NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Satpathy Found 17 matches. 2004BE17 Nucl.Phys. A734, 249 (2004) B.R.Behera, S.Kailas, K.Mahata, A.Chatterjee, P.Basu, S.Roy, M.Satpathy, S.K.Datta Role of Entrance Channel Properties in Heavy Ion Induced Fission Fragment Angular Distribution Studies NUCLEAR REACTIONS 232Th(14N, X), 235U(11B, X), 181Ta(16O, X), E* ≈ 45-65 MeV; analyzed fission fragment angular distributions, anisotropies; deduced entrance channel effects.
doi: 10.1016/j.nuclphysa.2004.01.046
2004BE28 Phys.Rev. C 69, 064603 (2004) B.R.Behera, M.Satpathy, S.Jena, S.Kailas, R.G.Thomas, K.Mahata, A.Chatterjee, S.Roy, P.Basu, M.K.Sharan, S.K.Datta Fission fragment angular distributions for the systems 14N + 232Th and 11B + 235U at near and sub-barrier energies NUCLEAR REACTIONS 232Th(14N, X), E=72-92 MeV; 235U(11B, X), E=51-74 MeV; measured fission σ, fragment angular distributions, anisotropy; deduced reaction mechanism features. Comparison with standard statistical saddle-point model predictions.
doi: 10.1103/PhysRevC.69.064603
2002BE78 Phys.Rev. C66, 047602 (2002) B.R.Behera, S.Jena, M.Satpathy, S.Roy, P.Basu, M.K.Sharan, M.L.Chatterjee, S.Kailas, K.Mahata, S.K.Datta Statistical model analysis of fission fragment angular distributions for the system 16O+181Ta NUCLEAR REACTIONS 181Ta(16O, F), E=90-110 MeV; measured fission, fusion, evaporation residue σ, fission fragment angular distributions, anisotropies. Comparison with saddle point model results, other data analyzed.
doi: 10.1103/PhysRevC.66.047602
2001BE52 Phys.Rev. C64, 041602 (2001) B.R.Behera, S.Jena, M.Satpathy, S.Kailas, K.Mahata, A.Shrivastava, A.Chatterjee, S.Roy, P.Basu, M.K.Sharan, S.K.Datta Entrance-Channel Effect in Fission Fragment Anisotropies from 11B + 235U and 14N + 232Th Systems NUCLEAR REACTIONS 235U(11B, F), E=64-72 MeV; 232Th(14N, F), E=80-92 MeV; measured fission fragment angular distributions, anisotropies; deduced entrance channel effect. Statistical saddle point model.
doi: 10.1103/PhysRevC.64.041602
2001BE76 Pramana 57, 199 (2001) B.Behera, S.Roy, P.Basu, M.K.Sharan, S.Jena, M.Satpathy, M.L.Chatterjee, S.K.Datta Measurement of Fission Anisotropy for 16O + 181Ta NUCLEAR REACTIONS 181Ta(16O, F), E=83-120 MeV; analyzed fission σ, fragment angular distributions, anisotropy. Transition state model.
doi: 10.1007/s12043-001-0175-9
1999BE70 Pramana 53, 563 (1999) B.R.Behera, S.Roy, P.Basu, M.K.Sharan, S.Jena, M.Satpathy, S.K.Datta, L.Satpathy, M.L.Chatterjee Fission Fragment Angular Distributions in 16O + 181Ta NUCLEAR REACTIONS 181Ta(16O, F), E=92, 98, 108 MeV; measured fission σ, fragments energies, angular distributions. Comparison with statistical model predictions.
doi: 10.1007/s12043-999-0032-9
1997DA13 Phys.Rev. C56, 1444 (1997) C.B.Das, A.Das, M.Satpathy, L.Satpathy Entrance Channel Dependence of Fragmentation Dynamics in Heavy-Ion Collisions NUCLEAR REACTIONS 40Ca, 197Au(40Ar, X), E=42, 92, 137 MeV/nucleon; 197Au(197Au, X), E=100, 400 MeV/nucleon; analyzed fragment mass distribution, multiplicity vs impact parameter; deduced spectator contribution. Dynamic statistical multifragmentation.
doi: 10.1103/PhysRevC.56.1444
1996DA08 Phys.Rev. C53, 1833 (1996) C.B.Das, A.Das, L.Satpathy, M.Satpathy Statistical Simultaneous Multifragmentation Model for Heavy Ion Collisions with Entrance Channel Characteristics NUCLEAR REACTIONS 45Sc(40Ar, X), E=35-115 MeV/nucleon; analyzed fragment charge, mass distribution, other features. Statistical simultaneous multi-fragmentation model.
doi: 10.1103/PhysRevC.53.1833
1994DA01 J.Phys.(London) G20, 189 (1994) The Effects of the Interfragment Nuclear Interaction on the Kinetic Energy Spectra in the Multifragmentation Process NUCLEAR REACTIONS Xe, Kr(p, X), E not given; calculated isotopic fragment yields, X=C, O, Ne, 14C, 19O vs mass, kinetic energy; deduced interfragment interaction role. Statistical fragmentation model.
doi: 10.1088/0954-3899/20/1/018
1993DA02 J.Phys.(London) G19, 319 (1993) A.Das, M.Mishra, M.Satpathy, L.Satpathy Effects of Interfragment Nuclear Interaction and Statistical Approach to Multifragmentation Phenomena NUCLEAR REACTIONS Ag, Cu, Ta, 197Au, Xe, Kr(p, X), E not given; calculated fragment yield vs mass; deduced interfragment nuclear interaction role. Multi-fragmentation, statiscal approach.
doi: 10.1088/0954-3899/19/2/014
1990SA11 Phys.Lett. 237B, 181 (1990) L.Satpathy, M.Mishra, A.Das, M.Satpathy Fragment Interactions in Nuclear Multifragmentation Phenomena NUCLEAR REACTIONS Kr, Cu, Xe(p, X), E=high; calculated fragment mass yields.
doi: 10.1016/0370-2693(90)91425-B
1988MI28 J.Phys.(London) G14, 1115 (1988) M.Mishra, M.Satpathy, L.Satpathy Is Multifragmentation a Signature of Liquid-Gas Phase Transitions ( Question ) NUCLEAR REACTIONS Xe, Kr(p, X), E=80-350 GeV; analyzed data. Statistical model.
doi: 10.1088/0305-4616/14/8/014
1981SA10 Phys.Rev. C23, 1777 (1981) R.Sahu, M.Satpathy, L.Satpathy Microscopic Triaxial Description of 187Ir, 187Os, and 189Ir NUCLEAR STRUCTURE 187,189Ir, 187Os; calculated levels, μ, quadrupole moment. Microscopic triaxial description, pairing + quadrupole-quadrupole interaction, Hartree-BCS model.
doi: 10.1103/PhysRevC.23.1777
1979SA03 Phys.Rev. C19, 263 (1979) L.Satpathy, A.Ansari, M.Satpathy Anomaly of High Spin States NUCLEAR STRUCTURE 158Er, 166Yb; calculated projected energies, square of angular momentum strength; deduced mechanism of backbending. Hartree-BCS formalism.
doi: 10.1103/PhysRevC.19.263
1979SA07 Phys.Rev. C19, 511 (1979); Erratum Phys.Rev. C19, 2424 (1979) R.Sahu, M.Satpathy, A.Ansari, L.Satpathy Triaxial Description of 188Os and 188Pt NUCLEAR STRUCTURE 188Os, 188Pt; calculated levels, B(E2), electromagnetic moments of ground, γ band. Hartree-BCS theory with pairing Q.Q interaction.
doi: 10.1103/PhysRevC.19.511
1978SA32 Pramana 10, 589 (1978) M.Satpathy, R.Sahu, A.Ansari, L.Satpathy An Angular Momentum Expansion of Energy and Structure of High Spin States NUCLEAR STRUCTURE 132Ce, 156,158Dy, 158,160,162Er, 166Yb; calculated energies of high spin states. Microscopic approach, angular momentum expansion of energy.
doi: 10.1007/BF02879546
1971SA02 Phys.Lett. 34B, 377 (1971) Shape-Fluctuation Model of Ground-State Bands in Even-Even Nuclei NUCLEAR STRUCTURE 120,122Xe, 126Ba, 128Ce, 152,154Sm, 158Er, 166Yb, 188Os, 194Pt, 232Th, 244Cm; calculated ground-state rotational bands. Shape-fluctuation models.
doi: 10.1016/0370-2693(71)90629-0
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