NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Bansal Found 5 matches. 2013CH34 Phys.Rev. C 88, 014615 (2013) S.Chopra, M.Bansal, M.K.Sharma, R.K.Gupta One-neutron and noncompound-nucleus decay contributions in the 12C + 93Nb reaction at energies near and below the fusion barrier NUCLEAR REACTIONS 93Nb(12C, X)105Ag*, E(cm)=41.1, 47.8, 54.2 MeV; calculated fusion evaporation residue (ER) σ, ER+intermediate mass fragments (IMF) σ, quasi-fission cross sections, l-summed fragment preformation probability. 93Nb(12C, X)105Ag*, E(cm)=40-56 MeV; calculated excitation functions, fusion-fission σ. Dynamical cluster-decay model (DCM) with deformation. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.014615
2012BA10 Rom.J.Phys. 57, 18 (2012) Cold Nuclear Phenomena and Collisions between Two Non-Coplanar Nuclei NUCLEAR REACTIONS 238U(48Ca, X)286Cn, 236U(50Ca, X)286Cn, 232Th(54Ti, X)286Cn, 226Ra(60Cr, X)286Cn, 208Pb(78Zn, X)286Cn, 206Hg(80Ge, X)286Cn, 194Os(92Kr, X)286Cn, 192W(94Sr, X)286Cn, 180Yb(106Mo, X)286Cn, 178Yb(108Mo, X)286Cn, 158Sm(128Sn, X)286Cn, 156Sm(130Sn, X)286Cn, 154Nd(132Te, X)286Cn, 152Nd(132Te, X)286Cn, 244Pu(48Ca, X)292Fl, 242Pu(50Ca, X)292Fl, 238U(54Ti, X)292Fl, 234Pu(58Ti, X)292Fl, 232Th(60Cr, X)292Fl, 222Rn(70Ni, X)292Fl, 220Rn(72Ni, X)292Fl, 210Pb(82Ge, X)292Fl, 208Pb(84Ge, X)292Fl, 206Hg(86Se, X)292Fl, 194Os(98Sr, X)292Fl, 192W(100Zr, X)292Fl, 190W(102Zr, X)292Fl, 184Hf(108Mo, X)292Fl, 164Gd(128Sn, X)292Fl, 162Gd(130Sn, X)292Fl, 160Gd(132Sn, X)292Fl, 158Sm(134Te, X)292Fl, E not given; calculated barriers, quadrupole and octupole deformation parameters, scattering and fragmentation potentials.
2012BA43 Phys.Rev. C 86, 034604 (2012) M.Bansal, S.Chopra, R.K.Gupta, R.Kumar, M.K.Sharma Dynamical cluster-decay model using various formulations of a proximity potential for compact non-coplanar nuclei: Application to the 64Ni + 100Mo reaction NUCLEAR REACTIONS 100Mo(64Ni, X)164Yb(*), E(cm)=119.5-158.8 MeV; calculated 1n to 4n evaporation σ(E) as function of angular momentum, fusion-evaporation and fusion-fission σ(E), fragment potentials for charge-favored fragments, fragment preformation probability, neck length parameter as function of incident energy. Dynamical cluster-decay model (DCM). Comparison with experimental data, and with CASCADE calculations.
doi: 10.1103/PhysRevC.86.034604
2010GU12 Nucl.Phys. A834, 176c (2010) R.K.Gupta, S.K.Arun, R.Kumar, M.Bansal Dynamical cluster-decay model for fusion cross-sections below the barrier NUCLEAR REACTIONS 64Ni(64Ni, xn), E(cm)=85-110 MeV; calculated σ, fusion barriers using DCM (Dynamical Cluster Model) and Wong formula. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.12.032
2009KU18 Phys.Rev. C 80, 034618 (2009) R.Kumar, M.Bansal, S.K.Arun, R.K.Gupta Angular momentum effects and barrier modification in sub-barrier fusion reactions using the proximity potential in the Wong formula NUCLEAR REACTIONS 58Ni(58Ni, X), E(cm)=92-110 MeV; 64Ni(64Ni, X), E(cm)=84-110 MeV; 100Mo(64Ni, X), E(cm)=120-158 MeV; 238U, 244Pu, 248Cm(48Ca, X), E(cm)=180-210 MeV; analyzed σ, interaction potentials, barrier heights and maximum angular momentum using Wong formula.
doi: 10.1103/PhysRevC.80.034618
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