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NSR database version of April 27, 2024.

Search: Author = Y.Z.Sun

Found 6 matches.

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2022JI03      Chin.Phys.C 46, 014003 (2022)

S.-Y.Jin, Y.-Z.Sun, S.-T.Wang, Z.-Y.Sun, X.-H.Zhang, Z.-Q.Chen, B.Mei, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.B.Ma, X.-M.Liu, R.Han

Fragmentation of stable and neutron-rich 12-16C into boron fragments at approximately 240 MeV/nucleon

NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X)10Be/13B/B, E=240 MeV/nucleon; measured reaction products; deduced σ. Comparison with EPAX3, modified EPAX2, FRACS, NUCFRG2, INCL++, JQMD, and JQMD-2.0 calculations. The ETF of the Institute of Modern Physics, Chinese Academy of Sciences.

doi: 10.1088/1674-1137/ac2ed5
Citations: PlumX Metrics

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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2022XU12      Chin.Phys.C 46, 111001 (2022)

Xi.-D.Xu, Y.-Z.Sun, S.-T.Wang, B.Mei, S.-Y.Jin, X.-H.Zhang, Z.-Y.Sun, Y.-X.Zhao, S.-W.Tang, Y.-H.Yu, D.Yan, F.Fang, Y.-J.Zhang, S.-B.Ma

Isotopic production cross sections of fragmentation residues produced by 18O ions on a carbon target near 260 MeV/nucleon

NUCLEAR REACTIONS C(18O, X)14N/15C/12C/12B/13B/10B, E=260 MeV/nucleon; measured reaction products, TOF; deduced isotopic σ. Comparison with available data. The HIRFL facility in Lanzhou (China).

doi: 10.1088/1674-1137/ac827c
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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.

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0188.

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.

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