NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = F.Niu Found 11 matches. 2022CH20 Phys.Rev. C 105, 034610 (2022) P.g-H.Chen, F.Niu, X.-X.Xu, Z.-X.Yang, X.-H.Zeng, Z.-Q.Feng Rare isotope formation in complete fusion and multinucleon transfer reactions in collisions of 48Ca+248Cm near Coulomb barrier energies NUCLEAR REACTIONS 248Cm(48Ca, F), E=5.5 MeV/nucleon; calculated interaction potential of the tip-tip and side-side collisions, reaction time, TKE-mass distribution, production σ of primary fragments. 248Cm(48Ca, F)242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/251Bk/252Bk/253Bk/254Bk/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/253Cf/254Cf/255Cf/256Cf/257Cf/258Cf/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/255Es/256Es/257Es/258Es/259Es/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm/258Fm/259Fm/260Fm/261Fm/252Md/253Md/254Md/255Md/256Md/257Md/258Md/259Md/260Md/261Md/262Md/263Md/254No/255No/256No/257No/258No/259No/260No/261No/262No/263No/264No/265No/266No/259Lr/260Lr/261Lr/262Lr/263Lr/264Lr/265Lr/266Lr/267Lr/261Rf/262Rf/263Rf/264Rf/265Rf/266Rf/267Rf/268Rf/269Rf, 248Cm(40Ca, F)237Bk/238Bk/239Bk/240Bk/241Bk/242Bk/243Bk/244Bk/245Bk/246Bk/247Bk/248Bk/249Bk/250Bk/238Cf/239Cf/240Cf/241Cf/242Cf/243Cf/244Cf/245Cf/246Cf/247Cf/248Cf/249Cf/250Cf/251Cf/252Cf/241Es/242Es/243Es/244Es/245Es/246Es/247Es/248Es/249Es/250Es/251Es/252Es/253Es/254Es/242Fm/243Fm/244Fm/245Fm/246Fm/247Fm/248Fm/249Fm/250Fm/251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/245Md/246Md/247Md/248Md/249Md/250Md/251Md/252Md/253Md/254Md/255Md/256Md/248No/249No/251No/252No/253No/254No/255No/251Lr/252Lr/253Lr/261R calculated σ. Dinuclear system model. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.034610
2020CH07 Phys.Rev. C 101, 024610 (2020) P.-H.Chen, F.Niu, W.Zuo, Z.-Q.Feng Approaching the neutron-rich heavy and superheavy nuclei by multinucleon transfer reactions with radioactive isotopes NUCLEAR REACTIONS 238U(124Sn, X), E=6.0 MeV/nucleon; calculated mass distribution of total kinetic energy of the primary binary fragments, potential energy surface in (N, Z) plane. 238U, 248Cm(238U, X), E=7.0 MeV/nucleon; calculated production cross sections of transcurium isotopes (Z=97-101, A=240-260), and compared with experimental data from GSI. 238U(124Sn, X), E=5.6, 6.0, 6.5 MeV/nucleon; calculated differential σ(θ) of Sn-like and U-like products. 238U, 248Cm(124Sn, X), (132Sn, X), E=6 MeV/nucleon; calculated production cross sections as functions of neutron and proton numbers of primary fragments and secondary fragments, production cross sections of Z=88-91, A=210-250, Z=93-96, A=226-260, Z=101-104, A=250-270, N=82, Z=74-90, N=126, Z=74-90, N=160-164, Z=87-98, N=150-154, Z=87-98, and Z=60-104, A=162-269 and above. Dinuclear system (DNS) model for production of neutron-rich isotopes via the multi-nucleon transfer (MNT) reactions.
doi: 10.1103/PhysRevC.101.024610
2020CH23 Phys.Rev. C 102, 014621 (2020) Production mechanism of proton-rich actinide isotopes in fusion reactions and via multinucleon transfer processes NUCLEAR REACTIONS 196Hg(36Ar, X), E(cm)=165 MeV; 238U(105Sn, X), E(cm)=437 MeV; 238U(110Sn, X), (115Sn, X), (120Sn, X), (125Sn, X), (130Sn, X), (58Cu, X), (69As, X), (90Nb, X), (91Tc, X), (94Rh, X), (118Xe, X), E=6 MeV/nucleon; calculated interaction potential, potential energy surfaces, total kinetic energy and mass distribution of primary fragments, and multi-nucleon transfer reaction σ(E) using dinuclear system (DNS) model. 203Tl, 204Pb, 209Bi(24Mg, X), E*=20-70 MeV; 197Au, 196Hg, 203Tl, 204Pb, 209Bi(28Si, X), E*=20-70 MeV; 191Ir, 190Pt, 197Au, 196Hg, 203Tl, 204Pb, 209Bi(32S, X), E*=20-70 MeV; 185Re, 184Os, 191Ir, 190Pt, 197Au, 196Hg, 203Tl, 204Pb, 209Bi(36Ar, X), E*=20-80 MeV; 181Ta, 180W, 185Re, 184Os, 191Ir, 190Pt, 197Au, 196Hg, 203Tl, 204Pb(40Ca, X), E*=20-80 MeV; calculated fusion evaporation reaction σ(E). Z=93, A=214-228; Z=94, A=215-231; Z=95, A=219-231; Z=96, A=220-235; Z=97, A=225-236; Z=98, A=227-236; Z=99, A=232-240; Z=100, A=232-243; calculated production σ for neutron-deficient actinides by the DNS model.
doi: 10.1103/PhysRevC.102.014621
2018GU19 Chin.Phys.C 42, 124106 (2018) Y.-F.Guo, P.-H.Chen, F.Niu, Z.-Q.Feng Isospin effect in peripheral heavy-ion collisions at Fermi energies NUCLEAR REACTIONS 208Pb(48Ca, X), (78Kr, X), (136Xe, X), 136Xe(136Xe, X), 124Sn(86Kr, X), (124Sn, X), E=15, 20, 30 MeV/nucleon; analyzed available data using the statistical code GEMINI; deduced isospin migration from the high-isospin density to the low-density matter occurrence in the neutron-rich nuclear reactions.
doi: 10.1088/1674-1137/42/12/124106
2018NI02 Chin.Phys.C 42, 034102 (2018) Pairing-energy coefficients of neutron-rich fragments in spallation reactions NUCLEAR REACTIONS 208Pb, 238U, 136Xe, 56Fe(p, X), E<1 GeV/nucleon; analyzed available data; deduced the ratio of pairing-energy coefficient to temperature of neutron-rich fragments.
doi: 10.1088/1674-1137/42/3/034102
2018NI05 Phys.Rev. C 97, 034609 (2018) F.Niu, P.-H.Chen, Y.-F.Guo, C.-W.Ma, Z.-Q.Feng Effect of isospin diffusion on the production of neutron-rich nuclei in multinucleon transfer reactions NUCLEAR REACTIONS 208Pb(58Ni, X), E=256 MeV; 208Pb(64Ni, X), E=268 MeV; 198Pt(78Kr, X), E=307 MeV; 198Pt(86Kr, X), E=302 MeV; 198Pt(91Kr, X), E=294 MeV; calculated potential energy surface for 58Ni+208Pb reaction as functions of the protons and neutrons of the projectile-like and target-like fragments, yields for projectile-like Z=22-27, N=24-42 and for target-like fragments Z=79-81, 83-85, N=104-130 fragments, charge and mass distributions of fragments in multinucleon transfers (MNT) in 58Ni+208Pb and 64Ni+208Pb reactions, yields of Z=71-78, N=90-130 fragments and N=126 isotonic distributions in 78,86,91Kr+198Pt reactions. Dinuclear system model for production cross sections of neutron-rich isotopes. Comparison with available experimental data.
doi: 10.1103/PhysRevC.97.034609
2017CH24 Eur.Phys.J. A 53, 95 (2017) P.-H.Chen, Z.-Q.Feng, F.Niu, Y.-F.Guo, H.-F.Zhang, J.-Q.Li, G.-M.Jin Production of proton-rich nuclei around Z = 84-90 in fusion-evaporation reactions NUCLEAR REACTIONS 165Ho, 169Tm, 170,171,172,173,174Yb, 175,176Lu, 175,176,177,178,179,180Hf, 181Ta(28Si, x), (32S, x), (40Ar, x), E*=30-100 MeV; calculated proton-rich nuclei around Z=84-90 production σ using dinuclear system model. Compared with available data.
doi: 10.1140/epja/i2017-12281-x
2017CH27 Eur.Phys.J. A 53, 128 (2017) J.Chen, Z.-Q.Feng, P.-H.Chen, F.Niu, Y.-F.Guo, J.-S.Wang In-medium and isospin effects on eta production in heavy-ion collisions near threshold energies
doi: 10.1140/epja/i2017-12325-3
2017GU33 Chin.Phys.C 41, 104104 (2017) Y.-F.Guo, P.-H.Chen, F.Niu, H.-F.Zhang, G.-M.Jin, Z.-Q.Feng Isospin splitting of nucleon effective mass and symmetry energy in isotopic nuclear reactions NUCLEAR REACTIONS 112Sn(112Sn, X), E=50 MeV/nucleon;124Sn(124Sn, X), E=120 MeV/nucleon; analyzed available data; deduced constraining the isospin splitting of nucleon effective mass and the symmetry energy at subsaturation densities.
doi: 10.1088/1674-1137/41/10/104104
2017NI17 Phys.Rev. C 96, 064622 (2017) F.Niu, P.-H.Chen, Y.-F.Guo, C.-W.Ma, Z.-Q.Feng Multinucleon transfer dynamics in heavy-ion collisions near Coulomb-barrier energies NUCLEAR REACTIONS 124Sn(48Ca, X), (40Ca, X), E(cm)/VC=1.12; 232Th(40Ca, X), (40Ar, X), (58Ni, X), E(cm)/VC=1; 248Cm(40Ca, X), (40Ar, X), (58Ni, X), E(cm)/VC=1, 1.02, 1.11; calculated σ for projectile-like (PLF) and target-like fragment (TLF) production. 248Cm(58Ni, X), E(cm)/VC=0.90, 1.01, 1.20; calculated σ for target-like fragment (TLF) production. Multistep model based on dinuclear system (DNS) concept for multinucleon transfer reactions near the Coulomb barrier energies.
doi: 10.1103/PhysRevC.96.064622
2016MA51 Phys.Rev. C 94, 024615 (2016) C.-W.Ma, F.Niu, C.-Y.Qiao, Y.-F.Niu, T.-Z.Yan Pairing energy of fragments produced in intermediate-energy heavy-ion collisions NUCLEAR REACTIONS 9Be, 181Ta(40Ca, X), (48Ca, X), (58Ni, X), (64Ni, X), E=140 MeV/nucleon; analyzed experimental data for isobaric yield ratios to obtain ratio of the pairing-energy coefficient for fragments to the temperature. AMD+GEMINI models in the framework of modified Fisher model (MFM).
doi: 10.1103/PhysRevC.94.024615
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