NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = K.Yabana Found 59 matches. 2016SE07 Phys.Rev. C 93, 054616 (2016) Time-dependent Hartree-Fock calculations for multinucleon transfer and quasifission processes in the 64Ni + 238U reaction NUCLEAR REACTIONS 238U(64Ni, X), E(cm)=277-495 MeV; calculated multinucleon transfer (MNT) and quasifission (QF) dynamics for three orientations of 238U, scattering angles, total kinetic energy (TKE), contact time, mass and charge of reaction products, density contours, production cross sections in proton-transfers channels (up to six protons), Mass-angle distribution (MAD) plots. Three-dimensional time-dependent Hartree-Fock (TDHF) calculations with Skyrme SLy5 energy density functional (EDF) for various initial conditions. Comparison with available experimental data.
doi: 10.1103/PhysRevC.93.054616
2015AK03 Phys.Rev. C 92, 022801 (2015) Imaginary-time formalism for triple-α reaction rates
doi: 10.1103/PhysRevC.92.022801
2014SE23 Phys.Rev. C 90, 064614 (2014) Particle-number projection method in time-dependent Hartree-Fock theory: Properties of reaction products NUCLEAR REACTIONS 16O(24O, X)14C/15N/16O/17O/18O/25F/22O/23O/24O/26Ne, E=2, 4, 8 MeV/nucleon; calculated deflection angle, TKEL, transfer probabilities with respect to target-like fragments (TLF) and projectile-like fragments (PLF), expectation values of the angular momentum operator for fragment nuclei as function of the distance of closest approach, average excitation energies of fragment nuclei. Time-dependent Hartree-Fock (TDHF) theory in three-dimensional Cartesian grid representation combined with particle-number projection method for one- and two-nucleon removal reactions.
doi: 10.1103/PhysRevC.90.064614
2013FU09 Phys.Rev. C 88, 014321 (2013) Y.Fukuoka, S.Shinohara, Y.Funaki, T.Nakatsukasa, K.Yabana Deformation and cluster structures in 12C studied with configuration mixing using Skyrme interactions NUCLEAR STRUCTURE 12C; calculated levels, J, π, B(E2), B(E3), E0 transition probability, mass rms radius of excited states, elastic form factor for E0 transitions, Slater determinants, nuclear density contour plots. Coupling between shell-model and cluster configurations. Configuration-mixing method with different parameters of Skyrme interaction. Three-α linear-chain configuration of second excited 0+ state. Comparison with previous theoretical studies, and with experimental data.
doi: 10.1103/PhysRevC.88.014321
2013IN06 Phys.Rev. C 88, 051305 (2013) T.Inakura, T.Nakatsukasa, K.Yabana Low-energy $E1$ strength in select nuclei: Possible constraints on neutron skin and symmetry energy NUCLEAR STRUCTURE 24O, 26Ne, 48,52,54Ca, 58Cr, 68,78,84Ni, 208Pb; calculated correlations between low-lying electric dipole (E1) strength (PDR) and neutron-skin thickness. 84Ni; calculated E1 strengths for PDR GDR. Self-consistent random-phase approximation by using several Skyrme energy functionals.
doi: 10.1103/PhysRevC.88.051305
2013OK01 Phys.Rev. C 88, 025801 (2013) M.Okamoto, T.Maruyama, K.Yabana, T.Tatsumi Nuclear "pasta" structures in low-density nuclear matter and properties of the neutron-star crust
doi: 10.1103/PhysRevC.88.025801
2013SE10 Phys.Rev. C 88, 014614 (2013); Erratum Phys.Rev. C 93, 029902 (2016) Time-dependent Hartree-Fock calculations for multinucleon transfer processes in 40, 48Ca+124Sn, 40Ca+208Pb, and 58Ni+208Pb reactions NUCLEAR REACTIONS 124Sn(40Ca, X), (48Ca, X), E=170, 174 MeV; 208Pb(40Ca, X), E=235, 249 MeV; 208Pb(58Ni, X), E=328.4 MeV; calculated total energy loss (TKEL), σ and σ(θ) for transfer channels, average number of nucleons transferred and transfer probabilities, N/Z ratios for multinucleon transfer reactions. Time-dependent Hartree-Fock (TDHF) calculations. Comparison with experimental data, and with other calculations.
doi: 10.1103/PhysRevC.88.014614
2012IN02 Prog.Theor.Phys.(Kyoto), Suppl. 196, 365 (2012) T.Inakura, T.Nakatsukasa, K.Yabana Shell and Neutron-Skin Effects on Pygmy Dipole Resonances NUCLEAR STRUCTURE Z=16-40; calculated low-lying dipole resonances, pygmy dipole resonances, E1 strengths. 68,84Ni; Comparison with available data.
doi: 10.1143/PTPS.196.365
2012YA06 Phys.Rev. C 85, 055803 (2012) Imaginary-time method for the radiative capture reaction rate NUCLEAR REACTIONS 16O(α, γ)20Ne, E at kT<1000 MeV; calculated radiative capture rate as function of inverse temperature. Spectral representation of Hamiltonian, solution of time-dependent Schrodinger equation in imaginary-time axis. Comparison with calculation using ordinary method.
doi: 10.1103/PhysRevC.85.055803
2011EB04 J.Phys.:Conf.Ser. 312, 092023 (2011) S.Ebata, T.Nakatsukasa, K.Yabana Linear response calculation using the canonical-basis TDHFB with a schematic pairing functional NUCLEAR STRUCTURE 18,20,22,24,26,28Mg; calculated quadrupole deformation parameters, pairing gaps, chemical potentials, E1 strength distribution.
doi: 10.1088/1742-6596/312/9/092023
2011IN02 Phys.Rev. C 84, 021302 (2011) T.Inakura, T.Nakatsukasa, K.Yabana Emergence of pygmy dipole resonances: Magic numbers and neutron skins NUCLEAR STRUCTURE 20,22,24,26,28,30,32,34Ne, 40,42,44,46,48,50,52,54,56,58,60Ca; calculated photoabsorption cross sections. Z=8-40, N=8-82; calculated fraction of photoabsorption cross section of pygmy dipole resonances (PDR) for even-even spherical and deformed nuclei. Z=16-40, N=16-82; calculated correlations between fraction of photoabsorption cross section of pygmy dipole resonances (PDR) and neutron skin thickness for even-even nuclei. B(E1) strengths. Random-phase approximation (RPA) calculations with the Skyrme functional SkM* using finite amplitude method (FAM).
doi: 10.1103/PhysRevC.84.021302
2010EB01 Phys.Rev. C 82, 034306 (2010) S.Ebata, T.Nakatsukasa, T.Inakura, K.Yoshida, Y.Hashimoto, K.Yabana Canonical-basis time-dependent Hartree-Fock-Bogoliubov theory and linear-response calculations NUCLEAR STRUCTURE 20,22,24,26,28,30,32Ne, 24,26,28,30,32,34,36,38,40Mg; calculated quadrupole deformation parameters, pairing gaps, chemical potentials, E1 and isoscalar quadrupole strength distributions, photoabsorption cross sections from equations derived from canonical-basis (Cb) formulation of the time-dependent Hartree-Fock-Bogoliubov (TDHFB) theory.
doi: 10.1103/PhysRevC.82.034306
2009IN03 Phys.Rev. C 80, 044301 (2009) T.Inakura, T.Nakatsukasa, K.Yabana Self-consistent calculation of nuclear photoabsorption cross sections: Finite amplitude method with Skyrme functionals in the three-dimensional real space NUCLEAR REACTIONS 16O(γ, X), E=0-50 MeV; 24Mg, 40Ca(γ, X), E=10-35 MeV; 90Zr, 120Sn, 208Pb(γ, X), E=5-25 MeV; calculated photoabsorption σ, transition density contour maps, GDR energies and widths using Finite Amplitude method with different Skyrme energy functionals in the 3-dimensional real space. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.044301
2009IN04 Int.J.Mod.Phys. E18, 2088 (2009) T.Inakura, T.Nakatsukasa, K.Yabana Response functions in the continuum of deformed nuclei studied with the time-dependent density-functional calculations NUCLEAR REACTIONS 16O, 24Mg, 28Si, 90Zr, 208Pb(γ, X), E<35 MeV; calculated photoabsorption σ, giant dipole resonance (GDR) peaks. Time-dependent density-functional theory (TDDFT).
doi: 10.1142/S0218301309014342
2009IN05 Eur.Phys.J. A 42, 591 (2009) T.Inakura, T.Nakatsukasa, K.Yabana Systematic study of electric-dipole excitations with fully self-consistent Skyrme HF plus RPA from light-to-medium-mass deformed nuclei NUCLEAR REACTIONS 16O, 24Mg, 28Si, 40Ca, 90Zr, 208Pb(γ, X), E<35MeV; calculated photoabsorption σ; analyzed deformation parameter. Finite amplitude method.
doi: 10.1140/epja/i2009-10811-9
2008NA08 Eur.Phys.J. Special Topics 156, 249 (2008) T.Nakatsukasa, K.Yabana, M.Ito Time-dependent approaches for reaction and response in unstable nuclei
doi: 10.1140\epjst/e2008-00622-2
2007IT05 Nucl.Phys. A787, 267c (2007) M.Ito, K.Yabana, T.Nakatsukasa, M.Ueda Fusion reaction of halo nuclei : A real-time wave-packet method for three-body tunneling dynamics NUCLEAR REACTIONS 209Bi(10Be, X), (11Be, X), E(cm)=36-50 MeV; 238U(α, X), (6He, X), E(cm)=14-32 MeV; calculated fusion σ. Three-body model, time-dependent wave-packet method to solve Schroedinger equation. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.12.042
2007NA19 Phys.Rev. C 76, 024318 (2007) T.Nakatsukasa, T.Inakura, K.Yabana Finite amplitude method for the solution of the random-phase approximation
doi: 10.1103/PhysRevC.76.024318
2007NA23 Nucl.Phys. A788, 349c (2007) Real-time Skyrme TDHF dynamics of giant resonances NUCLEAR STRUCTURE 8,14Be; calculated E1 strength distribution.
doi: 10.1016/j.nuclphysa.2007.01.064
2006IT04 Phys.Lett. B 637, 53 (2006) M.Ito, K.Yabana, T.Nakatsukasa, M.Ueda Suppressed fusion cross section for neutron halo nuclei NUCLEAR REACTIONS 209Bi(10B, X), (11B, X), E(cm)=30-50 MeV; 238U(α, X), (6He, X), E(cm)=14-32 MeV; calculated fusion σ. Three-body time-dependent wave-packet model, comparison with data.
doi: 10.1016/j.physletb.2006.03.027
2006SH22 Phys.Rev. C 74, 054315 (2006) S.Shinohara, H.Ohta, T.Nakatsukasa, K.Yabana Configuration mixing calculation for complete low-lying spectra with a mean-field Hamiltonian NUCLEAR STRUCTURE 12C, 16O, 20Ne; calculated levels, J, π, configurations. Extended mean-field approach, configuration mixing.
doi: 10.1103/PhysRevC.74.054315
2005IT03 Prog.Theor.Phys.(Kyoto) 113, 1047 (2005) Absorbing Kernels to Study Resonances in the Generator Coordinate Method NUCLEAR REACTIONS 6He(α, X), E(cm)=0-40 MeV; calculated total reaction σ, resonance parameters. Absorbing kernels, generator coordinate method.
doi: 10.1143/PTP.113.1047
2005NA06 Phys.Rev. C 71, 024301 (2005) Linear response theory in the continuum for deformed nuclei: Green's function vs time-dependent Hartree-Fock with the absorbing boundary condition NUCLEAR STRUCTURE 16O, 20Ne; calculated continuum strength functions. 16O; calculated continuum isovector GDR energies, energy-weighted sum rule. 8,10,12,14Be; calculated quadrupole deformation, electric dipole strength functions, energy-weighted sum rule. Linear response theory, continuum RPA, time-dependent Hartree-Fock.
doi: 10.1103/PhysRevC.71.024301
2005NA42 Eur.Phys.J. A 25, Supplement 1, 527 (2005) Unrestricted TDHF studies of nuclear response in the continuum NUCLEAR STRUCTURE 16O; calculated octupole strength distribution. 12,14Be; calculated dipole states energies, B(E1). Time-dependent Hartree-Fock theory.
doi: 10.1140/epjad/i2005-06-052-x
2005OH09 Eur.Phys.J. A 25, Supplement 1, 549 (2005) H.Ohta, T.Nakatsukasa, K.Yabana Light exotic nuclei studied with the parity-projected Hartree-Fock method NUCLEAR STRUCTURE 30,32,34Mg; calculated levels, J, π, deformation. Variation after projection.
doi: 10.1140/epjad/i2005-06-055-7
2004NA13 Eur.Phys.J. A 20, 163 (2004) Giant resonances in the deformed continuum NUCLEAR STRUCTURE 24Mg; calculated GDR features. Time-dependent Hartree-Fock theory, continuum effect.
doi: 10.1140/epja/i2002-10344-9
2004NA27 Prog.Theor.Phys.(Kyoto), Suppl. 154, 85 (2004) T.Nakatsukasa, K.Yabana, M.Ito, M.Kobayashi, M.Ueda Fusion Reaction of Halo Nuclei: Proton Halo versus Neutron Halo
doi: 10.1143/PTPS.154.85
2004OH06 Phys.Rev. C 70, 014301 (2004) H.Ohta, K.Yabana, T.Nakatsukasa Variation after parity projection calculation with the Skyrme interaction for light nuclei NUCLEAR STRUCTURE 12C, 20Ne; calculated levels, J, π, B(E2), matter density distributions; deduced cluster correlations. Self-consistent approach, Skyrme interaction, variation after parity projection.
doi: 10.1103/PhysRevC.70.014301
2004UE04 Nucl.Phys. A738, 288 (2004) M.Ueda, K.Yabana, T.Nakatsukasa Absorbing Boundary Condition Approach to Breakup Reactions of One-Neutron Halo Nuclei NUCLEAR REACTIONS 12C(11Be, n10Be), E=50, 67 MeV/nucleon; calculated fragments relative energy, σ(θ). Absorbing boundary condition method, comparison with data.
doi: 10.1016/j.nuclphysa.2004.04.047
2004YA19 Nucl.Phys. A738, 303 (2004) K.Yabana, M.Ito, M.Kobayashi, M.Ueda, T.Nakatsukasa Fusion reaction of halo nuclei: a time-dependent approach
doi: 10.1016/j.nuclphysa.2004.04.050
2003UE01 Phys.Rev. C 67, 014606 (2003) M.Ueda, K.Yabana, T.Nakatsukasa Application of an absorbing boundary condition to nuclear breakup reactions NUCLEAR REACTIONS 12C(16O, 16O), E=139.2 MeV; calculated elastic scattering matrix elements. 58Ni(d, np), E=80 MeV; calculated deuteron breakup matrix elements. Absorbing boundary condition method, comparison with coupled discretized continuum channels approach.
doi: 10.1103/PhysRevC.67.014606
2003YA17 Nucl.Phys. A722, 261c (2003) K.Yabana, M.Ueda, T.Nakatsukasa Time-dependent wave-packet approach for fusion reactions of halo nuclei NUCLEAR REACTIONS 208Pb(11Be, X), E=30-45 MeV; calculated wave-packet dynamics, fusion probability.
doi: 10.1016/S0375-9474(03)01375-7
2002MU20 Prog.Theor.Phys.(Kyoto) 108, 1065 (2002) A.Muta, J.-I.Iwata, Y.Hashimoto, K.Yabana Solving the RPA Eigenvalue Equation in Real-Space NUCLEAR STRUCTURE 16O, 20Ne; calculated level energies. Computational method for solution of RPA eigenvalue equation.
doi: 10.1143/PTP.108.1065
2002NA30 Prog.Theor.Phys.(Kyoto), Suppl. 146, 447 (2002) 3D Real-Space Calculation of the Continuum Response NUCLEAR STRUCTURE 8,10,12,14Be, 16O; calculated giant resonance strength functions.
doi: 10.1143/PTPS.146.447
2002YA19 Prog.Theor.Phys.(Kyoto), Suppl. 146, 329 (2002) K.Yabana, M.Ueda, T.Nakatsukasa Absorbing Boundary Condition Approach for Breakup Reactions of Halo Nuclei NUCLEAR REACTIONS 58Ni(d, d), E=80 MeV; calculated σ(θ). 12C(n, n), E=5-100 MeV; calculated σ. 12C(11Be, X), E=5-100 MeV/nucleon; calculated elastic breakup σ. Absorbing boundary condition approach, comparison with Eikonal approximation.
doi: 10.1143/PTPS.146.329
2001OG10 Prog.Theor.Phys.(Kyoto), Suppl. 142, 157 (2001) Y.Ogawa, T.Kido, K.Yabana, Y.Suzuki Microscopic Theories for the Reactions in Halo Nuclei NUCLEAR REACTIONS 1H, Be, C, 27Al, Cu, Pb(11Li, X), E=800 MeV/nucleon; calculated interaction σ, two-neutron removal σ. 12C(11Li, 9Li), E=800 MeV/nucleon; C(8B, 7BeX), E=1471 MeV/nucleon; calculated fragment longitudinal momentum distributions. 12C(11Li, X), E=10-200 MeV/nucleon; calculated reaction σ, breakup σ. Comparisons with data.
doi: 10.1143/PTPS.142.157
1999BE27 Nucl.Phys. A649, 423c (1999) Atomic Cluster with Nuclear Methods
doi: 10.1016/S0375-9474(99)00092-5
1998TA14 Phys.Lett. 431B, 242 (1998) Tetrahedral and Triangular Deformation of Z = N Nuclei in Mass Region A ∼ 60-80 NUCLEAR STRUCTURE 64Ge, 68Se, 72Kr, 76Sr, 80Zr, 84Mo; calculated non-axial deformation parameters, single-particle levels. Skyrme Hartree-Fock plus BCS method.
doi: 10.1016/S0370-2693(98)00545-0
1997YA07 Prog.Theor.Phys.(Kyoto) 97, 437 (1997) Low Energy Reactions of Halo Nuclei in a Three-Body Model NUCLEAR REACTIONS 40Ca(11Be, X), E=6-16 MeV; calculated transfer, breakup, fusion reaction probabilities; deduced neutron binding energy dependence. Three-body model.
doi: 10.1143/PTP.97.437
1996KI04 Phys.Rev. C53, 2296 (1996) Coulomb Breakup Mechanism of Neutron-Halo Nuclei in a Time-Dependent Method NUCLEAR REACTIONS 208Pb(11Be, X), E=72 MeV/nucleon; analyzed projectile Coulomb breakup data. Time-dependent Schrodinger equation.
doi: 10.1103/PhysRevC.53.2296
1996TA24 Prog.Theor.Phys.(Kyoto) 96, 407 (1996) Alpha Clustering of Light Nuclei in the Parity Projected Mean Field Method NUCLEAR STRUCTURE 20Ne, 4He, 8Be, 12C, 16O; calculated binding energies. 20Ne, 12C, 16O; calculated density distributions. Variation after parity projection approach.
doi: 10.1143/PTP.96.407
1995OG04 Nucl.Phys. A588, 77c (1995) Transverse Momentum Distributions of a 9Li Fragment in the (11Li, 9Li) Reaction and Neutron Correlations NUCLEAR REACTIONS 12C(11Li, 9Li), E=800 MeV/nucleon; calculated 9Li transverse, longitudinal momentum distributions; deduced halo neutron motion features. Glauber model, hybrid model wave function.
doi: 10.1016/0375-9474(95)00102-7
1995TA32 Prog.Theor.Phys.(Kyoto) 94, 1011 (1995) Deformations of Be Isotopes Studied with Skyrme Hartree-Fock Method NUCLEAR STRUCTURE 8,9,10,11,12,13,14Be; calculated binding energy, levels in some cases. 8,10,12,14Be; calculated density distribution; deduced deformation characteristics. Skyrme Hartee-Fock method.
doi: 10.1143/PTP.94.1011
1995YA09 Nucl.Phys. A588, 99c (1995) One Dimensional Three-Body Model for Low Energy Reactions of Halo Nuclei
doi: 10.1016/0375-9474(95)00106-B
1994KI12 Phys.Rev. C50, R1276 (1994) Coulomb Breakup Mechanism of Neutron Drip-Line Nuclei NUCLEAR REACTIONS 208Pb(11Be, X), E=72 MeV/nucleon; analyzed projectile Coulomb breakup σ vs E(relative) data; deduced projectile halo features. Time-dependent Schrodinger equation, three-dimensional space.
doi: 10.1103/PhysRevC.50.R1276
1994OG01 Nucl.Phys. A571, 784 (1994) Momentum Distributions of a 9Li Fragment Arising from the (11Li, 9Li) Reaction and Neutron Correlations NUCLEAR REACTIONS 12C(11Li, 9Li), E=800 MeV/nucleon; calculated 9Li longitudinal momentum distributions. Shell model plus di-neutron cluster model wave functions, Glauber theory.
doi: 10.1016/0375-9474(94)90720-X
1994SU02 Nucl.Phys. A567, 957 (1994) Y.Suzuki, T.Kido, Y.Ogawa, K.Yabana, D.Baye Fragmentation Cross Sections of He Isotopes and Neutron Correlations NUCLEAR REACTIONS 12C(6He, α), E=400 MeV/nucleon; calculated α-fragment momentum distribution. 9Be, C, 27Al, Cu, Pb(α, X), (6He, X), (8He, X), E=800 MeV/nucleon; calculated interaction, neutron removal σ. Glauber theory, projectile fragmentation.
doi: 10.1016/0375-9474(94)90336-0
1993SU04 Phys.Rev. C47, 1317 (1993) 11Li + p Elastic Scatterings in a Four-Body Model with the Eikonal Approximation NUCLEAR REACTIONS 11Li(p, p), E=62 MeV/nucleon; analyzed σ(θ); deduced target breakup, n-p interaction exchange force role. Four-body model, 11Li halo structure.
doi: 10.1103/PhysRevC.47.1317
1992OG02 Nucl.Phys. A543, 722 (1992) Glauber Model Analysis of the Fragmentation Reaction Cross Sections of 11Li NUCLEAR STRUCTURE 11Li, 9Be, 12C, 27Al, 63Cu, 208Pb; calculated point nucleon densities. Gaussian functions sum fitting. NUCLEAR REACTIONS 9Be, 12C, 27Al, Cu, Pb(11Li, X), E=800 MeV/nucleon; calculated reaction, two-neutron removal σ. Glauber model.
doi: 10.1016/0375-9474(92)90556-Y
1992YA02 Nucl.Phys. A539, 295 (1992) Reaction Mechanism of 11Li at Intermediate Energy NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; calculated elastic, breakup σ. Eikonal, coupled-discretized continuum channels models. 9Li, 12C(11Li, X), E ≈ 25-200 MeV/nucleon; calculated reaction σ(E).
doi: 10.1016/0375-9474(92)90272-L
1992YA04 Phys.Rev. C45, 2909 (1992) Break-Up Effect on the Elastic Scattering and the Optical Potential of 11Li NUCLEAR REACTIONS 58Ni(d, d), E=80 MeV; analyzed σ(θ). 12C(11Li, 11Li), E=60 MeV/nucleon; calculated σ(θ); deduced parameters, 11Li breakup role. Eikonal approximation, optical model with dynamic polarization potential.
doi: 10.1103/PhysRevC.45.2909
1991SU16 Phys.Lett. 272B, 173 (1991) Isobaric Analogue Halo States NUCLEAR STRUCTURE A=6, 8, 11, 12; calculated isospin multiplet level energies. 11Be; calculated level decay Γ into 9Li+p+n. Isobaric analog halo states.
doi: 10.1016/0370-2693(91)91814-C
1989YA10 Prog.Theor.Phys.(Kyoto) 82, 86 (1989) Effect of the Nucleus-Nucleus Potential on the High Energy Photon Production in the Intermediate Energy Heavy Ion Collision NUCLEAR REACTIONS 16O(α, X), E=40-100 MeV/nucleon; calculated high energy σ(Eγ, θγ). First chance nucleon-nucleon collision model.
doi: 10.1143/PTP.82.86
1989YA11 Prog.Theor.Phys.(Kyoto) 82, 75 (1989) S.Yamaguchi, K.Yabana, H.Horiuchi Microscopic Study of the Nucleus-Nucleus Interaction on the Basis of the Realistic Effective Interaction. II - Physical Consideration on the Effective Interaction and Comparison with Experiments in the α-α System - NUCLEAR REACTIONS 4He(α, α), E(cm) ≈ 0-60 MeV; calculated phase shifts vs E. Microscopic method, realistic effective interactions.
doi: 10.1143/PTP.82.75
1989YA15 Prog.Theor.Phys.(Kyoto) 82, 217 (1989) S.Yamaguchi, K.Yabana, H.Horiuchi Microscopic Study of the α-16O Interaction on the Basis of the Realistic Effective Interaction NUCLEAR REACTIONS 16O(α, α), E ≤ 100 MeV/nucleon; calculated complex potential parameters. Microscopic approach, effective interaction.
1989YA19 Prog.Theor.Phys.(Kyoto) 82, 1106 (1989) Microscopic Analysis of the Nucleus-Nucleus Optical Potential Based on the Feshbach Projection Operator Formalism. I - Formulation and Analysis of α-16O System - NUCLEAR REACTIONS 16O(α, α), E=20 MeV/nucleon; calculated potential parameters vs internuclear distance. Feshbach projection method, optical potential.
doi: 10.1143/PTP.82.1106
1988YA02 Prog.Theor.Phys.(Kyoto) 79, 19 (1988) Microscopic Derivation of the Nucleus-Nucleus Potential by the Use of the Density-Dependent Effective Interaction NUCLEAR REACTIONS 4He(α, α), E=20, 60 MeV; calculated potential parameters. Microscopic model, density dependent interactions.
doi: 10.1143/PTP.79.19
1986HO33 Prog.Theor.Phys.(Kyoto) 76, 837 (1986) Cranked Cluster Wave Function for Molecular States NUCLEAR REACTIONS 16O, 4He(α, α), 16O(16O, 16O), E not given; calculated potential energy vs ion-ion distance, critical angular momenta. Cranked cluster wave functions. NUCLEAR STRUCTURE 8Be, 32S, 20Ne; calculated rotational spectra. Cranked cluster wave function.
doi: 10.1143/PTP.76.837
1986YA15 Prog.Theor.Phys.(Kyoto) 76, 1071 (1986) Microscopic Analysis of Inelastic Coupling Potential Based on the Coupled Channel Resonating Group Method. I - Formulation and Study of 6Li-α System - NUCLEAR STRUCTURE 10B; calculated levels, J. Coupled-channel resonating group method, 6Li+α channel. NUCLEAR REACTIONS 6Li(α, α'), E(cm)=60, 100 MeV; calculated equivalent diagonal, coupling potentials, scattering matrix elements. Coupled-channel resonating group method.
doi: 10.1143/PTP.76.1071
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