NSR Query Results
Output year order : Descending NSR database version of May 21, 2024. Search: Author = Y.Waghmare Found 30 matches. 1989BH06 Pramana 32, L841 (1989) J.K.Bhattacharjee, L.Satpathy, Y.R.Waghmare A Possible Mechanism of Cold Fusion NUCLEAR REACTIONS 2H(d, n), E=low; analyzed cold fusion; deduced possible mechanism.
doi: 10.1007/BF02846004
1989GO16 Pramana 32, 435 (1989) Heavy-Ion Fusion in Classical and Semiclassical Microscopic Approaches NUCLEAR REACTIONS 16O(16O, X), E(cm) ≈ 12-50 MeV; 40Ca(40Ca, X), E(cm) ≈ 50-250 MeV; calculated fusion σ(E). Semi-classical microscopic approach.
doi: 10.1007/BF02845975
1987GO19 Pramana 28, 41 (1987) Heavy-Ion Fusion Cross-Section Calculations in Classical Microscopic Equations of Motion Approach NUCLEAR REACTIONS 16O(16O, γ), E(cm)=14-100 MeV; calculated fusion σ(E). Classical microscopic equations.
doi: 10.1007/BF02846806
1987GO30 Phys.Rev. C36, 1632 (1987) Classical Microscopic Calculations of 16O + 16O and 40Ca + 40Ca Fusion Cross Sections NUCLEAR REACTIONS, ICPND 16O(16O, X), E(cm) ≈ 12-100 MeV; 40Ca(40Ca, X), E(cm) ≈ 62-250 MeV; calculated fusion σ(E). Classical microscopic approach.
doi: 10.1103/PhysRevC.36.1632
1984MA33 Pramana 22, 257 (1984) A Study of Pion Absorption by 16O using Realistic Interactions - I. Two Nucleon Emission following Bound-Pion Absorption NUCLEAR REACTIONS 16O(π-, 2n), (π-, np), E at rest; calculated pion absorption rate. Hartree-Fock basis, antisymmetrization.
doi: 10.1007/BF02846378
1984MA63 Pramana 22, 457 (1984) Pion Absorption by 16O using Realistic Interactions - II: Free pion absorption followed by emission of proton NUCLEAR REACTIONS 16O(π+, p), E=70 MeV; calculated σ(θ) following pion absorption; deduced pion optical potential parameters. Klein-Gordon equation approach.
doi: 10.1007/BF02847113
1984SR05 Pramana 22, 513 (1984) V.N.Sridhar, R.Parthasarathy, Y.R.Waghmare Muon Capture by 16O - using a Microscopic Theory of Particle-Hole States NUCLEAR REACTIONS 16O(μ-, ν), E at rest; calculated partial capture rates; deduced meson exchange effects role. Landau-Migdal theory.
doi: 10.1007/BF02846401
1983DI15 Pramana 20, 523 (1983) A.N.Dixit, V.S.Ramamurthy, Y.R.Waghmare Classical Description of Low Energy 16O + 16O Collisions NUCLEAR REACTIONS, ICPND 16O(16O, X), E(cm)=16.64-66.56 MeV; calculated fusion σ(E); deduced classical approximation limitations. Lennard-Jones potential, classical microscopic description.
doi: 10.1007/BF02846287
1980MU01 Z.Phys. A294, 87 (1980) H.Muther, Y.R.Waghmare, A.Faessler Brueckner Random Phase Approximation, a Microscopic Description of Particle-Hole States NUCLEAR STRUCTURE 16O; calculated collective 3-, giant multipole states, B(λ). Brueckner RPA.
1979PA19 Pramana(India) 13, 457 (1979) Effect of Correlations on Nuclear Muon Capture NUCLEAR REACTIONS 12C(μ-, ν), E at rest; calculated partial, total capture rates, recoil polarization; deduced pseudoscalar, tensor coupling constants. Unitary model operator.
doi: 10.1007/BF02845874
1978BH01 Nucl.Phys. A298, 367 (1978) Bound-Pion Absorption Followed by Emission of Two Nucleons NUCLEAR REACTIONS 12C(π-, np), (π-, 2n); calculated σ(θ).
doi: 10.1016/0375-9474(78)90139-2
1976MU08 Phys.Lett. 64B, 125 (1976) H.Muther, Y.R.Waghmare, A.Faessler Structure of the Giant Resonances in 16O Using Brueckner-Random-Phase Approximation NUCLEAR STRUCTURE 16O; calculated giant resonances, B(λ). Self-consistent Brueckner-Hartree-Fock.
doi: 10.1016/0370-2693(76)90310-5
1976PR07 Z.Phys. A278, 155 (1976) M.Prakash, Y.R.Waghmare, I.Mehrotra Phenomenological Renormalization of Free Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 6Li, 18F, 18O, 42Sc, 42Ca, 58Ni, 92Zr; calculated levels.
doi: 10.1007/BF01437770
1975BH03 Pramana 5, 154 (1975) (π+, p) Reaction in 12C NUCLEAR REACTIONS 12C(π+, p); calculated σ(θ). Hartree-Fock.
doi: 10.1007/BF02875185
1975PR10 Pramana 5, 239 (1975) Phenomenological Effective Interaction for 40K NUCLEAR STRUCTURE 38Cl, 40K; calculated levels.
doi: 10.1007/BF02845947
1973JO03 Phys.Rev. C7, 874 (1973) Effective Interaction in Nuclei NUCLEAR STRUCTURE 18F calculated levels using Sussex interaction.
doi: 10.1103/PhysRevC.7.874
1973SI25 Phys.Lett. 45B, 199 (1973) R.Singh, G.K.Mehta, Y.R.Waghmare A Study of Configuration Mixing in Vibrational Nuclei NUCLEAR STRUCTURE 44Ca, 64,66Zn, 74Ge, 76,78,80Se, 84Sr, 100,104Ru, 106,108,110Pd, 110,112,114,116Cd, 122,124Te, 134Ba, 150Sm, 152Gd, 200Hg; calculated B(E2), quadrupole moment.
doi: 10.1016/0370-2693(73)90181-0
1972HA65 Phys.Lett. 41B, 264 (1972) Talmi Integrals and Effective Interaction
doi: 10.1016/0370-2693(72)90574-6
1972WA01 Phys.Lett. 38B, 13 (1972) Effective Interaction and Isospin Splitting
doi: 10.1016/0370-2693(72)90187-6
1971JA06 Phys.Rev. C3, 1466 (1971) M.C.Jain, G.K.Mehta, Y.R.Waghmare Effective Interaction and Level Structure of Nuclei with Free Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 6He, 6Li, 18O, 18F, 58Ni; calculated levels, effective interactions.
doi: 10.1103/PhysRevC.3.1466
1971KA14 Can.J.Phys. 49, 1874 (1971) On Spherical Hartree-Fock Calculations with Sussex Interaction NUCLEAR STRUCTURE 4He, 12C, 16O; calculated binding energies, radii, single-particle energies. Spherical Hartree-Fock method, Sussex interaction.
doi: 10.1139/p71-226
1970JA07 J.Phys. A3, 274 (1970) Nuclear Energy Gap Calculations Using Realistic and Delta-Function Forces NUCLEAR STRUCTURE 16,18,20O, 34,36,38S, 42,44,46Ca, 60,62,64,66Ni, 92,94,96Zr; calculated energy gap parameters. Realistic, delta-function forces.
doi: 10.1088/0305-4470/3/3/013
1970KA30 Phys.Rev. C2, 1191 (1970) Relative Strengths of Central, Spin-Orbit, and Tensor Parts of the Sussex Interaction NUCLEAR STRUCTURE 12C, 16O; calculated binding energy, radii, single-particle energies. Sussex interaction.
doi: 10.1103/PhysRevC.2.1191
1970KA32 Nucl.Phys. A156, 199 (1970) I.Kakkar, G.K.Mehta, Y.R.Waghmare Configuration Mixing Calculations in the Hartree-Fock Representation NUCLEAR STRUCTURE 10Be, 18F, 18O; calculated levels. Shell model, Hartree-Fock basis.
doi: 10.1016/0375-9474(70)91126-7
1969JA16 Phys.Rev. 188, 1568 (1969) Strength of the Pairing Force and Energy Gap in Finite Nuclei NUCLEAR STRUCTURE 60,62,64,66Ni, 92,94,96Zr; calculated pairing energies.
doi: 10.1103/PhysRev.188.1568
1969MU09 Nucl.Phys. A137, 579 (1969) Isobaric Analogue States in Nuclei of Mass 18 and 19 NUCLEAR STRUCTURE 18F, 18O, 18Ne, 19O, 19F, 19Ne, 19Na; calculated isobaric level shifts. Charge-dependent n-n potential.
doi: 10.1016/0375-9474(69)90094-3
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
1964WA20 Progr.Theoret.Phys.(Kyoto) 31, 765 (1964) Y.Waghmare, R.K.Gupta, N.Kumar S-State Interactions in Effective Two-Body Forces NUCLEAR STRUCTURE 58Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1143/PTP.31.765
1963SO04 Nucl.Phys. 46, 181 (1963) Nucleon-Nucleon Potential from Shell Model Calculations for Doublet Splittings NUCLEAR STRUCTURE 206Tl, 16N, 90Nb, 90Y, 91Nb, 88Y, 32S; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90578-9
1962WA29 Physica 28, 957 (1962) Energy Levels of 92Zr and 93Zr NUCLEAR STRUCTURE 93Zr, 92Zr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-8914(62)90082-4
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