NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.J.Lombard Found 73 matches. 2012DI01 Rom.J.Phys. 57, 159 (2012) A.Diaf, M.Lassaut, R.J.Lombard Approximate Centrifugal Barriers and Critical Angular Momentum
2010ME02 J.Phys.(London) G37, 075103 (2010) Spectral analysis: a consistency criterion. Application to the 208ΛPb hypernucleus NUCLEAR STRUCTURE 208Pb; analyzed particle in a local potential, constructed two sets of eigenvalues for 208Pb hypernucleus.
doi: 10.1088/0954-3899/37/7/075103
2006KE04 Few-Body Systems 38, 1 (2006) A.T.Kerris, F.-Z.Ighezou, R.J.Lombard, H.Ngo The Bertlmann-Martin Inequalities in the Three-Body Problem
doi: 10.1007/s00601-005-0122-2
2003LO04 Nucl.Phys. A720, 60 (2003) R.J.Lombard, A.I.Vdovin, N.Yu.Shirikova, A.V.Sushkov On M3-transition rates in selected odd-mass nuclei NUCLEAR STRUCTURE 159Ho, 175Yb, 179Hf, 179W, 183Pt; calculated transitions B(M3), level configurations. Quasiparticle-phonon model.
doi: 10.1016/S0375-9474(03)00742-5
2001IG01 Eur.Phys.J. A 11, 79 (2001) F.-Z.Ighezou, R.J.Lombard, J.Mares Spectral Analysis of 208Pb Muonic Atom ATOMIC PHYSICS, Mesic-Atoms 208Pb; calculated muonic atom potentials, level densities. Recurrence relations.
doi: 10.1007/s100500170097
2001LO20 Yad.Fiz. 64, No 7, 1315 (2001); Phys.Atomic Nuclei 64, 1240 (2001) Remarks on Halo Nuclei NUCLEAR STRUCTURE 6He, 11Li, 11Be, 14B, 15,17,19C; analyzed radius vs separation energy.
doi: 10.1134/1.1389549
2000BE34 Phys.Rev. C62, 024314 (2000) P.Bernardos, R.J.Lombard, M.Lopez-Quelle, S.Marcos, R.Niembro Derivative Coupling Model Description of Nuclear Matter in the Dirac-Hartree-Fock Approximation
doi: 10.1103/PhysRevC.62.024314
2000FA02 J.Phys.(London) G26, 167 (2000) G.Faldt, C.Lazard, R.J.Lombard The Reaction p + 3He → π+ + 4He NUCLEAR REACTIONS 3He(p, π+), E=800 MeV; calculated σ(θ), asymmetry; deduced Δ resonance role, other reaction mechanism features. Two-step model, comparison with data.
doi: 10.1088/0954-3899/26/2/306
1999FO13 J.Phys.(London) G25, 2107 (1999) J.Formanek, R.J.Lombard, J.-P.Maillet Elastic and Dissociation Scattering of Halo Nuclei NUCLEAR REACTIONS 12C(11Be, 11Be), E=60 MeV/nucleon; calculated σ(θ); deduced double scattering contribution. 12C(11Be, n10Be), E not given; calculated parallel momentum distributions.
doi: 10.1088/0954-3899/25/10/309
1999LA04 Eur.Phys.J. A 4, 111 (1999) Bounds to the Size of Halo Nuclei NUCLEAR STRUCTURE 2H, 11Be, 8,15B, 15,17,19C; calculated halo nuclei radius lower, upper bounds. Dimensional relationship for weakly-bound two-body systems.
doi: 10.1007/s100500050211
1998CA18 Phys.Rev. C57, 3237 (1998) F.Carstoiu, C.Lazard, R.J.Lombard Glauber Model for Transfer Reactions NUCLEAR REACTIONS 12C, 11Be(p, d), E=800 MeV; calculated pickup σ vs momentum transfer. Glauber model.
doi: 10.1103/PhysRevC.57.3237
1998MA10 Phys.Rev. C57, 1178 (1998) S.Marcos, R.J.Lombard, J.Mares Binding Energy of Double Λ Hypernuclei in Relativistic Mean Field Theory NUCLEAR STRUCTURE 6He, 10Be, 13B, 18O, 42Ca, 92Zr, 210Pb; calculated double Λ hypernuclei binding energies. Relativistic mean field approach.
doi: 10.1103/PhysRevC.57.1178
1997FO04 J.Phys.(London) G23, 423 (1997) Total Dissociation Cross Sections of Halo Nuclei NUCLEAR REACTIONS 12C(11Be, X), (11Li, X), E=50-200 MeV/nucleon; calculated dissociation σ vs model parameters; deduced halo wavefunction rms radius dependence.
doi: 10.1088/0954-3899/23/4/003
1995FO08 J.Phys.(London) G21, 87 (1995) 11Li-12C Scattering as a Four-Body Problem NUCLEAR REACTIONS 12C(11Li, 11Li), (11Li, X), E=50-200 MeV/nucleon; calculated σ(θ), inelastic, breakup σ vs E. Four-body treatment.
doi: 10.1088/0954-3899/21/1/010
1995LO04 Phys.Rev. C51, 1784 (1995) R.J.Lombard, S.Marcos, J.Mares Description of Hypernuclei in the Scalar Derivative Coupling Model NUCLEAR STRUCTURE A=17; A=41; A=90; A=140; calculated lambda single particle energies, hypernuclei. Scalar derivative-coupling model.
doi: 10.1103/PhysRevC.51.1784
1995LO08 Phys.Rev. C52, 170 (1995) Towards a Model Independent Analysis of Single Particle Spectra: Application to hypernuclei NUCLEAR STRUCTURE A=89; A=209; calculated hypernuclei single particle spectra, equivalent radii; deduced model independent local potential determination possibility.
doi: 10.1103/PhysRevC.52.170
1994CA07 Phys.Rev. C49, 2248 (1994) F.Carstoiu, M.Lassaut, R.J.Lombard Checking a Neutron Halo from Elastic Scattering NUCLEAR REACTIONS 12C(11C, 11C), (11Li, 11Li), E=60 MeV/nucleon; calculated σ(θ) difference vs q; deduced suitability for exhibiting matter distribution changes.
doi: 10.1103/PhysRevC.49.2248
1994LO13 Phys.Rev. C50, 2900 (1994) R.J.Lombard, S.Marcos, J.Mares Bertlmann-Martin Inequalities in Hypernuclei NUCLEAR STRUCTURE A=27-209; calculated hypernuclei single particle energies. Bertlmann-Martin inequalities extended to Hamiltonian.
doi: 10.1103/PhysRevC.50.2900
1993CA21 Phys.Rev. C48, 830 (1993) Eikonal Expansion for Total Cross Sections of Heavy Ion Reactions NUCLEAR REACTIONS, ICPND 12C(6Li, X), E(cm)=40-240 MeV; calculated reaction σ(E); deduced eikonal expansion validity, convergence features.
doi: 10.1103/PhysRevC.48.830
1993LA27 J.Phys.(London) G19, 2079 (1993) M.Lassaut, R.J.Lombard, J.Van de Wiele The Global Phase of the Nucleon-Nucleon Amplitudes and Proton-Nucleus Scattering NUCLEAR REACTIONS 12C(polarized p, p), E=0.8 GeV; calculated σ(θ), analyzing power vs momentum transfer. 16O(polarized p, p), E=0.8 GeV; calculated spin rotation parameter vs momentum transfer. Kerman-McManus-Thaler approximation to optical potential.
doi: 10.1088/0954-3899/19/12/013
1992CE01 Nucl.Phys. A537, 486 (1992) M.Centelles, X.Vinas, M.Barranco, S.Marcos, R.J.Lombard Semiclassical Approximations in Non-Linear σ(omega) Models NUCLEAR STRUCTURE 40Ca, 208Pb; calculated total energy, proton, neutron rms radii, nucleon densities. Nonlinear (sigma-omega) models, semi-classical approximations.
doi: 10.1016/0375-9474(92)90365-Q
1992LA13 Z.Phys. A341, 125 (1992) Influence of the Separation Energy on the Radius of Neutron Rich Nuclei NUCLEAR STRUCTURE 4,6,8He, 8,10,11,12,13,14,15B, 6,7,8,9,11Li, 12,13,14,15,16,17,18,19C, 7,9,10,11,12,14Be; calculated matter rms radii; deduced separation energy role. Hefter, de Llano and Mitropolsky model.
doi: 10.1007/BF01298471
1991BA28 Phys.Rev. C44, 178 (1991) M.Barranco, R.J.Lombard, S.Marcos, S.A.Moszkowski Multi-Lambda Matter in a Derivative Coupling Model NUCLEAR STRUCTURE 40Ca; calculated baryon density, spin orbit potential, scalar, vector fields. Mean field approximation.
doi: 10.1103/PhysRevC.44.178
1991LO03 J.Phys.(London) G17, 455 (1991) R.J.Lombard, D.Mas, S.A.Moszkowski On the Kinetic Energy Density NUCLEAR STRUCTURE 208Pb; calculated kinetic energy density p, n-components. Wigner transform.
doi: 10.1088/0954-3899/17/4/007
1991LO10 J.Phys.(London) G17, 1823 (1991) R.J.Lombard, J.P.Maillet, J.Van de Wiele Phase Variation of the Nucleon-Nucleon Amplitudes and Non-Eikonal Propagation NUCLEAR REACTIONS 4He(p, p), (polarized p, p), E=1 GeV; calculated σ(θ), polarization, spin rotation parameter; deduced nucleon-nucleon amplitude phase variation connection to noneikonal propogation.
doi: 10.1088/0954-3899/17/12/005
1990LO02 Phys.Rev. C41, R1348 (1990) Phase Variation of the Nucleon-Nucleon Amplitude and the Spin Observables in Proton-4He Elastic Scattering NUCLEAR REACTIONS 4He(polarized p, p), E=1.05 GeV; calculated σ(θ), polarization, spin-rotation parameter; deduced nucleon-nucleon amplitude phase dependence.
doi: 10.1103/PhysRevC.41.R1348
1990LO10 Europhys.Lett. 12, 119 (1990) On the Size of Light Nuclei NUCLEAR STRUCTURE 4,6,8He, 8,9,10,11,12,14Be, 7,8,9,11Li, 11,12,13,14,15,17B; calculated rms radii. Semi-empirical models.
doi: 10.1209/0295-5075/12/2/005
1990LO11 J.Phys.(London) G16, 1311 (1990) Self-Consistent Calculations of Light Nuclei NUCLEAR STRUCTURE A=8-46; calculated binding energy, rms charge, nucleon radii. Self-consistent formalism.
doi: 10.1088/0954-3899/16/9/008
1990LO13 Phys.Lett. 245B, 649 (1990) Asymptotic Contributions to Proton-4He Elastic Scattering NUCLEAR REACTIONS 4He(polarized p, p), E=high; analyzed σ, P, spin rotation parameter data. Glauber multiple scattering model.
doi: 10.1016/0370-2693(90)90706-C
1988MI12 Z.Phys. A330, 5 (1988) A.Milian, M.Barranco, D.Mas, R.J.Lombard Nuclear Collective States at Finite Temperature NUCLEAR STRUCTURE A=80-205; calculated isoscalar monopole, octupole giant resonance energy vs particle number. 90Zr, 40Ca, 208Pb; calculated levels, reduced transition probabilities. Energy density method.
1987TE01 J.Phys.(London) G13, 311 (1987) A.Tellez-Arenas, R.J.Lombard, J.P.Maillet Inclusive π+ and π- Production in Nucleon-Nucleus and 4He-Nucleus Collisions in the GeV Region NUCLEAR STRUCTURE Z=1-80; compiled, analyzed α-, proton-, neutron induced π+, π- production σ differences; deduced systematics.
doi: 10.1088/0305-4616/13/3/006
1986AN19 Z.Phys. A324, 299 (1986) Correlated Variations of Nuclear Radii and Binding Energies NUCLEAR STRUCTURE Z=10-95; analyzed data; deduced nuclear radii, binding energies correlation.
1986AU05 J.Phys.(London) G12, 317 (1986) J.P.Auger, A.Tellez-Arenas, C.Lazard, R.J.Lombard Spin-Dependent Nucleon-Nucleon Amplitudes and Proton-4He Elastic Scattering NUCLEAR REACTIONS 4He(p, p), (polarized p, p), E=800 MeV; calculated σ(θ), polarization, spin rotation parameter vs momentum transfer; deduced spin-dependent nucleon-nucleon amplitude role.
doi: 10.1088/0305-4616/12/4/005
1986AU10 J.Phys.(London) G12, 1341 (1986) Transition Densities and Intermediate Energy Hadron-Nucleus Inelastic Scattering NUCLEAR REACTIONS 88Sr(p, p'γ), E=600, 800 MeV; 88Sr(π+, π+'γ), (π-, π-'γ), E=700 MeV; 88Sr(K+, K+'γ), E=low energy; 88Sr(K-, K-'γ), E=1500 MeV; calculated transition densities, relative difference funtions. 40Ca, 58Ni, 90Zr, 120Sn, 144Sm, 208Pb(p, p'γ), E=800 MeV; calculated σ(θ), asymmetries. Glauber model.
doi: 10.1088/0305-4616/12/12/013
1986LO07 Ann.Phys.(New York) 167, 2 (1986) Semi-Empirical Description of Low Energy Nuclear Collective States NUCLEAR STRUCTURE 40,42,44,46,48Ca, 50Ti, 52Cr, 54Fe, 56,58,60Ni; calculated B(λ). 88Sr, 90Zr, 58Ni, 152Sm, 204,206,208Pb; calculated charge transition density. 40,48Ca, 54Fe, 58Ni, 88Sr, 116Sn, 140Ce, 206,208Pb; calculated proton, neutron transition densities. Semi-empirical model.
doi: 10.1016/S0003-4916(86)80003-3
1985AU02 J.Phys.(London) G11, 751 (1985) J.P.Auger, C.Lazard, R.J.Lombard, J.P.Maillet Proton-Nucleus Elastic Scattering at 800 MeV: The role of intermediate isobars NUCLEAR REACTIONS 16O, 40,48Ca, 208Pb(p, p), (polarized p, p), E=800 MeV; calculated polarization, spin rotation parameter vs momentum. Glauber model.
doi: 10.1088/0305-4616/11/6/012
1983AU04 J.Phys.(London) G9, 719 (1983) J.P.Auger, C.Lazard, R.J.Lombard Intermediate Isobars in Proton-Nucleus Elastic Scattering: The cases of 12C and 16O NUCLEAR REACTIONS 12C, 16O(p, p), E=1 GeV; calculated σ(θ), polarization; deduced intermediate nucleon isobar state. Glauber model, antisymmetrized wave functions.
doi: 10.1088/0305-4616/9/7/008
1983LO02 Phys.Lett. 120B, 23 (1983) Shell Effects at Z or N = 40: The example of 68Ni NUCLEAR STRUCTURE 58,60,62,64,66,68,70Ni; 82Ge, 84Se, 86Kr, 88Sr, 90Zr, 92Mo, 94Ru; calculated levels; deduced lowest 0+ state sensitivity to Fermi surface. Quasiparticle excitation, coupling to isoscalar GQR.
doi: 10.1016/0370-2693(83)90614-7
1981AU07 J.Phys.(London) G7, 1627 (1981) J.P.Auger, C.Lazard, R.J.Lombard Isobaric Intermediate States in Proton-Nucleus Elastic Scattering NUCLEAR REACTIONS 4He(p, p), E=1 GeV; calculated σ(θ) vs momentum transfer; deduced isobar intermediate state effects. Glauber model.
doi: 10.1088/0305-4616/7/12/011
1981GE08 Helv.Phys.Acta 54, 321 (1981) J.-F.Germond, R.J.Lombard, D.Waxman, C.Wilkin Corrections Eikonales pour un Potential Spin-Orbite NUCLEAR REACTIONS 12C(polarized p, p), E=800 MeV; calculated polarization, spin rotation parameters. Spin-orbit potential eikonal corrections.
1981WA20 Phys.Rev. C24, 578 (1981) D.Waxman, C.Wilkin, J.-F.Germond, R.J.Lombard Eikonal Corrections for Spin-Orbit Potentials NUCLEAR REACTIONS 12C(p, p), (polarized p, p), E=800 MeV; calculated σ(θ), polarization, spin rotation parameters. Eikonal approximations, modified Wallace approach.
doi: 10.1103/PhysRevC.24.578
1980AN04 J.Phys.(London) G6, 303 (1980) I.Angeli, M.Beiner, R.J.Lombard, D.Mas Trends in Nuclear Radii from the Energy Density Method NUCLEAR STRUCTURE A=15-220; calculated rms radii. 32S, 40,48Ca, 58Ni, 90Zr, 208Pb; calculated charge distributions. Energy density, Hartree-Fock-BCS methods.
doi: 10.1088/0305-4616/6/3/007
1980AU03 Phys.Lett. 90B, 200 (1980) Proton-Nucleus Elastic Scattering at 1 GeV in A = 48 Nuclei NUCLEAR REACTIONS 48Ca(p, p), 48Ti(p, p), E=1 GeV; calculated σ(θ). 48Ti, 48Ca deduced differences in rms radii. Glauber model, effective interactions.
doi: 10.1016/0370-2693(80)90723-6
1980AU09 Nucl.Phys. A350, 332 (1980) Remarks on P and Q in Proton-Nucleus Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 4He, 16O, 40Ca(p, p), E=1 GeV; calculated polarization, spin-rotation parameter; deduced imaginary, real components of spin-dependent nucleon-nucleon amplitude. Glauber model, optical limit.
doi: 10.1016/0375-9474(80)90462-5
1980BA13 Phys.Lett. 91B, 321 (1980) M.Barranco, R.J.Lombard, D.Mas Coupling of Two-Quasi-Particle 2+ States to the T = 0 Giant Quadrupole Resonance in the Even Pb-Isotopes NUCLEAR STRUCTURE 190,192,194,196,198,200,202,204,206,210,212,214Pb; calculated energy of 2+ levels. Two quasiparticle plus T=0, GQR coupling.
doi: 10.1016/0370-2693(80)90986-7
1980LO03 Nucl.Phys. A336, 185 (1980) Excitation Energies in the Energy Density Method NUCLEAR STRUCTURE 18O, 18F, 42Ca, 42Sc, 112,114,116,118,120,122,124Sn, 194,196,198,200,202,204,206,210Pb; calculated levels. Energy density method.
doi: 10.1016/0375-9474(80)90619-3
1979AU04 Nucl.Phys. A316, 205 (1979) Polarization in Proton-Nucleus Elastic Scattering Around 1 GeV NUCLEAR REACTIONS 58Ni, 208Pb(p, p), E=0.8, 1.0 GeV; calculated polarization. Glauber multiple scattering model.
doi: 10.1016/0375-9474(79)90033-2
1978AU11 Ann.Phys.(New York) 115, 442 (1978) Proton-Nucleus Elastic Scattering at 1 GeV in the Glauber Model NUCLEAR REACTIONS 1H, 4He, 16O, 28Si, 32,34S, 39K, 40,42,44,48Ca, 48Ti, 58,60,62,64Ni, 90Zr, 208Pb(p, p), E=1 GeV; calculated σ(θ), P(θ). Multiple-scattering formalism with Coulomb, spin effects.
doi: 10.1016/0003-4916(78)90163-X
1978AU12 J.Phys.(London) G4, L261 (1978) Effects of the Centre-of-Mass Correlations on the Hadron-Nucleus Elastic Differential Cross Section NUCLEAR REACTIONS 40Ca, 58Ni, 208Pb(p, p), E=1 GeV; calculated σ(θ). Model independent analysis including center-of-mass correlations.
doi: 10.1088/0305-4616/4/2/015
1978BA49 Phys.Lett. 78B, 542 (1978) Excitation Energy of the Lowest 2+ and 3- Levels in 32Mg and 146Gd NUCLEAR STRUCTURE 32Mg, 146Gd; calculated levels.
doi: 10.1016/0370-2693(78)90635-4
1976AU04 Nucl.Phys. A262, 372 (1976) J.P.Auger, J.Gillespie, R.J.Lombard Proton-4He Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 4He(p, p), E=0.6-24 GeV; calculated σ, polarization.
doi: 10.1016/0375-9474(76)90504-2
1976LA16 Nucl.Phys. A271, 317 (1976) C.Lazard, R.J.Lombard, Z.Maric Theoretical Study of Coherent Pion Photoproduction on the Deuteron NUCLEAR REACTIONS 2H(γ, π); calculated σ.
doi: 10.1016/0375-9474(76)90247-5
1976LO12 Phys.Lett. 65B, 193 (1976) Magic Numbers in Superheavy Elements NUCLEAR STRUCTURE A > 200; calculated p, n shell closure. Energy density method.
doi: 10.1016/0370-2693(76)90160-X
1975BE31 Nucl.Phys. A249, 1 (1975) Self-Consistent Calculations of Ground State Properties for Unstable Nuclei NUCLEAR REACTIONS 208Pb(Na, F), (K, F), (Rb, F); calculated influence of neutron excess on height of fission barrier. COMPILATION A=2-123; calculated binding energy.
doi: 10.1016/0375-9474(75)90089-5
1975GI07 Nucl.Phys. A242, 481 (1975) J.Gillespie, C.Gustafsson, R.J.Lombard Corrections to Eikonal Models for Hadron-Nucleus Scattering at High and Intermediate Energies NUCLEAR REACTIONS 4He, 16O(p, p), E=100, 500, 1000 MeV; calculated potential, phase shifts.
doi: 10.1016/0375-9474(75)90110-4
1975LA09 Lett.Nuovo Cim. 12, 379 (1975) C.Lazard, P.Petroff, R.J.Lombard, Z.Maric Coherent Pion Photoproduction from Deuteron NUCLEAR REACTIONS 2H(γ, π0); calculated σ.
doi: 10.1007/BF02845015
1975NG01 Nucl.Phys. A240, 353 (1975) C.Ngo, B.Tamain, J.Galin, M.Beiner, R.J.Lombard Calculation of Interaction Barriers Using the Energy Density Formalism NUCLEAR REACTIONS 24Mg, 27Al, 40Ca, 58Ni(32S, X), 238U(12C, X), (14N, X), 121Sb, 162Dy, 238U, 80Se, 118Sn, 209Bi(40Ar, X), 74Ge, 114Cd, 40Ca, 186W(84Kr, X), 197Au, 238U(63Cu, X), 118Sn(118Sn, X), (114Cd, X); calculated interaction parameters.
doi: 10.1016/0375-9474(75)90335-8
1975NG02 Nucl.Phys. A252, 237 (1975) C.Ngo, B.Tamain, M.Beiner, R.J.Lombard, D.Mas, H.H.Deubler Properties of Heavy Ion Interaction Potentials Calculated in the Energy Density Formalism NUCLEAR REACTIONS 108Ag(14N, X), 63Cu, 108Ag(20Ne, X), 63Cu, 108Ag, 118Sn, 121Sb(40Ar, X), 197Au(63Cu, X), 63Cu, 74Ge, 84Kr, 108Ag, 197Au, 209Bi(84Kr, X), 63Cu, 108Ag(136Xe, X), 40Ca(40Ca, X); calculated interaction potential.
doi: 10.1016/0375-9474(75)90614-4
1974AU02 Nuovo Cim. 21A, 529 (1974) High-Energy Reactions and Nuclear Densities NUCLEAR REACTIONS 208Pb, 40Ca(e, e), E=250 MeV; 208Pb, 16O(p, p), E=1 GeV; calculated σ(θ). 27Al, 208Pb(p, p), (p, p'), E=20 GeV; calculated σ(Ep', θ), σ(θ).
doi: 10.1007/BF02731355
1974BE56 Ann.Phys.(New York) 86, 262 (1974) The Energy Density Formalism and the Shell Structure Effects NUCLEAR STRUCTURE 39K, 41Ca, 89Y, 115,117,119Sn, 207Tl, 211At, 209Bi, 203,205,207,208,209Pb; calculated levels. 12C, 16O, 48,40Ca, 56,66,68Ni, 88Sr, 90Zr, 132Sn, 208Pb; calculated binding energies, neutron radii. NUCLEAR REACTIONS 40Ca, 208Pb(e, e), E=250 MeV; 58Ni, 90Zr(e, e), E=300 MeV; 120Sn(e, e), E=330 MeV; calculated σ(θ).
doi: 10.1016/0003-4916(74)90142-0
1973AU05 Phys.Lett. 45B, 115 (1973) P-Nucleus Elastic Scattering at 1 GeV NUCLEAR REACTIONS 12C, 58Ni, 208Pb(p, p), E=1.04 GeV; measured nothing, calculated σ(θ).
doi: 10.1016/0370-2693(73)90078-6
1973AU08 Phys.Lett. 47B, 261 (1973) High Energy Proton-Proton Total Cross Section and Cosmic-Ray Data NUCLEAR REACTIONS 12C, 14N, 16O, 56Fe(p, p'), E=20-100000 GeV; calculated σ.
doi: 10.1016/0370-2693(73)90726-0
1973BE62 Phys.Lett. 47B, 399 (1973) Bubble Density Distributions in Spherical Nuclei NUCLEAR STRUCTURE 36Ar, 84Se, 138Ce, 174Yb, 184,200Hg, 250Rf; calculated density distribution.
doi: 10.1016/0370-2693(73)90097-X
1973LO18 Ann.Phys.(New York) 77, 380 (1973) The Energy Density Formalism in Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 60Ni, 90Zr, 116Sn, 140Ce, 208Pb, 238U, 298Fl; calculated binding energies, proton, neutron separation energies, charge radii. NUCLEAR REACTIONS 40Ca, 208Pb(e, e), E=250 MeV; 90Zr(e, e), E=300 MeV; calculated σ(θ).
doi: 10.1016/0003-4916(73)90422-3
1972GI05 Nucl.Phys. A185, 321 (1972) J.Gizon, H.Ohlsson, J.Valentin, R.J.Lombard Rapports de Probabilites de Transition E0 et E2 dans 178Hf RADIOACTIVITY 178W, 178Ta; measured Iγ, I(ce). 178Hf deduced α(K), α(L), I(E0)/I(E2), transition probability ratios, nuclear deformation parameters β.
doi: 10.1016/0375-9474(72)90574-X
1971LO13 Phys.Lett. 35B, 493 (1971) On the Stability of the Even He-Isotopes NUCLEAR STRUCTURE 4,6,8,10He; calculated binding energy, symmetry energy contribution.
doi: 10.1016/0370-2693(71)90379-0
1970BR02 Phys.Lett. 31B, 97 (1970) K.A.Brueckner, M.J.Giannoni, R.J.Lombard Statistical Estimate of the Breathing Mode Energy NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 116Sn, 140Ce, 208Pb; calculated mass radii, binding energy, energy of breathing mode.
doi: 10.1016/0370-2693(70)90119-X
1970LO11 Phys.Lett. 32B, 652 (1970) Comparison between Hartree-Fock and Thomas-Fermi Calculations Using Effective Interactions NUCLEAR STRUCTURE 40Ca, 208Pb; calculated binding energy, radii. Hartree-Fock, energy density formalisms.
doi: 10.1016/0370-2693(70)90434-X
1969BR15 Phys.Rev. 181, 1506 (1969) K.A.Brueckner, W.-f.Lin, R.J.Lombard Isotope Shift of Nuclear Charge Distributions NUCLEAR STRUCTURE 40,48Ca, 116,124Sn, 202,208Pb; calculated isotope shift of nuclear charge distribution.
doi: 10.1103/PhysRev.181.1506
1969BR16 Phys.Rev. 181, 1543 (1969) K.A.Brueckner, J.R.Buchler, R.C.Clark, R.J.Lombard Statistical Theory of Nuclei. II. Medium and Heavy Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 116Sn, 140Ce, 208Pb, 246Pu; A = 298; calculated binding energies, separation energies, nuclear radii.
doi: 10.1103/PhysRev.181.1543
1968LO08 Nucl.Phys. A117, 365 (1968) Study of Neutron Closed-Shell Nuclei
doi: 10.1016/0375-9474(68)90850-6
1968LO16 Nucl.Phys. A110, 41 (1968) R.J.Lombard, C.F.Perdrisat, J.H.Brunner Internal Pair Formation and Multipolarity of Nuclear Transitions
doi: 10.1016/0375-9474(68)90681-7
1965LO05 Nucl.Phys. 71, 348 (1965) Magnetic Moments of Some Excited States of Sn and Pb Isotopes NUCLEAR STRUCTURE 202Pb, 200Pb, 206Pb, 204Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(65)90722-4
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