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NSR database version of April 11, 2024.

Search: Author = G.Yang

Found 35 matches.

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2024WA04      Phys.Rev. C 109, 014624 (2024)

K.Wang, Y.Y.Yang, Jin Lei, A.M.Moro, V.Guimaraes, J.G.Li, F.F.Duan, Z.Y.Sun, G.Yang, D.Y.Pang, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Liu, J.L.Lou, H.J.Ong, B.F.Lv, S.Guo, M.Kumar Raju, X.H.Wang, R.H.Li, X.X.Xu, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Elastic scattering and breakup reactions of the mirror nuclei 12B and 12N on 208Pb using ab initio structure inputs

doi: 10.1103/PhysRevC.109.014624
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2024YA05      Chin.Phys.C 48, 034001 (2024)

G.Yang, F.-F.Duan, K.Wang, Y.-Y.Yang, Zh.-Y.Sun, V.Guimaraes, D.-Y.Pang, W.-D.Chen, L.Jin, Sh.-W.Xu, J.-B.Ma, P.Ma, Zh.Bai, L.-H.Wang, Q.Liu, H.-J.Ong, B.-F.Lv, S.Guo, M.K.Raju, X.-H.Wang, R.-H.Li, Y.-H.Zhang, X.-H.Zhou, Zh.-G.Hu, H.-Sh.Xu

Elastic scattering of 13C and 14C isotopes on a 208Pb target at energies of approximately five times the Coulomb barriers

NUCLEAR REACTIONS 208Pb(13C, 13C), E=340 MeV; 208Pb(14C, 14C), E=294, 342 MeV; measured reaction products; deduced σ(θ) within the optical model and continuum-discretized coupled-channels (CDCC) framework. Comparison with available data. The Heavy-Ion Research Facility in Lanzhou (HIRFL), the National Laboratory of Heavy Ion Research of the Institute of Modern Physics.

doi: 10.1088/1674-1137/ad1678
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2023AG02      Phys.Lett. B 840, 137843 (2023)

A.Agarwal, H.Budd, J.Capo, P.Chong, G.Christodoulou, M.Danilov, A.Dergacheva, A.De Roeck, N.Dokania, D.Douqa, K.Dugas, S.Fedotov, S.Gwon, R.Howell, K.Iwamoto, C.Jesus-Valls, C.K.Jung, S.P.Kasetti, M.Khabibullin, A.Khotjantsev, T.Kikawa, U.Kose, Y.Kudenko, S.Kuribayashi, T.Kutter, D.Last, L.S.Lin, S.Lin, T.Lux, S.Manly, D.A.Martinez Caicedo, S.Martynenko, T.Matsubara, C.Mauger, K.McFarland, C.McGrew, A.Mefodiev, O.Mineev, T.Nakadaira, E.Noah, A.Olivier, V.Paolone, S.Palestini, A.Paul-Torres, R.Pellegrino, M.A.Ramírez, C.Riccio, J.Rodriguez Rondon, F.Sanchez, D.Sgalaberna, W.Shorrock, A.Sitraka, K.Siyeon, N.Skrobova, S.Suvorov, A.Teklu, M.Tzanov, Y.Uchida, C.Wret, G.Yang, N.Yershov, M.Yokoyama, P.Zilberman

Total neutron cross-section measurement on CH with a novel 3D-projection scintillator detector

NUCLEAR REACTIONS C, H(n, X), E=98-688 MeV; measured reaction products, En, In; deduced total neutron σ in scintillator. The neutron beamline at Los Alamos National Laboratory (LANL).

doi: 10.1016/j.physletb.2023.137843
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2023AN14      Sci. Rep. 13, 12657 (2023)

Z.An, W.Qiu, W.Jiang, G.Yang, X.Li, Z.Liao, Z.Zhuang, X.Zhang, S.Chen, C.Guo, E.Xiao, X.Fang, X.Li, H.Wang, X.Hu, Bi.Jiang, W.Shen, J.Wang, J.Ren, X.Ruan, D.Wang, S.-Y.Zhang, W.Luo, Z.Zhu, H.Lan, Z.Cao, X.Ma, Y.Liu, P.Wang, Y.Yang, P.Su, X.Deng, W.He, Y.Ma, C.Ma, Y.Wang, P.He, R.Tang, T.Zhou, J.Wang, H.Yi, Y.Zhang, Y.Chen, R.Fan, K.Gao, Q.Li, K.Sun, Z.Tan, M.Gu, H.Jing, J.Tang

Measurement of the 181Ta(n, γ) cross sections up to stellar s-process temperatures at the CSNS Back-n

NUCLEAR REACTIONS 181Ta(n, γ), E=0.001-800 keV; measured reaction products, En, In, TOF; deduced σ, resonance parameters using the R-Matrix code SAMMY, Maxwellian average cross sections (MACS). Comparison with available data. The back-streaming white neutron facility (Back-n) of China spallation neutron source (CSNS).

doi: 10.1038/s41598-023-39603-7
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2023AN15      J.Phys.(London) G50, 120501 (2023)

A.M.Ankowski, A.Ashkenazi, S.Bacca, J.L.Barrow, M.Betancourt, A.Bodek, M.E.Christy, L.Doria, S.Dytman, A.Friedland, O.Hen, C.J.Horowitz, N.Jachowicz, W.Ketchum, T.Lux, K.Mahn, C.Mariani, J.Newby, V.Pandey, A.Papadopoulou, E.Radicioni, F.Sanchez, C.Sfienti, J.M.Udias, L.Weinstein, L.Alvarez-Ruso, J.E.Amaro, C.A.Arguelles, A.B.Balantekin, S.Bolognesi, V.Brdar, P.Butti, S.Carey, Z.Djurcic, O.Dvornikov, S.Edayath, S.Gardiner, J.Isaacson, W.Jay, A.Klustova, K.S.McFarland, A.Nikolakopoulos, A.Norrick, S.Pastore, G.Paz, M.H.Reno, I.Ruiz Simo, J.E.Sobczyk, A.Sousa, N.Toro, Y.-D.Tsai, M.Wagman, J.G.Walsh, G.Yang

Electron scattering and neutrino physics

doi: 10.1088/1361-6471/acef42
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2023XI05      Nat.Phys. 19, 904 (2023)

T.-Y.Xia, W.-W.Sun, S.Ebser, W.Jiang, G.-M.Yang, H.-M.Yang, H.-M.Zhu, Y.-C.Fu, F.Huang, G.-D.Ming, T.Xia, Z.-T.Lu

Atom-trap trace analysis of 41Ca/Ca down to the 1017 level

ATOMIC MASSES 41Ca, Ca; measured frequencies; deduced the 41Ca/Ca ratio of a sample and uncertainties, precision. A table-top atom-trap trace analysis (ATTA) system, a magneto-optical trap.

doi: 10.1038/s41567-023-01969-w
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2023YA10      Phys.Rev. C 107, 044603 (2023)

G.Yang, D.Y.Pang, Y.Y.Yang, K.Wang, F.F.Duan, X.X.Wang, Z.Y.Sun

Systematic single-folding model nucleus-nucleus potential for peripheral collisions

NUCLEAR REACTIONS 16O(9Be, 9Be), E=20-157.7 MeV;27Al(9Be, 9Be), E=12-158.2 MeV;28Si(9Be, 9Be), E=13-201.6 MeV;40Ca(9Be, 9Be), E=45-158.1 MeV;60Ni(9Be, 9Be), E=158.2 MeV;64Zn(9Be, 9Be), E=19-28.97 MeV;80Se(9Be, 9Be), E=20.94-32.76 MeV;120Sn(9Be, 9Be), E=25.96-49.96 MeV;144Sm(9Be, 9Be), E=30.0-48.0 MeV;197Au(9Be, 9Be), E=36.94-158.2 MeV;208Pb(9Be, 9Be), E=37.8-88.00 MeV;209Bi(9Be, 9Be), E=37.8-48.0 MeV; analyzed experimental data on elastic scattering angular distributions of 9Be on different targets; deduced systematic nucleus-nucleus potential. 16O, 26Mg, 27Al, 28Si, 40Ca, 60Ni, 64Zn, 80Se, 89Y, 120Sn, 144Sm, 197Au, 208Pb, 209Bi(9Be, 9Be), E=12-158.2 MeV; 28Si, 40Ca, 54,56Fe, 58,60Ni, 64Zn, 89Y, 90Zr, 116,118Sn, 144Sm, 208Pb, 209Bi, 238U(7Li, 7Li), E=16-240; 16O, 26Mg, 28Si, 40Ca, 56Fe, 62Ni, 70Ge(14N, 14N), E=28-76 MeV; 124Sn, 208Pb(17O, 17O), E=340 MeV; 58Ni(20Ne, 20Ne), E=291, 340 MeV; 27Al(15N, 15N), E=32.82, 47.91, 62.07 MeV; 208Pb(24Ne, 24Ne), E=189.6 MeV; 27Al, 28Si, 56Fe, 92Zr, 116Sn(16O, 16O), E=31-64 MeV; 56Fe, 58Ni, 64Zn, 112,118,120Sn(18O, 18O), E=46-60 MeV; 64Zn, 208Pb, (10Be, 10Be), E=28-43 MeV; 64Zn, 208Pb, 209Bi, 197Au(11B, 11B), E=55-84 MeV; 28Si(13C, 13C), E=25, 60 MeV;16O, 40Ca, 56Fe, 60Ni, 66Zn, 88Sr, 92,100Mo, 138Ba, (14C, 14C), E=51, 64, 71 MeV; 58Ni(17F, 17F), E=43.5, 55.6, 62, 97 MeV; 208Pb(19F, 19F), E=96 MeV; 58Ni(8B, 8B), E=20.68-29.26 MeV; 12C(8B, 8B), E=25.8 MeV; 9Be(7Li, 7Li), E=24, 30 MeV; 9Be(6Li, 6Li), E=11.67, 20.0 MeV; 12C(6Li, 6Li), E=12.3 MeV; 12C(9Be, 9Be), E=14 MeV; 208Pb(8B, 8B), E=170, 178, 238 MeV; 208Pb(9C, 9C), E=227 MeV; calculated σ(θ). 27Al, 28Si, 58Ni, 59Co, 208Pb, 209Bi(6Li, 6Li), 28Si, 59Co, 208Pb(7Li, 7Li), 58Ni(7Be, 7Be), 28Si, 144Sm(9Be, 9Be), E=8-58 MeV; 12C, 28Si, 40Ca, 58Ni, 90Zr, 208Pb(6Li, 6Li), E=35 MeV/nucleon; 12C, 27Al, 64Zn, 93Nb, 107Ag, 118Sn, 150,154Sm, 181Ta, 208Pb(20Ne, 20Ne), E=30 MeV/nucleon; 12C, 27Al, 51V, 54Fe, 107Ag, 118Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; calculated total σ. Comparison to experimental data and calculation results performed with Sao Paulo potential of version 2. Analysis is performed by using a single-folding model based on the Bruyeres Jeukenne-Lejeune-Mahaux model nucleon-nucleus potentials.

doi: 10.1103/PhysRevC.107.044603
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2022CH32      Phys.Rev. A 105, 063108 (2022)

Y.-Q.Chu, Z.-F.Wan, F.Ritterbusch, W.-K.Hu, J.-Q.Gu, S.-M.Hu, Z.-H.Jia, W.Jiang, Z.-T.Lu, L.-T.Sun, A.-M.Tong, J.S.Wang, G.-M.Yang

Optically enhanced discharge excitation and trapping of 39Ar

ATOMIC PHYSICS 39Ar; measured frequencies; deduced loading rate in an atom trap by enhancing the generation of metastable atoms in a discharge source. Comparison with calculations.

doi: 10.1103/PhysRevA.105.063108
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2022DU05      Phys.Rev. C 105, 034602 (2022)

F.F.Duan, Y.Y.Yang, J.Lei, K.Wang, Z.Y.Sun, D.Y.Pang, J.S.Wang, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, Z.H.Gao, X.X.Xu, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, G.Yang, S.Y.Jin, Z.Z.Ren, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Elastic scattering and breakup reactions of neutron-rich nucleus 11Be on 208Pb at 210 MeV

NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, 10Be), E=210 MeV; measured reaction products; deduced σ(θ), σ. Comparison with CDCC calculations and experimental results for other reaction systems including tightly- and weakly-bound projectiles impinging on medium to heavy mass targets. Beam by Heavy-Ion Research Facility in Lanzhou (HIRFL, China).

doi: 10.1103/PhysRevC.105.034602
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2022GU07      Phys.Rev.Lett. 128, 242502 (2022)

S.Guo, B.Ding, X.H.Zhou, Y.B.Wu, J.G.Wang, S.W.Xu, Y.D.Fang, C.M.Petrache, E.A.Lawrie, Y.H.Qiang, Y.Y.Yang, H.J.Ong, J.B.Ma, J.L.Chen, F.Fang, Y.H.Yu, B.F.Lv, F.F.Zeng, Q.B.Zeng, H.Huang, Z.H.Jia, C.X.Jia, W.Liang, Y.Li, N.W.Huang, L.J.Liu, Y.Zheng, W.Q.Zhang, A.Rohilla, Z.Bai, S.L.Jin, K.Wang, F.F.Duan, G.Yang, J.H.Li, J.H.Xu, G.S.Li, M.L.Liu, Z.Liu, Z.G.Gan, M.Wang, Y.H.Zhang

Probing 93mMo Isomer Depletion with an Isomer Beam

RADIOACTIVITY 93Mo(IT) [from 12C(86Kr, 5n), E=559 MeV]; measured decay products, Eγ, Iγ; deduced γ-ray energies and relative intensities, lack of isomer depletion, excitation probability. Comparison with available data. Nuclear excitation by electron capture (NEEC).

doi: 10.1103/PhysRevLett.128.242502
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022LI72      Phys.Rev. C 106, 065804 (2022)

X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, D.X.Wang, S.Y.Zhang, G.L.Yang, X.K.Li, Z.D.An, J.J.He, W.Luo, X.G.Cao, L.L.Song, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, Y.D.Liu, C.W.Ma, Y.T.Wang, J.Su, L.Y.Zhang, Y.X.Yang, S.Feng, W.B.Liu, W.Q.Su, S.Jin, K.J.Chen

Experimental determination of the neutron resonance peak of 162Er at 67.8 eV

NUCLEAR REACTIONS 162Er(n, γ), E=20-100 eV; measured Eγ, Iγ; deduced neutron-capture yield, resonances, decay widths. Resonance parameters at 67.8 eV are extracted for the first time. R-matrix analysis. Comparison to other experimental results and ENDF/B-VIII.0 data. 4 C6D6 detectors. Neutron beam from Back-n Facility of the CSNS.

doi: 10.1103/PhysRevC.106.065804
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2022WA16      Phys.Rev. C 105, 054616 (2022)

K.Wang, Y.Y.Yang, V.Guimaraes, D.Y.Pang, F.F.Duan, Z.Y.Sun, J.Lei, G.Yang, S.W.Xu, J.B.Ma, Q.Liu, Z.Bai, H.J.Ong, B.F.Lv, S.Guo, X.H.Wang, R.H.Li, M.Kumar Raju, Z.G.Hu, H.S.Xu

Elastic scattering investigation of radioactive 13B and 13O projectiles on a 208Pb target at intermediate energies

NUCLEAR REACTIONS 208Pb(13B, 13B), E=254 MeV; 208Pb(13O, 13O), E=413 MeV; measured reaction products, time-of-flight, magnetic rigidity, angular distributions; deduced σ(θ). 13B, 13O; deduced proton, neutron and matter rms radii. Optical model analysis with Sao Paulo and Pang global potentials. Comparison to continuum discretized coupled channels (CDCC) calculations. Beams were produced by fragmentation of a primary 59.54 MeV/nucleon 16O beam delivered by the Heavy-Ion Research Facility in Lanzhou (HIRFL).

doi: 10.1103/PhysRevC.105.054616
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022YA21      Phys.Rev. C 106, 024325 (2022)

G.L.Yang, B.Qi, X.D.Wang, C.Qi

Neutron-proton interaction in odd-odd nuclei from statistical analysis

NUCLEAR STRUCTURE A=4-260; analyzed experimental binding energy data extracted from AME2020; deduced proton-neutron interactions, correlations for pn-interactions between neighboring nuclei. Additional attractive np-interaction which persists between the last proton and last neutron in odd-odd nuclei resulted from statistical analysis.

doi: 10.1103/PhysRevC.106.024325
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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
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2021WA12      Phys.Rev. C 103, 024606 (2021)

K.Wang, Y.Y.Yang, A.M.Moro, V.Guimaraes, J.Lei, D.Y.Pang, F.F.Duan, J.L.Lou, J.C.Zamora, J.S.Wang, Z.Y.Sun, H.J.Ong, X.Liu, S.W.Xu, J.B.Ma, P.Ma, Z.Bai, Q.Hu, X.X.Xu, Z.H.Gao, G.Yang, S.Y.Jin, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu, for the RIBLL Collaboration

Elastic scattering and breakup reactions of the proton drip-line nucleus 8B on 208Pb at 238 MeV

NUCLEAR REACTIONS 208Pb(3He, 3He), E=55 MeV; 208Pb(8B, 8B), (8B, X), E=238 MeV; 208Pb(7Be, 7Be), (7Be, X), E=175 MeV, [3He, 7Be and 8B secondary beams from 9Be(12C, X), E=59.7 MeV primary reaction followed by ΔE-E particle identification of fragments at RIBLL-HIRFL-Lanzhou facility]; measured reaction products, particle spectra, using double-sided silicon strip detectors (DSSDs) and a CsI(Tl) crystal array; deduced σ(θ) for elastic scattering and inelastic breakup (NEB) of 8B and 7Be, no significant Coulomb rainbow suppression. Comparison with optical model and continuum discretized coupled channels (CDCC) calculations.

doi: 10.1103/PhysRevC.103.024606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0265.


2020DU02      Chin.Phys.C 44, 024001 (2020)

F.-F.Duan, Y.-Y.Yang, D.-Y.Pang, B.-T.Hu, J.-S.Wang, K.Wang, G.Yang, V.Guimaraes, P.Ma, S.-W.Xu, X.-Q.Liu, J.-B.Ma, Z.Bai, Q.Hu, S.-Y.Jin, X.-X.Sun, J.-S.Yao, H.-K.Qi, Z.-Y.Sun

Experimental study of the elastic scattering of 10Be on 208Pb at the energy of around three times the Coulomb barrier

NUCLEAR REACTIONS 208Pb(8Be, 8Be), E=127 MeV; measured reaction products; deduced σ, optical model parameters.

doi: 10.1088/1674-1137/44/2/024001
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0229.


2020DU18      Phys.Lett. B 811, 135942 (2020)

F.F.Duan, Y.Y.Yang, K.Wang, A.M.Moro, V.Guimaraes, D.Y.Pang, J.S.Wang, Z.Y.Sun, J.Lei, A.Di Pietro, X.Liu, G.Yang, J.B.Ma, P.Ma, S.W.Xu, Z.Bai, X.X.Sun, Q.Hu, J.L.Lou, X.X.Xu, H.X.Li, S.Y.Jin, H.J.Ong, Q.Liu, J.S.Yao, H.K.Qi, C.J.Lin, H.M.Jia, N.R.Ma, L.J.Sun, D.X.Wang, Y.H.Zhang, X.H.Zhou, Z.G.Hu, H.S.Xu

Scattering of the halo nucleus 11Be from a lead target at 3.5 times the Coulomb barrier energy

NUCLEAR REACTIONS 208Pb(11Be, 11Be), (11Be, X), E=140 MeV; 208Pb(10Be, X), (10Be, X), E=127 MeV; 208Pb(9Be, 9Be), (9Be, X), E=88 MeV; measured reaction products. 9,10,11Be; deduced σ(θ), σ(E), σ. Comparison with continuum discretized coupled channel (CDCC) as well as by the XCDCC calculations.

doi: 10.1016/j.physletb.2020.135942
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0235.


2020XU02      Phys.Rev. C 101, 024609 (2020)

S.Xu, G.Yang, M.Jin, J.Su

Probing the deuteron breakup and linking the cross sections of residue production between the neutron- and deuteron-induced spallation at 500 MeV/nucleon

NUCLEAR REACTIONS 56Fe, 115In(p, X), E=800, 1500 MeV/nucleon; 137Cs(d, X), E=500 MeV/nucleon; calculated double-differential σ(θ, E) for neutron production, correlation of longitudinal momenta between neutron and proton from the deuteron, contributions of deuteron absorbing, neutron stripping, proton stripping, and elastic breakup of deuteron to the energy distribution of neutrons. 2H(137Cs, X), E=500 MeV/nucleon; calculated transverse momentum vs longitudinal momentum of neutrons and proton in d+137Cs spallation. 1,2H(136Xe, X), E=500 MeV/nucleon; calculated isotopic production cross sections of residual nuclei with Z=41-56 and N-Z=8-30. 1n, 2H(137Cs, X), E=500 MeV/nucleon; calculated isotopic production cross sections of residual nuclei with Z=33-56 and N-Z=4-30. Isospin-dependent quantum molecular dynamics (IQMD) model for the spallation process, and statistical model GEMINI based on the Hauser-Feshbach formalism to describe the deexcitation of the hot fragments. Comparison with available experimental data.

doi: 10.1103/PhysRevC.101.024609
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2019YA14      Chin.Phys.C 43, 104101 (2019)

G.Yang, S.Xu, M.Jin, J.Su

Prediction of the cross-sections of isotopes produced in deuteron-induced spallation of long-lived fission products

NUCLEAR REACTIONS 90Sr, 93Zr, 107Pd, 137Cs(d, X), E=200, 500, 1000 MeV/nucleon; calculated σ. Comparison with available data.

doi: 10.1088/1674-1137/43/10/104101
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2017YA30      Sci. Rep. 7, 15369 (2017)

G.Yang, H.Tazoe, M.Yamada

Can 129I track 135Cs, 236U, 239Pu, and 240Pu apart from 131I in soil samples from Fukushima Prefecture, Japan?

doi: 10.1038/s41598-017-15714-w
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2017YA31      Sci. Rep. 7, 13619 (2017)

G.Yang, H.Tazoe, K.Hayano, K.Okayama, M.Yamada

Isotopic compositions of 236U, 239Pu, and 240Pu in soil contaminated by the Fukushima Daiichi Nuclear Power Plant accident

doi: 10.1038/s41598-017-13998-6
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2016RA23      Eur.Phys.J. A 52, 194 (2016)

Md.S.Rahman, K.Kim, G.Kim, H.Naik, M.Nadeem, N.T.Hien, M.Shahid, S.-C.Yang, Y.-S.Cho, Y.-O.Lee, Y.-O.Lee, S.-G.Shin, M.-H.Cho, M.W.Lee, Y.-R.Kang, G.-M.Yang, T.-I.Ro

Measurement of flux-weighted average cross-sections and isomeric yield ratios for 103Rh(γ, xn) reactions in the bremsstrahlung end-point energies of 55 and 60 MeV

NUCLEAR REACTIONS 103Rh(γ, xn), E=55, 60 MeV[end-point energy]; measured bremsstrahlung induced Eγ, Iγ; deduced 103Rh(γ, xn, x=1-4) reaction flux-weighted average σ, isomeric ratios; calculated σ using TALYS 1.6. For comparison of data with calculations, present data are complemented by those of Lepretre (at lower energies).

doi: 10.1140/epja/i2016-16194-x
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetG3131.


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

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

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

doi: 10.1103/PhysRevC.92.035206
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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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2013YA25      Sci. Rep. 3, 1596 (2013)

G.-M.Yang, C.-F.Cheng, W.Jiang, Z.-T.Lu, R.Purtschert, Y.-R.Sun, L.-Y.Tu, S.-M.Hu

Analysis of 85Kr: a comparison at the 10-14 level using micro-liter samples

doi: 10.1038/srep01596
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2011TI08      Int.J.Mod.Phys. E20, 1755 (2011)

J.Tian, L.Ou, H.Hao, G.Yang, C.Bai

Dynamical shell effect in the fusion reactions

NUCLEAR REACTIONS 40Ca(48Ca, X)88Zr, 48Ca(48Ca, X)96Zr, 16O(208Pb, X)224Th, 48Ca(208Pb, X)256No, E not given; calculated fusion barriers, σ. ImQMD model, comparison with experimental data.

doi: 10.1142/S0218301311019556
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2005DZ03      J.Res.Natl.Inst.Stand.Technol. 110, 339 (2005)

S.N.Dzhosyuk, A.Copete, J.M.Doyle, L.Yang, K.J.Coakley, R.Golub, E.Korobkina, T.Kreft, S.K.Lamoreaux, A.K.Thompson, G.L.Yang, P.R.Huffman

Determination of the Neutron Lifetime Using Magnetically Trapped Neutrons

RADIOACTIVITY 1n(β-); measured T1/2. Comparison with previous results.

doi: 10.6028/jres.110.050
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2005KI12      Nucl.Phys. A755, 419c (2005)

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

Magnetic moments of exotic pentaquark baryons

doi: 10.1016/j.nuclphysa.2005.03.133
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2002CO15      Phys.Rev. C65, 064612 (2002)

K.J.Coakley, G.L.Yang

Estimation of the Neutron Lifetime: Comparison of Methods which Account for Background

RADIOACTIVITY 1n(β-); analyzed background effects in T1/2 determination.

doi: 10.1103/PhysRevC.65.064612
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2001YA01      Phys.Rev. C63, 014602 (2001)

G.L.Yang, K.J.Coakley

Likelihood Models for Two-Stage Neutron Lifetime Experiments

RADIOACTIVITY 1n(β-); calculated uncertainties in lifetime determination. Two-stage experiment, likelihood models.

doi: 10.1103/PhysRevC.63.014602
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2000AN10      Nucl.Phys. A663-664, 545c (2000)

B.D.Anderson, O.Osadchy, J.Sowinski, A.R.Baldwin, W.Franklin, J.W.Watson, S.Wissink, M.Wolanski, G.Yang, W.Glockle, H.Witala

Cross-Section and Analyzing-Power Measurements for the 2H(n, pn)n Reaction at 189 MeV

NUCLEAR REACTIONS 2H(polarized n, n), (polarized n, np), E=189 MeV; measured Ay(θ). Comparison with p-d reaction.

doi: 10.1016/S0375-9474(99)00652-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13953.


1991YA10      Nucl.Instrum.Methods Phys.Res. B61, 175 (1991)

G.Yang, F.Zhu, H.Xu, H.Pan

Proton Elastic Scattering for Light Element Cross Section Enhancement with E(p) > 2.5 MeV

NUCLEAR REACTIONS 12C, N, 16O(p, p), E=2.5-3.6 MeV; measured σ(θ=170°) vs E.

doi: 10.1016/0168-583X(91)95457-O
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0569.


1976YA01      Phys.Rev. C13, 1376 (1976)

G.C.Yang, P.P.Singh, A.van der Woude, A.G.Drentje

Isoscalar Multipole Strength in 24Mg Through Inelastic Alpha Scattering

NUCLEAR REACTIONS 24Mg(α, α'), E=70 MeV; measured σ(Eα', θ). 24Mg deduced quadrupole, octupole, hexadecapole strength. DWBA. Enriched targets.

doi: 10.1103/PhysRevC.13.1376
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1968YA06      Bull.Am.Phys.Soc. 13, No.3, 435, DH8 (1968)

G.C.Yang, J.B.Sampson

Electron Spin Resonance of Ru in TiO2

NUCLEAR STRUCTURE 101Ru, 99Ru; measured not abstracted; deduced nuclear properties.


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Note: The following list of authors and aliases matches the search parameter G.Yang: , G.C.YANG, G.L.YANG, G.M.YANG, G.S.YANG