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NSR database version of May 10, 2024.

Search: Author = Y.Oh

Found 73 matches.

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2022LE15      Eur.Phys.J. A 58, 252 (2022)

T.-S.H.Lee, S.Sakinah, Y.Oh

Models of J/Ψ photo-production reactions on the nucleon

doi: 10.1140/epja/s10050-022-00901-9
Citations: PlumX Metrics


2022SO19      Phys.Rev. C 106, 055807 (2022)

S.Son, S.-I.Ando, Y.Oh

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
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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
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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
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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
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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
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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
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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
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2017KI04      Phys.Rev. C 95, 055206 (2017)

S.-H.Kim, Y.Oh, A.I.Titov

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
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2017LI09      Phys.Rev. C 95, 034311 (2017)

Ye.Lim, Y.Oh

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
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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
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2016NA01      Nucl.Phys. A946, 89 (2016)

A.Nasirov, B.Kayumov, Y.Oh

Peculiarities of quasifission reactions in heavy ion collisions

doi: 10.1016/j.nuclphysa.2015.11.013
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2016SH26      Phys.Rev. C 94, 024320 (2016)

E.Shin, Y.Lim, C.H.Hyun, Y.Oh

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
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2015AN09      Phys.Rev. C 92, 024325 (2015)

S.-I.Ando, U.Raha, Y.Oh

Investigation of the Λ bound state in pionless effective theory

doi: 10.1103/PhysRevC.92.024325
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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
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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
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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
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2014AN01      Phys.Rev. C 89, 014318 (2014)

S.-I.Ando, G.-S.Yang, Y.Oh

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
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2014AN08      Phys.Rev. C 90, 037301 (2014)

S.-I.Ando, Y.Oh

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
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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
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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
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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
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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
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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
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2010KO26      Nucl.Phys. A834, 253c (2010)

C.M.Ko, Z.W.Lin, Y.Oh

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0018.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3101.


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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23103.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31688.


2010XU01      Phys.Rev. C 81, 024910 (2010)

J.Xu, C.M.Ko, Y.Oh

Isospin-dependent pion in-medium effects on the charged-pion ratio in heavy ion collisions

doi: 10.1103/PhysRevC.81.024910
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0015.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0019.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31656.


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
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2009OH02      Phys.Rev. C 79, 067902 (2009)

Y.Oh, C.M.Ko

Nuclear modification factor of nonphotonic electrons in heavy-ion collisions, and the heavy-flavor baryon-to-meson ratio

doi: 10.1103/PhysRevC.79.067902
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2009OH06      Phys.Rev. C 80, 064902 (2009)

Y.Oh, Z.-W.Lin, C.M.Ko

Deuteron production and elliptic flow in relativistic heavy ion collisions

doi: 10.1103/PhysRevC.80.064902
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG0016.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31675.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0758.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31607.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31602.


2008OH04      Phys.Rev. C 77, 045204 (2008)

Y.Oh, C.M.Ko, K.Nakayama

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31603.


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)

Y.Oh, W.Liu, C.M.Ko

J/ψ absorption by nucleons in the meson-exchange model

doi: 10.1103/PhysRevC.75.064903
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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
Citations: PlumX Metrics


2007OH06      Phys.Rev. C 76, 054910 (2007)

Y.Oh, C.M.Ko

Elliptic flow of deuterons in relativistic heavy-ion collisions

doi: 10.1103/PhysRevC.76.054910
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23081.


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
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2006OH01      Phys.Rep. 423, 49 (2006)

Y.Oh, K.Nakayama, T.-S.H.Lee

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
Citations: PlumX Metrics


2006OH04      Phys.Rev. C 73, 065202 (2006)

Y.Oh, H.Kim

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
Citations: PlumX Metrics


2006OH05      Phys.Rev. C 74, 015208 (2006)

Y.Oh, H.Kim

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
Citations: PlumX Metrics


2004OH02      Phys.Rev. C 69, 025201 (2004)

Y.Oh, T.-S.H.Lee

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
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2004OH14      Nucl.Phys. A745, 129 (2004)

Y.Oh, H.Kim, S.H.Lee

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
Citations: PlumX Metrics


2003OH08      Nucl.Phys. A721, 743c (2003)

Y.Oh, T.-S.H.Lee

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
Citations: PlumX Metrics


2002LE22      J.Phys.(London) G28, 1903 (2002)

S.H.Lee, Y.Oh

Charmonium-Hadron Interactions from QCD

doi: 10.1088/0954-3899/28/7/345
Citations: PlumX Metrics


2002OH02      Phys.Rev. C65, 067901 (2002)

Y.Oh, S.Kim, S.H.Lee

Quarkonium-Hadron Interactions in QCD

doi: 10.1103/PhysRevC.65.067901
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2002OH04      Phys.Rev. C66, 045201 (2002)

Y.Oh, T.-S.H.Lee

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
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2001OH01      Phys.Rev. C63, 025201 (2001)

Y.Oh, A.I.Titov, T.-S.H.Lee

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
Citations: PlumX Metrics


2001OH02      Phys.Rev. C63, 034901 (2001)

Y.Oh, T.Song, S.H.Lee

J/ψ Absorption by π and ρ Mesons in a Meson Exchange Model with Anomalous Parity Interactions

doi: 10.1103/PhysRevC.63.034901
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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
Citations: PlumX Metrics


2000LE09      Phys.Lett. 475B, 207 (2000)

T.Lee, Y.Oh

Higher Dimension Operators and Chiral Symmetry Breaking in Nambu-Jona-Lasinio Model

doi: 10.1016/S0370-2693(00)00072-1
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1999OH03      Eur.Phys.J. A 4, 363 (1999)

Y.Oh, W.Weise

Baryon Masses in Large Nc Chiral Perturbation Theory

doi: 10.1007/s100500050245
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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
Citations: PlumX Metrics


1998TI04      Phys.Lett. 422B, 33 (1998)

A.I.Titov, Y.Oh

Asymmetry in ω Meson Photoproduction and the Phase of ωπγ Coupling

doi: 10.1016/S0370-2693(98)00049-5
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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
Citations: PlumX Metrics


1997OH05      Z.Phys. A359, 83 (1997)

Y.Oh, B.-Y.Park

Solitons Bound to Heavy Mesons

doi: 10.1007/s002180050370
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1997TI01      Nucl.Phys. A618, 259 (1997)

A.I.Titov, S.N.Yang, Y.Oh

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
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1997TI04      Phys.Rev.Lett. 79, 1634 (1997)

A.I.Titov, Y.Oh, S.N.Yang

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
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1991MI16      Nucl.Phys. A530, 698 (1991)

D.P.Min, Y.Koh, Y.Oh, H.K.Lee

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
Citations: PlumX Metrics


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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Note: The following list of authors and aliases matches the search parameter Y.Oh: , Y.D.OH, Y.M.OH