NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = C.H.Lee Found 47 matches. 2022CH07 Phys.Rev. C 105, 024306 (2022) Y.-B.Choi, C.-H.Lee, M.-H.Mun, Y.Kim Bubble nuclei with shape coexistence in even-even isotopes of Hf to Hg NUCLEAR STRUCTURE 152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256Hf, 156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258W, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260Os, 170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262Pt, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264Hg; calculated quadrupole deformation parameters. 256Hf, 258W, 260Os, 256W; calculated neutron, proton and total nuclear densities. 196,208Os; calculated single-particle energy levels, J, π. 198,200,256Hf; calculated proton single-particle levels around the Fermi surface. Discussed the bubble structure and shape coexistence. Calculations based on deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) and relativistic continuum Hartree-Bogoliubov (RCHB) theory with spherical symmetry. Comparison with experimenatal values.
doi: 10.1103/PhysRevC.105.024306
2022KI19 Universe 8, 499 (2022) K.Kim, S.Jeon, C.-H.Lee, Y.Kim Nuclear Bubble Configuration in Heavy-Ion Collisions NUCLEAR REACTIONS 206Hg, 208Pb(206Hg, X), E=50, 100, 200 MeV/nucleon; analyzed available data; deduced the effects of a bubble configuration in a nucleus on heavy-ion collisions, π-/p+ ratio using the relativistic continuum Hartree-Bogoliubov theory and the DaeJeon-Boltzmann-Uehling-Uhlenbeck (DJBUU) transport model.
doi: 10.3390/universe8100499
2021CO10 Phys.Rev. C 104, 024603 (2021) M.Colonna, Y.-X.Zhang, Y.-J.Wang, D.Cozma, P.Danielewicz, C.M.Ko, A.Ono, M.B.Tsang, R.Wang, H.Wolter, J.Xu, Z.Zhang, L.-W.Chen, H.-G.Cheng, H.Elfner, Z.-Q.Feng, M.Kim, Y.Kim, S.Jeon, C.-H.Lee, B.-A.Li, Q.-F.Li, Z.-X.Li, S.Mallik, D.Oliinychenko, J.Su, T.Song, A.Sorensen, F.-S.Zhang Comparison of heavy-ion transport simulations: Mean-field dynamics in a box
doi: 10.1103/PhysRevC.104.024603
2020KI06 Phys.Rev. C 101, 064614 (2020) M.Kim, S.Jeon, Y.-M.Kim, Y.Kim, C.-H.Lee Extended parity doublet model with a new transport code NUCLEAR REACTIONS 197Au(197Au, X), E=100, 400 MeV/nucleon; calculated radial density profile, Pauli blocking factor, transverse flow, rapidity and momentum distributions, neutron and proton effective masses and densities, and proton directed flow using extended parity doublet model with a new transport code DaeJeon Boltzmann-Uehling-Uhlenbeck (DJBUU). Comparison with experimental data from FOPI collaboration. Dynamical properties of heavy-ion collisions and box calculations of collisions and blocking.
doi: 10.1103/PhysRevC.101.064614
2020KI09 Eur.Phys.J. A 56, 157 (2020) Y.-M.Kim, K.Kwak, C.H.Hyun, Ha.Gil, C.-H.Lee Neutron star equation of state and tidal deformability with nuclear energy density functionals
doi: 10.1140/epja/s10050-020-00164-2
2020KI14 Int.J.Mod.Phys. E29, 2030007 (2020) M.Kim, C.-H.Lee, Y.-M.Kim, K.Kwak, Y.Lim, C.H.Hyun Neutron star equations of state and their applications NUCLEAR STRUCTURE 16,28O, 40,48,60Ca, 90Zr, 132Sn, 208Pb; calculated binding energies, charge radii and neutron skin from five selected Skyrme type models.
doi: 10.1142/S0218301320300076
2018KI19 Phys.Rev. C 98, 065805 (2018) Y.-M.Kim, Y.Lim, K.Kwak, C.H.Hyun, C.-H.Lee Tidal deformability of neutron stars with realistic nuclear energy density functionals
doi: 10.1103/PhysRevC.98.065805
2017KI05 Phys.Rev. C 96, 015201 (2017) Y.-M.Kim, C.-H.Lee, D.Teaney, I.Zahed Direct photon elliptic flow at energies available at the BNL Relativistic Heavy Ion Collider and the CERN Large Hadron Collider
doi: 10.1103/PhysRevC.96.015201
2016CH56 Sci. Rep. 6, 36144 (2016) Y.Cheng, S.-H.Yang, M.Lan, C.-H.Lee Observations on the long-lived Mossbauer effects of 93mNb RADIOACTIVITY 92,93Nb(IT), 182Ta(β-); measured decay products, X-rays; deduced X-ray spectra, a long-predicted coherence for all 93mNb excitation in the crystal, superradiance and 4γ model.
doi: 10.1038/srep36144
2014LE17 928, 296 (2014) Supercritical accretion in the evolution of neutron star binaries and its implications
doi: 10.1016/j.nuclphysa.2014.04.019
2014LE25 Phys.Rev. C 90, 025204 (2014) Electromagnetic radiation in hot QCD matter: Rates, electric conductivity, flavor susceptibility, and diffusion
doi: 10.1103/PhysRevC.90.025204
2014LI23 Phys.Rev. C 89, 055804 (2014) Y.Lim, K.Kwak, C.H.Hyun, C.-H.Lee Kaon condensation in neutron stars with Skyrme-Hartree-Fock models
doi: 10.1103/PhysRevC.89.055804
2011LE44 J.Korean Phys.Soc. 59, 2118s (2011) C.-H.Lee, H.-S.Cho, Y.M.Kim, H.-Y.Park Kaon Condensation in Neutron Stars and Related Astrophysical Issues
doi: 10.3938/jkps.59.2118
2011RY06 Phys.Rev. C 84, 035809 (2011) Hyperons and nuclear symmetry energy in neutron star matter
doi: 10.1103/PhysRevC.84.035809
2007BR03 Phys.Rep. 439, 161 (2007) G.E.Brown, J.W.Holt, C.-H.Lee, M.Rho Vector manifestation and matter formed in relativistic heavy-ion processes
doi: 10.1016/j.physrep.2006.12.002
2006BR02 Phys.Rev.Lett. 96, 062303 (2006) G.E.Brown, C.-H.Lee, H.-J.Park, M.Rho Strangeness Condensation by Expanding about the Fixed Point of the Harada-Yamawaki Vector Manifestation
doi: 10.1103/PhysRevLett.96.062303
2006BR16 Phys.Rev. C 74, 024906 (2006) Vector manifestation of hidden local symmetry, hadronic freedom, and the STAR ρ0/π- ratio NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; analyzed meson yield ratio; deduced hadronic freedom. Vector manifestation fixed-point scenario.
doi: 10.1103/PhysRevC.74.024906
2006PA45 Nucl.Phys. A774, 889 (2006) H.-J.Park, C.-H.Lee, G.E.Brown, M.Rho The Problem of Mass: Mesonic Bound States Above Tc NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV/nucleon; calculated neutral ρ-meson to negative pion ratio. Bielefeld lattice gauge simulation. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.06.159
2005BR01 Nucl.Phys. A747, 530 (2005) Chemical equilibration in relativistic heavy ion collisions
doi: 10.1016/j.nuclphysa.2004.09.108
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
2005PA62 Nucl.Phys. A763, 197 (2005) H.-J.Park, C.-H.Lee, G.E.Brown The problem of mass: Mesonic bound states above Tc
doi: 10.1016/j.nuclphysa.2005.08.016
2004BR07 Phys.Rep. 391, 353 (2004) G.E.Brown, L.Grandchamp, C.-H.Lee, M.Rho Nature of the chiral restoration transition in QCD
doi: 10.1016/j.physrep.2003.10.009
2004BR32 Nucl.Phys. A740, 171 (2004) G.E.Brown, C.-H.Lee, M.Rho, E.Shuryak The (q-bar)q bound states and instanton molecules at T ≥ Tc
doi: 10.1016/j.nuclphysa.2004.04.116
2004BR37 J.Phys.(London) G30, S1275 (2004) G.E.Brown, C.-H.Lee, M.Rho, E.Shuryak The instanton molecule liquid and 'sticky molasses' above Tc
doi: 10.1088/0954-3899/30/8/107
1999LE07 Phys.Lett. 448B, 168 (1999) C.-H.Lee, J.Wirstam, I.Zahed, T.H.Hansson Thermal Dileptons from a Nonperturbative Quark-Gluon Phase NUCLEAR REACTIONS 197Au(S, X), (Pb, X), W(S, X), E=high; calculated dilepton yields; deduced quark-gluon plasma features. Fire ball model. Comparison with data.
doi: 10.1016/S0370-2693(99)00061-1
1999LE23 Nucl.Phys. A653, 185 (1999) C.-H.Lee, H.Yamagishi, I.Zahed Master Formulae Approach to Photon Fusion Reactions
doi: 10.1016/S0375-9474(99)00233-X
1999LI53 Nucl.Phys. (Supplement) A654, 523c (1999) Kaon Production in Heavy-Ion Collisions and Kaon Condensation in Neutron Stars NUCLEAR REACTIONS Ni(Ni, X), E=high; analyzed kaon production data; deduced in-medium properties. Implications for neutron stars discussed.
doi: 10.1016/S0375-9474(00)88492-4
1998BR24 Nucl.Phys. A639, 455c (1998) Stange Particles in Dense Matter and Kaon Condensates
doi: 10.1016/S0375-9474(98)00312-1
1998LE14 Phys.Rev. C57, 3488 (1998) C.-H.Lee, T.T.S.Kuo, G.Q.Li, G.E.Brown Nuclear Symmetry Energy
doi: 10.1103/PhysRevC.57.3488
1998LE32 Phys.Rev. C58, 2899 (1998) C.-H.Lee, H.Yamagishi, I.Zahed Dilepton and Photon Emission Rates from a Hadronic Gas. III NUCLEAR REACTIONS 197Au(S, X), (Pb, X), W(S, X), E=high; analyzed dilepton, photon emission rates; deduced hadron gas properties.
doi: 10.1103/PhysRevC.58.2899
1998LI30 Phys.Rev.Lett. 81, 2177 (1998) Li, Brown, and Lee Reply: Comment on 'Kaon production in heavy-ion collisions and maximum mass of neutron stars '
doi: 10.1103/PhysRevLett.81.2177
1997HA34 Phys.Rev. B55, 2687 (1997) J.K.Han, D.K.Oh, C.H.Lee, C.E.Lee, J.N.Kim, S.C.Kim 31P Nuclear-Magnetic-Relaxation Study of KTiOPO4 NUCLEAR MOMENTS 31P; measured NMR, spin-spin, spin-lattice relaxation; deduced phase transition in KTiOPO4.
doi: 10.1103/PhysRevB.55.2687
1997LE28 Phys.Lett. 412B, 235 (1997) C.-H.Lee, T.T.S.Kuo, G.Q.Li, G.E.Brown Momentum Dependence of Single Particle Potential in Dirac Brueckner Approach
doi: 10.1016/S0370-2693(97)01058-7
1997LI35 Nucl.Phys. A625, 372 (1997) Kaons in Dense Matter, Kaon Production in Heavy-Ion Collisions, and Kaon Condensation in Neutron Stars NUCLEAR REACTIONS Ni(Ni, X), E=1-2 GeV/nucleon; analyzed proton, pion, kaon rapidity, transverse mass distributions.
doi: 10.1016/S0375-9474(97)00489-2
1997LI37 Phys.Rev.Lett. 79, 5214 (1997) Kaon Production in Heavy-Ion Collisions and Maximum Mass of Neutron Stars NUCLEAR REACTIONS Ni(Ni, X), E=1, 1.8 GeV/nucleon; analyzed kaon spectra; deduced K- effective mass vs nuclear matter density, implications for neutron star mass.
doi: 10.1103/PhysRevLett.79.5214
1996LE10 Nucl.Phys. A602, 334 (1996) The Role of Λ(1405) in Kaon-Proton Interactions NUCLEAR REACTIONS 1H(K-, X), E ≈ threshold; calculated leading order contributions. 1H(K+, K+), E at ≤ 300 MeV/c; calculated S-wave phase shifts; deduced Λ(1405) role. Heavy-baryon chiral perturbation theory.
doi: 10.1016/0375-9474(96)00086-3
1996LE13 Phys.Rev. B53, 1896 (1996) C.H.Lee, C.E.Lee, J.-I.Jin, B.-K.Nam 1H NMR Study of Spin Dynamics in the I2-Doped PBMPV Conducting Polymers NUCLEAR MOMENTS 1H; measured NMR; deduced spin dynamics in I2-doped PBMPV conducting polymers.
doi: 10.1103/PhysRevB.53.1896
1995LE09 Nucl.Phys. A585, 401 (1995) C.-H.Lee, G.E.Brown, D.-P.Min, M.Rho An Effective Chiral Lagrangian Approach to Kaon-Nuclear Interactions. Kaonic Atom and Kaon Condensation
doi: 10.1016/0375-9474(94)00623-U
1994BR04 Nucl.Phys. A567, 937 (1994) G.E.Brown, C.-H.Lee, M.Rho, V.Thorsson From Kaon-Nuclear Interactions to Kaon Condensation
doi: 10.1016/0375-9474(94)90335-2
1994LE13 Phys.Lett. 326B, 14 (1994) C.-H.Lee, H.Jung, D.-P.Min, M.Rho Kaon-Nucleon Scattering from Chiral Lagrangians NUCLEAR REACTIONS 1H, 1n(K-, K-), E=high; calculated s-wave amplitude vs E. Scattering from chiral Lagrangians.
doi: 10.1016/0370-2693(94)91185-1
1994LE21 Phys.Lett. 335B, 266 (1994) Kaon Condensation in ' Nuclear Star ' Matter
doi: 10.1016/0370-2693(94)90348-4
1992WA23 J.Phys.(London) B25, 1385 (1992) C.W.Wang, Y.C.Yu, E.K.Lin, C.H.Lee, F.T.Chuang 3He Ion-Induced K X-Ray Emission Cross Section of Elements between Mn and Zn NUCLEAR REACTIONS Mn, Fe, Ni, Cu, Zn(3He, X), E=1.5-6 MeV; measured K X-ray production σ. Model comparison. ATOMIC PHYSICS Mn, Fe, Ni, Cu, Zn(3He, X), E=1.5-6 MeV; measured K X-ray production σ. Model comparison.
doi: 10.1088/0953-4075/25/7/010
1992YU03 J.Phys.Soc.Jpn. 61, 1939 (1992) Y.C.Yu, E.K.Lin, C.W.Wang, Y.M.Huang, C.H.Lee K-Shell Vacancy Production Cross Sections for Se, Br, Rb and Y Induced by 1.5 to 9.0 MeV 3He Ions NUCLEAR REACTIONS Se, Br, Rb, 89Y(3He, X), E=1.5-9 MeV; measured K X-ray production σ; deduced I(K(β))/I(K(α)). Model comparison. ATOMIC PHYSICS Se, Br, Rb, 89Y(3He, X), E=1.5-9 MeV; measured K X-ray production σ; deduced I(K(β))/I(K(α)). Model comparison.
1988LE18 Phys.Rev. C38, 1757 (1988); Erratum Phys.Rev. C39, 724 (1989) C.H.Lee, Y.W.Yu, D.Lee, H.Kudo, K.J.Moody, G.T.Seaborg Charge and Mass Distributions from the Reaction of 240 MeV 12C Ions with 238U NUCLEAR REACTIONS 238U(12C, F), E=240 MeV; measured fission fragment mass, charge distribution, yield vs mass; deduced formation σ for A=48-239. Radiochemistry techniques.
doi: 10.1103/PhysRevC.38.1757
1988LE21 J.Radioanal.Nucl.Chem. 123, 607 (1988) C.-H.Lee, C.-S.Chang, C.-C.Chen, Y.-W.Yu Computerized On-Line Measurement of the Yield of Short-Lived Bromine and Iodine Isotopes from Thermal Neutron Fission of 235U NUCLEAR REACTIONS 235U(n, F)86Br/134I/134mI/136I/136mI/137I/138I/87Br/88Br, E=thermal; measured Eγ, Iγ following fission; deduced fission products cumulative yields, 134,136I isomeric yield ratio.
doi: 10.1007/BF02034920
1987LE27 J.Radioanal.Nucl.Chem. 119, 101 (1987) C.H.Lee, L.T.Hwang, Y.S.Lin, Y.W.Yu Isomeric Yield Ratio of 146La and 84Br in the Thermal Neutron Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F)146La/146mLa/84Br/84mBr, E=thermal; measured fission product isomer yield ratio.
doi: 10.1007/BF02169838
1987YU01 Phys.Rev. C36, 2396 (1987) Y.W.Yu, C.H.Lee, K.J.Moody, H.Kudo, D.Lee, G.T.Seaborg Yield and Recoil Properties of Iodine Isotopes from the Interaction of 240 MeV 12C with 238U NUCLEAR REACTIONS 238U(12C, X)120I/121I/123I/124I/126I/128I/130I/131I/132I/132mI/133I/134I/135I, E=20 MeV/nucleon; measured residuals independent yields vs mass isotopic distribution; deduced production mechanism.
doi: 10.1103/PhysRevC.36.2396
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