NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = H.Kurasawa Found 23 matches. 2022KU07 Prog.Theor.Exp.Phys. 2022, 023D03 (2022) The mean-square radius of the neutron distribution in the relativistic and non-relativistic mean-field models NUCLEAR STRUCTURE 48Ca, 208Pb; calculated root msr of the point neutron and proton distributions with NL3, effective masses, the densities for neutrons and protons, neutron skin.
doi: 10.1093/ptep/ptac008
2021KU01 Prog.Theor.Exp.Phys. 2021, 013D02 (2021) The mean square radius of the neutron distribution and the skin thickness derived from electron scattering NUCLEAR REACTIONS 40,48Ca, 208Pb(e-, e-'), E not given; analyzed available data; calculated the second-order moment of the nuclear charge density, mean square radius of the point proton distribution, the fourth-order momentum, mean square radius of the point neutron distribution; deduced the skin thickness.
doi: 10.1093/ptep/ptaa177
2019KU20 Prog.Theor.Exp.Phys. 2019, 113D01 (2019) The nth-order moment of the nuclear charge density and contribution from the neutrons NUCLEAR STRUCTURE 40,48Ca, 208Pb; calculated mean square radius of the charge distribution, fourth-order moment of the charge distribution.
doi: 10.1093/ptep/ptz121
2006KU30 Int.J.Mod.Phys. E15, 1925 (2006) Roles of anti-nucleon degrees of freedom in relativistic nuclear models
doi: 10.1142/S0218301306005253
2005KU33 Prog.Theor.Phys.(Kyoto) 114, 805 (2005) H.Kurasawa, T.Suzuki, P.F.Bortignon Sum Rules of the Multiple Giant Resonance States
doi: 10.1143/PTP.114.805
2005MA12 Prog.Theor.Phys.(Kyoto) 113, 355 (2005) T.Maruyama, H.Kurasawa, T.Suzuki Role of the Landau-Migdal Parameters with the Pseudovector and Tensor Couplings in Relativistic Nuclear Models - The Quenching of the Gamow-Teller Strength -
doi: 10.1143/PTP.113.355
2004KU03 Phys.Rev. C 69, 014306 (2004) Energy-weighted and non-energy-weighted Gamow-Teller sum rules in the relativistic random phase approximation
doi: 10.1103/PhysRevC.69.014306
2004KU07 Nucl.Phys. A731, 114 (2004) H.Kurasawa, T.Suzuki, N.Van Giai The Gamow-Teller states and sum rule in relativistic models NUCLEAR STRUCTURE 48Sc; calculated Gamow-Teller strength for single-particle transitions, quenching due to relativistic effects.
doi: 10.1016/j.nuclphysa.2003.11.023
2004KU19 Yad.Fiz. 67, 1683 (2004); Phys.Atomic Nuclei 67, 1656 (2004) Effects of Dirac Sea on Giant Resonance States
doi: 10.1134/1.1802353
2003KU17 Phys.Rev.Lett. 91, 062501 (2003) H.Kurasawa, T.Suzuki, N.Van Giai Role of the Dirac Sea in the Quenching of Gamow-Teller Strength
doi: 10.1103/PhysRevLett.91.062501
2003KU41 Phys.Rev. C 68, 064311 (2003) H.Kurasawa, T.Suzuki, N.Van Giai Gamow-Teller states in relativistic nuclear models NUCLEAR STRUCTURE 48Ca; calculated Gamow-Teller strength distribution. Relativistic models.
doi: 10.1103/PhysRevC.68.064311
2000KU03 Phys.Lett. 474B, 262 (2000) Effects of the Dirac Sea on the Giant Monopole States
doi: 10.1016/S0370-2693(00)00046-0
2000KU32 Phys.Rev. C62, 054303 (2000) Effects of the Neutron Spin-Orbit Density on the Nuclear Charge Density in Relativistic Models NUCLEAR REACTIONS 40,48,52Ca(e, e), E=250 MeV; calculated σ(θ); deduced neutron spin-orbit density contribution, relativistic effect. Comparisons with data.
doi: 10.1103/PhysRevC.62.054303
1996KU02 Nucl.Phys. A597, 374 (1996) The Mean Energy, Strength and Width of the Double Giant Dipole States
doi: 10.1016/0375-9474(95)00483-1
1995KU40 Prog.Theor.Phys.(Kyoto) 94, 931 (1995) A Sum-Rule Constraint on the Soft Dipole Mode NUCLEAR STRUCTURE 11Li, 70Ca; calculated (αν), (βν) amplitude associated radii. 11Li deduced dipoles are distinct from soft mode.
doi: 10.1143/PTP.94.931
1990KU20 Prog.Theor.Phys.(Kyoto) 84, 1030 (1990) The (Omega)-Meson Mass and the Nucleon Size in Nuclei NUCLEAR STRUCTURE 1H; calculated rms charge radius; deduced omega-meson role.
doi: 10.1143/ptp/84.6.1030
1988KU10 Phys.Lett. 208B, 160 (1988) Modification of the Nucleon Size in Nuclei in the (σ-(Omega)) Model NUCLEAR STRUCTURE 1H; calculated radius vs baryon density, Sachs form factors.
doi: 10.1016/0370-2693(88)90410-8
1988KU28 Nucl.Phys. A490, 571 (1988) Effects of the Dirac Sea on the Coulomb Sum Value for Electron Scattering NUCLEAR REACTIONS 40Ca, 56Fe(e, e), E not given; calculated Coulomb sum values. RPA.
doi: 10.1016/0375-9474(88)90014-0
1988NI05 Phys.Lett. 209B, 6 (1988) S.Nishizaki, H.Kurasawa, T.Suzuki Nuclear Magnetic Moments and the Spin-Orbit Current in the Relativistic Mean Field Theory NUCLEAR STRUCTURE A=15, 17, 39, 41; calculated μ. Relativistic mean field theory.
doi: 10.1016/0370-2693(88)91818-7
1988NI08 Nucl.Phys. A485, 515 (1988) S.Nishizaki, T.Maruyama, H.Kurasawa, T.Suzuki Quasielastic Electron Scattering on 12C and 40Ca in the Relativistic Hartree Approximation Relativistic Corrections to the Resopnse Functions NUCLEAR REACTIONS 12C, 40Ca(e, e'), E ≈ 10-200 MeV; calculated longitudinal, transverse response functions, σ(θ(e'), E(e')). Relativistic Hartree approximation.
doi: 10.1016/0375-9474(88)90551-9
1986KU09 Phys.Lett. 173B, 377 (1986) The Coulomb Sum for Electron Scattering in the Relativistic Random Phase Approximation NUCLEAR REACTIONS 12C, 40Ca(e, e), E not given; calculated Coulomb sum value, longitudinal response function. Relativistic RPA.
doi: 10.1016/0370-2693(86)90398-9
1986NI03 Phys.Lett. 171B, 1 (1986) S.Nishizaki, H.Kurasawa, T.Suzuki Relativistic Hartree Response Function for Quasielastic Electron Scattering on 12C and 40Ca NUCLEAR REACTIONS 12C, 40Ca(e, e'), E not given; calculated response functions. Relativistic self-consistent Hartree approximation.
doi: 10.1016/0370-2693(86)90986-X
1984KU16 Phys.Lett. 144B, 151 (1984) Electroexitation of the New Magnetic Dipole States in Deformed Nuclei NUCLEAR REACTIONS 156Gd(e, e'), E not given; calculated transverse form factor; deduced low lying K=1+ state. RPA, deformed harmonic oscillator potential, isovector quadrupole-quadrupole force.
doi: 10.1016/0370-2693(84)91792-1
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