NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = H.Kim Found 222 matches. Showing 1 to 100. [Next]2023KI05 Phys.Rev. C 107, 024607 (2023) K.S.Kim, S.Choi, T.Miyatsu, M.-K.Cheoun, H.Kim, W.Y.So Quasielastic charged-current neutrino-nucleus scattering with relativistic nuclear models NUCLEAR REACTIONS 12C, 40Ar(ν, μ-), (ν-bar, μ+), E< GeV; calculated total σ, differential σ in term of energy loss, double differential σ in terms of the kinetic energy and polar angle of outgoing muon. Calculations with quantum hadrodynamics (QHD), the nonlinear σ (NL), the quark-meson coupling (QMC) and the chiral quark-meson coupling (QCMC) models. Comparison with experimental data from MiniBooNE, T2K, MicroBooNE and SciBooNE.
doi: 10.1103/PhysRevC.107.024607
2023TS02 Nucl.Instrum.Methods Phys.Res. A1046, 167666 (2023) P.Tsintari, G.Perdikakis, H.Y.Lee, S.A.Kuvin, A.Georgiadou, H.I.Kim, D.Votaw, L.Zavorka Implementation and validation of realistic (n, x) reaction yields in Geant4 utilizing a detailed evaluated nuclear reaction library below 20 MeV NUCLEAR REACTIONS 1H(n, n), 12C, 16O, 63Cu, 58Ni(n, α), 14N, 58Ni, 63Cu, 27Al(n, p), E<20 MeV; measured reaction products, En, In; deduced σ, yields. Comparison with Geant4 simulations. The Low Energy Neutron-induced charged-particle (Z) chamber (LENZ), at LANSCE.
doi: 10.1016/j.nima.2022.167666
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
2022KI04 Phys.Rev. C 105, 024606 (2022) K.S.Kim, S.Choi, M.-K.Cheoun, H.Kim Coulomb sum rule in the quasielastic region using various nuclear models NUCLEAR REACTIONS 12C, 56Fe(e-, e-'), E=2.02 GeV; 40Ca(e-, e-'), E=290, 545 MeV; 208Pb(e-, e-'), E=262, 485 MeV; calculated σ(θ), longitudinal and transverse structure functions, Coulomb sum rule. Rosenbluth separation with four different nuclear models: the relativistic Hartree model (QHD), the nonlinear sigma model, the quark-meson-coupling (QMC) model and the chiral QMC model. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.024606
2022KU12 Phys.Rev. C 105, 044608 (2022) S.A.Kuvin, H.Y.Lee, B.DiGiovine, C.Eiroa-Lledo, A.Georgiadou, M.Herman, T.Kawano, V.Mocko, S.Mosby, C.Vermeulen, D.Votaw, M.White, L.Zavorka, G.Perdikakis, P.Tsintari, H.I.Kim Direct measurement of 59Ni(n, p) 59Co and 59Ni(n, α)56Fe at fast-neutron energies from 500 keV to 10 MeV NUCLEAR REACTIONS 59Ni(n, p), (n, α), E=0.5-10 MeV; measured Ep, Ip, Eα, Iα, neutron time of flight, np-coin, nα-coin; deduced Q, inclusive and exclusive σ(E). Comparison to statistical Hauser-Feschbach calculations (TALYS, CoH3), evaluated data (ENDF/B-VIII.0, JEFF-3.3, JENDL-4.0) and other experimental results. Low Energy (n, z) (LENZ) setup consisting of annular double-sided silicon strip detectors at the WNR facility at the Los Alamos Neutron Science Center (LANSCE).
doi: 10.1103/PhysRevC.105.044608
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
2021YO11 J.Radioanal.Nucl.Chem. 330, 481 (2021) S.Yoon, H.Seo, Y.-S.Kim, C.Lee, H.-D.Kim Energy-dependent characteristics of prompt neutron anisotropic emission by 244Cm and 240Pu according to Monte Carlo simulations RADIOACTIVITY 252Cf, 244Cm, 240Pu(SF); calculated prompt neutrons from nuclear fissions using GEANT4 and FREYA codes.
doi: 10.1007/s10967-021-07893-8
2020KI03 Nucl.Instrum.Methods Phys.Res. A963, 163699(2020) H.I.Kim, H.Y.Lee, T.Kawano, A.Georgiadou, S.A.Kuvin, L.Zavorka, M.W.Herman New evaluation on angular distributions and energy spectra for neutron-induced charged-particle measurements
doi: 10.1016/j.nima.2020.163699
2020KU17 Phys.Rev. C 102, 024623 (2020) S.A.Kuvin, H.Y.Lee, T.Kawano, B.DiGiovine, A.Georgiadou, C.Vermeulen, M.White, L.Zavorka, H.I.Kim Nonstatistical fluctuations in the 35Cl(n, p)35S reaction cross section at fast-neutron energies from 0.6 to 6 MeV NUCLEAR REACTIONS 35Cl(n, p), (n, α), E=0.6-6 MeV spallation neutrons; measured charged particles from (n, p) and (n, α) reactions using the low energy LENZ experimental setup, flight path length using a sCVD diamond detector by measuring the neutron time of flight at the WNR facility of the Los Alamos Neutron Science Center (LANSCE); deduced Q value of the reaction from detected charged particle energy of the outgoing proton or α particle, and the corresponding neutron time-of-flight, σ(θ, E) for different reaction channels, angle-integrated partial cross section data for (n, p) and (n, α) channels. Comparison with statistical model HF calculation using the COH3 code, and Koning-Delaroche spherical optical potential and Kunieda coupled channel potential, and with evaluated cross section data in ENDF/B-VIII.0. 63Cu, 64Zn(n, p), (n, α), E=0.6-6 MeV; measured charged particles, σ(E) from the brass backing for background contributions, and to validate MCNP simulations using data from the present experiment, ENDF/B-VIII.0 evaluations, and from previous experiments.
doi: 10.1103/PhysRevC.102.024623
2020PL02 Eur.Phys.J. A 56, 181 (2020) A.J.M.Plompen, O.Cabellos, C.De Saint Jean, M.Fleming, A.Algora, M.Angelone, P.Archier, E.Bauge, O.Bersillon, A.Blokhin, F.Cantargi, A.Chebboubi, C.Diez, H.Duarte, E.Dupont, J.Dyrda, B.Erasmus, L.Fiorito, U.Fischer, D.Flammini, D.Foligno, M.R.Gilbert, J.R.Granada, W.Haeck, F.-J.Hambsch, P.Helgesson, S.Hilaire, I.Hill, M.Hursin, R.Ichou, R.Jacqmin, B.Jansky, C.Jouanne, M.A.Kellett, D.H.Kim, H.I.Kim, I.Kodeli, A.J.Koning, A.Yu.Konobeyev, S.Kopecky, B.Kos, A.Krasa, L.C.Leal, N.Leclaire, P.Leconte, Y.O.Lee, H.Leeb, O.Litaize, M.Majerle, J.I.Marquez Damian, F.Michel-Sendis, R.W.Mills, B.Morillon, G.Noguere, M.Pecchia, S.Pelloni, P.Pereslavtsev, R.J.Perry, D.Rochman, A.Rohrmoser, P.Romain, P.Romojaro, D.Roubtsov, P.Sauvan, P.Schillebeeckx, K.H.Schmidt, O.Serot, S.Simakov, I.Sirakov, H.Sjostrand, A.Stankovskiy, J.C.Sublet, P.Tamagno, A.Trkov, S.van der Marck, F.Alvarez-Velarde, R.Villari, T.C.Ware, K.Yokoyama, G.Zerovnik The joint evaluated fission and fusion nuclear data library, JEFF-3.3
doi: 10.1140/epja/s10050-020-00141-9
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
2018BE21 Eur.Phys.J. A 54, 81 (2018) R.Beyer, A.R.Junghans, P.Schillebeeckx, I.Sirakov, T.-Y.Song, D.Bemmerer, R.Capote, A.Ferrari, A.Hartmann, R.Hannaske, J.Heyse, H.I.Kim, J.W.Kim, T.Kogler, C.W.Lee, Yo.-O.Lee, R.Massarczyk, S.E.Muller, T.P.Reinhardt, M.Roder, K.Schmidt, R.Schwengner, T.Szucs, M.P.Takacs, A.Wagner, L.Wagner, S.-C.Yang The neutron transmission of natFe, 197Au and natW NUCLEAR REACTIONS 197Au, W(n, x), E=0.025-0.17 MeV; calculated transmission correction factor using MCNP. Fe, 197Au, W(n, x), E=0.15-8 MeV; measured reaction products using nELBE neutron ToF; deduced σ. Compared with other data (in a wider energy interval) and published calculations using optical model.
doi: 10.1140/epja/i2018-12505-7
2018CH12 Nucl.Data Sheets 148, 189 (2018) M.B.Chadwick, R.Capote, A.Trkov, M.W.Herman, D.A.Brown, G.M.Hale, A.C.Kahler, P.Talou, A.J.Plompen, P.Schillebeeckx, M.T.Pigni, L.Leal, Y.Danon, A.D.Carlson, P.Romain, B.Morillon, E.Bauge, F.-J.Hambsch, S.Kopecky, G.Giorginis, T.Kawano, J.Lestone, D.Neudecker, M.Rising, M.Paris, G.P.A.Nobre, R.Arcilla, O.Cabellos, I.Hill, E.Dupont, A.J.Koning, D.Cano-Ott, E.Mendoza, J.Balibrea, C.Paradela, I.Duran, J.Qian, Z.Ge, T.Liu, L.Hanlin, X.Ruan, W.Haicheng, M.Sin, G.Noguere, D.Bernard, R.Jacqmin, O.Bouland, C.De Saint Jean, V.G.Pronyaev, A.V.Ignatyuk, K.Yokoyama, M.Ishikawa, T.Fukahori, N.Iwamoto, O.Iwamoto, S.Kunieda, C.R.Lubitz, M.Salvatores, G.Palmiotti, I.Kodeli, B.Kiedrowski, D.Roubtsov, I.Thompson, S.Quaglioni, H.I.Kim, Y.O.Lee, U.Fischer, S.Simakov, M.Dunn, K.Guber, J.I.Marquez Damian, F.Cantargi, I.Sirakov, N.Otuka, A.Daskalakis, B.J.McDermott, S.C.van der Marck CIELO Collaboration Summary Results: International Evaluations of Neutron Reactions on Uranium, Plutonium, Iron, Oxygen and Hydrogen NUCLEAR REACTIONS 1H, 16O, 56Fe, 235,238U, 239Pu(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.003
2018KA01 Nucl.Instrum.Methods Phys.Res. A877, 328 (2018) S.Karki, P.Aryal, H.J.Kim, Y.D.Kim, H.K.Park Determination of Mo- and Ca-isotope ratios in 100CaO4 crystal for AMoRE-I experiment
doi: 10.1016/j.nima.2017.10.007
2018SI02 Prog.Theor.Exp.Phys. 2018, 023D01 (2018) Flavor structure of the nucleon electromagnetic form factors and transverse charge densities in the chiral quark-soliton model
doi: 10.1093/ptep/ptx190
2017CH33 Phys.Rev. C 96, 024311 (2017) S.Choi, Y.Zhang, M.-K.Cheoun, Y.Kwon, K.Kim, H.Kim Effects of pairing correlations on the neutron skin thickness and the symmetry energy NUCLEAR STRUCTURE 40,48Ca, 58,60,64Ni, 54,56,57Fe, 59Co, 90,96Zr, 106,116Cd, 112,116,120,124Sn, 122,124,126,128,130Te, 208Pb, 209Bi, 232Th, 238U; calculated neutron skin thickness (NST). 180,184,188,192,196,200,204,208,212Pb, 120,124,128,132,136,140,144,148,152Sn; calculated symmetry energies and asymmetry coefficients. 196Pb, 144Sn; calculated symmetry energy density distributions. Skyrme Hartree-Fock-Bogoliubov (HFB) model with SkI3, SLy4, SVI interactions and density-dependent δ interaction (DDDI) for the pairing force. Comparison of neutron skin thickness with experimental data from antiprotonic studies.
doi: 10.1103/PhysRevC.96.024311
2017KI12 Nucl.Phys. A968, 254 (2017) Wilson coefficients of dimension 6 gluon operators with spin indices in the heavy quark current correlation functions
doi: 10.1016/j.nuclphysa.2017.08.002
2017SI28 Eur.Phys.J. A 53, 199 (2017) I.Sirakov, R.Capote, O.Gritzay, H.I.Kim, S.Kopecky, B.Kos, C.Paradela, V.G.Pronyaev, P.Schillebeeckx, A.Trkov Evaluation of cross sections for neutron interactions with 238U in the energy region between 5 keV and 150 keV NUCLEAR REACTIONS 238U(n, x), E=5-150 keV; measured reaction products; deduced average total σ, average capture σ; calculated average total σ, average capture σ using dispersive coupled optical model and Hauser-Feshbach statistical theory with width fluctuations; deduced resonance parameters. Capture σ compared with ENDF/B-VII.1, JENDL-4, JEF-2.2, JEFF-3.2, JEFF-3.3T4 and data.
doi: 10.1140/epja/i2017-12394-2
2016HA43 IEEE trans.nucl.sci. 63, 1117 (2016) M.C.Han, HS.Kim, M.G.Pia, T.Basaglia, M.Batic, G.Hoff, C.H.Kim, P.Saracco Validation of Cross Sections for Monte Carlo Simulation of the Photoelectric Effect COMPILATION Z=1-92; compiled experimental atomic σ data; calculated total and partial photoionization σ.
doi: 10.1109/tns.2016.2521876
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
2016KI07 Eur.Phys.J. A 52, 107 (2016) K.S.Kim, M.-K.Cheoun, H.Kim, W.Y.So The effects of density-dependent form factors for (e, e'p) reaction in quasi-elastic region NUCLEAR REACTIONS 208Pb(e, e'p), E=412 MeV; calculated reduced dσ for knocked-out protons from different shells using relativistic single-particle model with density-dependent electromagnetic form-factors. Compared with NIKHEF data.
doi: 10.1140/epja/i2016-16107-1
2016KI10 Eur.Phys.J. A 52, 170 (2016) H.I.Kim, C.Paradela, I.Sirakov, B.Becker, R.Capote, F.Gunsing, G.N.Kim, S.Kopecky, C.Lampoudis, Y.-O.Lee, R.Massarczyk, A.Moens, M.Moxon, V.G.Pronyaev, P.Schillebeeckx, R.Wynants Neutron capture cross section measurements for 238U in the resonance region at GELINA NUCLEAR REACTIONS 238U(n, γ), E=0.5 eV - 300 keV; measured reaction products, yields vs neutron energy at GELINA ToF facility with C6D6 detectors; deduced transmission coefficients for s- and p-waves, neutron strength, neutron widths, resonance parameters below 1200 eV using REFIT code, average capture σ, dσ, covariance matrix; calculated σ, dσ using statistical code γDEX. Resultswere compared with other data and evaluations.
doi: 10.1140/epja/i2016-16170-6
2016KI13 Eur.Phys.J. A 52, 184 (2016) H.Kim, K.S.Kim, M.-K.Cheoun, D.Jido, M.Oka Testing the tetraquark structure for the X resonances in the low-lying region
doi: 10.1140/epja/i2016-16184-0
2016KI18 Phys.Rev. C 94, 064619 (2016) K.S.Kim, H.Kim, M.-K.Cheoun, W.Y.So Extraction of structure functions for lepton-nucleus scattering in the quasi-elastic region NUCLEAR REACTIONS 40Ca(e, e'), (ν, ν'), (ν-bar, ν-bar'), (ν, e-), E=200, 800 MeV; calculated σ(θ, E); deduced structure functions for inclusive reactions. Relativistic single-particle model.
doi: 10.1103/PhysRevC.94.064619
2015CH18 J.Phys.(London) G42, 345102 (2015) M.-K.Cheoun, K.S.Kim, H.Kim, W.Y.So, T.Maruyama, T.Kajino In-medium effect with muon-neutrino and anti-muon-neutrino quasi-elastic scattering from 12C nucleons
doi: 10.1088/0954-3899/42/4/045102
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
2015KI03 Nucl.Instrum.Methods Phys.Res. B349, 141 (2015) H.Kim, S.J.Noh, Y.-R.Kang, M.Lee, D.H.Jeong, J.K.Kim, K.Yang, T.-I.Ro, S.G.Shin, Y.U.Kye, M.-H.Cho, G.Kim Measurement of isomeric yield ratios in the photo-production of 133m, g;137m, gCe from natCe using 55-, 60-, and 65-MeV bremsstrahlung NUCLEAR REACTIONS Ce(γ, xn)133Ce/137Ce, E=55, 60, 65 MeV; measured reaction products, Eγ, Iγ; deduced isomeric yield ratios. Comparison with available data.
doi: 10.1016/j.nimb.2015.02.055
2015KI08 Phys.Rev. C 92, 044613 (2015) K.S.Kim, H.Kim, M.-K.Cheoun, G.-S.Yang, W.Y.So Influence of axial mass and strange axial form factor on neutrino-nucleus scattering in the quasielastic region NUCLEAR REACTIONS 12C(ν, ν'), (ν-bar, ν'-bar), E=0.5, 1.5 GeV; calculated differential cross sections as function of knocked-out neutron and proton kinetic energies, flux-averaged differential cross sections, asymmetry of flux-averaged differential cross sections, 12C(ν, μ-), (ν-bar, μ+), Q2<2 GeV/c2; calculated Flux-averaged differential cross sections, asymmetry of flux-averaged differential cross sections. Investigated effects of strange axial form factor (GA) and the axial mass (AM) within the framework of relativistic single-particle model. Comparison with MiniBooNE experimental data.
doi: 10.1103/PhysRevC.92.044613
2015YA17 Phys.Rev. C 92, 035206 (2015) Hyperon semileptonic decay constants with flavor SU(3) symmetry breaking
doi: 10.1103/PhysRevC.92.035206
2014BR09 Nucl.Data Sheets 118, 144 (2014) D.A.Brown, R.Arcilla, R.Capote, S.F.Mughabghab, M.W.Herman, A.Trkov, H.I.Kim Zirconium Evaluations for ENDF/B-VII.2 for the Fast Region COMPILATION 90,91,92,93,94,95,96Zr(n, x), E=0=20 MeV; calculated, evaluated σ, σ(θ) including resonance region using EMPIRE-3.1 code. Compared with available data and evaluated databases.
doi: 10.1016/j.nds.2014.04.021
2014HO04 Eur.Phys.J. A 50, 49 (2014) By.Hong, J.K.Ahn, Y.Go, G.Jhang, E.Joo, D.G.Kim, E.J.Kim, H.H.Kim, Y.H.Kim, Y.J.Kim, Y.-J.Kim, Y.K.Kim, H.S.Lee, J.W.Lee, K.Lee, K.S.Lee, S.H.Lee, S.K.Lee, B.Mulilo, H.Shim, C.C.Yun Plan for nuclear symmetry energy experiments using the LAMPS system at the RIB facility RAON in Korea
doi: 10.1140/epja/i2014-14049-2
2014KI04 Nucl.Data Sheets 118, 151 (2014) H.I.Kim, C.W.Lee, D.H.Kim, Y.-O.Lee Neutron Cross Section Evaluation of Tungsten and Tantalum NUCLEAR REACTIONS 184W(n, n), (n, n'), E=0.1-20 MeV; calculated elastic σ(θ), inelastic σ to discrete states. 181Ta, 182,184,186W, W(n, x), E=0.1-200 MeV; calculated total σ. 184W(n, n'), E=11.5, 26 MeV; calculated neutron spectra. EMPIRE code with optimized optical model parameters. Results compared with data; neutron spectra also with evaluated libraries.
doi: 10.1016/j.nds.2014.04.023
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
2014SO12 Nucl.Data Sheets 119, 249 (2014) T.Y.Song, J.W.Kim, H.I.Kim, C.W.Lee, Y.O.Lee, S.C.Yang, K.S.Kim, G.N.Kim Measurement of Activation Cross Sections of Erbium Irradiated by Proton Beam NUCLEAR REACTIONS Er(p, x), E=0-35, 60-70 MeV; measured activation Eγ, Iγ. 165,166Tm deduced σ; calculated σ using TALYS. Compared with Tarkanyi data.
doi: 10.1016/j.nds.2014.08.068
2014YA17 Nucl.Data Sheets 119, 314 (2014) S.C.Yang, K.Kim, G.N.Kim, H.I.Kim, Y.O.Lee, M.W.Lee, D.K.Pham, V.D.Nguyen, S.G.Shin, M.H.Cho Measurement of Isomeric Yield Ratio of 143m, gSm from natSm(γ, xn) Reaction with End-Point Bremsstrahlung Energies of 40-60 MeV NUCLEAR REACTIONS Sm(γ, xn), E=40, 50, 60 MeV; measured bremsstrahlung induced activation Eγ, Iγ; deduced isomeric yield ratio for each energy; calculated isomeric yield ratio using TALYS-1.4. Compared to other data.
doi: 10.1016/j.nds.2014.08.086
2012BH12 J.Phys.:Conf.Ser. 375, 042023 (2012) H.Bhang, R.S.Boiko, D.M.Chernyak, J.H.Choi, S.Choi, F.A.Danevich, K.V.Efendiev, C.Enss, A.Fleischmann, A.M.Gangapshev, L.Gastaldo, A.M.Gezhaev, Y.S.Hwang, H.Jiang, W.G.Kang, V.V.Kazalov, N.D.Khanbekov, H.J.Kim, K.B.Kim, S.K.Kim, S.C.Kim, Y.D.Kim, Y.H.Kim, V.V.Kobychev, V.N.Kornoukhov, V.V.Kuzminov, V.M.Mokina, H.S.Lee, J.I.Lee, J.M.Lee, K.B.Lee, M.J.Lee, M.K.Lee, S.J.Lee, J.Li, X.Li, S.S.Myung, A.S.Nikolaiko, S.Olsen, S.I.Panasenko, H.Park, D.V.Poda, R.B.Podviyanuk, O.G.Polischuk, P.A.Polozov, S.S.Ratkevich, Y.Satou, J.H.So, K.Tanida, V.I.Tretyak, S.P.Yakimenko, Q.Yue, Y.Yuryev AMoRE experiment: a search for neutrinoless double beta decay of 100Mo isotope with 40Ca100MoO4 cryogenic scintillation detector
doi: 10.1088/1742-6596/375/1/042023
2011CH50 J.Korean Phys.Soc. 59, 1418s (2011) H.L.Chang, F.X.Gao, W.I.Ko, H.D.Kim, S.Y.Lee Evaluation of Sigma-MUF (Material Unaccounted For) for the Conceptually Designed Korea Advanced Pyroprocess Facility
doi: 10.3938/jkps.59.1418
2011CH57 Nucl.Data Sheets 112, 2887 (2011) M.B.Chadwick, M.Herman, P.Oblozinsky, M.E.Dunn, Y.Danon, A.C.Kahler, D.L.Smith, B.Pritychenko, G.Arbanas, R.Arcilla, R.Brewer, D.A.Brown, R.Capote, A.D.Carlson, Y.S.Cho, H.Derrien, K.Guber, G.M.Hale, S.Hoblit, S.Holloway, T.D.Johnson, T.Kawano, B.C.Kiedrowski, H.Kim, S.Kunieda, N.M.Larson, L.Leal, J.P.Lestone, R.C.Little, E.A.McCutchan, R.E.MacFarlane, M.MacInnes, C.M.Mattoon, R.D.McKnight, S.F.Mughabghab, G.P.A.Nobre, G.Palmiotti, A.Palumbo, M.T.Pigni, V.G.Pronyaev, R.O.Sayer, A.A.Sonzogni, N.C.Summers, P.Talou, I.J.Thompson, A.Trkov, R.L.Vogt, S.C.van der Marck, A.Wallner, M.C.White, D.Wiarda, P.G.Young ENDF/B-VII.1 Nuclear Data for Science and Technology: Cross Sections, Covariances, Fission Product Yields and Decay Data COMPILATION Z=1-118; compiled, analyzed decay data, Maxwellian averaged neutron capture σ, neutron-induced fission σ. NUCLEAR REACTIONS 1,2H, 3He, 6,7Li, 7,9Be, 10,11B, C, 14,15N, 16,17O, 19F, 22,23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,33,34,36S, 35,37Cl, 36,38,40Ar, 39,40,41K, 40,42,43,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 50,51V, 50,52,53,54Cr, 55Mn, 54,56,57,58Fe, 58,59Co, 58,59,60,61,62,64Ni, 63,65Cu, 65,66,67,68,70Zn, 69,71Ga, 70,72,73,74,76Ge, 74,75As, 74,76,77,78,79,80,82Se, 79,81Br, 78,80,82,83,84,85,86Kr, 85,86,87Rb, 84,86,87,88,89,90Sr, 89,90,91Y, 90,91,92,93,94,95,96Zr, 93,94,95Nb, 92,94,95,96,97,98,99,100Mo, 99Tc, 96,98,99,100,101,102,103,104,105,106Ru, 103,105Rh, 102,104,105,106,107,108,110Pd, 107,109,110,111Ag, 106,108,110,111,112,113,114,115,116Cd, 113,115In, 112,113,114,115,116,117,118,119,120,122,123,124,125,126Sn, 121,123,124,125,126Sb, 120,122,123,124,125,126,127,128,129,130,132Te, 127,129,130,131,135I, 123,124,126,128,129,130,131,132,133,134,135,136Xe, 133,134,135,136,137Cs, 130,132,133,134,135,136,137,138,140Ba, 138,139,140La, 136,138,139,140,141,142,143,144Ce, 141,142,143Pr, 142,143,144,145,146,147,148,150Nd, 147,148,149,151Pm, 144,147,148,149,150,151,152,153,154Sm, 151,152,153,154,155,156,157Eu, 152,153,154,155,156,157,158,160Gd, 159,160Tb, 156,158,160,161,162,163,164Dy, 165,166Ho, 162,164,166,167,168,170Er, 168,169,170Tm, 175,176Lu, 174,176,177,178,179,180Hf, 180,181,182Ta, 180,182,183,184,186W, 185,187Re, 191,193Ir, 197Au, 196,198,199,200,201,202,204Hg, 203,205Tl, 204,206,207,208Pb, 209Bi, 223,224,225,226Ra, 225,226,227Ac, 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), E=30 keV; calculated Maxwellian-averaged σ using ENDF/B-VII.1 evaluated neutron library. Comparison with ENDF/B-VII.0 and KADONIS values. NUCLEAR REACTIONS 227,228,229,230,231,232,233,234Th, 229,230,231,232,233Pa, 230,231,232,233,234,235,236,237,238,239,240,241U, 234,235,236,237,238,239Np, 236,237,238,239,240,241,242,243,244,246Pu, 240,241,242,243,244Am, 240,241,242,243,244,245,246,247,248,249,250Cm, 245,246,247,249,250Bk, 246,248,249,250,251,252,253,254Cf, 251,252,253,254,255Es, 255Fm(n, γ), (n, F), E=thermal; calculated thermal σ. Comparison with ENDF/B-VII.0, JENDL-4.0 and Atlas of Neutron Resonances values.
doi: 10.1016/j.nds.2011.11.002
2011HA49 J.Korean Phys.Soc. 59, 1430s (2011) B.-Y.Han, H.Shin, S.-K.Ahn, S.-H.Eom, H.-D.Kim A Feasibility Study on the Measurement of Mixed Nuclear Material Composition by Using Fission Neutron Multiplicity Distribution
doi: 10.3938/jkps.59.1430
2011KI24 J.Korean Phys.Soc. 59, 839s (2011) Evaluation of Neutron Cross Section with Uncertainties for Complete Cm Isotopic Family NUCLEAR REACTIONS 240,241,242,243,244,245,246,247,248,249,250Cm(n, n), (n, f), (n, X), E=0.04-20 MeV; calculated σ. 244Cm(n, X), (n, f), E=0.04-20 MeV; evaluated σ correlations. Comparison to data.
doi: 10.3938/jkps.59.839
2011KI25 J.Korean Phys.Soc. 59, 1023s (2011) H.Il.Kim, D.H.Kim, Y.-O.Lee, M.Mun Nuclear Data Evaluations for Silicon Isotopes Induced by Proton, Deuteron and Alpha NUCLEAR REACTIONS 28,29,30Si(p, p'), (d, d'), (α, α'), E=0-200 MeV; calculated, evaluated σ; 28Si(p, p), E=5.93, 17.7, 28.4, 40.2, 51.9, 65, 80, 100, 179 MeV;29Si(p, p), E=10, 40, 80 MeV;30Si(p, p), E=40.8, 180 MeV;28Si(d, d), E=7, 11, 13, 17.9, 29.5, 52, 56 MeV;29Si(d, d), E=10, 12.3 MeV;30Si(d, d), E=10, 11.8, 12.3, 17 MeV;28Si(α, α'), E=5.96, 27, 40, 104, 120, 166 MeV;29Si(α, α'), E=26.3, 28, 41 MeV;30Si(α, α'), E=26.6, 27, 41 MeV; calculated, evaluated σ(θ). TALYS code. Calculations compared to data.
doi: 10.3938/jkps.59.1023
2011KI42 J.Korean Phys.Soc. 59, 2029s (2011) H.W.Kim, B.N.Lee, S.H.Lee, H.J.Choi, Y.S.Lee, H.S.Song, T.Zhou, Kh M.Gad, Y.H.Yeon, J.H.Oh, K.H.Park, S.H.Shin, M.H.Yoon, J.S.Chai Magnet Design of 4 MeV Cyclotron for the BNCT
doi: 10.3938/jkps.59.2029
2011LE04 Astropart.Phys. 34, 732 (2011) S.J.Lee, J.H.Choi, F.A.Danevich, Y.S.Jang, W.G.Kang, N.Khanbekov, H.J.Kim, I.H.Kim, S.C.Kim, S.K.Kim, Y.D.Kim, Y.H.Kim, V.V.Kobychev, V.N.Kornoukhov, J.I.Lee, J.S.Lee, K.B.Lee, M.K.Lee, Y.H.Lee, S.S.Myung, J.H.So, V.I.Tretyak, Y.Yuryev The development of a cryogenic detector with CaMoO4 crystals for neutrinoless double beta decay search
doi: 10.1016/j.astropartphys.2011.01.004
2011LE23 Nucl.Instrum.Methods Phys.Res. A654, 157 (2011) J.I.Lee, H.C.Bhang, J.H.Choi, E.J.Jeon, W.G.Kang, H.J.Kim, S.C.Kim, S.K.Kim, Y.D.Kim, J.H.Lee, M.J.Lee, S.J.Lee, K.J.Ma, S.S.Myung, S.Ryu, J.H.So Experimental study on neutrinoless double beta decay of 92Mo RADIOACTIVITY 92Mo(β+EC); measured decay products, Eβ, Iβ; deduced T1/2 limit. CaMoO4 scintillator.
doi: 10.1016/j.nima.2011.05.083
2011LE41 J.Korean Phys.Soc. 59, 2032s (2011) B.N.Lee, J.A.Park, Y.S.Lee, H.S.Song, H.W.Kim, T.Zhou, S.H.Lee, H.J.Choi, J.H.Oh, Y.H.Yeon, Y.Kadi, J.S.Chai Design of Neutron Targets with the 4 MeV Cyclotron for BNCT
doi: 10.3938/jkps.59.2032
2011SO34 J.Korean Phys.Soc. 59, 1999s (2011) H.S.Song, H.W.Kim, T.Zhou, B.N.Lee, Y.S.Lee, S.H.Lee, H.J.Choi, Y.H.Yeon, J.H.Oh, Kh.M.Gad, Y.Kadi, J.S.Chai Computer Simulation of CNT Field Emitter Based X-ray Spectra Using with FLUKA Code
doi: 10.3938/jkps.59.1999
2011YA03 Phys.Rev. C 83, 038203 (2011) Binding energy per nucleon and hadron properties in nuclear matter
doi: 10.1103/PhysRevC.83.038203
2009HW02 Astropart.Phys. 31, 412 (2009) M.J.Hwang, Y.J.Kwon, H.J.Kim, J.W.Kwak, S.C.Kim, S.K.Kim, T.Y.Kim, S.Y.Kim, H.S.Lee, M.J.Lee, S.S.Myung, Y.D.Kim, J.I.Lee, W.G.Kang, I.S.Hahn, M.H.Lee, and the KIMS Collaboration A search for 0νββ decay of 124Sn with tin-loaded liquid scintillator RADIOACTIVITY 124Sn(2β-); measured summed electron energy spectrum; deduced 0νββ-decay T1/2 lower limits.
doi: 10.1016/j.astropartphys.2009.05.001
2009KI07 Nucl.Technology 168, 274 (2009) D.He.Kim, H.I.Kim, C.-S.Gil, Y.-O.Lee Validation of New Neutron Production Cross Sections for Tungsten Isotopes
doi: 10.13182/NT09-A9194
2008KI12 Nucl.Sci.Eng. 160, 168 (2008) H.Kim, M.Herman, S.F.Mughabghab, P.Oblozinsky, D.Rochman, Y.-O.Lee Evaluation of Neutron Cross Sections for a Complete Set of Nd Isotopes NUCLEAR REACTIONS 142,143,144,145,146,147,148,150Nd(n, X), E < 20 MeV; analyzed cross sections.
doi: 10.13182/NSE160-168
2008KI15 Nucl.Instrum.Methods Phys.Res. B266, 3513 (2008) H.Kim, M.Herman, S.F.Mughabghab, P.Oblozinsky, Y.-O.Lee Evaluation of neutron cross sections for a complete set of Dy isotopes NUCLEAR REACTIONS 156,158,160,161,162,163,164Dy(n, X), E= 10- eV - 20 MeV; analyzed neutron σ; comparison with experimental data and ENDF/B-VI.8, JEFF-3.1 data libraries; EMPIRE-2.19.
doi: 10.1016/j.nimb.2008.05.020
2008KI19 Phys.Lett. B 669, 287 (2008) H.O.Kim, for the Belle Collaboration Study of intermediate two-body decays in B(bar)0 → Σc(2455)0p(bar)π+
doi: 10.1016/j.physletb.2008.09.059
2008LE22 Nucl.Phys. A811, 353 (2008) 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
2008SH04 J.Korean Phys.Soc. 52, 843 (2008) G.-H.Shin, K.-S.Ryu, H.-M.Kim, K.-W.Min Radiation Effect Test for Single-Crystalline and Polycrystalline Silicon Solar Cells
doi: 10.3938/jkps.52.843
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
2007KA62 Phys.Rev. C 76, 067602 (2007) W.G.Kang, Y.D.Kim, J.I.Lee, I.S.Hahn, A.R.Kim, H.J.Kim Measurement of the thermal neutron capture cross section of 180W NUCLEAR REACTIONS W(n, γ), E=thermal; measured Eγ, Iγ. 180,181,185,187W; measured capture cross sections.
doi: 10.1103/PhysRevC.76.067602
2007KI12 J.Nucl.Sci.Technol.(Tokyo) 44, 1117 (2007) Evaluation of Neutron Capture Gamma-ray Spectra for 89Y, 93Nb, 127I, 133Cs, 141Pr, 197Au, natTl, and 209Bi NUCLEAR REACTIONS 89Y, 93Nb, 127I, 141Pr, 197Au, Tl, 209Bi(n, γ), E not given; calculated Eγ, Iγ, cross sections using Hauser-Feshbach model. Compared results to available data.
doi: 10.1080/18811248.2007.9711354
2007KI13 Nucl.Phys. A793, 171 (2007) H.J.Kim, S.C.Kim, S.K.Kim, T.Y.Kim, H.S.Lee, J.Lee, M.J.Lee, Y.D.Kim, J.I.Lee, J.Y.Lee, M.J.Hwang, Y.J.Kwon, I.S.Hahn, M.H.Lee Searches for the β+/EC decays of 64Zn and 112Sn, and the ββ decay transitions of 124Sn to the excited states of 124Te RADIOACTIVITY 64Zn, 112Sn(β+), (EC);124Sn(2β-); measured Eγ, Iγ; deduced T1/2 lower limits for β+, EC and 0ν-accompanied 2β-decay to ground and excited states. Comparison with theoretical values and previous data.
doi: 10.1016/j.nuclphysa.2007.06.007
2007RO10 J.Korean Phys.Soc. 50, 1494 (2007) T.-I.Ro, Y.-R.Kang, H.Kim, W.-C.Chung, G.Kim, S.Lee, M.Igashira, T.Ohsaki Measurement of Capture Cross-Sections for the 165Ho (n, γ)166Ho Reaction in the Neutron Energy Region from 10 to 90 keV NUCLEAR REACTIONS 165Ho(n, γ), E=10-90 keV; measured capture cross sections relative to standard capture cross sections for 197Au.
doi: 10.3938/jkps.50.1494
2007RO11 J.Korean Phys.Soc. 50, 1598 (2007) T.-I.Ro, B.R.Park, Y.-R.Kang, H.Kim, W.-C.Chung, K.Kim, G.Kim, Y.Oh, S.Lee, M.Igashira, T.Ohsaki Measurement of Neutron Capture Cross-Sections of 105Pd with keV-Neutrons Produced by Using a Pulsed Proton Beam NUCLEAR REACTIONS 105Pd(n, γ), E=10-90 keV; measured capture cross sections relative to standard capture cross sections for 197Au.
doi: 10.3938/jkps.50.1598
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
2006KI18 J.Korean Phys.Soc. 49, 1908 (2006) Dynamics of a Phase Transition in (3+1)-Dimensional Scalar φ4 Theory
2006NA04 Phys.Lett. B 633, 483 (2006) 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
2006NA24 Phys.Rev. C 74, 025204 (2006) 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
2006NA35 J.Korean Phys.Soc. 49, 1928 (2006) 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).
2006OH04 Phys.Rev. C 73, 065202 (2006) K* photoproduction off the nucleon: γN → K* Λ NUCLEAR REACTIONS 1n, 1H(γ, X), E=1.5-4 GeV; calculated K*(892)Λ photoproduction σ, spin asymmetries.
doi: 10.1103/PhysRevC.73.065202
2006OH05 Phys.Rev. C 74, 015208 (2006) Scalar κ meson in K* photoproduction NUCLEAR REACTIONS 1H(γ, K0X), (γ, K+X), E ≈ 2-3 GeV; analyzed hyperon production associated σ, σ(θ); deduced role of κ-meson exchange.
doi: 10.1103/PhysRevC.74.015208
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
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
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
2005NA24 Nucl.Phys. A755, 423c (2005) 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
2005SA03 Phys.Rev.Lett. 94, 052502 (2005) P.Saha, T.Fukuda, W.Imoto, K.K.Ahn, A.Ajimura, K.Aoki, H.C.Bhang, H.Fujioka, H.Hotchi, J.I.Hwang, T.Itabashi, B.H.Kang, H.D.Kim, M.J.Kim, T.Kishimoto, A.Krutenkova, T.Maruta, Y.Miura, K.Miwa, T.Nagae, H.Noumi, H.Outa, T.Ohtaki, A.Sakaguchi, Y.Sato, M.Sekimoto, Y.Shimizu, H.Tamura, K.Tanida, A.Toyoda, M.Ukai, H.J.Kim Production of the Neutron-Rich Hypernucleus 10ΛLi in the (π-, K+) Double Charge-Exchange Reaction NUCLEAR REACTIONS 10B(π-, K+), 10B, 12C(π+, K+), E at 1.05, 1.2 GeV/c; measured missing mass spectra, hypernucleus production σ.
doi: 10.1103/PhysRevLett.94.052502
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
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
2004KI23 J.Korean Phys.Soc. 45, 1474 (2004) H.Kim, J.K.Ahn, G.Kim, T.-I.Ro, W.-C.Chung, M.Igashira, T.Ohsaki, S.Mizuno Measurement of Neutron Capture Cross-Sections and Capture γ-ray Spectra of 161, 162, 163, 164Dy at 550 keV NUCLEAR REACTIONS 161,162,163,164Dy(n, γ), E=550 keV; measured Eγ, Iγ, capture σ. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22767. 2004NA31 Phys.Lett. B 602, 180 (2004) 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
2004NA41 Phys.Rev. D 70, 114027 (2004) 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
2004OH14 Nucl.Phys. A745, 129 (2004) Spin asymmetries in γN → (K-bar)*Θ+ NUCLEAR REACTIONS 1n(γ, K-X), 1H(γ, K0X), E=1-5 GeV; calculated pentaquark production σ, σ(θ), spin asymmetries.
doi: 10.1016/j.nuclphysa.2004.09.010
2004SI31 Eur.Phys.J. A 22, 481 (2004) 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
2004TS08 Phys.Rev. C 70, 038501 (2004) Effect of the bound nucleon form factors on charged-current neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, μ-X), E=0-300 MeV; calculated bound nucleon form factors, σ(E), σ. Quark-meson coupling model.
doi: 10.1103/PhysRevC.70.038501
2003DO14 Nucl.Phys. A721, 755c (2003) The F/D Ratio and Meson-Baryon Couplings from QCD Sum Rules
doi: 10.1016/S0375-9474(03)01174-6
2003DU17 Phys.Rev. C 68, 035208 (2003) F.O.Duraes, H.Kim, S.H.Lee, F.S.Navarra, M.Nielsen Progress in the determination of the J/ψ-π cross section
doi: 10.1103/PhysRevC.68.035208
2003KI07 Nucl.Phys. A720, 368 (2003) Update on pion weak decay constants in nuclear matter
doi: 10.1016/S0375-9474(03)01004-2
2003SI18 Nucl.Phys. A721, 417c (2003) 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
2002FR03 Nucl.Phys. A699, 541 (2002) ΔS = 1, 2 Effective Weak Chiral Lagrangian from the Instanton Vacuum
doi: 10.1016/S0375-9474(01)01275-1
2002KI11 Phys.Rev. C65, 055201 (2002) In-Medium Pion Weak Decay Constants
doi: 10.1103/PhysRevC.65.055201
2002KI21 J.Korean Phys.Soc. 41, 655 (2002) H.Kim, E.Jung, J.K.Ahn, D.Lee, G.Kim, T.I.Ro, Y.Min, M.Igashira, T.Ohsaki, S.Mizuno Neutron-Capture Cross-Section Measurement for 163Dy in the Neutron Energy Range from 15 to 75 keV NUCLEAR REACTIONS 163Dy(n, γ), E=15-75 keV; measured Eγ, capture σ. Comparison with previous results. Pulse-height weighting technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22683. 2001KI14 J.Korean Phys.Soc. 38, 14 (2001) G.Kim, Y.S.Lee, V.Skoy, V.Kovalchuk, M.-H.Cho, I.S.Ko, W.Namkung, D.W.Lee, H.D.Kim, S.K.Ko, S.H.Park, D.S.Kim, T.I.Ro, Y.G.Min First Experiment at the Pohang Neutron Facility NUCLEAR REACTIONS Sm, Ta, W, Ag(n, X), E=low; measured transmission neutron spectra. Pulsed neutron source.
2001KI26 Ann.Nucl.Energy 28, 1549 (2001) G.Kim, Y.Lee, I.S.Ko, M.-H.Cho, W.Namkung, D.Lee, H.Kim, Y.Kim, T.-I.Ro, Y.Min, J.Moon, M.Igashira, S.Mizuno, T.Ohsaki, S.Y.Lee Measurement of keV-Neutron Capture Cross-Sections for 164Dy NUCLEAR REACTIONS 164Dy(n, γ), E=10-90 keV; measured Eγ, Iγ, capture σ. Comparison with previous results.
doi: 10.1016/S0306-4549(00)00138-9
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
2000DO24 Phys.Rev. C62, 055202 (2000) Pertinent Dirac Structure for QCD Sum Rules of Meson-Baryon Coupling Constants
doi: 10.1103/PhysRevC.62.055202
2000FR09 Nucl.Phys. A663-664, 995c (2000) Effective Weak Chiral Lagrangian from the Instanton Vacuum
doi: 10.1016/S0375-9474(99)00752-6
2000KI01 Nucl.Phys. A662, 371 (2000) Meson-Baryon Couplings and the F/D Ratio from QCD Sum Rules
doi: 10.1016/S0375-9474(99)00426-1
2000KI02 Eur.Phys.J. A 7, 121 (2000) πNN Coupling Determined Beyond the Chiral Limit
doi: 10.1007/s100500050019
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
2000KI14 Nucl.Phys. A670, 64c (2000) QCD Sum Rules with Two-Point Correlation Function
doi: 10.1016/S0375-9474(00)00070-1
2000KI29 Nucl.Phys. A678, 295 (2000) The F/D Ratio and Meson-Baryon Couplings from QCD Sum Rules II
doi: 10.1016/S0375-9474(00)00330-4
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.
1999FR13 Nucl.Phys. A653, 91 (1999) Constraints on Vector Mesons with Finite Momentum in Nuclear Matter
doi: 10.1016/S0375-9474(99)00171-2
1999KI10 Phys.Lett. 453B, 199 (1999) QCD Sum Rule Calculation of the πNN Coupling-Revisited
doi: 10.1016/S0370-2693(99)00379-2
Back to query form [Next] Note: The following list of authors and aliases matches the search parameter H.Kim: , H.B.KIM, H.C.KIM, H.D.KIM, H.H.KIM, H.I.KIM, H.J.KIM, H.L.KIM, H.M.KIM, H.O.KIM, H.S.KIM, H.W.KIM, H.Y.KIM |