NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Tian Found 50 matches. 2023CH42 At.Data Nucl.Data Tables 154, 101587 (2023) Y.Chen, H.Yao, M.Liu, J.Tian, P.Wen, N.Wang Systematic study of fusion barriers with energy dependent barrier radius NUCLEAR STRUCTURE Z<92; analyzed available data; deduced fusion barriers, a modified Siwek-Wilczynski (MSW) fusion σ formula.
doi: 10.1016/j.adt.2023.101587
2023ZO01 Chin.Phys.C 47, 044101 (2023) F.Zou, X.Sun, K.Zhang, H.Chen, J.Yan, J.Tian, Y.Cui Pre-neutron fragment mass yields for 235U(n, f) and 239Pu(n, f) reactions at incident energies from thermal up to 20 MeV NUCLEAR REACTIONS 235U, 239Pu(n, F), E<20 MeV; calculated pre-neutron fragment mass yields at incident energies from thermal up to 20 MeV using an empirical fission potential (EFP) model, the potential parameters of which are obtained from the measured data.
doi: 10.1088/1674-1137/acb910
2022PO03 Eur.Phys.J. A 58, 77 (2022) K.Pomorski, A.Dobrowolski, B.Nerlo-Pomorska, M.Warda, J.Bartel, Z.Xiao, Y.Chen, L.Liu, J.-L.Tian, X.Diao On the stability of superheavy nuclei
doi: 10.1140/epja/s10050-022-00737-3
2022WA03 Phys.Lett. B 825, 136856 (2022) Y.Wang, F.Guan, Q.Wu, X.Diao, Y.Huang, L.M.Lyu, Y.Qin, Z.Qin, D.Si, Z.Bai, F.Duan, L.Duan, Z.Gao, Q.Hu, R.J.Hu, G.Jin, S.Jin, J.Ma, P.Ma, J.Wang, P.Wang, Y.Wang, X.Wei, H.Yang, Y.Yang, G.Yu, Y.Yu, Y.Zhang, Q.Zhou, Y.Zhang, C.Ma, X.Hu, H.Wang, Y.Cui, J.Tian, Z.Xiao The emission order of hydrogen isotopes via correlation functions in 30 MeV/u Ar+Au reactions NUCLEAR REACTIONS 197Au(40Ar, X)1H/2H/3H, E=30 MeV/nucleon; measured reaction products, Ep, Ip; deduced correlation functions, emission rates. The Compact Spectrometer for Heavy IoN Experiment (CSHINE), the Heavy Ion Research Facility at Lanzhou (HIRFL).
doi: 10.1016/j.physletb.2021.136856
2022ZH07 Phys.Rev. C 105, 024328 (2022) H.B.Zhou, Z.Y.Li, Z.G.Gan, Z.Y.Zhang, H.Yao, N.Wang, H.B.Yang, L.Ma, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, J.L.Tian Modeling the fusion process with a modified Woods-Saxon potential in 40Ar-induced fusion reactions NUCLEAR REACTIONS 176Hf(40Ar, 2np)212Ac, (40Ar, 3np)213Ac, (40Ar, 2nα)209Ra, (40Ar, 3nα)210Ra, E=183, 190 MeV; measured reaction products, Eα, Iα; deduced σ(E), theory evaluation factors. Observed α peaks from decays of 211,212,213,213Ra, 214,215Ac. Comparison to density-constrained time-dependent Hartree-Fock theory calculations. Beam from Sector-Focusing Cyclotron of the Heavy Ion Research Facility in Lanzhou (HIRFL). 165Ho(40Ar, 4n), E(cm)=130-160 MeV; 169Tm(40Ar, 4n), E(cm)=130-170 MeV; 174Yb(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 175Lu(40Ar, 4n), (40Ar, 5n), E(cm)=130-170 MeV; 176Hf(40Ar, 4n), (40Ar, 5n), E(cm)=135-165 MeV; 181Ta(40Ar, 4n), E(cm)=130-160 MeV; analyzed σ(E) from 1984VE09.
doi: 10.1103/PhysRevC.105.024328
2021KO43 Chin.Phys.C 45, 124108 (2021) P.V.Kostryukov, A.Dobrowolski, B.Nerlo-Pomorska, M.Warda, Z.Xia, Y.Chen, L.Liu, J.-L.Tian, K.Pomorski Potential energy surfaces and fission fragment mass yields of even-even superheavy nuclei NUCLEAR STRUCTURE 254,256,258,260,262Rf, 258,260,262,264,266Sg, 264,266,268,270,272Hs, 276,278,280,282,284Ds, 278,280,282,284,286Cn, 282,284,286,288,290Fl, 286,288,290,292,294Lv, 290,292,294,296,298Og, 294,296,298,300,302120; calculated potential energy surfaces. The Lublin-Strasbourg Drop (LSD) model.
doi: 10.1088/1674-1137/ac29a3
2020PO09 Phys.Rev. C 101, 064602 (2020) K.Pomorski, A.Dobrowolski, R.Han, B.Nerlo-Pomorska, M.Warda, Z.Xiao, Y.Chen, L.Liu, J.-L.Tian Mass yields of fission fragments of Pt to Ra isotopes RADIOACTIVITY 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202Pt, 172,174,176,178,180,182,184,186,188,190,192,194,196,198,200,202Hg, 174,176,178,180,182,184,186,188,190,192,194,196,198,200,202,204Pb, 176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206Po, 196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226Rn, 198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228Ra, 236,238,240,242,244,246Pu(SF); calculated fission fragment mass distributions using collective three-dimensional model with Fourier nuclear shape parametrization and coupling fission, neck and mass asymmetry modes. 184Hg; calculated potential energy surfaces in (q2, q3) and (q3, q4) planes by macroscopic-microscopic model based on the Lublin-Strasbourg drop macroscopic energy and Yukawa-folded single-particle potential. Comparison with experimental fission fragment mass yields for 180,182,184Hg, 194,196Po, 202,204,206,208Rn, and 210,212,214,216,218Ra.
doi: 10.1103/PhysRevC.101.064602
2019CH12 Chin.J.Phys.(Taiwan) 58, 38 (2019) J.Cheng, D.Zhang, J.Li, J.Tian The odd-even effect of fragmentation cross sections produced in the de-excitation process NUCLEAR REACTIONS C, Al, Cu, Pb(36Ar, X), (40Ar, X), E=400 MeV/nucleon; calculated fragmentation σ, isotope distribution, excitation energy. Comparison with available data.
doi: 10.1016/j.cjph.2019.01.008
2018MA02 J.Phys.(London) G45, 015102 (2018) Mass dependence of temperature for intermediate mass fragment in heavy-ion reactions NUCLEAR REACTIONS 9Be(40Ca, X), (48Ca, X), E=140 MeV/nucleon; analyzed available data; deduced mass and temperature dependence in fragment distributions.
doi: 10.1088/1361-6471/aa8a24
2017TI02 Phys.Rev. C 95, 041601 (2017) Constraining presaddle dissipation with fission cross sections of light nuclear systems NUCLEAR STRUCTURE 205Bi, 215Fr, 225Pa, 230Np; calculated drop of fission cross sections over the statistical model values at different angular momenta and excitation energies using stochastic Langevin model.
doi: 10.1103/PhysRevC.95.041601
2017ZH18 Phys.Rev. C 95, 041602 (2017) Y.Zhang, J.Tian, W.Cheng, F.Guan, Y.Huang, H.Li, L.Lu, R.Wang, Y.Wang, Q.Wu, H.Yi, Z.Zhang, Y.Zhao, L.Duan, R.J.Hu, M.Huang, G.Jin, S.Jin, C.G.Lu, J.Ma, P.Ma, J.Wang, H.Yang, Y.Yang, J.Zhang, Ya.Zhang, Y.Zhang, C.Ma, C.Y.Qiao, M.B.Tsang, Z.Xiao Long-time drift of the isospin degree of freedom in heavy ion collisions NUCLEAR REACTIONS Au(40Ar, X), E=30 MeV/nucleon; measured light-charged particles (LCP), α-spectra, coincident fission fragments, (LCP)(fission fragments)-coin using parallel plate avalanche counters (PPAC) and nine ΔE telescopes at RIBLL-Lanzhou facility; deduced inclusive isotopic ratio for Z=1 and 2 isotopes as a function of laboratory angle, angular distribution of the relative neutron richness summed over the LCPs, drift of the isospin degree of freedom (IDOF). Comparison with ImQMD+GEMINI simulations.
doi: 10.1103/PhysRevC.95.041602
2016LI05 Phys.Rev. C 93, 014618 (2016) C.Li, F.Zhang, J.Li, L.Zhu, J.Tian, N.Wang, F.-S.Zhang Multinucleon transfer in the 136Xe + 208Pb reaction NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; calculated density distribution contours as function of time, lifetime of the neck, total-kinetic-energy-mass distributions for different impact parameters, TKEL distributions of primary binary fragments, average excitation energy of projectile-like fragments (PLFs) and target-like fragments (TLFs) as a function of neck lifetime, mass distributions of primary binary fragments at different impact parameters, production cross sections for N=110-140, Pt, Au, Hg, Tl, Pb, Bi, Po and At isotopes. Improved quantum molecular dynamics model (ImQMD) for multinucleon transfer reaction using statistical decay code GEMINI. Comparison with prediction of the dinuclear system and GRAZING model, and with available experimental data.
doi: 10.1103/PhysRevC.93.014618
2016TI05 Phys.Rev. C 94, 021601 (2016) Isospin effect on probing nuclear dissipation with fission cross sections NUCLEAR REACTIONS 208Pb, 209Bi(p, F), E*=60-210 MeV; calculated fission cross sections at different friction strengths using stochastic Langevin model; deduced isospin effects. Comparison with experimental data. 195,202,209Bi; calculated dynamical drop of fission cross sections at excitation energies of 50-200 MeV.
doi: 10.1103/PhysRevC.94.021601
2016TI06 Chin.Phys.C 40, 094101 (2016) J.-L.Tian, H.-T.Cui, T.Gao, N.Wang Effect of Wigner energy on the symmetry energy coefficient in nuclei NUCLEAR STRUCTURE A=80; calculated nuclear symmetry energy coefficients.
doi: 10.1088/1674-1137/40/9/094101
2016TI07 Chin.Phys.C 40, 094103 (2016) Effect of pre-equilibrium emission on probing postsaddle nuclear dissipation with neutrons NUCLEAR REACTIONS 238U(18O, X)256Fm, E=159 MeV; 208Pb(40Ar, X)248Fm, E=249 MeV; calculated neutron multiplicity, α-particle binding energies using deformation parameters of heavy fissioning systems 248,256Fm.
doi: 10.1088/1674-1137/40/9/094103
2016XU03 Phys.Rev. C 93, 044609 (2016) J.Xu, L.-W.Chen, M.Y.B.Tsang, H.Wolter, Y.-X.Zhang, J.Aichelin, M.Colonna, D.Cozma, P.Danielewicz, Z.-Q.Feng, A.Le Fevre, T.Gaitanos, C.Hartnack, K.Kim, Y.Kim, C.-M.Ko, B.-A.Li, Q.-F.Li, Z.-X.Li, P.Napolitani, A.Ono, M.Papa, T.Song, J.Su, J.-L.Tian, N.Wang, Y.-J.Wang, J.Weil, W.-J.Xie, F.-S.Zhang, G.-Q.Zhang Understanding transport simulations of heavy-ion collisions at 100A and 400A MeV: Comparison of heavy-ion transport codes under controlled conditions
doi: 10.1103/PhysRevC.93.044609
2016YE01 Phys.Rev. C 93, 044603 (2016) Probing postsaddle nuclear dissipation with excitation energy at scission NUCLEAR REACTIONS 238U(16O, F)254Fm*, E=288 MeV; 238U(18O, F)256Fm*, E=159 MeV; 159Tb(20Ne, F)179Re*, E=8-16 MeV/nucleon; calculated excitation energy at scission, prescission neutron multiplicity and compared to experimental data. 238U(16O, F)254Fm*, E=288 MeV; calculated postsaddle neutron multiplicity as a function of postsaddle dissipation strength. 246Cf at E(*)=50, 80, 180 MeV; calculated postsaddle neutron multiplicity, excitation energy at scission versus postsaddle friction strength. Stochastic Langevin model coupled with statistical decay model. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.044603
2015CH01 J.Phys.(London) G42, 15102 (2015) J.X.Cheng, J.L.Tian, D.H.Zhang The odd-even effect of fragmentation cross sections for 36Ar and 40Ar NUCLEAR REACTIONS C, Al, Cu, Pb(36Ar, X), (40Ar, X), E=400 MeV/nucleon; calculated projectile fragmentation σ using the improved quantum molecular dynamics model, together with the statistical model code GEMINI.
doi: 10.1088/0954-3899/42/1/015102
2015OU02 Phys.Rev.Lett. 115, 212501 (2015) L.Ou, Z.Xiao, H.Yi, N.Wang, M.liu, J.Tian Dynamic Isovector Reorientation of Deuteron as a Probe to Nuclear Symmetry Energy NUCLEAR REACTIONS 124Sn(polarized d, X), E=100 MeV/nucleon; calculated breakup reaction σ(θ). Comparison with available data.
doi: 10.1103/PhysRevLett.115.212501
2015TI01 Chin.Phys.C 39, 034102 (2015) Langevin analysis of fission excitation functions induced by protons NUCLEAR REACTIONS 206Pb, 209Bi(p, F), E<200 MeV; analyzed available data; deduced fits to measured excitation function data of fission σ.
doi: 10.1088/1674-1137/39/3/034102
2015WA14 Phys.Rev. C 91, 044308 (2015) N.Wang, M.Liu, H.Jiang, J.L.Tian, Y.M.Zhao Mass dependence of symmetry energy coefficients in the Skyrme force ATOMIC MASSES A=160; A=20-300; A=20-106; analyzed properties of nuclear symmetry energy as function of mass using the extended Thomas-Fermi (ETF2) approximation and 36 different Skyrme forces. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.91.044308
2015YE01 Phys.Rev. C 91, 064603 (2015) Spallation reaction versus heavy-ion fusion: Fission excitation functions as a fundamental probe of presaddle nuclear dissipation NUCLEAR STRUCTURE 224Th; calculated drop of fission σfdrop as function of presaddle dissipation strength in spallation and heavy-ion fusion reactions for the production of 224Th compound nucleus at E(*)=100-300 MeV and angular momentum l=10-30 ~h. Comparison of dynamical drop of fission cross section relative to statistical-model values. Combination of dynamical Langevin equations with a statistical decay model (CDSM).
doi: 10.1103/PhysRevC.91.064603
2014TI04 Phys.Rev. C 90, 024313 (2014) J.Tian, H.Cui, K.Zheng, N.Wang Effect of Coulomb energy on the symmetry energy coefficients of finite nuclei NUCLEAR STRUCTURE A=10-270; calculated symmetry energy coefficients from differences between the masses of isobaric nuclei, using masses from AME-2012 for more than 2400 nuclei; deduced mass and Coulomb energy dependence on symmetry energy.
doi: 10.1103/PhysRevC.90.024313
2014WA23 Phys.Rev. C 89, 064613 (2014) R.S.Wang, Y.Zhang, Z.G.Xiao, J.L.Tian, Y.X.Zhang, Q.H.Wu, L.M.Duan, G.M.Jin, R.J.Hu, S.F.Wang, Z.Y.Li, H.W.Wang, Z.Zhang, H.Yi, H.J.Li, W.J.Cheng, Y.Huang, L.M.Lu Time-dependent isospin composition of particles emitted in fission events following 40Ar + 197Au at 35 MeV/u NUCLEAR REACTIONS 197Au(40Ar, F), E=35 MeV/nucleon; measured particle spectra, (fission fragment)(light charged particles)-coin, mass asymmetry, double differential cross sections for proton, deuteron and triton at HRIFL-Lanzhou. Folding-angle method for reconstruction of fission events. Dependence of N/Z on the parameterization of the symmetry energy. Comparison with improved quantum molecular dynamics (ImQMD) transport-model calculations.
doi: 10.1103/PhysRevC.89.064613
2014YE07 Phys.Rev. C 90, 041604 (2014) Probing nuclear dissipation with particle multiplicity in heavy-ion-induced light fissioning systems NUCLEAR STRUCTURE 200Pb, 251Es; calculated postsaddle multiplicities and change in binding energies of neutrons, protons, and α particles as a function of deformation parameter and angular momentum at excitation energy 120 MeV for 200Pb and 70 MeV for 251Es in the framework of Langevin models coupled to a statistical decay model.
doi: 10.1103/PhysRevC.90.041604
2013LI29 Phys.Rev. C 87, 064615 (2013) Finite-size effects on fragmentation in heavy-ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=15, 35, 45 MeV/nucleon; 197Au (197Au, X), E=15, 35, 60 MeV/nucleon; 129Sn(120Xe, X), E=39 MeV/nucleon; 48Ca(58Ni, X), E=25, 35 MeV/nucleon; calculated fragment charge distribution, average number of nucleons emitted from the ground states, isotopic yields. Influence of nuclear finite-size effects on fragmentation in heavy-ion collisions. Improved quantum molecular dynamics model (ImQMD). Comparison with experimental data.
doi: 10.1103/PhysRevC.87.064615
2013LI51 Chin.Phys.C 37, 114101 (2013) C.Li, J.-L.Tian, Y.-J.Qin, J.-J.Li, N.Wang Determination of the nucleon-nucleon interaction in the ImQMD model by nuclear reactions at the Fermi energy region NUCLEAR REACTIONS 40Ca(40Ca, X), E=10-45 MeV/nucleon; 120Sn(129Xe, X), E=32, 45 MeV/nucleon; 197Au(197Au, X), E=35, 50 MeV/nucleon; 197Au(238U, X), E=15 MeV/nucleon; calculated charge fragment distribution, multiplicity. Improved quantum molecular dynamic model.
doi: 10.1088/1674-1137/37/11/114101
2013TI01 Phys.Rev. C 87, 014313 (2013) Improved Kelson-Garvey mass relations for proton-rich nuclei ATOMIC MASSES 5Be, 6B, 13F, 15Ne, 18Mg, 16,17Na, 19,20,21,22Al, 21,22,23Si, 22,23,24,25,26P, 24,25,26,27S, 25,26,27,28,29,30Cl, 28,29,30,31,32,33,34K, 27,28,29,30,31Ar, 30,31,32,33,34,35Ca, 31,32,33,34,35,36,37,38Sc, 33,34,35,36,37,38,39Ti, 35,36,37,38,39,40,41,42,43V, 37,38,39,40,41,42,43,44,45Cr, 39,40,41,42,43,44,45,46,47Mn, 41,42,43,44,45,46,47,48,49Fe, 43,44,45,46,47,48,49,50,51,52Co, 45,46,47,48,49,50,51,52,53Ni, 47,48,49,50,51,52,53,54,55,56Cu, 49,50,51,52,53,54,55,56,57Zn, 60Ga, 62Ge, 64As, 66Se, 68Br, 70Kr, 72Rb, 74Sr; calculated binding energies, mass excess, Sp, S2p using improved Kelson-Garvey (ImKG) mass relations. Comparison with experimental data for mirror analogs. Predictions of masses for proton-rich nuclides. Discussed diproton emission.
doi: 10.1103/PhysRevC.87.014313
2012QI08 Phys.Rev. C 85, 054623 (2012) Calculation of penetration probability across an arbitrary potential barrier in fusion reactions NUCLEAR REACTIONS 208Pb(18O, X), E=68-110 MeV; 90Zr(90Zr, X), E=190-210 MeV; calculated penetration probability, fusion σ(E), modified Bass potential barriers. Comparison with WKB (Wentzel-Kramers-Brillouin) approximation, Numerov calculations, and the transfer matrix approach. Double-hump barriers. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.054623
2011TI08 Int.J.Mod.Phys. E20, 1755 (2011) J.Tian, L.Ou, H.Hao, G.Yang, C.Bai Dynamical shell effect in the fusion reactions NUCLEAR REACTIONS 40Ca(48Ca, X)88Zr, 48Ca(48Ca, X)96Zr, 16O(208Pb, X)224Th, 48Ca(208Pb, X)256No, E not given; calculated fusion barriers, σ. ImQMD model, comparison with experimental data.
doi: 10.1142/S0218301311019556
2011WA41 Phys.Rev. C 84, 061601 (2011) Systematics of fusion probability in "hot" fusion reactions NUCLEAR REACTIONS 238U, 242,244Pu, 243Am, 245,248Cm, 249Bk, 249Cf(48Ca, 3n), (48Ca, 4n), E(cm)=190-220 MeV; 208Pb(48Ca, n), (48Ca, 2n), E(cm)=160-200 MeV; 208Pb(50Ti, n), (50Ti, 2n), E(cm)=170-210 MeV; 208Pb(54Cr, n), (54Cr, n), E(cm)=195-220 MeV; 208Pb(58Fe, n), (58Fe, 2n), E(cm)=210-230 MeV; 209Bi(58Fe, n), E(cm)=210-230 MeV; 208Pb(62Ni, n), E(cm)=235-255 MeV; 208Pb(64Ni, n), E(cm)=235-255 MeV; 208Pb(70Zn, n), E(cm)=250-270 MeV; 209Bi(64Ni, n), E(cm)=235-260 MeV; 209Bi(70Zn, n), E(cm)=255-270 MeV; 249Bk(50Ti, 3n), (50Ti, 4n), E(cm)=210-240 MeV; 248Cm(54Cr, 3n), (54Cr, 4n), E(cm)=230-255 MeV; 249Cf(50Ti, 3n), (50Ti, 4n), E(cm)=215-245 MeV; 244Pu(58Fe, 3n), (58Fe, 4n), E(cm)=240-270 MeV; calculated evaporation residual cross sections. Hot fusion reactions, super-heavy nuclei. Skyrme energy-density functionals. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.061601
2010TI01 Int.J.Mod.Phys. E19, 307 (2010) J.Tian, X.Li, S.Yan, Z.Wu, Z.Li Kinematic correlation of the ternary fission for the system 197Au + 197Au NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; measured reaction fragments; deduced mass number distributions, dynamical modes of ternary fission.
doi: 10.1142/S0218301310014777
2010TI07 Phys.Rev. C 82, 054608 (2010) J.Tian, X.Wu, Z.Li, K.Zhao, Y.Zhang, X.Li, S.Yan Mechanism of ternary breakup in the reaction 197Au+197Au at 15A MeV
doi: 10.1103/PhysRevC.82.054608
2009TI01 Chin.Phys.Lett. 26, 062502 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Possible Mechanisms of Ternary Fission in the 197Au+197Au System at 15 AMeV NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; Calculated ternary fission mass distribution, σ. ImQMD model.
doi: 10.1088/0256-307X/26/6/062502
2009TI06 Phys.Rev. C 79, 067901 (2009) J.Tian, J.H.Chen, Y.G.Ma, X.Z.Cai, F.Jin, G.L.Ma, S.Zhang, C.Zhong Breaking of the number-of-constituent-quark scaling for identified-particle elliptic flow as a signal of phase change in low-energy data taken at the BNL Relativistic Heavy Ion Collider (RHIC)
doi: 10.1103/PhysRevC.79.067901
2009TI12 Eur.Phys.J. A 42, 105 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Dynamic potential barrier in the entrance phase of heavy-ion fusion reactions NUCLEAR REACTIONS 100Mo(86Kr, X), E(cm)=153.9, 163.9, 173.9, 183.9, 203.9, 300.9 MeV; calculated fusion potential barrier and reaction mechanism features using an improved quantum molecular dynamics model.
doi: 10.1140/epja/i2009-10850-2
2009TI13 Chin.Phys.C 33, Supplement 1, 109 (2009) J.-L.Tian, X.Li, X.-Z.Wu, Z.-X.Li, S.-W.Yan Understanding of the dissipation mechanism in ternary fission for the system 197Au+197Au NUCLEAR REACTIONS 197Au(197Au, X), E=15 MeV/nucleon; calculated mass number distributions, impact parameter dependence of production probability of ternary fission and average mass number of fragments. Improved quantum molecular dynamics (ImQMD) model.
doi: 10.1088/1674-1137/33/S1/035
2009WU06 Chin.Phys.C 33, Supplement 1, 30 (2009) X.-Z.Wu, J.-L.Tian, K.Zhao, Y.-X.Zhang, Z.-X.Li Study on the formation of the composite system of 238U+238U NUCLEAR REACTIONS 238U(238U, X), E(cm)=680-1880 MeV; calculated potential and translation kinetic energies, single-particle potentials; deduced conditions for giant composite systems.
doi: 10.1088/1674-1137/33/S1/010
2008TI02 Phys.Rev. C 77, 064603 (2008) J.Tian, X.Wu, K.Zhao, Y.Zhang, Z.Li Properties of the composite systems formed in the reactions of 238U+238U and 232Th+250Cf NUCLEAR REACTIONS 197Au(197Au, X), E=35 MeV/nucleon; calculated charge distributions. 208Pb, 238U(48Ca, X), E(cm)=170-270 MeV; calculated σ. 238U(238U, X), 250Cf(232Th, X), E=680-1880 MeV; calculated lifetimes. 238U(238U, X), E=680-1880 MeV; calculated entrance channel potential energies, translation kinetic energies, excitation energies, single-particle energies, density distributions. Quantum dynamics model.
doi: 10.1103/PhysRevC.77.064603
2007OU02 J.Phys.(London) G34, 827 (2007) Analysis of intermediate energy proton-induced spallation reactions by an improved quantum molecular dynamics plus statistical decay model NUCLEAR REACTIONS 16O, 27Al, 56Fe, 208Pb(p, nX), E=113, 256, 597, 800 MeV; calculated spallation neutron spectra, σ(E, θ). Improved molecular dynamics model, statistical decay model, comparison with data.
doi: 10.1088/0954-3899/34/5/004
2007TI04 Chin.Phys.Lett. 24, 905 (2007) Modified Woods-Saxon Potential for Heavy-Ion Fusions Reaction NUCLEAR REACTIONS 92Zr(16O, X), (28Si, X), E(cm) ≈ 30-1000 MeV; 208Pb(16O, X), (48Ca, X), E(cm) ≈ 60-220 MeV; calculated interaction potentials, fusion excitation functions. 208Pb(48Ca, xn), (50Ti, xn), (54Cr, xn), (58Fe, xn), (62Ni, xn), (64Ni, xn), (70Zn, xn), 209Bi(58Fe, xn), (64Ni, xn), (70Zn, xn), E(cm) ≈ 160-280 MeV; compiled, analyzed evaporation σ. Modified Woods-Saxon potential.
doi: 10.1088/0256-307X/24/4/016
2007TI11 Chin.Phys.Lett. 24, 2796 (2007) J.-L.Tian, X.-Z.Wu, L.Ou, Z.-X.Li The Average Lifetime of Giant Composite Systems Formed in Strongly Damped Collisions NUCLEAR REACTIONS 238U(238U, X), E(cm)=680-1880 MeV; 250Cf(232Th, X), E(cm)=680-1880 MeV; calculated lifetimes and orientation angle distributions of the composite systems, and fragment charge distributions using the QMD model.
doi: 10.1088/0256-307X/24/10/023
2007ZH29 Phys.Rev. C 76, 014904 (2007) S.Zhang, G.L.Ma, Y.G.Ma, X.Z.Cai, J.H.Chen, H.Z.Huang, W.Q.Shen, X.H.Shi, F.Jin, J.Tian, C.Zhong, J.X.Zuo Transverse momentum and pseudorapidity dependences of Mach-like correlations for central Au+Au collisions at √ sNN = 200 GeV
doi: 10.1103/PhysRevC.76.014904
2004LI22 Phys.Rev. C 69, 034905 (2004) F.-H.Liu, X.-Y.Yin, J.-L.Tian, N.N.Abd Allah Charged-particle (pseudo)rapidity distributions in e+ e-, p(p-bar) and AA collisions at high energies NUCLEAR REACTIONS 1H(p-bar, X), 197Au(197Au, X), Pb(Pb, X), E=high; calculated charged particle pseudorapidity distributions. Two-cylinder model, unified formula, comparison with data.
doi: 10.1103/PhysRevC.69.034905
2004WA08 Phys.Rev. C 69, 034608 (2004) N.Wang, Z.Li, Z.Wu, J.Tian, Y.X.Zhang, M.Liu Further development of the improved quantum molecular dynamics model and its application to fusion reactions near the barrier NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 114,132Sn, 140Ce, 208Pb; calculated binding energies, radii. NUCLEAR REACTIONS 48Ca, 90Zr(40Ca, X), 16O, 208Pb(16O, X), 131I(131I, X), 208Pb(54Cr, X), 230Th(32S, X), 250Fm(12C, X), E not given; calculated static Coulomb barriers. 48Ca(40Ca, X), E(cm)=52, 54, 58, 60 MeV; calculated fusion probability. 48Ca, 48Ti, 90,96Zr(40Ca, X), E(cm)=48-112 MeV; 46Ti(46Ti, X), E(cm)=58-72 MeV; 89Y(32S, X), (34S, X), E(cm)=72-92 MeV; 92Zr(28Si, X), (35Cl, X), E(cm)=65-100 MeV; 64Ni(132Sn, X), E(cm)=140-168 MeV; calculated fusion σ. Improved quantum molecular dynamics model, comparison with data.
doi: 10.1103/PhysRevC.69.034608
2000LI02 Phys.Rev. C61, 024610 (2000) X.Z.Li, J.Tian, M.Y.Mei, C.X.Li Sub-Barrier Fusion and Selective Resonant Tunneling NUCLEAR REACTIONS 3H(d, X), E=7-1000 keV; calculated sub-barrier fusion σ. Selective resonant tunneling model, comparison with data.
doi: 10.1103/PhysRevC.61.024610
1998YU07 High Energy Phys. and Nucl.Phys. (China) 22, 1082 (1998) X.Yu, S.Shi, J.Gu, J.Liu, W.Li, J.Zeng, J.Tian, Y.Li, J.Zhou Low-lying level structure of 83Rb
1998ZH22 Phys.Rev. C58, 156 (1998) L.Zhang, J.Zhao, J.Zheng, J.Wang, Z.Qin, Y.Yang, C.Zhang, G.Jin, G.Guo, Y.Du, T.Guo, T.Wang, B.Guo, J.Tian, Y.Lou Neutron-Rich Heavy Residues and Exotic Multinucleon Transfer RADIOACTIVITY 209Hg(β-) [from Pb(18O, X), E=600 MeV]; measured Eγ, Iγ(t), βγ-coin; deduced T1/2. NUCLEAR REACTIONS, ICPND Pb(18O, X)203Hg/205Hg/206Hg/207Hg/208Hg/209Hg, E=600 MeV; measured production σ.
doi: 10.1103/PhysRevC.58.156
1993XU07 High Energy Phys. and Nucl.Phys. (China) 17, 985 (1993) S.Xu, Q.Pan, T.Zhang, S.Yuan, X.Zhang, S.Shi, J.Tian, W.Huang Experimental Measurements for the QEC-Value of 183Os-Decay
1992SH12 Z.Phys. A342, 369 (1992) S.Shi, W.D.Huang, Y.Li, D.Z.Yin, J.H.Gu, J.Q.Tian Identification of a New Neutron Rich Isotope 202Pt NUCLEAR REACTIONS 204Hg(n, n2p), E=fast; measured Eγ, Iγ, decay curve; deduced evidence for 202Pt. RADIOACTIVITY 202Pt(β-) [from 204Hg(n, n2p), E=fast]; measured Eγ, Iγ, decay curve; deduced T1/2.
doi: 10.1007/BF01291520
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