NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = G.M.Jin Found 85 matches. 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
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
2015FE08 Phys.Rev. C 92, 044604 (2015) Z.-Q.Feng, W.-J.Xie, P.-H.Chen, J.Chen, G.-M.Jin In-medium and isospin effects on particle production near threshold energies in heavy-ion collisions
doi: 10.1103/PhysRevC.92.044604
2014FE10 Phys.Rev. C 90, 064604 (2014) Nuclear in-medium effects of strange particles in proton-nucleus collisions
doi: 10.1103/PhysRevC.90.064604
2014WA23 Phys.Rev. C 89, 064613 (2014) R.S.Wang, Y.Zhang, Z.G.Xiao, J.L.Tian, Y.X.Zhang, Q.H.Wu, L.M.Duan, G.M.Jin, R.J.Hu, S.F.Wang, Z.Y.Li, H.W.Wang, Z.Zhang, H.Yi, H.J.Li, W.J.Cheng, Y.Huang, L.M.Lu Time-dependent isospin composition of particles emitted in fission events following 40Ar + 197Au at 35 MeV/u NUCLEAR REACTIONS 197Au(40Ar, F), E=35 MeV/nucleon; measured particle spectra, (fission fragment)(light charged particles)-coin, mass asymmetry, double differential cross sections for proton, deuteron and triton at HRIFL-Lanzhou. Folding-angle method for reconstruction of fission events. Dependence of N/Z on the parameterization of the symmetry energy. Comparison with improved quantum molecular dynamics (ImQMD) transport-model calculations.
doi: 10.1103/PhysRevC.89.064613
2010FE03 Nucl.Phys. A836, 82 (2010) Influence of entrance channels on the formation of superheavy nuclei in massive fusion reactions NUCLEAR REACTIONS 136Xe(136Xe, xn), 208Pb(64Fe, xn), 238U(34S, xn), (48Ca, xn), 244Pu(40Ar, xn), 250Cm(36S, xn), 252Cf(30Si, xn), (48Ca, xn), E not given; calculated evaporation residue σ versus excitation energy for Z=108, 112 SHE formation and systematics using a di-nuclear system model. Comparison with some data.
doi: 10.1016/j.nuclphysa.2010.01.244
2010FE06 Nucl.Phys. A834, 384c (2010) Z.-Q.Feng, G.-M.Jin, J.-Q.Li, W.Scheid Production mechanism of superheavy nuclei in massive fusion reactions NUCLEAR REACTIONS 208Pb, 209Bi(48Ca, n), (50Ti, n), (54Cr, n), (58Fe, n), (64Ni, n), (70Zn, n), (76Ge, n), (82Se, n), (86Kr, n), (88Sr, n), E not given; 232Th, 238U, 237Np, 242,244Pu, 243Am, 245,248Cm, 247Bk, 249Cf, 254Es, 257Fm(48Ca, 3n), (48Ca, 4n), E not given; calculated maximum σ systematics of Z=102-120 superheavy elements. 208Pb(76Se, X), (77Se, X), (78Se, X), (79Se, X), (80Se, X), (82Se, X), E*=11-14 MeV; 242,243,244,245,246,247,248,250Cm(48Ca, 3n), (48Ca, 4n), E*=28-42 MeV; calculated fusion σ systematics for Z=116 superheavy element production. Master equation within di-nuclear system model. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.046
2010FE10 Phys.Rev. C 82, 044615 (2010) Dynamics of pion production in heavy-ion collisions around 1A GeV energies
doi: 10.1103/PhysRevC.82.044615
2010FE12 Phys.Rev. C 82, 057901 (2010) Dynamics of strangeness production in heavy-ion collisions near threshold energies
doi: 10.1103/PhysRevC.82.057901
2009FE01 Nucl.Phys. A816, 33 (2009) Z.-Q.Feng, G.-M.Jin, J.-Q.Li, W.Scheid Production of heavy and superheavy nuclei in massive fusion reactions NUCLEAR REACTIONS 208Pb, 238U(16O, X), 148Sm(36Ar, X), 238U(26Mg, X), E not given; 232Th, 238U, 242,244Pu, 237Np, 243Am, 245,248Cm, 247Bk, 249Cf, 254Es, 257Fm(48Ca, X), E not given; 208Pb, 209Bi(48Ca, X), (50Ti, X), (54Cr, X), (58Fe, X), (64Ni, X), (70Zn, X), (76Ge, X), (82Se, X), (86Kr, X), (88Sr, X), E not given; 238U(40Ar, xn), (50Ti, xn), (54Cr, xn), (64Ni, xn), E not given; calculated fusion-fission σ vs compound nucleus excitation energy for superheavy element production. 244Pu, 248Cm(48Ca, X), E not given; calculated quasi-fission mass yields. 242,243,244,245,246,247,248,250Cm(48Ca, 3n), (48Ca, 4n), E not given; calculated fusion/fission barriers and neutron separation energy; 228,229,230,231,232Th(48Ca, 4n), E not given; 232,233,234,235,236,238U, 235,236,237Np(48Ca, 3n), E not given; 236,238,239,240,241,242,244Pu(48Ca, 3n), (48Ca, 4n), E not given; 241,242,243Am(48Ca, 3n), (48Ca, 4n), E not given; 247,248,249Bk(48Ca, 3n), E not given; 248,249,250,251,252Cf(48Ca, 3n), E not given; 238U(40Ar, 3n), (50Ti, 3n), (54Cr, 3n), (58Fe, 3n), (64Ni, 3n), E not given; calculated σ. Deduced isotopic trends for superheavy element production. Di-nuclear model.
doi: 10.1016/j.nuclphysa.2008.11.003
2009FE04 Phys.Rev. C 80, 037601 (2009) Fusion dynamics of symmetric systems near barrier energies NUCLEAR REACTIONS 58Ni(58Ni, X), 64Ni(64Ni, X), E(cm)=90-112 MeV; calculated dynamic fusion potentials and fusion barriers, nucleon transfers, ratio of neutron to proton in the neck region, and fusion excitation functions in the framework of isospin-dependent quantum molecular dynamics (ImIQMD) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.037601
2009FE06 Phys.Rev. C 80, 057601 (2009) Production of new superheavy Z=108-114 nuclei with 238U, 244Pu, and 248, 250Cm targets NUCLEAR REACTIONS 238U(36S, xn), (37Cl, xn), (40Ar, xn), (41K, xn), (45Sc, xn), (48Ti, xn), (50Ti, xn), 244Pu(30Si, xn), (31P, xn), (36S, xn), (37Cl, xn), (40Ar, xn), (41K, xn), 244Pu(30Si, xn), (31P, xn), (36S, xn), (37Cl, xn), (40Ar, xn), (41K, xn), 248,250Cm(26Mg, xn), (27Al, xn), (30Si, xn), (31P, xn), (36S, xn), (37Cl, xn), (40Ar, xn), E not given; calculated σ and optimal excitation energies using dinuclear system (DNS)model. Z=108-114; calculated cross sections for production of superheavy nuclei.
doi: 10.1103/PhysRevC.80.057601
2009FE08 Phys.Rev. C 80, 067601 (2009) Production of heavy isotopes in transfer reactions by collisions of 238U+238U NUCLEAR REACTIONS 238U(238U, X), E(cm)=800 MeV; calculated production cross sections and mass distributions of fragments with Z=80-108, A=200-270 within the framework of the DNS model.
doi: 10.1103/PhysRevC.80.067601
2009FE10 Chin.Phys.C 33, Supplement 1, 86 (2009) Z.-Q.Feng, G.-M.Jin, J.-Q.Li, W.Scheid Production mechanism of superheavy nuclei in massive fusion reactions NUCLEAR REACTIONS 208Pb(16O, X), E<80 MeV; 238U(16O, X), E<70 MeV; 148Sm(36Ar, X), E<75 MeV; 238U(26Mg, X), E<70 MeV; calculated fusion-fission σ, level density parameters, evaporation residue excitation functions. Dinuclear system (DNS) model.
doi: 10.1088/1674-1137/33/S1/028
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
2007BA76 Chin.Phys.Lett. 24, 3384 (2007) Z.Bai, Q.Wang, J.-L.Han, ZG.Xiao, H.-S.Xu, Z.-Y.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X-H.Yuan, Z.-G.Xu, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, J.-Q.Li, Y.-P.Zhang, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, W.Xu, G.-T.Fan, S.-Q.Zhang, D.-Y.Pang, Y.-K.Sergey Angular Dispersion and Deflection Function for Heavy Ion Elastic Scattering NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured differential cross sections, angular dispersion plots. 208Pb(16O, 16O), E=170.1 MeV; 208Pb(6He, 6He), E=27, 29.6 MeV; 208Pb(6Li, 6Li), E=73.7, 99 MeV; 208Pb(α, α), E=40 MeV; analyzed differential cross sections, angular dispersion plots.
doi: 10.1088/0256-307X/24/12/027
2007FE12 Chin.Phys.Lett. 24, 2551 (2007) Z.-Q.Feng, G.-M.Jin, M.-H.Huang, Z.-G.Gan, N.Wang, J.-Q.Li Possible Way to Synthesize Superheavy Element Z = 117 NUCLEAR REACTIONS 247,248,249Bk(48Ca, xn), 246Cm(45Sc, xn), 244Pu(51V, xn), 238U(55Mn, xn), 232Th(59Co, xn), 209Bi(76Se, n), (77Se, n), (78Se, n), (79Se, n), (80Se, n), (82Se, n), e not given; calculated cross sections and evaporation residue excitation functions within the framework of the dinuclear system model.
doi: 10.1088/0256-307X/24/9/024
2007FE17 Phys.Rev. C 76, 044606 (2007) Z.-Q.Feng, G.-M.Jin, J.-Q.Li, W.Scheid Formation of superheavy nuclei in cold fusion reactions NUCLEAR REACTIONS 208Pb(48Ca, n), (50Ti, n), (54Cr, n), (58Fe, n), (86Kr, n), (88Sr, n), (73Ge, n), (82Se, n), (86Kr, n), (88Sr, n), (59Ni, n), (60Ni, n), (61Ni, n), (62Ni, n), (63Ni, n), (64Ni, n), (65Ni, n), (65Zn, n), (66Zn, n), (67Zn, n), (68Zn, n), (69Zn, n), (70Ge, n), (72Ge, n), (73Ge, n), (74Ge, n), (75Ge, n), (76Ge, n), (76Se, n), (77Se, n), (78Se, n), (79Se, n), (80Se, n), (82Se, n), (84Sr, n), (86Sr, n), (87Sr, n), E=not given; 208Pb(70Zn, n), E=240-280 MeV; 209Bi(64Ni, n), (48Ca, n), (50Ti, n), (54Cr, n), (58Fe, n), (86Kr, n), (88Sr, n), (73Ge, n), (64Ni, n), (70Zn, n), (76Ge, n), (82Se, n), E=not given; calculated maximal production cross sections of Z=102-120 elements, fusion probabilities, comparison with experimental cross sections, DNS model.
doi: 10.1103/PhysRevC.76.044606
2006FE05 Nucl.Phys. A771, 50 (2006) Z.-Q.Feng, G.-M.Jin, F.Fu, J.-Q.Li Production cross sections of superheavy nuclei based on dinuclear system model NUCLEAR REACTIONS 206,208Pb(48Ca, X), (48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=5-60 MeV; calculated capture and evaporation σ. 242,244Pu, 248Cm(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E*=20-70 MeV; 238U(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E*=20-70 MeV; 243Am, 248Cm(48Ca, 3n), (48Ca, 4n), E*=20-70 MeV; calculated fusion-evaporation σ. 236,237,238,239,240,241,242,243,244Pu(48Ca, 3n), (48Ca, 3n), E not given; analyzed maximal production σ. Di-nuclear system model, comparisons with data.
doi: 10.1016/j.nuclphysa.2006.03.002
2006WA17 Chin.Phys.Lett. 23, 1731 (2006) Q.Wang, J.-L.Han, Z.-G.Xiao, H.-S.Xu, Z.-Yu.Sun, Z.-G.Hu, X.-Y.Zhang, H.-W.Wang, R.-S.Mao, X.-H.Yuan, Z.-G.Xu, T.-C.Zhao, H.-B.Zhang, H.-G.Xu, H.-R.Qi, Y.Wang, F.Jia, L.-J.Wu, X.-L.Ding, Q.Gao, H.Gao, S.-L.Li, Z.Bai, G.-Q.Xiao, G.-M.Jin, Z.-Z.Ren, S.-G.Zhou, Yu.-K.Sergey Exotic Behaviour of Angular Dispersion of Weakly Bound Nucleus 17F at Small Angles NUCLEAR REACTIONS 208Pb(17F, 17F), E=141 MeV; 208Pb(17O, 17O), E=128 MeV; measured σ(θ); deduced possible halo effects.
doi: 10.1088/0256-307X/23/7/021
2006XI01 Phys.Lett. B 639, 436 (2006) Z.G.Xiao, R.J.Hu, H.Y.Wu, G.M.Jin, Z.Y.Li, L.M.Duan, H.W.Wang, B.G.Zhang, S.F.Wang, Z.Y.Wei, H.S.Xu, Y.T.Zhu, S.L.Li, F.Fu, X.H.Yuan, Z.Q.Feng System dependence of the correlation function of IMFs in 36Ar + 112, 124Sn at 35 MeV/u NUCLEAR REACTIONS 112,124Sn(36Ar, X), E=35 MeV/nucleon; measured intermediate mass fragments charge, mass and velocity distributions and correlation function; deduced time sequence, related reaction mechanism features.
doi: 10.1016/j.physletb.2006.06.076
2006ZH39 Int.J.Mod.Phys. E15, 1601 (2006) 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
2005FE04 Nucl.Phys. A750, 232 (2005) Z.-Q.Feng, F.-S.Zhang, G.-M.Jin, X.Huang Improved isospin dependent quantum molecular dynamics model and its application to fusion reactions near Coulomb barrier NUCLEAR REACTIONS 40,48Ca(40Ca, X), (48Ca, X), E(cm) ≈ 48-68 MeV; calculated fusion excitation functions. Isospin-dependent quantum molecular dynamics model, comparison with data.
doi: 10.1016/j.nuclphysa.2005.01.001
2005FE05 Chin.Phys.Lett. 22, 846 (2005) Z.-Q.Feng, G.-M.Jin, F.Fu, F.S.Zhang, F.Jia, X.Huang, R.-J.Hu, W.-F.Li, J.-Q.Li Entrance Channel Dependence of Production Cross Sections of Superheavy Nuclei in Cold Fusion Reactions NUCLEAR REACTIONS 208Pb(50Ti, X), (58Fe, X), 124Sn(134Xe, X), 136Xe(130Xe, X), E not given; calculated interaction potentials. 208Pb(50Ti, n), E(cm) ≈ 176-196 MeV; 124Sn(136Xe, n), (134Xe, n), E(cm) ≈ 284-292 MeV; 208Pb(58Fe, n), E(cm) ≈ 212-225 MeV; 136Xe(130Xe, n), E(cm) ≈ 306-316 MeV; calculated evaporation residue σ. Dinuclear system model, comparisons with data.
doi: 10.1088/0256-307X/22/4/019
2005FE13 Chin.Phys.Lett. 22, 3040 (2005) Z.-Q.Feng, G.-M.Jin, F.-S.Zhang, F.Fu, X.Huang Dynamical Study on Fusion Barrier in the Synthesis of Superheavy Elements NUCLEAR REACTIONS 208Pb(48Ca, X), E not given; calculated interaction potential. 238U(48Ca, X), E(cm)=200 MeV; calculated fusion barrier height, nucleon transfer in neck region as a function of time. 208Pb(48Ca, X), E(cm)=180, 200 MeV; 238U(48Ca, X), E(cm)=190 MeV; calculated neck radius vs time. Z=110-116; calculated fusion barriers for various reaction systems leading to superheavy elements. Isospin-dependent quantum molecular dynamics model.
doi: 10.1088/0256-307X/22/12/015
2004GA29 Eur.Phys.J. A 20, 385 (2004) Z.G.Gan, J.S.Guo, X.L.Wu, Z.Qin, H.M.Fan, X.G.Lei, H.Y.Liu, B.Guo, H.G.Xu, R.F.Chen, C.F.Dong, F.M.Zhang, H.L.Wang, C.Y.Xie, Z.Q.Feng, Y.Zhen, L.T.Song, P.Luo, H.S.Xu, X.H.Zhou, G.M.Jin, Z.Ren New isotope 265Bh NUCLEAR REACTIONS 243Am(26Mg, 4n), E=168 MeV; measured delayed (recoil)α-, αα-coin following residual nucleus decay; deduced evidence for 265Bh. RADIOACTIVITY 264,265Bh, 261Db, 257Lr(α) [from 243Am(26Mg, 4n) and subsequent decay]; measured decay products, Eα, Iα; deduced T1/2.
doi: 10.1140/epja/i2004-10020-2
2004GA62 High Energy Phys. and Nucl.Phys. (China) 28, 332 (2004) Z.-G.Gan, H.-M.Fan, Z.Qin, X.-L.Wu, J.-S.Guo, X.-G.Lei, C.-F.Dong, H.-G.Xu, R.-F.Chen, F.-M.Zhang, B.Guo, H.-Y.Liu, H.-L.Wang, C.-Y.Xie, Z.-Q.Feng, Y.Zheng, L.-T.Song, P.Luo, H.-S.Xu, X.-H.Zhuo, G.-M.Jin, Z.-Z.Ren First Observation for Isotope 265Bh(Z=107)
2002CH31 Chin.Phys.Lett. 19, 921 (2002) T.Chen, Y.-L.Ye, Z.-H.Li, D.-X.Jiang, H.Hua, X.-Q.Li, Q.-J.Wang, Y.-C.Ge, D.-Y.Pang, Z.-Y.Di, G.-M.Jin, G.-Q.Xiao, Z.-Y.Guo, Z.-G.Xiao, H.-W.Wang, B.-G.Zhang, H.-Y.Wu, J.-X.Li, Z.-Y.Sun, W.-L.Zhan Quasi-Elastic Scattering of a Secondary 6He Beam on a 9Be Target at 25MeV/Nucleon NUCLEAR REACTIONS 9Be(6He, 6He), E=25 MeV/nucleon; measured σ(θ); deduced optical model parameters..
doi: 10.1088/0256-307X/19/7/311
2002GU33 J.Nucl.Radiochem.Sci. 3, No 1, 183 (2002) J.S.Guo, Z.Qin, Z.G.Gan, H.M.Fan, Y.B.Xu, J.J.He, X.G.Lei, X.L.Wu, H.Y.Liu, X.H.Zhou, S.G.Yuan, G.M.Jin Preparation of Thick Americium Targets and Synthesis of 259Db NUCLEAR REACTIONS 241Am(22Ne, 4n), E=118 MeV; measured delayed Eα, αα-coin; deduced evidence for 259Db. RADIOACTIVITY 259Db, 255Lr(α) [from 241Am(22Ne, 4n) and subsequent decay]; measured Eα, T1/2.
2002LI40 Chin.Phys.Lett. 10, 917 (2002) X.-Q.Li, D.-X.Jiang, Y.-L.Ye, H.Hua, T.Chen, Z.-H.Li, Y.-C.Ge, Q.-J.Wang, H.-Y.Wu, G.-M.Jin, L.-M.Duan, Z.-G.Xiao, H.-W.Wang, Z.-Y.Li, S.-F.Wang Isotopic Distributions of the 18N Fragmentation Products in Coincidence with Neutrons on Targets 197Au and 9Be NUCLEAR REACTIONS 9Be, 197Au(18N, X), E=33 MeV/nucleon; measured fragments isotopic yields, (fragment)(neutron)-coin. 18N deduced nucleon density distribution. Abrasion-ablation model.
2002WA33 High Energy Phys. and Nucl.Phys. (China) 26, 1117 (2002) H.-W.Wang, G.-M.Jin, H.-Y.Wu, Z.-G.Xiao, B.-G.Zhang, L.-M.Duan, Z.-Y.Wei, Z.-Y.Li, R.-J.Hu, Y.-Y.Liu, Z.-H.Lu, K.-L.Chen, S.-F.Wang, H.-D.Zhu, X.-Q.Li, T.Chen, H.Hua Experimental Study on 22Na(p, γ)23Mg Reaction
2002WU04 Phys.Lett. 538B, 39 (2002) H.-Y.Wu, Z.-G.Xiao, G.-M.Jin, B.-G.Zhang, Z.-Y.Li, L.-M.Duan, H.-W.Wang, Z.-Y.Wei, Y.-Y.Liu, S.-F.Wang, Z.-H.Lu, Y.-T.Zhu, H.-D.Zhu, R.-J.Hu Evidence of 'Slow ' Relaxation of Isospin Degree of Freedom NUCLEAR REACTIONS 112,124Sn(36Ar, X), (40Ar, X), E=35 MeV/nucleon; measured fragments isotope yield ratios vs kinetic energy; deduced isospin non-equilibrium in dissipative fragment emission process.
doi: 10.1016/S0370-2693(02)01971-8
2001FA25 High Energy Phys. and Nucl.Phys. (China) 25, 602 (2001) H.-M.Fan, Z.-G.Gan, Z.Qin, X.-G.Lei, Y.-B.Xu, J.-J.He, H.-Y.Liu, X.-L.Wu, J.-S.Guo, X.-H.Zhou, S.-G.Yuan, G.-M.Jin A New Isotope of Z=105 with Mass Number 259
2001GA20 Eur.Phys.J. A 10, 21 (2001) Z.G.Gan, Z.Qin, H.M.Fan, X.G.Lei, Y.B.Xu, J.J.He, H.Y.Liu, X.L.Wu, J.S.Guo, X.H.Zhou, S.G.Yuan, G.M.Jin A New Alpha-Particle-Emitting Isotope 259Db NUCLEAR REACTIONS 241Am(22Ne, 4n), (22Ne, 5n), E=118 MeV; measured Eα, αα-coin following residual nucleus decay; deduced evidence for 258,259Db. RADIOACTIVITY 258,259Db, 254,255Lr(α) [from 241Am(22Ne, xn) and subsequent decay]; measured Eα, T1/2.
doi: 10.1007/s100500170140
2001WA53 High Energy Phys. and Nucl.Phys. (China) 25, 731 (2001) H.-W.Wang, H.-Y.Wu, G.-M.Jin, B.-G.Zhang, Z.-G.Xiao, L.-M.Duan, Z.-Y.Wei, Z.-Y.Li, Z.-H.Lu, Y.-Y.Liu, K.-L.Chen, R.-J.Hu, H.-D.Zhu, L.Cen, S.-F.Wang, X.-Q.Li, T.Chen, H.Hua Measurement of β+ Delayed α Decay of 20Na
2001WA54 High Energy Phys. and Nucl.Phys. (China) 25, 971 (2001) H.-W.Wang, G.-M.Jin, H.-Y.Wu, B.-G.Zhang, Z.-G.Xiao, L.-M.Duan, Z.-Y.Wei, Z.-Y.Li, Z.-H.Lu, Y.-Y.Liu, K.-L.Chen, R.-J.Hu, H.-D.Zhu, L.Cen, S.-F.Wang, X.-Q.Li, T.Chen, H.Hua Measurement of β+ Delay Proton Decay of 23Al
2001XI02 Chin.Phys.Lett. 18, 1037 (2001) Z.-G.Xiao, G.-M.Jin, H.-Y.Wu, Z.-Y.Wei, H.-W.Wang, L.-M.Duan, Y.-Y.Liu, Z.-Y.Li, B.-G.Zhang, Y.-T.Zhu, S.-F.Wang, Z.-H.Lu, H.-D.Zhu, R.-J.Hu Experimental Probe to the Isospin-Dependent Properties of Hot Nuclei in Reactions 40Ar + 112, 124Sn at 30 MeV/u NUCLEAR REACTIONS 112,124Sn(40Ar, X), E=30 MeV/nucleon; measured light charged particles emission probability, energy spectra.
doi: 10.1088/0256-307X/18/8/313
2001ZH45 High Energy Phys. and Nucl.Phys. (China) 25, 636 (2001) B-G.Zhang, S.-F.Wang, L.-M.Duan, W.-X.Wen, G.-M.Jin, Z.-Y.Li, Z.-Y.He, H.-W.Wang, Z.-G.Xiao, J.-W.Zheng, H.-Y.Wu, Z.-Y.Wei Investigation of Nuclear Deformation in Excited 213Fr
2000FA06 Phys.Rev. C61, 044610 (2000) D.Q.Fang, W.Q.Shen, J.Feng, X.Z.Cai, J.S.Wang, Q.M.Su, Y.G.Ma, Y.T.Zhu, S.L.Li, H.Y.Wu, Q.B.Gou, G.M.Jin, W.L.Zhan, Z.Y.Guo, G.Q.Xiao Isospin Effect of Fragmentation Reactions Induced by Intermediate Energy Heavy Ions and Its Disappearance NUCLEAR REACTIONS Be(18O, X)14N/15N/16N/17N/12C/13C/14C/15C/10B/11B/12B/13B/9Be/10Be/11Be, E=60 MeV/nucleon; measured production σ. Be(16O, X), (18O, X), (36Ar, X), (40Ar, X), E=60 MeV/nucleon; calculated fragments isotopic production σ; deduced isospin effects. Modified statistical abrasion-ablation model.
doi: 10.1103/PhysRevC.61.044610
2000FA09 Chin.Phys.Lett. 17, 267 (2000) D.-Q.Fang, W.-Q.Shen, J.Feng, X.-Z.Cai, J.-S.Wang, Q.-M.Su, Y.-G.Ma, Y.-T.Zhu, S.-L.Li, H.-Y.Wu, Q.-B.Gou, G.-M.Jin, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao Isospin Effect of Fragmentation Reaction on the Isotopic Distribution Produced in Intermediate Energy Heavy Ion Collisions NUCLEAR REACTIONS Be(18O, X), E=60 MeV/nucleon; measured fragments isotopic yields; deduced isospin effects. Modified statistical abrasion-ablation model.
2000FA12 Phys.Rev. C61, 064311 (2000) D.Q.Fang, W.Q.Shen, J.Feng, X.Z.Cai, J.S.Wang, Q.M.Su, H.Y.Zhang, P.Y.Hu, Y.G.Ma, Y.T.Zhu, S.L.Li, H.Y.Wu, Q.B.Gou, G.M.Jin, W.L.Zhan, Z.Y.Guo, G.Q.Xiao Measurements of Total Reaction Cross Sections for Some Light Nuclei at Intermediate Energies NUCLEAR REACTIONS 12C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (14N, X), (15N, X), (16N, X), (17N, X), (16O, X), (17O, X), (18O, X), E ≈ 35 MeV/nucleon; measured reaction σ. Comparison with Glauber model calculations. Secondary beams from 18O fragmentation.
doi: 10.1103/PhysRevC.61.064311
2000FA17 Chin.Phys.Lett. 17, 655 (2000) D.-Q.Fang, W.-Q.Shen, J.Feng, X.-Z.Cai, J.-S.Wang, Q.-M.Su, H.-Y.Zhang, P.-Y.Hu, Y.-G.Ma, Y.-T.Zhu, S.-L.Li, H.-Y.Wu, Q.-B.Gou, G.-M.Jin, W.-L.Zhan, Z.-Y.Guo, G.-Q.Xiao Measurements of Total Reaction Cross Section for Light Nuclei and Evidence for the Anomalous Nuclear Structure in 15C NUCLEAR REACTIONS C(12C, X), (13C, X), (14C, X), (15C, X), (16C, X), (14N, X), (15N, X), (16N, X), (17N, X), (16O, X), (17O, X), (18O, X), E ≈ 27-41 MeV; measured reaction σ. 15C deduced possible anomalous structure.
2000HU08 Chin.Phys.Lett. 17, 188 (2000) H.Hua, D.-X.Jiang, X.-Q.Li, T.Qian, H.-Y.Wu, G.-M.Jin, W.-L.Zhan, L.-M.Duan, Z.-G.Xiao, Z.-Y.Guo, Z.-Y.Li, H.-W.Wang, S.-F.Wang Breakup of 33.4 MeV/u 17N on a 9Be Target NUCLEAR REACTIONS 9Be(17N, nX), E=33.4 MeV/nucleon; measured neutron spectra, σ(θ), (nitrogen)(neutron)-coin; deduced reaction mechanism features. Nuclear diffraction dissociation model, two-cluster wave function.
doi: 10.1088/0256-307X/17/3/012
2000ZA13 High Energy Phys. and Nucl.Phys. (China) 24, 823 (2000) L.Zang, Q.-Y.Hu, J.-H.Zhao, J.-W.Zheng, Z.-K.Li, S.-H.Li, Z.-G.Gan, Y.Yu, H.-M.Fan, B.Guo, T.-M.Zhang, C.-F.Wang, T.-Q.Wang, G.-M.Jin, K.Morita, A.Yoshita, Y.-H.Pu, H.Kuto, Y.Yano γ Scheme Following 208Hg β- Decay
1999CH22 Phys.Lett. 459B, 21 (1999) L.-W.Chen, F.-S.Zhang, G.-M.Jin, Z.-Y.Zhu Isospin Dependence of Radial Flow in Heavy-Ion Collisions at Intermediate Energies NUCLEAR REACTIONS 124Sn(124Sn, X), 124Ba(124Ba, X), E=100, 150, 200, 600 MeV/nucleon; calculated fragments mean kinetic energy vs charge, radial flow features; deduced isospin effects. Isospin-dependent QMD.
doi: 10.1016/S0370-2693(99)00628-0
1999GA41 Eur.Phys.J. A 6, 59 (1999) Z.G.Gan, Z.Qin, J.S.Guo, L.J.Shi, H.Y.Liu, T.R.Guo, X.G.Lei, R.C.Ma, W.X.Huang, S.G.Yuan, X.Q.Zhang, G.M.Jin Decay of the Very Neutron-Deficient Isotope 131Pm RADIOACTIVITY 131Pm(β+), (EC) [from 106Cd(32S, 4n3p), E=170 MeV]; measured Eγ, Iγ, γγ-, (X-ray)γ-coin, T1/2. 131Nd, 131Pr deduced levels.
doi: 10.1007/s100500050317
1999HU05 Phys.Rev. C59, 2402 (1999) W.X.Huang, R.C.Ma, S.W.Xu, X.J.Xu, J.S.Guo, X.F.Sun, Y.X.Xie, Z.K.Li, Y.X.Ge, Y.Y.Wang, C.F.Wang, T.M.Zhang, G.M.Jin, Y.X.Luo β-Delayed Proton Decays of the Tz = 1/2 Series Nuclei, 81Zr and 85Mo RADIOACTIVITY 81Zr, 85Mo(β+p) [from 58Ni(32S, xnypza)]; measured Eγ, Iγ, proton spectra, pγ-coin, T1/2; deduced proton decay branching ratios. 81Zr, 85Mo deduced ground-state J, π, mass excesses. He-jet, tape transportation.
doi: 10.1103/PhysRevC.59.2402
1999WU04 Chin.Phys.Lett. 16, 499 (1999) E.-J.Wu, J.-W.Zheng, Z.-G.Xiao, C.Zhang, J.-L.Tan, S.-Z.Yin, S.-F.Wang, G.-M.Jin, X.Yin, M.-T.Song, W.-Y.Jin, X.-P.Peng, Z.-Y.Li, H.-Y.Wu, Z.-Y.He, D.-X.Jiang, X.Qian Evidence for Different Fission Behavior of Hot Nuclei Formed in Central and Peripheral Collisions of 40Ar + 209Bi Reaction at 25 MeV/u NUCLEAR REACTIONS 209Bi(40Ar, X), E=25 MeV/nucleon; measured α spectra, fission fragments mass, energy distributions vs compound nucleus excitation energy; deduced two fission modes.
doi: 10.1088/0256-307X/16/7/011
1999XU05 Phys.Rev. C60, 061302 (1999) S.-W.Xu, Z.-K.Li, Y.-X.Xie, Q.-Y.Pan, Y.Yu, J.Adam, C.-F.Wang, J.-P.Xing, Q.-Y.Hu, S.-H.Li, H.-Y.Chen, T.-M.Zhang, G.-M.Jin, Y.-X.Luo, Yu.Penionzhkevich, Yu.Gangrsky New β-Delayed Proton Precursors in the Rare-Earth Region Near the Proton Drip Line RADIOACTIVITY 125Nd, 128Pm, 129Sm, 137Gd, 139Dy(β+p) [from 92Mo, 96Ru, 106Cd(36Ar, X)]; measured β-delayed proton spectra, Eγ, Iγ, pγ-coin, T1/2. 125Nd, 129Sm, 137Gd, 139Dy deduced ground-state J, π, deformation. He-jet tape transport system. NUCLEAR REACTIONS 92Mo(36Ar, 3n), E=169 MeV; 96Ru(36Ar, 3n), E=174 MeV; 96Ru(36Ar, 3np), E=165 MeV; 106Cd(36Ar, nα), (36Ar, 3n), E=176 MeV; measured production σ.
doi: 10.1103/PhysRevC.60.061302
1998HE03 Eur.Phys.J. A 1, 61 (1998) Z.Y.He, G.M.Jin, Z.Y.Li, L.M.Duan, G.X.Dai, B.G.Zhang, H.Y.Wu, W.X.Wen, Y.J.Qi, Q.Z.Luo, S.F.Wang Emission Order of Light Particles and Light Fragments from Hot Nuclei followed by Binary Fission NUCLEAR REACTIONS 197Au(40Ar, F), E=25 MeV/nucleon; measured light charged particles, fission fragments correlation; deduced light particles relative emission order.
doi: 10.1007/s100500050032
1998HE08 Phys.Rev. C57, 1824 (1998) Z.Y.He, G.M.Jin, Z.Y.Li, L.M.Duan, G.X.Dai, B.G.Zhang, H.Y.Wu, W.X.Wen, Y.J.Qi, Q.Z.Luo Emission Time Scales for Light Charged Particles from Symmetric and Asymmetric Fission Processes for 40Ar + 197Au Reactions at 25 MeV/nucleon NUCLEAR REACTIONS 197Au(40Ar, X), E=25 MeV/nucleon; measured fission-associated light charged particle spectra, coincidences; deduced two-particle correlation functions, emission time scale.
doi: 10.1103/PhysRevC.57.1824
1998HE14 Chin.Phys.Lett. 15, 13 (1998) Z.-Y.He, Z.-Y.Li, L.-M.Duan, B.-G.Zhang, G.-M.Jin, G.-X.Dai, Y.-B.Fu, H.-W.Wang, S.-F.Wang Rotational Effect of Intermediate Mass Fragments for 40Ar + 159Tb Reaction at 30 MeV/Nucleon NUCLEAR REACTIONS 159Tb(40Ar, X), E=30 MeV/nucleon; measured light particle, intermediate mass fragment yields, rapidity distributions; deduced in-plane enhancement.
doi: 10.1088/0256-307X/15/1/006
1998QI03 Chin.Phys.Lett. 15, 255 (1998) T.Qian, D.-X.Jiang, H.Hua, G.-M.Jin, E.-J.Wu, J.-W.Zheng, S.-Z.Yin, J.-L.Tan, Z.-Y.He, Z.-Y.Li, L.-M.Duan Non-Equilibrated Emission of Intermediate Mass Fragments in 25 MeV/n 40Ar + (nat)Ag Reaction NUCLEAR REACTIONS Ag(40Ar, X), E=25 MeV/nucleon; analyzed intermediate mass fragments σ(E, θ). Statistical model, quantum molecular dynamics model. Comparison with data.
doi: 10.1088/0256-307X/15/4/008
1998WU03 Phys.Rev. C57, 3178 (1998) H.-Y.Wu, G.-X.Dai, G.-M.Jin, Z.-Y.Li, L.-M.Duan, Z.-Y.He, W.-X.Wen, B.-G.Zhang, Y.-J.Qi, Q.-Z.Luo, Z.-K.Li Evolution of the Decay of Highly Excited Nuclei NUCLEAR REACTIONS 115In, 159Tb, 197Au, 209Bi(40Ar, X), E=25 MeV/nucleon; measured ternary fragment events angular correlations vs time; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.57.3178
1998ZH19 Eur.Phys.J. A 2, 5 (1998) L.Zhang, J.H.Zhao, J.W.Zheng, J.C.Wang, Z.Qin, Y.F.Yang, C.Zhang, G.M.Jin, G.H.Guo, Y.F.Du, T.R.Guo, T.Q.Wang, B.Guo, J.F.Tain Identification of 209Hg NUCLEAR REACTIONS Pb(18O, X), E=600 MeV; measured delayed γ activity; deduced evidence for 209Hg. 209Hg deduced T1/2.
doi: 10.1007/s100500050082
1997HE08 Nucl.Phys. A620, 214 (1997) Z.Y.He, L.M.Duan, G.M.Jin, Z.Y.Li, H.Y.Wu, B.G.Zhang, W.X.Wen, Y.J.Qi, Q.Z.Luo, G.X.Dai The Correlation Functions and Emission Time Scales for Light Particles and Light Fragments in 40Ar + 197Au Reactions at 25 MeV/nucleon NUCLEAR REACTIONS 197Au(40Ar, X), E=25 MeV/nucleon; measured light charged particles, intermediate mass fragments correlation functions; deduced mean emission time, temperature.
doi: 10.1016/S0375-9474(97)00161-9
1997HU07 Phys.Rev. C56, 1152 (1997) W.X.Huang, R.C.Ma, X.J.Xu, S.W.Xu, Y.X.Xie, Z.K.Li, Y.X.Ge, Y.Y.Wang, C.F.Wang, T.M.Zhang, X.F.Sun, G.M.Jin, Y.X.Luo Proton Branching Ratios in the β-Delayed Proton Decay of 87Mo RADIOACTIVITY 87Mo(EC), (β+p) [from 58Ni(32S, n2p), E=150 MeV]; measured Ep, Ip, Eγ, T1/2, γ-coin following β-delayed proton decay. 86Zr levels deduced proton branching ratios. Enriched 58Ni target, He-jet, Si(Au), hyperpure Ge detectors.
doi: 10.1103/PhysRevC.56.1152
1997HU15 Z.Phys. A359, 349 (1997) W.X.Huang, R.C.Ma, X.J.Xu, S.W.Xu, Y.X.Xie, Z.K.Li, Y.X.Ge, Y.Y.Wang, C.F.Wang, T.M.Zhang, X.F.Sun, G.M.Jin, Y.X.Luo Half-Lives of the T(z) = 1/2 Series Nuclei, 81Zr and 85Mo RADIOACTIVITY 81Zr, 85Mo(β+p) [from 58Ni(32S, X), E=170 MeV]; measured β-delayed Ep, Ip, Eγ, Iγ, (proton)γ-coin, T1/2. He-jet, fast tape transport.
doi: 10.1007/s002180050413
1997LI36 Z.Phys. A359, 247 (1997) Z.-Y.Li, Z.-Y.He, L.-M.Duan, G.-M.Jin, H.-Y.Wu, B.-G.Zhang, W.-X.Wen, Y.-J.Qi, Q.-Z.Luo, G.-X.Dai, H.-W.Wang Impact Parameter Selected Nuclear Temperatures of Hot Nuclei from Excited State Populations for 40Ar + 197Au Reactions at E/A = 25 MeV NUCLEAR REACTIONS 197Au(40Ar, X), E=25 MeV/nucleon; measured αα(fission fragment)-coin; deduced 8Be yield ratios vs temperature, reaction mechanism features.
doi: 10.1007/s002180050398
1997WE09 Nucl.Phys. A626, 561c (1997) B.W.Wei, Y.X.Luo, G.M.Jin, W.L.Zhan, J.W.Xia Proposal of a Cooler Storage Ring - An Upgrading Plan of HIRFL
doi: 10.1016/S0375-9474(97)00580-0
1996HE05 Nucl.Phys. A598, 248 (1996) Z.Y.He, J.C.Angelique, G.Auger, G.Bizard, R.Brou, A.Buta, C.Cabot, E.Crema, D.Cussol, G.X.Dai, Y.El Masri, Ph.Eudes, M.Gonin, K.Hagel, G.M.Jin, A.Kerambrun, C.Lebrun, Y.G.Ma, A.Peghaire, J.Peter, R.Popescu, R.Regimbart, E.Rosato, F.Saint-Laurent, W.Q.Shen, J.C.Steckmeyer, B.Tamain, E.Vient, R.Wada, F.S.Zhang Disappearance of Flow and the In-Medium Nucleon-Nucleon Cross Section for 64Zn + 27Al Collisions at Intermediate Energies NUCLEAR REACTIONS 27Al(64Zn, X), E=49-79 MeV/nucleon; measured light charged particle collective transverse momentum; deduced flow parameter, σ(NN).
doi: 10.1016/0375-9474(95)00486-6
1996HE15 Chin.Phys.Lett. 13, 168 (1996) Z.-Y.He, G.-M.Jin, Z.-Y.Li, L.-M.Duan, G.-X.Dai, B.-G.Zhang, H.-Y.Wu, W.-X.Wen, Q.-Z.Luo, Y.-J.Qi Evolution from Sequential Decay to Simultaneous Multifragmentation with Increasing Beam Energy NUCLEAR REACTIONS 197Au(40Ar, X), E=25 MeV/nucleon; measured (fragment)(fragment)-correlation functions; deduced light fragments mean emission time, sequential decay evidence. Comparison with other data, three-body trajectory calculation.
doi: 10.1088/0256-307X/13/3/003
1996WE16 Chin.Phys.Lett. 13, 724 (1996) W.-X.Wen, J.-Q.Zhong, G.-M.Jin Giant Monopole Resonance with Boltzmann-Nordheim-Vlasov Model NUCLEAR REACTIONS 40Ca(40Ca, X), 108Ag(40Ar, X), E=25 MeV/nucleon; calculated total kinetic energy, quadrupole moment, mean squared radii time evolution; deduced giant monopole resonance related features. Boltzmann-Nordheim-Vlasov model.
doi: 10.1088/0256-307X/13/10/002
1995DA07 Nucl.Phys. A583, 173c (1995) G.X.Dai, H.Y.Wu, Z.Y.He, Q.Z.Luo, L.M.Duan, B.G.Zhang, Y.J.Qi, Z.Y.Li, G.M.Jin, W.X.Wen The 4-Fold Fission in 40Ar + 209Bi, 197Au and 159Tb Reactions at 25 MeV/u NUCLEAR REACTIONS 197Au, 159Tb, 209Bi(40Ar, F), (40Ar, X), E=25 MeV/nucleon; measured fission, breakup fragment mass, velocity, total kinetic energy.
doi: 10.1016/0375-9474(94)00656-8
1995ZH53 Chin.J.Nucl.Phys. 17, No 3, 247 (1995) X.Zhang, W.-X.Li, X.M.Yin, W.-X.Wen, T.-Y.Sun, G.-M.Jin, Q.-Z.Luo Mass Yield Distribution in Intermediate Energy Heavy Ion Reactions NUCLEAR REACTIONS Cu(40Ar, X), E=40 MeV/nucleon; measured fragment mass yield distribution. Off-line γ-spectroscopy. Statistical binary decay model.
1994HE41 Chin.J.Nucl.Phys. 16, No 4, 313 (1994) Z.-Y.He, G.-X.Dai, G.-M.Jin, F.-S.Zhang, W.-Q.Shen, Y.-G.Ma Disappearance of Flow as a Function of Impact Parameter for 64Zn + 58Ni Collisions at Intermediate Energies NUCLEAR REACTIONS 58Ni(64Zn, X), E=49-120 MeV/nucleon; calculated nucleon transverse momentum distribution, flow parameter vs E balance energy vs input parameter; deduced in-medium σ(nucleon-nucleon), impact parameter dependences. BUU equation.
1994LI66 Chin.J.Nucl.Phys. 16, No 4, 328 (1994) Z.-Y.Li, Q.-Z.Luo, G.-M.Jin, H.-Y.Wu, Z.-Y.He, L.-M.Duan, B.-G.Zhang, Y.-J.Qi, W.-X.Wen, B.-R.Dang, D.-H.Yan, G.-X.Dai Particle-Particle Correlations for 40Ar Induced Reactions on 197Au at 25 MeV/A NUCLEAR REACTIONS 197Au(40Ar, X), E=25 MeV/nucleon; measured pp-, pt-, αα-correlations; deduced 8Be, 8Be(*) yields. 8Be deduced average α-emitting temperature. Statistical model.
1994LO02 Phys.Lett. 320B, 221 (1994) M.Louvel, A.Genoux-Lubain, G.Bizard, R.Bougault, R.Brou, A.Buta, H.Doubre, D.Durand, Y.El Masri, H.Fugiwara, K.Hagel, T.Hamdani, F.Hanappe, S.C.Jeong, G.M.Jin, S.Kato, J.L.Laville, C.LeBrun, J.F.Lecolley, S.M.Lee, T.Matsuse, T.Motobayashi, A.Peghaire, J.Peter, R.Regimbart, F.Saint-Laurent, J.C.Steckmeyer, B.Tamain Rapid Decrease of Fragment Emission Time in the Range of 3-5 MeV/u Excitation Energy NUCLEAR REACTIONS 197Au(40Ar, X), E=30, 60 MeV/nucleon; measured fragment correlation functions, relative velocity; deduced fragment emission time vs excitation energy.
doi: 10.1016/0370-2693(94)90648-3
1993CU04 Nucl.Phys. A561, 298 (1993) D.Cussol, G.Bizard, R.Brou, D.Durand, M.Louvel, J.P.Patry, J.Peter, R.Regimbart, J.C.Steckmeyer, J.P.Sullivan, B.Tamain, E.Crema, H.Doubre, K.Hagel, G.M.Jin, A.Peghaire, F.Saint-Laurent, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.MacGrath, S.C.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Charged-Particle Calorimetry of 40Ar + 27Al Reactions from 36 to 65 MeV/u NUCLEAR REACTIONS 27Al(40Ar, X), E=36-65 MeV/nucleon; measured fragment mass, velocity, energy distributions; deduced hot nuclei temperatures, excitation energies. Charged-particle calorimetry.
doi: 10.1016/0375-9474(93)90155-Q
1993LO07 Nucl.Phys. A559, 137 (1993) M.Louvel, T.Hamdani, G.Bizard, R.Bougault, R.Brou, H.Doubre, D.Durand, Y.El Masri, H.Fugiwara, A.Genoux-Lubain, K.Hagel, A.Hajfani, F.Hanappe, S.C.Jeong, G.M.Jin, S.Kato, J.L.Laville, C.Le Brun, J.F.Lecolley, S.Lee, T.Matsuse, T.Motobayashi, J.P.Patry, A.Peghaire, J.Peter, N.Prot, R.Regimbart, F.Saint-Laurent, J.C.Steckmeyer, B.Tamain Multifragment Decay of Highly Excited Nuclei NUCLEAR REACTIONS 197Au(40Ar, X), E=30, 60 MeV/nucleon; measured threefold, fourfold fragment events, light charged particles-coin, selected central collision events; deduced linear momentum transfer, residuals excitation energies, multiplicities, nuclear temperature.
doi: 10.1016/0375-9474(93)90183-X
1993RU04 Phys.Lett. 307B, 287 (1993) G.Rudolf, S.Tomasevic, M.Aboufirassi, J.C.Adloff, B.Bilwes, R.Bilwes, G.Bizard, R.Bougault, R.Brou, Y.Cassagnou, J.Colin, F.Cosmo, F.Delaunay, D.Durand, J.L.Ferrero, A.Genoux-Lubain, M.Glaser, F.Guilbault, G.M.Jin, J.L.Laville, C.Le Brun, C.Lebrun, J.F.Lecolley, F.Lefebvres, R.Legrain, J.Lemiere, O.Lopez, M.Louvel, M.Mahi, A.Peghaire, J.Peter, B.Rastegar, E.Rosato, F.Scheibling, J.C.Steckmeyer, L.Stuttge, B.Tamain Fragmentation Pattern in Sequential Emission Spectra NUCLEAR REACTIONS 197Au(84Kr, X), E=27, 44 MeV/nucleon; 197Au(86Kr, X), E=60 MeV/nucleon; measured σ(fragment θ, E); deduced thermalization process saturation features.
doi: 10.1016/0370-2693(93)90221-3
1993SH02 Nucl.Phys. A551, 333 (1993) W.Q.Shen, J.Peter, G.Bizard, R.Brou, D.Cussol, M.Louvel, J.P.Patry, R.Regimbart, J.C.Steckmeyer, J.P.Sullivan, B.Tamain, E.Crema, H.Doubre, K.Hagel, G.M.Jin, A.Peghaire, F.Saint-Laurent, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.MacGrath, S.C.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Components of Collective Flow and Azimuthal Distributions in 40Ar + 27Al and 40Ar + 58Ni Collisions below 85 MeV/u NUCLEAR REACTIONS 27Al, Ni(40Ar, X), E=25-85 MeV/nucleon; measured all charged product σ(φ); deduced transverse, longitudinal collective flow, flow angle, rotation-like behaviour. Multidetectors, event by event analysis, Monte Carlo simulations. Discussed determination of reaction plane.
doi: 10.1016/0375-9474(93)90485-G
1992BI01 Phys.Lett. 276B, 413 (1992) G.Bizard, D.Durand, A.Genoux-Lubain, M.Louvel, R.Bougault, R.Brou, H.Doubre, Y.El-Masri, H.Fugiwara, K.Hagel, A.Hajfani, F.Hanappe, S.Jeong, G.M.Jin, S.Kato, J.L.Laville, C.Le Brun, J.F.Lecolley, S.Lee, T.Matsuse, T.Motobayashi, J.P.Patry, A.Peghaire, J.Peter, N.Prot, R.Regimbart, F.Saint-Laurent, J.C.Steckmeyer, B.Tamain Three Fragment Sequential Decay of Heavy Nuclei Around 3 MeV/u Excitation Energy NUCLEAR REACTIONS 197Au(Ar, X), E=30 MeV/nucleon; calculated fragment yields vs velocity; deduced three fragment production mechanism.
doi: 10.1016/0370-2693(92)91659-W
1990BA43 Nucl.Phys. A518, 767 (1990) R.Barbera, A.Badala, A.Adorno, A.Bonasera, M.Di Toro, A.Palmeri, G.S.Pappalardo, G.Bizard, R.Bougault, D.Durand, A.Genoux-Lubain, J.L.Laville, F.Lefebvres, J.P.Patry, G.M.Jin, E.Rosato Evidence of a Two-Source Emission for Light Charged Particle in Coincidence with Pions Produced in 16O + 27Al Collisions at 94 MeV/Nucleon NUCLEAR REACTIONS 27Al(16O, π+X), (16O, π-X), E=1504 MeV; measured σ(Eπ, θ(X)) vs fragment velocity for light charged particle. Participant-spectator model.
doi: 10.1016/0375-9474(90)90190-W
1990BA53 Nucl.Phys. A519, 231c (1990) R.Barbera, A.Badala, A.Adorno, A.Bonasera, M.Di Toro, A.Palmeri, G.S.Pappalardo, F.Riggi, G.Russo, G.Bizard, D.Durand, J.L.Laville, G.M.Jin, E.Rosato Subthreshold Production of Pions in Coincidence with Light Particles NUCLEAR REACTIONS 27Al(16O, X), E=94 MeV/nucleon; measured (light charged particle)pion-coin, σ(θπ, Eπ); deduced pion emission mechanism.
doi: 10.1016/0375-9474(90)90630-5
1990DU02 Nucl.Phys. A511, 442 (1990) D.Durand, J.L.Laville, G.Bizard, R.Bougault, A.Genoux-Lubain, F.Lefebvres, J.P.Patry, A.Badala, R.Barbera, A.Palmeri, G.S.Pappalardo, A.Schillaci, G.M.Jin, E.Rosato Light Fragment Emission Correlated with Large Transverse Momentum Protons in 94 MeV/u 16O Induced Reactions NUCLEAR REACTIONS 27Al(16O, pX), E=94 MeV/nucleon; measured proton σ(E, θ), light particle multiplicities; deduced source size. Statistical model calculations.
doi: 10.1016/0375-9474(90)90169-M
1990PE04 Phys.Lett. 237B, 187 (1990) J.Peter, J.P.Sullivan, D.Cussol, G.Bizard, R.Brou, M.Louvel, J.P.Patry, R.Regimbart, J.C.Steckmeyer, B.Tamain, E.Crema, H.Doubre, K.Hagel, G.M.Jin, A.Peghaire, F.Saint-Laurent, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.Macgrath, S.C.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Strong Impact Parameter Dependence of Pre-Equilibrium Particle Emission in Nucleus-Nucleus Reactions at Intermediate Energies NUCLEAR REACTIONS 27Al(40Ar, X), E=45, 65 MeV/nucleon; measured fragment production invariant σ.
doi: 10.1016/0370-2693(90)91426-C
1990PE14 Nucl.Phys. A519, 611 (1990) J.Peter, D.Cussol, G.Bizard, R.Brou, M.Louvel, J.P.Patry, R.Regimbart, J.C.Steckmeyer, J.P.Sullivan, B.Tamain, E.Crema, H.Doubre, K.Hagel, G.M.Jin, A.Peghaire, F.Saint-Laurent, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.MacGrath, S.G.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Global Variables and Impact Parameter Determination in Nucleus-Nucleus Collisions Below 100 MeV/u NUCLEAR REACTIONS 27Al(40Ar, X), E=25-85 MeV/nucleon; measured all charged products; deduced global variables, correlations. Event-by-event analysis of impact parameter, multi-detectors.
doi: 10.1016/0375-9474(90)90449-V
1990PE15 Nucl.Phys. A519, 127c (1990) J.Peter, J.P.Sullivan, D.Cussol, G.Bizard, R.Brou, M.Louvel, J.P.Patry, R.Regimbart, J.C.Steckmeyer, B.Tamain, E.Crema, H.Doubre, K.Hagel, G.M.Jin, A.Peghaire, F.Saint-Laurent, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.MacGrath, S.C.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Exclusive Study of Nucleus-Nucleus Reactions at Intermediate Energies: Impact parameter dependence of pre-equilibrium emission, collective flow and hot nuclei formation NUCLEAR REACTIONS 27Al(40Ar, X), E=25-85 MeV/nucleon; measured fragment production invariant σ; deduced flow for Z=1, 2 vs beam energy, parallel velocity.
doi: 10.1016/0375-9474(90)90621-R
1990SU22 Phys.Lett. 249B, 8 (1990) J.P.Sullivan, J.Peter, D.Cussol, G.Bizard, R.Brou, M.Louvel, J.P.Patry, R.Regimbart, J.C.Steckmeyer, B.Tamain, E.Crema, H.Doubre, K.Hagel, G.M.Jin, A.Peghaire, F.Saint-Laurent, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.MacGrath, S.C.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Disappearance of Flow as a Function of Impact Parameter and Energy in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 27Al(Ar, X), E=25-85 MeV/nucleon; measured particle charge velocity; deduced collective nuclear flow dependence on impact parameter, beam energy.
doi: 10.1016/0370-2693(90)90519-C
1989HA31 Phys.Lett. 229B, 20 (1989) K.Hagel, A.Peghaire, G.M.Jin, D.Cussol, H.Doubre, J.Peter, F.Saint-Laurent, G.Bizard, R.Brou, M.Louvel, J.P.Patry, R.Regimbart, J.C.Steckmeyer, B.Tamain, Y.Cassagnou, R.Legrain, C.Lebrun, E.Rosato, R.MacGrath, S.C.Jeong, S.M.Lee, Y.Nagashima, T.Nakagawa, M.Ogihara, J.Kasagi, T.Motobayashi Incomplete Fusion in Nucleus-Nucleus Central Collisions. Study of 40Ar on 27Al from 25 to 85 MeV/u NUCLEAR REACTIONS 27Al(40Ar, X), E=25-85 MeV/nucleon; measured fragment charge, velocity distributions; deduced reaction mechanism.
doi: 10.1016/0370-2693(89)90147-0
1989SA10 Z.Phys. A332, 457 (1989) M.G.Saint-Laurent, R.Anne, D.Bazin, D.Guillemaud-Mueller, U.Jahnke, Jin Gen-Ming, A.C.Mueller, J.F.Bruandet, F.Glasser, S.Kox, E.Liatard, Tsan Ung Chan, G.J.Costa, C.Heitz, Y.El-Masri, F.Hanappe, R.Bimbot, E.Arnold, R.Neugart Total Cross Sections of Reactions Induced by Neutron-Rich Light Nuclei NUCLEAR REACTIONS Cu(X, X), E not given; measured reaction σ for projectile X=4,6He, 6,7,8,9,11Li, 7,9,10,11,12,14Be, 10,11,12,13,14,15,17B, 11,12,13,14,15,16,17,18,19C, 13,14,15,16,17,18,19N, 15,16,17,18,19,20,21O, 18,19,20,21F, 20,21Ne. Secondary beams, 4π γ method.
1988ZH02 Phys.Rev. C37, 669 (1988) Zhang Li, Wang Da-yan, Jin Gen-ming, Zhang Bao-guo, Wang Xi-ming Light Particle Emissions in 12C + 64Ni at E(12C) = 35-70 MeV NUCLEAR REACTIONS, MECPD 64Ni(12C, X), E=35.8-69 MeV; measured σ(fragment E, θ) for X=p, d, t, 3,4He. Galileo-invariant σ contour plots, moving source, coalescence models.
doi: 10.1103/PhysRevC.37.669
1981JI01 Phys.Rev.Lett. 46, 222 (1981) G.-M.Jin, J.D.Garrett, G.Lovhoiden, T.F.Thorsteinsen, J.C.Waddington, J.Rekstad Candidates for Low-Spin Members of the S Band in 160Dy NUCLEAR REACTIONS 161,162Dy(3He, α), E=24 MeV; measured σ(Eα, θ). 160Dy deduced levels, J, π, L, configuration, rotational band structure.
doi: 10.1103/PhysRevLett.46.222
1980JI02 Nucl.Phys. A349, 285 (1980) G.-M.Jin, Y.-X.Xie, Y.-T.Zhu, W.-Q.Shen, X.-J.Sun, J.-S.Guo, G.-X.Liu, J.-S.Yu, C.-C.Sun, J.D.Garrett Product Cross Sections for the Reaction of 12C with 209Bi NUCLEAR REACTIONS, Fission 209Bi(12C, 12C), (12C, X), (12C, F), E=61-73 MeV; measured σ(θ, elastic), σ(θ, evaporation residue), σ(fission), σ(Eα, θ). 221Ac deduced fission barriers.
doi: 10.1016/0375-9474(80)90455-8
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