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NSR database version of April 11, 2024.

Search: Author = M.Kaur

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2023KA25      Phys.Rev. C 108, 034611 (2023)

R.Kaur, B.B.Singh, M.Kaur, M.K.Sharma, P.P.Singh

Investigating 6, 7Li-induced reactions on 235, 238U through a collective clusterization approach

doi: 10.1103/PhysRevC.108.034611
Citations: PlumX Metrics

2022KA25      Phys.Rev. C 106, 024604 (2022)

R.Kaur, M.Kaur, S.Pal

Statistical model calculation of the compound nuclear fission timescale in fusion-fission reactions

NUCLEAR REACTIONS 194Pt(12C, X)206Po, 198Pt(12C, X)210Po, 194Pt(16O, X)210Rn, 194Pt(18O, X)212Rn, 204Pb(12C, X)216Ra, 197Au(19F, X)216Ra, E*=42-80 MeV; calculated fission σ(E), evaporation residue σ(E), prescission neutron multiplicities, fission-to-neutron decay width ratios, excitation energy dependence of the average saddle time, saddle-time distributions, multichance fission probabilities. Statistical model calculations. Comparison to experimental data

doi: 10.1103/PhysRevC.106.024604
Citations: PlumX Metrics

2021KA02      At.Data Nucl.Data Tables 137, 101381 (2021)

M.Kaur, D.Furekh Dar, B.K.Sahoo, B.Arora

Radiative transition properties of singly charged magnesium, calcium, strontium and barium ions

ATOMIC PHYSICS Mg, Ca, Sr, Ba; calculated electric dipole (E1) amplitudes along with their uncertainties using a relativistic all-order many-body method.

doi: 10.1016/j.adt.2020.101381
Citations: PlumX Metrics

2021KA24      Phys.Rev. C 103, 054608 (2021)

M.Kaur, B.B.Singh, S.K.Patra

Role of microscopic temperature-dependent binding energies in the decay of 32Si* formed in the 20O + 12C reaction

NUCLEAR REACTIONS 12C(20O, X)32Si*, E(cm)=7.35, 9.29 MeV; calculated fragmentation potential, mass dependence of fragmentation potential, macroscopic and microscopic binding energies for some isobars of A=10, 14, 18, 22, 26 and 30 at T=0 and 3.09 MeV, preformation probability potentials for the emission of 3H, 4He and 5He, fusion cross-sections for light-charged particles. Relativistic mean-field (RMF) calculations using quantum mechanical fragmentation-based dynamical cluster-decay model (DCM), and Davidson mass formula.

doi: 10.1103/PhysRevC.103.054608
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2021KA25      At.Data Nucl.Data Tables 140, 101422 (2021)

M.Kaur, S.Singh, B.K.Sahoo, B.Arora

Tune-out and magic wavelengths, and electric quadrupole transition properties of the singly charged alkaline-earth metal ions

ATOMIC PHYSICS Mg, Ca, Sr, Ba; analyzed available data; deduced magic wavelengths, the electric quadrupole (E2) matrix elements of a large number of forbidden transitions using an all-order relativistic many-body method and compare them with the previously reported values for a few selective transitions.

doi: 10.1016/j.adt.2021.101422
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2021KU07      Phys.Rev. C 103, 024305 (2021)

A.Kumar, H.C.Das, M.Kaur, M.Bhuyan, S.K.Patra

Application of the coherent density fluctuation model to study the nuclear matter properties of finite nuclei within the relativistic mean-field formalism

NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 116Sn, 208Pb; proton and neutron surface diffusion parameters, nuclear incompressibilities, symmetric energies, neutron pressure, slope and curvature parameters, density distributions of 16O and 208Pb. Coherent density fluctuation model (CDFM) for nuclear matter (NM) properties of finite nuclei within the effective relativistic mean-field (E-RMF) formalism with NL3 and G3 parameter sets. Comparison with calculations using Bruckner energy density functional within CDFM, and discussed resolution of Coster-Band problem.

doi: 10.1103/PhysRevC.103.024305
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2021SI22      J.Phys.(London) G48, 075104 (2021)

V.Singh, B.R.Behera, M.Kaur, A.Jhingan, R.Kaur, P.Sugathan, D.Siwal, S.Goyal, K.P.Singh, S.Pal, A.Saxena, S.Kailas

Measurement of fission excitation function for 19F + 194, 196, 198Pt reactions

NUCLEAR REACTIONS 194,196,198Pt(19F, F), E=90.5-118.7 MeV; measured reaction products. 213,215,217Fr; deduced fragment yields, σ, pre-scission neutron multiplicity. Comparison with statistical model calculations.

doi: 10.1088/1361-6471/abe8cd
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6408.

2020KA26      Phys.Rev. C 101, 044605 (2020)

R.Kaur, M.Kaur, V.Singh, M.Kaur, B.B.Singh, B.S.Sandhu

Dynamical aspects od 48Ti + 58Fe, 58Ni → 106Cd*, 106Sn reactions at energies near the Coulomb barrier

NUCLEAR REACTIONS 58Fe(48Ti, X)106Cd*,58Ni(48Ti, X)106Sn*, E=118.06-165.8 MeV; calculated fragmentation and scattering potentials, barrier lowering and neck-length parameters, preformation probabilities, σ(E) as function of light and heavy fragments of the compound nuclei. Dynamical cluster decay model (DCM).

doi: 10.1103/PhysRevC.101.044605
Citations: PlumX Metrics

2020KA28      Nucl.Phys. A1000, 121871 (2020)

M.Kaur, A.Quddus, A.Kumar, M.Bhuyan, S.K.Patra

Effect of temperature on the volume and surface contributions in the symmetry energy of rare earth nuclei

doi: 10.1016/j.nuclphysa.2020.121871
Citations: PlumX Metrics

2020KA50      J.Phys.(London) G47, 105102 (2020)

M.Kaur, A.Quddus, A.Kumar, M.Bhuyan, S.K.Patra

On the symmetry energy and deformed magic number at N = 100 in rare earth nuclei

NUCLEAR STRUCTURE 160Nd, 162Sm, 164Gd, 166Dy; calculated ground state neutron single particle spectra, variation of nuclear symmetry energy within the coherent density fluctuation model with relativistic mean densities with NL3 and IOPB-I parameter sets.

doi: 10.1088/1361-6471/ab92e4
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2020SI20      Phys.Rev. C 102, 034321 (2020)

S.Sihotra, D.Kumar, M.Kaur, V.Singh, S.Saha, J.Sethi, R.Palit, N.Singh, D.Mehta

Evidence of antimagnetic rotation in 100Pd

NUCLEAR REACTIONS 75As(31P, 2nα)100Pd, E=125 MeV; measured Eγ, Iγ, γγ-coin, level half-lives by DSAM using the INGA array at the Pelletron-LINAC facility of TIFR-Mumbai. 100Pd; deduced high-spin levels, J, π, B(E2), moment of inertia plots, anti-magnetic rotation (AMR) structure, configuration. Comparison with predictions of semiclassical particle-rotor model calculations.

doi: 10.1103/PhysRevC.102.034321
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2019KA05      Phys.Rev. C 99, 014614 (2019)

M.Kaur, B.B.Singh, S.Kaur, R.K.Gupta

N/Z dependence of decay channels in A=80 compound nuclei

NUCLEAR REACTIONS 40Ca(40Ca, X)80Zr*, E(cm)=62.14 MeV; 64Zn(16O, X)80Sr*, E(cm)=48.0 MeV; 48Ca(32S, X)80Kr*, E(cm)=39.8 MeV; calculated radial scattering potential profiles, fragmentation potential, preformation and penetration probability probabilities as function of fragment mass and angular momentum, fusion σ for emission of light particles, intermediate mass fragments, and symmetric mass fragments. Dynamical cluster-decay model. Comparison with experimental values of fusion σ.

doi: 10.1103/PhysRevC.99.014614
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2019KU03      Acta Phys.Pol. B50, 159 (2019)

S.Kumar, S.Sihotra, V.Singh, J.Rather, M.Kaur, J.Goswamy, N.Singh, D.Mehta, T.Trivedi, R.P.Singh, S.Muralithar, R.Palit

Shell-model Description in 99Rh and Systematics of Odd-A Rh Isotopes

NUCLEAR STRUCTURE 99Rh; calculated energy levels, J, π, bands. Comparison with experimental data and systematics.

doi: 10.5506/APhysPolB.50.159
Citations: PlumX Metrics

2019NA32      Int.J.Mod.Phys. E28, 1950100 (2019)

K.C.Naik, M.Kaur, A.Kumar, S.K.Patra

Density dependence of symmetry energy in deformed 162Sm nucleus

NUCLEAR STRUCTURE 162Sm; calculated axially deformed density, symmetry energy values.

doi: 10.1142/S0218301319501003
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2018KA02      Nucl.Phys. A969, 14 (2018)

M.Kaur, B.B.Singh, M.K.Sharma, R.K.Gupta

Analysis of intermediate and light mass fragments from composite systems 26-29Al* formed in 16, 18O + 10, 11B reactions

NUCLEAR REACTIONS 10,11B(16O, x), (18O, x), E=1-4 MeV/nucleon; calculated fragmentation potential for the composite system, fragment mass distribution, fragment preformation probability using DCM (Dynamical Cluster decay Model) for both spherical and deformed nucleus. Light particle emission σ compared to data.

doi: 10.1016/j.nuclphysa.2017.09.014
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2018KA43      Nucl.Phys. A980, 67 (2018)

M.Kaur, B.B.Singh, M.K.Sharma, R.K.Gupta

Study of α-induced reactions forming A=60 compound systems within dynamical cluster-decay model

doi: 10.1016/j.nuclphysa.2018.09.079
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2018KA53      Phys.Rev. C 98, 064612 (2018)

R.Kaur, M.Kaur, V.Singh, S.Kaur, B.B.Singh, B.S.Sandhu

Investigating the fusion enhancement for neutron-rich mid-mass nuclei using the dynamical cluster-decay model

NUCLEAR REACTIONS 28Si(39K, X)67As*,28Si(40K, X)68As*,28Si(41K, X)69As*,28Si(45K, X)73As*,28Si(46K, X)74As*,28Si(47K, X)75As*, E(cm)=36.8-42.6 MeV; calculated fragment potentials and l-summed preformation probability as a function of fragment mass number, scattering potentials for the compound nuclei decaying through one-proton and one-neutron channels, barrier lowering as function of incident energy, summed penetration probabilities, fusion σ(E), -summed fragment cross sections using dynamical cluster-decay model (DCM). Comparison with available experimental data.

doi: 10.1103/PhysRevC.98.064612
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2018MO05      Phys.Rev. C 97, 024610 (2018)

G.Montagnoli, A.M.Stefanini, C.L.Jiang, K.Hagino, F.Galtarossa, G.Colucci, S.Bottoni, C.Broggini, A.Caciolli, P.Colovic, L.Corradi, S.Courtin, R.Depalo, E.Fioretto, G.Fruet, A.Gal, A.Goasduff, M.Heine, S.P.Hu, M.Kaur, T.Mijatovic, M.Mazzocco, D.Montanari, F.Scarlassara, E.Strano, S.Szilner, G.X.Zhang

Fusion hindrance for the positive Q-value system 12C+30Si

NUCLEAR REACTIONS 12C(30Si, X), E=34-80 MeV; measured reaction products, fusion σ(E) at the XTU Tandem accelerator of INFN-LN, Legnaro. Comparison with coupled-channel calculations using Woods Saxon (WS) and Yukawa-plus-exponential (YPE) potentials.

doi: 10.1103/PhysRevC.97.024610
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0899.

2017KA05      Phys.Rev. C 95, 014611 (2017)

M.Kaur, B.B.Singh, S.K.Patra, R.K.Gupta

Clustering effects and decay analysis of the light-mass N=Z and N ≠ Z composite systems formed in heavy ion collisions

NUCLEAR REACTIONS 10B(10B, X)20Ne*, E(cm)=12-25 MeV; 16O(12C, X)28Si*, E(cm)=50.14-68.57 MeV; 28Si(12C, X)40Ca*, E(cm)=53.90 MeV; 10B(11B, X)21Ne*, E(cm)=13.09-26.19 MeV; 11B(11B, X)22Ne*, E(cm)=12-25 MeV; 11B(28Si, X)39K*, E(cm)=45.94 MeV; 12C(27Al, X)39K*, E(cm)=50.53 MeV; calculated preformation and penetration probabilities as function of fragment or cluster mass, scattering and fragment potentials for the decay of α- and non-α conjugate systems, fission-fusion σ(E). Dynamical cluster-decay model (DCM) based on quantum-mechanical fragmentation theory (QMFT). Comparison with experimental data.

doi: 10.1103/PhysRevC.95.014611
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2017KA40      Phys.Rev. C 96, 024626 (2017)

M.Kaur, M.Kaur, V.Kaur

Role of different parts of the nucleon-nucleon potential on fragment production in asymmetric collisions and their rapidity dependence

NUCLEAR REACTIONS 120Sn(120Sn, X), 158Gd(82Kr, X), 184W(56Fe, X), 205Tl(35Cl, X), E=50-200 MeV/nucleon; calculated time evolution of mean densities, Charge distribution of fragments of Z=1-75, variations of the multiplicities of light charged particles (LCPs) and intermediate-mass fragments (IMFs) in the participant and quasiparticipant regions. Role of different parts of nucleon-nucleon (NN) interaction potential on the production of LCPs and IMFs with different rapidities. Isospin-dependent quantum molecular-dynamics (IQMD) model. Comparison with available experimental data.

doi: 10.1103/PhysRevC.96.024626
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2017SI12      J.Phys.(London) G44, 075105 (2017)

V.Singh, S.Sihotra, S.Roy, M.Kaur, S.Saha, J.Sethi, R.Palit, N.Singh, S.S.Malik, H.C.Jain, D.Mehta

Investigation of antimagnetic rotation in 101Pd

NUCLEAR REACTIONS 75As(31P, 3n2p)101Pd, E=125 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, negative-parity bands, J, π, level T1/2, B(E2). Comparison with available data.

doi: 10.1088/1361-6471/aa718a
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Data from this article have been entered in the XUNDL database. For more information, click here.

2017SI14      Phys.Rev. C 95, 064312 (2017)

V.Singh, S.Sihotra, G.H.Bhat, J.A.Sheikh, M.Kaur, S.Kumar, K.Singh, J.Goswamy, S.Saha, J.Sethi, R.Palit, S.S.Malik, N.Singh, U.Garg, D.Mehta

Band structures in 101Pd

NUCLEAR REACTIONS 75As(31P, 3n2p), E=125 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(linear polarization), DSAM half-life analysis for some of the levels in band B3 using INGA array of 21 clover Ge detectors at Pelletron-LINAC facility of TIFR-Mumbai. 101Pd; deduced high-spin levels, J, π, bands, multipolarities, mixing ratios, alignments, experimental Routhians, configurations, anti-magnetic rotational band. Comparison with projected shell model, and hybrid version of tilted-axis cranking shell model calculations. Comparison with structure of 99Pd.

doi: 10.1103/PhysRevC.95.064312
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Data from this article have been entered in the XUNDL database. For more information, click here.

2016KA07      J.Phys.(London) G43, 025103 (2016)

M.Kaur, S.Gautam

Influence of the constant and density-dependent scaling of the scattering cross-section on reaction dynamics

NUCLEAR REACTIONS 40Ca(40Ca, X), 58Ni(58Ni, X), 93Nb(93Nb, X), 124Sn(124Sn, X), 119Sn(129Xe, X), 139La(139La, X), 197Au(197Au, X), E=1500 MeV/nucleon; calculated σ as a function of density, time evolution of the collision rate, participant matter, directed transverse flow. The energy of vanishing flow (EVF) as a function of system mass (A) for soft and SMD Equation of State with CS and DDS cross-sections. Comparison with available data.

doi: 10.1088/0954-3899/43/2/025103
Citations: PlumX Metrics

2016KA34      Nucl.Phys. A955, 133 (2016)

M.Kaur, S.Gautam, R.K.Puri

Fragmentation in isotopic and isobaric systems as probe of density dependence of nuclear symmetry energy

NUCLEAR REACTIONS 64Ni(64Ni, x), 64Zn(64Zn, x), 70Zn(70Zn, x), E=30-400 MeV/nucleon; calculated free neutrons, light charged particle, intermediate fragment yields vs (N/Z), yields time dependence vs incident energy, rapidity distribution using soft and stiff symmetry energy.

doi: 10.1016/j.nuclphysa.2016.06.008
Citations: PlumX Metrics

2015KA30      Phys.Rev. C 92, 024623 (2015)

M.Kaur, B.B.Singh, M.K.Sharma, R.K.Gupta

Decay analysis of compound nuclei with masses A ≈ 30-200 formed in reactions involving loosely bound projectiles

NUCLEAR REACTIONS 27Al(7Li, X), E(cm)=7.94 MeV; 28Si(7Li, X), E(cm)=7.79 MeV; 32S(7Li, X), E(cm)=8.21 MeV; 40Ca(7Li, X), E(cm)=8.51 MeV; 48Ti(7Li, X), E(cm)=8.72 MeV; 59Co(7Li, X), E(cm)=9.88 MeV; 27Al(7Be, X), E(cm)=13.50 MeV; 32S(7Be, X), E(cm)=13.99 MeV; 40Ca(7Be, X), E(cm)=14.47 MeV; 48Ti(7Be, X), E(cm)=14.84 MeV; 58Ni(7Be, X), E(cm)=14.99 MeV; 65Cu(7Be, X), E(cm)=15.35 MeV; 27Al(9Be, X), E(cm)=21.00 MeV; 28Si(9Be, X), E(cm)=21.19 MeV; 124Sn(9Be, X), E(cm)=26.18 MeV; 144Sm(9Be, X), E(cm)=26.54 MeV; 169Tm(9Be, X), E(cm)=26.58 MeV; 187Re(9Be, X), E(cm)=26.71 MeV; calculated barrier modification factors, fragmentation potentials for A=1-18 fragments for 7Li projectile, A=30-70 for 7Be projectile, preformation and penetration probabilities, fusion cross sections. Dynamical cluster-decay model (DCM) for heavy-ion reactions at low energies. Comparison with available experimental data.

doi: 10.1103/PhysRevC.92.024623
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2015SA16      Phys.Rev. C 91, 044621 (2015)

R.Sandal, B.R.Behera, V.Singh, M.Kaur, A.Kumar, G.Kaur, P.Sharma, N.Madhavan, S.Nath, J.Gehlot, A.Jhingan, K.S.Golda, H.Singh, S.Mandal, S.Verma, E.Prasad, K.M.Varier, A.M.Vinodkumar, A.Saxena, J.Sadhukhan, S.Pal

Probing nuclear dissipation via evaporation residue excitation functions for the 16, 18O+198Pt reactions

NUCLEAR REACTIONS 198Pt(16O, 16O), (16O, X)214Rn*, E=78.0-105.6 MeV; 198Pt(18O, 18O), (18O, X)216Rn*, E=77.8-105.4; measured evaporation residues (ER), scattered 16,18O spectra, TOF spectrum, angular distributions of ERs, σ(E) for ERs and fusion using HYRA analyzer at IUAC-New Delhi 15 UD Pelletron facility. Comparison with statistical model calculations of compound nuclear decay with Kramers' fission width.

doi: 10.1103/PhysRevC.91.044621
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6263.

2014KA10      Phys.Rev. C 89, 034621 (2014)

M.Kaur, B.R.Behera, G.Singh, V.Singh, R.Sandal, A.Kumar, H.Singh, G.Singh, K.P.Singh, N.Madhavan, S.Nath, A.Jhingan, J.Gehlot, K.S.Golda, P.Sugathan, D.Siwal, S.Kalkal, E.Prasad, S.Appannababu

Anomalous deviations from statistical evaporation spectra for the decay of the 73Br and 77Rb compound systems

NUCLEAR REACTIONS 45Sc(28Si, X)73Br*, E=125 MeV; 45Sc(32S, X)77Rb*, E=125 MeV; measured inclusive and exclusive light charged-particle and neutron spectra, time-of flight, energy loss versus time-of-flight, σ for α particles, protons, evaporation residue σ using HIRA spectrometer at IUAC accelerator facility. Comparison with statistical model calculations using CASCADE code. Discussed effects of multistep compound (MSC) process.

doi: 10.1103/PhysRevC.89.034621
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2014KA12      Eur.Phys.J. A 50, 61 (2014)

M.Kaur, M.K.Sharma

Dynamics of 58Ni + 54Fe → 112Xe* reaction across the Coulomb barrier

NUCLEAR REACTIONS 54Fe(68Ni, X), E(cm)≈85-110 MeV. 112Xe calculated fragment preformation probability, evaporation residue σ, fast fission σ, neck length vs E(cm) using DCM (dynamical cluster model). Compared with data.

doi: 10.1140/epja/i2014-14061-6
Citations: PlumX Metrics

2014KA29      Nucl.Data Sheets 118, 333 (2014)

V.Kaur, M.Kaur, S.Kumar

Study of Various Potentials in Heavy-ion Collisions at Intermediate Energies

NUCLEAR REACTIONS 56Fe(56Fe, x), 58Ni(58Ni, X), E=60, 70, 80, 100, 120, 140 MeV/nucleon; calculated rapidity distribution using IQMD (isospin-dependent QMD); deduced influence of different potentials.

doi: 10.1016/j.nds.2014.04.073
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2014MU11      J.Phys.(London) G41, 115103 (2014)

I.Mukul, A.Roy, P.Sugathan, J.Gehlot, G.Mohanto, S.Nath, N.Madhavan, R.Dubey, T.Banerjee, N.Saneesh, I.Mazumdar, D.A.Gothe, A.K.R.Kumar, P.Arumugam, M.Kaur

Decoupling the effect of temperature on GDR widths in excited compound nucleus 144Sm

NUCLEAR REACTIONS 116Cd(28Si, X)144Sm, E=170, 196.5 MeV; measured reaction products, Eγ, Iγ; deduced fusion σ, giant dipole resonance parameters. Thermal shape fluctuation model calculations.

doi: 10.1088/0954-3899/41/11/115103
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2014SI03      Phys.Rev. C 89, 024609 (2014)

V.Singh, B.R.Behera, M.Kaur, A.Kumar, K.P.Singh, N.Madhavan, S.Nath, J.Gehlot, G.Mohanto, A.Jhingan, Ish Mukul, T.Varughese, J.Sadhukhan, S.Pal, S.Goyal, A.Saxena, S.Santra, S.Kailas

Measurement of evaporation residue excitation functions for the 19F + 194, 196, 198Pt reactions

NUCLEAR REACTIONS 194Pt, 196Pt, 198Pt(19F, X)213Fr*/215Fr*/217Fr*, E=96.2-137.3 MeV; measured spectra and angular distribution of evaporation residues (ER), σ(ER, E) using HYRA analyzer at IUAC-Pelletron-Linac facility; deduced survival probability, scaling of the FRLDM fission barrier. Comparison with statistical model calculations.

doi: 10.1103/PhysRevC.89.024609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6237.

2013IS10      Phys.Rev. C 88, 024312 (2013)

Ish Mukul, A.Roy, P.Sugathan, J.Gehlot, G.Mohanto, N.Madhavan, S.Nath, R.Dubey, I.Mazumdar, D.A.Gothe, M.Kaur, A.K.R.Kumar, P.Arumugam

Effect of angular momentum on giant dipole resonance observables in the 28Si+116Cd reaction

NUCLEAR REACTIONS 116Cd(28Si, X)144Sm*, E=125, 140 MeV; measured Eγ, Iγ, γγ-coin, time-of-flight, fold distribution using 4π spin spectrometer at Pelletron facility of IUAC; deduced γ-ray multiplicity, angular momentum distribution, average angular momentum, GDR energies, centroids, widths, deformation parameter, and strength distribution. Statistical model analysis using CASCADE computer code. Comparison with thermal shape fluctuation model (TSFM)calculations. 144Sm; calculated potential energy surface contours at different angular momenta and temperatures in (β, γ) plane.

doi: 10.1103/PhysRevC.88.024312
Citations: PlumX Metrics

2013KA51      Phys.Rev. C 88, 054620 (2013)

M.Kaur, V.Kaur, S.Kumar

Dependence of the energy of vanishing flow on different components of the nuclear potential

doi: 10.1103/PhysRevC.88.054620
Citations: PlumX Metrics

2013MO26      Phys.Rev. C 88, 034606 (2013)

G.Mohanto, N.Madhavan, S.Nath, J.Gehlot, I. Mukul, A.Jhingan, T.Varughese, A.Roy, R.K.Bhowmik, I.Mazumdar, D.A.Gothe, P.B.Chavan, J.Sadhukhan, S.Pal, M.Kaur, V.Singh, A.K.Sinha, V.S.Ramamurthy

Evaporation residue excitation function and spin distribution for 31P+170Er

NUCLEAR REACTIONS 170Er(31P, xn), E=134.4, 136.5, 141.6, 146.7, 151.9, 157.0, 162.1, 167.3, 172.0, 177.2 MeV; measured reaction products, Eγ, Iγ, TOF, evaporation residue (ER) σ(E) and spin distribution, ER-gated γ-multiplicity distributions using HYbrid Recoil mass Analyzer (HYRA) and a 4π spin spectrometer for γ rays at IUAC facility in Delhi. Comparison with statistical model calculations using CCFULL computer code. Discussed effect of compound nucleus shell closure.

doi: 10.1103/PhysRevC.88.034606
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6228.

2013SA01      Phys.Rev. C 87, 014604 (2013); Erratum Phys.Rev. C 87, 069901 (2013)

R.Sandal, B.R.Behera, V.Singh, M.Kaur, A.Kumar, G.Singh, K.P.Singh, P.Sugathan, A.Jhingan, K.S.Golda, M.B.Chatterjee, R.K.Bhowmik, S.Kalkal, D.Siwal, S.Goyal, S.Mandal, E.Prasad, K.Mahata, A.Saxena, J.Sadhukhan, S.Pal

Effect of N/Z in pre-scission neutron multiplicity for 16, 18O + 194, 198Pt systems

NUCLEAR REACTIONS 194,198Pt(16O, X), (18O, X)210Rn*/212Rn*/214Rn*/216Rn*, E=50, 61, 71.7, 79 MeV; measured fission fragment and neutron spectra by TOF, σ(E, θ) using NAND neutron detector array at LINAC+Pelletron facility at IUAC; deduced pre-scission neutron multiplicity. Statistical model analysis. Shell closure effect at N=126 for 212Rn.

doi: 10.1103/PhysRevC.87.014604
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6203.

2013SI19      Phys.Rev. C 87, 064601 (2013)

V.Singh, B.R.Behera, M.Kaur, A.Kumar, P.Sugathan, K.S.Golda, A.Jhingan, M.B.Chatterjee, R.K.Bhowmik, D.Siwal, S.Goyal, J.Sadhukhan, S.Pal, A.Saxena, S.Santra, S.Kailas

Neutron multiplicity measurements for 19F+194, 196, 198Pt systems to investigate the effect of shell closure on nuclear dissipation

NUCLEAR REACTIONS 194,196,198Pt(19F, X)213Fr*/215Fr*/217Fr*, E=90.2-139.6 MeV; measured fragment spectra, E(n), (fragment)n-coin, time-of-flight, neutron angular distributions, pre- and post-scission neutron multiplicities using NAND array at IUAC facility in Delhi; deduced reduced dissipation coefficients β as function of excitation energy, shell effects on dissipation strength. Comparison with statistical model calculations using Kramers fission width.

doi: 10.1103/PhysRevC.87.064601
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2012KA01      Phys.Rev. C 85, 014609 (2012)

M.Kaur, R.Kumar, M.K.Sharma

Systematic study of the decay of 118, 122Ba* formed in 78, 82Kr-induced reactions at ELAB = 5.5 MeV/nucleon

NUCLEAR REACTIONS 78,82Kr(40Ca, X)118Ba*/122Ba*, E(cm)=145.42, 147.87 MeV; analyzed evaporation residue cross sections, total fission cross sections, preformation probability as a function of fragment mass number, fragmentation potential, fragment cross sections, neck-length parameter, σ(118Ba)/σ(122Ba) as a function of charge number. N/Z dependence of decay fragments for A=114-126 (even A) Ba isotopes. Dynamical cluster decay model (DCM).

doi: 10.1103/PhysRevC.85.014609
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2012KA05      Ukr.J.Phys. 57, 289 (2012)

M.Kaur, S.Kumar

Influence of Momentum-Dependent Interactions on the Nuclear Stopping in Symmetric Heavy-Ion Collisions

NUCLEAR REACTIONS 131Xe(131Xe, X), E=400 MeV/nucleon; 197Au(197Au, X), E<100 MeV/nucleon; calculated rapidity distribution, anisotropic ratio, impact parameter dependence of multiplicity.

2012KA15      Phys.Rev. C 85, 054605 (2012)

M.Kaur, M.K.Sharma

Decay mechanism of the 204Po* nucleus formed in 16O and 28Si induced reactions

NUCLEAR REACTIONS 188Os(16O, X)204Po*, 176Yb(28Si, X)204Po*, E=84-155 MeV; calculated scattering potentials, evaporation residue cross section, fission cross section, fragmentation potential, barrier heights, σ(E), fragment anisotropies, preformation probability for decay of 204Po compound nucleus. Dynamical cluster decay model (DCM). Comparison with experimental data.

doi: 10.1103/PhysRevC.85.054605
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2012KA39      Phys.Rev. C 86, 064610 (2012)

M.Kaur, M.K.Sharma, R.K.Gupta

Effects of deformations and orientations in the fission of the actinide nuclear system 254Fm* formed in the 11B + 243Am reaction

NUCLEAR REACTIONS 243Am(11B, X)254Fm*, E=60-72 MeV; calculated fragmentation potential, preformation probability, asymmetric to symmetric fission yields, fusion-fission σ(E), neck-length parameter, barrier-lowering parameter using spherical, β2, and β2 to β4 deformations. Dynamical cluster decay model (DCM). Comparison with experimental data.

doi: 10.1103/PhysRevC.86.064610
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2012SI12      Phys.Rev. C 86, 014609 (2012)

V.Singh, B.R.Behera, M.Kaur, P.Sugathan, K.S.Golda, A.Jhingan, J.Sadhukhan, D.Siwal, S.Goyal, S.Santra, A.Kumar, R.K.Bhowmik, M.B.Chatterjee, A.Saxena, S.Pal, S.Kailas

Search for an effect of shell closure on nuclear dissipation via a neutron-multiplicity measurement

NUCLEAR REACTIONS 194,196,198Pt(19F, X)213Fr/215Fr/217Fr, E=92-141 MeV; measured neutron spectra, n(fission fragment)-coin, prescission and total neutron multiplicity excitation functions using the NAND array at Pelletron+LINAC facility of IUAC, pulsed beam. Statistical model analysis. Shell effects on nuclear dissipation.

doi: 10.1103/PhysRevC.86.014609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6198.

2002DA06      J.Phys.(London) G28, 321 (2002)

S.Dahiya, M.Kaur, S.Dhamija

Bunching Parameter Analysis and Multifractal Multiplicity Distributions in Hadron-Hadron and Hadron-Nucleus Interactions

NUCLEAR REACTIONS 1H(p, X), E(cm)=13.9-62.2 GeV; 1H(π-, X), E(cm)=16.63-21.68 GeV; 1H(π+, X), E(cm)=16.66-21.68 GeV; 1H(K-, X), E(cm)=16.63 GeV; 1H(K+, X), E(cm)=16.64-21.68 GeV; Ne(π-, X), (π+, X), E=30-64 GeV; Au, W(p, X), E=200, 400 GeV; calculated charged particle multiplicity using Multifractal negative binomial distributions, bunching parameters. Comparison with data.

doi: 10.1088/0954-3899/28/2/310
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2002DH01      J.Phys.(London) G28, 1239 (2002)

S.Dhamija, M.Kaur, S.Dahiya

Inclusive Studies of Pion-Nucleus Interactions in the Framework of the Lund Fragmentation Model

NUCLEAR REACTIONS Ag, Br(π-, X), E=50 GeV; measured fragments multiplicity, pseudorapidity distributions; deduced reaction mechanism features. Multistring model analysis, Lund fragmentation scheme.

doi: 10.1088/0954-3899/28/6/307
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2002DH04      Can.J.Phys. 80, 1571 (2002)

S.Dhamija, M.Kaur, S.Dahiya

Analysis of pion-nucleus interactions in the framework of a multistring model

NUCLEAR REACTIONS Ag, Br(π-, X), E=50, 200, 340, 525 MeV; analyzed shower particle multiplicity, pseudorapidity distributions. Multistring model, Monte Carlo approach.

doi: 10.1139/p02-074
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2001DH01      Phys.Rev. C63, 035201 (2001)

S.Dhamija, M.Kaur, S.Dahiya

Analysis of Hadron-Nucleus Interactions in the Framework of Two Multistring Models

NUCLEAR REACTIONS Ag, Br(p, X), E at 200-800 GeV/c; analyzed fast and slow particles pseudorapidity, multiplicity distributions. Two multistring models compared.

doi: 10.1103/PhysRevC.63.035201
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1998DA22      J.Phys.(London) G24, 2027 (1998)

S.Dahiya, M.Kaur

Multifractal Multiplicity Distribution in e+e- and (p-bar)p Interactions from Nonlinear Markov Process

NUCLEAR REACTIONS 1H(p-bar, X), E=200, 900 GeV; analyzed multiplicity distributions. Multifractal negative binomial distribution.

doi: 10.1088/0954-3899/24/11/005
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1989AD13      Phys.Rev.Lett. 63, 2349 (1989)

M.Aderholz, M.M.Aggarwal, H.Akbari, P.P.Allport, P.V.K.S.Baba, S.K.Badyal, M.Barth, J.P.Baton, H.H.Bingham, E.B.Brucker, R.A.Burnstein, R.C.Campbell, R.Cence, T.K.Chatterjee, E.F.Clayton, G.Corrigan, C.Coutures, D.Deprospo, Devanand, E.De Wolf, P.J.W.Faulkner, W.B.Fretter, V.K.Gupta, J.Guy, J.Hanlon, G.Harigel, F.Harris, M.A.Jabiol, P.Jacques, V.Jain, G.T.Jones, M.D.Jones, R.W.L.Jones, T.Kafka, M.Kalelkar, P.Kasper, P.Kasper, G.L.Kaul, M.Kaur, J.M.Kohli, E.L.Koller, R.J.Krawiec, M.Lauko, J.Lys, W.A.Mann, P.Marage, R.H.Milburn, D.B.Miller, I.S.Mittra, M.M.Mobayyen, J.Moreels, D.R.O.Morrison, G.Myatt, P.Nailor, R.Naon, A.Napier, M.Neveu, D.Passmore, M.W.Peters, V.Z.Peterson, R.Plano, N.K.Rao, H.A.Rubin, J.Sacton, B.Saitta, P.Schmid, N.Schmitz, J.Schneps, R.Sekulin, S.Sewell, J.B.Singh, P.M.Sood, W.Smart, P.Stamer, K.E.Varvell, W.Venus, L.Verluyten, L.Voyvodic, H.Wachsmuth, S.Wainstein, S.Willocq, W.Wittek, G.P.Yost

Coherent Production of π+ and π- Mesons by Charged-Current Interactions of Neutrinos and Antineutrinos on Neon Nuclei at the Fermilab Tevatron

NUCLEAR REACTIONS 1H, Ne(ν, X), (ν-bar, X), E=40-300 GeV; measured coherent single π+, π- production σ, kinematic distributions. Meson dominance, partial axial-vector current conservation model.

doi: 10.1103/PhysRevLett.63.2349
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