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NSR database version of April 11, 2024.

Search: Author = B.S.Wang

Found 59 matches.

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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
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2024WA02      Phys.Rev. C 109, 014611 (2024)

B.Wang, Y.Xu, S.Goriely

Systematic study of the radiative proton capture including the compound, pre-equilibrium, and direct mechanisms

doi: 10.1103/PhysRevC.109.014611
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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
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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
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2023MU17      Int.J.Mod.Phys. E32, 2350045 (2023)

Y.-T.Mu, W.-J.Zhao, B.Wang

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
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2023WA36      Phys.Rev. C 108, 065805 (2023)

B.Wang, Y.Xu, X.Tang

Effective energy window of the E1 photon strength function for astrophysical neutron-capture reaction rates

doi: 10.1103/PhysRevC.108.065805
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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
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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
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2022YA22      Eur.Phys.J. A 58, 157 (2022)

J.-M.Yang, W.-J.Zhao, B.Wang

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
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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
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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
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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
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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
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2021WA20      Phys.Rev. C 103, 034605 (2021)

B.Wang, Z.-Y.Yue, W.-J.Zhao

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14632. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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2020ME07      Phys.Rev. C 101, 064002 (2020)

L.Meng, B.Wang, S.-L.Zhu

ΣcN interaction in chiral effective field theory

doi: 10.1103/PhysRevC.101.064002
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14685. Data from this article have been entered in the XUNDL database. For more information, click here.


2020WA05      Phys.Rev. C 101, 024606 (2020)

B.Wang, Z.Ren, D.Bai

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2009HU07      Appl.Radiat.Isot. 67, 1541 (2009)

X.Huang, B.Wang

Evaluation of 235U decay data

COMPILATION 235U; compiled, evaluated decay data.

doi: 10.1016/j.apradiso.2009.02.092
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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
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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
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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
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2007HU09      Appl.Radiat.Isot. 65, 712 (2007)

X.Huang, B.Wang

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
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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
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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
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2007WA28      Nucl.Phys. A790, 593c (2007)

B.Wang, Y.-x.Liu

Baryon structure in the global color symmetry model of QCD

doi: 10.1016/j.nuclphysa.2007.03.100
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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
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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
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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
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2005HU06      Appl.Radiat.Isot. 62, 797 (2005)

X.Huang, P.Liu, B.Wang

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
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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
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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
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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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