NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Kammuri Found 30 matches. 1996KU28 Phys.Rev. C54, 2331 (1996) T.Kubo, H.Sakamoto, T.Kammuri, T.Kishimoto Self-Consistent Velocity Dependent Effective Interactions NUCLEAR STRUCTURE 148,150Sm, 40Ca; calculated E1 transition strength function. 94,96,98,100Mo, 112,114,116,118,120,122,124Sn; calculated level energy, B(λ). Self-consistent velocity dependent effective interactions.
doi: 10.1103/PhysRevC.54.2331
1994KA19 Prog.Theor.Phys.(Kyoto) 91, 27 (1994) Rapidly Rotating Nuclei in the SU3 Model
doi: 10.1143/PTP.91.27
1994KA52 Prog.Theor.Phys.(Kyoto) 92, 319 (1994) Semiquantal Treatment of Sequential Two-Nucleon Transfer Reactions Induced by Heavy Ions
doi: 10.1143/ptp/92.2.319
1987MI14 Prog.Theor.Phys.(Kyoto) 77, 1209 (1987) Continuum Spectra in Heavy-Ion Induced One-Nucleon Transfer Reactions NUCLEAR REACTIONS 52Cr(14N, 13C), E=70, 80 MeV; 52Cr(12C, 11B), E=70 MeV; 208Pb(16O, 15N), E=312.6 MeV; analyzed particle spectra; deduced reaction mechanism. 209Bi deduced i11/2, j15/2 single particle state energies, widths.
doi: 10.1143/PTP.77.1209
1985MI22 Prog.Theor.Phys.(Kyoto) 74, 931 (1985) Nucleon Transfer to Resonant and Non-Resonant States in the Continuum Spectra of Heavy-Ion Direct Reactions NUCLEAR REACTIONS 92Mo(14N, 13C), E=97 MeV; analyzed data. 93Tc deduced resonant state population dominance.
doi: 10.1143/PTP.74.931
1982KU02 Nucl.Phys. A376, 401 (1982) P.D.Kunz, T.Kammuri, H.Shimaoka Microscopic Form Factor for DWBA Analysis of Light-Ion Induced Three-Nucleon Transfer Reactions NUCLEAR REACTIONS 118Sn(p, α), (polarized p, α), E=20.4, 22 MeV; analyzed σ(θ), analyzing power vs θ. Microscopic form factors, modified zero-range DWBA.
doi: 10.1016/0375-9474(82)90120-8
1982MA08 Nucl.Phys. A376, 341 (1982) Gross Properties of Heavy-Ion Transfer Reactions (II). Comparison with Experiment NUCLEAR REACTIONS 53Cr(14N, 13C), E=90 MeV; 96Mo(14N, 15O), E=97 MeV; 181Ta(16O, 17O), E=96 MeV; 208Pb(16O, 15N), E=312.6 MeV; calculated particle spectra. 100Mo(14N, 12B), E=90, 125, 200 MeV; 197Au(19F, 12B), E=186 MeV; calculated σ(θ, E(12B)), polarization vs E(12B). 40Ca(20Ne, 16O), E=262 MeV; 40Ca(14N, 10B), E=153 MeV; 40Ca(13C, 9Be); calculated σ(θ) vs particle energy. Heavy-ion transfer, semi-classical theory.
doi: 10.1016/0375-9474(82)90069-0
1980KA03 Phys.Lett. 90B, 197 (1980) T.Kammuri, H.Shimaoka, P.D.Kunz, S.Kato, K.Okada, M.Kondo, K.Hosono, T.Saito, N.Matsuoka, S.Nagamachi, T.Noro, K.Ogino, Y.Kadota DWBA Form Factor for Three-Particle Transfer Reaction NUCLEAR REACTIONS 13C(polarized p, α), E=65 MeV; analyzed σ(θ), A(θ). DWBA, three-particle transfer form factor, modified Bayman-Kallis model.
doi: 10.1016/0370-2693(80)90722-4
1980MA24 Prog.Theor.Phys.(Kyoto) 63, 1067 (1980) K.Matsuoka, T.Kammuri, M.Sano, N.Takahashi Spin Alignment of Products 12B in 14N Induced Reactions NUCLEAR REACTIONS 100Mo(14N, 12B), E=90 MeV; calculated 12B polarization vs Q. Semiclassical model, cluster transfer.
doi: 10.1143/PTP.63.1067
1978IS01 Phys.Lett. 73B, 281 (1978) M.Ishihara, K.Tanaka, T.Kammuri, K.Matsuoka, M.Sano Semiclassical Analysis of the Spin Polarization of 12B in the 100Mo(14N, 12B)102Ru Reaction NUCLEAR REACTIONS 100Mo(14N, 12B), E=90 MeV; calculated polarization, σ.
doi: 10.1016/0370-2693(78)90514-2
1978KA14 J.Phys.(London) G4, L93 (1978) T.Kammuri, T.Motobayashi, I.Kohno, S.Nakajima, M.Yoshie, K.Katori, T.Mikumo, H.Kamitsubo Effects of Recoil and Sequential Transfer on the 12C(14N, 12C)14N Reaction NUCLEAR REACTIONS 12C(14N, 12C), E=79, 155 MeV; calculated σ(θ). Full recoil, one-, two-step DWBA method.
doi: 10.1088/0305-4616/4/4/004
1978KA15 J.Phys.(London) G4, 541 (1978) Full-Recoil One- and Two-Step DWBA Analysis of the 64Ni(16O, 14C)66Zn Reaction NUCLEAR REACTIONS 64Ni(16O, 14C), E=56 MeV; calculated σ(θ). Full recoil, one-, two-step DWBA method.
doi: 10.1088/0305-4616/4/4/010
1978KA23 Z.Phys. A287, 85 (1978) Full-Recoil One- and Two-Step DWBA Analysis of the Two-Nucleon Transfer Reactions between Heavy Ions NUCLEAR REACTIONS 14C(16O, 18O), E=20, 25, 32 MeV; 26Mg(16O, 14C), E=33, 45, 60, 128 MeV; 48Ca(16O, 14C), E=56 MeV; calculated σ(θ).
doi: 10.1007/BF01408364
1978KA34 Z.Phys. A288, 203 (1978) Boson Description of Nuclear Collective Motion. III. Coupled System of the Quadrupole and Octupole Vibrations NUCLEAR STRUCTURE 100Ru, 112Cd, 150Sm, 150Gd; calculated yrast band, ground state band levels; polarizability of E1 transitions.
doi: 10.1007/BF01408651
1976KA04 Nucl.Phys. A259, 343 (1976) On the Importance of the Sequential Transfer Process in the Two-Nucleon Transfer between Heavy Ions NUCLEAR REACTIONS 12C(18O, 16O), E=24 MeV; 48Ca(16O, 14C), E=56 MeV; 60Ni(18O, 16O), E=65 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90071-3
1976KA13 Nucl.Phys. A263, 178 (1976) Effect of Tensor Force and One-Nucleon Exchange in the Quasielastic (6Li, 6He) Reaction NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; calculated σ(θ). Antisymmetrized DWBA.
doi: 10.1016/0375-9474(76)90192-5
1976KA17 Z.Phys. A278, 41 (1976) Boson Description of Nuclear Collective Motion. II. Application to Octupole Vibration NUCLEAR STRUCTURE 112Cd, 148Sm; calculated, compared quadrupole, octupole vibration. Boson expansion method.
doi: 10.1007/BF01547340
1974GA11 Nucl.Phys. A221, 238 (1974) Study of the (6Li, 6He) Reaction on the Targets 19F, 27Al and 58,60,64Ni NUCLEAR REACTIONS 19F, 27Al(6Li, 6He), E=34 MeV; 58,60,64Ni(6Li, 6He), E=36 MeV; measured σ(θ). 64Cu deduced levels, L, J, π. 40Ca(6Li, 6He), 88Sr(6Li, 6He), E=38 MeV upper limits for σ(θ). Enriched targets.
doi: 10.1016/0375-9474(74)90316-9
1974GA17 Nucl.Phys. A222, 579 (1974) C.Gaarde, T.Kammuri, F.Osterfeld The (6Li, 6He) Spin-Isospin-Flip Reaction NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; measured nothing, calculated σ(E(6He), θ). 48Sc levels deduced wavefunctions.
doi: 10.1016/0375-9474(74)90340-6
1974KA12 Phys.Lett. 49B, 332 (1974) Decoupling in the Positive Parity Bands in Odd-Mass Er Isotopes NUCLEAR STRUCTURE 157,159,161,163Er; calculated levels. Coriolis coupling calculation.
doi: 10.1016/0370-2693(74)90173-7
1974KA26 Phys.Lett. 51B, 442 (1974) Competition between Simultaneous and Successive Transfer Processes in the Two-Nucleon Transfer Reactions Induced by Heavy Ions NUCLEAR REACTIONS 64Ni(16O, 14C), E=56 MeV; calculated σ(E(14C), θ).
doi: 10.1016/0370-2693(74)90304-9
1973BR17 Phys.Lett. 45B, 23 (1973) R.A.Broglia, U.Gotz, M.Ichimura, T.Kammuri, A.Winther On the Reaction Mechanism of Two-Nucleon Transfer between Heavy Ions NUCLEAR REACTIONS 118Sn(120Sn, 118Sn);E=500 MeV; calculated scattering amplitudes.
doi: 10.1016/0370-2693(73)90243-8
1973GA21 Nucl.Phys. A215, 314 (1973) Study of the 48Ca(6Li, 6He)48Sc Reaction at 34 MeV NUCLEAR REACTIONS 48Ca(6Li, 6He), E=34 MeV; measured σ(E(6He), θ). 48Sc deduced levels, L, J, π. Enriched target.
doi: 10.1016/0375-9474(73)90658-1
1973KA29 Z.Phys. 262, 439 (1973) Two-Nucleon Transfer Reactions between Heavy Ions NUCLEAR REACTIONS 26Mg(18O, 16O), E=33.5, 35.7 MeV; measured nothing, calculated σ(θ). 28Mg levels calculated S, deformation parameters.
doi: 10.1007/BF01394543
1973KA41 Nucl.Phys. A215, 178 (1973) Rotations and Intrinsic Kπ = 1+ Excitations in Deformed Rare-Earth Nuclei NUCLEAR STRUCTURE 170Yb; calculated transitions, B(M1), B(E2).
doi: 10.1016/0375-9474(73)90109-7
1972KA05 Phys.Lett. 38B, 5 (1972) Effect of the Spin-Dependent Force on the Moment of Inertia NUCLEAR STRUCTURE A=152-186; calculated moments of inertia. Spin-dependent force.
doi: 10.1016/0370-2693(72)90185-2
1972KA14 Phys.Lett. 39B, 327 (1972) The Use of the Angular Momentum Projection Technique in Two-Nucleon Transfer Reactions on Deformed Nuclei NUCLEAR REACTIONS 154Sm(p, t), E=52 MeV; calculated σ, spectroscopic amplitude. Angular momentum projection.
doi: 10.1016/0370-2693(72)90129-3
1972KA51 Z.Phys. 255, 431 (1972) On a RPA Method with Angular Momentum Projection
doi: 10.1007/BF01392479
1972ST18 Phys.Rev.Lett. 29, 438 (1972) F.S.Stephens, R.M.Diamond, J.R.Leigh, T.Kammuri, K.Nakai Decoupled Yrast States in Odd-Mass Nuclei
doi: 10.1103/PhysRevLett.29.438
1969KA20 Nucl.Phys. A137, 641 (1969) Analysis of the Three-Nucleon Transfer Reactions in the Pairing Potential Model NUCLEAR REACTIONS 27Al, 28Si, 31P, 32S, 48Ca, 56Fe, 59Co, 60Ni(α, p), E = 18-31 MeV; 89Y, 92Zr(p, α), E = 20, 28 MeV; calculated σ(θ). DWBA analysis, pairing potential model.
doi: 10.1016/0375-9474(69)90099-2
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