NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = Niyti Found 12 matches. 2022NI05 Physics of Part.and Nuclei 53, 441 (2022) Niyti, A.Deep, R.Kharab, R.Singh, S.Chopra Study of Decay Properties of 260Sg* Nucleus Formed in 52Cr + 208Pb Reaction by Using GSkI Skyrme Force NUCLEAR REACTIONS 208Pb(52Cr, X)260Sg, E=13.3, 18.6 MeV; analyzed available data; deduced σ using the Dynamical Cluster-decay Model (DCM).
doi: 10.1134/S1063779622020642
2020DE33 Phys.Rev. C 102, 034607 (2020) A.Deep, Niyti, R.Kharab, R.Singh, S.Chopra Examining the entrance channel effects on the synthesis of the double deformed nucleus 270Hs: A theoretical study using the dynamical cluster-decay model including Skyrme forces NUCLEAR REACTIONS 26Mg(248Cm, xn)274Hs*,36S(238U, xn)274Hs*,48Ca(226Ra, xn)274Hs*, E*=40-51 MeV; calculated fusion evaporation residue cross sections for 3n-, 4n- and 5n-channels, mass fragmentation potentials, preformation yields, excitation function of individual 3n- to 5n-evaporation channels, best-fitted neck-length parameter using dynamical cluster-decay model (DCM), with Skyrme energy density functionals. Comparison with experimental data. Relevance to super-heavy nuclei.
doi: 10.1103/PhysRevC.102.034607
2019DE31 Int.J.Mod.Phys. E28, 1950079 (2019) A.Deep, Niyti, R.Kharab, R.Singh, S.Chopra Skyrme forces and isotopic dependence of evaporation residue cross-section in the decay of 252, 254-256No* formed in 204, 206, 207, 208Pb 48Ca reactions NUCLEAR REACTIONS 204,206,207,208Pb(48Ca, X)252,254,255,256No, E=20-45 MeV; analyzed available data; calculated preformation yields and probabilities, σ. RADIOACTIVITY 252,254,255,256No(n), (2n), (3n), (4n); analyzed available data; deduced fusion evaporation residue σ for he decay of compound nuclei using the Skyrme energy density functional (SEDF)-based on semi-classical extended Thomas Fermi (ETF) approach under frozen density approximation.
doi: 10.1142/S0218301319500794
2018NI10 Acta Phys.Pol. B49, 639 (2018) Niyti, R.Singh, A.Deep, R.Kharab, S.Chopra, R.K.Gupta Dynamical Cluster-decay Model Based on Skyrme Force KDE0(v1) and the Dynamics of208, 206, 204Pb+48Ca → 256, 254, 252No* Reaction NUCLEAR REACTIONS 204,206,208Pb(48Ca, xn)252,254,256No, E*=19.6-43.6 MeV; calculated channel cross section σxn for fixed x (x=1-4, but most of calculations done for 2n emission) vs E*; compared with available published data; calculated "optimum hot" fusion reactions σ using Dynamical Cluster-decay Model (DCM) with pocket formula for the proximity potential; deduced that they reproduce data well with neck-length parameter fitted.
doi: 10.5506/aphyspolb.49.639
2017NI04 Phys.Rev. C 95, 034602 (2017) Niyti, A.Deep, R.Kharab, S.Chopra, R.K.Gupta Skyrme forces and decay of the266104Rf* nucleus synthesized via different incoming channels NUCLEAR REACTIONS 248Cm(18O, X)266Rf*, E=88.2-101.3 MeV; 244Pu(22Ne, X)266Rf*, E=109.0-124.8 MeV; calculated mass fragmentation potentials, preformation yields. 248Cm(18O, 4n), (18O, 5n), (18O, 6n), 244Pu(22Ne, 4n), 244Pu(22Ne, 5n)244Pu(22Ne, 6n), E=80-130 MeV; calculated σ(E), neck-length parameters, preformation and penetration probabilities. 258Md(8Li, X), 254Es(12B, X), 242Pu(22Ne, X), 218Po(48Ca, X), 212Pb(54Ti, X), 205Au(61Mn, X), 242Pu(22Ne, X), 195Os(71Ni, X), 192W(74Zn, X), 182Yb(84Se, X), 157Nd(109Ru, X), 132Te(134Te, X), E=94.8 MeV; calculated evaporation residue σ for 4n-, 5n-, and 6n-decay channels of compound nucleus 266Rf in the dynamical cluster-decay model (DCM). Skyrme energy density functional (SEDF) based on semiclassical extended Thomas Fermi (ETF) approach, and using SIII, SIV, new GSkI and KDE0(v1) forces.
doi: 10.1103/PhysRevC.95.034602
2015NI04 Nucl.Phys. A938, 22 (2015) Evaporation residue cross-section in the decay of 254No* formed in 206Pb + 48Ca and its isotopic dependence using other Pb targets within the dynamical cluster-decay model NUCLEAR REACTIONS 206Pb(48Ca, xn), E=212.7-242.5 MeV. 254No* calculated fragment preformation probability, 1n to 4n preformation probability vs angular momentum, channel σ, evaporation σ. 204,206,207,208Pb(48Ca, 2n), E*≈19.8, 23.0, 24.5 MeV; calculated σ; deduced radius variation from the fit to σ data. DCM (dynamic cluster model) with deformation and orientation effects included.
doi: 10.1016/j.nuclphysa.2015.02.009
2015NI07 Phys.Rev. C 91, 054606 (2015) Niyti, G.Sawhney, M.K.Sharma, R.K.Gupta α-decay chains of recoiled superheavy nuclei: A theoretical study RADIOACTIVITY 271Sg, 270,271,272,274Bh, 275Hs, 274,275,276,278Mt, 279Ds, 278,279,280,282Rg, 283Cn, 282,283,284,285,286Nh, 286,287Fl, 287,288,289,290Mc, 290,291Lv, 293,294Ts, 294Og(α); calculated half-lives of isotopes, Z=113-118 formed in hot fusion heavy-ion reactions 237Np, 243Am, 244Pu, 245Cm, 249Bk, 249Cf(48Ca, xn). Extension of the quantum-mechanical fragmentation theory based on preformed cluster model (PCM) to include temperature dependence. Comparison with experimental values, and with other theoretical calculations. NUCLEAR REACTIONS 249Bk(48Ca, 4n)293Ts*, E not given; calculated mass fragmentation potential, preformation probability as function of fragment mass number. 237Np(48Ca, 3n)282Mc*, E not given; 242Pu(48Ca, 3n)287Fl*, E not given; 243Am(48Ca, 3n)288Mc*, E not given; 243Am(48Ca, 4n)287Mc*, E not given; 245Cm(48Ca, 3n)290Lv*, E not given; 249Cf(48Ca, 3n)294Og*, E not given; 249Bk(48Ca, 3n)294Ts*, E not given; 249Bk(48Ca, 4n)293Ts*, E not given; calculated best-fit neck-length parameter, preformation probability, penetrability as function of mass number of α-decay chains. Extension of the quantum-mechanical fragmentation theory based on preformed cluster model (PCM) to include temperature dependence.
doi: 10.1103/PhysRevC.91.054606
2014NI03 Phys.Rev. C 89, 014603 (2014) Synthesis of the doubly magic deformed nucleus 270108Hs162 in the decay of 274Hs formed via hot fusion reactions: Entrance-channel effects and role of magicity of 48Ca and 270Hs NUCLEAR REACTIONS 248Cm(26Mg, X)274Hs*, 238U(36S, X)274Hs*, 226Ra(48Ca, X)274Hs*; calculated A=6-268 mass fragmentation potentials, preformation yields, scattering potentials for cold fusion, neck-length parameter. Entrance channel effects. Cold and hot fusion. Hot compact and cold elongated configurations. 269,270,271Hs; calculated σ(E) for 3n, 4n and 5n evaporation channels from 274Hs compound nucleus, and comparison with experimental data. Quantum mechanical fragmentation theory (QMFT) for possible target-projectile combinations. Dynamical cluster-decay model (DCM) with quadrupole deformations for decay of compound nucleus.
doi: 10.1103/PhysRevC.89.014603
2010NI16 J.Phys.(London) G37, 115103 (2010) Establishing the island of stability for superheavy nuclei via the dynamical cluster-decay model applied to a hot fusion reaction 48Ca + 238U → 286112* NUCLEAR REACTIONS 238U(48Ca, X)286Cn, E(cm)=200.6 MeV; calculated scattering potentials, preformation probability for compound system, neck-length parameter, fusion ER σ. Dynamical cluster model (DCM).
doi: 10.1088/0954-3899/37/11/115103
2009GU06 Int.J.Mod.Phys. E18, 601 (2009) R.K.Gupta, Niyti, M.Manhas, S.Hofmann, W.Greiner Role of static deformation and compact orientation of target nucleus in measured fusion, fusion-fission and capture cross-sections of 244Pu + 48Ca reaction NUCLEAR REACTIONS 244Pu(48Ca, X), E≈ 31-53 MeV; calculated the fusion evaporation, fusion-fusion and quasi-fission excitation functions, neutron evaporation σ. Dynamical cluster decay model.
doi: 10.1142/S0218301309012744
2009GU25 J.Phys.(London) G36, 115105 (2009) R.K.Gupta, Niyti, M.Manhas, W.Greiner Island of stability for superheavy elements and the dynamical cluster-decay model for fusion evaporation residue cross sections: 48Ca+238U → 286112* as an example NUCLEAR REACTIONS 238U(48Ca, X)286Cn, E(cm)=200.6 MeV; calculated fusion evaporation residue σ for 3- and 4-neutron emission; deduced island of stability around Z=126 and N=184.
doi: 10.1088/0954-3899/36/11/115105
2008GU20 Int.J.Mod.Phys. E17, 2244 (2008) R.K.Gupta, S.K.Arun, D.Singh, R.Kumar, Niyti, SK.Patra, P.Arumugam, B.K.Sharma Clusters in light, heavy, super-heavy and super-superheavy nuclei
doi: 10.1142/S0218301308011422
Back to query form |