NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.X.Wei Found 12 matches. 2013LI55 Phys.Rev. C 88, 064307 (2013) J.Li, J.X.Wei, J.N.Hu, P.Ring, J.Meng Relativistic description of magnetic moments in nuclei with doubly closed shells plus or minus one nucleon NUCLEAR MOMENTS 207,209Pb, 207Tl, 209Bi; calculated magnetic moments using relativistic mean field point-coupling model with the density functional PC-PK1. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.064307
1998KE01 Nucl.Phys. A628, 1 (1998) N.Keeley, J.S.Lilley, J.X.Wei, M.Dasgupta, D.J.Hinde, J.R.Leigh, J.C.Mein, C.R.Morton, H.Timmers, N.Rowley Fusion Excitation Function Measurements for the 16O + 58Ni and 16O + 62Ni Systems NUCLEAR REACTIONS 58,62Ni(16O, 16O), (16O, 16O'), (16O, X), E=35-60 MeV; measured elastic, inelastic, transfer reaction differential σ; deduced σ, barrier distributions. Coupled-reaction-channels calculations.
doi: 10.1016/S0375-9474(97)00597-6
1995LE34 Phys.Rev. C52, 3151 (1995) J.R.Leigh, M.Dasgupta, D.J.Hinde, J.C.Mein, C.R.Morton, R.C.Lemmon, J.P.Lestone, J.O.Newton, H.Timmers, J.X.Wei, N.Rowley Barrier Distributions from the Fusion of Oxygen Ions with 144,148,154Sm and 186W NUCLEAR REACTIONS, ICPND 186W, 144,148,154Sm(16O, X), 144Sm(17O, X), E=50-110 MeV; measured fusion σ(E), σ(evaporation residue, θ) vs E; deduced fusion barrier distributions. Enriched targets. Coupled-channels analysis.
doi: 10.1103/PhysRevC.52.3151
1993LE01 Phys.Rev. C47, R437 (1993) J.R.Leigh, N.Rowley, R.C.Lemmon, D.J.Hinde, J.O.Newton, J.X.Wei, J.C.Mein, C.R.Morton, S.Kuyucak, A.T.Kruppa Reconciling Deformation Parameters from Fusion with Those from Coulomb Excitation NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-68 MeV; analyzed fusion data. 154Sm deduced deformation parameters consistency with Coulomb excitation fits.
doi: 10.1103/PhysRevC.47.R437
1993LE11 Nucl.Phys. A559, 277 (1993) J.P.Lestone, J.R.Leigh, J.O.Newton, D.J.Hinde, J.X.Wei, J.X.Chen, S.Elfstrom, M.Zielinska-Pfabe Pre-Scission Charged-Particle Multiplicities following the Reactions 164,167,170Er + 28Si NUCLEAR REACTIONS 164,167,170Er(28Si, F), E=140-185 MeV; measured fission (fragment)p-, (fragement)α-coin, σ(fragment, θ, E(α, p)); deduced pre-, post-fission proton and alpha multiplicities. 192,195,198Pb deduced statistical model level-density parameters, dynamical effects.
doi: 10.1016/0375-9474(93)90192-Z
1993LE17 Phys.Lett. 316B, 32 (1993) R.C.Lemmon, J.R.Leigh, J.X.Wei, C.R.Morton, D.J.Hinde, J.O.Newton, J.C.Mein, M.Dasgupta, N.Rowley Strong Dependence of Sub-Barrier Fusion on the Nuclear Hexadecapole Deformation NUCLEAR REACTIONS, ICPND 186W(16O, X), E=68-90 MeV; measured fusion σ(E). 154Sm(16O, X), E not given; analyzed data; deduced hexadecapole deformation role. 186W deduced deformation parameters.
doi: 10.1016/0370-2693(93)90653-Y
1992RO03 Phys.Rev. C45, 719 (1992) H.Rossner, D.J.Hinde, J.R.Leigh, J.P.Lestone, J.O.Newton, J.X.Wei, S.Elfstrom Influence of Pre-Fission Particle Emission on Fragment Angular Distributions Studied for 208Pb(16O, f) NUCLEAR REACTIONS 208Pb(16O, F), E=80-130 MeV; measured σ(fragment θ, En); deduced pre-, post-scission multiplicities. 224Th deduced fission yield vs decay time, temperature.
doi: 10.1103/PhysRevC.45.719
1991HI08 Phys.Lett. 258B, 35 (1991) D.J.Hinde, J.R.Leigh, J.P.Lestone, J.O.Newton, S.Elfstrom, J.X.Wei, M.Zielinska-Pfabe The Effect of the Angular Momentum Dependence of the Fission Probability on the Determination of Fission Time Scales from Fission Excitation Functions NUCLEAR REACTIONS 197Au(16O, F), 181Ta(19F, F), E not given; calculated fission probability vs excitation energy; deduced angular momentum role in fission time scales determination.
doi: 10.1016/0370-2693(91)91204-9
1991LE21 Phys.Rev.Lett. 67, 1078 (1991) J.P.Lestone, J.R.Leigh, J.O.Newton, D.J.Hinde, J.X.Wei, J.X.Chen, S.Elfstrom, D.G.Popescu Fission Time Scales from Prescisson Charged-Particle Multiplicities NUCLEAR REACTIONS 164,167,170Er(28Si, X), E=140-185 MeV; measured proton, α-spectra, multiplicities; deduced reaction mechanism. 192,195,198Pb deduced fission characteristics.
doi: 10.1103/PhysRevLett.67.1078
1991WE18 Phys.Rev.Lett. 67, 3368 (1991) J.X.Wei, J.R.Leigh, D.J.Hinde, J.O.Newton, R.C.Lemmon, S.Elfstrom, J.X.Chen, N.Rowley Experimental Determination of the Fusion-Barrier Distribution for the 154Sm + 16O Reaction NUCLEAR REACTIONS 154Sm(16O, X), E=54-110 MeV; measured σ(evaporation residue θ); deduced fusion σ(E), barrier distributions.
doi: 10.1103/PhysRevLett.67.3368
1991WE19 Nucl.Instrum.Methods Phys.Res. A306, 557 (1991) J.X.Wei, J.R.Leigh, D.C.Weisser, J.O.Newton, S.Elfstrom, J.P.Lestone, J.X.Chen, D.G.Popescu, D.J.Hinde A Compact Velocity Filter for Evaporation Residue Measurements NUCLEAR REACTIONS 130Te(28Si, X), E=100-160 MeV; 170Er(16O, X), E=110 MeV; 176Yb(16O, X), E=100 MeV; 186W(16O, X), E=70 MeV; 154Sm(16O, X), E=60 MeV; measured σ(evaporation residue θ). Velocity filter.
doi: 10.1016/0168-9002(91)90052-R
1990LE07 Nucl.Phys. A509, 178 (1990) J.P.Lestone, J.R.Leigh, J.O.Newton, J.X.Wei Fission Fragment Angular Distributions following Transfer Reactions for 232Th + 16O NUCLEAR REACTIONS 232Th(16O, F), E=80-92 MeV; measured fission fragment σ(E, θ), (fragment)(particle)-coin, σ(fragment φ, θ) following transfer, X=C, N.
doi: 10.1016/0375-9474(90)90380-5
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