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NSR database version of April 11, 2024.

Search: Author = L.Rikus

Found 10 matches.

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1988AM01      Phys.Rev. C37, 934 (1988)

K.Amos, L.Berge, F.A.Brieva, A.Katsogiannis, L.Petris, L.Rikus

Off-Shell Properties of the Two-Nucleon t Matrix

NUCLEAR STRUCTURE 2H; calculated binding energy.

doi: 10.1103/PhysRevC.37.934
Citations: PlumX Metrics

1985VO06      Lett.Nuovo Cim. 42, 209 (1985)

H.V.von Geramb, K.Nakano, L.Rikus

Microscopic Analysis of Antiproton Scattering from Carbon

NUCLEAR REACTIONS 12C(p-bar, p-bar), E at 300 MeV/c; analyzed data. Paris, Bryan-Phillips potentials, microscopic model.

doi: 10.1007/BF02739457
Citations: PlumX Metrics

1984LA04      Nucl.Phys. A414, 309 (1984)

G.La Rana, C.Ngo, A.Faessler, L.Rikus, R.Sartor, M.Barranco, X.Vinas

Heavy-Ion Optical Potentials at Finite Temperature Calculated using a Complex Effective Interaction Derived from a Realistic Force

NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=400, 800 MeV; 208Pb(40Ca, 40Ca), E=1 GeV; calculated optical potential parameters vs separation distance, temperature. Double folding method.

doi: 10.1016/0375-9474(84)90647-X
Citations: PlumX Metrics

1984RI03      Nucl.Phys. A414, 413 (1984)

L.Rikus, K.Nakano, H.V.Von Geramb

Microscopic Analysis of Elastic and Inelastic Proton Scattering from 12C

NUCLEAR REACTIONS 12C(p, p), (p, p'), (polarized p, p), (polarized p, p'), E=122-400 MeV; calculated σ(θ), polarization, analyzing power, spin flip probability vs θ. First-principle optical potentials, distorted wave inelastic transition amplitude.

doi: 10.1016/0375-9474(84)90611-0
Citations: PlumX Metrics

1984RI14      Nucl.Phys. A426, 496 (1984)

L.Rikus, H.V.Von Geramb

Microscopic Analyses of Proton Scattering from Lead

NUCLEAR REACTIONS 207Pb(p, p), E=134.8, 198.6 MeV; 208Pb(p, p), E=134.8-400 MeV; calculated σ(θ), P(θ). Microscopic optical potentials, Paris nucleon-nucleon potential.

doi: 10.1016/0375-9474(84)90160-X
Citations: PlumX Metrics

1983FA08      Nucl.Phys. A401, 157 (1983)

A.Faessler, L.Rikus, S.B.Khadkikar

The Heavy-Ion Potential and Its Increasing Transparency at Intermediate Energies

NUCLEAR REACTIONS 16O(16O, 16O), (16O, X), E(cm)=2.6-93.4 MeV/nucleon; calculated real part of interaction potential, reaction σ(E). 16O(16O, 16O), E=80 MeV; 16O(16O, 16O), E(cm)=23.3, 41.5, 93.4 MeV/nucleon; calculated σ(θ). 12C(12C, 12C), E=1016 MeV; calculated σ(θ). 12C(12C, X), E(cm) ≈ 2-100 MeV/nucleon; calculated total reaction σ(E). Bethe-Goldstone equation, complex reaction matrix.

doi: 10.1016/0375-9474(83)90342-1
Citations: PlumX Metrics

1982RI05      Aust.J.Phys. 35, 9 (1982); Corrigendum Aust.J.Phys. 35, 351 (1982)

L.Rikus, S.F.Collins, K.A.Amos, B.M.Spicer, G.G.Shute, I.Morrison, V.C.Officer, R.Smith, D.W.Devins, D.L.Friesel, W.P.Jones

Excitation of the 9.50 MeV (9/2+) States of 13C in Intermediate Energy Scattering Experiments

NUCLEAR REACTIONS 13C(p, p'), E=135 MeV; measured σ(θ). 13C state deduced total angular momentum transfer, configuration. Microscopic DWBA analysis.

1981KH03      Nucl.Phys. A369, 495 (1981)

S.B.Khadkikar, L.Rikus, A.Faessler, R.Sartor

Surface and Volume Contributions to Real and Imaginary Parts of the Heavy-Ion Optical Potential

NUCLEAR REACTIONS 16O(16O, 16O), E=80, 332 MeV; calculated σ(θ). Feshbach projection technique, heavy-ion optical potential.

doi: 10.1016/0375-9474(81)90034-8
Citations: PlumX Metrics

1980RI05      J.Phys.(London) G6, 1535 (1980)

L.Rikus, K.Amos

Low-Energy Neutron Scattering from 12C and Nuclear Spectroscopy

NUCLEAR REACTIONS 12C(n, n), E=0-4 MeV; calculated σ(E, total). R-matrix, shell model reduced widths.

doi: 10.1088/0305-4616/6/12/009
Citations: PlumX Metrics

1977RI11      Nucl.Phys. A286, 494 (1977)

L.Rikus, R.Smith, I.Morrison, K.Amos

A Microscopic Model Analysis of the 90Zr(p, n) IAS Transition

NUCLEAR REACTIONS 90Zr(p, n), E=18.5-45 MeV; calculated σ(E, θ) to IAS.

doi: 10.1016/0375-9474(77)90598-X
Citations: PlumX Metrics

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