NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = B.Wang Found 94 matches. 2024AT01 Nature(London) 626, 975 (2024) H.Atek, I.Labbe, L.J.Furtak, I.Chemerynska, S.Fujimoto, D.J.Setton, T.B.Miller, P.Oesch, R.Bezanson, S.H.Price, P.Dayal, A.Zitrin, V.Kokorev, J.R.Weaver, G.Brammer, P.v.Dokkum, Ch.C.Williams, S.E.Cutler, R.Feldmann, Y.Fudamoto, J.E.Greene, J.Leja, M.V.Maseda, A.Muzzin, R.Pan, C.Papovich, E.J.Nelson, Th.Nanayakkara, D.P.Stark, M.Stefanon, K.A.Suess, B.Wang, K.E.Whitaker Most of the photons that reionized the Universe came from dwarf galaxies
doi: 10.1038/s41586-024-07043-6
2024GU05 Eur.Phys.J. A 60, 36 (2024) D.Guo, X.He, P.Li, Zh.Qin, Ch.Hu, B.Wang, Y.Zhou, K.Zheng, Y.Zhang, X.Wei, H.Yang, D.Hu, M.Shao, L.Duan, Y.Yu, Zh.Sun, Y.Wang, Q.Li, Zh.Xiao Studies of nuclear equation of state with the HIRFL-CSR external-target experiment
doi: 10.1140/epja/s10050-024-01245-2
2024PE06 Nucl.Instrum.Methods Phys.Res. A1060, 169039 (2024) X.G.Peng, F.Y.Liu, L.Wang, P.Zhang, P.Kuang, X.Z.Cao, R.S.Yu, B.Y.Wang Triple-coincidence positron annihilation lifetime spectrometer based on ultrafast discrimination
doi: 10.1016/j.nima.2023.169039
2024WA02 Phys.Rev. C 109, 014611 (2024) Systematic study of the radiative proton capture including the compound, pre-equilibrium, and direct mechanisms
doi: 10.1103/PhysRevC.109.014611
2024WA15 Phys.Lett. B 850, 138515 (2024) First-forbidden transition of nuclear β decay by projected shell model RADIOACTIVITY 89Br, 90,92,93,95Rb, 91Kr, 94,96,97,98Y, 95Sr, 133Sn, 135Te, 135Sb, 136,137I, 142Cs, 86Br, 87Se, 136Te, 138I, 140Xe, 140,143Cs, 88Rb, 139Xe(β-); calculated dominant first-forbidden transitions for the reactor anti-neutrino spectral shoulder, log ft, the coefficients in the shape factor, parameters. Comparison with available data.
doi: 10.1016/j.physletb.2024.138515
2024ZH15 Nucl.Instrum.Methods Phys.Res. A1059, 168983 (2024) H.Q.Zhang, P.Kuang, X.T.Yu, P.Zhang, F.Y.Liu, R.S.Yu, X.Z.Cao, B.Y.Wang Development of novel positron lifetime measurement system for potential liquid material inspection
doi: 10.1016/j.nima.2023.168983
2023FR01 Ann.Nucl.Energy 181, 109475 (2023) D.Fritz, Y.Danon, M.Rapp, T.H.Trumbull, M.Zerkle, J.Holmes, C.W.Chapman, G.Arbanas, J.M.Brown, K.Ramic, X.Hu, S.Singh, A.Ney, P.Brain, K.Cook, B.Wang Total thermal neutron cross section measurements of yttrium hydride from 0.0005 - 3 eV NUCLEAR REACTIONS 89Y, H(n, X), E=0.0005 - 3 eV; measured reaction products, En, In; deduced total σ and uncertainties. Comparison with ENDF/B-VIII.0library. The RPI LINAC facility.
doi: 10.1016/j.anucene.2022.109475
2023HA08 Phys.Rev. A 107, L020803 (2023) P.Hao, K.Deng, F.F.Wu, Z.Y.Ma, W.Z.Wei, W.H.Yuan, Y.B.Du, H.L.Liu, H.X.Zhang, L.R.Pang, B.Wang, J.Zhang, Z.H.Lu Precision measurement of 25Mg+-ion D1 and D2 transition frequencies ATOMIC PHYSICS 25Mg; measured frequencies; deduced precise values of doublet transition frequencies using the decoherence-assisted spectroscopy method with the full use of spontaneous emission signals to improve the detection sensitivity.
doi: 10.1103/PhysRevA.107.L020803
2023MU17 Int.J.Mod.Phys. E32, 2350045 (2023) The empirical coupled-channel model with the new analytical penetration formula for fusion cross-sections NUCLEAR REACTIONS 16O, 208Pb(16O, X), 120Sn(6Li, X), 119Sn(7Li, X), E(cm)<20 MeV; calculated fusion σ using the empirical coupled-channel (ECC) model with the Hill-Wheeler (HW) formula based on the parabolic approximation.
doi: 10.1142/S0218301323500453
2023WA36 Phys.Rev. C 108, 065805 (2023) Effective energy window of the E1 photon strength function for astrophysical neutron-capture reaction rates
doi: 10.1103/PhysRevC.108.065805
2023XI06 J.Phys.(London) G50, 085102 (2023) Q.Xiao, J.-H.Cheng, B.-L.Wang, Y.-Y.Xu, Y.-T.Zou, T.-P.Yu Half-lives for proton emission and α decay within the deformed Gamow-like model RADIOACTIVITY 109I, 112,113Cs, 117La, 121Pr, 131Eu, 135Tb, 140,141Ho, 144,145,146,147Tm, 150,151Lu, 155,156,157Ta, 159,160,161Re, 164,165,166,167Ir, 170,171Au, 176,177Tl, 185Bi, 111Cs, 127Pm, 137Tb(p), 106,108Te, 108,110,112Xe, 114Ba, 144Nd, 146,148Sm, 148,150,152Gd, 150,152,154Dy, 152,154,156Er, 154,156Yb, 156,158,160,162Hf, 174Hf, 158,160,162,164,166,168W, 180W, 162,164,166,168,170,172,174Os, 186Os, 168,170,172,174,176,178,180,182,184,186,188,190Pt, 170,172,174,176,178,180,182,184,186,188Hg, 178,180,182,184,186,188,190,192,194Pb, 210Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210Ra, 214,216,218,220,222,224,226Ra, 210,212,214,216,218,220,222,224,226,228,230,232Th, 216,218,220,222,224,226,228,230,232,234,236,238U, 228,230,232,234,236,238,240,242,244Pu, 234,236,238,240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254Cf, 246,248,250,252,254,256Fm, 252,254,256No, 256,258Rf, 266,268,270Hs, 270Ds, 282Ds, 286Cn, 286,288,290Fl, 290,292Lv, 294Og, 105Te, 109Te, 109Xe, 147Sm, 149,151Gd, 151,153Dy, 153,155Er, 155Yb, 157,159Hf, 161,163W, 167W, 161Os, 167,169,171,173Os, 171,173,175,177,179,181,183,185Pt, 175,177,179,181,183,185Hg, 183,185,187,189Pb, 187,189,191,193,195,197,199,201,203,205,207,209,211,213,215,217,219Po, 193,195,197,199Rn, 203,205,207,209,211,213,215,217,219,221Rn, 201,203,205,207,209,211,213,215,217,219,221,223Ra, 211,213,215,217,219,221,223,225,227Th, 221,223,225,227,229,231,233,235U, 229,231,233,235,237,239,241Pu, 233Cm, 239,241,243,245,247Cm, 237Cf, 245,247,249,251,253Cf, 249,251,253,255,257Fm, 255,257,259No, 257Rf, 261Rf, 261Sg, 265Hs, 109I, 113I, 145Pm, 147Eu, 151Tb, 151,153Ho, 155,157Tm, 155Lu, 157,159Ta, 163,165Re, 167,169,171,173,175,177Ir, 173,175,177,179,181,183,185Au, 177,179,181Tl, 187,189,191,193,195Bi, 193,195,197,199,201,203,205,207,209,211,213,215,217,219,221,223,225,227Ac, 211,213,215,217,219,221,223,225,227,229,231Pa, 219Np, 223,225,227,229,231,233,235,237Np, 229Am, 235Am, 239,241,243Am, 243,245,247,249Bk, 247Es, 251,253Es, 249,251Md, 255,257Md, 253,255Lr, 259Lr, 259Db, 261Bh, 110,112I, 114Cs, 152,154Ho, 154,156Tm, 158Lu, 158Ta, 162Ta, 160,162Re, 168Re, 166,168Ir, 172,174Ir, 170Au, 176Au, 180Tl, 186Bi, 192,194Bi, 212,214Bi, 192At, 200,202,204,206,208,210,212,214,216,218At, 200Fr, 204,206,208,210,212,214,216,218,220Fr, 216,218,220,222,224,226Ac, 212Pa, 224Pa, 228,230Pa, 236Np, 236Am, 244Bk, 248Es, 258Md, 272Rg(α); calculated T1/2 with the deformed Gamow-like model, which introduces the effects of nucleus deformation; deduced the deformed model follows the Geiger-Nuttall law. Comparison with available data.
doi: 10.1088/1361-6471/acdfeb
2022BU16 Phys.Rev.Lett. 128, 202502 (2022) M.T.Burkey, G.Savard, A.T.Gallant, N.D.Scielzo, J.A.Clark, T.Y.Hirsh, L.Varriano, G.H.Sargsyan, K.D.Launey, M.Brodeur, D.P.Burdette, E.Heckmaier, K.Joerres, J.W.Klimes, K.Kolos, A.Laminack, K.G.Leach, A.F.Levand, B.Longfellow, B.Maass, S.T.Marley, G.E.Morgan, P.Mueller, R.Orford, S.W.Padgett, A.Perez Galvan, J.R.Pierce, D.Ray, R.Segel, K.Siegl, K.S.Sharma, B.S.Wang Improved Limit on Tensor Currents in the Weak Interaction from 8Li β Decay RADIOACTIVITY 8Li(β-); measured decay products, Eβ, Iβ; deduced tensor currents in the low-energy regime by examining the β-ν correlation of trapped 8Li ions with the Beta-decay Paul Trap. Comparison with the standard model prediction.
doi: 10.1103/PhysRevLett.128.202502
2022WA36 Chin.Phys.C 46, 104001 (2022) X.Y.Wang, N.T.Zhang, Z.C.Zhang, C.G.Lu, T.L.Pu, J.L.Zhang, L.M.Duan, B.S.Gao, K.A.Li, Y.T.Li, Y.Qian, L.H.Ru, B.Wang, X.D.Xu, H.Y.Zhao, W.P.Lin, Z.W.Cai, B.F.Ji, Q.T.Li, J.Y.Xu, X.D.Tang Studies of the 2α and 3α channels of the 12C+12C reaction in the range of Ec.m.=8.9 MeV to 21 MeV using the active target Time Projection Chamber NUCLEAR REACTIONS 12C(12C, 2α), (12C, 8Be), (12C, 3α), (12C, X), E(cm)=8.9-21 MeV; measured reaction products, Eα, Iα; deduced fusion σ. Comparison with available data. 1024-channel TPC named pMATE (prototype Multi-purpose time projection chamber for nuclear Astrophysical and Exotic beam experiments), the Heavy Ion Research Facility in Lanzhou (HIRFL), China.
doi: 10.1088/1674-1137/ac7a1d
2022WA42 Phys.Rev. C 106, 054320 (2022) B.-L.Wang, F.Gao, L.-J.Wang, Y.Sun Effective and efficient algorithm for the Wigner rotation matrix at high angular momenta NUCLEAR STRUCTURE 156Dy; calculated levels, energies of the yrast band, high-spin states. Method for evaluation of the Wigner d function based on the Jacobi polynomials. Comparison to other theoretical methods.
doi: 10.1103/PhysRevC.106.054320
2022YA22 Eur.Phys.J. A 58, 157 (2022) Investigation of dynamic effects on fusion cross sections for reactions 16, 18O + 112, 116, 118, 124Sn NUCLEAR REACTIONS 112,116,118,124Sn(16O, X), (18O, X), E(cm)<65 MeV; analyzed available data; calculated fusion σ using the empirical coupled-channel (ECC) model.
doi: 10.1140/epja/s10050-022-00814-7
2021AD18 Phys.Rev.Lett. 126, 171801 (2021); Erratum Phys.Rev.Lett. 131, 249902 (2023) D.Q.Adams, C.Alduino, K.Alfonso, F.T.Avignone, O.Azzolini, G.Bari, F.Bellini, G.Benato, M.Biassoni, A.Branca, C.Brofferio, C.Bucci, J.Camilleri, A.Caminata, A.Campani, L.Canonica, X.G.Cao, S.Capelli, L.Cappelli, L.Cardani, P.Carniti, N.Casali, D.Chiesa, M.Clemenza, S.Copello, C.Cosmelli, O.Cremonesi, R.J.Creswick, A.D'Addabbo, I.Dafinei, C.J.Davis, S.Dell'Oro, S.Di Domizio, V.Dompe, D.Q.Fang, G.Fantini, M.Faverzani, E.Ferri, F.Ferroni, E.Fiorini, M.A.Franceschi, S.J.Freedman, S.H.Fu, B.K.Fujikawa, A.Giachero, L.Gironi, A.Giuliani, P.Gorla, C.Gotti, T.D.Gutierrez, K.Han, K.M.Heeger, R.G.Huang, H.Z.Huang, J.Johnston, G.Keppel, Yu.G.Kolomensky, C.Ligi, L.Ma, Y.G.Ma, L.Marini, R.H.Maruyama, D.Mayer, Y.Mei, N.Moggi, S.Morganti, T.Napolitano, M.Nastasi, J.Nikkel, C.Nones, E.B.Norman, A.Nucciotti, I.Nutini, T.O'Donnell, J.L.Ouellet, S.Pagan, C.E.Pagliarone, L.Pagnanini, M.Pallavicini, L.Pattavina, M.Pavan, G.Pessina, V.Pettinacci, C.Pira, S.Pirro, S.Pozzi, E.Previtali, A.Puiu, C.Rosenfeld, C.Rusconi, M.Sakai, S.Sangiorgio, B.Schmidt, N.D.Scielzo, V.Sharma, V.Singh, M.Sisti, D.Speller, P.T.Surukuchi, L.Taffarello, F.Terranova, C.Tomei, K.J.Vetter, M.Vignati, S.L.Wagaarachchi, B.S.Wang, B.Welliver, J.Wilson, K.Wilson, L.A.Winslow, S.Zimmermann, S.Zucchelli Measurement of the 2νββ Decay Half-Life of 130Te with CUORE RADIOACTIVITY 130Te(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino mode T1/2. Comparison with available data. CUORE detector.
doi: 10.1103/PhysRevLett.126.171801
2021AK04 Phys.Rev. C 104, 065501 (2021) D.S.Akerib, A.K.Al Musalhi, S.K.Alsum, C.S.Amarasinghe, A.Ames, T.J.Anderson, N.Angelides, H.M.Araujo, J.E.Armstrong, M.Arthurs, X.Bai, J.Balajthy, S.Balashov, J.Bang, J.W.Bargemann, D.Bauer, A.Baxter, P.Beltrame, E.P.Bernard, A.Bernstein, A.Bhatti, A.Biekert, T.P.Biesiadzinski, H.J.Birch, G.M.Blockinger, E.Bodnia, B.Boxer, C.A.J.Brew, P.Bras, S.Burdin, J.K.Busenitz, M.Buuck, R.Cabrita, M.C.Carmona-Benitez, M.Cascella, C.Chan, N.I.Chott, A.Cole, M.V.Converse, A.Cottle, G.Cox, O.Creaner, J.E.Cutter, C.E.Dahl, L.de Viveiros, J.E.Y.Dobson, E.Druszkiewicz, S.R.Eriksen, A.Fan, S.Fayer, N.M.Fearon, S.Fiorucci, H.Flaecher, E.D.Fraser, T.Fruth, R.J.Gaitskell, J.Genovesi, C.Ghag, E.Gibson, S.Gokhale, M.G.D.van der Grinten, C.B.Gwilliam, C.R.Hall, S.J.Haselschwardt, S.A.Hertel, M.Horn, D.Q.Huang, M.C.I.gnarra, O.Jahangir, R.S.James, W.Ji, J.Johnson, A.C.Kaboth, A.C.Kamaha, K.Kamdin, K.Kazkaz, D.Khaitan, A.Khazov, I.Khurana, D.Kodroff, L.Korley, E.V.Korolkova, H.Kraus, S.Kravitz, L.Kreczko, B.Krikler, V.A.Kudryavtsev, E.A.Leason, J.Lee, D.S.Leonard, K.T.Lesko, C.Levy, J.Liao, J.Lin, A.Lindote, R.Linehan, W.H.Lippincott, X.Liu, M.I.Lopes, E.Lopez Asamar, B.Lopez Paredes, W.Lorenzon, S.Luitz, P.A.Majewski, A.Manalaysay, L.Manenti, R.L.Mannino, N.Marangou, M.E.McCarthy, D.N.McKinsey, J.McLaughlin, E.H.Miller, E.Mizrachi, A.Monte, M.E.Monzani, J.A.Morad, J.D.Morales Mendoza, E.Morrison, B.J.Mount, A.St.J.Murphy, D.Naim, A.Naylor, C.Nedlik, H.N.Nelson, F.Neves, J.A.Nikoleyczik, A.Nilima, I.Olcina, K.C.Oliver-Mallory, S.Pal, K.J.Palladino, J.Palmer, S.Patton, N.Parveen, E.K.Pease, B.Penning, G.Pereira, A.Piepke, Y.Qie, J.Reichenbacher, C.A.Rhyne, A.Richards, Q.Riffard, G.R.C.Rischbieter, R.Rosero, P.Rossiter, D.Santone, A.B.M.R.Sazzad, R.W.Schnee, P.R.Scovell, S.Shaw, T.A.Shutt, J.J.Silk, C.Silva, R.Smith, M.Solmaz, V.N.Solovov, P.Sorensen, J.Soria, I.Stancu, A.Stevens, K.Stifter, B.Suerfu, T.J.Sumner, N.Swanson, M.Szydagis, W.C.Taylor, R.Taylor, D.J.Temples, P.A.Terman, D.R.Tiedt, M.Timalsina, W.H.To, D.R.Tovey, M.Tripathi, D.R.Tronstad, W.Turner, U.Utku, A.Vaitkus, B.Wang, J.J.Wang, W.Wang, J.R.Watson, R.C.Webb, R.G.White, T.J.Whitis, M.Williams, F.L.H.Wolfs, D.Woodward, C.J.Wright, X.Xiang, J.Xu, M.Yeh, P.Zarzhitsky Projected sensitivity of the LUX-ZEPLIN experiment to the two-neutrino and neutrinoless double β decays of 134Xe RADIOACTIVITY 134Xe(2β-); measured recoiling nuclei and electrons, decay energy spectra using LUX-ZEPLIN (LZ) detector of liquid xenon (LXe), with scintillation and electro-luminescence light detected using 494 photomultipliers at Sanford Underground Research Facility (SURF) in South Dakota; deduced lower limits of T1/2 values for 2νββ and 0νββ decay modes.
doi: 10.1103/PhysRevC.104.065501
2021KO09 Nucl.Instrum.Methods Phys.Res. A1000, 165240 (2021) K.Kolos, A.M.Hennessy, N.D.Scielzo, V.E.Iacob, J.C.Hardy, M.A.Stoyer, A.P.Tonchev, W.-J.Ong, M.T.Burkey, B.Champine, J.A.Clark, P.Copp, A.Gallant, E.B.Norman, R.Orford, H.I.Park, J.Rohrer, D.Santiago-Gonzalez, G.Savard, A.J.Shaka, B.S.Wang, S.Zhu New approach to precisely measure γ-ray intensities for long-lived fission products, with results for the decay of 95Zr RADIOACTIVITY 95Zr, 95Nb, 95Sr, 95Y(β-); measured decay products, Eγ, Iγ, Eβ, Iβ, β-γ-coin.; deduced γ-ray energies and intensities, β-branching ratios. Comparison with a Monte Carlo decay code simulations. CARIBU facility, the reactor facility at TAMU.
doi: 10.1016/j.nima.2021.165240
2021LV03 Phys.Rev. C 103, 064616 (2021) X.-J.Lv, Z.-Y.Yue, W.-J.Zhao, B.Wang Theoretical study of evaporation-residue cross sections of superheavy nuclei NUCLEAR REACTIONS 208Pb, 209Bi(48Ca, xn), E(cm)=160-200 MeV; 208Pb, 209Bi(50Ti, xn), E(cm)=170-210 MeV; 208Pb, 209Bi(54Cr, xn), E(cm)=190-230 MeV; 208Pb, 209Bi(58Fe, xn), E(cm)=210-240 MeV; 208Pb, 209Bi(64Ni, xn), E(cm)=230-250 MeV; 208Pb, 209Bi(70Zn, xn), E(cm)=250-270 MeV; 238U, 237Np, 244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, xn), E(cm)=180-260 MeV; 249Cf(45Sc, xn), 249Bk(50Ti, xn), 248Cm(51V, xn), E(cm)=200-260 MeV; 243Am, 248Cm(54Cr, xn), E(cm)=220-290 MeV; 249,251Cf(50Ti, xn), E(cm)=200-270 MeV; 249Bk(51V, xn), E(cm)=220-270 MeV; calculated evaporation-residue cross sections at energies near and above the Coulomb barrier by combining an empirical coupled-channel model, an analytical formula for describing the fusion probability, and a statistical model. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.064616
2021RE10 Phys.Rev. A 104, 022811 (2021) B.Ren, Z.Xia, Y.Zhang, L.Wei, W.Yu, J.Han, B.Wang, Y.Zou, L.Chen, B.Wei Three-body fragmentation mechanism of C2H43+ produced by 18 - keV/uNe8+ impact NUCLEAR REACTIONS C, H(Ne, X), E=18 keV/nucleon; measured reaction products, TOF; deduced Dalitz plot of fragmentation channels. COLTRIMS technique.
doi: 10.1103/PhysRevA.104.022811
2021WA20 Phys.Rev. C 103, 034605 (2021) Theoretical study of evaporation-residue cross sections for fusion reactions at energies near the Coulomb barrier NUCLEAR REACTIONS 209Bi(6Li, xn), (7Li, xn), E(cm)=20-55 MeV; 169Tm, 181Ta(9Be, xn), E(cm)=25-55 MeV; 186W, 187Re(9Be, xn), E(cm)=30-60 MeV; 208Pb(9Be, xn), E(cm)=30-80 MeV; 209Bi(9Be, xn), E(cm)=30-70 MeV; 89Y(12C, xn), E(cm)=25-70 MeV; 152Sm(12C, xn), E(cm)=40-80 MeV; 159Tb(12C, xn), E(cm)=40-90 MeV; 194,198Pt(12C, xn), E(cm)=50-90 MeV; 197Au, 205Tl, 208Pb(12C, xn), E(cm)=50-100 MeV; 246Cm(12C, xn), E(cm)=40-125 MeV; 169Tm(13C, xn), E(cm)=40-100 MeV; 207Pb(13C, xn), E(cm)=50-100 MeV; 246Cm(13C, xn), E(cm)=40-125 MeV; 134Ba(16O, xn), E(cm)=50-120 MeV; 148,150Nd(16O, xn), E(cm)=50-90 MeV; 165Ho(16O, xn), E(cm)=50-120 MeV; 197Au(16O, xn), E(cm)=65-120 MeV; 208Pb(16O, xn), E(cm)=60-110 MeV; 238U(16O, xn), E(cm)=60-120 MeV; 148Nd(18O, xn), E(cm)=50-90 MeV; 197Au(18O, xn), E(cm)=60-120 MeV; 181Ta(19F, xn), E(cm)=65-120 MeV; 188,192Os(19F, xn), E(cm)=70-110 MeV; 150Nd(22Ne, xn), E(cm)=60-170 MeV; 194,196,198Pt(22Ne, xn), E(cm)=80-170 MeV; 164Dy(40Ar, xn), E(cm)=120-220 MeV; 165Ho(40Ar, xn), E(cm)=120-180 MeV; 169Tm, 174Yb(40Ar, xn), E(cm)=120-200 MeV; 170Er(30Si, xn), E(cm)=100-150 MeV; 122Sn(48Ti, xn), E(cm)=110-180 MeV; analyzed experimental data for evaporation-residue σ(E) of fission-fusion reactions at energies near the Coulomb barrier using an empirical coupled-channel model, and a statistical model.
doi: 10.1103/PhysRevC.103.034605
2021WI11 Nucl.Instrum.Methods Phys.Res. A1017, 165806 (2021) G.L.Wilson, T.S.Nagel, S.T.Marley, N.D.Scielzo, A.Aprahamian, J.A.Clark, A.Czeszumska, G.Savard, K.Siegl, B.S.Wang Reconstruction of β-delayed neutron energy spectra from recoil-ion spectroscopy of trapped ions RADIOACTIVITY 137I, 99Y, 135Sb(β-n); calculated neutron-energy spectrum and the probability of β-delayed neutron emission.
doi: 10.1016/j.nima.2021.165806
2021YA27 Phys.Rev. C 104, 034607 (2021) J.-M.Yang, Z.-W.Song, W.-J.Zhao, B.Wang Theoretical study of dynamic effects on fusion cross sections for reactions 32, 34, 36S + 204, 206, 208Pb NUCLEAR REACTIONS 204,206,208Pb(32S, X), (34S, X), (36S, X), E(cm)=130-190 MeV; calculated fusion σ(E), universal fusion functions (UFF) using an empirical coupled-channel (ECC) model to analyze the dynamic effects. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.034607
2020CZ01 Phys.Rev. C 101, 024312 (2020) A.Czeszumska, N.D.Scielzo, S.A.Caldwell, J.A.Clark, G.Savard, B.S.Wang, A.Aprahamian, M.T.Burkey, C.J.Chiara, J.Harker, A.F.Levand, S.T.Marley, G.Morgan, J.M.Munson, E.B.Norman, A.Nystrom, R.Orford, S.W.Padgett, A.Perez Galvan, K.S.Sharma, K.Siegl, S.Y.Strauss β-delayed neutron emission studies of 137,138I and 144,145Cs performed with trapped ions RADIOACTIVITY 137,138I, 144,145Cs(β-), (β-n)[252Cf(SF) CARIBU facility and mass scans of radioactive beams with the Canadian Penning Trap (CPT) mass spectrometer at Argonne National Laboratory]; measured recoil ions, Eβ, Eγ, (recoil ions)β- and βγ-coin using Beta-decay Paul Trap with two plastic-scintillator ΔE-E telescopes, two MCP detectors, and two HPGe detectors; deduced beta-delayed neutron spectra, beta-delayed neutron-emission probabilities (%β-n or Pn). Comparison with previous experimental results.
doi: 10.1103/PhysRevC.101.024312
2020MA08 Phys.Rev. C 101, 024904 (2020) H.-H.Ma, D.Wen, K.Lin, W.L.Qian, B.Wang, Y.Hama, T.Kodama Hydrodynamic results on multiplicity fluctuations in heavy-ion collisions
doi: 10.1103/PhysRevC.101.024904
2020ME07 Phys.Rev. C 101, 064002 (2020) ΣcN interaction in chiral effective field theory
doi: 10.1103/PhysRevC.101.064002
2020NU01 J.Low Temp.Physics 199, 519 (2020) I.Nutini, D.Q.Adams, C.Alduino, K.Alfonso, F.T.Avignone, O.Azzolini, G.Bari, F.Bellini, G.Benato, M.Biassoni, A.Branca, C.Brofferio, C.Bucci, A.Caminata, A.Campani, L.Canonica, X.G.Cao, S.Capelli, L.Cappelli, L.Cardani, P.Carniti, N.Casali, D.Chiesa, N.Chott, M.Clemenza, S.Copello, C.Cosmelli, O.Cremonesi, R.J.Creswick, A.D'Addabbo, D.D'Aguanno, I.Dafinei, C.J.Davis, S.Dell'Oro, S.Di Domizio, V.Dompe, D.Q.Fang, G.Fantini, M.Faverzani, E.Ferri, F.Ferroni, E.Fiorini, M.A.Franceschi, S.J.Freedman, B.K.Fujikawa, A.Giachero, L.Gironi, A.Giuliani, P.Gorla, C.Gotti, T.D.Gutierrez, K.Han, K.M.Heeger, R.G.Huang, H.Z.Huang, J.Johnston, G.Keppel, Yu.G.Kolomensky, C.Ligi, Y.G.Ma, L.Ma, L.Marini, R.H.Maruyama, Y.Mei, N.Moggi, S.Morganti, T.Napolitano, M.Nastasi, J.Nikkel, C.Nones, E.B.Norman, V.Novati, A.Nucciotti, T.O'Donnell, J.L.Ouellet, C.E.Pagliarone, L.Pagnanini, M.Pallavicini, L.Pattavina, M.Pavan, G.Pessina, V.Pettinacci, C.Pira, S.Pirro, S.Pozzi, E.Previtali, A.Puiu, C.Rosenfeld, C.Rusconi, M.Sakai, S.Sangiorgio, B.Schmidt, N.D.Scielzo, V.Singh, M.Sisti, D.Speller, L.Taffarello, F.Terranova, C.Tomei, M.Vignati, S.L.Wagaarachchi, B.S.Wang, B.Welliver, J.Wilson, K.Wilson, L.A.Winslow, L.Zanotti, S.Zimmermann, S.Zucchelli The CUORE Detector and Results RADIOACTIVITY 130Te(2β-); measured decay products, Eβ, Iβ; deduced two-neutron T1/2 and neutrinoless mode limit. The cryogenic underground observatory for rare events (CUORE).
doi: 10.1007/s10909-020-02402-9
2020WA04 Phys.Rev. C 101, 025806 (2020) B.S.Wang, S.A.Caldwell, N.D.Scielzo, A.Czeszumska, J.A.Clark, G.Savard, A.Aprahamian, M.T.Burkey, C.J.Chiara, J.Harker, A.F.Levand, S.T.Marley, G.E.Morgan, J.M.Munson, E.B.Norman, A.Nystrom, R.Orford, S.W.Padgett, A.Perez Galvan, K.S.Sharma, K.Siegl, S.Y.Strauss β-delayed-neutron studies of 135,136Sb and 140I performed with trapped ions RADIOACTIVITY 135,136Sb, 140I(β-), (β-n) [from 252Cf(SF) CARIBU facility and mass scans of radioactive beams with the Canadian Penning Trap (CPT) mass spectrometer at Argonne National Laboratory]; measured recoil ions, Eβ, Eγ, (recoil ions)β- and βγ-coin using Beta-decay Paul Trap with two plastic-scintillator ΔE-E telescopes, two MCP detectors, and two HPGe detectors; deduced beta-delayed neutron spectra, beta-delayed neutron-emission probabilities (%β-n or Pn). Comparison with earlier experimental results.
doi: 10.1103/PhysRevC.101.025806
2020WA05 Phys.Rev. C 101, 024606 (2020) 16-18O + 16O and 16, 18O + 12, 13C fusion-evaporation reactions at near-Coulomb-barrier energies from statistical model calculations NUCLEAR STRUCTURE 20,21,22Ne, 23,24,25Na, 23,24,25,26,27,28Mg, 26,27,28,29Al, 27,28,29Si; calculated Gilbert-Cameron level densities of the residual nuclei as a function of the excited energy for the oxygen + carbon system. NUCLEAR REACTIONS 16O(16O, X), E(cm)=9-14 MeV; 16O(17O, X), (18O, X), E(cm)=8-13 MeV; 12C(16O, X), (18O, X), E(cm)=6-15 MeV; 13C(16O, X), E(cm)=8-15 MeV; calculated α-emission σ(E). 16O(16O, n)31S, (16O, p)31P, (16O, 2p)30Si, (16O, np)30P, (16O, α)28Si, (16O, pα)27Al, (16O, 2α)24Mg, E(cm)=8-14 MeV; calculated production σ(E) of the residual nuclei. Calculations based on Hauser-Feshbach (HF) statistical-model using the original Gilbert-Cameron level-density formula, and the new level-density formula including the α-clustering effect. Comparison with experimental data. Relevance to nucleosynthesis in astrophysics and α-clustering effects in light nuclei.
doi: 10.1103/PhysRevC.101.024606
2020WE12 Eur.Phys.J. A 56, 222 (2020) D.Wen, K.Lin, W.-L.Qian, B.Wang, Y.Hama, T.Kodama On nonlinearity in hydrodynamic response to the initial geometry in relativistic heavy-ion collisions
doi: 10.1140/epja/s10050-020-00235-4
2019BU23 Hyperfine Interactions 240, 36 (2019) M.T.Burkey, G.Savard, A.Gallant, N.D.Scielzo, J.A.Clark, T.Y.Hirsh, D.P.Burdette, E.Heckmaier, J.Klimes, K.Kolos, S.T.Marley, G.E.Morgan, R.Orford, S.Padgett, J.Pierce, R.Segel, Ku.S.Sharma, L.Varriano, B.S.Wang Precision β - ν correlation measurements with the Beta-decay Paul Trap RADIOACTIVITY 8Li(β-); measured decay products, Eβ, Iβ; deduced correlations. Comparison with simulations.
doi: 10.1007/s10751-019-1580-0
2019MA77 Phys.Rev. A 100, 052506 (2019) D.L.Maser, E.Hoenig, B.-Y.Wang, P.M.Rupasinghe, S.G.Porsev, M.S.Safronova, P.K.Majumder High-precision measurement and ab initio calculation of the (6s26p2) 3P0 → 3P2 electric-quadrupole-transition amplitude in 208Pb ATOMIC PHYSICS 208Pb; measured frequencies; deduced electric quadrupole (E2) transition amplitude in atomic lead.
doi: 10.1103/PhysRevA.100.052506
2019SU09 Phys.Rev. C 99, 054316 (2019) T.-T.Sun, Z.-X.Liu, L.Qian, B.Wang, W.Zhang Continuum Skyrme-Hartree-Fock-Bogoliubov theory with Green's function method for odd-A nuclei NUCLEAR STRUCTURE 159Sn; calculated neutron occupation number density, neutron density and neutron pairing density distributions, neutron Hartree-Fock single-particle energy. Z=50, A=122-178; calculated S(2n), neutron quasiparticle levels, neutron rms radii and neutron densities. Self-consistent continuum Skyrme-HFB theory with the Green's function technique in the coordinate space including equal filling approximation blocking effects. Comparison with experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.99.054316
2019WA33 Phys.Rev. C 100, 064609 (2019) B.S.Wang, J.T.Harke, O.A.Akindele, R.J.Casperson, R.O.Hughes, J.D.Koglin, K.Kolos, E.B.Norman, S.Ota, A.Saastamoinen Determining the average prompt-fission-neutron multiplicity for 239Pu(n, f) via a 240Pu(α, α' f) surrogate reaction NUCLEAR REACTIONS 240Pu(α, α'F), E=53.9 MeV; measured fission fragments, charged particles, scattered α particles, Eα, Iα, E(n), I(n), α(fission fragment)- and αn(fission fragment)-coin using the NeutronSTARS array and NeutronBall at the K150 Cyclotron facility of Texas A and M University; deduced particle-identification plot for p, d, t, 3He and α particles. 239Pu(n, F), E=0.25-26.25 MeV; deduced average prompt-fission-neutron multiplicity using the results from surrogate reaction 240Pu(α, a°F). Comparison with previous experimental results from direct measurements.
doi: 10.1103/PhysRevC.100.064609
2018CH34 Phys.Lett. B 782, 652 (2018) A.Chyzh, P.Jaffke, C.Y.Wu, R.A.Henderson, P.Talou, I.Stetcu, J.Henderson, M.Q.Buckner, S.A.Sheets, R.Hughes, B.Wang, J.L.Ullmann, S.Mosby, T.A.Bredeweg, A.C.Hayes-Sterbenz, J.M.O'Donnell Dependence of the prompt fission γ-ray spectrum on the entrance channel of compound nucleus: Spontaneous vs. neutron-induced fission RADIOACTIVITY 240,242Pu(SF); measured decay products, Eγ, Iγ; deduced prompt γ-ray spectra. NUCLEAR REACTIONS 239,241Pu(n, F), E ∼ 100 keV; measured reaction products, Eγ, Iγ; deduced prompt fission γ-ray energy spectra. Comparison with Monte Carlo Hauser-Feshbach statistical model for the neutron-induced fission.
doi: 10.1016/j.physletb.2018.06.006
2018GO08 Phys.Rev. C 97, 054610 (2018) A.Gomez Camacho, B.Wang, H.Q.Zhang Systematic continuum-discretized coupled-channels calculations of total fusion for 6Li with targets 28Si, 59Co, 96Zr, 198Pt, and 209Bi: Effect of resonance states NUCLEAR REACTIONS 28Si, 59Co, 96Zr, 198Pt, 209Bi(6Li, 6Li), (6Li, dα), E(cm)=8-48 MeV; calculated total fusion σ(E) and fusion widths for elastic channel, resonance and non-resonance subspaces, net polarization potentials using continuum discretized coupled-channel calculations (CDCC); deduced effect of resonant break-up states on fusion σ. NUCLEAR STRUCTURE 6Li; calculated centroid energies and widths of 3+, 2+ and 1+ resonances, and compared with experimental values.
doi: 10.1103/PhysRevC.97.054610
2018WA16 Phys.Rev. C 98, 014615 (2018) B.Wang, W.-J.Zhao, E.-G.Zhao, S.-G.Zhou Theoretical study of the capture of stable 39K and neutron-rich radioactive 46K by 181Ta NUCLEAR REACTIONS 181Ta(39K, X), E=180-210 MeV; 181Ta(46K, X), E=190-215 MeV; calculated capture σ(E) using empirical coupled-channel (ECC) model and the universal fusion function (UFF) prescription; deduced barrier parameters, and fusion functions. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.014615
2018WU02 Phys.Rev. A 97, 032702 (2018) Y.Wu, Y.Liang, M.X.Xu, Y.Yuan, C.H.Chang, Z.C.Qian, B.Y.Wang, P.Kuang, P.Zhang Thick-target-method study of Mαβ x-ray production cross sections of Pb and Bi impacted by positrons up to 9 keV NUCLEAR REACTIONS Pb, 209Bi(e+, X), E<9 keV; measured reaction products, Eγ, Iγ, X-rays; deduced thick target production X-ray σ. Comparison with theoretical calculations.
doi: 10.1103/PhysRevA.97.032702
2017WA02 At.Data Nucl.Data Tables 114, 281 (2017) B.Wang, K.Wen, W.-J.Zhao, E.-G.Zhao, S.-G.Zhou Systematics of capture and fusion dynamics in heavy-ion collisions NUCLEAR REACTIONS 89Y(12C, X), 59Co(14N, X), E(cm)<100 MeV; calculated capture excitation functions by using an empirical coupled-channel (ECC) model for 182<ZpZt<1640. Comparison with available data.
doi: 10.1016/j.adt.2016.06.003
2016CH04 Phys.Rev. C 93, 014611 (2016) B.Champine, M.E.Gooden, Krishichayan, E.B.Norman, N.D.Scielzo, M.A.Stoyer, K.J.Thomas, A.P.Tonchev, W.Tornow, B.S.Wang Measurement of the 169Tm(n, 3n)167Tm cross section and the associated branching ratios in the decay of 167Tm NUCLEAR REACTIONS 169Tm(n, 3n), 58Ni, 90Zr, 169Tm(n, 2n), 94Zr(n, α), E=17.35, 18.34, 19.33, 20.32, 21.31 MeV, [quasimonoenergetic neutrons from 2H(d, n), E=15.0-19.2 at TUNL tandem Van de Graaff accelerator]; measured neutron spectra, Eγ, Iγ, σ(E) by activation method. Comparison with previous experimental data, compiled data in EXFOR database and evaluated data in ENDF database. Relevance to measurement of yield of reaction-in-flight neutrons at the LLNL National Ignition Facility (NIF). RADIOACTIVITY 167Tm(EC)[from 165Ho(α, 2n), E=29 MeV at LBNL cyclotron facility]; measured Eγ, Iγ, I(x rays), source activity; deduced branching ratios of 207.8-keV and 531.5-keV γ rays. Comparison with previous experimental values and evaluated data.
doi: 10.1103/PhysRevC.93.014611
2016WA04 Phys.Rev. C 93, 014615 (2016) B.Wang, W.-J.Zhao, A.Diaz-Torres, E.-G.Zhao, S.-G.Zhou Systematic study of suppression of complete fusion in reactions involving weakly bound nuclei at energies above the Coulomb barrier NUCLEAR REACTIONS 89Y, 124Sn, 144Sm, 169Tm, 181Ta, 187Re, 208Pb, 209Bi(9Be, X), E(cm)=10-55 MeV; 90,96Zr, 154Sm, 159Tb, 197Au, 198Pt, 208Pb, 209Bi(6Li, X), E=10-55 MeV; 159Tb, 165Ho, 197Au, 198Pt, 209Bi(7Li, X), E=10-60 MeV; 159Tb, 209Bi(10B, X), (11B, X), E(cm)=30-80 MeV; calculated complete fusion σ(E). Empirical coupled-channel model with and without breakup effects. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.014615
2015KI07 Phys.Rev. C 92, 035801 (2015) A.Kim, N.H.Lee, M.H.Han, J.S.Yoo, K.I.Hahn, H.Yamaguchi, D.N.Binh, T.Hashimoto, S.Hayakawa, D.Kahl, T.Kawabata, Y.Kurihara, Y.Wakabayashi, S.Kubono, S.Choi, Y.K.Kwon, J.Y.Moon, H.S.Jung, C.S.Lee, T.Teranishi, S.Kato, T.Komatsubara, B.Guo, W.P.Liu, B.Wang, Y.Wang Measurement of the 14O(α, p)17F cross section at Ec.m. ≈ 2.1-5.3MeV NUCLEAR REACTIONS 4He(14O, p), E=2.5 MeV/nucleon, [secondary 14O beam from 1H(14N, n), E=8.4 MeV/nucleon primary reaction at RIBF-RIKEN]; measured E(p), I(p), pp-coin, energy distribution of single- and double-proton events, differential cross sections by thick target method. 18Ne; deduced levels, resonances, J, π, proton and α widths by R-matrix analysis, astrophysical reaction rates, strong single-proton decay events, but no strong double-proton events. Relevance to trigger reaction for the x-ray burst and nucleosynthesis of heavy nuclei up to Cd.
doi: 10.1103/PhysRevC.92.035801
2015WA26 Phys.Rev. C 92, 024620 (2015) B.S.Wang, E.B.Norman, N.D.Scielzo, A.R.Smith, K.J.Thomas, S.A.Wender Cosmogenic-neutron activation of TeO2 and implications for neutrinoless double-β decay experiments NUCLEAR REACTIONS Te, O(n, X)7Be/60Co/101Rh/101mRh/102mRh/105Ag/106mAg/110Ag/110mAg/111Ag/111In/114mIn/113Sn/117mSn/118Sb/119Sb/120mSb/122Sb/124Sb/125Sb/126Sb/127Sb/131mXe/118Te/119mTe/121Te/121mTe/123mTe/125mTe/127Te/127mTe/129Te/129mTe/131Te/131mTe, E<800 MeV from LANSCE-LANL facility; measured off-line Eγ, Iγ at Low Background Facility of LBNL; deduced flux-averaged cross sections; estimated cosmogenic-activation background from 110Ag and 60Co in connection with 130Te 0νββ-decay experiments at CUORE and SNO-2. Benchmarking by GEANT4 simulations. Comparison of measured σ with calculations using ACTIVIA code based on Silberberg and Tsao (S and T) semiempirical formulas.
doi: 10.1103/PhysRevC.92.024620
2015ZH09 Chin.Phys.Lett. 32, 042501 (2015) H.-B.Zhang, X.-Y.Zhang, F.Ma, Y.-Q.Ju, H.-L.Ge, L.Chen, Y.-B.Zhang, J.-F.Wei, Y.-Y.Li, P.Luo, J.-G.Wang, B.Wang, X.-W.Xu, B.Zhou Residual Nuclides Induced in Cu Target by a 250 MeV Proton Beam* NUCLEAR REACTIONS Cu(p, X)51Cr/52Mn/54Mn/56Co/57Co/58Co, E=250 MeV; measured reaction products, Eγ, Iγ; deduced σ. MCNPX and GEANT4 codes calculations, comparison with experimental data.
doi: 10.1088/0256-307X/32/4/042501
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
2014WA36 Phys.Rev. C 90, 034612 (2014) B.Wang, W.-J.Zhao, P.R.S.Gomes, E.-G.Zhao, S.-G.Zhou Systematic study of breakup effects on complete fusion at energies above the Coulomb barrier NUCLEAR REACTIONS 90Zr(6Li, X), E not given; 165Ho, 208Pb(7Li, X), E not given; 144,152Sm, 159Tb, 197Au, 198Pt, 209Bi(6Li, X), (7Li, X), E not given; 89Y, 144Sm, 124Sn, 186W, 208Pb, 209Bi(9Be, X), E not given; 159Tb, 209Bi(10B, X), E not given; 159Tb, 209Bi(11B, X), E not given; 89Y, 152Sm, 159Tb, 181Ta, 208Pb(12C, X), E not given; 159Tb, 181Ta, 207Pb(13C, X), E not given; 103Rh, 148,150Nd, 159Tb, 169Tm(16O, X), E not given; calculated dimensionless complete fusion (CF) functions. Discussed systematics of suppression factors. Comparison with universal fusion functions, and available experimental values. Proposed an analytical formula between the CF suppression factor and the breakup threshold energy.
doi: 10.1103/PhysRevC.90.034612
2013CZ01 Phys.Rev. C 87, 034613 (2013) A.Czeszumska, C.T.Angell, J.T.Burke, N.D.Scielzo, E.B.Norman, R.A.E.Austin, G.Boutoux, R.J.Casperson, P.Chodash, R.O.Hughes, C.M.Mattoon, V.Meot, J.Munson, L.Phair, J.J.Ressler, O.Roig, T.J.Ross, E.Swanberg, B.Wang Determining the 239Np(n, f) cross section using the surrogate ratio method NUCLEAR REACTIONS 236,238U(3He, pF), E=29 MeV; measured proton, deuteron, triton, 3,4He spectra, fission events, fission anisotropies, particle-fission time-to-amplitude spectrum, (fission)p-coin using STARS array at LBNL cyclotron facility. 239Np(n, F), E=0.5-20 MeV; deduced cross section by surrogate ratio method. Comparison with ENDF/B-VII.0, JENDL-4.0, and CENDL-3.1 evaluated libraries. Impact on estimate of 240Pu produced during fuel burnup in calculations using reactor codes.
doi: 10.1103/PhysRevC.87.034613
2013GU12 Eur.Phys.J. A 49, 35 (2013) V.Guzey, M.Guzzi, P.M.Nadolsky, M.Strikman, B.Wang Massive neutral gauge boson production as a probe of nuclear modifications of parton distributions at the LHC
doi: 10.1140/epja/i2013-13035-6
2013LI09 Phys.Rev. C 87, 017601 (2013) Z.H.Li, Y.J.Li, J.Su, B.Guo, E.T.Li, K.J.Dong, X.X.Bai, Z.C.Li, J.C.Liu, S.Q.Yan, Y.B.Wang, S.Zeng, G.Lian, B.X.Wang, S.J.Jin, X.Liu, W.J.Zhang, W.Z.Huang, Q.W.Fan, L.Gan, Z.D.Wu, W.P.Liu New determination of the proton spectroscopic factor in 9Be from the 13C(9Be, 8Li)14N angular distribution NUCLEAR REACTIONS 13C(9Be, 8Li)14N, 12,13C(9Be, 9Be), E=40 MeV; measured particle spectra, Eα, differential s(θ) using Q3D magnetic spectrometer at HI-13 tandem accelerator facility in Beijing. 9Be; deduced proton spectroscopic factor for g.s. Optical model and DWBA analysis. Comparison with previous experimental and theoretical studies. Relevance to astrophysical S factor for 8Li(p, γ)9Be reaction.
doi: 10.1103/PhysRevC.87.017601
2013LI46 Phys.Rev. C 88, 037301 (2013) C.Liu, S.Y.Wang, B.Qi, D.P.Sun, S.Wang, C.J.Xu, L.Liu, P.Zhang, Z.Q.Li, B.Wang, X.C.Shen, M.R.Qin, H.L.Liu, Y.Gao, L.H.Zhu, X.G.Wu, G.S.Li, C.Y.He, Y.Zheng Signature splitting, shape evolution, and nearly degenerate bands in 108Ag NUCLEAR REACTIONS 104Ru(7Li, 3n), E=33 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO) at CIAE, Beijing facility. 108Ag; deduced high-spin levels, J, π, bands, multipolarities, configurations, signature splitting and signature inversion, staggering parameter. Total Routhian surface (TRS) calculations. Systematics of level energies, staggering parameter, B(M1)/B(E2) ratios, kinematic moments of inertial for bands in 98,100Tc, 104,106Rh, 106,108Ag, and comparison with behavior of chiral partner bands.
doi: 10.1103/PhysRevC.88.037301
2012GU18 Astrophys.J. 756, 193 (2012) B.Guo, Z.H.Li, M.Lugaro, J.Buntain, D.Y.Pang, Y.J.Li, J.Su, S.Q.Yan, X.X.Bai, Y.S.Chen, Q.W.Fan, S.J.Jin, A.I.Karakas, E.T.Li, Z.C.Li, G.Lian, J.C.Liu, X.Liu, J.R.Shi, N.C.Shu, B.X.Wang, Y.B.Wang, S.Zeng, W.P.Liu New Determination of the 13C(α, n)16O Reaction Rate and its Influence on the s-process Nucleosynthesis in AGB Stars NUCLEAR REACTIONS 12,13C(11B, 7Li), E=50 MeV; measured reaction products; deduced σ(θ), S-factors, stellar rates. Comparison with available data.
doi: 10.1088/0004-637X/756/2/193
2012LI14 Eur.Phys.J. A 48, 13 (2012); Erratum Eur.Phys.J. A 49, 106 (2013) Y.J.Li, Z.H.Li, E.T.Li, X.X.Bai, J.Su, B.Guo, B.X.Wang, S.Q.Yan, S.Zeng, Z.C.Li, J.C.Liu, X.Liu, S.J.Jin, Y.B.Wang, L.Y.Zhang, X.Q.Yu, L.Li, G.Lian, Q.W.Fan, W.P.Liu New determination of the astrophysical 13C(p, γ)14N S(E) factors and reaction rates via the 13C(7Li, 6He)14N reaction NUCLEAR REACTIONS 13C(7Li, 6He), (7Li, 7Li), E=34 MeV; measured reaction products using Q3D magnetic spectrometer; deduced astrophysical S-factor, σ(θ), spectroscopic factors, potential parameters, resonance parameters; calculated spectroscopic factors, reaction rates using DWBA code PTOLEMY. Comparison with other data.
doi: 10.1140/epja/i2012-12013-x
2012LI35 Chin.Phys.C 36, 716 (2012) X.Liu, Y.-B.Wang, Z.-H.Li, S.-J.Jin, B.-X.Wang, Y.-J.Li, E.-T.Li, X.-X.Bai, B.Guo, J.Su, S.Zeng, S.-Q.Yan, G.Lian, W.-Z.Huang, W.-P.Liu Angular distribution of 6He+p elastic scattering NUCLEAR REACTIONS 1H(6He, p), E(cm)=4.3 MeV; measured reaction products, Ep, Ip. 6He; deduced σ(θ), optical potential parameters. DWBA calculations, comparison with available data.
doi: 10.1088/1674-1137/36/8/006
2011LI18 Chin.Phys.Lett. 28, 052102 (2011) E.-T.Li, Z.-H.Li, J.Su, B.Guo, Y.-J.Li, S.-Q.Yan, X.-X.Bai, Y.-B.Wang, B.-X.Wang, G.Lian, S.Zeng, X.Fang, W.-J.Zhao, W.-P.Liu Astrophysical Rates for the 6He(p, γ)7Li Reaction NUCLEAR REACTIONS 1H(6He, γ), 2H(6He, n), E(cm)=9.1 MeV; measured reaction products; deduced σ(θ), S-factors, temperature-dependent reaction rates. Comparison with DWBA analysis, REACLIB library.
doi: 10.1088/0256-307X/
2011LI45 Int.J.Mod.Phys. E20, 2351 (2011) C.Liu, S.Y.Wang, B.Qi, D.P.Sun, C.J.Xu, L.Lu, B.Wang, X.C.Shen, M.R.Qin, H.Chen, L.H.Zhu, X.G.Wu, G.S.Li, C.Y.He, Y.Zheng, L.L.Wang, B.Zhang, G.Y.Liu, Y.W.Wang Configuration assignment of the positive-parity structures in 108Ag NUCLEAR REACTIONS 104Ru(7Li, 3n), E=33 MeV; measured reaction products, Eγ, Iγ; deduced high-spin band structure, level energies, J, π, B(M1)/B(E2) ratios. Comparison with cranked shell model and deformed Woods-Saxon potential calculations.
doi: 10.1142/S0218301311020368
2011LI55 J.Phys.:Conf.Ser. 312, 042013 (2011) W.P.Liu, Z.H.Li, B.Guo, Y.B.Wang, J.Su, X.X.Bai, G.Lian, B.X.Wang, S.Q.Yan, S.Zeng, Y.J.Li, E.T.Li, S.J.Jin, X.Liu Current progress of nuclear astrophysical reaction and decay study at CIAE NUCLEAR REACTIONS 2H(12N, 13O), E(cm)=8.4 MeV; measured reaction products using telescope with ΔE silicon and double-sided silicon strip detector and PPAC; deduced σ(θ); calculated σ(θ) using optical potential plus CN contribution. 7Li(6Li, 7Li), E(cm)=0.02-0.07 MeV; measured reaction products; deduced 6Li(n, γ) σ using spectroscopic factor. RADIOACTIVITY 147Sm(α)[in metal Sm and Sm2O3]; measured Eα, Iα; deduced T1/2.
doi: 10.1088/1742-6596/312/4/042013
2011WA02 Phys.Rev. C 83, 018801 (2011) B.Wang, C.A.Bertulani, A.B.Balantekin Electron screening and its effects on big-bang nucleosynthesis
doi: 10.1103/PhysRevC.83.018801
2010HA15 J.Korean Phys.Soc. 57, 40 (2010) I.Hahn, A.Kim, N.H.Lee, J.S.Yoo, M.H.Han, S.Kubono, H.Yamaguchi, S.Hayakawa, Y.Wakabayashi, D.Binh, H.Hashimoto, T.Kawabata, D.Kahl, Y.Kurihara, Y.K.Kwon, T.Teranishi, S.Kato, T.Komatsubara, B.Guo, B.Wang, Y.Yang, W.Liu Direct Measurement of the 140(α, α)14O Cross Section for Astrophysically Important 14O + α Resonances NUCLEAR REACTIONS 4He(14O, α), E=24, 35 MeV; 18Ne; measured reaction products; deduced 18Ne resonance parameters, σ(θ).
doi: 10.3938/jkps.57.40
2010JI02 Chin.Phys.Lett. 27, 032102 (2010) S.-J.Jin, Y.-B.Wang, B.-X.Wang, X.-X.Bai, X.Fang, B.Guo, E.-T.Li, Y.-J.Li, Z.-H.Li, G.Lian, J.Su, s.-Q.Yan, S.Zeng, Z.-E.Yao, W.-P.Liu Excited States in 18Ne Studied via 17F+p NUCLEAR REACTIONS 1H(17F, α), (17F, γ), E=55.5 MeV; measured recoil nuclei, Eα, Iα; deduced σ(θ), excitation function, 18Ne resonance states, J, π.
doi: 10.1088/0256-307X/27/3/032102
2010LI19 Eur.Phys.J. A 44, 1 (2010) Z.H.Li, E.T.Li, B.Guo, X.X.Bai, Y.J.Li, S.Q.Yan, Y.B.Wang, G.Lian, J.Su, B.X.Wang, S.Zeng, X.Fang, W.P.Liu First measurement of the 2H(6He, 7Li)n angular distribution and proton spectroscopic factor in 7Li NUCLEAR REACTIONS 2H(7Li, 6He)n, E=46 MeV; measured reaction products; deduced σ(θ), proton spectroscopic factor of 7Li ground state, optical potential parameters. Comparison with DWBA calculations.
doi: 10.1140/epja/i2010-10944-8
2010LI37 Nucl.Phys. A834, 651c (2010) W.P.Liu, Z.H.Li, X.X.Bai, Y.B.Wang, G.Lian, B.Guo, J.Su, S.Zeng, B.X.Wang, S.Q.Yan, Y.J.Li, E.T.Li Lithium induced nuclear reactions of astrophysical interest NUCLEAR REACTIONS 7Li(6Li, 7Li), E=tandem; measured E(particle), I(particle, θ); deduced spectroscopic factor, σ. 6Li(n, γ), E=0.01-0.1 MeV; deduced σ. Comparison with other data and systems, calculations.
doi: 10.1016/j.nuclphysa.2010.01.114
2010LI38 Nucl.Phys. A834, 661c (2010) Z.H.Li, J.Su, B.Guo, E.T.Li, Z.C.Li, X.X.Bai, Y.J.Li, J.C.Liu, S.Q.Yan, B.X.Wang, Y.B.Wang, G.Lian, S.Zeng, X.Fang, W.P.Liu, Y.S.Chen, N.C.Shu, Q.W.Fan 2H(6He, 7Li)n, 12C(7Li, 6He)13N reactions and 12C(p, γ)13N astrophysical S(E) factors NUCLEAR REACTIONS 2H(6He, 7Li), E not given; 12C(7Li, 6He), E=44.0 MeV; measured σ(θ); deduced 12C(p, γ) S-factor; calculated S-factor using DWBA and asymptotic normalization coefficient. Comparison with other data.
doi: 10.1016/j.nuclphysa.2010.01.117
2010SU08 Chin.Phys.Lett. 27, 052101 (2010) J.Su, Z.-H.Li, B.Guo, X.-X.Bai, Z.-C.Li, J.-C.Liu, Y.-B.Wang, G.Lian, S.Zeng, B.-X.Wang, S.-Q.Yan, Y.-J.Li, E.-T.Li, Q.-W.Fan, W.-P.Liu Neutron Spectroscopic Factors of 7Li and Astrophysical 6Li(n, γ)7Li Reaction Rates NUCLEAR REACTIONS 7Li(6Li, 7Li), (6Li, 6Li), E=23.7 MeV; measured reaction products; deduced σ(θ), spectroscopic factors. NUCLEAR REACTIONS 6Li(p, γ), (n, γ), E(cm)<1.2 MeV; calculated astrophysical reaction rates, S-factors. DWBA analysis.
doi: 10.1088/0256-307X/27/5/052101
2010SU30 Eur.Phys.J. A 46, 69 (2010) J.Su, Z.H.Li, L.C.Zhu, G.Lian, X.X.Bai, Y.B.Wang, B.Guo, B.X.Wang, S.Q.Yan, S.Zeng, Y.J.Li, E.T.Li, S.J.Jin, X.Liu, Q.W.Fan, J.L.Zhang, X.Y.Jiang, J.X.Lu, X.F.Lan, X.Z.Tang, W.P.Liu Alpha decay half-life of 147Sm in metal samarium and Sm2O3 RADIOACTIVITY 147Sm(α); measured Eα, Iα for metalic Sm and Sm oxide; deduced T1/2. Halflives in both forms are different.
doi: 10.1140/epja/i2010-11028-7
2010WA18 Nucl.Phys. A834, 100c (2010) Y.B.Wang, B.X.Wang, S.J.Jin, X.Qin, X.X.Bai, W.P.Liu, Z.H.Li, G.Lian, S.Zeng, B.Guo, S.Q.Yan, J.Su, Y.J.Li, E.T.Li, X.Fang Elastic resonance scattering of 13N+p and 17F+p NUCLEAR REACTIONS 2H(12C, 13N), (16O, 17F), E not given; 1H(13N, 13N), (17F, 17F), E=47.8 MeV; measured reaction products, proton spectrum; 14O, 18Ne; deduced resonance parameters, J, π, σ(θ); R-matrix analysis.
doi: 10.1016/j.nuclphysa.2010.01.030
2009HU07 Appl.Radiat.Isot. 67, 1541 (2009) Evaluation of 235U decay data COMPILATION 235U; compiled, evaluated decay data.
doi: 10.1016/j.apradiso.2009.02.092
2009LI27 Chin.Phys.Lett. 26, 072401 (2009) E.-T.Li, Z.-H.Li, Y.-J.Li, S.-Q.Yan, X.-X.Bai, B.Guo, J.Su, Y.-B.Wang, B.-X.Wang, G.Lian, S.Zeng, X.Fang, W.-J.Zhao, W.-P.Liu Angular Distribution of the 12C(6He, 7Li)11B Reaction NUCLEAR REACTIONS 12C(6He, 7Li), E = 34.6 MeV; measured σ(θ). comparison with DWBA calculation.
doi: 10.1088/0256-307X/26/7/072401
2009LI40 Phys.Rev. C 80, 034909 (2009) X.-y.Li, X.-f.Lu, B.Wang, W.-m.Sun, H.-s.Zong Properties of cold dense nuclear matter based on a nonperturbative approach inspired by chiral perturbation theory
doi: 10.1103/PhysRevC.80.034909
2009WA25 Chin.Phys.C 33, 181 (2009) Y.-B.Wang, X.Qin, B.-X.Wang, W.-P.Liu, Z.-H.Li, X.-X.Bai, G.Lian, B.Guo, S.Zeng, J.Su, Y.-J.Li, C.Jiang Simulation and analysis of 13N+p elastic resonance scattering NUCLEAR REACTIONS 1H(13N, p), E=47.8 MeV; measured reaction products; 14O; deduced σ, resonance parameters, J, π. Monte-Carlo simulations.
doi: 10.1088/1674-1137/33/3/004
2008HA14 Nucl.Phys. A804, 125 (2008) O.Hashimoto, S.N.Nakamura, A.Acha, A.Ahmidouch, D.Androic, A.Asaturyan, R.Asaturyan, O.K.Baker, P.Baturin, F.Benmokhtar, P.Bosted, R.Carlini, X.Chen, M.Christy, L.Cole, S.Danagoulian, A.Daniel, V.Dharmawardane, K.Egiyan, M.Elaasar, R.Ent, H.Fenker, Y.Fujii, M.Furic, L.Gan, D.Gaskell, A.Gasparian, E.F.Gibson, P.Gueye, R.Halkyard, D.Honda, T.Horn, B.Hu, S.Hu, Ed.V.Hungerford, M.Ispiryan, K.Johnston, M.Jones, N.Kalantarians, M.Kaneta, F.Kato, S.Kato, D.Kawama, C.Keppel, Y.Li, W.Luo, D.Mack, A.Margaryan, G.Marikyan, N.Maruyama, A.Matsumura, T.Miyoshi, A.Mkrtchyan, H.Mkrtchyan, T.Navasardyan, G.Niculescu, M.-I.Niculescu, H.Nomura, K.Nonaka, A.Ohtani, Y.Okayasu, P.Pamela, N.Perez, T.Petkovic, S.Randeniya, J.Reinhold, R.Rivera, J.Roche, V.M.Rodriguez, Y.Sato, T.Seva, L.Tang, N.Simicevic, G.Smith, M.Sumihama, Y.Song, V.Tadevosyan, T.Takahashi, H.Tamura, V.Tvaskis, W.Vulcan, B.Wang, S.Wells, S.Wood, C.Yan, L.Yuan, S.Zamkochian Hypernuclear spectroscopy program at JLab Hall C2008.01.029 NUCLEAR REACTIONS 1H, 12C, 28Si(e, e'K+), E=1.8 GeV; measured hypernuclei missing mass spectra using the Tilt method.
doi: 10.1016/j.nuclphysa.2008.01.029
2008LI02 Chin.Phys.Lett. 25, 70 (2008) G.Lian, J.Su, B-X.Wang, C.Jiang, X.-X.Bai, S.Zeng, Y.-N.Zheng, S.-Y.Zhu, L.-H.Zhu, W.-P.Liu, Z.-H.Li, Y.-B.Wang, B.Guo, Y.-J.Li, X.Qin Enhancement of β+-Decay Rate of 22Na in Metal Pd at Low Temperature RADIOACTIVITY 22Na(β+); measured Eγ, Iγ. Deduced evidence for temperature dependence of half life for decays in metallic environment.
doi: 10.1088/0256-307X/25/1/020
2008LI03 Chin.Phys.Lett. 25, 455 (2008) Y.-J.Li, Z.-H.Li, B.Guo, Y.-B.Wang, X.-X.Bai, J.Su, G.Lian, S.Zeng, B.-X.Wang, X.Qin, C.Jiang, W.-P.Liu, W.-J.Zhao Measurement of Angular Distribution for the 8Li(p, d)7Li Reaction NUCLEAR REACTIONS 1H(8Li, 7Li), E=39.8 MeV; measured particle energies and yields. 8Li(p, d), E(cm)=4.0 MeV; deduced cross sections and backward anglular distributions.
doi: 10.1088/0256-307X/25/2/028
2008WA09 Phys.Rev. C 77, 044304 (2008) Y.B.Wang, B.X.Wang, X.Qin, X.X.Bai, B.Guo, C.Jiang, Y.J.Li, Z.H.Li, G.Lian, J.Su, S.Zeng, W.P.Liu 13N + p elastic resonance scattering via a thick-target method NUCLEAR REACTIONS 2H(12C, 13N), E=72 MeV; measured excitation function. 1H(13N, 13N), E=47.8 MeV; measured proton energy, σ(θ). 13N, 14O; deduced levels, J, π, resonance parameters.
doi: 10.1103/PhysRevC.77.044304
2007HU09 Appl.Radiat.Isot. 65, 712 (2007) Evaluation of the 225Ac decay data RADIOACTIVITY 225Ac(α); compiled, analyzed Eγ, Iγ, T1/2. COMPILATION 225Ac; compiled, analyzed α-delayed Eγ, Iγ, T1/2.
doi: 10.1016/j.apradiso.2007.02.001
2007RA22 Eur.Phys.J. A 32, 51 (2007) F.Raiola, T.Spillane, B.Limata, B.Wang, S.Yan, M.Aliotta, H.W.Becker, J.Cruz, M.Fonseca, L.Gialanella, A.P.Jesus, K.U.Kettner, R.Kunze, H.Luis, J.P.Ribeiro, C.Rolfs, M.Romano, D.Schurmann, F.Strieder First hint on a change of the 210Po alpha-decay half-life in the metal Cu RADIOACTIVITY 210Po(α); measured Eα, Iα, T1/2 as a function of temperature by implanting Po ions in cooled metallic copper.
doi: 10.1140/epja/i2007-10012-8
2007WA26 Phys.Rev. C 76, 025201 (2007) B.Wang, H.Chen, L.Chang, Y.Liu Soliton in the global color model with a sophisticated effective gluon propagator
doi: 10.1103/PhysRevC.76.025201
2007WA28 Nucl.Phys. A790, 593c (2007) Baryon structure in the global color symmetry model of QCD
doi: 10.1016/j.nuclphysa.2007.03.100
2006LI34 Eur.Phys.J. A 28, 251 (2006) B.Limata, F.Raiola, B.Wang, S.Yan, H.W.Becker, A.D'Onofrio, L.Gialanella, V.Roca, C.Rolfs, M.Romano, D.Schurmann, F.Strieder, F.Terrasi First hints on a change of the 22Na β+-decay half-life in the metal Pd RADIOACTIVITY 22Na(β+) [from 19F(α, n)]; measured T1/2 for source implanted in Pd metal; deduced shorter T1/2 due to environmental effects.
doi: 10.1140/epja/i2006-10057-1
2006LI48 Phys.Rev. C 74, 035801 (2006) Z.H.Li, B.Guo, S.Q.Yan, G.Lian, X.X.Bai, Y.B.Wang, S.Zeng, J.Su, B.X.Wang, W.P.Liu, N.C.Shu, Y.S.Chen, H.W.Chang, L.Y.Jiang 13N(d, n)14O reaction and the astrophysical 13N(p, γ)14O reaction rate NUCLEAR REACTIONS 2H(13N, n), E(cm)=8.9 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 13N(p, γ), E(cm)=0-1.0 MeV; deduced astrophysical S-factors, reaction rate.
doi: 10.1103/PhysRevC.74.035801
2006LI62 Int.J.Mod.Phys. E15, 1899 (2006) W.-P.Liu, Z.-H.Li, X.-X.Bai, Y.-B.Wang, G.Lian, B.Guo, S.Zeng, S.-Q.Yan, B.-X.Wang, J.Su, N.-C.Shu, Y.-S.Chen Indirect measurements of nuclear astrophysics reactions using unstable nuclear beams NUCLEAR REACTIONS 2H(7Be, n), (11C, n), (8Li, p), (13N, n), E(cm) ≈ 6-9 MeV; analyzed σ, asymptotic normalization coefficients. 7Be, 11C, 8Li, 13N(p, γ), E=low; deduced astrophysical S-factors, reaction rates.
doi: 10.1142/S0218301306005514
2006SU01 Chin.Phys.Lett. 23, 55 (2006) J.Su, Z.-H.Li, B.Guo, W.-P.Liu, X.-X.Bai, S.Zeng, G.Lian, S.-Q.Yan, B.-X.Wang, Y.-B.Wang Astrophysical Reaction Rates of the 8Li(p, g)9Beg.s Direct Capture Reaction NUCLEAR REACTIONS 2H(8Li, n), E=40 MeV; measured σ(θ); deduced optical potential parameters. 8Li(p, γ), E(cm) ≈ 0-2 MeV; deduced astrophysical S-factors, reaction rates.
doi: 10.1088/0256-307X/23/1/017
2006WA04 Phys.Rev. C 73, 015206 (2006) B.Wang, H.Song, L.Chang, H.Chen, Yu.Liu Soliton with a pion field in the global color symmetry model
doi: 10.1103/PhysRevC.73.015206
2006WA21 Eur.Phys.J. A 28, 375 (2006) B.Wang, S.Yan, B.Limata, F.Raiola, M.Aliotta, H.W.Becker, J.Cruz, N.De Cesare, A.D'Onofrio, Z.Fulop, L.Gialanella, G.Gyurky, G.Imbriani, A.Jesus, J.P.Ribeiro, V.Roca, D.Rogalla, C.Rolfs, M.Romano, D.Schurmann, E.Somorjai, F.Strieder, F.Terrasi Change of the 7Be electron capture half-life in metallic environments RADIOACTIVITY 7Be(EC) [7Li(p, n)]; measured T1/2 for source implanted in Pd, In metals and Li2O insulator; deduced longer T1/2 due to environmental effects in the metals, no change in the insulator.
doi: 10.1140/epja/i2006-10068-x
2005GU29 Nucl.Phys. A761, 162 (2005) B.Guo, Z.H.Li, W.P.Liu, X.X.Bai, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, J.Su, Y.Lu The 8Li(d, p)9Li reaction and astrophysical 8B(p, γ)9C reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E(cm)=7.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 8B(p, γ), E=low; calculated astrophysical S-factor. DWBA analysis, inverse kinematics, comparison with data.
doi: 10.1016/j.nuclphysa.2005.07.013
2005HU06 Appl.Radiat.Isot. 62, 797 (2005) Evaluation of 233Pa decay data RADIOACTIVITY 233Pa(β-); compiled, analyzed Eγ, Iγ, E(ce), I(ce), δ, T1/2; deduced log ft, γ-emission probabilities. 233U deduced levels, β-feeding intensities.
doi: 10.1016/j.apradiso.2004.11.005
2005LI19 Phys.Rev. C 71, 052801 (2005) Z.H.Li, W.P.Liu, X.X.Bai, B.Guo, G.Lian, S.Q.Yan, B.X.Wang, S.Zeng, Y.Lu, J.Su, Y.S.Chen, K.S.Wu, N.C.Shu, T.Kajino The 8Li(d, p)9Li reaction and the astrophysical 8Li(n, γ)9Li reaction rate NUCLEAR REACTIONS 2H(8Li, 9Li), E=39 MeV; measured particle spectra, σ(θ). 8Li(n, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.71.052801
2005LI35 Chin.Phys.Lett. 22, 1870 (2005) Z.H.Li, B.Guo, W.-P.Liu, X.-X.Bai, G.Lian, J.Su, S.-Q.Yan, B.-X.Wang, S.Zeng Radius of 9C from the Asymptotic Normalization Coefficient NUCLEAR REACTIONS 2H(8Li, p), E(cm)=7.8 MeV; measured σ(θ); deduced asymptotic normalization coefficients. 9C deduced radius, density distributions, halo structure.
doi: 10.1088/0256-307X/22/8/013
2005LI40 Nucl.Phys. A758, 110c (2005) W.Liu, Z.Li, X.Bai, G.Lian, B.Guo, S.Zeng, S.Yan, B.Wang, N.Shu, K.Wu, Y.Chen Nuclear Astrophysics Experiments at CIAE NUCLEAR REACTIONS 2H(7Be, n), (11C, n), (8Li, p), E ≈ 5.8-9.8 MeV; measured σ(θ), total σ; deduced astrophysical S-factors.
doi: 10.1016/j.nuclphysa.2005.05.164
2005ZE03 Chin.Phys.Lett. 22, 2219 (2005) S.Zeng, W.-P.Liu, Z.-H.Li, X.-X.Bai, S.-Q.Yan, B.-X.Wang, G.Lian, J.Su Measurement of 2H(8Li, 9Be)n Reaction Relevant to Primordial Nucleosynthesis NUCLEAR REACTIONS 2H(8Li, 9Be), E=40.38 MeV; measured particle spectra, σ(θ); deduced astrophysical S-factors.
doi: 10.1088/0256-307X/22/9/022
2003LI51 Nucl.Phys. A728, 275 (2003) W.Liu, Z.Li, X.Bai, B.Guo, S.Zeng, Y.Chen, S.Yan, B.Wang, G.Lian, Y.Lu, K.Wu, N.Shu Determination of 11C(p, γ) 12N astrophysical S-factor via measurement of 11C(d, n)12N reaction NUCLEAR REACTIONS 2H(11C, 12N), E(cm)=9.8 MeV; measured σ(θ); deduced asymptotic normalization coefficient. 11C(p, γ), E=low; deduced astrophysical S-factor, reaction mechanism features. DWBA analysis.
doi: 10.1016/j.nuclphysa.2003.08.017
1997WA22 Chin.Phys.Lett. 14, 503 (1997) Systematics of β and γ Parameters of O(6)-Like Nuclei in the Interacting Boson Model NUCLEAR STRUCTURE 120,122,124,126,128,130,132Xe, 124,126,128,130,132,134Ba, 126,128,130,132,134,136Ce; calculated quadrupole moments, reduced transition probabilities; deduced proton, neutron boson numbers dependence. Interacting boson model, comparision with collective model.
1996ZH29 Chin.Phys.Lett. 13, 809 (1996) Q.-Y.Zhang, M.Feng, X.-L.Chen, B.-L.Wang Spectra of 230-238U by 1/N Expansion with Consistent Q Framework NUCLEAR STRUCTURE 230,232,234,236,238U; calculated levels, B(E2). Interacting boson model, consistent Q framework, 1/N expansion technique.
doi: 10.1088/0256-307X/13/11/003
1993SU32 Chin.J.Nucl.Phys. 15, No 3, 261 (1993) H.Sun, D.Liang, S.Chen, G.Si, Z.Chen, Y.Mao, Z.Hu, N.Mao, Q.Sun, H.Du, Z.Li, S.Liang, B.Wang, F.Wang, Q.Yang, Z.Mei, C.Ching An Upper Limit for the Electron Anti-Neutrino Mass RADIOACTIVITY 3H(β-); measured β-endpoint energy; deduced ((ν-bar)(e)), mass upper limit. Double focusing magnetic spectrometer.
1989SH05 Nucl.Phys. A491, 130 (1989) W.-Q.Shen, B.Wang, J.Feng, W.-L.Zhan, Y.-T.Zhu, E.-P.Feng Total Reaction Cross Section for Heavy-Ion Collisions and Its Relation to the Neutron Excess Degree of Freedom NUCLEAR REACTIONS, ICPND 68Zn, 27Al, 12C(12C, X), 12C(14N, X), 28Si(p, X), 28Si(16O, X), 12C(20Ne, X), 40Ca(16O, X), (40Ca, X), E=high; calculated reaction σ(E).
doi: 10.1016/0375-9474(89)90209-1
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