NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = S.W.Hong Found 38 matches. 2022CH06 Nucl.Phys. A1018, 122374 (2022) V.Chavan, C.Ham, S.-I.Bak, V.Gore, E.J.In, D.Moon, S.Oh, B.Park, T.-S.Park, V.Bhoraskar, S.-W.Hong Monoenergetic neutrons from the 9Be(p, n)9B reaction induced by 35, 40 and 45-MeV protons NUCLEAR REACTIONS 9Be(p, n), E=35, 40, 45 MeV; 209Bi(n, 4n)206Bi, E<42 MeV; measured reaction products, En, In, Eγ, Iγ; deduced σ, neutron spectra. Comparison with the EXFOR library, TALYS calculations.
doi: 10.1016/j.nuclphysa.2021.122374
2021IN02 Int.J.Mod.Phys. E30, 2150009 (2021) E.J.In, P.Papakonstantinou, Y.Kim, S.-W.Hong Neutron drip line in the deformed relativistic Hartree-Bogoliubov theory in continuum: Oxygen to Calcium NUCLEAR STRUCTURE 22,23,24,25,26,27,28,29,30,31,32,33,34Ne, 26,27,28,29,30,31,32,33,34,35,36,37,38Mg, 30,31,32,33,34,35,36,37,38,39,40Si, 34,35,36,37,38,39,40,41,42S, 38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54Ar; calculated deformation parameters.
doi: 10.1142/S0218301321500099
2020PA21 Int.J.Mod.Phys. E29, 2050012 (2020) Effects of transient nonthermal particles on the big bang nucleosynthesis ATOMIC MASSES 1,2,3H, 3He, 6,7Li, 7Be; calculated ratios of abundances of elements.
doi: 10.1142/S0218301320500123
2018LE15 Eur.Phys.J. A 54, 173 (2018) J.Lee, C.-S.Gil, Y.-O.Lee, T.-S.Park, S.-W.Hong Calculation of fission product yields for uranium isotopes by using a semi-empirical model
doi: 10.1140/epja/i2018-12607-2
2015SH10 Nucl.Instrum.Methods Phys.Res. B349, 221 (2015) J.W.Shin, K.J.Min, C.Ham, T.-S.Park, S.-W.Hong Yield estimation of neutron-rich rare isotopes induced by 200 MeV/u 132Sn beams by using GEANT4 NUCLEAR REACTIONS 9Be(132Sn, X), E=200 MeV/nucleon; 9Be(59Co, X), E=80 MeV/nucleon;9Be(72Zn, X), E=95 MeV/nucleon;9Be(92Mo, X), E=500 MeV/nucleon; calculated yield of neutron-rich rare isotopes using GEANT4 code.
doi: 10.1016/j.nimb.2015.03.005
2013SH40 Phys.Rev. C 88, 035501 (2013) J.W.Shin, C.H.Hyun, S.-I.Ando, S.W.Hong Polarization of the neutron induced by hadronic weak interactions in the photodisintegration of the deuteron NUCLEAR REACTIONS 2H(γ, n)p, E=2-15 MeV; calculated polarization observables of neutrons in photodisintegration of deuteron. Pionless field effect theory. Implication on the understanding of hadronic weak interactions.
doi: 10.1103/PhysRevC.88.035501
2011BA48 J.Korean Phys.Soc. 59, 2071s (2011) S.I.Bak, T.-S.Park, S.-W.Hong, J.W.Shin, I.S.Hahn GEANT4 Simulation of the Shielding of Neutrons from 252Cf Source
doi: 10.3938/jkps.59.2071
2011SA54 J.Korean Phys.Soc. 59, 1111s (2011) Sang In Bak, R.Brun, Fe.Carminati, J.S.Chai, A.Gheata, M.Gheata, S.-W.Hong, Y.Kadi, V.Manchanda, T.-S.Park, C.Tenreiro A New Format for Handling Nuclear Data
doi: 10.3938/jkps.59.1111
2011SH41 J.Korean Phys.Soc. 59, 2022s (2011) J.W.Shin, T.-S.Park, S.W.Hong, J.K.Park, J.T.Kim, J.-S.Chai Estimates of SEU for Semiconductors Using MC50 Cyclotron and GEANT4 Simulation.
doi: 10.3938/jkps.59.2022
2010SO06 Phys.Rev. C 81, 047604 (2010) W.Y.So, T.Udagawa, K.S.Kim, S.W.Hong, B.T.Kim Characteristics of the polarization part of the optical potential for a weakly bound projectile, 9Be NUCLEAR REACTIONS 28Si(9Be, X), E=9.1, 10.6, 12.9, 15.1, 17.4, 19.7 MeV; 144Sm(9Be, X), E=31.1, 32.0, 32.9, 34.8, 36.7, 38.6 MeV; 208Pb(9Be, X), E=36.4, 38.3, 40.3, 42.2, 44.1, 47.9 MeV; calculated ratios of elastic to Rutherford σ, direct reaction (DR) σ and fusion σ. Extended optical model with the double-folding potential.
doi: 10.1103/PhysRevC.81.047604
2009HA09 Phys.Rev. C 79, 037301 (2009) Rotational energy term in the empirical formula for the yrast energies in even-even nuclei NUCLEAR STRUCTURE A=2-250; analyzed excitation energies of yrast 2+, 4+, 6+, 8+ and 10+ states in even-even nuclei in rotational-model formalism. Comparisons with experimental data.
doi: 10.1103/PhysRevC.79.037301
2009LE20 Phys.Rev. C 79, 064612 (2009) J.-Y.Lee, I.Hahn, Y.Kim, S.-W.Hong, S.Chiba, E.Sh.Soukhovitskii Optical potentials for nuclear level structures and nucleon interactions data of tin isotopes based on the soft-rotator model NUCLEAR STRUCTURE 116,118,120,122Sn; calculated levels, J, π and deformation parameters based on the soft rotor model. Comparison with experimental data. NUCLEAR REACTIONS 116,118,120,122Sn(n, n), (n, n'), E=9.95-24 MeV; 116,118,120,122Sn(p, p), (p, p'), E=9.7-156.0 MeV; analyzed σ, σ(θ), optical potential parameters using coupled-channels optical-model calculations. 120Sn(n, X), E=0.1-200 MeV; 120Sn(p, X), E=10-200 MeV; calculated total σ. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064612
2008SO02 Phys.Rev. C 77, 024609 (2008) W.Y.So, T.Udagawa, S.W.Hong, B.T.Kim Extended optical model analyses of elastic scattering and fusion cross section data for the 12C+208Pb system at near-Coulomb-barrier energies by using a folding potential NUCLEAR REACTIONS 208Pb(12C, X), E=50-120 MeV; 208Pb(6Li, X), E=20-80 MeV; analyzed cross sections.
doi: 10.1103/PhysRevC.77.024609
2007AN32 Phys.Rev. C 76, 064001 (2007) S.Ando, J.W.Shin, C.H.Hyun, S.-W.Hong Low energy proton-proton scattering in effective field theory NUCLEAR REACTIONS p(p, X), E not given; calculated scattering amplitudes using pionless effective field theory.
doi: 10.1103/PhysRevC.76.064001
2007RY05 Phys.Rev. C 75, 055804 (2007) C.Y.Ryu, C.H.Hyun, S.W.Hong, B.T.Kim Kaon condensation and composition of neutron star matter in a modified quark-meson coupling model
doi: 10.1103/PhysRevC.75.055804
2007SO03 Phys.Rev. C 75, 024610 (2007) W.Y.So, T.Udagawa, K.S.Kim, S.W.Hong, B.T.Kim Extended optical model analyses of elastic scattering and fusion cross sections for the 6Li+208Pb system at near-Coulomb-barrier energies using a folding potential NUCLEAR REACTIONS 208Pb(6Li, X), (6Li, 6Li), E(cm) ≈ 20-45 MeV; analyzed fusion σ, elastic σ(θ), related data; deduced polarization potential features. Extended optical model approach.
doi: 10.1103/PhysRevC.75.024610
2007SO13 Phys.Rev. C 76, 024613 (2007) W.Y.So, T.Udagawa, K.S.Kim, S.W.Hong, B.T.Kim Extended optical model analyses of elastic scattering and fusion cross section data for the 7Li+208Pb system at near-Coulomb-barrier energies using a folding potential NUCLEAR REACTIONS 208Pb(7Li, X), E not given; analyzed elastic scattering and fusion cross sections using the extended optical model.
doi: 10.1103/PhysRevC.76.024613
2006AN16 Phys.Rev. C 74, 025809 (2006) S.Ando, R.H.Cyburt, S.W.Hong, C.H.Hyun Radiative neutron capture on a proton at big-bang nucleosynthesis energies NUCLEAR REACTIONS 1H(n, γ), E(cm) ≈ 0-1 MeV; 2H(γ, n), E(cm) ≈ 0-1 MeV; calculated total σ. 2H(polarized γ, n), E ≈ 0-1 MeV; calculate analyzing power.
doi: 10.1103/PhysRevC.74.025809
2005HY01 Eur.Phys.J. A 24, 129 (2005) C.H.Hyun, S.J.Lee, J.Haidenbauer, S.W.Hong Parity-nonconserving observables in thermal neutron capture on a proton NUCLEAR REACTIONS 1H(n, γ), (polarized n, γ), E ≈ threshold; calculated parity-nonconserving polarization observables. Several models compared.
doi: 10.1140/epja/i2004-10131-8
2005RY01 Eur.Phys.J. A 24, 149 (2005) C.Y.Ryu, C.H.Hyun, S.W.Hong, B.K.Jennings Hadron masses in medium and neutron star properties
doi: 10.1140/epja/i2004-10133-6
2005RY05 Phys.Rev. C 72, 045206 (2005) C.Y.Ryu, C.H.Hyun, J.Y.Lee, S.W.Hong Effective mass and decay of Θ+ in nuclear matter by using the quark-meson coupling models
doi: 10.1103/PhysRevC.72.045206
2005SO16 Phys.Rev. C 72, 064602 (2005) W.Y.So, S.W.Hong, B.T.Kim, T.Udagawa Extended optical model analyses of elastic scattering, direct reaction, and fusion cross sections for the 9Be + 208Pb system at near-Coulomb-barrier energies NUCLEAR REACTIONS 208Pb(9Be, 9Be), (9Be, X), E=36-48 MeV; analyzed elastic σ(θ), fusion and direct-reaction σ. Extended optical model.
doi: 10.1103/PhysRevC.72.064602
2004SO15 Phys.Rev. C 69, 064606 (2004) W.Y.So, S.W.Hong, B.T.Kim, T.Udagawa Extended optical model analyses of elastic scattering and fusion cross sections for heavy-ion collisions with loosely bound projectiles at near-Coulomb-barrier energies NUCLEAR REACTIONS 208Pb(6Li, X), (6Li, 6Li), E(cm)=28-38 MeV; 209Bi(9Be, X), (9Be, 9Be), E(cm)=38-46 MeV; analyzed fusion, breakup, and elastic scattering σ, σ(θ); deduced direct reaction and fusion potential features. Extended optical model analysis.
doi: 10.1103/PhysRevC.69.064606
2004SO24 Prog.Theor.Phys.(Kyoto), Suppl. 154, 217 (2004) W.Y.So, S.W.Hong, B.T.Kim, T.Udagawa Optical Model Analyses of Elastic Scattering, Fusion, and Breakup Reaction Induced by Loosely Bound Nuclei NUCLEAR REACTIONS 208Pb(16O, X), (16O, 16O), E(cm)=80-102 MeV; 208Pb(6Li, X), (6Li, 6Li), E(cm)=28-38 MeV; 209Bi(9Be, X), (9Be, 9Be), E(cm)=38-47 MeV; 209Bi(6He, X), (6He, 6He), E(cm)=14-22 MeV; analyzed fusion, elastic, breakup σ; deduced polarization potential. Extended optical model.
doi: 10.1143/PTPS.154.217
2003HY04 Nucl.Phys. A718, 709c (2003) Effects of Meson Mass Reduction on the Properties of Neutron Star Matter
doi: 10.1016/S0375-9474(03)00896-0
2003SU02 J.Nucl.Sci.Technol.(Tokyo) 40, 69 (2003) E.Sh.Sukhovitsky, S.Chiba, J.-Y.Lee, B.-T.Kim, S.-W.Hong Analysis of Nucleon Scattering Data of 52Cr with a Coupling Scheme Built with the Soft-rotator Model NUCLEAR REACTIONS 52Cr(n, n), (n, n'), (p, p), (p, p'), E=7-200 MeV; analyzed total σ, σ(E, θ); deduced global optical model parameters. Coupled-channels model. NUCLEAR STRUCTURE 52Cr; analyzed levels, J, π; deduced parameters. Soft rotor model.
2002KI07 Phys.Rev. C65, 044607 (2002) B.T.Kim, W.Y.So, S.W.Hong, T.Udagawa Semiclassical Character and Optical Model Description of Heavy Ion Scattering, Direct Reactions, and Fusion at Near-Barrier Energies NUCLEAR REACTIONS 208Pb(16O, X), E=90 MeV; calculated elastic, direct reaction, and fusion probabilities. 208Pb(16O, X), E=80-110 MeV; calculated direct reaction and fusion σ. 208Pb(16O, 16O), E=80-102 MeV; calculated σ(θ). Optical model, comparisons with data.
doi: 10.1103/PhysRevC.65.044607
2002KI08 Phys.Rev. C65, 044616 (2002) B.T.Kim, W.Y.So, S.W.Hong, T.Udagawa Simultaneous Optical Model Analyses of Elastic Scattering, Breakup, and Fusion Cross Section Data for the 6He + 209Bi System at Near-Coulomb-Barrier Energies NUCLEAR REACTIONS 209Bi(6He, X), E(cm)=18.5, 21.9 MeV; calculated elastic, direct reaction, and fusion probabilities. 209Bi(6He, X), E(cm)=14-22 MeV; calculated direct reaction and fusion σ. 209Bi(6He, 6He), E=14.3-21.4 MeV; calculated σ(θ). Optical model, comparisons with data.
doi: 10.1103/PhysRevC.65.044616
2002KI14 Eur.Phys.J. A 14, 239 (2002) K.S.Kim, M.K.Cheoun, S.W.Hong, Y.Chung Contribution of the Δ(1232) to the (e, e'p) Reaction Along with Coulomb Distortion Effects NUCLEAR REACTIONS 40Ca(e, e'p), E=500 MeV; calculated σ(θ) for different proton shell numbers. DWBA results, effects of Δ(1232) discussed.
doi: 10.1140/epja/i2001-10123-2
2001HO29 Phys.Rev. C64, 038203 (2001) Quark-Meson Coupling Model for a Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated mass. Quark-meson coupling model.
doi: 10.1103/PhysRevC.64.038203
2000LE38 J.Korean Phys.Soc. 36, 323 (2000) J.-Y.Lee, Y.-O.Lee, J.Chang, S.-W.Hong, B.-T.Kim Differential Cross Sections for 12C(γ, p0) and 12C(γ, n0) in the Continuum Random Phase Approximation NUCLEAR REACTIONS 12C(γ, p), (γ, n), E=40-80 MeV; calculated σ(θ=90°); deduced particle-hole correlation contributions. Continuum RPA, comparisons with data.
1999HO13 J.Phys.(London) G25, 1065 (1999) Phenomenological Local Potentials for π- + 12C Scattering from 120 to 766 MeV NUCLEAR REACTIONS 12C(π-, π-), (π-, X), E=120-766 MeV; calculated elastic, total, reaction σ(θ), σ; deduced parameters. Phenomenological local Woods-Saxon potentials, Klein-Gordon equation. Comparisons with data.
doi: 10.1088/0954-3899/25/5/310
1994UD01 Phys.Rev. C49, 3162 (1994) T.Udagawa, P.Oltmanns, F.Osterfeld, S.W.Hong Δ Excitations in Nuclei and Their Decay Properties NUCLEAR REACTIONS 1H(p, nX), 12C(p, n), E=0.8 GeV; 1H(3He, tX), 12C(3He, t), E=2 GeV; calculated σ(θ, En), σ(θ, Et). 1H(polarized p, nX), E=0.8 GeV; calculated spin transfer coefficient. Formalism for Δ excitation.
doi: 10.1103/PhysRevC.49.3162
1991OS02 Nucl.Phys. A527, 405c (1991) F.Osterfeld, S.-W.Hong, T.Udagawa Spin-Isospin Response of Nuclei in the Δ Resonance Region NUCLEAR REACTIONS 12C(p, n), E=800 MeV; 12C(3He, t), E=2 GeV; calculated ejectile spectra, σ(θ, E); deduced isobar peak shift features.
doi: 10.1016/0375-9474(91)90130-X
1990UD01 Phys.Lett. 245B, 1 (1990) T.Udagawa, S.-W.Hong, F.Osterfeld Δ Excitations in Nuclei NUCLEAR REACTIONS 1H, 12C(p, nX), E=0.8 GeV; 1H, 12C(3He, tX), E=2 GeV; calculated σ(θ, E); deduced Δ excitations role. TDA, DWIA.
doi: 10.1016/0370-2693(90)90154-X
1989HO04 Nucl.Phys. A491, 492 (1989) S.-W.Hong, T.Udagawa, T.Tamura The Size of the Fusion Potential NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E=83-102 MeV; calculated σ(θ), fusion σ(E); deduced model parameters.
doi: 10.1016/0375-9474(89)90582-4
1989HO10 Phys.Rev. C39, 2061 (1989) S.-W.Hong, Y.J.Lee, B.T.Kim, D.Cha Macroscopic Theory of Heavy-Ion Fusion Reactions NUCLEAR REACTIONS, ICPND 28Si(28Si, X), 32S(24Mg, X), E(cm) ≈ 30-100 MeV; 40Ca(16O, X), E(cm) ≈ 28-100 MeV; calculated fusion σ(E). Macroscopic model.
doi: 10.1103/PhysRevC.39.2061
1985UD02 Phys.Rev. C32, 1435 (1985) T.Udagawa, S.-W.Hong, T.Tamura Direct Reaction Description of Complete Fusion above Barrier NUCLEAR REACTIONS, ICPND 40Ca(16O, X), E=39.4-214 MeV; calculated fusion σ(E); deduced fusion radius parameter. Energy-dependent optical model.
doi: 10.1103/PhysRevC.32.1435
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