron-Rich Nuclei at Relativistic Energies and Determination of Effective Matter Radii NUCLEAR REACTIONS C(10B, X), (11B, X), (12C, X), (13C, X), (14C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), (14N, X), (15N, X), (16N, X), (18N, X), (19N, X), (21N, X), (22N, X), (23N, X), (16O, X), (17O, X), (18O, X), (19O, X), (21O, X), (22O, X), (23O, X), (24O, X), (18F, X), (19F, X), (21F, X), (23F, X), (24F, X), (25F, X), (26F, X), E ≈ 950 MeV/nucleon; measured interaction σ. 10,11B, 12,13,14,16,17,18,19,20C, 14,15,16,18,19,21,22,23N, 16,17,18,19,21,22,23,24O, 18,19,21,23,24,25,26F deduced radii. 19C, 22N, 23O, 24F deduced possible one-neutron halo features. Glauber model analysis.
doi: 10.1016/S0375-9474(01)00563-2
2000KA36 Nucl.Phys. A677, 171 (2000) R.Kanungo, I.Tanihata, Y.Ogawa, H.Toki, A.Ozawa Halo Structure in 19C: a Glauber model analysis NUCLEAR REACTIONS 12C(19C, X), E=910, 960 MeV/nucleon; 9Be(19C, X), E=88 MeV/nucleon; analyzed longitudinal momentum distributions, reaction σ. 19C deduced ground-state configuration. Glauber model analysis.
doi: 10.1016/S0375-9474(00)00306-7
2000OG03 Nucl.Phys. A673, 122 (2000) Y.Ogawa, K.Arai, Y.Suzuki, K.Varga Microscopic Four-Cluster Description of 10Be and 10C with the Stochastic Variational Method NUCLEAR STRUCTURE 10Be; calculated levels, J, π, spectroscopic factors. 10Be, 10C; calculated transition strengths. 8,9,10Be, 10C; calculated radii, density distributions. Microscopic four-cluster model.
doi: 10.1016/S0375-9474(00)00133-0
1999FU08 Nucl.Phys. A656, 209 (1999) M.Fukuda, M.Mihara, T.Fukao, S.Fukuda, M.Ishihara, S.Ito, T.Kobayashi, K.Matsuta, T.Minamisono, S.Momota, T.Nakamura, Y.Nojiri, Y.Ogawa, T.Ohtsubo, T.Onishi, A.Ozawa, T.Suzuki, M.Tanigaki, I.Tanihata, K.Yoshida Density Distribution of 8B Studied via Reaction Cross Sections NUCLEAR REACTIONS 9Be, 12C, 27Al(8B, X), (7Be, X), E≈ 35, 60 MeV/nucleon; 9Be, 12C, 27Al(6Li, X), E≈ 40 MeV/nucleon; measured interaction, reaction σ. 9Be, 12C, 27Al(8B, 7Be), E≈ 35, 60 MeV/nucleon; measured 1-proton removal σ. 8B deduced rms radius, halo features, density distributions. Glauber model analysis. Secondary beams from 12C fragmentation.
doi: 10.1016/S0375-9474(99)00308-5
1997OG01 Nucl.Phys. A616, 239c (1997) Momentum Distribution of 7Be from (8B, 7Be) Reaction within the Glauber Model NUCLEAR REACTIONS 12C(8B, p7Be), E=1.47 GeV/nucleon; calculated 7Be fragment longitudinal momentum distribution; deduced core absorption effect role. Glauber model.
doi: 10.1016/S0375-9474(97)00094-8
1997VA05 Nucl.Phys. A616, 383c (1997) K.Varga, Y.Suzuki, K.Arai, Y.Ogawa Microscopic Description of Light Unstable Nuclei with the Stochastic Variational Method NUCLEAR STRUCTURE 9Be; calculated levels, Γ, matter, nucleon radii, μ, quadrupole moment, interaction σ, B(λ). 9B; calculated levels, Γ. 6He, 7Li; calculated energies, rms radii. 6He, 7,8,9Li, 7Be, 8B, 9C, 9Be; calculated matter, nucleon radii vs occupation probability. 3,4,6He, 8Be, 16O; calculated binding energies. Microscopic multi-cluster model, stochastic variational method.
doi: 10.1016/S0375-9474(97)00105-X
1996AR05 Phys.Rev. C54, 132 (1996) K.Arai, Y.Ogawa, Y.Suzuki, K.Varga Structure of the Mirror Nuclei 9Be and 9B in a Microscopic Cluster Model NUCLEAR STRUCTURE 9Be; calculated levels, Γ, nucleon, matter radii, quadrupole moment, B(λ), μ, form factors, nucleon monopole, quadrupole density distributions. 9B calculated levels, Γ. Microscopic three-cluster model. RADIOACTIVITY 9Li(β-); calculated β-decay log ft. Microscopic three-cluster model.
doi: 10.1103/PhysRevC.54.132
1996OB01 Nucl.Phys. A609, 74 (1996) M.M.Obuti, T.Kobayashi, D.Hirata, Y.Ogawa, A.Ozawa, K.Sugimoto, I.Tanihata, D.Olson, W.Christie, H.Wieman Interaction Cross Section and Interaction Radius of the 8B Nucleus NUCLEAR REACTIONS C(8B, X), E=790 MeV/nucleon; measured interaction σ. 8B deduced nucleon distribution rms radius, halo tail, separation energy relationship.
doi: 10.1016/0375-9474(96)00267-9
1996SU11 Phys.Rev. C54, 2073 (1996) Y.Suzuki, K.Arai, Y.Ogawa, K.Varga Occupation Probability of Harmonic-Oscillator Quanta for Microscopic Cluster-Model Wave Functions NUCLEAR STRUCTURE 6He, 6,9Li, 9Be, 12C; caluclated harmonic oscillator quanta occupation probability; deduced possibility of quantifying excitation across major shell for different models. Microscopic cluster model.
doi: 10.1103/PhysRevC.54.2073
1995OG04 Nucl.Phys. A588, 77c (1995) Transverse Momentum Distributions of a 9Li Fragment in the (11Li, 9Li) Reaction and Neutron Correlations NUCLEAR REACTIONS 12C(11Li, 9Li), E=800 MeV/nucleon; calculated 9Li transverse, longitudinal momentum distributions; deduced halo neutron motion features. Glauber model, hybrid model wave function.
doi: 10.1016/0375-9474(95)00102-7
1994OG01 Nucl.Phys. A571, 784 (1994) Momentum Distributions of a 9Li Fragment Arising from the (11Li, 9Li) Reaction and Neutron Correlations NUCLEAR REACTIONS 12C(11Li, 9Li), E=800 MeV/nucleon; calculated 9Li longitudinal momentum distributions. Shell model plus di-neutron cluster model wave functions, Glauber theory.
doi: 10.1016/0375-9474(94)90720-X
1994SU02 Nucl.Phys. A567, 957 (1994) Y.Suzuki, T.Kido, Y.Ogawa, K.Yabana, D.Baye Fragmentation Cross Sections of He Isotopes and Neutron Correlations NUCLEAR REACTIONS 12C(6He, α), E=400 MeV/nucleon; calculated α-fragment momentum distribution. 9Be, C, 27Al, Cu, Pb(α, X), (6He, X), (8He, X), E=800 MeV/nucleon; calculated interaction, neutron removal σ. Glauber theory, projectile fragmentation.
doi: 10.1016/0375-9474(94)90336-0
1993SU04 Phys.Rev. C47, 1317 (1993) 11Li + p Elastic Scatterings in a Four-Body Model with the Eikonal Approximation NUCLEAR REACTIONS 11Li(p, p), E=62 MeV/nucleon; analyzed σ(θ); deduced target breakup, n-p interaction exchange force role. Four-body model, 11Li halo structure.
doi: 10.1103/PhysRevC.47.1317
1992OG02 Nucl.Phys. A543, 722 (1992) Glauber Model Analysis of the Fragmentation Reaction Cross Sections of 11Li NUCLEAR STRUCTURE 11Li, 9Be, 12C, 27Al, 63Cu, 208Pb; calculated point nucleon densities. Gaussian functions sum fitting. NUCLEAR REACTIONS 9Be, 12C, 27Al, Cu, Pb(11Li, X), E=800 MeV/nucleon; calculated reaction, two-neutron removal σ. Glauber model.
doi: 10.1016/0375-9474(92)90556-Y
1992YA02 Nucl.Phys. A539, 295 (1992) Reaction Mechanism of 11Li at Intermediate Energy NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; calculated elastic, breakup σ. Eikonal, coupled-discretized continuum channels models. 9Li, 12C(11Li, X), E ≈ 25-200 MeV/nucleon; calculated reaction σ(E).
doi: 10.1016/0375-9474(92)90272-L
1992YA04 Phys.Rev. C45, 2909 (1992) Break-Up Effect on the Elastic Scattering and the Optical Potential of 11Li NUCLEAR REACTIONS 58Ni(d, d), E=80 MeV; analyzed σ(θ). 12C(11Li, 11Li), E=60 MeV/nucleon; calculated σ(θ); deduced parameters, 11Li breakup role. Eikonal approximation, optical model with dynamic polarization potential.
doi: 10.1103/PhysRevC.45.2909
1977KO45 Ann.Nucl.Energy 4, 449 (1977) K.Kobayashi, Y.Fujita, Y.Ogawa Measurements of Neutron Total Cross Section Minima in Natural Iron and Silicon NUCLEAR REACTIONS Fe, Si(n, n'), (n, X), E ≈ 24, 147 keV; measured transmission, total neutron σ.
doi: 10.1016/0306-4549(77)90017-2
Back to query form |