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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, T_1/2 using DSSD detectors; deduced reduced α-decay width, and analyzed using N_pN_n scheme. ²¹⁸Ac, ²¹⁹Th, ²²⁰Pa(α); measured Eα, and T_1/2. 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 N_pN_n. 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, 69}V, 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 ^{72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102}Kr, ^{74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104}Sr, ^{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}Te, ^{110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156}Xe, ^{116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162}Ba, ^{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}Ce, ^{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}Nd, ^{130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165}Sm; 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 ^{37,38,39,40,41,42,43,44,45,46,47,48,49,50,51}K; 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 ^{57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81}Cu, ^{99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139}In; 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, ^{221,222,223,224}Ra, ²²⁶Ra, ²²⁵Ac, ²²⁴Th(¹⁴C), ²²⁸Th(²⁰O), ²³¹Pa(²³F), ²³⁰Th, ²³¹Pa, ^{232,233,234,235}U(²⁴Ne), ^233,235U(²⁵Ne), ²³⁴U, ²³⁶U, ^236,238Pu(²⁸Mg), ²³⁶U, ²³⁸Pu(³⁰Mg), ²³⁸Pu(³²Si), ²⁴²Cm(³⁴Si); calculated T_1/2; 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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 - ^{243,244,245,246,247,248}No.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, 267-269}Lr 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 ^{172,174,176,178}Hg, ^{178,180,182,184}Pb, ^{186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{194,196,198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra, ^{208,210,212,214,216,218,220,222,224,226,228,230}Th, ^{216,218,220,222,224,226,228,230,232,234,236}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{240,242,244,246,248}Cm, ^{238,240,242,244,246,248,250,252,254,256}Cf, ^{242,244,246,248,250,252,254,256,258}Fm, ^{252,254,256,258,260}No, ^{254,256,258,260,262}Rf, ^{258,260,262,264,266}Sg, ^{264,266,268,270}Hs, ²⁷⁰Ds, ²⁸⁰Ds, ^282,284Cn, ^284,286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated T_1/2. 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 T_1/2 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 ^{285,286,287,288,289}Fl, ^{287,288,289,290}Mc, ^{290,291,292,293}Lv, ^293,294Ts, ²⁹⁴Og, ^{287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}120, ^{294,295,296,297,298,299,300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}122, ^{300,301,302,303,304,305,306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}124, ^{306,307,308,309,310,311,312,313,314,315,316,317,318,319,320,321,322,323,324,325,326,327,328,329,330,331,332,333,334,335,336,337,338,339}126(α); calculated Q-values, T_1/2 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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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 Q_α, T_1/2 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: ^{198,200,202,204,206}Pt, ^{196,198,200,202,204}Os, ^{190,192,194,196,198}W, ^{186,188,190,192,194}Hf. 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, 269}Rf 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 ^{264,266,268,269}Rf 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 ^{280,281,282,283,284,285,286,287,288,289,290,291,292,293,294,295,296,297,298,299,300,301,302,303,304,305}Fl(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. ^{285,286,287,288,289}Fl, ^281,283,285Cn, ^277,279,281Ds, ^273,275Hs, ^269,271Sg(α); calculated T_1/2 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 ^{239,240,242,244}Pu(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. ^{280,281,282,283,291,292,293}Fl; 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, 67}₂₅Mn: 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, 86}Kr + 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)=1.10V_c; 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)=1.10V_c; calculated production σ for Pt isotopes. ^{209,210,211,212}Pt; 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 T_1/2 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 T_1/2, 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(V_CN=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, T_HeLi as a function of Z_bound/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 ^{15,16,17,18,19,20}C; 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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