NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.Kamimura Found 87 matches. 2023KA09 Phys.Rev. C 107, 034607 (2023) M.Kamimura, Y.Kino, T.Yamashita Comprehensive study of muon-catalyzed nuclear reaction processes in the dtμ molecule NUCLEAR REACTIONS 2H(t, nα), E(cm)=1-300 keV; calculated S(E) factors using three different sets of nuclear interactions. 4He(n, X), E=21.5-22.6 MeV; calculated total σ(E) using one set of nuclear interactions, and compared with experimental data; calculated muon-catalyzed fusion in a dtμ-molecule yielding reaction products of 4He+n+μ+17.6 MeV and 4Heμ+n+17.6 MeV; deduced fusion rate, momentum and energy spectra of emitted muon and 4Heμ-sticking probability using coupled-channel method and T-matrix method.
doi: 10.1103/PhysRevC.107.034607
2023KA17 Prog.Theor.Exp.Phys. 2023, 071D01 (2023) Derivation of transition density from the observed 4He(e, e')4He(0+2) form factor raising the α-particle monopole puzzle NUCLEAR REACTIONS 4He(e-, e-'), E not given; analyzed data. 4He; deduced energy levels, J, π, transition density from the monopole transition form factor of the electron-scattering excitation of the 0+2 state.
doi: 10.1093/ptep/ptad090
2017CA16 Few-Body Systems 58, 67 (2017) J.Carbonell, R.Lazauskas, E.Hiyama, M.Kamimura On the Possible Existence of Four Neutron Resonances NUCLEAR REACTIONS 3He(n, n), E=0.03-10 MeV;3He(n, x), E not given; calculated possible tetraneutron resonance trajectory for 0+ state; deduced resonance, σ, resonance energy and width vs other parameters, higher 4n resonances, tetraneutron production response function via double charge exchange; deduced parameters.
doi: 10.1007/s00601-017-1219-0
2016HI03 Phys.Rev. C 93, 044004 (2016) E.Hiyama, R.Lazauskas, J.Carbonell, M.Kamimura Possibility of generating a 4-neutron resonance with a T=3/2 isospin 3-neutron force NUCLEAR STRUCTURE 4n; calculated narrow resonant states of tetraneutron for Jπ=0+, 2+ and 2-. 4H, 4He, 4Li; calculated energies of the lowest T=1, Jπ=2- states. 3n; calculated resonance trajectories for Jπ=3/2-, 1/2- and 1/2+ states. Complex scaling method (CSM) for resonance positions and widths. Gaussian expansion method used to solve Schrodinger equation and Lagrange-mesh technique to solve Faddeev-Yakubovsky (FY) equation. Comparison with recent experimental data from RIKEN.
doi: 10.1103/PhysRevC.93.044004
2015HI04 Phys.Rev. C 91, 054316 (2015) E.Hiyama, M.Isaka, M.Kamimura, T.Myo, T.Motoba Resonant states of the neutron-rich Λ hypernucleus 7ΛHe NUCLEAR STRUCTURE 6He; calculated levels, J, π, widths. 7He; calculated levels, J, π, widths of hypernucleus in the framework of α+Λ+n+n four-body cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.054316
2013HI03 Nucl.Phys. A908, 29 (2013) E.Hiyama, S.Ohnishi, M.Kamimura, Y.Yamamoto Four-body structure of neutron-rich hypernucleus 6ΛH NUCLEAR STRUCTURE 6H; calculated λ hypernucleus 6H radial density distribution using tnnΛ four-body cluster model; deduced 6ΛH ground state as a resonant state.
doi: 10.1016/j.nuclphysa.2013.04.001
2013HI07 Few-Body Systems 54, 737 (2013) Four-Body Structure of Λ Hypernuclei and 4He Tetramer System NUCLEAR STRUCTURE 4H, 4He; calculated hypernuclei ground and excited states parameters, energy levels, J, π. Gaussian expansion method.
doi: 10.1007/s00601-012-0471-6
2013OH06 Prog.Theor.Exp.Phys. 2013, 073D02 (2013) S.-I.Ohtsubo, Y.Fukushima, M.Kamimura, E.Hiyama Complex-scaling calculation of three-body resonances using complex-range Gaussian basis functions: Application to 3α resonances in 12C NUCLEAR STRUCTURE 12C; calculated three-body α resonances, level energies, J, π. Comparison with available data.
doi: 10.1093/ptep/ptt048
2011OG12 J.Phys.:Conf.Ser. 312, 082008 (2011) K.Ogata, T.Matsumoto, S.Hashimoto, K.Minomo, T.Egami, Y.Iseri, M.Kohno, S.Chiba, C.A.Bertulani, Y.R.Shimizu, M.Kamimura, M.Yahiro Status of breakup reaction theory NUCLEAR REACTIONS 7Li(d, γ), (d, n), (d, p), E=10-50 MeV; calculated σ. 90Zr(p, p), E=65, 800 MeV; calculated dσ with and without Brieva-Rook localization. 208Pb(8B, X), E=250 MeV/nucleon; calculated breakup σ including relativistic corrections. 209Bi(6He, 6He), E=22.5 MeV; calculated σ with and without breakup effects, B(E1) strength distribution. Three- and four-body CDCC.
doi: 10.1088/1742-6596/312/4/082008
2010HI01 Phys.Rev.Lett. 104, 212502 (2010) E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba Five-Body Cluster Structure of the Double-Λ Hypernucleus 11ΛΛBe NUCLEAR STRUCTURE 11Be; calculated energy levels of double hypernucleus; deduced observation of the ground state of 11ΛΛBe in KEK-E373 experiment.
doi: 10.1103/PhysRevLett.104.212502
2010HI07 Prog.Theor.Phys.(Kyoto), Suppl. 185, 106 (2010) E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba, T.A.Rijken S = -1 Hypernuclear Structure NUCLEAR STRUCTURE 4H, 4,6,7He, 7Li, 7,9Be, 12,13C; calculated hypernucleus excitation energies, splittings, n-p relative and probability densities, B(E2). Comparison with experimental data.
doi: 10.1143/PTPS.185.106
2010HI08 Prog.Theor.Phys.(Kyoto), Suppl. 185, 152 (2010) E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba, T.A.Rijken S = -2 Hypernuclear Structure NUCLEAR STRUCTURE 5,7H, 7He, 7,8,9,10Li, 9,10,11,12Be; calculated double hypernucleus energy levels and ground state J, π, rms radii, density distribution, binding energies. Cluster model and the Gaussian Expansion Method (GEM).
doi: 10.1143/PTPS.185.152
2009HI12 Phys.Rev. C 80, 054321 (2009) E.Hiyama, Y.Yamamoto, T.Motoba, M.Kamimura Structure of A=7 iso-triplet Λ hypernuclei studied with the four-body cluster model NUCLEAR STRUCTURE 6He, 6Li, 6Be, 7He, 7Li, 7Be; calculated levels, J, π, total interaction energies, and density distributions of hypernuclei using four-body cluster model.
doi: 10.1103/PhysRevC.80.054321
2009MO40 Nucl.Phys. A827, 318c (2009) T.Motoba, S.Sugimoto, E.Hiyama, Y.Yamamoto, Th.A.Rijken, M.Kamimura Structure and production of p-shell Ξ-hypernuclei predicted with realistic interactions
doi: 10.1016/j.nuclphysa.2009.05.065
2008HI16 Phys.Rev. C 78, 054316 (2008) E.Hiyama, Y.Yamamoto, T.Motoba, Th.A.Rijken, M.Kamimura Light Ξ hypernuclei in four-body cluster models NUCLEAR STRUCTURE 5,7H, 9,10Li, 12Be; calculated level energies, density distributions, binding energies, rms radii. Gaussian expansion method. Hypernuclei.
doi: 10.1103/PhysRevC.78.054316
2008OG01 Nucl.Phys. A805, 447c (2008) K.Ogata, T.Matsumoto, T.Egami, Y.Iseri, M.Kamimura, M.Yahiro Full coupled-channel description of three-body and four-body breakup reactions NUCLEAR REACTIONS 208Pb(8B, X), E=52 MeV/nucleon; calculated breakup σ(θ) with eikonal CDCC; deduced 7Be(p, γ) astrophysical S-factor. 209Bi(6He, 6He), E=19, 22.5 MeV; calculated total, elastic σ(θ) using four-body CDCC. Comparison with data.
doi: 10.1016/j.nuclphysa.2008.02.283
2007HA38 Phys.Lett. B 650, 268 (2007) K.Hamaguchi, T.Hatsuda, M.Kamimura, Y.Kino, T.T.Yanagida Stau-catalyzed 6Li production in big-bang nucleosynthesis NUCLEAR REACTIONS 4He(d, γ)6Li, E=low; calculated stau-catalyzed fusion σ, astrophysical S-factor.
doi: 10.1016/j.physletb.2007.05.030
2006HI05 Few-Body Systems 38, 91 (2006) E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro Five-Body Calculation of Resonance and Scattering States of the uudd(s-bar) System
doi: 10.1007/s00601-005-0143-x
2006MA31 Phys.Rev. C 73, 051602 (2006) T.Matsumoto, T.Egami, K.Ogata, Y.Iseri, M.Kamimura, M.Yahiro Coulomb breakup effects on the elastic cross section of 6He + 209Bi scattering near Coulomb barrier energies NUCLEAR REACTIONS 209Bi(6He, 6He), E=19, 22.5 MeV; analyzed elastic σ(θ), Coulomb breakup effects. Four-body continuum-discretized coupled-channels model.
doi: 10.1103/PhysRevC.73.051602
2006OG01 Phys.Rev. C 73, 024605 (2006) K.Ogata, S.Hashimoto, Y.Iseri, M.Kamimura, M.Yahiro Determination of S17 from 8B breakup by means of the method of continuum-discretized coupled channels NUCLEAR REACTIONS 208Pb(8B, p7Be), E=52 MeV/nucleon; analyzed σ(θ). 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled channels method.
doi: 10.1103/PhysRevC.73.024605
2005HI13 Nucl.Phys. A754, 103c (2005) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Three- and four-body structure of light double Λ hypernuclei NUCLEAR STRUCTURE 6,7He, 7,8,9Li, 9,10Be; calculated two-Λ hypernucleus levels, J, π. Four-body model.
doi: 10.1016/j.nuclphysa.2004.12.075
2005HI14 Nucl.Phys. A755, 411c (2005) E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro Five-body calculation of resonance and continuum states of pentaquark baryons with quark-quark correlations
doi: 10.1016/j.nuclphysa.2005.03.047
2004EG04 Phys.Rev. C 70, 047604 (2004) T.Egami, K.Ogata, T.Matsumoto, Y.Iseri, M.Kamimura, M.Yahiro Gaussian expansion approach to nuclear and Coulomb breakup NUCLEAR REACTIONS 58Ni(8B, p7Be), E=25.8 MeV; calculated breakup σ(θ), Coulomb and nuclear contributions. Continuum discretized coupled channels approach, comparison with data.
doi: 10.1103/PhysRevC.70.047604
2004HI09 Nucl.Phys. A737, 138 (2004) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Few-body aspects of light hypernuclei NUCLEAR STRUCTURE 8Be; calculated level energies. 4,6,7He, 7,8,9Li, 9,10Be, 13C; calculated energy levels, J, π for single and double Λ hypernuclei.
doi: 10.1016/S0375-9474(04)00307-0
2004HI11 Nucl.Phys. A738, 175 (2004) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Clustering aspects of light hypernuclei NUCLEAR STRUCTURE 7He, 7,8,9Li, 9,10Be; calculated double-Λ hypernuclei energy levels. Gaussian expansion method.
doi: 10.1016/j.nuclphysa.2004.04.028
2004HI14 Prog.Theor.Phys.(Kyoto) 112, 99 (2004) E.Hiyama, K.Suzuki, H.Toki, M.Kamimura Role of the Quark-Quark Correlation in Baryon Structure and Non-Leptonic Weak Transitions of Hyperons
doi: 10.1143/PTP.112.99
2004HI21 Phys.Rev. C 70, 031001 (2004) E.Hiyama, B.F.Gibson, M.Kamimura Four-body calculation of the first excited state of 4He using a realistic NN interaction: 4He(e, e')4He(0+2) and the monopole sum rule NUCLEAR STRUCTURE 4He; calculated ground and excited states energies, radii, mass densities, wave functions. Two-body and three-body forces, Gaussian expansion method. NUCLEAR REACTIONS 4He(e, e'), E not given; calculated transition form factor. Two-body and three-body forces, Gaussian expansion method.
doi: 10.1103/PhysRevC.70.031001
2004MA57 Nucl.Phys. A738, 471 (2004) T.Matsumoto, E.Hiyama, M.Yahiro, K.Ogata, Y.Iseri, M.Kamimura Four-body CDCC analysis of 6He + 12C scattering NUCLEAR REACTIONS 12C(6He, 6He), E=38.3 MeV/nucleon; analyzed σ(θ); deduced halo effects. Continuum-discretized coupled-channels approach.
doi: 10.1016/j.nuclphysa.2004.04.089
2004MB01 Phys.Rev. C 70, 061601 (2004) T.Matsumoto, E.Hiyama, K.Ogata, Y.Iseri, M.Kamimura, S.Chiba, M.Yahiro Continuum-discretized coupled-channels method for four-body nuclear breakup in 6He+12C scattering NUCLEAR REACTIONS 12C(6He, 6He), (6He, 2nα), E=18, 229.8 MeV; calculated elastic and breakup σ(θ), reaction σ. Continuum-discretized coupled-channels method, comparison with data.
doi: 10.1103/PhysRevC.70.061601
2004OG09 Nucl.Phys. A738, 421 (2004) K.Ogata, M.Yahiro, Y.Iseri, T.Matsumoto, N.Yamashita, T.Kamizato, M.Kamimura Determination of S17 from 8B Coulomb dissociation NUCLEAR REACTIONS 58Ni(8B, p7Be), E=25.8 MeV; analyzed σ(θ); deduced asymptotic normalization coefficient. 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled-channels approach.
doi: 10.1016/j.nuclphysa.2004.04.078
2003HI09 Prog.Part.Nucl.Phys. 51, 1 (2003) Gaussian, Expansion Methods for Few-Body Systems
doi: 10.1016/S0146-6410(03)00082-6
2003HI24 Mod.Phys.Lett. A 18, 95 (2003) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Few-body aspects of hypernuclear physics NUCLEAR STRUCTURE 4H, 4,7He, 7,8,9Li, 9,10Be; calculated Λ and ΛΛ hypernucleus level energies, J, π.
doi: 10.1142/S021773230301003X
2003KI20 Hyperfine Interactions 146-147, 331 (2003) Y.Kino, N.Yamanaka, M.Kamimura, H.Kudo High-Precision Calculation of the Fine and Hyperfine Structure Splittings of Antiprotonic Helium-3, 4 Atoms ATOMIC PHYSICS 3,4He; calculated hfs in antiprotonic helium atoms.
doi: 10.1023/B:HYPE.0000004218.62114.f2
2003KI27 Mod.Phys.Lett. A 18, 388 (2003) High-precision Coulomb three-body calculation of antiprotonic helium atoms ATOMIC PHYSICS He; calculated energy levels and widths for antiprotonic helium.
doi: 10.1142/S0217732303010545
2003MA91 Phys.Rev. C 68, 064607 (2003) T.Matsumoto, T.Kamizato, K.Ogata, Y.Iseri, E.Hiyama, M.Kamimura, M.Yahiro New treatment of breakup continuum in the method of continuum discretized coupled channels NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; 40Ca(6Li, 6Li), (6Li, X), E=156 MeV; calculated elastic σ, breakup S-matrix elements. Continuum discretized coupled channels, pseudostate discretization.
doi: 10.1103/PhysRevC.68.064607
2003OG02 Phys.Rev. C 67, 011602 (2003); Erratum Phys.Rev. C 67, 019902 (2003) K.Ogata, M.Yahiro, Y.Iseri, M.Kamimura Determination of S17 from the 7Be(d, n)8B reaction NUCLEAR REACTIONS 7Li(d, d), E=8 MeV; 7Li(n, n), E=4.26 MeV; 7Be(d, n), E=7.5 MeV; analyzed σ(θ); deduced parameters. 7Be(p, γ), E not given; deduced astrophysical S-factor. Continuum-discretized coupled channels, three-body model.
doi: 10.1103/PhysRevC.67.011602
2003OG06 Phys.Rev. C 68, 064609 (2003) K.Ogata, M.Yahiro, Y.Iseri, T.Matsumoto, M.Kamimura New coupled-channel approach to nuclear and Coulomb breakup reactions NUCLEAR REACTIONS 58Ni(8B, p7Be), E=240 MeV; calculated breakup σ(θ). Hybrid calculation.
doi: 10.1103/PhysRevC.68.064609
2002HI01 Phys.Rev. C65, 011301 (2002) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Λ-Σ Conversion in Λ4He and Λ4H Based on a Four-Body Calculation NUCLEAR STRUCTURE 4H, 4He; calculated hypernucleus levels, J, π; deduced role of Λ-Σ conversion. Four-body calculations.
doi: 10.1103/PhysRevC.65.011301
2002HI15 Phys.Rev. C66, 024007 (2002) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Four-body cluster structure of A=7-10 double-Λ hypernuclei NUCLEAR STRUCTURE 7He, 7,8,9Li, 9,10Be; calculated double-Λ hypernuclei level energies, J, π. Four-body cluster model.
doi: 10.1103/PhysRevC.66.024007
2002IT09 Prog.Theor.Phys.(Kyoto), Suppl. 146, 573 (2002) M.Ito, K.Kato, Y.Sakuragi, M.Kamimura, E.Hiyama 6He + 6He Molecular States in Highly-Excited 12Be NUCLEAR STRUCTURE 12Be; calculated molecular states energies, J, coupling effects.
doi: 10.1143/PTPS.146.573
2001HI05 Nucl.Phys. A684, 227c (2001) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Three- and Four-Body Structure of Light Hypernuclei
doi: 10.1016/S0375-9474(01)00418-3
2001HI09 Nucl.Phys. A691, 107c (2001) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Three- and Four-Body Structure of Light Λ Hypernuclei NUCLEAR STRUCTURE 4H, 4He, 7Li, 9Be, 13C; calculated hypernucleus levels, spin-orbit splitting, B(E2), related features.
doi: 10.1016/S0375-9474(01)01015-6
2001KA47 Phys.Rev. C64, 044001 (2001) H.Kamada, A.Nogga, W.Glockle, E.Hiyama, M.Kamimura, K.Varga, Y.Suzuki, M.Viviani, A.Kievsky, S.Rosati, J.Carlson, S.C.Pieper, R.B.Wiringa, P.Navratil, B.R.Barrett, N.Barnea, W.Leidemann, G.Orlandini Benchmark Test Calculation of a Four-Nucleon Bound State NUCLEAR STRUCTURE A=4; calculated four-nucleon bound state energy, radius, related features. Several approaches compared.
doi: 10.1103/PhysRevC.64.044001
2000HI15 Phys.Rev.Lett. 85, 270 (2000) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto ΛN Spin-Orbit Splittings in Λ9Be and Λ13C Studied with One-Boson-Exchange ΛN Interactions NUCLEAR STRUCTURE 9Be, 13C; calculated hypernuclei levels, J, π, spin-orbit splitting related features. One-boson exchange models, quark models.
doi: 10.1103/PhysRevLett.85.270
2000SU11 Nucl.Phys. A670, 307c (2000) K.Suzuki, E.Hiyama, H.Toki, M.Kamimura Constituent Quark Model for Baryons with Strong Quark-Pair Correlations and Non-Leptonic Weak Transitions of Hyperon
doi: 10.1016/S0375-9474(00)00119-6
1999HI02 Phys.Rev. C59, 2351 (1999) E.Hiyama, M.Kamimura, K.Miyazaki, T.Motoba γ Transitions in A = 7 Hypernuclei and a Possible Derivation of Hypernuclear Size NUCLEAR STRUCTURE 7He, 7Li; calculated transitions B(E2), B(M1) in hypernuclei; deduced implications for radius measurement. Three-body model. NUCLEAR REACTIONS 7Li(π+, K+), E at 1.05 GeV/c; calculated hypernuclear states production σ(E).
doi: 10.1103/PhysRevC.59.2351
1999PI13 Phys.Rev. C60, 044611 (1999) R.A.D.Piyadasa, M.Kawai, M.Kamimura, M.Yahiro Convergence of the Solution of the Continuum Discretized Coupled Channels Method NUCLEAR REACTIONS 58Ni(d, d), (d, np), E=80 MeV; calculated S-matrix elements; deduced model convergence features. Continuum discretized coupled channels method.
doi: 10.1103/PhysRevC.60.044611
1998HI13 Nucl.Phys. A639, 169c (1998) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Four-Body Calculation of Λ4H and Λ4He with Realistic ΛN Interactions NUCLEAR STRUCTURE 4H, 4He; calculated hypernuclei binding energieslevels, J, π. Four-body calculations, 3N + Λ model.
doi: 10.1016/S0375-9474(98)00267-X
1998HI14 Nucl.Phys. A639, 173c (1998) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Four-Body Model Study of Competition between YN Spin-Spin and Spin-Orbit Interactions in Light Hypernuclei NUCLEAR STRUCTURE 7Li, 13C; calculated hypernuclei levels, J, π; deduced ΛN spin-spin, spin-orbit forces related features.
doi: 10.1016/S0375-9474(98)00268-1
1998KI07 Nucl.Phys. A631, 649c (1998) High-Accuracy 3-Body Coupled-Channel Calculation of Metastable States of Antiprotonic Helium Atoms ATOMIC PHYSICS 4He; calculated antiprotonic atoms metastable states energies, widths. Three-body coupled channels method.
doi: 10.1016/S0375-9474(98)00084-0
1997HI09 Prog.Theor.Phys.(Kyoto) 97, 881 (1997) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Three- and Four-Body Cluster Models of Hypernuclei using the G-Matrix ΛN Interaction (Λ)9Be, (Λ)13C, (Λ)(Λ)6He and (Λ)(Λ)10Be NUCLEAR STRUCTURE 6He, 9,10Be, 13C; calculated hypernucleus ground, excited states energies. Three-, four-body cluster models, ΛN interaction.
doi: 10.1143/PTP.97.881
1996HI03 Phys.Rev. C53, 2075 (1996) E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto Three-Body Model Study of A = 6-7 Hypernuclei: Halo and skin structures NUCLEAR STRUCTURE A=6; A=7; calculated hypernuclei states, binding energies. Three-body model.
doi: 10.1103/PhysRevC.53.2075
1995HI15 Nucl.Phys. A588, 35c (1995) Three-Body Structure of 6He = 4He + n + n using Realistic n-n Potentials NUCLEAR STRUCTURE 6He; calculated binding energy, two-neutron relative density. Coupled-rearrangement-channel variational method, realistic NN-potential.
doi: 10.1016/0375-9474(95)00096-J
1991IS06 Nucl.Phys. A533, 574 (1991) Y.Iseri, M.Tanifuji, H.Kameyama, M.Kamimura, M.Yahiro Spin-Dependent Interactions and Polarization Observables in Elastic Scattering of Deuterons at Intermediate Energies NUCLEAR REACTIONS 58Ni(polarized d, d), E=700 MeV; calculated vector, tensor analyzing power vs θ.
doi: 10.1016/0375-9474(91)90534-D
1990KA06 Nucl.Phys. A508, 17c (1990) Coupled Rearragement Channel Calculations of Muonic Molecules and A = 3 Nuclei NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, S-, D-state probability, asymptotic normalizations. 4He; calculated binding energy. Coupled rearragement channels method.
doi: 10.1016/0375-9474(90)90459-Y
1989KA19 Phys.Rev. C40, 974 (1989) H.Kameyama, M.Kamimura, Y.Fukushima Coupled-Rearrangement-Channel Gaussian-Basis Variational Method for Trinucleon Bound States NUCLEAR STRUCTURE 2H; calculated wave function. 3H, 3He; calculated binding energy, S-, P-, D-state probabilities, S-, D-wave asymptotic normalizations. Gaussian basis, coupled-rearrangement-channel variational method.
doi: 10.1103/PhysRevC.40.974
1989MY02 Z.Phys. A334, 423 (1989) K.S.Myint, Y.Akaishi, H.Tanaka, M.Kamimura, H.Narumi Relativistic and QED Contributions to the Coulomb Three-Body System in Muon-Catalyzed Fusion
1989TA07 Phys.Lett. 217B, 375 (1989) M.Tanifuji, H.Kameyama, M.Kamimura, Y.Iseri, M.Yahiro T(R) and T(L) Tensor Interactions in Deuteron Elastic Scattering NUCLEAR REACTIONS 58Ni(polarized d, d), E=700 MeV; calculated σ(θ), analyzing power.
doi: 10.1016/0370-2693(89)90063-4
1988IS02 Nucl.Phys. A490, 383 (1988) Y.Iseri, H.Kameyama, M.Kamimura, M.Yahiro, M.Tanifuji Virtual Breakup Effects in Elastic Scattering of Polarized Deuterons NUCLEAR REACTIONS 16O, 40Ca, 58Ni, 118Sn, 208Pb(polarized d, d), E=56 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ; deduced reaction mechansim.
doi: 10.1016/0375-9474(88)90512-X
1988KA09 Nucl.Phys. A480, 323 (1988) K.Katori, T.Shimoda, T.Fukuda, S.Shimoura, A.Sakaguchi, M.Tanaka, T.Yamagata, N.Takahashi, H.Ogata, M.Kamimura, Y.Sakuragi Breakup Effects of 6,7Li on Elastic and Inelastic Scattering from 12C at 18-28 MeV/Nucleon NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), E=123.5, 168.6 MeV; 12C(7Li, 7Li), (7Li, 7Li'), E=131.8 MeV; measured σ(θ); deduced reaction mechanism. Double-folding model, coupled-discretized continuum channels model.
doi: 10.1016/0375-9474(88)90400-9
1988SA10 Nucl.Phys. A480, 361 (1988) Y.Sakuragi, M.Yahiro, M.Kamimura, M.Tanifuji Effects of Projectile Breakup and Target Excitation in Scattering of Polarized 7Li NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=21 MeV; 26Mg(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; analyzed σ(θ), vector, tensor analyzing power. Projectile breakup, double folding interaction, coupled-channels.
doi: 10.1016/0375-9474(88)90402-2
1988SA15 Phys.Lett. 205B, 204 (1988) Y.Sakuragi, M.Kamimura, K.Katori Effects of 6Li → α + d and 12C → 3α Breakup Processes in 6Li + 12C Scattering NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), E=124, 169 MeV; analyzed σ(θ); deduced projectile, target breakup role. Coupled discretized continuum channels.
doi: 10.1016/0370-2693(88)91650-4
1987SA04 Nucl.Phys. A462, 173 (1987) Y.Sakuragi, M.Yahiro, M.Kamimura, M.Tanifuji Scattering of Polarized 7Li by 120Sn and Projectile-Target Spin-Dependent Interactions NUCLEAR REACTIONS 120Sn(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=20.3 MeV; calculated σ(θ), analyzing powers, form factors; deduced spin-orbit interaction, projectile virtual excitation effects, invariant amplitudes vs tensor interactions. Coupled-channels model, cluster-, double-folding interactions.
doi: 10.1016/0375-9474(87)90385-X
1987TA21 Phys.Rev. C36, 2146 (1987) M.Tanaka, T.Yamagata, S.Nakayama, M.Inoue, Y.Sakuragi, M.Kamimura, K.Goto, K.Katori, M.Yanagi, H.Ogata Observation of Vector Analyzing Power in Elastic Scattering of 150-MeV 6Li on 12C NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=150 MeV; measured σ(θ), left-right asymmetry; deduced iT11(θ). Cluster folding coupled channel calculations, projectile excitations.
doi: 10.1103/PhysRevC.36.2146
1987YA06 Nucl.Phys. A463, 435c (1987) M.Yahiro, Y.Iseri, H.Kameyama, M.Kamimura, M.Kawai, M.Tanifuji Deuteron Breakup Effects on Deuteron Elastic Scattering NUCLEAR REACTIONS 58Ni, 208Pb(polarized d, d), E=56, 400 MeV; calculated σ(θ), analyzing powers; deduced deuteron breakup effects. Coupled discretized continuum channels method.
doi: 10.1016/0375-9474(87)90687-7
1986SA15 Phys.Lett. 175B, 105 (1986) Y.Sakuragi, M.Kamimura, M.Yahiro, M.Tanifuji Roles of Folding Spin-Orbit Potentials in 6,7Li(pol) Scattering NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), E=21.1 MeV; analyzed iT11(θ). 120Sn(polarized 7Li, 7Li), E=44 MeV; calculated σ(θ), vector analyzing power vs θ; deduced folding spin-orbit potentials role.
doi: 10.1016/0370-2693(86)90696-9
1986YA11 Phys.Lett. 182B, 135 (1986) M.Yahiro, H.Kameyama, Y.Iseri, M.Kamimura, M.Kawai Coupled-Channel Approach to Deuteron Elastic Scattering at Intermediate Energy NUCLEAR REACTIONS 40Ca(polarized p, p), E=200 MeV; analyzed σ(θ), analyzing power vs θ; deduced proton optical potentials; 58Ni(polarized d, d), E=400 MeV; calculated σ(θ), vector, tensor analyzing powers. Coupled channels method.
doi: 10.1016/0370-2693(86)91563-7
1985KU23 Phys.Lett. 163B, 75 (1985) S.Kubono, M.Sugitani, M.H.Tanaka, K.Morita, Y.Sakuragi, M.Kamimura 3α-Breakup Induced Dynamical Polarization Potential of 12C at E/A ≥ 10 MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=139.5, 158.8 MeV; measured σ(θ); deduced breakup process role. 12C level deduced α-breakup. Coupled-channels analysis.
doi: 10.1016/0370-2693(85)90195-9
1985NA05 Prog.Theor.Phys.(Kyoto) 73, 512 (1985) S.Nagata, M.Kamimura, N.Yamaguchi On a Calculational Method of Folding Model Potential with Density-Dependent Effective Interactions NUCLEAR REACTIONS 40Ca(α, α), E=141.7 MeV; calculated folding potential real part. 40Ca(p, p), E=30 MeV; calculated exchange potential real, imaginary terms. Density-dependent effective interactions.
doi: 10.1143/PTP.73.512
1985OH01 Phys.Lett. 150B, 25 (1985) The Dynamically Induced Spin-Orbit Interaction of the 19F Projectile NUCLEAR REACTIONS 28Si(19F, 19F), E=60 MeV; calculated σ(θ), P(θ); deduced spin-orbit potential dynamical component. Coupled-channels formalism.
doi: 10.1016/0370-2693(85)90130-3
1985SA13 Phys.Lett. 153B, 372 (1985) Y.Sakuragi, M.Kamimura, M.Yahiro, M.Tanifuji Folding Interactions in the Scattering of Soft Heavy Ions by Light Nuclei NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), E=21.1 MeV; 16O(polarized 6Li, 6Li), E=22.8 MeV; analyzed σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced Coulomb barrier, reaction mechanism dependences. Coupled-channels method.
doi: 10.1016/0370-2693(85)90475-7
1985SA36 Z.Phys. A322, 627 (1985) Y.Sakuragi, M.Kamimura, S.Micek, H.Rebel, H.J.Gils 6Li Break-Up Effect on Elastic and Inelastic Scattering of 6Li + 6Li at 156 MeV NUCLEAR REACTIONS 6Li(6Li, 6Li), (6Li, 6Li'), E=156 MeV; measured σ(θ). 6Li deduced breakup channel coupling role. Coupled, discretized continuum channels model.
doi: 10.1007/BF01415144
1984OH01 Nucl.Phys. A415, 271 (1984) H.Ohnishi, M.Tanifuji, M.Kamimura, Y.Sakuragi, M.Yahiro Tensor Interactions and Polarization Phenomena in Heavy-Ion Scattering NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=14.2, 20.3 MeV; calculated σ(θ), analyzing power vs θ. Coupled-channels method, cluster-folding interactions.
doi: 10.1016/0375-9474(84)90623-7
1984SA31 Phys.Lett. 149B, 307 (1984) 12C → 3α Breakup Effect on the Scattering of 16O + 12C and 13C + 12C NUCLEAR REACTIONS 12C(16O, 16O), E=168, 216, 311 MeV; 12C(13C, 13C), E=260 MeV; calculated dynamical polarization potential, σ(θ). Microscopic α-breakup, coupled-channels method.
doi: 10.1016/0370-2693(84)90412-X
1984YA01 Phys.Lett. 141B, 19 (1984) M.Yahiro, Y.Iseri, M.Kamimura, M.Nakano A Coupled-Channel Approach to Deuteron Projectile Breakup NUCLEAR REACTIONS 12C, 51V, 118Sn(d, np), E=56 MeV; calculated σ(θn, θp, Ep), σ(breakup). Three-body model, discretized continuum coupled channels.
doi: 10.1016/0370-2693(84)90549-5
1983SA39 Prog.Theor.Phys.(Kyoto) 70, 1047 (1983) Y.Sakuragi, M.Yahiro, M.Kamimura Elastic Scattering and Breakup of 6Li - A New Type of Dynamical Polarization Potential NUCLEAR REACTIONS 4He(d, d), E(cm)=0-15 MeV; calculated phase shifts. Cluster model. 6Li(e, e), (e, e'), E not given; calculated charge form factors. 28Si(6Li, 6Li), E=99 MeV; 40Ca(6Li, 6Li), E=156 MeV; calculated σ(θ). Cluster model, projectile breakup, microscopic coupled-channels methods.
doi: 10.1143/PTP.70.1047
1982OH09 Phys.Lett. 118B, 16 (1982) H.Ohnishi, M.Tanifuji, M.Kamimura, M.Yahiro Effects of Tensor Interactions and Projectile Excitations in the Scattering of 7Li NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=20.3 MeV; analyzed σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced tensor interaction, projectile excitation roles. Coupled-channels method, folding model interactions.
doi: 10.1016/0370-2693(82)90592-5
1982SA16 Prog.Theor.Phys.(Kyoto) 68, 322 (1982) Y.Sakuragi, M.Yahiro, M.Kamimura Projectile Breakup Effect on 6Li Elastic Scattering from 28Si and 40Ca Studied by Microscopic Coupled-Channels Method NUCLEAR REACTIONS 40Ca(6Li, 6Li), E=156 MeV; 28Si(6Li, 6Li), E=99 MeV; calculated σ(θ); deduced projectile breakup effect. Discretized continuum, coupled-channels method, cluster model.
doi: 10.1143/PTP.68.322
1982YA03 Prog.Theor.Phys.(Kyoto) 67, 1467 (1982) M.Yahiro, M.Nakano, Y.Iseri, M.Kamimura Coupled-Discretized-Continuum-Channels Method for Deuteron Breakup Reactions Based on Three-Body Model - Justification of the Method for Truncation and Discretization of the p-n Continuum - NUCLEAR REACTIONS, ICPND 58Ni(d, d), (d, np), E=80 MeV; calculated σ(elastic), breakup σ. Coupled-channels method, continuum discretization.
doi: 10.1143/PTP.67.1467
1981KA03 Nucl.Phys. A351, 456 (1981) Transition Densities between the 0+1, 2+1, 4+1, 0+2, 2+2, 1-1 and 3-1 States in 12C Derived from Three-Alpha Resonating-Group Wave Functions NUCLEAR REACTIONS 12C(e, e), E=30-750 MeV; calculated form factors. Microscopic 3 α resonating group wave function. NUCLEAR STRUCTURE 12C; calculated multipole transition densities. Microscopic 3 α resonating group wave function.
doi: 10.1016/0375-9474(81)90182-2
1981NO13 Prog.Theor.Phys.(Kyoto) 66, 1906 (1981) T.Nojiri, M.Kamimura, M.Sano, M.Wakai, K.Yoro Coupled-Channel Study of Proton Inelastic Scattering from the Second 01 State in 12C by use of the 3α Resonating-Group Wave Function NUCLEAR REACTIONS 12C(p, p'), E=65 MeV; calculated σ(θ). Coupled-channel method, three alpha resonating group wave functions.
doi: 10.1143/PTP.66.1906
1976MI17 Progr.Theor.Phys. 56, 583 (1976) The Generator Coordinate Method for Composite-Particle Scattering Based on the Kohn-Hulthen Variational Principle. Application to α-α, 16O-α and 16O-16O Scattering NUCLEAR REACTIONS 4He(α, α), 16O(16O, 16O), (α, α), E(cm) ≤ 60 MeV; calculated wave functions, phase shifts. Generator coordinate method.
doi: 10.1143/PTP.56.583
1975MA26 Progr.Theor.Phys. 53, 706 (1975) T.Matsuse, M.Kamimura, Y.Fukushima Study of the Alpha-Clustering Structure of 20Ne Based on the Resonating Group Method for 16O + α - Analysis of Alpha-Decay Widths and the Exchange Kernel NUCLEAR STRUCTURE 20Ne; calculated α-clustering, levels, B(E2).
doi: 10.1143/PTP.53.706
1973MA50 Progr.Theor.Phys. 49, 1765 (1973) A Study of α-Widths of 20Ne Based on 16O and α-Cluster Model NUCLEAR STRUCTURE 20Ne; calculated levels, level-width.
doi: 10.1143/PTP.49.1765
1972KA39 Prog.Theor.Phys. 47, 1537 (1972) M.Kamimura, T.Matsuse, K.Takada Alpha-Like Spatial Four-Body Correlations in Light Nuclei NUCLEAR STRUCTURE 20Ne; calculated levels; analyzed spatial correlations, higher-shell mixing effects. α-like spatial 4-body correlations.
doi: 10.1143/PTP.47.1537
1972KA67 Progr.Theor.Phys.Suppl. 52, 282 (1972) M.Kamimura, T.Marumori, K.Takada Alpha-Like Four-Body Correlations and Molecular Aspects in Nuclei. Chapter VI. Many-Body Theoretical Description of Alpha-Like Four-Body Correlations NUCLEAR STRUCTURE 19F, 20,21Ne; calculated α-cluster structure.
doi: 10.1143/PTPS.52.282
1967KA05 Nucl.Phys. A95, 129 (1967) Giant Dipole States and Excited Giant Dipole States in 12C
doi: 10.1016/0375-9474(67)90156-X
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