NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = K.Takada Found 26 matches. 2006TA18 Prog.Theor.Phys.(Kyoto) 116, 107 (2006) K.Takada, S.Tazaki, S.Yasumoto Dyson Boson Mapping and Shell-Model Calculations for Even-Even Nuclei NUCLEAR STRUCTURE 22Ne, 24Mg, 46,48Ti, 52Cr; calculated levels, J, π, B(E2); deduced coupling effects between collective and non-collective degrees of freedom. Shell model, Dyson boson mapping, comparison with data.
doi: 10.1143/PTP.116.107
2004JE13 Nucl.Phys. A746, 293c (2004) S.C.Jeong, I.Katayama, H.Kawakami, H.Ishiyama, Y.Watanabe, H.Miyatake, E.Tojyo, M.Oyaizu, K.Enomoto, M.Sataka, S.Okayasu, H.Sugai, S.Ichikawa, K.Nishio, Y.Sugiyama, A.Iwase, M.Yahagi, T.Hashimoto, K.Takada, M.Watanabe, M.Tanigaki, T.Shinozuka 8Li and 18F diffusion experiments in solids - an application of accelerated RNB -
doi: 10.1016/j.nuclphysa.2004.09.026
2002TA12 Nucl.Phys. A706, 365 (2002) What is the Collective Subspace in the Many-Nucleon Hilbert Space ? NUCLEAR STRUCTURE 46,48,50Ca; calculated levels, J, π. Dyson boson mapping method, comparison with shell model results and data.
doi: 10.1016/S0375-9474(02)00880-1
2001TA20 Prog.Theor.Phys.(Kyoto), Suppl. 141, 179 (2001) Non-Unitary Boson Mapping and Its Application to Nuclear Collective Motions
doi: 10.1143/PTPS.141.179
2000TA28 Prog.Theor.Phys.(Kyoto) 104, 173 (2000) A New Formulation of a Many-Level Shell Model - A Method of Constructing Orthonormal Basis States Analytically -
doi: 10.1143/PTP.104.173
1998SA63 Prog.Theor.Phys.(Kyoto) 100, 581 (1998) Convergence of Boson Expansion Theory NUCLEAR STRUCTURE 208Pb; calculated excited levels vs octupole-force strength. Normal-ordered Holstein-Primakoff boson expansion.
doi: 10.1143/PTP.100.581
1996TA14 Prog.Theor.Phys.(Kyoto) 95, 1121 (1996) Two-Octupole-Phonon States in 146,148Gd NUCLEAR STRUCTURE 146,148Gd; calculated levels, B(λ); deduced Dyson boson mapping method applicability to two-octupole-phonon states.
doi: 10.1143/PTP.95.1121
1991TA04 Nucl.Phys. A523, 354 (1991) Two-Octupole-Phonon States in 208Pb NUCLEAR STRUCTURE 208Pb; calculated levels, B(λ). Collective multi-phonon space, Dyson boson mapping.
doi: 10.1016/0375-9474(91)90008-T
1989TA13 Nucl.Phys. A496, 224 (1989) Microscopic Study on the Shape Phase Transition in the Sm Isotopes (I). Effect of Ground-State Correlation NUCLEAR STRUCTURE 148,150,152,154Sm; calculated levels. Dyson boson mapping methods.
doi: 10.1016/0375-9474(89)90173-5
1989YA05 Nucl.Phys. A496, 239 (1989) Microscopic Study on the Shape Phase Transition in the Sm Isotopes: (II). Contribution from Non-Collective Degrees of Freedom NUCLEAR STRUCTURE 148,150,152,154Sm; calculated yrast levels. Dyson type self-consistent collective coordinate method.
doi: 10.1016/0375-9474(89)90174-7
1989YA14 Nucl.Phys. A503, 53 (1989) Microscopic Study on the Shape Phase Transition in the Sm Isotopes (III). E2 Transition NUCLEAR STRUCTURE 148,150,152,154Sm; calculated B(λ); deduced shape phase transition. Microscopic approach.
doi: 10.1016/0375-9474(89)90253-4
1988YA01 Nucl.Phys. A480, 143 (1988) Coupling Effect between Quadrupole Phonon and Pairing Vibration in Odd-Mass Nuclei NUCLEAR STRUCTURE 112,114,116,118,120,122Sn; 73,77,79,81Se; calculated levels. 72Se, 91Nb, 111,113,115,117,119,121Sn; calculated levels, B(E2). Quadrupole phonon, pairing vibration coupling.
doi: 10.1016/0375-9474(88)90389-2
1987TA02 Nucl.Phys. A462, 561 (1987) Application of Dyson Mapping to Odd-Mass Nuclei NUCLEAR STRUCTURE 100,102,104,106,108Ru, 101,103,105,107,109Rh; calculated levels. Dyson theory.
doi: 10.1016/0375-9474(87)90405-2
1987TS03 Nucl.Phys. A466, 70 (1987) Application of the Dyson Boson Mapping to the Analysis of the Phase Transition at N = 88-90 NUCLEAR STRUCTURE 146,148,150,152,154Sm; calculated neutron, proton gap energies, levels. Dyson boson mapping theory.
doi: 10.1016/0375-9474(87)90345-9
1986TA04 Nucl.Phys. A448, 56 (1986) Application of Dyson Boson Mapping to the Analysis of Mode-Mode Coupling in Ge and Se Isotopes NUCLEAR STRUCTURE 72,74,76,78,80Se, 70,72,74,76Ge; calculated levels, B(λ), quadrupole moment. Dyson boson mapping, quadrupole phonon, pairing vibrational mode coupling.
doi: 10.1016/0375-9474(86)90180-6
1985TA05 Nucl.Phys. A439, 489 (1985) Dyson-Type Boson Mapping and SU(6) Boson Model NUCLEAR STRUCTURE 74Se, 114Cd, 126Xe; calculated levels, yrast sequences, B(E2), ratios. Dyson type boson mapping, SU(6) model.
doi: 10.1016/0375-9474(85)90423-3
1984TA21 Nucl.Phys. A431, 16 (1984) Quasiparticle Shell-Model Calculation within Multi-Phonon Subspace and SU(6) Boson Model NUCLEAR STRUCTURE 74Se, 114Cd, 126Xe; calculated yrast levels, B(E2). Quasiparticle shell model, multi-phonon subspace, SU(6) boson formalism.
doi: 10.1016/0375-9474(84)90053-8
1983TA03 Nucl.Phys. A395, 165 (1983) E0 Transition and Coupling between Quadrupole and Pairing-Vibrational Modes NUCLEAR STRUCTURE 66,68,70,72Zn, 70,72,74,76Ge, 72,74,76,78,80Se, 78,80,82,84Kr, 78,80,82,84,86,92,94Sr, 94,96Zr, 92,96,98,100,102Mo, 96,98,100,102,104,106Ru; calculated E0 transition matrix elements, 0+ level energies, pairing-vibrational component. 104,106,108,110,112Pd, 106,108,110,112,114,116,118Cd, 112,114,116,118,120,122Sn; calculated 2+ level energies, B(E2), quadrupole moment. Two-phonon, pairing vibration mode-mode coupling.
doi: 10.1016/0375-9474(83)90093-3
1979TA26 Prog.Theor.Phys.(Kyoto) 61, 1666 (1979) Quasiparticle-Shell-Model Calculations of So-Called Two-phonon States in Cd and Sn Isotopes NUCLEAR STRUCTURE 112,114,116,118,120Sn, 106,108,110,112,114,116,118Cd; calculated levels, static quadrupole moment, B(E2); deduced anharmonicity effects. Quasiparticle shell model.
doi: 10.1143/PTP.61.1666
1979TA27 Prog.Theor.Phys.(Kyoto) 62, 440 (1979) Dynamical Anharmonicity Effects in Low-Lying Negative-Parity States of Odd-Mass Sn Isotopes NUCLEAR STRUCTURE 111,113,115,117,119,121Sn; calculated levels; deduced anharmonicity effects. Quasiparticle shell-model.
doi: 10.1143/PTP.62.440
1978SA12 Z.Phys. A286, 195 (1978) F.Sakata, S.Iwasaki, T.Marumori, K.Takada Structure of Excited States in Se-Isotopes NUCLEAR STRUCTURE 72,74,76,78,80Se; calculated structure, B(E2).
doi: 10.1007/BF01408976
1976IW04 Prog.Theor.Phys. 56, 1140 (1976) S.Iwasaki, T.Marumori, F.Sakata, K.Takada Structure of the Anomalous 0+' Excited States in Spherical Even-Even Nuclei with N or Z ≈ 40 NUCLEAR STRUCTURE 70,72,74,76Ge, 72,74,76,78,80Se, 84Kr, 86Sr, 88Zr, 90Mo, 114,116,118,120,122,124,126Te; calculated structure of anomalous 0+ levels in spherical nuclei with N, Z ≈ 40, N=66.
doi: 10.1143/PTP.56.1140
1974TA19 Progr.Theor.Phys. 52, 1205 (1974) Role of Particle-Hole Interaction in the Four-Particle-Four-Hole States in 16O NUCLEAR STRUCTURE 12C, 20Ne; calculated levels.
doi: 10.1143/PTP.52.1205
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
1962IK01 Progr.Theoret.Phys.(Kyoto) 27, 1077 (1962)
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