NSR Query Results


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NSR database version of April 11, 2024.

Search: Author = D.Y.Pang

Found 95 matches.

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2024WA03      Phys.Rev. C 109, 014621 (2024)

Y.H.Wang, D.Y.Pang, W.D.Chen, Y.P.Xu, W.L.Hai, R.Y.Chen

Nuclear radii from total reaction cross section measurements at intermediate energies with complex turning point corrections to the eikonal model

doi: 10.1103/PhysRevC.109.014621
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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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2023CH28      Phys.Rev. C 107, 064610 (2023)

W.Chen, D.Y.Pang, H.Guo, Y.Tao, W.Sun, Y.J.Ying

Continuum-discretized coupled-channels calculations for 6Li fusion reactions with closed channels

NUCLEAR REACTIONS 28Si(6Li, X), E(cm)=4-20 MeV;64Ni(6Li, X), E(cm)=11-25 MeV;144Sm(6Li, X), E(cm)=19-37 MeV;209Bi(6Li, X), E=28-48 MeV; calculated total and complete fusion σ(E), partial-wave fusion σ for J up to 30. 2H(α, α), E(cm)<8 MeV; calculated scattering phase-shift. 6Li(e, e'), E not given; calculated charge form factors. Continuum-discretized coupled-channels method. Comparison to available experimental data.

doi: 10.1103/PhysRevC.107.064610
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2023XI11      Phys.Rev. C 108, 064605 (2023)

B.L.Xia, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, W.Liu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, H.Y.Ge, W.W.Wan

Search for the missing d-wave neutron excitation states in 13B

doi: 10.1103/PhysRevC.108.064605
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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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2023YA30      Phys.Rev.Lett. 131, 242501 (2023)

Z.H.Yang, Y.L.Ye, B.Zhou, H.Baba, R.J.Chen, Y.C.Ge, B.S.Hu, H.Hua, D.X.Jiang, M.Kimura, C.Li, K.A.Li, J.G.Li, Q.T.Li, X.Q.Li, Z.H.Li, J.L.Lou, M.Nishimura, H.Otsu, D.Y.Pang, W.L.Pu, R.Qiao, S.Sakaguchi, H.Sakurai, Y.Satou, Y.Togano, K.Tshoo, H.Wang, S.Wang, K.Wei, J.Xiao, F.R.Xu, X.F.Yang, K.Yoneda, H.B.You, T.Zheng

Observation of the Exotic 0+2 Cluster State in 8He

NUCLEAR REACTIONS C, 1H(8He, 8He), E=82.3 MeV/nucleon; measured reaction products, En, In. 6,8He; deduced σ(θ), resonant state J, π, large isoscalar monopole transition strength, and the emission of a strongly correlated neutron pair. Comparison with theoretical calculations. RIPS beam line of RIKEN Nishina Center.

doi: 10.1103/PhysRevLett.131.242501
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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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2022LI15      Phys.Rev. C 105, 034613 (2022)

W.Liu, J.L.Lou, Y.L.Ye, S.M.Wang, Z.W.Tan, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, H.Y.Zhu, B.L.Xia

New investigation of low-lying states in 12Be via a 2H(13B, 3He) reaction

NUCLEAR REACTIONS 2H(13B, d), (13B, 3He), E=23 MeV/nucleon; measured reaction products, deuteron spectra, 3He spectra, angular distributions; deduced σ(θ), optical potential parameters. 12Be; deduced levels, J, π, spectroscopic factors, resonance widths. DWBA analysis. Comparison to various calculations in particular to one using the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach (for the resonance widths). Secondary beam from 18O(9Be, X), E=60 MeV/nucleon (RCNP, Osaka).

doi: 10.1103/PhysRevC.105.034613
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022LI47      Phys.Rev. C 106, 025807 (2022)

X.Y.Li, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, J.J.He, S.Q.Yan, Q.W.Fan, J.C.Liu, L.Gan, Z.Y.Han, E.T.Li, G.Lian, Y.P.Shen, Y.B.Wang, S.Zeng, W.P.Liu

Astrophysical 15N(n, γ)16N reaction rate from precision measurement of the 15N(d, p)16N angular distributions

NUCLEAR REACTIONS 15N(d, p), (d, d), E=15 MeV; measured particle spectra, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA and ADWA analysis. 15N(n, γ), T=0.01-10 GK; deduced astrophysical reaction rates; calculated σ(E). Comparison with previous experimental results, and with OXBASH shell-model predictions.

doi: 10.1103/PhysRevC.106.025807
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Data from this article have been entered in the XUNDL database. For more information, click here.


2022SU23      Phys.Rev. C 106, 034614 (2022)

Y.Z.Sun, S.T.Wang, Y.P.Xu, D.Y.Pang, J.G.Li, C.X.Yuan, L.F.Wan, Y.Qiao, Y.Q.Wang, X.Y.Chen

Spectroscopic strength reduction of intermediate-energy single-proton removal from oxygen isotopes

NUCLEAR STRUCTURE C(13O, p), E=397 MeV/nucleon;C(14O, p), E=305, 349 MeV/nucleon;C(15O, p), E=308 MeV/nucleon;C(16O, p), E=450 MeV/nucleon;C(17O, p), E=629 MeV/nucleon;C(18O, p), E=573 MeV/nucleon;C(19O, p), E=635 MeV/nucleon;C(20O, p), E=415 MeV/nucleon;C(22O, p), E=414 MeV/nucleon; calculated inclusive single-proton removal σ, shell-model spectroscopic factors, reduction factors of the spectroscopic factors with the experimental data. Glauber reaction model calculations performed with MOMDIS code. Comparison to experimental data obtained at GSI and ETF(Lanzhou, China).

doi: 10.1103/PhysRevC.106.034614
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2022TA09      Chin.Phys.C 46, 054001 (2022)

Z.W.Tan, J.L.Lou, Y.L.Ye, Y.Liu, D.Y.Pang, C.X.Yuan, J.G.Li, W.Liu, Y.Jiang, B.Yang, L.C.Tao, K.Ma, Z.H.Li, Q.T.Li, X.F.Yang, J.Y.Xu, H.Z.Yu, J.X.Han, S.W.Bai, S.W.Huang, G.Li, H.Y.Wu, H.L.Zang, J.Feng, J.S.Wang, Y.Y.Yang, P.Ma, Q.Hu, Z.Bai, Z.H.Gao, F.F.Duan, L.Y.Hu, J.H.Tan, S.Q.Sun, Y.S.Song, H.J.Ong, D.T.Tran, H.Y.Zhu, B.L.Xia

Investigation of negative-parity states in 16C via deuteron inelastic scattering

NUCLEAR REACTIONS 16C(d, d'), E=59.6 MeV/nucleon; measured reaction products; deduced σ(θ), optical model potentials, deformation lengths, energy levels, J, π. Comparison with the distorted-wave Born approximation (DWBA) and shell model calculations. The Radioactive Ion Beam Line in Lanzhou (RIBLL), Institute of Modern Physics (IMP), China.

doi: 10.1088/1674-1137/ac488b
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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.


2022XU07      Chin.Phys.C 46, 064102 (2022)

Y.-P.Xu, D.-Y.Pang, C.-X.Yuan, X.-Y.Yun

Quenching of single-particle strengths of carbon isotopes 9-12, 14-20C with knockout reactions for incident energies 43-2100 MeV/nucleon

NUCLEAR REACTIONS 9Be, C(9C, 8C), (10C, 9C), (11C, 10C), (12C, 11C), (14C, 13C), (15C, 14C), (16C, 15C), (17C, 16C), (18C, 17C), (19C, 18C), (20C, 19C), E=43-2100 MeV/nucleon; analyzed available data; deduced the quenching of single-particle strengths of carbon isotopes, dependence on the proton-neutron asymmetry.

doi: 10.1088/1674-1137/ac5236
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2021CH17      Phys.Rev. C 103, L031302 (2021)

J.Chen, S.M.Wang, H.T.Fortune, J.L.Lou, Y.L.Ye, Z.H.Li, N.Michel, J.G.Li, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, D.Y.Pang, F.R.Xu, W.Zuo, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, H.J.Ong, E.Ideguchi, Y.Ayyad, K.Hatanaka, D.T.Tran, D.Bazin, J.Lee, Y.N.Zhang, J.Wu, H.N.Liu, C.Wen, T.Yamamoto, M.Tanaka, T.Suzuki

Observation of the near-threshold intruder 0- resonance in 12Be

NUCLEAR REACTIONS 2H(11Be, p)12Be, E=26.9 MeV/nucleon; measured E(p), I(p), σ(θ) using two parallel-plate avalanche counters (PPACs), and a set of annular double-sided silicon detectors (ADSSDs) at the RCNP, Osaka University. 12Be; deduced missing-mass spectra of 12Be unbound states, levels, J, π, a 0- resonance just above S(n), decay width. DWBA analysis. Comparison with Gamow coupled-channel and Gamow shell-model calculations.

doi: 10.1103/PhysRevC.103.L031302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2690. Data from this article have been entered in the XUNDL database. For more information, click here.


2021LI17      Eur.Phys.J. A 57, 46 (2021)

Y.Li, D.Y.Pang

Elastic scattering angular distributions of neutron halo nucleus 11Be studied via dynamic polarization potentials

NUCLEAR REACTIONS 208Pb(11Be, 11Be), E=140 MeV; analyzed available data. 11Be; deduced σ, dynamic polarization potentials. CDCC calculations.

doi: 10.1140/epja/s10050-021-00360-8
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2021LI64      Phys.Rev. C 104, 064605 (2021)

W.Liu, J.L.Lou, Y.L.Ye, Z.H.Li, Q.T.Li, H.Hua, X.F.Yang, J.Y.Xu, H.J.Ong, D.T.Tran, N.Aoi, E.Ideguchi, D.Y.Pang, C.X.Yuan, S.M.Wang, Y.Jiang, B.Yang, Y.Liu, J.G.Li, Z.Q.Chen, J.X.Han, S.W.Bai, G.Li, K.Ma, Z.W.Tan, H.Y.Zhu, B.L.Xia

s- and d-wave intruder strengths in 13Bg.s. via the 1H(13B, d)12B reaction

NUCLEAR REACTIONS 1H(13B, p), (13B, d)12B, E=23 MeV/nucleon, [13B secondary beam from 9Be(18O, X), E=58 MeV/nucleon]; measured reaction products, E(d), I(d), E(p), I(p), σ(θ), (particle)(particle)-coin using four sets of charged-particle telescopes of double-sided silicon strip (DSSD) detectors at RCNP-Osaka accelerator facility. 12,13B; analyzed optical potential parameters for low energy elastic scattering and single-neutron transfer reaction. 13B; deduced levels, J, π, L-transfers from σ(θ) distributions relative spectroscopic factors, s- and d-wave intruder strengths in the ground state; calculated p-, s-, and d-wave intensities from the shell model with the YSOX interaction and Gamow coupled-channel (GCC) approach. Comparison with systematics of p-, s-, and d-wave intensities in the ground state of 12Be, 13B and 14C.

doi: 10.1103/PhysRevC.104.064605
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Data from this article have been entered in the XUNDL database. For more information, click here.


2021SU15      Phys.Rev. C 104, 014310 (2021)

Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, S.Y.Jin, Y.X.Zhao, D.Y.Pang, S.W.Tang, D.Yan, P.Ma, Y.H.Yu, K.Yue, F.Fang, Y.J.Zhang, C.G.Lu, L.M.Duan

Single-neutron removal from 14, 15, 16C near 240 MeV/nucleon

NUCLEAR REACTIONS C(14C, 13C), E=235 MeV/nucleon; C(15C, 14C), E=237 MeV/nucleon; C(16C, 15C), E=239 MeV/nucleon, [secondary 14,15,16C beams from 9Be(18O, X), E=280 MeV/nucleon primary reactions, followed by separation of fragments using RIBLL2 at the HIRFL-CSR-Lanzhou facility]; measured reaction products, particle identification spectra for neutron-removal products using ionization chambers and plastic scintillators. 13,14,15C; deduced levels, J, π, inclusive single-nucleon removal σ, isospin asymmetry dependence of the reduction factor (σ(exp)/σ(theory)). Comparison with Glauber model predictions using shell-model spectroscopic factors.

doi: 10.1103/PhysRevC.104.014310
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0277.


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.


2020JI04      Phys.Rev. C 101, 031304 (2020)

W.Jiang, Y.L.Ye, C.J.Lin, Z.H.Li, J.L.Lou, X.F.Yang, Q.T.Li, Y.C.Ge, H.Hua, D.X.Jiang, D.Y.Pang, J.Li, J.Chen, Z.H.Yang, X.H.Sun, Z.Y.Tian, J.Feng, B.Yang, H.L.Zang, Q.Liu, P.J.Li, Z.Q.Chen, Y.Liu, Y.Zhang, J.Ma, H.M.Jia, X.X.Xu, L.Yang, N.R.Ma, L.J.Sun

Determination of the cluster-decay branching ratio from a near-threshold molecular state in 10Be

NUCLEAR REACTIONS 9Be(9Be, 10Be)8Be, E=45 MeV; measured Eα, Iα, E(6He), I(6He), E(9Be), I(9Be), α(6He)-coin, and σ of 10Be population channel from the decay of 10Be* to α+6He using ΔE-E telescope detectors at CIAE HI-13 tandem accelerator facility. 10Be; deduced Q-value spectra, resonances, α-decay branching ratio, and α-cluster spectroscopic factor, σ-bond molecular rotational band. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.101.031304
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Data from this article have been entered in the XUNDL database. For more information, click here.


2020LI51      Phys.Rev. C 102, 064601 (2020)

J.J.Li, C.A.Bertulani, Y.Liu, J.L.Lou, D.Y.Pang, X.H.Sun, B.Yang, X.F.Yang, Y.L.Ye

Eikonal method for charge-exchange reactions at intermediate energies

NUCLEAR REACTIONS 26Mg, 120Sn(3He, t), E=140 MeV/nucleon; 13C(13N, 13C), E=105 MeV/nucleon; calculated differential σ(θ) and relativistic kinematical quantities for intermediate and high energy heavy-ion charge exchange reactions using Eikonal method and the DWBA model, with effective nucleon-nucleon interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.064601
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2020MU14      Eur.Phys.J. A 56, 233 (2020)

A.M.Mukhamedzhanov, A.S.Kadyrov, D.Y.Pang

Trojan horse method as an indirect approach to study resonant reactions in nuclear astrophysics

doi: 10.1140/epja/s10050-020-00214-9
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2020SH09      Phys.Rev.Lett. 124, 162701 (2020)

Y.P.Shen, B.Guo, R.J.deBoer, Z.H.Li, Y.J.Li, X.D.Tang, D.Y.Pang, S.Adhikari, C.Basu, J.Su, S.Q.Yan, Q.W.Fan, J.C.Liu, C.Chen, Z.Y.Han, X.Y.Li, G.Lian, T.L.Ma, W.Nan, W.K.Nan, Y.B.Wang, S.Zeng, H.Zhang, W.P.Liu

Constraining the External Capture to the 16O ground State and the E2 S Factor of the 12C(α, γ)16O reaction

NUCLEAR REACTIONS 12C(11B, 7Li)16O, E=50 MeV; measured reaction products; deduced σ(θ), the ground state asymptotic normalization coefficients, S-factors. Comparison with available data.

doi: 10.1103/PhysRevLett.124.162701
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0230. Data from this article have been entered in the XUNDL database. For more information, click here.


2019LI48      Chin.Phys.C 43, 124102 (2019)

J.-J.Li, D.-Y.Pang, Y.-L.Ye, J.-L.Lou, X.-F.Yang, Y.Liu, B.Yang

Improved eikonal approach for charge exchange reactions at intermediate energies

NUCLEAR REACTIONS 12,13C, 26Mg, 120Sn(3He, 3He), (3He, t), E=140 MeV/nucleon; calculated σ(θ). Comparison with available data.

doi: 10.1088/1674-1137/43/12/124102
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2019MA31      Nucl.Phys. A986, 26 (2019)

T.L.Ma, B.Guo, Z.H.Li, Y.J.Li, D.Y.Pang, Y.L.Han, Y.P.Shen, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu

Precision measurement of the angular distribution for the 16O(d, p)17O transfer reaction to the ground state of 17O

NUCLEAR REACTIONS 16O(d, p)17O, E=15 MeV; measured Ep, Ip(θ); deduced σ(θ) for reactions to 17O gs, spectroscopic factors, ANC; calculated σ(θ) for reactions to 17O gs using DWBA, ADWA (Adiabatic DWBA) and Continuum Discretized Coupled Channel (CDCC) vs radius parameter of Woods-Saxon potential with the same optical potential parameters in ADWA and CDCC. SF and ANC for 17O compared with published results in heavy ion transfer and with shell model calculations.

doi: 10.1016/j.nuclphysa.2019.03.004
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0218.


2019MU11      Phys.Rev. C 99, 064618 (2019)

A.M.Mukhamedzhanov, D.Y.Pang, A.S.Kadyrov

Astrophysical factors of 12C + 12C fusion extracted using the Trojan horse method

NUCLEAR REACTIONS 12C(14N, d)24Mg*, E(cm)=13.85 MeV; calculated differential σ(θ), and bin wave functions using DWBA. 12C(12C, p)23Na*, (12C, α)20Ne*, E=0.8-2.7 MeV; calculated astrophysical S factors using Trojan horse method. Comparison with calculations using plane-wave approximation. Relevance to carbon-carbon burning in stellar environments.

doi: 10.1103/PhysRevC.99.064618
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2019SH11      Phys.Rev. C 99, 025805 (2019)

Y.P.Shen, B.Guo, Z.H.Li, Y.J.Li, D.Y.Pang, S.Adhikari, Z.D.An, J.Su, S.Q.Yan, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, D.H.Li, E.T.Li, X.Y.Li, G.Lian, J.C.Liu, T.L.Ma, C.J.Pei, Y.Su, Y.B.Wang, S.Zeng, Y.Zhou, W.P.Liu

Astrophysical SE2 factor of the 12C (α, γ)16O reaction through the 12C(11B, 7Li)16O transfer reaction

NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; 16O(7Li, 7Li), E=26 MeV; measured charged-particle spectra, differential σ(θ) using the Q3D magnetic spectrograph at the HI-13 tandem accelerator of the CIAE-Beijing. 12C(α, γ), E(cm)<5 MeV; deduced astrophysical SE2(300) factor of the ground state. 16O; deduced asymptotic normalization coefficient (ANC) and reduced α width of the 6.917-MeV level from finite-range distorted wave Born approximation (FRDWBA) and coupled-reaction-channel (CRC) analysis using FRESCO code. Comparison with previous experimental values, and with theoretical model predictions. R-matrix analysis of scattering data.

doi: 10.1103/PhysRevC.99.025805
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0213. Data from this article have been entered in the XUNDL database. For more information, click here.


2019SH37      Phys.Lett. B 797, 134820 (2019)

Y.P.Shen, B.Guo, T.L.Ma, D.Y.Pang, D.D.Ni, Z.Z.Ren, Y.J.Li, Z.D.An, J.Su, J.C.Liu, Q.W.Fan, Z.Y.Han, X.Y.Li, Z.H.Li, G.Lian, Y.Su, Y.B.Wang, S.Q.Yan, S.Zeng, W.P.Liu

First experimental constraint of the spectroscopic amplitudes for the α-cluster in the 11B ground state

NUCLEAR REACTIONS 7Li(6Li, d), E=24 MeV; measured reaction products; deduced spectroscopic amplitudes (SA) for the α-cluster in the 11B ground state. Comparison with available data.

doi: 10.1016/j.physletb.2019.134820
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0220. Data from this article have been entered in the XUNDL database. For more information, click here.


2019SU03      Phys.Rev. C 99, 024605 (2019)

Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, B.H.Sun, J.W.Zhao, Y.P.Xu, D.Y.Pang, Y.H.Yu, K.Yue, S.W.Tang, C.Dong, Y.X.Zhao, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, P.Ma, H.R.Yang, C.G.Lu, L.M.Duan

Two-neutron removal cross sections from 15, 16C at around 240 MeV/nucleon

NUCLEAR REACTIONS 12C(15C, X), (15C, 13C), (16C, X), (16C, 14C)8Li/10Be/11Be/12B/13B/15C/16C/17N, E=237, 239 MeV/nucleon, [secondary 15,16C beams from 9Be(18O, X), E=280 MeV/nucleon primary reaction followed by in-flight fragment separator RIBLL2 at HIRFL-Lanzhou]; measured reaction products, particle identification spectra, time of flight of fragments, and two-neutron removal σ(E) using multiwire drift chambers for particle detection and identification, and plastic scintillators for time of flight measurements. Comparison with previous experimental values, and theoretical calculations for two-neutron removal σ based on eikonal-model and shell-model structure information. Systematics of odd-even staggering in two-neutron removal σ from 15,16,17,18,19,20C projectiles.

doi: 10.1103/PhysRevC.99.024605
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0188.


2019WA01      Phys.Scr. 94, 015302 (2019)

S.T.Wang, Y.P.Xu, D.Y.Pang

Energy dependence of the reduced single-particle strength for strongly-bound proton removal on 16C

NUCLEAR REACTIONS 12C(16C, 15B), E=400 MeV/nucleon; analyzed available data; deduced reduction factors of the one-proton σ.

doi: 10.1088/1402-4896/aaed64
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2019YU07      J.Phys.(London) G46, 105111 (2019)

X.Y.Yun, F.Colomer, D.Y.Pang, P.Capel

Extension of the ratio method to proton-rich nuclei

NUCLEAR REACTIONS 208Pb, 58Ni, 12C(8B, X), E=44 MeV/nucleon; 12C, 58Ni(17F, X), (25Al, X), (27P, X), E=60 MeV/nucleon; analyzed available data. 7Be; deduced σ(θ, E), ratio observables as a tool to study the structure of loosely-bound systems like halo nuclei.

doi: 10.1088/1361-6471/ab355e
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2019ZH39      Nucl.Phys. A990, 1 (2019)

Z.Zhang, R.R.Xu, Z.Y.Ma, Z.G.Ge, Y.Tian, D.Y.Pang, X.D.Sun, Y.L.Jin, X.Tao, Y.Zhang, J.M.Wang

Global α-nucleus optical model based on an Dirac Brueckner Hartree Fock approach

doi: 10.1016/j.nuclphysa.2019.06.013
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2019ZH46      Phys.Rev. C 100, 044609 (2019)

Y.X.Zhao, Y.Z.Sun, S.T.Wang, Z.Y.Sun, X.H.Zhang, D.Yan, D.Y.Pang, P.Ma, Y.H.Yu, K.Yue, S.W.Tang, S.M.Wang, F.Fang, Y.Sun, Z.H.Cheng, X.M.Liu, H.R.Yang, C.G.Lu, L.M.Duan

One-proton knockout from 16C at around 240 MeV/nucleon

NUCLEAR REACTIONS 12C(16C, 15B), E=239 MeV/nucleon, [secondary16O beam from 9Be(18O, X)8Li/10Be/11Be/13B/16C, E=280 MeV/nucleon primary reaction using RIBLL2 at HRIFL-Lanzhou facility]; measured reaction products by magnetic rigidity (Bρ), time of flight (TOF), and energy loss (ΔE), mass yields. 16C, 15B; deduced σ for one-proton knockout, spectroscopic reduction factor. Comparison to predictions based on the eikonal reaction model with shell-model structure inputs, and with previous experimental data for 9Be(16C, 15B), E=75 MeV/nucleon reaction. Discussed energy dependence of the spectroscopic reduction factor, and the role of surface neutrons as spectators.

doi: 10.1103/PhysRevC.100.044609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0221.


2018CH31      Phys.Lett. B 781, 412 (2018)

J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, D.Y.Pang, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, F.R.Xu, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki

A new measurement of the intruder configuration in 12Be

NUCLEAR REACTIONS 11Be(d, p), E=26.9 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), low-lying isomeric 0+ states, J, π, spectroscopic factors. Comparison with available data.

doi: 10.1016/j.physletb.2018.04.016
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2604. Data from this article have been entered in the XUNDL database. For more information, click here.


2018CH38      Phys.Rev. C 98, 014616 (2018)

J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, D.Y.Pang, C.X.Yuan, Y.C.Ge, Q.T.Li, H.Hua, D.X.Jiang, X.F.Yang, F.R.Xu, J.C.Pei, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, G.Li, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki

Low-lying states in 12Be using one-neutron transfer reaction

NUCLEAR REACTIONS 1,2H(11Be, 11Be), (11Be, p), E=26.9 MeV/nucleon; measured recoils, Ep, Ip, p(θ), Eγ and Iγ from decay of recoils, (recoil)p-coin, differential σ(θ) for low-lying 0+, 2+ and 1- states in 12Be, half-life of excited 0+ isomer by decay-tagging method using (CH2)n and (CD2)n targets, annular silicon detectors (ADSSD) for protons, detector telescopes for charged particle detection, and scintillation detectors for γ detection, and isomer-tagging method at RCNP-Osaka. DWBA analysis of σ(θ) data. 12Be; deduced levels, J, π, spectroscopic factors, single-particle components in the g.s. and excited 0+ state. Comparison with shell-model calculations, and with previous experimental results. 11,12Be; calculated B(E2), B(E1), S(n) and S(2n) from shell-model, and compared with experimental data in literature.

doi: 10.1103/PhysRevC.98.014616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2604. Data from this article have been entered in the XUNDL database. For more information, click here.


2018JI04      Chin.Phys.Lett. 35, 082501 (2018)

Y.Jiang, J.-L.Lou, Y.-L.Ye, D.-Y.Pang, J.Chen, Z.-H.Li, Y.-C.Ge, Q.-T.Li, J.Li, W.Jiang, Y.-Le.Sun, H.-L.Zang, Y.Zhang, W.Liu, Y.-D.Chen, G.Li, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.-N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, T.T.Nguyen

A New Measurement of 11Be(p, d) Transfer Reaction

NUCLEAR REACTIONS 1H(11Be, d), E=26.9 MeV/nucleon; measured reaction products. 10Be; deduced Q-value spectrum, σ(θ), spectroscopic factors to 0+ and 2+. Comparison with theoretical calculations.

doi: 10.1088/0256-307X/35/8/082501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0092. Data from this article have been entered in the XUNDL database. For more information, click here.


2018TI06      Phys.Rev. C 97, 064615 (2018)

Y.Tian, D.Y.Pang, Z.-y.Ma

Effects of nonlocality of nuclear potentials on direct capture reactions

NUCLEAR REACTIONS 48Ca(n, γ), E=0.01-0.4 MeV; 7Li(n, γ), E=0.01-2 MeV; 12C(p, γ), E=0-1.2 MeV; calculated local and non-local potential parameters, s-wave phase shifts of target nuclides as function of incident energy, and σ(E) with the Perey-Buck-type nonlocal potentials using a potential model; deduced effects of potential nonlocality in direct radiative capture reactions. Comparison with experimental values.

doi: 10.1103/PhysRevC.97.064615
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2018XU11      Phys.Rev. C 98, 044622 (2018)

Y.P.Xu, D.Y.Pang, X.Y.Yun, S.Kubono, C.A.Bertulani, C.X.Yuan

Possible determination of high-lying single-particle components with (d, p) reactions

NUCLEAR REACTIONS 12C, 24Mg, 28Si, 40Ca(d, p), E=51.93 MeV; analyzed experimental σ(θ) distributions, spectroscopic amplitudes for neutrons in normal and high-lying single-particle components in the ground and excited states by fitting the angular distributions of the ground and the j-forbidden excited states simultaneously, effects of one-step transfer (OST), two-step transfer (TST) and inelastic excitation processes in neutron pickup reactions. Coupled reaction channel calculations.

doi: 10.1103/PhysRevC.98.044622
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2018YA19      Phys.Rev. C 98, 044608 (2018)

Y.Y.Yang, X.Liu, D.Y.Pang, D.Patel, R.F.Chen, J.S.Wang, P.Ma, J.B.Ma, S.L.Jin, Z.Bai, V.Guimaraes, Q.Wang, W.H.Ma, F.F.Duan, Z.H.Gao, Y.C.Yu, Z.Y.Sun, Z.G.Hu, S.W.Xu, S.T.Wang, D.Yan, Y.Zhou, Y.H.Zhang, X.H.Zhou, H.S.Xu, G.Q.Xiao, W.L.Zhan

Elastic scattering of the proton drip line nuclei 7Be, 8B, and 9C on a lead target at energies around three times the Coulomb barriers

NUCLEAR REACTIONS Pb(7Be, 7Be), E=130 MeV; Pb(8B, 8B), E=178 MeV; Pb(9C, 9C), E=227 MeV; measured scattered particles, elastic scattering σ(θ) using silicon ΔE-E telescopes at RIBLL-HIRFL-Lanzhou accelerator facility. Comparison with continuum discretized coupled channels (CDCC) and optical model calculations.

doi: 10.1103/PhysRevC.98.044608
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0206.


2017QU02      Phys.Rev. C 95, 044616 (2017)

W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto

Repulsive three-body force and channel-coupling effects via 12C+12C scattering at 100A MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured scattered 12C using Grand Raiden high-resolution magnetic spectrometer, and 10B, 11C and other particles by the energy loss and time-of-flight (TOF) information, differential cross sections for the ground state, 4.44 MeV, 2+ state, and the sum of the 7.65 MeV, 0+ and the 9.64 MeV, 3- states in 12C using the Ring Cyclotron facility at RCNP-Osaka. Comparison with microscopic coupled-channel calculations, using the double folding method with three different complex G-matrix interactions, the ESC, CEG07b, and MPa.

doi: 10.1103/PhysRevC.95.044616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2546.


2017WE03      Chin.Phys.C 41, 054104 (2017)

C.Wen, Y-P.Xu, D.-Y.Pang, Y.-L.Ye

Quenching of neutron spectroscopic factors of radioactive carbon isotopes with knockout reactions within a wide energy range

NUCLEAR REACTIONS C(15C, X), E=54, 62 MeV; Be(15C, X), E=103, 700 MeV; C(16C, X), E=55, 83 MeV; Be(16C, X), E=62, 700 MeV; C(17C, X), E=49, 79, 904 MeV; Be(17C, X), E=62, 700 MeV; C(18C, X), E=43, 80 MeV; Be(18C, X), E=700 MeV; C(19C, X), E=243, 910 MeV; Be(19C, X), E=57, 64, 88, 700 MeV; analyzed available data; deduced quenching factors of one-neutron spectroscopic factors. Comparison with systematics.

doi: 10.1088/1674-1137/41/5/054104
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2016CH12      Phys.Rev. C 93, 034623 (2016)

J.Chen, J.L.Lou, Y.L.Ye, Z.H.Li, Y.C.Ge, Q.T.Li, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, N.Aoi, E.Ideguchi, H.J.Ong, Y.Ayyad, K.Hatanaka, D.T.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, N.T.Tho, J.Rangel, A.M.Moro, D.Y.Pang, J.Lee, J.Wu, H.N.Liu, C.Wen

Elastic scattering and breakup of 11Be on protons at 26.9A MeV

NUCLEAR REACTIONS 1H(11B, 11B), (11B, X), E=26.9 MeV/nucleon, [11B beam from 9Be(13C, X), E=60 MeV/nucleon]; measured 10,11Be, recoiled protons and deuterons, (10,11Be)p-coin, σ(θ) for elastic and breakup reactions using charged particle telescopes and annular silicon detectors at RCNP-Osaka accelerator facility. 11Be; deduced excitation energy spectrum for the ground state and the excited states. Analysis using Chapel Hill 89 (CH89) and Koning-Delaroche (KD) global optical model potentials (OMPs) for elastic scattering, and extended continuum-discretized coupled-channels (XCDCC) formalism for elastic scattering and breakup data.

doi: 10.1103/PhysRevC.93.034623
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2502.


2016CH51      Phys.Rev. C 94, 064620 (2016)

J.Chen, J.L.Lou, Y.L.Ye, J.Rangel, A.M.Moro, D.Y.Pang, Z.H.Li, Y.C.Ge, Q.T.Li, J.Li, W.Jiang, Y.L.Sun, H.L.Zang, Y.Zhang, N.Aoi, E.Ideguchi, H.J.Ong, J.Lee, J.Wu, H.N.Liu, C.Wen, Y.Ayyad, K.Hatanaka, T.D.Tran, T.Yamamoto, M.Tanaka, T.Suzuki, T.T.Nguyen

Elastic scattering and breakup of 11Be on deuterons at 26.9A MeV

NUCLEAR REACTIONS 2H(11Be, 11Be), (11Be, X), E=26.9 MeV/nucleon, [secondary 11Be beam from 9Be(13C, X), E=60 MeV/nucleon using EN-course beam line at RCNP-Osaka]; measured projectile-like isotopes and recoil light particles, (deuterons)(11Be)- and (deuterons)(10Be)-coin, angular distributions and angular correlations, elastic σ(θ) and breakup σ(θ) using TELE0 and TELE1 telescopes of double-sided silicon strip detector; deduced excitation energy spectrum for the ground state and unbound excited states of 11Be. Comparison of experimental cross sections with optical model calculations, and with continuum-discretized coupled-channels (XCDCC) formalism.

doi: 10.1103/PhysRevC.94.064620
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2527.


2016LI51      Chin.Phys.C 40, 114104 (2016)

E.T.Li, B.Guo, Z.H.Li, Y.B.Wang, Y.J.Li, Z.D.Wu, J.Su, D.Y.Pang, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, Z.Y.Han, X.Hao, S.P.Hu, J.J.He, L.Jing, S.J.Jin, L.Li, X.Y.Li, Z.C.Li, G.Lian, J.C.Liu, Q.Luo, L.H.Qiao, Y.P.Shen, H.B.Sun, S.Q.Yan, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, Y.Zhou, W.P.Liu

Radii of the bound states in 16N from the asymptotic normalization coefficients

RADIOACTIVITY 16N(n) [from 15N(7Li, 6Li)16N, E=44 MeV]; analyzed available data; deduced asymptotic normalization coefficients (ANCs), rms radii of the valence neutron, probabilities of the valence neutron staying out of the core potentials.

doi: 10.1088/1674-1137/40/11/114104
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2016SU05      Phys.Rev. C 93, 024316 (2016)

D.Suzuki, H.Iwasaki, D.Beaumel, M.Assie, H.Baba, Y.Blumenfeld, F.de Oliveira Santos, N.de Sereville, A.Drouart, S.Franchoo, J.Gibelin, A.Gillibert, S.Giron, S.Grevy, J.Guillot, M.Hackstein, F.Hammache, N.Keeley, V.Lapoux, F.Marechal, A.Matta, S.Michimasa, L.Nalpas, F.Naqvi, H.Okamura, H.Otsu, J.Pancin, D.Y.Pang, L.Perrot, C.M.Petrache, E.Pollacco, A.Ramus, W.Rother, P.Roussel-Chomaz, H.Sakurai, J.-A.Scarpaci, O.Sorlin, P.C.Srivastava, I.Stefan, C.Stodel, Y.Tanimura, S.Terashima

Second 0+ state of unbound 12O: Scaling of mirror asymmetry

NUCLEAR REACTIONS 1H(14O, t), E=51 MeV/nucleon, [14O secondary beam from 9Be(16O, X), E=90 MeV/nucleon primary reaction]; measured E(t), I(t), σ(θ), TKE versus θ(lab) using LISE spectrometer and MUST2 telescopes at GANIL. Missing-mass spectroscopy. 12O; deduced levels, J, π, L-transfers, two-proton decay width. Comparison of the second 0+ state of 12O to the mirror state in 12Be and theoretical predictions. Systematics of 0+ states in mirror nuclei pairs of 6Be-6He, 8C-8He, 10C-10Be, 12O-12Be, 14O-14C, 16Ne-16C, 18Ne-18O, 20Mg-20O, 22Mg-22Ne, 24Si-24Ne, 26Si-26Mg, 28S-28Mg, 30S-30Si, 32Ar-32Si, 34Ar-34S, 36Ca-36S, 38Ca-38Ar, 40Ti-40Ar, 42Ti-42Ca, 46Cr-46Ti, 48Ni-48Ca, 50Fe-50Cr, 54Zn-54Cr, 54Ni-54Fe and 58Zn-58Ni. Discussed importance of scaling of mirror asymmetry in the context of ab initio calculations near the drip lines.

doi: 10.1103/PhysRevC.93.024316
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2016YA13      Phys.Rev. C 94, 034614 (2016)

Y.Y.Yang, X.Liu, D.Y.Pang

Distinction between elastic scattering of weakly bound proton- and neutron-rich nuclei: The case of 8B and 11Be

NUCLEAR REACTIONS 64Zn(11Be, 11Be), E(cm)=24.9, 29, 66 MeV; 208Pb(11Be, 11Be), E(cm)=55, 143 MeV; 64Zn(8B, 8B), E(cm)=32, 86 MeV; 208Pb(8B, 8B), E(cm)=64, 170.3 MeV; calculated σ(θ, E) using continuum-discretized coupled channel (CDCC) method. Comparison with available experimental data.

doi: 10.1103/PhysRevC.94.034614
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2016ZH26      Phys.Rev. C 94, 014619 (2016)

Y.Zhang, D.Y.Pang, J.L.Lou

Optical model potential for deuteron elastic scattering with 1p-shell nuclei

NUCLEAR REACTIONS 6Li, 9Be, 10,11B, 12,13C, 14N, 16,18O(d, d), E=5.25-170 MeV; analyzed σ(E), σ(θ) for 67 sets of experimental data for deuteron elastic scattering; deduced a set of global optical model potential parameters. 9Be, 12C, 16O(d, X), E=30-105 MeV; calculated total reaction σ(E) using optical model, and compared with experimental data.

doi: 10.1103/PhysRevC.94.014619
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2015MU08      Phys.Rev. C 92, 014625 (2015)

A.M.Mukhamedzhanov, D.Y.Pang

Asymptotic normalization coefficients and radiative widths

NUCLEAR REACTIONS 11C, 12,14N, 16O(p, γ), E not given; analyzed resonance radiative widths (Γγ) for two transitions in 17F and one each in 12N, 13O and 15O using asymptotic normalization coefficients (ANCs). R-matrix method.

doi: 10.1103/PhysRevC.92.014625
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2015PA10      Phys.Rev. C 91, 024611 (2015)

D.Y.Pang, W.M.Dean, A.M.Mukhamedzhanov

Optical model potential of A=3 projectiles for 1p-shell nuclei

NUCLEAR REACTIONS 9Be, 10,11B, 12,13,14C, 14,15N, 16,17,18O(t, t), (3He, 3He), E=4-118.5 MeV; 6,7Li(t, t), (3He, 3He), E=3-44 MeV; analyzed σ(θ) for 142 sets of experimental data; deduced optical model parameters.

doi: 10.1103/PhysRevC.91.024611
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2015QU02      Phys.Lett. B 751, 1 (2015)

W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto

Effects of repulsive three-body force in 12C + 12C scattering at 100A MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Three double-folding models with complex G-matrix interactions, the CEG07b, MPa, and ESC model calculations.

doi: 10.1016/j.physletb.2015.10.008
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2014GU02      Phys.Rev. C 89, 012801 (2014)

B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, Z.D.Wu, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, L.Y.Zhang, W.J.Zhang, W.P.Liu

Spectroscopic factors for low-lying 16N levels and the astrophysical 15N(n, γ)16N

NUCLEAR REACTIONS 15N(7Li, 6Li)16N, E=44 MeV; measured 6Li spectrum, σ(θ) using Q3D magnetic spectrograph at CIAE's HI-13 tandem accelerator facility. 16N; deduced levels, J, π, configurations, spectroscopic factors for ground and first three excited states. DWBA analysis. Comparison with shell model calculations. 15N(n, γ)16N, at T=0.01-3 GK; deduced astrophysical reaction rates. Comparison with previous experimental and theoretical results.

doi: 10.1103/PhysRevC.89.012801
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2014LE27      Chin.Phys.Lett. 31, 092103 (2014)

J.Lee, D.-Y.Pang, Y.-L.Han, M.B.Tsang

Proton Spectroscopic Factors Deduced from Helium-3 Global Phenomenological and Microscopic Optical Model Potentials

NUCLEAR REACTIONS 16,18O, 19F, 23Na, 24,25,26Mg, 27Al, 28,30Si, 31P, 32,34S, 35,37Cl, 39K(3He, 3He), E=25 MeV; calculated σ, σ(θ), ground state proton spectroscopic factors. Global phenomenological and microscopic helium-3 optical model potentials, comparison with available data.

doi: 10.1088/0256-307X/31/9/092103
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2014LI49      Phys.Rev. C 90, 067601 (2014)

E.T.Li, Z.H.Li, Y.J.Li, B.Guo, Y.B.Wang, D.Y.Pang, J.Su, S.Q.Yan, S.Zeng, L.Gan, Z.C.Li, J.C.Liu, X.X.Bai, Z.D.Wu, S.J.Jin, L.Y.Zhang, X.Q.Yu, L.Li, H.B.Sun, G.Lian, Q.W.Fan, W.P.Liu

Proton spectroscopic factor of the 12C ground state from the 12C(11B, 12C) 11B elastic transfer reaction

NUCLEAR REACTIONS 12C(11B, 11B), (11B, 12C)11B, E=50 MeV; measured particle spectra, angular distributions using Q3D magnetic spectrometer at the HI-13 tandem accelerator of CIAE facility. 12C; deduced optical potential parameters, proton spectroscopic factor for 12C g.s., DWBA calculations. Comparison with previous experimental and theoretical results.

doi: 10.1103/PhysRevC.90.067601
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2014MU10      Phys.Rev. C 90, 034604 (2014)

A.M.Mukhamedzhanov, D.Y.Pang, C.A.Bertulani, A.S.Kadyrov

Surface-integral formalism of deuteron stripping

NUCLEAR REACTIONS 14C(d, p), E=23.4 MeV; 16O(d, p), E=36 MeV; calculated differential σ(θ), spectroscopic factors, neutron widths for deuteron stripping reactions to bound and resonant states. Distorted-wave Born approximation (DWBA), continuum-discretized coupled channels (CDCC), and surface-integral formalism.

doi: 10.1103/PhysRevC.90.034604
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2014PA05      Chin.Phys.C 38, 024104 (2014)

D.-Y.Pang

Effects of relativistic kinematics in heavy ion elastic scattering

NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(6Li, 6Li), (40Ar, 40Ar), E=80 MeV/nucleon; 208Pb(6Li, 6Li), (12C, 12C), (40Ar, 40Ar), E=20, 40, 60, 80, 100 MeV/nucleon; calculated relativistic corrections to the reaction kinematic parameters, σ(θ). Optical model, comparison with experimental data.

doi: 10.1088/1674-1137/38/2/024104
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2014PA49      Phys.Rev. C 90, 044611 (2014)

D.Y.Pang, A.M.Mukhamedzhanov

Asymptotic normalization coefficients and spectroscopic factors from deuteron stripping reactions

NUCLEAR REACTIONS 14C(d, p), E=23.4, 60 MeV; 58Ni(d, p), E=10, 56 MeV; 116Sn(d, p), E=12.2, 79.2 MeV; analyzed experimental data to determine σ(θ), asymptotic normalization coefficients (ANCs), spectroscopic factors by using three methods: distorted wave born approximation (DWBA), adiabatic distorted wave approximation (ADWA), and continuum discretized coupled-channels (CDCC) models. Discussed flaw in the treatment of the nuclear interior in nuclear reaction theory for higher energies in deuteron stripping reactions with 58Ni and 116Sn targets.

doi: 10.1103/PhysRevC.90.044611
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2014WU03      Phys.Rev. C 89, 054315 (2014)

Z.D.Wu, B.Guo, Z.H.Li, Y.J.Li, J.Su, D.Y.Pang, S.Q.Yan, E.T.Li, X.X.Bai, X.C.Du, Q.W.Fan, L.Gan, J.J.He, S.J.Jin, L.Jing, L.Li, Z.C.Li, G.Lian, J.C.Liu, Y.P.Shen, Y.B.Wang, X.Q.Yu, S.Zeng, D.H.Zhang, L.Y.Zhang, W.J.Zhang, W.P.Liu

Proton widths of the low-lying 16F states from the 15N(7Li, 6Li)16N reaction

NUCLEAR REACTIONS 15N(7Li, 7Li), (7Li, 6Li), E=34.5, 44 MeV; measured particle spectra, elastic and inelastic σ(θ) using Q3D magnetic spectrograph at CIAE facility. 16N; deduced levels, J, π, asymptotic normalization coefficients (ANCs), spectroscopic factors. DWBA analysis. 16F; deduced proton and single-particle widths, spectroscopic factors for first four levels from mirror analogy with 16N. Comparison with previous experimental results and compilation.

doi: 10.1103/PhysRevC.89.054315
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2014YA05      Chin.Phys.C 38, 034101 (2014)

J.-C.Yang, G.-L.Zhang, D.-Y.Pang

Systematic analysis of fusion barrier heights and positions for proton projectiles using the single folding model

NUCLEAR REACTIONS 51V, 59Co, 63,65Cu, 92,94Zr, 93Nb, 95,98Mo, 103Rh, 110Pd, 107Ag, 109Mo, 111,116Cd, 115In, 117,118,119,120,122,124Sn, 130Te(p, X), E not given; analyzed available data; parametrized fusion barrier height.

doi: 10.1088/1674-1137/38/3/034101
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2014YA15      Phys.Rev. C 90, 014606 (2014), Erratum Phys.Rev. C 106, 015802 (2022)

Y.Y.Yang, J.S.Wang, Q.Wang, D.Y.Pang, J.B.Ma, M.R.Huang, P.Ma, S.L.Jin, J.L.Han, Z.Bai, L.Jin, J.B.Chen, Q.Hu, R.Wada, S.Mukherjee, Z.Y.Sun, R.F.Chen, X.Y.Zhang, Z.G.Hu, X.H.Yuan, S.W.Xu, S.Z.Chen, X.G.Lei, L.X.Liu, W.H.Ma, S.T.Wang, D.Yan, X.H.Zhang, M.H.Zhao, Y.Zhou, Y.J.Zhou, Z.Y.Guo, Y.H.Zhang, H.S.Xu, G.Q.Xiao

Quasi-elastic scattering of 10, 11C and 10B from a natPb target

NUCLEAR REACTIONS Pb(10C, 10C), (10C, 10C'), E=226, 256 MeV; Pb(11C, 11C), (11C, 11C'), E=222, 226 MeV; Pb(10B, 10B), (10B, 10B'), E=173 MeV; measured particle spectra, time-of-flight, differential σ(θ, E) at HIRFL-RIBLL facility; deduced reduced total reactions σ, negligible contributions from inelastic scattering from Coupled-channel calculations. Optical model analysis.

doi: 10.1103/PhysRevC.90.014606
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2014ZH13      Chin.Phys.Lett. 31, 052401 (2014)

X.-F.Zhang, D.-Y.Pang

Notch Test for Radial Sensitivity on Neutron Density Distribution in 48Ca Probed by α-Particle Elastic Scattering

NUCLEAR REACTIONS 48Ca(α, α), E=104 MeV; calculated σ, neutron density distributions. Comparison with experimental data.

doi: 10.1088/0256-307X/31/5/052401
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2013MA55      Phys.Rev. C 88, 014608 (2013)

R.S.Mackintosh, D.Y.Pang

Significant features of 8B scattering from 208Pb at 170.3 MeV

NUCLEAR REACTIONS 208Pb(8B, 8B), E=170.3 MeV; calculated CDCC breakup S-matrix inversion, σ(θ); deduced dynamic polarization potentials. Continuum discretized coupled channels (CDCC) calculations. Discussed anomalous behavior.

doi: 10.1103/PhysRevC.88.014608
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2013ON02      Phys.Lett. B 725, 277 (2013)

H.J.Ong, I.Tanihata, A.Tamii, T.Myo, K.Ogata, M.Fukuda, K.Hirota, K.Ikeda, D.Ishikawa, T.Kawabata, H.Matsubara, K.Matsuta, M.Mihara, T.Naito, D.Nishimura, Y.Ogawa, H.Okamura, A.Ozawa, D.Y.Pang, H.Sakaguchi, K.Sekiguchi, T.Suzuki, M.Taniguchi, M.Takashina, H.Toki, Y.Yasuda, M.Yosoi, J.Zenihiro

Probing effect of tensor interactions in 16O via (p, d) reaction

NUCLEAR REACTIONS 16O(p, d), E=198, 295, 392 MeV; measured reaction products; deduced σ(θ), tensor interaction in one-nucleon transfer reactions.

doi: 10.1016/j.physletb.2013.07.038
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2013PA20      Phys.Rev. C 87, 064613 (2013)

D.Y.Pang, N.K.Timofeyuk, R.C.Johnson, J.A.Tostevin

Rapid convergence of the Weinberg expansion of the deuteron stripping amplitude

NUCLEAR REACTIONS 132Sn(d, p), E=30, 100 MeV; calculated σ(θ) using Weinberg distorted wave components. Weinberg states expansion method. Comparison with continuum discretized coupled channels (CDCC) calculations.

doi: 10.1103/PhysRevC.87.064613
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2013XU06      Phys.Rev. C 87, 044605 (2013)

Y.P.Xu, D.Y.Pang

Toward a systematic nucleus-nucleus potential for peripheral collisions

NUCLEAR REACTIONS 40Ca(6Li, 6Li), E=99.0, 156.0, 210.0, 240.0 MeV; 48Ca(6Li, 6Li), E=240.0 MeV; 58Ni(6Li, 6Li), E=12, 20, 34.0, 73.7, 90.0, 99.0, 240.0 MeV; 58Fe(6Li, 6Li), E=15 MeV; 65Cu(6Li, 6Li), E=25 MeV; 70Ge(6Li, 6Li), E=28 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=70.0, 73.7, 99.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 116Sn(6Li, 6Li), E=20, 240.0; 120Sn(6Li, 6Li), E=44.0, 90.0; 124Sn(6Li, 6Li), E=73.7 MeV; 144Sm(6Li, 6Li), E=21, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25, 31.0, 33.0, 35.0, 39.0, 50.6, 73.7, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=32.8, 36.0, 40.0 MeV; 40,48Ca(7Li, 7Li), E=34.0, 88.0 MeV; 44Ca(7Li, 7Li), E=34.0; 48Ca(7Li, 7Li), E=88 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe(7Li, 7Li), E=34.0; 58Ni(7Li, 7Li), E=34.0, 42.0, 73.7, 90, 99 MeV; 59Co(7Li, 7Li), E=12, 18 MeV; 60Ni(7Li, 7Li), E=34.0 MeV; 65Cu(7Li, 7Li), E=2 MeV; 80Se(7Li, 7Li), E=14, 23 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 90Zr(7Li, 7Li), E=34.0, 70, 99 MeV; 118Sn(7Li, 7Li), E=48.0 MeV; 120Sn(7Li, 7Li), E=90 MeV; 124Sn(7Li, 7Li), E=73.7 MeV; 144Sm(7Li, 7Li), E=21.6, 30.1, 35.1, 40.8, 42.3, 52.0 MeV; 208Pb(7Li, 7Li), E=27, 33.0, 39.0, 42.0, 52.0, 73.7 MeV; 208Pb(12C, 12C), E=58.9.64.9, 74.9, 84.9 MeV; 208Pb(16O, 16O), E=80, 90, 102 MeV; 12C, 28Si, 40Ca, 90Zr, 208Pb(16O, 16O), E=94 MeV/nucleon; 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; 40Ca, 58Ni, 96Mo(32S, 32S), E=151.5, 107.3, 180 MeV; analyzed σ(E, θ) data; deduced optical model parameters, and comparison with experimental data. 27Al, 40Ca, 54,56,57Fe, 64,66,68Zn, 89Y, Ag(12C, X), E=30, 83 MeV/nucleon; 12C, 27Al, 64Zn, 93Nb, 107Ag, 118Sn, 144,150,154Sm(20Ne, X), E=30 MeV/nucleon; 12C, 27Al, 51V, 54Fe, 107Ag, 118Sn, 208Pb(40Ar, X), E=44 MeV/nucleon; 27Al, 64Zn, 93Nb, 118Sn, 144Sm, 181Ta, 208Pb(40Ca, X), E=77 MeV/nucleon; analyzed total reaction cross sections with optical model calculations. A single-folding model based on Bruyeres Jeukenne-Lejeune-Mahaux (JLMB) nucleon-nucleus potential.

doi: 10.1103/PhysRevC.87.044605
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2013YA06      Phys.Rev. C 87, 044613 (2013), Pub.Note Phys.Rev. C 88, 019901 (2013)

Y.Y.Yang, J.S.Wang, Q.Wang, D.Y.Pang, J.B.Ma, M.R.Huang, J.L.Han, P.Ma, S.L.Jin, Z.Bai, Q.Hu, L.Jin, J.B.Chen, N.Keeley, R.Rusek, R.Wada, S.Mukherjee, Z.Y.Sun, R.F.Chen, X.Y.Zhang, Z.G.Hu, X.H.Yuan, X.G.Cao, Z.G.Xu, S.W.Xu, C.Zhen, Z.Q.Chen, Z.Chen, S.Z.Chen, C.M.Du, L.M.Duan, F.Fu, B.X.Gou, J.Hu, J.J.He, X.G.Lei, S.L.Li, Y.Li, Q.Y.Lin, L.X.Liu, F.D.Shi, S.W.Tang, G.Xu, X.Xu, L.Y.Zhang, X.H.Zhang, W.Zhang, M.H.Zhao, Z.Y.Guo, Y.H.Zhang, H.S.Xu, G.Q.Xiao

Elastic scattering of the proton drip-line nucleus 8B off a natPb target at 170.3 MeV

NUCLEAR REACTIONS Pb(8B, 8B), E=170.3 MeV, [secondary 8B beam from 9Be(12C, X), E=54.2 MeV/nucleon primary reaction]; measured reaction products, energy loss, time of flight, magnetic rigidity, σ(θ) at RIBLL-HRIFL facility in Lanzhou. Analysis of σ(θ) data by optical model using a single-folding-type potential, and by continuum discretized coupled-channels (CDCC) method. Effect of breakup-channel couplings. Comparison with previous experimental σ(θ) data for Pb(7Be, 7Be), E=125 MeV, and 208Pb(6Li, 6Li), E=99 MeV.

doi: 10.1103/PhysRevC.87.044613
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2012AS04      Phys.Lett. B 712, 198 (2012)

M.Assie, F.de Oliveira Santos, T.Davinson, F.de Grancey, L.Achouri, J.Alcantara-Nunez, T.Al Kalanee, J.-C.Angelique, C.Borcea, R.Borcea, L.Caceres, I.Celikovic, V.Chudoba, D.Y.Pang, C.Ducoin, M.Fallot, O.Kamalou, J.Kiener, Y.Lam, A.Lefebvre-Schuhl, G.Lotay, J.Mrazek, L.Perrot, A.M.Sanchez-Benitez, F.Rotaru, M.-G.Saint-Laurent, Yu.Sobolev, N.Smirnova, M.Stanoiu, I.Stefan, K.Subotic, P.Ujic, R.Wolski, P.J.Woods

Spectroscopy of 18Na: Bridging the two-proton radioactivity of 19Mg

RADIOACTIVITY 19Mg(2p), 18Na(p) [from H(17Ne, p)17Ne, E=4 MeV/nucleon]; measured decay products, Ep, Ip. 17Ne; deduced level energies, J, π. Comparison with theoretical calculations.

doi: 10.1016/j.physletb.2012.04.059
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2012CA05      Phys.Lett. B 707, 46 (2012)

Z.X.Cao, Y.L.Ye, J.Xiao, L.H.Lv, D.X.Jiang, T.Zheng, H.Hua, Z.H.Li, X.Q.Li, Y.C.Ge, J.L.Lou, R.Qiao, Q.T.Li, H.B.You, R.J.Chen, D.Y.Pang, H.Sakurai, H.Otsu, M.Nishimura, S.Sakaguchi, H.Baba, Y.Togano, K.Yoneda, C.Li, S.Wang, H.Wang, K.A.Li, T.Nakamura, Y.Nakayama, Y.Kondo, S.Deguchi, Y.Satou, K.Tshoo

Recoil proton tagged knockout reaction for 8He

NUCLEAR REACTIONS 9Be(13C, X)8He, E=115 MeV/nucleon; C, H(8He, p), E=82.3 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(θ), σ(E), neutron spectroscopic factor. Comparison with ab-initio Green's function Monte-Carlo calculations.

doi: 10.1016/j.physletb.2011.12.009
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2012GU18      Astrophys.J. 756, 193 (2012)

B.Guo, Z.H.Li, M.Lugaro, J.Buntain, D.Y.Pang, Y.J.Li, J.Su, S.Q.Yan, X.X.Bai, Y.S.Chen, Q.W.Fan, S.J.Jin, A.I.Karakas, E.T.Li, Z.C.Li, G.Lian, J.C.Liu, X.Liu, J.R.Shi, N.C.Shu, B.X.Wang, Y.B.Wang, S.Zeng, W.P.Liu

New Determination of the 13C(α, n)16O Reaction Rate and its Influence on the s-process Nucleosynthesis in AGB Stars

NUCLEAR REACTIONS 12,13C(11B, 7Li), E=50 MeV; measured reaction products; deduced σ(θ), S-factors, stellar rates. Comparison with available data.

doi: 10.1088/0004-637X/756/2/193
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2012LI45      Chin.Phys.Lett. 29, 102301 (2012)

K.-A.Li, Y.-L.Ye, H.Scheit, P.Doornenbal, S.Takeuchi, N.Aoi, M.Matsushita, E.Takeshita, T.Motobayashi, H.Sakurai, D.-Y.Pang

Inelastic Scattering of 32Mg at 190 MeV/Nucleon from a Thick Proton Target

NUCLEAR REACTIONS 1H(32Mg, 32Mg'), E=190 MeV/nucleon; measured reaction products, Eγ, Iγ. 32Mg; deduced deformation parameter, σ(θ). Comparison with available data, coupled-channel calculations.

doi: 10.1088/0256-307X/29/10/102301
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2012MA47      Phys.Rev. C 86, 047602 (2012)

R.S.Mackintosh, D.Y.Pang

Increase in lSLl induced by channel coupling: The case of deuteron breakup

NUCLEAR REACTIONS 58Ni(d, d), E=56, 79, 120 MeV; calculated elastic scattering matrix magnitude, σ(θ), dynamic polarization potentials (DPP) induced by S-wave and d-wave breakup (BU). Continuum discretized coupled channels (CDCC) calculations. Anomalous effect of couplings on S-matrix, relation of non-locality of optical model potentials. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.047602
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2012PA22      J.Phys.(London) G39, 095101 (2012)

D.Y.Pang, Y.L.Ye, F.R.Xu

Energy-dependent optical model potentials for α and deuteron with 12C

NUCLEAR REACTIONS 12C(α, α), (d, d), E=10-100 MeV/nucleon; calculated σ; deduced energy dependence of α- and d-potentials. Lane-consistent Bruyeres Jeukenne-Lejeune-Mahaux model nucleon-nucleus potentials, comparison with available data.

doi: 10.1088/0954-3899/39/9/095101
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2012XI03      Chin.Phys.Lett. 29, 082501 (2012)

J.Xiao, Y.-L.Ye, Z.-X.Cao, D.-X.Jiang, T.Zheng, H.Hua, Z.-H.Li, X.-Q.Li, Y.-C.Ge, J.-L.Lou, D.-Y.Pang, L.-H.Lv, Q.-T.Li, R.Qiao, H.-B.You, R.-J.Chen, H.Sakurai, H.Otsu, M.Nishimura, S.Sakaguchi, H.Baba, Y.Togano, K.Yoneda, C.Li, S.Wang, H.Wang, K.-A.Li, Y.Nakayama, Y.Kondo, S.Deguchi, Y.Satou, K.H.Tshoo

New Measurements for 8He Excited States

NUCLEAR REACTIONS H, C(8He, 2n)6He, E=82.3 MeV/nucleon; measured reaction products, En, In. 8He; deduced relative energy spectrum, resonances, resonant peaks, σ. Borromean nucleus, comparison with available data.

doi: 10.1088/0256-307X/29/8/082501
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2012ZH21      Eur.Phys.J. A 48, 65 (2012)

G.L.Zhang, C.L.Zhang, H.Q.Zhang, C.J.Lin, D.Y.Pang, X.K.Wu, H.M.Jia, G.P.An, Z.D.Wu, X.X.Xu, F.Yang, Z.H.Liu, S.Kubono, H.Yamaguchi, S.Hayakawa, D.N.Binh, Y.K.Kwon, N.Iwasa, M.Mazzocco, M.La Commara, M.Romoli, C.Signorini

Quasi-elastic scattering of the proton drip line nucleus 17F on 12C at 60 MeV

NUCLEAR REACTIONS 12C(17F, 17F'), E=60 MeV; measured E(17F), I(17F, θ); deduced σ(θ), σ; calculated σ(θ) using optical model and CDCC; deduced parameters. Compared with data, also for nearby projectiles.

doi: 10.1140/epja/i2012-12065-x
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2011AS07      Int.J.Mod.Phys. E20, 971 (2011)

M.Assie, F.De Oliveira Santos, F.De Grancey, L.Achouri, J.Alcantara-Nunez, J.-C.Angelique, C.Borcea, L.Caceres, I.Celikovic, V.Chudoba, D.Y.Pang, T.Davinson, C.Ducoin, M.Fallot, J.Kiener, A.Lefebvre-Schuhl, G.L.Lotay, J.Mrazek, L.Perrot, A.M.Sanchez-Benitez, F.Rotaru, M.-G.Saint-laurent, Yu.Sobolev, M.Stanoiu, R.Stanoiu, I.Stefan, K.Subotic, P.J.Woods, P.Ujic, R.Wolski

Spectroscopy of the unbound nucleus 18Na

NUCLEAR REACTIONS 1H(17Ne, 17Ne), 1H(17Ne, X)18Na, E=4 MeV/nucleon; measured reaction products, proton spectrum; deduced σ(θ), excited state width.

ATOMIC MASSES 18Na; measured TOF; deduced mass excess. Comparison with all available data.

doi: 10.1142/S0218301311019088
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2011LO07      Phys.Rev. C 83, 034612 (2011)

J.L.Lou, Y.L.Ye, D.Y.Pang, Z.X.Cao, D.X.Jiang, T.Zheng, H.Hua, Z.H.Li, X.Q.Li, Y.C.Ge, L.H.Lv, J.Xiao, Q.T.Li, R.Qiao, H.B.You, R.J.Chen, H.Sakurai, H.Otsu, M.Nishimura, S.Sakaguchi, H.Baba, Y.Togano, K.Yoneda, C.Li, S.Wang, H.Wang, K.A.Li, T.Nakamura, Y.Nakayama, Y.Kondo, S.Deguchi, Y.Satou, K.Tshoo

Quasielastic scattering of 6He from 12C at 82.3 MeV/nucleon

NUCLEAR REACTIONS 12C(6He, 6He'), [secondary 6He beam from 9Be(13C, X), E=115 MeV/nucleon primary reaction], E=82.3 MeV/nucleon; measured charged-particle spectra, σ(θ) of scattered 6He, σ/σ(Rutherford). Comparisons with optical model (OM) and continuum discretized coupling channel (CDCC) model calculations.

doi: 10.1103/PhysRevC.83.034612
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2011PA20      Phys.Rev. C 83, 064619 (2011)

D.Y.Pang, Y.L.Ye, F.R.Xu

Application of the Bruyeres Jeukenne-Lejeune-Mahaux model potential to composite nuclei with a single-folding approach

NUCLEAR REACTIONS 58Ni, 90Zr, 116Sn, 208Pb(α, α), (d, d), E=10-100 MeV/nucleon; calculated σ(θ), σ(E); deduced global optical model potential parameters. Single-folding (SF) model with the Lane-consistent Bruyeres Jeukenne-Lejeune-Mahaux nucleon-nucleus potential. Systematic differences in renormalization factors between α particles and deuterons. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064619
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2011PA37      Phys.Rev. C 84, 064611 (2011)

D.Y.Pang, R.S.Mackintosh

Dynamic polarization potential due to 6Li breakup on 12C

NUCLEAR REACTIONS 12C(6Li, 6Li), E=90-318 MeV; calculated σ(E, θ), breakup coupling, energy dynamic of dynamic polarization potentials (DPP), S-matrix inversion compared with trivially equivalent local potential (TELP). Continuum discretized coupled-channels (CDCC) formalism with a two-body cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.064611
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2010FA09      Chin.Phys.Lett. 27, 092501 (2010)

J.-Q.Faisal, J.-L.Lou, Y.-L.Ye, Z.-X.Cao, D.-X.Jiang, T.Zheng, H.Hua, Z.-H.Li, X.-Q.Li, Y.-C.Ge, D.-Y.Pang, Q.-T.Li, J.Xiao, L.-H.Lv, R.Qiao, H.-B.You, R.-J.Chen, F.Lu, H.Sakurai, H.Otsu, M.Nishimura, S.Sakaguchi, H.Baba, Y.Togano, K.Yoneda, C.Li, S.Wang, H.Wang, K.-A.Li, T.Nakamura, Y.Nakayama, Y.Kondo, S.Deguchi, Y.Satou, K.H.Tshoo

Elastic Scattering of 6He + p at 82.3 MeV/nucleon

NUCLEAR REACTIONS 1H(6He, 6He), E=82.3 MeV/nucleon; measured reaction products. 6He; deduced σ(θ). Comparison with optical model CH89 or KD02 global potentials.

doi: 10.1088/0256-307X/27/9/092501
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2009GO01      Phys.Lett. B 672, 22 (2009)

M.S.Golovkov, L.V.Grigorenko, G.M.Ter-Akopian, A.S.Fomichev, Yu.Ts.Oganessian, V.A.Gorshkov, S.A.Krupko, A.M.Rodin, S.I.Sidorchuk, R.S.Slepnev, S.V.Stepantsov, R.Wolski, D.Y.Pang, V.Chudoba, A.A.Korsheninnikov, E.A.Kuzmin, E.Yu.Nikolskii, B.G.Novatskii, D.N.Stepanov, P.Roussel-Chomaz, W.Mittig, A.Ninane, F.Hanappe, L.Stuttge, A.A.Yukhimchuk, V.V.Perevozchikov, Yu.I.Vinogradov, S.K.Grishechkin, S.V.Zlatoustovskiy

The 8He and 10He spectra studied in the (t, p) reaction

NUCLEAR REACTIONS 3H(6He, p), E=25 MeV/nucleon; 3H(8He, p), E=27.4 MeV/nucleon; measured fragment, proton energies, (fragment)(proton)-coin and missing mass spectra; deduced σ. 6,8He deduced ground state energies, E1 strength distribution. Comparison with other data and calculations. Secondary radioactive beam.

doi: 10.1016/j.physletb.2008.12.052
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2009GR03      Phys.Part. and Nucl.Lett. 6, 118 (2009)

L.V.Grigorenko, M.S.Golovkov, G.M.Ter-Akopian, A.S.Fomichev, Yu.Ts.Oganessian, V.A.Gorshkov, S.A.Krupko, A.M.Rodin, S.I.Sidorchuk, R.S.Slepnev, S.V.Stepantsov, R.Wolski, D.Y.Pang, V.Chudoba, A.A.Korsheninnikov, E.A.Kuzmin, E.Yu.Nikolskii, B.G.Novatskii, D.N.Stepanov, P.Roussel-Chomaz, W.Mittig, A.Ninane, F.Hanappe, L.Stuttge, A.A.Yukhimchuk, V.V.Perevozchikov, Yu.I.Vinogradov, S.K.Grishechkin, S.V.Zlatoustovskiy

Soft dipole mode in 8He

NUCLEAR REACTIONS 3H(6He, p), E not given; measured Ep, Ip, cross sections. Deduced B(E1).

doi: 10.1134/S1547477109020046
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2009PA07      Phys.Rev. C 79, 024615 (2009); Erratum Phys.Rev. C 81, 019902 (2010)

D.Y.Pang, P.Roussel-Chomaz, H.Savajols, R.L.Varner, R.Wolski

Global optical model potential for A = 3 projectiles

NUCLEAR REACTIONS 6Li, 27Al, 28Si, 32S, 46Ti, 48Ti, 56Fe, 68Zn(t, t), E=17 MeV; 9Be, 60Ni, 140Ce(t, t), E=15, 17 MeV; 12C(t, t), E=15, 17, 20, 33, 36, 38 MeV; 13C(t, t), E=38 MeV; 14C(t, t), E=71.7 MeV; 16O(t, t), E=33, 36 MeV; 19F, 48Ca, 51V, 89Y(t, t), E=33 MeV; 20Ne, 22Ne(t, t), E=33.4 MeV; 24Mg(t, t), E=15, 33.4 MeV; 26Mg, 30Si(t, t), E=17, 36 MeV; 40Ca(t, t), E=17, 20, 33 MeV; 52Cr, 62Ni(t, t), E=15, 20 MeV; 58Ni, 232Th(t, t), E=17, 33 MeV; 64Ni(t, t), E=20 MeV; 82Se, 86Sr, 87Rb(t, t), E=15 MeV; 90Zr(t, t), E=15, 17, 20 MeV; 94Zr, 116Sn(t, t), E=17, 20 MeV; 96Zr, 118Sn, 122Sn, 124Sn, 182W, 207Pb(t, t), E=20 MeV; 208Pb(t, t), E=20, 33 MeV; 6Li(3He, 3He), E=8-217 MeV; 9Be(3He, 3He), E=4-217 MeV; 12C(3He, 3He), E=11-217 MeV; 13C(3He, 3He), E=450 MeV; 24Mg(3He, 3He), E=12-130 MeV; 27Al(3He, 3He), E=5.5-118.5 MeV; 28Si(3He, 3He), E=450 MeV; 40Ca(3He, 3He), E=8.5-130, 31.0-217, 450 MeV; 58Ni(3He, 3He), E=12-217, 450 MeV; 64Ni(3He, 3He), E=21-118.5 MeV; 90Zr(3He, 3He), E=12-217, 450 MeV; 116Sn(3He, 3He), E=18-109.2 MeV; 120Sn(3He, 3He), E=130 MeV; 208Pb(3He, 3He), E=33.3-217, 450 MeV; analyzed σ(θ) using global optical model potential GDP08; deduced set of global optical potential parameters.

doi: 10.1103/PhysRevC.79.024615
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2007BA76      Chin.Phys.Lett. 24, 3384 (2007)

Z.Bai, Q.Wang, J.-L.Han, ZG.Xiao, H.-S.Xu, Z.-Y.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X-H.Yuan, Z.-G.Xu, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, J.-Q.Li, Y.-P.Zhang, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, W.Xu, G.-T.Fan, S.-Q.Zhang, D.-Y.Pang, Y.-K.Sergey

Angular Dispersion and Deflection Function for Heavy Ion Elastic Scattering

NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured differential cross sections, angular dispersion plots. 208Pb(16O, 16O), E=170.1 MeV; 208Pb(6He, 6He), E=27, 29.6 MeV; 208Pb(6Li, 6Li), E=73.7, 99 MeV; 208Pb(α, α), E=40 MeV; analyzed differential cross sections, angular dispersion plots.

doi: 10.1088/0256-307X/24/12/027
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2007LO05      Phys.Rev. C 75, 057302 (2007)

J.L.Lou, Z.H.Li, Y.L.Ye, H.Hua, D.X.Jiang, L.H.Lv, Z.Kong, Y.M.Zhang, F.R.Xu, T.Zheng, X.Q.Li, Y.C.Ge, C.Wu, G.L.Zhang, Z.Q.Chen, C.Li, D.Y.Pang, H.S.Xu, Z.Y.Sun, L.M.Duan, Z.G.Hu, R.J.Hu, H.G.Xu, R.S.Mao, Y.Wang, X.H.Yuan, H.Gao, L.J.Wu, H.R.Qi, T.H.Huang, F.Fu, F.Jia, Q.Gao, X.L.Ding, J.L.Han, X.Y.Zhang

Observation of a new transition in the beta-delayed neutron decay of 18N

RADIOACTIVITY 18N(β-); measured β-delayed neutron spectra. 18O; deduced level energies, J, π. Deduced B(GT), compared to shell model calculations.

doi: 10.1103/PhysRevC.75.057302
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2007PA10      Phys.Rev. C 75, 024601 (2007)

D.Y.Pang, F.M.Nunes, A.M.Mukhamedzhanov

Are spectroscopic factors from transfer reactions consistent with asymptotic normalization coefficients?

NUCLEAR REACTIONS 14C(d, p), E=14 MeV; 16O(d, p), E=15 MeV; 40Ca(d, p), E=11 MeV; analyzed σ(θ); deduced spectroscopic factors, asymptotic normalization coefficients.

doi: 10.1103/PhysRevC.75.024601
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2007PA39      Chin.Phys.Lett. 24, 2785 (2007)

D.-Y.Pang, Y.-L.Ye, D.-X.Jiang, T.Zheng, Z.-H.Li, X.-Q.Li, Y.-C.Ge, H.Hua, C.-E.Wu, J.-L.Lou, F.Lu, F.-Y.Fan, A.Ozawa, Y.Yamaguchi, R.Kanungo, D.Fang, I.Tanihata

Single-Proton Pickup Reaction of the Halo Nucleus 6He on a 9Be Target at 25 MeV/nucleon

NUCLEAR REACTIONS 9Be(6He, 7Li), E=25 MeV/nucleon; measured particle energies, yields, inclusive σ and angular distributions.

doi: 10.1088/0256-307X/24/10/020
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2006HU19      High Energy Phys. and Nucl.Phys. (China), Supplement 2, 30, 157 (2006)

H.Hua, S.Wamg, J.Meng, Z.-H.Li, S.-Q.Zhang, F.-R.Xu, H.-L.Liu, S.-G.Zhou, Y.-L.Ye, D.-X.Jiang, T.Zheng, L.-H.Mu, X.-G.Wu, G.-S.Li, Q.-J.Wang, Z.-Q.Chen, C.-E.Wu, G.-L.Zhang, D.-Y.Pang, J.Wang, J.-L.Lou, B.Guo, G.Jin, S.-X.Wen, C.-Y.He, X.-Z.Chui, Y.Liu

High-Spin States in 152Gd


2005LI60      Phys.Rev. C 72, 064327 (2005)

Z.H.Li, Y.L.Ye, H.Hua, D.X.Jiang, Y.M.Zhang, F.R.Xu, Q.Y.Hu, G.L.Zhang, Z.Q.Chen, T.Zheng, C.E.Wu, J.L.Lou, X.Q.Li, D.Y.Pang, S.Wang, C.Li, H.S.Xu, Z.Y.Sun, L.M.Duan, Z.G.Hu, R.J.Hu, H.G.Xu, R.S.Mao, Y.Wang, X.H.Yuan, H.Gao, L.J.Wu, H.R.Qi, T.H.Huang, F.Fu, F.Jia, Q.Gao, X.L.Ding, J.L.Han, X.Y.Zhang

β-decay of the neutron-rich nucleus 18N

RADIOACTIVITY 18N(β-), (β-n) [from Be(22Ne, X)]; measured T1/2, β-delayed neutron spectra, Eγ, Iγ; deduced branching ratios, Gamow-Teller strengths. 18O deduced levels, J, π. Comparison with shell model calculations.

doi: 10.1103/PhysRevC.72.064327
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2005WA14      Chin.Phys.Lett. 22, 1370 (2005)

J.Wang, Y.-L.Ye, D.-X.Jiang, G.-L.Zhang, D.-Y.Pang, Z.-H.Li, T.Zheng, X.-Q.Li, Q.-J.Wang, Q.-Y.Hu, C.-E.Wu, A.Ozawa, Y.Yamaguchi, R.Kanungo, D.Fang, I.Tanihata

Measurement of the Breakup Cross Sections in 6He + 9Be Reaction at 25 MeV/Nucleon

NUCLEAR REACTIONS 9Be(6He, αX), E=25 MeV/nucleon; measured Eα, σ(θ). Comparison with Serber model predictions.

doi: 10.1088/0256-307X/22/6/020
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1957.


2005WA23      Phys.Rev. C 72, 024317 (2005), Erratum Phys.Rev. C 105, 029903 (2022)

S.Wang, H.Hua, J.Meng, Z.H.Li, S.Q.Zhang, F.R.Xu, H.L.Liu, Y.L.Ye, D.X.Jiang, T.Zheng, Q.J.Wang, Z.Q.Chen, C.E.Wu, G.L.Zhang, D.Y.Pang, J.Wang, J.L.Lou, B.Guo, G.Jin, S.G.Zhou, L.H.Zhu, X.G.Wu, G.S.Li, S.X.Wen, C.Y.He, X.Z.Cui, Y.Liu

High-spin states in 152Gd

NUCLEAR REACTIONS 148Nd(9Be, 5n), E=42, 45, 48, 52, 55 MeV; measured Eγ, Iγ; deduced excitation function. 148Nd(9Be, 5n), E=54 MeV; measured Eγ, Iγ, γγ-coin. 152Gd deduced high-spin levels, J, π, configuration, quadrupole deformation. Total Routhian surface calculations.

doi: 10.1103/PhysRevC.72.024317
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2005YE01      Phys.Rev. C 71, 014604 (2005)

Y.L.Ye, D.Y.Pang, D.X.Jiang, T.Zheng, Q.J.Wang, Z.H.Li, X.Q.Li, Y.C.Ge, C.Wu, G.L.Zhang, Q.Y.Hu, J.Wang, Z.Q.Chen, A.Ozawa, Y.Yamaguchi, R.Kanungo, I.Tanihata

Quasielastic scattering of 6He on 9Be at 25 MeV/nucleon

NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured quasielastic σ(θ); deduced optical model parameters, inelastic channels contribution.

doi: 10.1103/PhysRevC.71.014604
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2005YE05      J.Phys.(London) G31, S1647 (2005)

Y.L.Ye, D.Y.Pang, G.L.Zhang, D.X.Jiang, T.Zheng, Z.H.Li, X.Q.Li, Q.J.Wang, Y.C.Ge, C.E.Wu, J.Wang, Z.Q.Chen, Y.Ai, A.Ozawa, Y.Yamaguchi, D.Q.Fang, I.Tanihata

Study of the halo nucleus 6He through the direct nuclear reactions

NUCLEAR REACTIONS 9Be(6He, 6He), (6He, 5He), (6He, α), (6He, αX), (6He, tX), E=25 MeV/nucleon; measured quasielastic, breakup, and transfer σ(θ). 6He deduced two-triton configuration.

doi: 10.1088/0954-3899/31/10/048
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2004PA35      Chin.Phys.Lett. 21, 2151 (2004)

D.-Y.Pang, Y.-L.Ye, D.-X.Jiang, T.Zheng, Q-J.Wang, Z.-H.Li, X.-Q.Li, Y.-C.Ge, C.-E.Wu, G.-L.Zhang, Q.-Y.Hu, J.Wang, A.Ozawa, Y.Yamaguchi, R.Kanungo, D.Fang, I.Tanihata

Quasielastic Scattering of the Halo Nucleus 6He at 25 MeV/u from a 9Be Target

NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured σ(θ); deduced optical potential parameters. Double folding model.

doi: 10.1088/0256-307X/21/11/021
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2002CH31      Chin.Phys.Lett. 19, 921 (2002)

T.Chen, Y.-L.Ye, Z.-H.Li, D.-X.Jiang, H.Hua, X.-Q.Li, Q.-J.Wang, Y.-C.Ge, D.-Y.Pang, Z.-Y.Di, G.-M.Jin, G.-Q.Xiao, Z.-Y.Guo, Z.-G.Xiao, H.-W.Wang, B.-G.Zhang, H.-Y.Wu, J.-X.Li, Z.-Y.Sun, W.-L.Zhan

Quasi-Elastic Scattering of a Secondary 6He Beam on a 9Be Target at 25MeV/Nucleon

NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured σ(θ); deduced optical model parameters..

doi: 10.1088/0256-307X/19/7/311
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