NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = Y.Oh Found 73 matches. 2022LE15 Eur.Phys.J. A 58, 252 (2022) Models of J/Ψ photo-production reactions on the nucleon
doi: 10.1140/epja/s10050-022-00901-9
2022SO19 Phys.Rev. C 106, 055807 (2022) Radiative proton capture on 15N within effective field theory NUCLEAR REACTIONS 15N(p, γ), E(cm)<2.3 MeV; calculated astrophysical S-factor energy dependence including value at zero energy, resonance parameters. Cluster effective field theory with effective Lagrangian appropriate for the reaction at low energies. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.055807
2021KI10 Phys.Rev. C 104, 045202 (2021) S.-H.Kim, T.-S.H.Lee, S.-i.Nam, Y.Oh Dynamical model of φ meson photoproduction on the nucleon and 4He NUCLEAR REACTIONS 1H(γ, pφ), E=1-400 GeV; calculated total σ(E) forphotoproduction of ρ0, φ, and J/ψ, total σ(E). 1H(γ, pφ), E=1.985-2.815 GeV; calculated differential σ(θ, E), total σ(E), and compared with experimental data from CLAS Collaboration and other experiments. 4He(γ, αφ), E=1.5-3 GeV; calculated differential σ(θ, E), and compared with experimental data from LEPS Collaboration and other experiments. Dynamical model based on a Hamiltonian describing production mechanisms by the Pomeron and meson exchanges.
doi: 10.1103/PhysRevC.104.045202
2020CH09 Phys.Rev. C 101, 024909 (2020) S.Cho, K.-J.Sun, C.M.Ko, S.H.Lee, Y.Oh Charmed hadron production in an improved quark coalescence model
doi: 10.1103/PhysRevC.101.024909
2019GI12 Phys.Rev. C 99, 064319 (2019) H.Gil, P.Papakonstantinou, C.H.Hyun, Y.Oh From homogeneous matter to finite nuclei: Role of the effective mass NUCLEAR STRUCTURE 16,28O, 40,42,44,46,48,50,52,54,56,58,60Ca, 90Zr, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 208Pb, 218U; calculated binding energy per nucleon, charge radii and neutron-skin thickness for 16,28O, 40,48,60Ca, 90Zr, 132Sn, 208Pb, 218U, and energies of occupied proton levels in 208Pb using microscopic Skyrme type energy density functional (EDF) generated from a immutable equation of state (EoS). Comparison with experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.99.064319
2019GI13 Phys.Rev. C 100, 014312 (2019) H.Gil, Y.-M.Kim, C.H.Hyun, P.Papakonstantinou, Y.Oh Analysis of nuclear structure in a converging power expansion scheme NUCLEAR STRUCTURE 16,28O, 40,48,60Ca, 90Zr, 132Sn, 208Pb; calculated binding energies per nucleon, charge radii, and neutron skin thickness using generalized energy density functional model (KIDS EDF) to parametrized nuclear equation of state (EoS). Comparison with experimental values.
doi: 10.1103/PhysRevC.100.014312
2019HU02 Phys.Rev. C 99, 015202 (2019) P.T.P.Hutauruk, Y.Oh, K.Tsushima Electroweak properties of pions in a nuclear medium
doi: 10.1103/PhysRevC.99.015202
2017GI05 Acta Phys.Pol. B48, 305 (2017) H.Gil, P.Papakonstantinou, C.H.Hyun, T.-S.Park, Y.Oh Nuclear Energy Density Functional for KIDS NUCLEAR STRUCTURE 16,28O, 40,60Ca; calculated energy per p article, mass excess, charge radius vs k-parameter of the radius using density functional theory. Masses compared with AME-2012 values.
doi: 10.5506/APhysPolB.48.305
2017KI04 Phys.Rev. C 95, 055206 (2017) Decay angular distributions of K* and D* vector mesons in pion-nucleon scattering NUCLEAR REACTIONS 1H(π-, Κ0Λ), at pion momentum of 6.15 GeV/c; calculated unpolarized differential cross sections, spin-density matrix elements, angular distributions and azimuthal angle distributions for K* and D* excitations using quark-gluon string model.
doi: 10.1103/PhysRevC.95.055206
2017LI09 Phys.Rev. C 95, 034311 (2017) Nuclear energy density functional and the nuclear α decay RADIOACTIVITY 271Sg, 270,272Bh, 275Hs, 274,275,276Mt, 279Ds, 278,279,280Rg, 283,285Cn, 282,283,284Nh, 286,287,288,289Fl, 287,288Mc, 290,291,292,293Lv, 294Og(α); calculated half-lives for α decay using the Skyrme SLy4 and Gogny D1S models as nonrelativistic models and the relativistic mean-field DD-ME2 model, and using experimental Q(α) values, half-lives compared with experimental values. 293,294,295,296,297,298Ts, 293,294,295,296,297,298Og, 293,294,295,296,297,298119, 299,300,301,302,303,304120, 301,302,303,304,305,306121, 302,303,304,305,306,307122(α); calculated half-lives for α decay using the Skyrme SLy4 and Gogny D1S models as nonrelativistic models and the relativistic mean-field DD-ME2 model, and Q(α) values calculated from liquid-drop model (LDM) and from a local formula. Nuclear energy density functional formalism applied to α decay, using a Skyrme-type force model to obtain the nuclear potential of the α particle as a functional of proton and neutron density profiles of the daughter nucleus obtained from non-relativistic Skyrme SLy4, Gogny D1S, and relativistic mean-field DD-ME2 models.
doi: 10.1103/PhysRevC.95.034311
2016KO08 Phys.Rev. C 93, 021901 (2016) N.Kochelev, H.-J.Lee, Y.Oh, B.Zhang, P.Zhang Nonperturbative collisional energy loss of heavy quarks in quark-gluon plasma
doi: 10.1103/PhysRevC.93.021901
2016NA01 Nucl.Phys. A946, 89 (2016) Peculiarities of quasifission reactions in heavy ion collisions
doi: 10.1016/j.nuclphysa.2015.11.013
2016SH26 Phys.Rev. C 94, 024320 (2016) Nuclear isospin asymmetry in α decay of heavy nuclei RADIOACTIVITY 270Db, 271Sg, 270,272,274Bh, 275Hs, 274,275,276,278Mt, 279Ds, 278,279,280,282Rg, 285Cn, 282,283,284,286Nh, 286,287,288,289Fl, 287,288,290Mc, 290,291,292,293Lv, 293,294,295,296,297,298Ts, 293,294,295,296,297,298Og, 293,294,295,296,297,298119, 299,300,301,302,303,304120, 301,302,303,304,305,306121, 302,303,304,305,306,307122(α); calculated half-lives using various phenomenological models of the nuclear potential for the α particle and Wentzel-Kramers-Brillouin (WKB) approximation: square-well potential, Woods-Saxon potential modified by including an isospin asymmetry term, energy density functional approach using Skyrme force model, and modified Viola and Seaborg formula to include isospin asymmetry effect. Comparison with available experimental results.
doi: 10.1103/PhysRevC.94.024320
2015AN09 Phys.Rev. C 92, 024325 (2015) Investigation of the Λ bound state in pionless effective theory
doi: 10.1103/PhysRevC.92.024325
2015JA03 Phys.Rev. C 91, 065208 (2015) B.C.Jackson, Y.Oh, H.Haberzettl, K.Nakayama K-bar + N → K + Ξ reaction and S = -1 hyperon resonances
doi: 10.1103/PhysRevC.91.065208
2015MU05 Phys.Rev. C 91, 054610 (2015) M.-H.Mun, G.G.Adamian, N.V.Antonenko, Y.Oh, Y.Kim Toward neutron-rich nuclei via transfer reactions with stable and radioactive beams NUCLEAR REACTIONS 160Gd, 164Dy, 170Er, 176Yb, 180Hf, 186W, 192Os, 204Hg, 208Pb, 232Th(48Ca, X)52Ca/54Ca/56Ca/58Ca, E(cm)=150-225 MeV; 64,66,68,70,72,74,76,78Ni, 86,88,90,92,94Kr(160Gd, X)166Gd/168Gd/170Gd/172Gd/174Gd, E(cm)=145-260 MeV; 48Ca, 50Ti, 54Cr, 58Fe, 64,66,68,70,72,74,76,78Ni, 70Zn, 76Ge, 82Se, 86,88,90,92,94Kr(164Dy, X)170Dy/172Dy/174Dy/176Dy/178Dy, E(cm)=150-260 MeV; 48Ca, 50Ti, 54Cr, 58Fe, 64,66,68,70,72,74,76,78Ni, 70Zn, 76Ge, 82Se, 86,88,90,92,94Kr(170Er, X)176Er/178Er/180Er/182Er/184Er, E(cm)=150-270 MeV; 48Ca, 50Ti, 54Cr, 58Fe, 64,66,68,70,72,74,76,78Ni, 70Zn, 76Ge, 82Se, 86,88,90,92,94Kr(176Yb, X)182Yb/184Yb/186Yb/188Yb/190Yb, E(cm)=160-270 MeV; 64,66,68,70,72,74,76,78Ni(180Hf, X)186Hf/188Hf/190Hf/192Hf/194Hf, E(cm)=190-230 MeV; 48Ca, 50Ti, 54Cr, 58Fe, 64,66,68,70,72,74,76,78Ni, 70Zn, 76Ge, 82Se(186W, X)192W/194W/196W/198W/200W, E(cm)=170-270 MeV; 48Ca, 50Ti, 54Cr, 58Fe, 64,66,68,70,72,74,76,78Ni, 70Zn, 76Ge, 82Se(192Os, X)196Os/198Os/200Os/202Os/204Os, E(cm)=165-270 MeV; 48Ca, 66,68,70,72,74,76,78Ni(204Hg, X)210Hg/212Hg/214Hg/216Hg, E(cm)=192-255 MeV; 48Ca, 66,68,70,72,74,76,78Ni(208Pb, X)214Pb/216Pb/218Pb/220Pb, E(cm)=200-268 MeV; 48Ca, 66,68,70,72,74,76,78Ni(232Th, X)238Th/240Th/242Th/244Th, E(cm)=199-261 MeV; calculated σ(E) for production of neutron-rich nuclei close to the neutron drip line in multi-nucleon transfer reactions. Dinuclear system (DNS) approach with synthesis through nucleon transfers and decay into two fragments.
doi: 10.1103/PhysRevC.91.054610
2015TA14 Phys.Rev. C 91, 054612 (2015) R.B.Tashkhodjaev, A.I.Muminov, A.K.Nasirov, W.von Oertzen, Y.Oh Theoretical study of the almost sequential mechanism of true ternary fission RADIOACTIVITY 252Cf(SF); calculated yield contours of massive clusters in ternary fission, potential-energy surface in (Z1, Z3) plane and collinear cluster tripartition (CCT), contour map of the calculated velocity of the middle fragment Z3. Collinear sequential ternary fission. Relevance to experiments by FOBOS group at FLNR-JINR facility.
doi: 10.1103/PhysRevC.91.054612
2014AN01 Phys.Rev. C 89, 014318 (2014) ΛΛ4H in halo effective field theory NUCLEAR STRUCTURE 4H; calculated ΛΛ hyperon bound state, S-wave hypertriton-Λ scattering length in spin singlet and triplet channels below the hypertriton breakup momentum, two-hyperon separation energy, coupling parameter of three-body contact interaction as a function of the cutoff parameter. Halo/cluster effective field theory treating the double-hyperon 4H hypernucleus system as a three-cluster (Λ-Λ-deuteron) system.
doi: 10.1103/PhysRevC.89.014318
2014AN08 Phys.Rev. C 90, 037301 (2014) 6ΛΛHe in cluster effective field theory NUCLEAR STRUCTURE 6He; calculated correlations between the double hyperon separation energy (BΛΛ) of 6ΛΛHe hypernucleus, and the scattering length aΛΛ of the s-wave ΛΛ scattering. Three-body (ΛΛα) cluster system in cluster effective field theory at leading order. Comparison with experimental BΛΛ value.
doi: 10.1103/PhysRevC.90.037301
2014JA04 Phys.Rev. C 89, 025206 (2014) B.C.Jackson, Y.Oh, H.Haberzettl, K.Nakayama Model-independent aspects of the reaction K(bar) + N → K + Κ
doi: 10.1103/PhysRevC.89.025206
2014KA30 Phys.Rev.Lett. 113, 022502 (2014) J.Katich, X.Qian, Y.X.Zhao, K.Allada, K.Aniol, J.R.M.Annand, T.Averett, F.Benmokhtar, W.Bertozzi, P.C.Bradshaw, P.Bosted, A.Camsonne, M.Canan, G.D.Cates, C.Chen, J.-P.Chen, W.Chen, K.Chirapatpimol, E.Chudakov, E.Cisbani, J.C.Cornejo, F.Cusanno, M.M.Dalton, W.Deconinck, C.W.de Jager, R.De Leo, X.Deng, A.Deur, H.Ding, P.A.M.Dolph, C.Dutta, D.Dutta, L.El Fassi, S.Frullani, H.Gao, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, O.Glamazdin, S.Golge, L.Guo, D.Hamilton, O.Hansen, D.W.Higinbotham, T.Holmstrom, J.Huang, M.Huang, H.F.Ibrahim, M.Iodice, X.Jiang, G.Jin, M.K.Jones, A.Kelleher, W.Kim, A.Kolarkar, W.Korsch, J.J.LeRose, X.Li, Y.Li, R.Lindgren, N.Liyanage, E.Long, H.-J.Lu, D.J.Margaziotis, P.Markowitz, S.Marrone, D.McNulty, Z.-E.Meziani, R.Michaels, B.Moffit, C.Munoz Camacho, S.Nanda, A.Narayan, V.Nelyubin, B.Norum, Y.Oh, M.Osipenko, D.Parno, J.C.Peng, S.K.Phillips, M.Posik, A.J.R.Puckett, Y.Qiang, A.Rakhman, R.D.Ransome, S.Riordan, A.Saha, B.Sawatzky, E.Schulte, A.Shahinyan, M.H.Shabestari, S.Sirca, S.Stepanyan, R.Subedi, V.Sulkosky, L.-G.Tang, A.Tobias, G.M.Urciuoli, I.Vilardi, K.Wang, Y.Wang, B.Wojtsekhowski, X.Yan, H.Yao, Y.Ye, Z.Ye, L.Yuan, X.Zhan, Y.Zhang, Y.-W.Zhang, B.Zhao, X.Zheng, L.Zhu, X.Zhu, X.Zong Measurement of the Target-Normal Single-Spin Asymmetry in Deep-Inelastic Scattering from the Reaction 3He ↑ (e, e')X
doi: 10.1103/PhysRevLett.113.022502
2014MU02 Phys.Rev. C 89, 034622 (2014) M.-H.Mun, G.G.Adamian, N.V.Antonenko, Y.Oh, Y.Kim Production cross section of neutron-rich isotopes with radioactive and stable beams NUCLEAR REACTIONS 48Ca, 70Zn, 86Kr, 88Sr(144Xe, X)148Xe/150Xe/152Xe, E(cm)=130-240 MeV; 48Ca(134Te, X), (136Te, X)136Te/138Te/140Te/142Te, E(cm)=120-170 MeV; 68,70Zn(142Xe, X), (144Xe, X)82Zn/84Zn/86Zn, E(cm)=160-195 MeV; 48Ca(134Te, X), (136Te, X)52Ca/54Ca/56Ca/58Ca/60Ca, E(cm)=125-165 MeV; 198Pt(48Ca, X), (50Ti, X), (54Cr, X), (58Fe, X), (64Ni, X), (70Zn, X), (76Ge, X)202Pt/204Pt/206Pt, E(cm)=170-270 MeV; 198Pt(48Ca, X)202Pt/203Pt/204Pt/205Pt/206Pt, E(cm)=170-220 MeV; 198Pt(64Ni, X), (66Ni, X), (68Ni, X), (70Ni, X), (72Ni, X)202Pt/204Pt/206Pt/208Pt/210Pt, E(cm)=215-260 MeV; calculated production σ for neutron-rich isotopes close to the neutron drip line using stable and radioactive beams. Diffusive multinucleon transfer reaction model.
doi: 10.1103/PhysRevC.89.034622
2012NA08 Phys.Rev. C 85, 042201 (2012) K.Nakayama, Y.Oh, H.Haberzettl Model-independent determination of the parity of Ξ hyperons
doi: 10.1103/PhysRevC.85.042201
2011KA14 Phys.Rev. C 83, 055201 (2011) J.Ka Shing Man, Y.Oh, K.Nakayama Role of high-spin hyperon resonances in the reaction of γp → K+K+Ξ-
doi: 10.1103/PhysRevC.83.055201
2010KO26 Nucl.Phys. A834, 253c (2010) Transport model study of deuteron production in relativistic heavy ion collisions NUCLEAR REACTIONS Au(Au, X), E(cm)=200 GeV; calculated deuteron elliptic flow, σ(E) using hadronic transport model. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.12.052
2010RA01 Nucl.Instrum.Methods Phys.Res. B268, 13 (2010) Md.S.Rahman, K.-S.Kim, M.Lee, G.Kim, Y.Oh, H.-S.Lee, M.-Hy.Cho, I.S.Ko, W.Namkung, N.V.Do, P.D.Khue, K.T.Thanh, T.-I.Ro Measurement of isomeric yield ratios in natIn and natSn with 50, 60, and 70 MeV bremsstrahlung photons NUCLEAR REACTIONS In(γ, xn)110In, 113In(γ, 2n), 111In, In(γ, xn), 111In, 113In(γ, n), 112In, In(γ, xn), 112In, 118Sn(γ, p), 117In, Sn(γ, xnp)117In, E<70 MeV; measured Eγ, Iγ; deduced isomeric yield ratios. Comparison with other values.
doi: 10.1016/j.nimb.2009.09.033
2010RA02 J.Radioanal.Nucl.Chem. 283, 519 (2010) M.S.Rahman, K.-S.Kim, M.Lee, G.Kim, Y.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung, V.D.Nguyen, D.K.Pham, T.T.Kim, T.-Ik.Ro Measurement of isomeric-yield ratios for the 197Au(γ, n)196m, gAu reactions induced by bremsstrahlung NUCLEAR REACTIONS 197Au(γ, n), E=0.05-2.5 GeV; measured Eγ, Iγ; deduced isomeric yield ratios.
doi: 10.1007/s10967-009-0375-1
2010RI03 Phys.Rev. C 82, 015202 (2010) F.Riek, R.Rapp, Y.Oh, T.-S.H.Lee Medium modifications of the ρ meson in nuclear photoproduction NUCLEAR REACTIONS 12C, 27Al, 56Fe, 88Sr, 120Sn, 152Sm, 197Au, 208Pb, 238U(γ, X), E=1-3.5 GeV; calculated invariant mass excess spectra, total σ of the dileptons, nuclear transparency ratio. Comparison with experimental data.
doi: 10.1103/PhysRevC.82.015202
2010WA03 Nucl.Instrum.Methods Phys.Res. B268, 440 (2010) T.Wang, M.Lee, G.Kim, Y.Oh, W.Namkung, T.-I.Ro, Y.-R.Kang, M.Igashira, T.Katabuchi Measurement of keV-neutron capture cross-sections and capture γ-ray spectra of 56Fe and 57Fe NUCLEAR REACTIONS 197Au, 56,57Fe(n, γ), E=10-90 keV; measured Eγ, Iγ; deduced σ. Comparison with ENDF/B-VII.0 and JENDL-3.3 data.
doi: 10.1016/j.nimb.2009.11.019
2010WA47 Nucl.Instrum.Methods Phys.Res. B 268, 106 (2010) T.F.Wang, M.W.Lee, K.S.Kim, G.N.Kim, Y.D.Oh, M.H.Cho, I.S.Ko, W.Namkung, T.I.Ro Measurement of neutron total cross-sections and resonance parameters of erbium at the Pohang Neutron Facility NUCLEAR REACTIONS Er(n, x), 166Er(n, n), 166Er(n, γ), 167Er(n, n), 167Er(n, γ), 168Er(n, n), 168Er(n, γ), 170Er(n, n), 170Er(n, γ), E=0.18344-200.6134 eV; measured products, Eγ, Iγ; deduced σ, σ(E), resonance parameters. Data were imported from EXFOR entry 31688.
doi: 10.1016/j.nimb.2009.10.184
2010XU01 Phys.Rev. C 81, 024910 (2010) Isospin-dependent pion in-medium effects on the charged-pion ratio in heavy ion collisions
doi: 10.1103/PhysRevC.81.024910
2009NA10 Nucl.Instrum.Methods Phys.Res. B267, 1891 (2009) H.Naik, S.Singh, A.V.R.Reddy, V.K.Manchanda, G.Kim, K.S.Kim, M.-W.Lee, S.Ganesan, D.Raj, H.-S.Lee, Y.D.Oh, M.-H.Cho, I.S.Ko, W.Namkung Product yields for the photo-fission of 209Bi with 2.5 GeV bremsstrahlung NUCLEAR REACTIONS 209Bi(γ, F), E=2.5 GeV; 47Sc;48V;59Fe;72Zn;75Se;77Br;83Rb;85Kr;87Y;88Kr;88Zr;89Zr;91Sr;92Sr; 95Zr;97Zr;99Mo;99Rh;103Ru;105Ru;105Rh;105Ag;111Ag;111In;112Ag;115Cd;117Cd;121Te;129Sb;69Zn;74As;82Br;84Rb;90Y;95Nb;96Nb;95Tc;96Tc;101Rh;106Ag;114In;120Sb;122Sb;123Sn;124I;126Sb; Measured Eγ, Iγ, fission yields.
doi: 10.1016/j.nimb.2009.04.001
2009NA36 Eur.Phys.J. A 41, 323 (2009) H.Naik, S.Singh, A.V.R.Reddy, V.K.Manchanda, S.Ganesan, D.Raj, Md.S.Rahman, K.S.Kim, M.W.Lee, G.Kim, Y.D.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung Measurement of photo-fission yields and photo-neutron cross-sections in 209Bi with 50 and 65 MeV bremsstrahlung NUCLEAR REACTIONS 209Bi(γ, F), E=50, 65 MeV bremsstrahlung; measured fission yields; 209Bi(γ, 3n), (γ, 4n), E=50, 65 MeV bremsstrahlung; measured Eγ, Iγ, σ. Comparison with other data and TALYS code.
doi: 10.1140/epja/i2009-10812-8
2009NG01 Nucl.Instrum.Methods Phys.Res. B267, 462 (2009) V.D.Nguyen, D.K.Pham, T.T.Kim, V.L.Bui, Md.S.Rahman, K.S.Kim, G.Kim, Y.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung Thermal neutron cross-section and resonance integral of the 98Mo(n, γ)99Mo reaction NUCLEAR REACTIONS 98Mo(n, γ), E=thermal; measured Eγ, Iγ, cross section; deduced resonance integral. Compared results to existing data and evaluated databases.
doi: 10.1016/j.nimb.2008.12.003
2009OH01 Phys.Rev. C 79, 044905 (2009) Y.Oh, C.-M.Ko, S.-H.Lee, S.Yasui Ratios of heavy baryons to heavy mesons in relativistic nucleus-nucleus collisions
doi: 10.1103/PhysRevC.79.044905
2009OH02 Phys.Rev. C 79, 067902 (2009) Nuclear modification factor of nonphotonic electrons in heavy-ion collisions, and the heavy-flavor baryon-to-meson ratio
doi: 10.1103/PhysRevC.79.067902
2009OH06 Phys.Rev. C 80, 064902 (2009) Deuteron production and elliptic flow in relativistic heavy ion collisions
doi: 10.1103/PhysRevC.80.064902
2009RA25 Nucl.Instrum.Methods Phys.Res. B267, 3511 (2009) Md.S.Rahman, K.-S.Kim, M.Lee, G.N.Kim, Y.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung, N.V.Do, P.D.Khue, K.T.Thanh, T.-Ik.Ro Measurement of isomeric yield ratios for 90Zr(γ, n)89m, gZr, natZr(γ, xn1p)86m, gY, and 89Y(γ, xn)87m, g, 86m, gY reactions with 50-, 60-, and 70-MeV bremsstrahlung NUCLEAR REACTIONS Zr(γ, X)89Zr/86Y, 89Y(γ, xn)87,86Y, E=50-70 MeV; measured E\G, Iγ; deduced isomeric yields ratios.
doi: 10.1016/j.nimb.2009.08.024
2009SK03 Nucl.Instrum.Methods Phys.Res. B267, 2351 (2009) V.R.Skoy, T.F.Wang, G.N.Kim, Y.D.Oh, M.H.Cho, I.S.Ko, W.Namkung Measurement of neutron total cross-section and resonance parameters of xenon NUCLEAR REACTIONS Xe(n, X);e=0.1-40 eV; measured neutron transmission, total cross sections; deduced resonance parameters.
doi: 10.10.1016/j.nimb.2009.04.016
2008DO22 Nucl.Instrum.Methods Phys.Res. B266, 5080 (2008) N.V.Do, P.D.Khue, T.T.Kim, T.S.Le, Md.S.Rahman, K.-S.Kim, M.Lee, G.Kim, Y.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung Isomeric yield ratios for the formation of 44m, gSc in the 45Sc(γ, n), natTi(γ, xnp), natFe(γ, xn5p) and natCu(γ, xn8p) reactions with 2.5 GeV bremsstrahlung NUCLEAR REACTIONS 45Sc(γ, n), Ti(γ, X)45Sc, Fe(γ, X)45Sc, Cu(γ, X)45Sc, E < 2.5 GeV; measured Eγ, Iγ, isomeric yield ratios using the activation technique.
doi: 10.1016/j.nimb.2008.09.017
2008DO28 Nucl.Instrum.Methods Phys.Res. B 266, 863 (2008) N.V.Do, P.D.Khue, K.T.Thanh, L.T.Son, G.Kim, Y.S.Lee, Y.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung Thermal neutron cross-section and resonance integral of the 186W(n, γ)187W reaction NUCLEAR REACTIONS 186W(n, γ), E=0.0253 eV; measured products, 187W, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 31607.
doi: 10.1016/j.nimb.2008.02.021
2008NG01 Nucl.Instrum.Methods Phys.Res. B266, 21 (2008) V.D.Nguyen, D.K.Pham, T.T.Kim, T.S.Le, Y.S.Lee, G.Kim, Y.Oh, H.-S.Lee, M.-H.Cho, I.S.Ko, W.Namkung Measurement of thermal neutron cross-sections and resonance integrals for 179Hf(n, γ)180mHf and 180Hf(n, γ)181Hf reactions at the Pohang neutron facility NUCLEAR REACTIONS 179,180Hf(n, γ), E=thermal; measured Eγ, Iγ, cross sections, and resonance integrals using the stacked foil activation technique.
doi: 10.1016/j.nimb.2007.10.012
2008OH04 Phys.Rev. C 77, 045204 (2008) Nucleon and Δ resonances in KΣ(1385) photoproduction from nucleons NUCLEAR REACTIONS p(γ, K+), E=1.6-3.8 GeV; analyzed resonances, cross sections, σ(θ), photon asymmetry for Σ0(1385).
doi: 10.1103/PhysRevC.77.045204
2008WA04 Nucl.Instrum.Methods Phys.Res. B266, 561 (2008) T.F.Wang, A.K.M.M.H.Meaze, M.U.Khandaker, M.S.Rahman, G.N.Kim, L.P.Zhu, H.H.Xia, Z.Y.Zhou, Y.D.Oh, H.Kang, M.H.Cho, I.S.Ko, W.Namkung Measurement of the total neutron cross-section and resonance parameters of molybdenum using pulsed neutrons generated by an electron linac NUCLEAR REACTIONS Mo(n, X), E=0.01 - 200 eV; measured total cross sections using the neutron transmission technique. Deduced resonance parameters using the SAMMY code.
doi: 10.1016/j.nimb.2007.11.051
2007ME06 Pramana 68, 279 (2007) A.K.M.M.H.Meaze, K.Devan, Y.S.Lee, Y.D.Oh, G.N.Kim, D.Son Neutron total cross-sections and resonance parameters of Mo and Ta NUCLEAR REACTIONS Mo, Ta(n, X), E=0-100 eV; measured total σ; deduced resonance parameters. Comparison with previous results. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31594. 2007NG01 J.Korean Phys.Soc. 50, 417 (2007) V.D.Nguyen, D.K.Pham, T.T.Kim, D.T.Tran, V.D.Phung, Y.S.Lee, G.Kim, Y.Oh, H.-S.Lee, H.Kang, M.-H.Cho, I.S.Ko, W.Namkung Measurement of Isomeric Cross-Section Ratios for the 45Sc(γ, n)44m, gSc, natTi(γ, x)44m, gSc, 103Rh(γ, 4n)99m, gRh, and natFe(γ, x)52m, gMn Reactions Induced by 65-MeV Bremsstrahlung NUCLEAR REACTIONS 45Sc(γ, n), 103Rh(γ, 4n), E=65 MeV/bremsstrahlung; Ti(γ, X)44Sc, E=65 MeV/bremsstrahlung; Fe(γ, X)52Mn, E=65 MeV/bremsstrahlung; measured σ, isomer ratios. Activation method. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0716. 2007OH04 Phys.Rev. C 75, 064903 (2007) J/ψ absorption by nucleons in the meson-exchange model
doi: 10.1103/PhysRevC.75.064903
2007OH05 Nucl.Phys. A790, 498c (2007) Y.Oh, H.Haberzettl, K.Nakayama Photoproduction of Cascade Baryon NUCLEAR REACTIONS 1H(γ, 2K+X), E≈2-5 GeV; calculated total σ for Ξ-production. Relativistic meson exchange model. Comparison with data.
doi: 10.1016/j.nuclphysa.2007.03.133
2007OH06 Phys.Rev. C 76, 054910 (2007) Elliptic flow of deuterons in relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.76.054910
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
2006NA29 Phys.Rev. C 74, 035205 (2006) K.Nakayama, Y.Oh, H.Haberzettl Photoproduction of Ξ off nucleons NUCLEAR REACTIONS 1n, 1H(γ, 2K+X), (γ, 2K0X), (γ, K+K0X), E ≈ 2-5 GeV; calculated Ξ production σ, σ(θ).
doi: 10.1103/PhysRevC.74.035205
2006OH01 Phys.Rep. 423, 49 (2006) Pentaquark Θ+ (1540) production in γN → K(K-bar)N reactions NUCLEAR REACTIONS 1n, 1H(γ, K+K-), E=1-4.5 GeV; calculated σ, invariant mass spectra, pentaquark production features.
doi: 10.1016/j.physrep.2005.10.002
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
2004OH02 Phys.Rev. C 69, 025201 (2004) ρ meson photoproduction at low energies NUCLEAR REACTIONS 1H(γ, X), E=2.8, 3.28, 3.55, 3.82 GeV; calculated ρ-meson production σ(E, θ), polarization asymmetries; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.69.025201
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
2003OH08 Nucl.Phys. A721, 743c (2003) π and ρ loop corrections to ω photoproduction in the resonance region NUCLEAR REACTIONS 1H(γ, X), E=1.125-1.68 GeV; calculated ω meson production σ(θ), one-loop corrections.
doi: 10.1016/S0375-9474(03)01171-0
2002LE22 J.Phys.(London) G28, 1903 (2002) Charmonium-Hadron Interactions from QCD
doi: 10.1088/0954-3899/28/7/345
2002OH02 Phys.Rev. C65, 067901 (2002) Quarkonium-Hadron Interactions in QCD
doi: 10.1103/PhysRevC.65.067901
2002OH04 Phys.Rev. C66, 045201 (2002) One-loop corrections to ω photoproduction near threshold NUCLEAR REACTIONS 1H(γ, X), (π-, X), E=high; calculated ω production σ(θ), one-loop corrections. Coupled-channels approach, comparison with data.
doi: 10.1103/PhysRevC.66.045201
2001OH01 Phys.Rev. C63, 025201 (2001) Nucleon Resonances in ω Photoproduction NUCLEAR REACTIONS 1H(γ, X), E=1.2-4.7 GeV; calculated ω meson production associated σ(E, θ); deduced resonance contributions.
doi: 10.1103/PhysRevC.63.025201
2001OH02 Phys.Rev. C63, 034901 (2001) J/ψ Absorption by π and ρ Mesons in a Meson Exchange Model with Anomalous Parity Interactions
doi: 10.1103/PhysRevC.63.034901
2001OH04 Nucl.Phys. A684, 354c (2001) Y.Oh, A.I.Titov, S.N.Yang, T.Morii Probing Nucleon Strangeness in φ Electroproduction NUCLEAR REACTIONS 1H(polarized e, e'X), E=high; calculated φ meson production σ(E), asymmetries; deduced sensitivity to nucleon strangeness. Comparison with data.
doi: 10.1016/S0375-9474(01)00372-4
2000LE09 Phys.Lett. 475B, 207 (2000) Higher Dimension Operators and Chiral Symmetry Breaking in Nambu-Jona-Lasinio Model
doi: 10.1016/S0370-2693(00)00072-1
1999OH03 Eur.Phys.J. A 4, 363 (1999) Baryon Masses in Large Nc Chiral Perturbation Theory
doi: 10.1007/s100500050245
1999OH08 Phys.Lett. 462B, 23 (1999) Y.Oh, A.I.Titov, S.N.Yang, T.Morii Probing Nucleon Strangeness Structure with φ Electroproduction NUCLEAR REACTIONS 1H(γ, X), E not given; calculated phi-meson production σ and double polarization asymetries. Virtual photons.
doi: 10.1016/S0370-2693(99)00912-0
1998TI04 Phys.Lett. 422B, 33 (1998) Asymmetry in ω Meson Photoproduction and the Phase of ωπγ Coupling
doi: 10.1016/S0370-2693(98)00049-5
1998TI10 Phys.Rev. C58, 2429 (1998) A.I.Titov, Y.Oh, S.N.Yang, T.Morii Photoproduction of φ Mesons from the Proton: Polarization observables and strangeness in the nucleon NUCLEAR REACTIONS 1H(polarized γ, X), E ≈ 2 GeV; calculated spin observables for φ-meson production; deduced proton strangeness content related features.
doi: 10.1103/PhysRevC.58.2429
1997OH05 Z.Phys. A359, 83 (1997) Solitons Bound to Heavy Mesons
doi: 10.1007/s002180050370
1997TI01 Nucl.Phys. A618, 259 (1997) Electroproduction of a φ Meson from the Proton and the Strangeness in the Nucleon NUCLEAR REACTIONS 1H(e, eX), E=11.5 GeV; calculated σ(Q2, W, t) forφ-meson production. 1H deduced strangeness content determination related features. Uud-s(s-bar) cluster model.
doi: 10.1016/S0375-9474(97)00022-5
1997TI04 Phys.Rev.Lett. 79, 1634 (1997) Polarization Observables in φ-Meson Photoproduction and the Strangeness Content of the Proton NUCLEAR REACTIONS 1H(γ, X), E=2 GeV; analyzed σ(θ) for φ-mesons; deduced longitudinal asymmetry, direct knockout process contribution to polarization observables. Pomeron-photon analogy, relativistic harmonic oscillator quark model.
doi: 10.1103/PhysRevLett.79.1634
1991MI16 Nucl.Phys. A530, 698 (1991) Vector Mesons and Magnetic Moments of Hyperons NUCLEAR STRUCTURE 1n, 1H; calculated μ. SU(3) Skyrme model, bound state approach.
doi: 10.1016/0375-9474(91)90775-2
1991OH04 Nucl.Phys. A534, 493 (1991) Y.Oh, D.-P.Min, M.Rho, N.N.Scoccola Massive-Quark Baryons as Skyrmions Magnetic Moments NUCLEAR STRUCTURE 1n, 1H; calculated μ. Skyrmion description.
doi: 10.1016/0375-9474(91)90458-I
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