NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = Wu Zhongli Found 28 matches. 2024HU03 Eur.Phys.J. A 60, (2024) Y.Hu, Yu.M.Gledenov, Z.Cui, J.Liu, H.Bai, C.Xia, Zh.Chen, Z.Wu, W.Ren, W.Cao, T.Fan, G.Zhang, E.Sansarbayar, G.Khuukhenkhuu, L.Krupa, I.Chuprakov, Q.Fan, X.Ruan, H.Huang, J.Ren, Y.Gao, X.Yang Cross section measurement for the 14N(n, α0, 1)11B reactions in the 4.5–11.5 MeV neutron energy region NUCLEAR REACTIONS 14N(n, α), E=4.5 -11.5 MeV; measured reaction products, En, In, Eα, Iα; deduced σ and uncertainties. Comparison with EXFOR, ENDF/B-VIII.0, ENDF/B-VII.1, JEFF-3.3, CENDL-3.2, ROSFOND-2010, ADS-2.0, JENDL-5, BROND-3.1, BROND-2.2, FENDL-3.2b, and TENDL-2021 libraries. The 4.5 MV Van de Graaff accelerator at Peking University and the HI-13 tandem accelerator of China Institute of Atomic Energy (CIAE).
doi: 10.1140/epja/s10050-024-01268-9
2024WU07 Chin.Phys.C 48, 024101 (2024) From masses and radii of neutron stars to EOS of nuclear matter through neural network
doi: 10.1088/1674-1137/ad0e04
2023XI04 Appl.Radiat.Isot. 197, 110817 (2023) Y.Xie, C.Cheng, W.Zhang, X.Wang, W.Qin, W.Liu, S.Lin, P.Xiao, Z.Wu, W.Jia Feasibility study of on-line monitoring gadolinium based on neutron induced gamma activation
doi: 10.1016/j.apradiso.2023.110817
2022WU05 Phys.Lett. B 825, 136886 (2022) Production of proton-rich nuclei in the vicinity of 100Sn via multinucleon transfer reactions NUCLEAR REACTIONS 112Sn(58Ni, X)Pd/Ag/Cd/In/Sn/Xe/I/Te/Sb, E(cm)=221.77 MeV; analyzed available data; calculated σ using TDHF+GEMINI approach.
doi: 10.1016/j.physletb.2022.136886
2019HU06 Nucl.Phys. A982, 927c (2019) H.Huang, B.Xiao, H.Xiong, Z.Wu, Y.Mu, H.Song Applications of deep learning to relativistic hydrodynamics
doi: 10.1016/j.nuclphysa.2018.11.004
2019WU07 Phys.Rev. C 99, 064902 (2019) Universal scaling of the σ field and net-protons from Langevin dynamics of model A
doi: 10.1103/PhysRevC.99.064902
2019WU09 Phys.Rev. C 100, 014612 (2019) Microscopic studies of production cross sections in multinucleon transfer reaction 58Ni 124Sn NUCLEAR REACTIONS 124Sn(58Ni, X), E(cm)=150, 153, 157, 160.6 MeV; calculated multinucleon transfer and production σ(E) for secondary fragments as function of number of transferred neutrons, energy dependence of the total cross sections integrated over all the neutron transfer channels, total kinetic energy loss, neutron to proton ratio of projectile-like and target-like fragments, transferred nucleon number, and neutron pickup and proton removal transfer probabilities using combined microscopic time-dependent Hartree-Fock (TDHF) and GEMINI++ statistical model approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.014612
2019XU05 Phys.Rev. C 99, 034618 (2019) Y.Xu, Y.Han, H.Liang, Z.Wu, H.Guo, C.Cai Global optical model potential for the weakly bound projectile 9Be NUCLEAR REACTIONS Mg(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 27Al(9Be, 9Be), E=12.0, 14.0, 18.0, 20.0, 22.0, 25.0, 28.0, 32.0, 33.0, 35.0.40.0, 47.5 MeV; 28Si(9Be, 9Be), E=12.0, 13.0, 14.0, 17.0, 20.0, 23.0, 26.0, 30.0, 45.0, 50.0, 60.0 MeV; 40Ca(9Be, 9Be), E=14.0, 20.0, 26.0, 45.0.50.0, 60.0 MeV; 58Ni(9Be, 9Be), E=20.0, 26.0 MeV; 64Zn(9Be, 9Be), E=17.0, 19.0, 21.0, 23.0, 26.0, 28.0, 28.4, 28.97 MeV; 89Y(9Be, 9Be), E=18.6, 20.6, 22.7, 24.7, 26.7, 28.7, 33.2 MeV; Ag(9Be, 9Be), E=26.0 MeV; 144Sm(9Be, 9Be), E=30.0, 31.5, 33.0, 34.0, 35.0, 37.0, 39.0, 41.0, 44.0, 48.0 MeV; 208Pb(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 9.5, 40.0, 41.0, 42.0, 44.0, 46.0, 47.2, 48.0, 50.0, 60.0, 68.0, 75.0 MeV; 209Bi(9Be, 9Be), E=37.0, 37.8, 38.0, 38.2, 38.5, 38.7, 39.0, 39.5, 40.0, 41.0, 42.0, 44.0, 46.0, 48.0 MeV; analyzed elastic σ(θ, E) data for global phenomenological energy-dependent optical model potential parameters for 9Be. 9Be, 12,13C, 27Al, 64Zn, 89Y, 144Sm(9Be, X), E=10-300 MeV; 28Si, Cu(9Be, X), E=10-500 MeV; 89Y(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (9Be, X), (11B, X); calculated reaction σ(E) using optical model and compared with experimental data. 9Be(9Be, 9Be), E=14.0, 20.0, 26.0 MeV; 12C(9Be, 9Be), E=13.0, 14.0, 14.5, 17.3, 19.0, 20.0, 21.0, 26.0, 153.8 MeV; 13C(9Be, 9Be), E=19.46, 25.05 MeV; 16O(9Be, 9Be), E=20.0, 25.94 MeV; calculated elastic σ(θ, E) using optical model parameters and compared with experimental data.
doi: 10.1103/PhysRevC.99.034618
2018GU21 Phys.Rev. C 98, 064609 (2018) Isotopic trends of quasifission and fusion-fission in the reactions 48Ca + 239, 244Pu NUCLEAR REACTIONS 239,244Pu(48Ca, X), E=204.02, 216.76 MeV; calculated time evolution of the mass density of 48Ca+239Pu, contact time, mass and charge of heavy fragments as a function of impact parameter for the tip and side collisions, mass-angle and total kinetic energy-mass distributions of quasi-fission (QF) fragments. Microscopic time-dependent Hartree-Fock (TDHF) method for the fusion and quasifission dynamics with the statistical evaporation model HIVAP for fusion-fission dynamics.
doi: 10.1103/PhysRevC.98.064609
2018XU01 Phys.Rev. C 97, 014615 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai Global phenomenological optical model potential for the 7Li projectile nucleus NUCLEAR REACTIONS 9Be(7Li, 7Li), E=15.75, 24.0, 30.0, 63.0, 130.0 MeV; 12C(7Li, 7Li), E=7.5, 9.0, 12.0, 15.0, 36.0, 131.8 MeV; 16O(7Li, 7Li), E=26.0, 36.0, 42.0, 50.0 MeV; 11B, 12,13C, 24Mg(7Li, 7Li), E=34.0 MeV; 24,26Mg(7Li, 7Li), E=88.7 MeV; 27Al(7Li, 7Li), E=6.0, 7.0, 8.0, 9.0, 10.0, 11.0, 12.0, 13.0, 14.0, 16.0, 18.0, 19.0, 24.0 MeV; 28Si(7Li, 7Li), E=8.0, 8.5, 9.0, 10.0, 11.0, 11.5, 13.0, 15.0, 16.0, 21.0, 26.0, 36.0, 177.8 MeV; 40,44,48Ca(7Li, 7Li), E=34.0; 40Ca(7Li, 7Li), E=88.7 MeV; 46,48Ti(7Li, 7Li), E=17.0 MeV; 54Fe(7Li, 7Li), E=36.0, 42.0, 48.0 MeV; 56Fe, 65Cu, 90Zr(7Li, 7Li), E=34.0 MeV; 58Ni(7Li, 7Li), E=14.22, 16.25.18.28, 19.0, 20.31.34.0, 42.0 MeV; 60,62Ni, 64,68Zn(7Li, 7Li), E=34.0 MeV; 80Se(7Li, 7Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 23.0, 26.0 MeV; 89Y(7Li, 7Li), E=60.0 MeV; 116Sn(7Li, 7Li), E=18.0, 19.0, 20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0 MeV; 120Sn(7Li, 7Li), E=19.5, 20.0, 20.5, 22.0, 24.0, 25.0, 26.0, 28.0, 30.044.0 MeV; 138Ba(7Li, 7Li), E=21.0, 22.0, 23.0, 24.0, 28.0, 30.0, 32.0, 52.0 MeV; 140Ce, 142Nd(7Li, 7Li), E=52.0 MeV; 144Sm(7Li, 7Li), E=21.6, 22.1, 22.6.23.0, 25.0, 27.0, 29.0, 30.0, 32.0, 35.0, 40.8, 52.0 MeV; 208Pb(7Li, 7Li), E=27.0, 29.0, 33.0, 39.0, 42.0, 52.0 MeV; 232Th(7Li, 7Li), E=24.0, 26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed σ(θ, E) experimental data by global phenomenological optical model potential. 13C, 27Al, 64Zn, 116Sn, 138Ba, (7Li, X), E<300 MeV; 28Si, Cu, 208Pb(7Li, X), E<400 MeV; calculated reaction σ(E) using optical model, and compared with experimental data.
doi: 10.1103/PhysRevC.97.014615
2018XU10 Phys.Rev. C 98, 024619 (2018) Y.Xu, Y.Han, J.Hu, H.Liang, Z.Wu, H.Guo, C.Cai 6Li global phenomenological optical model potential NUCLEAR REACTIONS 24Mg, 48Ca(6Li, 6Li), E=240.0 MeV; 25,26Mg, 39K, 91Zr(6Li, 6Li), E=34.0 MeV; 27Al(6Li, 6Li), E=7.0, 8.0, 10.0, 12.0, 18.0, 34.0 MeV; 28Si(6Li, 6Li), E=7.5, 9.0, 11.0, 13.0, 16.0, 20.0, 21.0, 25.0, 27.0, 34.0, 46.0, 99.0, 135.0, 154.0, 210.0, 240.0, 318.0, 350.0 MeV; 40Ca(6Li, 6Li), E=50.6, 99.0, 156.0, 210.0, 240.0 MeV; 54Fe(6Li, 6Li), E=38.0, 44.0, 50.0 MeV; 59Co(6Li, 6Li), E=12.0, 18.0, 26.0, 30.0 MeV; 58Ni(6Li, 6Li), E=9.85, 11.21, 12.13, 13.04, 14.04, 34.0, 50.6, 73.7, 90.0, 99.0, 210.0, 240.0 MeV; 65Cu(6Li, 6Li), E=25.0 MeV; 64Zn(6Li, 6Li), E=10.77, 11.69, 12.0, 12.43, 13.0, 13.54, 13.8, 14.92, 15.0, 16.30, 16.5, 18.0, 18.14, 19.98, 22.0 MeV; 72,74,76Ge(6Li, 6Li), E=28.0 MeV; 80Se(6Li, 6Li), E=14.0, 14.5, 15.0, 15.5, 16.0, 17.0, 18.0, 19.0, 20.0, 22.19, 23.0, 26.0 MeV; 89Y(6Li, 6Li), E=60.0 MeV; 90Zr(6Li, 6Li), E=11.0, 12.0, 13.0, 15.0, 17.0, 19.0, 21.0, 25.0, 30.0, 34.0, 60.0, 70.0, 73.7, 99.0, 156.0, 210.0, 240.0 MeV; 92,94,96Zr(6Li, 6Li), E=70.0 MeV; 112Sn(6Li, 6Li), E=21.0, 22.0, 23.0, 25.0, 30.0, 35.0 MeV; 116Sn(6Li, 6Li), E=20.0, 21.0, 22.0, 23.0, 24.0, 26.0, 30.0, 35.0, 40.0 MeV; 118Sn(6Li, 6Li), E=42.0 MeV; 120Sn(6Li, 6Li), E=30.0, 44.0, 90.0 MeV; 124Sn(6Li, 6Li), E=73.7 MeV; 138Ba(6Li, 6Li), E=21.0, 22.0, 23.0, 24.0, 26.0, 28.0 MeV; 144Sm(6Li, 6Li), E=21.0, 22.1, 22.6, 24.1, 26.0, 28.0, 30.1, 32.2, 35.1, 42.3 MeV; 208Pb(6Li, 6Li), E=25.0, 29.0, 31.0, 33.0, 35.0, 36.0, 37.0, 39.0, 42.0, 43.0, 46.0, 48.0, 50.6, 73.7, 88.0, 90.0, 99.0, 156.0, 210.0 MeV; 209Bi(6Li, 6Li), E=24.0, 26.0, 28.0, 29.9, 30.0, 32.0, 32.8, 34.0, 36.0, 40.0, 44.0, 50.0 MeV; 232Th(6Li, 6Li), E=26.0, 30.0, 32.0, 35.0, 40.0, 44.0 MeV; analyzed differential σ(θ, E) data; deduced a new set of 6Li global phenomenological energy-dependent optical potential parameters based on the form of the Woods-Saxon potential within the optical model. 63,65Cu, 64Zn, 112,116Sn, 138Ba, 208Pb(6Li, X), E<400 MeV; calculated reaction σ(E), and compared with experimental data.
doi: 10.1103/PhysRevC.98.024619
2017LI21 Nucl.Sci.Eng. 187, 107 (2017) H.Liang, Z.Wu, Z.Zhang, Y.Han, X.Jiao Calculations and Analysis of n+93Nb Reaction NUCLEAR REACTIONS 93Nb(n, X), E<200 MeV; calculated σ, σ(E), σ(θ), σ(θ, E) using theoretical models. Comparison with ENDF/B-VII, JENDL-4, TENDL-2015 libraries, experimental data.
doi: 10.1080/00295639.2017.1295699
2016LI45 Yuan.Wul.Ping. 33, 160 (2016); Nucl.Phys.Rev. 33, 160 (2016) C.Lin, X.Xu, J.Wang, L.Sun, H.Jia, L.Yang, P.Ma, J.Ma, Y.Yang, S.Jin, M.Huang, Z.Bai, Z.Wu, F.Yang, Z.Hu, M.Wang, X.Lei, H.Zhang, H.Xu, G.Xiao Proton and Two-proton Emissions from Proton-rich Nuclei with 10 ≤ Z ≤ 20 RADIOACTIVITY 28,29S, 26,27P, 17,18Ne(2p), 27S, 26P, 22,25Si, 20Mg, 23Si, 22Al, 21Mg, 24Si, 23Al, 36,37Ca(β+p), (β+2p); measured decay products, Ep, Ip; deduced energy, T1/2, branching-ratios.
doi: 10.11804/NuclPhysRev.33.02.160#
2016SU22 Yuan.Wul.Ping. 33, 230 (2016); Nucl.Phys.Rev. 33, 230 (2016) L.Sun, X.Xu, C.Lin, J.Wang, D.Fang, Z.Li, Y.Wang, J.Li, L.Yang, N.Ma, K.Wang, H.Zhang, H.Wang, C.Li, C.Shi, M.Nie, X.Li, H.Li, J.Ma, P.Ma, S.Jin, M.Huang, Z.Bai, J.Wang, F.Yang, H.Jia, H.Zhang, Z.Liu, P.Bao, S.Wang, Z.Wu, Y.Yang, Z.Chen, J.Su, Y.Shen, Y.Zhou, W.Ma, J.Chen An implantation and detection system for spectroscopy of 22, 24Si RADIOACTIVITY 22,24Si(β+p); measured decay products, Ep, Ip; deduced energy levels, J, π, T1/2, branchning ratios.
doi: 10.11804/NuclPhysRev.33.02.230
2016WU01 Phys.Rev. C 93, 034334 (2016) Empirical residual neutron-proton interaction in odd-odd nuclei ATOMIC MASSES A=10-260; analyzed np interactions from experimental binding energies for odd-A, even-even, odd-odd, and for all known (except N=Z) nuclei; calculated δnp interaction using mac-mic mass formula, shell model mass formulas with parameters taken from literature, and the HFB mass formula. Z=9-131, N=7-219; deduced δnp interaction for all the predicted 2564 odd-odd nuclei from mass formulas. Z=5-103, N=5-153; deduced δnp interaction for all the known 486 odd-odd nuclei from experimental binding energies and nuclear mass formula calculations. Numerical results for individual nuclei are given in two supplementary files.
doi: 10.1103/PhysRevC.93.034334
2014LI10 Ann.Nucl.Energy 69, 301 (2014) The energy spectra and double-differential cross-sections for p+92, 94, 95, 96, 97, 98, 100Mo reactions at the incident energies from threshold to 200 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, xn), (p, xp), (p, xd), (p, xα), (p, xt), E<160 MeV; calculated σ(E), σ(E, θ). Exciton model including the improved Iwamoto-Harada model, comparison with experimental data.
doi: 10.1016/j.anucene.2014.02.008
2014WU07 Ann.Nucl.Energy 73, 17 (2014) Z.Wu, H.Liang, J.Li, Z.Zhang, Y.Han Theoretical calculations and evaluations of n + 32, 33, 34, 36, nat.S reactions NUCLEAR REACTIONS 32,33,34,36S, S(n, n), (n, n'), (n, X), (n, p), (n, t), (n, xn), (n, xp), E<200 MeV; calculated σ, σ(θ, E), σ(θ). APMN nuclear model code, comparison ENDF/B-VII, JENDL-4, and TENDL-2012 libraries.
doi: 10.1016/j.anucene.2014.05.032
2011WU01 Nucl.Instrum.Methods Phys.Res. B269, 671 (2011) Calculation of cross-sections for p+ 92, 94, 95, 96, 97, 98, 100Mo reactions up to 160 MeV NUCLEAR REACTIONS 92,94,95,96,97,98,100Mo(p, p), (p, p'), (p, α), (p, nα), (p, pα), (p, n), (p, 2n), (p, 3α), (p, 3n), (p, 4n), (p, 4n2p), (p, 3He), (p, np), E<200 MeV; calculated σ. MEND nuclear reaction model code.
doi: 10.1016/j.nimb.2011.01.126
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
2004WA08 Phys.Rev. C 69, 034608 (2004) N.Wang, Z.Li, Z.Wu, J.Tian, Y.X.Zhang, M.Liu Further development of the improved quantum molecular dynamics model and its application to fusion reactions near the barrier NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 114,132Sn, 140Ce, 208Pb; calculated binding energies, radii. NUCLEAR REACTIONS 48Ca, 90Zr(40Ca, X), 16O, 208Pb(16O, X), 131I(131I, X), 208Pb(54Cr, X), 230Th(32S, X), 250Fm(12C, X), E not given; calculated static Coulomb barriers. 48Ca(40Ca, X), E(cm)=52, 54, 58, 60 MeV; calculated fusion probability. 48Ca, 48Ti, 90,96Zr(40Ca, X), E(cm)=48-112 MeV; 46Ti(46Ti, X), E(cm)=58-72 MeV; 89Y(32S, X), (34S, X), E(cm)=72-92 MeV; 92Zr(28Si, X), (35Cl, X), E(cm)=65-100 MeV; 64Ni(132Sn, X), E(cm)=140-168 MeV; calculated fusion σ. Improved quantum molecular dynamics model, comparison with data.
doi: 10.1103/PhysRevC.69.034608
1997AR02 Phys.Rev. C55, 788 (1997) Preferred Modes of Decay in Nuclear Fragmentation NUCLEAR STRUCTURE 120Sn; 240Pu; calculated partial widths ratio related quantity vs energy following fragmentation; deduced preferred modes of decay related features. Transition state theory.
doi: 10.1103/PhysRevC.55.788
1988LI15 Chin.J.Nucl.Phys. 10, 52 (1988) Li Jianwei, Wu Zhihua, Wu Songmao, Song Linggen, Yu Junsheng Measurements of the Cross Sections of the Reactions 115In(n, 2n)114mIn and 113In(n, 2n)112mIn NUCLEAR REACTIONS 113,115In(n, 2n), E=12.7-18.6 MeV; measured isomer production σ(E). 115In(n, 2n), E=15.75 MeV; measured isomer production. Activation technique. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30782. 1987GR23 Phys.Rev.Lett. 59, 1080 (1987) N.Grion, R.Rui, F.M.Rozon, T.Anderl, J.Ernst, D.R.Gill, M.Hanna, J.J.Kraushaar, R.R.Johnson, R.Olszewski, M.E.Sevior, G.Sheffer, G.R.Smith, R.P.Trelle, Z.Wu Measurement of the 16O(π+, π+π-) Reaction at T(π+) = 280 MeV NUCLEAR REACTIONS 16O(π+, π+π-), E=280 MeV; measured σ(E(π+), θ(π+), θ(π-)), σ(E(π+)). Tof.
doi: 10.1103/PhysRevLett.59.1080
1987WA29 Chin.J.Nucl.Phys. 9, 193 (1987) Wang Xiaozhong, Tang Hongqing, Zhang Ying, Xu Jun, Yu Chunying, Yu Zhirong, Wu Zhongming, Bai Xixiang Preequilibrium Effect in the Neutron Angular Distribution of the 40Ar(α, n)43Ca Reaction NUCLEAR REACTIONS, MECPD 40Ar(α, n), E=26 MeV; measured σ(En, θn). Gas target, tof. Exciton model.
1986FA15 Chin.J.Nucl.Phys. 8, 102 (1986) Fan Guoying, Zhu Yongtai, Miao Hobin, Li Songli, Yin Xu, Wang Qi, Feng Enpu, Shen Wenqing, Jin Genming, Zhan Wenlong, Wu Zhongli, Xie Yuonxiang, Song Shizhan, Guo Zhongyan, Qiao Weimin, Cai Jin-Gxiang, Wang Xiaoming Study of α-Particle Emission Mechanism in N + Ni Reaction at 96 MeV NUCLEAR REACTIONS 58Ni(14N, αX), E=96 MeV; measured Eα, αX-coin; deduced α-emission mechanism, shadow effect. ΔE-E telescopes.
1985SO11 Chin.J.Nucl.Phys. 7, 58 (1985) Song Linggen, Wu Songmao, Xu Zhizheng, Yu Junsheng, Wu Zhihua Measurement of Inelastic Cross Sections for the Reaction 87Sr(n, n')87mSr NUCLEAR REACTIONS 87Sr(n, n'), E=0.9-1.8, 3.2-5.7 MeV; measured σ(E), isomer production.Enriched target, activation techniques. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32503. 1984LI26 Chin.J.Nucl.Phys. 6, 250 (1984) Ling Yinsheng, Wu Zumei, Tu Chuanshi Group Theoretical Disscussion about the Energy Spectrum of Odd A Nucleus by Enlarging the Fermions Configuration Space NUCLEAR STRUCTURE 159Tb; calculated levels, B(E2). Group theoretical methods.
1982GU16 Chin.J.Nucl.Phys. 4, 209 (1982) Guo Zhendi, Qian Jinhua, Wu Zhihua, Xu Zhizheng, He Mianhong, Huang Shibin, Yang Fujia The γ Resonant Absorption Experiments of the 9.966 MeV Bound State in 24Mg and the 12.33 MeV Unbound State in 28Si NUCLEAR REACTIONS 24Mg(γ, γ'), E=9.983 MeV; 28Si(γ, γ'), E=12.33 MeV; measured level widths. Resonant absorption method, proton capture reaction gamma source.
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