NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = M.Takashina Found 23 matches. 2021FU07 Phys.Rev. C 103, 044602 (2021) Relation between transition density and proton inelastic scattering by 12C target at Ep = 65 and 200 MeV NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=65, 200 MeV; analyzed experimental data for σ(Ε, θ) and analyzing power Ay(E, θ) for ground state and Hoyle state using microscopic coupled channel (MCC) method with potentials from folding a complex G-matrix effective nucleon-nucleon interaction, and transition density from modified Algebraic Cluster Model (ACM) wave function.
doi: 10.1103/PhysRevC.103.044602
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
2012FU04 Phys.Rev. C 85, 044607 (2012); Erratum Phys.Rev. C 85, 069901 (2012) T.Furumoto, W.Horiuchi, M.Takashina, Y.Yamamoto, Y.Sakuragi Global optical potential for nucleus-nucleus systems from 50 MeV/u to 400 MeV/u NUCLEAR REACTIONS 16O(16O, 16O), E=21.9, 30, 44, 70 MeV/nucleon; 12C(16O, 16O), E=20.6, 38, 93.9 MeV/nucleon; 12C(12C, 12C), E=25, 30, 84.7, 120.75, 135, 200 MeV/nucleon; 28Si, 40Ca, 208Pb(16O, 16O), E=93.9 MeV/nucleon; 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; 40Ca(14C, 14C), (16C, 16C), (18C, 18C), (20C, 20C), (22C, 22C)(18O, 18O), (20O, 20O), (22O, 22O), (24O, 24O), E=100 MeV/nucleon; 40Ca(30Ne, 30Ne), (70Ca, 70Ca), E=100, 200, 300, 400 MeV/nucleon; calculated folding-model potentials (FMPs) elastic scattering cross sections as a function of momentum transfer. New global optical potential (GOP) in 50-400 MeV/nucleon range from microscopic CEG07 folding model with Sao Paulo density. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044607
2011KI11 Int.J.Mod.Phys. E20, 843 (2011) Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda Two-neutron correlations in halo nuclei via Coulomb breakup reactions
doi: 10.1142/S0218301311018812
2011KI40 Phys.Rev. C 84, 064610 (2011) Y.Kikuchi, N.Kurihara, A.Wano, K.Kato, T.Myo, M.Takashina Three-body model analysis of α+d$ elastic scattering and the 2H(α, γ)6Li reaction in complex-scaled solutions of the Lippmann-Schwinger equation NUCLEAR REACTIONS 2H(α, α), E(cm)<6 MeV; calculated elastic phase shifts, deuteron breakup effect on resonances. 2H(α, γ)6Li, E<6 MeV; calculated E2 transition strengths, σ(E) for radiative capture. 2H(α, γ)6Li, E<6 MeV; calculated σ(E) for photodisintegration. Complex-scaled solutions of the Lippmann-Schwinger equation (CSLS) for α+d scattering. Comparison with experimental data. NUCLEAR STRUCTURE 6Li; calculated levels, widths, ∼, π, rms matter and charge radii, quadrupole moment, considering α+p+n three-body structure of 6Li, and using Lippmann-Schwinger equation. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064610
2010AO01 Phys.Lett. B 692, 302 (2010) N.Aoi, S.Kanno, S.Takeuchi, H.Suzuki, D.Bazin, M.D.Bowen, C.M.Campbell, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, H.Iwasaki, T.Kubo, K.Kurita, T.Motobayashi, W.F.Mueller, T.Nakamura, H.Sakurai, M.Takashina, J.R.Terry, K.Yoneda, H.Zwahlen Enhanced collectivity in 74Ni NUCLEAR REACTIONS 1H(74Ni, 74Ni'), E=81 MeV/nucleon; measured Eγ, Iγ; 74Ni; deduced J, π, level energy, σ, deformation length and parameter.
doi: 10.1016/j.physletb.2010.07.052
2010HO08 Phys.Rev. C 81, 061602 (2010) K.Horii, M.Takashina, T.Furumoto, Y.Sakuragi, H.Toki Elastic scattering of 8B from 12C with internal three-cluster structure of 8B NUCLEAR REACTIONS 12C(8B, 8B), E=95 MeV; calculated σ, σ(θ) using adiabatic recoil and cluster folding calculations. 12C, 14N(7Be, 7Be), E=87 MeV; calculated σ(θ). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.061602
2010KI06 Phys.Rev. C 81, 044308 (2010) Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda Two-neutron correlations in 6He in a Coulomb breakup reaction NUCLEAR STRUCTURE 6He; calculated two-neutron density distribution, coulomb breakup cross-section of halo nucleus via α+n+n channel, E1 strength distributions, invariant mass spectra using Complex Scaling Lippmann-Schwinger method. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044308
2010TA06 Phys.Rev. C 81, 047605 (2010) M.Takashina, T.Furumoto, Y.Sakuragi 16O+16O inelastic scattering studied by a complex G-matrix interaction NUCLEAR REACTIONS 16O(16O, 16O'), E=1120 MeV; analyzed σ(θ) using microscopic coupled-channel (CC) method with complex G-matrix interaction.
doi: 10.1103/PhysRevC.81.047605
2009EL03 Phys.Rev. C 79, 011302 (2009) Z.Elekes, Zs.Dombradi, T.Aiba, N.Aoi, H.Baba, D.Bemmerer, B.A.Brown, T.Furumoto, Zs.Fulop, N.Iwasa, A.Kiss, T.Kobayashi, Y.Kondo, T.Motobayashi, T.Nakabayashi, T.Nannichi, Y.Sakuragi, H.Sakurai, D.Sohler, M.Takashina, S.Takeuchi, K.Tanaka, Y.Togano, K.Yamada, M.Yamaguchi, K.Yoneda Persistent decoupling of valence neutrons toward the dripline: Study of 20C by γ spectroscopy NUCLEAR REACTIONS 208Pb(20C, 20C'), E=37.6 MeV/nucleon; 1H(20C, 20C'), E=41.4 MeV/nucleon; measured Eγ, Iγ. 20C; deduced levels, J, π, charge and neutron transition probabilities, B(E2). Comparison with shell model calculations.
doi: 10.1103/PhysRevC.79.011302
2009TA08 Phys.Rev. C 79, 054319 (2009) S.Takeuchi, N.Aoi, T.Motobayashi, S.Ota, E.Takeshita, H.Suzuki, H.Baba, T.Fukui, Y.Hashimoto, K.Ieki, N.Imai, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, T.Minemura, T.Nakabayashi, T.Nakamura, T.Okumura, T.K.Onishi, H.Sakurai, S.Shimoura, R.Sugou, D.Suzuki, M.K.Suzuki, M.Takashina, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada Low-lying states in 32Mg studied by proton inelastic scattering NUCLEAR REACTIONS 1H(32Mg, 32Mg'), E=46.5 MeV/nucleon; measured Eγ, Iγ, scattered particle spectra, σ, σ(θ). 32Mg; deduced levels, J, π, deformation lengths, rms radii.Coupled-channel analysis of angular distribution cross sections. 24,26,28,30,32,34Mg; level systematics.
doi: 10.1103/PhysRevC.79.054319
2009TA18 Phys.Rev. C 80, 014605 (2009) Multistep effect in 16O+16O inelastic scattering NUCLEAR REACTIONS 16O(16O, 16O'), E=350, 1120 MeV; analyzed σ(θ) for first 2+ and 3- states using microscopic coupled-channel calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.014605
2008KI22 Int.J.Mod.Phys. E17, 2368 (2008) Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda Analysis on two-neutron correlation through Dalitz plot of Coulomb breakup reaction for 6He NUCLEAR STRUCTURE 6He; calculated the energy and Dalitz distributions of E1 transition strength; deduced dominance of sequential decay process. Lippmann-Schwinger equation.
doi: 10.1142/S021830130801163X
2008TA02 Phys.Rev. C 77, 014604 (2008) Inelastic proton scattering and neutron quadrupole transitions of 12Be NUCLEAR REACTIONS p(10Be, 10Be), (10Be, 10Be'), E=59.2 MeV/nucleon; p(12Be, 12Be), (12Be, 12Be'), E=55 MeV/nucleon; calculated density distributions, radii, transition strengths, single-particle transition densities, σ(θ). 10,12Be; deduced levels, J, π.12C(p, p), E=50 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.77.014604
2008TA21 Phys.Rev. C 78, 014602 (2008) Interpretation of a diffraction phenomenon observed in the angular distribution of α inelastic scattering on 12C exciting the 0+2 state NUCLEAR REACTIONS 12C(α, α'), E=240 MeV; calculated σ(θ). Eikonal wave Born approximation.
doi: 10.1103/PhysRevC.78.014602
2007WA32 Phys.Lett. B 653, 173 (2007) T.Wakasa, E.Ihara, K.Fujita, Y.Funaki, K.Hatanaka, H.Horiuchi, M.Itoh, J.Kamiya, G.Ropke, H.Sakaguchi, N.Sakamoto, Y.Sakemi, P.Schuck, Y.Shimizu, M.Takashina, S.Terashima, A.Tohsaki, M.Uchida, H.P.Yoshida, M.Yosoi New candidate for an alpha cluster condensed state in 16O(α, α') at 400 MeV NUCLEAR REACTIONS 16O(α, α'), E=400 MeV; analyzed elastic and inelastic σ(θ). Comparison with model calculations. Evidence for cluster structure.
doi: 10.1016/j.physletb.2007.08.016
2006TA27 Phys.Rev. C 74, 054606 (2006) α + 12C inelastic angular distribution and nuclear size of 12C(O+2) NUCLEAR REACTIONS 12C(α, α'), E=139-240 MeV; analyzed σ(E, θ), sensitivity to excited state radius.
doi: 10.1103/PhysRevC.74.054606
2005TA12 Phys.Rev. C 71, 054602 (2005) M.Takashina, Y.Kanada-En'yo, Y.Sakuragi 16C inelastic scattering studied with the microscopic coupled-channels method NUCLEAR REACTIONS 208Pb(16C, 16C'), E=52.7 MeV/nucleon; calculated σ(θ). Microscopic coupled-channels method, comparison with data.
doi: 10.1103/PhysRevC.71.054602
2005TA34 Eur.Phys.J. A 25, Supplement 1, 273 (2005) M.Takashina, Y.Sakuragi, Y.Iseri Effect of halo structure on 11Be + 12C elastic scattering NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ). Continuum-discretized coupled-channels method, comparison with data.
doi: 10.1140/epjad/i2005-06-077-1
2004TA21 Nucl.Phys. A738, 352 (2004) M.Takashina, M.Ito, Y.Kubo, S.Okabe, Y.Sakuragi 12C + 12C → 8Beg.s. + 16Og.s. resonance reactions and multi-cluster states of highly excited 24Mg nucleus NUCLEAR REACTIONS 12C(12C, 8Be), E(cm)=20-37 MeV; calculated σ(θ), excitation function; deduced resonance structure. 24Mg deduced molecular rotational band. Coupled channels Born approximation.
doi: 10.1016/j.nuclphysa.2004.04.060
2003TA01 Phys.Rev. C 67, 014609 (2003) M.Takashina, M.Ito, Y.Kudo, S.Okabe, Y.Sakuragi 12C+12C → 8Beg.s.+16Og.s. resonance reaction around Ec.m. = 32.5 MeV NUCLEAR REACTIONS 12C(12C, 8Be), E(cm) ≈ 27-36 MeV; calculated σ(θ), excitation function; deduced resonance features. Coupled-channels Born approximation, comparison with data.
doi: 10.1103/PhysRevC.67.014609
2003TA04 Phys.Rev. C 67, 037601 (2003) M.Takashina, S.Takagi, Y.Sakuragi, Y.Iseri Continuum-discretized coupled-channels study of the 11Be → 10Be+n breakup effect on 11Be elastic scattering NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), contribution of projectile breakup effect; deduced dynamical polarization potential. Continuum-discretized coupled-channels approach, comparison with data.
doi: 10.1103/PhysRevC.67.037601
2002TA31 Prog.Theor.Phys.(Kyoto), Suppl. 146, 630 (2002) S.Takagi, M.Takashina, Y.Sakuragi, Y.Iseri A CDCC Study of 11Be → 10Be + n Breakup Effect on the 11Be Elastic Scattering NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), breakup channel contribution. Continuum-discretized coupled-channels method, comparison with data.
doi: 10.1143/PTPS.146.630
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