NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = L.Satpathy Found 54 matches. 2010DA03 Phys.Rev. C 81, 014311 (2010) L.S.Danu, D.C.Biswas, A.Saxena, A.Shrivastava, A.Chatterjee, B.K.Nayak, R.G.Thomas, R.K.Choudhury, R.Palit, I.Mazumdar, P.Datta, S.Chattopadhyay, S.Pal, S.Bhattacharya, S.Muralithar, K.S.Golda, R.K.Bhowmik, J.J.Das, R.P.Singh, N.Madhavan, J.Gerl, S.K.Patra, L.Satpathy Fine structure dips in the fission fragment mass distribution for the 238U(18O, f) reaction NUCLEAR REACTIONS 238U(18O, F)Sr/Zr/Mo/Ru/Pd/Cd/Sn/Te/Xe/Ba/Ce/Nd/Sm, E=100 MeV; measured Eγ, Iγ, γγ-coin, fission fragment mass distribution and yields of Sr (A=90-96), Zr (A=96-102), Mo (A=98-108), Ru (A=104-112), Pd (A=108-116), Cd (A=114-122), Sn (A=116-128), Te (A=124-134), Xe (A=130-138), Ba (A=136-144), Ce (A=142-148), Nd (A=146-152) and Sm (A=150-158) using INGA array. Discussed effect of nuclear structure in the dynamical evolution of fissioning nucleus. 128Te; measured Eγ and γγ-coin.
doi: 10.1103/PhysRevC.81.014311
2010PA16 J.Phys.(London) G37, 085103 (2010) S.K.Patra, R.K.Choudhury, L.Satpathy Anatomy of neck configuration in fission decay NUCLEAR STRUCTURE 232,240,250,256Th, 236,250,256,260U; calculated binding energies, quadrupole deformation parameter, rms radii; deduced fission neck properties for highly deformed configurations. RMF theory.
doi: 10.1088/0954-3899/37/8/085103
2008SA23 Pramana 70, 847 (2008) Resonance states in 16O+16O, 12C+16O, α+16O and α+12C with modified Morse potentials
doi: 10.1007/s12043-008-0094-0
2005SA51 J.Phys.(London) G31, 1233 (2005) Resonance states in the 12C + 12C modified Morse potential NUCLEAR REACTIONS 12C(12C, X), E(cm) ≈ 2-12 MeV; calculated molecular resonance energies. Modified Morse potential.
doi: 10.1088/0954-3899/31/11/009
2004SA21 J.Phys.(London) G30, 771 (2004) Shell overcomes repulsive nuclear force instability NUCLEAR STRUCTURE Z=50-90; analyzed two-neutron separation energies, shell correction energies; deduced possible new islands of stability. 156Ba, 158Ce, 160Nd, 162Sm, 224W, 228Pt, 232Pb, 236Rn, 252Ra, 254Th, 256U, 258Pu; calculated single-particle level energies, binding energies, deformation. Relativistic mean field theory.
doi: 10.1088/0954-3899/30/6/007
2003SA49 Nucl.Phys. A722, 24c (2003) New magic numbers and new islands of stability in drip-line regions in mass model NUCLEAR STRUCTURE Z=50-90; calculated two-neutron separation energies; deduced shell closure features. 156Ba, 158Ce, 160Nd, 162Sm; calculated single-particle level energies. Relativistic mean field approach.
doi: 10.1016/S0375-9474(03)01330-7
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
1999NA42 At.Data Nucl.Data Tables 73, 213 (1999) Mass Predictions in the Infinite Nuclear Matter Model NUCLEAR STRUCTURE Z=4-120; A=8-270; calculated mass excesses, binding energies. Infinite nuclear matter model. ATOMIC MASSES Z=4-120; A=8-270; calculated mass excesses, binding energies. Infinite nuclear matter model.
doi: 10.1006/adnd.1999.0819
1999SA42 Phys.Rep. 319, 85 (1999) L.Satpathy, V.S.Uma Maheswari, R.C.Nayak Finite Nuclei to Nuclear Matter: A leptodermous approach NUCLEAR STRUCTURE A=40-200; analyzed masses; deduced nuclear matter density, binding energy per nucleon, incompressibility. Infinite nuclear matter model, comparison with liquid drop approach.
doi: 10.1016/S0370-1573(99)00011-3
1998DA01 Phys.Rev. C57, R35 (1998) Caloric Curve in Au + Au Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=35-130 MeV/nucleon; calculated temperature vs excitation energy; deduced nuclear interfragment interaction role. Dynamic statistical multifragmentation model.
doi: 10.1103/PhysRevC.57.R35
1998SA29 J.Phys.(London) G24, 1527 (1998) Study of Nuclei in the Drip-Line Regions NUCLEAR STRUCTURE Z=7-94; analyzed two-neutron separation energies, deduced shell quenching, new stability regions.
doi: 10.1088/0954-3899/24/8/029
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
1995NA12 Phys.Rev. C52, 711 (1995) R.Nayak, V.S.Uma Maheswari, L.Satpathy Saturation Properties and Incompressibility of Nuclear Matter: A consistent determination from nuclear masses
doi: 10.1103/PhysRevC.52.711
1995UM01 Phys.Rev. C52, 1431 (1995) V.S.Uma Maheswari, V.S.Ramamurthy, L.Satpathy Nuclear Incompressibility: An analytical study on the leptodermous expansion
doi: 10.1103/PhysRevC.52.1431
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
1994SA07 J.Phys.(London) G20, L37 (1994) The Mechanism of Nuclear Molecular Resonances and the α-Particle Chain Configuration in 24Mg NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=12-44 MeV; calculated partial σ(E) for L=14. 24Mg deduced molecular resonance evidence, J, π. Dynamical potential model.
doi: 10.1088/0954-3899/20/2/003
1994UM02 Phys.Rev. C49, 2854 (1994) V.S.Uma Maheswari, V.S.Ramamurthy, L.Satpathy Reply to ' Comment on ' Influence of Bulk Properties on the Surface Structure of Finite Nuclei ' '
doi: 10.1103/PhysRevC.49.2854
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
1992SA21 J.Phys.(London) G18, 1793 (1992) L.Satpathy, P.K.Sahu, P.Sarangi Quasi-Molecular States in the 12C + 16O and 16O + 16O Systems NUCLEAR REACTIONS 16O, 12C(16O, 16O), E not given; analyzed resonances data. Diatomic-like molecular picture, Morse-type bonding potential.
doi: 10.1088/0954-3899/18/11/012
1992SA26 Pramana 39, 279 (1992) Nuclear Molecular Resonances in α + 12C and α + 16O System NUCLEAR REACTIONS 16O, 12C(α, α), E(cm) ≈ 4-18 MeV; analyzed resonance data. Morse-type bonding potential, diatomic molecule picture.
doi: 10.1007/BF02847254
1990SA07 J.Phys.(London) G16, 469 (1990) Resonances of the Bonding Potential of 12C + 12C System NUCLEAR REACTIONS 12C(12C, 12C), E not given; calculated quasimolecular state excitation, phase shifts, σ vs E. Bonding potential from di-nuclear picture.
doi: 10.1088/0954-3899/16/3/017
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
1990SA48 Pramana 34, 111 (1990) Bonding Potential between Two 12C Nuclei NUCLEAR REACTIONS 12C(12C, 12C), E not given; calculated bonding potential parameters. Ali-Bodmer α-α potential.
doi: 10.1007/BF02847195
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
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
1988SA23 At.Data Nucl.Data Tables 39, 241 (1988) Masses of Atomic Nuclei in the Infinite Nuclear Matter Model NUCLEAR STRUCTURE A=18-267; calculated mass excesses. Infinite nuclear matter model. ATOMIC MASSES A=18-267; calculated mass excesses. Infinite nuclear matter model.
doi: 10.1016/0092-640X(88)90025-3
1987GU03 Z.Phys. A326, 221 (1987) A New Macroscopic-Microscopic Description of the Double-Humped Fission Barriers NUCLEAR STRUCTURE 228Ra, 228Ac, 228Th, 229Pa, 234U, 238Np, 239Pu, 241Am, 243Cm, 248Bk, 250Cf, 254Es, 255Fm, 256Md, 257No, 259Lr, 261Rf; calculated binding energies; Z=90-98; calculated doubled-humped fission barriers, shell energies. New mass relation.
1987SA19 J.Phys.(London) G13, 761 (1987) Infinite Nuclear Matter Based Model for Masses of Atomic Nuclei NUCLEAR STRUCTURE 30Mg, 42S, 42,43,44Cl, 34,43,46Ar, 49K, 43,44V, 44,45Cr, 46,47,48Mn, 49,50Fe, 51,52Co, 64,76Ga, 64,81Ge, 97Sr, 84,100Zr, 100Ag, 121Cd, 122Cs, 154Nd, 140,154,155,156Pm, 157,158Sm, 156Ho, 156,157,158,160Er, 159,156,158,160,157Tm, 160,161,157,162,163,164,159Yb, 157,158,161,162,163,164,160Lu, 158,159,161,163,164Hf, 162,163,164Ta, 213Pb, 215Bi, 208,229Ra, 211,215Ac, 215,216,219,220Th, 215,216,217,218,219,220,221,222,223Pa, 227U, 251Bk; calculated binding energies. 22Ne, 22Mg, 32P, 32Cl, 41Ca, 41Sc, 47V, 47,50Cr, 50,53Fe, 53,55Co, 55,58Ni, 58Zn; calculated binding energy differences. Infinite nuclear matter model.
doi: 10.1088/0305-4616/13/6/009
1986SA03 J.Phys.(London) G12, 201 (1986) L.Satpathy, P.Sarangi, A.Faessler Bonding Potential and the Mechanism of Quasi-Molecular States NUCLEAR REACTIONS 12C(12C, 12C), E not given; calculated bonding potential; deduced quasimolecular resonances, Γγ, B(E2), quadrupole moments.
doi: 10.1088/0305-4616/12/3/008
1983SA22 Phys.Rev.Lett. 51, 1243 (1983) Generalized Hugenholtz - Van Hove Theorem and a New Mass Relation for Finite Nuclei NUCLEAR STRUCTURE 22,29Mg, 24,31Al, 64Co, 84Se, 104Mo, 143Cs, 165Gd, 181Yb, 197Re, 204Pt, 221Po, 236Ac, 143Xe, 161Nd, 180Dy, 201Lu, 223Au, 238At, 258U, 28,30P, 34Cl, 42Sc, 46V, 50Mn, 38,39Ca, 42Ti; calculated binding energies; deduced deviation from experiment. Generalized Hugenholtz-Van Hove theorem, new mass relation, comparison with other mass formulae predictions.
doi: 10.1103/PhysRevLett.51.1243
1982GR04 Phys.Lett. 110B, 31 (1982) Capture Cross Section in the Surface Friction Model NUCLEAR REACTIONS 208Pb(26Mg, X), (27Al, X), E(cm) ≈ 100-250 MeV; 208Pb(48Ca, X), (50Ti, X), (52Cr, X), (58Fe, X), E(cm) ≈ 200-350 MeV; calculated σ(capture) vs E. Surface friction model.
doi: 10.1016/0370-2693(82)90945-5
1981GR03 Z.Phys. A299, 63 (1981) D.H.E.Gross, R.C.Nayak, L.Satpathy A Classical Description of Deep Inelastic Collisions with Surface Friction and Deformation NUCLEAR REACTIONS 232Th(40Ar, X), E=379 MeV; 209Bi(136Xe, X), E=1130 MeV; calculated distance of closest approach, deflection function vs L, nuclear potential vs deformation, final energy vs θ. Friction model, deep inelastic, fusion reactions.
doi: 10.1007/BF01415743
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
1978NA07 Nucl.Phys. A304, 64 (1978) Study of Exotic Nuclei with the Skyrme Interaction NUCLEAR STRUCTURE 4,8,10He, 12,14,20,22C, 16,22,24,28O, 28,30,34,42,46,48Si; calculated binding energies, single-particle energies.
doi: 10.1016/0375-9474(78)90096-9
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
1977NA22 Phys.Lett. 71B, 257 (1977) S.C.K.Nair, A.Ansari, L.Satpathy Neutron-Proton Interaction and Nuclear Deformations NUCLEAR STRUCTURE 20Ne, 24Mg; calculated intrinsic quadrupole moment Q0. Hartree-Fock-Bogoliubov. 154Sm, 160Gd, 162Dy, 168Er; calculated β. Baranger-Kumar.
doi: 10.1016/0370-2693(77)90208-8
1976SA21 Phys.Rev. C14, 1995 (1976) L.Satpathy, K.W.Schmid, S.Krewald, A.Faessler Intrashell Quartet States NUCLEAR STRUCTURE 20,22Ne, 24Mg; calculated intrashell quartet states. Angular momentum projection formalism.
doi: 10.1103/PhysRevC.14.1995
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
1975PA20 Phys.Rev. C12, 2038 (1975) R.Patnaik, R.Patra, L.Satpathy Simple Relations for the Excitation Energies E2 and the Transition Probabilities B(E2) of Neighboring Doubly Even Nuclides NUCLEAR STRUCTURE 68,78Ge, 72Se, 106,108,110,112Ru, 112,114Pd, 118Te, 124Xe, 144,146Ce, 152Nd, 146,156Sm, 162Gd, 172Er, 182,184,194Os; calculated B(E2).
doi: 10.1103/PhysRevC.12.2038
1974SC10 Z.Phys. 267, 337 (1974) K.W.Schmid, L.Satpathy, A.Faessler Study of Doubly Even s d-Shell Nuclei in the Multi-Configuration-Hartree-Fock Model. I. The Intrinsic Structure NUCLEAR STRUCTURE 20,22Ne, 24,26Mg, 28,30Si, 32S, 36Ar; calculated wavefunctions.
doi: 10.1007/BF01669964
1974SC11 Z.Phys. 267, 345 (1974) K.W.Schmid, L.Satpathy, A.Faessler Study of Doubly Even s d-Shell Nuclei in the Multi-Configuration-Hartree-Fock Model. II. The Influence of Correlations on the Ground State Rotational Spectra NUCLEAR STRUCTURE 20,22Ne, 24,26Mg, 28,30Si, 32S, 36Ar; calculated levels, quadrupole moment, B(E2).
doi: 10.1007/BF01669965
1974SC34 Z.Phys. 271, 149 (1974) K.W.Schmid, S.Krewald, A.Faessler, L.Satpathy The Angular Momentum Dependence of Correlations in the Ground State Rotational Spectra of 20Ne and 22Ne NUCLEAR STRUCTURE 20,22Ne; calculated levels, quadrupole moment.
doi: 10.1007/BF01676385
1972SA04 Nucl.Phys. A179, 177 (1972) L.Satpathy, K.Goeke, A.Faessler Higher Isospin States in s-d Shell Nuclei in Self-Consistent Models NUCLEAR STRUCTURE 20,22,24Ne, 20,22,24O, 24,26,28,30,32Mg, 26Ne, 28Ne, 28,30,32Si, 32,34,36S, 36Ar; calculated levels, quadrupole moment, binding energy, analog states, pairing energy. Hartree-Fock, Hartree-Fock-Bogoliubov theory.
doi: 10.1016/0375-9474(72)90114-5
1972SA07 Phys.Rev.Lett. 28, 832 (1972) L.Satpathy, K.W.Schmid, A.Faessler Intrashell Quartet Excitations in sd-Shell Nuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated intrashell quartet states. Phenomenological quartet shell model.
doi: 10.1103/PhysRevLett.28.832
1971FA08 Phys.Lett. 35B, 193 (1971) A.Faessler, K.Goeke, L.Satpathy Nature of the Lowest T = 2 States in 20Ne and 24Mg NUCLEAR STRUCTURE 20Ne, 24Mg; calculated T=2 levels. Projected Hartree-Fock-Bogoliubov model.
doi: 10.1016/0370-2693(71)90171-7
1971FR15 Phys.Lett. 36B, 189 (1971) H.Friedrich, L.Satpathy, A.Weiguny Why Is There No Rotational Band Based on the 7.65 MeV 0+ State in 12C (Question) NUCLEAR STRUCTURE 12C; investigated intrinsic structure of second 0+ state. α-cluster model.
doi: 10.1016/0370-2693(71)90064-5
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
1969SA19 Phys.Rev. 183, 887 (1969) L.Satpathy, D.Goss, M.K.Banerjee Hartree-Fock-Bogoliubov Calculations in the 2s, 1d Shell NUCLEAR STRUCTURE 20,22,24Ne, 24,26,28Mg, 28,30,32Si, 32,34,36S, 36,38Ar; calculated levels, quadrupole moment, moments of inertia.
doi: 10.1103/PhysRev.183.887
1968SA03 Nucl.Phys. A110, 400 (1968) Studies of Odd-Mass Co Isotopes in the Unified Model
doi: 10.1016/0375-9474(68)90549-6
1968SA04 Phys.Letters 26B, 716 (1968) Deformed Configuration Mixing Model for Some s-d Shell Nuclei
doi: 10.1016/0370-2693(68)90400-0
1968SA10 Phys.Rev. 174, 1324 (1968) Projected Tamm-Dancoff Spectra of Ne20 and Mg24
doi: 10.1103/PhysRev.174.1324
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