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NSR database version of May 8, 2024.

Search: Author = R.Reif

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1992TI03      Phys.Lett. 296B, 296 (1992)

G.-R.Tillack, R.Reif, A.Schulke, P.Frobrich, H.J.Krappe, H.G.Reusch

Light Particle Emission in the Langevin Dynamics of Heavy-Ion Induced Fission

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁸O, F), E=159 MeV; calculated fission fragment total kinetic energy distribution, (fragment)n-coin, prescission particle multiplicities. ²¹⁵Fr deduced light particle emission features. Langevin dynamics.

NUCLEAR STRUCTURE ²¹⁵Fr; calculated prescission fission induced light particle multiplicities; deduced light particle emission features. Langevin dynamics.

doi: 10.1016/0370-2693(92)91323-2
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1990MA16      Z.Phys. A335, 473 (1990)

P.Madler, R.Reif, G.-R.Tillack

Correlations between Preequilibrium Particles and Fission Fragments ( Question )

NUCLEAR REACTIONS ²⁵¹Bk(p, α), E=160 MeV; calculated σ(Eα, φα) following residue fission. ²⁵²Cf deduced symmetric fission features. Exciton model, preequilibrium particle emission.

1988MI25      Yad.Fiz. 48, 378 (1988); Sov.J.Nucl.Phys. 48, 237 (1988)

B.Milek, R.Reif

Semiclassical Description of a Realistic Nuclear Problem of Pseudocrossing between Two Terms

NUCLEAR REACTIONS ¹³C(¹⁷O, ¹⁷O'), E(cm) ≈ 16-25 MeV; calculated σ(E); deduced two level pseudocrossing features.

1986MI22      Nucl.Phys. A458, 354 (1986)

B.Milek, R.Reif

Gamow States in a Realistic Two-Center Potential and Nucleon Emission in Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁷O(¹⁶O, n), E=50 MeV; calculated neutron emission spectrum. ¹⁷O(¹⁶O, ¹⁶O), E=50 MeV; calculated Gamow state occupation probability, decay width, energy. Two-center shell model, coupled channel calculation.

doi: 10.1016/0375-9474(86)90361-1
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1985GU08      Nucl.Phys. A436, 294 (1985)

F.Guzman Martinez, R.Reif

Incomplete Deep-Inelastic Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁸¹Ta(²⁰Ne, α¹⁶O), E=166 MeV; calculated breakup σ decomposition, γ-multiplicity. ⁴⁰Ca(²⁰Ne, X), E=262 MeV; calculated σ(fragment E, θ). ⁴⁰Ca(²⁰Ne, α¹⁶O), E=262 MeV; calculated σ(θα, θ(¹⁶O)); ⁴⁰Ca(²⁰Ne, αX), E=151 MeV; calculated σ(fragment θ, Z). ¹⁹⁷Au(²⁰Ne, X), E=175 MeV; Cu(²⁰Ne, X), E=170 MeV; ⁵⁶Ni(²⁰Ne, X), E=164 MeV; ⁴⁰Ca(²⁰Ne, X), E=151 MeV; calculated σ(fragment Z). Phenomenological two-step model.

doi: 10.1016/0375-9474(85)90200-3
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1985MI13      Phys.Lett. 157B, 134 (1985)

B.Milek, R.Reif

Nuclear Landau-Zener Effect in ¹⁷O + ¹³C ( Question )

NUCLEAR REACTIONS, ICPND ¹³C(¹⁷O, ¹⁷O), E(cm)=15-25 MeV; calculated σ(E) for inelastic, transfer channels. Two-center shell model, truncated molecular orbit set.

doi: 10.1016/0370-2693(85)91532-1
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1984JA13      Nucl.Phys. A425, 152 (1984)

D.Janssen, M.Militzer, R.Reif

Microscopic Description of Heavy-Ion Collisions in Terms of Interacting RPA Modes

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=320 MeV; ²⁰⁸Pb(²⁰⁸Pb, X), E=1580.8 MeV; calculated intrinsic fragment spin L time dependence. Interacting RPA modes, microscopic model.

doi: 10.1016/0375-9474(84)90221-5
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1982MA03      Nucl.Phys. A373, 27 (1982)

P.Madler, R.Reif

Relaxation Phenomena in Nucleon-Induced Reactions and Preequilibrium Angular Distributions

NUCLEAR REACTIONS ⁹³Nb(n, n'), E=14.1 MeV; ²⁰⁸Pb(n, n'), E=14.6 MeV; calculated σ(θ); ²⁰⁸Pb(p, n), E=45 MeV; calculated σ(θn, En). Preequilibrium state, relaxation phenomena.

doi: 10.1016/0375-9474(82)90180-4
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1982OE01      Phys.Lett. 119B, 293 (1982)

L.Oehme, R.Reif

Direct and Dissipative Modes in Heavy-Ion Reactions: Incomplete deep inelastic collisions

NUCLEAR REACTIONS ⁴⁰Ca(²⁰Ne, ¹⁶OX), E=260 MeV; calculated σ(E(¹⁶O), θ). Incomplete deep inelastic collision, direct, dissipative modes.

doi: 10.1016/0370-2693(82)90673-6
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1982RE01      J.Phys.(London) G8, L21 (1982)

R.Reif, G.Saupe

Spin Alignment and Polarisation in (¹⁴N, ¹²B) Reactions

NUCLEAR REACTIONS ²³²Th, ¹⁰⁰Mo(¹⁴N, ¹²B), E=200 MeV; ²⁷Al, Cu(¹⁴N, ¹²B), E=120 MeV; calculated fragment polarization, alignment. Friction model, statistical fluctuations.

doi: 10.1088/0305-4616/8/2/002
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1982RE02      J.Phys.(London) G8, 257 (1982)

R.Reif, B.Weissbach, E.Betak, Ch.Stoyanov, A.I.Vdovin

Direct Inelastic Proton Scattering from Odd-A Nuclei within the Semimicroscopic Quasiparticle-Phonon Model

NUCLEAR REACTIONS ⁸⁸Sr(p, p'), E=20.2 MeV; ⁸⁹Y(p, p'), E=24.5 MeV; calculated σ(θ). ⁸⁸Sr, ⁸⁹Y levels deduced configuration. Semi-microscopic, quasiparticle-phonon model, DWBA, CCBA analyses.

doi: 10.1088/0305-4616/8/2/012
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1981SC07      J.Phys.(London) G7, 775 (1981)

R.Schmidt, R.Reif

Angular Momentum Dissipation and Orientation in Deep Inelastic Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁶⁶Er(⁸⁶Kr, X), E=515 MeV; ²³⁸U(⁸⁶Kr, X), E=730 MeV; ¹⁰⁰Mo(¹⁴N, X), E=90, 125, 200 MeV; analyzed total angular momentum dissipation, fragment polarization and alignment data. Deep inelastic collisions, linear response theory, classical model.

doi: 10.1088/0305-4616/7/6/011
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1981YO05      Yad.Fiz. 33, 1006 (1981)

M.I.Yousef, R.Reif

Cluster Transfer Reactions between Heavy Ions within a Generalized Diffraction Model

NUCLEAR REACTIONS ¹²C(¹¹B, ¹²C), E=28 MeV; ¹¹B(¹²C, ¹¹B), E=87 MeV; ¹²C(¹⁹F, ²⁰Ne), E=60 MeV; ⁴⁸Ca(¹⁶O, ¹⁴C), E=56 MeV; ⁶⁰Ni(¹⁸O, ¹⁶O), E=65 MeV; ²⁴Mg(¹⁶O, ¹²C), E=36, 48 MeV; ²⁸Si(¹⁶O, ¹²C), E=36, 42, 53 MeV; ³²S(¹⁶O, ¹²C), E=45 MeV; ²⁹Si(¹⁶O, ¹⁵N), E=60, 73.5 MeV; analyzed σ(θ). Cluster transfer, generalized diffraction model.

1980MA09      Nucl.Phys. A337, 445 (1980)

P.Madler, R.Reif

Angular Distributions of Preequilibrium Reactions within a Generalized Exciton Model

NUCLEAR REACTIONS ⁹³Nb(n, n'), E=14.1 MeV; ²⁰⁹Bi, ²⁷Al(p, p'), E=62 MeV; ¹¹⁹Sn(p, p'), E=17 MeV; ²⁰⁸Pb(p, n), E=45 MeV; calculated σ(θ). Preequilibrium reactions, generalized exciton model.

doi: 10.1016/0375-9474(80)90153-0
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1979SC23      J.Phys.(London) G5, L181 (1979)

R.Schmidt, R.Reif

Angular Momentum Dissipation in DIC within a Classical Friction Model

NUCLEAR REACTIONS ¹⁶⁶Er(⁸⁶Kr, X), E=515 MeV; calculated angular momentum loss, deflection function θ, interaction time vs incoming L. Classical friction model for deep-inelastic collisions.

doi: 10.1088/0305-4616/5/10/007
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1974RE08      Phys.Lett. 52B, 163 (1974)

R.Reif, R.Schmidt

Spin Dependence in Inelastic Proton Scattering from Odd-A Nuclei

NUCLEAR REACTIONS ⁶³Cu(p, p'), E=11 MeV; calculated σ(Ep', θ), P(θ).

doi: 10.1016/0370-2693(74)90078-1
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1972EL10      Nucl.Phys. A189, 305 (1972)

A.El-Naiem, R.Reif

Investigation of the Reaction ²⁸Si(d, p)²⁹Si at E = 10 MeV

NUCLEAR REACTIONS ²⁸Si(d, p), E=10 MeV; analyzed σ(θ). ²⁹Si deduced levels, L(n), J, π, S. DWBA.

doi: 10.1016/0375-9474(72)90297-7
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1972IW01      Nucl.Phys. A183, 105 (1972)

H.Iwe, R.Reif, C.Riedel

Reaction Spectroscopy with Even Tin Isotopes

NUCLEAR REACTIONS ^116,118Sn(t, p), E=12 MeV; ¹¹⁶Sn(p, p'), E=55 MeV; ^116,118,120Sn(p, p'), E=16 MeV; calculated σ(θ). DWBA.

doi: 10.1016/0375-9474(72)90933-5
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1969HO19      Nucl.Phys. A134, 289 (1969)

J.Hohn, H.Pose, D.Seeliger, R.Reif

Elastic and Inelastic Scattering of 14.7 MeV Neutrons from ²⁸Si

NUCLEAR REACTIONS ²⁸Si(n, n), (n, n'); E=14.7 MeV; measured σ(En', θ). ²⁸Si levels deduced deformation parameters β(L), interaction strengths V(S). Natural targets.

doi: 10.1016/0375-9474(69)91053-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22701.

1969RE10      Nucl.Phys. A137, 65 (1969)

R.Reif, J.Hohn

Inelastic Proton Scattering and One-Particle-One-Hole Excitations in Light Nuclei

NUCLEAR REACTIONS ¹⁶O, ²⁸Si, ³²S(p, p'), E = 17.5 MeV; calculated Q, P(θ), σ(θ), form factors.

doi: 10.1016/0375-9474(69)90072-4
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1968RE03      Phys.Letters 26B, 484 (1968)

R.Reif, J.Slotta, J.Hohn

Excitation of Non-Normal Parity States in Inelastic Proton Scattering

doi: 10.1016/0370-2693(68)90358-4
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1967SC16      Nucl.Phys. A101, 577 (1967)

H.Schulz, H.J.Wiebicke, R.Reif

Single-Particle States in Non-Local Potentials and Direct Nuclear Reactions

doi: 10.1016/0375-9474(67)90653-7
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1965BA31      Nucl.Phys. 73, 473 (1965)

H.W.Barz, R.Fulle, D.Netzband, R.Reif, K.Schlott, J.Slotta

The Reaction ¹⁰B(d, p₀)¹¹B

NUCLEAR REACTIONS ¹⁰B(d, p₀), E = 13.5 MeV; measured σ(θ). ¹¹B deduced level-width, L, S. Enriched target.

doi: 10.1016/0029-5582(65)90692-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0336.