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NSR database version of April 11, 2024.

Search: Author = H.C.Kim

Found 42 matches.

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2022JU01      Prog.Theor.Exp.Phys. 2022, 033D01 (2022)

Y.-S.Jun, H.-C.Kim, J.-Y.Kim, J.-M.Suh

Structure of the Ω baryon and the kaon cloud

doi: 10.1093/ptep/ptac028
Citations: PlumX Metrics

2021GH06      Phys.Rev. C 103, 064306 (2021)

N.-Y.Ghim, G.-S.Yang, H.-C.Kim, U.Yakhshiev

Baryonic matter and the medium modification of the baryon masses

NUCLEAR STRUCTURE 1H, 1n; calculated masses of the baryon octet and decuplet for proton, neutron, and Λ, Σ, Ξ, Δ and Ω baryons in free space and in different baryonic environments at normal nuclear matter density using meson mean-field approach or the generalized SU(3) chiral soliton model. Comparison with experimental masses. Relevance to properties of neutron stars.

doi: 10.1103/PhysRevC.103.064306
Citations: PlumX Metrics

2019HO05      Phys.Rev. C 99, 035212 (2019)

K.-H.Hong, U.Yakhshiev, H.-C.Kim

Modification of hyperon masses in nuclear matter

doi: 10.1103/PhysRevC.99.035212
Citations: PlumX Metrics

2018SI02      Prog.Theor.Exp.Phys. 2018, 023D01 (2018)

A.Silva, D.Urbano, H.-C.Kim

Flavor structure of the nucleon electromagnetic form factors and transverse charge densities in the chiral quark-soliton model

doi: 10.1093/ptep/ptx190
Citations: PlumX Metrics

2016HO12      Nucl.Phys. A954, 341 (2016)

A.Hosaka, E.Hiyama, S.H.Kim, H.-C.Kim, H.Nagahiro, H.Noumi, M.Oka, K.Shirotori, T.Yoshida, S.Yasui

Production and decay of charmed baryons

doi: 10.1016/j.nuclphysa.2016.05.009
Citations: PlumX Metrics

2015KI01      Phys.Rev. C 91, 014606 (2015)

K.S.Kim, M.-K.Cheoun, W.Y.So, H.C.Kim

Effects of density-dependent weak form factors on neutral-current neutrino (antineutrino)-nucleus scattering in the quasi-elastic region

NUCLEAR REACTIONS 12C(e, e'), E=2.02 GeV; calculated double differential σ as function of energy transfer, 12C(ν, ν'), (ν-bar, ν'-bar), E=0.5, 1.5 GeV; calculated differential, longitudinal and interference σ, and asymmetry as function of the kinetic energy of the knocked-out proton and neutron, flux-averaged differential cross sections; deduced effects of density-dependent form factors on the differential cross sections. Relativistic single-particle model, with the density-dependent weak form factors from a quark-meson coupling model. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.014606
Citations: PlumX Metrics

2015YA17      Phys.Rev. C 92, 035206 (2015)

G.-S.Yang, H.-C.Kim

Hyperon semileptonic decay constants with flavor SU(3) symmetry breaking

doi: 10.1103/PhysRevC.92.035206
Citations: PlumX Metrics

2014KI10      Few-Body Systems 55, 783 (2014)

H.-Ch.Kim, H.-Y.Ryu, A.Titov, A.Hosaka

φN photoproduction coupled with the K Λ* channel

doi: 10.1007/s00601-014-0883-6
Citations: PlumX Metrics

2011YA03      Phys.Rev. C 83, 038203 (2011)

U.Yakhshiev, H.-C.Kim

Binding energy per nucleon and hadron properties in nuclear matter

doi: 10.1103/PhysRevC.83.038203
Citations: PlumX Metrics

2008LE22      Nucl.Phys. A811, 353 (2008)

T.Ledwig, H.-C.Kim, K.Goeke

Vector transition form factors of the NK* → Θ+ and N(K-bar)* → Σ*-10-bar in the SU(3) chiral quark-solition model

doi: 10.1016/j.nuclphysa.2008.08.002
Citations: PlumX Metrics

2007GO33      Eur.Phys.J. A 32, 393 (2007)

K.Goeke, H.-C.Kim, A.Silva, D.Urbano

Strange nucleon form factors: Solitonic approach GsM, GsE, (G-∼)pA and (G-∼)nA and comparison with world data

doi: 10.1140/epja/i2006-10398-7
Citations: PlumX Metrics

2006CH21      Phys.Lett. B 636, 253 (2006)

K.-S.Choi, S.-I.Nam, A.Hosaka, H.-C.Kim

A new N*(1675) resonance in the γN → ηN reaction

NUCLEAR REACTIONS 1n, 1H(γ, X), E(cm)=1.4-1.9 GeV; calculated η production σ, resonance features. Effective Lagrangians and Born approximation, comparison with data.

doi: 10.1016/j.physletb.2006.03.058
Citations: PlumX Metrics

2006KI18      J.Korean Phys.Soc. 49, 1908 (2006)

H.-C.Kim, J.H.Yee

Dynamics of a Phase Transition in (3+1)-Dimensional Scalar φ4 Theory

2006NA04      Phys.Lett. B 633, 483 (2006)

S.-I.Nam, A.Hosaka, H.-C.Kim

Suppression of Θ+(JP = 3/2±)-photoproduction from the proton

NUCLEAR REACTIONS 1n, 1H(γ, X), E=1.73-2.10 GeV; calculated pentaquark production σ, σ(E, θ). Effective Langrangians, comparison with data.

doi: 10.1016/j.physletb.2005.12.059
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2006NA24      Phys.Rev. C 74, 025204 (2006)

S.-Il.Nam, A.Hosaka, H.-C.Kim

Pentaquark Θ+ production via γ N → (K-bar)*Θ+(3/2±)

NUCLEAR REACTIONS 1n, 1H(γ, X), E=2.5-3.5 GeV; calculated pentaquark production σ, σ(θ), asymmetry.

doi: 10.1103/PhysRevC.74.025204
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2006NA35      J.Korean Phys.Soc. 49, 1928 (2006)

S.Il.Nam, H.-C.Kim, A.Hosaka

Photo-Production of the Pentaquark Θ+ with Positive and Negative Parities

NUCLEAR REACTIONS 1n, 1H(γ, X), E=1.7-2.6 GeV; calculated pentaquark production σ. 1n, 1H(γ, X), E(cm)=2.1 GeV; calculated pentaquark production σ(θ).

2006SI29      Phys.Rev. D 74, 054011 (2006)

A.Silva, H.-C.Kim, D.Urbano, K.Goeke

Parity-violating asymmetries in elastic (e(pol)p) scattering in the chiral quark-soliton model: Comparison with the A4, G0, HAPPEX and SAMPLE experiments

NUCLEAR REACTIONS 1H(polarized e, e), E=high; analyzed parity-violating asymmetries. Chiral quark-soliton model.

doi: 10.1103/PhysRevD.74.054011
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2005KI12      Nucl.Phys. A755, 419c (2005)

H.-Ch.Kim, Gh.-S.Yang, M.Praszalowicz, K.Goeke

Magnetic moments of exotic pentaquark baryons

doi: 10.1016/j.nuclphysa.2005.03.133
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2005LE09      Eur.Phys.J. A 24, Supplement 2, 105 (2005)

H.-J.Lee, C.H.Hyun, C.-H.Lee, H.-C.Kim

Strangeness-conserving effective weak chiral Lagrangian

doi: 10.1140/epjad/s2005-04-024-0
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2005NA24      Nucl.Phys. A755, 423c (2005)

S.I.Nam, A.Hosaka, H.Ch.Kim

Determination of the parity of the pentaquark baryons : Θ+ and Ξ5

NUCLEAR REACTIONS 1H(polarized p, Σ+X), (K0, X), E(cm) ≈ 2.7-2.8 GeV; calculated pentaquark production σ, σ(θ), dependence on parity.

doi: 10.1016/j.nuclphysa.2005.03.049
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2005SI04      Eur.Phys.J. A 24, Supplement 2, 93 (2005)

A.Silva, D.Urbano, H.-C.Kim, K.Goeke

Strange form factors of the nucleon in the chiral quark-soliton model

NUCLEAR STRUCTURE 1n, 1H; calculated strange form factors. Chiral quark-soliton model.

doi: 10.1140/epjad/s2005-04-020-4
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2005YA23      Phys.Lett. B 628, 33 (2005)

U.T.Yakhshiev, M.M.Musakhanov, H.-Ch.Kim

Is there a crystalline state of nuclear matter?

doi: 10.1016/j.physletb.2005.09.029
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2004NA31      Phys.Lett. B 602, 180 (2004)

S.-I.Nam, A.Hosaka, H.-C.Kim

Threshold production of the Θ+ in a polarized proton reaction

NUCLEAR REACTIONS 1H(polarized p, X), E(cm)=2.72-2.82 GeV; calculated pentaquark production σ, σ(θ), analyzing powers.

doi: 10.1016/j.physletb.2004.09.035
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2004NA41      Phys.Rev. D 70, 114027 (2004)

S-Il.Nam, A.Hosaka, H.-C.Kim

Production of the pentaquark Θ+ in np scattering

NUCLEAR REACTIONS 1H(n, X), E(cm)=2.6-3.5 GeV; calculated hyperon, pentaquark production σ, σ(θ). Effective chiral Langrangians.

doi: 10.1103/PhysRevD.70.114027
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2004SI31      Eur.Phys.J. A 22, 481 (2004)

A.Silva, H.-Ch.Kim, K.Goeke

Strange and singlet form factors of the nucleon: Predictions for G0, A4, and HAPPEX II experiments

NUCLEAR STRUCTURE 1n, 1H; calculated electric and magnetic form factors. SU(3) chiral quark-soliton model.

doi: 10.1140/epja/i2003-10240-x
Citations: PlumX Metrics

2003SI18      Nucl.Phys. A721, 417c (2003)

A.Silva, H.-C.Kim, K.Goeke

Strange vector form factors in the context of the SAMPLE, A4, HAPPEX and G0 experiments

NUCLEAR STRUCTURE 1n, 1H; analyzed strange form factors, related data.

doi: 10.1016/S0375-9474(03)01086-8
Citations: PlumX Metrics

2002FR03      Nucl.Phys. A699, 541 (2002)

M.Franz, H.-C.Kim, K.Goeke

ΔS = 1, 2 Effective Weak Chiral Lagrangian from the Instanton Vacuum

doi: 10.1016/S0375-9474(01)01275-1
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2001KI32      Nucl.Phys. A691, 403c (2001)

H.-C.Kim, M.Praszalowicz, K.Goeke

Hyperon Semileptonic Decay Constants and Quark-Spin Content of the Octet Baryons

doi: 10.1016/S0375-9474(01)01065-X
Citations: PlumX Metrics

2000FR09      Nucl.Phys. A663-664, 995c (2000)

M.Franz, H.-C.Kim, K.Goeke

Effective Weak Chiral Lagrangian from the Instanton Vacuum

doi: 10.1016/S0375-9474(99)00752-6
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2000KI12      Phys.Rev. D61, 114006 (2000)

H.-C.Kim, M.Praszalowicz, K.Goeke

Hyperon Semileptonic Decays and Quark Spin Content of the Proton

NUCLEAR STRUCTURE 1H, 1n; analyzed spin structure, hyperon semileptonic decays. 1H deduced quark content of spin. Chiral-quark soliton model calculations.

doi: 10.1103/PhysRevD.61.114006
Citations: PlumX Metrics

2000YA23      J.Korean Phys.Soc. 37, 512 (2000)

T.K.Yang, S.T.Park, B.K.Seo, H.C.Kim, D.W.Lee, G.D.Kim, S.Y.Lee, M.Igashira

Lifetimes of Excited Levels in 32S from the Doppler Shift Attenuation Method

NUCLEAR REACTIONS 31P(p, γ), E=1.557, 1.583 MeV; measured Eγ, Iγ, DSA. 32S levels deduced T1/2.

1998BR32      Phys.Lett. 438B, 242 (1998)

W.Broniowski, M.Polyakov, H.-C.Kim, K.Goeke

Tensor Susceptibilities of the Vacuum from Constituent Quarks

doi: 10.1016/S0370-2693(98)01048-X
Citations: PlumX Metrics

1997KI05      Nucl.Phys. A616, 606 (1997)

H.-C.Kim, T.Watabe, K.Goeke

Strange Vector Form Factors of the Nucleon in the SU(3) Chiral Quark-Soliton Model with the Proper Kaon Cloud

doi: 10.1016/S0375-9474(96)00486-1
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1997KI26      Phys.Rev. D55, 5698 (1997)

H.-C.Kim, M.V.Polyakov, K.Goeke

Weak Electricity of the Nucleon in the Chiral Quark-Soliton Model

NUCLEAR STRUCTURE 1n, 1H; calculated pseudotensor constant. Chiral Quark-Soliton model.

doi: 10.1103/PhysRevD.55.5698
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1996KI02      Nucl.Phys. A596, 415 (1996)

H.-C.Kim, A.Blotz, C.Schneider, K.Goeke

Strangeness in the Scalar Form Factor of the Nucleon

doi: 10.1016/0375-9474(95)00404-1
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1996KI03      Nucl.Phys. A598, 379 (1996)

H.-C.Kim, M.V.Polyakov, A.Blotz, K.Goeke

Magnetic Moments of the SU(3) Octet Baryons in the Semibosonized SU(3) Nambu-Jona-Lasinio Model

NUCLEAR STRUCTURE 1,1n; calculated μ vs constituent quark mass. Framework of SU(3) semibosonized Nambu-Jona-Lasinio model.

doi: 10.1016/0375-9474(95)00506-4
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1996RE20      Nucl.Phys. A608, 243 (1996)

A.Reuber, K.Holinde, H.-C.Kim, J.Speth

Correlated ππ and K(K-bar) Exchange in the Baryon-Baryon Interaction

doi: 10.1016/S0375-9474(96)00256-4
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1995HO07      Nucl.Phys. A585, 149c (1995)

K.Holinde, H.-C.Kim, A.Reuber, J.Speth

Correlated Two-Pion Exchange in the Hyperon-Nucleon System

doi: 10.1016/0375-9474(94)00558-5
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1994KI05      Phys.Rev. C49, 2355 (1994)

H.-C.Kim, J.W.Durso, K.Holinde

Dynamical Model for Correlated Two-Pion Exchange in the NN Interaction

NUCLEAR REACTIONS 1n(p, p), E ≤ 300 MeV; calculated phase shifts vs E. Correlated two-pion exchange in NN-interaction, dynamical model.

doi: 10.1103/PhysRevC.49.2355
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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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1964KI05      Nucl.Phys. 57, 526 (1964)

H.C.Kim, R.F.Seiler, D.F.Herring, K.W.Jones

Cross sections for the O16(d, p0)O17, O16(d, p1)O17* and O16(d, α0)N14 reactions from 0.8 to 1.7 MeV

NUCLEAR REACTIONS 16O(d, α), 16O(d, p), E=786 keV-1.7 MeV; measured products, 17O, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry C1438.

doi: 10.1016/0029-5582(64)90350-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1438.

1962EP01      Bull.Am.Phys.Soc. 7, No.8, 532, B5 (1962)

H.M.Epstein, H.C.Kim, V.A.Otte, D.F.Herring, K.W.Jones

Polarization of Neutrons from the N14(d, n0)O15 Reaction at 1.32 MeV

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.

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