NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = Y.Sugahara Found 10 matches. 1998OY01 Nucl.Phys. A634, 3 (1998) K.Oyamatsu, I.Tanihata, Y.Sugahara, K.Sumiyoshi, H.Toki Can the Equation of State of Asymmetric Nuclear Matter be Studied using Unstable Nuclei ( Question ) NUCLEAR STRUCTURE Z=10-90; calculated densities, neutron skin thickness. Sn; calculated neutron, proton diffuseness. 208,266Pb; calculated neutron, proton radial distributions. Comparison of parameter sets. Implications for asymmetric nuclear matter.
doi: 10.1016/S0375-9474(98)00125-0
1998TO16 J.Phys.(London) G24, 1479 (1998) H.Toki, H.Shen, K.Sumiyoshi, D.Hirata, Y.Sugahara, I.Tanihata Relativistic Many-Body Theory for Unstable Nuclei and Astrophysics
doi: 10.1088/0954-3899/24/8/023
1997HI03 Nucl.Phys. A616, 438c (1997) D.Hirata, K.Sumiyoshi, I.Tanihata, Y.Sugahara, T.Tachibana, H.Toki A Systematic Study of Even-Even Nuclei Up to the Drip Lines within the Relativistic Mean Field Framework NUCLEAR STRUCTURE Z=8-120; 94,96,98,100,102Zr; calculated binding energy per particle; A ≈ 80-220; calculated relative r-process abundances. Relativistic mean field theory.
doi: 10.1016/S0375-9474(97)00115-2
1997SH10 Phys.Rev. C55, 1211 (1997) Relativistic Mean Field Approach with Density Dependent Couplings for Finite Nuclei NUCLEAR STRUCTURE 16,22O, 40,48Ca, 90Zr, 124Sn, 208,214Pb; calculated binding energy per particle, charge radii. Relativistic mean field approach.
doi: 10.1103/PhysRevC.55.1211
1996OZ01 Nucl.Phys. A608, 63 (1996) A.Ozawa, I.Tanihata, T.Kobayashi, Y.Sugahara, O.Yamakawa, K.Omata, K.Sugimoto, D.Olson, W.Christie, H.Wieman Interaction Cross Sections and Radii of Light Nuclei NUCLEAR REACTIONS 9Be, C, 27Al(15B, 15B), (9C, 9C), (10C, 10C), (15C, 15C), (13N, 13N), (13O, 13O), (14O, 14O), (15O, 15O), E ≈ 730 MeV/nucleon; measured interaction σ. 15B, 9,10,15C, 13N, 13,14,15O deduced effective radii.
doi: 10.1016/0375-9474(96)00241-2
1996SU24 Prog.Theor.Phys.(Kyoto) 96, 1165 (1996) Y.Sugahara, K.Sumiyoshi, H.Toki, A.Ozawa, I.Tanihata Study of Light Nuclei in the Relativistic Mean Field Theory and the Non-Relativistic Skyrme-Hartree-Fock Theory NUCLEAR STRUCTURE 3,4,5,6,7,8,9,10He, 6,7,8,9,10,11,12,13,14Be, 8,9,10,11,12,13,14,15,16,17,18,19,20,21,22C; calculated binding energies, matter radii. Comparison with data. Relativistic mean field, Skyrme-Hartree-Fock theories.
doi: 10.1143/PTP.96.1165
1995TO06 Nucl.Phys. A588, 357c (1995) H.Toki, D.Hirata, Y.Sugahara, K.Sumiyoshi, I.Tanihata Relativistic Many Body Approach for Unstable Nuclei and Supernova NUCLEAR STRUCTURE A=10-270; calculated binding energy per nucleon vs mass, proton, neutron radii for proton magic nuclei. Relativistic many body approach.
doi: 10.1016/0375-9474(95)00161-S
1994SU16 Nucl.Phys. A579, 557 (1994) Relativistic Mean-Field Theory for Unstable Nuclei with Non-Linear σ and (Omega) Terms NUCLEAR STRUCTURE A=8-80; A=30-270; calculated binding energy per particle, proton, neutron rms radii; deduced model parameters. Relativistic mean field theory.
doi: 10.1016/0375-9474(94)90923-7
1994SU34 Prog.Theor.Phys.(Kyoto) 92, 803 (1994) Relativistic Mean Field Theory for Lambda Hypernuclei and Neutron Stars NUCLEAR STRUCTURE 89Y, 51V, 40Ca, 32S, 28Si, 16O, 13,12C, 9Be; calculated lambda single particle states binding energy, hypernuclei, neutron stars; deduced sensitivity to lambda-omega tensor coupling strength in both cases. Relativistic mean field theory.
doi: 10.1143/ptp/92.4.803
1991TO03 Nucl.Phys. A524, 633 (1991) H.Toki, Y.Sugahara, D.Hirata, B.V.Carlson, I.Tanihata Properties of Nuclei Far from the Stability Line in the Relativistic Hartree Theory NUCLEAR STRUCTURE 12C, 16O, 40Ca, 90Zr; calculated binding energy per particle, p, n charge rms radii. 36,38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70Ca; calculated binding energy per particle, p, n charge rms radii, density distributions. Relativistic Hartree theory.
doi: 10.1016/0375-9474(91)90266-9
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