NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = S.K.Sharma Found 50 matches. 2019SI30 Acta Phys.Pol. B50, 1451 (2019) U.Singh, B.Kamys, S.K.Sharma, K.Pysz Odd-Even Staggering in the Yields of Intermediate Mass Fragments from p+Ag collisions at Ep = 480 MeV NUCLEAR REACTIONS Ag(p, X)Li/Be/B/C/N/O/F/Ne/Na/Mg, E=480 MeV; measured reaction products; deduced total production σ. Comparison with intranuclear cascade INCL++ and the second stage by GEMINI++ model or by two other models, namely ABLA07 and SMM.
doi: 10.5506/aphyspolb.50.1451
2018PA24 Phys.Rev. C 98, 014601 (2018) V.V.Parkar, S.K.Pandit, A.Shrivastava, R.Palit, K.Mahata, V.Jha, K.Ramachandran, S.Gupta, S.Santra, S.K.Sharma, S.Upadhyaya, T.N.Nag, S.Bhattacharya, T.Trivedi, S.Kailas Fusion reaction studies for the 6Li + 124Sn system at near-barrier energies NUCLEAR REACTIONS 124Sn(6Li, X)126I/127I/123Sn/125Sn/125Sb/124Sb/127Te/126Te, E=17.5-35.7 MeV; 159Tb(6Li, X)160Ho/162Ho, E=23.7-33.8 MeV; measured Eγ, Iγ, σ(E) for evaporation residues, complete, incomplete and total fusion (CF, ICF, TF), transfer and capture reactions by online and offline activation methods at the BARC-TIFR Pelletron-Linac facility. Comparison with previous experimental incomplete fusion σ for 209Bi, 197Au, 159Tb, 124Sn(7Li, X), (6Li, X) reactions, and with statistical model and coupled channel calculations using PACE and CCFULL codes.
doi: 10.1103/PhysRevC.98.014601
2018SI19 Eur.Phys.J. A 54, 109 (2018) U.Singh, D.Filges, F.Goldenbaum, B.Kamys, Z.Rudy, S.K.Sharma The predictive power of spallation models for isotopic cross sections NUCLEAR REACTIONS 1H(136Xe, x), E=1000 MeV/nucleon; calculated isotopic σ of IMFs with Z=3-56 using INCL++ coupled to ABLA07, GEM2, GEMINI++ and SMM. Compared to available data.
doi: 10.1140/epja/i2018-12546-x
2018TR02 Int.J.Mod.Phys. E27, 1850010 (2018) R.Tripathi, S.Sodaye, K.Ramachandran, S.K.Sharma, P.K.Pujari Incomplete mass transfer processes in 28Si+93Nb reaction
doi: 10.1142/S0218301318500106
2017SH21 Eur.Phys.J. A 53, 150 (2017) S.K.Sharma, B.Kamys, F.Goldenbaum, D.Filges Ranking and validation of spallation models for isotopic production cross sections of heavy residua NUCLEAR REACTIONS 1H(136Xe, x), E=500 MeV/nucleon; calculated isotopic σ (mass distributions), A-factor, both standardized and non-standardized H-factor and M-factors for elements of Z=41-56 using ABLA, GEM2, GEMINI and SMM codes. Compared to data.
doi: 10.1140/epja/i2017-12334-2
2017SU07 Phys.Rev. C 95, 024604 (2017) K.Sudarshan, R.Tripathi, S.Sodaye, S.K.Sharma, P.K.Pujari, J.Gehlot, N.Madhavan, S.Nath, G.Mohanto, I.Mukul, A.Jhingan, I.Mazumdar Spin distributions and cross sections of evaporation residues in the 28Si + 176Yb reaction NUCLEAR REACTIONS 176Yb(28Si, X), E=143-178 MeV in steps of 7 MeV; measured evaporation-residue σ(E), Eγ, Iγ, (residue)γ-coin, γ-ray multiplicities using the hybrid recoil mass analyzer (HYRA) coupled to TIFR 4π-spin spectrometer at the Pelletron-LINAC accelerator of IUAC-New Delhi, and off-line σ(E) of evaporation residues using the recoil catcher technique γ-detection at Pelletron-LINAC of BARC-TIFR-Mumbai. 198,199,200Po, 199,200mBi; measured formation σ(E). Comparison of average γ-ray multiplicities with predictions of the statistical model calculations using PACE2 and CCFUS codes.
doi: 10.1103/PhysRevC.95.024604
2016SH20 Eur.Phys.J. A 52, 171 (2016) S.K.Sharma, B.Kamys, F.Goldenbaum, D.Filges Ranking and validation of the spallation models for description of intermediate mass fragment emission from p + Ag collisions at 480 MeV incident proton beam energy NUCLEAR REACTIONS Ag(p, x), E=480 MeV; calculated intermediate mass fragments (6Li to 27Mg) σ(θ, E) using cascade code INCL4.6 combined with one of ABLA07, GEM2, GEMINI++, SMM; compared to published data; deduced reaction mechanisms, H- and M-factors for all intermediate mass fragments, ranking of model predictions.
doi: 10.1140/epja/i2016-16171-5
2014FI10 Phys.Rev. C 89, 054617 (2014) M.Fidelus, D.Filges, F.Goldenbaum, H.Hodde, A.Jany, L.Jarczyk, B.Kamys, M.Kistryn, St.Kistryn, St.Kliczewski, E.Kozik, P.Kulessa, H.Machner, A.Magiera, B.Piskor-Ignatowicz, K.Pysz, Z.Rudy, S.K.Sharma, R.Siudak, M.Wojciechowski, for the PISA Collaboration Sequential and simultaneous emission of particles from p + Al collisions at GeV energies NUCLEAR REACTIONS Al(p, X), E=1.2, 1.9, 2.5 GeV; measured particle spectra, σ(E, θ) of p, d, t, 3,4,6He, 6,7,8,9Li, 7,9,10Be, 10,11B by ΔE-E method using detector telescopes at COSY synchrotron of Julich Research Center under PISA collaboration. Comparison with intranuclear cascade model coupled to evaporation, and to statistical multifragmentation models.
doi: 10.1103/PhysRevC.89.054617
2014SH21 Nucl.Data Sheets 119, 307 (2014) S.K.Sharma, D.Filges, F.Goldenbaum, B.Kamys Dependence and Influence of Projectile Energy and Target Mass on the Production of Light Charged Particles and Intermediate Mass Fragments in Proton Induced Reactions NUCLEAR REACTIONS 19C, 27Al, Ni, 108Ag, 197Au(p, x), E=1.2, 1.9, 2.5 GeV; measured charged particles up to A=8; deduced σ(θ, E); calculated σ(θ, E) using INCL4.6 cascade model for fast stage and SMM, ABLA07 and GEMINI++ for emission from residual.
doi: 10.1016/j.nds.2014.08.084
2014SH36 Acta Phys.Pol. B45, 1963 (2014) S.K.Sharma, B.Kamys, F.Goldenbaum, D.Filges Validation of Spallation Models for p+Al Reactions at 180 MeV Incident Proton Beam Energy NUCLEAR REACTIONS 27Al(p, X), E=180 MeV; measured reaction fragments; deduced σ and σ(θ) for fragment production. Comparison with theoretical calculations.
doi: 10.5506/APhysPolB.45.1963
2014SO17 J.Phys.(London) G41, 125103 (2014) S.Sodaye, R.Tripathi, K.Sudarshan, S.K.Sharma, P.K.Pujari, R.Palit, S.Mukhopadhyay EC decay of 244Bk RADIOACTIVITY 244Bk(EC) [from 238U(11B, X), E=63.6 MeV]; measured decay products, Eγ, Iγ; deduced energy levels, relative intensities, decay level scheme, T1/2. Comparison with theoretical calculations.
doi: 10.1088/0954-3899/41/12/125103
2013GA11 Phys.Rev. C 87, 034317 (2013) R.Garg, S.Kumar, M.Saxena, S.Goyal, D.Siwal, S.Verma, R.Palit, S.Saha, J.Sethi, S.K.Sharma, T.Trivedi, S.K.Jadav, R.Donthi, B.S.Naidu, S.Mandal High spin states in 57135La78 NUCLEAR REACTIONS 128Te(11B, 4n), E=50.5 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ)(DCO), γγ(lin pol), using the INGA at the TIFR facility. 135La; deduced high-spin levels, J, π, multipolarity, bands, dipole bands, configurations, alignments, B(M1)/B(E2). Systematics of 11/2- bands in odd-A (A=129-137) La nuclei. Comparison with Tilted Axis Cranking (TAC) calculations.
doi: 10.1103/PhysRevC.87.034317
2011PA25 Radiochim.Acta Supp 1, Proc.in Radiochemistry 131 (2011) V.V.Parkar, R.Palit, S.K.Sharma, B.S.Naidu, P.K.Joshi, S.Santra, P.K.Rath, K.Ramachandran, K.Mahata, T.Trivedi, A.Raghav Complete and incomplete fusion in 9Be + 124Sn system NUCLEAR REACTIONS 124Sn(9Be, X), E=26-46 MeV; measured reaction products, Eγ, Iγ; deduced σ.
doi: 10.1524/rcpr.2011.0024
2009TR03 Phys.Rev. C 79, 064604 (2009) R.Tripathi, K.Sudarshan, S.Sodaye, A.V.R.Reddy, A.Goswami, B.K.Nayak, S.K.Sharma Cross sections of projectile-like fragments in the reaction 19F+66Zn in the beam energy range of 3-6 MeV/nucleon NUCLEAR REACTIONS 66Zn(19F, X)Li/Be/B/C/N/O, E=65, 85, 95, 112 MeV; measured spectra of projectile-like fragments and scattered beam particles, σ, σ(θ); deduced transmission coefficients, probability for complete fusion, transfer probabilities and optical model parameters. 66Zn(19F, X)9B/10B/11B/12C/13C/14C/13N/14N/15N/16O/17O/18O, E=61, 82, 92 MeV; deduced slope parameter α. Comparison with sum-rule model calculations and with data from 89Y(19F, X) reaction.
doi: 10.1103/PhysRevC.79.064604
2009TR04 Phys.Rev. C 79, 064607 (2009) R.Tripathi, K.Sudarshan, S.K.Sharma, K.Ramachandran, A.V.R.Reddy, P.K.Pujari, A.Goswami Fission fragment angular distributions in the reactions 16O+188Os and 28Si+176Yb NUCLEAR REACTIONS 188Os(16O, X), E=84, 89, 94, 99 MeV; 176Yb(28Si, X), E=138, 145, 149, 155 MeV; measured fission fragment spectra, fission and complete fusion σ, σ(θ) of fission fragments and anisotropies. Comparisons with statistical saddle point model predictions.
doi: 10.1103/PhysRevC.79.064607
2009TR08 Eur.Phys.J. A 42, 25 (2009) R.Tripathi, K.Sudarshan, S.Sodaye, S.K.Sharma, A.V.R.Reddy, A.Goswami Effect of projectile structure in incomplete fusion in 24Mg + 59Co reaction NUCLEAR REACTIONS 59Co(24Mg, X)Li/Be/B/C/N/O/F/Ne, E=93, 100, 108 MeV; measured fragment spectra, σ, σ(θ) from incomplete fusion; deduced transfer probabilities. Comparison with the sum rule model.
doi: 10.1140/epja/i2009-10863-9
2007TR02 Phys.Rev. C 75, 024609 (2007) R.Tripathi, K.Sudarshan, S.Sodaye, S.K.Sharma, A.V.R.Reddy Anomalous fission fragment angular distribution in the 11B+243Am reaction at near-barrier energies NUCLEAR REACTIONS 243Am(11B, F), E=60-72 MeV; measured fission fragment angular distributions, anisotropy; deduced role of target deformation. Comparison with statistical theory.
doi: 10.1103/PhysRevC.75.024609
1999SH14 J.Phys.(London) G25, 135 (1999) A.Sharma, S.Kumar, S.K.Sharma, N.Nath, V.Hairkumar, A.P.Pathak, L.N.S.Prakash Goteti, S.K.Hui, D.K.Avasthi An Experimental Study of Stopping Power for MeV Heavy Ions
doi: 10.1088/0954-3899/25/1/012
1995SH07 Appl.Radiat.Isot. 46, 39 (1995) S.K.Sharma, S.Kumar, J.S.Yadav, A.P.Sharma Stopping Power of Heavy Ions in Solids: A comparative study
doi: 10.1016/0969-8043(94)00087-G
1990SH02 Phys.Rev. C41, 1315 (1990) S.K.Sharma, G.Mukherjee, P.K.Rath Double Gamow-Teller Matrix Elements in the Germanium Region RADIOACTIVITY 76Ge, 82Se(2β); calculated 2β-decay matrix elements. Variational wave functions.
doi: 10.1103/PhysRevC.41.1315
1990SH19 Phys.Rev. C42, 635 (1990) Validity of the Adiabatic Rotational Model in the Case of the Hexadecupole Operator NUCLEAR STRUCTURE 48,50,52Ti, 50,52,54Cr, 52,54Fe; calculated intrinsic quadrupole moments, B(λ). Projected HFB, rotor models comparison.
doi: 10.1103/PhysRevC.42.635
1988RA14 Phys.Rev. C37, 1427 (1988) Form Factors and Transition Charge Densities for the Quadrupole and Hexadecupole Electroexcitation of some 2p-1f Shell Nuclei NUCLEAR STRUCTURE 48,50Ti, 50,52,54Cr, 54Fe, 58,60,62Ni, 64,66,68Zn; calculated electroexcitation form factors, transition charge densities. Hartree-Fock-Bogoliubov method, large valence space, realistic effective interactions.
doi: 10.1103/PhysRevC.37.1427
1988RA35 Phys.Rev. C38, 2928 (1988) Gyromagnetic Factors of the High-Spin Yrast States in Some Doubly Even Germanium and Selenium Isotopes NUCLEAR STRUCTURE 68,70,72,74,76Ge, 72,74,76,78,80Se; calculated g. Variation after projection.
doi: 10.1103/PhysRevC.38.2928
1988SH39 Phys.Rev. C38, 2935 (1988) S.K.Sharma, P.N.Tripathi, S.K.Khosa Onset of Large Deformation and the Occurrence of Anomalous High-Spin Yrast Spectra in the Zirconium Region NUCLEAR STRUCTURE 100,102,104,106Mo; calculated levels, B(λ), moments of inertia. Self-consistent HFB.
doi: 10.1103/PhysRevC.38.2935
1986GH01 Phys.Rev. C33, 1258 (1986) Elastic Magnetic Scattering on 51V NUCLEAR REACTIONS 51V(e, e'), E not given; calculated magnetic form factors; deduced 48Ca core role in anomalous M3 scattering.
doi: 10.1103/PhysRevC.33.1258
1986TR06 Phys.Rev. C34, 1081 (1986) High-Spin Yrast Levels in Doubly Even Germanium and Selenium Isotopes: Microscopic study in the variation-after-projection approach NUCLEAR STRUCTURE 68,70,72,74Ge, 70,72,74,76Se; calculated levels, yrast sequence, static quadrupole moments, B(E2). HFB, realistic effective interactions.
doi: 10.1103/PhysRevC.34.1081
1985GH02 Phys.Rev. C32, 643 (1985) Suppression of Elastic Magnetic Electron Scattering Form Factors NUCLEAR STRUCTURE 57Ni; calculated M1, M3 form factors. First-, second-order core polarization effects.
doi: 10.1103/PhysRevC.32.643
1985MU02 Phys.Rev. C31, 689 (1985) Inelastic Electron Scattering Form Factors Involving the Second Excited 2+ Levels in the Nuclei 48Ti and 50Cr NUCLEAR REACTIONS 48Ti, 50Cr(e, e'), E not given; calculated form factors. Realistic effective interactions, prolate oblate intrinsic states.
doi: 10.1103/PhysRevC.31.689
1985MU17 Phys.Rev. C32, 2122 (1985) Proton-Neutron Occupancies of Spherical Shells in the Ground States of some Doubly Even 2p-1f Shell Nuclei NUCLEAR STRUCTURE 46,48Ti, 50,52,54Cr, 54,56,58,60Fe, 56,58,60,62,64Ni, 64,66,68Zn, 70Ge; calculated subshell occupation numbers. Projected HFB calculations.
doi: 10.1103/PhysRevC.32.2122
1984MU14 Phys.Rev. C29, 2101 (1984) Inelastic Electron Scattering Form Factors for the Excitation of 2+ States in some 2p-1f Shell Nuclei NUCLEAR STRUCTURE 46,48,50Ti, 50,52Cr, 54,56Fe; calculated static quadrupole moment, B(E2). Projected HFB, effective Kuo-Brown interaction. NUCLEAR REACTIONS 46,48Ti, 50Cr, 56Fe(e, e'), E not given; calculated form factors. Projected HFB, effective Kuo-Brown interaction.
doi: 10.1103/PhysRevC.29.2101
1984TR04 Phys.Rev. C29, 1951 (1984) P.N.Tripathi, S.K.Sharma, S.K.Khosa Backbending Anomaly in Some Highly Neutron-Rich Molybdenum Isotopes NUCLEAR STRUCTURE 100,102,104,106Mo; calculated yrast spectra, B(E2), quadrupole moment, subshell occupation numbers, backbending plots. Variational approach.
doi: 10.1103/PhysRevC.29.1951
1982KH06 Phys.Lett. 119B, 257 (1982) S.K.Khosa, P.N.Tripathi, S.K.Sharma Microscopic Description of the Onset of Large Deformations in the Zirconium Region NUCLEAR STRUCTURE 100,102Zr; calculated yrast levels, neutron, proton occupation numbers, intrinsic quadrupole moments. 94,98Zr, 92,102,104,106Mo; calculated neutron, proton occupation numbers, intrinsic quadruppole moments. 94,96,98,100Mo; calculated neutron, proton occupation numbers, B(E2), intrinsic quadrupole moments. Self-consistent HFB method, pairing plus quadrupole-quadrupole interaction.
doi: 10.1016/0370-2693(82)90665-7
1982SH30 Phys.Rev. C26, 2706 (1982) S.K.Sharma, V.Potbhare, V.K.B.Kota Yrast Bands in Light Nuclei and the Effective Interactions in J = 0, 2 States NUCLEAR STRUCTURE 20,21,22O, 20Ne, 60Ni; calculated levels, yrast band, wave function overlaps. Effective interactions.
doi: 10.1103/PhysRevC.26.2706
1981KH06 Phys.Rev. C24, 2715 (1981) Deformation-Producing Tendency of the Like-Particle Effective Interactions in Nuclei NUCLEAR STRUCTURE 100,102Zr; calculated yrast levels; deduced deformation onset. Cranked Hartree-Fock calculations, effective interactions.
doi: 10.1103/PhysRevC.24.2715
1981PO15 Phys.Rev. C24, 2355 (1981) V.Potbhare, S.K.Sharma, S.P.Pandya High-Spin Yrast Cascade in 60Ni NUCLEAR STRUCTURE 60Ni; calculated yrast levels, B(λ), μ, quadrupole moments. Shell model.
doi: 10.1103/PhysRevC.24.2355
1981SH10 Phys.Lett. 102B, 85 (1981) On the Suppression of Magnetic Octupole Moments NUCLEAR MOMENTS 57Ni; calculated corrections to magnetic dipole, octupole moments. Perturbation theory, realistic interactions, renormalization graphs.
doi: 10.1016/0370-2693(81)91035-2
1980SH23 Phys.Rev. C22, 2612 (1980) Microscopic Description of the High-Spin Yrast Spectra in Some Doubly Even Zinc, Germanium, and Selenium Isotopes NUCLEAR STRUCTURE 62,64,66,68Zn, 72,74,76,78Se, 70,72,74,76Ge; calculated yrast levels, static quadrupole moments, B(E2), p to g-shell occupation numbers. HFB, angular momentum projection.
doi: 10.1103/PhysRevC.22.2612
1976AM03 Nuovo Cim. 35A, 527 (1976) Modified Hartree-Fock Calculations in 18O Nucleus NUCLEAR STRUCTURE 18O; calculated levels.
doi: 10.1007/BF02731785
1976SH07 Phys.Lett. 61B, 122 (1976) S.K.Sharma, L.Satpathy, S.B.Khadkikar, S.C.K.Nair On the Validity of the Cranked Hartree-Fock Approximation NUCLEAR STRUCTURE 20Ne, 52Fe; calculated dependence of moment of inertia on angular momenta.
doi: 10.1016/0370-2693(76)90604-3
1976SH09 Nucl.Phys. A260, 226 (1976) On the Microscopic Description of the Low-Lying States in Doubly Even 2p-1f Shell Nuclei NUCLEAR STRUCTURE 44,46,48,50Ti, 48,50,52,54Cr, 52,54,56,58Fe, 56,58,60,62Ni; calculated levels, quadrupole moment, B(E2).
doi: 10.1016/0375-9474(76)90026-9
1976SH18 Phys.Lett. 62B, 259 (1976) Magnetic Moment of 57Ni NUCLEAR MOMENTS 57Ni; calculated μ.
doi: 10.1016/0370-2693(76)90069-1
1975SH14 Phys.Lett. 57B, 210 (1975) On the Structure of Low-Lying Levels in 56Ni NUCLEAR STRUCTURE 56Ni; calculated levels.
doi: 10.1016/0370-2693(75)90055-6
1974AV05 Phys.Rev. C10, 2106 (1974) Improved Projected Hartree-Fock Description of the Low-Lying Quasirotational States in Nuclei NUCLEAR STRUCTURE 18O; calculated wave functions.
doi: 10.1103/PhysRevC.10.2106
1974SH04 Phys.Lett. 49B, 5 (1974) The Structure of the Ground States of Nickel Isotopes and the Effective Interactions in the 2p-1f Shell NUCLEAR STRUCTURE 56,58,60,62,64Ni; calculated subshell occupancies.
doi: 10.1016/0370-2693(74)90566-8
1974SH20 Phys.Lett. 52B, 299 (1974) Static Quadrupole Moments and B(E2)(0→2) Values in 2p-1f Shell Nuclei NUCLEAR STRUCTURE 44,46,48,50Ti, 48,50,52,54Cr, 52,54,56,58Fe, 58,60,62,64Ni; calculated quadrupole moment, B(E2).
doi: 10.1016/0370-2693(74)90046-X
1974SH22 Phys.Lett. 53B, 155 (1974) Hartree-Fock-Bogolubov Projected Spectra for Cr and Fe Isotopes and the Effective Interactions in the 2p-1f Shell NUCLEAR STRUCTURE 48,50,52,54Cr, 52,54,56,58Fe; calculated levels.
doi: 10.1016/0370-2693(74)90518-8
1973SH10 Phys.Lett. 44B, 491 (1973) Effective Interactions and the 1f7/2 Sub-Shell Closure in the 2p-1f Shell NUCLEAR STRUCTURE 56Ni; calculated f7/2 sub-shell closure.
doi: 10.1016/0370-2693(73)90005-1
1972SH19 Nucl.Phys. A192, 625 (1972) On the Non-Pairing Aspects of the T = 1 Interaction NUCLEAR STRUCTURE 44Ti, 44Ca, 46Ti, 48Cr, 52Cr, 52Fe, 56Ni; calculated Hartree-Fock energies, energy gaps, multipole moments.
doi: 10.1016/0375-9474(72)90094-2
1972SH23 Phys.Lett. 41B, 287 (1972) A Comparison of the Pairing Tendencies of the T = 1 and T = 0 Interactions NUCLEAR STRUCTURE 44,48Ti, 52Fe; calculated Hartree-Fock states, quadrupole moment, energy gap; analyzed T=0, 1 interaction pairing.
doi: 10.1016/0370-2693(72)90580-1
1971SH28 Phys.Lett. 36B, 550 (1971) On the Deformation Producing Tendency of the T = 1 Interaction NUCLEAR STRUCTURE 44,46Ti, 48,52Cr, 52,56Ti; calculated quadrupole, multipole moments. Deformed Hartree-Fock method.
doi: 10.1016/0370-2693(71)90086-4
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