NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.B.Khadkikar Found 36 matches. 1999VI01 Eur.Phys.J. A 4, 83 (1999) P.C.Vinodkumar, J.N.Pandya, V.M.Bannur, S.B.Khadkikar A Unified Scheme for Flavoured Mesons and Baryons
doi: 10.1007/s100500050206
1998VI02 Pramana 50, 149 (1998) K.B.Vijayakumar, S.B.Khadkikar Spin Observables of the NN Interaction in a Relativistic Harmonic Model with Confined Gluons and Mesons NUCLEAR REACTIONS 1H(n, X), E=50, 150, 300 MeV; calculated spin observables; deduced gluon confinement effects. Relativistic harmonic model.
doi: 10.1007/BF02847525
1997ME17 Nucl.Phys. A624, 391 (1997) U.Meyer, A.Faessler, S.B.Khadkikar The Triaxial Rotation Vibration Model in the Xe-Ba Region NUCLEAR STRUCTURE 126Xe, 130Ba; calculated levels, branching ratios; deduced β-vibrational band. Triaxial rotation vibration model, comparisons with interacting boson model, data.
doi: 10.1016/S0375-9474(97)00380-1
1995TE01 Nucl.Phys. A586, 249 (1995) G.Teneva, F.Simkovic, A.Bobyk, M.K.Cheoun, A.Faessler, S.B.Khadkikar Two-Vacua RPA and the Two-Neutrino DOuble-Beta Decay RADIOACTIVITY 48Ca(2β); calculated Gamow-Teller strength functions, 2ν-accompanied 2β-decay. Two-vacua RPA.
doi: 10.1016/0375-9474(94)00795-O
1993KU12 Nucl.Phys. A556, 396 (1993) NN Interaction in a Relativistic Harmonic Model with Confined Gluons NUCLEAR REACTIONS 1n, 1H(p, p), E=50-400 MeV; calculated σ(θ). Relativistic harmonic model of NN- interaction, confined gluons.
doi: 10.1016/0375-9474(93)90368-8
1993RA03 Phys.Rev. C47, 1990 (1993) A.K.Rath, C.R.Praharaj, S.B.Khadkikar Signature Effects in Some N = 90 Odd-Z Rare-Earth Nuclei NUCLEAR STRUCTURE 147La, 149Pr, 151Pm; calculated levels, Eγ, B(λ), band structure deduced signature inversion features. Axially symmetric deformed configuration mixing, angular momentum projection.
doi: 10.1103/PhysRevC.47.1990
1991SU07 Nucl.Phys. A529, 727 (1991) J.Suhonen, S.B.Khadkikar, A.Faessler Calculation of the Neutrinoless ββ Decay of 76Ge Using a Quark Model with Harmonic Confinement RADIOACTIVITY 76Ge(2β); calculated neutrinoless double β-decay T1/2. Relativistic quark confinement model.
doi: 10.1016/0375-9474(91)90595-W
1991SU14 Nucl.Phys. A535, 509 (1991) J.Suhonen, S.B.Khadkikar, A.Faessler The Neutrinoless Double Beta Decay of 76Ge, 82Se, 86Kr, 114Cd, 128,130Te and 134,136Xe in the Framework of a Relativistic Quark Confinement Model RADIOACTIVITY 76Ge, 82Se, 86Kr, 114Cd, 128,130Te, 134,136Xe(2β); calculated 0ν-decay T1/2; deduced effective ν-mass upper limit. Relativistic quark confinement model.
doi: 10.1016/0375-9474(91)90474-K
1990SU03 Phys.Lett. 237B, 8 (1990) J.Suhonen, S.B.Khadkikar, A.Faessler Confined Quarks and the Neutrinoless ββ Decay RADIOACTIVITY 76Ge, 76Se(2β); calculated zero-ν-decay T1/2. Relativistic quark confinement model.
doi: 10.1016/0370-2693(90)90451-B
1989VE04 Nucl.Phys. A492, 654 (1989) J.D.Vergados, S.B.Khadkikar, A.Faessler Non-Static Contributions to the 0+ → 0+ ββ-Decay in the Presence of the Δ((3/2), (3/2)) Resonance NUCLEAR STRUCTURE 48Ca(2β); calculated nonstatic contribution to two β-decay in presence of Δ resonance.
doi: 10.1016/0375-9474(89)90113-9
1983FA08 Nucl.Phys. A401, 157 (1983) A.Faessler, L.Rikus, S.B.Khadkikar The Heavy-Ion Potential and Its Increasing Transparency at Intermediate Energies NUCLEAR REACTIONS 16O(16O, 16O), (16O, X), E(cm)=2.6-93.4 MeV/nucleon; calculated real part of interaction potential, reaction σ(E). 16O(16O, 16O), E=80 MeV; 16O(16O, 16O), E(cm)=23.3, 41.5, 93.4 MeV/nucleon; calculated σ(θ). 12C(12C, 12C), E=1016 MeV; calculated σ(θ). 12C(12C, X), E(cm) ≈ 2-100 MeV/nucleon; calculated total reaction σ(E). Bethe-Goldstone equation, complex reaction matrix.
doi: 10.1016/0375-9474(83)90342-1
1983PR02 Phys.Rev.Lett. 50, 1254 (1983) Rotation-Alignment Effect in 198Hg in an Angular-Momentum-Projected Band-Mixing Calculation NUCLEAR STRUCTURE 198Hg; calculated levels. Angular momentum projection, band mixing, rotation alignment effect.
doi: 10.1103/PhysRevLett.50.1254
1981KH03 Nucl.Phys. A369, 495 (1981) S.B.Khadkikar, L.Rikus, A.Faessler, R.Sartor Surface and Volume Contributions to Real and Imaginary Parts of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 16O(16O, 16O), E=80, 332 MeV; calculated σ(θ). Feshbach projection technique, heavy-ion optical potential.
doi: 10.1016/0375-9474(81)90034-8
1981SA12 Nucl.Phys. A359, 467 (1981) R.Sartor, A.Faessler, S.B.Khadkikar, S.Krewald Folding Computation of the 16O + 16O Optical Potential with a Complex Effective Force NUCLEAR REACTIONS 16O(16O, 16O), E=0, 83, 332 MeV; calculated real, imaginary optical potential terms. Folding method, complex effective force.
doi: 10.1016/0375-9474(81)90250-5
1980PR01 J.Phys.(London) G6, 241 (1980) Shapes of Mercury Nuclei and Structure of Lowest Bands in 188Hg NUCLEAR STRUCTURE 184,186,188,190,192,194,196,198,200,202,204,187,185Hg; calculated n, p Fermi energies, intrinsic quadrupole moments. 188Hg deduced band structure. Hartree-Fock calculation, surface delta interaction, angular momentum projection.
doi: 10.1088/0305-4616/6/2/014
1979KA40 Pramana(India) 13, 475 (1979) Spectroscopy of Light Nuclei with Skyrme-type Interactions NUCLEAR STRUCTURE 8Be, 12C, 16O, 20Ne; calculated levels, electromagnetic properties. Density-dependent Hartree-Fock, Skyrme interaction.
doi: 10.1007/BF02845875
1976KH04 Phys.Lett. 64B, 131 (1976) Nuclear Spectroscopy with a Density Dependent Interaction NUCLEAR STRUCTURE 12C, 8Be; calculated levels.
doi: 10.1016/0370-2693(76)90312-9
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
1975KA29 Phys.Lett. 59B, 19 (1975) Structure of 12C with Density Independent Skyrme Interaction NUCLEAR STRUCTURE 12C; calculated levels, B(E2), quadrupole moment.
doi: 10.1016/0370-2693(75)90144-6
1974KH01 Nucl.Phys. A225, 352 (1974) Centre of Mass Motion and Single Particle Separation Energies in Hartree-Fock Theory NUCLEAR STRUCTURE 16O; calculated S(n), S(p).
doi: 10.1016/0375-9474(74)90545-4
1974KH03 Phys.Rev. C10, 1189 (1974) Generator-Coordinate Spectra of 4n Nuclei in d-s Shell NUCLEAR STRUCTURE 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated levels, J, quadrupole moment, B(E2). Generator coordinate method; constrained Hartree-Fock.
doi: 10.1103/PhysRevC.10.1189
1974KH07 Pramana 2, 259 (1974) S.B.Khadkikar, D.R.Kulkarni, S.P.Pandya Shape Mixing as an Approximation to Shell Model 24Ne NUCLEAR STRUCTURE 24Ne; calculated levels, B(E2).
doi: 10.1007/BF02847082
1973BA12 Phys.Rev. C7, 1010 (1973) B.Banerjee, S.B.Khadkikar, K.R.Sandhya Devi Hartree-Fock-Bogoliubov Projected Spectra; Cr and Fe Isotopes NUCLEAR STRUCTURE 48,50,52,54Cr, 54,56,58Fe calculated levels, neutron, proton pairing energy gaps.
doi: 10.1103/PhysRevC.7.1010
1972KH08 Phys.Rev. C6, 866 (1972) Generator-Coordinate Spectrum of 20Ne NUCLEAR STRUCTURE 20Ne; calculated T=0 levels. Generator coordinate method, constrained Hartree-Fock projection.
doi: 10.1103/PhysRevC.6.866
1971GU08 Phys.Rev. C3, 1936 (1971) M.R.Gunye, C.S.Warke, S.B.Khadkikar Two-Particle-Two-Hole Excitations and Intrinsic Shapes of Deformed Nuclei NUCLEAR STRUCTURE 24Mg, 20Ne, 28Si; calculated levels. Hartree-Fock method, 2p-2h contributions.
doi: 10.1103/PhysRevC.3.1936
1971GU09 Nucl.Phys. A165, 508 (1971) Electromagnetic Properties of the First Excited States of 58,60,62Ni NUCLEAR STRUCTURE 58,60,62Ni levels calculated μ, quadrupole moment. Hartree-Fock-Bogoliubov wave functions.
doi: 10.1016/0375-9474(71)90465-9
1971GU21 Phys.Rev. C4, 1073 (1971) Nuclear-Structure Calculations in 18F NUCLEAR STRUCTURE 18F; calculated levels, quadrupole moment, rms radius, T1/2. Hartree-Fock projection.
doi: 10.1103/PhysRevC.4.1073
1971KH06 Phys.Lett. 36B, 451 (1971) Alpha Clustering in Light Nuclei with a Skyrme Interaction NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne; calculated binding energy for different α-cluster configurations Skyrme interactions.
doi: 10.1016/0370-2693(71)90526-0
1971KH08 Phys.Lett. 36B, 290 (1971) S.B.Khadkikar, S.C.K.Nair, S.P.Pandya Shape Mixing in 24Ne NUCLEAR STRUCTURE 22,24Ne; calculated levels. Projected Hartree-Fock calculation, mixing of nearly degenerate prolate, oblate solutions.
doi: 10.1016/0370-2693(71)90705-2
1970KH01 Nucl.Phys. A144, 289 (1970) Hartree-Fock-Bogolyubov Calculations with a Realistic Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 12,14C, 22Ne, 24Mg, 28Si, 44,46,48,50Ti, 50,52,54Cr, 54,56,58Fe, 58,60,62,64Ni; calculated binding energies, rms radii, quadrupole moment, levels, inertial parameters. Hartree-Fock-Bogolyubov formalism.
doi: 10.1016/0375-9474(70)90361-1
1970RA04 Nucl.Phys. A142, 81 (1970) S.Radhakant, S.B.Khadkikar, B.Banerjee Note on the Charge Form Factor of 4He NUCLEAR STRUCTURE 4He; calculated binding energy, charge form factor.
doi: 10.1016/0375-9474(70)90476-8
1970SA10 Phys.Lett. 32B, 179 (1970) K.R.Sandhya Devi, S.B.Khadkikar, J.K.Parikh, B.Banerjee Projected Hartree-Fock-Bogolubov Calculation for Ti Isotopes NUCLEAR STRUCTURE 46,48,50Ti; calculated levels. Deformed Hartree-Fock-Bogolubov formalism.
doi: 10.1016/0370-2693(70)90466-1
1969GU11 Phys.Letters 30B, 609 (1969) Pairing Correlations in Nickel Isotopes NUCLEAR STRUCTURE 60,62Ni; calculated levels. Hartree-Fock-Bogoliubov formalism.
doi: 10.1016/0370-2693(69)90070-7
1969KH03 Nucl.Phys. A129, 220 (1969) Projected Hartree-Fock Method and Stretch Scheme-Energy Levels of 44Ti NUCLEAR STRUCTURE 44Ti; calculated levels.
doi: 10.1016/0375-9474(69)90923-3
1968KH02 Nucl.Phys. A110, 472 (1968) Projected Hartree-Fock Spectra in 1f-2p shell Nuclei
doi: 10.1016/0375-9474(68)90554-X
1966GU06 Nucl.Phys. 86, 449 (1966) K.K.Gupta, S.B.Khadkikar, J.C.Parikh A Method to Treat Configuration Mixing Across Major Shells NUCLEAR STRUCTURE 16O, 8Be; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90552-9
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