NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = L.Yao Found 14 matches. 2022MO03 Nucl.Instrum.Methods Phys.Res. A1021, 165864 (2022) M.Monterial, K.T.Schmitt, C.Prokop, E.Leal-Cidoncha, M.Anastasiou, N.S.Bowden, J.Bundgaard, R.J.Casperson, D.A.Cebra, T.Classen, D.H.Dongwi, N.Fotiades, J.Gearhart, V.Geppert-Kleinrath, U.Greife, C.Hagmann, M.Heffner, D.Hensle, D.Higgins, L.D.Isenhower, K.Kazkaz, A.Kemnitz, J.King, J.L.Klay, J.Latta, W.Loveland, J.A.Magee, B.Manning, M.P.Mendenhall, S.Mosby, D.Neudecker, S.Sangiorgio, B.Seilhan, L.Snyder, F.Tovesson, R.S.Towell, N.Walsh, T.S.Watson, L.Yao, W.Younes Measurement of material isotopics and atom number ratio with α-particle spectroscopy for a NIFFTE fission Time Projection Chamber actinide target NUCLEAR REACTIONS 235U, 239Pu(n, F), E not given; measured fission products, Eα, Iα; deduced isotopic concentrations and atomic number ratio.
doi: 10.1016/j.nima.2021.165864
2020CH50 Eur.Phys.J. A 56, 297 (2020) A.Chemey, A.Pica, L.Yao, W.Loveland, H.Y.Lee, S.A.Kuvin Total kinetic energy and mass yields from the fast neutron-induced fission of 239Pu NUCLEAR REACTIONS 239Pu(n, F), E=2.4-100 MeV; measured reaction products; deduced fission fragment mass distributions, mass yields, total kinetic energy (TKE) release in fission. Comparison with available data. The Los Alamos National Lab (LANL) WNR facility, on Flight Path 15R (FP15R).
doi: 10.1140/epja/s10050-020-00295-6
2020PI16 Phys.Rev. C 102, 064612 (2020) A.Pica, A.T.Chemey, L.Yao, W.Loveland, H.Y.Lee, S.A.Kuvin Total kinetic energy release in the fast-neutron-induced fission of 237Np NUCLEAR REACTIONS 237Np(n, F), E=2.6-100 MeV; measured fission fragments, time of flight of each interacting neutron using two arrays of nine Si PIN photodiodes at the LANSCE-WNR facility; deduced mass yield distributions, post- and pre-neutron emission total kinetic energy (TKEs), σ(E), product mass TKE distributions as function of neutron energy, dependence of asymmetric TKE events on neutron energy. Comparison with predictions of GEF (GEneral description of Fission observables) model.
doi: 10.1103/PhysRevC.102.064612
2018LO19 Eur.Phys.J. A 54, 140 (2018) W.Loveland, A.M.Vinodkumar, R.Yanez, L.Yao, J.King, J.Lassen, A.Rojas Sub-barrier fusion of 11Li with 208Pb NUCLEAR REACTIONS 208Pb(11Li, x), E=26.1-32.7[sub-barrier]; measured reaction products isotopes; deduced complete, incomplete, total fusion σ, added published σ of the same group at different energies; calculated nuclidic σ using HIVAP statistical model code.
doi: 10.1140/epja/i2018-12572-8
2018YA03 Phys.Rev. C 97, 014608 (2018) Survival-mediated capture and fusion cross sections for heavy-element synthesis NUCLEAR REACTIONS 249Cf(p, 3n)250Es*, E=23 MeV; 233U(3He, 5n)236Pu*, E=44.7 MeV; 249Cf(11B, 3n)260Lr*, E=63 MeV; 204Pb(12C, 5n)216Rn*, E=78 MeV; 232Th(12C, 4n)244Cm*, E=74 MeV; 232Th(12C, 5n)244Cm*, E=74 MeV; 233U(12C, 3n)245Cf*, E=67 MeV; 234U(12C, 4n)246Cf*, E=72 MeV; 235U(12C, 3n)247Cf*, E=67.5 MeV; 235U(12C, 4n)247Cf*, E=70.5 MeV; 235U(12C, 5n)247Cf*, E=77.5 MeV; 236U(12C, 3n)248Cf*, E=67.5 MeV; 236U(12C, 4n)248Cf*, E=70 MeV; 236U(12C, 5n)248Cf*, E=77.5 MeV; 238U(12C, 4n)250Cf*, E=67.5 MeV; 238U(12C, 5n)250Cf*, E=73.5 MeV; 237Np(12C, 4n)249Es*, E=67.6 MeV; 237Np(12C, 5n)249Es*, E=81 MeV; 239Pu(12C, 4n)251Fm*, E=74 MeV; 239Pu(12C, 5n)251Fm*, E=78 MeV; 241Pu(13C, 4n)254Fm*, E=67.3 MeV; 240Pu(12C, 4n)252Fm*, E=71 MeV; 242Pu(12C, 4n)254Fm*, E=64 MeV; 241Am(12C, 4n)253Md*, E=72 MeV; 241Am(12C, 5n)253Md*, E=81 MeV; 243Am(12C, 4n)255Md*, E=71 MeV; 243Am(12C, 5n)255Md*, E=81 MeV; 243Am(13C, 3n)256Md*, E=70 MeV; 243Am(13C, 4n)256Md*, E=70 MeV; 243Am(13C, 5n)256Md*, E=81 MeV; 244Cm(12C, 4n)256No*, E=73.3 MeV; 244Cm(12C, 5n)256No*, E=83 MeV; 244Cm(13C, 3n)257No*, E=69.8 MeV; 244Cm(13C, 4n)257No*, E=72.8 MeV; 244Cm(13C, 5n)257No*, E=82 MeV; 246Cm(12C, 4n)258No*, E=72 MeV; 246Cm(12C, 5n)258No*, E=83 MeV; 246Cm(13C, 3n)259No*, E=67.5 MeV; 246Cm(13C, 4n)259No*, E=69.5 MeV; 246Cm(13C, 5n)259No*, E=78.5 MeV; 248Cm(12C, 3n)260No*, E=69.2 MeV; 248Cm(12C, 4n)260No*, E=71.2 MeV; 248Cm(12C, 5n)260No*, E=77.8 MeV; 248Cm(13C, 4n)261No*, E=70.5 MeV; 248Cm(13C, 5n)261No*, E=74.8 MeV; 249Cf(12C, 4n)261Rf*, E=71 MeV; 249Cf(12C, 5n)261Rf*, E=85 MeV; 249Cf(13C, 4n)262Rf*, E=72 MeV; 235U(15N, 4n)250Es*, E=78 MeV; 238U(14N, 5n)252Es*, E=83 MeV; 208Pb(16O, 4n)224Th*, E=91 MeV; 209Bi(18O, 3n)227Pa*, E=92.6 MeV; 241Am(15N, 4n)256No*, E=82.9 MeV; 243Am(15N, 4n)258No*, E=83 MeV; 248Cm(15N, 3n)263Lr*, E=78 MeV; 248Cm(15N, 4n)263Lr*, E=81 MeV; 248Cm(15N, 5n)263Lr*, E=88 MeV; 58Ni(50Cr, 3n)108Te*, E=214 MeV; 249Bk(15N, 4n)264Rf*, E=81.6 MeV; 249Cf(15N, 4n)264Db*, E=86 MeV; 250Cf(15N, 4n)265Rf*, E=84 MeV; 233U(16O, 4n)249Fm*, E=93 MeV; 233U(16O, 5n)249Fm*, E=97 MeV; 238U(16O, 4n)254Fm*, E=91 MeV; 238U(16O, 5n)254Fm*, E=91 MeV; 238U(18O, 3n)256Fm*, E=88 MeV; 238U(18O, 4n)256Fm*, E=88 MeV; 238U(18O, 5n)256Fm*, E=94 MeV; 239Pu(18O, 4n)257No*, E=91 MeV; 239Pu(18O, 4n)257Fm*, E=91 MeV; 239Pu(18O, 5n)257Fm*, E=96 MeV; 242Pu(16O, 4n)258Fm*, E=89 MeV; 245Cm(18O, 4n)263Rf*, E=93 MeV; 246Cm(16O, 4n)262Rf*, E=95 MeV; 248Cm(16O, 4n)264Rf*, E=92 MeV; 248Cm(18O, 4n)266Rf*, E=89 MeV; 248Cm(18O, 4n)266Rf*, E=94 MeV; 249Bk(16O, 4n)265Db*, E=92 MeV; 249Bk(16O, 5n)265Db*, E=92 MeV; 249Bk(18O, 4n)267Db*, E=91 MeV; 249Bk(18O, 5n)267Db*, E=91 MeV; 249Cf(18O, 4n)267Sg*, E=95 MeV; 205Tl(22Ne, 3n)227Pa*, E=97 MeV; 238U(19F, 4n)257Md*, E=96 MeV; 238U(19F, 5n)257Md*, E=103 MeV; 209Bi(22Ne, 4n)231Np*, E=121 MeV; 209Bi(22Ne, 5n)231Np*, E=121 MeV; 248Cm(19F, 4n)267Db*, E=98 MeV; 248Cm(19F, 5n)267Db*, E=106 MeV; 232Th(22Ne, 4n)254Fm*, E=106 MeV; 236U(22Ne, 4n)258No*, E=112 MeV; 236U(22Ne, 5n)258No*, E=124 MeV; 238U(22Ne, 5n)260No*, E=117 MeV; 242Pu(22Ne, 4n)264Rf*, E=114 MeV; 242Pu(22Ne, 5n)264Rf*, E=114 MeV; 244Pu(22Ne, 5n)266Rf*, E=114 MeV; 241Am(22Ne, 4n)263Db*, E=118 MeV; 241Am(22Ne, 5n)263Db*, E=118 MeV; 243Am(22Ne, 4n)265Db*, E=116 MeV; 248Cm(22Ne, 5n)270Sg*, E=117.8 MeV; 249Bk(22Ne, 4n)271Bh*, E=120 MeV; 249Bk(22Ne, 5n)271Bh*, E=120 MeV; 208Pb(24Mg, 3n)232Pu*, E=132 MeV; 208Pb(24Mg, 4n)232Pu*, E=132 MeV; 208Pb(26Mg, 4n)234Pu*, E=135 MeV; 248Cm(23Na, 5n)271Bh*, E=132 MeV; 232Th(26Mg, 4n)258No*, E=136 MeV; 232Th(26Mg, 5n)258No*, E=136 MeV; 238U(26Mg, 3n)264Rf*, E=121.8 MeV; 238U(26Mg, 4n)264Rf*, E=128.1, 134 MeV; 238U(26Mg, 5n)264Rf*, E=138.5, 140 MeV; 243Am(26Mg, 4n)269Bh*, E=168 MeV; 243Am(26Mg, 5n)269Bh*, E=168 MeV; 248Cm(25Mg, 4n)273Hs*, E=140 MeV; 248Cm(25Mg, 5n)273Hs*, E=140 MeV; 248Cm(26Mg, 3n)274Hs*, E=145 MeV; 248Cm(26Mg, 4n)274Hs*, E=145 MeV; 248Cm(26Mg, 5n)274Hs*, E=145 MeV; 182W(32S, 3n)214Th*, E=195 MeV; 182W(32S, 4n)214Th*, E=195 MeV; 236U(27Al, 5n)263Db*, E=154 MeV; 181Ta(35Cl, 5n)216Th*, E=190.5 MeV; 198Pt(34S, 4n)232Pu*, E=171 MeV; 238U(30Si, 3n)268Sg*, E=151 MeV; 238U(30Si, 4n)268Sg*, E=151 MeV; 238U(30Si, 5n)268Sg*, E=161 MeV; 176Hf(40Ar, 3n)216Th*, E=172.5 MeV; 178Hf(40Ar, 3n)218Th*, E=167.6 MeV; 178Hf(40Ar, 4n)218Th*, E=178.6 MeV; 180Hf(40Ar, 3n)220Th*, E=167 MeV; 180Hf(40Ar, 4n)220Th*, E=177 MeV; 180Hf(40Ar, 3n)220Th*, E=187.5 MeV; 207Pb(34S, 3n)241Cf*, E=172 MeV; 204Pb(36S, 2n)240Cf*, E=163.6 MeV; 204Pb(36S, 3n)240Cf*, E=172.6 MeV; 206Pb(36S, 2n)242Cf*, E=163.6 MeV; 206Pb(36S, 3n)242Cf*, E=162.6 MeV; 207Pb(36S, 2n)243Cf*, E=165.5 MeV; 207Pb(36S, 3n)243Cf*, E=170.3 MeV; 181Ta(40Ar, 3n)221Pa*, E=177 MeV; 181Ta(40Ar, 4n)221Pa*, E=179.4 MeV; 182W(40Ar, 3n)222U*, E=194 MeV; 182W(40Ar, 4n)222U*, E=194 MeV; 144Sm(46Ti, 3n)190Po*, E=222 MeV; 172Yb(48Ca, 3n)220Th*, E=196.3 MeV; 172Yb(48Ca, 4n)220Th*, E=210.2 MeV; 172Yb(48Ca, 5n)220Th*, E=225.1 MeV; 173Yb(48Ca, 4n)221Th*, E=210.2 MeV; 173Yb(48Ca, 5n)221Th*, E=210.2 MeV; 176Yb(48Ca, 4n)224Th*, E=208.4 MeV; 209Bi(37Cl, 2n)246Fm*, E=220 MeV; 144Sm(51V, 3n)195At*, E=230 MeV; 180Hf(48Ca, 3n)228U*, E=203.5 MeV; 142Nd(50Cr, 3n)192Po*, E=231.4 MeV; 142Nd(50Cr, 4n)192Po*, E=245 MeV; 142Nd(52Cr, 2n)194Po*, E=221.8 MeV; 142Nd(52Cr, 3n)194Po*, E=235.5 MeV; 142Nd(52Cr, 4n)194Po*, E=250.5 MeV; 142Nd(52Cr, 5n)194Po*, E=271 MeV; 238U(34S, 4n)272Hs*, E=176 MeV; 238U(34S, 5n)272Hs*, E=187.4 MeV; 238U(36S, 3n)274Hs*, E=170 MeV; 238U(36S, 4n)274Hs*, E=177 MeV; 238U(36S, 5n)274Hs*, E=188 MeV; 238U(34S, 5n)272Hs*, E=186 MeV; 206Pb(40Ar, 4n)246Fm*, E=236 MeV; 207Pb(40Ar, n)247Fm*, E=220 MeV; 208Pb(40Ar, 2n)248Fm*, E=236 MeV; 208Pb(40Ar, 3n)248Fm*, E=191 MeV; 184W(48Ca, 3n)232Pu*, E=201.6 MeV; 209Bi(40Ar, 2n)249Md*, E=187 MeV; 209Bi(40Ar, 3n)249Md*, E=198 MeV; 170Er(51V, 3n)221Pa*, E=220 MeV; 170Er(51V, 4n)221Pa*, E=234.7 MeV; 204Hg(48Ca, 2n)252Fm*, E=207 MeV; 90Zr(90Zr, γ)180Hg, E=362 MeV; 90Zr(90Zr, n)180Hg*, E=362 MeV; 90Zr(90Zr, 2n)180Hg*, E=362 MeV; 205Tl(48Ca, 2n)253Md*, E=209 MeV; 208Pb(48Ca, n)256No*, E=209 MeV; 208Pb(48Ca, 2n)256No*, E=214 MeV; 208Pb(48Ca, 3n)256No*, E=225 MeV; 208Pb(48Ca, 4n)256No*, E=237 MeV; 206Pb(48Ca, n)254No*, E=209 MeV; 206Pb(48Ca, 2n)254No*, E=215 MeV; 206Pb(48Ca, 3n)254No*, E=226 MeV; 206Pb(48Ca, 4n)254No*, E=238 MeV; 204Pb(48Ca, 2n)252No*, E=216.7 MeV; 204Pb(48Ca, 2n)252No*, E=220 MeV; 204Pb(48Ca, 3n)252No*, E=227 MeV; 208Pb(44Ca, 2n)252No*, E=214 MeV; 208Pb(44Ca, 3n)252No*, E=225 MeV; 207Pb(48Ca, 2n)255No*, E=215 MeV; 106Pd(83Kr, 3n)189Pb*, E=357 MeV; 209Bi(48Ca, n)257Lr*, E=212.2 MeV; 209Bi(48Ca, 2n)257Lr*, E=219.4 MeV; 209Bi(48Ca, 3n)257Lr*, E=230.2 MeV; 209Bi(48Ca, 4n)257Lr*, E=240 MeV; 198Pt(50Ti, 2n)257Lr*, E=219.5 MeV; 198Pt(50Ti, 3n)257Lr*, E=232 MeV; 93Nb(94Mo, 2n)187Bi*, E=403 MeV; 93Nb(94Mo, 3n)187Bi*, E=428.8 MeV; 93Nb(95Mo, n)188Bi*, E=379.5 MeV; 93Nb(95Mo, 2n)188Bi*, E=403.7 MeV; 93Nb(95Mo, 3n)188Bi*, E=424 MeV; 114Cd(83Kr, 3n)197Po*, E=375 MeV; 154Sm(60Ni, 3n)214Th*, E=278 MeV; 154Sm(60Ni, 4n)214Th*, E=278 MeV; 226Ra(48Ca, 3n)274Hs*, E=229 MeV; 226Ra(48Ca, 4n)274Hs*, E=234 MeV; 226Ra(48Ca, 5n)274Hs*, E=241 MeV; 94Mo(100Mo, n)194Po*, E=385 MeV; 94Mo(100Mo, 2n)194Po*, E=403.7 MeV; 94Mo(100Mo, 3n)194Po*, E=424.3 MeV; 100Mo(100Mo, n)200Po*, E=372 MeV; 100Mo(100Mo, 2n)200Po*, E=384 MeV; 100Mo(100Mo, 3n)200Po*, E=400 MeV; 100Mo(100Mo, 4n)200Po*, E=420 MeV; 100Mo(100Mo, 5n)200Po*, E=436 MeV; 232Th(48Ca, 3n)280Ds*, E=260 MeV; 208Pb(48Ti, n)256Rf*, E=223.3 MeV; 208Pb(48Ti, 2n)256Rf*, E=232 MeV; 208Pb(49Ti, 2n)257Rf*, E=271 MeV; 208Pb(50Ti, n)258Rf*, E=229 MeV; 208Pb(50Ti, n)258Rf*, E=230.5 MeV; 208Pb(50Ti, 2n)258Rf*, E=239, 243 MeV; 208Pb(50Ti, 3n)258Rf*, E=247.6 MeV; 207Pb(50Ti, n)257Rf*, E=242.5 MeV; 207Pb(50Ti, 2n)257Rf*, E=242.5 MeV; 206Pb(50Ti, n)256Rf*, E=237.3 MeV; 206Pb(50Ti, 2n)256Rf*, E=237.3 MeV; 209Bi(50Ti, n)259Db*, E=232.6 MeV; 209Bi(50Ti, 2n)259Db*, E=240.7 MeV; 209Bi(50Ti, 3n)259Db*, E=254 MeV; 121Sb(86Kr, 2n)207Fr*, E=343.6 MeV; 121Sb(86Kr, 3n)207Fr*, E=361.1 MeV; 121Sb(86Kr, 4n)207Fr*, E=388.7 MeV; 123Sb(86Kr, 4n)209Fr*, E=379.1 MeV; 123Sb(86Kr, 5n)209Fr*, E=388.7 MeV; 208Pb(51V, n)259Db*, E=239.7 MeV; 208Pb(51V, 2n)259Db*, E=247.2 MeV; 209Bi(51V, 2n)260Sg*, E=250.4 MeV; 208Pb(52Cr, n)260Sg*, E=254 MeV; 208Pb(52Cr, 2n)260Sg*, E=262 MeV; 207Pb(54Cr, n)261Sg*, E=262 MeV; 207Pb(54Cr, 2n)261Sg*, E=262 MeV; 208Pb(54Cr, n)262Sg*, E=257.1 MeV; 208Pb(54Cr, 2n)262Sg*, E=268.5 MeV; 208Pb(54Cr, 3n)262Sg*, E=297 MeV; 209Bi(52Cr, n)261Bh*, E=252.8 MeV; 209Bi(54Cr, n)263Bh*, E=257.1 MeV; 209Bi(54Cr, 2n)263Bh*, E=260.9 MeV; 90Zr(124Sn, n)214Th*, E=503.4 MeV; 92Zr(124Sn, n)216Th*, E=492.3 MeV; 94Zr(124Sn, n)218Th*, E=493.5 MeV; 94Zr(124Sn, 2n)218Th*, E=506.4 MeV; 94Zr(124Sn, 3n)218Th*, E=518.8 MeV; 94Zr(124Sn, 4n)218Th*, E=545 MeV; 96Zr(124Sn, n)220Th*, E=494.6 MeV; 96Zr(124Sn, 2n)220Th*, E=494.6 MeV; 96Zr(124Sn, 3n)220Th*, E=519.2 MeV; 96Zr(124Sn, 4n)220Th*, E=531.7 MeV; 96Zr(124Sn, 5n)220Th*, E=567.7 MeV; 208Pb(55Mn, n)263Bh*, E=265.5 MeV; 208Pb(55Mn, 2n)263Bh*, E=273 MeV; 209Bi(55Mn, n)264Hs*, E=302.5 MeV; 208Pb(56Fe, n)264Hs*, E=275 MeV; 208Pb(58Fe, n)266Hs*, E=283.9 MeV; 208Pb(58Fe, 2n)266Hs*, E=291.2, 294.1 MeV; 207Pb(58Fe, n)265Hs*, E=285 MeV; 206Pb(58Fe, n)264Hs*, E=287.7 MeV; 209Bi(58Fe, n)267Mt*, E=287.6 MeV; 170Er(76Ge, 2n)246Fm*, E=357.5 MeV; 208Pb(59Co, n)267Mt*, E=291.5 MeV; 209Bi(59Co, n)268Ds*, E=300.9 MeV; 208Pb(62Ni, n)270Ds*, E=311 MeV; 208Pb(64Ni, n)272Ds*, E=314 MeV; 207Pb(64Fe, n)271Ds*, E=317 MeV; 160Gd(86Kr, 2n)246Fm*, E=380.5 MeV; 110Pd(136Xe, 2n)246Fm*, E=633.5 MeV; calculated capture cross section and evaporation residue formation cross section as function of spin, fusion probability PCN, survival probability, mean spins for the capture process and for the calculated evaporation residues (EVR); compiled experimental cross sections for evaporation residues. Comparison with available experimental data. List of reactions, experimental σ(EVR) and theoretical results in a table in Supplementary Material (ref. 17 in 2018Ya03). Relevance to heavy element formation.
doi: 10.1103/PhysRevC.97.014608
2014LO09 Nucl.Data Sheets 119, 383 (2014) W.Loveland, L.Yao, D.M.Asner, R.G.Baker, J.Bundgaard, E.Burgett, M.Cunningham, J.Deaven, D.L.Duke, U.Greife, S.Grimes, M.Heffner, T.Hill, D.Isenhower, J.L.Klay, V.Kleinrath, N.Kornilov, A.B.Laptev, T.N.Massey, R.Meharchand, H.Qu, J.Ruz, S.Sangiorgio, B.Selhan, L.Snyder, S.Stave, G.Tatishvili, R.T.Thornton, F.Tovesson, D.Towell, R.S.Towell, S.Watson, B.Wendt, L.Wood Targets for Precision Measurements
doi: 10.1016/j.nds.2014.08.106
2014YA07 Phys.Rev.Lett. 112, 152702 (2014) R.Yanez, W.Loveland, L.Yao, J.S.Barrett, S.Zhu, B.B.Back, T.L.Khoo, M.Alcorta, M.Albers Measurement of the Survival Probabilities for Hot Fusion Reactions RADIOACTIVITY 274Hs(n) [from 248Cm(25Mg, X), E=144.2 MeV; 248Cm(26Mg, X), E=160.7 MeV]; measured decay products, En, In; deduced neutron multiplicities, elastic and fission resonance widths, survival probability of excited superheavy nuclei.
doi: 10.1103/PhysRevLett.112.152702
2014YA10 Phys.Rev. C 89, 051604 (2014) R.Yanez, L.Yao, J.King, W.Loveland, F.Tovesson, N.Fotiades Excitation energy dependence of the total kinetic energy release in 235U(n, f) NUCLEAR REACTIONS 235U(n, F), E=3.2-50 MeV; measured (fission fragment)(fission fragment)-coin, time-of-flight, total kinetic energy (ETKE) release as function of incident neutron energy at WNR-LANSCE-LANL facility; deduced dependence of ETKE and total excitation energy (ETXE) on E(n). Comparison with GEF model predictions, and with previous experimental results.
doi: 10.1103/PhysRevC.89.051604
2013VI01 Phys.Rev. C 87, 044603 (2013) A.M.Vinodkumar, W.Loveland, R.Yanez, M.Leonard, L.Yao, P.Bricault, M.Dombsky, P.Kunz, J.Lassen, A.C.Morton, D.Ottewell, D.Preddy, M.Trinczek Interaction of 11Li with 208Pb NUCLEAR REACTIONS 208Pb(11Li, X)212At/213At/214At/215At/216At, E=39.9, 36.5, 32.7, 28.6 MeV; measured Eα, Iα from evaporation residues, production σ(E), complete and incomplete fusion σ(E), breakup σ(E) at TRIUMF-ISAC2 facility. 209Bi(7Li, X)212Rn/213Rn, E=34.90 MeV; measured complete fusion σ, and compared to earlier experimental results. Comparison with theoretical predictions, and with results from experimental results of other reaction.
doi: 10.1103/PhysRevC.87.044603
2013YA12 Phys.Rev. C 88, 014606 (2013) R.Yanez, W.Loveland, J.S.Barrett, L.Yao, B.B.Back, S.Zhu, T.L.Khoo Measurement of the fusion probability, PCN, for hot fusion reactions NUCLEAR REACTIONS 197Au(18O, F), E=101.2 MeV; 197Au(26Mg, F), E=147.3 MeV; 197Au(30Si, F), E=170.9 MeV; 197Au(36S, F), E=195.3 MeV; measured particle spectra, time-of-flight, fission fragment angular distributions at ATLAS-ANL facility; deduced fusion-fission and quasifission cross sections using formalism of Back, fusion probabilities PCN. Comparison with previous measurements, and with systematic dependence of PCN on fissility. Compiled experimental PCN values for several reactions.
doi: 10.1103/PhysRevC.88.014606
1998CA26 Phys.Rev. C58, 808 (1998) J.A.Cameron, J.L.Rodriguez, J.Jonkman, G.Hackman, S.M.Mullins, C.E.Svensson, J.C.Waddington, L.Yao, T.E.Drake, M.Cromaz, J.H.DeGraaf, G.Zwartz, H.R.Andrews, G.Ball, A.Galindo-Uribarri, V.P.Janzen, D.C.Radford, D.Ward Spectroscopy of Cross-Conjugate Nuclei 46Ti - 50Cr and 47V - 49Cr Near the f7/2-Shell Band Termination NUCLEAR REACTIONS 28Si(28Si, 2p2α), (28Si, p2α), (28Si, 2pα), (28Si, n2pα), E=125 MeV; measured Eγ, Iγ, γγ-coin, DSA. 49,50Cr, 47V, 46Ti deduced high-spin levels, J, π, T1/2, B(M1), B(E2).
doi: 10.1103/PhysRevC.58.808
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
1996WA25 Nucl.Phys. A608, 77 (1996) X.-H.Wang, C.-H.Yu, D.M.Cullen, D.C.Bryan, M.Devlin, M.J.Fitch, A.Galindo-Uribarri, R.W.Gray, D.M.Herrick, R.W.Ibbotson, K.L.Kurz, S.Mullins, S.Pilotte, D.C.Radford, M.R.Satteson, M.W.Simon, D.Ward, C.Y.Wu, L.H.Yao High-Spin States in Odd-Odd 164Lu NUCLEAR REACTIONS 149Sm(19F, 4n), E=85 MeV; 146Nd(23Na, 5n), E=110 MeV; measured Eγ, Iγ, γγ-coin. 164Lu deduced high-spin levels, J, π, γ-branching, B(M1)/B(E2) ratios, band crossings, signature inversion, neutron-proton interactions.
doi: 10.1016/S0375-9474(96)00254-0
1994MU16 Phys.Rev. C50, R2261 (1994) S.M.Mullins, N.C.Schmeing, S.Flibotte, G.Hackman, J.L.Rodriguez, J.C.Waddington, L.Yao, H.R.Andrews, A.Galindo-Uribarri, V.P.Janzen, D.C.Radford, D.Ward, J.DeGraaf, T.E.Drake, S.Pilotte, E.S.Paul Proton Configurations and Pairing Correlations at the N = 80 Superdeformed Shell Closure: Study of 145Tb NUCLEAR REACTIONS 112Sn(37Cl, 2n2p), E=187 MeV; 118Sn(31P, 4n), E=160 MeV; measured γγ(charged particle)-.γγ-coin, Eγ, Iγ. 145Tb deduced superdeformed rotational band, high-spin levels, J, π. Cranked Woods-Saxon-Strutinsky calculations. Hyperpure Ge detectors, BGO suppression shields, BGO total energy, multiplicity filter, CsI detectors coupled to photodiodes, enriched targets.
doi: 10.1103/PhysRevC.50.R2261
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