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NSR database version of April 11, 2024.

Search: Author = R.J.Lombard

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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)

R.Mezhoud, R.J.Lombard

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2001LO20      Yad.Fiz. 64, No 7, 1315 (2001); Phys.Atomic Nuclei 64, 1240 (2001)

R.J.Lombard

Remarks on Halo Nuclei

NUCLEAR STRUCTURE 6He, 11Li, 11Be, 14B, 15,17,19C; analyzed radius vs separation energy.

doi: 10.1134/1.1389549
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1999LA04      Eur.Phys.J. A 4, 111 (1999)

M.Lassaut, R.J.Lombard

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1997FO04      J.Phys.(London) G23, 423 (1997)

J.Formanek, R.J.Lombard

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
Citations: PlumX Metrics


1995FO08      J.Phys.(London) G21, 87 (1995)

J.Formanek, R.J.Lombard

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1995LO08      Phys.Rev. C52, 170 (1995)

R.J.Lombard, J.Mares

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1993CA21      Phys.Rev. C48, 830 (1993)

F.Carstoiu, R.J.Lombard

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
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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
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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
Citations: PlumX Metrics


1992LA13      Z.Phys. A341, 125 (1992)

M.Lassaut, R.J.Lombard

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1990LO02      Phys.Rev. C41, R1348 (1990)

R.J.Lombard, J.P.Maillet

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
Citations: PlumX Metrics


1990LO10      Europhys.Lett. 12, 119 (1990)

R.J.Lombard

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
Citations: PlumX Metrics


1990LO11      J.Phys.(London) G16, 1311 (1990)

R.J.Lombard

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
Citations: PlumX Metrics


1990LO13      Phys.Lett. 245B, 649 (1990)

R.J.Lombard, J.P.Maillet

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1986AN19      Z.Phys. A324, 299 (1986)

I.Angeli, R.J.Lombard

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
Citations: PlumX Metrics


1986AU10      J.Phys.(London) G12, 1341 (1986)

J.P.Auger, D.Mas, R.J.Lombard

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
Citations: PlumX Metrics


1986LO07      Ann.Phys.(New York) 167, 2 (1986)

R.J.Lombard, D.Mas

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1983LO02      Phys.Lett. 120B, 23 (1983)

R.J.Lombard, D.Mas

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


1980AU03      Phys.Lett. 90B, 200 (1980)

J.P.Auger, R.J.Lombard

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
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1980AU09      Nucl.Phys. A350, 332 (1980)

J.P.Auger, R.J.Lombard

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
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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
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1980LO03      Nucl.Phys. A336, 185 (1980)

R.J.Lombard, D.Mas

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
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1979AU04      Nucl.Phys. A316, 205 (1979)

J.P.Auger, R.J.Lombard

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
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1978AU11      Ann.Phys.(New York) 115, 442 (1978)

J.P.Auger, R.J.Lombard

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
Citations: PlumX Metrics


1978AU12      J.Phys.(London) G4, L261 (1978)

J.-P.Auger, R.J.Lombard

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
Citations: PlumX Metrics


1978BA49      Phys.Lett. 78B, 542 (1978)

M.Barranco, R.J.Lombard

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
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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
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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
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1976LO12      Phys.Lett. 65B, 193 (1976)

R.J.Lombard

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
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1975BE31      Nucl.Phys. A249, 1 (1975)

M.Beiner, R.J.Lombard, D.Mas

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
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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
Citations: PlumX Metrics


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
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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
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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
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1974AU02      Nuovo Cim. 21A, 529 (1974)

J.P.Auger, R.J.Lombard

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
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1974BE56      Ann.Phys.(New York) 86, 262 (1974)

M.Beiner, R.J.Lombard

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
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1973AU05      Phys.Lett. 45B, 115 (1973)

J.P.Auger, R.J.Lombard

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
Citations: PlumX Metrics


1973AU08      Phys.Lett. 47B, 261 (1973)

J.P.Auger, R.J.Lombard

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
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1973BE62      Phys.Lett. 47B, 399 (1973)

M.Beiner, R.J.Lombard

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
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1973LO18      Ann.Phys.(New York) 77, 380 (1973)

R.J.Lombard

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
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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
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1971LO13      Phys.Lett. 35B, 493 (1971)

R.J.Lombard

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
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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
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1970LO11      Phys.Lett. 32B, 652 (1970)

R.J.Lombard

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
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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
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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
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1968LO08      Nucl.Phys. A117, 365 (1968)

R.J.Lombard

Study of Neutron Closed-Shell Nuclei

doi: 10.1016/0375-9474(68)90850-6
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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
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1965LO05      Nucl.Phys. 71, 348 (1965)

R.J.Lombard

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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