NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = D.M.Nadkarnee Found 43 matches. 1999KA14 Phys.Rev. C59, 2580 (1999) S.Kailas, D.M.Nadkarni, A.Chatterjee, A.Saxena, S.S.Kapoor, R.Vandenbosch, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, J.D.Bierman Fission Fragment Folding Angle Distributions for the Systems 11B + 237Np, 12C + 236U, and 16O + 232Th in the Energy Range 1.1 < E/VB < 2.1 NUCLEAR REACTIONS 232Th(16O, F), E=100-144.8 MeV; 236U(12C, F), E=80-130 MeV; 237Np(11B, F), E=60-118 MeV; measured fission σ, folding angle distributions; deduced momentum transfer components, fission anisotropies. Saddle-point statistical model.
doi: 10.1103/PhysRevC.59.2580
1999NA03 Phys.Rev. C59, R580 (1999) D.M.Nadkarni, A.Saxena, D.C.Biswas, R.K.Choudhury, S.S.Kapoor, N.Majumdar, P.Bhattacharya Measurement of Fission Excitation Functions in 11B, 16O, 19F + 232Th Reactions in the Extreme Sub-Barrier Energy Region NUCLEAR REACTIONS 232Th(11B, F), E=19-65 MeV; 232Th(16O, F), (19F, F), E=55-80 MeV; measured fission fragments folding angle distributions, fusion and transfer induced fission σ; deduced fusion barrier distributions, low-momentum transfer fission component.
doi: 10.1103/PhysRevC.59.R580
1999SH42 Phys.Rev. C60, 061601 (1999) D.V.Shetty, R.K.Choudhury, B.K.Nayak, D.M.Nadkarni, S.S.Kapoor Suppression of Collective Spin Excitations for High-K States in Heavy Ion Induced Fission Reactions NUCLEAR REACTIONS 209Bi(12C, F), E=71-85 MeV; 209Bi(16O, F), E=89-98 MeV; 209Bi(19F, F), E=97-111 MeV; measured fission fragments spin vs emission angle; 232Th(12C, F), (16O, F), (19F, F), E not given; analyzed fission fragments spin vs emission angle; deduced suppression of collective spin for high-K states.
doi: 10.1103/PhysRevC.60.061601
1999SH46 Pramana 53, 521 (1999) D.V.Shetty, R.K.Choudhury, B.K.Nayak, D.M.Nadkarni, S.S.Kapoor Some Aspects of Heavy Ion Fusion-Fission Dynamics NUCLEAR REACTIONS 209Bi, 232Th(12C, F), (16O, F), (19F, F), E ≈ barrier; measured Eγ, Iγ, fragments angular distribution following fission; deduced fission fragments spin vs bombarding energy and emission angle.
doi: 10.1007/s12043-999-0024-9
1998MA75 Phys.Rev.Lett. 81, 4778 (1998) N.Majumdar, P.Bhattacharya, D.C.Biswas, R.K.Choudhury, D.M.Nadkarni, A.Saxena Majumdar et al. Reply: (Comment on ' Anomalous Peaklike Structure in the Fission Fragment Anisotropies at Sub-Barrier Energies in 11B, 12C, 16O, 19F + 232Th Reactions ')
doi: 10.1103/PhysRevLett.81.4778
1998SH19 Phys.Rev. C58, R616 (1998) D.V.Shetty, R.K.Choudhury, B.K.Nayak, D.M.Nadkarni, S.S.Kapoor Emission Angle Dependence of Fission Fragment Spin in 12C, 16O, and 19F + 232Th Reactions NUCLEAR REACTIONS 232Th(12C, F), E=60-90 MeV; 232Th(16O, F), E=85-100 MeV; 232Th(19F, F), E=105-113 MeV; measured γ-ray multiplicity following fission, (fragment)γ-coin; deduced average fragment spins vs emission angle, fragments collective excitation modes. Statistical model analysis.
doi: 10.1103/PhysRevC.58.R616
1998VA11 Phys.Rev. C57, 3462 (1998) R.Varma, S.Sinha, B.K.Nayak, R.G.Thomas, A.Saxena, D.C.Biswas, L.M.Pant, D.M.Nadkarni, R.K.Choudhury, P.Bhattacharya Fusion Barrier and Spin Distributions in 12C + 232Th Reaction Via Quasielastic Scattering NUCLEAR REACTIONS 232Th(12C, X), E=51-79 MeV; measured quasielastic σ(E, θ); deduced fusion barrier, spin distributions. Model comparisons.
doi: 10.1103/PhysRevC.57.3462
1997BI08 Phys.Rev. C56, 1926 (1997) D.C.Biswas, R.K.Choudhury, B.K.Nayak, D.M.Nadkarni, V.S.Ramamurthy Single and Multinucleon Transfer in 19F, 16O, 12C + 232Th Reactions at Near Barrier Energies NUCLEAR REACTIONS 232Th(19F, X), E=92-114 MeV; 232Th(16O, X), E=86.6, 94.8 MeV; 232Th(12C, X), E=59-82 MeV; measured projectile-like fragment σ(E, Z), σ(θ) for quasielastic, transfer reactions; deduced model parameters, transfer probabilities, Q-value dependence. Semiclassical model.
doi: 10.1103/PhysRevC.56.1926
1997NA10 Phys.Rev. C55, 2951 (1997) B.K.Nayak, R.K.Choudhury, D.C.Biswas, L.M.Pant, A.Saxena, D.M.Nadkarni, S.S.Kapoor Studies of One- and Two-Proton Transfer in 12C, 16O + 154Sm, and 16O + 115In Reactions NUCLEAR REACTIONS 154Sm(16O, X), E=100 MeV; 154Sm(12C, X), E=86 MeV; 115In(16O, X), E=90 MeV; measured σ(θ), spectra for 1p, 2p transfer channels; deduced transfer probabilities. Binding energies from semiclassical model, slope anomaly.
doi: 10.1103/PhysRevC.55.2951
1997SH22 Phys.Rev. C56, 868 (1997) D.V.Shetty, R.K.Choudhury, B.K.Nayak, D.M.Nadkarni, S.S.Kapoor Investigation of Fusion l Distributions at Near and Sub-Barrier Energies Through Fission Fragment γ Ray Multiplicity Measurements NUCLEAR REACTIONS 232Th(12C, F), E=60-86 MeV; 232Th(16O, F), E=84-100 MeV; measured fission fragment γ multiplicity vs E(beam); deduced fission fragment, compound nucleus spin distributions, nonequilibrium processes at sub-barrier energies.
doi: 10.1103/PhysRevC.56.868
1996MA03 Phys.Rev. C53, R544 (1996) N.Majumdar, P.Bhattacharya, D.C.Biswas, R.K.Choudhury, D.M.Nadkarni, A.Saxena Reexamination of the Nuclear Orientation Model of Quasifission Reactions to Explain Anomalous Fragment Anisotropies at Sub-Barrier Energies NUCLEAR REACTIONS 232Th(19F, F), E=84.5-106.5 MeV; 232Th(16O, F), E=95-77 MeV; 232Th(12C, F), E=54-84 MeV; measured fission fragment σ(θ), fusion σ(E).
doi: 10.1103/PhysRevC.53.R544
1996MA61 Phys.Rev.Lett. 77, 5027 (1996) N.Majumdar, P.Bhattacharya, D.C.Biswas, R.K.Choudhury, D.M.Nadkarni, A.Saxena Anomalous Peaklike Structure in the Fission Fragment Anisotropies at Sub-Barrier Energies in 11B, 12C, 16O, 19F + 232Th Reactions NUCLEAR REACTIONS 232Th(19F, F), E=73.5-80 MeV; 232Th(16O, F), E=69.2-74.8 MeV; 232Th(11B, F), E=43-49.7 MeV; 232Th(12C, F), E(cm)=40-70 MeV; measured fission fragment σ(θ); deduced anomalous peaklike structure explanation possibility.
doi: 10.1103/PhysRevLett.77.5027
1996PA27 Phys.Rev. C54, 2037 (1996) L.M.Pant, A.Saxena, R.K.Choudhury, D.M.Nadkarni Mass Dependence of Fragment Anisotropy in the Fission of 11B + 237Np and 16O + 209Bi Systems NUCLEAR REACTIONS 237Np(11B, F), E=76 MeV; 209Bi(16O, F), E=100 MeV; measured fission fragment angular anisotropy, mass dependence, mass, energy correlations. Statistical model analysis.
doi: 10.1103/PhysRevC.54.2037
1996VA12 Phys.Rev. C54, R977 (1996) R.Vandenbosch, J.D.Bierman, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, S.Kailas, D.M.Nadkarni, S.S.Kapoor Disappearance of Entrance Channel Dependence of Fission Fragment Anisotropies at Well-Above-Barrier Energies NUCLEAR REACTIONS 237Np(11B, F), E=60-118 MeV; 236U(12C, F), E=80-130 MeV; 232Th(16O, F), E=100-145 MeV; measured fission fragment σ(θ), anisotropies; deduced entrance channel independence.
doi: 10.1103/PhysRevC.54.R977
1995BH08 Nuovo Cim. 108, 819 (1995) P.Bhattacharya, N.Majumdar, P.Basu, M.L.Chatterjee, D.C.Biswas, A.Saxena, V.S.Ambekar, R.K.Choudhury, D.M.Nadkarni Measurement of Complete Fusion-Fission and Transfer-Fission Cross-Sections and Angular Distributions for 19F + 232Th at Sub-Barrier Energies by Fission Fragment Folding-Angle Technique NUCLEAR REACTIONS, ICPND 232Th(19F, F), E=78.5-106.5 MeV; measured σ(fragment) vs θ(folding) for transfer-, fusion fission, σ(E).
1995BI21 Phys.Rev. C52, R2827 (1995) D.C.Biswas, R.K.Choudhury, D.M.Nadkarni, V.S.Ramamurthy Evidence of Massive Cluster Transfers in 19F + 232Th Reaction at Near Barrier Energies NUCLEAR REACTIONS 232Th(19F, X), E=113.6, 106.5 MeV; measured σ(fragment θ); deduced reduced transfer probability, Q-value dependence.
doi: 10.1103/PhysRevC.52.R2827
1995CH65 Pramana 44, 177 (1995) R.K.Choudhury, D.M.Nadkarni, V.S.Ambekar, B.V.Dinesh, A.Saxena, M.S.Samant, D.C.Biswas, L.M.Pant Deep Inelastic Collisions of 32S + 27Al Reaction at 130 MeV Bombarding Energy NUCLEAR REACTIONS 27Al(32S, X), E=130 MeV; measured fragment distribution for Z=6-10, average kinetic energy vs fragment Z; deduced highly stretched scission configurations.
doi: 10.1007/BF02847697
1995KA10 Z.Phys. A351, 195 (1995) A.Karnik, S.Kailas, A.Chatterjee, P.Singh, A.Navin, D.C.Biswas, D.M.Nadkarni, A.Shrivastava, S.S.Kapoor Near-Barrier Fission of the System 12C + 232Th NUCLEAR REACTIONS, ICPND 232Th(12C, F), E ≈ 60-82.5 MeV; measured fission fragment anisotropies, σ vs E; deduced channel coupling evidence. Saddle point statistical model.
doi: 10.1007/BF01289529
1995MA41 Phys.Rev. C51, 3109 (1995) N.Majumdar, P.Bhattacharya, D.C.Biswas, R.K.Choudhury, D.M.Nadkarni, A.Saxena Fission-Fragment Angular Distributions and Excitation Functions in Fission Following Complete Fusion and Targetlike-fragment Fission Reactions of 19F + 232Th at Near- and Sub-Barrier Energies NUCLEAR REACTIONS 232Th(19F, F), E=84.5-106.5 MeV; measured fission σ(E), σ(fragment θ). Coupled-channels analysis.
doi: 10.1103/PhysRevC.51.3109
1995NA21 Phys.Rev. C52, 3081 (1995) B.K.Nayak, R.K.Choudhury, L.M.Pant, D.M.Nadkarni, S.S.Kapoor Fusion l Distribution in 16O, 28Si + 115In Reactions at Near- and Sub-Barrier Energies NUCLEAR REACTIONS 115In(16O, X), E=55-80 MeV; 115In(28Si, X), E=105-115 MeV; measured Eα, γ-multiplicity distributions; deduced l-distribution moments. One-dimensional barrier penetration model.
doi: 10.1103/PhysRevC.52.3081
1995SA27 Phys.Rev. C51, 3127 (1995) M.S.Samant, R.P.Anand, R.K.Choudhury, S.S.Kapoor, D.M.Nadkarni Prescission Neutron Emission in 235U(n(th), f) Through Fragment-Neutron Angular Correlation Studies NUCLEAR REACTIONS 235U(n, F), E=thermal; measured prompt neutron energy spectra, σ(θ), (fragment)(n)(θ) following fission; deduced prescission neutron multiplicity.
doi: 10.1103/PhysRevC.51.3127
1994SA03 Phys.Rev. C49, 932 (1994) A.Saxena, A.Chatterjee, R.K.Choudhury, S.S.Kapoor, D.M.Nadkarni Entrance Channel Effects in the Fusion-Fission Time Scales from Studies of Prescission Neutron Multiplicities NUCLEAR REACTIONS 232Th(11B, F), E not given; 232Th(12C, F), E=86 MeV; 232Th(16O, F), E=104 MeV; 237Np(11B, F), E=77 MeV; measured neutron emission spectra, different angles; deduced pre-scission neutron multiplicities in fusion-fission reactions, fusion-fission time-scales, transient, saddle-to-scission, formation delays.
doi: 10.1103/PhysRevC.49.932
1993KA35 Pramana 41, 339 (1993) S.Kailas, A.Navin, A.Chatterjee, P.Singh, A.Saxena, D.M.Nadkarni, D.C.Biswas, R.K.Choudhury, S.S.Kapoor Sub-Barrier Fission Fragment Angular Distributions for the System 19F + 232Th NUCLEAR REACTIONS 232Th(19F, F), E=89.3-93.6 MeV; measured fission fragment σ(θ), anisotropy. Statistical model analysis.
doi: 10.1007/BF02847398
1993SA25 Pramana 40, 299 (1993) M.S.Samant, R.P.Anand, R.K.Choudhury, S.S.Kapoor, K.Kumar, D.M.Nadkarni, A.Saxena Prompt Neutron Emission Spectra and Multiplicities in the Thermal Neutron Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment neutron emission spectra, total kinetic energies, multiplicities.
doi: 10.1007/BF02845849
1991KA03 Phys.Rev. C43, 1466 (1991) S.Kailas, A.Navin, A.Chatterjee, P.Singh, R.K.Choudhury, A.Saxena, D.M.Nadkarni, S.S.Kapoor, V.S.Ramamurthy, B.K.Nayak, S.V.Suryanarayana Fission Fragment Angular Distributions for the System 19F + 232Th NUCLEAR REACTIONS 232Th(19F, F), E=94-108 MeV; measured fission fragment σ(θ), anisotropy; deduced entrance channel dependences. Saddle-point statistical model.
doi: 10.1103/PhysRevC.43.1466
1989AJ01 Phys.Rev. C40, R1854 (1989) N.N.Ajitanand, K.N.Iyengar, R.P.Anand, D.M.Nadkarni Alpha-Induced Fission of 235U at Extreme Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 235U(α, F), E=3-27 MeV; measured fission σ(E). Plastic track recorders.
doi: 10.1103/PhysRevC.40.R1854
1989SI26 Pramana 33, 85 (1989) A.K.Sinha, D.M.Nadkarni, G.K.Mehta Light-Charged Particle Emission in Fission
doi: 10.1007/BF02845910
1987AJ01 Phys.Rev.Lett. 58, 1520 (1987) N.N.Ajitanand, K.N.Iyengar, R.P.Anand, D.M.Nadkarni, A.K.Mohanty Anomalous behavior of the proton-induced fission cross sections of 235U and 238U at extreme sub-barrier energies NUCLEAR REACTIONS, ICPND 235,238U(p, F), E=0.5-4.3 MeV; measured fission σ(E). Enriched 235U, natural Uranium targets, solid state track detectors.
doi: 10.1103/PhysRevLett.58.1520
1987CH04 Nucl.Phys. A463, 597 (1987) R.K.Choudhury, A.Saxena, V.S.Ramamurthy, D.M.Nadkarni, S.S.Kapoor Variation of Kinetic Energy Distributions of Fission Fragments with Bombarding Energy in 4He Induced Fision of 238U at Medium Energies NUCLEAR REACTIONS, ICPND 238U(α, F), E=32, 40, 48, 56 MeV; measured fission fragment yield vs mass, kinetic energy distributions.
doi: 10.1016/0375-9474(87)90632-4
1983GO22 Nucl.Phys. A410, 458 (1983) R.Govil, S.S.Kapoor, D.M.Nadkarni, S.R.S.Murthy, P.N.Rama Rao Measurements of Fragment Mass, Charge and Kinetic Energy Distributions in Thermal Neutron Fission of 235U with a Back-to-Back ΔE-E Detector System NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment mass, charge, kinetic energy distributions, correlations.
doi: 10.1016/0375-9474(83)90638-3
1982SI08 J.Phys.(London) G8, L85 (1982) A.K.Sinha, M.M.Sharma, S.C.L.Sharma, G.K.Mehta, D.M.Nadkarni Polar and Equatorial Emission of Light Charged Particles in keV Neutron-Induced Fission NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal, 600 keV; measured proton, triton, α yields, polar, equatorial emission; deduced polar emission mechanism. E-ΔE telescope.
doi: 10.1088/0305-4616/8/6/006
1981SH05 Nucl.Phys. A355, 13 (1981) S.C.L.Sharma, G.K.Mehta, R.K.Choudhury, D.M.Nadkarni, S.S.Kapoor Multiparameter Study of 1H, 3H and 4He in Fast Neutron Induced Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=0-550 keV; measured σ(Eα), σ(Et), σ(Ep).
doi: 10.1016/0375-9474(81)90129-9
1980CH26 Nucl.Phys. A346, 473 (1980) R.K.Choudhury, S.S.Kapoor, D.M.Nadkarni, P.N.Rama Rao Multiparameter Study of the Long-Range α-Particles Emitted in the Thermal Neutron Induced Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured fragment mass, kinetic energy distribution, (fragment)(fragment)(θ), Eα, (fragment)α(θ).
doi: 10.1016/0375-9474(80)90481-9
1977KR07 Pramana 8, 315 (1977) B.Krishnarajulu, G.K.Mehta, R.K.Choudhury, D.M.Nadkarni, S.S.Kapoor Yields and Energy Spectra of Light Charged Particles Emitted in Neutron Induced Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=0.1-1 MeV; measured light charged particle yields.
doi: 10.1007/BF02847801
1976CH09 Pramana 6, 64 (1976) R.K.Choudhury, S.S.Kapoor, D.M.Nadkarni, P.N.Rama Rao, S.R.Srinivas Murthy Studies of Mass and Energy Correlations in Thermal Neutron Fission of U-235 Accompanied by Long Range Alpha Particles NUCLEAR REACTIONS 235U(n, F), E=th; measured σ(E(fragment mass)).
doi: 10.1007/BF02848636
1974OG03 Yad.Fiz. 19, 486 (1974); Sov.J.Nucl.Phys. 19, 244 (1974) Y.T.Oganesyan, D.M.Nadkarni, Y.E.Penionzhkevich, B.I.Pustylnik, Nguen Tak An Energy Dependence of the Cross Sections for Fission and Nucleon Transfer in Interaction of 232Th with Accelerated 74Ge Ions NUCLEAR REACTIONS 232Th(74Ge, F), (74Ge, X), E=405-600 MeV; measured σ(E); deduced Coulomb barrier. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0028. 1973BE04 Indian J.Phys. 47, 232 (1973) A.G.Belov, Y.P.Gangrsky, B.Dalkhsuren, A.M.Kucher, T.Nagy, D.M.Nadkarni Production of Spontaneously Fissioning Isomers in Th, U, Np, Pu and Am Isotopes in Reactions Induced by 14.7 MeV Neutrons NUCLEAR REACTIONS 232Th, 235,238U, 237Np, 240,242Pu, 241,243Am(n, 2n), 239Pu, 241,243Am(n, n'), E=14.7 MeV; measured production σ for SF isomers, nF(t). 239m,241mPu, 240m,241m,242m,243mAm deduced T1/2.
1973DR10 At.Energ. 35, 279 (1973); Sov.At.Energy 35, 946 (1974) V.B.Druin, Y.V.Lobanov, D.M.Nadkarni, Y.P.Kharitonov, Y.S.Korotkin, S.P.Tretyakova, V.I.Krashonkin Nonobservance of Spontaneous Fission in Kurchatovium at Berkeley RADIOACTIVITY 259Rf; measured T1/2, SF/α. NUCLEAR REACTIONS 246Cm(18O, F), E=100 MeV; measured 259Rf yield.
1973OG02 Yad.Fiz. 18, 734 (1973); Sov.J.Nucl.Phys. 18, 377 (1974) Y.T.Oganesyan, Y.E.Penionzhkevich, Nguyen Tac Anh, D.M.Nadkarnee, K.A.Gavrilov, Kim De Yen, M.Yussonua Production of Nuclei in the Reactions with Kr and Xe Ions NUCLEAR REACTIONS 181Ta(40Ar, X), (84Kr, X), E=290, 380, 550 MeV; 197Au, 238U(136Xe, X), E=840 MeV; measured yields of 165,166,167,172Tm, 166,169,175Yb, 170,171,172,177Lu, 193,194,196m,196,198,199Au, 195m,197m,197m,197,203Hg, 199,200,202Tl, 200,203Pb, 205,206Bi, 191,195m,197Pt, 188,189,190Ir, 226,227,231,234Th, 228,230,232,233,237Pa, 237,239,240U, 238,239,240Np, 239,240,244Am.
1972NA20 Nucl.Phys. A196, 209 (1972) D.M.Nadkarni, S.K.Kataria, S.S.Kapoor, P.N.Rama Rao Correlation between Energies and Angles of α-Particles Emitted in Thermal-Neutron Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured (fragment)(α)-coin, (fragment)(α)(θ); deduced σ(Eα, θ(α)).
doi: 10.1016/0375-9474(72)90961-X
1971KA28 Phys.Rev. C4, 2165 (1971) S.S.Kapoor, S.K.Kataria, S.R.S.Murthy, D.M.Nadkarni, V.S.Ramamurthy, P.N.Rama Rao Studies of the Times of Emission and Multiplicities of K X Rays from Fission Fragments of Specified Atomic Numbers RADIOACTIVITY, Fission 236U, 252Cf; measured K X-ray average emission times, multiplicities.
doi: 10.1103/PhysRevC.4.2165
1968NA24 Nucl.Phys. A112, 241 (1968) Angular anisotropy of fission fragments in ternary fission of 235U induced by 3 MeV neutrons NUCLEAR REACTIONS 235U(n, f), E=0.025 eV-3 MeV; measured products; deduced σ(θ), yields, σ, σ(E). Data were imported from EXFOR entry 30093.
doi: 10.1016/0375-9474(68)90201-7
1965KA20 Phys.Rev. 137, B511 (1965) S.S.Kapoor, D.M.Nadkarni, R.Ramanna, P.N.Rama Rao Kinetic-energy distributions and the correlation of anisotropy and asymmetry in the 4-MeV neutron-induced fission of U235 NUCLEAR REACTIONS 235U(n, f), E=4.2 MeV; measured products; deduced yields, σ(θ). Data were imported from EXFOR entry 33032.
doi: 10.1103/physrev.137.b511
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