NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.Yan Found 94 matches. 2024XI06 Phys.Rev. C 109, 035804 (2024) W.Xian, S.Chen, S.Nikas, M.Rosenbusch, M.Wada, H.Ishiyama, D.Hou, S.Iimura, S.Nishimura, P.Schury, A.Takamine, S.Yan, F.Browne, P.Doornenbal, F.Flavigny, Y.Hirayama, Y.Ito, S.Kimura, T.M.Kojima, J.Lee, J.Liu, H.Miyatake, S.Michimasa, J.Y.Moon, S.Naimi, T.Niwase, T.Sonoda, D.Suzuki, Y.X.Watanabe, V.Werner, K.Wimmer, H.Wollnik Mass measurements of neutron-rich A ≈ 90 nuclei constrain element abundances
doi: 10.1103/PhysRevC.109.035804
2023HO11 Phys.Rev. C 108, 054312 (2023) D.S.Hou, A.Takamine, M.Rosenbusch, W.D.Xian, S.Iimura, S.D.Chen, M.Wada, H.Ishiyama, P.Schury, Z.M.Niu, H.Z.Liang, S.X.Yan, P.Doornenbal, Y.Hirayama, Y.Ito, S.Kimura, T.M.Kojima, W.Korten, J.Lee, J.J.Liu, Z.Liu, S.Michimasa, H.Miyatake, J.Y.Moon, S.Naimi, S.Nishimura, T.Niwase, T.Sonoda, D.Suzuki, Y.X.Watanabe, K.Wimmer, H.Wollnik First direct mass measurement for neutron-rich 112Mo with the new ZD-MRTOF mass spectrograph system
doi: 10.1103/PhysRevC.108.054312
2023II01 Phys.Rev.Lett. 130, 012501 (2023) S.Iimura, M.Rosenbusch, A.Takamine, Y.Tsunoda, M.Wada, S.Chen, D.S.Hou, W.Xian, H.Ishiyama, S.Yan, P.Schury, H.Crawford, P.Doornenbal, Y.Hirayama, Y.Ito, S.Kimura, T.Koiwai, T.M.Kojima, H.Koura, J.Lee, J.Liu, S.Michimasa, H.Miyatake, J.Y.Moon, S.Naimi, S.Nishimura, T.Niwase, A.Odahara, T.Otsuka, S.Paschalis, M.Petri, N.Shimizu, T.Sonoda, D.Suzuki, Y.X.Watanabe, K.Wimmer, H.Wollnik Study of the N=32 and N=34 Shell Gap for Ti and V by the First High-Precision Multireflection Time-of-Flight Mass Measurements at BigRIPS-SLOWRI ATOMIC MASSES 55Sc, 56,58Ti, 56,57,58,59V; measured TOF; deduced masses, nonexistence of the N=34 empirical two-neutron shell gaps for Ti and V, and the enhanced energy gap in Ca. Comparison with new Monte Carlo shell model calculations. RIKEN's Radioactive Isotope Beam Factory (RIBF).
doi: 10.1103/PhysRevLett.130.012501
2023SH06 Astrophys.J. 945, 41 (2023) Y.Shen, B.Guo, R.J.deBoer, E.Li, Z.Li, Y.Li, X.Tang, D.Pang, S.Adhikari, C.Basu, J.Su, S.Yan, Q.Fan, J.Liu, C.Chen, Z.Han, X.Li, G.Lian, T.Ma, W.Nan, W.Nan, Y.Wang, S.Zeng, H.Zhang, W.Liu New Determination of the 12C(α, γ)16O Reaction Rate and Its Impact on the Black-hole Mass Gap NUCLEAR REACTIONS 12C(11B, 7Li), (11B, 11B), E=50 MeV; measured reaction products. 16O; deduced σ(θ), the asymptotic normalization coefficient (ANC) for the 16O ground state (GS), astrophysical S-factor and the stellar rate. The HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE) in Beijing, China.
doi: 10.3847/1538-4357/acb7de
2023TO03 Phys.Rev. C 107, 054615 (2023) Roles of pairing dynamics in fusion enhancement or suppression in 124Sn + 40, 48Ca and 132Sn + 58Ni reactions at sub-barrier energies NUCLEAR REACTIONS 40,48Ca(124Sn, X), (132Sn, X), E(cm)=105-135 MeV; 58Ni(132Sn, X), E(cm)=150-200 MeV; calculated nucleus-nucleus interaction potentials, collective kinetic energies, real-space particle density distributions, reduced friction coefficients, internal excitation energies, reduced pairing energies, fusion σ(E). Real space density-constrained time-dependent Hartree-Fock-Bogoliubov (rDC-TDHFB) method. Comparison to experimental and other theoretical results.
doi: 10.1103/PhysRevC.107.054615
2023ZH26 Phys.Rev. C 107, 065801 (2023) H.Zhang, J.Su, Z.H.Li, Y.J.Li, E.T.Li, C.Chen, J.J.He, Y.P.Shen, G.Lian, B.Guo, X.Y.Li, L.Y.Zhang, Y.D.Sheng, Y.J.Chen, L.H.Wang, L.Zhang, F.Q.Cao, W.Nan, W.K.Nan, G.X.Li, N.Song, B.Q.Cui, L.H.Chen, R.G.Ma, Z.C.Zhang, T.Y.Jiao, B.S.Gao, X.D.Tang, Q.Wu, J.Q.Li, L.T.Sun, S.Wang, S.Q.Yan, J.H.Liao, Y.B.Wang, S.Zeng, D.Nan, Q.W.Fan, W.P.Liu Updated reaction rate of 25Mg(p, γ)26Al and its astrophysical implication NUCLEAR REACTIONS 25Mg(p, γ), E=117-350 keV; measured Eγ, Iγ, sum of γ energies; deduced γ-ray branching ratios, resonances, resonance strengths, astrophysical reaction rate (T=0.01-2.0 GK), contribution of individual resonances to the reaction rate, ground-state and isomeric state contribution. Comaprison to other experimental data and NACRE compilation. Evaluated the impact of the obtained data on the 26Al yield in stellar environment (code MESA). BGO detector array in nearby 4π geometry composed of 8 identical segments at high-current 400 kV JUNA accelerator (China JinPing underground Laboratory).
doi: 10.1103/PhysRevC.107.065801
2022LI28 Few-Body Systems 63, 43 (2022) W.P.Liu, Z.H.Li, J.J.He, X.D.Tang, G.Lian, J.Su, Y.P.Shen, Z.An, F.Q.Chao, J.J.Chang, L.H.Chen, H.Chen, X.J.Chen, Y.H.Chen, Z.J.Chen, B.Q.Cui, X.C.Du, X.Fang, C.B.Fu, L.Gan, B.Guo, Z.Y.Han, X.Y.Guo, G.Z.He, J.R.He, A.Heger, S.Q.Hou, H.X.Huang, N.Huang, B.L.Jia, L.Y.Jiang, S.Kubono, J.M.Li, M.C.Li, K.A.Li, E.T.Li, T.Li, Y.J.Li, M.Lugaro, X.B.Luo, H.Y.Ma, S.B.Ma, D.M.Mei, W.Nan, W.K.Nan, N.C.Qi, Y.Z.Qian, J.C.Qin, J.Ren, C.S.Shang, L.T.Sun, W.L.Sun, W.P.Tan, I.Tanihata, S.Wang, P.Wang, Y.B.Wang, Q.Wu, S.W.Xu, S.Q.Yan, L.T.Yang, Y.Yang, X.Q.Yu, Q.Yue, S.Zeng, L.Zhang, H.Zhang, H.Y.Zhang, L.Y.Zhang, N.T.Zhang, P.Zhang, Q.W.Zhang, T.Zhang, X.P.Zhang, X.Z.Zhang, W.Zhao, J.F.Zhou, Y.Zho Progress of Underground Nuclear Astrophysics Experiment JUNA in China NUCLEAR REACTIONS 12C(α, γ), 13C(α, n), 25Mg(p, γ), 19F(p, α), E(cm)<600 keV; measured reaction products; deduced yields near the Gamow window. Comparison with available data.
doi: 10.1007/s00601-022-01735-3
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
2022OR04 Phys.Rev. C 106, 064301 (2022) R.Orlandi, H.Makii, K.Nishio, K.Hirose, M.Asai, K.Tsukada, T.K.Sato, Y.Ito, F.Suzaki, Y.Nagame, A.N.Andreyev, E.Ideguchi, N.Aoi, T.T.Pham, S.Q.Yan, Y.P.Shen, B.Gao, G.Li New K isomers in 248Cf NUCLEAR REACTIONS 249Cf(18O, 19O)248Cf, E=140.4 MeV; measured reaction products, Eγ, Iγ, γγ-coin, particleγ-coin. 248Cf; deduced levels, J, π, transitions from isomeric states, T1/2 for 2 low-ling transitions, B(E1). Discussed possible configuration of newly observed isomeric state at 950 keV to be two-quasineutron K=8- and the two-quasiproton K=5-. Comparison to other experimental data. Radioactive target. Si-detectors array combined with γ-ray detector array consisted of 4 Ge detectors and 4 4x5 inch LaBr3 scintillators at Tokai Tandem accelerator facility of the Japan Atomic Energy Agency (JAEA).
doi: 10.1103/PhysRevC.106.064301
2022TO01 Phys.Rev. C 105, 014613 (2022) Real space density-constrained time-dependent Hartree-Fock-Bogoliubov method and pairing effects in the fusion of calcium isotopes NUCLEAR REACTIONS 40,44,48Ca(40Ca, X), E(cm)=55 MeV; 44Ca(44Ca, X), E(cm)=53 MeV; calculated nucleus-nucleus interaction potentials for head-on collisions and fusion σ(E) using a real space density-constrained time-dependent Hartree-Fock-Bogoliubov (rDC-TDHFB) method with Gogny interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.105.014613
2022TO10 Phys.Rev. C 106, 044611 (2022) Microscopic investigations into fission dynamics beyond the saddle point RADIOACTIVITY 240Pu(SF); calculated adiabatic and dynamical potentials for symmetric and asymmetric fission pathways along the quadrupole deformation Q20, the octupole Q30 and hexadecapole Q40 deformations before scission, proton and neutron number distribution in fragments, total pairing energies, the numbers of nucleon-transferring of asymmetric fission, proton and neutron pairing energies, proton and neutron spin-orbit energies, total kinetic energies TKE, collective accelerations of fission dynamics, internal excitation energies and deformation energies of fragments, total excitation energies. Real space density-constrained time-dependent Hartree-Fock-Bogoliubov (rDC-TDHFB) method with Gogny D1S interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.106.044611
2021NI08 Phys.Rev. C 104, 044617 (2021) T.Niwase, M.Wada, P.Schury, P.Brionnet, S.D.Chen, T.Hashimoto, H.Haba, Y.Hirayama, D.S.Hou, S.Iimura, H.Ishiyama, S.Ishizawa, Y.Ito, D.Kaji, S.Kimura, J.Liu, H.Miyatake, J.Y.Moon, K.Morimoto, K.Morita, D.Nagae, M.Rosenbusch, A.Takamine, T.Tanaka, Y.X.Watanabe, H.Wollnik, W.Xian, S.X.Yan α-decay-correlated mass measurement of 206, 207g, mRa using an α-TOF detector equipped multireflection time-of-flight mass spectrograph system ATOMIC MASSES 206,207,207mRa; measured time-of-flight spectra by α-decay-correlated mass spectroscopy using multireflection time-of-flight mass spectrograph (MRTOF-MS) system, with an α-TOF detector at SHE-Mass-II facility of RIBF-RIKEN; deduced mass excesses, and compared with evaluated data in AME2020. 207mRa; deduced excitation energy of the isomer, J, π. 206,207,207mRa isotopes produced in 159Tb(51V, X), E=306 MeV, followed by separation of evaporation residues using recoil ion separator GARIS-II at RIKEN. RADIOACTIVITY 206,207mRa(α)[from 159Tb(51V, X), E=306 MeV at RIBF-RIKEN]; measured Eα, Iα, T1/2 of decays of 206Ra and 207mRa, excitation energy of the isomer; deduced α-reduced width, configuration. Systematics of spins, parities, Eα, T1/2, α-branching ratios, reduced α widths for 203,203m,205,205m,207,207mRa. 198,199Po, 202,203At, 202,203Rn, 206,207Fr, 207Ra; observed α spectra from decays.
doi: 10.1103/PhysRevC.104.044617
2021SC14 Phys.Rev. C 104, L021304 (2021) P.Schury, T.Niwase, M.Wada, P.Brionnet, S.Chen, T.Hashimoto, H.Haba, Y.Hirayama, D.S.Hou, S.Iimura, H.Ishiyama, S.Ishizawa, Y.Ito, D.Kaji, S.Kimura, H.Koura, J.J.Liu, H.Miyatake, J.-Y.Moon, K.Morimoto, K.Morita, D.Nagae, M.Rosenbusch, A.Takamine, Y.X.Watanabe, H.Wollnik, W.Xian, S.X.Yan First high-precision direct determination of the atomic mass of a superheavy nuclide ATOMIC MASSES 257Db; measured Eα, time-of flight, distribution of time-of-flight (ToF)-correlated α-decay events using multireflection time-of-flight mass spectrograph (MRTOF-MS) at RIKEN Ring Cyclotron facility; deduced A/q and mass excess for each of the 11 observed correlated events assigned to 257Db. Comparison with AME2016 evaluated data. 257Db isotope produced in 208Pb(51V, 2n), E=306 MeV reaction, followed by separation of fragments using GARIS-II separator.
doi: 10.1103/PhysRevC.104.L021304
2021TO13 Phys.Rev. C 104, 064617 (2021) Prediction of neutron-induced fission product yields by a straightforward k-nearest-neighbor algorithm NUCLEAR REACTIONS 233,234,236,237,238U, 237,238Np, 238,239,240,241,242Pu, 241,243Am, 242,244,246,248Cm(n, F), E=0.4-2.0 MeV; analyzed mass distributions of fast neutron-induced fission products, and compared with evaluated experimental data in JENDL library. 232U(n, F), E=fast; predicted mass distributions of fast neutron-induced fission and compared with the recommended data of ENDF/B-VII.1 library. Machine learning algorithm for known fission product yields (FPYs) and predicted unknowns using k-nearest-neighbor algorithm (KNN) combined with a general description of the fission observable (GEF) method.
doi: 10.1103/PhysRevC.104.064617
2021YA29 Astrophys.J. 919, 84 (2021) S.Q.Yan, X.Y.Li, K.Nishio, M.Lugaro, Z.H.Li, H.Makii, M.Pignatari, Y.B.Wang, R.Orlandi, K.Hirose The 59Fe(n, γ)60Fe Cross Section from the Surrogate Ratio Method and Its Effect on the 60Fe Nucleosynthesis NUCLEAR REACTIONS 56,58Fe(18O, 16O), E=103 MeV; measured reaction products, Eγ, Iγ; deduced σ, Maxwellian-averaged σ. Comparison with TALYS calculations.
doi: 10.3847/1538-4357/ac12ce
2020GA03 Phys.Rev. C 101, 014612 (2020) L.Gan, H.B.Sun, Z.H.Li, S.P.Hu, Y.J.Li, J.Su, B.Guo, S.Q.Yan, Y.B.Wang, S.Zeng, Z.Y.Han, X.Y.Li, D.H.Li, T.L.Ma, Y.P.Shen, Y.Su, E.T.Li, W.P.Liu Experimental study of the spectroscopic factors of 116-125Sn NUCLEAR REACTIONS 116,118,120,122,124Sn(p, d), E=18.0 MeV; 116,118,120,122,124Sn(d, p), E=12.0 MeV; measured E(p), I(p), E(d), I(d), σ(θ) using the high-precision Q3D magnetic spectrograph at the CIAE-Beijing HI-13 tandem accelerator. 115,117,119,121,123,125Sn; deduced levels, L-transfers, J, π, spectroscopic factors (SFs). DWBA analysis of σ(θ) data and extraction of the neutron spectroscopic factors using two different sets of systematic optical potential parameters. Comparison with previous experimental data. Proposed a linear formula to relate SFs with S(n).
doi: 10.1103/PhysRevC.101.014612
2020LI31 Phys.Rev. C 102, 025804 (2020) Y.J.Li, Z.H.Li, E.T.Li, X.Y.Li, T.L.Ma, Y.P.Shen, J.C.Liu, L.Gan, Y.Su, L.H.Qiao, Z.Y.Han, Y.Zhou, J.Su, S.Q.Yan, S.Zeng, Y.B.Wang, B.Guo, G.Lian, D.Nan, X.X.Bai, W.P.Liu Indirect measurement of the 57.7 keV resonance strength for the astrophysical γ-ray source of the 25Mg(p, γ)26Al reaction NUCLEAR REACTIONS 24,25Mg(7Li, 6He), (7Li, 7Li), E=31.5 MeV; measured 6He and 7Li particle spectra using ΔE-E telescope of Si detectors, σ(θ) using Q3D magnetic spectrometer at the HI-13 tandem accelerator of CIAE-Beijing. 26Al; deduced levels, J, π, spectroscopic factors. DWBA analysis of σ(θ) data using the code FRESCO, with Woods-Saxon potential parameters deduced from analysis of the present data and the literature data for 27Al(6Li, 6Li) reaction. 25Mg(p, γ)26Al; deduced Γp and resonance strength of 57.7-keV proton resonance in 26Al. 25Mg(p, γ)26Al, T9=0.1-10; calculated astrophysical reaction rates for the ground and isomeric states in 26Al, and compared with the results in the NACRE database.
doi: 10.1103/PhysRevC.102.025804
2020RO16 Chin.Phys.C 44, 104003 (2020) C.-H.Rong, G.-L.Zhang, L.Gan, Z.-Ho.Li, L.C.Brandao, E.N.Cardozo, M.R.Cortes, Y.-J.Li, Ju.Su, S.-Q.Yan, S.Zeng, G.Lian, B.Guo, Y.-B.Wang, W.-P.Liu, J.Lubian The angular distributions of elastic scattering of 12, 13C+Zr NUCLEAR REACTIONS 90,91,92,94,96Zr(12C, 12C), (13C, 13C), E=66, 64 MeV; measured reaction products; deduced σ, the neutron spectroscopic amplitudes using the optical model and coupled channel calculations.
doi: 10.1088/1674-1137/abab8d
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
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
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
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
2018GA19 Phys.Rev. C 97, 064614 (2018) L.Gan, H.B.Sun, Z.H.Li, Y.J.Li, J.Su, B.Guo, S.Q.Yan, Y.B.Wang, S.Zeng, Z.Y.Han, X.Y.Li, D.H.Li, T.L.Ma, Y.P.Shen, Y.Su, E.T.Li, S.P.Hu, W.P.Liu Experimental study of the spectroscopic factors of 90-97Zr NUCLEAR REACTIONS 90,92,94,96Zr(12C, 12C), (12C, 13C), E=66 MeV; 90,92,94,96Zr(13C, 13C), (13C, 12C), E=64 MeV; measured particle spectra, differential σ(θ) using Q3D magnetic spectrograph at the HI-13 tandem accelerator facility of the CIAE, Beijing; deduced neutron spectroscopic factors using distorted-wave Born approximation (DWBA) calculations. Comparison of spectroscopic results with previous experiments. Relevance to neutron capture reactions in s process for synthesis of heavy elements.
doi: 10.1103/PhysRevC.97.064614
2018LI18 Chin.Phys.C 42, 044001 (2018) E.-T.Li, Z.H.Li, S.-Q.Yan, J.Su, B.Guo, Y.-J.Li, Y.-B.Wang, G.Lian, S.Zeng, S.-Z.Chen, S.-B.Ma, X.-Q.Li, C.He, H.-B.Sun, W.-P.Liu Measurement of the 2H(7Be, 6Li)3He reaction rate and its contribution to the primordial lithium abundance NUCLEAR REACTIONS 2H(7Be, 6Li)3He, E=17.7, 30.2 MeV; measured reaction products, Eα, Iα; deduced σ(θ), σ, reaction rates. Comparison with theoretical calculations.
doi: 10.1088/1674-1137/42/4/044001
2018LI24 Chin.Phys.C 42, 065001 (2018) Z.-H.Li, E.-T.Li, J.Su, Y.-J.Li, Y.-B.Wang, S.-Q.Yan, B.Guo, D.Nan, W.-P.Liu New determination of the 7Be ground state spectroscopic factor and the 6Li(p, γ)7Be astrophysical S(E)factors NUCLEAR REACTIONS 7Be(d, 3He)6Li, E(cm)=6.7 MeV; measured reaction products; deduced σ(θ). 6Li(p, γ)7Be, E(cm)<1 MeV; analyzed available data; deduced S factors. Comparison with DWBA calculation code TWOFNR.
doi: 10.1088/1674-1137/42/6/065001
2018WA34 Yuan.Wul.Ping. 35, 445 (2018); Nucl.Phys.Rev. 35, 445 (2018) Y.Wang, J.Su, Z.Han, B.Tang, B.Cui, T.Ge, Y.Lu, Z.Chen, B.Guo, X.Li, Y.Li, Z.Li, G.Lian, T.Ma, Y.Ma, Y.Shen, Y.Su, C.Wang, H.Wu, S.Yan, S.Zeng, Y.Zheng, C.Zhou, Y.Dang, G.Fu, Y.He, F.Liu, D.Wu, T.Zhang, W.Liu, for the BRIF collaboration Study of the Exotic Decay Mode of 20Na with an Intense ISOL Beam RADIOACTIVITY 20Na(β+α) [from 24Mg(p, nα), E<100 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced γ-ray energies and intensities, exotic β-γ-α decay mode.
doi: 10.11804/NuclPhysRev.35.04.445
2017GU03 Phys.Rev. A 95, 022705 (2017) D.L.Guo, X.Ma, S.F.Zhang, X.L.Zhu, W.T.Feng, R.T.Zhang, Y.Gao, B.Hai, M.Zhang, D.B.Qian, S.Yan, and P.Zhang Dynamics of transfer ionization in p-He collisions at intermediate energies NUCLEAR REACTIONS He(p, X), E=50-100 keV; measured reaction products, Eβ, Iβ; deduced that electron momentum distribution projected onto the scattering plane is consistent with the prediction of an independent two-step mechanism involving a binary encounter. Comparison with theoretical calculations.
doi: 10.1103/PhysRevA.95.022705
2017YA27 Astrophys.J. 848, 98 (2017) S.Q.Yan, Z.H.Li, Y.B.Wang, K.Nishio, M.Lugaro, A.I.Karakas, H.Makii, P.Mohr, J.Su, Y.J.Li, I.Nishinaka, K.Hirose, Y.L.Han, R.Orlandi, Y.P.Shen, B.Guo, S.Zeng, G.Lian, Y.S.Chen, W.P.Liu The 95Zr(n, γ)96Zr Cross Section from the Surrogate Ratio Method and Its Effect on s-process Nucleosynthesis NUCLEAR REACTIONS 94,90Zr(18O, 16O), E=117 MeV; measured reaction products; deduced σ for surrogate reactions. Comparison with KADONIS and ENDF/B-VII.1 evaluated nuclear library and TALYS nuclear code calculations.
doi: 10.3847/1538-4357/aa8c74
2017ZH45 Nucl.Instrum.Methods Phys.Res. B412, 81 (2017) J.P.Zhu, X.Xiao, S.Yan, Y.Gao, J.M.Xue, Y.G.Wang Measurement of differential cross section of D(3He, p)4He from 0.8 MeV to 3.6 MeV NUCLEAR REACTIONS 2H(3He, p), E=0.8-3.6 MeV; measured reaction products; deduced σ(θ). Comparison with available data.
doi: 10.1016/j.nimb.2017.07.020
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
2016SU10 Phys.Lett. B 756, 323 (2016) J.Su, W.P.Liu, N.T.Zhang, Y.P.Shen, Y.H.Lam, N.A.Smirnova, M.MacCormick, J.S.Wang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, Z.C.Gao, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li, G.Audi Revalidation of the isobaric multiplet mass equation at A = 53, T = 3/2 RADIOACTIVITY 53Ni(EC), (ECp) [from Be(58Ni, X)53Ni, E=68.3 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced T1/2, level scheme, J, π, isobaric analog state, mass excess, explanation of unexpected deviation from the isobaric multiplet mass equation (IMME) at A=53, T=3/2.
doi: 10.1016/j.physletb.2016.03.024
2016YA09 Phys.Rev. C 94, 015804 (2016) S.Q.Yan, Z.H.Li, Y.B.Wang, K.Nishio, H.Makii, J.Su, Y.J.Li, I.Nishinaka, K.Hirose, Y.L.Han, R.Orlandi, Y.P.Shen, B.Guo, S.Zeng, G.Lian, Y.S.Chen, X.X.Bai, L.H.Qiao, W.P.Liu Examination of the surrogate ratio method for the determination of the 93Zr (n, γ)94Zr cross section with 90, 92Zr(18O, 16O) 92, 94Zr reactions NUCLEAR REACTIONS 90,92Zr(18O, 16O), E=117 MeV; measured Eγ, Iγ, (16O)γ-coin at the Tandem accelerator of JAEA facility. 92,94Zr; measured γ-decay probability ratios. 93Zr(n, γ), E>3 MeV; deduced σ(E) by surrogate ratio method, using reference cross sections of the 91Zr(n, γ)92Zr reaction from ENDF/B-VII.1, and the measured γ-decay probability ratios.
doi: 10.1103/PhysRevC.94.015804
2016ZH08 Phys.Rev. A 93, 032709 (2016) R.T.Zhang, W.T.Feng, X.L.Zhu, S.F.Zhang, D.L.Guo, Y.Gao, D.B.Qian, S.Xu, S.C.Yan, P.Zhang, Z.K.Huang, H.B.Wang, B.Hai, D.M.Zhao, X.Ma Two-electron transfer and ionization mechanism in 80-keV/u Ne8+ on He collisions NUCLEAR REACTIONS He(Ne, X), E=80 keV/nucleon; measured reaction products, Eβ, Iβ; deduced autoionization decay from doubly excited states with symmetric and asymmetric configurations.
doi: 10.1103/PhysRevA.93.032709
2015NI09 Phys.Lett. B 748, 89 (2015) K.Nishio, A.N.Andreyev, R.Chapman, X.Derkx, Ch.E.Dullmann, L.Ghys, F.P.Hessberger, K.Hirose, H.Ikezoe, J.Khuyagbaatar, B.Kindler, B.Lommel, H.Makii, I.Nishinaka, T.Ohtsuki, S.D.Pain, R.Sagaidak, I.Tsekhanovich, M.Venhart, Y.Wakabayashi, S.Yan Excitation energy dependence of fragment-mass distributions from fission of 180, 190Hg formed in fusion reactions of 36Ar + 144, 154Sm NUCLEAR REACTIONS 144,154Sm(36Ar, X)180Hg/190Hg, E=148-198 MeV; measured reaction products; deduced fission fragment mass and total kinetic-energy distributions. Comparison with available data.
doi: 10.1016/j.physletb.2015.06.068
2015SH16 Phys.Rev. C 91, 047304 (2015) Y.P.Shen, W.P.Liu, J.Su, N.T.Zhang, L.Jing, Z.H.Li, Y.B.Wang, B.Guo, S.Q.Yan, Y.J.Li, S.Zeng, G.Lian, X.C.Du, L.Gan, X.X.Bai, J.S.Wang, Y.H.Zhang, X.H.Zhou, X.D.Tang, J.J.He, Y.Y.Yang, S.L.Jin, P.Ma, J.B.Ma, M.R.Huang, Z.Bai, Y.J.Zhou, W.H.Ma, J.Hu, S.W.Xu, S.B.Ma, S.Z.Chen, L.Y.Zhang, B.Ding, Z.H.Li Measurement of the 52Fe mass via the precise proton-decay energy of 53Com RADIOACTIVITY 53mCo(p)[from 9Be(58Ni, X), E=68.3 MeV/nucleon]; 41Ti(β+p); measured Ep, Ip, at RIBLL-HIRFL-Lanzhou facility; deduced mass excess of 52Fe and compared with AME-2012 evaluation. 51Fe, 52Co(β+); measured half-lives and compared with evaluated data in ENSDF. ATOMIC MASSES 52Fe; deduced mass excess from Q value of proton decay of 3174.1 keV, 19/2- isomer in 53Co determined from measured proton energy. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.047304
2015WE11 J.Radioanal.Nucl.Chem. 305, 455 (2015) Z.Wei, Z.Yao, C.Lan, J.Chen, Y.Yan, Y.Shi, S.Yan, J.Wang, J.Wang Monte Carlo simulation of fission yields, kinetic energy, fission neutron spectrum and decay γ-ray spectrum for 232Th(n, f) reaction induced by 3H(d, n) 4He neutron source NUCLEAR REACTIONS 232Th(n, F), E<20 MeV; calculated fission neutron yields, average kinetic energy, fission neutron and γ-ray spectra. Comparison with ENDF/B-VII.1 evaluated nuclear library, available data.
doi: 10.1007/s10967-014-3910-7
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
2014JI07 Phys.Rev. C 90, 024612 (2014) Effects of large mass transfer and statistical decay on ternary breakup in the reaction 238U + 197Au at 15A MeV NUCLEAR REACTIONS 197Au(238U, F), E=15 MeV/nucleon; calculated fragment multiplicity, fragment mass and charge, binary, ternary, quaternary and quinary breakup probabilities as a function of impact parameter, total kinetic energy. Hybrid model combining the improved quantum molecular dynamics (ImQMD) model with statistical code GEMINI++. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.024612
2014JI17 Phys.Rev. C 90, 064618 (2014) Microscopic study of noncentral effects in heavy-ion fusion reactions with spherical nuclei NUCLEAR REACTIONS 16O(16O, X), E(cm)=12, 20 MeV; 40Ca(40Ca, X), E(cm)=56, 58, 60, 70, 100, 48-75 MeV; 90Zr(40Ca, X), E(cm)=100, 110, 120, 180, 300 MeV; calculated time evolution of the moment of inertia for 16O+16O reaction, time evolution of the quadrupole moments, penetration probability as a function of impact parameter, and fusion σ(E) for 40Ca+40Ca reaction, N-N potentials and collective kinetic energies, effective mass parameters for head-on collisions and for various impact parameters. Three dimensional time-dependent Hartree-Fock approach (TDHF) with and without density constraint. Comparison with available experimental data.
doi: 10.1103/PhysRevC.90.064618
2014LI01 Chin.Phys.C 38, 014001 (2014) Y.-J.Li, D.-H.Zhang, S.-W.Yan, L.-C.Wang, J.-X.Cheng, J.-S.Li, S.Kodaira, N.Yasuda Projectile fragment emission in the fragmentation of 56Fe on C, Sl and CH2 targets at 471 A Mev NUCLEAR REACTIONS C, Al(56Fe, X)C/Ar/Cr/Mn, E=471 MeV/nucleon; measured reaction fragments; deduced transverse momentum distribution; deduced temperature parameter.
doi: 10.1088/1674-1137/38/1/014001
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
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
2013GU04 Phys.Rev. C 87, 015803 (2013) B.Guo, J.Su, Z.H.Li, Y.B.Wang, S.Q.Yan, Y.J.Li, N.C.Shu, Y.L.Han, X.X.Bai, Y.S.Chen, W.P.Liu, H.Yamaguchi, D.N.Binh, T.Hashimoto, S.Hayakawa, D.Kahl, S.Kubono, J.J.He, J.Hu, S.W.Xu, N.Iwasa, N.Kume, Z.H.Li Determination of the astrophysical 12N(p, γ)13O reaction rate from the 2H(12N, 13O)n reaction and its astrophysical implications NUCLEAR REACTIONS 2H(12N, 13O)1n, E=59 MeV; measured reaction products, energy loss, time-of-flight, differential σ(θ); deduced ANC, astrophysical S factors. 12N(p, γ)13O, at T9=0.3-3.0; deduced stellar reaction rate. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.87.015803
2013HE08 Phys.Rev. C 87, 034320 (2013), Erratum Phys.Rev. C 102, 029903 (2020) C.He, S.Shen, S.Wen, L.Zhu, X.Wu, G.Li, Y.Zhao, Y.Yan, Z.Bai, Y.Wu, Y.Li, G.Li, S.Yan, M.Oshima, Y.Toh, A.Osa, M.Koizumi, Y.Hatsukawa, M.Matsuda, T.Hagakawa Signature splitting inversion and backbending in 80Rb NUCLEAR REACTIONS 65Cu(19F, 3np), E=75 MeV; 66Zn(18O, 3np), E=76 MeV; 68Zn(16O, 3np), E=80 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at CIAE and JAERI facilities. 80Rb; deduced high-spin levels, J, π, bands, alignments, signature splitting and inversion. Comparison with structures of 78Rb and 82Y nuclei. Calculated total Routhian surface (TRS) plots. Projected shell-model calculations.
doi: 10.1103/PhysRevC.87.034320
2013JI13 Phys.Rev. C 88, 035801 (2013) S.J.Jin, Y.B.Wang, J.Su, S.Q.Yan, Y.J.Li, B.Guo, Z.H.Li, S.Zeng, G.Lian, X.X.Bai, W.P.Liu, H.Yamaguchi, S.Kubono, J.Hu, D.Kahl, H.S.Jung, J.Y.Moon, C.S.Lee, T.Teranishi, H.W.Wang, H.Ishiyama, N.Iwasa, T.Komatsubara, B.A.Brown Resonant scattering of 22Na+p studied by the thick-target inverse-kinematic method NUCLEAR REACTIONS 1H(22Na, 22Na), E<37.1 MeV, [22Na secondary beam from 1H(22Ne, 22Na), E=6.0 MeV/nucleon primary reaction]; measured back-angle recoil-proton spectra, TOF, differential σ(E) using thick target technique at RIBF-RIKEN facility. R-matrix analysis of resonance spectra. 23Mg; deduced levels, resonances, J, π, Γp, Γγ, resonance strengths, two s-wave resonances. Comparison with previous experimental data, and with shell-model calculations. 22Na(p, γ)23Mg, T9=0.01-10; deduced astrophysical reaction rates. Comparison with previous experimental data and NACRE evaluation. NUCLEAR STRUCTURE 23Mg; calculated levels, J, π, s-wave resonances, their spectroscopic factors and γ widths using shell model with usda and usdb interactions. Comparison with experimental data, and with structure of 23Na mirror nucleus.
doi: 10.1103/PhysRevC.88.035801
2013JI17 Phys.Rev. C 88, 044611 (2013) Dynamics of energy dissipation in heavy-ion fusion reactions NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=55, 100 MeV; 64Ni(64Ni, X), E(cm)=95, 190 MeV; 90Zr(90Zr, X), E(cm)=195, 300 MeV; 120Sn(120Sn, X), E(cm)=300, 500 MeV; calculated relative distance, quadrupole moment, nuclear stopping power as function of time, dynamic interaction potentials, dynamic reduced mass parameters, friction coefficients, relative distance dependence of the nucleons transferred, energies dissipated. Role of nucleon-nucleon two-body collisions in energy dissipation. Improved quantum molecular dynamics (ImQMD) model.
doi: 10.1103/PhysRevC.88.044611
2013LI09 Phys.Rev. C 87, 017601 (2013) Z.H.Li, Y.J.Li, J.Su, B.Guo, E.T.Li, K.J.Dong, X.X.Bai, Z.C.Li, J.C.Liu, S.Q.Yan, Y.B.Wang, S.Zeng, G.Lian, B.X.Wang, S.J.Jin, X.Liu, W.J.Zhang, W.Z.Huang, Q.W.Fan, L.Gan, Z.D.Wu, W.P.Liu New determination of the proton spectroscopic factor in 9Be from the 13C(9Be, 8Li)14N angular distribution NUCLEAR REACTIONS 13C(9Be, 8Li)14N, 12,13C(9Be, 9Be), E=40 MeV; measured particle spectra, Eα, differential s(θ) using Q3D magnetic spectrometer at HI-13 tandem accelerator facility in Beijing. 9Be; deduced proton spectroscopic factor for g.s. Optical model and DWBA analysis. Comparison with previous experimental and theoretical studies. Relevance to astrophysical S factor for 8Li(p, γ)9Be reaction.
doi: 10.1103/PhysRevC.87.017601
2013LI16 Nucl.Phys. A902, 1 (2013) Dynamical effects in heavy-ion induced ternary breakup NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni(58Ni, X), 100Mo(100Mo, X), 120Sn(120Sn, X), 197Au(197Au, X), 238U(238U, X), E≈15 MeV/nucleon; calculated fragments σ, ternary fission fragments σ using ImQMD model; deduced probability of cascade and direct ternary fission vs impact parameter, momentum anisotropy ratio. 100Mo+100Mo deduced nucleon number asymmetry vs impact parameter and vs incident energy, Comparison with available data and momentum anisotropy also with Jain calculation.
doi: 10.1016/j.nuclphysa.2013.02.015
2013SU07 Phys.Rev. C 87, 024312 (2013) J.Su, W.P.Liu, N.C.Shu, S.Q.Yan, Z.H.Li, B.Guo, W.Z.Huang, S.Zeng, E.T.Li, S.J.Jin, X.Liu, Y.B.Wang, G.Lian, Y.J.Li, Y.S.Chen, X.X.Bai, J.S.Wang, Y.Y.Yang, R.F.Chen, S.W.Xu, J.Hu, S.Z.Chen, S.B.Ma, J.L.Han, P.Ma, Q.Hu, J.B.Ma, X.G.Cao, S.L.Jin, Z.Bai, K.Yang, F.D.Shi, W.Zhang, Z.Chen, L.X.Liu, Q.Y.Lin, X.S.Yan, X.H.Zhang, F.Fu, J.J.He, X.Q.Li, C.He, M.S.Smith Reexamining the β decay of 53, 54Ni, 52, 53Co, 51Fe, and 50Mn RADIOACTIVITY 50Mn, 50Cr, 51Fe, 52,53Co, 53,54Ni(β+), (EC), (β+p)[from (58Ni, X), E=68.6 MeV/nucleon]; measured β-delayed protons, (proton)γ-coin, Eγ, Iγ, T1/2 at HIRFL facility in Lanzhou. Implications for r process. Comparison with previous experimental studies.
doi: 10.1103/PhysRevC.87.024312
2013WA26 Nucl.Phys. A920, 1 (2013) Odd-even and nonequilibrium effects in multifragmentation of 56Fe on C, Al targets at 471 A MeV NUCLEAR REACTIONS C, Al(56Fe, X), E=471 MeV/nucleon; calculated fragment σ, charge and mass distribution, σ(θ), time development of density distribution using ImQMD (Improved QMD) with statistical GEMINI model.Compared to data.
doi: 10.1016/j.nuclphysa.2013.10.007
2012CH01 Chin.Phys.C 36, 37 (2012) J.-X.Cheng, D.-H.Zhang, S.-W.Yan, J.-S.Li, L.-C.Wang, Y.-J.Li, N.Yasuda The fragmentation of 20Ne at 400 A MeV NUCLEAR REACTIONS C, Al, H(20Ne, X), E=400 MeV/nucleon; measured reaction fragments; deduced σ. Comparison with Bradt-Peters semi-empirical formula, NUCFRAG2 and PHITS models.
doi: 10.1088/1674-1137/36/1/006
2012CH15 J.Phys.(London) G39, 055104 (2012) J.X.Cheng, X.Jiang, S.W.Yan, D.H.Zhang The odd-even effect of 20Ne fragmentation cross sections NUCLEAR REACTIONS C, Al, Cu, Sn, Pb(20Ne, X), E=400 MeV/nucleon; calculated projectile fragmentation partial σ. GEMINI model, comparison with available data.
doi: 10.1088/0954-3899/39/5/055104
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
2012KH11 Phys.Rev. C 86, 064602 (2012) J.Khuyagbaatar, K.Nishio, S.Hofmann, D.Ackermann, M.Block, S.Heinz, F.P.Hessberger, K.Hirose, H.Ikezoe, B.Kinlder, B.Lommel, H.Makii, S.Mitsuoka, I.Nishinaka, T.Ohtsuki, Y.Wakabayashi, S.Yan Evidence for hindrance in fusion between sulfur and lead nuclei NUCLEAR REACTIONS 204,206,208Pb(34S, F), (36S, F), E=160-200 MeV; measured fission fragments, fission and ER σ at JAEA facility. Comparison with coupled-channel (HIVAP) calculations. Influence of coupling to the vibrational states in 34S.
doi: 10.1103/PhysRevC.86.064602
2012LI14 Eur.Phys.J. A 48, 13 (2012); Erratum Eur.Phys.J. A 49, 106 (2013) Y.J.Li, Z.H.Li, E.T.Li, X.X.Bai, J.Su, B.Guo, B.X.Wang, S.Q.Yan, S.Zeng, Z.C.Li, J.C.Liu, X.Liu, S.J.Jin, Y.B.Wang, L.Y.Zhang, X.Q.Yu, L.Li, G.Lian, Q.W.Fan, W.P.Liu New determination of the astrophysical 13C(p, γ)14N S(E) factors and reaction rates via the 13C(7Li, 6He)14N reaction NUCLEAR REACTIONS 13C(7Li, 6He), (7Li, 7Li), E=34 MeV; measured reaction products using Q3D magnetic spectrometer; deduced astrophysical S-factor, σ(θ), spectroscopic factors, potential parameters, resonance parameters; calculated spectroscopic factors, reaction rates using DWBA code PTOLEMY. Comparison with other data.
doi: 10.1140/epja/i2012-12013-x
2012LI35 Chin.Phys.C 36, 716 (2012) X.Liu, Y.-B.Wang, Z.-H.Li, S.-J.Jin, B.-X.Wang, Y.-J.Li, E.-T.Li, X.-X.Bai, B.Guo, J.Su, S.Zeng, S.-Q.Yan, G.Lian, W.-Z.Huang, W.-P.Liu Angular distribution of 6He+p elastic scattering NUCLEAR REACTIONS 1H(6He, p), E(cm)=4.3 MeV; measured reaction products, Ep, Ip. 6He; deduced σ(θ), optical potential parameters. DWBA calculations, comparison with available data.
doi: 10.1088/1674-1137/36/8/006
2012WA22 Acta Phys.Pol. B43, 1769 (2012) L.-C.Wang, D.-H.Zhang, S.Yan, Y.-J.Li, J.-X.Cheng, J.-S.Li, S.Kodaira, N.Yasuda Fragmentation Cross Sections of 56Fe at 471 A MeV on Al, C and CH2 Targets NUCLEAR REACTIONS Al, C(56Fe, X), E=471 MeV/nucleon; measured reaction products; deduced fragmentation total and partial charge-changing σ. Comparison with available data.
doi: 10.5506/APhysPolB.43.1769
2012ZH14 Chin.Phys.Lett. 29, 052101 (2012) Y.Zhao, X.-Z.Kang, S.-F.Shen, Y.-P.Yan, C.-Y.He, S.-W.Yan High-Spin States in Transuranium Nuclei 242, 244Pu NUCLEAR STRUCTURE 242,244Pu; calculated high-spin states, yrast band, J, π; deduced model modification parameters. Projected shell model, Nilsson model, comparison with available data.
doi: 10.1088/0256-307X/29/5/052101
2011LI18 Chin.Phys.Lett. 28, 052102 (2011) E.-T.Li, Z.-H.Li, J.Su, B.Guo, Y.-J.Li, S.-Q.Yan, X.-X.Bai, Y.-B.Wang, B.-X.Wang, G.Lian, S.Zeng, X.Fang, W.-J.Zhao, W.-P.Liu Astrophysical Rates for the 6He(p, γ)7Li Reaction NUCLEAR REACTIONS 1H(6He, γ), 2H(6He, n), E(cm)=9.1 MeV; measured reaction products; deduced σ(θ), S-factors, temperature-dependent reaction rates. Comparison with DWBA analysis, REACLIB library.
doi: 10.1088/0256-307X/
2011LI55 J.Phys.:Conf.Ser. 312, 042013 (2011) W.P.Liu, Z.H.Li, B.Guo, Y.B.Wang, J.Su, X.X.Bai, G.Lian, B.X.Wang, S.Q.Yan, S.Zeng, Y.J.Li, E.T.Li, S.J.Jin, X.Liu Current progress of nuclear astrophysical reaction and decay study at CIAE NUCLEAR REACTIONS 2H(12N, 13O), E(cm)=8.4 MeV; measured reaction products using telescope with ΔE silicon and double-sided silicon strip detector and PPAC; deduced σ(θ); calculated σ(θ) using optical potential plus CN contribution. 7Li(6Li, 7Li), E(cm)=0.02-0.07 MeV; measured reaction products; deduced 6Li(n, γ) σ using spectroscopic factor. RADIOACTIVITY 147Sm(α)[in metal Sm and Sm2O3]; measured Eα, Iα; deduced T1/2.
doi: 10.1088/1742-6596/312/4/042013
2010JI02 Chin.Phys.Lett. 27, 032102 (2010) S.-J.Jin, Y.-B.Wang, B.-X.Wang, X.-X.Bai, X.Fang, B.Guo, E.-T.Li, Y.-J.Li, Z.-H.Li, G.Lian, J.Su, s.-Q.Yan, S.Zeng, Z.-E.Yao, W.-P.Liu Excited States in 18Ne Studied via 17F+p NUCLEAR REACTIONS 1H(17F, α), (17F, γ), E=55.5 MeV; measured recoil nuclei, Eα, Iα; deduced σ(θ), excitation function, 18Ne resonance states, J, π.
doi: 10.1088/0256-307X/27/3/032102
2010LI19 Eur.Phys.J. A 44, 1 (2010) Z.H.Li, E.T.Li, B.Guo, X.X.Bai, Y.J.Li, S.Q.Yan, Y.B.Wang, G.Lian, J.Su, B.X.Wang, S.Zeng, X.Fang, W.P.Liu First measurement of the 2H(6He, 7Li)n angular distribution and proton spectroscopic factor in 7Li NUCLEAR REACTIONS 2H(7Li, 6He)n, E=46 MeV; measured reaction products; deduced σ(θ), proton spectroscopic factor of 7Li ground state, optical potential parameters. Comparison with DWBA calculations.
doi: 10.1140/epja/i2010-10944-8
2010LI37 Nucl.Phys. A834, 651c (2010) W.P.Liu, Z.H.Li, X.X.Bai, Y.B.Wang, G.Lian, B.Guo, J.Su, S.Zeng, B.X.Wang, S.Q.Yan, Y.J.Li, E.T.Li Lithium induced nuclear reactions of astrophysical interest NUCLEAR REACTIONS 7Li(6Li, 7Li), E=tandem; measured E(particle), I(particle, θ); deduced spectroscopic factor, σ. 6Li(n, γ), E=0.01-0.1 MeV; deduced σ. Comparison with other data and systems, calculations.
doi: 10.1016/j.nuclphysa.2010.01.114
2010LI38 Nucl.Phys. A834, 661c (2010) Z.H.Li, J.Su, B.Guo, E.T.Li, Z.C.Li, X.X.Bai, Y.J.Li, J.C.Liu, S.Q.Yan, B.X.Wang, Y.B.Wang, G.Lian, S.Zeng, X.Fang, W.P.Liu, Y.S.Chen, N.C.Shu, Q.W.Fan 2H(6He, 7Li)n, 12C(7Li, 6He)13N reactions and 12C(p, γ)13N astrophysical S(E) factors NUCLEAR REACTIONS 2H(6He, 7Li), E not given; 12C(7Li, 6He), E=44.0 MeV; measured σ(θ); deduced 12C(p, γ) S-factor; calculated S-factor using DWBA and asymptotic normalization coefficient. Comparison with other data.
doi: 10.1016/j.nuclphysa.2010.01.117
2010SU08 Chin.Phys.Lett. 27, 052101 (2010) J.Su, Z.-H.Li, B.Guo, X.-X.Bai, Z.-C.Li, J.-C.Liu, Y.-B.Wang, G.Lian, S.Zeng, B.-X.Wang, S.-Q.Yan, Y.-J.Li, E.-T.Li, Q.-W.Fan, W.-P.Liu Neutron Spectroscopic Factors of 7Li and Astrophysical 6Li(n, γ)7Li Reaction Rates NUCLEAR REACTIONS 7Li(6Li, 7Li), (6Li, 6Li), E=23.7 MeV; measured reaction products; deduced σ(θ), spectroscopic factors. NUCLEAR REACTIONS 6Li(p, γ), (n, γ), E(cm)<1.2 MeV; calculated astrophysical reaction rates, S-factors. DWBA analysis.
doi: 10.1088/0256-307X/27/5/052101
2010SU30 Eur.Phys.J. A 46, 69 (2010) J.Su, Z.H.Li, L.C.Zhu, G.Lian, X.X.Bai, Y.B.Wang, B.Guo, B.X.Wang, S.Q.Yan, S.Zeng, Y.J.Li, E.T.Li, S.J.Jin, X.Liu, Q.W.Fan, J.L.Zhang, X.Y.Jiang, J.X.Lu, X.F.Lan, X.Z.Tang, W.P.Liu Alpha decay half-life of 147Sm in metal samarium and Sm2O3 RADIOACTIVITY 147Sm(α); measured Eα, Iα for metalic Sm and Sm oxide; deduced T1/2. Halflives in both forms are different.
doi: 10.1140/epja/i2010-11028-7
2010TI01 Int.J.Mod.Phys. E19, 307 (2010) J.Tian, X.Li, S.Yan, Z.Wu, Z.Li Kinematic correlation of the ternary fission for the system 197Au + 197Au NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; measured reaction fragments; deduced mass number distributions, dynamical modes of ternary fission.
doi: 10.1142/S0218301310014777
2010TI07 Phys.Rev. C 82, 054608 (2010) J.Tian, X.Wu, Z.Li, K.Zhao, Y.Zhang, X.Li, S.Yan Mechanism of ternary breakup in the reaction 197Au+197Au at 15A MeV
doi: 10.1103/PhysRevC.82.054608
2010WA18 Nucl.Phys. A834, 100c (2010) Y.B.Wang, B.X.Wang, S.J.Jin, X.Qin, X.X.Bai, W.P.Liu, Z.H.Li, G.Lian, S.Zeng, B.Guo, S.Q.Yan, J.Su, Y.J.Li, E.T.Li, X.Fang Elastic resonance scattering of 13N+p and 17F+p NUCLEAR REACTIONS 2H(12C, 13N), (16O, 17F), E not given; 1H(13N, 13N), (17F, 17F), E=47.8 MeV; measured reaction products, proton spectrum; 14O, 18Ne; deduced resonance parameters, J, π, σ(θ); R-matrix analysis.
doi: 10.1016/j.nuclphysa.2010.01.030
2009LI27 Chin.Phys.Lett. 26, 072401 (2009) E.-T.Li, Z.-H.Li, Y.-J.Li, S.-Q.Yan, X.-X.Bai, B.Guo, J.Su, Y.-B.Wang, B.-X.Wang, G.Lian, S.Zeng, X.Fang, W.-J.Zhao, W.-P.Liu Angular Distribution of the 12C(6He, 7Li)11B Reaction NUCLEAR REACTIONS 12C(6He, 7Li), E = 34.6 MeV; measured σ(θ). comparison with DWBA calculation.
doi: 10.1088/0256-307X/26/7/072401
2009TI01 Chin.Phys.Lett. 26, 062502 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Possible Mechanisms of Ternary Fission in the 197Au+197Au System at 15 AMeV NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; Calculated ternary fission mass distribution, σ. ImQMD model.
doi: 10.1088/0256-307X/26/6/062502
2009TI12 Eur.Phys.J. A 42, 105 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Dynamic potential barrier in the entrance phase of heavy-ion fusion reactions NUCLEAR REACTIONS 100Mo(86Kr, X), E(cm)=153.9, 163.9, 173.9, 183.9, 203.9, 300.9 MeV; calculated fusion potential barrier and reaction mechanism features using an improved quantum molecular dynamics model.
doi: 10.1140/epja/i2009-10850-2
2009TI13 Chin.Phys.C 33, Supplement 1, 109 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Understanding of the dissipation mechanism in ternary fission for the system 197Au+197Au NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; calculated mass number distributions, impact parameter dependence of production probability of ternary fission and average mass number of fragments. Improved quantum molecular dynamics (ImQMD) model.
doi: 10.1088/1674-1137/33/S1/035
2007RA22 Eur.Phys.J. A 32, 51 (2007) F.Raiola, T.Spillane, B.Limata, B.Wang, S.Yan, M.Aliotta, H.W.Becker, J.Cruz, M.Fonseca, L.Gialanella, A.P.Jesus, K.U.Kettner, R.Kunze, H.Luis, J.P.Ribeiro, C.Rolfs, M.Romano, D.Schurmann, F.Strieder First hint on a change of the 210Po alpha-decay half-life in the metal Cu RADIOACTIVITY 210Po(α); measured Eα, Iα, T1/2 as a function of temperature by implanting Po ions in cooled metallic copper.
doi: 10.1140/epja/i2007-10012-8
2006LI34 Eur.Phys.J. A 28, 251 (2006) B.Limata, F.Raiola, B.Wang, S.Yan, H.W.Becker, A.D'Onofrio, L.Gialanella, V.Roca, C.Rolfs, M.Romano, D.Schurmann, F.Strieder, F.Terrasi First hints on a change of the 22Na β+-decay half-life in the metal Pd RADIOACTIVITY 22Na(β+) [from 19F(α, n)]; measured T1/2 for source implanted in Pd metal; deduced shorter T1/2 due to environmental effects.
doi: 10.1140/epja/i2006-10057-1
2006LI48 Phys.Rev. C 74, 035801 (2006) Z.H.Li, B.Guo, S.Q.Yan, G.Lian, X.X.Bai, Y.B.Wang, S.Zeng, J.Su, B.X.Wang, W.P.Liu, N.C.Shu, Y.S.Chen, H.W.Chang, L.Y.Jiang 13N(d, n)14O reaction and the astrophysical 13N(p, γ)14O reaction rate NUCLEAR REACTIONS 2H(13N, n), E(cm)=8.9 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 13N(p, γ), E(cm)=0-1.0 MeV; deduced astrophysical S-factors, reaction rate.
doi: 10.1103/PhysRevC.74.035801
2006LI62 Int.J.Mod.Phys. E15, 1899 (2006) W.-P.Liu, Z.-H.Li, X.-X.Bai, Y.-B.Wang, G.Lian, B.Guo, S.Zeng, S.-Q.Yan, B.-X.Wang, J.Su, N.-C.Shu, Y.-S.Chen Indirect measurements of nuclear astrophysics reactions using unstable nuclear beams NUCLEAR REACTIONS 2H(7Be, n), (11C, n), (8Li, p), (13N, n), E(cm) ≈ 6-9 MeV; analyzed σ, asymptotic normalization coefficients. 7Be, 11C, 8Li, 13N(p, γ), E=low; deduced astrophysical S-factors, reaction rates.
doi: 10.1142/S0218301306005514
2006SU01 Chin.Phys.Lett. 23, 55 (2006) J.Su, Z.-H.Li, B.Guo, W.-P.Liu, X.-X.Bai, S.Zeng, G.Lian, S.-Q.Yan, B.-X.Wang, Y.-B.Wang Astrophysical Reaction Rates of the 8Li(p, g)9Beg.s Direct Capture Reaction NUCLEAR REACTIONS 2H(8Li, n), E=40 MeV; measured σ(θ); deduced optical potential parameters. 8Li(p, γ), E(cm) ≈ 0-2 MeV; deduced astrophysical S-factors, reaction rates.
doi: 10.1088/0256-307X/23/1/017
2006WA21 Eur.Phys.J. A 28, 375 (2006) B.Wang, S.Yan, B.Limata, F.Raiola, M.Aliotta, H.W.Becker, J.Cruz, N.De Cesare, A.D'Onofrio, Z.Fulop, L.Gialanella, G.Gyurky, G.Imbriani, A.Jesus, J.P.Ribeiro, V.Roca, D.Rogalla, C.Rolfs, M.Romano, D.Schurmann, E.Somorjai, F.Strieder, F.Terrasi Change of the 7Be electron capture half-life in metallic environments RADIOACTIVITY 7Be(EC) [7Li(p, n)]; measured T1/2 for source implanted in Pd, In metals and Li2O insulator; deduced longer T1/2 due to environmental effects in the metals, no change in the insulator.
doi: 10.1140/epja/i2006-10068-x
2005GU29 Nucl.Phys. A761, 162 (2005) B.Guo, Z.H.Li, W.P.Liu, X.X.Bai, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, J.Su, Y.Lu The 8Li(d, p)9Li reaction and astrophysical 8B(p, γ)9C reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E(cm)=7.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 8B(p, γ), E=low; calculated astrophysical S-factor. DWBA analysis, inverse kinematics, comparison with data.
doi: 10.1016/j.nuclphysa.2005.07.013
2005LI19 Phys.Rev. C 71, 052801 (2005) Z.H.Li, W.P.Liu, X.X.Bai, B.Guo, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, Y.Lu, J.Su, Y.S.Chen, K.S.Wu, N.C.Shu, T.Kajino The 8Li(d, p)9Li reaction and the astrophysical 8Li(n, γ)9Li reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E=39 MeV; measured particle spectra, σ(θ). 8Li(n, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.71.052801
2005LI35 Chin.Phys.Lett. 22, 1870 (2005) Z.H.Li, B.Guo, W.-P.Liu, X.-X.Bai, G.Lian, J.Su, S.-Q.Yan, B.-X.Wang, S.Zeng Radius of 9C from the Asymptotic Normalization Coefficient NUCLEAR REACTIONS 2H(8Li, p), E(cm)=7.8 MeV; measured σ(θ); deduced asymptotic normalization coefficients. 9C deduced radius, density distributions, halo structure.
doi: 10.1088/0256-307X/22/8/013
2005LI40 Nucl.Phys. A758, 110c (2005) W.Liu, Z.Li, X.Bai, G.Lian, B.Guo, S.Zeng, S.Yan, B.Wang, N.Shu, K.Wu, Y.Chen Nuclear Astrophysics Experiments at CIAE NUCLEAR REACTIONS 2H(7Be, n), (11C, n), (8Li, p), E ≈ 5.8-9.8 MeV; measured σ(θ), total σ; deduced astrophysical S-factors.
doi: 10.1016/j.nuclphysa.2005.05.164
2005ZE03 Chin.Phys.Lett. 22, 2219 (2005) S.Zeng, W.-P.Liu, Z.-H.Li, X.-X.Bai, S.-Q.Yan, B.-X.Wang, G.Lian, J.Su Measurement of 2H(8Li, 9Be)n Reaction Relevant to Primordial Nucleosynthesis NUCLEAR REACTIONS 2H(8Li, 9Be), E=40.38 MeV; measured particle spectra, σ(θ); deduced astrophysical S-factors.
doi: 10.1088/0256-307X/22/9/022
2003LI51 Nucl.Phys. A728, 275 (2003) W.Liu, Z.Li, X.Bai, B.Guo, S.Zeng, Y.Chen, S.Yan, B.Wang, G.Lian, Y.Lu, K.Wu, N.Shu Determination of 11C(p, γ) 12N astrophysical S-factor via measurement of 11C(d, n)12N reaction NUCLEAR REACTIONS 2H(11C, 12N), E(cm)=9.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 11C(p, γ), E=low; deduced astrophysical S-factor, reaction mechanism features. DWBA analysis.
doi: 10.1016/j.nuclphysa.2003.08.017
2001SA45 Prog.Theor.Phys.(Kyoto), Suppl. 141, 1 (2001) F.Sakata, T.Marumori, Y.Hashimoto, S.-W.Yan Nonlinear Dynamics of Nuclear Collective Motion
doi: 10.1143/PTPS.141.1
1996DU11 Nucl.Instrum.Methods Phys.Res. A369, 424 (1996) H.Du, Y.Liu, J.Li, S.Yan, G.Li, Y.Zhu, L.Yao Progress in Preparation 4πβ Quantitative Sources RADIOACTIVITY 60Co(β-); measured βγ-coin; deduced detector plateau-characteristics.
doi: 10.1016/S0168-9002(96)80023-4
1993ZH01 Z.Phys. A344, 251 (1993) The Pick-Up Mechanism in Composite Particle Emission Processes NUCLEAR REACTIONS 27Al, 51V, 59Co, 93Nb, 115In, 139La, 181Ta, 209Bi(n, t), E ≈ 15-20 MeV; calculated reaction σ(E). Exciton model with nucleon-pickup mechanism.
1992WA21 Chin.J.Nucl.Phys. 14, No 1, 87 (1992) Sensitivity of Nuclear Level Density Parameters NUCLEAR REACTIONS 197Au(n, γ), E ≤ 10 MeV; 197Au(n, n'), (n, 2n), E ≤ 20 MeV; calculated σ(E); deduced level density parameter dependence. Statistical, preequilibrium models.
1992ZH39 Chin.J.Nucl.Phys. 14, No 4, 345 (1992) The Pick-Up Mechanism in Composite Particle Emission Processes NUCLEAR REACTIONS 27Al, 51V, 59Co, 93Nb, 115In, 139La, 181Ta, 209Bi(n, t), E ≈ 15-20 MeV; calculated σ(E). Exciton model.
1987SH07 Chin.J.Nucl.Phys. 9, 16 (1987) Shi Xiangjun, Yan Shiwei, Zhang Jingshang Statistical Theoretical Calculation of the Double Differential Cross Sections and Secondary Neutron Energy Spectra for 238U(n, n') Reaction NUCLEAR REACTIONS 238U(n, n'), E=14.2 MeV; calculated σ(En', θn'). Preequilibrium statistical theory, evaporation model.
1986WE10 Z.Phys. A324, 325 (1986) Wen Yuanqi, Shi Xiangjun, Yan Shiwei, Zhuo Yizhong, Han Huiyi A Semi-Classical Model of Multi-Step Direct and Compound Nuclear Reactions NUCLEAR REACTIONS 197Au, 120Sn(p, p'), E=62 MeV; 93Nb(n, n'), E=14.6 MeV; calculated σ(θ, Ep), σ(θ, En). Semi-classical model, multi-step direct, compound nuclear reactions.
1986WE14 Chin.J.Nucl.Phys. 8, 9 (1986) Wen Yuanqi, Han Huiyi, Shi Xiangjun, Yan Shiwei, Zhuo Yizhong The Multi-Step Energy Correlation of Exciton Model and the Calculation of Double Differential Cross Section NUCLEAR REACTIONS 93Nb(n, n'), E=15 MeV; 120Sn, 197Au(p, p'), E=62 MeV; calculated σ(θn, En), σ(θp, Ep). Exciton model, multi-step energy correlation.
1980LI23 J.Nucl.Radiochem. 2, 1 (1980) The absolute determination of cumulative yield of several nuclides from thermal neutron and fission spectrum neutron induced fission of 235U NUCLEAR REACTIONS 235U(n, F)95Zr/99Mo/144Ce, E thermal; measured reaction products by radiochemical technique; deduced cumulative fission yields. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32633. Back to query form Note: The following list of authors and aliases matches the search parameter S.Yan: , S.C.YAN, S.Q.YAN, S.W.YAN, S.X.YAN |