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Search: Author = F.S.Zhang

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2024SU01      Phys.Rev. C 109, 014321 (2024)

Sh.Sun, L.-G.Cao, F.-Sh.Zhang, H.Sagawa, G.Colo

Microscopic study of M1 resonances in Sn isotopes

doi: 10.1103/PhysRevC.109.014321
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2024SU06      Eur.Phys.J. A 60, (2024)

Sh.Sun, R.-Q.Yu, L.-G.Cao, Ch.-L.Zhang, F.-Sh.Zhang

Application of relativistic continuum random phase approximation to giant dipole resonance of 208Pb and 132Sn

NUCLEAR STRUCTURE 132Sn, 208Pb; calculated the properties of isovector giant dipole resonances (IVGDR) using the relativistic continuum random phase approximation (RCRPA).

doi: 10.1140/epja/s10050-024-01288-5
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2024ZH05      Phys.Rev. C 109, 014622 (2024)

M.-H.Zhang, Y.-H.Zhang, Y.Zou, Ch.Wang, L.Zhu, F.-Sh.Zhang

Predictions of synthesizing elements with Z=119 and 120 in fusion reactions

doi: 10.1103/PhysRevC.109.014622
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2024ZH08      Phys.Rev. C 109, 024606 (2024)

L.-L.Zhou, J.-J.Cai, L.-Q.Li, Z.-L.Wang, R.Zhu, X.-Y.Zhang, X.-R.Zhang, L.Zhu, G.Zhang, F.-Sh.Zhang

Fusion enhancement in the collisions with 44Ca beams and the production of neutron-deficient 245-250Lr isotopes

doi: 10.1103/PhysRevC.109.024606
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2023CH06      Chin.Phys.C 47, 024102 (2023)

S.-H.Cheng, J.Wen, L.-G.Cao, F.-S.Zhang

Neutron skin thickness of 90Zr and symmetry energy constrained by charge exchange spin-dipole excitations

NUCLEAR REACTIONS 90Zr(p, n), (n, p), E<50 MeV; analyzed available data. 90Zr; deduced charge exchange spin-dipole (SD) excitations using the Skyrme Hartee-Fock plus proton-neutron random phase approximation with SAMi-J interactions, neutron skin thickness.

doi: 10.1088/1674-1137/aca38e
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2023LI17      Int.J.Mod.Phys. E32, 2330002 (2023)

J.-J.Li, N.Tang, Y.-H.Zhang, M.-H.Zhang, C.Wang, X.-R.Zhang, L.Zhu, F.-S.Zhang

Progress on production cross-sections of unknown nuclei in fusion evaporation reactions and multinucleon transfer reactions

NUCLEAR REACTIONS 232Th(204Hg, X), E(cm)=678.1 MeV; 249Bk(238U, X), E(cm)=823.4 MeV; 248Cm(238U, X), E(cm)=824.9 MeV; calculated σ in fusion evaporation (FE) reactions and multinucleon transfer (MNT) reactions.

doi: 10.1142/S0218301323300023
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2023LU04      Phys.Rev. C 108, 014302 (2023)

H.Y.Lu, Z.Liu, Z.H.Li, X.Wang, J.Li, H.Hua, H.Huang, W.Q.Zhang, Q.B.Zeng, X.H.Yu, T.H.Huang, M.D.Sun, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, F.S.Zhang

Reinvestigation of 222U in high-precision digital α-decay spectroscopy: Solution to the reduced decay-width anomaly

RADIOACTIVITY 222U(α) [from 186W(40Ar, 4n), E=80 MeV, followed by separation of fragments using SHANS separator at HRIFL-Lanzhou]; 218Th, 214Ra(α)[from 222U α decay chain]; measured Eα, Iα, evaporation residues (ER)-α correlations, T1/2 using DSSD detectors; deduced reduced α-decay width, and analyzed using NpNn scheme. 218Ac, 219Th, 220Pa(α); measured Eα, and T1/2. Systematics of reduced α-decay widths for g.s. to g.s. α transitions in even-even Z=84-92, N≥126 isotopes as function of NpNn. Comparison with previous experimental results.

doi: 10.1103/PhysRevC.108.014302
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2023TA03      Phys.Rev. C 107, 014603 (2023)

N.Tang, B.Li, J.-J.Li, F.-S.Zhang

Production of 61Ca, 63Sc, 65Ti, 68, 69V, 71Cr, 77Fe and 79Co in projectile fragmentation with radioactive ion beams at 1A GeV

NUCLEAR REACTIONS 9Be(69Cu, X)37Ar/38Ar/39Ar/40Ar/41Ar/42Ar/43Ar/44Ar/39K/40K/41K/42K/43K/44K/45K/46K/41Ca/42Ca/43Ca/44Ca/45Ca/46Ca/47Ca/43Sc/44Sc/45Sc/46Sc/47Sc/48Sc/49Sc/50Sc/45Ti/46Ti/47Ti/48Ti/49Ti/50Ti/51Ti/52Ti/48V/49V/50V/51V/52V/53V/54V/55V/50Cr/51Cr/52Cr/53Cr/54Cr/55Cr/56Cr/57Cr/53Mn/54Mn/55Mn/56Mn/57Mn/58Mn/59Mn, E=98.1 MeV/nucleon; calculated isotopes production σ. 9Be(81Ga, X)48Ca/49Ca/50Ca/51Ca/52Ca/53Ca/54Ca/55Ca/56Ca/49Sc/50Sc/51Sc/52Sc/53Sc/54Sc/55Sc/56Sc/57Sc/58Sc/59Sc/60Sc/52Ti/53Ti/54Ti/55Ti/56Ti/57Ti/58Ti/59Ti/60Ti/61Ti/62Ti/63Ti/56V/57V/58V/59V/60V/61V/62V/63V/64V/65V/56Cr/57Cr/58Cr/59Cr/60Cr/61Cr/62Cr/63Cr/64Cr/65Cr/66Cr/67Cr/59Mn/60Mn/61Mn/62Mn/63Mn/64Mn/65Mn/66Mn/67Mn/68Mn/69Mn/62Fe/63Fe/64Fe/65Fe/66Fe/67Fe/68Fe/69Fe/70Fe/71Fe/72Fe/64Co/65Co/66Co/67Co/68Co/69Co/70Co/71Co/72Co/73Co, E=1 GeV/nucleon; 9Be(84Ga, X)48Ca/49Ca/50Ca/51Ca/52Ca/53Ca/54Ca/55Ca/56Ca/57Ca/58Ca/59Ca/60Ca/51Sc/52Sc/53Sc/54Sc/55Sc/56Sc/57Sc/58Sc/59Sc/60Sc/61Sc/53Ti/54Ti/55Ti/56Ti/57Ti/58Ti/59Ti/60Ti/61Ti/62Ti/63Ti/64Ti/57V/58V/59V/60V/61V/62V/63V/64V/65V/66V/58Cr/59Cr/60Cr/61Cr/62Cr/63Cr/64Cr/65Cr/66Cr/67Cr/68Cr/69Cr/60Mn/61Mn/62Mn/63Mn/64Mn/65Mn/66Mn/67Mn/68Mn/69Mn/70Mn/71Mn/72Mn/64Fe/65Fe/66Fe/67Fe/68Fe/69Fe/70Fe/71Fe/72Fe/73Fe/74Fe/75Fe/66Co/67Co/68Co/69Co/70Co/71Co/72Co/73Co/74Co/75Co/76Co/77Co, E=1 GeV/nucleon; 9Be(86Ga, X)48Ca/49Ca/50Ca/51Ca/52Ca/53Ca/54Ca/55Ca/56Ca/57Ca/58Ca/59Ca/60Ca/61Ca/51Sc/52Sc/53Sc/54Sc/55Sc/56Sc/57Sc/58Sc/59Sc/60Sc/61Sc/62Sc/63Sc/54Ti/55Ti/56Ti/57Ti/58Ti/59Ti/60Ti/61Ti/62Ti/63Ti/64Ti/65Ti/57V/58V/59V/60V/61V/62V/63V/64V/65V/66V/67V/68V/69V/59Cr/60Cr/61Cr/62Cr/63Cr/64Cr/65Cr/66Cr/67Cr/68Cr/69Cr/70Cr/71Cr/62Mn/63Mn/64Mn/65Mn/66Mn/67Mn/68Mn/69Mn/70Mn/71Mn/72Mn/73Mn/74Mn/75Mn/65Fe/66Fe/67Fe/68Fe/69Fe/70Fe/71Fe/72Fe/73Fe/74Fe/75Fe/76Fe/77Fe/67Co/68Co/69Co/70Co/71Co/72Co/73Co/74Co/75Co/76Co/77Co/78Co/79Co, E=1 GeV/nucleon; calculated isotopes production σ. Isospin-dependent Boltzmann-Langevin equation (IBLE) model. Comparison of model predictions with experimental data for 9Be(69Cu, X) reaction.

doi: 10.1103/PhysRevC.107.014603
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2023ZH09      Phys.Rev. C 107, 024604 (2023)

Y.-H.Zhang, J.-J.Li, N.Tang, X.-R.Zhang, Z.Liu, F.-S.Zhang

Production cross sections of new neutron-rich isotopes with Z=92-106 in the multinucleon transfer reaction 197Au + 232Th

NUCLEAR REACTIONS 232Th(197Au, X)258Es/259Es/260Es/261Es/262Es/260Fm/261Fm/262Fm/263Fm/261Md/262Md/263Md/264Md/265Md/261No/263No/264No/265No/266No/267No/263Lr/265Lr/267Lr/268Lr/264Rf/266Rf/268Rf/269Rf/270Rf/264Db/265Db/269Db/271Db/267Sg/268Sg/270Sg/272Sg/273Sg, E(cm)=690.69;232Th(197Au, X)243U/244U/245U/246U/247U/248U/249U/246Np/247Np/248Np/249Np/250Np/251Np/252Np/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/256Am/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/252Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/257Cf/258Cf/259Cf/260Cf/261Cf/258Es/259Es/260Es/261Es/262Es, E(cm)=756.47 MeV; calculated production σ. 232Th(197Au, X), E=690.7, 723.6, 756.5 MeV;232Th(186W, X), E=681, 2 MeV;232Th(238U, X), E=823.8; calculated final isotopic production σ for U, Np, Pu, Am, Cm, Bk, Cf, Es, Fm, Md, No, Lr, Rf, Db and Sg isotopes, calculated driving potentials, potential energy surfaces. 232Th(197Au, X), E=690.7, 723.6, 756.5, 789.4 MeV; interaction time as a function of the impact parameter. 249Cf(136Xe, X), E(cm)=567 MeV; calculated final production σ for Pu, Am, Cm, Bk, Cf, Es isotopes. Calculations performed within the framework of dinuclear system (DNS) model with a decay model GEMINI++. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.024604
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2022AN05      Phys.Rev. C 105, 014325 (2022)

R.An, X.Jiang, L.-G.Cao, F.-S.Zhang

Odd-even staggering and shell effects of charge radii for nuclei with even Z from 36 to 38 and from 52 to 62

NUCLEAR STRUCTURE 72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102Kr, 74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Sr, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150Te, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156Xe, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162Ba, 126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158Ce, 126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160Nd, 130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165Sm; calculated charge radii and odd-even staggering (OES) effects by the relativistic mean field (RMF-BCS) and the modified RMF(BCS)* approaches; deduced no significant influence of neutron-proton short-range correlations (np-SRCs) for some nuclei due to the strong coupling between different levels around Fermi surface. Comparison with available experimental data.

doi: 10.1103/PhysRevC.105.014325
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2022AN12      Chin.Phys.C 46, 054101 (2022)

R.An, S.-S.Zhang, L.-S.Geng, F.-S.Zhang

Charge radii of potassium isotopes in the RMF (BCS)* approach

NUCLEAR STRUCTURE 37,38,39,40,41,42,43,44,45,46,47,48,49,50,51K; calculated odd-even staggerings of binding energies, and charge radii of potassium isotopes. Comparison with available data.

doi: 10.1088/1674-1137/ac4b5c
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2022AN16      Chin.Phys.C 46, 064101 (2022)

R.An, X.Jiang, L.-G.Cao, F.-S.Zhang

Evolution of nuclear charge radii in copper and indium isotopes

NUCLEAR STRUCTURE 57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81Cu, 99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139In; calculated rms charge radii using the relativistic mean field (RMF) model with NL3, PK1 and NL3* parameter sets. Comparison with experimental data.

doi: 10.1088/1674-1137/ac501a
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2022CH47      Eur.Phys.J. A 58, 168 (2022)

S.Cheng, W.Wu, L.Cao, F.-S.Zhang

Isospin effects on α decay and cluster radioactivity

RADIOACTIVITY 221Fr, 221,222,223,224Ra, 226Ra, 225Ac, 224Th(14C), 228Th(20O), 231Pa(23F), 230Th, 231Pa, 232,233,234,235U(24Ne), 233,235U(25Ne), 234U, 236U, 236,238Pu(28Mg), 236U, 238Pu(30Mg), 238Pu(32Si), 242Cm(34Si); calculated T1/2; deduced semi-empirical formula based on WKB barrier penetrability. Comparison with available data.

doi: 10.1140/epja/s10050-022-00825-4
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2022LI39      Phys.Rev. C 106, 014606 (2022)

J.-J.Li, N.Tang, Y.-H.Zhang, X.-R.Zhang, G.Zhang, F.-S.Zhang

Theoretical study on the production of neutron-rich transuranium nuclei with radioactive beams in multinucleon transfer reactions

NUCLEAR REACTIONS 248Cm(136Xe, X)229Pu/230Pu/231Pu/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/233Am/234Am/235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/261Es/262Es , E(cm)=533 MeV; 249Cf(136Xe, X)229Pu/230Pu/231Pu/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/230Am/231Am/232Am/233Am/234Am/235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/233Cm/234Cm/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/236Bk/237Bk/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es, E(cm)=526 MeV; 238U(92Kr, X)/229Np/230Np/231Np/232Np/233Np/234Np/235Np/236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf, E(cm)=357 MeV; 238U(132Sn, X), 230Np/231Np/232Np/233Np/234Np/235Np/236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np/245Np/246Np/247Np/248Np/249Np/250Np/251Np/252Np/253Np/254Np/255Np/232Pu/233Pu/234Pu/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/253Pu/254Pu/255Pu/256Pu/257Pu/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/255Am/256Am/257Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/256Cm/257Cm/258Cm/259Cm/260Cm/261Cm/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/260Bk/261Bk/262Bk/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cm/258Cm/259Cm/260Cm/261Cm/262Cm/263Cm/264Cm, E(cm)=478, 521, 564 MeV; 238U(144Xe, X), 236Np/237Np/238Np/239Np/240Np/241Np/242Np/243Np/244Np//245Np/246Np/247Np/248Np/249Np/250Np/235Pu/236Pu/237Pu/238Pu/239Pu/240Pu/241Pu/242Pu/243Pu/244Pu/245Pu/246Pu/247Pu/248Pu/249Pu/250Pu/251Pu/252Pu/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/251Am/252Am/253Am/254Am/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/253Cm/254Cm/255Cm/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/265Bk/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cm/258Cm/259Cm/260Cm/261Cm/262Cm, E(cm)=511 MeV; calculated σ of the isotopes production, driving potential during the transfer of nucleons. Dinuclear system model (DNS) calculations performed with GEMINI++ code. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.014606
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2022LI45      Phys.Rev. C 106, 024601 (2022)

L.-Q.Li, G.Zhang, F.-S.Zhang

Production of unknown Fl isotopes in proton evaporation channels within the dinuclear system model

NUCLEAR REACTIONS 243Am(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=190-225 MeV; 248Cm(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=195-220 MeV;249Bk(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=195-225 MeV;249Cf(48Ca, 3n), E(cm)=205-215 MeV;244Am(48Ca, np), (48Ca, 2np), (48Ca, 3np), (48Ca, 4np), E*=25-70 MeV; 255Es(36S, np), (36S, 2np), (36S, 3np), (36S, 4np), E*=25-70 MeV;239Pa(54Cr, np), (54Cr, 2np), (54Cr, 3np), (54Cr, 4np), E*=25-70 MeV; calculated evaporation residues σ(E). 255Es(36S, X), (34S, X), (36S, X), E*=20-70 MeV; calculated capture σ(E), driving potential as a function of the mass asymmetry, fusion probability, fission barrier. 255Es(36S, np), (36S, 2np), (36S, 3np), (36S, 4np), (36S, np), (34S, 2np), (34S, 3np), (34S, 4np), (32S, np), (32S, 2np), (32S, 3np), (32S, 4np)E*=25-70 MeV; calculated survival probability. 255Es(36S, np)289Fl, E*=37.2 MeV;255Es(36S, 2np)288Fl, E*=38.8 MeV; 255Es(36S, 3np)287Fl, E*=45.5 MeV;255Es(36S, 4np)286Fl, E*=53.8 MeV;243Am(48Ca, np)289Fl, E*=30.9 MeV;243Am(48Ca, 2np)288Fl, E*=37.3 MeV;243Am(48Ca, 3np)287Fl, E*=45.8 MeV;243Am(48Ca, 4np)286Fl, E*=55.1 MeV;239Pa(54Cr, np)291Fl, E*=33.6 MeV; 239Pa(54Cr, 2np)290Fl, E*=37.2 MeV;239Pa(54Cr, 3np)288Fl, E*=4.1 MeV;239Pa(54Cr, 4np)288Fl, E*=53.4 MeV;244Am(48Ca, np)290Fl, E*=30.9 MeV;244Am(48Ca, 2np)289Fl, E*=38.4 MeV;244Am(48Ca, 3np)288Fl, E*=45.8 MeV;244Am(48Ca, 4np)287Fl, E*=55.4 MeV; calculated production σ. Dinuclear system model. Comparison to available experimental data.

doi: 10.1103/PhysRevC.106.024601
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2022TA17      Phys.Rev. C 106, 034601 (2022)

N.Tang, X.-R.Zhang, J.-J.Li, P.-W.Wen, F.-S.Zhang

Production of unknown neutron-rich isotopes with Z=99-102 in multinucleon transfer reactions near the Coulomb barrier

NUCLEAR REACTIONS 248Cm(86Kr, X)235Am/236Am/237Am/238Am/239Am/240Am/241Am/242Am/243Am/244Am/245Am/246Am/247Am/248Am/249Am/250Am/235Cm/236Cm/237Cm/238Cm/239Cm/240Cm/241Cm/242Cm/243Cm/244Cm/245Cm/246Cm/247Cm/248Cm/249Cm/250Cm/251Cm/252Cm/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm , E(cm)=386 MeV; calculated capture probability, isotopic production σ, σ dependence on angular momentum of 251Es and 254Fm reaction products. 249Cf(112Sn, X)230Bk/231Bk/232Bk/233Bk/234Bk/235Bk/236Bk/237Bk/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/231Cf/232Cf/233Cf/234Cf/235Cf/236Cf/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/239Es/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/240Fm/241Fm/242Fm/243Fm/244Fm/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm, E=475 MeV; 249Cf(124Sn, X)238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/237Cf/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/239Es/240Es/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/240Fm/241Fm/242Fm/243Fm/244Fm/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/262Fm, E=468 MeV; 249Cf(132Sn, X)239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/255Bk/256Bk/257Bk/258Bk/259Bk/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/259Cf/260Cf/261Cf/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/260Es/261Es/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/262Fm/263Fm/264Fm/265Fm/250Md/251Md/252Md/253Md/254Md/255Md/256Md/257Md/258Md/259Md/260Md/261Md/262Md/263Md/264Md/265Md/266Md/253No/254No/255No/256No/257No/258No/259No/260No/261No/262No/263No/264No/265No/266No/267No/268No, E=463 MeV; calculated isotope production σ, driving potential. Theoretical framework of a hybrid model combining the dinuclear system model and the GRAZING model. Comparison to experimental data.

doi: 10.1103/PhysRevC.106.034601
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2022ZH40      Phys.Rev. C 106, L011602 (2022)

K.Zhao, Z.Liu, F.S.Zhang, N.Wang, J.Z.Duan

Distinct sequential and massive transfer processes for production of neutron-rich N ≈ 126 nuclei in 238U + 198Pt

NUCLEAR REACTIONS 238U(198Pt, X)204Pt/204Os/200Re/198W/195Ta, E=8.0 MeV/nucleon; calculated σ, σ(θ), nucleon exchange rates, average lifetimes of the composite systems, distributions of the average number of neutrons evaporated from primary fragments, kinetic energy distributions of primary fragments. Improved quantum molecular dynamics model (ImQMD). Investigated underlying mechanisms responsible for the enhanced production of new neutron-rich nuclei with neutron numbers around 126. Established the role of sequential transfer and massive transfer of nucleons in producing targetlike and projectile like fragments.

doi: 10.1103/PhysRevC.106.L011602
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2022ZH42      Phys.Rev. C 106, 014625 (2022)

Y.-H.Zhang, G.Zhang, J.-J.Li, Z.Liu, A.V.Yeremin, F.-S.Zhang

Production cross sections of 243-248No isotopes in fusion reactions

NUCLEAR REACTIONS 208Pb(48Ca, X), E(cm)=165-220 MeV; 238U(20Ne, X), E(cm)=95-14 MeV; 242Pu(16O, X), E(cm)=80-130 MeV; 232Th(26Mg, X), E(cm)=110-160 MeV; 208Pb(48Ca, 2n), E(cm)=170-245 MeV; 208Pb(48Ca, 3n), E(cm)=180-258 MeV; 208Pb(48Ca, 4n), E(cm)=190-275 MeV; 208Pb(48Ca, 5n), E(cm)=200-280 MeV; 208Pb(40Ca, 2n), E(cm)=160-190 MeV; 208Pb(40Ca, 3n), E(cm)=170-200 MeV; 208Pb(40Ca, 4n), E(cm)=175-215 MeV; 208Pb(40Ca, 5n), E(cm)=200-220 MeV; 208Pb(44Ca, 2n), E(cm)=170-200 MeV; 208Pb(44Ca, 3n), E(cm)=175-210 MeV; 208Pb(44Ca, 4n), E(cm)=175-215 MeV; 208Pb(44Ca, 5n), E(cm)=180-225 MeV; 233U(20Ne, 4n), E(cm)=90-135 MeV; 233U(20Ne, 5n), E(cm)=105-140 MeV; 233U(20Ne, n), E(cm)=115-140 MeV; 235U(20Ne, 4n), E(cm)=90-135 MeV; 235U(20Ne, 5n), E(cm)=100-140 MeV; 235U(20Ne, n), E(cm)=110-140 MeV; 238U(20Ne, 4n), E(cm)=90-135 MeV; 238U(20Ne, 5n), E(cm)=95-140 MeV; 238U(20Ne, n), E(cm)=105-140 MeV; calculated σ(E), time evolution of binding energies and root-mean-square charge radii for 48Ca and 208Pb, excitation functions, static barrier in collision, evolution density profile for heads-on collision, production σ for new isotopes - 243,244,245,246,247,248No.Improved quantum molecular dynamical model (ImQMD) incorporated with a statistical model and the dinuclear system (DNS) model calculations. Comparison to available experimental data.

doi: 10.1103/PhysRevC.106.014625
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2022ZH54      J.Phys.(London) G49, 095104 (2022)

X.-r.Zhang, G.Zhang, J.-j.Li, Z.Liu, Y.-x.Yang, F.-s.Zhang

Production mechanism and prediction cross sections of unknown neutron-rich 263-265, 267-269Lr isotopes in multinucleon transfer reactions based on the dinuclear system model

NUCLEAR REACTIONS 235U(40Ar, X), E(cm)=184.6 MeV; 249Bk(130Te, X)263Lr/264Lr/265Lr/267Lr/268Lr/269Lr, E(cm)=526.7 MeV; analyzed available data; calculated production σ.

doi: 10.1088/1361-6471/ac81df
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2021CH44      J.Phys.(London) G48, 095106 (2021)

S.Cheng, Z.Ge, L.Cao, F.-S.Zhang

Theoretical calculations of the nuclear deformation effects on α-decay half-lives for heavy and super-heavy nuclei

RADIOACTIVITY 172,174,176,178Hg, 178,180,182,184Pb, 186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218Po, 194,196,198,200,202,204,206,208,210,212,214,216,218,220,222Rn, 202,204,206,208,210,212,214,216,218,220,222,224,226Ra, 208,210,212,214,216,218,220,222,224,226,228,230Th, 216,218,220,222,224,226,228,230,232,234,236U, 228,230,232,234,236,238,240,242,244Pu, 240,242,244,246,248Cm, 238,240,242,244,246,248,250,252,254,256Cf, 242,244,246,248,250,252,254,256,258Fm, 252,254,256,258,260No, 254,256,258,260,262Rf, 258,260,262,264,266Sg, 264,266,268,270Hs, 270Ds, 280Ds, 282,284Cn, 284,286,288Fl, 290,292Lv, 294Og(α); calculated T1/2. Comparison with available data.

doi: 10.1088/1361-6471/ac165f
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2021CO10      Phys.Rev. C 104, 024603 (2021)

M.Colonna, Y.-X.Zhang, Y.-J.Wang, D.Cozma, P.Danielewicz, C.M.Ko, A.Ono, M.B.Tsang, R.Wang, H.Wolter, J.Xu, Z.Zhang, L.-W.Chen, H.-G.Cheng, H.Elfner, Z.-Q.Feng, M.Kim, Y.Kim, S.Jeon, C.-H.Lee, B.-A.Li, Q.-F.Li, Z.-X.Li, S.Mallik, D.Oliinychenko, J.Su, T.Song, A.Sorensen, F.-S.Zhang

Comparison of heavy-ion transport simulations: Mean-field dynamics in a box

doi: 10.1103/PhysRevC.104.024603
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2021WE03      Chin.Phys.C 45, 014105 (2021)

P.-W.Wen, S.-S.Zhang, L.G.Cao, F.-S.Zhang

Fully self-consistent calculation of β-decay half-lives within Skyrme energy density functional

RADIOACTIVITY 22,24O, 34,42Si, 52Ca, 68,78Ni, 82Ge, 102Sr, 104,110Zr, 132Sn, 150Ce(β-); calculated T1/2 using Skyrme HF plus charge-exchange RPA approach with SGII, LNS, SKX, and SAMi interactions. Comparison with experimental data.

doi: 10.1088/1674-1137/abc1d1
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2021ZH16      Phys.Rev. C 103, 024608 (2021)

X.-R.Zhang, G.Zhang, J.-J.Li, S.H.Cheng, Z.Liu, F.-S.Zhang

Effects of nucleus orientation on transfer process and production of unknown neutron-rich isotopes with Z = 62-75 in 204Hg + 232Th based on the dinuclear system model

NUCLEAR REACTIONS 166Er(86Kr, X), E(cm)=464 MeV; calculated mass and charge distributions of total kinetic energy (TKE) of the primary binary fragments. 232Th(204Hg, X)168Sm/169Sm/170Eu/171Eu/172Eu/172Gd/173Gd/174Gd/175Gd/175Tb/176Tb/177Tb/177Dy/178Dy/179Dy/180Dy/179Ho/180Ho/181Ho/182Ho/181Er/182Er/183Er/184Er/185Er/182Tm/183Tm/184Tm/185Tm/186Tm/187Tm/186Yb/187Yb/188Yb/189Yb/190Yb/189Lu/190Lu/191Lu/192Lu/193Lu/191Hf/192Hf/193Hf/194Hf/195Hf/195Ta/196Ta/197Ta/198W/199W/200Re/201Re/202Re, E(cm)=678.1 MeV; calculated potential energies for the tip-to-tip and side-to-side configurations, production σ. Dinuclear system (DNS) model. Comparison with available experimental data.

doi: 10.1103/PhysRevC.103.024608
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2021ZH19      Phys.Lett. B 815, 136101 (2021)

K.Zhao, Z.Liu, F.S.Zhang, N.Wang

Production of neutron-rich N=126 nuclei in multinucleon transfer reactions: Comparison between 136Xe + 198Pt and 238U + 198Pt reactions

NUCLEAR REACTIONS 198Pt(136Xe, X), (238U, X)204Pt/203Ir/202Os, E=8 MeV/nucleon; calculated production σ for primary and residual fragments using improved quantum molecular dynamics (ImQMD) model incorporated with the statistical evaporation model (HIVAP code).

doi: 10.1016/j.physletb.2021.136101
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2021ZH53      Phys.Rev.Lett. 127, 152702 (2021)

L.Y.Zhang, J.Su, J.J.He, M.Wiescher, R.J.deBoer, D.Kahl, Y.J.Chen, X.Y.Li, J.G.Wang, L.Zhang, F.Q.Cao, H.Zhang, Z.C.Zhang, T.Y.Jiao, Y.D.Sheng, L.H.Wang, L.Y.Song, X.Z.Jiang, Z.M.Li, E.T.Li, S.Wang, G.Lian, Z.H.Li, X.D.Tang, H.W.Zhao, L.T.Sun, Q.Wu, J.Q.Li, B.Q.Cui, L.H.Chen, R.G.Ma, B.Guo, S.W.Xu, J.Y.Li, N.C.Qi, W.L.Sun, X.Y.Guo, P.Zhang, Y.H.Chen, Y.Zhou, J.F.Zhou, J.R.He, C.S.Shang, M.C.Li, X.H.Zhou, Y.H.Zhang, F.S.Zhang, Z.G.Hu, H.S.Xu, J.P.Chen, W.P.Liu

Direct Measurement of the Astrophysical 19F(p, αγ)16O Reaction in the Deepest Operational Underground Laboratory

NUCLEAR REACTIONS 19F(p, α), E(cm)=72.4-188.8 keV; measured reaction products, Eγ, Iγ; deduced yields, S-factors, reaction rates. The China Jinping Underground Laboratory (CJPL), JUNA accelerator.

doi: 10.1103/physrevlett.127.152702
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2020GE06      Chin.Phys.C 44, 104102 (2020)

Z.Ge, G.Zhang, S.Cheng, Yu.S.Tsyganov, F.-S.Zhang

Calculations of the α-decay properties of Z = 120, 122, 124, 126 isotopes

RADIOACTIVITY 285,286,287,288,289Fl, 287,288,289,290Mc, 290,291,292,293Lv, 293,294Ts, 294Og, 287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339120, 294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339122, 300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339124, 306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339126(α); calculated Q-values, T1/2 using the generalized liquid drop model (GLDM), Royer's formula, and universal decay law (UDL). Comparison with available data.

doi: 10.1088/1674-1137/abab00
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2020SU02      Phys.Lett. B 800, 135096 (2020)

M.D.Sun, Z.Liu, T.H.Huang, W.Q.Zhang, A.N.Andreyev, B.Ding, J.G.Wang, X.Y.Liu, H.Y.Lu, D.S.Hou, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, A.H.Feng, C.J.Lin, L.J.Sun, N.R.Ma, W.Zuo, H.S.Xu, X.H.Zhou, G.Q.Xiao, C.Qi, F.S.Zhang

Fine structure in the α decay of 223U

RADIOACTIVITY 223U, 219Th, 215Ra(α) [from 187Re(40Ar, 3np), E=188 MeV]; measured reaction products, Eα, Iα; deduced α-decay branches, fine structure.

doi: 10.1016/j.physletb.2019.135096
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Data from this article have been entered in the XUNDL database. For more information, click here.

2020SU18      Chin.Phys.C 44, 084106 (2020)

J.Su, L.Zhu, C.Guo, F.-S.Zhang

Isospin dependence of projectile fragmentation at hundreds of MeV/u

NUCLEAR REACTIONS 120Sn(124Sn, X), (107Sn, X), E=600 MeV/nucleon; 208Pb(136Xe, X), (124Xe, X), E=1000 MeV/nucleon; analyzed available data; deduced isospin observables, neutron-to-proton ratios of the light particles emitted from the fragmenting. Isospin-dependent quantum molecular dynamics (IQMD) model and permitting only evaporation in the statistical model GEMINI, the IQMD+GEMINI model.

doi: 10.1088/1674-1137/44/8/084106
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2020WA16      Nucl.Instrum.Methods Phys.Res. A971, 164068 (2020)

X.Wang, Z.H.Li, Z.Liu, J.Li, H.Hua, H.Y.Lu, W.Q.Zhang, T.H.Huang, M.D.Sun, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, C.J.Lin, L.J.Sun, N.R.Ma, H.S.Xu, X.H.Zhou, G.Q.Xiao, H.Y.Wu, C.Xu, S.Q.Zhang, X.Q.Li, R.Han, Z.Q.Chen, C.G.Wu, D.W.Luo, Y.Jin, J.Lin, D.X.Jiang, Y.L.Ye, F.S.Zhang

An effective digital pulse processing method for pile-up pulses in decay studies of short-lived nuclei

RADIOACTIVITY 219Th(α), 210,211Ra(IT) [from 175Lu, 186W, 187Re(40Ar, X), E=188 MeV]; measured decay products, Eα, Iα; deduced α spectra, proper baseline correction, standard pulse construction and plateau-region fitting, spectroscopic information of overlapping signals.

doi: 10.1016/j.nima.2020.164068
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2020ZH18      Bull.Rus.Acad.Sci.Phys. 84, 485 (2020)

G.Zhang, C.A.T.Sokhna, F.S.Zhang

The Production of the Isotopes with Z = 98-106 in the Multinucleon Transfer Reaction 238U + 251Cf

doi: 10.3103/S106287382004036X
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2020ZH22      Int.J.Mod.Phys. E29, 2030004 (2020)

L.Zhu, C.Li, C.-C.Guo, J.Su, P.W.Wen, G.Zhang, F.-S.Zhang

Theoretical progress on production of isotopes in the multinucleon transfer process

NUCLEAR REACTIONS 238U(64Ni, X), E(cm)=307.5 MeV; 208Pb(124Xe, X), E(cm)=50 MeV; 186W(160Gd, X), E=503 MeV; calculated transfer σ for production of neutron-rich transuranium nuclei.

doi: 10.1142/S0218301320300040
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2020ZH28      Phys.Rev. C 102, 024617 (2020)

G.Zhang, J.-J.Li, X.-R.Zhang, B.Li, C.A.T.Sokhna, C.Wang, Z.Liu, F.-S.Zhang

Role of the quasifission yields in the multinucleon transfer reactions of 136Xe + 208Pb

NUCLEAR REACTIONS 208Pb(136Xe, X), (136Xe, F), E(cm)=526 MeV; calculated mass distributions with and without the quasifission yields, σ(A) as function of the angular momentum, production σ of Hg, Pb, and Po isotopes contributed from quasifission yields, quasifission yields and excitation energies of 202Hg and 208Hg, isotopic distribution σ(Z) of Hg, Pb and Po isotopes. Dinuclear system (DNS) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.024617
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2019GE08      Eur.Phys.J. A 55, 166 (2019)

Z.Ge, G.Zhang, S.Cheng, Y.Li, N.Su, W.Guo, Yu.S.Tsyganov, F.-S.Zhang

Theoretical predictions for α-decay properties of 283-339Og using a shell-effect induced generalized liquid-drop model

RADIOACTIVITY Sg, Bh, Hs, Mt, Ds, Rg, Cn, Nh, Fl, Mc, Lv, Ts, Og(α) [all known isotopes]; compiled Qα, T1/2 available experimental values and calculations using Royer's formula, Universal Decay Law (UDL), Generalized Liquid-Drop Model (GLDM) with and without shell correction; calculated 283-339Og α-particle preformation factor.

doi: 10.1140/epja/i2019-12864-5
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2019LI08      Phys.Rev. C 99, 024602 (2019)

C.Li, X.Xu, J.Li, G.Zhang, B.Li, C.A.T.Sokhna, Z.Ge, F.Zhang, P.Wen, F.-S.Zhang

Production of new neutron-rich heavy nuclei with Z=56--80 in the multinucleon transfer reactions of 136Xe + 198Pt

NUCLEAR REACTIONS 198Pt(136Xe, X), E=5.25, 6.20, 7.98, 10.0, 15.0 MeV/nucleon; calculated σ(E) for isotopic distribution of primary and secondary fragments in A=110-230 and Z=52, 54, 56, 74, 76, 78, 80, 82, 84 region, average energy difference after multi-nucleon transfer (MNT), average excitation energy of primary target like fragments as a function of mass number, differential σ(θ) of secondary target like fragments: 198,200,202,204,206Pt, 196,198,200,202,204Os, 190,192,194,196,198W, 186,188,190,192,194Hf. Improved quantum molecular dynamics (ImQMD), ImQMD+GEMINI and GRAZING calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.024602
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2019LI13      Phys.Rev. C 99, 034619 (2019)

C.Li, C.A.T.Sokhna, X.Xu, J.Li, G.Zhang, B.Li, Z.Ge, F.-S.Zhang

Isospin equilibration in multinucleon transfer reaction at near-barrier energies

NUCLEAR REACTIONS 208Pb(124Xe, X), E(cm)=450 MeV; calculated single-particle potentials of neutrons and protons, time evolution of density profiles and isospin asymmetry, and neutron and proton transfer coefficients for the neutron and proton as function of symmetry energy coefficients. 208Pb(58Ni, X), E=328.4, 345 MeV; calculated isotope production σ(E) from Mn to Ni, total kinetic energy TKE-mass distributions and N/Z ratios of primary binary fragments. Improved quantum molecular dynamics model (ImQMD). Comparison with experimental values for 208Pb(58Ni, X) reaction.

doi: 10.1103/PhysRevC.99.034619
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2019ON02      Phys.Rev. C 100, 044617 (2019)

A.Ono, J.Xu, M.Colonna, P.Danielewicz, C.M.Ko, M.B.Tsang, Y.-J.Wang, H.Wolter, Y.-X.Zhang, L.-W.Chen, D.Cozma, H.Elfner, Z.-Q.Feng, N.Ikeno, B.-A.Li, S.Mallik, Y.Nara, T.Ogawa, A.Ohnishi, D.Oliinychenko, J.Su, T.Song, F.-S.Zhang, Z.Zhang

Comparison of heavy-ion transport simulations: Collision integral with pions and Δ resonances in a box

doi: 10.1103/PhysRevC.100.044617
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2019WE04      Phys.Rev. C 99, 034606 (2019)

P.W.Wen, C.J.Lin, C.Li, L.Zhu, F.Zhang, F.S.Zhang, H.M.Jia, F.Yang, N.R.Ma, L.J.Sun, D.X.Wang, F.P.Zhong, H.H.Sun, L.Yang, X.X.Xu

Evaporation and fission of the primary fragments produced by multinucleon transfer reactions

NUCLEAR REACTIONS 238U(64Ni, X), E(cm)=307.5 MeV; 238U(238U, X), E=1628, 1785, 2059 MeV; 248Cm(136Xe, X), E=769 MeV; calculated isotopic production σ using GRAZING model with GEMINI++ statistical-decay model for multinucleon transfer (MNT) reactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.034606
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2019XU06      Chin.Phys.C 43, 064105 (2019)

X.-X.Xu, G.Zhang, J.-J.Li, B.Li, C.A.T.Sokhna, X.-R.Zhang, X.-X.Yang, S.-H.Cheng, Y.-H.Zhang, Z.-S.Ge, C.Li, Z.Liu, F.-S.Zhang

Production of exotic neutron-deficient isotopes near N, Z = 50 in multinucleon transfer reactions

NUCLEAR REACTIONS 124Sn(40Ca, X), E=128.5 MeV; 112Sn(48Ca, X), (40Ca, X), (58Ni, X), (106Cd, X), E(cm)=280 MeV; 112Sn(106Cd, X)101Sb/112Sb/103Te/106I/107I, E(cm)=300, 500, 780 MeV; calculated production σ. Comparison with experimental data.

doi: 10.1088/1674-1137/43/6/064105
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2019ZH37      Phys.Rev. C 100, 024603 (2019)

F.Zhang, C.Li, P.-W.Wen, J.-W.Liu, J.Su, F.-S.Zhang

Time dependence of the thermal-photon thermometer

NUCLEAR REACTIONS 190W, 197Au(36Ar, X), E=60 MeV/nucleon; 168Er(36Ar, X), E=30 MeV/nucleon; 171Yb(36Ar, X), E=35, 40 MeV/nucleon; 176Lu(36Ar, X), E=40 MeV/nucleon; 188Os(36Ar, X), E=55, 60, 65 MeV/nucleon; 206Bi, 206Rn, 204Hg(36Ar, X), E=95 MeV/nucleon; calculated the time dependence of density contours, photon production rates, temperatures, mass, N/Z ratio, quadrupole moment. Systematic study of the thermal-photon thermometer via the isospin-dependent quantum molecular dynamics (IQMD) model.

doi: 10.1103/PhysRevC.100.024603
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2019ZH38      Phys.Rev. C 100, 024613 (2019)

G.Zhang, C.A.T.Sokhna, Z.Liu, F.-S.Zhang

Production of neutron-rich isotopes 264, 266, 268, 269Rf by multinucleon transfer reactions based on 238U beam

NUCLEAR REACTIONS 248Cm(238U, X), E=1760 MeV; calculated production cross sections of Z=97-100, A=235-265 isotopes, and compared to experimental data. 248Cf(238U, X), E(cm)=847.1 MeV; 249Bk(238U, X), E(cm)=892.1 MeV; 252Cf(238U, X), E(cm)=889.6 MeV; calculated production cross sections and driving potentials of A=250-271 Rf isotopes. 252Cf(238U, X), E(cm)=889.6 MeV; calculated N/Z ratio distribution of primary fragments as function of angular momentum, primary and final production cross sections of A=255-270 Rf isotopes. 252Cf(238U, X), E(cm)=849.1, 889.6, 970.4 MeV; calculated primary and final production cross sections of A=250-275 Rf isotopes. 248Cf(238U, X)264Rf/266Rf/268Rf/269Rf, E(cm)=847.1 MeV; 249Bk(238U, X)264Rf/266Rf/268Rf/269Rf, E(cm)=892.1 MeV; 252Cf(238U, X)264Rf/266Rf/268Rf/269Rf, E(cm)=849.1, 889.6, 970.4 MeV; calculated counts per day for 264,266,268,269Rf isotopes, with the highest counts for 238U+252Cf reaction. Dinuclear system (DNS) model with GEMINI++ code.

doi: 10.1103/PhysRevC.100.024613
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2018GE06      Phys.Rev. C 98, 034312 (2018)

Z.Ge, C.Li, J.Li, G.Zhang, B.Li, X.Xu, C.A.T.Sokhna, X.Bao, H.Zhang, Yu.S.Tsyganov, F.-S.Zhang

Effect of shell corrections on the α-decay properties of 280-305Fl isotopes

RADIOACTIVITY 280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305Fl(α), (SF); calculated Q(α) and half-lives using GLDM, the GLDM with shell correction, the UFM and the Royer's formula, and shell correction energies of the even-even nuclei. 285,286,287,288,289Fl, 281,283,285Cn, 277,279,281Ds, 273,275Hs, 269,271Sg(α); calculated T1/2 using Royer's, UDL, UFM, and GLDM formulas, and by input of experimental Q(α) values. Comparison with experimental values.

doi: 10.1103/PhysRevC.98.034312
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2018HU13      Phys.Rev. C 98, 044302 (2018)

T.H.Huang, W.Q.Zhang, M.D.Sun, Z.Liu, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, H.Y.Lu, A.H.Feng, C.J.Lin, L.J.Sun, N.R.Ma, D.X.Wang, F.S.Zhang, W.Zuo, X.H.Zhou, H.S.Xu, G.Q.Xiao

Identification of the new isotope 224Np

NUCLEAR REACTIONS 187Re(40Ar, 3n)224Np, E=188 MeV; measured evaporation residues (ERs), Eα, Iα of decaying ERs, production σ using SHANS separator and a double-sided silicon strip detector for α detection at SFC-HIRFL, Lanzhou; deduced evidence for the production of new isotope 224Np through the observation of six correlated α-decay chains, starting from 224Np to 212Fr.

RADIOACTIVITY 224Np, 220Pa, 220mPa, 216Ac(α)[from 187Re(40Ar, 3n)224Np, E=188 MeV, and successive α decays]; measured Eα, Iα, half-lives, αα-correlations. 220Pa, 216Ac, 212Fr; deduced levels, isomer in 220Pa.

doi: 10.1103/PhysRevC.98.044302
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2018LI02      Phys.Lett. B 776, 278 (2018)

C.Li, P.Wen, J.Li, G.Zhang, B.Li, X.Xu, Z.Liu, S.Zhu, F.-S.Zhang

Production mechanism of new neutron-rich heavy nuclei in the 136Xe + 198Pt reaction

NUCLEAR REACTIONS 136Xe(198Pt, X)199Pt/203Pt/208Pt, E=7.98 MeV/nucleon; analyzed available data; calculated σ.

doi: 10.1016/j.physletb.2017.11.060
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2018LI34      Phys.Rev. C 98, 014626 (2018)

J.Li, C.Li, G.Zhang, B.Li, X.Xu, Z.Liu, Yu.S.Tsyganov, F.-S.Zhang

Theoretical study on production of unknown neutron-deficient 280-283Fl and neutron-rich 290-292Fl isotopes by fusion reactions

NUCLEAR REACTIONS 239,240,242,244Pu(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=25-65 MeV; 242Pu(44Ca, 2n), (44Ca, 3n), (44Ca, 4n), (44Ca, 5n), E*=30-70 MeV; 249Cf(36S, 2n), (36S, 3n), (36S, 4n), (36S, 5n), E*=30-70 MeV; 250Cm(44Ar, 4n), (44Ar, 5n), E*=30-65 MeV; 248,250Cm(46Ar, 3n), (46Ar, 4n), (46Ar, 5n); calculated evaporation residue σ(E) using dinuclear system (DNS) model. 280,281,282,283,291,292,293Fl; calculated production cross sections using hot fusion reaction mechanism. Comparison with available experimental data.

doi: 10.1103/PhysRevC.98.014626
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2018LI46      Phys.Lett. B 784, 392 (2018)

X.Y.Liu, Z.Liu, B.Ding, P.Doornenbal, A.Obertelli, S.M.Lenzi, P.M.Walker, L.X.Chung, B.D.Linh, G.Authelet, H.Baba, D.Calvet, F.Chateau, A.Corsi, A.Delbart, J.-M.Gheller, A.Gillibert, T.Isobe, V.Lapoux, M.Matsushita, S.Momiyama, T.Motobayashi, M.Niikura, F.Nowacki, H.Otsu, C.Peron, A.Peyaud, E.C.Pollacco, J.-Y.Rousse, H.Sakurai, M.Sasano, Y.Shiga, S.Takeuchi, R.Taniuchi, T.Uesaka, H.Wang, K.Yoneda, Y.H.Lam, T.H.Huang, M.D.Sun, W.Q.Zhang, H.Y.Lu, D.S.Hou, F.Browne, Zs.Dombradi, S.Franchoo, F.Giacoppo, A.Gottardo, K.Hadynska-Klek, Z.Korkulu, S.Koyama, Y.Kubota, J.Lee, M.Lettmann, R.Lozeva, K.Matsui, T.Miyazaki, S.Nishimura, C.Louchart, L.Olivier, S.Ota, Z.Patel, E.Sahin, C.Santamaria, C.Shand, P.-A.Soderstrom, G.L.Stefan, D.Steppenbeck, T.Sumikama, D.Suzuki, Zs.Vajta, V.Werner, J.Wu, Z.Xu, X.H.Zhou, Y.H.Zhang, H.S.Xu, F.S.Zhang

Spectroscopy of 65, 6725Mn: Strong coupling in the N=40 "island of inversion"

NUCLEAR REACTIONS 1H(68Fe, X)63Mn/65Mn/67Mn, E=260 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π. Comparison with shell model predictions.

doi: 10.1016/j.physletb.2018.06.067
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2018SU12      Phys.Rev. C 98, 014610 (2018)

J.Su, W.Trautmann, L.Zhu, W.-J.Xie, F.-S.Zhang

Dynamical properties and secondary decay effects of projectile fragmentations in 124Sn, 107Sn + 120Sn collisions at 600 MeV/nucleon

NUCLEAR REACTIONS 120Sn(124Sn, X), (107Sn, X), E=600 MeV/nucleon; calculated mass number and excitation energy of fragments, longitudinal momenta, mean multiplicity of intermediate mass fragments (IMFs), σ(Z) of fragments, mean neutron-to-proton ratios of light fragments. Isospin-dependent quantum molecular dynamics model (IQMD) with and without the GEMINI statistical code. Comparison with experimental data for fragment yields from ALADIN Collaboration.

doi: 10.1103/PhysRevC.98.014610
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2018XI05      Phys.Rev. C 97, 064608 (2018)

W.-J.Xie, J.Su, L.Zhu, F.-S.Zhang

Effects of the pion-nucleon potential in 197Au + 197Au collisions at 1.5 GeV/nucleon

NUCLEAR REACTIONS 197Au(197Au, X), E=1.5 GeV/nucleon; calculated pion multiplicity, excitation function of pion multiplicity, rapidity distributions of directed and elliptic flows, rapidity dependence of the and centrality dependence of midrapidity and elliptic flows, polar angle distributions of π+ and π-, transverse momentum dependence of the strength function of the azimuthal anisotropy, using isospin-dependent quantum molecular dynamics (IQMD) model using various sets of the pion-nucleon (πN) potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.064608
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2018XI07      Chin.Phys.C 42, 104103 (2018)

W.-J.Xie, F.-S.Zhang

Effects of density- and momentum-dependent potentials in Au+Au collisions at intermediate energies

NUCLEAR REACTIONS 197Au(197Au, X), E=90, 120, 150, 400 MeV/nucleon; analyzed available data; calculated directed flow and elliptic flow for protons using isospin-dependent transport model, the effects of the density- and momentum-dependent potentials.

doi: 10.1088/1674-1137/42/10/104103
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2018ZH21      Chin.Phys.C 42, 054107 (2018)

D.-H.Zhang, F.-S.Zhang

Fragment distribution in 78, 86Kr + 181Ta reactions

NUCLEAR REACTIONS 181Ta(86Kr, X), E=80, 120, 160 MeV/nucleon; 181Ta(78Kr, X), E=160 MeV/nucleon; calculated fragment σ within the framework of the isospin-dependent quantum molecular dynamics model, along with the GEMINI model. Comparison with available data.

doi: 10.1088/1674-1137/42/5/054107
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2018ZH30      Phys.Rev. C 98, 014613 (2018)

G.Zhang, C.Li, P.-W.Wen, J.-J.Li, X.-X.Xu, B.Li, Z.Liu, F.-S.Zhang

Production of neutron-rich 209-212Pt isotopes based on a dinuclear system model

NUCLEAR REACTIONS 208Pb(64Ni, X)180Os/181Os/182Os/183Os/184Os/185Os/186Os/187Os/188Os/189Os/190Os/191Os/192Os/193Os/194Os/195Os/196Os/187Pt/188Pt/189Pt/190Pt/191Pt/192Pt/193Pt/194Pt/195Pt/196Pt/197Pt/198Pt/199Pt/200Pt/201Pt/202Pt/192Hg/193Hg/194Hg/195Hg/196Hg/197Hg/198Hg/199Hg/200Hg/201Hg/202Hg/203Hg/204Hg/205Hg/206Hg/207Hg, E(cm)=268 MeV; calculated isotopic production σ, and cross sections for production of A=50 to 200 masses. 208Pb(133Sn, X), (145Xe, X), (238U, X), E(cm)=1.10Vc; calculated driving potential for neutron pickup and stripping channels. 198Pt, 204Hg, 208Pb(133Sn, X), 208Pb(145Xe, X), (238U, X)190Pt/191Pt/192Pt/193Pt/194Pt/195Pt/196Pt/197Pt/198Pt/199Pt/200Pt/201Pt/202Pt/203Pt/204Pt/205Pt/206Pt/207Pt/208Pt/209Pt, E(cm)=1.10Vc; calculated production σ for Pt isotopes. 209,210,211,212Pt; calculated production cross sections in 208Pb+145Xe and 204Hg+133Sn reactions via multinucleon transfer reactions. Dinuclear system (DNS) model. Comparison with available experimental data.

doi: 10.1103/PhysRevC.98.014613
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2018ZH49      Eur.Phys.J. A 54, 180 (2018)

F.Zhang, C.Li, P.-W.Wen, J.-W.Liu, F.-S.Zhang

Thermal bremsstrahlung photons probing the isospin dependence of the nuclear temperatures

doi: 10.1140/epja/i2018-12621-4
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2017HU08      Phys.Rev. C 96, 014324 (2017)

T.H.Huang, W.Q.Zhang, M.D.Sun, Z.Liu, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, H.Y.Lu, C.J.Lin, L.J.Sun, N.R.Ma, Z.Z.Ren, F.S.Zhang, W.Zou, X.H.Zhou, H.S.Xu, G.Q.Xiao

α-decay chain of the short-lived isotope 220Pa established using a digital pulse processing technique

RADIOACTIVITY 220Pa(α)[from 187Re(40Ar, 3nα), E=188 MeV at HIRFL-Lanzhou facility]; 216Ac(α)[from 220Pa parent decay]; measured Eα, (evaporation residue)α-correlated events using the digital pulse processing technique, half-lives of decays of 220Pa and 216Ac; deduced J, π of the ground state of 220Pa, and reduced α-decay width. Comparison with previous experimental Eα and T1/2 for 220Pa.

doi: 10.1103/PhysRevC.96.014324
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2017LI16      Phys.Rev. C 95, 054612 (2017)

J.Li, C.Li, G.Zhang, L.Zhu, Z.Liu, F.-S.Zhang

Production cross sections of neutron-rich 261-263No isotopes

NUCLEAR REACTIONS 208Pb(48Ca, X), E*=10-45 MeV; 244Pu(18O, X), (22O, 4n), E*=30-70 MeV; calculated capture σ(E*). Compared with experimental data for 208Pb+48Ca. 244Pu(18O, 3n), (18O, 4n), (18O, 5n), 244Pu(22O, 3n), (22O, 4n), (22O, 5n), E*(CN)=20-80 MeV; calculated survival probabilities. 208Pb(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*(CN)=10-55 MeV; 228,230Th(26Mg, 3n), (26Mg, 4n), (26Mg, 5n), E*(CN)=35-75 MeV; 242,244Pu(18O, 3n), (18O, 4n), (18O, 5n), (22O, 3n), (22O, 4n), (22O, 5n), E*(CN)=30-80 MeV; calculated σ(E). 228Th(26Mg, 5n)249No, E=164.9 MeV; 204Pb(48Ca, 2n)250No, E=216.7 MeV; 206Pb(48Ca, 4n)250No, E=242.2 MeV; 228Th(26Mg, 4n)250No, E=140.4 MeV; 206Pb(48Ca, 3n)251No, E=226.2 MeV; 244Cm(12C, 5n)251No, E=83.0 MeV; 206Pb(48Ca, 2n)252No, E=217.1 MeV; 230Th(26Mg, 4n)252No, E=135.8 MeV; 244Cm(12C, 4n)252No, E=73.3 MeV; 206Pb(48Ca, n)253No, E=217.4 MeV; 207Pb(48Ca, 2n)253No, E=216.7 MeV; 230Th(26Mg, 3n)253No, E=133.6 MeV; 244Cm(13C, 4n)253No, E=72.8 MeV; 246Cm(12C, 5n)253No, E=83.0 MeV; 208Pb(48Ca, 2n)254No, E=216.7 MeV; 244Cm(13C, 3n)254No, E=69.8 MeV; 246Cm(12C, 4n)254No, E=72.0 MeV; 246Cm(13C, 5n)254No, E=78.5 MeV; 242Pu(18O, 5n)255No, E=106.8 MeV; 246Cm(13C, 4n)255No, E=69.5 MeV; 248Cm(12C, 5n)255No, E=77.8 MeV; 242Pu(18O, 4n)256No, E=93.9 MeV; 246Cm(13C, 3n)256No, E=67.5 MeV; 248Cm(12C, 4n)256No, E=71.2 MeV; 248Cm(13C, 5n)256No, E=74.8 MeV; 242Pu(18O, 3n)257No, E=91.8 MeV; 244Pu(18O, 5n)257No, E=105.8 MeV; 248Cm(12C, 3n)257No, E=69.2 MeV; 248Cm(13C, 4n)257No, E=70.5 MeV; 244Pu(18O, 4n)258No, E=95.0 MeV; 248Cm(13C, 3n)258No, E=71.1 MeV; 242Pu(22O, 5n)259No, E=106.9 MeV; 244Pu(18O, 3n)259No, E=90.7 MeV; 242Pu(22O, 4n)260No, E=93.8 MeV; 242Pu(22O, 3n)261No, E=91.6 MeV; 244Pu(22O, 5n)261No, E=100.8 MeV; 244Pu(22O, 4n)262No, E=92.1 MeV; 244Pu(22O, 3n)263No, E=89.9 MeV; calculated production σ, and compared with experimental data. Dinuclear system (DNS) model for fusion-evaporation (FE) reaction.

doi: 10.1103/PhysRevC.95.054612
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2017SU18      Phys.Lett. B 771, 303 (2017)

M.D.Sun, Z.Liu, T.H.Huang, W.Q.Zhang, J.G.Wang, X.Y.Liu, B.Ding, Z.G.Gan, L.Ma, H.B.Yang, Z.Y.Zhang, L.Yu, J.Jiang, K.L.Wang, Y.S.Wang, M.L.Liu, Z.H.Li, J.Li, X.Wang, H.Y.Lu, C.J.Lin, L.J.Sun, N.R.Ma, C.X.Yuan, W.Zuo, H.S.Xu, X.H.Zhou, G.Q.Xiao, C.Qi, F.S.Zhang

New short-lived isotope 223Np and the absence of the Z = 92 subshell closure near N = 126

RADIOACTIVITY 223Np, 219Pa, 219Th, 218Ac, 216Ra, 215Ac(α) [from 187Re(40Ar, X)223Np, E=188 MeV]; measured decay products, Eα, Iα; deduced T1/2, Q-values, disprove the existence of a Z=92 subshell closure. Comparison with available data.

doi: 10.1016/j.physletb.2017.03.074
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2017SU23      Phys.Rev. C 96, 024601 (2017)

J.Su, L.Zhu, C.-Y.Huang, W.-J.Xie, F.-S.Zhang

Effects of symmetry energy and effective k-mass splitting on central 96Ru(96Zr) + 96Zr(96) collisions at 50 to 400 MeV/nucleon

NUCLEAR REACTIONS 96Ru(96Zr, X), 96Zr(96Ru, X), E=50-400 MeV/nucleon; calculated slope and quantum temperatures, np, nn, and pp collisions as a function of time, observable n/p ratio from the free neutrons and protons as a function of rapidity; investigated isospin mixing in central heavy-ion collisions (HICs). Isospin-dependent quantum molecular dynamics model in combination with the statistical decay code GEMINI. Comparison with experimental data from FOPI Collaboration.

doi: 10.1103/PhysRevC.96.024601
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2017WE04      Chin.Phys.C 41, 064102 (2017)

P.-W.Wen, Z.-Q.Feng, F.Zhang, C.Li, C.-J.Lin, F.-S.Zhang

Effect of positive Q-value neutron transfers on sub-barrier fusion reactions

NUCLEAR REACTIONS 90,94,96Zr(40Ca, X), E<100 MeV/nucleon; calculated fusion σ, Q-values of ground state to ground state neutron transfers. Modified quantum coupled channels model with all order couplings (CCFULL).

doi: 10.1088/1674-1137/41/6/064102
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2017WE14      J.Phys.(London) G44, 115101 (2017)

P.-w.Wen, C.Li, L.Zhu, C.Lin, F.-s.Zhang

Mechanism of multinucleon transfer reaction based on the GRAZING model and DNS model

NUCLEAR REACTIONS 208Pb(136Xe, X), E(cm)=450 MeV; 238U(64Ni, X), E(cm)=307 MeV; calculated isotopic production σ of transfer products using GRAZING model, DNS model and the summation of the GRAZING and DNS models.

doi: 10.1088/1361-6471/aa8b07
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2017ZH21      Nucl.Phys. A964, 93 (2017)

L.Zhu, J.Su, F.-S.Zhang

Theoretical predictions on production of neutron-deficient nuclei with Z ≥ 93 in multinucleon transfer reactions

NUCLEAR REACTIONS 233U(58Ni, x), E(cm)=1.2, 1.3, 1.4 Coulomb barrier;238U(58Ni, x), (64Ni, x), E(cm)=1.3 Coulomb barrier;245Cm(40Ca, x), E(cm)=1.2, 1.3, 1.4 Coulomb barrier; calculated production σ of some neutron-deficient actinide isotopes; deduced feasible ways to produce neutron-deficient actinide nuclei in future.

doi: 10.1016/j.nuclphysa.2017.05.063
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2017ZH32      Phys.Rev. C 96, 024606 (2017)

L.Zhu, F.-S.Zhang, P.-W.Wen, J.Su, W.-J.Xie

Production of neutron-rich nuclei with Z=60-73 in reactions induced by Xe isotopes

NUCLEAR REACTIONS 238U(136Xe, X), E(cm)=636 MeV; calculated production σ for A=122-150 Ba, Cs, Te and I isotopes, and compared with experimental data. 238U(124Xe, X), (136Xe, X), (144Xe, X), E(cm)=473-493 MeV; calculated production σ for target-like fragments (TLFs) with A=206-250, Z=88-96 neutron-rich isotopes, PES as functions of Z and N in 144Xe+238U reaction, yield distributions of total primary fragments as a function of their N/Z ratio for 124Xe+238U and 144Xe+238U reactions. 160Gd, 170Er, 186W(136Xe, X), (144Xe, X), E(cm)=353-406 MeV; calculated production σ for A=140-190, Z=60-73 neutron-rich isotopes. Dinuclear system model.

doi: 10.1103/PhysRevC.96.024606
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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
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2016LI24      Nucl.Phys. A952, 18 (2016)

C.Li, S.R.Souza, M.B.Tsang, F.-S.Zhang

Nuclear energy release from fragmentation

NUCLEAR STRUCTURE 230,232Th, 235,238U; calculated energy release for fission or splitting into fragments with nearly equal size; deduced maximal energy release at splitting into three fragments.

doi: 10.1016/j.nuclphysa.2016.04.002
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2016SU18      Eur.Phys.J. A 52, 207 (2016)

J.Su, C.-Y.Huang, W.-J.Xie, F.-S.Zhang

Effects of in-medium nucleon-nucleon cross sections on stopping observable and ratio of free protons in heavy-ion collisions at 400 MeV/nucleon

NUCLEAR REACTIONS 96Zr, 96Ru(96Ru, x), E=400 MeV/nucleon; calculated in-medium factors vs energy and vs density using IQMD (Isospin-dependent Quantum Molecular Dynamics); deduced isospin effect using comparison with data.

doi: 10.1140/epja/i2016-16207-x
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2016SU21      Phys.Rev. C 94, 034619 (2016)

J.Su, L.Zhu, C.-Y.Huang, W.-J.Xie, F.-S.Zhang

Correlation between symmetry energy and effective k-mass splitting with an improved isospin- and momentum-dependent interaction

NUCLEAR REACTIONS 124Sn(124Sn, X), 112Sn(112Sn, X), E=50, 120 MeV/nucleon; analyzed double ratios of the coalescence invariant neutron and proton spectra in central collisions; extracted isospin transport ratios from the yield ratios of A=7 isotopes using IQMD+GEMINI model.

doi: 10.1103/PhysRevC.94.034619
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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
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2016ZH23      Phys.Rev. C 93, 064610 (2016)

L.Zhu, J.Su, F.-S.Zhang

Influence of the neutron numbers of projectile and target on the evaporation residue cross sections in hot fusion reactions

NUCLEAR REACTIONS 238U(34S, 3n)269Hs, 238U(34S, 4n)268Hs, 238U(34S, 5n)267Hs, 238U(36S, 3n)272Hs, 238U(36S, 4n)271Hs, 238U(36S, 5n)270Hs, E(cm)=140-210 MeV; 238Pu(48Ca, 3n)283Fl, 238Pu(48Ca, 4n)282Fl, 238Pu(48Ca, 5n)281Fl, 239Pu(48Ca, 3n)284Fl, 239Pu(48Ca, 4n)283Fl, 240Pu(48Ca, 3n)285Fl, 240Pu(48Ca, 4n)284Fl, 242Pu(48Ca, 2n)288Fl, 242Pu(48Ca, 3n)287Fl, 242Pu(48Ca, 4n)286Fl, 242Pu(48Ca, 5n)285Fl, 244Pu(48Ca, 3n)289Fl, 244Pu(48Ca, 4n)288Fl, 244Pu(48Ca, 5n)287Fl, 244Pu(42Ca, 3n)283Fl, 244Pu(42Ca, 4n)282Fl, 244Pu(42Ca, 5n)281Fl, 244Pu(43Ca, 3n)284Fl, 244Pu(43Ca, 4n)283Fl, 244Pu(43Ca, 5n)282Fl, 244Pu(44Ca, 3n)285Fl, 244Pu(44Ca, 4n)284Fl, 244Pu(44Ca, 5n)283Fl, 244Pu(46Ca, 3n)287Fl, 244Pu(46Ca, 4n)286Fl, 244Pu(46Ca, 5n)285Fl, 238U(44Ca, 3n)279Cn, 238U(44Ca, 4n)278Cn, 238U(44Ca, 5n)277Cn, 242Pu(44Ca, 3n)283Fl, 242Pu(44Ca, 4n)282Fl, 242Pu(44Ca, 5n)281Fl, 248Cm(44Ca, 3n)289Lv, 248Cm(44Ca, 4n)288Lv, 248Cm(44Ca, 5n)287Lv, 238U(46Ca, 3n)281Cn, 238U(46Ca, 4n)280Cn, 238U(46Ca, 5n)279Cn, 237Np(46Ca, 3n)280Nh, 237Np(46Ca, 4n)279Nh, 237Np(46Ca, 5n)278Nh, 239Pu(46Ca, 3n)282Fl, 239Pu(46Ca, 4n)281Fl, 239Pu(46Ca, 5n)280Fl, 240Pu(46Ca, 3n)283Fl, 240Pu(46Ca, 4n)282Fl, 240Pu(46Ca, 5n)281Fl, 241Am(46Ca, 3n)284Mc, 241Am(46Ca, 4n)283Mc, 241Am(46Ca, 5n)282Mc, 243Am(46Ca, 3n)286Mc, 243Am(46Ca, 4n)285Mc, 243Am(46Ca, 5n)284Mc, 243Cm(46Ca, 3n)286Lv, 243Cm(46Ca, 4n)285Lv, 243Cm(46Ca, 5n)284Lv, 245Cm(46Ca, 3n)288Lv, 245Cm(46Ca, 4n)287Lv, 245Cm(46Ca, 5n)286Lv, 235U(48Ca, 3n)280Cn, 235U(48Ca, 4n)279Cn, 235U(48Ca, 5n)278Cn, 241Am(48Ca, 3n)286Mc, 241Am(48Ca, 4n)285Mc, 241Am(48Ca, 5n)284Mc, 243Cm(48Ca, 3n)289Lv, 243Cm(48Ca, 4n)288Lv, 243Cm(48Ca, 5n)287Lv; Calculated evaporation residues (ER) cross sections for superheavy elements, and compared with available experimental data. Maximum cross sections deduced for 243Cm(46Ca, 3n)288Lv, E(cm)=200.7 MeV, 241Am(48Ca, 4n)285Mc, E(cm)=210.5 MeV, 248Cm(44Ca, 4n)288Lv, E(cm)=201.7 MeV, and 238Pu(48Ca, 4n)282Fl, E(cm)=208.7 MeV. Dinuclear system model.

doi: 10.1103/PhysRevC.93.064610
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2016ZH40      Eur.Phys.J. A 52, 281 (2016)

F.Zhang, C.Li, P.-W.Wen, H.Liu, F.-S.Zhang

Shear-viscosity-to-entropy-density ratio and phase transition in multifragmentation of quasiprojectile

NUCLEAR REACTIONS 197Au(197Au, x), E=400 MeV/nucleon; calculated multiplicity, yield charge distribution, temperature vs time and vs E*/A. Compared with available data.

doi: 10.1140/epja/i2016-16281-0
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2016ZH48      Phys.Rev. C 94, 054606 (2016)

L.Zhu, J.Su, W.-J.Xie, F.-S.Zhang

Production of neutron-rich transcalifornium nuclei in 238U-induced transfer reactions

NUCLEAR REACTIONS 248Cm(238U, X), E(cm)=800 MeV; calculated production σ for A=248-254 Es, Fm and Md isotopes, and compared with experimental data. 248,250Cm, 249Cf, (238U, X), E(cm)=1.1(VCN=interaction potential at the touching point); calculated production σ for A=245-270 Es, Fm, Md, No, Lr and Rf isotopes. Dinuclear system (DNS) model.

doi: 10.1103/PhysRevC.94.054606
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2016ZH50      Chin.Phys.C 40, 124105 (2016)

L.Zhu, J.Su, C.-Y.Huang, F.-S.Zhang

Effects of entrance channel on fusion probability in hot fusion reactions

NUCLEAR REACTIONS 248Cm(26Mg, X)274Hs, 238U(36S, X)274Hs, 226Ra(48Ca, X)274Hs, E<60 MeV/nucleon; 238U(48Ca, X)286Cn, 234U(52Ca, X)286Cn, 231Pa(55Sc, X)286Cn, E<60 MeV/nucleon; analyzed available data; calculated fusion probability as a function of dinuclear system excitation energy. Comparison with available data.

doi: 10.1088/1674-1137/40/12/124105
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2015CH40      Phys.Rev. C 92, 014308 (2015)

K.V.Cherevko, L.A.Bulavin, L.L.Jenkovszky, V.M.Sysoev, F.-S.Zhang

Curvature correction term as a constraint for the Skyrme interaction

doi: 10.1103/PhysRevC.92.014308
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2015GU07      Phys.Rev. C 91, 054615 (2015)

C.Guo, Y.Wang, Q.Li, Pe.Wen, F.-S.Zhang

Mass-splitting effect on flows in heavy-ion collisions in the Fermi-energy domain

NUCLEAR REACTIONS 197Au(197Au, X), E=100 MeV/nucleon; calculated time evolution of neutron and proton densities, rapidity distributions and transverse momentum of neutrons and protons, and effect of neutron-proton effective mass splitting (NPEMS) on flows in heavy-ion collisions at the Fermi-energy domain for directed and elliptic flows. Ultrarelativistic quantum molecular dynamics (UrQMD) model.

doi: 10.1103/PhysRevC.91.054615
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2015XI01      Phys.Rev. C 91, 054609 (2015)

W.-J.Xie, Z.-Q.Feng, J.Su, F.-S.Zhang

Probing the momentum-dependent symmetry potential via nuclear collective flows

NUCLEAR REACTIONS 197Au(197Au, X), E=250-800 MeV/nucleon; calculated directed and elliptic flow of protons, rapidity and transverse momentum dependence of the neutron-proton differential directed flow. Isospin-dependent quantum molecular dynamics (IQMD) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.054609
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2015ZH06      Phys.Rev. C 91, 034617 (2015)

F.Zhang, C.Li, L.Zhu, H.Liu, F.-S.Zhang

Effect of fragment emission time on the temperature of momentum quadrupole fluctuations

doi: 10.1103/PhysRevC.91.034617
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2015ZH11      Chin.Phys.C 39, 044103 (2015)

D.-H.Zhang, W.-J.Xie, J.Su, F.-S.Zhang

Production cross section of neutron-rich calcium isotopes in heavy ion collisions

NUCLEAR REACTIONS 112Sn(112Sn, X), 124Sn(124Sn, X)48Ca/54Ca, E<160 MeV; calculated production σ. IQMD+GEMINI model.

doi: 10.1088/1674-1137/39/4/044103
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2015ZH17      J.Phys.(London) G42, 085102 (2015)

L.Zhu, Z.Q.Feng, F.-S.Zhang

Production of heavy neutron-rich nuclei in transfer reactions within the dinuclear system model

NUCLEAR REACTIONS 208Pb(136Xe, X)210Po/222Rn/224Ra, E(cm)=514 MeV; 208Pb(58Ni, X), E(cm)=256.8 MeV; 248Cm(238U, X)Es/Fm/Md, E(cm)=800 MeV; 238U(176Yb, X)Eu/Yb/Ho, E(cm)=600 MeV; calculated σ. Comparison with experimental data.

doi: 10.1088/0954-3899/42/8/085102
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2014CH05      Phys.Rev. C 89, 014618 (2014)

K.Cherevko, L.Bulavin, J.Su, V.Sysoev, F.-S.Zhang

"Doughnut" nuclear shapes in head-on heavy ion collisions

doi: 10.1103/PhysRevC.89.014618
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2014CH32      Phys.Rev. C 90, 017303 (2014)

K.V.Cherevko, L.A.Bulavin, L.L.Jenkovszky, V.M.Sysoev, F.-S.Zhang

Evaluation of the curvature-correction term from the equation of state of nuclear matter

doi: 10.1103/PhysRevC.90.017303
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2014GU18      Phys.Rev. C 90, 034606 (2014)

C.Guo, Y.Wang, Q.Li, F.-S.Zhang

Effect of the spin-orbit interaction on flows in heavy-ion collisions at intermediate energies

doi: 10.1103/PhysRevC.90.034606
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2014SU03      Phys.Rev. C 89, 014619 (2014)

J.Su, K.Cherevko, W.-J.Xie, F.-S.Zhang

Nonisotropic and nonsingle explosion in central 129Xe + 120Sn collisions at 50-125 MeV/nucleon

NUCLEAR REACTIONS 129Xe(120Sn, X), E=50-125 MeV/nucleon; calculated average kinetic energy, average multiplicity of fragments as a function of charge for forward and sideward angles, collective and Coulomb expansion energy per nucleon as a function of polar angle, radial flow energies of H, He, Li, and Be fragments, contours of time evolutions of the density and the collective velocity, longitudinal and transverse collective velocity as a function of radius. Isospin-dependent quantum molecular dynamics model, and statistical decay code GEMINI. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.014619
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2014ZH08      Phys.Rev. C 89, 024615 (2014)

L.Zhu, W.-J.Xie, F.-S.Zhang

Production cross sections of superheavy elements Z=119 and 120 in hot fusion reactions

NUCLEAR REACTIONS 208Pb(48Ca, n), (48Ca, 2n), (48Ca, 3n), E(cm)=160-200 MeV; 208Pb, 209Bi(70Zn, n), E(cm)=250-270 MeV; 237Np, 242Pu, 243Am, 245Cm(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E(cm)=185-225 MeV; 244Pu, 249Bk(48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E(cm)=185-225 MeV; 248Cm, 249Cf(48Ca, 3n), (48Ca, 4n), E(cm)=185-225 MeV; 238U(48Ca, 3n), (48Ca, 4n), E(cm)=180-205 MeV; 252Es(48Ca, 3n), (48Ca, 4n), 249Bk(50Ti, 3n), (50Ti, 4n), 248Cm(51V, 3n), (48Ca, 4n), E(cm)=200-250 MeV; 249Cf(50Ti, 3n), (50Ti, 4n), 249Bk(51V, 3n), (51V, 4n), 248Cm(54Cr, 3n), (54Cr, 4n), E(cm)=220-260 MeV; calculated σ(E) for evaporation residues (ER) in hot fusion reactions for different orientations of deformed colliding nuclei, fusion probability; predicted evaporation residue cross sections for synthesizing Z=119 and 120 superheavy elements. Dinuclear system (DNS) concept. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.024615
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2014ZH25      Phys.Rev. C 90, 014612 (2014)

L.Zhu, Z.Q.Feng, C.Li, F.-S.Zhang

Orientation effects on evaporation residue cross sections in 48Ca- induced hot fusion reactions

NUCLEAR REACTIONS 238U, 237Np, 244Pu, 243Am, 248Cm, 249Bk, 249Cf, 252Es, 257Fm(48Ca, 3n), (48Ca, 4n), 243Am(48Ca, 2n), 244Pu, 249Bk(48Ca, 5n), E*=20-60 MeV; calculated σ(E, θ) for evaporation residue (ER) of superheavy (Z=113-120) nuclei, capture cross sections, dependence of fusion probability on excitation energies. Dinuclear system (DNS) model. Comparison with experimental results.

doi: 10.1103/PhysRevC.90.014612
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2013SU03      Phys.Rev. C 87, 017602 (2013)

J.Su, F.-S.Zhang

Non-equilibrium and residual memory in momentum space of fragmenting sources in central heavy-ion collisions

doi: 10.1103/PhysRevC.87.017602
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2013XI13      Phys.Rev. C 88, 061601 (2013)

W.-J.Xie, J.Su, L.Zhu, F.-S.Zhang

Neutron-proton effective mass splitting in a Boltzmann-Langevin approach

doi: 10.1103/PhysRevC.88.061601
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2013ZH36      Nucl.Phys. A915, 90 (2013)

L.Zhu, J.Su, W.-J.Xie, F.-S.Zhang

Study of the dynamical potential barriers in heavy ion collisions

NUCLEAR REACTIONS 58Ni(58Ni, X), E(cm)=94-110 MeV;64Ni(64Ni, X), E(cm)=90-109 MeV;154Sm(16O, X), E(cm)=52-90 MeV;208Pb(16O, X), E(cm)=72-280 MeV; calculated fusion σ using isospin-dependent QMD with shell corrections; deduced relative orientation of nuclei, nucleus-nucleus potentials. Compared to data.

doi: 10.1016/j.nuclphysa.2013.07.003
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2012SU03      Phys.Rev. C 85, 017604 (2012)

J.Su, L.Zhu, W.-J.Xie, F.-S.Zhang

Nuclear temperatures from kinetic characteristics

NUCLEAR REACTIONS Sn, 120Sn(129Xe, X), E=30-80 MeV/nucleon; 197Au(197Au, X), E=30-150 MeV/nucleon; calculated multiplicities as function of fragment charge (Z<60), kinetic energy spectra, temperatures. IQMD model accompanied by the GEMINI model.

doi: 10.1103/PhysRevC.85.017604
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2011LI33      Chin.Phys.C 35, 629 (2011)

M.Liu, Z.-X.Li, N.Wang, F.-S.Zhang

Exploring nuclear symmetry energy with isospin dependence in neutron skin thickness of nuclei

doi: 10.1088/1674-1137/35/7/006
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2011SU20      Phys.Rev. C 84, 037601 (2011)

J.Su, F.-S.Zhang

Isotopic dependence of nuclear temperatures

NUCLEAR REACTIONS 120Sn(107Sn, X), (124Sn, X), (124La, X), E=600 MeV/nucleon; 40Ca(36Ca, X), (44Ca, X), (52Ca, X), (78Zr, X), (94Zr, X), (110Zr, X), (176Pb, X), (192Pb, X), (208Pb, X), (224Pb, X), analyzed charge distributions, Z(bound) distributions, mean multiplicity of intermediate-mass fragments, THeLi as a function of Zbound/Zp; deduced isotope temperatures from double ratios of helium and lithium isotopic yields. Isospin-dependent quantum molecular dynamics with GEMINI model.

doi: 10.1103/PhysRevC.84.037601
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2011ZH22      Nucl.Instrum.Methods Phys.Res. A648, 192 (2011)

H.-Y.Zhou, F.-G.Deng, W.Cheng, F.-S.Zhang, Q.Zhao, J.Su, L.M.Dong, Q.Zhu, G.-Y.Fan

Associated gamma radiation in interaction of 14.9 MeV neutrons with natural silicon

NUCLEAR REACTIONS 28,29,30Si(n, xγ), (n, n'γ), (n, 2nγ), (n, npγ), (n, dγ), (n, pγ), (n, αγ), (n, nαγ), E=14.9 MeV; measured reaction products, Eγ, Iγ; deduced energies, M1 and E2 transition types. Comparison with GNASH nuclear reaction code calculations.

RADIOACTIVITY 28Al(β-) [from 28Si(n, p), E=14.9 MeV]; measured decay products, Eβ, Iβ; deduced energies, M1 and E2 transition types. Comparison with GNASH nuclear reaction code calculations.

doi: 10.1016/j.nima.2011.04.014
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32688.

2010BI05      Eur.Phys.J. A 43, 67 (2010)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Effect of shell structure in the fusion reactions

NUCLEAR REACTIONS 134,138Ba(82Se, X), 176,180Hf(40Ar, X), 92,96Zr(124Sn, X), E(cm)≈125-270 MeV; calculated fusion probabilities, barrier height, related features using the improved isospin dependent quantum molecular dynamics and Bass models. Comparison with data.

doi: 10.1140/epja/i2009-10889-y
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2010LI45      Phys.Rev. C 82, 064306 (2010)

M.Liu, N.Wang, Z.-X.Li, F.-S.Zhang

Nuclear symmetry energy at subnormal densities from measured nuclear masses

NUCLEAR STRUCTURE A=20-250; analyzed nuclear symmetry energy coefficients for more that 2000 previously measured masses using liquid drop formula with the contribution of the Wigner term. Comparison with other methods.

doi: 10.1103/PhysRevC.82.064306
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2010ZH44      Phys.Rev. C 82, 047602 (2010)

H.-Y.Zhou, F.-G.Deng, Q.Zhao, J.Su, B.-K.Zhao, L.-M.Dong, G.-Y.Fan, F.-S.Zhang

Investigation of discrete γ radiation in interactions of 14.9-MeV neutrons with natural silicon by a total γ-radiation measurement technique

NUCLEAR REACTIONS Si(n, γ)25Mg/26Mg/27Al/28Al/28Si/29Si/30Si, E=14.9 MeV; measured Eγ, Iγ, γ(θ); deduced σ, σ(θ), total γ radiation yield. Prompt and delayed γ. 28Si(n, p), (n, n'), (n, α), (n, np), (n, d), 29Si(n, n'), (n, α), 30Si(n, n'), E=14.9 MeV; deduced differential and integral isotopic cross sections. Comparisons with other experimental data and with evaluated results.

doi: 10.1103/PhysRevC.82.047602
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset32688.

2009BI10      Nucl.Phys. A829, 1 (2009)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fusion enhancement in the reactions of neutron-rich nuclei

NUCLEAR REACTIONS 197Au(27Al, X), (31Al, X), 181Ta, 208Pb(32S, X), (38S, X), 64Ni(124Sn, X), (132Sn, X), E(cm)≈100-270 MeV; calculated fusion barrier height, σ, related features using the improved isospin dependent quantum molecular dynamics and Bass models. Comparison with data.

doi: 10.1016/j.nuclphysa.2009.08.003
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2009CH45      Chin.Phys.Lett. 26, 112502 (2009)

Y.Chen, F.-S.Zhang, J.Su

A Discussion on Whether 15-20C Are All Skin Nuclei via Isospin-dependent Boltzmann-Langevin Equation

NUCLEAR STRUCTURE 15,16,17,18,19,20C; calculated radial density distribution, thickness of neutron skin.

NUCLEAR REACTIONS 12C(15C, X), (16C, X), (17C, X), (18C, X), (19C, X), (20C, X), E=30 MeV/nucleon; calculated total reaction σ using isospin-dependent Boltzmann-Langevin equation.

doi: 10.1088/0256-307X/26/11/112502
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2009ZH21      Chin.Phys.Lett. 26, 092501 (2009)

Q.Zhao, F.-S.Zhang, Z.-P.Wang, H.-Y.Zhou

Secondary Beam Fragments Produced by 200 and 400 MeV/u 12C6+ Ions in Water

doi: 10.1088/0256-307X/26/9/092501
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2008BI02      Chin.Phys.Lett. 25, 451 (2008)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fragmentation Cross Sections of 12C on Different Targets at Beam Energies from 50 to 100MeV/Nucleon

NUCLEAR REACTIONS 2H, 12C, 14N, 16O(12C, X), E=50-100 MeV/nucleon; calculated fragmentation cross sections using the isospin-dependent Boltzman-Langevin equation model.

doi: 10.1088/0256-307X/25/2/027
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2008BI11      Nucl.Phys. A807, 71 (2008)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fragmentation cross sections of 20Ne collisions with different targets at 600 MeV/nucleon

NUCLEAR REACTIONS 12C, 27Al, 63Cu, 120Sn, 181Ta, 208Pb(20Ne, X), E=600 MeV/nucleon; calculated Z=2-9 fragment production σ using an isospin-dependent Boltzmann?Langevin model. Comparison with data and other models.

doi: 10.1016/j.nuclphysa.2008.03.014
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2008BI18      Int.J.Mod.Phys. E17, 1927 (2008)

B.-A.Bian, F.-S.Zhang, H.-Y.Zhou

Fragmentation cross sections in heavy ion collisions

NUCLEAR REACTIONS C, Al, Cu, Sn, Ta, Pb(Ne, X), E=600 MeV/nucleon; 2H, 12C, 14N, 16O(12C, X), E=50-150 MeV/nucleon; calculated fragmentation cross sections.

doi: 10.1142/S0218301308010908
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2008BI20      Int.J.Mod.Phys. E17, Supplement 1, 80 (2008)

B.-A.Bian, F.-S.Zhang, S.-S.Du

Shell correction energy and the entrance channel effect on the formation of superheavy nuclei

NUCLEAR STRUCTURE 62Zn, 76Kr, 202Pb; calculated reaction systems forming compound nuclei, fusion σ.

doi: 10.1142/S021830130801177X
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2008DU20      Int.J.Mod.Phys. E17, 1979 (2008)

S.-S.Du, B.-A.Bian, F.-S.Zhang

Shell effect in synthesis of superheavy nuclei

NUCLEAR REACTIONS 154Sm(48Ca, X), E(cm) < 160 MeV; 208Pb(32S, X), E(cm) < 260 MeV; calculated fusion cross sections.

doi: 10.1142/S0218301308010957
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2008FE03      Nucl.Phys. A802, 91 (2008)

Z.-Q.Feng, G.-M.Jin, F.-S.Zhang

Dynamical analysis on heavy-ion fusion reactions near Coulomb barrier

NUCLEAR REACTIONS 90,96Zr(48Ca, X), E(cm)=90-115 MeV; 46Ti(46Ti, X), E(cm)=58-72 MeV; 112Sn(40Ca, X), E(cm)=107-135 MeV; 58Ni(18O, X), 60Ni(16O, X), E(cm)=28-48 MeV; 90,96Zr(36S, X), E(cm)=70-88 MeV; 144,154Sm(16O, X), E(cm)=54-72 MeV; calculated fusion σ. 208Pb, 238U(16O, X), E(cm)=70-110 MeV; 208Pb, 238U(48Ca, X), E(cm)=170-240 MeV; 244Pu, 248Cm(48Ca, X), E(cm)=185-230 MeV; calculated capture σ. Improved isospin dependent quantum molecular dynamics model with shell correction. Comparison with data.

doi: 10.1016/j.nuclphysa.2008.01.022
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2006ZH39      Int.J.Mod.Phys. E15, 1601 (2006)

F.S.Zhang, Z.Q.Feng, G.M.Jin

Importance of shell correction energy on synthesis of superheavy nuclei

NUCLEAR REACTIONS 208Pb, 238U(16O, X), E(cm) ≈ 70-110 MeV; calculated fusion σ, shell correction energy. Microscopic transport model.

doi: 10.1142/S0218301306005174
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