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Search: Author = B.T.Kim

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
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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
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2000KI03      Phys.Rev. C61, 044611 (2000)

B.T.Kim, D.P.Knobles, S.A.Stotts, T.Udagawa

Antisymmetric Distorted Wave Impulse Approximation Calculations of Spin Transfer Cross Sections for (3He(pol), t(pol)) Reactions to the Continuum

NUCLEAR REACTIONS 12C, 90Zr(polarized p, n), (polarized 3He, t), E=200, 300 MeV/nucleon; calculated σ(θ=0°), spin transfer coefficients. DWIA, continuum Tamm-Dancoff method. Comparisons with data.

doi: 10.1103/PhysRevC.61.044611
Citations: PlumX Metrics

2000LE37      J.Korean Phys.Soc. 36, 13 (2000)

J.-Y.Lee, Y.-O.Lee, J.Chang, B.-T.Kim

Cross Sections for the Reaction 16O(γ, p3)15N* up to 120 MeV in the Continuum Random Phase Approximation

NUCLEAR REACTIONS 16O(γ, p), E=15-120 MeV; calculated σ, σ(θ=90°) for reaction leading to 3/2- state. Continuum RPA, comparison with data.

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)

S.W.Hong, B.T.Kim

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
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1998KI10      Nucl.Instrum.Methods Phys.Res. A402, 354 (1998)

B.T.Kim, T.Udagawa

Intermediate Energy Charge-Exchange Reactions Induced by Polarized 3He

NUCLEAR REACTIONS 12C(polarized p, n), (polarized 3He, t), E=200, 300 MeV/nucleon; calculated polarization transfer coefficients, σ(θ); deduced l=2 component.

doi: 10.1016/S0168-9002(97)00862-0
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1995IZ01      Phys.Rev. C51, 761 (1995)

T.Izumoto, T.Udagawa, B.T.Kim

Coupled-Channels Analyses of Scattering and Fusion Cross Sections of 16O + 152,154Sm, 186W Systems at Sub- and Near-Coulomb Barrier Energies

NUCLEAR REACTIONS, ICPND 152Sm(16O, 16O), (16O, 16O'), (16O, X), E=59-72 MeV; analyzed σ(θ), fusion σ(E). 154Sm(16O, X), E(cm)=53-73 MeV; 186W(16O, X), E=63-83 MeV; analyzed fusion σ(E); deduced models parameters. Coupled-channels approach.

doi: 10.1103/PhysRevC.51.761
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1992UD01      Phys.Rev. C45, 876 (1992)

T.Udagawa, M.Naito, B.T.Kim

Systematics of Sub- and Near-Barrier Fusion Cross Sections and the Threshold Anomaly

NUCLEAR REACTIONS 60Ni(16O, X), E(cm)=30-48 MeV; calculated fusion σ related parameter 'S' vs E; deduced threshold energy ambiguity.

doi: 10.1103/PhysRevC.45.876
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1991KI16      Phys.Lett. 273B, 37 (1991)

B.T.Kim, T.Udagawa

Dynamical Fusion and Direct Reaction Polarization Potentials for Heavy-Ion Scattering and Fusion at Sub-Coulomb-Barrier Energies

NUCLEAR REACTIONS 208Pb(16O, X), E=80 MeV; calculated absorption density vs radius, fusion, direct reaction. Dynamical polarization potential.

doi: 10.1016/0370-2693(91)90549-6
Citations: PlumX Metrics

1990KI03      Phys.Lett. 237B, 19 (1990)

B.T.Kim, M.Naito, T.Udagawa

Polarization Potentials in Heavy Ion Scattering and Fusion

NUCLEAR REACTIONS, ICPND 208Pb(16O, 16O), E=80-104 MeV; calculated σ(θ). 208Pb(16O, X), E=80-104 MeV; calculated total, fusion, reaction σ(E). Polarization potential.

doi: 10.1016/0370-2693(90)90453-D
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1990KI09      Phys.Rev. C42, 1147 (1990)

B.T.Kim, T.Udagawa

Method for Nonlocal Optical Model Calculations

NUCLEAR REACTIONS 208Pb(n, n), E=7, 14.5 MeV; 208Pb(16O, 16O), E=80 MeV; analyzed data. Nonlocal optical model, rapid solving method.

doi: 10.1103/PhysRevC.42.1147
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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
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1989UD02      Phys.Rev. C39, 1840 (1989)

T.Udagawa, T.Tamura, B.T.Kim

Simultaneous Analyses of Elastic Scattering and Fusion Cross Sections for the 32S + 58,64Ni Systems at Energies Near the Coulomb Barrier

NUCLEAR REACTIONS, ICPND 58,64Ni(32S, X), (32S, 32S), E=82-108 MeV; calculated σ(θ), fusion σ(E); deduced fusion potential radius, optical model parameters.

doi: 10.1103/PhysRevC.39.1840
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1989UD03      Phys.Rev. C40, 2271 (1989)

T.Udagawa, B.T.Kim

Random-Phase-Approximation Calculations of Nuclear Response in the Continuum

NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated energy weighted quadrupole transition strength RPA.

doi: 10.1103/PhysRevC.40.2271
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1989UD04      Phys.Lett. 230B, 6 (1989)

T.Udagawa, B.T.Kim

Continuum Random-Phase-Approximation Study of Direct Decay of Giant Monopole Resonances in 90Zr and 208Pb

NUCLEAR STRUCTURE 90Zr, 208Pb; calculated giant monopole resonance widths, EWSR strength distribution. Continuum RPA.

doi: 10.1016/0370-2693(89)91643-2
Citations: PlumX Metrics

1988KI01      Phys.Rev. C37, 998 (1988)

B.T.Kim, H.C.Kim, K.E.Park

Heavy-Ion Optical Potential for Sub-Barrier Fusion Deduced from a Dispersion Relation

NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E ≈ 75-135 MeV; calculated fusion σ(E); deduced optical potential parameters. Direct reaction model, fusion, dispersion relation.

doi: 10.1103/PhysRevC.37.998
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1987KI01      Phys.Rev. C35, 363 (1987)

K.H.Kim, M.H.Park, B.T.Kim

Radiative Capture Reaction 7Be(p, γ)8B at Low Energies

NUCLEAR REACTIONS, ICPND 7Be(p, γ), E ≤ 2.5 MeV; calculated σ(E), σ(θ), spectroscopic factors; deduced solar temperature astrophysical factor, d-wave capture role. Radiative direct capture model.

doi: 10.1103/PhysRevC.35.363
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1987KI12      Phys.Rev. C35, 1605 (1987)

B.T.Kim, D.Cha

28Si + 12C Fusion Reactions at High Energies

NUCLEAR REACTIONS, ICPND 28Si(12C, X), 24Mg(16O, X), 20Ne(20Ne, X), E(cm)=15-55 MeV; calculated fusion σ(E). Direct reaction model.

doi: 10.1103/PhysRevC.35.1605
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1987KI21      Phys.Rev. C36, 1626 (1987)


Dynamic Polarization Potential for Coupled-Channels Effects on the Heavy-Ion Fusion Reactions

NUCLEAR REACTIONS, ICPND 152Sm(16O, 16O), E=66, 72 MeV; calculated σ(θ). 152Sm(16O, X), E(cm) ≈ 55-70 MeV; calculated fusion σ(E). Dynamic polarization potential, coupled-channels effects.

doi: 10.1103/PhysRevC.36.1626
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1986KI01      Phys.Rev. C33, 370 (1986)

B.T.Kim, T.Udagawa, T.Tamura

Spin Distribution of Compound Nucleus Formed by Near-Barrier Fusion

NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E(cm)=55-70 MeV; 144Nd(16O, X), 123Sb(37Cl, X), 96Zr(64Ni, X), 80Se(80Se, X), E(cm)=50-60 MeV; calculated fusion σ(E), compound system <J>. Direct reaction approach.

doi: 10.1103/PhysRevC.33.370
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1986KI04      Phys.Rev. C33, 1270 (1986)

B.T.Kim, T.Udagawa, M.Benhamou, T.Tamura

Knockout and Knockout-Fusion Contributions to the (p, p')-Type Singles Cross Sections

NUCLEAR REACTIONS 54Fe, 27Al(p, p'), E=62 MeV; calculated σ(θ, Ep'); deduced knockout, knockout-fusion contributions. Multi-step formalism.

doi: 10.1103/PhysRevC.33.1270
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1985UD01      Phys.Rev. C32, 124 (1985)

T.Udagawa, B.T.Kim, T.Tamura

Direct Reaction Description of Sub- and Above-Barrier Fusion of Heavy Ions

NUCLEAR REACTIONS, ICPND 148,152Sm(16O, X), E(cm)=55-70 MeV; 122Sn(40Ar, X), E(cm)=90-120 MeV; 208Pb(16O, X), E(cm)=75-95 MeV; 40,44Ca(40Ca, X), E(cm)=48-66 MeV; 118Sn(64Ni, X), E(cm)=150-180 MeV; 124Sn(58Ni, X), E(cm)=155-200 MeV; 58,64Ni(58Ni, X), E(cm) ≈ 90-110 MeV; 90,94Zr, 96Mo, 104Ru(81Br, X), E(cm) ≈ 150-200 MeV; calculated fusion σ(E); deduced fusion radius parameters. Optical model, coupled-channels methods.

doi: 10.1103/PhysRevC.32.124
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1984KI08      Phys.Rev. C30, 1087 (1984)

B.T.Kim, T.Udagawa, T.Tamura

Microscopic Calculations of Knockout Reactions Induced by 6Li

NUCLEAR REACTIONS 28Si(6Li, 6Li'), E=156 MeV; calculated σ(θ, E(6Li)), σ(θ). Knockout mechanism.

doi: 10.1103/PhysRevC.30.1087
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1981CU02      Nucl.Phys. A355, 261 (1981)

A.Cunsolo, A.Foti, G.Imme, G.Pappalardo, G.Raciti, N.Saunier, B.T.Kim

Charge Exchange Reaction 14C(6Li, 6He)14N

NUCLEAR REACTIONS 14C(6Li, 6He), E=34, 62 MeV; measured σ(θ); deduced spin-isospin dependent effective interaction. One-step charge exchange DWBA analysis.

doi: 10.1016/0375-9474(81)90141-X
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1981KI01      Phys.Rev. C23, 33 (1981)

B.T.Kim, T.Izumoto, K.Nagatani

Radiative Capture Reaction 3He(α, γ)7Be at Low Energies

NUCLEAR REACTIONS 3He(α, γ), E(cm)=50-2000 keV; calculated σ(θ, E), γ-branching ratios. Orthogonality condition model, direct capture mechanism.

doi: 10.1103/PhysRevC.23.33
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1981ME10      Phys.Rev. C24, 1512 (1981)

M.C.Mermaz, A.Greiner, B.T.Kim, M.J.LeVine, E.Muller, M.Ruscev, M.Petrascu, M.Petrovici, V.Simion

Intermediate Structure and Statistical Fluctuations in the 12C + 24Mg System

NUCLEAR REACTIONS 24Mg(12C, 12C), (12C, 12C'), E(cm)=12-27 MeV; measured σ(θ, E); 12C(24Mg, 12C), E=70.8 MeV; measured σ(E(12C)). 36Ar deduced intermediate structure autocorrelation, cross correlation functions.

doi: 10.1103/PhysRevC.24.1512
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1979FE03      Nucl.Phys. A317, 511 (1979)

M.A.G.Fernandes, B.T.Kim, N.Lisbona, M.C.Mermaz

Coupled-Channel Analysis with Double-Folding Potential of 16O and 18O Scattering on Ni and Ge Isotopes

NUCLEAR REACTIONS 72,74,76Ge(16O, 16O), (16O, 16O'), (18O, 18O'), 64Ni(16O, 16O), (16O, 16O'), E=56 MeV; calculated σ(θ). Coupled-channel calculations, double-folding potential.

doi: 10.1016/0375-9474(79)90495-0
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1979KA27      Phys.Rev. C20, 2124 (1979)

S.Kahana, B.T.Kim, M.Mermaz

Single Particle Transfer Reactions and Backward Angle Elastic Scattering for the 15N, 16O + 28Si Systems

NUCLEAR REACTIONS 28Si(15N, 16O), (15N, 14N), E=44 MeV; calculated σ(θ). DWBA analysis, imaginary potential consistent with surface transparency.

doi: 10.1103/PhysRevC.20.2124
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1979KI01      Phys.Lett. 80B, 353 (1979)


Nuclear Excitation Effects on Heavy-Ion Scattering

NUCLEAR REACTIONS 152Sm(16O, 16O), (16O, 16O'), E=72 MeV; calculated σ(θ) using optical model, coupled-channel, DWBA analysis. 152Sm levels deduced deformation lengths. Compared with light-ion, electron scattering, Coulomb excitation.

doi: 10.1016/0370-2693(79)91188-2
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1979KI09      Phys.Rev. C20, 1396 (1979)

B.T.Kim, A.Greiner, M.A.G.Fernandes, N.Lisbona, K.S.Low, M.C.Mermaz

Heavy-Ion Charge Exchange Reaction 28Si(18O, 18F)28Al

NUCLEAR REACTIONS 28Si(18O, 18F), E=56 MeV; measured σ(θ); deduced strength of spin-isospin term of two-body force. Microscopic, second order DWBA, recoil effects.

doi: 10.1103/PhysRevC.20.1396
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1979ME04      Phys.Rev. C19, 794 (1979)

M.C.Mermaz, M.A.G.Fernandes, A.Greiner, B.T.Kim, N.Lisbona

Elastic and Inelastic Scattering of 16O and 18O on 28Si at 56 MeV Incident Energy

NUCLEAR REACTIONS 28Si(16O, 16O), (16O, 16O'), E=56 MeV; 28Si(18O, 18O), (18O, 18O'), E=56 MeV; measured σ(θ). Optical model, coupled-channel analysis.

doi: 10.1103/PhysRevC.19.794
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1979ME12      Phys.Rev. C20, 2130 (1979)

M.C.Mermaz, A.Greiner, B.T.Kim, M.A.G.Fernandes, N.Lisbona, E.Muller, W.Chung, B.H.Wildenthal

Multinucleon Transfer Reactions Induced by 18O on 28Si

NUCLEAR REACTIONS 28Si(18O, 16O), (18O, 20Ne), (18O, 22Ne), (18O, 15N), (18O, 15O), E=56 MeV; measured σ(θ). DWBA analysis; shell-model analysis.

doi: 10.1103/PhysRevC.20.2130
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1979UD01      Phys.Lett. 82B, 349 (1979)

T.Udagawa, T.Tamura, B.T.Kim

Analysis of Continuous Spectra of the Reactions (20Ne, 16O) and (20Ne, 12C) in Terms of Multi-Step Direct Reaction Theory

NUCLEAR REACTIONS 27Al(20Ne, 16O), (20Ne, 12C), E=120 MeV; calculated σ. Quantum mechanical, multistep direct reaction theory.

doi: 10.1016/0370-2693(79)90239-9
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1978PE13      Phys.Rev. C18, 2179 (1978)

J.C.Peng, B.T.Kim, M.C.Mermaz, A.Greiner, N.Lisbona

One and Two-Step Processes in Stripping and Pick-up Reactions Induced By 15N on 28Si

NUCLEAR REACTIONS 28Si(15N, 14N), (15N, 16O), E=44 MeV; measured σ(θ). 29Si, 27Al levels deduced S. DWBA, CCBA analysis.

doi: 10.1103/PhysRevC.18.2179
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1977KI01      Phys.Rev. C15, 818 (1977)

Byung-taik Kim

Coulomb Excitation Effect in the Reaction 144Nd(12C, 14C)142Nd

NUCLEAR REACTIONS 144Nd(12C, 14C), E=78 MeV; calculated σ(θ). CCBA analysis.

doi: 10.1103/PhysRevC.15.818
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1973KI09      Phys.Rev. C8, 1920 (1973)

B.T.Kim, W.K.Chu, J.C.Glass

Spin and Magnetic Moment of the 1.094-MeV State in 168Er

RADIOACTIVITY 168Tm; measured γγ(θ, H, t). 168Er level deduced T1/2, J, γ-mixing, g.

doi: 10.1103/PhysRevC.8.1920
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Note: The following list of authors and aliases matches the search parameter B.T.Kim: , B.T.KIM