NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Kaneko Found 46 matches. 2020KA40 Nucl.Instrum.Methods Phys.Res. B478, 218 (2020) T.Kaneko, R.Usami, H.Morioka, Y.Saitoh, A.Chiba, K.Narumi Electron-loss and destruction processes in collision of MeV/atom carbon cluster ions with rare gases NUCLEAR REACTIONS He, Ne(C, X), E=2.5 MeV; calculated σ using the time-dependent quantum theory, assuming binary collision treatment and independent electron model.
doi: 10.1016/j.nimb.2020.06.031
2006TS04 Comput.Phys.Commun. 175, 665 (2006) S.Tsuno, T.Kaneko, Y.Kurihara, S.Odaka, K.Kato GR@PPA 2.7 event generator for pp/p(p-bar) collisions NUCLEAR REACTIONS 1H(p, X), (p-bar, X), E=high; calculated multi-jet production σ.
doi: 10.1016/j.cpc.2006.07.011
2004NA10 Nucl.Phys. A734, 124 (2004) Y.Nagame, H.Haba, K.Tsukada, M.Asai, A.Toyoshima, S.Goto, K.Akiyama, T.Kaneko, M.Sakama, M.Hirata, T.Yaita, I.Nishinaka, S.Ichikawa, H.Nakahara Chemical studies of the heaviest elements
doi: 10.1016/j.nuclphysa.2004.01.021
2004TS12 Phys.Rev. D 70, 111501 (2004) N.Tsutsui, S.Aoki, M.Fukugita, S.Hashimoto, K.-I.Ishikawa, N.Ishizuka, Y.Iwasaki, K.Kanaya, T.Kaneko, Y.Kuramashi, M.Okawa, T.Onogi, Y.Taniguchi, A.Ukawa, T.Yoshie, and the CP-PACS and JLQCD Collaborations Lattice QCD calculation of the proton decay matrix element in the continuum limit NUCLEAR STRUCTURE 1H; calculated proton decay matrix element, scaling violation effect. Quenched lattice QCD.
doi: 10.1103/PhysRevD.70.111501
2003AS01 Eur.Phys.J. A 16, 17 (2003) M.Asai, K.Tsukada, S.Ichikawa, M.Sakama, H.Haba, Y.Nagame, I.Nishinaka, K.Akiyama, A.Toyoshima, T.Kaneko, Y.Oura, Y.Kojima, M.Shibata Identification of the new isotope 241Bk NUCLEAR REACTIONS 239Pu(6Li, 4n), E=34-42 MeV; measured prompt and delayed Eγ, Iγ, (X-ray)γ-, (recoil)γ-coin; deduced evidence for 241Bk. Isotope separator. RADIOACTIVITY 241Bk(EC) [from 239Pu(6Li, 4n)]; measured Eγ, Iγ, (X-ray)γ-coin, T1/2; deduced ground-state configuration.
doi: 10.1140/epja/i2002-10112-y
2002KA42 Prog.Theor.Phys.(Kyoto) 107, 833 (2002) Resonating-Group Calculations with New Cluster Wave Function for p + 3, 4He Elastic Scattering NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies, radii. Cluster wave functions, resonating group method, comparison with data. NUCLEAR REACTIONS 3,4He(p, p), E ≈ 3-12 MeV; calculated σ(θ), polarization. Cluster wave functions, resonating group method, comparison with data.
doi: 10.1143/PTP.107.833
2000KA49 Few-Body Systems 29, 143 (2000) Study of 3He + Nucleus Scattering with a Simplified Resonating-Group Method NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr, 116,120Sn, 208Pb(3He, 3He), E=70-130 MeV; calculated σ(θ). Resonating-group method, comparisons with data.
doi: 10.1007/s006010070014
1999KA29 Prog.Theor.Phys.(Kyoto) 101, 591 (1999) Study of α + Nucleus Scattering with a Simplified Resonating-Group Method NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr, 124Sn, 208Pb(α, α), E ≈ 100, 140 MeV; calculated σ(θ). Simplified resonating-group method, comparison with data.
doi: 10.1143/PTP.101.591
1998KA07 Int.J.Mod.Phys. E7, 1 (1998) Simplified Resonating-Group Method for Light-Ion Scattering
doi: 10.1142/S0218301398000026
1998OR02 Nucl.Instrum.Methods Phys.Res. A402, 402 (1998) S.Oryu, E.Uzu, H.Sunahara, T.Yamada, G.Tabaru, T.Hino, T.Kaneko 3He(d, p)4He Reaction Calculation with Three-Body Faddeev Equations NUCLEAR REACTIONS 3He(d, p), (polarized d, p), E=270 MeV; calculated σ(θ). Three-body Fadeev equations, microscopic Pauli correct method, resonating group method. NUCLEAR STRUCTURE 5Li; calculated levels, J, π. Three-body Fadeev equations.
doi: 10.1016/S0168-9002(97)00880-2
1997KA06 Nucl.Phys. A612, 204 (1997) Scattering of Deuterons by Nuclei with Breakup Effects NUCLEAR REACTIONS 28Si, 40Ca(d, d), E=29.2 MeV; 58Ni(d, d), E=79.5 MeV; 120Sn, 208Pb(d, d), E=85 MeV; analyzed σ(θ). Microscopic resonating group method, direct deuteron breakup included.
doi: 10.1016/S0375-9474(96)00336-3
1996KA10 Nucl.Phys. A599, 545 (1996) Analysis of Deuteron + Nucleus Scattering Data with a Simplified Resonating-Group Method NUCLEAR REACTIONS 140Ce, 208Pb, 28Si, 58Ni, 90Zr(polarized d, d), E=52 MeV; 58Ni(polarized d, d), E=79.5 MeV; analyzed σ(θ), iT11(θ). 120Sn, 208Pb(d, d), E=85, 58.7 MeV; analyzed σ(θ); 40Ca(d, d), E=40, 60, 80 MeV; calculated σ(θ). Simplified resonating group method.
doi: 10.1016/0375-9474(95)00466-1
1995GO33 Hyperfine Interactions 96, 63 (1995) T.Goto, S.Koyama, T.Kaneko, S.Abe Effects of Nitrogen and Vanadium on the 57Fe Hyperfine Field of RFe(12-x)V(x)N(y)(R = Y, Nd) NUCLEAR REACTIONS 57Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced nitrogen, vanadium atoms effect on 57Fe hyperfine fields at different crystallographic sites. Ternary RFe(12-x)V(x)N(y)(R=Y, Nd).
doi: 10.1007/BF02066272
1995KA28 Nucl.Phys. A591, 209 (1995) Approximate Treatment of the Deuteron + Nucleus Interaction in the Resonating-Group Formulation NUCLEAR REACTIONS 16O(d, d), E=30 MeV; analyzed σ(θ). 40Ca(polarized d, d), E=49.52 MeV; analyzed σ(θ), iT11(θ). Microscopic resonating group method.
doi: 10.1016/0375-9474(95)00181-Y
1995KA60 Prog.Theor.Phys.(Kyoto) 94, 1061 (1995) Scattering and Reaction Cross Sections in the p + α System with the Multiconfiguration Resonating-Group Method NUCLEAR REACTIONS 4He(p, p), E=24.8-68 MeV; calculated reaction σ vs E, σ(θ). 4He(p, d), E=24.8-68 MeV; 4He(p, t), E=39.6 MeV; calculated σ(θ). Multi-configuration resonating group method.
doi: 10.1143/PTP.94.1061
1995KA65 Few-Body Systems 18, 1 (1995) Resonating-Group Study of Three-Nucleon Bound State and p + d Scattering NUCLEAR REACTIONS 2H(p, p), E ≤ 32 MeV; calculated phase shifts vs E, σ(θ), reaction σ(E). Resonating group method, multi-configurations.
doi: 10.1007/s006010050001
1993KA45 Prog.Theor.Phys.(Kyoto) 90, 1287 (1993) Analysis of Proton-Nucleus Scattering Data with a Simplified Resonating-Group Method NUCLEAR REACTIONS 12C, 40Ca, 58Ni, 90Zr, 208Pb(polarized p, p), E=16-65 MeV; calculated σ(θ), analyzing power vs θ. Nonlocal optical model, simplified resonating group method.
doi: 10.1143/ptp/90.6.1287
1993KA47 Prog.Theor.Phys.(Kyoto) 89, 1103 (1993) Microscopic Study of Proton-4He Scattering with Complex Effective N-N Interaction NUCLEAR REACTIONS 4He(p, p), (polarized p, p), E=51.9-117.6 MeV; analyzed σ(θ), analyzing power vs θ, reaction σ. Resonating group method, complex effective nucleon-nucleon potential.
doi: 10.1143/ptp/89.5.1103
1993ON04 Hyperfine Interactions 78, 451 (1993) H.Onodera, T.Kitai, M.Ohashi, Y.Yamaguchi, T.Kaneko 161Dy Mossbauer Study on Magnetic Properties in DyZn2 Intermetallics NUCLEAR REACTIONS 161Dy(γ, γ), E=74.6 keV; measured Mossbauer spectra.
doi: 10.1007/BF00568173
1992KA10 Phys.Rev. C45, 2409 (1992) General Features of Nucleon-Nucleus Interaction in the Resonating-Group Formulation NUCLEAR REACTIONS 40Ca(n, n), E=60 MeV; calculated σ(θ). Resonating group method, nonlocal K model.
doi: 10.1103/PhysRevC.45.2409
1992KA21 Phys.Rev. C46, 298 (1992) Analysis of Neutron + Nucleus Scattering Data with Nonlocal Optical Potentials Based on the Resonating-Group Formulation NUCLEAR REACTIONS 12C, 16O, 28Si, 32S, 40Ca(n, n), (polarized n, n), E=13-40 MeV; analyzed σ(θ), analyzing power vs θ. Nonlocal optical model, resonating group formulation.
doi: 10.1103/PhysRevC.46.298
1992KA34 Nucl.Phys. A548, 189 (1992) Resonating-Group Study of the Parameters in the Local Nucleon-Nucleus Optical-Model Potential NUCLEAR REACTIONS 120Sn(polarized n, n), E=13.88 MeV; 120Sn(polarized p, p), E=39.67 MeV; calculated σ(θ), analyzing power vs θ. 120Sn(n, n), E=20 MeV; 48Ca(p, p), E=40 MeV; calculated σ(θ). Local optical model, resonating group study.
doi: 10.1016/0375-9474(92)90008-8
1992KA41 Phys.Lett. 296B, 285 (1992) Approximate Resonating-Group Calculations with Woods-Saxon Target-Nucleus Wave Functions NUCLEAR REACTIONS 40Ca(n, n), (polarized n, n), E=20, 40, 13.56 MeV; 16O(n, n), (polarized n, n), E=21.65 MeV; calculated σ(θ), analyzing power vs θ. Approximate resonating group calculations.
doi: 10.1016/0370-2693(92)91321-Y
1991KA01 Phys.Rev. C43, 371 (1991) Reaction Cross Sections in the Four-Nucleon System with the Multiconfiguration Resonating-Group Method NUCLEAR REACTIONS 2H(d, X), E(cm) ≤ 14 MeV; calculated phase shifts, reaction σ vs E. 3H(t, X), E(cm) ≤ 18 MeV; calculated reaction σ vs E. Multi-configuration resonating group method.
doi: 10.1103/PhysRevC.43.371
1991KA19 Phys.Rev. C44, 1588 (1991) Approximate Treatment of the Nucleon-Nucleus Interaction in the Resonating-Group Formulation NUCLEAR REACTIONS 4He(n, n), E ≤ 50 MeV; 40Ca, 16O(n, n), E ≤ 30 MeV; calculated phase shifts vs E, σ(θ). 40Ca(n, n), E=4.2 MeV; calculated σ(θ). 40Ca(n, n), E=10, 30 MeV; calculated P(θ). Resonating group model.
doi: 10.1103/PhysRevC.44.1588
1991KA38 Few-Body Systems 11, 121 (1991) Multi-Configuration Resonating-Group Study of the Three-Nucleon System NUCLEAR REACTIONS, ICPND 2H(p, p), E ≤ 24 MeV; calculated phase shifts, reaction σ(E), σ(θ). Multi-configuration resonating group.
doi: 10.1007/BF01318557
1990MO07 Nucl.Phys. A510, 173 (1990) C.B.Moon, J.C.Kim, J.U.Kwon, B.N.Sung, K.Furuno, T.Komatsubara, T.Hosoda, T.Kaneko, S.C.Jeong, I.Kurniawan, T.Aoki The Band Structure and Triaxial Shape in 118Xe NUCLEAR REACTIONS 92Mo(29Si, n2p), E=110 MeV; measured Eγ, Iγ, Iγ(θ), γγ-coin. 118Xe deduced levels, J, π, band structure. Cranked shell model calculation. Enriched target, Ge, Ge(Li) detectors.
doi: 10.1016/0375-9474(90)90294-V
1989KA39 Nucl.Phys. A504, 529 (1989) Multi-Configuration Resonating-Group Study of the Five-Nucleon System NUCLEAR REACTIONS, ICPND 3He(d, d), E=10 MeV; 4He(p, p), E=28.08 MeV; calculated phase shifts, total reaction σ(E). Multi-configuration resonating group study.
doi: 10.1016/0375-9474(89)90556-3
1988KA25 Phys.Rev. C38, 2013 (1988) Convergence Features in the Pseudostate Theory of the d + α System NUCLEAR REACTIONS, ICPND 4He(d, d), E=2-40 MeV; calculated phase shift, σ(θ), σ(E). Pseudostate method, resonating group formulation.
doi: 10.1103/PhysRevC.38.2013
1988MO28 Z.Phys. A331, 111 (1988) C.B.Moon, J.C.Kim, K.Furuno, T.Komatsubara, T.Hosoda, T.Kaneko, S.C.Jeong, I.Kurniawan, T.Aoki Band Structure of 118Xe NUCLEAR REACTIONS 92Mo(29Si, n2p), E=110 MeV; measured γγ-coin, γ(θ). 118Xe deduced levels, J, π, band structure.
1987KA22 Phys.Lett. 192B, 259 (1987) T.Kaneko, M.Shirata, H.Kanada, Y.C.Tang Neutron and Proton Form Factors of 7Li and 7Be NUCLEAR STRUCTURE 7Li, 7Be; calculated point proton, neutron form factors, rms radii, spectroscopic quadrupole moments. Multi-configuration resonating group.
doi: 10.1016/0370-2693(87)90101-8
1987KO35 J.Phys.Soc.Jpn. 56, 2263 (1987) Y.Kohori, T.Kohara, H.Shibai, Y.Oda, T.Kaneko, Y.Kitaoka, K.Asayama 195Pt Knight Shift in the Heavy Fermion Superconductor UPt3 NUCLEAR MOMENTS 195Pt; measured NMR; deduced Knight shift in UPt3.
doi: 10.1143/JPSJ.56.2263
1986KA21 Phys.Rev. C34, 22 (1986) Microscopic Theory of the 4He System with Multichannel Resonating-Group Method NUCLEAR REACTIONS 2H(d, d), E(cm)=2.23-6.95 MeV; 3H(p, p), E(cm)=3.11-14.61 MeV; 3H(p, n), E=7.1, 10.2 MeV; 3H(p, d), E=10.2 MeV; calculated σ(θ). 3H(polarized p, p), E=3.11-10.2 MeV; 3He(polarized n, n), E=6, 12.83 MeV; calculated polarization vs θ. Multi-channel resonating group method.
doi: 10.1103/PhysRevC.34.22
1986KA28 Nucl.Phys. A457, 93 (1986) H.Kanada, T.Kaneko, P.N.Shen, Y.C.Tang Characteristic Features of Specific Distortion in Light Nuclear Systems NUCLEAR REACTIONS 3H(d, d), E ≈ 0-18 MeV; calculated phase shifts vs E. Deuteron cluster in (3/2) channel spin state.
doi: 10.1016/0375-9474(86)90521-X
1986KA30 Phys.Rev. C34, 771 (1986) T.Kaneko, M.Shirata, H.Kanada, Y.C.Tang Microscopic Theory of the 3H + α System with the Multichannel Resonating-Group Method NUCLEAR STRUCTURE 7Li; calculated ground state energy, rms radius, spectroscopic quadrupole moment. Multi-channel resonating group method, t+α cluster. NUCLEAR REACTIONS 3H(α, α), E ≤ 15 MeV; calculated σ(θ), polarization vs θ, phase shifts; deduced distortion effects role. Multichannel resonating group method.
doi: 10.1103/PhysRevC.34.771
1986KO35 J.Phys.Soc.Jpn. 55, 3819 (1986) Deuteron Distortion Effects in the (d, d) Scattering and (d, p) Reaction NUCLEAR REACTIONS 28Si(d, d), (d, p), E=18 MeV; calculated σ(θ); deduced deuteron distortion effects. DWBA.
doi: 10.1143/JPSJ.55.3819
1986SH12 Phys.Rev. C33, 1214 (1986) P.N.Shen, Y.C.Tang, H.Kanada, T.Kaneko Pseudostate Calculations in n + t and p + 3He Systems NUCLEAR REACTIONS 3H(n, n), E ≈ 0-36 MeV; calculated phase shifts. 3He(p, p), E=22.5-35.625 MeV; calculated σ(θ); deduced specific distortion. Resonating group method.
doi: 10.1103/PhysRevC.33.1214
1985KA20 Nucl.Phys. A444, 209 (1985) H.Kanada, T.Kaneko, S.Saito, Y.C.Tang Microscopic Study of the d + α Scattering System with the Multi-Channel Resonating-Group Method NUCLEAR REACTIONS 4He(d, d), E ≈ 0-30 MeV; calculated phase shifts vs E. 4He(polarized d, d), E=1.957-37.33 MeV; calculated σ(θ), vector, tensor polarizations vs θ. Multi-channel resonating group method, α+d cluster, distortion effects.
doi: 10.1016/0375-9474(85)90347-1
1982KA11 Nucl.Phys. A380, 87 (1982) Specific Distortion Effects in 3H + α and 3He + α Systems NUCLEAR STRUCTURE 3H, 3He, 7Li; calculated charge form factors. Resonating group method. NUCLEAR REACTIONS 3H, 3He(α, α), E=0-14 MeV; calculated phase shifts. 4He(t, t), E=1.22, 1.7 MeV; 4He(3He, 3He), E=1.41, 2.06 MeV; calculated σ(θ). 4He(t, t), E=6.17 MeV; calculated σ(θ), P(θ). Resonating group method.
doi: 10.1016/0375-9474(82)90584-X
1982KA24 Nucl.Phys. A389, 285 (1982) Specific Distortion Effects in the d + α System and Charge Form Factor of 6Li NUCLEAR REACTIONS 4He(d, d), (polarized d, d), E=3-25 MeV; calculated phase shifts, σ(θ), vector, tensor polarization; deduced large deuteron cluster compressibility. Resonating group method. NUCLEAR STRUCTURE 6Li; calculated charge form factor, rms charge radius; deduced large deuteron cluster compressibility role. Resonating group method.
doi: 10.1016/0375-9474(82)90520-6
1980KA15 Prog.Theor.Phys.(Kyoto) 63, 842 (1980) H.Kanada, T.Kaneko, H.Nishioka, S.Saito Microscopic Study of d-4He Scattering by RGM with Distortion Effect, phase shifts; deduced importance of deuteron distortion. Resonating group method, realistic effective nuclear interactions.
doi: 10.1143/PTP.63.842
1980NI07 Prog.Theor.Phys.(Kyoto) 63, 438 (1980) H.Nishioka, S.Saito, H.Kanada, T.Kaneko Study of Distortion Effects in the Elastic d-4He Scattering by Orthogonality Condition Model NUCLEAR REACTIONS 4He(d, d), E(cm)=2-16 MeV; calculated phase shifts. Variational method, deuteron distortion effect, orthogonality condition.
doi: 10.1143/PTP.63.438
1979KA17 Prog.Theor.Phys. 61, 1327 (1979) H.Kanada, T.Kaneko, S.Nagata, M.Nomoto Microscopic Study of Nucleon-4He Scattering and Effective Nuclear Potentials NUCLEAR REACTIONS 4He(n, n), E(cm) ≈ 0-15 MeV; calculated s-, p-wave phase shifts, σ(E). 4He(p, p), Ep=0-80 MeV; calculated s-, p-wave phase shifts, σ(θ), P(θ). Single-channel resonating group method, realistic effective two-body nuclear potentials.
doi: 10.1143/PTP.61.1327
1974MI14 Nucl.Phys. A230, 98 (1974) K.Miyano, M.Sekikawa, T.Kaneko, M.Nomoto Reactions on 209Bi Induced by Intermediate Energy Protons and the Effect of Direct Reactions NUCLEAR REACTIONS 209Bi(p, 3n), (p, 4n), (p, p3n), E=18-52 MeV; measured σ(E), mean recoil ion ranges.
doi: 10.1016/0375-9474(74)90532-6
1973KA46 Progr.Theor.Phys. 50, 1765 (1973) Spin-Orbit Interaction in Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 14N(14N, 14N), E=17.7 MeV; 14N(16O, 16O), E=18.3 MeV; calculated σ(θ).
doi: 10.1143/PTP.50.1765
1970KA41 Progr.Theor.Phys. 44, 292 (1970) Form Factor of Heavy Ion Transfer Reaction at Low Energy Region NUCLEAR REACTIONS 14N(14N, 13N), E=8 MeV cms; calculated σ(θ), form factor.
doi: 10.1143/PTP.44.292
Back to query form |