NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Y.Qiao Found 12 matches. 2024HA04 Appl.Radiat.Isot. 205, 111177 (2024) Y.Han, Y.Qiao, Zh.Li, X.Han, Q.Wang, K.Fang, Sh.Zhang Fission cross-section measurements for the 238U(n, f)97m+gNb, 238U(n, f)133gTe and 238U(n, f)130gSb reactions induced by D-T neutrons NUCLEAR REACTIONS 238U(n, F)97Nb/133Te/130Sb, E ∼ 14 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The K-400 D-T neutron generator of the China Academy of Engineering Physics.
doi: 10.1016/j.apradiso.2024.111177
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
2014QI01 Nucl.Instrum.Methods Phys.Res. A739, 44 (2014) Y.Qiao, M.Zhang, Y.Yang, S.Liu, J.Wu, B.Wang Determination of 235U isotopic abundance by fission-yield difference method NUCLEAR REACTIONS 235U(n, X)135I/88Rb/104Tc/107Rh/92Sr, E not given; measured reaction products, Eα, Iα, Eγ, Iγ; deduced fission yields and ratios of yields, isotopic abundance of 235U in the samples.
doi: 10.1016/j.nima.2013.11.035
2012QI02 Nucl.Instrum.Methods Phys.Res. A665, 70 (2012) Y.Qiao, J.Wu, Y.Yang, M.Zhang, S.Liu Determination of 235U isotope abundance by measuring selected pairs of fission products NUCLEAR REACTIONS U(n, F)92Sr/105Ru/135I, E=14 MeV; measured fission fragments, Eγ, Iγ. 235U; deduced isotopic abundance.
doi: 10.1016/j.nima.2011.10.020
1998HA71 High Energy Phys. and Nucl.Phys. (China) 22, 193 (1998) H.Han, S.Huang, G.Shen, Y.Qiao, G.Sun Anomalies of neutron and γ-ray emission in ternary fission of 252Cf
1997HA09 Nucl.Phys. A615, 162 (1997) H.Han, S.Huang, G.Shen, Y.Qiao, G.Sun Anomalies of Neutron and γ-Ray Emission in Light Charged Particle Accompanied Fission of 252Cf RADIOACTIVITY 252Cf(SF); measured γ(light charged particle)-, n(light charged particle)-coin; deduced n-, γ-emission related anomalies explanation. CsI(Tl) crystal, liquid scintillator, NaI(Tl) detector, particle pulse shape separation.
doi: 10.1016/S0375-9474(96)00470-8
1996LI14 Phys.Rev. C54, 761 (1996) Z.Liu, H.Zhang, J.Xu, Y.Qiao, X.Qian, C.Lin Fission Before K Equilibration NUCLEAR REACTIONS, ICPND 238U(11B, F), E(cm)=46.53-56.23 MeV; 237Np(11B, F), E=49.88-68.81 MeV; 232Th(16O, F), E=72.61-80.11 MeV; 232Th(19F, F), E=78-96.8 MeV; 237Np(12C, F), E=56.9-76.01 MeV; 238U(16O, F), E=76.49-84.09 MeV; measured fission σ(E), σ(fragment θ). Pre-equilibrium fission model analysis.
doi: 10.1103/PhysRevC.54.761
1995LI43 Phys.Lett. 353B, 173 (1995) Z.Liu, H.Zhang, J.Xu, Y.Qiao, X.Qian, C.Lin Preequilibrium Fission for Low Angular Momentum NUCLEAR REACTIONS 237Np(11B, F), 232Th(16O, F), E not given; analyzed fission fragment anisotropy data; deduced entrance channel dependence. New preequilibrium fission model.
doi: 10.1016/0370-2693(95)00461-S
1994LI27 Phys.Rev. C50, 1717 (1994) Z.Liu, H.Zhang, J.Xu, X.Quin, Y.Qiao, C.Lin, K.Xu Signature of Non-Compound-Nucleus Fission at Sub-Barrier Energies NUCLEAR REACTIONS 232Th(16O, F), (19F, F), 238U(16O, F), E ≈ barrier; analyzed fission fragment σ(θ) data; deduced noncompound nucleus fission signature.
doi: 10.1103/PhysRevC.50.1717
1994LI41 Chin.J.Nucl.Phys. 16, No 2, 108 (1994) Z.Liu, H.Zhang, J.Xu, X.Qian, Y.Qiao, C.Lin, K.Xu Probing the Non-Equilibration Component of Tilting Spin Mode NUCLEAR REACTIONS 232Th(16O, X), (19F, X), 238U(16O, X), E not given; measured σ(fragment θ); deduced nonequilibration component (of tilting spin) probabilities.
1994LI65 Chin.J.Nucl.Phys. 16, No 4, 323 (1994) Z.-H.Liu, H.-Q.Zhang, J.-C.Xu, X.Qian, Y.Qiao, C.-J.Lin, K.Xu Interplay between Scission-Point Model and Experimental Data for Sub-Barrier Fusion-Fission NUCLEAR REACTIONS 232Th(19F, F), (16O, F), 238U(16O, F), E ≈ sub-barrier; measured fission fragment σ(θ); deduced thermal equilibrium features at scission. Scission point model.
1994ZH04 Phys.Rev. C49, 926 (1994) H.Zhang, Z.Liu, J.Xu, X.Qian, Y.Qiao, C.Lin, K.Xu Anomalous Anisotropy of Fission Fragments in Near- and Sub-Barrier Complete Fusion-Fission Reactions of 16O + 232Th, 19F + 232Th, and 16O + 238U NUCLEAR REACTIONS, ICPND 232Th(16O, F), E=72.61-80.11 MeV; 232Th(19F, F), E=78-96.8 MeV; 238U(16O, F), E=76.49-84.09 MeV; measured fission σ(E), fragment anistropy. Coupled-channels model.
doi: 10.1103/PhysRevC.49.926
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