NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = X.Deng Found 17 matches. 2023AN14 Sci. Rep. 13, 12657 (2023) Z.An, W.Qiu, W.Jiang, G.Yang, X.Li, Z.Liao, Z.Zhuang, X.Zhang, S.Chen, C.Guo, E.Xiao, X.Fang, X.Li, H.Wang, X.Hu, Bi.Jiang, W.Shen, J.Wang, J.Ren, X.Ruan, D.Wang, S.-Y.Zhang, W.Luo, Z.Zhu, H.Lan, Z.Cao, X.Ma, Y.Liu, P.Wang, Y.Yang, P.Su, X.Deng, W.He, Y.Ma, C.Ma, Y.Wang, P.He, R.Tang, T.Zhou, J.Wang, H.Yi, Y.Zhang, Y.Chen, R.Fan, K.Gao, Q.Li, K.Sun, Z.Tan, M.Gu, H.Jing, J.Tang Measurement of the 181Ta(n, γ) cross sections up to stellar s-process temperatures at the CSNS Back-n NUCLEAR REACTIONS 181Ta(n, γ), E=0.001-800 keV; measured reaction products, En, In, TOF; deduced σ, resonance parameters using the R-Matrix code SAMMY, Maxwellian average cross sections (MACS). Comparison with available data. The back-streaming white neutron facility (Back-n) of China spallation neutron source (CSNS).
doi: 10.1038/s41598-023-39603-7
2023CA12 Phys.Rev. C 108, 024610 (2023) Effect of initial-state geometric configurations on the nuclear liquid-gas phase transition NUCLEAR REACTIONS 40Ca(16O, X), E(cm)=60-150 MeV/nucleon; calculated yields of proton, neutron, 2H, 3H, 3He and α dependence on the incident energy when 16O is polarized transversely, longitudinally, and unpolarized, dependence of yields on the 16O α-cluster geometrical configurations. Simulations within the framework of an extended quantum molecular dynamics model (EQMD) coupled to the GEMINI model used to deexcite heavy fragments.
doi: 10.1103/PhysRevC.108.024610
2023DE04 Phys.Rev. C 107, 014616 (2023) Examination of promising reactions with 241Am and 244Cm targets for the synthesis of new superheavy elements within the dinuclear system model with a dynamical potential energy surface NUCLEAR REACTIONS 249Cf(48Ca, X), 249Cf(48Ca, 2n), 249Cf(48Ca, 3n), 249Cf(48Ca, 4n), 249Cf(48Ca, 5n), E(cm)=170-250 MeV; calculated capture σ(E), fusion probability, survival probability, evolution with time of the dynamical potential energy surface. 238U(48Ca, 2n)284Cn, E(cm)=184.11 MeV;237Np(48Ca, 2n)283Nh, E(cm)=190.82 MeV;242Pu(48Ca, 2n)288Fl, E(cm)=186.62 MeV;244Pu(48Ca, 3n)289Fl, E(cm)=192.29 MeV;241Am(48Ca, 2n)287Mc, E(cm)=194.75 MeV;243Am(48Ca, 2n)289Mc, E(cm)=192.08 MeV;244Cm(48Ca, 2n)290Lv, E(cm)=196.92 MeV;245Cm(48Ca, 3n)290Lv, E(cm)=202.94 MeV;248Cm(48Ca, 3n)293Lv, E(cm)=197.23 MeV;249Bk(48Ca, 3n)294Ts, E(cm)=200.73 MeV;249Cf(48Ca, 2n)290Og, E(cm)=197.75 MeV;241Am(54Cr, 2n)293119, E(cm)=233.22 MeV;244Cm(54Cr, 2n)296120, E(cm)=237.11 MeV;241Am(55Mn, 2n)294120, E(cm)=242.67 MeV;244Cm(55Mn, 2n)297121, E(cm)=245.92 MeV;241Am(58Fe, 2n)297121, E(cm)=255.88 MeV;244Cm(58Fe, 2n)300122, E(cm)=258.80 MeV;241Am(59Co, 2n)298122, E(cm)=263.59 MeV; calculated capture σ, fusion probability, survival probability, maximum evaporation residue σ. 238U, 237Np, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=20-80 MeV; calculated evaporation residue σ(E). Calculations using the dinuclear system model with a dynamical potential energy surface. Comparison with available experimental data.
doi: 10.1103/PhysRevC.107.014616
2023DE33 Int.J.Mod.Phys. E32, 2340004 (2023) Ground state and fission properties of even-A uranium isotopes from multidimensionally-constrained relativistic mean field model NUCLEAR STRUCTURE 214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320,322,324,326,328,330,332,334,336,338,340,342,344,346,348,350U; calculated potential energy surfaces, the ground state properties, including two-neutron separation energies, root-mean-square radii for the neutron, proton, matter and charge distributions and quadrupole and octupole deformations using the MDC-RMF model.
doi: 10.1142/S0218301323400049
2023XI02 Eur.Phys.J. A 59, 33 (2023) B.-S.Xi, X.-G.Deng, S.Zhang, Y.-G.Ma Vorticity in isobar collisions of 9644Ru + 9644Ru and 9640Zr + 9640Zr at √ sNN = 200 GeV NUCLEAR REACTIONS 96Ru(96Ru, X), 96Zr(96Zr, X), E=200 GeV; calculated kinematic vorticity and thermal vorticity within the framework of Ultra-relativistic Quantum Molecular Dynamics model (UrQMD); deduced impact of deformation parameter.
doi: 10.1140/epja/s10050-023-00932-w
2022CA17 Phys.Rev. C 106, 014611 (2022), Erratum Phys.Rev. C 108, 049904 (2023) Impact of magnetic field on the giant dipole resonance of 40Ca using an extended quantum molecular dynamics model NUCLEAR REACTIONS 40Ca(16O, X), E=50-500 MeV/nucleon; calculated time evolution of the magnetic field at the central, dependence between magnetic-field integral over time and beam energy point, time evolution of the dipole moments, γ-emission probability. 40Ca; calculated giant dipole resonance features with taking into account magnetic field and particle acceleration effect in Coulomb excitation process. Extended quantum molecular dynamics (EQMD) model.
doi: 10.1103/PhysRevC.106.014611
2022DE12 Phys.Rev. C 105, 064613 (2022) X.G.Deng, P.Danielewicz, Y.G.Ma, H.Lin, Y.X.Zhang Impact of fragment formation on shear viscosity in the nuclear liquid-gas phase transition region
doi: 10.1103/PhysRevC.105.064613
2021DE24 Eur.Phys.J. A 57, 242 (2021) Green-Kubo formula for Boltzmann and Fermi-Dirac statistics
doi: 10.1140/epja/s10050-021-00550-4
2020DE16 Phys.Rev. C 101, 054610 (2020) Magnetic field effects in peripheral heavy ion collisions near 1 GeV/nucleon NUCLEAR REACTIONS 197Au(197Au, X), E=600-1500 MeV/nucleon; calculated time evolution of magnetic field, distribution of proton angles and that of two-particle correlators of proton angles as function of incident energies and impact parameters, neutron to proton ratios as function of angle, rapidity, transverse momentum, four-particle angle correlator with and without magnetic field effects. Calculations based on isospin-dependent quantum molecular-dynamics (IQMD) model.
doi: 10.1103/PhysRevC.101.054610
2020DE23 Phys.Rev. C 101, 064908 (2020) X.-G.Deng, X.-G.Huang, Y.-G.Ma, S.Zhang Vorticity in low-energy heavy-ion collisions
doi: 10.1103/PhysRevC.101.064908
2018DE37 Eur.Phys.J. A 54, 204 (2018) Magnetic field effects on photon emission in intermediate energy heavy-ion collisions NUCLEAR REACTIONS 208Pb(14N, γ), E=40 MeV/nucleon; calculated σ(θ, Eγ), σ(θ), time evolution of photon production at different impact parameters, effect of magnetic field using BUU (Boltzmann-Uehling-Uhlenbeck) model with photon production due to proton-neutron bremsstrahlung. Compared to data.
doi: 10.1140/epja/i2018-12635-x
2017GU14 Phys.Rev. C 95, 054622 (2017) C.Q.Guo, Y.G.Ma, W.B.He, X.G.Cao, D.Q.Fang, X.G.Deng, C.L.Zhou Isovector dipole resonance and shear viscosity in low energy heavy-ion collisions NUCLEAR REACTIONS 100Mo(40Ca, X), E=5, 7.5, 10, 12.5, 15 MeV/nucleon; calculated time evolution of nuclear matter density and kinetic-energy density, temperature, chemical potential, and the entropy density of the compound nucleus, post equilibration time evolution of the stress tensor, ratio of shear viscosity over entropy density as function of temperature, giant dipole moment in coordinate space, isovector giant dipole resonance (IVGDR) photon spectra and centroid energies. Green-Kubo method in the framework of an extended quantum molecular dynamics model (EQMD).
doi: 10.1103/PhysRevC.95.054622
2017LI44 Phys.Rev. C 96, 064604 (2017) H.L.Liu, Y.G.Ma, A.Bonasera, X.G.Deng, O.Lopez, M.Veselsky Mean free path and shear viscosity in central 129Xe + 119Sn collisions below 100 MeV/nucleon NUCLEAR REACTIONS 119Sn(129Xe, X), E=15-100 MeV/nucleon; calculated average density, temperature, shear viscosity, chemical potential, mean momentum, mean free path, nucleon-nucleon cross section, maximum density and corresponding moment, entropy density in central regions, in-medium nucleon cross section using the isospin-dependent quantum molecular dynamical (IQMD) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.064604
2016DE27 Phys.Rev. C 94, 044622 (2016) Thermal and transport properties in central heavy-ion reactions around a few hundred MeV/nucleon NUCLEAR REACTIONS 197Au(197Au, X), E=100-300 MeV/nucleon; calculated time evolution of the average density, temperature, entropy density, entropy per nucleon, shear viscosity, isospin diffusivity, heat conductivity, and isospin asymmetry as function of incident energy, thermal and transport quantities for nuclear matter. Van derWaalsBoltzmann-Uehling-Uhlenbeck (VdWBUU) model with the hard equation of state (EoS) and soft EoS.
doi: 10.1103/PhysRevC.94.044622
2014KA30 Phys.Rev.Lett. 113, 022502 (2014) J.Katich, X.Qian, Y.X.Zhao, K.Allada, K.Aniol, J.R.M.Annand, T.Averett, F.Benmokhtar, W.Bertozzi, P.C.Bradshaw, P.Bosted, A.Camsonne, M.Canan, G.D.Cates, C.Chen, J.-P.Chen, W.Chen, K.Chirapatpimol, E.Chudakov, E.Cisbani, J.C.Cornejo, F.Cusanno, M.M.Dalton, W.Deconinck, C.W.de Jager, R.De Leo, X.Deng, A.Deur, H.Ding, P.A.M.Dolph, C.Dutta, D.Dutta, L.El Fassi, S.Frullani, H.Gao, F.Garibaldi, D.Gaskell, S.Gilad, R.Gilman, O.Glamazdin, S.Golge, L.Guo, D.Hamilton, O.Hansen, D.W.Higinbotham, T.Holmstrom, J.Huang, M.Huang, H.F.Ibrahim, M.Iodice, X.Jiang, G.Jin, M.K.Jones, A.Kelleher, W.Kim, A.Kolarkar, W.Korsch, J.J.LeRose, X.Li, Y.Li, R.Lindgren, N.Liyanage, E.Long, H.-J.Lu, D.J.Margaziotis, P.Markowitz, S.Marrone, D.McNulty, Z.-E.Meziani, R.Michaels, B.Moffit, C.Munoz Camacho, S.Nanda, A.Narayan, V.Nelyubin, B.Norum, Y.Oh, M.Osipenko, D.Parno, J.C.Peng, S.K.Phillips, M.Posik, A.J.R.Puckett, Y.Qiang, A.Rakhman, R.D.Ransome, S.Riordan, A.Saha, B.Sawatzky, E.Schulte, A.Shahinyan, M.H.Shabestari, S.Sirca, S.Stepanyan, R.Subedi, V.Sulkosky, L.-G.Tang, A.Tobias, G.M.Urciuoli, I.Vilardi, K.Wang, Y.Wang, B.Wojtsekhowski, X.Yan, H.Yao, Y.Ye, Z.Ye, L.Yuan, X.Zhan, Y.Zhang, Y.-W.Zhang, B.Zhao, X.Zheng, L.Zhu, X.Zhu, X.Zong Measurement of the Target-Normal Single-Spin Asymmetry in Deep-Inelastic Scattering from the Reaction 3He ↑ (e, e')X
doi: 10.1103/PhysRevLett.113.022502
1983WU04 Chin.J.Nucl.Phys. 5, 158 (1983) Wu Jingxia, Deng Xinlin, Rong Chaofan, Sun Zhongfa, Zhou Huiming, Zhou Shuhua Measurement of Fission Cross Section for 238U Induced by Fast Neutrons NUCLEAR REACTIONS 238U(n, F), E=4-5.5 MeV; measured absolute fission σ(E). Recoil proton semiconductor detector telescope, ionization chamber. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30669. 1982ZH05 Chin.J.Nucl.Phys. 4, 131 (1982) Zhou Xianjian, Yan Wuguang, Zhou Huiming, Deng Xinlu, Rong Chaofan, Wu Jingxia, Sun Zhongfa, Zhou Shuhua, Ye Zhongyuan The Absolute Measurement of Fast Neutron Fission Cross Section of 239Pu NUCLEAR REACTIONS 239Pu(n, F), E=1-1.6, 3.4-5.6 MeV; measured absolute fission σ vs E. Fission ionization chamber. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30670. Back to query form Note: The following list of authors and aliases matches the search parameter X.Deng: , X.G.DENG, X.Q.DENG |