NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = M.A.Nagarajan Found 97 matches. 2005NA09 Eur.Phys.J. A 24, 63 (2005) M.A.Nagarajan, S.M.Lenzi, A.Vitturi Low-lying dipole strength for weakly bound systems: A simple analytic estimate NUCLEAR STRUCTURE 19C; calculated dipole strength distribution. Analytic expression.
doi: 10.1140/epja/i2004-10129-2
2003AN22 Nucl.Phys. A724, 113 (2003) M.V.Andres, J.Gomez-Camacho, M.A.Nagarajan Deviations from the adiabatic approximation in heavy-ion dynamic polarization potentials
doi: 10.1016/S0375-9474(03)01521-5
2001GU05 Nucl.Phys. A679, 393 (2001) R.Guardiola, I.Moliner, M.A.Nagarajan Alpha-Cluster Model for 8Be and 12C with Correlated Alpha Particles NUCLEAR STRUCTURE 8Be, 12C; calculated binding energies. Alpha-cluster model, comparison with previous results.
doi: 10.1016/S0375-9474(00)00366-3
2001NA14 Phys.Lett. 503B, 65 (2001) M.A.Nagarajan, C.H.Dasso, S.M.Lenzi, A.Vitturi Target-Mass Dependence of the Break-Up of Halo Nuclei NUCLEAR REACTIONS 12C, 58Ni, 208Pb(19C, X), E=67 MeV/nucleon; calculated breakup σ, nuclear and Coulomb components vs impact parameter; deduced target mass dependence features.
doi: 10.1016/S0370-2693(01)00189-7
1999CH03 J.Phys.(London) G25, 11 (1999) J.A.Christley, E.G.Lanza, S.M.Lenzi, M.A.Nagarajan, A.Vitturi Excitation of the GDR and the Compressional Isoscalar Dipole State by α Scattering NUCLEAR REACTIONS 28O(α, α'), E=68 MeV; 70Ca(α, α'), E=40 MeV; calculated GDR, isoscalar dipole state excitation σ(θ); deduced nuclear, Coulomb contributions.
doi: 10.1088/0954-3899/25/1/002
1998BR28 Acta Phys.Hung.N.S. 7, 113 (1998) F.Brandolini, S.M.Lenzi, D.R.Napoli, R.V.Ribas, H.Somacal, C.A.Ur, D.Bazzacco, J.A.Cameron, G.de Angelis, M.De Poli, A.Gadea, C.Fahlander, S.Lunardi, M.A.Nagarajan, C.Rossi Alvarez, C.Svensson DSAM Lifetimes of the Ground State Band in 48Cr NUCLEAR REACTIONS 28Si(28Si, 2α), E=115 MeV; measured Eγ, Iγ, γγ-coin, DSA. 48Cr deduced levels T1/2, B(E2).
1998SV02 Phys.Rev. C58, R2621 (1998) C.E.Svensson, S.M.Lenzi, D.R.Napoli, A.Poves, C.A.Ur, D.Bazzacco, F.Brandolini, J.A.Cameron, G.de Angelis, A.Gadea, D.S.Haslip, S.Lunardi, E.E.Maqueda, G.Martinez-Pinedo, M.A.Nagarajan, C.Rossi Alvarez, A.Vitturi, J.C.Waddington High-Spin States in the Odd-Odd N = Z Nucleus 50Mn NUCLEAR REACTIONS 28Si(28Si, npα), E=115 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 50Mn deduced high-spin levels, J, π, configuration. GASP, ISIS detector arrays. Shell model calculations.
doi: 10.1103/PhysRevC.58.R2621
1998UR05 Phys.Rev. C58, 3163 (1998) C.A.Ur, D.Bucurescu, S.M.Lenzi, G.Martinez-Pinedo, D.R.Napoli, D.Bazzacco, F.Brandolini, D.M.Brink, J.A.Cameron, E.Caurier, G.de Angelis, M.De Poli, A.Gadea, S.Lunardi, N.Marginean, M.A.Nagarajan, P.Pavan, C.Rossi Alvarez, C.E.Svensson Excited States in 52Fe and the Origin of the Yrast Trap at Iπ = 12+ NUCLEAR REACTIONS 28Si(28Si, α), E=115 MeV; measured Eγ, Iγ, γγ-coin, DSA. 52Fe deduced levels, J, π, T1/2, B(E2), isomer decay B(E4) upper limits. GASP spectrometer. NUCLEAR STRUCTURE 52Fe; calculated levels, J, π, quadrupole moments, isomer decay log ft, branching ratios. Comparison with 44Ti.
doi: 10.1103/PhysRevC.58.3163
1997AN01 Nucl.Phys. A612, 82 (1997) M.V.Andres, J.A.Christley, J.Gomez-Camacho, M.A.Nagarajan Dipole Coulomb Excitation in 11Be Scattering NUCLEAR REACTIONS, ICPND 197Au(11Be, 11Be'), E=30 MeV; calculated σ(θ), fusion σ vs spin; deduced projectile dipole Coulomb excitation related features. Dynamic polarization potentials, coupled-channels approach.
doi: 10.1016/S0375-9474(96)00324-7
1997AN18 Nucl.Phys. A625, 685 (1997) M.V.Andres, J.A.Christley, J.Gomez-Camacho, M.A.Nagarajan Spin-Orbit Dynamic Polarization Potential Due to Dipole Coulomb Excitation NUCLEAR REACTIONS 197Au(11Be, 11Be), E=30 MeV; calculated reaction σ, σ(θ), vector analyzing power; deduced Coulomb excitation role.
doi: 10.1016/S0375-9474(97)00388-6
1997BE45 Phys.Rev. C56, 1960 (1997) M.B.Becha, C.O.Blyth, C.N.Pinder, N.M.Clarke, R.P.Ward, P.R.Hayes, K.I.Pearce, D.L.Watson, A.Ghazarian, M.D.Cohler, I.J.Thompson, M.A.Nagarajan The 40Ca(t, p)42Ca Reaction at Triton Energies Near 10 MeV per Nucleon NUCLEAR REACTIONS 40Ca(t, p), E=28, 33, 37.3 MeV; measured proton spectra, σ(E, θ); deduced model parameters, reaction mechanism features. 48Ca(t, p), (t, d), E=37.3 MeV; measured σ(θ). 49Ca level deduced J, π. Shell model calculations, DWBA analysis.
doi: 10.1103/PhysRevC.56.1960
1997CA06 Nucl.Phys. A614, 86 (1997) F.Catara, E.G.Lanza, M.A.Nagarajan, A.Vitturi Collective Transition Densities in Neutron-Rich Nuclei NUCLEAR STRUCTURE 28O, 60Ca; calculated nucleon ground state densities, isoscalar, isovector transition strength distribution, RPA transition densities. 40Ca, 208Pb; calculated isoscalar, isovector transition strength distribution for RPA quadrupole states.
doi: 10.1016/S0375-9474(96)00457-5
1997CA51 Nucl.Phys. A624, 449 (1997) F.Catara, E.G.Lanza, M.A.Nagarajan, A.Vitturi Effect of Large Neutron Excess on the Dipole Response in the Region of the Giant Dipole Resonance NUCLEAR STRUCTURE 16,28O, 40,48,60,70Ca; calculated dipole response; 28O, 60,70Ca; calculated transition densities; deduced neutron excess effects. Hartree-Fock plus RPA, Skyrme interaction.
doi: 10.1016/S0375-9474(97)00485-5
1997DA26 Nucl.Phys. A627, 349 (1997) C.H.Dasso, H.M.Sofia, S.M.Lenzi, M.A.Nagarajan, A.Vitturi Excitation of Isovector Modes in Very Neutron-Rich Nuclei Via Heavy-Ion Isoscalar Probes NUCLEAR STRUCTURE 28O, 70Ca, 176Sn; calculated neutron, proton densities. 16,28O, 40,70Ca, 114,176Sn; calculated GDR, GQR transition densities. Collective model. NUCLEAR REACTIONS 16,28O, 40,70Ca, 114,176Sn(16O, 16O'), E not given; calculated GDR excitation radial formfactors. 70Ca(16O, 16O'), E(cm)=200 MeV; 28O(α, α'), E(cm)=150 MeV; calculated GDR excitation σ(θ); deduced nuclear, Coulomb contributions.
doi: 10.1016/S0375-9474(97)00391-6
1997LE15 Phys.Rev. C56, 1313 (1997) S.M.Lenzi, C.A.Ur, D.R.Napoli, M.A.Nagarajan, D.Bazzacco, D.M.Brink, M.A.Cardona, G.de Angelis, M.De Poli, A.Gadea, D.Hojman, S.Lunardi, N.H.Medina, C.Rossi Alvarez Band Termination and Second Backbending in 50Cr NUCLEAR REACTIONS 24Mg(32S, 2pα), E=130 MeV; measured Eγ, Iγ, γγ-, (charged-particle)γ-coin, γγ(θ), DCO ratios. 50Cr deduced high-spin levels, J, π, configurations, band structure. Cranked shell-model analysis.
doi: 10.1103/PhysRevC.56.1313
1997LE35 Acta Phys.Hung.N.S. 6, 95 (1997) S.M.Lenzi, C.H.Dasso, M.A.Nagarajan, H.M.Sofia, A.Vitturi Effects of Neutron Skin on the Excitation of Isovector Modes of Neutron-Rich Nuclei
1997NA19 J.Phys.(London) G23, 1479 (1997) Dipole Coulomb Excitation in Halo Nuclei NUCLEAR REACTIONS 197Au(11Be, 11Be), E=30, 42 MeV; calculated polarization potential, elastic σ(θ), reaction σ vs J; deduced halo nucleus dipole states elastic scattering effect. Halo nucleus dipole Coulomb excitation included.
doi: 10.1088/0954-3899/23/10/039
1996LE03 Z.Phys. A354, 117 (1996) S.M.Lenzi, D.R.Napoli, A.Gadea, M.A.Cardona, D.Hojman, M.A.Nagarajan, C.Rossi Alvarez, N.H.Medina, G.de Angelis, D.Bazzacco, M.E.Debray, M.De Poli, S.Lunardi, D.de Acuna High Spin States in 48Cr NUCLEAR REACTIONS 24Mg(32S, 2α), E=130 MeV; measured γγγ-, γγ(particle)-coin. 48Cr deduced high-spin levels, J, π, band structure.
doi: 10.1007/s002180050019
1996NA09 Phys.Rev. C54, 435 (1996) Structure of the Dynamical Polarization Potential
doi: 10.1103/PhysRevC.54.435
1995AN06 Nucl.Phys. A583, 817c (1995) M.V.Andres, J.Gomez-Camacho, M.A.Nagarajan Dynamic Polarization Potential Induced by Dipole Coulomb Excitation to Break-Up States in 11Li Scattering NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=50 MeV; calculated σ(θ). Polarization potential due to direct Coulomb excitation into the continuum.
doi: 10.1016/0375-9474(94)00765-F
1995CH21 Nucl.Phys. A587, 390 (1995) J.A.Christley, C.H.Dasso, S.M.Lenzi, M.A.Nagarajan, A.Vitturi Ion-Ion Potential for Neutron-Rich Radioactive Beams NUCLEAR STRUCTURE 16,25O, 40,48,70Ca, 114,176Sn; calculated neutron, proton Hartree-Fock densities. NUCLEAR REACTIONS 25,16O(16O, 16O), 40,61Ca(40Ca, 40Ca), 114,176Sn(16O, 16O); calculated microscopic double-folding potentials vs inter-nuclear distance. 25O(16O, 16O), E(cm)=13 MeV; calculated elastic σ(θ) relative to Rutherford σ(θ). 25O(16O, X), E(cm) ≈ 7-11 MeV; calculated fusion σ(E). Hartree-Fock approach based ion-ion potentials.
doi: 10.1016/0375-9474(94)00827-A
1995CH40 Nucl.Phys. A591, 341 (1995) J.A.Christley, M.A.Nagarajan, A.Vitturi Collision of Almost Identical Nuclei: Fusion cross sections and barrier distributions NUCLEAR REACTIONS, ICPND 30Si(28Si, X), E(cm) ≈ 28-40 MeV; calculated σ(E). 18O(16O, X), E=24 MeV; calculated σ(θ). 18O(16O, X), E ≈ 7.5-18 MeV; calculated σ(E).
doi: 10.1016/0375-9474(95)00186-5
1995CO16 Phys.Rev. C52, R1175 (1995) G.Colo, M.A.Nagarajan, P.Van Isacker, A.Vitturi Isospin Mixing in Proton-Rich N ≈ Z Nuclei NUCLEAR STRUCTURE 90Zr, 99,100Sn, 99In, 40Ca, 88Sr, 208Pb; calculated isospin admixtures. 100Sn; calculated isovector giant monopole resonance strength distribution. Hartree-Fock approach, Skyrme forces.
doi: 10.1103/PhysRevC.52.R1175
1995KE01 Nucl.Phys. A582, 314 (1995) N.Keeley, J.A.Christley, N.M.Clarke, B.R.Fulton, J.S.Lilley, M.A.Nagarajan, I.J.Thompson The Threshold Anomaly in the 16O + 58,60,62,64Ni Systems NUCLEAR REACTIONS 58,60,62,64Ni(16O, 16O), (16O, 16O'), E=60, 70, 80, 100, 120 MeV; measured σ(θ); deduced optical model parameters. Double-folding model, coupled-reaction-channels analyses.
doi: 10.1016/0375-9474(94)00485-6
1994AN21 Nucl.Phys. A579, 273 (1994) M.V.Andres, J.Gomez-Camacho, M.A.Nagarajan Dynamic Polarization Potential Induced by Dipole Coulomb Excitation NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=50 MeV; calculated σ(θ). Dipole Coulomb excitation induced dynamic polarization potential.
doi: 10.1016/0375-9474(94)90806-0
1994GO28 Nucl.Phys. A580, 156 (1994) J.Gomez-Camacho, M.V.Andres, M.A.Nagarajan Analytic Approximations for the Dynamic Polarization Effects Due to Coulomb Excitation NUCLEAR REACTIONS 184W(18O, 18O), (18O, 18O'), E=75, 90 MeV; calculated σ(θ); deduced dynamic polarization potential parameters. Coupled-channels approach.
doi: 10.1016/0375-9474(94)90820-6
1994KE08 Nucl.Phys. A571, 326 (1994) N.Keeley, S.J.Bennett, N.M.Clarke, B.R.Fulton, G.Tungate, P.V.Drumm, M.A.Nagarajan, J.S.Lilley Optical Model Analyses of 6,7Li + 208Pb Elastic Scattering Near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(6Li, 6Li), E=25-39 MeV; 208Pb(7Li, 7Li), E=25-60 MeV; measured σ(θ); deduced optical model parameters. Double folding model.
doi: 10.1016/0375-9474(94)90064-7
1994SH36 Ann.Phys.(New York) 231, 110 (1994) M.M.Sharma, M.A.Nagarajan, P.Ring The Relativistic Mean-Field, Effective Mass and the Compression Properties of Nuclei NUCLEAR STRUCTURE 16O; calculated p-shell spin-orbit splitting vs m(σ). Relativistic mean field, effective mass, compression properties.
doi: 10.1006/aphy.1994.1035
1993KR01 Phys.Rev. C47, R451 (1993) A.T.Kruppa, M.A.Nagarajan, J.P.Vary Charge Exchange Effects in Elastic Scattering with Radioactive Beams NUCLEAR REACTIONS 13N, 13C(13C, 13C), E(cm)=7.5-10 MeV; calculated σ(θ); deduced effective neutron-proton interaction extraction possibility. Four-body model.
doi: 10.1103/PhysRevC.47.R451
1993KR14 Nucl.Phys. A560, 845 (1993) A.T.Kruppa, P.Romain, M.A.Nagarajan, N.Rowley Effect of Multiphonon Coupling on Heavy-Ion Fusion NUCLEAR REACTIONS 92Zr(32S, 32S), (32S, 32S'), E(cm) ≈ 70-90 MeV; calculated elastic, quasielastic σ(E); deduced multi-phonon channels effect on barrier distribution. Fusion reactions, vibrational coupling effects.
doi: 10.1016/0375-9474(93)90174-V
1993SH13 Phys.Lett. 312B, 377 (1993) M.M.Sharma, M.A.Nagarajan, P.Ring Rho Meson Coupling in the Relativistic Mean Field Theory and Description of Exotic Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,124Sn, 208Pb; calculated binding energy, charge, neutron radii percentage deviations, neutron skin thickness. 112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142Xe; calculated binding energy, charge radii, deformations; deduced ρ-meson coupling role. Relativistic mean field theory.
doi: 10.1016/0370-2693(93)90970-S
1993SK05 Nucl.Phys. A561, 157 (1993) L.D.Skouras, H.Muther, M.A.Nagarajan Determination of Dipole Polarization Effects in 7Li and 11Li NUCLEAR STRUCTURE 6,7Li; calculated μ, quadrupole moment, rms radii, B(λ). 11Li; calculated μ, quadrupole moment, rms radii. Shell model.
doi: 10.1016/0375-9474(93)90148-Q
1991BO45 J.Phys.(London) G17, 1803 (1991) D.Bonatsos, L.D.Skouras, P.Van Isacker, M.A.Nagarajan An Application of the Democratic Mapping to the sd and fp Shells NUCLEAR STRUCTURE 20Ne, 42Sc, 44Ti; calculated levels. Democratic mapping method.
doi: 10.1088/0954-3899/17/12/004
1991CH27 J.Phys.(London) G17, L163 (1991) J.A.Christley, M.A.Nagarajan, I.J.Thompson Optical Fusion Potentials for 16O + 208Pb NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, X), E=80-90 MeV; calculated σ(θ), fusion σ(l); deduced model parameters.
doi: 10.1088/0954-3899/17/9/004
1991KR13 J.Phys.(London) G17, L209 (1991) A.T.Kruppa, M.A.Nagarajan, J.S.Lilley, I.J.Thompson Magnetic Substate Population in Heavy-Ion Inelastic Scattering at Energies Near the Coulomb Barrier NUCLEAR REACTIONS 92Zr(16O, 16O'), E=56 MeV; calculated magnetic substate population probability vs θ, σ(θ); deduced nuclear reorientation coupling role. Coupled-channels method.
doi: 10.1088/0954-3899/17/11/007
1990SA08 Phys.Rev. C41, 1869 (1990) G.R.Satchler, M.A.Nagarajan, J.S.Lilley, I.J.Thompson Comment on ' Simultaneous Analyses of Elastic Scattering and Fusion Cross Sections for the 32S + 58,64Ni Systems at Energies Near the Coulomb Barrier ' NUCLEAR REACTIONS 64Ni(32S, 32S), E=88 MeV; calculated σ(θ); deduced model parameters. Extension of Udagawa et al model.
doi: 10.1103/PhysRevC.41.1869
1990SA18 J.Phys.(London) G16, 639 (1990) Y.Sakuragi, N.Rowley, M.A.Nagarajan Symmetry Properties of Nearside and Farside Amplitudes in Polarized Heavy-Ion Scattering NUCLEAR REACTIONS 26Mg(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; calculated σ(θ), analyzing powers vs θ. Nearside, farside component treatment.
doi: 10.1088/0954-3899/16/4/014
1990SH03 Phys.Rev.Lett. 64, 376 (1990) J.A.Sheikh, N.Rowley, M.A.Nagarajan, H.G.Price Neutron-Proton Interactions in the Mass-80 Region NUCLEAR STRUCTURE A ≈ 80; calculated yrast band crossing structures; deduced n-p interaction dependence. Cranked shell model.
doi: 10.1103/PhysRevLett.64.376
1990SK08 Nucl.Phys. A516, 255 (1990) L.D.Skouras, P.Van Isacker, M.A.Nagarajan A Democratic Mapping between the Shell Model and the Interacting Boson Model NUCLEAR STRUCTURE 44,45,46Ti, 46,47V, 48Ca; calculated levels. Shell model, interacting boson model connection.
doi: 10.1016/0375-9474(90)90308-9
1990SM03 Nucl.Phys. A517, 193 (1990) M.J.Smithson, J.S.Lilley, M.A.Nagarajan, P.V.Drumm, R.A.Cunningham, B.R.Fulton, I.J.Thompson The Threshold Anomaly in Inelastic Scattering NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=70-94 MeV; measured σ(θ); deduced model parameters. 208Pb deduced deformation lengths, quadrupole moment. DWBA analysis.
doi: 10.1016/0375-9474(90)90268-Q
1989CH09 J.Phys.(London) G15, 457 (1989) H.D.Choi, G.Tungate, M.A.Nagarajan, N.Rowley Quasielastic Reactions in the Collision of Deformed Projectiles NUCLEAR REACTIONS 208Pb(polarized 23Na, 23Na), (polarized 23Na, 23Na'), E=170 MeV; calculated σ(θ), transverse tensor analyzing power vs θ.
doi: 10.1088/0954-3899/15/4/009
1989SA36 J.Phys.(London) G15, L209 (1989) Effect of Coulomb Excitation on Tidal Symmetry in the Scattering of Polarised Projectiles NUCLEAR REACTIONS 208Pb(polarized 23Na, 23Na), (polarized 23Na, 23Na'), E=170 MeV; calculated σ(θ), analyzing power vs θ; deduced tidal symmetry role.
doi: 10.1088/0954-3899/15/10/003
1989SA46 J.Phys.(London) G15, 1855 (1989) Y.Sakuragi, M.A.Nagarajan, N.Rowley Coupled-Channels Calculation for the System 23Na + 208Pb: A test of tidal symmetry NUCLEAR REACTIONS 208Pb(polarized 23Na, 23Na), (23Na, 23Na'), E=170 MeV; calculated σ(θ), vector, tensor analyzing power vs θ; deduced Coulomb excitation effects. Coupled-channels formalism.
doi: 10.1088/0954-3899/15/12/011
1989TH06 Nucl.Phys. A505, 84 (1989) I.J.Thompson, M.A.Nagarajan, J.S.Lilley, M.J.Smithson The Threshold Anomaly in 16O + 208Pb Scattering NUCLEAR REACTIONS, ICPND 208Pb(16O, 16O), E=78-102 MeV; calculated σ(θ), reaction σ vs E. Coupled reaction channels model.
doi: 10.1016/0375-9474(89)90417-X
1988AN01 Phys.Lett. 202B, 292 (1988) M.V.Andres, N.Rowley, M.A.Nagarajan Effect of Deformation on the Elastic and Quasielastic Scattering of Heavy Ions Near the Coulomb Barrier NUCLEAR REACTIONS 154Sm(16O, 16O), (16O, 16O'), (16O, X), E(cm)=63.45 MeV; calculated elastic, fusion σ(θ).
doi: 10.1016/0370-2693(88)90473-X
1988AN05 Nucl.Phys. A481, 600 (1988) M.V.Andres, N.Rowley, M.A.Nagarajan Deviations from Shape-Effect Relations in the Polarization of Inelastically Scattered Heavy Ions NUCLEAR REACTIONS 154Sm(polarized 16O, 16O), (polarized 16O, 16O'), E=60 MeV; calculated σ(θ), polarization vs θ. Coupled-channels method.
doi: 10.1016/0375-9474(88)90347-8
1988NA10 Nucl.Phys. A485, 360 (1988) M.A.Nagarajan, A.Faessler, R.Linden, N.Ohtsuka Causality and the Energy Dependence of Microscopic Nucleus-Nucleus Potential NUCLEAR REACTIONS 12C(12C, 12C), E ≈ 0-150 MeV/nucleon; calculated model parameters. Energy density method, microscopic nucleus-nucleus potentials.
doi: 10.1016/0375-9474(88)90107-8
1988SH20 J.Phys.(London) G14, L109 (1988) Extraction of Photocapture Cross Sections from Direct Coulomb Break-Up Reactions NUCLEAR REACTIONS 208Pb(7Li, tα), E=70 MeV; calculated σ(θα, θt). Direct Coulomb breakup.
doi: 10.1088/0305-4616/14/5/008
1988TH04 Nucl.Phys. A487, 141 (1988) I.J.Thompson, M.A.Nagarajan, J.S.Lilley, B.R.Fulton Evidence of Projectile Polarisation Effects on the Reaction 208Pb(17O, 16O)209Pb NUCLEAR REACTIONS 208Pb(17O, 16O), E=78-102 MeV; calculated σ(θ); deduced multi-step mechanism role. Coupled-reaction calculations.
doi: 10.1016/0375-9474(88)90133-9
1987LI04 Nucl.Phys. A463, 710 (1987) J.S.Lilley, M.A.Nagarajan, D.W.Banes, B.R.Fulton, I.J.Thompson Multistep Effects in Reactions of 17O with 208Pb near the Coulomb Barrier NUCLEAR REACTIONS 208Pb(17O, 17O), (17O, 17O'), (17O, 16O), (17O, 18O), E=78 MeV; measured σ(θ); deduced multistep effects on reactions, interaction potential. Enriched target. DWBA and CRC analyses.
doi: 10.1016/0375-9474(87)90639-7
1987NA13 Phys.Lett. 192B, 297 (1987) M.A.Nagarajan, M.V.Andres, M.Lozano Polarization Effects Due to Coupling of Elastic to Compound States NUCLEAR REACTIONS 24Mg, 28Si, 40Ca(16O, 16O), E=33-140 MeV; calculated σ vs L; deduced polarization potential.
doi: 10.1016/0370-2693(87)90109-2
1987SA38 Ann.Phys.(New York) 178, 110 (1987) G.R.Satchler, M.A.Nagarajan, J.S.Lilley, I.J.Thompson Heavy-Ion Fusion: Channel-coupling effects, the barrier penetration model, and the threshold anomaly for heavy-ion potentials NUCLEAR REACTIONS 208Pb(16O, X)(16O, 16O), (16O, 16O'), E=80, 102 MeV; 90Zr(46Ti, X), (46Ti, 46Ti), (46Ti, 46Ti'), E(cm)=105 MeV; calculated elastic, absorption, fusion, total σ. Channel-coupling effects, barrier penetration model.
doi: 10.1016/S0003-4916(87)80015-5
1986DA04 Phys.Lett. 166B, 379 (1986) Evidence for α-Cluster Monopole and Dipole Modes in 156Gd NUCLEAR STRUCTURE 156Gd; calculated levels, B(λ), ratios. Vibron model, α-clustering. 2H, 4He, 6Li, 8Be, 10B, 12C, 14N, 16O; calculated B(E1) vs mass. Core plus dinuclear system, α-cluster models.
doi: 10.1016/0370-2693(86)91583-2
1986NA06 Phys.Lett. 173B, 29 (1986) Comments on the Barrier Penetration Model for Heavy-Ion Fusion NUCLEAR REACTIONS 208Pb(16O, X), E=80 MeV; calculated fusion σ vs l. Barrier penetration model.
doi: 10.1016/0370-2693(86)91224-4
1985FU12 Phys.Lett. 162B, 55 (1985) B.R.Fulton, D.W.Banes, J.S.Lilley, M.A.Nagarajan, I.J.Thompson Energy Dependence of the 16O + 60Ni Potential and the Optical Model Dispersion Relation NUCLEAR REACTIONS 60Ni(16O, 16O), E=36-141.7 MeV; analyzed data; deduced optical potential parameter Coulomb barrier dependence.
doi: 10.1016/0370-2693(85)91060-3
1985GO11 Nucl.Phys. A440, 543 (1985) J.Gomez-Camacho, M.Lozano, M.A.Nagarajan Coupled-Channel Calculations for the Elastic Scattering of 7Li by 40,48Ca at 89 MeV NUCLEAR REACTIONS 40,48Ca(7Li, 7Li), (7Li, 7Li'), E=89 MeV; calculated σ(θ). Coupled-channels method.
doi: 10.1016/0375-9474(85)90245-3
1985GO20 Phys.Lett. 161B, 39 (1985) J.Gomez-Camacho, M.Lozano, M.A.Nagarajan Coupled Channel Effects in the Scattering of 6,7Li by 58Ni NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=12, 14, 16, 18, 20, 50.6, 73.7 MeV; 58Ni(7Li, 7Li), E=14.2, 16.3, 18.3, 20.3 MeV; calculated σ(θ). Coupled-channels formalism, effective interactions, model densities.
doi: 10.1016/0370-2693(85)90604-5
1985GO23 J.Phys.(London) G11, L239 (1985) J.Gomez-Camacho, M.A.Nagarajan Effect of Dipole Polarisation in the Quadrupole Coulomb Excitation NUCLEAR STRUCTURE 6,7Li; calculated B(E1), dipole polarizability correction; deduced GDR interaction splitting role.
doi: 10.1088/0305-4616/11/12/003
1985LI07 Phys.Lett. 151B, 181 (1985) J.S.Lilley, B.R.Fulton, M.A.Nagarajan, I.J.Thompson, D.W.Banes Evidence for a Progressive Failure of the Double Folding Model at Energies Approaching the Coulomb Barrier NUCLEAR REACTIONS 208Pb(16O, 16O), E=78 MeV; measured σ(θ); deduced optical potential parameter dependence on Coulomb barrier proximity. Other data input.
doi: 10.1016/0370-2693(85)90830-5
1985NA01 Phys.Rev.Lett. 54, 1136 (1985) M.A.Nagarajan, C.C.Mahaux, G.R.Satchler Dispersion Relation and the Low-Energy Behavior of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-220 MeV; calculated potential parameter energy dependence.
doi: 10.1103/PhysRevLett.54.1136
1985SH22 J.Phys.(London) G11, 1199 (1985) R.Shyam, R.G.Lovas, K.F.Pal, V.K.Sharma, M.A.Nagarajan DWBA Analyses of (7Li, t) Reactions with Realistic Potential Overlap NUCLEAR REACTIONS 12C, 40,44Ca, 58Ni(7Li, t), E=34 MeV; calculated σ(θ); deduced optical model potentials. 16O, 44,48Ti, 62Zn levels deduced Sα. Finite-range DWBA analysis.
doi: 10.1088/0305-4616/11/11/006
1985SH26 Ann.Phys.(New York) 163, 265 (1985) A Distorted-Wave Born-Approximation Theory of Heavy-Ion-Induced Projectile Breakup Reactions NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; 40Ca(14N, d10B), E=110 MeV; calculated transition amplitudes. DWBA, heavy ion induced projectile breakup.
doi: 10.1016/0003-4916(85)90382-3
1985TH06 Phys.Lett. 157B, 250 (1985) I.J.Thompson, M.A.Nagarajan, J.S.Lilley, B.R.Fulton Contribution of Multistep Transfers to Low-Energy Elastic and Reaction Cross Sections NUCLEAR REACTIONS 208Pb(16O, 16O), E=80, 102 MeV; calculated σ(θ). 208Pb(16O, 16O'), (16O, X), E=80 MeV; calculated fusion, inelastic, total, transfer σ; deduced multi-step transfer role. Coupled-channels method.
doi: 10.1016/0370-2693(85)90660-4
1984DA07 Phys.Lett. 139B, 150 (1984) T.Davinson, V.Rapp, A.C.Shotter, D.Branford, M.A.Nagarajan, I.J.Thompson, N.E.Sanderson Coulomb and Nuclear Contribution to the Excitation of 7Li Incident on Heavy Nuclei NUCLEAR REACTIONS 208Pb(7Li, 7Li), (7Li, 7Li'), E=68 MeV; measured σ(θ); deduced Coulomb, nuclear contribution relative importance. Coupled-channels, adiabatic model calculations.
doi: 10.1016/0370-2693(84)91233-4
1984FU02 Phys.Lett. 136B, 322 (1984) B.R.Fulton, J.S.Lilley, R.Lindsay, M.A.Nagarajan, N.Rowley, R.Shyam, T.M.Cormier, P.M.Stwertka Structure in the 02+ Excitation Function in 12C + 12C Scattering NUCLEAR REACTIONS, ICPND 12C(12C, 12C'), E(cm)=20-40 MeV; measured σ(E), σ(θ); deduced barrier matching, barrier, internal wave interference effects. DWBA, no resonance contribution.
doi: 10.1016/0370-2693(84)92012-4
1984GI02 Ann.Phys.(New York) 152, 475 (1984) B.G.Giraud, M.A.Nagarajan, I.J.Thompson Time-Independent Mean Field Description of Collisions NUCLEAR REACTIONS 3H(p, np), E=55.1, 103.6 MeV; calculated transition amplitude. Multi-step collisions, variational principle, breakup.
doi: 10.1016/0003-4916(84)90099-X
1984SH17 Phys.Rev.Lett. 53, 1539 (1984) A.C.Shotter, V.Rapp, T.Davinson, D.Branford, N.E.Sanderson, M.A.Nagarajan Direct Coulomb Breakup of 7Li NUCLEAR REACTIONS 120Sn(7Li, tα), E=70 MeV; measured σ(Eα); deduced projectile breakup mechanism.
doi: 10.1103/PhysRevLett.53.1539
1984SH26 J.Phys.(London) G10, 1703 (1984) Electromagnetic Properties of 7Li with Generator Coordinate Wavefunction NUCLEAR REACTIONS 7Li(e, e'), E not given; calculated charge, magnetic form factors. Generator coordinate method, α-triton cluster. NUCLEAR STRUCTURE 7Li; calculated ground state wave function, charge, magnetic form factors, rms charge radius, μ, quadrupole, octupole moments. Generator coordinate method, α-triton cluster.
doi: 10.1088/0305-4616/10/12/009
1983GI10 Phys.Rev. C28, 1918 (1983) Variational Estimate of a Breakup Amplitude NUCLEAR REACTIONS 3H(p, np), E not given; calculated breakup amplitude. Variational approach.
doi: 10.1103/PhysRevC.28.1918
1983LO09 Nucl.Phys. A402, 141 (1983) R.G.Lovas, K.F.Pal, M.A.Nagarajan Generator-Coordinate Calculation of the Potential Overlap for the DWBA Description of Cluster Transfer Reactions NUCLEAR REACTIONS 12C(7Li, t), E not given; calculated σ(θ). DWBA, cluster transfer, generator coordinate potential overlap calculation.
doi: 10.1016/0375-9474(83)90565-1
1983PA06 Nucl.Phys. A402, 114 (1983) K.F.Pal, R.G.Lovas, M.A.Nagarajan, B.Gyarmati, T.Vertse Microscopic Description of 7Li and 7Be for the DWBA Treatment of Cluster Transfer Reactions NUCLEAR REACTIONS 12C(7Li, t), E=34 MeV; calculated σ(θ); deduced potential parameters. Finite range DWBA, generator coordinate cluster for projectile, schematic nucleon-nucleon forces.
doi: 10.1016/0375-9474(83)90564-X
1983SH15 J.Phys.(London) G9, 901 (1983) Bound-State Shell Model with Full Correction for Spurious Centre-of-Mass Motion NUCLEAR REACTIONS 16O(d, p), E=8 MeV; 40Ca(d, p), E=7 MeV; calculated σ(θ). DWBA, center-of-mass corrected shell model form factor.
doi: 10.1088/0305-4616/9/8/013
1983TH04 Phys.Lett. 123B, 379 (1983) Elastic Breakup of 70 MeV 7Li Ions on Lead NUCLEAR REACTIONS 208Pb(7Li, tα), E=70 MeV; calculated breakup σ(θα, θt); deduced Coulomb distortion role. DWBA, adiabatic approximation.
doi: 10.1016/0370-2693(83)90976-0
1982NA07 Phys.Scr. 25, 463 (1982) Finite-Range DWBA Analyses of (p, t) and (t, p) Reactions with Realistic Triton and Nuclear Wave Functions NUCLEAR REACTIONS 18O(p, t), E=20 MeV; 208Pb(p, t), E=35 MeV; 48Ca(t, p), E=12 MeV; 90Zr(t, p), E=11.89, 20 MeV; calculated σ(θ). Finite-range DWBA, realistic triton nuclear wave functions.
doi: 10.1088/0031-8949/25/3/005
1982NA14 Nucl.Phys. A385, 525 (1982) M.A.Nagarajan, I.J.Thompson, R.C.Johnson Elastic Scattering of 89 MeV 7Li by 40Ca and 48Ca NUCLEAR REACTIONS 48,40Ca(7Li, 7Li), 48Ca(7Li, 7Li'), E=89 MeV; calculated σ(θ); deduced projectile breakup effects. Adiabatic model.
doi: 10.1016/0375-9474(82)90102-6
1982NA15 Phys.Rev. C26, 977 (1982) Finite Range Effects in (d(pol), 3He) Reactions on 54Fe at E(d) = 80 MeV NUCLEAR REACTIONS 54Fe(polarized d, 3He), E=80 MeV; calculated σ(θ), iT11(θ). 53Mn levels deduced S. Zero-range, finite-range DWBA, microscopic form factors.
doi: 10.1103/PhysRevC.26.977
1982NA22 Phys.Rev.Lett. 49, 1899 (1982) D-State Effects and J Dependence in (α, d) Reactions NUCLEAR REACTIONS, ICPND 208Pb(α, d), E=48 MeV; calculated angle integrated σ; deduced α-particle D-state effects. DWBA analysis.
doi: 10.1103/PhysRevLett.49.1899
1982SH21 Phys.Lett. 116B, 99 (1982) R.Shyam, M.A.Nagarajan, A.C.Shotter, A.N.Bice, J.Cerny Inelastic Scattering of 12C from 208Pb to the Second 0+ State of 12C NUCLEAR REACTIONS 208Pb(12C, 12C'), E=132, 187, 230 MeV; measured σ(θ); deduced real potential characteristics. Microscopic DWBA, folding model.
doi: 10.1016/0370-2693(82)90984-4
1981IO02 Phys.Lett. 103B, 187 (1981) A.A.Ioannides, M.A.Nagarajan, R.Shyam Finite-Range DWBA Analyses of (d(pol), t) and (d(pol), 3He) Reactions on 64Zn at E(d) = 13 MeV NUCLEAR REACTIONS 64Zn(polarized d, t), (polarized d, 3He), E=13 MeV; analyzed σ(θ), iT11(θ). Finite-range DWBA, microscopic overlap functions.
doi: 10.1016/0370-2693(81)90737-1
1981TH07 Phys.Lett. 106B, 163 (1981) Break-Up Effects in Elastic Scattering of 6Li Ions NUCLEAR MOMENTS 12C, 40Ca, 208Pb(6Li, 6Li), E=156 MeV; calculated σ(θ); deduced breakup effects. Adiabatic model, alpha-deuteron cluster.
doi: 10.1016/0370-2693(81)90899-6
1980FE01 Phys.Rev.Lett. 44, 1037 (1980) D.H.Feng, M.A.Nagarajan, M.R.Strayer, M.Vallieres, W.T.Pinkston Exact Finite-Range Distorted-Wave Born-Approximation Analyses of the Reactions 18O(p, t)16O, 48Ca(t, p)50Ca, and 90Zr(t, p)93Zr Using Realistic Triton and Nuclear Wave Functions NUCLEAR REACTIONS 18O(p, t), E=20 MeV; 48Ca(t, p), E=12.08 MeV; 90Zr(t, p), E=11.89 MeV; calculated σ(θ). Finite-range DWBA, realistic t-, structure overlap-functions.
doi: 10.1103/PhysRevLett.44.1037
1980WE03 Phys.Rev. C21, 2235 (1980) M.E.Werby, M.R.Strayer, M.A.Nagarajan Finite Range Distorted-Wave Born Approximation Analysis of (p, t) Reactions with a Realistic Triton Wave Function NUCLEAR REACTIONS 18O(p, t), E=20 MeV; 208Pb(p, t), E=35 MeV; calculated σ(θ). Exact finite range DWBA, realistic triton wave functions.
doi: 10.1103/PhysRevC.21.2235
1977NA11 Phys.Lett. 68B, 421 (1977) M.A.Nagarajan, M.R.Strayer, M.F.Werby Unnatural Parity Transitions in (p, t) Reactions Using Realistic Triton Wavefunctions NUCLEAR REACTIONS 208Pb(p, t), E=35 MeV; calculated σ(Et, θ).
doi: 10.1016/0370-2693(77)90458-0
1977WE06 J.Phys.(London) G3, L-115 (1977) The Evaluation of Generator Coordinate Amplitudes NUCLEAR REACTIONS 6Li(α, α); calculated interaction, generator-coordinate amplitudes.
doi: 10.1088/0305-4616/3/6/001
1975NA07 Phys.Rev. C11, 1167 (1975) M.A.Nagarajan, W.L.Wang, D.J.Ernst, R.M.Thaler Relation between the Watson and Kerman-McManus-Thaler Multiple Scattering Formalisms NUCLEAR REACTIONS 4He, 12C, 40Ca(p, p), E=90, 310, 1050 MeV; calculated σ.
doi: 10.1103/PhysRevC.11.1167
1973KO09 Phys.Rev.Lett. 30, 1075 (1973) D.G.Kovar, B.G.Harvey, F.D.Becchetti, J.Mahoney, D.L.Hendrie, H.Homeyer, W.von Oertzen, M.A.Nagarajan Evidence for Recoil Effects in Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 208Pb(12C, 11B), (16O, 15N), E(12C)=78 MeV, E(16O)=104, 140 MeV; measured σ(E(11B), E(15N), θ); deduced recoil effects. 209Bi levels deduced S.
doi: 10.1103/PhysRevLett.30.1075
1972NA07 Phys.Lett. 40B, 65 (1972) Comments on a Three Body Model of Stripping
doi: 10.1016/0370-2693(72)90283-3
1972NA19 Nucl.Phys. A196, 34 (1972) The Effect of Recoil on Single-Nucleon Transfer in Heavy-Ion Reactions
doi: 10.1016/0375-9474(72)90946-3
1968BR05 Phys.Letters 26B, 248 (1968) R.C.Braley, M.A.Nagarajan, M.W.Gilpatrick, R.W.Finlay On the Reaction C12(n, n'γ)C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90548-0
1968HA15 Nucl.Phys. A113, 412 (1968) A Shell-Model Calculation for the Reaction 15N(p, n)15O NUCLEAR STRUCTURE 15O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90415-6
1967DI01 Nucl.Phys. A93, 190(1967) G.U.Din, M.A.Nagarajan, R.Pollard The Study of 10B(d, n)11C and 11B(d, n)12C Reactions NUCLEAR REACTIONS 10B(d, n), E = 3.2 to 9 MeV; measured σ(E; En, θ); 11B(d, n), E = 1.1 to 2.9 MeV; measured σ(E; En). Enriched targets.
doi: 10.1016/0375-9474(67)90179-0
1964NA02 Nucl.Phys. 50, 61 (1964) Analysis of the Reaction B11(d, n)C12(4.43 Mev) NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90193-2
1963NA04 Nucl.Phys. 42, 454 (1963) Configuration Mixing in Mass 14 Nuclei NUCLEAR STRUCTURE 14N, 14C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90748-X
1963NA05 Nucl.News (Israel), p.8 (April 1963) Configuration Mixing in Mass 14 Nuclei NUCLEAR STRUCTURE 14C, 14N; measured not abstracted; deduced nuclear properties.
1962NA04 Bull.Am.Phys.Soc. 7, No.4, 269, CB11 (1962) Shell-Model Analysis of the Reaction B11(d, n)C12 NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1962NA10 Bull.Am.Phys.Soc. 7, No.8, 540, J9 (1962) 15.11-MeV Level of Carbon 12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962NA11 Bull.Am.Phys.Soc. 7, No.8, 559, SP1 (1962) Configuration Mixing in Nitrogen 14 NUCLEAR STRUCTURE 14N, 14C; measured not abstracted; deduced nuclear properties.
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