NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Y.X.Yang Found 12 matches. 2022LI72 Phys.Rev. C 106, 065804 (2022) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, D.X.Wang, S.Y.Zhang, G.L.Yang, X.K.Li, Z.D.An, J.J.He, W.Luo, X.G.Cao, L.L.Song, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, Y.D.Liu, C.W.Ma, Y.T.Wang, J.Su, L.Y.Zhang, Y.X.Yang, S.Feng, W.B.Liu, W.Q.Su, S.Jin, K.J.Chen Experimental determination of the neutron resonance peak of 162Er at 67.8 eV NUCLEAR REACTIONS 162Er(n, γ), E=20-100 eV; measured Eγ, Iγ; deduced neutron-capture yield, resonances, decay widths. Resonance parameters at 67.8 eV are extracted for the first time. R-matrix analysis. Comparison to other experimental results and ENDF/B-VIII.0 data. 4 C6D6 detectors. Neutron beam from Back-n Facility of the CSNS.
doi: 10.1103/PhysRevC.106.065804
2022ZH54 J.Phys.(London) G49, 095104 (2022) X.-r.Zhang, G.Zhang, J.-j.Li, Z.Liu, Y.-x.Yang, F.-s.Zhang Production mechanism and prediction cross sections of unknown neutron-rich 263-265, 267-269Lr isotopes in multinucleon transfer reactions based on the dinuclear system model NUCLEAR REACTIONS 235U(40Ar, X), E(cm)=184.6 MeV; 249Bk(130Te, X)263Lr/264Lr/265Lr/267Lr/268Lr/269Lr, E(cm)=526.7 MeV; analyzed available data; calculated production σ.
doi: 10.1088/1361-6471/ac81df
2021LI61 Phys.Rev. C 104, 054302 (2021) X.X.Li, L.X.Liu, W.Jiang, J.Ren, H.W.Wang, G.T.Fan, X.G.Cao, Y.Zhang, X.R.Hu, Z.R.Hao, P.Kuang, B.Jiang, X.H.Wang, J.F.Hu, J.C.Wang, D.X.Wang, S.Y.Zhang, Y.D.Liu, X.Ma, C.W.Ma, Y.T.Wang, Z.D.An, J.J.He, J.Su, L.Y.Zhang, Y.X.Yang, W.B.Liu, W.Q.Su New experimental measurement of natEr(n, γ) cross sections between 1 and 100 eV NUCLEAR REACTIONS 162,164,166,167,168,170Er, 12,13C, 197Au(n, γ), E=0.001-100 keV; measured E(n), I(n), Eγ, Iγ using C6D6 liquid scintillator and a silicon monitor and natural Er, C and Au targets at the China spallation neutron source (CSNS) facility; deduced neutron-capture σ(E), capture yields as function of E(n), neutron resonances in Er isotopes in the 1-100 eV region. 162,164,166,167,168Er; deduced energies of 43 neutron resonances (nine for 162Er, five for 164Er, three for 166Er, 25 for 167Er, one for 168Er), cross sections, widths Γγ and Γn by R-matrix analysis. Comparison with previous experimental data, and with data in evaluated databases ENDF/B-VIII.0, ENDF/B-VII.1, JENDL-4.0, and ROSFOND-2010.
doi: 10.1103/PhysRevC.104.054302
2015SU02 Chin.Phys.C 39, 014102 (2015) X.-J.Sun, C.-G.Yu, N.Wang, Y.-X.Yang, C.H.Pan Pre-neutron-emission mass distributions for reaction 238U(n, f) up to 60 MeV NUCLEAR REACTIONS 238U(n, F), E<60 MeV; analyzed available data; deduced σ, preneutron-emission mass distributions, fission yields. Empirical fission potential model, comparison with available data.
doi: 10.1088/1674-1137/39/1/014102
2010YA14 Phys.Rev. C 82, 024607 (2010) Elastic α+20Ne scattering in the α+16O model of 20Ne NUCLEAR REACTIONS 20Ne(α, α), E=31.1, 54.1, 104.0 MeV; analyzed differential σ(E, θ) data using a folding potential with Woods-Saxon type imaginary part, and based on 16O+α structure model.
doi: 10.1103/PhysRevC.82.024607
2009ON01 Eur.Phys.J. A 41, 229 (2009) Intermediate-energy proton- 20Ne elastic scattering in the α + 16O model of 20Ne NUCLEAR STRUCTURE 16O, 20Ne, 24Mg, 28Si; calculated form factors. Comparison with data. NUCLEAR REACTIONS 16O, 20Ne(p, p), E=0.2, 0.5, 0.8, 1.0 GeV; calculated σ(θ) based on a cluster model with analytical wave function. Comparison with data.
doi: 10.1140/epja/i2009-10824-4
2007YA13 Eur.Phys.J. A 32, 35 (2007) Optical potential analysis of proton elastic scattering from 12C based on the α-particle model NUCLEAR REACTIONS 4He(p, p), E=0.20-1.73 GeV; analyzed σ and analyzing powers to obtained the proton-4He amplitude. NUCLEAR REACTIONS 12C(p, p), E=0.2-1.04 GeV; calculated σ and analyzing powers based on an α-particle model. Deduced an optical potential for intermediate energy.
doi: 10.1140/epja/i2007-10365-x
2004YA03 Nucl.Phys. A732, 3 (2004) A folding model of the α + 12C elastic scattering based on an α-particle model for 12C NUCLEAR REACTIONS 12C(α, α), E=13-172.5 MeV; calculated σ(θ). Folding model, nuclear α-cluster model, comparison with data.
doi: 10.1016/j.nuclphysa.2003.12.005
2002YA15 J.Phys.(London) G28, 2561 (2002) Total reaction cross sections for the 12C + 12C system from a folding model analysis NUCLEAR REACTIONS 12C(12C, 12C), E=70-1016 MeV; calculated σ(θ), total reaction σ. α-folding model, comparison with data.
doi: 10.1088/0954-3899/28/10/303
1993LI13 Phys.Rev. C47, 2393 (1993) Folding Model Using a Bare Elementary Interaction for 12C + 12C Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=70.7-160 MeV; analyzed σ(θ). Folding potential, α-particle model of the nucleus.
doi: 10.1103/PhysRevC.47.2393
1993LI25 Nucl.Phys. A561, 181 (1993) Alpha-Particle Elastic Scattering on 16O in the Four α-Particle Model NUCLEAR REACTIONS 16O(α, α), E=25.4-54.1 MeV; calculated σ(θ). Folding potential.
doi: 10.1016/0375-9474(93)90149-R
1993YA08 Europhys.Lett. 21, 657 (1993) A Description of α + 16O Elastic Scattering Near E/A = 12 and 7 MeV by a Single-Folding Potential NUCLEAR REACTIONS 16O(α, α), E=7, 12 MeV/nucleon; calculated σ(θ). Single folding potential, α-particle model.
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