NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = R.Kharab

Found 34 matches.

Back to query form

2023CH21      Int.J.Mod.Phys. E32, 2350012 (2023)

Chetna, Md.M.Shaikh, P.Singh, R.Kharab

Analysis of elastic scattering angular distributions and fusion excitation functions of reactions induced by ⁹Be on ²⁷Al, ²⁸Si, ¹⁴⁴Sm and ²⁰⁸Pb targets at near barrier energies

NUCLEAR REACTIONS ²⁷Al, ²⁸Si, ¹⁴⁴Sm, ²⁰⁸Pb(⁹Be, ⁹Be), (⁹Be, X), E<20 MeV; analyzed available data; deduced σ, σ(θ) using continuum discretized coupled channels (CDCC) methodology.

doi: 10.1142/S021830132350012X
Citations: PlumX Metrics

2023KU02      Phys.Rev. C 107, 014610 (2023)

N.Kumari, A.Deep, S.Chopra, R.Kharab

Systematic analysis of the decay of ^{287, 288, 290, 292}Fl^* formed in the complete fusion reactions ^{239, 240, 242, 244}Pu + ⁴⁸Ca including Skyrme forces

NUCLEAR REACTIONS ²⁴⁴Pu(⁴⁸Ca, X)²⁹²Fl^*, E=46.9^*; calculated scattering potential for hot fusion at fixed temperature, mass fragmentation potential, preformation yields. ²³⁹Pu(⁴⁸Ca, X)²⁸⁷Fl^*,240Pu(⁴⁸Ca, X)²⁸⁸Fl^*,242Pu(⁴⁸Ca, X)²⁹⁰Fl^*,244Pu(⁴⁸Ca, X)²⁹²Fl^*, E=32.5-52.6 MeV; calculated σ (excitation functions) of 1n, 2n, 3n, 4n, 5n channels from compound nuclei ^{287,288,290,292}Fl^*. Quantum mechanical fragmentation theory (QMFT) based dynamical cluster-decay model (DCM) calculations using SLy4, SkM^* and KDE0(v1) Skyrme interactions. Comparison with available experimental data.

doi: 10.1103/PhysRevC.107.014610
Citations: PlumX Metrics

2022CH14      Nucl.Phys. A1021, 122418 (2022)

Chetna, M.M.Shaikh, P.Singh, R.Kharab

Exploring the effects of breakup couplings for weakly bound projectile ⁹Be on various targets at around barrier energies

NUCLEAR REACTIONS ¹⁴⁴Sm, ¹⁶⁹Tm, ¹⁸¹Ta, ¹⁸⁶W, ¹⁸⁷Re, ¹⁹⁷Au, ²⁰⁸Pb(⁹Be, X), E<54 MeV; analyzed available data; calculated total fusion and complete fusion σ within the framework of the Continuum Discretized Coupled Channel (CDCC) approach.

doi: 10.1016/j.nuclphysa.2022.122418
Citations: PlumX Metrics

2022GO14      Int.J.Mod.Phys. E31, 2250084 (2022)

M.Goyal, R.Kumar, P.Singh, R.K.Seth, R.Kharab

Investigation of simultaneous variation of surface diffuseness and central depression in the estimation of absorption effects

NUCLEAR REACTIONS ¹⁹⁷Au(⁸⁰Kr, X), E not given; analyzed available data; deduced the effect of simultaneous variation of surface diffuseness and central depression, in case of model-dependent Fermi matter density distributions, on the estimation of survival probability, Coulomb excitation σ and absorption effects.

doi: 10.1142/S0218301322500847
Citations: PlumX Metrics

2022KU05      Phys.Rev. C 105, 014628 (2022)

N.Kumari, A.Deep, R.Kharab

Theoretical study of evaporation residue cross sections in the decay of ²⁸⁶Cn^* formed via the ²³⁸U+⁴⁸Ca reaction using Skyrme force

NUCLEAR REACTIONS ²³⁸U(⁴⁸Ca, xn)²⁸⁶Cn^*, E^*=35 MeV; calculated scattering potentials for ²⁸⁶Cn to ²⁸³Cn+3n, mass fragmentation potential for the formation of ²⁸⁶Cn compound nucleus, preformation and penetration probabilities for hot and cold configurations, σ(E) for 1n-, 2n-, 3n- and 4n-evaporation channels, best fitted neck-length parameters, ²⁷⁸Mt(⁸Li, xn)²⁸⁶Cn^*,272Sg(¹⁴C, xn)²⁸⁶Cn^*,264Lr(²²F, xn)²⁸⁶Cn^*,248Cm(³⁸S, xn)²⁸⁶Cn^*,238U(⁴⁸Ca, xn)²⁸⁶Cn^*,218Po(⁶⁸Ni, xn)²⁸⁶Cn^*,202Pt(⁸⁴Se, xn)²⁸⁶Cn^*,195Os(⁹¹Kr, xn)²⁸⁶Cn^*,178Er(¹⁰⁸Ru, xn)²⁸⁶Cn^*,152Nd(¹³⁴Te, xn)²⁸⁶Cn^*,148Ce(¹³⁸Xe, xn)²⁸⁶Cn^*, E^*=35 MeV; calculated scattering potentials for "hot fusion" reaction valleys with "hot-compact" configurations, σ for 3n- and 4n-evaporation channels. Quantum mechanical fragmentation theory (QMFT) based dynamical cluster-decay model (DCM) calculations using GSkI and KDE0(v1) Skyrme interactions, and SIII interaction. Comparison with available experimental data.

doi: 10.1103/PhysRevC.105.014628
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2021CH43      Int.J.Mod.Phys. E30, 2150058 (2021)

Chetna, M.M.Shaikh, P.Singh, R.Kharab

Study of breakup induced fusion mechanisms for ⁹Be + ¹⁸¹Ta system at around barrier energies

NUCLEAR REACTIONS ¹⁸¹Ta(⁹Be, X), E<52 MeV; calculated total, complete and incomplete fusion σ by employing the code FRESCO based on continuum discretized coupled channel (CDCC) method. Comparison with available data.

doi: 10.1142/S0218301321500580
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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, 254-256}No^* formed in ^{204, 206, 207, 208}Pb ⁴⁸Ca reactions

NUCLEAR REACTIONS ^{204,206,207,208}Pb(⁴⁸Ca, X)^{252,254,255,256}No, E=20-45 MeV; analyzed available data; calculated preformation yields and probabilities, σ.

RADIOACTIVITY ^{252,254,255,256}No(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
Citations: PlumX Metrics

2019GO31      Nucl.Phys. A992, 121620 (2019)

M.Goyal, R.Kumar, P.Singh, R.K.Seth, R.Kharab

Effect of nuclear surface diffuseness on Coulomb excitation and total nuclear reaction cross sections

NUCLEAR REACTIONS ¹⁹⁷Au(⁸⁰Kr, x), E not given; calculated Coulomb excitation σ, σ of other processes, two-parameter Fermi type matter density distribution for ⁸⁰Kr, survival probability, Coulomb excitation σ, absorptioneffects for various values of b_min; deduced effect of nuclear diffuseness on Coulex and total σ.

doi: 10.1016/j.nuclphysa.2019.121620
Citations: PlumX Metrics

2019KH01      Nucl.Phys. A981, 62 (2019)

R.Kharab, A.Kumari

Influence of projectile breakup on fusion reactions induced by ⁹Be at near barrier energies

NUCLEAR REACTIONS ¹²⁴Sn, ¹⁴⁴Sm, ¹⁶⁹Tm, ¹⁸¹Ta, ¹⁸⁶W, ¹⁸⁷Re, ²⁰⁸Pb, ²⁰⁹Bi(⁹Be, x), E≈Coulomb barrier; calculated barrier, total and Complete fusion σ; compared with data; deduced σ best-fit curve, parameters. ²⁰⁸Pb(¹²C, x), E(cm)=56-90 MeV; calculated fusion σ. Quantum diffusion model by Sargsyan et al.

doi: 10.1016/j.nuclphysa.2018.10.081
Citations: PlumX Metrics

2019RA21      Nucl.Phys. A990, 149 (2019)

N.Rani, P.Singh, M.Singh, R.Kumar, R.Kumar, R.Kharab

Influence of coupling of excited states and of deuteron transfer on fusion reactions induced by ^{6, 7}Li on ⁶⁴Ni, ¹⁵²Sm and ²⁰⁹Bi targets

doi: 10.1016/j.nuclphysa.2019.07.007
Citations: PlumX Metrics

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 of^{208, 206, 204}Pb+⁴⁸Ca → ^{256, 254, 252}No^* Reaction

NUCLEAR REACTIONS ^204,206,208Pb(⁴⁸Ca, xn)^252,254,256No, E^*=19.6-43.6 MeV; calculated channel cross section σ_xn 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
Citations: PlumX Metrics

2017KH02      Nucl.Phys. A960, 11 (2017)

R.Kharab, R.Chahal, R.Kumar

Role of tunnelling in complete and incomplete fusion induced by ⁹Be on ¹⁶⁹Tm and ¹⁸⁷Re targets at around barrier energies

NUCLEAR REACTIONS ¹⁶⁹Tm, ¹⁸⁷Re(⁹Be, x), E(cm)=30-47 MeV; calculated complete fusion σ, incomplete fusion σ, total σ using PLATYPUS code (classical dynamical model) with tunelling correction. Compared with data.

doi: 10.1016/j.nuclphysa.2017.01.006
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2016KH03      Nucl.Phys. A946, 1 (2016)

R.Kharab, R.Chahal, R.Kumar

Investigation of contribution of incomplete fusion in the total fusion process induced by ⁹Be on ¹⁸¹Ta target at near barrier energies

doi: 10.1016/j.nuclphysa.2015.11.005
Citations: PlumX Metrics

2016KU03      Eur.Phys.J. A 52, 25 (2016)

R.Kumar, S.Sharma, P.Singh, R.Kharab

Determination of minimum impact parameter by modified touching spheres schemes for intermediate energy Coulomb excitation experiments

NUCLEAR REACTIONS ¹⁹⁷Au(²⁶Ne, x), (⁶⁸Fe, x), (¹⁰²Cd, x), (¹⁹⁷Au, x), E=30-500 MeV/nucleon; calculated minimum impact factor with inclusion of energy-dependent term.

doi: 10.1140/epja/i2016-16025-2
Citations: PlumX Metrics

2015KU01      Nucl.Phys. A933, 93 (2015)

A.Kumari, R.Kharab

Interplay of deformation and two neutrons transfer effects in ⁶He induced fusion reactions around barrier energies

NUCLEAR REACTIONS ^64,68Zn(⁶He, x), E(cm)=5-17 MeV;²⁰⁶Pb(⁶He, x), E(cm)=12-24 MeV;²⁰⁹Bi(⁶He, x), E(cm)=18-30 MeV;²³⁸U(⁶He, x), E(cm)=12-34 MeV; calculated fusion σ using quantum diffusion approach with and without neutron transfer. Compared with available data.

doi: 10.1016/j.nuclphysa.2014.09.112
Citations: PlumX Metrics

2015KU20      Nucl.Phys. A941, 38 (2015)

A.Kumari, R.Kharab

Role of projectile breakup in ⁶He and ⁶Li induced fusion reactions around barrier energies

NUCLEAR REACTIONS ⁶⁴Zn, ²⁰⁹Bi(⁶He, x), (⁶Li, x), E(cm)=5-50 MeV; calculated projectile breakup probability, fusion σ using quantum diffusion approach with account for deformation and different orientation of nuclei. Excitation function compared with data.

doi: 10.1016/j.nuclphysa.2015.05.007
Citations: PlumX Metrics

2015KU23      Europhys.Lett. 111, 32001 (2015)

R.Kumar, P.Singh, R.Kharab

Optimum forward scattering zone for intermediate-energy Coulomb excitation experiments

NUCLEAR REACTIONS ¹⁹⁷Au(¹¹Be, ¹¹Be'), (²⁶Ne, ²⁶Ne'), (³²Mg, ³²Mg'), (³⁸Si, ³⁸Si'), (⁴⁴S, ⁴⁴S'), (⁵⁶Ti, ⁵⁶Ti'), (⁷⁸Kr, ⁷⁸Kr'), (⁹⁶Mo, ⁹⁶Mo'), (¹¹⁰Sn, ¹¹⁰Sn'), (¹⁹⁷Au, ¹⁹⁷Au'), ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb'), E=30-1000 MeV/nucleon; calculated parameters for various projectile-target systems at incident beam energies. Comparison with available data.

doi: 10.1209/0295-5075/111/32001
Citations: PlumX Metrics

2015SI17      Phys.Atomic Nuclei 78, 720 (2015)

M.Singh, R.Kharab, R.M.Singh

Effects of first-order correction to eikonal approximation in the analysis of ⁹Be(¹⁵C, ¹⁴C + n)⁹Be stripping reaction

NUCLEAR REACTIONS ⁹Be(¹⁵C, n¹⁴C), E=54 MeV/nucleon; calculated eikonal phases, longitudinal momentum distribution of ¹⁴C. Comparison with available data.

doi: 10.1134/S1063778815050142
Citations: PlumX Metrics

2013SI01      Nucl.Phys. A897, 179 (2013)

M.Singh, Sukhvinder, R.Kharab

Analysis of fusion excitation functions of various systems using modified Woods-Saxon potential

NUCLEAR REACTIONS ^46,48,50Ti(⁴⁰Ca, X), E(cm)=53-85 MeV;⁶⁰Ni(⁵⁰Ti, X), E(cm)=72-95 MeV;⁶⁴Ni(⁴⁶Ti, X), E(cm)=72-95 MeV;⁹⁰Zr(⁴⁰Ca, X), E(cm)=93-112 MeV;(⁴⁸Ca, X), E(cm)=91-113 MeV;(⁴⁶Ti, X), E(cm)=100-120 MeV;(⁵⁰Ti, X), E(cm)=100-120 MeV;¹⁵⁴Sm(¹⁶O, X), E(cm)=52-100 MeV;calculated fusion σ using CC code CCFULL; deduced parameters of Woods-Saxon nuclear potential using published data on these reactions.

doi: 10.1016/j.nuclphysa.2012.11.007
Citations: PlumX Metrics

2013SI02      Nucl.Phys. A897, 198 (2013)

M.Singh, Sukhvinder, R.Kharab

Analysis of fusion excitation function data by using an energy dependent potential model

NUCLEAR REACTIONS ⁵⁴Fe(⁵⁸Ni, X), E(cm)=65-105 MeV;⁷⁰Ge(¹⁶O, X), E(cm)=30-55 MeV;⁷⁰Ge(²⁷Al, X), E(cm)=50-60 MeV;⁷⁰Ge(³⁷Cl, X), E(cm)=62-77 MeV;⁷²Ge(¹⁶O, X), E(cm)=30-53 MeV;⁷²Ge(²⁷Al, X), E(cm)=50-60 MeV;⁷²Ge(³⁷Cl, X), E(cm)=62-77 MeV;⁷⁴Ge(¹⁶O, X), E(cm)=30-60 MeV;⁷⁴Ge(²⁷Al, X), E(cm)=48-63 MeV;⁷⁴Ge(³⁷Cl, X)E(cm)=63-75 MeV;⁷⁶Ge(¹⁶O, X), E(cm)=30-60 MeV;⁷⁶Ge(²⁷Al, X), E(cm)=48-63 MeV;⁷⁶Ge(³⁷Cl, X), E(cm)=63-77 MeV;⁹⁰Zr(⁴⁰Ca, X), E not given;⁹⁰Zr(⁴⁸Ca, X), E(cm)=90-115 MeV;⁹²Zr(¹⁶O, X), E(cm)=35-70 MeV;⁹²Zr(²⁸Si, X), E(cm)=65-90 MeV;⁹⁶Zr(⁴⁸Ca, X), E(cm)=85-115 MeV;¹⁸⁶W(¹⁶O, X), E(cm)=60-95 MeV;^144,148Sm(¹⁶O, X), E(cm)=55-95 MeV;²⁰⁸Pb(¹⁶O, X), E(cm)=70-115 MeV;calculated fusion σ using Wong's formula and energy dependent potential; deduced potential parameters.

doi: 10.1016/j.nuclphysa.2012.11.002
Citations: PlumX Metrics

2012DU13      Int.J.Mod.Phys. E21, 1250054 (2012)

S.S.Duhan, M.Singh, R.Kharab

Effects of nuclear induced breakup on the fusion of ⁶Li + ¹²C and ⁶He + ¹²C systems around barrier energies

NUCLEAR REACTIONS ¹²C(⁶Li, X), (⁶He, X), E not given; calculated fusion σ. Dynamic polarization potential approach.

doi: 10.1142/S0218301312500541
Citations: PlumX Metrics

2011DU05      Phys.Atomic Nuclei 74, 49 (2011)

S.S.Duhan, M.Singh, R.Kharab, H.C.Sharma

Dynamic polarization potentials for ⁶He + ²⁰⁹Bi and ¹¹Li + ²⁰⁸Pb systems at near-barrier energies

NUCLEAR REACTIONS ²⁰⁹Bi(⁶He, X), ²⁰⁸Pb(¹¹Li, X), E(cm)<100 MeV; calculated internuclear separation, dynamic polarization potential, breakup transmission factors.

doi: 10.1134/S1063778811010066
Citations: PlumX Metrics

2011KU06      Nucl.Phys. A849, 182 (2011)

R.Kumar, R.Kharab, H.C.Sharma

Parameterization scheme for determining the reaction cross sections at intermediate beam energies for normal and exotic nuclei

NUCLEAR REACTIONS ¹²C(¹²C, X), E=20-1000 MeV/nucleon; ²⁸Si, ⁴⁰Ca, ^58,60Ni, ^{112,116,118,120,124}Sn, ²⁰⁸Pb(³He, X), E=32.1, 45.9 MeV/nucleon; ²⁸Si, ⁴⁰Ca, ^58,60Ni, ^{112,116,118,120,124}Sn, ²⁰⁸Pb(α, X), E=41, 48.1 MeV/nucleon; ¹²C(¹²C, X), (¹³C, X), (¹⁴C, X), (¹⁵C, X), (¹⁶C, X), E=20-40, 700-965 MeV/nucleon; ¹²C(¹⁷C, X), (¹⁸C, X), (¹⁹C, X), E=700-965 MeV/nucleon; ¹²C(¹³C, X), (¹⁴C, X), (¹⁵N, X), (¹⁶N, X), (¹⁷O, X), (¹⁸O, X), (¹⁹F, X), (²⁰F, X), (²¹Ne, X), (²²Ne, X), (²³Na, X), (²⁴Na, X), (²⁵Mg, X), (²⁶Mg, X), (²⁷Si, X), (²⁸Si, X), (²⁹S, X), E=30 MeV/nucleon; ¹²C(²³Al, X), (²⁴Al, X), (²⁵Al, X), (²⁶Al, X), (²⁷Al, X), (²⁸Al, X), (¹⁹F, X), (²⁰Ne, X), (²¹Na, X), (²²Mg, X), E=30 MeV/nucleon; ²⁸Si(¹²N, X), E=29.3 MeV/nucleon; ²⁸Si(¹²B, X), E=25.6 MeV/nucleon; ¹²C(¹⁷B, X), E=77 MeV/nucleon; calculated total σ. Comparison with other models and data.

doi: 10.1016/j.nuclphysa.2010.10.010
Citations: PlumX Metrics

2010KU06      Chin.Phys.Lett. 27, 032502 (2010)

R.Kumar, R.Kharab, H.C.Sharma

Intermediate Energy Coulomb Excitation of Neutron-Rich Nuclei

NUCLEAR STRUCTURE ^38,40,42S, ^44,46Ar; calculated B(E2) values suppression.

doi: 10.1088/0256-307X/27/3/032502
Citations: PlumX Metrics

2010KU08      Phys.Rev. C 81, 037602 (2010)

R.Kumar, R.Kharab, H.C.Sharma

Parametrization scheme for determining a safe lower limit of the impact parameter for Coulomb excitation experiments

NUCLEAR REACTIONS Au(²⁶Ne, ²⁶Ne'), Au(³²Mg, ³²Mg'), Au(³²Si, ³²Si'), Au(⁴²S, ⁴²S'), Au(⁴⁶Ar, ⁴⁶Ar'), Au(⁵²Fe, ⁵²Fe'), Au(⁷⁸Kr, ⁷⁸Kr'), E at Coulomb barrier; calculated σ; parametrization of scattering angle and impact parameter. Hartree-Fock-Bogoliubov (HFB) method. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.037602
Citations: PlumX Metrics

2009KU07      Phys.Atomic Nuclei 72, 969 (2009)

R.Kumar, R.Kharab, H.C.Sharma

The B(E1) strength of ¹¹Be extracted from the Coulomb excitation measurements

NUCLEAR REACTIONS Pb(¹¹Be, ¹¹Be'), E=43 MeV/nucleon; analyzed Coulomb excitation data, extracted B(E1).

doi: 10.1134/S106377880906009X
Citations: PlumX Metrics

2008KH04      Int.J.Mod.Phys. E17, 693 (2008)

R.Kharab, P.Singh, R.Kumar, H.C.Sharma

Contribution of E2 and E1-E2 interference in the Coulomb breakup of ¹¹Be

NUCLEAR REACTIONS ²³⁸U(¹¹Be, n¹⁰Be), E=63 MeV/nucleon; ²³⁸U(¹¹Be, n¹⁰Be), E=72 MeV/nucleon; analyzed ¹⁰Be longitudinal momentum distributions from Coulomb dissociation including the effect of higher order multipole transitions.

doi: 10.1142/S0218301308010088
Citations: PlumX Metrics

2008SI07      Nucl.Phys. A802, 82 (2008)

P.Singh, R.Kumar, R.Kharab, H.C.Sharma

Structural analysis of ¹⁹C through Coulomb dissociation reactions

NUCLEAR REACTIONS ¹⁸¹Ta, ²⁰⁸Pb(¹⁹C, n¹⁸C), E=67-88 MeV/nucleon; calculated σ, relative energy spectra and momentum distribution for Coulomb breakup using eikonal approximation; deduced configuration. Comparison with data.

doi: 10.1016/j.nuclphysa.2008.01.020
Citations: PlumX Metrics

2008SI27      Phys.Atomic Nuclei 71, 1932 (2008)

P.Singh, R.Kumar, R.Kharab

Coulomb breakup of neutron-rich isotopes of light nuclei

NUCLEAR REACTIONS Pb(¹¹Be, n¹⁰Be), E=72 MeV/nucleon; Pb(¹⁴B, n¹³B), E=86 MeV/nucleon; Pb(¹⁵C, n¹⁴C), E=550 MeV/nucleon; Pb(¹⁹C, n¹⁸C), E=77 MeV/nucleon; calculated coulomb dissociation cross sections.

doi: 10.1134/S1063778808110100
Citations: PlumX Metrics

2007KH03      Chin.Phys.Lett. 24, 656 (2007)

R.Kharab, P.Singh, R.Kumar

Effects of E2 and E1-E2 Interference on Coulomb Dissociation of ¹⁹C

NUCLEAR REACTIONS Ta, Pb(¹⁹C, X), E=67, 77, 88 MeV/nucleon; calculated Coulomb breakup σ, multipole contributions, interference effects.

doi: 10.1088/0256-307X/24/3/019
Citations: PlumX Metrics

2007KH08      Pramana 68, 779 (2007)

R.Kharab, R.Kumar, P.Singh, H.C.Sharma

One-neutron stripping reactions of ¹¹Be and ¹⁹C on light target

NUCLEAR REACTIONS ⁹Be(¹¹Be, X), E=63 MeV/nucleon; ⁹Be(¹⁹C, X), E=88 MeV/nucleon; calculated one-neutron absorption cross section and longitudinal momentum distribution of the core fragment within the framework of eikonal approximation.

doi: 10.1007/s12043-007-0077-6
Citations: PlumX Metrics