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NSR database version of May 24, 2024.

Search: Author = S.K.Sharma

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6342.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6330.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6317.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0733.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the XUNDL database. For more information, click here.

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
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Data from this article have been entered in the XUNDL database. For more information, click here.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1710.

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1713.

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6040.

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6050.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1990SH19      Phys.Rev. C42, 635 (1990)

S.K.Sharma, P.K.Raina

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
Citations: PlumX Metrics

1988RA14      Phys.Rev. C37, 1427 (1988)

P.K.Raina, S.K.Sharma

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
Citations: PlumX Metrics

1988RA35      Phys.Rev. C38, 2928 (1988)

P.K.Rath, S.K.Sharma

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1986GH01      Phys.Rev. C33, 1258 (1986)

B.Ghosh, S.K.Sharma

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
Citations: PlumX Metrics

1986TR06      Phys.Rev. C34, 1081 (1986)

P.N.Tripathi, S.K.Sharma

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
Citations: PlumX Metrics

1985GH02      Phys.Rev. C32, 643 (1985)

B.Ghosh, S.K.Sharma

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
Citations: PlumX Metrics

1985MU02      Phys.Rev. C31, 689 (1985)

G.Mukherjee, S.K.Sharma

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
Citations: PlumX Metrics

1985MU17      Phys.Rev. C32, 2122 (1985)

G.Mukherjee, S.K.Sharma

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
Citations: PlumX Metrics

1984MU14      Phys.Rev. C29, 2101 (1984)

G.Mukherjee, S.K.Sharma

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1981KH06      Phys.Rev. C24, 2715 (1981)

S.K.Khosa, S.K.Sharma

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1976AM03      Nuovo Cim. 35A, 527 (1976)

A.Amusa, S.K.Sharma

Modified Hartree-Fock Calculations in 18O Nucleus

NUCLEAR STRUCTURE 18O; calculated levels.

doi: 10.1007/BF02731785
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1976SH18      Phys.Lett. 62B, 259 (1976)


Magnetic Moment of 57Ni

NUCLEAR MOMENTS 57Ni; calculated μ.

doi: 10.1016/0370-2693(76)90069-1
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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
Citations: PlumX Metrics

1974AV05      Phys.Rev. C10, 2106 (1974)

F.T.Avignone III, S.K.Sharma

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1973SH10      Phys.Lett. 44B, 491 (1973)

S.K.Sharma, K.H.Bhatt

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
Citations: PlumX Metrics

1972SH19      Nucl.Phys. A192, 625 (1972)

S.K.Sharma, K.H.Bhatt

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
Citations: PlumX Metrics

1972SH23      Phys.Lett. 41B, 287 (1972)

S.K.Sharma, K.H.Bhatt

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
Citations: PlumX Metrics

1971SH28      Phys.Lett. 36B, 550 (1971)

S.K.Sharma, K.H.Bhatt

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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