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NSR database version of April 29, 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
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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
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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
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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