NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = W.Wang Found 72 matches. 2024YA08 Phys.Rev.Lett. 132, 152502 (2024) X.Yan, Zh.Cheng, A.Abdukerim, Z.Bo, W.Chen, X.Chen, Ch.Cheng, X.Cui, Y.Fan, D.Fang, Ch.Fu, M.Fu, L.Geng, K.Giboni, L.Gu, X.Guo, Ch.Han, K.Han, Ch.He, J.He, D.Huang, Y.Huang, J.Huang, Zh.Huang, R.Hou, Y.Hou, X.Ji, Y.Ju, Ch.Li, J.Li, M.Li, Sh.Li, T.Li, Q.Lin, J.Liu, X.Lu, C.Lu, L.Luo, Y.Luo, W.Ma, Y.Ma, Y.Mao, Y.Meng, X.Ning, B.Pang, N.Qi, Zh.Qian, X.Ren, N.Shaheed, X.Shang, X.Shao, G.Shen, L.Si, W.Sun, A.Tan, Y.Tao, A.Wang, M.Wang, Q.Wang, Sh.Wang, S.Wang, W.Wang, X.Wang, Zh.Wang, Y.Wei, M.Wu, W.Wu, J.Xia, M.Xiao, X.Xiao, P.Xie, B.Yan, J.Yang, Y.Yang, Y.Yao, Ch.Yu, Y.Yuan, Zh.Yuan, X.Zeng, D.Zhang, M.Zhang, P.Zhang, Sh.Zhang, Sh.Zhang, T.Zhang, W.Zhang, Y.Zhang, Y.Zhang, Y.Zhang, L.Zhao, Q.Zheng, J.Zhou, N.Zhou, X.Zhou, Y.Zhou, Y.Zhou, for the PandaX Collaboration Searching for Two-Neutrino and Neutrinoless Double Beta Decay of 134Xe with the PandaX-4T Experiment RADIOACTIVITY 134Xe(2β-); measured decay products, Eβ, Iβ; deduced two-neutrino and neutrinoless T1/2 limits. Comparison with available data. The cylindrical active volume PandaX-4T dual-phase TPC.
doi: 10.1103/PhysRevLett.132.152502
2023MA04 Phys.Rev. C 107, 014310 (2023) N.-N.Ma, Ti.-L.Zhao, W.-Xi.Wang, H.-F.Zhang Simple deep-learning approach for α-decay half-life studies RADIOACTIVITY N=90-180(α); A=160-320(α); Z=80-120(α); calculated T1/2. The deep learning algorithm trained directly with sets of experimental α-decay half-lives.
doi: 10.1103/PhysRevC.107.014310
2023WA17 Phys.Lett. B 843, 138034 (2023) W.Wang, C.Lv, X.Zhang, C.Fu, B.Guo, H.Cai, L.Chen, L.Cheng, C.He, J.He, L.Li, X.Xi, D.Yuan, G.Zhang, W.Sun, Z.Zhang, J.Zhang, Y.Ma First measurement of the 7Li(D, n) astrophysical S-factor in laser-induced full plasma NUCLEAR REACTIONS 7Li(d, n), E(cm)<0.7 MeV; measured reaction products, En, In; deduced neutron yields, neutron groups, astrophysical S-factor. The Shenguang-II laser facility, the National Laboratory on High Power Lasers and Physics, Shanghai, China.
doi: 10.1016/j.physletb.2023.138034
2022FE02 Phys.Rev.Lett. 128, O52501 (2022) J.Feng, W.Wang, C.Fu, L.Chen, J.Tan, Y.Li, J.Wang, Y.Li, G.Zhang, Y.Ma, J.Zhang Femtosecond Pumping of Nuclear Isomeric States by the Coulomb Collision of Ions with Quivering Electrons RADIOACTIVITY 83Kr(IT); measured decay products, X-rays; deduced T1/2. Femtosecond pumping of nuclear isomeric states by the Coulomb excitation of ions with the quivering electrons induced by laser fields.
doi: 10.1103/PhysRevLett.128.052501
2022HU06 Phys.Lett. B 831, 137183 (2022) H.Hu, W.-L.Guo, J.Su, W.Wang, C.Yuan Implementation of residual nucleus de-excitations associated with proton decays in 12C based on the GENIE generator and TALYS code RADIOACTIVITY 12C(p); analyzed available dat. 11B, 10B, 10Be; calculated de-excitation processes of residual nuclei associated with proton decays in based on the GENIE generator and TALYS code.
doi: 10.1016/j.physletb.2022.137183
2022LI57 Phys.Rev. C 106, 044601 (2022) J.-X.Li, W.-X.Wang, H.-F.Zhang Properties and synthesis of the superheavy nucleus 298114Fl NUCLEAR REACTIONS 238U(64Ti, X), E*=32-60 MeV;242Pu(48Ca, X), E*=25-60 MeV; calculated capture σ(E), fusion probabilities, fusion barrier, potential-energy surfaces, survival probabilities in the 4n channels. 238U(64Ti, 4n)298Fl, E*=33-60 MeV; 242Pu, 244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=30-60 MeV; calculated evaporation residue σ(E). Dinuclear system model. Suggested 238U(64Ti, 4n) at 43 MeV excitation energy as preferred way for the synthesis of 298Fl. Comparison with available experimental data. NUCLEAR STRUCTURE 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304Fl, 292HS, 293Mt, 294Ds, 295Rg, 296Cn, 297Nh, 299Mc, 300Lv, 301Ts, 302Og, 303119, 304120; calculated S(n), S(2n). Finite-range droplet model (FRDM2012). Discuss the evidence that 298Fl could be spherical double-magic nucleus and also the center of the stability island of superheavy nuclei. RADIOACTIVITY 284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304Fl, 292HS, 293Mt, 294Ds, 295Rg, 296Cn, 297Nh, 299Mc, 300Lv, 301Ts, 302Og, 303119, 304120(α), (SF); calculated Q-value, T1/2. Finite-range droplet model (FRDM2012).
doi: 10.1103/PhysRevC.106.044601
2022XI05 Nucl.Phys. A1023, 122443 (2022) Y.-Z.Xing, W.-X.Wang, H.-F.Zhang, Y.-M.Zheng General chaotic behaviors of heavy ion collisions at intermediate energy based on dynamical transport model NUCLEAR REACTIONS 40Ca(40Ca, X), E=800 MeV/nucleon; analyzed available data; deduced the multifragmentation entropy, information dimension and the dynamical fluctuations of fragment mass distribution in the final state of the reaction.
doi: 10.1016/j.nuclphysa.2022.122443
2022ZH61 Phys.Rev. C 106, 044604 (2022) Nuclear excitation cross section of 229Th via inelastic electron scattering NUCLEAR REACTIONS 229Th(e, e'), E<1 GeV; calculated σ(E) of the isomeric 1+ state excitation, contributions from the E2 or the M1 channels to the σ(E). Dirac distorted wave Born approximation (DWBA) calculations. Calculations show that inelastic scattering at energies below 100 eV is most efficient for the isomer excitation.
doi: 10.1103/PhysRevC.106.044604
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
2021SH26 Eur.Phys.J. A 57, 237 (2021) Hidden charm pentaquark states in a diquark model
doi: 10.1140/epja/s10050-021-00542-4
2021WA37 Phys.Rev.Lett. 127, 052501 (2021) Exciting the Isomeric 229Th Nuclear State via Laser-Driven Electron Recollision RADIOACTIVITY 229Th(IT); analyzed available data; calculated isomeric excitation probability for a laser-driven electron recollision process.
doi: 10.1103/PhysRevLett.127.052501
2021WA56 J.Phys.(London) B54, 244001 (2021) Strong-field atomic physics meets 229Th nuclear physics RADIOACTIVITY 229Th(IT); analyzed available data; calculated electronic excitation σ, flux density of the recolliding electron, ionization probabilities, nuclear isomeric excitation probabilities. Recollision-induced nuclear excitation (RINE).
doi: 10.1088/1361-6455/ac45ce
2020DU15 Nucl.Instrum.Methods Phys.Res. B483, 1 (2020) Y.Duan, W.Ding, W.Wang, W.Zhang, L.Shi Differential cross-section for the T(12C, T)12C elastic recoil reaction NUCLEAR REACTIONS 3H(12C, 12C), E=5.2-12.2 MeV; measured reaction products; deduced σ(θ). Comparison with available data.
doi: 10.1016/j.nimb.2020.10.001
2020GA34 J.Phys.(London) G47, 045108 (2020) J.Galan, X.Chen, H.Du, C.Fu, K.Giboni, F.Giuliani, K.Han, B.Jiang, X.Ji, H.Lin, Y.Lin, J.Liu, K.Ni, X.Ren, S.Wang, S.Wu, C.Xie, Y.Yang, T.Zhang, L.Zhao, S.Aune, Y.Bedfer, E.Berthoumieux, D.Calvet, N.d'Hose, E.Ferrer-Ribas, F.Kunne, B.Manier, D.Neyret, T.Papaevangelou, L.Chen, S.Hu, P.Li, X.Li, H.Zhang, M.Zhao, J.Zhou, Y.Mao, H.Qiao, S.Wang, Y.Yuan, M.Wang, Y.Chen, A.N.Khan, J.Tang, W.Wang, H.Chen, C.Feng, J.Liu, S.Liu, X.Wang, D.Zhu, J.F.Castel, S.Cebrian, T.Dafni, I.G.Irastorza, G.Luzon, H.Mirallas, X.Sun, A.Tan, W.Haxton, Y.Mei, C.Kobdaj, Y.Yan Topological background discrimination in the PandaX-III neutrinoless double beta decay experiment
doi: 10.1088/1361-6471/ab4dbe
2020WA01 Astrophys.J. 889, 169 (2020) W.Wang, T.Siegert, Z.G.Dai, R.Diehl, J.Greiner, A.Heger, M.Krause, M.Lang, M.M.M.Pleintinger, X.L.Zhang Gamma-Ray Emission of 60Fe and 26Al Radioactivity in Our Galaxy RADIOACTIVITY 26Al(EC), 60Fe(β-); measured decay products, Eγ, Iγ; deduced γ-ray flux and ratio from nucleosynthesis in the Galaxy.
doi: 10.3847/1538-4357/ab6336
2020WA20 Phys.Rev. C 102, 015203 (2020) A.-C.Wang, F.Huang, W.-L.Wang, G.-X.Peng Photoproduction γp → K*+ Λ in a Reggeized model
doi: 10.1103/PhysRevC.102.015203
2020YA22 Phys.Rev. A 102, 042803 (2020) B.Yang, D.Yu, C.Shao, Y.S.Kozhedub, Y.Xue, W.Wang, M.Zhang, J.Liu, Z.Song, R.Lu, F.Ruan, Y.Wu, X.Cai Alignment of the projectile 2p3/2 state created by nonradiative electron capture in 95- and 146-MeV/u Xe 54+ with Kr and Xe collisions NUCLEAR REACTIONS Kr(Xe, X), E=95, 146 MeV/nucleon; measured reaction products, X-rays; deduced X-ray spectra, angular distributions of Lymann-α transitions, electron capture.
doi: 10.1103/PhysRevA.102.042803
2019AS01 Nucl.Instrum.Methods Phys.Res. A922, 287 (2019) J.Ashenfelter, A.B.Balantekin, C.Baldenegro, H.R.Band, C.D.Bass, D.E.Bergeron, D.Berish, L.J.Bignell, N.S.Bowden, J.Boyle, J.Bricco, J.P.Brodsky, C.D.Bryan, A.B.Telles, J.J.Cherwinka, T.Classen, K.Commeford, A.J.Conant, A.A.Cox, D.Davee, D.Dean, G.Deichert, M.V.Diwan, M.J.Dolinski, A.Erickson, M.Febbraro, B.T.Foust, J.K.Gaison, A.Galindo-Uribarri, C.E.Gilbert, K.E.Gilje, A.Glenn, B.W.Goddard, B.T.Hackett, K.Han, S.Hans, A.B.Hansell, K.M.Heeger, B.Heffron, J.Insler, D.E.Jaffe, X.Ji, D.C.Jones, K.Koehler, O.Kyzylova, C.E.Lane, T.J.Langford, J.LaRosa, B.R.Littlejohn, F.Lopez, X.Lu, D.A.Martinez Caicedo, J.T.Matta, R.D.McKeown, M.P.Mendenhall, H.J.Miller, J.M.Minock, P.E.Mueller, H.P.Mumm, J.Napolitano, R.Neilson, J.A.Nikkel, D.Norcini, S.Nour, D.A.Pushin, X.Qian, E.Romero-Romero, R.Rosero, D.Sarenac, B.S.Seilhan, R.Sharma, P.T.Surukuchi, C.Trinh, M.A.Tyra, R.L.Varner, B.Viren, J.M.Wagner, W.Wang, B.White, C.White, J.Wilhelmi, T.Wise, H.Yao, M.Yeh, Y.-R.Yen, A.Zhang, C.Zhang, X.Zhang, M.Zhao The PROSPECT reactor antineutrino experiment
doi: 10.1016/j.nima.2018.12.079
2018CA07 Nucl.Data Sheets 148, 143 (2018), Erratum Nucl.Data Sheets 163, 280 (2020) A.D.Carlson, V.G.Pronyaev, R.Capote, G.M.Hale, Z.-P.Chen, I.Duran, F.-J.Hambsch, S.Kunieda, W.Mannhart, B.Marcinkevicius, R.O.Nelson, D.Neudecker, G.Noguere, M.Paris, S.P.Simakov, P.Schillebeeckx, D.L.Smith, X.Tao, A.Trkov, A.Wallner, W.Wang Evaluation of the Neutron Data Standards NUCLEAR REACTIONS H, C(n, n), 6Li(n, t), 10B(n, αγ), 197Au(n, γ), 235,238U, 239Pu(n, F), 238U(n, γ), E<20 MeV; analyzed available data; deduced σ and Maxwellian spectrum averaged cross section for the 197Au(n, γ) σ at 30 keV, covariance matrices of the uncertainties. RADIOACTIVITY 252Cf(SF); analyzed available data; deduced spontaneous fission neutron spectrum.
doi: 10.1016/j.nds.2018.02.002
2018WA17 Phys.Rev. C 98, 015801 (2018) W.-H.Wang, X.-P.Zheng, X.Huang, K.Tian Recursion relations connecting the net reaction rate with the total emissivity of neutrinos in nonequilibrium β processes
doi: 10.1103/PhysRevC.98.015801
2018WA30 Phys.Rev. C 98, 045209 (2018) Effects of Δ (1905) 5/2+ on K*Σ photoproduction NUCLEAR REACTIONS 1H(γ, Κ+Σ0), E=1850-3750 MeV; 1H(γ, Κ0Σ+), E=1750-2450 MeV; calculated differential σ(θ), and total σ for resonances with individual contributions from exchanges, and target nucleon asymmetries using an effective Lagrangian approach at the tree-level Born approximation. Comparison with experimental data from CLAS Collaboration.
doi: 10.1103/PhysRevC.98.045209
2017WA21 Phys.Rev. C 95, 065802 (2017) W.-H.Wang, X.Huang, X.-P.Zheng Net reaction rate and neutrino emissivity for the Urca process in departure from chemical equilibrium RADIOACTIVITY 81Se, 49Sc, 65Ni, 55Cr, 69Cu, 57Mn, 55Cr, 67Ni, 63Co, 25Na, 81As, 73Zn, 79Ge, 23Ne, 101Nb, 57Cr(β-); analyzed departures from chemical equilibrium in 15 strongest ocean Urca pairs in accreting neutron stars: 81Br-81Se, 49Ti-49Sc, 65Cu-65Ni, 55Mn-55Cr, 69Zn-69Cu, 57Fe*-57Mn, 67Cu-67Ni, 63Ni*-63Co, 25Mg-25Na, 81Se-81As, 73Ga-73Zn, 79As-79Ge, 23Na-23Ne, 101Mo*-101Nb and 57Mn-57Cr. Calculated net reaction rates and neutrino luminosity. Discussed effect of compression on Urca shells in the ocean and crust of accreting neutron stars.
doi: 10.1103/PhysRevC.95.065802
2017WA34 Phys.Rev. C 96, 035206 (2017) A.C.Wang, W.L.Wang, F.Huang, H.Haberzettl, K.Nakayama Nucleon resonances in γp → K*+Λ NUCLEAR REACTIONS 1H(γ, K*+Λ), E=1850-3850 MeV; analyzed high-precision differential σ(θ, E) data from the CLAS Collaboration at Jefferson National Accelerator facility using effective Lagrangian approach in the tree-level approximation; deduced model parameters in five different fits, total σ(E), and photon beam asymmetry.
doi: 10.1103/PhysRevC.96.035206
2016CH49 Eur.Phys.J. A 52, 310 (2016) D.-Y.Chen, Y.-B.Dong, M.-T.Li, W.-L.Wang Pionic transition from Y(4260) to Zc(3900) in a hadronic molecular scenario
doi: 10.1140/epja/i2016-16310-0
2015CA01 Nucl.Data Sheets 123, 27 (2015) A.D.Carlson, V.G.Pronyaev, R.Capote, G.M.Hale, F.-J.Hambsch, T.Kawano, S.Kunieda, W.Mannhart, R.O.Nelson, D.Neudecker, P.Schillebeeckx, S.Simakov, D.L.Smith, P.Talou, X.Tao, A.Wallner, W.Wang Recent Work Leading Towards a New Evaluation of the Neutron Standards NUCLEAR REACTIONS H, C(n, n), 3He(n, p), 6Li(n, t), 10B(n, α), (n, αγ), Au(n, γ), 235,238U(n, F), E<20 MeV; analyzed available data; deduced neutron σ standards.
doi: 10.1016/j.nds.2014.12.006
2015ZH41 Phys.Rev. C 92, 054616 (2015) Q.Z.Zhao, X.M.Wang, W.Wang, M.He, K.J.Dong, C.J.Xiao, X.D.Ruan, H.T.Shen, S.Y.Wu, X.R.Yang, L.Dou, Y.N.Xu, L.Cai, F.F.Pang, H.Zhang, Y.J.Pang, S.Jiang Determination of the α-decay half-life of 210Po based on film and slice bismuth samples at room temperature RADIOACTIVITY 210Po(α)[from 209Po(n, γ), E=thermal]; measured Eα, Iα, T1/2 for a film sample of Bi2O3 and slice sample of Bi metal; deduced no difference in T1/2 using samples with two different physical configurations. Comparison with the recommended value in the ENSDF database.
doi: 10.1103/PhysRevC.92.054616
2014LI07 Phys.Rev. C 89, 034627 (2014) Y.-J.Liang, M.Zhu, Z.-H.Liu, W.-Z.Wang Role of the "window" component of the friction tensor in the formation of superheavy nuclei NUCLEAR REACTIONS 132Xe(132Xe, n), (132Xe, 2n), (132Xe, 3n), (132Xe, 4n), E=310-355 MeV; 136Xe(136Xe, n), (136Xe, 2n), (136Xe, 3n), (136Xe, 4n), E=308-345 MeV; calculated probability distribution of fusion and injection point, inner barrier height distribution, evaporation residue σ(E) with and without consideration of the "window" term of the friction tensor. Superheavy elements. Discussed synthesis of doubly-magic 270Hs.
doi: 10.1103/PhysRevC.89.034627
2014SA35 Nucl.Data Sheets 118, 38 (2014) M.Salvatores, G.Palmiotti, G.Aliberti, P.Archier, C.De Saint Jean, E.Dupont, M.Herman, M.Ishikawa, T.Ivanova, E.Ivanov, S.-J.Kim, I.Kodeli, G.Manturov, R.McKnight, S.Pelloni, C.Perfetti, A.J.M.Plompen, B.T.Rearden, D.Rochman, K.Sugino, A.Trkov, W.Wang, H.Wu, W.-S.Yang Methods and Issues for the Combined Use of Integral Experiments and Covariance Data: Results of a NEA International Collaborative Study NUCLEAR REACTIONS 238U(n, n'), E=100 eV-10 MeV;239,241Pu(n, F), E=100 eV-10 MeV; calculated relative σ uncertaintites. 239Pu(n, γ), E=100 ev-10 MeV; calculated parameters uncertainty.
doi: 10.1016/j.nds.2014.04.005
2014WA56 Chin.Phys.B 23, 113201 (2014) R.R.Wang, G.Jia, Z.-H.Fang, W.Wang, X.-F.Meng, Z.-Y.Xie, F.Zhang Broadband time-resolved elliptical crystal spectrometer for X-ray spectroscopic measurements in laser-produced plasmas ATOMIC PHYSICS Ti; measured X-rays; deduced temporal variations of Ti K-shell emissions of Ti He-α, He-β, He-γ, Li-α, and Li-β spectra.
doi: 10.1088/1674-1056/23/11/113201
2014YI06 Sci. Rep. 4, 4171 (2014) L.Yi, B.Shen, L.Ji, K.Lotov, A.Sosedkin, X.Zhang, W.Wang, J.Xu, Y.Shi, L.Zhang, Z.Xu Positron acceleration in a hollow plasma channel up to TeV regime
doi: 10.1038/srep04171
2013LI19 Phys.Rev. C 87, 047602 (2013) Y.-J.Liang, M.Zhu, Z.-H.Liu, W.-Z.Wang Nucleon flow in the process of evolution from dinucleus to mononucleus investigated with a dynamic model NUCLEAR REACTIONS 238U(48Ca, 3n), (48Ca, 4n), E(cm)=187-212 MeV; 248Cm(58Fe, 3n), (58Fe, 4n), E(cm)=257 MeV; calculated injection distance distributions, σ(E) of evaporation residues using modified fusion-by-diffusion (FBD) model with coupled Langevin equations in two- and three-dimensional collective space. Nucleon flow from dinucleus to mononucleus. Fusion probability. Mass asymmetry. Comparison with experimental data, and with other theoretical predictions.
doi: 10.1103/PhysRevC.87.047602
2013LU09 Eur.Phys.J. A 49, 58 (2013) C.-D.Lu, U.-G.Meissner, W.Wang, Q.Zhao Hunting for a scalar glueball in exclusive B decays
doi: 10.1140/epja/i2013-13058-y
2013ZH33 Chin.Phys.Lett. 30, 082401 (2013) M.Zhu, J.-L.Fu, Z.Qu, Z.-H.Liu, W.-Z.Wang The Role of Neck Evolution in the Synthesis of Superheavy Element 112 NUCLEAR REACTIONS 238U(48Ca, X)283Cn/282Cn, E(cm)=200 MeV; calculated evaporation residue σ, probability distributions, T1/2. Frozen approximation, comparison with available data.
doi: 10.1088/0256-307X/30/8/082401
2012LI43 Phys.Rev. C 86, 037602 (2012) Y.-J.Liang, M.Zhu, Z.-H.Liu, W.-Z.Wang Theoretical analysis of element 120 synthesized in the 58Fe + 244Pu hot fusion reaction NUCLEAR REACTIONS 244Pu(58Fe, 3n)120299, 244Pu(58Fe, 4n)120298, E*=25-55 MeV; calculated fusion probabilities, σ(E) using modified fusion by diffusion (FBD) model with two-dimensional coupled Langenvin equations. Comparison with previous theoretical studies.
doi: 10.1103/PhysRevC.86.037602
2012LI47 Eur.Phys.J. A 48, 133 (2012) Y.-J.Liang, M.Zhu, Z.-H.Liu, W.-Z.Wang Evolution from dinucleus to mononucleus and its implication in the synthesis of superheavy nuclei NUCLEAR REACTIONS 244Pu(58Fe, X), (58Fe, 3n), (58Fe, 4n), E(cm)=260 MeV; calculated neck formation vs time, ER σ using Langevin equation and frozen approximation.
doi: 10.1140/epja/i2012-12133-3
2011GO30 Nucl.Instrum.Methods Phys.Res. B269, 2745 (2011) J.Gong, C.Li, W.Wang, G.Zheng, H.Hu, M.He, S.Jiang 32Si AMS measurement with ΔE-Q3D method NUCLEAR REACTIONS 31P(n, γ), E=thermal; 32P(n, p), E=fast; calculated yields.
doi: 10.1016/j.nimb.2011.08.026
2011WA18 Phys.Rev. C 84, 015203 (2011) W.L.Wang, F.Huang, Z.Y.Zhang, B.S.Zou ΣcD and ΛcD states in a chiral quark model
doi: 10.1103/PhysRevC.84.015203
2011WA39 Phys.Rev. C 84, 054006 (2011) Dynamical coupled-channels study of K*K-bar* and ωφ states in a chiral quark model
doi: 10.1103/PhysRevC.84.054006
2011WA40 J.Korean Phys.Soc. 59, 1681s (2011) W.M.Wang, X.Li, Z.X.Zhao, Z.Y.Zhou, H.C.Wu, T.F.Wang, G.N.Kim, M.W.Lee, K.S.Kim, M.H.Cho, I.S.Ko, W.Namkung Total Cross-Section Measurements of 169Tm below 100 eV NUCLEAR REACTIONS 169Tm(n, X), E=0.01-100 eV; measured En, In using ToF; deduced σ, transmission coefficients, resonance parameters using R-matrix code SAMMY; calculated, fitted neutron transmission coefficients. Comparison of σ with other data and Mughabghab; resonance parameters with Mughabghab.
doi: 10.3938/jkps.59.1681
2011ZH07 Phys.Rev. C 83, 035801 (2011) D.-R.Zhang, P.-L.Yin, W.Wang, Q.-C.Wang, W.-Z.Jiang Effects of a weakly interacting light U boson on the nuclear equation of state and properties of neutron stars in relativistic models
doi: 10.1103/PhysRevC.83.035801
2010FU13 Int.J.Mod.Phys. E19, 2480 (2010) Y.Fujii, A.Chiba, D.Doi, T.Gogami, O.Hashimoto, H.Kanda, M.Kaneta, D.Kawama, K.Maeda, T.Maruta, A.Matsumura, S.Nagao, S.N.Nakamura, A.Shichijo, H.Tamura, N.Taniya, T.Yamamoto, K.Yokota, S.Kato, Y.Sato, T.Takahashi, H.Noumi, T.Motoba, E.Hiyama, I.Albayrak, O.Ates, C.Chen, M.Christy, C.Keppel, M.Kohl, Y.Li, A.Liyanage, L.Tang, T.Walton, Z.Ye, L.Yuan, L.Zhu, P.Baturin, W.Boeglin, S.Dhamija, P.Markowitz, B.Raue, J.Reinhold, Ed.V.Hungerford, R.Ent, H.Fenker, D.Gaskell, T.Horn, M.Jones, G.Smith, W.Vulcan, S.A.Wood, C.Johnston, N.Simicevic, S.Wells, C.Samanta, B.Hu, J.Shen, W.Wang, X.Zhang, Y.Zhang, J.Feng, Y.Fu, J.Zhou, S.Zhou, Y.Jiang, H.Lu, X.Yan, Y.Ye, L.Gan, A.Ahmidouch, S.Danagoulian, A.Gasparian, M.Elaasar, F.R.Wesselmann, A.Asaturyan, A.Margaryan, A.Mkrtchyan, H.Mkrtchyan, V.Tadevosyan, D.Androic, M.Furic, T.Petkovic, T.Seva, G.Niculescu, I.Niculescu, V.M.Rodriguez Lopez, E.Cisbani, F.Cusanno, F.Garibaldi, G.M.Uuciuoli, R.De Leo, S.Maronne Hypernuclear spectroscopy with electron beam at JLab HALL C NUCLEAR REACTIONS 7Li, 12C, 28Si(E, EK+)7He/12B/28Al, E=1.2 GeV; measured reaction products; deduced hypernuclear spectroscopy, missing mass spectrum.
doi: 10.1142/S0218301310016983
2010LA20 J.Phys.:Conf.Ser. 202, 012032 (2010) M.G.Lang, R.Diehl, W.Wang, P.Martin, R.Voss, K.Kretschmer Observations of cosmic nuclear gamma-ray lines
doi: 10.1088/1742-6596/202/1/012032
2010WA16 Chin.Phys.C 34, 177 (2010) W.-M.Wang, X.Li, Z.-X.Zhao, Z.-Y.Zhou, H.-W.Yu, H.-C.Wu, Y.-X.Wei, T.F.Wang, G.N.Kim, M.W.Lee, K.S.Kim, M.H.Cho, I.S.Ko, W.Namkung Measurement of neutron cross sections and resonance parameters of 169Tm below 100 eV NUCLEAR REACTIONS 169Tm(n, X), E=0.001-100 eV; measured neutron time-of-flight (TOF), En, In; deduced total σ, resonance parameters. Comparison with SAMMY and Atlas of Neutron Resonances.
doi: 10.1088/1674-1137/34/2/004
2009LU19 Phys.Rev. A 80, 051201 (2009) H.Y.Lu, J.S.Liu, C.Wang, W.T.Wang, Z.L.Zhou, A.H.Deng, C.Q.Xia, Y.Xu, X.M.Lu, Y.H.Jiang, Y.X.Leng, X.Y.Liang, G.Q.Ni, R.X.Li, Z.Z.Xu Efficient fusion neutron generation from heteronuclear clusters in intense femtosecond laser fields NUCLEAR REACTIONS 2H(γ, xnyp), E not given; measured densities and average kinetic energies of deuterium ions; deduced fusion neutron yields as a function of laser energy.
doi: 10.1103/PhysRevA.80.051201
2007HU18 Phys.Rev. C 76, 018201 (2007) F.Huang, W.L.Wang, Z.Y.Zhang, Y.W.Yu Preliminary study of the (K-bar) N interaction in a chiral constituent quark model
doi: 10.1103/PhysRevC.76.018201
2007WA36 Eur.Phys.J. A 32, 293 (2007) W.L.Wang, F.Huang, Z.Y.Zhang, Y.W.Yu, F.Liu A possible Ωπ molecular state
doi: 10.1140/epja/i2007-10376-7
2006PE16 Phys.Rev. C 74, 014313 (2006) F.Perrot, F.Marechal, C.Jollet, Ph.Dessagne, J.-C.Angelique, G.Ban, P.Baumann, F.Benrachi, U.Bergmann, C.Borcea, A.Buta, J.Cederkall, S.Courtin, J.-M.Daugas, L.M.Fraile, S.Grevy, A.Jokinen, F.R.Lecolley, E.Lienard, G.Le Scornet, V.Meot, Ch.Miehe, F.Negoita, N.A.Orr, S.Pietri, E.Poirier, M.Ramdhane, O.Roig, I.Stefan, W.Wang β-decay studies of neutron-rich K isotopes RADIOACTIVITY 51,52,53K(β-), (β-n) [from U(p, X)]; measured β-delayed Eγ, En, γγ-, nγ-coin, T1/2; deduced one- and two-neutron emission probabilities. 50,51,52,53Ca deduced transitions, levels.
doi: 10.1103/PhysRevC.74.014313
2005YU03 Chin.Phys.Lett. 22, 1083 (2005) Searching for the Vector-Like Top Quark T at the Future Linac-Ring-Type ep Collider NUCLEAR REACTIONS 1H(e, X), E(cm)=3.7 TeV; calculated vector-like top quark production σ.
doi: 10.1088/0256-307X/22/5/015
2004WA21 J.Phys.(London) G30, S1251 (2004) Recent developments in weak-coupling colour superconductivity
doi: 10.1088/0954-3899/30/8/101
2003YU05 Nucl.Phys. B667, 349 (2003) Top-pions and single top production at the HERA and THERA colliders NUCLEAR REACTIONS 1H(e, X), (e+, X), E(cm)=320, 1000 GeV; calculated top-pion production σ. Topcolor-assisted technicolor models.
doi: 10.1016/S0550-3213(03)00553-4
1998ZH30 Phys.Rev. C58, 2311 (1998) W.N.Zhang, L.Huo, X.J.Chen, W.Wang, Y.M.Liu Multipion Correlations as a Signal for Quark-Gluon Plasma Formation in High Energy Heavy Ion Collisions
doi: 10.1103/PhysRevC.58.2311
1994AL09 J.Phys.(London) G20, 339 (1994) A.M.Al-Harkan, I.S.Batkin, W.W.Wang Optical Bremsstrahlung Accompanying Nuclear Beta Decay RADIOACTIVITY 3H(β-); calculated optical bremsstrahlung photon CP from β-decay; deduced nuclear weak interaction applications.
doi: 10.1088/0954-3899/20/2/011
1988YA04 Chin.J.Nucl.Phys. 10, 166 (1988) Yan Yiming, Zhou Hongyu, Tang Lin, Wen Chenlin, Zhang Shengji, Hua Ming, Ding Xiaoji, Rong Yaning, Liu Shuzhen, Fu Jingquan, Lu Ting, Wang Qi, Sun Suxu, Lan Liqiao, Xu Jinkui, Wang Wanhong, Yang Hua, Han Chongzhan, He Peilun, Ye Wenxiang, Han Xiuqing A Facility for Measurements of γ-Ray Production Cross Sections from (n, xγ) Reactions using the Pulsed Neutron Source NUCLEAR REACTIONS 56Fe(n, n'γ), E=14.9 MeV; measured γγ(t), nγ(t); deduced γ production σ. Pulsed beam. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30904. 1986QI01 Radiat.Eff. 96, 13 (1986) H.-Q.Qi, Y.-C.Liu, Z.-P.Chen, X.-C.Wu, W.-H.Wang, J.Chang The Measurement of Neutron Scattering Cross Sections at Small Angle NUCLEAR REACTIONS Pb(n, n), E=14.7 MeV; measured σ(θ). Position sensitive neutron detector.
1976KI07 Ann.Phys. (New York) 99, 374 (1976) The Isobar-Doorway Theory for Pion-Nucleus Interactions NUCLEAR REACTIONS 12C(π-, π-), (π-, X), E=100-280 MeV; calculated σ(E, θ).
doi: 10.1016/0003-4916(76)90100-7
1975NA07 Phys.Rev. C11, 1167 (1975) M.A.Nagarajan, W.L.Wang, D.J.Ernst, R.M.Thaler Relation between the Watson and Kerman-McManus-Thaler Multiple Scattering Formalisms NUCLEAR REACTIONS 4He, 12C, 40Ca(p, p), E=90, 310, 1050 MeV; calculated σ.
doi: 10.1103/PhysRevC.11.1167
1974WA02 Phys.Rev. C9, 814 (1974) Heavy-Ion Elastic Scattering at High Energies NUCLEAR REACTIONS 4He, 12C, 16O(α, α), (12C, 12C), (16O, 16O), E=2.1 GeV per nucleon; calculated σ(θ).
doi: 10.1103/PhysRevC.9.814
1974WA12 Phys.Rev. C9, 2144 (1974) Angular Distribution and Polarization of 16O(γ, n0)15O NUCLEAR REACTIONS 16O(γ, n), E=21-26 MeV; calculated σ(E, En, θ), deduced giant resonances.
doi: 10.1103/PhysRevC.9.2144
1973KI03 Phys.Rev.Lett. 30, 1071 (1973) Pion-Nucleus Scattering in an Isobar-Doorway Model NUCLEAR REACTIONS 12C(π-, π-); calculated σ(E, θ); isobar-doorway model.
doi: 10.1103/PhysRevLett.30.1071
1973WA03 Phys.Rev.Lett. 30, 301 (1973) Evidence for a Giant Quadrupole Resonance in Oxygen-16 NUCLEAR REACTIONS 16O(γ, n), E < 26 MeV; calculated σ(E;θ(n)), P(n)(E;θ). 16O deduced giant quadrupole resonance structure.
doi: 10.1103/PhysRevLett.30.301
1973YU03 Chin.J.Phys. 11, 1 (1973) Gamma Rays from Thermal Neutron Capture in 128Te RADIOACTIVITY 110Ag, 129Te; measured Eγ, γγ-coin. 110Cd, 129I deduced levels, J, π.
1972HA34 Nucl.Phys. A188, 89 (1972) E.L.Haase, R.Hagelberg, W.N.Wang Investigation of Excited States of 4He Through Deuteron-Induced Three-Particle Reactions on 6Li NUCLEAR REACTIONS 6Li(d, tα), (d, 3Heα), (d, dα), E=52 MeV; measured σ(E, θ). 4He deduced resonance parameters.
doi: 10.1016/0375-9474(72)90184-4
1972LI21 Nuovo Cim. 8A, 801 (1972) Investigation of the 26Mg(d, p)27Mg Reaction below 4 MeV NUCLEAR REACTIONS 26Mg(d, p), E=2-3 MeV; measured σ(E;θ). 27Mg deduced S.
1972WA13 Phys.Rev. C5, 1898 (1972) Intermediate Structure and the Photodisintegration of O16 NUCLEAR REACTIONS 16O(γ, n), (γ, p), E=20-26 MeV; calculated σ(E). 16O; analyzed resonance structure. Projection operator formalism.
doi: 10.1103/PhysRevC.5.1898
1972WA33 Chin.J.Phys.(Taiwan) 10, 1 (1972) Differential Cross Sections for Elastic Scattering of Low-Energy Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), E=1.5-3.0 MeV; measured σ(E;θ). 25,27Al deduced resonances, level-width. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1030. 1971HA41 Nucl.Phys. A172, 81 (1971) E.L.Haase, W.N.Wang, M.A.Fawzi Kinematically Complete Investigation of T=0 Excited States of 4He by Inelastic Scattering of α-Particles on 4He NUCLEAR REACTIONS 4He(α, α't), 4He(α, α'3He), 4He(α, α'd), E=104 MeV; measured σ(E1, E2, θ(1), θ(2)). 4He deduced resonance parameters. Natural gas target.
doi: 10.1016/0375-9474(71)90117-5
1971SH05 Phys.Rev.Lett. 26, 902 (1971) Intermediate Structure and the Giant-Dipole Resonance in O16 NUCLEAR REACTIONS 16O(γ, n), E < 26 MeV; calculated σ(E). 16O calculated giant dipole resonance structure. 3p-3h model.
doi: 10.1103/PhysRevLett.26.902
1970LI26 Chin.J.Phys.(Taiwan) 8, 36 (1970) E.K.Lin, W.N.Wang, G.C.Kiang, C.C.Hsu, P.S.Song, L.P.Liang The 26Mg(d, α)24Na Reaction at Low Energies NUCLEAR REACTIONS 26Mg(d, α), E=2.5-3.0 MeV; measured σ(E;θ); deduced reaction mechanism. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1029. 1970WA43 Chin.J.Phys. 8, 1 (1970) Study of 27Al(n, d)26Mg Reaction by 14.1 MeV Neutrons NUCLEAR REACTIONS 27Al(n, d), E=14.1 MeV; measured σ(Ed, θ). 26Mg deduced S, L.
1969HS01 Nuovo Cimento 59B, 39 (1969) Fluctuation Analysis of the 24Mg(d, α)22Na Reaction NUCLEAR REACTIONS 24Mg(d, α)22Na, E=1.8-3.05 MeV; measured σ(E;Eα); deduced reaction mechanism, Ericson fluctuation analysis. 26Al deduced level-width, mean level spacing.
doi: 10.1007/BF02712012
1967WA15 Nucl.Phys. A102, 537(1967) W.N.Wang, E.K.Lin, R.Chiba, T.J.Lee, Y.C.Yang, C.C.Hsu, T.Chiao The 2J+1 Rule in the 25Mg(d, α)23Na Reaction at Low Energies NUCLEAR REACTIONS 25Mg(d, α), E=2-3 MeV; measured σ(E; Eα, θ). 23Na deduced levels. Enriched target.
doi: 10.1016/0375-9474(67)90392-2
1965WA14 Phys.Rev. 140, B882 (1965) (n, d) Reaction Studies on Ni58, Cu63, and Zn64 NUCLEAR STRUCTURE 57Co, 63Cu, 62Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B882
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