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NSR database version of April 27, 2024.

Search: Author = M.Bansal

Found 5 matches.

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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
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2012BA10      Rom.J.Phys. 57, 18 (2012)

M.Bansal, R.K.Gupta

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
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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
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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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