NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.S.Warke Found 35 matches. 1999GA57 Pramana 53, 279 (1999) Nuclear Magnetic Moment: Relativistic mean field description NUCLEAR MOMENTS 15N, 15,17O, 17,19F, 39K, 39,41Ca, 41Sc, 49Ti, 53Cr, 53Mn, 61,63Ni, 71Ga, 85Kr, 85Rb, 87Sr, 89Y, 91Zr, 93Nb, 107In, 111,115Sn, 133Cs, 131,133Ba, 133La, 141Pr, 135Nd, 205,207Pb, 209Bi; calculated μ. 11B, 11,13C, 13,15N, 15,17O, 17F, 27Al, 27Si, 39K, 39,41Ca, 41Sc; calculated isoscalar μ. Relativistic mean field approach, comparisons with previous calculations and with data.
doi: 10.1007/s12043-999-0128-2
1998GA41 Eur.Phys.J. A 3, 255 (1998) Y.K.Gambhir, J.P.Maharana, C.S.Warke Pseudo-Spin as a Relativistic Symmetry NUCLEAR STRUCTURE 208Pb; calculated single-particle levels, radii, spin-orbit splitting; deduced possible broken pseudospin symmetry. Relativistic mean field approach.
doi: 10.1007/s100500050175
1998KU05 Phys.Rev. C57, 1485 (1998) S.Kulkarni, C.S.Warke, Y.K.Gambhir Relativistic Mean Field Calculation of Parity-Violating Observables in Francium NUCLEAR STRUCTURE 133,134Cs, 209,210Fr, 209Rn, 133Xe; calculated binding energy, radii, hyperfine transition amplitudes, parity-violating observables. Relativistic mean field.
doi: 10.1103/PhysRevC.57.1485
1998LA13 Phys.Rev. C58, R45 (1998) G.A.Lalazissis, Y.K.Gambhir, J.P.Maharana, C.S.Warke, P.Ring Relativistic Mean Field Approach and the Pseudospin Symmetry NUCLEAR STRUCTURE 154Dy, 208Pb; calculated single-particle levels; deduced quasidegenerate pseudospin doublets. Spherical, deformed relativistic mean field.
doi: 10.1103/PhysRevC.58.R45
1995KU24 Phys.Rev. C52, 1047 (1995) S.Kulkarni, C.S.Warke, Y.K.Gambhir Relativistic Mean-Field Approach to Anapole Moment: Atomic parity-violating hyperfine transitions NUCLEAR STRUCTURE 85Rb, 133Cs, 209Bi; calculated binding energy, point nucleon, charge radii, μ. 125,127,129,131,133,135,137,139Cs; calculated proton mean square radii. 133Cs; calculated hyperfine amplitudes. Relativistic mean field approach.
doi: 10.1103/PhysRevC.52.1047
1994KU26 Nucl.Phys. A577, 457c (1994) S.Kulkarni, C.S.Warke, Y.K.Gambhir Nuclear Parity Violating Effects: Anapole Moment NUCLEAR STRUCTURE 85Rb, 133Cs, 203,205Tl, 207Pb, 209Bi; calculated binding energy, nucleon point radii, rms radii. 209Bi; calculated charge density. 133Cs; calculated anapole moment. Relativistic mean field approach.
doi: 10.1016/0375-9474(94)90896-6
1989WA23 Pramana 32, 541 (1989) Electric and Magnetic Polarizabilities of Nucleon and QCD Quark Models NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic polarizabilities. Chiral bag models.
doi: 10.1007/BF02845984
1986BH09 Phys.Rev. C34, 1920 (1986); Erratum Phys.Rev. C36, 467 (1987) ' Exact ' Relativistic Theory of Two-Body Bound-State Wave Functions NUCLEAR STRUCTURE 2H; analyzed wave functions. Exact Bethe-Salpeter equation, relativistic approach.
doi: 10.1103/PhysRevC.34.1920
1984MO31 Pramana 23, 165 (1984) S.V.Moholkar, C.S.Warke, M.R.Gunye Side-Bands in 170Yb NUCLEAR STRUCTURE 170Yb; calculated levels, band structure. Microscopic method, number conservation, variation after angular momentum projection.
doi: 10.1007/BF02846513
1983MO05 J.Phys.(London) G9, 535 (1983) S.V.Moholkar, C.S.Warke, M.R.Gunye Microscopic Calculations in Odd-Odd Nuclei NUCLEAR STRUCTURE 168Tm, 170Yb; calculated levels. Microscopic model, variation after angular momentum projection.
doi: 10.1088/0305-4616/9/5/006
1983WA14 J.Phys.(London) G9, L159 (1983) An Explicit Spin-Dependence of the Nucleon Partial Decay Amplitudes NUCLEAR STRUCTURE 1H; calculated partial decay amplitude, width, T1/2. Quark correlation, spin flavor SU(6) symmetry breaking effects.
doi: 10.1088/0305-4616/9/8/003
1982MO08 J.Phys.(London) G8, 699 (1982) S.V.Moholkar, C.S.Warke, M.R.Gunye Microscopic Calculations in Odd-A Nuclei NUCLEAR STRUCTURE 153,154Gd, 153Eu; calculated levels, yrast band; deduced i13/2 neutron pair role. Microscopic model, number conservation, variation after projection.
doi: 10.1088/0305-4616/8/5/011
1981HA34 J.Phys.(London) G7, 1501 (1981) Optical-Model Dependence of Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 26Mg(11B, 10B), (11B, 10Be), E=114 MeV; 24Mg(16O, 12C), E=48, 56 MeV; 40Ca(12C, 8Be), E=45 MeV; calculated σ(θ), transfer amplitudes; deduced optical model parameter dependence.
doi: 10.1088/0305-4616/7/11/009
1981MO26 Pramana 17, 369 (1981) S.V.Moholkar, C.S.Warke, M.R.Gunye Microscopic Study of Odd-A Nuclei NUCLEAR STRUCTURE 155Dy, 155Tb; calculated levels. Microscopic method, variation after projection.
doi: 10.1007/BF02847202
1981WA01 J.Phys.(London) G7, L1 (1981) C.S.Warke, R.Shanker, W.Greiner Isobaric Component of the Deuteron as Determined from the De Rujula-Georgi-Glashow Quark Model NUCLEAR STRUCTURE 2H; calculated isobaric spectroscopic factor. Correlated baryon cluster wave function, De Rujula-Georgi-Glashow quark model.
doi: 10.1088/0305-4616/7/1/004
1980DA15 Phys.Rev. C22, 1787 (1980) V.M.Datar, C.V.K.Baba, S.N.Acharya, S.A.Chitambar, H.C.Jain, S.K.Bhattacherjee, C.S.Warke Radial Quantum Number Selection Rule in the Beta-Decay of 209Tl RADIOACTIVITY 209Tl; measured β-branching ratio. 209Pb level deduced neutron, proton radius equality. Shell model.
doi: 10.1103/PhysRevC.22.1787
1980MO29 Pramana 15, 449 (1980) S.V.Moholkar, C.S.Warke, M.R.Gunye Microscopic Band-Mixing Calculations in 154,156Gd NUCLEAR STRUCTURE 154,156Gd; calculated yrast, excited band levels, B(E2). Microscopic band mixing formalism, number conservation, angular momentum projection.
doi: 10.1007/BF02847883
1979GU05 J.Phys.(London) G5, L83 (1979) Effect of Number Conservation on Energy Spectra of 158,160Er NUCLEAR STRUCTURE 158,160Er; calculated enegy levels, B(E2) in variational projected, number-conserving BCS formalism.
doi: 10.1088/0305-4616/5/4/008
1979GU11 Phys.Rev. C20, 372 (1979) Effect of Number Conservation on High Spoin States and Nuclear Deformation NUCLEAR STRUCTURE 158,160,162Er; calculated energy spectra, quadrupole moments, B(E2). Microscopic Hamiltonian, quadrupole plus pairing interactions, number conservation, variation after projection.
doi: 10.1103/PhysRevC.20.372
1979HA13 Nucl.Phys. A318, 523 (1979) Semiclassical Analysis of α-Transfer Reactions NUCLEAR REACTIONS 208Pb(16O, 12C), E=93 MeV; 40Ca(12C, 8Be), E=45 MeV; calculated σ(θ). Semiclassical, one step DWBA treatment of α-transfer.
doi: 10.1016/0375-9474(79)90665-1
1976WA01 Phys.Rev. C13, 859 (1976) Theoretical Investigations of the Yrast States of Even Erbium Isotopes NUCLEAR STRUCTURE 156,158,160,162Er, 156Dy; calculated levels, B(E2).
doi: 10.1103/PhysRevC.13.859
1975WA25 Phys.Rev. C12, 1647 (1975) High Spin States in Dy Isotopes from Many-Body Variational Approach NUCLEAR STRUCTURE 158,160,162,164Dy; calculated levels. 160,162,164Dy; calculated B(E2).
doi: 10.1103/PhysRevC.12.1647
1974WA15 J.Phys.(London) A7, 718 (1974) The Jastrow Cluster Expansion Method for Finite Nuclei NUCLEAR STRUCTURE 16O, 28Si, 32S, 40,48Ca, 56Ni, 72Ge, 88Sr, 90,96Zr, 120Sn, 140Ce, 146Gd, 208Pb; calculated binding energy per nucleon.
doi: 10.1088/0305-4470/7/6/008
1973RO01 Phys.Rev.Lett. 30, 55 (1973) Angular-Momentum Conservation in the Strutinsky Method
doi: 10.1103/PhysRevLett.30.55
1972GU05 Phys.Rev. C5, 1860 (1972) Electromagnetic Transitions from the Isobaric Analog States in 13C, 19F, and 31P NUCLEAR STRUCTURE 13C, 19F, 31P; analyzed isobaric analog state decay; calculated μ, quadrupole moment, transition strengths. 13B, 13N, 31Si; calculated μ, quadrupole moment. Hartree-Fock projection method.
doi: 10.1103/PhysRevC.5.1860
1972SI35 Can.J.Phys. 50, 2574 (1972) Y.Singh, C.S.Warke, R.K.Bhaduri Partly Nonlocal Potentials in Nuclear Matter
doi: 10.1139/p72-343
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
1971OS01 Phys.Lett. 34B, 113 (1971) Core-Renormalization of the pf-Shell Effective Interaction for an RPA-Description of the Core NUCLEAR STRUCTURE 40Ca; calculated core polarization contribution to effective interaction. RPA.
doi: 10.1016/0370-2693(71)90682-4
1971OS03 Nucl.Phys. A168, 190 (1971) Core Polarization of the Effective Two-Nucleon Interaction for Different Descriptions of the Core NUCLEAR STRUCTURE 16O; calculated levels. Core polarization effects.
doi: 10.1016/0375-9474(71)90658-0
1970GU13 Phys.Rev. C2, 2106 (1970) Binding Energies of Finite Nuclei in the Oscillator Model NUCLEAR STRUCTURE 14C, 16O, 28Si, 40,48Ca, 56Ni; calculated nuclear radii, binding energy.
doi: 10.1103/PhysRevC.2.2106
1970OS01 Nucl.Phys. A154, 331 (1970) Nuclear Structure Information from Isovector Electromagnetic Transitions in 51V NUCLEAR STRUCTURE 51V; calculated levels, B(E2), μ.
doi: 10.1016/0375-9474(70)90161-2
1969OS01 Phys.Letters 30B, 306 (1969) On the Renormalization of the Effective Two-Nucleon Interaction by Core-Polarization Processes NUCLEAR STRUCTURE 18O, 18F; calculated levels. Random phase approximation, core polarization corrections.
doi: 10.1016/0370-2693(69)90487-0
1967GU05 Phys.Rev. 156, 1087 (1967) Projected Hartree-Fock Spectra of 2s-1d-Shell Nuclei
doi: 10.1103/PhysRev.156.1087
1967GU09 Phys.Rev. 164, 1264 (1967) Electron Scattering, ft Values, and Single-Particle Reduced Widths as Calculated from Projected Hartree-Fock Wave Functions
doi: 10.1103/PhysRev.164.1264
1964WA17 Phys.Rev. 135, B872 (1964) Shape Independence of Low-Lying States of Nuclei NUCLEAR STRUCTURE 58Ni, 206Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.135.B872
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