NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.Kaki Found 14 matches. 2018CH27 Prog.Theor.Exp.Phys. 2018, 053D01 (2018) S.Chebotaryov, S.Sakaguchi, T.Uesaka, T.Akieda, Y.Ando, M.Assie, D.Beaumel, N.Chiga, M.Dozono, A.Galindo-Uribarri, B.Heffron, A.Hirayama, T.Isobe, K.Kaki, S.Kawase, W.Kim, T.Kobayashi, H.Kon, Y.Kondo, Y.Kubota, S.Leblond, H.Lee, T.Lokotko, Y.Maeda, Y.Matsuda, K.Miki, E.Milman, T.Motobayashi, T.Mukai, S.Nakai, T.Nakamura, A.Ni, T.Noro, S.Ota, H.Otsu, T.Ozaki, V.Panin, S.Park, A.Saito, H.Sakai, M.Sasano, H.Sato, K.Sekiguchi, Y.Shimizu, I.Stefan, L.Stuhl, M.Takaki, K.Taniue, K.Tateishi, S.Terashima, Y.Togano, T.Tomai, Y.Wada, T.Wakasa, T.Wakui, A.Watanabe, H.Yamada, Zh.Yang, M.Yasuda, J.Yasuda, K.Yoneda, J.Zenihiro Proton elastic scattering at 200 A MeV and high momentum transfers of 1.7-2.7 fm-1 as a probe of the nuclear matter density of 6He NUCLEAR REACTIONS 1H(6He, 6He), E=200 MeV/nucleon; measured reaction products; deduced σ(θ). Comparison with available data, relativistic impulse approximation model predictions.
doi: 10.1093/ptep/pty048
2017KA45 Prog.Theor.Exp.Phys. 2017, 093D01 (2017) Reaction cross sections of proton scattering from carbon isotopes (A=8-22) by means of the relativistic impulse approximation NUCLEAR STRUCTURE 8,9,10,11,12,13,14,15,16,17,18,19,20,21,22C; calculated proton and neutron distributions, rms radii. NUCLEAR REACTIONS 8,9,10,11,12,13,14,15,16,17,18,19,20,21,22C(p, p), E=71, 100, 200, 300, 425, 550, 650 MeV; calculated σ, σ(q). Comparison with available data.
doi: 10.1093/ptep/ptx116
2015KA09 Int.J.Mod.Phys. E24, 1550015 (2015) Neutron density distributions analyzed in terms of relativistic impulse approximation for nickel isotopes NUCLEAR REACTIONS 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82Ni(p, p), E=200-500 MeV; calculated root-mean-square radii, nuclear density distributions. Relativistic impulse approximation (RIA), and nuclear density distributions are provided by relativistic mean-field (RMF), comparison with available data.
doi: 10.1142/S0218301315500159
2014KA05 Phys.Rev. C 89, 014620 (2014);Erratum Phys.Rev. C 89, 059903 (2014) Relativistic impulse approximation analysis of elastic proton scattering from He isotopes NUCLEAR REACTIONS 4,6,8He(p, p), E=71 MeV; 4He(p, p), E=300, 500 MeV; 6He(p, p), E=0.7 GeV; analyzed differential cross sections σ(E, θ), analyzing power Ay(E, θ), Schrodinger equivalent optical potentials, rms radius of proton and neutron distributions based on based on RMF. Relativistic impulse approximation (RIA).
doi: 10.1103/PhysRevC.89.014620
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
2009KA21 Phys.Rev. C 79, 064609 (2009) Relativistic impulse approximation analysis of unstable calcium isotopes: 60-74Ca NUCLEAR REACTIONS 60,62,64,66,68,70,72,74Ca(p, p), E=100-500 MeV; calculated σ, σ(θ), analyzing power, spin rotation function, density distributions, occupation ratio of outer shells, rms radii of neutron and proton densities, depth of Dirac scalar and vector optical potentials using relativistic impulse approximation (RIA).
doi: 10.1103/PhysRevC.79.064609
2004KA54 Int.J.Mod.Phys. E13, 787 (2004) A model analysis of neutron distribution of 208Pb based on the relativistic impulse approximation of proton elastic scattering NUCLEAR REACTIONS 208Pb(p, p), E=300 MeV; analyzed σ(θ), Ay(θ), spin rotation function. 208Pb deduced neutron distribution. Relativistic impulse approximation, Woods-Saxon potential.
doi: 10.1142/S0218301304002466
2003KA36 Nucl.Phys. A724, 99 (2003) Neutron distribution of 208Pb in the relativistic impulse approximation of proton-elastic scattering NUCLEAR REACTIONS 208Pb(p, p), E=300, 400 MeV; analyzed σ(θ), Ay(θ). 208Pb deduced neutron distributions, radii. Relativistic impulse approximation, relativistic mean-field theory.
doi: 10.1016/S0375-9474(03)01481-7
2001KA60 Nucl.Phys. A696, 453 (2001) Relativistic Impulse Approach for Proton Elastic Scattering with 58Ni and 120Sn at Ep = 200, 300 and 400 MeV NUCLEAR REACTIONS 58Ni, 120Sn(p, p), E=200, 300, 400 MeV; calculated σ(θ); deduced role of Pauli effect, vacuum polarization effect. Relativistic impulse approach, comparisons with data.
doi: 10.1016/S0375-9474(01)01222-2
1999KA30 Int.J.Mod.Phys. E8, 167 (1999) Proton Elastic Scattering and Neutron Distribution of Unstable Nuclei NUCLEAR REACTIONS 40,60Ca(p, p), E=300 MeV; calculated σ(θ); deduced sensitivity to neutron density distribution. Relativistic impulse model.
doi: 10.1142/S0218301399000136
1999KO58 Nuovo Cim. 112A, 1431 (1999) H.Kozima, M.Ohta, M.Fujii, K.Arai, H.Kudoh, K.Kaki Analysis of Energy Spectrum of Neutrons in Cold-Fusion Experiments by the TNCF Model NUCLEAR REACTIONS 2H(d, n), E=low; analyzed neutron spectra. Trapped neutron catalyzed fusion.
1996KA18 Nucl.Phys. A601, 445 (1996) Relativistic Description of Exculusive Pion Production in Nucleon-Nucleus Scattering NUCLEAR REACTIONS 12C(p, nπ+), E=0.82 GeV; calculated coincidence σ. Relativistic impulse approximation.
doi: 10.1016/0375-9474(95)00495-5
1991KA22 Nucl.Phys. A531, 478 (1991) Relativistic Impulse Approximation for Neutron Elastic Scattering by a Spin-Zero Nucleus NUCLEAR REACTIONS 16O, 40Ca, 90Zr, 208Pb(polarized n, n), (polarized p, p), E=100, 200 MeV; calculated σ(θ), analyzing power vs θ, spin rotation parameter vs θ. Relativistic impulse approximation.
doi: 10.1016/0375-9474(91)90737-Q
1990KA29 Nucl.Phys. A516, 603 (1990) Multiple Scattering Contributions to the RIA Optical Potential NUCLEAR REACTIONS 40Ca(polarized p, p), E=100-800 MeV; calculated σ(θ), A(θ), spin rotation parameter vs θ. Relativistic impulse approximation, optical model, multiple scattering effects.
doi: 10.1016/0375-9474(90)90130-E
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